Tianchang Ma , Leon Shimmi , Yuyang Bai , Tomotaka Miyazawa , Sukyoung Hwang , Shigeo Arai , Toshiyuki Fujii
{"title":"近1¯11取向铜单晶循环变形过程中细胞边界的结晶学性质","authors":"Tianchang Ma , Leon Shimmi , Yuyang Bai , Tomotaka Miyazawa , Sukyoung Hwang , Shigeo Arai , Toshiyuki Fujii","doi":"10.1016/j.ijfatigue.2025.109328","DOIUrl":null,"url":null,"abstract":"<div><div>Given the strong correlation between fatigue crack initiation and dislocation cell structures, elucidating the crystallographic nature of cell boundaries is fundamental to understanding fatigue mechanisms. In this study, three-dimensional electron backscatter diffraction combined with focused ion beam slicing was employed to characterize the formation planes of cell boundaries in a fatigued copper single crystal oriented near the <span><math><mrow><mfenced><mrow><mover><mrow><mtext>1</mtext></mrow><mrow><mo>¯</mo></mrow></mover><mtext>11</mtext></mrow></mfenced></mrow></math></span> direction. Beyond the (111) boundaries representative of mature cell structures, (110), (011), and (121) boundaries were identified as geometrically necessary segments initiated by cross-slip, which forms at the early stage of cell structures. The (110) and (011) boundaries include dislocation networks formed by Shockley partials dissociated from the perfect dislocations on different potentially activated slip planes. Subsequently, the (121) boundaries emerge after the cross-slip of screw dislocations and pile-up on the cross-slip plane. Cell bands preferentially form along the (121) plane because of the symmetrically arranged alternating {110} boundaries. The rotation axis between adjacent cells exhibits a strong dependence on misorientation angle, and the rotation axes are scattered around the [111] and [121] directions when the misorientation is small (<1.0°). The [121] axis originates from the vector sum of [110] and [011], which corresponds to twist boundaries on the (110) and (011) planes. The (111) twist boundaries form and gradually replace the other geometrically necessary boundaries with an increase in the misorientation to accommodate increasing plastic incompatibility. This study uncovers the crystallographic nature of fatigue-induced cell structures and offers insights into enhancing metal performance through dislocation control.</div></div>","PeriodicalId":14112,"journal":{"name":"International Journal of Fatigue","volume":"203 ","pages":"Article 109328"},"PeriodicalIF":6.8000,"publicationDate":"2025-10-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Crystallographic nature of cell boundaries developed during cyclic deformation of a near-1¯11-oriented copper single crystal\",\"authors\":\"Tianchang Ma , Leon Shimmi , Yuyang Bai , Tomotaka Miyazawa , Sukyoung Hwang , Shigeo Arai , Toshiyuki Fujii\",\"doi\":\"10.1016/j.ijfatigue.2025.109328\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Given the strong correlation between fatigue crack initiation and dislocation cell structures, elucidating the crystallographic nature of cell boundaries is fundamental to understanding fatigue mechanisms. In this study, three-dimensional electron backscatter diffraction combined with focused ion beam slicing was employed to characterize the formation planes of cell boundaries in a fatigued copper single crystal oriented near the <span><math><mrow><mfenced><mrow><mover><mrow><mtext>1</mtext></mrow><mrow><mo>¯</mo></mrow></mover><mtext>11</mtext></mrow></mfenced></mrow></math></span> direction. Beyond the (111) boundaries representative of mature cell structures, (110), (011), and (121) boundaries were identified as geometrically necessary segments initiated by cross-slip, which forms at the early stage of cell structures. The (110) and (011) boundaries include dislocation networks formed by Shockley partials dissociated from the perfect dislocations on different potentially activated slip planes. Subsequently, the (121) boundaries emerge after the cross-slip of screw dislocations and pile-up on the cross-slip plane. Cell bands preferentially form along the (121) plane because of the symmetrically arranged alternating {110} boundaries. The rotation axis between adjacent cells exhibits a strong dependence on misorientation angle, and the rotation axes are scattered around the [111] and [121] directions when the misorientation is small (<1.0°). The [121] axis originates from the vector sum of [110] and [011], which corresponds to twist boundaries on the (110) and (011) planes. The (111) twist boundaries form and gradually replace the other geometrically necessary boundaries with an increase in the misorientation to accommodate increasing plastic incompatibility. This study uncovers the crystallographic nature of fatigue-induced cell structures and offers insights into enhancing metal performance through dislocation control.