paper muhammad alwi dkk - seismic image enhancement using ssa bpi on stacked-delta reservoir -3

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  • 8/18/2019 Paper Muhammad Alwi Dkk - Seismic Image Enhancement Using SSA BPI on Stacked-Delta Reservoir -3

    1/7

    PROCEEDINGS

    Joint Convention Balikpapan 2015

    HAGI-IAGI-IAFMI-IATMI

    5–8 October 2015

    !

    Seismic Image Enhancement using Singular Spectrum Analysis (SSA) and Basis Pursuit

    Inversion (BPI) on Stacked-deltaic Reservoir.

    Case Study: TGA field, Onshore Brantas Block, North East Java Basin.

     Muhammad Alwi1 , Rian Novico

    1 , Khairul Ummah

    2 , Mokhammad Puput Erlangga

    2 , Dythia Prayudhatama

    1 Lapindo Bratas, 2 Waviv Technologies

     Abstract

    One of the common challenges for seismic interpreters in Indonesia is dealing with below seismic resolution of

    thin layers reservoir with limited data availability, like what we have encountered on some seismic lines in

     Brantas Block onshore area, especially on TGA field. TGA reservoir type is thin layer sand-shale interbedded

    which deposited in fluvial deltaic system. The original seismic lines have poor quality. Surface problems when

    acquisition, tuning and gas effect are some of major factors. It contributes in making the seismic image blurry

    and hard to be interpreted in detail. Consequently, it is difficult to delineate reservoir thickness laterally,

    analyze seismic internal character and stratigraphy.

    To overcome such challenges, we came with alternative solution that is by using Singular Spectrum Analysis

    (SSA) as a precondition then continued by applying a sparse layer inversion technique using Basis Pursuit

     Inversion (BPI) method to the original post-stack of the seismic lines. The result shows that SSA and BPI works

    excellent to reconstruct the high frequency seismic that missing on the old section. Furthermore, the technique

     gives a significant image improvement, enhances the lateral continuity and vertical resolution, and consequently

     gives us a more confidence in interpretation.

    INTRODUCTION

    TGA gas field are located in onshore area of Brantas

    Block, East Java Basin and administrative area of East

    Java province of Indonesia. TGA field has 5

     production wells and covered by 14 seismic lines

    which has variety of vintage. Most of the seismic lines

    have low-to-medium quality. The seismic quality in

    the reservoir level (0-1500ms) is quite low, as it is

    caused by surface problems when acquisition. There

    are thin layer reservoirs, which are below seismic

    resolution or tuning. The existing gas effect has also

    contributed to reduce the high frequency content in the

    seismic data. The obstacles are exaggerated by the factthat acquiring new and proper seismic data with higher

    resolution has not been an option yet from economic

     point of view. Moreover, the surface condition has

     become high-dense population, which trigger social

     problems; the biggest issue in recording seismic

    operation.

    As we know, naturally seismic data contains both of

    coherent and incoherent noises. Coherent noises

    usually have special frequency range but more

    challenging than incoherent noise. Besides that, tuningand gas effect is another obstacle that commonly

    happens on the thin layer deltaic reservoir. The other

    factor that may happen in TGA field are the faulting

    with short-displacement and facies changes that hardly

    detected by the existing 2D seismic lines.

    Considering the technical and non-technical problems,

    we tried to come up with seismic enhancement

    technique to optimize the data that we already have.

    Along with some conventional reprocessing programs,

    we are also strained to study directly to the seismic

    enhancement processing. In this study we applied a

    sparse layer inversion technique using Basis Pursuit

    Inversion (BPI) method. Two key lines that exactly

    lies on the center of TGA closure, line 168 (S-Ndirection) and line 322 (W-E direction), are the objects

    of study in this paper. These lines are old vintages that

    acquired on 1991 & 1992. The expected image

    enhancement can help the interpreters to understand

    the stratigraphy of the area.

    GEOLOGY

    The North East Java Basin covers an area of

    approximately 50,000 km2 from Central Java eastward

    across East Java, the East Java Sea, Madura island and

    the Madura Straits (Figure-1). The present dayvolcanic arc is the most prominent surface geological

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    HAGI-IAGI-IAFMI-IATMI

    5–8 October 2015

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    feature of East Java. South of the volcanic arc

    Miocene and Oligocene rocks crop out in the Southern

    Mountains. North of the volcanic arc the surface

    geology shows two major anti-formal features (the

    Kendeng Zone and the Tuban Ridge) that haveoutcrops of Miocene to Pleistocene rocks. Holocene

    alluvial sediments cover the remaining area.

