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Question: In an experiment to measure the internal resistance of a cell by a potentiometer, it is found that t...

In an experiment to measure the internal resistance of a cell by a potentiometer, it is found that the balance point is at a length of 2m when the cell is shunted by a 5ω\omega resistance and is at a length of 3m when the cell is shunted by a 10ω\omega resistance, the internal resistance of the cell is then
A. 1.5ω\text{A}\text{. }1.5\omega
B. 10ω\text{B}\text{. }10\omega
C. 15ω\text{C}\text{. }15\omega
D. 1ω\text{D}\text{. }1\omega

Explanation

Solution

Hint: The ratio of the potential difference across both the shunt resistances is equal to the ratio of the respective balancing lengths, i.e. V1V2=l1l2\dfrac{{{V}_{1}}}{{{V}_{2}}}=\dfrac{{{l}_{1}}}{{{l}_{2}}}. The potential difference across a shunt resistance R is V=ER(r+R)V=\dfrac{ER}{(r+R)}. Use these formulas to find the internal resistance of the cell.

Formula used:
V=iR

Complete step by step answer:
Let us first understand the working of a potentiometer. To understand better follow the given figure. This given figure is a simple setup of a potentiometer when it is used to measure the internal resistance of the unknown cell.

A potentiometer consists of a long wire of some known resistance and its total length is L (AB). It is connected to a cell and a potential difference is created across the wire.
J is a moveable point to find the balancing length. When there is zero current found in the galvanometer, the circuit is balanced.
When the circuit is balanced, the voltage (V) across the shunt resistance (R) is directly proportional to the balancing length (l) i.e. VlV\propto l.
Therefore, V=kl, where k is a constant.
When the circuit is balanced, V=EirV=E-ir and V=iR, where I is the current in the circuit PQRS and r is the internal resistance of the cell (E).
This implies that E - ir = iR.
E=i(r+R)i=E(r+R)\Rightarrow E=i(r+R)\Rightarrow i=\dfrac{E}{(r+R)}.
Therefore,
V=Eir=E(E(r+R))r\Rightarrow V=E-ir=E-\left( \dfrac{E}{(r+R)} \right)r
V=E(1r(r+R))=ER(r+R)\Rightarrow V=E\left( 1-\dfrac{r}{(r+R)} \right)=\dfrac{ER}{(r+R)}
Let the voltage across the shunted resistance of 5ω\omega be V1{{V}_{1}} and the balancing length be l1{{l}_{1}}.
Therefore, V1=kl1{{V}_{1}}=k{{l}_{1}} …. (i).
And V1=5E(r+5){{V}_{1}}=\dfrac{5E}{(r+5)} …. (ii).
Let the voltage across the shunted resistance of 10ω\omega be V2{{V}_{2}} and the balancing length be l2{{l}_{2}}.
Therefore, V2=kl2{{V}_{2}}=k{{l}_{2}} …. (iii).
And V2=10E(r+10){{V}_{2}}=\dfrac{10E}{(r+10)} ….. (iv).
Divide equations (i) and (iii).
V1V2=l1l2\Rightarrow \dfrac{{{V}_{1}}}{{{V}_{2}}}=\dfrac{{{l}_{1}}}{{{l}_{2}}}.
Here, l1{{l}_{1}}= 2cm and l2{{l}_{2}}= 3cm.
This gives us that
V1V2=23\dfrac{{{V}_{1}}}{{{V}_{2}}}=\dfrac{2}{3}.
Now, divide equations (ii) and (iv).
V1V2=5E(r+5)10E(r+10)=(r+10)2(r+5)\dfrac{{{V}_{1}}}{{{V}_{2}}}=\dfrac{\dfrac{5E}{(r+5)}}{\dfrac{10E}{(r+10)}}=\dfrac{(r+10)}{2(r+5)}
But V1V2=23\dfrac{{{V}_{1}}}{{{V}_{2}}}=\dfrac{2}{3}.
Therefore,
(r+10)2(r+5)=23\dfrac{(r+10)}{2(r+5)}=\dfrac{2}{3}
3(r+10)=4(r+5)\Rightarrow 3(r+10)=4(r+5)
3r+30=4r+20\Rightarrow 3r+30=4r+20
r=10ω\Rightarrow r=10\omega
Hence, the correct option is B.

Note: Note that the emf of the unknown cell must always be less the emf of the main cell. If the emf of the cell that is to be measured is more than the emf of the main cell, then the balancing length will be more than the length of the resistance wire and we will not be able to measure the emf of the cell.