The Physics of Inertial Fusion: BeamPlasma Interaction, Hydrodynamics, Hot Dense MatterThis book is on inertial confinement fusion, an alternative way to produce electrical power from hydrogen fuel by using powerful lasers or particle beams. It involves the compression of tiny amounts (micrograms) of fuel to thousand times solid density and pressures otherwise existing only in the centre of stars. Thanks to advances in laser technology, it is now possible to produce such extreme states of matter in the laboratory. Recent developments have boosted laser intensities again with new possibilities for laser particle accelerators, laser nuclear physics, and fast ignition of fusion targets. This is a reference book for those working on beam plasma physics, be it in the context of fundamental research or applications to fusion energy or novel ultra-bright laser sources. The book combines quite different areas of physics: beam target interaction, dense plasmas, hydrodynamic implosion and instabilities, radiative energy transfer as well as fusion reactions. Particular attention is given to simple and useful modelling, including dimensional analysis and similarity solutions. Both authors have worked in this field for more than 20 years. They want to address in particular those teaching this topic to students and all those interested in understanding the technical basis. |
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Table des matières
| 1 | |
| 10 | |
| 11 | |
| 22 | |
| 31 | |
| 37 | |
| 47 | |
| 65 | |
1 | 231 |
hydrodynamic | 232 |
5 | 250 |
8 | 285 |
275 | 310 |
Atoms in dense plasma | 323 |
Global equations of state | 339 |
Radiative processes | 345 |
| 66 | |
| 72 | |
| 82 | |
| 96 | |
| 101 | |
| 102 | |
Hydrodynamics | 129 |
Plane isentropic flow | 138 |
6 | 140 |
Rarefaction in Lagrange | 146 |
solutions | 161 |
Scaleinvariant similarity | 170 |
Thermal waves and ablative | 195 |
Beamtarget interaction | 371 |
wavelength | 380 |
plasma | 392 |
6 | 399 |
382 | 405 |
388 | 411 |
Appendix | 429 |
References | 435 |
396 | 438 |
284 | 443 |
Index | 453 |
Autres éditions - Tout afficher
The Physics of Inertial Fusion: Beam Plasma Interaction, Hydrodynamics, Hot ... Stefano Atzeni,Jürgen Meyer-ter-Vehn Aucun aperçu disponible - 2009 |
The Physics of Inertial Fusion: BeamPlasma Interaction, Hydrodynamics, Hot ... Stefano Atzeni,Jürgen Meyer-ter-Vehn Aucun aperçu disponible - 2004 |
Expressions et termes fréquents
a-particles ablation front ablation pressure absorption acceleration adiabatic amplitude approximation Atzeni Basko beam bremsstrahlung burn capsule Chapter coefficient cold fuel compression configuration constant corresponding Coulomb logarithm deflagration density depends derived described deuterium dimensional dimensional analysis drive electron emission entropy equation evolution factor fast ignition flow fluid flux fuel mass function fusion reactions gain curves given growth rate heat conduction heating wave hohlraum hohlraum targets hot spot hydrodynamic ICF target ignition condition implosion implosion velocity inertial initial instability integral interface ionization irradiation isentropic isobaric isochoric layer limit Lindl linear Mbar modes neutrons non-linear obtained opacity optically thick particle perturbation photon physics plane plasma profiles propagation radiation radiative radius rarefaction ratio refer regime region scaling self-heating shell shock front shown in Fig shows simulations solid spherical stagnation surface symmetry temperature thermal thermonuclear tion trajectories tritium values wavelength X-ray
Fréquemment cités
Page ii - Brownian motion: fluctuations, dynamics, and applications 111. H. Nishimori: Statistical physics of spin glasses and information processing: an introduction 110.
Page vi - In thermonuclear weapons, radiation from a fission explosive can be contained and used to transfer energy to compress and ignite a physically separate component containing thermonuclear fuel.
Page 165 - They are equivalent to each other in the sense that they can be...
Page v - At the same time at the American Optical Company it was shown that a laser could be made with any one of a number of rare-earth oxides dissolved in glass, instead of ruby.
Page 421 - The beat wave accelerator depends on the generation of a large amplitude plasma wave with a phase velocity close to the velocity of light c. The plasma wave (wsuh(p), ksuh(p)) is generated by beating colinear laser beams (o>i, ki) and (o>a,ki) with ojsub(p) = <ih-G>j, kvuWp) — ki-kj.
Page 108 - When more beam energy is available to form the compressed fuel region around the igniting spark, propagating burn occurs. This leads to steeply rising gain due to the sharp increase in p R and the fuel burn-up.
