Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 38
... orthogonal to g , i.e. ef . ( III.1.6 ) , hence fa2 kk 8 ( k1g ) = ( 1 − 88 ) = w , π g 2 Dis m 2π * log log Afd3v ' wt ( v ' ) · fæ w¡¡f ( v ' ) . Now , using the relations displayed between the integrals , the F.P.E. may be written ...
... orthogonal to g , i.e. ef . ( III.1.6 ) , hence fa2 kk 8 ( k1g ) = ( 1 − 88 ) = w , π g 2 Dis m 2π * log log Afd3v ' wt ( v ' ) · fæ w¡¡f ( v ' ) . Now , using the relations displayed between the integrals , the F.P.E. may be written ...
Page 63
... orthogonal Jes . 5 QEn ' Em dt = 0 if wn wn . Proof ( w ) plane impossible Fig . 4 . ( w- — cm ) | Q5nm dt = | ( En · F ( Em ) — Em · F ( En ) ) dt = 0 . - [ √ ( 52 · · = We assume that the E are chosen orthogonal for equal on's also ...
... orthogonal Jes . 5 QEn ' Em dt = 0 if wn wn . Proof ( w ) plane impossible Fig . 4 . ( w- — cm ) | Q5nm dt = | ( En · F ( Em ) — Em · F ( En ) ) dt = 0 . - [ √ ( 52 · · = We assume that the E are chosen orthogonal for equal on's also ...
Page 261
... orthogonal to B is ( E × B ) / B2 , which is well known . From ( 3 ) trivially follows ( 4 ) E.B = ( ( ε ) , which is a condition not so much on the trajectory as on the given fields . Since physically E and B seem independent of ε ...
... orthogonal to B is ( E × B ) / B2 , which is well known . From ( 3 ) trivially follows ( 4 ) E.B = ( ( ε ) , which is a condition not so much on the trajectory as on the given fields . Since physically E and B seem independent of ε ...
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