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1.
Sassa and others in the Disaster Prevention Research Institute (DPRI), Kyoto University, developed a series of undrained ring-shear apparatus to physically simulate landslide initiation and motion, from DPRI-3 (Sassa 1992) to DPRI-7 (Sassa et al., Landslides 1(1):7–19, 2004). The maximum undrained capacities in the DPRI series ranged from 300 to 650 kPa. Sassa and others in the International Consortium on Landslides (ICL) have developed a new series of undrained ring-shear apparatus (ICL-1and ICL-2) for two projects of the International Programme on Landslides (IPL-161 and IPL-175). Both projects are supported by the Science and Technology Research Partnership for Sustainable Development Program (SATREPS) of Japan. ICL-1 was developed to create a compact and transportable apparatus for practical use in Croatia; one set was donated to Croatia in 2012. ICL-2 was developed in 2012–2013 to simulate the initiation and motion of megaslides of more than 100 m in thickness. The successful undrained capacity of ICL-2 is 3 MPa. This apparatus was applied to simulate possible conditions for the initiation and motion of the 1792 Unzen–Mayuyama megaslide (volume, 3.4?×?108 m3; maximum depth, 400 m) triggered by an earthquake. The megaslide and resulting tsunami killed about 15,000 people. The Unzen Restoration Office of the Ministry of Land, Infrastructure and Transport (MLIT) of Japan systematically collected various papers and reports and published two summary leaflets: one in English in 2002 and an extended version in Japanese in 2003. Samples were taken from the source area (for initiation) and the moving area (for motion). The hazard area was estimated by the integrated landslide simulation model LS-RAPID, using parameters obtained with the ICL-2 undrained ring-shear apparatus. The estimated hazard area agrees reasonably with the landslide moving area reported in the Ministry leaflets.  相似文献   

2.
The 2008 Ms 8.0 Wenchuan earthquake triggered a large number of extensive landslides. It also affected geologic properties of the mountains such that large-scale landslides followed the earthquake, resulting in the formation of a disaster chain. On 10 July 2013, a catastrophic landslide–debris flow suddenly occurred in the Dujiangyan area of Sichuan Province in southeast China. This caused the deaths of 166 people and the burying or damage of 11 buildings along the runout path. The landslide involved the failure of ≈1.47 million m3, and the displaced material from the source area was ≈0.3 million m3. This landslide displayed shear failure at a high level under the effects of a rainstorm, which impacted and scraped an accumulated layer underneath and a heavily weathered rock layer during the release of potential and kinetic energies. The landslide body entrained a large volume of surface residual diluvial soil, and then moved downstream along a gully to produce a debris flow disaster. This was determined to be a typical landslide–debris flow disaster type. The runout of displaced material had a horizontal extent of 1200 m and a vertical extent of 400 m. This was equivalent to the angle of reach (fahrböschung angle) of 19° and covered an area of 0.2 km2. The background and motion of the landslide are described in this study. On the basis of the above analysis, dynamic simulation software (DAN3D) and rheological models were used to simulate the runout behavior of the displaced landslide materials in order to provide information for the hazard zonation of similar types of potential landslide–debris flows in southeast China following the Wenchuan earthquake. The simulation results of the Sanxicun landslide revealed that the frictional model had the best performance for the source area, while the Voellmy model was most suitable for the scraping and accumulation areas. The simulations estimated that the motion could last for ≈70 s, with a maximum speed of 47.7 m/s.  相似文献   

