Location

Location ANSS

The ANSS event ID is usp000hwz2 and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/usp000hwz2/executive.

2011/03/13 20:16:21 32.995 -100.767 5.0 3.8 Texas

Focal Mechanism

 USGS/SLU Moment Tensor Solution
 ENS  2011/03/13 20:16:21:0  32.99 -100.77   5.0 3.8 Texas
 
 Stations used:
   IM.TX31 IU.ANMO TA.133A TA.134A TA.135A TA.137A TA.233A 
   TA.234A TA.237A TA.333A TA.334A TA.335A TA.336A TA.433A 
   TA.434A TA.435B TA.533A TA.534A TA.535A TA.633A TA.634A 
   TA.636A TA.832A TA.833A TA.ABTX TA.MSTX TA.S30A TA.TUL1 
   TA.V32A TA.V36A TA.WHTX TA.X34A TA.X35A TA.Y33A TA.Y34A 
   TA.Y35A TA.Y36A TA.Y37A TA.Z33A TA.Z34A TA.Z35A TA.Z36A 
   TA.Z37A US.AMTX US.JCT US.MNTX X4.GC09 X4.GC14 X4.GC15 
   X4.GC18 XR.SC04 XR.SC50 
 
 Filtering commands used:
   hp c 0.02 n 3
   lp c 0.10 n 3
   br c 0.12 0.25 n 4 p 2
 
 Best Fitting Double Couple
  Mo = 6.76e+21 dyne-cm
  Mw = 3.82 
  Z  = 2 km
  Plane   Strike  Dip  Rake
   NP1       70    60   -50
   NP2      191    48   -138
  Principal Axes:
   Axis    Value   Plunge  Azimuth
    T   6.76e+21      7     133
    N   0.00e+00     34     227
    P  -6.76e+21     55      33

 Moment Tensor: (dyne-cm)
    Component   Value
       Mxx     1.54e+21
       Mxy    -4.32e+21
       Mxz    -3.18e+21
       Myy     2.94e+21
       Myz    -1.16e+21
       Mzz    -4.49e+21
                                                     
                                                     
                                                     
                                                     
                     #########-----                  
                 ##########------------              
              ###########-----------------           
             ##########--------------------          
           ###########-----------------------        
          ###########-------------------------       
         ###########-----------   -------------      
        ###########------------ P -------------#     
        ##########-------------   ------------##     
       ###########---------------------------####    
       ###########-------------------------######    
       ##########-------------------------#######    
       ##########----------------------##########    
        #########-------------------############     
        #########---------------################     
         --#######---------####################      
          --------############################       
           --------######################   #        
             ------###################### T          
              ------#####################            
                 ----##################              
                     --############                  
                                                     
                                                     
                                                     
 Global CMT Convention Moment Tensor:
      R          T          P
 -4.49e+21  -3.18e+21   1.16e+21 
 -3.18e+21   1.54e+21   4.32e+21 
  1.16e+21   4.32e+21   2.94e+21 


Details of the solution is found at

http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20110313201621/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 = 70
      DIP = 60
     RAKE = -50
       MW = 3.82
       HS = 2.0

The NDK file is 20110313201621.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 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.

mLg Magnitude


Left: mLg computed using the IASPEI formula. Center: mLg residuals versus epicentral distance ; the values used for the trimmed mean magnitude estimate are indicated. Right: residuals as a function of distance and azimuth.

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:

hp c 0.02 n 3
lp c 0.10 n 3
br c 0.12 0.25 n 4 p 2
The results of this grid search are as follow:

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    0.5    80    70   -35   3.72 0.3825
WVFGRD96    1.0    75    65   -40   3.75 0.3983
WVFGRD96    2.0    70    60   -50   3.82 0.4136
WVFGRD96    3.0    70    65   -55   3.86 0.3980
WVFGRD96    4.0    70    70   -55   3.88 0.3788
WVFGRD96    5.0    80    85   -45   3.85 0.3710
WVFGRD96    6.0   270    70    30   3.83 0.3734
WVFGRD96    7.0   270    70    30   3.83 0.3792
WVFGRD96    8.0   270    70    30   3.84 0.3833
WVFGRD96    9.0   270    70    30   3.84 0.3858
WVFGRD96   10.0   270    70    35   3.86 0.3838
WVFGRD96   11.0    95    65    40   3.87 0.3859
WVFGRD96   12.0    95    65    40   3.88 0.3870
WVFGRD96   13.0    95    65    40   3.88 0.3870
WVFGRD96   14.0    95    65    40   3.89 0.3861
WVFGRD96   15.0    95    65    40   3.90 0.3845
WVFGRD96   16.0    95    65    40   3.91 0.3824
WVFGRD96   17.0    95    65    40   3.91 0.3799
WVFGRD96   18.0    95    65    40   3.92 0.3771
WVFGRD96   19.0   270    70    40   3.93 0.3722
WVFGRD96   20.0    95    65    45   3.96 0.3693
WVFGRD96   21.0    95    65    45   3.97 0.3651
WVFGRD96   22.0    95    65    45   3.98 0.3603
WVFGRD96   23.0   275    65    50   3.99 0.3581
WVFGRD96   24.0   275    65    50   4.00 0.3540
WVFGRD96   25.0   275    65    50   4.01 0.3495
WVFGRD96   26.0   275    65    50   4.02 0.3443
WVFGRD96   27.0   275    65    50   4.03 0.3390
WVFGRD96   28.0   275    65    55   4.04 0.3333
WVFGRD96   29.0    10    60    40   4.00 0.3246

The best solution is

WVFGRD96    2.0    70    60   -50   3.82 0.4136

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

hp c 0.02 n 3
lp c 0.10 n 3
br c 0.12 0.25 n 4 p 2
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:

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 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 
Last Changed Sat Apr 27 12:22:47 PM CDT 2024