Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 196
... Hamiltonian nature of the system , we may establish the following relations ( 6.7 ) ( 6.8 ) TS .. rwa + sob 0 , 8Srs roa + swb = 0 . These equations are identical with the equations established by MANLEY and ROWE [ 11 ] for electrical ...
... Hamiltonian nature of the system , we may establish the following relations ( 6.7 ) ( 6.8 ) TS .. rwa + sob 0 , 8Srs roa + swb = 0 . These equations are identical with the equations established by MANLEY and ROWE [ 11 ] for electrical ...
Page 206
... Hamiltonian will in general be expressible as ( A - 4.3 ) = H ÕH1 ÷ Õ2H11 + .... We wish to find a canonical transformation of the above form for which H1 = 0 . The essential properties of the original variables and Hamiltonian are ...
... Hamiltonian will in general be expressible as ( A - 4.3 ) = H ÕH1 ÷ Õ2H11 + .... We wish to find a canonical transformation of the above form for which H1 = 0 . The essential properties of the original variables and Hamiltonian are ...
Page 264
... series of ( nonnegative ) powers of ɛ with coefficients which are functions of 0 and t , periodic in 0 with period 27. From here on the argument proceeds quite generally for any system describable by a Hamiltonian ; it 264 M. KRUSKAL.
... series of ( nonnegative ) powers of ɛ with coefficients which are functions of 0 and t , periodic in 0 with period 27. From here on the argument proceeds quite generally for any system describable by a Hamiltonian ; it 264 M. KRUSKAL.
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