1992
DOI: 10.1016/0956-716x(92)90686-9
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Steady-state creep deformation of investment cast near-gamma titanium aluminide

Abstract: IntroductionThe ongoing search for increased aircraft engine performance has prompted the materials community to investigate intermetallic compounds as potential replacement materials for nickel-and cobalt-based superalloys. Of particular interest over the past decade has been near-gamma titanium aluminides due to their low density, high modulus and strength retention at elevated temperatures, and good environmental resistance (1,2).While many investigators have studied the microstructure/property relationship… Show more

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Cited by 44 publications
(5 citation statements)
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“…Figure 18 shows the plot ln ᠨ e versus ln s from which the stress exponent was obtained as the slope of the line. The values obtained, n 8, is typical of this type of alloy 11,14 and indicates that the secondary stage of creep cannot be described by simple recovery processes. 22 When such high stress exponents are obtained, it is possible to rationalize the creep behavior assuming the existence of an athermal threshold stress, s 0 , and express the strain rate as: ᠨ e A (s 2 s 0 ) n 0 exp͑2Q͞RT ͒.…”
Section: Discussionmentioning
confidence: 80%
See 1 more Smart Citation
“…Figure 18 shows the plot ln ᠨ e versus ln s from which the stress exponent was obtained as the slope of the line. The values obtained, n 8, is typical of this type of alloy 11,14 and indicates that the secondary stage of creep cannot be described by simple recovery processes. 22 When such high stress exponents are obtained, it is possible to rationalize the creep behavior assuming the existence of an athermal threshold stress, s 0 , and express the strain rate as: ᠨ e A (s 2 s 0 ) n 0 exp͑2Q͞RT ͒.…”
Section: Discussionmentioning
confidence: 80%
“…Although it is generally accepted that the alloys exhibit power law creep behavior, the values of the stress exponent, n, appear to increase with increasing applied stress. 9,11 This has been interpreted as being due to a transition from diffusional creep at low stresses to dislocation glide creep at high stresses. 5,[12][13][14] Although mechanical twinning during creep deformation of TiAl alloys has been extensively reported, 5,[15][16][17] its contribution to the creep process is not easily interpreted since traditional creep theories do not include such contributions.…”
Section: Introductionmentioning
confidence: 99%
“…This is followed by the growth of secondary lamellae to form a discontinuous region on both sides of the grain boundary. The coarsening of lamellae in the alloy Ti-48Al-2Nb-2Cr after heat treatment at 1350 °C and after creep testing at 850 °C of heat-treated samples has been reported by Wheeler et al [24] Ramanujan [15] has studied the coarsening of primary lamellae in the alloy Ti-48Al-2Mn-2Nb annealing at 1200 °C, 1350°C, and 1420 °C for various annealing times followed by water quenching and has observed discontinuous and continuous coarsening. The annealing at 1200 °C shows dissolution of ␣/␣ 2 phases.…”
Section: Discussionmentioning
confidence: 87%
“…[20,21] Microstructural changes have been observed during creep deformation such as dynamic recrystallization, [20][21][22][23] spherodization, [24,25,26] dissolution of ␣ 2 phase, [27][28][29][30][31] and coarsening of lamellar. [24,27,29,30] The dissolution of ␣ 2 lamellae results in disappearance of the ␣ 2 phase and coarsening of lamellar structure that can degrade the creep properties by increasing both the primary and secondary creep strain rates.…”
Section: Introductionmentioning
confidence: 99%