6061铝合金的静动态力学性能和弹道行为

冯治建 胡孟磊 张雪峰

冯治建, 胡孟磊, 张雪峰. 6061铝合金的静动态力学性能和弹道行为[J]. 高压物理学报, 2026, 40(3): 034101. doi: 10.11858/gywlxb.20251108
引用本文: 冯治建, 胡孟磊, 张雪峰. 6061铝合金的静动态力学性能和弹道行为[J]. 高压物理学报, 2026, 40(3): 034101. doi: 10.11858/gywlxb.20251108
FENG Zhijian, HU Menglei, ZHANG Xuefeng. Static and Dynamic Mechanical Properties and Ballistic Behavior of 6061 Aluminum Alloy[J]. Chinese Journal of High Pressure Physics, 2026, 40(3): 034101. doi: 10.11858/gywlxb.20251108
Citation: FENG Zhijian, HU Menglei, ZHANG Xuefeng. Static and Dynamic Mechanical Properties and Ballistic Behavior of 6061 Aluminum Alloy[J]. Chinese Journal of High Pressure Physics, 2026, 40(3): 034101. doi: 10.11858/gywlxb.20251108

6061铝合金的静动态力学性能和弹道行为

doi: 10.11858/gywlxb.20251108
详细信息
    通讯作者:

    冯治建(1980-),男,技术员,主要从事爆炸冲击测试研究. E-mail:zjfeng@bit.edu.cn

  • 中图分类号: O385; O521.9

Static and Dynamic Mechanical Properties and Ballistic Behavior of 6061 Aluminum Alloy

Funds: CHEN G, CHEN X W, CHEN Z F, et al. Simulations of A3 steel blunt projectiles impacting onto 45 steel plates [J]. Explosion and Shock Waves, 2007, 27(5): 390-397. DOI: 10.3321/j.issn:1001-1455.2007.05.002.
  • 摘要: 铝合金具有优异的力学性能,被广泛应用于航空航天、船舶及高新领域,其服役时常需承受动态冲击载荷,研究其在动态加载下的力学响应具有重要的理论和工程意义。以6061铝合金为研究对象,通过系统的实验测试和数值模拟深入研究其静、动态力学性能及弹道响应特性。实验结果表明,在0.001~3 800 s−1应变率范围内,6061铝合金表现出显著的应变率强化效应,流动应力随应变率的提高而显著增大,增幅达18.5%,但其应变硬化行为在不同应变率下保持相对稳定。基于最小二乘法标定的Johnson-Cook本构模型参数能够准确描述材料在不同应变率下的力学响应。弹道实验研究表明,球形弹丸侵彻6061铝合金靶板的弹道极限为282.6 m/s,且残余速度与入射速度在超弹道极限条件下呈良好的线性关系。靶板失效形貌分析揭示了其破坏模式与冲击速度的关系:低速冲击下主要表现为复合应力主导的整体变形,而高速侵彻时则以局部剪切破坏为主。建立有限元模型复现实验观测的弹道响应和破坏模式,验证了拟合的本构模型参数和数值方法的可靠性。采用经过实验验证的有限元模型,对不同直径球形弹丸侵彻6061铝合金靶板的弹道响应进行研究,在弹丸直径为10、8、6 mm时,靶板的弹道极限速度分别为283、392、443 m/s。因此,当靶板厚度不变时,弹丸质量越小,靶板的弹道极限速度越高。研究结果为6061铝合金在冲击载荷条件下的工程应用提供了重要的理论依据和实验数据支撑。

     

  • 图  SHPB实验系统

    Figure  1.  SHPB experimental system

    图  弹道实验测试系统

    Figure  2.  Ballistic experiment testing system

    图  弹丸-弹托配合示意图和靶板尺寸 (单位:mm)

    Figure  3.  Schematic diagram of the projectile and projectile-holder combination and the dimension of the target plate (Unit: mm)

    图  有限元模型及网格细节

    Figure  4.  FEM model and mesh detail

    图  6061铝合金的静动态力学性能

    Figure  5.  Static and dynamic mechanical properties of 6061 aluminum alloy

    图  准静态应力-应变线性拟合结果

    Figure  6.  Linearly fitted result of the quasi-static stress-strain

    图  实验与J-C模型拟合的应力-应变曲线对比

    Figure  7.  Comparison of stress-strain curves between the experiment results and fitted results

    图  6061铝合金弹道实验结果及弹道曲线

    Figure  8.  Experimental results and trajectory curve of 6061 aluminum alloy projectile

    图  回收靶板的宏观破坏

    Figure  9.  Macroscopic damage of the recycled target plates

    图  10  数值模拟和实验得到的初始-残余速度曲线对比

    Figure  10.  Comparison of the initial velocity-residual velocity curves obtained from numerical simulation and experiments

    图  11  不同速度冲击下靶板在不同时刻的应力分布及破坏演化

    Figure  11.  Stress distribution and failure evolution of the target plate under different impact velocities at various times

    图  12  不同直径球形弹丸侵彻5 mm厚6061铝合金靶板的有限元模型

    Figure  12.  FEM of spherical projectiles of different diameters penetrating a 5 mm thick 6061Al target plate

    图  13  数值模拟得到的不同直径球形弹丸侵彻6061铝合金靶板的弹道曲线

    Figure  13.  Ballistic curves obtained from FEM of different diameter spherical projectiles penetrating 6061Al

    表  1  拟合得到的6061铝合金的J-C本构模型参数

    Table  1.   Parameters of the J-C constitutive model for 6061 aluminum alloy obtained through fitting

    Material A/MPa B/MPa n C
    6061 Al 292 94 0.168 0.011 2
    下载: 导出CSV

    表  2  Q235钢的J-C本构模型参数[26]

    Table  2.   Parameters of the J-C constitutive model for Q235 steel[26]

    A/MPa B/MPa n C m
    410 20 0.08 0.1 0.55
    下载: 导出CSV

    表  3  靶板和弹丸的的基本参数

    Table  3.   Basic parameters of the target plate and projectile

    Part Material Density/(g·cm–3) Young’s modulus/GPa Poisson’s ratio
    Target 6061Al 2.70 70 0.33
    Projectile Q235 steel 7.85 200 0.30
    下载: 导出CSV
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出版历程
  • 收稿日期:  2025-06-11
  • 修回日期:  2025-07-24
  • 网络出版日期:  2025-07-27
  • 刊出日期:  2026-02-05

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