Modeling Seismic Cycles of Great Megathrust Earthquakes Across the Scales With Focus at Postseismic Phase

Subduction is substantially multiscale process where the stresses are built by long‐term tectonic motions, modified by sudden jerky deformations during earthquakes, and then restored by following multiple relaxation processes. Here we develop a cross‐scale thermomechanical model aimed to simulate th...

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Bibliographic Details
Published inGeochemistry, geophysics, geosystems : G3 Vol. 18; no. 12; pp. 4387 - 4408
Main Authors Sobolev, Stephan V., Muldashev, Iskander A.
Format Journal Article
LanguageEnglish
Published Washington John Wiley & Sons, Inc 01.12.2017
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Summary:Subduction is substantially multiscale process where the stresses are built by long‐term tectonic motions, modified by sudden jerky deformations during earthquakes, and then restored by following multiple relaxation processes. Here we develop a cross‐scale thermomechanical model aimed to simulate the subduction process from 1 min to million years' time scale. The model employs elasticity, nonlinear transient viscous rheology, and rate‐and‐state friction. It generates spontaneous earthquake sequences and by using an adaptive time step algorithm, recreates the deformation process as observed naturally during the seismic cycle and multiple seismic cycles. The model predicts that viscosity in the mantle wedge drops by more than three orders of magnitude during the great earthquake with a magnitude above 9. As a result, the surface velocities just an hour or day after the earthquake are controlled by viscoelastic relaxation in the several hundred km of mantle landward of the trench and not by the afterslip localized at the fault as is currently believed. Our model replicates centuries‐long seismic cycles exhibited by the greatest earthquakes and is consistent with the postseismic surface displacements recorded after the Great Tohoku Earthquake. We demonstrate that there is no contradiction between extremely low mechanical coupling at the subduction megathrust in South Chile inferred from long‐term geodynamic models and appearance of the largest earthquakes, like the Great Chile 1960 Earthquake. Key Points We model seismic cycles of great subduction earthquakes in time scales from minute to millennia with nonlinear transient rheology Viscosity in the mantle wedge drops by more than three orders of magnitude during a great earthquake with a magnitude above nine Pronounced viscoelastic relaxation in mantle wedge starts already hours or days after the great earthquake
ISSN:1525-2027
1525-2027
DOI:10.1002/2017GC007230