USGS/SLU Moment Tensor Solution ENS 2021/01/06 17:01:43:1 45.44 16.26 10.0 5.0 Croatia Stations used: AC.BCI BW.ALFT BW.BGDS BW.BIB BW.FFB1 BW.GELB BW.GRMB BW.KW1 BW.MGS02 BW.MGS03 BW.MGS05 BW.PART BW.RNHA BW.RNON BW.ROTZ BW.SCE BW.ZUGS CH.BERNI CH.DAVOX CH.FUORN CH.LIENZ CH.LLS CH.PLONS CH.ROMAN CH.SGT05 CH.VDR CR.ZAG GE.MATE GR.FUR GR.GEC7 GR.GRA4 GR.GRB4 GR.GRC1 GR.GRC2 GR.GRC3 GR.GRC4 GR.UBR GR.WET HU.AMBH HU.BEHE HU.BSZH HU.BUD HU.CSKK HU.EGYH HU.KOVH HU.MORH HU.PSZ HU.SOP HU.TIH MN.BLY MN.PDG MN.TRI MN.TUE OE.ABTA OE.ARSA OE.BIOA OE.CONA OE.CSNA OE.DAVA OE.FETA OE.KBA OE.LESA OE.MOA OE.MOTA OE.MYKA OE.OBKA OE.RETA OE.RONA OE.SOKA OE.SQTA OE.VIE OE.WATA OX.ACOM OX.AGOR OX.BAD OX.BOO OX.CAE OX.CIMO OX.CLUD OX.DRE OX.MLN OX.MPRI OX.SABO RO.BZS RO.PUNG SL.BOJS SL.CADS SL.CEY SL.CRES SL.CRNS SL.DOBS SL.GBAS SL.GBRS SL.GCIS SL.GOLS SL.GORS SL.GROS SL.JAVS SL.KNDS SL.LJU SL.MOZS SL.PDKS SL.PERS SL.ROBS SL.SKDS SL.VISS SL.VNDS SL.ZAVS Filtering commands used: cut o DIST/3.3 -40 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.06 n 3 Best Fitting Double Couple Mo = 1.62e+23 dyne-cm Mw = 4.74 Z = 13 km Plane Strike Dip Rake NP1 50 90 10 NP2 320 80 180 Principal Axes: Axis Value Plunge Azimuth T 1.62e+23 7 275 N 0.00e+00 80 50 P -1.62e+23 7 185 Moment Tensor: (dyne-cm) Component Value Mxx -1.57e+23 Mxy -2.77e+22 Mxz 2.16e+22 Myy 1.57e+23 Myz -1.81e+22 Mzz -2.46e+15 -------------- ---------------------- #--------------------------- #####------------------------- #########----------------------### ############------------------###### ###############--------------######### ##################----------############ ###################-------############## ###################--################## T ###################--################## #################-----################# ##################--------################ ##############-------------############# ############----------------############ #########-------------------########## ######-----------------------####### ###--------------------------##### ---------------------------### ---------------------------# -------- ----------- ---- P ------- Global CMT Convention Moment Tensor: R T P -2.46e+15 2.16e+22 1.81e+22 2.16e+22 -1.57e+23 2.77e+22 1.81e+22 2.77e+22 1.57e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20210106170143/index.html |
STK = 50 DIP = 90 RAKE = 10 MW = 4.74 HS = 13.0
The NDK file is 20210106170143.ndk The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2021/01/06 17:01:43:1 45.44 16.26 10.0 5.0 Croatia Stations used: AC.BCI BW.ALFT BW.BGDS BW.BIB BW.FFB1 BW.GELB BW.GRMB BW.KW1 BW.MGS02 BW.MGS03 BW.MGS05 BW.PART BW.RNHA BW.RNON BW.ROTZ BW.SCE BW.ZUGS CH.BERNI CH.DAVOX CH.FUORN CH.LIENZ CH.LLS CH.PLONS CH.ROMAN CH.SGT05 CH.VDR CR.ZAG GE.MATE GR.FUR GR.GEC7 GR.GRA4 GR.GRB4 GR.GRC1 GR.GRC2 GR.GRC3 GR.GRC4 GR.UBR GR.WET HU.AMBH HU.BEHE HU.BSZH HU.BUD HU.CSKK HU.EGYH HU.KOVH HU.MORH HU.PSZ HU.SOP HU.TIH MN.BLY MN.PDG MN.TRI MN.TUE OE.ABTA OE.ARSA OE.BIOA OE.CONA OE.CSNA OE.DAVA OE.FETA OE.KBA OE.LESA OE.MOA OE.MOTA OE.MYKA OE.OBKA OE.RETA OE.RONA OE.SOKA OE.SQTA OE.VIE OE.WATA OX.ACOM OX.AGOR OX.BAD