强震作用下陡倾顺层岩质边坡动力响应与破坏模式研究

以陡倾顺层岩质边坡为研究对象,采用振动台模型试验与FLAC^3D数值模拟方法,对强震作用下陡倾顺层岩质边坡的动力响应规律和变形破坏模式进行了研究。研究结果表明：陡倾顺层岩质边坡在坡表及坡内竖直方向的加速度响应均表现出高程放大效应,而水平方向上的加速度响应则表现为趋表效应;输入波类型对边坡模型加速度响应有显著影响,正弦波作用下的加速度响应明显强于天然地震波;加速度放大系数随地震波振幅的增大,呈现先增大后减小的变化规律;地震波加载持续时间对陡倾顺层岩质边坡加速度响应的影响较小。对模型试验和数值模拟中边坡变形破坏特征的分析,得到陡倾顺层岩质边坡在强震作用下的破坏模式为：地震诱发-坡表岩层出露处岩块松弛张裂-坡肩岩层处拉裂张开-坡面中部出现剪切裂缝-裂缝逐渐贯通-发生多级高位滑坡。     

重庆小南海滑坡形成机制离散元模拟分析

重庆小南海滑坡是烈度相对较低地区发生的地震高位滑坡,其成因一直令人费解。基于重庆黔江小南海相关研究资料,通过对复原的小南海坡体进行失稳分析,计算得出使岩体产生崩滑破坏的地震力临界条件,即只有当地震波地形放大后滑坡才能启动。为了进一步验证计算所得的结论,运用UDEC软件建立小南海典型二维场地模型,施加相应的地震力对坡体失稳崩滑的全过程进行模拟,以研究地震作用下地形放大效应触发具平行坡面陡倾控制性结构面的高位岩质斜坡地震机理。研究结果表明,在地震波传播过程中,具平行坡面陡倾控制性结构面的高陡突出地形对地震波有明显的放大作用。该坡体运动模式为：峰值加速度放大-增加的振幅迫使岩体顺平行坡面陡倾控制性结构面迅速拉裂-沿缓倾层面滑移-高速脱离滑源区-巨大的势能和动能驱动坡体做长距离运动,其间伴随解体、颗粒间相互碰撞、铲刮作用,具有二相甚至三相流体性质。分析揭示地震力作用下斜坡体中质点加速度具有地形放大效应。对比结构面监测点和基岩监测点加速度放大系数,表明,滑坡启动时具有较大的加速度,当遇到平行坡面的不连续结构面时,斜坡动力响应强烈,最终导致坡体失稳。     

考虑地震动地形效应的边坡破坏概率——以金沙江下游新市镇附近边坡为例

边坡在地震作用下的破坏概率是地震边坡危险性评价的参数之一。在区域范围内计算地震边坡破坏概率一般采用实际地震滑坡和Newmark永久位移拟合得到的破坏概率公式进行计算。计算中所需的地震动峰值加速度数值大小受不规则地形的影响较大。为了较准确计算出区域地震边坡的破坏概率,本文利用公式分别计算了地震动峰值加速度地形效应系数和地震边坡滑坡概率,实现了地震动峰值加速度及滑坡概率的连续分布。在计算地表30 m平均剪切波速时,利用回归分析方法得出了Vs30与地形梯度G的连续性关系。这些方法充分考虑了地形在地震动峰值加速度中所起的作用,能够实现地震边坡破坏概率计算结果的连续性,如实反映了地震边坡破坏概率的实际状况,为更准确评价地震边坡滑坡危险性提供了新的思路。     

水平地震力作用下顺倾结构面对岩质边坡破坏影响分析

基于断裂理论和波动理论对水平地震力作用下对岩质边坡顺倾结构面的破坏建立了数学模型,在不考虑结构面填充物的影响下分析了结构面的长度、埋深及倾角在水平地震动力作用下对边坡破坏的影响。分析结果表明,当结构面埋深与长度h/L相差不大时,对于一定的水平地震加速度a,结构面埋深和长度越大,边坡在地震作用下越容易破坏;当结构面埋深和长度一定时,边坡破坏随着水平地震加速度的增大而增强。另外,结构面的倾角在增大过程中,岩体所受的拉应力逐渐增大,剪应力则表现为先增大,后减小。这是由于当结构面的埋深与长度一定时,随着倾角的增大,地震作用下边坡是从剪切破坏逐渐向拉张破坏过渡。该模型对地震作用时边坡稳定性分析具有一定的参考意义。     

