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

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Page 165

0,. must be satisfied everywhere except in a small interval. The general

procedure in the S → co, 0 < y < 1 limit is therefore as follows. We obtain

solutions to eq. (20) that

solutions cannot, in ...

0,. must be satisfied everywhere except in a small interval. The general

procedure in the S → co, 0 < y < 1 limit is therefore as follows. We obtain

solutions to eq. (20) that

**vanish**at u = u, , u, , the external boundaries. Thesesolutions cannot, in ...

Page 254

That the magnetic moment of the particle is a constant in all orders would imply

that any change in it must

smallness, i.e., the relative change of the field over the Larmor radius. This does ...

That the magnetic moment of the particle is a constant in all orders would imply

that any change in it must

**vanish**more rapidly than any power of the parameter ofsmallness, i.e., the relative change of the field over the Larmor radius. This does ...

Page 258

... W. Wo + W. 2 W, -i-... + WoW, . In deriving eq. (19) we have used eq. (17) to

cancel the to term and in eq. (20) we have used the fact that a is independent of T

. Note from the equations corresponding to (19) and (20) that all odd orders

... W. Wo + W. 2 W, -i-... + WoW, . In deriving eq. (19) we have used eq. (17) to

cancel the to term and in eq. (20) we have used the fact that a is independent of T

. Note from the equations corresponding to (19) and (20) that all odd orders

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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