Question:

A potentiometer circuit has been set up for finding the internal resistance of a given cell. The main battery, used across the potentiometer wire, has an emf of $2.0\, V$ and a negligible internal resistance. The potentiometer wire itself is $4\, m$ long. When the resistance $R$, connected across the given cell, has values of (i) infinity (ii) $9.5\, \Omega $ the balancing lengths on the potentiometer wire are found to be $3 \,m$ and $2.85\, m$, respectively. The value of internal resistance of the cell is

Updated On: Apr 22, 2024
  • $0.25\, \Omega$
  • $0.95\, \Omega$
  • $0.5\, \Omega$
  • $0.75\, \Omega$
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The Correct Option is C

Approach Solution - 1

The internal resistance of the cell is
$r = \bigg(\frac{l_1}{l_2}-1\bigg) R$
Here, $l_1=3\, m,t_2=2.85\, m, R=9.5\, \Omega$
$\therefore \, \, \, \, r = \bigg(\frac{3}{2.85}-1\bigg) (9.5\, \Omega)= \frac{0.15}{2.85} \times 9.5\, \Omega=0.5\, \Omega $
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Approach Solution -2

First, we need to understand the working method of a potentiometer. Let's follow the given figure. This figure is a simple setup of a potentiometer when it is used for measuring the internal resistance of a cell.


A potentiometer has a long wire with a known resistance (R), and its total length is L (AB). It is attached to a cell and a potential difference is generated across the wire.

J is a moveable point for finding the balancing length. When 0 current in the galvanometer, the circuit is balanced.

When the circuit is balanced, the voltage (V) through the resistance (R) is directly proportional to the balancing length (l) i.e. 

V∝l

Therefore, V = kl, where k is a constant.

When the circuit is balanced, 

V=E−ir and V=iR, where i is the current in the circuit PQRS and r is the internal resistance of the cell (E).

It means that E - ir = iR.

⇒E=i(r+R) ⇒ i=E(r+R)

Therefore,

⇒V=E−ir=E−\((\frac{E}{(r+R)})\)r

⇒V=E(1−\(\frac{r}{(r+R)}\))

⇒V=\(\frac{ER}{(r+R)}\)

⇒V=\(\frac{\frac{ER}{R}}{\frac{r+R}{R}}\)

\(\frac{E}{\frac{r}{R}+1}\)

When a resistance of infinity, let the voltage across the resistance be 

V1 and the balancing length be l1

Therefore, V1=kl1 …. (i).

And 

V1=\(\frac{E}{\frac{r}{R}+1}\)

But, if 

R→∞ then 

r/R→0

⇒V1=\(\frac{E}{0+1}\)=E…. (ii).

Let the voltage across the shunted resistance of 9.5Ω be V2 and the balancing length be l2

Therefore, V2=kl2…..(iii).

And 

V2=\(\frac{9.5E}{r+9.5}\) ….. (iv).

Divide equations (i) and (iii).

\(\frac{V_1}{V_2}\) =\(\frac{I_1}{I_2}\)

Here, l1= 3 cm and l2 = 2.85cm.

This gives us that

\(\frac{V_1}{V_2}\)=\(\frac{3}{2.85}\)

Now, divide equations (ii) and (iv).

\(\frac{V_1}{V_2}\)=\(\frac{E}{\frac{9.5E}{r+9.5}}\) =\(\frac{r+9.5}{9.5}\)

But \(\frac{V_1}{V_2}\) =\(\frac{3}{2.85}\)

Therefore,

\(\frac{r+9.5}{9.5}\) = \(\frac{3}{2.85}\)

⇒2.85(r+9.5)=3(9.5)

⇒2.85r+27.075=28.5

⇒r=\(\frac{(28.5-27.075)}{2.85}\) = \(\frac{1.425}{2.85}\) = 0.5Ω

Therefore, the internal resistance of that cell is 0.5Ω

Option (C)  is correct.

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Approach Solution -3

Here,

 The formula for the Internal resistance, r = (\(\frac{E-V}{V}\))R = (\(\frac{I_1 - I_2}{I_2}\))R

=(\(\frac{3-2.85}{2.85}\))(9.5)Ω = 0.5Ω

So, Option (c) is the correct answer.

 

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Concepts Used:

Current Electricity

Current electricity is defined as the flow of electrons from one section of the circuit to another.

Types of Current Electricity

There are two types of current electricity as follows:

Direct Current

The current electricity whose direction remains the same is known as direct current. Direct current is defined by the constant flow of electrons from a region of high electron density to a region of low electron density. DC is used in many household appliances and applications that involve a battery.

Alternating Current

The current electricity that is bidirectional and keeps changing the direction of the charge flow is known as alternating current. The bi-directionality is caused by a sinusoidally varying current and voltage that reverses directions, creating a periodic back-and-forth motion for the current. The electrical outlets at our homes and industries are supplied with alternating current.