Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 188
... variables are appropriate for setting up an action principle to describe the behavior of the plasma . By introducing a Green function to characterize the ... variables . In linear theory , the variables a ( k , 188 P. A. STURROCK.
... variables are appropriate for setting up an action principle to describe the behavior of the plasma . By introducing a Green function to characterize the ... variables . In linear theory , the variables a ( k , 188 P. A. STURROCK.
Page 189
In linear theory , the variables a ( k , t ) are in fact independent of time . When nonlinear terms of the equations of motion are taken into account , it is found that the resulting modification of the dynamical variables may be ...
In linear theory , the variables a ( k , t ) are in fact independent of time . When nonlinear terms of the equations of motion are taken into account , it is found that the resulting modification of the dynamical variables may be ...
Page 206
... variables P ,, Q , and a new Hamiltonian H ( P ,, Q ,, t ) . We consider the transformation of variables to be expressible in the form ( A - 4.2 ) p1 = P1 + ~ P ; + ☎2 P11 + ... Pr = qr = Qr + õQ ; + ☎2Qμ + wherein P etc. are to be ...
... variables P ,, Q , and a new Hamiltonian H ( P ,, Q ,, t ) . We consider the transformation of variables to be expressible in the form ( A - 4.2 ) p1 = P1 + ~ P ; + ☎2 P11 + ... Pr = qr = Qr + õQ ; + ☎2Qμ + wherein P etc. are to be ...
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