For , the chain rule gives and . Applying it twice to the radial function gives
Using , Laplace's equation becomes
Two integrations now give
These are the general solutions of the specified radial function form on an annulus or a punctured plane. If the solution must extend continuously to the origin, the logarithm term forces , leaving only a constant function.
Use the product rule for the Laplace operator:
Thus Laplace's equation, away from the origin, reduces to . On the line the displayed expression vanishes automatically; requiring the equation on an open region gives the same radial equation by continuity from . Multiplying by gives , so and . Therefore
If extension through the origin is required, : along the horizontal axis the second term is . The remaining harmonic function is .

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