高速撞击下不同背板碳化硼陶瓷复合靶板的陶瓷锥形成机制

王新德 李明树 王仁杰 王永刚 蒋招绣

王新德, 李明树, 王仁杰, 王永刚, 蒋招绣. 高速撞击下不同背板碳化硼陶瓷复合靶板的陶瓷锥形成机制[J]. 高压物理学报. doi: 10.11858/gywlxb.20261037
引用本文: 王新德, 李明树, 王仁杰, 王永刚, 蒋招绣. 高速撞击下不同背板碳化硼陶瓷复合靶板的陶瓷锥形成机制[J]. 高压物理学报. doi: 10.11858/gywlxb.20261037
WANG Xinde, LI Mingshu, WANG Renjie, WANG Yonggang, JIANG Zhaoxiu. Formation Mechanism of Ceramic Cones in Boron Carbide Ceramic Composite Targets with Different Backplates under High-Velocity Impact[J]. Chinese Journal of High Pressure Physics. doi: 10.11858/gywlxb.20261037
Citation: WANG Xinde, LI Mingshu, WANG Renjie, WANG Yonggang, JIANG Zhaoxiu. Formation Mechanism of Ceramic Cones in Boron Carbide Ceramic Composite Targets with Different Backplates under High-Velocity Impact[J]. Chinese Journal of High Pressure Physics. doi: 10.11858/gywlxb.20261037

高速撞击下不同背板碳化硼陶瓷复合靶板的陶瓷锥形成机制

doi: 10.11858/gywlxb.20261037
基金项目: 国家自然科学基金(12102213,U2530210)
详细信息
    作者简介:

    王新德(2005-),男,本科,主要从事爆炸与冲击动力学研究. E-mail:wangxinhao1999@foxmail.com

    通讯作者:

    蒋招绣(1986-),男,博士,副研究员,主要从事爆炸与冲击动力学研究. E-mail:jiangzhaoxiu@nbu.edu.cn

  • 中图分类号: O385; O521.9

Formation Mechanism of Ceramic Cones in Boron Carbide Ceramic Composite Targets with Different Backplates under High-Velocity Impact

  • 摘要: 陶瓷锥是轻型陶瓷复合装甲实现抗弹侵彻能量耗散的关键物理机制。为此,针对碳化硼陶瓷复合装甲,选取6061铝合金、7075铝合金、T300碳纤维板及超高分子量聚乙烯板(ultra-high molecular weight polyethylene, UHMWPE)4种典型背板材料,采用一级轻气炮弹道冲击实验与LS-DYNA数值模拟相结合的方法,系统研究了背板屈服强度、刚度及波阻抗对陶瓷锥形态及演化的影响规律。结果表明:陶瓷锥对背板的载荷传递并非仅依赖单一外锥,而是通过外锥与内锥等多条裂纹的共同作用实现;背板的屈服强度对主要锥形的裂纹扩展无明显影响;在刚度方面,外锥角随弹性模量的增加而线性减小,内锥角则呈指数增大;波阻抗通过调控应力波反射/透射改变陶瓷内部应力场变化,致使内锥角随着波阻抗的增加呈线性增大,外锥角则随之呈指数减小。

     

  • 图  陶瓷复合装甲结构

    Figure  1.  Components of ceramic composite armor

    图  弹靶侵彻实验装置示意图

    Figure  2.  Schematic diagram of the projectile-target penetration experimental setup

    图  回收靶板与剩余弹体的照片

    Figure  3.  Photographs of the recovered target plate and residual projectile

    图  不同背板条件下碳化硼陶瓷复合靶板的三维锥体重构断裂面

    Figure  4.  Fracture surfaces of 3D reconstructed cones of boron carbide ceramic composite target plates under different backplate conditions

    图  弹道冲击模拟的数值模型示意图

    Figure  5.  Schematic diagram of the ballistic impact simulation model

    图  模拟与实验结果的对比

    Figure  6.  Comparison of simulated and experimental results

    图  6061铝合金/碳化硼陶瓷复合靶板的冲击响应

    Figure  7.  Impact response of a boron carbide ceramic composite target with a 6061 aluminum alloy backplate

    图  不同时刻不同背板碳化硼陶瓷复合靶板的陶瓷破坏行为

    Figure  8.  Failure behavior of ceramics in boron carbide ceramic composite plates with different backplates at different time

    图  背板的能量吸收率与屈服强度的相关性

    Figure  9.  Correlation between energy absorption rate of backplate and yield strength

