拉普拉斯方程的球坐标系解法\[\begin{cases}\frac{1}{r^2}\frac{\partial}{\partialr}\left(r^2\frac{\partialu}{\partialr}\right)+\frac{1}{r^2\sin\theta}\frac{\partial}{\partial\theta}\left(\sin\theta\frac{\partialu}{\partial\theta}\right)=0,