Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 16
... equations are derived for the sepa- rate contributions to e.g. those arising ... equation in ( II.3.8 ) may be reduced to ( II.3.9 ) . The problem of solving ... field , the equation to be solved takes on the form ( II.4.1 ) y ( c ) = K ...
... equations are derived for the sepa- rate contributions to e.g. those arising ... equation in ( II.3.8 ) may be reduced to ( II.3.9 ) . The problem of solving ... field , the equation to be solved takes on the form ( II.4.1 ) y ( c ) = K ...
Page 55
... equations . The basic equations underlying all three theories . will be the Fokker - Planck equation [ 6 ] for the Boltzmann distribution function of each particle and Maxwell's equations for the electromagnetic field . In each of the ...
... equations . The basic equations underlying all three theories . will be the Fokker - Planck equation [ 6 ] for the Boltzmann distribution function of each particle and Maxwell's equations for the electromagnetic field . In each of the ...
Page 172
... field . For a zero - order field that is not a vacuum field , possibilities of lowering po- tential energy are ... equations specifying B and to be solenoidal hold as well for the vector components in the ky - plane taken alone . Thus we have ...
... field . For a zero - order field that is not a vacuum field , possibilities of lowering po- tential energy are ... equations specifying B and to be solenoidal hold as well for the vector components in the ky - plane taken alone . Thus we have ...
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