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连续排水边界下成层陆域吹填地基一维固结解析解

张云鹏 王宗琴 宗梦繁 吴文兵 王立兴

张云鹏, 王宗琴, 宗梦繁, 吴文兵, 王立兴. 连续排水边界下成层陆域吹填地基一维固结解析解[J]. 地质科技通报, 2023, 42(3): 38-45. doi: 10.19509/j.cnki.dzkq.2022.0171
引用本文: 张云鹏, 王宗琴, 宗梦繁, 吴文兵, 王立兴. 连续排水边界下成层陆域吹填地基一维固结解析解[J]. 地质科技通报, 2023, 42(3): 38-45. doi: 10.19509/j.cnki.dzkq.2022.0171
Zhang Yunpeng, Wang Zongqin, Zong Mengfan, Wu Wenbing, Wang Lixing. Analytical solution for one-dimensional consolidation in layered filled soil based on continuous boundary conditions[J]. Bulletin of Geological Science and Technology, 2023, 42(3): 38-45. doi: 10.19509/j.cnki.dzkq.2022.0171
Citation: Zhang Yunpeng, Wang Zongqin, Zong Mengfan, Wu Wenbing, Wang Lixing. Analytical solution for one-dimensional consolidation in layered filled soil based on continuous boundary conditions[J]. Bulletin of Geological Science and Technology, 2023, 42(3): 38-45. doi: 10.19509/j.cnki.dzkq.2022.0171

连续排水边界下成层陆域吹填地基一维固结解析解

doi: 10.19509/j.cnki.dzkq.2022.0171
基金项目: 

国家自然科学基金项目 52178371

浙江省杰出科学基金项目 LR21E080005

详细信息
    作者简介:

    张云鹏(1995—),男,现正攻读地质工程专业博士学位,主要从事土体固结理论与桩基动力学方面的研究工作。E-mail: zypsky@cug.edu.cn

    通讯作者:

    吴文兵(1988—),男,教授,博士生导师,主要从事土体固结理论与桩基动力学方面的研究与教学工作。E-mail:zjuwwb1126@163.com

  • 中图分类号: TU41

Analytical solution for one-dimensional consolidation in layered filled soil based on continuous boundary conditions

  • 摘要:

    新近吹填地基的固结效应十分显著,地基土内超静孔隙水压力的消散将引起地表的整体沉降,对吹填地基上基础工程的稳定性产生不利影响。基于连续排水边界,综合考虑吹填土的自重和下伏原状海床的成层特性,建立了吹填土自重驱动下的吹填地基-原状海床一维固结方程,并基于本征函数法推导了孔隙水压力响应、固结度等的解析解。通过边界条件和模型的退化,验证了解答的正确性。利用该解答讨论了吹填土自重、成层地基模量、时间因数、地表附加荷载等时空条件对吹填地基固结沉降的影响。研究结果表明:①吹填土自重是吹填地基固结的驱动因素,在实际工程中不可忽略;②土体渗透系数对超静孔隙水压力的影响较为复杂,某一层土的渗透性改变后,对其上覆和下伏土层的超静孔隙水压力将产生相反的影响;③土层的体积压缩系数对超静孔隙水压力的影响十分显著,且深部土体的体积压缩系数影响更大;④地表堆载等引起的附加荷载会减缓超静孔隙水压力的消散。

     

  • 图 1  首个填海造陆机场——大连金州湾国际机场[1]

    Figure 1.  First sea reclamation airport: Dalian Jinzhou Bay International Airport

    图 2  成层陆域吹填地基数学模型

    kvimvi分别为第i层土的渗透系数和体积压缩系数;Hhi分别表示地基总厚度和第i层土的厚度;zi为第i层地基距离土体表面的厚度;γ′为吹填土的有效重度;σ(x)为x处土体的有效应力分布;x为土体距离土体表面的深度

    Figure 2.  Mathematical model of layered soil in reclamation area

    图 3  连续排水边界退化后超静孔隙水压力和土体沉降曲线

    Figure 3.  Excess pore water pressure and soil settlement curve after degradation of continuous drainage boundary

    图 4  不同吹填土有效重度(γ′)的超静孔隙水压力(a)和土体沉降(b)曲线(α, a, b均为无量纲参数; q为均布荷载;γ′为有效重度;Tv为时间因数;图 5

    Figure 4.  Influence of effective weight of filled soil: excess pore water pressure (a) and soil settlement (b)

    图 5  不同吹填土厚度(h1)的超静孔隙水压力(a)和土体沉降(b)曲线

    Figure 5.  Influence of height of filled soil: excess pore water pressure (a) and soil settlement (b)

    图 6  不同渗透系数(kvi)时超静孔隙水压力曲线

    Figure 6.  Influence of permeability on excess pore water pressure

    图 7  不同渗透系数(kvi)和时间因数(Tv)时超静孔隙水压力曲线

    Figure 7.  Influence of permeability and time factor on excess pore water pressure

    图 8  不同压缩系数(mvi)时超静孔隙水压力曲线

    Figure 8.  Influence of compressibility on excess water pressure

    图 9  不同时间因数(Tv)时超静孔隙水压力曲线

    Figure 9.  Influence of surcharge loads on excess pore water pressure

    图 10  不同界面参数(α)时平均固结度(Us)曲线

    Figure 10.  Influence of interface parameters on average degree of consolidation

    图 11  不同均布荷载(q0)下超静孔隙水压力曲线

    Figure 11.  Influence of surcharge loads on excess pore water pressure

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