Physics Part Ii Chapter 10 Wave Optics
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    NCERT Solution For Class 12 Physics Physics Part Ii

    Wave Optics Here is the CBSE Physics Chapter 10 for Class 12 students. Summary and detailed explanation of the lesson, including the definitions of difficult words. All of the exercises and questions and answers from the lesson's back end have been completed. NCERT Solutions for Class 12 Physics Wave Optics Chapter 10 NCERT Solutions for Class 12 Physics Wave Optics Chapter 10 The following is a summary in Hindi and English for the academic year 2021-2022. You can save these solutions to your computer or use the Class 12 Physics.

    Question 1
    CBSEENPH12038172

    A small candle, 2.5 cm in size is placed at 27 cm in front of a concave mirror of radius of curvature 36 cm. At what distance from the mirror should a screen be placed in order to obtain a sharp image? Describe the nature and size of the image. If the candle is moved closer to the mirror, how would the screen have to be moved?

    Solution
    Given, 

    Object size = 2.5 cm

    Object distance, u = -27 cmRadius of curvature, R = 36 cmFocal length,  f =R2 = -362 = -18 cmImage distance, 1v = 1f-1u = -118-1-27                         1v = 127-118 =- 154i.e.,                          v = -54 cm

    The negative sign indicates that the image is formed in front of the mirror. Thus, the screen should be placed at a distance of 54 cm in front of the mirror on the same side as that of the object. 

    Now,
    Magnification, m = IO = -vu

                  I2.5 =-54-27         I = - 5 cm 

    As size of image is (–)ve. So image is inverted and real. 

    When the candle is moved closer to mirror, the screen would have to be moved farther and farther. However, when the candle is closer than 18 cm from the mirror, the image would be virtual and therefore cannot be collected on the screen.


    Question 2
    CBSEENPH12038173

    A 4.5 cm needle is placed 12 cm away from a convex mirror of focal length 15 cm. Give the location of the image and the magnification. Describe what happens as the needle is moved farther from the mirror.

    Solution

    Given,

    Object distance, u = -12 cmFocal length, f = + 15 cmSize of the object, O = 4.5 cm

    Now using the mirror formula, 
                        1u+1v =1f 
    we have, 

                 1v =1f-1u       =115+112        = 4+560        = 960 v = 60/9 = 6.7 cm

    ∴ Image is formed at 6.7 cm at the back of the mirror ( because v is positive)
    Now,
    Magnification, m = IO = -vu 

                           I4.5 = -6.7-12        I = 6.7 × 4.512          = 2.5 cm. 

    Hence, the image formed is erect, and of course virtual. 

    As, needle is moved farther away from the mirror then as a result, image moves away from the mirror (upto F) and keeps on decreasing in size.

    Question 3
    CBSEENPH12038174

    A tank is filled with water to a height of 12.5 cm. The apparent depth of a needle lying at the bottom of the tank is measured by a microscope to be 9.4 cm. What is the refractive index of water? If water is replaced by a liquid of refractive index 1.63 up to the same height, by what distance would the mircoscope have to be moved to focus on the needle again?

    Solution
    Case I: When tank is filled with water.

    Given, real depth = 12.5 cm;
              apparent depth = 9.4 cm 

    Now, using the formula, 

                        μ = real depthapparent depth

    we have,
    Refractive index,  μ = 12.59.4 = 1.33

    Case II: When water in the tank is replaced by another liquid.

    Refractive index of liquid, μ = 1.63Real depth = 12.5 cm
    Therefore,
    apparent depth = real depthμ 

    i.e., apparent depth = 12.51.63 = 7.67 cm

    Distance through which microscope has to be moved downward is = (9.4 – 7.67) cm = 1.73 cm.

    Question 4
    CBSEENPH12038175

    Figures (a) and (b) show refraction of a ray in air incident at 60° with the normal to a glass-air and water-air interface, respectively. Predict the angle of refraction in glass when the angle of incidence in water is 45° with the normal to a water-glass interface. [ Fig. 9.34 (c)].


    Solution

    (a)
    Given, 

    Angle of incidence, i = 60°Angle of refraction,  r = 35° 

    Using Snell's law, we have 

    Refractive index of glass with respect to air,     μga = sin isin r = sin 60°sin 35°

             = 0.86600.5736 = 1.51                                   

    (b) 

    Angle of incidence, i = 60°Angle of refraction, r = 41° 

    Using Snell's law, 

    Refractive index of water wr.to air, μwa = sin isin r = sin  60°sin 41° = 1.32 

    (c)
    Angle of incidence in water, i =45°

    Refractive index of glass wr.to water,
     μgω = μgaμwa =sin isin r
             1.511.32 = sin 45°sin r = 0.7071sin r

     sin r = 1.32 × 0.70711.51 = 0.6181 

        r = 38.2°, which is the required angle of refraction of glass.


           

    Question 5
    CBSEENPH12038176

    A prism is made of glass of unknown refractive index. A parallel beam of light is incident on a face of the prism. The angle of minimum deviation is measured to be 40°. What is the refractive index of the material of the prism? The refracting angle of the prism is 60°. If the prism is placed in water (refractive index 1.33), predict the new angle of minimum deviation of a parallel beam of light.

    Solution

    Given, 

    Refracting angle of prism, A = 60°Angle of minimum deviation,  δm = 40° 
    Refractive index of glass w.r.t air, aμg = SinA+δm2SinA/2 
              μga = sin 50°sin 30° = 0.7660.54 = 1.532 

    After the prism is placed in water, 

    Refractive index of water = 1.33
    Using the formula,

                    μgω = sinA+δ'm2Sin A/2

                  μgaμwa = sin 60+δ'm2sin 30° 

    sin 30°+δ'm2 = 12×1.5321.33 = 0.5759

       30°+δ'm2 = 35°10' 

            A+δ'm2= 35o10' 
               A + δ'm = 70o 20'δ'm = 70o 20' - A       = 70020' - 60o 

    i.e.,     δ'm = 10°20'.

    which is the reqiured angle of minimum deviation. 

    Question 6
    CBSEENPH12038177

    Double-convex lenses are to be manufactured from a glass of refractive index 1.55, with both faces of the same radius of curvature. What is the radius of curvature required if the focal length is to be 20 cm?

    Solution
    Given,
    Refractive index, μ = 1.55
    Radius of curvature, R
    1 = R and R2 = – R
    Focal length, f = 20 cm. 

    Using the lensmaker formula,
    1f = (μ -1) 1R1-1R2 
    we have, 
    120 = (1.55 - 1) 1R+1R = 1.10R 

    Hence, 
    R = 20 × 1.1 = 22 cm, which is the required radius of curvature. 
    Question 7
    CBSEENPH12038178

    A beam of light converges at a point P. Now a lens is placed in the path of the convergent beam 12 cm from P. At what point does the beam converge if the lens is (a) a convex lens of a focal length 20 cm, and (b) a concave lens of focal length 16 cm?

    Solution
    Here, the point P on the right of the lens acts as a virtual object.

    Object distance, u = 12 cm
     Focal length, f = 20 cm 

    (a) Using the lens formula,
                   1v =1f+1u

               1v =120+112      =3+560 =860

    i.e.,           v = 60/8 = 7.5 cm. 

    Image is at a distance of 7.5 cm to the right of the lens, where the beam converges.

    (b)
    Now,
    Focal length of concave lens, f = –16 cm
    Object distance, u = 12 cm 

     
              1v=1f+1u     =-116+112     = -3+448    =148 

          v = 48 cm 

    Hence, the image is at a distance of 48 cm to the right of the lens, where the beam would converge.
    Question 8
    CBSEENPH12038179

    An object of size 3.0 cm is placed 14 cm in front of a concave lens of focal length 21 cm. Describe the image produced by the lens. What happens if the object is moved further away from the lens?

    Solution
    Size of object, O = 3.0 cm
    Object distance, u = – 14 cm
    Focal length, f = – 21 cm 
    Image distance, v = ?

    Using the lens formula,

    1v = 1f+1u      =-121-114      =-3514 × 21   v = -8.4 cm. 

    The image is located 8.4 cm from the lens on the same side as that of the object.

    Magnification, m = IO =vu 

     Image size, I = vu× O   = -8.4-14×3   = 1.8 cm 

    As size of image is +ve. So, image is errect and virtual of smallar size. 

    As the object is moved away from the lens, the virtual image moves towards the focus of the lens but never beyond. The image progressively diminishes in size.
    Question 9
    CBSEENPH12038180

    What is the focal length of a convex lens of focal length 30 cm in contact with a concave lens of focal length 20 cm? Is the system a converging or a diverging lens? Ignore thickness of the lenses.

    Solution
    Given,
    Focal length of the convex lens, f
    1 = 30 cm
    Focal length of concave lens, f
    2 = –20 cm

    Therefore, the focal length of the combination of lenses,
                         1f = 1f1+1f2

                      1f = 130-120      =2-360      =-160

                            f = -60 cm
    ∴ The combination of lenses behaves as a concave lens as their focal length is negative. Hence, the system is not converging.
    Question 10
    CBSEENPH12038181

    A compound microscope consists of an objective lens of focal length 2.0 cm and an eyepiece of focal length 6.25 cm separated by a distance of 15 cm. How far from the objective should an object be placed in order to obtain the final image at (a) the least distance of distinct vision (25 cm), and (b) at infinity? What is the magnifying power of the microscope in each case?

    Solution
    Given,
    ,Focal length of the objective lens, f0 = 2 cmFocal length of the eyepiece, fe = 6.25 cmDistance between eyepiece and objective lens = 15 cmDistance of object from objective lens, u0 = ?


    (a) For eyepiece,

    Image distance, ve = -25 cm (given as least distance of distict vision)

    Now, using the formula,
                          1ve-1ue = 1fe  1ue = 1ve-1fe 

                            1ue = 1-25-16.25 = -15
    i.e.,                        ue = - 5 cm, which is the distance of the object from the eyepiece.

    Now, 
    Distance of object from objective lens, v0 = 15-ue      = 10 cm 
    Therefore, for objective 

    Using the formula, 

                    1v0-1u0 =1f0 1u0 = 1v0-1f0  

                         1u0 = 110-12        = -25    u0 = -52 cm = -2.5 cm 

    Magnifying power,  M = v0u01+Dfe
                               M = 10-2.51+256.25 = -20


    (b) If the image formed by the objective is in the focal plane of the eyepiece then, the final image will be formed at infinity.

     object distance, ue = fe = 6.25 cm;
    Image distance from objecrtive lens,  v0 = (15-6.25) cm = 8.75 cm 

    Now, using the formula, we have
                    1u0 = 1v0-1f0        = 18.75-12         =-6.758.75 ×2 

     u0 = 8.75 × 26.75 cm uo = -2.59 cm 

    which is the distance of the object from the objective lens. 

    Magnifying power M, =8.75-2.59×256.25= -13.5.
    Question 11
    CBSEENPH12038182

    A person with a normal near point (25 cm) using a compound microscope with objective of focal length 8.0 mm and an eye piece of focal length 2.5 cm can bring an object placed 9.0 mm from the objective in sharp focus. What is the separation between the two lenses? Calculate the magnifying power of the microscope?

    Solution
    Here,
    Distance of object from the objective lens, u
    0 = –0.9 cm
    Focal length of objective lens, f
    0 = 0.8 cm 

    As,      1v0-1u0 = 1f0
          1v0 = 1f0+1u0        =10.8-10.9       =17.2 

    i.e.,     v0 = 7.2 cm 
    which is the distnce of the imge from the objective.

    Now for the eyepiece, we have
    Focal length of eyepiece, f
    e = 2.5 cm
    Image distance from eyepiece, v
    e = – D = -25 cm
    Object distance from eyepiece, u
    e =?
    Since, 
            1ue = 1ve-1fe        =-125-12.5        =-1125

    i.e.,      ue=-2511=-2.27 cm 

    Separation between the two lenses,  = v0+ue= 7.2 + 2.27 = 9.47 cm

    Magnifying power,   M = M0 × Me
                                  M = v0u01+Dfe    = 7.20.91+2525  

                                    = 8 × 11 = 88
    Question 12
    CBSEENPH12038183

    A small telescope has an objective lens of focal length 144 cm and an eyepiece of focal length 6.0 cm. What is the magnifying power of the telescope? What is the separation between the objective and the eyepiece?

    Solution

    Here,
    Focal length of the objective, f0 = 144 cmFocal length of eyepiece,  fe = 6.0 cm
    Magnifying power of telescope,
                 m = -f0fe     = -1446.0    = -24 

    Seperation between the objective and the eyepiece,  L = f0+fe    = 144+6.0 = 150 cm.

    Question 13
    CBSEENPH12038184

    A giant refracting telescope at an observatory has an objective lens of focal length 15 m. If an eyepiece of focal length 1.0 cm is used, what is the angular magnification of telescope?

    Solution
    Given,
    Focal length of objective lens, fo
     = 15 m
    Focal length of eyepiece, f
    e = 1.0 cm = 10–2 m 
    Therefore,
    Angular magnification =  f0fe=1510-2 = 1500
    Question 14
    CBSEENPH12038185

    If this telescope is used to view the moon, what is the diameter of the image of the moon formed by the objective lens? The diameter of the moon is 3.48 x 106 m and radius of lunar orbit is 3.8 x 108 m.

    Solution

    Given,
    Diameter of moon = 3.48 x 106 m 
    Radius of lunar orbit, r = 3.8 x 108 m 
    Focal length of objective, fo = 15 cm 

    If d is diameter of the image, then
    Angle subtended by diameter of moon = 3.48 × 1063.8 × 108
    and,

    Angle subtended by image= df0= d15
                                 d15 =3.48 × 1063.8 × 108 

    Therefore,
    Diameter of the image of the moon  formed by objective lens, d = 3.48 × 15 × 10-23.8
                             = 13.73 × 10-2m = 13.73 cm.                        

     
    Question 15
    CBSEENPH12038186

    Use the mirror equation to deduce that:
    an object placed between f and 2f of a concave mirror produces a real image beyond 2f.

    Solution
    The mirror formula is
                      1u+1v=1f
                   
                  1v = 1f-1u 

    Now for a concave mirror, f < 0 and for an object on the left u < 0.
                    
     2f < u < f

                   12f>1u>1f

                 -12f<-1u<-1f

                 1f-12f<1f-1u<1f-1f

                   12f<1v<0 

    This implies that v < 0 so that real image is formed on left. Also, the above inequality implies that

                         2f>v 
                       2f > v          2f and v are -ve 

    i.e., real image is formed beyond 2f. 
    Question 16
    CBSEENPH12038187

    Use the mirror equation to deduce that:
    a convex mirror always produces a virtual image independent of the location of the object.

    Solution
    For convex mirror, f > 0 and for an object of left, u < 0. 
    From mirror formula, 

                   1v =1f-1u

               1v>0   or  v>0 

    This shows that whatever be the value of u, a convex mirror form a virtual image on the right (because v is positive).
    Question 17
    CBSEENPH12038188

    Use the mirror equation to deduce that:
    an object placed between the pole and focus of a concave mirror produces a virtual and enlarged image.
    [Note: This exercise helps you deduce algebraically properties of images that one obtains from explicit ray diagrams.]

    Solution
    From the mirror formula, for a concave mirror, f < 0 and for an object located between the pole and focus of a concave mirror, 
                               f<u<0 

                         1f>1u 
                      1f-1u>0
                   1v>0  or  v>0          1v = 1f-1u 
    i.e., a virtual image is formed on the right. 
     
    Also,                     1v<1u  or  v>u 

                              m = vu>1.

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    Question 18
    CBSEENPH12038189

    A small pin fixed on a table top is viewed from above from a distance of 50 cm. By what distance would the pin appear to be raised if it is viewed from the same point through a 15 cm thick glass slab held parallel to the table? Refractive index of glass = 1.5. Does the answer depend on the location of the slab?

    Solution
    Given, 
    Refractive index of glass = 1.5
    Real depth = 15 cm

    Image of pin appear through glass slab,
                         μ = real depthapparent depth 

    apparent depth = real depth (thickness of glass slab)μ
                           = 151.5 = 10 cm 

      Image is raised up by  = 15 - 10 = 5 cm. 

    Location of slab will not affect the answer is any way.
    Question 19
    CBSEENPH12038190

    Figure shows a cross-section of a ‘light pipe’ made of a glass fibre of refractive index 1.68.
    The outer covering of the pipe is made of a material of refractive index 1.44. What is the range of the angles of the incident rays with the axis of the pipe for which total reflection inside the pipe take place, as shown in the figure.
    (b) What is the answer if there is no outer covering of the pipe?


    Solution

    (a) Given, a cross-section of a light pipe. 

    Refractive index of glass-fibre, μ2 = 1.68Refractive index of outer covering   μ1 = 1.44 

     μ = μ2μ1 = isin ic

     Critical angle ic' is given by

    sin i'c = μ1μ2 = 1.441.68 = 0.8571
     i'c = 59° 

    Total internal reflection will occur if angle of incidence is greater than the critical angle, i’ > ic
    i.e., if i’ > 59° or,
    when r < r
    max, where r = 90°– 59° = 31°, which is the angle of reflection. 

    Now using Snell's law
     

                     sin imaxsin rmax = 1.68

                   sin imax = 1.68 × sin rmax 

                                  = 1.68 × sin 31°= 1.68 × 0.5150 = 0.8662

                        imax = 60°. 

    Therefore,  in the pipe the rays having incident angles in the range 0 < i < 60° with the axis of the pipe will suffer total internal reflection. 
    For the finite length of the pipe, the lower limit on i is determined by the ratio of the diameter to the length of the pipe. The lower limit of angle of incidence is not 0o

    (b) If there is no outer covering of the pipe then,

                         μ2 = 1.68 ,  μ1 = 1 
    Hence,
                sin i'c = μ1μ2 = 11.68 = 0.5952
                i'c = 36.5 ° 

    Now, for angle of incidence, i = 36.5° 

                  sin isin r =μ = 1.68 sin 90o1.68 = sin r11.68 = sin r  r = 36.5o 

    we have r = 36.5° and,
    i’ = 90° – 36.5° = 53.5°, which is greater than the critical angle, i
    c

    Thus all rays which are incident at angle in the range 0 < i < 90° will suffer total internal reflection.


    Question 20
    CBSEENPH12038191

    Answer the following questions:
    You have learnt that plane and convex mirrors produce virtual images of objects. Can they produce real images under some circumstances? Explain. 

    Solution
    Rays converging to a point ‘behind’ a plane or convex mirror are reflected to a point in front of the mirror on a screen. In other words, a plane or convex mirror can produce a real image if the object is virtual.
    Question 21
    CBSEENPH12038192

    Answer the following questions:
    A virtual image, we always say, cannot be caught on a screen. Yet when we ‘see’ a virtual image, we are obviously bringing it on to the ‘screen’ (i.e., the retina) of our eye. Is there a contradiction?

    Solution
    When the reflected or refracted rays are divergent, the image is virtual. The divergent rays can be converged on to a screen with the help of a suitable converging lens. The convex lens of the eye performs this function precisely. In this case, the virtual image being seen on the retina, serves as the virtual object for the lens to produce a real image.

    Note: Here the screen is not located at the position of the virtual image. 

    Question 22
    CBSEENPH12038193

    Answer the following questions:
    A diver under water, looks obliquely at a fisherman standing on the bank of a lake. Would the fisherman look taller or shorter to the diver than what he actually is?

    Solution
    The fisherman will look taller to the diver apparently. When the object is in rarer medium and the observer is in denser medium, then the “apparent depth” is greater than “real depth”. 
    Question 23
    CBSEENPH12038194

    Answer the following questions:
    Does the apparent depth of a tank of water change if viewed obliquely? If so, does the apparent depth increase or decrease?

    Solution
    The apparent depth of oblique viewing decreases from its real value for near-normal viewing.
    Question 24
    CBSEENPH12038195

    Answer the following questions:
    The refractive index of diamond is much greater than that of ordinary glass. Is this fact of some use to a diamond cutter?

    Solution
    Refractive index of diamond is nearly 2.42 which is much larger than that of ordinary glass (nearly 1.5). The critical angle for diamond is nearly 24° and, is less than the critical angle of glass. A skilled diamond cutter exploits the large range of angles of incidence in the diamond (24° to 90°), to ensure that light entering the diamond is totally reflected from many faces before getting out. This produces brilliant sparkling effect in the diamond.
    Question 25
    CBSEENPH12038196

    The image of a small electric bulb fixed on the wall of a room is to be obtained on the opposite wall 3 m away by means of a large convex lens. What is the maximum possible focal length of the lens required for the purpose?

    Solution
    For a real image to be obtained on the wall, minimum distance between the object and image should be 4f.
    That is, 
                              4f = 3 m
                            f = 34m = 0.75 m.
    is the maximum focal length of the lens required.
    Question 26
    CBSEENPH12038197

    A screen is placed 90 cm from an object. The image of the object on the screen is formed by a convex lens at two different locations separated by 20 cm. Determine the focal length of the lens. 

    Solution

    Here,
    Distance between object and screen, D = 90 cm
    Distance between two locations of convex lens, d = 20 cm
    Since,
    Focal length of the lens is, f =D2-d24D

                                         f = (90)2-(20)24 × 90  = (90+20) (90-20)360   = 110 × 736

                                        f = 21.4 cm. 

    Question 27
    CBSEENPH12038198

    Determine the ‘effective focal length’ of the combination of the two lenses having focal lenghs 30 cm and - 20 cm; if they are placed 8.0 cm apart with their principal axes coincident. Does the answer depend on which side of the combination a beam of parallel light is incident? Is the notion of effective focal length of this system useful at all?

    Solution
    Here,
    Focal length of first lens, f
    1 = 30 cm
    Focal length of second lens, f
    2 = –20 cm
    Distance between the lens, d = 8.0 cm 

    Let a parallel beam be incident on the convex lens first. If second lens were absent, then
              u1 =  and  f1 = 30 cm 

    In the formula, as      
                        1v1-1u1 =1f1 

                     1v1-1 = 130 

    i.e.,                    v1 = 30 cm 

    This image would now act as a virtual object for second lens. 

                u2 = +(30-8) = + 22 cm 

                     f2 = -20 cm
    Since,            
               1v2 = 1f2+1u2        1v2 = 1-20+122 

                  = -11+10220 =-1220 

              v2 = -220 cm. 

    ∴ Parallel incident beam would appear to diverge from a point 220 – 4 = 216 cm from the centre of the two lens system. 

    (ii) Assume that a parallel beam of light from the left is incident first on the concave lens.
     u1 = -,   f1 = -20 cm 

    As,         1v1-1u1 =1f1 

                      1v1 = 1f1+1u1         = 1-20+1-       =-120  
                           v1 = -20 cm 

    This image acts as a real object for the second lens
                                    u2 = -(20+8) = -28 cm  and,  f2 = 30 cm 

    Since,    1v2-1u2 = 1f2 

                      1v2 = 1f2+1u2         = 130-128        = 14-15420 

                            v2 = -420 cm

    ∴ The parallel beam appears to diverge from a point 420 – 4 = 416 cm, on the left of the centre of the two lens system. 

    We finally conclude that the answer depends on the side of the lens system where the parallel beam is incident. Therefore, the notion of effective focal length does not seem to be meaningful here.

    Question 28
    CBSEENPH12038199

    An object 1.5 cm in size is placed on the side of the convex lens in the arrangement (a) above. The distance between the object and the convex lens is 40 cm. Determine the magnification produced by the two-lens system, and the size of the image.

    Solution
    For convex lens, 

    Object distance from the lens, u = –40 cm
    Focal length, f = 30 cm
    Object size, O = 1.5 cm

    Using lens formula

                            1v-1u=1f

    We get,        1v-1-40=130 

                 1v=130-140=1120 

    i.e.,                            v =120 cm (for real object) 

    From relation,
    Magnification,        
                          m = -vu,  we getm = -120-40 = +3

    The image formed by the convex lens becomes object for concave lens at a distance of (120 – 8) = 112 cm on the other side. 

    For concave lens,  

    Focal length, f = – 20 cm
    Object distance, u = + 112 cm (on the other side)
    Image distance, v = ? 

    Using lens formula, we get 

                      1v-1u = 1f 

    Now,       1v-1112=1-20

                   1v=-120+1112     =-23560

                         v = -56023 cm (for virtual object)

    Using the formula of magnification  m = vu,  we get
                         m = -560/23-112    =-56023×1112    =-523 

    Net magnification, 

    m= 3 × -523    =-1523    = 0.652  (negative due to virtual image) 

    and as,
                            m =I0
                              I = m × 0   = 0.652 ×  1.5    = 0.98 cm (size of final image).

    Question 29
    CBSEENPH12038200

    At what angle should a ray of light be incident on the face of a prism of refracting angle 60° so that it just suffers total internal reflection at the other face? The refractive index of the material of the prism is 1.524.

    Solution

    The refracted ray in the prism is incident on the second face at critical angle ic. 

    Given, angle of prism, A = 60o
    Refracting index of the material = 1.524 

    Now, 60° + 90° – r + 90° – ic = 180° [ sum of all angles of  is 1800

    and,

                         r1+r2 = A

                      r = 60° - ic 

    Now,         sin ic = 1μ = 11.524
                     ic = sin-111.524
                      ic  41° 

                       r = 60° -41° = 19° 

    Using Snell's law,

                   sin i = sin 19° × 1.524         = 0.4962      i = sin-1(0.4962)        = 29.75°.



     
    Question 30
    CBSEENPH12038201

    You are given prisms made of crown glass and flint glass with a wide variety of angles. Suggest a combination of prisms which will
    (i)    deviate a pencil of white light without much dispersion.
    (ii)   disperse (and displace) a pencil of white light without much deviation.

    Solution
    (i) Angular dispersion produced by two prisms should be zero so that, no dispersion take place. 

    The sum of angular dispersion by crown glass prism and angular dispersion by flint glass prism is equal to zero.
    i.e.,         (μb – μr)A + (μb’ – μr’)A’ = 0. 

    Since (μb’ – μr’) for flint glass is more than that for crown glass, therefore, 
                                     A'< A 

    Hence, the combination of prism is such that the, flint glass prism of smaller angle has to be suitably combined with crown glass prism of larger angle. 

    (ii) For almost no deviation,
                   (μy – 1) A’ + (μy’ – 1)A’ = 0 

    To disperse without deviation, we need flint glass prism of greater so that the deviation due to two prisms are equal and opposite. In the final combination however, angle of flint glass prism will be smaller than the angle of crown glass prism because the refractive index is more for flint glass as compared to the refractive index of crown glass.
    Question 31
    CBSEENPH12038202

    For a normal eye, the far point is at infinity and the near point of distinct vision is about 25 cm in front of the eye. The cornea of the eye provides a converging power of about 40 dioptres, and the least converging power of the eye-lens behind the cornea is about 20 dioptres. From this rough data estimate the range of accommodation (i.e., the range of converging power of the eye-lens) of a normal eye.

    Solution

    For a normal eye, near point of distinct vision = 25 cm.
    i.e.,                u = –25 cm
    Converging power = +40 D 

    To see objects at infinity, the eye uses its least converging power = 40 + 20 = 60 dioptres. This gives the rough idea of the distance between the retina and cornea eye-lens. 
     to focus an object at near point,
    Focal length of eye-lens = 100P=106=53cm
                                  v = -53cm 

    Now, using the formula, 
                              1f =1v-1u 

                                   = 35+125= 1625 

    i.e., f = 2516, corresponding to a converging power given by, 

                     P = 1002516 = 64 dioptre. 

     the power of the eye lens = 64 - 60 = 24 dioptre.

    Hence, we can say that the range of accommodation of the eye-lens is roughly 20 to 24 dioptre.

    Question 32
    CBSEENPH12038203

    Does short-sightedness (myopia) or longsightedness (hypermetropia) imply necessarily that the eye has partially lost its ability of accommodation? If not, what might cause these defects of vision?

    Solution

    No, a person may have normal ability of accommodation yet, he may be myopic or hypermetropic. 
    In fact, myopia arises when length of eye ball (from front to back) gets elongated and hypermetropia arises when length of eye ball gets shortened.
    However, when eye ball has normal length, but the eye-lens losses partially its power of accommodation, this defect is called presbiopia.

    Question 33
    CBSEENPH12038204

    A myopic person has been using spectacles of power —1.0 dioptre for distant vision. During old age, he also needs to use separate reading glass of power +2.0 dioptres. Explain what may have happened.

    Solution

    Power of spectacles, P = -1D
     Focal length, f = -100 cm
    That is, the far point of the person is at 100 cm.
    Near point of the eye might have been normal (i.e., 25 cm).

    The objects at infinity produce virtual images at 100 cm (using spectacles).
    To see objects between 25 cm to 100 cm, the person uses the ability of accommodation of his eye-lens. This ability is partially lost in old age.
    The near point of the eye may recede to 50 cm. He has, therefore, to use glasses of suitable power for reading.

    Here,
    Object distance, u = –25 cm
    Image distance, v = –50 cm

    Since,          1v-1u = 1f = -150+125

    i.e.,    focal length, f = 50 cm 

    Power,    P = 100f = 10050 = +2 dioptre.

    Question 34
    CBSEENPH12038205

    A person looking at a person wearing a shirt with a pattern comprising vertical and horizontal lines is able to see the vertical lines more distinctly than the horizontal ones. What is this defect due to? How is such a defect of vision corrected?

    Solution

    The defect is called Astigmatism. When the curvature of the cornea plus eye-lens refracting system is not the same in different planes, this defect arises. As vertical lines are seen distinctly, the curvature in the vertical plane is enough, but the curvature of the lens system is insufficient in the horizontal plane and, the lines cannot be seen distinctly. 

    This defect is removed by using a cylindrical lens with its axis along the vertical plane.

     

    Question 35
    CBSEENPH12038206

    A man with normal near point (25 cm) reads a book with small print using a magnifying glass a thin convex lens of focal length 5 cm.
    What is the closest and farthest distance at which he should keep the lens from the page so that he can read the book, when viewing through the magnifying glass?

    Solution

    For the closest distance,

    Image distance, v = -25 cm
    Focal length of thin convex lens, f = 5 cm  

    Using the formula,
                    1v-1u=1f 

                1u = 1v-1f

                        = 1-25-15 =-1-525=-625 

                     u =-256 = -4.2 cm 

    i.e., 4.2 cm is the closest distance at which the man can read the book. 

    For the farthest image, 

    Image distance, v = Focal length, f = 5 cm  

    Using the formula, 
                       1v-1u = 1f 

                       1u = 1v-1f 

                           = 1-15=-15 

                        u = -5 cm 
    which is the object distance.

    This is the farthest distance at which the man can read the book.

    Question 36
    CBSEENPH12038207

    A man with normal near point (25 cm) reads a book with small print using a magnifying glass a thin convex lens of focal length 5 cm.
    What is the maximum and the minimum angular magnification (magnifying power) possible using the above simple microscope?

    Solution

    Normal near point of human eye = 25 cm 
    Focal length , f = 5 cm 

    Maximum angular magnification is 

                           DUmin = 2525/6 = 6 

    Minimum angular magnification is 

                           DUmax = 255 = 5.

    Question 37
    CBSEENPH12038208

    A card sheet divided into squares each of size 1 mm2 is being viewed at a distance of 9 cm through a magnifying glass (a converging lens of focal length 10 cm) held close to the eye. What is the magnification produced by the lens? How much is the area of each square in the virtual image?

    Solution
    Given,
    Object distance, u = –9 cm
    Focal length of converging lens, f = 10 cm 

    Now, Using the formula, 

                       1v-1u = 1f 

                   1v = 1f+1u  

                   1v =110+1-9        = -9+10-90       =-190 

    i.e.,                 v = -90 cm 

    Magnification, m= vu=-90-9 = 10 

    Therefore, 

    Area of the each square in the virtual image=(10 x 10 x 1) mm
    2 100 mm2 = 1 cm2
    Question 38
    CBSEENPH12038209
    Question 39
    CBSEENPH12038210

    A card sheet divided into squares each of size 1 mm2 is being viewed at a distance of 9 cm through a magnifying glass (a converging lens of focl length 10 cm) held close to the eye. 
    Is the magnification equal to the magnifying power in this case? Explain.

    Solution
    No. Magnification of an image by a lens and angular magnification (or magnifying power) of an optical instrument are different from each other.

    Angular magnification is the ratio of the angular size of the image (even if the image is magnified) to the angular size of the object if placed at the near point (25 cm).
    Thus, magnification magnitude = vu and,
    Magnifying power is 25u = Du. 

    Only when the image is located at the least distance of distinct vision, we can have both the quantities equal. 
     

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    Question 40
    CBSEENPH12038211

    At what distance should the lens be held from the figure in Question 9.29 in order to view the squares distinctly with the maximum possible magnifying power?

    Solution
    Maximum magnifying power is obtained when the image is at the near point (25 cm).

    Thus,
    Image distance, v = -25 cm
    Focal length, f = + 10 cm
    Object distance, u = ? 

    Using the formula , 

             1v-1u = 1f 

          1u = 1v-1f 
                  = 1-25-110 =-2-550=-750

    i.e.,      u = -507 = -7.14 cm. 

    So the lens should be held at a distance of 7.14 cm away so as to have a maximum possible magnifying power.
    Question 41
    CBSEENPH12038212

    What is the magnification in this case?

    Solution
    We have,
    Least distance of distinct vision, v = 25 cm
    Object distance, u = 7.14 cm 

    Therefore, 

    Magnitude of magnification, m =vu                                                        =257.14                                                        = 3.5
    Question 42
    CBSEENPH12038213

    Is the magnification equal to the magnifying power in this case? Explain.

    Solution
    Near point, D = 25 cm 
    Distance where the object is kept, u = 7.14 cm

    Magnifying power of the lens, M = D/u 

                                                     = 257.14    = 3.5  

    Here, in this case since the image is formed at the least distance of distinct vision, the magnifying power is equal to the magnitude of magnification.

    Question 43
    CBSEENPH12038214

    What should be the distance between the object (in Question 9.30) and the magnifying glass if the virtual image of each square in the figure is to have an area of 6.25 mm2. Would you be able to see the squares distinctly with your eyes very close to the magnifier?

    Solution
    Here,
    Magnification in area = 6.25
    ∴ Linear magnification,
                                        m = vuv = mu   = 2.5 u
    Using formula,
                            1v-1u = 1f

                   12.5 u-1u = 110

                           1-2.52.5 u = 110

                                2.5 u = -15 

    i.e.,                             u = -6 cm 

                                   v = 2.5 u    = 2.5 (-6)    = -15 cm 

    The virtual image is at 15 cm; whereas distance of distinct vision is 25 cm, therefore, the image cannot be seen distinctly by the eye.
    Question 44
    CBSEENPH12038215

    Answer the following questions:
    The angle subtended at the eye by an object is equal to the angle subtended at the eye by the virtual image produced by a magnifying glass. In what sense then does a magnifying glass provide angular magnification?

    Solution
    Even though the absolute image size is bigger than object size, the angular size of the image is equal to the angular size of the object. When magnifier is not used, the object would be placed no closer than 25 cm; and when magnifier is used, the object can be placed much closer. The closer object has larger angular size than the same object at 25 cm. It is in this sense that angular magnification is achieved.
    Question 45
    CBSEENPH12038216

    Answer the following questions:
    In viewing through a magnifying glass, one usually positions one's eyes very close to the lens. Does angular magnification change if the eye is moved back?

    Solution
    The angular magnification decreases in a slight manner when we move our eyes back because, then the angle subtended at the eye by the image will be faintly less than the angle subtended by the image at the lens. Also, angle subtended by the object at the eye is also less than the angle subtended by the object at the lens. However, this decrease is very minute as compared to the case of image. 

    Also, when the eye is separated from the lens, the angles subtended at the eye by the object and its image are not equal.
    Further it may be noted that if the image is away at a very large distance and, we move our eyes back from the lens, then, the effect on magnification is negligible. 

    Question 46
    CBSEENPH12038217

    Answer the following questions:
    Magnifying power of a simple microscope is inversely proportional to the focal length of the lens. What then stops us from using a convex lens of smaller and smaller focal length and achieving greater and greater magnifying power?

    Solution
    First, grinding lenses of very small focal lengths is not easy. Secondly and more importantly, if the focal length of the lens is decreased, the spherical and chromatic abberation becomes more pronounced. Hence, practically we cannot achieve a magnifying power greater than 3 in a simple convex lens. 
    However, if an aberration-corrected lens system is implemented, one can increase the magnifying power by a factor of approximately 10. 
    Question 47
    CBSEENPH12038218

    Answer the following questions:
    Why must both the objective and eyepiece of a compound microscope have short focal lengths?

    Solution
    Angular magnification of eyepiece = 25fe (cm)+1.  

    Thus, angular magnification increases if fe is smaller.

    Magnification of the objective = v0u0 = 1u0f-1 
    Magnification is large when u0 is slightly greater than f(focal length of the objective)
    As the object lies close to the focus of objective lens, u = fo. And, to increse this magnification (v/fo ), fo should be small.

    Question 48
    CBSEENPH12038219

    Answer the following questions:
    When viewing through a compound microscope, our eyes should be positioned not on the eyepiece but a short distance away from it for best viewing. Why? How much should be that short distance between the eye and eyepiece?

    Solution
    When viewing through a compound microscope, our eyes should be positioned at a short distance away from the eyepiece. The image of the objective lens in the eyepiece is known as the ‘eye-ring’. All the rays (from object), refracted by the objective go through the eye-ring. Therefore, it is an ideal position of our eyes for viewing.

    If we position our eyes too close to the eyepiece, the path of light rays would be obstructed and this reduce our field of view. If we position our eyes on the eye-ring and if, the area of the pupil of our eye is greater or equal to the area of the eye-ring, our eyes will collect all the light refracted by the objective lens. 

    The precise location of the eye-ring naturally depends on the separation between the objective and the eyepiece and the focal length of the eyepiece. When, we view through a microscope by placing our eyes on one end, the ideal distance between the eye and the eyepiece is usually built in the design of the instrument.
    Question 49
    CBSEENPH12038220

    A small telescope has an objective lens of focal length 140 cm and an eyepiece of focal length 5.0 cm. What is the magnifying power of the telescope for viewing distant objects when the telescope is in normal adjustment (i.e., when the final image is at infinity)?

    Solution
    Given, the telescope is in normal adjustment. 
    Focal length of the objective lens, f
    0 = 140 cm
    Focal length of the eyepiece,  f
    e = 5 cm

    Therefore,
    Magnifying power, m= f0fe=-1405 = -28 

    Question 50
    CBSEENPH12038221

    A small telescope has an objective lens of focal length 140 cm and an eyepiece of focal length 5.0 cm. What is the magnifying power of the telescope for viewing distant objects when the final image is formed at the least distance of distinct vision (25 cm)?

    Solution
    Given,
    Focal length of objective lens, f
    0 = 140 cm
    Focal length of eyepiece, f
    e = 5 cm

    Magnifying power when the final image is formed at least distance of distinct vision, m =-f0fe1+feD 

                                     m = -14051+525 -33.6.

    Question 51
    CBSEENPH12038222

    For the telescope describe in Question 9.34 (a), what is the separation between the objective lens and the eyepiece?

    Solution
    In normal adjustment, separation between objective and eye-lens is,  

                         L = f0+fe    = 140 + 5    = 145 cm.
    Question 52
    CBSEENPH12038223

    If the telescope (described in ques. 34) is used to view a 100 m tall tower 3 km away, what is the height of the image of the tower formed by the objective lens?

    Solution
    Height of the building = 100 m
    Distance between the building and telescope = 3000 m 

     Angle subtended by 100 m tall tower at 3 km,

                   θ = 1003 × 1000 = 130 radian 

    Let, y be the height of the image formed by the objective,
    then,             θ =yfo= y140 

                         130 = y140  

    i.e.,                        y = 4.7 cm.
     
    Question 53
    CBSEENPH12038224

    What is the height of the final image of the tower if it is formed at 25 cm?

    Solution
    Given, 
    Focal length of the eye-piece, fe = 5 cm 
    Magnification produced by eyepiece, m
                                                             = 1+Dfe =1+255 = 6
                               
     Height of final image  = 4.7 × 6 = 28.2 cm.
    Question 54
    CBSEENPH12038225

    A Cassegrain telescope uses two mirrors as shown in figure below. Such a telescope is built with the mirrors 20 mm apart. If the radius of curvature of the large mirror is 220 mm and the small mirror is 140 mm, where will the final image of an object at infinity be?

    Fig. Schematic diagram of a reflecting telescope (Cassegrain)

    Solution
    Here given,
    Radius of curvature of objective mirror,R1 = 220 mm
    Radius of curvature of secondary mirror, R= 140 mm
    Distance between the two mirror, d = 20 mm 
    We can calculate the focal length of both mirrors.
     Focal length of objective mirror, f1R12=2202=110 mm
    Focal length of secondary mirror,  f2 =R22 =1402 = 70 mm

    When object is at infinity, parallel rays falling on objective mirror, on reflection, would collect at its focus at f1
    In turn, they fall on secondary mirror which is at a distance of 20 mm from objective mirror. 

    For secondary mirror,
    Object distance, u = f
    1 – d = 110 – 20 = 90 mm 

    Now, using formula,   1v+1u =1f2

                                     1v = 1f2-1u      = 170-190      =9-7630      =2630 

                                       v = 6302   = 315 mm = 31.5 cm 
    to the right of secondary mirror.

    Question 55
    CBSEENPH12038226

    Light incident normally on a plane mirror attached to a galvanometer coil retraces backwards as shown in figure A current in the coil produces a deflection of 3.5° of the mirror. What is the displacement of the reflected spot of light on a screen placed 1.5 m away?

    Solution
    We know that if the mirror is turned by an angle θ, the reflected ray turns by an angle 2θ.

    The current in the coil has produced a deflection of 3.5° in the mirror, therefore, the reflected ray will be deflected by an angle 2 x 3.5° = 7°. 

    From the figure,  we have
    d1.5 = tan 7°              tan θ = perpendicularbase

     d = 1.5 tan 7°         = 1.5 × 0.123          = 0.184 m         = 18.4 cm.
    Question 56
    CBSEENPH12038227

    The following figure shows an equiconvex lens (of refractive index 1.50) in contact with a liquid layer on top of a plane mirror. A small needle with its tip on the principal axis is moved along the axis until its inverted image is found at the position of the needle. The distance of the needle from the lens is measured to be 45.0 cm. The liquid is removed and the experiment is repeated. The new distance is measured to be 30.0 cm. What is the refractive index of the liquid?


    Solution
    Suppose,
    Focal length of convex lens of glass = f
    1 = 30 cm

    Focal length of plane concave lens of liquid be = f
    2  
    and, 

    Combined focal length, F = 45.0 cm 

    As,               1f1+1f2 =1F 

                   1f2 = 1F-1f1       = 145-130      =-190
                        f2 = -90 cm 

    For glass lens, let R1 = R,  R2 = -R 

    Using lens maker's formula,
                    1f1 = (μ -1)1R1-1R2
    we have, 

               130 = 32-1 1R+1R 

                         = 12×2R =1R 

    Thus,          R = 30 cm 

    For liquid lens, 
                           R1 = -R = -30.0 cmR2 = 1f2 = (μl-1) 1R1-1R2        = (μl-1) 1-30-1 

                   1-90 = (μl-1) × 1-30

                 (μl-1) = 3090 = 13 

                            μl =1+13= 43. 

    which is the refractive index of the liquid.
                            
    Question 57
    CBSEENPH12038228

    Two thin lenses of power +4D and -2D are in contact. What is the focal length of the combination?

    Solution
    Power of first lens = +4 D
    Power of second lens = -2 D
    Power of the combination of lens,
    P = P1+P2      = 4 - 2     = + 2D
    Since focal length, f = 1P
    Focal length of the lens,
     f = 12 = 0.5 m               = 50 cm
    Question 58
    CBSEENPH12038229

    Here three lenses have been given. Which two lenses will you use as an eyepiece and as an objective to construct an astronomical telescope? 

    Lenses

    Power (P)

    Aperture (A)

    L1

    3D

    8 cm

    L2

    6D

    1 cm

    L3

    10D

    1 cm

     

    Solution
    For an astronomical telescope, since the aperture of lens L1 is largest, it is used as objective for a telescope. The focal length of lens L3 is smaller and hence cn be used as eyepiece.
    Question 59
    CBSEENPH12038230

    What are the laws of reflection?

    Solution

    Laws of reflection: 

    (i) The incident ray, the reflected ray and the normal all three lie in the same plane.
    (ii) The angle of incidence (i) is equal to the angle of reflection (r).
    i.e.,                        ∠i = ∠r.

    Question 60
    CBSEENPH12038231

    What is presbyopia? How can it be corrected? 

    Solution

    Presbyopia is a progressive form of far-sightedness that affects most people with ageing. The power of accomodation of the eye decreases. 
    Presbyopia arises due to the gradual weakening of the ciliary muscles and diminishing flexibility of the crystalline lens. 
    Simple reading eyeglasses with convex lenses correct most cases of presbyopia.

    Question 61
    CBSEENPH12038232

    A glass lens of refractive index 1.5 is placed in a trough of liquid. What must be the refractive index of the liquid in order to make the lens disappear?

    Solution
    The refractive index of liquid must be greater than or equal to 1.5 inorder to make the lens disappear. 
    Question 62
    CBSEENPH12038233

    A converging lens of refractive index 1.5 is kept in a liquid medium having same refractive index. What would be the focal length of the lens in this medium?

    Solution
    Refractive index of the lens = 1.5 = Refractive index of medium.

    The lens in the liquid will act like a plane sheet of glass. 

    ∴ Its focal length will be infinite (∞) 

    By using the formula of lens maker, 

                
    1f = (μ-1) 1R1-1R2 

               1f =μ2μ1-1 1R1-1R2 

                         μ1 = μ2  

                     1f = 0 
    Thus,               f = . 
    Question 63
    CBSEENPH12038234

    How does the power of a convex lens vary, if the incident red light replaced by violet light?

    Solution
    Using lens maker's formula
                     1f = (μ-1) 1R1-1R2 

      Power of lens,
                    P = 1f      = (μ-1) 1R1-1R2
    Refractive index of violet light is greater than refractive index of red light.
    Therefore, power of the lens will be increased when red light is replaced by violet light.
    Question 64
    CBSEENPH12038235

    How does the angle of minimum deviation of a glass prism vary, if the incident violet light is replaced with red light? 

    Solution
    Wavelength of red light is greater than that of violet light. And, refractive index of any light is inversely proportional to the wavelength. Therefore, refractive index of red light is less. In turn, angle of minimum deviation has a linear dependance with refractive index. 

                                δ = (μ-1) A 

    Thus, when violet light is replaced with red light, angle of minimu deviation decreases. 

    Question 65
    CBSEENPH12038236

    How does the angle of minimum deviation of a glass prism of refractive index 1.5 change, if it is immersed in a liquid of refractive index 1.3?

    Solution
    Given,
    Refractive index of glass w.r.to air, 
    aμg = 1.5
    Refractive index of water w.r.to air, 
    aμ= 1.3 

    As, δ = (μ-1)A 

    For deviation in air, μ = μgμa= 1.51 = 1.50 

     Angle of deviation, δ = (1.15 - 1) × 60° = 30°

    For deviation in water, μ = μgμw = 1.51.3 = 1.15  

     Angle of deviation, δ = (1.15-1) × 60° = 9°

    Therefore, the angle of deviation of glass prism is decreased when it is immersed in aliquid of refractive index of 1.3.
    Question 66
    CBSEENPH12038237

    Write the necessary conditions, for the phenomenon of total internal reflection to take place.

    Solution
    Necessary conditions for the total internal reflection are:
    (i) Light must travel from denser medium to rarer medium.
    (ii) The angle of incidence (in the denser medium) must be greater than the critical angle ic where sin ic = 1μ.
    Question 67
    CBSEENPH12038238

    An object is placed at the focus of concave lens. Where will its image be formed?

    Solution
    When the object is placed at focus of the concave lens, image is formed at infinity.
    Question 68
    CBSEENPH12038239

    A lens of glass is immersed in water. What will be its effect on the power of the lens?

    Solution
    When a lens of glass is immersed in water, refractive index increases and hence, power increases.
    Question 69
    CBSEENPH12038240

    Why is convex mirror used as driver's mirror?   

    Solution
    The image formed in a convex mirror is virtual, erect and is within the focal length of the mirror (nearby). Added to that, the field of view of a convex mirror is large and hence, is used as a rear view mirror in vehicles.
    Question 70
    CBSEENPH12038241

    A ray of light falls on a mirror normally. What are the values of angle of incidence and the angle of reflection.

    Solution
    When a ray of light falls on a mirror normally, both angle of incidence and the angle of reflection is zero.
    Question 71
    CBSEENPH12038242

    What is the number of images of an object held between two parallel plane mirrors?

    Solution

    Given, θ = 0°
     Number of images, n = 360°θ-1  

                                        = 360°0°-1= infinite. 

    Question 72
    CBSEENPH12038243

    What is the length of a telescope in a normal adjustment?

    Solution
    Length of a telescope is given by the sum of the focal length of the objective and the eyepiece.

                                    L = f0+fe
    where, 
    fo is the focal length of the objective and, 
    fe is the focal length of the eyepiece.
    Question 73
    CBSEENPH12038244

    If a telescope is inverted, will it be able to work as a microscope?

    Solution
    An inverted telescope will not work as a microscope. 
    Question 74
    CBSEENPH12038245

    What is the magnification produced by a single convex lens used as a simple microscope in normal use?

    Solution
    The magnification produced by a single convex lens is,
                            M = 1+Df. 
    where,
    M is the mgnification,
    f is the focal length.
    Question 75
    CBSEENPH12038246

    Which of the two main parts of an optical fibre has a higher value of refractive index?

     

    Solution
    The two main parts of the optical fibre are:
    i) core and,
    ii) cladding. 
    The refractive index of core is greater than that of cladding. 
    Question 76
    CBSEENPH12038247

    A lens when immersed in a transparent liquid becomes invisible. Under what condition does it happens?

    Solution

    A lens which is immersed in a transparent liquid becomes invisible when, refractive index of liquid is equal to or greater than the refractive index of glass.

    Question 77
    CBSEENPH12038248

    What is the physical principle on which the working of optical fibre is based?

    Solution
    The principle on which the optical fibre works is total internal reflection.
    Question 78
    CBSEENPH12038249

    Write the relation for the the refractive index μ of the prism in terms of the angle of minimum deviation δm and the angle A of prism.

    Solution
    The required relation is, 
                         μ = sinA+δm2sin A/2. 
    where,
    μ is the refractive index, 
    A is the angle of prism and, 
    δm is the minimum angle of deviation.
    Question 79
    CBSEENPH12038250

    Sponsor Area

    Question 80
    CBSEENPH12038251

    In a simple microscope, why the focal length of the lens should be small?

    Solution
    Focal length is inversely proprtional to the angular magnification and therefore the focal length of lens should be small for a microscope. 
    Question 81
    CBSEENPH12038252

    Define refractive index of a transparent medium. A ray of light passes through a triangular prism. Plot a graph showing the variation of the angle of deviation with the angle of incidence.

    Solution

    Ratio of the speed of light in air (vacuum) to the speed of light in the medium is called the refractive index of the medium. 

    Graph: The graph of angle of deviation (δ) versus angle of incidence (i) for a triangular prism is given as follow:

    Question 82
    CBSEENPH12038253

    Draw a labelled ray diagram of a reflecting type telescope. Write its any one advantage over refracting type telescope.

    Solution
    The ray diagram of a reflecting type telescope is shown below: 

     

    Since a reflecting telescope has mirror objective, the image formed is free from chromatic aberration.

    Question 83
    CBSEENPH12038254

    A convex lens of refractive index 1.5 has a focal length of 18 cm in air. Calculate the change in its focal length when it is immersed in water of refractive index 4/3. 

    Solution

    Given, a convex lens.
    Refractive index of lens, μga  = 1.5 
    Focal length of lens in air, fa = 18 
    Refractive index of water, μwa = 43

    For the lens in air,
                   1fa = (μga-1) 1R1-1R2 

                  118= (1.5 - 1) 1R1-1R2 

                   1R1-1R2= 14 

    When the lens is immersed in water
                   1fw = μgaμwa-1 1R1-1R2 

                        = 1.54/3-1 × 14= 18× 14 = 132 

    Thus,        fw = 32 cm.  

    Hence, focal length changes from 18 to 32.

    Question 84
    CBSEENPH12038255

    A convex mirror always produces a virtual image independent of the location of the object. Use mirror equation to prove it.

    Solution
    Using mirror formula, 

                          1v+1u =1f 

                      1v = 1f-1u 

    Object distance u is negative and the focal length f is positivefor convex mirror. 

    Therefore,
    1v = 1+f-1-u=1f+1u 
    which, is a positive quantity. 

    This implies, the image distance is always positive in case of convex mirror and the image is always formed on the other side of the object i.e., behind the convex mirror. Hence, the convex mirror always form a virtual image.
    Question 85
    CBSEENPH12038256

    Draw a ray diagram of a compound microscope. Write the expression for its magnifying power.

    Solution
    Ray diagram of a compound microscope.

    When the final image is formed at the least distance of distinct vision, 
    magnifying power is, 

                       m = -v0u01+Dfe 

    For the image to be formed at infinity, ue = fe

    and              m = -v0u0.Dfe 

    By making focal length of the objective lens small, the magnifying power can be increased.
    Question 86
    CBSEENPH12038257

    Draw a ray diagram of an astronomical telescope in the near point adjustment. Write down expression for its magnifying power.

    Solution

    The figure below shows the ray diagram of an astronomical telescope in the near point adjustment. 



    Magnifying power is given as,
                          m = F0Fe1+FeD

    Question 87
    CBSEENPH12038258

    An object 0.5 cm high is placed 30 cm from a convex mirror whose focal length is 20 cm. Find the position, size and nature of the image.

    Solution

    We have,
    Distance of object from the mirror, u = –30 cm;
    Distance of image, v = ?
    Focal length, f = + 20 cm 

    We know, using the mirror formula,
                         1v+1u =1f

                        v =ufu-f    =(-30) (+20)-30-20      = + 12 cm 

    The image is virtual and erect as, it is formed at a distance of 12 cm behind the mirror. 

    Now, size if the object, O = 0.5 cm 
    sixe of the image = I
    Magnification,  m = IO = -vu=-12-30
                                 I = 25×O   = 25× 0.5  = +0.2 cm 

    Hence, the height of the image = + 0.2 cm.
    The positive sign indicates that the image is erect is smaller in size

    Question 88
    CBSEENPH12038259

    An object 0.2 cm high is placed 15 cm from a concave mirror length 5 cm. Find the position and size of the image.

    Solution

    We have, 

    object distance, u = -15 cmFocal length, f = -5 cmImage distance, v = ? 

    Using formula, 

      1v+1u = 1f            

    v = ufu-f        =(-15) (-5)-15+5        = -7.5 cm

    The image is formed at a distance of 7.5 cm in front of mirror. 
    Now,
    Magnification, m = IO = -vu

    where,
    I is the image size and, 

    O is the object size. 

                 IO=-(-7.5)(-15)         I =-0.1 cm 

    The negative sign indicates that the image is inverted and is diminished in size.

    Question 89
    CBSEENPH12038260

    A fish rising vertically to the surface of water in a lake uniformly at the rate of 3 m/s observes a king fisher bird diving vertically towards water at the rate 9 m/s vertically above it. If the refractive index of water is 4/3, find the actual velocity of the dive of the bird.

    Solution
    Given,
    Rate at which the fist is rising = 3 m/s
    Rate at which the king fisher is diving = 9 m/s 
    Refractive index of water = 4/3 

    If at any instant, the fish is at a depth ‘x’ below water surface while, the bird is at a height 'y' above the surface, then the apparent height of the bird from the surface as seen by the fish will be given by
                     μ = Apparent heightReal height

    or,             Apparent height = μy 

    So, the total apparent distance of the bird as seen by the fish in water will be h = x + μy 
    Now, differentiating w.r.t time, we get 

                          dhdt=dxdt+μdydt 

                         9 = 3+μdydt 

                     dydt = 6(4/3) = 4.5 m/s.

    Thus, the kingfisher bird is diving with a velocity of 4.5 m/s. 
    Question 90
    CBSEENPH12038261

    A compound microscope with an objective of 1.0 cm focal length and an eyepiece of 2.0 cm focal length has a tube length of 20 cm. Calculate the magnifying power of microscope, if the final image is formed at the near point of the eye.

    Solution
    Here we are given a compound microscope.
    Length of the tube, l = 20 cm
    Near point, D = 25 cm
    Focal length of objective, f
    0 = 1 cm and,
    Focal length of eye-piece, f
    e = 2 

    Magnifying powe of objective, m0 = lf0 = 201 = 20

    Magnifying power of eyepiece, me = Df0 = 252
    Therefore, magnifying power of microscope,m = m0me = 20 × 252 = 250.

    Question 91
    CBSEENPH12038262

    A ray of light incident at 49° on the face of an equilateral prism passes symmetrically. Calculate the refractive index of the material of the prism.

    Solution
    The prism given is an equilateral prism.
    Angle of prism, A = 60°.
    Angle of incidence, i = 49o 

    Since the ray of light passes symmetrically, the prism is in the position of minimum deviation.
    This implies,
    Angle of reflection,  r =A/2 = 60°2 = 30° 

     Refractive index, μ = sin isin r  

                                     = sin 49°sin 30° = 0.75470.5

    i.e.,                         μ = 1.5. 
    Question 92
    CBSEENPH12038263

    The magnifying power of an astronomical telescope in the normal adjustment position is 100. The distance between the objective and the eyepiece is 101 cm. Calculate the focal lengths of the objective and of the eyepiece. 

    Solution

    Here we are given an astronomical telescope.
    Distance between objective and eyepiece, l = 101 cm

    Magnification, m = f0fe = 100

                      f0 = 100 fe

    Since,        f0+fe = 101

    Then,   100fe+fe = 101

                        fe = 1 cm  and, f0 = 100 cm.

    Question 93
    CBSEENPH12038264

    A prism of refractive index of √2 has a refracting angle of 60°. At what angle must a ray be incident on it so that it suffers a minimum deviation?

    Solution
    Given,
    Refractive index of prism = 2 
    angle of prism = 600 

    For minimum deviation, i = e. 

    Therefore,        A+δm = i + r 

                        i = A+δm2  for δ minimum  i = r 

    Now,       μ = sin A+δm2sin A/2 = sin isin A/2

    i.e.              sin i = μ sin A/2 
     
                  sin i = μ sin 60°2         = 2  sin  30°         = 12
    Hence,             i = 45°.

    When, angle of incidence is 45o the ray suffers minimum deviation.
     
    Question 95
    CBSEENPH12038266

    The refracting angle of the prism is 60° and the refractive index of the material of the prism is 1.632. Calculate the angle of minimum deviation.

    Solution
    Given,
    Angle of prism, A = 60°
    Refractive index, μ = 1.632 

    Now, using the formula, 

                   μ = sin A+δm2sin A2 

            1.632 = sin 60°+δm2sin 60°2              = sin 60+δm2sin 30°
     sin 60°+δm2 = 1.632 sin 30° = 1.632 × .5

          sin 60°+δm2 = 0.816           60°+δm2 = 54°42'                        δm = 49°24'.
    is the required angle of minimum deviation.
    Question 96
    CBSEENPH12038267

    A vessel 20 cm deep is half-filled with oil of refractive index 1.37 and the other half is filled with water of refractive index 1.33. Find the apparent depth of the vessel when viewed from above.

    Solution
    The formula for apparent depth of the vessel is,
     
                   AD = t1μ1+t2μ2        = t21μ1+1μ2        = t (μ1+μ2)2μ2μ2 

    where, 

    Depth of the vessel, t = 20 cm,
    Refractive index of oil, μ
    1 = 1.37 and
    Refractive index of water, μ
    2 = 1.33

    Substituting for t, μ
    1 and μ2, we get
    Apparent depth, AD = 15.37 cm.


    Question 97
    CBSEENPH12038268

    Show that the least possible distance between an object and its real image in a convex lens is 4f where f is the focal length of the lens.

    Solution

    To prove: Least possible distance between an object and real image = 4f 

    Suppose, I is the real image of an object O.
    Let, d be the distance between the image and the object.
    If the image distance from the lens is x, the object distance from the lens will be (d – x).

    Thus, u = – (d – x) and v = + x.

    Sustituting in the lens formula 

                   1v - 1u = 1f
    we have,
                  1x-1-(d-x) =1f 

                 1x+1(d-x)= 1f 

                  x2-xd-fd =0

    For a real image, the value of x must be real,
    i.e., the roots of the above equation must be real. This is possible if,
                     d2 ≥ 4fd
    i.e.,             d ≥ 4f 

    Hence, 4f is the minimum distance between the object and its real image formed by a convex lens.

    Question 98
    CBSEENPH12038269

    What is the relation between critical angle and refractive index of a material?

    Solution
    The relation between critical angle and the refractive index of a material is, 

                      μ = sin i
    c or n21 = sin i

    where,
    n
    21 is the refractive index of rarer medium 1 with respect to denser medium 2 and,
    ic is the critical angle.
    Question 99
    CBSEENPH12038270

    Does critical angle depend on the colour of light? Explain.  

    Solution
    As refractive index (μ) depends on wavelength, therefore, critical angle for the same pair of media in contact will be different for different colours because critical angle is dependent on refractive index.
    Question 100
    CBSEENPH12038271

    A ray of light falls on one side of a prism whose refracting angle is 60°. Find the angle of incidence in order that the emergent ray may just graze the other side. μ =32

    Solution
    Given,
    Angle of prism, A = 60°
    Angle of emergent ray, e =90
    Refractive index, μ = 32

    ∴ r2 = C, the critical angle of the prism. 

    Now,           μga= 1sin C

                sin C = 1μ =23
                     C = 41° 49' 

    Again,        A = r1+r2 

                r1  = A - r2      = 60° - 41°49' 

                        = 18°11'


    For refraction at the surface AB, we have 

                         μ = sin isin r1 (Snell's law) 

                  sin i = μ sin r1 

                            = 1.5 × sin 18° 11'= 1.5 × 0.3121= 0.46815 

    i.e.,                 i = 27°55'. 

    is the required angle of incidence such that the emergent ray may just graze the other side.
    Question 101
    CBSEENPH12038272

    Two Plano-concave lens of glass of refractive index 1.5 have radii of curvature 20 cm and 30 cm. They are placed in contact with curved surfaces towards each other and the space between them is filled with a liquid of refractive index 4/3. Find the focal length of the system.

    Solution
    As shown in the figure, the system is equivalent to combination of three lenses in contact,

     
    Refractive index, μ = 1.5  
    Refractive index of liquid = 43 
    Radius of curvature of first lens, R= 20 cm 
    Radius of curvature of second lens, R2 = 30 cm 

    We know,
                     1F= 1f1+1f2+1f3 

    By lens makers formula
                    1f = (μ-1) 1R1-1R2 
    Now,

    1f1 = 32-1 1-120 = 140 cm

    1f2 = 43-1 120-1-30 = 5180cm

    1f3 = 32-1 1-30-1 =-160 cm 

      1F =-140+5180-160 

        F = -72 cm. 

    Thus, the system will behave as a concave lens of focal length 72 cm.
    Question 102
    CBSEENPH12038273

    A convex lens of crown glass (μg = 1.5) has a focal length of 15 cm. The lens is placed in (a) water (μw = 1.33) and (b) carbon bisulphide (μc = 1.65). Determine in each case, whether the lens behaves as a converging or diverging lens and determine its focal length.

    Solution
    Given,
    Refractive index of crown glass = 1.5
    Focal length of glss = 15 cm 
    Refractive index of water = 1.33
    Refractive index of carbon bisulphide = 1.65 

    For lens in glass, 

    115 =(μ-1) 1R1-1R2
           = (1.5 -1 ) 1R1-1R2= 0.5 1R1-1R2                                    ...(i)

    For lens in water, 
         1fw =μg-μwμw 1R1-1R2        = 1.5-1.331.33 1R1-1R2         = 0.171.331R1-1R2                                       ...(ii)

    For lens in carbon bisulphide, 

    1fc = μg-μcμc 1R1-1R2
         = 1.5-1.651.651R1-1R2
         = -0.151.651R1-1R2                          ...(iii) 

    Dividing (i) by (ii), we get 

    Focal length of lens when placed in water, f
    w = – 58.7 cm.
    The positive sign indicates that the lens is converging. 

    Dividing (i) by (iii), we get
    Focal length of lens when placed in carbon bi-sulphide, fe = – 82.5 cm.
    The negative sign indicates that the lens behaves as a diverging lens when it is immersed in carbon bisulphide.
     
    Question 103
    CBSEENPH12038274

    An astronomical telescope consists of two thin lenses set 36 cm apart and has a magnifying power of 8 in normal adjustment. Calculate the focal lengths of lenses.

    Solution
    We are given an astronomical telescope.
    distance between lenses = 36 cm 
    magnifying power = 8 

    In the normal adjustment, the final image is formed at infinity.
                          f0+fe =36              ...(i) 

    and                  -f0fe=  -8 

                            f0 = 8fe                 ...(ii) 

      From equations (i) and (ii), we have
                                 8fe+fe =36
                                       9fe = 36
                                         fe = 4 cm 

    and                               f0 = 8×4     = 32 cm. 
    where, 
    fo is the focal length of objective and, 
    fe is the focal length of eye- piece.
    Question 104
    CBSEENPH12038275

    Two thin lenses, both of 10 cm focal length—one convex and other concave, are placed 5 cm apart. An object is placed 20 cm in front of the convex lens. Find the nature and position of the final image.

    Solution
    Given, two thin lenses, 
    Focal length of both convex and concave lens, f = 10 cm 
    Distance between two lenses = 5 cm 
    For refraction at convex lens,

    Distance of object from the convex lens, u = 20 cm
    Image distance, v = v1 =? 

    Using lens formula, we have
         1v1-1(-20) =110 


                     v1 = 0 +20 cm

    The convex lens produces converging rays trying to meet at I1, at a distance of 20 cm from the convex lens, i.e., 15 cm behind the concave lens.
    I1 will serve as a virtual object for the concave lens. 

    For refraction at the concave lens, we have
     
    Object distance, u = 20 - 5 = 15 cm
    Focal length, f = -10 cm 

    As per sign convention
                          u = -15f = -10 

    Now using lens formula, 
                         1f = 1v+1u 

                          1v = 1f+1u
                              =-110-115=-3-230 =-630  

                         1v =-15
                           v = -5 cm 

    i.e., this image is in the side of object at a distance of 5 cm to the right of concave lens and at a distance of 10 cm(5 + 5) from convex lens.  

    Now,
    u = + 15 cm; v =?, f = –10cm

    Using lens formula, we have 

                     1v-115=-110
                            v = -30 cm 

    Hence, the final image is virtual and is located at 30 cm to the left of the concave lens.

    Question 105
    CBSEENPH12038276

    An equi-convex lens of refractive index μg = 1.5 and focal length 10cm is placed on the surface of water (μw = 4/3) such that its lower surface is immersed in water but its upper surface is in contact with air outside, (a) At what distance from the lens will a beam parallel to its principal axis come to focus? (b) How is the position of the focus altered if the lens is wholly immersed in water?

    Solution
    Let, the radius of curvature of each face of the lens be x cm. Then R1 = + x cm and R2= – x cm. Also,
    Refractive index f glass, μ
    g = 1.5
    Refractive index of water, μw = 4/3
    Focal length, f = + 10 cm.


    Substituting inthe lens makers formula,
                     1f =(ug-1) 1R1-1R2
    We have,
                   110 = (1.5 - 1) 1x-1-x 

    which gives,
                        x = 10 cm
    Thus, R1 = + 10 cm and R2 = –10 cm. 

    (a) As shown in the figure above, I is the image of object O due to refraction at the upper face.

    Since the refractive index of the incident ray which is in air is given by μ
    a and the refracted ray in glass is of refractive index μg, we have
    refractive index on this surface (whose radius of curvature is given by R1)

                    μgv'-μau = μg-μaR1            ...(i) 

    where,                  v' = PI' 

    The image I’ serves as the virtual object for refraction at the lower surface.
    For refraction at this surface, the incident ray is in glass and the refracted ray in water and I is the final image.
    Thus, for refraction at the lower surface (whose radius of curvature is R
    2) we have
                     μwv-μgv' = μw-μgR2           ...(ii) 

    Adding (i) and (ii) we get      
          
                 μwv-μau = μg-μaR1+μw-μgR2
    Now, substituting the values,
                     u = -;   R1 = +10 cm,  R2 = -10 cm
                                    μw = 4/3, μg = 1.5  and μa = 1,  we getv = 20 cm 

    (b) If the lens is wholly immersed in water, the formula is
                 1v-1u =μg-μwμ2 1R1-1R2 

    which (for u = – ∞) gives v = 40 cm. 

    The focus of the rays when immersed in water increases by 20 cm.

    Question 106
    CBSEENPH12038277

    A thin equi-convex lens (radius of curvature of either face being 33 cm) is placed on a horizontal plane mirror and a pin held 20 cm vertically above the lens coincides in position with its own image. The space between the lower surface of the lens and the mirror is filled with a liquid and then, to coincide with the image as before, the pin has to be raised to a distance of 25 cm from the lens. Find the refractive index of the liquid.

    Solution
    Given, a thin equi-convex lens. 
    Radius of curvature, R = 33 cm 
    Distance of the pin from the lens = 20 cm 


    In the first case, the image will coincide with the pin if the rays from the pin, after refraction through the lens, fall normally on the mirror and retrace their path, as shown in Fig.(a).

    This means that the focal length of the convex lens is 20 cm.
    i.e., f = 20 cm 

    In the second case, the focal length F of the combination of the convex lens and the plano-concave liquid lens is 25 cm. 
    i.e., F = 25 cm 

    Let f2 be the focal length of the liquid lens, then
                           1F = 1f1+1f2 

                       1f2 = 1F-1f1      =125-120 

                            f2 = -100 cm


    For the liquid lens,
    Radius of curvature of the common surface, R
    1 = –33 cm,
    R
    2 = ∞.

    If μ is refractive index of the liquid.
    Using Lens makers formula, 
                      1f2 = (μ-1) 1R1-1R2
                -1100 = μ-1 1R1-1R2
              μ - 1 =  33100 = 0.33
    i.e.,               μ = 1.33.
     
    Question 107
    CBSEENPH12038278

     The near point of a hypermetropic person is 50 cm from the eye. What is the power of the lens required to enable the person to read clearly a book held at 25 cm from the eye?

    Solution
    Given,
    Object distance, u = -25 cm
    Image distance, v = -50 cm
    Focal length, f = ? 

    Now, using lens formula,
                           1f = 1v-1u      =1-50-1-25       = -150+125 

                                = -1+250 = 150 

                           f = 50 cm. 

    Power of the lens, P = 1f(in m) = 100f(in cm) 

                           P =10050 = + 2 D 

    Hence, the corrective lens is convex because, power of the lens is positive. 


    Question 108
    CBSEENPH12038279

    Use the formula of refractive index of a prism to calculate the angle of minimum deviation for an equilateral triangular prism of refractive index √3. 

    Solution
     Given,

    Refractive index of prism, μ = 3Angle of prism, A = 60° 

    Now using the prism formula, 

                    μ = sin (A+δm)/2sin A/2

             3 = sin δm+60°2sin 60°/2   

         3 × sin 30° = sin δm+60°2 

       sin δm+60°2 = 3 ×12= sin 60°

              δm+60°2 = 60° 

                δm+60° = 120° 

                         δm = 60°  is the required minimum angle of deviation.
    Question 109
    CBSEENPH12038280

    A parallel beam of light travelling in water (refractive index = 4/3) is refracted by a spherical air bubble of radius 2 mm situated in water. Assuming the light rays to be paraxial, (a) find the position of the image due to refraction at the first surface and the position of the final image and (b) draw a ray diagram showing the positions of both the images.

    Solution

    Refractive index of water = 4/3 
    Radius of spherical air bubble, r = 2 mm 

    (a) For refraction at the first surface, using the formula,
                      μ2v-μ1u = μ2-μ1R
    whereμ1 = 4/3,  μ2 = 1  and u =   and R = 2 mm.

    Thus,

                     1v1-4/3 = 1-4/32
    which gives,  v1 = –6 mm.
    Negative sign indicates that the image I
    1 is virtual and is on the same side as the object at a distance of 6 mm from the first surface. 

    For refraction at the second surface, the image I1 serves as the virtual object which is at a distance of 6 mm + 4 mm = 10 mm from the second surface.

    For refraction to take place, we use
                    μ1v2-μ2u = μ1-μ2R
    where,
    object distance, u = -10 mm  and Radius of curvature, R = -2 mm. 

    Thus, substituting the values in the formula, we get

                     4/3v2-1-10 = 4/3-1(-2) 

    which given v2 = –5 mm.  

    The final image I
    2 is virtual and is formed at a distance of 5 mm from the second surface to the left of the second surface, i.e., the final image is formed at a distance of 1 mm from the first surface.

    (b) Figure given below shows the ray diagram.
                                     μ1v2-μ2u = μ1-μ2R

    Question 110
    CBSEENPH12038281

    With the help of ray diagram, show the formation of image of a point object by refraction of light at a spherical surface separating two media of refractive indices nand n2 (n2 > n1) respectively. Using this diagram, derive the relation.

    n2v-n1u = n2-n1R 

    What happens to the focal length of convex lens when it is immersed in water? 

    Solution
    (i) In the ray diagram below, AMB is a convex surface separating two media of refractive indices n1 and n2 (n2> n1). Consider a point object O placed on the principal axis. A ray ON is incident at N and refracts along NI. The ray along ON goes straight and meets the previous ray at I. Thus, I is the real image of O.



    From Snell's law,     n2 = sin isin r

                            n1 sin i = n2 sin r     n2n1 = sin isin r
                            n1i = n2r 

    In  NOC,          i = α + γ
    In  NIC,           γ = r - β
                              r = γ - β 

             n1 (α + γ) = n2(γ - β) 

    i.e.,       n1α + n2β = (n2-n1) γ 

    But,       α  tan α = NPOP = NPOM                                 [P is close to M]

                 β  tan β = NPPI = NPMI

                 γ  tan γ =  NPPC = NPMC

           n1. NPOM+n2. NPMI = (n2-n1) NPMC

                     n1OM+n2MI = n2-n1MC 

    Now, using Cartesian sign convention,
                                   OM = -u,   MI = +v,   MC = + R

                n1-u+n2v = n2-n1R

                 n2v-n1u = n2-n1R 

    The lens makers formula gives us the relationship,
                    1f=(μ-1) 1R1-1R2
    That is, focal length and refractive index has inverse dependence.
    Refractive index of water is greater than that of air and so, focal length of the lens will reduce when immersed in water.




    Question 111
    CBSEENPH12038282

    Two concave glass refracting surfaces, each with radius of curvature R = 35 cm and refractive index μ = 1.5, are placed facing each other in air as shown in Fig. A point object O is placed at a distance of R/2 from one of the surfaces as shown. Find the separation between the images of O formed by each refracting surface.


    Solution
    Given, two concave glasses.
    Radius of curvature of each glass, R = 35 cm
    Refractive index = 1.5 

    For refraction at the first surface, we have

    Object distance, u = AO = -3R2 = -1052cm
    μ2 = 1.5μ1 = 1Radius of curvature, R = -35 cm 

    The distance v1 of the image I1 from A is given by the relation 
                     
    μ2v1-μ1u = μ2-μ1R     
                
              1.5v1-1-105/2 = 1.5-1-35

    v1 = -45 cm   i.e.,    AI1 = 45 cm. 

    Since the radius of curvature is 35 cm, this image is 10 cm to the right of P.
    i.e., PI
    1 = 10 cm. 

    For refraction at second surface we have 

    Object distance, u = BO = -R2 = -352cm 

    The distance v2, of the image I2 , from the second surface is given by

                     μ2v2-μ1u =μ2-μ1R 

    which gives v2 = – 21 cm or BI2 = 21 cm.  

    Thus, the image is 14 cm to the right of P.
    i.e., PI
    2 = 14 cm. 

    Hence, the separation between the two images (I, I
    2) = 14 – 10 = 4 cm.

    Question 112
    CBSEENPH12038283

    Two convex lenses A and B of focal lengths 20 cm and 10 cm are placed coaxially 10 cm apart. An object is placed on the common axis at a distance of 10 cm from lens A. Find the position and magnification of the final image.

    Solution



    Given, two convex lenses A and B.
    Focal length of first lens, fA = + 20 cm
    Object distance from lens A, u
    1 = –10 cm 
    The image distance v1 is given by,
                      1v1 = 1f1+1u1        = 120+1(-10)        =120-110 

                       v1 = -20 cm 

    Thus, a virtual image is formed at I1 at a distance of 20 cm from lens A, in case, if the lens B were absent.  

    Now, this image acts as a virtual object for lens B which forms the final image at I
    2 at a distance v2 from lens B. 

    For lens B we have,
    x = 10 cm,
    Object distance from second lens, u2 = – (20+10) = –30 cm
    Focal lengtn of lens B, fB = +10 cm.


    The image distance v2 is given by
                   1v2 = 1f2+1u2        = 110-130        = 115
    i.e.,           v2 = + 15 cm 

    Thus, a real image I2 is formed at a distance of 15 cm from lens B. 

    Magnification due to lens A, m1 = v1u1 = -20-10 = +2 

    Magnification due to lens B, m2= v2u2 =15-30 = -12 

     Magnification of the final image is

                  m = m1 × m2     = +2 × (-1/2)     = -1 

    Since the magnification is negative, the final image is inverted and is of the same size as that of the object.

    Question 113
    CBSEENPH12038284

    A prism is found to give a minimum deviation of 51°. The same prism gives a deviation of 62°48’ for two values of the angles of incidence, namely, 40°6’ and 82°42’. Determine the refractive angle of the prism and the refractive index of its material.

    Solution
    Angle of minimum deviaton of prism = 51o

    The incident ray is deviated through an angle of 62°48’ (δ) wen angle of incidence = 40°6’.
    The emergent ray, for which angle of emergence, e= 82°42’ is also deviated through the same angle δ.      [ Using principle of reversibility] 



    Now,
                          δ = (i + e) - A
    i.e.,                A = (i + e) - δ
                            = 40°6' + 82°42' - 62°48'
    i.e.,,               A = 60°
    which is the refracting angle of the prism. 

    For minimum deviation, i = e. 

                 δm = 2i - A
    i.e.,              i = δmin+A2   
                         
    = (51°+60°)2 =55°30'                
    Which is the required angle of incidence at minimum deviation.

    The refractive index of the material of the prism is given by

                        μ = sin δmin+A2sinA2 

    i.e.,               μ = sin 51°+60°2sin60°2 

    i.e.,               μ = 1.648.
    Question 114
    CBSEENPH12038285

    A magnifying lens has a focal length of 10 cm. (i) Where should the object be placed if the image is to be 30 cm from the lens? (ii) What will be the magnification?

    Solution
    Given , a magnifying lens. 
    Focal length of the lens, f = 10 cm 
    Image distance, v = -30 cm

     

    In case of magnifying lens, the lens is convergent and the image is erect, virtual and enlarged and between infinity and the object on the same side of the lens as shown in the above diagram.

    Let ‘x’ be the object distance.
    Now, using lens formula
                             1f =1v-1u
    We have,
                        1-30-1(-x) =110 

                                 x = 7.5 cm 

    (ii) Magnification, m = IO = vu =-30-8.5 = +4 

    Since, the magnification is positive, the image is erect and virtual and four times that of the object.
    Question 115
    CBSEENPH12038286

    The focal length of objective and eyepiece of an astronomical telescope are 25 cm and 2.5 cm respectively. The telescope is focused on an object 1.5 m from objective, the final image is at 25 cm from the eye of the observer. Calculate the length of the telescope.

    Solution

    Here given an astronomical telescope.

    Focal length of the objective, f0 = 25 cmFocal length of eyepiece, fe = 2.5 cm

    Object distance, u0 = -1.5 m = -150 cm, Distance of image from eyepiece, ve = 25 cm 

    From the formula,
                       1v0-1u0 = 1f0 

                       1v0 = 1f0+1u0       =125-1150        =5150       = 130 
     
    i.e.,              v0 = 30 cm. 
    which is the required distance from the objective. 
    Now, again using the formula,
                         1ve-1ue =1fe 

                   - 1ue =1fe-1ve 

                 - 1ue = 12.5-125 = 925 

    i.e.,                  ue = -259cm

    Length of the telescope is given by,
                        L = v0+ue    = 30+259     = 2959 = 32.8 cm.

    Question 116
    CBSEENPH12038287

    A slide projector has to project a 35 mm slide (35 mm x 35 mm) on a 2m x 2m screen at a distance of 10 m from the lens. What should be the focal length of the lens in the projector?

    Solution

    Given, a slide projector. 

    Magnification, m = -2 m35 mm = -2 × 10335 

                     vu = -200035 

    u = -352000v = -352000× 10 × 103 mm

                           = -175 mm = -0.175 m 

    which is the object distance. 

    Now, using the lens formula,  

                  1v-1u =1f 

          110+10.175 =1f 

            1f = 10.1751.75

          f = 1.7510.175cm = 0.172 m. is the required focal length of lens in the projector. 

    Question 117
    CBSEENPH12038288

    You are given 3 lenses having powers P1 = 6D, P2 = 3D and P3 = 12D. Which two of these lenses will you select to construct a microscope?

    Solution

    Given, three lenses.
    Power of first lens, P1 = 6 D
    Power of second lens, P2 = 3D
    Power of third lens, P3 = 12 D 

    Magnifying power of a microscope is given by, 

                       m  1f0.1fe P0Pe 

    Since power and magnification have direct dependence, lens of greater power is required for magnification.

    Hence, we use P
    1 = 6D and P3 = 12D for constructing a microscope. 

                           As P0>Pe 

    Therefore, P3 = 12D should serve as objective lens and P1 = 6D should serve as eye-lens.

    Question 118
    CBSEENPH12038289

    A point object is placed at a distance of 12 cm on the axis of a convex lens of focal length 10 cm. On the other side of the lens, a convex mirror is placed at the distance of 10 cm from the lens such that the image formed by the combination coincides with the object itself. What is the focal length of the mirror?

    Solution
    For refraction at convex lens, we have


    Object distance, u = –12 cm
    Image distance, v = ?
    Focal length, f = + 10 cm 

    Using lens formula, we have

                   1v-1(-12) =110 

    i.e.,,               v = + 60 cm

    Thus, convex lens will form the image I1, at a distance of 60 cm behind the lens.  
    As the mirror is at a distance of 10 cm from the lens, image I1 will be at a distance of (60 – 10) = 50 cm from the mirror, i.e., MI1 = 50 cm. 

    Now, as the final image I2 is formed at the object itself, the rays after reflection from the mirror retraces its path, i.e., the rays on the mirror are incident normally, i.e., I1 is the centre of the mirror so that
                          R = MI1 = + 50 cm 

    and                 f = R2 =502 =25 cm. 

    which is the focal length of the mirror.



    Question 119
    CBSEENPH12038290

    The plane surface of a plano-convex lens of focal length 60 cm is silvered. A point object is placed at a distance 20 cm from the lens. Find the position and nature of the final image formed.

    Solution
    Given, a plane surface of plano-convex lens.
    Focal length, f1 = 60 cm
    Object distance from the lens = 20cm

    Let f be the focal length of the equivalent spherical mirror.

    We have, 
                        1f =1f1+1fm+1f1

    i.e.,                1f =2f1+1fm

    Here,            f1 = + 60 cm
                        fm = 

                  1f=260+1 =130

                   f = +30 cm     
     
    Now, the problem is reduced to a simple case where a point object is placed in front of a concave mirror. 

    Using mirror formula, 

                        1u+1v =1f,  

    we have   1-20+1v =1-30 

                       v = 60 cm 
    and, 
    Magnification, m =-vu=-60-20 = +3 
    The image is erect and virtual and is 3 times the size of object.

     

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    Question 120
    CBSEENPH12038291

    An equi-convex lens with radii of curvature of magnitude r each, is put over a liquid layer poured on top of a plane mirror. A small needle with its tip on the principal axis of the lens is moved along the axis until its inverted real image coincides with the needle itself. The distance of needle from lens is measured to be a. On removing the liquid layer and repeating the experiment, the distance is found to b. Given that two values of distances measured represent the real length values in the two cases, obtain a formula for refractive index of the liquid.

    Solution
    Given, an equi-convex lens and a pane mirror.



    Here, combined focal length of glass lens and liquid lens, F = a, and
    Focal length of convex lens, f
    1 = b. 
    If f2 is focal length of liquid lens, then
                      1f1+1f2 = 1F1f2 =1F-1f1        = 1a-1b 

    The liquid lens is plano-concave lens for which,
    Radius of curvature,
      R1 = -r,    R2 =  

    Using the lens makers formula,
              1f2 = (μ-1) 1R1-1R2 

    i.e.,    1a-1b = (μ-1) 1-r-1 

              μ-1 = rb-ra 

                     μ =1+rb-ra.
    Question 121
    CBSEENPH12038292

    A short-sighted person can see objects most distinctly at a distance of 16 cm. If he wears spectacles at a distance of 1 cm from the eye, what focal length should they have so as to enable him to see distinctly at a distance of 26 cm?

    Solution
    The person is suffering from myopia (shortsightedness) and wears spectacles at a distance of 1 cm from the eyes.
    Therefore,
    Image is formed at a distance, v = -(16-1) = 15 cm 

    Also given,
    Object distance, u = -(26-1) cm  = -25 cm 
    Using len's formula, 
                 1f = 1v-1u      = 1-15-1-25 

                     = 125-115= -275 

                   f =-752cm  = -37.5 cm 

    Focal length is nagative. So, a concave lens of focal length 37.5 cm is to be used.
    Question 122
    CBSEENPH12038293

    In the Fig. the direct image formed by the lens (f = 10 cm) of an object placed at O, and that formed after reflection from the spherical mirror are formed at same point O. What is the radius of curvature of the mirror?

    Solution
    Here,
    Focal length of the lens, f = 10 cm,
    Distance of object from the lens, u = –15 cm. 

    Let v be the distance of image I formed by the lens L.
     

    Using lens formula,
                      1v-1u = 1f 

                      1v =1f+1u       =110-115      =130
    i.e., image is at a distance, v =LI = 30 cm 

    If, I coincides with the centre of curvatureC of the mirror then, the image will be formed at I.

    ∴ Radius of curvature, R = PC = PI
                                         = PL – LI
                                         = 50 – 30
                                         = 20 cm.

    Question 123
    CBSEENPH12038294

    The least distance of distinct vision of a long sighted man is 50 cm. He reduces this distance to 10 cm by wearing spectacles. What is the power and type of lenses used by him?

    Solution
    A person is suffering from long-sightedness.

    Object is at, u = –10 cm and
    Least distance of distict vision, v = –50 cm. 

    N
    ow, using the lens formula we have,
                         1f=1v-1u 

                        1f =1-50+110      = +450

                      f = + 504 = + 12.5 cm 

    Therefore, power of the lens, P = 100f
                              P = 10012.5 = 8D 

    ∴   The type of lenses used is convex lens.
    Question 124
    CBSEENPH12038295

    A ray of light, incident on a equilateral glass prism (μmedium =3) moves parallel to the base of the prism inside it. What is the angle of incidence for this way?

    Solution

    Given, an equilateral glass prism.
    Angle of prism = 60o 
    Refractive inex of the medium, μ =3 

    When light ray moves parallel to the base of the prism inside it,  then 
                              r1 = r2
    so that ,the minimum deviation takes place. 

    For minimum deviation r = A/2  = 30° 

    Now, using Snell's law,
                            μ = sin isin r

                     3  = sin isin 30° = sin i1/2 

                    sin i = 32
                        i =sin-132 = 60° 
    is the required angle of incidence so that, the ray travels parallel to the base ofthe prism.

    Question 125
    CBSEENPH12038296

    An object is placed at a distance of 15 cm from a convex lens of focal length 10 cm. On the other side of the lens, a convex mirror is placed such that its distance, from the lens, equals the focal length of the lens. The image formed by this combination is observed to coincide with the object itself. Find the focal length of the convex mirror.

    Solution

    In the case of convex lens

    Object distance, u = -15 cm
    Focal length, f = 10 cm 

    Now, using the lens formula, 

                       1f = 1v-1u

                       1v = 1f+1u 
                            = 110+1-15

                             = 3-230 =130 

    i.e., the image is formed at a distance of 30 cm. 

    For convex mirror,

    Object distance, u = 30 - 10 = 20 cm 
    Image distance, v = 10 + 15 = 25 cm 

    Now, using mirror formula,

                   1f = 1v+1u 

                        = 125+1-20 

                        = 4-5100=-1100
    i.e.,            f = -100 cm. 

    Therefore, focal length of the convex mirror is 100 cm. 

    Question 126
    CBSEENPH12038297

    A 5 cm long needle is placed 10 cm from a convex mirror of focal length 40 cm. Find the position, nature and size of image of the needle. What happens to the size of the image when the needle is moved further away from the mirror?

    Solution
    Given,
    Length of the needle = 5 cm
    Distance of object from the convex mirror, u = -10 cm
    Focal length, f = 40 cm 

    Using the mirror formula, 

                      1f =1v+1u1v =1f-1u      = 140-1-10       =1+440       =540 
     
                    v = 405    =8 cm.  

    Now, magnification, m = -vu 

    When needle moves further away from the convex mirror, the image moves further behind the mirror towards the focus and size of the image decreases. When it is far off, it appears almost as a point image of the object.
    Question 127
    CBSEENPH12038298

    A luminescent object is placed at a depth of ‘d’ in a (optically) denser medium of refractive index ‘μ’. Prove that radius r of the base of the cone of light, from the object, that can emerge out from the surface is r = dμ2-1.

    Solution
    A luminescent object is placed at a depth of 'd' in an optically denser medium of refractive index 'μ'. 


    Cone of light is formed due to total internal reflection. 

    ∴ For total internal reflection to take place,
                          sin ic = 1μ 

    and, from the fig.,
                          tan ic = rd 

            sin ic1-sin2ic = rd 
                  r = dμ2-1. 

    Question 128
    CBSEENPH12038299

    A plot between the angle of deviation (δ) and angle of incidence (i) for triangular prism is shown below. Explain any given value of ‘δ’ corresponds to two values of angle of incidence? State the significance of point P on the graph. Use this information to derive an expression for refractive index of the material of the prism.

    Solution
    Generally, any given value of angle of minimum deviation δ, corresponds to two values i and e, except for i = e. This, in fact, is expected from the symmetry of i and e as,
                   δ = i + e – A,
    i.e., δ remains the same even if i and e are interchanged. 


                            Fig.(a) 

    In the fig. above, point P is the point of minimum deviation. This is related to the fact that the path of the ray as shown in fig (b) can be traced back, resulting in the same angle of deviation. 

     
                           Fig. (b)
    At the minimum deviation D
    m, the refracted ray inside the prism becomes parallel to the base.
    For,                       δ = Dm;
    we have,                i = e                    and,
                               r1 = r2 = r
                          2r = A
                            r = A/2 

    In the same way,  

                             Dm = 2i - A 

                            i = A+Dm2 
    ∴ The refractive index of the prism is 

                     μ =sin (A+Dm)sinA/2. 


    Question 129
    CBSEENPH12038300

    A thin lens, made of material of refractive index μ has a focal length f. If the lens is placed in a transparent medium of refractive index ‘n’ (n < μ), obtain an expression for the change in focal length of the lens. Use the result to show that the focal length of a lens of the glass = becomes μw(μg-1)(μg-μw) times its focal length in air, when it is placed in water (μ = μw).

    Solution
    Here, we have a thin lens of refractive index 'μ' and focal length 'f'. This lens is placed in a transparent medium of refractive index 'n'.
    Let, the radii if curvature of the lens be R1 and R2
    Therefore, using lens makers formula , focal length is given by, 
              1f = (μ-1) 1R1-1R2                 ...(i) 

    When the lens is put in a transparent medium, the refractive index of the material of the lens with respect to the medium = μn. 

    Thus focal length f' of the lens in the medium is given by, 
            1f' = μn-1 1R1-1R2                 ...(ii) 

    Now, from Eqns. (i) and (ii),  

                   ff' = (μ-1)μn-1 

    i.e.,         f' = (μ-1)n(μ-n).f                         ...(iii) 

    Thus, change in focal length is, 

    f = f' -f (μ-1)n(μ-n)f-f 

         = f(μ-1)n - (μ-n)(μ-n) 

         = fμn-n-μ+n(μ-n)
         = 1(μ-1) 1R1-1R2μn-μ(μ-n) 

         = R1R2(R2-R1) (μ-1)μ(n-1)(μ-n) 

    f = R1R2(R2-R1)n(μ-n)-1(μ-1)            ...(iv) 

    From equation (iii), we have  

                     f' = (μ-1)n(μ-n).f 

    Putting,  μ = μg and n = μw 
    where, 
    μg is the refractive index of glass and, 
    μw is te refractive index of water.  

              f' = (μg-1)μw(μg-μw). f 

    The ray diagram is as shown below:

     




    Question 133
    CBSEENPH12038304
    Question 134
    CBSEENPH12038305
    Question 141
    CBSEENPH12038312
    Question 145
    CBSEENPH12038316

    A ray of light passing through an equilateral triangular glass prism form air undergoes minimum deviation when angle of incidence is 3/4th of the angle of prism. Calculate the speed of light in the prism.

    Solution

    Angle of prism, A = 60o 
    Refractive index of prism = 1.5 
    Given, angle of incidence , i1=i234A = 3445o = 45o
    As,                    A + δ = i1 + i
                    60δ = 45o + 45

    Then, angle of minimum deviation, δ =  90o - 60o                                                           = 30
    We know that, velocity of light in vacuum = 3×108 m/s 
    Now, using the formula, 

                    μ = sin (A+δm)/2sin A/2 = cv
    That is,  
                    v = c sin A/2sin (A+δm)/2   = 3× 108  sin 30osin (60o + 30o)/2    = 3× 108 sin 30osin 45o    =  3× 108 ×0.50000.7071   = 2.12 × 108 m/s  
     
    is the required speed of light in the prism.

    Question 147
    CBSEENPH12038318

    i.) Derive the lens formula, 1/ f = 1/v – 1/u for a concave lens, using the necessary ray diagram.
    ii.) How does the angle of minimum deviation of a glass prism of refractive index 1.15 change, if it is immersed in a liquid of refractive index 1.3?

    Solution
    i.) Derivation of len's formula : 

    Len's formula gives us the relation between focal length of a lens and distances of object and image from the optical centre of the lens. 
    Let's consider a convex lens and O be the optical centre ; F the principal focus with focal length f. 

    Let, AB be the object held perpendicular to the principal axis at a distance beyond the focal length of the lens. And, as seen from the fig. above a real, inverted and magnified image A'B' is formed. 
    We can see that,  ABO and A'B'O is similar .

             A'B'AB = OB'OB 

    and also, 

    A'B'F and OCF are similar. 

                  A'B'OC=FB'OF 

    But, OC = AB 

               A'B'AB= FB'OF 
    From the above equations, we get 

          OB'OB = FB'OF= OB' - OFOF 
    Using the sign convention, 
               OB= -u , OB' = +v, OF = +f 

      v-u = v-ff 

      vf = -uv + uf  or uv = uf -vf  

    Dividing both sides by uvf, we have 

              uvuvf = ufuvf-vf uvf 

    i.e.,         1f = 1v-1u 

    which is the required lens formula. 

    ii.) Given, a glass prism of refractive index = 1.5 
    When, this prism is immersed in a liquid of refractive index 1.3 then, angle of minimum deviation of the prism reduces. 




    Question 148
    CBSEENPH12038319

    How does the fringe width of interference fringes change, when the whole apparatus of Young's experiment is kept in a liquid of refractive index 1.13?

    Solution

    Fringe width is directly proportional to wavelength and inversely proportional to refractive index.  

    The formula is given by, 

    In air, Fringe width, x = Dλd 

    In medium, Fringe width, x = μd
    where,
    d is the distance between the slits and, 
    D is the distance between the screen and the slit. 

    Therefore, fringe width decreases by a factor of μ (1.33) when placed in the liquid. 



    Question 149
    CBSEENPH12038320

    How is a wavefront defined? Using Huygen’s construction draw a figure showing the propagation of a plane wave refracting at a plane surface separating two media. Hence verify Snell's law of refraction.

    Solution

    Wavefront is a locus of all particles of the medium, vibrating in the same phase. 

    Huygen's wave theory: 

    Consider two media namely, 1 and 2 and, let XY be the surface seperating two media. 
    The speed of the waves in these media will be v1 and v2


    Suppose, a plane wavefront AB in first medium is incident obliquely on the boundary surface XY, and its end A touches the second surface at a point A' at time t = 0 while, the other end B reaches the second surface at point B' after time-interval t.
    Here,               BB' = t 

    As per Huygen’s principle, secondary spherical wavelets emanates from points A and B , which travel with speed v1 in the first medium and speed v2 in the second medium. 

    Distance traversed by secondary wavelets in medium 2 in time t , AA' = v2
    Distance traversed by point of wavefront in medium 1 in time t = BB' = v1

    Now, considering A as the centre we will draw an arc and a tangent( B'A') is drawn from B' to this point. So, as the incident wavefront advances, secondary wavelets start from points in-between A and B' and will reach A'B' simultaneously. 
    According to Huygen’s principle A'B' is the new position of wavefront AB in the second medium and, A'B' is the refracted wavefront. 

    Let the incident wavefront AB and refracted wavefront A'B' make angles i and r respectively with refracting surface XY. 

    In right AB'B,
     
        sin i= sin BAB' = BB'AB'=v1tAB'    ... (i)

    Similarly, in right AA'B'

       sin r = sin AB'A' = AA'AB'=v2tAB'    ...(ii) 

    Dividing equations (i) by (ii) , we have  

                  sin isin r = v1v2 = constant  

    which is the required Snell's law.  

    Hence proved. 






    Question 150
    CBSEENPH12038321

    For a ray of light travelling from a denser, medium of refractive index n1 to a rarer medium of refractive index n2. Prove that n/ n1= sin ic where ic is the critical angle of incidence for the media.

    Solution

    Given, a ray of light travelling from denser medium of refractive index n1 to a rarer medium of refractive index n2. 
    Snell's law is given by,
      
                           sin isin r = n2n1

    Now, critical angle is the angle of incidence in denser medium for which angle of refraction in rarer medium is 90o
    i.e.,    i = ic  when r = 90o

    Thus, putting these values in snell's law , we have 

                        sin icsin 90o = n2n1 
     
    i.e.,                      n2n1 = sin ic 
     

    Question 151
    CBSEENPH12038322

    The convex lenses of same focal length but of apertures 5 cm and 10 cm are used as objective lenses in two astronomical telescopes.
    (i)    What will be the ratio of their resolving power?
    (ii)    Compare the intensity of image formed in two power?

    Solution

    Given, two convex lenses. 
    Aperture of first lens = 5 cm
    Aperture of second lens = 10 cm

    i) Resolving power is directly proportional to the diameter. 
    Therefore, the ratio of resolving power is, 

                        R.P1R.P2= 510=12

    ii) Intensity is directly proportional to the area of objective lens.

                      I1I2 = 52102 = 14 


    Question 152
    CBSEENPH12038323

    The refractive indices of glass and water with respect to air are 3/2 and 4/3 respectively. What will be the refractive index of glass with respect to water?

    Solution

    Refractive index of water, μair = 1 
    Given, 
    Refractive index of glass w.r.t. air, μga = 32 

    Refractive inex of water w.r.t air, μwa = 43  

     refractive index of glass w.r.t. water, = μgw = μgaμwa = 3243 = 98

    Question 153
    CBSEENPH12038324

    An angular magnification (magnifying power) of 30X is desired using an objective of focal length 1.25 cm and an eyepiece of focal length 5 cm. How will you set up the compound microscope?

    Solution
    Given, angular magnification = 30 
    Focal length of objective, fo = 1.25 cm
    Focal length of eyepiece, fe = 5 cm 

    In normal adjustment, image is formed at least distance of distinct vision, d = 25 cm.

    Using formula, 
    Angular magnification of eyepiece  = 1+Dfe
                                                        = 1+255 = 6 

    Now, magnification of objective lens,   m =306 = 5 

     m =-v0u0 =5  or, v0 = -5u0 

    For objective lens, using the lens formula,  

                 1v0-1u0= 1f0
        1-5μ0-1μ0= 11.25 

                       -65μ0= 11.25

                          u0 =-6 × 1.255      = -1.5 cm 

    i.e., object should be held at a distance 1.5 cm in front of objective lens.

    As,       v0 = -5 μ0 

            v0 =-5(-1.5)      = 7.5 cm

    For eyepiece lens,  

                 1ve-1ue=1fe   [using len's formula]
    we have,
               1μe = 1ve-1fe        = 1-25-15        = -625 

                 ue =-256    = - 4.17 cm 

    Thus, the object is at a distance of 4.17 cm from the eyepiece. 

    Separation between the objective lens and eyepiece = | u
    | + | v0 | = 4.17 + 7.5 = 11.67 cm.
    Question 154
    CBSEENPH12038325

    Monochromatic light of wavelength 589 nm is incident from air on a water surface. What are the wavelength, frequency and speed of (a) reflected, and (b) refracted light? Refractive index of water is 1.33.

    Solution

    Given, 
    Wavelength of monochromatic light, λ = 589 nmSpeed of light, c = 3 × 108 m/sRefractive index, μ = 1.33

    (a) For reflected light,
    Wavelength is going to remain the same for incident and reflected light. 
    Wavelength, λ = 589 nm = 589 × 10-9m
    Frequency of light, v = cλ                                     = 3 × 108589 × 10-9                                      = 5.09 × 1014Hz.
    Speed of lightwill remain invariant in two media.
    Therefore, v = c = 3 × 108 m/s 

    (b) For refracted light, 
    Refractive index of water w.r.t. air,   μωa = vavω 

    i.e.,                                                 μωa = vaλavωλω
                     va = vω
    So, wavelength of light 

    λω = λaμωa = 589 × 10-91.33                       = 4.42 × 10-7m
                              
    As frequency remains unaffected on entering another medium, therefore, 
               νω = νa = 5.09 × 1014 Hz 

    Speed,
                  v' = vaμω = 3 × 1081.33     = 2.25 × 108 m/s.  

    i.e., speed of the light has decresed when it entered the second medium.

    Question 155
    CBSEENPH12038326

    What is the shape of the wavefront in each of the following cases:
     Light diverging from a point source.

    Solution
    The wavefront is spherical in shape when light is diverging from the point source.
    Question 156
    CBSEENPH12038327

    What is the shape of the wavefront in each of the following cases:
     Light emerging out of a convex lens when a point source is placed at its focus.

    Solution
    We have a plane wavefront for, light emerging out of a convex lens when a point source is placed at it's focus.
    Question 157
    CBSEENPH12038328

    What is the shape of the wavefront in each of the following cases:
    The portion of the wavefront of light from a distant star intercepted by the Earth. 

    Solution
    We have a plane wavefront, because a small area on the surface of a large sphere is nearly planar.
    Question 158
    CBSEENPH12038329

    The refractive index of glass is 1.5. What is the speed of light in glass? (Speed of light in vacuum is 3.0 × 108 ms-1)

    Solution

    Given, refractive index of glass, μg = 1.5 

    Refractive index is given by, 

                 μ = speed of light in vacuumspeed of light in the medium

      Speed of light in glass= speed of light in vaccumμg
                                          = 3.0 × 1061.5= 2.0 × 106 ms-1.

