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Acta Metall Sin  2025, Vol. 61 Issue (11): 1738-1746    DOI: 10.11900/0412.1961.2024.00071
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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
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%.

Key words:  bulk metallic glasses      glass-forming ability      room temperature plasticity      amorphous fragment      overpressure peak     
Received:  08 March 2024     
ZTFLH:  TG139  
Corresponding Authors:  ZHANG Xingguo, professor, Tel: (0411)84706183, E-mail: zxgwj@dlut.edu.cn

URL: 

https://www.ams.org.cn/EN/10.11900/0412.1961.2024.00071     OR     https://www.ams.org.cn/EN/Y2025/V61/I11/1738

Fig.1  XRD spectra of as-cast Zr55Al10Ni5Cu30 - x Hf x (x = 0, 1, 3, 5, 7, 10; atomic fraction, %) bulk metallic glasses (BMGs) with their critical diameters (Dc)
Fig.2  DSC curves of Zr55Al10Ni5Cu30 - x Hf x BMGs (Tg—glass transition temperature, Tx—crystallization temperature)
Fig.3  Line graph depicting the variation of Tg, Tx, and ΔTx with Hf content in Zr55Al10Ni5Cu30 - x Hf x BMGs (ΔTx—undercooled liquid phase range, ΔTx = Tx - Tg)
Fig.4  Compressive stress-strain curves of Zr55Al10Ni5-Cu30 - x Hf x (x = 0-10) BMGs with a diameter of 2 mm at room temperature
Fig.5  Line graph showing the changes in σy, σf, and εp with varying Hf content in Zr55Al10Ni5Cu30 - x Hf xBMGs (σy—yield strength, σf—fracture strength, εp—compressive plastic strain)
Fig.6  Serrated flow deformation diagram of compressive stress-strain curve for Zr55Al10Ni5Cu25Hf5 BMGs (Inset is a localized magnified view of the stress-strain curve in the strain range of 10.0% to 10.5%, Δσ—stress drop, ΔσE—stress increment, ΔεE—strain increment)
Fig.7  Δσ distribution histogram of Zr55Al10Ni5Cu25Hf5 BMGs (N—amount of stress drop)
Fig.8  Fractured surface morphologies of Zr55Al10Ni5Cu30 - x Hf x BMGs under compression (side view)
(a) x = 0 (b) x = 1 (c) x = 3 (d) x = 5 (e) x = 7 (f) x = 10
Fig.9  Shear band morphologies on the lateral surface of Zr55Al10Ni5Cu25Hf5 BMG
(a) shear bands (PSB—persistent shear band, SSB—second-order shear band, TSB—third-order shear band)
(b) region of formation of third-order shear bands (shown as the circle region)
Fig.10  Schematic of the spherical Zr55Al10Ni5Cu25Hf5 fragment impact in a quasi-confined chamber for overpressure measurement
Fig.11  High-speed photographic images of the impact fracture reaction process of Zr55Al10Ni5Cu25Hf5 fragments at different fragment impact velocities (v) (t—time)
(a) v = 734 m/s (b) v = 1079 m/s (c) v = 1360 m/s
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
Table 1  Experimental data of overpressure peak value for Zr55Al10Ni5Cu25Hf5 fragments
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
Table 2  Energy release efficiency of Zr55Al10Ni5Cu25Hf5 fragments
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