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Black Holes

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Title: A Brief History of Planetary Science Author: Lee Carkner Description: Lee Carkner's standard AS311 power point template Last modified by: Carkner, Lee – PowerPoint PPT presentation

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Title: Black Holes


1
Black Holes
  • Astronomy 315
  • Professor Lee Carkner
  • Lecture 16

2
Relativity
  • Relativity asks the question
  • How do physical phenomena depend on the
    observers 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.

3
Special Relativity
  • Two postulates
  • The speed of light is the same for everyone
  • c 3X108 m/s
  • This is the fastest anything can travel

4
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
5
Moving Clock
  • Someone standing outside the train would see the
    mirror and detector moving
  • Since the moving laser beam has farther to travel
    (d gt d0)
  • so the time seen outside the train is
  • Compared to a clock at rest
  • t0 2d0/c
  • t gt t0

d
6
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

7
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!

8
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

9
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

10
Graviatational Red Shift
  • The ball slows down and loses energy
  • The frequency of light changes as it moves near a
    mass

11
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

12
Black Hole
  • Mass
  • Size singularity
  • Density
  • Supported by unsupported
  • Progenitor
  • Example high mass X-ray binaries

13
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

14
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

15
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 (c3X108 m/s), the light
    cannot escape and the object is a black hole
  • If light cant escape, nothing can
  • Light is gravitationally red shifted to zero

16
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

17
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

18
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

19
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

20
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

21
Deneb
Vega
Cygnus X-1
Altair
22
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

23
Next Time
  • Read Chapter 23.1-23.7
  • Observing List 2 due Monday
  • Test 2 on Wednesday
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