Advanced Plasma TheoryM. N. Rosenbluth |
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Page 101
... Electric field . β Field enhancement factor . Coefficient of particle liberation . ა Dirac function . Work function . μ Mobility . Ο Supply function . II Current of energy . Section 4 : B , C , D , e , h , k , k , m , n , p , r , T , V ...
... Electric field . β Field enhancement factor . Coefficient of particle liberation . ა Dirac function . Work function . μ Mobility . Ο Supply function . II Current of energy . Section 4 : B , C , D , e , h , k , k , m , n , p , r , T , V ...
Page 104
... electric field ( X ) but only approximate analytical formulae for very high or very small electric fields . log ( 4 / A / cm2 ) To judge whether the T - F - mechanism is able to explain the production 9 8 = 35 7 9 = 102 B = 1 9-10 9-10 ...
... electric field ( X ) but only approximate analytical formulae for very high or very small electric fields . log ( 4 / A / cm2 ) To judge whether the T - F - mechanism is able to explain the production 9 8 = 35 7 9 = 102 B = 1 9-10 9-10 ...
Page 126
... Electric field ( E ) , relative axial density of the negative ions ( yon - c / neo ) and relative axial posi- tive ... field E independent of the current . How- ever with decreasing current we reach a region where the electric field ...
... Electric field ( E ) , relative axial density of the negative ions ( yon - c / neo ) and relative axial posi- tive ... field E independent of the current . How- ever with decreasing current we reach a region where the electric field ...
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