织物结构混杂纤维增强复合材料的抗侵彻性能

朱雨璇 蔡凤娇 刘志成 孙九霄 王静南 马玉斌

朱雨璇, 蔡凤娇, 刘志成, 孙九霄, 王静南, 马玉斌. 织物结构混杂纤维增强复合材料的抗侵彻性能[J]. 高压物理学报, 2025, 39(11): 110111. doi: 10.11858/gywlxb.20251179
引用本文: 朱雨璇, 蔡凤娇, 刘志成, 孙九霄, 王静南, 马玉斌. 织物结构混杂纤维增强复合材料的抗侵彻性能[J]. 高压物理学报, 2025, 39(11): 110111. doi: 10.11858/gywlxb.20251179
ZHU Yuxuan, CAI Fengjiao, LIU Zhicheng, SUN Jiuxiao, WANG Jingnan, MA Yubin. Effect of Fabric Structure Hybrid on Penetration Resistance Performance of Fiber Reinforced Composite[J]. Chinese Journal of High Pressure Physics, 2025, 39(11): 110111. doi: 10.11858/gywlxb.20251179
Citation: ZHU Yuxuan, CAI Fengjiao, LIU Zhicheng, SUN Jiuxiao, WANG Jingnan, MA Yubin. Effect of Fabric Structure Hybrid on Penetration Resistance Performance of Fiber Reinforced Composite[J]. Chinese Journal of High Pressure Physics, 2025, 39(11): 110111. doi: 10.11858/gywlxb.20251179

织物结构混杂纤维增强复合材料的抗侵彻性能

doi: 10.11858/gywlxb.20251179
基金项目: 湖北省自然科学基金(2025AFC029);湖北省JD计划(JD2023009)
详细信息
    作者简介:

    朱雨璇(1995-),女,博士,主要从事复合材料计算模拟研究. E-mail:2022140@wtu.edu.cn

    通讯作者:

    孙九霄(1981-),男,博士,教授,主要从事复合材料研究. E-mail:2017002@wtu.edu.cn

  • 中图分类号: O347.5; O521.9; TB33

Effect of Fabric Structure Hybrid on Penetration Resistance Performance of Fiber Reinforced Composite

  • 摘要: 针对提升军事装备安全性的迫切需求,聚焦纤维增强复合材料的失效模式、损伤演化和能量吸收机理,探讨了织物结构混杂对纤维增强复合材料抗侵彻性能的影响规律及机制,通过弹道侵彻实验和多尺度计算,分析了平纹和缎纹织物结构混杂对芳纶/热塑性聚氨酯(thermoplastic polyurethanes,TPU)复合材料抗侵彻性能的影响机制,考察了其剩余速度、损伤机理、吸能特性和破坏形貌。结果表明,平纹织物提供高平面内刚度,缎纹织物则利于平面外变形和能量耗散。以平纹织物为迎弹面、缎纹织物为背弹面的混杂结构的抗侵彻性能更优:前层(平纹)使子弹钝化并分散冲击能量,后层(缎纹)使能量耗散最大化。其中,排列顺序为K6D21的芳纶/TPU复合材料性能最优,其剩余速度为455.81 m/s,比吸能为28.51 J/(kg·m2),抗侵彻性能提升了9.50%。通过多特征参数SHAP(shapley additive explanations)值分析,可从织物结构、纤维性能以及混杂铺层方面优化复合材料结构设计,结合多尺度数值计算与实验验证扩充数据库,为复合材料的性能提升提供坚实的理论基础。

     

  • 图  一体化梯度热压成型工艺:(a)~(b)橡胶平板硫化机,(c) 制备过程

    Figure  1.  Integrated gradient hot pressing process: (a)–(b) rubber plate vulcanizing machines; (c) forming process

    图  多尺度建模示意图

    Figure  2.  Schematic diagram of multiscale modeling

    图  K27在(610±10) m/s冲击速度下的剩余速度曲线和横截面损伤形态

    Figure  3.  Residual velocity curve and cross-sectional damage morphology of K27 at an impact velocity of (610±10) m/s

    图  织物结构混杂复合材料在(610±10) m/s冲击速度下的能量吸收:(a) δBPI,(b) 应变能,(c) 摩擦能,(d) 非弹性损耗能

    Figure  4.  Energy absorption of fabric-structured hybrid composite material at impact velocity of (610±10) m/s: (a) δBPI; (b) strain energy; (c) frictional energy; (d) dissipation energy

