Plasma Astrophysics, Part II: Reconnection and FlaresSpringer Science & Business Media, 31 дек. 2007 г. - Всего страниц: 428 Magnetic ?elds are easily generated in astrophysical plasma owing to its ?6 high conductivity. Magnetic ?elds, having strengths of order few 10 G, correlated on several kiloparsec scales are seen in spiral galaxies. Their origin could be due to ampli?cation of a small seed ?eld by a turbulent galactic dynamo. In several galaxies, like the famous M51, magnetic ?elds are well correlated (or anti-correlated) with the optical spiral arms. These are the weakest large-scale ?elds observed in cosmic space. The strongest magnets in space are presumably the so-called magnetars, the highly mag- 15 netized (with the strength of the ?eld of about 10 G) young neutron stars formed in the supernova explosions. The energy of magnetic ?elds is accumulated in astrophysical plasma, and the sudden release of this energy – an original electrodynamical ‘burst’ or‘explosion’–takesplaceunderde?nitebutquitegeneralconditions(P- att, 1992; Sturrock, 1994; Kivelson and Russell, 1995; Rose, 1998; Priest and Forbes, 2000; Somov, 2000; Kundt, 2001). Such a ‘?are’ in ast- physical plasma is accompanied by fast directed ejections (jets) of plasma, powerful ?ows of heat and hard electromagnetic radiation as well as by impulsive acceleration of charged particles to high energies. |
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| 3 | |
| 11 | |
| 19 | |
Comments on numerical simulations | 47 |
Motion of a Charged Particle in Given Fields | 79 |
Adiabatic Invariants in Astrophysical Plasma | 103 |
WaveParticle Interaction in Astrophysical Plasma | 115 |
The principles of particle acceleration by waves | 122 |
3 | 47 |
The Bastille Day 2000 Flare | 77 |
888 | 88 |
5 | 99 |
80 | 118 |
81 | 147 |
7 | 153 |
Solartype Flares in Laboratory and Space | 193 |
Exercises and Answers | 128 |
Macroscopic Description of Astrophysical Plasma | 163 |
MultiFluid Models of Astrophysical Plasma | 183 |
The Generalized Ohms Law in Plasma | 193 |
SingleFluid Models for Astrophysical Plasma | 205 |
Magnetohydrodynamics in Astrophysics | 223 |
Plasma Flows in a Strong Magnetic Field | 243 |
MHD Waves in Astrophysical Plasma | 263 |
Discontinuous Flows in a MHD Medium | 277 |
Evolutionarity of MHD Discontinuities | 305 |
1 | 327 |
Bibliography | 405 |
Index | 426 |
Contents | vii |
1 | 5 |
Stationary Flows in a Magnetic Field | 20 |
Reconnection in a Strong Magnetic Field | 21 |
9 | 211 |
Structural Instability of Reconnecting Current Layers 237 | 237 |
11 | 269 |
Magnetic Reconnection and Turbulence 297 | 297 |
13 | 319 |
22 | 337 |
14 | 339 |
15 | 352 |
26 | 358 |
Epilogue 365 | 365 |
28 | 375 |
| 391 | |
| 406 | |
| 407 | |
| 412 | |
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acceleration accretion disk active region Alfvén Alfvén waves approximation astrophysical plasma Bastille day flare boundary conditions Chapter charged particles chromosphere collisionless component Coulomb collisions curl density diffusion discontinuity dissipation distribution function drift electric current electric field electromagnetic electrons and ions example Exercise fast electrons fast particles follows footpoints force formula gradient gravitational heating hydrodynamic inside instability interaction Landau Larmor linear longitudinal loops Lorentz force magnetic energy magnetic field magnetic field lines magnetic flux magnetic reconnection momentum motion neutral observed Ohm's law parameter particles of kind perpendicular perturbation phase space photospheric physical plane plasma flows problem protons radius reconnecting current layer relativistic Section separatrices shock wave shown in Figure SHTCL solar corona solar flares solution Somov stars surface Syrovatskii temperature term thermal tion trap turbulence vector velocity X-ray Yohkoh zero zeroth
