2016/10/29 23:01:34 43.0653 13.0667 8.6 3.3 Macerata
USGS Felt map for this earthquake
SLU Moment Tensor Solution
ENS 2016/10/29 23:01:34:1 43.07 13.07 8.6 3.3 Macerata
Stations used:
IV.ARVD IV.ATFO IV.ATTE IV.CING IV.CRE IV.CSNT IV.GUMA
IV.MGAB IV.MTCE IV.MURB IV.OFFI IV.OSSC IV.PTQR IV.RMP
IV.SACS IV.SNTG MN.AQU
Filtering commands used:
cut o DIST/3.3 -20 o DIST/3.3 +40
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 9.77e+20 dyne-cm
Mw = 3.26
Z = 5 km
Plane Strike Dip Rake
NP1 160 65 -65
NP2 292 35 -132
Principal Axes:
Axis Value Plunge Azimuth
T 9.77e+20 16 232
N 0.00e+00 23 329
P -9.77e+20 62 109
Moment Tensor: (dyne-cm)
Component Value
Mxx 3.20e+20
Mxy 5.05e+20
Mxz -3.07e+19
Myy 3.59e+20
Myz -5.95e+20
Mzz -6.78e+20
##############
---###################
------######################
------#---------##############
---#####---------------###########
-########-------------------########
###########--------------------#######
############----------------------######
############-----------------------#####
##############------------------------####
##############-------------------------###
###############------------ ---------###
###############------------ P ----------##
###############----------- ----------#
################-----------------------#
### ##########----------------------
## T ###########--------------------
# ############------------------
###############---------------
################------------
###############-------
##############
Global CMT Convention Moment Tensor:
R T P
-6.78e+20 -3.07e+19 5.95e+20
-3.07e+19 3.20e+20 -5.05e+20
5.95e+20 -5.05e+20 3.59e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161029230134/index.html
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STK = 160
DIP = 65
RAKE = -65
MW = 3.26
HS = 5.0
The NDK file is 20161029230134.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution
ENS 2016/10/29 23:01:34:1 43.07 13.07 8.6 3.3 Macerata
Stations used:
IV.ARVD IV.ATFO IV.ATTE IV.CING IV.CRE IV.CSNT IV.GUMA
IV.MGAB IV.MTCE IV.MURB IV.OFFI IV.OSSC IV.PTQR IV.RMP
IV.SACS IV.SNTG MN.AQU
Filtering commands used:
cut o DIST/3.3 -20 o DIST/3.3 +40
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 9.77e+20 dyne-cm
Mw = 3.26
Z = 5 km
Plane Strike Dip Rake
NP1 160 65 -65
NP2 292 35 -132
Principal Axes:
Axis Value Plunge Azimuth
T 9.77e+20 16 232
N 0.00e+00 23 329
P -9.77e+20 62 109
Moment Tensor: (dyne-cm)
Component Value
Mxx 3.20e+20
Mxy 5.05e+20
Mxz -3.07e+19
Myy 3.59e+20
Myz -5.95e+20
Mzz -6.78e+20
##############
---###################
------######################
------#---------##############
---#####---------------###########
-########-------------------########
###########--------------------#######
############----------------------######
############-----------------------#####
##############------------------------####
##############-------------------------###
###############------------ ---------###
###############------------ P ----------##
###############----------- ----------#
################-----------------------#
### ##########----------------------
## T ###########--------------------
# ############------------------
###############---------------
################------------
###############-------
##############
Global CMT Convention Moment Tensor:
R T P
-6.78e+20 -3.07e+19 5.95e+20
-3.07e+19 3.20e+20 -5.05e+20
5.95e+20 -5.05e+20 3.59e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161029230134/index.html
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The focal mechanism was determined using broadband seismic waveforms. The location of the event and the and stations used for the waveform inversion are shown in the next figure.
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The program wvfgrd96 was used with good traces observed at short distance to determine the focal mechanism, depth and seismic moment. This technique requires a high quality signal and well determined velocity model for the Green functions. To the extent that these are the quality data, this type of mechanism should be preferred over the radiation pattern technique which requires the separate step of defining the pressure and tension quadrants and the correct strike.
