横向槽沟内非均匀流的试验研究

以横向槽沟中产生的非均匀流为研究对象,通过水槽概化模型试验,在实测纵向流速分布的基础上,分析了不同来流条件及不同槽沟边坡角度下的槽沟内水面流速、槽底流速等沿程变化规律,同时还得到了计算槽沟内反向平均流速及正向平均流速的经验公式.     

泥沙颗粒形状对非均匀沙起动条件的影响

根据非均匀沙颗粒的不均匀性,引入颗粒形状系数,通过分析泥沙颗粒形状系数和相对暴露度的影响,建立了等效粒径表达式;并通过泥沙起动受力分析,推导得到泥沙起动临界条件表达式.实测资料验证表明,计算值与实测值符合较好.     

不同粒度颗粒在非恒定管流中跟随性试验

管道中固液两相流水击对管道和输送系统可能产生严重的破坏,而固液两相在这种非恒定流中的运动特性是计算最大水击压力变化的重要依据。采用粒子图像测速技术（Particle Image Velocimetry,PIV）,通过试验研究水击发生时,水平圆管中不同平均流速、颗粒粒径条件下,流体介质和粗颗粒在管道断面的速度分布以及粗颗粒跟随性的变化规律。研究结果表明:①在水击发生的不同时刻,圆管流中粗颗粒的流速在管道断面分布呈不规则的抛物线型分布,主要表现为靠近管道壁面底部的颗粒流速略小于靠近管道顶部流速,当颗粒粒径大于1.5 mm,平均流速小于2.5 m/s时,粗颗粒表现出明显的沉降特性;②粗颗粒的跟随性与颗粒受力有密切关系,其中颗粒速度与流体速度的变化量是影响颗粒受力的重要参数;③基于试验数据拟合得到了水击条件下粗颗粒跟随性系数k的经验公式,并分析了颗粒粒径、管道直径、两相流平均流速以及水击发生时间等不同参数对粗颗粒跟随性系数的影响,公式计算值与实测值之间的误差在5%以内。     

颗粒流理论模拟砂土的力学性质

文中采用颗粒流理论模拟了砂土双轴试验和砂土剪切带的形成与发展机理。通过颗粒流数值模拟试验再现了砂土应力－应变关系曲线，同时研究了砂土细观参数变化时其宏观力学性质的反应。对比研究了室内试验与颗粒流试验砂土剪切带的形成与发展机理，同时研究了当细观参数如颗粒大小、刚度、摩擦系数变化时，砂土剪切带的变化规律。     

三门峡库区一维非恒定非均匀泥沙输移数学模型

黄河是高含沙河流,含沙量季节差异显著。因此研究黄河干流的非恒定水沙输移规律以及库区泥沙的淤积问题极为重要。应用圣维南方程组以及非恒定泥沙连续方程建立了非恒定非均匀泥沙含沙量计算公式,并根据沙量平衡方程推求出三门峡库区河底高程的变化规律。使用已有的资料对模型进行的验证表明:模型计算与实测资料符合良好,该模型具有较好的应用前景。     

基于非均质地层参数表征的颗粒流模型构建

非均质地层参数的获取与表征方法是浅层地质体改造的重要依据。基于非均质地层的地质建模,表征具有随机不确定性和模糊不确定性的土体表观参数和物理力学参数。利用 Weibull 分布统计描述局部地层信息,并应用Diamond-Square分形插值方法,结合差分盒子维计算非均质地层分形维数,进一步合理演算整体地层参数。采用PFC3D数值模拟软件,结合马尔科夫链蒙特卡洛方法采样数据,对非均质地层块石颗粒及土颗粒进行建模。通过非均质地层模拟结果,发现其破坏过程与应力应变曲线要比均质土体复杂得多,由于块石大颗粒的含量、分布特性对土样力学性质影响显著。本文建模方法有助于非均质地层参数表征研究。     

崩落矿岩散粒体流动性能试验研究

崩落矿岩散粒体的流动性能对于降低损失贫化具有重要的意义。分析了影响散粒体流动性能的因素,采用标志颗粒法进行了崩落矿岩散粒体流动性能试验,主要考虑的因素有放矿口大小、散体颗粒的粒径以及不同的散体材料。试验内容有放矿口大小与散体移动带试验;不同散体粒径与散体移动带试验、不同散体材料与散体移动带试验;平面和立体模型时放矿口尺寸对放出量影响试验;散体堆积高度与散体移动带试验。研究结果表明,（1）移动边界与散体的材料、颗粒的尺寸大小、放矿口大小等因素有关,而散体堆积高度对其影响不大;（2）散体的流动速度与散体颗粒的大小和放矿口尺寸有关。根据所得试验结果,提出了采矿设计参数的确定方法。     

