粉末残余二次相对Bi-2212超导丝Jc和显微组织的主导影响

IF 5.6 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC
L.H. Jin, G.Q. Liu, J.Q. Feng, X.Y. Xu, G.F. Jiao, S.N. Zhang, Q.B. Hao, P.X. Zhang, C.S. Li
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引用次数: 0

摘要

Bi2Sr2CaCu2O8+δ(Bi-2212)超导圆导线在高场应用中表现出巨大的潜力。前体粉末的纯度对于导线的传输电流至关重要。然而,残留的第二相在前体粉末中的作用还没有完全理解。在此,研究了使用超声波喷雾热解(USP)和煅烧工艺制备的前体粉末中第二相的来源。分析了前驱体粉末在结晶过程中的微观结构和相演变。此外,还系统地讨论了残余二次相对Bi-2212多丝丝的熔融行为、形态特性和超电流流动的影响。细丝中残留的第二相导致进一步结晶,这导致在熔化过程开始时形成更多更大的Bi-2201晶粒。最终Bi-2212导线的不良微观结构和低临界电流可归因于残余富铜相的存在。用完全结晶的粉末制备的Bi-2212线在4.2K自场下具有6773A/mm2的高临界电流密度(Jc)。结果表明,控制前体粉末中的第二相对于获得优异的Jc值具有重要意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Dominant effect of residual secondary phase of powders on Jc and microstructure of Bi-2212 superconducting wires

Bi2Sr2CaCu2O8+δ (Bi-2212) superconducting round wires exhibited great potential for use in high-field applications. The purity of the precursor powders is critical for the transport current of the wires. However, the role of the residual secondary phase in the precursor powders is not fully understood. Here, the origin of the secondary phase was investigated in precursor powders that were prepared using ultrasonic spray pyrolysis (USP) and calcination processing. The microstructure and phase evolution of the precursor powders during the crystallization process were analyzed. Moreover, the effects that the residual secondary phase has on melting behavior, morphology properties, and the supercurrent flow of Bi-2212 multi-filamentary wires are systematically discussed. The residual secondary phase in the filament caused further crystallization, and this led to the formation of more and larger Bi-2201 grains at the onset of the melting process. The poor microstructure and low critical current of the final Bi-2212 wires can be attributed to the presence of the residual copper-rich phase. Bi-2212 wires that were prepared with fully crystallized powders had a high critical current density (Jc) of 6773 A/mm2 at 4.2 K, self-field. It was revealed that control of the secondary phases in precursor powders is greatly significant for achieving superior values of Jc.

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