A heavy neutron star has mass and radius

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

Relativity and Gravitation, Ch Escape velocity, the Schwarzschild radius and the idea of a black hole

Problem

A heavy neutron star has mass M=2.0 M⊙M = 2.0\,M_\odot and radius R=11 kmR = 11\ \mathrm{km}. Treat it as spherically symmetric and non-rotating, and suppose a clock on its surface emits light of a known frequency which is received very far away, effectively at infinity. ((a)) Estimate the Schwarzschild radius rs=2GM/c2r_s = 2GM/c^{2} of this star, in km. ((b)) Estimate its compactness parameter GM/Rc2GM/Rc^{2}. ((c)) Estimate the redshift of the received light in two ways: with the first-order formula z≈ΔΦ/c2z \approx \Delta\Phi/c^{2} of Chapter 9, where ΔΦ=Φrec−Φem\Delta\Phi = \Phi_{\rm rec} - \Phi_{\rm em}, and with the exact factor quoted in this chapter from the full theory of gravity, 1+z=(1−2GM/Rc2)−1/21 + z = (1 - 2GM/Rc^{2})^{-1/2}. ((d)) By what fraction of the exact value does the first-order estimate fall short? Hence decide whether the first-order formula may be used for this star. Use G=6.674×10−11 N m2 kg−2G = 6.674 \times 10^{-11}\ \mathrm{N\,m^2\,kg^{-2}}, c=2.998×108 m s−1c = 2.998 \times 10^{8}\ \mathrm{m\,s^{-1}} and M⊙=1.989×1030 kgM_\odot = 1.989 \times 10^{30}\ \mathrm{kg}.

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