$A$ conducting rod of length $L$ rotates with angular speed $\omega$ in a uniform magnetic field of induction $B$ which is perpendicular to its motion. The induced emf developed between the two ends of the rod is

  • A
    $\frac{B L^2 \omega}{4}$
  • B
    $\frac{B L^2 \omega}{2}$
  • C
    $B L^2 \omega$
  • D
    $2 B L^2 \omega$

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