Modeling the 2D behavior of dry‐stone retaining walls by a fully discrete element method

The dry‐stone retaining walls (DSRW) have been tipped as a promising solution for sustainable development. However, before recently, their behavior is relatively obscure. In this study, discrete element method (DEM) approach was applied to simulate the plane strain failure of these walls. A commercial DEM package (PFC2D™) was used throughout this study. The authors used a fully discrete approach; thus, both the wall and the backfill were modeled as discrete elements. The methodology for obtaining the micromechanical parameters was discussed in detail; this includes the three mechanical sub‐systems of DSRWs: wall, backfill and interface. The models were loaded progressively until failure, and then the results were compared with the full‐scale experimental results where the walls were loaded, respectively, with hydrostatic load and backfill. Despite its complexity and its intensive calculation time, DEM model can then be used to validate a more simplified approach. Copyright © 2015 John Wiley & Sons, Ltd.     

Constitutive modelling of fine-grained gassy soil: A composite approach

Fine-grained marine sediments containing large undissolved gas bubbles are widely distributed around the world. Presence of the bubbles could degrade the undrained shear strength (s_u ) of the soil, when the gas pressure u_g is relatively high as compared with the effective stress in the saturated soil matrix. Meanwhile, the addition of bubbles may also increase s_u when the difference between u_g and pore water pressure u_w becomes smaller than the water entry value, causing partial water drainage from the saturated matrix into the bubbles (bubble flooding) during globally undrained shearing. A new constitutive model for describing the two competing effects on the stress-strain relationship of fine-grained gassy soil is proposed within the framework of critical state soil mechanics. The gassy soil is considered as a three-phase composite material with compressible cavities, which allows water entry from the saturated matrix. Bubble flooding is modelled by introducing an additional positive volumetric strain increment of the saturated clay matrix, which is dependent on the difference between pore gas and pore water pressure based on experimental observations. A modified hardening law based on that of the modified Cam clay model is employed, which in conjunction with the expression for bubble flooding, can describe both the detrimental and beneficial effects of gas bubbles on soil strength and plastic hardening in shear. Only two extra parameters in addition to those in the modified Cam clay model are used. It is shown that the key features of the stress-strain relationship of three fine-grained gassy soils can be reproduced satisfactorily.     

Borehole failure analysis in a sandstone under anisotropic stresses

Borehole failure under anisotropic stresses in a sandstone is analyze numerically for various borehole sizes using a nonlinear elastic–plastic constitutive model for a Cosserat continuum. Borehole failure is identified as macroscopic failure of the borehole through the development of shear bands and breakouts. The results compare well both qualitatively and quantitatively with experimental results from polyaxial tests on Red Wildmoor sandstone. They show that the hole size effect of the borehole failure strength is independent of the far‐field stress anisotropy and follows a ? power law of the hole size. A similar scale effect equation with a ? power law is proposed for the scale effect of the maximum plastic shear strain at failure. This equation can be useful for better predicting hole‐size‐dependent failure with standard codes based on classical continua. The effect of stress anisotropy on the borehole failure stress is found to be independent of the hole size. The failure stress decreases linearly to 40% as the stress anisotropy increases. However, the maximum plastic shear strain at failure is stress anisotropy independent and therefore the critical plastic shear strain for failure is only hole‐size dependent. Copyright © 2009 John Wiley & Sons, Ltd.     

