Annual Meeting - SCEC.org
Annual Meeting - SCEC.org
Annual Meeting - SCEC.org
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Group 1 – CDM | Poster Abstracts<br />
Bernardino Mountains from San Clemente Island to southwestern Nevada. Published Holocene to<br />
late Pleistocene slip rates (Peterson et al., 1996) for faults within the transect do not fit the GPS<br />
velocity data from CMM3. The CMM3 data are best fit by rates in the Eastern California shear zone<br />
(ESCZ) that are higher than rates estimated over geologic time scales, and by rates for the San<br />
Andreas and San Jacinto faults that are lower than published geologic rates. Locking depths of13-<br />
18 km were used in the modeling (Peterson et al., 1996). Slip rates that fit the CMM data well are as<br />
follows: the Eastern California shear zone, 20 mm/yr; San Andreas fault, 11 mm/yr; San Jacinto<br />
fault, 6mm/yr; the Elsinore fault, 5 mm/yr; the NIFZ, 2 mm/yr, and the Palos Verde fault, 3<br />
mm/yr. The discrepancy between geologically and geodetically estimated slip rates for the San<br />
Andreas and San Jacinto faults and for the ESCZ could be a result of variations in strain<br />
accumulation rates at different stages of the earthquake cycle (for a viscoelastic medium). The low<br />
rate of geodetically measured strain accumulation on the San Andreas fault could be because it is<br />
in the late stage of the earthquake cycle. The high rate of strain accumulation modeled in the ECSZ<br />
could be a result of recent activity--the Landers and Hector Mine earthquakes. An alternative<br />
hypothesis could simply be that the San Andreas fault is no longer the primary fault in the vicinity,<br />
but movement has been shifted to the ECSZ within the last few decades.<br />
1-114<br />
B4-AUGMENTED IDENTIFICATIONS OF SAN ANDREAS FAULT SURFACE<br />
FEATURES: SPATIAL STRUCTURE OF THE PLATE BOUNDARY BETWEEN<br />
BOMBAY BEACH AND DESERT HOT SPRINGS Lynch DK, and Hudnut KW<br />
We present preliminary results of a hyper-accurate (± few m) inventory of SAF features between<br />
Bombay Beach and Desert Hot Springs based on overhead imagery. The ultimate goal is to identify<br />
fault features that can be used to determine offset distance and slip rates. Many fault structures<br />
have been previously reported and about two dozen new ones have been found in this study.<br />
Using approximately 80 fault components we defined a map view piecewise continuous trace of<br />
features (and interpolations when no structure could be discerned) that we are calling the<br />
provisional plate boundary (PPB). The resulting PPB trace closely matches the faults reported by<br />
Clark (1984) and those in the qfaults data base. We analyzed the PPB and present evidence of<br />
spatial structure on scales of a few hundred meters.<br />
1-115<br />
SMALL-SCALE UPPER MANTLE CONVECTION AND CRUSTAL DYNAMICS IN<br />
SOUTHERN CALIFORNIA Fay NP, Bennett RA, Spinler JC, and Humphreys ED<br />
We present numerical modeling of the forces acting on the base of the crust caused by small-scale<br />
convection of the upper mantle in southern California. Three-dimensional upper mantle shear<br />
wave velocity structure is mapped to three-dimensional density structure that is used to load a<br />
finite element model of instantaneous upper mantle flow with respect to a rigid crust, providing an<br />
estimate of the tractions acting on the base of the crust. Upwelling beneath the southern Walker<br />
Lane Belt and Salton Trough region and downwelling beneath the southern Great Valley and<br />
eastern and western Transverse Ranges dominate the upper mantle flow and resulting crustal<br />
tractions. Divergent horizontal and upward directed vertical tractions create a tensional to<br />
transtensional crustal stress state in the Walker Lane Belt and Salton Trough, consistent with<br />
transtensional tectonics in these areas. Convergent horizontal and downward directed vertical<br />
tractions in the Transverse Ranges cause approximately N–S crustal compression, consistent with<br />
active shortening and transpressional deformation near the ‘‘Big Bend’’ of the San Andreas fault.<br />
Model predictions of crustal dilatation and the forces acting on the Mojave block compare<br />
favorably with observations suggesting that small-scale upper mantle convection provides an<br />
important contribution to the sum of forces driving transpressional crustal deformation in southern<br />
2008 <strong>SCEC</strong> <strong>Annual</strong> <strong>Meeting</strong> | 129