2009/04/30 04:54:57 58.9830 -151.2980 50.0 4.80 KODIAK ISLAND REGION, ALASKA
USGS Felt map for this earthquake
USGS/SLU Moment Tensor Solution ENS 2009/04/30 04:54:57:0 58.98 -151.30 50.0 4.8 KODIAK ISLAND REGION, ALASKA Stations used: AK.BMR AK.BRLK AK.DIV AK.EYAK AK.MCK AK.PAX AK.RAG AK.RC01 AK.SWD AK.TRF AT.MID AT.OHAK AT.PMR AT.SVW2 Filtering commands used: hp c 0.0200 n 3 lp c 0.050 n 3 Best Fitting Double Couple Mo = 2.82e+23 dyne-cm Mw = 4.90 Z = 45 km Plane Strike Dip Rake NP1 184 66 -97 NP2 20 25 -75 Principal Axes: Axis Value Plunge Azimuth T 2.82e+23 21 279 N 0.00e+00 6 186 P -2.82e+23 68 80 Moment Tensor: (dyne-cm) Component Value Mxx 4.58e+21 Mxy -4.34e+22 Mxz -2.27e+21 Myy 2.04e+23 Myz -1.87e+23 Mzz -2.09e+23 #######------- ##########-----------# ############-------------### ############----------------## #############------------------### ##############-------------------### ##############--------------------#### ###############---------------------#### ## #########----------------------#### ### T #########---------- ---------##### ### #########---------- P ---------##### ###############---------- ---------##### ###############----------------------##### ##############---------------------##### ##############--------------------###### #############--------------------##### ############------------------###### ############----------------###### ##########--------------###### ##########-----------####### ########-------####### ############## Global CMT Convention Moment Tensor: R T P -2.09e+23 -2.27e+21 1.87e+23 -2.27e+21 4.58e+21 4.34e+22 1.87e+23 4.34e+22 2.04e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20090430045457/index.html |
STK = 20 DIP = 25 RAKE = -75 MW = 4.90 HS = 45.0
The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution ENS 2009/04/30 04:54:57:0 58.98 -151.30 50.0 4.8 KODIAK ISLAND REGION, ALASKA Stations used: AK.BMR AK.BRLK AK.DIV AK.EYAK AK.MCK AK.PAX AK.RAG AK.RC01 AK.SWD AK.TRF AT.MID AT.OHAK AT.PMR AT.SVW2 Filtering commands used: hp c 0.0200 n 3 lp c 0.050 n 3 Best Fitting Double Couple Mo = 2.82e+23 dyne-cm Mw = 4.90 Z = 45 km Plane Strike Dip Rake NP1 184 66 -97 NP2 20 25 -75 Principal Axes: Axis Value Plunge Azimuth T 2.82e+23 21 279 N 0.00e+00 6 186 P -2.82e+23 68 80 Moment Tensor: (dyne-cm) Component Value Mxx 4.58e+21 Mxy -4.34e+22 Mxz -2.27e+21 Myy 2.04e+23 Myz -1.87e+23 Mzz -2.09e+23 #######------- ##########-----------# ############-------------### ############----------------## #############------------------### ##############-------------------### ##############--------------------#### ###############---------------------#### ## #########----------------------#### ### T #########---------- ---------##### ### #########---------- P ---------##### ###############---------- ---------##### ###############----------------------##### ##############---------------------##### ##############--------------------###### #############--------------------##### ############------------------###### ############----------------###### ##########--------------###### ##########-----------####### ########-------####### ############## Global CMT Convention Moment Tensor: R T P -2.09e+23 -2.27e+21 1.87e+23 -2.27e+21 4.58e+21 4.34e+22 1.87e+23 4.34e+22 2.04e+23 Details of the solution is found at http://www.eas.slu.edu/eqc/eqc_mt/MECH.NA/20090430045457/index.html |
Moment tensor inversion summary for event 2009/04/30 04:54 Date: 2009/04/30 Time: 04:54 (UTC) Region: Kodiak Island Region of Alaska Mw=4.9 Location: Lat. 58.9833; Lon. -151.2986; Depth 35 km (Best-fitting depth from moment tensor inversion) Solution quality: good; Number of stations = 5 Best Double Couple: strike dip rake Plane 1: 194.5 61.2 -91.4 Plane 2: 17.5 28.8 -87.4 Moment Tensor Parameters: Mo = 2.76043e+23 dyn-cm Mxx = 0.40; Mxy = -0.49; Mxz = 0.31 Myy = 1.95; Myz = -1.37; Mzz = -2.35 Principal Axes: value azimuth plunge T: 2.51 285.56 16.17 N: 0.26 195.19 1.26 P: -2.76 100.85 73.77 |
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 0.0200 n 3 lp c 0.050 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT WVFGRD96 30.0 0 20 -95 4.65 0.4793 WVFGRD96 31.0 0 20 -95 4.66 0.4873 WVFGRD96 32.0 5 20 -90 4.67 0.4947 WVFGRD96 33.0 5 20 -90 4.67 0.5015 WVFGRD96 34.0 10 20 -85 4.68 0.5073 WVFGRD96 35.0 5 25 -90 4.68 0.5129 WVFGRD96 36.0 10 25 -85 4.69 0.5180 WVFGRD96 37.0 10 25 -85 4.70 0.5226 WVFGRD96 38.0 15 25 -85 4.72 0.5266 WVFGRD96 39.0 20 25 -80 4.73 0.5305 WVFGRD96 40.0 20 25 -75 4.86 0.5285 WVFGRD96 41.0 20 25 -75 4.87 0.5331 WVFGRD96 42.0 20 25 -75 4.88 0.5365 WVFGRD96 43.0 20 25 -75 4.89 0.5389 WVFGRD96 44.0 20 25 -75 4.89 0.5404 WVFGRD96 45.0 20 25 -75 4.90 0.5409 WVFGRD96 46.0 20 25 -75 4.91 0.5407 WVFGRD96 47.0 20 25 -75 4.91 0.5396 WVFGRD96 48.0 20 25 -75 4.92 0.5377 WVFGRD96 49.0 25 30 -70 4.93 0.5355 WVFGRD96 50.0 25 30 -70 4.93 0.5326 WVFGRD96 51.0 25 30 -70 4.94 0.5290 WVFGRD96 52.0 25 30 -70 4.95 0.5246 WVFGRD96 53.0 25 30 -65 4.93 0.5200 WVFGRD96 54.0 25 30 -65 4.94 0.5148 WVFGRD96 55.0 30 30 -65 4.96 0.5092 WVFGRD96 56.0 30 30 -65 4.97 0.5031 WVFGRD96 57.0 30 30 -65 4.97 0.4966 WVFGRD96 58.0 30 30 -60 4.96 0.4898 WVFGRD96 59.0 30 30 -60 4.96 0.4827
The best solution is
WVFGRD96 45.0 20 25 -75 4.90 0.5409
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 0.0200 n 3 lp c 0.050 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=Fri May 1 10:07:33 CDT 2009