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Geoengineer.org has gathered and presented educational material on the following Slope Stability topics:
Slopes are typically categorized in two types: natural and artificially-made slopes. Natural slopes are formed due to physical processes that include plate tectonics and weathering/erosion of rock masses that result in material deposition. Artificially-made slopes are established to facilitate infrastructure projects, ex., embankments, earth dams, road cuttings etc.
The stability of a slope is of critical importance in Geotechnical Engineering applications. A slope movement (also referred as a landslide) can lead to severe issues including infrastructure damage or/and casualties. Slope stability depends on the capability of the soil mass to withstand its gravitational forces, the additional loads acting on the slope, as well as potential dynamic loads (such as that of an earthquake).
A common misconception is that landslides occur in steep and remote slopes and do not actually impact human infrastructure. However, statistics show that most of world’s regions are impacted by (at least) some types of landslide phenomena that can be triggered by several factors including erosion, precipitation, earthquakes, human activity etc.
Landslides may occur rapidly or progress steadily at a fixed rate. They are common in soils and rockmasses with poor mechanical properties (highly fractured or weathered). However, a landslide can be triggered also by deformations along discontinuity layers of strong rocks. The nature and type of landslide phenomena are complex and are further analyzed below.
The most common and complete classification system of landslides is that provided by Varnes (1978), who introduces a system that requires the definition of the landslide material and the type of the movement induced. The ground materials are distinguished in 5 categories:
The 5 types of landslide movements that can be observed are categorized as following:
Slides refer to ground movements along a specified surface or zone of weakness. A slide occurs when the shear stress applied along a surface overcomes its shear strength. The failure may propagate progressively initiating from a local failure zone. The main body of the slide will move downwards separating the stable from the unstable ground.
There are two main types of slides: rotational and translational slides. In rotational slides, the failure surface is curved inwards and points upwards and the landslide mass is approximately rotating around an axis transverse to the slide movement and parallel to the surface of the ground. The movement is usually associated with shear failure of the ground with its 3-dimensional geometry being “spoon-shaped”. Certain features are defined to characterize a rotational slide as shown in Figure 3. The surface of rupture is the zone in which the ground material slides. The main scarp refers to a relatively steep edge at the head of the landslide that reveals the undisturbed ground and the visible component of the rupture surface. The crown is the area above the main scarp that has not moved downwards. The main body of the slide is the entire soil mass that has slipped along the failure surface. The head is the upper section of the slide between the main scarp and the displaced ground material. The toe is the most distanced part from the main scarp where landslide material has accumulated and the foot refers to the part of the failed material that has been deposited over the initial ground surface.
Figure 3: Main features of a rotational landslide (USGS, 2004)
Nevertheless, sometimes the failure surface is controlled by pre-existing weakness planes (e.g., faults, fissures, cracks or joints). In this case, an engineering assessment must recognize those features since the failure would not be entirely controlled by the material’s shearing component. A rotational slide will eventually stop propagating as a stress equilibrium is restored with the mass movement. An example of a rotational slide is given in Figure 4.
Figure 4: The rotational Holbeck Hall landslide landslide, in Scarborough North Yorkshire, England (June 1993) (photo from British Geological Survey)
Translational slides occur along a pre-defined planar surface and the ground is subjected to no or little rotation. Translational slides are mainly controlled by weakness surfaces (joints, bedding planes etc.) or by the contact of materials with different shear strength. Theoretically, a translational slide may propagate indefinitely given that the rupture surface maintains its inclination and that its shear strength resistance remains lower that the driving force.
Figure 5. a) Illustration of a translational landslide (USGS, 2004) and b) Co-seismic translational landslide triggered in Japan in 2016 (Highland and Bobrowsky, 2018 by Khang Dang and Kyoji Sassa)
Lateral spreads are deformational phenomena caused by liquefaction, the process during which a saturated soil (usually sands) experiences loss of strength after a sudden change in its initial stress conditions. Therefore, the soil tends to behave more like a liquid than a solid. Such deformations occur on less steep slopes and are usually triggered by dynamic loads such as that of an earthquake. Lateral spreading is usually a progressive process that occurs mainly near shores, riverbanks, and ports where loose and saturated sandy soils exist. Infrastructure founded on those type of soils is prone to extensive damage (Figure 5).
Figure 5. a) An illustration of a translational landslide (USGS, 2004) and b) Lateral spreading example caused by an earthquake in Pakistan (Independent)
According to Varnes (1978), not all types of slope movements can be categorized in the aforementioned categories. There are certain landslide phenomena that take the form of slow or fast-moving flows. In rocks, there are types of slow movements that result in folding or bending. Due to the fact that these displacements resemble viscous fluids, they can be characterized as rock flows.
Regarding flows in soil materials, Varnes (1978) distinguished 5 main categories:
Figure 6: Illustration of a) debris flow, b) debris avalanche, c) earthflow and d) creeping flow (USGS, 2004)
Slope failures can be triggered by natural of human-induced causes, or a combination of the two. The natural causes of landslides include: gravitational forces that tend to destabilize the ground, water saturation, erosion, dynamic loads (e.g., earthquakes), the sudden uplift of the aquifer level, volcanic eruptions and freeze-thaw weathering cycles.
The presence of water is one of the most common factors that triggers landslides. Water saturation can be caused as a result of heavy precipitation, snow melt or changes in the ground water level. Water saturation reduces the shear strength of soils. In particular, it decreases the normal effective stress that acts between the grains and hence, the frictional resistance is reduced. The Mohr-Coulomb failure criterion suggests that the shear strength of the ground is proportional to the normal effective stress as:
Where t is the shear strength, σn is the effective stress, σt is the total stress, u is the pore-water pressure, c is the cohesion, and φ the friction angle.
Earthquakes are also triggering factors of landslides. Ground shaking imposes destabilizing horizontal and vertical loads (with the first being the most important) and can also result in liquefaction. Seismic shaking can also act as a contributing rather than a triggering factor as it may cause deterioration of the ground’s shear strength and destabilize the slope. The slope may subsequently be prone to landsliding in static conditions, for example after heavy precipitation, or when another earthquake occurs.
The human-induced causes of landslides are actions that can destabilize slopes, including: toe excavations, infrastructure loads acting on a slope, machine vibrations that apply dynamic loads, construction of weak embankments or earth dams, and deforestation that may exacerbate extensive flooding and debris/earth flows.
Conforti, M., Muto, F., Rago, V. and Critelli S. (2014). Landslide inventory map of north-eastern Calabria (South Italy), Journal of Maps, 10:1, 90-102, DOI: 10.1080/17445647.2013.852142
Corominas, J., Mavrouli, O. and Roger R.C. (2017). Rockfall Occurrence and Fragmentation. 75-97. 10.1007/978-3-319-59469-9_4.
GEER (2020). The September 18-20 2020 Medicane Ianos Impact on Greece - Phase I Reconnaissance Report. GEER-068, https://doi.org/10.18118/G6MT1T
Highland, L. and Bobrowsky, P. (2018). TXT-tool 0.001-2.1 Landslide Types: Descriptions, Illustrations and Photos. 10.1007/978-3-319-57774-6_1.
United States Geological Survey (2004). Landslide Types and Processes. Fact Sheet 2004-3072.
Varnes, D.J. (1978). Slope movement types and processes. In: Special Report 176: Landslides: Analysis and Control (Eds: Schuster, R. L. & Krizek, R. J.). Transportation and Road Research Board, National Academy of Science, Washington D. C., 11-33.
WG/WLI (1994). A suggested method for reporting landslide causes. Bull. Int. Assoc. Eng. Geol. 50 (1), 71e74.
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