MHT CET · Physics · Electrostatics
A spherical conducting shell of inner radius ' \(r_1\) ' and outer radius ' \(r_2\) ' has a charge ' \(Q\) '. A charge \(-q\) is placed at the center of the shell. The surface charge density on the inner and outer surface of the shell will be

- A \(\frac{\mathrm{q}}{4 \pi \mathrm{r}_1^2}\) and \(\frac{\mathrm{Q}-\mathrm{q}}{4 \pi \mathrm{r}_2^2}\)
- B \(\frac{\mathrm{q}}{4 \pi \mathrm{r}_1^2}\) and \(\frac{\mathrm{Q}}{4 \pi \mathrm{r}_2^2}\)
- C \(\frac{-\mathrm{q}}{4 \pi \mathrm{r}_1^2}\) and \(\frac{\mathrm{Q}+\mathrm{q}}{4 \pi \mathrm{r}_2^2}\)
- D zero and \(\frac{\mathrm{Q}-\mathrm{q}}{4 \pi \mathrm{r}_2^2}\)
Answer & Solution
Correct Answer
(A) \(\frac{\mathrm{q}}{4 \pi \mathrm{r}_1^2}\) and \(\frac{\mathrm{Q}-\mathrm{q}}{4 \pi \mathrm{r}_2^2}\)
Step-by-step Solution
Detailed explanation
Due to charge \(-q\) at the center of the shell, a charge \(q\) will be induced on the inner surface and \(-q\) on the outer surface. The charge on outer surface will become \(Q-q\). Hence surface charge densities will be \(\frac{\mathrm{q}}{4 \pi \mathrm{r}_1^2}\) and \(\frac{\mathrm{Q}-\mathrm{q}}{4 \pi \mathrm{r}_2^2}\)
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