2016/11/01 18:47:50 42.7288 13.2203 10.0 3.4 Rieti
USGS Felt map for this earthquake
SLU Moment Tensor Solution ENS 2016/11/01 18:47:50:8 42.73 13.22 10.0 3.4 Rieti Stations used: IV.AOI IV.ARCI IV.ARVD IV.CAFI IV.CERT IV.CESX IV.CING IV.FDMO IV.FIAM IV.GUAR IV.GUMA IV.LATE IV.LAV9 IV.MA9 IV.MGAB IV.MTCE IV.OFFI IV.PIEI IV.PTQR IV.RMP IV.SACS IV.SAMA IV.SNTG IV.TERO IV.TOLF Filtering commands used: cut o DIST/3.3 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 1.20e+21 dyne-cm Mw = 3.32 Z = 6 km Plane Strike Dip Rake NP1 317 73 -108 NP2 185 25 -45 Principal Axes: Axis Value Plunge Azimuth T 1.20e+21 25 61 N 0.00e+00 17 323 P -1.20e+21 58 202 Moment Tensor: (dyne-cm) Component Value Mxx -5.74e+19 Mxy 2.97e+20 Mxz 7.20e+20 Myy 7.09e+20 Myz 6.12e+20 Mzz -6.51e+20 ----########## -----################# -----####################### ####-######################### #####-----######################## #####--------################# ### #####------------############## T #### #####---------------############ ##### #####-----------------################## #####-------------------################## #####---------------------################ #####-----------------------############## #####------------------------############# #####------------------------########### #####---------- ------------########## #####--------- P --------------####### ####--------- --------------###### ####--------------------------#### ####-------------------------# ####------------------------ ###------------------- ##------------ Global CMT Convention Moment Tensor: R T P -6.51e+20 7.20e+20 -6.12e+20 7.20e+20 -5.74e+19 -2.97e+20 -6.12e+20 -2.97e+20 7.09e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161101184750/index.html |
STK = 185 DIP = 25 RAKE = -45 MW = 3.32 HS = 6.0
The NDK file is 20161101184750.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution ENS 2016/11/01 18:47:50:8 42.73 13.22 10.0 3.4 Rieti Stations used: IV.AOI IV.ARCI IV.ARVD IV.CAFI IV.CERT IV.CESX IV.CING IV.FDMO IV.FIAM IV.GUAR IV.GUMA IV.LATE IV.LAV9 IV.MA9 IV.MGAB IV.MTCE IV.OFFI IV.PIEI IV.PTQR IV.RMP IV.SACS IV.SAMA IV.SNTG IV.TERO IV.TOLF Filtering commands used: cut o DIST/3.3 -20 o DIST/3.3 +40 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3 Best Fitting Double Couple Mo = 1.20e+21 dyne-cm Mw = 3.32 Z = 6 km Plane Strike Dip Rake NP1 317 73 -108 NP2 185 25 -45 Principal Axes: Axis Value Plunge Azimuth T 1.20e+21 25 61 N 0.00e+00 17 323 P -1.20e+21 58 202 Moment Tensor: (dyne-cm) Component Value Mxx -5.74e+19 Mxy 2.97e+20 Mxz 7.20e+20 Myy 7.09e+20 Myz 6.12e+20 Mzz -6.51e+20 ----########## -----################# -----####################### ####-######################### #####-----######################## #####--------################# ### #####------------############## T #### #####---------------############ ##### #####-----------------################## #####-------------------################## #####---------------------################ #####-----------------------############## #####------------------------############# #####------------------------########### #####---------- ------------########## #####--------- P --------------####### ####--------- --------------###### ####--------------------------#### ####-------------------------# ####------------------------ ###------------------- ##------------ Global CMT Convention Moment Tensor: R T P -6.51e+20 7.20e+20 -6.12e+20 7.20e+20 -5.74e+19 -2.97e+20 -6.12e+20 -2.97e+20 7.09e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161101184750/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 0.03 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 1.0 310 35 -95 3.16 0.5144 WVFGRD96 2.0 140 70 -85 3.26 0.4901 WVFGRD96 3.0 180 20 -45 3.24 0.5350 WVFGRD96 4.0 180 25 -50 3.23 0.5710 WVFGRD96 5.0 180 20 -50 3.33 0.6027 WVFGRD96 6.0 185 25 -45 3.32 0.6069 WVFGRD96 7.0 195 30 -30 3.31 0.5991 WVFGRD96 8.0 215 45 20 3.28 0.5867 WVFGRD96 9.0 220 40 5 3.29 0.5791 WVFGRD96 10.0 220 40 5 3.30 0.5668 WVFGRD96 11.0 220 45 10 3.32 0.5516 WVFGRD96 12.0 220 45 10 3.32 0.5338 WVFGRD96 13.0 220 45 10 3.33 0.5142 WVFGRD96 14.0 220 45 5 3.34 0.4954 WVFGRD96 15.0 130 70 85 3.35 0.4772 WVFGRD96 16.0 130 70 85 3.36 0.4657 WVFGRD96 17.0 130 70 85 3.37 0.4537 WVFGRD96 18.0 125 70 75 3.37 0.4429 WVFGRD96 19.0 125 70 75 3.38 0.4319
The best solution is
WVFGRD96 6.0 185 25 -45 3.32 0.6069
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 0.03 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=Fri Nov 18 09:44:36 CST 2016