顺倾层状碎裂结构岩质边坡地震动力响应及破坏模式分析

顺倾层状边坡沿软弱带剪切方式破坏是滑坡的主要类型之一。采用块体砌筑斜坡振动台模型,在多维多参数地震动作用下,考虑斜坡不同工况下力学参数弱化的过程,研究了层状碎裂结构岩质边坡的地震动力响应和失稳破坏模式。结果表明：斜坡地震动特性和斜坡地质结构是决定斜坡地震动力稳定性以及破坏模式的决定因素;斜坡水平动力响应具有明显的高程和坡表放大效应,高程对斜坡的垂直动力响应影响较小,地震动放大效应与结构面力学强度、地震波波形、频谱特性等均有一定的关系,正弦波较天然波对坡体放大效应影响更为显著;坡体裂纹依托优势结构面在最弱部位起裂萌生扩展,并向节理面追踪形成蠕滑段和锁固段,节理面强度参数在外界地质营力作用下发生弱化,使潜在滑带出现由后缘向前端搭接贯通的前进式破坏模式和由前端向后缘的后退式破坏模式的分化,滑体也由高位剪出向溃散破坏演变。     

四川茂县新磨村滑坡高速启动机理研究

2017年6月24日,四川省茂县新磨村发生的大型高速远程岩质滑坡,在约2 min的时间内,水平运动距离超过了2500 m。为了研究滑坡的高速启动机理,通过详细的现场地质调查,将滑坡的全程运动过程划分为高速启程、抛射“飞行”、高速铲刮和减速堆积4个阶段。基于物理模型试验,研究了新磨村滑坡的破坏失稳模式。试验过程中,监测得到的加速度数据显示,在锁固段岩体破裂瞬间,滑坡体受到了指向临空面方向的震动力,并由此产生了高达0.94g的瞬时加速度。模型试验结果表明,处于滑源区的锁固岩体,在破裂瞬间的弹性应变能释放,产生了强烈的震动效应,直接作用于滑坡体的瞬时震动力对滑坡的高速启程起到重要作用。计算表明,受到强烈震动的滑坡体,将以0.98g的瞬时加速度沿与水平面成15.5°的抛射角加速启程。采用Rockfall数值计算方法,模拟分析了滑坡体在不同启程速度下(0, 10,20, 30, 40和50 m·s^-1)的高速运动特征,结果表明,当滑体的初始速度达到30 m·s^-1时,剧动失稳的滑体可以直接撞击到地面的铲刮区,由此估算出新磨村滑坡的主滑时间约为60 s,...     

强震作用下顺层岩质斜坡动力失稳机制及启动速度研究

岩质斜坡地震稳定性评价和地震滑坡启动速度计算是边坡地震失稳防治中的难点。结合5•12四川汶川地震诱发的大型高速滑坡,重点以唐家山高速滑坡为例,提出强震作用下中陡倾顺层岩质斜坡动力失稳机制为拉裂－楔劈－滑移－剪断,并着重阐述了拉裂面形成机制、“楔劈”岩块的杠杆作用和碎屑岩块的滚动摩擦效应。对应于该失稳模式,采用弹性力学理论,推导出地震作用下顺层岩体斜坡锁固段的破坏判据和突发剪断时锁固段岩体的形变能公式。考虑锁固段岩体形变能释放的优势方向,运用能量转化原理,给出了更为合理和精确的顺层岩质滑坡突发启动速度公式,进而确定滑坡启程速度。其研究结果为滑坡灾害范围和冲击损害程度提供有效定量计算方法。     

平面剪切岩质边坡滑裂面的确定及稳定性分析

由于传统搜索方法对岩质边坡滑裂面的确定无法兼顾效率与精度,如何迅速准确确定潜在滑裂面仍然是个难题.极限平衡法在岩质边坡稳定性分析中备受认可,采用岩质边坡平面剪切滑动模型,以滑裂面的倾角来表征潜在滑裂面的位置;基于极值法,推导了极限平衡条件下平面剪切破坏型岩质边坡潜在滑裂面的解析解,并结合香港秀茂坪路边坡对其准确性进行了...     

