Step 1: Understand Laplace's equation
Laplace’s equation is a special case of Poisson’s equation:
\[
\nabla^2 V = -\frac{\rho}{\varepsilon}
\]
Where:
- \( V \) is the electric potential,
- \( \rho \) is the charge density,
- \( \varepsilon \) is the permittivity. Step 2: Conditions for Laplace's equation
When \( \rho = 0 \) (no free charges in the region), then Poisson’s equation reduces to Laplace’s equation:
\[
\nabla^2 V = 0
\]
This condition is often found in:
- Electrostatics in vacuum or homogeneous media without charges
- Solving for potential in a charge-free region
\[
\boxed{\nabla^2 V = 0}
\]