disputable n on-d c c omponents of s everal s trong e arthquakes

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Disputable Disputable n n on-D on-D C C c c omponents of omponents of s s everal everal s s trong trong e e arthquakes arthquakes Petra Adamov Petra Adamov á á Jan Šílený Jan Šílený

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Disputable n on-D C c omponents of s everal s trong e arthquakes. Petra Adamov á Jan Šílený. Motivation. For some strong events a large non-DC component is reported by agencies - PowerPoint PPT Presentation

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Page 1: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Disputable Disputable nnon-Don-DCC ccomponents of omponents of sseveral everal

sstrong trong eearthquakes arthquakes

Petra AdamovPetra Adamováá

Jan ŠílenýJan Šílený

Page 2: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

MotivationMotivation

For some strong events a large non-DC component is reported by agencies

This component is often questionable (large events, tectonic origin) it can be false due to source finiteness (strong event is modeled as point source)

Page 3: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Introduction to second degree Introduction to second degree momentsmoments

Standard moment tensorPoint source: couple of planes

a ‘dot’

Page 4: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Introduction to second degree Introduction to second degree momentsmoments

“Finite source” parameters from point source approximation

• Detailed modeling of slip on the fault plane:

- costly

- often data not available (near the fault)

• 2nd degree moments are advantageous alternative

geometry of the source duration of the source process average slip on the fault spatial and temporal centroid rupture velocity vector

Inside the ‘dot’

Page 5: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

TheoryTheory

Moments till degree 2, Doornbos (1982)Moments till degree 2, Doornbos (1982)Temporal centroid

Spatial centroid

Source ellipsoidRupture propagation

Source process duration

Zero degree moment tensor (standard MT)Zero degree moment tensor (standard MT)

Page 6: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Inverse scheme: full waveform inversionInverse scheme: full waveform inversion

exclusion of the non-physical solutions inversion is faster

Standard MT

Estimation of second degree moments

Page 7: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Applications: Location of earthquakesApplications: Location of earthquakes

Page 8: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Standard focal mechanismsStandard focal mechanismszero degree moments

Page 9: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Jack-knife test - Izmit and KobeJack-knife test - Izmit and Kobe

Page 10: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Kobe – 2Kobe – 2ndnd degree moments degree moments

Ide et al. (1996)10 km

Page 11: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Example of seismogram fitExample of seismogram fit

Black: observed seismograms

Red: synthetic seismograms

Page 12: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Izmit – 2Izmit – 2ndnd degree moments degree moments

Clevede et al. (2004)

Page 13: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Synthetic experiment: Estimate of Synthetic experiment: Estimate of error due to noise for the Izmit error due to noise for the Izmit

earthquakeearthquake5 samples of random noise of 20% and 30% of maximum amplitude superimposed on the records

Level 20%: stable solution, small deviation,

for source ellipsoid orientation – max. deviation 5 degrees

Level 30%: unstable solution, large deviation

for source ellipsoid orientation – max. deviation 17 degrees

Black ellipsoid: extreme deviation with 20 % noise

Blue ellipsoid: extreme deviation with 30 % noise

Page 14: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

Focal mechanismsFocal mechanisms

Standard MT

Standard MT without second degree effects

• computing standard MT

• estimation of 2nd degree moments

• removing 2nd degree moments from the data

• computing new standard MT

Page 15: Disputable  n on-D C c omponents of  s everal  s trong  e arthquakes

ConclusionsConclusions• Second degree moments bring additional information above standard MT: source ellipsoid, duration of the source process, average rupture velocity

• Neglect of source finiteness, which remains in the data even after an essential low-pass filtering may originate spurious non-DC components in the mechanism.

• The procedure suggested reduces spurious non-DC components substantially