Three dimensional large deformation analysis of phase transformation in shape memory alloys

Shape memory alloys(SMAs)have been explored as smart materials and used as dampers,actuator elements,and smart sensors.An important character of SMAs is its ability to recover all of its large deformations in mechanical loading-unloading cycles without showing permanent deformation.This paper presen...

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Published inApplied mathematics and mechanics Vol. 31; no. 10; pp. 1261 - 1272
Main Author 夏开明 潘同燕 刘山洪
Format Journal Article
LanguageEnglish
Published Heidelberg Shanghai University Press 01.10.2010
Division of Engineering, Colorado School of Mines, Golden 80401, USA%Department of Civil and Environmental Engineering, Virginia Tech,Blackburg, VA 24061, USA%Department of Bridge Engineering, Chongqing Jiaotong University,Chongqing 400074, P. R. China
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Summary:Shape memory alloys(SMAs)have been explored as smart materials and used as dampers,actuator elements,and smart sensors.An important character of SMAs is its ability to recover all of its large deformations in mechanical loading-unloading cycles without showing permanent deformation.This paper presents a stress-induced phenomenological constitutive equation for SMAs,which can be used to describe the superelastic hysteresis loops and phase transformation between Martensite and Austenite.The Martensite fraction of SMAs is assumed to be dependent on deviatoric stress tensor.Therefore,phase transformation of SMAs is volume preserving during the phase transformation.The model is implemented in large deformation finite element code and cast in the updated Lagrangian scheme.In order to use the Cauchy stress and the linear strain in constitutive laws,a frame indifferent stress objective rate has to be used.In this paper,the Jaumann stress rate is used.Results of the numerical experiments conducted in this study show that the superelastic hysteresis loops arising with the phase transformation can be effectively captured.
Bibliography:shape memory alloys
TG139.6
shape memory alloys; phase transformation; superelasticity; large deformation; finite element
finite element
phase transformation
TB324
superelasticity
31-1650/O1
large deformation
ObjectType-Article-2
SourceType-Scholarly Journals-1
ObjectType-Feature-1
content type line 23
ISSN:0253-4827
1573-2754
DOI:10.1007/s10483-010-1359-7