A copper rod ab of length l pivoted at one end a
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Explanation:
A copper rod ab of length l pivoted at one end a rotates at a constant angular velocity w at right angles to a uniform magnetic field of induction b the emf developed between the mid point c of the rod and end b.
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Answered by
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Motional EMF induced in a conductor of length L moving in magnetic field is given by equation
EMF = vBL
now lets take a small part of length "dx" which is at distance"x" from the hinge point
the speed of the point is given by
v = x\omega
now the motional emf in that small part of the rod will be
EMF =_{x=L/2}^{x=L}\int vBdx
EMF = _{x=L/2}^{x=L}\int x\omega Bdx
EMF = \frac{(L^2 - (L/2)^2)}{2} \omega B
EMF = \frac{3B \omega L^2}{8}
so above is the induced EMF frm centre of rod to end of rod
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