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

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Page 99

consists of a cylindrical plasma column and the typical cathodic parts of the glow.

In these cathodic parts there is a mutual production of electrons at the cathode

surface ...

**transition**. region. we have the so-called subnormal glow discharge whichconsists of a cylindrical plasma column and the typical cathodic parts of the glow.

In these cathodic parts there is a mutual production of electrons at the cathode

surface ...

Page 239

In plasma physics every charge sheath problem features two characteristic

lengths, whose ratio is very small: the Debye length and the mean free path for

collisions or ionization. It can be expected, therefore, that the

vacuum or ...

In plasma physics every charge sheath problem features two characteristic

lengths, whose ratio is very small: the Debye length and the mean free path for

collisions or ionization. It can be expected, therefore, that the

**transition**fromvacuum or ...

Page 240

The most interesting one, perhaps, is the

magnetic field—a fundamental problem in the theory of confinement. One

considers a situation where every quantity depends only on as and there is a

magnetic field ...

The most interesting one, perhaps, is the

**transition**between a plasma andmagnetic field—a fundamental problem in the theory of confinement. One

considers a situation where every quantity depends only on as and there is a

magnetic field ...

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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