3.
The distinctive bathymetric feature exists in the Suruga Bay, Japan. It has been called as Senoumi (Stone flower sea) from old times. Senoumi is a 30?km wide and 20?km long concave feature. Its origin has not been explained yet; however, the feature might be a combined consequence of intensive tectonic activity in the plate border, landslides, and a submarine flow coming from the Oi River. If the Senoumi was caused by a landslide, the latter would be larger than any on-land landslide in Japan. The downshelf “exit” from this feature is much narrower than its central part. This is not usual shape of landslides, but it is similar to the liquefied landslides such as those in quick clays which mobilize great strength reduction after failure. To study Senoumi as a landslide, the shear behaviors of the following three soil samples were investigated by the cyclic and seismic undrained stress control ring shear tests. One sample is volcanic ash taken from the base of landslide deposits (mass transport deposits), from 130 to 190?m deep layer below the submarine floor which was drilled and cored by the Integrated Ocean Drilling Program Expedition 333. Another two samples are the Neogene silty–sand and silt taken from the Omaezaki hill adjacent to the Senoumi, because the shear zone might have been formed in Neogene layers extending from on-land to the continental shelf. The largest strength reduction from peak to steady-state shear resistance in the undrained cyclic loading test was found in volcanic ash. The strength reduction in Neogene silty–sand was smaller than volcanic ash, while the Neogene silt mobilized the least post-failure strength reduction. An integrated model simulating the initiation and motion of earthquake-induced rapid landslides (landslide simulation (LS)-RAPID, Sassa et al. Landslides 7–3:219–236, 2010) was applied to this study. The steady-state shear resistance and other geotechnical parameters measured by the undrained ring shear tests and the greatest strong motion record in the 2011 off-the-Pacific Coast of Tohoku earthquake (M w 9.0), also known as “2011 Tohoku Earthquake” at the observation point MYG004 (2,933?gal) were input to this model. As the result, it was found that landslides would be triggered by 0.30–1.0 times of MYG004 in volcanic ash, 0.4–1.0 times of MYG004 in Neogene silty–sand and Neogene silt, though the depth and area of triggered landslides were different in soils and intensity of shaking. Feature, created by LS-RAPID using the parameters of volcanic ash, was most similar to the Senoumi in depth and extent. The result obtained from this study includes a hypothesis to be proved, but presents the strong need to investigate the risk of the large-scale submarine landslides which could enhance tsunami wave and possibly enlarge the submarine landslide retrogressively into the adjacent coastal plain by the upcoming mega earthquake in the Nankai Trough.  相似文献   

4.
On 11 January 2013, a catastrophic landslide of ~0.2 million m3 due to a prolonged low-intensity rainfall occurred in Zhenxiong, Yunnan, southwestern China. This landslide destroyed the village of Zhaojiagou and killed 46 people in the distal part of its path. The displaced landslide material traveled a horizontal distance of ~800 m with a vertical drop of ~280 m and stopped at 1520 m a.s.l. To examine the possible mechanism and behavior of the landslide from initiation to runout, the shear behavior of soil samples collected from the sliding surface and runout path was examined by means of ring shear tests. The test results show that the shear strength of sample from the sliding surface is less affected by shear rate while the shear rate has a negative effect on the shear strength of runout path material. It is suggested that the source and runout path materials follow the frictional and Voellmy rheology, respectively. Post-failure behavior of the landslide was modeled by using a DAN-W model, and the numerical results show that the selected rheological relationships and parameters based on the results of ring shear tests may provide good performance in modeling the Zhenxiong landslide.  相似文献   

5.
Extreme heavy rainfall due to Typhoon Talas on September 2–4, 2011 in the Kii Peninsula, Japan, triggered numerous floods and landslides. This study investigates the mechanism and the entire process of rainfall-induced deep-seated landslides forming two massive dams in the Kuridaira and Akatani valleys, respectively. The mechanism of the rapid deep-seated landslides is examined through a series of laboratory experiments on samples from sliding surfaces by using undrained high-stress dynamic-loading ring-shear apparatus. The test results indicate that the failure of samples is triggered by excess pore water pressure generation under a shear displacement from 2 to 7 mm with a pore pressure ratio ranging from 0.33 to 0.37. The rapid movement of landslides is mainly attributed to high mobility due to the liquefaction behavior of both sandstone-rich and shale samples. Geomorphic settings and landslide mobility are major contributing factors to the dam formation. Additionally, shear displacement control tests show that a certain amount of shear displacement between 2 and 7 mm along the sliding surfaces of the gravitationally deformed slopes might have led to the failures. Importantly, computer simulation with LS-RAPID software using input parameters obtained from physical experiments is employed to interpret the entire formation process of the abovementioned two landslide dams. The simulation results are examined in accordance with the observed on-site geomorphic features and recorded data to explain the possibility of sliding processes. The results further point out that local failures are initiated from the lower middle part of the landslide bodies where the geological boundary exists. This condition most probably influences the landslide initiation in the two case studies. This research is therefore helpful for hazard assessment of slopes that are susceptible to deep-seated landslides and other sequential processes in areas with geology and geomorphology similar to that of the Kii Peninsula.  相似文献   

