2014/01/22 19:35:01 40.441 15.119 6.3 3.70 Italy
USGS Felt map for this earthquake
SLU Moment Tensor Solution ENS 2014/01/22 19:35:01:0 40.44 15.12 6.3 3.7 Italy Stations used: IV.ACER IV.BSSO IV.CDRU IV.MCEL IV.MCRV IV.MESG IV.MGR IV.MODR IV.MRLC IV.MRVN IV.MSAG IV.MTSN IV.NOCI IV.PALZ IV.PTQR IV.SGRT IV.SIRI IV.SLCN IV.VAGA MN.TIP Filtering commands used: cut a -10 a 90 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.05 n 3 Best Fitting Double Couple Mo = 3.51e+21 dyne-cm Mw = 3.63 Z = 5 km Plane Strike Dip Rake NP1 307 67 99 NP2 105 25 70 Principal Axes: Axis Value Plunge Azimuth T 3.51e+21 67 234 N 0.00e+00 8 123 P -3.51e+21 21 30 Moment Tensor: (dyne-cm) Component Value Mxx -2.10e+21 Mxy -1.07e+21 Mxz -1.77e+21 Myy -4.23e+20 Myz -1.60e+21 Mzz 2.52e+21 -------------- ---------------------- --------------------- ---- ---------------------- P ----- ######------------------ ------- ############------------------------ #################--------------------- #####################------------------- ########################---------------- -##########################--------------- -############################------------- --############# #############----------- --############# T ###############--------- --############ ################------- ---###############################-----# ----##############################---# -----############################### ------#########################--- -------###################---- ------------#######--------- ---------------------- -------------- Global CMT Convention Moment Tensor: R T P 2.52e+21 -1.77e+21 1.60e+21 -1.77e+21 -2.10e+21 1.07e+21 1.60e+21 1.07e+21 -4.23e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20140122193501/index.html |
STK = 105 DIP = 25 RAKE = 70 MW = 3.63 HS = 5.0
The NDK file is 20140122193501.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution ENS 2014/01/22 19:35:01:0 40.44 15.12 6.3 3.7 Italy Stations used: IV.ACER IV.BSSO IV.CDRU IV.MCEL IV.MCRV IV.MESG IV.MGR IV.MODR IV.MRLC IV.MRVN IV.MSAG IV.MTSN IV.NOCI IV.PALZ IV.PTQR IV.SGRT IV.SIRI IV.SLCN IV.VAGA MN.TIP Filtering commands used: cut a -10 a 90 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.05 n 3 Best Fitting Double Couple Mo = 3.51e+21 dyne-cm Mw = 3.63 Z = 5 km Plane Strike Dip Rake NP1 307 67 99 NP2 105 25 70 Principal Axes: Axis Value Plunge Azimuth T 3.51e+21 67 234 N 0.00e+00 8 123 P -3.51e+21 21 30 Moment Tensor: (dyne-cm) Component Value Mxx -2.10e+21 Mxy -1.07e+21 Mxz -1.77e+21 Myy -4.23e+20 Myz -1.60e+21 Mzz 2.52e+21 -------------- ---------------------- --------------------- ---- ---------------------- P ----- ######------------------ ------- ############------------------------ #################--------------------- #####################------------------- ########################---------------- -##########################--------------- -############################------------- --############# #############----------- --############# T ###############--------- --############ ################------- ---###############################-----# ----##############################---# -----############################### ------#########################--- -------###################---- ------------#######--------- ---------------------- -------------- Global CMT Convention Moment Tensor: R T P 2.52e+21 -1.77e+21 1.60e+21 -1.77e+21 -2.10e+21 1.07e+21 1.60e+21 1.07e+21 -4.23e+20 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20140122193501/index.html |
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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 a -10 a 90 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.05 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 95 35 50 3.45 0.3656 WVFGRD96 2.0 95 25 40 3.56 0.3872 WVFGRD96 3.0 100 25 55 3.56 0.4059 WVFGRD96 4.0 105 30 70 3.57 0.4087 WVFGRD96 5.0 105 25 70 3.63 0.4096 WVFGRD96 6.0 110 25 80 3.62 0.3928 WVFGRD96 7.0 115 25 85 3.61 0.3740 WVFGRD96 8.0 105 30 80 3.56 0.3525 WVFGRD96 9.0 105 30 80 3.55 0.3455 WVFGRD96 10.0 110 30 85 3.54 0.3377 WVFGRD96 11.0 105 30 85 3.53 0.3313 WVFGRD96 12.0 115 30 95 3.53 0.3250 WVFGRD96 13.0 115 30 95 3.52 0.3177 WVFGRD96 14.0 290 60 85 3.52 0.3082 WVFGRD96 15.0 130 25 -65 3.55 0.3080 WVFGRD96 16.0 130 25 -65 3.55 0.3066 WVFGRD96 17.0 130 25 -65 3.55 0.3040 WVFGRD96 18.0 130 25 -65 3.55 0.3007 WVFGRD96 19.0 140 30 -55 3.56 0.2979 WVFGRD96 20.0 140 30 -55 3.56 0.2941 WVFGRD96 21.0 135 30 -55 3.56 0.2904 WVFGRD96 22.0 140 35 -50 3.57 0.2874 WVFGRD96 23.0 140 35 -50 3.58 0.2842 WVFGRD96 24.0 140 35 -50 3.58 0.2803 WVFGRD96 25.0 140 40 -50 3.59 0.2770 WVFGRD96 26.0 140 40 -50 3.60 0.2729 WVFGRD96 27.0 135 40 -55 3.60 0.2677 WVFGRD96 28.0 135 40 -55 3.61 0.2618 WVFGRD96 29.0 135 40 -60 3.62 0.2543
The best solution is
WVFGRD96 5.0 105 25 70 3.63 0.4096
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 a -10 a 90 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.05 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=Thu Jan 23 06:26:22 CST 2014