共查询到18条相似文献，搜索用时 906 毫秒
1.
在工程荷载范围内,不计骨架颗粒的变形,骨架的变形实际是颗粒接触面变形的总和。当剪应力达到某个临界值时,黏性土骨架中有一部分颗粒接触面开始滑动,随着剪应力的增大,出现滑动的颗粒接触面的取向范围也会扩大。将这种颗粒接触面的滑动视为一种损伤。在损伤阶段,黏性土骨架中既有未滑动的接触面,也有已滑动的接触面,宏观剪切模量是这两种接触面的剪切模量的加权平均。在 平面中,根据应力圆与颗粒起始滑动包络线的相对位置,计算出已出现了滑动的颗粒接触面的取向范围,并定义该取向范围与其所能达到的最大值（由破坏时的应力圆计算）之比为骨架的损伤比。按损伤比进行加权平均得到骨架的整体剪切模量。模型中的参数完全可以根据常规三轴试验确定,模型的形式简单,可适用于复杂的应力路径。对试验结果的拟合表明,该模型能较好地反映黏性土在固结不排水条件下剪切变形的主要特征。 相似文献
2.
在工程荷载范围内,不计骨架颗粒的变形,骨架的变形实际是颗粒接触面变形的总和。当剪应力达到某个临界值时,黏性土骨架中有一部分颗粒接触面开始滑动,随着剪应力的增大,出现滑动的颗粒接触面的取向范围也会扩大。将这种颗粒接触面的滑动视为一种损伤。在损伤阶段,黏性土骨架中既有未滑动的接触面,也有已滑动的接触面,宏观剪切模量是这两种接触面的剪切模量的加权平均。在σ-τ平面中,根据应力圆与颗粒起始滑动包络线的相对位置,计算出已出现了滑动的颗粒接触面的取向范围,并定义该取向范围与其所能达到的最大值（由破坏时的应力圆计算）之比为骨架的损伤比。按损伤比进行加权平均得到骨架的整体剪切模量。模型中的参数完全可以根据常规三轴试验确定,模型的形式简单,可适用于复杂的应力路径。对试验结果的拟合表明,该模型能较好地反映黏性土在固结不排水条件下剪切变形的主要特征。 相似文献
3.
基于细观分析的黏土本构模型 总被引：1，自引：0，他引：1
根据黏性土在固结排水条件下的加、卸载变形特征,分析了孔隙水,固体骨架在不同变形阶段的力学响应行为,按照细观力学分析中的自洽方法,建立了在固结排水条件下的黏土损伤本构模型。模型中考虑了孔隙水和固体骨架在加、卸载阶段的不同特性,认为在损伤阶段整体剪切模量的降低是由固体骨架颗粒接触面滑移而引起,与骨架中滑动相的体积百分比和滑动相的剪切模量有关,并给出了求解整体变形模量的解析方法,最后将模型预测与不同初始固结压力,不同应力路径的排水试验结果作了比较,证明该模型是合理的。 相似文献
4.
将数字图像测量技术运用于三轴剪切蠕变试验,试验结果表明,土粒间水膜厚度对土的蠕变有很大的影响,不排水时,试样土颗粒间水膜保持不变,土的黏滞系数基本为一定值,土的流变变形较大;排水时,随着水的排出土体发生固结硬化,土颗粒间水膜变薄,土的密度增大,黏滞性增强,流变变形较小。在排水条件下,加载瞬间孔隙水压力会持续上升产生Manadei-Cryer效应,整个过程历时约10 min。随着偏应力水平的增加,试样发生鼓胀变形,进而形成剪切面发生剪切破坏;受排水路径的影响,剪切面通常位于试样偏下部位。对比数字图像测量方法和试样排水体积换算法在获得剪切应变时的试验结果,表明试验过程中试样变形的不均匀会导致排水体积换算法在计算剪切应变时产生较大误差;Singh-Mitchell模型很好地描述土的剪切流变特性,确定参数时两种方法得到的参数相差不大,偏应力水平较低时可采用排水量换算法进行确定。 相似文献
5.
结构性土颗粒间的胶结使试样剪切破坏最终应力比高于相应重塑土,也限制了试样剪切时体积应变的自由发挥。在考虑结构垮塌为主的结构性土统一硬化(UH)模型基础上,将应力空间中静止的临界状态线扩展为动态的移动临界状态线。据此,通过建立新的屈服面方程并修正剪胀方程,将结构性土统一硬化(UH)模型扩展为胶结结构性土统一硬化(UH)模型。相对于原模型,新模型增加了1个模型参数,即初始胶结应力,反映土颗粒之间的初始胶结作用。通过4种结构性土试验数据与模型预测对照表明：所提模型能够较合理地描述结构性土等向压缩、常规三轴排水与不排水剪切等特性。 相似文献
6.
