Predictions of H-mode access and edge pedestal instability in the EHL-2 spherical torus

被引:0
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作者
王嵎民 [1 ,2 ]
李凯 [3 ]
黄卓 [4 ]
刘一良 [5 ]
戴舒宇 [5 ]
张洁 [6 ]
黄艳清 [7 ]
顾翔 [1 ,2 ]
赵毅航 [1 ,2 ]
徐帅 [8 ]
王二辉 [8 ]
郭栋 [1 ,2 ]
石跃江 [1 ,2 ]
谢华生 [1 ,2 ]
梁云峰 [1 ,8 ]
刘敏胜 [1 ,2 ]
the EHL Team [2 ,1 ,2 ]
机构
[1] Hebei Key Laboratory of Compact Fusion
[2] ENN Science and Technology Development Co, Ltd
[3] Centre for Theoretical and Computational Physics, College of Physics, Qingdao University
[4] College of Computer Science, South-Central Minzu University
[5] Key Laboratory of Materials Modification by Laser, Ion and Electron Beams (Ministry of Education),School of Physics, Dalian University of Technology
[6] Department of Plasma Physics and Fusion Engineering, University of Science and Technology of China
[7] College of Physics and Electronic Engineering, Hengyang Normal University
[8] Forschungszentrum Jülich GmbH, Institute of Fusion Energy and Nuclear Waste
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TL631.24 [];
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摘要
The EHL-2 spherical torus is designed to demonstrate proton-boron(p-11B) fusion within a compact spherical tokamak.Its planned heating system includes a negative ion-based neutral beam injection(N-NBI),two positive ion-based NBI systems(P-NBI),electron cyclotron resonance heating(ECRH),ion cyclotron resonance heating(ICRH),and high harmonic fast wave(HHFW),with a total power output of 31 MW.According to scaling law estimates,the device is capable of achieving H-mode operation.The plasma density,ne,min,at the minimum LH power threshold,PLH,is estimated to be 4.4× 1019 m-3.The pedestal parameters were calculated using the REPED model.Assuming B as the primary impurity ion,the predicted pedestal width and height are lower compared to the typical case with carbon impurities.The pedestal collisionality for EHL-2 is estimated to range between 0.06 and 0.17,indicating the potential for significant energy loss due to edge localized modes(ELMs).The heat flux on the divertor plate has been calculated using the JOREK code.The peak heat fluxes during ELM bursts are approximately 31.0 MW/m2 at the lower inboard target and 39.5 MW/m2 at the lower outboard target.A preliminary design of the resonant magnetic perturbation(RMP) coils has been completed to both control type-Ⅰ ELMs and correct error fields.The system comprises 16coils arranged into 2×4 pairs.In ELM control mode,a 14/2 component is generated at 1.7 G/kAt,with a current of 4.9 kA required to achieve σChirikov=1 at the resonant surface,where the normalized poloidal magnetic flux is 0.85.In error field(EF) modulation mode,2/1 and 3/1components are generated at 3.5 G/kAt and 2.8 G/kAt,respectively.
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页码:59 / 68
页数:10
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