2018
DOI: 10.1016/j.jallcom.2018.07.024
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Hot deformation behavior and processing map of a superlight dual-phase Mg–Li alloy

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Cited by 59 publications
(12 citation statements)
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“…In the first stage of alloy deformation, the dislocation multiplication rate was fast, correspondingly occurring during the rapid development of dislocation density. Hence, the stress increased, and the work hardening process was principal [ 30 ]. However, when the strain grew to a specific point, the storage energy of deformation increased, attended by dynamic softening, but work hardening was still the primary deformation phenomenon.…”
Section: Resultsmentioning
confidence: 99%
“…In the first stage of alloy deformation, the dislocation multiplication rate was fast, correspondingly occurring during the rapid development of dislocation density. Hence, the stress increased, and the work hardening process was principal [ 30 ]. However, when the strain grew to a specific point, the storage energy of deformation increased, attended by dynamic softening, but work hardening was still the primary deformation phenomenon.…”
Section: Resultsmentioning
confidence: 99%
“…Numerous interactions inhibit the dislocation motion. Therefore, the stress rises sharply at very low strain in this stage and the work hardening process is predominant [21]. When the strain increases to a certain degree, the deformation storage energy increases, accompanied by dynamic softening, but work hardening is still the main deformation mechanism.…”
Section: Hot Compression Flow Behaviormentioning
confidence: 99%
“…Deformation temperature and strain rate are important factors controlling the hot deformation flow stress. The hyperbolic sinusoidal constitutive equation in the Arrhenius model has been widely used to describe the complex relationships among flow stress, heat distortion temperature, and strain rate [8][9][10][11][12][13][14][15][16][17][18][19]27]. Sellars and McTegart proposed the use of a hyperbolic sine function including the thermal deformation activation energy Q and temperature T to describe the thermal activation behavior of the material.…”
Section: Constitutive Equationsmentioning
confidence: 99%
“…= exp = sinh (12 By applying the natural logarithm in Equation 12, we can obtain the following equation: ln = ln + = ln sinh + ln (13 By substituting the values of T and ln into Equation 13, the value of the Zener-Hollom arameter (lnZ) at different temperatures and strain rates can be obtained. As shown in Figure 5 worth noting that the value change trend of lnZ is the same as the flow stress, and increases as t eformation temperature decreases or the strain rate increases.…”
Section: Constitutive Equationsmentioning
confidence: 99%
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