Normal-zone Propagation in Helical Coils of Large Helical Device

S. Imagawa, T. Obana, S. Hamaguchi, N. Yanagi, T. Mito
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Abstract

Synopsis: Large Helical Device (LHD) has been in operation since 1998. Propagation of a normal zone has been observed 26 times in a pair of helical coils, named H1 and H2, of the LHD during the 21 years of operation. The only fourth propagation resulted in quick discharge due to the imbalance voltage higher than the preset value of 0.2 V, whereas the propagation in the other cases stopped within a few seconds. Each the coil is divided into three blocks, named H-I, H-M, and H-O, from the inside. Since the conductor of the helical coils consists of NbTi/Cu strands, a pure aluminum stabilizer clad with a Cu-2%Ni layer, and a copper sheath, the current center shifts from the superconducting wires to the pure aluminum stabilizer at the normal zone. Therefore, imbalance voltages between H1 and H2 are induced in all the blocks during propagation of a normal zone. The crosssectional position of the conductor in which the normal zone propagates can be estimated from the difference of the imbalance voltages among the blocks. In 2001, pickup coils were installed along the helical coils by the pitch of 30 degree of the poloidal angle in order to detect the position of a propagating normal zone. The pickup coils detect the change in magnetic field by a shift of current center at the normal zone. The position and velocity of propagating normal zones were detected successfully 15 times after the 10th propagation. Most of the normal zones were induced at the bottom of the coils, and all of them propagated to one side, which is downstream of the transport current, with recovery on the opposite side. As the results of investigation of all the data, normal zones are considered to have been induced in the conductor in the first or last turn of the first or second layer of the H-I block. Therefore, normal zones should be induced at the position under the worst cooling condition with large disturbance due to slippage of the conductor against the helical coil case.
大型螺旋装置螺旋线圈的法向区传播
简介:大型螺旋装置(LHD)自1998年开始运行。在21年的运行中,在LHD的一对名为H1和H2的螺旋线圈中观察到26次正常区的传播。由于不平衡电压高于预设值0.2 V,只有第四次传播导致快速放电,而其他情况下的传播在几秒钟内停止。每个线圈从内部分成三个块,分别命名为H-I、H-M和H-O。由于螺旋线圈的导体由NbTi/Cu股、覆有Cu-2% ni层的纯铝稳定剂和铜护套组成,电流中心在正常区域从超导导线转移到纯铝稳定剂。因此,在正常区域的传播过程中,H1和H2之间的不平衡电压在所有块中都被诱导。导体中正常区传播的横截面位置可以通过块间不平衡电压的差来估计。在2001年,拾取线圈沿着螺旋线圈以30度的极向角安装,以检测传播的法线区域的位置。感应线圈通过电流中心在正常区域的移动来检测磁场的变化。在第10次繁殖后,成功检测了15次繁殖正常区的位置和速度。大部分的正常区在线圈的底部产生,所有的正常区都传播到输运电流的下游一侧,恢复在相反的一侧。根据所有数据的调查结果,认为在H-I块的第1层或第2层的第1匝或最后1匝导体中已感应到正常带。因此,正常区应在最坏的冷却条件下,由于导体对螺旋线圈外壳的滑动而产生较大扰动的位置诱导。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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