A one-dimensional model for a shape memory alloy is proposed. It provides a simplied description of the pseudo-elastic regime, where stressinduced transitions from austenitic to oriented martensitic phases occurs. The stress-strain evolution is ruled by a bilinear rate-independent o.d.e. which also accounts for the ne structure of minor hysteresis loops and applies to the case of single crystals only. The temperature enters the model as a parameter through the yield limit y. Above the critical temperature A , the austenitemartensite phase transformations are described by a Ginzburg-Landau theory involving an order parameter ', which is related to the anelastic deformation. As usual, the basic ingredient is the Gibbs free energy, which is a function of the order parameter, the stress and the temperature. Unlike other approaches, the expression of this thermodynamic potential is derived rather then assumed, here. The explicit expressions of the minimum and maximum free energies are obtained by exploiting the Clausius-Duhem inequality, which ensures the compatibility with thermodynamics, and the complete controllability of the system. This allows us to highlight the role of the Ginzburg-Landau equation when phase transitions in materials with hysteresis are involved.

Free energies and pseudo-elastic transitions for shape memory alloys

BERTI, ALESSIA;
2013-01-01

Abstract

A one-dimensional model for a shape memory alloy is proposed. It provides a simplied description of the pseudo-elastic regime, where stressinduced transitions from austenitic to oriented martensitic phases occurs. The stress-strain evolution is ruled by a bilinear rate-independent o.d.e. which also accounts for the ne structure of minor hysteresis loops and applies to the case of single crystals only. The temperature enters the model as a parameter through the yield limit y. Above the critical temperature A , the austenitemartensite phase transformations are described by a Ginzburg-Landau theory involving an order parameter ', which is related to the anelastic deformation. As usual, the basic ingredient is the Gibbs free energy, which is a function of the order parameter, the stress and the temperature. Unlike other approaches, the expression of this thermodynamic potential is derived rather then assumed, here. The explicit expressions of the minimum and maximum free energies are obtained by exploiting the Clausius-Duhem inequality, which ensures the compatibility with thermodynamics, and the complete controllability of the system. This allows us to highlight the role of the Ginzburg-Landau equation when phase transitions in materials with hysteresis are involved.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11389/11780
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