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Journal articles on the topic 'Lhcd'

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Published: 8 June 2024

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1

Shi, Bo, Zhen-Dong Yang, Bin Zhang, Cheng Yang, Kai-Fu Gan, Mei-Wen Chen, Jin-Hong Yang, et al. "Heat Flux on EAST Divertor Plate in H-mode with LHCD/LHCD+NBI." Chinese Physics Letters 34, no. 9 (August 2017): 095201. http://dx.doi.org/10.1088/0256-307x/34/9/095201.

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2

Hao, Xu, and Yi Yun Huang. "The Design of High Voltage DC Power Supply of 4.6GHZ/500MW LHCD." Applied Mechanics and Materials 135-136 (October 2011): 1027–36. http://dx.doi.org/10.4028/www.scientific.net/amm.135-136.1027.

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The steady-state and transient performances of the power supply system of LHCD (Lower Hybrid Current Drive) heating system are highly demanded which makes it difficult to design the power source. In this thesis, the method of designing the 4.6GHZ/6MW power source of LHCD of EAST is discussed. And the results of the experiment are provided and some special characteristics are analysed to prove the accuracy of the method.

3

Sharma, P. K., D. Raju, S. K. Pathak, R. Srinivasan, K. K. Ambulkar, P. R. Parmar, C. G. Virani, et al. "Current drive experiments in SST1 tokamak with lower hybrid waves." Nuclear Fusion 62, no. 5 (March 28, 2022): 056020. http://dx.doi.org/10.1088/1741-4326/ac4297.

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Abstract The steadystate superconducting tokamak (SST1) is aimed to demonstrate long pulse plasma discharges employing non-inductive current drive by means of lower hybrid current drive (LHCD) system. The major and minor radius of the machine is 1.1 m and 0.2 m, respectively. The LHCD system for SST1 comprises of klystrons, each rated for 0.5 MW-CW rf power at a frequency of 3.7 GHz. The grill antenna comprises of two rows, each row accommodating 32 waveguide elements. Electron cyclotron resonance breakdown assisted Ohmic plasma is formed in SST1 to overcome the issues associated with low loop voltage start-ups. With recent modifications in the poloidal coils configuration, even with narrow EC pulse (∼50 ms), good repeatable and consistent Ohmic plasmas could be produced which helped in carrying out LHCD current drive experiments on SST1. These experiments demonstrated both fully as well as partially driven non-inductive plasma current in SST1 tokamak. Discharges with zero loop voltages were obtained. The interaction of lower hybrid waves with plasma and generation of suprathermal electrons could be established using energy spectra measured by CdTe detectors. Various other signatures like drop in loop voltages, negative loop voltages, spikes in hard x-rays and increase in second harmonic ECE signal, further confirmed the current drive by LHW’s. The beneficial effect of LHW’s in suppressing hard x-rays was also demonstrated in these experiments. The longest discharge of ∼650 ms could be obtained in SST1 with the help of LHW’s. In this paper, the experimental results obtained with LHCD experiments on SST1 is reported and discussed in more details.

4

Bing-ren, Shi. "Electron Heating in Tokamak LHCD Experiment." Plasma Science and Technology 2, no. 5 (October 2000): 423–29. http://dx.doi.org/10.1088/1009-0630/2/5/001.

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5

Bibet, Ph, B. Beaumont, J. H. Belo, L. Delpech, A. Ekedahl, G. Granucci, F. Kazarian, et al. "Toward a LHCD system for ITER." Fusion Engineering and Design 74, no. 1-4 (November 2005): 419–23. http://dx.doi.org/10.1016/j.fusengdes.2005.06.014.

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6

Pi, Xiong, Lirong Tian, Huai-En Dai, Xiaochun Qin, Lingpeng Cheng, Tingyun Kuang, Sen-Fang Sui, and Jian-Ren Shen. "Unique organization of photosystem I–light-harvesting supercomplex revealed by cryo-EM from a red alga." Proceedings of the National Academy of Sciences 115, no. 17 (April 9, 2018): 4423–28. http://dx.doi.org/10.1073/pnas.1722482115.

