The ANSS event ID is nn00903470 and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/nn00903470/executive.
2025/08/30 18:59:53 41.177 -116.801 6.0 5.3 Nevada
USGS/SLU Moment Tensor Solution ENS 2025/08/30 18:59:53.0 41.18 -116.80 6.0 5.3 Nevada Stations used: BK.BIGV BK.EAGL BK.HATC BK.MNLT BK.MZTA BK.RAVE BK.SWNM BK.YUBA IE.NPRI IM.NV31 IW.MFID IW.PLID NC.AFD NC.LDH NN.BEK NN.BFC NN.DIX NN.GMN NN.KVN NN.LHV NN.MPK NN.OUT1 NN.PNT NN.PYM2 NN.Q09A NN.R11B NN.S11A NN.WAK NN.WASH NN.YER UO.ADEL UO.HAMAK UO.PRONG US.BMO US.DUG US.ELK US.HLID US.HWUT US.WVOR UU.BEID UU.BGU UU.CTU UU.FSU UU.HDUT UU.MCU UU.MOUT UU.NLU UU.NOQ UU.SPU UW.IRON UW.IZEE UW.TREE WW.CNCL WW.IRMR Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 1.68e+23 dyne-cm Mw = 4.75 Z = 8 km Plane Strike Dip Rake NP1 25 57 -123 NP2 255 45 -50 Principal Axes: Axis Value Plunge Azimuth T 1.68e+23 7 138 N 0.00e+00 27 44 P -1.68e+23 62 241 Moment Tensor: (dyne-cm) Component Value Mxx 8.18e+22 Mxy -9.82e+22 Mxz 1.97e+22 Myy 4.68e+22 Myz 7.37e+22 Mzz -1.29e+23 ############## ####################-- ########################---- #########################----- ############################------ #############----------------##----- ##########--------------------######-- ########----------------------#########- ######------------------------########## #####--------------------------########### ####--------------------------############ ###----------- -------------############ ##------------ P ------------############# ------------- -----------############# --------------------------############## ------------------------############## ---------------------############### -------------------########## ## ---------------############ T ------------############## ------################ ############## Global CMT Convention Moment Tensor: R T P -1.29e+23 1.97e+22 -7.37e+22 1.97e+22 8.18e+22 9.82e+22 -7.37e+22 9.82e+22 4.68e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20250830185953/index.html |
STK = 255 DIP = 45 RAKE = -50 MW = 4.75 HS = 8.0
The NDK file is 20250830185953.ndk The waveform inversion is preferred.
The following compares this source inversion to those provided by others. The purpose is to look for major differences and also to note slight differences that might be inherent to the processing procedure. For completeness the USGS/SLU solution is repeated from above.
USGS/SLU Moment Tensor Solution ENS 2025/08/30 18:59:53.0 41.18 -116.80 6.0 5.3 Nevada Stations used: BK.BIGV BK.EAGL BK.HATC BK.MNLT BK.MZTA BK.RAVE BK.SWNM BK.YUBA IE.NPRI IM.NV31 IW.MFID IW.PLID NC.AFD NC.LDH NN.BEK NN.BFC NN.DIX NN.GMN NN.KVN NN.LHV NN.MPK NN.OUT1 NN.PNT NN.PYM2 NN.Q09A NN.R11B NN.S11A NN.WAK NN.WASH NN.YER UO.ADEL UO.HAMAK UO.PRONG US.BMO US.DUG US.ELK US.HLID US.HWUT US.WVOR UU.BEID UU.BGU UU.CTU UU.FSU UU.HDUT UU.MCU UU.MOUT UU.NLU UU.NOQ UU.SPU UW.IRON UW.IZEE UW.TREE WW.CNCL WW.IRMR Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 1.68e+23 dyne-cm Mw = 4.75 Z = 8 km Plane Strike Dip Rake NP1 25 57 -123 NP2 255 45 -50 Principal Axes: Axis Value Plunge Azimuth T 1.68e+23 7 138 N 0.00e+00 27 44 P -1.68e+23 62 241 Moment Tensor: (dyne-cm) Component Value Mxx 8.18e+22 Mxy -9.82e+22 Mxz 1.97e+22 Myy 4.68e+22 Myz 7.37e+22 Mzz -1.29e+23 ############## ####################-- ########################---- #########################----- ############################------ #############----------------##----- ##########--------------------######-- ########----------------------#########- ######------------------------########## #####--------------------------########### ####--------------------------############ ###----------- -------------############ ##------------ P ------------############# ------------- -----------############# --------------------------############## ------------------------############## ---------------------############### -------------------########## ## ---------------############ T ------------############## ------################ ############## Global CMT Convention Moment Tensor: R T P -1.29e+23 1.97e+22 -7.37e+22 1.97e+22 8.18e+22 9.82e+22 -7.37e+22 9.82e+22 4.68e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20250830185953/index.html |
