Question:

A dielectric sphere of radius \( R \) has constant polarization \( \mathbf{P} = P_0 \hat{z} \) so that the field inside the sphere is \( \mathbf{E} = - \frac{P_0}{3 \epsilon_0} \hat{z} \). Then, which of the following is (are) correct?

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For a polarized dielectric sphere, the electric field outside behaves like a dipole field, decaying as \( \frac{1}{r^2} \) at large distances.
Updated On: Nov 18, 2025
  • The bound surface charge density is \( P_0 \cos\theta \).
  • The electric field at a distance \( r \) on the z-axis varies as \( \frac{1}{r^2} \) for \( r \gg R \).
  • The electric potential at a distance \( 2R \) on the z-axis is \( \frac{P_0 R}{12 \epsilon_0} \).
  • The electric field outside is equivalent to that of a dipole at the origin.
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The Correct Option is B

Solution and Explanation

Step 1: Understanding the polarization of the dielectric sphere.
For a dielectric sphere with constant polarization, the field outside the sphere behaves like the field of a dipole. However, at distances large compared to the radius, the electric field falls off as \( \frac{1}{r^2} \), just like the field of a dipole. The surface charge density and potential outside depend on the polarization.
Step 2: Conclusion.
Thus, the correct answer is option (B).
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