6.
A calamitous landslide happened at 22:00 on September 1, 2014 in the Yunyang area of Chongqing City, southwest China, enforcing the evacuation of 508 people and damaging 23 buildings. The landslide volume comprised 1.44 million m3 of material in the source area and 0.4 million m3 of shoveled material. The debris flow runout extended 400 m vertically and 1600 m horizontally. The Xianchi reservoir landslide event has been investigated as follows: (1) samples collected from the main body of landslide were carried out using GCTS ring shear apparatus; (2) the parameters of shear and pore water pressure have been measured; and (3) the post-failure characteristics of landslide have been analyzed using the numerical simulation method. The excess pore-water pressure and erosion in the motion path are considered to be the key reasons for the long-runout motion and the scale-up of landslides, such as that at Xianchi, were caused by the heavy rainfall. The aim of this paper is to acquired numerical parameters and the basic resistance model, which is beneficial to improve simulation accuracy for hazard assessment for similar to potentially dangerous hillslopes in China and elsewhere.  相似文献   

7.
陕西华县高楼村黄土滑坡泥流的成因分析   总被引:2,自引:0,他引:2  
滑坡泥流具有高速远程运动的特点,一般先形成滑坡,随即转为高速泥流,虽不多见,但破坏性大。陕西华县高楼村黄土滑坡泥流是一个由于引水渠漏水引起的典型案例。对滑坡形成区后壁黄土的物理性质测试表明,可转化为泥流的滑坡具有疏松的结构,一般饱和含水率大于液限。对其在饱和状态的三轴固结不排水试验表明,试样在很小应变下发生剪缩,产生较高的超孔隙水压力,超孔隙水压力达到一定程度,使其由固态转化为流态,从而形成快速、远距离的流动。当边坡被引水渠渗漏的水浸湿,潜在滑带几乎处于饱和时,在静水压力作用下,其稳定性接近临界状态; 一旦开始破坏,剪力作用下疏松的结构发生剪缩,沿滑动带产生较高的超静孔隙水压力,导致滑带呈流态高速下滑,此时的滑带只有很低的强度,因此沿着坡度较陡的沟底保持高速流动,到沟口平坦处势能完全释放后才停滞。用Sassa K.滑坡运动模型,对该滑坡的运动过程模拟,模拟结果与现场实测滑坡发生后的地形较为一致。  相似文献   

8.
陕西泾阳东风高速远程黄土滑坡运动过程的模拟   总被引:1,自引:0,他引:1  
陕西泾阳南塬的东风滑坡是一个典型的高速远程黄土滑坡,由于斜坡顶部的黄土台塬长期灌溉所诱发。通过野外调查,采取滑坡后缘斜坡的黄土试样,对斜坡中部的Q2黄土做天然含水率的固结不排水剪试验,对斜坡底部地下水位面附近的Q1黄土做饱和固结不排水剪试验,结果表明非饱和的Q2黄土和饱和的Q1黄土在破坏后都具有显著的应力降,但前者是由结构强度引起,而后者则是由剪切形成的超孔隙水压力引起,由此表明该斜坡一旦破坏,就会有较高的启动速度。对滑坡坡脚以外一级阶地上的砂卵层做环剪慢剪试验,测得其有效残余摩擦角,根据滑坡各部分含水状态给定孔隙水压力参数,利用Sassa. K滑坡运动模型对该滑坡运动过程进行模拟,从模拟结果反映出滑坡运动过程中的覆盖范围和速度的变化,模拟的滑坡运动距离和覆盖范围与实测比较吻合,最高速可达到37m s-1,为高速滑坡。黄土滑坡以高的初速度下滑到坡脚下一级阶地上的饱和砂卵层上,砂卵层上液化是导致其远程运动的主要原因。  相似文献   

