Ohm’s law states that the current density j at a given location in a plasma is proportional to the electric field E at that location. We propose here a rigorous derivation of this law (and of some extensions of it) starting from a microscopic model consisting of two species of charged particles interacting both via the self-consistent electromagnetic field, and via some collisional processes.
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Über dieses Kapitel
Titel
Deriving Ohm’s Law from the Vlasov-Maxwell-Boltzmann System
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