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Black Holes

Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

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Page 1: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Black Holes

Page 2: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Underlying principles of General Underlying principles of General RelativityRelativity

The Equivalence Principle

No difference between a steady acceleration and a gravitational field

Page 3: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Gravity and Acceleration cannot be distinguished

Page 4: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

h

V = a h/c

Page 5: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

h Gravitational field

Equivalence principle – this situation should be the same

Page 6: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Principe May 1919

Eddington tests General Relativity and spacetime curvature

GR predicts light-bending of order 1 arcsecond near the limb of the Sun

Page 7: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Lensing of distant galaxies by a foreground cluster

Page 8: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field
Page 9: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

QSO 2237+0305

The Einstein cross

Page 10: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Curved Space: A 2-dimensional analogy

Flat space

Angles of a triangle add up to 180 degrees

Radius r

Circumference of a circle is 2πr

Page 11: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Positive and Negative Curvature

Triangle angles >180 degrees

Circle circumference < 2πr

Triangle angles <180 degrees

Circle circumference > 2πr

Page 12: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

The effects of curvature only become noticeable on scales comparable to the radius of curvature. Locally, space is flat.

Page 13: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

A geodesic – the “shortest possible path”** a body can take between two points in spacetime (with no external forces). Particles with mass follow timelike geodesics. Light follows “null” geodesics.

** This is actually the path that takes the maximum “proper” time.

Space

Time

Spacelike

Timelike

Curved geodesic caused by acceleration OR gravity

Matter tells space(time) how to curve

Spacetime curvature tells matter how to move

Page 14: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Mass (and energy, pressure, momentum) tell spacetime how to curve;

Curved spacetime tells matter how to move

A formidable problem to solve, except in symmetric cases – “chicken and egg”

Page 15: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Curvature of space in spherical symmetry – e.g. around the Sun

Page 16: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

h

V = (2ah)1/2

Special Relativity

A moving clock runs slow

Page 17: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Observer ON TRAIN Observer BY TRACKSIDE

Speed of light is c=300,000 km/s

t’ = 2d / c

Width of carriage

Is d meters

Train speed v

d

vt/2

s

t = 2s / cSo t’ is smaller than t

Observers don’t agree! Smaller by a factor

Where v2/c2)

Page 18: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

h

V = (2ah)1/2

Special Relativity

A moving ruler is shorter

Page 19: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

h

Gravitational field

According to the equivalence principle, this is the same as

Page 20: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Curvature of space in spherical symmetry – e.g. around the Sun

Page 21: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Spacetime curvature near a black hole

Page 22: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

A black hole forms when a mass is squashed inside it’s Schwarzschild Radius RS = 3 (M/Msun) km

Time dilation factor

1/(1 – RS/r)1/2

Becomes infinite when r=RS

Page 23: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field
Page 24: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field
Page 25: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field
Page 26: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Remnant < 1.4 M

Progenitor < 8 M

White Dwarf

Planetary Nebula

A cooling C/O core, supported by quantum mechanics! Electron degeneracy pressure.

The Chandrasekhar limit

Cools forever – gravity loses!

Page 27: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Progenitor > 8 M

Black Hole – gravity wins!

Supernova

Neutron star, supported by quantum mechanics! Neutron degeneracy pressure.

Cools forever – gravity loses!

Remnant < 2.5 M Remnant > 2.5 M

20 km

Page 28: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Black Holes in binary systems

Page 29: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field
Page 30: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

M3 sin3i = 0.25 (M + m)2 Period = 6 days

Cygnus X-1

M > 5 Msun

Page 31: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Ellipsoidal light curve variations

Depend on mass ratio and orbit inclination

Page 32: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

BH mass

Black hole mass 10 –15 x Msun

Combine ellipsoidal model with radial velocity curve

Page 33: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Spinning black holes – the Kerr metric

Page 34: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field
Page 35: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Spaghettification

A 10g stretching force felt at 3700 km (>RS) from a 10 Msun black hole

Force increases as 1/r3

Page 36: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Supermassive Black Holes

Jets propelled by twisted magnetic field lines attached to gas spiralling around a central black hole

Page 37: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Supermassive Black Hole in the Galactic Centre

Mass is 4 millions times that of the Sun

Schwarzschild radius 12 million km = 0.08 au

Page 38: Black Holes. Underlying principles of General Relativity The Equivalence Principle No difference between a steady acceleration and a gravitational field

Falling into a black hole