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

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Page 193

Coupling of

section, we considered the coupling of electrostatic waves among themselves

and found that the coupling occurs basically in groups of four waves. In this

section, we ...

Coupling of

**plasma oscillations**and electromagnetic waves. In the previoussection, we considered the coupling of electrostatic waves among themselves

and found that the coupling occurs basically in groups of four waves. In this

section, we ...

Page 194

In some problems, it would be convenient to follow the amplitudes of the

rather than of time. This approach is appropriate, for instance, in the study of ...

In some problems, it would be convenient to follow the amplitudes of the

**plasma****oscillations**and electromagnetic waves as functions of the spatial co-ordinatesrather than of time. This approach is appropriate, for instance, in the study of ...

Page 195

where r, is the phase velocity of the

modulation of the

electron plasma. For parameters appropriate to a laboratory experiment, L would

...

where r, is the phase velocity of the

**plasma oscillations**and D is the « depth ofmodulation of the

**plasma oscillations**, i.e. the fractional change in density of theelectron plasma. For parameters appropriate to a laboratory experiment, L would

...

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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