High-Z material erosion and its control in DIII-D carbon divertor

R. Ding, D. L. Rudakov, P. C. Stangeby, W. R. Wampler, T. Abrams, S. Brezinsek, A. Briesemeister, I. Bykov, V. S. Chan, C. P. Chrobak, J. D. Elder, H. Y. Guo, J. Guterl, A. Kirschner, C. J. Lasnier, A. W. Leonard, M. A. Makowski, A. G. McLean, P. B. Snyder, D. M. ThomasD. Tskhakaya, E. A. Unterberg, H. Q. Wang, J. G. Watkins

Research output: Contribution to journalArticlepeer-review

7 Scopus citations

Abstract

As High-Z materials will likely be used as plasma-facing components (PFCs) in future fusion devices, the erosion of high-Z materials is a key issue for high-power, long pulse operation. High-Z material erosion and redeposition have been studied using tungsten and molybdenum coated samples exposed in well-diagnosed DIII-D divertor plasma discharges. By coupling dedicated experiments and modelling using the 3D Monte Carlo code ERO, the roles of sheath potential and background carbon impurities in determining high-Z material erosion are identified. Different methods suggested by modelling have been investigated to control high-Z material erosion in DIII-D experiments. The erosion of Mo and W is found to be strongly suppressed by local injection of methane and deuterium gases. The 13C deposition resulting from local 13CH4 injection also provides information on radial transport due to E × B drifts and cross field diffusion. Finally, D2 gas puffing is found to cause local plasma perturbation, suppressing W erosion because of the lower effective sputtering yield of W at lower plasma temperature and for higher carbon concentration in the mixed surface layer.

Original languageEnglish
Pages (from-to)247-252
Number of pages6
JournalNuclear Materials and Energy
Volume12
DOIs
StatePublished - Aug 2017

Funding

This material is based upon work supported by the US Department of Energy, Office of Science, Office of Fusion Energy Sciences and Office of Advanced Scientific Computing Research through the Scientific Discovery through Advanced Computing (SciDAC) project on Plasma-Surface Interactions, under Award No. GA-DE-SC0008698, using the DIII-D National Fusion Facility, a DOE Office of Science user facility, under Awards DE-AC05-06OR23100, DE-FG02-07ER54917, DE-AC05-00OR22725, DE-FC02-04ER54698, and DE-AC52-07NA27344. Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation, for the US Department of Energy's National Nuclear Security Administration under contract DE-AC04-94AL85000. The first author acknowledges the supports by the National Magnetic Confinement Fusion Science Program of China under contract No 2013GB107004 , the National Natural Science Foundation of China under Contract No 11375010 , 11675218 and the Sino-German Centre for Research Promotion under Contract No GZ769 . DIII-D data shown in this paper can be obtained in digital format by following the links at https://fusion.gat.com/global/D3D_DMP . This material is based upon work supported by the US Department of Energy, Office of Science, Office of Fusion Energy Sciences and Office of Advanced Scientific Computing Research through the Scientific Discovery through Advanced Computing (SciDAC) project on Plasma-Surface Interactions, under Award No. GA-DE-SC0008698, using the DIII-D National Fusion Facility, a DOE Office of Science user facility, under Awards DE-AC05-06OR23100, DE-FG02-07ER54917, DE-AC05-00OR22725, DE-FC02-04ER54698, and DE-AC52-07NA27344. Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation, for the US Department of Energy's National Nuclear Security Administration under contract DE-AC04-94AL85000. The first author acknowledges the supports by the National Magnetic Confinement Fusion Science Program of China under contract No 2013GB107004, the National Natural Science Foundation of China under Contract No 11375010, 11675218 and the Sino-German Centre for Research Promotion under Contract No GZ769. DIII-D data shown in this paper can be obtained in digital format by following the links at https://fusion.gat.com/global/D3D_DMP.

FundersFunder number
DIII-D National Fusion Facility
DOE Office of Science user facilityDE-AC05-00OR22725, DE-FC02-04ER54698, DE-AC52-07NA27344, DE-FG02-07ER54917, DE-AC05-06OR23100
Office of Fusion Energy Sciences and Office of Advanced Scientific Computing ResearchGA-DE-SC0008698
Sandia Corporation
Sino-German Centre for Research PromotionGZ769
US Department of Energy
US Department of Energy's National Nuclear Security AdministrationDE-AC04-94AL85000
Lockheed Martin Corporation
Office of Science
Advanced Scientific Computing Research
Fusion Energy Sciences
Sandia National Laboratories
National Natural Science Foundation of China11675218, 11375010
National Magnetic Confinement Fusion Program of China2013GB107004

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