The Death of Low-Mass Stars-Chapter 23

23.1 The Death of Low-Mass Stars

Learning Objectives

  • Understand the final mass of stars less than approximately 1.4 times the mass of the Sun (M_{Sun}) and why this mass is critical.
  • Recognize that low-mass stars constitute the majority in the universe, akin to a few musicians becoming superstars in the music industry.

General Concept of Low-Mass Stars

  • Most stars have a final mass < 1.4 M_{Sun}.
  • Mass Loss: Many stars initiating with initial masses > 1.4 M_{Sun} eventually decrease to below this threshold due to mass loss.
    • E.g., stars starting with 8.0 M{Sun} may lose mass and end up below 1.4 M{Sun}.

A Star in Crisis

  • Previous section ended with a Sun-like star in the red-giant region and shedding outer layers, forming a planetary nebula.
  • The core is in energy crisis:
    • Previously stable helium fusion produced carbon and oxygen until helium was exhausted.
    • Without pressure from fusion, the core collapses under gravity until it reaches extreme densities (1 million times that of water).

Core Contraction and White Dwarfs

  • Core Collapse: Continued collapse leads to density nearing 200,000 times Earth's average density.
  • At this density, a new behavior of matter begins, stabilizing the star into a white dwarf.

Degenerate Stars

  • White dwarfs exhibit behavior indicative of degenerate matter; very dense and stabilized by electron degeneracy pressure.
  • Pauli Exclusion Principle: No two electrons may occupy the same place and state at once.
    • High density leads to significant resistance against further contraction by electrons.
    • This phenomenon allows white dwarfs to maintain their structure without additional heat input.
    • Electrons in degenerate gas experience restricted movement due to proximity constraints.
  • Atomic nuclei are not in a degenerate state unless subjected to higher densities.
  • Core collapse stops due to electron degeneracy pressure, and thus white dwarfs are compact with electron-degenerate cores.

Characteristics of White Dwarfs

  • Subrahmanyan Chandrasekhar's Contributions:
    • Calculated that white dwarfs would contract until electrons achieve maximum density, limiting mass to about 1.4 M_{Sun} (the Chandrasekhar Limit).
    • Beyond this mass, collapse cannot be prevented by electron degeneracy pressure, leading to different end states for stars.

Diagram of Mass-Radius Relationship

  • White dwarf radius decreases as mass increases. A typical white dwarf mass > 1.4 M_{Sun} would compress to a zero radius.

Ultimate Fate of White Dwarfs

  • After fusion ceases, white dwarfs cool and eventually become black dwarfs, transitioning through billions of years.
  • They predominantly consist of carbon, oxygen, and neon.
  • Carbon crystallization results in a diamond-like structure.

Mass Loss Implications on Star Evolution

  • Stars below Chandrasekhar limit become white dwarfs based on how mass is shed during red-giant phase.
    • Evidence suggests stars > 8 M_{Sun} can shed enough mass to transition into white dwarfs.
    • Example: A star that initially had mass of 6 M{Sun} must shed sufficient mass to fall under 1.4 M{Sun}.
    • Main-sequence stars can lose significant mass during evolution to reach this final threshold.

23.2 Evolution of Massive Stars: An Explosive Finish

Learning Objectives

  • Understand nuclear fusion complexities in massive stars.
  • Describe core collapse steps in massive stars leading to supernovae.
  • Analyze hazards associated with nearby supernovae.

Brief Overview of Massive Stars

  • Stars initiating at 8 M{Sun} potentially end as white dwarfs, though stars exceeding 150 M{Sun} undergo explosive deaths.

Nuclear Fusion in Heavy Elements

  • After helium depletion, core contraction raises temperatures to fuse carbon, generating heavier elements like oxygen and iron.
  • Rates of fusion reaction increase drastically, with heavy elements forming rapidly in comparison to the longer main-sequence phase.
  • Core resembles an internal structure similar to an onion with layers of differing element states.

Iron Crisis and Core Collapse

  • Iron fusion halts energy output leading to catastrophic collapse with core densities approaching nuclear densities.
  • Neutron Creation: Electrons merge with protons to create neutrons and neutrinos, with resultant core shrinkage and neutron disk formation preventing further collapse.
  • Below a certain threshold (approximately 3 M_{Sun}), neutron stars are formed.

Collapse and Supernova Explosion

  • The collapse leading to supernovae releases immense energy, with neutrino luminosity surpassing light from billion galaxies.
  • A regular star (mass > 8 M{Sun}) expels > 5 M{Sun} during supernova phenomena.

Conditions for a Supernova

  • Explosive core collapse releases energy that ejects outer layers in explosive spectacular events.
  • Type II Supernovae results from massive star collapses versus Type Ia explosions arising from white dwarfs in binary systems.

Summary of Mass Outcomes and Stellar Events

  • Initial mass and outcomes categorized:
    • < 0.01 M_{Sun} = Planet
    • 0.01 to 0.08 M_{Sun} = Brown dwarf
    • 0.08 to 0.25 M_{Sun} = White dwarf (helium)
    • 0.25 to 8 M_{Sun} = White dwarf (carbon-oxygen)
    • 8 to 10 M_{Sun} = White dwarf (oxygen/neon/magnesium)
    • 10 to 40 M_{Sun} = Supernova (neutron star)
    • >40 M_{Sun} = Supernova (black hole)

Conclusion: The Supernova Cycle

  • Supernova has cyclical implications, enriching interstellar medium with heavy elements crucial for future star formation and life's origin.
  • Supernova explosions recycle materials necessary for new planetary systems, sustaining the universe's evolutionary cycle.
  • The creation of elements heavier than iron occurs primarily through supernova processes and neutron star mergers.