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 |
DOI | 10.1088/1741-4326/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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