Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 65
... energy rather than defined by ( 20 ) . For , for an unstable normal mode w , is imaginary let the kinetic energy be SW exp [ 2io , t ] ; K = iføš dr . This is also proportional to exp [ 2io , t ] . If 8W > 0 we have - u = K + SW ~ exp ...
... energy rather than defined by ( 20 ) . For , for an unstable normal mode w , is imaginary let the kinetic energy be SW exp [ 2io , t ] ; K = iføš dr . This is also proportional to exp [ 2io , t ] . If 8W > 0 we have - u = K + SW ~ exp ...
Page 67
... energy principle has the advantage . This is facilitated by the fact that the energy has a physically intuitive ... kinetic energy at the expense of potential energy it need not remain propor- tional to . may change direction and move ...
... energy principle has the advantage . This is facilitated by the fact that the energy has a physically intuitive ... kinetic energy at the expense of potential energy it need not remain propor- tional to . may change direction and move ...
Page 139
... kinetic energy of the system E mv2 2 fd3x d3v , subject to the constancy of the total number of particles and of S ... energy of the system consistent with this constraint is that defined by the initial distribution fo . In other words ...
... kinetic energy of the system E mv2 2 fd3x d3v , subject to the constancy of the total number of particles and of S ... energy of the system consistent with this constraint is that defined by the initial distribution fo . In other words ...
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