$A$ particle with charge $-Q$ and mass $m$ enters a magnetic field of magnitude $B$, which exists only to the of the boundary $YZ$. The direction of the motion of the particle is perpendicular to the direction of $B$. Let $T = 2\pi \frac{m}{QB}$. The time spent by the particle in the field will be:

  • A
    $T\theta$
  • B
    $2T\theta$
  • C
    $T \left( \frac{\pi + 2\theta}{2\pi} \right)$
  • D
    $T \left( \frac{\pi - 2\theta}{2\pi} \right)$

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