The second phase in the evolution of a
→ supernova remnant (SNR)
occurring after the → free expansion phase.
After the passage of the → reverse shock,
the interior of the SNR is so hot that the energy
losses by radiation are very small (all atoms are → ionized,
no → recombination).
The expansion is driven by the → thermal pressure
of the hot gas and can therefore be regarded as → adiabatic;
the → cooling of the
gas is only due to the → expansion.
Pressure forces accelerate the swept-up → interstellar medium (ISM)
converting → thermal energy
(which came from original explosion) into → kinetic energy
of the → shell of swept-up mass.
As the mass of the ISM swept up by the shell
increases, it eventually reaches densities which start to
impede the free expansion. → Rayleigh-Taylor
instabilities arise once
the mass of the swept-up ISM approaches that of the ejected
material. This causes the SNR’s ejecta to become
mixed with the gas that was just shocked by the initial → shock wave.
The Sedov-Taylor phase lasts some 104 years and
is followed by the radiative or → snowplow phase.
Also called → adiabatic phase.
See also: After Sedov, L. (1959, Similarity and Dimensional Methods in Mechanics, New York,
Academic Press) and Taylor, G. I. (1950, Proc. Roy. Soc. London, A, 201, 159 and 175);
→ phase.