A white dwarf has mass and radius

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=1.02 M⊙M = 1.02\,M_\odot and radius R⋆=8000 kmR_\star = 8000\ \mathrm{km}. Take GM⊙/c2=1.48 kmGM_\odot/c^2 = 1.48\ \mathrm{km}. ((a)) In the general static, spherically symmetric ansatz ds2=−e2A(r)c2dt2+e2B(r)dr2+r2dΩ2ds^2 = -e^{2\mathcal{A}(r)}c^2dt^2 + e^{2\mathcal{B}(r)}dr^2 + r^2d\Omega^2, name the Killing-vector property that forces (i) A\mathcal{A} and B\mathcal{B} to be independent of tt, and (ii) the absence of any cross-term dt drdt\,dr. ((b)) Using the weak-field metric derived from linearised gravity, matched to the Schwarzschild metric at large rr, evaluate the Schwarzschild radius rsr_s of this white dwarf in kilometres. ((c)) Independently estimate the fractional frequency shift zz of a photon climbing from the white dwarf's surface to a distant observer, using the Newtonian-potential redshift relation z≈GM/(R⋆c2)z \approx GM/(R_\star c^2) from the equivalence-principle argument for gravitational redshift, and check that it equals rs/(2R⋆)r_s/(2R_\star) to the precision quoted.

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