Abstract
The form of the distribution functionf (P i, Qi,t) is determined in terms of the integralW of the diffusion equation and of the initial distribution functionf 0(P i, Qi, t).W gives the probability of the occurrence of a particle in the phase space Pi, Qk.
The Hamiltonian function of the particle and the distribution functionf obtained in the above way are used for establishing the value of the absorbed energy and the rate of absorption in the case of the homogeneous magnetostatic fields. We discuss the conservative r.f. field-particle system (also in the nonlinear approximation), the effect of the nonlinearity of the diffusion tensor and the meaning of the resonance for the rate of absorption. We discuss also shortly the effect of the external stochastic field on the stability of plasma, already mentioned in earlier literary sources.
Similar content being viewed by others
References
Krlín L.: IPPCZ-76 Institute of Plasma Physics, Prague 1967.
Prigogin I.: Non-equilibrium Statistical Mechanics (in Russian). Mir, Moscow 1964, 81.
Sturrock P. A.: Phys. Rev.141 (1966), 186.
Chandrasekhar S.: Rev. Mod. Phys.15 (1943), 1.
Krlín L.: Czech. J. Phys.B 18 (1968), 977.
Bass F. G., Faynberg J. B., Shapiro V. D.: Zh. eks. tekh. fiz.49 (1965), 329.
Dupree T. H.: Phys. Fluids10 (1967), 1049.
Thomassen K. I.: Phys. Lett.26A (1967), 22.
Author information
Authors and Affiliations
Additional information
The author wishes to thank Dr. J. Lacina for valuable discussions.
Rights and permissions
About this article
Cite this article
Krlín, L. Some comments on the diffusion of particles in stochastic r.f. fields. Czech J Phys 19, 1076–1091 (1969). https://doi.org/10.1007/BF01691757
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01691757