MATHEMATICAL TRIPOS
Part III
Thursday, 4 June, 2015
9:00 am to 12:00 pm
PAPER 54
BLACKHOLES
Attempt no more than
THREE
questions.
There are
FOUR
questions in total.
The questions carry equal weight.
STATIONERY REQUIREMENTS
SPECIAL REQUIREMENTS
Cover sheet
None
Treasury Tag
Script paper
You may not start to read the questions
printed on the subsequent pages until
instructed to do so by the Invigilator.

21A spacetime containing a static, spherically symmetric, star has line elementds2=-e2Φ(r)dt2+parenleftbigg1-2m(r)rparenrightbigg-1dr2+r2dΩ2.The matter inside the star is described by a perfect fluid with energy momentum tensorTab= (ρ+p)uaub+pgaband barotropic equation of statep=p(ρ) withρ, pgreaterorequalslant0,dp/dρ >0.The Einstein equation reduces to the Tolman-Oppenheimer-Volkov (TOV) equations:dmdr= 4πr2ρdΦdr=m+ 4πr3pr(r-2m)dpdr=-(p+ρ)(m+ 4πr3p)r(r-2m)(a)(i) LetRdenote the radius of the star, sop, ρvanish forr > R. Show that the metricoutside the star is the Schwarzschild metric.(ii) Explain why smooth solutions of the TOV equations form a 1-parameter family,labelled uniquely byρc≡ρ(0).(iii) Assume that the equation of state is known forρlessorequalslantρ0but not forρ > ρ0. Explainwhy there is a maximum possible mass for the star that is independent of the equation ofstate forρ > ρ0.
