Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 75
F" can no longer be taken arbitrarily as a function of t, r, w, q as one would
conclude from the zeroth order equation, but must be taken to solve ... These
equations suggest an alternative way to obtain the Boltzmann equation to lowest
order.
F" can no longer be taken arbitrarily as a function of t, r, w, q as one would
conclude from the zeroth order equation, but must be taken to solve ... These
equations suggest an alternative way to obtain the Boltzmann equation to lowest
order.
Page 78
Hence we must proceed to zeroth order in (16) to find ČEsőt (strictly speaking (16
) is three equations). ... These equations which form the system include all of the
Boltzmann and Maxwell equations each to their lowest order. (16), and (16), are ...
Hence we must proceed to zeroth order in (16) to find ČEsőt (strictly speaking (16
) is three equations). ... These equations which form the system include all of the
Boltzmann and Maxwell equations each to their lowest order. (16), and (16), are ...
Page 263
Carrying out the derivation of (6) to the next order gives (13) F = R, VE -- R, X B --
R, X (R, WB) – & R, -2C R, + O(e). This together with (12) gives to lowest order a
first-order differential equation for R, . Since R, has already been determined up ...
Carrying out the derivation of (6) to the next order gives (13) F = R, VE -- R, X B --
R, X (R, WB) – & R, -2C R, + O(e). This together with (12) gives to lowest order a
first-order differential equation for R, . Since R, has already been determined up ...
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Contents
LEZIONI | 1 |
carrier mass | 159 |
hydrodynamique au voisinage dun axe magnétique | 214 |
Copyright | |
2 other sections not shown
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Common terms and phrases
adiabatic invariant amplitude approximation assumed Boltzmann equation boundary conditions boundary layer calculated cathode charge coefficient collision components consider const constant contraction corresponds courbe critère current density Debye length derived differential equations discharge dispersion relation distribution function dºr eigenvalue electric field electromagnetic waves electrostatic energy principle equations of motion equilibrium exp i(k exp ioctl exp ior experimental finite fluid theory frequency given Hence instability integral interaction ioctl ionized KRUSKAL l'axe magnétique lignes limit lowest order magnetic field Maxwell's equations negative ions nonlinear obtain parameter particle perturbation Phys plasma oscillations Plasma Physics Poisson's equation potential problem quantities radial region satisfied saturation current ſº solution solving stabilité stability surface temperature thermal tion values vanish variables vector velocity voisinage waves in plasmas zero zero-order
Bibliographic information
| Title | Proceedings of the International School of Physics "Enrico Fermi.", Volume 25 Proceedings of the International School of Physics "Enrico Fermi.", Società italiana di fisica Rivista del nuovo cimento |
| Contributor | Società italiana di fisica |
| Publisher | N. Zanichelli, 1953 |
| Original from | the University of California |
| Digitized | 13 Nov 2008 |
| Export Citation | BiBTeX EndNote RefMan |