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

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Page 77

Thus Maxwell's equations to minus first

qdwdq = 0. It is easily shown from (11) that the time derivative of (22) is

) is satisfied. (This is just (60-16t)+V-J-1 = 0.) Similarly the time derivative of (23) ...

Thus Maxwell's equations to minus first

**order**give (22) X's " dw da = 0, (23) X es "qdwdq = 0. It is easily shown from (11) that the time derivative of (22) is

**zero**if (23) is satisfied. (This is just (60-16t)+V-J-1 = 0.) Similarly the time derivative of (23) ...

Page 78

Hence we must proceed to

) is three equations). The component parallel to n is ... To proceed to

(16) we need J to

Hence we must proceed to

**zeroth order**in (16) to find ČEsőt (strictly speaking (16) is three equations). The component parallel to n is ... To proceed to

**zero order**in(16) we need J to

**zero order**which by (18) involves f". Because of (11) eq.Page 132

Since we consider a three-component plasma in a longitudinal magnetic field the

stationary

o = 0 due to the assumption of weak ionization. If the index (0) designates the ...

Since we consider a three-component plasma in a longitudinal magnetic field the

stationary

**zero**-**order**solution is already given in the preceding chapter if we useo = 0 due to the assumption of weak ionization. If the index (0) designates the ...

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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