A probe orbits a moon of gravitational parameter at circular radius

PHYSICS · Subjective · Fermi University Physics · Mathematical Methods for Physics · Computational Physics · Simulating classical dynamical systems

Computational Physics, Ch An orbit that must not drift

Problem

A probe orbits a moon of gravitational parameter GM=4.90×1012 m3 s−2GM = 4.90\times10^{12}\,\mathrm{m^3\,s^{-2}} at circular radius r=1.0×106 mr = 1.0\times10^{6}\,\mathrm{m}, all given in SI units. Following the strategy used for the Earth's orbit about the Sun, choose a distance unit D=1.0×106 mD = 1.0\times10^{6}\,\mathrm{m} (so r=1.0 Dr = 1.0\,D) and a time unit TuT_u chosen so that GM=4π2 D3 Tu−2GM = 4\pi^2\,D^3\,T_u^{-2} exactly, as was done with the astronomical unit and the year. (a) Find TuT_u in seconds, to three significant figures. (b) Write the four-component system for (x,y,vx,vy)(x,y,v_x,v_y) in the units DD and TuT_u, and give the initial condition, in these units, for a circular orbit at r=1.0 Dr=1.0\,D that closes after exactly one TuT_u. (c) Convert the initial tangential speed found in part 2 back into SI units (m s−1^{-1}).

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