Cu-Zr大块金属玻璃力学性能与局部原子结构的关系

S. Jekal
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引用次数: 0

摘要

大块金属玻璃(bmg)因其优异的弹性应变极限和高拉伸屈服应力等力学性能而备受关注[1-6]。例如,它们的屈服强度可达1 ~ 5GPa,弹性应变极限可达~2%[7-10]。然而,由于bmg表现出局部应变软化,导致失效和脆性,因此它们在工程应用中的应用一直具有挑战性。潜在的原子尺度塑性机制被认为是由局部微观机制介导的[11-14]。这种局部化过程已经在高应变变形原子模拟中被观察到[15-22],激发了剪切转变区(STZ)概念和非热玻璃塑性有效温度理论的发展[23-25]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Links Between Mechanical Properties and Local Atomic Structures of Cu–Zr Bulk Metallic Glasses
Bulk metallic glasses (BMGs) have drawn much attention due to their interesting mechanical properties such as extraordinary elastic strain limits and a high tensile yield stress [1-6]. For example, their yield strengths can be up to 1 to 5GPa and elastic strain limits up to ~2% [7-10]. However, their use for engineering applications has been challenging since BMGs exhibit localized strain softening leading to failure and brittleness. The underlying atomicscale plastic mechanisms are believed to be mediated by a local microscopic mechanism [11-14]. Such localized processes have been observed during high-strain deformation atomistuc simulations [15-22] inspiring the development of the shear transformation zone (STZ) concept and the effective temperature theory of athermal glass plasticity [23-25].
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