Initial stages of Nb3Sn phase formation in Nb-bronze matrix composite wires investigated by means of electron microscopy

被引:0
作者
Li, Shu-Rui [1 ]
Hu, Bin [2 ]
Ren, Hui-Jie [3 ]
Wang, Lei [1 ]
Wang, Xing-Ming [1 ]
机构
[1] GRINM Resources & Environm Technol Co Ltd, Beijing 101407, Peoples R China
[2] GRINM Grp Co Ltd, Beijing 100088, Peoples R China
[3] CRRC Beijing ERQI Vehicle Co Ltd, Beijing 100072, Peoples R China
关键词
Nb3Sn phase; Quantitative characterization; Isothermal annealing; Microstructural evolution; Formation mechanism; REACTIVE DIFFUSION; GROWTH; KINETICS; ALLOY;
D O I
10.1007/s12598-020-01398-1
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
At present, Nb3Sn superconductors are becoming more popular in high magnetic fields. The growth law of Nb3Sn phase in a planar CuSn/Nb diffusion couple has been studied, whereas the formation mechanism of Nb3Sn phase in a cylindrical CuSn/Nb diffusion couple is still controversial. The purpose of this work is to investigate the growth exponent of Nb3Sn phase at the initial stage of annealing by use of scanning electron microscopy (SEM) through which the thickness of Nb3Sn layer can be obtained. In this study, bronze-processed Nb3Sn multifilamentary wires with different annealing time were investigated. The Nb3Sn phase was formed during isothermal annealing at 670 degrees C by solid-state diffusion, which was accomplished by the movement of Sn atoms from the CuSn/Nb3Sn interface to Nb3Sn/Nb interface. However, the formation mechanism of Nb3Sn phase at the initial stage of annealing is still not well understood. Microstructural evolution of Nb3Sn phase during isothermal annealing was studied by SEM. The mean thickness of the Nb3Sn layer (Delta xNb3Sn) is expressed as a power function of the annealing time (t) by the equation Delta xNb3Sn2=k(t/t0)n, where t(0) is the unit time, k is the reaction rate constant and n is the growth exponent. The growth exponent has the average value of 0.82, which means that the formation of the Nb3Sn phase is both governed by the interface reaction and the grain boundary diffusion.
引用
收藏
页码:708 / 713
页数:6
相关论文
共 30 条
  • [1] Blaugher R. D., 1969, Journal of Low Temperature Physics, V1, P539, DOI 10.1007/BF00627932
  • [2] Cantoni M., 2008, Microsc. Microanal., V14, P1146
  • [3] THE PHYSICAL AND STRUCTURAL-PROPERTIES OF SUPERCONDUCTING A15-TYPE NB-SN ALLOYS
    DEVANTAY, H
    JORDA, JL
    DECROUX, M
    MULLER, J
    FLUKIGER, R
    [J]. JOURNAL OF MATERIALS SCIENCE, 1981, 16 (08) : 2145 - 2153
  • [4] Engler O, 2010, INTRODUCTION TO TEXTURE ANALYSIS: MACROTEXTURE, MICROTEXTURE, AND ORIENTATION MAPPING, 2ND EDITION, P1
  • [5] DIFFUSION MECHANISMS FOR GROWTH OF NB3SN INTERMETALLIC LAYERS
    FARRELL, HH
    GILMER, GH
    SUENAGA, M
    [J]. THIN SOLID FILMS, 1975, 25 (01) : 253 - 264
  • [6] GRAIN-BOUNDARY DIFFUSION AND GROWTH OF INTERMETALLIC LAYERS - NB3SN
    FARRELL, HH
    GILMER, GH
    [J]. JOURNAL OF APPLIED PHYSICS, 1974, 45 (09) : 4025 - 4035
  • [7] Microstructure, composition and critical current density of superconducting Nb3Sn wires
    Fluekiger, R.
    Uglietti, D.
    Senatore, C.
    Buta, F.
    [J]. CRYOGENICS, 2008, 48 (7-8) : 293 - 307
  • [8] Foner S, 1981, SUPERCONDUCTOR MAT S, P201
  • [9] A review of the properties of Nb3Sn and their variation with A15 composition, morphology and strain state
    Godeke, A.
    [J]. SUPERCONDUCTOR SCIENCE & TECHNOLOGY, 2006, 19 (08) : R68 - R80
  • [10] Goldstein J.I., 2003, SCANNING ELECT MICRO, P453