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A Post-Loma Prieta Progress Report on Earthquake Triggering by a Continuum of Deformations
Presented By Joan Gomberg
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A pleasingly simple correlation….
Response of Regional Seismicity to Static Stress Change Produced by the Loma Prieta Earthquake. Reasenberg & Simpson, 1992
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When should correlation imply causation?
Normal Stress Change Stress transfer by the M=5.3 and 5.4 Lake Elsman foreshocks to the Loma Prieta fault: Unclamping at the site of peak mainshock slip. Perfettini et al., 1999 Right-lateral Stress Change Reverse Stress Change Coulomb Stress Change
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One End Member - Static Load Change
shear stress failure threshold time Dt
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One End Member - Static Load Change
Dt failure threshold Dt shear stress time
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The Other End Member - Dynamic Load Change
shear stress failure threshold time
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Static Triggering -> Load or Strength Change
Dynamic Triggering -> Strength Change failure threshold Dt shear stress time
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The Picture Post-Loma Prieta:
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A wide spectrum of triggers between the end members:
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The Picture Post-Loma Prieta:
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A Popular Physical Model:
The ‘Dieterich (1994)’ or ‘Clock-Advance’ Model
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Stress -> Rate Change Highly Non-linear.
The ‘Dieterich (1994)’ or ‘Clock-Advance’ Model
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Frictional Model Rate Change Predicted for Stress Step
perturbed Rate Change background Afterslip and Aftershocks in the Rate-state Friction Law. Helmstetter & Shaw, 2009
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Other Slowly-Developing, Permanent Load Changes:
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Frictional Model Rate Change Predicted for Stress Step & Afterslip
perturbed Rate Change background Afterslip and Aftershocks in the Rate-state Friction Law. Helmstetter & Shaw, 2009
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Measured Afterslip Deformation & Aftershock Rate -> Linear Relationship
Cumulative # of Aftershocks Post-seismic Deformation Time after Landers (yr) Modeling Afterslip and Aftershocks Following the 1992 Landers Earthquake Perfettini & Avouac, 2007
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Oscillatory, continuous loads:
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Rainfall Modulated Seismicity
Earthquake Rate Geodetically Measured Displacement River Elevation Seasonal Variations of Seismicity and Geodetic Strain in the Himalaya Induced by Surface Hydrology Bettinelli et al., 2008
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Lack of tidal modulation constrains nucleation time.
Earthquake Rate +2-4 kPa Geodetically Measured Displacement River Elevation Seasonal Variations of Seismicity and Geodetic Strain in the Himalaya Induced by Surface Hydrology Bettinelli et al., 2008
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‘Dynamic’ Triggering (by seismic waves).
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The ‘Dieterich (1994)’ or ‘Clock-Advance’ Model
The Failure of Earthquake Failure Models. Gomberg, 2001
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A Few More Outstanding Questions…
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Measured Linear Aftershock Densities
Aftershock Scale Independence -> Large & Small Earthquakes Triggered Identically Measured Linear Aftershock Densities Felzer & Brodsky, 2006
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Foreshock Scale Dependence -> Large & Small Earthquakes Begin Differently
M3 source dimension M4 source dimension Evidence for Mogi Doughnut Behavior in Seismicity Preceding Small Earthquakes in Southern California Shearer & Lin, 2009
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Complex Aftershock Behaviors: Rate Increases Precede Quiescences
background rate quiescence background rate quiescence background rate quiescence background rate quiescence The Response of Seismicity to Coulomb Stress Triggers & Shadows of the 1999 Mw=7.6 ChiChi Earthquake Ma et al., 2005
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Complex Aftershock Behaviors Reflect Stress Heterogeneity
seismicity rate change background rate time (ta units) Can Coseismic Stress Variability Suppress Seismicity Shadows? Insights from a Rate-State Friction Model Marsan, 2006
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Complex Aftershock Behaviors Reflect Fault Patch Depletion
A Frictional Population Model of Seismicity Rate Change Gomberg et al., 2005
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“There are known knowns. These are things we know that we know
“There are known knowns. These are things we know that we know. There are known unknowns. That is to say, there are things that we know we don't know. But there are also unknown unknowns. There are things we don't know we don't know.” Thank You!
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