研究论文

B含量调控Fe98.5 -x B x Cu1.5 纳米晶合金组织结构和磁性能

  • 朱春健 ,
  • 李艳辉 ,
  • 朱正旺 ,
  • 吴立成 ,
  • 张海峰 ,
  • 张伟
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  • 1.大连理工大学 材料科学与工程学院 大连 116024
    2.东北大学 冶金学院 沈阳 110819
朱春健,男,1998年生,硕士生
张 伟,wzhang@dlut.edu.cn,主要从事非晶态合金、纳米材料和磁性材料的研究

收稿日期: 2023-05-08

  修回日期: 2023-06-22

  网络出版日期: 2023-07-21

基金资助

国家重点研发计划项目(2022YFB3804100);国家自然科学基金项目(52171153)

Regulation of Structure and Magnetic Properties of Fe98.5 -x B x Cu1.5 Nanocrystalline Alloys Based on B Content

  • ZHU Chunjian ,
  • LI Yanhui ,
  • ZHU Zhengwang ,
  • WU Licheng ,
  • ZHANG Haifeng ,
  • ZHANG Wei
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  • 1.School of Materials Science and Engineering, Dalian University of Technology, Dalian 116024, China
    2.School of Metallurgy, Northeastern University, Shenyang 110819, China
ZHANG Wei, professor, Tel: (0411)84706063, E-mail: wzhang@dlut.edu.cn

Received date: 2023-05-08

  Revised date: 2023-06-22

  Online published: 2023-07-21

Supported by

National Key Research and Development Program of China(2022YFB3804100);National Natural Science Foundation of China(52171153)

摘要

为研发具有良好软磁性和工艺性的高饱和磁感应强度(Bs) 铁基纳米晶合金,本工作以高Fe含量的Fe-B-Cu合金体系为对象,研究了B含量对Fe98.5 - x B x Cu1.5 (x = 12~18,原子分数,%)系快淬合金带材的微结构、结晶化组织和磁性能的影响,分析了B含量-快淬微结构-结晶化组织-磁性能间的关联。结果表明,快淬合金均为非晶基体中分布着纳米尺度α-Fe晶粒(预存α-Fe晶)的结构;随x由12增加至18,非晶基体中预存α-Fe晶的数密度和晶粒尺寸逐渐降低,结构转变为近非晶态。经低升温速率热处理后,x = 12~17时合金均为非晶/α-Fe纳米晶双相结构,而x = 18时合金形成了非晶/α-Fe/Fe3B纳米复相组织结构;x = 13~16时合金具有微细的纳米晶组织和较好的软磁性能,α-Fe相的平均晶粒尺寸(D¯α-Fe)、Bs和矫顽力(Hc)分别在15.8~16.3 nm、1.80~1.91 T和18.9~22.7 A/m的范围内,其中x = 15时合金的D¯α-Fe、BsHc分别为16.0 nm、1.86 T和18.9 A/m。基于合金热处理前后的组织结构演化,提出了不同B含量快淬合金的结晶化模型,阐明了快淬合金非晶基体中高数密度的细小预存α-Fe晶粒间以及与热处理结晶化新生α-Fe晶粒间的强竞争生长效应,导致均匀、微细纳米晶组织形成的机制。

本文引用格式

朱春健 , 李艳辉 , 朱正旺 , 吴立成 , 张海峰 , 张伟 . B含量调控Fe98.5 -x B x Cu1.5 纳米晶合金组织结构和磁性能[J]. 金属学报, 2025 , 61(8) : 1174 -1182 . DOI: 10.11900/0412.1961.2023.00205

Abstract

With the development of electromagnetic devices towards high-frequency, miniaturization, and high efficiency, the demand for the soft magnetic nanocrystalline alloys with high saturation magnetic flux density (Bs), excellent high-frequency performance, as well as good manufacturability is becoming increasingly urgent. In this work, the effects of B content on the melt-spun structure, thermal stability, crystallization structure, and magnetic properties of Fe98.5 - x B x Cu1.5 (x = 12-18, atomic fraction, %) alloy ribbons were investigated; and the correlation among B content, melt-spun structure, crystallization structure, and magnetic properties was explored. The results show that the melt-spun structure of all the alloys is a dual-phase composed of α-Fe nanograins distributing in an amorphous matrix. As the x increases from 12 to 18, the number density and grain size of the α-Fe grains gradually decrease, and the structure transforms into a nearly amorphous state. After crystallization annealing under a low heating rate, the alloys with x = 12-17 have the amorphous/nanocrystalline α-Fe dual-phase structure, while the x = 18 alloy forms a amorphous/α-Fe/Fe3B tri-phase structure. The alloys with x = 13-16 exhibit a fine nanocrystalline structure and good soft magnetic properties with the average α-Fe grain size (D¯α-Fe) of 15.8-16.3 nm, Bs of 1.80-1.91 T, and coercivity (Hc)of 18.9-22.7 A/m. Among them, the alloywith x = 15 has the D¯α-Fe, Bs, and Hc of 16.0 nm, 1.86 T, and 18.9 A/m, respectively. Based on the structure of the alloys before and after annealing, a crystallization model for the melt-spun alloys with different B contents was proposed, and the mechanism of which the strong competitive growth effect between the high-number-density pre-existing fine α-Fe nanograins in the amorphous matrix of the melt-spun alloys along with the newly-formed α-Fe grains during crystallization annealing results in the uniform and fine nanocrystalline structure of the alloys was elucidated.

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