Abstract
Real-time in-situ neutron diffraction was conducted during uniaxial cycling compression of a Ni49.3Fe18Ga27Co5.7 shape memory alloy to explore the mechanism on its superelasticity at room temperature, which was manifested by the almost recoverable large strains and the apparent cyclic softening. Based on the Rietveld refinements, the real-time evolution of volume fraction of martensite was in-situ monitored, indicating the incremental amount of residual martensite with increasing load cycles. Real-time changes in intensities and lattice strains of {hkl} reflections for individual phase were obtained through fitting individual peaks, which reveal the quantitative information on phase transformation kinetics as a function of grain orientation and stress/strain partitioning. Moreover, a large compressive residual stress was evidenced in the parent phase, which should be balanced by the residual martensite after the second unloading cycle. The large compressive residual stress found in the parent austenite phase may account for the cyclic effect on critical stress required for triggering the martensitic transformation in the subsequent loading.
Original language | English |
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Pages (from-to) | 324-328 |
Number of pages | 5 |
Journal | Materials Science and Engineering: A |
Volume | 680 |
DOIs | |
State | Published - Jan 5 2017 |
Funding
This work was supported by National Science Foundation of China (NSFC) (Grant No.s 51471032 and 51527801), the National Basic Research Program of China (973 Program) under Contract No. 2012CB619405. H. Y. would like to thank the China Scholarship Council for the financial support during the visit to University of Tennessee, TN and SNS, ORNL. Neutron scattering experiment was carried out at Spallation Neutron Source (SNS) which is national user facilities sponsored by the Scientific User Facilities Division, Office of Basic Energy Sciences (BES), U.S. Department of Energy.
Keywords
- Ferromagnetic shape memory alloy
- Neutron diffraction
- Ni-Fe-Ga-Co
- Stress-induced martensitic transformation
- Superelasticity