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QSHA meeting, 1/Juin/2007, Nice. The surface profiles in Grenoble area determined by the MASW measurements. Seiji Tsuno, Cecile Cornou, Pierre-Yves Bard (LGIT). Today’s presentation. Procedure of the MASW measurements in Grenoble area and those analyses - PowerPoint PPT Presentation
Citation preview
The surface profilesin Grenoble area
determinedby the MASW
measurements
The surface profilesin Grenoble area
determinedby the MASW
measurements
Seiji Tsuno, Cecile Cornou, Pierre-Yves Bard (LGIT)
Seiji Tsuno, Cecile Cornou, Pierre-Yves Bard (LGIT)
QSHA meeting, 1/Juin/2007, NiceQSHA meeting, 1/Juin/2007, Nice
Today’s presentationToday’s presentation
• Procedure of the MASW measurements in Grenoble area and those analyses
• Inversion of Rayleigh wave to S-wave velocity profiles
• Wave-length of Rayleigh in Grenoble area (combining between our results and the results by BRGM)
• Distribution maps of surface velocities and engineering bedrock
(combining between our results and the results by BRGM)
• On higher modes obtained by the MASW method
• Estimation of damping factors on surface
MASW measurements and the analyses
MASW measurements and the analyses
Concept of MASW methodConcept of MASW method
Measurement sitesMeasurement sites
ILL
MONSIEUR
G15
STADE
RAILWAY
MSPORT
G12KAWASE2
KAWASE1
IMPOT
CASERNE
BASTILE
CAMPUSTAILLAT
FORAGE
G03
ROCK Belledonne G10
ROCK Vercors G17
ROCK Bastile
G18
H/V Seismic station
MASW by BRGM
Outline of MeasurementOutline of MeasurementSite Longitude Latitude Date Interval Sampling Off-set distance Mass
Campus 5.772694 45.198379 22/1/2007 2m 4000Hz 0, 5, 10, 15, 20m 3, 5kg
Taillat 5.789989 45.194184 23/1/2007 3m 1000Hz 0, 10, 20m 5kg
G03 5.808 45.217 23/1/2007 2m 1000Hz 0, 10, 33m 3, 5kg
Forage 5.821 45.209 26/1/2007 3m 1000Hz 0, 10, 20, 40, 60m 5kg
Caserne 5.725 45.184 30/1/2007 2m 1000Hz 0, 10, 20m 5kg
Kawase1 5.722326 45.176963 29/1/2007 3m 1000Hz 0, 10,20m 5kg
Impot 5.705763 45.177218 25/1/2007 2m 1000Hz 0, 10m 5kg
Ill 5.695507 45.20791 29/1/2007 3m 1000Hz 0, 10, 20, 40m 5kg
Kawase2 5.720384 45.162182 25/1/2007 3m 1000Hz 0, 10, 20, 30m 5kg
G12 5.750955 45.154165 25/1/2007 2m 1000Hz 0, 10, 20, 30m 5kg
Msport 5.727886 45.144167 31/1/2007 3m 1000Hz 0, 20m 5kg
Railway 5.707417 45.150354 31/1/2007 3m 1000Hz 0, 20m 5kg
G18 5.676175 45.225047 24/1/2007 2m 1000Hz 0, 10m 5kg
Monsieur 5.683277 45.20038 24/1/2007 3m 1000Hz 0, 10, 15, 20, 40m 5kg
G15 5.686412 45.195187 24/1/2007 2m 1000Hz 0, 10, 20, 40m 5kg
Stade 5.693 45.165 25/1/2007 3m 1000Hz 0,10, 20m 5kg
Bastille 5.725 45.2 31/1/2007 1, 4m 4000Hz 0m 3, 5kg
G17 5.632 45.167 1/2/2007 1m 4000Hz 0, 20m 3kg
G10 5.85 45.198 1/2/2007 1m 4000Hz 0, 20, 40m 3kg
* Except Kawase1, we made hammer shots at both sites.
* At Bastille in Chartreuse, at G17 in Vercors, at G10 in Belledonne, we also made the measurements of MASW on horizontal waves.
Process of analysisProcess of analysis
Normalization (for the distance between a shot point and receivers)
High resolusion method (Capon)
Using the records integrated
Stacking (in time domain)
Multi-offset (in frequency domain)
HR BFM
Offset-40m
Offset-0m
Does the excitation of modes depend on the condition of shot points ? (and on the wave-length ?)
