Solution:
Using the formula for induced e.m.f. in a rotating conductor:
$$e = \frac{1}{2} B \omega L^2 = \frac{1}{2} B (2\pi f) L^2$$
Substituting
$$e = \frac{1}{2} \times (0.4 \times 10^{-4}) \times (4\pi) \times (0.5)^2 = 6.28 \times 10^{-5}\text{ V}$$
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