</div></div>\",\"PeriodicalId\":14112,\"journal\":{\"name\":\"International Journal of Fatigue\",\"volume\":\"203 \",\"pages\":\"Article 109328\"},\"PeriodicalIF\":6.8000,\"publicationDate\":\"2025-10-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Fatigue\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0142112325005250\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ENGINEERING, MECHANICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Fatigue","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0142112325005250","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, MECHANICAL","Score":null,"Total":0}
Crystallographic nature of cell boundaries developed during cyclic deformation of a near-1¯11-oriented copper single crystal
Given the strong correlation between fatigue crack initiation and dislocation cell structures, elucidating the crystallographic nature of cell boundaries is fundamental to understanding fatigue mechanisms. In this study, three-dimensional electron backscatter diffraction combined with focused ion beam slicing was employed to characterize the formation planes of cell boundaries in a fatigued copper single crystal oriented near the direction. Beyond the (111) boundaries representative of mature cell structures, (110), (011), and (121) boundaries were identified as geometrically necessary segments initiated by cross-slip, which forms at the early stage of cell structures. The (110) and (011) boundaries include dislocation networks formed by Shockley partials dissociated from the perfect dislocations on different potentially activated slip planes. Subsequently, the (121) boundaries emerge after the cross-slip of screw dislocations and pile-up on the cross-slip plane. Cell bands preferentially form along the (121) plane because of the symmetrically arranged alternating {110} boundaries. The rotation axis between adjacent cells exhibits a strong dependence on misorientation angle, and the rotation axes are scattered around the [111] and [121] directions when the misorientation is small (<1.0°). The [121] axis originates from the vector sum of [110] and [011], which corresponds to twist boundaries on the (110) and (011) planes. The (111) twist boundaries form and gradually replace the other geometrically necessary boundaries with an increase in the misorientation to accommodate increasing plastic incompatibility. This study uncovers the crystallographic nature of fatigue-induced cell structures and offers insights into enhancing metal performance through dislocation control.
期刊介绍:
Typical subjects discussed in International Journal of Fatigue address:
Novel fatigue testing and characterization methods (new kinds of fatigue tests, critical evaluation of existing methods, in situ measurement of fatigue degradation, non-contact field measurements)
Multiaxial fatigue and complex loading effects of materials and structures, exploring state-of-the-art concepts in degradation under cyclic loading
Fatigue in the very high cycle regime, including failure mode transitions from surface to subsurface, effects of surface treatment, processing, and loading conditions
Modeling (including degradation processes and related driving forces, multiscale/multi-resolution methods, computational hierarchical and concurrent methods for coupled component and material responses, novel methods for notch root analysis, fracture mechanics, damage mechanics, crack growth kinetics, life prediction and durability, and prediction of stochastic fatigue behavior reflecting microstructure and service conditions)
Models for early stages of fatigue crack formation and growth that explicitly consider microstructure and relevant materials science aspects
Understanding the influence or manufacturing and processing route on fatigue degradation, and embedding this understanding in more predictive schemes for mitigation and design against fatigue
Prognosis and damage state awareness (including sensors, monitoring, methodology, interactive control, accelerated methods, data interpretation)
Applications of technologies associated with fatigue and their implications for structural integrity and reliability. This includes issues related to design, operation and maintenance, i.e., life cycle engineering
Smart materials and structures that can sense and mitigate fatigue degradation
Fatigue of devices and structures at small scales, including effects of process route and surfaces/interfaces.