Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 75
... order equation , but must be taken to solve ( 11 ) . Incidentally we know that ( 12 ) Fo Fo Fo + r · ▽ Fo + ŵ + ġ ... lowest order in 1 / e . The right - hand side of these equations represent the time derivatives averaged over a ...
... order equation , but must be taken to solve ( 11 ) . Incidentally we know that ( 12 ) Fo Fo Fo + r · ▽ Fo + ŵ + ġ ... lowest order in 1 / e . The right - hand side of these equations represent the time derivatives averaged over a ...
Page 78
... order in ( 16 ) to find E / et ( strictly speaking ( 16 ) is three equations ) . The component parallel to n is ... lowest order . ( 16 ) and ( 16 ) , are of different orders of course . ( 17 ) is taken to minus first and zeroth order ...
... order in ( 16 ) to find E / et ( strictly speaking ( 16 ) is three equations ) . The component parallel to n is ... lowest order . ( 16 ) and ( 16 ) , are of different orders of course . ( 17 ) is taken to minus first and zeroth order ...
Page 264
... order differential equation involving R , and R1 . It may be noted that ( 17 ) can be integrated explicitly to lowest order yielding ( 18 ) | R12B = k + O ( ɛ ) , where k is a constant . This exhibits the well - known lowest - order ...
... order differential equation involving R , and R1 . It may be noted that ( 17 ) can be integrated explicitly to lowest order yielding ( 18 ) | R12B = k + O ( ɛ ) , where k is a constant . This exhibits the well - known lowest - order ...
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