The behaviour of a L~RENTZ plasma in a spatially homogeneous rotating magnetic field, 3. constant magnetic field parallel to the rotation axis, the induced electric field and an external alternating electric field (of the same frequency) is treated within the framework of kinetic theory. The BOLTZNAXN equation with collision integral is solved using a FOWRIEB expansion.The tensors of electrical conductivity, diffusion and thermal diffusion are calculated and then discussed by means of the ONSAGER-CASIMIR reciprocity relationa and the KRONIO-KRAMERS relations. A generalized version of the KROXI~~KRAMERS relations is given. Finally, the case of a spatially rotating magnetic field with arbitrarily space dependent phase (helical field) is treated.
With the methods of kinetic theory on the basis of the Boltzmann and Fokker-Planck kinetic equations the behaviour of a Lorentz plasma in a circularly polarized (rotating) magnetic field (rotation frequencyw), a n alternating electric field (frequency 0') and additional constant electromagnetic fields is inveatigated. By means of a generalized Fourier expansion it is shown that the above fields create in the plasma currenta of the frequencies 0, w', w-w', w, w+w', 2w-w', 20, and 2w+w'. Tramport, coefficients are calculated explicitly and the validity of Onsager reciprocity relations and that of Kronig-liramers relations is discussed. The special c&98 of the electric field induced by the rotating magnetic field is treated separately. Finally, problems of plasma containment are discussed.
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