    图  10  陶瓷锥角与弹性模量的相关性

    Figure  10.  Correlation between ceramic cone angle and elastic modulus

    图  11  陶瓷锥角与波阻抗的相关性

    Figure  11.  Correlation between ceramic cone angle and wave impedance

    表  1  不同背板陶瓷靶体的失效特征

    Table  1.   Failure characteristics of ceramic targets with different backplates

    Target materials v0/(m·s−1) $ {\beta }_{1} $/(°) $\varDelta $/(°) Vc/mm3 d/mm
    B4C/6061Al 245.1 76.7 1.3 55942.11 95.10
    B4C/7075Al 249.6 83.8 2.1 41108.19 86.88
    B4C/CF-T300 247.8 73.8 2.4 37152.59 74.50
    B4C/UHMWPE 252.3 85.1 1.9 21263.85 64.46
    下载: 导出CSV

    表  2  弹体材料的模型参数[19]

    Table  2.   Material model parameters of the projectile[19]

    Material $ \rho $/(g·cm−3) E/GPa ν A1/MPa B1/MPa n1 C1 C2
    CDX2 steel 7.850 252.3 0.295 3544 5606 0.85 0.012 0.086
    下载: 导出CSV

    表  3  金属背板材料的模型参数[2021]

    Table  3.   Material model parameters of the metal backplate[2021]

    Materials $ \rho $/(g·cm−3) G/GPa A/MPa B/MPa C m n Tm/K
    6061Al 2.704 26.69 256 113.8 0.002 1.350 0.420 877.6
    7075Al 2.810 27.00 568 327.0 0.014 1.015 0.378 893.0
    Materials Tr/K D1 D2 D3 D4 D5 c/(m·s−1) S1
    6061Al 293 −0.770 1.450 −0.47 0 1.6 5240 1.40
    7075Al 293 0.059 0.246 0 0 0 5190 1.33
    下载: 导出CSV

    表  4  T300碳纤维板的材料模型参数[23]

    Table  4.   Material model parameters of T300 carbon fiber board[23]

    E1/GPa E2/GPa E3/GPa G12/GPa G13/GPa G23/GPa ν12 ν13 ν23
    1409.09.04.64.63.0820.320.280.21
    ρ/(kg·m−3)XT/MPaXC/MPaYT/MPaYC/MPaSxy/MPaSxz/MPaSyz/MPa
    17501760110051130706060
    下载: 导出CSV

    表  5  UHMWPE纤维板的材料模型参数[25]

    Table  5.   Material model parameters of UHMWPE fiber board[25]

    E1/GPa E2/GPa E3/GPa G12/GPa G13/GPa G23/GPa $ {\nu }_{12} $ $ {\nu }_{13} $ $ {\nu }_{23} $
    40.6 40.6 2.6 174 548 548 0.008 0.044 0.044
    SN/MPa SC/MPa XT/MPa YT/GPa YC/GPa S23/MPa S13/MPa $ \rho \text{/(kg∙}{\text{m}}^{-3}) $
    900 0.5 3.6 3.6 3.0 900 900 1006
    下载: 导出CSV

    表  6  碳化硼材料模型参数[26]

    Table  6.   Model parameters of boron carbide material[26]

    ρ/(kg·m−3) G/GPa Ai Bi Ci M N $ {\dot{\varepsilon }}_{0}/{\rm s}^{-1} $ $ {t}_{\max }\text{/GPa} $
    2510 462 0.927 0.7 0.005 0.85 0.67 1 0.26
    $ {\sigma }_{\text{HEL}} $/GPa $ {p}_{\text{HEL}} $/GPa $ \beta $ $ {K}_{1} $ $ {K}_{2} $ $ {K}_{3} $ $ {D}_{\text{p1}} $ $ {D}_{\text{p2}} $ Fs
    15.44 8.71 1 233 −593 2800 0.001 0.5 0.8
    下载: 导出CSV

    表  7  实验与模拟结果的对比

    Table  7.   Comparison of experimental and simulated results

    Blackplate
    materials
    Lr β1 d
    Exp./mm Sim./mm Error/% Exp./(°) Sim./(°) Error/% Exp./mm Sim./mm Error/%
    6061Al 34.3 36.8 7.3 76.7 80.1 4.4 95.1 81.6 14.1
    7075Al 31.6 33.2 5.1 83.8 76.1 9.2 86.9 77.2 11.1
    CF-T300 32.7 34.8 6.4 73.8 68.5 7.2 74.5 70.2 5.8
    UHMWPE 38.4 41.2 7.3 85.1 84.5 0.7 68.5 59.1 13.7
    下载: 导出CSV
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  • 收稿日期:  2026-03-05
  • 修回日期:  2026-05-14
  • 网络出版日期:  2026-05-19

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