    Question 159
    CBSEENPH12038330

    Is the speed of light in glass independent of the colour of light? If not, which of the two colours red and violet travels slower in a glass prism?

    Solution
    Indeed, the colour of the light influence the refractive index and speed of light in a medium. That is, both of them depends on the wavelength of the light.
    We know that, μ > μr.
    Hence,  vviolet < vred.
    Thus, the violet component of white light travels slower in prism as compared to the red light.
    Question 160
    CBSEENPH12038331

    In a Young's double-slit experiment, the slits are separated by 0.28 mm and the screen is placed 1.4 m away. The distance between the central bright fringe and the fourth bright fringe is measured to be 1.2 m. Determine the wavelength of light used in the experiment.

    Solution

    Given,
    Distance between the screen and slits, D = 1.4 m,   Distance between slits, d = 0.28 mm =0.28 × 10-3 m 

    Fringe width,ω = 1.24 = 0.3 × 10-2m   (as the distance 1.2 m is of fourth fringe from central maxima)

    Using formula, we have 

    Fringe width, ω = d 
      λ = ωdD    = 0.3 × 10-2 × 0.28 × 10-31.4   = 0.06 × 10-5    = 600 × 10-9    = 600 nm.  

    which is the required wavelength.

    Question 161
    CBSEENPH12038332

    In Young’s double-slit experiment using monochromatic light of wavelength λ, the intensity of light at a point on the screen where path difference is λ, is K units. What is the intensity of light at a point where path difference is ?

    Solution
    Intensity of light = K units 
    Phase difference corresponding to λ is 2π and phase difference corresponding to λ/3 is 2π/3. 

    Now, using the formula of intensity,
                   I = I1+I2+2I1I2 cos ϕ 

    Let, 
    I1 = I2 = I0       
                   
    In the first case, when path difference is λ.
                  K = I0+I0+2I0 cos 2π = 4I0 

    In the second case, when path difference is λ3
                 K' = I0+I0+2I0cos2π3
                     = I0+I0-2I012 = I0 

    Now,
    K'K = I04I0 =14  =
      K' = K4 

    Therefore, intensity is one-fourth of it's initial value when path difference is λ/3.
                           .
     
    Question 162
    CBSEENPH12038333

    A beam of light consisting of two wavelengths, 650 nm and 520 nm, is used to obtain interference fringes in a Young's double-slit experiment.
    Find the distance of the third bright fringe on the screen from the central maximum for wavelength 650 nm.

    Solution

    Here,
    Wavelength of the beam of light, λ1 = 650 nm = 650 × 10-9m
    Wavelength of beam of light,  λ2 = 520 nm = 520 × 10-9 m

    Suppose, 
    d = distance between two slits and, 
    D is the distance between the screen and slit. 

    For third bright fringe, n = 3
    Distance of third bright fringe from the central maximum, x =n.λ1.Dd
                        = 3 × 650 × 10-7 × 1200.2= 0.117 cm = 1.17 mm

    Question 163
    CBSEENPH12038334

    A beam of light consisting of two wavelengths, 650 nm and 520 nm, is used to obtain interference fringes in a Young's double-slit experiment.
    What is the least distance from the central maximum where the bright fringes due to both the wavelengths coincide?

    Solution

    Here, a beam of light consists of two wavelengths. 

    Wavelength, λ1 = 650 nm = 650 × 10-9m
    Wavelength, λ2 = 520 nm = 520 × 10-9 m 

    Suppose,                  d = distance between two slits
                                     D = distance of screen from the slits. 

    Let n fringes of wavelength 650 nm coincide with (n + 1) fringes of wavelength 520 nm.

             x = 1D/d = (n + 1)  λ2 D/d

         x = n × 650 = (n + 1) × 520 

        n+1n = 650520 = 54 

        1+1n = 54   1n =54-1 = 14

                n = 4
    Hence,
    Distance from the central maximum, x = n.λ1Dd
                                                                 = 4 ×650 ×10-7×1200.2= 1.56 mm.

    Question 164
    CBSEENPH12038335

    In a double-slit experiment the angular width of a fringe is found to be 0.2° on a screen placed 1 m away. The wavelength of light used as 600 nm. What will be the angular width of the fringe if the entire experiment apparatus is immersed in water? Take refractive index of water to be 4/3.

    Solution
    Given, 
    Angular width of a fringe = 0.2o 
    Wavelength of light used, λ = 600 nm 
    Refractive index of water, μ = 43 

    Angular fringe separation, θ = λd or d = λθ
    In water, d = λ'θ' 

             λθ = λ'θ'
           θ'θ =λ'λ =1μ = 3/4         μωa = λαλω

    Angular fringe width when immersed in water, 
                                                                 θ' = 34θ     = 34× 0.2°    = 0.15°.                
    Question 165
    CBSEENPH12038336

    What is the Brewster angle for air to glass transition? (Refractive index of glass = 1.5.)

    Solution

    Given,
    Refractive index of glass, μ = 1.5 

    Using formula,
                            tan ip = μ
                              ip = tan-1(μ)
                                     = tan-1(1.5)
    Thus,                     ip = 56.3°,
    is the required polarizing angle or brewster angle.

    Question 166
    CBSEENPH12038337

    Light of wavelength 5000 Å falls on a plane reflecting surface. What are the wavelength and frequency of the reflected light? For what angle of incidence is the reflected ray normal to the incident ray?

    Solution

    Given, 
    Wavelength of incident light, λ = 5000 Ao 

    The wavelength and frequency of the reflected light are the same as that of the incident light. 

    ∴ Wavelength of reflected light = 5000 Å
    Frequency of reflected light, ν = c/λ
                                                = 3 × 1085000 × 10-10Hz = 6 × 1014Hz


    According to the law of reflection, i = r 

    When, the reflected ray is normal to the incident ray, we have
                             i + r = 90°
                             i + i = 90°
                                 2i = 90°
    i.e.,                          i = 45°.

    Question 167
    CBSEENPH12038338

    Estimate the distance for which ray optics is good approximation for an aperture of 4 mm and wavelength 400 nm.

    Solution

    Here,
    Aperture, a = 4 mm = 4 × 10-3 m
    Wavelength, λ = 400 nm = 400 × 10-9 m = 4 × 10-7 m 

    Ray optics is good approximation upto distances equal to Fresnel's distance (ZF).
    Fresnel's distance is given by, 
                     ZF = a2λ = 4 × 10-324 × 10-7 = 40 m.

    Question 168
    CBSEENPH12038339

    The 6563 Å Hα line emitted by hydrogen in a star is found to be red-shifted by 15A. Estimate the speed with which the star is receding from the Earth.

    Solution
    Given, 
    Wavelength of  line, λ = 6563 Å = 6563 × 10-10m
     
    Redshift, λ' - λ = 15 Å = 15 × 10-10m 

    Now, according to the formula, 

                            λ' -λ = Vsλc 

    we have,                  Vs = cλ(λ' -λ)
                                       = 3.0 × 1086563 ×10-10× 15 × 10-10
                                      = 6.8566 × 105 ms-1
    i.e.,                         Vs = 6.86 × 105 ms-1. 

    therefore, the start is receding from the earth at a speed of 6.86 × 105 m/s. 

    Question 169
    CBSEENPH12038340

    Explain how Newton’s Corpuscular theory predicts the speed of light in a medium, say water, to be greater than the speed of light in vacuum. Is the prediction confirmed by experimental determination of the speed of light in water? If not, which alternative picture of light is consistent with experiment?

    Solution

    According to Newton's Corpuscular theory of light, when corpuscles of light strike the interface XY, separating a denser medium from a rarer medium, the component of their velocity along XY remains the same.


    If v1 is velocity of light in rarer medium (air),
    v2 is velocity of light in denser medium (water),
    i is angle of incidence, and
    r is angle of refraction then, 
    Component of v1 along XY = v1 sin i
    Component of v2 along XY = v2 sin r

    As,                 v1 sin i = v2 sin r 

                          v2v1 = sin isin r = μ 

    Since, μ>1           
          v2>v1 

    i.e., light should travel faster in water than in air.

    This prediction of Newton s theory is opposite to the experimental result. 

    Huygens wave theory predicts that v2 < v1, which is consistent with experimental conclusion.

    Question 170
    CBSEENPH12038341

    You have learnt in the text how Huygens' principle leads to the laws of reflection and refraction. Use the same principle to deduce directly that a point object placed in front of a plane mirror produces a virtual image whose distance from the mirror is equal to the object distance from the mirror.

    Solution
    We are given a plane mirror XY and let, O be a point object at a distane OP, in front of the plane mirror. A part RPQ of the wavefront touches the plane mirror at P and from this point spherical wavefronts start emanating.
    Whereas disturbance from R and Q continue moving forward, along the normal rays OR and OQ, that reflects back v. When, disturbances from R, P and Q reach the mirror at A, B'and C respectively, reflected spehrical wavefront is formed. 

     

    The reflected wavefront AB'C, appears to start from I. Hence, I becomes virtual image for O as real point object.
    Draw AN normal to XY, hence parallel to OP.

    Now, OA is the incident ray (being normal to incident wavefront ABC) and AD is reflected ray (being normal to reflected wavefront AB'C). 

    Thus,  ∠OAN = ∠DAN = ө    [i = r]
    But,    ∠OAN = alternate ∠AOP
    and    ∠DAN = corresponding ∠AIP
          ∠AOP = ∠AIP 

    Now, in ∆AIP and ∆AOP 

    ∠AIP = ∠AOP    (each ө)
    ∠APl = ∠APO = 90°    (each 90°)
    AP is common to both
    s become congruent
    Hence,    PI = PQ 

    i.e., normal distance of image from the mirror = normal distance of object from the mirror. 

    Thus, virtual image is formed as much behind the mirror as the object in front of it




    Question 171
    CBSEENPH12038342

    Let us list some of the factors which could possibly influence the speed of wave propagation:
    (i) nature of source.
    (ii) direction of propagation. 
    (iii) motion of source and/or observer.
    (iv) wave length.
    (v) intensity of the wave.
    On which of these factors, if any, does
    (a) the speed of light in vacuum,
    (b) the speed of light in a medium (say, the glass or water) depend?

    Solution

    (a) Speed of light in vacuum is an absolute constant, according to Einstein's theory of relativity. It does not depend upon any of the factors listed above or any other factor. 

    (b) The speed of light in a medium like water or glass:

    (i) does not depend upon the nature of the source.

    (ii) does not depend upon the direction of propagation, when the medium is isotropic.

    (iii) does not depend upon motion of the source w.r.t. the medium, but depends on motion of the observer relative to the medium. 

    (iv) depends on wavelength of light, being lesser for shorter wavelength and vice-versa. 

    (v) does not depend upon intensity of light.

    Question 172
    CBSEENPH12038343

    For sound waves, the Doppler formula for frequency shift differs slightly between the two situations:
    (i) source at rest; observer moving, and
    (ii) source moving; observer at rest.
    The exact Doppler formulas for the case of light wave in vacuum, are however, strictly identical for these situations. Explain why this should be so. Would you expect the formulas to be strictly identical for the two situations in case of light travelling in a medium?

    Solution
    Sound waves require a medium for propagation. Thus, even though both the situations may correspond to the same relative motion (between the source and the observer), they are not identical physically since, the motion of the observer, relative to the medium is different in the two situations. Therefore, we cannot expect Doppler formulas for sound to be identical for (i) and (ii).

    For light waves in vacuum, there is clearly nothing to distinguish between two cases given. Here only the relative motion between the source and the observer counts and the relativistic Doppler formula is the same for both cases.
    For light propagation in a medium, once again like for sound waves, the two situations are not identical and we should expect the Doppler formulas for this case to be different for the two situations (i) and (ii).
    Question 173
    CBSEENPH12038344

    In double-slit experiment using light of wavelength 600 nm, the angular width of a fringe formed on a distant screen is 0.1°. What is the spacing between the two slits?

    Solution

    Wavelength of light, λ = 600 nm = 600 × 10-9 m

    Angular fringe width, Bθ =λd

                                  d = λβθ

    where, d is the distance between the slits.

    Now, 
     βθ = 0.1° = 0.1 × π180radian                   = 0.1 × 3.14180radian

     d = 600 ×10-9× 1800.1 × 3.14m = 3.44 × 10-4m.
    is the required spacing between the two slits. 

    Question 174
    CBSEENPH12038345

    Answer the following questions:
    In a single slit diffraction experiment, the width of the slit is made double the original width. How does this affect the size and intensity of the central diffraction band?

    Solution
    Width of central diffraction band = 2D λd.
    where, d is the width of the slit.
    So, on doubling the width of the slit, the size of the central diffraction band reduces to half value. But, the light amplitude becomes double, which increases the intensity four fold.
    Question 175
    CBSEENPH12038346

    Answer the following questions:
    In what way is diffraction from each slit related to interference pattern in a double-slit experiment?

    Solution
    If, width of each slit is of the order λ, then the intensity of interference fringes in Young's double-slit experiment is modified by the diffraction pattern of each slit.
    Question 176
    CBSEENPH12038347

    Answer the following questions:
    When a tiny circular obstacle is placed in the path of light from a distant source, a bright spot is seen at the centre of the shadow of the obstacle. Explain why?

    Solution
    A bright spot is seen at the center of the shadow of objective because, wave diffracted from the edge of the circular obstacle interface constructively at the centre of the shadow producing a bright spot.
    Question 177
    CBSEENPH12038348

    Answer the following questions:
    Two students are separated by a 7 m partition wall in a room 10 m high. If both light and sound waves can bend around obstacles, how is it that the students are unable to see each other even though they can converse easily.

    Solution
    The size of the obstacle or aperture should be comparable to the wavelength for diffraction of waves by obstacles, through a large angle. 

    This follows from sin θ = λa.
    For light waves,  

    Wavelength, λ = 10-7 m and, 
    size of the wall, a = 10 m

     sin θ = 10-710= 10-8 
     
    This implies, θ0 

    That is, light goes almost unbent and hence, the students are unable to see each other. 

    For sound waves,  

    Frequency, ν = 1000 Hz  

    i.e.,          cν= 3301000=0.33 m

             sinθ = λa=0.3310 = 0.033 m

    Here, θ has a definite value and the waves will bend around the partition. Hence, students can converse easily.

    Question 178
    CBSEENPH12038349

    Answer the following questions:
    Ray optics is based on the assumption that light travels in a straight line. Diffraction effects (observed when light propagates through small apertures/slits or around small obstacles) disprove this assumption. Yet the ray optics assumption is so commonly used in understanding location and several other properties of images in optical instruments. What is the justification?

    Solution
    Typical sizes of the apertures involved in ordinary optical instruments are much large than the wavelength of light. Henceforth, the diffraction effects of light waves are negligibly small in these instruments and is of negligible or no significance. Thus, the assumption that light travels in straight lines can be safely used in the optical instruments. 
    Question 179
    CBSEENPH12038350

    Two towers on top of two hills are 40 km apart. The line joining them passes 50 m above a hill halfway between the towers. What is the longest wavelength of radio waves, which can be sent between the towers without appreciable diffraction effects?

    Solution

    Distance between the two towers = 40 km 
    Size of aperture, a = 50 m
    Distance of aperture from tower, Zf

    Fresnel distance is the half of the distance between the towers. 

    i.e., z= 402 = 20 km = 20 × 103 m.
    Therefore, now using the formula, 

    Fresnel distance, ZF =a2λ 

    we have,       λ = a2ZF = (50)220 × 103

                       λ = 125 × 10-3 m = 12.5 cm. 

    This is the required longest wavelength of radio waves, which can be sent in between the towers without considerable diffraction effects.

    Question 180
    CBSEENPH12038351

    A parallel beam of light of wavelength 500 nm falls on a narrow slit and the resulting diffraction pattern is observed on a screen 1 m away. It is observed that the first minimum is at a distance of 2.5 mm from the centre of the screen. Find the width of the slit.

    Solution

    Given,
    Distance of the screen from the slit, D = 1 m

    Distance of the first minimum when the centre of screen, x = 2.5 mm = 2.5 × 10-3m
    n=1 is the first minimum.

    Wavelength of light, λ =500 nm = 500 × 10-9m                                                             = 5 × 10-7 m

    Using formula,
                            x = nλDd

    we have,           d = nλDx
                        d = 1 × 5 × 10-7 × 12.5 × 10-3    =2 × 10-4m    = 0.2 mm 

    is the required width of the slit.

    Question 181
    CBSEENPH12038352

    Answer the following question:
    When a low flying aircraft passes overhead, we sometimes notice a slight shaking of the picture on our TV screen. Suggest a possible explanation.

    Solution
    A low flying aircraft reflects the TV signal. The slight shaking on the TV screen is due to interference between the direct signal and the reflected signal.
    Question 182
    CBSEENPH12038353

    Answer the following question:
    As you have learnt in the text, the principle of linear superposition of wave displacement is basic to understanding intensity distributions in diffraction and interference patterns. What is the justification of this principle?

    Solution
    Superposition principle is in accordance with the linear character of the differential equation governing wavemotion. If, y1 and y2 are solutions of the wave equation, then any linear combination of y1 and y2 is also a solution of the wave-equation. When amplitudes are large (e.g., high intensity laser beams) and non-linear effects are important, the situation is for more complicated.
    Question 183
    CBSEENPH12038354

    In deriving the single slit diffraction pattern, it was stated that the intensity is zero at angles of nλ/a. Justify this by suitably dividing the slit to bring out the cancellation.

    Solution
    Let the slit width 'a' be divided into n equal parts of width ' a' ' so that,
                                    a' = an
    i.e.,                           a = na'

    Then,
    Angle, θ = a = na'

    i.e.,      θ = λa' 

    At this derived angle, each slit will make first diffraction minimum. Hence, the resultant intensity for all slits will be zero at an angle of a.
    Question 184
    CBSEENPH12038355

    How would the angular separation of interference fringes in Young's double slit experiment change when the distance between the slits and screen is halved?

    Solution

    Angular seperation of interference fringes is given by,   
                           ω = λDd 
    D is the distance between screen and slit and, 
    d is the distance between slits.

    Now, when the distance between the slits and the screen is halved we have, 
         
                   ω1 = λ. D/2d = 12λDd 

               ω1 = 12 ω. 
    That is, angular seperation becomes half of the initial value.

    Question 185
    CBSEENPH12038356

    Unpolarised light is incident on a plane surface of glass of refractive index μ at angle i. If the refracted light gets totally polarized, write the relation between the angle i and refractive index μ.   

    Solution
    Relation between the angle 'ip' and refractive index 'μ' is given by, 
                                μ = tan ip
    Question 186
    CBSEENPH12038357

    What is the value of refractive index of a medium of polarizing angle 60°?

    Solution

    Polarizing angle, ip = 60

    Therefore, refractive index of the medium is, 

                        μ = tan ip 

                    μ = tan 60° 

                    μ = 3.

    Question 187
    CBSEENPH12038358

    In a single slit diffraction experiment, the width of the slit is halved. How does it affect the size and intensity of the central maximum?

    Solution
    Size of central maximum  λa
    When, width of the slit is halved, size becomes double and intensity reduces to one-fourth.  
    Question 188
    CBSEENPH12038359

    If the angle between the pass axis of polarizer and the analyser is 45°, write the ratio of the intensities of original light and the transmitted light after passing through the analyser.

    Solution

    Given,
    Angle between pass axis of polarizer and analyser, θ = 45° 

    Using formula,
                              I = I0 cos2θ 

                         I = I0(cos 45°)2 

                          I =I0122 

                          II0 = 12 

    i.e.,                    I : I0 = 1:2. 

    is the required ratio of intensities of original light and transmitted lightafter passing through the analyzer. 

    Question 189
    CBSEENPH12038360

    How does the angular separation of interference fringes change, in Young's experiment, if the distance between the slits is increased?

    Solution
    Angular seperation of interference fring is given by, 

                          ω = λDd 

    Therefore, when separation between slits (d) is increased, then fringe width 'ω' is decreased since, they have an inverse dependence. 
    Question 190
    CBSEENPH12038361

    How does the fringe width of interference fringes change, when whole apparatus of Young's experiment is kept in a liquid of refractive index 1.3?

    Solution
    The fringe width in a Young's double-slit experiment is given by
     
                                 ω =λDd 

    The fringe width is not affected if the whole apparatus is placed in a liquid of refractive index 1.3.
    Question 191
    CBSEENPH12038362

    A ray of light falls an a transparent slab of μ = 1.732. If reflected and refracted rays are mutually perpendicular, what is the angle of incidence?

    Solution
    Refractive index of transparent slab, μ = 1.732 
    Reflected rays and refracted rays are mutually perpendicular to each other. 

    Using formula,

                              tan ip = μ 

                          tan ip = 1.732 

                                ip = tan-1(1.732)     = tan-1(3) 

    i.e.,                           ip = 60°.
    Question 192
    CBSEENPH12038363

    How does the resolving power of telescope change when the aperture of the objective is increased?

    Solution
    When the aperture of the objective lens is increased, the resolving power of telescope increases. 
    Question 193
    CBSEENPH12038364

    The monochromatic source of light in Young's double-slit experiment is replaced by another monochromatic source of shorter wavelength. What will be the effect?

    Solution
    When the monochromatic source of light is replaced by another monochromatic source of light of shorter wavelength, both the fringe width and the angular separation decreases as per the formula given below. 
                             ω = d. 
    Here, ω is the angular seperation, 
    λ is the wavelength of light.
    Question 194
    CBSEENPH12038365

    State the path difference between two waves for destructive interference.

    Solution
    For destructive interference path difference is given by,
                         = (2n+1)λ/2 

    where, n = 0,1, 2... so on. 
    Question 195
    CBSEENPH12038366

    Why cannot we obtain interference using two independent sources of light?

    Solution
    For interference to take place, we need two coherent sources. In case of two independent sources of light, they cannot be coherent, as their relative phases are changing randomly.
    Question 196
    CBSEENPH12038367

    Why bubbles of colourless soap solution appear coloured in sunlight?

    Solution
    The bubbles of colourless soap solution appear coloured in sunlight due to the interference of white light from the thin film of soap bubbles.
    Question 197
    CBSEENPH12038368

    What will be the effect on the fringes, if Young's double-slit experiment set up is immersed in water?

    Solution
    If the young's double slit experiment set-up is immersed in water, then the fringes become narrower.
    Question 198
    CBSEENPH12038369

    Is the speed of light in glass independent of the colour of light?

    Solution
    No. The refractive index and hence the speed of light in a medium depends on the wavelength of the light .
    Question 199
    CBSEENPH12038370

    The phase difference between two waves reaching a point is π/2. What is the resultant amplitude,  if the individual amplitudes are 3 mm and 4 mm?

    Solution
    Amplitude of first wave, a = 3 mm 
    Amplitude of second wave, b = 4 mm  

    The formula for resultant amplitude is given by, 
    R = a2+b2+2ab cos π/2 

    Therefore,
     
    R = 32+42+2×3×4×0           (cos π/2 = 0)   = 2 5   = 5 mm
    Question 200
    CBSEENPH12038371

    What is the relation of a wavefront with a ray of light?

    Solution
    Ray of light is always normal to the wavefront.
    Question 201
    CBSEENPH12038372

    What is the ratio of slit widths when amplitudes of light waves from them have a ratio 2:1.

    Solution
    Given, ratio of amplitude of light waves = 2: 1 

    Therefore,
                       ω1ω2 = I1I2  =a2b2 

                   ω1ω2 = 212 = 21 

    i.e.,          ω1:ω2 = 2:1. 

    So, the slit widths are in the ratio of 2:1.
    Question 202
    CBSEENPH12038373

    What is a polaroid?

    Solution
    Polaroid is a thin and large sheet made of crystalline polarising material, which produces plane polarised beam of light.
    Question 203
    CBSEENPH12038374

    Which three phenomena establish the wave nature of light?

    Solution
    Interference, diffraction and polarisation of light establishes the wave nature of light.
    Question 204
    CBSEENPH12038375

    How does the resolving power of microscope change on (i) decreasing wavelength of light, (ii) decreasing diameter of objective lens.

    Solution
    Resolving power,
    (i) increases on decreasing the wavelength of light,and
    (ii) decreases on decreasing the diameter of objective lens.
    Question 205
    CBSEENPH12038376

    Monochromatic light from a narrow slit illuminates two narrow slits 0.3 mm apart, producing an interference pattern with bright fringes 1.5 mm apart on a screen 75 cm away. Find the wavelength of the light. How will the fringe width be altered if (a) the distance of the screen is doubled and (b) the separation between the slits is doubled?

    Solution

    Here,
    Distance between the slits, d = 0.3 mm = 0.3 × 10-3 m
    Fringe width, β = 1.5 mm = 1.5 × 10-3 m
    distance between screen and the slit, D = 7.5 cm = 0.75 m 

    Wavelength λ is given by
                                β = λDd 

    i.e.,                       λ = βdD
               λ = 1.5 × 10-3×0.3 × 10-30.75   = 6000 × 10-10m = 6000 Å 


    (a) Fringe width is given by, β = λDd

    when D is doubled, fringe width β is also doubled. 

    i.e.,  β = 1.5 × 2 = 3.0 mm 

    (b) When d is doubled, β is reduced to half. 

    i.e.,      β = 1.52 = 0.75 mm.

    Question 206
    CBSEENPH12038377

    In Young's double-slit experiment, monochromatic light of wavelength 600 m illuminates the pair of slits and produces an interference pattern in which two consecutive bright fringes are separated by 10 mm. Another source of monochromatic light produces the interference pattern in which the two consecutive bright fringes are separated by 8 mm. Find the wavelength of light from the second source.
    What is the effect on the interference fringes if the monochromatic source is replaced by a source of white light?

    Solution

    Here, we are given young's double slit experiment.
    Wavelength of monochromatic light, λ1 = 600 nm = 600 × 10-9 m
    Fringe width, β1 = 10 mm = 10 × 10-3 m
    Fringe width, β2 = 8 mm = 8 × 10-3 m 

    Let d be the slit width and D the distance between slit and screen, then we have 

    Fringe width due to first source, β1 = λ1Dd  and,Fringe width due to second source, β2  = λ2Dd 

      β1β2 = λ1Ddλ2Dd 


      β1β2 = λ1λ2 

      10 × 10-38 × 10-3 = 600 × 10-9λ2 

      108 = 600 × 10-9λ2

    i.e., λ2 = 8 × 600 × 10-910 = 480 × 10-9 m
              = 480 nm. 

    is the required wavelength of light from the second source.

    If the monochromatic source is replaced by white light, then we will not be able to see the interference fringes because white light is not a coherent source of light. The condition for interference to take place is, the availabilty of coherent sources of light. 

    Question 207
    CBSEENPH12038378

    In a Young's double-slit experiment, the two slits are kept 2 mm apart and the screen is positioned 140 cm away from the plane of the slits. The slits are illuminated with light of wavelength 600 nm. Find the distance of the third bright fringe, from the central maximum, in the interference pattern obtained on the screen.
    If the wavelength of the incident light were changed to 480 nm, find out the shift in the position of third bright fringe from the central maximum. 
    If the wavelength of the incident light were changed to 480 nm, find out the shift in the position of third bright fringe from the central maximum.  

    Solution

    We have Young's double slit experiment. 
    Distance between the slits, d = 2 mm = 2 × 10-3 m
    Distance between the slit and the screen, D = 140 cm = 1.40 m
    Wavelength of the monochromatic source of light, λ = 600 nm = 600 × 10-9m = 6 × 10-7
    m
    Position of bright fringes is given by, 

                  xn = Dd 

    Here, we are considering the third fringe.

    ∴ Distance of the third bright fringe is, 
               x3 = 3λDd
           x3 = 3×6×10-7×1.402 × 10-3
                   = 12.6 × 10-4 = 1.26 × 10-3 m= 1.26 mm  

    If the wavelength of incident light is changed to 480 nm, then
     λ = 480 nm = 480 × 10-9 = 4.8 × 10-7m 

    Distance of the third bright fringe is

                x3 = 3λDd     = 3 × 4.8 × 10-7 × 1.402 × 10-3     = 10.08 × 10-4      = 1.008 × 10-3m     = 1.01 × 10-3m      = 1.01 mm. 

     Shift in the position of third bright fringe when there is a change in wavelngth,
            = 1.26 - 1.01 = 0.25 mm.

    Question 208
    CBSEENPH12038379

    When one of the slits in Young’s experiment is covered with a transparent sheet of thickness 3.6 × 10-3 cm the central fringe shifts to a position originally occupied by the 30th bright fringe. If λ = 6000Å, find the refractive index of the sheet.

    Solution
    We, are considering young's double slit experiment. 
    Wavelength of the monochromatic source, λ = 6000 A o= 6000 × 10-10 m 
    Thickness of the transparent sheet, t = 3.6 × 10-3 cm 
    refractive index of the sheet, μ = ? 

    The position of the 30th bright fringe is given by,  xn =nλDd 
     
    i.e., x30 = 30λDd 

    Shift of the central fringe is, x0 = 30λDd

    But, we have  x0 =Dd(μ-1)t 
    where, D is the distance between the screen and slit.
    d is the distance between slits.

     30λDd = Dd(μ-1)t
     (μ-1) = 30λt                   =30 × 6000 × 10-103.6 × 10-5                   = 0.5 

    i.e.,     μ =1+0.5   =1.5 

    is the required refractive index of the sheet.

    Question 209
    CBSEENPH12038380

    What are coherent sources? How does the width of interference fringes in Young’s double-slit experiment change when
    (a) the distance between the slits and screen is decreased?
    (b) frequency of the source is increased?
    Justify your answer in each case. 

    Solution
    Two sources which produce waves of same frequency and the phase difference of produced waves does not change with time i.e., they have zero or constant phase difference. These sources are said to be coherent sources. 

    Fringe width in young's double slit experiment is given by, β = d = Dd.cv              c =  
    where, 
    D is the distance between the screen and the slit and, 
    d is the distance between the slits.

    (a) Since, fringe width (β) has a direct dependence on D, fringe width decreases if the distance between the slits and screen is decreased. 

    (b) The fringe width decreases if, the frequency (ν) of the source is increased because, fringe width and frequency have inversely dependent on each other.

    Question 210
    CBSEENPH12038381

    In a single slit diffraction experiment, a slit of width 'd' is illuminated by red light of wavelength 650 nm. For what value of 'd' will
    (i)    the first minimum fall at an angle of diffraction of 30°, and
    (ii)    the first maximum fall at an angle of diffraction of 30°?

    Solution
    Given, width of the slit is 'd'. 
    Wavelength of red light, λ = 650 nm = 650 650 × 10-9 m  

    (i) Angle of diffraction, θ = 30o (given) 

    For, first minimum fall

                             λ = d sin θ   or,  = d sinθ 

                       650 = d sin 30°
                        650 = d × 12
    i.e.,                       d = 1300 nm. 

    (ii) For, first maximum fall at the same angle of diffraction, 
                     (2n+1) λ2 = d sin θ 

    i.e.,                       3λ = 2d sin θ

                   3 × 650 = 2d sin θ                  = 2d sin 30° 

                       1950 = 2d × 12
    i.e.,                        d =1950 nm.
    Question 211
    CBSEENPH12038382

    Two sources of intensity I and 4I are used in an interference experiment. Find the intensity at a point where the waves from the two sources superimpose with a phase difference of (i) zero (ii) π/2 (iii) π.

    Solution
    Given, two sources with interference I and 4I respectively. 

    In case of interference,
                       I = I1+I2+2I1I2  cosϕ 

    (i) When phase difference, ϕ = 0 then, cos ϕ = 1 

                I = 4I + I + 24I × I × 1 = 9I 

    (ii) When phase difference, ϕ = π/2,  cos ϕ = 0 

               I = 4I + I + 24I×I× 0 = 5I 

    (iii) when phase difference, ϕ = π,  cos ϕ = -1 

               I = 4I +I +24I × I × (-1) = I.
     
    Question 212
    CBSEENPH12038383

    (a) A ray of light is incident on a glass surface at an angle of 60°. If the reflected and refracted rays are perpendicular to each other, find the refractive index of glass.
    (b) What is the value of the refractive index of a medium of polarizing angle 60°.

    Solution
    Given that, a ray of light is incident on a glass surface.
    Angle of incidence, i = 60o
    Since, reflected and refracted light rays are perpendicular to each other, we will have angle of incidence equal to polarizing angle.

    Now, using the formula, 
    μ = tan ip    

    ip = 60°
                  μ = tan 60° 
                   μ = 3

    i.e.,             μ = 1.732 is the value of refractive index of the medium. 
    Question 213
    CBSEENPH12038384

    A slit of width 3 mm is illuminated by light of λ= 600 nm at normal incidence. If the distance of the screen from the slit is 60 cm, calculate the distance between the first order minimum on both sides of central maximum.

    Solution

    Given,
    Distance between the slits, d = 3 mm = 3 × 10-3 m
    Wavelength of light, λ = 600 nm = 6 × 10-7 m
    Distance between the slit and the screen, D = 60 cm = 0.60 m 

    Distance of first order minima from central maximum is,  
                         xn = nλDdx1 = 1 × λDd 

    Therefore, distance between first order minimum on both sides of the central maximum is, 

                      2x1 = 2λDd
                  2x1 = 2 × 6 × 10-7 × 0.63 × 10-3
                            = 0.24 × 10-3 m or 0.24 mm.

    Question 214
    CBSEENPH12038385

    How is a wavefront defined? Using Huygen's construction draw a figure showing the propagation of a plane wave reflecting at the interface of the two media. Show that the angle of incidence is equal to the angle of reflection. 

    Solution

    A wavefront is an imaginary surface over which an optical wave has a constant phase. The shape of a wavefront is usually determined by the geometry of the source. 

    Huygen's principle:

    (i) Every point on a given wavefront acts as a fresh source of secondary wavelets which travel in all directions with the speed of light.
    (ii) The forward envelope of these secondary wavelets gives the new wavefront at any instant. 

    Laws of reflection by Huygen's principle
    Let, PQ be reflecting surface and a plane wavefront AB is moving through the medium (air) towards the surface PQ to meet at the point B.
     

    Let, c be the velocity of light and t be the time taken by the wave to reach A' from A. 
    Then,  AA' = ct.

    Using Huygen's principle, secondary wavelets starts from B and cover a distance ct in time t and reaches B'.

    To obtain new wavefront, draw a circle with point B as centre and ct (AA' = BB') as radius. Draw a tangent A'B' from the point A'. 

    Then, A'B' represents the reflected wavelets travelling at right angle. Therefore, incident wavefront AB, reflected wavefront A'B' and normal lies in the same plane.

    Consider ∆ABA' and B'BA'
    AA' = BB' = ct       [∵ AA' = BB' = BD = radii of same circle]
    BA' = BA'              [common]
    ∠BAA' = ∆BB'A'     [each 90°]
    ∴ ∆ABA' ≅ ∠DBA'    [by R.H.S]
    ∠ABA' = ∠B'A'B    [corresponding parts of congruent triangles] 

    ∴ incident angle i = reflected angle r
    i.e.,                 ∠i = ∠r





    Question 215
    CBSEENPH12038386

    Find the maximum intensity in case of interference of n identical waves each of intensity Io if the interference is
    (i) coherent                     (ii) incoherent

    Solution
    Given, n identical waves, each of intensity I

    (i) In case of two coherent sources, resultant intensity is given by, 
                 IR = I1+I2+2I1I2 cos ϕ 

    IR will be maximum when, 
                cos ϕ = 1 (maximum) 

    So for n identical waves each of intensity I0,

                (Imax) = I1+I2+2I1I2 

                   (Imax) = I0+I0......2
                              = I1+I22  
                              = nI02= n2I0 

    (ii) In case of incoherent sources, resultant intensity is given by, 

                   IR = I+ I2 + ............
                       = I0 + I+ .............
                       = nI0.
    Question 216
    CBSEENPH12038387

    In Young's double-slit experiment using monochromatic light the fringe pattern shifts by a certain distance on the screen when a mica sheet of refractive index 1.6 and thickness 1.964 microns is introduced in the path of one of the interfering waves. The mica sheet is then removed and the distance between the plane of the slits and the screen is doubled. It is found that the distance between the successive maximum now is the same as the observed fringe shift upon the introduction of mica sheet. Calculate the wavelength of the light.

    Solution
    Given, a mica sheet is introduced in between the path of the interfering waves.
    Refractive index of the mica sheet, μ = 1.6 
    Thickness of the mica sheet, t = 1.964 microns = 1.964 × 10-6 m

    Due to introduction of mica sheet, the shift on the screen is, 
                        Y0 = Dd(μ -1)t

    Now, when the distance between the plane of slits and screen is changed from D to 2D, fringe width will become, 

                          β= 2Dd(λ) 

    According to given problem, 

                    β = λ( 2D)d = 2 λDd   

    and,          (μ-1) t . Dd = 2λ Dd 

                                λ = (μ-1)t2
                                        = (1.6-1) × 1.964 × 10-62= 5892 Å

    is the required wavelength of the light. 
    Question 217
    CBSEENPH12038388

    The maximum intensity in Young's double-slit experiment is I0. Distance between the slits is d = 5λ, where λ is the wavelength of monochromatic light used in the experiment. What will be the intensity of light in front of one of the slits on a screen at a distance D = 10d?

    Solution

    Given, 
    Maximum intensity = Io
    Distance between the slits, d = 5λ 
    Distance of screen from the slit, D = 10d 

    Using the formula,
    Path difference, x = ydD
    Here,                         y = d2 = 5λ2 (as d = 5λ) and,D = 10d = 50λ 

    So, 
            x = 5λ2 5λ50λ = λ4 

    Corresponding phase difference will be

                  ϕ = 2πλ(x)       = 2πλ λ4

                     = π/2

    i.e.,      ϕ2 = π4

     Intensity of light, I = I0 cos2ϕ2 

                                    I = I0cos2π4 = I02.

    Question 218
    CBSEENPH12038389

    State two conditions to obtain sustained interference of light.
    In Young's double-slit experiment, using light of wavelength 400 nm, interference fringes of width 'X' are obtained. The wavelength of light is increased to 600 nm and the separation between the slits is halved. If one wants the observed fringe width on the screen to be the same in the two cases, find the ratio of the distance between the screen and the plane of the interfering sources in the two arrangements.

    Solution

    Condition for sustained interference are: 

    (i) The two sources of light should emit light continuously.
    (ii) The two waves must be in same phase or bear a constant phase difference. 

    Wavelength of light, λ = 400 nm.
    Width of interference fringes = x

    Fringe width in first case is,
                         β = d   

    i.e.,                X = D × 400d 

    In the second case, 
    Wavelength of light = 600 nm 
    Distance between the slits = d/2 

    Since, fringe width in second case is given to be the same, we have 

               β = D' × 600d/2 = D' × 1200d 

    Therefore, the ratio of the distance between the screen and the plane of interfering sources n the two arrangements is given as, 

                 D × 400d=  D' × 1200d 

                      DD' = 31

    i.e.,               D:D' = 3 : 2.

    Question 219
    CBSEENPH12038390

    Why is interference pattern not detected, when two coherent sources are far apart?
    In Young’s experiment, the width of the fringes obtained with light of wavelength 6000 Å is 2.0 mm. Calculate the fringe width if the entire apparatus is immersed in a liquid medium of refractive index 1.33.    

    Solution

    The fringe width will be very small (almost negligible) and fringes will not be separately visible if the separation between the two coherent sources is large.

    Given, 
    Fringe width, β = 2 mm 
    Wavelength of light used, λ = 6000 Ao 

    Formula for fringe width in air,   β = d 

    Fringe width in liquid is, β' = Dλ'd = Dλdμ

    Refractive index of the medium, μ = 1.33  (given)

    Therefore,
                                β' = βμ 

    i.e.,                      β' = 2.01.33 = 1.5 mm.

    Question 220
    CBSEENPH12038391

    Two wavelengths of sodium light 590 nm, 596 nm are used, in turn, to study the diffraction taking place at a single slit of aperture 2 × 10-6 m. The distance between the slit and the screen is 1.5 m. Calculate the separation between the position of first maximum of the diffraction pattern obtained in the two cases. 

    Solution
    Wavelength of first sodium line, λ1 = 590 nm
    Wavelength of second sodium line, λ2 = 596 nm
    Aperture or width of single slit, d =  2 × 10-6 m
    Distance between the slit and the screen , D = 1.5 m

    Separation between the first secondary maximum in the two cases is,

                           x2-x1 = 322d-321d

                      x2-x1 = 3D2d(λ2-λ1) 

    x2-x1 = 3 × 1.52 × 2 × 10-6 (596 × 10-9 - 590 × 10-9)

                      x2-x1 = 3 × 1.5 × 6 × 10-34 

                                     = 6.75 × 10-3m = 6.75 mm.
    Question 221
    CBSEENPH12038392

    In Young's double-slit experiment dD = 10-4 (d = distance between slits, D = distance of screen from slits). At a point P on the screen resulting intensity is equal to the intensity due to individual slit I0. Find the distance of point P from the central maximum. (λ = 6000Å).

    Solution
    Given,
    Ratio of slit width to distance between the screen and slit, dD = 10-4 
    Wavelength of the light source, λ = 6000 Ao 
    and also, 
    Resultant intensity is equal to the intensity due to individual slit Io

    This implies, 
                     I = 4I0 cos 2(ϕ/2) 

    i.e.,          I0 = 4I0 cos2(ϕ/2) 

                cos(ϕ/2) = 1/2 

                      ϕ/2 = π/3 or, 

                              ϕ = 2π3
    and,
    Relation between phase difference and path difference is,
                             ϕ = 2πλ. x 

    or,                  2π3 = 2πλydD        x = ydD
                          Y = λ3 × d/D

                         γ = 6 × 10-73 × 10-4   = 2 × 10-3m 

                             γ = 2 mm. 

    Therefore, the distance of point P (on the screen) from the central maximum is 2 mm .
    Question 222
    CBSEENPH12038393

    Two coherent light sources of intensity ratio 25 : 4 are employed in an interference experiment what is the ratio of the intensities of the maxima and minima in the interference pattern?

    Solution
    Let I1 and I2 be the intensities of the two coherent beams and A1 and A2 their respective amplitudes.

    Now given, 
    Intensity ratio, I1I2 = 254, 
    therefore,
                          A1A2 = I1I2 

    Amplitude ratio , A1A2 = 254 = 52 

    i.e.,                      A1 = 5 units and, 
                                A2 = 2 units

    At maxima: Amax = A1+A2 = 7 units At minima: Amin   = A1-A2 = 3 units 

    Hence,
                              ImaxImin = Amax2Amin2 

                           ImaxImin = (7)2(3)2 

                     Imax : Imin = 49 : 9  

    is the ratio of intensities of the maxima and minima in the interference pattern.
    Question 223
    CBSEENPH12038394

    What are polaroids? How are they used to demonstrate that (i) light waves are transverse in nature, (ii) if an unpolarized light wave is incident then light waves will get linearly polarized?

    Solution

    Polaroid is a thin and large sheet made of crystalline polarizing material which is used to produces plane polarized beam of light. 

    (i) Polaroids can be used to demonstrate the transverse nature of light waves.

    • The electric field, associated with propagation of light waves is always perpendicular to the direction of propagation of the wave.
    • If a light wave is incident on the polaroid, the electric vectors assosciated with the propagating wave, along the direction of the aligned molecules get absorbed. 

    (ii) If an unpolarized light wave is incident on a polaroid then, the the light wave will get linearly polarised with the electric vector oscillating along a direction perpendicular to the aligned molecules.

    Question 224
    CBSEENPH12038395

    What is Brewster's angle? When an unpolarized light is incident on a plane glass surface, what should be the angle of incidence so that the reflected and refracted rays are perpendicular to each other?

    Solution

    Brewster's angle:

    The partially reflected light gets partially plane polarized when ordinary light, is allowed to undergo refraction. However, there is an angle of incidence at which, an ordinary light undergoes refraction as well as reflection (partial) and then the partially reflected ray is richly plane polarized. Such an angle is known as polarizing angle or Brewster's angle. It is denoted by ip

    Light can be polarized by reflecting it from a transparent medium. The extent of polarization depends on the angle of incidence. At a particular angle of incidence, called Brewster's angle, the reflected light is completely polarized as shown in the diagram below: 



    When reflected and refracted rays are perpendicular to each other, angle of incidence becomes equal to the polarizing angle. 

                        i = tan-1 μ 

    where, μ is the refractive index of the medium.

    Question 225
    CBSEENPH12038396

    (a) What are coherent sources of light? Two slits in Young's double-slit experiment are illuminated by two different sodium lamps emitting light of the same wavelength.
    Why is no interference pattern observed?
    (b) Obtain the condition for getting dark and bright fringes in Young's experiment. Hence write the expression for the fringe width.
    (c) If s is the size of the source and its distance from the plane of the two slits, what should be the criteria for the interference fringes to be seen?

    Solution

    (a) Coherent sources:
    Sources emitting waves of same frequency or wavelength having either zero or a constant phase difference are said to be coherent sources of light. 

    Two independent sources of light do not fulfil the requirement of constant phase difference. Since, the sodium lamps considered here are independent sources of light and are not coherent sources we cannot observe interference pattern. 

    (b) For bright fringes (maxima), 

    Path difference,  xdD = 
                            x = nλDd
    where,  n = 0, 1, 2, 3... so on. 

    For dark fringes (minima),

    Path difference,   xdD = (2n-1) λ/2
                               x = (2n-1) λ2Dd'
    Where n = 0, 1, 2, 3 ...so on. 

    The separation between the centre of two consecutive bright fringes is the width of a dark fringe. 

     Fringe width,    β = xn-xn-1 

                                β = nλDd-(n-1)λDd 

    i.e.,                      β = λDd 

    (c) The condition for interference fringes is to be:
    Sd<λ/d.
    where, 
    s is the source and, 
    d is the distance between the two slits.

    Question 226
    CBSEENPH12038397

    A ray of light incident normally on one of the faces of a right-angled isosceles prism is found to be totally reflected as shown.
    (a)    What is the minimum value of the refractive index of the material of the prism?
    (b)    When the prism is immersed in water trace the path of the emergent ray for the same incident ray indicating the values of all the angles. (μ of water = 4/3).


    Solution

    (a)
    ABC is the section of the prism right angled at B.
    A and C are equal angles i.e., A = C = 45°. 



    The ray PQ is normally incident on the face AB. Hence it is normally refracted and the ray QR strikes the face AC at an angle of incidence 45°.
    It is given that the ray does not undergo refraction but is totally reflected at the face AC. This gives a maximum value for the critical angle as 45°. 
    Therefore,
                           Sin C = sin 45° = 12
    Since,                   μ = 1sin C = 2  

                            μ = 1sin 45° 

    i.e.,                   μmin = 2
    Thus, the minimum value of refractive index = 2. 

    (b) When the prism is immersed in water the critical angle for the glass-water interface is given by
    sin C1 = 4/32 = 432
     C1 =70.53°

    The angle of incidence at R continues to be 45° and obviously, 45° < 70.53°.
    Hence, there is refraction taking place now and the refracted ray is RS.

    The angle of refraction r is given by,
                μ
    g sin i = μw sin r 

     
    Refractive index of water w.r.t glass is, 

                    g μω = sin isin r

                     μωμg = sin isin r 

           2 sin 45° = 43 sin r 

                     sin r = 324sin 45° 

                            = 324×12 = 34
    i.e.,                r =sin-134 = 48°36' 
    The angle of refraction in water = 48°36'.

    Question 227
    CBSEENPH12038398

    What is interference of light? Write two essential condition for sustained interference pattern to be produced on the screen.
    Draw a graph showing the variation of intensity versus the position on the screen in Young's experiment when (a) both the slits are opened and (b) one of the slit is closed.
    What is the effect on the interference pattern in Young's double-slit experiment when:
    (i) screen is moved closer to the plane of slits?
    (ii) separation between two slits is increased. Explain your answer in each case.

    Solution

    Interference of light:
    The phenomenon of redistribution of light energy in a medium on account of superposition of light waves from two coherent sources is called interference of light.
    Conditions for sustained interference:
    The two essential conditions of sustained interference are as follows:
    (i) The two sources of light should emit light continuously.
    (ii) The light waves should be of same wavelength. (Monochromatic).

    When both the slits are open, we get interference pattern on the screen. Then the following intensity distribution curve is obtained.



    When one of the slits is closed, diffraction pattern is obtained on the screen. The following intensity curve is obtained.


    Fringe width, β = d
    where, 
    D is the distance between the screen and the slit and,
    d is the distance between the slits.

    (i) When screen is moved closer to the plane of slits, D decreases and hence, fringe with of the interference pattern also decreases. 

    (ii) Fringe width β decreases if, separation d between two slits is increased.

    Question 228
    CBSEENPH12038399

    (a) What is plane polarised light? Two polaroids are placed at 90° to each other and the transmitted intensity is zero. What happens when one more polaroid is placed between these two, bisecting the angle between them? How will the intensity of transmitted light vary on further rotating the third polaroid?
    (b) If a light beam shows no intensity variation when transmitted through a polaroid which is rotated, does it mean that the light is unpolarized? Explain briefly.

    Solution
    (a) In plane polarized light, electric field E oscillates back and fourth in one plane perpendicular to the direction of the propagation of light.
    The intensity of polarised light through a polarizer at an angle of ө, is given by I = I0 cos2θ.
    If there are N polaroids placed in between the polarizer and analyzer with equal successive angular separation, then the overall intensity at the analyzer is given by,   I = I0cosπ2N2N

    Hence, the intensity of the polarised light coming out from the analyzer is, 

                              I = I0cosπ42×2     = I0(cos 45°)4   = I024   = I04

    According to law of Malus, when a beam of completely plane polarized light is incident on an analyzer, the resultant intensity of light (I0) transmitted from the analyzer varies directly as the square of the cosine of the angle (ө) between planes of transmission of analyzer and polarizer.

    i.e.,                        I = I0cos2ө.

    The variation of intensity of transmitted light with rotating angle is given. 



    (b) Yes, if a light beam shows no variation when transmitted through a polaroid which is rotated, this means that light is unpolarized. If an unpolarized light from an ordinary source passes through a polaroid sheet P1, it is observed that its intensity is reduced by half. Rotating P1 has no effect on the transmitted beam and transmitted intensity remains constant. Now, let an identical piece of polaroid P2 be placed before P1. The light from the lamp is reduced in intensity on passing through P2 alone. In one position, the intensity transmitted by P2  is nearly zero. When turned by 90° from this position, Ptransmits nearly the full intensity emerging from P2.

     



    Question 229
    CBSEENPH12038400

    What is diffraction of light? Draw a graph showing the variation of intensity with angle in a single slit diffraction experiment. Write one feature which distinguishes the observed pattern from the double-slit interference pattern.
    How would the diffraction pattern of a single slit be affected when:
    (i)    the width of the slit is decreased?
    (ii)    the monochromatic source of light is replaced by a source of white light? 

    Solution

    Diffraction of light:
    Phenomenon of bending of light around the comers of an obstacle or aperture is called diffraction. 

    Variation of intensity with angle in a single slit diffraction experiment is as shown below :


    In interference, all the bright fringes are of the same intensity whereas, in diffraction phenomenon, the intensity of bright fringes decreases as the distance from the central bright fringe increases.

    (i) The diffraction pattern of a single slit becomes narrower if the width of the slit is decreased. 

    (ii) A coloured diffraction pattern is obtained if monochromatic source is replaced by white light source. The red fringe will be wider than the violet fringe because, the central band is white.

    Question 230
    CBSEENPH12038401

    A narrow monochromatic beam of light of intensity I is incident on a glass plate A as shown in (Fig. a). Another identical glass plate B is kept close to A and parallel to it. Each glass plate reflects 25% of the light intensity incident on it and transmits the remaining. Find the ratio of the minimum and maximum intensities in the interference pattern formed by the two beams obtained after one reflection at each plate.

    Solution


    A beam of light of intensity I is incident on plate A. Since the plate reflects 25% of I, the intensity of the reflected beam I (see Fig. b) is 

                     I1 = I × 25100 = I4 

    The remaining intensity 3I/4 falls on plate B which reflects 25% of the intensity incident on it. Hence, intensity of beam reflected from B is
                     3 I4× 25100 = 3 I16 

    A beam of intensity 3 I/16 falls on plate A which transmits 75% of this intensity. Hence the intensity of beam 2 is
                      I2 = 3 I16 ×75100 = 9 I64 

    Now, intensity ∝(amplitude)2.

    If a
    1 and a2 are the amplitudes of beam 1 and 2 respectively, then 

                         I1 = ka12  and I2 = ka22

                a12a22 = I1I2 = I/49I/64 = 169

                 a1a2 = 43 

    i.e.,              a1 = 4 units and a2 = 3 units. 

    The resultant amplitude at maxima = a1 + a2 and at minima = a- a2

    Therefore, the ratio of the intensities at maxima and minima of the interference pattern is 

    ImaxImin = a1+a2a1-a22 = 4+34-32 = 49:1

             

    Question 231
    CBSEENPH12038402

    Two convex lens of same focal length but their aperture and focal lengths 5 cm and 10 cm are used as object lens in two astronomical telescope.
    (a)   What will be the ratio of their
    (i)     resolving power
    (ii)    magnifying power
    (b)   Compare the intensity of images formed in these cases.

    Solution
    Given, two convex lens of same focal length.
    Aperture of the first lens, D1 = 5 cm 
    Aperture of second lens, D2 = 10 cm

    (i) Ratio of resolving power is, 
     D11.22 λD21.22 λi.e.,  D1D2 = 510 = 12 

    (ii) Ratio of magnifying power is given by,
     f0fe1f0fe2 = f01(f0)2 = 510 = 12 

    (b) Intensity of image is directly proportional to the size of aperture hence, it will also have a ratio of 12.
    Question 232
    CBSEENPH12038403

    The ratio of the intensities at minima to maxima in the interference pattern is 9 : 25. What will be the ratio of the widths of the two slits in the Young's double-slit experiment?

    Solution
    Given,
    Ratio of intensities at minima to maxima = 9:25 

    Intensity is proportional to width of slit.

    So, amplitude a
    1 and a2 is proportional to the square root of the width of the slit.
                         a1a2 = ω1ω2
    Here ω1 and ω2 represent the widths of the two slits. 

    Now, we have

    IminImax = (a1-a2)2(a1+a2)2 = 1-a2a121+a2a12 

                               925 = 1-a2a121+a2a12                     35 = 1-a2a11+a2a1 

                     8a2a1 =2

                      a1a2 = 4 

    Thus,           ω1ω2 = 41 

    i.e.,             ω1ω2 = 161     ω1:ω2 = 16 : 1.



    Question 233
    CBSEENPH12038404

    In a double-slit experiment, two coherent sources have slightly different intensities I and (I + δI), such that δ << I, show that resultant intensity at maxima is near 4I, while that at minima is nearly (δl)2/4l.

    Solution

    Given, Young's double slit experiment with two coherent sources.
    Intensity of first source, I1 = I 
    Intensity of second source, I2 = I + δI

    Now, using the formula for resultant intensity,  

    For maxima,

                  I = I1+I2+2I1I2cos ϕ 

              Imax = I1+I2+2I1I2cos0°        = I+(I+δI)+2(I(I+δI) 

    As δI<<I, therefore,  

              Imax = I+I+2I = 4I 

    For minima, 

                       I = I1+I2+2I1I2 cos ϕ 

                   Imin = I+(I+δI) + 2I(I+δI) cos 180° 

                   Imin = 2I + δI - 2I1+δII1/2
                          = 2I + δI - 2I1+12δII+1212-12δII2
                                
                        = 2I + δI - 2I - δI + 14 I δII2
              Imin = δI24I. 

    Hence proved.
             

    Question 234
    CBSEENPH12038405

    A double-slit is illuminated by light of wavelength 6000A. The slits are 0.1 cm apart and the screen is placed 1 m away. Calculate (i) angular position of 10 th maximum in radian (ii) separation of two adjacent minima.

    Solution
    Given , 
    Wavelength of the light source, λ = 6000 Ao 
    Distance between the slits, d = 0.1 cm = 0.1 × 10-2 m 
    Distance between the screen and the slit, D = 1 m

    (i) Angular position of nth maximum is given by, 

                              θn = xnD = nDλdD = d                                        χn = nDλd 

    Angular position of 10th maximum, 

                 θ10 = 10 × 6000 × 10-100.1 × 10-2       = 6 × 10-3 radian 

    (ii) Separation between two adjacent minima 

    i.e., fringe width, ω = d
                          ω = 1 × 6000 × 10-1010-3 
                                  = 6 × 10-4m = 0.6 mm.
     
    Question 235
    CBSEENPH12038406

    In a Young's experiment, the width of the fringes obtained with light of wavelength 6000A is 2.0 mm. What will be the fringe width, if the entire apparatus is immersed in a liquid of refractive index 1.33?

    Solution
    Given, 
    Width of fringes, ω = 2 × 10-3m Wavelength of light used, λ = 6000 Å = 6 × 10-7m 

    The formula for fringe width is,
                        ω = d
                   Dd = ωλ = 2 × 10-36 × 10-7 = 13 × 104 

    When the apparatus is immersed in liquid 

    Wavelength, λ' = λμ  = 6 × 10-71.33m

    Fringe width, ω' = Ddλ' 

                    ω' = 13× 104 × 6 × 10-71.33m
                             = 1.5 × 10-3 m = 1.5 mm.

    Question 236
    CBSEENPH12038407

    A beam of light consisting of two wavelengths 6500 A and 5200 A, is used to obtain interference fringes in a Young's double-slit experiment.
    (i) Find the distance of the third bright fringe on the screen from the central maximum for wavelength 6500 A.
    (ii) What is the least distance from the central maximum where the bright fringes due to both the wavelengths coincide?
    The distance between the slits is 2 mm and the distance between the plane of the slits and the screen is 120 cm.

    Solution
    Given, 
    Wavelength, λ1 = 6500 Ao
    Wavelength, λ2 = 5200 Ao 

    (i) The distance of the mth bright fringe from the central maximum is given by 

                    ym = mλDd 

                 y3 = 3λDd     = 3 × 6500 × 10-10 × 1.202 ×10-3
                       = 1.17 × 10-3m = 1.17 mm 

    (ii) Let, the nth bright fringe of wavelength λn and the mth bright fringe of wavelength λcoincide at a distance y from the central maximum, then
                     y = mDd = nDd
    i.e.,        mn = λnλm= 65005200= 54 

    The least integral value of m and n which satisfy the above are m = 5 and n = 4 

    i.e., the 5th bright fringe of wavelength 5200 A0coincides with the 4th bright fringe of wavelength 6500 Ao.

    The smallest value of y at which the bright fringes coincides is, 

    ymin = mDd = 5 × 5200 × 10-10 × 1.202 × 10-3         = 1.56 × 10-3m = 1.56 mm.
    Question 237
    CBSEENPH12038408

    How would the angular separation of interference fringes in Young’s double-slit experiment change when the distance of separation between slits and screen is doubled?

    Solution

    In young's double slit experiment,
    Angular separation is given by,
                θ = βD = λd.           fringe width β = λDd 

    Angular seperation does not depend on D i.e., the distance of separation between slits and screen. Therefore, θ remains unaffected.

    Question 238
    CBSEENPH12038409

    How is resolving power of a microscope affected when (i) wavelength of illuminating radiations is decreased (ii) the diameter of objective lens is decreased? Justify.

    Solution
    For a microscope,
     
                Resolving power = 2μ sin θλ 

    (i) When λ is decreased, resolving power increases. 

    (ii) When diameter of objective lens is decreased, ө decreases, sinө decreases. Hence resolving power of microscope also decreases.
    Question 239
    CBSEENPH12038410

    In a two-slit experiment with monochromatic light, fringes are obtained on a screen placed at some distance from the slits. If the screen is moved by 5 × 10-2 m towards the slits, the change infringe width is 3 × 10-5 m. If the distance between the slits is 10-3 m, calculate the wavelength of light used.

    Solution

    Given, 
    Change in fringe width, β = 3 × 10-5 m
    Change in distance between the screen and slit, D =  5 × 10-2 m
    Distance between the slits, d = 10-3 m

    Fringe width, β = λdD
    Therefore,
                      β = λdD 

               λ = dβD
               λ = 10-33 × 10-55 × 10-2m   = 6 × 10-7m

    i.e.,         λ = 6 × 10-7 × 1010 Å = 6000Å. is the wavelength of the light used in the experiment.

    Question 240
    CBSEENPH12038411

    In Young's double-slit experiment how many maximas can be obtained on a screen (including the central maximum) on both sides of the central fringe if λ = 2000 Å and d = 7000Å. Given that perpendicular distance of a screen from the mid-point of two slits is 3.5 cm.

    Solution
    For,  
    Wavelength, λ = 2000 Å
    Distance between the slits, d = 7000Å 
    Perpendicular distance of a screen from the mid point of two slits = 3.5 cm

    Maximum intensity on the screen 

                  d sin θ = n λ 

    i.e.,            sin θ = d = n(2000)(7000) = n3.5 

    Since,                            sin θ 1                  n = 0, 1, 2, 3  only 

    Thus, a total of only seven maximas can be obtained on both sides of the screen.
    Question 241
    CBSEENPH12038412

    The intensity at the central maxima (0) in a Young's double slit set up is I0. If the distance OP equals one third of the fringe width of the pattern, show that the intensity, at point P, would equal to I0/4.

    Solution

    Intensity at the central maxima = I
    Distance OP is one-third of the fringe width, x = 13β (given)

    Fringe width is given by λDd

                              x = λD3d

     Path difference, p = xdD  and, 

    Phase difference, ϕ = 2πλ(P) 

                                 = 2π/3
    Intensity at point P, I = I0 cos2 ϕ2

                                    = I0 cos22π3 = I0/4
    Hence proved.

    Question 242
    CBSEENPH12038413

    (a) A plane wavefront approaches a plane surface separating two media. If medium one is (optically) denser and medium two is optically rarer, construct the refracted wavefront using Huygen’s principle.
    (b) Draw the shape of refracted wavefront when a plane wavefront is incident on (i) prism and (ii) convex mirror. Give a brief explanation for the construction.

    Solution
    (a) Construction of refracted wavefront.

     

    (b)
    i) When a plane wave is incident on the prism. 
     
    ii) When a plane wave is incident obn convex mirror.



    Time taken by any disturbance to travel from incident wavefront to the refracted wavefront is same.
    Question 243
    CBSEENPH12038414

    How will the intensity of maxima and minima, in the Young's double experiment change, if one of the two slits is covered by a transparent paper which transmits only half of light intensity?

    Solution
    In young's double slit experiment, if one of the slits is covered by a transparent paper such that, only half of light intensity is transmitted then, the intensity of maxima decreases and the intensity of minima increases.
    Question 244
    CBSEENPH12038415

    In the double slit experiment, the pattern on the screen is actually a superposition of single slit diffraction from each slit and the double slit interference pattern in a double slit pattern. In what way is the diffraction from each slit related to the interference pattern in a double slit experiment? Explain.

    Solution

    The pattern shows a broader diffraction peak in which, there appear several fringes of smaller width, due to the double slit interference phenomenon. 

    The number of interference fringes depends upon the ratio of the distance between the two slits to the width of a slit.

    Question 245
    CBSEENPH12038416

    A slit of width 'd' is illuminated by white light. For what value of 'd' is the first minimum for red light of λ = 650 nm located at point P. For what value of the wavelength of light will the first diffraction maxima also fall at P?

    Solution
    Given, width of the slit = d 
    Wavelength, λ = 650 nm 

    At first minimum, n = 1

    ∴             d sin 30° = nλ
                        d2 = 1 × 650 nm
    i.e.,                    d = 1300 nm 

    For first maxima to be at P
                        d sin θ = 32 λ' 

                          λ' = 2d sin ϕ3     = 2 × 1300 × sin 30°3nm
                                  = 433.3 nm.
    Question 246
    CBSEENPH12038417
    Question 257
    CBSEENPH12038428
    Question 261
    CBSEENPH12038432

    In Young's double slit experiment, three lights of blue, yellow and red colour are used successively. The fringe width will be maximum for which colour of light and why?

    Solution

    In visible spectrum, red light has the greatest wavelength. And, fringe width is directly proportional to the wavelength of light. Therefore, the fringe width will maximum for red light. 

    Question 262
    CBSEENPH12038433

    In the diffraction at a single slit experiment, how would the width and the intensity of central maximum change if (i) slit width is halved (ii) visible light of longer wavelength is used?

    Solution

    In a single slit experiment, 

    As, size of central max  λa
    Therefore, 

    i) When slit width is halved, size of the central maxima is doubled. Hence, intensity reduces to one-fourth of it's initial value. 

    ii) When longer wavelength is used, size of central maximum is increased. Hence, intensity reduces. 

    Question 263
    CBSEENPH12038434

    The light of wavelength 600 nm is incident normally on a slit of width 3 mm. Calculate the linear width of central maximum on a screen kept 3 m away from the slit.

    Solution

    Given, 
    Wavelength of light, λ = 600 nm = 600 × 10-9 m
    Slit width, d = 3 mm = 3× 10-3 m
    Distance of the screen from the slit, D = 3 m 

    Now, 
    Linear width of central maximum = 2d 
                                                       = 2×3×600×10-93×10-3 
                                                       = 1.2 mm

    Question 264
    CBSEENPH12038435

    The polarising, angle of a medium is 60°. What is the refractive index of the medium?

    Solution

    Given, 
    Polarising angle for a medium = 60o 
    Therefore, refractive index of the medium is given by Brewster's law. 

    Thus , 
                         μ = tan ip    = tan 60o    = 3   = 1.732 

    Question 265
    CBSEENPH12038436

    A ray of light goes from medium 1 to medium 2. Velocity of light in the two media are c1 and c2 respectively. For an angle of incidence 0 in medium 1, the corresponding angle of refraction in medium 2 is ө/2.
    (i)    Which of the two media is optically denser and why?
    (ii)    Establish the relationship between ө, c1 and c2.

    Solution

    Given, 

    i) Angle of incidence in medium 1 = θ 
    Angle of refraction in medium 2 = θ2 

    Angle of refraction in medium 2 is less than angle of incidence in medium 1. That is, the ray is bending towards the normal. Therefore, medium 2 is optically denser than medium 1. 

    ii) Using Snell's law, 
         μ = sin isin r = sin θsin θ2 = 2 sin θ2. cos θ2sin θ2 
            =  2 cos θ2

    Also, refractive index μ = c1c2 
    This implies, 
                       μ = 2 cos θ2 = c1c2

    i.e.,              θ = 2 cos-1 c12c2 
    which is the required relationship between ө, c1 and c2 .





    Question 266
    CBSEENPH12038437

    If the angle between the axis of polariser and the analyser is 45°, write the ratio of the intensities of original light and transmitted light after passing through the analyser.

    Solution
    Given , 
    Angle between the pass axis of polariser and analyser = 45o 

    Let, Io be the intensity of original light. Then,  

    Intensity of original light passing through the polariser = Io2 

    Intensity of light passing through the analyser is, 
    I = Io2cos245o 

    ⇒  IoI = 2cos2 45  = 2(12)2=41 
    Thus, ratio of intensities of original light to transmitted light is 4:1.
    Question 267
    CBSEENPH12038438

    What type of wavefront will emerge from a (i) point source, and (ii) distant light source?

    Solution
    i) Spherical wavefronts are emitted for a point source in space. 

    ii) A distant light source often acts as a point source and hence spherical wavefronts will emerge.
    Question 268
    CBSEENPH12038439

    Draw a diagram to show refraction of a plane wavefront incident on a convex lens and hence draw the refracted wavefront.

    Solution



     
    Refracted spherical wavefront emerges out which is converging towards the focus of a lens.



    Question 269
    CBSEENPH12038440

    At what angle of incident rays should a light beam strike a glass slab of refractive index , such that the reflected and the refracted rays are perpendicular to each other.

    Solution

    The reflected and refracted ray is mutually perpendicular to each other at the polarising angle. 

    Therefore, according to Brewster's law , we have
                               iP = tan-1 μ
    where, μ is the refractive index of the medium. 

    Question 270
    CBSEENPH12038441

    Differentiate between a rays and wavefront.

    Solution

    A ray is a line extending outward from the source and representing the direction of propagation of the wave at any point along it. Rays are perpendicular to wave fronts. 

    A wave front is a line representing all parts of a wave that are in phase. The shape of the wave front depends upon the nature of the source; a point source will emit waves having circular or spherical wave fronts, while a large, extended source will emit waves whose wave fronts are effectively flat, or plane.

    Question 271
    CBSEENPH12038442

    Explain both the objective and the eyepiece of a compound microscope must have short focal lengths?

    Solution

    The objective and the eyepiece of a compound microscope must have short focal length so as to have larger angular magnification and magnifying power. 

    Question 272
    CBSEENPH12038443

    Find the
    (a)    maximum frequency, and
    (b)    minimum wavelength of X-rays produced by 30 kV electrons.

    Solution
    Here,
    Voltage, V = 30 kV = 30 x 10
    3V = 3 x 104

    (a) Using the formula,
                             hvmax = eV

                               vmax = eVh        = 1.6 × 10-19×3 × 1046.63 × 10-34Hz 
                                     =7.24 × 1018 Hz 
    is the required maximum frequency.

    (b) Minimum wavelength of x-rays produced, 

                       λmin = cvmax          = 3 × 1087.24 × 1018m
                   λmin = 0.414 × 10-10m        = 0.414 Å 

                             = 0.0414 nm.
    Question 273
    CBSEENPH12038444

    The work function of caesium metal is 2.14 eV. When light of frequency 6 x 1014Hz is incident on the metal surface, photoemission of electrons occurs. What is the maximum kinetic energy of the emitted electrons?

    Solution
    Given,
    Work function of caesium metal = 2.14 eV 
    Frequency of light, ν = 6 x 1014Hz 

    Maximum kinetic energy of the emitted electrons,
           K.E.max = hv-ϕ0               = 6.63 × 10-34 × 6 × 10141.6 × 10-19-2.14 

              Emax = 0.346 eV = 0.35 eV

    Question 274
    CBSEENPH12038445

    The work function of caesium metal is 2.14 eV. When light of frequency 6 x 1014Hz is incident on the metal surface, photoemission of electrons occurs. What is the stopping potential?

    Solution
    Work function of caesium metal = 2.14 eV
    frequency of light wave = 6 x 1014Hz 

    The stopping potential can be calculated as,

                           eV0 = K.E.max 

                         V0 = K.E.maxe      = 0.35 eVe     = 0.35 V
    Question 275
    CBSEENPH12038446

    The work function of caesium metal is 2.14 eV. When light of frequency 6 x 1014Hz is incident on the metal surface, photoemission of electrons occurs. What is the maximum speed of the emitted photoelectrons?

    Solution
    Given, a ceasium metal.
    Work function = 2.14 eV 
    Frequency of light, ν = 6 x 1014Hz 

    Maximum kinetic energy is given by, 
    12mv2max = 0.346 eV = 0.346 × 1.6 × 10-19J 

        vmax = 0.346 × 1.6 × 10-19 × 29.1 × 10-31ms-1 

                   = 3.488 × 105 ms-1= 348.8 km s-1 

    i.e.,   vmax = 349 km s-1. 

    which is the required maximum speed of the photoelectrons. 
    Question 276
    CBSEENPH12038447

    The photoelectric cut-off voltage in a certain experiment is 1.5 V. What is the maximum kinetic energy of photoelectrons emitted?

    Solution
    Given, cut-off voltage, Vo = 1.5 V 

    Maximum kinetic energy of photoelectrons emitted is, 
                      K.E.max = eV0                 = 1.5 × 1.6 × 10-19J                 = 2.4 × 10-19 J
    Question 277
    CBSEENPH12038448

    Monochromatic light of wavelength 632.8 nm is produced by a helium-neon laser. The power emitted is 9.42 mW.
    a.) Find the energy and momentum of each photon in the light beam. 

    b.) How many photons per second, on the average arrive at a target irradiated by this beam?

    c.) How fast does a hydrogen atom have to travel in order to have the same  momentum as that of the photon?

    Solution
    Given,
    Wavelength of monochromatic light, λ = 632.8 nm = 632.8 x 10
    –9 m
     Frequency, v = cλ = 3 × 108632.8 × 10-9Hz 

                                     = 4.74 × 1014Hz

    (a) Energy of a photon, E = hv

                                           = 6.63 × 10-34× 4.74 × 1014J= 3.14 × 10-19J.

    Momentum of each photon, p (momentum) = hλ                            = 6.63 × 10-34632.8 × 10-9                              = 1.05 × 10-27 kg ms-1 

    (b) Power emitted, P = 9.42 mW = 9.42 x 10–3 W
    Now, P = nE  

    This implies, 

    n = PE = 9.42 × 10-3W3.14 × 10-19J                = 3 × 1016 photons/sec. 
    Thus, these many number of protons arrive at the target.

    (c) Velocity of hydrogen atom 

                        = Momentum 'p' of H2 atom (mv)Mass of H2 atom(m) 

                      v = 1.05 × 10-271.673 × 10-27ms-1   

                        = 0.63 ms-1. 
    Thus, the hydrogen atom travel at a speed of 0.63 m/s  to have the same  momentum as that of the photon.
    Question 278
    CBSEENPH12038449

    The energy flux of sunlight reaching the surface of the earth is 1.388 x 103 W/m2. How many photons (nearly) per square metre are incident on the earth per second? Assume that the photons in the sunlight have an average wavelength of 550 nm.

    Solution

    Energy flux of sunlight = Total energy per square metre per second = 1.388 x 103 Wm–2 

    Energy of each photon is given by,

                           E = hcλ 
    Therefore, 
     Power of each photon, P  = nE                                               = 6.63 × 10-34× 3 × 108550 × 10-9J                                              = 3.62 × 10-19J 
    Number of photons incident on earth's surface per square metre per second is, 

    = Total energy per square metre per secondEnergy of one photon 

    = 1.388 × 1033.62 × 10-19 = 3.8 × 1021.

    Question 279
    CBSEENPH12038450

    In an experiment on photoelectric effect, the slope of the cut-off voltage versus frequency of incident light is found to be 4.12 x 10–15 Vs.
    Calculate the value of Planck's constant.

    Solution
    The slope of the cut-off voltage versus frequency of incident light is given as, 

                        Vν = 4.12 × 10-15Vs           = 4.12 × 10-15 J.s.C 

    When we multiply this result with the charge of an electron, which is the fundamental charge (e = 1.6 x 10–19 C) we get, 

                         E = hv
                     h = Ev = J.s.
                     h = 4.12 × 10-15 × 1.6 × 10-19 

    i.e.,                h = 6.592 × 10-34Js. 

    is the value of the planck's constant.
    Question 280
    CBSEENPH12038451

    A 100 W sodium lamp radiates energy uniformly in all directions. The lamp is located at the centre of a large sphere that absorbs all the sodium light which is incident on it. The wavelength of the sodium light is 589 nm. (a) What is the energy per photon associated with the sodium light? (b) At what rate are the photons delivered to the sphere?

    Solution

    Given,
    Power, P (power) = 100 W
    Wavelength of sodium light, λ = 589 x 10–9 m 

    (a) Energy of each photon assosciated with the sodium light,
                    E = hv = hcλ    =6.63 × 10-34 × 3 × 108589 × 10-9J 

               E = 3.38 × 10-19J 

    (b) Number of photons delivered to sphere per second, 
    As,              P= nE

                     n = Energy radiated per secondEnergy of each proton     

                     n = 1003.38 × 10-19    = 3 × 1020 photon/s.

    Question 281
    CBSEENPH12038452

    The threshold frequency for a certain metal is 3.3 x 1014 Hz. If light of frequency 8.2 x 1014 Hz is incident on the metal, predict the cut-off voltage for the photoelectric emission.

    Solution
    Given,
    Threshold frequency, v
    0 = 3.3 x 1014 Hz
    Frequency of light, v = 8.2 x 10
    14 Hz
    Planck's constant, h = 6.63 x 10
    –34 Js

    Using Einstein's photoelectric equation,
               12mv2max = h(v-v0) = eV0

                      V0 = h(v-v0)e
                      V0 = 6.62 × 10-341.6 × 10-19(8.2 × 1014 - 3.3 × 1014) 

    i.e.,                V0 = 2.03 V. 

    is the required cut=off voltage for photoelectric emission.
    Question 282
    CBSEENPH12038453

    The work function for a certain metal is 4.2 eV. Will this metal give photoelectric emission for incident radiation of wavelength 330 nm?

    Solution
    Work function of the metal, ɸ0 = 4.2 eV
                                                   = 4.2 x 1.6 x 10
    –19 J
                                                   = 6.72 x10
    –19 J 
    Wavelength of incident radiation, λ = 330 nm 

    Now, using the formula for energy of a photon, E = hcλ

           E = 6.62 × 10-34 × 3 × 108330 × 10-9        = 6.018 × 10-19J 

    As energy of incident photon E < ɸ0, hence no photoelectric emission will take place.
    Question 283
    CBSEENPH12038454

    Light of frequency 7.21 x 1014 Hz is incident on a metal surface. Electrons with a maximum speed of 6.0 x 105 m/s are ejected from the surface. What is the threshold frequency for photoemission of electrons?

    Solution

    Given,
    Frequency of light, ν = 7.21 x 1014 Hz
    Maximum speed of electrons, vmax = 6.0 x 105 ms–1
    Mass of the electron, m = 9 x 10–31 kg

    Applying Einstein's photoelectric equation,
                    K.E.max = 12mv2max = h(v-v0)

           12mv2max = h(v-v0)
                      v0  = v - mv2max2h
                                  v0 = 7.21 × 1014 - (9.1 × 10-31) × (6 × 105)22 × (6.63 × 10-34)
                               = 4.74 × 1014Hz.

    Question 284
    CBSEENPH12038455

    Light of wavelength 488 nm is produced by an argon laser which is used in the photoelectric effect. When light from this spectral line is incident on the emitter, the stopping (cut-off) potential of photoelectrons is 0.38 V. Find the work function of the material from which the emitter is made.

    Solution

    Given,
    Wavelength of light, λ = 488 nm = 488 x 10–9 m
    Stopping potential, V0 = 0.38V 

    As,            eV0 = hv - ϕ0

                 eV0 = hcλ-ϕ0

                  ϕ0 = hcλ-eV0

                               = 6.63 × 10-34 × 3 × 108488 × 10-9 × 1.6 × 10-19-1.6 × 10-19 × 0.381.6 × 10-19

                          = (2.55 - 0.38) eV = 2.17 eV.

    Question 285
    CBSEENPH12038456

    Calculate the
    (a)    momentum, and
    (b)    de-Broglie wavelength of the electrons accelerated through a potential difference of 56 V. 

    Solution
    Given, 
    Potential difference, V = 56 V

    Energy of electron accelerated, 
    = 56 eV = 56 × 1.6 × 10-19J
    (a) As, Energy, E = p22m               [p = mv,  E = 12mv2]
                      p2 = 2mE 

                       p = 2mE 

                       p = 2 × 9 × 10-31 × 56 × 1.6 × 10-19 

                           p = 4.02 × 10-24 kg ms-1 
    is the momentum of the electron. 

    (b) Now, using De-broglie formula we have,  p = hλ
            λ = hp = 6.62 × 10-344.02 × 10-24 

                  = 1.64 × 10-10m = 0.164 × 10-9m 
     
    i.e.,      λ = 0.164 nm , is the De-broglie wavelength of the electron.
    Question 286
    CBSEENPH12038457

    What is the
    (a)    momentum,
    (b)    speed, and
    (c)    de-Broglie wavelength of an electron with kinetic energy of 120 eV.

    Solution

    given, 
    Kinetic energy of the electron, K.E = 120 eV

    (a) Momentum of the electron is given as, p  = 2mE 

     p = 2 ×(9 × 10-31) × (120 × 1.6 × 10-19)    = 5.88 × 10-24 kg ms-1

    (b) Now, since p = mv 
    we have,      
                         v = pm    = 5.88 × 10-249.1 × 10-31 
                                  
                     v = 6.46 × 106 m/s 

    (c) De- broglie wavelength of electron is given by, 
                     λ = hp    = 6.63 × 10-345.88 × 10-24    = 1.13 × 10-10m

                        = 1.13 Å.                



    Question 287
    CBSEENPH12038458

    The wavelength of light from the spectral emission line of sodium is 589 nm. Find the kinetic energy at which
    (a)    an electron, and
    (b)    a neutron, would have the same de-Broglie wavelength.

    Solution

    Given, 
    Wavelength of sodium light, λ = 589 nm 

    We know that,   λ = h2mE 

                         E = h22λ2m 

    (a) For electron, 

    Energy, E = (6.63 × 10-34)22 × (589 × 10-9)2 × 9 × 10-31 

                   = 7.03 × 10-25J 

    (b) For neutron,

    Energy, E = (6.63 × 10-34)22 × (589 × 10-9)2 × 1.66 × 10-27 

                   = 3.81 × 10-28J.

    Question 288
    CBSEENPH12038459

    What is the de-Broglie wavelength of
    (a)    a bullet of mass 0.040 kg travelling at the speed of 1.0 km/s.
    (b)    a ball of mass 0.060 kg moving at a speed of 1.0 m/s and
    (c)    a dust particle of mass 1.0 x 10–9 kg drifting with a speed of 2.2 m/s?

    Solution

    (a) Given,

    Mass of the bullet, m = 0.040 kgVelocity with which the bullet is travelling, v = 1 kms-1 = 103 ms-1Using the formula of momentum,                                                               p = mv                                                                  = 0.040 × 103                                                                   = 40 kg ms-1
     De-broglie wavelength is, 
                             λ = hp     = 6.62 × 10-3440      = 1.7 × 10-35m 


    (b) Mass of the ball, m = 0.060 kg 
         Velocity with which the ball is moving, v = 1.0 ms-1
         Momentum of the particle,  p = mv = 0.060 kg ms-1

    Therefore, 

    De-broglie wavelength of the particle, λ = hp    = 6.62 × 10-340.060    = 1.1 × 10-32

    (c) Mass of the dust particle, m = 1.0 × 10-9 kg
         Velocity of the particle, v= 2.2 m/s Momentum of the particle, p = mv = 2.2 × 10-9Therefore,De-broglie wavelength, λ = hp = 6.62 × 10-342.2 × 10-19                                                             = 3 × 10-25m.

    Question 289
    CBSEENPH12038460

    An electron and a photon each have a wavelength of 1.00 nm. Find
    (a)    their momenta,
    (b)    the energy of the photon, and
    (c)    the kinetic energy of electron.
    (Take h = 6.63 x 10–34 Js).

    Solution
    Given,
    Wavelength of electron and photon, λe = λp = 1.00 nm = 1 x 10
    –9 m 

    (a) Momenta of the particle, 

       p = hλ = 6.63 × 10-341.00 × 10-19kg ms-1 

                    = 6.63 × 10-25 kg ms-1

    (b) Energy of the photon, E = hv = hcλ

                                               = 6.63 × 10-34 × 3 × 1081 × 10-9J
                                             = 1.989 × 10-16J= 1.989 × 10-161.6 × 10-19eV
                                             = 1.243 ke V 

    (c) Now, using the de-broglie formula, we have   h2mEk= λ
               2mEk = hλ
    i.e.,                 Ek = h222
                      Ek = (6.63 × 10-34)22 × 9.1 × 10-31 × (10-9)2 
                              = 43.96 × 10-6818.2 × 10-49J = 2.4 × 10-19J 

                          Ek = 2.4 × 10-191.6 × 10-19eV      = 1.5 eV.              
    Question 290
    CBSEENPH12038461

    For what kinetic energy of a neutron will the associated de-Broglie wavelength be 1.40 x 10–10 m?

    Solution
    De-broglie wavelength, λ = 1.40×10-10 m

    Mass of neutron, m = 1.675 × 10-27 kgPlanck's constant, h = 6.63 × 10-34 Js De-brogliw wavelength is given by, λ = hmv  

    i.e., v = h   v = 6.63×10-341.675×10-27 × 1.40×10-10           = 28.28 × 102 m/s  

    Kinetic energy is given by, K.E = 12mv2  

                 = 12×1.675×10-27×( 28.8×102)2 = 6.634 × 10-21 J
    Question 291
    CBSEENPH12038462

    Also find the de-Broglie wavelength of a neutron, in thermal equilibrium with matter, having an average kinetic energy of  32kT at 300 K.

    Solution
    Given, 
    Average Kinetic energy, E = 32kT                                                 = 32×(1.38 × 10-23) × 300                                                 = 6.21 × 10-21J
                      (Here, k is Boltzmann constant.  The value of k is 1.38 × 10-38JK-1)

    De-broglie wavelength is given by,
               λ =h2mE
          λ = 6.63 × 10-342 ×6.21 ×10-21×1.675 × 10-27 

    i.e.,    λ = 1.45 × 10-10 m.
    Question 292
    CBSEENPH12038463

    Show that the wavelength of electromagnetic radiation equal to the de-Broglie wavelength of its quantum (photon).

    Solution
    De-Broglie wavelength of a photon is, λ = hp
    Momentum of a photon, p = hvc 

    Hence,
                         λ = hhvc = cv 

    which proves that it is same as the wavelength of electromagnetic radiation.
    Question 293
    CBSEENPH12038464

    What is the de-Broglie wavelength of a nitrogen molecule in air at 300 K? Assume that the molecule is moving with the root-mean square speed of molecules at this temperature. (Atomic mass of nitrogen = 14.0076 u).

    Solution
    Temperature, T = 300 K
    Atomic mass of nitrogen = 14.0076 u. 

     Mass of nitrogen molecule, m = 2 × 14.0076 u
                                                   = 2 × 14.0076 × 1.6606 × 10-27kg= 46.52 × 10-27kg 

    Now, de-Broglie wavelength is given by, 

              λ = hmv = hp 

         λ = h2mEk   = h2m(32kBT)   = h3mkBT       Ek = 32kgJ
                                                                                  (where kB is Boltzmann constant)
     λ = 6.63 ×10-343 × 46.52 × 10-27 × 1.38 × 10-23 × 300

      = 6.63240.37 × 10-9m = 0.0276 nm 

      = 0.276 Å
    Question 294
    CBSEENPH12038465

    Estimate the speed with which electrons emitted from a heated emitter of an evacuated tube impinge on the collector maintained at a potential difference of 500 V with respect to the emitter. Ignore the small initial speeds of the electrons. The specific charge of the electron, i.e., its e/m is given to be 1.76 x 1011 C kg–1.

    Solution
    Here,
    Potential difference, V = 500 V
    Specific charge on electron, em = 1.76 × 1011 C kg-1 

    kinetic energy is the work done on the electron by potential difference between the cathode and the anode.
    Thus,

        12mv2 = eV
            v = 2eVm   = 2 × 1.76 × 1011 × 500 

    i.e.,      v = 1.327 × 107 ms-1 

    is the speed with which the electrons are getting impinged on the collector.
    Question 295
    CBSEENPH12038466

    Use the same formula you employ in (a) to obtain electron speed for a collector potential of 10 MV. Do you see what is wrong? In what way is the formula to be modified?

    Solution

    Here,
    Potential, V = 10 MV = 10 × 106 = 107 V
    Specific charge ratio,  em = 1.76 × 1011 C kg-1 

    Now,
           v = 2eVm = 2 × 1.76 × 1011 × 107
    i.e., v = 1.876 × 109 ms-1 

    The obtained speed is not possible because, it is greater than the speed of light. Now, since,  m = m01-v2c2 therefore, as v approaches c, mass of the electron becomes infinite. 
    Hence, the formula needs to be modified. 

    Question 296
    CBSEENPH12038467

    monoenergetic electron beam with electron speed of 5.20 x 106 ms–3 is subject to a magnetic field of 1.30 x 10–4 T normal to the beam velocity. What is the radius of the circle traced by the beam, given e/m for electron equals 1.76 x 1011C kg–1.

    Solution

    Given,
    Velocity of electron, v = 5.20 x 106 m/s
    Magnetic field, B = 1.30 x 10–4 T
    specific charge ratio, e/m = 1.76 x 1011 C kg–1 

    Centripetal force is provided by the force exerted by magnetic field on electron, 

                        mv2r = Bev

                              r = mvBe   = vB(e/m)

                              r = 5.20 ×1061.30 × 10-4 × 1.76 × 1011m
                                  = 0.227 m = 22.7 cm.

    Question 297
    CBSEENPH12038468

    Is the formula you employ in (a) valid for calculating radius of the path of a 20 MeV electron beam? If not, in what way is it modified?

    Solution
    Given, 
    Energy of the electron beam = 20 MeV

    Energy is given by, 
                          12mv2 = 20 Mev              = 20 × 1.6 × 10-13J 
    Therefore, 
                               velocity, v = 2 × 20 × 1.6 × 10-139.1 × 10-31 m/s                  = 2.65 × 109 m/s

    The velocity of the electron beam is greater than velocity of light. Thus, we can say that the electron is clearly moving at relativisitic speed.

    So, the non-relativistic formula 
    r = m0veB 
    is not valid.

    We should use relativistic formula:

    Thus,
    Radius of the path is given by, r = mveB
    That is , 
                            r = m0veB1-v2c2. 
    where, mo is the relativistic mass. 
    Question 298
    CBSEENPH12038469

    An electron gun with its collector at a potential of 100 V fires out electrons in a spherical bulb containing hydrogen gas at low pressure (–10–2 mm of Hg). A magnetic field of 2.83 x 10–4 T curves the path of the electrons in a circular orbit of radius 12.0 cm. (The path can be viewed because the gas ions in the path focus the beam by attracting electrons, and emitting light by electron capture; this method is known as the ‘fine beam tube’ method.) Determine e/m from the data.

    Solution

    Here,
    Potential at collector, V = 100 V;
    Magnetic field, B = 2.83 x 10–4 T
    Radius of the circular orbit, r = 12.0 cm = 12.0 x 10–2 m
    When electrons are accelerated through apotential of V volt, the gain in kinetic energy K.E. of the electron is given by,

                             12mv2 = eV

                            v2 = 2eVm                                       ...(i) 

    Since the electron moves in circular orbit under magnetic field, therefore, force on the electron due to magnetic field provides the centripetal force to the electron.
                                 evB = mv2r

                                  eB = mvr

                                  v2 = e2B2r2m2                      ....(ii) 

    From equations (i) and (ii), we get 

                     2eVm = e2B2r2m2 

                    em = 2Vr2B2
                         em = 2 × 100(12 × 10-2)2 × (2.83 × 10-4)2 

                             = 1.73 × 1011 C kg-1.                    





    Question 299
    CBSEENPH12038470

    (a) An X-ray tube produces a continuous spectrum of radiation with its short wavelength end at 0.45 Å. What is the maximum energy of a photon in the radiation?
    (b) From your answer to (a), guess what order of accelerating voltage (for electrons) is required in such a tube?

    Solution

    We are given an x-ray tube.

    Wavelength of the radiation, λ = 0.45 Å = 0.45 x 10–10 m
    Planck's constant, h = 6.62 x 10–34 Js
    speed of light, c = 3 x 108 ms–1 

    (a) The maximum energy of photon is given by, 
                    E = hv = hcλ 

                E = 6.62 × 10-34 × 3 × 1080.45 × 10-10   = 44 × 10-16J                               
     i.e.,         E = 44 × 10-161.6 × 10-19eV    = 27.5 × 103 eV   = 27.5 keV. 

    (b) To produce electrons of 27.5 keV, accelerating potential of 27.5 kV to 30 KV is required.

    Question 300
    CBSEENPH12038471

    In an accelerator experiment on high-energy collisions of electrons with positrons, a certain event is interpreted as annihilation of an electron-positron pair of total energy 10.2 BeV into two γ-rays of equal energy. What is the wavelength associated with each γ-ray? (1BeV = 109eV)

    Solution
    Total energy of 2 γ-rays = 10.2 BeV = 10.2 x 109 eV 

    ∴         Energy of each γ-ray is,

    E = 12(10.2 × 109 × 1.6 × 10-19) J
      
    = 8.16 × 10-10J          
                             
    Now, using the formula for energy of a photon, 

                           E = hv = hcλ 

                   λ = hcE    = 6.63 × 10-34 × 3 × 1088.16 × 10-10  = 2.436 × 10-16m. 

    is the required wavelength assosciated with each γ-ray.
    Question 301
    CBSEENPH12038472

    Estimating the following two numbers should be interesting. The first number will tell you why radio engineers do not need to worry much about photons! The second number tells you why our eye can never ‘count photons,’ even in barely detectable light.
    The number of photons emitted per second by a medium wave transmitter of 10 kW power emitting radio waves of length 500 m.

    Solution

    Given,
    Wavelength of radio waves, λ = 500 m 
    Energy of photon, E = hv

    Now, using the formula for energy of a photon,
                    
                 E = hcλ     = 6.63 × 10-34 × 3 × 108500J  

                E = 3.98 × 10-28J 

    Number of photons emitted per second, 

         = Power of transmitterEnergy of one photon    P = ne 

         = 104Js-13.98 × 10-28J 

         = 3 × 1031 s-1 

    We can see, that the energy of a radiophoton is exceedingly small, and the number of photons emitted per second from a radio beam is enormously large. Thus, there is negligible error involved in ignoring the existence of a minimum quantum of energy of photon and treating the total energy of a radiowave as continuous.

    Question 302
    CBSEENPH12038473

    Estimating the following two numbers should be interesting. The first number will tell you why radio engineers do not need to worry much about photons! The second number tells you why our eye can never ‘count photons,’ even in barely detectable light.
    The number of photons entering the pupil of our eye per second corresponding to the minimum intensity of white light that we humans can perceive (~10–10 Wm–2). Take the area of the pupil to be about 0.4 cm2, and the average frequency of white light to be about 6 x 104 Hz.

    Solution
    Given,
    Average frequency of white light, ν = 6 x 10
    14 Hz
    Energy of photon, E = hv = 6.63 x 10
    –34 x 6 x 1014 J ≃ 4 x 10–19 J.

    Photon flux corresponding to minimum intensity, 

                    = 10-10 Wm-24 × 10-19J   P = nE= 2.5 × 108 m-2 s-1 

    Number of photons entering the pupil per second = 2.5 x 108 x 0.4 x 10–4 s–1 = 104 s–1

    Though this number is not as large as in (a) of the previous question, but it is large enough and it is impossible to count the photons with our naked eyes. 

    Question 303
    CBSEENPH12038474

    Ultraviolet light of wavelength 2271 Å from a 100 W mercury source irradiates a photo-cell made of molybdenum metal. If the stopping potential is -1.3 volt, estimate the work function of the metal. How would the photo-cell respond to a high intensity (~ 105Wm–2) red light of wavelength 6328 Å produced by He-Ne laser?

    Solution

    Here,
    Sopping potential,  V0 = 1.3 V 
    Wavelength of ultraviolet light, λ = 2271  Å                                                            = 2271 × 10-10m

    Now, using Einstein's photoelectric equation, 

            hv = hv0+12mv2max = ϕ0+eV0  

       ϕ0 = hcλ-eV0 
    where, ϕo is the work function of the metal. 

    Taking,      h = 6.62 × 10-34 Js
                     e = 1.6 × 10-19C
                     c = 3 × 108 ms-1 
    We have,

    ϕ0 = 6.62 × 10-34× 3 × 1082271 × 10-10-1.6 × 10-19 × 1.3

        ϕ0 = 8.745 × 10-19-2.08 × 10-19     = 6.665 × 10-19J   

    i.e.,  ϕ0 = 6.665 × 10-191.6 × 10-19 = 4.166 eV. 

    Threshold wavelength is given by, 

          λ0 = hcϕ0       = 6.62 × 10-34 × 3 × 1086.665 × 10-19      = 2.98 × 10-7m 

    i.e., λ0 = 2980 Å 

    As calculated above, wavelength of red light is greater than threshold wavelength λ0. Therefore, photocell will not respond when red light of wavelength 6328 A produced by He-Ne laser is incident on the photocell.

    Question 304
    CBSEENPH12038475

    The work function for the following metals is given:
    Na: 2.75 eV; K: 2.30 eV; Mo: 4.17 eV; Ni: 5.15 eV.
    Which of these metals will not give photoelectric emission for a radiation of wavelength 3300 A from a He-Cd laser placed 1m away from the photocell? What happens if the laser is brought nearer and placed 50 cm away?

    Solution
    Given,
    Work function of Na is, 
    ϕNa = 1.92  eV = 1.92 × 1.6 × 10-19J  
    Wavelength of the radiation light emitted,  λ  = 3300 Å = 3300 × 10-10m

    Using the formula of energy of a photon,

     E = hcλ    = 6.6 ×10-34 × 3 × 1083300 × 10-10J

    E = 6.6 × 3 × 10-34+8+10-233 × 10J

      = 6 × 10-18-11.6 × 10-19eV

      = 6010eV 

    E = 3.75 eV 

    It is observed that energy of incident radiation is less thanwork function of Ni and Mo but larger than the work function of Na and K.
    So, photoemission current take place from Na and K but not from Mo and Ni.

    The intensity of the radiation increases, if the laser is brought closer and the photoelectric current from Na and K will increase. But, however this will not bring any change in the result derived. 

    Question 305
    CBSEENPH12038476

    Light of intensity 10–5 W m–2 falls on a sodium photo-cell of surface area 2 cm2. Assuming that the top 5 layers of sodium absorb the incident energy, estimate time required for photoelectric emission in the wave-picture of radiation. The work function for the metal is given to be about 2 eV. What is the implication of your answer?

    Solution
    Given, 
    Intensity of light = 10–5 W m–2
    Surface are of the sodium photocell, A = 2 cm2

    Top five layers of sodium absorb the incident energy. (given)

    work function for the metal, ϕo = 2 eV

    Therefore,  

    N
    umber of atoms in 5 layers of sodium is, 
     
        = 5 × area of each layerEffective area of atom= 5 × 2 × 10-410-20 = 1017 

    Assume that there is only one conduction electron per sodium atom. 
    ∴ Number of electrons in 5 layers = 1017 

    Energy received by an electron per sec is, 

            = Power of incident lightNumber of electrons= 10-5 ×2×10-41017 = 2 ×10-26W 

    Time required for photoemission is, 

    = Energy required per electronEnergy absorbed per second per electron= 2 × 1.6 × 10-192 × 10-26s= 1.6 × 107s. 

    Thus, it is contrary to the observed fact that there is no time lag between the incidence of light and the emission of photoelectrons.
    Question 306
    CBSEENPH12038477

    Crystal diffraction experiments can be performed using X-rays, or electrons accelerated through appropriate voltage. Which probe has greater energy, an X-ray photon or the electron? (For quantitative comparison, take the wavelength of the probe equal to 1 Å, which is of the order of interatomic spacing in the lattice) (me = 9.11 x 10–31 kg).

    Solution

    Wavelength of the probe = 1 Ao
    Mass of electron, me = 9.11 x 10–31 kg

    Energy of photon, E = hv = hcλ
                                    = 6.63 × 10-34 × 3 × 10810-10J= 19.89 × 10-16J 
                     i.e.,E = 19.89 × 10-161.6 × 10-19eV = 12.43 keV 

    For the case of electron, 

                            λ = h2mE 

                 2mE = hλ 

                   2mE = h2λ2
                        E = h222
                        E = 6.63 × 10-3422 × 9.11 × 10-31 × 10-20J
                             = (6.63 × 10-34)22 × 9.11 × 10-31 ×10-20×1.6 × 10-19eV
    i.e.,                   E = 150.8 eV 

    From the above calculations, we can see that, for the same given wavelength, kinetic energy of a photon is much greater than that of electron.

    Question 307
    CBSEENPH12038478

    Obtain the de-Broglie wavelength of a neutron of kinetic energy 150 eV. As you have seen in Question 11.31, an electron beam of this energy is suitable for crystal diffraction experiments. Would a neutron beam of the same energy be equally suitable? Explain. Given (mn = 1.675 x 10–27 kg.)

    Solution
    Here,
    Kinetic energy, K.E. of neutron, E = 150 eV = 150 x 1.6 x 10
    –19 J,
    Mass of neutron, m = 1.675 x 10–27 kg. 

    We know, K.E. of neutron, 

    E = 12mv2    or   mv = 2Em 

            λ = hmv = h2Em
                   = 6.63 × 10-342 × 150 × 1.6 × 10-19 × 1.675 × 10-27 = 2.33 × 10-12m.

    The interatomic spacing ~ 1 Å (= 10
    –10 m) is about a hundred times greater than this wavelength. Therefore, a neutron beam of energy 150 eV is not suitable for diffraction experiment.
    Question 308
    CBSEENPH12038479

    Obtain the de-Broglie wavelength associated with thermal neutrons at room temperature (27°C). Hence explain why a fast neutron beam needs to be thermalised with the environment before it can be used for neutron diffraction experiments.

    Solution

    We are given,
    Room tempertaure, T = 27 + 273 = 300 K
    Boltzmann's constant, k = 1.38 x 10–23 J mol–1 K–1

    We know, average kinetic energy of neutron at absolute temperature T is given by, 

                  E = 32kT.
    where k is the Boltzmann's constant. 

    Now, wavelength, λ = h2mE = h3mkT 
     λ = 6.63 × 10-343 × 1.675 × 10-27 × 1.38 × 10-23 ×300 = 1.45 × 10-10m 

    Since this wavelength is comparable to interatomic spacing (~ 1 Å) in a crystal, therefore, thermal neutrons are suitable for diffraction experiments. So, a high energy neutron beam should be first thermalised before using it for diffraction.

    Question 309
    CBSEENPH12038480

    An electron microscope uses electrons accelerated by a voltage of 50 kV. Determine the de-Broglie wavelength associated with the electrons. If other factors (such as numerical aperture, etc.) are taken to be roughly the same, how does the resolving power of an electron microscope compare with that of an optical microscope which uses yellow light?

    Solution
    Given,
    Accelerating voltage, 
    V = 50 kV
    ∴ Energy of electrons, E = eV = 50 keV
    or, Energy, E = 50 x 103 x 1.6 x 10–19 J 

    De-broglie wavelength is given by,
    λ = h2mE 
     λ = 6.62 × 10-342×9.1 ×10-31×50 ×103×1.6×10-19  

    λ = 6.62 × 10-341.21 × 10-22 = 5.47 × 10-12m. 

    Resolving power of microscope  1λ
     R.P. of electron microscopeR.P. of optical microscope = λyλ+5.9 × 10-75.47 × 10-17                                                      10+5 
    where, λy = wavelength yellow light

    Resolving power of a microscope is inversely proportional to the wavelength of the radiation used.
    Since the wavelength of yellow light is 5.99 x 10
    –7 m, so it follows that electron microscope will have resolving power 105 times that of optical microscope.
     
    Question 310
    CBSEENPH12038481

    The wavelength of a probe is roughly a measure of the size of a structure that it can probe in some detail. The quark structure of protons and neutrons appears at the minute length-scale of 10–15 m or less. This structure was first probed in early 1970’s using high energy electron beams produced by a linear accelerator at Stanford, USA. Guess what might have been the order of energy of these electron beams. (Rest mass energy of electron = 0.511 MeV.)

    Solution
    Using the formula, 

    Momentum of the particle is, p = hλ = 6.63 × 10-34Js10-15m
                                                   = 6.63 × 10-19 Kg ms-1 

    Now, the relativistic formula for energy gives us: 

                          E2 = c2p2+m02c4
     E2 = 9 × (6.63)2 × 10-22+(0.511 × 1.6)2 × 10-26 

              9 × (6.63)2 × 10-22 

    the second term (rest mass energy) being negligible. 

