粘结单元在模拟FRP层合板低速冲击响应中的应用

蒋振 文鹤鸣

蒋振, 文鹤鸣. 粘结单元在模拟FRP层合板低速冲击响应中的应用[J]. 爆炸与冲击, 2019, 39(4): 043202. doi: 10.11883/bzycj-2017-0245
引用本文: 蒋振, 文鹤鸣. 粘结单元在模拟FRP层合板低速冲击响应中的应用[J]. 爆炸与冲击, 2019, 39(4): 043202. doi: 10.11883/bzycj-2017-0245
JIANG Zhen, WEN Heming. Application of cohesive elements in modeling the low-velocity impact responseand failure of fiber reinforced plastic laminates[J]. Explosion And Shock Waves, 2019, 39(4): 043202. doi: 10.11883/bzycj-2017-0245
Citation: JIANG Zhen, WEN Heming. Application of cohesive elements in modeling the low-velocity impact responseand failure of fiber reinforced plastic laminates[J]. Explosion And Shock Waves, 2019, 39(4): 043202. doi: 10.11883/bzycj-2017-0245

粘结单元在模拟FRP层合板低速冲击响应中的应用

doi: 10.11883/bzycj-2017-0245
详细信息
    作者简介:

    蒋 振(1991- ),男,硕士研究生,zj0510@mail.ustc.edu.cn

    通讯作者:

    文鹤鸣(1965- ),男,博士,教授, hmwen@mail.ustc.edu.cn

  • 中图分类号: O347.3

Application of cohesive elements in modeling the low-velocity impact responseand failure of fiber reinforced plastic laminates

  • 摘要: 纤维增强树脂基复合材料层合板(fibre reinforced plastic composites,FRP)在航空、航天、交通、造船等诸多工程中得到了日益广泛的应用,而其在冲击载荷下的响应和破坏特别是分层一直为学术界所关注。本文中对FRP层合板在冲击载荷下的响应和破坏进行数值模拟,并通过引入粘结层重点研究其分层破坏。首先,介绍一种基于改进的粘结区域方法的粘结层损伤模型;其次,详细介绍了有限元模型建模过程和建模细节;最后,对有限元模型进行验证,并分析分层损伤发生的原因。模拟结果表明,该模型不仅能准确预测FRP层合板在低速冲击载荷下的载荷-时间曲线和载荷-位移曲线,还能成功地预测其分层破坏。
  • 图  1  牵引力-位移准则示意图

    Figure  1.  Schematic diagram of traction-separation law

    图  2  FRP层合板组成示意图

    Figure  2.  Schematic diagram of FRP laminates

    图  3  将粘结单元插入实体单元示意图

    Figure  3.  Illustration of cohesive elements inserted in solid elements

    图  4  低速冲击下CFRP层合板的有限元模型

    Figure  4.  Finite element model for CFRP laminates under low velocity impact

    图  5  数值模拟得到的载荷-时间历程与实验观察[15]的比较

    Figure  5.  Comparison of the numerically predicted load-time histories with the experimental observations[15]

    图  6  数值模拟得到的载荷-位移曲线与实验观察[15]的比较

    Figure  6.  Comparison of the numerically predicted load-displacement cures with the experimental observations[15]

    图  7  数值模拟得到的分层形貌与实验结果[15]的比较

    Figure  7.  Comparison of the numerically predicted delamination areas with the experimental observations[15]

    表  1  模型中用到的粘结层参数

    Table  1.   cohesive interface properties used in present model

    材料参数 数值 材料参数 数值 材料参数 数值
    $ {\tau _{n}^{\left( {\rm{s}} \right)}}$ 11 MPa $ {\tau _{s}^{\left( {\rm{s}} \right)}}$ 17 MPa $ {\tau _{t}^{\left( {\rm{s}} \right)}}$ 17 MPa
    $ {G_{{\rm{IC}}}}$ 0.3 N/mm[17] $ {G_{{\rm{IIC}}}}$ 0.8 N/mm[17] $ {G_{{\rm{IIIC}}}}$ 0.8 N/mm[17]
    $ {K_{n}^{\left( {\rm{s}} \right)}}$ 850 MPa[21] $ {K_{s}^{\left( {\rm{s}} \right)}}$ 850 MPa[21] $ {K_{t}^{\left( {\rm{s}} \right)}}$ 850 MPa[21]
    $ {A_{\rm{i}}}$ 2.5[22] $ {B_{\rm{i}}}$ 0.9[22] $ {C_{\rm{i}}}$ 3.7[22]
    $ {A_{\rm{m}}}$ 1.85[22] $ {B_{\rm{m}}}$ 0.5[22] $ {C_{\rm{m}}}$ 1.3[22]
    下载: 导出CSV

    表  2  Graphite/epoxy单层板的参数值

    Table  2.   Parameters for graphite/epoxy laminates

    材料参数 数值 材料参数 数值 材料参数 数值
    $ {{E}_{11}}$ 143.4 GPa[17] $ {Y_{\rm{t}}}$ 54 MPa[17] $ {{\nu }_{23}}$. 0.52[17]
    $ {{E}_{22}}$ 9.27 GPa[17] $ {{X}_{\rm{c}}}$ 1 650 MPa[17] $ {{\nu }_{13}},{{\nu }_{12}}$ 0.31[17]
    $ {{E}_{33}}$ 9.27 GPa[17] $ {{Y}_{\rm{c}}}$ 240 MPa[17] $ {{\delta }_{1}^{\left( \rm{f} \right)}},\rm{ }{{\delta }_{2}^{\left( \rm{f} \right)}}$ 5.7×10−2 mm[12]
    $ {G_{12}}$ 3.8 GPa[17] $ {Z_{\rm{t}}}$ 54 MPa[17] $ {\delta _7^{\left( {\rm{f}} \right)}}$ 2.7×10−2 mm[12]
    $ {G_{23}}$ 3.2 GPa[17] $ {Z_{\rm{c}}}$ 240 MPa[17] $ {\delta _3^{\left( {\rm{f}} \right)}},{\rm{ }}{\delta _4^{\left( {\rm{f}} \right)}}$ 7.65×10−2 mm[12]
    $ {G_{31}}$ 3.8 GPa[17] $ {S_{12}}$ 100 MPa[17] $ {\delta _5^{\left( {\rm{f}} \right)}}$ 5×10−3 mm[12]
    $ {X_{\rm{t}}}$ 2 945 MPa[17] $ {S_{31}},{S_{23}}$ 100 MPa[17] $ {\delta _6^{\left( {\rm{f}} \right)}}$ 5×10−2 mm[12]
    下载: 导出CSV
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出版历程
  • 收稿日期:  2017-06-30
  • 修回日期:  2017-08-28
  • 网络出版日期:  2019-03-25
  • 刊出日期:  2019-04-01

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