USGS/SLU Moment Tensor Solution ENS 2022/04/22 21:07:50:0 43.04 18.19 19.2 5.6 Bosnia-Herzegovina Stations used: AC.BCI AC.KBN AC.PHP BS.BLKB CR.ZAG HL.PENT HT.FNA1 HT.FNA5 HT.GRG HT.KPRO HT.LIT HT.NEST HT.THE HU.AMBH HU.BEHE HU.CSKK HU.EGYH HU.KOVH HU.MORH HU.MPLH HU.TIH MN.BLY MN.PDG MN.TIR MN.TRI OE.OBKA OE.SOKA RO.BAIL RO.BZS RO.DEV RO.GZR RO.HERR RO.MDVR RO.PUNG RO.SIRR SJ.BBLS SJ.FRGS SL.BOJS SL.CEY SL.CRES SL.DOBS SL.GBAS SL.GBRS SL.GOLS SL.GROS SL.JAVS SL.KNDS SL.KOGS SL.LJU SL.MOZS SL.PDKS SL.PERS SL.SKDS SL.VISS SL.VNDS SL.VOJS Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 3.16e+24 dyne-cm Mw = 5.60 Z = 24 km Plane Strike Dip Rake NP1 116 65 95 NP2 285 25 80 Principal Axes: Axis Value Plunge Azimuth T 3.16e+24 69 35 N 0.00e+00 4 294 P -3.16e+24 20 203 Moment Tensor: (dyne-cm) Component Value Mxx -2.11e+24 Mxy -7.97e+23 Mxz 1.80e+24 Myy -2.76e+23 Myz 9.99e+23 Mzz 2.39e+24 -------------- ---------------------- ---------#######------------ ----###################------- ---#########################------ --#############################----- ##################################---- #--################### ############--- ----################## T #############-- -------################ ##############-- --------################################-- -----------##############################- -------------############################- ---------------######################### -------------------##################### -----------------------############### ------------------------------------ ---------------------------------- ------- -------------------- ------ P ------------------- --- ---------------- -------------- Global CMT Convention Moment Tensor: R T P 2.39e+24 1.80e+24 -9.99e+23 1.80e+24 -2.11e+24 7.97e+23 -9.99e+23 7.97e+23 -2.76e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20220422210750/index.html |
STK = 285 DIP = 25 RAKE = 80 MW = 5.60 HS = 24.0
The NDK file is 20220422210750.ndk The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2022/04/22 21:07:50:0 43.04 18.19 19.2 5.6 Bosnia-Herzegovina Stations used: AC.BCI AC.KBN AC.PHP BS.BLKB CR.ZAG HL.PENT HT.FNA1 HT.FNA5 HT.GRG HT.KPRO HT.LIT HT.NEST HT.THE HU.AMBH HU.BEHE HU.CSKK HU.EGYH HU.KOVH HU.MORH HU.MPLH HU.TIH MN.BLY MN.PDG MN.TIR MN.TRI OE.OBKA OE.SOKA RO.BAIL RO.BZS RO.DEV RO.GZR RO.HERR RO.MDVR RO.PUNG RO.SIRR SJ.BBLS SJ.FRGS SL.BOJS SL.CEY SL.CRES SL.DOBS SL.GBAS SL.GBRS SL.GOLS SL.GROS SL.JAVS SL.KNDS SL.KOGS SL.LJU SL.MOZS SL.PDKS SL.PERS SL.SKDS SL.VISS SL.VNDS SL.VOJS Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 3.16e+24 dyne-cm Mw = 5.60 Z = 24 km Plane Strike Dip Rake NP1 116 65 95 NP2 285 25 80 Principal Axes: Axis Value Plunge Azimuth T 3.16e+24 69 35 N 0.00e+00 4 294 P -3.16e+24 20 203 Moment Tensor: (dyne-cm) Component Value Mxx -2.11e+24 Mxy -7.97e+23 Mxz 1.80e+24 Myy -2.76e+23 Myz 9.99e+23 Mzz 2.39e+24 -------------- ---------------------- ---------#######------------ ----###################------- ---#########################------ --#############################----- ##################################---- #--################### ############--- ----################## T #############-- -------################ ##############-- --------################################-- -----------##############################- -------------############################- ---------------######################### -------------------##################### -----------------------############### ------------------------------------ ---------------------------------- ------- -------------------- ------ P ------------------- --- ---------------- -------------- Global CMT Convention Moment Tensor: R T P 2.39e+24 1.80e+24 -9.99e+23 1.80e+24 -2.11e+24 7.97e+23 -9.99e+23 7.97e+23 -2.76e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20220422210750/index.html |
