E. Zhu, Fuguo Li, Qian Zhao, Xuehan An, Jingyuan Niu, Anisah Farooq Hashmi
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The results demonstrate that there is no obvious SIM <span>\\({\\alpha }^{\\prime\\prime}\\)</span> stress platform in the compressive stress–strain curve; however, it exhibits a higher yield stress and strain hardening capability than tensile deformation although SIM <span>\\({\\alpha }^{\\prime\\prime}\\)</span> and <span>\\({\\alpha }^{\\prime\\prime}\\)</span> martensite twinning are the major deformation products that appeared in metastable <span>\\(\\beta\\)</span> Ti-1023 alloy under both tensile and compressive loading. In fact, SIM <span>\\({\\alpha }^{\\prime\\prime}\\)</span> is preferentially activated in well-oriented <span>\\(\\beta\\)</span> grains at the beginning of deformation, and those activated variants have the largest phase transformation strain along the loading direction affected by the loading stress state. As the accumulated deformation strain increases, SIM <span>\\({\\alpha }^{\\prime\\prime}\\)</span> is reoriented to form a martensite co-deformation region with twin structures through {111}<sub><i>α</i>″</sub> type I and <211><sub><i>α</i>″</sub> type II twinning systems. Then, the primary lath <span>\\({\\alpha }^{\\prime\\prime}\\)</span> martensite is consumed, resulting in the development of the {130} <310><sub><i>α</i>″</sub> and {110} <span>\\(<\\!110\\!>_{{\\alpha }^{\\prime\\prime}}\\)</span> deformation twinning inside the martensite. In comparison with tensile deformation, compressive deformation produces a higher volume fraction of SIM <span>\\({\\alpha }^{\\prime\\prime}\\)</span> and <span>\\({\\alpha }^{\\prime\\prime}\\)</span> martensite twins in <span>\\(\\beta\\)</span> grains, along with a higher density of dislocations in the <span>\\({\\alpha }^{\\prime\\prime}\\)</span> martensite and the coordinated deformation region of the martensite. This results in a higher work hardening ability of the alloy under compression and a marked asymmetry of mechanical characteristics compared to tensile deformation.</p></div>","PeriodicalId":645,"journal":{"name":"Journal of Materials Science","volume":"59 30","pages":"13978 - 13999"},"PeriodicalIF":3.5000,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Asymmetry of microstructure and mechanical characteristics in metastable Ti–10V–2Fe–3Al alloy under tension and compression\",\"authors\":\"E. Zhu, Fuguo Li, Qian Zhao, Xuehan An, Jingyuan Niu, Anisah Farooq Hashmi\",\"doi\":\"10.1007/s10853-024-09955-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The microstructure evolution of stress-induced martensite (SIM) <span>\\\\({\\\\alpha }^{\\\\prime\\\\prime}\\\\)</span> and mechanical twins in metastable <span>\\\\(\\\\beta\\\\)</span> Ti-1023 alloy under different strains during tensile and compressive deformation was investigated by the help of X-ray diffraction, scanning electron microscopy, electron backscatter diffraction and transmission electron microscopy. The results demonstrate that there is no obvious SIM <span>\\\\({\\\\alpha }^{\\\\prime\\\\prime}\\\\)</span> stress platform in the compressive stress–strain curve; however, it exhibits a higher yield stress and strain hardening capability than tensile deformation although SIM <span>\\\\({\\\\alpha }^{\\\\prime\\\\prime}\\\\)</span> and <span>\\\\({\\\\alpha }^{\\\\prime\\\\prime}\\\\)</span> martensite twinning are the major deformation products that appeared in metastable <span>\\\\(\\\\beta\\\\)</span> Ti-1023 alloy under both tensile and compressive loading. In fact, SIM <span>\\\\({\\\\alpha }^{\\\\prime\\\\prime}\\\\)</span> is preferentially activated in well-oriented <span>\\\\(\\\\beta\\\\)</span> grains at the beginning of deformation, and those activated variants have the largest phase transformation strain along the loading direction affected by the loading stress state. As the accumulated deformation strain increases, SIM <span>\\\\({\\\\alpha }^{\\\\prime\\\\prime}\\\\)</span> is reoriented to form a martensite co-deformation region with twin structures through {111}<sub><i>α</i>″</sub> type I and <211><sub><i>α</i>″</sub> type II twinning systems. Then, the primary lath <span>\\\\({\\\\alpha }^{\\\\prime\\\\prime}\\\\)</span> martensite is consumed, resulting in the development of the {130} <310><sub><i>α</i>″</sub> and {110} <span>\\\\(<\\\\!110\\\\!>_{{\\\\alpha }^{\\\\prime\\\\prime}}\\\\)</span> deformation twinning inside the martensite. 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引用次数: 0
