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Dive into the research topics where Yaowei Yu is active.

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Featured researches published by Yaowei Yu.


Nuclear Fusion | 2007

Extension of operational limits on EAST

X. Gao; Jiangang Li; Baonian Wan; Junyu Zhao; Liqun Hu; Haiqing Liu; Yinxian Jie; Q. Xu; Zhenwei Wu; Yu Yang; X.Z. Gong; Biao Shen; Jiansheng Hu; Yuejiang Shi; Bili Ling; Jun Wang; S. Sajjad; Qing Zang; Wei Gao; Tao Zhang; Yaowei Yu; Yao Yang; Xiaofeng Han; Nan Shi; Tingfeng Ming; Ang Ti; Wenyang Zhang; Guosheng Xu; Junling Chen; Guang-Nan Luo

The first plasma has been achieved successfully in the Experimental Advanced Superconducting Tokamak (EAST). Boronization by the glow discharge (GDC) method was studied in experiments. The plasma performance was obviously improved by GDC boronization. Extension of the operational region and improvement in the plasma performance were obtained. Sawtooth discharges were observed by means of soft x-ray signals, electron cyclotron emission signals and line averaged electron density after boronization. Lower qa and more stable operation were also achieved following GDC boronization. The plasma current ramp-up rate was also improved as a result of decreased impurity content and low averaged loop voltage due to boronization. PLEASE NOTE: THERE HAS BEEN A RETRACTION PUBLISHED FOR THIS ARTICLE.


Plasma Physics and Controlled Fusion | 2013

Study of runaway current generation following disruptions in KSTAR

Z. Y. Chen; W C Kim; Yaowei Yu; A C England; J W Yoo; S H Hahn; S.W. Yoon; K D Lee; Y K Oh; J G Kwak; M Kwon

The high fraction of runaway current conversion following disruptions has an important effect on the first wall for next-generation tokamaks. Because of the potentially severe consequences of a large full current runaway beam on the first wall in an unmitigated disruption, runaway suppression is given a high priority. The behavior of runaway currents both in spontaneous disruptions and in D2 massive gas injection (MGI) shutdown experiments is investigated in the KSTAR tokamak. The experiments in KSTAR show that the toroidal magnetic field threshold, BT >2 T, for runaway generation is not absolute. A high fraction of runaway current conversion following spontaneous disruptions is observed at a much lower toroidal magnetic field of BT = 1.3 T. A dedicated fast valve for high-pressure gas injection with 39.7 bar is developed for the study of disruptions. A study of runaway current parameters shows that the conversion efficiency of pre-disruptive plasma currents into runaway current can reach over 80% both in spontaneous disruptions and in D2 MGI shutdown experiments in KSTAR.


Review of Scientific Instruments | 2012

First results on disruption mitigation by massive gas injection in Korea Superconducting Tokamak Advanced Research

Yaowei Yu; Young-Ok Kim; Hak-Kun Kim; Hong-Tack Kim; Woong-Chae Kim; Kwang-Pyo Kim; Soohyun Son; Eunnam Bang; Huidong Zhuang; Zhongyong Chen; Suk-Ho Hong; S.W. Yoon

Massive gas injection (MGI) system was developed on Korea Superconducting Tokamak Advanced Research (KSTAR) in 2011 campaign for disruption studies. The MGI valve has a volume of 80 ml and maximum injection pressure of 50 bar, the diameter of valve orifice to vacuum vessel is 18.4 mm, the distance between MGI valve and plasma edge is ~3.4 m. The MGI power supply employs a large capacitor of 1 mF with the maximum voltage of 3 kV, the valve can be opened in less than 0.1 ms, and the amount of MGI can be controlled by the imposed voltage. During KSTAR 2011 campaign, MGI disruptions are carried out by triggering MGI during the flat top of circular and limiter discharges with plasma current 400 kA and magnetic field 2-3.5 T, deuterium injection pressure 39.7 bar, and imposed voltage 1.1-1.4 kV. The results show that MGI could mitigate the heat load and prevent runaway electrons with proper MGI amount, and MGI penetration is deeper under higher amount of MGI or lower magnetic field. However, plasma start-up is difficult after some of D(2) MGI disruptions due to the high deuterium retention and consequently strong outgassing of deuterium in next shot, special effort should be made to get successful plasma start-up after deuterium MGI under the graphite first wall.


