4. A conductor of length šæ moves at a steady speed vat right angles to a uniform magnetic fieldĀ
of flux density šµ. Show that the e.m.f. šø across the ends of the conductor is given by theĀ
equation šø = šµšš£.Ā
Consider the area enclosed by the moving rod, rails and resistor. B is perpendicular to this area, and the area is increasing as the rod moves. Thus the magnetic flux enclosed by the rails, rod and resistor is increasing. When flux changes, an EMF is induced according to Faradayās law of induction.
To find the magnitude of EMF induced along the moving rod, we use Faradayās law of induction without the sign:
In this equation, N=1 and the flux Ī¦=BAcosĪø. We have Īø=0Āŗ and cosĪø=1, since B is perpendicular to A. Now ĪĪ¦=Ī(BA)=BĪA, since B is uniform. Note that the area swept out by the rod is ĪA=āx. Entering these quantities into the expression for EMF yields:
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