Entropic stabilization of austenite in shape memory alloys

被引:3
作者
Elliott, Ryan S. [1 ]
Karls, Daniel S. [1 ]
机构
[1] Univ Minnesota, Dept Aerosp Engn & Mech, Minneapolis, MN 55455 USA
基金
美国国家科学基金会;
关键词
Entropic stabilization; Phase transformation; Vibrations; Constitutive behavior; Stability and bifurcation; MARTENSITIC PHASE-TRANSFORMATIONS; MOLECULAR-DYNAMICS SIMULATIONS; NI-AL ALLOYS; PSEUDOELASTIC BEHAVIOR; CRYSTALLINE SOLIDS; SINGLE-CRYSTALS; STABILITY; MODEL; TRANSITIONS; TENSION;
D O I
10.1016/j.jmps.2013.07.013
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Martensitic transformations (MTs) are the key phenomena responsible for the remarkable properties of Shape Memory Alloys (SMAs). Recent Density Functional Theory (DFT) electronic structure calculations have revealed that the austenite structure of many SMAs is a saddle-point of the material's potential energy landscape. Correspondingly, the austenite is unstable and thus unobservable at zero temperature. Thus, the observable high temperature austenite structure in many SMAs is entropically stabilized by nonlinear dynamic effects. This paper discusses the phenomenon of entropic stabilization of the austenite phase in SMAs and explicitly demonstrates it using Molecular Dynamics (MD) and a three-dimensional all-atom potential energy model whose equilibria crystal structures correspond to commonly observed SMA phases. A new technique is used to carefully select a model so that it is likely to lead to entropic stabilization of a B2 cubic austenite from a B19 orthorhombic martensite. This is accomplished by using a detailed branch-following and bifurcation (BFB) parametric study of the Morse pair potential binary alloy model. The results of the MD simulation clearly demonstrate the entropic stabilization of the B2 austenite phase at high temperature. Analysis of the dynamics of the B2 austenite phase indicates that its stabilization may be viewed as a result of individual atoms randomly visiting the B19 and alpha IrV phases (with only occasional visits to the B2 and L1(0) phases). This occurs without long-range correlations in such a way that each atom's time-average configuration corresponds to the B2 structure. (C) 2013 Elsevier Ltd. All rights reserved.
引用
收藏
页码:2522 / 2536
页数:15
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