## Proceedings of the International School of Physics "Enrico Fermi.", Volume 25 |

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Page 108

To find the particle density (n1), and the average velocity (c.1). it is necessary to

know the

turn requires the evaluation of the energy balance for the whole cathode region

of ...

To find the particle density (n1), and the average velocity (c.1). it is necessary to

know the

**temperature**close to the boundary (s) of the contraction region. This inturn requires the evaluation of the energy balance for the whole cathode region

of ...

Page 113

O The general shape of the curves T.(R) *, 2 corresponds to the curves given in

Fig. (7) and (8). The electrode

currents I 1–1–1–1 l J and gas

dence ...

O The general shape of the curves T.(R) *, 2 corresponds to the curves given in

Fig. (7) and (8). The electrode

**temperature**T.(R) is shown in Fig. 9 for variouscurrents I 1–1–1–1 l J and gas

**temperatures**T.. The depen- * 2 4 6 810 2 . ; : ydence ...

Page 131

But now an additional difficulty arises, since in the case of the fully ionized

column with external particle production we can no longer introduce the

assumption of constant

governed by ...

But now an additional difficulty arises, since in the case of the fully ionized

column with external particle production we can no longer introduce the

assumption of constant

**temperature**. Here the**temperature**of the particles is notgoverned by ...

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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