The ANSS event ID is ak019eagemve and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak019eagemve/executive.
2019/11/07 07:17:12 61.554 -149.916 46.2 3.6 Alaska
USGS/SLU Moment Tensor Solution
ENS 2019/11/07 07:17:12:0 61.55 -149.92 46.2 3.6 Alaska
Stations used:
AK.CUT AK.GHO AK.KNK AK.KTH AK.RC01 AK.SSN AT.PMR TA.M22K
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 0.10 n 3
Best Fitting Double Couple
Mo = 8.61e+21 dyne-cm
Mw = 3.89
Z = 60 km
Plane Strike Dip Rake
NP1 28 50 -94
NP2 215 40 -85
Principal Axes:
Axis Value Plunge Azimuth
T 8.61e+21 5 121
N 0.00e+00 3 31
P -8.61e+21 84 269
Moment Tensor: (dyne-cm)
Component Value
Mxx 2.33e+21
Mxy -3.80e+21
Mxz -3.83e+20
Myy 6.12e+21
Myz 1.55e+21
Mzz -8.45e+21
##############
#####################-
##############-----------###
############---------------###
###########------------------#####
##########--------------------######
##########---------------------#######
#########-----------------------########
########------------------------########
########-------------------------#########
########-------- -------------##########
#######--------- P -------------##########
#######--------- ------------###########
#####------------------------###########
#####-----------------------############
####----------------------######## #
####-------------------########## T
###-----------------############
##--------------##############
#-----------################
-----#################
##############
Global CMT Convention Moment Tensor:
R T P
-8.45e+21 -3.83e+20 -1.55e+21
-3.83e+20 2.33e+21 3.80e+21
-1.55e+21 3.80e+21 6.12e+21
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20191107071712/index.html
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STK = 215
DIP = 40
RAKE = -85
MW = 3.89
HS = 60.0
The NDK file is 20191107071712.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:
cut o DIST/3.3 -40 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT
WVFGRD96 2.0 360 45 85 3.21 0.2243
WVFGRD96 4.0 135 90 50 3.27 0.2327
WVFGRD96 6.0 310 80 -50 3.31 0.2670
WVFGRD96 8.0 85 20 40 3.37 0.2803
WVFGRD96 10.0 115 20 70 3.40 0.2899
WVFGRD96 12.0 295 40 45 3.41 0.2880
WVFGRD96 14.0 290 45 45 3.44 0.2974
WVFGRD96 16.0 290 45 45 3.46 0.2971
WVFGRD96 18.0 295 45 40 3.49 0.2902
WVFGRD96 20.0 290 50 30 3.50 0.2803
WVFGRD96 22.0 285 35 15 3.50 0.2787
WVFGRD96 24.0 285 35 15 3.52 0.2805
WVFGRD96 26.0 275 30 -10 3.54 0.2836
WVFGRD96 28.0 270 30 -15 3.55 0.2882
WVFGRD96 30.0 270 30 -20 3.58 0.2934
WVFGRD96 32.0 265 30 -25 3.59 0.2959
WVFGRD96 34.0 215 35 -80 3.64 0.3203
WVFGRD96 36.0 210 40 -90 3.67 0.3441
WVFGRD96 38.0 210 40 -90 3.69 0.3702
WVFGRD96 40.0 25 50 -90 3.78 0.3796
WVFGRD96 42.0 25 50 -90 3.80 0.3902
WVFGRD96 44.0 25 50 -90 3.82 0.3986
WVFGRD96 46.0 210 40 -85 3.83 0.4051
WVFGRD96 48.0 210 40 -85 3.84 0.4114
WVFGRD96 50.0 210 40 -85 3.85 0.4165
WVFGRD96 52.0 210 40 -85 3.86 0.4199
WVFGRD96 54.0 215 40 -85 3.87 0.4247
WVFGRD96 56.0 215 40 -85 3.87 0.4283
WVFGRD96 58.0 215 40 -85 3.88 0.4299
WVFGRD96 60.0 215 40 -85 3.89 0.4299
WVFGRD96 62.0 215 40 -85 3.89 0.4279
WVFGRD96 64.0 215 40 -85 3.90 0.4284
WVFGRD96 66.0 215 40 -85 3.90 0.4281
WVFGRD96 68.0 215 40 -85 3.91 0.4245
WVFGRD96 70.0 215 40 -85 3.91 0.4214
WVFGRD96 72.0 215 40 -85 3.92 0.4191
WVFGRD96 74.0 215 40 -85 3.93 0.4149
WVFGRD96 76.0 215 40 -85 3.93 0.4116
WVFGRD96 78.0 215 40 -85 3.94 0.4069
WVFGRD96 80.0 215 40 -85 3.94 0.4014
WVFGRD96 82.0 215 45 -85 3.95 0.3977
WVFGRD96 84.0 215 45 -85 3.95 0.3917
WVFGRD96 86.0 210 45 -85 3.96 0.3874
WVFGRD96 88.0 210 45 -85 3.96 0.3819
WVFGRD96 90.0 210 45 -85 3.97 0.3766
WVFGRD96 92.0 210 45 -85 3.97 0.3717
WVFGRD96 94.0 210 45 -85 3.98 0.3655
WVFGRD96 96.0 210 45 -85 3.98 0.3606
WVFGRD96 98.0 25 45 -95 3.99 0.3532
The best solution is
WVFGRD96 60.0 215 40 -85 3.89 0.4299
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 -40 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 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