用不同的多脉冲磁化方法比较计算块体高温超导体的陷波场和陷波磁通量

Yong Yang and Guolong Deng
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摘要

块状高温超导体(HTS)可以捕获高磁场,作为伪永磁体可用于多种应用。与准静态磁场冷却和零磁场冷却技术相比,块状高温超导体的脉冲磁场磁化(PFM)技术成本低、应用灵活。为了实现高困磁场和大困磁通量等优异的磁化性能,许多研究都提出了许多脉冲场磁化方法。为了阐明采用不同典型 PFM 方法的块状 HTS 的磁化特性,我们使用基于 H 公式结合热导方程的仿真模型对几种典型 PFM 方法进行了比较分析。利用螺线管型线圈对块体 HTS 进行磁化,数值计算了采用不同 PFM 方法的块体 HTS 磁化过程中的电磁和热行为。计算结果表明,多脉冲磁化方法能有效增强块体的陷波场和陷波磁通量,不同的多脉冲磁化方法对这些性能的增强效率不同。在研究中考虑的所有多脉冲磁化方法中,具有阶跃冷却的改良多脉冲技术与减幅脉冲场迭代磁化方法的组合方法同时对困绕磁场和困绕磁通量的改善最大。
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Comparative calculations of trapped field and trapped magnetic flux with different multi-pulse magnetization methods for a bulk high-temperature superconductor
Bulk high-temperature superconductors (HTSs) can trap high magnetic field and are potentially useful for a variety of applications as pseudo-permanent magnets. The pulsed field magnetization (PFM) for bulk HTSs is cost effective and flexible in application compared with quasi-static field cooling and zero field cooling techniques. Many PFM methods have been proposed in many studies to achieve the excellent magnetization performances such as high trapped field and large trapped magnetic flux. In order to clarify the magnetization characteristics of bulk HTSs using different typical PFM methods, we comparatively analyze several typical PFM methods using a simulation model based on the H-formulation combining the thermal conductivity equation. The electromagnetic and thermal behaviors during the magnetization of a bulk HTS with different PFM methods are numerically achieved using the solenoid-type coil to magnetize the bulk. The calculations show that multi-pulse magnetization methods can effectively enhance the trapped field and trapped magnetic flux of the bulk, and different multi-pulse magnetization methods have different efficiencies enhancing these performances. Among all considered PFM methods in the study, the combination method of modified multi-pulse technique with step-wise cooling and iteratively magnetizing pulsed-field method with reducing amplitude has the largest improvement for the trapped magnetic field and the trapped flux simultaneously.
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