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 magnetic induction `B`, constant in time and space, pointing perpendicular and into the plane of the loop exists everywhere.
The current induced in the loop is

A conducting square loop of side L and resistance R moves in its plane with a unifrom velocity v perpendicular to one of its sides. A magnetic induction B constant in time and space, pointing perpendicular and into the plane of the loop exists every where. the current induced in the loop is

A conduting square loop of side L and resistnce R moves in its plane with a uniform velocity v perpendicular to one of its sides. A magnitude induction B constant in time and space, pointing perpendicular and into to plane at the loop exists every with half the loop outside the field, as shown in figure. The induced emf is

A conducting square loop of side L and resistance R moves in its to one of tis sides. A magnetic induction B , constant in time and space, pointing perpendicular to and into the plane of the loop exists every where. The current induced in the loop is

A conducting square loop of side l and resistance R moves in its plane with a uniform velocity v perpendicular ot one of its sides. A uniform and constant magnetic field B exists along the perpendicualr ot the plane of the loop as shown in . The current induced in the loop is (##HCV_VOL2_C38_E01_025_Q01##)

A conducting square loop of side l and resistance R moves in its plane with a uniform velocity v perpendicular ot one of its sides. A uniform and constant magnetic field B exists along the perpendicualr ot the plane of the loop as shown in . The current induced in the loop is