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When a 'J' shaped conducting rod rotating in its own plane with constant angular velocity omega, avout one of its end P, in a uniform magnetic field vec(B) directed normally into the plane of paper) then magnetic of emf induced across it will be |
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Answer» `Bomegasqrt(L^(2)+l^(2))` `e=1/2Bomega(l^(2)+L^(2))`
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