2016/10/26 18:39:19 42.8808 13.0925 10.0 3.4 Perugia
USGS Felt map for this earthquake
SLU Moment Tensor Solution
ENS 2016/10/26 18:39:19:4 42.88 13.09 10.0 3.4 Perugia
Stations used:
IV.AOI IV.ARVD IV.ATPC IV.ATTE IV.CAFI IV.CING IV.FDMO
IV.GUMA IV.MGAB IV.MTCE IV.MURB IV.PIEI IV.RMP IV.SACS
IV.SAMA IV.SNTG IV.TERO IV.TOLF 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 = 1.12e+21 dyne-cm
Mw = 3.30
Z = 6 km
Plane Strike Dip Rake
NP1 339 66 -97
NP2 175 25 -75
Principal Axes:
Axis Value Plunge Azimuth
T 1.12e+21 21 74
N 0.00e+00 6 341
P -1.12e+21 68 235
Moment Tensor: (dyne-cm)
Component Value
Mxx 2.76e+19
Mxy 1.93e+20
Mxz 3.23e+20
Myy 8.03e+20
Myz 6.71e+20
Mzz -8.30e+20
--############
###---################
####-------#################
####----------################
####-------------#################
####----------------################
#####-----------------################
#####-------------------########### ##
#####--------------------########## T ##
#####---------------------########## ###
#####----------------------###############
#####---------- ----------##############
#####---------- P ----------##############
#####--------- -----------############
#####-----------------------############
#####----------------------###########
#####----------------------#########
#####---------------------########
#####-------------------######
#####-----------------######
#####--------------###
####----------
Global CMT Convention Moment Tensor:
R T P
-8.30e+20 3.23e+20 -6.71e+20
3.23e+20 2.76e+19 -1.93e+20
-6.71e+20 -1.93e+20 8.03e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161026183919/index.html
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STK = 175
DIP = 25
RAKE = -75
MW = 3.30
HS = 6.0
The NDK file is 20161026183919.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution
ENS 2016/10/26 18:39:19:4 42.88 13.09 10.0 3.4 Perugia
Stations used:
IV.AOI IV.ARVD IV.ATPC IV.ATTE IV.CAFI IV.CING IV.FDMO
IV.GUMA IV.MGAB IV.MTCE IV.MURB IV.PIEI IV.RMP IV.SACS
IV.SAMA IV.SNTG IV.TERO IV.TOLF 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 = 1.12e+21 dyne-cm
Mw = 3.30
Z = 6 km
Plane Strike Dip Rake
NP1 339 66 -97
NP2 175 25 -75
Principal Axes:
Axis Value Plunge Azimuth
T 1.12e+21 21 74
N 0.00e+00 6 341
P -1.12e+21 68 235
Moment Tensor: (dyne-cm)
Component Value
Mxx 2.76e+19
Mxy 1.93e+20
Mxz 3.23e+20
Myy 8.03e+20
Myz 6.71e+20
Mzz -8.30e+20
--############
###---################
####-------#################
####----------################
####-------------#################
####----------------################
#####-----------------################
#####-------------------########### ##
#####--------------------########## T ##
#####---------------------########## ###
#####----------------------###############
#####---------- ----------##############
#####---------- P ----------##############
#####--------- -----------############
#####-----------------------############
#####----------------------###########
#####----------------------#########
#####---------------------########
#####-------------------######
#####-----------------######
#####--------------###
####----------
Global CMT Convention Moment Tensor:
R T P
-8.30e+20 3.23e+20 -6.71e+20
3.23e+20 2.76e+19 -1.93e+20
-6.71e+20 -1.93e+20 8.03e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161026183919/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 1.0 180 55 -70 3.06 0.4458
WVFGRD96 2.0 195 65 -55 3.09 0.4581
WVFGRD96 3.0 185 20 -60 3.18 0.5149
WVFGRD96 4.0 180 25 -70 3.19 0.5688
WVFGRD96 5.0 180 25 -70 3.29 0.6131
WVFGRD96 6.0 175 25 -75 3.30 0.6248
WVFGRD96 7.0 170 30 -80 3.29 0.6112
WVFGRD96 8.0 180 30 -70 3.25 0.5727
WVFGRD96 9.0 175 30 -75 3.25 0.5479
WVFGRD96 10.0 215 65 30 3.23 0.5352
WVFGRD96 11.0 215 65 30 3.24 0.5234
WVFGRD96 12.0 215 65 25 3.25 0.5092
WVFGRD96 13.0 215 65 25 3.27 0.4952
WVFGRD96 14.0 215 60 25 3.28 0.4813
WVFGRD96 15.0 215 60 25 3.30 0.4558
WVFGRD96 16.0 215 60 25 3.31 0.4380
WVFGRD96 17.0 195 50 -45 3.28 0.4231
WVFGRD96 18.0 200 55 -40 3.29 0.4174
WVFGRD96 19.0 200 55 -40 3.30 0.4138
WVFGRD96 20.0 200 55 -40 3.31 0.4097
WVFGRD96 21.0 200 55 -40 3.32 0.4063
WVFGRD96 22.0 200 55 -40 3.33 0.4025
WVFGRD96 23.0 345 40 -90 3.37 0.3993
WVFGRD96 24.0 200 60 -35 3.34 0.3968
WVFGRD96 25.0 200 60 -35 3.35 0.3918
WVFGRD96 26.0 195 60 -40 3.36 0.3891
WVFGRD96 27.0 195 60 -40 3.37 0.3842
WVFGRD96 28.0 195 65 -45 3.38 0.3774
WVFGRD96 29.0 195 65 -45 3.39 0.3743
The best solution is
WVFGRD96 6.0 175 25 -75 3.30 0.6248
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=Thu Oct 27 15:09:35 CDT 2016