2002
DOI: 10.1016/s1359-6454(01)00351-2
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Characterization of the variant selection occurring during the α→β→α phase transformations of a cold rolled titanium sheet

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Cited by 240 publications
(109 citation statements)
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“…In comparison with the theoretical representation (10%, 20% + 30% → 50%, 20%, 20%) our results are dierent. It follows that the variant selection is not random, which is in accordance with the literature [11]. It is reported that these uneven volumefractions of the variants are caused by mutual orientations of original β-grains [11,12].…”
Section: Discussionsupporting
confidence: 85%
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“…In comparison with the theoretical representation (10%, 20% + 30% → 50%, 20%, 20%) our results are dierent. It follows that the variant selection is not random, which is in accordance with the literature [11]. It is reported that these uneven volumefractions of the variants are caused by mutual orientations of original β-grains [11,12].…”
Section: Discussionsupporting
confidence: 85%
“…In results from the literature, these peaks are predicted, but they are not distinguishable experimentally [7,11]. On the other hand, peaks for angles of 60…”
Section: Discussionmentioning
confidence: 95%
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“…It is also apparent, because the 45 • texture component is weaker than the remaining original component, that a degree of texture memory exists -less randomisation is observed than might naively be expected. It has been reported that in two-phase Ti-6Al-4V, the nucleation of new β grains from the α matrix which follow the Burgers orientation relationship (OR) is thermodynamically less favourable than growth of existing residual β-phase in the room temperature material [22,[25][26][27]. However, on cooling from the β phase field (i.e.…”
Section: β-Annealmentioning
confidence: 99%
“…The simulated random distributions in the cubic and hexagonal systems are shown in Figure 10. [34,35] Assuming that the areas of LAB, MAB, and HAB occupied the same area proportions in the cubic and hexagonal systems, the LAB, MAB, and HAB could be roughly assigned to be 0 to 13 deg, 13 to 35 deg, and over 35 deg, respectively, in the completely random hexagonal system. The misorientation angle distributions in the ␣ 2 and ␤ phases in the as-received alloy, and the post-SP 0 deg specimen at the fracture tip loaded at 750 °C and 920 °C are shown in Figure 11.…”
Section: Grain Misorientation Distributions Under Various Conditionsmentioning
confidence: 99%