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Numerical Investigation of Impurity Seeded Radiation Enhancement in the Divertor region with Magnetic Perturbations in ASDEX Upgrade

机译:随着ASDEX升级中磁性扰动的杂质地区杂质种子辐射增强的数值研究

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Introduction Currently one of the most promising concepts for future fusion devices, such as ITER and DEMO, is the divertor tokamak, in which power and particles leaving the confined region are transported to the divertor targets. The power flux to the targets can locally exceed the tolerable target heat flux limit and it is therefore required that a large fraction of the power is dissipated before reaching the target. It has been shown in various experiments that this goal can be achieved by seeding low to medium Z impurities [2]. In [3] an empirical scaling formula for the power radiated by the nitrogen impurities has been found that depends linearly on the power decay length λ_q [1]. One way to increase λ_q could be the application of Magnetic Perturbations (MPs). MP coils were introduced at ASDEX Upgrade (AUG) and a number of other tokamaks to study their mitigating effect on Edge Localized Modes (ELMs) [4], intermittent high power flux bursts which can pose a serious risk for the targets. MPs can change the magnetic topology strongly and lead to the formation of stochastic regions inside the separatrix and finger-like deformations of the separatrix, so called lobes. To study numerically how the application of MPs affects the impurity radiation in the SOL and divertor, the edge code EMC3-Eirene [5] was employed to simulate an AUG L-mode deuterium bulk plasma with and without MPs. Subsequently nitrogen seeding simulations were performed on these bulk plasmas and the impurity radiation distribution between the MP-on and off cases considered in detail.
机译:简介目前未来融合设备(例如迭代设备)的最有希望的概念之一是偏转器Tokamak,其中将留下限制区域的功率和颗粒被输送到转栓靶。目标的电源通量可以局部地超过可容许的目标热通量限制,因此要求在到达目标之前散发大部分电力。已经显示在各种实验中,即通过播种低至中Z杂质可以实现这种目标[2]。在[3]中,已经发现由氮杂质辐射的功率辐射的经验缩放公式,其在功率衰减长度λ_q[1]上线性取决于线性取决于λ_q[1]。增加λ_q的一种方法可以是磁性扰动(MPS)的应用。 MP线圈在Asdex升级(AUG)和一些其他托卡马克介绍,以研究它们对边缘局部模式(ELMS)的缓解效果[4],间歇高功率通量突发,这可能对目标构成严重风险。 MPS可以强烈地改变磁性拓扑,导致分离器内的随机区域和分离rix的指状变形,所以称为裂片。为了在数值上学习MPS如何影响溶胶和偏移器中的杂质辐射,所以采用边缘代码EMC3-烯烯[5]来模拟8月L模式的氘氘体等离子体,没有MPS。随后对这些散装等离子体进行氮播种模拟,并详细考虑的MP-ON和OFF病例之间的杂质辐射分布。

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