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Scaling study for positive magnetic shear ELMy H-mode plasmas in JT-60U

机译:JT-60U正磁剪切ELMY H模式等离子体的缩放研究

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Scaling of the density peaking for positive magnetic shear ELMy H-mode plasmas in JT-60U has been developed. Although the density peaking generally depends on collisionality, a variation of the density peaking factor for the same collisionality exists, and the variation is different between plasmas with co-directed and ctr-directed toroidal rotation(co-V-T plasmas and ctr-V-T plasmas). The variation of the co-V-T plasmas can be explained by particle source profile. As a result of scaling, the peaking factor of the co-V-T plasmas depends on the particle source rate profile from neutral beams (NBs) as much as collisionality. The dataset of the ctr-V-T plasmas has a larger variation of the peaking factor compared to that of the co-V-T plasmas. The larger variation stems from that the peaking factor of the ctr-V-T plasmas also depends on the normalized ion temperature gradient at the edge region. As a result of scaling, the normalized ion temperature gradient influences the peaking factor as much as or a little larger than collisionality. The parameter regime of the ctr-V-T plasmas ranges from the trapped electron mode (TEM) to the ion temperature gradient mode (ITG mode). The plasmas with the positive correlation between the normalized density gradient and the normalized ion temperature gradient are dominated by the TEM. On the other hand, the plasmas with the negative correlation are dominated by the ITG mode.
机译:开发了JT-60U中正磁剪切ELMY H模式等离子体的密度峰值的缩放。尽管密度峰值通常取决于撞击性,但是存在相同的罚性的密度峰值因子的变化,并且在具有共定向和CTR定向环形旋转(CO-VT等离子体和CTR-VT等离子体)之间的等离子体之间的变化是不同的。可以通过粒子源分布解释CO-V-T等离子体的变化。作为缩放的结果,CO-V-T等离子体的峰值因子取决于来自中性光束(NBS)的粒子源率曲线和接收性。与COR-V-T等离子体相比,CTR-V-T等离子体的数据集具有更大的峰值因子的变化。较大的变化源于CTR-V-T等离子体的峰值因子也取决于边缘区域处的标准化离子温度梯度。由于缩放的结果,归一化离子温度梯度影响比收集性大多数或大的峰值因子。 CTR-V-T等离子体的参数制度从被困的电子模式(TEM)到离子温度梯度模式(ITG模式)。具有归一化密度梯度与标准化离子温度梯度之间的正相关的等离子体由TEM主导。另一方面,具有负相关的等离子体由ITG模式主导。

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