$A$ line charge ($\lambda$ per unit length) is in the form of a circular wheel of radius $a$ and moment of inertia $I$,initially at rest. It is free to rotate in a horizontal plane. There is a coaxial magnetic field $B = B_0 \hat{k}$ extending up to a radius $b$ $(b < a)$. If the magnetic field is switched off,the angular velocity $\omega$ of the wheel is given by:

  • A
    $\frac{\pi a^2 b \lambda B}{I}$ clockwise as seen from above
  • B
    $\frac{\pi a b^2 \lambda B}{I}$ clockwise as seen from above
  • C
    $\frac{\pi a b^2 \lambda B}{2I}$ anticlockwise as seen from above
  • D
    $\frac{\pi a b^2 \lambda B}{I}$ anticlockwise as seen from above

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