For a cone, the solid angle subtended at the center is:
\[ \Omega = 2\pi \left( 1 - \cos\theta \right) \]
The flux through each plane surface is:
\[ \varphi = \frac{\Omega}{4\pi \epsilon_0} Q = \frac{Q}{2\epsilon_0} (1 - \cos\theta) \]
Flux through both plane surfaces:
The flux through the curved surface is:
\[ \Phi_{\text{curved}} = \frac{Q}{\epsilon_0} \cos\theta \]
When \( \theta = 30^\circ \):
\[ 2\varphi = \frac{Q}{\epsilon_0} (1 - \cos\theta) \] \[ \Phi = \frac{Q}{\epsilon_0} \cdot \frac{\sqrt{3}}{2} \]
When \( \theta = 60^\circ \):
\[ \Phi' = \frac{Q}{\epsilon_0} \cdot \frac{1}{2} \] \[ \sqrt{n} = \sqrt{3} \quad \Rightarrow \quad n = 3 \]
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)
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: