2009/03/27 02:58:40 61.01 -138.41 1.0 5.0 Yukon, Canada (NRCAN)
2009/03/27 02:58:39 61.0820 -138.4780 10.0 5.10 Yukon, Canada (USGS/NEIC)
USGS Felt map for this earthquake
USGS/SLU Moment Tensor Solution ENS 2009/03/27 02:58:38:9 61.01 -138.41 10.0 5.0 Yukon, Canada Stations used: AK.BMR AK.DIV AK.DOT AK.PAX AK.PNL AT.PMR CN.DAWY CN.DLBC CN.WHY Filtering commands used: hp c 0.02 n 3 lp c 0.06 n 3 Best Fitting Double Couple Mo = 3.24e+23 dyne-cm Mw = 4.94 Z = 13 km Plane Strike Dip Rake NP1 285 70 75 NP2 143 25 125 Principal Axes: Axis Value Plunge Azimuth T 3.24e+23 62 172 N 0.00e+00 14 290 P -3.24e+23 24 27 Moment Tensor: (dyne-cm) Component Value Mxx -1.48e+23 Mxy -1.18e+23 Mxz -2.39e+23 Myy -5.28e+22 Myz -3.43e+22 Mzz 2.01e+23 -------------- ---------------------- #------------------- ----- #-------------------- P ------ ##--------------------- -------- ##---------------------------------- ##------------------------------------ ###-#########--------------------------- ---###################------------------ ----#########################------------- ----#############################--------- ----################################------ -----#################################---- -----############## #################- -----############## T ################## ------############ ################# ------############################## -------########################### -------####################### ---------################### ----------###########- -------------- Global CMT Convention Moment Tensor: R T P 2.01e+23 -2.39e+23 3.43e+22 -2.39e+23 -1.48e+23 1.18e+23 3.43e+22 1.18e+23 -5.28e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20090327025839/index.html |
STK = 285 DIP = 70 RAKE = 75 MW = 4.94 HS = 13.0
Only the waveform inversion was applied. The initial USGS solution did not use the vertical and radial at the station DIV. Using the bandpass fitler band of 0.02 - 0.05 Hz,The solution was
H=17 km STK=285 DIP=80 RAKE=80 MW=4.85 FIT=0.7191.
When using slightly high frequency, e.g., 0.02 - 0.06 Hz, we get
H=13.0 km STK=285 DIP=70 RAKE=75 MW=4.94 FIT=0.8208. This is the final solution. We also use the NRCAN location.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2009/03/27 02:58:38:9 61.01 -138.41 10.0 5.0 Yukon, Canada Stations used: AK.BMR AK.DIV AK.DOT AK.PAX AK.PNL AT.PMR CN.DAWY CN.DLBC CN.WHY Filtering commands used: hp c 0.02 n 3 lp c 0.06 n 3 Best Fitting Double Couple Mo = 3.24e+23 dyne-cm Mw = 4.94 Z = 13 km Plane Strike Dip Rake NP1 285 70 75 NP2 143 25 125 Principal Axes: Axis Value Plunge Azimuth T 3.24e+23 62 172 N 0.00e+00 14 290 P -3.24e+23 24 27 Moment Tensor: (dyne-cm) Component Value Mxx -1.48e+23 Mxy -1.18e+23 Mxz -2.39e+23 Myy -5.28e+22 Myz -3.43e+22 Mzz 2.01e+23 -------------- ---------------------- #------------------- ----- #-------------------- P ------ ##--------------------- -------- ##---------------------------------- ##------------------------------------ ###-#########--------------------------- ---###################------------------ ----#########################------------- ----#############################--------- ----################################------ -----#################################---- -----############## #################- -----############## T ################## ------############ ################# ------############################## -------########################### -------####################### ---------################### ----------###########- -------------- Global CMT Convention Moment Tensor: R T P 2.01e+23 -2.39e+23 3.43e+22 -2.39e+23 -1.48e+23 1.18e+23 3.43e+22 1.18e+23 -5.28e+22 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20090327025839/index.html |
Moment tensor inversion summary for event 2009/03/27 02:58 Date: 2009/03/27 Time: 02:58 (UTC) Region: Yukon Territory Mw=5.0 Location: Lat. 60.9670; Lon. -138.3647; Depth 15 km (Best-fitting depth from moment tensor inversion) Solution quality: good; Number of stations = 6 Best Double Couple: strike dip rake Plane 1: 297.0 49.6 91.3 Plane 2: 115.0 40.4 88.4 Moment Tensor Parameters: Mo = 3.09237e+23 dyn-cm Mxx = -2.50; Mxy = -1.29; Mxz = -0.42 Myy = -0.48; Myz = -0.26; Mzz = 2.98 Principal Axes: value azimuth plunge T: 3.02 218.67 85.31 N: 0.15 116.15 1.02 P: -3.17 26.07 4.58 |
******************************************************************** This is a preliminary centroid-moment-tensor (CMT) solution for an earthquake occurred in West Canada or adjacent regions. To best view this message, please set the font to Courier New, 10 points, and single spacing. If you have any questions, please contact pgc_info@pgc.nrcan.gc.ca ******************************************************************** CNSN Earthquake Report: origin time: 2009 3 27 2: 58: 39.00 hypocenter: 61.08 -138.48 17.00 km ML: 4.8 CNSN CMT Solution: -1.6526368 -1.2456304 -0.0766009 -1.2456304 -0.2123804 -0.3621007 x 1.0E+16 Nt-m -0.0766009 -0.3621007 2.1155586 centroid depth: 14 km seismic moment: 0.23E+17 Nt-m Mw: 4.85 CLVD component: 30.6% Iso. component: 3.5% average misfit: 0.405 ( A class-B3 solution. The fit is good. ) Best Double Couple Solutions : nodal plane(1) strike / dip / slip: 111 / 43 / 76 nodal plane(2) strike / dip / slip: 309 / 49 / 102 ------------ ----------------- P -------------------- --- ###############--------------- ####################------------ ########################---------- --############ ##########--------- ---########### T ############------- ----########## #############------ ------#########################----- -------#######################---- ---------#####################-# --------------###########----# -------------------------- -------------------- ------------ |
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.
