Deformation of Nanoglass under High-pressure Torsion

Yue Dong, H. Fecht
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Abstract

Metallic glasses are amorphous solids with metallic atomic bonds. Different from traditional crystalline metals, they have no long-range atomic order. Only short-range order on the scale of 0.5–1 nm can be detected [1-4]. Because of the lack of a lattice dislocation slip system, as in crystalline alloys, metallic glasses exhibit some outstanding properties, such as high elastic strain, high hardness and high strength [5-7]. The yield strengths of Zr-based bulk metallic glasses (BMGs) are approximately 2 GPa in compression. Unfortunately, this special structure also creates problems; that is, plastic deformation in BMGs is always concentrated in localized regions, namely, shear bands, resulting in catastrophic failure [8]. This brittleness restricts their industrial applications. Zr64Ni10Al7Cu19 is a BMG system [9,10] with good glass forming ability and high strength but no plastic strain under tensile testing.
高压扭转作用下纳米玻璃的变形
金属玻璃是具有金属原子键的无定形固体。与传统的结晶金属不同,它们没有长程原子序。只能检测到0.5-1 nm尺度上的短程序列[1-4]。由于缺乏晶格位错滑移系统,金属玻璃表现出一些突出的性能,如高弹性应变、高硬度和高强度[5-7]。zr基大块金属玻璃(bmg)的屈服强度约为2gpa。不幸的是,这种特殊的结构也会产生问题;即bmg的塑性变形总是集中在局部区域,即剪切带,导致突变破坏[8]。这种脆性限制了它们的工业应用。Zr64Ni10Al7Cu19是一种BMG体系[9,10],具有良好的玻璃化形成能力和高强度,但拉伸试验无塑性应变。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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