The ANSS event ID is usp000jrdv and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/usp000jrdv/executive.
2012/09/01 10:57:34 66.836 -135.612 20.0 4 Yukon, Canada
USGS/SLU Moment Tensor Solution ENS 2012/09/01 10:57:34:0 66.84 -135.61 20.0 4.0 Yukon, Canada Stations used: AK.BPAW AK.CAST AK.CCB AK.COLD AK.DHY AK.DIV AK.DOT AK.FYU AK.GHO AK.GLM AK.HDA CN.BVCY CN.CLVN CN.DAWY CN.INK IU.COLA US.EGAK Filtering commands used: hp c 0.02 n 3 lp c 0.06 n 3 br c 0.12 0.25 n 4 p 2 Best Fitting Double Couple Mo = 8.32e+21 dyne-cm Mw = 3.88 Z = 26 km Plane Strike Dip Rake NP1 359 82 145 NP2 95 55 10 Principal Axes: Axis Value Plunge Azimuth T 8.32e+21 30 311 N 0.00e+00 54 168 P -8.32e+21 18 52 Moment Tensor: (dyne-cm) Component Value Mxx -1.82e+20 Mxy -6.73e+21 Mxz 9.02e+20 Myy -1.18e+21 Myz -4.64e+21 Mzz 1.36e+21 #######------- ############---------- ###############------------- ################-------------- ##### ##########----------- -- ###### T ###########---------- P --- ####### ###########---------- ---- ######################------------------ ######################------------------ #######################------------------- -######################------------------- --#####################------------------- ----###################------------------# ------################----------------## ----------############------------###### ---------------######-------########## --------------------################ -------------------############### -----------------############# ---------------############# ------------########## --------###### Global CMT Convention Moment Tensor: R T P 1.36e+21 9.02e+20 4.64e+21 9.02e+20 -1.82e+20 6.73e+21 4.64e+21 6.73e+21 -1.18e+21 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20120901105734/index.html |
STK = 95 DIP = 55 RAKE = 10 MW = 3.88 HS = 26.0
The NDK file is 20120901105734.ndk The waveform inversion is preferred.
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:
hp c 0.02 n 3 lp c 0.06 n 3 br c 0.12 0.25 n 4 p 2The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 0.5 50 40 -90 3.71 0.3249 WVFGRD96 1.0 180 50 -80 3.53 0.3144 WVFGRD96 2.0 180 50 -85 3.60 0.3353 WVFGRD96 3.0 180 50 -80 3.66 0.3294 WVFGRD96 4.0 300 40 45 3.68 0.3125 WVFGRD96 5.0 290 40 35 3.72 0.3110 WVFGRD96 6.0 270 50 0 3.72 0.3137 WVFGRD96 7.0 265 45 -20 3.72 0.3192 WVFGRD96 8.0 260 40 -30 3.79 0.3262 WVFGRD96 9.0 260 40 -35 3.79 0.3358 WVFGRD96 10.0 260 40 -35 3.78 0.3441 WVFGRD96 11.0 260 45 -40 3.78 0.3525 WVFGRD96 12.0 260 40 -40 3.78 0.3596 WVFGRD96 13.0 265 45 -35 3.78 0.3658 WVFGRD96 14.0 265 45 -35 3.78 0.3714 WVFGRD96 15.0 90 50 -10 3.78 0.3757 WVFGRD96 16.0 100 45 20 3.78 0.3847 WVFGRD96 17.0 100 45 20 3.79 0.3951 WVFGRD96 18.0 100 45 20 3.79 0.4042 WVFGRD96 19.0 100 50 20 3.82 0.4121 WVFGRD96 20.0 100 50 20 3.82 0.4190 WVFGRD96 21.0 100 50 20 3.83 0.4240 WVFGRD96 22.0 100 50 15 3.84 0.4283 WVFGRD96 23.0 100 50 15 3.85 0.4319 WVFGRD96 24.0 95 55 10 3.87 0.4342 WVFGRD96 25.0 95 55 10 3.88 0.4357 WVFGRD96 26.0 95 55 10 3.88 0.4363 WVFGRD96 27.0 95 55 5 3.90 0.4362 WVFGRD96 28.0 95 55 5 3.90 0.4354 WVFGRD96 29.0 95 55 5 3.91 0.4339 WVFGRD96 30.0 95 55 5 3.92 0.4316 WVFGRD96 31.0 95 55 5 3.93 0.4287 WVFGRD96 32.0 95 55 5 3.93 0.4251 WVFGRD96 33.0 95 55 5 3.94 0.4210 WVFGRD96 34.0 95 60 5 3.97 0.4166 WVFGRD96 35.0 95 60 5 3.98 0.4117 WVFGRD96 36.0 310 60 30 3.96 0.4041 WVFGRD96 37.0 305 60 30 3.97 0.3988 WVFGRD96 38.0 305 60 30 3.99 0.3925 WVFGRD96 39.0 90 60 5 4.01 0.3855 WVFGRD96 40.0 95 45 10 4.07 0.3799 WVFGRD96 41.0 95 45 10 4.07 0.3733 WVFGRD96 42.0 100 45 15 4.08 0.3664 WVFGRD96 43.0 100 45 15 4.08 0.3594 WVFGRD96 44.0 95 50 10 4.10 0.3521 WVFGRD96 45.0 95 50 10 4.10 0.3444 WVFGRD96 46.0 95 50 10 4.11 0.3363 WVFGRD96 47.0 100 50 15 4.11 0.3283 WVFGRD96 48.0 100 50 15 4.12 0.3203 WVFGRD96 49.0 100 50 15 4.12 0.3119
The best solution is
WVFGRD96 26.0 95 55 10 3.88 0.4363
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
hp c 0.02 n 3 lp c 0.06 n 3 br c 0.12 0.25 n 4 p 2
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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 CUS.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 CUS Model with Q from simple gamma values 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 1.0000 5.0000 2.8900 2.5000 0.172E-02 0.387E-02 0.00 0.00 1.00 1.00 9.0000 6.1000 3.5200 2.7300 0.160E-02 0.363E-02 0.00 0.00 1.00 1.00 10.0000 6.4000 3.7000 2.8200 0.149E-02 0.336E-02 0.00 0.00 1.00 1.00 20.0000 6.7000 3.8700 2.9020 0.000E-04 0.000E-04 0.00 0.00 1.00 1.00 0.0000 8.1500 4.7000 3.3640 0.194E-02 0.431E-02 0.00 0.00 1.00 1.00