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Communication Dans Un Congrès Année : 2018

Mean field and full field simulations of dynamic recrystallization of austenitic 304L steel

Résumé

During hot deformation of austenitic 304L steel several physical mechanisms take place at different scales which may lead to the fullregeneration of the microstructure. The level of plastic deformation, recovery and recrystallization actually defines the finalmicrostructure. Therefore, in order to control the different microstructure features (e.g. grain size, recrystallized fraction anddislocation density), it is of prime importance to be able to simulate those mechanisms and to link them to the thermomechanicalconditions. In the present work, we propose a full field model with explicit description of the microstructure and a mean field modelwith implicit description of the microstructure. In both models, plasticity, recovery and nucleation are modeled withphenomenological laws. As for grain boundary migration, it is driven by stored energy gradients and capillarity effects. Hence, themigration velocity of each grain boundary is affected by the neighboring grains. Since microstructure is explicitly described in fullfield simulations, the neighborhood can be directly determined and grain boundary curvature can be locally calculated. However, inmean field simulations, the microstructure is statistically described. The novelty of the present model is that neighborhood of a givengrain is implicitly described through statistical topological laws. The comparison of the results of both models validates the proposedstatistical neighborhood description. Simulation results are also compared to experimental ones.

Domaines

Matériaux
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Dates et versions

hal-01973194 , version 1 (08-01-2019)

Identifiants

  • HAL Id : hal-01973194 , version 1

Citer

Ludovic Maire, Julien Fausty, Nathalie Bozzolo, Marc Bernacki, Daniel Pino Muñoz, et al.. Mean field and full field simulations of dynamic recrystallization of austenitic 304L steel. Matériaux 2018, Nov 2018, Strasbourg, France. ⟨hal-01973194⟩
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