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The End of a High Mass Star

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O-16, Ne-20, Mg-24, Si-28, S-32, Ar-36, Ca-40, Ti-44, Cr-48, ... N49 in the Large Magellanic Cloud. Cassiopeia A. Supernova. 1987A. In the Large Magellanic Cloud ... – PowerPoint PPT presentation

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Title: The End of a High Mass Star


1
The End of a High Mass Star
2
Fusion of Heavy Elements
  • Very massive stars can fuse larger and larger
    elements
  • Hydrogen to Helium
  • Helium to Carbon
  • Elements after carbon are created by Helium
    capture
  • O-16, Ne-20, Mg-24, Si-28, S-32, Ar-36, Ca-40,
    Ti-44, Cr-48, Fe-52, Ni-56
  • Ni-56 is unstable and decays to Fe-56

3
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4
The Iron Core
  • Iron-56 is the most stable of all nuclei
  • Elements smaller than Fe-56 release energy
    through FUSION
  • Elements larger than Fe-56 release energy through
    FISSION
  • Once Fe-56 is formed, the energy production of
    the star completely stops

5
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6
Stellar Nucleosynthesis
  • Hydrogen and Helium are primordial elements
  • They have existed since the beginning of the
    universe
  • Elements larger than these are created in the
    cores of stars and released when they die
  • Fusion creates C and others (4, 4, etc)
  • Elements and isotopes between H and Fe are
    created by decay, proton or neutron capture, or
    side reactions but are less common

7
Elements larger than Iron
  • Fusion is out of the question, because too much
    energy is required
  • Heavier elements form from neutron capture
    followed by decay (usually beta decay)
  • Called the s-process (the s is for slow)
  • Large quantities are not produced
  • Most of this is done during the impending
    explosion

8
The Fate of a High Mass Star
  • Once fusion produces an iron core, energy
    production ceases and the core contracts
  • The heat caused by this contraction is so great
    (10 billion K) that photons have enough energy to
    split the iron back down until there are only
    protons, neutrons, and electrons
  • Called photodisintegration
  • The process absorbs some of the energy and causes
    the core to contract even further

9
Neutronization
  • Protons and Electrons are crushed together
  • Forms a neutron and a neutrino
  • The neutrino carries away a lot of energy,
    further reducing the cores support
  • The disappearance of electrons eliminates the
    electron degeneracy pressure, so the core can be
    compressed all until the neutrons come in contact
    with each other
  • Density of 1 billion kg per cubic centimeter

10
The Bounce
  • By the time the collapse is halted by the neutron
    degeneracy pressure, it has overshot its
    equilibrium
  • The core bounces back
  • Entire process from beginning of collapse to
    bounce lasts just seconds
  • An enormously energetic shockwave travels out,
    blasting all layers into space
  • Core-Collapse Supernova

11
Novae vs. Supernovae
  • Appear similar
  • Both increase luminosity significantly
  • Very different
  • Supernovae are WAY brighter
  • Novae arise from accretion around a white dwarf
    in a binary system
  • Supernovae are the explosions of high mass stars

12
Types of Supernovae
  • Spectroscopy indicates that there are two
    distinct types of supernovae
  • Type I is lacking in hydrogen
  • Type II is hydrogen rich
  • The two types even remain bright for different
    lengths of time
  • Type II supernovae are caused by the
    implosion-explosion of a massive star

13
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14
Type I Supernovae
  • In a binary system with a white dwarf, accretion
    can cause novae
  • With each nova, not ALL of the material is
    ejected
  • Can build up over time
  • If the total mass of the white dwarf exceeds
    about 1.4 solar masses (the Chandrasekhar Mass),
    the degeneracy pressure is overcome and the star
    collapses
  • Carbon begins to fuse everywhere at once and the
    white dwarf explodes
  • Explains why the spectra are lacking in hydrogen

15
Supernovae
  • The probability of witnessing a supernova is low,
    but there are examples throughout history
  • In 1054 AD Chinese astronomers recorded a bright
    star that could be seen during the day for nearly
    a month
  • Tycho observed one in 1572
  • Kepler observed one in 1604
  • Hundreds have been observed in other galaxies
    since then

16
Supernova Remnants
  • We can see the remains of the star after it
    explodes
  • The hydrogen envelope is ejected and excited by
    the energy produced
  • A new kind of nebula

17
The Crab Nebula Supernova of 1054 AD
18
Tychos Star
19
Vela Supernova Remnant
20
Remnant N 63A
21
Keplers Supernova
22
N49 in the Large Magellanic Cloud
23
Cassiopeia A
24
Supernova 1987A In the Large Magellanic Cloud
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