The dependence of MAR on the plasma temperature near the divertor target is investigated by using the collisional-radiative model including the transport processes for plasma and neutral species, and the formation of neutral particles on the divertor target. In the model of the recycling process, th
Geometrical Effects in Plasma Stability and Dynamics of Coherent Structures in the Divertor
β Scribed by D. D. Ryutov; R. H. Cohen
- Publisher
- John Wiley and Sons
- Year
- 2008
- Tongue
- English
- Weight
- 179 KB
- Volume
- 48
- Category
- Article
- ISSN
- 0005-8025
No coin nor oath required. For personal study only.
β¦ Synopsis
Abstract
The effects of the strong Xβpoint magnetic shear, of the orientation of the divertor legs with respect to the major axis, and of the tilt of the divertor plates with respect to the poloidal field on plasma dynamics in the divertor region have been studied. The linear stability analysis of flute and resistive ballooning modes is presented for the Xβpoint geometry, with emphasis on the private flux region. The dynamics of isolated plasma filaments (βblobsβ) passing near the X point is described. In both cases the correct accounting for the geometry turns out to be critically important. (Β© 2008 WILEYβVCH Verlag GmbH & Co. KGaA, Weinheim)
π SIMILAR VOLUMES
Strong nonuniformity in the helical divertor flux distribution is seen both in numerical calculations and in experiments. Flux profiles along the divertor trace on the vacuum vessel change according to vacuum magnetic configurations. Diverted particles choose one of two X-points as the escaping chan
## Abstract If vibrationally excited molecules are discretised into individual species and proper account is taken of the toroidal geometry in simulating neutrals, some improvement can be made in simulating the anomalous detachment behaviour seen at the outer target of TCV singleβnull lower Lβmode
The neutrals in a tokamak divertor in the so-called "detached" mode of operation may be in a kinetic regime (long mean free path) in some regions and in a fluid regime (short mean free path) elsewhere. For example, a kinetic description is necessary in the thin ionization front, while the cold neutr