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Analyis of Bridge Structures Crossing Fault Rupture Zones: Seismic Ground Motion Simulation
Douglas Dreger, Gabriel Hurtado, and Anil Chopra University of California, Berkeley
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Objective Develop a set of characteristic near-fault (10s of meters distance) ground motions for engineering design. Explore ground motion sensitivity to faulting style and rupture behavior. In particular consider cases with surface rupture where ground motions have both dynamic and static components.
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Elastic Dislocation of a Mw6.5 Earthquake
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Computational Method 4th order staggered grid finite-differences
Complete wavefield computation Arbitrary model complexity Velocity Structure Half-space, layered (1D) Source Complexity Uniform slip Variable slip, rise time and rupture velocity Computational requirements Grid spacing (20m), fmax (20 Hz), model size (2.3 Gp), requiring 119 Gbytes of memory Computations are performed on the LLNL MCR supercomputer using 512 processors
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Finite-Difference Grid and Station Subarray Position
FP FN
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Considered Fault Geometries
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Source Characteristics
Mw 6.5 28.8km x 9.3km length by width fault from Wells and Coppersmith (1994) 0.71m of uniform slip variety of faulting style (strike-slip to thrust) constant 0.5 second rise time from Somerville et al. (1999) sensitivity to rise time is examined constant rupture velocity of 80% of the shear wave velocity sensitivity to rupture velocity is examined
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Comparison of Displacement Results
Strike-slip Oblique Reverse Thrust
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Comparison of Velocity Results
Strike-slip Oblique Reverse Thrust
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Strike-Slip Results Fling Controlled
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Strike-Slip Results Fling Controlled Directivity Controlled
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Are The Peak Ground Velocities Reasonable?
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Dip-Slip Results Strike-Slip Case Dip=40; rake=110 case
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Z component Displacement Motions Away from Fault
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Rise Time Sensitivity - FP Component
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Rise Time Sensitivity - FN Component
rt=0.3s rt=0.5s rt=0.7s
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Variable Slip Models Kinematic Model
Method of Mai and Beroza (2001) to obtain random slip distributions Assume constant rupture velocity Assume constant slip velocity - leads to variable rise time Models have variable variable static offset close to the fault, and degrees of rupture directivity Cumulative Slip
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Conclusions
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