When a rod of length $l$ is rotated with angular velocity $\omega$ in a uniform magnetic field of induction $B$ perpendicular to the plane of rotation,about one of its ends,the induced emf across its ends is:

  • A
    $B l^{2} \omega$
  • B
    $\frac{B l^{2} \omega}{2}$
  • C
    $Bl\omega$
  • D
    $\frac{B l \omega}{2}$

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