2014/10/25 20:09:47 38.166 15.937 18.9 3.5 Italy
USGS Felt map for this earthquake
SLU Moment Tensor Solution ENS 2014/10/25 20:09:47:0 38.17 15.94 18.9 3.5 Italy Stations used: IV.CAR1 IV.CELI IV.JOPP IV.MCSR IV.MPNC IV.PLAC IV.SERS MN.CEL Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 9.44e+20 dyne-cm Mw = 3.25 Z = 12 km Plane Strike Dip Rake NP1 275 75 -65 NP2 34 29 -148 Principal Axes: Axis Value Plunge Azimuth T 9.44e+20 26 346 N 0.00e+00 24 88 P -9.44e+20 53 215 Moment Tensor: (dyne-cm) Component Value Mxx 4.91e+20 Mxy -3.42e+20 Mxz 7.29e+20 Myy -6.37e+19 Myz 1.67e+20 Mzz -4.28e+20 ############## ###### ############# ######### T ###############- ########## ################- ################################-- #################################--- ###################################--- ####################################---- ####################################---- ###--------------------------########----- ------------------------------------#----- -------------------------------------###-- ------------------------------------###### ----------------------------------###### ------------- ------------------###### ------------ P ----------------####### ----------- ---------------####### --------------------------######## ----------------------######## ------------------########## #---------############ ############## Global CMT Convention Moment Tensor: R T P -4.28e+20 7.29e+20 -1.67e+20 7.29e+20 4.91e+20 3.42e+20 -1.67e+20 3.42e+20 -6.37e+19 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20141025200947/index.html |
STK = 275 DIP = 75 RAKE = -65 MW = 3.25 HS = 12.0
The NDK file is 20141025200947.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution ENS 2014/10/25 20:09:47:0 38.17 15.94 18.9 3.5 Italy Stations used: IV.CAR1 IV.CELI IV.JOPP IV.MCSR IV.MPNC IV.PLAC IV.SERS MN.CEL Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 9.44e+20 dyne-cm Mw = 3.25 Z = 12 km Plane Strike Dip Rake NP1 275 75 -65 NP2 34 29 -148 Principal Axes: Axis Value Plunge Azimuth T 9.44e+20 26 346 N 0.00e+00 24 88 P -9.44e+20 53 215 Moment Tensor: (dyne-cm) Component Value Mxx 4.91e+20 Mxy -3.42e+20 Mxz 7.29e+20 Myy -6.37e+19 Myz 1.67e+20 Mzz -4.28e+20 ############## ###### ############# ######### T ###############- ########## ################- ################################-- #################################--- ###################################--- ####################################---- ####################################---- ###--------------------------########----- ------------------------------------#----- -------------------------------------###-- ------------------------------------###### ----------------------------------###### ------------- ------------------###### ------------ P ----------------####### ----------- ---------------####### --------------------------######## ----------------------######## ------------------########## #---------############ ############## Global CMT Convention Moment Tensor: R T P -4.28e+20 7.29e+20 -1.67e+20 7.29e+20 4.91e+20 3.42e+20 -1.67e+20 3.42e+20 -6.37e+19 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20141025200947/index.html |
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 -30 o DIST/3.3 +70 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 95 45 85 3.01 0.3323 WVFGRD96 2.0 85 35 75 3.10 0.3081 WVFGRD96 3.0 280 90 -75 3.11 0.3154 WVFGRD96 4.0 280 90 -70 3.09 0.3649 WVFGRD96 5.0 100 90 70 3.21 0.4012 WVFGRD96 6.0 275 85 -70 3.21 0.4422 WVFGRD96 7.0 275 80 -70 3.23 0.4749 WVFGRD96 8.0 275 80 -65 3.20 0.4989 WVFGRD96 9.0 280 80 -65 3.21 0.5131 WVFGRD96 10.0 275 75 -65 3.23 0.5216 WVFGRD96 11.0 275 75 -65 3.24 0.5270 WVFGRD96 12.0 275 75 -65 3.25 0.5280 WVFGRD96 13.0 280 75 -65 3.26 0.5273 WVFGRD96 14.0 275 70 -70 3.26 0.5247 WVFGRD96 15.0 275 70 -70 3.32 0.5236 WVFGRD96 16.0 275 70 -70 3.33 0.5176 WVFGRD96 17.0 275 70 -70 3.34 0.5095 WVFGRD96 18.0 270 65 -80 3.35 0.4984 WVFGRD96 19.0 270 65 -80 3.36 0.4868 WVFGRD96 20.0 275 65 -75 3.37 0.4736 WVFGRD96 21.0 270 60 -80 3.38 0.4601 WVFGRD96 22.0 275 60 -75 3.39 0.4466 WVFGRD96 23.0 275 60 -75 3.40 0.4333 WVFGRD96 24.0 275 60 -75 3.41 0.4201 WVFGRD96 25.0 280 60 -70 3.42 0.4076 WVFGRD96 26.0 170 30 5 3.47 0.3951 WVFGRD96 27.0 180 50 0 3.51 0.3893 WVFGRD96 28.0 180 50 0 3.52 0.3836 WVFGRD96 29.0 180 50 0 3.52 0.3778
The best solution is
WVFGRD96 12.0 275 75 -65 3.25 0.5280
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 -30 o DIST/3.3 +70 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 25 20:04:11 CDT 2014