    Therefore, E = 1.989 × 10-10J

                    E = 1.989 × 10-101.6 ×10-11 BeV = 1.24 BeV. 

    Thus, the order of energy of these electron beams is of the order of few Bev.
    Question 311
    CBSEENPH12038482

    Find the typical de-Broglie wavelength associated with a He atom in helium gas at room temperature (27 °C) and 1 atm pressure; and compare it with the mean separation between two atoms under these conditions.

    Solution
    Mass of He atom,   m = Atomic mass of HeAvogadro's number 

                                    = 46 × 1023g
                            m = 6.67 × 10-27 kg 

    De- broglie wavelength, λ = hp = h3mkTm
                                            = 6.63 × 10-343×6.67×10-27×1.38×10-23×300m
    i.e.,                              λ = 7.3 × 10-11m 

    Now, using the kinetic gas equation for one mole of a gas,  PV = RT = kNT

        VN = KTP 

    Mean separation, 

             r0 = Molar volumeAvogadro's number1/3    = VN1/3     = kTP1/3

         r0 = 1.38 × 10-23 × 3001.01 × 1051/3m 

    i.e.,   r0 = 3.4 × 10-9m 

    From the above calculations, we can say that the mean separation between two atoms is much larger than the de-Broglie wavelength.
    Question 312
    CBSEENPH12038483

    Compute the typical de-Broglie wavelength of an electron in a metal at 27°C and compare it with the mean separation between two electrons in a metal which is given to be about 2 x 10–10 m.
    [Note: Questions 11.35 and 11.36 reveal that while the wave-packets associated with gaseous molecules under ordinary conditions are non-overlapping, the electron wave-packets in a metal strongly overlap with one another. This suggests that whereas molecules in an ordinary gas can be distinguished apart, electrons in a metal cannot be distinguished apart from one another. This indistinguishibility has many fundamental implications which you will explore in more advanced Physics courses.]

    Solution

    Here, 
     Temperature, T = 27°C   T = 273 + 27 = 300 K

    Mass of electron, m = 9.1 × 10-31kg 

    Using formula, 
                           λ = h3mkT 

     λ = 6.63 × 10-343 × 9.1 × 10-31 × 8.31 × 1036 × 1023 × 300
    λ = 62.15 × 10-10m 

    Interelectronic separation, r = 2 × 10-10m 

    Hence, r<λ. That is, interelectronic spacing is less than the wavelength. 
    We find that wave-packets in metals strongly overlap with one another whereas, this is not the case in gas atoms.

    Question 313
    CBSEENPH12038484

    Quarks inside protons and neutrons are thought to carry fractional charges [(+ 2/3)e; (–1/3e). Why do they not show up in Millikan’s oil-drop experiment?

    Solution
    Quarks are thought to be confined within a proton or neutron by forces which grow stronger if one tries to pull them apart. That is the reason, the quarks always remain together. The fact is, though fractional charges exist in nature, the observable charges are always integral multiple of charge of electron.
    Question 314
    CBSEENPH12038485

    What is so special about the combination e/m? Why do we not simply talk of e and m separately?

    Solution
    Electric and magnetic field is related with basic equations like,  

           eV =1/2 mv
    2 or eE = ma and,
                        eBv = mv
    2/r

    In all these equations, the dynamics of electrons is determined not by e and m separately but by the combination e/m. Hence, we do not talk of e and m seperately.
    Question 315
    CBSEENPH12038486

    Why should gases be insulators at ordinary pressures and start conducting at very low pressures?

    Solution
    At low pressures, uner the effect of high voltage ions acquire sufficient energy; have a chance to reach their respective electrodes and constitute a current.

    At ordinary pressures, positive ions and electrons produced by ionisation of gas molecules do not reach the electrodes even at higher potential. this is because, of the frequent collisions of molecules and their recombination. Hence, at ordinary pressure gases act as insulators. 
    Question 316
    CBSEENPH12038487

    Every metal has a definite work function. Why do all photoelectrons not come out with the same energy if incident radiation is monochromatic? Why is there an energy distribution of photoelectrons?

    Solution
    Work function indicates the minimum energy required for the electron in the highest level of the conduction band to get out of the metal.
    Not all electrons in the metal belong to this level but, rather they occupy a continuous band of levels. Consequently, for the same incident radiation, electrons knocked off from different levels come out with different energies.
    Question 317
    CBSEENPH12038488

    The energy and momentum of an electron are related to the frequency and wavelength of the associated matter wave by the relations
    E = hv,  p = hλ
    But while the value of A is physically significant, the value of v (and therefore, the value of the phase speed v λ) has no physical significance. Why?

    Solution
    For a moving particle,  

    De-broglie wavelength is given by, λ= hp or, p = hλ 
    p is momentum. 

    Energy of a photon is, E=  = hcλ  

    Therefore, 
    Energy of a moving particle = p22m=hλ22m= h22 λ2 m  

    From the above relation we can see that, ν has no direct significance on relation of E and p. 
    Question 318
    CBSEENPH12038489

    An electron and alpha particle have the same de-Broglie wavelength associated with them. How are their kinetic energies related to each other?

    Solution

    Given, de-broglie wavelength assosciated with electron and an alpha particle is same. 

    Now, 

    Kinetic energy, K.E. = 12mv2 = 12m p2m2  

                   K.E. = p22m  ... (1)           ( p = mv)

    and,
                                  λe = λαhpe =hpα 

    where, pe and pα is the momentum of electron and alpha particle respectively. 

    So,                    pe2 = pα2 - I 

    From equation (1)

                             K.E.eK.E.α = 12pe22me12ρα22mα 

                         K.E.eK.E.α = mαme× pe2pα = mαme. 

    is the required relation.


    Question 319
    CBSEENPH12038490

    Monochromatic radiation of wavelength 640.2 nm (1 nm = 10–9 m) from a neon lamp irradiates a photosensitive material made of caesium on tungsten. The stopping voltage is measured to be 0.54 V. The source is replaced by an iron source and its 427.2 nm line irradiates the same photocell. Predict the new stopping voltage.

    Solution
    Here, we are given a neon lamp.
                                   Wavelength of radiation, λ = 640.2 nm = 640.2 × 10-9mStopping potential, V1           = 0.54 V

    The source is replaced by an iron source whose wavelength is 427.2 nm.
    Stopping potential applied to the iron source, V2 = ?

    Using the formula of Einstein's energy equation, 

                              eV1 =hcλ1- ϕ0 

                              eV2 = hcλ2-ϕ  

    On subtracting both equations,

                      eV2-eV1 = hc1λ2-1λ1 

                     V2-V1 = hce1λ2-1λ1  

                   V2 = V1 = hce1λ2-1λ1
                    V2 = 0.54 + 6.63 × 10-24 × 3 × 1081.6 × 10-191427.2 ×10-9-1640.2 × 10-9
                             = 0.54 + 6.63×3×10-24+8+91.6 1427.2-1640.2

                              = 0.54 + 6.63 × 31.6640.2 - 427.2640.2 × 427.2× 10-7

                           = 0.54 + 0.97

    That is ,       V2 = 1.51 V.


    Question 320
    CBSEENPH12038491

    A mercury lamp is convenient source for studying frequency dependence of photoelectric emission, since it gives a number of spectral lines ranging from the UV to the red end of the visible spectrum. In our experiment with rubidium photocell, the following lines from a mercury source were used:
    λ1 = 3650 Å, λ2 = 4047 Å, λ3 = 4358 Å, λ4 = 5461 Å, λ5 = 6907 Å
    The stopping voltages, respectively were measured to be:
    V01 = 1.28 V,V02 = 0.95 V,V03 = 0.74 V, V04 = 0.16 V,V05 = 0V
    (a)    Determine the value of Planck's constant h.
    (b)    Estimate the threshold frequency and work function for the material.



    Solution

    Using the given data, we first determine frequency in each case and then plot a graph between stopping potential V0 and frequency v. 

    v1 = cλ1 = 3 × 1083650 × 10-10 = 8.219 × 1014Hzv2  = cλ2 = 3 × 1084047 × 10-10 = 7.412 × 1014Hzv3 = cλ3 = 3 × 1084358 × 10-10 = 6.884 × 1014Hzv4 = cλ4 = 3 × 1085461 × 10-10 = 5.493 × 1014Hzv5 = cλ5 = 3 × 1086907 × 10-10 = 4.343 × 1014Hz 

    Vversus v plot is shown below: 

     

    The first four points lie nearly on a straight line which intercepts the frequency axis at threshold frequency v0 = 5.0 x 1014 Hz.

    The fifth point v (= 4.3 x 1014 Hz) corresponds to v < v0, so there is no photoelectric emission and not stopping voltage is required to stop the current.

    Slope of V
    0 versus v graph is, 

    V v = (1.28 - 0)V(8.2-5.0) × 1014s-1             = 4.0 × 10-15 Vs 

    Now, from Einstein's photoelectric equation, 

    Kinetic energy of photon, K.E. = eV = hv - W0 

                         eV = hv                      [W0 (work function) is  a constant ] 

                        Vν = he 

    Hence,             he = 4.0 × 10-15 Vs 

    Planck's constant, h = e × 4.0 × 10-15Js

                              h = 1.6 × 10-19 × 4.0 × 10-15Js 

                                 = 6.4 × 10-34Js 

    (b) Threshold frequency, v0 = 5.0 × 1014Hz
           Work function of the metal,  ϕ0 = hv0                                                                = 6.4 × 1034 × 5.0 × 1014

    i.e.,   ϕ0 = 6.4 ×5×10-201.6 × 10-19eV = 2.00 eV is the required work function of the metal.






    Question 321
    CBSEENPH12038492

    How does the stopping potential applied to a photocell change, if the distance between the light source and the cathode of the cell is doubled? 

    Solution
    When the distance between the light source and the cathode is changed, the intensity of light changes accordingly. However, the stopping potential does not depend upon the intensity of incident light.
    Question 322
    CBSEENPH12038493

    de-Broglie wavelength associated with an electron accelerated through a potential difference V is X. What will be its wavelength when the accelerating potential is increased to 4 V?

    Solution
    De-Broglie wavelength assosciated with an electron is,
               λ = 1.227Vnm
    That is, wavelength is inversely proportional to the square -root of potential.
    Thus,
    When potential difference is increased 4 times,wavelength becomes half it's value. 

    Question 323
    CBSEENPH12038494

    Two metals A and B have work function 2 eV and 5 eV respectively. Which metal has lower threshold wavelength?

    Solution

    Given, work function of metal A = 2 eV
    Work function of metal B = 5 eV

    As,                ϕ0 = hcλ         λ = hcϕ0


    i.e.                   λ   1ϕ0 

    Thus, metal B has lower threshold wavelength of radiation since its work function is greater.

    Question 324
    CBSEENPH12038495

    Two lines, A and B in the plot given below show the variation of de-Broglie wavelength, A versus 1V, where V is the accelerating potential difference, for two particles carrying the same charge.
    Which one of two represents a particle of smaller mass? 

    Solution
    De-broglie wavelength is given by,  λ = hp                                                                     λ = hmv                                                                    λ = 1.227V 

                            slope =  λ1/V = h/V1/V 
     
                                slope = hmv × V1.22

    Since,  Slope of B > slope of A   Slope  1m 

                   1mB >  1mA       mB  <  mA 

                  mB < mA 

    Therefore, line B represents a particle of smaller mass.



    Question 325
    CBSEENPH12038496

    The maximum kinetic energy of a photoelectron is 3 eV. What is its stopping potential?

    Solution

    Maximum K.E of particle = 3 eV

    Since,            K.E.max = eV0

      3 × 1.6 × 10-19 = 1.6 × 10-19 V0 
            
     Stopping potential, V0 = 3V.


             

    Question 326
    CBSEENPH12038497

    Ultraviolet light is incident on two photosensitive materials having work functions W1 and W2 (W1 > W2). In which case will the kinetic energy of the emitted electrons be greater? Why?

    Solution
    According to the formula,

    K.E. of photoelectron = hv – W
    That is, more is the kinetic energy less would be the work function or vice-cersa. 

    Given,   W1 > W(W1 and W2 are the work function of material respectively.)

    Since, W2 is lesser than W1 thus, the kinetic energy of the emitted electrons for the photoelectric material having work function W2 will be greater.


    Question 327
    CBSEENPH12038498

    The frequency (v) of the incident radiation is greater than threshold frequency (v0) in a photocell. How will the stopping potential vary if frequency v is increased, keeping other factors constant?

    Solution

    Given, the frequency of the incident radiation is greater than the threshold frequency. 

    The formula gives us, 12mvmax2 = eV0 = h(v-v0) 

    Therefore, the value of stopping potential (V0) increases with increase in frequency (v) of the incident radiation and K.E. increaseses.

    Question 328
    CBSEENPH12038499

    What is the de-Broglie wavelength associated with an electron accelerated through a potential of 100 volts?

    Solution
    Accelerating potential, v = 100 V

    De-Broglie wavelength is given by, 

                              λ = 1.227Vnm

                          λ = 1.227100nm = 0.123 nm.
    Question 330
    CBSEENPH12038501

    What is the effect on the velocity of the emitted photoelectrons if the wavelength of the incident light is decreased?

    Solution
    There will be an increase in the velocity of the emitted photoelectrons if the wavelength of the incident light is decreased. 

    As,                   12mv2max = hcλ-ϕ0.
    Question 332
    CBSEENPH12038503

    An electron, an alpha-particle and a proton have the same kinetic energy. Which one of these particles has the largest de-Broglie wavelength?   

    Solution
    As per the formula, 
                                 λ = hp 

    Since,                    λ = hmv 

    Thus,                     λ  1m. 
    Wavelength and mass has inverse dependence.

    Since, mass of electron is the least out of all the three particles therefore, electron has the largest de-Broglie wavelength. 

    Question 333
    CBSEENPH12038504

    Light of frequency 1.5 times the threshold frequency is incident on a photosensitive material. If the frequency is halved and intensity is doubled, what happens to photoelectric current?

    Solution
    If the frequency is halved and intensity is doubled, the frequency of incident light will become 152 = 0.75 times the threshold frequency. Hence, photoelectric current will be zero. 
    Question 334
    CBSEENPH12038505
    Question 335
    CBSEENPH12038506

    Ultraviolet radiations of different frequencies v1 and v2 are incident on two photosensitive materials having work functions W1 and W2 (W1 > W2) respectively. The kinetic energy of the emitted electrons is same in both the cases. Which one of the two radiations will be of higher frequency? 

    Solution

    Given, the kinetic energy of the emitted electrons is same in both cases.

    Kinetic energy is given by, 
                               K.E.  = hv-ϕ 

    ν is the frequency of radiation and ϕ is the work function of materials.
    Therefore, as per given, 

                        K.E. = hv1-W1                    hv1 = K.E. + W1

    and,
                                  K.E. = hv2-W2                            hv2 = K.E.+W2


     Given that,  W1 > W2 
    Thus,    v1 > v2.

    Question 336
    CBSEENPH12038507

    How will the photoelectric current change on decreasing the wavelength of incident radiation for a given photosensitive material?

    Solution
    On decreasing the wavelength of incident radiation, the photoelectric current will remain invariant. 
    Question 337
    CBSEENPH12038508

    Why are alkali metals most suited for photoelectric emission?

    Solution
    Alkali metals have low degree of work function and hence the electrons are less bound to the atoms. It is easer to remove electrons from alkali metals as compared to other metals.
    Question 338
    CBSEENPH12038509

    What is the difference between thermionic emission and photoelectric emission?

    Solution
    During thermionic emission electrons are emitted from metal surface by providing heat energy, whereas, during photoelectric emission light energy is emitted when, electrons are emitted from the surface of metal. 
    Question 339
    CBSEENPH12038510

    The emitter in a photoelectric tube has a threshold wavelength of 6000 Å. Determine the wavelength of the light incident on the tube if the stopping potential for this light is 2.5 V.

    Solution
    Given, threshold wavelength, λo = 6000 Å 
    Stopping potential for the light, Vo = 2.5 V

    Now, the formula gives us, 

    The work function is, 

    ϕ0 = hvth      = hcλth    = 12.4 × 103eV × Å6000 Å   = 2.07 eV 

    The photoelectric equation then gives,

                              eV0 = hv - ϕ0

                         eV0 = hcλ-ϕ0 

             2.5 eV = 12.4 × 103 eV. Åλ-2.07 eV 

    i.e.,                      λ = 2713 Ao . 
    Question 340
    CBSEENPH12038511

    An electron and a proton are accelerated through the same potential. Which one of the two has (i) greater value of de-Broglie wavelength associated with it and (ii) less momentum? Justify answer.  

    Solution
    (i) The de-Broglie wavelength associated with same potential V is given by, 

                             λ = hp  or   λ = hmv

                          λ    1m
    As electron's mass is lesser than proton. Thus, λ electron > λ proton.

    (ii) Now as, λ = hp

                 p = hλ  or   p  1λ
    Since,   λe > λproton
    Hence, momentum of electron will be lesser than proton because, momentum and wavelength have inverse dependence.
    Question 341
    CBSEENPH12038512

    A proton and an alpha particle are accelerated through the same potential. Which one of the two has (i) greater value of de-Broglie wavelength associated with it, and (ii) less kinetic energy? Justify your answer.   

    Solution
    (i) The de-Broglie wavelength associated with same potential V is,
                          λ = hp    or   λ = hmv
                          λ    1m
    Wavelength and mass has inverse dependence a seen from the above relation. 

    As proton's mass is less than the mass of alpha particle thus,
                          λproton > λalpha. 
    Proton has greater value of de-broglie wavelength assosciated with it. 

    (ii) Now,
    Energy of a photon is, E = hν  

     i.e.,                       K.E. = hcλ 

                              K.E.   1λ
    Since,                  λproton > λalpha. [from (i) ] 

    Thus, kinetic energy of proton will be lesser than that of alpha particle.
    Question 342
    CBSEENPH12038513

    Find the de-Broglie wavelengths of (a) a 46-g golf ball with a velocity of 30 m/s, and (b) an electron with a velocity of 107 m/s.

    Solution
    (a) For a golf ball, 
    Since Velocity of wave < < speed of light, we can let m = m
    0
    This is the relativistic mass.
    Hence,

                  λ = hmv = 6.63 × 10-34Js(0.046 kg) (30 m/s) 

                  λ = 4.8 × 10-34 m 

    The wavelength of the golf ball is so small as compared with its dimensions that we would not expect to find any wave aspects in its behaviour. 

    (b) For an electron,
    Again V < < c, so with m = m
    0 = 9.1 x 10–31 kg, 

    We have, 

    De-broglie wavelength assosciated with the electron, λ = hmv = 6.63 × 10-34Js(9.1 ×10-31 kg) (107 m/s) 

                     = 7.3 × 10-11m 

    The dimensions of electron is comparable with this figure—the radius of the hydrogen atom, for instance is 5.3 x 10–11 m.

    It is therefore not surprising that the wave character of moving electrons is the key to understanding atomic structure and behaviour.
    Question 343
    CBSEENPH12038514

    For what kinetic energy of a proton, will the associated de-Broglie wavelength be 16.5 nm?

    Solution

    Given,
    De-broglie wavelength, λ = 16.5 nm = 16.5 x 10–9 m
    Mass of proton m = 1.6 x 10–27 kg 

    Using de-Broglie equation, 

                     λ = hmv

                 v = h
             K.E. = 12mv2 = 12 m .   h2m2 λ2
                K.E. = h222
                       = 6.63 × 10-34 × 6.63 × 10-342 × 1.6 × 10-27 ×16.5 ×10-9 × 16.5 × 10-9

               K.E. = 6.63 ×6.63×10-34-34+27+9+92×1.6×16.5×16.5

    i.e.,          K.E. = 0.05045 × 10-68+45         = 5.045 × 10-2 × 10-23K.E. = 5.045 × 10-25J.

    is the calculated kinetic energy of proton.
                   

    Question 344
    CBSEENPH12038515

    Mention the significance of Davisson and Germer’s experiment. An α-particle and a proton are accelerated from rest through the same potential difference V. Find the ratio of de-Broglie wavelengths associated with them.

    Solution

    The Davisson and Germer’s experiment established famous de-Broglie hypothesis of wave-particle duality by confirming the wave nature of moving particle.

    Given, an alpha particle and a proton are accelerated from rest by the same potential.

    The energy acquired by alpha-particle, Eα = 2eV
    The energy acquired by proton, Ep = eV

    de-Broglie wavelength,   λ = h2mE

    Hence, the ratio of wavelengths,

                         λαλp = mpEpmαEα         = mpEp(4mp) (2Ep)               [   mα = 4 mp  and Eα = 2Ep]

                   λαλp = 122 

    i.e.,          λα : λp = 1:22.

    is the obtained ratio of the de-broglie wavelength asosciated with the particles.

    Question 345
    CBSEENPH12038516

    Radiations of frequency 1015 Hz are incident on two photosensitive surfaces A and B. Following observations are recorded:
    Surface A: No photoemission takes place.
    Surface B: Photoemission takes place but photoelectrons have zero energy.
    Explain the above observations on the basis of Einstein's photoelectric equation.
    How will the observation with surface B change when the wavelength of incident radiations is decreased?    

    Solution
    Given, 
    Radiation of frequencies incident on the photoelectric surface = 1015 Hz 

    Now, according to Einstein's photoelectric equation, kinetic energy of a photoelectron is given by,  

                                 Kmax = hv-ϕ0                         Kmax = h(v-v0) 

    i.e.,                 Kmax = hc1λ-1λ0 

    (i) The threshold frequency of surface A is greater than 1015 Hz, and that is the reason no photoemission takes place. 

    (ii) For surface B, the threshold frequency is equal to 1015 Hz. So, photoemission takes place but photoelectrons have zero kinetic energy.
    If, the kinetic energy of the elctrons emitted from surface B has to be increased then, the wavelength of the incident radiation has to be decreased.
    Question 346
    CBSEENPH12038517

    Calculate de-Broglie wavelength in nm associated with a ball of mass 66 g moving with a velocity 2.5 x 105 ms–1. Given h = 6.6 x 10–34 Js.

    Solution

    Given, 
                   Mass of the ball, m = 66 g = 66 × 10-3kgVelocity with which the ball is moving, v =  2.5 × 105 ms-1

    We know,
                     λ = hmv
                 λ = 6.6 × 10-3466×10-3×2.5×105
                       = 4×10-38m = 4×10-3810-9nm
    i.e.,            λ = 4 × 10-29 nm. 

    Question 347
    CBSEENPH12038518

    Sketch the graphs showing the variation of stopping potential with frequency of incident radiations for two photosensitive materials A and B having threshold frequencies v> v0respectively.
    (i)    Which of the two metals, A or B has higher work function?
    (ii)    What information do you get from the slope of the graphs?
    (iii)    What does the value of the intercept of graph ‘A’ on the potential axis represent ?

    Solution

    The above graph gives us the variation of stopping potential with frequency of incident radiation.

    (i) Since work function ɸ = hv 

    i.e.,                           ɸ0’ = hv0’ 

    Metal ‘A’ has higher work function as v0’ > v0

    (ii)
      The graph gives us Voν                    Slope of graph = he 
    (iii) Intercept of graph A on the potential axis is -ϕ0'e = -hv0'e.


    Question 348
    CBSEENPH12038519

    A nucleus of mass M initially at rest splits into two fragments of masses m/3 and 2m/3. Find the ratio of de-Broglie wavelength of the two fragments.

    Solution

    Given, a molecule of mass M. 
    It splits into two fragments of masses m/3 and 2m/3. 

    Let,    
               m1 = m3  and m2 = 2m3
    But,
              m1+m2 = M      m1 = M - m2 

    Following the law of conservation of linear momentum,
                        m1v1+m2v2 = 0 

                     m1v1 = -m2v2 

    Also,De-broglie wavelength is, λ = hmv 

    Hence, λ1λ2 = m2v2m1v1 = 1. 

    Thus, the ratio of wavelength is 1. 

    Question 349
    CBSEENPH12038520

    The work function of lithium is 2.3 eV. What does it mean? What is the relation between the work function ‘W’ and threshold wavelength ‘A’ of a metal?

    Solution

    The work function of lithium is 2.3 eV.
    This means that to remove the outermost electron from the ground shell of a lithium atom, an energy of 2.3 eV is required. 

    The relation of work function (W) and wavelength (λ) is given as, 

                      W = hv 

    i.e.,             W = hcλ. 

    Question 350
    CBSEENPH12038521

    Why are de-Broglie waves associated with a moving football not visible?
    The wavelength, X, of a photon and the de-Broglie wavelength of an electron have the same value.
    Show that the energy of the photon is 2λmch times the kinetic energy of the electron, where m, c and h have their usual meanings for electron.   




    Solution
    Because of large mass of a football, the wavelength associated with a moving football is small. So its wave nature is not visible.  

    De-Broglie wavelength of electron,
                              λ = hp
    Momentum of electron,
                             p = hλ
    Kinetic energy of electron is,= 12mv2 = p22m = h22                                      [ p = mv]

    Energy of a photon = hcλ
     Kinetic energy of photonKinetic energy of electron = hcλ.22h2 = 2λmch
              Energy of photon = 2λmcλ × K.E. of electron


    Question 351
    CBSEENPH12038522

    Red light, however bright it is, cannot produce the emission of electrons from a clean zinc surface. But even weak ultraviolet radiation can do so. Why?
    X-ray of wavelength ‘λ’ fall on a photosensitive surface, emitting electrons. Assuming that the work function of the surface can be neglected, prove that the de-Broglie wavelength of the electrons emitted will be /2mc.

    Solution

    For any material to emit photoelectrons, the threshold frequency has to be greater than or comparable to the frequency of incident radiation. Therefore, the frequency of incident light affects the emission of photoelectrons whereas, intensity does not.
    Here, the threshold frequency of zinc surface is not greater than that of the frequency of red light. Hence, no emission of electrons take place.

    The kinetic energy of photoelectron is given by,
                        12mv2max = hv - ϕ0 
    12mv2max   hv = hcλ (Neglecting the term for work function)

            m2v2max = 2mhcλ
                      p = mvmax = 2mhcλ
    But de-Broglie wavelength is given by,

                           λ = hp     = h2mhc/λ    = 2mc.
    Hence, proved.

    Question 352
    CBSEENPH12038523

    The wavelength of light in the visible region is about 390 nm for violet colour, about 550 nm (average wavelength) for yellow-green colour and about 760 nm for red colour.
    What are the energies of photons in (eV) at the (i) violet end, (ii) average wavelength, yellow-green colour, and (iii) red end of the visible spectrum? (Take h = 6.63 x 10–34 Js and 1 eV = 1.6 x 10–19J).

    Solution
    Given, 
    Wavelength of violet colour, λv = 390 nm
    Wavelength of yellow-green colour, λyg = 550 nm
    Wavelength of red color, λrλr = 760 nm

    Energy of the incident photon,
     E = hv = hcλ 

    E = (6.63 × 10-34Js) (3 × 108 ms-1)/λ 

          =  1.989×10-25Jmλ 

    (i) For violet light, λ1 = 390 nm  (lower wavelength end) 

    Incident photon energy, 

    E1 = 1.989 × 10-25Jm390 × 10-9m = 5.10 × 10-19J       = 5.10 ×10-19J1.6 ×10-19J/eV = 3.19 eV
     
    (ii) For yellow-green light, λ2 = 550 nm (average wavelength)

    Incident photon energy, 
      E2 = 1.989 × 10-25Jm550 × 10-9 m 

                                       E2 = 3.62 × 10-19J = 2.26 eV 

    (iii) For red light,λ3 = 760 nm (higher wavelength end) 

    Incident photon energy, E3 = 1.989 × 10-25Jm760 × 10-9m
                                     E3 = 2.62 × 10-19J = 1.64 eV.
    Question 353
    CBSEENPH12038524

    The following graph shown the variation of stopping potential V0 with the frequency v of the incident radiation for two photosensitive metals P and Q:

    (i) Explain which metal has smaller threshold wavelengths.
    (ii) Explain, giving reason, which metal emits photoelectrons having smaller kinetic energy.
    (iii) If the distance between the light source and metal P is doubled, how will the stopping potential change? 

    Solution
    The graph shows the variation of stopping potential Vo with frequency ν.

    (i) Suppose the frequency of incident radiations of metal P and Q be v
    0 and v0’ respectively. 
    From the graph, 

                    v0 < v0' 

                    v0 = cλ0 

                   cλ0> cλ0'cλ0 < cλ0' 

                    λ0 > λ0' 

    Therefore,  metal 'Q' has smaller wavelength. 

    (ii) As we know, energy of a photon is E = hv

                                   E   v0

    Energy is directly proportional to frequency. P has a lesser frequency.
    Hence, metal 'P' has smaller kinetc energy. 

    (iii) If the distance between the light source and metal P is doubled, stopping potential remains unaffected because the value of stopping potential for a given metal surface does not depend on the intensity of the incident radiation. It depends on the frequency of incident radiation.
    Question 354
    CBSEENPH12038525

    Light of wavelength 2000 A falls on an aluminium surface (work function of aluminium 4.2 eV). Calculate
    (a) the kinetic energy of the fastest and slowest emitted photoelectrons
    (b) stopping potential
    (c) cut-off wavelength for aluminium.

    Solution
     (a)
    We know that, 
    Energy of photon = hcλ 

                       E = 6.62 × 10-34 × 3 × 1082000 × 10-10J 

    i.e.,                 E = 6.62 ×10-34 × 3 × 1082 × 10-7 × 1.6 × 10-19eV    = 6.20 eV

    Energy of the fastest emitted photoelectron,
        = h (v – v0)    (Where v0 is the work function)
        = (6.2 – 4.2) eV
        = 2.0 eV 
     
    Since, the emitted electrons from a metal surface have an energy distribution, the minimum energy in this distribution being zero, the energy of slowest photoelectrons is also zero. 

    (b) Since,  eV0 = 12mv2max 
    where, is the maximum energy of the emitted photo electrons and V0 is the stopping potential, the stopping potential is 2V. 

    (c) The threshold frequency is related to the work function by the relation,
                   ϕ0 = hv0 = hcλ0 

     1λ0 = ϕ0hc = 4.2×1.6×10-19J6.62×10-34Js×3×108ms-1 

       λ0 = 3 × 10-7m = 3000Å , is the required cut-off wavelength for aluminum.


    Question 355
    CBSEENPH12038526

    Define the terms: (i) work function, (ii) threshold frequency and (iii) stopping potential, with reference to photoelectric effect.
    Calculate the maximum kinetic energy of electrons emitted from a photosensitive surface of work function 3.2 eV, for the incident radiation of wavelength 300 nm.    

    Solution

    Work function is the minimum amount of energy required to remove an electron to infinity, from the surface of a given metal.

    Threshold frequency is the minimum frequency of the incident light which can cause the ejection of electrons without giving them additional energy.

    The amount of potential that is required to stop the electron having the maximum kinetic energy from moving is known as stopping potential. 

    Numerical.
    The maximum kinetic energy of emitted photoelectron is given by
                  K.E. = 12mv2max = hv-ϕ0

                          E = hcλ-ϕ0
                            E = 6.6 × 10-34×3×108300 × 10-9-3.2 ×1.6×10-19

    = 6.6 × 10-19-5.12 × 10-19= 1.48 × 10-19J.

    Question 356
    CBSEENPH12038527

    In Davisson and Germer experiment if the peak diffraction pattern is obtained at the voltage of 54 V, find the wavelength associated with the electron used for obtaining the diffraction pattern. What should be the angle corresponding to this voltage, which gives maximum diffraction.

    Solution

    Given, 
    Voltage, V = 54 V

    Using the formula, 
                                 λ = 1.227V     = 1.22754    = 0.165 nm    = 1.65 Å 

    From Bragg's law,    2d sin θ =  = λ    [For first order diffraction, n = 1] 

    For Ni crystal,      
    Inter-atomic spacing, d = 0.91 Å 
    Substituting this in the formula, 
    We have, 
             2 × 0.91 × 10-10 sin  θ = 1.65 × 10-10 

                                              θ = 65°
    But,                                    θ = 12(180° - ϕ)
    Hence,
    for θ = 65°, the scattering angle, ϕ = 50°.

    Question 357
    CBSEENPH12038528

    Light of wavelength 5000 A falls on a sensitive plate with work function 1.90 eV. Calculate (a) the energy of the photon in eV, (b) kinetic energy of the emitted photoelectrons and (c) stopping potential.

    Solution
    Given,
    Planck's constant, h = 6.62 x 10
    –34 Js.
    (a) energy of a photon, E = hv  

                                            = hcλ= 6.62×10-34×3×1085000×10-10J

    i.e.,                              E = 6.62 ×35×10-19J

                                           = 6.62 × 35 × 1.6 × 10-19×10-19eV= 2.48 eV

    (b) Kinetic energy of the emitted photoelectrons,

                                       K.E. = E-ϕ0           = (2.48-1.90) eV          = 0.58 eV

    (c) Stopping potential is given by, eV0 = K.E.   
                                                         V0 = K.E.e      = 0.58 eVe      = 0.58 V.

    Question 358
    CBSEENPH12038529

    A proton and an electron have same de-Broglie wavelength which of them moves fast and which possesses more K.E. Justify your answer.

    Solution
    Kinetic energy of particle of mass m having momentum p is, 
                       K.E = 12p2m                   p = 2mK 

    De-Broglie wavelength, λ = hp = h2mK 

                                    p = hλ                  ....(i)
    and,
                                      K = h222             ....(ii) 

    If λ is constant, then from equation (i), p = constant. 

    i.e.,               mpvp = meve     

                          vpve = memp<1   or      vp<ve

    If λ is constant, then from (ii), K 1m
                        KpKe = memp<1   

                               Kp<Ke 

    It means the velocity of electron is greater than that of proton. Kinetic energy of electron is greater than that of proton.
    Question 359
    CBSEENPH12038530

    For a photosensitive surface, threshold wavelength is λ0. Does photoemission occur, if the wavelength (λ) of the incident radiation is (a) more than λ0 (b) less than λ0? Justify your answer. 

    Solution
    Einstein's photoelectric equation gives us,
                     hv = hv0+12mv2max 

                   hcλ = hcλ0+12mv2max

    (a) When, λ > λ0,  12mv2max is negative. Therefore, photoemission will not occur. 

    (b) When λ > λ0,  12mv2max is negative. So, photoemission will occur.
    Here, λo is the threshold wavelength.
    Question 360
    CBSEENPH12038531

    Find the maximum velocity of photoelectrons emitted by radiation of frequency 3 x 1015 Hz from a photoelectric surface having a work function 4.0 eV.

    Solution
    Given, 
    Frequency of radiation, ν = 3 x 1015 Hz 
    Work function of the material, ϕo = 4.0 eV

    As per Einstein's photoelectric equation, 

                    12mv2max = hv-ϕ0 

                           = 6.63 × 10-34 × 3 × 1015-4×1.6 ×10-19 

            v2max = 2[19.89 ×10-19-6.4×10-19]9.1 × 10-31

                        =  26.98 × 10-199.1 × 10-31 = 2.96 × 1012 

                 vmax = 1.72 × 106 ms-1. is the required maximum velocity of photoelectrons.
    Question 361
    CBSEENPH12038532

    Find the de-Broglie wavelength of neutron at 27°C. Given, Boltzmann constant, 1.38 x 1023 J molecule–1 k–1, h = 6.63 x 10–34 Js; mass of neutron 1.66 x 10–23 kg.

    Solution

    Here,
    Temperature, T = 27°C = 27 + 273 = 300 K.
    Mass of neutron, m = 1.66 x 10–23 kg.

    Energy of neutron at temperature Tk is, 

                       E = 32kT    = 32×1.38 × 10-23 × 300   = 6.21 × 10-21J
    Now,

                      λ = h2mE    = 6.63 ×10-342×1.66×10-27×6.21×10-21
    i.e.,            λ = 1.46 Å, is the de-broglie wavelength of the neutron.

    Question 362
    CBSEENPH12038533

    Ultraviolet light of wavelengths 800 Å and 700 Å, when allowed to fall on hydrogen atom in their ground state, is able to liberate electrons with kinetic energy 1.8 eV and 4.0 eV respectively. Find the value of Planck's constant.

    Solution
    The energy E is related to wavelength λ, velocity of light c and Planck’s constant by the relation,
            E = hcλ                                       (h  Planck's constant) 

    For radiations of wavelengths λ1 and λ2 respectively, energies E1 and E2

    Energy, E1 = hcλ1  and E2 = hcλ2 

    On subtracting the two,
                    E1-E2 = hc 1λ1-1λ2

                        h = (E1-E2)λ1 λ2c(λ2-λ1) 

     h = (4.0 - 1.8) ×1.6×10-19×700×10-10×800 × 10-103 × 108 × 100 × 10-10 

    i.e.,         h = 6.57 × 10-34Js. is thevalue of the planck's constant.

    Question 363
    CBSEENPH12038534

    Show, on a graph the nature of variation of the (associated) de-Broglie wavelength (λ) with the accelerating potential (V), for an electron initially at rest.

    Solution
     

    The above graph shows the variation of de-broglie wavelength λ with accelerating potential, V.
    Question 364
    CBSEENPH12038535

    A proton and an alpha particle, both initially at rest, are (suitablly) accelerated so as to have the same kinetic energy. What is the ratio of their de-Broglie wavelengths?


    Solution
    Given, a proton and an alpha particle, both initially at rest are accelerated such that they have the same kinetic energy.

    De-broglie wavelength is given by,
                   λ = hp = h2mE           (for same K.E) 

    Therefore, the ratio of their de-broglie wavelength is, 
              λpλα = mαmp = 4mm = 2.
    Question 365
    CBSEENPH12038536

    What two main observations in photoelectricity led Einstein to suggest the photon theory for the interaction of light with the free electrons in metal? Obtain an expression for threshold frequency for photoelectric emission in terms of the work function of the metal.

    Solution

    The two main observations are: 

    (i) The maximum kinetic energy of emitted photoelectron is independent of intensity of light. 

    (ii) For each photoelectron, there must be a threshold frequency of incident light below which no emission takes place. 

    For a metal of work function ɸ, the kinetic energy of photoelectron emitted due to falling of photon of frequency v is, 
                           12mv2max = hv - ϕ                     = hv - hv0 

    where v0 is the threshold frequency. 

    For photoelectric emission, 

                           vmax = 0 

                          hv = hv0 = ϕ 

    or                      v0  = ϕh.
    gives us the relationship between threshold frequency and work function of the metal.

    Question 366
    CBSEENPH12038537

    The maximum velocity of electrons, emitted from a metal surface of negligible work function is v, when frequency of light falling on it is f. What will be the maximum velocity when the frequency of incident light made 4f?

    Solution
    Maximum velocity of electrons = v
    Frequency of incident light = f

    Max. velocity when incident light is 4f = ?

    Using Einstein's photoelectric equation, we have

                        1 half mv subscript straight x squared space equals space hf space minus space straight ϕ
    Since, work function is negligibe, straight ϕ space equals space 0 

                       straight v subscript straight x squared space equals fraction numerator 2 hf over denominator straight m end fraction comma space space straight v subscript straight x space equals space square root of fraction numerator 2 hf over denominator straight m end fraction end root 

    Thus, for frequency, straight f apostrophe space equals space 4 straight f 

    we have,               straight v subscript straight x apostrophe space equals space square root of fraction numerator 2 straight h 4 straight f over denominator straight m end fraction end root space equals space 2 straight v subscript straight x 

    Thus, maximum velocity will be doubled when, frequency is made 4 times.
    Question 367
    CBSEENPH12038538

    What reasoning led de-Broglie to put forward the concept of matter wave? The wavelength λ, of a photon, and de-Broglie wavelength associated with a particle of mass m has the same value, say λ. Show that the energy of photon is 2λmch times the kinetic energy of the particle.

    Solution
    De-broglie reasoned that nature is symmetrical and that the two basic physical entities, matter and energy must have symmetrical character. This led him to put forward the bold hypothesis that moving particles of matter should display wave-like properties under suitable conditions. If radiation shows a dual nature, so should matter exhibit dual radiation.

    Now, kinetic energy is given by, 

                            K.E = P22m              P = hλ
                     K.E = h222 

    Also, Energy of a photon = hcλ 

                                KE = h2mcλ

                                 E = 2mcλh. K.
    Question 372
    CBSEENPH12038543
    Question 383
    CBSEENPH12038554

    The photosensitive surface is receiving light of wavelength 5000 A at the rate of 10–8 Js–1. Find the number of photons received per second.

    Solution

    Wavelength of the photon, λ = 5000 Ao = 5000× 10-10 m 

    Rate at which the photons are emitted = 10-8 J/s 

    So, number of photons emitted, n = 
    n = Ehcλ= 10-86.6×10-34×3×1085000×10-10 = 252 × 108 photons

    Question 384
    CBSEENPH12038555

    In Davisson and Germer experiment, state the observations which led to (i) show the wave nature of electrons and (ii) confirm the de-Broglie relation.

    Solution

    i) In Davison and germer experiment,

    The appearance of peak in a particular direction is due to constructive interference of electrons scattered from different layers of regularly spaced atoms of the crystal, i.e., the diffraction of electrons take place. This established the wave nature of electron. 

    ii) According to Davison- Germer experiment, the wavelength of the wave is found out to be 1.65 Ao

    According to De- Broglie hypothesis, wavelength is given by 1.66 Ao

    There is a close agreement with the estimated value of both experiments. 

    Hence, the De-broglie relation is established. 

    Question 385
    CBSEENPH12038556

    Derive the expression for the de-Broglie wavelength of an electron moving under a potential difference of V volt.
    Describe the Davisson and Germer experiment to establish the wave nature of electrons. Draw labelled diagram of the apparatus used.  


    Solution

    Consider an electron of mass 'm' and charge 'e'. Let v be the velocity acquired by electron when accelerated from rest through a potential difference of V volt. 

    Gain in K.E of electron = 12mv2 
    Work done = eV

    If λ is the De- Broglie wavelegth assosciated with the electron, then 

    λ = hmv = hm 2eV/m = h2meV

    In order to establish the wave nature of electrons an experiment was performed by Davison and Germer. 

    i) A fine beam of accelerated electrons obtained from electron gun is made to fall normally on the surface of nickel crystal.

    ii) Incident electrons are scattered in different directions by the atoms of the crystals.
    iii) Intensity of the elctron beam,  is scattered in a different direction. 

    iv) By rotating the electron detector on circular scale at different positions, intensity of the scattered beam is measured for different values of scattering angle φ.

    v) The experiment was performed by varying the accelerating voltage 44 V to 68 V. 

    vi) In an accelerating voltage at 54 V, a graph with axis of variation of intensity (I) and scattering angle (φ) was plotted. 

    vi) The appearance of peak in a particular direction is due to constructive interference of electrons scattered from different layers of regularly spaced atoms of the crystal, i.e., the diffraction of electrons takes place. 

    This established the wave nature of electrons. 



    Question 386
    CBSEENPH12038557

    When a surface is irradiated with light of λ = 4950 Å, a photocurrent appears which vanishes if a retarding potential greater than 0.6 V is applied across the photo tube. When a different source of light is used, it is found that the critical retarding potential is changed to 1.1 V. What is the work function of the surface and the wavelength of the second source? If the photoelectrons (after emission from the source) are subjected to a magnetic field of 10 tesla what changes will be observed in the above two retarding potentials?

    Solution
    Given, wavelength of light used, λ = 4950 Ao 
    Stopping potential, Vo = 0.6 V
    Magnetic field, B = 10 T

    According to Einstein's photoelectric equation, we have 
                  12mv2max = eV0 = hv-v0      ... ( 1)

                      eV0 = hcλ-ϕ0 

    where,
    ɸ0 is the work function,
    X wavelength of incident light and
    V0 is the stopping potential. 

    For the first source,
                               λ1 = 4950 Å = 4950 × 10-10mV0 = 0.6 V 

    Putting these values in equation 1, 
          1.6 × 10-19 × 0.6 = 6.6 × 10-34 ×3 × 108495 ×10-9-ϕ0

                 0.96×10-19 = 4×10-19-ϕ0 

                                 ϕ0 = 3.04 × 10-19J             ...(I)
                                         = 3.04 × 10-191.6 ×10-19eV= 1.9 eV 

    Let λ2 be the wavelength of the second source.
    Stopping potential, V0’ = 1.1 V (given) 

    Therefore, 1.6 ×10-19 ×1.1 = 6.6 ×10-34×3×108λ2-3.04 × 10-19J     (from I)
      1.76 × 10-19 = 19.8 ×10-26λ2-3.04 ×10-19 

              19.8 × 10-26λ2 = 4.8 × 10-19
        λ2 = 19.8 × 10-264.8 × 10-19m = 4.125 × 10-7m
                                              = 4125 Å 

    When the ejected photoelectrons are subjected to the action of a magnetic field no change in retarding potential will be observed because, a magnetic field does not alter the kinetic energy of the photoelectrons. The magnetic field only changes the direction of motion.


    Question 392
    CBSEENPH12038563

    Suppose you are given a chance to repeat the alpha-particle scattering experiment using a thin sheet of solid hydrogen in place of the gold foil. (Hydrogen is a solid at temperatures below 14 K.) What results do you expect?

    Solution
    The nucleus of a hydrogen atom is a proton of mass 1.67 × 10–27 kg which has only about one-fourth of the mass of an alpha particle (6.64 × 10–27 kg). Alpha particle is more massive and it won't bounce back in even a head-on collision with a proton. It is like a bowling ball colliding with a ping-pong ball at rest. Thus, there would be no large angle scattering in this case. 

    In Rutherford's experiment, by contrast, there was large-angle scattering because a gold nucleus is more massive than an alpha-particle. The analogy is there is a ping-pong ball hitting a bowling ball at rest. 
    Question 393
    CBSEENPH12038564

    What is the shortest wavelength present in the Paschen series of spectral lines?

    Solution
    For the shortest wavelength in Paschen series, 
    n2 and n1 = 3 

    Using Rydberg's formula, 

                      1λ = R 1n12 - 1n22  

    where, the value of R is 1.097 × 10m-1.

    Therefore,

                     1λmin = R132-12 = R9

                   λmin = 9R = 91.097 × 107m

    i.e.,              λmin = 9 × 10-7 × 10101.097Å

                              = 8204.2 Å, is the value of the shortest wavelength.
    Question 394
    CBSEENPH12038565

    A difference of 2.3 eV separates two energy levels in an atom. What is the frequency of radiation emitted when the atom make a transition from the upper level to the lower level?

    Solution
    Difference between energy levels, E2-E1 = 2.3 eV                                                                            = 2.3 × 1.6 × 10-19JFrequency of the emitted radiation is,  v  = E2-E1h                                                                    v = 2.3 × 1.6 × 10-196.6 × 10-34 
                                                        v = 3.68 × 10156.6
                                                                = 0.557 × 1015Hz= 5.6 × 1014Hz.
    Question 395
    CBSEENPH12038566

    The ground state energy of hydrogen atom is – 13.6 eV. What are the kinetic and potential energies of the electron in this state?

    Solution
    Here,

    Ground state Energy, E = – 13.6 eV 

    Kinetic Energy, Ek = 14πε0.e22r and, 
    Potential Energy, Ep = -14πε0e2r

       Ep = -kq1q2r   and    [Ek = 2Ep] 

    Therefore, total energy, E = Ek+Ep 

                           = 14πε0.e22r-14πε0.e2r 

                        E = -1214πε0.e2r 

           -13.6  = - 1214πε0.e2r 

       14πε0e2r = 27.2 

               
    Kinetic energy,    Ek = 14πε0.e22r     = 27.22eV     = 13.6 eV 

    Potential energy, Ep = -14πε0.e2r     = -27.2 eV. 
    Question 396
    CBSEENPH12038567

    The radius of the innermost electron orbit of a hydrogen atom is 5.3 × 10–11 m. What are the radii of the n = 2 and n = 3 orbits?

    Solution

    Given,
                            Radius of the innermost electron orbit, r0 = 5.3 × 10-11m

    As oper the formula of radius of orbit,   r = r0 . n2 

    (i) When, n = 2  

    Radius, r =  5.3 × 10-11 × (2)2 

               r = 21.2 × 10-11m   = 2.12 × 10-10m       

    (ii) When n= 3 

    We have,  

    Radius, r =  5.3 × 10-11 m × (3)2
                 = 47.7 × 10-11m = 4.77 × 10-10m.

    Question 397
    CBSEENPH12038568

    A 12.5 eV electron beam is used to bombard gaseous hydrogen at room temperature. What series of wavelengths will be emitted?

    Solution
    In ground state, energy of gaseous hydrogen at room temperature = – 13.6 eV.

    Energy of electron beam used to bombard the gaseous hydrogen = 12.5 eV 

    Therefore, after bombardment,
    Energy of gaseous hydrogen = –13.6 + 12.6
                                               = – 1.1 eV.

    Since, En = -13.6n2       
     So,          n2 = -13.6-1.1 = 12.3        n  = 3 

    That is, the electron would jump from n = 1 to n = 3, where E3 = -13.632 = -1.5 eV. 
    On de-excitation, the electron may jump from n = 3 to n = 2 giving rise to Balmer series.

    It may also jump from n = 3 to n = 1, giving rise to Lyman series. 


    So, number of spectral line is,

    = n(n-1)2 = 3(3-1)2 = 3 

    Thus, three spectral lines appear.

    Question 398
    CBSEENPH12038569

    In accordance with the Bohr's model, find the quantum number that characterises the earth's revolution around the sun in an orbit of radius 1.5 × 1011 m with orbital speed 3 × 104m/s. (Mass of earth = 6.0 × 1024 kg.)

    Solution
    Given, 
    Radius of the orbit, r = 1.5 × 1011 m 
    Orbital speed, v = 3 × 104m/s. 
    Mass of the earth, m = 6.0 × 1024 kg

    Now, according to Bohr's theory
                       mvr = nh2π 

    or,                   n= 2π mvrh 
                        

                           
                             = 2.56 × 1074.
    Question 399
    CBSEENPH12038570

    A hydrogen atom initially in the ground level absorbs a photon, which excites it to the n = 4 level. Determine the wavelength and frequency of photon.

    Solution
    Initially, hydrogen is in the ground state. 
    After absorption of photon Hydrogen atom excited to level, n=4.

    Energy of an electron in n
    th orbit of H atom is, 

                                      En = -13.6n2eVwhen n=1;           E1 = -13.6 eV 

    Energy in 4th (n = 4) level 

                      E4 = -13.642 = -0.85
                 E = E4-E1

                                                           E = -0.85 - (-13.6) eV                                             = -0.85 + 13.6                                 E =12.75 eV  Now, energy of a photon = hνTherefore,                                     hv  = 12.75 eV                                 hv = 12.75 × 1.6 × 10-19J                                   v = 12.75×1.6×10-196.6 ×10-34i.e.,                                v = 3.078 ×1015 Hz, is the required frequency of the photon.Now, wavelength of photon is ,                                       λ = cλ = 3 × 1083.078 × 1015i.e.,                               λ = 974.4 Å
    Question 400
    CBSEENPH12038571

    (a) Using the Bohr's model calculate the speed of the electron in a hydrogen atom in the n = 1, 2, and 3 levels. (b) Calculate the orbital period in each of these levels.

    Solution

    (a) From the relation, 

    v = cnα,      where   α = 2π Ke2ch = 0.0073

    Therefore, the speed of electron in hydrogen atom in n=1, 2 and 3 is given by, 
                        v1 = 3×1081×0.0073 = 2.19×106 m/sv2 = 3×1082×0.0073 = 1.095 ×106 m/sv3 =3×1083×0.0073 =7.3×105 m/s.

    (b) Orbital period in each of the level is given by, 

    T = 2πrv  As  r1 = 0.53×10-10m  

    T1 = 2π×0.53×10-102.19×106= 1.52×10-16s ' 

    As,  r2 = 4 r1    and   v2  = 12v1 

             T2 =  8 T1      = 8 × 1.52 × 10-16s      = 1.216 × 10-15s 

    Also as, r3 = 9 r1   and  v3 = 13v1 
     T3 = 27 T1 = 27 × 1.52 × 10-16s                      = 4.1 × 10-15 s. 

    T1, T2 and T3 are respectively the orbital time period for n1, nand n3

    Question 402
    CBSEENPH12038573

    Answer the following questions, which help you understand the difference between Thomson's model and Rutherford's model better.
    Is the probability of backward scattering (i.e., scattering of α-particles at angles greater than 90°) predicted by Thomson's model much less, about the same, or much greater than that predicted by Rutherford's model?

    Solution
    In rutherford's model we have a large massive core called the nucleus whereas, in thomson's model we do not have. Thus, the probability of backward scattering predicted by Thomson's model is much less than that predicted by Rutherford model.
    Question 403
    CBSEENPH12038574

    Answer the following questions, which help you understand the difference between Thomson's model and Rutherford's model better.
    Keeping other factors fixed, it is found experimentally that for small thickness t, the number of α-particles scattered at moderate angles is proportional to t. What clue does this linear dependence on t provide?

    Solution
    It suggests that scattering is predominantly due to a single collision, because the chance of a single collision increases linearly with the number of target atoms, and hence linearly with the thickness of the foil.
    Question 404
    CBSEENPH12038575

    Answer the following questions, which help you understand the difference between Thomson's model and Rutherford's model better.
    In which model is it completely wrong to ignore multiple scattering for the calculation of average angle of scattering of α-particles by a thin foil?

    Solution

    In Thomson's model, a single collision causes very little deflection. Multiple scattering has to be taken into account inorder to explain the average angle of scattering. So it is wrong to ignore multiple scattering in Thomson's model.
    On the contrary, in Rutherford's model, most of the scattering comes through a single collision and multiple scattering effects can be ignored as a first approximation.

     
    Question 405
    CBSEENPH12038576

    The gravitational attraction between electron and proton in a hydrogen atom is weaker than the coulomb attraction by a factor of about 10–40. An alternative way of looking at this fact is to estimate the radius of the first Bohr orbit of a hydrogen atom if the electron and proton were bound by gravitational attraction. You will find the answer interesting.

    Solution
    The radius of the first orbit of hydrogen atom in Bohr's model is given by,  
                r = ε0 h2π me2 Multiplying and dividing by 4π r= 4πε0e2h24π2m  
    Therefore, 

    Radius,  r = n2h24π2mkZe2      here k = 14πε0          Z = 1,   n = 1 

    If electrostatic force 14πε0.e2r2 is replaced by gravitational force GMmr2, we put GMm in place of e24πε0 in above expression. 

    Hence, radius of first orbit under gravitational force,
              rG = 1GMm.h24π2m 

                 = h24π2GMm2 , where     M = mass of protonm = mass of electron 

    rG = (6.26 × 10-34)24 × (3.14)2 (6.67 ×10-11) × (1.672 × 10-27) × (9.1 ×10-31)2 

            = 6626×6626×10-744×3.14×3.14×667×16724×19×19×10-112 = 1.21 ×1029 m. 

    The radius of the first orbit, when electron and proton are bounded together under the influence of graviatational force, turns out to be larger than the size of the universe. 


    Question 406
    CBSEENPH12038577

    Obtain an expression for the frequency of radiations emitted when a hydrogen atom de-excites from level n to level (n – 1). For large n, show that the frequency equals the classical frequency of revolution of the electron in the orbit.

    Solution
    The frequency v of the emitted radiation when a hydrogen atom de-excites from level n to level (n — 1) is given by, 
                    E = hv = E2-E1 v = 12mc2α2h1n12-1n22  where   α = 2πKe2ch = fine structure constant v = 12mc2α2h1(n-1)2-1n2 = mc2α22h  n2-(n-1)2n2 (n-1)2   = mc2α2(n+n-1) (n-n+1)2hn2 (n-1)2v = mc2α2(2n-1)2h n2 (n-1)2. 

    For large n, (2n - 1)2n,   and 

                        (n - 1) n

    Therefore,   v = mc2α2. 2n2h n2. n2 = mc2α2hn3

    On putting,
             α = 2π Ke2ch,   we get   v = mc2hn3.4π2K2e4c2h2 

    i.e.,    v = 4π2mK2e4n3h3               ... (1)

    In Bohr's atomic model, velocity of electron in nth orbit is, v = nh2π mr ; and 

    Radius of nth orbit is, r = n2h24π2mKe2              (  Z = 1) 

      Frequency of revolution of electron is, 

    v = v2πr = nh2π mr4π2mKe22π. n2h2 

                 v = Ke2nh .r = Ke2nh4π2mKe2n2h2v = 4π2mK2e4n3h3  which is same as (1). 

    Hence proved that, for large values of n, classical frequency of revolution of electron in nth orbit is the same as the frequency of radiation emitted when hydrogen atom de-excites from level (n) to level (n – 1).

    Question 407
    CBSEENPH12038578

    Classically, an electron can be in any orbit around the nucleus of an atom. Then what determines the typical atomic size? Why is an atom not, say, thousand times bigger than its typical size? The question had greatly puzzled Bohr before he arrived at his famous model of the atom that you have learnt in the text. To simulate what he might well have done before his discovery, let us play as follows with the basic constants of nature and see if we can get a quantity with the dimensions of length that is roughly equal to the known size of an atom (~ 10-10m).
    (a) Construct a quantity with the dimensions of length from the fundamental constants e, me and c. Determine its numerical value.
    (b) You will find that the length obtained in (a) is many orders of magnitude smaller than the atomic dimensions. Further, it involves c. But energies of atoms are mostly in non-relativistic domain where c is not expected to play any role. This is what may have suggested Bohr to discard c and look for 'something else' to get the right atomic size. Now, the Planck's constant h had already made its appearance elsewhere. Bohr's great insight lay in recognising that h, me and e will yield the right atomic size. Construct a quantity with the dimension of length from h, mc, and e and confirm that its numerical value has indeed the correct order of magnitude.


    Solution
    (a) Coulomb's law of force between hydrogen nucleus and electron gives us, 

                     F = 14πε0.e.er2 

                 r = 14πε0e.eF.r 

    Now, using the fundamental constants e, me and c, we will obtain a quantity which has the dimensions of length.
    But, 
    F.r (force x distance) gives us the work or energy = mc
    2
                               r = 14πε0e2mc2 = 2.8 × 10-15 m. 

    which is much smaller than typical atomic size. 

    (b) From Bohr's formula for first hydrogen orbit, 

    we have r = ε0h2πme2 = 0.53 × 10-10m 

    which is of the order of atomic size.
    Question 408
    CBSEENPH12038579

     The total energy of an electron in the first excited state of the hydrogen atom is about – 3.4 eV.
    (a) What is the kinetic energy of the electron in this state?
    (b) What is the potential energy of the electron in this state?
    (c) Which of the answers above would change if the choice of the zero of potential energy is changed?

    Solution

    In Bohr's model, as per the quantisation of angular momentum we have,

           mvr = nh2π  ; and 

         mv2r = Ze24πε0r2 

    which gives 
    Kinetic energy, Ek = 12mv2 = Ze28πε0r;   r  = 4πε0h2Ze2mn2. 
    Here, we have 14πεo = K 
     Kinetic energy, K.E = Kze22r 

    These relations have nothing to do with choice of the zero of potential energy.

    Now, choosing the zero of potential energy at infinity, we have 

     Ep = -Ze24πε0r= -kZe2r which gives, Ep = -2 Ek
    Ep is the potential energy. 

    Thus, total energy, E = Ek+EP = -Ek

    (a) The quoted value of E = – 3.4 eV is based on the customary choice of zero of potential energy at infinity.
    From the above result of E = – Ek, the kinetic energy of electron in this state is + 3.4 eV. 

    (b) Using Ep = – 2 Ek, potential energy of the electron is – 2 × 3.4 eV = – 6.8 eV. 

    (c) If the zero of potential energy is chosen differently, kinetic energy does not change. Its value is + 3.4 eV. This is independent of the choice of the zero of potential energy.

    The potential energy, and the total energy of the state, however, would alter if a different zero of the potential energy is chosen.



    Question 409
    CBSEENPH12038580

    If Bohr's quantisation postulate (angular momentum = nh/2π) is a basic law of nature, it should be equally valid for the case of planetary motion also. Why then do we never speak of quantisation of orbits of planets around the sun?

    Solution
    1. Bohr's quantisation postulate is in terms of h. Angular momenta associated with planetary motion are incomparably large relative to h.
    2. For example, angular momentum of the earth in its orbital motion is of the order of 10
    70 h. In terms of the Bohr's quantisation postulate, this corresponds to a very large value of n (of the order of 1070).
    3. For such enormous values of n, the differences in the successive energies and angular momenta of the quantised levels of the Bohr model is so small as compared to the energy levels and angular momenta that one can practically consider as continuous. 
    Question 410
    CBSEENPH12038581

    Obtain the first Bohr's radius and the ground state energy of a muonic hydrogen atom [i.e., an atom in which a negatively charged muon (μ) of mass about 207 me orbits around a proton].

    Solution
    Mass of muon, Mμ = 207 me 

    The first Bohr's radius of Hydrogen atom is given by, 
    r1 = 4πε0 h24π2mee2    = 5.29 × 10-11m 

    If r1' is the first Bohr's radius of muonic hydrogen atom, then
     r1' = 4πε0h24π2(207 me)e2     =5.29 ×10-11207    = 2.5 × 10-12m 

    The ground state (n = 1) energy of H-atom is given by, 

    E1 = -14πε02.2π2mee2h2 = 13.6 eV  

    If E1' is ground state energy of muonic hydrogen atom, then we have 

    E1' = -14πε02. 2π2(207 me) e2h2      = -13.6 × 207      = -2815.2 eV.
    Question 411
    CBSEENPH12038582

    In a Rutherford's α-scattering experiment with thin gold foil, 8100 scintillations per minute are observed at an angle of 60°. What will be the number of scintillations per minute at an angle of 120°?

    Solution
    Given,
    Number of scintillations per minute at an angle 60°, n1 = 8100 m
    Number of scintillations per minute at an angle 120° , n2 =? 

    The scattering in the Rutherford's experiment is proportional to cot4ϕ2. 

             n2n1 = cot4ϕ2/2cot4ϕ1/2  

    Therefore,
     
              n2n1 = cot4120°2cot460°2         = cot 4 60°cot4 30°        = 1334         = 181 
    This implies, 

           n2 = 181× n1     = 181×8100     =100.



    Question 412
    CBSEENPH12038583

    Name the series of hydrogen spectrum lying in the infrared region.

    Solution
    The series of hydrogen spectrum lying in the infra-red region are Paschen series, Brackett series and Pfund series.
    Question 413
    CBSEENPH12038584

    Can a hydrogen atom absorb a photon having energy more than 13.6 eV?

    Solution
    Yes, a hydrogen atom can absorb a photon having energy more than 13.6 eV. But the atom should be ionised for this to happen.
    Question 414
    CBSEENPH12038585

    Name the series of hydrogen spectrum which does not lie in the visible region.

    Solution
    Lyman series of the hydrogen spectrum does not lie in the visible region. 
    Question 415
    CBSEENPH12038586

    Which of the following given transitions in a hydrogen atom emits the photon of lowest frequency?
    (i) n = 2 to n = 1
    (ii) n = 4 to n = 3.

    Solution
    (ii) n = 4 to n = 3 

    As n increases, the energy levels gradually gets more closer. And, as a result hydrogen atom emits photon of lowest frequency in the transition. 
    Question 416
    CBSEENPH12038587

    The shortest wavelength in the Lyman Series is 911.6 Å. Then the longest wavelength in the Lyman's series will be?

    Solution
    Given, shortest wavelength in the lyman series = 911.6 A0 

    For the Lyman Series,

    we have   λLλs = 43 

    Hence,       λL = 43 × λS 

                 λL = 43×911.6 Å 

                         = 1215 Å , will be the longest wavelength in the lyman series. 
    Question 417
    CBSEENPH12038588

    Name the series of hydrogen atom spectrum which lies in the visible region.

    Solution
    Balmer Series lies in the visible region of the hydrogen atom spectrum. 
    Question 418
    CBSEENPH12038589

    What are the values of first and second excitation potential of hydrogen atom?

    Solution
    Excitation potential is the amount of energy required in electron volt to excite the atom from it's ground state to a higher state. 
    When there is transition from n=1 to n=2 we will have first excitation potential.  

    For hydrogen atom,
    First excitation potential = -3.4 - (-13.6) eV= 10.2 eV 

    When electron jumps from n=1 level to n=3 level, we will have second exciation potential.

    Second excitation potential = - 1.5 - (-13.6)= 12.09 eV.
    Question 419
    CBSEENPH12038590

    What is the ratio of volume of atom to the volume of nucleus?

    Solution
    Scattering of alpha particle experiment suggested that radius of nucleus was smaller than the radius of atom by a factor of 4. 
    Therefore, 
    Ratio of the volume of atom to the volume of a nucleus is 1012 .
    Question 420
    CBSEENPH12038591

    If electron-orbits with principal quantum number n > 3 were not allowed, what would be the number of possible elements?

    Solution
    The maximum number of electrons that can be accommodated in orbits with n = 3 is
    2 × 12 + 2 × 22 + 2 × 32 = 28.
    Question 421
    CBSEENPH12038592

    What is the impact parameter for scattering of α-particle by 180°?

    Solution
    The formula for impact parameter is ,
     
     Impact parameter,  b = Ze2cotθ24πε012mv2 

    We will have cot 90o= 0. 
    Therefore, 
    Impact parameter is zero. 
    Question 422
    CBSEENPH12038593

    How many times does the electron go round the first Bohr orbit in a second?

    Solution
    The frequency of electron is given by, 

                         v = v2πr  
    where, vis the velocity with which the electrons are moving and, 
    r is the radiusof the hydrogen atom.

    Velocity, v = 2.2 × 106 m/s 
    radius of the orbit, r = 0.5287 × 10-10

      f = 2.2×1062×3.14×0.5287×10-10 = 6.6 × 1015 Hz


       
    Question 423
    CBSEENPH12038594

    The Rydberg constant for hydrogen is 10967700 m–1. Calculate the short and long wavelength limits of Lyman series.

    Solution
    For Lyman series, the wave number is given by
    v = 1λ = RH 112-1n2 

    For the short wavelength limit (λ = λs), n = ∞ 

              vs¯ = 1λs = RH 112-12 = RH

              λs = 1RH = 110967700m     = 9.116 × 10-8m    = 911.6 Å 

    For long wavelength limit (λ = λL.), n = 2 

        v¯L = 1λL = RH112-122 = 34RH

    So,
                 λL = 43 RH   

                    = 43×911.6 Å = 1215 Ao         

    Question 424
    CBSEENPH12038595

    The energy of the electron, the hydrogen atom, is known to be expressible in the form
    En = -13.6 eVn2    (n =1, 2, 3, ....)
    Use this expression to show that the
    (i) electron in the hydrogen atom can not have an energy of – 2 V.
    (ii) spacing between the lines (consecutive energy levels) within the given set of the observed hydrogen atom spectrum decreases as n increases.


    Solution

    Energy for the hydrogen atom is given by,
     
             En = -13.6 eVn2 

    Putting n = 1, 2, 3............n,  we get

                                E1 = -13.612 = -13.6 eVE2 = -13.622=-13.64=3.4 eVE3 = -13.632=-13.69= -1.51 eV 

    E4 = -13.642=-13.616= -.85 V..........................................................................En = -13.62 = 0 eV

    (i) Hence, from the above expressions it can be observed that the electron in the hydrogen atom cannot have an energy of – 2V.

    (ii) As n increases, energies of the excited states come closer and closer together. Therefore, as n increases, En becomes less negative until at n = ∞, we get En = 0. 



    Question 425
    CBSEENPH12038596

    Calculate the nearest distance of approach of an α-particle of energy 2.5 eV being scattered by a gold nucleus (Z = 79).

    Solution
    Energy of the α - particle = 2.5 eV 
    Atomic number of the gold nucleus, Z = 79 

    The potential energy of an α-particle when it is at a distance x, from the nucleus is given by,

    PE = Ze4πε0x2e = 2Ze2(4πε0x)' 

    '2e' being the charge on α-particle.

    Since the α-particle is momentarily stopped at a distance x, its initial kinetic energy is completely changed into potential energy here.

    Hence, 
    12m v2 = 2Ze24πε0x           (at nearest approach K.E. = P.E.)

        x = 2Ze24πε0× 1mv22         ... (1)

    Now energy of α-particle = 12m v2 = 2.5 MeV
                                          = 2.5 × 106 × 1.6 × 10-19 J= 2.5 × 1.6 × 10-13J

    Substituting values in equation (1) we get,
                                         x = 2×79×1.6×1.6×10-38×9×1092.5 ×1.6 × 10-13m

       = 9.101 × 10-14 m.
    which is the nearest distance of approach. 
    Question 426
    CBSEENPH12038597

    In Bohr's theory of hydrogen atom, calculate the energy of the photon emitted during a transition of the electron from the first excitated state to its ground state. Write in which region of the electromagnetic spectrum this transition lies.
    Given Rydberg constant R = 1.03 × 107 m–1.

    Solution
    Energy for nth level of hydrogen atom is given by, 

                          En = -13.6n2eV 

    Energy of the photon emitted during a transition of the electron from the first excited state (n=2) to its ground state (n=1) is, 

     E = E2 - E1    = -13.622--13.612    = -13.64+13.61    = -3.40+13.6     = 10.2 eV 

    This transition lies in the region of Lyman series.
    Question 427
    CBSEENPH12038598

    The wavelength of the first member of the Balmer series in hydrogen spectrum is 6563 A. What is the wavelength of the first member of Lyman series?

    Solution
    Wavelength of hydrogen spectrum in the balmer series , λ1 = 6563 Ao 

    For Balmer series, 

    1λ1 = R122-132  = 5R36

    For Lyman series,

    1λ2 = R112-122 = 3R4      λ2λ1 =43R×5R36 = 20108 = 527        λ2 = 527×λ1 = 527×6563 = 1215 Å.  

    is the wavelength of the first member of the Lyman series. 
    Question 428
    CBSEENPH12038599

    The ground state energy of hydrogen atom is - 13.6 eV.
    (i) What is the potential energy of an electron in the 3rd excited state?
    (ii) If the electron jumps to the ground state from the 3rd excited state, calculate the wavelength of the photon emitted. 

    Solution

    The energy of an electron in nth orbit is given by, En = -13.6n2eV 

    (i) For 3rd excited state, n = 4 

     Energy at the third excited level is given by, 

     E4 = -13.642= -13.616= -0.85 eV

    (ii) Required energy to jump electron to the ground state from the 3rd excited state is,

     E = E4-E1 

        = -13.642--13.612=-0.85+13.6  = 12.75 eV 

    ∴    Wavelength of the photon emitted is, 

    λ = hcE                      E = hcλ 

       λ = 6.63 ×10-34 ×3 ×10812.75 ×1.6 ×10-19

             = 19.878×10-720.4=0.974 ×10-7 = 974 Å.  
    is the wavelength of the photon emitted. 


     

    Question 429
    CBSEENPH12038600

    If the average life time of an excited state of hydrogen is of the order of 10–8 s, estimate how many rotation an electron makes when it is in the state n = 2 and before it suffers a transition to state n = 1. Bohr radius = 5.3 × 10–11 m.

    Solution
    Average lifetime of an excited state of hydrogen = 10-8 sec 
    Bohr radius, r = 5.3 × 10-11

    Velocity of electron in the nth orbit of hydrogen atom,

                 vn = v1n = 2.19 ×106nm/s
      
                   
    If,     n = 2,   vn = 2.19 ×106nm/s 

    Radius of n = 2 orbit,  

    rn = n2r1 = 4 × Bohr radius

      rn = 4 × 5.3 × 10-11m 

    Number of revolutions made in 1 sec
                                          = vn2πr = 2.19 ×1062 ×2π ×4 ×5.3 × 10-11 

    Therefore, number of revolutions made in 10-8 sec, 

    = 2.19 × 106 × 10-82 × 2π ×4 × 5.3 × 10-11= 8.22 × 106 revolutions.
    Question 430
    CBSEENPH12038601

    A hydrogen atom initially in the ground state absorbs a photon; which excites it to the n = 4 level. Determine the wavelength and frequency of photon.

    Solution

    Initially, hydrogen atom is in the ground state. 
    After absorption of photon, atom is excited to n=4th level.

    USing the Rydberg's formula,
                 1λ = R1n12-1n22

    we have,   
                 1λ = 1.09 × 107 112-142       = 1.09 × 107 × 1516

              λ = 161.09 × 107 × 15   = 9.8 × 10-8m is the wavelength of the photon.


       Frequency of the photon, ν is given by,
     
              v = cλ = 3 × 1089.8 × 10-8                = 3.06 × 1015 s-1. 

    Question 431
    CBSEENPH12038602

    A doubly ionised lithium atom is hydrogen-like with atomic number 3:
    (i) Find the wavelength of the radiation required to excite the electron in Li++ from the first to the third Bohr orbit. (Ionisation energy of the hydrogen atom equals 13.6 eV.)
    (ii) How many spectral lines are observed in the emission spectrum of the above excited system?

    Solution
    Given, a doubly ionised lithium atom with atomic no. Z=3. 

    (i) The energy difference of electron in Li
    ++ between the first and the third orbit is,

                        = E3 - E1 

        E3 - E1 = 13.6 × Z21n12-1n22 

                        = 13.6×(3)2 112-132= 13.6 ×9×89×1.6×10-19J 

    Therefore, the equivalent wavelength λ is given by equating difference in energy with energy of a photon.
                E3 - E1 = hcλ 
     
                           λ = hcE3-E1                              = 6.63×10-34×3×10813.6×8×1.6×10-19                               = 1.137×10-8m                               = 113.7 Å.

    (ii) The following three spectral lines are observed due to the following transitions:
    3rd to 1st orbit
    3rd to 2nd orbit
    2nd to 1st orbit




    Question 432
    CBSEENPH12038603

    A single electron, orbits around a stationary nucleus of charge ze, where z is a constant and e is the electronic charge. It requires 47.2 eV to excite the electron from the second Bohr orbit to 3rd Bohr orbit. Find,
    (i) The value of z.
    (ii) The energy required to excite the electron from the third to the fourth Bohr orbit.
    (iii) The wavelength of electromagnetic radiation required to remove the electron from the first Bohr orbit to infinity.
    (iv) The kinetic energy, potential energy and angular momentum of the electron in the first Bohr orbit.
    (v) The radius of the first Bohr orbit.
    (Ionisation energy of hydrogen atom = 13.6 eV. Bohr radius = 5.3 × 10–11 m, velocity of light = 3 × 108 m/s and Planck's constant = 6.6 × 10–34 Js)

    Solution
    Given,
    Amount of energy required to excite the electron from second orbit to 3rd orbit = 47.2 eV

    (i) Change in energy for a general hydrogen-like atom is, En2 - En1 = Z2E01n12-1n22eV  

    where E0 is the ionisation energy of hydrogen atom.
    Now,
             E = Z2 × 13.6 122-132       = 47.2 

     
    Z2×13.636×5 = 47.2 

     
      Z2 = 47.2×3613.6×5 = 25Z = 5 

    (ii) Energy required to excite the electron from third to fourth orbit,
     
          E4-E3 = 52×13.6132-142eV
                     = 25×13.6×7144 = 16.53 eV

    (iii) Energy required to excite the electron from ground state to infinity, 

    E - E1 = Z2 × 13.6 112-1                   = 13.6 × 25 eV

    Thus, wavelength of electromagnetic radiation required to remove the electron from first Bohr orbit to infinity is,

    λ = hcE   = (6.6 × 10-34) × 3 × 10813.6 × 25 × 1.6 × 10-19    = 0.03640 × 10-7    = 36.4 × 10-10    = 36.4  Å

    (iv) Kinetic energy of first Bohr orbit is numerically equal to the energy of the orbit. 

    Therefore, 
                    E1 = -Z2E0       = -25 × 13.6 eV 

              K.E. = 25×13.6×1.6×10-19J          = 544×10-19J

    Potential energy of electron = -2×K.E.
                                               = -2×544×10-19J= -1088 × 10-19J 

    Angular momentum of the electron is given by, 

                 L = mvr = nh2π = h2π

          n = 1 for first bohr orbit. 

     i.e.,  L = 6.6×10-342π   = 1.05×10-34Js 

    (v) Radius r1 of the first Bohr orbit is, rn = n2r0Z  for n = 1. 

    That is, r1 = 12×5.3×10-115 = 1.06×10-11m.
    E - E1 = Z2×13.6112-1 = 13.6×25 eV
     
    Question 433
    CBSEENPH12038604

    Hydrogen atom in its ground state is excited by means of monochromatic radiation of wavelength 975 Å. How many different lines are possible in the resulting spectrum? Calculate the longest wavelength amongst them. You may assume the ionization energy for hydrogen atom as 13.6 eV.

    Solution
    Given,
    Wavelength of the monochromatic radiation, λ = 975 Å
    Ionization energy for hydrogen atom = 13.6 eV

    The energy of monochromatic radiation of wavelength 975 Å is,

    E = hcλ     = 6.63×10-34×3×108975×10-10×1.6×10-9eV 

      =12.75 eV              ( 1 eV = 1.6 ×10-19J)

      12.75 = 13.6112-1n2 

             1n2 = 1-12.7513.6       = 0.8513.6       =116 

             n=4  

    Thus, number of lines possible in the resultant spectrum = 6. 


    The longest wavelength will be emitted for transition from 4th orbit to 3rd orbit with an energy.
                 En2-En1 = E0Z21n12-1n22 

    Atomic no. Z = 1

                      E43 = 13.6132-142           = 13.619-116   

                      E43 = 13.6×7144eV           = 13.6 ×7144×1.6×10-19J  

    The longest wavelength, λ =hcE43
                                              = 6.63×10-34×3×108×14413.6×7×1.6×10-19m 

                                          λ=1.88 × 10-6m = 18800 Å

    Question 434
    CBSEENPH12038605

    In a hydrogen like atom the ionisation energy equals 4 times Rydberg's constant for hydrogen. What is the wavelength of radiations emitted when a jump takes place from the first excited state to the ground state? What is the radius of first Bohr's orbit?

    Solution
    The ionization energy E of a hydrogen-like Bohr atom of atomic number Z is given by, E = -Rz2 = -2πk2z2me4n2h2 

    where the Rydberg constant is R=2π2kme4n2h2=2.2×10-18J 

    Given that, 
    Ionisation energy is equal to four times the rydberg constant. 

    i.e.,                E= 4×Rydberg constant   = 4 R, we have 

                  4 R = RZ2
    or,                 Z =2 

    (i) Energy of radiation emitted (E) when the electron jumps from the first excited state to the ground state is given by,

                         E =RZ2112-122    = 4R1-14   = 3 R   =3×2.2×10-18J 

    i.e.,                E=6.6 ×10-18J. 

    Wavelength of the radiation emitted, λ = hcE    = 6.6 × 10-34 × 3× 1086.6×10-18    = 3×10-8m 

    (ii) Radius of the first Bohr orbit, = Bohr radius of hydrogen atomZ= 5×10-112=2.5×10-11m.
    Question 435
    CBSEENPH12038606

    Draw a labelled diagram for α-particle scattering experiment. Give Rutherford's observation and discuss the significance of this experiment.

    Solution
    Alpha-particle experiment led rutherford to the discovery of atomic nicleus.  

     
    Observations of the α particle experiment. 

    i) Most of the alpha particles pass straight through the gold foil. It means that they do not suffer any collision with the gold atoms.

    ii) Only about 0.14 % of incident alpha particles are scattered by more than 1o

    iii) About 1 alpha particle in every 8000 alpha particles deflect by more than 90o

    Significance of rutherford's experiment:

    His experiment led him to conclude that, the entire positive charge of the atom must be concentrated in a tiny central core of the atom. The tiny massive central core of the atom was named as the atomic nucleus. 
    Question 436
    CBSEENPH12038607

    If the short series limit of the Balmer series for hydrogen is 3646 Å, calculate the atomic number of the element which gives X-ray wavelengths down to 1.0 Å. Identify the element. 

    Solution
    Given, wavelength of the balmer series = 3646 Å 

    The short limit of the Balmer series is given by the Rydberg's formula, 

                  v¯ = 1λ =R122-12v¯ = R4 

             R =4λ= 43646×1010m-1 

    Further the wavelengths of the Kα series are given by the relation,

    v¯ =1λ = R(Z-1)2 112-1n2 

    The maximum wave number corresponds to n = ∞ and, therefore, we must have
     
                          v¯ = 1λ= R(Z-1)2 
             (Z-1)2 = 1               =3646×10-104×1×10-10               = 911.5 

              (Z-1) = 911.5
                        30.2 

                     Z = 31.2 31 

    Thus, the atomic number of the element concerned is 31.

    We can infer that the element having atomic number Z = 31 is Gallium.
    Question 437
    CBSEENPH12038608

    Using Bohr's formula for energy quantisation, determine the longest wavelength in the Lyman series of hydrogen atom spectrum.

    Solution
    Wavelengths of radiation of the Lyman series is given by, 

                    λn = 64π3ε02h3cme4n2n2-12
    For longest wavelength in the lyman series, we have n=2. 

    Therefore, 
    Wavelength assosciated with n=2 is,  

    λ2 = 64 π3 εo2 h3 cme42222 - 12     = 1225 Ao


    Question 438
    CBSEENPH12038609

    Using Bohr's formula for energy quantisation, determine the excitation energy of the n = 3 level of He+ atom.

    Solution
    The energy required to excite the electron from the ground state,n = 1 to the n = 3 state is given by, 

                    E3 -E1 = mZ2e432π2ε02h2112-132               = 48.1 eV
    Here,            Z = 2.

    Question 439
    CBSEENPH12038610

    Using Bohr's formula for energy quantisation, determine the ionisation potential of the ground state of Li++ atom.

    Solution
    Ionisation energy is given by, 

            E-E1 = mZ2e432π2ε02h2 (with Z = 3)
                        = 122 eV 

    Thus, ionisation potential is 122 V.
    Question 440
    CBSEENPH12038611

    Which state of the triply ionized Be+++ has the same orbital radius as that of the ground state of hydrogen? Compare the energies of two states.

    Solution
    Radius of nth orbit is given by, r = n2h24π2mKZe2 

      i.e.,   r  n2Z 

    For hydrogen,  Z = 1, n = 1 in ground state. 

             n2Z = 121 = 1 

    For Berylium, Z = 4, as orbital radius is same,n2Z=1 

                 n2 = 1 × Z = 1× 4 = 4n = 4 = 2 

    Hence n = 2.

    Thus, second level of triply ionised Be+++ has same radius as the ground state of hydrogen. 

    Now energy of electron in nth orbit is given by, E=-2π2mK2Z2e4n2h2 

                   E Z2n2

              E(Be)EH = Z2/n2BeZ2/n2 = 16/41/1 = 4 

    Therefore, energy of ionized Be is greater than the energy of hydrogen in the ground state. 
    Question 441
    CBSEENPH12038612

    Prove that the ionisation energy of hydrogen atom is 13.6 eV. 

    Solution
    We know that,

    Energy, E =-2π2mK2Z2e4n2h2          (n = 1,  Z = 1)

    Energy required or the amount of work done to remove the electron from it's ground state to a higher level is, 

                   W = k22π2me4h21n12-1n22 

    Ionisation energy is the energy required to remove an electron from ground state to infinity. 

    Here,              n1= 1,   n2 =

                       W =k22π2me4h211-1

                              = k22π2me4h2
     W = (9×109)2×2(3.142)2×9×10-31×(1.6×10-19)4(6.63×10-34)2J

        = 21.45 × 10-19J = 21.45×10-191.6×10-19eV = 13.6 eV. 

    Thus, the ionisation of hydrogen atom is 13.6 eV.
    Question 442
    CBSEENPH12038613

    A positronium atom is a bound state of an electron (e) and its antiparticle, the positron (e+) revolving round their centre of mass. In which part of the em spectrum does the system radiate when it de-excites from its first excited state to the ground state?

    Solution
    1. The motion of nucleus is ignored in an ordinary atom as the first approximation because the atom is too heavy.
    2. In a positronium atom, a positron replaces proton of hydrogen atom. As electron and positron masses are equal, the motion of the positron cannot be ignored.
    3. The motion of electron and positron about their centre of mass is considered.
    4. A detailed analysis will show that formulae of Bohr model apply to positronium atom provided that we replace mass of electron (m
    ) by what is known as reduced mass of the electron. The reduced mass is me/2 for positronium atom.
    5. 
    In the transition from n = 2 to n = 1, the wavelength of radiation emitted is double than that of the corresponding radiation emitted for a similar transition in hydrogen atom, which has a wavelength of 1217 Å and, is equal to 2 × 1217 = 2434 Å.
    6.This radiation lies in the ultra-violet part of the electromagnetic spectrum.
    Question 443
    CBSEENPH12038614

    The wavelength of the first member of Lyman series is 1216 Å. Calculate the wavelength of second member of Balmer series.

    Solution

    Given, 
    Wavelength of the first member of lyman series = 1216 Å 

    Now, the rydberg's formula gives us, 

                  1λ = R1n12-1n22

    For first member of Lyman series, n1 =1 and n2 = 2.
                  1λ1 = R112-14 

                  1λ1 = 3R4 

                    λ1 = 43R                       ...(i) 

    For second member of Balmer series, n1 =2,  n2 = 4 

    Therefore,
                    1λ2 = R122-142 = 3R16 

                  λ2 = 163R                           ...(ii) 

    Dividing equation (ii) by (i), we get 

                   λ2λ1 =163R×3R4 = 4  

                 λ2 = 4 λ1     = 4×1216 Å      = 4864 Å. 

    is the wavelength of the second member of balmer series. 

    Question 444
    CBSEENPH12038615

    Determine the speed of electron in n = 3 orbit of He+. Is the non-relativistic approximation valid?

    Solution
    The speed of electron in nth orbit is given by  v = 2π KZe2nh 

    For,   He,  Z = 2 and n = 3  

    Therefore,   v = 2π K2 e23h 

                     = 4×3.14×9×109(1.6×10-19)23 ×6.6 ×10-34 

                       v = 1.46 ×106 m/s 

    Now, the ratio of the speed of electron to the speed of light would tell us if relativistic or non-relativistic approximation is true.

    So,                vc = 1.46 ×1063×108 = 0.048 << 1 

     Hence non-relativistic approximation is valid.
    Question 445
    CBSEENPH12038616

    Calculate the radius of the first orbit of hydrogen atom. Show that the velocity of electron in the first orbit is 1137 times the velocity of light.

    Solution

    Radius of any orbit is given by the formula,

                   r = n2h24π2mKZe2 

    We have, n = 1 for 1st orbit and,
    h = 6.6 ×10-34Jsm =9 ×10-31kgK =9×109 Nm2C-2Z=1 for hydrogen, e =1.6 × 10-19 coulomb 

    Therefore, putting the values in the formula, 

    we get,      
                r = 0.53×10-10m , is the radius of the first orbit of hydrogen atom. 

    Now,
    Velocity of electron in the first orbit is,
             v= 2πKe2nh= cn2π Ke2ch  

              = c1×2×227×9×109×(1.6×10-19)23×108×6.6×10-34 

    ie.,   v =1137c. 

    Hence proved. 

    Question 446
    CBSEENPH12038617

    The energy levels of hydrogen atoms are as shown in Fig. Which of the shown transition will result in the emission of a photon of wavelength 275 nm?
    Which of the transition corresponds to emission of radiation of (i) maximum and (ii) minimum wavelength?

    Solution
    Wavelength of photon, λ = 275 nm 

    Therefore, 
    Energy of the photon is given by, 

    E = hcλ =6.6×10-34×3×108275×10-9J         = 6.6 ×10-34×3×108275×10-9×1.6×10-19eV         = 6.6 ×3275×1.6×102 eV         = 6.0 eV 

    As shown in the fig. , 

    i) Maximum radiation is emitted in transition A. 

    ii) Minimum radiation is emitted in transition D. 

    Question 448
    CBSEENPH12038619

    The ground state energy of hydrogen atoms is – 13.6 eV.
    (i) Which are the potential and kinetic energy of an electron in the third excited state?
    (ii) If the electron jumps to the ground state from the third excited state. Calculate the frequency of photon emitted.

    Solution
    Given, ground state of hydrogen atom = -13.6 eV

    (i) Ground state energy in hydrogen atom is given by, 
                  E = -(K.E.) = 12(P.E.) 

    ∴ Potential energy of electron in third excited state,  
              = 2(E)(4)2=-2×13.616eV= -1.7 eV 
    and,

    Kinetic energy of an electron, 
    = -12(1.7) = 0.85 eV 

    (ii) When the electron jumps from the ground state to the third excited state, 

    Frequency of the photon , v = Eh  

                        = -13.6(4)2+13.6(1)21.6 ×10-196.6×10-34 

                         = 11.9×1.6×10-196.6×10-34Hz 2.9 × 1015 Hz. 
     
    Question 454
    CBSEENPH12038625
    Question 464
    CBSEENPH12038635

    State the limitation of alpha scattering experiment.

    Solution

    Limitation of Rutherford's alpha-particle scattering experiment:

     In the model, it was proposed that the electron is revolving aroung the nucleus and is continuously experiencing a centripetal force. Thus, the electron has an accelerated motion. And, as per classical theory, the electron must radiate energy in the form of electromagnetic waves. So, the revolving electron is constantly losing energy and, it must spiral inwards eventually, falling into the nucleus. 
    But, since the matter is stable, the atom is not expected to collapse. This was a major drawback of rutherford's model. 

    Question 465
    CBSEENPH12038636

    Is Bohr's atomic theory applicable only for hydrogen atom?

    Solution

    No, Bohr's atomic theory is applicable for all single elctron atoms like He+, Li2+ etc. 
    In Bohr's theory we assume that centripetal force is provided by the electrostatic force of attraction by the nucleus. 

    In multiple elctron atoms, there will also be repulsion due to other electrons present in the nucleus. 

    Question 466
    CBSEENPH12038637

    Name the different spectral lines in hydrogen atom.

    Solution

    The different spectral lines in hydrogen atom are:

    n=1, Lyman series
    n=2, Balmer series
    n=3, Paschen series
    n=4, Brackett series
    n=5, Pfund series

    Question 467
    CBSEENPH12038638

    Does the Bohr's atomic theory explain the variation of intensity of different spectral line on the basis of frequency of photons emitted? Justify your answer.

    Solution

    One of the shortcomings of Bohr's Theory was that it could not explain the variation of intensity of the spectral lines of an element on the basis of frequency of photons emitted. 

    The intensity can be explained only by quantum mechanics. 

    Question 468
    CBSEENPH12038639

    What will be the total energy of an electron in hydrogen atom in third orbit. (Take total energy of electron in its ground state in – 13.6 eV).

    Solution

    In the third orbit, n =3 

    For hydrogen atom, energy of an electron is given by, 

    En-13.6n2 = -13.632= -13.69= - 1.5 eV

    Question 469
    CBSEENPH12038640

    What does the negative total energy of electron in its excited state signify?

    Solution

    The negative total energy of electron in it's excited state signify that the elctron is bound to the nucleus and is not free to leave it. 

    Question 470
    CBSEENPH12038641

    Two stable isotopes of lithium Li36 and Li37 have respective abundances of 7.5% and 92.5%. These isotopes have masses 6.01512 u and 7.01600 u, respectively. Find the atomic mass of lithium.

    Solution

    Given, 
    Mass of isotope 1 = 6.01512 u
    Mass of isotope 2 = 7.01600 u 
    Abundance of isoptope 1 = 7.5 %
    Abundance of isotope 2 = 92.5 %

    Atomic mass of Li =  weighted average of the isotopes 

                               = 6.01512×7.5+7.01600×92.5(7.5+92.5) 

                               = 45.1134+648.98100= 6.941 u

    Question 471
    CBSEENPH12038642

    Boron has two stable isotopes, B510 and B511. Their respective masses are 10.01294 u and 11.00931 u, and the atomic mass of boron is 10.81u. Find the abundances of B510 and B511.

    Solution

    Let, the relative abundance of B510 be x% 

      Relative abundance of B511 = (100-x)% 

    Atomic weight = weighted average of the isotopes,

      10.811 = 10.01294(x)+11.00931×(100-x)100

    i.e.,          x = 19.9%   and (100 - x) = 80.1%.

    Question 472
    CBSEENPH12038643

    The three stable isotopes of neon: Ne1020,  Ne1021  and  Ne1022 have respective abundances of 90.51%, 0.27% and 9.22%. The atomic masses of the three isotopes are 19.99 u, 20.99 u and 21.99 u, respectively. Obtain the average atomic mass of neon.

    Solution
    Given, the masses of isotopes of neon are, 19.99u, 20.99u and 21.99u.
    Relative abundance of the isotopes are 90.51 %, 0.27 % and 9.22 % . 
    Therefore, 
    Average atomic mass of neon is, 

    m = 90.51×19.99+0.27×20.99+9.22×21.99(90.51+0.27+9.22) 
     
       = 18.9.29+5.67+202.75100 

       =2017.7100 = 20.17 u
             



     
    Question 473
    CBSEENPH12038644

    Obtain the binding energy (in MeV) of a nitrogen nucleus 
    N714, given m N714 = 14.00307 u.

    Solution
    N714 nucleus is made up of 7 protons and 7 neutrons.

    Mass of nucleons forming nucleus = 7mp + 7m

           = Mass of 7 protons + Mass of 7 neutrons 

           = 7 × 1.00783 + 7 × 1.00867 u 

           = 7.05431 + 7.06069 u 

           = 14.11550.u 

    Mass of nucleus, mN = 14.00307 u 

    Therefore,

    Mass defect = 14.11550 - 14.00307 = 0.11243 a.m.u. 

    Energy equivalent to mass defect = 0.11243 × 931 = 104.67 MeV 

    ∴   Binding energy = 104.67 MeV.
    Question 474
    CBSEENPH12038645

    A given coin has a mass of 3.0 g. Calculate the nuclear energy that would be required to separate all the neutrons and protons from each other. For simplicity assume that the coin is entirely made of Cu2963 atoms (of mass 62.92960 u).

    Solution

    Given, mass of the coin = 3.0 g 

    Mass of atom = 62.92960 u

    Each atom of the copper contains 29 protons and 34 neutrons.

    Mass of 29 electrons = 29 x 0.000548 u
                                    = 0.015892 u

    Mass of nucleus  = (62.92960 - 0.015892) u

                              = 62.913708 u

    Mass of 29 protons = 29 x 1.007825 u
                                 = 29.226925 u 

    Mass of 34 neutrons = 34 x 1.008665 u 

                                    = 34.29461 u
    Total mass of protons and neutrons  = (29.226925 + 34.29461) u
                                                           = 63.521535 u

    Binding energy  = (63.521535 - 62.913708) x 931.5 MeV
                            = 0.607827 x 931.5 MeV 

     Required energy = 6.023 × 102363×3×0.607827× 931.5 MeV
                                  = 1.6 × 1025 MeV = 2.6 ×1012J.

    Question 475
    CBSEENPH12038646

    A radioactive isotope has a half-life of T years. How long will it take the activity to reduce to (a) 3.125%, (b) 1% of its original value?

    Solution

    Given, the sample has a half life of T years. 

    (a) The fraction of the original sample left is ,
                     NNo3.125100
                          = 132= 125

               
    Hence,  there are 5 half lives of T years spent. Thus, the time taken is 5T years.

    (b) The fraction of the original sample left = 1100=12n 

     i.e.,     2n = 100  

      n log 2 = log 100 

    Hence, n = log 100log 2=20.301  = 6.64 

    From, t= nT we have, t = 6.64 T.

    Hence, there are 6.64 half lives of T years spent. Thus, the time taken is 6.64T years.

    Question 476
    CBSEENPH12038647

    The normal activity of living carbon-containing matter is found to be about 15 decays per minute for every gram of carbon. This activity arises from the small proportion of radioactive C614C614 present with the stable carbon istope C612. When the organism is dead, its interaction with the atmosphere (which maintains the above equilibrium activity) ceases and its activity begins to drop. From the known half-life (5730 years) of C614, and the measured activity, the age of the specimen can be approximately estimated. This is the principle of  C614 dating used in archaeology.
    Suppose a specimen from Mohenjodaro gives an activity of 9 decays per minute per gram of carbon. Estimate the approximate age of the Indus Valley Civilisation.

    Solution
    Given,
    Normal activity, R
    0 = 15 decays/min,
    Present activity R = 9 decays/min,
    Half life, T = 5730 years,
    Age t =? 

    As, activity is proportional to the number of radioactive atoms, therefore,

                       NN0 = RR0 = 915 

    But,             NN0 = e-λt

                    e-λt = 915 =35 

                       e+λt = 53

         λt logee = loge53 = 2.3026 log 1.6667

                λt = 2.3026 × 0.2218    = 0.5109  t = 0.5109λ 

    But, λ = 0.693T =0.6935730 Yr-1

    Therefore,
                   t =0.51090.693/5730 = 0.5109 × 57300.693

                   t = 4224.3 years. is the approximate age.
    Question 477
    CBSEENPH12038648

    The half-life of Sr3890 is 28 years. What is the disintegration rate of 15 mg of this isotope?

    Solution

    Given,
    Half- life of Sr3890 = 28 years. 

    Using the formula,
                               λ =0.693T

                           λ = 0.69328×365×24×60×60
                                      
                                  = 7.85 × 10-10 s-1 
    90 g of Sr contains 6.023 x 1023 atoms.

     15 mg of Sr contains,

    N0 = 6.023 × 1023 × 15 × 10-390atoms 

    N0 = 1.0038 × 1020 atoms

    Disintegration rate, dNdt = -λ N0

                                           = -7.85 × 10-10 × 1.0038 × 1020= 7.88 ×1010 dps or Bq= 7.88 × 10103.7 × 1010Ci

                                        = 2.13 Ci.

    Question 478
    CBSEENPH12038649

    Obtain approximately the ratio of the nuclear radii of the gold isotope Au79197 and the silver isotope Ag47107.

    Solution

    Using the relation between the radius of nucleus and atomic mass,
                                 R  A1/3 

    Atomic mass of gold, A1 = 197 
    Atomic mass of silver, A2 = 107

                           R1R2 = A1A21/3 

                                    = 1971071/3 = (1.84)1/3 

    Now, taking log on both sides, 

             log10R1R2 = log10(1.84)1/3 

             log10R1R2 = 13log10(1.84)             

                                  = 13×0.2648= 0.08827 

                       R1R2 = antilog(0.08827) 
                                  = 1.23, which is the required ratio of the nucleii. 

    Question 479
    CBSEENPH12038650

    The radionuclide C11 decays according to C611  B511+e++v;  T1/2 = 20.3 min.
    The maximum energy of the emitted positron is 0.960 MeV. Given the mass values:
    mC611 = 11.011434 u  and  m B511 = 11.009305 u.
    Calculate Q and compare it with the maximum energy of the positron emitted.

    Solution

    For the given reaction, mass defect is, 
                                   m =  [m C611 - 6me - m B511 - 5 me+me        =  mC611 - m(B511) -  2 me        =  11.011434 u - 11.009305 u - 2 × 0.000548 u        =  0.001033 u

    Now, Q-value is , 

                  Q = 0.001033 × 931.5 MeV     = 0.962 MeV 

    which, is the maximum energy of the positron. 
    We have, 
                         Q = Ed+Ee+Ev 
    The daughter nucleus is too heavy compared to e+ and v. So, it carries negligible energy (Ed ≈ 0). If the kinetic energy (Ev) carried by the neutrino is minimum (i.e., zero), the positron carries maximum energy, and this is practically all energy Q.
    Hence, maximum E
    e≈ Q.

    Question 480
    CBSEENPH12038651

    The nucleus Ne1023 decays by β- emission. Write down the β-decay equation and determine the maximum kinetic energy of the electrons emitted from the following data:
    m(Ne1023) = 22.994466 um(Na1123) = 22.989770 u

    Solution

    The β-decay of Ne1023 may be represented as:

                Ne1023  Na1123 - e-10 + v¯ + Q 

    Ignoring the rest mass of antineutrino v¯ and electron , we get 

    Mass defect,                  
                       m = m(Ne1023) - m (Na1123)         = 22.994466 - 22.989770          = 0.004696 u          

      Q = 0.004696×931 MeV = 4.372 MeV. 

    This energy of 4.3792 MeV, is shared by e- and v¯ pair because, Na1123 is very massive.

    The maximum K.E. of e- = 4.372 MeV, when energy carried by v¯ is zero.

    Question 481
    CBSEENPH12038652

    The Q-value of a nuclear reaction A + b → C + d is defined by
    Q = [m
    A + mb - mc - md] c2
    where the masses refer to the respective nuclei. Determine from the given data the Q-value of the following reactions and state whether the reactions are exothermic or endothermic.
    (i) H11+H13  H12+H12 
    (ii) C612+C612  Ne1020 + He24
    Atomic masses are given to be
                          m(H12) = 2.014102 u;  m (H31) = 3.0160409 um (C612) = 12.000000  u; m (Ne2010)  = 19.992439 u.

    Solution

    (i) Considering the first reaction,

                        H11 +H13  H12 + H12 

    Q-value is given by,
                         Q = m×931.5 MeV     = [m(H11) + m(H13) - 2m (H12)] × 931 MeV     = [1.007825+3.016049 -2×2.014102] × 931 Mev     = -4.03 MeV 
    Since, Q-value is negative, this reaction is endothermic.

    (ii) The second reaction is, 

                      C612 + C612  Ne1020 + He24 

    Q-value is given by,
                          Q = m×931 MeV     = [2 m (C612) - m (Ne1020) - m(He24)] × 931 MeV     = [24.000000 - 19.992439 - 4.002603] × 931 MeV     = + 4.61 MeV

    Since, the Q-value is positive , the reaction is exothermic.

    Question 482
    CBSEENPH12038653

    Suppose, we think of fission of a Fe2656 nucleus  into two equal fragments Al1328. Is the fission energetically possible? Argue by working out Q of the process.
    Given m(Fe2656) = 55.93494 u,  m (Al1328) = 27.98191 u.

    Solution
    Q- value is given by,

    Q = [m (Fe2656) - 2m(Al1328) × 931.5 MeV     = [55.93494 - 2 × 27.98191] × 931.5 MeV 

     Q= -0.02886 × 931.5 MeV = -26.88 MeV, which is negative. 

    Since, the Q-value is negative (energy released from the reaction is negative), the fission is not possible energetically.
    Question 483
    CBSEENPH12038654

    The fission properties of Pu94239 are very similar to those of U92235. The average energy released per fission is 180 MeV. How much energy, in MeV, is released if all the atoms in 1 kg of pure Pu94239 undergo fission?

    Solution

    Given, 
    Average amount of energy released per fission,    Pu94239 = 180 MeV 

    Quantity of fissionable material  = 1 kg 

    In 239 gm Pu, number of fissionable atom or nuclei = 6.023×1023 

    In 1 g of Pu, number of fissionable atom or nuclei = 6.023×1023239 

    In 1000 gm of Pu, number of fissionable atom or nuclei, 
    = 6.023 × 1023239 × 1000= 25.2 × 1023 

    Therefore,
    Total energy released in fission of 25.2 x 1023 Pu nucleus or in fission of 1 kg pure Pu is, 
                                       = 180 x 25.2 x 1023
                                       
    = 4536 x 1023 MeV
                                       = 4.5 x 1026 MeV.

    Question 484
    CBSEENPH12038655

    A 1000 MW fission reactor consumes half of its fuel in 5.00 y. How much U92235 did it contain initially? Assume that the reactor operates 80% of the time that all the energy generated arises from the fission of U92235 and that this nuclide is consumed only by the fission process.

