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Pulsars

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Title: Pulsars


1
Pulsars
  • A pulsar is a neutron star that beams radiation
    along a magnetic axis that is not aligned with
    the rotation axis

2
Pulsars
  • The radiation beams sweep through space like
    lighthouse beams as the neutron star rotates

3
Why Pulsars must be Neutron Stars
Circumference of NS 2p (radius) 60
km Spin Rate of Fast Pulsars 1000 cycles per
second Surface Rotation Velocity 60,000
km/s 20 speed of light
escape velocity from NS
Anything else would be torn to pieces!
4
What can happen to a neutron star in a close
binary system?
5
Matter falling toward a neutron star forms an
accretion disk, just as in a white-dwarf binary
6
Accreting matter adds angular momentum to a
neutron star, increasing its spin Episodes of
fusion on the surface lead to X-ray bursts
7
A black hole is an object whose gravity is so
powerful that not even light can escape it.
8
Supernovae/Supernova Remnants
  • Massive stars fuse heavier elements, up to Iron
    (Fe)
  • Core is billions of Kelvin and greater than
    Chandrasekhar Limit (1.4 Msun)
  • Rapid collapse to neutron star
  • Rebound of core results in expulsion of outer
    layers ? Supernova Remnant

9
Before/After!
10
Tycho SNR (1572)
11
(No Transcript)
12
Supernova 1987A (light took 170,000 years to get
here!)
13
Black HolesThe Science Behind The Science
Fiction

14
A black hole is an object whose gravity is so
powerful that not even light can escape it.
15
Thought Question
  • What happens to the escape velocity from an
    object if you shrink it?
  • A. It increases
  • B. It decreases
  • C. It stays the same
  • Hint

16
Escape Velocity
Initial Kinetic Energy
Final Gravitational Potential Energy

(escape velocity)2 G x (mass)

2 (radius)
17
Eluding Gravitys Grasp

Escape Velocity
Escape Velocity Speed Needed To Escape An
Objects Gravitational Pull
Mass M Radius R
Earth Vesc 27,000 miles/hour (11 km/s) Sun
Vesc 1.4 million miles/hour (600 km/s)
18
Dark Stars Rev. John Michell (1783)
Pierre-Simon Laplace (1796)
Speed of light ? 1 billion miles/hour (3x105 km/s)
  • What if a star were so small, escape speed gt
    speed of light?
  • A star we couldnt see!

Earth mass R ? 1 inch Solar mass R ? 2
miles
Vesc speed of light ?
19
Surface of a Black Hole
  • The surface of a black hole is the radius at
    which the escape velocity equals the speed of
    light.
  • This spherical surface is known as the event
    horizon.
  • The radius of the event horizon is known as the
    Schwarzschild radius.

20
Neutron star
3 MSun Black Hole
The event horizon of a 3 MSun black hole is also
about as big as a small city
21
No Escape
  • Nothing can escape from within the event horizon
    because nothing can go faster than light.
  • No escape means there is no more contact with
    something that falls in.

22
Mass versus radius for a neutron star
Objects too heavy to be neutron stars collapse to
black holes
23
Neutron Star Limit
  • Neutron pressure can no longer support a neutron
    star against gravity if its mass exceeds about 3
    Msun
  • Some massive star supernovae can make black hole
    if enough mass falls onto core

24
Singularity
  • Beyond the neutron star limit, no known force can
    resist the crush of gravity.
  • As far as we know, gravity crushes all the matter
    into a single point known as a singularity.

25
Singularity
  • The shrunken star too small to be measured but
    with indefinite density

26
If the Sun shrank into a black hole, its gravity
would be different only near the event horizon
Black holes dont suck!
27
Einsteins theory of gravity is built on the
principle that
  1. The speed of light is constant.
  2. As an object speeds up its clock runs faster.
  3. The effects of gravity cannot be distinguished
    from the effects of acceleration.
  4. Motion is a relative state.

