Show that the potential due to a conducting disk of radius \(a\) and charge \(q\) is \begin{equation} \phi(r,z) = \frac{q}{4\pi\epsilon_0 a}\int_0^\infty e^{-k|z|} J_0(kr) \frac{\sin ka }{k}\, dk \end{equation}
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4934: EM-HOME, 4727: Diamond Point
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