The ANSS event ID is ak01386kg7tb and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak01386kg7tb/executive.
2013/06/27 11:40:47 61.328 -150.019 55.3 4.2 Alaska
USGS/SLU Moment Tensor Solution ENS 2013/06/27 11:40:47:0 61.33 -150.02 55.3 4.2 Alaska Stations used: AK.BPAW AK.BWN AK.GHO AK.GLI AK.HDA AK.HIN AK.KNK AK.KTH AK.MCK AK.RC01 AK.SAW AK.SCM AK.SKN AK.WRH II.KDAK IU.COLA Filtering commands used: cut a -10 a 150 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.06 n 3 Best Fitting Double Couple Mo = 3.67e+22 dyne-cm Mw = 4.31 Z = 58 km Plane Strike Dip Rake NP1 200 65 -35 NP2 306 59 -150 Principal Axes: Axis Value Plunge Azimuth T 3.67e+22 4 254 N 0.00e+00 48 349 P -3.67e+22 42 161 Moment Tensor: (dyne-cm) Component Value Mxx -1.56e+22 Mxy 1.57e+22 Mxz 1.66e+22 Myy 3.18e+22 Myz -8.38e+21 Mzz -1.61e+22 -------------- ---------------####### ----------------############ ---------------############### ##########------################## #################################### ################-----################# ################---------############### ###############------------############# ###############---------------############ ###############-----------------########## ##############-------------------######### ###########--------------------######## T ##########----------------------###### ##########-----------------------##### ###########------------------------### #########----------- -----------## ########----------- P ------------ #######---------- ---------- ######---------------------- ###------------------- -------------- Global CMT Convention Moment Tensor: R T P -1.61e+22 1.66e+22 8.38e+21 1.66e+22 -1.56e+22 -1.57e+22 8.38e+21 -1.57e+22 3.18e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20130627114047/index.html |
STK = 200 DIP = 65 RAKE = -35 MW = 4.31 HS = 58.0
The NDK file is 20130627114047.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 2013/06/27 11:40:47:0 61.33 -150.02 55.3 4.2 Alaska Stations used: AK.BPAW AK.BWN AK.GHO AK.GLI AK.HDA AK.HIN AK.KNK AK.KTH AK.MCK AK.RC01 AK.SAW AK.SCM AK.SKN AK.WRH II.KDAK IU.COLA Filtering commands used: cut a -10 a 150 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.06 n 3 Best Fitting Double Couple Mo = 3.67e+22 dyne-cm Mw = 4.31 Z = 58 km Plane Strike Dip Rake NP1 200 65 -35 NP2 306 59 -150 Principal Axes: Axis Value Plunge Azimuth T 3.67e+22 4 254 N 0.00e+00 48 349 P -3.67e+22 42 161 Moment Tensor: (dyne-cm) Component Value Mxx -1.56e+22 Mxy 1.57e+22 Mxz 1.66e+22 Myy 3.18e+22 Myz -8.38e+21 Mzz -1.61e+22 -------------- ---------------####### ----------------############ ---------------############### ##########------################## #################################### ################-----################# ################---------############### ###############------------############# ###############---------------############ ###############-----------------########## ##############-------------------######### ###########--------------------######## T ##########----------------------###### ##########-----------------------##### ###########------------------------### #########----------- -----------## ########----------- P ------------ #######---------- ---------- ######---------------------- ###------------------- -------------- Global CMT Convention Moment Tensor: R T P -1.61e+22 1.66e+22 8.38e+21 1.66e+22 -1.56e+22 -1.57e+22 8.38e+21 -1.57e+22 3.18e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20130627114047/index.html |
