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Stellar Evolution

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Title: Stellar Evolution


1
Stellar Evolution
  • We have lots of information about stars, but we
    still need to consider two more areas before we
    begin to put this all together and see if we can
    see some kind of stellar life cycle (also
    called stellar evolution). Those last two areas
    are
  • interstellar material atoms, dust, and nebula
  • and variable stars.

2
Stellar Evolution

The Crab Nebula, M1, as imaged by Hubble Space
Telescope and the Mount Palomar telescope.
3
How do we know what is in interstellar space?
  • Gas and dust in space can
  • scatter light
  • absorb light, heat up, and then re-emit light

4
Scattered Light
  • In scattering light, blue light scatters more
    than red light. This gas and dust will then tend
    to redden starlight that passes through it.
    This effect is seen on the earth the sky is
    blue because the blue light is scattered more
    than the red light but the sunrise and sunsets
    appear red because most of the blue has been
    scattered out of the direct sunlight.

5
Absorb Light
  • Atoms will selectively absorb light of particular
    frequencies called an absorption spectrum.
    They will later re-emit that light, but in
    different directions the emission spectrum.
  • Dust particles will absorb light of most any
    frequency and tend to heat up. They will emit
    blackbody radiation based on their temperature.

6
Nebula
  • This combination of absorption and emission of
    light by gas and dust results in different
    types of nebula (areas of relatively high gas
    and dust) dark nebula and glowing nebula.
  • See web sites
  • http//nssdc.gsfc.nasa.gov/photo_gallery/photogall
    ery-astro-nebula.html
  • http//www.robgendlerastropics.com/Nebulas.html

Image of the youngest known planetary nebula, the
Stingray nebula (Hen-1357).
7
Interstellar Space
  • Liquid water has about 3 x 1022 water molecules
    per cubic centimeter (in English about 30 billion
    trillion). Most solids and liquids have similar
    numbers.
  • At the earths surface our atmosphere has about
    2.4 x 1019 molecules per cubic centimeter (about
    a thousand times less dense than liquid water).
  • In most of interstellar space, there is about 1
    hydrogen atom per cubic centimeter.
  • There are regions of interstellar space, though,
    that have much higher densities. In nebula, that
    number can reach a million atoms per cubic
    centimeter.

8
Variable Stars
  • While most stars appear to be quite stable, at
    least on a human time frame, some stars do show
    variations in brightness. A few show huge
    changes that appear to be catastrophic events.
    Others have brightness changes in a very periodic
    manner, some on the order of seconds, others on
    the order of days.

9
Cepheid Variables
  • One type of star, a Cepheid Variable, has a
    brightness that varies by up to about half a
    magnitude with a period that ranges from 1 to 100
    days.
  • By looking at star clusters where all of its
    stars appear to be about the same distance away,
    we find that the period of the star is related to
    the luminosity of the star! The lower the
    period, the lower the average luminosity.
    Cepheid variables with a period of 1 day have an
    absolute magnitude (luminosity) of about 2. On
    the other end, Cepheid variables with a period of
    100 days have an absolute magnitude of about
    8.

10
Cepheid Variables
  • These are all very luminous stars (giants), and
    can be seen from very far away.
  • What makes this important are the following
    relations. We can always measure brightness. It
    is also easy to measure the period of a Cepheid
    Variable. With the period-luminosity
    relationship, we can then get the luminosity.
    Finally, knowing the brightness and luminosity,
    we can calculate the distance!
  • This distance determination will be an important
    tool in Part 5 of the course where we look at the
    overall size and structure of the universe.

11
Stellar Evolution
  • Lets now try to put all of this info together
    into a theory that will explain our observations
    and lead us to make further observations to
    support, refine, or refute our theory.

12
1. Beginning Gravitational formation
  • Most of space is fairly empty of matter and cold.
    However, there are areas of relatively high gas
    and dust (nebula). Over time, gravity will tend
    to pull the gas and dust together. As it does,
    it will tend to convert the gravitational energy
    into heat energy (the speed of falling is
    converted into heat).

13
1. Beginning Gravitational formation
  • The cloud of gas and dust will tend to get
    smaller and hotter. A smaller size tends to
    reduce the luminosity, but hotter tends to
    increase luminosity. The position of the newly
    forming star on the H-R diagram will move to the
    left as it heats up but wander up and down
    somewhat as its size shrinks.
  • This process takes about 50 million years for a
    star like the sun, but may take a much shorter
    time for a more massive star since there will be
    more gravity. A ten solar mass star will only
    spend about 200,000 years in this initial stage.

14
H-R DiagramGravitational formation
-10

Luminosi ty
-5
1
0
Sun G2 at 4.8 Magnitude
5
10
15
O0
B0
A0
F0
G0
K0
M0
Temperature / Color
15
Nuclear Fusion of HydrogenStability on the Main
Sequence
  • When the temperature and pressure at the core of
    the newly forming star reaches a certain point,
    the hydrogen atoms will collide with one another
    so hard that nuclear fusion will occur (basically
    four hydrogen atoms combine to form one helium
    atom plus LOTS of energy). This hydrogen bomb
    process tends to blow the star apart, but gravity
    continues to try to collapse the star.

16
2. Nuclear Fusion of HydrogenStability on the
Main Sequence
  • The result of these competing tendencies is a
    stable star, both in size and in temperature (and
    hence in position on the H-R diagram on the Main
    Sequence).
  • More massive stars have more fuel, but they also
    have more gravity that causes the core to burn
    the fuel at a faster rate than less massive
    stars. The result is that more massive stars are
    hotter and more luminous and are higher on the
    Main Sequence than less massive stars, and they
    remain stable on the Main Sequence for less time.

