Strumenti personali
Tu sei qui: Portale Projects Landslides SNAC experiments
Azioni sul documento

3D simulation of landslide failure and incipient runout

creato da Colin StarkUltima modifica 18/03/2009 20:48

Explanation of SNAC elastoplastic deformation modeling of slope failure.

Colin P. Stark, Lamont-Doherty Earth Observatory, cstark@ldeo.columbia.edu
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

    
Strain rate



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.

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.


Sviluppato con Plone, il sistema open source di gestione dei contenuti