An insulating thin rod of length $l$ has a linear charge density $\rho(x) = \rho_0 \frac{x}{l}$ on it. The rod is rotated about an axis passing through the origin $(x = 0)$ and perpendicular to the rod. If the rod makes $n$ rotations per second,then the time-averaged magnetic moment of the rod is:

  • A
    $\pi n \rho_0 l^3$
  • B
    $\frac{\pi}{3} n \rho_0 l^3$
  • C
    $\frac{\pi}{4} n \rho_0 l^3$
  • D
    $n \rho_0 l^3$

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