2016
DOI: 10.1016/j.ijplas.2016.04.008
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A three-dimensional finite-strain phenomenological model for shape-memory polymers: Formulation, numerical simulations, and comparison with experimental data

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Cited by 58 publications
(49 citation statements)
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“…Particularly, Young's moduli for the glassy and rubbery phases, respectively, E g and E r , were defined from the data presented in Figure 3a, and 3b, respectively; Poisson's coefficients for the glassy and rubbery phases, respectively, ν g and ν r , were taken from ref. [34]; transformation temperature, θ t , was calibrated from values shown in Figure 1b; the parameter defining half-width of the temperature range, ∆θ, and the transformation coefficient, w, were chosen taking into account that both inks are in a fully amorphous phase at 60 • C; the plastic hardening coefficient, h, and the stress limit, R p g , for plastic yielding of the glassy phase were calibrated from the stress-strain relationships below the transition temperature (see Figures S1 and S5) and above the transition temperature ( Figures S7 and S11). No imperfect material behavior was assumed.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Particularly, Young's moduli for the glassy and rubbery phases, respectively, E g and E r , were defined from the data presented in Figure 3a, and 3b, respectively; Poisson's coefficients for the glassy and rubbery phases, respectively, ν g and ν r , were taken from ref. [34]; transformation temperature, θ t , was calibrated from values shown in Figure 1b; the parameter defining half-width of the temperature range, ∆θ, and the transformation coefficient, w, were chosen taking into account that both inks are in a fully amorphous phase at 60 • C; the plastic hardening coefficient, h, and the stress limit, R p g , for plastic yielding of the glassy phase were calibrated from the stress-strain relationships below the transition temperature (see Figures S1 and S5) and above the transition temperature ( Figures S7 and S11). No imperfect material behavior was assumed.…”
Section: Resultsmentioning
confidence: 99%
“…The geometry was meshed by using eight-node linear isoparametric hexahedral elements with full integration. The thermo-mechanical response of the pure and mixed inks was captured by using the three-dimensional finite-strain constitutive model for SMPs, as proposed in [34]. Specifically, the model is based on a phase transition approach and formulated within a thermodynamically consistent mathematical framework.…”
Section: Smp Behavior Characterizationmentioning
confidence: 99%
“…In the last example of this paper, we demonstrate the robustness of the proposed SPH algorithm on a complex geometry displayed in Figure 28. As reported in Reference [61], the geometry used in this example is a simplified version of a cardiovascular stent used in biomedical applications. The structure has an initial outer diameter of 20 mm, a thickness of 0.5 mm and a total length of 20 mm.…”
Section: Complex Geometrymentioning
confidence: 99%
“…Based on the abovementioned meso-mechanical method with a mixture rule, a threedimensional model was proposed for TSMPs [48], which distinguishes between two phases presenting different properties. The model can reproduce both heating-stretching-cooling and cold drawing shape-fixing procedures and was applied in the simulations from simple uniaxial and biaxial tests to complex loadings of biomedical devices.…”
Section: Meso-mechanical Modelmentioning
confidence: 99%