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

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Page 54

General. Stability.

Plasma Physics Laboratory, Princeton University - Princeton, N. J. 1. –

Introduction. In this course we shall consider three energy principles for the

stability of static ...

General. Stability.

**Theory**. in. Plasma. Physics. RUSSEL KULSRUD PrincetonPlasma Physics Laboratory, Princeton University - Princeton, N. J. 1. –

Introduction. In this course we shall consider three energy principles for the

stability of static ...

Page 55

The

governed by the magnetic moment being an adiabatic invariant. In the double

adiabatic

independent ...

The

**theory**is designated as adiabatic because the motion of each particle isgoverned by the magnetic moment being an adiabatic invariant. In the double

adiabatic

**theory**a separate equation of state is derived for each of the twoindependent ...

Page 91

But 3W, gives a necessary and sufficient result for stability on the fluid

Hence if the fluid

the fluid

But 3W, gives a necessary and sufficient result for stability on the fluid

**theory**.Hence if the fluid

**theory**gives stability so must the adiabatic**theory**. Thus, we seethe fluid

**theory**gives reliable results even in cases where one would suppose it ...### 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