Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 117
... ions and electrons leave the discharge zone . In a stationary state the loss ... ion stream of high density enters the ILZ from the end of the contraction zone ... magnetic field . For a description of the ion motion we use the Lorentz ...
... ions and electrons leave the discharge zone . In a stationary state the loss ... ion stream of high density enters the ILZ from the end of the contraction zone ... magnetic field . For a description of the ion motion we use the Lorentz ...
Page 121
... ions ) without a magnetic field in the whole normal and subnormal region . 2 ) The three - component , quasi - neutral system in a magnetic field including temperature variation and external particle production . 3 ) The instability of ...
... ions ) without a magnetic field in the whole normal and subnormal region . 2 ) The three - component , quasi - neutral system in a magnetic field including temperature variation and external particle production . 3 ) The instability of ...
Page 148
... magnetic field . In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency in a tepid C's plasma when the electron drift velocity parallel to the magnetic field exceeds about three times ...
... magnetic field . In a recent experiment , D'ANGELO and coworkers have observed oscilla- tions near the ion cyclotron frequency in a tepid C's plasma when the electron drift velocity parallel to the magnetic field exceeds about three times ...
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