    Solution

    Given, 

    Power of reactor  = 1000 MW = 103 MW
                              = 109W
                              = 109 Js-1 

    Energy generated by reactor in 5 Years = 5 x 365 x 24 x 60 x 60 x 10

    Average energy generated = 200 MeV
                                            = 200 x 1.6 x 10-13 

    Number of fission taking place or number of U235 nuclei required, 
                      = 5 × 365 × 24 × 60 × 60 × 109200 × 1.6 × 10-13

                      = 8.2125 × 1026 ×6= 49.275 × 1026 

    Mass of 6.023 x 1023 nuclei of U = 235 gm = 235 x 10-3 kg 

    Mass of 8.2125 x 1026 nuclei of U,  
                 = 235 × 10-36.023 ×1023 × 6 × 8.2125 × 1026 = 1932 kg 
    12 of fuel = 1932 kg  Total fuel = 3864 kg.

     

    Question 485
    CBSEENPH12038656

    How long can an electric lamp of 100 W be kept glowing by fusion of 2.0 kg of deuterium? Take the fusion reaction as:
    H12 + H12   He23+n+3.2 MeV.

    Solution

    Power of the electric lamp = 100 W 

    When two nuclei of deuterium fuse together, energy released = 3.2 MeV 

    Number of deuterium atoms in 2 kg is, 
               = 6.023 × 10232×2000 = 6.023 × 1026

    Energy released when 6.023 × 1026 nuclei of deuterium fuse together, 

                   = 3.22×6.023×1026 MeV= 3.22×6.023 × 1026 ×1.6 × 10-13J = 1.54 × 1014 J or Ws 
    If the lamp glows for time t, then the electrical energy consumed by the lamp is 100 t, 

     100 t =  1.54 × 1014    

                t = 1.54 × 1012s

                 = 1.54 × 10123.154 ×107years  = 4.88 × 104 years.

    which is the life span of an electric lamp. 

    Question 486
    CBSEENPH12038657

    Calculate the height of the potential barrier for a head on collision of two deuterons.(Hint: The height of the potential barrier is given by the Coulomb repulsion between the two deuterons when they just touch each other.) Assume that they can be taken as hard spheres of radius 2.0 fm.

    Solution
    Suppose, the two particles are fired at each other with the same kinetic energy K.E, so that they are brought to rest by their mutual Coulomb repulsion when they are just touching each other. 

    Distance between the centres of two deutrons, during head on collision, r = 2 × radius 

    Therefore, 
    r = 4 fm = 4 × 10-15

    Charge on each deutron, e = 1.6 × 10-19 C

    Now, potential energy = e24πεor 

                                     =  9×109 ×(1.6 ×10-19)24× 10-15 

                                     = 9×1.6×1.6×10-144×1.6×10-16 keV  

                                       =360 keV 

    Now, since, potential energy is equal to twice the kinetic energy of deutron. 

    This implies, 
    K.E of each deutron = 3602 = 180 keV 

    which is a measure of the height of the coulomb barrier. 
    Question 487
    CBSEENPH12038658

    From the relation R = R0A1/3, where R0 is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e., independent of A).

    Solution
    Radius of a nucleus of mass number A is given by, 
                            R =R0 A1/3 

    where,            R0 = 1.2 × 10-15m. 

    This implies that the volume of the nucleus, which is proportional to R3 is proportional to A. 

    Volume of nucleus = 43πr3 

                                = 43π (R0 A1/3)3= 43π R03A  

     Density of nucleus = mass of nucleusvolume of nucleus

                                 = mA43πR03A

                                 = 3m4π R03 

    The above derived equation shows that density of nucleus is constant, independent of A for all nuclei. Density of nuclear matter is approximately 2.3 × 107 kg/m3 which is very large as compared to ordinary matter. 
    Question 488
    CBSEENPH12038659

    For the (positron) emission from a nucleus, there is another competing process known as electron capture (electron from an inner orbit, say, the K-shell, is captured by the nucleus and a neutrino is emitted).
    e++XZA  YZ-1A + v
    Show that if β++ emission is energetically allowed, electron capture is necessarily allowed but not vice-versa.

    Solution
    Consider the two competing reaction processes: 

    XZA  YZ-1A + e+ +ve + Q1  (positron emission) 

    e-+XZA  YZ-1A +ve+Q2 (electron capture)

    Q-value for the first reaction process is,
            Q1 = mN XZA - mNYZ-1A-mec2      = mXZA-Zme-mYZ-1A+ (Z-1)me-mec2      = m XZA - mYZ-1A - 2mec2

    Q-value for the second reaction is given by, 

     Q2 = mNXZA + me - mN YZ-1Ac2 

         = mXZA -mYZ-1Ac2  

    where,
    mN is the mass of nucleus and, 
    m denotes the mass of atom. 

    Therefore, if positron emission is allowed energetically then, electron capture is allowed. 

    That is, if Q1 > 0 implies Q2 > 0 but,
    Q
    2 > 0 does not necessarily mean Q1 > 0.

    Hence the result.



    Question 489
    CBSEENPH12038660

    The neutron separation energy is defined as the energy required to remove a neutron from the nucleus. Obtain the neutron separation energies of the nuclei Ca2041 and Al1327 from the following data:
    mCa2040 = 39.962591 umCa2041 = 40.962278 umAl1326 = 25.986895 umAl1327 = 26.981541 u.

    Solution
    The enrgy equation, when neutron is seperated from Ca2041 is given by, 

                   Ca2041+Q1  Ca2040 + n01

    Mass defect is given by,
          m = mCa2040+m(n01) - m(Ca2041) 

                 = 39.962591+1.008665-40.962278 = 0.008978 u

    But,  1 u  931.5 MeV 

    Hence,  
              0.008978 u  0.008978 × 931.5 = 8.363 MeV 
    is the neutron seperation energy. 

    The equations for the neutron separation in second case can be written as, 

                   Al1327+Q2  Al1326 + n01          
    Mass defect, m = m(Al1326) + m(n01) - m(Al1327) 

    But, 1 u  931.5 MeV 

    Hence,
         0.014019 u  0.014019 × 931.5 = 13.06 MeV.is the neutron seperation energy. 
    Question 490
    CBSEENPH12038661

    A source contains two phosphorous radio nuclides P1532 (T1/2 = 14.3 d) and P1533 (T1/2 = 25.3 d). Initially, 10% of the decays come from P1533. How long one must wait until 90% do so?

    Solution

    We know that rate of disintegration is,
                         -dNdt N. 

    So, clearly the initial ratio of the phosphorous radio nuclides, P1533 and P1532 is 1:9.

    We have to find the time at which the ratio is 9:1.

    Initially, if the amount of P1533 is x, then the amount of P1532 is 9x.

    Finally, if the amount of P1533 is 9y, the amount of P1532 is y.

    Now, from the formula, 
               NNo = 12n = 12tT =2 -tT 

    Therefore, 
    Using,             N = N02t/T 

                     9y = x2t/25.3  y = 9x2t/14.3 

    On dividing,         9 = x2t/25.3×2t/14.39x 

                        81 = 2t14.3-t25.3
                        81 = 211t361.79 

                 log1081 = 11t361.79log102                 = 11×0.3010 t361.79

        9.15 × 10-3t = 1.91 

    i.e.,                      t =1.91×10009.15d    = 208.7 days 

    Question 491
    CBSEENPH12038662

    Under certain circumstances, a nucleus can decay by emitting a particle more massive than an α-particle. Consider the following decay processes:
    Ra88223     Pb82209 + C614Ra88223    Rn86219 +He24
    Calculate the Q-values for these decays and determine that both are energetically allowed.

    Solution

    (i) For the first decay process,
             
                    Ra88223  Pb82209 + C614 + Q

    Mass defect, 

    m = mass of Ra223-(mass of Pb209+mass of C14) 
           = 223.01850 - (208.98107+14.00324)= 0.03419 u
    Therefore, 
    Energy released, Q = 0.03419 × 931 MeV = 31.83 MeV

    (ii) Now, for second decay process we have, 

                  Ra88223  Rn86219 + He24 + Q

    Mass defect, m = mass of Ra223- (mass of Rn219 + mass of He4

                               = 223.01850 - (219.00948+4.00260)= 0.00642 u 

     Energy released,Q = 0.00642 × 931 MeV = 5.98 MeV 

    Both the above given decay processes are energetically possible because the Q-value i.e., energy released in the reaction is positive. 

    Question 492
    CBSEENPH12038663

    Consider the fission of U92238 by fast neutrons. In one fission event,  no neutrons are emitted and the final end products, after the beta decay of the primary fragments, are Ce58140 and Ru4499. Calculate Q for this fission process. The relevant atomic and particle masses are
    m 92238U = 238.05079 um 58140Ce =139.90543 u mRu4499  = 98.90594 u.

    Solution
    Fission reaction is given by, 

                U92238 + n01  Ce58140 + Ru4499+ Q

    Q-value = (mass of U238 + mass of n01 - mass of Ce140-mass of Ru99) x 931.5 MeV
                             = (238.05079+1.00867-139.90543-98.90594) × 931.5 MeV= 231.1 MeV.


    Question 493
    CBSEENPH12038664

    Consider the D-T reaction (deuterium-tritium fusion)
    H12 + H13   He24  +n
    (a) Calculate the energy released in MeV in this reaction from the data:
    mH12 = 2.014102 umH13 = 3.016049 u
    (b) Consider the radius of both deuterium and tritium to be approximately 2.0 fm. What is the kinetic energy needed to overcome the Coulomb repulsion between the two nuclei? To what temperature must the gas be heated to initiate the reaction?
    (Hint: Kinetic energy required for one fusion event = average thermal kinetic energy available with the interacting particles = 2(3kT/2); k = Boltzman's constant, T = absolute temperature.)

    Solution

    (a) The reaction process is,  

                   H12 +H13  He24 + n + Q
                Q-value  = [mass of H12 + mass of H13 - mass of He24 -mass of n]  x 931 MeV  

                     = (2.014102+3.016049 -4.002603-1.00867) × 931 MeV = 0.018878 × 931 = 17.58 MeV 
    (b) Repulsive potential energy of two nuclei when they almost touch each other is given by, 

              q24πε0(2r) = 9×109(1.6 ×10-19)22×2×10-15joule 

                             = 5.76 × 10-14J 

    Classically, this amount of K.E. is at least required to overcome Coulomb repulsion.

    Now, using the relation, 

          KE = 32kT    T = 2K.E.3k             = 2×5.76×10-143×1.38×10-23             = 2.78 × 109K 

    though the temperature required for triggering the reaction is somewhat less practically.

    Question 494
    CBSEENPH12038665

    Calculate and compare the energy released by

    (a) fusion of 1.0 kg of hydrogen deep within the sun, and
    (b) the fission of 1.0 kg of 
    U235 in a fission reactor.

    Solution
    a.) In sun, a He nucleus is formed by the fusion four hydrogen nucleii by releasing an amount of 26 MeV energy.

    Therefore, 

    Energy released by fusion of 1 kg of hydrogen,

             = 6 × 1023 × 264×103 MeV 

         E1 = 39 × 1026 MeV 

    b.)
    As energy released in fission of one atom of U23592 = 200 MeV 

       Energy released in fission of 1 kg of U23592
             = 6×1023×1000235×200 MeV 

         E2 =5.1 × 1026 MeV 

    Thus, 
           E1E2 = 39 × 10265.1 × 1026 = 7.65 

    i.e., energy released in fusion is 7.65 times the energy released in fission.
     
    Question 495
    CBSEENPH12038666

    Suppose India had a target of producting by 2020 A.D., 2 × 105 MW of electric power, ten percent of which was to be obtained from nuclear power plants. Suppose we are given that on an average, the efficiency of utilization (i.e., conversion to electrical energy) of thermal energy produced in a reactor is 25%. How much amount of fissionable uranium would our country need per year by 2020? Take the heat energy per fission of U235 to be about 200 MeV.

    Solution
    Given,
    Target of electric power to be produced = 100,000 MW.
    10% power is to be obtained from nuclear power plants. 
    Heat energy per fission of U235 = 200 MeV

    Therefore, 

    Required electric power from nuclear plants,  = 100000 × 10100 = 10,000 MW 

    Therefore, required electric energy from nuclear plants per year,
    = (10,000 × 106 W) × 365 × 24 × 60 × 60= 3.1536 × 1017J
     

    Electrical energy recovered from the fission of one U235 nucleus, 
    = 200 ×25100 = 50 MeV= 50 × 1.6 × 10-13= 8 × 10-12J  

      Number of fissions of U235 nucleus required is, = 3.1536 ×1078×10-12 = 3.942 ×1028 

    Number of moles of U235 required per year
    = 3.942 × 10286.023 × 1023 = 6.5449 × 104 

    Therefore, mass of U235 required per year, = 6.5449 × 104 × 235= 1538.054 g= 1.538054 kg.
    Question 496
    CBSEENPH12038667

    Obtain the maximum kinetic energy of β-particles, and the radiation frequencies of γ decays in the decay scheme shown in Fig. You are given that
    m (198Au) = 197.968233 u
    m (198Hg) = 197.966760 u

    Solution

    To obtain the maximum kinetic energy of β- particles = ? 

    Radiation frequency, v = (E2 -E1)h

    Frequency, v(γ1) = (1.088-0) ×1.6×10-136.62 ×10-34  

                             = 2.63 × 1020 s-1  

     1 MeV = 106 × 1.6 × 10-19J1 MeV = 1.6 × 10-13J


    Frequency, v(γ2) = (0.412-0) × 1.6 × 10-136.62 × 10-34                               = 9.96 × 1020s-1Frequency, v(γ3) = (1.088-0.412) ×1.6×10-136.62×10-34                                 = 1.63×1020s-1 

    The emission process of β1- decay may be represented as:
                 Au79198  Hg80198 + e-10 + E(β1-) + E(γ1)

    where,               E(γ1) = 1.088 MeV ( as per the fig.)

    Now,
          E(β1-) = m Au79198 - mHg80198 - me × 931.5 - E(γ1)

    where,

    m( 79198Au)  and m  80198Hg are masses of the  79198Au and Hg80198 nuclei. 

     Eβ1- = M  79198Au -79 me - M Hg80198 - 80 me-me × 931.5-1.088

             = M  79198Au - M 80198Hg × 931.5 - 1.088 

              = (197.968233 - 197.966760) x 931.5 - 1.088
              = 1.372 -1.088 = 0.284 MeV 

    The emission process of β2- decay may be represented as: 

                Au79198 Hg80198 + e-10 + E(β2-) + E(γ2) 

    As in case of β1- decay, it can be deduced in a similar manner.  

      E(β2-) = M Au79198 -MHg80198 × 931.5 - E (γ2)   

                 = 1.372 - 0.412 = 0.960 MeV.

    Question 497
    CBSEENPH12038668

    Obtain the binding energy of the nuclei Fe2656 and Bi83209 in units of MeV from the following data:
    m(Fe2656) = 55.934939   u;    m(Bi83209) = 208.980388 u


    Solution
    i) 
    F2656 nucleus contains 26 protons and,
    Number of neutrons = (56 - 26) = 30 neutrons 

    Now,

    Mass of 26 protons = 26 x 1.007825 = 26.20345 u 

    Mass of 30 neutrons  = 30 x 1.008665 = 30.25995 u 

    Total mass of 56 nucleons = 56.46340 u

    Mass of  Fe2656 nucleus = 55.934939 u 

     Mass defect, m = 56.46340 - 55.934939         = 0.528461 u 

    Total binding energy = 0.528461 x 931.5 MeV = 492.26 MeV 

    Average binding energy per nucleon = 492.2656 = 8.790 MeV. 

    ii) 
    Bi20983 nucleus contains 83 protons and, 

    Number of neutrons = (209-83) = 126 neutrons. 

    Mass of 83 protons = 83 × 1.007825 = 83.649475 amu 

    Mass of 126 neutrons = 126 ×1.008665 = 127.091790 amu 

    Therefore, total mass of nucleons = (83.649475+127.091790) = 210.741260 amu 

    mass of nucleus = 208.980388 a.m.u (given) 

    Now, mass defect, m =  210.741260 - 208.980388 = 1.760872  

    Total binding energy = 1.760872 × 931.5 = 1640.26 MeV 

    Therefore, average B.E. per nucleon = 1640.26209 = 7.848 MeV 

    Question 498
    CBSEENPH12038669

    Write nuclear reaction equation for
    (i) α-decay of  Ra88226   (ii) α-decay of  94242Pu

    (iii) β- decay of P1532        (iv) β- decay of Bi83210

    (v) β+ decay of C611         (vi) β+ decay of Tc4397


    Solution

    (i) Ra88226  Rn86222 + He24

    (ii) Pu94242  U92238 + He24

    (iii) P1532  S1632 + e-1 + v¯

    (iv) Bi83210  Po84210 + e-1+v¯

    (v)  C611  B511 + e++v

    (vi) Tc4397  Mo4297 + e+ +v

    (vii) Xc54120 + e-  I53120 + v

    Question 499
    CBSEENPH12038670

    Obtain the amount of Co2760 necessary to provide a radioactive source of 8.0 mCi strength. The half-life of Co2760 is 5.3 years.

    Solution

    Given, 
    Half life , T = 5.3 years 

    Strength of radioactive source,
    = 8.0 mCi = 8.0 x 10-3 Ci
    = 8.0 x 10-3 x 3.7 x 10-10 disintegrations s-1
    = 29.6 x 107 disintegrations s-1
                         
    Since the strength of the source decreases with time,
                  dNdt = -29.6 × 107

    But            dNdt = -λN 

                  -λN = -29.6 × 107 

                    λN = 29.6 × 107 

                      N = 29.6 × 107λ
                      N = 29.6 × 107× T0.693             λ = 0.693T
                              = 29.6 × 107 × 5.3 × 365 ×24 ×60×600.693 

                            = 7.139 × 1016 

    Number of atoms in 60 g of cobalt = 6.023 x  1023 

    Therefore,

    Mass of 1 atom of cobalt  = 606.023 × 1023g 

    Mass of 7.139 × 1016 atoms is, 

    = 606.023 × 1023 × 7.139 × 1016g 

    = 7.11 μg.                                             

    Question 500
    CBSEENPH12038671

    Find the Q-value and the kinetic energy of the emitted α-particle in α-decay of (a) Ra88226 and (b) Rn86220
    Given   mRa88226 = 226.02540 u;   mRn86222 = 222.01750 u;mRn86220 = 220.01137 u;   mPo84216 = 216.00189 u. 


    Solution

    (a) The reaction invoved is,  

                       Ra88226  Rn86222 + He24

    The difference in mass between the original nucleus and the decay products = 226.02540 u - (222.01750 u  + 4.00260 u)
                                        = + 0.0053 u 

     Energy equivalent or Q-value  = 0.0053 x 931.5 MeV 

                                                      = 4.93695 MeV 

                                                      = 4.94 MeV 

    The decay products would emerge with total kinetic energy 4.94 MeV.

    Momentum is conserved. If the parent nucleus is at rest, the daughter and the α-particle have momenta of equal magnitude p but, in the opposite direction.

    Kinetic energy,  K = p22m. 

    Since, p is the same for the two particles therefore the kinetic energy divides inversely as their masses.

    The α-particle gets 222222+4 of the total i.e., 222226×4.94 MeV or 4.85 MeV. 


    (b) The difference in mass between the original nucleus and the decay products = 220.01137 u - (216.00189 u + 4.00260 u)
                                                    = 0.00688 u
     Q-value or Energy equivalent = 0.00688 x 931.5 MeV
                                                     = 6.41 MeV
    Energy of the alpha particle, Eα= 216216+4×6.41 MeV = 6.29 MeV. 

    Question 501
    CBSEENPH12038672

    Two nuclei have mass numbers in the ratio 27:125. What is the ratio of their nuclear radii?

    Solution

    Given,
    Rato of mass numbers , A1:A2 = 27:125 

                                       A1A2 = 27125

    Radius of nucleus is, R = R0 A1/3 

    Therefore,
                         R1R2 = A1A21/3         = 271251/3         = 35

    Thus, Ratio of radii is 3:5. 

    Question 502
    CBSEENPH12038673

    Two nuclei have mass numbers in the ratio 1: 3. What is the ratio of their nuclear densities?

    Solution
    Ratio of mass number in the nucleii, A1 :A2 = 1:3 

    Since, the nuclear density is same for all nuclei and is independent of the mass ratio, therefore, 
    ∴   ρ12 = 1:1
    Question 503
    CBSEENPH12038674

    Out of the two characteristics—the mass number (A) and the atomic number (Z) of a nucleus, which one does not change during nuclear α-decay?   

    Solution
    For, nuclear alpha-decay, β = -1e

    Thus, the mass number (A) of the element ZXA does not change during the nuclear alpha-decay. 
    Question 504
    CBSEENPH12038675

    Name the absorbing material used to control the reaction rate of neutrons in a nuclear reactor.

    Solution

    Heavy water is used an absorbant to control the reaction rate of neutrons in a nuclear reactor. 

    Question 505
    CBSEENPH12038676

    Define the term 'activity' of a radionuclide. Write its SI unit.

    Solution
    The number of radioactive disintegrations taking place per second in a given sample is called the activity of a sample. 

    Its SI unit is becquerel.
    Question 506
    CBSEENPH12038677

    The radioactive isotope D decays according to the sequence.

    If the mass number and atomic number of D2 are 176 and 71 respectively, what is (i) the mass number, (ii) atomic number of D?   

    Solution
    The isotope's atomic number reduces by 1 and mass number remains the same while undergoing β- decay. 
    When it udergoes α decay, mass number increases by 4 and atomic number by 2. 

    Therefore, 

    Decay process can be written as:


    (i) Mass number of D = 172. 

    (ii) Atomic number of D = 70.

    Question 507
    CBSEENPH12038678

    Draw the graph showing the distribution of kinetic energy of electrons emitted during beta decay.

    Solution
     

    The above graph shows us the distribution of kinetic energy of electrons during beta decay. 
    Question 508
    CBSEENPH12038679

    What is the nuclear radius of Fe125, if that of Al27 is 3.6 fermi?

    Solution
    Relation between nuclear radius and mass number is as follows,
                                R A1/3 
    This implies, 

                   RFeRAl = AFeAAl1/3           = 125271/3           = 53           = 1.67 

    Therefore,
    Nuclear radius, RFe = 1.67 × RAl  

                                = 53×3.6 = 6 fermi. 

    Question 509
    CBSEENPH12038680

    Name the reaction which takes place when a slow neutron beam strikes. U92235 nuclei. Write the nuclear reaction involved.

    Solution
    Nuclear fission of nuclei takes place when a slow neutron strikes  92235U

    The nuclear reaction involved is, 

          U92235 + n01  Ba56141 + Kr3692 + 3 n01 + energy.
    Question 510
    CBSEENPH12038681

    'Heavy water is often used as a moderator in thermal nuclear reactors'? Give reason.

    Solution
    Heavy water is used as a moderator because its mass is nearest to that of a neutron and it has negligible chances for neutron absorption.
    Question 511
    CBSEENPH12038682

    A nucleus nXm emits one alpha particle and one beta particle. Find the mass number and atomic number of the product nucleus. 

    Solution
    During alpha decay, the mass number and atomic number goes down by 4 and 2 respectively. 
    In beta-decay, mass number remains same but, atomic number decreases by 1. 

    The nuclear reaction is as follows: 

     Therefore, 

    Mass number of product nucleus = m - 4 and, 

    Atomic number of product nucleus = n - 1.

    Question 512
    CBSEENPH12038683

    Define decay constant.

    Solution
    Decay constant of a radioactive element is defined as the reciprocal of the time during which, the number of atoms left in the sample reduces to 1e times the original number of atoms in the sample. 
    Question 513
    CBSEENPH12038684

    Name two radioactive elements which are not found in observable quantities?

    Solution
    Tritium and Plutonium are two radioactive elements which are not found in observable quantities. 
    Question 514
    CBSEENPH12038685

    Why is the ionizing power of α-particle greater than that of gamma rays?

    Solution
    Alpha-particle is positively charged and can interact more strongly with matter as compared to gamma rays. So, ionizing power of alpha particles is greater than that of gamma rays.
    Question 515
    CBSEENPH12038686

    The isotope O816 has 8 protons, 8 neutrons and 8 electrons while Be48 has 4 protons 4 neutrons and 4 electrons. Yet the ratio of their atomic masses is not exactly same. Why?

    Solution
    The binding energy does not only depend upon the neutron to proton ratio but, it also varies with increase in mass number.
    In the present case, the binding energy per nucleon increases with the increase in the mass number for lighter nuclei.
    Question 516
    CBSEENPH12038687

    Does the ratio of neutrons to proton in a nucleus increase, decrease or remain the same after emission of
    (1)    α-particle
    (2)    β-particle.

    Solution

    1. The ratio of neutron to proton in a nucleus increases after the emission of alpha-particle. 

    2. The ratio of neutron to proton in a nucleus decreases after the emission of beta- particle. 

    Question 517
    CBSEENPH12038688

    Which one is unstable among neutron, proton, electron and α-particle?

    Solution
    Neutron is unstable among the four. It decays into proton, electron and an anti-particle called anti-neutrino. Neutron has a mean life of 1000s. 
    Question 518
    CBSEENPH12038689

    Name two elementary particles which have almost infinite life time.

    Solution
    Electron and proton are two elementary particles having almost infinite life time.
    Question 519
    CBSEENPH12038690

    A radioactive material has a half-life of 1 minute. If one of the nuclei decays now, when will the next one decay?

    Solution
    The decay time of the nucleus is not dependent on the half life of the previous nucleus. That is, the next nucleus can decay any time.
    Question 520
    CBSEENPH12038691

    How are average life and decay constant related?

    Solution
    Average life of nucleus is related to the decay constant as:
                              τ = 1λ.
    where, 
    T is the average life and, 
    λ is the decay constant. 
    Question 521
    CBSEENPH12038692

    Write the equation of decay of the radioactive nuclei.

    Solution
    The equation of decay of the radioactive nuclei is given by: 
     
                               N = N
    0 e-λt
    where, 
    N is the number of nuclei in the sample at time t, 
    No is the number of radioactive nuclei at any arbitary time to , and
    λ is the decay constant. 
    Question 522
    CBSEENPH12038693

    Why is a neutron most effective as a bullet in nuclear reaction?

    Solution
    Neutron is most affective as a bullet in nuclear reaction because a neutron carries no charge. It can hit the nucleus directly without being repelled by the nucleus or electrons.
    Question 523
    CBSEENPH12038694

    Define the activity of a radionuclide. Write its SI unit. Give a plot of the activity of a radioactive species versus time. 

    Solution

    The number of radioactive disintegrations taking place per second in a given sample is called the activity of a sample. 

    Its SI unit is becquerel.

    The graph between the activity of a radioactive species and time is given below: 

     


    Question 524
    CBSEENPH12038695

    What is the activity of one gram of Ra88226, whose half-life is 1622 years?

    Solution
    The number of atoms in 1g of radium is, 

                 N = 6.023 × 1023226   = 2.666 ×1021 atoms 

    The decay constant is related to the half-life by,
                             λ = 0.693T1/2  

    Therefore, 
    λ = 0.6931622 y 1y365 d 1d8.64 × 104s    = 1.355 × 1011s-1 

    The activity is then found from, 

    Activity = λN               = (1.355 × 10-11 s-1) (2.666 × 1021)               = 3.612 × 1010 disintegration/s. 

    The definition of the curie is 1 Ci = 3.7 × 1010 disintegrations/s. This is approximately equal to the value found above.
    Question 525
    CBSEENPH12038696

    Why is it necessary to slow down the neutrons, produced through the fission of U92235 nuclei (by neutrons), to sustain a chain reaction? What type of nuclei are (preferably) needed for slowing down fast neutrons?

    Solution
    Slow neutrons have a much higher intrinsic probability of inducing fission in U92235 than fast neutrons.
    Any substance which is used to slow down fast moving neutrons to thermal energies is called a moderator. Moderators are provided along with the fissionable nuclei for slowing down fast neutrons.

    The commonly used moderators are water, heavy water (D
    2O) and graphite.
    Question 526
    CBSEENPH12038697

    It is found from an experiment that the radioactive substance emits one beta particle for each decay process. Also an average of 8.4 beta particles are emitted each second by 2.5 milligram of substance. The atomic weight of substance is 230. What is the half-life?

     

    Solution

    The activity = 8.4 sec-1
    Atomic weight of the substance = 230 kg 

    Number of atoms in kilomole (i.e., 230 kg) = 6.02 x 1026 
    Therefore, 
    Number of atoms,   N = 6.02×1026230×2.5 ×10-6  

                                 = 6.54 × 1018 

                       8.4 = λN        = λ×6.54×1018   λ  = 8.4 × 10-186.54       = 1.28 ×10-18/sec 

    Half-life, T = 0.693λ  

                    = 0.6931.28 × 10-18 = 5.41 × 1017 sec

                    = 5.41×10173.16×107= 1.7×1010 years.

    Question 527
    CBSEENPH12038698

    In the deuterium-tritium fusion reaction find the rate at which deuterium and tritium are consumed to produce 1 MW. The Q-value of deuterium-tritium reaction is 17.6 MeV. You can assume that the efficiency is 100%. 

    Solution
    Energy released per fusion = 17.6 MeV 

    Number of fusion reactions to produce 1 MW, = 10617.6×1.6×10-19×106 = 3.55 × 1017 

    In each reaction one atom of deuterium and one atom of tritium are consumed. 

    Mass of 3.55 × 1017 atoms of deuterium consumed per second, 

              = 2×3.55×10176.023×1023 g = 1.1788 × 10-6 g/s= 1.179 × 10-19 kg/s 

    Mass of tritium consumed per second = 3×3.55×1076.023×1023 g/s = 1.768 × 10-6 g/s
                                                             = 1.768 × 10-9 kg/s
    Question 528
    CBSEENPH12038699

    Would the energy be released or needed for the following D-T reaction 
    H12+H13He24+n01  to occur?
    Given:
                             m(H12) = 2.014102 u,       m(H13) = 3.016049 u
                          m(He24) = 4.002603 u,     m(n01) = 1.008665 u
    and                        1 u = 931 MeV/c2
    Calculate this energy in MeV.

    Solution

    We have,

    Mass (H12) + mass (H13)  =  2.014102 + 3.016049
                                       = 5.030151 u
    and
             m (He24) + m(n01) = 4.002603 + 1.008665                                = 5.011268 u

    As seen from above, since, mass of the reactants is larger than mass of the products therefore, energy is released in this reaction.

    Now,

    Mass defect (m) = 5.030151 - 5.011268                                   = 0.018863 u 

    So, energy required  = (m) × 931 MeV 

                                   = 0.018863 × 931 MeV = 17.561453 MeV = 17.56 MeV.

    Question 529
    CBSEENPH12038700

    A radionuclide sample has No nuclei at t = 0. Its number of undecayed nuclei get reduced to No/e at t = τ. What does the term 'τ' stand for? Write, in terms of 'τ', the time interval 'T', in which half of the original number of nuclei of this radionuclide would have got decayed.

    Solution
    Here, 
    Nucleii at time t = 0 is No 
    Nucleii at time t = τ is Noe

    τ  here is the average life time of the radioactive element and is given by,  

                               τ = 1.44 T 

    where, T is the half life of the element. 

    i.e., the average life time of a radioactive element is 1.44 times the half-life of the element.
    Question 530
    CBSEENPH12038701

    Draw the graph to show variation of binding energy per nucleon with mass number of different atomic nuclei. Calculate binding energy/nucleon of Ca2040 nucleus.
    Given:
            mass of Ca2040 = 39.962589 u
           mass of proton = 1.007825 u
           mass of neutron = 1.008665 u
                  and 1 u = 931 MeV/c2.

    Solution
    The graph showing the variation of binding energy per nucleon with mass number of atomic nuclei is shown on below.


    Numerical:

    Q-value for the gien nucleus is, 

    Q = [20 mn + 20 mp - m(Ca)] c2                   
        = (20×1.008665+20×1.007825-39.962589) c2

       = 0.367211 u × 931.5u MeV= 342 MeV 

    Hence, the B.E. per nucleon of Ca2040 nucleus is, 

    QA = 34240 = 8.55 MeV/nucleon. 
    Question 532
    CBSEENPH12038703

    Define the activity of a radioactive nucleus and state its SI unit.

    Solution
    The activity of a radioactive substance is defined as the rate at which, the nuclei of its atoms in the sample disintegrate.

    Its SI unit is becquerel (or Bq).
    Question 533
    CBSEENPH12038704

    Two radioactive nuclei X and Y initially contain equal number of atoms. The half life is 1 hour and 2 hours respectively. Calculate the ratio of their rates of disintegration after two hours.

    Solution
    Given, nucleii X and Y contain equal number of atoms.
    Half-life of X , T1 = 1 hr 
    Half-life of Y , T2 = 2 hr  

    Ratio of radioactive sample of X left after 2 hours, 

                        N1=  122/1N0 = 14N0 

    Ratio of radioactive sample of Y left after 2 hours, 

                      N2 = 122/2N0 = 12N0 

    Now, deacay rate is given by, 

                  R = λN = 0.693 NT1/2 

                  R   NT1/2 

    i.e.,         R1R2 = (T1/2)2(T1/2)1×N1N2        =  21× N04N02         = 1 

    Hence, the activity of the two samples will be equal after 2 hours.
    Question 534
    CBSEENPH12038705

    Tritium has a half-life of 12.5 years against β-decay. What fraction of a sample of pure tritium will remain undecayed after 37.5 years?

    Solution

    Given, 
    Half life of tritium, T = 12.5 years
    t = 37.5 years

    Now, using the formula for decay rate,  

                    NN0 = 12n = 121T1/2 

    we have, NN0 = 1237.512.5 = 123 = 18. 

    Thus, one-eighth of the sample will remain undecayed after 13.5 years.

    Question 535
    CBSEENPH12038706

    Define the term decay constant of a radioactive nucleus.
    Two nuclei P, Q have equal number of atoms at t = 0. Their half lives are 3 hours and 9 hours respectively. Compare their rates of disintegration, after 18 hours from the start.

    Solution
    Decay constant of a radioactive element is the reciprocal of the time during which the number of atoms left in the sample reduces to 1e times the number of atoms in the original sample. 

    Given, two nucleii  P and Q. 
    P and Q have equal number of atoms at t=0. 
    Half life of P = 3 hours. 
    Half life of Q = 9 hours. 

    and, t = 18 hours

    Number of half lives of P in 18 hours  =tT12183=6 

    Number of nuclei P left undecayed after 6 half lives is, 
                          N1 = N126 

    Number of half lives of Q in 18 hours=tT12 = 189=2 

    Number of nuclei of Q left undecayed after 2 half lives is, 

                           N2 = N122 

    Ratio of their decay rate is, 

                   R1R2 = λ1 N1λ2 N2 = T2 N1T1 N2 

      R = λ N and T = 0.693λ 

                   R1R2 = 93×N126N122 = 316 

    Hence ratio of disintegration is, R1:R2 = 3 :16
    Question 536
    CBSEENPH12038707

    A radioactive sample contains 2.2 mg of pure C611, which has half-life period of 1224 seconds.
    Calculate
    (i)    the number of atoms present initially.
    (ii)   the activity when 5 μg of the sample will be left. 

    Solution
    Given, 
    Mass of pure sample of carbon, C611 = 2.2 mg 
    Half-life period of sample, T1/2 = 1224 seconds 


    (i) The number of atoms present intially is, 

    = 2.2×10-3×6.023×102311= 1.2 × 1020 atoms 

    (ii) The number of atoms present in 5 μg, 

    = 5×10-6×6.023 ×102311 = 2.74 × 1017 atoms 

    Activity is given by, 

                          R = λN     = 0.693 NT1/2    = 0.693 × 2.74 × 10171224    = 1.55 × 1014.
     
    Question 537
    CBSEENPH12038708

    A neutron is absorbed by a Li36 nucleus with the subsequent emission of an alpha particle.
    (i)    Write the corresponding nuclear reaction.
    (ii)   Calculate the energy released, in MeV, in this reaction.
    [Given: mass Li36 = 6.015126 u;   mass (neutron) = 1.0086654 u  mass (alpha particle) = 4.0026044 and mass (triton) = 3.0100000 u.  Take 1 u = 931 MeV/c2].

    Solution

    i) Nuclear reaction is given as, 

                    Li36 + n01  He24 + H13 + Q 

    ii) Mass defect (m)

         = [m (Li36) + m(n01) - m(He24) - m(H13)]= [6.015126+1.0086654-4.0026044 - 3.01]

        = [7.0237914 u  - 7.0126044 u]= 0.0111870 u     

     Energy released = 0.0111870 x 931
                                  = 10.415 MeV.

    Question 538
    CBSEENPH12038709

    Calculate the force between two fission fragments of equal masses and sizes that are produced in the fission of Pu94239 (by a thermal neutron) in which 4 neutrons are emitted. Given R0 = 1.2 fm. 

    Solution

    The undertaking fission process can be wriiten as : 

                  Pu94239 + n01  2 X47118 + 4 n01 + Q 

    Total mass number of Pu94239 and neutron = 240 

    Mass number of each fragment = 240-42 = 118

    Atomic number of each fragment = 942 = 47 

    Radius of each nucleus formed by the fission of Pu94239 is, 

                           R = R0 A1/3 

                              = 1.2 × 10-15 × (118)1/3 = 5.886 × 10-15m 

    Distance between the centre of the two fragments = 2 × 5.886 ×10-15 m = 11.77 × 10-15m 

    Electrostatic force between them is given by Coulomb's law, 
                            F = 14πεoq1q2r2 

    Therefore, 

          F = 14πε0(47×1.6×10-19)2(11.77 ×10-15)2 = 3.763 × 103N.

    Question 539
    CBSEENPH12038710

    Explain, with the help of a nuclear reaction in each of the following cases, how the neutron to proton ratio changes during α-decay.

    Solution

    The α-decay of Uranium is given by, 

                      U92238  Th90234 + He24 

    Neutron to proton ratio before α-decay= 238-9292 = 14692
                                       
    Neutron to proton ratio after α-decay= 234-9090 = 14490
                                           
    Since,          14490>14692      


    Thus, the neutron to proton increases is an α-decay

    Question 540
    CBSEENPH12038711

    Explain, with the help of a nuclear reaction in each of the following cases, how the neutron to proton ratio changes during β-decay?

    Solution
    Alpha-decay of Bismuth is shown below: 

                       Bi83210  Po84210 + e-10 

    Neutron to proton ratio before β-decay= 210-8383= 12783
                                    
    Neutron to proton ratio after β-decay= 210-8484 = 12684
                                      

    Since,          12684<12783 

    Thus, the neutron to proton ratio decreases in a β-decay.

    Question 541
    CBSEENPH12038712

    Group the following six nuclides into three pairs of (i) isotones, (ii) isotopes and (iii) isobars:
     612C,   23He,   80198Hg,  13H,  79197Au,  614C
    How does the size of a nucleus depend on its mass number? Hence explain why the density of nuclear matter should be independent of the size of the nucleus.  

    Solution

    Classification of nuclides is as follows: 

    IsotopesC 612, C614 ; has the same atomic number but, different mass number. 

    Isobars : He23, H13 ; has the same mass number but, different atomic number.

    Isotones 80198Hg,  79197Au ; has same neutron number but, different proton number. 

    Now, 

    Radius of nucleus, R = R0 A1/3                          ...(i) 
    where,  R0 is the range of nuclear force (or Nuclear Unit Radius) 

    Density is given by, ρ = M43πR3                        ...(ii) 

    But,                         M A                               ...(iii) 

    From (i) and (iii), we get

    R M1/3  R3  M   R3 = kM where,

    kproportionality constant                                 ...(iv) 

    From (ii) and (iv), we have
                                       ρ = M43πR3= 34πMKM = constant.

    Thus, we can see that nuclear density is clearly independent of mass number A. 

    Question 542
    CBSEENPH12038713

    Write the nuclear reactions for the following:
    (i) α-decay of Po84204

    (ii) β- decay of P1532

    (iii) β+ decay of C611

    Solution

    Nuclear reactions are given by: 

    (i)  α-decay : Po84204  Pb82200 + He24

    (ii) β- decay : P1532  S1632 + e-10 + v¯.

    (iii) β+ decay : C116   B511 + e+10 + v.¯

    Question 543
    CBSEENPH12038714

    The binding energy per nucleon of O816 is 7.97 MeV and that of O17 is 7.75 MeV. Calculate the energy required to remove a neutron from O817.

    Solution
    The nuclear reaction is represented as follow: 

                            O817   O816 + n01 

    B.E per nucleon of O816 = 7.97 MeV 

    B.E per nucleon of O17 = 7.75 MeV 

    Energy required to remove a neutron from O817 = ? 

    If mp represents the mass of a proton and mn that of a neutron, the energy required to remove a neutron from O817 is given by, 

    E = energy equivalent of (mass of O816 + mn - mass of O817)

        = (8 mp + 8 mn- 7.97 ×16) + mn - (8mp+9mn - 7.75 × 17)

       =[7.75×17-7.97×16] MeV  = 4.23 MeV. 


    Question 544
    CBSEENPH12038715

    The half-life of U92238 against α-decay is 4.5 × 109 years. Calculate the activity of 1g  sample of U92238.

    Solution
    Given, 

    Half life of Uranium, T1/2 = 4.5×109 years                                               = 4.5 × 109 × 3.156 × 107s 

    Number of atoms in 1g of uranium,  N = 6.023 × 1023238 atoms 

    Activity of the sample  = λN 

                                      = 0.693T1/2×N 

                                      = 0.693 × 6.023 × 10234.5 ×3.156×1016×238
                                       = 1.235 × 104 disintegration/second.
    Question 545
    CBSEENPH12038716

    Show that the decay rate 'R' of a sample of a radionuclide is related to the number of radioactive nuclei 'N' at the same instant by the expression R = λ N.

    Solution

    (a) For, a radioactive sample, rate of disintegration is given by, 

                               R = -dNdt                           ...(i) 

    According to radioactive decay law,
                            -dNdt N 

                       -dNdt = λN                             ...(ii) 

                               R = λN                  [By equation (i) and (ii)] 

    (b) Activity of a sample is, 

                            R = λN = 0.693T1/2× N          λ = 0.693T1/2
                               = 0.6931.5×1017×25×1020 

                               = 11550 disintegrations/second.

    Question 546
    CBSEENPH12038717

    Define nuclear force. Give its two most important characteristics.What is the energy released if all the deuterium atoms in a lake of cross sectional area 2.56 × 105 (km)2 and depth 80 m is used in fusion? Given abundance of H12 = 0.0156% of hydrogen density of water = 103 kg m-3 energy released due to fusion of one atom of H12 = 7.17 MeV. 

    Solution
    Nuclear force is a strong attractive force acting between the nucleons of the atomic nucleus that holds the nucleus together. 

    Characteristics of nuclear force : 

    i) Nuclear forces are short range forces operating upto a distance which is of the order of a few fermi. 

    ii) Nuclear forces are strongest force in nature. It's magnitude is 100 times that of the electrostatic force and 1038 times that of the gravitational force. 

    Numerical:

    The volume  V of lake is, V = 2.56 ×105 × 106 × 80 m3   = 2.048 × 1013 m3 

     Mass of water, M in lake  = 2.048 x 1013 x 103
                                              = 2.048 x 1016 kg
                                              = 2.048 x 1019 gm 

    Now, 18 g of water contains 2 g of hydrogen. 

     Mass of hydrogen atom in lake = 19×2.048×1019g 

     Number of atoms of hydrogen in lake = 
    6.023 × 1023 × 2.048 × 10199
                                                                   = 1.37 × 1042 

    Since abundance of H12 is only 0.0156% of hydrogen atoms, the number of H12 atoms in lake, 

    = 1.37 × 1042 × 1.56 × 10-4 = 2.137 × 1038 

    Energy released due to fusion of one atom of   H12 = 7.17 MeV 

     Energy released when all H12 atoms present undergo fusion, 

                  = 2.137 × 1038 × 7.17 MeV= 1.532 × 1039 MeV.
    Question 547
    CBSEENPH12038718

    An unstable element is produced in nuclear reactor at a constant rate R. If its half-life β--decay is T1/2, how much time, in terms of T1/2, is required to produce 50% of the equilibrium quantity?

    Solution

    We have, 

    Rate of increase of element = number of nuclei by reactor1 second-number of nuclei decaying1 second

    That is, 
                     dNdt = R - λN   or   dNdt+λN  = R 
                          
    The solution to this is the sum of the homogeneous solution, 
                  Nh = ce-λt, where c is a constant, and

    a particular solution, Nl = Rλ. 

    Therefore, the required solution is, 

                           N = Nh+Np = ce-λt+Rλ 

    The constant c is obtained from the requirement that the initial number of nuclei be zero, 
                               N(0) = 0 = c+Rλ  
      c = -Rλ
    so that,                N = Rλ(1-e-λt) 

    The equilibrium value is (t) = R/λ. 

    Setting N equal to 1/2 of this value gives, 

                      12Rλ = Rλ(1-e-λt) 

                           e-λt = 12    

               t = ln 2λ = T1/2 

    The result is independent of R.

    Question 548
    CBSEENPH12038719

    State the laws of radioactivity.
    A radioactive substance has a half-life period of 30 days. Calculate (i) time taken for 34 of original number of atoms to disintegrate and (ii) time taken for 18 of the original number of atoms to remain unchanged.

    Solution
    In any radioactive sample, undergoing α, β or γdecay, the number of nucleii undergoing decay per unit time is directly proportional to the total number of nuclei in the sample. This is known as the radioactive decay law. 

    Let, N be the number of nucleii in the sample, 
    N is the sample undergoing decay and, 
    t  is the time then, 

                                Nt  N 

                            Nt= λN 

    where, λ is the decay constant. 


    Numerical: 

    Half -period of radioactive substance = 30 days
    Number of atoms disintegrated = 34  N0
    Number of atoms left after time t,  N = N0 - 34N0 = 14N0 

    Number of half lives in time t days,
                                        
                            n = tT = t30
    where, 

    T = Half life time
    n = no. of half lives
    t = time for disintegrates 

    Number of nuclei left after n half lives is given by, 

                          N = N012N 
    Therefore, 
                        N04 = N012t/30  

                (2)t/30 = 4 = (2)2

                   t30 = 2  or  t = 60 days

    (ii) Now, using the formula,  N = N012n

                        N08 = N012t/30

                   (2)t/30 = 8 = (2)3      
          
                      t30 = 3
    i.e.,                      t = 90 days, is the time taken for 1/8 of the original number of atoms to remain unchanged.

                                            
                                        

     
    Question 549
    CBSEENPH12038720

    It is proposed to use the nuclear fusion reaction
    H12+H12  He24
    in a nuclear reactor of 200 MW rating. If the energy from the above reaction is used with a 25% efficiency in the reactor, how many grams of deuterium fuel will be needed per day? 
    (The masses of H12 and He24 are 2.0141 atomic mass unit and 4.0026 atomic mass unit (u) respectively.)

    Solution
    The given nuclear fusion reaction is, 

                     H12 + H12  He24 

    The 'mass defect' for this reaction is, 

    m = (2 × 2.0141 - 4.0026) u          = (4.0282 - 4.0026) u          = 0.0256 u 

    Therefore, 
    Energy released is,

      E' = 0.0256 × 931 MeV          = 23.8336 MeV         = 23.8336 × 1.6 × 10-13J           = 38.134 × 10-13J 

    Since the reaction has a utilization efficiency of 25%, the energy utilized per reaction is, 

    E = 38.134 × 10-13 × 25100J        = 9.533 × 10-13J 

    The reactor rating is 200 MW. 

    Hence, the total energy required per day is, 

    E = 200 × 106×24×60×60 s 

      = 172.8 × 1011J 

    Now, 2 deuterium atoms provide us with an 'available energy' of 9.533 x 10-13J. 

    Hence, the number of deuterium atoms needed per day is, 
                                 n = EE = 172.8 × 1011 ×29.533 × 10-13                    = 36.25 × 1024 

    Now, 1 mole = 6.02 × 1023 atoms of deuterium has a mass of 2.0141 g.

    Thus, the mass of deuterium needed per day is, 

         m = 2.0141 × 36.256.02 × 1023× 1024g      = 121.3 g.
    Question 550
    CBSEENPH12038721

    A nucleus with A = 235 splits into two new nuclei whose mass number are in the ratio of 2:1. Find the radii of the new nuclei.

    Solution
    Relation between radius R of a nucleus and mass number A is given by, 

                            R = R0 A1/3 

    where, Ro = 1.4 fm.

    Mass number of the nucleus, A = 235 

    Let A
    1 and A2 represent the mass numbers of the new nuclei which are formed when the nucleus with mass number A splits into two halves.
    Let R
    1 and R2 be the radii of the new nuclei so formed.

    Given, 
                        A1 + A2 = 235 and
                         A1 : A2 = 2:1 
    This implies, 
                             A2 = 2 A1

    Then we have,

                           A1 = 13(235)

    and,                A2 = 23(235) 

    Using,                R = R0 (A)1/3  

    we have,          R1 = R0 (A)1/3

    That is,  
         R1 = (1.4 fm) 23531/3 = 5.99 fm 

    and                  R2 = R0(A2)1/3

      R2= (1.4 fm) 235 × 231/3 = 7.55 fm. 

    Thus, radii of the new nucleii are 5.99 fm and 7.55 fm respectively.
    Question 551
    CBSEENPH12038722

    The radioactive decay rate of a radioactive element is found to be 10disintegrations/sec., at a certain time. If half-life of the element is one second, what would be the decay rate after 1 sec., and after 3 sec.?

    Solution
    Radioactive decay rate is directly proportional to the number of nuclei left. 

    N0 = 10disintegrations/sec. 

    Half-life, T = 1 sec., 

    Therefore, 

    (i) Number of half lives in 1 sec., n = 1 

    As,               N = N012n                

                     N = 1000121 = 500 

     Number of disintegrations/sec. after one sec. = 500
    (ii) Number of half lives in 3 sec. = n = 31 = 3
    As,             N = N012n 

          N = 1000123 = 10008 = 125 

    Therefore, number of disintegrations per second after three second is 125.
    Question 552
    CBSEENPH12038723

    The disintegration rate of a certain radioactive sample at any instant is 4750 disintegrations per minute. 5 minutes after, the rate becomes 2700 disintegrations per minute. Calculate the decay constant.(log10 1.76 = 0.2455).

    Solution
    Disintegration rate is proportional to the number of atoms present. 

                  N0N = 47502700 = 1.76

    Now, using the relation, 

                               N = N0e-λt

                            N0N = eλt     

                   logeN0N = λt

            λ = loge(N0/N)t = 2.3026 log10 (1.76)t

            λ= 2.3026 × 0.24555 = 0.1131 min-1. is the required value of decay constant. 
    Question 553
    CBSEENPH12038724

    A radioactive isotope X has a half-life of 3 seconds. At t = 0 second, a given sample of this isotope X contains 8000 atoms. Calculate (a) its decay constant, (b) the time t1'when 1000 atoms of the isotope X remain in the sample and (c) the number of decays per second in the sample at t = t1 second.

    Solution

    Half life of isotope X = 3 seconds.
    Number of atoms at t=0 is 8000 atoms. 

    (a) Decay constant,  
                              λ  = 0.6931T    = 0.69313    = 0.231 s-1 

    (b) Atoms remaining in the sample = 1000

    Time t1 at which these many sample is remaining = ?

    Now, using the formula of the law of radioactive decay we have, 

                  t1= 1λlogeN0N  = 2.30260.231 log10 8  = 9s 

    (c) Number of decays per second in the sample is, 
                -dNdt = λN              = 0.231 × 1000             = 231 s-1

    Question 554
    CBSEENPH12038725

    Why heavy stable nucleus must contain more neutrons than protons? What is the effect on neutron to proton ratio in a nucleus when
    (i) an electron is emitted
    (ii) a positron is emitted?

    Solution
    Heavy nuclei generally have neutron to proton ratio lower than 1. In order to be stable, the neutron to proton ratio must approach 1. Hence, heavy stable nucleus must contain more neutrons than protons. 

    (i) When an electron is emitted, neutron to proton ratio decreaes. 

    (ii) Neutron to proton ratio decreases when positron is emitted.
    Question 555
    CBSEENPH12038726

    You are given two nuclei X37 and Y34. Explain giving reasons, as to which one of the two nuclei is likely to be more stable?

    Solution

    In case of X37

    Neutron to proton ratio is, 

    neutron numberproton number = 7-33 = 43 = 1.33 

    In case of Y34, neutron to proton ratio is given by, 
                             neutron numberproton number =4-33 = 13 = 0.33 

    For stability, this ratio has to be close to one. 

    Therefore, nucleus X37 is more stable than the nucleus Y34.

    Question 556
    CBSEENPH12038727

    The mean-life of a radioactive sample is Tm. What is the time in which 50% of this sample would get decayed?

    Solution

    The half-life period is, 
     
                       T1/2 = 0.693 Tm 

    where, Tm is the mean half-life.

    To decay by 50% of the sample one half-life is required.

    Therefore, time taken is 0.693 Tm to decay by 50%.

    Question 557
    CBSEENPH12038728

    10 mg of carbon from living matter produce 200 counts per minute due to a small proportion of the radioactive isotope carbon-14. A piece of ancient wood of mass 10 mg is found to give 50 counts per minute. Find the age of the wood assuming that carbon-14 content of the atmosphere has remained unchanged. The half-life of carbon-14 is 5700 years.

    Solution
    The amount of 14C in the atmosphere remains constant. A living matter represents the amount of C14 present in the atmosphere. Ancient wood has 50 counts per minute. 10 mg in the beginning, must have the same count rates as from living matter. 

    Thus, the age of the ancient wood is the time in which the 
    14C count rate has decreased from the initial value of 200 counts per minute from 10 mg to the final value of 50 counts per minute from 10 mg. 

    We know that half life (T1/2) for carbon is 5700 years.

    If n is no of half lives then, 

                  N = N0. 12n50 = 200 12n50200 = 12n 

                      14 = 12n122 =12n
     
     n = 2 half lives required time    = 5700 × 2     = 11400 years     = 1.14 × 104 years.

    Question 558
    CBSEENPH12038729

    Name the physical quantity whose SI unit is becquerel (Bq). How is this quantity related to (i) disintegration constant, (ii) half-life, and (iii) mean-life of the radioactive element?

    Solution

    Radioactivity is the physical quantity whose SI unit is Bq. 

    (i) Relation between radioactivity and disintegration constant is as follows: 

                       R = R0e-λt or R = λN

    where, λ is disintegration constant. 

    (ii) Relation between radioactivity and half life is,

                              R = 0.693T1/2N 

    where T1/2 is the half-life period.

    (iii) Relation between radioactivity and mean-life of the element is,
                               R = 1TmN 

    where, Tm is the mean-life.

    Question 559
    CBSEENPH12038730

    Write the equations for the two types of β-decay. Why is it very difficult to detect the neutrino?

    Solution
    Equation for negative β decay, 

                      XZA  YZ+1A +e01 + v¯ 

    Reaction process for positive β-decay,

                      XZA  YZ-1A + e01 + v 

    Neutrino is an uncharged particle which interacts very weakly with matter and hence escapes undetected.
    Question 575
    CBSEENPH12038746

    Calculate the half-life period of a radioactive substance if its activity drops to 1/16th of its initial value in 30 years.

    Solution

    The activity of a radioactive substance at any time 't' is given by, 
                           A = Ao e-λt                ... (1) 
    where, 

    A is the radioactivity material remaining after time 't,
    Ao is the initial activity of the material, and
    λ is the decay constant. 

    Given that, AAo = 116  

    t = 30 years 

    Now, putting these values in equation (1), we get

          116 = e-30λ  e30λ = 16  30 λ = ln 16 = 2 ln 2        λ = ln 2 15 

    And, half life of a radioactive substance is given by, 

    T12 = ln 2λ Putting the value of λ, we get T12 = ln 2ln 215 = 15 years , 
    is the required half-period of the radioactive substance. 


    Question 576
    CBSEENPH12038747

    Derive an expression for the radius of nth orbit of hydrogen atom using Bohr's postulates. Interpret the nature of variation of the radius of orbit with the principal quantum number n.

    Solution

    According to Bohr's postulates, 

          mvr = nh2π       v = nh2πmr ... (1)Now, using the Bohr's equation,   mv2r = KZ2e2r2    ... (2)Putting (1) in equation (2), we have  

          mrn2h24π2m2r2 = KZe2r2         r = n2h24π2mKZe2 For hydrogen atom, Z= 1      r  = n2h24π2mKe2            r  n2 

    Question 577
    CBSEENPH12038748

    Two nuclei have mass numbers in the ratio 1 : 2. What is the ratio of the their nuclei densities?

    Solution

    Given, the ratio of mass number is 1:2. 

    Nuclear density is inversely proportional to mass number. 

    Therefore, 

                   ρ1ρ2 = A2A1 = 21 = 2:1 

    Question 578
    CBSEENPH12038749

    A radioactive nucleus 'A' undergoes a series of decays according to the following scheme:
    AαA1βA2αA3γA4
    The mass number and atomic number of A are 180 and 72 respectively. What are these numbers for A4?

    Solution
    In α - decay, the mass number decreases by 4 and atomic number decreases by 2. 

    In β - decay, mass number remains the same but atomic number increases by 1. 

    In γ - decay, mass number and atomic number remains the same. 

    Therefore, the equation is, 

    A18072 α A170 176  β A271176 α A369172 γ A469172 

    Mass number of A4 is 172 
    Atomic number of A4 is 69
    Question 579
    CBSEENPH12038750

    Draw a plot of potential energy of a pair of nucleons as a function of their separation. What is the significant of negative potential energy in the graph drawn?

    Solution

    Potential energy of a pair of nucleons as a function of their seperation can be shown as below: 


    The negative potential energy in the graph exhibits that the system is bounded. 

    Question 580
    CBSEENPH12038751

    The half-life period of a radioactive element X is same as the mean life time of another radio active element Y. Initially if they have the same number of atoms then which will take a faster decay?

    Solution

    Given,

    Half life for X is the same as mean life time of another radio active element Y. 

    i.e., TX = τY = 1.44 TY 

    Now, as half life of Y is shorter than half life of X, therefore Y will decay faster than X.
     

    Question 581
    CBSEENPH12038752

    Explain with an example, whether the neutron-proton ratio in a nucleus increases or decreases due to beta (P) decay.

    Solution

    Neutron to proton ratio of an atomic nucleus is the ratio of the number of neutrons to it's number of protons. This ratio generally increases with increase in atomic number, in a stable nuclei. 

    Beta decay decreases the ratio of neutron to proton. 

    e.g.,           C614 N714 + e +νe¯

    It is clearly visible that the neutron-proton decreases. 

    Question 582
    CBSEENPH12038753

    How many disintegrations per second will occur in one gram of U23892, if half life against alpha decay 8is 1.42 × 1017 s?

    Solution

    Given, half life period (T) = 0.693λ = 1.42 ×1017 s

    Therefore,

     λ = 0.6931.42×1017 = 4.88 × 10-18 

    Avogadro's number = 6.023 ×1023 

    n is the number of atoms present in 1 g of U92238 = NA  =0.623×1023238 = 25.30 ×1020  

    Number of disintegrations is given by, 

    dNdt = λn           = 4.88 ×10-18 × 25.30 × 1020           = 1.2346 × 104 disintegrations per sec

    Question 583
    CBSEENPH12038754

    In the series of radioactive disintegration of XZA first one α-particle and then one β-particle is emitted. What is the atomic number and mass number of the new nucleus formed by these successive disintegrations?

    Solution

    When an alpha particle is emitted, mass number decreases by 2 and atomic number decreases by 2 and when a beta particle is emitted, mass number remains the same and atomic number increases by 1. 

                  XZA  α Z-2   A-4X  β   XZ-1A-4 

    So, mass number becomes (A-4) and atomic number becomes (Z-1). 

    Question 584
    CBSEENPH12038755

    Calculate binding energy per nucleon of Ca2040 nucleus.
    (Given: mass of Ca2040 = 39.962589 u; mass of proton = 1.007825 u;  mass of neutron = 1.00865 u;   1 atomic unit (1u) = 931 MeV)

    Solution

    Given, Ca2040 contains 20 protons and (40-20) = 20 neutrons. 

    Mass of 20 protons = 20 × 1.007825 = 20.1565 a.m.u
    Mass of 20 neutrons  = 20 × 1.008665 = 20.1733 a.m.u 

    Therefore, total mass of 40 nucleons = 40.3298 a.m.u

    Given that mass of Ca2040 =  39.962589 a.m.u 

    Therefore, mass defect,m = 40.3298 - 39.962589 = 0.367211 a.m.u 

    Total binding energy per nucleon is given by, 

    0.367211×931.540 = 8.55 MeV
     


    Question 585
    CBSEENPH12038756

    Calculate the mass of 1 curie of RaB (Pb2) from its half-life of 26.8 minutes.

    Solution

    Given, 
    Half life of RaB = 26.8 min

    Activity of RaB = dNdt = 1 curie = 3.7 × 1010 disintegrations/s

    If, λ is the disintegration constant of RaB, we have
                        λ = 0.693T

                           = 0.69326.8 ×60s-1

    Let N be the number of atoms of RaB having an activity of 1 curie. Then , 

    we have       dNdt = λN

                         N = dNdtλ 

                  N = 3.7×1010×26.8×600.693

    Further we know that, 

    1g of atom = 6.02 × 1023 atoms. 

    Mass of 1 curie of atom = 214g = 2146.02 × 1023 

    Therefore, the mass of RaB having an activity of 1 curie is, 

             = 214 × 3.7 × 1010 × 26.8 × 606.02 × 1023 × 0.693= 30.52 × 10-9g. 

    Question 586
    CBSEENPH12038757

    We are given the following atomic masses: 

    U92238 = 238.05079 u     He24 = 4.00260 uTh90234 = 234.04363 u    H11 = 1.00783 uPa91237 = 237.05121 u 

    Here the symbol Pa is for the element protactinium (Z = 91). 

    (a) Calculate the energy released during the alpha decay of U92238. 

    (b) Calculate the kinetic energy of the emitted α-particles. 

    (c) Show that U92238 cannot spontaneously emit a proton.

    Solution

    (a) The alpha decay of U92238 is given by, 

                     U92238 α  Th90234 + He24 

    The energy released in this process is given by 

                  Q = (Mu - MTh - MHe) c2    ... (1)

    Substituting the atomic masses as given in the data in equation (1), we find 
                              Q = (238.05079 - 234.04363 - 4.00260) u x c2 
       = (0.00456 u) c2= (0.00456 u) (931.5 MeV/u)= 4.25 MeV 

    (b) The kinetic energy of the α- particle is, 

     Eα  A-4AQ       = 234238×4.25       = 4.18 MeV 

    (c) If U92238  spontaneously emits a proton, the decay process would be, 

                 U92238  Pa91237 + H11 

    The Q for this process to happen is, 

    = (MU - MPa - MH) c2 = (238.05079 - 237.05121 - 1.00783) u × c2= (-0.00825 u) c2= -(0.00825 u) (931.5 MeV/u)= -7.68 MeV 

    Since the Q-value for this process is negative, it cannot proceed spontaneously and will require 7.68 MeV energy. 

    Question 588
    CBSEENPH12038759

    Which of the statements given in Question 14.1 is true for p-type semiconductors.

    Solution
    In p-type semiconductor holes are majority carriers and electrons are minority carriers and p-type semiconductor is obtained by doping Ge or Si with trivalent atoms.  

    Hence (d) is correct.
    Question 590
    CBSEENPH12038761

    In an unbiased p-n junction, holes diffuse from the p-region to n-region because
    (a)    free electrons in the n-region attract them.
    (b)    they move across the junction by the potential difference.
    (c)    hole concentration in p-region is more as compared to n-region.
    (d)    all the above.

    Solution
    (c) is the correct statement. 

    In an unbiased p-n junction, hole concentration in p-region is more than in n-region and due to difference in concentration of charge carriers, holes diffuse from p-region to n-region.
    Question 591
    CBSEENPH12038762

    State True or False:

    When a forward bias is applied to a p-n junction, it

    A.

    Raises the potential barrier.

    B.

    Reduces the majority carrier current to zero.

    C.

    Lowers the potential barrier.

    D.

    None of the above.

    Solution
    A. FALSE
    B. FALSE
    C. TRUE
    D. FALSE
    When a forward bias is applied across the p-n junction, the applied voltage opposes the barrier voltage. Due to it, the potential barrier across the junction is lowered. Hence answer (c) is correct.
    Question 592
    CBSEENPH12038763

    State True or False:

    For transistor action, which of the following statements are correct:

    A.

    Base, emitter and collector regions should have similar size and doping concentrations.

    B.

    The base region must be very thin and lightly doped.

    C.

    The emitter junction is forward biased and collector junction is reverse biased.

    D.

    Both the emitter junction as well as the collector junction are forward biased.

    Solution
    A. FALSE
    B. TRUE
    C. TRUE
    D. FALSE
    Statements (b) and (c) are true. 

    For a transistor, β = ICIB  

                         IB = ICβ 

                       Ri = ViIB = ViICβ

     i.e.,                 Ri  IIc 

    Therefore, Ri depends upon collector current IC.

    For a transistor action, the emitted junction is forward biased and collector junction is reverse biased.

    Question 593
    CBSEENPH12038764

    For a transistor amplifier, the voltage gain
    • remains constant for all frequencies.
    • is high at high and low frequencies and constant in the middle frequency range.
    • is low at high and low frequencies and constant at mid frequencies.
    • None of the above

    Solution

    C.

    is low at high and low frequencies and constant at mid frequencies.For a transistor amplifier, the voltage gain is low at high and low frequencies and constant at mid frequencies.
    Question 594
    CBSEENPH12038765

    In half-wave rectification, what is the output frequency if the input frequency is 50 Hz. What is the output frequency of a full-wave rectifier for the same input frequency.

    Solution
    Given,
    Input frequency for half-wave and full-wave rectifier = 50 Hz. 

    Input and output waveforms of half-wave and full-wave rectifier are shown in figures (a) and (b).
     

    During a cycle, half-wave rectifier conducts once and 
    full-wave rectifier conducts twice.
    Therefore, output frequency for half-wave and full-wave rectifier are 50 Hz and 100 Hz respectively.

    Question 595
    CBSEENPH12038766

    For a common emitter-transistor, amplifier, the audio signal voltage across the collector resistance of 2 kΩ is 2 V. Suppose the current amplification factor of the transistor is 100, find the input signal voltage and base current, if the base resistance is 1 kΩ.

    Solution

    Given, a common-emitter transistor configuration. 

    Collector resistance, Rc = 2000 ΩOutput voltage, V0 = 2 VCurrent amplification factor, βac = 100Input voltage, Vi = ? Current across base, Ib = ?   Input resistance, Ri = 1000 Ω 

    As, voltage gain, Av = V0Vi = βacR0Ri 

     Input signal voltage, Vi = V0βac. (R0/Ri)   

                                            = 2100(2000/1000) = 0.01 V 

    Base current,  Ib = ViRi = 0.01 V1000 Ω = 10 μA.

    Question 596
    CBSEENPH12038767

    Two amplifiers are connected one after the other in series (cascaded). The first amplifier has a voltage gain of 10 and the second has a voltage gain of 20. If the input signal is 0.01 V, calculate the output a.c. signal.

    Solution

    Given, two amplifiers are cascaded in series.

    Voltage gain of first amplifier = 10 
    Voltage gain of second amplifier = 20 
    Input signal = 0.01 V

    Therefore,
    Total voltage gain, AV =  V0Vi = Av1 × Av2

                         V0 = Vi × AV1 × AV2  

                                     = 0.01 × 10 × 20 = 2 V.

    is the output a.c. signal. 

    Question 597
    CBSEENPH12038768

     A p-n photodiode is fabricated from a semiconductor with band gap of 2.8 eV. Can it detect a wavelength of 600 nm?

    Solution

    Given, 
    Energy band gap, Eg = 2.8 eV 
    Wavelength of the photon, λ = 600 nm 

    Using the formula for energy of a photon, 

                             E = hcλ  

    we have, E = 6.6 ×10-34×3×108600×10-9×1.6×10-19eV  

                      = 2.06 eV < 2.8 eV (Eg) 


    As, E < Eg, so p-n junction cannot detect the radiation of given wavelength.

    Question 598
    CBSEENPH12038769

    The number of silicon atoms per m3 is 5 x 1028. This is doped simultaneously with 5 x 1022 atoms per m3 of Arsenic and 5 x 1020 per m3 atoms of Indium. Calculate the number of electrons and holes. Given that ni = 1.5 x 1016 m–3. Is the material n-type or p-type?

    Solution
    Number of Arsenic atoms per m3 =5 x 1022 
    Number of Indium atoms per m3 = 5 × 1020
    Intrinsic concentration, n= 1.5 x 1016 m–3

    Therefore, 

    Number of electrons, n
    e = 5 x 1022 – 5 x 1020 

                                         = (5 – 0.05) x 1022 

    Now, number of holes is, nh = ni2ne 

                                         = 1.5 × 10164.95 × 1022 = 4.54 × 109 m-3 

    Since, ne > n, so the material is n-type semiconductor.
    Question 599
    CBSEENPH12038770

    In an intrinsic semiconductor the energy gap Eg is 1.2 eV. Its hole mobility is much smaller than electron mobility and independent of temperature. What is the ratio between conductivity at 600 K and 300 K? Assume that the temperature dependence of intrinsic carrier concentration ni is given by
    ni = n0 exp -Eg2 kBT, where n0 is a constant and kB = 8.62 x 10–5 eV/K.

    Solution
    Given, 
    Energy gap in a semiconductor, Eg = 1.2 eV

    Assuming, temperature dependance of intrisic semiconductor is, 
                       ni = n0 exp -Eg2 kBT 
    and here, 

    Eg2k1T1 - 1T21.22×8.62×10-51300-1600 = 11.59

    Therefore,

                    ni1ni2 = 1.2 eVe2×kB×6001.2 eVe2×kB×300 


                           = e1.2 eV2 ×kB 1300-1600 

                           = e1.2×1.6×10-192×1.381×10-23×600 

                ni1ni2 = e11.59 = 1.072 × 105 

    is the required ratio of conductivity.


    Question 600
    CBSEENPH12038771

    You are given the two circuits as shown in figure. Show that circuit (a) acts as OR gate while the circuit (b) acts as AND gate.

    Solution
    (a) Here,
    In figure (a) input A and B is applied to NOR gate. So the output of NOR gate is Y’. 
    Truth table is given below:

    A

    B

    Y’

    0

    0

    1

    0

    1

    0

    1

    0

    0

    1

    1

    0

    Now Y’ is feeded as input into NOT gate.
    So output Y is represented in form of truth table as shown.

    Input

    Y’

    Output

    Y = Y’

    1

    0

    0

    1

    0

    1

    0

    1

    which is similar to the truth table of OR gate.

    The boolean expression for the circuit is as follows: 
                   y = A+B______ = A+B which is the expression for OR gate. 

    (b) Here in figure (b), input A and B are given to two NOT gates and these inverted input is provided to NOR gate.
    Its truth table can be represented as:

     

    Output of NOT gats

    A

    B

    Ā

    B¯

    0

    0

    1

    1

    0

    1

    1

    0

    1

    0

    0

    1

    1

    1

    0

    0

    Now output of NOT gate is fed as input to NOR gate. So its truth table can be represented as:

    Input

    Output

    Ā

    B¯

    Y

    1

    1

    0

    1

    0

    0

    0

    1

    0

    0

    0

    1

    which represents AND operation.

    The boolean expression for circuit (b) is: 

                y = A- + B - = A- . B -  = A . B which the expression for AND gate. 

     
    Question 601
    CBSEENPH12038772

    Write the truth table for a NAND gate connected as given in figure.
     

    Hence identify the exact logic operation carried out by this circuit.

    Solution
    The truth table for the circuit:

    A

    Y

    0

    1

    1

    0

     
     
    This can be represented as Y = Ā 

    Therefore, according to the truth table, the circuit represents NOT gate.
    Question 602
    CBSEENPH12038773

    You are given two circuits as shown in figure, which consist of NAND gates. Identify the logic operation carried out by the two circuits. 


    Solution

     The truth table for first circuit:
    (a)

    A

    B

    Y’

    Y

    0

    0

    1

    0

    0

    1

    1

    0

    1

    0

    1

    0

    1

    1

    0

    1

    If we remove the intermediate output Y’, the overall result stands for the AND gate.

    A

    B

    Y

    0

    0

    0

    0

    1

    0

    1

    0

    0

    1

    1

    1

    Hence, the combinational circuit is equivalent to AND gate.

    The truth table for second circuit:
    (b)

    A

    B

    Ā

    B¯

    Y

    0

    0

    1

    1

    0

    0

    1

    1

    0

    1

    1

    0

    0

    1

    1

    1

    1

    0

    0

    1

    If we remove the intermediate output Ā and B¯, the overall result stands for the OR gate.

    Truth table for the OR gate is:

    A

    B

    Y

    0

    0

    0

    0

    1

    1

    1

    0

    1

    1

    1

    1

    This can be represented as Y = A + B

    Hence, the circuit is an equivalent OR gate.

    Question 603
    CBSEENPH12038774

    Write the truth table for circuit given in figure below consisting of NOR gates and identify the logic operation (OR, AND, NOT), which this circuit is performing.

    (Hint: A = 0, B = 1 then A and B inputs of second NOR gate will be 0 and hence Y = 1. Similarly work out the values of Y for other combinations of A and B. Compare with the truth table of OR, AND, NOT gates and find the correct one.)

    Solution
    In the given figure first portion represents NOR gate, second represents NOT gate.

    First operation is to calculate the output of 1 which acts as input for 2.

    Second gate inverts it and we get final output Y. 





    Which is truth table for OR gate.

    The boolean expression for the given circuit is, 

    y, = A+B = A . B

    and 

    y = y' = A . B = A -  + B-  = A + B  which is the expresson for OR gate. 
    Question 604
    CBSEENPH12038775

    Write the truth table for the circuits given in figure. Consisting of NOR gates only. Identify the logic operations (OR, AND, NOT) performed by the two circuits.

    Solution

    Figure (a) represents NOT gate. 

    Here, when   A = 1, Y = 0
    and
            when    A = 0, Y = 1 

    Figure (b) represents two NOT gates whose outputs are given to NOR gate. 

    Truth table for this circuit is:

    A

    B

    Ā

    B¯

    Y

    0

    0

    1

    1

    0

    0

    1

    1

    0

    0

    1

    0

    0

    1

    0

    1

    1

    0

    0

    1


    which is the truth table of AND gate.

    The logic operation performed by circuit in figure (b) is AND operation.

    Question 605
    CBSEENPH12038776

    In a p-n junction diode, the current I can be expressed as
    I = I0expeV2kgT-1
    where I0 is called the reverse saturation current, V is the voltage across the diode and is positive for forward bias and negative for reverse bias, and I is the current through the diode, kB is the Boltzmann constant (8.6 x 10–5 eV/K) and T is the absolute temperature. If for a given diode I0 = 5 x 10–12 A and T = 300 K, then 

    (a) What will be the forward current at a forward voltage of 0.6 V? 

    (b) What will be the increase in the current if the voltage across the diode is increased to 0.7 V?
    (c) What is the dynamic resistance?
    (d) What will be the current if reverse bias voltage changes from 1 V to 2 V?

    Solution

    Given,
    Reverse saturation current, I0 = 5 × 10-12A
    Absolute temperature, T = 300 K 
    Boltzman constant, kB = 8.6 × 10-5eVk-1                                         = 8.6 × 10-5× 1.6 × 10-19 JK-1 
    (a) Forward voltage, V = 0.6 V, then 

    eVkBT = 1.6 ×10-19×0.68.6×10-5×1.6×10-19×300 = 23.26

    and

          I = I0exp eVkBT-1   = 5×10-12 [e23.26-1]   = 5×10-12[1.259 × 1010-1]   = 5×10-12×1.259×1010   = 0.063 A is the required forward current. 

    (b) If the forward voltage is increased to V = 0.7 V,  then 
               eVkBT=1.6×10-19×0.78.6×10-5×1.6×10-19×300          =27.14

    Therefore, 
    Forward current,  I = I0expeVkBT-1                                  = 5×10-12[e27.14-1]                                 =5×10-12[6.07×1011 - 1]                                   =5×10-12×6.07×1011                                 = 3.035 A

    Thus, increase in current is,
             I = (3.035 - 0.063) = 2.972 A 

    (c) As, I = 2.972 A,  V = 0.7 - 0.6 = 0.1 V

    Therefore, '
    Dynamic resistance =VI = 0.1 V2.972A =0.0336 Ω 

    (d) For both the voltages, the current I will be almost equal to I
    0. This implies that the circuit offers infinite dynamic resistance in the reverse bias.

    Question 606
    CBSEENPH12038777

    Give the logic symbol of AND gate.   

    Solution
    Logic symbol of AND gate is as shown below: 



    Question 607
    CBSEENPH12038778

    Give the logic symbol of NAND gate.

    Solution
     

    The above diagram gives us the logic symbol of NAND gate. 
    Question 608
    CBSEENPH12038779

    Why should a photodiode be operated at a reverse bias?

    Solution
    When, the photodiode is reverse biased then, the amount of electrons which is flowing through the p-n junction barrier is proportional to the amount of light illuminating the diode. And, as a result of the absorption of light, current is generated in the depletion region. This current which is generated is directly proportional to the intensity of light. 
    Also, the change in saturation reverse current is linearly dependent on varying incident light flux which can be measured accurately. But, this is not the same condition when the diode is forward biased. 
    Question 609
    CBSEENPH12038780

    State the factor, which controls:
    (i) Wavelength of light and (ii) intensity of light emitted by an LED.

    Solution

    (i) Wavelength of photons emitted depends upon the band gap. Thus, energy is a factor controlling the wavelength of light.

    (ii) The forward current increases as the intensity of light increases and reaches a maximum value. Further increase in the forward current results in decrease of light intensity.

    LEDs are biased such that the light emitting efficiency is maximum.

    Question 610
    CBSEENPH12038781

    At what temperature would an intrinsic semiconductor behave like a perfect insulator?

    Solution
    At T = O K, an intrinsic semiconductor will behave like a perfect insulator.
    Question 611
    CBSEENPH12038782

    Name the type of biasing of a p-n junction diode so that the junction offers very high resistance.

    Solution
    Reverse biasing is to be done so that the p-n junction offers very high resistance. 
    Question 612
    CBSEENPH12038783

    A transistor has a current gain of 50. In a CE amplifier circuit, the collector resistance is chosen as 5 kilo ohms and the input resistance is 1 kilo ohm. Calculate the output voltage if input voltage is 0.01 V.

    Solution

    Given,
    Current gain, β =50 
    Collector resistance, Rc = 5  = 5000 Ω
    Input resistance, RB = 1  = 1000 Ω
    Input voltage, vi = 0.01 V

    Using the formula for voltage gain, we have

    Voltage gain, Av = v0vi = βRCRB

     Output voltage,
                                  v0 = βRCRB × vi     = 50 × 50001000×0.01    = 2.5 V.

    Question 613
    CBSEENPH12038784

    Name one impurity each, which when added to pure Si, produces (i) n-type and (ii) p-type semiconductor.   

    Solution
    (i) On adding As (Arsenic) to pure Si, we get n-type semiconductor.

    (ii) P-type semiconductor can be obtained by doping In (Indium) to pure silicon.
    Question 614
    CBSEENPH12038785

    Why is the conductivity of n-type semiconductor greater than that of the p-type semiconductor even when both of these have same level of doping?

    Solution
    The conductivity of n-type semiconductor is greater than that of the p-type semiconductor because mobility of electrons is greater than that of holes.
    Question 615
    CBSEENPH12038786

    What is the main cause of electron's diffusion from n-type region to p-type region, even when there is no external supply used?

    Solution
    In an n-type semiconductor, the majority carriers are electrons i.e., electrons per unit volume is more whereas, in a p-type holes are the majority charge carriers. It is because of this concencentration gradient across the n- side and p- side that, the electrons diffuse from n-type region to p-type region. Mobility of electrons also contribute to the diffusion of electrons from n-type to p-type region. 
    Question 616
    CBSEENPH12038787

    Name two factors on which electrical conductivity of a pure semiconductor at a given temperature depends. 

    Solution
    Electrical conductivity of a pure semiconductor depends upon:

    (i) The width of the forbidden band.
    (ii) Intrinsic charge carrier concentration.
    Question 617
    CBSEENPH12038788

    How will collector current be affected on increasing the thickness of base in a transistor?

    Solution
    Base controls the flow of majority charge carriers from emitter to collector. Base is made thin and hence, the measure of recombination of electrons and holes is minimum. Therefore, most of the holes  or electrons coming from the emitter diffuse across the base and reach the collector. Thus, the collector current is almost equal to the emitter current.

    If the base is made thick, then most of the recombination of electrons and holes takes place in there and, the amount of collector current will enormously decrease as compared to the emitter current.
    Question 618
    CBSEENPH12038789

    How does the d.c. current gain of a transistor change, if the width of the base region is increased?

    Solution
    If the width of base region is increased then, rate of electron- hole combination process in the base increases and hence, the d.c current gain of a transistor decreases.
    Question 619
    CBSEENPH12038790

    What is the main cause of Zener breakdown?

    Solution
    Zener diode is fabricated by heavily doping p-side and n-side. So, even for a small reverse bias voltage, the electric field of the junction is extremely high. The high electric field strength pull the valence electrons from the host atoms on the p-side which are accelerated to the n-side. The electrons emitted account for high current flow, causing a breakdown called zener breakdown. 
    Question 620
    CBSEENPH12038791

    What is the ratio of the number of holes and the number of conduction electrons in an intrinsic semiconductor?

    Solution
    The ratio of the number of holes to the number of conduction electrons in an intrinsic semiconductor is 1.
    Question 621
    CBSEENPH12038792

    What type of charge carriers are there in a p-type semiconductor?

    Solution
    Holes are the majority charge carriers and free electrons are the minority charge carriers in a p-type semiconductor.
    Question 622
    CBSEENPH12038793

    What is doping?

    Solution
    The addition of a desirable impurity to an intrinsic semiconductor is called doping.
    Question 623
    CBSEENPH12038794

    What type of charge carriers are there in a n-type semiconductor?

    Solution
    Free electrons are majority charge carriers and holes are minority charge carriers in a n-type semiconductor.
    Question 624
    CBSEENPH12038795

    The a.c. current gain of a transistor is 120. What is the change in the collector current in the transistor whose base current changes by 100 μA? 

    Solution

    Given, 
    Current gain, β = 120 
    Change in base current, IB = 100 μA

    A.c current gain, βac = ICIB 

                      ICIB = 120   

                  IC100 μA =120 

           IC100×10-6 = 120 

                        IC = 120 × 100 × 10-6A         = 12 × 10-3A         = 12 mA is the change in the collector current. 

    Question 625
    CBSEENPH12038796

    In n-p-n transistor circuit the collector current is 10 mA. If 90% of the electrons emitted reach to the collector, find the base current and emitter current.

    Solution
    Given, an n-p-n transistor.

    Collector current, IC = 10 mA                    IC = 90% of IE    (given)               IC = 90100×IE               IE = IC×10090                       = 10 mA × 10090                        = 11.11 mA. 

    Base current, IB = IE - I
                           
                             = (11.11- 10) = 1.11 mA 
    Question 626
    CBSEENPH12038797

    How many NAND gates are required to make one NOT gate?

    Solution
    Only one NAND gate is required to make a NOT gate. If one input of a NAND gate is made permanently high, we get a NOT gate [see figure (a)]. 

     

    Alternatively, if both the inputs of a NAND gate are tied together, we get a NOT gate. [see figure (b)].
    Question 627
    CBSEENPH12038798

    In a transistor, current gain for common base and common emitter configurations are α and β respectively. What is the relation between a and β?

    Solution
    The relation between α and β is,  

                          β = α1-α 
    where, 
    α is current gain for common-base configuration, and
    β is current gain for common-emitter configuration. 


    Question 628
    CBSEENPH12038799

    Using the concept of electron and hole current, write an expression for the conductivity of a semiconductor.

    Solution
    The conductivity of a semiconductor,

               σ = n
    e + nh eμh

    where, 
    ne is the number of electrons, 
    e is the electronic charge, 
    μe and μh is the mobility of electron and hole respectively. 
    Question 629
    CBSEENPH12038800

    Why is NAND (or NOR) gate called a digital building block (or universal gates)?

    Solution
    All types of gates can be prepared using NAND or NOR gates. Hence, they are called digital building block or universal gates.
    Question 630
    CBSEENPH12038801

    (i) Sketch the output waveform from an AND gate for the inputs A and B shown in the figure.
     

    (ii) If the output of the above AND gate is fed to a NOT gate, name the gate of the combination so formed.  

    Solution
    (i) The output waveform of AND gate is given below: 

     

    (ii) If the output of the AND gate as shown is fed to a NOT gate, the combination so formed will be NAND gate.
    Question 631
    CBSEENPH12038802

    The output of a 2 input AND gate is fed to a NOT gate. Give the name of the combination and its logic symbol. Write down its truth table.  

    Solution
    The combination so formed is NAND gate. 



    Truth table: 

    A

    B

    Y = AB¯

    0

    0

    1

    0

    1

    1

    1

    0

    1

    1

    1

    Question 632
    CBSEENPH12038803

    Draw the (i) symbol and (ii) the reverse I-V characteristics of a zener diode. Explain briefly, which property of the characteristics enables us to use Zener diode as voltage regulator.

    Solution
    (i) Symbol of Zener diode

     

    (ii) I-V characteristics

     


    Zener diode as voltage regulator:

    When A.C. input voltage fluctuates in a rectifier, the output also varies. So, we use a zener diode as a voltage regulator to get a constant dc voltage from the unregulated dc output of a rectifier. 

     

    For input voltage Vi > V(zener voltage), Zener diode is in the breakdown condition. Thus, for wide range of values of load (RL), current through the Zener diode may change but the voltage across it remains constant. This property of the I-V characteristics enables us to use zener diode as a voltage regulator.


    Question 633
    CBSEENPH12038804

    Draw the output wave form at X, using the given inputs A, B for the logic circuit shown below. Also identify the gate.



    Solution
    NAND followed by a NOT represents an AND gate. Hence, the output waveform for the given input form will be:

     

    The combination of the gate is AND gate. 

    Question 634
    CBSEENPH12038805

    If the output of a 2 input NOR gate is fed as both inputs A and B to another NOR gate, write down a truth table to find the final output, for all the combinations of A, B. 

    Solution
    When the output of NOR gate if fed to both inputs of another NOR gate. 



    Truth table: 

    A

    B

    X

    Y

    0

    0

    1

    0

    0

    1

    0

    1

    1

    0

    0

    1

    1

    1

    0

    1


     

    Question 635
    CBSEENPH12038806

    Two signals A, B as given below, are applied as input to (i) AND (ii) NOR and (iii) NAND gates. Draw the output waveform in each case

    Solution
    Two signals A and B is given. The figure below shows us the output waveform when A and B is applied as input. 

    i) Case 1 : A and B is applied as input to AND gate.
    ii) Case 2 : A and B is applied as input to NOR gate.
    iii) Case 3 : A and B is applied as input to NAND gate.


    Question 636
    CBSEENPH12038807

    The output of an OR gate is connected to both the inputs of a NAND gate. Draw the logic circuit of this combination of gates and write its truth table.

    Solution
    The output of an OR gate is connected to both the inputs of a NAND gate. 

    Logic circuit: 



    Truth table

    A

    B

    Y’ = A + B

    Y = Y'¯

    0

    0

    0

    1

    0

    1

    1

    0

    1

    0

    1

    0

    1

    1

    1

    0

    Question 638
    CBSEENPH12038809

    Draw and explain the output waveform across the load resistor R, if the input waveform is as shown in the given figure. 

    Solution
    When the input voltage is +5V, the diode gets forward biased, the output across R is +5V, as shown in figure. 

    Output waveform



    When the input voltage is –5V, the diode gets reverse biased. No output is obtained across R when the diode is reverse biased. 

    Question 639
    CBSEENPH12038810

    What is an intrinsic semiconductor? How can this material be converted into (i) P-type , (ii) N-type extrinsic semiconductor? Draw the energy band diagram of both.

    Solution

    Semiconductors in which the number of electrons ne is equal to the number of holes nh are intrinsic semiconductors.
    When a small amount of suitable impurity is added to the intrinsic semiconductor we can convert it into an extrinsic semiconductor of either p-type or n-type. Doping changes the concentration of charge carriers in the element. 

    i) P- type: When Si or Ge is doped with any trivalent impurity like Al, B etc we get a p-type semiconductor. The dopant has one valence electron less. Thus, this atom form covalent bond with the neighbouring three atoms and, is less of one electron to offer to the fourth silicon atom and as a result there is a vacancy. Hence, an electron in the outer orbit of the neighbouring atom may jump to fill this vacancy leaving a vacancy or hole at it's own site. This hole is the conducting charge carrier. Therefore, doping with a trivalent impurity gives us p-type semiconductor. 

    Energy band diagram for a p-type semiconductor is as shown below: 




    ii) n - type: When we dope Si or Ge with pentavalent impurities like As, P then four electrons of this atom will form covalent bonds with the neighbouring Si atom in the lattice. Whereas, the fifth electron will remain loosely bound to it's parent atom. Hence, the ionisation energy which is required to make this electron free is very less and it will move around even in room temperature. Thus, the pentavalent dopant will donate one extra electron for conduction and this acts as an n-type semiconductor. 

    Energy band diagram for n-type semiconductor is as shown below: 



    Question 640
    CBSEENPH12038811

    The output of an unregulated d.c. power supply is to be regulated. Name the device that can be used for this purpose and draw the relevant circuit diagram. 

    Solution
    Zener diode is used to regulate the output of an unregulated d.c. power supply. Thus, zener diode is used as a voltage regulator.

    The relevant circuit diagram is given below. 


    Question 641
    CBSEENPH12038812

    Identify the gate shown in the figure. Explain with the help of a circuit diagram, how this gate is realised in practice. 

    Solution

    The gate shown in the figure is OR gate. 



    (i) When A = 0, and B = 0, both diodes are reverse biased, hence Y = 0. 

    (ii) When A = 0, and B = 1, diode D2 is forward biased, hence Y = 1. 

    (iii) When A = 1, and B = 0, diode D1 is forward biased, hence Y = 1. 

    (iv) When A = 1, and B = 1, diode D1 and D2 both are forward biased, hence Y = 1. 


    Question 642
    CBSEENPH12038813

    Explain, with the help of a circuit diagram, how the thickness of depletion layer in a p-n junction diode changes when it is forward biased. In the following circuits which one of the two diodes is forward biased and which is reverse biased?
    (i)

     

    Solution

    When applied voltage is such that n-side of the diode is connected to the negative terminal of the battery and p-side is connected to positive terminal of the battery, the applied voltage is opposite to the barrier potential. The direction of applied potential is opposite to that of the built-in potential.
    Hence, the effective barrier potential becomes V- V, and the energy barrier across the junction decreases. Thus, the junction width decreases. 


    In the figure given, 

    (i) p-n junction is forward biased.
    (ii) p-n junction is reverse biased. 



    Question 643
    CBSEENPH12038814

    Explain, with the help of a circuit diagram, how the thickness of depletion layer in a p-n junction diode changes when it is forward biased. In the following circuit which one of the two diodes is forward biased and which is reverse biased? 


    Solution

    (i) In this case, the p-side of the diode is at -10 V, whereas the n-side is at 0 V.
    Here, Vp < VN, therefore, the diode is reverse biased. 

    (ii) In this case, the p-side of the diode is at 0 V, whereas the n-side is at -10 V.
    Thus, Vp > VN, hence, the diode is forward biased. 

    When applied voltage is such that n-side is connected to the negative terminal of the battery and p-side is connected to positive terminal, the applied voltage is opposite to the barrier potential. Hence, the effective barrier potential becomes VB-V, and the energy barrier across the junction decreases. Thus, the junction width decreases. 



                           

    Question 644
    CBSEENPH12038815

    Justify the output wave form (Y) of the OR gate for inputs (A) and (B) as given in the following figure:


    Solution
    The output waveform shown is depicted in the form of truth table as follows: 

    Time interval

    Input A

    Input B

    Output, Y = A + B

    t < t1

    0

    0

    0

    t< t < t2

    1

    0

    1

    t2 < t < t3

    1

    1

    1

    t< t < t4

    0

    1

    1

    t< t < t5

    0

    0

    0

    t< t < t6

    1

    0

    1

    t > t 6

    0

    1

    1

    Question 645
    CBSEENPH12038816

    Draw a circuit diagram for use of n-p-n transistor as an amplifier in common emitter configuration. The input resistance of a transistor is 1000 Ω. On changing its base current by 10 μA, the collector current increases by 2 mA. If a load resistance of 5 kΩ is used in the circuit, calculate:
    (i) the current gain,
    (ii) voltage gain of the amplifier. 

    Solution
    Circuit of n-p-n transistor as an amplifier in common emitter configuration is given below: 


    Numerical: 

    Given,

    Change in base current, IB = 10 μAChange in collector current, IC = 2 mALoad resistance, RL = 5   Input resistance, Ri = 1 

    (i) The current  gain is given by,

                    β = ICIBVCE    = 2 × 10-310 × 10-6    = 200

    (ii) Voltage gain is,
                          AV = β×RLRi      = 200 × 51      = 1000. 

    Question 646
    CBSEENPH12038817

    Mention two advantages and disadvantages of semiconductor devices.

    Solution

    Advantages of semiconductor devices: 

    (i) Low cost
    (ii) No noise 

    Disadvantages of semiconductor: 

    (i) Cannot operate at high voltage
    (ii) Cannot operate at high current.

    Question 647
    CBSEENPH12038818
    Question 648
    CBSEENPH12038819

    In a silicon transistor, a change of 7.89 mA in the emitter current produces a change of 7.8 mA in the collector current. What change in the base current is necessary to produce an equivalent change in the collector current?

    Solution
    Given,    
    Change in emitter current, ΔI
    e = 7.89 mA
    Change in collector current, ΔI
    c = 7.8 mA 

    Since,          
    Current gain, αac = IcIe= 7.87.89 = 0.9886 

    and,

    Voltage gain,    βac =α1-α =0.98861-0.9886 = 86.72 

    Also since,       βac = IcIb 

     Change in base current, Ib = Icβac                                                     = 7.886.72                                                     = 89.94 × 10-3mA.

    Question 649
    CBSEENPH12038820

    A change of 8.0 mA in the emitter current brings a change of 7.6 mA in the collector current. How much change in the base current is required to have the same change (= 7.6 mA) in collector current. Find the value of a and β.

    Solution

    Given,  

    Change in emitter current, Ie = 8.0 mAChange in collector current,  Ic = 7.6 mA 

    As, change in emitter current, Ie = Ib+Ic

    This implies, 
    Change in base current, Ib = Ie - Ic
                                               = 8.0-7.6 = 0.4 mA 

     α = IcIe = 7.68.0 = 0.95 and

    β = IcIb = 7.60.4                    

    i.e.,       β = 19.
                            

    Question 650
    CBSEENPH12038821

    For a common base amplifier, if the values of voltage gain and resistance gain are 2800 and 3000 respectively, find the current gain and power gain of this amplifier.

    Solution

    Given, 
    Voltage gain = 2800 
    Resistance  gain = 3000 

    Therefore, 

    Current gain, α  = voltage gainresistance gain

                     α = 28003000 = 0.93

    Power gain = (voltage gain)2resistance gain

                     =  (2800)23000 =  2613.3
                         

    Question 651
    CBSEENPH12038822

    The gain of common-emitter amplifier is given by AV= – gmRL. If RL is increasing indefinitely, will the gain of the amplifier also increase indefinitely? Explain.

    Solution
    Gain of the common-emitter amplifier is given by, 

                                   AV= – gmRL ...... (1)

    No, if the load resistance is increased indefinitely, the output current will become zero. Hence, the voltage gain will be zero. Therefore, there will be 0 gain in the amplifier.

    In equation (1) g
    m is called transconductance and is equal to current gain per unit input resistance.
    Question 652
    CBSEENPH12038823

    In a transistor, connected in a common-emitter mode Rc = 4 kΩ; Ri = 1 kΩ; Ic = 1mA and lb = 20 μA. Find the voltage gain.

    Solution

    Given, a common emitter configuration. 

    Collector resistance, Rc = 4 kΩ 
    Internal resistance, Ri = 1 kΩ 
    Current across collector, Ic = 1 mA
    Current across base, Ib = 20 μA

    Using the formula for current gain,
     
                       β = IcIb     = 10-320 × 10-6     = 50 

    Therefore,
    Voltage gain is, 
                            AV = βRcRi       = 50 × 40001000      = 200.

    Question 653
    CBSEENPH12038824

    In the following figure, circuit symbol of a logic gate and input waveform is shown. (i) Name the logic gate, (ii) write its truth table and (iii) give the output waveform.


    Solution

    (i) The given logic gate is NOT gate. 

    (ii) Truth table of NOT gate.


    Input A

    Output Y¯ = A¯

     0

    1

    1

    0


    (iii) The output waveform of the input is as shown below:

    Question 654
    CBSEENPH12038825

    State the principle of working of p-n diode as a rectifier. Explain, with help of a circuit diagram, the use of p-n diode as a full wave rectifier. Draw a sketch of the input and output waveforms.

    Solution
    Principle of rectifier:

    The rectifier is a device that is capable of converting an alternating current into a unidirectional or pulsating form of direct current.
    The process of conversion of alternating currents into direct currents is known as rectification.

    Circuit diagram for a full wave rectifier: 



    Working of a rectifier


    1. A full wave rectifier uses two diodes and gives the rectified output voltage corresponding to both the positive and negative half-cycle of alternating current. 
    2. The p-side of the two diodes are connected to the ends of the secondary of the transformer and, the n-sides of the diodes are connected together. 
    3. Output is taken from between the common-point of the two diodes and secondary of the transformer. Hence, the secondary of the transformer is provided with center tapping and is also called the centre-tap transformer. 
    4. Let, the input voltage to A with respect to the centre be positive and, at the same instant, voltage at B being out-of-phase will be negative. Therefore, diode D1 is forward biased and starts conducting whereas, D2 being reverse biased does not conduct. 
    5. Thus, we get an output current and a output voltage across the load resistance RL in the first positive half-cycle.
    6. During the course of the negative half - cycle, that is, when voltage at A becomes negative and voltage at B becomes positive, We will have D1 as reverse biased and D2 forward biased.
    7. In the negative part of the cycle, only diode D2 will conduct giving an output current and output voltage across RL
    8. For both positive and negative half cycle we will get the output voltage. This rectified output voltage has the shape of half sinusoids.

    Input and output waveforms:
     
    Question 655
    CBSEENPH12038826

    Explain the function of base region of a transistor. Why is this region made thin and lightly doped?
    Draw a circuit diagram to study the input and output characteristics of n-p-n transistor in a common emitter (CE) configuration. Show these characteristics graphically. Explain how current amplification factor of the transistor is calculated using output characteristics.

    Solution
    The base provides proper interaction between the charge carriers of emitter and collector. The flow of majority charge carriers from emitter to the collector is controlled by the base of a transistor.
    When the emitter is forward biased, electrons and holes recombination process occurs in the base region.
    If the base is thin and lightly doped, it will have a small number density of majority charge carriers. This reduces the rate of electron hole recombination, which is necessary for a transistor action. 

    A circuit for drawing the input and output characteristics of an n-p-n transistor is shown in figure below:



    The corresponding input and output characteristics are also shown graphically: 




    The variation of current on the input side with input voltage (IB versus VBE) is known as input characteristics, while the variation in the output current with output voltage (Icversus VCE) is known as output characteristics.

    Current amplification factor of the transistor (βac- The ratio of change in collector current to the change in base current when, the collector-emitter voltage (VCE) is constant. The transistor is in active state. 

    Therefore, 
                       βac = IcIB 

    As seen in the graph, we can say that, Ic is increasing almost linearly with IB.




    Question 656
    CBSEENPH12038827

    Distinguish between metals, insulators and semiconductors on the basis of their energy bands.

    Solution
    Metals: In metals, either the conduction band is partially filled or valence band is partially empty. Many electrons from below the Fermi level, by acquiring a little more energy from any source, can shift to the higher energy levels above the Fermi level in the conduction band and behave as free electrons. The conduction band and the valence band overlap each other ( there is no forbidden energy gap) in metals. In this situation, large number of electrons are available for electrical conduction, hence the resistance of such a material is low or the conductivity is high. Even if a small electric field is applied across the metal, these free electrons start moving in a direction opposite to the direction of electric field. As a result, current begins to flow through it and hence, metal behaves as a conductor.
    The energy band diagram for metal is shown in fig. (i).


    Insulators: In insulators, the valence band is completely filled, the conduction band is empty and energy gap is quite large (Eg> 3 eV). As a result of huge energy gap, no electron will jump from the valence band to the conduction band even if electric field is applied. The energy band diagram of insulator is shown in figure (ii). 

    Thus, electrical conduction is not possible and hence these materials behave as insulators. eg. diamond ( Eg = 6 eV).

    Semiconductors: In semiconductors, the valence band is completely filled  and conduction band is empty but, energy gap between them is less than 3 eV. The energy band diagram of a semiconductor is shown in figure (c.) 



    At 0 K, conduction band remains totally empty because the electrons in the valence band are not able to get excited to the higher level. However, at room temperature, some electrons in the valence band acquire thermal energy greater than energy band gap and, jump over to the conduction band where they are free to move under the influence of even a small electric field.  As a result of it, the semiconductor acquires small conductivity at room temperature.

    The resistance of semiconductor would not be as high as that of insulator.




    Question 657
    CBSEENPH12038828

    A photodiode is fabricated from a semiconductor with band gap of 2.8 eV. Can it detect a wavelength of 6000 nm? Justify.  

    Solution

    Given, 
    Wavelength, λ = 6000 nm = 6 x 10–6 m
    Energy band gap, Eg = 2.8 eV 

    Using the formula for energy of a photon,

                            E = hcλ    

    we have,    E = 6.6 × 10-34×3×1086×10-6    = 3.3×10-20J 

                 E = 3.3 × 10-201.6×10-19 = 0.206 eV 

    As, the energy of the photon is less than energy band gap (Eg= 2.8 eV) of the semiconductor, so a wavelength of 6000 nm cannot be detected.

    Question 658
    CBSEENPH12038829

    Draw a circuit diagram for a two input OR gate and explain its working with the help of input, output waveforms.

    Solution
    The OR gate can be made with the help of two p-n junction diodes D1 and D2 as given in the circuit below: 
     

    Working: The negative terminal of the battery is gounded and corresponds to the 0 state and the positive (i.e., voltage 5 V in the present case) to the 1 state. 

    Input and output waveform: 



    - When both A and B are connected to 0, no current passes through the diode and therefore no voltage develops across R and the output is zero. 

    - When input A is connected to zero and B to 1, the diode D2 is forward biased and the current through it is limited by a current limiting resistance. This current causes a 5 V drop across the resistance assuming the diode to be ideal and this gives an output of 5 V or 1.

    - Now, interchanging A and B to 1 and 0 will still give a 5 V drop across the resistance as D1 will conduct. 

