Advanced Plasma TheoryM. N. Rosenbluth |
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Page 54
... pressure always remains a scalar , but however , still so weak that the conductivity may be taken as infinite . The adiabatic theory corresponds to the limit of no collisions and to the limit where the gyration radius of each type of ...
... pressure always remains a scalar , but however , still so weak that the conductivity may be taken as infinite . The adiabatic theory corresponds to the limit of no collisions and to the limit where the gyration radius of each type of ...
Page 56
... pressure of the fluid ( assumed scalar ) , j , B , E and q are the current , magnetic field , electric field and charge density . The units used are Gaussian except j is given in e.m.u .; d / dt indi- cates /t+V.V as usual . 7 , c and σ ...
... pressure of the fluid ( assumed scalar ) , j , B , E and q are the current , magnetic field , electric field and charge density . The units used are Gaussian except j is given in e.m.u .; d / dt indi- cates /t+V.V as usual . 7 , c and σ ...
Page 115
... pressure , than we move from ( 01 ) to ( 02 ) . Simultaneously and in accord- ance with experiment the contraction ... pressure J - Je Fig . 12 . - E - diagram which explains the existence of the critical pressure PR- 10 100 Ro / R with ...
... pressure , than we move from ( 01 ) to ( 02 ) . Simultaneously and in accord- ance with experiment the contraction ... pressure J - Je Fig . 12 . - E - diagram which explains the existence of the critical pressure PR- 10 100 Ro / R with ...
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