<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJOGas</journal-id><journal-title-group><journal-title>Open Journal of Yangtze Oil and Gas</journal-title></journal-title-group><issn pub-type="epub">2473-1889</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojogas.2017.23014</article-id><article-id pub-id-type="publisher-id">OJOGas-77631</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Analyses of Nature of Fault through Production Data
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Haijun</surname><given-names>Fan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Atif</surname><given-names>Zafar</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>S.</surname><given-names>G. Alam</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Muhammad</surname><given-names>Kashif</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Asif</surname><given-names>Mehmood</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>University of Karachi, Karachi, Pakistan</addr-line></aff><aff id="aff1"><addr-line>China University of Petroleum (East China), Qingdao, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>atif_zafar1984@yahoo.com(AZ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>14</day><month>07</month><year>2017</year></pub-date><volume>02</volume><issue>03</issue><fpage>176</fpage><lpage>190</lpage><history><date date-type="received"><day>April</day>	<month>7,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>July</month>	<year>11,</year>	</date><date date-type="accepted"><day>July</day>	<month>14,</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  An application of integration of reservoir production data in analysis for nature of fault is presented in this paper. The real data of a Gas Field (namely RS Gas Field) of L-Basin of Pakistan are used. The basic concept behind this work is to enlighten the importance of production data analysis in a broader way like for finding out the nature of fault i.e. conductive or non-conductive and if it is conductive, what is the leakage factor of the fault etc. Normally in the case of fault analysis we rely on geological and geophysical methods to some extent but in some cases where these geological and geophysical methods are not able to reach any final and firm conclusion because of data limitation or any other reason, production data analysis may play a great role in answering the ambiguities regarding any fault/faults present there. This paper describes the successful implementation of reservoir production data analysis in RS Gas Field where the main uncertainties were identified during initial stage of field development when location of new development well was going to be marked. Numbers and locations of well are important factors of Oil and Gas Filed Developments; but specifically, for Gas Field Development, these factors become more crucial as compared to Oil Field Development; so clear knowledge of any heterogeneity, barrier, boundary or fault is necessary to develop a gas field optimally and economically.
 
</p></abstract><kwd-group><kwd>Fault Analysis</kwd><kwd> Leakage Factor</kwd><kwd> Production Data</kwd><kwd> Reservoir Engineering</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The RS concession lies in the L-Basin of Pakistan and in a highly prospective area where the large gas fields of Pakistan are found. The primary objective in this area is the M-Limestone; the secondary objective was the U-Limestone. Both are of early Eocene age. The Late Cretaceous Sandstone provided a tertiary objective. The source rock for the gas is the Lower Cretaceous Shales. Seal for the M-Limestone is provided by the S-Shale, for the U-Limestone, seal is provided by the G-shale.</p><p>RS gas field was brought on production in April 2010 with an initial production rate of 16.5 MMscfd gas. Presently (December 2015), the well is producing 14 MMscfd gas, thus showing a decline of 3.24% per year.</p><p>After production of more than five years of RS-1 well, the reservoir has been appraised and level of confidence has been increased on initial gas in place estimated through different methods. For further field development, the development well (RS-2) was proposed on the south of the RS-1 (<xref ref-type="fig" rid="fig1">Figure 1</xref>) well on the basis of following assumptions and limitations:</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> 2D Structure map of RS gas field</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x2.png"/></fig><p>1) The fault near the RS-1 Well is a sealing fault</p><p>2) East and West compartment of the reservoir along the fault are not in communication</p><p>3) West part may be different reservoir or may not be any reservoir because of lack of seismic data control on that side</p><p>The location for RS-2 well was proposed on the basis of some relatively high tops of reservoir. Top of reservoir in RS-1 Well is 1290 m whereas in proposed RS-2 well top of reservoir is 1285 m. It indicates additional 5 m of reservoir in proposed RS-2 well.</p></sec><sec id="s2"><title>2. Methodology</title><p>To determine the nature of fault of RS Gas Field Structure, study will be carried</p><p>out in two stages. In first stage the pressure and production history will be used in order to calculate initial gas in place of RS Gas Reservoir. This initial gas in place will be verified by volumetric estimation method. If initial gas in place from both the methods is in agreement it will show that dynamic and static methods are on same page that is fault is non-sealing. If it will be the case then further investigation regarding the degree of leakage of fault will be carried out through simulation as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Methodology flow chart</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x3.png"/></fig><sec id="s2_1"><title>2.1. Initial Gas In-Place Estimation</title><p>This section is concerned with fluid flow in the bulk of the RS Gas Reservoir. The integration of geology and well test analyses will be very helpful [<xref ref-type="bibr" rid="scirp.77631-ref1">1</xref>] . An understanding of the mechanisms controlling fluid displacement will help in maximizing the technically recoverable reserves through</p><p>1) Planning reservoir development strategies.</p><p>2) Optimizing off take rates at field and reservoir layer level.</p><p>3) Marking initial well locations.