Simulation of edge-divertor plasma transport for high-performance operation in KSTAR
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作者:
Han, Hyunsun
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Natl Fus Res Inst, Taejon 305806, South Korea
Seoul Natl Univ, Dept Nucl Engn, Seoul 151742, South KoreaNatl Fus Res Inst, Taejon 305806, South Korea
Han, Hyunsun
[1
,3
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Kim, Ki Min
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Princeton Plasma Phys Lab, Princeton, NJ 08543 USANatl Fus Res Inst, Taejon 305806, South Korea
Kim, Ki Min
[2
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Park, Jin-Woo
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Seoul Natl Univ, Dept Nucl Engn, Seoul 151742, South KoreaNatl Fus Res Inst, Taejon 305806, South Korea
Park, Jin-Woo
[3
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Hong, Sang Hee
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Seoul Natl Univ, Dept Nucl Engn, Seoul 151742, South KoreaNatl Fus Res Inst, Taejon 305806, South Korea
Hong, Sang Hee
[3
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Kwon, Ohjin
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Daegu Univ, Dept Phys, Gyeongbuk 712714, South KoreaNatl Fus Res Inst, Taejon 305806, South Korea
Kwon, Ohjin
[4
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Na, Yong-Su
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Seoul Natl Univ, Dept Nucl Engn, Seoul 151742, South KoreaNatl Fus Res Inst, Taejon 305806, South Korea
Na, Yong-Su
[3
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机构:
[1] Natl Fus Res Inst, Taejon 305806, South Korea
[2] Princeton Plasma Phys Lab, Princeton, NJ 08543 USA
[3] Seoul Natl Univ, Dept Nucl Engn, Seoul 151742, South Korea
[4] Daegu Univ, Dept Phys, Gyeongbuk 712714, South Korea
The edge-divertor plasma transport responding to type-I edge localized modes (ELMs) in a hybrid scenario and a conventional H-mode operation of the KSTAR (Korea Superconducting Tokamak Advanced Research) tokamak is simulated using a newly developed two-dimensional fluid code named 'EPST', which can be used in time-dependent analyses of the edge-private flux-scrape-off layer region. It is verified through a benchmark test with the B2.5 code for a double-null configuration of the KSTAR tokamak. In this simulation, the KSTAR operation modes are distinguished by their beta(N) values and the threshold pedestal heights for ELM triggering. Type-I ELMs are simulated under the ELM triggering condition by an ad hoc method of time-periodic changes in the transport coefficients in the near-separatrix region. As a result of numerical simulation, the overall distributions of plasma properties responding to the ELM bursts appear to be the same in the edge-divertor region regardless of their beta(N). However, the increased ballooning limit in the higher beta(N) case makes the ELM frequency become lower, while it makes the maximum heat flux on the divertor plate higher compared with the lower beta(N) case.
机构:
Chinese Acad Sci, Inst Plasma Phys, Hefei 230031, Peoples R China
Chinese Acad Sci, Ctr Magnet Fus Theory, Hefei 230031, Peoples R ChinaChinese Acad Sci, Inst Plasma Phys, Hefei 230031, Peoples R China
Ou Jing
Yang Jin-Hong
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Chinese Acad Sci, Inst Plasma Phys, Hefei 230031, Peoples R ChinaChinese Acad Sci, Inst Plasma Phys, Hefei 230031, Peoples R China