2014/01/23 06:15:05 45.42 26.26 127.0 4.7 Romania
USGS Felt map for this earthquake
USGS/SLU Moment Tensor Solution ENS 2014/01/23 06:15:05:0 45.42 26.26 127.0 4.7 Romania Stations used: GE.TIRR RO.ARR RO.CFR RO.ISR RO.MLR RO.PLOR1 RO.TESR RO.VOIR RO.VRI Filtering commands used: cut a -30 a 60 rtr taper w 0.1 hp c 0.05 n 3 lp c 0.25 n 3 Best Fitting Double Couple Mo = 4.52e+22 dyne-cm Mw = 4.37 Z = 118 km Plane Strike Dip Rake NP1 277 56 113 NP2 60 40 60 Principal Axes: Axis Value Plunge Azimuth T 4.52e+22 69 238 N 0.00e+00 19 84 P -4.52e+22 9 351 Moment Tensor: (dyne-cm) Component Value Mxx -4.15e+22 Mxy 9.43e+21 Mxz -1.45e+22 Myy 2.94e+21 Myz -1.16e+22 Mzz 3.85e+22 --- P -------- ------- ------------ ---------------------------- ------------------------------ ---------------------------------- ------------------------------------ ----------###########----------------# -----########################---------## --###############################-----## -####################################-#### ######################################-### ############### ###################----# ############### T ##################------ ############## ################------- ################################-------- #############################--------- #########################----------- --###################------------- -----#######------------------ ---------------------------- ---------------------- -------------- Global CMT Convention Moment Tensor: R T P 3.85e+22 -1.45e+22 1.16e+22 -1.45e+22 -4.15e+22 -9.43e+21 1.16e+22 -9.43e+21 2.94e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.EU/20140123061505/index.html |
STK = 60 DIP = 40 RAKE = 60 MW = 4.37 HS = 118.0
The NDK file is 20140123061505.ndk The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2014/01/23 06:15:05:0 45.42 26.26 127.0 4.7 Romania Stations used: GE.TIRR RO.ARR RO.CFR RO.ISR RO.MLR RO.PLOR1 RO.TESR RO.VOIR RO.VRI Filtering commands used: cut a -30 a 60 rtr taper w 0.1 hp c 0.05 n 3 lp c 0.25 n 3 Best Fitting Double Couple Mo = 4.52e+22 dyne-cm Mw = 4.37 Z = 118 km Plane Strike Dip Rake NP1 277 56 113 NP2 60 40 60 Principal Axes: Axis Value Plunge Azimuth T 4.52e+22 69 238 N 0.00e+00 19 84 P -4.52e+22 9 351 Moment Tensor: (dyne-cm) Component Value Mxx -4.15e+22 Mxy 9.43e+21 Mxz -1.45e+22 Myy 2.94e+21 Myz -1.16e+22 Mzz 3.85e+22 --- P -------- ------- ------------ ---------------------------- ------------------------------ ---------------------------------- ------------------------------------ ----------###########----------------# -----########################---------## --###############################-----## -####################################-#### ######################################-### ############### ###################----# ############### T ##################------ ############## ################------- ################################-------- #############################--------- #########################----------- --###################------------- -----#######------------------ ---------------------------- ---------------------- -------------- Global CMT Convention Moment Tensor: R T P 3.85e+22 -1.45e+22 1.16e+22 -1.45e+22 -4.15e+22 -9.43e+21 1.16e+22 -9.43e+21 2.94e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.EU/20140123061505/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 a -30 a 60 rtr taper w 0.1 hp c 0.05 n 3 lp c 0.25 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 2.0 230 80 35 3.22 0.1016 WVFGRD96 4.0 80 60 80 3.41 0.1403 WVFGRD96 6.0 80 60 85 3.50 0.1571 WVFGRD96 8.0 300 40 -35 3.65 0.1475 WVFGRD96 10.0 75 30 -95 3.74 0.1563 WVFGRD96 12.0 270 45 -75 3.82 0.2010 WVFGRD96 14.0 270 45 -70 3.86 0.2241 WVFGRD96 16.0 270 50 -65 3.88 0.2260 WVFGRD96 18.0 270 50 -65 3.89 0.2245 WVFGRD96 20.0 270 55 -65 3.91 0.2319 WVFGRD96 22.0 270 50 -65 3.91 0.2310 WVFGRD96 24.0 