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  2. Stellar evolution - Wikipedia

    en.wikipedia.org/wiki/Stellar_evolution

    The timescale for complete fusion of a carbon core to an iron core is so short, just a few hundred years, that the outer layers of the star are unable to react and the appearance of the star is largely unchanged. The iron core grows until it reaches an effective Chandrasekhar mass, higher than the formal Chandrasekhar mass due to various ...

  3. Stellar core - Wikipedia

    en.wikipedia.org/wiki/Stellar_core

    A stellar core is the extremely hot, dense region at the center of a star. For an ordinary main sequence star, the core region is the volume where the temperature and pressure conditions allow for energy production through thermonuclear fusion of hydrogen into helium. This energy in turn counterbalances the mass of the star pressing inward; a ...

  4. Iron star - Wikipedia

    en.wikipedia.org/wiki/Iron_star

    In astronomy, an iron star is a hypothetical type of compact star . Unrelatedly, the term "iron star" is also used for blue supergiants which have a forest of forbidden Fe II lines in their spectra. They are potentially quiescent hot luminous blue variables. Eta Carinae has been described as a prototypical example. [1] [2]

  5. White dwarf - Wikipedia

    en.wikipedia.org/wiki/White_dwarf

    If a star is massive enough, its core will eventually become sufficiently hot to fuse carbon to neon, and then to fuse neon to iron. Such a star will not become a white dwarf, because the mass of its central, non-fusing core, initially supported by electron degeneracy pressure, will eventually exceed the largest possible mass supportable by ...

  6. Oxygen-burning process - Wikipedia

    en.wikipedia.org/wiki/Oxygen-burning_process

    The oxygen fuel within the core of the star is exhausted after 0.01–5 years, depending on the star's mass and other parameters. [1] [3] The silicon-burning process , which follows, creates iron, but this iron cannot react further to create energy to support the star.

  7. Chandrasekhar limit - Wikipedia

    en.wikipedia.org/wiki/Chandrasekhar_limit

    For more-massive stars, electron degeneracy pressure does not keep the iron core from collapsing to very great density, leading to formation of a neutron star, black hole, or, speculatively, a quark star. (For very massive, low-metallicity stars, it is also possible that instabilities destroy the star completely.)

  8. Stellar structure - Wikipedia

    en.wikipedia.org/wiki/Stellar_structure

    Stellar structure. Cross-section of the Sun. Stellar structure models describe the internal structure of a star in detail and make predictions about the luminosity, the color and the future evolution of the star. Different classes and ages of stars have different internal structures, reflecting their elemental makeup and energy transport ...

  9. Silicon-burning process - Wikipedia

    en.wikipedia.org/wiki/Silicon-burning_process

    The nickel-56 decays first to cobalt-56 and then to iron-56, with half-lives of 6 and 77 days respectively, but this happens later, because only minutes are available within the core of a massive star. The star has run out of nuclear fuel and within minutes its core begins to contract. [citation needed]