| \(\mathrm{A.}\) |
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. |