50 25 45 3.94 0.2188 WVFGRD96 26.0 55 25 50 3.95 0.2330 WVFGRD96 28.0 55 50 50 3.96 0.2660 WVFGRD96 30.0 55 45 55 3.96 0.2858 WVFGRD96 32.0 55 50 50 3.96 0.2800 WVFGRD96 34.0 60 45 60 3.97 0.2706 WVFGRD96 36.0 65 45 65 3.99 0.2883 WVFGRD96 38.0 75 30 75 3.99 0.2941 WVFGRD96 40.0 75 30 75 4.10 0.3068 WVFGRD96 42.0 75 30 75 4.13 0.3006 WVFGRD96 44.0 70 30 75 4.15 0.2992 WVFGRD96 46.0 65 30 70 4.17 0.3055 WVFGRD96 48.0 60 30 65 4.18 0.3165 WVFGRD96 50.0 55 55 55 4.16 0.3261 WVFGRD96 52.0 55 55 55 4.17 0.3318 WVFGRD96 54.0 55 55 55 4.18 0.3358 WVFGRD96 56.0 55 55 55 4.19 0.3383 WVFGRD96 58.0 55 55 55 4.20 0.3466 WVFGRD96 60.0 55 40 55 4.21 0.3524 WVFGRD96 62.0 55 40 55 4.21 0.3576 WVFGRD96 64.0 55 40 55 4.22 0.3576 WVFGRD96 66.0 55 40 55 4.23 0.3655 WVFGRD96 68.0 55 40 55 4.23 0.3646 WVFGRD96 70.0 55 40 55 4.24 0.3674 WVFGRD96 72.0 55 40 55 4.25 0.3673 WVFGRD96 74.0 55 45 55 4.26 0.3670 WVFGRD96 76.0 55 40 60 4.26 0.3689 WVFGRD96 78.0 50 40 55 4.26 0.3572 WVFGRD96 80.0 55 45 55 4.27 0.3600 WVFGRD96 82.0 35 40 40 4.27 0.3598 WVFGRD96 84.0 35 40 40 4.28 0.3653 WVFGRD96 86.0 35 40 40 4.28 0.3640 WVFGRD96 88.0 35 40 40 4.29 0.3710 WVFGRD96 90.0 35 45 40 4.28 0.3676 WVFGRD96 92.0 35 45 40 4.29 0.3708 WVFGRD96 94.0 35 45 40 4.29 0.3673 WVFGRD96 96.0 50 35 50 4.30 0.3698 WVFGRD96 98.0 50 35 50 4.30 0.3721 WVFGRD96 100.0 50 35 50 4.31 0.3738 WVFGRD96 102.0 55 40 50 4.33 0.3777 WVFGRD96 104.0 55 40 50 4.33 0.3784 WVFGRD96 106.0 55 40 50 4.34 0.3852 WVFGRD96 108.0 60 40 55 4.35 0.3903 WVFGRD96 110.0 60 40 55 4.35 0.3935 WVFGRD96 112.0 60 40 55 4.36 0.3974 WVFGRD96 114.0 60 40 55 4.36 0.3985 WVFGRD96 116.0 60 40 55 4.37 0.4035 WVFGRD96 118.0 60 40 60 4.37 0.4042 WVFGRD96 120.0 60 40 60 4.38 0.4020 WVFGRD96 122.0 60 40 60 4.38 0.4035 WVFGRD96 124.0 60 40 60 4.38 0.4006 WVFGRD96 126.0 55 40 55 4.37 0.3976 WVFGRD96 128.0 55 40 55 4.38 0.3962 WVFGRD96 130.0 55 40 55 4.38 0.3943 WVFGRD96 132.0 55 40 55 4.38 0.3939 WVFGRD96 134.0 50 40 50 4.38 0.3910 WVFGRD96 136.0 50 40 50 4.38 0.3866 WVFGRD96 138.0 45 40 50 4.37 0.3853
The best solution is
WVFGRD96 118.0 60 40 60 4.37 0.4042
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 -30 a 60 rtr taper w 0.1 hp c 0.05 n 3 lp c 0.25 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.
Should the national backbone of the USGS Advanced National Seismic System (ANSS) be implemented with an interstation separation of 300 km, it is very likely that an earthquake such as this would have been recorded at distances on the order of 100-200 km. This means that the closest station would have information on source depth and mechanism that was lacking here.
Dr. Harley Benz, USGS, provided the USGS USNSN digital data. The digital data used in this study were provided by Natural Resources Canada through their AUTODRM site http://www.seismo.nrcan.gc.ca/nwfa/autodrm/autodrm_req_e.php, and IRIS using their BUD interface.
Thanks also to the many seismic network operators whose dedication make this effort possible: University of Alaska, University of Washington, Oregon State University, University of Utah, Montana Bureas of Mines, UC Berkely, Caltech, UC San Diego, Saint L ouis University, Universityof Memphis, Lamont Doehrty Earth Observatory, Boston College, the Iris stations and the Transportable Array of EarthScope.
The WUS used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows:
MODEL.01 Model after 8 iterations 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 1.9000 3.4065 2.0089 2.2150 0.302E-02 0.679E-02 0.00 0.00 1.00 1.00 6.1000 5.5445 3.2953 2.6089 0.349E-02 0.784E-02 0.00 0.00 1.00 1.00 13.0000 6.2708 3.7396 2.7812 0.212E-02 0.476E-02 0.00 0.00 1.00 1.00 19.0000 6.4075 3.7680 2.8223 0.111E-02 0.249E-02 0.00 0.00 1.00 1.00 0.0000 7.9000 4.6200 3.2760 0.164E-10 0.370E-10 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 09:19:34 CST 2014