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基于元胞自动机的开裂混凝土氯离子扩散模拟与分析

马俊军 蔺鹏臻 刘应龙 何志刚

马俊军, 蔺鹏臻, 刘应龙, 何志刚. 基于元胞自动机的开裂混凝土氯离子扩散模拟与分析[J]. 西南交通大学学报, 2022, 57(2): 360-368. doi: 10.3969/j.issn.0258-2724.20210359
引用本文: 马俊军, 蔺鹏臻, 刘应龙, 何志刚. 基于元胞自动机的开裂混凝土氯离子扩散模拟与分析[J]. 西南交通大学学报, 2022, 57(2): 360-368. doi: 10.3969/j.issn.0258-2724.20210359
MA Junjun, LIN Pengzhen, LIU Yinglong, HE Zhigang. Simulation and Analysis of Chloride Ion Diffusion in Cracked Concrete Based on Cellular Automata[J]. Journal of Southwest Jiaotong University, 2022, 57(2): 360-368. doi: 10.3969/j.issn.0258-2724.20210359
Citation: MA Junjun, LIN Pengzhen, LIU Yinglong, HE Zhigang. Simulation and Analysis of Chloride Ion Diffusion in Cracked Concrete Based on Cellular Automata[J]. Journal of Southwest Jiaotong University, 2022, 57(2): 360-368. doi: 10.3969/j.issn.0258-2724.20210359

基于元胞自动机的开裂混凝土氯离子扩散模拟与分析

doi: 10.3969/j.issn.0258-2724.20210359
基金项目: 国家自然科学基金(U1934205,51878323);甘肃省建设科技攻关项目(JK2021-03);甘肃省教育科技创新项目(2021CXZX-568);甘肃省教育厅青年博士基金(2021QB-056)
详细信息
    作者简介:

    马俊军(1994—), 男, 博士研究生, 研究方向为桥梁结构设计理论及耐久性, E-mail:majjlz@163.com

    通讯作者:

    蔺鹏臻(1977—), 男, 教授, 博士, 博导, 研究方向为桥梁结构设计理论及耐久性研究, E-mail:pzhlin@mail.lzjtu.cn

  • 中图分类号: TU528

Simulation and Analysis of Chloride Ion Diffusion in Cracked Concrete Based on Cellular Automata

  • 摘要:

    为获得氯离子在开裂混凝土中的浓度分布以及分析裂缝形状、分布形式、偏转角度对混凝土中氯离子扩散效应的影响,根据氯离子在开裂混凝土中的扩散机理,利用元胞自动机和均匀化等效分析方法,建立了模拟开裂混凝土中氯离子扩散过程的元胞自动机模型,并利用数值试验对模型中元胞尺寸进行了优化. 研究结果表明:在不影响计算精度的情况下,为提高模型的计算效率,推荐采用元胞尺寸大小为0.5 mm;除个别数据外,模型模拟结果、试验结果与有限元分析结果吻合良好,最大偏差不超过10%;“V”形裂缝中氯离子浓度约为矩形裂缝的0.52倍;曲线形裂缝和折线形裂缝中氯离子浓度约为直线形裂缝的0.87倍和0.89倍;当裂缝偏转角从0° 分别增大至10°、20°、30° 时,裂缝端部氯离子浓度分别减小3.3%、21.9%、29.8%;裂缝对其周围氯离子扩散区域的影响范围与裂缝形状、分布形式和偏转角度无关,对裂缝周围氯离子扩散效应的影响主要集中在裂缝左右18 mm的范围内.

     

  • 图 1  元胞组合示意

    Figure 1.  Diagram of schematic of cellular assemblage

    图 2  氯离子扩散系数等效示意

    Figure 2.  Diagram of equivalent chlorine ion diffusion coefficient

    图 3  氯离子浓度随扩散深度的变化规律

    Figure 3.  Variation law of chloride ion concentration with diffusion depth

    图 4  利用CA模型获得的截面氯离子浓度分布结果

    Figure 4.  Chloride concentration distribution in section simulated by CA model

    图 5  利用有限元法模拟的截面氯离子浓度分布结果

    Figure 5.  Chloride concentration distribution in the cross section simulated by finite element method

    图 6  模型模拟结果与有限元解和试验值的比较

    Figure 6.  Comparison of model simulation results with element solutions and experimental values

    图 7  模型模拟值与有限元解和试验值的比较

    Figure 7.  Comparison of model simulation values with finite element solutions and experimental values

    图 8  不同裂缝形状下截面氯离子浓度模拟结果

    Figure 8.  Simulation results of chloride ion concentration in section under different crack shapes

    图 9  截面氯离子浓度沿截面宽度的变化规律

    Figure 9.  Variation law of chloride ion concentration in cross section with cross section width

    图 10  裂缝中心截面氯离子浓度随扩散深度的变化

    Figure 10.  Variation law of chloride ion concentration in central section of crack with diffusion depth

    图 11  不同裂缝分布形式下截面氯离子浓度模拟结果

    Figure 11.  Simulation results of chloride ion concentration in cross section under different crack distribution forms

    图 12  截面氯离子浓度沿截面宽度的变化

    Figure 12.  Variation law of chloride ion concentration in cross section with cross section width

    图 13  裂缝中心截面氯离子浓度随扩散深度的变化

    Figure 13.  Variation law of chloride ion concentration in central section of crack with diffusion depth

    图 14  不同裂缝偏转角下截面氯离子浓度模拟结果

    Figure 14.  Simulation results of chloride ion concentration in cross section under different fracture deflection angles

    图 15  截面氯离子浓度沿截面宽度的变化

    Figure 15.  Variation law of chloride ion concentration in cross section with cross section width

    图 16  裂缝端部截面氯离子浓度随扩散深度的变化

    Figure 16.  Variation law of chloride ion concentration in section of fracture end with diffusion depth

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出版历程
  • 收稿日期:  2021-05-06
  • 录用日期:  2021-12-27
  • 修回日期:  2021-10-29
  • 刊出日期:  2021-11-18

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