A conducting square loop of side ℓ and resistance R moves in its plane with a uniform velocity v perpendicular to one of its sides. A uniform and constant magnetic field B exists along the perpendicular to the plane of the loop, as shown in the figure. The current induced in the loop is
if we draw the equivalent circuit, it will be look like
The formula used: The emf induces across the ends AB and CD is given by
Where E is the emf
V is the velocity
B is the magnetic field
l is the length
Apply KVL in the loop in fig(b).
Here the current I become zero means that there is no current induced in the loop. So the current induced in the loop will be zero.