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A solid sphere of radius R with its center at origin has a volume charge density \(\rho = A\sqrt{r}\), where A is a constant. The magnitude of electric field, \(\bar{E}\), at \(r \lt R\), varies with r as ........ .

  • A.\(E \propto r^{-\frac{1}{2}}\)
  • B.\(E \propto r^{\frac{1}{2}}\)
  • C.\(E \propto r^{\frac{3}{2}}\)
  • D.\(E \propto r^{-2}\)

Answer: C

Inside the sphere, \(E \propto r^{3/2}\).

By Gauss's law, the field at radius r depends on the charge enclosed:

\[ \begin{aligned} q(r) &= \int_{0}^{r} A\sqrt{r'}\, 4\pi r'^{2}\, dr' \\ &= \frac{8\pi A}{7} r^{7/2} \\ E &= \frac{q(r)}{4\pi\epsilon_{0}r^{2}} = \frac{2A}{7\epsilon_{0}} r^{3/2} \end{aligned} \]

For a uniform density the same steps give \(E \propto r\); the extra factor \(\sqrt{r}\) in the density raises it to \(r^{3/2}\). \(r^{-2}\) is the law outside the sphere, and \(r^{\pm 1/2}\) would come from forgetting the \(r^{2}\) of the volume element.

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