9.
The Sanxicun landslide occurred on July 10, 2013, in Sanxicun Village, which is located in Dujiangyan City, Sichuan Province, China. It travelled up to 1200 m, destroyed 11 houses, and killed 166 people in the village. To explain how this landslide could travel such a large distance and cause such serious damage, this study used a thermo-poro-elastic approach coupled with the Savage–Hutter model to simulate the dynamic process of the Sanxicun landslide. The simulated results were compared with the actual results, as well as those of other researchers. It showed that the simulated results for the landslide profile and mass accumulation scope were basically consistent with the actual results. The simulated landslide runout was 1242 m, which was quite close to the actual value. The simulated maximum mass accumulation thickness was 16.4 m. The maximum velocity was 32.6 m/s, which was between those calculated by Yin et al. (J Eng Geol 22(2):309–318, 2014), Yin et al. (Landslide 13:9–23, 2016), and the various trends were found to be consistent. The temperature change and the pore water pressure evolution in the shear zone during sliding are also obtained by simulation. This study had recreated the Sanxicun landslide motion process from the view of thermo-poro-elastic coupling within the shear zone.  相似文献   

10.
侵蚀作用诱发黄土滑坡的机制研究   总被引:1,自引:0,他引:1  
侵蚀作用诱发的黄土滑坡是黄土高原区域内一种主要的滑坡类型,对其破坏机制开展深入研究具有重要实际意义。以陕西省耀州区的庵里滑坡为例,对该类黄土滑坡的发生机制进行分析和探讨,建立了滑坡发生前侵蚀作用的不同阶段边坡的有限元模型,计算了相应的应力场和位移场,在此基础上求得各模型沿最终滑面上的正应力、剪应力和抗剪强度分布,采用极限平衡法计算边坡整体稳定系数。结果表明,随着侵蚀作用的不断加深,沿滑动面上的剪应力增大,抗剪强度减小,整体稳定性降低至最终破坏。试验结果表明,小的应变在饱和黄土中会产生显著的超孔隙水压力,因此,基岩面上饱和滑带中的超孔隙水压力加剧了该类滑坡的发生。比较滑面上的剪应力和抗剪强度发现,自前滑坡破坏从坡脚开始,向后逐步扩展,表明该类滑坡具有牵引式破坏特点。  相似文献   

11.
本文的主要目的是探讨地震诱发的高速远程滑坡的液化机理。通过排水和不排水环剪的对比试验,以及对地震诱发的不同类型的滑坡实例的现场调查,考察了土结构破坏和土粒子破碎产生的滑动带液化的不同机理。土结构破坏引起的液化在滑坡发生时即可产生,而土粒子破碎引起的液化需要在滑动过程中产生。在此基础上提出了滑动带向滑体内的扩展模型,并分析了两种液化机理引起的滑坡体形态的差异。本文的独到之处在于揭示了土粒子破碎对高速远程滑坡的重要影响,强调了在滑坡灾害预测研究中必须同等重视滑坡体结构和土粒子易破碎性的调查分析。  相似文献   

12.
高速远程地震黄土滑坡发生机制试验研究   总被引:2,自引:1,他引:1  
1920年海原大地震触发了多处典型高速远程地震黄土滑坡,本文在对西吉党家岔滑坡进行野外调研的基础上,采集了具有代表性的滑带土作为试验样品,以1940年5月18日美国帝国谷强震记录作为波动输入,利用DPRI环剪试验机,对该滑坡的发生机制进行了一系列环剪试验研究。结果表明,地震发生时,坡体潜在滑面的滑带土在强震作用下发生的滑动面液化(Sliding surface liquefaction)现象是导致高速远程滑坡形成的一个重要因素。伴随着滑动面液化过程,滑体产生了逐渐增大的剪切位移及孔隙水压力(地震力作用结束瞬间已分别达到2.03m及104kPa),并获得了较大的速度,为高速远程滑坡的发生提供了条件。  相似文献   