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Photosystem I (PSI) is one of the two photosystems present in oxygenic photosynthetic organisms and functions to harvest and convert light energy into chemical energy in photosynthesis. In eukaryotic algae and higher plants, PSI consists of a core surrounded by variable species and numbers of light-harvesting complex (LHC)I proteins, forming a PSI-LHCI supercomplex. Here, we report cryo-EM structures of PSI-LHCR from the red alga Cyanidioschyzon merolae in two forms, one with three Lhcr subunits attached to the side, similar to that of higher plants, and the other with two additional Lhcr subunits attached to the opposite side, indicating an ancient form of PSI-LHCI. Furthermore, the red algal PSI core showed features of both cyanobacterial and higher plant PSI, suggesting an intermediate type during evolution from prokaryotes to eukaryotes. The structure of PsaO, existing in eukaryotic organisms, was identified in the PSI core and binds three chlorophylls a and may be important in harvesting energy and in mediating energy transfer from LHCII to the PSI core under state-2 conditions. Individual attaching sites of LHCRs with the core subunits were identified, and each Lhcr was found to contain 11 to 13 chlorophylls a and 5 zeaxanthins, which are apparently different from those of LHCs in plant PSI-LHCI. Together, our results reveal unique energy transfer pathways different from those of higher plant PSI-LHCI, its adaptation to the changing environment, and the possible changes of PSI-LHCI during evolution from prokaryotes to eukaryotes.

7

Esterkin, A. R., and A. D. Piliya. "Fast ray tracing code for LHCD simulations." Nuclear Fusion 36, no. 11 (November 1996): 1501–12. http://dx.doi.org/10.1088/0029-5515/36/11/i05.

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8

Ding, Bojiang, Erhua Kong, Miaohui Li, Yongliang Qin, Lei Zhang, Mao Wang, Handong Xu, et al. "Recent Results of LHCD Experiments in EAST." Plasma Science and Technology 13, no. 2 (April 2011): 153–56. http://dx.doi.org/10.1088/1009-0630/13/2/05.

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9

Park, S., H. Do, J. H. Jeong, W. Namkung, M. H. Cho, H. Park, Y. S. Bae, et al. "Development status of KSTAR 5GHz LHCD system." Fusion Engineering and Design 85, no. 2 (April 2010): 197–204. http://dx.doi.org/10.1016/j.fusengdes.2009.12.004.

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10

Wu, Qiuran, Peng Lu, Yu Zheng, Hua Du, Liang Liu, Qingjun Zhu, and Songlin Liu. "Neutronics assessments of LHCD antenna system for CFETR." Fusion Engineering and Design 172 (November 2021): 112877. http://dx.doi.org/10.1016/j.fusengdes.2021.112877.

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11

Maebara, Sunao, Masami Seki, Yoshitaka Ikeda, Satoshi Suzuki, Kenji Yokoyama, Kazuaki Suganuma, Kimihiro Kiyono, et al. "Development of plasma facing component for LHCD antenna." Fusion Engineering and Design 39-40 (September 1998): 355–61. http://dx.doi.org/10.1016/s0920-3796(97)00183-x.

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12

Kazarian, F., B. Beaumont, E. Bertrand, L. Delpech, S. Dutheil, C. Goletto, M. Prou, A. Beunas, F. Peauger, and Ph Thouvenin. "Developing the next LHCD source for Tore Supra." Fusion Engineering and Design 74, no. 1-4 (November 2005): 425–29. http://dx.doi.org/10.1016/j.fusengdes.2005.06.065.

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13

Kim, Jeehyun, Hyunho Wi, Mi Joung, Sonjong Wang, and Julien Hillairet. "High field side LHCD launcher study for KSTAR." Fusion Engineering and Design 146 (September 2019): 406–10. http://dx.doi.org/10.1016/j.fusengdes.2018.12.078.

