Location

2011/03/01 16:03:05 35.239 -92.390 5.1 3.50 Arkansas

Arrival Times (from USGS)

Arrival time list

Felt Map

USGS Felt map for this earthquake

USGS Felt reports main page

Focal Mechanism

 USGS/SLU Moment Tensor Solution
 ENS  2011/03/01 16:03:05:0  35.24  -92.39   5.1 3.5 Arkansas
 
 Stations used:
   AG.FCAR AG.WHAR NM.UALR NM.X102 TA.U38A TA.U39A TA.U40A 
   TA.V39A TA.W38A TA.W39A TA.W40A TA.X40A 
 
 Filtering commands used:
   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 = 1.24e+21 dyne-cm
  Mw = 3.33 
  Z  = 3 km
  Plane   Strike  Dip  Rake
   NP1       24    81   -155
   NP2      290    65   -10
  Principal Axes:
   Axis    Value   Plunge  Azimuth
    T   1.24e+21     11     155
    N   0.00e+00     63      43
    P  -1.24e+21     24     250

 Moment Tensor: (dyne-cm)
    Component   Value
       Mxx     8.60e+20
       Mxy    -7.98e+20
       Mxz    -4.66e+19
       Myy    -6.95e+20
       Myz     5.34e+20
       Mzz    -1.66e+20
                                                     
                                                     
                                                     
                                                     
                     ##############                  
                 ###################---              
              ######################------           
             #######################-------          
           ########################----------        
          ########################------------       
         ####-------##############-------------      
        ---------------------####---------------     
        ------------------------#---------------     
       -------------------------#####------------    
       ------------------------#########---------    
       -----------------------############-------    
       ----------------------###############-----    
        ----   -------------##################--     
        ---- P ------------####################-     
         ---   -----------#####################      
          ---------------#####################       
           -------------#####################        
             ----------####################          
              --------############   #####           
                 ----############# T ##              
                     #############                   
                                                     
                                                     
                                                     
 Global CMT Convention Moment Tensor:
      R          T          P
 -1.66e+20  -4.66e+19  -5.34e+20 
 -4.66e+19   8.60e+20   7.98e+20 
 -5.34e+20   7.98e+20  -6.95e+20 


Details of the solution is found at

http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20110301160305/index.html
        

Preferred Solution

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

      STK = 290
      DIP = 65
     RAKE = -10
       MW = 3.33
       HS = 3.0

The NDK file is 20110301160305.ndk The waveform inversion is preferred.

Moment Tensor Comparison

The following compares this source inversion to others
SLU
SLUFM
 USGS/SLU Moment Tensor Solution
 ENS  2011/03/01 16:03:05:0  35.24  -92.39   5.1 3.5 Arkansas
 
 Stations used:
   AG.FCAR AG.WHAR NM.UALR NM.X102 TA.U38A TA.U39A TA.U40A 
   TA.V39A TA.W38A TA.W39A TA.W40A TA.X40A 
 
 Filtering commands used:
   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 = 1.24e+21 dyne-cm
  Mw = 3.33 
  Z  = 3 km
  Plane   Strike  Dip  Rake
   NP1       24    81   -155
   NP2      290    65   -10
  Principal Axes:
   Axis    Value   Plunge  Azimuth
    T   1.24e+21     11     155
    N   0.00e+00     63      43
    P  -1.24e+21     24     250

 Moment Tensor: (dyne-cm)
    Component   Value
       Mxx     8.60e+20
       Mxy    -7.98e+20
       Mxz    -4.66e+19
       Myy    -6.95e+20
       Myz     5.34e+20
       Mzz    -1.66e+20
                                                     
                                                     
                                                     
                                                     
                     ##############                  
                 ###################---              
              ######################------           
             #######################-------          
           ########################----------        
          ########################------------       
         ####-------##############-------------      
        ---------------------####---------------     
        ------------------------#---------------     
       -------------------------#####------------    
       ------------------------#########---------    
       -----------------------############-------    
       ----------------------###############-----    
        ----   -------------##################--     
        ---- P ------------####################-     
         ---   -----------#####################      
          ---------------#####################       
           -------------#####################        
             ----------####################          
              --------############   #####           
                 ----############# T ##              
                     #############                   
                                                     
                                                     
                                                     
 Global CMT Convention Moment Tensor:
      R          T          P
 -1.66e+20  -4.66e+19  -5.34e+20 
 -4.66e+19   8.60e+20   7.98e+20 
 -5.34e+20   7.98e+20  -6.95e+20 


Details of the solution is found at

http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20110301160305/index.html
	


First motions and takeoff angles from an elocate run.

