Rice Local Phase Angle Study for a Delamination Problem Between a Shape Memory Alloy and an Elastic Material

Abstract

The present study is an extension of a recent paper of Freed et al. (J Mech Phys Solids 56:3003-3020, 2008). The final aim is to describe the transformation toughening behavior of a static crack along an interface between a shape memory alloy (SMA) and a linear elastic isotropic material. With an SMA as an equivalent Huber-Von Mises stress model (hypothesis of symmetric behavior between tension and compression), Freed et al. determine the initiation (ending) phase transformation yield surfaces in terms of the local phase angle introduced by Rice et al. (Metal ceramic interfaces, Pergamon Press, New York, pp 269-294, 1990). In this paper we give the general framework to determine this angle for a model integrating the asymmetry between tension and compression (experimentally measured: Vacher and Lexcellent in Proc ICM 6:231-236, 1991; Orgéas and Favier in Acta Mater 46(15): [5579][5580][5581][5582][5583][5584][5585][5586][5587][5588][5589][5590][5591] 2000), the Huber-Von Mises model being only a particular case. We demonstrate the local phase angle existence in an appropriate framing domain and give a sufficient hypothesis for its uniqueness and an algorithm to obtain it. Estimates are obtained in terms of physical quantities such as the Young modulus ratio, the bimaterial Poisson modulus values and also the choice of the yield loading functions. Finally, we illustrate this theoretical study by an application linking the asymmetry intensity on the width and the shape on predicted phase transformation surfaces and by a comparison with the symmetric case.

Phase transformation surfaces around a crack tip for a shape memory alloys

“…This result is the direct consequence of the convexity condition of the G yield function (see Laydi and Lexcellent [13]) which imposes the necessary condition on the f function…”

Determination of phase transformation surfaces around crack tip in shape memory alloys

“…This result is the direct consequence of the G convexity (Laydi et Lexcellent [11]) which imposes to f the necessary following condition :…”