Theocharis Baxevanis
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Theocharis Baxevanis has a total of 73 co-authors. Here are the top co-authors by number of shared publications:
- Dimitris C. Lagoudas
Texas A&M University
17 shared publications Dimitris C. Lagoudas
5 shared publications- Ibrahim Karaman
Department of Materials Science and Engineering, Texas A&M University, College Station, TX 77843, USA
5 shared publications - Sameer Jape
Texas A&M Univ. (United States)
4 shared publications - Theodoros Katsaounis
University of Crete
4 shared publications Austin Cox
Texas A&M University
3 shared publications
Latest Publications
- 3 November 2026
- Published by Elsevier in Engineering Fracture Mechanics
- Vol. 348
Are phase-field fracture models nonlocal damage models? A constructive answer for the at2 model
- 3 November 2026
- Published by Elsevier in Engineering Fracture Mechanics
- Vol. 348
Are phase-field fracture models nonlocal damage models? A constructive answer for the at2 model
- Open Access
- 8 September 2026
- Published by Elsevier in SSRN Electronic Journal
Is the phase-field fracture model indeed a nonlocal damage model?
The question of the title is answered constructively: the \at{2} phase-field model of brittle fracture is assembled from the standard ingredients of nonlocal damage mechanics. The local damage model combines the quadratic degradation function $(1-D)^2$ of damage $D$ with a damage surface $f=\Y-\kappa\le0$ driven by the damage energy release rate $\Y=2(1-D)\,\psi_0^+$, and a linear damage--threshold relation $\kappa=kD$ with vanishing initial threshold. Damage growth is made irreversible by evaluating the driving energy at the largest value it has attained, \emph{i.e.}, by the strain-energy history field $\mathcal H$, which integrates the loading/unloading conditions in closed form. The model is regularized by the weighted spatial average $\bar\kappa$ of the damage threshold $\kappa$. Since the damage--threshold relation is linear, the damage average inherits the weight of the history average, which is built from the Green's function of the damage-screened operator $-l^2\Delta+1/(1-D)$, where $l$ is the length parameter and $\Delta$ the Laplacian operator. The weight's interaction range, $\ell=l\sqrt{1-D}$, contracts with damage, so that a fully developed crack severs nonlocal interaction. Calibrating the model's two constants, $k$ and $l$, against the toughness $G_c$ and the tensile strength $\sigma_c$ results in a total potential that coincides with the Ambrosio--Tortorelli functional and delivers the governing equations of the history-field \at{2} model.- 8 September 2026
- Published by Elsevier in SSRN Electronic Journal
Open AccessIs the phase-field fracture model indeed a nonlocal damage model?
The question of the title is answered constructively: the \at{2} phase-field model of brittle fracture is assembled from the standard ingredients of nonlocal damage mechanics. The local damage model combines the quadratic degradation function $(1-D)^2$ of damage $D$ with a damage surface $f=\Y-\kappa\le0$ driven by the damage energy release rate $\Y=2(1-D)\,\psi_0^+$, and a linear damage--threshold relation $\kappa=kD$ with vanishing initial threshold. Damage growth is made irreversible by evaluating the driving energy at the largest value it has attained, \emph{i.e.}, by the strain-energy history field $\mathcal H$, which integrates the loading/unloading conditions in closed form. The model is regularized by the weighted spatial average $\bar\kappa$ of the damage threshold $\kappa$. Since the damage--threshold relation is linear, the damage average inherits the weight of the history average, which is built from the Green's function of the damage-screened operator $-l^2\Delta+1/(1-D)$, where $l$ is the length parameter and $\Delta$ the Laplacian operator. The weight's interaction range, $\ell=l\sqrt{1-D}$, contracts with damage, so that a fully developed crack severs nonlocal interaction. Calibrating the model's two constants, $k$ and $l$, against the toughness $G_c$ and the tensile strength $\sigma_c$ results in a total potential that coincides with the Ambrosio--Tortorelli functional and delivers the governing equations of the history-field \at{2} model. - Open Access
- 1 March 2026
- Published by The Royal Society in Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences
- Vol. 482 (2333)
A continuum macro-model for bistable periodic auxetic surfaces
A macro-constitutive model for the deformation response of periodic rotating bistable auxetic surfaces is developed. Focus is placed on isotropic surfaces made of bistable hexagonal cells composed of six triangular units with two stable equilibrium states. Adopting a variational formulation, the effective stress–strain response is derived from a free-energy function expressed in terms of the invariants of the logarithmic strain. To address the mathematical ill-posedness and numerical artefacts—such as mesh sensitivity—arising from the double-well nature of the free energy, two regularization approaches are introduced: (i) a gradient-enhanced first invariant of the logarithmic strain and (ii) an artificial material rate dependency. Although neither regularization guarantees solution uniqueness, the former mitigates mesh sensitivity, while the latter improves the convergence behaviour of the nonlinear numerical scheme by promoting smooth temporal evolution of transition localization and enabling the system to overcome snap-backs induced by local non-proportional loading near transition fronts. The model is implemented using membrane/shell structural elements and plane stress continuum ones within the ABAQUS finite-element suite. Numerical simulations demonstrate the efficacy of the proposed formulation and its implementation.
