$A$ conducting rod of length $2l$ is rotating with constant angular speed $\omega$ about its perpendicular bisector. $A$ uniform magnetic field $\vec{B}$ exists parallel to the axis of rotation. The $e.m.f.$ induced between two ends of the rod is

  • A
    $B\omega l^2$
  • B
    $\frac{1}{2}B\omega l^2$
  • C
    $\frac{1}{8}B\omega l^2$
  • D
    Zero

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