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

### From inside the book

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Page 108

muir's saturation current (3.6) I+ = ... R."." calculated at the boundary of the

.1). it is necessary to know the temperature close to the boundary (s) of the

muir's saturation current (3.6) I+ = ... R."." calculated at the boundary of the

**contraction**region (s). 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**...Page 112

We claim that the

simply from the application of the physical laws of electrodynamics, statistical

mechanics and quantum mechanics to our problem. To prove this assertion we

make ...

We claim that the

**contraction**itself and the extension of the**contraction**followssimply from the application of the physical laws of electrodynamics, statistical

mechanics and quantum mechanics to our problem. To prove this assertion we

make ...

Page 115

The essential feature is, that in any case a point of intersection occurs in the

range of weak end

point which belongs to extreme

O1) is ...

The essential feature is, that in any case a point of intersection occurs in the

range of weak end

**contraction**(R, R & 1). In addition we have only one other E-point which belongs to extreme

**contraction**. The point with very little**contraction**(O1) is ...

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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