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Geol 600 Notable Historical Earthquakes Finite fault rupture propagation http://www- rohan.sdsu.edu/~kbolsen/geol600_nhe_source_inversion.ppt
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9 Force Couples M ij (the moment tensor), 6 different (M ij =M ji ). |M|=fd M 11 M 12 M 13 Good approximation for distant M= M 21 M 22 M 23 earthquakes due to a point source M 31 M 32 M 33 Larger earthquakes can be modeled as sum of point sources
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Description of earthquakes using moment tensors: Parameters: strike , dip , rake Right-lateral =180 o, left-lateral =0 o, =90 reverse, =-90 normal faulting Strike, dip, rake, slip define the focal mechanism
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Description of earthquakes using moment tensors: M 11 = -M 0 (sin cos sin2 s + sin2 sin sin 2 s ), M 12 = M 0 (sin cos cos2 s + 0.5 sin2 sin sin2 s ), M 13 = -M 0 (cos cos cos s + cos2 sin sin s ), M 22 = M 0 (sin cos sin2 s - sin2 sin cos 2 s ), M 23 = -M 0 (cos cos sin s - cos2 sin cos s ), M 33 = M 0 sin2 sin
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P-waves S-waves
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Finite-size Fault Plane Divide into ‘sub-faults’ ‘sub-faults’ x x x x
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Define rupture parameters (distributions of slip, rake, rupture speed, source-time function, stress, friction, etc) wave-propagation code Compute synthetic seismograms at receiver locations Compare synthetic to observed seismograms Synthetics fit data? Yes no
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Kinematic source inversion: Solves for slip history on the fault Dynamic source inversion: Solves for stress and friction on the fault
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Kinematic Source Inversion
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Landers: Classic Vertical Strike-Slip Event
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Test case: 1992 M 7.3 Landers Well-recorded event
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Slip-weakening Rupture Model
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Dynamic Rupture From Trial-and-Error Finite-Difference Modeling
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How is rupture propagation affected by realistic variation of dynamic parameters? Let’s look at changes in the stress drop…
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Inverted (Trial-and- Error) Dynamic Radiation Versus Data
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Stress Field (a)
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Stress Field (b)
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Stress Field (c)
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1994 M6.7 Northridge
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2004 M6.0 Parkfield
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1999 M7.4 Izmit
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SOURCE TIME FUNCTION DURATION ALSO VARIES WITH STATION AZIMUTH FROM FAULT. THIS DIRECTIVITY CAN CONSTRAIN WHICH NODAL PLANE IS THE FAULT PLANE For earthquake, V/V R ~1.2 for shear waves and 2.2 for P waves. Maximum duration is 180° from the rupture direction, and the minimum is in the rupture direction. Analogous effect: thunder generated by sudden heating of air along a lightning channel in the atmosphere. Here V/V R ~0, so observers perpendicular to the channel hear a brief, loud, thunder clap, whereas observers in the channel direction hear a prolonged rumble. Directivity similar to Doppler Shift, but differs in requiring finite source dimension Stein & Wysession, 2003
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