2014/04/19 21:27:53 43.347 12.533 8.4 3.70 Italy
USGS Felt map for this earthquake
SLU Moment Tensor Solution
ENS 2014/04/19 21:27:53:0 43.35 12.53 8.4 3.7 Italy
Stations used:
GU.MAIM IV.ARVD IV.ASQU IV.BDI IV.CAFI IV.CAMP IV.CASP
IV.CERA IV.CESX IV.CING IV.CRE IV.CRMI IV.CSNT IV.FDMO
IV.FIAM IV.FSSB IV.GUMA IV.MGAB IV.MTCE IV.NRCA IV.OFFI
IV.OSSC IV.PARC IV.PLMA IV.PTQR IV.SACS IV.SNTG IV.SSFR
MN.VLC
Filtering commands used:
cut a -10 a 60
rtr
taper w 0.1
hp c 0.02 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 4.03e+21 dyne-cm
Mw = 3.67
Z = 3 km
Plane Strike Dip Rake
NP1 330 65 -80
NP2 127 27 -110
Principal Axes:
Axis Value Plunge Azimuth
T 4.03e+21 19 53
N 0.00e+00 9 146
P -4.03e+21 68 260
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.31e+21
Mxy 1.63e+21
Mxz 1.02e+21
Myy 1.73e+21
Myz 2.36e+21
Mzz -3.04e+21
##############
--####################
--------####################
------------##################
----------------############# ##
#------------------########### T ###
#--------------------########## ####
##---------------------#################
##-----------------------###############
###------------------------###############
###----------- -----------##############
####---------- P ------------#############
####---------- ------------#############
####-------------------------###########
#####-------------------------##########
######-----------------------#########
######----------------------########
#######---------------------######
########------------------####
###########-----------------
#####################-
##############
Global CMT Convention Moment Tensor:
R T P
-3.04e+21 1.02e+21 -2.36e+21
1.02e+21 1.31e+21 -1.63e+21
-2.36e+21 -1.63e+21 1.73e+21
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20140419212753/index.html
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STK = 330
DIP = 65
RAKE = -80
MW = 3.67
HS = 3.0
The NDK file is 20140419212753.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution
ENS 2014/04/19 21:27:53:0 43.35 12.53 8.4 3.7 Italy
Stations used:
GU.MAIM IV.ARVD IV.ASQU IV.BDI IV.CAFI IV.CAMP IV.CASP
IV.CERA IV.CESX IV.CING IV.CRE IV.CRMI IV.CSNT IV.FDMO
IV.FIAM IV.FSSB IV.GUMA IV.MGAB IV.MTCE IV.NRCA IV.OFFI
IV.OSSC IV.PARC IV.PLMA IV.PTQR IV.SACS IV.SNTG IV.SSFR
MN.VLC
Filtering commands used:
cut a -10 a 60
rtr
taper w 0.1
hp c 0.02 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 4.03e+21 dyne-cm
Mw = 3.67
Z = 3 km
Plane Strike Dip Rake
NP1 330 65 -80
NP2 127 27 -110
Principal Axes:
Axis Value Plunge Azimuth
T 4.03e+21 19 53
N 0.00e+00 9 146
P -4.03e+21 68 260
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.31e+21
Mxy 1.63e+21
Mxz 1.02e+21
Myy 1.73e+21
Myz 2.36e+21
Mzz -3.04e+21
##############
--####################
--------####################
------------##################
----------------############# ##
#------------------########### T ###
#--------------------########## ####
##---------------------#################
##-----------------------###############
###------------------------###############
###----------- -----------##############
####---------- P ------------#############
####---------- ------------#############
####-------------------------###########
#####-------------------------##########
######-----------------------#########
######----------------------########
#######---------------------######
########------------------####
###########-----------------
#####################-
##############
Global CMT Convention Moment Tensor:
R T P
-3.04e+21 1.02e+21 -2.36e+21
1.02e+21 1.31e+21 -1.63e+21
-2.36e+21 -1.63e+21 1.73e+21
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20140419212753/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 a -10 a 60 rtr taper w 0.1 hp c 0.02 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 1.0 340 70 -75 3.59 0.4851
WVFGRD96 2.0 335 70 -80 3.67 0.5499
WVFGRD96 3.0 330 65 -80 3.67 0.5657
WVFGRD96 4.0 330 60 -80 3.67 0.5390
WVFGRD96 5.0 325 60 -85 3.75 0.5315
WVFGRD96 6.0 325 65 -90 3.71 0.4524
WVFGRD96 7.0 355 75 -50 3.65 0.3962
WVFGRD96 8.0 195 65 30 3.65 0.3905
WVFGRD96 9.0 195 65 30 3.65 0.3798
WVFGRD96 10.0 195 65 30 3.66 0.3698
WVFGRD96 11.0 195 60 25 3.68 0.3602
WVFGRD96 12.0 195 60 25 3.69 0.3514
WVFGRD96 13.0 195 60 25 3.70 0.3430
WVFGRD96 14.0 195 60 25 3.71 0.3365
WVFGRD96 15.0 195 60 30 3.73 0.3198
WVFGRD96 16.0 195 60 25 3.73 0.3118
WVFGRD96 17.0 195 60 25 3.74 0.3050
WVFGRD96 18.0 195 60 25 3.75 0.2988
WVFGRD96 19.0 195 60 25 3.76 0.2930
WVFGRD96 20.0 195 60 25 3.77 0.2878
WVFGRD96 21.0 290 55 50 3.78 0.2877
WVFGRD96 22.0 290 55 50 3.79 0.2874
WVFGRD96 23.0 295 50 55 3.80 0.2876
WVFGRD96 24.0 155 50 110 3.81 0.2915
WVFGRD96 25.0 310 40 75 3.82 0.2961
WVFGRD96 26.0 315 40 80 3.83 0.3008
WVFGRD96 27.0 135 50 80 3.85 0.3042
WVFGRD96 28.0 330 40 100 3.86 0.3058
WVFGRD96 29.0 140 50 85 3.88 0.3049
The best solution is
WVFGRD96 3.0 330 65 -80 3.67 0.5657
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 a -10 a 60 rtr taper w 0.1 hp c 0.02 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 Apr 19 17:17:54 CDT 2014