Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 98
... region of interest will present itself not as a uniform region , but as composed of various different model regions . Since each model region is described by a number of physical laws the gas discharge problem is much more complex than ...
... region of interest will present itself not as a uniform region , but as composed of various different model regions . Since each model region is described by a number of physical laws the gas discharge problem is much more complex than ...
Page 99
... region . In the column particles are produced by electron collisions and lost by diffusion and wall recombination . Characteristic for the subnormal region is that the diffusion is not ambipolar since the particle den- sities are too ...
... region . In the column particles are produced by electron collisions and lost by diffusion and wall recombination . Characteristic for the subnormal region is that the diffusion is not ambipolar since the particle den- sities are too ...
Page 257
... region with a displacement 。 and zero velocity . The initial conditions on W and S are chosen such that W is constant throughout the initial region . From eqs . ( 3 ) , ( 4 ) , ( 7 ) and ( 9 ) . ( 10 ) ( 11 ) ( 12 ) S = ± w ( in the ...
... region with a displacement 。 and zero velocity . The initial conditions on W and S are chosen such that W is constant throughout the initial region . From eqs . ( 3 ) , ( 4 ) , ( 7 ) and ( 9 ) . ( 10 ) ( 11 ) ( 12 ) S = ± w ( in 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