| People | Locations | Statistics |
|---|---|---|
| Naji, M. |
| |
| Motta, Antonella |
| |
| Aletan, Dirar |
| |
| Mohamed, Tarek |
| |
| Ertürk, Emre |
| |
| Taccardi, Nicola |
| |
| Kononenko, Denys |
| |
| Petrov, R. H. | Madrid |
|
| Alshaaer, Mazen | Brussels |
|
| Bih, L. |
| |
| Casati, R. |
| |
| Muller, Hermance |
| |
| Kočí, Jan | Prague |
|
| Šuljagić, Marija |
| |
| Kalteremidou, Kalliopi-Artemi | Brussels |
|
| Azam, Siraj |
| |
| Ospanova, Alyiya |
| |
| Blanpain, Bart |
| |
| Ali, M. A. |
| |
| Popa, V. |
| |
| Rančić, M. |
| |
| Ollier, Nadège |
| |
| Azevedo, Nuno Monteiro |
| |
| Landes, Michael |
| |
| Rignanese, Gian-Marco |
|
Merzouki, Tarek
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (21/21 displayed)
- 2024An efficient numerical model for free vibration of temperature-dependent porous FG nano-scale beams using a nonlocal strain gradient theory
- 2023Bending Responses of Bi-Directional Advanced Composite Nanobeams Using Higher Order Nonlocal Strain Gradient Theorycitations
- 2022Elastic stability of functionally graded graphene reinforced porous nanocomposite beams using two variables shear deformation
- 2022Bending analysis of functionally graded porous nanocomposite beams based on a non-local strain gradient theorycitations
- 2021A robust method for the reliability-based design optimization of shape memory alloy actuatorcitations
- 2020Surrogate models for uncertainty analysis of micro-actuatorcitations
- 2019An approach for the reliability-based design optimization of shape memory alloy structurecitations
- 2018Uncertainty analysis of an actuator for a shape memory alloy micro-pump with uncertain parameterscitations
- 2018Uncertainty analysis of an actuator for a shape memory alloy micro-pump with uncertain parameterscitations
- 2017Edge Effect on Nanoparticles of an Interconnect Alloy from the ABV Model
- 2013Contribution to the modeling of hydration and chemical shrinkage of slag-blended cement at early agecitations
- 2013Contribution to the modeling of hydration and chemical shrinkage of slag-blended cement at early agecitations
- 2012Finite Element analysis of a shape memory alloy actuator for a micropumpcitations
- 2012Finite Element analysis of a shape memory alloy actuator for a micropumpcitations
- 2010Coupling between measured kinematic fields and multicrystal SMA finite element calculationscitations
- 2010Coupling between measured kinematic fields and multicrystal SMA finite element calculationscitations
- 2009Coupling between experiment and numerical simulation of shape memory alloy multicrystalcitations
- 2009Coupling between experiment and numerical simulation of shape memory alloy multicrystalcitations
- 2009Dialogue entre expérience et simulation numérique pour un multicristal en alliage à mémoire de forme
- 2009Dialogue entre expérience et simulation numérique pour un multicristal en alliage à mémoire de forme
- 2008Experimental identification and micromechancial modeling of the behavior of a multicrystal out of shape memory alloy
Places of action
| Organizations | Location | People |
|---|
article
Dialogue entre expérience et simulation numérique pour un multicristal en alliage à mémoire de forme
Abstract
Dialog between the experiment and the numerical simulation for a shape memory alloy multicrystal. The aim of this study is to make dialog between the numerical simulation and the experiment in the case of the tensile test behavior for a CuAlBe shape memory alloy multicrystal. This dialog allows to compare qualitatively the distributions of martensitic transformation, observed through a long distance microscope, with obtained by Finite element simulation using a thermomechanical behavior law. The last is based on the description of martensitic transformation on a single crystal scale. It is implemented in the Abaqus(R) finite element code. The applied boundary conditions for modeling correspond to the measured ones at the edge of the area by a technique of digital image correlation. Geometrical and crystallographic properties of the various grains of the multicrystal are experimentally determined. The tensile test is carried out at room temperature where the alloy has a superelastic behavior. A good agreement between the experimental observation and numerical results is observed.