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

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Page 189

When

found that the resulting modification of the dynamical variables may be separated

into two parts: a change of « wave-form », which one can represent by the

addition ...

When

**nonlinear**terms of the equations of motion are taken into account, it isfound that the resulting modification of the dynamical variables may be separated

into two parts: a change of « wave-form », which one can represent by the

addition ...

Page 197

We may now review the topics which we have treated in detail, in order to discuss

the extent to which they are typical of plasma phenomena, and to list the various

We may now review the topics which we have treated in detail, in order to discuss

the extent to which they are typical of plasma phenomena, and to list the various

**nonlinear**effects which have so far not been treated. As we have already ...Page 198

Interaction of this type has recently been examined in great detail in connection

with the study of ionospheric densities by the « incoherent backscatter 9 method [

20]. There are certainly many other

...

Interaction of this type has recently been examined in great detail in connection

with the study of ionospheric densities by the « incoherent backscatter 9 method [

20]. There are certainly many other

**nonlinear**phenomana than those which have...

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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