A particle with charge $q$, moving with a momentum $p$, enters a uniform magnetic field normally. The magnetic field has magnitude $B$ and is confined to a region of width $d$, where $d < \frac{p}{{Bq}}$, The particle is deflected by an angle $\theta $ in crossing the field
  • A$\sin \theta = \frac{{Bqd}}{p}$
  • B$\sin \,\theta \, = \frac{p}{{Bqd}}$
  • C$\sin \,\theta \, = \frac{{Bp}}{{qd}}$
  • D$\sin \,\theta \, = \frac{{pd}}{{Bq}}$
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