    The Brantas Block is located in the East Java Basin

    which initially developed as a result of the north-

    westward subduction of the Australian oceanic plate

     below the Sunda continent during Late Cretaceous

    time. A major extensional tectonic system prevailed

    during Early Tertiary time caused by complex

    interactions among the Australian, Eurasian and

    Pacific plates. This created extensional graben systems

    that trended approximately northeast-southwest,

    shifting to an east-west direction further to the south.

    Reservoir Description

    TGA field consists of numerous volcanic clastic sands

    ranging in depth from 600 feet to 3000 feet.

    Information from sidewall cores, logs, DST’s, and

    RFT’s indicate there are 7 zones with potential oil and

    gas reserves. The reservoirs are volcanic clastic sand

    classified as lithic arkoses or feldspathic litharenites.

    Clay content is variable and is dominated by smectite.

    The reservoirs are generally poorly cemented.

    Figure-2 shows the East-West cross section andcorrelation of the TGA wells. In a total distance of 5

    km a large number of reservoir units exist in all

    existing wells. This picture shows that reservoir levels

    have good correlation between the wells. Faults are

    indicated to exist and segmented TGA structure into

    four segments. This segmentation will be discussed

    later in the fault modeling section below.

    Based on this correlation, it is believed that most

    reservoir levels are widespread throughout the area.

    Paleo-environmental correlation of the main reservoirs

    F-10 and G-10 between TGA and the adjacent fields,

    namely Carat and Wunut indicate that the reservoirswere deposited in the transitional environment (upper

    to lower deltaic plain).

    Depositional Model and Trap Description

    The Pucangan Formation in TGA is volcanic clastic

    sand, consisting of volcanic sandstone with some part

    of volcanic lithic fragment. The Pucangan is volcanic

    detrital in nature; some of the grains are loosely

    cemented together (friable) and some are tight. The

    volcanic sands are product of the old Arjuna arc in the

    southern part of TGA that was deposited in the marine

    environment or possible outer littoral environment.

    This was indicated by the foraminifera which are

     present in most sample analyzed in cutting and side

    sidewall core samples of TGA wells. The shallow

    sections of TGA (E to B reservoirs) are shallow

    marine to inter-tidal channel.

    In TGA, most of the rock is fine to coarse grained, and

    moderately to well sorted with variable detrital

    volcanic rock fragment (andesite). Most of the matrix

    of sand consist of feldspar and heavy mineral like

    magnetite, hornblende and augite with volcanic lithic

    deposited under a deltaic channel setting. The trap

    TGA structure is a four way dip closure with structural

    trap mechanism for the B to E reservoirs and

    stratigraphic trap mechanism for the F and G

    reservoirs.

    METHODOLOGY

    In this study, we applied a combination of two

    methods to the data. First, we applied a Singular

    Spectrum Analysis (SSA) as data preconditioning to

    enhance the S/N ratio and give better input for the next

     process. Second, we applied Basis Pursuit Inversion

    (BPI) to increase vertical resolution.

    Singular Spectrum Analysis

    Singular spectrum analysis (SSA) is a method utilized

    for the analysis of time series arising from dynamical

    systems. The method is used to capture oscillationsfrom a given time series via the analysis of the

    eigenspectra of the so-called trajectory matrix. The

    trajectory matrix is composed of multiple data views.

    The singular value decomposition (SVD) of the

    trajectory matrix can be used for rank reduction and

    noise elimination. We apply SSA in the FX domain

    and present a comparison with classical FX

    deconvolution. The algorithm arising from SSA

    analysis is equivalent to Cadzow FX noise attenuation,

    a method recently proposed by Trickett (2008). It is

    important to stress, however, that Cadzow filtering is a

    general framework for noise reduction of signals and

    images. Cadzow filtering is equivalent to SSA when

    considering sinusoidal waveforms immersed in

    additive random noise. The intention of this abstract is

    to provide a simple explanation of the basic

    assumptions made in SSA and its application to the

    modeling of plane waves (Sacchi, 2009).

