共查询到18条相似文献，搜索用时 140 毫秒
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基于ABAQUS有限元软件平台,应用流固耦合两相介质动力模型孔压单元模拟场地饱和土体,进行了饱和土体-地下结构地震反应的计算研究。结果表明：在地震输入的最后时刻结构的两侧底角区域应力值最大;土体的孔隙压力和竖向位移主要集中在结构下方的区域,结构两侧土体的孔压与竖向位移呈对称分布;场地土体的竖向位移随深度的增加逐渐减小;体系最大地震反应出现的时刻对应于输入地震动的最大加速度出现的时刻。表明了流固耦合两相介质动力模型孔压单元在饱和土体-地下结构体系地震反应研究中的有效性。 相似文献
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二维饱和孔隙介质的三场有限元方法 总被引：1，自引：0，他引：1
根据流固两相混合物连续介质力学理论,采用伽辽金加权残值法,选取固相位移,液相位移,孔隙不压作为场变量,对固液两相耦联方程进行有限元离散化,得到解耦方程组。然后在时域上采用Ｗｉｓｏｎ－θ进行了逐步积分,得到一种分析二维饱和孔隙介质地震反应的三场有限元方法。 相似文献
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文中对含两种不相混流体的饱和孔隙介质模型进行了波场模拟,该模型基于封闭型系统假设,考虑了流相与固相的相对运动和孔隙率、饱和度(毛细管压力)的松弛机制,可以较好的模拟波场的数值衰减。与目前常用的等效流体方法和基于开敞系统假设的非饱和孔隙介质模型相比,更符合勘探阶段的实际情况。前人对该介质模型平面波的速度和衰减做了一定的研究,但对整个波场的计算研究还未见报道。本文推导了该模型包含毛细管压力和孔隙度松弛机制的波动方程,并利用有限元的方法进行了波场模拟,并对波场特征进行了分析。数值模拟结果表明,在地震频段,非湿相位移波场中慢波p3较为清晰;毛细管压力(饱和度)和孔隙度的松弛效应对非湿相流体位移有较大影响,随松弛系数的增大,位移减小。 相似文献
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层状饱水软土地基三维非轴对称动力响应分析方法 总被引：1，自引：0，他引：1
将饱水软土地基视为两相介质、考虑水的渗流和土骨架9变形的耦合作用，用Fourier展开和Hankel积分变换分析三维非称对称饱和弹性土层波动方程，用刚度矩阵方法，建立了层状饱和软土地基三维非轴对称动力响应的解析分析方法。以数值算例对比分析了单相土介质与两相饱和土介质三维非轴对称稳态动力响应，结果表明：在饱水软土地基动力响应分析中应该考虑土体中孔隙流体的影响。 相似文献
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为探究孔隙尺寸效应(非局部参数表征)和介质局部非均匀效应(尺寸因子表征)对饱和土地基动力响应的影响,基于应变梯度非局部Biot理论,采用无网格法编制循环荷载下饱和土地基动力响应计算程序,验证无网格法程序的正确性。结果表明,尺寸因子为定值时,随着非局部参数的增加,观测点位移及孔压起始响应的时间有所延迟;而非局部参数为定值时,随尺寸因子的增加,观测点位移及孔压起始响应时间有所提前;说明考虑孔隙尺寸效应会减小系统的宏观模量,而考虑土体结构的非均匀效应则会增加系统的宏观模量。研究提出采用无网格法求解饱和土动力问题的方法和思路,可为今后研究饱和土动力学问题的研究提供借鉴。 相似文献
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非均匀介质孔隙流体参数地震散射波反演 总被引：2，自引：0，他引：2
印兴耀 《中国科学:地球科学》2013,(12):1934-1942
弹性波逆散射是非均匀介质参数反演的有效途径．本文从弹性波逆散射理论出发,利用微扰理论和稳相法,将非均匀介质参数视为背景介质与扰动介质参数的叠加,建立了纵波散射系数和非均匀介质中背景介质与扰动介质孔隙流体参数,剪切模量与密度间的直接关系．进而发展了一种非均匀介质孔隙流体参数叠前地震贝叶斯反演方法．该方法假设模型参数（扰动介质与背景介质孔隙流体参数,剪切模量与密度的比值）服从柯西分布,反演目标似然函数服从高斯分布,并采用平滑初始模型约束提高反演稳定性．模型和实际资料处理表明,该反演方法能够稳定合理的直接从叠前地震资料中获取孔隙流体参数,提供了一种高可靠性的非均匀介质流体描述方法． 相似文献
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水库诱发地震活动与水的渗透有密切关系,本文认为水库诱发地震中,前震活动主要是由于水的渗透引起孔隙压力扩散,岩石强度弱化所致。由于水库区地下岩石渗透性质的复杂性,将库区岩石介质分为均匀、非均匀渗透的两种情况,利用两相(固、液)多孔介质中孔隙压力扩散理论,分别对水库蓄水所引起的孔隙压力场进行了数值模拟计算,计算结果表明,非均匀渗透模型中水渗透所形成的孔隙压力分布与水库地震发生的空间位置对应得较好,孔隙压力峰值扩散到水库诱发地震的前震震源处的时间(1.8天～45天)与水库蓄水后引起前震活动的滞后时间大体一致。 相似文献
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强地震作用下,饱和土体将进入非线性,有必要考虑非线性饱和土的地震响应以及非线性饱和土-结构相互作用问题。本文采用Biot饱和多孔介质模型,基于不规则加卸载准则的修正Davidenkov模型来描述近场区域内饱和土骨架的非线性特性,并采用集中质量显式有限元方法进行分析;远场区介质假定为线弹性饱和多孔介质,通过多次透射人工边界进行模拟;结构采用Newmark隐式时步积分方法进行分析。通过自编程序实现了非线性饱和土体的地震反应分析以及非线性饱和土-基础-结构相互作用分析。通过算例,对比分析了土体非线性对饱和土体、基础和结构反应的影响。 相似文献
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考虑水-饱和土场地-结构耦合时的沉管隧道地震反应分析 总被引：6，自引：0，他引：6
用理想流体介质模拟水层、流体饱和多孔介质模拟饱和土地层,在理想流体介质与流体饱和多孔介质相连接边界的连续条件基础上,结合已有的对理想流体介质、流体饱和多孔介质进行动力反应分析的显式有限元方法,开考虑地层与结构的动力相互作用,建立了进行水与场地、结构耦合动力分析的方法。利用该方法对沉管隧道的地震响应进行了研究,重点分析了水深、地质条件等因素对沉管隧道地震反应的影响,并从中得出了一些可供相关人员进行沉管隧道抗震分析时参考的结论。 相似文献
