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October 2, 2025Metals4 citationsOpen Access

Dynamic Recrystallization and Microstructural Evolution During Hot Deformation of Al-Cu-Mg Alloy

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FHFang HeXWXiaolan WuZRZeyu Rong

Key Points

  • Dynamic recrystallization and recovery influence the microstructural evolution during hot deformation.
  • At high strain rates, discontinuous dynamic recrystallization primarily occurs, while continuous forms dominate at intermediate conditions.
  • The analysis employed inverse pole figure, grain boundary, and grain orientation spread characterization techniques.
  • Results indicate that the dynamic recrystallization process is highly dependent on both the deformation temperature and strain rate.

Abstract

Isothermal hot compression tests were performed on an Al-4.8Cu-0.25Mg-0.32Mn-0.17Si alloy using a Gleeble-3500 thermomechanical simulator within the temperature range of 350–510 °C and strain rate range of 0.001–10 s−1, achieving a true strain of 0.9. The constitutive equation and hot processing maps were established to predict the flow behavior of the alloy. The hot deformation mechanisms were investigated through microstructural characterization using inverse pole figure (IPF), grain boundary (GB), and grain orientation spread (GOS) analysis. The results demonstrate that both dynamic recovery (DRV) and dynamic recrystallization (DRX) occur during hot deformation. At high lnZ values (high strain rates and low deformation temperatures), discontinuous dynamic recrystallization (DDRX) dominates. Under middle lnZ conditions (low strain rate or high deformation temperature), both continuous dynamic recrystallization (CDRX) and DDRX are the primary mechanisms. Conversely, at low lnZ values (low strain rates and high temperatures), CDRX and geometric dynamic recrystallization (GDRX) become predominant. The DRX process in the Al-Cu-Mg alloy is controlled by the deformation temperature and strain rate.

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Cite This Study

He et al. (2025) studied this question.

synapsesocial.com/papers/68de5d9c83cbc991d0a20370https://doi.org/10.3390/met15101100
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