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

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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 116

If the phenomenon of the arc without cathode spot had not already been

observed, we would have to infer it from the

quite clearly we repeat in Fig. 13 the curves of Fig. 10 which are essential for our

...

If the phenomenon of the arc without cathode spot had not already been

observed, we would have to infer it from the

**calculations**. To indicate the processquite clearly we repeat in Fig. 13 the curves of Fig. 10 which are essential for our

...

Page 239

They usually start from the concept of sheath thickness, while the main task of the

theory should be to arrive at its definition and its explicit

a discontinuous transition between the sheath and the rest of the plasma.

They usually start from the concept of sheath thickness, while the main task of the

theory should be to arrive at its definition and its explicit

**calculation**: and assumea discontinuous transition between the sheath and the rest of the plasma.

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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