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Suppression of error-field-induced magnetic islands by Alfven resonance effect in rotating plasmas

机译:旋转等离子体中Alfven共振效应对误差场感应磁岛的抑制

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摘要

Error-field penetration is numerically studied in cylindrical tokamak geometry with plasma rotation. For a static error field, non-rotating magnetic islands are generated in the steady state. The penetrated perturbed magnetic flux is effectively reduced by the plasma rotation at small resistivity. Twin current sheets are formed at the Alfven resonance positions when the plasma rotation is fast enough, and thereby the error-field penetration is significantly changed. The electromagnetic torque increases linearly in the plasma rotation velocity especially at high rotation velocity and low resistivity regime, which agrees with previous theoretical prediction, although the linear scaling can be easily affected if the Alfven resonance is located close to the plasma edge. The electromagnetic torque in this regime does not depend on the resistivity. For high beta or small resistivity plasmas, the resultant volume-integrated electromagnetic torque, which brakes the plasma rotation, becomes maximum at very small, almost zero experimentally, rotation velocity.
机译:在具有等离子体旋转的圆柱托卡马克几何中,对误差场穿透进行了数值研究。对于静态误差场,在稳定状态下会生成不旋转的磁岛。通过在小电阻率下的等离子体旋转,有效地减小了所穿透的扰动磁通量。当等离子体旋转足够快时,在Alfven共振位置处会形成双电流片,从而使误差场的穿透度显着改变。电磁转矩在等离子体旋转速度中呈线性增加,特别是在高旋转速度和低电阻率状态下,这与先前的理论预测相符,尽管如果Alfven共振位于等离子体边缘附近,则线性缩放容易受到影响。在这种情况下的电磁转矩不取决于电阻率。对于高β或小电阻率的等离子体,制动等离子体旋转的最终体积积分电磁转矩在非常小(实验上几乎为零)的旋转速度下变为最大值。

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