Abstract
This paper introduces a novel three-dimensional constitutive model that describes the thermomechanical behavior of shape memory alloys (SMAs). The model is developed within the framework of continuum mechanics and the standard generalized materials. Four macrocospic phases are considered associated with austenite and three variants of martensite. Phase transformations can be induced by temperature, volumetric and deviatoric strains. The description of plasticity is also of concern assuming kinematic and isotropic hardening. Numerical simulations are carried out showing that the proposed model is able to capture the general thermomechanical behavior of SMAs for uniaxial and multiaxial tests, even in situations with complex thermomechanical loading paths.
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Abbreviations
- B + :
-
Thermodynamic force related to the volume fraction due to positive detwinned martensite
- B − :
-
Thermodynamic force related to the volume fraction due to negative detwinned martensite
- B A :
-
Thermodynamic force related to the volume fraction due to austenite
- \(E_{ijkl}\) :
-
Elastic tensor
- \(E_{ijkl}^{A} , E_{ijkl}^{M}\) :
-
Elastic tensor for autenitic and martensitic phases
- G :
-
Shear modulus
- H :
-
Kinematic hardening modulus
- \(H^{A} ,H^{M}\) :
-
Kinematic hardening modulus of austenite and martensite
- \(I_{\varTheta }\) :
-
Indicator function associated with the convex set Θ
- \(I_{\pi }\) :
-
Indicator function associated with the convex π
- \(I_{\chi }\) :
-
Indicator function of the convex set χ
- \(I_{f}\) :
-
Indicator function associated with yield surface (classical plasticity)
- K :
-
Isotropic plastic modulus
- \(L_{0}^{ + } ,L_{{}}^{ + }\) :
-
Parameters related to the critical stress due to positive detwinned martensite phase
- \(L_{0}^{ - } ,L_{{}}^{ - }\) :
-
Parameters related to the critical stress due to negative detwinned martensite phase
- \(L_{0}^{A} ,L_{{}}^{A}\) :
-
Parameters related to the critical stress due to the austenitic phase
- \(q_{j}\) :
-
Heat flux
- \(r_{ij}\) :
-
Second-order tensor defined from the loading history
- T :
-
Temperature
- T A :
-
Temperature above with the austenitic phase is stable
- T M :
-
Temperature below with the martensitic phase is stable
- T 0 :
-
Reference temperature in a stress-free state
- T F :
-
Reference temperature to determine the yield strength at high temperatures
- \(X_{ij}\) :
-
Thermodynamic force associated with the plastic strain tensor
- Y :
-
Thermodynamic force associated with the isotropic hardening
- \(Z_{ij}\) :
-
Thermodynamic force associated with the kinematic hardening tensor
- \(\alpha\) :
-
Parameter that controls the stress–strain hysteresis loop height
- \(\alpha_{ijkl}^{h}\) :
-
Fourth-order tensor that controls the stress–strain hysteresis loop width
- \(\alpha_{N}^{h} ,\alpha_{s}^{h}\) :
-
Normal and shear components of the tensor \(\alpha_{ijkl}^{h}\)
- \(\varLambda^{A} ,\varLambda^{M}\) :
-
Phase transformation temperature functions related to austenite and martensite
- \(\varLambda ,\varLambda^{\aleph }\) :
-
Phase transformation temperature functions
- \(\beta^{ + }\) :
-
Volume fraction related to the positive detwinned martensite
- \(\beta^{ - }\) :
-
Volume fraction related to the negative detwinned martensite
- \(\beta^{A}\) :
-
Volume fraction referring to austenite
- \(\beta^{M}\) :
-
Volume fraction related to the twinned martensite
- \(\beta_{s}^{ + } ,\beta_{s}^{ - }\) :
-
Volume fraction associated with the starting of phase transformation process
- \(\varepsilon_{ij}\) :
-
Total strain tensor
- \(\hat{\varepsilon }_{ij}\) :
-
Deviatoric strain tensor
- \(\varepsilon_{ij}^{e}\) :
-
Elastic strain tensor
- \(\varepsilon_{ij}^{p}\) :
-
Plastic strain tensor
- \(\varepsilon_{ij}^{t}\) :
-
Phase transformation strain tensor
- \(\vartheta\) :
-
Internal variable associated with isotropic hardening
- \(\varsigma_{ij}\) :
-
Internal variable associated with kinematic hardening
- \(\rho\) :
-
Density
- \(\sigma_{ij}\) :
-
Stress tensor
- \(\hat{\sigma }_{ij}\) :
-
Deviatoric stress tensor
- \(\sigma^{Y}\) :
-
Yield stress
- \(\sigma_{Y}^{A} ,\sigma_{Y}^{M}\) :
-
Yield stress of the austenitic and martensitic phases
- \(\sigma_{A,i}^{Y} ,\sigma_{A,f}^{Y}\) :
-
Yield stress at temperature T A and T F
- \(\gamma\) :
-
Plastic multiplier
- \(\eta^{ + } ,\eta^{ - } ,\eta^{A}\) :
-
Parameter associated with the internal dissipation (positive detwinned martensite, negative detwinned martensite and austenite)
- \(\eta^{I}\) :
-
Parameter that defines the coupling between the phase transformation and isotropic hardening
- \(\eta_{ij}^{k}\) :
-
Parameter that defines the coupling between the phase transformation and kinematic hardening
- \(\lambda ,\mu\) :
-
Lamé coefficients
- \(\lambda^{A} ,\lambda^{M}\) :
-
Lamé coefficients referring to austenite and martensite
- \(\mu^{A} ,\mu^{M}\) :
-
Lamé coefficients related to austenite and martensite
- \(\varPhi\) :
-
Pseudo-potential of dissipation
- \(\varPhi^{M}\) :
-
Mechanical part of the pseudo-potential of dissipation
- \(\varPhi^{H}\) :
-
Mechanical part of the pseudo-potential of dissipation
- \(\psi\) :
-
Helmholtz free energy density
- \(\psi^{ + } ,\psi^{ - } ,\psi^{A} ,\psi^{M}\) :
-
Helmholtz free energy density of isolated phases (positive detwinned martensite, negative detwinned martensite, austenite and twinned martensite)
- Γ :
-
Equivalent strain field
- υ :
-
Poisson’s ratio
- \(\upsilon^{A} ,\upsilon^{M}\) :
-
Poisson’s ratio associated with austenite and martensite
- \(\varOmega_{ij}\) :
-
Tensor related to the thermal expansion coefficients
- \(\varOmega_{ij}^{A} ,\varOmega_{ij}^{M}\) :
-
Tensor related to the thermal expansion coefficients of the austenite and martensite
- τ :
-
Set related to subdifferential associated with the convex set π (tetrahedron)
- \(\daleth\) :
-
Set related to subdifferential associated with the convex set χ
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Acknowledgments
The authors would like to acknowledge the support of the Brazilian Research Agencies CNPq, CAPES and FAPERJ and through the INCT-EIE (National Institute of Science and Technology—Smart Structures in Engineering) the CNPq and FAPEMIG. The Air Force Office of Scientific Research (AFOSR) is also acknowledged.
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Oliveira, S.A., Savi, M.A. & Zouain, N. A three-dimensional description of shape memory alloy thermomechanical behavior including plasticity. J Braz. Soc. Mech. Sci. Eng. 38, 1451–1472 (2016). https://doi.org/10.1007/s40430-015-0476-4
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DOI: https://doi.org/10.1007/s40430-015-0476-4