    Basis Pursuit Inversion

    Basis Pursuit Inversion (BPI) can be thought as an

    inversion strategy which utilizes the key that any local

    earth impedance structure can be represented by

    superposition of a limited number of layers, and thus,

    the seismogram can be represented locally as the

    superposition of a limited number of layer responses

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    HAGI-IAGI-IAFMI-IATMI

    5–8 October 2015

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    as well (Chen, 2001; Zhang, 2008; Zhang, 2011). The

    resulted inversion would then assume a low number of

    layers that can be parameterized to resolve thinner

    layers. In our study, we improve the BPI algorithm by

    optimizing the searching process for the most suitableregularization parameter (! ) in order to obtain

    optimum inverted reflectivity results with maximum

    noise suppression. General algorithm of BPI relies on

    the convolution model of seismic trace:

    d = Gm + n, (1)

    where d is the seismic trace, G is a dictionary of time-

    shifted pre-defined seismic responses, and m  are the

    weights for these responses that result from

    minimizing the objective function:

    (2)

    where the subscripts refer to the L2 and L1 norms,

    respectively, and !   is a regularization parameter that

    controls the sparsity of the solution. Basis pursuit

    algorithm is used here to find the minimal L1 norm

    least square solution by finding the solution that

    minimizes the objective function in equation 2.

    BPI requires a series of symmetrical and asymmetrical

    layer reflectivity pairs over a pre-defined range ofthicknesses to be constructed. The dictionary of

    seismic layer responses, G, is then produced by

    convolving the series of symmetrical and

    asymmetrical layer reflectivity pairs with the seismic

    model. If top and base reflectors of a thin bed have

    reflection coefficients of c and d , the reflections can be

    represented as two impulse functions c!(t)  and

    d !(t+n"t) where n"t  is time thickness of the thin bed

    and "t   is the seismic sample rate. The reflector pair

    can be further decomposed, using dipole

    decomposition (Puryear and Castagna, 2008), into

    unique odd and even pairs given by equation 3 (Zhang,

    2011).

    (3)

    The entire reflectivity series is represented as a

    summation of layer reflectivities:

    (4)

    where m is the layer number and M is the total number

    of layers. Seismogram equation is obtained when

    seismic wavelet is convolved on both sides of equation

    4:

    (5)

    where W e and W o are seismic responses constituting G.

    Basis pursuit algorithm is used then as a linear

    equation to solve for the coefficients an,m  and bn,m  in

    equation 5, and the results can be substituted to obtain

    the final reflectivity inversion, so called BPI

    reflectivity, given by equation 4.

    Original Post-stack Section

    Two original lines, PSTM Stack of 168 & 322, are

    used as input data in this work. These lines are

     primary lines that lays through the existing wells. Both

    of this original lines are product of conventional

     processing. The quality of the lines as shown on

    Figure-3 is defined as low-to-medium quality. These

    sections cannot show a detail layers in the reservoir

    target zone as we identify from log data. Some parts

    are blurry and low lateral continuity reflector. Since

    the poor of quality input, it is a good opportunity for

    SSA & BPI to show how much improvement can be

    achieved.

    RESULT AND DISCUSSION

    This work conducted in two main steps. First, data

     preconditioning using SSA technique and then

    continued with BPI method for seismic enhancement.

    To get the best of BPI, preconditioning data is a

    necessity to avoid inversion of noises. As we know,

    BPI works without any well involved and calculates

    independently for each trace to predict high frequency

    content. Figure-5 and Figure-6 show us thecomparison between original section, SSA result and

    BPI result of line 168 and 322.

    Both of the lines shows that frequency dominant

    spectrum of original line is around 10-70 Hz. SSA

    sections that is applied as precondition to increase S/N

    ratio of original lines also have the same frequency

    with the original one. For BPI lines, the frequency

    spectrum is gained up at high frequency and extended

    to 125 Hz. In addition, BPI also gains the low

    frequency part. The original product of BPI containshigher resolution data, as shown in the amplitude

    frequency spectrum. Unfortunately for this data, some

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    5–8 October 2015

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    of BPI’s new reflectors are quite small amplitude and

    hardly visible. Therefore, some methods such as

    automatic gain control (AGC) or amplitude

    weightening cosine phase may be applied to help

     provide a better visible image.

    Wide Wiew

    For wide view, we can see clearer image and higher

    resolution as a result of SSA and BPI. The detail

     becomes more visible after applying AGC. The SSA

    and BPI together produced a significant increase to

    the lateral continuity, as well as better layering and

    gaining of the vertical resolution. Some seismic

    features become more visible. For instance, in the line

    168 (Figure-5) on the reservoir zone (from 200-1200ms), it shows a significant improvement. The

     blurry area at 600 ms of the original section can be

    reconstructed greatly by SSA and BPI. Some pinchout

     pattern on 1100 ms and 1300 ms now can be displayed

    clearer. Onlapping feature on 1700 ms also becomes

    stronger, that we may interpret as a prograding pattern.

