Participants of Nurmerical Benchmark Test and Misfit Criteria for Summarizing the Results Seiji Tsuno (LGIT)

Slides:



Advertisements
Similar presentations
Real-Time Estimation of Earthquake Location and Magnitude for Seismic Early Warning in Campania Region, southern Italy A. Zollo and RISSC-Lab Research.
Advertisements

Time-frequency-domain modal identification of ambient vibration structures using Wavelet Transform Numerical example.
1 1 Symposium Bjørn Gjevik 70 år Harald E. Krogstad, Department of Mathematical Sciences, NTNU, Trondheim and work in progress with Karsten Trulsen, Department.
Quantification of Nonlinearity and Nonstionarity Norden E. Huang With collaboration of Zhaohua Wu; Men-Tzung Lo; Wan-Hsin Hsieh; Chung-Kang Peng; Xianyao.
FilteringComputational Geophysics and Data Analysis 1 Filtering Geophysical Data: Be careful!  Filtering: basic concepts  Seismogram examples, high-low-bandpass.
Nirmal Jayaram Nilesh Shome Helmut Krawinkler 2010 SCEC Annual Meeting A statistical analysis of the responses of tall buildings to recorded and simulated.
Ground motion simulations and site effect estimation for Istanbul, Turkey Mathilde Bøttger Sørensen 1, Nelson Pulido 2, Sylvette Bonnefoy-Claudet 3, Kuvvet.
用近震波形分析2013 年6 月2 日南投地震的震源過程 謝銘哲1, 趙里2, 馬國鳳1 1國立中央大學地球物理研究所
Sismovalp final meeting, Martigny, 02/10/2006 SISMOVALP WP6 Alpine ground motion Numerical benchmark of ground motion simulation in the Grenoble valley.
1 Workshop on GMSM for Nonlinear Analysis, Berkeley CA, October 26, 2006 ATC-63 Selection and Scaling Method Charles Kircher Curt B. Haselton Gregory G.
March 7, 2008NGA-East 2nd Workshop1 RECENT DEVELOPMENTS IN STRONG MOTION SIMULATIONS FOR CEUS Paul Somerville and Robert Graves URS Pasadena MOTIVATION:
Characterization of Ground Motion Hazard PEER Summative Meeting - June 13, 2007 Yousef Bozorgnia PEER Associate Director.
Xi’an Jiaotong University 1 Quality Factor Inversion from Prestack CMP data using EPIF Matching Jing Zhao, Jinghuai Gao Institute of Wave and Information,
The surface profiles in Grenoble area determined by the MASW measurements Seiji Tsuno, Cecile Cornou, Pierre-Yves Bard (LGIT) QSHA meeting, 1/Juin/2007,
The RSNI Seismic Network Laboratory of seismology, DISTAV - University of Genoa (Italy) RSNI STAFF RSNI STAFF : Spallarossa D.,
UNIVERSITY OF ATHENS Faculty of Geology and Geoenvironment Department of Geophysics and Geothermics A. Agalos (1), P. Papadimitriou (1), K. Makropoulos.
Average properties of Southern California earthquake ground motions envelopes… G. Cua, T. Heaton Caltech.
Selection of Time Series for Seismic Analyses
5: EARTHQUAKES WAVEFORM MODELING S&W SOMETIMES FIRST MOTIONS DON’T CONSTRAIN FOCAL MECHANISM Especially likely when - Few nearby stations, as.
Spectra: ApplicationsComputational Geophysics and Data Analysis 1 Fourier Transform: Applications in seismology Estimation of spectra –windowing –resampling.
