Gauss’s law states that the electric flux (\( \Phi \)) through a closed surface is proportional to the enclosed charge (\( q \)) and inversely proportional to the permittivity of free space (\( \varepsilon_0 \)):
\[ \Phi = \frac{q}{\varepsilon_0}. \]
The charge (\( q \)) on a capacitor is related to its capacitance (\( C \)) and the potential difference (\( V \)) across it by the formula:
\[ q = C \cdot V. \]
Substitute \( q = C \cdot V \) into Gauss’s law:
\[ \Phi = \frac{q}{\varepsilon_0} = \frac{C \cdot V}{\varepsilon_0}. \]
The flux of the electric field through the closed surface is:
\[ \Phi = \frac{C \cdot V}{\varepsilon_0}. \]
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)
A metallic sphere of radius \( R \) carrying a charge \( q \) is kept at a certain distance from another metallic sphere of radius \( R_4 \) carrying a charge \( Q \). What is the electric flux at any point inside the metallic sphere of radius \( R \) due to the sphere of radius \( R_4 \)?
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: