For white dwarfs consisting essentially of the carbon isotope
or the oxygen isotope
valid:

This results directly in the mentioned critical mass of 1.457 solar masses. An example for such a star is SiriusB.
For white dwarfs with an iron core of , on the other hand, holds:

Its limiting mass is therefore 1.256 solar masses. The Chandrasekhar limit is therefore not to be understood in such a way that it is the same for every star. It rather depends on the kind of stellar matter, which upper limit is present in each case.
Thermonuclear supernovae Ia are interpreted as a consequence of exceeding the Chandrasekhar limit mass. These supernovae show a rather uniform course of the light curve and in their absolute brightness. A subset of type Ia supernovae, those of the super-Chandrasekhar Ia supernovae, has a much higher luminosity, suggesting a collapsed white dwarf with a mass of up to 2.5 solar masses. Attempts have been made to model white dwarfs with high magnetic field densities, stabilizing the degenerate matter against collapse. However, Lorentz forces should prevent a large increase in Chandrasekhar's limiting mass.
Neutron stars and quark stars
For neutron stars there is an equivalent limit, the Tolman-Oppenheimer-Volkoff limit. Likewise, an equivalent limit is assumed for the hypothetical quark stars, but the equations of state of these exotic types of degenerate matter are not yet precisely known.