Recording
Sampling 1000Hz (4000Hz in rock site)
Array length of 46 or 69m – interval 2 or 3m (23 and/or 92m in rock site)
4.5Hz (Vertical sensors)
14Hz (Horizontal sensors in rock site)
Dispersion curve - north-east basin
Dispersion curve - north-east basin
Campus Taillat
G03 Forage
1st higher mode ?
Fundamental mode
PV =
100m/s
Dispersion curve - centre villeDispersion curve - centre ville
Caserne Kawase1
Impot Ill
PV =
200m/s
Dispersion curve - south of Grenoble
Dispersion curve - south of Grenoble
Kawase2 G12
Msport Railway
PV =
250m/s
Dispersion curve - west of Grenoble
Dispersion curve - west of Grenoble
G18 Monsieur
G15 Stade
PV =
100m/s
Dispersion curve - Rock sitesDispersion curve - Rock sites
Bastille G17
G10
2000m/s
1000m/s
2000m/s
Array response
- Array length 24m
Dispersion curve of Love wave - Rock sites
Dispersion curve of Love wave - Rock sites
Bastille G17
G10
1200m/s 500m/s
1400m/s
Array response
- Array length 24m
Comparison with dispersion curves
determined by microtremors
Comparison with dispersion curves
determined by microtremors
Campus Forage Taillat
Frequency (Hz)P
hase
ve
loci
ty (
m/s
ec)
Taillat
MASW(MLM) FK(F0) FK(H1) SPAC
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Forage
MASW(MLM) MASW(MLM) MASW(MLM) FK(F0) FK(H1) SPAC
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Campus
MASW(MLM) MASW(MLM) FK(F0) FK(H1) SPAC
0 10 20 30 40 50
100
200
300
400
500
Array response
Inversion of Rayleigh wave to S-wave velocity
profiles
Inversion of Rayleigh wave to S-wave velocity
profiles
InversionInversion Genetic algorithm after Yamanaka and Ishida (1995)
Target of fundamental mode of Rayleigh wave
Adopting of 3 or 4 layers
5 trials with different random numbers
Selection of minimum misfit result
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Campus
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
De
pth
(m
)S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
GA
S-wave vel. profiles - north-east basin
S-wave vel. profiles - north-east basin
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Campus
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Taillat
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Forage
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G03
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
S-wave vel. profiles - centre ville
S-wave vel. profiles - centre ville
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
CASERNE
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Kawase1
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
IMPOT
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
ILL
Observation Theoretical
0 10 20 30 40 50 60 70
100
200
300
400
500
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
S-wave vel. profiles - south of Grenoble
S-wave vel. profiles - south of Grenoble
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
KAWASE2
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G12
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
MSPORT
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
RAILWAY
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
S-wave vel. profiles - west of Grenoble
S-wave vel. profiles - west of Grenoble
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G18
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Monsieur
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G15
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
STADE
Observation Theoretical
0 10 20 30 40 50
100
200
300
400
500
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
S-wave velocity profiles - Rock sites
S-wave velocity profiles - Rock sites
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BASTILLE
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G17
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G10
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Dep
th (
m)
S-wave vel. (m/s)0 1000 2000 3000
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 1000 2000 3000
-60
-50
-40
-30
-20
-10
0
Dep
th (
m)
S-wave vel. (m/s)0 1000 2000 3000
-60
-50
-40
-30
-20
-10
0
Comparison of Love wave dispersion
Comparison of Love wave dispersion
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BASTILLE
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G17
