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Microstructure evolution and its influence on deformation mechanisms during high temperature creep of a nickel base superalloy
Authors:Javad Safari  Saeed Nategh
Affiliation:1. Materials Science and Engineering Department, Shahid Chamran University, Ahwaz, Iran;2. Materials Science and Engineering Department, Sharif University of Technology, P.O. Box 11365-9466, Tehran, Iran;1. Department of Mechanical Engineering, Whiting School of Engineering, The Johns Hopkins University, Baltimore, MD 21218-2682, USA;2. Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson AFB, OH 45433-7817, USA;3. Institute of Mechanical Engineering, EPFL, Lausanne, Switzerland;4. UES Inc., 4401 Dayton-Xenia Road, Dayton, OH 45432-1894, USA;1. Department of Materials Science and Engineering, Pusan National University, Busan 609-735, Republic of Korea;2. Neutron Science Division, HANARO Center, Korea Atomic Energy Research Institute, Daejeon 305-353, Republic of Korea;3. Advanced Metallic Materials Division, Korea Institute of Materials Science, Changwon 642-831, Republic of Korea;4. Research and Development Center, KOS Limited, Yangsan 626-230, Republic of Korea
Abstract:The interaction of dislocation with strengthening particles, including primary and secondary γ′, during different stages of creep of Rene-80 was investigated by scanning electron microscopy (SEM) and transmission electron microscopy (TEM). During creep of the alloy at 871 °C under stress of 290 MPa, the dislocation network was formed during the early stages of creep, and the dislocation glide and climb process were the predominant mechanism of deformation. The density of dislocation network became more populated during the later stages of the creep, and at the latest stage of the creep, primary particles shearing were observed alongside with the dislocation glide and climb. Shearing of γ′ particles in creep at 871 °C under stress of 475 MPa was commenced at the earlier creep times and governed the creep deformation mechanism. In two levels of examined stresses, as far as the creep deformation was controlled by glide and climb, creep curves were found to be at the second stage of creep and commence of the tertiary creep, with increasing creep rate, were found to be in coincidence with the particles shearing. Microstructure evolution, with regard to γ′ strengthening particles, led to particles growth and promoted activation of other deformation mechanisms such as dislocation bypassing by orowan loop formation. Dislocation-secondary γ′ particles interaction was detected to be the glide and climb at the early stages of creep, while at the later stages, the dislocation bypassed the secondary precipitation by means of orowan loops formation, as the secondary particle were grown and the mean inter-particle distance increased.
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