Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 71
... symmetric . What are A and K ? To find them we take { = 0 ; so V = ¿ , SB = Sp = 8Q = 0 , dr = dτo and U = dr . 2 ... symmetrical in and έ so K F GENERAL STABILITY THEORY IN PLASMA PHYSICS 71.
... symmetric . What are A and K ? To find them we take { = 0 ; so V = ¿ , SB = Sp = 8Q = 0 , dr = dτo and U = dr . 2 ... symmetrical in and έ so K F GENERAL STABILITY THEORY IN PLASMA PHYSICS 71.
Page 170
... symmetric near Mo , we have 4. As we move towards the other limit , < 1 ( i.e. , large positive 4 ' ) the eigenvalues that were slightly below move to points slightly above , 3 , .... The fastest growing mode of this series again occurs ...
... symmetric near Mo , we have 4. As we move towards the other limit , < 1 ( i.e. , large positive 4 ' ) the eigenvalues that were slightly below move to points slightly above , 3 , .... The fastest growing mode of this series again occurs ...
Page 171
... symmetric case » where F " 0 at F - 0 . A lower limit to a is set by eq . ( 44a ) . ( 58 ) F12 1 + 1 F2 ) { . 3.3S The ... symmetry or because « 1 . 6. Summary and elucidation of principal results . - In the high - S limit , a current ...
... symmetric case » where F " 0 at F - 0 . A lower limit to a is set by eq . ( 44a ) . ( 58 ) F12 1 + 1 F2 ) { . 3.3S The ... symmetry or because « 1 . 6. Summary and elucidation of principal results . - In the high - S limit , a current ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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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 electrons and ions electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ KRUSKAL l'axe magnétique limit Liouville function 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 region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity x₁ zero zero-order Απ