White Dwarf -- from Eric Weisstein's World of Physics

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White Dwarf

White dwarfs are supported by electron degeneracy pressure. Because is small for the electrons in a compact white dwarf, must be large (by the uncertainty principle). This means that electrons gain a large momentum which exerts a pressure and supports the star. This leads to the paradoxical result that the more massive a white dwarf, the smaller its radius. The Chandrasekhar limit is the maximum mass a white dwarf may have, where is the solar mass. Eric Weisstein's World of Astronomy Shu (1982, p. 128) gives . The most massive white dwarf observed is RE J0317-853, with a mass of , where is the solar mass (Barstow et al. 1995). Most white dwarfs have masses and radii , where is the Earth radius. Eric Weisstein's World of Astronomy A white dwarf shines by radiating internal heat, eventually cooling to a black dwarf.

Black Dwarf, Chandrasekhar Limit, Electron Degeneracy Pressure, Fermion Degeneracy Pressure




References

Barstow et al. Mon. Not. Roy. Astron. Soc., Dec. 1, 1995.

Glendenning, N. K. Compact Stars: Nuclear Physics, Particle Physics, and General Relativity, 2nd ed. New York: Springer-Verlag, 2000.

Shapiro, S. L. and Teukolsky, S. A. Black Holes, White Dwarfs, and Neutron Stars: The Physics of Compact Objects. New York: Wiley, 1983.

Shu, F. H. The Physical Universe: An Introduction to Astronomy. Mill Valley, CA: University Science Books, p. 128, 1982.



© 1996-2007 Eric W. Weisstein

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