    图  高速摄影获得的弹丸侵彻下织物结构混杂复合材料的变形进程(背弹面)

    Figure  5.  Deformation process of fabric-structured hybrid composite material ballistic penetration under high-speed photography (back surface)

    图  织物结构混杂复合材料在(610±10) m/s的冲击速度下迎弹面和背弹面的损伤形态

    Figure  6.  Damage morphologies of the front and back surfaces of fabric-structured hybrid composite materials under an impact velocity of (610±10) m/s

    图  织物结构混杂复合材料迎弹面的应力分布

    Figure  7.  Stress distribution of the front surface for fabric-structured hybrid composite material

    图  织物结构混杂复合材料背弹面的应力分布

    Figure  8.  Stress distribution of the back surface for fabric-structured hybrid composite material

    图  芳纶复合材料的多结构参数-抗侵彻性能影响分析

    Figure  9.  Influence of multi-structural parameters on the penetration resistance performance of aramid composite materials

    表  1  混杂复合材料参数

    Table  1.   Parameters of the hybrid composite materials

    MaterialMass/gThickness/mmArea density/(kg·m–2)
    K27271.48.4512.06
    D27269.38.2111.97
    K3D24268.18.2911.92
    K6D21269.38.3111.97
    K9D18270.68.3412.03
    下载: 导出CSV

    表  2  纤维增强复合材料的本构模型参数[20]

    Table  2.   Parameters for constitutive model of fiber reinforced composite materials[20]

    Material ρ/(g·cm–3) E1+/GPa E2+/GPa $ {\nu }_{12+} $ G12/GPa $ X $1+/MPa $ X $1−/MPa $ X $2+/MPa $ X $2−/MPa
    Plain weave AF 1.44 13.486 11.763 0.09 1.387 349.15 53.17 8 15
    Satin and sateen AF 1.41 14.297 10.438 0.09 1.247 373.35 49.80 8 15
    Material S/MPa $ {G}_{\mathrm{f}}^{1+} $/
    (kJ·m–2)
    $ {G}_{\mathrm{f}}^{1-} $/
    (kJ·m–2)
    $ {G}_{\mathrm{f}}^{2+} $/
    (kJ·m–2)
    $ {G}_{\mathrm{f}}^{2-} $/
    (kJ·m–2)
    $ {\alpha }_{12} $ $ {\alpha }_{12}^{\mathrm{m}\mathrm{a}\mathrm{x}} $ $ {\widetilde{\sigma }}_{\mathrm{y}0} $/GPa $ {d}_{\mathrm{m}\mathrm{a}\mathrm{x}} $
    Plain weave AF 20 1 0.307 8.4 0.9 1.44×10−9 13 485.67 11.763 0.09
    Satin and sateen AF 20 1 0.307 8.4 0.9 1.41×10−9 14 297.06 10.438 0.09
    下载: 导出CSV

    表  3  内聚力模型参数[21]

    Table  3.   Cohesive model parameters[21]

    ρ/(g·cm–3) E/GPa $ {{t}}_{\text{n}}^{\text{o}} $/MPa $ {{t}}_{\text{s}}^{\text{o}}/{{t}}_{\text{t}}^{\text{o}} $ $ {G}_{\text{Ⅰ}\text{C}} $/(N·mm–1) $ \mathit{{G}}_{\text{Ⅱ}\text{C}}\text{/}{G}_{\text{Ⅲ}\text{C}} $
    1 1 000 69 79 0.9 2
    下载: 导出CSV

    表  4  不同织物结构混杂复合材料靶板的弹道侵彻实验结果与多尺度计算结果

    Table  4.   Ballistic penetration experiment results and multi-scale calculation results of hybrid composite target plates with different fabric structures

    Specimens Striking velocity/
    (m·s–1)
    Residual velocity δBPI/
    (J·kg–1·m–2
    Hoist/%
    Exp./(m·s−1) Sim./(m·s−1) Error/%
    K27 618.24 476.21 484.27 2.0 26.04
    D27 615.76 462.57 459.28 1.1 27.88 7.05
    K3D24 616.51 461.24 457.46 1.0 28.36 8.90
    K6D21 613.78 455.81 449.23 1.4 28.51 9.50
    K9D18 617.52 463.63 455.67 1.7 27.94 7.29
    下载: 导出CSV
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出版历程
  • 收稿日期:  2025-08-29
  • 修回日期:  2025-09-25
  • 网络出版日期:  2025-10-09
  • 刊出日期:  2025-11-05

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