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Q. $A$ 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. Then
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Moving Charges and Magnetism

Solution:

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$A$ to $D$ is part of circle with centre $C$ and radius $CD = r$
$mv=p=BQr$ or $r=\frac{P}{BQ}$
$sin\, \theta = \frac{ED}{CD}=\frac{d}{r}$
$=\frac{BQd}{P}$