Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 20
Page 192
... vector k + k1 · We shall not here attempt exact evaluation of the sum in ( 4.18 ) , but merely estimate the magnitude of the effect . For this purpose , we note that if ( is the mean square value of the « background » wave vectors , k2 ...
... vector k + k1 · We shall not here attempt exact evaluation of the sum in ( 4.18 ) , but merely estimate the magnitude of the effect . For this purpose , we note that if ( is the mean square value of the « background » wave vectors , k2 ...
Page 193
... vector parallel to k ,, e , is the polarization vector normal to k ,, which may be given two values for each wave vector , and or satisfies the dispersion relation ( 5.3 ) w1 = w2 + c2 k2 . Two distinct types of coupling are possible in ...
... vector parallel to k ,, e , is the polarization vector normal to k ,, which may be given two values for each wave vector , and or satisfies the dispersion relation ( 5.3 ) w1 = w2 + c2 k2 . Two distinct types of coupling are possible in ...
Page 211
where 1 , is the unit vector parallel to k ,, e , is the unit polarization vector normal to k ,, or is the plasma frequency and o , satisfies the dispersion relation ( A - 6.9 ) or = w2 + c2 k2 . The summation is over all vectors k ...
where 1 , is the unit vector parallel to k ,, e , is the unit polarization vector normal to k ,, or is the plasma frequency and o , satisfies the dispersion relation ( A - 6.9 ) or = w2 + c2 k2 . The summation is over all vectors k ...
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