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Chen Guoxing Zhou Enquan Wang Zhihua Wang Binghui Li Xiaojun 《Bulletin of Earthquake Engineering》2016,14(8):2185-2212
Liquefaction of saturated loose sand is a major cause of extensive damage to buildings and infrastructures during large earthquakes. A better understanding of the behaviour of liquefied soil is becoming increasingly necessary to mitigate earthquake damage, and the fluid method has become an increasingly popular means to study the behaviour of liquefied soils. The purpose of this study is to determine the fluid characteristics of liquefied fine sand. In this paper, the apparent viscosity was measured as an index of fluid characteristics using the shaking table tests of pre-liquefaction behaviour of saturated fine sand at approximately 45 % relative density; the relationship of apparent viscosity and shear strain rate on liquefying fine sand was indicated as a power-law shear-thinning non-Newtonian fluid; and liquefying fine sand has the alternating behaviour of shear dilatancy and compressibility during cyclic loading. Additionally, a series of a monotonic axial compression loading tests in an undrained manner were performed to measure the shear stress and excess pore pressure ratio relationship on the post-liquefaction saturated fine sand at approximately 50 % relative density. The fluid characteristics of post-liquefaction fine sand exhibits rate dependence and can be described by a combined fluid model of time-independent and time-dependent power-law functions; the time-independent viscous resistance is not relevant to the excess pore pressure ratio; but the time-dependent frictional resistance is closely related to the excess pore pressure ratio. Furthermore, the results of the verification tests demonstrate that the proposed fluid model has good applicability for the fluid behaviour of the post-liquefaction fine sand. 相似文献
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LNAPL Distribution in a Cohesionless Soil: A Field Investigation and Cryogenic Sampler 总被引：1，自引：0，他引：1
D. Durnford J. Brookman J. Billica J. Milligan 《Ground Water Monitoring & Remediation》1991,11(3):115-122
Lighter-than-water Non-Aqueous Phase Liquids (LNAPLs), such as jet fuels or gasolines, are common contaminants of soils and ground water. However, the total volume and distribution of an LNAPL is difficult to accurately determine during a site investigation. LNAPL that is entrapped in the saturated zone due to fluctuating water table conditions is particularly difficult to quantify. Yet, the amount of entrapped product in the saturated zone is theoretically higher, per volume of soil, than the residual product in the unsaturated zone, and small amounts of LNAPL in the saturated zone can contaminate large volumes of ground water.
