Suppressed martensitic transformation under biaxial loading in low stacking fault energy metastable austenitic steels

Phase maps showing the γ-austenite grains which belong to the “high Schmid factor” orientation regime for the LPDs (with blue) and the “high Schmid factor” orientation regime for the TPDs (with red), ε-martensite and α′-martensite for: (a) uniaxial, (b) equibiaxial both at ~ 13% equivalent strain. (c) Magnification of the highlighted area in (a) showing significant amount of α′-martensite within the bands of ε-martensite. (d) Magnification of the highlighted area in (b) showing that α′-martensite forms at the intersection of ε-martensite. Yellow: α’-martensite, green: ε-martensite.

The effect of uniaxial/biaxial loading on the martensitic transformation of low stacking fault energy, metastable austenitic stainless steel was studied by in-situ neutron diffraction on cruciform-shaped/dogbone samples. Uniaxial loading favors the martensitic transformation following the sequence γ → ε → α′ (i.e. fcc→hcp→bcc/bct crystal structure), where at low strains ε-martensite is the precursor of α′. During equibiaxial-loading, the formation of ε-martensite is suppressed and considerably less α′-martensite is observed at high strains.

Post mortem EBSD investigation reveal that the different deformation textures formed during uniaxial and equibiaxial loading play a significant role on the appearance/absence of ε-martensite which is a precursor for the martensitic transformation. The uniaxial-deformation texture facilitates the formation stacking faults as the majority of the grains have orientations (with respect to the loading direction) that the leading partial dislocations (LPDs) have higher Schmid factor than the trailing partial dislocations (TPDs), see Fig. 1. The appearance of stacking faults facilitates the local appearance of ε-martensite with an hcp crystal structure. In the opposite case, upon biaxial loading, the majority of the grains have orientations (with respect to the loading direction) that the LPDs have lower Schmid factor than the TPDs (see Fig. 1); this results in suppression of the formation of ε-martensite. In both loading states, the grains that contain martensite belong to orientations for which the LPDs have higher Schmid factor than the TPDs (see Figure).

Contact
Efthymios Polatidis
Photons for Engineering and Manufacturing Group
Paul Scherrer Institut, Villigen, Switzerland
Telephone: +41 56 310 3948
E-mail: efthymios.polatidis@psi.ch


Prof. Dr. Helena van Swygenhoven
Photons for Engineering and Manufacturing Group
Paul Scherrer Institut, Villigen, Switzerland and
Neutrons and X-rays for Mechanics of Materials
Ecole Polytechnique Fédéral de Lausanne, Lausanne, Switzerland
Telephone: +41 56 310 2931
E-mail: helena.vanswygenhoven@psi.ch
Original Publication
Suppressed martensitic transformation under biaxial loading in low stacking fault energy metastable austenitic steels
E. Polatidis, W.-N. Hsu, M. Šmíd, T. Panzner, S. Chakrabarty, P. Pant, H. Van Swygenhoven
Scripta Materialia 147 (2018) 27
DOI: 10.1016/j.scriptamat.2017.12.026