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

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Results 1-3 of 6

Page 150

Since we are concerned with

R, 31; T. = 1; T.o. - 0. Moreover we see that since u/ru. 31 the argument of the

electron W

Since we are concerned with

**wave**lengths comparable to the ion-gyroradius, k,R, 31; T. = 1; T.o. - 0. Moreover we see that since u/ru. 31 the argument of the

electron W

**function**is very small. Since we are concerned with a**wave**nearly at ...Page 198

This would clearly give rise to a frequency shift between the transmitted 9 and 6

reflected

Construction of the Lagrangian and Hamiltonian

consider is ...

This would clearly give rise to a frequency shift between the transmitted 9 and 6

reflected

**waves**. Interaction of this type has recently ... A PP E N DIX IConstruction of the Lagrangian and Hamiltonian

**functions**. The model which weconsider is ...

Page 208

this term would represent the dominant

transformed variables as bo(k), b(k) and the transformed Hamiltonian as H. Then

we see from Appendix I that the generating

the ...

this term would represent the dominant

**wave**interaction. ... We write thetransformed variables as bo(k), b(k) and the transformed Hamiltonian as H. Then

we see from Appendix I that the generating

**function**U"(b'(k), (k), t) is defined bythe ...

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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