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

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Page 160

... infinite-conductivity case, and where generalizations to nonplanar

an be introduced as desired. In Section 2 of this paper we derive the basis

equations. In Section

modes.

... infinite-conductivity case, and where generalizations to nonplanar

**geometry**'an be introduced as desired. In Section 2 of this paper we derive the basis

equations. In Section

**3**we demonstrate some general properties of the unstablemodes.

Page 211

The summation is over all vectors k permitted by the

all pairs of values of the polarization vector e. We now anticipate ... It follows from

(A-6.9) that (A-6.12) k} =

...

The summation is over all vectors k permitted by the

**geometry**of the model andall pairs of values of the polarization vector e. We now anticipate ... It follows from

(A-6.9) that (A-6.12) k} =

**3**o - - We mow assume that solutions of the eqs. (A-6.5)...

Page 241

and, as it was done by FRIEMAN and SANDRI [

expansion methods where also the time scale is ... The

of charges by a small electrode in a very strong magnetic field. where a is the

Larmor ...

and, as it was done by FRIEMAN and SANDRI [

**3**], can be discussed byexpansion methods where also the time scale is ... The

**geometry**of the collectionof charges by a small electrode in a very strong magnetic field. where a is the

Larmor ...

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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