17
2. Nuclear Fusion of HydrogenStability on the
Main Sequence
  • A star like the sun will last about 10 billion
    years on the Main Sequence.
  • A star with 15 times the mass of the sun will
    only last about 10 million years on the Main
    Sequence. In the same way, stars with less mass
    then the sun will stay on the main sequence much
    longer than 10 billion years.

18
Red GiantNuclear Fusion of Helium
  • When the hydrogen starts to run out in the core,
    the explosive energy production of nuclear fusion
    no longer can balance the gravitational tendency
    to collapse, and so the core of the star will
    again start to collapse while hydrogen is still
    burning on the outside of the core. This gravity
    collapse of the core will again heat up the core,
    and this extra heat will cause the stars surface
    to expand. As the surface expands, it will tend
    to cool. The result is a red giant state
    higher luminosity but a little cooler surface.

19
3. Red GiantNuclear Fusion of Helium
  • For a star like the sun, this expansion of the
    surface will be large enough to reach the orbit
    of Venus or even the Earth.
  • When the core gets hot enough, it will start to
    have the helium atoms (ashes of the hydrogen
    fusion) combine in nuclear fusion to form carbon
    and release energy.
  • This process takes roughly about 10 of the time
    of the Main Sequence hydrogen burning.

20
H-R DiagramRed Giant
-10

Luminosi ty
-5
3
1
0
Sun G2 at 4.8 Magnitude
5
2
10
15
O0
B0
A0
F0
G0
K0
M0
Temperature / Color
21
4. Unstable stars
  • After the helium fuel in the core runs out, there
    are different scenarios for different masses of
    stars.
  • For a star with about the mass of the sun or
    less, the core will again collapse and the
    gravitational energy of the collapse will eject
    some of the outer layers of the star (called
    planetary nebula ejection) and the core (now at
    about 0.6 of the original mass of the star) will
    heat up (move to the left and tend to move up)
    and shrink (tend to move down).

22
H-R DiagramUnstable
-10
4

eject planetary nebula
Cepheid Variables
Luminosi ty
-5
3
1
0
Sun G2 at 4.8 Magnitude
5
2
10
15
O0
B0
A0
F0
G0
K0
M0
Temperature / Color
23
4. Unstable stars
  • For more massive stars, the situation is more
    complicated. With the higher gravity, the core
    can get hot enough to start burning the carbon to
    get even heavier elements. This proceeds until
    the core turns into iron. Since the nucleus of
    iron is tightest bound of all atoms, iron cannot
    undergo nuclear fusion to release energy like the
    less massive atoms can.

24
4. Unstable stars
  • When the core cannot continue with fusion, there
    is nothing to balance gravity, and the core will
    totally collapse. The implosion of the core will
    release so much energy that it will blow the
    outer parts of the star completely away in a
    supernova explosion.

25
Final Stage Death of the Star
  • There are three possibilities for the collapsed
    core depending on the mass of the remaining core
  • 1) If the final mass after the planetary nebula
    release is less than 1.4 solar masses, the
    remaining mass of the star will collapse down to
    a size about that of the earth. It will be a
    white dwarf star, and then as it cools it will
    become a brown dwarf and then eventually cool
    even further.

26
H-R DiagramFinal Stage Death
-10
4

eject planetary nebula
Cepheid Variables
Luminosi ty
-5
3
1
0
Sun G2 at 4.8 Magnitude
5
2
5
10
White dwarf
15
O0
B0
A0
F0
G0
K0
M0
Temperature / Color
27
Final Stage Death of the Star
  • If the final mass (after the supernova explosion)
    is more than 1.4 solar masses but less than about
    3 solar masses, the core will stop collapsing
    when the atoms are so compacted that the
    electrons are shoved into the protons and the
    whole mass becomes neutrons that stick together
    by gravity. This is called a neutron star. Its
    diameter is only about 20 kilometers (compared to
    about 12,000 kilometers for a white dwarf!).

28
Pulsar
  • 2-continued) If the original star had an
    appreciable magnetic field and a rotation, the
    resulting neutron star may still have that
    magnetic field and it will have a much higher
    rotational speed due to the collapse. The
    magnetic field may cause light to be emitted in a
    beam, and with the rotation this beam may rotate
    at a high angular speed. We have seen pulses of
    light with periods of a few seconds from these
    spinning neutron stars and so we call them
    pulsars.

29
Final Stage Death of the Star
  • 3) If the final mass of the core after the
    supernova explosion is more than about 3 solar
    masses, then gravity is so strong it will
    collapse the matter even beyond the neutron star
    size. We know of nothing that would stop the
    collapse. This is called a black hole.

30
Black Holes
  • Note that the mass of a black hole is still there
    and its gravity will affect things around it.
  • But gravity is so strong near it that even light
    can be trapped so that it does not escape from
    the black hole.
  • Further away, though, other stars will feel the
    gravity just like they feel the gravity of other
    massive objects.

31
Mass back to nebula and space
  • In the ejection of the planetary nebula and in
    supernova explosions, some and sometimes most of
    the mass of the star is ejected back into space.
    There is a difference, though. The initial mass
    of the collapsing nebula consisted of mostly
    hydrogen. The final mass of the expanding nebula
    is enriched in the heavier elements. The energy
    in a supernova is so high that elements heavier
    than iron are made.
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