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

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Page 9

Transport Processes in Fully

ed equations. When instead of a simple gas, an

considered several new complications arise, many of which may be clarified by a

...

Transport Processes in Fully

**Ionized**Gases - Normal Solutions. 1. – The lineari:ed equations. When instead of a simple gas, an

**ionized**gas in a magnetic field isconsidered several new complications arise, many of which may be clarified by a

...

Page 21

... and differential equations are obtained for the time-dependence of the

moments. This method has been applied to the

by Lyley and Herdan; it is not noticeably simpler than the normal solution

procedure. 6.

... and differential equations are obtained for the time-dependence of the

moments. This method has been applied to the

**ionized**plasma by Kolodner, andby Lyley and Herdan; it is not noticeably simpler than the normal solution

procedure. 6.

Page 121

Different production mechanisms are for instance present in the normal glow

column (electron collisions) and in the contact-

hollow cathode discharge (external production). Different destruction processes ...

Different production mechanisms are for instance present in the normal glow

column (electron collisions) and in the contact-

**ionized**cesium discharge and thehollow cathode discharge (external production). Different destruction processes ...

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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