刘家湾滑坡特征及成因机制探讨

刘家湾滑坡位于青川东河口红光乡刘家湾,为汶川地震触发的特大型岩质山体滑坡。野外调查结果表明,该滑坡堆积体与一般汶川地震滑坡运动堆积体迥异的是滑体在沿碳质板岩与白云岩划分带破坏溃滑后,滑源区又沿白云岩风化卸荷带触发了二次溃滑,形成二级堆积平台的形态且以不同岩性区分,在岩性划分带及风化卸荷带呈现出明显的动力破坏特性。通过对该滑坡堆积体进行岩体物理力学试验及波速测试研究表明,该滑坡由白云岩、碳质板岩及千枚岩组成的内硬外软岩质边坡具有明显的量化差异特性,强震条件下差异岩性组合边坡岩层接触面的动力突变效应耦合凸出地形是导致该边坡破坏的主要因素。近一步研究显示该滑坡运动可大致分山体震裂阶段、地质分界面应力突变阶段、高速溃滑阶段、碎屑流堆积阶段、二次溃滑堆积5个动力过程。     

汶川地震触发平溪村滑坡特征及成因分析

平溪村滑坡是汶川地震触发的高速岩质滑坡,面积为3.7×104m2,体积约65×104m3。滑坡距离映秀—北川发震断裂带中的石坎断层不足500m,在强大地震力作用下,滑坡滑动面陡峭、粗糙,与重力作用下呈圆弧、平滑的滑面迥异。地震触发的滑坡可分为三个阶段:①震动拉裂阶段;②摩擦阻力降低、"锁固段"剪断阶段;③滑体溃滑,高速流动堆积阶段。然后结合结构面的力学分析,通过数值模拟对地震作用下的应力变化和震裂机制进行了初步分析。     

Analysis on mechanism of landslides under ground shaking: a typical landslide in the Wenchuan earthquake

A high steep rock hill with two-side slopes near National Road 213 is used as a prototype in this paper. The full process from initial deformation to sliding of the slope during ground shaking is simulated by a new discrete element method—continuum-based discrete element method. Then, the seismic responses of a high steep rock hill with two-side slopes are researched from the base of time, frequency and joint time–frequency domain using Hilbert–Huang transform and Fourier Transform. The findings are: first, the stress concentration phenomenon occurs at the top of the sliding mass, and then some tension and shear failure points appear, which expand from the top toward the toe of the sliding mass along the structural plane. At the same time, the number of tension failure points gradually increases. Then the toe of the sliding mass fails, and shears out from its toe which results in the landslide. If the material parameters are under the same conditions, the landslide in the middle of the slope occurs before that at the foot of slope, and the starting time of landslide and the arrival time of the peak ground acceleration are synchronous or the former slightly lags behind the latter. The difference of distribution and dissipation of earthquake energy in the sliding body and sliding bed is the major influence factor to induce the landslide. When the accelerations are small, the instantaneous frequency of accelerations between sliding bed and sliding body is generally consistent, the energy transmittance coefficients of the sliding structural plane and the controlled frequency band of the energy all range in a limitation; with the increase of the seismic intensity, the instantaneous frequency and the energy transmittance coefficients gradually decrease, and then they are steady within the lower limitation. At the same time, the controlled frequency band also shifts gradually from high frequency band to the lower one. Based on the input seismic wave, the peak acceleration amplifies as the increase of elevation, regardless of the monitoring points on the steep slope, gentle slope side or inside of the slope. Generally speaking, amplification of the vertical peak acceleration is stronger than that of the horizontal peak acceleration, and amplification of the peak acceleration on a steep slope is stronger than that on a gentle slope, and that of inside of the slope is the weakest amplification.     

