The Laplace PDE is defined dU/dt)partial=Nabla^2 U solution has two main approaches, i- FDM approach which transforms the Nabla^2 PDE U=b into a set of n linear algebraic equations Au=u to be solved by Gaussian elimination or any other method.

ii-non-mathematical physical statistical approach which assumes that if the solution U=A^-1 b is already known then A^-1 must be subjected to:

A^-1=D , where the matrix D is defined via D=E-I and the matrix E itself is easy to find via ,E=B^0+B+B ^2.....+B^N . Obviously, matrix B is the well-known statistical transition matrix.

This physical solution applies to Poisson PDE and time-dependent heat PDE with arbitrary initial conditions.

Personally I suppose there is a jump somewhere but how?

I appreciate your comments.

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