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- Today: Ch. 10: The
Deaths of Stars
- Go over exam Friday
- EC Articles.
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- IC 3568 from the
Hubble Space Telescope
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- M2-9 (from the Hubble Space Telescope)
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- Can move mass between stars
- 1st (massive) star becomes red giant
- Its envelope transferred to other star
- Hot (white dwarf) core exposed
- 2nd star becomes red giant
- Its envelope transferred to white dwarf
- Accretion disk around white dwarf
- Angular momentum doesn’t let material fall directly to white
dwarf surface
- Recurrent nova explosions
- White dwarf hot enough for fusion, but no Hydrogen fuel
- New fuel comes in from companion
- Occasionally ignites explosively,
blowing away
remaining fuel
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- Imagine compressing a star slightly (without removing energy)
- Pressure goes up (trying to make star expand)
- Gravity also goes up (trying to make star collapse)
- Does pressure go up faster than gravity?
- If Yes: star is stable
– it bounces back to original size
- If No: star is
unstable – gravity makes it collapses
- Ordinary gas: P does go up fast – stable
- Non-relativistic degenerate gas: P does go up fast
– stable
- Relativistic degenerate gas: P does not go up fast – unstable
- Relativistic: Mean
are the electrons moving at close to the speed of light
- Non-relativistic degenerate gas: increasing r means not only more
electrons, but faster electrons, which raises pressure a lot.
- Relativistic degenerate gas:
increasing r
can’t increase electron velocity (they are already going close to
speed of light) so pressure doesn’t go up as much
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- Add mass to an existing white dwarf
- Pressure (P) must increase to balance stronger gravity
- For degenerate matter, P depends only on density (r), not temperature, so must have higher density
- P vs. r rule such
that higher mass star must actually have smaller radius to provide
enough P
- As Mstar ® 1.4 MSun velectron
® c
- Requires much higher r to provide high enough P, so star must be much
smaller.
- Strong gravity which goes with higher r makes this a losing game.
- For M ³ 1.4
MSun no increase in r can provide enough increase in P – star
collapses
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- Stars less massive than 1.4 MSun can end as white dwarfs
- Stars more massive than 1.4 MSun can end as white dwarfs, if
they lose enough of their mass (during PN stage) that they end up with
less than 1.4 MSun
- Stars whose degenerate cores grow more massive than 1.4 MSun
will undergo a catastrophic core collapse:
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- When the degenerate core of a star exceeds 1.4 MSun it
collapses
- Type II: Massive star where
it runs out of fuel after converting core to Fe
- Type I: White dwarf in binary, which
receives mass from its companion.
- Events:
- Star’s core begins to collapse
- Huge amounts of gravitational energy liberated
- Extreme densities allows weak force to convert matter to neutrons
p+ + e- ® n +
n
- Neutrinos (n) escape, carrying away much of energy, aiding
collapse
- Collapsing outer part is heated, “bounces” off core, is
ejected into space
- Light from very hot ejected matter makes supernova very bright
- Ejected matter contains heavy elements from fusion and neutron capture
- Core collapses into either:
- Neutron stars or Black Holes (Chapter 11)
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- Supernova 1994D in NGC 4526
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- Now seen by the Chandra X-ray Observatory as an expanding cloud.
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- Can see expansion between 1973 and 2001
- Kitt Peak National Observatory Images
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- Neutron star (more in next chapter)
- Quantum rules also resist neutron packing
- Densities much higher than white dwarfs allowed
- R ~ 5 km
r ~ 1014
gm/cm3
(similar to nucleus)
- M limit uncertain, ~2 or
~3 MSun before it collapses
- Spins very fast (by conservation of angular momentum)
- Trapped spinning magnetic field makes it:
- Act like a “lighthouse” beaming out E-M radiation (radio,
light)
- Accelerates nearby charged particles
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- Red: Ha
- Blue:
“Synchrotron” emission from high speed electrons
trapped in magnetic field
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