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G10
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G10
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BASTILLE
Observation Theoretical
0 10 20 30 40 50 60 70 80 90 100
1000
2000
3000
4000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G17
Observation Theoretical
0 10 20 30 40 50
500
1000
1500
2000
Love Wave
Rayleigh Wave
Wave-length of Rayleigh in Grenoble
area
Wave-length of Rayleigh in Grenoble
area
Dispersion of Rayleigh waves- Sedimentary basin -
Dispersion of Rayleigh waves- Sedimentary basin -
Measurement by LGIT Measurement by BRGM
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
LGIT
0 10 20 30 40 50 60 70 80
100
200
300
400
500
600
700
800
900
1000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BRGM
0 10 20 30 40 50 60 70 80
100
200
300
400
500
600
700
800
900
1000
Wave length of Rayleigh waves
- Sedimentary basin -
Wave length of Rayleigh waves
- Sedimentary basin -
Measurement by LGIT Measurement by BRGM
Wa
ve le
ngth
(m
)
Phase velocity (m/s)
BRGM
0 200 400 600 800 1000
-140
-120
-100
-80
-60
-40
-20
0
Wa
ve le
ngth
(m
)
Phase velocity (m/s)
LGIT
0 200 400 600 800 1000
-140
-120
-100
-80
-60
-40
-20
0
Dispersion and Wave-length of Rayleigh waves - Rock site -
Dispersion and Wave-length of Rayleigh waves - Rock site -
Dispersion curve Wave-length
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BRGM LGIT Rock sites
0 10 20 30 40 50 60 70 80
500
1000
1500
2000
2500
3000
Wa
ve le
ngth
(m
)
Phase velocity (m/s)
BRGM LGIT Rock sites
0 500 10001500200025003000
-140
-120
-100
-80
-60
-40
-20
0
Dispersion and Wave-length of Love waves - Rock site -
Dispersion and Wave-length of Love waves - Rock site -
Wa
ve le
ngth
(m
)
Phase velocity (m/s)
Rayleigh Love
G17
0 500 1000 1500 2000 2500 3000
-140
-120
-100
-80
-60
-40
-20
0
Dispersion curve Wave-length
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Rayleigh Love
G170 10 20 30 40 50 60 70 80
500
1000
1500
2000
2500
3000
Dispersion and Wave-length of Rayleigh waves -
Microtremors -
Dispersion and Wave-length of Rayleigh waves -
Microtremors -
Dispersion curve Wave-length
Phase velocity (m/sec)
Wa
ve le
ngth
(m
)
MASW(F0) SPAC(F0) FK(F0) ESG model
0 500 1000 1500 2000-4000
-3000
-2000
-1000
0
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
MASW(F0) SPAC(F0) FK(F0) ESG model
1 100
500
1000
1500
2000
Comparison of wave-lengh of observation with ESG
model
Comparison of wave-lengh of observation with ESG
model
Wave-length
Phase velocity (m/sec)
Wa
ve le
ngth
(m
)
MASW(F0) SPAC(F0) FK(F0) ESG model
0 100 200 300 400 500 600 700-700
-600
-500
-400
-300
-200
-100
0
Vs 400m/s
Distribution maps of surface velocity and engineering
bedrockin Grenoble area
Distribution maps of surface velocity and engineering
bedrockin Grenoble area
Distribution of surface velocity of Rayleigh
wave
Distribution of surface velocity of Rayleigh
wave
Bedrock map in Grenoble basin
Phase velocity (m/sec)
Wa
ve le
ngth
(m
)
MASW(F0) SPAC(F0) FK(F0) ESG model
0 100 200 300 400 500 600 700-700
-600
-500
-400
-300
-200
-100
0
Distribution of surface velocity of Rayleigh wave - comparison of dif.
WL
Distribution of surface velocity of Rayleigh wave - comparison of dif.
WL
On surface
At WL 20m
At WL 50m
Distribution of surface velocity of Rayleigh wave -2
Distribution of surface velocity of Rayleigh wave -2
Distribution of surface velocity of Rayleigh wave - (m/s)
Observation map in Grenoble area
Observation map in Grenoble area
ILL -221
MONSIEUR -118
G15 -124
STADE -149
RAILWAY -256
MSPORT -327
G12 -232KAWASE2 -312
KAWASE1 -243
IMPOT -237
CASERNE -220
BASTILE -218
CAMPUS -116
TAILLAT -160
FORAGE -102
G03 -113
ROCK Belledonne G10 -217
ROCK Vercors G17 -145
ROCK Bastile -218
G18 -146
Unit – m/sec
253
86177
113
188151
262
146207276
167
115
119136
14286
172130
184
127117
115133177174
133
Depth of engineering bedrock (Vs 400 - 500m/s)
Depth of engineering bedrock (Vs 400 - 500m/s)
Bedrock map in Grenoble basin
Distribution of surface velocity of Rayleigh wave - (m/s)
Higher mode
- Can we use the dispersion of higher mode to invert for S-
wave velocity profiles ?
Higher mode
- Can we use the dispersion of higher mode to invert for S-
wave velocity profiles ?