Chapter 5 AM, FM, and Digital Modulated Systems
Ground Motion Parameters Measured by triaxial accelerographs 2 orthogonal horizontal components 1 vertical component Digitized to time step of
Elastic and inelastic relations..... mx+cx+Q(x)= -ma x Q x Q Q=kx elasticinelastic.
Comparison of Recorded and Simulated Ground Motions Presented by: Emel Seyhan, PhD Student University of California, Los Angeles Collaborators: Lisa M.
Automatic detection and location of microseismic events
COMPILATION OF STRONG MOTION DATA FROM EASTERN CANADA FOR NGA-EAST PROJECT Lan Lin Postdoctoral Fellow, Geological Survey of Canada.
Invited Workshop on Strong-Motion Record Processing Convened by The Consortium of Organizations for Strong-Motion Observation Systems (COSMOS) Pacific.
The kinematic representation of seismic source. The double-couple solution double-couple solution in an infinite, homogeneous isotropic medium. Radiation.
An Extension of Stochastic Green ’ s Function Method to Long-Period Strong Ground-motion Simulation Y. Hisada and J. Bielak.
Mid-Term Review Meeting, February 13-14, Tutzing Seismic wave Propagation and Imaging in Complex media: a European network MARTIN GÁLIS.
DISCRIMINATING SMALL EARTHQUAKES FROM QUARRY BLASTS USING PEAK AMPLITUDE RATIO Vmax/Hmax MA, S., EATON, D., & DINEVA, S. Department of Earth Sciences The.
Zadonina E.O. (1), Caldeira B. (1,2), Bezzeghoud M. (1,2), Borges J.F. (1,2) (1) Centro de Geofísica de Évora (2) Departamento de Física, Universidade.
Observation of diffuse seismic waves at teleseismic distances
DISCRIMINATING SMALL EARTHQUAKES FROM QUARRY BLASTS USING PEAK AMPLITUDE RATIO Vmax/Hmax MA, S., EATON, D., & DINEVA, S. Department of Earth Sciences The.
Validation of physics-based ground motion earthquake simulations using a velocity model improved by tomographic inversion results 1 Ricardo Taborda, 1.
High Resolution Finite Fault Inversions for M>4.8 Earthquakes in the 2012 Brawley Swarm Shengji Wei Acknowledgement Don Helmberger (Caltech) Rob Graves.
SPICE Research and Training Workshop III, July 22-28, Kinsale, Ireland Seismic wave Propagation and Imaging in Complex media: a European.
1 Wavelet Transform. 2 Definition of The Continuous Wavelet Transform CWT The continuous-time wavelet transform (CWT) of f(x) with respect to a wavelet.
GG313 Lecture 24 11/17/05 Power Spectrum, Phase Spectrum, and Aliasing.
Engineering Perspective on Application of Simulated Ground Motions Jonathan P. Stewart & Emel Seyhan University of California, Los Angeles Robert W. Graves.
Ground motion simulations in the Pollino region (Southern Italy) for Mw 6.4 scenario events.
Phase 1: Comparison of Results at 4Hz Phase 1 Goal: Compare 4Hz ground motion results from different codes to establish whether the codes produce equivalent.
Surface-wave Derived Focal Mechanisms in Mid-America R. B. Herrmann 1, C. J. Ammon 2 and H. M. Benz 3 1 Saint Louis University, 2 Pennsylvania State University,