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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 0.02 n 3 lp c 0.06 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 0.5 260 65 -90 4.82 0.5037 WVFGRD96 1.0 125 45 90 4.76 0.4917 WVFGRD96 2.0 90 85 -85 5.05 0.5391 WVFGRD96 3.0 290 90 80 4.98 0.6036 WVFGRD96 4.0 290 90 80 4.94 0.6502 WVFGRD96 5.0 290 85 80 4.92 0.6853 WVFGRD96 6.0 290 85 80 4.91 0.7165 WVFGRD96 7.0 295 80 80 4.90 0.7458 WVFGRD96 8.0 290 75 80 4.91 0.7717 WVFGRD96 9.0 290 70 80 4.92 0.7955 WVFGRD96 10.0 290 70 80 4.94 0.8062 WVFGRD96 11.0 290 70 80 4.94 0.8166 WVFGRD96 12.0 280 70 75 4.94 0.8208 WVFGRD96 13.0 285 70 75 4.94 0.8211 WVFGRD96 14.0 285 70 75 4.93 0.8164 WVFGRD96 15.0 285 70 75 4.93 0.8090 WVFGRD96 16.0 285 70 75 4.93 0.7986 WVFGRD96 17.0 285 70 75 4.93 0.7862 WVFGRD96 18.0 285 70 75 4.93 0.7721 WVFGRD96 19.0 285 75 75 4.93 0.7581 WVFGRD96 20.0 290 75 80 4.96 0.7452 WVFGRD96 21.0 290 75 80 4.96 0.7301 WVFGRD96 22.0 290 80 80 4.96 0.7144 WVFGRD96 23.0 290 80 80 4.96 0.6997 WVFGRD96 24.0 295 80 80 4.97 0.6844 WVFGRD96 25.0 295 85 80 4.97 0.6689 WVFGRD96 26.0 295 85 80 4.98 0.6543 WVFGRD96 27.0 295 85 80 4.98 0.6391 WVFGRD96 28.0 115 90 -75 4.99 0.6241 WVFGRD96 29.0 295 90 75 4.99 0.6097
The best solution is
WVFGRD96 13.0 285 70 75 4.94 0.8211
The mechanism correspond to the best fit is
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The best fit as a function of depth is given in the following figure:
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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 componnet is plotted to the same scale and peak amplitudes are indicated by the numbers to the left of each trace. The number in black at the rightr of each predicted traces 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 bandpass filter used in the processing and for the display was
hp c 0.02 n 3 lp c 0.06 n 3
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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. |
Should the national backbone of the USGS Advanced National Seismic System (ANSS) be implemented with an interstation separation of 300 km, it is very likely that an earthquake such as this would have been recorded at distances on the order of 100-200 km. This means that the closest station would have information on source depth and mechanism that was lacking here.
Dr. Harley Benz, USGS, provided the USGS USNSN digital data. The digital data used in this study were provided by Natural Resources Canada through their AUTODRM site http://www.seismo.nrcan.gc.ca/nwfa/autodrm/autodrm_req_e.php, and IRIS using their BUD interface.
Thanks also to the many seismic network operators whose dedication make this effort possible: University of Alaska, University of Washington, Oregon State University, University of Utah, Montana Bureas of Mines, UC Berkely, Caltech, UC San Diego, Saint L ouis University, Universityof Memphis, Lamont Doehrty Earth Observatory, Boston College, the Iris stations and the Transportable Array of EarthScope.
The WUS used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows:
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
Here we tabulate the reasons for not using certain digital data sets
The following stations did not have a valid response files:
DATE=Sat Mar 28 12:29:34 CDT 2009