2012
DOI: 10.1016/j.ijplas.2012.06.001
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Deformation mechanisms and kinetics of time-dependent twinning in an α-titanium alloy

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Cited by 57 publications
(18 citation statements)
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“…However, twins were not detected for the current joints. In general, the formation of some types of twinning in hcp structures (α-Ti phase) is a way to accommodate plastic deformation [ 38 ]. For the Ti-6Al-4V alloy, the presence of the cubic crystalline (β-Ti phase) structure may relieve deformations through the larger amount of available slip systems of the bcc structure.…”
Section: Resultsmentioning
confidence: 99%
“…However, twins were not detected for the current joints. In general, the formation of some types of twinning in hcp structures (α-Ti phase) is a way to accommodate plastic deformation [ 38 ]. For the Ti-6Al-4V alloy, the presence of the cubic crystalline (β-Ti phase) structure may relieve deformations through the larger amount of available slip systems of the bcc structure.…”
Section: Resultsmentioning
confidence: 99%
“…During creep loading, twins in -Ti grow slowly over many hundreds of hours [2,3] potentially restricted by the presence of O interstitials. Further, strain-rate sensitivity of twin width during quasi-static testing as shown in Figure 3 indicates that a time dependent mechanism is involved in twinning for some -Ti alloys [13]; despite constant total strain and total twin volume fraction across all three strain rates, twin width decreases dramatically at higher strain rates. O interstitials also impede other shear-dominated processes such as the martensitic -phase to -phase transformation in Ti [14] and Zr [15].…”
Section: Twinning and Oxygen Interstitialsmentioning
confidence: 96%
“…Figure 3. Average twin thickness measured in post-deformation samples of -Ti-1.6V (wt.%) loaded to 3% total strain at room temperature in uniaxial tension (data from [13] Hex.…”
Section: Twinning and Oxygen Interstitialsmentioning
confidence: 99%
“…The curve of ln  -1/T was plotted as shown in Fig.7, which has a slope that is proportional (by a factor of R) to the activation energy at that particular creep strain. The value of activation energy for deformation of α titanium when slip is the rate-limiting deformation mechanism is given in the range of 30~40 kJ/mol [17,22] , while the activation energy for twin growth is 66 kJ/mol [17,18] . The low temperature primary creep activation energy of TA2 at different strain level is always higher than the activation energy for slip but lower than that for twinning, and thus both slip and twinning are active creep deformation mechanisms for TA2 at low temperature.…”
Section: Creep Deformation Mechanismmentioning
confidence: 99%