虎盆含金剪切带的厘定及其地质意义

黔东南虎盆金矿区处于杨子陆块与江南造山带的过渡地带,偏江南造山带一侧,区域性北东向稳江背斜北西翼,是黔东南地区典型的石英脉型金矿床。长期以来黔东南地区是否存在剪切带构造及其与金成矿的关系一直存在争议（卢焕章等,2005;陶平等,2011）,直接影响到该地区金矿的找矿工作方向。因此,黔东南地区剪切带构造的厘定对于完善该地区成矿模式研究具有重要意义。本文在充分总结虎盆矿床地质特征的基础上,利用宏观构造研究和显微构造研究及电子背散射衍射技术（EBSD）技术,首次厘定了虎盆含金剪切带,并探讨其与金成矿之间的关系及矿床成矿动力学背景,并结合区域成矿作用探讨区域找矿意义。     

长江中下游地区暖区暴雨特征分析

利用2007到2013年5-9月间常规和非常规资料以及6 h一次的NCEP 1°×1°再分析资料,将长江中下游地区暖区暴雨按天气形势划分为冷锋前暖区暴雨、暖切变暖区暴雨以及副热带高压边缘暖区暴雨三种类型。统计表明暖区暴雨一般发生在距离切变线(锋线)100~300 km的暖区内。主要结论包括:(1)冷锋型降水强度偏弱且分布均匀,集中在5、6月;暖切变型发生次数最多且强度大,主要发生在6、7月长江中下游地区的偏南部;副热带高压边缘型发生次数最少但强度较大,发生在7、8月。暖区暴雨的发生次数及强度在大别山、皖南山区较为集中。(2)暖区暴雨中短时强降水贡献大。(3)冷锋背景下的暖区暴雨一般产生在锋前低压槽中,暴雨落区与高低空急流耦合有紧密联系;暖切变型以低层暖切变线为主要天气背景,地面常有弱静止锋,暖区对流活动与中尺度急流结构、地形强迫等因素存在较高的相关性;副热带高压边缘暖区暴雨与局地的水汽积累和对流不稳定条件的发展有密切关系。据此建立三类暖区暴雨的概念模型。     

1998-2009年间台风不活跃期间热带云团活动分析

热带云团是台风生成的前兆,虽然一些研究将近20 a来台风不活跃与大尺度环境场相联系,但是还没有人分析台风不活跃期热带云团的活动特点。本文利用目前仅有的1989-2009年全球热带云团资料,分析了西北太平洋热带云团近20 a的变化特征。1998年以后西北太平洋台风生成减少主要发生在7-10月,集中在南海（13～23°N,110～120°E）和西北太平洋台风活动区域的东部（13～23°N,145～170°E）。热带云团除1月外各月都有增加的趋势,特别是与台风生成显著减少区域相联系的热带云团活动具有显著的增加趋势。通过对NCEP/NCAR再分析资料分析发现,1998年后热带云团活动增加与环境风垂直切变增加有关,而增强的垂直切变不利于台风生成。     

京津冀地区中α尺度飑线过程中大风特征分析及成因初探

应用常规天气观测资料、地面加密自动气象站资料、大风灾情报资料、京津冀地区7部多普勒天气雷达组网观测资料及VDRAS资料,从多个角度对2013年8月4日京津冀地区一次飑线过程产生的大范围大风天气过程进行了分析,结果显示:此次过程是在高空冷空气南下、低层暖湿气流北上、系统前倾及位势不稳定的有利层结条件下,由多单体风暴演变为中α尺度的强飑线所致。飑线形成于低层垂直切变加强、冷池合并之后;大风主要发生在飑线主体回波中,其次是主体回波前和中前,主体回波后很少发生。大风发生的位置取决于飑线结构中气流的性质,气流的性质与冷池前进的程度和对流的强度关系密切。大风大部分由下沉冷气流产生,少数为近地面上升暖气流导致。大风发生的范围和强度与低层风垂直切变的强度呈正比,大范围低层风垂直切变的加强增强了飑线入流和出流的强度,是大范围大风、局部强风形成的重要原因。大风发生站次与冷池的强度和范围密切相关,冷池的加强和范围的扩大加强了后侧冷入流和前侧暖入流的强度和范围,也是大范围大风形成的重要因素。     

