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

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Page 100

In addition we further define: the electrode

of the arc, respectively, the entire region of the glow in so far as it is influenced by

the presence of the electrodes. That means the entire region within which ...

In addition we further define: the electrode

**components**include the entire regionof the arc, respectively, the entire region of the glow in so far as it is influenced by

the presence of the electrodes. That means the entire region within which ...

Page 102

Electrode

research have produced a vast amount of experimental details about the

behaviour of the electrode

not ...

Electrode

**components**of the arc discharge. Fifty years of intensive experimentalresearch have produced a vast amount of experimental details about the

behaviour of the electrode

**components**of an arc discharge. The material seemsnot ...

Page 172

The reasons for this decoupling effect are readily seen. The co-ordinate along n

is ignorable: therefore, the field lines of the

the perturbation. The only manner in which the magnitude of B, could affect the ...

The reasons for this decoupling effect are readily seen. The co-ordinate along n

is ignorable: therefore, the field lines of the

**component**B, are not distorted duringthe perturbation. The only manner in which the magnitude of B, could affect the ...

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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