Diffuse bifurcations engraving diverse shear bands in granular materials

Shear bands with characteristic spatial patterns observed in an experiment for a cubic or parallelepiped specimen of dry dense sand were simulated by numerical bifurcation analysis using the Cam‐clay plasticity model. By incorporating the subloading surface concept into the plasticity model, the model became capable of reproducing hardening/softening and contractive/dilative behavior observed in the experiment. The model was reformulated to be compatible with the multiplicative hyperelasto‐plasticity for finite strains. This enhanced constitutive model was implemented into a finite‐element code reinforced by a stress updating algorithm based on the return‐mapping scheme, and by an efficient numerical procedure to compute critical eigenvectors of elastoplastic tangent stiffness matrix at bifurcation points. The emergence of diamond‐ and column‐like diffuse bifurcation modes breaking uniformity of the materials, followed by the evolution of shear bands through strain localization, was observed in the analysis. In the bifurcation analysis of plane strain compression test, unexpected bifurcation modes, which broke out‐of‐plane uniformity and led to 3‐dimensional diamond‐like patterns, were detected. Diffuse bifurcations, which were difficult to observe by experiments, have thus been found as a catalyst creating diverse shear band patterns.     

基于图像相关分析的土体剪切带识别方法

提出了一种基于数字照相量测和图像相关性分析技术的土体剪切带识别方法。首先,在模型试验中,用数码相机采集土体全程变形图像序列;接着,在图像全局观测范围内粗略搜索到剪切带发生的大致区域;然后,布置跨越剪切区域的多对测点线,进行局部范围精密搜索,识别出剪切带的准确位置与形状, 并确定剪切带的边界点。与在模型上描画网格线等传统方法相比,该法操作简单,量测准确,适用于模型试验中岩土材料的剪切带识别及其厚度、倾角、带内变形和演变过程等特性的试验研究;最后,给出了一个大型砂土剪切试验中的应用实例。结果表明,基于图像相关分析的识别土体剪切带的方法是可行而有效的。     

含细粒砂土反常剪切行为的数值模拟研究

针对含细颗粒砂土的反常剪切行为,开展了双轴剪切试验的数值模拟,从宏细观角度分析了其反常剪切行为发生的内在机制。数值模拟结果表明,增加围压能提高含细颗粒砂土的抗剪切液化能力,该反常行为的根本原因在于围压上升使得粗细颗粒更有效地参与了力链传递,增加了颗粒间的接触,增强了土体的密实度。细颗粒在土骨架中的移动对砂土的液化起着至关重要的作用,而粗颗粒仅起次要作用。研究表明,细颗粒在剪切过程中会持续从有效土骨架中移出成为无效颗粒,而部分粗颗粒也因失去细颗粒的支撑作用会脱离土骨架,直至试样最终液化。细颗粒一般参与土骨架中的弱力链,而粗颗粒则一般参与强力链,导致细颗粒较粗颗粒更容易在土骨架中移动。     

考虑剩余剪应力的滑带土强度再生试验

用改造的直剪仪研究了滑带土再生强度与滑动面剩余剪应力比PRSS和强度再生时间的关系。结果表明,滑带土强度再生与上覆滑体压应力关系不大,但较高的剩余剪应力比PRSS妨碍滑带土强度再生,滑带土强度有效再生的界限PRSS在55%到70%之间。剩余剪应力比PRSS小于等于55%时,90 d时滑带土再生强度可达到慢剪强度的70%以上,PRSS大于等于70%时,90 d时滑带土再生强度不足慢剪强度的25%。滑带土强度再生过程中,黏聚力和内摩擦角增速不一致,PRSS小于等于55%时,黏聚力C在前30 d增速较快,30 d时增至慢剪强度[C]的44.6%,此后增速均明显放缓,90 d时其值为慢剪强度[C]的49%。内摩擦角φ在前90 d增速基本一致,90 d时其值占慢剪强度[φ]的90.4%。黏聚力和内摩擦角90 d以后均趋于稳定。     

