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

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Page 78

The part perpendicular to n is

11) eq. (9) may be solved for f' but not uniquely; only up to a function of t, r, w and

...

The part perpendicular to n is

**zero**order which we use to find El). To proceed to**zero**order in (16) we need J to**zero**order which by (18) involves f". Because of (11) eq. (9) may be solved for f' but not uniquely; only up to a function of t, r, w and

...

Page 132

Since we consider a three-component plasma in a longitudinal magnetic field the

stationary

o = 0 due to the assumption of weak ionization. If the index (0) designates the ...

Since we consider a three-component plasma in a longitudinal magnetic field the

stationary

**zero**-order solution is already given in the preceding chapter if we useo = 0 due to the assumption of weak ionization. If the index (0) designates the ...

Page 208

this term would represent the dominant wave interaction. Since H* contains a

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

...

this term would represent the dominant wave interaction. Since H* contains a

**zero**-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