Shown in the figure is a circular loop of radius r and resistance R. A variable magnetic field of induction B = B0e−t is established inside the coil. If the key (K) is closed, the electrical power developed right after closing the switch is equal to
P=e2R;e=−ddt(BA)=−Addt(Boe−t)=ABoe−t
⇒ P=1R(ABoe−t)2=A2B2oe−2tR
At the time of starting t = 0 so P=A2B2oR
⇒ P=(π r2)2B2oR=B2oπ2 r4R