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

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Page 78

This would complete our system of equations for zeroth order

system is (11), (15), (16), and (24) with side conditions (14), (22) and (23). [(16),

means the perpendicular part of (16), the parallel part is actually (24)] (11) is an ...

This would complete our system of equations for zeroth order

**quantities**. Thissystem is (11), (15), (16), and (24) with side conditions (14), (22) and (23). [(16),

means the perpendicular part of (16), the parallel part is actually (24)] (11) is an ...

Page 121

The

to the particle components with which the test particle collides. The prime (')

characterizes

The

**quantities**without index refer to the particle under consideration, the index (i)to the particle components with which the test particle collides. The prime (')

characterizes

**quantities**after collision. The bar indicates the velocity average (r).Page 133

We should remember that in general both eigenfunctions and the eigenvalue

itself may be complex

judge by the imaginary part of the eigenvalues whether a given mode grows or

decays, ...

We should remember that in general both eigenfunctions and the eigenvalue

itself may be complex

**quantities**. If we had solved this problem then we couldjudge by the imaginary part of the eigenvalues whether a given mode grows or

decays, ...

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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