DEFORESTATION AROUND THE WORLD - India Environment Portal
DEFORESTATION AROUND THE WORLD - India Environment Portal
DEFORESTATION AROUND THE WORLD - India Environment Portal
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Landslides Caused Deforestation<br />
rainfall threshold is a power-law curve that fit the points in the scatter plot (actually a lower<br />
envelope in that is a point lies to the right upper of the curve, landslides may occur), usually<br />
b<br />
take the form I aD <br />
, where a and b are positive constants that vary with soil, vegetation<br />
and land use.<br />
Godt et al. (2006) suggested that landslide-triggering rainfall must be considered in terms of<br />
its relationship with antecedent rainfall. For example, a heavy rainfall event within a dry<br />
period is not likely to trigger shallow landslides, while the opposite is true for lighter<br />
rainfall within a wet period. As it directly affects soil moisture conditions, Godt et al. (2006)<br />
correctly claim that antecedent rainfall must be included in an empirical model’s assessing<br />
of a rainfall’s potential in causing landslide. Godt et al. (2006) therefore is a significant<br />
improvement over Caine’s (1980) seminal rainfall intensity-duration threshold line<br />
approach. The antecedent rainfall index is usually defined as a red noise of the accumulative<br />
rainfall amount 3 days (for tropics) and 7 days (temperate climate zone) prior the landslide<br />
event. Recent empirical methods also compile many soil hydrological parameters by using<br />
water-balance models with little physical basis but are convenient for estimating soil<br />
moisture conditions. For example, Godt et al. (2006) uses a detailed assessment of rainfall<br />
triggering conditions, hill slope hydrologic properties, soil mechanical properties, and slope<br />
stability analyses. The accumulation of sliding material is a slow process (either rockfalls or<br />
aeolian processes or damaging erosion processes from weathering) compared with the<br />
sliding. Previous sliding will reshape the sliding material profile and may even completely<br />
remove the sliding layer. These will increase the stability of the slope and a similar rainfall<br />
amount may cause sliding on a reduced scale, or not at all. Thus, the empirical parameters (a<br />
and b) in the ID approach vary not only spatially but also temporally. In this sense, all<br />
previous ID approaches still lack the important time varying features.<br />
A synthetic consideration of preparatory and triggering factors, however, demands a more<br />
comprehensive modeling of the physical processes involved in landslides (Costa, 1984;<br />
Iverson, 1997). The overview by Iverson (1997) suggested several criteria for dynamic<br />
landslide models, including that a model should be capable of simulating the full startmovement-spread-cessation<br />
cycle of the detached material, and should cover a wide<br />
spectrum of debris flows. With continued growth and expansion of human population, raintriggered<br />
shallow landslides increasingly result in loss of life and significant economic cost.<br />
From an ecological viewpoint, landslides are an important factor in desertification over<br />
mountainous regions because they are very effective in transferring biomass from live to<br />
dead respiring pools (Ren et al., 2009).<br />
Along these lines of walking, there are physically-based slope stability models to simulate<br />
the transient dynamical response of pore pressure to spatiotemporal variability of rainfall<br />
(e.g., Transient Rainfall Infiltration and Grid-based Regional Slope-Stability Analysis—<br />
TRIGRS, Baum et al. 2008); commercially available numerical modeling codes for<br />
geotechnical analysis of soil, rock and structural support in three dimensions (e.g., FLAC-<br />
3D, www.itascacg.com/flac3d), and fully three dimensional, full Navier-Stokes and multirheological<br />
modeling systems such as the scalable, extensible geo-fluid model, known as<br />
SEGMENT (Ren et al., 2008; Ren et al., 2009, Ren et al. 2010; Ren et al. 2011a,b).<br />
Slope stability models are based on the following reasoning: On a sloping surface, the<br />
gravitational force can be partitioned into a component normal to the slope (Fn),<br />
contributing to friction that resists sliding erosion, and a component parallel to the slope (Fp)<br />
that promotes sliding. A stability parameter, S, is defined as SF / F , where is the<br />
n p<br />
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