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首页> 外文期刊>Applied Superconductivity, IEEE Transactions on >Transport Performance and Current Distribution of HTS Current Lead Prepared by YBCO Tapes
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Transport Performance and Current Distribution of HTS Current Lead Prepared by YBCO Tapes

机译:YBCO胶带制备的高温超导电流引线的传输性能和电流分布

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High-temperature superconducting (HTS) current lead has been prepared by the trifluoro acetates–metal organic deposition (TFA–MOD) processed YBCO tapes. The YBCO tape has higher critical current density and better magnetic property than the Bi2223 tape. Furthermore, the thermal conductivity of the YBCO tape with a thin Ag layer is much lower than that of the Ag-sheathed Bi2223 tape. The critical current of the YBCO tapes ranges from 150 to 180 A in liquid nitrogen and self-field. A current lead is composed of eight bundles stacked by two YBCO tapes (16 tapes), Cu end caps, and a pair of stainless-steel boards. Rogowski coils and Hall sensors used for estimation of current distribution are attached on each YBCO bundle. The transport current of 1.6 kA was carried with no voltage on every YBCO tape at 77 K. Although voltage of several tens of microvolts on some YBCO tapes appeared, transport current of 1.8 kA was successfully carried with no quenching. The voltages between the Cu cap and YBCO tapes almost linearly increased with increasing transport current, and they range from 0.75 to 0.93 mV and 1.02 to 1.21 mV at 1.8 kA, respectively. The low voltages correspond to 0.42–0.52 and 0.57–0.67 . The low contact resistance results in low joule heating at Cu joints. The current calculated by Rogowski coils in eight bundles varies from 137 to 355 A at 1.8 kA and sweep rate of 800 A/s. Therefore, the imbalance among eight bundles is evaluated to be 218 A. The current of eight bundles calculated by Rogowski coils sums up to 1808 A, which is the slight difference of 8 A in comparison with transport current of 1800 A. Rogowski coils and Hall sensors are effective at evaluating of current distribution for cu- rent lead.
机译:高温超导(HTS)电流引线是由三氟乙酸盐-金属有机沉积(TFA-MOD)处理的YBCO胶带制成的。与Bi2223胶带相比,YBCO胶带具有更高的临界电流密度和更好的磁性。此外,具有薄的Ag层的YBCO带的热导率比带有Ag的Bi2223带的热导率低得多。在液氮和自电场作用下,YBCO胶带的临界电流范围为150至180A。电流引线由八束捆绑而成,由两根YBCO胶带(16根胶带),Cu端盖和一对不锈钢板堆叠而成。用于估算电流分布的Rogowski线圈和霍尔传感器安装在每个YBCO束上。每个YBCO胶带在77 K的电压下都没有电压输送1.6 kA的输送电流。尽管在某些YBCO胶带上出现了几十微伏的电压,但成功地输送了1.8 kA的输送电流而没有淬火。 Cu盖带和YBCO带之间的电压几乎随传输电流的增加而线性增加,在1.8 kA时,它们的电压分别为0.75至0.93 mV和1.02至1.21 mV。低压对应于0.42-0.52和0.57-0.67。低的接触电阻导致铜接头处的焦耳热低。罗戈夫斯基线圈计算的八束电流在1.8 kA和800 A / s的扫描速率下从137至355 A不等。因此,估计八束之间的不平衡度为218A。由Rogowski线圈计算出的八束电流的总和为1808 A,与1800 A的传输电流相比,相差8A。Rogowski线圈和霍尔传感器可有效评估电流引线的电流分布。

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