鲁中南一次暴雨过程的特征和成因分析

利用常规气象观测资料、NCEP 1°×1°逐6h的再分析资料、GPS可降雨资料和地闪定位资料,对2013年7月4—5日山东中南部出现的暴雨到大暴雨天气过程的不同阶段特征和成因进行了分析,结果表明:本次暴雨过程是冷暖切变线所引发,暴雨的水汽源于南海;低空急流的强弱和水汽通量的大小呈正相关;暖切变线暴雨的雨强、影响范围和持续时间明显大于冷切变线暴雨;冷、暖切变线GPS可降雨量表现不同,前者短时间内增幅大,地面强降雨在峰值出现1h后发生,对地面降雨变化反映较敏感,后者强降雨出现前8h可降雨量快速上升,可降雨量峰值对应地面降雨大值,对地面降雨变化反映不敏感;冷切变线对流性更强,地闪频次为暖切变线降雨的2倍,正地闪频次为暖切变线降雨的1/2,负地闪频次为暖切变线降雨的2倍;降雨云团正、负地闪活跃程度呈反相位关系,正、负地闪的变化能很好地反映强降雨的变化;冷、暖切变线动力结构不同,前者物理量场从低层到高层向北倾斜,后者则为垂直分布;冷切变线上升运动区较暖切变线深厚。     

桐柏山L构造岩形成机制构造解析及其对造山带演化的制约

桐柏杂岩中发育一套典型的L构造岩,其构造位置位于桐柏造山带核部,被两条近似对称的韧性剪切带所夹持,北侧剪切带左旋,南侧剪切带右旋。由于L构造岩构造位置特殊,其位于剪切带、桐柏背形、桐柏穹窿等多种构造体的交叉部位,L构造岩的构造成因解析可以为桐柏造山带的形成演化提供重要制约。通过对桐柏造山带L构造岩的构造成因机理解析和其变形温压条件的研究,同时结合前人对桐柏山其它主要构造单元的研究,我们提出,桐柏山L构造岩的形成主要受其南北两侧两条韧性剪切带控制,传统意义的桐柏杂岩体白垩纪之前与南北一体的韧性剪切带沿近似东西方向发生管状韧性剪切,剪切作用形成了一套典型的L构造岩。L构造岩的形成指示了桐柏山单元可能经历了一期中下地壳物质的管状的韧性的向东剪切流动,后期白垩纪桐柏山核部的L构造岩经历了大规模的岩浆上升与浮力增加,该L构造岩同剪切带一起发生隆升但管状剪切构造特征并未被改造,随着不均匀隆升桐柏山出现了现今的几何学特征。L构造岩反映出管状剪切形成了现今桐柏造山带近东西向线状构造样式的主体。     

运动学涡度在藏南冈底斯岩浆带中段谢通门-曲水韧性剪切带中的应用

一般剪切带主要由纯剪切和简单剪切共同作用,不同的剪切带及不同的构造位置两者所占有的比例不同。利用运动学涡度(Wk)可以定量地分析两者间的比值大小。本文通过极莫尔圆法和有限应变轴率Rs/石英c轴组构法对冈底斯岩浆带中段谢通门-曲水滑覆型韧性剪切带的运动学涡度进行了计算,两种方法获得了较为一致的结果。通过极莫尔圆法,对剪切带中的9组糜棱岩样品进行了运动学涡度计算,获得了Wk=0.73~0.96,平均值Wk=0.83。运用有限应变轴率Rs/石英c轴组构法对4个样品进行了分析,得到Wk=0.85~0.93,均值为0.88,两种方法获得了较为一致的应变结果。还根据极莫尔圆图解,计算了该韧性剪切带的减薄量S=0.09~0.35,平均减薄量为0.20。研究表明该韧性剪切带为典型的以简单剪切为主伴有部分纯剪切的一般剪切,该剪切带的形成可能与拉萨地体在中新世时从挤压到侧向伸展的转换有关。该剪切带变形特征和运动学涡度的确定深化了对藏南冈底斯地区的构造演化过程的理解,并对青藏高原中南部的地质研究具有推进作用。