福建省高速公路边坡病害类型分析

为解决边坡防护加固设计依据不足的问题,本文结合福建省高速公路路堑边坡工程实践,归纳了风化剥落、流石流泥、掉块落石、溜坍、坍塌、崩塌、倾倒、错落和滑坡等9大类路堑边坡常见病害类型,并对各病害类型的变形破坏特点进行分析：路堑边坡小规模变形破坏在富水土体中以流、溜、坍运动模式为主,在风化岩石中以剥、落运动模式为主;大规模变形破坏则受控于岩土体中结构面的空间位置及其组合形式,反倾岩层易产生＂倒＂,节理岩体易产生＂崩＂,残存结构面的软弱岩土体易形成＂塌＂,存在陡倾结构面和软弱坡脚的岩土体易形成＂错＂,以及沿特定软弱面做整体水平运动的＂滑＂等多种运动模式。     

大别造山带岳西县斜坡变形破坏演化模式

岳西县自然斜坡在地球内、外动力共同作用下,容易变形并遭到破坏,造成人员伤亡和财产损失,严重制约了当地的经济发展。通过系统的工程地质调查和浅表生改造理论分析,查明了岳西县斜坡变形破坏特征及其成因,并探讨了其演化模式。结果表明,岳西县不同岩组的抗风化能力和力学特性存在差异,斜坡发生地质灾害的机理也不相同。根据斜坡结构特征,岳西县滑坡分为全风化层滑坡、强风化层滑坡和顺层岩质滑坡：全风化层滑坡的滑面位于全风化层中或全风化层与强风化层的分界线处;强风化层滑坡的滑面主要发育于强风化层与中风化层的分界线处;顺层岩质滑坡主要发育于片麻岩发育的顺向坡中。根据变形破坏方式,岳西县崩塌可分为滑移式崩塌、倾倒式崩塌和坠落式崩塌：滑移式崩塌主要由一组缓倾坡外结构面和另一组陡倾(坡外或者坡内)结构面控制;倾倒式崩塌主要由一组陡倾坡内结构面和另一组近水平发育的结构面控制;坠落式崩塌主要由一组结构面陡倾或近直立发育的结构面控制。岳西县滑坡多发育于风化壳厚度较大、岩体较松散、结构面强度低的地区;崩塌多发育于斜坡高陡、岩质风化程度低、结构面发育的地区。研究成果对岳西县乃至整个大别山地区地质灾害的研究及防治工作具有一定的借...     

Analysis of an anti-dip landslide triggered by the 2008 Wenchuan earthquake in China

The Guantan landslide, with a total displaced mass of about 468 × 10⁴ m³, was triggered by the 2008 Wenchuan earthquake and succeeding rainfall in Jushui Town, Sichuan Province, China. The landslide occurred on an anti-dip hard rock slope with a weak rock founding stratum of 200 m in thickness. To investigate the failure mechanism of the Guantan landslide, dynamic behaviors of hard and soft rock slopes were investigated by means of large scale shaking table tests. The laboratory models attempted to simulate the field geological conditions of the Guantan landslide. Sinusoidal waves and actual seismic waves measured from the Wenchuan Earthquake were applied on the slope models under 37 loading configurations. The experimental results indicated that deformation mainly developed at a shallow depth in the upper part of the hard rock slope and in the upper (near the crest) and lower (near the toe) parts of the soft rock slope. An equation for predicting the depth of sliding plane was proposed based on the location of the maximum horizontal acceleration. Finally, it was concluded that the failure process of the Guantan landslide occurred in three stages: (1) toppling failure caused by compression of the underlying soft rock strata, (2) formation of crushed hard rock and sliding surface in soft rock as the result of seismic shocks, particularly in the horizontal direction, and (3) aftershock rainfall accelerates the process of mass movement along the sliding plane.     

Landslides and neotectonic activities in the Main Boundary Thrust (MBT) zone: Southeastern Kumaun,Uttarakhand

Main Boundary Thrust (MBT) zone is constituted of some of the landslide prone areas in southeastern part of Kumaun Sub-Himalaya. Role of landslides as natural hazard and hill slope modifying agent is well documented from various part of Himalayan region and southern hills of Kumaun particularly in the MBT zone, which are susceptible to various type of mass movement. The rocks making up the slopes has been put to a number of brittle deformation phases during the movement along the MBT, and are traversed by number of joint sets. In the open slope these intersecting joint sets forms wedges and are the most favorable site for initiation of rockfalls and other types of landslides. Landslides are taking place primarily due to high angle slopes, formation of structural wedges along the free steep slopes, sheared nature of the rocks due to proximity to the MBT and neotectonic activities along the MBT and other transverse faults. Wedge failure is a common type of landslides in rock slopes characterized by multiple joints and acts as sliding planes for the failed blocks. Field observations and wedge failure analysis indicates most of the landslides taking place in MBT zone of Kumaun Sub-Himalaya are joint controlled. Safety Factor analysis suggests MBT zone of Kumaun Sub-Himalayan region is prone to landslides and related mass movements. This zone is also neotectonically active as indicated by various geomorphic signatures such as structurally controlled drainage pattern, offsetting of fan by MBT and formation of number of small lakes.     

