3D simulation of landslide failure and incipient runout
Explanation of SNAC elastoplastic deformation modeling of slope failure.
Eunseo Choi, Lamont-Doherty Earth Observatory, echoi@ldeo.columbia.edu
Matteo Convertino, IMAGE Dept., Univ. of Padova, convertino@idra.unipd.it
Landslides are a major environmental hazard and a
fundamental process in the erosion of mountain landscapes. In both contexts, a major question is this: if a slope fails, how big will the landslide be?
The question is a challenging one to study
in the field or model numerically, because landslide volumes span many orders
of magnitude and frequency, and because the mechanisms that control failure
geometry are a matter of debate. We
are conducting a pilot study to see whether this issue can be addressed through
the modeling of large ensembles of landslide failures in 3D. We have chosen to use SNAC (Choi et al., 2008) and its ability to simulate
the deformation of a heterogeneous Mohr-Coulomb material prone to strain weakening.
SNAC model landslide Visualization of strain rate 2+1D parallelized simulation | | |
Our aim is to generate ~100 realizations
of incipient slope failure given stochasticity in the governing physical and
topographic properties. Of particular
interest are: (1) complexity in the way in which landslide ruptures grow; (2)
how strain weakening mechanisms and heterogeneity distributions affect the
structure of deformation; (3) the nature of scaling relations between length,
depth, area and volume. These results
will be compared with observations of landslide structures, variability and
scaling to determine the quality of the modeling. Armed with these insights, we will then be
able to evaluate the practicality and efficacy of a larger project (>1000
realizations) to study what controls the probability distribution (PDF) of
landslide volumes.
In terms of testing specific hypotheses, we will be able to discriminate between the idea of Katz & Aharonov (2006) that the PDF is a mix of two types of landslide generated in different ways and at two distinct scale ranges, and the model of Stark & Guzzetti (2009) that the PDF and its power-law scaling is the result of a single stochastic process of rupture propagation.
In terms of SNAC/CIG code development, at the time of
writing we have built a new SNAC plugin called hillSlope to handle model domain geometry, material heterogeneity,
and simulation tracking. In addition we
have made improvements to post-processing tools. These adaptations are currently undergoing
testing on TeraGrid Ranger (project# TG-EAR090034).
Simulations
- Pilot 2+1D experiment: hillslope17
- First successful SNAC simulation of landslide failure. Only 2+1D rather than true 3D. Domain: 395m x 100m x 5m. Cells: 5m at surface. Elastic constants: 10^7 Pa. Weak points: uniform seeding in subdomain spanning whole slope (276.5m) and 80m depth. SNAC revision 14173.
- Pilot parallelized 2+1D experiment: hillslope24
- First successful run on TeraGrid Ranger. Parallelized with 16 cores
solving as 16 vertical (y) layers. Computational domain size: Nx=200,
Ny=49, Nz=2 (mesh nodes). Physical domain size: Lx=398m, Ly=96m,
Lz=2m. Element size at surface: 2x2x2m^3. Elastic equilibration
achieved at t=9638. Plastic deformation during t=9501-12001. Simple uniform weak point seeding in
top-central subdomain. SNAC revision 14232
- Example high-resolution, parallelized 2+1D experiment: plastic_highres2d
- Example large-scale model run on TeraGrid Ranger. Parallelized with 64 cores
solving as 16 horizontal (x) by 4 vertical (y) blocks. Computational domain size: Nx=577,
Ny=128, Nz=2 (mesh nodes). Physical domain size: Lx=576m, Ly=128m,
Lz=1m. Element size at surface: 1x1x1m^3. Elastic equilibration
deemed to be achieved at t=60001. Plastic deformation evaluated for span t=60001-64410, which takes 8299 CPU seconds. Simple uniform weak point seeding in
top-central subdomain with relatively low imposed cohesion (weak) and thus rapid deformation. SNAC revision 14300 with minor plastic reporting mod.
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References
Choi, E., L. Lavier, and M. Gurnis. Thermomechanics of mid-ocean ridge segmentation, Phys. Earth Planet. Interiors, 171(1-4): 374-386, doi:10.1016/j.pepi.2008.08.010, 2008.
Katz, O., and E. Aharonov. Landslides in vibrating sand box: What controls types of slope failure and frequency magnitude relations?, Earth and Planetary Science Letters, 247(3–4): 280–294, doi:10.1016/j.epsl.2006.05.009, 2006.
Stark, C.P., and F. Guzzetti. Landslide rupture, area and volume distribution, and debris mobilization, Jour. Geophys. Res., in review, 2009.