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Analysis of JET halo currents

机译:JET晕电流分析

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The halo current detection system in JET was refurbished in 2001. The collected data confirm previous results, obtained with a smaller number of sensors, and are consistent with the ITER assumptions. An analysis of recent disruptions shows that the local halo current density in JET is linked to the average plasma current quench rate (the slower the disruption, the larger the local halo load), rather than the plasma current. The largest local halo current densities are more likely to occur when the equilibrium boundary safety factor is low and when it decreases to a critical value, close to 1, during the disruption. The largest halo current fractions are found for the most vertically unstable configurations (i.e. low ratio of resistive vessel time to vertical displacement growth time). The information from the new pick-up coils and Rogowski coils and the only surviving old sensor (a pick-up coil located outboard of the new system) provides an estimate of the size, and an improved picture of the movement, of the halo/wall interaction region during disruptions.
机译:JET的晕轮电流检测系统于2001年进行了翻新。所收集的数据证实了以前的结果,该结果是使用较少数量的传感器获得的,并且与ITER的假设一致。对最近破坏的分析表明,JET中的局部光晕电流密度与平均等离子体电流猝灭速率(破坏速度越慢,局部光晕负载越大)有关,而不是与等离子体电流有关。当平衡边界安全系数很低并且在破坏过程中平衡边界安全系数降低到接近1的临界值时,最可能出现最大的局部光晕电流密度。对于大多数垂直不稳定的配置(即电阻容器时间与垂直位移生长时间的比率低),发现了最大的晕电流分数。来自新的拾波线圈和Rogowski线圈以及唯一幸存的旧传感器(位于新系统外侧的拾波线圈)提供的信息可估算光晕/破坏过程中的壁相互作用区域。

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