2016
DOI: 10.1016/j.msea.2016.09.088
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Precipitation behavior during high-temperature isothermal compressive deformation of Inconel 718 alloy

Abstract: The precipitation behaviors of γ″ and δ phases during high-temperature isothermal compressive deformation of Inconel 718 alloy are investigated under the strain rate of 2.2·10 -4 s -1 . It is found that the precipitation behaviors are tailored by deformation temperatures, and lead to the disparately abnormal deformation characteristics. Under the deformation temperature of 800 o C, the microstructure is composed of incoherent needle-shaped γ″ precipitates at grain boundaries and ultrafine spherical γ″ particle… Show more

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Cited by 73 publications
(24 citation statements)
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References 36 publications
(42 reference statements)
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“…Jiang et al [32] analyzed the evolution of twins and substructures in hot deformation, and found that the dominant nucleation mechanism for Inconel 617B superalloy is original grain boundary bulging at low strain rates. Zhang et al [33] discussed the influences of γ′′ and δ phases on the high-temperature deformation behavior of Inconel 718 superalloy. Mei et al [34] discussed analyzed the effects of cold rolling on the precipitation and the morphology of δ-phase in Inconel 718 alloy.…”
Section: Introductionmentioning
confidence: 99%
“…Jiang et al [32] analyzed the evolution of twins and substructures in hot deformation, and found that the dominant nucleation mechanism for Inconel 617B superalloy is original grain boundary bulging at low strain rates. Zhang et al [33] discussed the influences of γ′′ and δ phases on the high-temperature deformation behavior of Inconel 718 superalloy. Mei et al [34] discussed analyzed the effects of cold rolling on the precipitation and the morphology of δ-phase in Inconel 718 alloy.…”
Section: Introductionmentioning
confidence: 99%
“…In these tests, a computer control automatic data acquisition system was applied to monitor the experimental data continuously. The recorded normal stress and normal strain were converted into the homologous true stress and true strain according to the formulae in Equations (1) and (2).…”
Section: Materials and Experiments Proceduresmentioning
confidence: 99%
“…ε T = ln(1 + ε N ) (2) where ε N and ε T are respectively the nominal strain and true strain, σ N and σ T are the nominal stress and true stress [21].…”
Section: Materials and Experiments Proceduresmentioning
confidence: 99%
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