$A$ charge $q$ is spread uniformly over an isolated ring of radius $R$. The ring is rotated about its natural axis with an angular velocity $\omega$. Magnetic dipole moment of the ring is

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

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