Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 126
For a fictitious gas with quantities similar to oxygen, we evaluated as well the
eigenvalues E, yo = n_o|neo, Zo = m los m.o., as the radial electron density
distribution n(r) for various values of the experimental parameters. 5 4 - w w - \ - \ .
o-2 s' ...
For a fictitious gas with quantities similar to oxygen, we evaluated as well the
eigenvalues E, yo = n_o|neo, Zo = m los m.o., as the radial electron density
distribution n(r) for various values of the experimental parameters. 5 4 - w w - \ - \ .
o-2 s' ...
Page 133
this is again an eigenvalue problem which defines a whole set of functions and
the eigenvalues à). We should remember that in general both eigenfunctions and
the eigenvalue itself may be complex quantities. If we had solved this problem ...
this is again an eigenvalue problem which defines a whole set of functions and
the eigenvalues à). We should remember that in general both eigenfunctions and
the eigenvalue itself may be complex quantities. If we had solved this problem ...
Page 170
(For other reasonable choices of 0), o 0 the A-spectrum is modified only slightly.)
In the limit x > 1, which according to eq. (23) corresponds to large negative A', we
find that the eigenvalues A lie slightly below the points , 3, 3, .... For the fastest ...
(For other reasonable choices of 0), o 0 the A-spectrum is modified only slightly.)
In the limit x > 1, which according to eq. (23) corresponds to large negative A', we
find that the eigenvalues A lie slightly below the points , 3, 3, .... For the fastest ...
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Contents
LEZIONI | 1 |
carrier mass | 159 |
hydrodynamique au voisinage dun axe magnétique | 214 |
Copyright | |
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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