2013/04/22 22:28:47 47.69 20.34 10.0 4.50 Hungary
USGS Felt map for this earthquake
USGS/SLU Moment Tensor Solution
ENS 2013/04/22 22:28:47:0 47.69 20.34 10.0 4.5 Hungary
Stations used:
CZ.JAVC CZ.KHC CZ.NKC CZ.OKC CZ.PRU CZ.VRAC GE.MORC GR.BRG
GR.FUR GR.GRB3 GR.GRC2 GR.WET HU.BUD HU.PSZ HU.SOP HU.TRPA
MN.BLY MN.PDG MN.TRI NI.ACOM NI.CGRP NI.CIMO NI.CLUD NI.DRE
NI.FUSE NI.PRED NI.SABO NI.ZOU2 OE.ARSA OE.KBA OE.MOA
OE.OBKA OE.WTTA PL.BEL PL.GKP PL.KSP PL.OJC RO.BUR31 RO.BZS
RO.MLR SJ.BBLS SJ.FRGS SL.BOJS SL.CADS SL.CRNS SL.GBAS
SL.GBRS SL.GCIS SL.GORS SL.GROS SL.JAVS SL.KNDS SL.KOGS
SL.LJU SL.MOZS SL.PERS SL.ROBS SL.SKDS SL.VNDS SL.VOJS
SX.TANN TH.MODW
Filtering commands used:
hp c 0.02 n 3
lp c 0.04 n 3
Best Fitting Double Couple
Mo = 3.80e+22 dyne-cm
Mw = 4.32
Z = 4 km
Plane Strike Dip Rake
NP1 130 45 90
NP2 310 45 90
Principal Axes:
Axis Value Plunge Azimuth
T 3.80e+22 90 95
N 0.00e+00 -0 310
P -3.80e+22 -0 220
Moment Tensor: (dyne-cm)
Component Value
Mxx -2.23e+22
Mxy -1.87e+22
Mxz -5.18e+14
Myy -1.57e+22
Myz -1.97e+15
Mzz 3.80e+22
--------------
----------------------
----------------------------
#############-----------------
-##################---------------
--#####################-------------
---########################-----------
----#########################-----------
----###########################---------
------###########################---------
------################# #########-------
-------################ T ##########------
---------############## ##########------
---------###########################----
-----------#########################----
-----------########################---
-------------#####################--
---------------##################-
--------------#############
P --------------------------
----------------------
--------------
Global CMT Convention Moment Tensor:
R T P
3.80e+22 -5.18e+14 1.97e+15
-5.18e+14 -2.23e+22 1.87e+22
1.97e+15 1.87e+22 -1.57e+22
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.EU/20130422222847/index.html
|
STK = 310
DIP = 45
RAKE = 90
MW = 4.32
HS = 4.0
The waveform inversion is preferred.
