Location

Location ANSS

The ANSS event ID is ci10589037 and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ci10589037/executive.

2010/04/08 16:44:26 32.165 -115.268 10.0 5.29 Baja California, Mexico

Focal Mechanism

 USGS/SLU Moment Tensor Solution
 ENS  2010/04/08 16:44:26:0  32.17 -115.27  10.0 5.3 Baja California, Mexico
 
 Stations used:
   AE.X16A AZ.BZN AZ.CPE AZ.CRY AZ.FRD AZ.HWB AZ.KNW AZ.LVA2 
   AZ.MONP2 AZ.RDM AZ.SMER AZ.SND AZ.SOL AZ.TRO AZ.WMC CI.ADO 
   CI.ARV CI.BAK CI.BAR CI.BBR CI.BFS CI.CIA CI.DEC CI.DGR 
   CI.DJJ CI.EDW2 CI.GLA CI.ISA CI.LRL CI.MUR CI.MWC CI.NEE2 
   CI.OSI CI.PASC CI.PLM CI.RPV CI.SCI2 CI.SCZ2 CI.SDD CI.SLA 
   CI.SMM CI.SVD CI.SWS CI.VCS CI.VES CI.VTV II.PFO TA.109C 
   TA.113A TA.Y14A US.WUAZ 
 
 Filtering commands used:
   cut o DIST/3.3 -30 o DIST/3.3 +50
   rtr
   taper w 0.1
   hp c 0.02 n 3 
   lp c 0.05 n 3 
 
 Best Fitting Double Couple
  Mo = 1.16e+24 dyne-cm
  Mw = 5.31 
  Z  = 12 km
  Plane   Strike  Dip  Rake
   NP1      306    76   164
   NP2       40    75    15
  Principal Axes:
   Axis    Value   Plunge  Azimuth
    T   1.16e+24     21     263
    N   0.00e+00     69      84
    P  -1.16e+24      0     353

 Moment Tensor: (dyne-cm)
    Component   Value
       Mxx    -1.13e+24
       Mxy     2.62e+23
       Mxz    -5.51e+22
       Myy     9.79e+23
       Myz    -3.86e+23
       Mzz     1.50e+23
                                                     
                                                     
                                                     
                                                     
                     --- P --------                  
                 -------   ------------              
              ---------------------------#           
             ----------------------------##          
           #----------------------------#####        
          ########---------------------#######       
         #############----------------#########      
        #################------------###########     
        ####################--------############     
       #######################-----##############    
       ##########################-###############    
       ###   ###################---##############    
       ### T ##################------############    
        ##   ################----------#########     
        ###################--------------#######     
         ################-----------------#####      
          #############---------------------##       
           ##########------------------------        
             ######------------------------          
              #---------------------------           
                 ----------------------              
                     --------------                  
                                                     
                                                     
                                                     
 Global CMT Convention Moment Tensor:
      R          T          P
  1.50e+23  -5.51e+22   3.86e+23 
 -5.51e+22  -1.13e+24  -2.62e+23 
  3.86e+23  -2.62e+23   9.79e+23 


Details of the solution is found at

http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20100408164426/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 = 40
      DIP = 75
     RAKE = 15
       MW = 5.31
       HS = 12.0

The NDK file is 20100408164426.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.

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 0.02 n 3 
lp c 0.05 n 3 
The results of this grid search are as follow:

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    1.0   215    90     0   5.02 0.5055
WVFGRD96    2.0   215    90     0   5.10 0.6306
WVFGRD96    3.0   215    90     5   5.13 0.6730
WVFGRD96    4.0   215    90     5   5.16 0.7041
WVFGRD96    5.0    35    80   -15   5.19 0.7300
WVFGRD96    6.0   215    90    10   5.20 0.7503
WVFGRD96    7.0   215    90    10   5.22 0.7684
WVFGRD96    8.0    35    75   -15   5.26 0.7864
WVFGRD96    9.0    35    75   -15   5.27 0.7939
WVFGRD96   10.0    40    80    15   5.28 0.7968
WVFGRD96   11.0    40    75    15   5.29 0.8003
WVFGRD96   12.0    40    75    15   5.31 0.8016
WVFGRD96   13.0    40    75    15   5.32 0.8008
WVFGRD96   14.0    40    75    15   5.33 0.7980
WVFGRD96   15.0    35    65   -10   5.35 0.7938
WVFGRD96   16.0    35    65   -10   5.36 0.7884
WVFGRD96   17.0    35    65   -10   5.37 0.7817
WVFGRD96   18.0    35    65   -10   5.37 0.7738
WVFGRD96   19.0    35    70   -10   5.37 0.7651
WVFGRD96   20.0    35    70   -10   5.38 0.7555
WVFGRD96   21.0    35    70   -10   5.39 0.7449
WVFGRD96   22.0    35    70   -10   5.40 0.7337
WVFGRD96   23.0   215    65    -5   5.41 0.7221
WVFGRD96   24.0   215    65    -5   5.42 0.7098
WVFGRD96   25.0   215    60    -5   5.44 0.6975
WVFGRD96   26.0   215    60    -5   5.45 0.6844
WVFGRD96   27.0   220    65    10   5.44 0.6710
WVFGRD96   28.0    40    35     5   5.52 0.6607
WVFGRD96   29.0    40    35     5   5.53 0.6490

The best solution is

WVFGRD96   12.0    40    75    15   5.31 0.8016

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 0.02 n 3 
lp c 0.05 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:

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 11:49:02 AM CDT 2024