Physically this equation describes how a function diffuses in space. They can be seen everywhere in science and thus also in real life. Some examples include
Poisson's equation for gravity,
Δϕ = 4 π G ρ .
Poisson's equation for electrostatics, which is
Δφ = − ρ ε .
Poisson's equation for pressure field in incompressible fluid flow,
Sarmad, Poisson Equation is applied in Fluid Dynamics for computing pressure field when velocity field is known (e.g. in a numerical iterative algorithm one computes velocity field from Navier-Stokes equations, then it can be computed pressure by Poisson eqn).
Perhaps the more known application of Poisson eqn is the computation of scalar electric potential, known the charges distribution.
Physically this equation describes how a function diffuses in space. They can be seen everywhere in science and thus also in real life. Some examples include
Poisson's equation for gravity,
Δϕ = 4 π G ρ .
Poisson's equation for electrostatics, which is
Δφ = − ρ ε .
Poisson's equation for pressure field in incompressible fluid flow,
My only comment is: his approach with Green's function is too formal! Integration by parts is how I do this in class, to reduce it to the variational formulation.
Any physical model that is second order, frame invariant, Galilean invariant and homogeneous must be a combination of div, grad and curl. The only scalar combination is div grad . Thus NOT getting a Laplacian is the exceptional case.
When we use the Poisson equation, we are within the class of PDE called elliptic equations that governs the equilibrium problems in physics. The answer above provided several example, I can add the case of the stream-function when a vorticity field is known (in 3D you get 3 Poissone equations) but also in the elastic field you can get a system of two Poisson equations (a deforming panel under the action of a normal stress)