Step 1: Gauss' Law of Electrostatics.
Gauss' law states that the electric flux \( \Phi_E \) through any closed surface is proportional to the net charge enclosed within that surface. Mathematically, it is given by:
\[
\Phi_E = \oint \vec{E} \cdot d\vec{A} = \frac{Q_{\text{enc}}}{\varepsilon_0}
\]
where:
- \( \vec{E} \) is the electric field,
- \( d\vec{A} \) is the infinitesimal area vector on the closed surface,
- \( Q_{\text{enc}} \) is the total charge enclosed within the surface,
- \( \varepsilon_0 \) is the permittivity of free space.
Step 2: Deriving Coulomb's Law from Gauss' Law.
Consider a point charge \( Q \) at the center of a spherical Gaussian surface of radius \( r \). By symmetry, the electric field \( E \) is radial and uniform over the surface, so the electric flux is:
\[
\Phi_E = E \cdot 4\pi r^2
\]
According to Gauss' law:
\[
\Phi_E = \frac{Q}{\varepsilon_0}
\]
Equating the two expressions for electric flux:
\[
E \cdot 4\pi r^2 = \frac{Q}{\varepsilon_0}
\]
Solving for \( E \):
\[
E = \frac{Q}{4 \pi \varepsilon_0 r^2}
\]
This is the electric field due to a point charge. The force \( F \) on another charge \( q \) due to this electric field is:
\[
F = qE = \frac{1}{4 \pi \varepsilon_0} \frac{Qq}{r^2}
\]
This is Coulomb's law, which gives the electrostatic force between two point charges \( Q \) and \( q \) separated by a distance \( r \).
Step 3: Conclusion.
Gauss' law leads directly to Coulomb's law, which describes the force between two point charges.