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

### From inside the book

Results 1-3 of 53

Page 191

... plasma may be

4.14), the background waves parallel to ... (4.17) to the dispersion relation is

much less than that

].

... plasma may be

**obtained**on a one-dimensional model, whereas, according to (4.14), the background waves parallel to ... (4.17) to the dispersion relation is

much less than that

**obtained**in linear theory based on the Boltzmann equation [5].

Page 212

If we pick out the contribution to (A-6.6) involving exp [-ior t|, we

ior C (11.1 : C (11.1 . , C (11.1 A-6.16 — k", l. – ik k, k, , -" + ik, , -" — ( ) C2 Li “ril at

a "ria "old ar, * &r, 6'a 6'a 6'a - - - _l * ---> 1.-- L1 - L1 – io), k, k, , , – '' – icok, k + ...

If we pick out the contribution to (A-6.6) involving exp [-ior t|, we

**obtain**~ 1 2 I pI –ior C (11.1 : C (11.1 . , C (11.1 A-6.16 — k", l. – ik k, k, , -" + ik, , -" — ( ) C2 Li “ril at

a "ria "old ar, * &r, 6'a 6'a 6'a - - - _l * ---> 1.-- L1 - L1 – io), k, k, , , – '' – icok, k + ...

Page 263

Returning once again to the substitution of (2) into (1), from the terms involving

exp [in Cse] (n > 2) we

determined is not an eigenvalue of the homogeneous equation for R,

from (14) by ...

Returning once again to the substitution of (2) into (1), from the terms involving

exp [in Cse] (n > 2) we

**obtain**(14) n°C*R, - no ... Since Č as previouslydetermined is not an eigenvalue of the homogeneous equation for R,

**obtained**from (14) by ...

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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