Lecture Chap18 v1
Transcript of Lecture Chap18 v1
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 1/61
Chapter 18
The Bizarre Stellar Graveyard
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 2/61
What Happens At the End?
Very high-mass star
High-mass star
Low-mass star
Black Hole
Neutron Star
White Dwarf
Core evolves into:
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 3/61
18.1 White Dwarfs
Our goals for learning
• What is a white dwarf?
•
What can happen to a white dwarf in a close binary system?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 4/61
What is a white dwarf?
Very high-mass star
High-mass star
Low-mass star
Black Hole
Neutron Star
White Dwarf
Core evolves into:
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 5/61
Off Main Sequence
! Planetary Nebula and White Dwarf
•
Double-shell burning ends with a pulse that ejects the
H and He into spaceas a planetarynebula
•
The core left behind becomes a whitedwarf
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 6/61
White Dwarfs•
White dwarfs are
the remaining cores
of dead stars
• Electron
degeneracy pressure
supports themagainst gravity
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 7/61
White dwarfs
cool off and
grow dimmer with time
No fusion in white dwarf,
but radiation at low level
! losing energy gradually.
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 8/61
Size of a White Dwarf
• White dwarfs with same mass as Sun areabout same size as Earth
• Higher mass white dwarfs are smaller
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 9/61
The White Dwarf Limit• Degeneracy pressure is not strong enough to support a
white dwarf with >1.4 M Sun against its gravity
• A white dwarf cannot be more massive than 1.4 M Sun,the white dwarf limit (or Chandrasekhar limit )
What happens if white dwarf mass exceeds
the white dwarf limit?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 10/61
If nothing happens,
white dwarfs cool off
and grow dimmer
with time, and fade
away forever .
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 11/61
What can happen to a white
dwarf in a close binary system?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 12/61
Binary system
Two stars next to each other – do they somehow interact?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 13/61
Star that started with less
mass gains mass from its
companion
What happens next?
What happens if the lessmassive star is a white
dwarf? – can the mass
exceed the white dwarf
limit (1.4Msun)?
Massive Less Massive
Off mainsequence first,
and becomes
giants
Mass transfer
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 14/61
Accretion Disks
•
Mass falling toward
a white dwarf from
its close binary
companion hassome angular
momentum
•
The matter
therefore orbits the
white dwarf in an
accretion disk
Mass does not get directly onto the secondary star (white dwarf).
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 15/61
Accretion Disk Formation
Star
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 16/61
Accretion Disks
•
Friction between orbiting rings of matter in the disktransfers angular momentum outward and causes the
disk to heat up and glow.
• Material gradually moves inward, and falls onto the star.
Friction: “C” is moving slower than“B”, and drags “B” backward.
! Move angular momentum outward.
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 17/61
Thought Question
What happens to a white dwarf when it accretes enoughmatter to reach the 1.4 M Sun limit?
A. It explodes
B. It collapses into a neutron star
C. It gradually begins fusing carbon in its core
Remember: the question is
What happens if the less massive star is
a white dwarf? – can the mass exceed
the white dwarf limit (1.4Msun)?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 18/61
Two Types of Supernova
Massive star supernova: -- End of Massive Stars
Iron core of massive star reaches
white dwarf limit and collapses into a
neutron star, causing explosion
White dwarf supernova:
Carbon fusion suddenly begins as white
dwarf in close binary system reachesthe white dwarf limit, causing total explosion
Complete explosion of white dwarf, nothing left behind
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 19/61
One way to tell supernova types apart is with a light
curve showing how luminosity changes with time
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 20/61
Supernova Type:
Massive Star or White Dwarf?
• Light curves differ
• Spectra differ (exploding white dwarfs
don’t have hydrogen absorption lines)
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 21/61
White Dwarf Supernova:
Standard Candle•
White Dwarf Supernova always has the
mass of about 1.4 Msun.
•
That means, we know the amount of fuel forexplosion, and therefore, we know the
luminosity.
• If we compare the brightness measured on
Earth with the predicted luminosity, we can
get distance.
Supernova is bright
It is used to measure the expansion rate of the Universe.
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 22/61
What have we learned?
•
What is a white dwarf?
–
A white dwarf is the inert core of a dead star
– Electron degeneracy pressure balances theinward pull of gravity
• What can happen to a white dwarf in aclose binary system?
– Matter from its close binary companion can
fall onto the white dwarf through an accretiondisk
–
Accretion of matter can lead to novae andwhite dwarf supernovae
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 23/61
18.2 Neutron Stars
Our goals for learning
• What is a neutron star?
•
How were neutron stars discovered?
• What can happen to a neutron star in a close binary system?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 24/61
Midterm 2
•
Wednesday, Nov 5 (11:00-11:50) • Place – Simons Center 103 (regular class room)
• Chapters: 14, 15, 16, 17, 18, S4 (textbook & notes)
•
Bring: Student ID, Pencils, & Eraser
• NO MAKEUP:
– Only on the basis of
• Valid medical absence (with written evidence)
•
Jury Duty
• Military service
• Ask help before exam, not after.
–
I cannot help after exam (want to be fair to all students
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 25/61
What is a neutron star?
