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用于核聚变的极高电流密度钇钡铜氧超导电线的研发与大规模生产。

Development and large volume production of extremely high current density YBaCuO superconducting wires for fusion.

作者信息

Molodyk A, Samoilenkov S, Markelov A, Degtyarenko P, Lee S, Petrykin V, Gaifullin M, Mankevich A, Vavilov A, Sorbom B, Cheng J, Garberg S, Kesler L, Hartwig Z, Gavrilkin S, Tsvetkov A, Okada T, Awaji S, Abraimov D, Francis A, Bradford G, Larbalestier D, Senatore C, Bonura M, Pantoja A E, Wimbush S C, Strickland N M, Vasiliev A

机构信息

S-Innovations, Moscow, Russia.

SuperOx, Moscow, Russia.

出版信息

Sci Rep. 2021 Jan 22;11(1):2084. doi: 10.1038/s41598-021-81559-z.

DOI:10.1038/s41598-021-81559-z
PMID:33483553
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7822827/
Abstract

The fusion power density produced in a tokamak is proportional to its magnetic field strength to the fourth power. Second-generation high temperature superconductor (2G HTS) wires demonstrate remarkable engineering current density (averaged over the full wire), J, at very high magnetic fields, driving progress in fusion and other applications. The key challenge for HTS wires has been to offer an acceptable combination of high and consistent superconducting performance in high magnetic fields, high volume supply, and low price. Here we report a very high and reproducible J in practical HTS wires based on a simple YBaCuO (YBCO) superconductor formulation with YO nanoparticles, which have been delivered in just nine months to a commercial fusion customer in the largest-volume order the HTS industry has seen to date. We demonstrate a novel YBCO superconductor formulation without the c-axis correlated nano-columnar defects that are widely believed to be prerequisite for high in-field performance. The simplicity of this new formulation allows robust and scalable manufacturing, providing, for the first time, large volumes of consistently high performance wire, and the economies of scale necessary to lower HTS wire prices to a level acceptable for fusion and ultimately for the widespread commercial adoption of HTS.

摘要

托卡马克中产生的聚变功率密度与其磁场强度的四次方成正比。第二代高温超导(2G HTS)导线在非常高的磁场下展现出显著的工程电流密度(在整根导线上平均)J,推动了聚变及其他应用的发展。高温超导导线面临的关键挑战在于,要在高磁场下提供高且一致的超导性能、高产量供应以及低价格这三者的可接受组合。在此,我们报告了基于一种含有YO纳米颗粒的简单钇钡铜氧(YBCO)超导体制备的实用高温超导导线中具有非常高且可重复的J,该导线在短短九个月内就以高温超导行业迄今为止最大的批量订单交付给了一位商业聚变客户。我们展示了一种新型的YBCO超导体制备方法,其没有c轴相关的纳米柱状缺陷,而这些缺陷被广泛认为是高场性能的先决条件。这种新制备方法的简单性使得大规模且可扩展的制造成为可能,首次提供了大量性能始终如一的高性能导线,以及将高温超导导线价格降低到聚变可接受水平并最终实现高温超导广泛商业应用所需的规模经济。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/853fb376911d/41598_2021_81559_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/3e79bf62f07b/41598_2021_81559_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/84e5cff19efa/41598_2021_81559_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/31f131a6060b/41598_2021_81559_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/fc0a7e341b2b/41598_2021_81559_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/bfc5fdc12e1e/41598_2021_81559_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/4a7c0feecd5b/41598_2021_81559_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/853fb376911d/41598_2021_81559_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/3e79bf62f07b/41598_2021_81559_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/84e5cff19efa/41598_2021_81559_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/31f131a6060b/41598_2021_81559_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/fc0a7e341b2b/41598_2021_81559_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/bfc5fdc12e1e/41598_2021_81559_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/4a7c0feecd5b/41598_2021_81559_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6df6/7822827/853fb376911d/41598_2021_81559_Fig7_HTML.jpg

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