Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 5
... Boltzmann's equation and determining . the transport coefficients . 2. Hydrodynamic equations from the transport equation . As a preliminary to any attempt to solve the Boltzmann equation we will use it to form the hydrodynamic equations ...
... Boltzmann's equation and determining . the transport coefficients . 2. Hydrodynamic equations from the transport equation . As a preliminary to any attempt to solve the Boltzmann equation we will use it to form the hydrodynamic equations ...
Page 24
... Equation . Introduction . - Having shown how the Boltzmann equation leads to the appearance of transport coefficients and to phenomena associated with « real » fluids , we turn to the prior question , that of determining the correct ...
... Equation . Introduction . - Having shown how the Boltzmann equation leads to the appearance of transport coefficients and to phenomena associated with « real » fluids , we turn to the prior question , that of determining the correct ...
Page 72
... Boltzmann equation . The adiabatic theory corresponds to the limit of no collisions and small gyration radius . Therefore we start with the Vlasov or collisionless Boltzmann equation for each kind of particle , ions and electrons ( 1 ) ...
... Boltzmann equation . The adiabatic theory corresponds to the limit of no collisions and small gyration radius . Therefore we start with the Vlasov or collisionless Boltzmann equation for each kind of particle , ions and electrons ( 1 ) ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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adiabatic invariant amplitude approximation Boltzmann equation boundary conditions boundary layer calculated cathode coefficient collision components consider constant contraction corresponds courbe critère current density d³k d³v Debye length derived differential equations discharge dispersion relation distribution function eigenvalue electric field electrons and ions electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ KRUSKAL l'axe magnétique limit Liouville function lowest order magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle périodique perturbation Phys plasma oscillations Plasma Physics Poisson's equation potential problem quantities R₁ region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity x₁ zero zero-order Απ