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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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    3

    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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