Regional Moment Tensor (Mwr) Moment 1.854e+16 N-m Magnitude 4.78 Mwr Depth 8.0 km Percent DC 88% Half Duration - Catalog US Data Source US Contributor US Nodal Planes Plane Strike Dip Rake NP1 55 53 -85 NP2 227 37 -96 Principal Axes Axis Value Plunge Azimuth T 1.907e+16 8 141 N -0.113e+16 4 232 P -1.795e+16 81 347 |
W-phase Moment Tensor (Mww) Moment 2.571e+16 N-m Magnitude 4.87 Mww Depth 11.5 km Percent DC 94% Half Duration 0.50 s Catalog US Data Source US Contributor US Nodal Planes Plane Strike Dip Rake NP1 66 58 -72 NP2 215 36 -116 Principal Axes Axis Value Plunge Azimuth T 2.611e+16 11 143 N -0.081e+16 15 236 P -2.530e+16 71 18 |
Given the availability of digital waveforms for determination of the moment tensor, this section documents the added processing leading to mLg, if appropriate to the region, and ML by application of the respective IASPEI formulae. As a research study, the linear distance term of the IASPEI formula for ML is adjusted to remove a linear distance trend in residuals to give a regionally defined ML. The defined ML uses horizontal component recordings, but the same procedure is applied to the vertical components since there may be some interest in vertical component ground motions. Residual plots versus distance may indicate interesting features of ground motion scaling in some distance ranges. A residual plot of the regionalized magnitude is given as a function of distance and azimuth, since data sets may transcend different wave propagation provinces.
Left: ML computed using the IASPEI formula for Horizontal components. Center: 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.
Right: Residuals from new relation as a function of distance and azimuth.
Left: ML computed using the IASPEI formula for Vertical components (research). Center: 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.
Right: Residuals from new relation as a function of distance and azimuth.
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The focal mechanism was determined using broadband seismic waveforms. The location of the event (star) and the stations used for (red) 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's 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 0.03 n 3 lp c 0.07 n 3The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 1.0 270 70 -15 4.42 0.4190 WVFGRD96 2.0 270 65 -20 4.51 0.4780 WVFGRD96 3.0 270 45 -15 4.60 0.5085 WVFGRD96 4.0 265 45 -25 4.63 0.5491 WVFGRD96 5.0 265 45 -30 4.65 0.5848 WVFGRD96 6.0 265 50 -35 4.66 0.6100 WVFGRD96 7.0 265 50 -35 4.67 0.6223 WVFGRD96 8.0 255 45 -50 4.75 0.6456 WVFGRD96 9.0 265 50 -35 4.72 0.6424 WVFGRD96 10.0 265 55 -35 4.73 0.6348 WVFGRD96 11.0 270 60 -20 4.72 0.6265 WVFGRD96 12.0 270 60 -20 4.73 0.6154 WVFGRD96 13.0 270 60 -15 4.73 0.6008 WVFGRD96 14.0 275 65 -10 4.74 0.5866 WVFGRD96 15.0 280 65 15 4.75 0.5715 WVFGRD96 16.0 280 65 15 4.76 0.5558 WVFGRD96 17.0 105 65 20 4.76 0.5394 WVFGRD96 18.0 100 65 15 4.77 0.5246 WVFGRD96 19.0 100 65 15 4.77 0.5092 WVFGRD96 20.0 100 65 15 4.78 0.4930 WVFGRD96 21.0 100 65 10 4.78 0.4772 WVFGRD96 22.0 100 65 10 4.79 0.4612 WVFGRD96 23.0 100 65 10 4.79 0.4452 WVFGRD96 24.0 100 65 10 4.80 0.4293 WVFGRD96 25.0 100 65 10 4.80 0.4135 WVFGRD96 26.0 100 65 10 4.81 0.3981 WVFGRD96 27.0 100 65 5 4.81 0.3831 WVFGRD96 28.0 100 65 5 4.81 0.3685 WVFGRD96 29.0 100 65 5 4.82 0.3542
The best solution is
WVFGRD96 8.0 255 45 -50 4.75 0.6456
The mechanism corresponding 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, the velocity model used in the predictions may not be perfect and the epicentral parameters may be be off. 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 0.03 n 3 lp c 0.07 n 3
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Figure 3. Waveform comparison for selected depth. Red: observed; Blue - predicted. The time shift with respect to the model prediction is indicated. The percent of fit is also indicated. The time scale is relative to the first trace sample. |
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Focal mechanism sensitivity at the preferred depth. The red color indicates a very good fit to the waveforms. 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 WUS.model used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows (The format is in the model96 format of Computer Programs in Seismology).
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