OX.BOO OX.CAE OX.CIMO OX.CLUD OX.DRE OX.MLN OX.MPRI OX.SABO RO.BZS RO.PUNG SL.BOJS SL.CADS SL.CEY SL.CRES SL.CRNS SL.DOBS SL.GBAS SL.GBRS SL.GCIS SL.GOLS SL.GORS SL.GROS SL.JAVS SL.KNDS SL.LJU SL.MOZS SL.PDKS SL.PERS SL.ROBS SL.SKDS SL.VISS SL.VNDS SL.ZAVS Filtering commands used: cut o DIST/3.3 -40 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.06 n 3 Best Fitting Double Couple Mo = 1.62e+23 dyne-cm Mw = 4.74 Z = 13 km Plane Strike Dip Rake NP1 50 90 10 NP2 320 80 180 Principal Axes: Axis Value Plunge Azimuth T 1.62e+23 7 275 N 0.00e+00 80 50 P -1.62e+23 7 185 Moment Tensor: (dyne-cm) Component Value Mxx -1.57e+23 Mxy -2.77e+22 Mxz 2.16e+22 Myy 1.57e+23 Myz -1.81e+22 Mzz -2.46e+15 -------------- ---------------------- #--------------------------- #####------------------------- #########----------------------### ############------------------###### ###############--------------######### ##################----------############ ###################-------############## ###################--################## T ###################--################## #################-----################# ##################--------################ ##############-------------############# ############----------------############ #########-------------------########## ######-----------------------####### ###--------------------------##### ---------------------------### ---------------------------# -------- ----------- ---- P ------- Global CMT Convention Moment Tensor: R T P -2.46e+15 2.16e+22 1.81e+22 2.16e+22 -1.57e+23 2.77e+22 1.81e+22 2.77e+22 1.57e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20210106170143/index.html |
https://www.croatiaweek.com/magnitude-5-0-earthquake-hits-central-croatia/ |
(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 -40 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.06 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 50 85 10 4.35 0.3478 WVFGRD96 2.0 55 75 25 4.49 0.4552 WVFGRD96 3.0 55 75 20 4.53 0.5026 WVFGRD96 4.0 50 90 20 4.55 0.5423 WVFGRD96 5.0 230 90 -20 4.58 0.5769 WVFGRD96 6.0 50 90 15 4.60 0.6089 WVFGRD96 7.0 230 85 -15 4.63 0.6373 WVFGRD96 8.0 230 85 -15 4.66 0.6637 WVFGRD96 9.0 50 90 15 4.68 0.6809 WVFGRD96 10.0 230 85 -15 4.70 0.6945 WVFGRD96 11.0 50 90 10 4.71 0.7007 WVFGRD96 12.0 50 90 10 4.72 0.7053 WVFGRD96 13.0 50 90 10 4.74 0.7060 WVFGRD96 14.0 230 90 -10 4.75 0.7039 WVFGRD96 15.0 50 90 10 4.76 0.7003 WVFGRD96 16.0 230 90 -10 4.76 0.6955 WVFGRD96 17.0 230 90 -10 4.77 0.6890 WVFGRD96 18.0 230 90 -10 4.78 0.6816 WVFGRD96 19.0 50 90 10 4.79 0.6736 WVFGRD96 20.0 50 85 10 4.80 0.6648 WVFGRD96 21.0 50 85 10 4.80 0.6558 WVFGRD96 22.0 230 90 -10 4.81 0.6450 WVFGRD96 23.0 230 90 -10 4.81 0.6344 WVFGRD96 24.0 50 85 10 4.82 0.6252 WVFGRD96 25.0 50 85 10 4.83 0.6141 WVFGRD96 26.0 50 85 10 4.83 0.6028 WVFGRD96 27.0 50 85 10 4.84 0.5915 WVFGRD96 28.0 50 85 10 4.84 0.5800 WVFGRD96 29.0 50 85 10 4.85 0.5683
The best solution is
WVFGRD96 13.0 50 90 10 4.74 0.7060
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 -40 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.06 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: