A conducting loop of finite resistance lies on the x-y plane. There is a constant magnetic field in the z direction. The area of the loop varies with time t, as A = A0(1 + t) in appropriate units. The figure that correctly indicates the qualitative behaviour of the power P dissipated in the loop as a function of time is:
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Answer
(3) [figure]
Solution
Magnetic flux through the loop is = B A = B A0 (1 + t).
Induced emf in the loop:
E = - d dt = -B A0 t
Power dissipated in the loop of resistance R:
P = E2R = B2 A02R 2 t = P0 2 t
At t = 0, P(0) = P0 (maximum value).
At t = 2, P = 0.
At t = , P = P0.
This periodic 2 t behaviour starting at a maximum at t = 0 is correctly shown in graph (3).
Answer: (3)