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孔隙坍塌行为对多孔材料冲击压缩特性的影响理论分析

马路遥 张先锋 熊玮 刘闯 谈梦婷 邓宇轩 侯先苇

马路遥, 张先锋, 熊玮, 刘闯, 谈梦婷, 邓宇轩, 侯先苇. 孔隙坍塌行为对多孔材料冲击压缩特性的影响理论分析[J]. 爆炸与冲击. doi: 10.11883/bzycj-2024-0502
引用本文: 马路遥, 张先锋, 熊玮, 刘闯, 谈梦婷, 邓宇轩, 侯先苇. 孔隙坍塌行为对多孔材料冲击压缩特性的影响理论分析[J]. 爆炸与冲击. doi: 10.11883/bzycj-2024-0502
MA Luyao, ZHANG Xianfeng, XIONG Wei, LIU Chuang, DENG Yuxuan, HOU Xianwei, . Theoretical analysis of the influence of pore collapse behavior on the shock compression characteristics of porous materials[J]. Explosion And Shock Waves. doi: 10.11883/bzycj-2024-0502
Citation: MA Luyao, ZHANG Xianfeng, XIONG Wei, LIU Chuang, DENG Yuxuan, HOU Xianwei, . Theoretical analysis of the influence of pore collapse behavior on the shock compression characteristics of porous materials[J]. Explosion And Shock Waves. doi: 10.11883/bzycj-2024-0502

孔隙坍塌行为对多孔材料冲击压缩特性的影响理论分析

doi: 10.11883/bzycj-2024-0502
基金项目: 国家自然科学基金项目(12141202,12202205)
详细信息
    作者简介:

    马路遥(2001- ),男,博士研究生,3501093819@qq.com

    通讯作者:

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

  • 中图分类号: O346.3

Theoretical analysis of the influence of pore collapse behavior on the shock compression characteristics of porous materials

  • 摘要: 多孔材料在冲击压缩过程中伴随着孔隙坍塌行为,本文基于前人开展的试验中所观测到的冲击波结构,对多孔材料的冲击波形成过程及孔隙坍塌行为间的联系进行了理论分析。首先,考虑多孔材料的压缩曲线特性和冲击波追赶问题,提出了多孔材料的冲击波结构存在低压单波模式、双冲击波模式和高压单波三种模式。进一步,结合Wu-Jing物态方程发展了与不同冲击波模式相容的冲击压缩特性计算方法,得到了与单冲击波模式相容的冲击比容计算方程,可以无需采取近似条件直接计算临界比容。此外,通过对弹性阶段与弹塑性阶段材料的孔隙度随压力的变化规律采取线性近似,并考虑了多孔材料中基体材料受力与宏观应力之间的关系,修正了Carroll建立的孔隙坍塌关系方程。基于本文发展的考虑孔隙坍塌行为的冲击压缩特性计算模型,对材料的Hugoniot数据进行了计算,讨论了孔隙坍塌行为对多孔材料冲击压缩特性的影响。结果表明在较低压力时材料的冲击物态特性受孔隙坍塌行为影响明显,本文模型能够更加精确地预测多孔材料的冲击波参量。
  • 图  1  典型的具有三波结构的波剖面[18]

    Figure  1.  Typical wave profile with three-wave structure

    图  2  具有三波结构的多孔材料冲击波波剖面示意图

    Figure  2.  Schematic diagram of shock wave profile of porous material with three-wave structure

    图  3  不同压缩曲线的材料在压缩过程中的波系特征示意图

    Figure  3.  The schematic diagram of wave system characteristics of materials with different compression curves in the process of compression

    图  4  多孔材料冲击绝热线示意图

    Figure  4.  Schematic diagram of Hugoniot curve of porous material

    图  5  多孔材料简化模型冲击绝热线示意图

    Figure  5.  Schematic diagram of Hugoniot curve of porous material in Simplified mode

    图  6  冲击波追赶问题示意图

    Figure  6.  Characteristic line diagram of shock wave overtaking problem

    图  7  多孔材料中的三种冲击波模式

    Figure  7.  Three shock wave modes in porous materials

    图  8  三种计算方式下Hugoniot数据计算结果与实验结果对比

    Figure  8.  Comparison of the experimental results and computation of Hugoniot data under three calculation methods

    图  9  不同的孔隙坍塌模型下前驱冲击波波速与试验结果[15, 16]的对比

    Figure  9.  Comparison of precursor shock wave velocity with experimental results under different pore collapse models

    图  10  多孔钨的不同屈服强度下前驱冲击波波速与剪切模量及初始孔隙度的关系

    Figure  10.  The relationship between precursor shock wave velocity and shear modulus and initial porosity under different yield strength

    图  11  不同屈服强度下多孔铜Hugoniot数据计算结果与实验结果对比

    Figure  11.  Comparison of the experimental results and computation of Hugoniot data of porous copper under different yield strength

    图  12  不同初始孔隙度下多孔铁Hugoniot数据计算结果与实验结果对比

    Figure  12.  Comparison of the experimental results and computation of Hugoniot data of porous iron under different initial porosity

    表  1  计算密实材料Hugoniot数据所需的材料常数

    Table  1.   The material constants required for dense materials to calculate Hugoniot data

    材料 ρ0(g/cm3) Q(Gpa) q σy(Gpa) G(Gpa)
    8.924 52.90 10.0696 0.6[27] 47.7[27]
    19.2 185.27 7.1086 2.2[27] 160[27]
    7.856 34.94 11.9378 0.68[28] 89[28]
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