Plasma Physics and Controlled Fusion | 2016

Density limits investigation and high density operation in EAST tokamak

X.W. Zheng; Jiangang Li; Jiansheng Hu; Haiqing Liu; Yinxian Jie; Shouxin Wang; Jiahong Li; Yanming Duan; M. H. Li; Yongchun Li; Ling Zhang; Yang Ye; Qingquan Yang; Tao Zhang; Yingjie Cheng; Jichan Xu; Liang Wang; Liqing Xu; H.L. Zhao; Fudi Wang; S. Y. Lin; Bin Wu; B. Lyu; Guosheng Xu; X. Gao; Tonghui Shi; Kaiyang He; H. Lan; Nan Chu; Bin Cao

Increasing the density in a tokamak is limited by the so-called density limit, which is generally performed as an appearance of disruption causing loss of plasma confinement, or a degradation of high confinement mode which could further lead to a H → L transition. The L-mode and H-mode density limit has been investigated in EAST tokamak. Experimental results suggest that density limits could be triggered by either edge cooling or excessive central radiation. The L-mode density limit disruption is generally triggered by edge cooling, which leads to the current profile shrinkage and then destabilizes a 2/1 tearing mode, ultimately resulting in a disruption. The L-mode density limit scaling agrees well with the Greenwald limit in EAST. The observed H-mode density limit in EAST is an operational-space limit with a value of . High density H-mode heated by neutral beam injection (NBI) and lower hybrid current drive (LHCD) are analyzed, respectively. The constancy of the edge density gradients in H-mode indicates a critical limit caused perhaps by e.g. ballooning induced transport. The maximum density is accessed at the H → L transition which is generally caused by the excessive core radiation due to high Z impurities (Fe, Cu). Operating at a high density () is favorable for suppressing the beam shine through NBI. High density H-mode up to could be sustained by 2 MW 4.6 GHz LHCD alone, and its current drive efficiency is studied. Statistics show that good control of impurities and recycling facilitate high density operation. With careful control of these factors, high density up to 0.93 stable H-mode operation was carried out heated by 1.7 MW LHCD and 1.9 MW ion cyclotron resonance heating with supersonic molecular beam injection fueling.


Review of Scientific Instruments | 2014

Preparations for the motional Stark effect diagnostic on EASTa)

Jia Fu; Yingying Li; B. Lyu; P. Sheng; Y. Zhang; X. H. Yin; Y. J. Shi; Yaowei Yu; Minyou Ye; Baonian Wan

Measurement and control of the current profile is essential for high performance and steady state operation of Experimental Advanced Superconducting Tokamak (EAST). For this purpose, a conventional Motional Stark Effect (MSE) diagnostics utilizing photoelastic modulators is proposed and investigated. The pilot experiment includes one channel to verify the feasibility of MSE, whose sightline intersects with Neutral Beam Injection at major radius of R = 2.12 m. A beam splitter is adopted for simultaneous measurements of Stark multiplets and their polarization directions. A simplified simulation code was also developed to explore the Stark splitting spectra. Finally, the filter is optimized based on the viewing geometry and neutral beam parameters.


Plasma Physics and Controlled Fusion | 2012

First comprehensive particle balance study in KSTAR with a full graphite first wall and diverted plasmas

Yaowei Yu; Suk-Ho Hong; S.W. Yoon; Kwang-Pyo Kim; Woong-Chae Kim; Jae-Min Park; Young-Suk Oh; Hoonkyun Na; J. G. Bak; Kyu-Sun Chung

The first comprehensive particle balance study is carried out in the KSTAR 2010 campaign with a full graphite first wall and diverted plasmas. The dominant retention is observed during the gas puffing into the plasmas. Statistical analysis shows that deuterium retention is increased with the number of injected particles. Particle balance analysis in the whole campaign shows that the long-term retention ratio is ~21%, and the retention via implantation can be partially recovered by He-glow discharge cleaning (GDC), while long-term retention via co-deposition. The wall pumping capability is decreased with the D2 plasma due to fuel accumulation in the first wall, and He-GDC is effective in recovering the wall pumping. Boronization assisted by the D2 glow discharge using C2B10H12 strongly enhances the wall puffing and leads to negative retentions, but the wall pumping capability is recovered in 2–3 days by He-GDCs. Electron cyclotron resonance heating enhances wall outgassing during the discharge. During a diverted H-mode discharge, the retention rate decreases to a very low value, and a high divertor particle flux of ~1.5 × 1023 D s−1 is observed indicating the strong recycling divertor. The amount of recovered deuterium after discharges mainly depends on the plasma–wall interaction when the plasma is terminated, and disruptive discharges release more particles from the first wall.


Review of Scientific Instruments | 2016

Fast-ion Dα spectrum diagnostic in the EAST

Y. M. Hou; C. R. Wu; Jia-Qi Huang; W.W. Heidbrink; M. von Hellermann; Z. Xu; Z. Jin; J. F. Chang; Y. B. Zhu; Wen Gao; Yue Chen; B. Lyu; R. J. Hu; Pengfei Zhang; L. Zhang; Zhiwei Wu; Yaowei Yu; Minyou Ye; East Team

