
Internal structure of a Sun-like star and a red giant.
ESO image.A
giant star is a
star with substantially larger
radius and
luminosity than a
main sequence star of the same
surface temperature.
[Giant star, entry in Astronomy Encyclopedia, ed. Patrick Moore, New York: Oxford University Press, 2002. ISBN 0-19-521833-7.] Typically, giant stars have radii between 10 and 100
solar radii and luminosities between 10 and 1,000 times that of the
Sun. Stars still more luminous than giants are referred to as
supergiants and
hypergiants.
[, entry in The Encyclopedia of Astrobiology, Astronomy, and Spaceflight, David Darling, on line, accessed May 15, 2007.] A hot, luminous
main sequence star may also be referred to as a giant.
[Giant star, entry in Cambridge Dictionary of Astronomy, Jacqueline Mitton, Cambridge: Cambridge University Press, 2001. ISBN 0-521-80045-5.] Apart from this, because of their large radii and luminosities, giant stars lie above the main sequence (luminosity class
V in the
Yerkes spectral classification) on the
Hertzsprung-Russell diagram and correspond to luminosity classes
II or
III.
[giant, entry in The Facts on File Dictionary of Astronomy, ed. John Daintith and William Gould, New York: Facts On File, Inc., 5th ed., 2006. ISBN 0-8160-5998-5.]Formation
A star becomes a giant star after all the
hydrogen available for
fusion at its core has been depleted and, as a result, it has left the
main sequence.
A star whose initial mass is less than approximately 0.25
solar masses will not become a giant star. For most of their lifetimes, such stars have their interior thoroughly mixed by
convection and so they can continue fusing hydrogen for a time in excess of 10
12 years, much longer than the current age of the
Universe. Eventually, however, they will develop a radiative core, subsequently exhausting hydrogen in the core and burning hydrogen in a shell surrounding the core. (Stars with mass in excess of 0.16 solar masses may expand at this point, but will never become very large.) Shortly thereafter the star's supply of hydrogen will be completely exhausted and it will become a
helium white dwarf.
[The End of the Main Sequence, Gregory Laughlin, Peter Bodenheimer, and Fred C. Adams, The Astrophysical Journal, 482 (June 10, 1997), pp. 420–432. . .]If a star is more massive than 0.25 solar masses, then when it consumes all of the
hydrogen in its core available for
fusion, the core will begin to contract. Hydrogen now fuses to
helium in a shell around the helium-rich core, and the portion of the star outside the shell expands and cools. During this portion of its
evolution, labeled the
subgiant branch on the
Hertzsprung-Russell diagram, the
luminosity of the star remains approximately constant and its
surface temperature decreases. Eventually the star will start to ascend the
red giant branch on the
Hertzsprung-Russell diagram. At this point, the
surface temperature of the star, now typically a
red giant, will remain approximately constant as its
luminosity and radius increase drastically. The core will continue to contract, raising its temperature.
[Evolution of Stars and Stellar Populations, Maurizio Salaris and Santi Cassisi, Chichester, UK: John Wiley & Sons, Ltd., 2005. ISBN 0-470-09219-X.], § 5.9.If the star's mass, when on the main sequence, was below approximately 0.5
solar masses, it is thought that it will never attain the central temperatures necessary to fuse
helium.
, p. 169. It will therefore remain a hydrogen-fusing red giant until it eventually becomes a helium white dwarf.
, § 4.1, 6.1. Otherwise, when the core temperature reaches approximately 10
8 K, helium will begin to fuse to
carbon and
oxygen in the core by the
triple-alpha process.
,§ 5.9, chapter 6. The energy generated by helium fusion causes the core to expand. This causes the pressure in the surrounding hydrogen-burning shell to decrease, which reduces its energy-generation rate. The luminosity of the star decreases, its outer envelope contracts again, and the star leaves the
red giant branch.
[, class notes, Robin Ciardullo, Astronomy 534, Penn State University.] Its subsequent evolution will depend on its mass. If not very massive, it may be found in the
horizontal branch on the Hertzsprung-Russell diagram, or its position in the diagram may move in loops.
, chapter 6. If the star is not heavier than approximately 8
solar masses, it will eventually exhaust the helium at its core and begin to fuse helium in a shell around the core. It will then increase in luminosity again as, now an
AGB star, it ascends the
asymptotic giant branch of the Hertzsprung-Russell diagram. After the star sheds most of its mass, its core will remain as a carbon-oxygen
white dwarf.
, § 7.1–7.4.For main-sequence stars with masses great enough to eventually fuse
carbon (approximately 8
solar masses)
, p. 189, this picture must be modified in many ways. These stars do not increase greatly in luminosity after leaving the main sequence, but they will become redder. They may become
red supergiants, or
mass loss may cause them to become
blue supergiants.
, pp. 33–35; Eventually, they will become
white dwarfs composed of
oxygen and
neon, or will undergo a
core-collapse supernova to form
neutron stars, or
black holes.
, § 7.4.4–7.8.Examples
Well-known giant stars of various colors include:
- Alcyone (η Tauri), a blue-white (B-type) giant, the brightest star in the Pleiades.
- Thuban (α Draconis), a white (A-type) giant.
- α Aurigae Aa, a yellow-white (G-type) giant, one of the stars making up Capella.
- Pollux (β Geminorum), an orange (K-type) giant.
- Mira (ο Ceti), a red (M-type) giant.
See also