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应力状态与应变率对平纹编织CFRP面内力学行为的影响

张雪松 孙晓旺 王显会 姚土灶 肖杉雨 许丁鹏 付条奇 何佳豪

张雪松, 孙晓旺, 王显会, 等. 应力状态与应变率对平纹编织CFRP面内力学行为的影响[J]. 复合材料学报, 2024, 42(0): 1-12.
引用本文: 张雪松, 孙晓旺, 王显会, 等. 应力状态与应变率对平纹编织CFRP面内力学行为的影响[J]. 复合材料学报, 2024, 42(0): 1-12.
ZHANG Xuesong, SUN Xiaowang, WANG Xianhui, et al. Effects of stress state and strain rate on the in-plane mechanical behavior of plain woven CFRP[J]. Acta Materiae Compositae Sinica.
Citation: ZHANG Xuesong, SUN Xiaowang, WANG Xianhui, et al. Effects of stress state and strain rate on the in-plane mechanical behavior of plain woven CFRP[J]. Acta Materiae Compositae Sinica.

应力状态与应变率对平纹编织CFRP面内力学行为的影响

基金项目: 国家自然科学基金 (52272370);先进越野系统技术全国重点实验室开放基金项目
详细信息
    通讯作者:

    孙晓旺,博士,副教授,硕士生导师,研究方向为材料动态力学行为、车辆结构优化设计 E-mail: xwsun@njust.edu.cn

  • 中图分类号: TB332

Effects of stress state and strain rate on the in-plane mechanical behavior of plain woven CFRP

Funds: National Natural Science Foundation of China (52272370); Open Fund of Chinese Scholar Tree Ridge State Key Laboratory
  • 摘要: 平纹编织碳纤维增强聚合物基复合材料(Plain Weave Carbon Fiber Reinforced Polymer,PWCFRP)因其均匀的面内力学性能而被广泛应用于航空、航天、车辆等工程领域,但其力学性能的表征和失效机制的揭示一直是应用中的难点。为探究应力状态与应变率对PWCFRP面内力学行为的影响,进行了准静态拉伸、压缩、剪切实验和动态拉伸实验,分析了材料的力学性能与损伤机制,并基于Tsai-Wu失效准则定量分析了材料在多轴应力状态、不同应变率、不同离轴角下的失效包络。结果表明:准静态载荷下PWCFRP表现出显著的拉压不对称性,拉伸强度相较压缩强度提高了120.46%;拉伸和剪切载荷下PWCFRP的力学行为具有非线性。拉伸状态下材料的失效主要为纤维束的拉伸断裂,断裂位置呈现一定随机性;压缩状态下材料的失效主要是由局部高剪切应力引起的纤维束扭结断裂导致的,断裂角度约呈37°;剪切状态下材料的失效模式主要为树脂的拉剪耦合失效。动态拉伸载荷下PWCFRP的拉伸强度随着应变率的提高先增大后减小,2000 s−1应变率时强度值最高。多轴应力状态下,PWCFRP的拉伸强度和应变率效应显著程度均与离轴角度(0°~45°)呈负相关趋势。

     

  • 图  1  样件制备流程

    Figure  1.  Preparation process of the experimental sample

    图  2  准静态面内力学实验装置

    Figure  2.  Quasi-static in-plane mechanics experimental device

    图  3  SHTB实验装置

    Figure  3.  SHTB experimental device

    图  4  PWCFRP准静态拉伸真实应力-应变曲线

    Figure  4.  Quasi-static tensile true stress-strain curve of PWCFRP

    图  5  PWCFRP准静态拉伸宏观损伤

    Figure  5.  Macroscopic damage of PWCFRP during quasi-static tensile testing

    图  6  PWCFRP准静态拉伸细观损伤

    Figure  6.  Microscopic damage of PWCFRP during quasi-static tensile testing

    图  7  PWCFRP准静态压缩真实应力-应变曲线

    Figure  7.  Quasi-static compression true stress-strain curve of PWCFRP

    图  8  PWCFRP准静态压缩宏观损伤

    Figure  8.  Macroscopic damage of PWCFRP during quasi-static compression testing

    图  9  PWCFRP准静态压缩细观损伤

    Figure  9.  Microscopic damage of PWCFRP during quasi-static compression testing

    图  10  PWCFRP准静态剪切真实应力-应变曲线

    Figure  10.  Quasi-static shear true stress-strain curve of PWCFRP

    图  11  PWCFRP准静态剪切宏观损伤

    Figure  11.  Macroscopic damage of PWCFRP during quasi-static shear testing

    图  12  PWCFRP准静态剪切细观损伤

    Figure  12.  Microscopic damage of PWCFRP during quasi-static shear testing

    图  13  PWCFRP动态面内拉伸真实应力-应变曲线

    Figure  13.  True stress-strain curve of PWCFRP in-plane dynamic tension

    图  14  PWCFRP动态拉伸宏观损伤

    Figure  14.  Macroscopic damage of PWCFRP during dynamic tensile testing

    图  15  PWCFRP拉伸强度-应变率关系拟合

    Figure  15.  Fitting of tensile strength-strain rate relationship of PWCFRP

    图  16  PWCFRP多轴正应力状态下失效包络线

    Figure  16.  Failure envelope of PWCFRP under multiaxial normal stress state

    图  17  PWCFRP在不同离轴角下的强度

    Figure  17.  Strength of PWCFRP at different off-axis angles

    表  1  准静态力学实验设计

    Table  1.   Experimental design of quasi-static mechanics

    Sample number Displacement rate/(mm·min−1) Strain rate/s−1
    T-0-1 ~ T-0-5 0.9 1×10−4
    C-0-1 ~ C-0-5 0.08
    S-12-1 ~ S-12-5 0.18
    Notes:T represents tensile test; C represents compression test; S represents shear plane; 0 represents the warp direction of the yarn; 12 represents the in-plane shear plane; 1~5 represents the test number value.
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  • 收稿日期:  2024-07-01
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