The ANSS event ID is ak00856o20f and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak00856o20f/executive.
2008/01/03 13:53:10 66.322 -142.392 10.0 4 Alaska
USGS/SLU Moment Tensor Solution
ENS 2008/01/03 13:53:10:0 66.32 -142.39 10.0 4.0 Alaska
Stations used:
AK.BPAW AK.COLD AK.KTH AK.MCK AK.TRF CN.WHY IU.COLA US.EGAK
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
br c 0.12 0.25 n 4 p 2
Best Fitting Double Couple
Mo = 5.50e+21 dyne-cm
Mw = 3.76
Z = 8 km
Plane Strike Dip Rake
NP1 225 85 20
NP2 133 70 175
Principal Axes:
Axis Value Plunge Azimuth
T 5.50e+21 18 91
N 0.00e+00 69 238
P -5.50e+21 10 357
Moment Tensor: (dyne-cm)
Component Value
Mxx -5.31e+21
Mxy 1.63e+20
Mxz -9.91e+20
Myy 4.98e+21
Myz 1.63e+21
Mzz 3.26e+20
----- P ------
--------- ----------
----------------------------
-----------------------------#
##--------------------------######
####-----------------------#########
######--------------------############
########-----------------###############
#########--------------#################
############----------####################
#############-------################# ##
###############---################### T ##
################-#################### ##
##############----######################
############--------####################
#########------------#################
#######----------------#############
####---------------------#########
#---------------------------##
----------------------------
----------------------
--------------
Global CMT Convention Moment Tensor:
R T P
3.26e+20 -9.91e+20 -1.63e+21
-9.91e+20 -5.31e+21 -1.63e+20
-1.63e+21 -1.63e+20 4.98e+21
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20080103135310/index.html
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STK = 225
DIP = 85
RAKE = 20
MW = 3.76
HS = 8.0
The NDK file is 20080103135310.ndk The waveform inversion is preferred.
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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 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 1.0 45 80 -15 3.51 0.5485
WVFGRD96 2.0 45 75 -15 3.60 0.6714
WVFGRD96 3.0 45 80 -5 3.62 0.7136
WVFGRD96 4.0 225 90 5 3.65 0.7352
WVFGRD96 5.0 225 85 10 3.68 0.7486
WVFGRD96 6.0 225 85 15 3.71 0.7599
WVFGRD96 7.0 225 85 15 3.73 0.7686
WVFGRD96 8.0 225 85 20 3.76 0.7745
WVFGRD96 9.0 225 85 15 3.77 0.7735
WVFGRD96 10.0 45 75 -10 3.78 0.7710
WVFGRD96 11.0 45 75 -10 3.79 0.7669
WVFGRD96 12.0 230 75 -10 3.78 0.7622
WVFGRD96 13.0 230 80 -10 3.80 0.7591
WVFGRD96 14.0 230 80 -10 3.81 0.7542
WVFGRD96 15.0 230 80 -10 3.83 0.7464
WVFGRD96 16.0 230 80 -10 3.84 0.7354
WVFGRD96 17.0 230 80 -10 3.85 0.7219
WVFGRD96 18.0 230 80 -10 3.86 0.7057
WVFGRD96 19.0 55 80 15 3.86 0.6924
WVFGRD96 20.0 55 80 15 3.87 0.6761
WVFGRD96 21.0 55 75 15 3.89 0.6587
WVFGRD96 22.0 55 75 15 3.90 0.6405
WVFGRD96 23.0 55 75 15 3.90 0.6222
WVFGRD96 24.0 55 75 15 3.91 0.6040
WVFGRD96 25.0 60 70 15 3.92 0.5864
WVFGRD96 26.0 60 70 15 3.92 0.5686
WVFGRD96 27.0 60 70 15 3.93 0.5519
WVFGRD96 28.0 60 65 15 3.94 0.5371
WVFGRD96 29.0 60 65 15 3.95 0.5215
The best solution is
WVFGRD96 8.0 225 85 20 3.76 0.7745
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 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