us ak10746531-neic-mwr Type Mwr Moment 3.62e+15 N-m Magnitude 4.3 Percent DC 77% Depth 56.0 km Author neic Updated 2013-06-27 16:56:42 UTC Principal Axes Axis Value Plunge Azimuth T 3.413 8 266 N 0.388 40 3 P -3.801 49 166 Nodal Planes Plane Strike Dip Rake NP1 206 64 -45 NP2 320 50 -146 |
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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 a -10 a 150 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.06 n 3The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 0.5 160 45 60 3.48 0.1538 WVFGRD96 1.0 160 50 65 3.53 0.1632 WVFGRD96 2.0 165 45 65 3.64 0.2076 WVFGRD96 3.0 160 50 60 3.71 0.2215 WVFGRD96 4.0 160 50 55 3.74 0.2160 WVFGRD96 5.0 150 65 40 3.73 0.2042 WVFGRD96 6.0 305 70 -25 3.72 0.2057 WVFGRD96 7.0 325 85 30 3.74 0.2123 WVFGRD96 8.0 330 80 40 3.79 0.2195 WVFGRD96 9.0 325 85 35 3.80 0.2250 WVFGRD96 10.0 140 90 -35 3.80 0.2289 WVFGRD96 11.0 140 90 -35 3.81 0.2326 WVFGRD96 12.0 320 90 35 3.82 0.2362 WVFGRD96 13.0 305 90 35 3.84 0.2390 WVFGRD96 14.0 305 90 35 3.85 0.2417 WVFGRD96 15.0 305 90 35 3.86 0.2449 WVFGRD96 16.0 305 85 35 3.87 0.2463 WVFGRD96 17.0 305 85 35 3.88 0.2478 WVFGRD96 18.0 305 85 35 3.89 0.2493 WVFGRD96 19.0 305 85 35 3.90 0.2508 WVFGRD96 20.0 40 70 -30 3.90 0.2515 WVFGRD96 21.0 40 70 -30 3.91 0.2579 WVFGRD96 22.0 40 70 -30 3.92 0.2647 WVFGRD96 23.0 40 70 -30 3.93 0.2710 WVFGRD96 24.0 40 70 -30 3.94 0.2768 WVFGRD96 25.0 40 70 -30 3.95 0.2826 WVFGRD96 26.0 40 70 -30 3.96 0.2874 WVFGRD96 27.0 40 70 -30 3.96 0.2923 WVFGRD96 28.0 40 70 -30 3.97 0.2967 WVFGRD96 29.0 40 70 -30 3.98 0.3007 WVFGRD96 30.0 40 70 -25 3.99 0.3048 WVFGRD96 31.0 215 65 -15 4.03 0.3157 WVFGRD96 32.0 215 65 -15 4.04 0.3238 WVFGRD96 33.0 215 65 -20 4.05 0.3317 WVFGRD96 34.0 215 65 -20 4.06 0.3389 WVFGRD96 35.0 215 65 -20 4.07 0.3459 WVFGRD96 36.0 215 65 -20 4.09 0.3523 WVFGRD96 37.0 215 65 -20 4.10 0.3583 WVFGRD96 38.0 215 65 -20 4.11 0.3640 WVFGRD96 39.0 210 65 -20 4.13 0.3704 WVFGRD96 40.0 210 60 -30 4.18 0.3661 WVFGRD96 41.0 210 60 -30 4.19 0.3727 WVFGRD96 42.0 210 60 -30 4.20 0.3783 WVFGRD96 43.0 210 60 -30 4.21 0.3827 WVFGRD96 44.0 210 60 -30 4.22 0.3860 WVFGRD96 45.0 210 60 -30 4.23 0.3891 WVFGRD96 46.0 210 60 -35 4.24 0.3914 WVFGRD96 47.0 210 60 -35 4.24 0.3932 WVFGRD96 48.0 210 60 -35 4.25 0.3943 WVFGRD96 49.0 205 65 -30 4.26 0.3955 WVFGRD96 50.0 205 65 -30 4.27 0.3976 WVFGRD96 51.0 205 65 -30 4.27 0.3991 WVFGRD96 52.0 205 65 -30 4.28 0.4005 WVFGRD96 53.0 205 65 -35 4.28 0.4016 WVFGRD96 54.0 200 65 -35 4.30 0.4024 WVFGRD96 55.0 200 65 -35 4.30 0.4038 WVFGRD96 56.0 200 65 -35 4.30 0.4047 WVFGRD96 57.0 200 65 -35 4.31 0.4054 WVFGRD96 58.0 200 65 -35 4.31 0.4054 WVFGRD96 59.0 200 65 -35 4.32 0.4047 WVFGRD96 60.0 200 65 -35 4.32 0.4037 WVFGRD96 61.0 200 65 -35 4.32 0.4026 WVFGRD96 62.0 200 65 -35 4.32 0.4013 WVFGRD96 63.0 200 65 -35 4.33 0.3992 WVFGRD96 64.0 200 65 -35 4.33 0.3968 WVFGRD96 65.0 200 70 -35 4.34 0.3959 WVFGRD96 66.0 200 70 -35 4.34 0.3953 WVFGRD96 67.0 200 70 -35 4.34 0.3935 WVFGRD96 68.0 200 70 -35 4.35 0.3914 WVFGRD96 69.0 200 70 -35 4.35 0.3899 WVFGRD96 70.0 200 70 -35 4.35 0.3876 WVFGRD96 71.0 200 70 -35 4.35 0.3857 WVFGRD96 72.0 200 70 -35 4.35 0.3831 WVFGRD96 73.0 200 70 -35 4.35 0.3808 WVFGRD96 74.0 200 70 -35 4.35 0.3780 WVFGRD96 75.0 200 70 -35 4.35 0.3754 WVFGRD96 76.0 200 70 -35 4.35 0.3732 WVFGRD96 77.0 200 75 -35 4.37 0.3701 WVFGRD96 78.0 200 75 -35 4.37 0.3684 WVFGRD96 79.0 200 75 -35 4.37 0.3661
The best solution is
WVFGRD96 58.0 200 65 -35 4.31 0.4054
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 a -10 a 150 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.06 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