Linear frictional forces cause orbits to neither circularize nor precess

Physics – Classical Physics

Scientific paper

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16 pages. 1 figure, Rewrite for resubmission

Scientific paper

10.1088/1751-8113/41/23/235205

For the undamped Kepler potential the lack of precession has historically been understood in terms of the Runge-Lenz symmetry. For the damped Kepler problem this result may be understood in terms of the generalization of Poisson structure to damped systems suggested recently by Tarasov[1]. In this generalized algebraic structure the orbit-averaged Runge-Lenz vector remains a constant in the linearly damped Kepler problem to leading order in the damping coe

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