In Evan's book of Partial Differential Equation, for Laplace's equation it is noted that: "In looking for explicit solutions, it is often wise to restrict attention to classes of functions with certain symmetry properties. Since Laplace's equation is invariant under rotations, it consequently seems advisable to search for radial solutions, that is, functions of $r=|x| = (x_1^2+\dots+x_n^2)^{\frac{1}{2}}$."
This radial solution leads to the fundamental solution of Laplace's equation. I know the mathematical definition of symmetry and radial solution which I found in the Internet where the independent variable is a spatial variable varying over a domain with radial symmetry such as a ball centered at the origin.
My questions are:
- What is the relation of radial solution with the symmetry property?
- Is there any other solution (instead of radial solution), to derive the fundamental solution? Is this also need to be related to symmetry property?
- Should we consider radial solutions for any symmetric differential operator to obtain the fundamental solution?
Thanks in advance.