Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 5
... solving ( I.1.10 ) for a given form of I and deducing the moments required for a macroscopic description of phenomena . For diffuse gases in which a strong but localized interaction occurs between the particles , a coarse - grained ...
... solving ( I.1.10 ) for a given form of I and deducing the moments required for a macroscopic description of phenomena . For diffuse gases in which a strong but localized interaction occurs between the particles , a coarse - grained ...
Page 16
... solving this equation is however still sufficiently formidable that recourse is had to a variational pro- cedure which is a suitable modification of that introduced by HIRSCHFELDER et al . for normal gases , and used by Marshall . - 4 ...
... solving this equation is however still sufficiently formidable that recourse is had to a variational pro- cedure which is a suitable modification of that introduced by HIRSCHFELDER et al . for normal gases , and used by Marshall . - 4 ...
Page 177
... solving the equation ( 82 ) 1 d2y hk dy ( k μ Y へん cosh ( hy ) Now using the zero - order pressure - balance condition ( eq . ( 77 ) ) , we find that eq . ( 81 ) reduces to μ = 2h / k . Equation ( 81 ) is then seen to be equivalent to ...
... solving the equation ( 82 ) 1 d2y hk dy ( k μ Y へん cosh ( hy ) Now using the zero - order pressure - balance condition ( eq . ( 77 ) ) , we find that eq . ( 81 ) reduces to μ = 2h / k . Equation ( 81 ) is then seen to be equivalent to ...
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