Modelling and consequences of drift effects in the edge plasma of Alcator C-Mod

被引:15
|
作者
Bonnin, X
Coster, D
Schneider, R
Reiter, D
Rozhansky, V
Voskoboynikov, S
机构
[1] EURATOM, Max Planck Inst Plasmaphys, Teilinst Greifswald, D-17491 Greifswald, Germany
[2] EURATOM, Max Planck Inst Plasmaphys, D-85748 Garching, Germany
[3] Forschungszentrum Julich GmbH, EURATOM Assoc KFA, Inst Plasmaphys, D-52425 Julich, Germany
[4] St Petersburg State Tech Univ, St Petersburg 195251, Russia
关键词
edge modelling; Alcator C-Mod; B2-Eirene; particle drifts; B-field reversal; CONSISTENT ELECTRIC-FIELDS; TOKAMAK; CODE; SOL; FLOW; JET;
D O I
10.1016/j.jnucmat.2004.10.102
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We model the plasma edge of Alcator C-Mod with the B2-Eirene SOLPS5.0 code. The drifts, currents and neutral effects contribute to strong plasma rotation in the edge, as measured experimentally [B. LaBombard, S. Gangadhara, B. Lipschultz, C.S. Pitcher, J. Nucl. Mater. 313-316 (2003) 995; B. LaBombard, N. Smick, B. Lipschultz, J.L. Terry, J. Rice, these Proceedings; N. Smick, B. LaBombard, C.S. Pitcher, these Proceedings]. The plasma flow patterns are a complex superposition of several competing effects, including Pfirsch-Schluter flows and currents, toroidal momentum generation and transport (with main chamber neutral recycling and drag playing an important role), as well as the E x B and diamagnetic drift flows. In the standard field direction the E x B flow in the core region adds to the toroidal plasma rotation, while in the reverse direction their respective contributions are roughly of the same order of magnitude but with opposite signs in the plasma core. However, in the edge, all terms can be of the same sign over most if not all of the radial extent of the SOL, leading to complex patterns and very strong flows. (c) 2004 Elsevier B.V. All rights reserved.
引用
收藏
页码:301 / 304
页数:4
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