Question:

A small electric dipole \(\bar{P_0}\), having a moment of inertia I about its center, is kept at a distance r from the center of a spherical shell of radius R. The surface charge density \(\sigma\)is uniformly distributed on the spherical shell. The dipole is initially oriented at a small angle πœƒ as shown in the figure. While staying at a distance r, the dipole is free to rotate about its center.If released from rest, then which of the following statement(s) is(are) correct?
Alternative_text
If released from rest, then which of the following statement(s) is(are) correct?

Updated On: Mar 8, 2025
  • The dipole will undergo small oscillations at any finite value of r > R.
  • The dipole will undergo small oscillations at any finite value of r > R.
  • The dipole will undergo small oscillations with an angular frequency of \(\sqrt\frac{2\sigma p_0}{\epsilon_0I} \ at\ r=2R\)
  • The dipole will undergo small oscillations with an angular frequency of \(\sqrt\frac{6 p_0}{100\epsilon_0I} \ at\ r=10R\)
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The Correct Option is B, D

Solution and Explanation

Electric Field and Torque on the Dipole 

For \( r > R \), the electric field outside the shell is:

\[ E_0 = \frac{\sigma \cdot 4\pi R^2}{4\pi \epsilon_0 r^2} \]

The torque on the dipole is:

\[ \tau = \mathbf{p} \times \mathbf{E} = p_0 E \sin\theta \]

At \( r = 2R \):

\[ \frac{2\sigma p_0}{\epsilon_0 I} \]

At \( r = 25 \):

\[ \frac{\sigma p_0}{100 \epsilon_0 I} \]

Using the Moment of Inertia:

\[ I \alpha = p_0 E \sin\theta \quad \Rightarrow \quad \alpha \approx \frac{p_0 E}{I} \]

Substituting:

The angular frequency is:

\[ \alpha = \frac{p_0 \cdot \sigma \cdot 4\pi R^2}{4\pi \epsilon_0 I r^2} \cdot \theta \] \[ \omega = \frac{p_0 R^2}{\epsilon_0 I r^3} \]

For \( r = 2R \), \( \omega \) does not match the given options. For \( r = 10R \), we get:

\[ \omega = \dots \]

Conclusion:

Thus, Options (2) and (4) are correct.

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