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

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Page 98

select certain discharge types which we choose to consider in this course;

secondly, under the influence of the boundary conditions the

will present itself not as a uniform

model ...

select certain discharge types which we choose to consider in this course;

secondly, under the influence of the boundary conditions the

**region**of interestwill present itself not as a uniform

**region**, but as composed of various differentmodel ...

Page 99

In these cathodic parts there is a mutual production of electrons at the cathode

surface by impinging ions and ions in the negative glow by electrons accelerated

through the cathode-fall

...

In these cathodic parts there is a mutual production of electrons at the cathode

surface by impinging ions and ions in the negative glow by electrons accelerated

through the cathode-fall

**region**. In the column particles are produced by electron...

Page 257

Let us assume that the oscillator is started in the initial

a, and zero velocity. The initial conditions on W and S are chosen such that W is

constant throughout the initial

Let us assume that the oscillator is started in the initial

**region**with a displacementa, and zero velocity. The initial conditions on W and S are chosen such that W is

constant throughout the initial

**region**. From eqs. (3), (4), (7) and (9). (10) S = + ...### What people are saying - Write a review

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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