Flux penetration of an HTS coated-conductor tape by an approaching permanent magnet

IF 5.6 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC
R.W. Taylor , T. Booth , M.D. Ainslie , H.W. Weijers , R.A. Badcock , C.W. Bumby
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引用次数: 2

Abstract

Interactions between inhomogeneous magnetic fields and a superconductor lie at the heart of several high-temperature superconducting (HTS) devices. An example is the situation where the magnetic field from a small permanent magnet (PM) is applied to a coated-conductor HTS tape, such that flux penetrates the superconductor. The PM field is highly spatially inhomogeneous, such that there is significant variation in the applied field magnitude and direction across the tape. This leads to a varying local critical current density, Jc(B,θ), across the tape, and consequently different ‘shielding’ (magnetic flux penetration) behaviour than is the case for a uniform applied field. Here, we report results from measurements and numerical simulations of the penetrating magnetic field within an HTS coated-conductor tape which occur as a PM dipole approaches from a distance. Electromagnetic simulations were performed using a finite-element model based on the H-formulation, and which incorporated experimentally-measured anisotropic Jc(B,θ) properties from a coated-conductor tape. This showed good agreement with experimental measurements. The effects of varying key modelling assumptions and parameters were then studied, including changing the widths of the PM and HTS tape and the magnitude of Jc(B,θ).

The inhomogeneity of the PM field leads to a characteristic gull-wing distribution of magnetic flux across the superconductor at elevated applied fields. Close approach of the PM to the tape suppresses Jc in the centre of the tape, and this results in the observation of a characteristic maxima for the total shielding currents circulating in the tape. A figure of merit is introduced which uses this effect to provide a threshold definition for ‘full flux penetration’ of an HTS tape by an inhomogeneous dipole field.

接近的永磁体对高温超导涂层导体带的磁通渗透
非均匀磁场和超导体之间的相互作用是一些高温超导(HTS)设备的核心。例如,将来自小型永磁体(PM)的磁场施加到涂覆导体的高温超导磁带上,使磁通量穿透超导体。PM场在空间上是高度不均匀的,因此在整个磁带上施加的场的大小和方向有显著的变化。这导致不同的局部临界电流密度,Jc(B,θ),在整个磁带,因此不同的“屏蔽”(磁通穿透)行为,而不是在一个均匀的应用领域的情况下。在这里,我们报告了高温超导涂层导体带内穿透磁场的测量和数值模拟结果,该磁场发生在PM偶极子从远处接近时。采用基于h公式的有限元模型进行了电磁模拟,该模型结合了实验测量的涂覆导体带的各向异性Jc(B,θ)特性。这与实验测量结果吻合良好。然后研究了不同关键建模假设和参数的影响,包括改变PM和HTS带的宽度以及Jc(B,θ)的大小。永磁磁场的不均匀性导致在高外加磁场下超导体的磁通呈鸥翼状分布。PM接近磁带抑制了磁带中心的Jc,这导致观察到磁带中循环的总屏蔽电流的特征最大值。引入了一个利用该效应的优点值,为非均匀偶极子场对高温超导带的“全通量穿透”提供了阈值定义。
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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来源期刊
CiteScore
3.90
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