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Toroidal modelling of resonant magnetic perturbations response in ASDEX-Upgrade: coupling between field pitch aligned response and kink amplification

机译:ASDEX-Upgrade中共振磁扰动响应的环形建模:场距对准响应与扭结放大之间的耦合

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Using the MARS-F code (Liu et al 2000 Phys. Plasmas 7 3681), the single fluid resistive MHD plasma response to applied n = 2 resonant magnetic perturbations is computed, for a plasma discharge in the ASDEX-Upgrade tokamak. The computation predicts strong kink amplification, as previously predicted in DIII-D (Haskey et al 2014 Plasma Phys. Control. Fusion 56 035005), which is strongly dependent on the toroidal phase shift between the upper and lower coils, Delta phi(ul). In particular, edge localised low n peeling modes with poloidal mode numbers just above pitch resonance-a subset of the kink response-are amplified. The robustness of the amplified peeling response with respect to truncation of the X point is investigated, by recomputing the plasma response for a range of edge geometries. It is found that the computed peeling response, when plotted against the safety factor, is not sensitive to the numerical truncation near the X point. It is also predicted that near the plasma edge where resistivity is large, the pitch aligned components are finite and also strongly dependent on Delta phi(ul). A previous proposal that the amplified peeling response may indirectly drive the pitch aligned components by spectral proximity (Lanctot et al 2013 Nucl. Fusion 53 083019), is investigated by numerically applying magnetic perturbations of a single poloidal harmonic, as a boundary condition at the plasma edge. It is found that poloidal harmonic coupling causes harmonics to couple to and drive harmonics directly beneath them spectrally, and also that the pitch aligned components can be driven by this mechanism. This suggests that it is quite possible that the amplified low n peeling response can drive the pitch aligned components when it is strongly amplified, which would alter the coil configuration for optimum plasma stochastization, with implications for ELM control by RMPs.
机译:使用MARS-F代码(Liu等,2000 Phys.Plasmas 7 3681),针对在ASDEX-Upgrade托卡马克中的等离子体放电,计算了对施加的n = 2个共振磁扰动的单个流体电阻MHD等离子体响应。如先前在DIII-D(Haskey et al 2014 Plasma Phys.Control.Fusion 56 035005)中所预测的那样,该计算预测了强烈的扭结放大,这在很大程度上取决于上下线圈之间的环形相移Delta phi(ul) 。尤其是,放大了刚好位于音高共振(即扭结响应的一个子集)上方的极点模式编号的边缘局部低n剥离模式。通过重新计算一系列边缘几何形状的等离子体响应,研究了放大的剥离响应相对于X点截断的鲁棒性。已经发现,相对于安全系数绘制的剥离响应对X点附近的数字截断不敏感。还可以预见,在电阻率较大的等离子边缘附近,节距对准的分量是有限的,并且也强烈依赖于Δφ(ul)。以前的建议,即放大的剥离响应可能通过光谱邻近性间接驱动间距对准的组件(Lanctot等,2013 Nucl。Fusion 53 083019),是通过将单个多倍性谐波的磁扰动数值化为等离子的边界条件来研究的边缘。已发现,极谱谐波耦合会导致谐波在频谱上耦合并直接在其下方驱动谐波,而且音高对齐的组件也可以通过此机制来驱动。这表明,放大后的低n剥离响应很可能会在强烈放大时驱动间距对齐的分量,这将改变线圈配置以实现最佳的等离子体随机化,这对RMP的ELM控制具有影响。

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