## Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |

### From inside the book

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Page 97

More important we consider the plasma under the actual experimental conditions

, that means the qualities of the circuit and 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 theelectrodes 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

having chosen the left

(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

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 thephysicist is, ...

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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