A Multivariant model for single crystal shape memory alloy behavior

Abstract A general 3-D multivariant model based on thermodynamics and micromechanics for single crystal shape memory alloy (SMA) behavior is presented. This model is based on the habit plane and transformation directions for the variants of martensite in a given material. From this information, the single crystal behavior of the material to temperature and mechanical loads is derived using the concept of a thermodynamic driving force. The Eshelby–Kroner approach is utilized to determine the interaction energy between the variants, where it is assumed that variants can be subdivided into several self-accommodating groups in which variants can grow together compatibly. This model is examined initially for a simple 2-variant case and then extended to the typical 24 variant case. The multivariant model is shown to exhibit appropriate responses for uniaxial results on single crystals : the transformations occur instantaneously when the critical stress\temperature is reached ; both pseudoelasticity and the shape memory effect are captured. The model is also examined for responses to multiaxial loadings and the distinction between perfectly compatible and imperfectly compatible variants (with nonzero volumetric transformation strain) is discussed.

[1]  T. Shield Orientation dependence of the pseudoelastic behavior of single crystals of CuAlNi in tension , 1995 .

[2]  J. Ball,et al.  Fine phase mixtures as minimizers of energy , 1987 .

[3]  L. Brinson One-Dimensional Constitutive Behavior of Shape Memory Alloys: Thermomechanical Derivation with Non-Constant Material Functions and Redefined Martensite Internal Variable , 1993 .

[4]  F. Falk Ginzburg-Landau theory of static domain walls in shape-memory alloys , 1983 .

[5]  Keh Chih Hwang,et al.  Micromechanics modelling for the constitutive behavior of polycrystalline shape memory alloys. II: Study of the individual phenomena , 1993 .

[6]  L. Brinson,et al.  Temperature-induced phase transformation in a shape memory alloy: Phase diagram based kinetics approach , 1997 .

[7]  George J. Weng,et al.  Martensitic transformation and stress-strain relations of shape-memory alloys , 1997 .

[8]  Thomas J. Pence,et al.  A constitutive model for hysteretic phase transition behavior , 1994 .

[9]  C. Lexcellent,et al.  Micromechanics-based modeling of two-way memory effect of a single crystalline shape-memory alloy , 1997 .

[10]  Craig A. Rogers,et al.  One-Dimensional Thermomechanical Constitutive Relations for Shape Memory Materials , 1990 .

[11]  E. Kröner Zur plastischen verformung des vielkristalls , 1961 .

[12]  Franz Dieter Fischer,et al.  A micromechanical model for the kinetics of martensitic transformation , 1992 .

[13]  Toshio Mura,et al.  Micromechanics of defects in solids , 1982 .

[14]  T. Mura,et al.  The elastic field caused by a general ellipsoidal inclusion and the application to martensite formation , 1976 .

[15]  D. Lagoudas,et al.  Thermomechanical Response of Shape Memory Composites , 1994 .

[16]  Qingping Sun,et al.  Micromechanics modelling for the constitutive behavior of polycrystalline shape memory alloys. I: Derivation of general relations , 1993 .

[17]  C. Liang,et al.  A multi-dimensional constitutive model for shape memory alloys , 1992 .

[18]  K. Hwang,et al.  A micromechanics constitutive model of transformation plasticity with shear and dilatation effect , 1991 .

[19]  D. Lagoudas,et al.  A thermodynamical constitutive model for shape memory materials. Part I. The monolithic shape memory alloy , 1996 .

[20]  James K. Knowles,et al.  On the driving traction acting on a surface of strain discontinuity in a continuum , 1990 .

[21]  L. Schetky Shape-memory alloys , 1979 .

[22]  K. Tanaka,et al.  Thermodynamic models of pseudoelastic behaviour of shape memory alloys , 1992 .