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Effects of plasma shape and profiles on edge stability in DIII-D

机译:等离子体形状和轮廓对DIII-D中边缘稳定性的影响

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The results of recent experimental and theoretical studies concerning the effects of plasma shape and current and pressure profiles on edge instabilities in DIII--D are presented. Magnetic oscil- lations with toroidal mode number n ≈ 2--9 and a fast growth time γ~(-1) = 20--150 μs are often observed prior to the first giant type I ELM in discharges with moderate squareness. High n ideal second ballooning stability access encourages edge instabilities by facilitating the buildup of the edge pressure gradient and bootstrap current density, which destabilize the intermediate to low n modes. Analysis suggests that discharges with large edge pressure gradient and bootstrap current density are more unstable to n > 1 modes. Calculations and experimental results show that ELM amplitude and frequency can be varied by controlling access to the second ballooning stability regime at the edge through variation of the squareness of the discharge shape. A new method is proposed to control edge instabilities by reducing access to the second ballooning stability regime at the edge using high order local perturbation of the plasma shape in the outboard bad curvature region.
机译:提出了有关等离子形状,电流和压力分布对DIII-D边缘不稳定性的影响的最新实验和理论研究结果。在第一个巨型I ELM之前,在中等矩形度的放电中,通常会观察到环形模数n≈2--9和快速生长时间γ〜(-1)= 20--150μs的磁振荡。高n个理想的第二个膨胀稳定性通道可通过促进边缘压力梯度和自举电流密度的建立来促进边缘不稳定性,这会破坏中低模态的稳定性。分析表明,具有较大边缘压力梯度和自举电流密度的放电在n> 1模式下更加不稳定。计算和实验结果表明,通过改变放电形状的矩形度,可以控制进入边缘的第二个膨胀稳定性制度,从而改变ELM幅度和频率。提出了一种新方法来控制边缘不稳定性,方法是使用外侧不良曲率区域中的等离子体形状进行高阶局部扰动,从而减少对边缘处第二种膨胀稳定状态的访问。

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