2009/06/29 05:54:33 42.463 13.366 13.5 3.10 Italy
USGS Felt map for this earthquake
USGS/SLU Moment Tensor Solution ENS 2009/06/29 05:54:33:0 42.46 13.37 13.5 3.1 Italy Stations used: IV.ASSB IV.CERT IV.CESI IV.CESX IV.CING IV.FDMO IV.FIAM IV.GIUL IV.GUMA IV.INTR IV.LNSS IV.MTCE IV.NRCA IV.OFFI IV.RNI2 IV.SACS IV.TERO IV.TOLF MN.AQU Filtering commands used: hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 8.22e+20 dyne-cm Mw = 3.21 Z = 10 km Plane Strike Dip Rake NP1 335 65 -60 NP2 101 38 -137 Principal Axes: Axis Value Plunge Azimuth T 8.22e+20 15 44 N 0.00e+00 27 141 P -8.22e+20 59 288 Moment Tensor: (dyne-cm) Component Value Mxx 3.83e+20 Mxy 4.48e+20 Mxz 3.60e+19 Myy 1.63e+20 Myz 4.88e+20 Mzz -5.45e+20 ############## -----################# ----------############## # -------------############ T ## -----------------########## #### -------------------################# ----------------------################ ------------------------################ ----------- -----------############### #----------- P ------------############### #----------- -------------############## ##--------------------------############## ###--------------------------############# ####------------------------############ #####------------------------#########-- #######---------------------########-- #########------------------#####---- ############--------------#------- #########################----- #######################----- ####################-- ############## Global CMT Convention Moment Tensor: R T P -5.45e+20 3.60e+19 -4.88e+20 3.60e+19 3.83e+20 -4.48e+20 -4.88e+20 -4.48e+20 1.63e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20090629055433/index.html |
STK = 335 DIP = 65 RAKE = -60 MW = 3.21 HS = 10.0
The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2009/06/29 05:54:33:0 42.46 13.37 13.5 3.1 Italy Stations used: IV.ASSB IV.CERT IV.CESI IV.CESX IV.CING IV.FDMO IV.FIAM IV.GIUL IV.GUMA IV.INTR IV.LNSS IV.MTCE IV.NRCA IV.OFFI IV.RNI2 IV.SACS IV.TERO IV.TOLF MN.AQU Filtering commands used: hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 8.22e+20 dyne-cm Mw = 3.21 Z = 10 km Plane Strike Dip Rake NP1 335 65 -60 NP2 101 38 -137 Principal Axes: Axis Value Plunge Azimuth T 8.22e+20 15 44 N 0.00e+00 27 141 P -8.22e+20 59 288 Moment Tensor: (dyne-cm) Component Value Mxx 3.83e+20 Mxy 4.48e+20 Mxz 3.60e+19 Myy 1.63e+20 Myz 4.88e+20 Mzz -5.45e+20 ############## -----################# ----------############## # -------------############ T ## -----------------########## #### -------------------################# ----------------------################ ------------------------################ ----------- -----------############### #----------- P ------------############### #----------- -------------############## ##--------------------------############## ###--------------------------############# ####------------------------############ #####------------------------#########-- #######---------------------########-- #########------------------#####---- ############--------------#------- #########################----- #######################----- ####################-- ############## Global CMT Convention Moment Tensor: R T P -5.45e+20 3.60e+19 -4.88e+20 3.60e+19 3.83e+20 -4.48e+20 -4.88e+20 -4.48e+20 1.63e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20090629055433/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.
![]() |
|
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:
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 0.5 315 40 -85 2.94 0.2934 WVFGRD96 1.0 345 45 -40 2.96 0.2706 WVFGRD96 2.0 345 35 -35 3.04 0.2873 WVFGRD96 3.0 350 80 -65 3.08 0.3233 WVFGRD96 4.0 345 75 -65 3.09 0.3738 WVFGRD96 5.0 340 70 -70 3.20 0.4222 WVFGRD96 6.0 335 65 -70 3.22 0.4791 WVFGRD96 7.0 335 65 -65 3.22 0.5173 WVFGRD96 8.0 335 65 -60 3.20 0.5302 WVFGRD96 9.0 335 65 -60 3.20 0.5378 WVFGRD96 10.0 335 65 -60 3.21 0.5393 WVFGRD96 11.0 335 65 -60 3.22 0.5340 WVFGRD96 12.0 335 65 -65 3.23 0.5235 WVFGRD96 13.0 335 70 -65 3.23 0.5144 WVFGRD96 14.0 335 70 -65 3.24 0.5020 WVFGRD96 15.0 335 70 -65 3.28 0.4922 WVFGRD96 16.0 340 70 -65 3.29 0.4770 WVFGRD96 17.0 340 70 -65 3.30 0.4609 WVFGRD96 18.0 345 75 -60 3.30 0.4465 WVFGRD96 19.0 345 75 -60 3.31 0.4326 WVFGRD96 20.0 345 75 -60 3.32 0.4202 WVFGRD96 21.0 345 75 -60 3.33 0.4089 WVFGRD96 22.0 345 75 -60 3.34 0.4005 WVFGRD96 23.0 345 75 -60 3.34 0.3941 WVFGRD96 24.0 345 75 -60 3.35 0.3869 WVFGRD96 25.0 345 75 -60 3.36 0.3782 WVFGRD96 26.0 345 75 -60 3.36 0.3684 WVFGRD96 27.0 345 75 -55 3.37 0.3572 WVFGRD96 28.0 345 75 -55 3.37 0.3456 WVFGRD96 29.0 345 75 -55 3.38 0.3344
The best solution is
WVFGRD96 10.0 335 65 -60 3.21 0.5393
The mechanism correspond to the best fit is
![]() |
|
The best fit as a function of depth is given in the following figure:
![]() |
|
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. The number in black at the rightr of each predicted traces 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 bandpass filter used in the processing and for the display was
hp c 0.02 n 3 lp c 0.10 n 3
![]() |
|
![]() |
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. |
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=Mon Jun 29 08:11:46 CDT 2009