The observed and predicted traces are filtered using the following gsac commands:
cut o DIST/3.3 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT
WVFGRD96 1.0 175 80 -55 3.05 0.4857
WVFGRD96 2.0 175 80 -60 3.14 0.5568
WVFGRD96 3.0 165 70 -60 3.16 0.6034
WVFGRD96 4.0 160 60 -60 3.19 0.6265
WVFGRD96 5.0 160 65 -65 3.26 0.6386
WVFGRD96 6.0 160 60 -60 3.26 0.6330
WVFGRD96 7.0 155 55 -65 3.29 0.6168
WVFGRD96 8.0 165 55 -45 3.25 0.5944
WVFGRD96 9.0 170 65 -40 3.23 0.5785
WVFGRD96 10.0 165 50 -45 3.29 0.5617
WVFGRD96 11.0 10 70 30 3.23 0.5497
WVFGRD96 12.0 10 70 30 3.24 0.5369
WVFGRD96 13.0 10 70 30 3.25 0.5234
WVFGRD96 14.0 10 65 30 3.27 0.5114
WVFGRD96 15.0 10 70 35 3.28 0.4978
WVFGRD96 16.0 10 65 35 3.30 0.4868
WVFGRD96 17.0 15 60 40 3.32 0.4760
WVFGRD96 18.0 15 60 40 3.32 0.4664
WVFGRD96 19.0 15 60 40 3.33 0.4562
WVFGRD96 20.0 15 60 40 3.33 0.4476
WVFGRD96 21.0 15 60 40 3.34 0.4371
WVFGRD96 22.0 15 60 40 3.34 0.4263
WVFGRD96 23.0 20 45 45 3.38 0.4166
WVFGRD96 24.0 20 50 45 3.38 0.4127
WVFGRD96 25.0 20 50 45 3.38 0.4086
WVFGRD96 26.0 20 50 45 3.39 0.4041
WVFGRD96 27.0 15 50 40 3.39 0.4003
WVFGRD96 28.0 15 50 40 3.40 0.3975
WVFGRD96 29.0 15 50 40 3.42 0.3976
The best solution is
WVFGRD96 5.0 160 65 -65 3.26 0.6386
The mechanism correspond to the best fit is
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The best fit as a function of depth is given in the following figure:
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The comparison of the observed and predicted waveforms is given in the next figure. The red traces are the observed and the blue are the predicted. Each observed-predicted component is plotted to the same scale and peak amplitudes are indicated by the numbers to the left of each trace. A pair of numbers is given in black at the right of each predicted traces. The upper number it the time shift required for maximum correlation between the observed and predicted traces. This time shift is required because the synthetics are not computed at exactly the same distance as the observed and because the velocity model used in the predictions may not be perfect. A positive time shift indicates that the prediction is too fast and should be delayed to match the observed trace (shift to the right in this figure). A negative value indicates that the prediction is too slow. The lower number gives the percentage of variance reduction to characterize the individual goodness of fit (100% indicates a perfect fit).
The bandpass filter used in the processing and for the display was
cut o DIST/3.3 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3
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| Focal mechanism sensitivity at the preferred depth. The red color indicates a very good fit to thewavefroms. Each solution is plotted as a vector at a given value of strike and dip with the angle of the vector representing the rake angle, measured, with respect to the upward vertical (N) in the figure. |
A check on the assumed source location is possible by looking at the time shifts between the observed and predicted traces. The time shifts for waveform matching arise for several reasons:
Time_shift = A + B cos Azimuth + C Sin Azimuth
The time shifts for this inversion lead to the next figure:
The derived shift in origin time and epicentral coordinates are given at the bottom of the figure.
The nnCIA used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows:
MODEL.01
C.It. A. Di Luzio et al Earth Plan Lettrs 280 (2009) 1-12 Fig 5. 7-8 MODEL/SURF3
ISOTROPIC
KGS
FLAT EARTH
1-D
CONSTANT VELOCITY
LINE08
LINE09
LINE10
LINE11
H(KM) VP(KM/S) VS(KM/S) RHO(GM/CC) QP QS ETAP ETAS FREFP FREFS
1.5000 3.7497 2.1436 2.2753 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00
3.0000 4.9399 2.8210 2.4858 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00
3.0000 6.0129 3.4336 2.7058 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00
7.0000 5.5516 3.1475 2.6093 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
15.0000 5.8805 3.3583 2.6770 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
6.0000 7.1059 4.0081 3.0002 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
8.0000 7.1000 3.9864 3.0120 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
0.0000 7.9000 4.4036 3.2760 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
Here we tabulate the reasons for not using certain digital data sets
The following stations did not have a valid response files:
DATE=Sat Oct 29 20:33:36 CDT 2016