| 1. | \(60\times10^{3}~\text{Vm}^{-1}\) | 2. | \(90\times10^{3}~\text{Vm}^{-1}\) |
| 3. | zero | 4. | infinite |

The electric flux through the surface:

| 1. | in figure-(iv) is the largest |
| 2. | in figure-(iii) is the least |
| 3. | in figure-(ii) is same as figure-(iii) but is smaller than figure-(iv) |
| 4. | is the same for all the figures |
| 1. | \(180\) | 2. | \(150\) |
| 3. | \(170\) | 4. | \(130\) |
The electric field in a region is given \(\vec{E}=\dfrac{4}{5}\hat{j}~\text{N/C}\). The electric flux (in SI units) through the rectangular surface of area \(5~\text{m}^2\) (parallel to \(XZ\)-plane) is:
1. \(1\)
2. \(2\)
3. \(3\)
4. \(4\)
| 1. | \(q / \varepsilon_0\) | 2. | zero |
| 3. | \(-q / \varepsilon_0\) | 4. | \(2q / \varepsilon_0\) |
Given below are two statements:
| Assertion (A): | When an electric dipole is completely enclosed by a closed Gaussian surface, the total electric flux through the surface is zero. |
| Reason (R): | The net charge enclosed within the surface is zero. |
| 1. | Both (A) and (R) are True and (R) is the correct explanation of (A). |
| 2. | Both (A) and (R) are True but (R) is not the correct explanation of (A). |
| 3. | (A) is True but (R) is False. |
| 4. | Both (A) and (R) are False. |
| 1. | \(\oint_{s} \vec{E} \cdot d \vec{s} \neq 0\) on any surface. |
| 2. | \(\oint_{s} \vec{E} \cdot d \vec{s}=0\) if the charge is outside the surface. |
| 3. | \(\oint_{s} \vec{E} \cdot d \vec{s}=\frac{q}{\varepsilon_{0}}\) if charges of magnitude \(q\) were inside the surface. |
| 4. | Both (2) and (3) are correct. |