Abstract

The complex and intricate microstructure of B19’ martensite in shape memory nickel titanium alloys is generally explained with the Phenomenological Theory of Martensitic Crystallography (PTMC). For the last decade, we have developed an alternative approach that supposes the existence of a “natural” parent-daughter orientation relationship (OR). As the previous TEM studies could not capture the global crystallographic characteristics of the B2-B19’ transformation required to discriminate the models, we used Electron BackScatter Diffraction (EBSD) and Transmission Kikuchi Diffraction (TKD) to investigate a polycrystalline NiTi alloy constituted of B19’ martensite. The EBSD maps show the large martensite plates and reveal a coexistence of different ORs. The TKD maps permit to image the “twins” and confirm a continuum of orientations. The results are interpreted without PTMC, with anew hypotheses. The predominant OR in EBSD is the “natural” OR for which the dense directions and dense planes of B2 and B19’ phases are parallel, i.e. (010)B19’ // (110)B2 & [101]B19’ // [ -111]B2 . The natural OR was used to automatically reconstruct the prior parent B2 grains in the EBSD and TKD maps. From the distortion matrix associated to this OR, we calculated that the habit plane could be (1-12)B2 // (10-1 )B19’. The traces of these planes are in good agreement with the EBSD maps. We interpret the other ORs as “closing-gap” ORs derived from the natural OR to allow the compatibility between the distortion variants. Each of them restores a parent symmetry element between the variants that was lost by distortion but preserved by correspondence. The oral presentation is divided in three parts: 0-26 min : Introduction, some words about the limits of the PTMC, 26-50 min : Experimental EBSD and TKD Results, 50-80 min : Interpretations and conclusions. All the details can be found in https://doi.org/10.3390/cryst10070562.

Highlights

  • The B2-B19’ orientation relationships and their continuums revealed by EBSD and TKD observations of NiTi alloys

  • I was teaching as most of us teach this, by showing schematic pictures as the one on the right hand side: as I have a long experience of EBSD, I decided to look inside literature to find experimental EBSD maps showing the B2 austenite B19’ martensite transformation during tensile tests of superelastic NiTi, or the B19’ variant re-orientation effect during deformation of a martensitic NiTi alloy

  • I have started to doubt about Phenomenolgical Theory of Martensite Crystallography (PTMC) and this paradigm nearly 10 years ago when I started to study fcc-bcc martensitic transformation in steels

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Summary

Cyril Cayron

Motivations of the study: 1. Three years ago, I started to teach “phase transformations” to Bachelor students. I included a part about shape memory alloys, and one of their most classical representative alloy: Ni-Ti. I was teaching as most of us teach this, by showing schematic pictures as the one on the right hand side: as I have a long experience of EBSD, I decided to look inside literature to find experimental EBSD maps showing the B2 austenite B19’ martensite transformation during tensile tests of superelastic NiTi, or the B19’ variant re-orientation effect during deformation of a martensitic NiTi alloy. I found numerous TEM and HRTEM studies, but to my big surprize I could not find any EBSD map of B19’ martensite! 2. The classical theory used to explain/describe the complex microstructure of B19’. Martensite is the Phenomenolgical Theory of Martensite Crystallography (PTMC) born in the 1950s. I have started to doubt about PTMC and this paradigm nearly 10 years ago when I started to study fcc-bcc martensitic transformation in steels. Let me make a very brief summary of what is PTMC

From HKDH Bhadeshia
Square phase core
Methodology for the EBSD and TKD on NiTi alloys
Simulated disorientation histogram with ORs
List of expected habit planes
Conclusion
Full Text
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