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

### From inside the book

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Page 6

... interaction integral does not vanish, but leads to terms representing the transfer

of energy and momentum between the two components. Alternatively these

equations may be combined and as in Section 1, the mean velocity may be

... interaction integral does not vanish, but leads to terms representing the transfer

of energy and momentum between the two components. Alternatively these

equations may be combined and as in Section 1, the mean velocity may be

**defined**...Page 78

[(16), means the perpendicular part of (16), the parallel part is actually (24)] (11)

is an equation for F", (15) for B, (16), for E, and (24) for E, . In (11), o, n, and e

occur. These are

which is ...

[(16), means the perpendicular part of (16), the parallel part is actually (24)] (11)

is an equation for F", (15) for B, (16), for E, and (24) for E, . In (11), o, n, and e

occur. These are

**defined**by (3), B||B and eE, respectively. In (16), , j, occurswhich is ...

Page 239

... be to arrive at its

discontinuous transition between the sheath and the rest ... be

conveniently used in the calculation BOUND ARY LAYER PROBLEMS IN

PLASMA PHYSICS 239.

... be to arrive at its

**definition**and its explicit calculation: and assume adiscontinuous transition between the sheath and the rest ... be

**defined**andconveniently used in the calculation BOUND ARY LAYER PROBLEMS IN

PLASMA PHYSICS 239.

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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