Example. Laplace equation in polar coordinates $\frac{\partial^2 u}{\partial r^2} + \frac{1}{r}\frac{\partial u}{\partial r} + \frac{1}{r^2}\frac{\partial^2 u}{\partial \theta^2} = 0$ $u = u(r, \theta), 0 < r < 1, 0 < \theta < 2\pi$ $u(1, \theta) = \theta$ Prove that: $u(r, \theta) = 2 - 2 \sum_{n=0}^{\infty} \frac{1}{n}r^n \sin n\theta$
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First, let's assume that the solution to the Laplace equation in polar coordinates is of the form u(r,θ) = R(r)Θ(θ), where R(r) is a function of r only and Θ(θ) is a function of θ only. Show more…
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