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14

Ambulkar, K. K., P. K. Sharma, C. G. Virani, P. R. Parmar, A. L. Thakur, and S. V. Kulkarni. "Measurement of LHCD antenna position in Aditya tokamak." Journal of Physics: Conference Series 208 (February 1, 2010): 012025. http://dx.doi.org/10.1088/1742-6596/208/1/012025.

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15

Sharma, P. K. "Advances In LHCD System For SST-1 Tokamak." Fusion Science and Technology 65, no. 1 (January 2014): 103–19. http://dx.doi.org/10.13182/fst13-639.

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16

Liu, Liang, Yong Yang, Miaohui Li, Lianmin Zhao, Wendong Ma, Tai'an Zhou, Chengzhou Liu, et al. "Conceptual design of the LHCD system on CFETR." Fusion Engineering and Design 189 (April 2023): 113444. http://dx.doi.org/10.1016/j.fusengdes.2023.113444.

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17

Jiao Yi-Ming, Long Yong-Xing, Dong Jia-Qi, Shi Bing-Ren, and Gao Qing-Di. "Effects of the trapping effect on LHCD in tokamak." Acta Physica Sinica 54, no. 1 (2005): 180. http://dx.doi.org/10.7498/aps.54.180.

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18

Wallace, G. M., F. Poli, M. A. Chilenski, J. W. Hughes, R. T. Mumgaard, S. D. Scott, S. Shiraiwa, and S. J. Wukitch. "LHCD during current ramp experiments on Alcator C-Mod." EPJ Web of Conferences 157 (2017): 03063. http://dx.doi.org/10.1051/epjconf/201715703063.

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19

Xu, Li-Qing, Li-Qun Hu, Kai-Yun Chen, and Miao-Hui Li. "Compound sawtooth in EAST LHCD plasma: An experimental study." Chinese Physics B 23, no. 8 (July 31, 2014): 085201. http://dx.doi.org/10.1088/1674-1056/23/8/085201.

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20

朱, 学光. "The 3D Model of Antenna Coupling in LHCD System." Modern Physics 02, no. 03 (2012): 38–42. http://dx.doi.org/10.12677/mp.2012.23007.

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21

Jian-an, Lin, Kuang Guang-li, Liu Yue-xiu, Shan Jia-fang, Liu Den-cheng, Shang Lian-quan, Yu Jia-wen, Huang Yi-yun, Zheng Guang-hua, and Shen Wei-ci. "Composition of HT-7 LHCD and its Protection Systems." Plasma Science and Technology 3, no. 6 (December 2001): 1075–84. http://dx.doi.org/10.1088/1009-0630/3/6/010.

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22

Wei, Wei, Ding Bojiang, and Kuang Guangli. "Numerical Simulation of Modified Radial Electric Field by LHCD." Plasma Science and Technology 7, no. 2 (April 2005): 2723–26. http://dx.doi.org/10.1088/1009-0630/7/2/007.

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23

Yonghua, Ding, Wan Baonian, Lin Shiyao, Chen Zhongyong, Hu Xiwei, Shi Yuejiang, Hu Liqun, Kong Wei, and Zhang Xiaoqing. "Electron Heating of LHCD Plasma in HT-7 Tokamak." Plasma Science and Technology 8, no. 4 (July 2006): 390–93. http://dx.doi.org/10.1088/1009-0630/8/4/04.

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24

Baranov, Yu F., C. Bourdelle, T. Bolzonella, M. De Baar, C. D. Challis, C. Giroud, N. C. Hawkes, E. Joffrin, and V. Pericoli Ridolfini. "Effect of hysteresis in JET ITB plasma with LHCD." Plasma Physics and Controlled Fusion 47, no. 7 (May 31, 2005): 975–93. http://dx.doi.org/10.1088/0741-3335/47/7/002.

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25

Chouli, B., C. Fenzi, X. Garbet, C. Bourdelle, Y. Sarazin, J. Rice, T. Aniel, et al. "Investigations of LHCD induced plasma rotation in Tore Supra." Plasma Physics and Controlled Fusion 57, no. 12 (October 16, 2015): 125007. http://dx.doi.org/10.1088/0741-3335/57/12/125007.

