Location

Location ANSS

The ANSS event ID is ak0175gzldxl and the event page is at https://earthquake.usgs.gov/earthquakes/eventpage/ak0175gzldxl/executive.

2017/04/29 11:15:48 63.123 -151.166 11.9 4.9 Alaska

Focal Mechanism

USGS/SLU Moment Tensor Solution ENS 2017/04/29 11:15:48:0 63.12 -151.17 11.9 4.9 Alaska Stations used: AK.BPAW AK.BWN AK.CAPN AK.CAST AK.CCB AK.CUT AK.DIV AK.DOT AK.GHO AK.GLB AK.HDA AK.KLU AK.KNK AK.KTH AK.MCK AK.MDM AK.MLY AK.NEA2 AK.PAX AK.PPD AK.PPLA AK.PWL AK.RC01 AK.RIDG AK.RND AK.SAW AK.SCM AK.SCRK AK.SKN AK.SSN AK.SWD AK.TRF AK.WRH AT.MENT AT.PMR AV.ILSW IU.COLA TA.H21K TA.H23K TA.H24K TA.I21K TA.I23K TA.J20K TA.J25K TA.J26L TA.K20K TA.L19K TA.L26K TA.M19K TA.M20K TA.M22K TA.M24K TA.M26K TA.N18K TA.N19K TA.N25K TA.O19K TA.O22K TA.P19K TA.POKR Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 1.93e+23 dyne-cm Mw = 4.79 Z = 14 km Plane Strike Dip Rake NP1 216 85 120 NP2 315 30 10 Principal Axes: Axis Value Plunge Azimuth T 1.93e+23 42 155 N 0.00e+00 29 33 P -1.93e+23 33 282 Moment Tensor: (dyne-cm) Component Value Mxx 8.04e+22 Mxy -1.45e+22 Mxz -1.04e+23 Myy -1.09e+23 Myz 1.28e+23 Mzz 2.90e+22 ############## ###################### ##--------------#########--- ---------------------####----- -------------------------#-------- ------------------------#####------- ------------------------#######------- -----------------------###########------ ----- --------------#############----- ------ P ------------###############------ ------ -----------#################----- -------------------###################---- -----------------#####################---- ---------------######################--- --------------#######################--- ------------########### ##########-- ---------############# T #########-- -------############## #########- ----########################## --########################## ###################### ############## Global CMT Convention Moment Tensor: R T P 2.90e+22 -1.04e+23 -1.28e+23 -1.04e+23 8.04e+22 1.45e+22 -1.28e+23 1.45e+22 -1.09e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20170429111548/index.html

Preferred Solution

      STK = 315
      DIP = 30
     RAKE = 10
       MW = 4.79
       HS = 14.0

The NDK file is 20170429111548.ndk The waveform inversion is preferred.

Moment Tensor Comparison

The following compares this source inversion to those provided by others. The purpose is to look for major differences and also to note slight differences that might be inherent to the processing procedure. For completeness the USGS/SLU solution is repeated from above.

