baizura_jmm
Transcript of baizura_jmm
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Outline
Introduction Background Importance of the Study
Theory and Methodology Velocity model for Malay Peninsula Focal mechanism solution using polarities and amplitude ratios Data used for determination of focal mechanism
Results and Discussion with related studies Focal mechanisms of four Bukit Tinggi events Comparison of the P and T axes distributions Observed polarities of the first motion of Pwaves
Conclusion2
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Locations of Earthquakes from 2007-2010
A network of 4 broadband and 3
short period sensor currentlyoperational in Malay Peninsula
(MMD).
A total of 30 weak and felt
earthquakes have been recordedin the Malay Peninsula from 2007
2010 (MMD Database as of
April 2011).
Most of these earthquakes are
located near the Bukit Tinggi faultzone and Kuala Lumpur fault
zone, which classified as inactive
(MMGD, 2008).
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Year Month No. EQEpicenter
(Lat/Long/Location)
Depth
(km)
Magnitude
(mb) MMI
2007
Nov 3 3.3 3.4 N 101-102 E Bukit Tinggi < 7 3.2 3.5 III
Dec 63.3 3.5 N 101-102 E Bukit Tinggi
< 52.6 3.5
III
2008
Jan 43.3 3.4 N 101-102 E Bukit Tinggi < 3 2.4 3.4
III
Mar 3
3.3 3.4 N 101-102 E Bukit Tinggi
Shallow
2.5 3.3
III
May 1 3.4 N 101.8 EBukit Tinggi Shallow
2.6 III
2009
Mar 1 3.9 N 102.5 E Jerantut 50 3.2 III
Apr 1 4.2 N 100.7 E Manjung 22 2.8 III
Oct 63.3 3.4 N 101-102 E Bukit Tinggi
< 10 1 - 2.8 III
Nov 4 2.7 2.8 N 102 E Kuala Pilah< 15 3.0 3.5
2.6 3.2 mlI
Dec 1 3.2 N 102 E Bukit Tinggi 5 2.2 I
2010 No Felt EQ in Malay Peninsula
Local Felt EQs in Malay Peninsula (2007-2010)
4 MMD, as of April 2011
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Distributions of the Local Felt EQs since its
first occurrence on November 30th, 2007
5
0
1
2
3
4
0 90 180 270 360 450 540 630 720 810
Day (s) since its first occurrence
Mantumb
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Importance of the Study
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Although hypocenters and magnitudes of these local
earthquakes are determined by the MMD, their focal
mechanisms have not been determined. Due to an absenceof the surface movement observed, these focal mechanisms
are important in improving our understanding of seismic
pattern and fault behavior in the Bukit Tinggi fault zone.
Since far field seismic is less of a threat, it is suggested to (re)focus on
local earthquake or near field earthquake, esp. in the vicinity of an 80-km
long Bentong fault, close to Bukit Tinggi fault line, where earthquake M3.5
has been recorded
-Jeffrey Chiang, the Chairman of Working Group
in Designing Building Code in Malaysia
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We selected three crust structure models, of which two are from
CRUST2.0 (http://igpweb.ucsd.edu/~gabi/crust2.html) and the other
one is model iasp91 (Kennet and Engdahl, 1991).
We compared the observed travel time differences between P and S
to those computed for these models. We performed the similar
comparison for the P-arrival. We calculated the root mean square
(RMS) for both comparisons using the following equation :
where is the i-th observed data, is the i-th calculated data
and is the total number of data.
Velocity Model for Malay Peninsula
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CRUST 2.0 is a global crustal
model at 2x2 degrees scale.
Composed of 360 key 1d-profilesand one of these is assigned to
each 2x2 degree cell.
Each profile is a 7 layer 1D-model
(ice, water, soft sediments, hardsediments, upper crust, middle
crust and lower crust .
For Malay Peninsula, models J1
and C2 are available fromCRUST2.0 .
http://igppweb.ucsd.edu/~gabi/crust2.html
Source :Crustal Model CRUST2 page
Crustal Profile based on CRUST 2.0
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Depth(k
m)
Velocity (km/s)
Comparison of Velocity Structure between
CRUST2.0 (J1 and C2), and iasp91
Vs Vp
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Observing P and S Onset (IPM)
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Time series of vertical channel (a) and horizontal channel (b), of IPM
station for the BUkit Tinggi event occurred at 02:13 UTC, November30, 2007 with magnitude of 3.5mb. The upper, middle and lower
traces are velocity, squared velocity, and integration of squared
velocity, respectively
(a) (b)
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ObservedS-P(s)
Theoretical S-P (s)
S-P Travel-time Differences
Obs = 6.36
J1 = 6.79C2 = 6.84
Iasp91 = 6.5
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Comparison of P- phase Arrivals
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P-h
asearrival(M
MDPicking)
Theoretical P-arrival
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Comparisons of RMS
among JI, C2 and iasp91
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RMS VELOCITY MODEL
J1 C2 iasp91
S-P travel time all 2.65 2.68 2.57
excluding large
residuals (>3s)
1.44 1.44 1.25
P-phase arrival 1.49 1.01 0.85
The lowest RMS are consistently obtained by model iasp91, which suggests
that model iasp91 predicts the observed travel times better than the modelsfrom CRUST2.0.
This is consistent with the result obtained by Din (2011) in which crustal
thickness beneath station IPM is similar to the thickness of iasp91 (35km).