- 1 March 2026
- Published by The Royal Society in Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences
- Vol. 482 (2333)
Open AccessA continuum macro-model for bistable periodic auxetic surfaces
A macro-constitutive model for the deformation response of periodic rotating bistable auxetic surfaces is developed. Focus is placed on isotropic surfaces made of bistable hexagonal cells composed of six triangular units with two stable equilibrium states. Adopting a variational formulation, the effective stress–strain response is derived from a free-energy function expressed in terms of the invariants of the logarithmic strain. To address the mathematical ill-posedness and numerical artefacts—such as mesh sensitivity—arising from the double-well nature of the free energy, two regularization approaches are introduced: (i) a gradient-enhanced first invariant of the logarithmic strain and (ii) an artificial material rate dependency. Although neither regularization guarantees solution uniqueness, the former mitigates mesh sensitivity, while the latter improves the convergence behaviour of the nonlinear numerical scheme by promoting smooth temporal evolution of transition localization and enabling the system to overcome snap-backs induced by local non-proportional loading near transition fronts. The model is implemented using membrane/shell structural elements and plane stress continuum ones within the ABAQUS finite-element suite. Numerical simulations demonstrate the efficacy of the proposed formulation and its implementation.
- Open Access
- 8 December 2025
- Published by Elsevier in Engineering Fracture Mechanics
- Vol. 332
A phase-field regularization of porous–ductile fracture
- 8 December 2025
- Published by Elsevier in Engineering Fracture Mechanics
- Vol. 332
Open AccessA phase-field regularization of porous–ductile fracture
- 12 December 2024
- Published by Wiley in Journal of Applied Mechanics
- Vol. 92 (2) , 1-23
Extraction of Mechanical Properties of Shape Memory Alloys From Instrumented Spherical Indentation
An approach to infer mechanical properties of shape memory alloys (SMAs) from instrumented spherical indentation records of indenter tip loading force, P, versus the resultant indentation depth, h, during indentation loading and unloading is proposed. The approach is based on (i) a finite element (FE) model for describing the forward problem of determining the indentation response, i.e., the P−h curve, for a given set of SMA mechanical properties, (ii) a computationally efficient Gaussian process surrogate model to replace the costly FE one, and (iii) an iterative solution strategy, which approximates the unknown model parameters from an experimentally determined P−h record and their corresponding probability densities via a Bayesian inference framework and a Markov Chain Monte Carlo sampling strategy. The efficacy of the proposed approach is demonstrated using numerical experiments, i.e., indentation curves generated by evaluating the FE model at points in the parameter space.
- 12 December 2024
- Published by Wiley in Journal of Applied Mechanics
- Vol. 92 (2) , 1-23
Extraction of Mechanical Properties of Shape Memory Alloys From Instrumented Spherical Indentation
An approach to infer mechanical properties of shape memory alloys (SMAs) from instrumented spherical indentation records of indenter tip loading force, P, versus the resultant indentation depth, h, during indentation loading and unloading is proposed. The approach is based on (i) a finite element (FE) model for describing the forward problem of determining the indentation response, i.e., the P−h curve, for a given set of SMA mechanical properties, (ii) a computationally efficient Gaussian process surrogate model to replace the costly FE one, and (iii) an iterative solution strategy, which approximates the unknown model parameters from an experimentally determined P−h record and their corresponding probability densities via a Bayesian inference framework and a Markov Chain Monte Carlo sampling strategy. The efficacy of the proposed approach is demonstrated using numerical experiments, i.e., indentation curves generated by evaluating the FE model at points in the parameter space.
