| \(\mathrm{A.}\) | Inside a conductor, the electrostatic field is zero. |
| \(\mathrm{B.}\) | The electric field at the surface of a charged conductor does not depend on its surface charge density. |
| \(\mathrm{C.}\) | The interior of a charged conductor can have no excess charge in the static situation. |
| \(\mathrm{D.}\) | At the surface of a charged conductor, the electrostatic field must be normal to the surface at every point. |
| \(\mathrm{E.}\) | The electrostatic potential is zero everywhere inside a charged conductor. |

| 1. | \(E_A \neq 0, E_B < E_C\) | 2. | \(E_A = 0, E_B = E_C\) |
| 3. | \(E_A \neq 0, E_B = E_C\) | 4. | \(E_A = 0, E_B > E_C\) |
| 1. | \(\sqrt{\dfrac{Qq}{4\pi\epsilon_0 mR}}~\) | 2. | \(\sqrt{\dfrac{3Qq}{4\pi\epsilon_0 mR}}~\) |
| 3. | \(\sqrt{\dfrac{2Qq}{3\pi\epsilon_0 mR}}~\) | 4. | \(\sqrt{\dfrac{Qq}{3\pi\epsilon_0 mR}}~\) |


2.
3.
4.
| 1. | \(1.2~\text{J}\) | 2. | \(1.5~\text{J}\) |
| 3. | \(0.8~\text{J}\) | 4. | \(1.0~\text{J}\) |
| 1. | \(1 \times 10^5\) | 2. | \(0.5 \times 10^5\) |
| 3. | \(\text{zero}\) | 4. | \(3 \times 10^5\) |