2014/11/30 09:34:25 44.573 9.426 12.0 3.8 Italy
USGS Felt map for this earthquake
SLU Moment Tensor Solution ENS 2014/11/30 09:34:25:0 44.57 9.43 12.0 3.8 Italy Stations used: FR.SAOF FR.TURF GU.FINB GU.MAIM GU.PZZ GU.STV IV.ASQU IV.BDI IV.BOB IV.CAFI IV.CRE IV.CRMI IV.CSNT IV.GROG IV.OSSC IV.PARC IV.PLMA IV.QLNO MN.BNI MN.VLC Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 4.79e+21 dyne-cm Mw = 3.72 Z = 7 km Plane Strike Dip Rake NP1 311 55 -87 NP2 125 35 -95 Principal Axes: Axis Value Plunge Azimuth T 4.79e+21 10 39 N 0.00e+00 3 129 P -4.79e+21 80 235 Moment Tensor: (dyne-cm) Component Value Mxx 2.78e+21 Mxy 2.19e+21 Mxz 1.14e+21 Myy 1.70e+21 Myz 1.22e+21 Mzz -4.48e+21 ############## ###################### ######################### #-----#################### T # --------------############## ### #------------------################# #----------------------############### ##------------------------############## ##--------------------------############ ####---------------------------########### ####-------------- -----------########## #####------------- P ------------######### ######------------ -------------######## ######----------------------------###### #######----------------------------##### ########--------------------------#### #########-------------------------## ###########----------------------# ############-----------------# ############################ ###################### ############## Global CMT Convention Moment Tensor: R T P -4.48e+21 1.14e+21 -1.22e+21 1.14e+21 2.78e+21 -2.19e+21 -1.22e+21 -2.19e+21 1.70e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20141130093425/index.html |
STK = 125 DIP = 35 RAKE = -95 MW = 3.72 HS = 7.0
The NDK file is 20141130093425.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution ENS 2014/11/30 09:34:25:0 44.57 9.43 12.0 3.8 Italy Stations used: FR.SAOF FR.TURF GU.FINB GU.MAIM GU.PZZ GU.STV IV.ASQU IV.BDI IV.BOB IV.CAFI IV.CRE IV.CRMI IV.CSNT IV.GROG IV.OSSC IV.PARC IV.PLMA IV.QLNO MN.BNI MN.VLC Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 4.79e+21 dyne-cm Mw = 3.72 Z = 7 km Plane Strike Dip Rake NP1 311 55 -87 NP2 125 35 -95 Principal Axes: Axis Value Plunge Azimuth T 4.79e+21 10 39 N 0.00e+00 3 129 P -4.79e+21 80 235 Moment Tensor: (dyne-cm) Component Value Mxx 2.78e+21 Mxy 2.19e+21 Mxz 1.14e+21 Myy 1.70e+21 Myz 1.22e+21 Mzz -4.48e+21 ############## ###################### ######################### #-----#################### T # --------------############## ### #------------------################# #----------------------############### ##------------------------############## ##--------------------------############ ####---------------------------########### ####-------------- -----------########## #####------------- P ------------######### ######------------ -------------######## ######----------------------------###### #######----------------------------##### ########--------------------------#### #########-------------------------## ###########----------------------# ############-----------------# ############################ ###################### ############## Global CMT Convention Moment Tensor: R T P -4.48e+21 1.14e+21 -1.22e+21 1.14e+21 2.78e+21 -2.19e+21 -1.22e+21 -2.19e+21 1.70e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20141130093425/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 +50 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 1.0 170 55 -30 3.44 0.3885 WVFGRD96 2.0 165 50 -35 3.52 0.4208 WVFGRD96 3.0 165 55 -40 3.54 0.4483 WVFGRD96 4.0 315 60 -75 3.61 0.5026 WVFGRD96 5.0 315 60 -80 3.71 0.5491 WVFGRD96 6.0 125 35 -95 3.73 0.5972 WVFGRD96 7.0 125 35 -95 3.72 0.6063 WVFGRD96 8.0 310 50 -85 3.68 0.5806 WVFGRD96 9.0 310 50 -85 3.68 0.5586 WVFGRD96 10.0 315 50 -80 3.68 0.5319 WVFGRD96 11.0 320 50 -70 3.67 0.5025 WVFGRD96 12.0 315 45 -75 3.67 0.4743 WVFGRD96 13.0 305 40 -85 3.68 0.4479 WVFGRD96 14.0 -10 75 30 3.65 0.4382 WVFGRD96 15.0 145 65 -55 3.70 0.4371 WVFGRD96 16.0 150 70 -50 3.71 0.4314 WVFGRD96 17.0 150 70 -50 3.72 0.4270 WVFGRD96 18.0 150 75 -50 3.73 0.4208 WVFGRD96 19.0 150 75 -50 3.74 0.4165 WVFGRD96 20.0 150 75 -50 3.76 0.4105 WVFGRD96 21.0 150 75 -50 3.77 0.4028 WVFGRD96 22.0 150 75 -50 3.78 0.3973 WVFGRD96 23.0 150 75 -50 3.79 0.3912 WVFGRD96 24.0 155 75 -45 3.79 0.3860 WVFGRD96 25.0 155 75 -45 3.80 0.3824 WVFGRD96 26.0 155 75 -45 3.81 0.3788 WVFGRD96 27.0 155 75 -45 3.82 0.3789 WVFGRD96 28.0 155 75 -45 3.83 0.3794 WVFGRD96 29.0 155 75 -40 3.84 0.3780
The best solution is
WVFGRD96 7.0 125 35 -95 3.72 0.6063
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 +50 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=Sun Nov 30 17:15:36 CST 2014