HIGH FREQUENCY GROUND MOTION SCALING IN THE YUNNAN REGION W. Winston Chan, Multimax, Inc., Largo, MD W. Winston Chan, Multimax, Inc., Largo, MD Robert.
Near Fault Ground Motions and Fault Rupture Directivity Pulse Norm Abrahamson Pacific Gas & Electric Company.
P wave amplitudes in 3D Earth Guust Nolet, Caryl Michaelson, Ileana Tibuleac, Ivan Koulakov, Princeton University.
February 12, John Anderson GE/CEE 479/679 Earthquake Engineering GE / CE - 479/679 Topic 7. Response and Fourier Spectra John G. Anderson Professor.
1 Wavefield Calibration Using Regional Network Data R. B. Herrmann Saint Louis University.
UCERF3 Uniform California Earthquake Rupture Forecast (UCERF3) 14 Full-3D tomographic model CVM-S4.26 of S. California 2 CyberShake 14.2 seismic hazard.
Focal mechanisms and moment tensors of micro-earthquakes in the Malé Karpaty (Little Carpathians) Mts., Slovakia Lucia Fojtíková 1, Václav Vavryčuk 2,
2002/05/07ACES Workshop Spatio-temporal slip distribution around the Japanese Islands deduced from Geodetic Data Takeshi Sagiya Geographical Survey Institute.
Need for an Objective Goodness-of-Fit Measure for: Broadband synthetic time histories from different methodologies Broadband synthetic time histories versus.
Shaking and Flooding by the Tohoku-Oki earthquake Shengji Wei*, Rob Graves**, Don Helmberger*, Jean-Philippe Avouac* and Junle Jiang* * Seismological Lab,
Fourier Transform and Spectra
Attenuation of High frequency P and S Waves in Khorasan Province, Iran Jafar Shoja-Taheri, and Mohsen Farrokhi Earthquake Research Center, Ferdowsi University.
Date of download: 7/3/2016 Copyright © ASME. All rights reserved. From: An Intelligent Prognostic System for Gear Performance Degradation Assessment and.
Novel Approach to Strong Ground Motion Attenuation Modeling Vladimir Graizer U.S. Nuclear Regulatory Commission Erol Kalkan California Geological Survey.
Site effect characterization of the Ulaanbaatar basin
Susan L. Beck George Zandt Kevin M. Ward Jonathan R. Delph.
PRISM: PROCESSING AND REVIEW INTERFACE FOR STRONG MOTION DATA SOFTWARE
Brazilian “Strong-Motion” Data Stéphane Drouet, ON, Rio de Janeiro Marlon Pirchiner, IAG/USP, São Paulo Marcelo Assumpção, IAG/USP, São Paulo Luis Carlos.
Filtering Geophysical Data: Be careful!
Chapter 5 AM, FM, and Digital Modulated Systems
Université Joseph Fourier Grenoble, France
Sound shadow effect Depends on the size of the obstructing object and the wavelength of the sound. If comparable: Then sound shadow occurs. I:\users\mnshriv\3032.
Ken Creager, Wendy McClausland and Steve Malone
Notes on the Intensity Measure Breakout Session - PEER Annual Meeting - Jan. 17, 2002   ·   Testbeds will not provide definitive answers as to the best.
by Satoshi Ide, Annemarie Baltay, and Gregory C. Beroza
Fourier Transform and Spectra
Lec.6:Discrete Fourier Transform and Signal Spectrum
Presentation transcript:

