A navigation satellite moves on an eccentric orbit with perigee radius and apogee radius

PHYSICS · Multi-part · Fermi University Physics · Mechanics & Dynamical Systems · Relativity & Gravitation · The equivalence principle and gravity as geometry

The Geometry of Gravity, Ch Redshift, local inertial frames and the failure of flat spacetime

Problem

A navigation satellite moves on an eccentric orbit with perigee radius rperi=2.60×107 mr_{\rm peri}=2.60\times10^{7}\ \mathrm{m} and apogee radius rapo=2.70×107 mr_{\rm apo}=2.70\times10^{7}\ \mathrm{m}. Take GM⊕=3.986×1014 m3 s−2GM_\oplus=3.986\times10^{14}\ \mathrm{m^3\,s^{-2}}. Along the orbit, the clock's rate against a ground clock is a fixed constant plus −2GM⊕/(rc2)-2GM_\oplus/(rc^2). ((a)) Find the swing in the fractional rate between perigee and apogee. ((b)) Treat the varying part of the rate as a sinusoid in time, with half that swing as its amplitude and a period equal to the orbital period T=2πa3/GM⊕T=2\pi\sqrt{a^3/GM_\oplus}, where a=(rperi+rapo)/2a=(r_{\rm peri}+r_{\rm apo})/2. Find the amplitude of the periodic time offset it produces, in nanoseconds. ((c)) Convert that amplitude into metres of range.

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