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MHD limits and plasma response in high-beta hybrid operations in ASDEX Upgrade

机译:ASDEX升级中高β混合操作中的MHD限制和血浆响应

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The improved H-mode scenario (or high β hybrid operations) is one of the main candidates for high-fusion performance tokamak operation that offers a potential steady-state scenario. In this case, the normalized pressure must be maximized and pressure-driven instabilities will limit the plasma performance. These instabilities could have either resistive ((m = 2, n = 1) and (3,2) neoclassical tearing modes (NTMs)) or ideal character (n = 1 ideal kink mode). In ASDEX Upgrade (AUG), the first limit for maximum achievable β_n is set by the NTMs. The application of pre-emptive electron cyclotron current drive at the q = 2 and q = 1.5 resonant surfaces reduces this problem, so that higher values of β_n can be reached. AUG experiments have shown that, in spite of the fact that hybrids are mainly limited by NTMs, the proximity to the no-wall limit leads to amplification of the external fields that strongly influence the plasma profiles. For example, rotation braking is observed throughout the plasma and peaks in the core. In this situation, even small external fields are amplified and their effect becomes visible. To quantify these effects, the plasma response to the magnetic fields produced by B-coils is measured as β_n approaches the no-wall limit. These experiments and corresponding modeling allow the identification of the main limiting factors, which depend on the stabilizing influence of the conducting components facing the plasma surface, the existence of external actuators, and the kinetic interaction between the plasma and the marginally stable ideal modes. Analysis of the plasma reaction to external perturbations allowed us to identify optimal correction currents for compensating the intrinsic error field in the device. Such correction, together with the analysis of kinetic effects, will help to increase further in β_n future experiments.
机译:改进的H模式方案(或高β混合操作)是高融合性能托卡马克操作的主要候选方案之一,可提供潜在的稳态方案。在这种情况下,必须最大化标准化压力,并且压力驱动的不稳定性将限制等离子体性能。这些不稳定性可能具有电阻性((m = 2,n = 1)和(3,2)新古典撕裂模式(NTM))或理想特性(n = 1理想扭结模式)。在ASDEX升级(AUG)中,最大可达到的β_n的第一个限制是由NTM设置的。在q = 2和q = 1.5谐振表面上应用抢先电子回旋加速器电流驱动可以减少此问题,从而可以实现更高的β_n值。 AUG实验表明,尽管杂种主要受NTM限制,但接近无壁限制会导致外部场放大,从而强烈影响血浆分布。例如,在整个等离子体中观察到旋转制动,并且在芯中达到峰值。在这种情况下,即使很小的外部场也被放大,并且它们的作用变得可见。为了量化这些影响,当β_n接近无壁极限时,测量对B线圈产生的磁场的等离子体响应。这些实验和相应的模型允许确定主要的限制因素,这些因素取决于面对等离子体表面的导电组件的稳定影响,外部致动器的存在以及等离子体与边际稳定理想模式之间的动力学相互作用。通过分析等离子体对外部扰动的反应,我们可以确定最佳的校正电流,以补偿器件中的固有误差场。这种校正以及动力学效应的分析将有助于在未来的实验中进一步增加。

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