梯度蜂窝夹芯板在爆炸荷载作用下的动力响应

李世强 李鑫 吴桂英 王志华 赵隆茂

李世强, 李鑫, 吴桂英, 王志华, 赵隆茂. 梯度蜂窝夹芯板在爆炸荷载作用下的动力响应[J]. 爆炸与冲击, 2016, 36(3): 333-339. doi: 10.11883/1001-1455(2016)03-0333-07
引用本文: 李世强, 李鑫, 吴桂英, 王志华, 赵隆茂. 梯度蜂窝夹芯板在爆炸荷载作用下的动力响应[J]. 爆炸与冲击, 2016, 36(3): 333-339. doi: 10.11883/1001-1455(2016)03-0333-07
Li Shiqiang, Li Xin, Wu Guiying, Wang Zhihua, Zhao Longmao. Dynamic response of functionally graded honeycomb sandwich plates under blast loading[J]. Explosion And Shock Waves, 2016, 36(3): 333-339. doi: 10.11883/1001-1455(2016)03-0333-07
Citation: Li Shiqiang, Li Xin, Wu Guiying, Wang Zhihua, Zhao Longmao. Dynamic response of functionally graded honeycomb sandwich plates under blast loading[J]. Explosion And Shock Waves, 2016, 36(3): 333-339. doi: 10.11883/1001-1455(2016)03-0333-07

梯度蜂窝夹芯板在爆炸荷载作用下的动力响应

doi: 10.11883/1001-1455(2016)03-0333-07
基金项目: 

国家自然科学基金项目 11172196

山西省自然科学基金项目 2014011009-1

详细信息
    作者简介:

    李世强(1986-),男,博士

    通讯作者:

    吴桂英,wgy2005112@163.com

  • 中图分类号: O381

Dynamic response of functionally graded honeycomb sandwich plates under blast loading

  • 摘要: 利用弹道冲击摆锤系统对分层梯度蜂窝夹芯板在爆炸荷载下的动力响应进行了实验研究,分析了梯度蜂窝夹芯板在爆炸荷载作用下的变形失效模式,并与传统非梯度蜂窝夹芯板的抗爆性能做了对比。通过一维应力波理论,分析了应力波在梯度芯层中的传播规律。应力波透射系数在梯度试件中比非梯度芯层中小,而且相对密度递减的芯层组合有最小的应力波透射系数。综合考虑结构变形失效模式,后面板挠度,芯层压缩量以及应力波传播特点得到:分层梯度蜂窝夹芯板的抗爆性能明显优于传统的非梯度夹芯板,在所研究的荷载范围内,芯层相对密度从大到小排列试件的抗爆性能相对较好。
  • 图  1  夹芯板试件

    Figure  1.  Specimens of sandwich plates

    图  2  冲击摆锤系统

    Figure  2.  Ballistic pendulum system

    图  3  TNT装药

    Figure  3.  TNT charge

    图  4  非梯度试件变形模式

    Figure  4.  Deformation modes of ungraded sandwich plates

    图  5  梯度试件变形模式

    Figure  5.  Deformation modes of graded sandwich plates

    图  6  芯层压缩区域划分

    Figure  6.  Failure pattern of the honeycomb core

    图  7  不同工况下后面板残余挠度

    Figure  7.  Permanent mid-point deflections of the back-face-sheet under differente conditions

    图  8  W=20g,R=200mm时的芯层压缩量

    Figure  8.  Core compressions while W=20g, R=200mm

    表  1  试件分组与实验结果

    Table  1.   Specimen configurations and blast loading results

    试件 芯层排列 W/g R/mm I/(N·s) γ/mm δ/mm
    C1 C2 C3
    G1 L-M-S 20 200 20.27 22.1 6.31 6.21 0.52
    G2 L-S-M 20 200 20.06 17.4 5.91 3.74 1.93
    G3 M-L-S 20 200 20.36 19.1 5.40 5.30 0.58
    G4 M-S-L 20 200 20.32 18.6 5.79 1.50 4.05
    G5 S-L-M 20 200 20.23 17.6 4.31 5.79 1.45
    G6 S-M-L 20 200 20.01 18.1 5.53 4.67 4.41
    G6 S-M-L 25 250 20.21 22.6 5.42 1.22 4.04
    G6 S-M-L 30 300 20.54 25.3 5.68 5.86 6.00
    UG1 S 20 120 20.19 34.6 贯穿
    UG1 S 20 150 20.03 21.7 贯穿
    UG1 S 20 200 20.14 20.6 7.70
    UG2 M 20 200 15.65 18.3 8.55
    UG2 M 30 300 19.25 28.6 10.88
    UG2 M 25 250 18.23 26.7 9.40
    UG3 L 20 200 15.31 24.0 13.60
    UG3 L 25 250 16.41 26.6 13.50
    UG3 L 30 300 19.03 26.1 13.00
    下载: 导出CSV

    表  2  材料力学性能参数

    Table  2.   Mechanical properties of aluminum alloys

    材料 σ0.2/MPa E/GPa ρs/(g·cm-3) ν
    AL5052 325 70 2.7 0.3
    AL1200 163 70 2.7 0.3
    下载: 导出CSV

    表  3  梯度试件芯层变形区域面积对比(W=20g,R=200mm)

    Table  3.   Comparison of the deformation area of the core layers (W=20g, R=200mm)

    试件 芯层排列 S1/mm2 S2/mm2
    C1 C2 C3 C1 C2 C3
    G1 L-M-S 254.3 78.5 12.7 132.7 28.3 0
    G2 L-S-M 213.7 63.6 12.6 86.5 0 0
    G3 M-L-S 176.6 132.7 7.1 50.2 28.3 0
    G4 M-S-L 201.0 50.2 78.5 63.6 0 7.1
    G5 S-L-M 132.7 153.9 15.9 0 28.3 0
    G6 S-M-L 103.8 38.5 201.0 33.2 5.0 0
    下载: 导出CSV
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出版历程
  • 收稿日期:  2014-10-13
  • 修回日期:  2015-02-10
  • 刊出日期:  2016-05-25

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