Location

Location ANSS

The ANSS event ID is usp000hjav and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/usp000hjav/executive.

2010/08/17 02:49:55 43.593 -110.344 5.0 4.1 Wyoming

Focal Mechanism

USGS/SLU Moment Tensor Solution ENS 2010/08/17 02:49:55:0 43.59 -110.34 5.0 4.1 Wyoming Stations used: IU.RSSD IW.DLMT IW.FLWY IW.FXWY IW.IMW IW.MFID IW.MOOW IW.PLID IW.REDW IW.SNOW IW.TPAW TA.H17A TA.H19A TA.H21A TA.H22A TA.I19A TA.I20A TA.I21A TA.I25A TA.J19A TA.K25A TA.N23A US.BOZ US.BW06 US.DUG US.MSO US.RLMT UU.BGU UU.HVU UU.NOQ UU.SPU UU.TCU WY.YHB WY.YUF XV.BB3 XV.BH1A XV.BH1B XV.BH2A XV.BH2C XV.BH2E XV.BH3A XV.BH4A XV.BHM2 XV.BHM7 YX.C12 YX.D02 Z2.CFWY Z2.EHMT Z2.IPID Z2.PCWY Filtering commands used: cut o DIST/3.3 -30 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 = 2.26e+22 dyne-cm Mw = 4.17 Z = 9 km Plane Strike Dip Rake NP1 230 85 15 NP2 139 75 175 Principal Axes: Axis Value Plunge Azimuth T 2.26e+22 14 95 N 0.00e+00 74 248 P -2.26e+22 7 3 Moment Tensor: (dyne-cm) Component Value Mxx -2.21e+22 Mxy -3.28e+21 Mxz -3.20e+21 Myy 2.10e+22 Myz 5.17e+21 Mzz 1.02e+21 ------- P ---- ----------- -------- ---------------------------- ##---------------------------- ####---------------------------### ######-----------------------####### ########-------------------########### ##########----------------############## ############------------################ ##############--------#################### ###############-----################## # #################-#################### T # ################--#################### # #############------##################### ###########----------################### ########--------------################ #####------------------############# ##----------------------########## -------------------------##### ---------------------------- ---------------------- -------------- Global CMT Convention Moment Tensor: R T P 1.02e+21 -3.20e+21 -5.17e+21 -3.20e+21 -2.21e+22 3.28e+21 -5.17e+21 3.28e+21 2.10e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20100817024955/index.html

Preferred Solution

The preferred solution from an analysis of the surface-wave spectral amplitude radiation pattern, waveform inversion or first motion observations is

      STK = 230
      DIP = 85
     RAKE = 15
       MW = 4.17
       HS = 9.0

The NDK file is 20100817024955.ndk The waveform inversion is preferred.

Magnitudes

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 M_L by application of the respective IASPEI formulae. As a research study, the linear distance term of the IASPEI formula for M_L is adjusted to remove a linear distance trend in residuals to give a regionally defined M_L. The defined M_L 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.

ML Magnitude

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.

Context

The left panel of the next figure presents the focal mechanism for this earthquake (red) in the context of other nearby events (blue) in the SLU Moment Tensor Catalog. The right panel shows the inferred direction of maximum compressive stress and the type of faulting (green is strike-slip, red is normal, blue is thrust; oblique is shown by a combination of colors). Thus context plot is useful for assessing the appropriateness of the moment tensor of this event.

Waveform Inversion using wvfgrd96

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.

Location of broadband stations used for waveform inversion

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 -30 o DIST/3.3 +50
rtr
taper w 0.1
hp c 0.03 n 3 
lp c 0.10 n 3

The results of this grid search are as follow:

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    1.0   235    85     0   3.73 0.3658
WVFGRD96    2.0    55    90    -5   3.88 0.4948
WVFGRD96    3.0    50    85   -20   3.96 0.5454
WVFGRD96    4.0   230    85    25   4.01 0.5854
WVFGRD96    5.0   230    85    20   4.04 0.6142
WVFGRD96    6.0    50    90   -20   4.07 0.6358
WVFGRD96    7.0   230    85    15   4.11 0.6555
WVFGRD96    8.0   230    85    20   4.15 0.6676
WVFGRD96    9.0   230    85    15   4.17 0.6680
WVFGRD96   10.0    50    85   -15   4.19 0.6637
WVFGRD96   11.0    50    85   -10   4.21 0.6560
WVFGRD96   12.0    50    85   -10   4.22 0.6452
WVFGRD96   13.0    50    85   -10   4.24 0.6315
WVFGRD96   14.0    50    80    -5   4.25 0.6163
WVFGRD96   15.0    50    80    -5   4.27 0.6006
WVFGRD96   16.0    50    80    -5   4.28 0.5834
WVFGRD96   17.0    50    80    -5   4.29 0.5661
WVFGRD96   18.0    50    80    -5   4.29 0.5470
WVFGRD96   19.0    55    85     5   4.29 0.5288
WVFGRD96   20.0    55    85     5   4.30 0.5111
WVFGRD96   21.0    55    85     5   4.31 0.4935
WVFGRD96   22.0    55    85     5   4.31 0.4775
WVFGRD96   23.0    55    85    10   4.32 0.4627
WVFGRD96   24.0    55    85    10   4.32 0.4489
WVFGRD96   25.0    55    85    10   4.33 0.4367
WVFGRD96   26.0    50    80    -5   4.33 0.4250
WVFGRD96   27.0    50    80   -10   4.33 0.4165
WVFGRD96   28.0    50    80   -10   4.33 0.4112
WVFGRD96   29.0    50    80   -10   4.34 0.4062

The best solution is

WVFGRD96    9.0   230    85    15   4.17 0.6680

The mechanism corresponding to the best fit is

Figure 1. Waveform inversion focal mechanism

The best fit as a function of depth is given in the following figure:

Figure 2. Depth sensitivity for waveform mechanism

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 -30 o DIST/3.3 +50
rtr
taper w 0.1
hp c 0.03 n 3 
lp c 0.10 n 3

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.

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:

The origin time and epicentral distance are incorrect
The velocity model used for the inversion is incorrect
The velocity model used to define the P-arrival time is not the same as the velocity model used for the waveform inversion (assuming that the initial trace alignment is based on the P arrival time)

Assuming only a mislocation, the time shifts are fit to a functional form:

 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.

Velocity Model

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

Last Changed Sat Apr 27 01:01:35 PM CDT 2024