Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
From inside the book
Results 1-3 of 22
Page 97
More important we consider the plasma under the actual experimental conditions
, that means the qualities of the circuit and the boundary conditions of the
electrodes and the container walls enter our calculations. In other words:
whereas the ...
More important we consider the plasma under the actual experimental conditions
, that means the qualities of the circuit and the boundary conditions of the
electrodes and the container walls enter our calculations. In other words:
whereas the ...
Page 235
(1) shows the appearance of two boundary layers, corresponding to the two
boundary conditions (e.g. y(–1) = y(1) = 1). In our example one of them is absent,
having chosen the left boundary condition to fit the fundamental solution yo–0.
(1) shows the appearance of two boundary layers, corresponding to the two
boundary conditions (e.g. y(–1) = y(1) = 1). In our example one of them is absent,
having chosen the left boundary condition to fit the fundamental solution yo–0.
Page 236
The theorem says then that a solution a (t, e) of (7) for fixed initial conditions
converges uniformly for e -- 0 to a solution ... of some uniformly convergent
solutions, which in practice correspond to good y boundary conditions; but the
physicist is, ...
The theorem says then that a solution a (t, e) of (7) for fixed initial conditions
converges uniformly for e -- 0 to a solution ... of some uniformly convergent
solutions, which in practice correspond to good y boundary conditions; but the
physicist is, ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
LEZIONI | 1 |
carrier mass | 159 |
hydrodynamique au voisinage dun axe magnétique | 214 |
Copyright | |
2 other sections not shown
Other editions - View all
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 |