2013/07/12 04:58:04 44.219 10.110 10.3 3.3 Italy
USGS Felt map for this earthquake
SLU Moment Tensor Solution
ENS 2013/07/12 04:58:04:0 44.22 10.11 10.3 3.3 Italy
Stations used:
GU.ENR GU.FINB GU.GORR GU.MAIM GU.PCP GU.PZZ GU.STV IV.ARVD
IV.ASQU IV.BDI IV.BOB IV.CRMI IV.CSNT IV.FNVD IV.GROG
IV.IMI IV.MGAB IV.MSSA IV.MURB IV.OSSC IV.PARC IV.PIEI
IV.PLMA IV.QLNO IV.SSFR IV.ZCCA MN.VLC
Filtering commands used:
cut a -10 a 80
rtr
taper w 0.1
hp c 0.02 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 1.16e+21 dyne-cm
Mw = 3.31
Z = 7 km
Plane Strike Dip Rake
NP1 280 45 -90
NP2 100 45 -90
Principal Axes:
Axis Value Plunge Azimuth
T 1.16e+21 -0 10
N 0.00e+00 -0 280
P -1.16e+21 90 135
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.13e+21
Mxy 1.99e+20
Mxz -5.62e+13
Myy 3.50e+19
Myz 2.65e+13
Mzz -1.16e+21
######### T ##
############# ######
############################
##############################
##################################
#######-----------------############
####-------------------------#########
##-------------------------------#######
-----------------------------------#####
#-------------------------------------####
##-------------------------------------###
###------------------- ---------------##
####------------------ P ----------------#
#####---------------- ----------------
#######-------------------------------##
#########-------------------------####
############-----------------#######
##################################
##############################
############################
######################
##############
Global CMT Convention Moment Tensor:
R T P
-1.16e+21 -5.62e+13 -2.65e+13
-5.62e+13 1.13e+21 -1.99e+20
-2.65e+13 -1.99e+20 3.50e+19
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20130712045804/index.html
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STK = 100
DIP = 45
RAKE = -90
MW = 3.31
HS = 7.0
The NDK file is 20130712045804.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution
ENS 2013/07/12 04:58:04:0 44.22 10.11 10.3 3.3 Italy
Stations used:
GU.ENR GU.FINB GU.GORR GU.MAIM GU.PCP GU.PZZ GU.STV IV.ARVD
IV.ASQU IV.BDI IV.BOB IV.CRMI IV.CSNT IV.FNVD IV.GROG
IV.IMI IV.MGAB IV.MSSA IV.MURB IV.OSSC IV.PARC IV.PIEI
IV.PLMA IV.QLNO IV.SSFR IV.ZCCA MN.VLC
Filtering commands used:
cut a -10 a 80
rtr
taper w 0.1
hp c 0.02 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 1.16e+21 dyne-cm
Mw = 3.31
Z = 7 km
Plane Strike Dip Rake
NP1 280 45 -90
NP2 100 45 -90
Principal Axes:
Axis Value Plunge Azimuth
T 1.16e+21 -0 10
N 0.00e+00 -0 280
P -1.16e+21 90 135
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.13e+21
Mxy 1.99e+20
Mxz -5.62e+13
Myy 3.50e+19
Myz 2.65e+13
Mzz -1.16e+21
######### T ##
############# ######
############################
##############################
##################################
#######-----------------############
####-------------------------#########
##-------------------------------#######
-----------------------------------#####
#-------------------------------------####
##-------------------------------------###
###------------------- ---------------##
####------------------ P ----------------#
#####---------------- ----------------
#######-------------------------------##
#########-------------------------####
############-----------------#######
##################################
##############################
############################
######################
##############
Global CMT Convention Moment Tensor:
R T P
-1.16e+21 -5.62e+13 -2.65e+13
-5.62e+13 1.13e+21 -1.99e+20
-2.65e+13 -1.99e+20 3.50e+19
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20130712045804/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 80 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 65 60 2.96 0.2713
WVFGRD96 2.0 140 25 30 3.07 0.2998
WVFGRD96 3.0 325 70 -50 3.13 0.3583
WVFGRD96 4.0 310 60 -60 3.17 0.4091
WVFGRD96 5.0 305 55 -65 3.27 0.4301
WVFGRD96 6.0 105 50 -95 3.34 0.4924
WVFGRD96 7.0 100 45 -90 3.31 0.5069
WVFGRD96 8.0 100 45 -90 3.27 0.4804
WVFGRD96 9.0 100 45 -90 3.27 0.4577
WVFGRD96 10.0 100 45 -90 3.26 0.4326
WVFGRD96 11.0 100 45 -90 3.26 0.4075
WVFGRD96 12.0 300 60 -60 3.23 0.3838
WVFGRD96 13.0 300 65 -55 3.23 0.3663
WVFGRD96 14.0 320 60 40 3.22 0.3497
WVFGRD96 15.0 320 60 40 3.24 0.3356
WVFGRD96 16.0 320 60 40 3.25 0.3240
WVFGRD96 17.0 320 60 35 3.25 0.3113
WVFGRD96 18.0 320 60 35 3.26 0.2987
WVFGRD96 19.0 320 60 35 3.26 0.2859
WVFGRD96 20.0 320 60 35 3.27 0.2751
WVFGRD96 21.0 320 65 35 3.28 0.2658
WVFGRD96 22.0 320 60 35 3.28 0.2579
WVFGRD96 23.0 150 75 40 3.29 0.2530
WVFGRD96 24.0 155 70 40 3.29 0.2502
WVFGRD96 25.0 155 70 40 3.30 0.2474
WVFGRD96 26.0 155 70 40 3.31 0.2463
WVFGRD96 27.0 155 70 35 3.32 0.2444
WVFGRD96 28.0 155 65 45 3.32 0.2423
WVFGRD96 29.0 155 65 45 3.33 0.2393
The best solution is
WVFGRD96 7.0 100 45 -90 3.31 0.5069
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 80 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 08:17:26 CDT 2013