《岩土力学》2020,(6)
研究结构性黏土在不同应力路径下的微观结构变化可深入了解K_0固结下结构性黏土结构性特性变化的内在机制。在对衡水地区天然黏土进行不同应力路径条件下三轴剪切试验的基础上,利用微观定量化技术,对比不同应力路径条件下土样的微观结构,从微观角度对结构性黏土的微观结构特征变化机制进行了解释。结果表明:在不同应力路径下土体的孔隙直径、颗粒和孔隙的定向排列变化较大,而颗粒和孔隙的形状特征变化较小。增大球应力使土颗粒变得密实,使孔隙压缩,土体体积减小;减小球应力使土颗粒变得松散,孔隙直径增大,土体体积膨胀。增大或减小偏应力对土体微观结构的影响相似,在土体结构破坏前使土骨架变形产生一定压缩,在土体结构破坏后使颗粒错动、翻滚并相互搭接,扩大了粒间孔隙,使土体出现剪胀。土颗粒形状的不规则性导致球应力和偏应力对体应变和剪应变的交叉影响。研究结果揭示了不同应力路径下结构性黏土应力-应变特性的微观机制。 相似文献
7.
在深入探讨海相沉积原状软黏土压缩、变形等力学特性和详细分析加载屈服面随荷载情况变化的基础上,确认了海相沉积原状软黏土的强度、变形特性与结构屈服应力密切相关。即当固结压力小于结构屈服应力时,其力学特性与超固结重塑土的力学特性类似;当固结压力大于结构屈服应力时,其力学特性与正常固结重塑土的力学特性类似。为描述海相沉积原状软黏土的上述力学特性,将姚仰平等提出的超固结重塑土本构模型引入到海相沉积软黏土弹塑性本构模型的构建中。在本构模型构建过程中,考虑了海相沉积原状软黏土具有的抗拉强度及其演化规律,软黏土强度包线的特点及其进一步修正的表达式,使模型更符合海相原状软黏土的强度、变形特性。最后,将3种不同海相沉积软黏土固结排水剪切试验得到的应力-应变-体变曲线与模型预测结果进行对比。比较结果显示,本文提出的弹塑性本构模型能很好地描述海相沉积原状软黏土的剪缩硬化、剪胀软化以及变形的应力水平依存性等力学特性。 相似文献
8.
长久以来有色金属矿山的开采对矿山周围土体造成了严重的重金属污染问题。使用自制的重金属淋滤污染装置,制备室内重金属Zn2+污染土,进行固结不排水三轴剪切试验,研究淋滤条件下重金属Zn2+对桂林红黏土强度及其强度损伤规律的影响。试验结果表明:重金属Zn2+对桂林红黏土的强度损伤行为是明显的,抗剪强度平均下降了30.61% ~56.6%不等,应力-硬化关系均呈现应变硬化型,损伤变量D在0.478~0.566之间。淋滤条件下重金属Zn2+对桂林红黏土强度的损伤主要是由于Zn2+对红黏土胶结结构以及土颗粒的双电层结构产生了不可逆的侵蚀破坏,降低土体内部的联结强度,随着浓度的增大,其强度呈现出下降的趋势,其损伤变量亦有所增长,但相差较小。这是因为在长时间的淋滤过程中,红黏土对Zn2+具有一定的吸附作用,导致尽管是在低浓度的污染溶液淋滤作用下,土体的累积损伤和高浓度的效果相近似。 相似文献
9.
饱和黏土不排水剪切的热破坏 总被引：1，自引：1，他引：0
试验资料表明：饱和黏土在不排水常载升温条件下会产生很大的变形并最终可发生热破坏现象,因此,升温也成为一种加载方式。基于姚仰平等提出的热UH临界状态模型,推导了受温度影响的热不排水抗剪强度表达式,对不同超固结度饱和黏土在升温下的不排水抗剪强度模拟与试验结果对比表明：所提公式能够合理反映试验资料中受温度影响的不排水抗剪强度变化规律。利用热UH模型对不排水常载-升温过程进行了模拟,模拟结果表明,热UH模型可合理地反映不排水常载-升温条件下饱和黏土的应力-应变关系以及强度变化规律。针对能影响热破坏过程的几种因素如升温初始时的偏应力比、升温幅度、超固结度以及先期固结压力等进行了讨论分析,得到了各因素对于饱和黏土不排水剪切下的应力-应变关系及强度特性的影响规律。 相似文献
10.
