First EMC3-Eirene simulations of the TCV snowflake divertor

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.

[1]  P. Valanju,et al.  Super-X divertors and high power density fusion devices , 2009 .

[2]  D. Reiter,et al.  The EIRENE and B2-EIRENE Codes , 2005 .

[3]  T. Eich,et al.  Inter-ELM power decay length for JET and ASDEX upgrade: measurement and comparison with heuristic drift-based model. , 2011, Physical review letters.

[4]  M. Keilhacker,et al.  Characteristics of the divertor plasma in neutral-beam-heated ASDEX discharges , 1983 .

[5]  D. Ryutov,et al.  Comparison of ELM heat loads in snowflake and standard divertors , 2012 .

[6]  D. Ryutov,et al.  A snowflake divertor: a possible solution to the power exhaust problem for tokamaks , 2012 .

[7]  D. Ryutov,et al.  Local properties of the magnetic field in a snowflake divertor , 2010 .

[8]  R. H. Bulmer,et al.  Analysis of geometric variations in high-power tokamak divertors , 2009 .

[9]  J. Contributors,et al.  Validating the 3D edge code EMC3-EIRENE against 2D simulations with EDGE2D-EIRENE for JET single null configurations , 2011 .

[10]  G. Calabrò,et al.  Preliminary 2D code simulation of the quasi-snowflake divertor configuration in the FAST tokamak , 2013 .

[11]  E. Kolemen,et al.  “Snowflake” divertor configuration in NSTX , 2010 .

[12]  J-M Moret,et al.  "Snowflake" H mode in a tokamak plasma. , 2010, Physical review letters.

[13]  References , 1971 .

[14]  S. Coda,et al.  Power distribution in the snowflake divertor in TCV , 2013 .

[15]  F. Wagner,et al.  Regime of Improved Confinement and High Beta in Neutral-Beam-Heated Divertor Discharges of the ASDEX Tokamak , 1982 .

[16]  M. V. Umansky,et al.  The magnetic field structure of a snowflake divertor , 2008 .

[17]  Faa Federico Felici,et al.  Snowflake divertor plasmas on TCV , 2009 .

[18]  D. Ryutov,et al.  Plasma Convection Near the Magnetic Null of a Snowflake Divertor During an ELM Event , 2012 .

[19]  D. Ryutov Geometrical properties of a “snowflake” divertor , 2007 .

[20]  H. Zohm Edge localized modes (ELMs) , 1996 .

[21]  F. Sardei,et al.  3D Edge Modeling and Island Divertor Physics , 2004 .