Comparison of theoretical
dispersions with observations
Comparison of theoretical
dispersions with observations
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G03
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Taillat
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Phase velocity - TaillatPhase velocity – G03
F-K
Spe
ctra
Frequency (Hz)
TAILLAT
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
G03
Fundamental 1st higher mode
0 10 20 30 40 50
0.1
0.2
0.3
0.4
Power spectra (G03 and Taillat)
Dispersion curve in Forage
(borehole site)
Dispersion curve in Forage
(borehole site)
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Forage
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Phase velocityF-K spectra
F-K
Spe
ctra
Frequency (Hz)
Forage
Fundamental 1st higher mode
0 10 20 30 40 50
0.005
0.01
0.015
0.02
Power spectra
Estimation of damping factors
- Examples -
Estimation of damping factors
- Examples -
Waveform inversion using recordings of the MASW measurment (at Forage)
Waveform inversion using recordings of the MASW measurment (at Forage)
Comparison of theoretical waveforms (red line) calculated by DWM with observation recording (black line) generated by hammer hit
Q = 15 Q = 50(Frequency independent model)Propagation
Forage
Time (sec)
6m
9m
12m
15m
18m
21m
24m
27m
30m
0 0.2 0.4 0.6 0.8 1-180000
-170000
-160000
-150000
-140000
-130000
-120000
-110000
-100000
-90000
-80000
-70000
-60000
-50000
-40000
-30000
-20000
-10000
0
10000
20000
Forage
Time (sec)
6m
9m
12m
15m
18m
21m
24m
27m
30m
0 0.2 0.4 0.6 0.8 1-180000
-170000
-160000
-150000
-140000
-130000
-120000
-110000
-100000
-90000
-80000
-70000
-60000
-50000
-40000
-30000
-20000
-10000
0
10000
20000
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Ricker wavelet used in DWM (Forage)
Ricker wavelet used in DWM (Forage)
F-K spectraSource (Ricker wavelet 0.03s)
Dominant Period - 0.03s
0.4 0.45 0.5 0.55 0.6
-1
0
1
Frequency (Hz)
Po
we
r sp
ect
rum
Forage
Observation - offset 6m Ricker wave - 0.03s
1 10 1001e-06
1e-05
0.0001
0.001
0.01
0.1
Waveform inversion using recordings of the MASW
measurment (at G03)
Waveform inversion using recordings of the MASW
measurment (at G03)
Comparison of theoretical waveforms (red line) calculated by DWM with observation recording (black line) generated by hammer hit
Q = 15 Q = 50(Frequency independent model)Propagation
G03
Time (sec)
4m
8m
10m
12m
14m
16m
18m
20m
6m
0 0.2 0.4 0.6 0.8 1-200000
-190000
-180000
-170000
-160000
-150000
-140000
-130000
-120000
-110000
-100000
-90000
-80000
-70000
-60000
-50000
-40000
-30000
-20000
-10000
0
G03
Time (sec)
4m
8m
10m
12m
14m
16m
18m
20m
6m
0 0.2 0.4 0.6 0.8 1-200000
-190000
-180000
-170000
-160000
-150000
-140000
-130000
-120000
-110000
-100000
-90000
-80000
-70000
-60000
-50000
-40000
-30000
-20000
-10000
0
Dep
th (
m)
S-wave vel. (m/s)0 200 400 600
-60
-50
-40
-30
-20
-10
0
Ricker wavelet used in DWM (G03)
Ricker wavelet used in DWM (G03)
F-K spectraSource (Ricker wavelet 0.03s)
Dominant Period - 0.03s
0.4 0.45 0.5 0.55 0.6
-1
0
1
Frequency (Hz)
Po
we
r sp
ect
rum
Forage
Observation - offset 4m Ricker wave - 0.03s
1 10 1001e-06
1e-05
0.0001
0.001
0.01
0.1
ConclusionConclusion
• We determined the surface profiles in Grenoble area by the MASW method. Also, we made the distribution map of the engineering bedrock (Vs 400-500m/s) in Grenoble area.
• The dispersions of Rayleigh waves obtained by the MASW method are in agreement with those by microtremors.
• The S-wave velocity of 400-500m/sec is entirely appeared in Grenoble basin. On the other hand, the surface velocities higher than Vs 400m/s are quite various. Especially in the middle-west of Grenoble basin, the soft sediment (Vs < 400m/s) is deeply covered.
• We determined the S-wave velocity (Vs > 2km/sec) in rock sites.• The wave-length of Rayleigh waves in Grenoble area observed by
this study is slightly different from the previous model (ESG model).• We proposed the estimation method on quality factors of surface
layers using the waveforms excited by the hammer shot.
