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Poisson's and Laplace's equations
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Differential equations for potential.
∇²V = −ρ/ε₀∇²V = −ρ/ε₀ (Poisson) relates potential to charge density; with ρ = 0 it is Laplace's equation. Solutions are unique given boundary conditions.
Used in numerical field calculations.
Potential has no local maxima in empty space.
In more detail
Poisson's equation relates the electric potential to the charge density, ∇²V = −ρ/ε0. Laplace's equation is the special case with no charge, ∇²V = 0.
Real-world uses
- Solving electrostatic problems numerically in engineering software.
- Modelling electric fields in semiconductors and plasmas.
- Engineers use Poisson's equation to compute the potential in complicated geometries such as semiconductor devices.
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Frequently asked questions
Why are these equations important?
They determine the potential everywhere given boundary conditions.
When is Laplace's equation used?
In regions without charge, such as between electrodes.
What do the two equations mean?
Poisson's equation relates the potential to the charge density, and Laplace's equation is the special case with no charge.
Related topics in Electrostatics
Motion of charge in uniform field · Cathode ray tube · Method of images · Multipole expansion · Boundary conditions at interfaces · Electrostatic energy of a sphere