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26

Belo, J. H., Ph Bibet, M. Missirlian, J. Achard, B. Beaumont, B. Bertrand, M. Chantant, et al. "ITER-like PAM launcher for Tore Supra's LHCD system." Fusion Engineering and Design 74, no. 1-4 (November 2005): 283–88. http://dx.doi.org/10.1016/j.fusengdes.2005.06.173.

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27

Portafaix, C., P. Bibet, J. H. Belo, A. Boué, M. Chantant, L. Delpech, A. Ekedahl, J. P. Gaston, and M. Goniche. "Thermal behavior of the LHCD launchers in Tore Supra." Fusion Engineering and Design 82, no. 5-14 (October 2007): 658–61. http://dx.doi.org/10.1016/j.fusengdes.2007.05.074.

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28

Kim, Jeehyun, Jongwon Han, Sonjong Wang, Julien Hillairet, Lena Delpech, Jong-gu Kwak, Won Namkung, and Moohyun Cho. "Mid-plane PAM launcher study for KSTAR LHCD system." Fusion Engineering and Design 144 (July 2019): 29–39. http://dx.doi.org/10.1016/j.fusengdes.2019.04.045.

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29

Xu-dong, Cao, and Wang Zhong-tian. "Synergetic Effects of LHCD and ECCD in Tokamak Plasma." Communications in Theoretical Physics 10, no. 4 (December 1988): 485–89. http://dx.doi.org/10.1088/0253-6102/10/4/485.

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30

Hao, Xu, and Yi Yun Huang. "The Analysis and Simulation of PSM Single-Module Based on Simplorer." Applied Mechanics and Materials 135-136 (October 2011): 995–1001. http://dx.doi.org/10.4028/www.scientific.net/amm.135-136.995.

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The power supply system of the LHCD heating systems of Tokamak (EAST) is required to be reliable and have good dynamic performances. In this thesis, an optimization model of the Single-module of PSM power source is proposed to analyze its dynamic performances theoretically and the special simulation tools in SIMPLORER are used for the modeling and simulation of the system.

31

Rutherford, Grant, Andrew H. Seltzman, and Stephen J. Wukitch. "Predicted performance of a tangential viewing hard x-ray camera for the DIII-D high field side lower hybrid current drive experiment." Review of Scientific Instruments 93, no. 10 (October 1, 2022): 103529. http://dx.doi.org/10.1063/5.0099168.

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High field side launch of lower hybrid current drive (LHCD) has improved accessibility and penetration over low field side launch on DIII-D. Simulations predict single pass absorption under a wide range of plasma conditions. Hard x-ray (HXR) measurement of LHCD generated fast electron bremsstrahlung (50–250 keV) will validate wave propagation and absorption. Emissivity profiles are recovered from one-dimensional inversion of HXR brightness to determine LH damping location, fast electron slowing down time, and some indication of the fast electron energy. The camera will be implemented by populating 32 tangential sightlines of the existing Gamma Ray Imager with Kromek SPEARTM Cadmium Zinc Telluride (CZT) detectors sensitive to 10–1000 keV photons with 10 keV energy resolution. Expected count rates allow for <0.5 ms time resolution. Pulses are processed using 50 ns shaping time Cremat CR-200 Gaussian shaping modules and are digitized by 25 MHz D-TACQ ACQ216 digitizers. The performance of the HXR camera is evaluated by comparing predicted fast electron density profiles and inverted synthetic brightnesses obtained from the ray-tracing/Fokker–Planck codes GENRAY/CQL3D. Inversions closely matched predicted fast electron profiles for a range of experimental parameters.

32

Barbui, T., O. Chellaï, L. F. Delgado-Aparicio, Y. Peysson, B. Stratton, R. Dumont, K. W. Hill, and N. A. Pablant. "Spatial calibration and synthetic diagnostic of a multi-energy hard x-ray camera at WEST tokamak." Review of Scientific Instruments 93, no. 10 (October 1, 2022): 103508. http://dx.doi.org/10.1063/5.0101794.

