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Fig. 2

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Simulated frictionless tra jectories. A variety of trajectories simulated from equations (1) and (2) for parameter choices µ = 0, r0 = 30 cm, MA = 0.32 kg, and simulation time t = 9 s. Despite the classical nature of the mass-string problem, simulated trajectories resemble astrophysical orbits with small-orbital-radius revolutions separating apoapsides, n-fold symmetries, and apsidal precession.

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