Elsevier Masson, Annals of Physics, 11(323), p. 2654-2661
DOI: 10.1016/j.aop.2008.01.010
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We solve exactly the classical non-relativistic Landau–Lifshitz equations of motion for a charged particle moving in a Coulomb potential, including radiation damping. The general solution involves the Painlevè transcendent of type II. It confirms our physical intuition that a negatively charged classical particle will spiral into the nucleus, supporting the validity of the Landau–Lifshitz equation.