- Gauss's Law in Electrostatics:
Gauss's law states that the electric flux through a closed surface is proportional to the enclosed electric charge. It is given by:
\[
\Phi_E = \oint \vec{E} \cdot d\vec{A} = \frac{q_{\text{enc}}}{\epsilon_0},
\]
where:
- \( \Phi_E \) is the electric flux,
- \( \vec{E} \) is the electric field,
- \( d\vec{A} \) is the differential area element on the closed surface,
- \( q_{\text{enc}} \) is the total charge enclosed within the surface,
- \( \epsilon_0 \) is the permittivity of free space.
- (A) Electric Field due to a Point Source Charge \( q \):
Consider a spherical Gaussian surface with a radius \( r \) centered at a point charge \( q \). Applying Gauss's law, we get:
\[
E \cdot 4\pi r^2 = \frac{q}{\epsilon_0},
\]
where \( E \) is the electric field at distance \( r \) from the charge. Solving for \( E \), we get:
\[
E = \frac{1}{4\pi\epsilon_0} \cdot \frac{q}{r^2}.
\]
- (B) Deduce Coulomb’s Law:
Using the expression for \( E \), the force on a test charge \( q_0 \) placed in the electric field \( E \) is given by:
\[
F = q_0 \cdot E = q_0 \cdot \frac{1}{4\pi\epsilon_0} \cdot \frac{q}{r^2}.
\]
This is Coulomb’s law, which states that the force between two point charges \( q \) and \( q_0 \) separated by a distance \( r \) is:
\[
F = \frac{1}{4\pi\epsilon_0} \cdot \frac{q \cdot q_0}{r^2}.
\]