When a metal rod of length L placed normal to a uniform magnetic field B is moved at a velocity of v perpendicular to the field, the induced emf across its ends is |
0 $BLv$ $BL/v$ $(BLv)/2$ |
$BLv$ |
The correct answer is Option (2) → $BLv$ Explanation: When a metal rod of length $ L $ moves with velocity $ v $ perpendicular to a uniform magnetic field $ B $, charges in the rod experience a magnetic force, leading to separation of charges and generation of an emf. Expression for induced emf: $ \varepsilon = B L v $ where $ B $ = magnetic field strength, $ L $ = length of the rod, $ v $ = velocity of the rod. Therefore, the induced emf across its ends is $ \varepsilon = B L v $. |