Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 55
... equations . The basic equations underlying all three theories . will be the Fokker - Planck equation [ 6 ] for the Boltzmann distribution function of each particle and Maxwell's equations for the electromagnetic field . In each of the ...
... equations . The basic equations underlying all three theories . will be the Fokker - Planck equation [ 6 ] for the Boltzmann distribution function of each particle and Maxwell's equations for the electromagnetic field . In each of the ...
Page 75
... Maxwell's equations to zero order . - Equation ( 11 ) gives F in terms of ɑ , n , ɛ as functions of r and t , Also the definitions of q and w depend on a and n . To find the behavior of a = ( E × B ) | B2 , n = B || B❘ and ε ( En ) n ...
... Maxwell's equations to zero order . - Equation ( 11 ) gives F in terms of ɑ , n , ɛ as functions of r and t , Also the definitions of q and w depend on a and n . To find the behavior of a = ( E × B ) | B2 , n = B || B❘ and ε ( En ) n ...
Page 77
... equation for ions and electrons dotting with n and subtracting ( see ref . [ 13 ] ) . It is easily shown that ( 25 ) Po = - p1 ( I — nn ) + p1nn , where ( 26 ) ( 27 ) P1 = m / w Fo2лdw dq , P q2 Fo2л dw dq . = m fq2 Thus , Maxwell's ...
... equation for ions and electrons dotting with n and subtracting ( see ref . [ 13 ] ) . It is easily shown that ( 25 ) Po = - p1 ( I — nn ) + p1nn , where ( 26 ) ( 27 ) P1 = m / w Fo2лdw dq , P q2 Fo2л dw dq . = m fq2 Thus , Maxwell's ...
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