热-水-力耦合作用下非饱和土变形特性的弹塑性模拟 总被引：1，自引：0，他引：1
《岩土力学》2017,(4):1060-1068
在已有的非饱和土水-力耦合模型基础上,耦合考虑温度影响,建立了一个热-水-力耦合作用下非饱和土弹塑性本构模型。该模型以土骨架平均应力、修正吸力和温度为应力状态变量,以土骨架应变、饱和度和熵为应变状态变量。通过引入与温度相关的屈服面(LY、TY)以及相应的硬化规律来考虑温度对土体变形的影响。利用建立的模型,对文献中不同吸力和温度条件下的等向压缩和三轴排水剪切试验进行预测,预测结果表明,该模型能够较好地定量描述热-水-力耦合作用下非饱和土的变形特性。 相似文献
11.
旋转平推式滑坡在青藏高原东北缘地区集中分布,论文系统梳理了该类滑坡的分布特征、几何应变模型,结合室外调查、试验与数值模拟计算,探讨了近水平滑动带变形的动力机制。研究表明：（1）旋转平推滑坡集中分布于东北缘上新世泥岩盆地内,其活动强度受到青藏高原隆升过程的影响,自高原腹地至边缘盆地,滑体体积逐步减小。巨大型滑坡群集中于黄河水系上游地区;大、中型型滑坡群分别集中于下游地区;（2）旋转平推滑坡均由高黏粒含量、超固结上新世泥岩组成,河流的侵蚀是近水平剪切应力形成的控制性因素。在水平应力作用下,超固结泥岩趋向与膨胀,表现出剪胀、渐进性破坏。薄层剪切带呈现韧、脆性变形,区域内随机排列的黏土颗粒的逐步定向,表现出低于10o的内摩擦角。（3）滑动带的蠕变、裂隙扩展与地下水的增湿加速材料的流变,滑面选择粘粒含量高、碳酸钙的含量低的软弱层扩展。滑带内粘土矿物蠕变、呈粘滞性流动,导致宏观变形逐步积累,并逐步出现剪切面、裂纹的扩展,是滑坡变形的动力因素之一。 相似文献
12.
Analysis and research results show that the sliding plane of Jiudingshan landslide is along the weak intercalated layer (clay-filled) in the limestone and the sliding block is separated by the tension crack on the slope crest. The earlier study results show that for the rough, ups and downs structural plane, when i is greater than 2.0, the shear strength of the structural surface is intensely close to the strength of the filling. By the earlier theory, this failure must be through the clay filling. In this study, the failure is back-analyzed and the shear strength of the infilling is tested by the laboratory direct shear tests for which samples were retrieved in the field. The failure cannot be explained by the laboratory results of shear strength parameters. To simulate the field conditions, the real strength parameters of sliding surface are measured by the in situ shear tests for the weak intercalated layer. By the in situ tests, it is shown that the failure initiates along the contacts between the clay infilling and the limestone boundaries, but not through the clay itself. Though the contact surface is the interface of the clay–limestone, the cohesion is not 0 and it is not negligible too. 相似文献
13.
A robust contact theory can be regarded as key to three dimensional discontinuous deformation analyses (3D-DDA). Not only must this theory provide an efficient algorithm to judge the type and location of contacts but also it must be able to present comprehensive formulations for every kind of contact (open, sliding and locked contact). There are six types of contact in three dimensional discontinuous deformation analyses (vertex-to-vertex, vertex-to-edge, vertex-to-face, edge-to-edge, edge-to-face and face-to-face) that can be converted to vertex-to-face and edge-to-edge contacts. This paper presents a new model of edge-to-edge contact to three dimensional discontinuous deformation analyses (3D-DDA). This new model considers both kinds of edge-to-edge contact (cross-over and parallel edge-to-edge contact) and presents a criterion for inter-penetration. Sub matrices of normal and shear spring and friction force are derived by geometrical analysis and penalty method. This new model is implemented in a 3D-DDA computer programme, and the example results demonstrate the validity of the model. 相似文献
14.
The present paper deals with the impact of shear deformation on the geometric arrangement of particles within the soil specimen,
which is termed as the microfabric of soil. A series of compression and extension lubricated end triaxial tests are performed
on cylindrical specimens of Kaolinite clay with two extreme microfabrics; dispersed and flocculated, which are obtained using
slurry consolidation technique. Flocculated microfabric has random orientation of particles within the soil mass having face-to-edge
particle contacts; however, dispersed microfabric has parallel orientation of particles containing face-to-face particle contacts.
