含LPSO相的Mg-Zn-Y-Sn合金在高应变速率下的变形行为

  • 徐志超 ,
  • 高松涛 ,
  • 米国发 ,
  • 潘虎成 ,
  • 秦高梧 ,
  • Md Shahriar A. Hossain
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  • 1 河南理工大学 材料科学与工程学院  焦作 454003

    2 东北大学 材料科学与工程学院 材料各向异性与织构教育部重点实验室  沈阳 110819

    3 The University of Queensland, EAIT, School of Mechanical and Mining Engineering, Brisbane, QLD 4072, Australia

收稿日期: 2025-10-23

  修回日期: 2026-05-11

  录用日期: 2026-05-26

  网络出版日期: 2026-05-27

基金资助

国家自然科学基金(52103290)

Deformation Behavior of Mg–Zn–Y–Sn Alloy Containing Long-Period Stacking Ordered Phase Under High Strain Rates

  • PAN, Hu Cheng ,
  • QIN, Gaowu
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  • 1 School of Materials Science and Engineering, Henan Polytechnic University, Jiaozuo 454003, China

    2 Key Laboratory for Anisotropy and Texture of Materials (Ministry of Education), College of Materials Science and Engineering, Northeastern University, Shenyang 110819, China

    3 School of Mechanical and Mining Engineering, EAIT, The University of Queensland, Brisbane, QLD 4072, Australia

Received date: 2025-10-23

  Revised date: 2026-05-11

  Accepted date: 2026-05-26

  Online published: 2026-05-27

摘要

为明确含长周期堆垛有序(LPSO)相Mg‑Zn‑Y系合金在高应变速率剪切条件下的强度响应、主导变形机制及其与显微组织演化的耦合关系,本工作采用分离式Hopkinson压杆(SHPB)装置,在800~1800 s-1应变速率下,对铸态和挤压态合金的组织演化和动态力学行为进行了对比分析。结果表明,随着应变速率由800 s-1提升至1800 s-1,挤压态Mg-4Zn-12Y合金的极限抗压强度由279.16 MPa提升至354.78 MPa,增幅约为27.1%。加入Sn元素后,随着应变速率由800 s-1提升至1600 s-1,挤压态合金的极限抗压强度由342 MPa提高至433 MPa,提升幅度约为26.6%。Sn元素的加入增强了合金的强度和加工硬化能力。其中,{1012}拉伸孪晶是协调塑性应变的主要方式,LPSO相的扭曲在协调变形中起到了关键作用。同时,在晶界三叉结处观察到大量几何必需位错的聚集,该现象导致局部晶格发生显著畸变,并为孪晶形核提供了有利条件。此外,LPSO相周围发生了动态再结晶,其主要由颗粒诱发形核机制及LPSO相与基体界面的复杂形貌所驱动。

本文引用格式

徐志超 , 高松涛 , 米国发 , 潘虎成 , 秦高梧 , Md Shahriar A. Hossain . 含LPSO相的Mg-Zn-Y-Sn合金在高应变速率下的变形行为[J]. 金属学报, 0 : 0 . DOI: 10.11900/0412.1961.2025.00329

Abstract

Lightweight Mg alloys are desirable for transportation and defense applications owing to their high specific strength and energy‑absorption capacity under impact loading. Among these, Mg–Zn–Y alloys containing long-period stacking-ordered (LPSO) phases exhibit exceptional comprehensive mechanical properties; however, their deformation behavior and underlying micromechanisms under high-speed shear remain poorly understood. Therefore, this study performs a comparative analysis of the microstructural evolution and dynamic mechanical behavior of as-cast and extruded Mg–Zn–Y–0.3Sn (mass fraction, %) alloys containing LPSO phases using a split Hopkinson pressure bar at strain rates ranging from 800 s−1 to 1800 s−1. The aim is to elucidate the strength response, identify the dominant deformation mechanisms, and clarify how microstructural evolution, including features characteristic of LPSO-containing Mg–Zn–Y alloys, couples with the high-strain-rate shear response. The results show that as the strain rate increases from 800 s−1 to 1800 s−1, the ultimate compressive strength of the extruded Mg–4Zn–12Y alloy increases from 279.16 MPa to 354.78 MPa, showcasing an enhancement of approximately 27.1%. Similarly, increasing the strain rate from 800 s−1 to 1600 s−1 raises the ultimate compressive strength of the extruded Mg–4Zn–12Y–0.3Sn alloy from 342 MPa to 433 MPa, corresponding to an improvement of approximately 26.6%. The Sn addition enhances the alloy’s strength and work-hardening capacity. The {1012} tensile twinning primarily serves to coordinate plastic strain, whereas kinking the LPSO phase plays a critical role in coordinating the deformation. High densities of geometrically necessary dislocations accumulate at grain-boundary triple junctions, producing considerable local lattice distortion and providing favorable conditions for twin nucleation. Furthermore, dynamic recrystallization occurs around the LPSO phase, driven primarily by the particle-stimulated nucleation mechanism and the complex morphology of the LPSO phase/matrix interface. These findings provide crucial insights into the deformation micromechanisms of LPSO-containing Mg alloys under high-strain-rate conditions.
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