The first phase of → supernova remnant (SNR) evolution in
which the surrounding → interstellar medium (ISM) has no influence
on the expansion of the → shock wave,
and the pressure of the interstellar gas is negligible.
The shock wave created by the → supernova explosion
moves outward into the
interstellar gas at highly → supersonic
speed. Assuming that most of the → supernova energy
ESN is transformed into → kinetic energy
of the ejected gas, the ejection velocity
ve can be estimated from ESN by using
ESN = (1/2) Meve2, which
leads to
ve = (2ESN / Me)(1/2),
where Me is the ejected mass.
The schematic structure of the SNR at this phase can be described as follows: behind
the strong → shock front
which moves outward into the ISM, compressed interstellar gas
accumulates forming a → shell of interstellar gas.
This shell of swept-up material in front of shock
does not represent a significant increase in the mass of the system.
After some time the accumulated mass equals the ejected mass of stellar
material, and it will start to affect the expansion of the SNR. By definition,
this is the end of the free
expansion phase, and the corresponding radius of the SNR, called
→ sweep-up radius,
RSW, is defined by
Me = (4π/3) RSW3ρ0,
that is RSW =
(3Me / 4πρ0)(1/3),
where ρ0 is the initial density of the ISM.
This radius is reached at the
sweep-up time tSW = RSW/ve.
The free expansion phase lasts some 100-200 years until the
mass of the material swept up by the shock wave exceeds the mass of
the ejected material. Then the following → snowplow phase
starts.
See also: → free; → expansion;
→ phase.