For , define . Differentiate under the integral and use Laplace's equation:
Thus is constant. The top Neumann boundary condition gives , so
For the included endpoint , the integral is interpreted as an improper integral at the bottom corners if necessary. The Fourier series constructed in c gives, on ,
The second series is absolutely and uniformly convergent; the first term has only integrable logarithmic singularities. Its integral is zero since , while every cosine term also has zero integral. This proves the endpoint as well:
For completeness, the logarithmic integral follows without any endpoint differentiation. Put and substitute to obtain . Adding and using gives , hence and the required full-interval result.

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