A semicircle loop PQ of radius ′R′ is moved with velocity ′v′ in transverse magnetic field as shown in figure. The value of induced emf. at the end of loop is :-
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Solution
Induced emf=−dθdtE=−ddt(BAcosθ)E=−BdAdtcosθ because the ring falls with its vertical plane in horizontal mehnetic induction →B.θ=0andcosθ=1orE=−B.ddt(2Rdx)E=−2RB(dxdt)|E|=2RBV
This is equal to the emf developed in an imaginary rod joining M &Q
According to fleming right hand rule, M is at low potential and Q is at high potential and induced emf is from M to Q.