    - When the terminals A and B are connected to 1, then both the diodes D1 and D2 conduct. However, the voltage drop across R cannot exceed 5 V and the output is 1. 


    Question 659
    CBSEENPH12038830

    For an n-p-n transistor in the common emitter configuration, draw a labelled circuit diagram of an arrangement for measuring the collector current as a function of collector emitter voltage for at least two different values of base current. Draw the shape of the curves obtained. Define the terms:
    (i) ‘output resistance’ and           (ii) ‘current amplification factor’ .

    Solution
    Circuit diagram for drawing characteristics of a common emitter n-p-n transistor is given as follows: 

     

    The output characteristics are drawn by plotting current IC versus collector emitter voltages VCE, keeping the base current Ib constant. 

     

    Output resistance: 

    It is defined as the ratio of the collector emitter voltage (ΔV
    CE) to the corresponding change in collector current (ΔIC) at a constant base current lb.

                      R0 = VCEIcIb = constant 

    Current amplification factor: 

    It is defined as the ratio of the change in collector current to the change in base current. 

                           β = ICEIbVCB = constant
    Question 660
    CBSEENPH12038831

    The current gain for common emitter amplifier is 59. If the emitter current is 6.0 mA,find (i) base current and (ii) collector current.

    Solution

    Given, a common emitter configuration. 
    Current gain, β = 59 
    Emitter current, IE = 6 mA

    Now, using the relation,

                         α = β1+β  

    we have,       α = 5960

    But,              α = ICIE

     Collector current, IC = α.  IE

                    IC = 5960 ×  6mA     = 5.9 mA  

    and, 

    Base current, IB = IE - IC  =  6.0 - 5.9 = 0.1 mA.                

    Question 661
    CBSEENPH12038832

    Distinguish between intrinsic and extrinsic semiconductors.

    Solution
    Intrinsic and extrinsic semiconductors can be differentiated as follows: 

    Intrinsic  Extrinsic
    1. It is a pure semiconductor and no impurities are added to it. 1. It is prepared by doping a small quantity of impurity atoms to the pure semiconducting material.
    2. Number of free electrons in conduction band is equal to the number of holes in valence band. 2. Number of free electrons and holes vary in n-type and p-type semiconductor. There is excess of electrons in n-type and excess of holes in p-type.
    3. It's electrical conductivity is low. 3. Electrical conductivity is high.
    4. Electrical conductivity is solely a function of temperature. 4. Electrical conductivity depends upon temperature as well as on the quantity of dopants.
       




    Question 662
    CBSEENPH12038833

    Using a suitable combination from a NOR, an OR and a NOT gate. Draw circuits to obtain the truth table given below:

    Solution
    (i) Circuit diagram for the given truth table:

     
    Verification: 

     


    (ii) Circuit diagram for given truth table: 


    Verfication:

    A

    B

    Ā

    Y = Ā + B

    0

    0

    1

    1

    0

    1

    1

    1

    1

    0

    0

    0

    1

    1

    0

    1

    Question 663
    CBSEENPH12038834

    What is a p-n junction? How is a p-n junction made?

    Solution
    When a p-type semiconductor crystal and an n-type semiconductor crystal is brought in close contact, the resulting arrangement so formed is p-n junction. 

    Formation of p-n junction: 

    1. Silicon crystals are cut into thin slices of wafer to form an n-type and p-type. 
    2. Now, an aluminium film is placed on a wafer of n-type silicon and, is heated to a high temperature of about ~580o C such that, aluminium diffuses into silicon. 
    3. Hence, as a result of the diffusion a p-type semiconductor is formed on an n-type semiconductor. This formation of p-region on an n-region is called a p-n junction. 
    Question 664
    CBSEENPH12038835

    The given circuit diagram shows a transistor configuration along with its output characteristics. Identify
    (i) the type of transistor used and
    (ii) the transistor configuration employed.

    Using the curve, find the gain at VCE = 3 V 



    Solution

    (i) The transistor used is n-p-n transistor. 

    (ii) The transistor configuration employed is common emitter (CE) configuration.

    Numerical:

    Current amplification factor is given by, 

                               βac = ICIB at vCEβac = ICIB at vCE = 3V

    From the characteristic curve, 

                     βac = (9.5-2.5)mA(60-10)μA 

                              = 7.0 × 10-350-10-6 = 140.

    Question 665
    CBSEENPH12038836

    The ratios of number density of free electron to holes, nenh, for two different materials A and B, are equal to one and less than one respectively. Name the type of semiconductors to which A and B belong. Draw energy level diagram for A and B.

    Solution
    For A :
    ne/nh = 1. 
    This implies, ne = nh
    A is an intrinsic semi-conductor. 

    For B:
    ne/nh < 1. 
    This implies, 
    ne < nh.
    Therefore,
    B is p-type semi-conductor. 


    Question 666
    CBSEENPH12038837

    A Zener diode has a contact potential of 0.8 V in the absence of biasing. It undergoes Zener breakdown for an electric field of 106 Vm–1 at the depletion region of p-n junction. If the width of the depletion region is 2.4 μm, what should be the reverse biased potential for the Zener breakdown to occur?

    Solution

    Here,
    Breakdown electric field of the Zener diode, E = 106Vm–1
    Width of the depletion region, d =2.4 μm= 2.4 x 10–6m


    ∴ Reverse biased potential,  Vbreakdown = E x d

                                                               = 106 x 2.4 x 10–6 
                                                               = 2.4 V.

    Question 667
    CBSEENPH12038838

    From the output characteristics shown in figure calculate the values of current amplification factor of the transistor when VCE is 2V.

    Solution

    Given, 
    VCE = 2 V
    Current amplification factor,  β  = ICIBVCE

    Consider characteristics for any two values of IB (say, 10 and 60 μA).
    Then for V
    CE = 2 V from the graph,

    we have,         
    IB   (60-10) μA = 50 μAIC  (9.5 -2.5) mA = 7.0 mA
                             
    Therefore,          β = 7×10-3A50×10-6A = 140. 

    Question 668
    CBSEENPH12038839

    Calculate the value of V0 and I if the Si diode and the Ge diode conduct at 0.7V and 0.3V respectively, in the circuit given in figure. If now Ge diode connections are reversed, what will be the new values of Vo and I.



    Solution
    As in the given circuit, 

    Voltage, V = 12 V
    Resistance, R = 5 kΩ

    Therefore, 

    Current, I = 12-0.35 k Ω = 11.7V5×103Ω 

                   =2.34 mA 

    Output voltage,  
                         V0 = RI      = (5×103)×(2.34×10-3)      = 11.7 V 

    When the connections of Ge diode are reversed, then current will be through silicon. 

    In this case,

    Current, I = (12-0.7)V5 k Ω  = 11.3V5×10-3Ω = 2.26 mA

    Therefore,

    Output voltage, V0 = IR                                   = (2.26 × 10-3) × (5 × 103)                                   = 11.3 V.
    Question 669
    CBSEENPH12038840

    An a.c. supply of 230 V is applied to a half-wave rectifier circuit through a transformer of turn ratio 10: 1. Find the output d.c. voltage. Assume the diode to be ideal.

    Solution
    Given,

    R.M.S. primary voltage, = 230 V
    Primary to secondary turn ratio, n
    p/ns = 10
    Therefore,
    Maximum primary voltage,

                Vpm = 2×Vrms          = 2 ×230          = 325.3 V

    Maximum secondary voltage, 

                  Vsm = Vpm × nsnp        = 325.3×110         = 32.53V  

    Half-wave rectified current, 

                           Id.c. = I0π 

     Output d.c. voltage = Id.c × RL 

                                     "
    Question 670
    CBSEENPH12038841

    For a CE-transistor amplifier, the audio signal voltage across the collector resistance of 2 k Ω is 2 V. If the current amplification factor of the transistor is 100, calculate (i) input signal voltage
    (ii) base current. Given that the value of the base resistance is 1 kΩ.

    Solution

    (i) Given, 
    Collector resistance, Rc = 2 kΩ
    Audio signal voltage, Vo = 2 V
    Current amplification factor, β = 100

    Now, using the formula,

                           Av = βRCRB                        Av = 100× 20001000                            =200 

    Output voltage, V Av × Vi 

     Vi = V0Av =2200=1100V = 0.01 V   
    is the input signal voltage. 

    (ii) Now, current amplification factor, β = ICIB

     Base current, IB = ICβ = V0Rc×1β 

                                   = 22000 × 100 =1105A = 10-5A 
                      
                          IB = 10×10-6A = 10 μA.
                     

    Question 671
    CBSEENPH12038842

    Show that a bubbled OR gate is equivalent to a NAND gate. Hence prove the identity.

    Solution
    A bubbled OR gate is the combination of two NOT gates and one OR gate. That is, the output of two NOT gates is made as input of OR gate.

    The Boolean expression for output of this gate is 

                         Y = A¯+B¯ =A.B¯ (From De-Morgan’s Theorem).

    This expression represents NAND gate.

    Hence, a bubbled OR gate is equivalent to a NAND gate.

    Question 672
    CBSEENPH12038843

    State the basic electronic circuit involved in the electronic circuit of figure and find the value of the output y. Name the gate formed and set up a truth table for it.


    Solution
    The logic gate shown is a bubbled AND gate.

    It is a combination of two NOT gates and one AND gate, i.e., the output of two NOT gates is applied as the input of AND gate. 

    The Boolean expression for output of this gate is,
                    y = A¯.B¯ = A+B¯        (From De-Morgan's Theorem). 

    This expression represents a NOR gate.

    Hence, a bubbled AND gate is equivalent to a NOR gate.

    Truth table of NOR gate is as shown in the table below: 

     


    Question 673
    CBSEENPH12038844

    In figure, a battery of emf 2V is used. The length of the block is 0.1m and the area is 1 x 10–4m2. If the block is of intrinsic silicon at 300 k, find the electron and hole currents.

    What will be the magnitude of the total current? What will be the magnitude of total current if germanium is used instead of silicon?
    Given-For silicon:
    Mobility of electrons = 0.135 SI units
    Mobility of holes    = 0.048 SI units
    Number density of electrons holes
    = 1.5 x 1016 per unit volume
    For germanium:
    Mobility of electrons = 0.39 SI units
    Mobility of holes = 0.19 SI units
    Number density of electrons holes = 2.4 x 1019 per unit volume

    Solution
    We know,
    Current i due to charge carriers of density 'n' and having charge 'e' through a block of cross-section area A is given by, 

                            i = n A e v                    ...(i)
    where, v is the average drift speed of the charge carriers. 

    The mobility μ of charge carriers is velocity attained per unit external field E. 

     i.e, 
                      μ = vE 

                         v = μE                         ....(ii) 

    The electric field E due to the applied potential V,
                             E = Vl                       ....(iii)

    From equations (i) and (ii) and (iii), we have

                            i = n A  Vl

    Electron current for silicon, 
    E.m.f of the battery = 2 V 
    Length of the bloack = 0.1 m 
    Area of the block, A = 1 x 10–4m2
    Temperature, T = 300 K
    Mobility, μ1 = 0.135
    Number density of elcetrons/holes, n = 1.5 x 1016 per unit volume

    For electron current, i1 = An11Vl 

                                         
    =10-4×1.5×1016×1.6×10-19×0.135×20.1= 6.45 × 10-7A = 0.645 μA 

    Similarly, for holes μ2= 0.048 SI units.

    Therefore, 
    Hole current, i2 = A n22 VI 


                     i2 =10-4×1.5×1016×1.6×10-19×0.048×20.1   =2.304 ×10-7 = 0.2304 μA 

    Thus, total current is, 

                                i = i1+i2
                                   = 0.645+0.2304 = 0.8754 μA

    If germanium is used instead of silicon then,

    Number density, n = 2.4×1019 per unit volume
                              μ1' = mobility of electrons = 0.39 SI units

     Electronic current, i1' 

    = 2.4 × 1019 × 10-4 × 1.6 × 10-19 × 0.39 × 20.1= 2.99×10-3A = 2.99 mA

    The mobility μ2’ of holes in germanium = 0.19 SI units
                            Hole current , i'2 = 1.49 × 10-3A = 1.49 mA 

      The total current i' is 

                           i' = i'1+i'2   = 2.99+1.49    = 4.48 mA.
    Question 674
    CBSEENPH12038845

    Assume that the silicon diode in the following circuit requires a minimum current of 1 mA to be above the knee point (0.7 V) of its I–V characteristics. Also assume that the voltage across the diodes is independent of the current above the knee point.
    (a)    If VB = 5 V, what should be the maximum value of R so that the voltage is above the knee point?
    (b)    If VB = 5 V, what should be the value of R to establish a current of 5mA in the circuit ?
    (c)    What is the power dissipated in the resistance R and in the diode, when a current of 5 mA flows in the circuit at VB = 6 V.
    (d)    If R = 1 kΩ, what is the minimum voltage VB required to keep the diode above the knee point?

    Solution

    (a) Here,
    Minimum current required by the silicon diode = 1mA= 10–3 A. 

    Minimum voltage across the diode is 0.7 V (so that it is above the knee point of the characteristic curve). 

    So, voltage drop across the resistance R = (5 – 0.7) V = 4.3 V.

    The minimum current i = 1 mA .

     Maximum value of resistance, R =vi = 4.310-3Ω =  4.3  

    (b) Current through resistance R = 5 mA = 5 x 10–3 A.

    Voltage drop across R = (5 – 0.7) V = 4.3 V

                  R = 4.35×10-3                      = 0.86 × 10-3Ω = 860 Ω 

    (c) Here, VB = 6 V. 

    Voltage V' across the resistance = 6 – 0.7 = 5.3 V 

    Current, i = 5 mA = 5 x 10–3 A 

    Power dissipated through the resistance R, P = i V’  
                                                                       = 5 x 10–3 x 5.3 W
                                                                       = 26.5 x 10–3 W
                                                                       = 26.5 mW 

    Power dissipated in the diode is P’' = i x 0.7 W
                                                        = 5 x 10–3 x 7 x 10–1 W
                                                        = 3.5 x 10–3 W
                                                        = 3.5 mW

    (d) For keeping diode above the knee point, the minimum current required is 1 mA.

    Voltage drop across R (= 1 kΩ), V= 1 x 103 x 103
                                                         = 1 V 

    Minimum voltage drop across the diode = 0.7 V

    Therefore,
    Minimum voltage required, VB = (1 + 0.7) V = 1.7 V.

    Question 675
    CBSEENPH12038846

    The characteristic curve of a diode is shown in the above figure. Determine the d.c. and a.c. resistance around point.

    Solution

    From the characteristic curve of a diode, we have

    D.C. resistance,
                            rdc = 0.55×10-3 = 100 Ω 

    A.C. resistance,
                            rac = 0.8-0.5(80-20) × 10-3      = 0.360 ×10-3 = 5 Ω

    Question 676
    CBSEENPH12038847

    The following figure shows the V-I characteristics of a semiconductor diode
    (i)   Identify the semiconductor diode used.
    (ii) Draw the circuit diagram to obtain the given characteristic of this device.


    iii) How the characteristic of zener diode can be used as a voltage regulator? 

    Solution

    (i) The semiconductor diode whose V-I characteristic is shown in the figure is Zener diode.

    (ii) Circuit diagram to obtain the given characteristic is shown in Fig. 



    (iii) The circuit of Zener diode used as voltage regulator is shown in Fig. 



    The voltage to be regulated is applied across Zener diode. When input voltage increases, the current in Zener diode circuit  also increases. As a result, voltage drop across series resistance Rs increases but, voltage drop across RL remain same. That is, the voltage drop across Zener diode remains the same.
    Similarly, when voltage decreases, current in the zener diode circuit decreases and voltage drop across series R
    s resistance decreases but, across the load resistance remains the same. This is how, voltage is regulated using a zener diode. 

    Question 677
    CBSEENPH12038848

    Identify the gate equivalent to the ‘dotted box’ shown here and give its symbol and truth table.

    The inputs A and B shown here, are used as the two inputs in this set up. Give the shape of the output Y obtained from these inputs.


    Solution
    The truth table of the given gates combination is: 



    The combination of gates is equivalent to the AND gate.

    Output waveform is as shown in figure below: 


    Question 678
    CBSEENPH12038849

    The black box, shown here, converts the input voltage waveform into the output voltage waveform as is shown in the figure.

    Draw the circuit diagram of the circuit present in the black box.

    Solution
    Circuit diagram present in black box is drawn in Fig.
    The black box shown here is full wave rectifier. 

    Circuit diagram for full wave rectifier is: 



    The input and output waveform diagram is shown in the figure below:



    Question 694
    CBSEENPH12038865

    Deduce an expression for the conductivity of a p-type semiconductor.

     

    Solution

    Consider a block of semiconductor of length l and area of cross-section A, having electron density nand hole density nh. Let, V be the the potential difference applied across the ends of the semiconductor. The magnitude of the applied electric field is given by,

                               E = Vl         ....... ( 1)

    Due to the applied electric field, both electrons and holes move in a mutually opposite direction with drift velocities ve and vh and contribute current Ie and Ih

     Total current, I = Ie + Ih 
    Electrons and holes in the conduction band and valence band respectivel are moving in a random fashion. Therefore, 
                          Ie = ne A e ve 
                          Ih = nh A e vh 

    Thus, 
    Total current, I = ne A e ve + nh A e vh 

                           = eA (neve + nh vh)
                 IA = e (neve + nh vh)        ... (2) 

    Let R be the resistance of the semiconductor and ρ is it's resistivity. 

    Then, 
                            ρ= RAl                     ... (3) 

    Now, dividing 1 by 3, we get 

                       Eρ = VRA= IA                ...(4) 

    Therefore, from (2) and (4), we get

                   Eρ = e (neve + nh vh)

    Now, mobility of electrons is defined as the drift velocity per unit electric field. Drift velocity is zero when, no electric field is applied. 

     mobility of electrons, μe = veE 

                                    νe = μe E 
    Similarly, 
                                        νh = μh E

                      Eρ = e[ne.μe + nhμh]E
     
                     1ρ =  e[ne.μe + nhμh] 

    We know, electrical conductivity is the reciprocal of resistivity. 

    So, electrical conductivity, 

                     σ = 1ρ =  e[ne.μe + nhμh] 

    For a p-type semiconductor, 
    nh >> ne  and nh = Nwhere, NA is the number density of acceptor atoms. 

    Hence, conductivity of a p-type semiconductor is given by, 
                             σp = e NA μh 
    is the required result. 

    Question 695
    CBSEENPH12038866

    How does the energy gap in an intrinsic semiconductor vary when doped with a potential impurity?

    Solution

    The gap which is seperationg the valence band and the conduction band is known as fermi level.

    When an intrinsic semiconductor is doped with impurity it becomes an extrinsic semiconductor.

    Now, the fermi level will have to move away from it's mid-gap position inorder to conserve the number of particles as well as to maintain the electrical charge neutrality.

    In an n-type semiconductor, energy gap decreases. Fermi-level shifts towards the conduction bandwhere, higher number of electrons are available for conduction. In a p-type semiconductor, energy band increases. Fermi levels shifts closer to the valence band because, holes are the majority carriers.

    Question 696
    CBSEENPH12038867

    Draw the circuit diagram of a common emitter amplifier with appropriate biasing. What is the phase difference between the input and output signals? State two reasons why a common emitter amplifier is preferred to a common base amplifier. 

    Solution

    The circuit diagram of a common-emitter amplifier is given below: 

     

    In a CE amplifier, the phase difference between the input and output signals is 180o

    Common emitter amplifier is preferred over common base amplifier because the current gain in CE amplifier is very high. 

    In CB amplifier the current gain is less than 1. 

    Question 697
    CBSEENPH12038868

    A semiconductor has equal electron and hole concentration of 2 x 108/m3. On doping with a certain impurity, the hole concentration increases to 4 x 1010/m3.
    (i) What type of semiconductor is obtained on doping?
    (ii) Calculate the new electron concentration of the semiconductor.
    (iii) How does the energy gap vary with doping?

    Solution
    Given, 
    Intrinsic concentration, ni = 2 x 108/m3
    After doping, 
    Hole concentration, nh = 4 x 1010/m3

    i) Since there is an increase in hole current, the semiconductor formed is p-type. 

    ii) We know that, 
                                ni2 = ne.n

                      ne = ni2nh = (2×108)24×1010 

                  ne = 10m-3 is the new electronic concentration. 

    iii) Energy gap decreases with doping because an acceptor levels gets created between valence band and conduction band.

    Question 698
    CBSEENPH12038869

    Which of the following frequencies will be suitable for beyond-the-horizon communication using sky waves?
    • 10 kHZ

    • 10 MHz

    • 1 GHz

    • 1000 GHz

    Solution

    A.

    10 kHZ

    10 kHz cannot be radiated because the size of antenna is large. 1 GHz and 1000 GHz will penetrate.
    Question 699
    CBSEENPH12038870

    Frequencies in the UHF range normally propagate by means of
    • Ground waves.
    • Sky waves.
    • Surface waves.
    • Space waves.

    Solution

    D.

    Space waves.Reason: Propagation of waves in ultra high frequency range 0.3 - 3 GHz is possible by space waves. Because these waves can reflect from ionosphere.
    Question 701
    CBSEENPH12038872

    Is it necessary for a transmitting antenna to be at the same height as that of the receiving antenna for line-of-sight communication? A TV transmitting antenna is 81 m tall. How much service area can it cover if the receiving antenna is at the ground level?

    Solution
    No. For line of sight communication, the transmitting antenna do not necessarily be of the same height as that of the receiving antenna. 

                      dT2 = (R+h)2-R2      = R21+hR2-1      = R21+2hR-1      =R2.2hRdT2 = 2h . R 
    where dT is the distance to the horizon, 
    R is the radius of the earth, and 
    hT is the height of the transmitting antenna. 


                        

    Height of the antenna, h = 81 m 

    ∴   Service area will be, 

                 A = π(dT)2    = 227×(2hR)    = 227×2×81×6.4×106     = 3258 km2.

     
    Question 702
    CBSEENPH12038873

    A carrier wave of peak voltage 12V is used to transmit a message signal. What should be the peak voltage of the modulating signal in order to have a modulation index of 75%?

    Solution
    Peak voltage, Ac = 12 V 

    Modulation index = 75 % = 0.75  
     
                       μ = 0.75 = AmAc 

    Hence,       Am = 0.75 Ac 

         Am = 0.75 × 12 V = 9 V is the peak voltage. 
    Question 703
    CBSEENPH12038874

    A modulating signal is a square wave as shown in Fig. 

     

    The carrier wave is given by c(t) = 2 sin ( 8 πt) volt.

    (i) Sketch the amplitude modulated waveform:
    (ii) What is the modulation index?


    Solution

    (i) The amplitude modulated waveform is given by superimposition of modulating signal on carrier wave and is shown below : 


    (ii) We have, 

    Am = 1 V , Ac = 2V .

    Therefore, modulation index is given by, 

                   μ = AmAC = 12 = 0.5 

    Question 704
    CBSEENPH12038875

    For an amplitude modulated wave, the maximum amplitude is found to be 10 V while the minimum amplitude is found to be 2 V. Determine the modulation index, μ.
    What would be the value of μ if the minimum amplitude is zero volt?

    Solution

    The AM wave is given by (Ac + Am sin ωmt) cos ωct where, 
    Ac is the amplitude of carrier wave and, 
    Am is the amplitude of message signal wave.

    The maximum amplitude is M1 = Ac + Am = 10 V
    while,
    Minimum amplitude is M
    2 = Ac - Am = 2 V

    Hence, the modulation index is, 

                         μ = AmAc    = M1-M2M1+M2    = 812    = 23. 

    When the minimum aplitude is M2 = 0. Then, we have clearly μ = 1, irrespective of M1.

    Question 705
    CBSEENPH12038876

    For an amplitude modulated wave, the maximum amplitude is found to be 10 V while the minimum amplitude is found to be 2 V. Determine the modulation index, μ. What would be the value of μ if the minimum amplitude is zero volt?

    Solution
    Let, Aand Am be the amplitude of carrier wave and message signal wave. 

    Given, 

    Amax = Ac + Am = 10 V
    Amin = AC - Am = 2V

    On solving the above equations, we get

    AC = 6V ; Am = 4V 

    Amax = 6+4 = 10 V
    Amin = 6-4 = 2 V

    The maximum amplitude is M
    1 = Ac + Am while the minimum amplitude is M2 = Ac - Am.

    Hence, the modulation index is 

    μ = AmAc = M1-M2M1+M2 = 812 = 23. 

    With M2 = 0, clearly, μ = 1, irrespective of M1.
    Question 706
    CBSEENPH12038877

    Due to economic reasons, only the upper sideband of an AM wave is transmitted, but at the receiving station, there is a facility for generating the carrier. Show that if a device is available which can multiply two signals, then it is possible to recover the modulating signal at the receiver station.

    Solution

    The received signal is given by,

                 A1 cos (ωc + ωm) t 

    Carrier signal is given by, 

                     Ac cos ωc t 

    where, 
    ωc and ωm are the angular frequency of the carrier wave and message signal wave. 

    The carrier Ac cos ωct is available at the receiving station.

    On multiplying the two signals, we get

         A1 Ac cos (ωc + ωm) t cos ωct

    = A1Ac2[2 cos (ωc + ωm) t.  cos ωct]

    = A1 Ac2[cos (2 ωc + ωm) t + cos ωmt] 

    If this signal is passed through a low-pass filter, it will pass through the high frequency signals and block the low frequency signals.

    Thus, modulating signal, is given by A1 Ac2cos ωmt. 
    of a single frequency ωm .

    Question 707
    CBSEENPH12038878

    What is space wave propagation?

    Solution
    The mode of wave propagation in which the radio waves emitted from the transmitter antenna reach the receiving antenna through space in a straight line is known as space wave propagation. Space waves are the radio waves of frequency-range from 54 MHz to 4.2 GHz. 
    Space wave propagation is used in line of sight communication and satelite communication.
    Question 708
    CBSEENPH12038879

    What is sky wave propagation?

    Solution
    Sky wave propagation is a mode of wave propagation in which the radiowaves emitted from the transmitter antenna reach the receiving antenna after reflection by the ionosphere.

    In sky wave propagation, the frequency of radio waves range from 1710 kHz to 40 MHz. 

    This mode of propagation is uded by short wave broadcast service. 


    Question 709
    CBSEENPH12038880

    What is the meaning of the term 'attenuation' in communication system?

    Solution
    Attenuation is refererred to as the reduction in the strength of a signal while propagating through a medium. Attenuation is possible for both digital and analog signals as a result of long distance transmission.
    Question 710
    CBSEENPH12038881

    What are the three basic units of a communication system?  

    Solution

    The three basic units of communication system are:

    (i) Transmitter: It convert the message signal produced by the source of information into a form suitable for transmission.

    (ii) Communication channel: The signal is passed through the channel for fulther processing of the information. 

    (iii) Receiver: It operates on the received signal in such a way that it is recognisable by the user of information. 

    Question 711
    CBSEENPH12038882

    Why are short waves used in long distance broadcasts?

    Solution
    Short waves can be reflected from the ionosphere and hence, can travel a longer distances from transmitter to receiver. Wavelength of short waves is approximately less than 200 m. 
    Question 712
    CBSEENPH12038883

    What is the purpose of modulating a signal in transmission? 

    Solution

    Modulation is necessary for: 

    i) transmitting a low frequency signal to a distant place. 

    ii) avoiding mixing up of signals from different transmitters. 

    iii) so as to keep the height of antenna small.

    iv) Modulation helps us to filter out the unwanted noises present in the signal and process out a more clearer form of information.

    Question 713
    CBSEENPH12038884

    What is the length of the dipole antenna to transmit signals of frequency 200 MHz?

    Solution
    The formula for
    Length of dipole antenna = λ2 

    Frequency of signal, ν = 200 MHz

    Therefore,

    Length of dipole antenna= c2v                                              = 3×1082×200×106                                              = 0.75 m.
    Question 714
    CBSEENPH12038885

    State two factors by which the range of transmission of signals by a TV tower can be increased?

    Solution

    The range of transmission of signals by a TV tower can be increased by the following ways:

    (i) By increasing the height of the transmission tower. 

    (ii) By increasing the height of the receiving antenna, so that it may directly intercept the signal from the transmitting antenna.

    Question 715
    CBSEENPH12038886

    Name the type of communication system according to the mode of communication.

    Solution
    According to the mode, communication can be classifies as:

    i) Analog communication and
    ii) Digital communication.
    Question 716
    CBSEENPH12038887

    What should be the length of the dipole antenna for a carrier wave of frequency 3 × 108 Hz?

    Solution

    Frequency of the carrier wave, ν = 3 × 108 Hz 

     Wavelength, λ = cv = 3×1083×108 = 1m 

    The size of the antenna should be 14 of the wavelength in case of a dipole antenna. 

    i.e., Length of the antenna = 14 m

    Question 717
    CBSEENPH12038888

    It is necessary to use satellites for long distance TV transmission. Why?

    Solution
    Television signals are not reflected by ionosphere. Therefore, we use artificial satellite so that, the signals can be reflected to earth without any sort of interruption or bending.


    Question 718
    CBSEENPH12038889

    Name the device which can represent digital data by analog signals and vice-versa.

    Solution
    Modem can represent digital data by analog signals and vice-versa. 
    Question 719
    CBSEENPH12038890

    How does the effective power radiated by an antenna vary with wavelength?

    Solution
    Effective power radiated by an antenna is inversely proportional to the square of the wavelength. 
    Question 720
    CBSEENPH12038891

    Name an appropriate communication channel needed to send a signal of bandwidth 100 kHz over a distance of 8 km. 

    Solution
    Space wave with the use of line-of-sight method can transmit a signal of bandwidth 100 kHz. 
    Question 721
    CBSEENPH12038892

    Why is ground wave transmission of signals restricted to a frequency of 1500 kHz?

    Solution
    In ground wave propagation, as the frequency increases, there is  loss of energy in the signal due to interaction with matter. Frequencies above 1500 kHz get heavily interrupted and damaged. So ground wave propagation is restricted to a frequency less than 1500 kHz.
    Question 722
    CBSEENPH12038893

    Name the type of modulation scheme preferred for digital communication.

    Solution
    Pulse code modulation (PCM) is preferred for digital modulation. PCM represents the sampled analog signals in a digitalized manner.
    Question 723
    CBSEENPH12038894

    Name the factors which decides the quality of reproduced document sent by Fax. 

    Solution
    The quality of reproduced document sent by fax, depends on the quality of the optical scanning of the original document. 


    Question 724
    CBSEENPH12038895

    Name the process of superimposing signal frequency (i.e., audio wave) on the carrier wave.

    Solution
    Modulation is the process by which the signal frequency is superimposed on the carrier wave and a resultant modulated wave is obtained. 
    Question 725
    CBSEENPH12038896

    An antenna behaves as resonant circuit only when its length is:

    Solution
    Antenna behaves as a resonant circuit when its

    length is λ2 or integral multiple of λ2.
    Question 726
    CBSEENPH12038897

    What type of modulation is employed in India for radio transmission?

    Solution
    For radio transmission we use amplitude modulation.
    Question 727
    CBSEENPH12038898

    Write any two advantages of optical fibre.

    Solution

    Two advantages of optical fibre: 

    (i)  High bandwidth.
    (ii) High data transmission capacity.

    Question 728
    CBSEENPH12038899

    What is meant by 'bandwidth'?

    Solution
    The range of frequencies over which the transmission of information operates is known as the bandwidth of transmission.
    Question 729
    CBSEENPH12038900

    What is meant by deviation in frequency of FM wave?

    Solution

    For frequency modulation, deviation in frequency is given by,
                                  δ= v - vc
    where, vc is constant frequency of carrier wave and v is instantaneous frequency of the FM wave at any time t.

    Question 730
    CBSEENPH12038901

    Write the function of (i) Transducer and (ii) Repeater in the context of communication system.

    Solution

    (i) Transducer: It is a device which converts one form of energy into another. It converts physical variable like pressure, displacement, force, temperature etc. into it's corresponding electrical signal at it's output. 

    (ii) Repeater: A repeater is a combination of receiver and transmitter placed along the path of signal so as to extend the range of the communication system. Repeater picks up the signal from transmitter, amplifies it and re-transmits it to the receiver with a change in carrier frequency sometimes. 

    Question 731
    CBSEENPH12038902

    What does the term 'LOS communication' mean? Name the types of waves that are used for this communication. Give typical examples, with the help of suitable figure, of communication systems that use space wave mode propagation.  

    Solution

    Mode of radio wave propagation by space waves, in which the wave travels in a straight line from transmitting antenna to the receiving antenna, is called line-of-sight (LOS) communication.

    Two types of waves used for LOS communication are space wave and ground wave.

    At frequencies above 40 MHz, LOS communication is essentially limited to line-of-sight paths.

    The diagram below shows various communication systems that use space wave mode of propagation.


    Question 732
    CBSEENPH12038903

    Why are high frequency carrier waves used for transmission?

    Solution
    High frequency carrier ( HFC) waves travel through space or medium with a speed approximately equal to the speed of light and are not obstructed by the earth's atmosphere. Hence, HFC is used for transmission purposes.
    Question 733
    CBSEENPH12038904

    Draw a block diagram of a detector for an amplitude modulated signal explaining briefly the function of each of its components.  

    Solution



    (i) AM Detector: The modulated wave is fed into a circuit for demodulation purpose. This circuit is called detector. 

    (ii) Envelope Detector: A diode followed by a suitable filter circuit is used for the detection of AM waves. The half wave rectification is done by the diode. 

    After these steps the desired original modulating signal is displayed at the output. 

    Question 734
    CBSEENPH12038905

    Distinguish between frequency modulation and amplitude modulation. Why is an FM signal less susceptible to noise than AM signal?  

    Solution

    Amplitude modulation:
    - The modulation technique is comparitively simple  and instruments are cheap.
    - The modulated signal's amplitude varies as per the modulating signal.

    Frequency modulation:
    - Modulation instruments and techniques are more costly and complex than AM.
    - The modulated signal's frequency varies as per the modulating signal.
    - It is less noisy and gives better quality transmission and has a larger bandwidth.

    The noise in any signal is related to the amplitude variation of the signal emitted by a source. In FM, only frequency changes and amplitude remains constant. Therefore, FM signal is less susceptible to noise than an AM signal. 

    Question 735
    CBSEENPH12038906

    Explain, why high frequency carrier waves are needed for effective transmission of signals.
    A message signal of 12 kHz and peak voltage 20 V is used to modulate a carrier wave of frequency 12 MHz and peak voltage 30 V. Calculate the (i) modulation index and (ii) side-band frequencies.

    Solution
    High frequency carrier waves travel fast, approximately with the speed of light and are not interrupted by earth's atmosphere or surface. Hence, high frequency waves are used for transmission.

    Numerical:    

    Here, 

    Frequency of message signal, vm = 12 kHzPeak voltage, Em = 20 V

    Frequency of carrier wave, vc = 12 MHz = 12000 kHZPeak voltage of carrier wave, Ec = 30 V

    (i) Modulation index, μa = EmEC = 2030 = 0.67 

    (ii) The side-bands frequencies are:

    USB =  vc+vm = 12000+12 = 12012 kHz

    LSB =   vc-vm = 12000-12 = 11988 kHz
    Question 736
    CBSEENPH12038907

    What is an optical detector? State its three essential characteristics. Name the factor which decides how good a detector is.

    Solution

    Optical detector is a device at the receiver end, which converts light into electrical signal so that the transmitted information may be decoded.

    Characteristics of optical detector:
    - Size is compatible with that of the optical fibre.

    - High sensitivity at the desired optical wave-length. 

    - High response time for fast-speed data transmission/reception. 

    The efficiency of generating electron-hole pairs in a photodiode decides the quality of detector.

    Question 737
    CBSEENPH12038908

    A TV tower has a height of 400 m at a given place. Calculate as coverage range, if the radius of the earth is 6400 km.

    Solution
    Given, 
    Height of tv tower, h = 400 m
    Radius of the earth, R = 6400 km

    Coverage range is given by,

    d = 2hR =2×400×6400×1000                     = 71.554 × 103m                     = 71.554 km. 
    Question 738
    CBSEENPH12038909

    What are the different parameters or characteristics of a carrier wave which are varied in accordance with the modulating or message signal?

    Solution

    The parameters of carrier wave that vary in accordance with the modulating or message signal, in case of a sinusoidal wave are:

    (a) Amplitude
    (b) Frequency
    (c) Phase.

    And, in the case of pulsed wave the parameters varying are:

    (a) Amplitude of pulse
    (b) Width of pulse
    (c) Position of pulse.


    Question 739
    CBSEENPH12038910

    Why communication at frequencies above 20 MHz is generally carried out with the help of satellites?

    Solution

    Frequency above 20 MHz is carried out with the help of satellites because

    a) Higher frequencies being greater than critical frequency cannot be reflected by the ionosphere.

    (b) The co-axial cables and wires are extremely radiating in nature at this high frequency which causes disruption in transmission.

    Question 740
    CBSEENPH12038911

    Communication in UHF/VHF regions can be established by space or tropospheric wave. Why is it restricted to or limited to line-of-sight distance of about 40 km?

    Solution
    For a range of 40 km, the height of the antenna is given by, 
                                     d = 2rh                                  h = d22r                                      = (40000)22×6.4×106                                      = 125 m 

    The height of the antenna comes out to be 125 m for a range of 40 km. It is not practically possible to increase the height of the antenna greater than this value. 
    Question 741
    CBSEENPH12038912

    A ground receiver station is receiving a signal at (a) 5 MHz and (b) 100 MHz, transmitted from a ground transmitter at a height of 300 m located at a distance of 100 km. Identify whether it is coming via space wave or sky wave propagation or satellite transponder.
    (Given the value of radius of the earth is 6400 km and maximum electron density, Nmax = 1012 m-3).   

    Solution

    Given, 
    Height of the ground transmitter = 300 m 
    Range of transmission = 100 km

    Maximum distance covered by space wave propagation is, 

                          d = 2Rh     = 2×6.4×106×300     = 62 km 


    As receiver-transmitter distance is 100 km, so space wave propagation is not possible for both 5 MHz and 100 MHz waves. 

    Critical frequency for ionospheric propagation is, 

                 fc = 9 (Nmax)1/2     = 9(1012)1/2 

                    = 9×106 = 9 MHz 

    As frequency (5 MHz) of signal is less than the critical frequency, hence, this signal comes via ionospheric mode while signal of frequency 100 MHz is transmitted through the satellite mode.

    Question 742
    CBSEENPH12038913

    Define term modulation. Name three types of modulation used for a message signal using a sinusoidal continuous carrier wave. State briefly the meaning of any one of these. 

    Solution
    The process where we superimpose a low audio frequency message or information signals called modulating signals onto a high frequency wave called the carrier wave is known as modulation. The resultant signal wave so obtained is known as the modulated wave. 

    The three types of modulation are:
    1. Amplitude modulation (AM), 
    2. Frequency modulation (FM), and
    3. Phase modulation. 

    Amplitude modulation: In amplitude modulation, the amplitude of the carrier wave varies in accordance with the amplitude of the audio frequency modulating signal. 
    Question 743
    CBSEENPH12038914

    A TV tower has a height of 100 m, how much population will be covered by the TV broadcast if the average population density around the tower is 10000 per km2

    Solution
    Given, 
    Height of TV tower, h = 100 m 
    Average population density around the TV tower = 10000 per km2. 

    Now, range is given by, 

                        d = 2rh    =2×6.4×106×100    = 3.6×104m 

    Area = πd2           = 227×3.6 × 1062          = 4.1 × 1013m2 

    Population of the area covered is = 4.1 × 107 km2 × 10000 per km2 = 4.1 × 1011.
    Question 744
    CBSEENPH12038915

    A photodetector is made from a semiconductor having Eg = 0.73 eV. What is the maximum wavelength which it can detect? 

    Solution

    Given, Eg = 0.73 eV 

    Energy of a photon is given by,  Eg = hcλ 

    Therefore,

     Wavelength, λ = hcEg                           = 6.63×10-34×3×1080.73×1.6×10-19                            = 1703 ×10-9m                             = 1703 nm.

    Question 745
    CBSEENPH12038916

    A radio can tune to any station in the 7.5 MHz to 12 MHz band. What is the corresponding wavelength band?

    Solution
    Given, frequency bands are 7.5 MHz and 12 MHz.

    Wavelength, λ1 = 3×1087.5×106 = 40 mWavelength, λ2 = 3×10812×106 = 25 m 

    The corresponding wavelength band is 40 m - 25 m.
    Question 746
    CBSEENPH12038917

    The maximum peak to peak voltage of an AM wave is 26 mV and minimum peak to peak voltage is 4 mV. Find modulation index.


    Solution
    Maximum voltage of AM wave = 26 mV 
    Minimum peak to peak voltage = 4 mV
     
    Therefore, 

    Maximum voltage of AM wave, 

    Vmax = 262mV = 13 mV 

    Minimum voltage of Am wave, 

    Vmin = 42mV = 2 mV

           Modulation index,  m = Vmax-VminVmax+Vmin                                                 = 13-213+2                                                 =1115                                                =0.73.
    Question 747
    CBSEENPH12038918

    What is the total modulation index when a carrier wave is modulated by three sine waves for which modulation μ1 = 0.41, μ2 = 0.51 and μ3 = 0.45 respectively?

    Solution

    Given, 
    modulation index, μ1 = 0.41, μ2 = 0.51 and μ3 = 0.45

    Total modulation index , μ = μ12+μ22+μ321/2

     
            μ = [(0.4)2+(0.51)2+(0.45)2]1/2    = 0.79

    Question 748
    CBSEENPH12038919

    A signal wave of frequency 11.5 kHz is modulated with a carrier wave of frequency 3.45 MHz. What are the deviation in frequency of FM wave and bandwidth of it?

    Solution

    Given,
    Frequency of signal wave, νs = 11.5 kHz 

    Frequency of carrier wave, νc = 3.45 MHz = 3450 kHz 

    Therefore, 

    v =Deviation in frequency = vc-vs

          =3450-11.5 = 3438.5 KHz

    bandwidth = 2 vs                     =  2 ×11.5                      = 23.0 KHz

    Question 749
    CBSEENPH12038920

    What is meant by selectivity and sensitivity of radio receiver?

    Solution

    The ability of a radio receiver to reject the unwanted noises and receive the desired signals is known as selectivity. 

    The ability of a receiver to amplify the desired weak signal is known as sensitivity.

    Question 750
    CBSEENPH12038921

    A TV tower has a height of 150 m. By how much the height of tower be increased to double its coverage range?

    Solution

    Height of tv tower, h = 150 m 

     Range, d' = 2 d = 2Rh'           d = 2Rh

    Height of the tower, h' = 4 h  = 4 × 150 m = 600 m 

     Increase in height of tower = 600 - 150 = 450 m.

    Question 751
    CBSEENPH12038922

    You are given three semiconductors —A, B and C with respective bandgaps of 3 eV, 2 eV and 1 eV for use in a photodetector to detect λ = 1400 nm. Select the suitable semiconductor. Give reasons.

    Solution
    Given that, 
    Energy band gap of semiconductors are 3 eV, 2 eV and 1 eV respectively. 
    Wavelength, λ = 1400 nm

    Energy of the photon, E= hcλ 

                                         = 6.63×10-34×3×1081400×10-9J= 6.63 × 10-34×3×1081400×10-9×1.6×10-19eV= 0.89 eV 


    Eg has to be less than hv or hcλ. 

    None of the semiconductor is suitable since Eg for 1400 nm is 0.89 eV which is less than the band gap Eg of the given semiconductors.
    Question 752
    CBSEENPH12038923

    An AM transmitter records an antenna current of 10.5 A. The antenna current drops to 10 A when only carrier is transmitted. What is the percentage modulation?

    Solution

    Given, 

    Antenna current, It = 10.5 A   Antenna current when only carrier is transmitted, Ic = 10 A


    We have,
                    1+μ22 =ItIc = 10.510 = 2120

                    1+μ22 = 441400 = 1+41400

                               μ2 = 82400      = 0.205 μ   = .205     = 0.456     = 45.3%.  

    is the required percentage modulation.
     

    Question 753
    CBSEENPH12038924

    A block diagram of a receiver is as shown

    Identify X and Y State their function.

    Solution
    X is the intermediate frequency(IF) stage.
    Y is amplifier. 

    Function:

    Intermediate frequency stage is to change carrier frequency to a (standard) lower frequency function.

    The detected signal is not strong enough to be bought in use and hence is fed into the amplifier to further amplify the signal. 
    Question 754
    CBSEENPH12038925

    Give reasons for the following:
    For ground wave transmission, size of antenna (I) should be comparable to wavelength of signal i.e., λ/4.

    Solution
    In ground wave transmission, the time variation of the signal can be properly sensed by the antenna only if, the size of the antenna is comparable to the wavelength of the signal. 
    Question 755
    CBSEENPH12038926

    Give reasons for the following:
    Audio signals, converted into an em wave, are not directly transmitted as such.

    Solution
    An electromagnetic wave, of audio signal frequency, will have a very high wavelength. It would therefore, need an antenna, whose size is practically unattainable. Thus, these signals are not transmitted diractly as such. 
    Question 756
    CBSEENPH12038927

    Give reasons for the following:
    The amplitude of modulating signal is kept less than the amplitude of carrier wave.

    Solution
    Comparable amplitude of both modulating signal and carrier wave causes distortion of signal and, hence, the amplitude of modulating signal is kept less than that of the carrier wave. 
    Question 757
    CBSEENPH12038928

    State various modes of propagation of electromagnetic waves. Explain briefly using a proper diagram, the mode of propagation used is the frequency range from a few MHz up to 40 MHz.

    Solution

    Electromagnetic waves are propagated through the following modes:
    (i) ground wave propagation
    (ii) sky wave propagation, and
    (iii) space wave propagation. 

    For transmission of signal having frequency range from a few MHz up to 40 MHz, sky wave propagation mode is used. 

    Sky wave propagation:

    The mode of wave propagation in which the radiowaves emitted from the transmitter antenna reach the receiving antenna after reflection by the ionosphere. 




    Question 760
    CBSEENPH12038931

    Complete the following block diagram depicting the essential elements of a basic communication system.



    Name the two basic modes of communication. Which of these modes is used for telephonic communication?

    Solution
    The block diagram is given below:



    The two basic modes of transmission are:

    (i) Point to point: Communication takes place over a link between a single transmitter and receiver.
    (ii) Broadcast mode: Transmission of signals take place over a large number of receivers corresponding to a single transmitter. 

    For telephonic conversation, point to point mode of communication is used. 
    Question 761
    CBSEENPH12038932

    Is it necessary for the transmitting antenna and receiving antenna to be of the same height for line of sight communication? Find an expression for maximum line of sight distance dM between these two antennas of heights hT and hR.

    Solution
    No. It is not necessary that the transmitting antenna and receiving antenna should be of the same height. 

     

    For transmitting antenna of height ht, we have 

                          (ht+Re)2 = x2+Re2 

                              ht <<Re 

    where, ht is the height of the transmitting antenna and
    Re is the radius of the earth. 

                              x = dt 

    This implies,
                       (ht+Re)2 = dt2+Re2

                                    =dt2+Re2                (ht2 is negligible)
                            dt = 2Reht 


    where, dt is called the radio horizon of the transmitting antenna. 

    The maximum line of sight distance dx between the two antennas is given by, 

                 dm = 2Reht+2RehR 

    where hR is the height of receiving antenna.

                                                          
    Question 764
    CBSEENPH12038935
    Question 773
    CBSEENPH12038944
    Question 775
    CBSEENPH12038946
    Question 778
    CBSEENPH12038949

    What is 'amplitude modulation'? Represent the process graphically. Write the limitation of amplitude modulation. 

    Solution

    In amplitude modulation, the amplitude of the carrier wave is varied in accordance with the amplitude of the audio frequency modulating signal.
    In this case, the frequency of the amplitude modulated wave remains the same as that of the carrier wave. 




    Limitation of amplitude modulation:

    1. The amplitude of modulated signal obtaind can be transmitted only by amplifying it first and then fed to an antenna of appropriate size for radiation. 
    The size of the antenna matters. 

    Question 779
    CBSEENPH12038950

    A message signal has a bandwidth of 5 MHz, suggest a possible communication channel for its transmission.

    Solution

    The best mode of communication channel in this case is a twisted pair cable. 

    Twisted pair cables consists of pairs of plastic-coated copper wires that are twisted together.

    Question 780
    CBSEENPH12038951

    By what percentage will the transmission range of a T.V. tower be affected when the height of the tower is increased by 21%?

    Solution

    Range is given by, 
    dT = 2RhT Let the transmission of the tower before transmission be dT1 Range after increase in height is given by, dT2 Ratio of their range is given by, dT1dT2 = 2RhT22RhT1 = hT2hT1 

    Given that height increase = 21%

    Thus, 121100hT1 = hT2dT2dT1 = 121hT1100 hT2  dT2 : dT1 = 11: 10 Percentage increase in height is given by, dT2 - dT1dT1×100 = 11-1010×100                                 = 10%

    Question 781
    CBSEENPH12038952

    What is ground propagation?

    Solution
    Ground or surface wave propagation is in which the ground has a strong influence on the propagation of signal waves from the transmitting antenna to receiving antenna. The signal wave glides over the surface of the earth in this mode of propagation. 
    Question 782
    CBSEENPH12038953

    What is space wave propagation?

    Solution
    Space wave propagation is that mode of propagation where the radiowaves emitted from the transmitter antenna reach the receiving antenna through space. These radiowaves are called space waves.

    Spacewaves are the radiowaves of frequency range from 54 MHz to 4.2 GHz. 

    Space waves travel in a straight line from the transmitting antena to the receiving antenna. 
    Question 783
    CBSEENPH12038954

    A small bulb is placed at the bottom of a tank containing water to a depth of 80cm. What is the area of the surface of water through which light from the bulb can emerge out? Refractive index of water is 1.33. (Consider the bulb to be a point source.) 

    Solution

    Here, the source of light (S) is 80 cm below the surface of water. 

    i.e., SO = 80 cm = 0.8 m 

    When angle of incidence, 

     i = C,for SA and SB and r = 90° 

    Therefore, Area of the surface of water through which light from the bulb can emerge is area of the circle of radius, 

    r =AB2= OA = OBAs, μ =  1sincsinc = 1μ = 11.33 = 0.75C = 48.6°In OBS, tan C = OBOS   OB = OS tanc = 0.8 tan 48.6°r = 0.8 × 1.1345  = 0.907 mSo, area of the surface water  = πr2 = 3.14(0.907)2 = 25.18 m2

    Question 784
    CBSEENPH12038961
    Question 785
    CBSEENPH12038964

    Define the activity of a given radioactive substance. Write its S.I. unit.          

    Solution

    The rate of decay of a radioactive substance is called activity of that substance. Activity is the negative of the rate of decay of the radioactive substance. 

    SI unit is Becquerel (Bq.)

    Question 786
    CBSEENPH12038966

    Write the expression for the de Broglie wavelength associated with a charged particle having charge ‘q’ and mass ‘m’, when it is accelerated by a potential V.

    Solution

    De-broglie wavelength for a charged particle is given by, 
                                straight lambda space equals space straight h over straight p space equals space fraction numerator straight h over denominator square root of 2 mqV end root end fraction

    Question 787
    CBSEENPH12038967

    Draw typical output characteristics of an n-p-n transistor in CE configuration. Show how these characteristics can be used to determine output resistance.        

    Solution

    The output characteristics of an n-p-n transistor in CE configuration are shown below:

    Output resistance is defined as the ratio of change in collector-emitter voltage to change in collector current at a constant base current. The reciprocal of the slope of the linear part of the output characteristics represents the output resistance.

     straight r subscript straight o space equals space open parentheses fraction numerator increment straight V subscript CE over denominator increment straight I subscript straight c end fraction close parentheses subscript straight I subscript straight B end subscript

    Question 788
    CBSEENPH12038968
    Question 789
    CBSEENPH12038973

    A convex lens of focal length f1 is kept in contact with a concave lens of focal length f2. Find the focal length of the combination.

    Solution

    Focal length of convex lens = +f1

     Now, using lens formula, we have
    plus 1 over straight f subscript 1 space equals space fraction numerator 1 over denominator v apostrophe end fraction space minus space 1 over u                       ... (1) 

    For concave lens of formula, focal length is (-f2)
    negative 1 over straight f subscript 2 equals 1 over v space minus space fraction numerator 1 over denominator v apostrophe end fraction space                       ... (2) 
    Now, adding equations (1) and (2), we have
    1 over straight f subscript 1 space minus space 1 over f subscript 2 space equals space 1 over v space minus space 1 over u               ... (3) 

    Now, for the combined lens using the lens formula, we have,
    1 over straight f space equals space 1 over v space minus space 1 over u                        ... (4) 
    Therefore, from equations (3) and (4), we have
    1 over straight f space equals space 1 over f subscript 1 space minus space 1 over f subscript 2

    This is the required focal length of the combination of lenses.

    Question 790
    CBSEENPH12038974

    In the block diagram of a simple modulator for obtaining an AM signal, shown in the figure, identify the boxes A and B. Write their functions. 

         

    Solution

    In the block diagram,

    A is the square law device- This is a non-linear device and produces a non-linear output of message and carrier signals.

    B is the band pass filter and it rejects high and low frequencies. It allows only a band of frequencies to pass through.

    Question 791
    CBSEENPH12038975

    In the circuit shown in the figure, identify the equivalent gate of the circuit and make its truth table. 

    Solution

    A and B act as NOT gate which is then AND’ed.
    So comma space

straight y space equals space top enclose top enclose straight A. top enclose straight B end enclose space equals space straight A space plus space straight B 

    The equivalent of these combination of gates is the OR gate.

     Truth table of the combination is given by, 

    Truth table of OR gate is as shown below:

    Question 792
    CBSEENPH12038981

    Draw V – I characteristics of a p–n junction diode. Answer the following questions, giving reasons:

    (i) Why is the current under reverse bias almost independent of the applied potential up to a critical voltage?

    (ii) Why does the reverse current show a sudden increase at the critical voltage?

     Name any semiconductor device which operates under the reverse bias in the breakdown region. 




    Solution

    V-I characteristics of p-n junction diode are as shown on the right side:

    i) The current of order in reverse biasing is due to the drifting of minority charge carriers from one region to another through the junction. A small amount of applied voltage is sufficient to sweep the minority charge carriers through the junction. So reverse current is almost independent of critical voltage.

    ii) During the critical voltage or most commonly called breakdown voltage, enormous covalent bonds break. As a result, large number of charge carriers increase. Therefore, current increases at critical voltage.

    Zener diode operates under the reverse bias in the breakdown region.

    Question 793
    CBSEENPH12038982

    Draw a labelled ray diagram of a refracting telescope. Define its magnifying power and write the expression for it.

    Write two important limitations of a refracting telescope over a reflecting type telescope.

    Solution

    The labelled diagram of a refracting telescope is as shown below:

    Magnification power is defined as the ratio of the angle () subtended by the final image on the eye to the angle () subtended by the object on eye.

    The mathematical formula is given by,
    straight M thin space equals space fraction numerator tan space straight beta over denominator tan space straight alpha end fraction space equals space open parentheses straight beta over straight alpha close parentheses 
    Also, it is given by,

    Magnifying space power comma space straight M space equals space fraction numerator negative space straight f subscript straight o over denominator straight f subscript straight e end fraction space

space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space equals space fraction numerator negative space straight f subscript straight o over denominator straight f subscript straight e end fraction space open parentheses 1 space plus space straight f subscript straight e over straight D close parentheses

    Limitations of refracting telescope over a reflecting telescope are:

     (i) Image is not free from chromatic aberration and spherical aberration.

     (ii) Aperture of the objective lens should be large for high resolving power.

    Question 794
    CBSEENPH12038983

    Write Einstein’s photoelectric equation and point out any two characteristic properties of photons on which this equation is based. Briefly explain the three observed features which can be explained by this equation. 

    Solution

    Einstein’s photoelectric equation is given by, 
                       straight K subscript max space equals space 1 half mv squared subscript max space equals space hν space minus space hν subscript straight o

    Characteristic property of photons:

    i) Energy of photon is directly proportional to the frequency.

    ii) Total energy and momentum of the system of two constituent particles remain constant in photon-electron collision.

    Three observed features of photoelectric effect are:

    i) When frequency of incident photon increases, kinetic energy of emitted electron increases. Kinetic energy does not have any effect on Intensity of radiations.

    ii) When intensity of incident light increases, the number of incident photons increases. The increase in intensity will increase the number of ejected electrons. That is, photocurrent will increase with increase of intensity. Frequency has no effect on photocurrent.

    iii) When the energy of incident photon is greater than work function, the photoelectron is immediately ejected. Thus, there is no time lag between incidence of light and emission of photoelectrons.

    Question 795
    CBSEENPH12038984

    Name the type of waves which are used for line of sight (LOS) communication. What is the range of their frequencies? 

    A transmitting antenna at the top of a tower has a height of 20 m and the height of the receiving antenna is 45 m. Calculate the maximum distance between them for satisfactory communication in LOS mode. (Radius of the Earth = 6.4 × 106 m)

    Solution

    Types of waves are:

     i) space waves

     ii) radio waves

     iii) microwave
    The frequency range for LOS communication is 40 MHz.

    Given,

    Height of the transmitting antenna, h = 20 m

    Height of receiving antenna = 45 m
    So, maximum distance between transmitting antenna and receiving antenna is given by,
    straight d subscript max space equals space square root of 2 Rh subscript straight T end root space minus space square root of 2 Rh subscript straight R end root space

space space space space space space space space space equals space square root of 2 space straight x space 6.4 space straight x space 10 to the power of 6 straight x 20 end root space plus space square root of 2 straight x 6.4 straight x 10 to the power of 6 straight x 45 end root

space space space space space space space space space equals space left parenthesis 16 space plus space 24 right parenthesis space straight x space 10 cubed space straight m space

space space space space space space space space space equals space 40 space km

    Question 796
    CBSEENPH12038985

    (a) What is linearly polarized light? Describe briefly using a diagram how sunlight is polarised.

    (b) Unpolarized light is incident on a Polaroid. How would the intensity of transmitted light change when the polaroid is rotated? 

    Solution

    a) When an unpolarized light is transmitted through a polarizer, only one component is along the direction of propagation. This transmitted light is called as linearly polarized light.
    The incident sunlight is unpolarized. Molecule in air acts as a dipole radiator. When the sunlight falls on a molecule, dipole molecule does not scatter energy along the dipole axis; however the electric field vector of light wave vibrates just in one direction perpendicular to the direction of the propagation. The light wave having direction of electric field vector in a plane is said to be linearly polarized.

    b) When unpolarized light is incident on a Polaroid, the transmitted light has electric vibrations in the plane consisting of Polaroid axis and direction of wave propagation.

    The plane of polarization will change when the Polaroid is rotated. However, the intensity of transmitted light will remain unchanged.

    Question 797
    CBSEENPH12038986

    One day Chetan’s mother developed a severe stomach ache all of a sudden. She was rushed to the doctor who suggested for an immediate endoscopy test and gave an estimate of expenditure for the same. Chetan immediately contacted his class teacher and shared the information with her. The class teacher arranged for the money and rushed to the hospital. On realizing that Chetan belonged to a below average income group family, even the doctor offered concession for the test fee. The test was conducted successfully.

    Answer the following questions based on the above information:

    (a) Which principle in optics is made use of in endoscopy?

    (b) Briefly explain the values reflected in the action taken by the teacher.

    (c) In what way do you appreciate the response of the doctor on the given situation? 

    Solution

    a) The principle of total internal reflection is made use of in endoscopy. If a light ray enters one end of an optic fiber coated with a material of low refractive index, it refracted and strikes the walls at angle greater than critical angle. Thus light rays show multiple reflections, without being absorbed at the side walls.

    b) The values reflected from the character of teacher are caring nature, a helping attitude towards the kids. Being hospitable towards others makes one a better being and makes the society also a better place to live in.

    c) Being sympathetic towards Chetan and his family’s condition, the doctor gave a reduction in the fee, which is highly appreciable. Such professional ethics of doctor in the society would be of immense help to a person belonging to average income groups.

    Question 798
    CBSEENPH12038991

    Using Bohr’s postulates, derive the expression for the frequency of radiation emitted when electron in hydrogen atom undergoes transition from higher energy state (quantum number ni ) to the lower state, (nf ).

    When electron in hydrogen atom jumps from energy state ni =4 to nf =3, 2, 1, identify the spectral series to which the emission lines belong.

    Solution

    According to Bohr’s postulates, in a hydrogen atom, a single electron revolves around a nucleus of charge +e. For an electron moving with a uniform speed in a circular orbit on a given radius, the centripetal force is provided by the Coulomb force of attraction between the electron and the nucleus.

    Therefore, 
    fraction numerator m v squared over denominator r end fraction space equals space fraction numerator 1 space left parenthesis Z e right parenthesis space left parenthesis e right parenthesis over denominator 4 pi epsilon subscript o r squared end fraction                                       ... (1) 
    rightwards double arrow m v squared space equals fraction numerator 1 space over denominator 4 pi epsilon subscript o end fraction fraction numerator Z e squared over denominator r end fraction
    So, Kinetic Energy, K.E = 1 half m v squared
    K. E equals fraction numerator 1 over denominator 4 pi epsilon subscript o end fraction fraction numerator Z e squared over denominator r end fraction
    Potential energy is given by, P.E = fraction numerator 1 over denominator 4 pi epsilon subscript o end fraction fraction numerator left parenthesis Z e right parenthesis space left parenthesis negative e right parenthesis over denominator r end fraction space equals space minus fraction numerator 1 space over denominator 4 pi epsilon subscript o end fraction fraction numerator Z e squared over denominator r end fraction
    Therefore, total energy is given by, E = K.E + P.E = Error converting from MathML to accessible text.
    E =  negative fraction numerator 1 space over denominator 4 pi epsilon subscript o end fraction fraction numerator Z e squared over denominator 2 r end fraction, is the total energy. 
    For nth orbit, E can be written as En,
    straight E subscript straight n space equals negative space fraction numerator 1 over denominator 4 πε subscript straight o end fraction fraction numerator Ze squared over denominator 2 straight r subscript straight n end fraction italic space                           ... (2) 
    Now, using Bohr's postulate for quantization of angular momentum, we have
    mvr space equals space fraction numerator nh over denominator 2 straight pi end fraction
    rightwards double arrow straight v space equals space fraction numerator nh over denominator 2 πmr end fraction 

    Putting this value of v in equation (1), we get
    Error converting from MathML to accessible text.
    rightwards double arrow space straight r space equals space fraction numerator straight epsilon subscript straight o straight h squared straight n squared over denominator πmZe squared end fraction

    rightwards double arrow space straight r space equals space fraction numerator straight epsilon subscript straight o straight h squared straight n squared over denominator πmZe squared end fraction 

    Now, putting value of rn in equation (2), we get
    Error converting from MathML to accessible text. 
    R is the rydberg constant. 

    For hydrogen atom Z =1,
    straight E subscript straight n space equals space fraction numerator negative Rch over denominator straight n squared end fraction
    If ni and nf are the quantum numbers of initial and final states and Ei & Ef are energies of electron in H-atom in initial and final state, we have 

    straight E subscript straight i space equals negative space Rhc over straight n subscript straight i squared space and space straight E subscript straight f space equals space fraction numerator negative Rhc over denominator straight n subscript straight f squared end fraction 
    If comma space straight upsilon space is space the space frequency space of space emitted space radiation comma space we space get space
    straight nu space equals space fraction numerator straight E subscript straight i space minus space straight E subscript space straight f end subscript over denominator straight h end fraction

straight nu space equals space fraction numerator negative Rc over denominator straight n subscript straight i squared end fraction minus open parentheses fraction numerator negative Rc over denominator straight n subscript straight f squared end fraction close parentheses space equals space Rc open square brackets 1 over straight n subscript straight f squared space minus space 1 over straight n subscript straight i squared close square brackets

    That is, when electron jumps from ni = 4 to nf = 3.21 .
    Radiation belongs to Paschen, Balmer and Lyman series.

    Question 799
    CBSEENPH12038992

    (a) Draw the plot of binding energy per nucleon (BE/A) as a function of mass number A. Write two important conclusions that can be drawn regarding the nature of nuclear force.

    (b) Use this graph to explain the release of energy in both the processes of nuclear fusion and fission.

    (c) Write the basic nuclear process of neutron undergoing –decay. Why is the detection of neutrinos found very difficult?

    Solution

    Graphical representation of (BE/A) for nucleons with mass number A.

    The variation of binding energy per nucleon VS. mass number is shown in the figure:
    Characteristics of Nuclear force:

    (i) Nuclear forces non-central and short ranged force.
    (ii) Nuclear forces between proton-neutron and neutron-neutron are strong and attractive in nature.

    b) When a heavy nucleus (A > 235 say) breaks into two lighter nuclei (nuclear fission), the binding energy per nucleon increases i.e, nucleons get more tightly bound. This implies that energy would be released in nuclear fission.
    When two very light nuclei (A £10) join to form a heavy nucleus, the binding is energy per nucleon of fused heavier nucleus more than the binding energy per nucleon of lighter nuclei, so again energy would be released in nuclear fusion.

    c) During the decay process of neutron, we have
    n presubscript 0 presuperscript 1 space rightwards arrow space p presubscript 1 presuperscript 1 space plus space beta presubscript negative 1 end presubscript presuperscript 0 space plus space nu with bar on top space 
    Neutrinos show weak interaction with other particles. Hence, its detection is very different.

    Question 800
    CBSEENPH12038995

    A concave lens of refractive index 1.5 is immersed in a medium of refractive index 1.65. What is the nature of the lens ? 

    Solution

    Here, a concave lens is placed in a medium of refractive index greater than the refractive index of the material of the lens. 
    So, the given lens will behave as a diverging lens. 

    Question 801
    CBSEENPH12038996

    How are side bands produced?

    Solution

    When the audio frequency modulating signal wave is superimposed on a high frequency wave called carrier wave, the modulation process produce frequencies that are the sum and difference of carrier and modulating frequencies. These frequencies are side bands.
    Lower side band frequency =  f subscript c space minus space f subscript m
    Upper side band frequency = f subscript c space plus space f subscript m
    where,
    f subscript c is the carrier wave frequency and
    f subscript m is the modulating/audio signal frequency.

    Question 802
    CBSEENPH12038998

    A proton and an α-particle have the same de-Broglie wavelength. Determine the ratio of

    (i) their accelerating potentials
    (ii) their speeds.

    Solution

    De-broglie wavelength of the particle is given by, 
    lambda space equals space h over p space equals space fraction numerator h over denominator m v end fraction equals fraction numerator h over denominator square root of 2 m q V end root end fraction;
    where, V= Accelerating potential and v is the speed of the particle. 
    Given that, the de-broglie wavelength is same for both proton and a-particle.
    Charge on straight alpha particle = 2 qp;
    Mass of straight alpha-particle = 4 mp 
    Charge on proton= qp
    Mass of proton =  mp 
    lambda subscript a space equals space lambda subscript p
    rightwards double arrow space fraction numerator h over denominator square root of 2 m subscript alpha q subscript alpha V subscript alpha end root end fraction space equals space fraction numerator h over denominator square root of 2 m subscript p q subscript p V subscript p end root end fraction

italic rightwards double arrow italic space italic space m subscript alpha q subscript alpha V subscript alpha space equals space m subscript p q subscript p V subscript p

rightwards double arrow space space V subscript p over V subscript alpha space equals space fraction numerator m subscript alpha q subscript alpha over denominator m subscript p q subscript p end fraction equals space fraction numerator italic 4 space m subscript p over denominator m subscript p end fraction cross times fraction numerator italic 2 q subscript p over denominator q subscript p end fraction space equals space 2 over 1

    2 : 1 is the required ratio of the accelerating potential.
    Also, 
    lambda subscript a space equals space lambda subscript p

rightwards double arrow space space space fraction numerator h over denominator m subscript alpha nu subscript alpha end fraction space equals space fraction numerator h over denominator m subscript p nu subscript p end fraction

rightwards double arrow space space space space space space space space v subscript p over v subscript alpha space equals space m subscript alpha over m subscript p equals space fraction numerator italic 4 space m subscript p over denominator m subscript p end fraction space equals space italic 4 over italic 1
    4 : 1 is the required ratio of the speed of proton to speed of alpha-particle.  

    Question 803
    CBSEENPH12038999

    Show that the radius of the orbit in hydrogen atom varies as , where n is the principal quantum number of the atom. 

    Solution

    The electrostatic force of attraction between nucleus and the electron is, 
                                                    straight F equals ke squared over straight r

    According to Bohr’s theory, a hydrogen atom consists of a nucleus with a positive charge e and a single electron of charge –e, which revolves around it in circular orbit of radius r.

    To keep electron bound to its orbit, centripetal force on the electron becomes equal to the electrostatic attraction. Therefore, 
    space space space space space space space space space space space space space space space mv squared over straight r equals ke squared over straight r space

space space space space space space space space space space space space space space space space space mv squared space equals space ke squared over straight r

rightwards double arrow space space space space space space space space space space space space space space space italic space space straight r space equals space italic ke to the power of italic 2 over italic mv to the power of italic 2 italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic. italic. italic. italic space italic left parenthesis italic 1 italic right parenthesis

    where,
    m is the mass of electron, and

    v is the speed of an orbit of radius r. 

    Now, using  Bohr’s  quantisation condition for angular momentum,

    straight L straight space equals straight space mvr straight space equals straight space fraction numerator nh over denominator 2 straight pi end fraction

rightwards double arrow space space space space space space space straight v straight space equals straight space fraction numerator nh over denominator 2 πmr end fraction space space space space space space space space space space... space left parenthesis 2 right parenthesis thin space

Putting space left parenthesis 2 right parenthesis space in space equation space left parenthesis 1 right parenthesis comma space we space have

straight r straight space equals straight space fraction numerator ke squared over denominator straight m left parenthesis fraction numerator nh over denominator 2 πmr end fraction right parenthesis squared end fraction

space straight r equals straight space fraction numerator ke squared over denominator fraction numerator mn squared straight h squared over denominator 4 straight pi squared straight m squared straight r squared end fraction end fraction

   straight r straight space equals straight space fraction numerator ke squared over denominator mn squared straight h squared end fraction left parenthesis 4 straight pi squared straight m squared straight r squared right parenthesis

   straight r straight space equals straight space fraction numerator straight n squared straight h squared over denominator 4 straight pi squared mke squared end fraction

space space space straight r straight space proportional to straight space straight n squared  
    where, n is the principal quantum number.

    Question 804
    CBSEENPH12039000

    Distinguish between intrinsic and extrinsic semiconductors? 

    Solution

    Intrinsic semiconductor

    Extrinsic semiconductor

    1. It is a pure semiconductor material with no impurity atoms in it. 

    1. The pure semiconductors doped with tetravalent or pentavalent impurity atoms are called extrinsic semiconductors.

    2. Their electrical conductivity is low.

    2. Their electrical conductivity is high.

    3. Number of free electrons in the conduction band is equal to the number of holes in the valence band.

    3. Number of holes is never equal to the number of electrons. No. of electrons is greater in n-type semiconductor and number of holes is greater in p-type semiconductor.

    Question 805
    CBSEENPH12039001

    Use the mirror equation to show that an object placed between f and 2f of a concave mirror produces a real image beyond 2f?

    Solution

    Mirror formula is given by, 
                                 1 over v plus 1 over u space equals space 1 over f

    where,
    u is the distance of the object from the mirror,

    v is the distance of image from the mirror, and

    f is the focal-length of the mirror. 

    For a concave mirror, f < 0.

    Object distance is negative for an object on the left side. i.e., u< 0.

    Given, f < u <2f.

    Subtracting throughout from 1 over f, we get
    1 over f minus fraction numerator 1 over denominator 2 f end fraction greater than 1 over f minus 1 over u greater than 1 over f minus 1 over f
    fraction numerator 1 over denominator 2 f end fraction space less than space 1 over v space less than thin space 0

    Therefore, the image formed is negative and is on the left side.

    Also, the inequality implies, 2f > v. i.e., |2f| < |v|. 

    That is, the real image is formed beyond 2f. 





    Question 806
    CBSEENPH12039002

    Find an expression for intensity of transmitted light when a polaroid sheet is rotated between two crossed polaroids. In which position of the polaroid sheet will the transmitted intensity be maximum?

    Solution

    Let us consider three polaroids A, B and C where C is kept in between A and B.

    Using Malu’s Law, the intensity of light emerging from the middle polaroid C is given by,
    straight I subscript 1 space equals space straight I subscript straight o cos squared straight theta space semicolon space straight I subscript straight o is straight space the straight space intensity straight space of straight space light straight space falling straight space on straight space middle straight space polaroid.
    Therefore, intensity  falls on the polaroid at the end (polaroid B) whose polarisation axis makes an angle of (90 degree space – space straight theta right parenthesis spacewith the polarisation axis of the angle of middle polaroid.

    Therefore, Intensity of light emerging from Polaroid B is, 
    straight I subscript 2 space equals space straight I subscript 1 cos squared space left parenthesis space 90 minus straight theta right parenthesis

space space space equals space left parenthesis straight I subscript straight o cos squared straight theta right parenthesis space cos squared left parenthesis 90 space minus space straight theta right parenthesis space

italic space italic space italic space equals space straight I subscript o cos to the power of italic 2 θsin to the power of italic 2 straight theta

space space space space equals space fraction numerator 1 over denominator 4 space end fraction straight I subscript 0 space left parenthesis 2 space sinθcosθ right parenthesis squared space
straight I subscript italic 2 space equals space I subscript o over italic 4 sin to the power of italic 2 space 2 straight theta  

    That is, transmitted intensity will be maximum when sin 2 straight theta = 1 
    2 straight theta space equals space 90 to the power of straight o

rightwards double arrow space space space space space space straight theta space space equals space 45 to the power of straight o

    Question 807
    CBSEENPH12039005

    (i) A giant refracting telescope has an objective lens of focal length 15 m. If an eye piece of focal length 1.0 cm is used, what is the angular magnification of the telescope?

    (ii) If this telescope is used to view the moon, what is the diameter of the image of the moon formed by the objective lens ? The diameter of the moon is 3.48 × 106  m and the radius of lunar orbit is 3.8 × 108 m.

    Solution
    (i)
    Angular magnification is given by, 

    Error converting from MathML to accessible text.

    where,   
    fo  is the focal length of the objective lens, and

    fe is the focal length of the eye-piece.
    ii)
    Given, diameter of the moon = 3.48 × 106 m

    Radius of the lunar orbit = 3.8 × 108  m
    Diameter of the image of moon formed by the objective lens is given by, d = straight alpha space straight f subscript straight o 
    straight d space equals space fraction numerator Diameter space of space the space moon over denominator Radius space of space the space lunar space orbit end fraction space cross times space straight f subscript straight o 
     Error converting from MathML to accessible text.


     

    Question 808
    CBSEENPH12039006

    Write Einstein’s photoelectric equation and mention which important features in photoelectric effect can be explained with the help of this equation. The maximum kinetic energy of the photoelectrons gets doubled when the wavelength of light incident on the surface changes from  straight lambda subscript 1 to straight lambda subscript 2 . Derive the expressions for the threshold wavelength  straight lambda subscript straight o and work function for the metal surface. 

    Solution

    Einstein’s photoelectric equation is given as: 
    hν space equals space straight ϕ subscript straight o plus space straight K. straight E subscript max
    where, hstraight nu is the energy of the photon,
    straight ϕ subscript straight o, is the work function of the metal,
    straight K. straight E subscript max is the maximum kinetic energy of the emitted photoelectron. 

    Maximum kinetic energy is given by,
    straight K. straight E subscript max space equals space 1 half mv subscript max superscript 2 space equals space hν space minus space straight ϕ subscript straight o space equals space hν space minus space hν subscript straight o ;  
    where,straight space straight nu subscript straight o is the threshold frequency of the metal surface.

    Features of the equation of photo-electric effect are:

    a) When  a photon of suitable radiation falls on the metal surface, a photoelectron is ejected. If the intensity of the light is increased number of photons incident on the metal surface increases and hence, the number of photo-electrons ejected also increases. This implies, photo current is proportional to intensity and radiation.

    b) If frequency is less than the threshold frequency, i.e.,  the, photoelectric emission does not take place for incident radiation.

    c) When frequency of the incident light is greater than the threshold frequency, maximum K.E increases. This implies, maximum K.E of photoelectrons depends upon the frequency of incident light. 

    Einstein’s equation corresponding to wavelength straight lambda subscript 1 space end subscript is comma space 
    straight K. straight E subscript max space equals space hc over straight lambda subscript 1 minus straight ϕ subscript straight o space space space space space space space space space space end subscript space space... space left parenthesis 1 right parenthesis 
    Einstein’s equation corresponding to wavelength straight lambda subscript 2 is, 
    2 straight K. straight E subscript max space equals space hc over straight lambda subscript 2 minus straight ϕ subscript straight o
rightwards double arrow space space space space space straight K. straight E subscript max space equals space fraction numerator hc over denominator 2 straight lambda subscript 2 end fraction minus straight ϕ subscript straight o over 2 space space space space space space space space space space space space space space space... space left parenthesis 2 right parenthesis thin space
 
    From equation (1) and (2), we have
    Error converting from MathML to accessible text. 
    where, straight lambda subscript straight o is the threshold wavelength.  

     

    Question 809
    CBSEENPH12039007

    In the study of Geiger-Marsdon experiment on scattering of straight alpha particles by a thin foil of gold, draw the trajectory of -particles in the coulomb field of target nucleus. Explain briefly how one gets the information on the size of the nucleus from this study. From the relation straight R space equals space straight R subscript straight o space straight A to the power of begin inline style bevelled 1 third end style end exponent where Ro is constant and A is the mass number of the nucleus, show that nuclear matter density is independent of A. 

    Solution


    Consider an alpha-particle with initial K.E = 1 half m space v squared directed towards the center of nucleus of an atom.
    The force that exists between nucleus and α-particle is Coulomb’s repulsive force. On account of this force, at the distance of closest approach r subscript o , the particle stops and cannot go further closer to the nucleus. And, K.E gets converted to P.E. 
    That is, 
    Error converting from MathML to accessible text. 

    Hence, we can see that the size of the nucleus is approximately equal to the distance of closest approach, ro  .

    Now,

    If ‘m’ is the average mass of the nucleon and r the radius of nucleus, then

    Mass of nucleus = mA; where A is the mass number of the element.
    Volume of the nucleus, straight V space equals space 4 divided by 3 space πR cubed
    This implies, 
    Error converting from MathML to accessible text. 
    Therefore, the nuclear density is independent of mass number A. 


    Question 810
    CBSEENPH12039008

    Distinguish between nuclear fission and fusion. Show how in both these processes energy is released.

    Calculate the energy release in MeV in the deuterium-tritium fusion reaction: 

    Error converting from MathML to accessible text.

    Solution

    Nuclear Fission

    Nuclear Fusion

    The process of breaking a heavy nucleus into two or more lighter nuclei.

    The phenomenon of combining or fusing two or more lighter nuclei to form a single nucleus.

     Error converting from MathML to accessible text.  Error converting from MathML to accessible text.

    The given equation is, 
    straight H presubscript 1 presuperscript 2 straight space plus straight space straight H presubscript 1 presuperscript 3 rightwards arrow He presubscript 2 presuperscript 4 plus straight space straight n
    Mass of the reactant, straight m subscript straight r space equals space straight m left parenthesis straight H presubscript 1 presuperscript 2 right parenthesis space plus space straight m left parenthesis straight H presubscript 1 presuperscript 2 right parenthesis

                                     = (2.014102 + 3.016049) u

                                     = 5.030151u  
    Mass of the product, straight m subscript straight p space equals space straight m space left parenthesis He presubscript 2 presuperscript 4 right parenthesis space plus space straight m subscript straight n

                                     = (4.002603 + 1.008665) u

                                     = 5.011268 u 
    Difference in energy, increment straight m straight space equals straight space straight m subscript straight r straight space minus straight space straight m subscript straight p

                                        = (5.030151 – 5.011268) u

                                        = 0.018883u 

    Therefore, Energy released, E = increment straight m straight space straight c squared

                                          = 0.018883 × 931.5 MeV 

                                          = 17.589514 MeV 

    Question 811
    CBSEENPH12039009

    Draw a block diagram of a detector for AM signal and show, using necessary processes and the waveforms, how the original message signal is detected from the input AM waves.

    Solution

    Detection is the process of recovering modulating signal from the modulated carrier wave.

    On receiving the message, the modulated signal is passed through a rectifier and an envelope signal is produced. This envelope signal is the message signal. The message signal is retrieved by passing it through an envelope detector. This way, modulating signal is obtained.

    Question 812
    CBSEENPH12039013

    With what considerations in view, a photodiode is fabricated? State it’s working with the help of a suitable diagram.

    Even though the current in the forward bias is known to be more than in the reverse bias, yet the photodiode works in reverse bias. What is the reason? 

    Solution

    A photodiode is used to observe the variation in current when the light intensity changes under reverse bias condition below the breakdown voltage.

    A material of band gap ~1.5 eV or lower is chosen so that solar conversion efficiency is better. Hence, Ga-As or Si material is chosen for the fabrication of photo-diode.

    Working: It is a p – n junction fabricated with a transparent window to allow light photons to fall on it. Upon absorption, these photons generate electron hole pairs. If the junction is reverse biased using an electrical circuit, these electron hole pair move in opposite directions so as to produce current in the circuit. This current is very small and is detected by the micro-ammeter connected to the circuit. 

    The change in reverse saturation current is directly proportional to the change in incident light intensity when photo-diode is operated in reverse condition. This is not the case when the photo-diode is forward biased.

    Question 813
    CBSEENPH12039014

    Draw a circuit diagram of a transistor amplifier in CE configuration.

    Define the terms: (i) Input resistance and (ii) Current amplification factor. How are these determined using typical input and output characteristics?

    Solution

    The circuit diagram of a transistor amplifier in CE configuration is given by, 

    Input resistance-: 

    a)The ratio of change in base-emitter voltage to base current gives us the input resistance. We can calculate change in VBE and change in IB from the input characteristics. To find the input resistance, mark a point P on the input characteristic. Draw a tangent at point P. The reciprocal of slope AB will give us the input resistance. 
     
    b) Current amplification factor: It is defined as the ratio of change in collector current to the change in base current. Output characteristics will help to calculate the current amplification factor.

    Question 814
    CBSEENPH12039015

    Answer the following questions:

    (a) In a double slit experiment using light of wavelength 600 nm, the angular width of the fringe formed on a distant screen is 0.1°. Find the spacing between the two slits.

    (b) Light of wavelength 5000 Å propagating in air gets partly reflected from the surface of water. How will the wavelengths and frequencies of the reflected and refracted light be affected? 

    Solution

    Wavelength of light, straight lambda equals straight space 600 straight space nm straight space equals straight space 600 straight space cross times straight space 10 to the power of – 9 end exponent straight space straight m 

    Angular width of the fringe, straight theta equals space 0.1 degree space

    Using the formula, theta space equals fraction numerator space lambda over denominator d end fraction
    Spacing between the slits, straight d straight space equals fraction numerator straight space straight lambda over denominator straight theta straight space end fraction space equals fraction numerator 600 cross times 10 to the power of negative 9 end exponent over denominator bold italic pi over 180 cross times 0.1 end fraction
                                         equals space fraction numerator 600 cross times 10 to the power of negative 9 end exponent cross times 180 cross times 10 over denominator 3.14 end fraction
                                         equals straight space 34394.90 straight space cross times straight space 10 to the power of – 8 end exponent

equals straight space 0.343 straight space cross times straight space 10 to the power of – 3 end exponent straight space straight m

equals 0.343 straight space cross times straight space 10 to the power of – 3 end exponent straight m
    b) Wavelength of light, straight lambda equals straight space 5000 straight space straight A with straight o on top  

    Frequency of reflected and refracted light is going to be the same.

    Therefore,

    Frequency, straight nu straight space equals straight space straight c over straight lambda 
                     equals space fraction numerator 3 cross times 10 to the power of 8 over denominator 5000 cross times 10 to the power of negative 10 end exponent end fraction

italic equals fraction numerator italic 3 italic cross times italic 10 to the power of italic 8 over denominator italic 5 italic cross times italic 10 to the power of italic minus italic 7 end exponent end fraction

equals space italic 3 over italic 5 cross times 10 to the power of italic 15 italic space end exponent

equals space italic 30 over italic 5 cross times 10 to the power of italic 14
equals space 6 cross times 10 to the power of 14 space bold italic H bold italic z
    This is the required frequency of both refracted and reflected light. 

    Refractive index of water, straight mu space equals space fraction numerator Speed straight space of straight space light straight space in straight space air over denominator Speed straight space of straight space light straight space in straight space water end fraction
    4 over 3 equals straight space fraction numerator 3 cross times 10 to the power of 8 over denominator straight v end fraction

space space straight v space equals space fraction numerator 3 cross times 10 to the power of 8 cross times 3 over denominator 4 end fraction space equals space 2.25 space cross times 10 to the power of 8 straight m divided by straight s
    Therefore, wavelength of the refracted light,
                      straight lambda to the power of apostrophe space equals space fraction numerator 2.25 space cross times 10 to the power of 8 over denominator 6 cross times 10 to the power of 14 end fraction space equals space 0.375 cross times 10 to the power of negative 6 end exponent straight m                                                

    Question 815
    CBSEENPH12039020

    (a) Using Huygens’s construction of secondary wavelets explain how a diffraction pattern is obtained on a screen due to a narrow slit on which a monochromatic beam of light is incident normally.

    (b) Show that the angular width of the first diffraction fringe is half that of the central fringe.

    (c) Explain why the maxima at straight theta equals left parenthesis straight n plus 1 half right parenthesis straight lambda over straight a  become weaker and weaker with increasing n. 

    Solution

    a) Diffraction of light at a Single slit

    A single narrow slit is illuminated by a monochromatic source of light. The diffraction pattern is obtained on the screen placed in front of the slits. There is a central bright region called as central maximum. All the waves reaching this region are in phase hence the intensity is maximum. On both side of central maximum, there are alternate dark and bright regions, the intensity becoming weaker away from the center. The intensity at any point P on the screen depends on the path difference between the waves arising from different parts of the wave-front at the slit.

    According to the figure, the path difference (BP – AP) between the two edges of the slit can be calculated. 
    Path difference, BP – AP = NQ = straight a space sinθ space space almost equal to space aθ
    Angle straight theta is zero at the central point C on the screen, therefore all path difference are zero and hence all the parts of slit are in phase.
    Due to this, the intensity at C is maximum. If this path difference is, (the wavelength of light used), then P will be point of minimum intensity.
    This is because the whole wave-front can be considered to be divided into two equal halves CA and CB and if the path difference between the secondary waves from A and B is straight lambda, then the path difference between the secondary waves from A and C reaching P will be straight lambda/2, and path difference between the secondary waves from B and C reaching P will again be straight lambda/2. Also, for every point in the upper half AC, there is a corresponding point in the lower half CB for which the path difference between the secondary waves, reaching P is straight lambda/2. Thus, destructive interference takes place at P and therefore, P is a point of first secondary minimum. 
    b)
    Central bright lies between, straight theta equals fraction numerator plus straight lambda over denominator straight a end fraction and space straight theta straight space equals straight space fraction numerator negative straight lambda over denominator straight a end fraction
    Therefore, Angular width of central bright fringe = 2 straight theta equals fraction numerator 2 straight lambda over denominator straight a end fraction
    So, 1st diffraction fringe lies between straight theta equals straight lambda over straight a space and space space straight theta equals fraction numerator 2 straight lambda over denominator straight a end fraction
    Therefore, 
    Angular width of first diffraction fringe is, fraction numerator 2 straight lambda over denominator straight a end fraction minus straight lambda over straight a equals straight lambda over straight a
    Hence proved. 

    c) As n increases, part of the slit contributing towards maximum decreases. Therefore, maxima gets weaker with increasing n. 

    Question 817
    CBSEENPH12039029

    A convex lens is placed in contact with a plane mirror. A point object at a distance of 20 cm on the axis of this combination has its image coinciding with itself. What is the focal length of the lens? 

    Solution

    Given, convex lens placed in contact with a plane mirror.
    Image of the object coincides with the object.
    So, the rays refracted from the first lens and then reflected by the plane mirror will be retracing their path.  This would happen when rays refracted by the convex lens fall normally on the mirror i.e., the refracted rays form a beam parallel to principal axis of the lens.

    Hence, the object is at the focus of the convex lens.

    Therefore, focal length, f = 20 cm

    Question 818
    CBSEENPH12039031

    The figure given below shows the block diagram of a generalized communication system. Identify the element labelled 'X' and write its function.


    Solution

    The element labelled 'X' is called 'channel'.
    Channel connects transmitter and receiver. The signal from the transmitter is carried to the receiver by the communication channel.




    Question 819
    CBSEENPH12039034

    For a single slit of width "a", the first minimum of the interference pattern of a monochromatic light of wavelength λ occurs at an angle of lambda over a . At the same angle of lambda over a  , we get a maximum for two narrow slits separated by a distance "a". Explain. 

    Solution

    Width of the slit = a

    The path difference between two secondary wavelets is given by,

                           N λ = a sin θ.

    Since, θ is very small sin  θ =  θ.

    So, for the first order diffraction n = 1, the angle is λ/a.

    Now we know that θ must be very small θ = 0 (nearly) because of which the diffraction pattern is minimum.

    Now for interference case, for two interfering waves of intensity I1 and I2 we must have two slits separated by a distance.

    We have the resultant intensity, I = straight I subscript 1 space plus space straight I subscript 2 space plus 2 square root of straight I subscript 1 straight I subscript 2 cosθ end root 
    Since, θ = 0 (nearly) corresponding to angle λ/a so cos θ = 1 (nearly) 


    So,
    space space space space space space space space space straight I space equals straight I subscript 1 space plus space straight I subscript 2 space plus 2 square root of straight I subscript 1 straight I subscript 2 cosθ end root

rightwards double arrow space space space italic space straight I space equals space straight I subscript 1 space plus space straight I subscript 2 space plus 2 space square root of straight I subscript 1 straight I subscript 2 end root cos left parenthesis 0 right parenthesis

rightwards double arrow space space space space straight I space equals space straight I subscript 1 space plus space straight I subscript 2 space plus 2 space square root of straight I subscript 1 straight I subscript 2 end root italic space


    We see the resultant intensity is sum of the two intensities, so there is a maxima corresponding to the angle λ/a.

    This is why at the same angle of λ/a we get a maximum for two narrow slits separated by a distance "a".

    Question 820
    CBSEENPH12039035

    Write the truth table for the combination of the gates shown. Name the gates used. 

    Solution

    From the logic gates given above, we can say that

    R is the OR GATE

    S is the AND GATE

      A

      B

      Y' = A+B

      Y = Y'.A

      0

      0

      0

      0

      0

      1

      1

      0

      1

      0

      1

      1

      1

      1

      1

      1

    Question 821
    CBSEENPH12039036

    Identify the logic gates marked 'P' and 'Q' in the given circuit. Write the truth table for the combination.


    Solution

    P is NAND GATE and Q is the OR GATE

    Assume:

    X'= top enclose straight A. straight B end enclose

      A

      B

    X'= top enclose straight A. straight B end enclose

      X =B +top enclose straight A. straight B end enclose

      0

      0

      1

      1

      0

      1

      1

      1

      1

      0

      1

      1

      1

      1

      0

      1

    Question 822
    CBSEENPH12039041

    A proton and a deuteron are accelerated through the same accelerating potential. Which one of the two has
    (a) greater value of de-Broglie wavelength associated with it, and

    (b) less momentum?

    Give reasons to justify your answer.

    Solution

    De-Broglie wavelength of a particle depends upon its mass and charge for same accelerating potential, such that

    lambda equals fraction numerator h over denominator square root of 2 m V subscript o q end root end fraction space proportional to fraction numerator 1 over denominator square root of m end fraction

    Wavelength is inversely proportional to q and m. 

    Now, for proton and deuteron, we have   
    lambda subscript P over lambda subscript D equals fraction numerator square root of m subscript D q subscript D end root over denominator square root of m subscript p q subscript P end root end fraction equals fraction numerator square root of left parenthesis 2 m subscript p right parenthesis left parenthesis e right parenthesis end root over denominator square root of left parenthesis m subscript p right parenthesis left parenthesis e right parenthesis end root end fraction equals square root of 2

    where, e is the charge of an electron and mp is the mass of proton.

    Thus, de-Broglie wavelength associated with proton is 2√ times of the de-Broglie wavelength of deuteron and hence it is more.

    (b) Momentum is inversely proportional to the wavelength.

    Mathematically it is given by,

                                      straight p straight space equals straight space straight h over straight lambda ; 

    where, h = plank's constant.

    Wavelength of a proton is more than that of deuteron thus the momentum of a proton is lesser than that of deuteron.

    Question 823
    CBSEENPH12039042

    (i) Monochromatic light of frequency 6.0 × 1014 Hz is produced by a laser. The power emitted is 2.0 × 10−3 W. Estimate the number of photons emitted per second on an average by the source. 

    (ii) Draw a plot showing the variation of photoelectric current versus the intensity of incident radiation on a given photosensitive surface. 

    Solution

    i) Given,

    Frequency of light, straight nu straight space equals 6.0 straight space cross times straight space 10 to the power of 14 straight space Hz
    Power emitted by light, straight P straight space equals straight space 2.0 straight space cross times straight space 10 to the power of negative 3 end exponent straight space straight W

    Number of photons emitted per second on an average is equal to Power per unit energy of one photon.

    Energy of one photon is given by, Energy = hν.

    Therefore,

    Number of photons emitted per second = fraction numerator P o w e r over denominator E n e r g y space o f space o n e space p h o t o n end fraction equals fraction numerator 2 cross times 10 to the power of negative 3 end exponent over denominator 6.63 cross times 10 to the power of negative 34 end exponent cross times 6 cross times 10 to the power of 14 end fraction = 5.03 space cross times space space 10 to the power of 15

    (ii) The plot below shows the variation of photoelectric current Vs. Intensity of incident radiation on a given photosensitive surface. The plot shows a linear proportion.


    Question 824
    CBSEENPH12039043

    A 12.5 eV electron beam is used to bombard gaseous hydrogen at room temperature. Upto which energy levels the hydrogen atoms would be excited?

    Calculate the wavelengths of the first member of Lyman and first member of Balmer series. 

    Solution

    Amount of energy required to excite the electron = 12.5 eV
    Energy of the electron in the nth state of an atom = negative fraction numerator 13.6 straight space straight z squared over denominator straight n squared end fraction straight space eV ; Z is the atomic number of the atom. [Z=1 for hydrogen atom]
    Energy required to excite an atom from the initial state (ni) to the final state (nf) = negative fraction numerator 13.6 over denominator straight n subscript straight f squared end fraction plus fraction numerator 13.6 over denominator straight n subscript straight i squared end fraction

    This energy must be equal to or less than the energy of the incident electron beam.

     

    negative straight space fraction numerator 13.6 over denominator straight n subscript straight f squared end fraction plus fraction numerator straight space 13.6 over denominator straight n subscript straight i to the power of straight space 2 end exponent end fraction straight space equals straight space 12.5 straight space   … (1)

    i=1 for ground state of hydrogen atom.

     

    Energy of the electron in the ground state = −13.6 eV

    Now, putting this in equation (1),
    therefore space minus straight space fraction numerator 13.6 over denominator straight n subscript straight f squared end fraction space plus space 13.6 space equals space 12.5 space

rightwards double arrow space 13.6 space minus space 12.5 space equals space minus straight space fraction numerator 13.6 over denominator straight n subscript straight f squared end fraction

rightwards double arrow space straight n subscript straight f squared straight space equals straight space fraction numerator 13.6 over denominator 1.1 end fraction straight space equals straight space 12.36

rightwards double arrow space straight n subscript straight f space equals space 3.5 

    Since, the state cannot be a fractional number we have nf = 3

    Therefore, hydrogen atom would be excited up to 3rd energy level. 
    b) Rydberg formula is given by, Error converting from MathML to accessible text. ;  straight lambda spaceis the wavelength and R is the Rydberg constant. 
    R = 1.097373157 × 10 7 m-1  

    For the first member of Lyman series, i=1; f=2 
    So, Error converting from MathML to accessible text.
    rightwards double arrow bold lambda space equals space 1215 space cross times 10 to the power of negative 11 end exponent
    For the first member of the Balmer series, i=2; f=3 
    So, 
    Error converting from MathML to accessible text.

    Question 825
    CBSEENPH12039044

    When Sunita, a class XII student, came to know that her parents are planning to rent out the top floor of their house to a mobile company she protested. She tried hard to convince her parents that this move would be a health hazard.

    Ultimately her parents agreed:

    (1) In what way can the setting up of transmission tower by a mobile company in a residential colony prove to be injurious to health?

    (2) By objecting to this move of her parents, what value did Sunita display?
    (3) Estimate the range of E.M waves which can be transmitted by an antenna of height 20 m. (Given radius of the earth = 6400 km)

    Solution

    1) Harmful electromagnetic waves such as microwaves which can cause severe health hazards like tumor and cancer are emitted by the transmitting tower. Added to that, the transmitting antenna operates on very high power. Hence, the chances of someone getting burnt are high. Therefore, TV tower should not be set up in residential areas.

    (2) By objecting to this move of her parents, Sunita has displayed awareness towards the health and environment of her society. 
    (3) Range of the transmitting antenna, d = square root of 2 hR end root; h is the height of the antenna and R is the radius of the earth.

    Given,

    Height of the antenna, h = 20 m

    R = 6400 km = 64 ×105 m

    Therefore, 
    Range, d = square root of 2 cross times 20 cross times 64 cross times 10 to the power of 5 end root
                 =1600 m

    Question 826
    CBSEENPH12039046

    (a) Draw a labelled ray diagram showing the formation of a final image by a compound microscope at least distance of distinct vision.

    (b) The total magnification produced by a compound microscope is 20. The magnification produced by the eye piece is 5. The microscope is focused on a certain object. The distance between the objective and eyepiece is observed to be 14 cm. If least distance of distinct vision is 20 cm, calculate the focal length of the objective and the eye piece. 

    Solution

    a) The fig. below shows the formation of image by a compound microscope at least distance of distinct vision.

    where, AB = object, A'B' = image formed by objective and A''B'' = image formed by eyepiece.


    fo = focal length of objective,

    uo = object distance from objective

    vo = image distance from objective

    D = distance of least distinct vision

    L
     = length of the microscope

    (b) Total magnification for least distance of clear vision is given by, 
                          Error converting from MathML to accessible text.                       ... (1) 

    where,

    L is the separation between the eyepiece and the objective


    fo is the focal length of the objective,

    fe is the focal length of the eyepiece,

    D is the least distance for clear vision,

    me is the magnification of the eyepiece,

    mo is the magnification of the objective. 

    Here, m =20, L =14 cm, D = 20 cm, me = 5
    Magnification for the eyepiece:
    space space space space space space straight m subscript straight e space equals space 5 space equals space straight m subscript straight e space equals space 1 plus straight D over straight f subscript straight e
rightwards double arrow space 5 straight space equals straight space 1 plus 20 over straight f subscript straight e

rightwards double arrow straight f subscript straight e straight space equals straight space 5 straight space cm comma space is space the space focal space length space of space the space eye minus piece.

    Now, putting the value of mo and me in equation (1), we get
    straight M straight space equals straight space straight m subscript straight o straight m subscript straight e
    space rightwards double arrow space 20 space equals space m subscript o 5

rightwards double arrow space m subscript o space equals space 20 over 5 equals space 4

Now comma space using space the space equation comma space

space space space space space space space space space space space space space space m subscript o equals L over f subscript o
    We have,
    straight f subscript straight o straight space equals straight space 14 over 4 equals 3.5 straight space cm ;is the required focal length of the objective lens.

    Question 827
    CBSEENPH12039047

    (a) A mobile phone lies along the principal axis of a concave mirror. Show, with the help of a suitable diagram, the formation of its image. Explain why magnification is not uniform. (b) Suppose the lower half of the concave mirror's reflecting surface is covered with an opaque material. What effect this will have on the image of the object? Explain.

    Solution

    (a) Formation of image by the concave mirror is shown in the figure below:

    The magnification of each part of the mobile phone is not uniform. The part of the mobile phone at centre of curvature will form image of the same size.
    The part that lies between C and F will form an enlarged image beyond C as shown in the fig. above.
    Since, the nature of the image is not the same at all sections of the principal axis, magnification varies. 

    (b) If lower half of the concave mirror is covered with an opaque material, the size of the image will not vary. But, since the reflecting surface has been reduced, the intensity of the image will be less. That is, brightness of the image will decrease.

    Question 828
    CBSEENPH12039051

    a) Deduce the expression, N = N0 e−λt, for the law of radioactive decay.

    (b) (i) Write symbolically the process expressing the β+ decay of Na presubscript 11 presuperscript 22 . Also write the basic nuclear process underlying this decay.

    (ii) Is the nucleus formed in the decay of the nucleus Na presubscript 11 presuperscript 22 , an isotope or isobar?

    Solution

    As per the law of radioactive decay, we have
    fraction numerator increment straight N over denominator increment straight t end fraction proportional to straight N

    where,

    N = Number of nuclei in the sample

    ΔN = Amount of nuclei undergoing decay

    Δt = Time taken for decay 

    So, fraction numerator increment straight N over denominator increment straight t end fraction equals λN space semicolon spacewhere λ is Decay constant or disintegration constant.
    Δt = 0
    therefore space dN over dt equals space minus straight lambda space straight N
dN over straight N equals space minus straight lambda space dt

Integrating space both space sides comma space we space get

integral subscript straight N subscript straight o end subscript superscript straight N dN over straight N space equals space minus space straight lambda space integral subscript straight t subscript straight o end subscript superscript straight t dt space

ln space straight N space minus space ln space straight N subscript straight o space equals space minus straight lambda space left parenthesis straight t minus straight t subscript straight o right parenthesis

At space straight t subscript 0 space equals space 0 colon

ln space straight N over straight N subscript straight o space equals space minus straight lambda space straight t space

therefore space straight N space left parenthesis straight t right parenthesis space equals space straight N subscript straight o space straight e to the power of negative λt end exponent space 

    (b)
    (i) The β+ decay for  is given below:
    Na presubscript 11 presuperscript 22 space rightwards arrow space Ne presubscript 10 presuperscript 22 straight space plus straight space straight beta to the power of plus straight space plus straight space straight nu

    A proton is converted into neutron if, the unstable nucleus has excess protons than required for stability.

    In the process, a positron e+ (or a β+) and a neutrino ν are created and emitted from the nucleus.
    p → n + β+ + ν
    This process is called beta plus decay.
    (ii) The nucleus so formed is an isobar of Na presubscript 11 presuperscript 22 because the mass number is same, whereas the atomic numbers are different.

    Question 829
    CBSEENPH12039052

    (a) (i) 'Two independent monochromatic sources of light cannot produce a sustained interference pattern'. Give reason.

    (ii) Light waves each of amplitude "a" and frequency "ω", emanating from two coherent light sources superpose at a point. If the displacements due to these waves is given by y1 = a cos ωt and y2 = a cos(ωt + ϕ) where ϕ is the phase difference between the two, obtain the expression for the resultant intensity at the point.

    (b) In Young's double slit experiment, using monochromatic light of wavelength λ, the intensity of light at a point on the screen where path difference is λ, is K units. Find out the intensity of light at a point where path difference is λ/3.

