(d) When a ring moves in a magnetic field in a direction perpendicular to its plane, we replace the ring by a diameter (2r) perpendicular to the direction of motion. The emf is induced across this diameter. Current flow in the ring will be through the two semicircular portions in parallel.
Induced emf = $B\ (2\ r)v.$
Resistance of each half of ring = R /2
As the two halves are in parallel, therefore, equivalent resistance = R /4
$\therefore\ \ $ Current in the section $= \ \frac{B(2r)v}{R/4}$
$I = \frac{8Brv}{R}$