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Announcements March 31

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Covers Chapters 16-18,S2,S3 (Stellar evolution, neutron stars, black holes) ... annihilate each other if only one manages to survive a trip along the event horizon. ... – PowerPoint PPT presentation

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Title: Announcements March 31


1
AnnouncementsMarch 31
  • Exam III Wednesday, April 5
  • Covers Chapters 16-18,S2,S3 (Stellar evolution,
    neutron stars, black holes)
  • Monday Start Chapter 19 (Milky Way Galaxy)
  • Observing Test
  • If your last name starts with A-L, you must pass
    this test by Thursday April 20.
  • If you name begins with M-Z, by Thursday May 4
    (last Thursday before final exams).
  • Clear sky patrol hours now 9 pm 11 pm if clear
    weather!
  • Can check status at 5pm Clear Sky Status Page
    on website
  • Observing list is on the course website (Obs.
    Project).

2
Black Holes
Black holes form when matter collapses to a point
- a singularity. Nothing not even light can
escape from within the event horizon above a
black hole. The event horizon is one
Schwarzschild radius (RS) from the singularity.
3
As the gravitational field of an object
increases, the curvature of space-time near its
surface increases to the point (for black holes)
where not even light can escape.
4
Light Bending Near a Black Hole
5
Falling Into a Black Hole
  • A probe falling into a black hole
  • would be distorted by the immense
    gravitational forces
  • photons leaving the probe would lose more
    and more energy
  • they would be redshifted to longer
    wavelengths.
  • time on the probe would appear to move
    slower and slower
  • to the observer who sent it in
  • Time becomes infinitely long as probe
    approaches event horizon!

6
Black Holes
are not cosmic vacuum cleaners!
7
Observing Black Holes
We can see accreting black holes in binary star
systems via their X-ray emission.
8
X-ray Exotica
Compact objects give rise to a wide variety of
phenomena, all of which have associated X-ray
emission.
The Black Widow Pulsar
9
X-ray Exotica
Jets from a black-hole binary
10
Summary of Stellar Evolution Death
  • Initial mass lt 0.4 Msun ? He white dwarf
  • Initial mass 0.4-4 Msun
  • ? planetary nebul
  • ? C-O white dwarf
  • Iniital mass 4-8 Msun ? planetary nebula/
  • white dwarf likely
  • Initial Mass 8-25 Msun
  • ? supernova
  • ? neutron star
  • Initial mass gt 25 Msun
  • ? supernova
  • ? black hole

11
If we apply General Relativity to a collapsing
stellar core, we find that it can be sufficiently
dense to trap light in its gravity.
12
Wormholes Fact or Fiction This diagram shows an
Einstein-Rosen bridge where a black hole becomes
a tunnel to a parallel universe.
13
A non-rotating black hole has only a center and
a surface
  • The black hole is surrounded by an event horizon
    which is the sphere for which light cannot escape
  • The distance between the black hole and its event
    horizon is the Schwarzschild radius (RSch
    2GM/c2)
  • The center of the black hole is a point of
    infinite density and zero volume, called a
    singularity

14
Falling into a black hole is an infinite voyage
as 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.
Falling into a black hole revisited What would
it be like?
Note A black hole of Mass M has EXACTLY the same
gravitational force outside the event horizon as
an ordinary object of mass M
15
Myths and Truths about journeys to Black holes
  • 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)
  • Signals sent from the freely falling observer a
    regular intervals (clock ticks) would be
  • Dilated (take a longer time interval as measured
    by distant receiver
  • Redshifted
  • Once inside the event horizon, no communication
    with external world ever possible
  • But incoming signals from external world can
    enter
  • The tidal force near the event horizon
  • A black hole of mas M has exactly the same
    gravitational field as an ordinary mass M at
    large distances

16
Certain binary star systems probably contain
black holes
  • Black holes cannot been seen because they do not
    emit nor reflect light
  • Black holes that are in binary systems might be
    able to be detected
  • As material races toward a black hole, it heats
    and emits X-rays

This star is unrelated (foreground star)
17
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18
Q. A distant observer watches an object falling
directly into a black hole. The object emits
pulses of blue light. What is seen as the object
approaches the event horizon?
  • Object speeds up, emits blue light
  • Object speeds up, emits red light
  • Object slows down, emits blue light
  • Object slows down, emits red light
  • Object travels a constant speed, emits no light

19
Black holes often found in binary systems
X-rays emitted from hot accretion disk around
black hole
20
Black holes in galactic cores has masses between
106 and 109 solar masses!
21
Supermassive black holes at the centers of many
galaxies
22
Black holes evaporate
  • Virtual particles that appear in pairs near an
    event horizon may not be able to mutually
    annihilate each other if only one manages to
    survive a trip along the event horizon.

23
Rotating Black Holes!
Structure of a Kerr (Rotating) Black Hole
24
Q. What is the most common way to detect a
black hole?
  • Redshifted optical emission from jets
  • Radio pulses from rotating searchlight
  • Periodic Gamma ray bursts
  • Observations of matter crashing into event
    horizon
  • X ray emission form accretion disk surrounding
    black hole
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