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Ideal MHD Stability Prediction and Required Power for EAST Advanced Scenario

Ideal MHD Stability Prediction and Required Power for EAST Advanced Scenario
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摘要 The Experimental Advanced Superconducting Tokamak (EAST) is the first fully superconducting tokamak with a D-shaped cross-sectional plasma presently in operation. The ideal magnetohydrodynamic (MHD) stability and required power for the EAST advanced tokamak (AT) scenario with negative central shear and double transport barrier (DTB) are investigated. With the equilibrium code TOQ and stability code GATO, the ideal MHD stability is analyzed. It is shown that a moderate ratio of edge transport barriers' (ETB) height to internal transport barriers' (ITBs) height is beneficial to ideal MHD stability. The normalized beta/3N limit is about 2.20 (without wall) and 3.70 (with ideal wall). With the scaling law of energy confinement time, the required heating power for EAST AT scenario is calculated. The total heating power Pt increases as the toroidal magnetic field BT or the normalized beta βN is increased. The Experimental Advanced Superconducting Tokamak (EAST) is the first fully superconducting tokamak with a D-shaped cross-sectional plasma presently in operation. The ideal magnetohydrodynamic (MHD) stability and required power for the EAST advanced tokamak (AT) scenario with negative central shear and double transport barrier (DTB) are investigated. With the equilibrium code TOQ and stability code GATO, the ideal MHD stability is analyzed. It is shown that a moderate ratio of edge transport barriers' (ETB) height to internal transport barriers' (ITBs) height is beneficial to ideal MHD stability. The normalized beta/3N limit is about 2.20 (without wall) and 3.70 (with ideal wall). With the scaling law of energy confinement time, the required heating power for EAST AT scenario is calculated. The total heating power Pt increases as the toroidal magnetic field BT or the normalized beta βN is increased.
出处 《Plasma Science and Technology》 SCIE EI CAS CSCD 2012年第11期947-952,共6页 等离子体科学和技术(英文版)
基金 supported by the National Natural Science Foundation of China (No.10975161) the Special Project of the Ministry of Science and Technology of China (No.2009GB101001)
关键词 ideal MHD BETA AT ITB ETB ideal MHD, beta, AT, ITB, ETB
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  • 1Goldston R J, Batha S H, Bulmer R H, et al. 1994 Plasma Phys. Control. Fusion, 36:B213. 被引量:1
  • 2Taylor T S. 1997, Plasma Phys. Control. Fusion, 39 B47. 被引量:1
  • 3Shimada M, Campbell D J, Mukhovatov V, et al. 2007 Nucl. Fusion, 47:S1. 被引量:1
  • 4Rice B W, Burrell K H, Lao L L, et al. 1996, Phys Plasmas, 3:1983. 被引量:1
  • 5Gruber O, Wolf R C, Dux R, et al. 1999, Phys. Rev Lett., 83:1787. 被引量:1
  • 6Gruber O, Wolf R, Bosch H S, et al. 2000, Nucl. Fu- sion, 40:1145. 被引量:1
  • 7Greenfield C M, Burrell K H, DeBoo J C, et al. 2001, Phys. Rev. Lett., 86:4544. 被引量:1
  • 8Perkins F W, Post D E, Uckan N A, et al. 1999, Nucl. Fusion, 39:2137. 被引量:1
  • 9Miller R L and Van Dam. 1987, Nucl. Fusion, 27:2101. 被引量:1
  • 10Miller R L, Lin-Liu Y R, Turnbull A D, et al. 1997, Phys. Plasmas, 4:1062. 被引量:1

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