$A$ circular metal plate of radius $R$ is rotating with a uniform angular velocity $\omega$ with its plane perpendicular to a uniform magnetic field $B$. Then the emf developed between the centre and the rim of the plate is

  • A
    $\pi \omega B R^2$
  • B
    $\omega B R^2$
  • C
    $\frac{\pi \omega B R^2}{2}$
  • D
    $\frac{\omega B R^2}{2}$

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