2002
DOI: 10.1016/s1044-5803(02)00286-3
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Synchrotron X-ray diffraction study of the phase transformations in titanium alloys

Abstract: High-resolution synchrotron X-ray diffraction was used to study the phase transformations in titanium alloys. Three titanium alloys were investigated: Ti -6Al -4V, Ti -6Al -2Sn -4Zr -2Mo -0.08Si and b21s. Both room and high temperature measurements were performed. The room temperature experiments were performed to study the structure of the alloys after different heat treatments, namely as received (AR), furnace cooling (FC), water quenching (WQ) and water quenching followed by ageing. The a, a 0 , a 00 and b … Show more

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Cited by 148 publications
(67 citation statements)
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“…The α and β values of the bulk alloy are always lower than those determined in the present experiments on powder. For comparison, the data of Malinov et al [8] are contrasted with the present results in Fig. 4 The differences displayed by Fig.…”
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confidence: 50%
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“…The α and β values of the bulk alloy are always lower than those determined in the present experiments on powder. For comparison, the data of Malinov et al [8] are contrasted with the present results in Fig. 4 The differences displayed by Fig.…”
mentioning
confidence: 50%
“…Results of analogous experiments performed on bulk Ti6Al-4V alloy are reported in the literature [8][9][10]. The expansion coefficients determined from tests in vacuum (pressure of 2.5 × 10 − 3 mbar) [8] were α = 1.043 × 10 − 5°C− 1 and β = 1.448 ×…”
Section: Resultsmentioning
confidence: 88%
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“…Using the diffusivity of hydrogen in β titanium, calculated from the equation given by Wasilewski and Kehl [42], and the lattice parameter for the β phase in Ti-6-4 reported by Malinov et al [44], the relaxation time at 298 K for octahedraloctahedral movement, τ oct , was calculated to be 1.1×10 −9 s and for tetrahedral-tetrahedral movement, τ tet , as 5.6×10 −10 s. The relaxation time determined from the experimental values aggregated in the present study, τ av , is 3.4×10 −9 s. This is on the order of τ oct Figure 6. (colour online) Behaviour of Q −1 with inverse temperature for the resonance with frequency 412 kHz at 298 K. Two fits for Snoek-like behaviour, with E act fixed at 23 kJ mol −1 are also shown.…”
Section: Acoustic Lossesmentioning
confidence: 99%