Participants of Nurmerical Benchmark Test and Misfit Criteria for Summarizing the Results Seiji Tsuno (LGIT)

Participants MethodCaseParticipants 11D(+Nonlinear)FSfabian bonilla 21DFSpacific engineering 32DS1, S2corinne lacave 42DS1, S2, W1, W2delepine 52DFSpacific engineering 63FS1, S2, W1, W2hideo aochi 73FS1, S2, W1, W2moczo 83FS1, S2, W1, W2s TS1, S2, W1, W2louie 103TFSstupa 11EMS1, S2carine sansorny 12EMS1, FSjavier ruiz 13EMS1, FSmathieu causse 142D(Nonlinear) fabian bonilla 153T emmanuel chaljub 163T martin 173F robert graves FS: at station OGFH (borehole location) for a Mw=6.0 strike-slip event occuring on the Eastern part of the Belledonne Border Fault

Output # Waveforms (Acceleration, velocity and displacement) # Fourier spectra # Response spectra (Pseudo-velocity response spectra; h=5%) # Maximum value of acceleration, velocity and displacement # Misfit criteria (Anderson’s method & Kristekova’s method) # Spectral ratio (for reference site;OGMU or of bore-hole;OGFB) # Standard deviation error and RMS misfit in each output.

Misfit criteria # We will evaluate the results estimated by participants, using the misfit criteria proposed by J. Anderson and M. Kristekova. # Mainly, J. Anderson and M. Kristekova evaluated the performance of the proposed misfit-criteria by horizontal components of observed earthquake records and canonical signals, respectively. But… # In this numerical benchmark, we can compared many theoretical seismograms estimated by participants with observation.

Quantitative measure of the goodness-of-fit of synthetic seismograms Proposed by John G. Anderson (13 th World Conference on Earthquake Engineering ) # He calibrated the proposal criterion, using two components of synthetic seismograms with 1000 pairs and observations with 1165 pairs. # And also, he applied this measurement system to two horizontal components of a single station recording the M8.1 Michoacan earthquake. # Lastly, this criterion was applied to a blind prediction of ground motions at a station PS10 for comparison of observation with synthetic seismograms.

Criteria Goodness of fit measurementsFrequency bands used (Hz) C1 Arias DurationB – 0.1 C2 Energy DurationB2 0.1 – 0.2 C3 Arias IntegralB3 0.2 – 0.5 C4 Energy IntegralB4 0.5 – 1.0 C5 Peak AccelerationB5 1.0 – 2.0 C6 Peak VelocityB6 2.0 – 5.0 C7 Peak DisplacementB7 5.0 – 10.0 C8 Response SpectraB – 20.0 C9 Fourier SpectraB 20.0 – 50.0 C10 Cross CorrelationB – 50.0 The similarity score (S1) is averaged by all fit criterion.

Example (application) Fig. Acceleration records of NS and EW components at PS10 PS10 Fig. Fourier spectra for acceleration records at PS10 Where PS10 is 3km from the fault In the M7.9 Denali Fault, Alaska, earthquake of Nov. 3, 2002.

Individual scores -1

Individual scores -2

Similarity score S1 =

Definition of familiar function Fig. Definitions of function related to similarity score Fig. Definitions of function related to similarity score (normalized)

Misfit criteria for quantitative comparison of seismograms Proposed by Miriam Kristekova. et al. (Submitted to BSSA, January 2006) # The proposal criteria are based on the time-frequency representation (TFR) of the seismograms obtained as the continuous wavelet transform (CWT) with the analyzing Morlet wavelet. # They tested properties of the misfit criteria using canonical signals, which were specifically amplitude, phase-shift, time-shift, and frequency modified. # And also, they calculated the misfit criteria for four different numerical solutions for a single layer over half-space (the SCEC LOH.3 Problem) and the reference FK (frequency-wavenumber) solution.

Criteria Misfit Criteria TFEM -Time-frequency envelope misfit TFPM -Time-frequency phase misfit TEM - Time-dependent envelope misfit TPM - Time-dependent phase misfit FEM - Frequency-dependent envelope misfit FPM - Frequency-dependent phase misfit EM - Single-valued envelope misfit PM - Single-valued phase misfit The single-value about EM, PM is obtained.

Exemple (application) -reproduced Fig. Acceleration records of NS and EW components at PS10 PS10 Fig. Fourier spectra for acceleration records at PS10 PS10 where is 3km from the fault In the M7.9 Denali Fault, Alaska, earthquake of Nov. 3, 2002.

Continuous wavelet transform (CWT) 5sec shifted early in each result

Misfit Criteria -1 TFEM -Time-frequency envelope misfit TFPM -Time-frequency phase misfit

Misfit Criteria -2 Time-dependent envelope misfit Time-dependent phase misfit Frequency-dependent envelope misfit Frequency-dependent phase misfit

Misfit score EM PMRMS STATION CODE EM PM RMS PS09-Alaska PS10-Alaska PS11-Alaska FA02-Alaska STATION CODE SIMILARITY SCORE(S1) M PS09-Alaska PS10-Alaska PS11-Alaska FA02-Alaska