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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Geijselaers, Hubert
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (31/31 displayed)
- 2023Computing Sheet Rolling Instabilities with a Shell Finite Element Model
- 2022Discontinuous Galerkin FEM with Hot Element Addition for the Thermal Simulation of Additive Manufacturing
- 2021Efficient thermal simulation of large-scale metal additive manufacturing using hot element additioncitations
- 2021Efficient analysis of dense fiber reinforcement using a reduced embedded formulationcitations
- 2020Optimization of the Interacting StiffenedSkins and Ribs Made of Composite Materialscitations
- 2020A New in-Plane Bending Test to Determine Flow Curves for Materials with Low Uniform Elongationcitations
- 2019Experimental investigation of pinching phenomena in cold rolling of thin steel sheetscitations
- 20191D squeeze flow analysis of chopped long fibre thermoplastic composite
- 2018A level-set-based strategy for thickness optimization of blended composite structurescitations
- 2018Deformation mechanism in compression molding of discontinuous thermoplastic composites
- 2017Effect of flake distribution in mold on the flow during compression molding of unidirectional long fiber thermoplastic flakes
- 2016Interpolation of final geometry and result fields in process parameter spacecitations
- 2016The softened heat-affected zone in resistance spot welded tailor hardened boron steel: a material model for crash simulation
- 2016Plasticity and fracture modeling of the heat-affected zone in resistance spot welded tailor hardened boron steelcitations
- 2016Parameter Study for Friction Surface Cladding of AA1050 on AA2024-T351
- 2015Friction Surface Cladding of AA1050 on AA2024-T351; influence of clad layer thickness and tool rotation rate
- 2015Thermal and Flow Analysis of Friction Surface Cladding with Varying Clad Layer Thickness
- 2015Single scan vector prediction in selective laser meltingcitations
- 2015Cyclic shear behavior of austenitic stainless steel sheet
- 2015Large strain cyclic behavior of metastable austenic stainless steelcitations
- 2015Friction surface claddingcitations
- 2015Influence of ring growth rate on damage development in hot ring rollingcitations
- 2014Influence of feed rate on damage development in hot ring rollingcitations
- 2013Modeling of the Austenite-Martensite Transformation in Stainless and TRIP Steelscitations
- 2013Strain direction dependency of martensitic transformation in austenitic stainless steels: The effect of gamma-texturecitations
- 2013Cladding of Advanced Al Alloys Employing Friction Stir Weldingcitations
- 2013Multi-Stage FE Simulation of Hot Ring Rollingcitations
- 2012Free Surface Modeling of Contacting Solid Metal Flows Employing the ALE formulationcitations
- 2011Comparison of ALE finite element method and adaptive smoothed finite element method for the numerical simulation of friction stir welding
- 2007Numerical forming simulations and optimisation in advanced materials
- 2000Improvements in FE-analysis of real-life sheet metal forming
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document
Modeling of the Austenite-Martensite Transformation in Stainless and TRIP Steels
Abstract
The transformation of austenite to martensite is a dominant factor in the description of the constitutive behavior during forming of TRIP assisted steels. To predict this transformation different models are currently available. In this paper the transformation is regarded as a stress induced process based on the thermodynamic action of the local stresses during transformation. A threshold for the thermodynamic action, above which transformation will occur, can be easily measured in a properly instrumented tensile test. The martensitic transformation is a diffusionless lattice shear. It is characterized by a habit plane normal n and a shear vector m, which are both defined with respect to the austenite lattice coordinate system. Therefore the thermodynamic action in each material grain strongly depends on the orientation of the grain with respect to the applied stress.Uniaxial tensile tests on both a non-textured austenitic stainless steel and one with a strong crystallographic texture were performed in both the rolling and the transverse directions. Both materials show mechanically induced phase transformation from austenite to martensite. When a strong texture is present in the austenite, differences between transformations during deformation in different directions can be observed clearly. The stress induced transformation theory, in combination with the textures measured before and after deformation, is used to explain and model the difference in transformation behavior when straining in various directions. During deformation the texture changes. This can have consequences for modeling of the transformation during non-proportional deformation.