散体材料中应力传递的细观机制分析

    Meso-mechanism for stress transition within granular assemblies

    • 摘要: 基于离散单元法,对不同密实度的散体试样开展了双轴压缩试验的数值模拟,以细观loop结构作为基本单元,探讨了剪切过程中散粒体内部的应力承载特征与传递机制。通过以平均应力为指标划分强/弱结构loop单元,分析其结构重组与应力响应的演化规律。结果表明,不同密实度试样在剪切过程中,loop单元均呈现出应变硬化/软化行为,并逐步演化至各自的细观临界状态。强结构loop倾向沿加载方向取向,形成细长结构链以主导偏应力传递;弱结构loop也沿加载方向取向,但其聚集成块状填充于强结构链空隙中,起到辅助支撑的作用。此外,散粒体强/弱结构更倾向于重组为各向异性较强的高阶6+-cycle单元,且宏观应力水平越高,细观组构各向异性对试样整体贡献越强。在临界状态下,不同初始密实度散粒体内部细观结构趋向于重组成具有相同数量、几何和力学水平的拓扑构型,以此来承载和传递同一围压下的临界常应力,在宏观尺度上表现为临界状态的唯一性。

       

      Abstract: Numerical simulations of biaxial compression tests were conducted on granular specimens with different initial densities using the discrete element method. The meso-loops formed by contacting particles were identified as fundamental structure to analyze the characteristics of stress-bearing and transmission during shear. Based on average stress, meso-loops were divided into strong and weak structures, and their structural reorganization and stress response evolution were analyzed. Numerical results show that the strain hardening/softening and unique meso critical stress state are also observed for different loop types in granular assemblies with different densities under shearing. Strong loops tend to be oriented in the loading direction, forming elongated chains that dominate deviatoric stress transmission. In contrast, weak loops also orient in the loading direction but aggregate into blocky clusters that fill voids between strong chains, providing auxiliary support. Moreover, both strong and weak structures tend to reorganize into highly anisotropic high-order 6+-cycle units, with greater macroscopic stress levels corresponding to stronger contributions of structural anisotropy. At the critical state, granular assemblies with different initial densities evolve toward topologically identical configurations in terms of quantity, geometry, and mechanical levels, thereby supporting and transmitting a unique critical stress under the same confining pressure. This reveals the structural uniqueness of the critical state at the macroscopic scale.

       

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