Location

Location ANSS

The ANSS event ID is nn00466648 and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/nn00466648/executive.

2014/11/07 08:05:54 41.880 -119.630 0.0 4.7 Nevada

Focal Mechanism

USGS/SLU Moment Tensor Solution ENS 2014/11/07 08:05:54:0 41.88 -119.63 0.0 4.7 Nevada Stations used: BK.SAO BK.WDC IM.NV31 IU.COR IW.MFID IW.PLID LB.TPH NC.AFD NC.KBO NC.KCPB NC.KEB NC.KHMB NC.KMR NC.KRMB NC.MDPB NN.BEK NN.KVN NN.LHV NN.OMMB NN.PAH NN.PNT NN.REDF NN.RUB NN.RYN NN.VCN NN.WAK NN.WDEM TA.R11A UO.PINE US.BMO US.ELK US.HAWA US.HLID UU.BGU UU.HVU UW.BLOW UW.BRAN UW.CCRK UW.DDRF UW.IRON UW.IZEE UW.LON UW.PHIN UW.TUCA UW.UMAT UW.WOLL UW.YACT Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.02 n 3 lp c 0.06 n 3 Best Fitting Double Couple Mo = 8.13e+22 dyne-cm Mw = 4.54 Z = 10 km Plane Strike Dip Rake NP1 25 65 -75 NP2 173 29 -119 Principal Axes: Axis Value Plunge Azimuth T 8.13e+22 19 104 N 0.00e+00 14 199 P -8.13e+22 67 322 Moment Tensor: (dyne-cm) Component Value Mxx -3.86e+21 Mxy -1.08e+22 Mxz -2.94e+22 Myy 6.40e+22 Myz 4.20e+22 Mzz -6.01e+22 ##------------ ###-----------------## ####-------------------##### ####---------------------##### #####----------------------####### #####----------------------######### #####-----------------------########## ######--------- -----------########### #####---------- P ----------############ ######---------- ----------############# ######----------------------############## ######----------------------############## ######---------------------######### ### ######-------------------########## T ## ######------------------########### ## ######----------------################ ######-------------################# ######-----------################# ######-------################# ######----################## #####-################ -----######### Global CMT Convention Moment Tensor: R T P -6.01e+22 -2.94e+22 -4.20e+22 -2.94e+22 -3.86e+21 1.08e+22 -4.20e+22 1.08e+22 6.40e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20141107080554/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 = 25
      DIP = 65
     RAKE = -75
       MW = 4.54
       HS = 10.0

The NDK file is 20141107080554.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 +70
rtr
taper w 0.1
hp c 0.02 n 3 
lp c 0.06 n 3

The results of this grid search are as follow:

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    1.0   225    60   -10   4.24 0.4537
WVFGRD96    2.0   225    55   -10   4.32 0.4920
WVFGRD96    3.0   225    80   -35   4.35 0.4933
WVFGRD96    4.0    40    75   -55   4.44 0.5235
WVFGRD96    5.0    40    80   -60   4.44 0.5609
WVFGRD96    6.0    35    75   -65   4.45 0.5921
WVFGRD96    7.0    35    75   -65   4.44 0.6132
WVFGRD96    8.0    30    70   -70   4.53 0.6441
WVFGRD96    9.0    30    70   -70   4.53 0.6585
WVFGRD96   10.0    25    65   -75   4.54 0.6641
WVFGRD96   11.0    25    65   -75   4.54 0.6632
WVFGRD96   12.0    30    65   -70   4.53 0.6563
WVFGRD96   13.0    50    90   -40   4.51 0.6471
WVFGRD96   14.0    50    90   -40   4.51 0.6439
WVFGRD96   15.0    50    90   -40   4.52 0.6376
WVFGRD96   16.0    50    90   -40   4.52 0.6291
WVFGRD96   17.0    50    90   -35   4.53 0.6191
WVFGRD96   18.0    50    90   -35   4.54 0.6083
WVFGRD96   19.0    50    90   -35   4.54 0.5960
WVFGRD96   20.0   230    90    35   4.55 0.5828
WVFGRD96   21.0    50    90   -35   4.55 0.5690
WVFGRD96   22.0   230    90    35   4.56 0.5545
WVFGRD96   23.0   230    90    35   4.56 0.5396
WVFGRD96   24.0   230    90    35   4.57 0.5245
WVFGRD96   25.0    50    90   -35   4.57 0.5094
WVFGRD96   26.0   230    90    35   4.57 0.4943
WVFGRD96   27.0   230    90    30   4.59 0.4794
WVFGRD96   28.0   230    85    30   4.59 0.4650
WVFGRD96   29.0   230    85    30   4.59 0.4508

The best solution is

WVFGRD96   10.0    25    65   -75   4.54 0.6641

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 +70
rtr
taper w 0.1
hp c 0.02 n 3 
lp c 0.06 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 02:39:38 AM CDT 2024