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WEST (tungsten environment in steady-state tokamak) is starting operation for the first time with a water-cooled full tungsten divertor, enabling long pulse operation. Heating is provided by radiofrequency systems, including lower hybrid current drive (LHCD). In this context, a compact multi-energy hard x-ray camera has been installed for energy and space-resolved measurements of the electron temperature, the fast electron tail density produced by LHCD and runaway electrons, and the beam–target emission of tungsten at the target due to fast electron losses interacting with the divertor plates. The diagnostic is a pinhole camera based on a 2D pixel array detector (Pilatus 3 CdTe CMOS Hybrid-Pixel detector produced by DECTRIS). The novelty of this diagnostic technique is the detector’s capability of adjusting the threshold energy at pixel level. This innovation provides great flexibility in the energy configuration, allowing simultaneous space and energy-resolved x-ray measurements. This contribution details two important steps in the preparation of the diagnostic operation. First, the in-vessel spatial calibration that was carried out with a radioactive source. Second, the synthetic diagnostic is obtained by the suite of codes ALOHA/C3PO/LUKE/R5-X2, which simulates LH wave propagation and absorption, as well as the fast electron bremsstrahlung production.

33

Lu, B., M. Huang, H. Zeng, X. Y. Bai, X. H. Mao, Z. H. Lu, J. Liang, et al. "Development of the 3.7 GHz LHCD system on HL-2A." Journal of the Korean Physical Society 65, no. 8 (October 2014): 1243–46. http://dx.doi.org/10.3938/jkps.65.1243.

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34

Kupfer, K., and D. Moreau. "Wave chaos and the dependence of LHCD efficiency on temperature." Nuclear Fusion 32, no. 10 (October 1992): 1845–51. http://dx.doi.org/10.1088/0029-5515/32/10/i12.

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35

Guang-li, Kuang. "Ion heating effects in LHCD sustained low density tokamak plasmas." Acta Physica Sinica (Overseas Edition) 8, no. 1 (January 1999): 32–39. http://dx.doi.org/10.1088/1004-423x/8/1/006.

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36

Tuccillo, A. A., E. Barbato, Y. S. Bae, A. Becoulet, S. Bernabei, P. Bibet, G. Calabrò, et al. "Progress in LHCD: a tool for advanced regimes on ITER." Plasma Physics and Controlled Fusion 47, no. 12B (November 7, 2005): B363—B377. http://dx.doi.org/10.1088/0741-3335/47/12b/s26.

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37

Mirizzi, F., Ph Bibet, and S. Kuzikov. "The main microwave components of the LHCD system for ITER." Fusion Engineering and Design 66-68 (September 2003): 487–90. http://dx.doi.org/10.1016/s0920-3796(03)00081-4.

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38

Mirizzi, F., Ph Bibet, G. Calabrò, V. Pericoli Ridolfini, and A. A. Tuccillo. "PAM, multijunction and conventional LHCD grills: Operational experience on FTU." Fusion Engineering and Design 82, no. 5-14 (October 2007): 751–57. http://dx.doi.org/10.1016/j.fusengdes.2007.05.068.

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39

Marfisi, L., M. Goniche, C. Hamlyn-Harris, J. Hillairet, J. F. Artaud, Y. S. Bae, J. Belo, et al. "Thermal and mechanical analysis of ITER-relevant LHCD antenna elements." Fusion Engineering and Design 86, no. 6-8 (October 2011): 810–14. http://dx.doi.org/10.1016/j.fusengdes.2011.01.025.

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40

Yamagiwa, Mitsuru, Toshinori Michishita, and Masao Okamoto. "Numerical Calculation on a Mechanism of Current Sustainment during LHCD." Journal of the Physical Society of Japan 54, no. 6 (June 15, 1985): 2146–54. http://dx.doi.org/10.1143/jpsj.54.2146.

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41

Liu, L., F. K. Liu, H. Jia, W. H. Zhu, L. M. Zhao, X. J. Wang, J. F. Shan, et al. "4.6-GHz LHCD Launcher System of Experimental Advanced Superconducting Tokamak." Fusion Science and Technology 75, no. 1 (November 2, 2018): 49–58. http://dx.doi.org/10.1080/15361055.2018.1516416.

