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

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Page 58

Equations (9)–(14) are closed equations for 0, V, p, and B. These are

respectively by (9), (10), (11) and (13), J is

be eliminated with no trouble. (12) is a side condition; that is always satisfied if it

is ...

Equations (9)–(14) are closed equations for 0, V, p, and B. These are

**given**respectively by (9), (10), (11) and (13), J is

**given**as a definition by (14) and couldbe eliminated with no trouble. (12) is a side condition; that is always satisfied if it

is ...

Page 60

We wish to consider motions of the fluid in the neighborhood of the static

equilibrium

From (14) J' = V × B'. p', V", B' and o' can be

...

We wish to consider motions of the fluid in the neighborhood of the static

equilibrium

**given**above. We write at a fixed point r p = p" + p", W = W', B = B^+ B',From (14) J' = V × B'. p', V", B' and o' can be

**given**independently initially and then...

Page 78

6E/6t is

16) to find ČEsőt (strictly speaking (16) is three equations). The component

parallel to n is minus first order, which we used to find E, . The part perpendicular

to n ...

6E/6t is

**given**by (16) to zeroth order. Hence we must proceed to zeroth order in (16) to find ČEsőt (strictly speaking (16) is three equations). The component

parallel to n is minus first order, which we used to find E, . The part perpendicular

to n ...

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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