Generated by DeepSeek V3.2| Chandrasekhar limit | |
|---|---|
| Name | Chandrasekhar limit |
| Caption | Subrahmanyan Chandrasekhar, after whom the limit is named. |
| Unit | Solar mass |
| Value | ≈1.4 M☉ |
| Discovered | 1930 |
Chandrasekhar limit. It is the maximum stable mass for a white dwarf star, approximately 1.4 times the mass of the Sun. Beyond this critical value, electron degeneracy pressure can no longer support the star against its own gravity, leading to catastrophic collapse. This fundamental threshold governs the fate of most stars and is pivotal in understanding stellar evolution and explosive supernova events.
The precise value arises from the balance between the inward pull of gravity and the outward pressure from degenerate matter, specifically relativistic electrons. The derivation, first performed by Subrahmanyan Chandrasekhar, combines principles from quantum mechanics, special relativity, and hydrostatic equilibrium. Key equations include the Tolman–Oppenheimer–Volkoff equation for stellar structure and the equation of state for an ideal Fermi gas. The limit depends slightly on composition, with a pure helium or carbon core yielding a value near 1.4 solar mass, while the presence of iron can alter it. This theoretical cornerstone connects the physics of dense matter to observable astrophysical phenomena.
This mass limit dictates the end state for the vast majority of stars, including our own Sun. Stars with initial masses below roughly eight solar mass typically evolve into white dwarfs, but only if their final core mass resides below the critical threshold. Exceeding it triggers a Type Ia supernova, a titanic thermonuclear explosion that completely disrupts the white dwarf. These luminous events serve as crucial standard candles for measuring cosmic distances, aiding discoveries like the accelerating expansion of the universe. The collapse of a super-Chandrasekhar mass object can also form a neutron star or a black hole, linking to the study of compact objects and gravitational waves.
The concept emerged in the early 1930s from the work of Subrahmanyan Chandrasekhar during his voyage to study at the University of Cambridge. He challenged the then-prevailing view, championed by Arthur Eddington, that all stars cooled into white dwarfs regardless of mass. Chandrasekhar's incorporation of special relativity into R. H. Fowler's theory of degenerate matter predicted the existence of the mass limit. His famous confrontation with Eddington at a 1935 meeting of the Royal Astronomical Society became a landmark in astrophysics history. Chandrasekhar's work was later vindicated, earning him the Nobel Prize in Physics in 1983, and fundamentally altered the understanding of stellar evolution.
Several important concepts in astrophysics and theoretical physics are directly connected. The Tolman–Oppenheimer–Volkoff limit describes the maximum mass for a stable neutron star, analogous to the white dwarf case. The process of accretion in binary systems, such as those studied in X-ray binaries, can push a white dwarf toward the critical mass. Theoretical extensions consider the effects of rapid rotation, strong magnetic fields, and alternative theories of gravity on the limiting mass. Observations of superluminous Type Ia supernova events have prompted investigations into potential super-Chandrasekhar mass progenitors. These studies interface with broader research into nuclear astrophysics, cosmology, and high-energy astrophysics.
Category:Astrophysics Category:Stellar evolution Category:Physical constants