2016/09/15 13:51:29 42.7792 13.1278 10.2 3.1 Perugia
USGS Felt map for this earthquake
SLU Moment Tensor Solution ENS 2016/09/15 13:51:29:9 42.78 13.13 10.2 3.1 Perugia Stations used: IV.ARVD IV.ATTE IV.CERT IV.CESX IV.CING IV.FDMO IV.FIAM IV.GUAR IV.GUMA IV.LNSS IV.MGAB IV.MTCE IV.MURB IV.OFFI IV.SACS IV.SNTG IV.TERO MN.AQU Filtering commands used: cut o DIST/3.3 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.04 n 3 lp c 0.15 n 3 Best Fitting Double Couple Mo = 2.92e+20 dyne-cm Mw = 2.91 Z = 2 km Plane Strike Dip Rake NP1 330 60 -85 NP2 140 30 -99 Principal Axes: Axis Value Plunge Azimuth T 2.92e+20 15 56 N 0.00e+00 4 147 P -2.92e+20 74 253 Moment Tensor: (dyne-cm) Component Value Mxx 8.20e+19 Mxy 1.20e+20 Mxz 6.16e+19 Myy 1.70e+20 Myz 1.32e+20 Mzz -2.52e+20 ############## --#################### #--------################### -------------################# ##---------------############# # ##------------------########### T ## ###--------------------######### ### ###----------------------############### ###-----------------------############## #####-----------------------############## #####----------- ----------############# #####----------- P -----------############ ######---------- ------------########### ######------------------------########## #######------------------------######### #######-----------------------######## ########---------------------####### ########--------------------###### #########-----------------#### ###########--------------### ###################### ############## Global CMT Convention Moment Tensor: R T P -2.52e+20 6.16e+19 -1.32e+20 6.16e+19 8.20e+19 -1.20e+20 -1.32e+20 -1.20e+20 1.70e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20160915135129/index.html |
STK = 330 DIP = 60 RAKE = -85 MW = 2.91 HS = 2.0
The NDK file is 20160915135129.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution ENS 2016/09/15 13:51:29:9 42.78 13.13 10.2 3.1 Perugia Stations used: IV.ARVD IV.ATTE IV.CERT IV.CESX IV.CING IV.FDMO IV.FIAM IV.GUAR IV.GUMA IV.LNSS IV.MGAB IV.MTCE IV.MURB IV.OFFI IV.SACS IV.SNTG IV.TERO MN.AQU Filtering commands used: cut o DIST/3.3 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.04 n 3 lp c 0.15 n 3 Best Fitting Double Couple Mo = 2.92e+20 dyne-cm Mw = 2.91 Z = 2 km Plane Strike Dip Rake NP1 330 60 -85 NP2 140 30 -99 Principal Axes: Axis Value Plunge Azimuth T 2.92e+20 15 56 N 0.00e+00 4 147 P -2.92e+20 74 253 Moment Tensor: (dyne-cm) Component Value Mxx 8.20e+19 Mxy 1.20e+20 Mxz 6.16e+19 Myy 1.70e+20 Myz 1.32e+20 Mzz -2.52e+20 ############## --#################### #--------################### -------------################# ##---------------############# # ##------------------########### T ## ###--------------------######### ### ###----------------------############### ###-----------------------############## #####-----------------------############## #####----------- ----------############# #####----------- P -----------############ ######---------- ------------########### ######------------------------########## #######------------------------######### #######-----------------------######## ########---------------------####### ########--------------------###### #########-----------------#### ###########--------------### ###################### ############## Global CMT Convention Moment Tensor: R T P -2.52e+20 6.16e+19 -1.32e+20 6.16e+19 8.20e+19 -1.20e+20 -1.32e+20 -1.20e+20 1.70e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20160915135129/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 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.04 n 3 lp c 0.15 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 1.0 145 25 -90 2.84 0.3907 WVFGRD96 2.0 330 60 -85 2.91 0.4169 WVFGRD96 3.0 330 60 -80 2.91 0.3886 WVFGRD96 4.0 15 65 55 2.90 0.3833 WVFGRD96 5.0 10 70 60 2.99 0.3637 WVFGRD96 6.0 20 60 45 2.99 0.3534 WVFGRD96 7.0 15 65 45 3.00 0.3348 WVFGRD96 8.0 15 65 40 2.99 0.3221 WVFGRD96 9.0 15 65 40 3.01 0.3008 WVFGRD96 10.0 15 70 40 3.02 0.2789 WVFGRD96 11.0 35 45 -5 3.04 0.2599 WVFGRD96 12.0 30 45 -15 3.05 0.2438 WVFGRD96 13.0 30 45 -15 3.06 0.2286 WVFGRD96 14.0 30 45 -15 3.06 0.2151 WVFGRD96 15.0 315 45 80 3.11 0.2145 WVFGRD96 16.0 320 45 85 3.13 0.2184 WVFGRD96 17.0 315 45 80 3.14 0.2222 WVFGRD96 18.0 300 45 55 3.14 0.2270 WVFGRD96 19.0 300 45 55 3.15 0.2325 WVFGRD96 20.0 295 45 45 3.15 0.2360 WVFGRD96 21.0 295 45 45 3.15 0.2359 WVFGRD96 22.0 295 50 45 3.16 0.2453 WVFGRD96 23.0 295 55 45 3.17 0.2532 WVFGRD96 24.0 295 55 50 3.18 0.2610 WVFGRD96 25.0 295 55 50 3.19 0.2678 WVFGRD96 26.0 295 55 45 3.19 0.2734 WVFGRD96 27.0 295 55 45 3.20 0.2775 WVFGRD96 28.0 290 65 40 3.21 0.2823 WVFGRD96 29.0 290 65 40 3.23 0.2850
The best solution is
WVFGRD96 2.0 330 60 -85 2.91 0.4169
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 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.04 n 3 lp c 0.15 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 Oct 28 09:34:54 CDT 2016