To solve this problem, we need to understand the conditions under which Gauss's law can be applied using the formula:
$\left|\overrightarrow{E}\right|= \frac{q_{enc}}{\epsilon_{0}\left|A\right|}$
Gauss's Law Description:
Gauss's law relates the electric flux passing through a closed surface (Gaussian surface) to the charge enclosed by that surface. Mathematically, it can be stated as:
$\Phi_{E} = \oint \overrightarrow{E} \cdot d\overrightarrow{A} = \frac{q_{enc}}{\epsilon_{0}}$
where $\Phi_{E}$ is the electric flux, $d\overrightarrow{A}$ is an infinitesimal area vector on the surface, and $q_{enc}$ is the charge enclosed.
Conditions for Using the Given Formula:
The formula $\left|\overrightarrow{E}\right|= \frac{q_{enc}}{\epsilon_{0}\left|A\right|}$ assumes that:
- The electric field $|\overrightarrow{E}|$ is constant in magnitude over the Gaussian surface.
- The Gaussian surface is an equipotential surface such that the angle between $d\overrightarrow{A}$ and $|\overrightarrow{E}|$ is zero everywhere, making the dot product constant.
Explanation of Options:
- Option 1: For any choice of Gaussian surface.
This option is incorrect because the formula cannot be generally applied to any Gaussian surface unless $|\overrightarrow{E}|$ is constant on it.
- Option 2: Only when the Gaussian surface is an equipotential surface.
This option is insufficient because, apart from being an equipotential surface, $|\overrightarrow{E}|$ must also be constant.
- Option 3: Only when the Gaussian surface is an equipotential surface and $|\overrightarrow{E}|$ is constant on the surface.
This option is correct as it satisfies both necessary conditions.
- Option 4: Only when $|\overrightarrow{E}| = $ constant on the surface.
This is incorrect as being constant alone does not ensure the surface is equipotential.
Conclusion:
The correct answer is: Only when the Gaussian surface is an equipotential surface and $|\overrightarrow{E}|$ is constant on the surface.