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

### From inside the book

Results 1-3 of 6

Page xi

In addition to these

discussed by R. KULSRUD following two important papers by KULSRUD himself

and M. KRUSKAL. They are reprinted 6 in extenso ). Further seminars on

specialized ...

In addition to these

**formal**lectures the theory of adiabatic invariants wasdiscussed by R. KULSRUD following two important papers by KULSRUD himself

and M. KRUSKAL. They are reprinted 6 in extenso ). Further seminars on

specialized ...

Page 3

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

can be effected by employing a distribution function f; a quantity which describes

...

[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 macroscopiccan be effected by employing a distribution function f; a quantity which describes

...

Page 240

The theory of orbits in a strong magnetic field is based on a

powers of m/e [8], the coefficient of the acceleration. The drift motion is then

determined only by four initial data (position and longitudinal velocity) instead of

six.

The theory of orbits in a strong magnetic field is based on a

**formal**expansion inpowers of m/e [8], the coefficient of the acceleration. The drift motion is then

determined only by four initial data (position and longitudinal velocity) instead of

six.

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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