Step 1: Case 1 – Cells connected in series
In series, the total emf = \( 5E \)
Total internal resistance = \( 5r \)
Using Ohm’s law, the total current through the external resistance \( R \) is:
\( I_s = \frac{5E}{R + 5r} \)
Step 2: Case 2 – Cells connected in parallel
In parallel, the equivalent emf remains \( E \) (since all have same emf)
The equivalent internal resistance becomes \( \frac{r}{5} \)
So the current through the same external resistance \( R \) is:
\( I_p = \frac{E}{R + \frac{r}{5}} \)
Step 3: Given condition
The current through \( R \) is the same in both cases:
So, \( I_s = I_p \)
\[
\frac{5E}{R + 5r} = \frac{E}{R + \frac{r}{5}}
\]
Step 4: Cancel \( E \) from both sides and cross-multiply
\[
\frac{5}{R + 5r} = \frac{1}{R + \frac{r}{5}}
\]
Cross-multiplying:
\[
5 \left( R + \frac{r}{5} \right) = R + 5r
\]
\[
5R + r = R + 5r
\]
Step 5: Simplify the equation
\[
5R - R = 5r - r \Rightarrow 4R = 4r \Rightarrow R = r
\]
Final Answer:
\( \frac{R}{r} = 1 \)