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

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Page 39

C 6v m ov where now the

form v, 6 6,(1921 (? and *, *, *), ôr, ri – r. c Ör, |ri – rel the first representing electric

and the second magnetic

C 6v m ov where now the

**interaction**forces Fis include, in general, terms of theform v, 6 6,(1921 (? and *, *, *), ôr, ri – r. c Ör, |ri – rel the first representing electric

and the second magnetic

**interactions**. Note that the ratio of the 2nd to the 1st is ...Page 189

In Appendices III, IV and V, two distinct techniques are developed for evaluating

the nonlinear

extracted from these calculations, but will not be discussed here. The more ...

In Appendices III, IV and V, two distinct techniques are developed for evaluating

the nonlinear

**interaction**by perturbation methods. The harmonic content can beextracted from these calculations, but will not be discussed here. The more ...

Page 208

this term would represent the dominant wave

zero-frequency term, this certainly contributes to the dominant

must also consider the possibility that Ho gives rise to a wave-

...

this term would represent the dominant wave

**interaction**. Since H* contains azero-frequency term, this certainly contributes to the dominant

**interaction**, but onemust also consider the possibility that Ho gives rise to a wave-

**interaction**process...

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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