Slip line morphology, distribution and identification of sample A with 0.8 % tensile strain. Continuous and dotted black lines represent the calculated traces of basal and prismatic slip systems, respectively. (a) SEM image and slip line identification; (b) IPF map corresponding to Fig. 2a, step size 0.4 lm; (c) SEM image with higher magnification and slip line identification; (d) {110} b /{0002} a and {111} b /{11 20} a pole figures of a lamellae (labeled a, b) and thin b layers (labeled o) in Fig. 2c.

Slip line morphology, distribution and identification of sample A with 0.8 % tensile strain. Continuous and dotted black lines represent the calculated traces of basal and prismatic slip systems, respectively. (a) SEM image and slip line identification; (b) IPF map corresponding to Fig. 2a, step size 0.4 lm; (c) SEM image with higher magnification and slip line identification; (d) {110} b /{0002} a and {111} b /{11 20} a pole figures of a lamellae (labeled a, b) and thin b layers (labeled o) in Fig. 2c.

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This study combines geometrically necessary dislocation analysis and statistically-stored dislocation identification to investigate plastic deformation mechanisms in TA15 titanium alloy. Tensile tests were conducted up to different strains at room temperature. The slip lines were observed and identified using high resolution scanning electron micro...

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Context 1
... sample A with 0.8 % tensile strain, basal and prismatic slip system activations were detected in the selected a grains, which possess relatively high basal or prismatic slip Schmid factors (SFs), as shown in Fig. 2 and Table 3. At this deformation stage, the slip lines are straight and relatively fine (see the grains labeled 1, 2, and 8 in Fig. 2a). The slip lines show an almost equidistant distribution in the a grains. The slip lines originate from grain/phase boundaries and gradually extend into the grain interior. Two equivalent {10 10}<11 20> ...
Context 2
... sample A with 0.8 % tensile strain, basal and prismatic slip system activations were detected in the selected a grains, which possess relatively high basal or prismatic slip Schmid factors (SFs), as shown in Fig. 2 and Table 3. At this deformation stage, the slip lines are straight and relatively fine (see the grains labeled 1, 2, and 8 in Fig. 2a). The slip lines show an almost equidistant distribution in the a grains. The slip lines originate from grain/phase boundaries and gradually extend into the grain interior. Two equivalent {10 10}<11 20> slip system traces are additionally presented in some a grains (see grains 3 and 4 in Fig. ...
Context 3
... fine (see the grains labeled 1, 2, and 8 in Fig. 2a). The slip lines show an almost equidistant distribution in the a grains. The slip lines originate from grain/phase boundaries and gradually extend into the grain interior. Two equivalent {10 10}<11 20> slip system traces are additionally presented in some a grains (see grains 3 and 4 in Fig. ...
Context 4
... the distributions of slip lines in the observed zone are heterogeneous. No obvious slip traces were detected in some a grains, such as grains 5 and 6 in Fig. 2a, which also possess relative high SFs for basal or prismatic slip. These results indicate that, for polycrystals/multiphase materials, the slip system activations are not only determined by the relationships between crystallographic orientation and load axis, but other factors, such as grain morphology, neighbor phase and grains ...
Context 5
... the deformation strain is very small (Sample A, 0.8 % tensile strain), the slip is not constrained to one grain. Slip transmission phenomenon is observed in some regions, as shown in Fig. 2c. It shows clearly that slip transfers from one a lamella (labeled a) into another neighboring a grain (labeled b) by activating the related slip system of the b layer (labeled o) between them. This result is different from Bridier group's work on slip line morphology observation during Ti-6Al-4V in situ tensile deformation, which ...
Context 6
... alloy, which contains only 8.1 % b phase (volume fraction). Thus, the b layer is relatively thin and the slip is easy to transfer in comparison with a/b Ti-6Al-4V. Second, the Burgers orientation relationship (OR) ({0001} a ||{110} b ,< 1 1 20> a ||<111> b ) is fully maintained between a lamellae (labeled a and b) and b layer (labeled o) (see Fig. 2d). This special OR may facilitate the slip transmission [37,38]. The nature and distribution of gliding of sample B evolves significantly with increasing tensile strain. More a grains have been activated compared with sample A, as shown in Fig. 3a. Basal and prismatic slip systems are still the dominant deformation modes for a grains in ...

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TA15 (Ti–6Al–2Zr–1Mo–1V) is a near-α titanium alloy and has wide applications in the aerospace industry because of its high strength to mass ratio, good weldability, and superior creep resistance at high temperatures up to 550 °C, compared to other titanium alloys. This study investigates the flow behavior and microstructural evolution as functions of temperatures and strain rates during deformations under the superplastic conditions at 880 °C/0.01s⁻¹, 900 °C/0.01s⁻¹, 880 °C/0.001s−1, and 920 °C/0.0005s⁻¹. Results showed that this alloy exhibit excellent superplastic behavior for all selected temperatures and strain rates. The maximum tensile elongation of 1450% is achieved at 880 °C with a strain rate of 0.001s⁻¹. Flow softening is observed under deformation conditions of 880 °C/0.01s⁻¹ and 900 °C/0.01s⁻¹, while strain hardening is observed at deformation conditions of 880 °C/0.001s⁻¹ and 920 °C/0.0005s⁻¹. These complex flow behaviors are rationalized by characterizing the underlying microstructures on the interrupted tensile samples using electron backscatter diffraction (EBSD) and backscattered electrons (BSE). The geometrically necessary dislocations (GNDs) density, which is caused by lattice rotation and misorientations and plays a vital role in the plastic constitutive behaviors, was for the first time, systematically revealed. Together with other key microstructures, i.e. grain sizes, texture, phase fractions, the results show that the dominant deformation mode changes at initial, intermediate, and final stages of the deformation. The probable deformation mechanisms, such as grain boundary sliding (GBS) under different deformation conditions, are discussed in terms of grain morphology, GNDs, and texture evolution. Also, it is observed that the β-phase transformation is accelerated during deformation and contributes to the enhancement of superplasticity.