2010
DOI: 10.1007/s00466-010-0555-4
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Finite element simulations of poly-crystalline shape memory alloys based on a micromechanical model

Abstract: We present a finite element implementation of a micromechanically motivated model for poly-crystalline shape memory alloys, based on energy minimization principles. The implementation allows simulation of anisotropic material behavior as well as the pseudo-elastic and pseudoplastic material response of whole samples. The evolving phase distribution over the entire specimen is calculated. The finite element model predicts the material properties for a relatively small number of grains. For different points of i… Show more

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Cited by 18 publications
(9 citation statements)
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“…In the present work, the material model developed by is used which is a mathematically condensed version of the micromechanical models introduced in Hackl et al (2004), Hackl and Heinen (2008), and Junker and Hackl (2011). Due to a simplified description of the polycrystalline orientation distribution function of the martensitic strain (which must not be confused with an orientation distribution function for the grains or texture), this model proves to be numerically very efficient.…”
Section: Model For Polycrystalline Shape Memory Alloysmentioning
confidence: 98%
See 1 more Smart Citation
“…In the present work, the material model developed by is used which is a mathematically condensed version of the micromechanical models introduced in Hackl et al (2004), Hackl and Heinen (2008), and Junker and Hackl (2011). Due to a simplified description of the polycrystalline orientation distribution function of the martensitic strain (which must not be confused with an orientation distribution function for the grains or texture), this model proves to be numerically very efficient.…”
Section: Model For Polycrystalline Shape Memory Alloysmentioning
confidence: 98%
“…A detailed excursion into implementation issues for polycrystalline shape memory can be found in Junker and Hackl (2011). Let us mention that the result of any finite element calculation is an approximation of the minimizer of the Gibbs free energy , defined as…”
Section: Finite Element Simulations Of Tension Testsmentioning
confidence: 99%
“…While phase transformation is proceeding, other grains may become active until (nearly) the entire material has transformed. However, implementation of such a model into a finite element code reveals that such a model is very time consuming and thus not appropriate for an industrial use (see [15]). Therefore, the polycrystalline character is condensed to a modeling approach in which a dynamically evolving orientation distribution function is considered and parameterized by Euler angles.…”
Section: Materials Modelmentioning
confidence: 99%
“…In addition to the energy, we need to make assumptions concerning the dissipation functional. As in previous works, for example, , we chose the dissipation functional to consist of the norm of the rate of the volume fractions truebold-italicλ̇, and newly of the skew symmetric matrix of angular velocities bold-italicΩ MathClass-punc:MathClass-rel=truebold-italicQ̇MathClass-bin⋅QMathClass-bin−1, weighted with some parameters r λ and r α , thus, scriptDMathClass-rel=rλMathClass-rel|truebold-italicλ̇MathClass-rel|MathClass-bin+rαMathClass-rel|MathClass-rel|bold-italicΩMathClass-rel|MathClass-rel|MathClass-rel=rλMathClass-rel|truebold-italicλ̇MathClass-rel|MathClass-bin+2rα ()trueϕ̇2 MathClass-bin+ trueν̇2 MathClass-bin+2trueϕ̇trueω̇normalcosν MathClass-bin+ trueω̇21MathClass-bin∕22.56804pttmspace The use of Ω , instead of truebold-italicα̇ for instance, ensures frame‐independence. The respective derivatives then yield scriptD truebold-italicλ̇ MathClass-rel=rλ truebold-italicλ̇ MathClass-rel|truebold-italicλ̇MathClass-rel|2emqquadand2emqquad scriptD truebold-italicα̇ MathClass-rel=2 rα MathClass-rel|MathClass-rel|bold-italicΩMathClass-rel|MathClass-rel| …”
Section: Materials Modelmentioning
confidence: 99%
“…In addition to the energy, we need to make assumptions concerning the dissipation functional. As in previous works, for example, [11,17,26], we chose the dissipation functional to consist of the norm of the rate of the volume fractions P , and newly of the skew symmetric matrix of angular velocities WD P Q Q 1 , weighted with some parameters r and r˛, thus,…”
Section: Dissipation Functionalmentioning
confidence: 99%