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Mechanical Models of the Southern San Andreas Fault

Mechanical Models of the Southern San Andreas Fault. Michele Cooke ( UMass ) , Justin Herbert ( UMass ) and Scott Marshall ( App State ). SAF Models!. Forward Mechanical Models BEM: e.g. Du & Aydin (1996); Cooke & Dair (2011), Herbert & Cooke (in press)

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Mechanical Models of the Southern San Andreas Fault

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  1. Mechanical Models of the Southern San Andreas Fault Michele Cooke (UMass), Justin Herbert (UMass) and Scott Marshall (App State)

  2. SAF Models! • Forward Mechanical Models • BEM: e.g. Du & Aydin (1996); Cooke & Dair (2011), Herbert & Cooke (in press) • FEM: e.g. Bird & Kong (2004), Smith & Sandwell (2003); Li & Liu (2006) • Inversions for slip rates • GPS: Bennett et al (1996); Meade and Hager, 2005; Johnson et al. (2007); Spinler et al. (2010); Loveless and Meade 2011) • GPS and focal mechanisms: Becker et al. (2005) • InSar & GPS: Fialko (2006) • Inversions for stress • Parsons (2006)

  3. Active fault geometry through the San Gorgonio Pass 95 ka soils are not offset by the Mill Creek strand of the San Andreas Fault (Kendrick et al., 2011 SCEC mtg.) Active geometry, Garnet Hill – San Gorgonio Pass Thrust (SGPT), highlighted in red Mill Creek strand From the award winning paper, Yule & Sieh, 2003

  4. Forward Mechanical Models • BEM: e.g. Du & Aydin (1996); Cooke & Dair (2011), Herbert & Cooke (in press) • FEM: e.g. Bird & Kong (2004), Smith & Sandwell (2003); Li & Liu (2006) • Inversions for slip rates • GPS: Bennett et al (1996); Meade and Hager, 2005; Johnson et al. (2007); Spinler et al. (2010); Loveless and Meade 2011) • GPS and focal mechanisms: Becker et al. (2005) • InSar & GPS: Fialko (2006) • Inversions for stress • Parsons (2006)

  5. Boundary Element Method (BEM) Model Set Up • Plate motions applied at the edges of the model. • Faults are freely-slipping and tie into horizontal detachment – slip in response to tectonic loading and interaction with other faults • Faults defined with triangular elements ~ 4km diameter • 63 faults Mill Creek Garnet Hill - San Gorgonio Pass Thrust (SGPT)

  6. Slip Rates Garnet Hill - SGPT Mill Creek • Mill creek geometry may overestimate SAF strike slip by as much as 300% • Increasing slip on the SAF results in decreases slip on the San Jacinto though they are not hard linked at Cajon Pass • Co-dependent a la Bennett et al., 2004 From: Cooke and Dair, 2011 JGR

  7. Strike-Slip rates along the SAF through the San Gorgonio Pass • The Mill Creek model does not match strike-slip rates along the San Bernardino strand of the SAF Weldon & Sieh, 1985 McGill et al , 2008 Harden & Matti, 1989 Behr et al, 2010 Van der Woerd et al, 2006 McGill etal, 2010 McGill et al , 2008 Orozco, 2004 Yule & Sieh, 2003 From: Cooke and Dair, 2011 JGR; Herbert and Cooke, in press

  8. Sensitivity of uplift to fault geometry Mill Creek Garnet Hill - SGPT From: Cooke and Dair, 2011 JGR From: Herbert and Cooke, 2012 BSSA Uplift with isostatic correction

  9. Interseismic Model • Back slip approach • Slip from geologic time-scale model applied below locking depth • GPS data processing • Seismic offset removed • Annual and semi-annual signals • Post-seismic – up to 5 years following hector mine • Principal component analysis

  10. Interseismic GPS Velocities • Garnet Hill-SGPT model better matches GPS station velocities.

  11. Stressing Rate Mill Creek Mill Creek strike shear stress dip shear stress Garnet Hill - SGPT Garnet Hill - SGPT strike shear stress dip shear stress

  12. Data Gaps: Holocene slip rates on Banning & Garnet Hill Conclusions • Mill Creek strand of the SAF produces different slip rates, interseismic deformation field and stressing rates than the Garnet Hill strand and SGPT • Slip rates and GPS station velocities are better matched with the Garnet Hill/SGPT active system • Discussion: Will these differences impact the nature of earthquake rupture through the region? Photo along the abandoned Mill Creek strand of the SAF

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