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GUJCET · Physics · Electric Charges and Fields
The charge density of uniformly charged infinite plane is \(\sigma\). A simple pendulum is suspended vertically downward near it. Charge \(q_0\) is placed on metallic bob. If the angle made by the string is \(\theta\) with vertical direction then _______.
- A \(\sigma \alpha \frac{q_0}{\tan \theta}\)
- B \(\sigma \alpha \frac{\tan \theta}{q_0}\)
- C \(\sigma \alpha \tan \theta\)
- D \(\sigma \alpha \frac{\cot \theta}{q_0}\)
Answer & Solution
Correct Answer
(C) \(\sigma \alpha \tan \theta\)
Step-by-step Solution
Detailed explanation
(C)

From fig.
\(\begin{aligned}
T \sin \theta =q_0 E \\
T \cos \theta =m g \\
\tan \theta =\frac{q_0 E}{m g}\end{aligned}\)
But for uniformly charge infinite plane electric field
\(
\begin{array}{l}
E \quad=\frac{\sigma}{2 \varepsilon_0} \\
\therefore \tan \theta=\frac{q_0}{m g} \frac{\sigma}{2 \varepsilon_0} \\
\therefore \sigma \alpha \tan \theta\left(\because m \text { and } q_0 \text { constant }\right)
\end{array}
\)

From fig.
\(\begin{aligned}
T \sin \theta =q_0 E \\
T \cos \theta =m g \\
\tan \theta =\frac{q_0 E}{m g}\end{aligned}\)
But for uniformly charge infinite plane electric field
\(
\begin{array}{l}
E \quad=\frac{\sigma}{2 \varepsilon_0} \\
\therefore \tan \theta=\frac{q_0}{m g} \frac{\sigma}{2 \varepsilon_0} \\
\therefore \sigma \alpha \tan \theta\left(\because m \text { and } q_0 \text { constant }\right)
\end{array}
\)
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