Very high-mass star
High-mass star
Low-mass star
Black Hole
Neutron Star
White Dwarf
Core evolves into:
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 26/61
A neutron star
is the ball ofneutrons left
behind by a
massive-star
supernova
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 27/61
Electron degeneracy pressuregoes away because electrons
combine with protons, making
neutrons and neutrinos
Neutrons collapse to the center,
forming a neutron star
Super Onion Structure
At the end of high-mass star
Angular momentum must be
conserved, so a neutron star is often
spinning very rapidly.
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 28/61
A neutron star is about the same size as a small city (~ 10km)
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 29/61
How were neutron stars
discovered?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 30/61
Discovery of Neutron Stars
• Using a radio telescope in 1967, Jocelyn Bell noticed
very regular pulses of radio emission coming from asingle part of the sky
•
The pulses were coming from a spinning neutron star
—a pulsar
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 31/61
Pulsar at center
of Crab Nebula pulses 30 times
per second !!
Imagine a star with the
size of Stony Brook is
spinning 30 times per
second.
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 32/61
Series of images observed by the Hubble Space Telescope.
Pulsation
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 33/61
Pulsars
•
A pulsar is a
neutron star that
beams radiation
along a magneticaxis that is not
aligned with the
rotation axis
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 34/61
Pulsars
•
The radiation beams
sweep through
space like
lighthouse beams as
the neutron starrotates
Radiation beam has to be
directed toward us.Otherwise, we cannot see
them.
We have to be lucky to find it.
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 35/61
Why Pulsars must be Neutron Stars
Circumference of NS = 2! (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
If not as compact as (theoretically predicted) neutron star,
it would be torn to pieces!
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 36/61
What have we learned?
•
What is a neutron star?
–
A ball of neutrons left over from a massivestar supernova and supported by neutrondegeneracy pressure
•
How were neutron stars discovered?
– Beams of radiation from a rotating neutronstar sweep through space like lighthouse beams, making them appear to pulse
–
Observations of these pulses were the firstevidence for neutron stars
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 37/61
What have we learned?
•
What can happen to a neutron star in aclose binary system?
– The accretion disk around a neutron star getshot enough to produce X-rays, making thesystem an X-ray binary
– Sudden fusion events periodically occur on athe surface of an accreting neutron star, producing X-ray bursts
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 39/61
What is a black hole?
Very high-mass star
High-mass star
Low-mass star
Black Hole
Neutron Star
White Dwarf
Core evolves into:
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 40/61
A black hole is an object whose gravity is so powerful
that even light cannot escape from it!
What is a black hole?
This is not a science fiction, so it’s not like
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 41/61
What does “no escape” mean?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 42/61
Thought Question
A. It increases
B. It decreases
C. It stays the same
Escape velocity?
What happens to the escapevelocity from the surface of an
object if you shrink it?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 43/61
“Surface” of a Black Hole
•
The “surface” of a black hole is the radius at which
the escape velocity equals the speed of light, not the
surface of the star itself.
• This spherical surface is known as the event horizon .
• The radius of the event horizon is known as the
Schwarzschild radius .
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 44/61
“Surface” of a Black Hole
Schwarzschild radius
event horizon
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 45/61
The event horizon of a 3 M Sun black hole is also about
as big as a small city
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 46/61
Event horizon is
larger for black
holes of larger mass
Larger mass
! Stronger gravity
! More difficult to escape
! Larger radius of event horizon
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 47/61
A black hole’s mass
strongly warps
space and time in
vicinity of event
horizon
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 48/61
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. It increases the black hole
mass, changes the spin or charge, but otherwise
loses its identity.
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 49/61
Neutron Star Limit
• Strong force (force between nucleon) can no
longer support a neutron star against gravity if its
mass exceeds about 3 M sun
•
Some massive star supernovae can make a black
hole if enough mass falls onto core
Remember: The White dwarf limit is 1.4 Msun. Beyond that, theelectron degeneracy pressure is not strong enough to support the white
dwarf against gravity.
Neutron star is supported by “strong force” – force between nucleons
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 50/61
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 .
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 51/61
What would it be like to visit a
black hole?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 52/61
Light waves take extra time to climb out of a deep hole in
spacetime, leading to a gravitational redshift
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 53/61
Remember: Time in Gravity
•
Light pulses travelmore quickly fromfront to back of anaccelerating spaceshipthan in other direction
• Everyone on shipagrees that time runsfaster in front than in
back
• Effects of gravity areexactly equivalent to
those of acceleration
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 54/61
Time passes more slowly near the event horizon
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 55/61
Tidal forces near the
event horizon of a
3 M Sun black holewould be lethal to
humans
Tidal forces would be
gentler near a
supermassive blackhole because its radius
is much bigger
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 56/61
Do black holes really exist?
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 57/61
Black Hole Verification• Need to measure mass
—
Use orbital properties of companion
—
Measure velocity and distance of orbiting gas
•
It’s a black hole if it’s not a star and its mass
exceeds the neutron star limit (~3 M Sun
)
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 58/61
Some X-ray binaries contain compact objects of mass
exceeding 3 M Sun which are likely to be black holes
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 59/61
One famous X-ray binary with a likely black hole is in
the constellation Cygnus
8/10/2019 Lecture Chap18 v1
http://slidepdf.com/reader/full/lecture-chap18-v1 60/61
What have we learned?
•
What is a black hole? –
A black hole is a massive object whose radiusis so small that the escape velocity exceedsthe speed of light
•
What would it be like to visit a black hole?
– You can orbit a black hole like any otherobject of the same mass—black holes don’tsuck!
–
Near the event horizon time slows down andtidal forces are very strong