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

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Page ix

M. N. ROSENBLUTH General Atomic, Division of General

- San Diego, Cal. Unhappily, I am finally writing this introduction in the days

following the awful events of President Kennedy's assassination which is

dominating ...

M. N. ROSENBLUTH General Atomic, Division of General

**Dynamics**Corporation- San Diego, Cal. Unhappily, I am finally writing this introduction in the days

following the awful events of President Kennedy's assassination which is

dominating ...

Page xi

As in other types of fluid

obscured by our inability to treat nonlinear problems effectively. Some important

beginnings have been made and are discussed in the lectures of Professor

PETER ...

As in other types of fluid

**dynamics**a great many of the answers we seek areobscured by our inability to treat nonlinear problems effectively. Some important

beginnings have been made and are discussed in the lectures of Professor

PETER ...

Page 3

*s, to ... ry), F] = 0 , which is completely equivalent to the microscopic

being the complete Hamiltonian. This can be written, introducing the acceleration

field A, (or, ... ary), 6F 6F' 6 '. . X (or 40,...o.)=0. - The equivalence of Liouville's ...

*s, to ... ry), F] = 0 , which is completely equivalent to the microscopic

**dynamics**, Hbeing the complete Hamiltonian. This can be written, introducing the acceleration

field A, (or, ... ary), 6F 6F' 6 '. . X (or 40,...o.)=0. - The equivalence of Liouville's ...

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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