2009/04/06 09:30:12 42.373 13.341 10.1 3.00 Italy
USGS Felt map for this earthquake
USGS/SLU Moment Tensor Solution ENS 2009/04/06 09:30:12:0 42.37 13.34 10.1 3.0 Italy Stations used: IV.ASSB IV.CERA IV.CERT IV.CESI IV.CING IV.FDMO IV.GUAR IV.INTR IV.LPEL IV.MGAB IV.MNS IV.MTCE IV.OFFI IV.TERO IV.TOLF Filtering commands used: hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 1.01e+21 dyne-cm Mw = 3.27 Z = 9 km Plane Strike Dip Rake NP1 123 61 -132 NP2 5 50 -40 Principal Axes: Axis Value Plunge Azimuth T 1.01e+21 6 242 N 0.00e+00 36 148 P -1.01e+21 53 340 Moment Tensor: (dyne-cm) Component Value Mxx -9.82e+19 Mxy 5.29e+20 Mxz -5.06e+20 Myy 7.39e+20 Myz 6.91e+19 Mzz -6.40e+20 ----------#### ----------------###### --------------------######## ----------------------######## -------------------------######### #------------ -----------######### ##------------ P -----------########## ####----------- ------------########## #####-------------------------########## #######------------------------########### #########----------------------########### ##########---------------------########### ############-------------------########### ##############---------------########### # ############-------------########### T ###############---------########### ####################----########## ########################---------- #####################--------- ##################---------- ##############-------- #######------- Global CMT Convention Moment Tensor: R T P -6.40e+20 -5.06e+20 -6.91e+19 -5.06e+20 -9.82e+19 -5.29e+20 -6.91e+19 -5.29e+20 7.39e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20090406093012/index.html |
STK = 5 DIP = 50 RAKE = -40 MW = 3.27 HS = 9.0
The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2009/04/06 09:30:12:0 42.37 13.34 10.1 3.0 Italy Stations used: IV.ASSB IV.CERA IV.CERT IV.CESI IV.CING IV.FDMO IV.GUAR IV.INTR IV.LPEL IV.MGAB IV.MNS IV.MTCE IV.OFFI IV.TERO IV.TOLF Filtering commands used: hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 1.01e+21 dyne-cm Mw = 3.27 Z = 9 km Plane Strike Dip Rake NP1 123 61 -132 NP2 5 50 -40 Principal Axes: Axis Value Plunge Azimuth T 1.01e+21 6 242 N 0.00e+00 36 148 P -1.01e+21 53 340 Moment Tensor: (dyne-cm) Component Value Mxx -9.82e+19 Mxy 5.29e+20 Mxz -5.06e+20 Myy 7.39e+20 Myz 6.91e+19 Mzz -6.40e+20 ----------#### ----------------###### --------------------######## ----------------------######## -------------------------######### #------------ -----------######### ##------------ P -----------########## ####----------- ------------########## #####-------------------------########## #######------------------------########### #########----------------------########### ##########---------------------########### ############-------------------########### ##############---------------########### # ############-------------########### T ###############---------########### ####################----########## ########################---------- #####################--------- ##################---------- ##############-------- #######------- Global CMT Convention Moment Tensor: R T P -6.40e+20 -5.06e+20 -6.91e+19 -5.06e+20 -9.82e+19 -5.29e+20 -6.91e+19 -5.29e+20 7.39e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20090406093012/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:
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 0.5 245 35 65 2.99 0.2450 WVFGRD96 1.0 230 40 40 3.03 0.2482 WVFGRD96 2.0 220 35 25 3.13 0.2902 WVFGRD96 3.0 215 40 20 3.14 0.3360 WVFGRD96 4.0 215 50 25 3.16 0.3682 WVFGRD96 5.0 15 40 -15 3.23 0.3958 WVFGRD96 6.0 0 40 -50 3.28 0.4349 WVFGRD96 7.0 0 45 -50 3.29 0.4633 WVFGRD96 8.0 5 50 -40 3.26 0.4622 WVFGRD96 9.0 5 50 -40 3.27 0.4640 WVFGRD96 10.0 10 55 -30 3.28 0.4623 WVFGRD96 11.0 10 55 -30 3.29 0.4563 WVFGRD96 12.0 15 55 -25 3.30 0.4471 WVFGRD96 13.0 15 55 -20 3.30 0.4377 WVFGRD96 14.0 15 55 -20 3.31 0.4273 WVFGRD96 15.0 15 55 -20 3.34 0.4230 WVFGRD96 16.0 15 55 -20 3.35 0.4141 WVFGRD96 17.0 20 55 -15 3.36 0.4066 WVFGRD96 18.0 20 55 -10 3.37 0.4001 WVFGRD96 19.0 20 55 -10 3.38 0.3939 WVFGRD96 20.0 20 55 -10 3.38 0.3881 WVFGRD96 21.0 20 50 -5 3.39 0.3836 WVFGRD96 22.0 25 50 0 3.40 0.3806 WVFGRD96 23.0 25 50 0 3.41 0.3791 WVFGRD96 24.0 25 50 0 3.42 0.3766 WVFGRD96 25.0 25 50 0 3.43 0.3726 WVFGRD96 26.0 20 55 -5 3.44 0.3694 WVFGRD96 27.0 20 55 -10 3.45 0.3667 WVFGRD96 28.0 20 55 -5 3.46 0.3644 WVFGRD96 29.0 20 60 -5 3.47 0.3614
The best solution is
WVFGRD96 9.0 5 50 -40 3.27 0.4640
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. 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
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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. |
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 May 1 16:06:49 CDT 2009