地震作用下岩质边坡倾倒破坏分析

倾倒破坏是陡倾层状岩体边坡一类主要的变形破坏形式,地震作用下岩质边坡块体倾倒破坏分析具有重要的工程指导意义。基于块体极限平衡,针对岩块长细比较大的情况,推导出了地震作用下岩质边坡倾倒破坏的一般解析解。对于简单的反倾边坡,给出了地震作用下倾倒破坏的显式解析解,并推导了岩块间法向力、破坏模式转变点和坡脚剩余下滑力计算公式。通过4个典型算例研究了地震作用对反倾边坡破坏模式、倾倒破坏时所允许的最大陡倾节理视倾角、破坏模式转变点和坡脚剩余下滑力的影响,为反倾边坡的抗震支护设计提供了理论基础。最后,根据地震影响系数与破坏模式转变点和坡脚剩余下滑力的定量关系对比分析了解析法与传递系数法,结果显示,当岩块长细比大于20时,解析法具有足够的计算精度。     

岩质顺层边坡的平面滑移破坏机制分析

沿岩层层面的平面滑动破坏是顺层边坡发生最多、规模很大的一种破坏模式,根据其顺层滑移的力学机制将平面破坏分为滑移-拉裂型和水力驱动型两种类型。根据平面刚体模型,给出了滑移-拉裂型滑坡的失稳判据,即滑坡的条件为边坡高度要大于临界高度。地下水在顺层边坡后缘张裂隙和滑动面形成的渗流通道中运动时,对滑体将产生3个方面的力学作用：张裂隙静水压力、滑动面扬压力和拖曳力。根据水力-驱动型滑坡的计算分析表明,边坡后缘张裂隙充水高度直接决定了3种水压力的大小,当张裂隙充水高度达到临界值后,边坡在水压力作用下发生滑移破坏。     

基于R型因子分析法的滑坡发育影响因素分析

以陕西省岚皋县境内滑坡为研究对象,借助R型因子分析法,对滑坡发育的影响因素进行分析研究。结果表明:起主导作用的主项因素按照其影响作用的大小依次为滑坡前缘河流影响距、人类工程活动、地形地貌和控滑结构面; 影响较大的分项因素按照其影响作用的大小依次为滑坡体前缘河流影响距、开挖坡脚、原始斜坡坡向、控滑结构面倾向、耕地（占坡体百分比）和滑坡体碎石含量。结合影响滑坡发育的主项因素和分项因素,综合确定影响滑坡发育的主控因素按照其影响的作用大小依次为河流影响距、开挖坡脚、原始斜坡坡向、控滑结构面倾向。该问题的研究不仅可以为滑坡灾害的分析提供新的方法,而且对滑坡灾害的防灾减灾提供了一种新思路。     

Identification of deformation and failure characteristics in cataclinal slopes using physical modeling

This study investigates the deformation characteristics of cataclinal slopes in central Taiwan prior to landslide failure. Field surveys and physical model tests were performed to explain the gravitational deformation characteristics of cataclinal slopes under various conditions and to derive the deformation process and failure characteristics. The results show that the distribution of erosion gullies (different length of the slope mass), the extent of erosion (different thickness of the slope mass), the foliation dip angle, and the geological material critically affect the deformation of cataclinal slope masses in the study area. The results of physical model tests indicate that increasing the foliation dip angle, the thickness and the length of sliding mass, particle size (spacing between foliations) increases the depth of slope deformation. Foliation dip angle is the most critical factor that controls the deformation of slate slopes. When the cataclinal slopes reached maximum deformation, a shear failure and translational slide occurred within a short period. The deformation zone exhibited significant cracking at the scarp and the bulging of the slope toe, which facilitated the infiltration of surface water and groundwater, accelerating the deformation to failure.