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多装置ELM能量定标及向SPARC与ITER外推的第一步

First step toward multi machine ELM energy scalings and extrapolations to SPARC and ITER

R. Perillo, A. Redl, T. Eich, C. J. Lasnier, A. Nelson, R. Rizkallah, D. Silvagni, A. Stagni, J. A. Boedo, A. McLean, P. Traverso, N. Vianello, the DIII-D team, JET contributors, the ASDEX Upgrade team, the TCV team, the EUROfusion Tokamak Exploitation team

arXiv 2608.21179首次发表:更新:

AI 中文总结

本研究基于7台托卡马克的多装置数据库,建立了I型与小/QCE型ELM的能量损失定标关系,完成了向SPARC和ITER相关工况的初步外推,为未来反应堆工况预测提供了基础。

AI 中文摘要

研究表明,高密度小/QCE(准连续)ELM(边缘局域模)工况下,经等离子体储能归一化的ELM能量损失(ΔEELM/Wplasma)与分界面湍流参数α_t呈反比关系。相比之下,根据Loarte定标律(《Plasma Phys. Control. Fusion》2003年第45卷第1549页),台基顶部的新经典电子碰撞率ν*e,neo本应调控ΔEELM/Wplasma,但它无法充分匹配剥离气球模受限的I型ELM、以及气球模受限的小/QCE ELM的ΔEELM/Wplasma数据,这限制了其仅适用于单一工况窗口的外推。本研究分析了涵盖7台托卡马克的多装置数据库,其中ΔEELM/Wplasma范围为0.5%至14%。仅针对I型ELM的回归分析得到定标关系:((ΔE_ELM)/W_plasma )_(Type-I ) [%]=6.8*T_(e,ped)^0.03 n_(e,ped)^(-0.4) κ^(-0.4) R_major^0.4,代入标称SPARC台基参数时ΔEELM/Wplasma为4.5%,对应ITER D-T Q=10工况时为12%。而对于小/QCE ELM类别,随着α_t增大,台基向气球模受限边界移动,环向模数增加,ELM频率遵循f_ELM=46e^((2.25*α_t))的定标关系上升,ΔEELM/Wplasma则通过关系式(ΔE_ELM)/W_plasma [%]=1.6e^(-(α_t/2))下降。对于SPARC QCE相关的α_t=0.86以及ITER高加料工况的α_t=0.64,该定标律预测的ΔEELM/Wplasma分别为1.0%和1.2%,结果较为理想;若将小/QCE ELM工况推至α_t>1,该值会低于1%。小/QCE ELM的拟合结果是未来开展更广泛数据集分析的初步一步,而这类分析对提升未来反应堆相关工况预测的准确性是必要的。

英文摘要

It is shown that the ELM energy loss normalized by the plasma stored energy (ΔEELM/Wplasma) for high-density small/QCE ELM regimes scales inversely with the separatrix turbulence parameter a_t. In contrast, the neoclassical electron collisionality at the pedestal top, nu*e,neo, expected to regulate ΔEELM/Wplasma according to the Loarte scaling (Plasma Phys. Control. Fusion 2003 45 1549), does not adequately capture ΔEELM/Wplasma data for peeling-ballooning-limited type-I ELMs and ballooning-limited small/QCE ELMs, limiting its applicability for extrapolation to one scenario window. A multi-machine database including seven tokamaks and with ΔEELM/Wplasma ranging from 0.5% to 14%, has been analyzed. A regression analysis on only type-I ELMs yields ((ΔE_ELM)/W_plasma )_(Type-I ) [%]=6.8*T_(e,ped)^0.03 n_(e,ped)^(-0.4) \k{appa}^(-0.4) R_major^0.4, corresponding to ΔEELM/Wplasma =4.5% for nominal SPARC pedestal parameters and 12% for the ITER D-T Q=10 scenario. For the small/QCE ELM class, however, as a_t increases, the pedestal moves toward a ballooning-limited boundary, the toroidal mode number increases, the ELM frequency rises following the scaling f_ELM=46e^((2.25*a_t)), and ΔEELM/Wplasma decreases via the relation (ΔE_ELM)/W_plasma [%]=1.6e^(-(α_t/2)). For SPARC QCE-relevant a_t=0.86 and ITER high-fueling scenario a_t = 0.64, the scaling favorably predicts ΔEELM/Wplasma of 1.0% and 1.2%, respectively, with values below 1% if the small/QCE ELM regime is pushed beyond a_t >1. The small/QCE ELM-fitted results represent an initial step toward future analysis on broader datasets, which will be necessary to improve the accuracy of projections for future reactor-relevant scenarios.

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