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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 magnetic induction B constant in time and space, pointing perpendicular and into the plane at the loop exists everywhere with half the loop outside the field, as shown in figure. The induced emf is 
Held on 30 Apr 2002 · Verified 6 Jul 2026.
zero
RvB
VBL/R
VBL
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