1995
DOI: 10.1016/0079-6425(94)00007-7
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Deformation twinning

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Cited by 3,298 publications
(1,540 citation statements)
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References 228 publications
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“…Austenitic steels with high Mn content exhibit the most attractive combination of tensile strength and superior ductility due to their extraordinary strain-hardening rate, which is interpreted in terms of twinning-induced plasticity (TWIP) [2][3][4][5][6]. It is known that in face-centered cubic (fcc) metals with low stacking fault energies (SFEs),extensive deformation twinning results in the formation of deformation twins with a plate-like shape as well as nanometer spacing and thickness [2,[7][8][9]. The twin boundaries, which are special (low ÀΣ coincidence site lattice) high-angle boundaries [7] and contain a high density of sessile dislocations [8], act as equally effective obstacles to dislocation gliding as conventional grain boundaries in polycrystalline austenitic steels [10].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Austenitic steels with high Mn content exhibit the most attractive combination of tensile strength and superior ductility due to their extraordinary strain-hardening rate, which is interpreted in terms of twinning-induced plasticity (TWIP) [2][3][4][5][6]. It is known that in face-centered cubic (fcc) metals with low stacking fault energies (SFEs),extensive deformation twinning results in the formation of deformation twins with a plate-like shape as well as nanometer spacing and thickness [2,[7][8][9]. The twin boundaries, which are special (low ÀΣ coincidence site lattice) high-angle boundaries [7] and contain a high density of sessile dislocations [8], act as equally effective obstacles to dislocation gliding as conventional grain boundaries in polycrystalline austenitic steels [10].…”
Section: Introductionmentioning
confidence: 99%
“…It is known that in face-centered cubic (fcc) metals with low stacking fault energies (SFEs),extensive deformation twinning results in the formation of deformation twins with a plate-like shape as well as nanometer spacing and thickness [2,[7][8][9]. The twin boundaries, which are special (low ÀΣ coincidence site lattice) high-angle boundaries [7] and contain a high density of sessile dislocations [8], act as equally effective obstacles to dislocation gliding as conventional grain boundaries in polycrystalline austenitic steels [10]. The subdivision of initial grains into lamellas with thicknesses ranging from 10 to 40 nm [2][3][4][5][6]8] leads to a significant decrease in the effective grain size and, therefore, results in remarkable strengthening in accordance with the Hall-Petch relationship [11-13]: σ 0:2 ¼ σ 0 þK H d À 0:5 ð1Þ where σ 0.2 is the offset yield strength; d is the effective grain size, which is the distance between barriers to dislocation glide and can be estimated to be twice the width of lamellae [14]; σ 0 is the friction stress; and K H is the Hall-Petch coefficient.…”
Section: Introductionmentioning
confidence: 99%
“…Deformation twinning in hcp materials is directional, with a unique sense of shear, and results in the formation of a sheared domain, contributing to plastic deformation along the c -axis. 2 The article by Liao et al highlights several of these studies with a focus on the twinning system {10 1 2}〈10 11 〉, which is commonly activated in most hcp materials. The authors point out several technical challenges associated with deformation twinning in hcp materials.…”
Section: Deformation Twinning In Hexagonal Materialsmentioning
confidence: 99%
“…This is particularly the case during compression loading [7]. In α titanium, four different twinning modes have been reported [8]. At room temperature, the predominant twinning mode is the {10-12}<-1011> tensile twin [9,10] , which corresponds to a rotation of 85° around the <11-20> axis.…”
Section: Introductionmentioning
confidence: 99%