Individual dispersion(Sedimental basin)
Individual dispersion(Sedimental basin)
CampusCampus
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Campus
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Wave-length = 57.6m
Wave-length = 45.5m
TaillatTaillat
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Taillat
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Phase velocityF-K spectra
Wave-length = 66.5m
Wave-length = 84.7m
G03G03
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G03
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Wave-length = 65.7m
Wave-length = 95.8m
ForageForage
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Forage
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Wave-length = 53.4m
Wave-length = 26.6m
CaserneCaserne
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
CASERNE
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Wave-length = 25.7m
Wave-length = 43.8m
Kawase1Kawase1
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Kawase1
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Wave-length = 33.4m
Wave-length = 23.9m
ImpotImpot
Phase velocityF-K spectra
Wave-length = 44.5m
Wave-length = 48.8m
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)IMPOT
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
IllIll
Phase velocityF-K spectra
Wave-length = 22.3m
Wave-length = 81.1m
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
ILL
Fundamental Higher mode
0 10 20 30 40 50 60 70
100
200
300
400
500
Kawase2Kawase2
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
KAWASE2
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Wave-length = 44.3m
Wave-length = 41.1m
G12G12
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G12
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Wave-length = 46.5m
Wave-length = 83.2m
MsportMsport
Phase velocityF-K spectra
Wave-length = 47.4m
Wave-length = 52.7m
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
MSPORT
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
RailwayRailway
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
RAILWAY
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Wave-length = 69.4m
Wave-length = 62.5m
G18G18
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G18
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Wave-length = 45.5m
Wave-length = 43.3m
MonsieurMonsieur
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)Monsieur
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Wave-length = 41.2m
Wave-length = 39.9m
G15G15
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G15
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Wave-length = 33.8m
Wave-length = 30.1m
StadeStade
Phase velocityF-K spectra
Wave-length = 35.8m
Wave-length = 71.4m
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
STADE
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Higher mode dispersion -1
Higher mode dispersion -1
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Campus
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Taillat
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G03
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Forage
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
CASERNE
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
Kawase1
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Higher mode dispersion -2Higher mode dispersion -2
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G12
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)ILL
Fundamental Higher mode
0 10 20 30 40 50 60 70
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
MSPORT
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
IMPOT
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
KAWASE2
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
RAILWAY
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Higher mode dispersion -3
Higher mode dispersion -3
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G18
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
600
700
800
900
1000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)Monsieur
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G15
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
STADE
Fundamental Higher mode
0 10 20 30 40 50
100
200
300
400
500
F-K Power spectra -1F-K Power spectra -1F
-K S
pect
ra
Frequency (Hz)
Forage
Fundamental 1st higher mode
0 10 20 30 40 50
0.005
0.01
0.015
0.02
F-K
Spe
ctra
Frequency (Hz)
Campus
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
TAILLAT
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
G03
Fundamental 1st higher mode
0 10 20 30 40 50
0.1
0.2
0.3
0.4
F-K
Spe
ctra
Frequency (Hz)
CASERNE
Fundamental 1st higher mode
0 10 20 30 40 50
0.01
0.02
0.03
0.04
F-K
Spe
ctra
Frequency (Hz)
KAWASE1
Fundamental 1st higher mode
0 10 20 30 40 50
0.01
0.02
0.03
0.04
F-K Power spectra -2F-K Power spectra -2F
-K S
pect
ra
Frequency (Hz)
IMPOT
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
ILL
Fundamental 1st higher mode
0 10 20 30 40 50
