PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Differential geometry of curved spacetime · Schwarzschild spacetime and the tests of general relativity
The Geometry of Gravity, Ch The Schwarzschild geometry and Birkhoff's theorem
Problem
A white dwarf has mass M=1.02M⊙ and radius R⋆=8000km. Take GM⊙/c2=1.48km.
((a)) In the general static, spherically symmetric ansatz ds2=−e2A(r)c2dt2+e2B(r)dr2+r2dΩ2, name the Killing-vector property that forces (i) A and B to be independent of t, and (ii) the absence of any cross-term dtdr.
((b)) Using the weak-field metric derived from linearised gravity, matched to the Schwarzschild metric at large r, evaluate the Schwarzschild radius rs of this white dwarf in kilometres.
((c)) Independently estimate the fractional frequency shift z of a photon climbing from the white dwarf's surface to a distant observer, using the Newtonian-potential redshift relation z≈GM/(R⋆c2) from the equivalence-principle argument for gravitational redshift, and check that it equals rs/(2R⋆) to the precision quoted.