5. Gravitational Collapse and Black Holes Flashcards
Describe the properties of the interior of a star
The stress energy momentum tensor is not 0 (like it is for a vacuum)
- Approximated as a perfect fluid
- Made of fermions (electrons, protons, neutrons)
What is hydrostatic equilibrium?
When the pressure gradient balances with the gravitational force of attraction
How do stars generate their massive pressure to support it against the gravitational force?
Burn nucler fuel
- Gives a high temperature and a corresponding high pressure
What state is an old star in at the end of its life?
In its quantum ground state
What provides the pressure against the gravitational forces for old stars in their quantum ground state?
The fermions form a degenerate Fermi gas
- Gives a degenerate pressure which opposes gravity
What defines a white dwarf?
When the degeneracy pressure is balanced against the gravitational pressure (equilibrium)
What is a consequence of the equation of state for a white dwarf in relation to the mass of the star?
That more massive stars are more dense
- Fermions are more tightly confined
- Momenta from the uncertainty principle puts them into a relativistic regime
What is the Chandrasekhar limit?
1.44 Mass of the sun
What is a consequence of the Chandrasekhar limit?
Stars more massive than the limit have no known mechanism for supporting themselves against the gravity
- Stars more massive than the limit cannot end up as white dwarfs
What is the mass limit for a neutron star?
2 -> 3 stellar masses
- Heavier stars than this collapse into a black hole
State the two extra parameters in the metric for the Kerr black hole
- mass m = GM/c^2
- spin a = J/Mc
State what happens to the Kerr metric if you set the values of a or m to 0
- a=0 you recover the Schwarz. solution
- m=0 you recover the Minkowski metric in bispherical coordinates
State the symmetry properties of the Kerr metric
- Axissymmetric meaning it is constant under translations of the phi angle
- Not spherically symmetric
- Also stationary (constant under time translations), but not static (not time reversal)
What are the necessary conditions for event horizon to exist, and when is there an extremal black hole?
Only exists when the spin a <= m
- Extremal when a=m
What is the consequence of the Penrose conjecture and the properties of a black hole?
Penrose conjected that all black holes must have event horizons
- This means the spin is always less than or equal to the mass of the black hole implying a limit on the angular momentum of a BH