• ISSN 1001-1455  CN 51-1148/O3
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单轴压缩下断续节理岩体动态损伤本构模型

刘红岩 李俊峰 裴小龙

刘红岩, 李俊峰, 裴小龙. 单轴压缩下断续节理岩体动态损伤本构模型[J]. 爆炸与冲击, 2018, 38(2): 316-323. doi: 10.11883/bzycj-2016-0261
引用本文: 刘红岩, 李俊峰, 裴小龙. 单轴压缩下断续节理岩体动态损伤本构模型[J]. 爆炸与冲击, 2018, 38(2): 316-323. doi: 10.11883/bzycj-2016-0261
LIU Hongyan, LI Junfeng, PEI Xiaolong. A dynamic damage constitutive model for rockmass with intermittent joints under uniaxial compression[J]. Explosion And Shock Waves, 2018, 38(2): 316-323. doi: 10.11883/bzycj-2016-0261
Citation: LIU Hongyan, LI Junfeng, PEI Xiaolong. A dynamic damage constitutive model for rockmass with intermittent joints under uniaxial compression[J]. Explosion And Shock Waves, 2018, 38(2): 316-323. doi: 10.11883/bzycj-2016-0261

单轴压缩下断续节理岩体动态损伤本构模型

doi: 10.11883/bzycj-2016-0261
基金项目: 

国家自然科学基金项目 41162009

详细信息
    作者简介:

    刘红岩(1975—), 男, 博士, 教授, lhyan1204@126.com

  • 中图分类号: O382.2;O319.56

A dynamic damage constitutive model for rockmass with intermittent joints under uniaxial compression

  • 摘要: 断续节理将对工程岩体的强度及变形等力学特性产生显著影响,损伤力学中视节理为岩体的一种宏观损伤,因而采用损伤张量来刻画其对岩体的影响。目前学术界提出了用节理的几何、强度及变形等3类参数来描述节理的物理力学性质,而目前的岩体损伤张量计算方法都只涉及前2类参数,均没有涉及其变形参数即法向及切向刚度。为此,在前人研究的基础上,基于断裂及损伤理论提出了考虑节理法向及切向刚度的单轴压缩下单条断续节理引起的损伤张量计算公式,进而通过考虑节理间相互作用给出了单组单排或多排节理岩体损伤张量计算公式。其次,以岩石细观动态损伤模型为基础,结合宏细观损伤耦合观点提出了一个能够同时考虑节理几何、强度及变形参数的断续节理岩体动态损伤本构模型。最后,利用该模型讨论了节理参数及载荷应变率等对岩体动态力学特性的影响,认为节理长度减小及摩擦角增大将导致岩体动态峰值强度及弹性模量增大;岩体动态峰值强度及弹性模量则随着节理法向及切向刚度的增大分别减小或增大;而当节理法向及切向刚度按照同一比例增大时,岩体动态峰值强度及弹性模量则是增大的。岩体动态峰值强度与载荷应变率呈正相关。
  • 图  1  翼裂纹扩展模型

    Figure  1.  A wing joint growth model

    图  2  含单排及多排断续节理的岩体模型

    Figure  2.  A model of the jointed rockmass with one or more rows of intermittent joints

    图  3  岩体模型

    Figure  3.  A model for rockmass

    图  4  岩体单轴压缩动态应力应变计算曲线

    Figure  4.  Calculated dynamic stress-strain curves of rockmass under axial compression

    图  5  不同节理摩擦角的试件动态应力应变曲线

    Figure  5.  Dynamic stress-strain curves of the samples with different joint friction angles

    图  6a  不同节理法向刚度试件的动态应力应变曲线

    Figure  6a.  Dynamic stress-strain curves of the samples with different joint normal stiffnesses

    6b  不同节理切向刚度试件的动态应力应变曲线

    6b.  Dynamic stress-strain curves of the samples with different joint shear stiffnesses

    6c  节理法向及切向刚度按相同比例变化时的试件动态应力应变曲线

    6c.  Dynamic stress-strain curves of the samples at the same joint normal-to-shear stiffnesses ratios

    图  7  节理长度对试件动态特性的影响

    Figure  7.  Effects of joint length on dynamic mechanical behaviors of the samples

    图  8  应变率对试件动态特性的影响

    Figure  8.  Effects of strain rate on dynamic mechanical behaviors of the samples

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  • 收稿日期:  2016-08-25
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