Advanced Plasma Theory, Volume 25M. N. Rosenbluth |
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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 ...
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