2013/07/12 03:34:06 44.206 10.108 10.8 3.5 Italy
USGS Felt map for this earthquake
SLU Moment Tensor Solution
ENS 2013/07/12 03:34:06:0 44.21 10.11 10.8 3.5 Italy
Stations used:
GU.BHB GU.ENR GU.FINB GU.GORR GU.MAIM GU.PCP GU.PZZ GU.STV
IV.ARVD IV.ASQU IV.BDI IV.BOB IV.CASP IV.CRMI IV.CSNT
IV.DOI IV.GROG IV.MGAB IV.MSSA IV.OSSC IV.PLMA IV.QLNO
IV.SSFR MN.VLC
Filtering commands used:
cut a -10 a 70
rtr
taper w 0.1
hp c 0.02 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 1.53e+21 dyne-cm
Mw = 3.39
Z = 7 km
Plane Strike Dip Rake
NP1 291 55 -87
NP2 105 35 -95
Principal Axes:
Axis Value Plunge Azimuth
T 1.53e+21 10 19
N 0.00e+00 3 109
P -1.53e+21 80 215
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.30e+21
Mxy 4.25e+20
Mxz 4.76e+20
Myy 1.34e+20
Myz 2.41e+20
Mzz -1.43e+21
############
################ T ###
################### ######
##############################
##################################
######--------######################
#---------------------################
---------------------------#############
------------------------------##########
#--------------------------------#########
##---------------------------------#######
###--------------- ----------------#####
####-------------- P -----------------####
####------------- ------------------##
#####-----------------------------------
######-------------------------------#
########-------------------------###
##########-------------------#####
################----##########
############################
######################
##############
Global CMT Convention Moment Tensor:
R T P
-1.43e+21 4.76e+20 -2.41e+20
4.76e+20 1.30e+21 -4.25e+20
-2.41e+20 -4.25e+20 1.34e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20130712033406/index.html
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STK = 105
DIP = 35
RAKE = -95
MW = 3.39
HS = 7.0
The NDK file is 20130712033406.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution
ENS 2013/07/12 03:34:06:0 44.21 10.11 10.8 3.5 Italy
Stations used:
GU.BHB GU.ENR GU.FINB GU.GORR GU.MAIM GU.PCP GU.PZZ GU.STV
IV.ARVD IV.ASQU IV.BDI IV.BOB IV.CASP IV.CRMI IV.CSNT
IV.DOI IV.GROG IV.MGAB IV.MSSA IV.OSSC IV.PLMA IV.QLNO
IV.SSFR MN.VLC
Filtering commands used:
cut a -10 a 70
rtr
taper w 0.1
hp c 0.02 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 1.53e+21 dyne-cm
Mw = 3.39
Z = 7 km
Plane Strike Dip Rake
NP1 291 55 -87
NP2 105 35 -95
Principal Axes:
Axis Value Plunge Azimuth
T 1.53e+21 10 19
N 0.00e+00 3 109
P -1.53e+21 80 215
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.30e+21
Mxy 4.25e+20
Mxz 4.76e+20
Myy 1.34e+20
Myz 2.41e+20
Mzz -1.43e+21
############
################ T ###
################### ######
##############################
##################################
######--------######################
#---------------------################
---------------------------#############
------------------------------##########
#--------------------------------#########
##---------------------------------#######
###--------------- ----------------#####
####-------------- P -----------------####
####------------- ------------------##
#####-----------------------------------
######-------------------------------#
########-------------------------###
##########-------------------#####
################----##########
############################
######################
##############
Global CMT Convention Moment Tensor:
R T P
-1.43e+21 4.76e+20 -2.41e+20
4.76e+20 1.30e+21 -4.25e+20
-2.41e+20 -4.25e+20 1.34e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20130712033406/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 70 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 90 -35 3.05 0.3477
WVFGRD96 2.0 160 90 60 3.18 0.3742
WVFGRD96 3.0 325 65 -50 3.22 0.4635
WVFGRD96 4.0 310 55 -65 3.27 0.5304
WVFGRD96 5.0 310 55 -70 3.37 0.5726
WVFGRD96 6.0 105 40 -100 3.40 0.6409
WVFGRD96 7.0 105 35 -95 3.39 0.6499
WVFGRD96 8.0 290 55 -85 3.35 0.6175
WVFGRD96 9.0 290 55 -85 3.34 0.5841
WVFGRD96 10.0 290 55 -85 3.33 0.5487
WVFGRD96 11.0 295 60 -80 3.33 0.5193
WVFGRD96 12.0 295 60 -80 3.33 0.4940
WVFGRD96 13.0 295 60 -80 3.34 0.4698
WVFGRD96 14.0 295 65 -80 3.34 0.4482
WVFGRD96 15.0 295 65 -80 3.38 0.4328
WVFGRD96 16.0 295 65 -85 3.39 0.4129
WVFGRD96 17.0 300 70 -80 3.39 0.3971
WVFGRD96 18.0 300 70 -80 3.40 0.3816
WVFGRD96 19.0 300 70 -80 3.41 0.3629
WVFGRD96 20.0 305 75 -80 3.41 0.3445
WVFGRD96 21.0 305 75 -80 3.42 0.3289
WVFGRD96 22.0 325 80 -60 3.37 0.3114
WVFGRD96 23.0 325 80 -65 3.38 0.3000
WVFGRD96 24.0 240 35 30 3.42 0.2901
WVFGRD96 25.0 240 35 30 3.43 0.2861
WVFGRD96 26.0 240 35 30 3.44 0.2819
WVFGRD96 27.0 245 35 35 3.45 0.2771
WVFGRD96 28.0 250 45 25 3.46 0.2721
WVFGRD96 29.0 250 45 25 3.47 0.2725
The best solution is
WVFGRD96 7.0 105 35 -95 3.39 0.6499
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 70 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=Fri Jul 12 08:17:45 CDT 2013