Magnitudes

mLg Magnitude


(a) mLg computed using the IASPEI formula; (b) mLg residuals ; the values used for the trimmed mean are indicated.

ML Magnitude


(a) ML computed using the IASPEI formula for Horizontal components; (b) 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.


(a) ML computed using the IASPEI formula for Vertical components (research); (b) 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.

Context

The next figure presents the focal mechanism for this earthquake (red) in the context of other events (blue) in the SLU Moment Tensor Catalog which are within ± 0.5 degrees of the new event. This comparison is shown in the left panel of the figure. 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).

Waveform Inversion

The focal mechanism was determined using broadband seismic waveforms. The location of the event and the and stations used for 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 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 0.03 n 3
lp c 0.10 n 3
br c 0.12 0.25 n 4 p 2
The results of this grid search from 0.5 to 19 km depth are as follow:

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    0.5   290    75   -20   3.24 0.5885
WVFGRD96    1.0   290    75   -20   3.26 0.6168
WVFGRD96    2.0   290    65   -10   3.31 0.6519
WVFGRD96    3.0   290    65   -10   3.33 0.6583
WVFGRD96    4.0   115    90   -10   3.33 0.6553
WVFGRD96    5.0   115    90   -10   3.34 0.6483
WVFGRD96    6.0   295    75    15   3.35 0.6450
WVFGRD96    7.0   295    75    15   3.36 0.6412
WVFGRD96    8.0   295    75    15   3.37 0.6402
WVFGRD96    9.0   295    75    15   3.38 0.6395
WVFGRD96   10.0   295    70    15   3.39 0.6378
WVFGRD96   11.0   295    70    15   3.40 0.6364
WVFGRD96   12.0   295    70    15   3.41 0.6321
WVFGRD96   13.0   295    65    15   3.42 0.6295
WVFGRD96   14.0   295    65    15   3.43 0.6261
WVFGRD96   15.0   295    60    15   3.44 0.6251
WVFGRD96   16.0   295    65    10   3.44 0.6224
WVFGRD96   17.0   295    60    10   3.45 0.6201
WVFGRD96   18.0   295    60    10   3.46 0.6185
WVFGRD96   19.0   295    60    10   3.47 0.6159
WVFGRD96   20.0   295    55    10   3.49 0.6139
WVFGRD96   21.0   295    55    10   3.49 0.6124
WVFGRD96   22.0   295    55    10   3.50 0.6093
WVFGRD96   23.0   295    55    10   3.51 0.6053
WVFGRD96   24.0   295    50    10   3.52 0.6028
WVFGRD96   25.0   295    50    10   3.53 0.6000
WVFGRD96   26.0   295    50    15   3.53 0.5958
WVFGRD96   27.0   295    50    15   3.54 0.5904
WVFGRD96   28.0   295    55    10   3.53 0.5851
WVFGRD96   29.0   295    55    10   3.54 0.5810

The best solution is

WVFGRD96    3.0   290    65   -10   3.33 0.6583

The mechanism correspond 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 and because the velocity model used in the predictions may not be perfect. 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 0.03 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
Focal mechanism sensitivity at the preferred depth. The red color indicates a very good fit to thewavefroms. 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.

Discussion

Acknowledgements

Thanks also to the many seismic network operators whose dedication make this effort possible: University of Nevada Reno, University of Alaska, University of Washington, Oregon State University, University of Utah, Montana Bureas of Mines, UC Berkely, Caltech, UC San Diego, Saint Louis University, University of Memphis, Lamont Doherty Earth Observatory, the Iris stations and the Transportable Array of EarthScope.

Velocity Model

The CUS model used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows:

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 

Quality Control

Here we tabulate the reasons for not using certain digital data sets

The following stations did not have a valid response files:

Last Changed Sun Dec 6 19:30:43 CST 2015