A rod ab of lenght l is rotted with ontant anguar velocity w about an ais
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Motional EMF induced in a conductor of length L moving in magnetic field is given by equation
EMF = vBLEMF=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\omegav=xω
now the motional emf in that small part of the rod will be
EMF =_{x=L/2}^{x=L}\int vBdxEMF=
x=L/2
x=L
∫vBdx
EMF = _{x=L/2}^{x=L}\int x\omega BdxEMF=
x=L/2
x=L
∫xωBdx
EMF = \frac{(L^2 - (L/2)^2)}{2} \omega BEMF=
2
(L
2
−(L/2)
2
)
ωB
EMF = \frac{3B \omega L^2}{8}EMF=
8
3BωL
2
so above is the induced EMF frm centre of rod to end of rod
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