Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 12
Page 17
... respect to % , then ( II.4.4 ) δλ = - 2 { [ ( x , Kx ) ¥ — ( 2 , 4 ) Kx ] 2 ( x , y ) ( x , Ky ) 2 which vanishes if ( x , y ) Y - ( x , Kx ) χ satisfies ( II.4.1 ) . By carrying the variation out to 2nd order in 8 % , 2 is shown to be ...
... respect to % , then ( II.4.4 ) δλ = - 2 { [ ( x , Kx ) ¥ — ( 2 , 4 ) Kx ] 2 ( x , y ) ( x , Ky ) 2 which vanishes if ( x , y ) Y - ( x , Kx ) χ satisfies ( II.4.1 ) . By carrying the variation out to 2nd order in 8 % , 2 is shown to be ...
Page 152
... respect to microinstabilities . In particular , we study a low ẞ situation which implies electrostatic instabilities and consider simple localized instabilities . We also choose the simplest geometry : magnetic field in the direction ...
... respect to microinstabilities . In particular , we study a low ẞ situation which implies electrostatic instabilities and consider simple localized instabilities . We also choose the simplest geometry : magnetic field in the direction ...
Page 237
... respect to ɛ ; moreover , they are such that the reduced differential equa- tion ( 10 ) F1 ( x , y , 0 ) y ' + F2 ( x , y , 0 ) = 0 has a solution y = y , ( x ) which fulfils the second boundary condition . The first theorem proves that ...
... respect to ɛ ; moreover , they are such that the reduced differential equa- tion ( 10 ) F1 ( x , y , 0 ) y ' + F2 ( x , y , 0 ) = 0 has a solution y = y , ( x ) which fulfils the second boundary condition . The first theorem proves that ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
3 other sections not shown
Other editions - View all
Common terms and phrases
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