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

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Page 110

It depends strongly on the value of the end contraction and is found automatically

from the solution of the

preceding paragraph. The result is shown in Fig. 8. The other contribution comes

from ...

It depends strongly on the value of the end contraction and is found automatically

from the solution of the

**problem**of the contraction region described in thepreceding paragraph. The result is shown in Fig. 8. The other contribution comes

from ...

Page 239

to 2 a. is, respectively. The

differential eqs. (10) and (15), each of which is much simpler than original one (8)

. The last theorem by WAsow provides for a rigorous justification of this method. A

more ...

to 2 a. is, respectively. The

**problem**is then reduced to the solution of twodifferential eqs. (10) and (15), each of which is much simpler than original one (8)

. The last theorem by WAsow provides for a rigorous justification of this method. A

more ...

Page 255

In order to approach the

orders, this paper treats another simpler

exists. Consider the classic one-dimensional

spring ...

In order to approach the

**problem**of the constancy of adiabatic invariants to allorders, this paper treats another simpler

**problem**in which an adiabatic invariantexists. Consider the classic one-dimensional

**problem**of an oscillator whosespring ...

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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