Advanced Plasma TheoryM. N. Rosenbluth |
From inside the book
Results 1-3 of 91
Page 58
... given in the paper by BERNSTEIN , FRIEMAN , KRUSKAL and KULSRUD [ 4 ] . We parallel the development of the consequences of these equations given in this paper . The energy principle for the fluid theory derived in these notes was first ...
... given in the paper by BERNSTEIN , FRIEMAN , KRUSKAL and KULSRUD [ 4 ] . We parallel the development of the consequences of these equations given in this paper . The energy principle for the fluid theory derived in these notes was first ...
Page 60
... given above . We write at a fixed point r . p = po + p ' , V B Q = - = V ' , Bo + B ' , Qo + g ' , J = Jo + J ' . From ( 14 ) J ' = V × B ' . p ' , V ' , B ' and ' can be given independently initially and then ( 9 ) - ( 14 ) give § ( r ...
... given above . We write at a fixed point r . p = po + p ' , V B Q = - = V ' , Bo + B ' , Qo + g ' , J = Jo + J ' . From ( 14 ) J ' = V × B ' . p ' , V ' , B ' and ' can be given independently initially and then ( 9 ) - ( 14 ) give § ( r ...
Page 89
... given by KRUSKAL and OBERMAN and differs from ours due to a difference in definition of ɛ . Their ε is Eko vp + q2 / 2 with no y . Expression ( 88 ) is identical with that given by KRUSKAL and OBERMAN after one sets f + = ƒ_ in their ...
... given by KRUSKAL and OBERMAN and differs from ours due to a difference in definition of ɛ . Their ε is Eko vp + q2 / 2 with no y . Expression ( 88 ) is identical with that given by KRUSKAL and OBERMAN after one sets f + = ƒ_ in their ...
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