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Deformation in NiAl bicrystals
Affiliation:1. Cracow University of Technology, Jana Pawła II 37 Street, Cracow, Poland;2. ABB Corporate Research, Starowislna 13A Street, Cracow, Poland;3. Warsaw University of Technology, Woloska 141 Street, Warsaw, Poland;1. Herbert Gleiter Institute of Nanoscience, School of Materials Science and Engineering, Nanjing University of Science and Technology, Nanjing 210094, China;2. Institute for Advanced Studies in Precision Materials, Yantai University, Yantai 264005, China;3. Metalink International Co., Ltd., Nanjing 211153, China;4. Nano and Heterogeneous Materials Center, School of Materials Science and Engineering, Nanjing University of Science and Technology, Nanjing 210094, China;1. School of Materials Science & Engineering, South China University of Technology, Guangzhou 510640, China;2. EMAT, Department of Physics, University of Antwerp, B-2020 Antwerp, Belgium;3. School of Materials Science and Energy Engineering, Foshan University, Foshan 528000, China;1. College of Nursing, Eulji University, Daejeon, Korea;2. Department of Surgery, Eulji University Hospital, Daejeon, Korea
Abstract:The effects of a concentrated local stress arising from elastic and plastic incompatibility at internal NiAl grain boundaries have been investigated in oriented NiAl bicrystals. Observations of surface slip markings and TEM characterization of the dislocations responsible for bicrystal deformation have been made. The glide of a〈110〉 dislocations on {110} planes is the primary mode of deformation in the vicinity of the oriented bicrystal interfaces investigated. The dominant mode of a〈110〉 dislocation generation is the nucleation of loops away from the bicrystal interface. The macroscopic stress required to activate these dislocations, in the presence of a stress concentration such as that produced by a dislocation pile-up at a grain boundary, is the same as that required to nucleate a〈100〉 dislocations in “soft” single crystals of NiAl. Although the statistical relevance of this phenomenon as it pertains to the deformation of NiAl polycrystals has not been established, it is speculated that the glide of non-a〈100〉 dislocations may play an important role in the ductility of polycrystalline NiAl at the ductile-to-brittle transition temperature. The movement of a〈100〉 dislocations provides the primary mode of deformation for several bicrystals investigated far (> 3 mm) from the bicrystal interface. It is suggested that the vacancies required for the extensive climb of a[100] vacancy loops is supplied by the climb of a[100] and a[010] dislocations, and that the gradient in the concentration of vacancies provides the driving force for the motion of the a[100] and a[010] dislocations.
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