3Al單晶;晶體塑性;位錯(cuò);滑移系;有限元;本構(gòu)關(guān)系"/> 3Al單晶的細(xì)觀本構(gòu)關(guān)系,并利用ABAQUS/UMAT用戶子程序接口開發(fā)本構(gòu)關(guān)系子程序,將其應(yīng)用于不同取向Ti3Al單晶的單向壓縮模擬。分析不同取向時(shí)晶體滑移系的啟動(dòng)情況,以及滑移系啟動(dòng)與取向的相互關(guān)系。結(jié)果表明:基面滑移系(0001)<110>,柱面滑移系{100}<110>和錐面滑移系{111}<116>均被激活,但由于滑移系之間臨界剪切應(yīng)力和施密特因子的不同,各滑移系的啟動(dòng)情況存在顯著差異?;婧湾F面滑移系的臨界剪切應(yīng)力較大,僅在施密特因子較大時(shí)啟動(dòng);特別是錐面滑移系,其臨界剪切應(yīng)力最大,因而該滑移系只有在壓縮軸接近[0001]方向時(shí)才被激活。柱面滑移系的啟動(dòng)較為容易,對(duì)塑性變形的貢獻(xiàn)也最大。同時(shí)與實(shí)驗(yàn)結(jié)果相比較,本研究模擬結(jié)果基本與之吻合。"/>

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Ti3Al單晶塑性變形行為的晶體塑性有限元模擬
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湘潭大學(xué)機(jī)械工程學(xué)院,湘潭大學(xué)機(jī)械工程學(xué)院,湘潭大學(xué)機(jī)械工程學(xué)院,東北大學(xué)材料科學(xué)與工程學(xué)院,湘潭大學(xué)機(jī)械工程學(xué)院,蘇州大學(xué)沙鋼鋼鐵學(xué)院

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國家自然科學(xué)基金資助(項(xiàng)目號(hào)51175445,51201147,51304141),湖南省自然科學(xué)基金資助(項(xiàng)目號(hào)14JJ6016)


Simulation of Plastic Deformation Behaviors of Ti3Al Single Crystal with Crystal Plasticity Finite Element Method
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School of Mechanical Engineering,Xiangtan University,School of Mechanical Engineering,Xiangtan University,School of Mechanical Engineering,Xiangtan University,,School of Mechanical Engineering,Xiangtan University,Shagang School of Iron and Steel,Soochow University

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    基于晶體塑性理論,本研究建立滑移變形機(jī)制下Ti3Al單晶的細(xì)觀本構(gòu)關(guān)系,并利用ABAQUS/UMAT用戶子程序接口開發(fā)本構(gòu)關(guān)系子程序,將其應(yīng)用于不同取向Ti3Al單晶的單向壓縮模擬。分析不同取向時(shí)晶體滑移系的啟動(dòng)情況,以及滑移系啟動(dòng)與取向的相互關(guān)系。結(jié)果表明:基面滑移系(0001)<110>,柱面滑移系{100}<110>和錐面滑移系{111}<116>均被激活,但由于滑移系之間臨界剪切應(yīng)力和施密特因子的不同,各滑移系的啟動(dòng)情況存在顯著差異。基面和錐面滑移系的臨界剪切應(yīng)力較大,僅在施密特因子較大時(shí)啟動(dòng);特別是錐面滑移系,其臨界剪切應(yīng)力最大,因而該滑移系只有在壓縮軸接近[0001]方向時(shí)才被激活。柱面滑移系的啟動(dòng)較為容易,對(duì)塑性變形的貢獻(xiàn)也最大。同時(shí)與實(shí)驗(yàn)結(jié)果相比較,本研究模擬結(jié)果基本與之吻合。

    Abstract:

    A crystal plasticity constitutive model for Ti3Al single crystal was established based on slip deformation mechanism within the frame of crystal plasticity theory, and it was compiled to a program to describe it by means of secondary development of ABAQUS/UMAT user subroutine. Then we applied it to simulate the mechanical behaviors of Ti3Al single crystal with different orientations during unidirectional compression deformation. The activation of slip systems and the interaction between activation and orientation has been analyzed. The simulation results show that basal slip of (0001)<112(—)0>, prismatic slip of {101(—)0}<112(—)0> , and pyramidal slip of {112(—)1}<112(—)6> can be activated. However, there are dramatic diference on the ease or complexity of activation of various slip systems, which is due to the difference of critical shearing stress and schmid factor. It is difficult for basal slip and pyramidal slip to be activated because of their larger critical shearing stress, which leads that the activation of basal slip and pyramidal slip just occurs with larger schmid factor. Pyramidal slip systems only can be initiated when compression axis is close to [0001] direction due to the maximum shearing critical shearing stress, especially. Prismatic slip is much easier to be activated and also has the largest contribution to plastic deformation. Furthermore, the simulation results were compared and in good agreement with the experimental results.

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趙文娟,唐安,林啟權(quán),任玉平,徐俊瑞,宋濱娜. Ti3Al單晶塑性變形行為的晶體塑性有限元模擬[J].稀有金屬材料與工程,2018,47(6):1753~1759.[Zhao Wenjuan, Tang An, Lin Qiquan, Ren Yuping, Xu Junrui, Song Binna. Simulation of Plastic Deformation Behaviors of Ti3Al Single Crystal with Crystal Plasticity Finite Element Method[J]. Rare Metal Materials and Engineering,2018,47(6):1753~1759.]
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  • 收稿日期:2016-05-06
  • 最后修改日期:2016-06-08
  • 錄用日期:2016-07-15
  • 在線發(fā)布日期: 2018-09-06
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