模糊识别模式在粉土液化判别中的应用

基于模糊数学的基本原理和方法,分析了粉土液化的影响因素,选取粉土的平均粒径,相对密度,标准贯入击数和上覆有效压力作为评价指标,构造粉土液化的模糊识别模式。验证和应用结果表明,模糊识别模式具有很好的映射能力,是粉土液化势预测的有效手段。     

饱和土蠕(滑)动液化的研究

本文在文献[1],[2]的基础上对黄土区饱和土蠕动及滑动液化作了进一步研究。文中首先列举了黄土滑坡现场饱和土液化的一些典型实例及其所造成的宏观危害。从不同的角度提出了饱和土蠕(滑)动液化的定义,在大量现场及室内试验的基础上分析了饱和土蠕(滑)动液化的机理和影响因素,最后给出了液化势的评价方法。     

天津地区饱和粉土地震液化的试验研究

地震液化是导致地基失稳和上部结构受损的直接原因之一。通过对天津地区粉土进行原位取土以及现场原位测试分析,研究了粉土土质特点对液化判别的影响,并在动三轴试验基础上阐述了该区域粉土的动力特性和液化机制。结合原位测试方法比较了现有的地震液化判别方法,指出该区域粉土液化判别应考虑粉土成分特征的影响,并提出孔压达到围压的60%～90%,双幅应变达到4%可作为液化的判别标准。     

饱和粉土振动液化分析

液化是造成场地地震破坏的首要原因之一。自Casagrande的经典工作以来,对地震液化的研究已经取得了很大的进展。然而这些研究大多是针对于砂土而进行的,对于粉土液化研究的相对较少,且粉土的液化特性也有别于砂土。因此,在已有研究的基础之上利用粉土液化试验得出的结果,分析了粉土液化的机理、影响因素以及在振动过程中粉土中孔隙水压力的增长规律,认为粉土中的粘粒含量、密实度以及土的结构性对其抗液化能力有较大的影响。考虑到试验中振动次数的离散性,引入了时间参数的概念,根据动三轴试验结果提出了孔隙水压力增长的经验公式,可以比较方便地应用于计算液化的有限元程序中去。     

砂土液化内部应力变化规律与工程液化判别

以往对砂土液化的研究主要侧重于水平场地、自由应力场条件下有关地基液化机理与判别等问题的研究。通常将Δu=σz=ΔUmax作为地基土液化的判据，而对工程结构物和场地条件的影响考虑不足。基于当前砂土液化问题的研究现状及工程特性，提出了将液化分为理论液化和工程液化。前者主要研究地基土液化的一般规律性问题；后者则针对具体工程结构物而言。其液化标准是以地基土在遭受地震液化时是否会导致工程结构物的破坏为依据。通过对砂土在震动液化过程中内部应力变化规律的理论分析，阐明了水平应力σx或σy对斜坡场地地基土发生侧向液化的作用机理，不能将斜坡场地的地基看作半无限空间体处理，提出了液化膨胀侧扩势Ψ的概念与计算式。指出：对斜坡场地，为避免这种侧向液化流动变形破坏，采取加强可液化土体的侧向约束、缩小偏应力差是必要的。根据工程结构物的承载力极限状态和正常使用极限状态，提出工程液化的判别准则：(1)可液化土体的地基强度τ降低到工程结构物所允许的强度值[τ，]；(2)可液化土体的膨胀侧扩势Ψ增加到其侧向约束强度[τh]；(3)可液化土体地基的变形s增大到工程结构物所允许的变形值[s]。     

文克尔地基模型下液化土桩基水平振动响应分析

在桩基顶部承受竖向荷载作用的条件下,将完全液化后的上层土体视为流体,将桩基等效为欧拉-伯努利梁模型,探讨了桩底嵌固时桩基顶部的水平振动阻抗。运用流体动力方程模拟顶部液化土层的运动,运用文克尔地基模拟下部非液化分层土的运动。结合传递矩阵法,利用液化土与非液化分层土交界面处的位移、转角和内力连续条件,得到桩基顶部和底部的相关位移?内力表达关系式。根据桩基底部的嵌固条件,求得桩顶阻抗的表达式。与已有文献解进行对比,验证了分析过程的正确性。对阻抗影响条件进行参数分析,表明液化深度、轴力和流体密度大小对桩顶阻抗有不同的影响。     