    Solution

    (a)
    (i) The condition for the sustained interference is that both the sources must be coherent (i.e. they must have the same wavelength and the same frequency, and they must have the same phase or constant phase difference).
    Two sources are monochromatic if they have the same frequency and wavelength. Since they are independent, i.e. they have different phases with irregular difference, they are not coherent sources.
    ii) 

    Let the displacement of the waves from the sources S1 and S2 at point P on the screen at any time t be given by: 

    y1 = a cos ωt

    y2 = a cos (ωt + Φ)

    where, Φ is the constant phase difference between the two waves.
    By the superposition principle, the resultant displacement at point P is given by:

    y = y1 + y2

    y = a cos ωt a cos (ωt + Φ)

     

      =2 a[cos cos Error converting from MathML to accessible text. 
    y = 2 acos open parentheses fraction numerator bold italic omega bold italic t plus bold italic ϕ over denominator 2 end fraction close parenthesescos open parentheses bold italic ϕ over 2 close parentheses              ... (i) 
     Let space 2 space straight a space cos space open parentheses straight ϕ over 2 close parentheses space equals space straight A                        ... (2)

    Then, equation (i) becomes:
    y = A cos (ωt+straight space bold italic ϕ over 2 right parenthesis

    Now, we have:

     straight A to the power of 2 space end exponent equals space 4 space straight a squared space cos 2 space left parenthesis straight ϕ divided by 2 right parenthesis space space space space space space space space                    ... (3)

    The intensity of light is directly proportional to the square of the amplitude of the wave. The intensity of light at point P on the screen is given by:
    I = 4 a2 cos2 (bold italic ϕ over 2)                                  ... (4) 

    (b) Wavelength of monochromatic light = straight lambda

    Path difference = bold italic lambda divided by 3.
    So, phase difference,straight phi space equals space fraction numerator 2 straight pi over denominator straight lambda end fraction cross times straight lambda space equals 2 straight space straight pi 

    Intensity of light = K units
    Intensity is given by, I = straight I space equals space 4 space straight I subscript space 0 end subscript cos to the power of space 2 end exponent bevelled straight ϕ over 2
    When path difference is bold italic lambda divided by 3 comma space phase space difference space becomes space straight phi space equals space fraction numerator 2 straight pi over denominator 3 end fraction
    Intensity of light, I’=4 straight space straight I subscript straight space 0 end subscript cos to the power of straight space 2 end exponent bevelled straight ϕ over 2 = 4 space straight I subscript space 0 end subscript cos to the power of space 2 end exponent straight pi over 3 equals straight I subscript straight o
    rightwards double arrow bold I apostrophe space equals space bold K over 4 italic comma italic space i s italic space t h e italic space n e w italic space i n t e n s i t y italic space o f italic space l i g h t italic. italic space

    Question 830
    CBSEENPH12039053

    (a) How does one demonstrate, using a suitable diagram, that unpolarized light when passed through a Polaroid gets polarized?

    (b) A beam of unpolarized light is incident on a glass-air interface. Show, using a suitable ray diagram, that light reflected from the interface is totally polarized, when μ = tan iB, where μ is the refractive index of glass with respect to air and iB is the Brewster's angle. 

    Solution

     

    Polarization of light is referred to as restricting the vibration of light in a perpendicular direction perpendicular to the direction of propagation of wave.

    The vibration of particles of light which is parallel to the axis of crystal passes through the Polaroid on passing an unpolarized light. All other vibrations are absorbed and that is why intensity of emerging light is reduced.

    The plane of vibration here is ABCD, in which the vibrations of the polarized light is confined and the plane KLMN is called plane of polarization. KLMN is perpendicular to the plane of vibration.

    Reflected light is totally polarized, when unpolarized light is incident on the glass-air interface at the Brewster angle iB. This is known as Brewster’s law.

    The reflected component OB and refracted component OC are mutually perpendicular to each other, when light is incident at Brewster’s angle.


    angle space B O y space plus space angle Y O C space equals space 90 to the power of o

left parenthesis 90 to the power of 0 space minus space bold italic i subscript bold italic B right parenthesis space plus space left parenthesis 90 to the power of 0 space plus space bold italic r right parenthesis space equals space 90 to the power of bold italic o

    Now, using Snell’s law, we have

    straight mu straight space equals straight space fraction numerator sin straight space straight i over denominator sin straight space straight r end fraction

    i = iB and r = (900 – iB)
    Therefore,
    straight mu straight space equals straight space fraction numerator sini subscript straight B over denominator sin straight space left parenthesis 90 to the power of straight o straight space minus straight space straight i subscript straight B right parenthesis end fraction straight space equals straight space sini subscript straight B over cosi subscript straight B straight space equals straight space tani subscript straight B

    Question 831
    CBSEENPH12039056

    (a) State briefly the processes involved in the formation of p-n junction explaining clearly how the depletion region is formed.

    (b) Using the necessary circuit diagrams, show how the V-I characteristics of a p-n junction are obtained in
    (i) Forward biasing

    (ii) Reverse biasing

    How these characteristics are made use in rectification?

    Solution

    (a) The n-type semi-conductor has more concentration of electrons than that of a holes and p-type semi-conductor has more concentration of holes. Holes diffuse from p-side to n-side whereas electrons diffuse from n-side to p-side due to difference in concentration of charge carriers.

    An ionized donor is left behind on n-side when electron diffuses from n side to p-side. The ionized donor (+ ve charge) is immobile as it is bound by the surrounding atoms. Therefore, a layer of positive charge is developed on the n-side of the junction. Similarly, a layer of negative charge is developed on the p-side. Hence, a space-charge region is formed on either side of the junction, which has immobile ions and is devoid of any charge carrier, called as depletion layer or depletion region.

    (b) 
    For a p-n junction diode under forward bias, p-side is connected to the positive terminal and n-side is connected to the negative terminal.

    When voltage is applied, electrons in n-region and holes in the p-region moves towards the p-n junction. Hence, there is decrease in the width of the depletion region thereby, offering less resistance. Diffusion of majority carriers takes place in the junction giving rise to a forward current.

    The V-I characteristic of p-n junction in forward bias is shown below:


    (ii) When p-n junction diode is reverse biased, the positive terminal of battery is connected to n-side and negative terminal to p-side. 


    The barrier height increases and the width of depletion region also increase as a result of reverse biasing. There is no conduction across the junction because of the lack of majority charge carriers. After applying a high reverse biased voltage, few minority carriers cross the junction. Hence, a current flows in reverse direction which is known as the reverse current.
    The V-I characteristic of p-n junction diode in reverse bias is shown below:


    p-n junction can be used for rectification purpose. Its working is based on the fact that, resistance of junction becomes low when forward biased and R becomes high when reverse biased.

    Question 832
    CBSEENPH12039057

    (a) Differentiate between three segments of a transistor on the basis of their size and level of doping.

    (b) How is a transistor biased to be in active state?

    (c) With the help of necessary circuit diagram, describe briefly how n-p-n transistor in CE configuration amplifies a small sinusoidal input voltage. Write the expression for the ac current gain.  

    Solution

    On the basis of size and level of doping,

    (a)
    Emitter (E) - Emitter is heavily doped and is the left hand side thick layer of the transistor. 

    Base (B) - It is the central thin layer of the transistor, which is lightly doped.

    Collector (C) - It is the right hand side thick layer of the transistor, which is moderately doped.
    (b)
    There are two conditions for a transistor to be into an active region.

    1. The input circuit should be forward biased by using a low voltage battery.

    2. The output circuit should be reverse biased by using a high voltage battery.

    (c)
    n-p-n Transistor as an amplifier:

    The input circuit is forward biased by using a low voltage battery. Hence, the resistance of the input circuit is small. The output circuit is reverses biased using a high voltage battery. Hence, the resistance of the output circuit is large.

    The operating point is fixed in the middle of its active region.
     

    The output is taken between the collector and the ground.

    Applying Kirchhoff’s law to the output loop:
    VCC = VCE + ICRC
    If Vc is the collector voltage then,
    Vc = VCE − ICRC                                                      ... (A)

    When the input signal voltage is fed to the emitter base circuit, it will change the emitter voltage and hence to the emitter current, which in turn will change the collector current. Due to this the collector voltage VC will vary in accordance with relation (A). This variation in collector voltage appears as the amplified output.

    VBB = VBE + IBRB

    Here, vi ≠ O

    Then, VBB + vi = VBE + IBRB + ΔIB (RB + ri)

     

     

    Error converting from MathML to accessible text. 
    S o comma space beta subscript a c end subscript space equals space fraction numerator increment I subscript c over denominator increment I subscript B end fraction ; is the required expression for current gain.

    Question 833
    CBSEENPH12039063

    Under what condition does a biconvex lens of glass having a certain refractive index act as a plane glass sheet when immersed in a liquid?

    Solution

    When immersed in a liquid, a bi-convex lens of glass will behave as a plane glass, 

    when, mu subscript L space equals space mu subscript gmu subscript L is the refractive index of liquid and  is the refractive index of glass. 
    Question 834
    CBSEENPH12039065

    State de-Broglie hypothesis.

    Solution

    According to hypothesis of de Broglie "The atomic particles of matter moving with a given velocity, can display the wave like properties.
    i.e., straight lambda straight space equals straight space straight h over mv

    Question 835
    CBSEENPH12039066

    A ray of light, incident on an equilateral glass prism ( bold italic mu subscript bold italic g equals square root of 3) moves parallel to the base line of the prism inside it. Find the angle of incidence for this ray.

    Solution

    Since the prism is equilateral in shape, 

    Angle of prism, A = 60o

    Angle of refraction, r = A/2 = 30o

    Now, using Snell’s law, 
    mu subscript g over mu subscript i equals fraction numerator sin space i over denominator sin space r end fraction 

    fraction numerator square root of 3 over denominator 1 end fraction equals fraction numerator sin space i over denominator sin space 30 degree end fraction 
    rightwards double arrow straight space sin straight space straight i straight space equals straight space fraction numerator square root of 3 over denominator 2 end fraction
    i. e. comma space A n g l e space o f space i n c i d e n c e comma space i space equals space 60 degree

    Question 836
    CBSEENPH12039067

    Distinguish between ‘Analog and Digital signals’.

    Solution

    Difference between analog and digital signals is:

    Analog signal

    Digital signal

    They are continuous signals i.e., continuous variation of voltage or current.

    These are the signals which can take only discrete values. In digital signal, high means 1 and low means 0.

    E.g. Sound of a human

    E.g., Temperature


    Question 837
    CBSEENPH12039068

    Mention the function of any two of the following used in communication system:

    (i) Transducer                                       (ii) Repeater

    (iii) Transmitter                                    (iv) Band pass Filter

    Solution

    i) Transducer: A device which converts energy from one form to another form. It is used in microphone for converting sound energy into electrical energy and vice-versa.

    ii) Repeater: It is a combination of a receiver and a transmitter. It is used in transmission system to regenerate the signal by picking up a signal, amplifying it and then transmitting it to the receiver.

    iii) Transmitter: A device which processes the incoming message signal so as to make it suitable for transmission through a channel and for its subsequent reception.

    iv) Bandpass filter: A device which allows only signals of a certain frequency range and blocks the rest of the frequencies. It is used in an electronic filter.

    Question 838
    CBSEENPH12039075

    The current in the forward bias is known to be more (~mA) than the current in the reverse bias (~ A). What is the reason, then, to operate the photodiode in reverse bias?        

    Solution

    The photodiode works in reverse biased condition although the current produced is less. In reverse bias, the width of depletion layer increases thereby reducing the capacitance across the junction. Hence, the response time for absorption of photons increases. Thus, the sensitivity of the photo-diode is increased which is certainly desired.

    Question 839
    CBSEENPH12039079

    (a) Using Bohr’s second postulate of quantization of orbital angular momentum show that the circumference of the electron in the nth orbital state in hydrogen atom is n times the de Broglie wavelength associated with it.

    (b) The electron in hydrogen atom is initially in the third excited state.

    What is the maximum number of spectral lines which can be emitted when it finally moves to the ground state?

    Solution

    i) According to Bohr’s second postulate, we have 
    space space space space space mvr subscript straight n straight space equals straight space straight n fraction numerator straight h over denominator 2 straight pi end fraction
rightwards double arrow straight space 2 πr subscript straight n straight space equals straight space nh over mv

    But, as per De- broglie hypothesis

    straight h over mv equals straight space straight h over straight p equals straight lambda

    Therefore, 2 πr subscript straight n straight space equals straight space nλ ; where  is the de- broglie wavelength.
    ii) Given, electron in the hydrogen atom is in the third excited state.

    For third excited state, n = 4

    For ground state n= 1

    Now, total number of possible spectral lines is given by,
    N space equals space fraction numerator n left parenthesis n minus 1 right parenthesis over denominator 2 end fraction
N space equals space fraction numerator italic 4 italic left parenthesis italic 4 italic minus italic 1 italic right parenthesis over denominator italic 2 end fraction
N equals space fraction numerator italic 4 italic cross times italic 3 over denominator italic 2 end fraction equals space 6 

    The transition states are as shown in the figure above.

    Question 840
    CBSEENPH12039081

    (i) What characteristic property of nuclear force explains the constancy of binding energy per nucleon (BE/A) in the range of mass number ‘A’ lying 30 < A < 170?

    (ii) Show that the density of nucleus over a wide range of nuclei is constant- independent of mass number A.

    Solution

    i) The characteristic property of nuclear force that explains the constancy of binding energy per nucleon is the saturation or short range nature of nuclear forces.

    In heavy nuclei, nuclear size > range of nuclear force.

    ii) Using the formula for radius of the nucleon, we have
    straight R straight space equals straight space straight R subscript 0 straight A to the power of bevelled 1 third end exponent

    Let, m be the mass of nucleon.

    Therefore,

    Density, Error converting from MathML to accessible text. 

    Thus, we can see that density is independent of mass number A.

    Question 841
    CBSEENPH12039082

    Write any two factor which justify the need for modulating a signal.

    Draw a diagram showing an amplitude modulated wave by superposing a modulating signal over a sinusoidal carrier wave.

    Solution

    Two factors justifying the need for modulation are:

    (i) Practical size of antenna.

    (ii) To avoid mixing up of signals from different transmitters i.e., avoid fluctuation and reduce the noise of signal.

    The figures shows how modulated wave is formed by superimposing modulating signal over a carrier wave.


    Question 842
    CBSEENPH12039083

    Write Einstein’s photoelectric equation. State clearly how this equation is obtained using the photon picture of electromagnetic radiation.

    Write the three salient features observed in photoelectric effect which can be explained using this equation. 

    Solution

    Einstein’s photo electric equation is given by, 
                                          hν equals straight phi subscript 0 straight space end subscript plus straight space straight K subscript max
    where, h is planck’s constant, straight nu is the frequency and straight phi spaceis the work function. 

    The energy (hstraight nu ) carried by a photon of frequency  is absorbed by electrons on the surface to 

    i) overcome the work function of metal .

    ii) impart maximum K.E. to the emitted electron (Kmax.)

    Salient features observed in photoelectric effect are:

    i) The stopping potential and maximum kinetic energy of emitted electrons varies linearly with the frequency of incident radiation.

    ii) Photoelectric emission is possible when, bold italic nu space greater than space bold italic nu subscript bold italic o where, straight nu is the cut-off frequency.

    Question 843
    CBSEENPH12039084

    a) Why are coherent sources necessary to produce a sustained interference pattern?

    (b) In Young’s double slit experiment using monochromatic light of wavelength bold italic lambda , the intensity of light at a point on the screen where path difference is bold italic lambda is K units. Find out the intensity of light at a point where path difference is straight lambda over 3.

    Solution

    a)
    Coherent sources have almost the same wavelength. Coherent sources are necessary to ensure that the positions of maxima and minima do not change with time. Thereby, producing a sustained interference pattern.
    b)
    Wavelength of monochromatic light = straight lambda
    Path difference = bold lambda over bold 3 
    So, phase difference, straight phi space equals space fraction numerator 2 straight pi over denominator straight lambda end fraction cross times straight lambda space equals space 2 straight space straight pi

    Intensity of light = K units
    Intensity is given by, I equals space straight I space equals space 4 space straight I subscript space 0 end subscript cos to the power of space 2 end exponent bevelled straight ϕ over 2
    When path difference is bold italic lambda divided by 3, phase difference becomes straight phi straight space equals straight space fraction numerator 2 straight pi over denominator 3 end fraction
    Intensity of light I’ = 4 space straight I subscript space 0 end subscript cos to the power of space 2 end exponent bevelled straight ϕ over 2 equals 4 space straight I subscript space 0 end subscript cos to the power of space 2 end exponent straight pi over 3 equals straight I subscript straight o
    rightwards double arrow bold I apostrophe space equals space bold K over 4, is the new intensity of light. 

    Question 844
    CBSEENPH12039085

    Use Huygen’s principle to explain the formation of diffraction pattern due to a single slit illuminated by a monochromatic source of light.

    When the width of slit is made double the original width, how this affect the size and intensity of the central diffraction band?

    Solution

    According to Huygen's principle "The net effect at any point due to a number of wavelets is equal to sum total of contribution of all wavelets with proper phase difference.

    The point O is maxima because contribution from each half of the slit S1S2 is in phase, i.e., the path difference is zero.

    At point P,
    i) If straight S subscript 2 straight P space minus space straight S subscript 1 straight P space equals space nλ straight space then comma space point straight space straight P straight space would straight space be straight space point straight space of straight space minima.
    ii) If Error converting from MathML to accessible text., then point P would be maxima. At the point of maxima, intensity would decrease.
    The width of the central maxima is given by, fraction numerator 2 bold italic lambda bold italic D over denominator bold italic a end fraction

    where a is the size of the slit; D is the distance between the screen and the slit.

     

    When the width of the slit is made double the original width, then the size of central maxima will be reduced to half and intensity will be four times.

    Question 845
    CBSEENPH12039088

    Define magnifying power of a telescope. Write its expression.

    A small telescope has an objective lens of focal length 150 cm and an eye piece of focal length 5 cm. If this telescope is used to view a 100 m high tower 3 km away, find the height of the final image when it is formed 25 cm away from the eye piece.

    Solution

    a) Magnifying power of telescope is the ratio of the angle subtended at the eye by the image to the angle subtended at the unaided eye by the object.

    Mathematically, we can write
    Error converting from MathML to accessible text.
    where, fo is the focal length of the objective, fe is the focal length of the eye-piece and D is the least distance of distinct vision.

    b) Using, the lens equation for objective lens,
    1 over straight f subscript straight o equals 1 over straight v subscript straight o minus 1 over straight u subscript straight o space

rightwards double arrow 1 over 150 equals straight space 1 over straight v subscript straight o minus fraction numerator 1 over denominator negative 3 cross times 10 to the power of 5 end fraction space

rightwards double arrow 1 over 150 minus fraction numerator 1 over denominator 3 cross times 10 to the power of 5 end fraction equals straight space 1 over straight v subscript straight o space

rightwards double arrow straight v subscript straight o straight space equals fraction numerator 3 cross times 10 to the power of 5 over denominator 1999 end fraction equals straight space 150 straight space cm

    Hence, magnification due to the objective lens is given by,
    bold m subscript bold o straight space equals straight space bold v subscript bold o over bold u subscript bold o equals fraction numerator 150 cross times 10 to the power of negative 2 end exponent over denominator 3000 end fraction equals straight space 10 to the power of negative 2 end exponent over 20
    italic rightwards double arrow italic space m subscript o space italic equals space italic 0 italic. italic 05 italic cross times italic 10 to the power of italic minus italic 2 end exponent

    Now, using lens formula for eye-piece, we get
    space space space space space space space space 1 over bold italic f subscript bold italic e equals 1 over bold italic v subscript bold italic e minus 1 over bold italic u subscript bold italic e

rightwards double arrow space space space space space space 1 fifth equals fraction numerator 1 over denominator negative 25 end fraction minus 1 over bold italic u subscript bold italic e
rightwards double arrow space space space space space bold italic u subscript bold italic e space equals space fraction numerator negative 25 over denominator 6 end fraction bold italic c bold italic m
    Therefore, magnification due to eyepiece me = fraction numerator negative 25 over denominator negative 25 over 6 end fraction equals straight space 6 straight space cm
    Hence, total magnification, straight m straight space equals straight space straight m subscript straight e cross times straight m subscript straight o
    bold italic m equals space 6 space cross times 5 cross times 10 to the power of negative 4 end exponent

space space space equals space 30 cross times 10 to the power of negative 4 end exponent
    So, size of final image = 30 cross times 10 to the power of negative 4 end exponent cross times 100 space straight m space equals space 30 space cm

    Question 846
    CBSEENPH12039089

    Draw a simple circuit of a CE transistor amplifier. Explain its working. Show that the voltage gain AV, of the amplifier is given by A subscript v space equals space minus fraction numerator beta subscript a c end subscript R subscript L over denominator r subscript i end fraction, where bold italic beta subscript bold italic a bold italic c end subscript is the current gain, RL is the load resistance and ri is the input resistance of the transistor. What is the significance of the negative sign in the expression for the voltage gain?

    Solution

    Circuit diagram of CE transistor amplifier, 
     

    When an ac input signal VI (to be amplified) is superimposed on the bias VBB, the output, which is measured between collector and ground, increases.

    We first assume that Vi = 0.

    Applying Kirchoff’s law to the output loop,

           VCC = VCE + IC RL

    Similarly, the input loop gives, 
            VBB = VBE + IB RB

    When Vi is not zero, we have

    VBE + Vi = VBE + IB RBincrement I subscript B space left parenthesis R subscript B space plus space R subscript i right parenthesis

    rightwards double arrow straight space straight V subscript straight i straight space equals straight space increment straight I subscript straight B left parenthesis straight space straight R subscript straight B plus straight R subscript straight i right parenthesis

rightwards double arrow straight space straight V subscript straight i straight space equals straight space straight r increment straight I subscript straight B
    Change in IB causes changes in Ic

    Hence, straight beta subscript ac straight space equals straight space fraction numerator increment straight I subscript straight c over denominator increment straight I subscript straight B end fraction straight space equals straight space straight I subscript straight C over straight I subscript straight B 
    As, increment straight V subscript CC straight space end subscript equals increment straight space straight V subscript CE straight space plus straight space straight R subscript straight L increment straight I subscript straight C straight space equals straight space 0
         rightwards double arrow straight space increment straight V subscript CE straight space equals straight space minus straight R subscript straight L increment straight I subscript straight C
    The change in VCE is the output voltage Vis, 
    rightwards double arrow straight space straight V subscript straight o straight space end subscript equals straight space minus straight R subscript straight L increment straight I subscript straight C

space space space space space space space space equals space straight beta subscript ac increment straight I subscript straight B straight R subscript straight L

    The voltage gain of the amplifier is,

    straight A subscript straight V straight space equals straight space straight V subscript straight o over straight V subscript straight i equals fraction numerator increment straight V subscript CE over denominator straight r increment straight I subscript straight B end fraction equals straight space fraction numerator negative straight beta subscript ac increment straight I subscript straight B straight R subscript straight L over denominator straight r increment straight I subscript straight B end fraction equals negative straight beta subscript ac straight R subscript straight L over straight r

    Negative sign in the expression shows the output voltage and input voltage have phase difference of straight pi.

    Question 847
    CBSEENPH12039090

    Draw the circuit diagram of a full wave rectifier using p-n junction diode. Explain its working and show the output, input waveforms.

    (b) Show the output waveforms (Y) for the following inputs A and B of

    (i) OR gate  

    ii) NAND gate



    Solution

    a)
                         

    Working: The AC input voltage across secondary s1 and s2 changes polarity after each half cycle. Suppose during the first half cycle of input AC signal, the terminal s1 is positive relative to centre tap O and s2 is negative relative to O. Then diode D1 is forward biased and diode D2 is reverse biased. Therefore, diode D1 conducts while diode D2 does not. The direction of current (i1) due to diode D1 in load resistance RL is directed from A to B. In next half cycle, the terminal s1 is negative and s2 is positive relative to centre tap O. The diode D1 is reverse biased and diode D2 is forward biased. Therefore, diode D2 conducts while D1does not. The direction of current (i2 ) due to diode D2 in load resistance RL is still from A to B. Thus the current in load resistance RL is in the same direction for both half cycles of input AC voltage. Thus for input AC signal the output current is a continuous series of unidirectional pulses.


    In a full wave rectifier, if input frequency is f hertz, then output frequency will be 2f hertz because for each cycle of input, two positive half cycles of output are obtained.

    b) Output waveforms for the following inputs A and B of OR gate and NAND gate.

    Question 848
    CBSEENPH12039095
    Question 849
    CBSEENPH12039096

    In a transistor, doping level in base is increased slightly. How will it affect (i) collector current and (ii) base current?    

    Solution

    When doping level is increased in base,

    i) collector current decreases

    ii) base current increases slightly.

    Question 850
    CBSEENPH12039098

    When monochromatic light travels from one medium to another its wavelength changes but frequency remains the same, Explain.      

    Solution

    When monochromatic light travels from one medium to another it’s wavelength and speed both changes and the frequency remains unchanged.

                                                 nu subscript 1 over lambda subscript 1 equals nu subscript 2 over lambda subscript 2

    Question 851
    CBSEENPH12039103

    Two convex lenses of same focal length but of aperture A1 and A2 (A2 < A1), are used as the objective lenses in two astronomical telescopes having identical eyepieces. What is the ratio of their resolving power? Which telescope will you prefer and why? Give reason. 

    Solution

    Resolving power is given by, R = fraction numerator A over denominator 122 space lambda end fraction ; where A is the aperture. 
    therefore space space space space space space space space R subscript 1 over R subscript 2 equals A subscript 1 over A subscript 2
    Magnification of telescope is given by, m = f subscript o over f subscript e

    m is same for both. 
    Inorder to view the finer details of the object we use telescope of high resolving power.

    Therefore, telescope having convex lens aperture A1 is used

    Question 852
    CBSEENPH12039104

    Draw the output waveform at X, using the given inputs A and B for the logic circuit shown below. Also, identify the logic operation performed by this circuit.   


    Solution

    From the waveform given, we can say that 
    Y space equals stack A plus B with bar on top space equals fraction numerator top enclose A. top enclose B over denominator left parenthesis A with bar on top. B with bar on top right parenthesis plus A with bar on top. B with bar on top end fraction space equals top enclose A with bar on top. space top enclose B end enclose space equals space top enclose top enclose A end enclose plus top enclose top enclose B end enclose space equals space A plus B
    which is the Boolean expression of OR.

    The output waveform for OR gate is given by, 

    Question 853
    CBSEENPH12039105

    Name the semiconductor device that can be used to regulate an unregulated dc power supply. With the help of I-V characteristics of this device, explain its working principle.

    Solution

    Zener diode can be used to regulate an unregulated dc power supply. 
     

    Working principle of Zener diode as per the V-I characteristics:

    In reverse breakdown region or zener region, a very small change in voltage across the zener diode produces very large change in current through the circuit but the voltage across the zener remains constant.

    Question 854
    CBSEENPH12039107

    Draw the transfer characteristic curve of a base biased transistor in CE configuration. Explain clearly how the active region of the V0 versus Vi curve in a transistor is used as an amplifier. 

    Solution

    The transfer characteristic curve of a base biased transistor in CE configuration is shown below: 

    In the active region, a small increase of input voltage (Vi)results in a large increase in IC. The gradual increase in current is a linear phenomenon. This results in an increase in the voltage drop across RC

    Question 855
    CBSEENPH12039108

    (i) Define modulation index.

    (ii) Why is the amplitude of modulating signal kept less than the amplitude of carrier wave?

    Solution

    i) The ratio of the amplitude of modulating signal (Em) to the amplitude of carrier wave (Ec) is known as the modulation index of an amplitude modulated wave or amplitude modulation index.

    Mathematically it is given by, 
    m subscript a space equals space E subscript m over E subscript c

    For a modulated wave, we have 
    m subscript a space equals space fraction numerator E subscript m a x end subscript minus E subscript m i n end subscript over denominator E subscript m a x end subscript plus E subscript m i n end subscript end fraction

E subscript m space less than space E subscript c

    ii) Keeping the amplitude of modulating signal less than the amplitude of carrier wave helps one to reduce the distortions in the signal.

    Question 856
    CBSEENPH12039112

    An electron and a photon each have a wavelength 1.00 nm. Find

    (i) their momenta,

    (ii) the energy of the photon and

    (iii) the kinetic energy of electron.

    Solution

    Given, wavelength,lambda space equals space 1 space n m space equals space 1 cross times 10 to the power of negative 9 space end exponent m
    i) Momenta of electron = momenta of photon.
    Therefore,
     Error converting from MathML to accessible text.
    ii) Energy of photon, E = h nu space equals space h c over lambda equals h over lambda c space equals space p c
    Error converting from MathML to accessible text. 
    iii) Kinetic energy of electron, straight E subscript straight k space equals 1 half m subscript e v squared space equals fraction numerator p squared over denominator 2 m subscript e end fraction
                                                   Error converting from MathML to accessible text.

    Question 857
    CBSEENPH12039113

    Draw a schematic diagram showing the (i) ground wave (ii) sky wave and (iii) space wave propagation modes for EM waves.

    Write the frequency range for each of the following:

    (i) Standard AM broadcast

    (ii) Television

    (iii) Satellite communication

    Solution

    The diagram below illustrates the various modes of propagation for EM waves:
     

    i) Standard AM broadcast used frequency of range 540-1600 kHz

    ii) A frequency range of 54–890 MHz is used by television sets.

    iii) Satellite communication uses 5.925–6.425 GHz as uplink frequency and 3.7–4.2 GHz downlink frequency. 

    Question 858
    CBSEENPH12039114

    Describe Young's double slit experiment to produce interference pattern due to a monochromatic source of light. Deduce the expression for the fringe width.

    Solution

    Conditions for Young’s double slit experiment are:

    (i) The sources should be monochromatic and originating from common single source.

    (ii) The amplitudes of the waves should be equal.

    Let S1 and S2 be two coherent sources separated by a distance d.

    Let the distance of the screen from the coherent sources be D. Let point M be the foot of the perpendicular drawn from O, which is the midpoint of S1 and S2 on the screen. Obviously point M is equidistant from S1 and S2. Therefore the path difference between the two waves at point M is zero. Thus the point M has the maximum intensity.

    Now, Consider a point P on the screen at a distance y from M. Draw S1N perpendicular from S1 on S2 P. 

    The path difference between two waves reaching at P from S1 and S2 is given by, 
    increment straight space equals straight space straight S subscript 2 straight P minus straight S subscript 1 straight P straight space almost equal to straight space straight S subscript 2 straight N 
    Since, D >> d, s o italic comma italic space angle S subscript 2 S subscript 1 N space equals space theta italic space i s italic space v e r y italic space s m a l l italic. italic space
    Error converting from MathML to accessible text.

    Expression for Fringe Width:

    Distance between any two consecutive bright fringes or any two consecutive dark fringes are called the fringe width. It is denoted by straight omega
    Let, y subscript n plus 1 end subscript space a n d space y subscript n be the distance of two consecutive fringes. Then, we have
    y subscript n plus 1 end subscript space equals space left parenthesis n plus 1 right parenthesis fraction numerator D lambda over denominator d end fraction a n d space space y subscript n equals fraction numerator n D lambda over denominator d end fraction
    So, fringe width is equals space y subscript n plus 1 end subscript minus space space y subscript n space end subscript equals space left parenthesis n plus 1 right parenthesis fraction numerator D lambda over denominator d end fraction minus fraction numerator n D lambda over denominator d end fraction equals fraction numerator D lambda over denominator d end fraction
    Fringe width is same for both bright and dark fringe. 

    Question 859
    CBSEENPH12039115

    Use Huygens principle to verify the laws of refraction.

    Solution

    Proof of Snell’s law of Refraction using Huygens wave theory is: 

    As seen in the fig. above let XY be a surface separating the two media ‘1’ and ‘2’. Let v1 and v2 be the speeds of waves in these media.

    A plane wavefront AB in the first medium is incident obliquely on the boundary surface XY and its end A touches the surface at A at time t = 0 while the other end B reaches the surface at point B after time-interval t.

    Here, BB apostrophe space equals space straight v subscript 1 straight t

    As the wavefront AB advances, it strikes the points between A and B¢ of boundary surface.

    According to Huygens principle, secondary spherical wavelets emanate from these points, which travel with speed v1 in the first medium and speed v2 in the second medium.

    Secondary wavelet starting from A, traverses a distance AA’ = v2t in second medium in time t. In the same time, point of wavefront traverses a distance in first medium and reaches B’, from where the secondary wavelet starts. 

    So, BB apostrophe space equals space straight v subscript 1 straight t  and AA’ = v2t. 
    Assuming A as centre, we draw a spherical arc of radius AA’ (= v2t) and draw tangent B’A’ on this arc from B’. As the incident wavefront AB advances, the secondary wavelets start from points between A and B’, one after the other and will touch A’B’ simultaneously. 

    According to Huygens principle A’B’ is the new position of wavefront AB in the second medium. Hence A’B’ will be the refracted wavefront.

    First law: As AB, A’B’ and surface XY are in the plane of paper, therefore the perpendicular drawn on them will be in the same plane. As the lines drawn normal to wavefront denote the rays, therefore we may say that the incident ray, refracted ray and the normal at the point of incidence all lie in the same plane.

    This is the first law of refraction.

    Second law: Let the angle made by incident wavefront be i and angle made by the refracted wavefront A’B’ be r.

    In increment space AB apostrophe straight B
    angle ABB apostrophe space equals space 90 to the power of 0 
    therefore space space space space space sin straight space straight i space equals space sin space angle BAB apostrophe 
                                     fraction numerator BB apostrophe over denominator AB apostrophe end fraction equals space fraction numerator straight v subscript 1 straight t over denominator AB apostrophe end fraction italic space italic space italic space italic space italic space italic space italic space italic space                    ... (1)

    Similarly, in right-angled triangle,  <AA'B,
                                       angle AA apostrophe straight B apostrophe space equals space 90 to the power of straight o
    Therefore, 
                                  sin space straight i space equals space sin space space angle space AB apostrophe straight A apostrophe space 
                                        fraction numerator AA apostrophe over denominator AB apostrophe end fraction equals fraction numerator straight v subscript 2 straight t over denominator AB apostrophe end fraction space space space space space space space space space space space space space space space space space space space space space space space space space space space space space... space left parenthesis 2 right parenthesis

    Now, dividing equation (1) by (2), we have 
    sini over sinr space equals space straight v subscript 1 over straight v subscript 2 space equals space constant
    The ratio of sine of angle of incidence and the sine of angle of refraction is a constant and is equal to the ratio of velocities of waves in the two media. This is the second law of refraction, and is called the Snell’s law.

    Question 860
    CBSEENPH12039116

    (a) Describe briefly, with the help of suitable diagram, how the transverse nature of light can be demonstrated by the phenomenon of polarization.

    (b) When unpolarized light passes from air to a transparent medium, under what condition does the reflected light get polarized?

    Solution
    a) Light from a source S is allowed to fall normally on the flat surface of a thin plate of a tourmaline crystal, cut parallel to its axis. Only a part of this light is transmitted through A. If now the plate A is rotated, the character of transmitted light remains unchanged. Now another similar plate B is placed at some distance from A such that the axis of B is parallel to that of A. If the light transmitted through A is passed through B, the light is almost completely transmitted through B and no change is observed in the light coming out of B.


    If now the crystal A is kept fixed and B is gradually rotated in its own plane, the intensity of light emerging out of B decreases and becomes zero when the axis of B is perpendicular to that of A. If B is further rotated, the intensity begins to increase and becomes maximum when the axes of A and B are again parallel. Thus, we see that the intensity of light transmitted through B is maximum when axes of A and B are parallel and minimum when they are at right angles. From this experiment, it is obvious that light waves are transverse and not longitudinal; because, if they were longitudinal, the rotation of crystal B would not produce any change in the intensity of light.

    b) When reflected and refracted rays are perpendicular to each other then, the reflected ray is totally plane polarized.

    Question 861
    CBSEENPH12039117

    The energy levels of a hypothetical atom are shown below. Which of the shown transitions will result in the emission of a photon of wavelength 275 nm?

    Which of these transitions correspond to emission of radiation of (i) maximum and (ii) minimum wavelength? 


    Solution

    Given, wavelength of the photon, straight lambda = 275 nm

    Energy of the photon is given by,
    Error converting from MathML to accessible text. 

    This corresponds to transition B as from the figure.

    i)   increment straight E space equals space hc over straight lambda space rightwards double arrow space straight lambda space equals space fraction numerator hc over denominator increment straight E end fraction 
    For maximum wavelength  should be minimum.
    Minimum energy corresponds to transition A.

    ii) For minimum wavelength,  should be maximum. Maximum energy corresponds to transition D.

    Question 862
    CBSEENPH12039118

    State the law of radioactive decay.

    Plot a graph showing the number (N) of undecayed nuclei as a function of time (t) for a given radioactive sample having half-life T½.

    Depict in the plot the number of undecayed nuclei at (i) t = 3 T½ and (ii) t = 5 T½.

    Solution

    Law of radioactive decay states that, the number of nuclei undergoing decay per unit time, at any instant, is proportional to the total number of nuclei present in the sample at that instant.
     
    Number of undecayed nuclei at t = 3T1/2 is fraction numerator straight N subscript straight o over denominator space 8 end fraction
    And, at t = 5T1/2  the number of undecayed nuclei is straight N subscript straight o over 32

    Question 863
    CBSEENPH12039122

    (a) Draw a ray diagram to show refraction of a ray of monochromatic light passing through a glass prism.

    Deduce the expression for the refractive index of glass in terms of angle of prism and angle of minimum deviation.

    (b) Explain briefly how the phenomenon of total internal reflection is used in fiber optics.

    Solution

    a) The phenomenon of refraction for a ray of monochromatic light passing through a glass prism is shown as below: 

    Let, PQR be the principal section of the prism.
    The refracting angle of prism is A. Monochromatic light EF is incident on face PQ at angle of incidence i1. This ray enters from a rarer to denser medium and hence is refracted towards the normal FN. Refracted ray is FG. Angle of refraction for this face is r1. Refracted ray FG becomes incident on face PR and is refracted away from the normal GN2 and emerges in the direction GH. The angle of incidence on this face is r2 (into prism) and angle of refraction (into air) is i2. At point O, incident and the emergent ray meet. The angle between these two rays is called the angle of deviation ‘straight delta’. 
    angle OFG space equals straight i subscript 1 space minus space straight r subscript 1 space space and space angle OGF space equals space straight i subscript 2 space minus space straight r subscript 2
    increment F O G comma space delta space i s space t h e space e x t e r i o r space a n g l e.
    delta space equals space angle O F G plus angle O G F space

italic space italic space equals space left parenthesis i subscript 1 space minus space r subscript 1 right parenthesis plus left parenthesis i subscript 2 space minus space r subscript 2 right parenthesis space equals space left parenthesis i subscript 1 plus i subscript 2 right parenthesis minus left parenthesis r subscript 1 plus r subscript 2 right parenthesis                    ... (1) 

    The normal FN1 and GN2 on faces PQ and PR respectively, when produced meet at N.
    Let, angle space F N G space equals space theta
    r subscript 1 space plus space r subscript 2 space plus theta space equals space 180 to the power of o                              ... (2) 
    I n space q u a d r i l a t e r a l space P F N G comma space angle P F N space equals space 90 to the power of o

therefore space A plus space 90 degree plus theta plus 90 degree space equals space 360 degree

space italic space italic space italic space A plus theta space equals space 180 degree space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space... space left parenthesis 3 right parenthesis

Comparing space equations space left parenthesis 2 right parenthesis space and space left parenthesis 3 right parenthesis comma space we space get space

straight r subscript 1 space end subscript plus space straight r subscript 2 space end subscript equals space straight A space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space... space left parenthesis 4 right parenthesis space space space space space space space space space space space space space space
Putting space this space in space equation space left parenthesis 1 right parenthesis comma space we space get

delta space equals space i subscript 1 plus i subscript 2 space minus space A italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space space space... space left parenthesis 5 right parenthesis space space space

rightwards double arrow space i subscript 1 plus i subscript 2 space equals space A plus delta italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space... space left parenthesis 6 right parenthesis

Now comma space using space Snell ’ straight s space law comma space we space get

n space equals space fraction numerator sin i subscript 1 over denominator sin r subscript 1 end fraction equals fraction numerator sin i subscript 2 over denominator sin r subscript 2 end fraction space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space... space left parenthesis 7 right parenthesis space
    We can see that, for one angle of deviation we have two angles of incidence. But, angle of deviation is minimum for only one particular angle if incidence. Angle of minimum deviation is denoted by delta subscript m.

    So let,                            i1 = i2 = i

    And                               r1 = r2 = r

    Therefore, we have (4) and (6), we have
    space space space space space straight r plus straight r space equals space straight A space space

rightwards double arrow space r space equals space bevelled A over 2 a n d space i plus i equals space A plus delta subscript m

rightwards double arrow space i equals fraction numerator A italic plus delta subscript m over denominator italic 2 end fraction 
    Error converting from MathML to accessible text.

    b) An optical fiber is a device based on total internal reflection by which a light signal may be transmitted from one place to another with a negligible loss of energy. When a light ray is incident on one end at a small angle of incidence, it suffers refraction from air to quartz and strikes the quartz-coating interface at an angle more than the critical angle. Hence, total internal reflection happens and the ray of light strikes the opposite face again at an angle greater than critical angle. The phenomenon of total internal reflection takes place. Thus the ray within the fiber suffers multiple total internal reflections and finally strikes the other end at an angle less than critical angle for quartz-air interface and emerges in air.

    Question 864
    CBSEENPH12039123

    (a) Obtain lens makers formula using the expression

     n subscript 2 over v minus n subscript 1 over u equals fraction numerator left parenthesis n subscript 2 minus n subscript 1 right parenthesis over denominator R end fraction

    Here the ray of light propagating from a rarer medium of refractive index (n1) to a denser medium of refractive index (n2) is incident on the convex side of spherical refracting surface of radius of curvature R.

    (b) Draw a ray diagram to show the image formation by a concave mirror when the object is kept between its focus and the pole. Using this diagram, derive the magnification formula for the image formed.

    Solution

    Len’s Makers formula:

    Consider a thick lens L. The refractive index of the material of lens is n2. The lens is placed in a medium of refractive index n1. R1 and R2 is the radius of curvature of the lens and poles are represented by P1 and P2. Thickness of the lens is given by t. O is a point object which is placed on the principal axis of the lens.

    Object distance from pole P1 is u.

    Image formed is at a distance of v’ from P1.
    Now, using the refraction formula at spherical surface, we have 
    fraction numerator straight n subscript 2 over denominator straight v straight apostrophe end fraction minus straight n subscript 1 over straight u equals fraction numerator straight n subscript 2 straight space minus straight space straight n subscript 1 over denominator straight R end fraction                                                 ... (1)

    Image I’ acts as a virtual object for second surface and after refraction at second surface, final image is formed at I.

    Distance of I from pole P2 of second surface is v.

    Distance of virtual object I’ from pole P2 is (v’ – t).
    For refraction at second surface, the ray is going from second medium (refractive index n2) to first medium (refractive index n1), therefore from refraction formula at spherical surface.
    i.e.,  n subscript 1 over v minus fraction numerator n subscript 2 over denominator left parenthesis v apostrophe minus t right parenthesis end fraction equals fraction numerator n subscript 1 space minus space n subscript 2 over denominator R subscript 2 end fraction

    Thickness of the lens is negligibly small as compared to v’. 
    Therefore, 
    n subscript 1 over v minus fraction numerator n subscript 2 over denominator left parenthesis v apostrophe right parenthesis end fraction equals negative fraction numerator n subscript 2 space minus space n subscript 1 over denominator R subscript 2 end fraction                              ... (2)

    Now, adding equations (1) and (2), we have 
    Error converting from MathML to accessible text.

    Now, using the lens formula, we get 
    Error converting from MathML to accessible text.
    Error converting from MathML to accessible text. is the required Lens maker’s formula. 

    b) Ray diagram for the image formation of an object between focus (F) and pole (P) of a concave mirror is given by,

    Magnification, m =fraction numerator Size straight space of straight space image left parenthesis straight A straight apostrophe straight B straight apostrophe right parenthesis over denominator Size straight space of straight space object straight space left parenthesis AB right parenthesis end fraction 
    From fig. angle space A P B space equals space angle B P Q space equals space i
    Also, angle space A P B space equals space angle B P Q space equals space i
    I n space increment A P B comma space tan space i space equals space fraction numerator A B over denominator B P end fraction italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic. italic. italic. italic space italic left parenthesis italic 1 italic right parenthesis
I n space increment A apostrophe P B apostrophe comma space tan space i space equals fraction numerator A apostrophe B apostrophe over denominator B apostrophe P end fraction space space space space space space space space space space space space space space space space space space space space space... space left parenthesis 2 right parenthesis thin space
N o w italic comma italic space f r o m italic space e q u a t i o n italic space italic left parenthesis italic 1 italic right parenthesis italic space a n d italic space italic left parenthesis italic 2 italic right parenthesis italic comma italic space w e italic space h a v e

fraction numerator A B over denominator B P end fraction equals fraction numerator A apostrophe B apostrophe over denominator B apostrophe P end fraction

rightwards double arrow space Magnification comma space fraction numerator A apostrophe B apostrophe over denominator A B end fraction equals fraction numerator B apostrophe P over denominator B P end fraction

straight i. straight e. comma space straight m space equals negative straight v over straight u
So comma space straight m space equals space minus straight v over straight u
Hence comma space proved. space

    Question 865
    CBSEENPH12039128

    Which of the following waves can be polarized (i) Heat waves (ii) Sound waves?

    Solution

    i) Heat waves can be polarized because they are transverse and electromagnetic in nature.

    ii) Sound waves are longitudinal in nature and hence, cannot be polarized.

    Question 866
    CBSEENPH12039130

    Write the relationship between angle of incidence ‘i’, prism ‘A’ and angle of minimum deviation for a triangular prism. 

    Solution

    The relationship between i, A and straight delta subscript straight m for a triangular prism is given by, 
                                               straight i space equals fraction numerator straight A plus space straight delta subscript straight m over denominator 2 end fraction

    Question 867
    CBSEENPH12039131

    The given graph shows the variation of photo-electric current (I) versus applied voltage (V) for two different photosensitive materials and for two different intensities of the incident radiation. Identify the pairs of curves that correspond to different materials but same intensity of incident radiation. 


    Solution

    The pair of curves (1, 3) and (2, 4) corresponds to different materials but having same intensity of incident radiation. The value of stopping potential for the curves (1, 2) and (3, 4) is same implying that they correspond to similar materials. 

    Question 868
    CBSEENPH12039134

    (a) Write the necessary conditions for the phenomenon of total internal reflections to occur.

    (b) Write the relation between the refractive index and critical angle for a given pair of optical media.

    Solution

    a) Conditions for total internal reflection to take place:

    i) Light ray must travel from denser medium into rarer medium.

    ii) The angle of incidence in denser medium must be greater than the critical angle for given pair of optical media. 

    b) Relation between refractive index and critical angle for a given pair is,
        As per Snell’s law, 
    fraction numerator sini subscript straight c over denominator sin 90 to the power of straight o end fraction equals n subscript 21 space equals space n subscript 1 over n subscript 2 italic space

therefore space space space space space space space space sin i subscript c space equals space n subscript italic 1 over n subscript italic 2 

    Question 869
    CBSEENPH12039138

    In the given circuit diagram, a voltmeter ‘V’ is connected across a lamp ‘L’. How would (i) the brightness of the lamp and (ii) voltmeter reading ‘V’ be affected, if the value of resistance ‘R’ is decreased? Justify your answer.    


        

    Solution

    The given figure is a Common Emitter configuration of an npn transistor. Input circuit is forward biased and collector circuit is reverse biased.

    i)
    If the value of the resistance R is reduced, the current in the forward biased input circuit increases. The emitter current IE and the collector current IC (= IE – IB) both increase. Hence, the brightness of the lamp increases.
    ii) 
    Due to increase in IC, the potential drop across lamp L increases and hence the voltmeter reading V increases.

    Question 870
    CBSEENPH12039140

    Block diagram of a receiver is shown in the figure:



    (a) Identify ‘X’ and ‘Y’.

    (b) Write their functions.

    Solution

    a) X represents Intermediate frequency stage and Y represents amplifier.

    b) IF stage changes the electromagnetic wave of high frequency to a lower frequency for further detection in detector.

    Function of amplifier is to enhance the power of the signals upto a required level.

    Question 871
    CBSEENPH12039141

    Explain, with the help of a circuit diagram, the working of a photo-diode. Write briefly how it is used to detect the optical signals. 

    OR

    Mention the important considerations required while fabricating a p-n junction diode to be used as a Light Emitting Diode (LED). What should be the order of band gap of an LED if it is required to emit light in the visible range?              

    Solution

    In any diode, an electric field ‘E’ exists across the junction from n-side to p-side, when light with energy h greater than energy gap Eg illuminates the junction. Then electron-hole pairs are generated due to absorption of photons, in or near the depletion region of the diode. Due to existing electric field, electrons and holes get separated. The free electrons are collected on n-side and holes are collected on p-side, giving rise to an emf.

    Due to this generated emf, an electric current of straight muA order flows through the external resistance.

    The figure above is the circuit diagram of photodiode.

    Detection of optical signals:

    Photodiode can be used to detect optical signals if we observe the change in current with change in light intensity when a reverse bias is applied.
                                                             OR

    Important considerations in the fabrication of LED:

    i) LED is heavily doped p-n junction.

    ii) Reverse breakdown voltage of LED’s are very low, typically around 5 V.

    The order of band gap of an LED to emit light in the visible range is about 3 eV to 1.8 eV.

    Question 872
    CBSEENPH12039142

    Write three important factors which justify the need of modulating a message signal. Show diagrammatically how an amplitude modulate wave is obtained when a modulating signal is superimposed on a carrier wave.    

    Solution

    Three factors for the need of modulating a message signal:

    a) Size of the antenna or aerial should be straight lambda/4.

    b) Effective power radiated by an antenna should be close to Error converting from MathML to accessible text.
    c) Interference of signals from different transmitters. Inorder to avoid the interference of the signals, high frequency is required which can be acquired by modulation. 

    Question 873
    CBSEENPH12039144

    a) In a typical nuclear reaction, e.g. , Error converting from MathML to accessible text.

    Although number of nucleons is conserved, yet energy is released. How? Explain.

    b) Show that nuclear density in a given nucleus is independent of mass number A.

    Solution

    a) 
    In a nuclear reaction, 

                               Error converting from MathML to accessible text.

    In a nuclear reaction, the sum of the masses of the of the target nucleus and the bombarding particle may be greater or less than the sum of masses of the product nucleus and the outgoing particle. Therefore, from the law of conservation of mass-energy around 3.27 MeV is evolved or involved in a nuclear reaction. This energy is called the Q-value of the nuclear reaction.

    Cause of the energy released:

    i) Binding energy per nucleon of  becomes more than the BE/A of H presubscript 1 presuperscript 2 
    ii) Mass defect between the reactant and the product nuclei.

    b) The radius of nucleus of mass number A is given by R = R subscript o A to the power of bevelled 1 third end exponent
    Volume of the nucleus, V space equals space 4 over 3 pi R cubed space equals 4 over 3 pi R subscript o cubed space A 
    Density of the matter in the nucleus is given by, 
                                  straight rho space equals space space Mass divided by Volume

space space space equals fraction numerator A left parenthesis u right parenthesis over denominator 4 over 3 pi R subscript o cubed A end fraction
space space space equals fraction numerator 1 over denominator 4 over 3 pi R subscript o cubed end fraction

space space space space equals fraction numerator 3 over denominator 4 πR subscript straight o cubed end fraction 
    Hence, density is independent of mass number A.

    Question 874
    CBSEENPH12039145

    (a) Why photoelectric effect cannot be explained on the basis of wave nature of light? Give reasons.

    (b) Write the basis features of photon picture of electromagnetic radiation on which Einstein’s photoelectric equation is based. 

    Solution

    a) Wave theory of light cannot explain the photoelectric effect because of the following reasons:

    i) Wave nature does not explain the instantaneous ejection of photoelectrons.

    ii) It does not explain to us the threshold frequency for a metal surface.

    iii) Wave nature do not tell us, why kinetic energy of the emitted electrons is independent of the intensity of light and depends upon its frequency.

    Basic features of photon picture of electromagnetic radiation on which Einstein’s photoelectric equation is based upon is: 

    b) Features of photons:

    i) Photons are particles of light having energy, E = hν and momentum, p = h over lambda where h is Planck constant.

    ii) Photons travel with the speed of light in vacuum, independent of the frame of reference.

    iii) Intensity of light depends on the number of photons crossing unit area in a unit time.

    Question 875
    CBSEENPH12039147

    Output characteristics of an n-p-n transistor in CE configuration is shown in the figure. Determine:

    (a) Dynamic output resistance

    (b) DC current gain and

    (c) AC current gain at an operating point VCE=10V, when IB=30 straight muA.        


    Solution

    Dynamic output resistance is given by,

     Error converting from MathML to accessible text.

    For IB = 30 straight muA,  = (12-8) = 4V and  = (3.6-3.4) = 0.2 mA

    Therefore, output resistance, Error converting from MathML to accessible text. 

     ii) dc current gain is given by, beta subscript d c end subscript space equals space I subscript c over I subscript B

    At  = 10 V and Ib = 30 straight muA

    Ic = 3.5 mA
    beta subscript d c end subscript= Error converting from MathML to accessible text. = 117

    iii) AC current gain is given by,  beta subscript a c end subscript space equals space fraction numerator increment I subscript c over denominator increment I subscript B end fraction

     At VCE = 10 V, = (3.5 -2.5) mA = 1 mA and 

     increment I subscript B italic space italic equals italic left parenthesis italic 30 italic space italic minus italic space italic 20 italic right parenthesis italic space mu italic space A italic space italic equals italic space italic 10 italic space mu A= (30 -20) A = 10 A
    therefore space space space space space beta subscript a c end subscript space equals space 1 over 10 space equals 100

    Question 876
    CBSEENPH12039148

    Using Bohr’s postulates, obtain the expression for the total energy of the electron in the stationary states of the hydrogen atom. Hence draw the energy level diagram showing how the line spectra corresponding to Balmer series occur due to transition between energy levels.

    Solution

    According to Bohr’s postulates, in a hydrogen atom, a single electron revolves around a nucleus of charge +e. For an electron moving with a uniform speed in a circular orbit on a given radius, the centripetal force is provided by the Coulomb force of attraction between the electron and the nucleus.

    Therefore, 
    fraction numerator m v squared over denominator r end fraction space equals space fraction numerator 1 space left parenthesis Z e right parenthesis space left parenthesis e right parenthesis over denominator 4 pi epsilon subscript o r squared end fraction                        ... (1)
    rightwards double arrow m v squared space equals fraction numerator 1 space over denominator 4 pi epsilon subscript o end fraction fraction numerator Z e squared over denominator r end fraction

So comma space
Kinetic space energy comma space straight K. straight E. space equals space 1 half m v squared
K. E equals fraction numerator italic 1 over denominator italic 4 pi epsilon subscript o end fraction fraction numerator Z e to the power of italic 2 over denominator r end fraction 
    Potential energy is given by, P.E = fraction numerator 1 over denominator 4 pi epsilon subscript o end fraction fraction numerator left parenthesis Z e right parenthesis space left parenthesis negative e right parenthesis over denominator r end fraction space equals space fraction numerator 1 over denominator 4 pi epsilon subscript o end fraction fraction numerator left parenthesis Z e right parenthesis space left parenthesis negative e right parenthesis over denominator r end fraction
    Therefore, total energy is given by, E = K.E + P.E = Error converting from MathML to accessible text.
    E = negative fraction numerator 1 space over denominator 4 pi epsilon subscript o end fraction fraction numerator Z e squared over denominator 2 r end fraction comma space is space the space total space energy.

    For nth orbit, E can be written as En
    straight E subscript straight n space equals negative space fraction numerator 1 over denominator 4 πε subscript straight o end fraction fraction numerator Ze squared over denominator 2 straight r subscript straight n end fraction                           ... (2)
    Now, using Bohr's postulate for quantization of angular momentum, we have
    mvr space equals space fraction numerator nh over denominator 2 straight pi end fraction
    rightwards double arrow straight v space equals space fraction numerator nh over denominator 2 πmr end fraction

    Putting this value of v in equation (1), we get
    Error converting from MathML to accessible text. 

    Question 877
    CBSEENPH12039149

    (a) In what way is diffraction from each slit related to the interference pattern in a double slit experiment?

    (b) Two wavelength of sodium light 590 nm and 596 nm are used, in turn, to study the diffraction taking place at a single slit of aperture 2 x 10-4 m. The distance between the slit and the screen is 1.5.m. Calculate the separation between the positions of the first maxima of the diffraction pattern obtained in the two cases.               

    Solution

    = (a) When a plane wavefront of monochromatic light illuminates, the slit LN, each point in the slit LN becomes the source of secondary wavelets.

    The secondary wavelets originating from different points superpose on each, while travelling towards the point C and point P; at angle q. However the superposition of the secondary wavelets produces a diffraction pattern of varying intensity, as shown in fig.

    b) For maxima other than central maxima, 
    Error converting from MathML to accessible text.
    For light of wavelength, straight lambda subscript 1 = 590 nm
    Error converting from MathML to accessible text.

    Question 878
    CBSEENPH12039152

    (a) Draw a ray diagram showing the image formation by a compound microscope.

    Hence obtain expression for total magnification when the image is formed at infinity.

    (b) Distinguish between myopia and hypermetropia. Show diagrammatically how these defects can be corrected.

    OR

    State Huygens principle. Using this principle draw a diagram to show how a plane wave front incident at the interface of the two media gets refracted when it propagates from a rarer to a denser medium. Hence verify Snell’s law of refraction.

    (b) When monochromatic light travels from a rarer to a denser medium, explain the following, giving reasons:

    (i) Is the frequency of reflected and reflected light same as the frequency of incident light?

    (ii) Does the decrease in speed imply a reduction in the energy carried by light wave?

    Solution

    a) The fig. below shows the formation of image by a compound microscope.
     

    If the object AB is very close to the focus of the objective lens of focal length fo, then magnification Mo by the objective lens is given by, 
    Error converting from MathML to accessible text.

    b) Difference between myopia and hypermetropia,

    Myopia

    Hypermetropia

    1. The eye ball is elongated.

    1. The eye ball is shortened

     2. Person cannot see distant objects clearly.

     2. Person cannot see near objects clearly.

     

    A concave lens is used for the correction of myopic eye.

    Hypermetropia is corrected using a convex lens.

    OR

     

    a) Law of Reflection: Let XY is a reflecting surface at which a wavefront is being incident obliquely. Let v be the speed of the wavefront and at time t = 0, the wavefront touches the surface XY at A. After time t, the point B of wavefront reaches the point B¢ of the surface. According to Huygens principle each point of wavefront acts as a source of secondary waves. When the point A of wavefront strikes the reflecting surface, then due to presence of reflecting surface, it cannot advance further; but the secondary wavelet originating from point A begins to spread in all directions in the first medium with speed v. As the wavefront AB advances further, its points A1, A2, A3… etc. strike the reflecting surface successively and send spherical secondary wavelets in the first medium. 
                                 

    First of all the secondary wavelet starts from point A and traverses distance AA (= vt) in first medium in time t. In the same time t, the point B of wavefront, after travelling a distance BB’, reaches point B’ (of the surface), from where the secondary wavelet now starts. Now taking A as centre we draw a spherical arc of radius AA’ (= vt) and draw tangent A’B’ on this arc from point B’. As the incident wavefront AB advances, the secondary wavelets starting from points between A and B’, one after the other and will touch A’B’ simultaneously. According to Huygens principle wavefront A’B’ represents the new position of AB, i.e., A’B’ is the reflected wavefront corresponding to incident wavefront AB. 

    Now, in right-angled  ABB’ and AA’B’

     angle ABB apostrophe space equals space angle AA apostrophe straight B apostrophe
side space BB apostrophe space equals space side space AA apostrophe space

straight i. straight e. comma space both space triangles space are space congruent.
therefore space space space space space space space space space space space space space space space space space space space space space space angle BAB apostrophe space equals space angle AB apostrophe straight A apostrophe 

    i.e., incident wavefront AB and reflected wavefront A¢ B¢ make equal angles with the reflecting surface XY. As the rays are always normal to the wavefront, therefore the incident and the reflected rays make equal angles with the normal drawn on the surface XY.

    i.e., angle of incidence i = angle of reflection r

     

    This is the second law of reflection.

    b)  (i) If the radiation of certain frequency interact with the atoms/molecules of the matter, they start to vibrate with the same frequency under forced oscillations.

    Thus, the frequency of the scattered light (under reflection and refraction) equals to the frequency of incident radiation.

    (ii) No, energy carried by the wave depends on the amplitude of the wave, but not on the speed of the wave.

    Question 879
    CBSEENPH12039156

    What is the function of a 'Repeater' used in communication system?

    Solution

    Repeater is used to increase the range of the transmission in communication systems with the help of a set of receiver and transmitter.

    Question 880
    CBSEENPH12039157

    The line AB in the ray diagram represents a lens State whether the lens is convex or concave.


     

    Solution

    We can see that the lens slightly diverges the path of refracted light. Hence, the lens is concave in nature.

    Question 881
    CBSEENPH12039160

    How does one explain, using de Broglie hypothesis, Bohr's second postulate of quantization of orbital angular momentum? 

    Solution

    According to de-Broglie hypothesis, a stationary orbit is the one that contains an integral number of de-Broglie waves associated with the revolving electron.

    Total distance covered by electron = Circumference of the orbit =  

    For the permissible orbit,
    2 pi r subscript n italic space italic equals italic space n italic space lambda                          ... (1)

    Now, according to De-Broglie wavelength,

    lambda equals fraction numerator h over denominator m v end fraction

    Now, putting this in equation (1), we have

     2 pi r subscript n = nh over mv 
    rightwards double arrow mvn rn =  fraction numerator nh over denominator 2 straight pi end fraction; which is the required Bohr’s second postulate of quantization of orbital angular momentum.

    Question 882
    CBSEENPH12039162

    What is ground wave communication? Explain why this mode cannot be used for long distance communication using high frequencies.       

    Solution

    Ground waves travel along the surface of the earth. In ground wave propagation, a large portion of wave energy is in space near the surface of the Earth. The propagation of the wave is guided along the Earth's surface and follows the curvature of the Earth.

    High frequency wave propagation is not possible through ground waves for long-distance communication because while progressing, ground waves induce current in the ground and bend round the corner of the objects on the Earth due to which the energy of the ground waves of high frequency is almost absorbed by the surface of the Earth after travelling a small distance. Such signals are also absorbed by the obstacles (like mountains, tall buildings and trees) between the transmitter and the receiver. This loss in power of ground waves increases with the increase in frequency. Thus, ground wave communication is not suited for high frequency.

    Question 884
    CBSEENPH12039164

    A ray of light passes through an equilateral glass prism such that the angle of incidence is equal to the angle of emergence and each of these angles is equal to 3/4 of angle of prism. Find the angle of deviation.

                                                                  OR 

    Calculate the speed of light in a medium whose critical angle is 45°. Does critical angle for a given pair of media depend on the wavelength of incident light? Give reason.          

    Solution

    Given, i = e = ¾ A,                              …(1)

    where,
    A is the angle of prism.

    Angle of deviation for a ray of light in a prism is given by,
    straight delta space equals space straight i space plus space straight e space minus space straight A

Since space straight e space equals space straight i. space we space have

straight delta space equals space 2 straight i space minus space straight A

Therefore space from space eqn. space left parenthesis 1 space right parenthesis comma space we space have space

space space space space straight delta space equals space 2 space straight x space 3 over 4 space straight A space minus space straight A
rightwards double arrow space straight delta space equals space 1 half straight A
    Prism is an equilateral triangle. 
    That is A= 60o
    rightwards double arrow space delta space equals space 1 half cross times 60 space equals space 30 degree space semicolon space is space the space required space
angle space of space minimum space deviation. space


                                                              OR

    Using the snell's law we have
    mu space equals space fraction numerator 1 over denominator sin space C end fraction                                       ... (1)
    where, C is the critical angle of the medium and straight mu is the refractive index of  the medium.
    Also, mu space equals space c over nu                                     ... (2)

    Now, from equations (1) and (2), we have 
    straight c over straight nu equals straight space fraction numerator 1 over denominator sin straight space straight C end fraction
    Error converting from MathML to accessible text.
    This is the speed of the light in the medium. 
    Refractive index of a medium is inversely proportional to the wavelength of light. So, critical angle also depends upon the wavelength of incident light.

    Question 885
    CBSEENPH12039165

    Write two important considerations used while fabricating a Zener diode. Explain, with the help of a circuit diagram, the principle and working of a Zener diode as voltage regular. 

    Solution

    Important considerations while fabricating Zener diode are: 

    i) Heavily doped p and n junctions are to be used for fabricating Zener diode.

    ii) The breakdown voltage of the material must be noted down to avoid destruction of the device.

    Principle: A properly doped p–n ​junction that is supposed to work in a breakdown region is called a Zener diode. Such a junction when reverse biased shows a sudden increase in current to a high value at a certain voltage known as the breakdown voltage or the Zener voltage.

    Working: A Zener diode is connected across the fluctuating voltage source through a resistance R. A constant voltage supply is maintained across the load resistance RL.

    When the input voltage increases, the resistance of the Zener diode decreases and hence the current through the diode increases. Thus, a large voltage drop is seen across the resistance R and the output voltage across RL remains at a constant value. When the input voltage decreases, the resistance of the Zener diode increases and hence the current through the diode decreases. Only a small voltage drop takes place now across the resistance R and the output voltage at RL remains constant. Thus, we get a constant voltage in spite of the fluctuating input voltage. In this way, a Zener diode acts as a voltage regulator.

    Question 886
    CBSEENPH12039166

    Draw the necessary energy band diagrams to distinguish between conductors, semiconductors and insulators.

    How does the change in temperature affect the behaviour of these materials? Explain briefly. 

    Solution

    Energy band diagram is as given below:


    Conductors: 

    i) The valence band is completely filled and the conduction band can have two possibilities—either it is partially filled with an extremely small energy gap between the valence and conduction bands or it is empty, with the two bands overlapping each other.

    ii) On applying an even small electric field, conductors can conduct electricity.

    Insulators:

    i) For insulators, the energy gap between the conduction and valence bands is very large. Also, the conduction band is practically empty. 

    ii) When an electric field is applied across such a solid, the electrons find it difficult to acquire such a large amount of energy to reach the conduction band. Thus, the conduction band continues to be empty. That is why no current flows through insulators.

    Semiconductors:

    i) The energy band structure of semiconductors is similar to that of insulators, but in their case, the size of forbidden energy gap is much smaller than that of the insulators.

    ii) When an electric field is applied to a semiconductor, the electrons in the valence band find it comparatively easier to shift to the conduction band. So, the conductivity of semiconductors lies between the conductivity of conductors and insulators. 

    Question 887
    CBSEENPH12039167

    (a) What are the three basic units in communication systems? Write briefly the function of each of these.

    (b) Write any three applications of the Internet used in communication systems. 

    Solution

    a) A communication system consists of three basic units:

    (i) Transmitter: This unit is used for transmitting the information after modifying it to a suitable form. It basically consists of a transducer that converts signal in any physical form to electrical signal for transmission. After that, the signal is modulated to transmit over long distances.

    (ii) Communication channel: This unit carries the modulated signal from the transmitter to the receiver. Transmission lines act as a communication channel in case of telephony, whereas the free space serves the purpose of communication channel in case of the radio communication.

    (iii) Receiver: This unit consists of an antenna, which receives the signal, followed by a demodulator, an amplifier and a transducer. The demodulator demodulates the modulated signal, the amplifier boosts up its intensity and the transducer converts it back again from electrical form to the needed physical form.

    b) Application of internet used in communication system is:

    i) E-banking: Financial transactions can be made through this mode.

    ii) Internet surfing: Navigation over World Wide Web (www) from one webpage/website to another is called Internet surfing. It is an interesting way of searching and viewing information on any topic of interest.

    iii) E-commerce: This is a mode of electronic commerce by which consumers can buy the products or the services over internet.

    Question 888
    CBSEENPH12039168

    (a) Write the necessary conditions to obtain sustained interference fringes.

    (b) In Young's double slit experiment, plot a graph showing the variation of fringe width versus the distance of the screen from the plane of the slits keeping other parameters same. What information can one obtain from the slope of the curve?

    (c) What is the effect on the fringe width if the distance between the slits is reduced keeping other parameters same?

    Solution

    a) Necessary conditions for sustained interference fringes are:

    i)     Two sources must be coherent. They should emit continuous light waves of same wavelength or frequency.

    ii)    Two sources of light must be narrow.

    iii)  Sources of light must be monochromatic.

    b) Fringe width is given by:

                                           straight beta space equals space λD over straight d
    where, D is the distance between the slit and the screen.

    Fringe width and distance of screen from the slit is a linear graph.

    The slope of the curve gives is  straight lambda over straight d
    That is, when fringe width varies linearly with distance of screen from the slits, the ratio of wavelength to distance between the slits remain constant. That is why it is advised to take wavelengths of incident light nearly equal to the width of the slit.

    c) If the distance between the slits is reduced by keeping other parameters same. Then, fringe width would become broader.

    Question 889
    CBSEENPH12039170

    (a) Give two reasons to explain why reflecting telescopes are preferred over refracting type. 

    (b) Use mirror equation to show that convex mirror always produces a virtual image independent of the location of the object.         

    Solution

    a) Reflecting telescopes are preferred over refracting because of the following reasons:

    i) There is no chromatic aberration as the objective is a mirror

    ii) Spherical aberration is reduced in case of reflecting telescope by using mirror objective.

    b) Focal length is always positive for convex mirror.

    Consider an object placed on the left side of the mirror. That is u < 0.

    Now, using the mirror formula,
    1 over straight f space equals space 1 over v space plus space 1 over u

rightwards double arrow space 1 over v space equals space 1 over f minus 1 over u

    Focal length is positive and object distance is negative.

    Therefore, 
    1 over straight v greater than 0
rightwards double arrow space v space less than space 0 space

    Hence, a virtual image is always formed at the back side of a mirror. That is, image formed by a convex mirror is virtual in nature.

    Question 890
    CBSEENPH12039173

    Obtain the relation between the decay constant and half-life of a radioactive sample.

    The half-life of a certain radioactive material against straight alpha decay is 100 days. After how much time, will the undecayed fraction of the material be 6.25%?

    Solution

    In a radioactive sample, number of atoms at any instant is given by, 
    straight N space equals space straight N subscript straight o space straight e to the power of negative λt end exponent

    Now, when t = T, where T is the half-life of the sample.
    Error converting from MathML to accessible text. 

    This implies, half-life of a radioactive substance is inversely proportional to decay constant.

    Numerical: 

    We have,

    Number of undecayed nuclei left = 6.25 % = 6.25/ 100 = 1/16

    Let, t be the required time after which the undecayed fraction of the material will be 6.25%.
    therefore space N space equals space N subscript o over 16
    Error converting from MathML to accessible text.

    Question 891
    CBSEENPH12039176

    (a) Define the term 'intensity of radiation' in terms of photon picture of light.

    (b) Two monochromatic beams, one red and the other blue, have the same intensity.

    In which case:

    (i) the number of photons per unit area per second is larger,

    (ii) the maximum kinetic energy of the photoelectrons is more? Justify your answer.

    Solution

    a) The number of photons falling per unit area in unit time is defined as the intensity of radiation.

    b)

    i) Since, the two beams have the same intensity therefore, the number of photons emitted per unit are per unit time is the same.

    ii) Maximum Kinetic energy of photoelectrons is given by, straight E straight space equals straight space hν straight space – straight space straight ϕ
    We know that the frequency of blue beam is more than that of the red beam. Therefore, maximum Kinetic energy of the blue beam will be more.

    Question 892
    CBSEENPH12039179

    (a) Use Huygens' principle to show the propagation of a plane wavefront from a denser medium to a rarer medium. Hence find the ratio of the speeds of wavefront in the two media.

    (b) (i) Why does an unpolarized light incident on a polaroid get linearly polarized ?

    (ii) Derive the expression of Brewster's law when unpolarized light passing from a rarer to a denser medium gets polarized on reflection at the interface.

    Solution

    a) 


    As seen in the fig. above let XY be a surface separating the two media ‘1’ and ‘2’. Let v1 and v2 be the speeds of waves in these media.

    A plane wavefront AB in the first medium is incident obliquely on the boundary surface XY and its end A touches the surface at A at time t = 0 while the other end B reaches the surface at point B after time-interval t.

    Here, BB apostrophe space equals space straight v subscript 1 straight t.

    As the wavefront AB advances, it strikes the points between A and B’ of boundary surface.

    According to Huygens principle, secondary spherical wavelets emanate from these points, which travel with speed v1 in the first medium and speed v2 in the second medium.

    Secondary wavelet starting from A, traverses a distance AA’ = v2t in second medium in time t. In the same time, point of wavefront traverses a distance  in first medium and reaches B’, from where the secondary wavelet starts.

    So, BB' = v1 t and AA’ = v2t.

    Assuming A as centre, we draw a spherical arc of radius AA’ (= v2t) and draw tangent B’A’ on this arc from B’. As the incident wavefront AB advances, the secondary wavelets start from points between A and B’, one after the other and will touch A’B’ simultaneously. 

    According to Huygens principle A’B’ is the new position of wavefront AB in the second medium. Hence A’B’ will be the refracted wavefront.

    Let the angle made by incident wavefront be i and angle made by the refracted wavefront A’B’ be r.

    In space increment space AB apostrophe straight B comma space

space space space space space space space space space space space space space space space space space space space straight angle ABB '  equals straight space 90 to the power of 0

Hence comma space space space space space space space space space space space space space space sin straight space straight i straight space equals straight space sin  ∠ BAB ' 

space space space space space space space space space space space space space space space space space space space space space space space fraction numerator BB straight apostrophe over denominator AB straight apostrophe end fraction equals straight space fraction numerator straight v subscript 1 straight t over denominator AB straight apostrophe end fraction space space space space space space space space space space space space space space space space space space space space... space left parenthesis 1 right parenthesis thin space

Similarly comma space in space right minus angled space triangle comma space angle AA apostrophe straight B comma space
straight angle AA straight apostrophe straight B '  equals straight space 90 to the power of straight o

therefore space space space space space space space space space space space space space space space space space space sin space straight i straight space equals straight space sin    ∠  AB straight apostrophe straight A straight apostrophe

space space space space space space space space space space space space space space space space space space space space space fraction numerator AA straight apostrophe over denominator AB straight apostrophe end fraction equals fraction numerator straight v subscript 2 straight t over denominator AB straight apostrophe end fraction space space space space space space space space space space space space space space space space space space space space space space space... space left parenthesis 2 right parenthesis

Now comma space dividing space equation space left parenthesis 1 right parenthesis space by space left parenthesis 2 right parenthesis comma space we space have space

space space space space fraction numerator sin space straight i over denominator sin space straight r end fraction straight space equals straight space straight v subscript 1 over straight v subscript 2 straight space equals straight space constant

This space is space the space Snell ’ straight s space law space of space refraction.

straight lambda subscript 1 space and space straight lambda subscript 2 space represents space the space wavelength space of space light
space in space the space rarer space medium space and space denser space medium space respectively.

Then comma space

space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space straight lambda subscript 1 over straight lambda subscript 2 equals straight space straight v subscript 1 over straight v subscript 2 
    b) 

     

    Polarization of light is referred to as restricting the vibration of light in a perpendicular direction perpendicular to the direction of propagation of wave.

    The vibration of particles of light which is parallel to the axis of crystal passes through the Polaroid on passing an unpolarized light. All other vibrations are absorbed and that is why intensity of emerging light is reduced.
    The plane of vibration here is ABCD, in which the vibrations of the polarized light is confined and the plane KLMN is called plane of polarization. KLMN is perpendicular to the plane of vibration.

    Reflected light is totally polarized, when unpolarized light is incident on the glass-air interface at the Brewster angle iB. This is known as Brewster’s law.

    The reflected component OB and refracted component OC are mutually perpendicular to each other, when light is incident at Brewster’s angle.

    italic space italic space italic space italic space italic space italic space angle space B O y space plus space angle Y O C space equals space 90 to the power of o

space space space space space space left parenthesis 90 to the power of 0 space minus space i subscript B right parenthesis space plus space left parenthesis 90 to the power of 0 space plus space r right parenthesis space equals space 90 to the power of o
Now comma space using space Snell ’ straight s space law comma space we space have

space space space space space mu space equals space fraction numerator sin space i over denominator sin space r end fraction 

    i = iB and r = (900 – iB)

    Therefore, 
    mu space equals space fraction numerator sin i subscript B over denominator sin space left parenthesis 90 to the power of o space minus space i subscript B right parenthesis end fraction space equals space fraction numerator sin i subscript B over denominator cos i subscript B end fraction space equals space tan i subscript B , is the expression for Brewster’s law.

    Question 893
    CBSEENPH12039180

    A biconvex lens with its two faces of equal radius of curvature R is made of a transparent medium of refractive index straight mu1. It is kept in contact with a medium of refractive index as shown in the figure.

                                                      

    a) Find the equivalent focal length of the combination.

    b) Obtain the condition when this combination acts as a diverging lens.

    c) Draw the ray diagram for the case mu subscript 1 space greater than thin space left parenthesis mu subscript 2 space plus space 1 right parenthesis divided by 2 space comma spacewhen the object is kept far away from the lens. Point out the nature of the image formed by the system.

    Solution

    a) Using the Len’s maker’s formula, we have

     1 over straight f space equals space open parentheses mu space minus space 1 close parentheses space open square brackets fraction numerator 1 over denominator space R subscript 1 end fraction space minus space 1 over R subscript 2 close square brackets

L e t space f subscript 1 space a n d space f subscript 2 space b e space t h e space f o c a l space l e n g t h s space o f space t h e space
t w o space m e d i u m. space

1 over straight f subscript 1 space equals space open parentheses mu space minus space 1 close parentheses space open square brackets fraction numerator 1 over denominator space R end fraction space minus space open parentheses negative 1 over R subscript 2 close parentheses close square brackets

rightwards double arrow space 1 over straight f space equals space open parentheses mu space minus space 1 close parentheses open parentheses 2 over straight R close parentheses

space 1 over straight f subscript 2 space equals space open parentheses mu subscript italic 2 space minus space 1 close parentheses space open square brackets open parentheses negative fraction numerator 1 over denominator space R end fraction close parentheses space minus space 1 over infinity close square brackets

rightwards double arrow space 1 over straight f subscript 2 space equals space open parentheses mu subscript italic 2 space minus space 1 close parentheses space open parentheses negative 1 over straight R close parentheses
    Let feq is the equivalent focal length of the combination, then
    1 over f subscript e q end subscript space equals space 1 over f subscript 1 plus 1 over f subscript 2

rightwards double arrow space 1 over straight f subscript eq space equals space fraction numerator 1 space left parenthesis straight mu subscript 1 space minus space 1 right parenthesis over denominator straight R end fraction space minus space fraction numerator left parenthesis straight mu subscript 2 space minus space 1 right parenthesis over denominator straight R end fraction

rightwards double arrow space 1 over straight f subscript eq space equals space fraction numerator 2 straight mu subscript 1 space minus space straight mu subscript 2 space minus space 1 over denominator straight R end fraction

rightwards double arrow space straight f subscript eq space equals space fraction numerator straight R over denominator 2 straight mu subscript 1 space minus space straight mu subscript 2 space minus space 1 end fraction 
    b) 

    For, the combination of lenses to behave as diverging lens, equivalent focal length < 0.

     rightwards double arrow space fraction numerator R over denominator 2 mu subscript 1 space minus space mu subscript 2 minus 1 end fraction less than space 0

rightwards double arrow space space 2 straight mu subscript 1 space minus space straight mu subscript 2 space minus space 1 space less than 0

rightwards double arrow space straight mu subscript 1 space less than space fraction numerator left parenthesis straight mu subscript 2 space plus space 1 right parenthesis over denominator 2 end fraction 
    c) 
    For mu subscript 1 space greater than thin space left parenthesis mu subscript 2 space plus space 1 right parenthesis divided by 2 comma spacethe combination of lenses will behave as converging lens. An object placed far from the lens will form image at the focus of the lens.


    Image formed is real and diminished in nature.

    Question 894
    CBSEENPH12039186

    Define intensity of radiation on the basis of photon picture of light. Write its S.I. unit.        

    Solution

    The amount of light or photon energy incident per metre square per second is called the intensity of radiation. S.I unit is W/m2.

    Question 895
    CBSEENPH12039188

    Why is it found experimentally difficult to detect neutrinos in nuclear straight beta-decay? 

    Solution

    Neutrinos are chargeless, massless particles that hardly interact with matter. Hence, their detection during the experiment is very difficult.

    Question 896
    CBSEENPH12039190

    A biconvex lens made of a transparent material of refractive index 1.25 is immersed in water of refractive index 1.33. Will the lens behave as a converging or a diverging lens? Give reason. 

    Solution

    The lens will behave as a diverging lens when light rays enter from air to lens. The refractive of lens is lesser than the refractive index of the medium i.e., water. So. The lens will behave as a converging lens when light rays travel from lens to water.

    Question 897
    CBSEENPH12039191

    Using Rutherford model of the atom, derive the expression for the total energy of the electron in hydrogen atom. What is the significance of total negative energy possessed by the electron?

    OR

    Using Bohr’s postulates of the atomic model derive the expression for radius of nth electron orbit. Hence obtain the expression for Bohr’s radius. 

    Solution

    According to Rutherford’s model, we have
    mv squared over straight r space equals space fraction numerator 1 over denominator 4 pi epsilon subscript o end fraction fraction numerator z e squared over denominator r squared end fraction

rightwards double arrow space mv squared space equals space fraction numerator 1 over denominator 4 pi epsilon subscript o end fraction fraction numerator z e squared over denominator r end fraction

Therefore comma space

Total space energy space equals space straight P. straight E space plus space straight K. straight E

straight T. straight E. space equals space minus fraction numerator 1 over denominator 4 πε subscript straight o end fraction ze squared over straight r space plus space 1 half mv squared

space space space space space space space equals space minus 1 half. fraction numerator 1 over denominator 4 πε subscript straight o end fraction space ze squared over straight r

space space space space space space space equals space minus space. fraction numerator 1 over denominator 8 πε subscript straight o end fraction ze squared over straight r 
    Energy is negative implies that the electron –nucleus is a bound or attractive system.

                                                               OR

    According to the Bohr’s atomic model, electrons revolve around the nucleus only in those orbits for which the angular momentum is an integral multiple of  fraction numerator straight h over denominator 2 straight pi end fraction.
    So, as per Bohr’s postulate, we have
    mvr space equals space fraction numerator nh over denominator 2 straight pi end fraction space

Therefore comma space

mv squared over straight r space equals space fraction numerator 1 over denominator 4 πε subscript straight o end fraction ze squared over straight r squared

mvr space equals fraction numerator nh over denominator 2 straight pi end fraction

therefore space space straight m squared straight v squared straight r squared space equals space fraction numerator straight n squared straight h squared over denominator 4 straight pi squared end fraction

This space implies comma

straight r space equals space fraction numerator straight epsilon subscript straight o straight n squared straight h squared over denominator πze squared straight m end fraction 
    This is the required expression for Bohr's radius. 

    Question 898
    CBSEENPH12039195

    Explain, with the help of a circuit diagram, the working of a p-n junction diode as a half-wave rectifier. 

    Solution

    Circuit for p-n junction diode as half-wave rectifier is given below:
     

    During the positive half cycle: The p-n junction is forward biased i.e the forward current flows from p to n, the diode offers a low resistance path to the current. Thus we get output across-load i.e. a.c input will be obtained as d.c output.
    During the negative half cycle: The p-n junction is reversed biased i.e the reverse current flows from n to p, the diode offers a high resistance path to the current. Therefore, output across the load is not obtained.
    Question 899
    CBSEENPH12039197

    Two monochromatic rays of light are incident normally on the face AB of an isosceles right-angled prism ABC. The refractive indices of the glass prism for the two rays ‘1’ and ‘2’ are respectively 1.35 and 1.45. Trace the path of these rays after entering through the prism. 


    Solution

    The propagation of ray diagrams is as shown below:

    Both the rays will fall on the side AC with angle of incidence (i) equal to 45°.
    Critical angle of ray 1 is greater than that of angle of incidence. Hence, it will emerge from the prism. Critical angle of ray 2 is less than that of i. Hence, it will be internally reflected.

    Question 900
    CBSEENPH12039198

    Write the functions of the following in communication systems:

    (i) Transducer

    (ii) Repeater

    Solution

    Transducer: Any device that converts one form of energy to another.

    Repeater: A repeater accepts the signal from the transmitter amplifies and retransmits it to the receiver.

    Question 901
    CBSEENPH12039200

    Draw a circuit diagram of n-p-n transistor amplifier in CE configuration. Under what condition does the transistor act as an amplifier? 

    Solution

    The circuit diagram for n-p-n transistor in CE configuration is as shown below:
     

    The transistor acts as an amplifier when the emitter-base junction is forward biased and the collector-emitter junction is reverse biased with a high voltage VCC.

    Question 902
    CBSEENPH12039201

    (a) Using the phenomenon of polarization, show how transverse nature of light can be demonstrated.

    (b) Two Polaroid P1 and P2 are placed with their pass axes perpendicular to each other. Unpolarised light of intensity Io is incident on P1. A third Polaroid P3 is kept in between P1 and P2 such that its pass axis makes an angle of 30o with that of P1. Determine the intensity of light transmitted through P1, P2 and P3

    Solution

    a)
    i. Light from a source S is allowed to fall normally on the flat surface of a thin plate of a tourmaline crystal, cut parallel to its axis. Only a part of this light is transmitted through A.
    ii. If now the plate A is rotated, the character of transmitted light remains unchanged.
    iii. Now another similar plate B is placed at some distance from A such that the axis of B is parallel to that of A.
    iv. If the light transmitted through A is passed through B, the light is almost completely transmitted through B and no change is observed in the light coming out of B. 
     

    v. If now the crystal A is kept fixed and B is gradually rotated in its own plane, the intensity of light emerging out of B decreases and becomes zero when the axis of B is perpendicular to that of A.
    vi. If B is further rotated, the intensity begins to increase and becomes maximum when the axes of A and B are again parallel. Thus, we see that the intensity of light transmitted through B is maximum when axes of A and B are parallel and minimum when they are at right angles.
    From this experiment, it is obvious that light waves are transverse and not longitudinal; because, if they were longitudinal, the rotation of crystal B would not produce any change in the intensity of light.

    b) 

    Intensity of light transmitted through P1  = Io/2

    Intensity of light transmitted through P3 = ( Io / 2) cos 2 30o = 3 Io / 8

    Intensity of light transmitted through P2 =  3/8 Io cos2 60o = 3/32 Io

    Question 903
    CBSEENPH12039204

    A convex lens of focal length 20 cm is placed coaxially with a convex mirror of radius of curvature 20 cm. The two are kept at 15 cm apart. A point object lies 60 cm in front of the convex lens. Draw a ray diagram to show the formation of the image by the combination. Determine the nature and position of the image formed. 

    Solution

    For convex lens,

    Focal length, f = + 20 cm

    Object distance, u = - 60 cm

    Now, using the lens formula, we have
    1 over straight v minus 1 over straight u space equals space 1 over straight f 

    Putting in the values, we get

    Image distance, v = + 30 cm 

    Now, for convex mirror

    Object distance, u = + (30- 15) cm = 15 cm

    Focal length, f = + 20/2 cm = +10 cm

    Object distance, u = + (30- 15) cm = 15 cm

    Focal length, f = + 20/2 cm = +10 cm

    Now, using the mirror formula we have
    1 over straight v space plus space 1 over u space equals space 1 over f

    Putting all the values, we get

    Image distance, v = + 30 cm

    Therefore, the final image is formed at a distance of 30 cm from the convex mirror or at a distance of 45 cm from the convex lens to the right of the convex mirror.

    Therefore, the final image formed is a virtual image.

    Ray diagram for the image formation is given below:

    Question 904
    CBSEENPH12039206

    Write any two distinguishing features between conductors, semiconductors and insulators on the basis of energy band diagrams.

    Solution

    Energy band diagram is given below:

    Two distinguishing features of conductors, semiconductors and insulators are:

    Conductors: 
    i) The valence band is completely filled and the conduction band can have two possibilities—either it is partially filled with an extremely small energy gap between the valence and conduction bands or it is empty, with the two bands overlapping each other. 
    ii) On applying an even small electric field, conductors can conduct electricity. 
    Insulators: 
    i) For insulators, the energy gap between the conduction and valence bands is very large. Also, the conduction band is practically empty. 
    ii) When an electric field is applied across such a solid, the electrons find it difficult to acquire such a large amount of energy to reach the conduction band. Thus, the conduction band continues to be empty. That is why no current flows through insulators. 
    Semiconductors: 
    i) The energy band structure of semiconductors is similar to that of insulators, but in their case, the size of forbidden energy gap is much smaller than that of the insulators. 
    ii) When an electric field is applied to a semiconductor, the electrons in the valence band find it comparatively easier to shift to the conduction band. So, the conductivity of semiconductors lies between the conductivity of conductors and insulators. 
    Question 905
    CBSEENPH12039207

    For the past some time, Aarti had been observing some erratic body movement, unsteadiness and lack of coordination in the activities of her sister Radha, who also used to complain of severe headache occasionally. Aarti suggested to her parents to get a medical check-up of Radha. The doctor thoroughly examined Radha and diagnosed that she has a brain tumor. 

    (a) What, according to you, are the values displayed by Aarti?

    (b) How can radioisotopes help a doctor to diagnose brain tumor?

    Solution

    a) Aarti has incessantly displayed care towards the health of her sister. She has been a keen observer and concerned for others.

    b) Using a radio-isotope, a doctor can understand the movement of a normal brain and a brain having tumor in it. A radio-isotope is made to enter the body along with the elements and a compound, whose absorption, functioning and distribution to the brain is studied. The isotope emits radiation and these radiations are detected for absorption and function of the compounds. So, a doctor can diagnose the brain tumor.

    Question 906
    CBSEENPH12039208

    Write two basic modes of communication. Explain the process of amplitude modulation. Draw a schematic sketch showing how amplitude modulated signal is obtained by superposing a modulating signal over a sinusoidal carrier wave. 

    Solution

    The two basic modes of communication are:

    1. Point-to-point communication
    2. Broadcast communication

    In amplitude modulation, the amplitude of the carrier wave is varied in accordance with the amplitude of the modulating wave. 

    Let, the carrier wave be given by, 
                                            straight c left parenthesis straight t right parenthesis space equals space straight A subscript straight c sinω subscript straight c straight t

    Modulating signal is given by, 
                                          straight m left parenthesis straight t right parenthesis space equals space straight A subscript straight m sinω subscript straight m straight t
    straight omega subscript straight m is the angular frequency of the message signal.

    Therefore, modulated signal is given by,
    Error converting from MathML to accessible text.
    Error converting from MathML to accessible text.

    Amplitude modulated signal is produced by superposing a modulating signal over a sinusoidal carrier wave. The process is illustrated in the fig. below.
     

    Question 907
    CBSEENPH12039209

    An electron microscope uses electrons accelerated by a voltage of 50 kV. Determine the de-Broglie wavelength associated with the electrons. Taking other factors, such as numerical aperture etc. to be same, how does the resolving power of an electron microscope compare with that of an optical microscope which uses yellow light?

    Solution

    Given,

    Accelerating voltage for electrons = 50 kV = 50 x 103 V

     

    De-Broglie wavelength is given by, 
    Error converting from MathML to accessible text. 

    So, from the above formula, we can say that the resolving power of an electron microscope is much greater than that of optical microscope.

    Question 908
    CBSEENPH12039212

    (a) In Young's double slit experiment, describe briefly how bright and dark fringes are obtained on the screen kept in front of a double slit. Hence obtain the expression for the fringe width.

    (b) The ratio of the intensities at minima to the maxima in the Young's double slit experiment is 9: 25. Find the ratio of the widths of the two slits.

    Solution

    a)
    Let S1 and S2 be two coherent sources separated by a distance d.

    Let the distance of the screen from the coherent sources be D. Let point M be the foot of the perpendicular drawn from O, which is the midpoint of S1 and S2 on the screen. Obviously point M is equidistant from S1 and S2. Therefore the path difference between the two waves at point M is zero. Thus the point M has the maximum intensity.

    Now, Consider a point P on the screen at a distance y from M. Draw S1N perpendicular from S1 on S2 P. 

    The path difference between two waves reaching at P from S1 and S2 is given by, 
    increment space equals space S subscript 2 P minus S subscript 1 P space almost equal to space S subscript 2 N 
    Since, D >> d, so angle S subscript 2 S subscript 1 N space equals space theta is very small.
    angle S subscript 2 S subscript 1 N space equals space angle M O P space equals space theta 
    In space increment space S subscript 1 S subscript 2 N italic comma

italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space sin space theta space equals space fraction numerator S subscript italic 2 N over denominator S subscript italic 1 S subscript italic 2 end fraction
I n italic space italic increment M O P italic comma italic space

italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space sin space theta space equals space theta space equals space tan space theta italic space

italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space fraction numerator S subscript italic 2 N over denominator S subscript italic 1 S subscript italic 2 end fraction space equals space fraction numerator M P over denominator O M end fraction
italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space S subscript italic 2 N space equals space S subscript italic 1 S subscript italic 2 space cross times space fraction numerator M P over denominator O M end fraction space equals space d. y over D

Therefore comma space

Path space difference comma space increment equals S subscript 2 P minus S subscript 1 P space equals S subscript 2 N space equals space fraction numerator y d over denominator D end fraction italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic. italic. italic. italic space italic left parenthesis italic 1 italic right parenthesis

F o r italic space b r i g h t italic space f r i n g e italic comma italic space w e italic space h a v e italic space

fraction numerator y d over denominator D end fraction equals space n lambda italic comma italic space n italic space italic equals italic space italic 0 italic comma italic 1 italic comma italic 2 italic comma italic 3 italic comma italic. italic. italic.

T h e r e f o r e italic comma italic space

italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space italic space y subscript n equals fraction numerator n D lambda over denominator d end fraction  
    Error converting from MathML to accessible text.

    For dark fringe, path difference is an odd multiple of half wavelength.
    So, we have  
    Error converting from MathML to accessible text. 

    Let, straight y subscript straight n plus 1 end subscript straight space and straight space straight y subscript straight n italic spacebe the distance of two consecutive fringes. Then, we have
    y subscript n plus 1 end subscript space equals space left parenthesis n plus 1 right parenthesis fraction numerator D lambda over denominator d end fraction a n d space space y subscript n equals fraction numerator n D lambda over denominator d end fraction

So comma space fringe space width space is comma space
space y subscript n plus 1 end subscript italic space minus space space y subscript n space end subscript equals space left parenthesis n plus 1 right parenthesis fraction numerator D lambda over denominator d end fraction minus fraction numerator n D lambda over denominator d end fraction equals fraction numerator D lambda over denominator d end fraction 

    Fringe width is same for both bright and dark fringe.

    b)
    Give, ratio of minima to maxima intensity is given by, 9:25

    That is, 
    I subscript m i n end subscript over I subscript m a x end subscript equals space fraction numerator left parenthesis a subscript 1 minus a subscript 2 right parenthesis squared over denominator left parenthesis a subscript 1 plus a subscript 2 right parenthesis squared end fraction equals space 9 over 25 
    rightwards double arrow straight space fraction numerator straight a subscript 1 minus straight a subscript 2 over denominator straight a subscript 1 plus straight a subscript 2 end fraction equals straight space 3 over 5 semicolon

where space straight a space is space the space amplitude space of space the space slit space and space straight I space the space intensity.

So comma space
space space space space space straight a subscript 1 over straight a subscript 2 equals straight space 4 over 1
fraction numerator straight space straight w subscript 1 over denominator straight w subscript 2 end fraction equals straight space fraction numerator left parenthesis straight a subscript 1 right parenthesis squared over denominator left parenthesis straight a subscript 2 right parenthesis end subscript squared end fraction equals straight space 16 over 1 semicolon space is space the space ratio space of space the

space width space of space the space slit.

    Question 909
    CBSEENPH12039213

    (a) Describe briefly how a diffraction pattern is obtained on a screen due to a single narrow slit illuminated by a monochromatic source of light. Hence obtain the conditions for the angular width of secondary maxima and secondary minima.

    (b) Two wavelengths of sodium light of 590 nm and 596 nm are used in turn to study the diffraction taking place at a single slit of aperture 2 × 10−6 m. The distance between the slit and the screen is 1·5 m. Calculate the separation between the positions of first maxima of the diffraction pattern obtained in the two cases.

    Solution

    a) Diffraction of light at a Single slit

    A single narrow slit is illuminated by a monochromatic source of light. The diffraction pattern is obtained on the screen placed in front of the slits. There is a central bright region called as central maximum. All the waves reaching this region are in phase hence the intensity is maximum. On both side of central maximum, there are alternate dark and bright regions, the intensity becoming weaker away from the center. The intensity at any point P on the screen depends on the path difference between the waves arising from different parts of the wave-front at the slit.

    According to the figure, the path difference (BP – AP) between the two edges of the slit can be calculated.

    Path difference, BP – AP = NQ = a sin straight theta space almost equal to space aθ

    Angle straight theta  is zero at the central point C on the screen, therefore all path difference are zero and hence all the parts of slit are in phase. Due to this, the intensity at C is maximum. If this path difference is, (the wavelength of light used), then P will be point of minimum intensity. This is because the whole wave-front can be considered to be divided into two equal halves CA and CB and if the path difference between the secondary waves from A and B is , then the path difference between the secondary waves from A and C reaching P will be straight lambda /2, and path difference between the secondary waves from B and C reaching P will again be straight lambda /2. Also, for every point in the upper half AC, there is a corresponding point in the lower half CB for which the path difference between the secondary waves, reaching P is straight lambda/2. Thus, destructive interference takes place at P and therefore, P is a point of first secondary minimum. 

    Width of secondary maximum is given by, 
    space space space space space straight beta straight space equals straight space straight y subscript straight n straight space minus straight space straight y subscript straight n minus 1 end subscript straight space equals straight space nDλ over straight a minus straight space fraction numerator left parenthesis straight n minus 1 right parenthesis Dλ over denominator straight a end fraction

therefore space straight space straight beta straight space equals straight space Dλ over straight a 

    Width of secondary minima is given by,  

    straight beta '  straight space equals straight space nDλ over straight a minus straight space fraction numerator left parenthesis straight n minus 1 right parenthesis Dλ over denominator straight a end fraction
therefore space beta apostrophe space equals space fraction numerator D lambda over denominator a end fraction

    Since angular width is independent of n. all secondary minima and maxima are of the same width.

    b) Given,
    lambda subscript 1 space equals space 590 space n m space
lambda subscript italic 2 space equals space 596 space n m
    Aperture of the slit, a = 2  10 -6 m

    Distance between slit and screen = 1.5 m

    Therefore, linear separation, between the first maxima (n=1) of the two wavelengths, on the screen, is given by, 

                                fraction numerator 3 left parenthesis straight lambda subscript 2 minus straight lambda subscript 1 right parenthesis over denominator straight a end fraction cross times straight D
    Therefore, separation is given by, 

    Error converting from MathML to accessible text.

    Question 910
    CBSEENPH12039218

    How does the angular separation between fringes in single-slit diffraction experiment change when the distance of separation between the slit and screen is doubled? 

    Solution

    Angular separation is given by,
    straight theta space equals space straight beta over straight D space equals space fraction numerator Dλ divided by straight d over denominator straight D end fraction equals straight lambda over straight d

    Angular separation would remain same when the distance of separation between the slit and the screen is doubled.

    Question 911
    CBSEENPH12039220

    For the same value of angle incidence, the angles of refraction in three media A, B and C are 15°, 25° and 35° respectively. In which medium would the velocity of light be minimum? 

    Solution

    As per Snell’s law we have,
    straight n space equals space fraction numerator sin space straight i over denominator sin space straight r end fraction space equals space straight c over straight v 
    For given i, v proportional tosin r 
    r is minimum in medium A, so velocity of light is minimum in medium A.



    Question 912
    CBSEENPH12039221

    A proton and an electron have same kinetic energy. Which one has greater de-Broglie wavelength and why?

    Solution

    As per De-broglies formula, 

    straight lambda space equals space fraction numerator straight h over denominator square root of 2 mE subscript straight k end root end fraction 

    Kinetic energy of proton is equal to kinetic energy of proton.

    Since, mass of proton > mass of electron,

    This implies, 
    straight lambda subscript straight e space greater than space straight lambda subscript straight p
    That is, wavelength of electron is greater than the wavelength of proton.

    Question 913
    CBSEENPH12039228

    An object AB is kept in front of a concave mirror as shown in the figure.

     

    (i) Complete the ray diagram showing the image formation of the object.

    (ii) How will the position and intensity of the image be affected if the lower half of the mirror’s reflecting surface is painted black?        

    Solution

    (i) Image formed will be inverted diminished between C and F.

     

    ii) When the lower half of the mirror’s reflecting surface is painted black, the position of the image and its intensity will get reduced.

    Question 914
    CBSEENPH12039229

    Draw a labelled ray diagram of a reflecting telescope. Mention its two advantages over the refracting telescope

    Solution

     

     

     

    Advantages of reflecting telescope over refracting telescope:

    (i) It is free from chromatic aberration.

    (ii) Its resolving power is greater than refracting telescope due to larger aperture of mirror.

    Question 915
    CBSEENPH12039230

    Describe briefly with the help of a circuit diagram, how the flow of current carries in a p-n-p transistor is regulated with emitter-base junction forward biased and base-collector junction reverse biased. 

    Solution

    The emitter-base junction is given a small forward bias, while base collector junction is given a large reverse bias.
    Under the forward biasing of emitter-base region, the positive holes of P - region move towards the base. Due to thin base most of holes (about 98%) entering it pass onto collector while a very few of them (nearly 2%) combine with the electrons of base.
    As soon as a hole combines with the electron, a fresh electron leaves the negative terminal of battery VEE and enters the base. This causes a very small base current I B. The holes entering the collector move under the aiding reverse bias towards terminal C. As a hole reaches terminal C, an electron leaves the negative terminal of battery VCC and neutralizes the hole.
    This causes the collector current IC . Both these currents IB and IC combine to form the emitter current Ie.

    i. e., IE = IB + IC
    Obviously the holes are the charge carriers within the p-n-p transistor while the electrons are charge carriers in external circuit.

    Question 916
    CBSEENPH12039231

    In the given block diagram of a receiver, identify the boxes labelled as X and Y and write their functions.

    Solution

    The element labelled 'X' is called 'channel'. Channel connects transmitter and receiver. The signal from the transmitter is carried to the receiver by the communication channel.

    Question 917
    CBSEENPH12039236

    You are given three lenses L1, L2 and L3 each of focal length 20 cm. An object is kept at 40 cm in front of L1, as shown. The final real image is formed at the focus ‘I’ of L3. Find the separations between L1, L2 and L3.

