Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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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 107
... calculated in this way resembles somewhat the influence of surface roughness ( B ) , however in distinction to ẞ it is a com- pletely fundamental and gener- al effect and does not depend on special experimental con- ditions . Using a ...
... calculated in this way resembles somewhat the influence of surface roughness ( B ) , however in distinction to ẞ it is a com- pletely fundamental and gener- al effect and does not depend on special experimental con- ditions . Using a ...
Common terms and phrases
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 electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ k₂ KRUSKAL KULSRUD l'axe magnétique limit lowest order m₁ magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle perturbation Phys plasma oscillations plasma physics Poisson's equation potential problem quantities R₁ radial region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity voisinage waves in plasmas zero zero-order Απ