Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 21
... obtained is not the solution f , but some rather crude approximation to the normal solution . This being so , it might be appropriate to consider not the equation for f , but the equations for the moments of f . The moment equations do ...
... obtained is not the solution f , but some rather crude approximation to the normal solution . This being so , it might be appropriate to consider not the equation for f , but the equations for the moments of f . The moment equations do ...
Page 165
... obtain solu- tions to eq . ( 20 ) that vanish at μ = μ1 , μ2 , the external boundaries . These solutions cannot , in ... obtained near the same point and only there . The second stage of the general solution therefore consists in solv ...
... obtain solu- tions to eq . ( 20 ) that vanish at μ = μ1 , μ2 , the external boundaries . These solutions cannot , in ... obtained near the same point and only there . The second stage of the general solution therefore consists in solv ...
Page 191
... obtained on a one - dimensional model , whereas , according to ( 4.14 ) , the background waves parallel to the test wave make no contribution to ( 4.17 ) . However , in a thermal plasma , for which the excitation of background waves is ...
... obtained on a one - dimensional model , whereas , according to ( 4.14 ) , the background waves parallel to the test wave make no contribution to ( 4.17 ) . However , in a thermal plasma , for which the excitation of background waves is ...
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