Vlasov-type and Liouville-type equations, their microscopic, energetic and hydrodynamical consequences

We give a derivation of the Vlasov-Maxwell and Vlasov-Poisson-Poisson equations from the Lagrangians of classical electrodynamics. The equations of electromagnetic hydrodynamics (EMHD) and electrostatics with gravitation are derived from them by means of a 'hydrodynamical' substitution. We obtain and compare the Lagrange identities for various types of Vlasov equations and EMHD equations. We discuss the advantages of writing the EMHD equations in Godunov's double divergence form. We analyze stationary solutions of the Vlasov-Poisson-Poisson equation, which give rise to non-linear elliptic equations with various properties and various kinds of behaviour of the trajectories of particles as the mass passes through a critical value. We show that the classical equations can be derived from the Liouville equation by the Hamilton-Jacobi method and give an analogue of this procedure for the Vlasov equation as well as in the non-Hamiltonian case. © 2017 Russian Academy of Sciences (DoM), London Mathematical Society, Turpion Ltd. All rights reserved.

Авторы
Vedenyapin V.V. 1 , Negmatov M.A.2 , Fimin N.N. 1
Журнал
Издательство
Institute of Physics Publishing
Номер выпуска
3
Язык
Английский
Страницы
505-541
Статус
Опубликовано
Том
81
Год
2017
Организации
  • 1 Keldysh Institute of Applied Mathematics, Russian Academy of Sciences, Moscow Peoples Friendship University of Russia, Moscow, Russian Federation
  • 2 Central Research Institute of Machinery, Russian Federation
Ключевые слова
Hamilton-Jacobi method; Hydrodynamical substitution; Lagrange identity; Liouville equation; Vlasov-Maxwell equation; Vlasov-Poisson-Poisson equation
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