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Polycrystalline modeling of the cyclic hardening/softening behavior of an austenitic-ferritic stainless steel

Authors :
Véronique Aubin
Suzanne Degallaix
Pierre Evrard
I. Alvarez-Armas
Laboratoire de Mécanique de Lille - FRE 3723 (LML)
Université de Lille, Sciences et Technologies-Centrale Lille-Centre National de la Recherche Scientifique (CNRS)
Instituto de Física de Rosario [Santa Fe] (IFIR)
Consejo Nacional de Investigaciones Científicas y Técnicas [Buenos Aires] (CONICET)-Facultad de Ciencias Exactas, Ingenieria y Agrimensura [Rosario] (FCEIA)
Universidad Nacional de Rosario [Santa Fe]-Universidad Nacional de Rosario [Santa Fe]
Laboratoire de mécanique des sols, structures et matériaux (MSSMat)
CentraleSupélec-Centre National de la Recherche Scientifique (CNRS)
Université de Lille, Sciences et Technologies-Ecole Centrale de Lille-Université de Lille-Centre National de la Recherche Scientifique (CNRS)
Source :
Mechanics of Materials, Mechanics of Materials, Elsevier, 2010, 42 (4), pp.395-404. ⟨10.1016/j.mechmat.2010.01.007⟩
Publication Year :
2010
Publisher :
HAL CCSD, 2010.

Abstract

International audience; As other metallic materials, in low-cycle fatigue, duplex stainless steels (DSS) exhibit a cyclic hardening, followed by a cyclic softening, before stabilization of the stress. In order to simulate the cyclic hardening/softening curves in low-cycle fatigue of an austenitic–ferritic or duplex stainless steel (DSS), a new polycrystalline model is proposed. The polycrystalline model developed by (Cailletaud, 1992) and (Pilvin, 1990) and modified by Hoc and Forest (2001) was previously extended in Evrard et al. (2008) in order to take into account the bi-phased character of the DSS. This model correctly accounts for the cyclic hardening, but it is not able to simulate the cyclic softening, consequently, stresses at the stabilized state are overestimated. TEM observations of the dislocation structures built during a cyclic uniaxial tension/compression test show that, during the cyclic hardening, planar arrangements are observed in austenitic grains and no significant evolution is observed during the subsequent cyclic softening and stabilization stage. On the contrary, in ferritic grains, dislocations are homogeneously distributed during cyclic hardening, and the microstructure evolves during the subsequent cyclic softening and stabilization stage. Dislocation structures build progressively, consisting of hard zones or walls, separated by soft zones or channels. We propose to model the cyclic softening through dislocation structure evolution within ferritic grains. The single crystal law used by Hoc and Forest (2001) is modified in order to take into account the heterogeneous distribution of dislocations in the ferrite. Numerical simulations are compared with experimental data. A good agreement is observed between experimental and calculated hardening/softening curves and stabilized hysteresis loops.

Details

Language :
English
ISSN :
01676636
Database :
OpenAIRE
Journal :
Mechanics of Materials, Mechanics of Materials, Elsevier, 2010, 42 (4), pp.395-404. ⟨10.1016/j.mechmat.2010.01.007⟩
Accession number :
edsair.doi.dedup.....69c1a9e2c4797a45af15f5f0612d36df
Full Text :
https://doi.org/10.1016/j.mechmat.2010.01.007⟩