Improvement of lower hybrid current drive systems for high-power and long-pulse operation on EAST

限制器 材料科学 核工程 等离子体 光电子学 聚变能 电气工程 物理 工程类 量子力学 冶金
作者
Mao Wang,L. Liu,L.M. Zhao,Miaohui Li,W.D. Ma,Haiping Hu,Zege Wu,J.Q. Feng,Yongheng Yang,Liang Zhu,M. Chen,Taian Zhou,H. Jia,Jie Zhang,L. Cao,Ling Zhang,R.R. Liang,B. J. Ding,Xinnan Zhang,Jiafang Shan,F.K. Liu,A. Ekedahl,M. Goniche,J. Hillairet,L. Delpech
出处
期刊:Nuclear Engineering and Technology [Elsevier]
卷期号:54 (11): 4102-4110 被引量:7
标识
DOI:10.1016/j.net.2022.06.003
摘要

Aiming at high-power and long-pulse operation up to 1000 s, some improvements have been made for both 2.45 GHz and 4.6 GHz lower hybrid (LH) systems during the recent 5 years. At first, the guard limiters of the LH antennas with graphite tiles were upgraded to tungsten, the most promising material for plasma facing components in nuclear fusion devices. These new guard limiters can operate at a peak power density of 12.9 MW/m2. Strong hot spots were usually observed on the old graphite limiters when 4.6 GHz system operated with power >2.0 MW [B. N. Wan et al., Nucl. Fusion 57 (2017) 102019], leading to a reduction of the maximum power capability. With the new limiters, 4.6 GHz LH system, the main current drive (CD) and electron heating tool for EAST, can be operated with power >2.5 MW routinely. Long-pulse operation up to 100 s with 4.6 GHz LH power of 2.4 MW was achieved in 2021 and the maximal temperature on the guard limiters measured by an infrared (IR) camera was about 540 °C, much below the permissible value of tungsten material (∼1200 °C). A discharge with a duration of 1056 s was achieved and the 4.6 GHz LH energy injected into the plasma was up to 1.05 GJ. Secondly, the fully-active-multijunction (FAM) launcher of 2.45 GHz system was upgraded to a passive-active-multijunction (PAM), for which the density of optimum coupling was relatively low (below the cut-off value). Good coupling with reflection coefficient ∼3% has been achieved with plasma-antenna distance up to 11 cm for the new PAM. Finally, in order to eliminate the effect of ion cyclotron range of frequencies (ICRF) wave on 4.6 GHz LH wave coupling, the location of the ICRF launcher was changed to a port that is located 157.5° toroidally from the 4.6 GHz LH system and is not magnetically connected.

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