In toroidal magnetic fusion devices, fast-ion D-alpha diagnostic (FIDA) is a powerful method to study the fast-ion feature. The fast-ion characteristics can be inferred from the Doppler shifted spectrum of Dα light according to charge exchange recombination process between fast ions and probe beam. Since conceptual design presented in the last HTPD conference, significant progress has been made to apply FIDA systems on the Experimental Advanced Superconducting Tokamak (EAST). Both co-current and counter-current neutral beam injectors are available, and each can deliver 2-4 MW beam power with 50-80 keV beam energy. Presently, two sets of high throughput spectrometer systems have been installed on EAST, allowing to capture passing and trapped fast-ion characteristics simultaneously, using Kaiser HoloSpec transmission grating spectrometer and Bunkoukeiki FLP-200 volume phase holographic spectrometer coupled with Princeton Instruments ProEM 1024B eXcelon and Andor DU-888 iXon3 1024 CCD camera, respectively. This paper will present the details of the hardware descriptions and experimental spectrum.


Plasma Physics and Controlled Fusion | 2011

ICRF (ion cyclotron range of frequencies) discharge cleaning with toroidal and vertical fields on EAST

Yaowei Yu; Jiansheng Hu; Yanping Zhao; X. Gao; Jiangang Li

ICRF (ion cyclotron range of frequencies) discharge cleaning with a toroidal field and an additional vertical field was carried out on EAST recently. With the injected ICRF power of 10 kW, He pressure of 10−3 Pa, toroidal field of 0.5 T and vertical field of 0.01 T, ICRF plasmas became approximately symmetric in both major radial and vertical directions, and the removal rate of hydrogen increased by 32%. A comparison of ICRF discharge cleaning between stainless steel and graphite walls was carried out, which showed that ICRF plasmas had a similar effect on the first walls of both materials. ICRF discharge cleaning between plasma shots after a major disruption was studied in detail, and it was observed that ICRF discharge cleaning under a toroidal field of 2 T was effective in recovering plasma performance quickly after a major disruption.


Physica Scripta | 2009

ECR plasmas for wall conditioning of the HT-7 tokamak

Yaowei Yu; X. Gao; Jiafang Shan; Jiangang Li; Jiansheng Hu

Electron cyclotron resonance (ECR) plasmas produced by radio frequency (RF) waves were investigated for wall conditioning, with a toroidal field of 0.066?0.088?T in the HT-7 superconducting tokamak. Effective wall conditioning was obtained. The influences of toroidal magnetic field, radio frequency (RF) powers, pressures and working gas species on removal rates have been investigated by the partial pressures of the relevant gases. It was shown that ECR plasmas were toroidally homogeneous on the HT-7 tokamak, and the radial position of ECR plasmas was controlled by adjusting the toroidal magnetic field. Moreover, ECR plasmas were more localized by imposing a vertical field. In the experiment, RF powers made the difference, whereas higher pressure brought better cleaning. It was also observed that ECR discharge cleaning in deuterium resulted in a higher removal rate than that in helium under similar parameters. It was shown that the removal rate of hydrogen in ECR discharge cleaning is 5?10 times lower than that in ion cyclotron resonance (ICR) discharge cleaning.


Review of Scientific Instruments | 2016

Mass separation of deuterium and helium with conventional quadrupole mass spectrometer by using varied ionization energy

Yaowei Yu; Jiansheng Hu; Zhao Wan; Jinhua Wu; Wang H; Bin Cao

Deuterium pressure in deuterium-helium mixture gas is successfully measured by a common quadrupole mass spectrometer (model: RGA200) with a resolution of ∼0.5 atomic mass unit (AMU), by using varied ionization energy together with new developed software and dedicated calibration for RGA200. The new software is developed by using MATLAB with the new functions: electron energy (EE) scanning, deuterium partial pressure measurement, and automatic data saving. RGA200 with new software is calibrated in pure deuterium and pure helium 1.0 × 10(-6)-5.0 × 10(-2) Pa, and the relation between pressure and ion current of AMU4 under EE = 25 eV and EE = 70 eV is obtained. From the calibration result and RGA200 scanning with varied ionization energy in deuterium and helium mixture gas, both deuterium partial pressures (P(D2)) and helium partial pressure (P(He)) could be obtained. The result shows that deuterium partial pressure could be measured if P(D2) > 10(-6) Pa (limited by ultimate pressure of calibration vessel), and helium pressure could be measured only if P(He)/P(D2) > 0.45, and the measurement error is evaluated as 15%. This method is successfully employed in EAST 2015 summer campaign to monitor deuterium outgassing/desorption during helium discharge cleaning.

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Jiansheng Hu

Chinese Academy of Sciences

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X. Gao

Chinese Academy of Sciences

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J.S. Hu

Chinese Academy of Sciences

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Jiangang Li

Chinese Academy of Sciences

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J.G. Li

Chinese Academy of Sciences

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X.Z. Gong

Chinese Academy of Sciences

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Guang-Nan Luo

Chinese Academy of Sciences

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Baonian Wan

Chinese Academy of Sciences

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Bin Cao

Chinese Academy of Sciences

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