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块状高温超导块材与由商用涂层导体制备的高温超导带材堆叠体之间悬浮特性的比较

Comparison of Levitation Properties between Bulk High-Temperature Superconductor Blocks and High-Temperature Superconductor Tape Stacks Prepared from Commercial Coated Conductors.

作者信息

Kirchner Anke, Espenhahn Tilo, Klug Sebastian, Nielsch Kornelius, Hühne Ruben

机构信息

Leibniz Institute for Solid State and Materials Research, Helmholtzstr. 20, 01069 Dresden, Germany.

Institute for Materials, TUD Dresden University of Technology, 01062 Dresden, Germany.

出版信息

Materials (Basel). 2024 Sep 14;17(18):4516. doi: 10.3390/ma17184516.

DOI:10.3390/ma17184516
PMID:39336257
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11433627/
Abstract

Bulk high-temperature superconductors (HTSs) such as BaCuO (BCO, = Y, Gd) are commonly used in rotationally symmetric superconducting magnetic bearings. However, such bulks have several disadvantages such as brittleness, limited availability and high costs due to the time-consuming and energy-intensive fabrication process. Alternatively, tape stacks of HTS-coated conductors might be used for these devices promising an improved bearing efficiency due to a simplification of manufacturing processes for the required shapes, higher mechanical strength, improved thermal performance, higher availability and therefore potentially reduced costs. Hence, tape stacks with a base area of (12 × 12) mm and a height of up to 12 mm were prepared and compared to commercial bulks of the same size. The trapped field measurements at 77 K showed slightly higher values for the tape stacks if compared to bulks with the same size. Afterwards, the maximum levitation forces in zero field (ZFC) and field cooling (FC) modes were measured while approaching a permanent magnet, which allows the stiffness in the vertical and lateral directions to be determined. Similar levitation forces were measured in the vertical direction for bulk samples and tape stacks in ZFC and FC modes, whereas the lateral forces were almost zero for stacks with the BCO films parallel to the magnet. A 90° rotation of the tape stacks with respect to the magnet results in the opposite behavior, i.e., a high lateral but negligible vertical stiffness. This anisotropy originates from the arrangement of decoupled superconducting layers in the tape stacks. Therefore, a combination of stacks with vertical and lateral alignment is required for stable levitation in a bearing.

摘要

诸如BaCuO(BCO,其中= Y、Gd)之类的块状高温超导材料(HTS)通常用于旋转对称超导磁轴承。然而,此类块状材料存在若干缺点,例如脆性、可用性有限以及由于制造过程耗时且耗能而导致成本高昂。另外,HTS涂层导体的带材堆叠可用于这些设备,由于所需形状的制造工艺得以简化、机械强度更高、热性能改善、可用性提高且因此成本可能降低,有望提高轴承效率。因此,制备了底面尺寸为(12×12)毫米且高度高达12毫米的带材堆叠,并与相同尺寸的商用块状材料进行比较。77 K下的俘获场测量结果表明,与相同尺寸的块状材料相比,带材堆叠的值略高。之后,在靠近永磁体时测量了零场(ZFC)和场冷(FC)模式下的最大悬浮力,这使得能够确定垂直和横向方向的刚度。在ZFC和FC模式下,块状样品和带材堆叠在垂直方向上测得的悬浮力相似,而对于BCO薄膜与磁体平行的堆叠,横向力几乎为零。带材堆叠相对于磁体旋转90°会导致相反的情况,即横向刚度高但垂直刚度可忽略不计。这种各向异性源于带材堆叠中解耦超导层的排列。因此,为了在轴承中实现稳定悬浮,需要垂直和横向排列的堆叠组合。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/d67071cdd8a0/materials-17-04516-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/35237235aa49/materials-17-04516-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/505f5124c7ab/materials-17-04516-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/f90a57b03344/materials-17-04516-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/c9f79f6991e7/materials-17-04516-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/977e79e0a427/materials-17-04516-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/6e04c99f4038/materials-17-04516-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/d67071cdd8a0/materials-17-04516-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/35237235aa49/materials-17-04516-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/505f5124c7ab/materials-17-04516-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/f90a57b03344/materials-17-04516-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/c9f79f6991e7/materials-17-04516-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/977e79e0a427/materials-17-04516-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/6e04c99f4038/materials-17-04516-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/271b/11433627/d67071cdd8a0/materials-17-04516-g007.jpg

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