When the specimen is subjected to large stress levels during its shear deformation, the particle orientation and the geometric
arrangement within the soil specimen gets affected due to the force acting on the clay platelets. The variation in microfabric
of soil before and after shear deformation process is evaluated by obtaining X-ray diffraction patterns of the clay specimen
at three different locations using standard X-ray diffractometer. The discussion includes an analysis of the orientation of
soil particles located at shear banding zones of the clay specimens, which may be useful for understanding the strain localization
development in clays. 相似文献
15.
The evolution of the microstructure of an assembly of cohesionless granular materials with associated pores, which carry the overall applied stresses through frictional contacts is a complex phenomenon. The macroscopic flow of such materials take place by the virtue of the relative rolling and sliding of the grains on the micro‐scale. A new discrete element method for biaxial compression simulations of random assemblies of oval particles with mixed sizes is introduced. During the course of deformation, the new positions of the grains are determined by employing the static equilibrium equations. A key aspect of the method is that, it is formulated for ellipse cross‐sectional particles, hence desirable inherent anisotropies are possible. A robust algorithm for the determination of the contact points between neighbouring grains is given. Employing the present methodology, many aspects of the behaviour of two‐dimensional assemblies of oval cross‐sectional rods have been successfully addressed. The effects of initial void ratio, interparticle friction angle, aspect ratio, and bedding angle on the rolling and sliding contacts are examined. The distribution of normals to the rolling and sliding contacts have different patterns and are concentrated along directions, which are approximately perpendicular to one another. On the other hand, the distribution of all contact normals (combined rolling and sliding) are close to that of rolling contacts, which confirm that rolling is the dominant mechanism. This phenomenon becomes more pronounced for higher intergranular friction angle. Characteristics of the rolling and sliding contacts are also discussed in the context of the force angle, which is the inclination of contact force with respect to the contact normal. Copyright © 2003 John Wiley & Sons, Ltd. 相似文献
16.
The Jinlong village landslide is located in Zitong County, Sichuan and approximately 150 km east of Wenchuan. The landslide has exhibited creep deformation for nearly 30 years. Field investigations indicated that the slope deformation was caused by the combined effects of unfavorable topographic and geological conditions and earthquakes. The sliding surface is along a contact between silty clay and mudstone. The Wenchuan earthquake accelerated the creep, causing bulging of the ground surface. Shear test results of the silty clay near the sliding surface indicated that the residual strength is consistent with the stability state of the landslide. The factors of safety were calculated using the limit equilibrium method (LEM) and the method of fast Lagrangian analysis of continua in two dimensions. The results using the LEM indicate that the stability is clearly affected by seismic shaking, and when the peak ground acceleration is 0.08g, the slope reaches the limit state. The shear failure surface given by numerical simulation develops on the contact between the clay and silty mudstone, which confirmed the assumed sliding surfaces’ location using the LEM. 相似文献
17.
To study the damage process of microscale to macroscale in coarse-grained granite specimen under uniaxial compressive stress, we have observed micro-damage localization and propagation by using a newly developed experimental system that allows us to observe the damaging process continuously.
The results showed that pre-existing microcracks lead to macroscopic shear fracture through the damage development process. The mechanism of micro-damage initiation in a granite specimen under uniaxial compressive stress may be considered for two cases. One is that two grains such as quartz and feldspar contact each other in the same direction as the axial stress, and the other is that a biotite grain inclined to the axial stress direction is surrounded by feldspar grains. The homogenization theory was applied to verify numerically the micromechanics of stress-induced damage in the mineral contacts. Local stress distribution in the periodic-micro structure was also calculated by the homogenization theory. It is shown that this analysis, which takes into account the initial state of the specimen, is well adapted to the behavior of two grains for which microcracking is the fundamental mechanism of damage. 相似文献
18.
Ajanta Sachan 《Geotechnical and Geological Engineering》2013,31(1):213-228
The present paper evaluates the role of microfabric in strain localization patterns observed in soil specimens during its shear deformation in compression and extension triaxial testing. A series of compression and extension lubricated end triaxial tests are performed on Kaolin clay with extreme as well as intermediate microfabrics, which are obtained using slurry consolidation technique by varying calagon content from 0 to 3 %. Intermediate microfabric is the geometric arrangement of particles within the soil mass, which lies in between the particle orientation during two extreme microfabrics; flocculated and dispersed. Flocculated has random orientation of particles with face-to-edge particle contacts and dispersed has parallel orientation of particles with face-to-face particle contacts. When the specimen is subjected to large stress levels in triaxial testing, the particle orientation and geometric arrangement get affected due to the force acting on the clay platelets. In this experimental research, the variation in clay’s stress–strain and pore pressure response and initiation, propagation and formation of shear bands at different levels of compression and extension shearing is evaluated using digital image analysis setup associated with triaxial system. 相似文献