First EMC3-Eirene simulations of the TCV snowflake divertor

被引:36
作者
Lunt, T. [1 ]
Canal, G. P. [2 ]
Feng, Y. [3 ]
Reimerdes, H. [2 ]
Duval, B. P. [2 ]
Labit, B. [2 ]
Vijvers, W. A. J. [2 ]
Coster, D. [1 ]
Lackner, K. [1 ]
Wischmeier, M. [1 ]
机构
[1] Max Planck Inst Plasma Phys, EURATOM Assoc, D-85748 Garching, Germany
[2] Ecole Polytech Fed Lausanne, Ctr Rech Phys Plasmas, EURATOM Assoc, CH-1015 Lausanne, Switzerland
[3] Max Planck Inst Plasma Phys, EURATOM Assoc, D-17491 Greifswald, Germany
关键词
snowflake divertor; confinement; alternative confinement concepts; EMC3-Eirene; DEMO; beta poloidal instability; DISCHARGES; PLASMA;
D O I
10.1088/0741-3335/56/3/035009
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
One of the approaches to solve the heat load problem in a divertor tokamak is the so called 'snowflake' (SF) configuration, a magnetic equilibrium with two nearby x-points and two additional divertor legs. Here we report on the first EMC3-Eirene simulations of plasma-and neutral particle transport in the scrape-off layer of a series of TCV SF equilibria with different values of sigma, the distance between the x-points normalized to the minor radius of the plasma. The constant cross-field transport coefficients were chosen such that the power-and particle deposition profiles at the primary inner strike point (SP) match the Langmuir probe measurements for the sigma = 0.1 case. At the secondary SP on the floor, however, a significantly larger power flux than that predicted by the simulation was measured by the probes, indicating an enhanced transport across the primary separatrix. As the ideal SF configuration (sigma = 0) is approached, the density as well as the radiation maximum are predicted to move from the target plates upward to the x-point by the simulation.
引用
收藏
页数:13
相关论文
共 26 条
[1]  
Allen S L, 2012, 24 IAEA FEC SAN DIEG, pPD 1
[2]   Inter-ELM Power Decay Length for JET and ASDEX Upgrade: Measurement and Comparison with Heuristic Drift-Based Model [J].
Eich, T. ;
Sieglin, B. ;
Scarabosio, A. ;
Fundamenski, W. ;
Goldston, R. J. ;
Herrmann, A. .
PHYSICAL REVIEW LETTERS, 2011, 107 (21)
[3]  
Feng Y, 2004, CONTRIB PLASM PHYS, V44, P57, DOI 10.1002/ctpp.20041009
[4]  
FENG Y, 2011, 38 EPS 2011 C PLASM
[5]   Validating the 3D edge code EMC3-EIRENE against 2D simulations with EDGE2D-EIRENE for JET single null configurations [J].
Harting, D. ;
Wiesen, S. ;
Frerichs, H. ;
Reiter, D. ;
Boerner, P. ;
Feng, Y. .
JOURNAL OF NUCLEAR MATERIALS, 2011, 415 (01) :S540-S544
[6]  
Ivanov A A, 2009, KELDYSH I PREPRINTS, V39
[7]  
LUNT T, 2009, 36 EPS C PLASM PHY E, V33
[8]  
Pericoli-Ridolfini V, 2013, FUSION ENG DES, V88, P1677
[9]   "Snowflake" H Mode in a Tokamak Plasma [J].
Piras, F. ;
Coda, S. ;
Duval, B. P. ;
Labit, B. ;
Marki, J. ;
Medvedev, S. Yu. ;
Moret, J. -M. ;
Pitzschke, A. ;
Sauter, O. .
PHYSICAL REVIEW LETTERS, 2010, 105 (15)
[10]   Snowflake divertor plasmas on TCV [J].
Piras, F. ;
Coda, S. ;
Furno, I. ;
Moret, J-M ;
Pitts, R. A. ;
Sauter, O. ;
Tal, B. ;
Turri, G. ;
Bencze, A. ;
Duval, B. P. ;
Felici, F. ;
Pochelon, A. ;
Zucca, C. .
PLASMA PHYSICS AND CONTROLLED FUSION, 2009, 51 (05)