摘要
通过 X 射线衍射、扫描电子显微镜、电子反向散射衍射和透射电子显微镜,研究了在拉伸和压缩变形过程中,不同应变下应力诱导马氏体(SIM)的显微组织演化和孪晶。结果表明,在压缩应力-应变曲线上没有明显的 SIM ({\alpha }^{\prime\prime}\)应力平台;然而,与拉伸变形相比,它表现出了更高的屈服应力和应变硬化能力,尽管在拉伸和压缩载荷下,SIM ({\alpha }^{prime\prime})和马氏体孪晶是可变型 \(\beta\) Ti-1023 合金中出现的主要变形产物。事实上,SIM ({\alpha }^{\prime\prime}\)在变形开始时优先在取向良好的(beta)晶粒中活化,并且这些活化变体受加载应力状态的影响沿加载方向具有最大的相变应变。随着累积变形应变的增加,SIM({\α }^{\prime\prime}\)被重新定向,通过{111}α″ I 型和 <211>α″ II 型孪晶体系形成具有孪晶结构的马氏体共变形区。然后,初级板条马氏体被消耗,导致马氏体内部发展出{130} <310>α″和{110} \(<\!110!>_{/α}^{/prime/prime}})变形孪晶。与拉伸变形相比,压缩变形在马氏体晶粒中产生了更高体积分数的SIM({\alpha }^{\prime\prime}\)和({\alpha }^{\prime\prime}\)马氏体孪晶,同时在({\alpha }^{\prime\prime}\)马氏体和马氏体的协调变形区域产生了更高密度的位错。这使得合金在压缩条件下具有更高的加工硬化能力,与拉伸变形相比,其机械特性具有明显的不对称性。
Asymmetry of microstructure and mechanical characteristics in metastable Ti–10V–2Fe–3Al alloy under tension and compression
The microstructure evolution of stress-induced martensite (SIM) \({\alpha }^{\prime\prime}\) and mechanical twins in metastable \(\beta\) Ti-1023 alloy under different strains during tensile and compressive deformation was investigated by the help of X-ray diffraction, scanning electron microscopy, electron backscatter diffraction and transmission electron microscopy. The results demonstrate that there is no obvious SIM \({\alpha }^{\prime\prime}\) stress platform in the compressive stress–strain curve; however, it exhibits a higher yield stress and strain hardening capability than tensile deformation although SIM \({\alpha }^{\prime\prime}\) and \({\alpha }^{\prime\prime}\) martensite twinning are the major deformation products that appeared in metastable \(\beta\) Ti-1023 alloy under both tensile and compressive loading. In fact, SIM \({\alpha }^{\prime\prime}\) is preferentially activated in well-oriented \(\beta\) grains at the beginning of deformation, and those activated variants have the largest phase transformation strain along the loading direction affected by the loading stress state. As the accumulated deformation strain increases, SIM \({\alpha }^{\prime\prime}\) is reoriented to form a martensite co-deformation region with twin structures through {111}α″ type I and <211>α″ type II twinning systems. Then, the primary lath \({\alpha }^{\prime\prime}\) martensite is consumed, resulting in the development of the {130} <310>α″ and {110} \(<\!110\!>_{{\alpha }^{\prime\prime}}\) deformation twinning inside the martensite. In comparison with tensile deformation, compressive deformation produces a higher volume fraction of SIM \({\alpha }^{\prime\prime}\) and \({\alpha }^{\prime\prime}\) martensite twins in \(\beta\) grains, along with a higher density of dislocations in the \({\alpha }^{\prime\prime}\) martensite and the coordinated deformation region of the martensite. This results in a higher work hardening ability of the alloy under compression and a marked asymmetry of mechanical characteristics compared to tensile deformation.
期刊介绍:
The Journal of Materials Science publishes reviews, full-length papers, and short Communications recording original research results on, or techniques for studying the relationship between structure, properties, and uses of materials. The subjects are seen from international and interdisciplinary perspectives covering areas including metals, ceramics, glasses, polymers, electrical materials, composite materials, fibers, nanostructured materials, nanocomposites, and biological and biomedical materials. The Journal of Materials Science is now firmly established as the leading source of primary communication for scientists investigating the structure and properties of all engineering materials.