13.
Rapid debris flows are among the most destructive natural hazards in steep mountainous terrains. Prediction of their path and impact hinges on knowledge of initiation location and the size and constitution of the released mass. To better link mass release initiation with debris flow paths and runout lengths, we propose to capitalize on a newly developed model for rainfall-induced landslide initiation (“Catchment-scale Hydro-mechanical Landslide Triggering” CHLT model, von Ruette et al. 2013) and couple it with simple estimates of debris flow runout distances and pathways. Landslide locations and volumes provided by the CHLT model are used as inputs to simulate debris flow runout distances with two empirical- and two physically-based models. The debris flow runout models were calibrated using two landslide inventories in the Swiss Alps obtained following a large rainfall event in 2005. We first fitted and tested the models for the “Prättigau” inventory, where detailed information on runout path was available, and then applied the models to landslides inventoried from a different catchment (“Napf”). The predicted debris flow runout distances (emanating from CHLT simulated landslide positions) were well in the range of observed values for the physically-based approaches. The empirical approaches tend to overestimate runout distances relative to observations. These preliminary results demonstrate the added value of linking shallow landslide triggering models with predictions of debris flow runout pathways for a range of soil states and triggering events, thus providing a more complete hazard assessment picture for debris flow exposure at the catchment scale.  相似文献   

14.
A mathematical model is developed for the dynamic analysis of earthquake‐triggered rapid landslides, considering two mechanically coupled systems: (a) the accelerating deformable body of the slide and (b) the rapidly deforming shear band at the base of the slide. The main body of the slide is considered as a one‐phase mixture of Newtonian incompressible fluids and Coulomb solids sliding on a plane of variable inclination. The evolution of the landslide is modeled via a depth‐integrated model of the Savage–Hutter type coupled with: (a) a cyclic hysteretic constitutive model of the Bouc–Wen type and (b) Voellmy's rheology for the deformation of the material within the shear band. The original shallow‐water equations that govern the landslide motion are appropriately reformulated to account for inertial forces due to seismic loading, and to allow for a smooth transition between the active and the passive state. The capability of the developed model is tested against the Higashi–Takezawa landslide. Triggered by the 2004 Niigata‐ken Chuetsu earthquake, the slide produced about 100m displacement of a large wedge from an originally rather mild slope. The mechanism of material softening inside the shear band responsible for the surprisingly large run‐out of the landslide is described by a set of equations for grain crushing‐induced pore‐water pressures. The back‐analysis reveals interesting patterns on the flow dynamics, and the numerical results compare well with field observations. It is shown that the mechanism of material softening is a crucial factor for the initiation and evolution of the landslide, while viscoplastic frictional resistance is a key requirement for successfully reproducing the field data. Copyright © 2009 John Wiley & Sons, Ltd.  相似文献   

15.
In the village of Donghekou (in Qingchuan County, Sichuan Province, China), a major landslide was triggered by the Wenchuan earthquake in 2008 with more than 10 × 106 m3 of rock displaced. The kinematic behavior of this landslide is simulated using a 2D discrete element model. The numerical model used in this work is composed of discs bonded together. The initial boundary conditions are applied along the ball–wall contacts by using an initial velocity estimated from the strong motion data. The constraints are mainly issued from the final geometry of the landslide including its capacity to dam the river. The modeling thus indicates that a low friction coefficient (about 0.1) is required to account for the actual landslide characteristics. The runout behaviors are analyzed and some useful conclusions are drawn.  相似文献   

16.
2008年汶川地震触发的大光包滑坡滑带形成背景是渗水层间错动带,该带强度变化是决定滑坡启动的主要因素,动孔压发展是土体材料强度劣化的根本原因,故基于系列室内动三轴试验研究该带材料孔压特性。结果表明,动载下层间错动带材料孔压快速增长,循环剪应力比越大,孔压增长越快,不同荷载条件下应变达到5%时动孔压比等于1,材料液化,根据动孔压比与振次比曲线的拟合关系提出幂函数应力模型。从能量角度描述层间错动带材料孔压增长特性,揭示出循环剪应力比对累积能量耗损与动孔压比曲线影响较小而围压对其影响较大,并进一步提出孔压增长的能量模型。  相似文献   

