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

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Page 35

turbation which is adiabatically switched on, or considering a model of residual

collision process as in (II.4.1), all lead to the conclusion that, with Ps = Cauchy

principle value, - - — or f t - t (III.3.8) sa," – so," ano-so",

turbation which is adiabatically switched on, or considering a model of residual

collision process as in (II.4.1), all lead to the conclusion that, with Ps = Cauchy

principle value, - - — or f t - t (III.3.8) sa," – so," ano-so",

**hence**e is complex.Page 138

phase. We would not expect then that these microinstabilities would lead to a

gross disassembly of the plasma such as occurs for example in the

hydromagnetic ...

**Hence**, such instabilities do not remain for long in the exponentially growingphase. We would not expect then that these microinstabilities would lead to a

gross disassembly of the plasma such as occurs for example in the

hydromagnetic ...

Page 154

encircled, may be decided by looking at Re F at a) = 0 and o = co. At 0) = co, Re F

= — (kān)”, i.e., Re F * 0. At 0) = 0, Re F = (yse) ln to , i.e., Re Fox 0.

**Hence**Im F = 0 only at to - 0 and the question of stability i.e. whether the origin isencircled, may be decided by looking at Re F at a) = 0 and o = co. At 0) = co, Re F

= — (kān)”, i.e., Re F * 0. At 0) = 0, Re F = (yse) ln to , i.e., Re Fox 0.

**Hence**the ...### 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 | |

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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