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Titlebook: Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas; John Rice Book 2022 Springer Nature Switzerland AG 2022 r

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21#
發(fā)表于 2025-3-25 04:38:57 | 只看該作者
22#
發(fā)表于 2025-3-25 09:41:44 | 只看該作者
23#
發(fā)表于 2025-3-25 15:32:23 | 只看該作者
Comparison with Neo-Classical Theory, Helander (Phys Plasmas 13:102505, 2006), and Wong et al. (Phys Plasmas 15:082503, 2008) and have been incorporated into a variety of codes including NCLASS, HAGIS, NEOART and NEO. In Sect. 4.3, edge poloidal asymmetries will be addressed.
24#
發(fā)表于 2025-3-25 19:41:56 | 只看該作者
Momentum Sources,mbipolar radial particle shifts or orbit losses (Sect. 2.2), the latter due to toroidal magnetic field ripple for example. Direct rotation drive can be from neutral beam injection, transfer of momentum from radio frequency waves (ICRF, LH or EC) or from neutral gas or compact torus injection.
25#
發(fā)表于 2025-3-25 22:16:27 | 只看該作者
Momentum Transport,ree parameters. In certain circumstances it is possible to isolate each of the three, or two of the three, and the results will be covered in Sects. 6.1, 6.2, and 6.3, respectively, with a comparison to theory in Sect. 6.4
26#
發(fā)表于 2025-3-26 02:29:46 | 只看該作者
27#
發(fā)表于 2025-3-26 07:40:56 | 只看該作者
Entscheidungsfindung und Handelnples will be provided in this section of how the rotation can be driven by changes in various gradients, as well as the collisionality and magnetic configuration, using external heating and current drive, and in Ohmic plasmas. In the absence of external momentum sources, if the initial velocity and
28#
發(fā)表于 2025-3-26 08:59:24 | 只看該作者
29#
發(fā)表于 2025-3-26 13:40:00 | 只看該作者
30#
發(fā)表于 2025-3-26 17:02:45 | 只看該作者
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