Two particles each of mass $m$ and charge $q$ are attached to the two ends of a light rigid rod of length $2R$. The rod is rotated at a constant angular speed $\omega$ about a perpendicular axis passing through its centre. The ratio of the magnitudes of the magnetic moment of the system and its angular momentum about the centre of the rod is:

  • A
    $\frac{q}{2m}$
  • B
    $\frac{q}{m}$
  • C
    $\frac{2q}{m}$
  • D
    $\frac{q}{\pi m}$

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