Instabilities Induced by Phase Fronts Coalescence During the Phase Transitions in a Thin Sma Layer: Mechanism and Analytical Descriptions

TL;DR

This paper develops an analytical model to understand the instabilities during phase front coalescence in thin SMA layers, revealing the role of limited points and specimen geometry in stress jumps and drops.

Contribution

It introduces a quasi-2D analytical framework capturing the coalescence phenomena and the influence of thickness-length ratio on phase transition instabilities in SMA layers.

Findings

Instabilities are caused by limited points leading to mode switches.

Analytical solutions describe the entire coalescence process.

Thickness-length ratio critically affects stress jumps and drops.

Abstract

Systematic experiments on stress-induced phase transitions in thin SMA structures in literature have revealed two interesting instability phenomena: the coalescence of two martensite-austenite fronts leads to a sudden stress drop and that of two austenite-martensite fronts leads to a sudden stress jump. In order to get an insight into these two phenomena, in this work we carry out an analytical study on the stress-induced phase transitions in a thin SMA layer (a simple structure in which the two coalescence processes can happen). We derive a quasi-2D model with a non-convex effective strain energy function while taking into account the rate-independent dissipation effect. By using a coupled series-asymptotic expansion method, we manage to express the total energy dissipation in terms of the leading-order term of the axial strain. The equilibrium equations are obtained by maximizing the total energy dissipation, which are then solved analytically under suitable boundary conditions. The analytical results reveal that the mechanism for such instabilities is the presence of "limited points", which cause the switch of nontrivial solution modes to trivial solution modes. Descriptions for the whole coalescence processes of two fronts are also provided based on the analytical solutions, which also capture the morphology varies of the specimen. It is also revealed the key role played by the thickness-length ratio on these instabilities: the zero limit of which can lead to the smooth switch of nontrivial modes to trivial modes with no stress drop or stress jump.