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

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Page 5

and the general equation of transport for f becomes ôf , ... of , , , of n ° s 6 3. #; +w

... At present we will concentrate on the second problem, that of solving

Hydrodynamic ...

and the general equation of transport for f becomes ôf , ... of , , , of n ° s 6 3. #; +w

... At present we will concentrate on the second problem, that of solving

**Boltzmann's equation**and determining the transport coefficients. 2. –Hydrodynamic ...

Page 55

but the difficulty of solving this equation is reduced by the assumption of small

gyration radius. The equation reduces to a one-dimensional

where the one dimension comprises the position and velocity of a particle along

a ...

but the difficulty of solving this equation is reduced by the assumption of small

gyration radius. The equation reduces to a one-dimensional

**Boltzmann equation**where the one dimension comprises the position and velocity of a particle along

a ...

Page 72

The

collisions and small gyration radius. Therefore we start with the Vlasov or

collisionless

B C of (1) ...

The

**Boltzmann equation**. – The adiabatic theory corresponds to the limit of nocollisions and small gyration radius. Therefore we start with the Vlasov or

collisionless

**Boltzmann equation**for each kind of particle, ions and electrons v ×B C of (1) ...

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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