For flux calculations:
\( \frac{q}{2\epsilon_0} \)
\( \frac{q}{6\epsilon_0} \)
\( \frac{q}{12\epsilon_0} \)
\( \frac{q}{3\epsilon_0} \)
To solve this problem, we need to understand the concept of electric flux and how it relates to charges enclosed by surfaces. According to Gauss's law, the total electric flux \(\Phi\) through a closed surface is given by:
\(\Phi = \frac{Q_{\text{enclosed}}}{\epsilon_0}\)
where \(Q_{\text{enclosed}}\) is the total charge enclosed by the surface, and \(\epsilon_0\) is the permittivity of free space.
In this cuboid with dimensions \((2L \times 2L \times L)\), the charge \(q\) is placed at the center of a surface \(S\) of area \(4L^2\). This surface is one of the \(2L \times 2L\) surfaces of the cuboid.
The opposite surface to ‘S’ is another \(2L \times 2L\) surface, which is parallel to ‘S’.
Since the charge is placed at the center of the surface 'S', it will influence the flux distribution through the opposite surface as follows:
So, the flux through the opposite surface to ‘S’ is:
\(\Phi_{\text{opposite to S}} = \frac{1}{3} \times \frac{q}{\epsilon_0} \div 2 = \frac{q}{6\epsilon_0}\)
Hence, the correct answer is \(\frac{q}{6\epsilon_0}\).
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)