Chandrasekhar Limit
| Value | 2.86e30 kg |
| Status | Measured: ± 1.00e+29 kg (0.035 relative) |
| Source | Chandrasekhar (1931); classical value 1.44 M⊙ for μₑ = 2 |
| Categories | Astronomicalstellarrelativity |
| microgram | 2.8600000e+39 μg |
| milligram | 2.8600000e+36 mg |
| gram | 2.8600000e+33 g |
| kilogram | 2.8600000e+30 kg |
| metric tonne | 2.8600000e+27 t |
| ounce | 1.0088353e+32 oz |
| pound | 6.3052207e+30 lb |
| stone | 4.5037291e+29 st |
| US short ton | 3.1526103e+27 ton |
| grain | 4.4136545e+34 gr |
| unified atomic mass unit (dalton) | 1.7223323e+57 u |
Learning zone
Subrahmanyan Chandrasekhar worked it out in 1930 at the age of nineteen, on the boat from Madras to Cambridge. Electron degeneracy pressure — the quantum refusal of electrons to share states — can hold up a cooling stellar core, but only until the electrons become relativistic, at which point the pressure stiffens too slowly to keep pace with gravity and there is a hard ceiling near 1.44 M⊙ for typical carbon-oxygen composition. Eddington ridiculed the result publicly for years; Chandrasekhar received the Nobel Prize for it in 1983.
The limit is the reason Type Ia supernovae are useful. A white dwarf accreting from a companion detonates as it approaches the limit, and because the trigger mass is always about the same, the explosions have nearly uniform peak brightness — the standard candles that revealed cosmic acceleration in 1998. The value quoted is the classical result for a mean molecular weight per electron of 2; rotation, composition and general-relativistic corrections shift it by a few per cent.