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.