液化地基中桩的破坏机理研究进展

地震诱发的地基液化对桩基础的破坏极大,液化地基中桩的破坏机理是岩土地震工程中的一个重要研究课题。目前地基液化时桩土结构系统的地震性态尚没有认识充分,已有的研究内容较多局限于桩身材料的强度破坏方面,难以考虑液化土体侧向流动、基桩屈曲失稳、以及土与结构动力相互作用等复杂因素的影响。本文重点加强以下3个方面的深入探讨和研究:(1)液化地基中桩的屈曲失稳;(2)液化地基中桩基破坏的数值模拟新方法;(3)液化地基中桩-土-结构的动力相互作用分析。     

饱和粉土液化后变形特性试验研究

利用多功能静动液压剪切三轴仪,进行了一系列饱和粉土液化后变形特性试验,研究了干密度和液化程度对粉土液化后变形特性的影响,并考虑试验动加载前小幅预振和不规则动加载对粉土液化后变形特性的影响。试验结果表明,液化后变形可由两段应变 和 组成。干密度越小, 越大, 段剪切模量越低;液化越严重 越大,不同液化程度对 段剪切模量影响很小;动加载前小幅预振和不规则动加载对液化后变形影响较小。提出了饱和粉土液化后变形模型,给出了模型参数的推导。验证结果表明,该模型的计算值与试验值吻合较好,说明该模型能很好地描述这种变形行为。     

饱和粉土静态液化性能试验研究

通过固结不排水三轴压缩试验,分析了围压、固结比和干密度等因素对饱和粉土静态液化特性的影响。试验结果表明,在干密度较小时,饱和粉土的偏应力-应变曲线呈现明显的硬变软化型,随轴向应变增大超静孔隙水压力增加、有效应力减小而发生静态液化,当干密度达到1.58 g· cm-3时,饱和粉土的偏应力-应变曲线表现出硬变硬化现象,超静孔隙水压力为负值或接近0,饱和粉土不再发生静态液化,即饱和粉土存在静态液化的干密度临界值;其他条件不变,随着围压、固结比或干密度的增大,偏应力峰值和残余强度均增大,静态液化势降低;根据有效应力路径建立了流滑面以作为饱和粉土稳定区与非稳定区的分界面。     

饱和砂土液化后大变形机理的离散元细观分析

采用颗粒流软件模拟了饱和砂土在不排水条件下的循环剪切试验,研究了不同因素对液化的影响,并进一步分析了饱和砂土液化后宏观变形的基本规律。在此基础上,从孔隙分布角度解释了砂土液化后的大变形的细观物理机制。通过自编程序对颗粒排列和孔隙分布的演化过程进行定量描述,给出孔隙率标准差作为液化后体积收缩势的度量,并研究了孔隙率标准差与液化后大变形的关系。结果表明,试样初始状态并不会影响液化后的极限状态,仅对初始液化所需循环次数有影响。数值模拟可再现室内试验中的宏观现象,证实了室内试验中饱和砂土液化后的有限剪切大变形是客观真实的材料响应。土体体积收缩势的累积所导致的孔隙均匀化以及土颗粒间自由空隙增大正是饱和砂土液化后循环剪应变逐渐增大的细观机理。孔隙率标准差作为孔隙均匀化的量化指标,与循环剪应变各周次幅值有良好相关性。     

Prediction of cyclic resistance ratio for silty sands and its applications in the simplified liquefaction analysis

Liquefaction resistance of granular soils is commonly characterized by the cyclic resistance ratio (CRR) in the simplified shear stress procedure of liquefaction potential assessment. This parameter is commonly estimated by cyclic tests on reconstituted samples or empirical correlations between liquefied/non-liquefied case histories. The current study employs results of cyclic triaxial tests on reconstituted soil specimens and presents a predictive equation for cyclic resistance ratio (CRR) of clean and silty sands. The CRR equation is a function of relative density, effective mean confining pressure, non-plastic fines content, number of harmonic cycles for liquefaction onset, and some other basic soil properties. It is demonstrated that the developed relationship obtains reasonable accuracy in the prediction of laboratory-based CRR. Based on the developed CRR model, new relationships are then presented for the coefficient of effective overburden pressure (K_σ) and magnitude scaling factor (MSF), two important modification factors in the simplified shear stress procedure. These new modification factors are then compared with those recommended by previous researchers. Finally, the possible application of the proposed CRR model in field condition is shown for a specific case. This study provides a preliminary insight into the liquefaction resistance of silty sands prior to the complementary laboratory studies.     

