Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 67
... oscillator with negative spring constant and moving in field B to its plane ( see Fig . 7 ) . The potential energy isk . Let the oscillator have a charge e . If √km ( eB / me ) the system is stable although W < 0 always . 4 Fig . 7 . B ...
... oscillator with negative spring constant and moving in field B to its plane ( see Fig . 7 ) . The potential energy isk . Let the oscillator have a charge e . If √km ( eB / me ) the system is stable although W < 0 always . 4 Fig . 7 . B ...
Page 254
... /2 ] has this behavior since at 2 = 0 all derivatives of Ac vanish , ( ) Reprinted from Phys . Rev. , 106 , 205 ( 1957 ) . An example of an adiabatic invariant in quantum mechanics would Adiabatic invariant of the harmonic oscillator.
... /2 ] has this behavior since at 2 = 0 all derivatives of Ac vanish , ( ) Reprinted from Phys . Rev. , 106 , 205 ( 1957 ) . An example of an adiabatic invariant in quantum mechanics would Adiabatic invariant of the harmonic oscillator.
Page 259
... oscillator when it reaches the discontinuity . N may Ф be either even or odd . REFERENCES [ 1 ] E. FERMI : Phys . Rev. , 75 , 1169 ( 1949 ) . [ 2 ] L. SPITZER : Astrophys . Journ . , 116 , 299 ( 1952 ) . [ 3 ] H. ALFVÉN : Cosmical ...
... oscillator when it reaches the discontinuity . N may Ф be either even or odd . REFERENCES [ 1 ] E. FERMI : Phys . Rev. , 75 , 1169 ( 1949 ) . [ 2 ] L. SPITZER : Astrophys . Journ . , 116 , 299 ( 1952 ) . [ 3 ] H. ALFVÉN : Cosmical ...
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