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Crustal Deformation and Fault Mechanics

 
    Crustal Deformation and Fault Mechanics

 

 

 

Geodetic Strain used to improve earthquake forecasts in the San Francisco Bay Region

Since H.F. Reid’s classic study of the 1906 San Francisco earthquake, we have known that elastic strain accumulates slowly over centuries but is released suddenly in great earthquakes.  In Reid’s day crustal strain was measured by repeated triangulation surveys, starting in the 1960’s with laser distance measuring devices, and in the last few decades with continuous GPS networks.  Geodetic strain plays a central role in forecasting future seismic hazards:  the higher the rate of strain accumulation, either the more frequent or the larger the earthquakes must ultimately be to relieve that strain.  One of our most important goals is to quantify these relations.

To accomplish this we require the most accurate measurements possible, mechanically consistent physical models of the strain accumulation process, and inversion methodologies to relate the data to the unknown model parameters.  With former student Kaj Johnson (Univ. Indiana) we are applying these ideas to the San Francisco Bay area where several major faults present significant hazards.   Our goals are to better constrain estimates of the long-term slip rates on these faults and the average recurrence times of damaging earthquakes.  We are investigating how geodetic strain measurements can reduce uncertainties in fault slip-rates and recurrence times inferred from paleoseismic investigations. 

Figure 1:  Average GPS velocities in the San Francisco Bay region shown relative to stable North America.  Also shown are major creeping and locked faults.

Kaj has extended earlier two-dimensional models of faults in an elastic layer overlying a viscoelastic lower crust and upper mantle to three dimensions.  This approach accounts for the long-term motion of crustal blocks, but better accounts for geometric complexities where, for example, thrust faults must accommodate motion oblique to the major strike-slip faults.  The deformation is rigorously coupled to the visco-elastic substrate and we account analytically for an infinite sequence of past repeating earthquakes.

The estimation strategy is based on a Bayesian analysis, where we take the paleoseismic estimates of fault slip-rate and recurrence time as a priori estimates (assumed to have uniform distribution between broad lower and upper bounds).  We then analyze the geodetic data and compute posterior probability distributions on parameters of interest, such as slip-rate and recurrence time.

Preliminary results demonstrate that the geodetic data provide strong constraints on slip-rate as expected.  For example the San Andreas slips at rates near 33 mm/yr south of the Bay Area, but drops to below 15 mm/yr on the San Francisco Peninsula as slip is transferred to the Hayward and Calaveras faults.  The uncertainty in the recurrence times of large earthquakes is only slightly reduced by adding the geodetic observations: to 180-300 years on the San Andreas, vs 270-400 years on the Rogers Creek Fault.  Further work will be required to improve the mechanical forward models and to understand whether the bounds on the recurrence times can be narrowed further.


Figure 2.  Posterior probability density functions for slip-rates on major fault segments.  Prior bounds are shown by gray bars.


Figure 3.  Recurrence times for large earthquakes on the San Andreas Fault Peninsula (upper left), north of the Bay (upper right), and Rogers Creek fault (lower left).  The most recent earthquake on the San Andreas is 1906.  Estimates of the most recent large quake on the Rogers Creek Fault are shown in the lower right.  Grey bars represent prior bounds. Dark bars represent 95% confidence intervals on the posterior distribution.

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