非线性波浪荷载作用下海上风机管桩基础周围海床液化研究

为研究近浅海领域内海上风机大直径单桩基础周围的砂质海床在非线性荷载作用下的瞬时液化的稳定性,在OpenFOAM平台上建立波浪-单桩-海床三维数值模型(WSSI模型),采用olaFoam求解器求解RANS方程模拟波浪的非线性运动,将Biot方程作为海床模型的控制方程研究单桩周围海床的液化规律。对以往的数值解析结果和实验结果进行对比分析,验证本文建立三维波浪模型和海床模型的准确性和有效性。将建立的波浪-管桩-海床相互作用三维数值模型应用到实际工况中,对数值模型在实际工程中的海床响应进行分析评估。研究结果表明,单桩周围海床的孔隙水压力场和有效应力场在水深方向发生较大变化,在水平方向变化较小。在该工况下海床的最大液化深度可达到10 m,且在垂直于波浪运动方向的海床更容易发生液化,为实际工程预测海床液化提供一定的技术支持。     

论砂土液化深度的Gan-Chen模式计算法

地震引起地基土层中的砂土液化，其临界液化深度是多少?世界岩土工程界进行了大量的实际资料分析和试验研究，至今众说纷纭。笔者在综合分析各国专家研究成果时，从中发现地震引起砂土液化的普遍自然规律，并建立起Gan—chen模式，可简易计算砂土液化的临界深度在5～12m范围内。     

剪切波速测试技术及场地土液化势判别

文章简要地介绍了剪切波测试技术的基本原理、野外测试方法及其在工程中的主要用途.结合工程实例,对于在资料处理中碰到的场地液化势判别的问题,采用石兆吉判别式,丁伯阳判别式,谢生荪判别式及标准贯入试验法等目前运用较多的多种液化判别方法进行对比分析,最后得出在本次工程中石兆吉判别式结果最切合本次工程,其结果予以采用,并且就液化判别问题提出了一些建议.     

Reliability analysis of soil liquefaction based on standard penetration test

A review of probabilistic and deterministic liquefaction evaluation procedures reveals that there is a need for a comprehensive approach that accounts for different sources of uncertainty in liquefaction evaluations. For the same set of input parameters, different models provide different factors of safety and/or probabilities of liquefaction. To account for the different uncertainties, including both the model and measurement uncertainties, reliability analysis is necessary. This paper presents a review and comparative study of such reliability approaches that can be used to obtain the probability of liquefaction and the corresponding factor of safety. Using a simplified deterministic Seed method, this reliability analysis has been performed. The probability of liquefaction along with the corresponding factor of safety have been determined based on a first order second moment (FOSM) method, an advanced FOSM (Hasofer–Lind) reliability method, a point estimation method (PEM) and a Monte Carlo simulation (MCS) method. A combined method that uses both FOSM and PEM is presented and found to be simple and reliable for liquefaction analysis. Based on the FOSM reliability approach, the minimum safety factor value to be adopted for soil liquefaction analysis (depending on the variability of soil resistance, shear stress parameters and acceptable risk) has been studied and a new design safety factor based on a reliability approach is proposed.     

颗粒物质在等比例应变加载下的分散性失稳模式

由地下水引起的静力液化可能是边坡失稳的隐含机制之一,松砂在不排水剪切条件下可能发生静力液化,密实的颗粒集合体在特定的应变路径下也会出现相似的现象,即试样整体发生急剧的失稳,应力状态尚处于峰值强度线以内。该种失稳模式称为分散性失稳,是为了强调失稳模式中没有出现应变局部化或者剪切带。采用连续-离散耦合分析方法,研究由不规则形状颗粒组成的密实集合体在等比例应变加载路径下的力学特性。根据Hill的材料失稳理论,当试样的应力增量 和应变增量 对应的2阶功 为负时,试样即发生不可逆的整体失稳破坏。以根据不同等比例应变路径得到 曲线为界,在 平面内将试样的应力状态分为剪缩区、剪胀-稳定区和剪胀-非稳定区,连接不同围压下试样发生分散性失稳时的应力状态形成失稳线发现,峰值强度线高于临界状态线,临界状态线高于失稳线。     

