![]() | Annu. Rev. Astron. Astrophys. 1990. 28:
37-70 Copyright © 1990 by Annual Reviews. All rights reserved |
The density, velocity, magnetic field strength, and temperature of gas within the interstellar medium vary continuously with position and fluctuate over all scale lengths of interest. However, various regimes of temperature and density differ markedly in the nature of their basic physical processes, especially heating and cooling. It is convenient to refer to these regimes as specific ``phases'' of the interstellar medium. A summary of the physical conditions and physical processes in thise phases is given in the table below.
The primary discriminent in phases is the condition of the hydrogen.
Another important property is the temperature. The gas pressure follows
from the density and temperature, P = nkT. Note that the
pressure, not tabulated below, is approximately constant for most of the
phases, suggesting that a given parcel of gas might spend most of its
time in the condition nT 3000 cm-3 K. Of course, there are motions
within the diffuse ISM, so the pressure is only approximate. Also, the
contribution of the magnetic fielf and cosmic rays to the total pressure
is not negligible, and may even be dominant.