The ANSS event ID is usp00089hq and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/usp00089hq/executive.
1997/10/24 08:35:17 31.118 -87.339 10.0 4.8 Alabama
USGS/SLU Moment Tensor Solution
ENS 1997/10/24 08:35:17:0 31.12 -87.34 10.0 4.8 Alabama
Stations used:
IU.CCM IU.SSPA IU.WCI NM.SLM US.AAM US.BLA US.CBKS US.CEH
US.GOGA US.JFWS US.MCWV US.MIAR US.OXF US.WMOK
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 = 8.41e+22 dyne-cm
Mw = 4.55
Z = 2 km
Plane Strike Dip Rake
NP1 285 50 -85
NP2 97 40 -96
Principal Axes:
Axis Value Plunge Azimuth
T 8.41e+22 5 11
N 0.00e+00 4 102
P -8.41e+22 84 230
Moment Tensor: (dyne-cm)
Component Value
Mxx 7.98e+22
Mxy 1.58e+22
Mxz 1.28e+22
Myy 2.72e+21
Myz 8.32e+21
Mzz -8.25e+22
######### T ##
############# ######
############################
##############################
##################################
#######------------#################
###-----------------------############
#-----------------------------##########
---------------------------------#######
------------------------------------######
#----------------- -----------------####
##---------------- P ------------------###
###--------------- -------------------##
###------------------------------------#
#####---------------------------------##
#######---------------------------####
#########---------------------######
##############---------###########
##############################
############################
######################
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Global CMT Convention Moment Tensor:
R T P
-8.25e+22 1.28e+22 -8.32e+21
1.28e+22 7.98e+22 -1.58e+22
-8.32e+21 -1.58e+22 2.72e+21
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/19971024083517/index.html
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STK = 285
DIP = 50
RAKE = -85
MW = 4.55
HS = 2.0
The NDK file is 19971024083517.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 3The results of this grid search are as follow:
DEPTH STK DIP RAKE MW FIT
WVFGRD96 1.0 125 40 -50 4.45 0.2094
WVFGRD96 2.0 285 50 -85 4.55 0.2389
WVFGRD96 3.0 95 40 -95 4.61 0.2198
WVFGRD96 4.0 280 55 -80 4.55 0.1646
WVFGRD96 5.0 80 30 -110 4.47 0.1418
WVFGRD96 6.0 285 65 -75 4.44 0.1424
WVFGRD96 7.0 155 65 35 4.46 0.1501
WVFGRD96 8.0 155 65 35 4.47 0.1581
WVFGRD96 9.0 150 65 40 4.47 0.1652
WVFGRD96 10.0 155 60 40 4.51 0.1690
WVFGRD96 11.0 155 55 50 4.52 0.1753
WVFGRD96 12.0 155 55 50 4.53 0.1816
WVFGRD96 13.0 155 55 50 4.54 0.1870
WVFGRD96 14.0 155 55 50 4.55 0.1916
WVFGRD96 15.0 95 55 85 4.53 0.1960
WVFGRD96 16.0 95 55 85 4.54 0.2019
WVFGRD96 17.0 95 55 85 4.56 0.2073
WVFGRD96 18.0 95 55 85 4.57 0.2121
WVFGRD96 19.0 95 55 85 4.58 0.2164
WVFGRD96 20.0 95 55 85 4.62 0.2203
WVFGRD96 21.0 95 55 85 4.63 0.2234
WVFGRD96 22.0 95 55 90 4.64 0.2256
WVFGRD96 23.0 275 35 90 4.65 0.2273
WVFGRD96 24.0 275 35 90 4.66 0.2281
WVFGRD96 25.0 270 40 85 4.67 0.2284
WVFGRD96 26.0 270 40 85 4.68 0.2286
WVFGRD96 27.0 270 40 85 4.68 0.2282
WVFGRD96 28.0 100 50 95 4.69 0.2272
WVFGRD96 29.0 270 45 85 4.70 0.2260
The best solution is
WVFGRD96 2.0 285 50 -85 4.55 0.2389
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 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