弹体侵彻YAG透明陶瓷/玻璃的剩余深度

陈贝贝 张先锋 邓佳杰 章健 包阔 谈梦婷

陈贝贝, 张先锋, 邓佳杰, 章健, 包阔, 谈梦婷. 弹体侵彻YAG透明陶瓷/玻璃的剩余深度[J]. 爆炸与冲击, 2020, 40(8): 083301. doi: 10.11883/bzycj-2019-0372
引用本文: 陈贝贝, 张先锋, 邓佳杰, 章健, 包阔, 谈梦婷. 弹体侵彻YAG透明陶瓷/玻璃的剩余深度[J]. 爆炸与冲击, 2020, 40(8): 083301. doi: 10.11883/bzycj-2019-0372
CHEN Beibei, ZHANG Xianfeng, DENG Jiajie, ZHANG Jian, BAO Kuo, TAN Mengting. Residual penetration depth of a projectile into YAG transparent ceramic/glass[J]. Explosion And Shock Waves, 2020, 40(8): 083301. doi: 10.11883/bzycj-2019-0372
Citation: CHEN Beibei, ZHANG Xianfeng, DENG Jiajie, ZHANG Jian, BAO Kuo, TAN Mengting. Residual penetration depth of a projectile into YAG transparent ceramic/glass[J]. Explosion And Shock Waves, 2020, 40(8): 083301. doi: 10.11883/bzycj-2019-0372

弹体侵彻YAG透明陶瓷/玻璃的剩余深度

doi: 10.11883/bzycj-2019-0372
基金项目: 国家自然科学基金(11772159);中央高校基本科研业务费专项资金(30917011104);高性能陶瓷和超微结构国家重点实验室开放基金(SKL201602SIC)
详细信息
    作者简介:

    陈贝贝(1993- ),男,硕士研究生,r.chan@njust.edu.cn

    通讯作者:

    张先锋(1978- ),男,博士,教授,lynx@njust.edu.cn

  • 中图分类号: O383

Residual penetration depth of a projectile into YAG transparent ceramic/glass

  • 摘要: 为了研究钇铝石榴石(yttrium aluminum garnet, YAG)透明陶瓷及玻璃材料的抗弹性能和冲击破坏机制,开展了12.7 mm穿甲燃烧弹侵彻YAG透明陶瓷/玻璃的剩余侵彻深度实验研究。基于变形侵彻和刚性侵彻机制建立理论模型分析子弹撞击YAG透明陶瓷和玻璃的作用过程,并利用空腔膨胀模型确定了剩余弹体对2024T351航空铝的剩余侵彻深度。实验结果表明:YAG透明陶瓷对子弹有较强的破碎作用,其防护能力显著高于玻璃材料。理论模型计算得到的剩余弹体质量和侵彻深度结果与实验结果吻合较好,可见本文建立的理论模型可用于评估不同面板材料的抗弹性能。
  • 图  1  剩余穿深试验用弹体和靶体以及试验原理

    Figure  1.  Projectile, target and principle of residual penetration test

    图  2  试验靶体的典型破坏形态

    Figure  2.  Damage morphologies in targets used in tests

    图  3  靶板中的侵彻弹道

    Figure  3.  Penetration trajectories in targets

    图  4  侵彻弹道对比

    Figure  4.  Comparison of penetration trajectories

    图  5  试验回收弹体

    Figure  5.  Recycled projectiles after tests

    图  6  侵彻过程示意图

    Figure  6.  Diagram of penetration

    图  7  尖卵形弹体弹形示意图

    Figure  7.  Diagram of an ogive-nosed projectile

    图  8  弹体质量损失计算模型的试验验证

    Figure  8.  Experimental verification of the calculation model for projectile mass loss

    图  9  模型预测结果与试验结果对比

    Figure  9.  Comparison of model prediction results with experimental results

    图  10  透明陶瓷厚度对剩余侵深的影响

    Figure  10.  Effect of transparent ceramic thickness on residual depth of penetration

    图  11  陶瓷厚度对弹体质量损失和剩余弹体速度的影响

    Figure  11.  Effects of ceramic thickness on mass loss and residual velocity of a projectile

    图  12  弹体强度对剩余侵彻深度的影响

    Figure  12.  Effect of projectile strength on depth of penetration

    图  13  弹体强度对侵彻过程的影响

    Figure  13.  Effects of different projectile strengths on penetration process

    图  14  不同撞击速度下剩余侵彻深度与陶瓷锥半锥角的关系

    Figure  14.  Relation of residual depth of penetration to the semi-angle of the ceramic cone under different impact velocities

    表  1  靶体尺寸及材料参数

    Table  1.   Sizes and material parametes for targets

    材料长/mm宽/mm高/mm密度/(g·cm−3)面密度/(kg·m−2)
    YAG透明陶瓷 81.4 69.7 9.24.5541.86
    硅酸盐玻璃100.0100.0 7.92.5320.24
    航空铝(2024T351)120.0120.0120.02.78
    下载: 导出CSV

    表  2  剩余侵彻深度试验结果

    Table  2.   Experimental results of residual depth of penetration

    试验弹速/(m·s−1)面板材料剩余穿深/mm防护因数
    1-1833.42024T351航空铝70.01.000
    1-2835.469.01.000
    2-1836.0YAG透明陶瓷29.01.589
    2-2838.128.81.596
    3-1835.9硅酸盐玻璃56.51.098
    3-2834.455.51.115
    下载: 导出CSV

    表  3  弹靶材料动态强度

    Table  3.   Dynamic strength of projectile and target materials

    材料动态屈服强度/MPa
    弹芯(高碳钢)1 600
    YAG透明陶瓷3 400
    硅酸盐玻璃 510[15]
    2024航空铝 400
    下载: 导出CSV

    表  4  尖卵形弹体参数

    Table  4.   Parameters of the ogive-nosed projectile

    参数数值及单位参数数值
    弹体强度Yp1.6 GPa[16]N11.09
    弹体初速v0835 m/sN20.112 7
    铝合金Y400 MPa[19]N*0.106 9
    铝合金E70 GPa[19]Ψ2.988
    玻璃强度σt5.1 GPa[18]μm0.02
    A3.64φ056.38°
    B1.15
    下载: 导出CSV
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出版历程
  • 收稿日期:  2019-09-25
  • 修回日期:  2019-11-13
  • 网络出版日期:  2020-06-25
  • 刊出日期:  2020-08-01

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