The only method currently available to quantify the amount of LNAPL is direct soil-core sampling combined with laboratory analysis of the fluid extracted from the soil cores. However, direct sampling of saturated ground water systems with conventional samplers presents a number of problems. In this study, a new sampler was developed that can be used to retrieve undisturbed soil and pore fluid samples from below the water table in cohesionless soils. The sampler uses carbon dioxide to cool the bottom of a saturated soil sample in situ to near freezing. Results of a field study where a prototype sampler was tested demonstrate the usefulness of a cryogenic sampler and show that the amount of LNAPL entrapped below the water table can be a significant part of the total LNAPL in the soil. 相似文献
The only method currently available to quantify the amount of LNAPL is direct soil-core sampling combined with laboratory analysis of the fluid extracted from the soil cores. However, direct sampling of saturated ground water systems with conventional samplers presents a number of problems. In this study, a new sampler was developed that can be used to retrieve undisturbed soil and pore fluid samples from below the water table in cohesionless soils. The sampler uses carbon dioxide to cool the bottom of a saturated soil sample in situ to near freezing. Results of a field study where a prototype sampler was tested demonstrate the usefulness of a cryogenic sampler and show that the amount of LNAPL entrapped below the water table can be a significant part of the total LNAPL in the soil. 相似文献
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基于孔隙介质的Biot理论,首先利用Laplace变换,给出圆柱坐标系下横观各向同性饱和弹性多孔介质在变换域上的波动方程;将波动方程解耦后,根据方位角的Fourier展开和径向Hankel变换,求解了Biot波动方程,得到以土骨架位移、孔隙水压力和土介质总应力分量的积分形式的一般解;借助一般解,建立了有限厚度饱和土层和饱和半空间的精确动力刚度矩阵,并由土层的层间界面连续条件建立三维非轴对称层状饱和地基的总刚度方程;在此基础上,系统研究了横观各向同性饱和半空间体在内部集中荷载激励下的动力响应,并给出了问题的瞬态解答.该研究为运用边界元法求解饱和地基动力响应奠定了理论基础. 相似文献
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In this paper, a novel coupled pore-scale model of pore-fluid interacting with discrete particles is presented for modeling liquefaction of saturated granular soil. A microscale idealization of the solid phase is achieved using the discrete element method (DEM) while the fluid phase is modeled at a pore-scale using the lattice Boltzmann method (LBM). The fluid forces applied on the particles are calculated based on the momentum exchange between the fluid and particles. The presented model is based on a first principles formulation in which pore-pressure develops due to actual changes in pore space as particles׳ rearrangement occurs during shaking. The proposed approach is used to model the response of a saturated soil deposit subjected to low and large amplitude seismic excitations. Results of conducted simulations show that at low amplitude shaking, the input motion propagates following the theory of wave propagation in elastic solids. The deposit response to the strong input motion indicates that liquefaction took place and it was due to reduction in void space during shaking that led to buildup in pore-fluid pressure. Soil liquefaction was associated with soil stiffness degradation and significant loss of interparticle contacts. Simulation results also indicate that the level of shaking-induced shear strains and associated volumetric strains play a major role in the onset of liquefaction and the rate of pore-pressure buildup. 相似文献
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The transient dynamic response of saturated soil under suddenly applied normal and horizontal concentrated loading is studied in this paper. The behavior of saturated soil is governed by Biot's consolidation theory. The general solutions for Biot equations of equilibrium are derived in terms of displacements and variations of fluid volume, using Laplace–Hankel integral transforms. The solutions in the time domain can be evaluated by numerical inverse Laplace–Hankel transforms. Selected numerical results for displacements, stresses, and pore pressures are presented. Comparisons with existing closed-form solutions for the elastic half-space are made to confirm the accuracy of the present solutions. The solutions can be used to study a variety of transient wave propagation problems and dynamical interactions between saturated soil and structures. 相似文献