Room temperature nanoindentation creep behavior of detonation sprayed Fe-based amorphous coating

2022 ◽  
Vol 141 ◽  
pp. 107426
Author(s):  
Haimin Zhai ◽  
Xu Ma ◽  
Bo Cheng ◽  
Dongqing He ◽  
Xinjian Zhang ◽  
...  
2021 ◽  
Vol 283 ◽  
pp. 128768
Author(s):  
Anil Kumar ◽  
Sapan Kumar Nayak ◽  
Atanu Banerjee ◽  
Tapas Laha

2009 ◽  
Vol 106 (8) ◽  
pp. 086105 ◽  
Author(s):  
Guoyong Wang ◽  
Jianshe Lian ◽  
Zhonghao Jiang ◽  
Liyuan Qin ◽  
Qing Jiang

e-Polymers ◽  
2007 ◽  
Vol 7 (1) ◽  
Author(s):  
Wenbo Luo ◽  
Said Jazouli ◽  
Toan Vu-Khanh

AbstractThe creep behavior of a commercial grade polycarbonate was investigated in this study. 10 different constant stresses ranging from 8 MPa to 50 MPa were applied to the specimen, and the resultant creep strains were measured at room temperature. It was found that the creep could be modeled linearly below 15 MPa, and nonlinearly above 15 MPa. Different nonlinear viscoelastic models have been briefly reviewed and used to fit the test data. It is shown that the Findley model is a special case of the Schapery model, and both the Findley model and the simplified multiple integral representation are suitable for properly describing the creep behavior of the polycarbonate investigated in this paper; however, the Findley model fit the data better than the simplified multiple integral with three terms.


1991 ◽  
Vol 18 (6) ◽  
pp. 1125-1130 ◽  
Author(s):  
G. Y. Gao ◽  
S. C. Dexter

Materials ◽  
2019 ◽  
Vol 12 (24) ◽  
pp. 4213
Author(s):  
Wei Hang ◽  
Xianwei Huang ◽  
Min Liu ◽  
Yi Ma

Relying on nanoindentation technology, the room-temperature creep behavior of a LiTaO3 single crystal in the typical orientation (01 1 ¯ 2), i.e., Y-42° plane was investigated. Three kinds of spherical tips with the radii of 0.76, 2.95 and 9.8 μm were respectively applied to detect nanoindentation length scale effect on creep deformation at both elastic and plastic regions. Superficially, both creep displacement and rate were nearly linearly increased with increasing holding depth and independent of tip size, which could be ascribed to the simultaneously enlarged holding strain and deformation volume beneath the indenter. At a similar holding strain, creep deformation, i.e., creep strain and strain rate were more pronounced under smaller spherical tips. Strain rate sensitivities of creep flows under different spherical tips and holding strains were also estimated. The potential room-temperature creep mechanism of LiTaO3 under high shear compression stress was discussed.


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