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

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Page 54

Stability. Theory. in. Plasma. Physics. RUSSEL KULSRUD Princeton Plasma

Physics Laboratory, Princeton University ... We shall designate these three

different approaches by the

adiabatic ...

Stability. Theory. in. Plasma. Physics. RUSSEL KULSRUD Princeton Plasma

Physics Laboratory, Princeton University ... We shall designate these three

different approaches by the

**fluid theory**, the adiabatic theory and the doubleadiabatic ...

Page 55

In the double adiabatic theory a separate equation of state is derived for each of

the two independent components of the stress tensor, with each equation similar

to the simple equation in the

In the double adiabatic theory a separate equation of state is derived for each of

the two independent components of the stress tensor, with each equation similar

to the simple equation in the

**fluid theory**. Thus, since these equations arise from ...Page 91

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

Hence if the

the

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 | |

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