To solve this question, we need to understand the relationship between the electric field and electric flux for a capacitor.
When a capacitor of capacitance \(C\) is charged to a potential difference \(V\), the charge on the capacitor is given by the formula:
| \(Q = CV\) |
The electric flux \(\Phi\) through a closed surface is related to the enclosed charge \(Q_{\text{enclosed}}\) and the permittivity of free space \(\epsilon_0\) by Gauss's Law:
| \(\Phi = \frac{Q_{\text{enclosed}}}{\epsilon_0}\) |
In this problem, we are interested in the flux through a closed surface enclosing only the positive plate of the capacitor. The crucial concept here is that the charge on the positive plate of the capacitor is explicit, which is \(+\frac{Q}{2}\) if only half of the total charge \(Q\) is considered (as half equivalently charges each plate).
Hence, the charge enclosed \(Q_{\text{enclosed}}\) by the closed surface around the positive plate is:
| \(+\frac{CV}{2}\) |
Therefore, the flux through the closed surface is:
| \(\Phi = \frac{+\frac{CV}{2}}{\epsilon_0} = \frac{CV}{2\epsilon_0}\) |
This matches the given correct answer \(\frac{CV}{2\epsilon_0}\).
Moreover, let's rule out other options:
Thus, the correct answer is \(\frac{CV}{2\epsilon_0}\).
Two charges of \(5Q\) and \(-2Q\) are situated at the points \((3a, 0)\) and \((-5a, 0)\) respectively. The electric flux through a sphere of radius \(4a\) having its center at the origin is:

A line charge of length \( \frac{a}{2} \) is kept at the center of an edge BC of a cube ABCDEFGH having edge length \( a \). If the density of the line is \( \lambda C \) per unit length, then the total electric flux through all the faces of the cube will be : (Take \( \varepsilon_0 \) as the free space permittivity)