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A charged ball B hangs from a silk thread $S$ which makes an angle $\theta$ with a large charged conducting sheet $\mathrm{P}$, as show in the figure. The surface charge density $\sigma$ of the sheet is proportional to

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$\tan \theta$
$\tan \theta$

$\tan \theta=\frac{q \sigma}{\left(2 \varepsilon_{\circ}\right) m g}$
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