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

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Page 75

These equations suggest an alternative way to obtain the Boltzmann equation to

derive (11). 32. Marwell's equations to zero order. – Equation (11) gives F. in

terms ...

These equations suggest an alternative way to obtain the Boltzmann equation to

**lowest order**. Derive (13) directly from the equations of motion and use (12) toderive (11). 32. Marwell's equations to zero order. – Equation (11) gives F. in

terms ...

Page 78

These equations which form the system include all of the Boltzmann and Maxwell

equations each to their

course. (17) is taken to minus first and zeroth order but in zeroth order it

determines ...

These equations which form the system include all of the Boltzmann and Maxwell

equations each to their

**lowest order**. (16), and (16), are of different orders ofcourse. (17) is taken to minus first and zeroth order but in zeroth order it

determines ...

Page 263

Carrying out the derivation of (6) to the next order gives (13) F = R, VE -- R, X B --

R, X (R, WB) – & R, -2C R, + O(e). This together with (12) gives to

first-order differential equation for R, . Since R, has already been determined up ...

Carrying out the derivation of (6) to the next order gives (13) F = R, VE -- R, X B --

R, X (R, WB) – & R, -2C R, + O(e). This together with (12) gives to

**lowest order**afirst-order differential equation for R, . Since R, has already been determined up ...

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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