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Wave Optics

Question
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, 

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