2017/01/18 09:25:40 42.5470 13.2620 9.2 5.30
SLU Moment Tensor Solution
ENS 2017/01/18 09:25:40:3 42.55 13.26 9.2 5.3
Stations used:
IV.ATFO IV.ATMI IV.ATVO IV.CERT IV.CESI IV.CESX IV.FIAM
IV.GIGS IV.GIUL IV.GUAR IV.LATE IV.LAV9 IV.LPEL IV.LRP
IV.MA9 IV.MGAB IV.MOMA IV.MTCE IV.MURB IV.POFI IV.PTQR
IV.RMP IV.SACS IV.SAMA IV.SNTG IV.SRES IV.SSFR IV.T0110
IV.TRTR IV.VIVA IV.VVLD
Filtering commands used:
cut o DIST/3.3 -20 o DIST/3.3 +40
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 6.03e+23 dyne-cm
Mw = 5.12
Z = 6 km
Plane Strike Dip Rake
NP1 329 60 -93
NP2 155 30 -85
Principal Axes:
Axis Value Plunge Azimuth
T 6.03e+23 15 61
N 0.00e+00 2 331
P -6.03e+23 75 231
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.13e+23
Mxy 2.16e+23
Mxz 1.68e+23
Myy 4.07e+23
Myz 2.53e+23
Mzz -5.20e+23
##############
#-####################
##-------###################
##-----------#################
###--------------#################
####----------------############ #
####------------------########### T ##
#####--------------------######### ###
#####---------------------##############
######----------------------##############
######-----------------------#############
######---------- -----------############
######---------- P ------------###########
######--------- ------------##########
#######------------------------#########
#######-----------------------########
#######----------------------#######
########--------------------######
#######-------------------####
#########----------------###
#########-------------
##############
Global CMT Convention Moment Tensor:
R T P
-5.20e+23 1.68e+23 -2.53e+23
1.68e+23 1.13e+23 -2.16e+23
-2.53e+23 -2.16e+23 4.07e+23
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20170118092540/index.html
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STK = 155
DIP = 30
RAKE = -85
MW = 5.12
HS = 6.0
The waveform inversion is preferred.
The following compares this source inversion to others
SLU Moment Tensor Solution
ENS 2017/01/18 09:25:40:3 42.55 13.26 9.2 5.3
Stations used:
IV.ATFO IV.ATMI IV.ATVO IV.CERT IV.CESI IV.CESX IV.FIAM
IV.GIGS IV.GIUL IV.GUAR IV.LATE IV.LAV9 IV.LPEL IV.LRP
IV.MA9 IV.MGAB IV.MOMA IV.MTCE IV.MURB IV.POFI IV.PTQR
IV.RMP IV.SACS IV.SAMA IV.SNTG IV.SRES IV.SSFR IV.T0110
IV.TRTR IV.VIVA IV.VVLD
Filtering commands used:
cut o DIST/3.3 -20 o DIST/3.3 +40
rtr
taper w 0.1
hp c 0.03 n 3
lp c 0.10 n 3
Best Fitting Double Couple
Mo = 6.03e+23 dyne-cm
Mw = 5.12
Z = 6 km
Plane Strike Dip Rake
NP1 329 60 -93
NP2 155 30 -85
Principal Axes:
Axis Value Plunge Azimuth
T 6.03e+23 15 61
N 0.00e+00 2 331
P -6.03e+23 75 231
Moment Tensor: (dyne-cm)
Component Value
Mxx 1.13e+23
Mxy 2.16e+23
Mxz 1.68e+23
Myy 4.07e+23
Myz 2.53e+23
Mzz -5.20e+23
##############
#-####################
##-------###################
##-----------#################
###--------------#################
####----------------############ #
####------------------########### T ##
#####--------------------######### ###
#####---------------------##############
######----------------------##############
######-----------------------#############
######---------- -----------############
######---------- P ------------###########
######--------- ------------##########
#######------------------------#########
#######-----------------------########
#######----------------------#######
########--------------------######
#######-------------------####
#########----------------###
#########-------------
##############
Global CMT Convention Moment Tensor:
R T P
-5.20e+23 1.68e+23 -2.53e+23
1.68e+23 1.13e+23 -2.16e+23
-2.53e+23 -2.16e+23 4.07e+23
Details of the solution is found at
http://www.eas.slu.edu/eqc/eqc_mt/MECH.IT/20170118092540/index.html
|
January 18, 2017, CENTRAL ITALY, MW=5.4
Meredith Nettles
CENTROID-MOMENT-TENSOR SOLUTION
GCMT EVENT: C201701180925A
DATA: II IU CU IC LD G GE DK MN
KP
L.P.BODY WAVES:105S, 168C, T= 40
SURFACE WAVES: 130S, 248C, T= 50
TIMESTAMP: Q-20170118102313
CENTROID LOCATION:
ORIGIN TIME: 09:25:44.6 0.1
LAT:42.49N 0.01;LON: 13.26E 0.01
DEP: 12.9 0.3;TRIANG HDUR: 1.2
MOMENT TENSOR: SCALE 10**24 D-CM
RR=-1.270 0.023; TT= 0.236 0.017
PP= 1.040 0.017; RT=-0.193 0.042
RP=-0.487 0.039; TP=-0.562 0.013
PRINCIPAL AXES:
1.(T) VAL= 1.376;PLG= 8;AZM= 65
2.(N) 0.057; 15; 157
3.(P) -1.426; 73; 309
BEST DBLE.COUPLE:M0= 1.40*10**24
NP1: STRIKE=138;DIP=40;SLIP=-115
NP2: STRIKE=348;DIP=55;SLIP= -71
---########
----------#########
--------------#########
##---------------##########
##-----------------########
###------------------####### T
###-------- --------######
####-------- P --------##########
#####------- ---------#########
#####-------------------#########
######------------------#########
######-----------------########
########---------------########
#########-------------#######
##########----------#######
############------#####
###############----
#########--
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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 +40 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 1.0 165 50 -75 4.88 0.4291
WVFGRD96 2.0 185 30 -35 4.95 0.4428
WVFGRD96 3.0 180 30 -50 4.97 0.5067
WVFGRD96 4.0 160 30 -80 5.01 0.5684
WVFGRD96 5.0 155 25 -90 5.11 0.6355
WVFGRD96 6.0 155 30 -85 5.12 0.6717
WVFGRD96 7.0 160 30 -80 5.11 0.6652
WVFGRD96 8.0 170 35 -70 5.07 0.6169
WVFGRD96 9.0 185 35 -50 5.05 0.5926
WVFGRD96 10.0 195 45 -30 5.05 0.5738
WVFGRD96 11.0 200 50 -20 5.05 0.5570
WVFGRD96 12.0 200 55 -15 5.06 0.5393
WVFGRD96 13.0 200 55 -15 5.07 0.5190
WVFGRD96 14.0 205 60 10 5.08 0.4966
WVFGRD96 15.0 200 50 -15 5.11 0.4799
The best solution is
WVFGRD96 6.0 155 30 -85 5.12 0.6717
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 +40 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=Wed Jan 18 09:59:15 CST 2017