$A$ rod of length $l$ is oscillating as a physical pendulum about one of its ends with a small angular amplitude $\alpha$ in a crossed magnetic field $B$. The maximum $emf$ induced in the rod will be:

  • A
    $B\alpha \sqrt {\frac{1}{2}g{l^3}} $
  • B
    $B\alpha \sqrt {\frac{3}{8}g{l^3}} $
  • C
    $B\alpha \sqrt {\frac{1}{3}g{l^3}} $
  • D
    $B\alpha \sqrt {g{l^3}} $

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