Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 21
... calculating the integrals appearing in I. There is a happy agreement between transport coefficients calculated this way and the strong field limits of those calculated by Marshall . ( As corrected by Haas and Vaughan Williams . ) Yet ...
... calculating the integrals appearing in I. There is a happy agreement between transport coefficients calculated this way and the strong field limits of those calculated by Marshall . ( As corrected by Haas and Vaughan Williams . ) Yet ...
Page 33
... Calculation of the spectrum . To calculate the spectrum we can again assume that the electric field within the plasma is weak , and the interactions are small . At the same time , the effect of the field on the distribution function ...
... Calculation of the spectrum . To calculate the spectrum we can again assume that the electric field within the plasma is weak , and the interactions are small . At the same time , the effect of the field on the distribution function ...
Page 104
... calculated from the equation ( 3.1 ) ง = Emin E ) .∞ ( E ) dE , where P. denotes the emission probability of an electron of energy E , ( E ) the supply function . Both functions are given in the work of MURPHY and Good ( † ) . There is ...
... calculated from the equation ( 3.1 ) ง = Emin E ) .∞ ( E ) dE , where P. denotes the emission probability of an electron of energy E , ( E ) the supply function . Both functions are given in the work of MURPHY and Good ( † ) . There 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