The following compares this source inversion to others
USGS/SLU Moment Tensor Solution
ENS 2013/04/22 22:28:47:0 47.69 20.34 10.0 4.5 Hungary
Stations used:
CZ.JAVC CZ.KHC CZ.NKC CZ.OKC CZ.PRU CZ.VRAC GE.MORC GR.BRG
GR.FUR GR.GRB3 GR.GRC2 GR.WET HU.BUD HU.PSZ HU.SOP HU.TRPA
MN.BLY MN.PDG MN.TRI NI.ACOM NI.CGRP NI.CIMO NI.CLUD NI.DRE
NI.FUSE NI.PRED NI.SABO NI.ZOU2 OE.ARSA OE.KBA OE.MOA
OE.OBKA OE.WTTA PL.BEL PL.GKP PL.KSP PL.OJC RO.BUR31 RO.BZS
RO.MLR SJ.BBLS SJ.FRGS SL.BOJS SL.CADS SL.CRNS SL.GBAS
SL.GBRS SL.GCIS SL.GORS SL.GROS SL.JAVS SL.KNDS SL.KOGS
SL.LJU SL.MOZS SL.PERS SL.ROBS SL.SKDS SL.VNDS SL.VOJS
SX.TANN TH.MODW
Filtering commands used:
hp c 0.02 n 3
lp c 0.04 n 3
Best Fitting Double Couple
Mo = 3.80e+22 dyne-cm
Mw = 4.32
Z = 4 km
Plane Strike Dip Rake
NP1 130 45 90
NP2 310 45 90
Principal Axes:
Axis Value Plunge Azimuth
T 3.80e+22 90 95
N 0.00e+00 -0 310
P -3.80e+22 -0 220
Moment Tensor: (dyne-cm)
Component Value
Mxx -2.23e+22
Mxy -1.87e+22
Mxz -5.18e+14
Myy -1.57e+22
Myz -1.97e+15
Mzz 3.80e+22
--------------
----------------------
----------------------------
#############-----------------
-##################---------------
--#####################-------------
---########################-----------
----#########################-----------
----###########################---------
------###########################---------
------################# #########-------
-------################ T ##########------
---------############## ##########------
---------###########################----
-----------#########################----
-----------########################---
-------------#####################--
---------------##################-
--------------#############
P --------------------------
----------------------
--------------
Global CMT Convention Moment Tensor:
R T P
3.80e+22 -5.18e+14 1.97e+15
-5.18e+14 -2.23e+22 1.87e+22
1.97e+15 1.87e+22 -1.57e+22
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.EU/20130422222847/index.html
|
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.
|
|
|
|
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 0.04 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT
WVFGRD96 0.5 290 45 60 4.13 0.3435
WVFGRD96 1.0 295 45 70 4.16 0.3573
WVFGRD96 2.0 290 45 60 4.23 0.4265
WVFGRD96 3.0 300 45 75 4.28 0.4567
WVFGRD96 4.0 310 45 90 4.32 0.4624
WVFGRD96 5.0 315 40 95 4.34 0.4433
WVFGRD96 6.0 320 40 100 4.34 0.4095
WVFGRD96 7.0 120 55 75 4.34 0.3697
WVFGRD96 8.0 120 55 75 4.38 0.3977
WVFGRD96 9.0 95 35 40 4.32 0.3721
WVFGRD96 10.0 90 35 30 4.31 0.3818
WVFGRD96 11.0 90 40 30 4.31 0.3914
WVFGRD96 12.0 90 40 30 4.31 0.4005
WVFGRD96 13.0 90 40 30 4.32 0.4089
WVFGRD96 14.0 90 40 30 4.32 0.4160
WVFGRD96 15.0 85 45 25 4.32 0.4216
WVFGRD96 16.0 85 45 25 4.33 0.4274
WVFGRD96 17.0 85 45 25 4.33 0.4316
WVFGRD96 18.0 85 45 25 4.34 0.4343
WVFGRD96 19.0 85 45 25 4.34 0.4357
WVFGRD96 20.0 85 50 25 4.35 0.4364
WVFGRD96 21.0 85 50 25 4.36 0.4373
WVFGRD96 22.0 85 50 25 4.36 0.4370
WVFGRD96 23.0 85 50 25 4.37 0.4356
WVFGRD96 24.0 85 50 25 4.37 0.4333
WVFGRD96 25.0 85 50 25 4.38 0.4302
WVFGRD96 26.0 85 50 25 4.38 0.4263
WVFGRD96 27.0 85 55 25 4.39 0.4222
WVFGRD96 28.0 80 55 20 4.39 0.4180
WVFGRD96 29.0 80 55 20 4.40 0.4134
The best solution is
WVFGRD96 4.0 310 45 90 4.32 0.4624
The mechanism correspond to the best fit is
|
|
|
The best fit as a function of depth is given in the following figure:
|
|
|
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 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 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
hp c 0.02 n 3 lp c 0.04 n 3
|
|
|
|
| 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. |
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:
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.
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=Tue Apr 23 07:47:55 CDT 2013