$A$ proton (mass $m$,charge $q$) accelerated by a potential difference $V$ flies through a uniform transverse magnetic field $B$. The field occupies a region of space of width $d$. If $\alpha$ is the angle of deviation of the proton from the initial direction of motion (see figure),the value of $\sin \alpha$ will be:

  • A
    $qV \sqrt{\frac{Bd}{2m}}$
  • B
    $\frac{B}{2} \sqrt{\frac{qd}{mV}}$
  • C
    $\frac{B}{d} \sqrt{\frac{q}{2mV}}$
  • D
    $Bd \sqrt{\frac{q}{2mV}}$

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