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

### From inside the book

Results 1-3 of 25

Page 3

[V p_—j x B] + [E -i- VX B) – m j = 0 , where ; m— |ne- nel 'J - no | F_+ F. - A more

formal treatment of the relation between the microscopic and the macroscopic

can be effected by employing a

...

[V p_—j x B] + [E -i- VX B) – m j = 0 , where ; m— |ne- nel 'J - no | F_+ F. - A more

formal treatment of the relation between the microscopic and the macroscopic

can be effected by employing a

**distribution function**f; a quantity which describes...

Page 21

By selecting as a zero-order distribution the Maxwellian, this is also valid for slow

motions in strong fields. The

where Dfo = 06fisop so that 1. 5 m f = , so (*- }) c × b : V log T – FT (exo-a-v ...

By selecting as a zero-order distribution the Maxwellian, this is also valid for slow

motions in strong fields. The

**distribution function**is written as f = fo -i- f| + f2,where Dfo = 06fisop so that 1. 5 m f = , so (*- }) c × b : V log T – FT (exo-a-v ...

Page 49

V. – Correlation Functions and Scattering of Radiation from a Plasma. 1. – The

correlation functions in a plasma. ... exp [iot] ôv, Having the (space-dependent)

perturbation induced in the

particle ...

V. – Correlation Functions and Scattering of Radiation from a Plasma. 1. – The

correlation functions in a plasma. ... exp [iot] ôv, Having the (space-dependent)

perturbation induced in the

**distribution function**by the potential of a chargedparticle ...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

LEZIONI | 1 |

carrier mass | 159 |

hydrodynamique au voisinage dun axe magnétique | 214 |

Copyright | |

2 other sections not shown

### Other editions - View all

### 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