A red dwarf of mass and radius has a brown dwarf companion of mass and radius

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Relativistic stars and compact objects · Relativistic stars and compact objects

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

Problem

A red dwarf of mass M=2.446×1029 kgM = 2.446\times10^{29}\ \mathrm{kg} and radius R=1.07×108 mR = 1.07\times10^{8}\ \mathrm{m} has a brown dwarf companion of mass M=1.193×1029 kgM = 1.193\times10^{29}\ \mathrm{kg} and radius R=7.00×107 mR = 7.00\times10^{7}\ \mathrm{m}. Treat both as non-rotating spheres whose external potential is Φ=−GM/r\Phi = -GM/r, zero at infinity, and ignore the field of each on the other. Take G=6.674×10−11 N m2 kg−2G = 6.674\times10^{-11}\ \mathrm{N\,m^2\,kg^{-2}}, c=2.998×108 m s−1c = 2.998\times10^{8}\ \mathrm{m\,s^{-1}} and M⊙=1.989×1030 kgM_\odot = 1.989\times10^{30}\ \mathrm{kg}. ((a)) Compute the compactness parameter GM/Rc2GM/Rc^2 of each star and rank them. ((b)) Compute the escape speed from the surface of the red dwarf. ((c)) Light leaves the red dwarf's photosphere and is received by a distant observer at rest. Give the redshift zz to first order in Φ/c2\Phi/c^2, and estimate the fractional amount by which this falls short of the exact factor 1+z=(1−2GM/Rc2)−1/21 + z = (1 - 2GM/Rc^2)^{-1/2}, quoted in this chapter from the full theory and not derived here. Does the first-order result apply to this star? ((d)) An astronaut of length 1.80 m1.80\ \mathrm{m}, oriented radially, falls freely through the event horizon of a 60 M⊙60\,M_\odot black hole. Compute the tidal stretch (the relative acceleration of head and feet) at the horizon.

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