    Solution

    Given, 
    f1 = f2 = f3 = 20 cm 

    In case of lens L1,

    Object distance, u1 = -40 cm

    Using Lens formula,
    space space space space space 1 over straight v subscript 1 space minus space 1 over straight u subscript 1 space equals space 1 over straight f subscript 1

rightwards double arrow space 1 over straight v subscript 1 space equals space 1 over 20 space minus space minus 1 over 40

rightwards double arrow space space straight v subscript 1 space equals space 40 space cm
    For lens L3,
    straight f subscript 3 space equals space 20 space cm. space straight v subscript 3 space equals space 20 space cm

Object space distance comma space straight u subscript 3 space equals space ?

Using space lens space formula comma space we space have

1 over straight v subscript 3 minus 1 over straight u subscript 3 space equals space 1 over straight f subscript 3 space

rightwards double arrow space 1 over 20 minus 1 over straight u subscript 3 space equals space 1 over 20

rightwards double arrow space space 1 over straight u subscript 3 space equals 0 space
rightwards double arrow space space space space straight u subscript 3 space equals space infinity 

    So, lens L2 should produce the image at infinity. Thus, objective should be at focus. The image formed by lens L1 is at 40 cm on the right side of lens L1 which lies at 20 cm left of lens L2 i.e., focus of lens L2.

    Hence, the distance between L1 and L2 = 40 + 20 = 60 cm.

    Question 918
    CBSEENPH12039237

    Define the terms (i) ‘cut-off voltage’ and (ii) ‘threshold frequency’ in relation to the phenomenon of photoelectric effect.

    Using Einstein’s photoelectric equation shows how the cut-off voltage and threshold frequency for a given photosensitive material can be determined with the help of a suitable plot/graph.        

    Solution

    i) Cut-off or stopping potential is that minimum value of negative potential at anode which just stops the photo electric current.

    ii) The minimum frequency of light below which no photo electric emission will take place is known as threshold frequency.
     

    Now using Einstein’s photoelectric equation, we have 
     

    Clearly, Vostraight nu graph is a straight line.

    Question 919
    CBSEENPH12039239

    Mention three ‘different modes of propagation used in communication system. Explain with the help of a diagram how long distance communication can be achieved by ionospheric reflection of radio waves.           

    Solution

    Three modes of propagation of electromagnetic waves:

    (i) Ground waves

    (ii) Sky waves

    (iii) Space waves

    Sky wave propagation is used for long distance communication. In this process, radio waves are reflected by ionosphere. When radio waves of frequency range 3 MHz to 30 MHz, emitted from transmitting antenna reach the receiving antenna after reflection from the ionosphere acts as a reflector for radio waves.

    Question 920
    CBSEENPH12039240

    Draw a plot of potential energy of a pair of nucleons as a function of their separations. Mark the regions where the nuclear force is (i) attractive and (ii) repulsive. Write any two characteristic features of nuclear forces. 

    Solution

    The below figure shows the plot of potential energy of a pair of nucleons as a function of their separation.
     

    AB represents repulsive force and part BCD reprtesents attractive force.

    Properties of nuclear forces are:

    (1) Nuclear forces are attractive and stronger, then electrostatic force.

    (2) Nuclear forces are charge-independent.

    Question 921
    CBSEENPH12039241

    In a Geiger–Marsden experiment, calculate the distance of closest approach to the nucleus of Z =80, when an a-particle of 8 MeV energy impinges on it before it comes momentarily to rest and reverses its direction.

    How will the distance of closest approach be affected when the kinetic energy of the a-particle is doubled?

    Solution

    Let ro be the distance of closest approach where the kinetic energy of the alpha-particle is converted into it’s potential energy.

    Given, Z = 80, Ek = 8 MeV

    Since, 
    straight r subscript straight o space proportional to space 1 over straight K

    Kinetic energy of the particle becomes doubled if the distance of closest approach becomes half.

    Question 922
    CBSEENPH12039242

    The ground state energy of hydrogen atom is – 13.6 eV. If an electron makes a transition from an energy level – 0.85 eV to –3.4 eV, calculate the wavelength of the spectral line emitted. To which series of hydrogen spectrum does this wavelength belong?

    Solution

    Using the formula,

    For, n=1; E1 = - 13.6 eV

    During the electron transmission, EA = - 0.85 eV to EB = -3.4 eV

    So, from equation (i), we have
     

    Therefore, electron transition takes place from n=4 to n=2 which corresponds to Balmer series.

    We know,

    Here, 
    nA = 4 ; nB = 2 ; R = 1.097 x 107 m-1

    Then, 
    space space space space 1 over straight lambda space equals space 1.097 space x space 10 to the power of 7 open parentheses 1 over 2 squared space minus space 1 over 4 squared close parentheses
rightwards double arrow space space lambda space equals space 4862 space A with o on top

    Question 923
    CBSEENPH12039244

    a) In Young’s double slit experiment, derive the condition for (i) constructive interference and

    (ii) Destructive interference at a point on the screen.

    (b) A beam of light consisting of two wavelengths, 800 nm and 600 nm is used to obtain the interference fringes in a Young’s double slit experiment on a screen placed 1.4 m away. If the two slits are separated by 0.28 mm, calculate the least distance from the central bright maximum where the bright fringes of the two wavelengths coincide.

    Solution

    a)
    Conditions of constructive interference and destructive interference.

    Consider two coherent waves travelling in the same direction along a straight line.

    Frequency of each wave is given by fraction numerator straight omega over denominator 2 straight pi end fraction

    Amplitude of electric field vectors are a1 and a2 rspectively.

    Wave equation is represented by, 
    straight y subscript 1 space equals space straight a subscript 1 space sin space straight omega space straight t space space space space space space space space space space space space space space space space space... space left parenthesis straight i right parenthesis

straight y subscript 2 space equals space straight a subscript 2 space sin space left parenthesis ωt space plus space straight ϕ right parenthesis space space space space space space space space space... space left parenthesis ii right parenthesis thin space

Using space the space theory space of space superposition comma space

straight y space equals space straight y subscript 1 space plus space straight y subscript 2 space space space space space space space space space space space space space space space space space space space space space... space left parenthesis iii right parenthesis thin space

Here comma space straight y subscript 1 space and space straight y subscript 2 space are space the space points space of space electric space field. space

Putting space values space from space left parenthesis ii right parenthesis space and space left parenthesis iii right parenthesis space in space left parenthesis straight i right parenthesis comma space we space have

straight y space equals space straight a subscript 1 space sin space straight omega space straight t space plus space straight a subscript 2 space sin space space left parenthesis ωt space plus space straight ϕ right parenthesis space space

Now space using space trignometric space identities comma space we space have 
    sin space left parenthesis omega t space plus space ϕ right parenthesis thin space equals space sin space ωt space cos space straight ϕ space plus space cos space ωt space sin space straight ϕ

we space get comma

straight y space equals space straight a subscript 1 space sin space ωt space plus space straight a subscript 2 space left parenthesis sin space ωt space cos space straight ϕ space plus space cos space ωt space sin space straight ϕ right parenthesis

space space equals space left parenthesis straight a subscript 1 space plus space straight a subscript 2 space cos space straight ϕ right parenthesis thin space sin space straight omega space straight t space plus space left parenthesis straight a subscript 2 space sin space straight ϕ space right parenthesis space cos space ωt space space space space space space space space... space left parenthesis iv right parenthesis

Assume comma space
space straight a subscript 1 space plus space space straight a subscript 2 space cos space straight ϕ space equals space straight A space cos space straight theta
and
space space space space space space space space space space space straight a subscript 2 space sin space straight ϕ space space equals space straight A space sin space straight theta

So comma space eqn. space left parenthesis iv right parenthesis thin space gives comma space

straight y space equals space straight A space cos space straight theta thin space sin space straight omega space straight t space plus straight A space sin space straight theta space space cos space ωt space

space space equals space straight A space sin space left parenthesis ωt space plus space straight ϕ right parenthesis

Amplitude space of space the space resultant space wave space is space given space by comma space

Amplitude comma space straight A space equals space square root of straight a subscript 1 squared space plus space straight a subscript 2 squared space plus space 2 straight a subscript 1 straight a subscript 2 cos space straight ϕ end root space space

    Intensity of the wave is proportional to the amplitude of the wave.

    Thus, Intensity of the resultant wave is given by, 
    straight I thin space equals straight A squared space equals space straight a subscript 1 squared space plus space straight a subscript 2 squared space plus space 2 straight a subscript 1 straight a subscript 2 space end subscript cos space straight ϕ

    Constructive interference: For maximum intensity at any point, cos  = +1

    So, maximum intensity is, 

    Path difference is, 

    Constructive interference is obtained when the path difference between the waves is an integral multiple of straight lambda 

    Destructive Interference: For minimum intensity at any point, cos  = -1

    Phase difference is given by, 
    straight ϕ space equals space straight pi comma space 3 straight pi comma space 5 straight pi comma space 7 straight pi comma....

space space equals left parenthesis 2 straight n space minus 1 right parenthesis space straight pi comma space straight n space equals space 1 comma 2 comma 3 comma...

Minimum space intensity space is comma space

straight I subscript min space equals space straight a subscript 1 squared space plus space straight a subscript 2 squared space minus space 2 space straight a subscript 1 space straight a subscript 2 space equals space left parenthesis straight a subscript 1 space minus space straight a subscript 2 right parenthesis squared  
    Path difference is, 

    In destructive interference, path difference is odd multiple of  straight lambda over 2.
    b)
    Given,
     
    d = 0.28 mm = 0.28 x 10-3 m
    As, straight lambda subscript 1 space greater than space straight lambda subscript 2

    If n1 = n then, n2 = n+1

     
             

    Question 924
    CBSEENPH12039245

    (a) How does an unpolarized light incident on a Polaroid get polarized?

    Describe briefly, with the help of a necessary diagram, the polarization of light by reflection from a transparent medium.

    (b) Two Polaroid’s ‘A’ and ‘B’ are kept in crossed position. How should a third Polaroid ‘C’ be placed between them so that the intensity of polarized light transmitted by Polaroid B reduces to 1/8th of the intensity of unpolarized light incident on A?

    Solution

    a) When an unpolarized light falls on a polaroid, only those electric vectors that are oscillating along a direction perpendicular to the aligned molecules will pass through. Thus, incident light gets linearly polarized.

    Electric vectors which are along the direction of the aligned molecules gets absorbed.
     

    Whenever unpolarized light is incident on the boundary between two transparent media, the reflected light gets partially or completely polarized. When reflected light is perpendicular to the refracted light, the reflected light is a completely polarized light.

    b) Let the angle between A and C be straight theta .
    Intensity of light passing through A = Io/2 
    Intensity of light passing through C = Io/2 cos2 straight theta
    Intensity of light passing through B = Io/2 cos2 straight theta. cos2 (90 - straight theta)
    Given that, 
     

    Thus, the third polaroid is placed at an angle of 45o.

    Question 925
    CBSEENPH12039246

    (a) Describe briefly, with the help of a diagram, the role of the two important processes involved in the formation of a p-n junction.

    (b) Name the device which is used as a voltage-regulator. Draw the necessary circuit diagram and explain its working.

    OR

     

    (a) Explain briefly the principle on which a transistor-amplifier works as an oscillator. Draw the necessary circuit diagram and explain its working.

    (b) Identify the equivalent gate for the following circuit and write its truth table. 


    Solution

    a) Important process occurring during the formation of p-n junction are:

    1) Diffusion: When p-n junction is formed due to concentration gradient, the holes diffuse from p-side to n-side and electrons diffuse from n-side to p-side. This motion of charge carriers gives rise to diffusion current across the junction.

    2) Drift: Drift of charge carriers occurs due to the applied electric field. As a result of the potential barrier, an electric field from n-region to p-region is developed across the junction. This electric field causes motion of electrons on p-side of the junction to n-side of the junction. Holes are moved from n-side to p-side. Thus, a drift current starts which is opposite to the direction of diffusion current.

    b) Zener diode is used as voltage regulator. 

    There is a voltage drop across Rs whenever there is decrease or increase in the input voltage. Change in voltage across Rs does not affect the voltage across Zener diode.

                                                            OR

    a) The below fig. is that of a transistor amplifier.

    The transistor amplifier works on the principle of mutual induction.

    The above circuit contains tuned circuit made of variable capacitor C and an inductor L in the collector circuit and hence is named as tuned collector oscillator. The feedback coil L¢ connected to base circuit is mutually coupled with coil L.

    The biasing is provided by emitter resistance RE and potential divider arrangement consisting of resistances R1 and R2. The capacitor C1 connected in the base circuit provides low reactance path to the oscillations and the capacitor CE is the emitter by-pass capacitor so that the resistor RE has no effect on the ac operation of the circuit.

    Closing switch S will switch on the collector supply voltage. So, collector current starts increasing and capacitor C is charged. When the capacitor attains maximum charge, it discharges through coil L , setting up oscillations of natural frequency which is given by, 

    These oscillations induce a small voltage in coil L’ by mutual induction. This induced voltage is the feedback voltage; its frequency is same as that of resonant LC circuit but its magnitude depends on the number of turns in L’ and coupling between L and L’ . The feedback voltage is applied between the base and emitter and appears in the amplified form in the collector circuit. A part of this amplifier energy is used to meet losses taking place in oscillatory circuit to maintain oscillations in tank circuit and the balance is radiated out in the form of electromagnetic waves.

    b) The Boolean expression for the output is given by, 

    This is the expression for AND gate.

    Symbol for AND gate is given by, 

    Truth table is given by, 

    Question 926
    CBSEENPH12039253

    Write any two characteristic properties of nuclear force.

    Solution

    (i) Nuclear forces are short range attractive forces. 
    (ii) Nuclear forces are charge – independent.

    Question 927
    CBSEENPH12039255

    What happens to the width of depletion layer of a p-n junction when it is (i) forward biased, (ii) reverse biased? 

    Solution

    (i) When forward biased, the width of depletion layer decreases.

    (ii) When reverse biased, the width of depletion layer increases.

    Question 928
    CBSEENPH12039256

    Define the term ‘stopping potential’ in relation to photoelectric effect. 

    Solution

    Stopping potential is the minimum retarding or negative potential of anode of a photoelectric tube for which photoelectric current stops or becomes zero. 

    Question 929
    CBSEENPH12039261

    What is sky wave communication? Why is this mode of propagation restricted to the frequencies only up to few MHz?

    Solution

    Sky wave propagation is a mode of propagation in which communication of radio waves in frequency range 30 MHz–40 MHz takes place due to reflection from the ionosphere.

    For frequencies higher than few MHz, the sky waves penetrate the ionosphere and are not reflected back.

    Question 930
    CBSEENPH12039265

    Using the curve for the binding energy per nucleon as a function of mass number A, state clearly how the release in energy in the processes of nuclear fission and nuclear fusion can be explained.              

    Solution
     

    The binding energy per nucleon increases when a heavy nucleus breaks into two lighter nuclei. That is, energy would be released during the process of nuclear fusion.

    When light nuclei join to form a heavy nucleus, the binding energy per nucleon of fused heavier nucleus is more than the binding energy per nucleon of lighter nuclei. Again, there is release of energy in this process
    Question 931
    CBSEENPH12039267

    A convex lens made up of glass of refractive index 1.5 is dipped, in turn, in (i) a medium of refractive index 1.65, (ii) a medium of refractive index 1.33.

    (a) Will it behave as a converging or a diverging lens in the two cases?

    (b) How will its focal length change in the two media?

    Solution

    Given, refractive index of glass, ng = 1.5

    Therefore, focal length of lens in liquid, 

    a)       i) ng = 1.5, n

                 

    So fi and fa are of opposite sign.

    Therefore, convex in liquid 1 behaves as a diverging lens.

    ii) Refractive index of medium, nl = 1.33

    Therefore, fl and fa are of the same sign.

    So, convex lens in liquid l behaves a s a convergent lens.
    b) 

     i) Focal length, f1 is, 

    Focal length becomes negative and it’s magnitude increases.

    ii) Focal length f2 is given by, 

    Focal length increases in magnitude and is positive.

    Question 932
    CBSEENPH12039268

    Draw a plot showing the variation of photoelectric current with collector plate potential for two different frequencies, v1 >v2 , of incident radiation having the same intensity. In which case will the stopping potential be higher? Justify your answer. 

    Solution

    The plots showing the variation of photoelectric current with collector potential is shown below.

    Stopping potential is directly proportional to the frequency of incident radiation.

    Question 933
    CBSEENPH12039269

    Write briefly any two factors which demonstrate the need for modulating a signal.

    Draw a suitable diagram to show amplitude modulation using a sinusoidal signal as the modulating signal. 

    Solution

    Two factors justifying the need for modulation are:

    (i) Practical size of antenna.
    (ii) To avoid mixing up of signals from different transmitters i.e., avoid fluctuation and reduce the noise of signal.

    Question 934
    CBSEENPH12039270

    Use the mirror equation to show that:

    (a) an object placed between f and 2f of a concave mirror produces a real image beyond 2f.

    (b) a convex mirror always produces a virtual image independent of the location of the object.

    (c) an object placed between the pole and focus of a concave mirror produces a virtual and enlarged image.

    Solution

    Mirror equation is given by,
    space space space space space space 1 over straight f space equals space 1 over v plus 1 over u

rightwards double arrow space space space 1 over v space equals space 1 over f space minus space 1 over u 

    a)
    For a concave mirror, f is negative, i.e., f < 0

    For a real object i.e., which is on the left side of the mirror, 
    For u between f and 2f implies that 1/u lies between 1/f and 1/2f
    i.e.,   space space space space space fraction numerator 1 over denominator 2 straight f end fraction greater than fraction numerator 1 over denominator straight u space end fraction greater than 1 over straight f space left parenthesis as space straight u comma straight f space are space negative right parenthesis

rightwards double arrow space 1 over straight f minus fraction numerator 1 over denominator 2 straight f end fraction less than space 1 over straight f minus fraction numerator 1 over denominator straight u space end fraction less than space 0

rightwards double arrow space fraction numerator 1 over denominator 2 straight f end fraction less than space 1 over straight v less than 0

straight i. straight e. comma space space space space 1 over straight v space is space negative. space
    Implies, v is negative and greater than 2f. Therefore, image lies beyond 2f and it is real.

    b)
    Focal length is positive for convex mirror, i.e., f > 0.

    For a real object on the left side of the mirror, u is negative.
    1 over straight f space equals 1 over v space plus space 1 over u
    That is, 
    1 over straight v space equals space 1 over straight f space minus space 1 over straight u

    Since u is negative and f is positive so, 1/v should also be positive, so v must be positive.

    Hence, image is virtual and lies behind the mirror.
    c) 
    Using the mirror equation, we have
    1 over straight v space equals space 1 over straight f space minus space 1 over straight u

For space straight a space concave space mirror comma space straight f space is space negative semicolon space straight f space less than space 0

As space straight u space is space also space negative comma space so space straight f space less than space straight u less than 0

This space implies comma space

1 over straight f space minus space 1 over straight u greater than 0

Then space from space left parenthesis 1 right parenthesis comma space 1 over straight v space greater than thin space 0 space or space straight v space is space positive. space

straight i. straight e. comma space image space is space formed space on space the space right space
hand space side space and space is space virtual. space

Magnification comma space straight m space equals negative straight v over straight u space equals space minus fraction numerator straight f over denominator straight u minus straight f end fraction

As space straight u space is space negative space and space straight f space is space positive comma space

magnification comma space straight m space equals space fraction numerator vertical line straight f vertical line over denominator vertical line straight f vertical line space minus space vertical line straight u vertical line end fraction greater than thin space 1 
    That is, the image is enlarged.

    Question 935
    CBSEENPH12039272

    (a) Using de Broglie’s hypothesis, explain with the help of a suitable diagram, Bohr’s second postulate of quantization of energy levels in a hydrogen atom.

    (b) The ground state energy of hydrogen atom is –13.6 eV. What are the kinetic and potential energies of the electron in this state?

    Solution

    a) According to De- broglie hypothesis

    straight h over mv equals straight lambda                                   …(i) 

    As per De-broglie’s condition of stationary orbits, the stationary orbits are those which contain complete de-Broglie wavelength.

     2 πr space equals space nλ                              ... (ii)                                                    

    Putting value of  from equation (i) into (ii)

     

    which is the required postulate for Bohr’s quantization of energy levels.

     

    b) Given, ground state energy of hydrogen atom = -13.6 eV

    Kinetic energy is given by,

     
    Potential energy is given by,

     

    So, total energy is given by,

    Now, from equations (i), (ii) and (iii), we can see that

    K.E = - E and U = 2E

    We have, E = -13.6 eV

    So,

    K.E = 13.6 eV

    P.E, U = 2 x (-13.6) = -27.2 eV

    Question 936
    CBSEENPH12039273

    You are given a circuit below. Write its truth table. Hence, identify the logic operation carried out by this circuit. Draw the logic symbol of the gate it corresponds to. 


    Solution

    The logical expression for output is given by, 
                                

    which is the equivalent of AND gate.

    Logic symbol for AND gate is given by, 

    Truth table for AND gate is given by, 

    Question 937
    CBSEENPH12039274

    A compound microscope uses an objective lens of focal length 4 cm and eyepiece lens of focal length 10 cm. An object is placed at 6 cm from the objective lens. Calculate the magnifying power of the compound microscope. Also calculate the length of the microscope.

     

    OR

     

    A giant refracting telescope at an observatory has an objective lens of focal length 15 m. If an eyepiece lens of focal length 1.0 cm is used, find the angular magnification of the telescope.

    If this telescope is used to view the moon, what is the diameter of the image of the moon formed by the objective lens? The diameter of the moon is 3.42 × 106 m and the radius of the lunar orbit is 3.8 × 108 m.

    Solution

    Focal length of the objective lens, fo = 4 cm

    Focal length of the eyepiece, fe = 10 cm

    Object distance, uo = -6 cm

    Magnifying power of a microscope is given by, 

    Now, using the lens formula, we have
               1 over straight f subscript straight o space equals space 1 over v subscript o space minus space 1 over u subscript o
                      

    Negative sign shows that the image is inverted.

    Length of the microscope is given by, 
                                   

    For eyepiece of the microscope,

       
    We have, ve = D = -25 cm


    Here, L is the length of the microscope. 

                                                               OR

    Angular magnification is given by, 
    Error converting from MathML to accessible text.

    where, fo is the focal length of the objective lens, and

               fe is the focal length of the eye-piece. 

    Given, diameter of the moon = 3.48 × 106 m

    Radius of the lunar orbit = 3.8 × 108 m

    Diameter of the image of moon formed by the objective lens is given by, d =  αf subscript straight o
    Error converting from MathML to accessible text.

    Question 938
    CBSEENPH12039278

    State the importance of coherent sources in the phenomenon of interference.

    In Young’s double slit experiment to produce interference pattern, obtain the conditions for constructive and destructive interference. Hence, deduce the expression for the fringe width.

    How does the fringe width get affected, if the entire experimental apparatus of Young is immersed in water?

    Solution

    If coherent sources are not taken, the phase difference between two interfering waves, will change continuously and a sustained interference pattern will not be obtained. Thus, coherent sources provide sustained interference pattern.

    Let S1 and S2 be two coherent sources separated by a distance d.

    Let the distance of the screen from the coherent sources be D. Let point M be the foot of the perpendicular drawn from O, which is the midpoint of S1 and S2 on the screen. Obviously point M is equidistant from S1 and S2. Therefore the path difference between the two waves at point M is zero. Thus the point M has the maximum intensity.

    Now, Consider a point P on the screen at a distance y from M. Draw S1N perpendicular from S1 on S2 P. 
     

    The path difference between two waves reaching at P from S1 and S2 is given by, 
    Error converting from MathML to accessible text. 

    Expression for Fringe Width:

    Distance between any two consecutive bright fringes or any two consecutive dark fringes are called the fringe width. It is denoted by straight omega . 
    Let, y subscript n plus 1 end subscript space a n d space y subscript n be the distance of two consecutive fringes. Then, we have

    y subscript n plus 1 end subscript space equals space left parenthesis n plus 1 right parenthesis fraction numerator D lambda over denominator d end fraction a n d space space y subscript n equals fraction numerator n D lambda over denominator d end fraction
    So, fringe width = y subscript n plus 1 end subscript minus space space y subscript n space end subscript equals space left parenthesis n plus 1 right parenthesis fraction numerator D lambda over denominator d end fraction minus fraction numerator n D lambda over denominator d end fraction equals fraction numerator D lambda over denominator d end fraction

    Fringe width is same for both bright and dark fringe.

    When the entire apparatus is immersed in water, the fringe width decreases. 

    Question 939
    CBSEENPH12039279

    (a) State Huygens principle. Using this principle explain how a diffraction pattern is obtained on a screen due to a narrow slit on which a narrow beam coming from a monochromatic source of light is incident normally.

    (b) Show that the angular width of the first diffraction fringe is half of that of the central fringe.

    (c) If a monochromatic source of light is replaced by white light, what change would you observe in the diffraction pattern?

    Solution

    Huygen’s principle:

    (i) Every point on a given wavefront may be regarded as a source of new disturbance.

    (ii) The new disturbances from each point spread out in all directions with the velocity of light and are called the secondary wavelets.

    (iii) The surface of tangency to the secondary wavelets in forward direction at any instant gives the new position of the wavefront at that time. 

    a) Diffraction of light at a Single slit

    A single narrow slit is illuminated by a monochromatic source of light. The diffraction pattern is obtained on the screen placed in front of the slits. There is a central bright region called as central maximum. All the waves reaching this region are in phase hence the intensity is maximum. On both side of central maximum, there are alternate dark and bright regions, the intensity becoming weaker away from the center. The intensity at any point P on the screen depends on the path difference between the waves arising from different parts of the wave-front at the slit.
     

    According to the figure, the path difference (BP – AP) between the two edges of the slit can be calculated.

    Path difference, BP – AP = NQ = a sin straight theta 

    Angle  is zero at the central point C on the screen, therefore all path difference are zero and hence all the parts of slit are in phase. Due to this, the intensity at C is maximum. If this path difference is straight lambda, (the wavelength of light used), then P will be point of minimum intensity. This is because the whole wave-front can be considered to be divided into two equal halves CA and CB and if the path difference between the secondary waves from A and B is straight lambda, then the path difference between the secondary waves from A and C reaching P will be straight lambda/2, and path difference between the secondary waves from B and C reaching P will again be straight lambda/2. Also, for every point in the upper half AC, there is a corresponding point in the lower half CB for which the path difference between the secondary waves, reaching P is straight lambda/2. Thus, destructive interference takes place at P and therefore, P is a point of first secondary minimum. 
    b) 

    Central bright lies between  straight theta equals fraction numerator plus straight lambda over denominator straight a end fraction andθ space equals space fraction numerator negative straight lambda over denominator straight a end fraction 

    Therefore, Angular width of central bright fringe = 2 straight theta equals fraction numerator 2 straight lambda over denominator straight a end fraction 

    So, 1st diffraction fringe lies between straight theta equals straight lambda over straight a and straight theta equals fraction numerator 2 straight lambda over denominator straight a end fraction

    Therefore,
    Angular width of first diffraction fringe is, fraction numerator 2 straight lambda over denominator straight a end fraction minus straight lambda over straight a equals straight lambda over straight a 

    So, fraction numerator straight beta subscript straight I over denominator left parenthesis straight beta subscript straight theta right parenthesis subscript straight C end fraction straight space equals straight space 1 half

    c) When monochromatic light is replaced by white light, each diffraction band splits into a number of colored bands. Angular width of violet being the least and that of red light is maximum.

    Question 940
    CBSEENPH12039287

    Explain the terms (i) Attenuation and (ii) Demodulation used in Communication System.

    Solution
    (i) Attenuation: Attenuation is the process of loss in the strength of signal while propagating through a medium. 
    (ii) Demodulation: Demodulation is the process of retrieval of information from the carrier wave at the receiver end. It is the reverse process of modulation.
    Question 941
    CBSEENPH12039288

    Plot a graph showing variation of de Broglie wavelength λ versus fraction numerator 1 over denominator square root of straight V end fraction, where V is the is accelerating potential for two particles A and B, carrying the same charge but different masses m1 and m2 (m1 > m2). Which one of the two represents a particle of smaller mass and why? 

    Solution

    Given, 
    Charge (q) is the same but the mass of both particles is different (m1 > m2).
    The De-broglie wavelength given by, 

    straight lambda space equals space fraction numerator straight h over denominator square root of 2 mqV end root end fraction
    The slope of the graph of λ versus fraction numerator 1 over denominator square root of straight V end fraction  = fraction numerator straight h over denominator square root of 2 mqV end root end fraction
                                        
    The slope of the smaller mass is larger; therefore, plat A in the above graph represents mass m2.

    Question 942
    CBSEENPH12039289

    A nucleus with mass number A = 240 and BE/A = 7.6 MeV breaks into two fragments, each of A = 120 with BE/A = 8.5 MeV. Calculate the released energy.

                                                   OR

    Calculate the energy in the fusion reaction: 

    straight H presubscript 1 presuperscript 2 space plus space straight H presubscript 1 presuperscript 2 space rightwards arrow He presubscript 2 presuperscript 3 space plus space straight n space comma

where space straight B. straight E. space of space straight H presubscript 1 presuperscript 2 space equals space 2.23 space MeV

space space space space space space space space space space space space straight B. straight E. space of space He presubscript 2 presuperscript 3 space equals space 7.73 space MeV

    Solution

    The B.E. of the nucleus of mass number 240, B1 = 7.6 x 240 = 1824 MeV
    The B.E of each product nucleus, B2 = 8.5 x 120 - 1020 MeV
    Then, the energy released as the nucleus breaks is given by, 
    E = 2B2 - B1 = 2 x 1020 - 1824 = 216 MeV 
                                                     OR
    Given: 
    B.E of straight H presubscript 1 presuperscript 2 comma space straight E subscript 1 space equals space 2.23 space MeV
    B.E of He presubscript 2 presuperscript 3 comma space straight E subscript 2 space equals space 7.73 space MeV
    Energy in the fusion reaction is given by, 

    increment straight E space equals space straight E subscript 2 space minus space 2 straight E subscript 1 space equals space 7.73 space minus space left parenthesis 2 space straight x space 2.23 right parenthesis space equals space 3.27 space MeV

    Question 943
    CBSEENPH12039291

    State Brewster's law. 
    The value of Brewster's angle for a transparent medium is different for light of different colours. Give reason.

    Solution
    Brewster discovered a relation between polarising angle, ip and the refrcative index n of the transparent material with respect to the surrounding medium.
    The law is given by, 
                                                       straight mu space equals space tan space straight i subscript straight p
    When a light is incident on a transparent surface at the polarising angle, the reflected and the refracted rays are perpendicular to each other. 
    The lights of different colours have different wavelength hence, there are different values of refractive index for a medium. That is why these lights have different values of brewster's angles.
    Question 944
    CBSEENPH12039293

    Write three characteristic features in photoelectric effect that cannot be explained on the basis of wave theory of light, but can be explained only using Einstein's equation.

    Solution

    The three characteristics of photoelectric effect, which cannot be explained on the basis of wave theory of light are: 
    1. For a given metal and frequency of incident radiation, the number of photoelectrons ejected per second is directly proportional to the intensity of the incident light. 
    2. For a given metal, a certain minimum frequency of the incident radiation below which no emission of photoelectrons take place. The is the threshold frequency. 
    3. Above the threshold frequency, the maximum kinetic energy of the emitted photoelectron is independent of the intensity of the incident light and is dependent only upon the frequency or wavelength of the incident light. 

    Question 945
    CBSEENPH12039299

    (a) Explain any two factors that justify the need of modulating a low-frequency signal.
     
    (b) Write two advantages of frequency modulation over amplitude modulation.

    Solution

    Modulating low-frequency signals are required because: 
    i) Size of the antenna: Antenna is required for both transmission and reception of the signal whose size (at least straight lambda over 4) should be comparable to the wavelength of the signal so that time variation of the signal can be properly sensed by the antenna. For a low-frequency signal, the wavelength is large. Therefore, a large antenna of such a huge height is practically impossible to construct and operate.
    Hence, the need for high-frequency transmission arises. 
    ii) Overlapping signals from different transmitters: When an information is transmitted using different transmitters, the signals get overlapped and the information is lost. Hence, high-frequency transmission is required. Each band should be allocated to each frequency range in order to avoid mixing of signals. 
    iii) Higher energy: High-frequency signals have high energy and therefore, even after loss due to attenuation, signals can be carried over longer distances. 
    b) 
    Advantage of frequency modulation over amplitude modulation are: 
    i) FM is more efficient than AM because the amplitude of an FM wave is constant, irrespective of its modulation index. Thus, the transmitted power is constant. Also, in AM the transmitted power goes waste in the transmitted carrier.  
    ii) FM reception is quite immune to noise in comparison to AM reception. Noise is a form of amplitude variation in the transmitted signal. Thus, using amplitude limiters in the FM receivers, the noise is eliminated.   

    Question 946
    CBSEENPH12039300

    (i) Write the functions of three segments of a transistor.

    (ii) Draw a circuit diagram for studying the input and output characteristics of a n-p-n transistor in common emitter configuration. Using the circuit, explain how input, output characteristics are obtained.

    Solution

    i) The function of three segments of a transistor are: 
     
    Emitter: Emits the majority charge carriers
    Collector: Collects the majority charge carriers
    Base: Base provides the interaction between the collector and the base
    ii) An n-p-n transistor is as shown below: 

    Input characteristics: The variation between the base current and the base-emitter voltage is obtained. Input characteristics is used to find input dynamic resistance of the transistor as it is represented by the slope. 
    Output characteristics: A graph representing the variation of the collector current and emitter voltage is obtained, keeping base current fixed. The slope fo the output characteristic graph gives us the output dynamic resistance.

    Question 947
    CBSEENPH12039301

    (a) Calculate the distance of an object of height h from a concave mirror of radius of curvature 20 cm, so as to obtain a real image of magnification 2. Find the location of image also.

    (b) Using mirror formula, explain why does a convex mirror always produce a virtual image.

    Solution

    a) 
    Given, 
    Radius of curvature, R = 20 cm
    So, focal length, f = R/2 = - 10 cm
    Since the image obtained is real, therefore magnification of the image, m = -2 
    Now, using the formula, 

    space space space space straight m space equals space fraction numerator negative straight v over denominator straight u end fraction
rightwards double arrow space minus 2 space equals space fraction numerator negative straight v over denominator straight u end fraction space
rightwards double arrow space straight v space equals space 2 straight u space

Using space the space mirror space formula comma space

1 over straight f space equals space 1 over straight v space plus space 1 over straight u

space space space space space equals space fraction numerator 1 over denominator 2 straight u end fraction space plus space space 1 over straight u space equals space fraction numerator 3 over denominator 2 straight u end fraction
rightwards double arrow space straight u space equals space begin inline style 3 over 2 end style space straight f space
space space space space space space space space space equals space 3 over 2 space straight x space left parenthesis negative 10 right parenthesis space
space space space space space space space space space equals space minus 15 space cm space

Therefore comma space

straight v space equals space space 2 straight u space equals space minus 30 space cm
    Therefore, the distance of the object is 15 cm in front of the mirror and the position of the image is  30 cm, formed in front of the mirror. 
    b) 
    For a convex mirror, 
    Focal length, f > 0 
    Position of the object, u < 0
    Using mirror formula, we have
    space space space space space space space space 1 over straight f space equals space 1 over v space plus space 1 over u

rightwards double arrow space space 1 over v space equals space space space 1 over straight f space minus space 1 over u

rightwards double arrow space 1 over v space greater than space 0 space

therefore space straight v thin space greater than space 0 space
    That is, the image formed by a convex lens is always behind the mirror and hence is virtual. 

    Question 948
    CBSEENPH12039302

    (i) State Bohr's quantization condition for defining stationary orbits. How does the de Broglie hypothesis explain the stationary orbits?

    (ii) Find the relation between three wavelengths λ1, λ2 and λ3  from the energy-level diagram shown below.


    Solution

    Bohr's Quantisation Rule: 
    According to Bohr, an electron can revolve only in certain discrete, non-radiating orbits for which the total angular momentum of the revolving electron is an integral multiple of fraction numerator straight h over denominator 2 straight pi end fraction ; where h is the Planck's constant. 
    That is,    mvr space equals space fraction numerator nh over denominator 2 straight pi end fraction
    b) 
    Using Rydberg's formula for spectra of hydrogen atom, we have
    1 over straight lambda subscript 1 space equals space R space open parentheses 1 over n subscript 2 squared space minus space 1 over n subscript 3 squared close parentheses space space space space space space space space space space space space... space left parenthesis 1 right parenthesis thin space

1 over straight lambda subscript 2 space equals space R space open parentheses 1 over n subscript 1 squared space minus space 1 over n subscript 2 squared close parentheses space space space space space space space space space space space space... space left parenthesis 2 right parenthesis thin space

1 over straight lambda subscript 3 equals space R space open parentheses 1 over n subscript 1 squared space minus space 1 over n subscript 3 squared close parentheses space space space space space space space space space space space space space... space left parenthesis 3 right parenthesis thin space

Now comma space adding space left parenthesis 1 right parenthesis thin space and space left parenthesis 2 right parenthesis comma space we space get

1 over straight lambda subscript 1 space plus space 1 over straight lambda subscript 2 space equals space space R space open parentheses 1 over n subscript 1 squared space minus space 1 over n subscript 3 squared close parentheses space equals space 1 over straight lambda subscript 3 space semicolon space
    Hence, the relation between 3 wavelengths from the energy-level diagram is obtained. 

    Question 949
    CBSEENPH12039303

    Draw a schematic ray diagram of a reflecting telescope showing how rays coming from a distant object are received at the eyepiece. Write its two important advantages over a refracting telescope.

    Solution

    A reflecting telescope is as shown below: 
     
    In a reflecting telescope, an image is formed by reflection from a curved mirror. The image formed is then magnified by a secondary mirror. 
    Advantages of reflecting telescope over a refracting telescope are:
    1. There is no chromatic aberration for reflecting telescopes as the objective is a mirror. 
    2. Spherical aberration is reduced in the case of reflecting telescopes by using mirror objective in the form of a paraboloid. 

    Question 950
    CBSEENPH12039304

    Meeta's father was driving her to school. At the traffic signal, she noticed that each traffic light was made of many tiny lights instead of a single bulb. When Meeta asked this question to her father, he explained the reason for this.

    Answer the following questions based on above information:

    (i) What were the values displayed by Meeta and her father?

    (ii) What answer did Meeta's father give?

    (iii) What are the tiny lights in traffic signals called and how do these operate?

    Solution

    i)
    The values displayed by Meeta and her father are:
    Meeta: Curious mind
    Meeta's Father: knowledge and patience
    ii)
    The answer that Meeta's father had given would be the advantages of using LED lights over a single bulb. 
    Advantages of LED: 
    a) LED's consume very less power as compared to an incandescent bulb. 
    b) The cost of tiny LED is much less than of a bulb. This reduces the maintenance cost of LED bulbs. 
    c) The working of the traffic will remain unhindered even if one of the bulbs is not working. 
    iii) 
    The tiny lights are called LED (Light Emitting Diode) and they work on the principle of de-excitation of electrons in a forward biased semiconductor upon passing electricity through them. 

    Question 951
    CBSEENPH12039307

    (i) In Young's double-slit experiment, deduce the condition for (a) constructive and (b) destructive interference at a point on the screen. Draw a graph showing variation of intensity in the interference pattern against position 'x' on the screen.

    (b) Compare the interference pattern observed in Young's double-slit experiment with single-slit diffraction pattern, pointing out three distinguishing features.

    Solution

    Expression for fringe width in Young's Double Slit Experiment

    Let S1 and S2 be two slits separated by a distance d.
    GG' is the screen at a distance D from the slits S1 and S2.
    Point C is equidistant from both of the slits.
    The intensity of light will be maximum at this point because the path difference of the waves reaching this point will be zero. 
    At point P, the path difference between the rays coming from the slits is given by, 
    S1 = S2 P - S1
    Now, S1 S2 = d, EF = d, and S2 F = D
    In increment straight S subscript 2 PF
    S2P = S subscript 2 P space equals space square root of straight S subscript 2 straight F squared plus PF squared end root space

S subscript 2 P italic space italic equals italic space open square brackets D to the power of italic 2 italic space italic plus italic space open parentheses x italic plus begin display style d over italic 2 end style close parentheses to the power of italic 2 over D to the power of italic 2 close square brackets to the power of begin inline style bevelled italic 1 over italic 2 end style end exponent

italic space italic space italic space italic space italic space italic space italic space italic space italic space italic equals italic space D italic space open square brackets italic 1 italic plus open parentheses x italic plus begin display style d over italic 2 end style close parentheses to the power of italic 2 over D to the power of italic 2 close square brackets to the power of begin inline style bevelled italic 1 over italic 2 end style end exponent

S i m i l a r l y italic comma italic space i n italic space italic increment S subscript italic 1 P E italic comma

S subscript italic 1 P italic space italic equals italic space D italic space open square brackets italic 1 italic plus italic 1 over italic 2 open parentheses x italic plus d over italic 2 close parentheses to the power of italic 2 over D to the power of italic 2 close square brackets italic space italic minus italic space D open square brackets italic 1 italic plus italic 1 over italic 2 open parentheses x italic minus d over italic 2 close parentheses to the power of italic 2 over D to the power of italic 2 close square brackets

O n italic space e x p a n d i n g italic space b i n o m i a l l y italic comma italic space w e italic space g e t

S subscript italic 2 P italic space italic minus italic space S subscript italic 1 P italic space italic equals italic space fraction numerator italic 1 over denominator italic 2 D end fraction open square brackets italic 4 x d over italic 2 close square brackets italic space italic equals italic space fraction numerator x d over denominator D end fraction 
    For constructive interference, the path difference is an integral multiple of wavelengths, that is, path difference is nstraight lambda.
    Therefore comma space

nλ space equals space xd over straight D

straight x space equals space nλD over straight d semicolon space where space straight n space equals space 0 comma 1 comma 2 comma 3 comma 4 comma....

Similarly space for space destructive space interference comma space

straight x subscript straight n space equals space left parenthesis 2 straight n minus 1 right parenthesis space straight lambda over 2 straight D over straight d
    Graph of intensity distribution in young's double slit experiment is, 
     
    ii) 
    Three distinguishing features observed in Young's Double Slit experiment as compared to single slit diffraction pattern is,
    1. In the interference pattern, all the bright fringes have the same intensity. The bright fringes are not of the same intensity in a diffraction pattern. 
    2. In interference pattern, the dark fringes have zero or small intensity so that the bright and dark fringes can be easily distinguished. While in diffraction pattern, all the dark fringes are not of zero intensity.
    3. In interference pattern, the width of all fringes are almost the same, whereas in diffraction pattern, the fringes are of different widths. 

    Question 952
    CBSEENPH12039308

    (i) Plot a graph to show variation of the angle of deviation as a function of angle of incidence for light passing through a prism. Derive an expression for refractive index of the prism in terms of angle of minimum deviation and angle of prism.

    (ii) What is dispersion of light? What is its cause? 

    (iii) A ray of light incident normally on one face of a right isosceles prism is totally reflected, as shown in fig. What must be the minimum value of refractive index of glass? Give relevant calculations.



    Solution

    i)

    If the angle of incidence is increased gradually, then the angle of deviation first decreases, attains a minimum value (straight delta subscript straight m) and then again starts increasing.

    When angle of deviation is minimum, the prism is at a minimum deviation position. 
    When space straight delta space equals space straight delta subscript straight m comma space

straight e space equals space straight i space and space straight r subscript 2 space equals space straight r subscript 1 space equals space straight r space space space space space space space space space space space... space left parenthesis straight i right parenthesis

because space straight r subscript 1 space plus space straight r subscript 2 space equals space straight A

From space left parenthesis straight i right parenthesis comma space we space get

straight r space plus space straight r space equals space straight A

straight r space space equals space straight A over 2
Also comma space we space have

straight A space plus space straight delta space equals space straight i space plus space straight e

Substituting space straight delta space equals space straight delta subscript straight m space and space straight e space equals space straight i comma

straight A space plus space straight delta subscript straight m space equals space straight i space plus space straight i space

straight i space equals space fraction numerator open parentheses straight A space plus space straight delta subscript straight m close parentheses over denominator 2 end fraction

because space straight mu space equals space fraction numerator sin space straight i over denominator sin space straight r end fraction

Therefore comma space

straight mu space equals space fraction numerator sin space open parentheses fraction numerator straight A space plus space straight delta subscript straight m over denominator 2 end fraction close parentheses over denominator sin space open parentheses begin display style straight A over 2 end style close parentheses end fraction
    ii) 
    The splitting of light into its component colors is known as dispersion of light. 
    When a narrow beam of light is incident on a glass prism, the emergent light splits into seven colours called VIBGYOR. 
    Reason for dispersion: The colors in the spectrum have different wavelengths. The wavelength of violet light is smaller than that of red light. the refractive index of a material in terms of the wavelength of the light is given by the Cauchy's expression. 
    straight mu space equals space straight a space plus space straight b over straight lambda squared space plus space straight c over straight lambda to the power of 4 ; where a, b and c are constants. 
    Thus the refractive index is different for different colours and hence, dispersion occurs. 
    iii) 


    The light which is incident normally on one face of a right-angled isosceles triangle prism is totally reflected.
    straight mu space equals space fraction numerator 1 over denominator sin space straight c end fraction space semicolon space where space straight c space is space the space critical space angle space equals space 45 to the power of straight o

Therefore comma space

straight mu space equals space fraction numerator 1 over denominator sin space 45 to the power of straight o end fraction

straight mu space equals space square root of 2 space equals space 1.41 space
    Therefore, minimum value of the refractive index of the glass is 1.41
    Question 953
    CBSEENPH12039333

    Name the essential components of a communication system.

    Solution

    Essential components of communication system:
    1. Transmitter
    2. Channel
    3. Receiver

    Question 954
    CBSEENPH12039334

    Why does sun appear red at sunrise and sunset?

    Solution

    Sun appears red at sunrise and sunset because of least scattering of red light as it has the lowest wavelength.
    As per Rayleigh scattering, the amount of light scattered proportional to space 1 over straight lambda to the power of 4.

    Question 955
    CBSEENPH12039336

    Define modulation index. Why is it kept low ? What is the role of a bandpass filter?

    Solution

    Modulation index is the ratio of the amplitude of modulating signal to that of carrier wave.
    straight mu space equals space straight A subscript straight m over straight A subscript straight C
    Modulation index is kept low in order to avoid distortion. The low frequency modulating signal is mixed with high-frequency carrier wave, the distortion is restricted due the high-frequency carrier wave for modulation index lying between 0 and 1.
    Bandpass filter rejects low and high frequencies and allows a band of frequencies to pass through.

    Question 957
    CBSEENPH12039338

    Calculate the de-Broglie wavelength of the electron orbitting in the n=2 state of hydrogen atom.

    Solution

    Given,
    n =2
    K.E for the second state, Ek,
     fraction numerator 13.6 over denominator straight n squared end fraction space equals space fraction numerator 13.6 over denominator 4 end fraction
space space space space space space space space space space space equals space 3.4 space x space 1.6 space x space 10 to the power of negative 19 end exponent space J
    De-Broglie wavelength, straight lambda space equals space fraction numerator straight h over denominator square root of 2 mE subscript straight k end root end fraction
       equals space fraction numerator 6.63 space straight x space 10 to the power of negative 34 end exponent over denominator square root of 2 space straight x space 9.1 space straight x space 10 to the power of negative 31 end exponent straight x 3.4 straight x 1.6 straight x 10 to the power of negative 19 end exponent end root end fraction

equals space 0.067 space straight m

    Question 958
    CBSEENPH12039339

    Define ionisation energy.

    How would the ionisation energy change when electron in hydrogen atom is replaced by a particle of mass 200 times that of the electron but having the same charge ?

    Solution

    The minimum energy, required to free the electron from the ground state of the hydrogen atom, is known as ionization energy.
    Ionisation energy is given by,
    space space space space space space space straight E subscript straight o space equals space fraction numerator me to the power of 4 over denominator 8 straight epsilon subscript straight o squared straight h squared end fraction
straight i. straight e. comma space straight E subscript straight o space proportional to space straight m
    Since, ionisation energy is directly proportional to mass, the Ionization energy will become 200 times.

    Question 959
    CBSEENPH12039340
    Question 960
    CBSEENPH12039343

    (i) State law of Malus.

    (ii) Draw a graph showing the variation of intensity (I) of polarised light transmitted by an analyser with angle (straight theta) between polarizer and analyser.
    (iii) What is the value of refractive index of a medium of polarising angle 60o?

    Solution

    i) Law of Malus states that when a completely plane polarised light beam is incident on an analyser, the intensity of the emergent light varies as the square of the cosine of the angle between the plane of transmission of the analyser and the polariser.
                                   I = Io cos2straight theta
    ii) The variation of intensity (I) of polarised light transmitted by an analyser with angle straight theta.


    iii) According to the Brewster's law, we have
    straight mu space equals space tan space straight i subscript straight p

straight mu space equals space tan space 60 to the power of straight o

straight mu space equals space square root of 3
    The refractive index of the material is 1.73
     
    Question 961
    CBSEENPH12039344

    Sketch the graphs showing variation of stopping potential with frequency of incident radiations for two photosensitive materials A and B having threshold frequencies straight nuA > straight nuB.

    (i) In which case is the stopping potential more and why?

    (ii) Does the slope of the graph depend on the nature of the material used? Explain.

    Solution

    Graph showing the variation of stopping potential with frequency of incident radiations:


    From the above graph, we can observe that,
    i) The stopping potential is inversely proportional to the threshold frequency. Hence, the stopping potential is higher for metal B.
    ii)The slope of the graph does not depend on the nature of the material used:
    We know that,
    straight K subscript max space equals space hν space minus straight ϕ subscript straight o space equals space eV subscript straight o
    Dividing the equation throughout by e, we get
    hν over straight e minus ϕ subscript o over e space equals space V subscript o
    On comparing the above equation with the straight line equation, we get
    Slope of the graph = straight h over straight e
    That is, the slope of the graph does not depend on the nature of the material used.

    Question 962
    CBSEENPH12039345

    a) Write the basic nuclear process involved in the emission of beta plus in a symbolic form, by a radioactive nucleus.

    b) In the reactions given below:

    i right parenthesis space straight C presubscript 6 presuperscript 11 space rightwards arrow space straight B presubscript straight y presuperscript straight z plus space straight x plus straight nu
ii right parenthesis space straight C presubscript 6 presuperscript 12 space plus straight C presubscript 6 presuperscript 12 space rightwards arrow space Ne presubscript straight a presuperscript 20 space plus space He presubscript straight b presuperscript straight c
    Find the values of x, y and z and a, b and c.

    Solution

    a)
    The basic nuclear process involved in the emission of beta plus in a symbolic form, by a radioactive nucleus,
    straight p space rightwards arrow space straight n space plus space straight beta to the power of plus plus straight nu
    In a beta-plus decay, a proton transforms into a neutron within the nucleus.
    b)
    i) straight C presubscript 6 presuperscript 11 space rightwards arrow space straight B presubscript 5 presuperscript 11 space plus space straight beta presubscript 1 presuperscript 0 space plus space straight nu
    The corresponding y and z are 5 and 11 respectively.
    Here, x is the positron.
    ii) straight C presubscript 6 presuperscript 12 space plus straight C presubscript 6 presuperscript 12 space rightwards arrow space Ne presubscript 10 presuperscript 20 space plus space He presubscript 2 presuperscript 4
    The corresponding values of a, b and c are 10, 2 and 4 respectively.

    Question 963
    CBSEENPH12039348

    (i) Explain with the help of a diagram the formation of depletion region and barrier potential in a p-n junction.

    (ii) Draw the circuit diagram of a half wave rectifier and explain its working.

    Solution

    i) 

    In a p-n junction, a p-type and an n-type material are joined together. P-type has a higher concentration of holes and n-type has a higher concentration of electrons. Hence, there is a concentration gradient between the p-type and n-type materials. Therefore, holes drift from p-side to n-side by the process of diffusion due to concentration gradient. In a similar manner, electrons move from n-side to p-side.
    As a result of the movement of holes from p-side, they leave ionised spaces (negative charge) on p-side near the junction. Similarly, a positive space charge region is formed on the n-side due to the diffusion of electrons from n-side. The two space charge regions on either side of the junction is called as depletion region.
    A potential difference is developed across the junction of two regions, which is known as the barrier potential. The reverse polarity of this potential opposes further flow of carriers.
    ii) Half wave rectifier:


    Working: When an alternating voltage is applied across a diode in series with a load, a pulsating voltage will appear across the load only during that half cycle on the AC input during which the diode is forward biased.
    In the positive half cycle of AC input, a current flows through load resistance RL and we get the output voltage.
    In the negative half cycle, there is no output. Therefore, the output voltage is restricted to only one direction and is said to be rectified.
    Question 964
    CBSEENPH12039349

    (i) Which mode of propagation is used by shortwave broadcast services having frequency range from a few MHz upto 30 MHz ? Explain diagrammatically how long distance communication can be achieved by this mode.

    (ii) Why is there an upper limit to frequency of waves used in this mode?

    Solution

    i) Sky-wave propagation is used for long distance communication. Long distance communication is achieved by reflection of radio waves by the ionosphere, back towards the earth. This ionosphere layer acts as a reflector for certain range of frequencies from few MHz to 30 MHz.


    ii) There is an upper limit to the frequency of waves used in sky wave propagation because electromagnetic waves of frequencies higher than 30MHz, penetrate the ionosphere and escape whereas waves less than 30 MHz are reflected back to the earth by the ionosphere.
    Question 965
    CBSEENPH12039351

    For a CE-transistor amplifier, the audio signal voltage across the collector resistance of 2 kstraight capital omega is 2 V. Suppose the current amplification factor of the transistor is 100, find the input signal voltage and base current, if the base resistance is 1 kV.

    Solution

    Given,
    Output voltage, Vo = 2 V
    Output resistance, Ro = 2 kstraight capital omega
    Base resistance, Ri = 1 kstraight capital omega
    Current amplification factor, straight beta space equals space 100
    Then input signal voltage is,
    space space space straight V subscript straight o over Vf space equals space R subscript o over R subscript f space cross times beta
space space 2 over V subscript f space equals space 2 over 1 x 100
rightwards double arrow space V subscript i space equals space 10 space m V
    Now, collector current is,
    ICstraight V subscript straight o over straight R subscript straight o space equals space 2 over 2 space equals space 1 space m A
    Therefore,
    Base current, IB straight I subscript straight C over straight beta space equals space fraction numerator 1 space m A over denominator 100 end fraction equals 10 mu A

    Question 966
    CBSEENPH12039352

    Define the term wave front. State Huygen’s principle.

    Consider a plane wave front incident on a thin convex lens. Draw a proper diagram to show how the incident wave front traverses through the lens and after refraction focusses on the focal point of the lens, giving the shape of the emergent wave front.


                                                                         OR


    Explain the following, giving reasons :

    (i) When monochromatic light is incident on a surface separating two media, the reflected and refracted light both have the same frequency as the incident frequency.

    ii) When light travels from a rarer to a denser medium, the speed decreases. Does this decrease in speed imply a reduction in the energy carried by the wave?

    (iii) In the wave picture of light, intensity of light is determined by the square of the amplitude of the wave. What determines the intensity in the photon picture of light?

    Solution

    Wavefront is defined as the locus of all the points in space that reach a particular distance by a propagating wave at the same instant.
    Huygen's principle:
    i) Each point of the wavefront is the source of a secondary disturbance and the wavelets emanating from these points spread out in all directions. These travel with the same velocity as that of the original wavefront.
    ii) The shape and position of the wave-front, after time 't', is given by the tangential envelope to the secondary wavelets.
    A plane wavefront is incident on a thin convex lens:

                                                        OR

    i) Reflection and refraction arise through interaction of incident light with atomic constituents of matter which vibrate with the same frequency as that of the incident light. Hence, frequency remains unchanged.
    ii) No, energy carried by a wave depends on the amplitude of the wave, not on the speed of wave propagation.
    iii) For a given frequency, intensity of light in the photon picture is determined by the number of photon incident normally on crossing unit area per unit time.

    Question 967
    CBSEENPH12039357

    (i) Derive the mathematical relation between refractive indices n1 and n2 of two radii and radius of curvature R for refraction at a convex spherical surface. Consider the object to be a point since lying on the principle axis in rarer medium of refractive index n1 and a real image formed in the denser medium of refractive index n2. Hence, derive lens maker’s formula.

    (ii) Light from a point source in air falls on a convex spherical glass surface of refractive index 1.5 and radius of curvature 20 cm. The distance of light source from the glass surface is 100 cm. At what position is the image formed ?

    Solution
    i)
    The figure given above shows the geometry of formation of real image I of an object O and the principal axis of a spherical surface with centre of curvature c and radius of curvature R.
    Assumptions:
    1. The aperture of the surface is small compared to other distance involved.
    2. NM is taken to be nearly equal to to the length of the perpendicular from the point N on the principal axis.
    tan space angle N O M space equals space fraction numerator M N over denominator O M end fraction
tan space angle N C M space equals space fraction numerator M N over denominator M C end fraction
tan space angle N I M space equals space fraction numerator M N over denominator M I end fraction
F o r space increment N O C comma
i space i s space t h e space e x t e r i o r space a n g l e.
    Assuming the incident ray is very close to the principal axis, all the angles are very small. Hence, for small angles,
    tan x = x = sin x
    Therefore,
    straight i space equals space angle NOM plus angle NCM

straight i space equals space MN over OM plus MN over MC space bold space bold. bold. bold. bold space bold left parenthesis bold i bold right parenthesis

Similarly comma

space straight r space equals space angle NCM space minus space angle NIM

straight r equals space MN over MC space minus space MN over MI space bold space bold. bold. bold. bold space bold left parenthesis bold ii bold right parenthesis

Using space Snell apostrophe straight s space law comma

straight n subscript 1 space sin space straight i space equals space straight n subscript 2 space sin space straight r

For space small space angles comma

straight n subscript 1 straight i space equals space straight n subscript 2 space straight r
    Putting the values of i and r from eqns. from (i) and (ii), we have
    straight n subscript 1 open parentheses MN over OM plus MN over MC close parentheses space equals space straight n subscript 2 open parentheses MN over MC minus MN over MI close parentheses

straight n subscript 1 over OM plus straight n subscript 2 over MI equals fraction numerator space straight n subscript 2 minus straight n subscript 1 over denominator MC end fraction space bold. bold. bold. bold space bold left parenthesis bold iii bold right parenthesis
    Applying new cartesian sign conventions,
    OM = -u, MI = + v, MC = +R
    Putting these values in equation (iii), we have
    straight n subscript 2 over straight v minus n subscript 1 over u space equals space fraction numerator n subscript 2 minus n subscript 1 over denominator R end fraction
    ii) According to the question,

    space space space straight n subscript 2 over straight v minus n subscript 1 over u equals fraction numerator n subscript 2 minus n subscript 1 over denominator R end fraction

rightwards double arrow space fraction numerator 1.5 over denominator V end fraction minus fraction numerator 1 over denominator left parenthesis negative 100 right parenthesis end fraction equals fraction numerator 1.5 minus 1 over denominator 20 end fraction
space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space space equals space 1 over 40
rightwards double arrow space fraction numerator 1.5 over denominator V end fraction equals 1 over 40 minus 1 over 100
space space space space space space space space space space space space space space equals fraction numerator 5 minus 2 over denominator 200 end fraction
space space space space space space space space space space space space space space equals space 3 over 200
rightwards double arrow space v space equals space fraction numerator 1.5 space x 200 over denominator 3 end fraction
space space space space space space space space space equals 100 space c m
    Therefore, the image is formed at a distance of 100 cm in the denser medium.
    Question 968
    CBSEENPH12039358

    (a) Draw a labelled ray diagram to obtain the real image formed by an astronomical telescope in normal adjustment position. Define its magnifying power.

    (b) You are given three lenses of power 0.5 D, 4 D and 10 D to design a telescope.

    (i) Which lenses should he used as objective and eyepiece ? Justify your answer.

    ii) Why is the aperture of the objective preferred to be large?

    Solution

    a) The image formed by an astronomical telescope in normal adjustment position is given below,


    In normal adjustment, the image is formed at infinity.
    Magnification power is defined as the angle subtended at the eye, by the final image, to the angle subtended at the eye, by the object directly, when the final image and the object both are at infinity.
    Mathematically, it is given by
    Magnification, m = straight beta over straight alpha
    Since straight alpha space and space straight beta are very small,
    straight beta space equals space tan space straight beta
straight alpha space equals space tan space straight alpha
rightwards double arrow straight m equals space fraction numerator tan space straight beta over denominator tan space straight alpha end fraction
    b) Given, three lenses of power 0.5 D, 0.4 D and 10 D.
    i) The formula for magnification, M = straight f subscript straight o over straight f subscript straight e equals P subscript e over P subscript o
    Therefore, an objective with power = 0.5 D and eyepiece of power 10 D should be used.
    This choice would give a higher magnification.
    ii) The aperture is preferred to be large so that the telescope can collect maximum amount of light coming from the distant object. 
    Question 969
    CBSEENPH12039364
    Question 970
    CBSEENPH12039367

    Define the distance of closest approach. A α-particle of kinetic energy 'K' is bombarded on a thin gold foil. The distance of the closest approach is 'r'. What will be the distance of closest approach for a α-particle of double the kinetic energy?   

    Solution

    It is the distance of charged particle from the centre of the nucleus, at
    which the whole of the initial kinetic energy of the (far off) charged
    particle gets converted into the electric potential energy of the system.
    Distance of closest approach (rc) is given by
    straight r subscript straight c space equals space fraction numerator 1 over denominator 4 πε subscript 0 end fraction. fraction numerator 2 space Ze squared over denominator straight K end fraction
    (rc) is inversely proportional to K. Thus,
    ‘K’ is doubled therefore rc becomes r/2

    Question 971
    CBSEENPH12039368

    Write two important limitations of Rutherford nuclear model of the atom.

    Solution

    1. According to Rutherford model, an electron orbiting around the nucleus continuously radiates energy due to the acceleration; hence the atom will not remain stable.
    2. As electron spirals inwards; its angular velocity and frequency change continuously; therefore it will emit a continuous spectrum.

    Question 972
    CBSEENPH12039369

    Find out the wavelength of the electron orbiting in the ground state of the hydrogen atom.

    Solution

    Radius of ground state of hydrogen atom =0.53A°  = 0.53 x10-10m
    According to de Broglie relation 2πr = nλ
    For ground state n=1
    2 x 3.14 x 0.53 x 10-10= 1 x λ
    therefore, λ = 3.32 x10-10 m
    = 3.32 A° 

    Question 973
    CBSEENPH12039370

    Define the magnifying power of a compound microscope when the final image is formed at infinity. Why must both the objective and the eyepiece of a compound microscope has short focal lengths? Explain.

    Solution

    Magnifying power is defined as the angle subtended at the eye by the image
    to the angle subtended (at the unaided eye) by the object.
    straight m space equals space straight m subscript straight o space straight x space straight m subscript straight e space equals space straight L over straight f subscript straight o space straight x straight D over straight f subscript straight e

    To increase the magnifying power both the objective and eyepiece must have short focal lengths such as straight m space space equals space straight L over straight f subscript straight o space straight x straight D over straight f subscript straight e 

    Question 974
    CBSEENPH12039371

    Which basic mode of communication is used in satellite communication? What type of wave propagation is used in this mode? Write, giving a reason, the frequency range used in this mode of propagation.

    Solution

    There are two basic modes of communication which are used in satellite communication:
    (i) point-to-point and broadcast-  In the broadcast mode, there are a large number of receivers corresponding to a single transmitter. Satellite communication is an example of the broadcast mode of communication.

    (ii) Space wave mode of propagation: In the frequency range 30 MHz to 1000 Mhz, the wavelengths are in the range of 30 cm to 10 m. At these wavelengths the diffraction of waves is high and the waves lose their directional property. So frequency range of 5.925 - 6.425 GHz is used in satellite communication.

    Question 975
    CBSEENPH12039373

    Write the two processes that take place in the formation of a p-n junction. Explain with the help of a diagram, the formation of the depletion region and barrier potential in a p-n junction.  

    Solution

    Diffusion and Drift are the two processes that take place in the formation of a p-n junction.

    In an n-type semiconductor, the concentration of electrons (number of electrons per unit volume) is more compared to the concentration of holes. Similarly, in a P -type semiconductor, the concentration of holes is more than the concentration of electrons. During the formation of p-n junction.
    Due to the diffusion of electrons and holes across the junction a region of
    (immobile) positive charge is created on the n-side and a region of(immobile) negative charge is created on the p-side, near the junction; this is called depletion region.

    Barrier potential is formed due to loss of electrons from n-region and gain of electrons by p-region. Its polarity is such that it opposes the movement of charge carriers across the junction.

    Question 976
    CBSEENPH12039374

    (i) Obtain the expression for the cyclotron frequency.
    (ii) A deuteron and a proton are accelerated by the cyclotron. Can both be accelerated with the same oscillator frequency? Give reason to justify your answer.

    Solution

    When a charged particle (q) moves inside a magnetic field B with velocity v, it experiences a force F = q(v xB) when v is perpendicular to B, the force F on the charged acts as the centripetal force and makes it move along a circular path.
    Let m be the mass of particle and r is radius  of circular path
    straight q space left parenthesis straight v with rightwards arrow on top space straight x straight B with rightwards arrow on top right parenthesis space equals space mv squared over straight r
qvB space equals space mv squared over straight r
rightwards double arrow space straight r space equals space mv over Bq
    Time period of the circular motion of a charged particle is given by
    straight T space equals space fraction numerator 2 πr over denominator straight v end fraction
space equals fraction numerator 2 πmv over denominator straight v space Bq end fraction
rightwards double arrow space straight T space equals space fraction numerator 2 πm over denominator Bq end fraction
Angular space frequency space comma
straight omega space equals space fraction numerator 2 straight pi over denominator straight T end fraction
therefore space straight omega space equals space Bq over straight m
    ii) No, The mass of the two particles, i.e deuteron and proton, is different.Since (cyclotron) frequency depends inversely on the mass, they cannot be accelerated by the same oscillator frequency.

    Question 977
    CBSEENPH12039375

    How does one explain the emission of electrons from a photosensitive surface with the help of Einstein's photoelectric equation?

     

    Solution

    Einstein’s Photoelectric equation is
    hv space equals space straight phi subscript 0 space plus straight K subscript max
    When a photon of energy is incident on the metal, some part of this
    energy is utilized as work function to eject the electron and remaining
    energy appears as the kinetic energy of the emitted electron.

    Question 978
    CBSEENPH12039376

    The work function of the following metals is given : Na 2.75 ev, K = 2.3 eV, Mo = 4.17 eV and Ni = 5.15 eV. Which of these metals will not cause photoelectric emission for radiation of wavelength 3300 Å from a laser source placed 1 m away from these metals? What happens if the laser source is brought nearer and placed 50 cm away?

    Solution
    straight E space equals space hc over straight lambda space equals space fraction numerator 6.63 space straight x 10 to the power of negative 34 end exponent space straight x space 3 space straight x space 10 to the power of 8 over denominator 3.3 space straight x space 10 to the power of negative 7 end exponent space straight x 1.6 space straight x 10 to the power of negative 19 end exponent end fraction eV
space equals space 3.77 space eV

    The work function of Mo and Ni is more than the energy of the incident
    photons; so photoelectric emission will not take place from these metals.
    Kinetic energy of photo electrons will not change, only photoelectric current
    will change.

    Question 979
    CBSEENPH12039378

    Define the term 'amplitude modulation'. Explain any two factors which justify the need for modulating a low-frequency base band signal.

    Solution

    It is the process of superposition of information/message signal over a carrier wave in such a way that the amplitude of carrier wave is varied according to the information signal/message signal.
    Direct transmission, of the low frequency base band information signal, is not possible due to the following reasons;
    (i) Size of Antenna: For transmitting a signal, minimum height of the antenna should be λ/4; with the help of modulation wavelength of signal decreases, hence the height of antenna becomes manageable.
    (ii) Effective power radiated by an antenna: Effective power radiated by an antenna varies inversely as λ2, hence effective power radiated into the space, by the antenna, increases.
    (iii)To avoid mixing up of signals from different transmitters.

    Question 980
    CBSEENPH12039382

    A radioactive nucleus 'A' undergoes a series of decays as given below:
    straight A space rightwards arrow with straight alpha on top space straight A subscript 1 space rightwards arrow with straight beta on top space straight A subscript 2 space rightwards arrow with straight alpha on top space straight A subscript 3 space rightwards arrow with straight gamma on top space straight A subscript 4
    The mass number and atomic number of A2 are 176 and 71 respectively. Determine the mass and atomic number of A4 and A.

    Solution

    straight A subscript 74 superscript 180 space rightwards arrow with space straight alpha space on top space straight A subscript 72 superscript 176 space rightwards arrow with space straight beta on top space straight A subscript 71 superscript 176 space rightwards arrow with straight alpha on top space straight A subscript 69 superscript 172 space rightwards arrow with straight gamma on top straight A subscript 69 superscript 172
    The mass number and atomic number of A4 is 172 and 69, respectively.
    The mass number and atomic number of A is 180 and 74, respectively.

    Question 981
    CBSEENPH12039383

    Write the basic nuclear process underlying β+ and β- decays.

    Solution

    Basic process underlying  β+ and  β- decay are
    During a weak interaction an atomic nucleus converts into a nucleus with one higher atomic number while emitting one electron and an electron antineutrino this is called beta minus decay.
    straight X subscript straight Z superscript straight A space rightwards arrow with space on top space straight Y subscript straight Z plus 1 end subscript superscript straight A space plus straight e to the power of minus space plus top enclose straight v subscript straight e end enclose

    During a weak interaction an atomic nucleus converts into a nucleus with one Lower atomic number while emitting one electron and an electron neutrino this is called beta minus decay.
    straight X subscript straight Z superscript straight A space rightwards arrow with space on top space straight Y subscript straight Z plus 1 end subscript superscript straight A space plus straight e to the power of plus space plus straight v subscript straight e

    Question 983
    CBSEENPH12039385

    Mrs Rashmi Singh broke her reading glasses. When she went to the shopkeeper to order new specs, he suggested that she should get spectacles with plastic lenses instead of glass lenses. On getting the new spectacles, she found that the new ones were thicker than the earlier ones. She asked this question to the shopkeeper but he could not offer a satisfactory explanation for this. At home, Mrs Singh raised the same question to her daughter Anuja who explained why plastic lenses were thicker.

    (a) Write two qualities displayed each by Anuja and her mother.

    (b) How do you explain this fact using lens maker's formula?

    Solution

    (a) Two qualities displayed each by Anuja and her mother:
    Anuja has good knowledge of lens and she is very co-operative.
    Mrs Rashmi is curious to know about lenses and science behind it.
    (b)The lens maker formula is given as  1 over straight f space space equals open parentheses straight mu minus 1 close parentheses space open parentheses 1 over straight R subscript 1 minus 1 over straight R subscript 2 close parentheses

    where f is the focal length, μ is the refractive index and R1 and R2 is the radius of curvature of the lens.
    Since μgp
    where g stands for glass and p stands for plastic
    Therefore, we get (μ-1)> (μp-1)
    Now, using the lens maker formula, we see that focal length is inversely proportioned to (μ-1)
    Hence, fp>fg
    Thus, in the case of the plastic lens, the thickness of the lens should be increased to keep the same focal length as that of the glass lens to give the same power.

    Question 984
    CBSEENPH12039386

    (i) A ray of light incident on face AB of an equilateral glass prism shows the minimum deviation of 30°. Calculate the speed of light through the prism.


    (ii) Find the angle of incidence at face AB so that the emergent ray grazes along the face AC.

    Solution


    At the minimum deviation, the refracted ray inside the prism becomes parallel to its base.
    Angle of minimum deviation is given as Dm = 30°
    Since, the prism is equilateral, So, A = 60° 
    Refractive index of the prism
    straight mu space equals space fraction numerator Sin space open parentheses begin display style fraction numerator straight A space plus space straight D subscript straight m over denominator 2 end fraction end style close parentheses over denominator Sin space begin display style straight A over 2 end style end fraction
space equals space fraction numerator Sin space begin display style 90 over 2 end style over denominator Sin space begin display style 60 over 2 end style end fraction
space equals space fraction numerator begin display style fraction numerator 1 over denominator square root of 2 end fraction end style over denominator 1 divided by 2 end fraction space equals space square root of 2

    We know that μ = v1/v2
    Hence the speed of light in prism would be 1/√2 times the speed of light in air i.e = 3 x108 /1.414 = 2.121 x108 m/s
    (ii) 

    From Snell's law, we know that fraction numerator sin space straight i over denominator sin space straight r end fraction space equals space straight mu subscript 12
    For the emergent ray to graze at the face AC, the angle of refraction should be 90
    So, applying snell's law at face AC, we get
    fraction numerator sin space straight i subscript AC over denominator sin space straight r subscript AC end fraction space equals space straight mu subscript 21 space rightwards double arrow space fraction numerator sin begin display style space end style begin display style begin display style straight i end style subscript AC end style over denominator sin begin display style space end style begin display style begin display style 90 end style to the power of straight o end style end fraction space equals space fraction numerator 1 over denominator square root of 2 end fraction space or space straight i subscript AC space equals space 45 to the power of straight o

    From figure, we can see that angle of refraction at face AB is 15
    So applying Snell's law we get
    Sin iAB = sin rAB x μ12
    or iAB = sin-1 (√sin 15°)

    Question 985
    CBSEENPH12039392

    Distinguish between unpolarized light and linearly polarized light. How does one get the linearly polarised light with the help of a polar?

    Solution

    In a beam of unpolarized light, the vibrations of light vectors are in all directions in a plane perpendicular to the direction of propagation. 

    In the linearly polarised light, the vibrations of light take place in a particular direction, perpendicular to the direction of wave motion.

    Polarized light can be distinguished, from unpolarized light, when it is allowed to pass through a Polaroid. Polarized light does can show the change in its intensity, on passing through a Polaroid; intensity remains same in case of unpolarized light.

    When the unpolarised light wave is incident on a polaroid, then the electric vectors along the direction of its aligned molecules, get absorbed; the electric vector, oscillating along a direction perpendicular to the aligned molecules, pass through. This light is called linearly polarized light.

    Question 987
    CBSEENPH12039394

    Explain two features to distinguish between the interference pattern in Young's double slit experiment with the diffraction pattern obtained due to a single slit.

    Solution
    Interference pattern Diffraction pattern 
    1) All fringes are of equal width.  1) The width of central maxima is twice the width of higher order band.
    2) Intensity of all bright bands is equal. 2) The intensity goes on decreasing for a higher order of diffraction bands.
    Question 989
    CBSEENPH12039421

    If one of two identical slits producing interference in Young’s experiment is convered with glass, so that the light intensity passing through it is reduced to 50%, find the ratio of the maximum and minimum intensity of the fringe in the interference pattern.

    Solution

    As we know that intensity is directly proportional to the square of the amplitude.

    I  a2If I1 =I2If intensity reduced to 50%, amplitude will be a2then r = 2thenImaxImin = (r +1)2(r-1)2 = (2+ 1)2(2-1)2ImaxImin = 2.4140.4142 = (5.83)2ImaxImin = 33.98 = 34

    Question 990
    CBSEENPH12039422

    What kind of fringes do you expect to observe if white light is used instead of monochromatic light?

    Solution

    If the White light is used instead of monochromatic light then we see a sequence in which central fringe will be white and remaining will be coloured in VIBGYOR sequence.

    Question 991
    CBSEENPH12039441

    Define a wavefront. Using Huygens’ principle, verify the laws of reflection at a plane surface.

    Solution

    A wavefront is an imaginary surface over which an optical wave has a constant phase. The shape of a wavefront is usually determined by the geometry of the source. 
    Huygen's principle: 
    (i) Every point on a given wavefront acts as a fresh source of secondary wavelets which travel in all directions with the speed of light.
    (ii) The forward envelope of these secondary wavelets gives the new wavefront at any instant. 
    Laws of reflection by Huygen's principle: 
    Let, PQ be reflecting surface and a plane wavefront AB is moving through the medium (air) towards the surface PQ to meet at the point B. 
    Define a wavefront. Using Huygens’ principle, verify the laws of 
    Let, c be the velocity of light and t be the time taken by the wave to reach A' from A. 
    Then,  AA' = ct.

    Using Huygen's principle, secondary wavelets starts from B and cover a distance ct in time t and reaches B'.

    To obtain new wavefront, draw a circle with point B as centre and ct (AA' = BB') as radius. Draw a tangent A'B' from the point A'. 
    Then, A'B' represents the reflected wavelets travelling at right angle. Therefore, incident wavefront AB, reflected wavefront A'B' and normal lies in the same plane. 
    Consider ∆ABA' and B'BA'
    AA' = BB' = ct       [∵ AA' = BB' = BD = radii of same circle]
    BA' = BA'              [common]
    ∠BAA' = ∆BB'A'     [each 90°]
    ∴ ∆ABA' ≅ ∠DBA'    [by R.H.S]
    ∠ABA' = ∠B'A'B    [corresponding parts of congruent triangles] 
    ∴ incident angle i = reflected angle r
    i.e.,                 ∠i = ∠r

    Question 993
    CBSEENPH12039443

    When a tiny circular obstacle is placed in the path of light from a distant source, a bright spot is seen at the centre of the obstacle. Explain why

    Solution

    A bright spot is seen at the centre of the shadow of objective because wave diffracted from the edge of the circular obstacle interface constructively at the centre of the shadow producing a bright spot.

    Question 994
    CBSEENPH12039460

    The temperature dependence of resistances of Cu and undoped Si in the temperature range 300-400 K is best described by:

    • Linear increase for Cu, linear increase for Si.

    • Linear increase for Cu, exponential increase for Si.

    • Linear increase for Cu, exponential decrease for Si.

    • Linear decrease for Cu, linear decrease for Si.

    Solution

    C.

    Linear increase for Cu, exponential decrease for Si.

    As we know Cu is a conductor, so increase in temperature, resistance will increase.  Then, Si is a semiconductor, so with the increase in temperature, resistance will decrease.

    Question 995
    CBSEENPH12039464

    Arrange the following electromagnetic radiations per quantum in the order of increasing energy:

    A: Blue light
    B: Yellow light
    C: X-ray
    D: Radiowave

    • D, B, A, C

    • A, B, D, C

    • C, A, B, D

    • B, A, D, C

    Solution

    A.

    D, B, A, C

    As, we know energy liberated, E = hc/λ
    i.e straight E space proportional to space 1 over straight lambda
    So, lesser the wavelength greater will be energy liberated by electromagnetic radiations per quantum.
    As, order of wavelength is given by
    X- rays, VIBGYOR, Radio waves
    therefore, the order of electromagnetic radiations per quantum.
    D<B<A<C

    Question 996
    CBSEENPH12039465

    An observer looks at a distant tree of height 10 m with a telescope of magnifying power of 20. To the observer the tree appears:

    • 10 times taller.

    • 10 times nearer.

    • 20 times taller.

    • 20 times nearer

    Solution

    C.

    20 times taller.

    The height of image depends upon magnifying rows to see 20 times taller object, angular magnification should be 20 and we observe angular magnification option (c) would not be very correct as the telescope can be adjusted to form the image anywhere between infinity and least distance for distinct vision.Suppose that the image is formed at infinity. Then. the observer will have to focus the eyes at infinity to observe the image. Hence, it is incorrect to say that the image will appear nearer to the observer.

    Question 998
    CBSEENPH12039467

    Radiation of wavelength λ is incident on a photocell. The fastest emitted electron has to speed v. If the wavelength is changed to 3λ/4, the speed of the fastest emitted electron will be:

    • less than straight v space open parentheses 4 over 3 close parentheses to the power of 1 divided by 2 end exponent
    •  = v(4/3)1/2

    • =v(3/4)1/2

    Solution

    A.

    According to the law of conservation of energy, i.e. Energy of a photon (hv) = work function (Φ) + Kinetic energy of the photoelectron (mv2/2)
    according to Einstein's photoelectric emission of light,
    E =(KE)max + Φ
    As, hc/λ = (KE)max + Φ
    If the wavelength of radiation is changed to 3λ/4
    then,
    4 over 3 hc over straight lambda space equals space open parentheses 4 over 3 left parenthesis KE right parenthesis subscript max space plus space straight capital phi over 3 close parentheses plus straight capital phi

For space fastest space emitted space electron comma space left parenthesis KE right parenthesis subscript max space equals space 1 half space mv squared space plus straight capital phi
fraction numerator begin display style 1 end style over denominator begin display style 2 end style end fraction space mv squared space space equals space 4 over 3 space open parentheses 1 half mv squared close parentheses space plus straight capital phi over 3
straight i. straight e comma space straight v apostrophe greater than space straight v open parentheses 4 over 3 close parentheses to the power of 1 divided by 2 end exponent

    Question 999
    CBSEENPH12039468

    Half-lives of two radioactive elements A and B are 20 minutes and 40 minutes, respectively. Initially, the samples have equal number of nuclei. After 80 minutes, the ratio of decayed numbers of A and B nuclei will be:

    • 1: 16

    • 4 : 1

    • 1: 4

    • 5: 4

    Solution

    D.

    5: 4

    Given 80 min = 4 half-lives of A = 2 half-lives of B.
    Let the initial number of nuclei in each sample be N.
    For radioactive element A,
    NA after 80 min = N/24
    ⇒ Number of A nuclides decayed  =straight N minus straight N over 16 space equals space 15 over 16 straight N


    For radioactive element B,
    NB after 80 min  = N/22
    ⇒ Number of B nuclides decayed
    straight N minus straight N over 4 space equals space 3 over 4 straight N
    therefore, the ratio of decayed numbers of A and B nuclei will be
    fraction numerator open parentheses 15 divided by 16 close parentheses straight N over denominator left parenthesis 3 divided by 4 right parenthesis straight N end fraction space equals space 5 over 4
    Question 1000
    CBSEENPH12039469

    If a, b, c, d are inputs to a gate and x is its output, then, as per the following time graph, the gate is:


    • NOT

    • AND

    • OR

    • NAND

    Solution

    C.

    OR

    The output of OR gate is 0 when all inputs are 0 and output is 1 when at least one of the input is 1.
    Observing output x it is 0 when all inputs are 0 and it is 1 when at least one of the inputs is 1.
    therefore, the gate is OR

    Question 1001
    CBSEENPH12039470

    Choose the correct statement:

    • In amplitude modulation, the amplitude of the high-frequency carrier wave is made to vary in proportion to the amplitude of the audio signal.

    • In amplitude modulation, the frequency of the high-frequency carrier wave is made to vary in proportion to the amplitude of the audio signal.

    • In frequency modulation, the amplitude of the high-frequency carrier wave is made to vary in proportion to the amplitude of the audio signal.

    • In frequency modulation, the amplitude of the high-frequency carrier wave is made to vary in proportion to the frequency of the audio signal.

    Solution

    B.

    In amplitude modulation, the frequency of the high-frequency carrier wave is made to vary in proportion to the amplitude of the audio signal.

    As, we know, an amplitude modulated wave, the bandwidth is twice the frequency of modulating the signal. Therefore, amplitude modulation (AM), the frequency of the high-frequency carrier wave is made to vary in proportion to the amplitude of the audio signal.

    Question 1002
    CBSEENPH12039471

    A pipe open at both ends has a fundamental frequency f in the air. The pipe is dipped vertically in water so that half of it is in water. The fundamental frequency of the air column is now:

    • f/2

    • 3f/4

    • 2f

    • f

    Solution

    D.

    f

    For open ends, fundamental frequency f in air
    we have

    straight lambda over 2 space equals space straight l
straight lambda space equals space 2 straight l
straight v space equals fλ
straight f equals straight v over straight lambda space equals space fraction numerator straight v over denominator 2 straight l end fraction
    When a pipe is dipped vertically in the water, so that half of it is in water, we have

    straight lambda over 4 space equals space 1 half
straight lambda space equals space 2 straight l rightwards double arrow space straight v equals space straight f apostrophe straight lambda
straight f apostrophe space equals space straight v over straight lambda space equals fraction numerator straight v over denominator 2 straight l end fraction space equals space straight f
    Thus, the fundamental frequency of the air column is now,
    f=f'

    Question 1003
    CBSEENPH12039473

    In an experiment for determination of refractive index of glass of a prism by i− δ, plot, it was found that a ray incident at angle 35o, suffers a deviation of 408 and that it emerges at angle 79o ⋅ Ιn that case which of the following is closest to the maximum possible value of the refractive index?

    • 1.5

    • 1.6

    • 1.7

    • 1.8

    Solution

    A.

    1.5

    C.

    1.7

    If μ is the refractive index of the material of prism, the from shell's law
    straight mu space equals space fraction numerator sin space straight i over denominator sin space straight r end fraction space equals space fraction numerator sin space left parenthesis straight A space plus straight delta subscript straight m right parenthesis divided by 2 over denominator sin space straight A divided by 2 end fraction space space left parenthesis straight i right parenthesis
Where space straight A space is space angle space of space prism space and space straight delta subscript straight m space is space minimum space deviation space through space prism
Given comma space straight i space equals space 35 to the power of straight o comma space straight delta space equals space 40 to the power of straight o comma space straight e space equals space 79 to the power of straight o
so comma space angle space of space deviation space by space straight a space glass space prism comma
straight delta space equals space straight i space plus space straight e minus space straight A
40 to the power of straight o space equals space 35 to the power of straight o space plus 79 to the power of straight o minus space straight A
straight i. straight e space angle space of space prism space rightwards double arrow space straight A space equals space 74 to the power of straight o
So space angle space of space deviation space by space straight a space glass space prism
straight delta space equals space straight i space plus space straight e minus straight A
rightwards double arrow space 40 to the power of straight o space equals space 35 to the power of straight o space plus 79 to the power of straight o minus space straight A
straight i. straight e space angle space of space prism space rightwards double arrow space straight A space equals space 74 to the power of straight o
let space us space put space straight mu space equals space 15 space in space eq space left parenthesis straight i right parenthesis space we space get
1.5 space equals space fraction numerator sin open parentheses begin display style fraction numerator straight A space plus straight delta subscript min over denominator 2 end fraction end style close parentheses over denominator Sin space straight A divided by 2 end fraction
1.5 space equals space fraction numerator sin open parentheses begin display style fraction numerator 74 to the power of straight o space plus straight delta subscript min over denominator 2 end fraction end style close parentheses over denominator Sin 37 to the power of straight o end fraction
0.9 space equals space sin space open parentheses 37 to the power of o space plus delta subscript m i n end subscript over 2 close parentheses left parenthesis therefore space sin space 37 to the power of straight o space equals space 0.6 right parenthesis
sin space 64 to the power of straight o space equals space sin space open parentheses 37 to the power of straight o space plus straight delta subscript min over 2 close parentheses space left parenthesis therefore space sin space 64 to the power of straight o space equals space 0.9 right parenthesis
37 to the power of o space plus delta subscript m i n end subscript over 2 space equals space 64 to the power of straight o space rightwards double arrow straight delta subscript min space equals space 54 to the power of straight o space
    This angle is greater than the 40o and deviation angle already given. For greaterμ deviation will be even higher. Hence μ of the given prism should be lesser than 1.5. Hence, the closest option will be 1.5

    Question 1004
    CBSEENPH12039474

    Identify the semiconductor devices whose characteristics are given below, in the order (a), (b), (c), (d):

    Solution

    A.

    Zener diode works in breakdown region
     So, simple  diode → (a)
    zener diode (b)
    solar cell → (c)
    Light dependent resistance → (d)

    Question 1005
    CBSEENPH12039475

    A signal of 5 kHz frequency is amplitude modulated on a carrier wave of frequency 2 MHz. The frequencies of the resultant signal is/are:

    • 2005 kHz, and 1995 kHz

    • 2005 kHz, 2000 kHz and 1995 kHz

    • 2000 kHz and 1995 kHz

    • 2 MHz only

    Solution

    C.

    2000 kHz and 1995 kHz

    Frequency associated with AM are
    fc - fm, f, fc + fm
    according to the question
    fc = 2 MHz = 2000 kHz

    fm = 5 kHz
    Thus, frequency of the resultant signal is are carrier frequency fc = 2000 kHz, LSB frequency  fc-fm = 2000 kHz-5kHz = 1995 kHz and USB frequency fc+fm = 2005 kHz
    Question 1006
    CBSEENPH12039476
    Question 1007
    CBSEENPH12039477

    As an electron makes a transition from an excited state to the ground state of a hydrogen – like atom/ion:

    • kinetic energy, potential energy and total energy decrease

    • kinetic energy decreases, potential energy increases but total energy remains same

    • kinetic energy and total energy decrease but potential energy increases

    • its kinetic energy increases but the potential energy and total energy decrease

    Solution

    A.

    kinetic energy, potential energy and total energy decrease

    As we know that kinetic energy of an electron is 
    KE ∝ (Z/n)
    when the electron makes the transition from an excited state of the ground state then n, decreases and KE increases. We know that PE is lowest for the ground state. As TE=- KE and TE also decreases.

    Question 1011
    CBSEENPH12039491

    Monochromatic light is incident on a glass prism of angle A. If the refractive index of the material oft the prism is μ, a ray incident at an angle θ, on the face AB would get transmitted through the face AC of the prism provided

    • straight theta space greater than space sin to the power of negative 1 end exponent open square brackets straight mu space sin space open parentheses straight A minus sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close parentheses close square brackets
    • straight theta space less than space sin to the power of negative 1 end exponent open square brackets straight mu space sin space open parentheses straight A minus sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close parentheses close square brackets
    • straight theta less than cos to the power of negative 1 end exponent open square brackets straight mu space sin space open parentheses straight A minus sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close parentheses close square brackets
    • straight theta space greater than cos to the power of negative 1 end exponent open square brackets straight mu space sin space open parentheses straight A minus sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close parentheses close square brackets

    Solution

    A.

    straight theta space greater than space sin to the power of negative 1 end exponent open square brackets straight mu space sin space open parentheses straight A minus sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close parentheses close square brackets

    The Ray will get transmitted through face AC if iAC < iC
    Consider the ray diagram is shown below θ.

    A ray of light incident on face AB at angle 
    r1 = Angle of refraction on face AB
    r2 = Angle of incidence at face AC
    For transmission of light through face AC
    iAC < iC or A-ri < iC
     or Sin (A-r1)1)< 1/μ
    straight A minus straight r subscript 1 space less than space sin to the power of negative 1 end exponent space open parentheses 1 over straight mu close parentheses
sin space straight r subscript 1 space greater than space sin space open square brackets straight A minus sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close square brackets
    Now, applying snell's law at the face AB
    1 x sin θ = μ sin r1 or sinr1 = sinθ/μ
    fraction numerator sin space straight theta over denominator straight mu end fraction space greater than space sin space open square brackets straight A minus sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close square brackets
straight theta greater than space sin to the power of negative 1 end exponent open square brackets straight mu space sin space open curly brackets straight A space minus space sin to the power of negative 1 end exponent open parentheses 1 over straight mu close parentheses close curly brackets close square brackets

    Question 1012
    CBSEENPH12039501

    A thin convex lens made from crown glass open parentheses straight mu space equals space 3 over 2 close parentheses has focal length f. When it is measured in two different liquids having refractive indices 4/3 and 5/3, it has the focal lengths f1 and f2 respectively. The correct

    •  f1  = f2 <f

    •  f1  >f and f2 becomes negative

    •  f2  >f and f1 becomes negative

    • f1 and f2 both become negative

    Solution

    B.

     f1  >f and f2 becomes negative

    according to lens maker's formula, when the lens in the air.
    1 over straight f space equals space open parentheses 3 over 2 minus 1 close parentheses open parentheses 1 over straight R subscript 1 minus 1 over straight R subscript 2 close parentheses
1 over straight f space equals space fraction numerator 1 over denominator 2 straight x end fraction rightwards double arrow space straight f space equals 2 straight x
Here comma space open parentheses 1 over straight x space equals space 1 over straight R subscript 1 minus 1 over straight R subscript 2 close parentheses
    In case of liquid, where refractive index is 4/3 and 5/3
    we get
    Focal length in first liquid
    1 over straight f subscript 1 space equals space open parentheses straight mu subscript straight s over straight mu subscript straight l subscript 2 end subscript minus 1 close parentheses open parentheses 1 over straight R subscript 1 minus 1 over straight R subscript 2 close parentheses
1 over straight f subscript 1 space equals space open parentheses fraction numerator begin display style 3 over 2 end style over denominator begin display style 4 over 3 end style end fraction minus 1 close parentheses space 1 over straight x
    ⇒ f1 is positive.
    1 over straight f subscript 1 space minus space fraction numerator 1 over denominator 8 straight x end fraction space equals space fraction numerator 1 over denominator 4 left parenthesis 2 straight x right parenthesis end fraction space equals space fraction numerator 1 over denominator 4 straight f end fraction rightwards double arrow space straight f subscript 1 space equals space 4 straight f
    Focal length in second liquid
    1 over straight f subscript 2 space equals space open parentheses straight mu subscript straight s over straight mu subscript l subscript 2 end subscript minus 1 close parentheses open parentheses 1 over straight R subscript 1 minus 1 over straight R subscript 2 close parentheses
rightwards double arrow space 1 over straight f subscript 1 space equals space open parentheses fraction numerator begin display style 3 over 2 end style over denominator begin display style 5 over 3 end style end fraction minus 1 close parentheses open parentheses 1 over straight x close parentheses
rightwards double arrow space straight f subscript 2 space is space negative

    Question 1013
    CBSEENPH12039502

    A green light is an incident from the water to the air – water interface at the critical angle (θ). Select the correct statement

    • The entire spectrum of visible light will come out of the water at various angles to the normal.

    • The spectrum of visible light whose frequency is less than that of green light will come out to the air medium

    • The spectrum of visible light whose frequency is more than that of green light will come out to the air medium.

    • The entire spectrum of visible light will come out of the water at an angle of 900 to the normal.

    Solution

    D.

    The entire spectrum of visible light will come out of the water at an angle of 900 to the normal.

    As the frequency of visible light increases refractive index increases. With the increase of refractive index critical angle decreases. So that light having a frequency greater than green will get total internal reflection and the light having the frequency less than green will pass to air.

    Question 1017
    CBSEENPH12039506

    The forward biased diode connection is

    Solution

    A.

    Question 1023
    CBSEENPH12039517

    The anode voltage of a photocell is kept fixed. The wavelength λ of the light falling on the cathode is gradually changed. The plate current I of the photocell varies as follows:

    Solution

    D.

    As λ is increased, there will be a value of λ above which photoelectrons will cease to come out. So, photocurrent will be zero.

    Question 1024
    CBSEENPH12039518

    The I-V characteristic of an LED is

    Solution

    A.

    For same value of current, higher value of voltage is required for higher frequency.

    Question 1029
    CBSEENPH12039527

    A cylindrical tube, open at both ends, has a fundamental frequency, f, in the air. The tube is dipped vertically in water so that half of it is in water. The fundamental frequency of the air-column is now

    • f

    • f/2

    • 3f/4

    • 2f

    Solution

    A.

    f

    Initially for open organ pipe, fundamental frequency,
    straight v subscript straight o space equals space fraction numerator straight v over denominator 2 l end fraction space equals straight f
    But when it is half dipped in water, then it becomes closed organ pipe of length l/2. In this case fundamental frequency.
    straight v subscript straight c space equals space fraction numerator straight v over denominator 4 l end fraction space equals space fraction numerator straight v over denominator 4 begin display style l over 2 end style end fraction space equals space fraction numerator straight V over denominator 2 l end fraction space equals straight f

    Question 1031
    CBSEENPH12039529
    Question 1032
    CBSEENPH12039530
    Question 1045
    CBSEENPH12039559

    A nucleus of mass M + Δm is at rest and decays into two daughter nuclei of equal mass M/2 each. The speed of light is c.
    The binding energy per nucleon for the parent nucleus is E1 and that for the daughter nuclei is E2. Then

    • E1 = 2E2

    • E2 = 2E1

    • E1 > E2

    • E2 > E1

    Solution

    D.

    E2 > E1

    After decay, the daughter nuclei will be more stable hence, binding energy per nucleon will be more than that of their parent nucleus.

    Question 1046
    CBSEENPH12039560

    A nucleus of mass M + Δm is at rest and decays into two daughter nuclei of equal mass M/2 each. Speed of light is c.

    The speed of daughter nuclei is

    • fraction numerator increment straight m over denominator straight M plus increment straight m end fraction
    • square root of fraction numerator 2 increment straight m over denominator straight M end fraction end root
    • straight c square root of fraction numerator increment straight m over denominator straight M end fraction end root
    • straight c space square root of fraction numerator increment straight m over denominator straight M space plus space increment straight m end fraction end root

    Solution

    B.

    square root of fraction numerator 2 increment straight m over denominator straight M end fraction end root

    Conserving the momentum
    0 space equals space space straight M over 2 straight V subscript 1 space minus space straight M over 2 space straight V subscript 2 space left parenthesis therefore space initial space Velocity space equals space 0 right parenthesis
rightwards double arrow space straight v subscript 1 space equals space straight v subscript 2 space..... space left parenthesis straight i right parenthesis
    Now, from energy conservation and mass -energy equivalence

    Question 1047
    CBSEENPH12039561

    A radioactive nucleus (initial mass number A and atomic number Z) emits 3 α–particles and 2 positions. The ratio of number of neutrons to that of protons in the final nucleus will be

    • fraction numerator straight A minus straight Z minus 8 over denominator straight Z minus 4 end fraction
    • fraction numerator straight A minus straight Z minus 4 over denominator straight Z minus 4 end fraction
    • fraction numerator straight A minus straight Z minus 12 over denominator straight Z minus 4 end fraction
    • fraction numerator straight A minus straight Z minus 4 over denominator straight Z minus 2 end fraction

    Solution

    B.

    fraction numerator straight A minus straight Z minus 4 over denominator straight Z minus 4 end fraction

    In positive beta decay a, proton is transformed into a neutron and a positron is emitted
    p+ → n0 + e+
    Number of neutrons initially was A-Z
    Number of neutrons after decay (A-Z) -3 x 2  (due to alpha particles) + 2 x 1 (due to positive beta decay)
    The number of protons will reduce by 8. so, the ratio number of neutrons to that of protons = fraction numerator straight A minus straight Z minus 4 over denominator straight Z minus 8 end fraction

    Question 1048
    CBSEENPH12039563

    The combination of gates shown below yields

    • OR gate

    • NOT gate

    • XOR gate

    • NAND gate

    Solution

    A.

    OR gate

    A B X
    0 0 0
    0 1 1
    1 0 1
    1 1 1

    This comes out be truth table of OR gate
    Question 1049
    CBSEENPH12039564

    If a source of power 4kW produces 1020 photons/second, the radiation belongs to a part of the spectrum called

    • X -rays

    • ultraviolet rays

    • microwaves

    • γ rays

    Solution

    A.

    X -rays

    As power of source = 4 x 103 = 1020 x hv
    (∴ P/E = Number of photons)
    straight v equals space fraction numerator 4 space straight x space 10 cubed over denominator 10 to the power of 20 space straight x space 6.023 space straight x space 10 to the power of negative 34 end exponent end fraction
space straight v space equals space 6.64 space straight x space 10 to the power of 16 space Hz

    Question 1051
    CBSEENPH12039568

    The speed of light in the medium is

    •  maximum on the axis of the beam

    • minimum on the axis of the beam

    • the same everywhere in the beam

    • directly proportional to the intensity I.

    Solution

    B.

    minimum on the axis of the beam

    The speed of light at the surface or interface of the medium is maximum while on the axis of the medium is minimum

    Question 1054
    CBSEENPH12039572

    A diverging lens with the magnitude of focal length 25 cm is placed at a distance of 15 cm from a converging lens of the magnitude of focal length 20 cm. A beam of parallel light falls on the diverging lens. The final image formed is

    • real and at a distance of 40 cm from the divergent lens

    • real and at a distance of 6 cm from the convergent lens

    • real and at a distance of 40 cm from the convergent lens

    • virtual and at a distance of 40 cm from the convergent lens

    Solution

    C.

    real and at a distance of 40 cm from the convergent lens

    As parallel beam incident on diverging lens if forms virtual image at v1 = –25 cm from the diverging lens which works as an object for the converging lens (f = 20 cm)

    So for converging lens u = -40 cm, f = 20 cm
    therefore final image
    1 over straight v space minus fraction numerator 1 over denominator negative 40 end fraction space equals space 1 over 20
    V = 40 cm from the converging lens.


    Question 1055
    CBSEENPH12039573

    In a common emitter amplifier circuit using an n-p-n transistor, the phase difference between the input and the output voltages will be

    • 135°

    • 180°

    • 45°

    • 90°

    Solution

    B.

    180°

    In common emitter amplifier circuit input and output voltage are out of phase. When the input voltage is increased then ib is increased, ic also increases so the voltage drop across Rc is increased. However, increase in voltage across RC is in opposite sense.

    Question 1067
    CBSEENPH12039690

    When an unpolarized light of intensity I0 is incident on a polarizing sheet, the intensity of the light which does not get transmitted is

    • I0 /2

    • I0 /4

    • zero

    • I0 

    Solution

    A.

    I0 /2

    When unpolarised light of intensity Io is incident on a polarizing sheet, only Io/2 is transmitted.

    Question 1068
    CBSEENPH12039750
    Question 1069
    CBSEENPH12039779

    To get output for the following circuit, the correct choice for the input is,

    • A=1, B=0, C = 0

    • A=1, B=1, C = 0

    • A=1, B=0, C=1

    • A=0, B=1, C=0

    Solution

    C.

    A=1, B=0, C=1

    Consider the figure below,
    The resultant boolean expression of the above logic circuit is given by,
    Y = (A+B).C
    Using the inputs given in the options,
    If A=0, B=0,C=0, we have
    Y = (0+0).0
    i.e., Y = 0
    If A=1, B=1, C=0, then we have
    Y = (1+1).0
    i.e., Y = 1.0 = 0
    If A=1, B=0, C=1, then
    Y = (1+0).1
    i.e., Y = 1.1 = 1
    If A=0, B = 1, C =0, then
    Y = (0+1).0
    i.e., Y = 1.0
    Y = 0
    Therefore, output Y = 1 only when inputs A=1, B=0 and C=1.

    Question 1070
    CBSEENPH12039781

    When a metallic surface is illuminated with radiation of wavelength straight lambda, the stopping potential is V. If the same surface is illuminated with radiation of wavelength 2 straight lambda, the stopping potential is V/4. The threshold wavelength for the metallic surface is,

    • 5 straight lambda
    • 5 over 2 lambda
    • 3straight lambda

    • 4straight lambda

    Solution

    C.

    3straight lambda

    When a metallic surface is illuminated with radiation of wavelength straight lambda, the stopping potential is V.
    Photoelectric equation can be written as,
    eV equals space space hc over straight lambda minus hc over straight lambda subscript straight o        ... (i)
    Now, when the same surface is illuminated with radiation of wavelength 2straight lambda, the stopping potential is V/4. So, photoelectric equation can be written as,
    space space space space space space eV over 4 equals fraction numerator h c over denominator 2 lambda end fraction minus fraction numerator h c over denominator lambda subscript o end fraction
rightwards double arrow space e V space equals space fraction numerator 4 h c over denominator 2 lambda end fraction minus fraction numerator italic 4 h c over denominator lambda subscript o end fraction space space space space... space left parenthesis i i right parenthesis
    From equations (i) and (ii), we get
    space space space hc over straight lambda minus hc over straight lambda subscript straight o equals fraction numerator 4 h c over denominator 2 lambda end fraction minus fraction numerator 4 h c over denominator straight lambda subscript straight o end fraction
rightwards double arrow space 1 over straight lambda minus 1 over straight lambda subscript straight o equals italic 2 over lambda minus 4 over straight lambda subscript straight o
rightwards double arrow space space straight lambda subscript straight o space equals space 3 straight lambda

    Question 1071
    CBSEENPH12039782

    The intensity at the maximum in a Young's double slit experiment is Io. Distance between two slits is d = 5 straight lambda, where straight lambda is the wavelength of light used in the experiment. What will be the intensity infront  of one of the slits on the screen placed at a distance D = 10 d?

