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| 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 |
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Cite this article:
ZHOU Bingwen, ZHU Mengqi, ZHAO Jinbei, JU Pengcheng, XIE Ye, LIU Yunfeng, MENG Linggang, YA Bin, ZHANG Xingguo. Mechanical Properties and Energy Release Mechanism of Zr-Al-Ni-Cu-Hf Bulk Metallic Glasses. Acta Metall Sin, 2025, 61(11): 1738-1746.
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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%.
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Received: 08 March 2024
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Corresponding Authors:
ZHANG Xingguo, professor, Tel: (0411)84706183, E-mail: zxgwj@dlut.edu.cn
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