Outline
- Stellar Evolution in a Nutshell
- The Smallest Stars: Brown and Red Dwarfs
- Sun-Like Stars
Red Giants, then White Dwarfs
- Stars with M>4 MSun: Main Sequence
Supernova!
- How stellar evolution looks on the H-R Diagram
Terms to Know
brown dwarf
red dwarf
white dwarf
red giant
hydrogen shell burning
helium flash
degenerate matter
planetary nebula
Chandrasekhar limit (1.4 MSun)
neutron star
black hole
supernova
1. Stellar Evolution in a Nutshell
We have seen how stars are born when huge clouds of gas and dust get
nudged by a passing shock wave (from e.g., a nearby supernova)
and collapse under their own gravity. Eventually, the collapse leads
to temperatures and pressures high enough to ignite nuclear fusion in
the core of the protostar. Leftover gas from the cloud either clumps
together to form planets, or else gets blown away by the new star's
intense radiation and stellar wind.
The star soon settles into a stable life converting H to He in its
core, with gravity and pressure balanced by the "thermostat" of
hydrostatic equilibrium. Stars in this long middle-age stage lie on
the main sequence of the Hertzprung-Russell Diagram.
What happens when a star uses up its fuel, i.e., converts
all the hydrogen in its core to helium? It all depends on the mass
of the star:
-
If the mass is much lower than 1 MSun
(red dwarfs), the star could live on the main sequence for hundreds
of billions of years, much longer than the current age of the
Universe! Eventually, it will either blow away its mass (mostly in
the form of helium) or contract and turn into a small, hot, ember: a
white dwarf.
-
If the mass is close to the Sun's
mass, the star will turn into a red
giant, and then blow away much of its atmosphere, becoming a planetary nebula and eventually
turning into a white dwarf. This is the fate of the Sun.
- If the mass is greater than about 4
MSun, the star will explode in a spectacular
catastrophe: a supernova! The
remains are either a tiny neutron star or an even tinier black hole, surrounded by an expanding
shell of gas.
2. The Smallest Stars: Brown and Red Dwarfs
Some protostars don't even quite make it to star-hood: if its mass is less
than about 0.08 MSun, a ball of H and He gas won't have
enough gravity to produce the temperature and pressure necessary for
nuclear fusion. These luke-warm failed stars are called brown dwarfs.
If the star is just massive enough to ignite nuclear fusion in its
core, but not much more, what happens when it uses up its hydrogen?
It will contract and heat up -- but not enough to fuse helium atoms
together -- winding up as a small, hot, glowing helium ember, emitting
thermal radiation and cooling over billions of years: a white
dwarf.
Note that very low-mass stars like red dwarfs are fully
convective: they mix up their insides constantly like boiling
water. Therefore H gets used up throughout the star, not just in the
core.
3. Sun-Like Stars --> Red Giants, then
White Dwarfs
If a star has a mass between about 0.4 MSun and 4
MSun, something different happens when the H runs out in a
star's core:
- Now the star has a core of helium, surrounded by hydrogen too
cool to fuse.
- No fusion? No pressure support! Gravity takes over again, and the core
collapses under the weight of all the gas above it.
- Core heats up as it collapses.
- Eventually, temperature gets high enough to fuse the hydrogen
outside the helium core:
hydrogren shell burning.
- Surge of energy from the H shell
burning makes star's outer parts blow up like a balloon. The star's
atmosphere cools at the same time, producing a red giant. Size can be larger than
Earth's orbit! Their huge surface area makes red giants bright even
though they're not hot.
- Helium core continues to contract until
it becomes
degenerate (electrons are squeezed together as tightly as
possible).
- Degenerate matter heats up without pressure
increasing
- When core T finally reaches 100,000,000 K, helium
can now fuse to form carbon -- there's a new burst of energy, the
helium flash. Star enters
new phase of relative stability (though much shorter than main
sequence) fusing helium into carbon
and oxygen in core.
NOW what happens? After the helium is all used up, that's
it. Core contracts to degenerate state again, while rest of star
blows away in stellar wind, forming a planetary nebula (so
called because early astronomers thought they resembled planets; now
we know they have nothing to do with each other). The Sun will die
this way in about 5-6 billion years.
Note that the maximum mass allowed for white dwarfs is 1.4
MSun; this is the Chandrasekhar limit. If the white
dwarf has more mass than that, it will collapse to a black hole! So stars that begin with more
than 1.4 MSun must lose all but that 1.4 MSun
during their lifetime if they are going to finish up as white dwarfs.
4. Stars with M>4 MSun: Main Sequence --> Supernova!
Really massive stars, like firecrackers, are spectacular but
short-lived, and they too go out in a blaze of glory.
When the hydrogen is used up in the core of a massive star (which
takes only a few million years for a star with
M=20MSun), the star goes through the same stages
(core contraction, hydrogen shell burning, envelope expansion, core
contraction, helium flash) as solar-type stars. But it keeps on
going: the crushing force of gravity is so strong that it can heat up
the core enough to fuse carbon into oxygen, oxygen into neon, followed
by magnesium, silicon, sulfur, and finally iron, in multiple layers like an onion's.
But when the very interior fuses sulfur into iron, it has reached
the end of the line . Further fusion will actually
consume energy, not release it, because iron is the most strongly bound of all the
elements. The iron core is a dead end.
When fusion in the core stops, pressure support disappears, and
gravity takes over once again, crushing the core of the star in
less than a second. This is too fast! The tremendous rush
towards the center of the star results in a rebound, like a
superball thrown against the floor, and most of the star is hurled out
into space in a spectacular explosion, a supernova.
What is left behind?
- a neutron star -- made up of degenerate matter, like a white
dwarf, but so dense that protons and electrons are squeezed together
to form a soup of neutrons. One sugar cube of neutron soup would
weigh 100 million tons.
or
- a black hole. If the remnant
core has more mass than the Chandrasekhar limit (1.4 MSun),
not even degenerate neutrons can stop the crush of gravity, and the
whole core of the star winks out of sight as it collapses into a black hole. Not even light can escape
from a black hole. A black hole
with a mass of 1.4 MSun has a radius of only 4 km. Imagine
a star more massive than our Sun compressed into a ball the size of
the Smith College campus.
What about the material that is blown away by the supernova? It
drifts about between the stars, possibly collecting into clouds that
eventually form new stars later on. This gas consists of lots of
"heavy elements" such as carbon, oxygen, silicon, and iron. This
is where we came from: every atom in your body has been processed
by a massive star!
5. How stellar evolution looks on
the H-R Diagram
Remember: the mass of a star determines almost everything in its
life: its lifetime, luminosity, temperature, eventual composition,
and ultimate fate.
- Stars start life as a dust and gas cloud, collapse, begin
hydrogen fusion, and show up on the H-R Diagram on the main sequence.
- When the H fuel is exhausted, star puffs up and becomes red
giant. Therefore, on H-R Diagram, star leaves main sequence and moves
up and to the right (or, if mass is very low, star turns
directly into white dwarf, left in H-R Diagram, bypassing red
giant phase).
- Star may go through several additional phases (H shell burning,
He flash, etc., depending on mass), which cause star to make small
loops in H-R Diagram.
- Eventually, star explodes in supernova (luminosity way above
ceiling on most H-R Diagrams!) or becomes planetary nebula and then
white dwarf: in H-R Diagram, star moves hotter and bluer (to the
left), then fainter (lower). White dwarfs cool slowly, moving to the
bottom right in the H-R Diagram over time.
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Last updated: Nov. 22, 2004 James D. Lowenthal