Advanced Plasma TheoryM. N. Rosenbluth |
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Page 43
... coefficient becomes compli- cated by the presence of the magnetic field . 2 . - The dielectric coefficient of a magnetized plasma . We will require the field induced in a plasma by the presence of charge , q , and as a preliminary , we ...
... coefficient becomes compli- cated by the presence of the magnetic field . 2 . - The dielectric coefficient of a magnetized plasma . We will require the field induced in a plasma by the presence of charge , q , and as a preliminary , we ...
Page 101
... coefficient . e Elementary charge . E Energy . h i I j J k k L m n 0 P q r Current per unit area . Current . Boltzmann constant . Direction vector . Energy loss of the electrode . Mass of particles . Number of particles per unit volume ...
... coefficient . e Elementary charge . E Energy . h i I j J k k L m n 0 P q r Current per unit area . Current . Boltzmann constant . Direction vector . Energy loss of the electrode . Mass of particles . Number of particles per unit volume ...
Page 127
... coefficient D .. To have equal ion and electron currents flowing to the wall the ion density must surpass the electron density . The concept of quasi - neutrality fails and we are in the so - called « subnormal region » . The presence ...
... coefficient D .. To have equal ion and electron currents flowing to the wall the ion density must surpass the electron density . The concept of quasi - neutrality fails and we are in the so - called « subnormal region » . The presence ...
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 KRUSKAL KULSRUD l'axe magnétique limit 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 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