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潘晓霞 余勇 谭云 陈裕泽. FeCrNi合金静动态物理本构模型研究[J]. 力学学报, 2008, 40(3): 407-412. DOI: 10.6052/0459-1879-2008-3-2006-543
引用本文: 潘晓霞 余勇 谭云 陈裕泽. FeCrNi合金静动态物理本构模型研究[J]. 力学学报, 2008, 40(3): 407-412. DOI: 10.6052/0459-1879-2008-3-2006-543
Xiaoxia Pan, Yong Yu, Yun Tan, Yuze Chen. The constitutive model of fecrni alloy subjected to static and dynamic loading[J]. Chinese Journal of Theoretical and Applied Mechanics, 2008, 40(3): 407-412. DOI: 10.6052/0459-1879-2008-3-2006-543
Citation: Xiaoxia Pan, Yong Yu, Yun Tan, Yuze Chen. The constitutive model of fecrni alloy subjected to static and dynamic loading[J]. Chinese Journal of Theoretical and Applied Mechanics, 2008, 40(3): 407-412. DOI: 10.6052/0459-1879-2008-3-2006-543

FeCrNi合金静动态物理本构模型研究

The constitutive model of fecrni alloy subjected to static and dynamic loading

  • 摘要: 以金属材料塑性变形的位错动力学为基础,将FeCrNi合金的流动应力分解为非热应力和热激活应力两部分.通过对该合金屈服应力随温度变化特性、屈服应力的应变速率特性、孪晶组织的温度特性及位错组态的应变速率特性进行分析,认为非热应力不只是应变的函数,还与温度和应变速率相关,因此对Johnson-Cook模型方程形式进行修正以描述非热应力. 同时认为影响热激活应力的微结构参数主要为位错阻碍间距\Deltal, 定义并推导出表征\Delta l演化的g函数的表达式,将其引入Kocks的热激活方程,从而建立FeCrNi合金的物理型本构模型.该模型初步实现了对FeCrNi合金从室温到高温、从准静态到动态塑性变形行为的描述.

     

    Abstract: In the present work, the flow stress of FeCrNi alloy is dividedinto two parts, athermal stress (long-range) and thermally activated stress(short-range), based on the dislocation dynamics of plastic deformation ofmetal material. Firstly, the yield stress, twins and dislocationconfigurations of the alloy are analyzed with the effect of temperature andstrain rate. Hence, modified Johnson-Cook model is introduced to describethe athermal stress. Secondly, the distance between dislocation barriers\Delta l was found to mainly affect the thermally activated stress andthe g(\gamma, \dot \gamma, T) function was educed andinput in the Kocks model. Therefore theconstitutive model of FeCrNi alloy was developed to describe the plasticresponse of FeCrNi alloy from low temperature to high temperature, andfrom static loading to dynamic loading.

     

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