The ANSS event ID is usb000se5p and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/usb000se5p/executive.
2014/09/19 01:31:53 36.603 -97.613 4.6 3.8 Oklahoma
USGS/SLU Moment Tensor Solution ENS 2014/09/19 01:31:53:0 36.60 -97.61 4.6 3.8 Oklahoma Stations used: AG.HHAR AG.LCAR AG.WHAR AG.WLAR GS.KAN10 GS.KAN13 GS.OK025 GS.OK026 GS.OK027 GS.OK028 GS.OK029 N4.N33B N4.N35B N4.P38B N4.R32B N4.S39B N4.T35B N4.U38B N4.Z35B NM.MGMO NM.UALR OK.BCOK OK.CROK OK.FNO OK.KAY1 OK.U32A OK.X37A TA.ABTX TA.KSCO TA.TUL1 TA.U40A TA.W39A TA.WHTX TA.X40A US.AMTX US.KSU1 US.MIAR US.WMOK Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 4.62e+21 dyne-cm Mw = 3.71 Z = 3 km Plane Strike Dip Rake NP1 335 80 -30 NP2 71 61 -168 Principal Axes: Axis Value Plunge Azimuth T 4.62e+21 13 26 N 0.00e+00 59 138 P -4.62e+21 28 289 Moment Tensor: (dyne-cm) Component Value Mxx 3.16e+21 Mxy 2.84e+21 Mxz 2.88e+20 Myy -2.37e+21 Myz 2.26e+21 Mzz -7.91e+20 ############## ---############### # --------############# T #### ----------############ ##### -------------##################### ----------------#################### ------------------#################### ---- -------------###################- ---- P --------------#################-- ----- ---------------###############---- -----------------------##############----- ------------------------###########------- -------------------------#######---------- -------------------------###------------ ------------------------##-------------- ###--------------########------------- #########################----------- ########################---------- #######################------- ######################------ ####################-- ############## Global CMT Convention Moment Tensor: R T P -7.91e+20 2.88e+20 -2.26e+21 2.88e+20 3.16e+21 -2.84e+21 -2.26e+21 -2.84e+21 -2.37e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20140919013153/index.html |
STK = 335 DIP = 80 RAKE = -30 MW = 3.71 HS = 3.0
The NDK file is 20140919013153.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 2014/09/19 01:31:53:0 36.60 -97.61 4.6 3.8 Oklahoma Stations used: AG.HHAR AG.LCAR AG.WHAR AG.WLAR GS.KAN10 GS.KAN13 GS.OK025 GS.OK026 GS.OK027 GS.OK028 GS.OK029 N4.N33B N4.N35B N4.P38B N4.R32B N4.S39B N4.T35B N4.U38B N4.Z35B NM.MGMO NM.UALR OK.BCOK OK.CROK OK.FNO OK.KAY1 OK.U32A OK.X37A TA.ABTX TA.KSCO TA.TUL1 TA.U40A TA.W39A TA.WHTX TA.X40A US.AMTX US.KSU1 US.MIAR US.WMOK Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 4.62e+21 dyne-cm Mw = 3.71 Z = 3 km Plane Strike Dip Rake NP1 335 80 -30 NP2 71 61 -168 Principal Axes: Axis Value Plunge Azimuth T 4.62e+21 13 26 N 0.00e+00 59 138 P -4.62e+21 28 289 Moment Tensor: (dyne-cm) Component Value Mxx 3.16e+21 Mxy 2.84e+21 Mxz 2.88e+20 Myy -2.37e+21 Myz 2.26e+21 Mzz -7.91e+20 ############## ---############### # --------############# T #### ----------############ ##### -------------##################### ----------------#################### ------------------#################### ---- -------------###################- ---- P --------------#################-- ----- ---------------###############---- -----------------------##############----- ------------------------###########------- -------------------------#######---------- -------------------------###------------ ------------------------##-------------- ###--------------########------------- #########################----------- ########################---------- #######################------- ######################------ ####################-- ############## Global CMT Convention Moment Tensor: R T P -7.91e+20 2.88e+20 -2.26e+21 2.88e+20 3.16e+21 -2.84e+21 -2.26e+21 -2.84e+21 -2.37e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20140919013153/index.html |
Moment 6.83e+14 N-m Magnitude 3.8 Percent DC 87% Depth 4.0 km Updated 2014-09-19 03:57:22 UTC Author us Catalog us Contributor us Code us_b000se5p_mwr Principal Axes Axis Value Plunge Azimuth T 6.612 5 24 N 0.424 52 287 P -7.036 38 117 Nodal Planes Plane Strike Dip Rake NP1 257 68 -148 NP2 153 60 -25 |
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: mLg computed using the IASPEI formula. Center: mLg residuals versus epicentral distance ; the values used for the trimmed mean magnitude estimate are indicated.
Right: residuals as a function of distance and azimuth.
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 +50 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 1.0 335 75 -35 3.57 0.5518 WVFGRD96 2.0 335 80 -45 3.71 0.6419 WVFGRD96 3.0 335 80 -30 3.71 0.6584 WVFGRD96 4.0 155 90 20 3.72 0.6469 WVFGRD96 5.0 340 75 0 3.73 0.6343 WVFGRD96 6.0 340 75 -5 3.75 0.6220 WVFGRD96 7.0 340 75 0 3.77 0.6074 WVFGRD96 8.0 340 75 10 3.80 0.5886 WVFGRD96 9.0 340 75 10 3.81 0.5720 WVFGRD96 10.0 340 75 15 3.83 0.5558 WVFGRD96 11.0 340 75 15 3.84 0.5422 WVFGRD96 12.0 160 75 15 3.85 0.5307 WVFGRD96 13.0 160 75 15 3.86 0.5198 WVFGRD96 14.0 160 75 15 3.87 0.5081 WVFGRD96 15.0 160 75 15 3.88 0.4972 WVFGRD96 16.0 160 75 15 3.89 0.4860 WVFGRD96 17.0 160 75 15 3.90 0.4751 WVFGRD96 18.0 160 75 -5 3.89 0.4649 WVFGRD96 19.0 160 75 -5 3.90 0.4561 WVFGRD96 20.0 160 75 -5 3.91 0.4475 WVFGRD96 21.0 160 75 -5 3.91 0.4389 WVFGRD96 22.0 160 75 -5 3.92 0.4311 WVFGRD96 23.0 160 75 -5 3.92 0.4228 WVFGRD96 24.0 160 75 -10 3.93 0.4146 WVFGRD96 25.0 160 75 -10 3.93 0.4074 WVFGRD96 26.0 160 75 -10 3.94 0.3994 WVFGRD96 27.0 155 75 -15 3.95 0.3926 WVFGRD96 28.0 155 75 -15 3.95 0.3861 WVFGRD96 29.0 155 75 -15 3.96 0.3802
The best solution is
WVFGRD96 3.0 335 80 -30 3.71 0.6584
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 +50 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