17.
By combining landslide dynamics research and tsunami research, we present an integrated series of numerical models quantitatively simulating the complete evolution of a landslide-induced tsunami. The integrated model simulating the landslide initiation and motion uses measured landslide dynamic parameters from a high-stress undrained dynamic-loading ring shear apparatus. It provides the numerical data of a landslide mass entering and moving under water to the tsunami simulation model as the trigger of tsunami. The series of landslide and tsunami simulation models were applied to the 1792 Unzen-Mayuyama megaslide and the ensuing tsunami disaster, which is the largest landslide disaster, the largest volcanic disaster, and the largest landslide-induced tsunami disaster to have occurred in Japan. Both the 1792 megaslide and the tsunami portions of the disaster are well documented, making this an excellent test of the reliability and precision of the new simulation model. The simulated tsunami heights at the coasts well match the historical tsunami heights recorded by “Tsunami-Dome-Ishi” (a stone showing the tsunami reaching point) and memorial stone pillars.  相似文献   

18.
于国强  张茂省  张成航 《地质通报》2015,34(11):2100-2107
滑坡启动机理研究是滑坡防治的前提条件。应用三维连续介质动态数值模型方法,采用摩擦模型、Voellmy模型2种流变模型,对滑坡启动过程进行分析求解,开展滑坡启动机理数值模拟研究。结果表明,不论是限制坡面(渠道型)还是无限制坡面,在2种流变模型和侵蚀率下,随着坡度逐渐增加,地形所提供给滑坡体的能量进一步增大,物质运动距离进一步增加,其相应的平均速度、最大速度(前端速度)和总动能也会进一步加大,经历了从缓慢蠕变至快速增加的过程。根据不同坡度下滑坡的启动、运动规律、堆积过程及各坡度下动力参数延程变化规律,可以将滑坡的启动坡度设定为25°~30°。该滑坡启动坡度的设定可为地质灾害防治措施和监测预警提供技术参考。  相似文献   

19.
合理的流变参数选取对准确刻画泥石流、高速远程滑坡运动过程和动力行为至关重要。本研究基于三维连续介质动态数值模型,构建Voellmy流变模型,结合方差分析方法,比较了不同流变参数对泥石流运动行为的影响程度。结果表明:动力底摩擦角和湍流系数均会对泥石流与高速远程滑坡的动力特征产生一定的影响,但影响程度各异。较大的动力底摩擦角会产生更大、更快的能量耗散过程,使得运动过程整体滞后;较高的湍流系数增加了流体层之间的动量交换强度,具有较大的与周围界质混合的能力,对周围介质的卷吸作用增大。物源区体积(湍流系数)在一定程度上仅影响泥石流运动速度,对致灾范围和规模影响作用不大。沟道下垫面情况、颗粒物组成、孔隙水压力(底摩擦角)与灾害体流速、移动距离和堆积区体积、面积关系很密切,在很大程度上影响泥石流、滑坡强度,致灾范围和规模。研究成果以期为流变参数选取提供很好的借鉴方法,也为地质灾害防治提供一定的技术参考。  相似文献   

20.
2008年汶川Ms8.0级强震触发了体积近12×108 m3的大光包滑坡。该滑坡发生于古生代碳酸盐岩地层,滑带地质背景为斜坡内部深埋400 m、最大厚度达5 m的先期层间构造错动带。最新调查表明,该错动带是斜坡内部地下水通道,错动带岩体处于饱和状态。为揭示强震过程与地下水相关的大光包滑坡启动机制,提出了一种具有软弱层带的硬质碳酸盐岩边坡简化模型,将层间构造错动带概化为碳酸盐岩硬层内部软弱层带,采用FLAC3D程序中的流固耦合算法模拟了模型的响应特性。研究结果表明:强震过程中软弱层带上下碳酸盐岩硬层的变形响应时间、波型、大小出现明显差异,上硬层相对于下硬层产生了张离、压缩和剪切3种非协调变形模式,由此对软弱层带产生了振动冲压-张拉和振动剪切动力学行为,饱水软弱层带形成了具有瞬间放大和累积增涨特征的超孔隙水压力。这里将上下硬层差异性变形称为非协调变形,认为非协调变形是软弱层带应力放大成因,推测软弱层带应力瞬间放大以及放大应力长持时作用下的岩体致损是超孔隙水压力激发和累积的成因;强震过程软弱层带超孔隙水压力导致其内有效应力快速降低,使得斜坡前部锁固段应力快速集中,而后被突然剪断,滑坡骤然启动,揭示了强震过程中超孔隙水压力是大光包滑坡启动的主要原因。  相似文献   

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