    • straight I subscript straight o over 4
    • 3straight I subscript straight o over 4

    • straight I subscript straight o over 2
    • Io

    Solution

    C.

    straight I subscript straight o over 2
    In the fig., S1 and S2 are the two different slits.
    Given, distances between slits S1 and S2
    d = 5 straight lambda
    Distance between the screen and slits, D = 10 d = 50 straight lambda
    straight lambda is the wavelength of the light used in the experiment.
    In Young's double slit experiment, the maximum intensity is Io.
    rightwards double arrow space straight I subscript max space equals space straight I subscript straight o
    Path difference, dY subscript straight n over straight D equals fraction numerator d x begin display style d over 2 end style over denominator 10 space d end fraction equals d over 20 equals lambda over 4
space space space space space space space space space space space space space space space space space space space space space space space space space space space space left square bracket space d space equals space 5 lambda right square bracket
    Path difference of straight lambda corresponds to phase difference 2straight pi.
    So, for path difference straight lambda over 4, phase difference is
    straight ϕ space equals space fraction numerator 2 straight pi over denominator straight lambda end fraction straight x straight lambda over 4 equals straight pi over 2 equals 90 to the power of straight o
    We know,
    I = Io cos2 90 to the power of straight o over 2
    space space space space space space straight I space equals space straight I subscript straight o space straight x open parentheses fraction numerator 1 over denominator square root of 2 end fraction close parentheses squared
rightwards double arrow space straight I space equals space straight I subscript straight o over 2
    Question 1072
    CBSEENPH12039783

    Given the value of rydberg constant is 10 m-1, the wave number of the last line of the Balmer series in hydrogen spectrum will be:

    • 0.5 x 107 m-1

    • 0.25 x 107 m-1

    • 2.5 x10m-1

    • 0.025 x 104 m-1

    Solution

    B.

    0.25 x 107 m-1

    Rydberg constant, r = 107 m-1
    For last line in Balmer series,


    n2infinity; n1 = 2
    We know,
    space space space space 1 over straight lambda equals space R open parentheses 1 over n subscript 1 squared minus 1 over n subscript 2 squared close parentheses
rightwards double arrow space 1 over straight lambda equals italic 10 to the power of italic 7 open parentheses 1 over 2 squared minus 1 over italic infinity close parentheses
italic rightwards double arrow italic space nu with italic bar on top italic space italic equals italic space italic 1 over lambda italic equals italic 10 to the power of italic 7 over italic 4
italic space italic space italic space italic space italic space italic space italic space italic space italic space italic equals italic 0 italic. italic 25 italic space x italic space italic 10 to the power of italic 7 italic space m to the power of italic minus italic 1 end exponent
    Question 1073
    CBSEENPH12039784

    The ratio of escape velocity at earth (Ve) to the escape velocity at a planet (vp) whose radius and mean density are twice as that of earth is,

    • 1:2 square root of 2

    • 1:4

    • 1:square root of 2

    • 1:2

    Solution

    A.

    1:2 square root of 2

    Escape velocity of earth can be given as,
    vesquare root of 2 gR end root = Rsquare root of 8 over 3 πGρ end root, where straight rho is the density of the earth.
    rightwards double arrow space straight v subscript straight e space equals space straight R square root of 8 over 3 πGρ end root  ... (i)
    Given that the radius and mean density of planet are twice as that of earth.
    So, escape velocity at planet will be,
    straight v subscript straight p space equals space 2 straight R space square root of 8 over 3 πG 2 straight rho end root space space space... space left parenthesis ii right parenthesis
Dividing space eqn. space by space left parenthesis straight i right parenthesis space by space left parenthesis ii right parenthesis comma
straight v subscript straight e over straight v subscript straight p space equals space fraction numerator straight R square root of 8 over 3 πGρ end root space over denominator 2 straight R square root of 8 over 3 πG 2 straight rho end root end fraction
rightwards double arrow space straight v subscript straight e over straight v subscript straight p space equals fraction numerator 1 over denominator 2 square root of 2 end fraction

    Question 1074
    CBSEENPH12039787

    A siren emitting a sound of frequency 800 Hz moves away from an observer towards a cliff at a speed of 15 m/s. Then, the frequency of sound that the observer hears in the echo reflected from the cliff is (Take, velocity of sound in air = 330 m/s)

    • 800 Hz

    • 838 Hz

    • 885 Hz

    • 765 Hz

    Solution

    B.

    838 Hz

    The situation can be illustrated as follows:

    Frequency of sound that the observer hear in the echo reflected from the cliff is given by,
    f' = open parentheses fraction numerator straight v over denominator straight v minus straight v subscript straight s end fraction close parentheses
    where,
    f = original frequency of source
    v= velocity of the sound
    vs = velocity of the source
    So, straight f apostrophe space equals space open parentheses fraction numerator 330 over denominator 330 minus 15 end fraction close parentheses 800 space equals space 838 space Hz
    Question 1075
    CBSEENPH12039788

    In a diffraction pattern due to single slit of width a, the first minimum is obsrved at an angle 30o when light of wavelength 5000 space straight A with straight o on top is incident on the slit. The first secondary maximum is observed at an angle of:

    • sin-1 (2/3)

    • sin-1 (1/2)

    • sin-1 (3/4)

    • sin-1 (1/4)

    Solution

    C.

    sin-1 (3/4)

    Given that, first minimum is observed at an angle of 30o in a diffraction pattern due to a single slit of width a.
    i.e., n =1, straight theta space equals space 30 to the power of straight o
    According to the Bragg's law of diffraction,
    space space space space space straight a space sin space straight theta space equals space nλ
rightwards double arrow space straight a space sin space 30 to the power of straight o space equals space left parenthesis 1 right parenthesis straight lambda space space left square bracket space straight n equals 1 right square bracket
rightwards double arrow space straight a space equals space 2 straight lambda space space space space space... bold space bold left parenthesis bold i bold right parenthesis bold space open curly brackets space sin space 30 to the power of straight o equals 1 half close curly brackets
    For 1st secondary maxima,
    rightwards double arrow space straight a space sinθ subscript 1 space equals space fraction numerator 3 straight lambda over denominator 2 end fraction
rightwards double arrow space sin space straight theta subscript 1 space equals space fraction numerator 3 straight lambda over denominator 2 straight a end fraction   ... (2)
    Putting the value of a from Eqn. (i) to Eqn. (ii), we get
    space space space space space space sin space theta subscript 1 space equals space fraction numerator 3 lambda over denominator 4 lambda end fraction
rightwards double arrow space sin space theta subscript 1 space equals space 3 over 4
rightwards double arrow space space theta subscript 1 italic space italic equals italic space space sin to the power of negative 1 end exponent open parentheses 3 over 4 close parentheses

    Question 1076
    CBSEENPH12039790

    A black body is at a temperature of 5760 K. The energy of radiation emitted by the body at wavelength 250 nm is U1, at wavelength 500 nm is U2 and that at 1000 nm is U3. Wien's constant, b = 2.88 x 106 nmK. Which of the following is correct?

    • U3 = 0

    • U1 > U2

    • U2 > U1

    • U1 = 0

    Solution

    C.

    U2 > U1

    Given, temperature, T1 = 5760 K
    Given that energy of radiation emitted by the body at wavelength 250 nm in U1, at wavelength 500 nm is U2 and that at 1000 nm is U3.
    Now, according to Wein's law, we get
    straight lambda subscript straight m straight T space equals space straight b
    where, b = Wien's constant = 2.88 x 106 nmK
    rightwards double arrow space straight lambda subscript straight m space equals space straight b over straight T
    rightwards double arrowstraight lambda subscript straight m space equals space fraction numerator 2.88 space straight x space 10 to the power of 6 space nmk over denominator 5760 space straight K end fraction
    rightwards double arrow space straight lambda subscript straight m space equals 500 space nm
    straight lambda subscript straight m is the wavelength corresponding to maximum energy, so U2 > U1.

    Question 1077
    CBSEENPH12039791

    Consider the junction diode as ideal. The value of current flowing through AB is,

     
    • 10-2 A

    • 10-1 A

    • 10-3 A

    • 0 A

    Solution

    A.

    10-2 A

    Let, I be the current through the diode.
    From the given condition,
    straight I space equals space fraction numerator straight V subscript straight A space minus space straight V subscript straight B over denominator straight R end fraction
space space equals fraction numerator 4 minus left parenthesis negative 6 right parenthesis over denominator 1 space kΩ end fraction
space space equals space fraction numerator 10 over denominator 1 space straight x space 10 cubed end fraction
space space equals space 10 to the power of negative 2 end exponent space straight A

    Question 1078
    CBSEENPH12039792

    An astronomical telescope has objective eyepiece of focal lengths 40 cm and 4 cm respectively. To view an object 200 cm away from the objective lens, the lenses must be separated by a distance,

    • 46.0 cm

    • 50.0 cm

    • 54.0 cm

    • 37.3 cm

    Solution

    C.

    54.0 cm

    According to a question,
    Focal length of the objective lens, Fo = +40 cm
    Focal length of eyepiece, Fe = 4 cm
    Object distance for objective lens (uo) = -200 cm
    Applying lens formula for objective lens,

    space space space space space 1 over straight v minus 1 over u equals 1 over f
rightwards double arrow space 1 over v space minus space fraction numerator 1 over denominator negative 200 end fraction space equals space 1 over 40
rightwards double arrow space 1 over v equals space 1 over 40 space minus 1 over 200 space
space space space space space space space space space equals space fraction numerator 5 minus 1 over denominator 200 end fraction
space space space space space space space space space equals space 4 over 200
rightwards double arrow space v space equals space 50 space c m
    Image will be formed at the focus of a eyepiece lens.
    So, for normal adjustment distance between objectives and eyepiece (length of tube) will be,
    straight v space plus space straight F subscript straight e space equals space 50 space plus space 4 space equals space 54 space cm

    Question 1079
    CBSEENPH12039793

    A p-n-p transistor is connected in a common emitter configuration in a given amplifier. A load resistance of 800 ohm is connected in the collector circuit and the voltage drop across it is 0.8 V. If the current amplification factor is 0.96 and the input resistance of the circuit is 192 ohm, the voltage gain and the power gain of the amplifier will respectively be,

    • 3.69,3.84

    • 4,4

    • 4,3.69

    • 4, 3.84

    Solution

    D.

    4, 3.84

    Given,
    Resistance across load, RL = 800 ohm
    Voltage drop across load, VL = 0.8 V
    Input resistance of the circuit, Ri = 192 ohm
    Collector current is given by,
    straight I subscript straight C space equals space straight V subscript straight L over straight R subscript straight L equals fraction numerator 0.8 over denominator 800 end fraction equals 8 over 8000 equals 1 space mA
    Therefore, Current amplification = fraction numerator Output space current over denominator Input space current end fraction
    equals straight I subscript straight c over straight I subscript straight B equals 0.96
rightwards double arrow I subscript B space equals space fraction numerator 1 space m A over denominator 0.96 end fraction
    Voltage gain, AV is,
    straight V subscript straight L over straight V subscript in space equals space fraction numerator V subscript L over denominator I subscript B R subscript i end fraction
space space space space space space space equals space fraction numerator 0.8 space x space 0.96 over denominator 10 to the power of negative 3 end exponent space x space 192 end fraction
space space space space space space space equals space 4
rightwards double arrow space A subscript V space equals space 4
    Power gain,
    APfraction numerator straight I squared subscript straight C straight R subscript straight L over denominator straight I squared subscript straight B space straight R subscript straight i end fraction space equals space open parentheses I subscript C over I subscript B close parentheses squared. R subscript L over R subscript i space equals space left parenthesis 0.96 right parenthesis squared x 800 over 192
        = (0.96)2800 over 192
    AP = 3.84

    Question 1080
    CBSEENPH12039795

    Match the corresponding entries of Column 1 with Column 2. [ where m is the magnification produced by the mirror]

    Column 1 Column 2
    A. m = -2 a. convex mirror
    B. m = -1/2 b. Concave mirror
    C. m = +2 c. Real image
    D. m = +1/2 d. Virtual image
    • A --> a and c; B --> a and d; C --> a and b ; D --> c and d

    • A --> a and d; B -->  b and c; C --> b and d; D --> b and c

    • A --> c and d; B --> b and d; C --> b and c; D --> a and d

    • A --> b and c; B --> b and c; C --> b and d; D --> a and d

    Solution

    D.

    A --> b and c; B --> b and c; C --> b and d; D --> a and d

    A concave mirror forms real and virtual image, whose magnification can be negative or positive depending upon the position of the object.
    If object is placed between focus and pole the image obtained will be virtual and its magnification will be positive. In all other cases concave mirror forms real images whose magnification will be negative.
    A convex mirror always forms a virtual image whose magnification will always be positive.

    Question 1088
    CBSEENPH12039814

    An electron of mass m and a photon have the same energy E. The ratio of de-Broglie wavelength associated with them is,

    • open parentheses fraction numerator straight E over denominator 2 straight m end fraction close parentheses to the power of begin inline style bevelled 1 half end style end exponent
    • straight c space left parenthesis 2 mE right parenthesis to the power of begin inline style bevelled 1 half end style end exponent
    • 1 over straight c open parentheses fraction numerator 2 m over denominator E end fraction close parentheses to the power of begin inline style bevelled 1 half end style end exponent
    • 1 over straight c open parentheses fraction numerator E over denominator 2 m end fraction close parentheses to the power of begin inline style bevelled 1 half end style end exponent

    Solution

    D.

    1 over straight c open parentheses fraction numerator E over denominator 2 m end fraction close parentheses to the power of begin inline style bevelled 1 half end style end exponent

    Given that electron has a mass m.
    De-Broglie wavelength for an electron will be given as,

    straight lambda subscript straight e space equals space straight h over straight p space space space space space space space space space... space left parenthesis straight i right parenthesis
    where,
    h is the Planck's constant, and
    p is the linear momentum of electron
    Kinetic energy of electron is given by, E = fraction numerator straight p squared over denominator 2 straight m end fraction
    rightwards double arrow space space space space straight p equals space square root of 2 mE end root space space space space space space space space space space space space space space space... space left parenthesis ii right parenthesis
    From equation (i) and (ii), we have
    straight lambda subscript straight e space equals space fraction numerator straight h over denominator square root of 2 mE end root end fraction space space space space space space space space space space space space... space left parenthesis iii right parenthesis
    Energy of a photon can be given as,
    straight E space equals space straight h space straight nu
    rightwards double arrow space straight E space equals space hc over straight lambda subscript straight P

rightwards double arrow space space straight lambda subscript straight P space equals space hc over straight E space space space space space space space space space space... space left parenthesis iv right parenthesis
    Hence, straight lambda subscript straight P is the de-Broglie wavelength of photon.
    Now, dividing equation (iii) by (iv), we get
    space space space space space space straight lambda subscript straight e over straight lambda subscript straight P space equals space fraction numerator h over denominator square root of 2 m E end root end fraction. fraction numerator E over denominator h c end fraction

rightwards double arrow space space space straight lambda subscript straight e over straight lambda subscript straight P space equals space 1 over straight c. square root of fraction numerator straight E over denominator 2 straight m end fraction end root

    Question 1090
    CBSEENPH12039816

    Which of the following figures represent the variation of particle momentum and the associated de-Broglie wavelength?

    Solution

    B.

    The de-Broglie wavelength is given by
    straight lambda space equals space straight h over straight P
rightwards double arrow space Pλ space equals straight h
    This equation is in the form of yx =c, which is the equation of a rectangular hyperbola.

    Question 1091
    CBSEENPH12039817

    If in a p-n junction, a square input signal of 10 V is applied as shown,


    then the output across RL will be

    Solution

    D.

    As it is forward biased so it takes positive value. Hence, option (d) is correct.

    Question 1092
    CBSEENPH12039818

    Which logic gate is represented by this following combination of logic gates?

    • OR

    • NAND

    • AND

    • NOR

    Solution

    C.

    AND

    The truth table for the given circuit is

    A

    B

    y1

    y2

    y= y1 +y2

    0

    0

    1

    1

    0

    0

    1

    1

    0

    0

    1

    0

    0

    1

    0

    1

    1

    0

    0

    1


    The truth table shows that both the inputs are high, then we are getting a high value of output otherwise zero. Hence, the combination represents AND gate.
    Question 1093
    CBSEENPH12039819

    When an alpha particle of mass m moving with velocity v bombards on a heavy nucleus of charge Ze, its distance of closest approach from the nucleus depends on mass as,

    • fraction numerator 1 over denominator square root of straight m end fraction
    • 1 over straight m squared
    • m

    • 1 over straight m

    Solution

    D.

    1 over straight m

    When an alpha particle moving with velocity v bombards on a heavy nucleus of charge Ze, then there will be no loss of energy.
    Initial Kinetic energy of the alpha particle = Potential energy of alpha particle at closest approach.
    That is,
    rightwards double arrow space 1 half m v squared space equals space fraction numerator 2 Z e squared over denominator 4 pi epsilon subscript o r subscript o end fraction

rightwards double arrow space r subscript o space proportional to space 1 over m
    This is the required distance of closest approach to alpha particle from the nucleus.

    Question 1094
    CBSEENPH12039820

    The angle of incidence for a ray of light at a refracting surface of a prism is 45o. The angle of prism is 60o. If the ray suffers minimum deviation through the prism, the angle of minimum deviation and refractive index of the material of the prism respectively, are

    • 30osquare root of 2

    • 45osquare root of 2

    • 30ofraction numerator 1 over denominator square root of 2 end fraction

    • 45ofraction numerator 1 over denominator square root of 2 end fraction

    Solution

    A.

    30osquare root of 2

    Consider a ray of light PQ incident on the surface AB and moves along RS, after passing through the prism ABC.

    Given that, incident ray suffers minimum deviation. therefore, the ray inside the prism must be parallel to the base BC of the prism.
    From the geometry of the prism and the ray diagram, it is evident that
    Angle of incidence, i = 45o
    Angle of refraction, r = r' = 30o
    Angle of emergence, e = 45o

    Therefore, minimum deviation suffered by the ray is,
    straight delta subscript min space equals space left parenthesis straight i plus straight e right parenthesis space minus space left parenthesis straight r plus straight r apostrophe right parenthesis
space space space space space space space space equals space 90 to the power of straight o space minus space 60 to the power of straight o space
space space space space space space space space space equals space 30 to the power of straight o

    Also, using the formula,
    straight mu space equals space fraction numerator sin space open parentheses begin display style fraction numerator straight A plus straight delta subscript straight m over denominator 2 end fraction end style close parentheses over denominator sin space straight A divided by 2 end fraction
    where, straight mu is the refractive index of the material of the prism.
    A = Angle of prism = 60o
    Therefore,
    straight mu space equals space fraction numerator sin space open parentheses begin display style fraction numerator 60 to the power of straight o plus 30 to the power of straight o over denominator 2 end fraction end style close parentheses over denominator sin space begin display style 60 to the power of straight o over 2 end style end fraction

space space space equals space fraction numerator sin space 45 to the power of straight o over denominator sin space 30 to the power of straight o end fraction

space space equals space fraction numerator begin display style bevelled fraction numerator 1 over denominator square root of 2 end fraction end style over denominator 1 divided by 2 end fraction

space space equals fraction numerator 2 over denominator square root of 2 end fraction

space space equals space square root of 2
    Question 1100
    CBSEENPH12039834

    The transition from the state n = 3 to n=1 in a hydrogen-like atom results in ultraviolet radiation. Infrared radiation will be obtained in the transition from.

    • 2→ 1 

    • 3 →2

    • 4 → 2

    • 4 →3

    Solution

    D.

    4 →3

    Infrared radiation is found in Paschen, Brackett and pfund series nd it is obtained when electron transition occurs from high energy level to minimum third level.

    Question 1103
    CBSEENPH12039837

    To get an output Y = 1 in given circuit which of the following input will be correct



    • A

      B

      C

      1

      0

      0

    • A

      B

      C

      1

      0

      1

    • A

      B

      C

      1

      1

      0

    • A

      B

      C

      0

      1

      0

    Solution

    B.

    A

    B

    C

    1

    0

    1

    Here Y = (A+B).C
    Truth Table

    A

    B

    C

    Y = (A+B).C

    0

    0

    0

    0

    1

    0

    0

    0

    0

    1

    0

    0

    0

    1

    0

    0

    0

    1

    1

    1

    1

    0

    1

    1

    1

    1

    1

    1


    C should be 1 either A and B or Both A and B are 1
    Therefore , A =1, B = 0, C = 1
    Question 1107
    CBSEENPH12039844

    When a biconvex lens of glass having refractive index 1.47 is dipped in a liquid, it acts as a plane sheet of glass. This implies that the liquid must have refractive index

    • equal to that of glass

    • less than one

    • greater than that of glass

    • less than that of glass

    Solution

    A.

    equal to that of glass

    If biconvex lens behaves like a plane sheet, the ray will pass undeviated through it only when the medium has a same refractive index as that of a biconvex lens.

    Question 1115
    CBSEENPH12039860

    The figure shows a logic circuit with two inputs A and B and the output C. The voltage waveforms across A, B and C are as given. The logic circuit gate is

    • OR Gate

    • NOR Gate

    • AND Gate

    • NAND Gate

    Solution

    A.

    OR Gate

    From the given waveforms, the following truth table can be made.

    Inputs

    Output

    A

    B

    C

    0

    0

    0

    1

    0

    1

    1

    1

    1

    0

    1

    1


    This truth table is required to 'OR' gate. So, logic circuit gate is OR gate.
    Question 1119
    CBSEENPH12039875

    Light with an energy flux of 25 x 104 W/m2 falls on a perfectly reflecting surfaces at normal incidence. If the surface area is 15 cm2, the average force exerted on the surface is,

    • 1.25 x 10-6 N

    • 2.50 x 10-6 N

    • 1.20 x 10-6 N

    • 3.0 x 10-6 N

    Solution

    A.

    1.25 x 10-6 N

    Energy flux = fraction numerator 25 space straight x space 10 to the power of 4 space straight J over denominator sm squared end fraction
    Force on unit area = momentum transferred in unit time on unit area = fraction numerator 25 space straight x space 10 to the power of 4 over denominator straight c end fraction
    space equals space fraction numerator 250 space straight x space 10 to the power of 4 over denominator 3 space straight x space 10 to the power of 8 end fraction
equals space 8.3 space x space 10 to the power of negative 4 end exponent space N divided by m squared
    Force on the 15 x 10-4 m2 area,
            = 8.3 x 10-4 N/m2 x 15 x 10-4 m2

            = 124.5 x 10-8 N
            = 1.25 x 10-6 N

    Question 1121
    CBSEENPH12039878

    In the young's double slit experiment, the intensity of light at a point on the screen (where the path difference is straight lambda) is K. The intensity at a point where the path difference is bevelled straight lambda over 4 will be,

    • K

    • K/4

    • K/2

    • zero

    Solution

    C.

    K/2

    For net intensity,
    I' = 4 Io cos2 straight ϕ over 2 open parentheses straight ϕ space equals fraction numerator 2 straight pi over denominator straight lambda end fraction xλ close parentheses
    For the first case,
    K = 4 Io cos2 straight pi
    K = 4 Io                    ... (i)
    For the second case,
    straight K apostrophe space equals space 4 straight I subscript straight o space cos squared open parentheses fraction numerator begin display style bevelled straight pi over 2 end style over denominator 2 end fraction close parentheses space open parentheses straight ϕ equals fraction numerator 2 straight pi over denominator straight lambda end fraction straight x straight lambda over 4 close parentheses
space space space space equals space 4 space straight I subscript straight o space cos squared space left square bracket straight pi divided by 2 right square bracket
space space space space equals space 2 straight I subscript straight o  ... (ii)
    Comparing equations (i) and (ii), we have
    K' = K/2

    Question 1122
    CBSEENPH12039879

    If the focal length of the objective lens is increased, then the magnifying power of,

    • microscope will increase but that of telescope will decrease

    • microscope and telescope both will increase

    • microscope and telescope both will decrease

    • microscope will decrease but that of telescope will increase

    Solution

    D.

    microscope will decrease but that of telescope will increase

    For microscope, m = straight L over straight f subscript straight o. D over f subscript e
    rightwards double arrow space straight m space proportional to space 1 over straight f subscript straight o
    For telescope, m = straight f subscript straight o over straight f subscript straight e
    proportional to fo
    Therefore, the magnifying power of microscope will decrease but the magnifying power of telescope will increase.

    Question 1124
    CBSEENPH12039881

    When the energy of the incident radiation is increased by 20%, the kinetic energy of the photoelectrons emitted from a metal surface increased from 0.5 eV to 0.8 eV. The work function of the metal is,

    • 0.65 eV

    • 1.0 eV

    • 1.3 eV

    • 1.5 eV

    Solution

    B.

    1.0 eV

    For photoelectric equation,
    (KE)minhν space minus space straight ϕ subscript straight o
    For the first condition,
    0.5 = E - straight ϕ subscript straight o                ... (i)
    For the second condition,
    0.8 space equals space 1.2 space straight E space minus space straight ϕ subscript straight o      ... (ii)
    From equations (i) and (ii),
    0.5 space equals space straight E space minus space straight ϕ subscript straight o and 
    0.8 space equals space 1.2 space straight E space minus space straight ϕ subscript straight o
    -0.3 = -0.2 E
    E = fraction numerator 0.3 over denominator 0.2 end fraction equals 1.5 space e V
    From expression (i),
    0.5 = 1.5 - straight ϕ subscript straight o
    rightwards double arrow space straight ϕ subscript straight o space equals space 0.5 space minus 0.5 space
space space space space space space space space space space equals space 1 space eV

    Question 1125
    CBSEENPH12039882

    If the kinetic energy of the particle is increased to 16 times its previous value, the percentage change in the de-Broglie wavelength of the particle is,

    • 25

    • 75

    • 60

    • 50

    Solution

    B.

    75

    For de-Broglie wavelength,
    straight lambda subscript 1 space equals space straight h over straight p equals fraction numerator straight h over denominator square root of 2 mK end root end fraction space         ... (i)
    straight lambda subscript 2 space equals space fraction numerator straight h over denominator square root of 2 straight m 16 space straight K end root end fraction space
space space space space equals space fraction numerator straight h over denominator 4 square root of 2 mK end root end fraction
space space space space equals space straight lambda subscript 1 over 4          ... (ii)
    From equations (i) and (ii),
    straight lambda subscript 2 space equals space 25 percent sign space of space straight lambda subscript 1
    There is 75% change in the wavelength.

    Question 1126
    CBSEENPH12039883

    Hydrogen atom in ground state is excited by a monochromatic radiation of straight lambda space equals space 975 space straight A with straight o on top. The number of spectral lines in the resulting spectrum emitted will be,

    • 3

    • 2

    • 6

    • 10

    Solution

    B.

    2

    Energy provided to the ground state electron,
    equals space hc over straight lambda space

equals space fraction numerator 6.6 space straight x space 10 to the power of negative 34 end exponent space straight x space 3 space straight x space 10 to the power of 8 over denominator 975 space straight x space 10 to the power of negative 10 end exponent end fraction

equals space fraction numerator 6.6 space straight x space 3 over denominator 975 end fraction straight x 10 to the power of negative 16 end exponent

equals space 0.020 space straight x space 10 to the power of negative 16 end exponent

equals space 2 space straight x space 10 to the power of negative 18 end exponent space straight J

equals space fraction numerator 20 space straight x space 10 to the power of negative 19 end exponent over denominator 1.6 space straight x space 10 to the power of negative 19 end exponent end fraction space eV

equals space fraction numerator 20 over denominator 1.6 end fraction space eV

equals space 12.5 space eV
    The electron will jump from n= 3 to n=1.
    The number of possible field lines from n=3 to n=1 is 2.

    Question 1127
    CBSEENPH12039884

    The binding energy per nucleon of Li presubscript 3 presuperscript 7 space and space He presubscript 2 presuperscript 4 nuclei are 5.60 MeV and 7.06 MeV, respectively. In the nuclear reaction, Li presubscript 3 presuperscript 7 space plus space straight H presubscript 1 presuperscript 1 space rightwards arrow space He presubscript 2 presuperscript 4 space plus space straight Q, the value of energy Q released is,

    • 19.6 MeV

    • -2.4 MeV

    • 8.4 MeV

    • 17.3 MeV

    Solution

    D.

    17.3 MeV

    The binding energy for straight H presubscript 1 superscript 1 is around zero and also not given in the question so we can ignore it,
    straight Q space equals space 2 space left parenthesis 4 space straight x space 7.06 right parenthesis space minus space 7 space straight x space left parenthesis 5.60 right parenthesis

space space space space equals space left parenthesis 56.48 space minus space 39.2 right parenthesis MeV

space space space space equals space 17.28 space MeV

space space space space equals 17.3 space MeV

    Question 1128
    CBSEENPH12039885

    Two ideal diodes are connected to a battery as shown in the circuit. The current supplied by the battery is

    • 0.75 A

    • zero

    • 0.25

    • 0.5 A

    Solution

    D.

    0.5 A

    Here in circuit D1 is forward bias and D2 is reverse bias. Current flow only in diode D1
    The current supplied by the battery
     i = 5/10 = 0.5 A

    Question 1129
    CBSEENPH12039886

    A radio isotope X with a half life 1.4 x 109 yr decays of Y which is stable. A sample of the rock from a cave was found to contain X and Y in the ratio 1:7. The age of the rock is,

    • 1.96 x 109 yr

    • 3.92 x 109 yr

    • 4.20 x 109 yr

    • 8.40 x 109 yr

    Solution

    C.

    4.20 x 109 yr

    Ratio of X:Y is given = 1:7
    That is,
    straight m subscript straight x over straight m subscript straight y equals 1 over 7
    rightwards double arrow space 7 straight m subscript straight x space equals space straight m subscript straight y
    Let, the initial total mass is m.

    rightwards double arrow space straight m subscript straight x space plus space straight m subscript straight y space equals space straight m
rightwards double arrow space straight m subscript straight y over 7 plus straight m subscript straight y space equals space straight m
rightwards double arrow space space space space space space fraction numerator 8 straight m subscript straight y over denominator 7 end fraction space equals space straight m
rightwards double arrow space straight m subscript straight y space equals space 7 over 8 space straight m
only space 1 divided by 8 space part space remain

rightwards double arrow space 1 space rightwards arrow with straight T subscript begin inline style bevelled 1 half end style space space end subscript on top space space space 1 half space space rightwards arrow with straight T subscript begin inline style bevelled 1 half space space end style end subscript on top space 1 fourth rightwards arrow with straight T subscript begin inline style bevelled 1 half space space end style end subscript on top space 1 over 8
    Therefore, time taken to become 1/8 unstable part
    = 3 x T1/2
    = 3 x 1.4 x 109
    = 4.2 x 109 y

    Question 1131
    CBSEENPH12039889

    The barrier potential of a p-n junction diode depends on:
    i) type of semiconductor material
    ii) amount of doping
    iii) temperature

    Which one of the following is correct?

    • (i) and (ii) only

    • (ii) only

    • (ii) and (iii) only

    • (i), (ii) and (iii)

    Solution

    D.

    (i), (ii) and (iii)

    Barrier potential depends on the material used to make p-n junction diode (whether it is Si or Ge).
    It should also depend on the amount of doping due to which the number of majority charge carriers will change. Also, it depends on temperature due to which the number of minority carriers will change.

    Question 1132
    CBSEENPH12039890

    The output (X) of the logic circuit shown in a figure will be.

    • straight X space equals stack space straight A with equals on top. straight B with equals on top
    • straight X space equals stack straight A. straight B with ____ on top
    • X = A. B

    • straight X space equals stack space straight A space plus straight B with overparenthesis on top

    Solution

    C.

    X = A. B

    straight X space equals AB with equals on top space equals space straight A. straight B space left parenthesis straight i. straight e. comma space AND space gate right parenthesis
    If the output X of NAND gate is connected to the input of NOT gate (made from NAND gate by joining two inputs) from the given figure then we get back an AND gate.
    Question 1134
    CBSEENPH12039892

    In an n-type semiconductor, which of the following statement is true?

    • Electrons are majority carriers and trivalent atoms are dopants

    • Electrons are minority carriers and pentavalent atoms are dopants

    • Holes are minority carriers and pentavalent atoms are dopants

    • Holes are majority carriers and trivalent atoms are dopants

    Solution

    C.

    Holes are minority carriers and pentavalent atoms are dopants

    The n-type semiconductor can be produced by doping impurity atoms of valence 5 i.e., pentavalent atoms, i.e., phosphorous.

    Question 1144
    CBSEENPH12039911

    In the Davisson and Germer experiment, the velocity of electrons emitted from the electron gun can be increased by

    • Increasing the filament current

    • decreasing the filament current

    • decreasing the potential difference between the anode and filament

    • increasing the potential difference between the anode and filament

    Solution

    D.

    increasing the potential difference between the anode and filament

    In the Davisson and Germer experiment, the velocity of the electron emitted from the electron gun can be increased by increasing the potential difference between the anode and filament.

    Question 1146
    CBSEENPH12039913

    The power obtained in a reactor using U235 disintegration is  1000kW. The mass decay of U235 per hour is

    • 20 μg

    • 40 μg

    • μg

    • 10 μg

    Solution

    B.

    40 μg

    Let assume power P = 1000 W
    Energy per hour = 1000 x 3600 J
    Energy per fission = 200 MeV
    = 200 x 1.6 x 10-13 J
    therefore number per hour 
    straight n space equals space fraction numerator 1000 space straight x space 3600 over denominator 200 space straight x space 1.6 space straight x space 10 to the power of negative 13 end exponent 0 end fraction

Number space of space mole space per space hour space space equals space straight n over straight N
therefore comma space
Mass space per space hour space equals space straight n over straight N space straight x space 235

equals space fraction numerator 1000 space straight x space 3600 space straight x space 235 over denominator 200 space straight x space 1.6 space straight x space 10 to the power of negative 13 end exponent space straight x space 6.02 space straight x space 10 to the power of 23 end fraction

equals space 43.9 space straight x space 10 to the power of negative 6 space end exponent straight g
    The nearest value is 40 μg, Hence option b is correct.

    Question 1149
    CBSEENPH12039917

    Symbolic representation of four logic gates are shown as,




    Pick out which ones are for AND, NAND and NOT gates, respectively.

    • (iii), (ii)  and (i)

    • (iii), (ii) and (i)

    • (ii), (iv), and (iii)

    • (ii), (iii) and (iv)

    Solution

    C.

    (ii), (iv), and (iii)

    In symbol given in problem are 
    (i) OR gate
    (ii)  AND gate
    (iii) Not gate
    (iv) NAND gate

    Question 1150
    CBSEENPH12039919

    If a small amount of antimony is added to germanium crystal

    • the antimony becomes an acceptor atom

    • there will be more free electrons than holes in the semiconductor

    • its resistance is increased

    • it becomes a p - type semiconductor

    Solution

    B.

    there will be more free electrons than holes in the semiconductor

    When a small amount of antimony is added to germanium crystal, the crystal becomes n- type semiconductor because antimony is  a pentavalent substrate. It excess free electrons.

    Question 1151
    CBSEENPH12039924

    Fusion reaction takes place at high temperature because

    • atoms get ionised at high temperature

    • kinetic energy is high enough to overcome the coulomb repulsion between nuclei

    • molecules break up at high temperature

    • nuclei break up at high temperature

    Solution

    B.

    kinetic energy is high enough to overcome the coulomb repulsion between nuclei

    Fusion reaction takes place at high temperature because kinetic energy is high enough to overcome the coulomb repulsion between nuclei.

    Question 1153
    CBSEENPH12039927

    Photoelectric emission occurs only when the incident light has more than a certain minimum

    • wavelength

    • intensity

    • frequency

    • power

    Solution

    C.

    frequency

    By the concept of threshold minimum frequency needed for photoelectric emission.

    1 half space mv squared space equals space straight h space left parenthesis straight v minus space straight v subscript straight o right parenthesis

straight v space greater or equal than space straight v subscript straight o

    Question 1157
    CBSEENPH12039933

    Which of the following is not due to total internal reflection ?

    • Difference between apparent and real depth of a pond

    • Mirage on hot summer days

    • Brilliance of diamond

    • Working of optical fibre

    Solution

    A.

    Difference between apparent and real depth of a pond

    Real and apparent depth are explains on the basis of refraction only. The concept of TIR is not involve here.

    Question 1160
    CBSEENPH12039941
    Question 1161
    CBSEENPH12039944

    A photoelectric surface is illuminated successively by monochromatic light of wavelength λ and λ/2. If the maximum kinetic energy of the emitted photoelectrons in the second case is 3 times that in the first case, the work function of the surface of the material is 

    (h = planck's constant, c= speed of light)

    • hc/ 2λ

    • hc/λ

    • 2 hc/λ

    • hc/3λ

    Solution

    A.

    hc/ 2λ

    According to Einstein photoelectric equation,
    E = Kmax + Φ
    Where Kmax is the maximum kinetic energy of emitted electron and Φ is work function of electrons.
    Kmax = E - Φ = hv - Φ
    Kmaxhc over straight lambda minus ϕ
    Similarly, in the second case, maximum kinetic energy of emitted electron is 3 times that in the first case, we get
    3Kmax hc over straight lambda minus ϕ 
    solving EQs (i) and (ii), we get work function of an emitted electron from a metal surface.
    Φ = hc/2λ

    Question 1163
    CBSEENPH12039947
    Question 1165
    CBSEENPH12039949

    Two slits in  Young's experiment have widths in the ratio 1:25.The ratio of intensity at the maxima and minima in the interference pattern Imax/Imin is

    • 9/4

    • 121/49

    • 49/121

    • 4/9

    Solution

    A.

    9/4

    Given, YDSE experiment, having two slits of width are in the ratio of 1:25
    So, ratio of intensity

    straight I subscript 1 over straight I subscript 2 space equals space straight W subscript 1 over straight W subscript 2 space equals space 1 over 25

rightwards double arrow space straight I subscript 2 over straight I subscript 1 space equals space 25 over 1
therefore comma
straight I subscript max over straight I subscript min space equals space fraction numerator left parenthesis square root of straight I subscript 2 end root space plus square root of straight I subscript 2 end root right parenthesis squared over denominator left parenthesis square root of straight I subscript 2 end root minus square root of straight I subscript 1 end root right parenthesis squared end fraction space equals space open square brackets fraction numerator square root of begin display style straight I subscript 2 over straight I subscript 1 end style end root plus 1 over denominator square root of straight I subscript 2 over straight I subscript 1 end root minus 1 end fraction close square brackets squared

rightwards double arrow space open square brackets fraction numerator 5 plus 1 over denominator 5 minus 1 end fraction close square brackets squared space equals space open parentheses 6 over 4 close parentheses squared space equals space 36 over 16 space equals space 9 over 4

Thus space straight I subscript max over straight I subscript min space equals space 9 over 4straight I subscript 1 over straight I subscript 2 space equals space straight W subscript 1 over straight W subscript 2 space equals space 1 over 25

rightwards double arrow space straight I subscript 2 over straight I subscript 1 space equals space 25 over 1
therefore comma
straight I subscript max over straight I subscript min space equals space fraction numerator left parenthesis square root of straight I subscript 2 end root space plus square root of straight I subscript 2 end root right parenthesis squared over denominator left parenthesis square root of straight I subscript 2 end root minus square root of straight I subscript 1 end root right parenthesis squared end fraction space equals space open square brackets fraction numerator square root of begin display style straight I subscript 2 over straight I subscript 1 end style end root plus 1 over denominator square root of straight I subscript 2 over straight I subscript 1 end root minus 1 end fraction close square brackets squared

rightwards double arrow space open square brackets fraction numerator 5 plus 1 over denominator 5 minus 1 end fraction close square brackets squared space equals space open parentheses 6 over 4 close parentheses squared space equals space 36 over 16 space equals space 9 over 4

Thus space straight I subscript max over straight I subscript min space equals space 9 over 4

    Question 1170
    CBSEENPH12039960

    In the following figure, the diodes which are forward biased, are

    Solution

    B.

    For forward bias p-type should be higher potential and n-type at a lower potential.

    Question 1172
    CBSEENPH12039969

    An electron in the hydrogen atom jumps from excited state n to the ground state. The wavlength so emitted illuminates a photo -sensitive material having work function 2.75 eV. If the stopping potential of the photo-electron is 10 V, the value of n is 

    • 3

    • 4

    • 5

    • 2

    Solution

    A.

    3

    E = KEmax + W
    eVo + W
     = 10 + 2.75
    E = 12.75 eV


    The difference of 4 and 1 energy level is 12.75 eV. So, the higher energy level is 4 to the ground and excited state is n=3.

    Question 1176
    CBSEENPH12039975

    The mass of a Li presubscript 3 presuperscript 7 nucleus is 0.042u less than the sum of the masses of all its nucleons. The binding energy per nucleon is Li presubscript 3 presuperscript 7 nucleus is nearly

    • 46 MeV

    • 5.6 MeV

    • 3.9 MeV

    • 23 MeV

    Solution

    B.

    5.6 MeV

    If, m = 1 u, c= 3 x 108 ms-1, then 
    E = 931 MeV i.e. 1 u = 931 MeV
    Binding energy = 0.042 x 931 = 39.10 MeV
    therefore, Binding energy per nucleon
    = 39.10/7 = 5.58 = 5.6 MeV

    Question 1177
    CBSEENPH12039976

    Which one of the following statement is false?

    • Pure Si doped with trivalent impurities given a p- type semiconductor

    • Majority carriers in a p- type semiconductor are holes

    • Minority carriers in a p- type semiconductor are electron

    • The resistance of intrinsic semiconductor decreases with increase of temperature

    Solution

    A.

    Pure Si doped with trivalent impurities given a p- type semiconductor

    p-type semiconductor is obtained by adding a small amount of trivalent impurity to a pure sample of semiconductor (Ge).
    Majority charge carriers - holes
    Minority charge carriers - electrons
    n - type  semiconductor are obtained by adding a small amount of pentavalent impurity to a pure sample of semiconductor (Ge)
    Majority charge carriers - electrons
    The resistance of intrinsic semiconductors decreases with the increase of temperature.

    Question 1180
    CBSEENPH12039982

    The device that can act as a complete electronic circuit is

    • Junction diode

    • Integrated circuit

    • Junction transistor

    • Zener diode

    Solution

    B.

    Integrated circuit

    Integrated circuits are miniature electronic circuits produced within a single crystal of semiconductors such as silicon. They contain a million or so transistors and resistors or capacitors. They are widely used in memory circuits, microcomputers, pocket calculators and electronic watches on account of their low cost and bulk, reliability into specific regions of the semiconductor crystals.

    Question 1181
    CBSEENPH12039986

    The energy of a hydrogen atom in the ground state is -13.6 eV. The energy of a He+ ion in the first excited state will be

    • -13.6 eV

    • -27.2 eV

    • -54.4eV

    • -6.8 eV

    Solution

    A.

    -13.6 eV

    Energy E of an atom with principal quantum number n is given n 

    straight E space equals space minus space fraction numerator 13.6 over denominator straight n squared end fraction straight Z squared space for space first space excited space state space straight n space equals space 2 space and space for space He to the power of plus space straight Z space equals space 2
rightwards double arrow space straight E space equals fraction numerator space minus 13.6 space straight x space left parenthesis 2 right parenthesis squared over denominator left parenthesis 2 right parenthesis squared end fraction

space equals space minus 13.6 space eV

    Question 1185
    CBSEENPH12039995

    The potential difference that must be applied to stop the fastest photoelectrons emitted by a nickel surface, having work function 5.01 eV, when ultraviolet light of 200 nm falls on it, must be

    • 2.4 V

    • -1.2 V

    • -2.4 V

    • 1.2 V

    Solution

    D.

    1.2 V

    Energy of incident light E (eV) = 12375/2000 = 6.2 eV (200 nm = 2000 A)
    According to the relation E = Wo +eVo
    rightwards double arrow space straight V subscript straight o space equals fraction numerator straight E space minus straight W subscript straight o over denominator straight e end fraction
space equals fraction numerator left parenthesis 6.2 space minus 5.01 right parenthesis straight e over denominator straight e end fraction
space equals space 1.2 space straight V

    Question 1186
    CBSEENPH12039999

    To get an output Y = 1 from the circuit shown below, the input must be

    • A

      B

      C

      0

      1

      0

    • A

      B

      C

      0

      0

      1
    • A
      B
      C
      1
      0
      1
    • A
      B
      C
      1
      0
      0

    Solution

    C.

    A
    B
    C
    1
    0
    1

    Gate I is OR gate Y' = A + B

    Gate II is AND gate Y = Y'.C
    therefore,
    A = 1, B = 0, C = 1 will give Y = 1

    Question 1187
    CBSEENPH12040000

    A ray of light is incident on a 60o prism at the minimum deviation position. The angle of refraction at the first face (ie, incident face) of the prism is

    • zero

    • 30o

    • 45o

    • 60o

    Solution

    B.

    30o

    The refracting angle of prism 
    A = r1 + r2
    For minimum deviation


    r1 = r2 = r
    A = 2r
    r = A/2  = 60o/2 = 30o
    Question 1192
    CBSEENPH12040013

    When monochromatic radiation of intensity I falls on a metal surface, the number of photoelectrons and their maximum kinetic energy and N and T respectively. If the intensity of radiation is 2I, the number of emitted electrons and their maximum kinetic energy are respectively

    • N and 2T

    • 2N and T

    • 2N and 2T

    • N and T

    Solution

    B.

    2N and T

    i) Kinetic energy of photoelectrons depends on the frequency of incident radiations and is independent of the intensity of illumination.
    ii) A number of photoelectrons depend upon the intensity.
    So, the number of emitted electrons and their maximum kinetic energy are 2N and T respectively.

    Question 1194
    CBSEENPH12040017

    In the nuclear decay given below,

    straight X presubscript straight Z presuperscript straight A space rightwards arrow straight Y presubscript straight Z plus 1 end presubscript presuperscript straight A space rightwards arrow space straight B presubscript straight Z minus 1 end presubscript presuperscript straight A minus 4 end presuperscript asterisk times space rightwards arrow space straight B presubscript straight Z minus 1 end presubscript presuperscript straight A minus 4 end presuperscript
    the particle emitted in the sequence are

    • β, α, γ

    • γ, β, α, 

    •  β,γ, α

    • α, β,γ 

    Solution

    A.

    β, α, γ

    In a nuclear reaction conservation of charge number and mass, the number must hold good.
    Alpha particles are positively charged particles with charge +2e and mass 4 m. Emission of an α particle reduces the mass of the radionuclide by 4 and its atomic number by 2. β- particles are negatively charged particles with rest mass as well as charge same as that of electrons. γ  particles carry no charge and mass.
    Radioactive transition will be as follows.
    straight X presubscript straight Z presuperscript straight A space rightwards arrow space straight Y presubscript straight Z plus 1 end presubscript presuperscript straight A space plus space straight beta subscript negative 1 end subscript superscript 0

straight Y presubscript straight Z plus 1 end presubscript presuperscript straight A space rightwards arrow space straight beta presubscript straight Z minus 1 end presubscript presuperscript straight A minus 4 end presuperscript space plus straight alpha subscript 2 superscript 4

straight beta presubscript straight Z plus 1 end presubscript presuperscript straight A minus 4 end presuperscript space rightwards arrow space presubscript straight Z minus 1 end presubscript presuperscript straight A minus 4 end presuperscript straight beta space plus space straight gamma subscript 0 superscript 0

    Question 1195
    CBSEENPH12040018

    A p-n photodiode is fabricated from a semiconductor with a band gap of 2.5 eV. It ca detect a signal of wavelength

    • 6000 Ao

    • 4000 nm

    • 6000 nm

    • 4000 Ao

    Solution

    D.

    4000 Ao

    Only signals having wavelength less than threshold wavelength will be detected.
    Energy E = hv = hc/λ

    λ = hc / E
    substituting the values of h, c and E in the above equation

    straight lambda space equals space fraction numerator 6.6 space straight x space 10 to the power of negative 34 end exponent space straight x space 3 space straight x space 10 to the power of 8 space over denominator 2.5 space straight x space 1.6 space straight x space 10 to the power of negative 19 end exponent end fraction space equals space 5000 straight A to the power of straight o

As space 4000 space straight A to the power of 0 space less than space 5000 space straight A thin space to the power of straight o
signal space of space wavelength space 4000 space straight A to the power of straight o space can space be space detected space by space the space photodiode.

    Question 1196
    CBSEENPH12040019

    If a diamagnetic substance is brought near the north or the south pole of a bar magnet, it is 

    • repelled by both the poles

    • repelled by the north pole and attracted by the south pole

    • attracted by the north pole and repelled by the south  pole

    • attracted by both the poles

    Solution

    A.

    repelled by both the poles

    The diamagnetic substance is weakly magnetised in a direction opposite to that of applied magnetic field. These are repelled in an external magnetic field ie, have a tendency to move from high to low field region.

    Question 1197
    CBSEENPH12040020

    The number of beta particles emitted by radioactive substance is twice the number  of alpha particle emitted by it. The resulting daughter is an 

    • isobar of parent

    • isomer of parent

    • isotone of parent

    • isotope of parent

    Solution

    D.

    isotope of parent

    Let the radioactive transition is given by
    straight X presubscript straight Z presuperscript straight A space rightwards arrow with negative straight alpha on top space space straight X presubscript straight Z minus 2 end presubscript presuperscript straight A minus 4 end presuperscript space space rightwards arrow with negative 2 straight beta space on top space straight X presubscript straight Z presuperscript straight A minus 4 end presuperscript
    The atoms of an element having a same atomic number but a differnent mass number are called isotopes.
    So, straight X presubscript straight Z presuperscript straight A space and space straight X presubscript straight Z presuperscript straight A minus 4 end presuperscript space are space isotopes.

    Question 1199
    CBSEENPH12040025
    Question 1200
    CBSEENPH12040027

    In a Rutherford scattering experiment when a projectile of charge Z1 and mass M1 approaches a target nucleus of charge Z2 and mass M2, the distance of closest approach is ro.The energy of the projectile is 

    • directly proportional to M1 x M2

    • directly proportional to Z1Z2

    • inversely proportional to Z1

    • directly proportional to mass M1

    Solution

    B.

    directly proportional to Z1Z2

    The particle of mass M1 and charge z1 possess initial velocity u when it at a large distance from the nucleus of an atom having atomic number z2. At the distance of closest approach, the kinetic energy of the particle is completely converted to potential energy. Mathematically,
    1 half M subscript 1 u squared space equals space fraction numerator 1 over denominator 4 pi epsilon subscript o end fraction fraction numerator z subscript 1 z subscript 2 over denominator r subscript 0 end fraction
    so the energy of the particle is directly proportional to z1z2

    Question 1201
    CBSEENPH12040030

    The ionisation energy of the electron in the hydrogen atom in its ground state is 13.6 eV. The atoms are excited to higher energy levels to emit radiations of 6 wavelengths. Maximum wavelength of emitted radiation corresponds to the transition between

    • n = 3 to n =2 states

    • n = 3 to n = 1 states

    • n = 2 to n = 1 states

    • n = 4 to n =3 states

    Solution

    D.

    n = 4 to n =3 states

    Number of spectral lines obtained due to transition of electron from nth orbit to lower orbit is N = n(n-1)/2 and for maximum wavelength, the difference between the orbits of the series should be minimum
    Number of spectral lines N = n (n-1)/2
    = n (n-1)/2 = 6
    = n2-n-12 = 0
    (n-4)(n+3) = 0
    n=4
    Now as the first line of the series has the maximum wavelength, therefore, electrons jump from the 4th orbit to the third orbit.

    Question 1202
    CBSEENPH12040031
    Question 1203
    CBSEENPH12040032

    The number  of photoelectrons emitted from light of a frequency v (higher than the threshold frequency vo) is proportional to 

    • v-vo

    • threshold frequency (vo)

    • the intensity of light

    • the frequency of light (v)

    Solution

    C.

    the intensity of light

    The number of photoelectrons emitted is directly proportional to the intensity of light.

    Question 1206
    CBSEENPH12040043

    The work function of a surface of a photosensitive material is 6.2 eV. The wavelength of the incident radiation for which the stopping potential is 5 V lies in the 

    • ultraviolet region

    • visible region

    • infrared region

    • X-ray region

    Solution

    A.

    ultraviolet region

    According to laws of photoelectric effect
    KEmax = E - Φ
    where Φ is work function and KEmax is the maximum  kinetic energy of photoelectron.
    hv = eVo + Φ
    or
    hv = 5eV + 6.2 eV = 11.2 eV
    therefore, λ = (12400/11.2) = 1000 A
    Hence, the radiation lies in ultraviolet region.

    Question 1207
    CBSEENPH12040044

    The ground state energy of hydrogen atom is -13.6 eV. When its electron is in the first excited state, its excitation energy is

    • 3.4 eV

    • 6.8 eV

    • 10.2 eV

    • zero

    Solution

    C.

    10.2 eV

    Excitation energy is defined as the energy required to take the electron from ground level orbit to any higher order orbit (ie, n = 2,3,4...)

    Given, ground state energy of hydrogen atom

    E1 = - 13.6/(2)2 eV

    Energy of electron in first excited state (ie, n = 2)
    E2 = - 13.6/ (2)2 eV

    Therefore, excitation energy

    ΔE = E2-E1
     =(-13.6/4) - (-13.6)
     = - 3.4 + 13.6 = 10.2 eV

    Question 1208
    CBSEENPH12040046

    A p-n photodiode is made of a material with a band gap of 2.0 eV. The minimum frequency of the radiation that can be absorbed by the material is nearly

    • 10 x 1014 Hz

    • 5 x 1014 Hz

    • 1 x 1014 Hz

    • 20 x 1014 Hz

    Solution

    B.

    5 x 1014 Hz

    the p-n photodiode is a semiconductor diode that produces a significant current when illuminated. It is reversed biased but is operated below the breakdown voltage.
    Energy of radiation = band gap energy
    ie, hv = 2.0 eV
    or  v= 2.0 x 1.6 x 10-19 / 6.6 x 10-34 = 5 x 1014 Hz

    Question 1210
    CBSEENPH12040048

    Two thin lenses of focal lengths f1 and f2 are in contact and coaxial. The power of the combination is 

    • square root of straight f subscript 1 over straight f subscript 2 end root
    • square root of straight f subscript 2 over straight f subscript 1 end root
    • fraction numerator straight f subscript 1 straight f subscript 2 over denominator straight f subscript 1 space plus straight f subscript 2 end fraction
    • fraction numerator straight f subscript 1 plus straight f subscript 2 over denominator straight f subscript 1 straight f subscript 2 end fraction

    Solution

    D.

    fraction numerator straight f subscript 1 plus straight f subscript 2 over denominator straight f subscript 1 straight f subscript 2 end fraction

    If two thin lenses of focal lengths f1, f2 are placed in contact coaxially, then equivalent focal length of combination is 
    1 over straight F space equals 1 over f subscript 1 plus 1 over f subscript 2 minus fraction numerator 0 over denominator f subscript 1 f subscript 2 end fraction space equals space 1 over f subscript 1 plus 1 over f subscript 2
P o w e r space f o r space t h e space c o m b i n a t i o n space i s space
P space equals space 1 over F space space equals 1 over f subscript 1 space plus 1 over f subscript 2 space equals space fraction numerator f subscript 1 plus f subscript 2 over denominator f subscript 1 f subscript 2 end fraction

    Question 1213
    CBSEENPH12040055

    Two periodic waves of intensities I2 and I2 pass through a region at the same time in the same direction. The sum of the maximum and minimum intensities is 

    • I1 + I2

    • open parentheses square root of straight I subscript 1 end root plus square root of straight I subscript 2 end root close parentheses squared
    • left parenthesis square root of straight I subscript 1 end root minus square root of straight I subscript 2 end root right parenthesis squared
    • 2(I1 +I2)

    Solution

    D.

    2(I1 +I2)

    Resultant intensity of two periodic waves is given by
    straight I space equals space straight I subscript 1 space plus space straight I subscript 2 space plus space 2 square root of straight I subscript 1 straight I subscript 2 end root space cosδ
    where δ is the phase difference between the waves. For minimum intensity 
    δ = 2nπ; n = 0,1,2,...... etc.
    Therefore, for zero order maxima, cos δ =-1
    straight I subscript max space equals space straight I subscript 1 space plus straight I subscript 2 space plus space 2 square root of straight I subscript 1 straight I subscript 2 end root space equals space left parenthesis square root of straight I subscript 1 end root space plus space square root of straight I subscript 2 end root right parenthesis squared
For space minimum space intensity comma space space equals space left parenthesis 2 straight n minus 1 right parenthesis straight pi semicolon
straight n space equals space 1 comma 2 comma.... etc.
Therefore space for space 1 space st space order space minima comma space cos space space equals space minus space 1
straight I subscript min space equals space straight I subscript 1 space plus space straight I subscript italic 2 space minus space 2 square root of straight I subscript 1 straight I subscript 2 end root
left parenthesis square root of straight I subscript 1 end root space minus space square root of straight I subscript 2 end root right parenthesis squared
therefore
straight I subscript max space plus straight I subscript min space equals space space left parenthesis square root of straight I subscript 1 end root space plus space square root of straight I subscript 2 end root right parenthesis squared space plus left parenthesis square root of straight I subscript 1 end root space minus space square root of straight I subscript 2 end root right parenthesis squared
equals space 2 space left parenthesis straight I subscript 1 space plus straight I subscript 2 right parenthesis

    Question 1215
    CBSEENPH12040062

    Two points are located at a distance of 10 m and 15 m from the source of oscillation. The period of oscillation is 0.05 s and the velocity of the wave is 300 m/s. What is the phase difference between the oscillation of two points?

    • π/3

    • 2π/3

    • π

    • π/6

    Solution

    B.

    2π/3

    Phase difference = (2π/λ) x path difference
    path difference between two points,
    Δ x = 15-10 = 5 m
    Time period, T = 0.05 s
    ⇒ frequency v = 1/T
     = 1/0.05 = 20 Hz
    Velocity, v= 300 m/s
    therefore, wavelength, λ = v/V = 300/20 = 15 m
    Hence, phase difference
    Δ Φ = (2π /λ) x Δ x
     = (2π /15) x 5 = (2π /3)

    Question 1216
    CBSEENPH12040063

    Two nuclei have their mass number in the ratio of 1:3. The ratio of their nuclear densities would be

    • 1:3

    • 3:1

    • (3)1/3 : 1

    • 1:1

    Solution

    D.

    1:1

    Density of nuclear matter is independent of mass number, so the required ratio is 1:1
    Alternative :
    A1 : A2 = 1:3
    Their radii will be in the ratio
    straight R subscript straight o straight A subscript 1 superscript 1 divided by 3 end superscript space colon space straight R subscript straight o straight A subscript 2 superscript 1 divided by 3 end superscript space equals space 1 colon space 3 to the power of 1 divided by 3 end exponent
Density space equals space fraction numerator straight A over denominator begin display style 4 over 3 end style πR cubed end fraction
therefore comma space
straight rho subscript straight A subscript 1 space end subscript colon space straight rho subscript straight A subscript 2 end subscript space space equals space fraction numerator 1 over denominator begin display style 4 over 3 end style πR subscript 0 cubed.1 cubed end fraction space equals fraction numerator 1 over denominator begin display style 4 over 3 πR subscript 0 cubed. left parenthesis 3 to the power of 1 divided by 3 right parenthesis end exponent right parenthesis cubed end style end fraction
    Their nuclear densities will be the same.

    Tips: -

    Question 1217
    CBSEENPH12040066

    The Circuit is equivalent to 


    • AND gate

    • NAND gate

    • NOR gate

    • OR Gate

    Solution

    C.

    NOR gate

    The gate circuit can be shown by giving two inputs A and B.

    Output of NOR gate,

    Output space of space NOR space gate comma
straight Y subscript 1 space equals space stack straight A space plus straight B with bar on top
output space of space NAND space gate comma
straight Y subscript 2 space equals space stack straight Y subscript 1. straight Y subscript 1 with bar on top
equals space stack stack straight A plus straight B with bar on top space. space stack straight A plus straight B with bar on top with bar on top
space equals stack stack straight A plus straight B with bar on top with bar on top space plus space stack stack straight A plus straight B with bar on top with bar on top
equals space left parenthesis straight A plus straight B right parenthesis space plus space left parenthesis straight A plus straight B right parenthesis
equals space straight A plus straight B
Output space of space NOT space gate comma space
straight Y space equals stack straight Y subscript 2 with bar on top
equals space stack straight A plus straight B with bar on top
    Which is output of NOR gate.

    Question 1218
    CBSEENPH12040067

    In radioactive decay process, the negatively charged emitted beta particles are:

    • the electrons present inside the nucleus

    • the electrons produced as a result  of the decay of neutrons inside the nucleus

    • the electrons produced as a result of collisions between atoms

    • the electrons produced as a result of collisions between atoms

    Solution

    B.

    the electrons produced as a result  of the decay of neutrons inside the nucleus

    Beta decay can involve the emission of either electrons or positirons. The electrons or positrons emitted in a beta-decay do not exist inside the nucleus. They are only createdat the time of emission, just as photons are created when an atom makes a  transition from higher to a lower energy state. 
    In negative Beta decay a neutron in the nucleus is transformed into a proton, an electron and an antineutrino. Hence, in radioactive decay process, the negatively charged emitted beta process are the electrons produced as a result of the decay of neutrons present inside the nucleus.

    Question 1219
    CBSEENPH12040069

    A nucleus has straight X presubscript straight Z presuperscript straight A mass represented by  M (A, Z). If Mp and Mn denote the mass of proton and neutron respectively and BE the binding energy (in MeV), then:

    • BE = [M(A,Z)-ZMp - (A-Z)Mn]c2

    • BE = [ZMp + (A-Z)Mn -M(A,Z)]c2

    • BE = [ZMp + AMn - M (A,Z)]c2

    • BE = M (A,Z)- ZMp - (A-Z) Mn

    Solution

    B.

    BE = [ZMp + (A-Z)Mn -M(A,Z)]c2

    In the case of formation of a nucleus, the evolution of energy equal to the binding energy of the nucleus takes place due to the disappearance of a fraction of the total mass. If the quantity of mass disappearing is ΔM, then the binding energy is
    BE = ΔMc2
    From the above discussion, it is clear that the mass of the nucleus must be less than the sum of the masses of the constituent neutrons and protons. We can then write.


    ΔM= [ZMp + (A-Z)Mn -M(A,Z)
    Where M (A, Z)  is the mass of the atom of mass number A and atomic number Z. Hence, the binding energy of the nucleus is
    BE = [ZMp + (A-Z)Mn -M(A,Z)]c2

    Where N = A -Z = number of neutrons.
    Question 1220
    CBSEENPH12040070

    If the nucleus Al presubscript 13 presuperscript 27 has a nuclear radius of about 3.6 fm, then Te presubscript 52 presuperscript 125 would have its radius approximately as: 

    • 6.0 fm

    • 9.6 fm

    • 12.0 fm

    • 4.8 fm

    Solution

    A.

    6.0 fm

    If R is the radius of the nucleus, the corresponding volume 4πR3/3 has been found to be proportional to A.
    This relationship is expressed in inverse form as
     R = Ro A1/3
    The value of Ro is 1.2 x 10-15 m, ie, 1.2 fm

    straight R subscript Al over straight R subscript Te space equals space fraction numerator R subscript o left parenthesis A subscript A l end subscript right parenthesis to the power of 1 divided by 3 end exponent over denominator R subscript o left parenthesis A subscript T e end subscript right parenthesis to the power of 1 divided by 3 end exponent end fraction

straight R subscript Al over straight R subscript Te space equals space fraction numerator left parenthesis A subscript A l end subscript right parenthesis to the power of 1 divided by 3 end exponent over denominator left parenthesis A subscript T e end subscript right parenthesis to the power of 1 divided by 3 end exponent end fraction

space equals space fraction numerator left parenthesis 27 right parenthesis to the power of 1 divided by 3 end exponent over denominator left parenthesis 125 right parenthesis to the power of 1 divided by 3 end exponent end fraction space equals space 3 over 5
straight R subscript Te space equals space 5 over 3 space straight x space straight R subscript Al space equals space 5 over 3 straight x space 3.6
6 space fm

    Question 1221
    CBSEENPH12040075

    The total energy of an electron in the ground state of a hydrogen atom is -13.6 eV. The kinetic energy of an electron in the first excited state is: 

    • 3.4 eV

    • 6.8 eV

    • 13.6 eV

    • 1.7 eV

    Solution

    A.

    3.4 eV

    The total energy of an electron in the orbit is equal to negative of its kinetic energy.
     The energy of hydrogen atom when the electron revolves in nth orbit is 
    E = -13.6/n2 eV
    In the ground state: n =1
    E = - -13.6/12 = -13.6 eV
    For n = 2, E  = -13.6/22 = -3.4 eV
    so, the kinetic energy of an electron in the first excited state (i,e, for n = 2 ) is
    K = - E = - (-3.4) - 3.4 eV

    Question 1222
    CBSEENPH12040077

    Monochromatic light of frequency 6.0 x 1014 Hz is produced by a laser. The power emitted is 2 x 10-3 W. The number of photons emitted, on the average, by the source per second is:

    • 5 x 1015

    • 5 x 1016

    • 5 x 1017

    •  5 x104

    Solution

    A.

    5 x 1015

    Photons are the packets of energy. Power emitted ,
    P = 2 x 10-3 W
    Energy of photon, 
    E = hv 
     = 6.6 x 10-34 x 6 x 1014 J
    h being planck's constant.
    Numer of photons emitted per second
    n = P/E
    =  2 x 10-3 / 6.6 x 10-34 x 6 x 1014
     = 5 x 1015

    Question 1223
    CBSEENPH12040078

    The frequency  of a light wave in the material is 2 x 10 Hz and wavelength is 5000 A. the refractive index of material will be:

    • 1.40

    • 1.50

    • 3.00

    • 1.33

    Solution

    C.

    3.00

    The velocity of light waves in the material is 
    ν = vλ ... (i)
    Refractive index of material is
    μ = c/v  .... (ii)
    where c is the speed  of light in vacuum or air 
    Where c is speed of light in vacuum or air 
    or μ = c/vλ   (iii)
    Given, v = 2 x 1014 Hz,
    λ = 5000 A = 5000 x 10-10 m,
    c =  3x 108 m/s
    Hence from Eq. (iii), we get
     μ = 3 x 108 / 2 x 1014 x 500 x 10-10 = 3.00

    Question 1224
    CBSEENPH12040079

    A  5 W source emits monochromatic light of wavelength 5000 A. When placed 0.5 m away, it liberates photoelectrons from a photosensitive metallic surface. when the source si moved to a distance of 1.0 m, the number of photoelectrons liberated will be reduced by a factor  of:

    • 4

    • 8

    • 16

    • 2

    Solution

    A.

    4

    The intensity of light is inversely proportional to the square of the distance.
    straight I space proportional to space 1 over straight r squared
straight I subscript 1 over straight I subscript 2 space equals space fraction numerator left parenthesis straight r subscript 1 right parenthesis squared over denominator left parenthesis straight r subscript 2 right parenthesis squared end fraction
Given space comma space straight r subscript 1 space equals space 0.5 space straight m comma space straight r subscript 2 space equals space 1.0 space straight m
therefore comma
straight I subscript 2 over straight I subscript 1 space equals space fraction numerator left parenthesis 0.5 right parenthesis squared over denominator left parenthesis 1 right parenthesis squared end fraction space equals space 1 fourth
    Now, since number of photoelectric emitted per second is directly proportional intensity, so number of electrons emitted would decrease by factor of 4.

    Question 1225
    CBSEENPH12040080

    Two radioactive substance A and B have decay constants 5λ and λ respectively. At t = 0 they have the same number of nuclei. The ratio of a number of nuclei of A t\o those of B will be open parentheses 1 over straight e close parentheses squared after a time interval:

    • 1/ 4λ

    • 1/2λ

    Solution

    D.

    1/2λ

    Number of nuclei remained after time t can be written as
    N = Noe-λt
    where No is initial number of nuclei of both the substances.
    straight N subscript 1 space equals space straight N subscript straight o straight e to the power of negative 5 λt space end exponent space space... space left parenthesis straight i right parenthesis
straight N subscript 2 space equals space straight N subscript straight o straight e to the power of negative λt end exponent space space space space space.... space left parenthesis ii right parenthesis
Dividing space eq. space left parenthesis straight i right parenthesis space by space Eq space left parenthesis ii right parenthesis space obtain
straight N subscript 1 over straight N subscript 2 space equals space open parentheses 1 over straight e close parentheses squared space equals space open parentheses 1 over straight e squared close parentheses
hence comma space 1 over straight e squared space equals space 1 over straight e to the power of 4 λt end exponent
Comparing space the space powers comma space we space get
2 space equals space 4 λt
straight t space equals space fraction numerator 2 over denominator 4 straight lambda end fraction space equals space fraction numerator 1 over denominator 2 straight lambda end fractionstraight N subscript 1 space equals space straight N subscript straight o straight e to the power of negative 5 λt space end exponent space space... space left parenthesis straight i right parenthesis
straight N subscript 2 space equals space straight N subscript straight o straight e to the power of negative λt end exponent space space space space space.... space left parenthesis ii right parenthesis
Dividing space eq. space left parenthesis straight i right parenthesis space by space Eq space left parenthesis ii right parenthesis space obtain
straight N subscript 1 over straight N subscript 2 space equals space open parentheses 1 over straight e close parentheses squared space equals space open parentheses 1 over straight e squared close parentheses
hence comma space 1 over straight e squared space equals space 1 over straight e to the power of 4 λt end exponent
Comparing space the space powers comma space we space get
2 space equals space 4 λt
straight t space equals space fraction numerator 2 over denominator 4 straight lambda end fraction space equals space fraction numerator 1 over denominator 2 straight lambda end fraction

    Question 1226
    CBSEENPH12040082

    Monochromatic light of frequency 6.0 x 1014 Hz is produced by a laser. The power emitted is 2 x 10-3 W The number of photons emitted, on the average, by the source per second is:

    • 5 x 1015

    • 5 x 106

    • 5 x 1017

    • 5 x 1014

    Solution

    A.

    5 x 1015

    Photons are the packest of energy.
    Power emitted,
    P = 2 x 10-3 W
    Energy of photon,
    E = hv
    = 6.6 x 10-34 x 6 x 1014 J
    h being Planck's constant
    Number of photons emitted per second
    n = P/E
     =fraction numerator 2 space straight x space 10 to the power of negative 3 end exponent over denominator 6.6 space straight x space 10 to the power of negative 34 end exponent space straight x space 6 space straight x space 10 to the power of 14 end fraction
     = 5 x 1015

    Question 1227
    CBSEENPH12040088

    The binding energy of deuteron is 2.2 MeV and that of  He presubscript 2 presuperscript 4 is 28 MeV. If two deuterons are fused to form one He presubscript 2 presuperscript 4 then the energy released is

    • 25.8 MeV

    • 23.6 MeV

    • 19.2 MeV

    • 30.2 MeV

    Solution

    B.

    23.6 MeV

    The reaction can be written as:
    straight H presubscript 1 superscript 2 space plus space straight H presubscript 1 superscript 2 space space space rightwards arrow space space space He presubscript 2 superscript 4 space plus space energy
    The energy released in the reaction is difference of binding energies of daughter and parent nuclei.
    Hence, energy released.
     = binding energy of He presubscript 2 superscript 4 - 2 x binding energy of straight H presubscript 1 superscript 2
     = 28 - 2 x 2.2 = 23.6 MeV

    Question 1228
    CBSEENPH12040089

    In a radioactive material the activity at time t1 is R1 and at a later time t2, it is R2. If the dacay constant of the material is λ, then

    • R1 = R2 e-λ(t1 -t2 )

    • R1 = R2 eλ(t1 -t2 )

    • R1 = R2 e(t2 /t1 )

    • R1 = R2

    Solution

    A.

    R1 = R2 e-λ(t1 -t2 )

    The decay rate R of radioactive materials the number of decays per second.
    From radioactive decay law.
          negative dN over dt proportional to space straight N space space or space space space minus dN over dt space equals λN
    Thus,   straight R equals negative dN over dt space space or space space straight R space proportional to space space straight N
    or         straight R space equals space λN space space space or space space space straight R space equals space λN subscript 0 straight e to the power of negative λt end exponent                    ...(i)
    where straight R subscript 0 space equals space λN subscript 0 is the activity of the radioactive material at time t = 0.
    At time t1,  straight R subscript 1 space equals space straight R subscript 0 straight e to the power of negative λt subscript 1 end exponent       ...(ii)
    At time t2,   straight R subscript 2 space equals space straight R subscript 0 straight e to the power of negative λt subscript 2 end exponent      ...(iii)
    Dividing Eq. (ii) by (iii), we have,
                          straight R subscript 1 over straight R subscript 2 space equals space straight e to the power of negative λt subscript 1 end exponent over straight e to the power of negative λt subscript 2 end exponent space equals space straight e to the power of negative straight lambda left parenthesis straight t subscript 1 minus straight t subscript 2 right parenthesis end exponent
or space space space straight R subscript 1 space equals space straight R subscript 2 straight e to the power of negative straight lambda left parenthesis straight t subscript 1 minus straight t subscript 2 right parenthesis end exponent

    Question 1229
    CBSEENPH12040090

    Ionization potential of hydrogen atom is 13.6 eV. Hydrogen atoms in the ground state are excited by monochromatic radiation of photon energy 12.1 eV. According to Bohr's theory, the spectral lines emitted by hydrogen will be

    • two 

    • three

    • four

    • one

    Solution

    B.

    three

    Ionization energy corresponding to ionization potential  = -13.6 eV.
    Photon energy incident = 12.1 eV
    So, the energy of electron in excited state
        = -13.6 + 12.1 = -1.5 eV
    i.e.,      straight E subscript straight n space equals space minus fraction numerator 13.6 over denominator straight n squared end fraction space rightwards double arrow space space straight n squared space equals space minus fraction numerator 13.6 over denominator negative 1.5 end fraction space equals space 9
    therefore space space space space space space straight n space equals space 3
    i.e., energy of electron in excited state corresponds to third orbit.
    The possible spectral lines are when electron jumps from orbit 3rd to 2nd; 3rd to 1st and 2nd to 1st. Thus, 3 spectral lines are emitted.

    Question 1230
    CBSEENPH12040091

    A microscope is focussed on a mark on a piece of paper and then a slab of glass of thickness 3 cm and refractive index 1.5 is placed over the mark. How should the microscope be moved to get the mark in focus again?

    • 1 cm upward

    • 4.5 cm downward

    • 1 cm downward

    • 2 cm upward

    Solution

    A.

    1 cm upward

    Apparent depth of mark as seen through a glass slab of thickness x and refractive index straight mu is
    Apparent space depth space equals space fraction numerator Real space depth over denominator Refractive space index end fraction
or space space space space straight x apostrophe space equals space straight x over straight mu space equals space fraction numerator 3 over denominator 1.5 end fraction space equals space 2 space cm
    As image appears to be raised by 1 cm, therefore, microscope must be moved upward by 1 cm.

    Question 1231
    CBSEENPH12040092

    A photo-cell employs photoelectric effect to convert

    • change in the frequency of light into a change in electric voltage

    • change in the intensity of illumination into a change in photoelectric current

    • change in the intensity of illumination into a change in the work function of the photocathode

    • change in the frequency of light into a change in the electric current

    Solution

    B.

    change in the intensity of illumination into a change in photoelectric current

    In photoelectric effect when monochromatic radiations of suitable frequency fall on the photo-sensitive plate called cathode, the photoelectrons are emitted which get accelerated towards anode. These electrons flow in the outer circuit resulting in the photoelectric current.
    Using the incident radiations of a fixed frequency, it is found that the photoelectric current increases linearly with the intensity of incident light as shown in figure. Hence, a photocell employs photoelectric effect to convert change in the intensity of illumination into a change in photoelectric current.

    Question 1232
    CBSEENPH12040096

    When photons of energy hv fall on an aluminium plate (of work function E0), photoelectrons of maximum kinetic energy K are ejected. If the frequency of the radiation is doubled, the maximum kinetic energy of the ejected photoelectrons will be

    • K+E0

    • 2K

    • K

    • K+hv

    Solution

    D.

    K+hv

    The energy of photon is used in liberating the electron from metal surface and in imparting the kinetic energy to emitted photoelectron.
    According to Einstein's photoelectric effect energy of photon = KE of photoelectron + work function of metal
    i.e.,                  hv space equals space 1 half mv squared plus straight E subscript 0
    or                   hv space equals space straight K subscript max space plus space straight E subscript 0 space space space space space space space space space space space space space space space space space space space space space space space space space space... left parenthesis straight i right parenthesis
    Now, we have given, 
                               straight v apostrophe space equals space 2 straight v
    Therefore,       straight K apostrophe subscript max space equals space straight h left parenthesis 2 straight v right parenthesis minus straight E subscript 0
                          straight K apostrophe subscript max space equals space 2 hv minus straight E subscript 0                     ...(ii)
    From Eqs. (i) and (ii), we have
              straight K apostrophe subscript max space equals space 2 left parenthesis straight K subscript max space plus space straight E subscript 0 right parenthesis space minus straight E subscript 0
space space space space space space space space space equals 2 straight K subscript max space plus space straight E subscript 0
space space space space space space space space space equals space straight K subscript max space plus space left parenthesis straight K subscript max space plus space straight E subscript 0 right parenthesis
                      equals straight K subscript max space plus hv space space space space space left square bracket From space Eq. space left parenthesis straight i right parenthesis right square bracket
    Putting             straight K subscript max space equals space straight K
    therefore space space space space space space space space straight K apostrophe subscript max space equals space straight K space plus space hv

    Question 1233
    CBSEENPH12040098

    The momentum of a photon of energy 1 MeV in kg m/s, will be

    • 0.33 space cross times space 10 to the power of 6
    • 7 cross times 10 to the power of negative 24 end exponent
    • 10 to the power of negative 22 end exponent
    • 5 cross times 10 to the power of negative 22 end exponent

    Solution

    D.

    5 cross times 10 to the power of negative 22 end exponent

    Energy of photon is given by
                     straight E space equals space hc over straight lambda                                 ...(i)
    Where h is Planck's constant, c the velocity of light and straight lambda its wavelength.
    de-Broglie wavelength is given by
                             straight lambda space equals space straight h over straight p                           ...(ii)
               p being momentum of photon. 
    From Eqs. (i) and (ii), we can have         
                                straight E space equals space fraction numerator hc over denominator straight h divided by straight p end fraction space equals space pc
                   or space space space space space space space space space space space space space space space straight p space equals space straight E divided by straight c
    Given comma space space straight E space equals space 1 space MeV space equals space 1 cross times 10 to the power of 6 cross times 1.6 cross times 10 to the power of negative 19 end exponent straight J
                    straight C space equals 3 space cross times space 10 to the power of 8 space straight m divided by straight s
    Hence, after putting numerical values, we obtain
                straight p equals fraction numerator 1 cross times 10 to the power of 6 cross times 1.6 cross times 10 to the power of negative 19 end exponent over denominator 3 cross times 10 to the power of 8 end fraction kgm divided by straight s
space space space equals space 5 space cross times space 10 to the power of negative 22 end exponent space kgm divided by straight s

    Question 1234
    CBSEENPH12040099

    The radius of germanium (Ge) nuclide is measured to be twice the radius of Be presubscript 4 presuperscript 9. The number of nucleons in Ge are

    • 73

    • 74

    • 75

    • 72

    Solution

    D.

    72

    Let radius of Be presubscript 4 presuperscript 9 be nucleus be r. Then radius of germanium (Ge) nucleus will be 2r.
    Radius of a nucleus is given by:
                 space space space space space space space straight R space equals space straight R subscript 0 straight A to the power of 1 divided by 3 end exponent
therefore space space space space straight R subscript 1 over straight R subscript 2 space equals space open parentheses straight A subscript 1 over straight A subscript 2 close parentheses to the power of 1 divided by 3 end exponent
rightwards double arrow space space space fraction numerator straight r over denominator 2 straight r end fraction space equals space open parentheses 9 over straight A subscript 2 close parentheses to the power of 1 divided by 3 end exponent space space space space space space space space space space space space space space space space space space space space space open parentheses because space space straight A subscript 1 equals space 9 close parentheses
rightwards double arrow space space space open parentheses 1 half close parentheses cubed space equals space 9 over straight A subscript 2
Hence comma space space space space space straight A subscript 2 space equals 9 space cross times space left parenthesis 2 right parenthesis cubed
space space space space space space space space space space space space space space space space space space equals space 9 space cross times space 8
space space space space space space space space space space space space space space space space space space equals space 72
    Thus, in germanium (Ge) nucleus number of nucleons is 72.

    Question 1235
    CBSEENPH12040102

    A convex lens and a concave lens, each having same focal length of 25 cm, are put in contact to form a combination of lenses. The power in diopters of the combination is

    • 25

    • 50

    • infinite

    • zero

    Solution

    D.

    zero

    Focal length of combination of lenses placed in contact is
                           1 over straight F space equals space 1 over straight f subscript 1 space plus space 1 over straight f subscript 2
    For convex lens,   straight f subscript 1 space equals space 25 space cm
    For concave lens, straight f subscript 2 space equals space minus 25 space cm
    Hence,         1 over straight F space equals space 1 over 25 plus fraction numerator 1 over denominator negative 25 end fraction
                                    equals 1 over 25 minus 1 over 25 space equals space 0
    therefore                           straight F space equals space 1 over 0 space equals space infinity
    Hence, power of combination
                        straight P space equals space 1 over straight F space equals space 0 space straight D

    Question 1237
    CBSEENPH12040135
    Question 1238
    CBSEENPH12040136

    An em wave is propagating in a medium with a velocity V = Vi^ . The instataneous oscillating electric field of this em wave is along +y axis. Then the direction of oscillating magnetic field of the em wave will be along

    • -z direction

    • +z direction

    • -x direction

    • -y-direction

    Solution

    B.

    +z direction

    As we know, 

    E  x B = V(Ej^ ) x (B) = Vi^

    (Therefore , electric field vector is along + y axis)

    So, B = Bk^

    i.e., direction of magnetic field vector is along + z direction.

    Question 1239
    CBSEENPH12040158

    The maximum numbers of possible interference maxima for slit separation equal to twice the wavelength in Young's double slit experiment is

    • infinite

    • five

    • three

    • zero

    Solution

    B.

    five

    The condition of interference maxima is

    d sin θ = sin θ  = dGiven, d = 2λsin θ = 2λ = n/2

    The magnitude of sin θ lies between 0 and 1

    When n = 0, sinθ = 0 ⇒θ = 0°

    When n = 1, sin θ = 1/2 ⇒ θ =30°

    When n = 2, sin θ = 1⇒ θ =90°

    Thus, there is central maximum ( θ = 0°), on other side of it maxima lie at θ = 30° and θ = 90°, so maximum number of possible interference maxima is 5.

    Question 1240
    CBSEENPH12040174

    Light of wavelength 6000 A0 is reflected at nearly normal incidence from a soap film of refractive index 1.4. The least thickness of the film that will appear black is

    • 200 A0

    • 2000 A0

    • 1000 A0

    • Infinity

    Solution

    B.

    2000 A0

    for the minimum in reflected light

    2μtcosr =nλ

    t=2μcosrtmin=λ2μ=6000A02×1.4    =2142A02000A0

    Question 1241
    CBSEENPH12040175

    Light travels faster in air than that in glass .This is accordance with

    • wave theory of light

    • corpuscular theory of light

    • Neither(a) nor(b)

    • Both (a) and (b)

    Solution

    A.

    wave theory of light

    Light travels faster in air than in glass. This is accordance with wave theory of light.

    Question 1242
    CBSEENPH12040176

    In Young's double slit experiment, light of wavelength 6000 A0 is used to produced fringes of width 0.8 mm at a distance of 2.5 m. If the whole appart is dropped in liquid of refractive index 1.6, then the fringe width will be

    • 0.2mm

    • 0.4mm

    • 0.5mm

    • 0.6mm

    Solution

    C.

    0.5mm

    The Young's double slit experiment belongs to a general class of "double path "experiments, in which a wave is split into two separate waves that later combine into a single wave.

    In water λ is reduced to λμ so λ' so λ' =λ16As ω=dλ      ω'ω=λ'λ=λ16λ  or ω'=0.81.6=0.5mm

    Question 1243
    CBSEENPH12040177

    The electric potential at the surface of an atomic nucleus (Z = 50) of radius 9.0×10-15m is

    • 8×106 V

    • 80V

    • 9×105 V

    • 9V

    Solution

    A.

    8×106 V

    V=14πεoQR=14πεoZeR                    =9×109×50×1.6×10-199.0×10-15                  V  =8×106Volt

    Question 1244
    CBSEENPH12040183

     In forward biased if the p-n junctions diode is forward biased, then width of potential barrier in p-n junction diode

    • remains constant

    • increase

    • decrease

    • None of these

    Solution

    C.

    decrease

    In forward bias the terminal of the same polarities are connected between the diode and the supply. Hence by repulsion excess number of holes or electron come out and width of potential barrier can be decreased.

    Question 1245
    CBSEENPH12040184

    If the energy released in the fission of one nucleus is 3.2x10-11J, then number of nuclei required per second in a power plant of 16 kW is

    • 0.5×1014

    • 0.5×1012

    • 5×1012

    • 5×1014

    Solution

    D.

    5×1014

    The number of nuclei required per second is

            n=PE=16×1033.2×10-11=5×1014

    Question 1246
    CBSEENPH12040187

    A light of wavelength 2000 Afalls on a metallic surface of work function 5.01 eV then required potential difference to slope fastest photoelectron is (h = 6.62 x 10-34J-s)

    • 4.8V

    • 3.6V

    • 2.4V

    • 1.2V

    Solution

    D.

    1.2V

    We know that,Energy of photon=hcλ=6.62×10-34×3×1082000×10-10J=6.62×10-34×3×1082×10-7×1.6×10-19eV                 since 1eV=1.6×10-19= 6.20eVEnergy of the fastest emitted photoelectron,=hν-νo                                where νo is the work function=6.2-5.01=1.19V=1.2V

    Question 1247
    CBSEENPH12040193

    The enregy of a photon corresponding to the visible light maximum wavelength is nearly

    • 7ev

    • 3.2eV

    • 1eV

    • 1.6eV

    Solution

    D.

    1.6eV

    In the visible light λmax= 7800Ao

    E=hcλ=123757800eV=1.6 eV

    Question 1249
    CBSEENPH12040195

    The radius of electron second stationary orbit in Bohr's atom is R. The radius of third orbit will be

    • 2.25R

    • 3R

    • R/3

    • 9R

    Solution

    D.

    9R

    rn=n2mh2π24πεoe2rnn2For second orbit n=2r2= Rfor third orbit n=3r3=32Rr3=9R

    Question 1250
    CBSEENPH12040196

    The slope of plate characteristic and mutual characteristic curves of a triode valve is 0.02 mA / V and 1 mA / V. The amplification factor of triode valve is

    • 2×108

    • 20

    • 50

    • 40

    Solution

    C.

    50

    Triode amplification factor μslope of anode charecteristics =VaVg                                              =1mA/V0.02mA/V=50

    Question 1251
    CBSEENPH12040198

    In junction diode, the holes are because of

    • Missing electrons

    • extra electrons

    • protons

    • neutrons

    Solution

    A.

    Missing electrons

    In semiconductor, when an electron leaves its place, a positive charge is left behind and it is known as hole. Hence, holes are created because of missing electrons.

    Question 1252
    CBSEENPH12040199

    The half-life of a radioactive substance is 3.6 days. How much of 20 mg of this radioactive substance will remain after 36 days?

    • 0.0019 mg

    • 1.019 mg

    • 1.109 mg

    • 0.019 mg

    Solution

    D.

    0.019 mg

    Half time T1/2 = 3.6 days

    Initial quantity N0 =20 mg

    Total time = 36 days

    The number of half lives

    n= tT1/2 =363.6 =10Hence the mass of radioactive substance left after 10 half livesN =No × 12n= 20×11024N  = 0.0019 mg

    Question 1253
    CBSEENPH12040200

    The kinetic energy of an electron is 5eV. Calculate the de-Broglie wavelength associated with it (h=6.6×10-34 Js, me =9.1×10-31 kg)

    • 5.47Ao

    • 10.9Ao

    • 2.7Ao

    • None of these

    Solution

    A.

    5.47Ao

    Here:- E =5ev=5×1.6×10-19Jλ=h2mE  =6.6×10-342×9.1×10-31×5×1.6×10-19=6.6×10-341.2066×10-24=5.47×10-10 m=5.47Ao

    Question 1254
    CBSEENPH12040202

    The energy in MeV is released due to transformation of 1kg mass completely into energy is (c=3×108 m/s)

    • 7.625×10MeV

    • 10.5×1029MeV

    • 2.8×10-28MeV

    • 5.625×1029MeV

    Solution

    D.

    5.625×1029MeV

    According to Einstein's  mass energy equivalence

    E=mc2 =1×(3×108)2 =9×1016 J

      =9×10161.6×10-13MeV           (since 1MeV =1.6×10-13J)=5.625×1029 MeV

    Question 1255
    CBSEENPH12040203

    20 kV potential is applied across X-ray tube, the minimum wavelength of X-ray emitted will be

    • 0.62 Ao

    • 0.37 Ao

    • 1.62 Ao

    • 1.31 Ao

    Solution

    A.

    0.62 Ao

    (i)The minimum energy required to eject an electron from the surface is

    called the photoelectric work function of the metal.

    (ii)Energy greater than the work function of the metal (Φo)

    required for electron emission from the metal surface can be supplied by suitably heating

    (or) applying strong electric field or irradiating it by suitable frequency.

    From relation hcλmin =eV λmin =hceV =6.6×10-34×3×1081.6×10-19×20×103     λmin =0.62×10-10 =0.62 Ao

    Question 1256
    CBSEENPH12040204

    In the CB mode of a transistor, when the collector voltage is changed by 0.5 volt, the collector current changes by 0.05 mA. The output resistance will be

    • 10 kΩ

    • 20 kΩ

    • 5 kΩ

    • 2.5 kΩ

    Solution

    A.

    10 kΩ

    Here: ΔVc = 0.5 volt

    ΔI=0.05 mA=0.05×10-3 

    Output resistance is defined as the ratio of change in output voltage or collector voltage (VCB) to the corresponding change in output current or collector current (IC), with the input current or emitter current (IE) kept at constant.

    Output resistance is given byRout =VcIc=0.50.05×10-3        =104 Ω =10

    Question 1257
    CBSEENPH12040219

    A student can distinctly see the object upto a distance 15 cm. He wants to see the blackboard at a distance of 3m. Focal length and power of lens used respectively will be

    • -4.8cm, -3.3D

    • -5.8cm, -4.3D

    • -7.5cm, -6.3D

    • -15.8cm, -6.33D

    Solution

    D.

    -15.8cm, -6.33D

    The rays emanating from a point actually meet at another point after reflection and/or refraction. That point is called the image of the first point. The image is real if the rays actually converge to the point, it is virtual if the rays do not actually meet but appear to diverge from the point from the point when produces backwards.

    The student should use a lens which forms image at a distance of 15 cm of the object placed at 3m i.e object distance u= -3 m =-3000 cm, image distance v =-15 cm

    From lens formula1v-1u=1fwe get         1-15-1-300=1f1f=1300-115=-19300f=-30019=-15.8 cmNow power of the lens isP=100fcm=100-015.8=-6.33 D

    Question 1258
    CBSEENPH12040220

    A thin glass prism (μ =15) in the position of minimum deviation deviates the monochromatic light ray by 10o, the refracting angle of prism is

    • 20o

    • 10o

    • 30o

    • 45o

    Solution

    A.

    20o

    When a narrow beam of sunlight, is incident on a glass prism the emergent light is seen to be consisting of several colours. There is actually a continuous  variation of colour, but broadly in seven colours (acronym VIBGYOR)

    The phenomenon of splitting of light into different colours known as dispersion.  

    Given :- δm =10o ,μ= 15For a thin prism of minimum deviationδm =μ-1A or A=100.5=20o

    Question 1259
    CBSEENPH12040221

    Two thin lenses of powers 12 D and-2D respectively are placed in contact, the power, focal length and nature
    respectively will be

    • 8D, 0.8m, convex

    • 14D, 0.5m, convex

    • 5D, 0.2m, convex

    • 10D, 0.1m, convex

    Solution

    D.

    10D, 0.1m, convex

    Given:- P1=12D, P2=-2DPower of combinationP=P1+P2=12-2=10DFocal length f=1P=110m=0.1mThe combined lens will  be convex (convergent)

    Convex lens refers to the lens which merges the light at a particular point, that travels through it.

    Question 1260
    CBSEENPH12047771

    Interference was observed in an interference chamber when air was present. Now, the chamber is evacuated and if the same light is used, a careful observation will show

    • no interference

    • interference with bright band

    • interference with dark bands

    • interference in which breadth of the fringe will be slightly increased 

    Solution

    D.

    interference in which breadth of the fringe will be slightly increased 

    When chamber is evacuated, the refractive index (µ) decreases. Therefore, wavelength λ  1μ increases.

     Now, fringe width is given by 

                         β  = λDd

                       β ∝  λ 
    Therefore, as wavelength increases, the fringe width will increase.

    Question 1261
    CBSEENPH12047790

    Two coherent light beams of intensities I and 4I are superposed. The maximum and minimum possible intensities in the resulting beam are

    • 5I and I

    • 5 I and 3 I

    • 9 I and I

    • 9 I and 3 I

    Solution

    C.

    9 I and I

    Given:   I1 = I, I2 = 4I

             Imax = I1 + I22

                   = I + 4I 2 

             Imax = 3 I2

              Imax  = 9I       

              Imax = I1 - I2 2

             Imin= I1 - 4I2

                   = - I 2

              Imin =  I

    Question 1262
    CBSEENPH12047838

    The tip of a needle does not give a sharp image on a screen. This is due to

    • polarisation

    • interference

    • diffraction

    • None of these

    Solution

    C.

    diffraction

    As the size of tip of the needle is very small ( because its a point ) and it comes under the range of wavelength of light, so the ray coming from back side of needle ( i.e consider needle's tip just blocking a ray of light) will bend across the tip.

    And hence on screen, that ray will also give brightness near so formed image of needle's tip, hence reducing the original sharpness of the needle's tip.

    The tip of a needle does not give a sharp image, it is due to diffraction.

    Question 1263
    CBSEENPH12047852

    Two coherent light beams of intensities I and 41 are superposed. The maximum and minimum possible  intensities in the resulting beam are

    • 5I and I

    • 5I and 3I

    • 9I and I

    • 9I and 3I

    Solution

    C.

    9I and I

    Given:- I1 = I, I2 = 4I

    Resultant intensity = I1 + I2 2 I1I2 cosδ

    where δ is the phase difference between two waves.

    intensity will be maximum when δ = 0          ....(cos 0o = 1)

                Imax4 I + I + 2 4 I × I cos (0)

                        = 4 I + I + 2 4I2

                        = 4I + I + 2 ( 2I)

               Imax = 9I

    Intensity will be minimum when δ = 0

    and    Imin4I  + I + 24I ×I cos 180   

                    = 4I + I + 2 (2I) (-1)A                  .....(cos 180o = -1)

             Imin = I

    Question 1264
    CBSEENPH12047874

    If prism angle α = 1o , μ= 1.54, distance between screen and prism (D) = 0. 7 m, distance between prism and source α = 0.3 m , λ = 180 π nm, then in Fresnal biprism find the value of β (fringe width).

    • 10-4 m

    • 10-3 mm

    • 10-4 × πm

    • π × 10-3 m

    Solution

    B.

    10-3 mm

    a = 0.3 

    α = 1o

    μ = 1.54

    We know that

       d = 2a ( μ - 1 )

          = 2 × 0.3 ( 1.54 - 1 ) × 1

          = 2 × 0.3 × 0.54 

       d = 0.324

     Fringe width F = D λd

                           = 0.7 × 180 π × 10-90.324

                           = 7 × 180π × 10-6324

                        F = 10-3 mm

    Question 1265
    CBSEENPH12047924

    The magnification produced by a astronomical telescope for normal adjustment is 10 and the length of the telescope is 1.1 m. The magnification, when the image is formed atleast distance of distinct vision is

    • 6

    • 18

    • 16

    • 14

    Solution

    D.

    14

    Given:-

     m = 10, length of telescope= 1.1 m

    We know that,

     Magnification   m = f0fe

          10 = f0fe

           f0 = 10 fe

    ∴     fe + f0 = 1.1 m

    ⇒    fe + 10 fe = 1.1 mm                ....[ f0 = 10fe ]

    ⇒   fe ( 1 + 10 ) = 1.1 m

    ⇒   fe = 0.1 m or 10 cm

    Magnification least distance of distinct vision,

          Mbf0fe1+ feD

                = 10 1 + 1025                   .....[ since D = 25 cm ]

                 = 10 × 3525

           Mb = 14

    Question 1266
    CBSEENPH12047953

    Two slits are separated by a distance of 0.5 mm and illuminated with light of wavelength λ = 6000 Ao. If the screen is placed at 2.5 m from the slits. The distance of the third bright fringe from the centre will be

    • 1.5 mm

    • 3 mm

    • 6 mm

    • 9 mm

    Solution

    D.

    9 mm

    Distance of  nth  bright fringe from the centre,

               xnn D λd

    where n = 0, ± 1,±2,.....

    The third bright fringe width from the centre,

               x3 = 3 × 2.5 × 6000 × 10-100.5 × 10-3

                     = 9 × 10-3 m

               x3 = 9 mm

    Question 1267
    CBSEENPH12047963

    Assertion:  A ray of light is incident from outside on a glass sphere surrounded by air. This ray may suffer total internal reflection at second interface.

    Reason:  If a ray of light goes from denser to rarer medium, it bends away from the normal.

    • If both assertion and reason are true and reason is the correct explanation of assertion.

    • If both assertion and reason are true but reason is not the correct explanation of assertion.

    • If assertion is true but reason is false.

    • If both assertion and reason are false.

    Solution

    B.

    If both assertion and reason are true but reason is not the correct explanation of assertion.

    When a ray of light enters a spherical glass sphere,  it is first refracted at first interface and then it strike the inner surface of sphere (second interface) and get totally internally reflected if the angle between the refracted ray and normal to the drop surface is greater than the critical angle (42°, in this case). 

    Question 1269
    CBSEENPH12047969

    In a Fraunhofer diffraction at single slit of width  d  with incident light of wavelength 5500 Ao,  the first minimum is observed, at angle 30°. The first secondary maximum is observed at an angle θ = 

    • sin-1 12

    • sin-114

    • sin-134

    • sin-132

    Solution

    C.

    sin-134

    Slit width = d

        λ = 5500 Ao

        Ao = 5.5 × 10-7 m

       θn = 30o

    For first secondary minima

       d sin θ= λ

           d = λsin θn

    ⇒    d = 5.5 × 10-7sin 30o

    ⇒    d = 11 × 10-7 m

    For first secondary maxima

           d sin θ3 λ2

    ⇒     sinθn3 λ2 d

                    = 3 × 5.5 × 10-72 × 11 × 10-7

    ⇒      sinθ34

    ⇒         θ= sin-1 (3/4 )

    Question 1270
    CBSEENPH12047980

    The intensity ratio of the maxima and minima in an interference pattern produced by two coherent sources of light is 9 : 1. The intensities of the used light sources are in ratio

    • 3 : 1

    • 4 : 1

    • 9 : 1

    • 10 : 1

    Solution

    B.

    4 : 1

    Given:- The intensity ratio interference pattern produced by two coherent sources of light 9:1.    

               ImaxImin = a+ b2a - b2

                       91 =  a + b 2 a - b 2

                       31 = a + ba - b

    ⇒     3 ( a - b ) = a + b

    ⇒     3a - 3b = a + b

    ⇒               2a = 4b

    ⇒                  a = 2b

    ∴                 I1I2 = a2b2

    ∴                   I1I2 = 41

    Question 1271
    CBSEENPH12047985

    The two coherent sources with intensity ratio β produce interference. The fringe visibility will be

    • 2 β1 + β

    • 2 β

    • 21 + β

    • β1 + β

    Solution

    A.

    2 β1 + β

                I1I2 = a2b2 = β

    ∴            ab= β

    Imax = ( a + b )2   and   Imin = ( a - b )2

    Fringe visibility is given by

         V = Imax - IminImax + Imin 

            = a + b2 - a - ba + b2 + a - b 

         V =  4ab2 a2 + b2

         V =  2  aba2b2 + 1

        V = 2 ββ + 1

    Question 1272
    CBSEENPH12047990

    Assertion: In YDSE bright and dark fringe are equally spaced.

    Reason: It only depends upon phase difference.

    • If both assertion and reason are true and reason is the correct explanation of assertion.

    • If both assertion and reason are true but reason is not the correct explanation of assertion.

    • If assertion is true but reason is false.

    • If both assertion and reason are false.

    Solution

    C.

    If assertion is true but reason is false.

    Fringe width is given by

                         β = D λd

    where, D= distance between slits and screen,

    d = distance between coherent sources of light 

    and A = wavelength of incident light.

    The assertion is true but reason is false. Young's Double-slit Experiment depends on distance between slits and screen (D), the wavelength of light used (λ),  distance between the two slits (d).

    Question 1273
    CBSEENPH12048015

    In a certain double slit experimental arrangement, interference fringes of width 1 mm each are observed when light of wavelength 5000 Ao  is used. Keeping the setup unaltered, if the source is replaced by another of wavelength 6000 Ao, the fringe width will be

    • 1.2 mm

    • 0.5 mm

    • 1 mm

    • 1.5 mm

    Solution

    A.

    1.2 mm

    Fringe width

             β = λ Dd

    Since, D and d are unaltered  β ∝ λ

    ∴       β'β = λ'λ

              β' = β ×  λ'λ 

                   = 1 ×  60001600

    ⇒        β = 1.2 mm

    Question 1275
    CBSEENPH12048035

    Assertion:  A secondary rainbow have inverted colours than the primary rainbow. 

    Reason:  The secondary rainbow is formed by single total internal reflection.

    • If both assertion and reason are true and reason is the correct explanation of assertion.

    • If both assertion and reason are true but reason is not the correct explanation of assertion.

    • If assertion is true but reason is false.

    • If both assertion and reason are false.

    Solution

    C.

    If assertion is true but reason is false.

    In the formation of secondary rainbow, light suffers two total internal reflections instead of one. In this, ray undergoes two internal partial reflections having a maximum deviation of about  50°  for red and  54°  for violet. Also secondary rainbow will sometimes be formed with inverted colours. Secondary rainbow is fainter than the primary for two reason

    (i) the light has undergone two internal reflections and has thereby becomes weakened,

    (ii) there is greater angular dispersion in this rainbow than in the primary.

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