28
How about if there is wind?
29
Speed of light is constant
30
Our conceptions of space and time has to be
changed.
  • Facts
  • Regardless of speed or direction, observers
    always measure the speed of light to be the same
    value.
  • Speed of light is maximum possible speed.
  • Consequences
  • The length of an object decreases as its speed
    increases
  • Clocks passing by you run more slowly than do
    clocks at rest (example solar wind particles)

31
Time dilation
32
Special Relativity Length Contraction
33
Equivalence principle
34
Gravitational redshift
35
Gravity deforms space-time
36
Precession of Mercurys orbit
37
Gravity bends the path of light
38
Geodesics in curved spacetime
39

40
Gravity bends the path of light
41
Light waves are stretched out leading to a
gravitational redshift
42
Tidal forces near the event horizon of a 3 MSun
black hole would be lethal to humans Tidal
forces would be gentler near a supermassive black
hole because its radius is much bigger
43
Falling into a black hole
Falling into a black hole gravitational tidal
forces pull spacetime in such a way that time
becomes infinitely long (as viewed by distant
observer). The falling observer sees ordinary
free fall in a finite time.
44
Falling into a black holes
  • With a sufficiently large black hole, a freely
    falling observer would pass right through the
    event horizon in a finite time, would be not feel
    the event horizon.
  • A distant observer watching the freely falling
    observer would never see her fall through the
    event horizon (takes an infinite time).
  • Falling into smaller black hole, the freely
    falling observer would be ripped apart by tidal
    effects.

45
Falling into a black hole
  • Signals sent from the freely falling observer
    would be time dilated and redshifted.
  • Once inside the event horizon, no communication
    with the universe outside the event horizon is
    possible.
  • But incoming signals from external world can
    enter.
  • Time travel and other fairy tales

46
Seeing black holes
47
Seeing black holes
48
How do we know its a BH?
  • Nature is tricky couldnt it be another small
    star like a neutron star or a
    white dwarf?
  • Measure mass of X-ray star by motion of its
    companion (a star like the sun)
  • Mass gt 3 solar
  • masses ? BH!
  • Roughly a dozen BHs found this way (tip of the
    iceberg)

Chandrasekhar
49
Black Hole Verification
  • Need to measure mass
  • Use orbital properties of companion
  • Measure velocity and distance of orbiting gas
  • Its a black hole if its not a star and its mass
    exceeds the neutron star limit (3 MSun)

50
One famous X-ray binary with a likely black hole
is in the constellation Cygnus
51
Gamma-Ray Bursts
  • Brief bursts of gamma-rays coming from space were
    first detected in the 1960s

52
  • Observations in the 1990s showed that many
    gamma-ray bursts were coming from very distant
    galaxies
  • They must be among the most powerful explosions
    in the universecould be the formation of a black
    hole

53
Supernovae and Gamma-Ray Bursts
  • Observations show that at least some gamma-ray
    bursts may be produced by supernova explosions
  • Some others may come from collisions between
    neutron stars

54
Quasars
  • Small, powerful source of energy thought to be
    cores of distant spiral galaxies

55
Quasars and Active Galaxies
  • Active galaxies are galaxies with exceptionally
    bright and compact nuclear regions, called
    Active Galactic Nuclei (AGN).
  • The energy source of AGN is ultimately gravity,
    in the form of accretion of gas onto a
    super- massive black hole, one the most
    efficient engines in the Universe.

56
THE AGN ZOO jet-powered radio lobes
57
What is the energy source of AGN?
The one characteristic that all AGN share is fast
variability, from which astronomers infer the
size of the central engine.
58
A Unified Model for AGN
Are the different classes of AGN truly different
beasts? In the Unified Model for AGN, the
apparent differences are mainly due to
inclination effects. The ingredients are the
hole, the disk, the jet, some orbiting clouds of
gas, plus a dusty torus that surrounds the inner
disk.
59
A Unified Model for AGN
60
A Unified Model for AGN observational
confirmations
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