    While for line 322 (Figure-6), the blurry part at time

    1200 ms has the most notable improvements.

    Ultimately, the continuity reflectors inside the blurry

    zone are now more convenient to be interpreted.

    Ant View

    If we look more into detail, as shown in the Figure-4,

    BPI's wiggle found to be sharper and slimmer

    compared to the original traces and SSA. It brings us

    an advantage; we now have a better quality image that

    can be interpreted more precisely and with higher

    confidence. If we analyze some traces which close to

    the well, it is shown that BPI delivers reflectors which

    have good match to lithology marker from well.

    Without side lobes, BPI reflectors can be easily to tied

    up to the well marker. We try to visualize interpreted

    trace section (right) using similar color to GR-log. It

    shows that most of lithology or facies that represented

    with different color in GR-log can be identified much

    more convenient than by using the original section.

     Notice that almost of all of lithology boundaries from

    well now has its reflector on seismic. Moreover, it has

    a very good lateral continuation on traces. The BPI’s

    reflectors which are sharper than original can help the

    interpreters to be more confident defines the thickness

    of each reservoir layers precisely. In other words, BPI

    has lessened the ambiguity and increased the

    consistency of seismic interpretation. Hence, using

    BPI image we can estimate the reserve more

    accurately.

    Wavelet Issue

    Similar to other inversion technique, wavelet is always

    an essential issue. Phase and frequency dominant in

    the wavelet are variables that can affect to the

    inversion result. In BPI works, wavelet has crucial

    rules. The information of original line we give to the

    BPI algorithm is all carried on by the wavelet. Thus,

    wavelet time variant extraction from seismic should be

    ensuring very careful. Wavelet has to be extracted

    from the interest zone and should be low noise ratio.

    In this research we went through a priceless

    experience, that is when we used wrong wavelet andended up with a new section produced by BPI which

    quite different from the original. Besides the

    enhancement of the resolution, using wrong wavelet in

    BPI will produces artifact reflectors in unexpected

    zone, while removes some confirmed reflectors. From

    that experience, we found that BPI is very sensitive to

    time variant wavelet. We overcome this problem using

    average wavelet from more traces, hence suppressing

    the noise. The result becomes stable and consistent to

    the well-log.

    CONCLUSIONS

    In our case, seismic enhancement works to the thin

    layers stacking-delta reservoir using BPI method,

    which is previously preconditioned by SSA. The result

    shows a big improvement of seismic image quality.

    Combination of SSA and BPI method can enhance the

    reflectors consistency, lateral continuity and vertical

    resolution. The workflow can also tackle the gas effect

    through the data due to great amplitude enhancement

    in the dimming reflektor zones. Inversion process can

     predict and restore missing reflectors by reconstruct

    high frequency spectrum, which is more correlable to

    the lithology information from well. BPI also shows

    its robustness to the presence of noise.

    The BPI’s reflectors which are sharper than original

    can help the interpreters to be more confident in

    defining the thichkness of each reservoir layer

     precisely. In other words, BPI has lessened the

    ambiguity and increased consistency of seismic

    interpretation.

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    Joint Convention Balikpapan 2015

    HAGI-IAGI-IAFMI-IATMI

    5–8 October 2015

    (

    ACKNOWLEDGEMENTS

    Authors would like to thank Lapindo Brantas Inc. for

     permission to publish this paper.

    REFFERENCES 

    Zhang, R., 2008, Seismic reflection inversion by basis

     pursuit,  Doctoral dissertation at University of

     Houston.Mauricio D. Sacchi, 2009, FX Singular Spectrum

    Analysis, CSPG CSEG CWLS Convention,

    Calgary, Alberta, Canada.

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    5–8 October 2015

    )

    LIST OF FIGURES

    Figure-1 Regional Geology of East Java Basin.

    Figure-2 Wells correlation of TGA field.

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    Figure-3 Original section of line 168 S-N (left) and line 322 W-E (right).

    Figure-4 Comparison of logs, original seismic (left, 12 traces), SSA (center left, 12 traces), BPI (center right, 12

    traces), and interpreted BPI (right, 24 traces). Interpreted BPI is a manual interpretation of lithology; facies color

    is referred to GR-log color. Inserted curve (red bold) in seismic traces is GR-log.