Question:

A simple pendulum of length \( l \) has a bob of mass \( m \), with a charge \( q \). On it a vertical sheet of charge with surface charge density \( \sigma \) passes through the point of suspension. At equilibrium, if the string makes an angle \( \theta \) with the vertical, then

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For any particle under gravity and a constant horizontal force \( F_h \), the angle \( \theta \) of suspension with the vertical at equilibrium always satisfies \( \tan\theta = \frac{F_h}{mg} \). Simply substituting the electric force as \( F_h \) gives the result immediately.
Updated On: May 28, 2026
  • \( \tan\theta = \frac{\sigma q}{2\varepsilon_0 mg} \)
  • \( \tan\theta = \frac{\sigma q}{\varepsilon_0 mg} \)
  • \( \cot\theta = \frac{\sigma q}{2\varepsilon_0 mg} \)
  • \( \cot\theta = \frac{\sigma q}{\varepsilon_0 mg} \)
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The Correct Option is A

Solution and Explanation

Step 1: Understanding the Question:
A simple pendulum with a charged bob is in equilibrium under the influence of gravity and a horizontal electrostatic force produced by an infinite vertical sheet of charge passing through its point of suspension. We need to find the relation for \( \tan\theta \), where \( \theta \) is the angle the string makes with the vertical at equilibrium.

Step 2: Key Formula or Approach:

1. Electric field of a sheet of charge: An infinite plane sheet of charge with surface charge density \( \sigma \) produces a uniform electric field directed perpendicular to the sheet:
\[ E = \frac{\sigma}{2\varepsilon_0} \]
Since the sheet is vertical, the electric field is horizontal.
2. Electrostatic Force: The force on the charge \( q \) is:
\[ F_e = q E = \frac{\sigma q}{2\varepsilon_0} \]
3. Equilibrium of the bob: By resolving the tension \( T \) in the string of the pendulum into horizontal and vertical components:
\[ T \sin\theta = F_e \]
\[ T \cos\theta = mg \]

Step 3: Detailed Explanation:

Dividing the horizontal equilibrium equation by the vertical equilibrium equation:
\[ \frac{T \sin\theta}{T \cos\theta} = \frac{F_e}{mg} \]
\[ \tan\theta = \frac{\left( \frac{\sigma q}{2\varepsilon_0} \right)}{mg} \]
\[ \tan\theta = \frac{\sigma q}{2\varepsilon_0 mg} \]

Step 4: Final Answer:

The equilibrium angle \( \theta \) satisfies \( \tan\theta = \frac{\sigma q}{2\varepsilon_0 mg} \), which corresponds to option (A).
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