A proposed gyroscope satellite in circular orbit around Jupiter would measure the…

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Schwarzschild spacetime and the tests of general relativity · Schwarzschild spacetime and the tests of general relativity

The Geometry of Gravity, Ch Solar-system tests, the PPN framework and alternative theories

Problem

A proposed gyroscope satellite in circular orbit around Jupiter would measure the geodetic precession of its spin axis. General relativity (γPPN=1\gamma_{\rm PPN}=1) predicts a magnitude ΩGR=200.0 mas yr−1\Omega_{\rm GR}=200.0\ \mathrm{mas\,yr^{-1}} for the proposed orbit. In the PPN framework the same precession is Ω=1+2γPPN3 ΩGR\Omega = \dfrac{1+2\gamma_{\rm PPN}}{3}\,\Omega_{\rm GR}, where ΩGR\Omega_{\rm GR} is defined so that it already contains the factor evaluated at γPPN=1\gamma_{\rm PPN}=1, namely (1+2)/3=1(1+2)/3=1. The mission returns a measured precession Ωmeas=199.5±0.8 mas yr−1\Omega_{\rm meas}=199.5\pm0.8\ \mathrm{mas\,yr^{-1}}. ((a)) Find γPPN−1\gamma_{\rm PPN}-1 and its 1σ1\sigma uncertainty from this result. ((b)) Using twice the 1σ1\sigma uncertainty as the two-standard-deviation bound on ∣γPPN−1∣|\gamma_{\rm PPN}-1|, derive the corresponding lower bound on the Brans-Dicke coupling ωBD\omega_{\rm BD}. ((c)) State whether this bound is stronger or weaker than a Cassini-type time-delay bound of ωBD>4×104\omega_{\rm BD} > 4\times10^4, and explain why in terms of the two experiments' precisions.

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