Laplace Equation – Cartesian & Cylindrical Coordinates
1. Standard Laplace Equation (Cartesian Coordinates)
The Laplace equation describes steady-state fields such as electric potential, temperature, or fluid flow:
∇²V = 0
In Cartesian coordinates (x, y, z), it is written as:
∂²V/∂x² + ∂²V/∂y² + ∂²V/∂z² = 0
- V → potential function
- ∂²V/∂x², ∂²V/∂y², ∂²V/∂z² → second derivatives in each direction
2. Laplace Equation in Cylindrical Coordinates
Cylindrical coordinates are (r, φ, z), where r = radial distance, φ = azimuthal angle, z = axial coordinate.
∇²V = (1/r) ∂/∂r ( r ∂V/∂r ) + (1/r²) ∂²V/∂φ² + ∂²V/∂z² = 0
3. Special Cases in Cylindrical Coordinates
- Radial only (V depends on r only):
(1/r) d/dr ( r dV/dr ) = 0
- Axial only (V depends on z only):
d²V/dz² = 0
- 2D cylindrical (no z dependence):
(1/r) ∂/∂r ( r ∂V/∂r ) + (1/r²) ∂²V/∂φ² = 0
4. Applications
- Electric potential in Cartesian geometries (plates, boxes)
- Electric potential in cylindrical structures (wires, coaxial cables)
- Temperature distribution in rods and cylinders
- Magnetic field analysis in cylindrical systems
Exam Tip: Cartesian Laplace → ∂²V/∂x² + ∂²V/∂y² + ∂²V/∂z² = 0
Cylindrical Laplace → ∇²V = (1/r) ∂/∂r ( r ∂V/∂r ) + (1/r²) ∂²V/∂φ² + ∂²V/∂z²
Cylindrical Laplace → ∇²V = (1/r) ∂/∂r ( r ∂V/∂r ) + (1/r²) ∂²V/∂φ² + ∂²V/∂z²