中国科学院机构知识库网格
Chinese Academy of Sciences Institutional Repositories Grid
Application of an empirical saturation rule to TGLF to unify low-k and high-k turbulence dominated regimes

文献类型:期刊论文

作者Jian, Xiang1; Chan, Vincent S.2,3; Chen, Jiale4; Li, Zeyu5; Garofalo, Andrea M.3; Zhuang, Ge1,6; CFETR Phys Team
刊名NUCLEAR FUSION
出版日期2018
卷号58期号:1页码:1-14
关键词Plasma Turbulence Tglf Model Multi-scale Simulation Experimental Validation
DOI10.1088/1741-4326/aa8fb2
文献子类Article
英文摘要We propose a phenomenological turbulence saturation model and apply it to the TGLF turbulence transport model (Staebler et al 2007 Phys. Plasmas 14 055909), which captures the physics of interaction between low-k and high-k turbulence consistent with the multiscale gyro-kinetic simulation result reported by Howard (2016 Nucl. Fusion. 23 056109). The new model, TGLF-Vx is tested with three discharges from DIII-D and EAST tokamak, which cover both low-k and high-k turbulence dominated regimes. It is found that the profile match can be substantially improved over previous models when evolving Te, Ti and ne simultaneously. Good agreement for all three discharges is obtained with one fixed parameter in the model when taking experimental uncertainties into consideration. Lastly, TGLF-Vx is applied to explore the sensitivity of the predicted CFETR steady-state performance to different transport models. Our result shows that a scenario using only RF auxiliary heating could be significantly affected.
WOS关键词TOKAMAK ; HEAT
WOS研究方向Physics
语种英语
WOS记录号WOS:000414591400005
资助机构National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; 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US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National Magnetic Confinement Fusion Research Program of China(2014GB110001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; National ITER Plans Program of China(2013GB106001 ; NSFC(11405218) ; NSFC(11405218) ; NSFC(11405218) ; NSFC(11405218) ; NSFC(11405218) ; NSFC(11405218) ; NSFC(11405218) ; NSFC(11405218) ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; Fundamental Research Funds for the Central Universities(HUST: cx16-007 ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; US DOE Office of Fusion Energy Science(DE-FC02-04ER54698) ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2014GB110002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; 2013GB111002 ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; cx16-008) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2014GB110003) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001) ; 2015GB110001)
源URL[http://ir.hfcas.ac.cn:8080/handle/334002/33839]  
专题合肥物质科学研究院_中科院等离子体物理研究所
作者单位1.Huazhong Univ Sci & Technol, Sch Elect & Elect Engn, State Key Lab Adv Electromagnet Engn & Technol, Wuhan 430074, Hubei, Peoples R China
2.Univ Sci & Technol China, Sch Nucl Sci & Technol, Hefei 230026, Anhui, Peoples R China
3.Gen Atom, POB 85608, San Diego, CA 92186 USA
4.Chinese Acad Sci, Inst Plasma Phys, Hefei 230031, Anhui, Peoples R China
5.Peking Univ, Sch Phys, State Key Lab Nucl Phys & Technol, Beijing 100871, Peoples R China
6.Univ Sci & Technol China, Sch Phys Sci, Hefei 230026, Anhui, Peoples R China
推荐引用方式
GB/T 7714
Jian, Xiang,Chan, Vincent S.,Chen, Jiale,et al. Application of an empirical saturation rule to TGLF to unify low-k and high-k turbulence dominated regimes[J]. NUCLEAR FUSION,2018,58(1):1-14.
APA Jian, Xiang.,Chan, Vincent S..,Chen, Jiale.,Li, Zeyu.,Garofalo, Andrea M..,...&CFETR Phys Team.(2018).Application of an empirical saturation rule to TGLF to unify low-k and high-k turbulence dominated regimes.NUCLEAR FUSION,58(1),1-14.
MLA Jian, Xiang,et al."Application of an empirical saturation rule to TGLF to unify low-k and high-k turbulence dominated regimes".NUCLEAR FUSION 58.1(2018):1-14.

入库方式: OAI收割

来源:合肥物质科学研究院

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