Abstract
Table 1.1 shows that the cosmic media can have very different properties as their parameters vary within exceptionally broad ranges. In particular, the gas ionization can vary from almost zero (neutral media, e.g., clouds of cold neutral hydrogen) to almost unity (fully ionized plasma). It is worthwhile, therefore, to start with a simpler case of equation set for the neutral gas. We assume that the reader is familiar with the hydrodynamics (HD) fundamentals, so we just remind the equations and briefly discuss the meaning of the terms entering them without going into the detail too deeply. The relation of HD to the kinetic theory has been outlined in Sect. 1.3.
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Notes
- 1.
The term GD is more appropriate in our case because the astrophysical media represent typically a gas (neutral or ionized) phase rather than a fluid, which would imply use of the term “hydro” (water).
- 2.
It must be noted that such hydrostatic equilibrium is not necessarily stable: for example, it can be convectively unstable if the temperature gradient is large; see Chaps. 6.
- 3.
The model considered here was proposed by Parker (1959) to describe the interplanetary magnetic field produced by the solar plasma flows composing the solar wind.
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Fleishman, G.D., Toptygin, I.N. (2013). Magnetohydrodynamics of the Cosmic Plasma. In: Cosmic Electrodynamics. Astrophysics and Space Science Library, vol 388. Springer, New York, NY. https://doi.org/10.1007/978-1-4614-5782-4_2
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