一种控制直剪蠕变试验剪应力的简易装置

土的蠕变是指土在保持应力不变的条件下,应变随时间延长而增加的现象。研究土的蠕变性质对于确定土的长期强度有重要意义,土的蠕变研究也是近几年的研究热点。然而,土的蠕变试验周期特别长,因此简便、易行又有一定可信度的蠕变试验仪器,对于土蠕变性质的研究有较大的推动意义。直剪蠕变试验是研究确定土的蠕变性质的一种最简单、最直观的试验方法。但由于该试验只是控制剪切力不变,剪切过程中,试样受剪面积逐渐减小,剪应力持续增大,整个过程并不是蠕变。通过在传统仪器上附加一个简单装置,利用液体的浮力来控制试验剪切力,从而使得试样在剪切过程中的剪应力不变。在对仪器进行相应改进后,做了对比试验,检验该装置对剪应力的控制效果,试验结果表明,该简易装置可在一定程度上控制剪应力。     

Revisiting the existence of an effective stress for wet granular soils with micromechanics

A possible effective stress variable for wet granular materials is numerically investigated based on an adapted discrete element method (DEM) model for an ideal three‐phase system. The DEM simulations consider granular materials made of nearly monodisperse spherical particles, in the pendular regime with the pore fluid mixture consisting of distinct water menisci bridging particle pairs. The contact force‐related stress contribution to the total stresses is isolated and tested as the effective stress candidate for dense or loose systems. It is first recalled that this contact stress tensor is indeed an adequate effective stress that describes stress limit states of wet samples with the same Mohr‐Coulomb criterion associated with their dry counterparts. As for constitutive relationships, it is demonstrated that the contact stress tensor used in conjunction with dry constitutive relations does describe the strains of wet samples during an initial strain regime but not beyond. Outside this so‐called quasi‐static strain regime, whose extent is much greater for dense than loose materials, dramatic changes in the contact network prevent macroscale contact stress‐strain relationships to apply in the same manner to dry and unsaturated conditions. The presented numerical results also reveal unexpected constitutive bifurcations for the loose material, related to stick‐slip macrobehavior.     

Micromechanical aspects of the shear strength of wet granular soils

This paper presents a micromechanical model for the analysis of wet granular soils at low saturation (below 30%). The discrete element method is employed to model the solid particles. The capillary water is assumed to be in a pendular state and thus exists in the form of liquid bridges at the particle‐to‐particle contacts. The resulting inter‐particle adhesion is accounted for using the toroidal approximation of the bridge. Hydraulic hysteresis is accounted for based on the possible mechanism of the formation and breakage of the liquid bridges during wetting and drying phases. Shear test computational simulations were conducted at different water contents under relatively low net normal stresses. The results of these simulations suggest that capillary‐induced attractive forces and hydraulic hysteresis play an important role in affecting the shear strength of the soil. These attractive forces produce a tensile stress that contributes to the apparent cohesion of the soil and increases its stiffness. During a drying phase, capillary‐induced tensile stresses, and hence shear strength, tend to be larger than those during a wetting phase. The proposed model appears to capture the macroscopic response of wet granular materials and revealed a number of salient micromechanical mechanisms and response patterns consistent with theoretical considerations. Copyright © 2008 John Wiley & Sons, Ltd.     

风化岩体中压力型锚索锚固段的剪应力分析

岩体在风化过程中,其物理力学性质会随着风化程度的不同有所差异。结合均质岩体中压力型锚索受力特点,以及内部对称荷载作用下横观各向同性弹性体内的剪应力分布特点,推导出了压力型锚索在横观各向同性弹性岩体内的剪应力分布方程。假定风化岩体为横观各向同性弹性体,其弹性模量及剪切模量均按指数函数变化,分析结果表明：①由于风化岩体的弹性模量随着深度的变化,锚索锚固段的剪应力也随着岩体的弹性模量的增加（减小）而增加（减小）;②在承压板附近,锚索锚固段的剪应力随锚索孔半径的增加而减小,由于风化岩体剪切模量的变化,因而导致剪应力的变化量很大;③在承压板附近,锚索锚固段接触面上的剪应力随着垂直于岩体横向等向面的剪切模量的改变而相应的改变。研究成果可为实际工程中压力型锚索设计提供参考。