Three circular orbits at

PHYSICS · Multi-part · Fermi University Physics · Computational Physics · Mechanics & Dynamical Systems · Simulating classical dynamical systems

Computational Physics, Ch An orbit that must not drift

Problem

Three circular orbits at a=1.00a = 1.00, 3.003.00 and 9.00 AU9.00\,\mathrm{AU} are integrated by velocity Verlet at Δt=10−3 yr\Delta t = 10^{-3}\,\mathrm{yr} in units where GM⊙=4π2 AU3 yr−2GM_\odot = 4\pi^2\,\mathrm{AU^3\,yr^{-2}}, and their periods are measured from the trajectories as T=1.000013T = 1.000013, 5.1961555.196155 and 27.000000 yr27.000000\,\mathrm{yr}. ((a)) For each of the three pairs of orbits form the exponent p=ln⁡(Tj/Ti)/ln⁡(aj/ai)p = \ln(T_j/T_i)/\ln(a_j/a_i), and quote the exponent as a mean with an uncertainty taken from the spread of the three. ((b)) Recover GM⊙GM_\odot from each orbit separately as 4π24\pi^2 times a3/T2a^3/T^2, say which orbit gives the value furthest from 4π24\pi^2, and explain why that one is the worst at a step that is the same for all three. ((c)) A fourth body moves on an orbit of a=2.00 AUa = 2.00\,\mathrm{AU} and eccentricity e=0.20e = 0.20. Using Kepler's equation and two Newton steps from E0=ME_0 = M, find its position (x,y)(x,y) a quarter of a period after perihelion.

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