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金属学报  2025, Vol. 61 Issue (11): 1738-1746    DOI: 10.11900/0412.1961.2024.00071
  研究论文 本期目录 | 过刊浏览 |
Zr-Al-Ni-Cu-Hf块体非晶合金的力学性能和释能机理
周秉文1,2, 朱梦奇1,2, 赵进北1, 鞠鹏程1, 解野1,2, 刘运峰2, 孟令刚1,2, 亚斌1,2, 张兴国1,2()
1 大连理工大学 材料科学与工程学院 大连 116081
2 大连理工大学宁波研究院 宁波 315016
Mechanical Properties and Energy Release Mechanism of Zr-Al-Ni-Cu-Hf Bulk Metallic Glasses
ZHOU Bingwen1,2, ZHU Mengqi1,2, ZHAO Jinbei1, JU Pengcheng1, XIE Ye1,2, LIU Yunfeng2, MENG Linggang1,2, YA Bin1,2, ZHANG Xingguo1,2()
1 School of Materials Science and Engineering, Dalian University of Technology, Dalian 116081, China
2 NingBo Institute of Dalian University of Technology, Ningbo 315016, China
引用本文:

周秉文, 朱梦奇, 赵进北, 鞠鹏程, 解野, 刘运峰, 孟令刚, 亚斌, 张兴国. Zr-Al-Ni-Cu-Hf块体非晶合金的力学性能和释能机理[J]. 金属学报, 2025, 61(11): 1738-1746.
Bingwen ZHOU, Mengqi ZHU, Jinbei ZHAO, Pengcheng JU, Ye XIE, Yunfeng LIU, Linggang MENG, Bin YA, Xingguo ZHANG. Mechanical Properties and Energy Release Mechanism of Zr-Al-Ni-Cu-Hf Bulk Metallic Glasses[J]. Acta Metall Sin, 2025, 61(11): 1738-1746.

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摘要: 

为制备兼具大玻璃形成能力和一定塑韧性的锆基非晶合金新成分,实现其在含能破片领域的应用,本工作以Zr-Al-Ni-Cu合金体系为研究对象,利用XRD、DSC、SEM及万能试验机等测试分析了Hf替换Cu对Zr55Al10Ni5Cu30 - x Hf x (x = 0、1、3、5、7、10,原子分数,%)块体非晶合金玻璃形成能力和性能的影响。结果表明,适量的Hf替换Cu有利于增强Zr55Al10Ni5Cu30非晶合金的玻璃形成能力、热稳定性和压缩塑性。当Hf含量为7%时,非晶合金具有最大的临界直径12 mm和最大的过冷液相区间(85 K)。当Hf含量为5%时,非晶合金具有10 mm的临界直径和75 K的过冷液相区间,且压缩塑性应变高达13.3%,较原始成分获得了显著提升。采用真空压铸法制备了直径9.4 mm的Zr55Al10Ni5Cu25Hf5球形非晶破片,并对其进行准密闭箱冲击超压实验。结果表明,破片临界超压速率约为600 m/s,在1360 m/s的冲击速率下,最大超压峰值可以达到0.3291 MPa,此时破片具有最大释能效率(63.17%)。

关键词 块体非晶合金玻璃形成能力室温塑性非晶破片超压峰值    
Abstract

Zr-based amorphous alloys possess excellent glass-forming ability and high energy density, which facilitate the development of new energetic fragments. However, their poor plasticity limits their application in fragment-based systems. This study aims to investigate the Zr-Al-Ni-Cu alloy system by substituting Hf for Cu to examine its effects on the glass-forming ability and mechanical properties of Zr55Al10Ni5Cu30 - x Hf x (x = 0, 1, 3, 5, 7, 10, atomic fraction, %) bulk metallic glasses (BMGs). The investigation used XRD, DSC, SEM, and a universal testing machine for characterizing the alloy system. Results demonstrate that moderate Hf substitution for Cu enhances the glass-forming ability, thermal stability, and compressive ductility of Zr55Al10Ni5Cu30 BMGs. With an Hf content of 7%, the alloy achieves a maximum critical diameter of 12 mm and an expanded undercooled liquid phase interval of 85 K. With an Hf content of 5%, the alloy achieves a critical diameter of 10 mm, an undercooled liquid phase interval of 75 K, and substantially improved compressive plastic strain of 13.3%, thereby enhancing its performance compared with the original composition. Spherical specimens of Zr55Al10Ni5Cu25Hf5 with a diameter of 9.4 mm were prepared using vacuum suction casting, followed by quasi-sealed chamber impact overpressure experiments. The results indicate that the critical overpressure velocity of the specimens is approximately 600 m/s, and an impact velocity of 1360 m/s produces a maximum overpressure peak of 0.3291 MPa, where the specimens achieve a peak energy release efficiency of 63.17%.

Key wordsbulk metallic glasses    glass-forming ability    room temperature plasticity    amorphous fragment    overpressure peak
收稿日期: 2024-03-08     
ZTFLH:  TG139  
通讯作者: 张兴国,zxgwj@dlut.edu.cn,主要从事非晶纳米晶合金、功能材料和高性能钢铁材料等方面研究
Corresponding author: ZHANG Xingguo, professor, Tel: (0411)84706183, E-mail: zxgwj@dlut.edu.cn
作者简介: 周秉文,1981年生,副教授,博士
图1  铸态Zr55Al10Ni5Cu30 - x Hf x 非晶合金达到临界直径(Dc)时样品的XRD谱
图2  Zr55Al10Ni5Cu30 - x Hf x 非晶合金的DSC曲线
图3  Zr55Al10Ni5Cu30 - x Hf x 非晶合金的特征温度随Hf含量的变化折线图
图4  Zr55Al10Ni5Cu30 - x Hf x(x = 0~10%) 非晶合金室温压缩应力-应变曲线
图5  Zr55Al10Ni5Cu30 - x Hf x(x = 0~10%) 非晶合金的力学性能随Hf含量变化折线图
图6  Zr55Al10Ni5Cu25Hf5非晶合金压缩应力-应变曲线锯齿流变图
图7  Zr55Al10Ni5Cu25Hf5非晶合金的应力降幅分布直方图
图8  Zr55Al10Ni5Cu30 - x Hf x 非晶合金压缩断裂侧表面形貌
图9  Zr55Al10Ni5Cu25Hf5非晶合金侧表面剪切带形貌
图10  Zr55Al10Ni5Cu25Hf5球形破片准密闭箱冲击超压实验原理图
图11  Zr55Al10Ni5Cu25Hf5破片冲击破碎反应过程高速摄影图像
v / (m·s-1)Mc / gm / gΔP / MPa
5153.0823.30-
6093.0833.600.0216
7343.0814.700.0585
8033.0825.000.0931
10793.0796.800.1225
13603.0849.050.3291
表1  Zr55Al10Ni5Cu25Hf5破片超压峰值实验数据
v / (m·s-1)ΔQ / kJΔEk / kJec / (kJ·g-1)Qc / (kJ·g-1)y / %
515-----
6091.460.170.4210.963.82
7343.950.251.2010.9610.96
8036.280.301.9410.9617.70
10798.270.542.5110.9622.90
136022.210.866.9210.9663.17
表2  Zr55Al10Ni5Cu25Hf5破片释能效率
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