Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 15
... form . Simple rational expres- sions were obtained for the transport coefficient , the simplicity being enforced by ... factor . If now the p's are substituted in ( II.3.7 ) KINETIC THEORY OF PLASMA 15.
... form . Simple rational expres- sions were obtained for the transport coefficient , the simplicity being enforced by ... factor . If now the p's are substituted in ( II.3.7 ) KINETIC THEORY OF PLASMA 15.
Page 52
yields an expression for the intensity at large distances in the form ( V.2.4 ) d'1 ... factor ( 1 + cos2 ) for an unpolarized incident beam . If the only ... form ( An ) 2 , the random phase approximation may be invoked whereupon Zexp ...
yields an expression for the intensity at large distances in the form ( V.2.4 ) d'1 ... factor ( 1 + cos2 ) for an unpolarized incident beam . If the only ... form ( An ) 2 , the random phase approximation may be invoked whereupon Zexp ...
Page 125
... factor of order of magnitude unity . For a three - carrier - component system the situation is more complicated ... form ( 4.25 ) ( Σ Γ . ) . = 0 . i As we see it , the problem of solving the four - component system presents itself as an ...
... factor of order of magnitude unity . For a three - carrier - component system the situation is more complicated ... form ( 4.25 ) ( Σ Γ . ) . = 0 . i As we see it , the problem of solving the four - component system presents itself as an ...
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