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42

Ageladarakis, P. A., N. P. O'Dowd, G. A. Webster, and S. Papastergiou. "Theoretical and experimental simulation of accident scenarios of the Joint European Torus cryogenic components Part 2: The Lower Hybrid Current Drive cryopump." Proceedings of the Institution of Mechanical Engineers, Part C: Journal of Mechanical Engineering Science 212, no. 6 (June 1, 1998): 525–30. http://dx.doi.org/10.1243/0954406981521411.

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A flexible mathematical model has been developed in Part 1 to simulate the transient thermal response of a number of nuclear fusion components, including cryogenic devices that operate inside the JET Tokamak. The present work reports on the simulation of an accident scenario, as well as further studies of hypothetical off-normal scenarios concerning an out-of-vessel cryopump (the LHCD cryopump). These studies resulted in a complete safety protection system for the cryopump, which has been implemented into the JET operating routines.

43

SHI BING-REN. "ANALYTIC STUDY OF LOWER HYBRID WAVE PROPAGATION IN TOKAMAK LHCD EXPERIMENTS." Acta Physica Sinica 49, no. 12 (2000): 2394. http://dx.doi.org/10.7498/aps.49.2394.

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44

Yi, Liu, Qiu Xiao-Ming, Dong Yun-Bo, Guo Gan-Cheng, Zhong Yun-Ze, Fu Bing-Zhong, and Liu Yong. "Sawtooth-Stabilization and Snake-Excitation during LHCD on the HL-1M." Chinese Physics Letters 21, no. 2 (February 2004): 360–63. http://dx.doi.org/10.1088/0256-307x/21/2/041.

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45

Bonoli, P. T., R. R. Parker, M. Porkolab, J. J. Ramos, S. J. Wukitch, Y. Takase, S. Bernabei, J. C. Hosea, G. Schilling, and J. R. Wilson. "Modelling of advanced tokamak scenarios with LHCD in Alcator C-Mod." Nuclear Fusion 40, no. 6 (June 2000): 1251–56. http://dx.doi.org/10.1088/0029-5515/40/6/319.

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46

Nakamura, K., S. Itoh, H. Zushi, M. Sakamoto, K. Hanada, E. Jotaki, Y. D. Pan, S. Kawasaki, and H. Nakashima. "Current profile control experiments in the LHCD plasma on TRIAM-1M." Nuclear Fusion 42, no. 3 (March 1, 2002): 340–43. http://dx.doi.org/10.1088/0029-5515/42/3/315.

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47

Zheng-ying, Cui, Osamu Naito, Takeshi Fukudai, Hiroshi Shirai, Yoshitaka Ikeda, and Kenkichi Ushigusa. "Simulation Study on the ITB Formation during LHCD in JT-60U." Plasma Science and Technology 4, no. 2 (April 2002): 1197–206. http://dx.doi.org/10.1088/1009-0630/4/2/004.

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48

Min, Jiang, Kuang Guangli, Shan Jiafang, Jian'an Lin, Kong Jun, and HT-7. Team. "Feedback Control System for Antenna Phase Difference in the LHCD Experiments." Plasma Science and Technology 7, no. 6 (December 2005): 3107–10. http://dx.doi.org/10.1088/1009-0630/7/6/007.

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49

Yiming, Jiao, Dong Jiaqi, Gao Qingdi, Wang Aike, and Liu Yong. "Study of LHCD in HL-2A Non-Circular Cross Section Tokamak." Plasma Science and Technology 9, no. 1 (February 2007): 19–22. http://dx.doi.org/10.1088/1009-0630/9/1/05.

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50

Xiaojie, Wang, Liu Fukun, Jia Hua, and Kuang Guangli. "Design of a TE10Taper Used in the LHCD Launcher for EAST." Plasma Science and Technology 10, no. 4 (August 2008): 499–502. http://dx.doi.org/10.1088/1009-0630/10/4/20.

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