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On modeling induced seismicity. Flaminia Catalli. with. Valentin Gischig Men-Andrin Meier Stefan Wiemer. Sebastian Hainzl Torsten Dahm. First Story : earthquake interactions, the Basel case and a stochastic model. A). C). Catalli et al., GRL (2013). D). B).
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On modeling induced seismicity Flaminia Catalli with Valentin Gischig Men-Andrin Meier Stefan Wiemer Sebastian Hainzl Torsten Dahm
First Story : earthquake interactions,the Basel case and a stochastic model
A) C) Catalli et al., GRL (2013) D) B)
Geomechanical stochastic seed model Gischig and Wiemer, GJI (2013) • Can we reproduce the CI observed behavior? • How considering event interactions may improve a PSHA?
A) • Potential earthquakes (seeds) uniformly random distributed over modeling area • Differential stressestimate from in-situ stress field • Mohr-Coulomb failure criterion assuming θ optimally oriented • Local b-value and magnitude • EQ interactions • Retriggeringstress-drop, DCFS and a new stress state are assigned to all seeds B) Goertz-Allmann and Wiemer, Geophys. (2013)
P DCFSint P+DCFSint t=3days t=5days t=7days
injection+interactions injection only
Still an open question DCFSp DCFSint
Conclusions #1 : • Interaction Coulomb stress changes may improve the spatial assessment of induced seismicity • We need a robust null hypothesis to confirm the validity of the CI time-distance behavior • Do we maybe need a more realistic hypocenter distribution considering fractal clustering?
Second Story : Rate-and-state effect of pore-pressure diffusion on induced seismicity
Rate-and-state model no perturbation stressing rate change sudden stress change Toda et al. Nature (2002)
D = 0.05 m2/sec radius of the source = 1 m
Conclusions #2 : • Rate-and-state does not have a tuning parameter to fit the total number of events without providing physical reasons • Rate-and-state based predictions are very sensitive to the pressure model or to local variations of the background