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

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Page 3

If this and a similar equation for A V1 are multiplied by a product of density and

charge there results D; - +- ( 2 2 2 }++ v p + ... The equivalence of Liouville's

equation and the

system is ...

If this and a similar equation for A V1 are multiplied by a product of density and

charge there results D; - +- ( 2 2 2 }++ v p + ... The equivalence of Liouville's

equation and the

**equations of motion**is established by observing that if thesystem is ...

Page 75

where we use ss's dop = w(I — nn) I the unit dyadic, in the first equation, and also

the notation ab:Vc = a- (b. Vc). Combining these results ... Derive (13) directly

from the

to ...

where we use ss's dop = w(I — nn) I the unit dyadic, in the first equation, and also

the notation ab:Vc = a- (b. Vc). Combining these results ... Derive (13) directly

from the

**equations of motion**and use (12) to derive (11). 32. Marwell's equationsto ...

Page 199

the motion of the electron gas is given by the action principle (A-1.2) SS = 0 ,

where 1 65,\* 1 - - ! ... Since $, E=0 is a solution of the

also expect that S" may be ignored, and it may be verified by calculation that S" =

0.

the motion of the electron gas is given by the action principle (A-1.2) SS = 0 ,

where 1 65,\* 1 - - ! ... Since $, E=0 is a solution of the

**equations of motion**, wealso expect that S" may be ignored, and it may be verified by calculation that S" =

0.

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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