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

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Page 21

... I = I(f", q) and q = filfo, and the problem is then reduced to that of

integrals appearing in I. There is a happy agreement between transport

coefficients

Marshall.

... I = I(f", q) and q = filfo, and the problem is then reduced to that of

**calculating**theintegrals appearing in I. There is a happy agreement between transport

coefficients

**calculated**this way and the strong field limits of those**calculated**byMarshall.

Page 33

that the electric field within the plasma is weak, and the interactions are small. At

the same time, the effect of the field on the distribution function must be retained

in ...

**Calculation**of the spectrum. - To**calculate**the spectrum we can again assumethat the electric field within the plasma is weak, and the interactions are small. At

the same time, the effect of the field on the distribution function must be retained

in ...

Page 107

The effect

roughness (B), however in distinction to B it is a completely fundamental and

general effect and does not depend on special experimental conditions. Using a

...

The effect

**calculated**in this way resembles somewhat the influence of surfaceroughness (B), however in distinction to B it is a completely fundamental and

general effect and does not depend on special experimental conditions. Using a

...

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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