(b) A moving conductor is equivalent to battery of emf
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = vBl$ (motion emf)
Equivalent circuit
$\ \ \ \ \ \ \ \ \ \ \ I = I_{2} + I_{2}$
Applying Kirchhoff’s law
$I_{1}R + IR - vBl = 0\ \ \ \ \ \ \ \ \ \ \ \ldots(i)$
$I_{2}R + IR - vBl = 0$ …(ii)
Adding Eqs. (i) and (ii), we get
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ 2IR + IR = 2vBl$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ I = \frac{2vBl}{3R}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ I_{1} = I_{2} = \frac{vBl}{3R}$