以剪切波速与地表峰值加速度为依据的地震液化确定性及概率判别法

剪切波速作为土性的基本参数,为评价土体抵抗地震液化的能力提供了一种方法。回顾了以剪切波速和地表峰值加速度为依据的场地地震液化判别方法的演化历史,依据他人收集的现场液化资料,合计49次地震、618例液化/不液化场地数据,提出了确定液化临界曲线的基本原则,给出了基于修正剪切波速与地表峰值加速度的液化临界曲线,验证了液化临界曲线的位置对细粒含量、有效上覆压力、震级等因素取值变化的合理性,分析了估计土层循环应力比CSR的剪应力折减系数、震级标定系数、有效上覆压力修正系数等因素的不确定性对液化临界曲线的敏感性。结果表明：液化临界曲线对各种影响因素具有很好的适用性。利用Monte Carlo模拟、加权最大似然法和加权经验概率法,给出了建议的液化临界曲线的名义抗液化安全系数与液化概率的经验关系式及概率等值线,并对核电厂Ⅰ类、Ⅱ类和Ⅲ类抗震物项地基,分别建议了相应的液化临界曲线。该方法以丰富的现场液化数据为依据,具有广泛的应用前景。     

考虑场地动应力条件的饱和海洋粉细砂液化特性

确保地震荷载作用下海床场地的动力稳定性是海洋工程全寿命周期安全运行的重要保证,然而对复杂海域环境下饱和粉细砂的液化特性研究尚属少见。基于海域场地动应力计算方法,确定各试验工况的场地循环应力比CSR,并对试样施加与之对应的不排水循环荷载。试验结果表明：可液化的海洋粉细砂在考虑其场地动应力条件的循环荷载作用下出现不同的液化可能性;粉细砂呈循环破坏模式,将双幅轴向应变>5%作为循环破坏标准;海洋粉细砂的液化可能性与土体的埋深及动应力均不呈单一相关性,而是随着干密度的增大,液化振次逐渐增大,当干密度＞1.72 g/cm3时土体不再液化。该结果可为杭州湾区抗震区划及海洋工程结构抗震设计提供参考。     

砂土地震液化的模糊概率评判方法

利用模糊数学中的模糊概率理论,建立了砂土地震液化的模糊概率综合评判模型。在此模型中,提出了模糊权重的概念,可充分考虑权重的模糊性,从而避免权重取值带来的不确定性。结合砂土地震液化特点,选取地震烈度、标准贯入击数、平均粒径和上覆有效压力作为主要评价影响因子,同时将液化程度划分为不液化、轻微液化、中等液化和严重液化4个等级,进而使其评判结果更为精细化。通过算例分析,表明文中方法对砂土液化评判的合理性与有效性。     

Dynamic liquefaction of shear zones in intact loess during simulated earthquake loading

The 2010–2011 Canterbury earthquake sequence in New Zealand exposed loess-mantled slopes in the area to very high levels of seismic excitation (locally measured as >2?g). Few loess slopes showed permanent local downslope deformation, and most of these showed only limited accumulated displacement. A series of innovative dynamic back-pressured shear box tests were undertaken on intact and remoulded loess samples collected from one of the recently active slopes replicating field conditions under different simplified horizontal seismic excitations. During each test, the strength reduction and excess pore water pressures generated were measured as the sample failed. Test results suggest that although dynamic liquefaction could have occurred, a key factor was likely to have been that the loess was largely unsaturated at the times of the large earthquake events. The failure of intact loess samples in the tests was complex and variable due to the highly variable geotechnical characteristics of the material. Some loess samples failed rapidly as a result of dynamic liquefaction as seismic excitation generated an increase in pore water pressure, triggering rapid loss of strength and, thus, of shear resistance. Following initial failure, pore pressure dissipated with continued seismic excitation and the sample consolidated, resulting in partial shear strength recovery. Once excess pore water pressures had dissipated, deformation continued in a critical effective stress state with no further change in volume. Remoulded and weaker samples, however, did not liquefy and instead immediately reduced in volume with an accompanying slower and more sustained increase in pore pressure as the sample consolidated. Thereafter, excess pressures dissipated and deformation continued at a critical state. The complex behaviour explained why, despite exceptionally strong ground shaking, there was only limited displacement and lack of run-out: dynamic liquefaction was unlikely to occur in the freely draining slopes. Dynamic liquefaction, however, remained a plausible mechanism to explain loess failure in some of the low-angle toe slopes, where a permanent water table was present in the loess.