In a potentiometer experiment it is found that no current passes through the galvanometer when the terminals of the cell are connected across `0.52 m` of the potentiometer wire. If the cell is shunted by a resistance of `5Omega` balance is obtained when the cell connected across` 0.4m` of the wire. Find the internal resistance of the cell.
In a potentiometer experiment it is found that no current passes through the galvanometer when the terminals of the cell are connected across `0.52 m` of the potentiometer wire. If the cell is shunted by a resistance of `5Omega` balance is obtained when the cell connected across` 0.4m` of the wire. Find the internal resistance of the cell.
A
`2.5 Omega`
B
`1 Omega`
C
`1.5 Omega`
D
`2 Omega`
Text Solution
AI Generated Solution
The correct Answer is:
To find the internal resistance of the cell in the potentiometer experiment, we can follow these steps:
### Step 1: Understand the initial condition
In the first scenario, no current passes through the galvanometer when the terminals of the cell are connected across `0.52 m` of the potentiometer wire. This means that the electromotive force (E) of the cell is balanced by the potential drop across the potentiometer wire.
Let:
- \( V \) = potential drop per unit length of the potentiometer wire
- \( L_1 = 0.52 \, m \)
From this, we can write the equation:
\[
E = V \cdot L_1
\]
Substituting \( L_1 \):
\[
E = V \cdot 0.52
\]
### Step 2: Understand the second condition
In the second scenario, the cell is shunted by a resistance of `5Ω`, and balance is obtained when the cell is connected across `0.4 m` of the wire.
Let:
- \( L_2 = 0.4 \, m \)
The current through the circuit when the resistance is connected can be calculated as:
\[
I = \frac{E}{R + r}
\]
where \( R = 5 \, \Omega \) (the shunt resistance) and \( r \) is the internal resistance of the cell.
The potential drop across the shunt resistance can be expressed as:
\[
V \cdot L_2 = I \cdot R
\]
Substituting for \( I \):
\[
V \cdot L_2 = \left(\frac{E}{R + r}\right) \cdot R
\]
Substituting \( L_2 \):
\[
V \cdot 0.4 = \left(\frac{E}{5 + r}\right) \cdot 5
\]
### Step 3: Set up the equations
Now we have two equations:
1. \( E = V \cdot 0.52 \)
2. \( V \cdot 0.4 = \frac{5E}{5 + r} \)
### Step 4: Substitute the first equation into the second
Substituting \( E \) from the first equation into the second:
\[
V \cdot 0.4 = \frac{5(V \cdot 0.52)}{5 + r}
\]
### Step 5: Simplify the equation
Cancelling \( V \) from both sides (assuming \( V \neq 0 \)):
\[
0.4 = \frac{5 \cdot 0.52}{5 + r}
\]
Cross-multiplying gives:
\[
0.4(5 + r) = 5 \cdot 0.52
\]
Expanding the left side:
\[
2 + 0.4r = 2.6
\]
### Step 6: Solve for \( r \)
Rearranging gives:
\[
0.4r = 2.6 - 2
\]
\[
0.4r = 0.6
\]
Dividing both sides by \( 0.4 \):
\[
r = \frac{0.6}{0.4} = 1.5 \, \Omega
\]
### Final Answer
The internal resistance of the cell is \( r = 1.5 \, \Omega \).
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