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纳米压痕过程中纳米孪晶铜孪晶界内禀扭折缺陷与位错相互作用的原子尺度研究

Atomistic Study of Interactions between Intrinsic Kink Defects and Dislocations in Twin Boundaries of Nanotwinned Copper during Nanoindentation.

作者信息

Hu Xiaowen, Ni Yushan, Zhang Zhongli

机构信息

Department of Aeronautics and Astronautics, Fudan University, Shanghai 200433, China.

Shanghai Institute of Measurement and Testing Technology, Shanghai 201203, China.

出版信息

Nanomaterials (Basel). 2020 Jan 28;10(2):221. doi: 10.3390/nano10020221.

DOI:10.3390/nano10020221
PMID:32012856
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7074976/
Abstract

In order to study the effects of kink-like defects in twin boundaries on deformation mechanisms and interaction between dislocations and defects in twin boundaries under localized load, nanotwinned Cu with two defective twin (TDT) boundaries is compared with the nanotwinned Cu with two perfect twin (TPT) boundaries, and nanotwinned Cu with single defective twin (SDT) boundary and single perfect twin boundary by simulating spherical nanoindentations using molecular mechanics. The indenter force-depth and hardness-contact strain responses were analyzed. Results show that the existence of intrinsic defects in twin boundary could reduce the critical load and critical hardness of nanotwinned material. A quantitative parameter was first proposed to evaluate the degree of surface atom accumulation around the indenter during nanoindentation, and it can be inferred that the surface morphology in TDT changes more frequently than the surface morphologies in TPT and SDT. The atomistic configurations of incipient plastic structures of three different models were also analyzed. We found that the intrinsic defects in twin boundary will affect the incipient plastic structures. The formation of twinning partial slip on the defective twin boundary happens before the contact of the dislocation and twin boundary. The kink-like defects could introduce Frank partial dislocation to the twin boundary during interaction between dislocation and twin boundary, which was not detected on the perfect twin boundary. In addition, the area of twinning partial slips on the upper twin boundary in the incipient plastic structures in SDT and TDT are larger than the twinning partial slip area in TPT, which results in the reduction of the critical hardness in SDT and TDT. The kink-like defects could also block the expansion of twinning partial slip on the twin boundary. Furthermore, we investigated the dislocation transmission processes in three different models. It is found that the dislocation transmission event could be delayed in model containing single defective twin boundary, while the transmission process could be advanced in model containing two consecutive defective twin boundaries. The quantitative analysis of dislocation length was also implemented. Result shows that the main emitted dislocation during nanoindentation is Shockley partial, and the dislocation nucleation in SDT and TDT is earlier than the dislocation nucleation in TPT due to the existence of defects. It is inferred that the intrinsic defects on twin boundaries could enhance the interaction between dislocations and twin boundaries, and could strongly change the structure evolution and promote the dislocation nucleation and emission. These findings about kink-like defects in twin boundaries show that the inherent kink-like defects play a crucial role in the deformation mechanisms and it should be taken into consideration in future investigations. Single defective twin boundary structure is recommended to delay the transmission and block the expansion of twin boundary migration. Some of the results are in good agreement with experiments.

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/f2fe7ffe14bf/nanomaterials-10-00221-g012a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/b5c241e58cb2/nanomaterials-10-00221-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/c1c890869bd9/nanomaterials-10-00221-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/4dd9e062113e/nanomaterials-10-00221-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/8b84243c0f5e/nanomaterials-10-00221-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/122416bce17d/nanomaterials-10-00221-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/c86a58fd8ce6/nanomaterials-10-00221-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/caab61a29355/nanomaterials-10-00221-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/c8195b998966/nanomaterials-10-00221-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/5d48f4883aaa/nanomaterials-10-00221-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/faa06ff4952e/nanomaterials-10-00221-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/4a4d6ea9e9d5/nanomaterials-10-00221-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/f2fe7ffe14bf/nanomaterials-10-00221-g012a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/b5c241e58cb2/nanomaterials-10-00221-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/c1c890869bd9/nanomaterials-10-00221-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/4dd9e062113e/nanomaterials-10-00221-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/8b84243c0f5e/nanomaterials-10-00221-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/122416bce17d/nanomaterials-10-00221-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/c86a58fd8ce6/nanomaterials-10-00221-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/caab61a29355/nanomaterials-10-00221-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/c8195b998966/nanomaterials-10-00221-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/5d48f4883aaa/nanomaterials-10-00221-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/faa06ff4952e/nanomaterials-10-00221-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/4a4d6ea9e9d5/nanomaterials-10-00221-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/49eb/7074976/f2fe7ffe14bf/nanomaterials-10-00221-g012a.jpg
摘要

为了研究孪晶界中的扭折状缺陷对局部载荷下孪晶界中位错与缺陷之间的变形机制及相互作用的影响,通过分子力学模拟球形纳米压痕,将具有两个缺陷孪晶(TDT)界的纳米孪晶铜与具有两个完美孪晶(TPT)界的纳米孪晶铜、具有单个缺陷孪晶(SDT)界和单个完美孪晶界的纳米孪晶铜进行比较。分析了压痕力-深度和硬度-接触应变响应。结果表明,孪晶界中本征缺陷的存在会降低纳米孪晶材料的临界载荷和临界硬度。首次提出了一个定量参数来评估纳米压痕过程中压头周围表面原子积累的程度,可以推断TDT中的表面形貌比TPT和SDT中的表面形貌变化更频繁。还分析了三种不同模型初始塑性结构的原子构型。我们发现孪晶界中的本征缺陷会影响初始塑性结构。在缺陷孪晶界上孪生部分滑移的形成发生在位错与孪晶界接触之前。在与孪晶界相互作用过程中,扭折状缺陷会将弗兰克部分位错引入孪晶界,而在完美孪晶界上未检测到这种情况。此外,SDT和TDT初始塑性结构中上部孪晶界上孪生部分滑移的面积大于TPT中孪生部分滑移的面积,这导致SDT和TDT中临界硬度降低。扭折状缺陷还会阻碍孪晶界上孪生部分滑移的扩展。此外,我们研究了三种不同模型中的位错传输过程。发现在包含单个缺陷孪晶界的模型中,位错传输事件可能会延迟,而在包含两个连续缺陷孪晶界的模型中,传输过程可能会提前。还对位错长度进行了定量分析。结果表明,纳米压痕过程中主要发射的位错是肖克利部分位错,由于缺陷的存在,SDT和TDT中的位错形核比TPT中的位错形核更早。推断孪晶界上的本征缺陷会增强位错与孪晶界之间的相互作用,并能强烈改变结构演化,促进位错形核和发射。关于孪晶界中扭折状缺陷的这些发现表明,固有的扭折状缺陷在变形机制中起关键作用,在未来的研究中应予以考虑。建议采用单个缺陷孪晶界结构来延迟传输并阻碍孪晶界迁移的扩展。部分结果与实验结果吻合良好。

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