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无过多且可预先确定缺陷的金属玻璃中的剪切转变

Shear transformations in metallic glasses without excessive and predefinable defects.

作者信息

Zhang Zhen, Ding Jun, Ma Evan

机构信息

Center for Alloy Innovation and Design (CAID), State Key Laboratory for Mechanical Behavior of Materials, Xi'an Jiaotong University, Xi'an 710049, China.

出版信息

Proc Natl Acad Sci U S A. 2022 Nov 29;119(48):e2213941119. doi: 10.1073/pnas.2213941119. Epub 2022 Nov 21.

DOI:10.1073/pnas.2213941119
PMID:36409913
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9860280/
Abstract

Plastic flow in metallic glasses (MGs) is known to be mediated by shear transformations (STs), which have been hypothesized to preferentially initiate from identifiable local "defect" regions with loose atomic packing. Here we show that the above idea is incorrect, i.e., STs do not arise from signature structural defects that can be recognized . This conclusion is reached via a realistic MG model obtained by combining molecular dynamics (MD) and Monte Carlo simulations, achieving liquid solidification at an effective cooling rate as slow as 500 K/s to approach that typical in experiments for producing bulk MGs. At shear stresses before global yielding, only about 2% of the total atoms participate in STs, each event involving typically ~10 atoms. These observations rectify the excessive content of "liquid-like regions" retained from unrealistically fast quench in MD-produced glass models. Our findings also shed light on the indeterministic aspect of the ST sites/zones, which emerge with varying spatial locations and distribution depending on specific mechanical loading conditions.

摘要

众所周知,金属玻璃(MGs)中的塑性流动是由剪切转变(STs)介导的,据推测,剪切转变优先从具有疏松原子堆积的可识别局部“缺陷”区域开始。在此,我们表明上述观点是错误的,即剪切转变并非源于可识别的标志性结构缺陷。这一结论是通过结合分子动力学(MD)和蒙特卡罗模拟得到的一个真实的金属玻璃模型得出的,该模型在低至500K/s的有效冷却速率下实现液体凝固,以接近生产块状金属玻璃的典型实验速率。在整体屈服前的剪切应力作用下,仅约2%的总原子参与剪切转变,每次事件通常涉及约10个原子。这些观察结果纠正了分子动力学产生的玻璃模型中因不切实际的快速淬火而保留的过多“类液区域”内容。我们的研究结果还揭示了剪切转变位点/区域的不确定性,其会根据特定的机械加载条件以不同的空间位置和分布出现。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/4020884c83cc/pnas.2213941119fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/210c62d14e81/pnas.2213941119fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/281ce0566bf4/pnas.2213941119fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/c86cd01f3530/pnas.2213941119fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/485e4b137989/pnas.2213941119fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/4020884c83cc/pnas.2213941119fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/210c62d14e81/pnas.2213941119fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/281ce0566bf4/pnas.2213941119fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/c86cd01f3530/pnas.2213941119fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/485e4b137989/pnas.2213941119fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b03/9860280/4020884c83cc/pnas.2213941119fig05.jpg

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