Unified Constitutive Laws of Plastic Deformation 1996
DOI: 10.1016/b978-012425970-6/50009-6
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Modeling the Role of Dislocation Substructure during Class M and Exponential Creep

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Cited by 14 publications
(6 citation statements)
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“…This model was used by Raj and Pharr [1989] to describe flow of halite at relatively high stresses ( σ > 4.44 MPa). Note that at moderate temperatures (320–640°K) the activation energy for creep of sodium chloride is not strongly dependent on stress [ Raj et al , 1996].…”
Section: Discussionmentioning
confidence: 99%
“…This model was used by Raj and Pharr [1989] to describe flow of halite at relatively high stresses ( σ > 4.44 MPa). Note that at moderate temperatures (320–640°K) the activation energy for creep of sodium chloride is not strongly dependent on stress [ Raj et al , 1996].…”
Section: Discussionmentioning
confidence: 99%
“…In literature [ 28 ], the cell consists of a wide and diffused boundary containing dislocation tangle, while the sub-boundary is narrow, where the misorientation angle across the sub-boundary is larger than that across the cell wall. Accounting the bright field images, distinctive differences in crystal orientations are apparent, but the dense dislocations more influence the strain contrast at the grain interior for the higher magnitude of plastic strain in Figure 3 f.…”
Section: Resultsmentioning
confidence: 99%
“…2 [37][38][39][40][41]. A number of studies have reported an inverse relationship between the subgrain/cell size and the applied stress [38,46,47]. The subgrain/cell size,  varies with the applied stress,  following the relationship:…”
Section: Creep Deformation Mechanism In Am 316l Ssmentioning
confidence: 99%