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

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Page 38

In the dominant

become (III.4.4) 1. dog daioi go! (v +gologA, 4 ov 2 (III.4.5) }Josia kko(kg)f(p +g) #

log. - Note that (III.4.4) = 6/6 v . (III.4.5), ... (eism,)E = – 6/6 v. D, whilein (III.4.4) the

...

In the dominant

**approximation**only this term is retained; and the integralsbecome (III.4.4) 1. dog daioi go! (v +gologA, 4 ov 2 (III.4.5) }Josia kko(kg)f(p +g) #

log. - Note that (III.4.4) = 6/6 v . (III.4.5), ... (eism,)E = – 6/6 v. D, whilein (III.4.4) the

...

Page 97

Consequently in a course on the theory of the plasma you will expect that one

model, namely an unbounded many-particle system consisting of an electron, ion

and neutral particle component, is treated in various mathematical

Consequently in a course on the theory of the plasma you will expect that one

model, namely an unbounded many-particle system consisting of an electron, ion

and neutral particle component, is treated in various mathematical

**approximations**...Page 244

The role played by the two

show that the collected current density, for an arbitrary value of the parameter x (

see (21)) is co (29) j=on.sd5 exp [- st($)], where the t|5) is the time that a particle ...

The role played by the two

**approximation**to q becomes then apparent. One canshow that the collected current density, for an arbitrary value of the parameter x (

see (21)) is co (29) j=on.sd5 exp [- st($)], where the t|5) is the time that a particle ...

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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