2016/10/20 00:09:54 40.7563 15.6518 17.3 3.4 Potenza
USGS Felt map for this earthquake
SLU Moment Tensor Solution
ENS 2016/10/20 00:09:54:6 40.76 15.65 17.3 3.4 Potenza
Stations used:
IV.AMUR IV.CDRU IV.CERA IV.CMPR IV.MCRV IV.MESG IV.MGR
IV.MIGL IV.MODR IV.MTSN IV.NOCI IV.PALZ IV.PIGN IV.PSB1
IV.SGRT IV.VAGA MN.TIP
Filtering commands used:
cut o DIST/3.3 -20 o DIST/3.3 +50
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 2.16e+21 dyne-cm
Mw = 3.49
Z = 16 km
Plane Strike Dip Rake
NP1 150 89 100
NP2 245 10 5
Principal Axes:
Axis Value Plunge Azimuth
T 2.16e+21 45 70
N 0.00e+00 10 330
P -2.16e+21 43 230
Moment Tensor: (dyne-cm)
Component Value
Mxx -3.40e+20
Mxy -2.16e+20
Mxz 1.06e+21
Myy 2.75e+20
Myz 1.85e+21
Mzz 6.45e+19
--------------
#---################--
####-#####################--
##-----#######################
##--------#######################-
##----------########################
##------------########################
##--------------############# ########
#----------------############ T ########
#------------------########### #########
#-------------------######################
#--------------------#####################
#---------------------####################
----------------------##################
--------- -----------#################
-------- P -------------##############
------- --------------############
------------------------##########
-----------------------#######
-----------------------#####
---------------------#
--------------
Global CMT Convention Moment Tensor:
R T P
6.45e+19 1.06e+21 -1.85e+21
1.06e+21 -3.40e+20 2.16e+20
-1.85e+21 2.16e+20 2.75e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161020000954/index.html
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STK = 245
DIP = 10
RAKE = 5
MW = 3.49
HS = 16.0
The NDK file is 20161020000954.ndk The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution
ENS 2016/10/20 00:09:54:6 40.76 15.65 17.3 3.4 Potenza
Stations used:
IV.AMUR IV.CDRU IV.CERA IV.CMPR IV.MCRV IV.MESG IV.MGR
IV.MIGL IV.MODR IV.MTSN IV.NOCI IV.PALZ IV.PIGN IV.PSB1
IV.SGRT IV.VAGA MN.TIP
Filtering commands used:
cut o DIST/3.3 -20 o DIST/3.3 +50
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 2.16e+21 dyne-cm
Mw = 3.49
Z = 16 km
Plane Strike Dip Rake
NP1 150 89 100
NP2 245 10 5
Principal Axes:
Axis Value Plunge Azimuth
T 2.16e+21 45 70
N 0.00e+00 10 330
P -2.16e+21 43 230
Moment Tensor: (dyne-cm)
Component Value
Mxx -3.40e+20
Mxy -2.16e+20
Mxz 1.06e+21
Myy 2.75e+20
Myz 1.85e+21
Mzz 6.45e+19
--------------
#---################--
####-#####################--
##-----#######################
##--------#######################-
##----------########################
##------------########################
##--------------############# ########
#----------------############ T ########
#------------------########### #########
#-------------------######################
#--------------------#####################
#---------------------####################
----------------------##################
--------- -----------#################
-------- P -------------##############
------- --------------############
------------------------##########
-----------------------#######
-----------------------#####
---------------------#
--------------
Global CMT Convention Moment Tensor:
R T P
6.45e+19 1.06e+21 -1.85e+21
1.06e+21 -3.40e+20 2.16e+20
-1.85e+21 2.16e+20 2.75e+20
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20161020000954/index.html
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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:
cut o DIST/3.3 -20 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 n 3The results of this grid search from 0.5 to 19 km depth are as follow:
DEPTH STK DIP RAKE MW FIT
WVFGRD96 1.0 335 45 -90 3.22 0.3651
WVFGRD96 2.0 335 50 -90 3.28 0.3148
WVFGRD96 3.0 355 15 -60 3.28 0.3084
WVFGRD96 4.0 350 15 -70 3.26 0.3518
WVFGRD96 5.0 340 15 -80 3.38 0.3984
WVFGRD96 6.0 335 15 -85 3.38 0.4377
WVFGRD96 7.0 335 10 -85 3.38 0.4708
WVFGRD96 8.0 360 15 -60 3.35 0.5005
WVFGRD96 9.0 335 15 -80 3.37 0.5236
WVFGRD96 10.0 335 15 -80 3.38 0.5423
WVFGRD96 11.0 230 10 -10 3.38 0.5579
WVFGRD96 12.0 245 10 5 3.40 0.5794
WVFGRD96 13.0 245 10 5 3.41 0.5958
WVFGRD96 14.0 245 10 5 3.42 0.6065
WVFGRD96 15.0 245 10 5 3.48 0.6129
WVFGRD96 16.0 245 10 5 3.49 0.6155
WVFGRD96 17.0 250 10 10 3.50 0.6145
WVFGRD96 18.0 245 10 5 3.52 0.6099
WVFGRD96 19.0 150 90 80 3.53 0.6021
WVFGRD96 20.0 150 90 80 3.54 0.5912
WVFGRD96 21.0 150 90 80 3.55 0.5773
WVFGRD96 22.0 150 90 80 3.55 0.5613
WVFGRD96 23.0 330 85 -90 3.56 0.5447
WVFGRD96 24.0 150 90 80 3.57 0.5209
WVFGRD96 25.0 330 85 -85 3.57 0.5030
WVFGRD96 26.0 135 5 -105 3.57 0.4812
WVFGRD96 27.0 330 85 -85 3.57 0.4604
WVFGRD96 28.0 135 10 -105 3.57 0.4414
WVFGRD96 29.0 140 10 -95 3.57 0.4251
The best solution is
WVFGRD96 16.0 245 10 5 3.49 0.6155
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 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
cut o DIST/3.3 -20 o DIST/3.3 +50 rtr taper w 0.1 hp c 0.03 n 3 lp c 0.10 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. |
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.
The nnCIA used for the waveform synthetic seismograms and for the surface wave eigenfunctions and dispersion is as follows:
MODEL.01
C.It. A. Di Luzio et al Earth Plan Lettrs 280 (2009) 1-12 Fig 5. 7-8 MODEL/SURF3
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
1.5000 3.7497 2.1436 2.2753 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00
3.0000 4.9399 2.8210 2.4858 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00
3.0000 6.0129 3.4336 2.7058 0.500E-02 0.100E-01 0.00 0.00 1.00 1.00
7.0000 5.5516 3.1475 2.6093 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
15.0000 5.8805 3.3583 2.6770 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
6.0000 7.1059 4.0081 3.0002 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
8.0000 7.1000 3.9864 3.0120 0.167E-02 0.333E-02 0.00 0.00 1.00 1.00
0.0000 7.9000 4.4036 3.2760 0.167E-02 0.333E-02 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 Oct 25 17:52:25 CDT 2016