Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 97
... initial and boundary conditions , our analysis - using these solutions - will be governed just by these initial and boundary conditions . This produces two consequences : first , since we have an infinite number of possible initial and ...
... initial and boundary conditions , our analysis - using these solutions - will be governed just by these initial and boundary conditions . This produces two consequences : first , since we have an infinite number of possible initial and ...
Page 139
... initial distribution fo . In other words , any departure from the initial state increases the kinetic energy of the system . Any electric and magnetic fields which may develop must also increase the energy , since the original constant ...
... initial distribution fo . In other words , any departure from the initial state increases the kinetic energy of the system . Any electric and magnetic fields which may develop must also increase the energy , since the original constant ...
Page 257
... initial region with a displacement 。 and zero velocity . The initial conditions on W and S are chosen such that W is constant throughout the initial region . From eqs . ( 3 ) , ( 4 ) , ( 7 ) and ( 9 ) . ( 10 ) ( 11 ) ( 12 ) S = ± w ...
... initial region with a displacement 。 and zero velocity . The initial conditions on W and S are chosen such that W is constant throughout the initial region . From eqs . ( 3 ) , ( 4 ) , ( 7 ) and ( 9 ) . ( 10 ) ( 11 ) ( 12 ) S = ± w ...
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