- 8 December 2023
- Published by Elsevier in Computer Methods in Applied Mechanics and Engineering
- Vol. 419
Phase-field description of fracture in NiTi single crystals
- 8 December 2023
- Published by Elsevier in Computer Methods in Applied Mechanics and Engineering
- Vol. 419
Phase-field description of fracture in NiTi single crystals
- 1 November 2022
- Published by Springer Nature in Shape Memory and Superelasticity
- Vol. 8 (4) , 356-372
A Finite-Strain Phase-Field Description of Thermomechanically Induced Fracture in Shape Memory Alloys
- 1 November 2022
- Published by Springer Nature in Shape Memory and Superelasticity
- Vol. 8 (4) , 356-372
A Finite-Strain Phase-Field Description of Thermomechanically Induced Fracture in Shape Memory Alloys
- Open Access
- 16 May 2022
- Published by ASM International
- Vol. 84291, 71-72
A Phenomenological Model for the Anisotropic (Positive/Zero/Negative) Thermal Expansion in Shape Memory Alloys and its dependence on Phase Transformation and (Re)orientation of Martensite Variants
Thermal expansion (TE) is inherent material property and a critical design parameter in applications in which dimensional stability and/or thermal fatigue resistance over a wide range of temperatures are required. Examples include high precision instruments, satellite antennas, and optical instruments. Metallic materials that undergo martensitic transformation have been recently shown to exhibit tailorable bulk TE due to the TE anisotropy of the low-crystallographic-symmetry martensite lattice. In these materials, the TE anisotropy of bulk polycrystals can be exploited through martensite variant "orientation" upon deformation processing. This work proposes a constitutive model for tailoring the anisotropic CTE in shape memory alloys (SMAs) during martensite variant texturing, which is validated against experimental data from NiTiPd. A description of the evolution of the anisotropic macroscopic thermal expansion (TE) tensor of bulk shape memory alloys (SMAs) during phase transformation and martensite (re)orientation is proposed. Given that the tailorability of the TE of SMAs originates from the crystallographic TE anisotropy of the low-crystallographic-symmetry martensite, the TE tensor is approximated by a function of the oriented martensite volume fraction and the orientation direction unitary tensor. The proposed model is validated against recent experiments on tailoring TE through martensite orientation in a NiTiPd high temperature SMA. In those experiments, the TE tensor component in the loading direction of NiTiPd in the martensite state was shown to decrease with increasing inelastic strain induced by uniaxial tensile loading. According to the model, the TE tensor components in the transverse to the loading directions decrease with increasing tensile inelastic strain.
- 16 May 2022
- Published by ASM International
- Vol. 84291, 71-72
Open AccessA Phenomenological Model for the Anisotropic (Positive/Zero/Negative) Thermal Expansion in Shape Memory Alloys and its dependence on Phase Transformation and (Re)orientation of Martensite Variants
Thermal expansion (TE) is inherent material property and a critical design parameter in applications in which dimensional stability and/or thermal fatigue resistance over a wide range of temperatures are required. Examples include high precision instruments, satellite antennas, and optical instruments. Metallic materials that undergo martensitic transformation have been recently shown to exhibit tailorable bulk TE due to the TE anisotropy of the low-crystallographic-symmetry martensite lattice. In these materials, the TE anisotropy of bulk polycrystals can be exploited through martensite variant "orientation" upon deformation processing. This work proposes a constitutive model for tailoring the anisotropic CTE in shape memory alloys (SMAs) during martensite variant texturing, which is validated against experimental data from NiTiPd. A description of the evolution of the anisotropic macroscopic thermal expansion (TE) tensor of bulk shape memory alloys (SMAs) during phase transformation and martensite (re)orientation is proposed. Given that the tailorability of the TE of SMAs originates from the crystallographic TE anisotropy of the low-crystallographic-symmetry martensite, the TE tensor is approximated by a function of the oriented martensite volume fraction and the orientation direction unitary tensor. The proposed model is validated against recent experiments on tailoring TE through martensite orientation in a NiTiPd high temperature SMA. In those experiments, the TE tensor component in the loading direction of NiTiPd in the martensite state was shown to decrease with increasing inelastic strain induced by uniaxial tensile loading. According to the model, the TE tensor components in the transverse to the loading directions decrease with increasing tensile inelastic strain.
- 1 December 2021
- Published by Elsevier in Engineering Fracture Mechanics
- Vol. 258
Fracture resistance of shape memory alloys under thermomechanical loading
- 1 December 2021
- Published by Elsevier in Engineering Fracture Mechanics
- Vol. 258
Fracture resistance of shape memory alloys under thermomechanical loading