(b) As both cells are in series, the circuit current
$i = \frac{E + E}{r_{1} + r_{2} + R} = \frac{2E}{r_{1} + r_{2} = R}$
As terminal potential drop across 1st cell is zero, hence
$V_{1} = E - ir_{1} = E - \frac{2E}{(r_{1} + r_{2} + R)}r_{1} = 0$
[image:3_image181.emf]
$\Rightarrow \ E = \frac{2Er_{1}}{(r_{1} + r_{2} + R)}or\ r_{1} + r_{2} + R = 2r_{1} = R = (r_{1} - r_{2})$