Spherical coordinate for Poisson and Laplace equation

Mathematics

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Here are Poisson's and Laplace's equations in spherical coordinates:

The Laplacian operator ∇2\nabla^2 in spherical coordinates (r,θ,ϕ)(r, \theta, \phi) is given by:

∇2V=1r2∂∂r(r2∂V∂r)+1r2sin⁡θ∂∂θ(sin⁡θ∂V∂θ)+1r2sin⁡2θ∂2V∂ϕ2\nabla^2 V = \frac{1}{r^2} \frac{\partial}{\partial r} \left( r^2 \frac{\partial V}{\partial r} \right) + \frac{1}{r^2 \sin \theta} \frac{\partial}{\partial \theta} \left( \sin \theta \frac{\partial V}{\partial \theta} \right) + \frac{1}{r^2 \sin^2 \theta} \frac{\partial^2 V}{\partial \phi^2}
  1. Poisson's Equation in Spherical Coordinates

    Poisson's equation is ∇2V=−ρϵ0\nabla^2 V = -\frac{\rho}{\epsilon_0}, where VV is the electric potential, ρ\rho is the volume charge density, and ϵ0\epsilon_0 is the permittivity of free space.

    1r2∂∂r(r2∂V∂r)+1r2sin⁡θ∂∂θ(sin⁡θ∂V∂θ)+1r2sin⁡2θ∂2V∂ϕ2=−ρϵ0\boxed{\frac{1}{r^2} \frac{\partial}{\partial r} \left( r^2 \frac{\partial V}{\partial r} \right) + \frac{1}{r^2 \sin \theta} \frac{\partial}{\partial \theta} \left( \sin \theta \frac{\partial V}{\partial \theta} \right) + \frac{1}{r^2 \sin^2 \theta} \frac{\partial^2 V}{\partial \phi^2} = -\frac{\rho}{\epsilon_0}}
  2. Laplace's Equation in Spherical Coordinates

    Laplace's equation is ∇2V=0\nabla^2 V = 0, which is a special case of Poisson's equation where the charge density ρ=0\rho = 0.

    1r2∂∂r(r2∂V∂r)+1r2sin⁡θ∂∂θ(sin⁡θ∂V∂θ)+1r2sin⁡2θ∂2V∂ϕ2=0\boxed{\frac{1}{r^2} \frac{\partial}{\partial r} \left( r^2 \frac{\partial V}{\partial r} \right) + \frac{1}{r^2 \sin \theta} \frac{\partial}{\partial \theta} \left( \sin \theta \frac{\partial V}{\partial \theta} \right) + \frac{1}{r^2 \sin^2 \theta} \frac{\partial^2 V}{\partial \phi^2} = 0}
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