水泥砂浆抗弹性能研究

苗春贺 陈丽娜 单俊芳 王鹏飞 徐松林

苗春贺, 陈丽娜, 单俊芳, 王鹏飞, 徐松林. 水泥砂浆抗弹性能研究[J]. 高压物理学报, 2021, 35(2): 024205. doi: 10.11858/gywlxb.20200609
引用本文: 苗春贺, 陈丽娜, 单俊芳, 王鹏飞, 徐松林. 水泥砂浆抗弹性能研究[J]. 高压物理学报, 2021, 35(2): 024205. doi: 10.11858/gywlxb.20200609
MIAO Chunhe, CHEN Lina, SHAN Junfang, WANG Pengfei, XU Songlin. Research on the Ballistic Performance of Cement Mortar[J]. Chinese Journal of High Pressure Physics, 2021, 35(2): 024205. doi: 10.11858/gywlxb.20200609
Citation: MIAO Chunhe, CHEN Lina, SHAN Junfang, WANG Pengfei, XU Songlin. Research on the Ballistic Performance of Cement Mortar[J]. Chinese Journal of High Pressure Physics, 2021, 35(2): 024205. doi: 10.11858/gywlxb.20200609

水泥砂浆抗弹性能研究

doi: 10.11858/gywlxb.20200609
基金项目: 高压物理与地震科技联合实验室开放基金(2019HPPES01);国家自然科学基金(11672286,11602267);中石油-中科院战略合作重大项目(2015A-4812)
详细信息
    作者简介:

    苗春贺(1994-),男,博士研究生,主要从事冲击作用下脆性材料的损伤与破碎研究. E-mail:mch@mail.ustc.edu.cn

    通讯作者:

    徐松林(1971-),男,博士,研究员,博士生导师,主要从事材料在冲击下的动态响应研究.E-mail:slxu99@ustc.edu.cn

  • 中图分类号: O347; O385

Research on the Ballistic Performance of Cement Mortar

  • 摘要: 对于水泥砂浆的抗弹性能研究,目前很少考虑靶体所处的应力状态,为此基于自研的真三轴静载混凝土侵彻实验装置和水泥砂浆抗弹性能实验结果,讨论了水泥砂浆在不同应力状态下的开坑深度和开坑阻力。应用侵彻深度的经验公式和基于HJC模型的有限元数值计算方法,对比分析了水泥砂浆侵彻实验,结果表明,对于低速冲击过程,采用UMIST公式和HJC模型的数值分析对开坑深度的预测较为有效。应力状态对开坑深度有明显的影响,即随着侧限增加,水泥砂浆的三轴强度提高,弹丸的开坑深度减小。应用基于HJC模型的数值分析方法,研究了弹丸开坑过程中弹体内的加速度波形和y轴支撑杆上的波形,结果表明:弹丸开坑过程对两种波形都有影响,其中y轴支撑杆上的波形可以更好地反映开坑过程。虽然数值模拟结果与实验波形的趋势基本一致,但是应力幅值有一定的差异,说明基于HJC模型的数值分析对开坑阻力的计算能力尚待提高。

     

  • 图  真三轴静载混凝土侵彻实验装置

    Figure  1.  Experimental device of concrete specimen under true tri-axial confinement

    图  有限元计算模型

    Figure  2.  Finite element model

    图  不同侧限状态下的开坑深度

    Figure  3.  Pit depths under different lateral confinements

    图  不同侧限状态下开坑深度的拟合[15]

    Figure  4.  Fitting results of pit depth under different lateral confinement[15]

    图  开坑深度的进一步拟合

    Figure  5.  Further fitting of pit depth

    图  弹体侵彻过程中弹丸中的波形[25-26]

    Figure  6.  Recorded wave in the bullet during the penetration[25-26]

    图  模拟弹体侵彻过程中穿过试件的波形

    Figure  7.  Simulated wave profiles across specimen during penetration

    图  弹体侵彻过程中穿过试件的波形[15]

    Figure  8.  Wave profiles across specimen during penetration[15]

    图  弹丸加速度时程曲线

    Figure  9.  Acceleration wave profiles in bullet

    图  10  应力状态对波形的影响

    Figure  10.  Influence of stress state on waveform

    表  1  水泥砂浆的HJC本构模型参数

    Table  1.   Parameters of HJC model for cement mortar

    ${\;\rho {_0} }$/(kg·m−3)$G$/GPaAHJC/GPaBHJC/GPaCHJCNHJC$f{'} $/MPa
    18441.320.661.3350.00180.84514.4
    T/MPa${\dot \varepsilon{_0} }$/s−1$\varepsilon $f,minSmax${p{\rm{_c}} }$/MPa${\;\mu {\rm{_c}} }$${p{\rm{_l} } }$/GPa
    2.010.0180.2413.80.00751.096
    ${\;\mu {\rm{_l} } }$k1/GPak2/GPak3/GPaD1D2
    0.1585−1712080.0066291.0
    下载: 导出CSV

    表  2  弹丸JC本构模型参数

    Table  2.   Parameters of JC model of projectile

    ${\rho{_0} }$/(kg·m−3)G/GPaT0/Kc/(J·kg−1·K−1)AJC/MPaBJC/MPanJC
    7830772934777925100.26
    CJCTm/Kd1d2d3d4d5
    0.01417930.053.44−2.120.0020.61
    下载: 导出CSV

    表  3  无量纲侵彻深度公式参数

    Table  3.   Formula parameters of dimensionless penetration depth

    Stress statek0m1m2m3
    No confinement0.900.701.210.60
    Unilateral confinement1.020.551.250.65
    Bilateral confinement1.050.401.300.68
    下载: 导出CSV
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出版历程
  • 收稿日期:  2020-09-01
  • 修回日期:  2020-09-23
  • 刊出日期:  2021-03-25

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