Transcript Black Holes

Black Holes
Astronomy 315
Professor Lee Carkner
Lecture 16
Relativity

Relativity asks the question:
How do physical phenomena depend on the
observer’s frame of reference?

Most effects are hard to see except at high
speeds or near large masses
n.b. The Theory of Relativity does not mean,
“Everything is relative.”
Special Relativity
Two postulates

The speed of light is the same for everyone

c = 3X108 m/s
This is the fastest anything can travel
Laser Clock

 The beam then bounces back down into a
detector mounted next to the laser on the
floor
 If the distance between the floor and
the ceiling is d0, the time from laser
firing to detection can be found
 velocity = distance /time
t0 = 2d0/v
 This is for a clock at rest
d0
Moving Clock

 Someone standing outside the train
would see the mirror and detector
moving

 Since the moving laser beam has
farther to travel (d > d0)

 so the time seen outside the train is
 Compared to a clock at rest
t0 = 2d0/c
t > t0
d
Time Dilation

Each tick takes longer for the moving clock

Less time passes on the train
Called time dilation

Time dilation is very small unless you are
moving very fast
Twin Paradox
Imagine a pair of twins

One making a round trip to alpha Centauri
on a spaceship traveling 0.99c

Twin on ship would feel 1 year pass
Earth twin is now 5 years older!
General Relativity

Key idea:
Mass and energy are the same thing

This means that light near a large mass
is affected the same way a solid object is
Curved Spacetime

The star would pull
on the ball causing the
path to bend

Spacetime is curved
near a mass
Mass causes light to
bend
Graviatational Red Shift

The ball slows down
and loses energy

The frequency of light
changes as it moves
near a mass
Gravitational Time Dilation
The curved spacetime near a mass affects
light similar to the way our moving train did

More time passes near a mass

If you jump into a black hole, to people watching
you it would take a long time for you to get
anywhere
Black Hole
Mass:
Size: singularity
Density:
Supported by: unsupported
Progenitor:
Example: high mass X-ray binaries
Limits of Neutron Degeneracy

There is no force that can stop the
collapse, so the core contracts to an
infinitely small point called a
singularity

The object is called a black hole
Escape Velocity

Must have the escape velocity
Velocity is related to kinetic energy (KE =
½mv2) , so the object must have more kinetic
energy than the gravitational energy that
holds it back

High mass, small radius means you need a high
velocity to escape
Escaping a Black Hole

Thus, light has to fight gravity to escape from a
mass
If the escape velocity of an object is greater
than the speed of light (c=3X108 m/s), the
light cannot escape and the object is a
black hole
If light can’t escape, nothing can

Light is gravitationally red shifted to zero
Structure of a Black Hole
Once you get closer to a black hole than the event
horizon, you can never get back out

The radius of the event horizon is called the
Schwarzschild radius:
RS = (2GM/c2)

This is the definition of a black hole
Tidal Force

F = GMm/r2

The smaller r is, the greater the force
Imagine you are falling feet first into a black
hole

If the difference is large enough, you will be
pulled apart

Nothing can get to the event horizon intact
X-ray Binary

Material from the normal star gets pulled onto the
compact object
Material falling onto a compact object gets very
hot and produces high energy radiation
Why?

Tidal forces and friction heat the disk

X-ray binary
Finding Black Holes

By getting the Doppler shifts for the
stars we can find the orbital parameters

Even though the black holes are invisible,
they manifest themselves by their strong
gravitational fields
Cygnus X-1

Matches up with a bright O star with an
unseen companion
Mass of companion about 9 Msun

X-ray emission varies rapidly, implying
emitting region is very small

Produces a pair of jets out through the poles
One of the best black hole candidates
Deneb
Vega
Cygnus X-1
Altair
X-ray Binaries
Compact objects in binary systems can exhibit
many properties due to mass transfer from
the normal star to the compact object:
Cataclysimic variable:
X-ray Burster: irregular outbursts of fusion from
hydrogen building up on a neutron star
High mass X-ray Binary:
Next Time
Read Chapter 23.1-23.7
Observing List #2 due Monday
Test 2 on Wednesday