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

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Page 234

method to solve a wide class of problems which often occur in plasma theory, as

well as in many other branches of physics; an introduction will be given to the ...

**Boundary layer**problems. The purpose of these lectures is to point out a generalmethod to solve a wide class of problems which often occur in plasma theory, as

well as in many other branches of physics; an introduction will be given to the ...

Page 237

has a solution y = y,(a) which fulfils the second boundary condition. The first

theorem ... One can say, therefore, the appearance of a

put at the door of a violent 9, though very probable, choice of a boundary

condition.

has a solution y = y,(a) which fulfils the second boundary condition. The first

theorem ... One can say, therefore, the appearance of a

**boundary layer**is to beput at the door of a violent 9, though very probable, choice of a boundary

condition.

Page 239

A more accurate approximation in the

expansion of w(ar, e) in e, for more details and a far reaching generalization of

this method, see [3]. In the case of eqs. (5) and (2) the

reads ...

A more accurate approximation in the

**boundary layer**could be provided by anexpansion of w(ar, e) in e, for more details and a far reaching generalization of

this method, see [3]. In the case of eqs. (5) and (2) the

**boundary layer**eq. (11)reads ...

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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