Answer:
Option D
Explanation:
Let emf of each source be E . When they are connected in series , the current in the circuit
$I= \frac{E_{tot}}{R_{tot}}=\frac{E+E}{r_{1}+r_{2}+R}=\frac{2E}{r_{1}+r_{2}+R}$
potential drop across the cell of internal
resistance $r_{2},\left(\frac{2E}{r_{1}+r_{2}+R}\right)r_{2}$
Hence, $E=\frac{2E}{(r_{1}+r_{2}+R)}.r_{2}=0$
$r_{1}+r_{2}+R=2r_{2}$
$\Rightarrow$ $R=r_{2}-r_{1}$