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Current Electricity

Question
CBSEENPH12039153

(a) State the working principle of a potentiometer. With the help of the circuit diagram; explain how a potentiometer is used to compare the emf’s of two primary cells. Obtain the required expression used for comparing the emf’s.

(b) Write two possible causes for one sided deflection in a potentiometer experiment.

OR

(a) State Kirchhoff’s rules for an electric network. Using Kirchhoff’s rules, obtain the balance condition in terms of the resistances of four arms of Wheatstone bridge.

(b) In the meter bridge experimental set up, shown in the figure, the null point ’D’ is obtained at a distance of 40 cm from end A of the meter bridge wire. If a resistance of 10W is connected in series with R1, null point is obtained at AD=60 cm. Calculated the values of R1 and R2


Solution

(a) Working Principle of Potentiometer

Principle:
Consider a long resistance wire AB of uniform cross-section. It’s one end A is connected to the positive terminal of battery B1 whose negative terminal is connected to the other end B of the wire through key K and a rheostat (Rh).
The battery B1 connected in circuit is called the driver battery and this circuit is called the primary circuit. By the help of this circuit a definite potential difference is applied across the wire AB; the potential falls continuously along the wire from A to B. The fall of potential per unit length of wire is called the potential gradient. It is denoted by ‘k’.
A cell e is connected such that it’s positive terminal is connected to end A and the negative terminal to a jockey J through the galvanometer G. This circuit is called the secondary circuit. In primary circuit the rheostat (Rh) is so adjusted that the deflection in galvanometer is on one side when jockey is touched on wire at point A and on the other side when jockey is touched on wire at point B.
The jockey is moved and touched to the potentiometer wire and the position is found where galvanometer gives no deflection. Such a point P is called null deflection point. VAB is the potential difference between points A and B and L meter be the length of wire, then the potential gradient is given by, 
                                                 straight k space equals space straight V subscript AB over straight L

If the length of wire AP in the null deflection position be l, then the potential difference

between points A and P,

                                                      VAP = kl

Therefore, Emf of the cell  = VAP= kl

In this way the emf of a cell may be determined by a potentiometer.

Comparison of two emfs’ of a cell:

First of all the ends of potentiometer are connected to a battery B1, key K and rheostat Rh such that the positive terminal of battery B1 is connected to end A of the wire. This completes the primary circuit.

Now the positive terminals of the cells C1 and C2 whose emfs’ are to be compared are connected to A and the negative terminals to the jockey J through a two-way key and a galvanometer (fig). This is the secondary circuit.


Distance if P1 from A is l1.

So, AP1 = l1

Emf of cell C1 is given by, straight epsilon1 = kl1                                                    … (1)

Now, plug is taken from terminals 1 and 3 and inserted between the terminals 2 and 3 to bring cell C2 in the circuit. Null deflection point is obtained at P2.

Distance from P2 to A is l2.

Emf of cell C2, straight epsilon2 = kl2                                                                        … (2)

Now, dividing equation (1) by (2), we get
                                                  straight epsilon subscript 1 over straight epsilon subscript 2 equals straight l subscript 1 over straight l subscript 2
Out of these cells if one is standard cell. 

OR

 

Kirchhoff’s rule states that,

(i) At any junction, the sum of the currents entering the junction is equal to the sum of the currents leaving the junction.

(ii) The algebraic sum of the charges in potential around any closed loop involving resistors and cells in the loop is zero.

Conditions of balance of a Wheatstone bridge:

P, Q, R and S are four resistance forming a closed bridge, called Wheatstone bridge.
                                          

A battery is connected across A and C, while a galvanometer is connected B and D. Current is absent in the galvanometer’s balance point.

Derivation of Formula: Let the current given by battery in the balanced position be I. This current on reaching point A is divided into two parts I1 and I2. At the balanced point, current is zero.

Applying Kirchhoff’s I law at point A,

I - I1 - I 2 = 0 or

 I = I1 + I 2                                                              ...(i)

 

Applying Kirchhoff’s II law to closed mesh ABDA,

- I1P + I 2R = 0 or

  I1P = I 2 R                                                            ...(ii)

Applying Kirchhoff’s II law to mesh BCDB,

- I1Q + I 2S = 0 or

 I1Q = I 2S                                                              ...(iii)


Dviding equation (ii) by (iii), we get, 

                                          fraction numerator straight I subscript 1 straight P over denominator straight I subscript 1 straight Q end fraction equals space fraction numerator straight I subscript 2 straight R over denominator straight I subscript 2 straight S end fraction

rightwards double arrow space space straight P divided by straight Q equals space space straight R divided by straight S space ; which is the required condition of balance for Wheatstone bridge.
b) 

             

For space null space point space at space straight D comma space balance space length space straight l subscript 1 space equals space 40 space cm space

So comma space straight R subscript 1 over straight R subscript 2 equals AD over DC equals fraction numerator 40 over denominator left parenthesis 100 minus 40 right parenthesis end fraction equals 2 over 3 space space space space space space space space space space space space space space... space left parenthesis 1 right parenthesis

If space resistance space 10 space straight capital omega space is space connected space in space series space of space straight R 1 comma
space balance space point space shifts space towards space ‘ straight y ’ space straight i. straight e. comma space AD space equals space 60 space cm

fraction numerator straight R subscript 1 plus 10 over denominator straight R subscript 2 end fraction equals fraction numerator AD straight apostrophe over denominator straight D straight apostrophe straight C end fraction equals fraction numerator 60 over denominator 100 minus 60 end fraction equals 3 over 2 space space space space space space space space space space space space space space space... space left parenthesis 2 right parenthesis

space space space space space space space fraction numerator space straight R subscript 1 over denominator space straight R subscript 2 end fraction plus 10 over straight R subscript 2 equals 3 over 2

From space equations space left parenthesis 1 right parenthesis space and space left parenthesis 2 right parenthesis comma space we space have

2 over 3 plus 10 over straight R subscript 2 equals 3 over 2

rightwards double arrow 10 over straight R subscript 2 equals straight space 3 over 2 minus 2 over 3 equals straight space fraction numerator 9 minus 4 over denominator 6 end fraction equals 5 over 6

rightwards double arrow space straight R subscript 2 straight space equals straight space fraction numerator 10 cross times 6 over denominator 5 end fraction equals straight space 12 straight space ohm
From space equation space left parenthesis 1 right parenthesis comma space we space have

straight R subscript 1 over 12 equals 2 over 3

rightwards double arrow straight space straight R subscript 1 straight space equals straight space fraction numerator 12 straight space cross times 2 over denominator 3 end fraction equals straight space 8 straight space ohm

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