Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 180
... electrostatic waves in a cold homogeneous plasma , free from magnetic field , is ( 1.1 ) w2 = w } , ( ) This study was supported by the Air Force Office of Scientific Research under grant no . AF - AFOSR - 62-343 . where , is the ...
... electrostatic waves in a cold homogeneous plasma , free from magnetic field , is ( 1.1 ) w2 = w } , ( ) This study was supported by the Air Force Office of Scientific Research under grant no . AF - AFOSR - 62-343 . where , is the ...
Page 197
... electrostatic and electromagnetic waves in plasmas may be regarded as typical of the phenomenon of mode- coupling which is a consequence of nonlinearity of wave equations . Coupling between other wave types could be discussed in a ...
... electrostatic and electromagnetic waves in plasmas may be regarded as typical of the phenomenon of mode- coupling which is a consequence of nonlinearity of wave equations . Coupling between other wave types could be discussed in a ...
Page 241
... Electrostatic probe in a strong magnetic field . We will consider now an example which I have worked out in detail . It concerns the theory of charge - collection by an electrode whose size is larger than the Larmor radius of the ...
... Electrostatic probe in a strong magnetic field . We will consider now an example which I have worked out in detail . It concerns the theory of charge - collection by an electrode whose size is larger than the Larmor radius of the ...
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