W-phase Moment Tensor (Mww) Moment 4.649e+17 N-m Magnitude 5.71 Mww Depth 17.5 km Percent DC 69% Half Duration 1.86 s Catalog US Data Source US 1 Contributor US 1 Nodal Planes Plane Strike Dip Rake NP1 298° 18° 94° NP2 114° 73° 89° Principal Axes Axis Value Plunge Azimuth T 4.215e+17 N-m 62° 22° N 0.771e+17 N-m 1° 114° P -4.986e+17 N-m 27° 205° |
EMSC-CSEM |
(a) ML computed using the IASPEI formula for Horizontal components; (b) ML residuals computed using a modified IASPEI formula that accounts for path specific attenuation; the values used for the trimmed mean are indicated. The ML relation used for each figure is given at the bottom of each plot.
(a) ML computed using the IASPEI formula for Vertical components (research); (b) ML residuals computed using a modified IASPEI formula that accounts for path specific attenuation; the values used for the trimmed mean are indicated. The ML relation used for each figure is given at the bottom of each plot.
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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 o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.07 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 1.0 110 45 -90 5.20 0.3048 WVFGRD96 2.0 110 45 -90 5.29 0.3696 WVFGRD96 3.0 120 50 -90 5.36 0.3261 WVFGRD96 4.0 85 80 -25 5.29 0.2944 WVFGRD96 5.0 85 85 -30 5.31 0.2911 WVFGRD96 6.0 265 90 35 5.32 0.2948 WVFGRD96 7.0 175 20 -20 5.33 0.3214 WVFGRD96 8.0 155 15 -40 5.41 0.3476 WVFGRD96 9.0 105 80 85 5.42 0.3806 WVFGRD96 10.0 300 15 100 5.44 0.4171 WVFGRD96 11.0 110 70 85 5.46 0.4525 WVFGRD96 12.0 295 20 95 5.47 0.4871 WVFGRD96 13.0 290 20 90 5.48 0.5169 WVFGRD96 14.0 110 65 90 5.50 0.5435 WVFGRD96 15.0 290 25 90 5.51 0.5680 WVFGRD96 16.0 290 25 90 5.52 0.5887 WVFGRD96 17.0 115 65 95 5.53 0.6059 WVFGRD96 18.0 115 65 95 5.54 0.6202 WVFGRD96 19.0 115 65 95 5.55 0.6315 WVFGRD96 20.0 115 65 95 5.56 0.6406 WVFGRD96 21.0 115 65 95 5.58 0.6472 WVFGRD96 22.0 285 25 80 5.59 0.6512 WVFGRD96 23.0 285 25 80 5.59 0.6534 WVFGRD96 24.0 285 25 80 5.60 0.6537 WVFGRD96 25.0 285 25 80 5.61 0.6528 WVFGRD96 26.0 285 25 80 5.62 0.6503 WVFGRD96 27.0 285 25 80 5.62 0.6461 WVFGRD96 28.0 285 25 80 5.63 0.6407 WVFGRD96 29.0 280 30 70 5.64 0.6338
The best solution is
WVFGRD96 24.0 285 25 80 5.60 0.6537
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 +70 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.07 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.
Thanks also to the many seismic network operators whose dedication make this effort possible: University of Nevada Reno, University of Alaska, University of Washington, Oregon State University, University of Utah, Montana Bureas of Mines, UC Berkely, Caltech, UC San Diego, Saint Louis University, University of Memphis, Lamont Doherty Earth Observatory, the Iris stations and the Transportable Array of EarthScope.
The WUS.model 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: