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

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Page 149

We note that for k” X vo; yo/(kåp)*, the only possible root is vo = (x,a)—the pure

nm, c* and k2(k2%) B2 1 —- - - - - - - = − S 1. y? 4tnmovi, p X Thus we need only ...

We note that for k” X vo; yo/(kåp)*, the only possible root is vo = (x,a)—the pure

**electrostatic**mode in which Elk. If we put v - (2, , |- *, we find (oys, " ... 1, oth i 47nm, c* and k2(k2%) B2 1 —- - - - - - - = − S 1. y? 4tnmovi, p X Thus we need only ...

Page 197

The discussion of the coupling between

in plasmas may be regarded as typical of the phenomenon of modecoupling

which is a consequence of nonlinearity of wave equations. Coupling between

other ...

The discussion of the coupling between

**electrostatic**and electromagnetic wavesin plasmas may be regarded as typical of the phenomenon of modecoupling

which is a consequence of nonlinearity of wave equations. Coupling between

other ...

Page 241

which I have worked out in detail. It concerns the theory of charge-collection by

an electrode whose size is larger than the Larmor radius of the collected particles

, ...

**Electrostatic**probe in a strong magnetic field. We will consider now an examplewhich I have worked out in detail. It concerns the theory of charge-collection by

an electrode whose size is larger than the Larmor radius of the collected particles

, ...

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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