基于多边形各向异性电阻率的用于无绝缘 HTS 线圈电磁模拟的快速准确 3D 有限元模型

Zhuoyan Zhong, Wei Wu, Zhijian Jin
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摘要

对于无绝缘(NI)高温超导(HTS)线圈,仍然需要一种快速准确、有利于建立并可直接进行多物理场耦合的三维电磁模型。本文介绍了用于 NI HTS 线圈三维有限元电磁模拟的多边形各向异性电阻率 (PAR) 方法。该模型避免了将每个磁带划分为特定的 HTS 磁带层和匝间接触层,从而:(1) 减轻了计算负担;(2) 由于元素纵横比更小,收敛性得到改善。PAR 方法的意义在于它在实现具有高计算速度和精度的三维各向异性电阻率模型方面发挥了不可或缺的作用。所提出的 PAR 模型通过三类模拟进行了严格评估:(1) 充电和放电测试;(2) 直流电源下 NI 线圈在交流场中的交流损耗;(3) 热触发淬火和恢复情景。在这些模拟中,PAR 模型通过与全元素模型(即在 H 型模型中明确包含每个特定 HTS 带层和匝间接触层的 3D FEM 模型)的比较进行了验证,并通过之前的交流损耗实验数据进行了验证。该模型具有良好的一致性。经测试,在精度相同的情况下,PAR 模型的计算速度是全元素模型的 12-38 倍。在 HTS 磁带宽度和长度网格密度相同的情况下,PAR 模型比全元素模型减少了 40% 的自由度,从而在相同的计算内存限制下,实现了更精确、更大规模的线圈模拟。此外,PAR 模型完全消除了传统各向异性电阻率三维模型中固有的不准确性,这种不准确性源于排列的各向异性电阻率与实际计算的线圈网格之间的差异。建议的 PAR 模型将提高 NI HTS 线圈三维电磁分析的普及率。
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Fast and accurate 3D FEM model for electromagnetic simulations of no-insulation HTS coils based on polygon-anisotropic-resistivity
For no-insulation (NI) high-temperature superconducting (HTS) coils, a 3D electromagnetic model, which is fast and accurate, conducive to establish, and straightforward to multi-physics coupling, is still required. This paper introduces a polygon-anisotropic-resistivity (PAR) method for 3D FEM electromagnetic simulations of NI HTS coils. This model avoids dividing each tape into the specific HTS-tape layer and turn-to-turn contact layer, which yields: (1) a reduced computational burden; (2) improved convergence due to smaller element aspect ratios. The significance of the PAR method lies in its indispensable role in achieving a 3D anisotropic-resistivity model with high computing speed and accuracy. The proposed PAR model is rigorously evaluated through three types of simulations: (1) charge and discharge tests; (2) AC losses of the NI coil subjected to AC fields with a DC current supply; (3) heat-triggered quench and recovery scenarios. For these simulations, the PAR model is validated by comparisons with the full-element model, namely, the 3D FEM model that explicitly incorporates each specific HTS-tape layer and turn-to-turn contact layer in the H-formulation model, and is also validated by previous experimental data for AC losses. Good consistency is observed. The computing speed of the PAR model is tested to be 12–38 times that of the full-element model with the same accuracy. The PAR model achieves a 40% reduction in degrees of freedom compared to the full-element model, with the same mesh density along the HTS tape width and length, facilitating more precise and larger scale coil simulations within the same computational memory limits. Additionally, the PAR model entirely eliminates the inherent inaccuracies found in the conventional-anisotropic-resistivity 3D model, which stem from discrepancies between the arranged anisotropic-resistivity and the actual computed coil meshes. The proposed PAR model will enhance the prevalence of 3D electromagnetic analyses of NI HTS coils.
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