Change in shape of hysteresis loop during cyclic deformation on austenitic stainless steel single crystals oriented for single slip
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Cited by (13)
Unified factor controlling the dislocation evolution of fatigued face-centered cubic crystals
2017, Acta MaterialiaCitation Excerpt :In wavy-slip materials the dislocations can easily change their slip plane by cross slip, which is essential for the formation of 3D composite structures [2–4]. In the classical textbook “Fatigue of Materials”, Suresh [5] systematically summarized the research results of different kinds of fatigued fcc crystals [6–16]. At room temperature the saturation shear stresses in the prominent plateau of the cyclic stress-strain (CSS) curves for single-slip oriented Cu and Ni single crystals are 27.5 MPa and 50 MPa, respectively, while the saturation plateau stress of single-slip oriented Ag single crystal is only ∼20 MPa [17].
Fundamental factors on formation mechanism of dislocation arrangements in cyclically deformed fcc single crystals
2011, Progress in Materials ScienceCitation Excerpt :However, fcc alloy single crystals have their characters of the cyclic deformation behaviors. In the classical textbook “Fatigue of Materials”, Suresh [16] systematically summarized the research results of different kinds of fcc crystals in the past three decades [18,31,40,71,97–103], as listed in Table 3. At room temperature the saturation plateau stresses of copper, nickel single crystals are 27.5 MPa and 50 MPa, respectively, while the saturation plateau stress of silver single crystal is only 20 MPa [83].
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2007, Comprehensive Structural IntegrityElectron channeling contrast imaging of dislocation structures in fatigued austenitic stainless steels
2005, Materials Science and Engineering: AModelling of the scatter in short fatigue cracks growth kinetics in relation with the polycrystalline microstructure
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2003, Comprehensive Structural Integrity: Nine Volume Set