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Laplace's and Poisson's Equations, final discretized version

Inserting in Laplace's equation we obtain ui,j=14[ui,j+1+ui,j1+ui+1,j+ui1,j].

This is our final numerical scheme for solving Laplace's equation. Poisson's equation adds only a minor complication to the above equation since in this case we have uxx+uyy=ρ(x,y), and we need only to add a discretized version of ρ(x) resulting in ui,j=14[ui,j+1+ui,j1+ui+1,j+ui1,j]+h24ρi,j.