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

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Page 126

For a fictitious gas with quantities similar to oxygen, we evaluated as well the

axial positive ion density (zo = n +o/meo) as calculated from the

problem.

For a fictitious gas with quantities similar to oxygen, we evaluated as well the

**eigenvalues**E, yo = n_o|neo, Zo = m los m.o. ... ions (yo– m -o/neo) and relativeaxial positive ion density (zo = n +o/meo) as calculated from the

**eigenvalue**problem.

Page 133

this is again an

the

the

this is again an

**eigenvalue**problem which defines a whole set of functions andthe

**eigenvalues**à). We should remember that in general both eigenfunctions andthe

**eigenvalue**itself may be complex quantities. If we had solved this problem ...Page 170

(For other reasonable choices of 0), o 0 the A-spectrum is modified only slightly.)

In the limit x > 1, which according to eq. (23) corresponds to large negative A', we

find that the

(For other reasonable choices of 0), o 0 the A-spectrum is modified only slightly.)

In the limit x > 1, which according to eq. (23) corresponds to large negative A', we

find that the

**eigenvalues**A lie slightly below the points , 3, 3, .... For the fastest ...### What people are saying - Write a review

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### Contents

LEZIONI | 1 |

carrier mass | 159 |

hydrodynamique au voisinage dun axe magnétique | 214 |

Copyright | |

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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