Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 1
... distribution function f , ranging from the Liouville function F ( x1 , X2 , ... , Xx , V1 , ... , v ) to the Boltzmann single - particle function f ( x , v ) . The Liouville function is a function of the complete set of micro co ...
... distribution function f , ranging from the Liouville function F ( x1 , X2 , ... , Xx , V1 , ... , v ) to the Boltzmann single - particle function f ( x , v ) . The Liouville function is a function of the complete set of micro co ...
Page 21
... distribution the Maxwellian , this is also valid for slow motions in strong fields . The distribution function is written as ƒ = fo + f1 + ƒ2 , where Dfowof / cq so that = fi = 1 fo m cxb Vlog T ( e × b ) · d − ( V_V_ × b − b × VV ) ...
... distribution the Maxwellian , this is also valid for slow motions in strong fields . The distribution function is written as ƒ = fo + f1 + ƒ2 , where Dfowof / cq so that = fi = 1 fo m cxb Vlog T ( e × b ) · d − ( V_V_ × b − b × VV ) ...
Page 187
... distribution function of the trapped electrons . It can be readily solved by the Laplace transformation , yielding ... distribution function . By considering various trapping regions of a wave of arbitrary form suc- cessively , filling a ...
... distribution function of the trapped electrons . It can be readily solved by the Laplace transformation , yielding ... distribution function . By considering various trapping regions of a wave of arbitrary form suc- cessively , filling a ...
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