Step 1: Understanding the Problem
Two cells with the same emf (\( E \)) but different internal resistances (\( r_1 \) and \( r_2 \)) are connected in series with an external resistance \( R \). We need to find the value of \( R \) such that the potential difference across the second cell is zero.
Step 2: Analyzing the Circuit
The total emf in the circuit is \( 2E \) (since the cells are in series).
The total internal resistance is \( r_1 + r_2 \).
The total resistance in the circuit is \( R + r_1 + r_2 \).
The current (\( I \)) in the circuit is given by:
\[
I = \frac{2E}{R + r_1 + r_2}.
\]
Step 3: Potential Difference Across the Second Cell
The potential difference across the second cell is zero, which means the voltage drop across its internal resistance (\( r_2 \)) equals its emf (\( E \)):
\[
E = I \cdot r_2.
\]
Substitute the expression for \( I \):
\[
E = \frac{2E}{R + r_1 + r_2} \cdot r_2.
\]
Simplify the equation:
\[
1 = \frac{2r_2}{R + r_1 + r_2}.
\]
\[
R + r_1 + r_2 = 2r_2.
\]
\[
R + r_1 = r_2.
\]
\[
R = r_2 - r_1.
\]
Step 4: Matching with the Options
The value of \( R \) is \( r_2 - r_1 \), which corresponds to option (A).
Final Answer: The value of resistance \( R \) is \( r_2 - r_1 \).