We used a velocity model from iasp91 for the calculation of take off angles.
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FOCMEC Software Package (Snoke, 1984)
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We used the FOCMEC software package available at http://www.iris.edu/software/downloads/processing/
This software determines focal mechanisms using polarities (P,SV, SH) and amplitude ratios (SV/P, SH/P, SV/SH).
Focmecprogram calculates all acceptable solutions. We can useFocpltfor further analysis and display.
Horizontal components are being rotated into radial andtransverse components to separate SV and SH.
SH to P amplitude ratio provides what could be considered almostindependent data. Polarities and ratios involving SH are likely to be
more reliable than those involving SV.
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Data Used to Determine Focal Mechanism
We requested three-componentbroadband waveform data recorded at
stations of IPM and KOM for four largest
Bukit Tinggi events (mb 3 - 3.5) using
BREQ_FAST (Batch REQuest, FAST),
which provides batch access to the IRIS
DMC archive.
This was done by emailing a formatted
file to [email protected]
YEAR MONTH DAY TIME(UTC)
EPICENTER DEPTH(KM)
MAGNITUDELAT LONG
2007 Nov 30 02:13 3.36N 101.80E 2.3 3.5 mb
2007 Nov 30 12:42 3.31N 101.84E 6.7 3.2 mb
2007 Dec 12 10:01 3.47N 101.79E 10 3.2 mb
2008 Jan 10 15:38 3.39N 101.73E 3.0 3.0 mb
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Rotation of the 02:13 UTC,November 30, 2007
Bukit Tinggi waveform data
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Coordinat
e
rota+on
East-West
North-South
Radial
Transverse
Ver+cal
Ver+cal
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Observing polarities of the 02:13 UTC
November 30, 2007 Bukit Tinggi event
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E-W
N-S
Radial
Transverse
Ver+cal
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Input Parameters for FOCMEC (1)
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Station Azimuth Take offAngle Key Log10 (S/P)IPM 325.23 46.17 DIPM 325.23 46.17 FIPM 325.23 46.17 LIPM 325.23 46.17 H 0.85281SHKOM
KOM 127.25127.25 46.1746.17 DFKOM 127.25 46.17 LKOM 127.25 46.17 H 0.77248SH
Input parameters for the November 30th, 2007, 02:13 UTC Bukit Tinggi
event.D = Dilatation, F = Away from event , L=Left and H = Log10(SH/
P)
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Focal Mechanism of the 02:13 UTC
November 30, 2007 Bukit Tinggi event
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58 acceptable solutions
dip
strike
rake
Fault Plane 1 Fault Plane 2
F1
F2
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Focal Mechanism of the 12:42 UTC
November 30, 2007 Bukit Tinggi event
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10 acceptable solutions
dip
strike
rake
Fault Plane 1 Fault Plane 2F1
F2
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Focal Mechanism of the 10:01 UTC
December 12, 2007 Bukit Tinggi event
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6 acceptable solutions
rake
strike
dip
Fault Plane 1 Fault Plane 2F1
F2
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Focal Mechanism of the 15:38 UTC
January 10, 2008 Bukit Tinggi event
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2 acceptable solutions
rake
strike
dip
Fault Plane 1 Fault Plane 2F1
F2
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Comparison of the P and T axes distribution
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02:13 UTC
Nov 30, 2007
3.5 mb
12:42UTC
Nov 30, 2007
3.2mb
10:01UTC
Dec 12, 2007
3.2 mb
15:38 UTC
Jan 10, 2008
3.0 mb
P, T and B are the maximum compressional, minimum compressional and
null axes, respectively).
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P-wave First Motion Polarities Observations
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The similar waveforms
imply that the
mechanisms of the
events are similar.
The observed polarity
at a given station
should be the same
for each event in
cluster (Hardebeckand Shearer, 2002).
Waveform data of the 02:13 UTC Nov, 30,2007(left) and the 15:38 UTC Jan 10, 2008 (right)
Waveform data of the 12:55 UTC Dec, 9,2007
(left) and the 00:50 UTC Mar 15, 2008 (right)
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Discussion on Focal Mechanism of
Bukit Tinggi with Related Studies
1. The orientation of P and T axes are differentfrom Simons et. al (2007): compression is in theNE-SW direction
2. One possible explanation : weak-zone-normalextension mechanisms. (Hurukawa and Imoto,
1992).
3.
Westward motion of the Sunda Plate cause theweak zone in the vicinity of the Bukit Tinggi
fault to rupture or open due to an extensional
movement in the East-West direction (Lat and
Ibrahim, 2009).
4. (Fatt et al., 2011) shows that epicenters of BukitTinggi events are scattered along the Bukit
Tinggi fault (striking NW-SE directions and
dipping toward the NE) and Kuala Lumpur fault
(striking NW-SE directions and dipping toward
the SW).
T
P
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Conclusions
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We obtained relatively well-constrained solutions of the eventswe analysed although the constraint for dip angles is weaker.
The focal mechanisms of the largest 3.5mb event is mostlystrike slip with some dip slip, while that of three events are strike
slip fault type.
The maximum compressional (P) axes of the largest 3.5mbevent are in the NNW-SSE direction while the three strike slip
events are in the NW-SE direction.
The minimum compressional (T) axes of the strike slip eventsare in the NE-SW direction.
Since there is no surface trace of ruptures this result isimportant to improve our understanding of these seismic activities.
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Thank You
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