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

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Page 98

Since each model

discharge problem is much more complex than ... where we have several

interacting model

physical laws.

Since each model

**region**is described by a number of physical laws the gasdischarge problem is much more complex than ... where we have several

interacting model

**regions**governed by a large number of essentially differentphysical laws.

Page 99

cylindrical plasma column and the typical ... surface by impinging ions and ions in

the negative glow by electrons accelerated through the cathode-fall

**region**. we have the so-called subnormal glow discharge which consists of acylindrical plasma column and the typical ... surface by impinging ions and ions in

the negative glow by electrons accelerated through the cathode-fall

**region**.Page 257

Let us assume that the oscillator is started in the initial

a, and zero velocity. The initial conditions on W and S are chosen such that W is

constant throughout the initial

Let us assume that the oscillator is started in the initial

**region**with a displacementa, and zero velocity. The initial conditions on W and S are chosen such that W is

constant throughout the initial

**region**. From eqs. (3), (4), (7) and (9). (10) S = + ...### What people are saying - Write a review

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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