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

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Results 1-3 of 54

Page 105

3 assuming certain

of the T-F- and M-curves define the

density j, for which the T-F-mechanism can operate. As one sees from the figure ...

3 assuming certain

**values**of the parameters q = j.j, and p. The intersection pointsof the T-F- and M-curves define the

**value**BX, and the electron emission currentdensity j, for which the T-F-mechanism can operate. As one sees from the figure ...

Page 135

The

defines the critical magnetic field B, for this pressure and radius. The

corresponding

...

The

**value**of the magnetic field where the horizontal line is tangent to the X-curvedefines the critical magnetic field B, for this pressure and radius. The

corresponding

**values**shown in Fig. 24 are different from those with the results of...

Page 165

The discontinuity in p's p corresponds to large local

and (17) we see that such

Equation (13) implies that large local

same ...

The discontinuity in p's p corresponds to large local

**values**of p". From eqs. (16)and (17) we see that such

**values**can be obtained only near the point F= 0.Equation (13) implies that large local

**values**of W are also obtained near thesame ...

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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