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ation of physics-based ground motion earthquake simulat a velocity model improved by tomographic inversion res 1 ardo Taborda, 1 En-Jui Lee, 2 David Gill, 3 Chen, 4 Philip Maechling, 3 Thomas H. Jordan 2,3 ter for Earthquake Research and Information, and Department of Civil Engineering, University of Memph artment of Earth Sciences, University of Southern California thern California Earthquake Center, University of Southern California artment of Geology and Geophysics, University of Wyoming
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1

Validation of physics-based ground motion earthquake simulations using a velocity model improved by tomographic inversion results

Ricardo Taborda,1 En-Jui Lee,2 David Gill,3 Po Chen,4 Philip Maechling,3 Thomas H. Jordan2,3

1 Center for Earthquake Research and Information, and Department of Civil Engineering, University of Memphis2 Department of Earth Sciences, University of Southern California3 Southern California Earthquake Center, University of Southern California4 Department of Geology and Geophysics, University of Wyoming

2

southernCaliforniamodels

CVM-H+GTLCVM-S4.26

CVM-HCVM-S

Alternative velocity modelsfor southern California

Magistrale et al. (1996, 200)Kohler et al. (2003)

(…) +Chen et al. (2011)

Lee et al. (2011, 2013)Gil et al. (2013, 2014)

Süss and Shaw (2003)Süss et al. (2005)Plesch et al. (2007, 2009)

(…) +Ely et al. (2010)

3

Crustal structurebasin depths at fixedvalues of Vs

4

Basins geometrydepth to Vs = 1 km/s

CVM-S CVM-H

5

Taborda and Bielak (2014)BSSA, 104(4): in press

Recent work using different velocity modelscase study: 2008 Chino Hills earthquake

Taborda and Bielak (2013)BSSA, 103(1): 131–156

6

southernCaliforniamodels

CVM-H+GTLCVM-S4.26

CVM-HCVM-S

Alternative velocity modelsfor southern California

Magistrale et al. (1996, 200)Kohler et al. (2003)

(…) +Chen et al. (2011)

Lee et al. (2011, 2013)Gil et al. (2013, 2014)

7

The latest CVM-S4.26 velocity modeltomographic inversion results and merge into CVM-S

CVM-S4.26(Final Model)

CVM-S(Base Model)

Magistrale et al. (1996, 200)Kohler et al. (2003)

Built as a model with“arbitrary” resolution

(…) +Chen et al. (2011)

Lee et al. (2011, 2013)

Starting model

discrete version of themodel with fixed resolution:regular grid every 500 mand minimum Vs = 1000 m/s

3D tomographicinversion yieldsperturbations tostarting model

inversion processincluded 26 iterationsPo Chen and En-Jui Lee

Recovering and merging process

various scheme(s) devised to recover model featurestruncated by the startingmodel and merge the pertur-bations back into the modelfor “arbitrary” queryingresolution

Distributedvia SCEC’s UCVM

(…) +Gil et al. (2013, 2014)

8

The CVM-S4.26 velocity modelmerging alternatives

Option 1

Base Vs < 1 km/s

UseStarting Props.+ Perturbation

NegativePerturbation

Final Model

NO YES

UseBase Props.

+ Perturbation

UseBase Props.

NO YES

checks whether base model is softer than starting model—inside a basin?—

if the base model is softerchecks whether the perturbationwill make it even softer

prevents the perturbation from making softer than the base model—preserves floor base props.—

otherwise ithardens thebase model

otherwise ithardens thestarting model

9

The CVM-S4.26 velocity modelmerging alternatives

Option 2

Base Props.< Starting

UseBase Props.

NegativePerturbation

Final Model

NO YES

Starting Values+

Perturbation

UseBase Props.

NO YESPositivePerturbation

YES

checks whether base model is softer than starting model—inside a basin?—

if the base model is softer, checks whetherthe perturbation will make it even softer

prevents the perturbation from making softer than the base model

prevents the perturbationfrom making stiffer than

the base model

if the base model is stiffer, checks whether

the perturbation will make it even stiffer

10

The CVM-S4.26 velocity modelmerging alternatives

Option 3

Base Props. < Starting

UseStarting Props.+ Perturbation

Final Model

NO YES

UseBase Props.

checks whether base model is softer than starting model—inside a basin?—

the base model ispreserved everywhereit is softer than thestarting model

the inversion results are used everywhere else

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Comparison between base and merged models

CVM-S CVM-S4.26 Option 1

CVM-S4.26 Option 2 CVM-S4.26 Option 3

Surface shear wave velocity (Vs) in m/s

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• Largest earthquake in the L.A. region since the 1994 Northridge earthquake.

• Combination of thrust and strike-slip faulting between the Whittier and Chino faults.

• No significant damages, no fatalities.

• Excellent opportunity for testing assumptions and methodologies.

• Recorded in over 450 strong motion station from different seismic networks. 336 surface stations within simulation domain.

The 2008 chino hills earthquakeand region of interest

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Low-frequency (0–0.5 Hz) ground motionselected locations

DataStarting model

Inverted model

14

“High”-frequency (0–4 Hz) ground motionselected locations

DataBase model

Merge Option 1Merge Option 2

Merge Option 3

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6 – 8Good

4 – 6Fair

0 – 4Poor

8 – 10Excellent

» Anderson (2004)13th World Conf. Earthq. Eng.

» as modified inTaborda and Bielak (2013)Bull. Seismol. Soc. Am. 103(1):131–156

AriasIntensity

EnergyIntegral

Duration

PGA PGV PGD

FourierSpectrum

ResponseSpectrum

CrossCorrelation

Validation criteriagoodness of fit

16CVM-S CVM-S4.26 Option 1

CVM-S4.26 Option 2 CVM-S4.26 Option 3

GOF scorescomparison(0–0.25 Hz)

17

CVM-S4.26 Option 1

CVM-S4.26 Option 2 CVM-S4.26 Option 3

GOF scores improvementwith respect to the base model(0–0.25 Hz)

Scale corresponds to change in the GOFscore with respect to the values obtained forthe simulation using the base CVM-S model

18

CVM-S CVM-S4.26 (Option 1)

GOF scores improvementwith respect to the base model (0–0.25 Hz)

19

CVM-S CVM-S4.26 (Option 1)

GOF scores improvementwith respect to the base model (0–0.25 Hz)

20

Improvements beyond inversion fmax

with respect to the base model (0–4 Hz)

CVM-S CVM-S4.26 (Option 1)

21

Improvements beyond inversion fmax

with respect to the base model (0–4 Hz)

GOF score change w.r.t. base model validation

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» general improvements in the synthetics are obtained but some areas will need further attention

» changes in GOF scores are of the order of 1 to 4 points maximum

» additional improvements are unlike to come from marginal changes to the velocity models at this point, therefore other aspects (like frequency dependent attenuation and coherency in the source model) will need to be considered

Closing remarks and future work

23

Validation of physics-based ground motion earthquake simulations using a velocity model improved by tomographic inversion results

Ricardo Taborda,1 En-Jui Lee,2 David Gill,3 Po Chen,4 Philip Maechling,3 Thomas H. Jordan2,3

1 Center for Earthquake Research and Information, and Department of Civil Engineering, University of Memphis2 Department of Earth Sciences, University of Southern California3 Southern California Earthquake Center, University of Southern California4 Department of Geology and Geophysics, University of Wyoming


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