When a $J$-shaped conducting rod is rotating in its own plane with constant angular velocity $\omega$,about one of its ends $P$,in a uniform magnetic field $\vec B$ (directed normally into the plane of the paper),then the magnitude of the emf induced across it will be:

  • A
    $B\omega\sqrt{L^2 + l^2}$
  • B
    $\frac{1}{2}B\omega L^2$
  • C
    $\frac{1}{2}B\omega(L^2 + l^2)$
  • D
    $\frac{1}{2}B\omega l^2$

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