
Landslide rupture and the probability distribution of mobilized debris volumes
Author(s) -
Stark C. P.,
Guzzetti F.
Publication year - 2009
Publication title -
journal of geophysical research: earth surface
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2008jf001008
Subject(s) - debris , landslide , geology , seismology , oceanography
Landslide‐driven erosion is controlled by the scale and frequency of slope failures and by the consequent fluxes of debris off the hillslopes. In this paper, we tackle the magnitude‐frequency part of the process and develop a theory of initial slope failure and debris mobilization that reproduces the heavy‐tailed distributions (probability density function or PDFs) observed for landslide source areas and volumes. Landslide rupture propagation is treated as a quasi‐static, noninertial process of simplified elastoplastic deformation with strain weakening; debris runout is not considered. The model tracks the stochastically evolving imbalance of frictional, cohesive, and body forces across a failing slope and uses safety factor concepts to convert the evolving imbalance into a series of incremental rupture growth or arrest probabilities. A single rupture is simulated with a sequence of weighted “coin tosses” with weights set by the growth probabilities. Slope failure treated in this stochastic way is a survival process that generates asymptotically power‐law‐tail PDFs of area and volume for rock and debris slides; predicted scaling exponents are consistent with analyses of landslide inventories. The primary control on the shape of the model PDFs is the relative importance of cohesion over friction in setting slope stability; the scaling of smaller, shallower failures, and the size of the most common landslide volumes, are the result of the low cohesion of soil and regolith, whereas the negative power‐law‐tail scaling for larger failures is tied to the greater cohesion of bedrock.