Paper 4, Section II, D

General Relativity | Part II, 2009

The Schwarzschild metric is given by

ds2=(12Mr)dt2+(12Mr)1dr2+r2(dθ2+sin2θdϕ2)d s^{2}=-\left(1-\frac{2 M}{r}\right) d t^{2}+\left(1-\frac{2 M}{r}\right)^{-1} d r^{2}+r^{2}\left(d \theta^{2}+\sin ^{2} \theta d \phi^{2}\right)

where MM is the mass in gravitational units. By using the radial component of the geodesic equations, or otherwise, show for a particle moving on a geodesic in the equatorial plane θ=π/2\theta=\pi / 2 with rr constant that

(dϕdt)2=Mr3\left(\frac{d \phi}{d t}\right)^{2}=\frac{M}{r^{3}}

Show that such an orbit is stable for r>6Mr>6 M.

An astronaut circles the Earth freely for a long time on a circular orbit of radius RR, while the astronaut's twin remains motionless on Earth, which is assumed to be spherical, with radius R0R_{0}, and non-rotating. Show that, on returning to Earth, the astronaut will be younger than the twin only if 2R<3R02 R<3 R_{0}.

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