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Titlebook: Kinetic Theory of Gases and Plasmas; P. P. J. M. Schram Book 1991 Kluwer Academic Publishers 1991 Boltzmann equation.H-theorem.Liouville e

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31#
發(fā)表于 2025-3-26 23:51:49 | 只看該作者
32#
發(fā)表于 2025-3-27 02:34:34 | 只看該作者
Kinetic Theory of Gases and Plasmas978-94-011-3612-9Series ISSN 0168-1222 Series E-ISSN 2365-6425
33#
發(fā)表于 2025-3-27 05:19:08 | 只看該作者
34#
發(fā)表于 2025-3-27 09:41:49 | 只看該作者
35#
發(fā)表于 2025-3-27 14:18:56 | 只看該作者
Introduction,) and the macroscopic (or phenomenological) description of physical transport phenomena in continuous media. Examples of macroscopic theories are hydrodynamics and the Chew-Goldberger-Low theory in plasma physics. These theories consist always of a closed system of partial differential equations for
36#
發(fā)表于 2025-3-27 19:20:51 | 只看該作者
Klimontovich Equation, B.B.G.K.Y.-Hierarchy and Vlasov-Maxwell Equations,he starting point for the derivation of a hierarchy of equations for the multiple distribution functions introduced in Chapter 1. As a simple example the description of collisionless plasmas is based on this general theory.
37#
發(fā)表于 2025-3-28 00:51:27 | 只看該作者
38#
發(fā)表于 2025-3-28 04:09:00 | 只看該作者
Kinetic Theory of Plasmas in the Binary Collision Approximation,ns, electrons and neutrals) and the interaction forces between charged particles have a long range character. The present chapter is mainly devoted to the first aspect and to the response of plasmas to external electric fields.
39#
發(fā)表于 2025-3-28 09:47:14 | 只看該作者
40#
發(fā)表于 2025-3-28 13:09:40 | 只看該作者
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