SLU

USGSMT

USGS/SLU Moment Tensor Solution ENS 2017/04/29 11:15:48:0 63.12 -151.17 11.9 4.9 Alaska Stations used: AK.BPAW AK.BWN AK.CAPN AK.CAST AK.CCB AK.CUT AK.DIV AK.DOT AK.GHO AK.GLB AK.HDA AK.KLU AK.KNK AK.KTH AK.MCK AK.MDM AK.MLY AK.NEA2 AK.PAX AK.PPD AK.PPLA AK.PWL AK.RC01 AK.RIDG AK.RND AK.SAW AK.SCM AK.SCRK AK.SKN AK.SSN AK.SWD AK.TRF AK.WRH AT.MENT AT.PMR AV.ILSW IU.COLA TA.H21K TA.H23K TA.H24K TA.I21K TA.I23K TA.J20K TA.J25K TA.J26L TA.K20K TA.L19K TA.L26K TA.M19K TA.M20K TA.M22K TA.M24K TA.M26K TA.N18K TA.N19K TA.N25K TA.O19K TA.O22K TA.P19K TA.POKR Filtering commands used: cut o DIST/3.3 -30 o DIST/3.3 +70 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.07 n 3 Best Fitting Double Couple Mo = 1.93e+23 dyne-cm Mw = 4.79 Z = 14 km Plane Strike Dip Rake NP1 216 85 120 NP2 315 30 10 Principal Axes: Axis Value Plunge Azimuth T 1.93e+23 42 155 N 0.00e+00 29 33 P -1.93e+23 33 282 Moment Tensor: (dyne-cm) Component Value Mxx 8.04e+22 Mxy -1.45e+22 Mxz -1.04e+23 Myy -1.09e+23 Myz 1.28e+23 Mzz 2.90e+22 ############## ###################### ##--------------#########--- ---------------------####----- -------------------------#-------- ------------------------#####------- ------------------------#######------- -----------------------###########------ ----- --------------#############----- ------ P ------------###############------ ------ -----------#################----- -------------------###################---- -----------------#####################---- ---------------######################--- --------------#######################--- ------------########### ##########-- ---------############# T #########-- -------############## #########- ----########################## --########################## ###################### ############## Global CMT Convention Moment Tensor: R T P 2.90e+22 -1.04e+23 -1.28e+23 -1.04e+23 8.04e+22 1.45e+22 -1.28e+23 1.45e+22 -1.09e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20170429111548/index.html

Regional Moment Tensor (Mwr) Moment 2.107e+16 N-m Magnitude 4.8 Mwr Depth 10.0 km Percent DC 94 % Half Duration - Catalog US Data Source US2 Contributor US2 Nodal Planes Plane Strike Dip Rake NP1 317 29 13 NP2 215 84 118 Principal Axes Axis Value Plunge Azimuth T 2.075e+16 N-m 44 153 N 0.061e+16 N-m 28 32 P -2.137e+16 N-m 33 282

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

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 0.03 n 3 
lp c 0.07 n 3 

           DEPTH  STK   DIP  RAKE   MW    FIT
WVFGRD96    1.0   205    45    90   4.47 0.3631
WVFGRD96    2.0    20    45    90   4.58 0.4629
WVFGRD96    3.0   190    35    80   4.63 0.3969
WVFGRD96    4.0   315    30    10   4.62 0.4585
WVFGRD96    5.0   315    25    10   4.66 0.5375
WVFGRD96    6.0   315    30    10   4.66 0.6025
WVFGRD96    7.0   315    30    10   4.67 0.6536
WVFGRD96    8.0   315    25    10   4.74 0.6898
WVFGRD96    9.0   315    25    10   4.75 0.7278
WVFGRD96   10.0   315    30    10   4.76 0.7565
WVFGRD96   11.0   315    30    10   4.77 0.7757
WVFGRD96   12.0   315    30    10   4.77 0.7873
WVFGRD96   13.0   315    30    10   4.78 0.7928
WVFGRD96   14.0   315    30    10   4.79 0.7934
WVFGRD96   15.0   310    35     5   4.80 0.7907
WVFGRD96   16.0   310    35     5   4.80 0.7846
WVFGRD96   17.0   310    35     5   4.81 0.7756
WVFGRD96   18.0   310    35     5   4.82 0.7641
WVFGRD96   19.0   310    35     5   4.82 0.7509
WVFGRD96   20.0   305    35    -5   4.83 0.7364
WVFGRD96   21.0   315    30    10   4.84 0.7212
WVFGRD96   22.0   305    30    -5   4.84 0.7051
WVFGRD96   23.0   305    30    -5   4.85 0.6881
WVFGRD96   24.0   305    30    -5   4.85 0.6706
WVFGRD96   25.0   305    30    -5   4.86 0.6524
WVFGRD96   26.0   305    30    -5   4.86 0.6335
WVFGRD96   27.0   305    30    -5   4.87 0.6143
WVFGRD96   28.0   305    30    -5   4.87 0.5949
WVFGRD96   29.0   305    30    -5   4.87 0.5751

The best solution is

WVFGRD96   14.0   315    30    10   4.79 0.7934

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 0.03 n 3 
lp c 0.07 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)

 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