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Zr基非晶合金的高温动态力学行为与局域失稳机制

HIGH-TEMPERATURE DYNAMIC MECHANICAL BEHAVIOR AND LOCALIZED INSTABILITY MECHANISMS OF ZR-BASED METALLIC GLASS

  • 摘要: 厘清非晶合金在高温、高应变率条件下的动态力学响应与局域失稳机制, 对理解其塑性变形、剪切带演化及灾变失效行为具有重要意义. 围绕室温玻璃态、过冷液相区及晶化敏感温区的 Zr41.2Ti13.8Cu12.5Ni10Be22.5 非晶合金静动态失效机制, 开展了298 K、673 K和873 K条件下的静、动态压缩试验, 应变率范围10−3 s−1 ~ 3000 s−1. 结合扫描电子显微镜对回收试样断口形貌进行微观表征. 并结合应力失效模型与温度软化模型对失效机制进行分析. 研究结果表明: 在 298 K和 673 K下, 材料由准静态进入动态加载后失效应力明显降低, 高应变率区间逐渐趋于稳定, 失效应变在动态加载范围内整体低于准静态加载水平; 在873 K下, 准静态压缩试样在测试应变范围内未发生宏观剪切断裂, 而动态加载下仍发生失稳破坏, 且失效应变维持较高水平, 说明材料在晶化敏感区的变形和失稳模式发生明显变化. 典型应变率(2586 s−1)加载下回收的试样断口形貌显示, 298 K时断口以局域化剪切特征为主, 673 K时滑移和熔融特征最显著, 873 K时细胞脉络状图案分布更均匀, 熔融区域占比降低. 应变能密度和归一化局域热失稳系数分析表明, 873 K下材料失效前具有较高的变形吸能能力, 但能量耗散更趋于分散. 结合应变率相关软化模型和温度软化修正可知, 673 K下失效应力降低主要源于高温软化作用, 而 873 K下实验失效应力随应变率先升高后缓慢降低, 表明结构状态变化对动态失效过程产生附加影响. 综合力学响应和断口形貌可知, 温度通过影响高温软化、剪切局域化、结构状态演化和能量耗散方式, 决定了 Zr 基非晶合金在动态压缩条件下的力学响应与局域失稳模式.

     

    Abstract: Clarifying the dynamic mechanical response and localized instability mechanism of metallic glasses under high-temperature and high-strain-rate conditions is essential for understanding their plastic deformation, shear-band evolution, and catastrophic failure behavior. Quasi-static and dynamic compression tests were conducted on Zr41.2Ti13.8Cu12.5Ni10Be22.5 bulk metallic glass over a strain-rate range of 10−3 s−1 ~ 3000 s−1 at 298 K, 673 K, and 873 K, corresponding to the room-temperature glassy state, supercooled liquid region, and crystallization-sensitive temperature region, respectively. The fracture morphologies of the recovered specimens were further characterized by scanning electron microscopy. The failure mechanism of the material was also analyzed by integrating the stress-failure model with the temperature-softening model. The results show that at 298 K and 673 K, the failure stress decreases markedly when the loading condition changes from quasi-static to dynamic compression and then tends to stabilize at higher dynamic strain rates, while the failure strain under dynamic loading is generally lower than that under quasi-static loading. At 873 K, the specimen under quasi-static compression does not exhibit macroscopic shear fracture within the tested strain range, whereas unstable failure still occurs under dynamic loading. Meanwhile, the failure strain remains at a relatively high level, indicating a marked change in deformation and instability mode. Fracture morphologies of specimens recovered at a representative strain rate of 2586 s−1 show that localized shear features dominate at 298 K, sliding and local melting features are most pronounced at 673 K, and the cell-like vein patterns become more uniformly distributed at 873 K with a reduced fraction of molten regions. Strain energy density and normalized local thermal instability coefficient analyses indicate that the alloy exhibits higher deformation energy absorption before failure at 873 K, while the energy dissipation becomes more dispersed. Combined with the strain-rate-correlated softening model and temperature-softening correction, the reduction in failure stress at 673 K is mainly attributed to high-temperature softening, whereas the failure stress at 873 K first increases and then decreases slowly with increasing strain rate, suggesting an additional effect of structural-state evolution on dynamic failure. These results indicate that temperature governs the dynamic compression response and localized instability mode of the Zr-based bulk metallic glass by regulating high-temperature softening, shear localization, structural-state evolution, and energy dissipation pathways.

     

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