0.005
0.01
0.015
0.02
F-K
Spe
ctra
Frequency (Hz)
KAWASE2
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
MSPORT
Fundamental 1st higher mode
0 10 20 30 40 50
0.01
0.02
0.03
0.04
F-K
Spe
ctra
Frequency (Hz)
RAILWAY
Fundamental 1st higher mode
0 10 20 30 40 50
0.01
0.02
0.03
0.04
F-K
Spe
ctra
Frequency (Hz)
G12
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K Power spectra -3F-K Power spectra -3F
-K S
pect
ra
Frequency (Hz)
G18
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
MONSIEUR
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
G15
Fundamental 1st higher mode
0 10 20 30 40 50
0.005
0.01
0.015
0.02
F-K
Spe
ctra
Frequency (Hz)
STADE
Fundamental 1st higher mode
0 10 20 30 40 50
0.05
0.1
0.15
0.2
Individual dispersion(Rock sites)
Individual dispersion(Rock sites)
Bastile - Rayleigh waveBastile - Rayleigh wave
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BASTILLE
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
Wave-length = 20.7m
Wave-length = 92.9m
G17 - Rayleigh waveG17 - Rayleigh wave
Phase velocityF-K spectra
Wave-length = 32m
Wave-length = 94.2m
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G17
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
G10 - Rayleigh waveG10 - Rayleigh wave
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G10
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Wave-length = 34.9m
Wave-length = 101.5m
Bastile - Love waveBastile - Love wave
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BASTILLE
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
1000
2000
3000
4000
Wave-length = 29.4m
Wave-length = 120.4m
G17 - Love waveG17 - Love wave
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G17
Fundamental Higher mode
0 10 20 30 40 50
500
1000
1500
2000
Wave-length = 31.3m
Wave-length = 53.4m
G10 - Love waveG10 - Love wave
Phase velocityF-K spectraFrequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G10
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Wave-length = 19.3m
Wave-length = 113.2m
Higher mode and Love wave dispersion
Higher mode and Love wave dispersion
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BASTILLE
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G17
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Love Wave
Rayleigh Wave
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G10
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
BASTILLE
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
1000
2000
3000
4000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G17
Fundamental Higher mode
0 10 20 30 40 50
500
1000
1500
2000
Frequency (Hz)
Pha
se v
elo
city
(m
/se
c)
G10
Fundamental Higher mode
0 10 20 30 40 50 60 70 80 90 100
500
1000
1500
2000
2500
3000
3500
4000
F-K Power spectra - R. and L.
F-K Power spectra - R. and L.
F-K
Spe
ctra
Frequency (Hz)
G10
Fundamental 1st higher mode
0 10 20 30 40 50 60 70 80 90 100
0.05
0.1
0.15
0.2
F-K
Spe
ctra
Frequency (Hz)
G17
Fundamental 1st higher mode
0 10 20 30 40 50 60 70 80 90 100
0.2
0.4
0.6
0.8
F-K
Spe
ctra
Frequency (Hz)
BASTILLE
Fundamental 1st higher mode
0 10 20 30 40 50 60 70 80 90 100
0.02
0.04
0.06
0.08
F-K
Spe
ctra
Frequency (Hz)
BASTILLE
Fundamental 1st higher mode
0 10 20 30 40 50 60 70 80 90 100
0.02
0.04
0.06
0.08
F-K
Spe
ctra
Frequency (Hz)
G17
Fundamental 1st higher mode
0 10 20 30 40 50 60 70 80 90 100
0.2
0.4
0.6
0.8
F-K
Spe
ctra
Frequency (Hz)
G10
Fundamental 1st higher mode
0 10 20 30 40 50 60 70 80 90 100
0.05
0.1
0.15
0.2
Love Wave
Rayleigh Wave
Next stepNext step• Estimation of S-wave velocity structures at measurement sites• Categorization of surface structures in Grenoble Basin• Comparison of the geological data• Detecting of common minimum velocity layer in Grenoble - for 3D simulation• For this purpose, do we need to take into account the results of array microtremors ?• Do we need to make more MASW measurements in Grenoble basin, for detail categorization on surface structures ? • Comparison these results with the proposed model
• Confirmation of the estimated shallow structures by using earthquake recordings (which recordings do we select ?)• We would estimate the damping factor on surface by applying the waveform inversion with the discrete wave-number method.• We include the higher mode and/or Love wave dispersion, to invert the S-wave velocity structures.
InversionInversion
We have three steps to invert the basin structures.
• With the dispersion of Rayleigh wave estimated by MASW method
• Taking account of the dispersion estimated by Array Microtermors
→ To determine deeper structures
• Including of Higher modes and/or the dispersion of Love wave
→ To determine structures in detail
Measurement errorsMeasurement errors
Time (sec)dV
/V (
Per
.)
Error
T=0.05s
T=0.1s
0 0.02 0.04 0.06 0.08
0
10
20
30
40
50
Distance (m)
dV/V
(P
er.)
Error
D=3m
D=2m
0 0.2 0.4 0.6 0.8 1
0
10
20
30
40
50
Time errorDistance error
Spectral inversion using earthquake
recording
Spectral inversion using earthquake
recording