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Brinson model is one of the most-widely used models for shape memory alloy (SMA) wires.
The B-Spline surfaces are imported into a CAD system to construct parametric solid models for shape optimization.
This study employs two continuum models for shape memory alloys to simulate the phase transformation and the stress distribution around a hard defect in a shape memory matrix.
This paper reports a bibliographic review on the characteristics and uniaxial macroscale constitutive models for shape memory alloys, of interest for a significant number of applications, most often based on wires and bars.
Additionally, models for shape representation often need to provide local shape control and they need to be able to reproduce common shape primitives such as ellipsoids, spheres, cylinders, or tori.
Existing constitutive models for Shape Memory Alloys (SMAs) assume that both forward and reverse transformations occur when the thermodynamic driving force reaches a specific amount regardless of loading history.
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MSE is creating computer models for shaping the magnetic fields that form the engine's nozzle.
In this paper a material model for shape memory alloys from Seelecke (1999) is investigated.
In this paper we suggest a new phenomenological material model for shape memory alloys.
The most widely cited classical model for shape control of crystals is given by Gibbs Curie Willff theorem.
In this work we investigate passivity of the Müller-Achenbach-Seelecke Model for shape memory alloy (SMA) wires.
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