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

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Page 57

(Of course, there are other conditions that must be satisfied in the fluid theory

such as small gyration radius, small

the fluid theory.) Substituting (8') in (5) and (7) and these in (2) we have dW 1.

(Of course, there are other conditions that must be satisfied in the fluid theory

such as small gyration radius, small

**Debye length**, etc. We do not stress these inthe fluid theory.) Substituting (8') in (5) and (7) and these in (2) we have dW 1.

Page 78

Thus, we have attained our goal of determining a system of equations for the

zeroth-order quantities. In these notes we shall work only with lowest order

quantities. In general, these equations are valid if 1) the gyration radius and

Thus, we have attained our goal of determining a system of equations for the

zeroth-order quantities. In these notes we shall work only with lowest order

quantities. In general, these equations are valid if 1) the gyration radius and

**Debye length**...Page 97

A plasma was defined by Langmuir to be a partially ionized gas in which the

course on the theory of the plasma you will expect that one model, namely an ...

A plasma was defined by Langmuir to be a partially ionized gas in which the

**Debye length**is small compared with other lengths of interest. Consequently in acourse on the theory of the plasma you will expect that one model, namely an ...

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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