</p><p>4) Designing initial well completions and identifying subsequent interventions.</p><p>Knowledge of reservoir drive mechanism is necessary in order to prepare dynamic model to calculate initial gas in-place [<xref ref-type="bibr" rid="scirp.77631-ref2">2</xref>] . Normally, gas reservoirs are produced by expansion of the gas contained in the reservoir. The high compressibility of the gas relative to the water in the reservoir (either connate water or underlying aquifer) makes the gas expansion the dominant drive mechanism. But this depletion drive mechanism changes to water drive mechanism by different indices in different reservoirs depending upon the properties and geometries of the reservoir and aquifer.</p><p>To investigate the drive mechanism of RS Gas Reservoir the P/Z Vs G<sub>p</sub> Plot (<xref ref-type="fig" rid="fig3">Figure 3</xref>) was generated by using the production and pressure history as given in <xref ref-type="table" rid="table1">Table 1</xref>.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> P/Z Vs G<sub>p</sub> plot of RS gas reservoir</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x4.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Pressure and production history of RS gas field</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Year</th><th align="center" valign="middle" >Pressure (P*)/psi</th><th align="center" valign="middle" >Z</th><th align="center" valign="middle" >G<sub>p</sub>/BSCF</th><th align="center" valign="middle" >P/Z</th></tr></thead><tr><td align="center" valign="middle" >Initial</td><td align="center" valign="middle" >2080</td><td align="center" valign="middle" >0.9732</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >2137</td></tr><tr><td align="center" valign="middle" >2011</td><td align="center" valign="middle" >1967.7</td><td align="center" valign="middle" >0.9725</td><td align="center" valign="middle" >7.2517</td><td align="center" valign="middle" >2023</td></tr><tr><td align="center" valign="middle" >2012</td><td align="center" valign="middle" >1911</td><td align="center" valign="middle" >0.9723</td><td align="center" valign="middle" >12.713</td><td align="center" valign="middle" >1965</td></tr><tr><td align="center" valign="middle" >2013</td><td align="center" valign="middle" >1866</td><td align="center" valign="middle" >0.9721</td><td align="center" valign="middle" >19.242</td><td align="center" valign="middle" >1920</td></tr><tr><td align="center" valign="middle" >2015</td><td align="center" valign="middle" >1789</td><td align="center" valign="middle" >0.9720</td><td align="center" valign="middle" >27.917</td><td align="center" valign="middle" >1841</td></tr></tbody></table></table-wrap><p>For a volumetric reservoir, the relationship between (P/Z) and G<sub>p</sub> is essentially linear because of volumetric depletion of gas reservoir and by extrapolation of the straight line to abscissa, i.e., at P/Z = 0, gives the value of the gas initially in place as G = G<sub>p</sub> [<xref ref-type="bibr" rid="scirp.77631-ref3">3</xref>] . But the graphical representation of pressure and production history of RS Reservoir shows the presence of water influx, as shown <xref ref-type="fig" rid="fig1">Figure 1</xref> where the plot of (P/Z) versus G<sub>p</sub> deviates from the linear relationship, it indicates the presence of water encroachment [<xref ref-type="bibr" rid="scirp.77631-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.77631-ref5">5</xref>] .</p><p>After confirming by P/Z Vs G<sub>p</sub> plot that there is water encroachment in the reservoir [<xref ref-type="bibr" rid="scirp.77631-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.77631-ref7">7</xref>] , the next step is to generate the Cole plot which is more sensitive reservoir drive mechanism diagnostic plot [<xref ref-type="bibr" rid="scirp.77631-ref8">8</xref>] .</p><p>Cole plot of RS Gas Reservoir (<xref ref-type="fig" rid="fig4">Figure 4</xref>) shows that reservoir has water drive mechanism means it is has some degree of pressure maintenance due to water encroachment into the reservoir from the aquifer. After validation of reservoir drive mechanism now the question arises about the strength of aquifer support. Accurate aquifer modeling will be done in next step by verifying the history matching and production and pressure simulation. If the comparison of P/Z Vs G<sub>p</sub> plot (<xref ref-type="fig" rid="fig3">Figure 3</xref>) and Cole plot (<xref ref-type="fig" rid="fig4">Figure 4</xref>) is made with their benchmark plots (<xref ref-type="fig" rid="fig5">Figure 5</xref>) it reveals that RS Gas Reservoir has moderate water dive support or in other words it has partial water drive mechanism.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Cole plot of RS gas reservoir</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x5.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> General shapes of P/Z Vs G<sub>p</sub> and Cole plot as a function of aquifer strength</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x6.png"/></fig><p>Material Balance Method is adopted to estimate the initial gas in place of Jin Gas Reservoir by using the pressure values obtained by well test interpretation using the commercial software. The material balance is based on the principle of the conservation of mass:</p><p>Mass of fluids originally in place = Fluids produced + Remaining fluids in place.</p><p>The material balance program uses a conceptual model of the reservoir to predict the reservoir behavior based on the effects of reservoir fluids production [<xref ref-type="bibr" rid="scirp.77631-ref9">9</xref>] . The material balance equation is zero-dimensional, meaning that it is based on a tank model and does not take into account the geometry of the reservoir, the drainage areas, the position and orientation of the wells, etc [<xref ref-type="bibr" rid="scirp.77631-ref10">10</xref>] . However, the material balance approach proved to be a very useful tool in this study in performing many tasks i.e. in quantifying different parameters of a reservoir such as hydrocarbon in place, in determining the presence, the type and size of an aquifer, encroachment angle, etc., in predicting the reservoir performance and manifold back pressures for a given production schedule and also in predicting the reservoir performance and well production for a given manifold pressure schedule [<xref ref-type="bibr" rid="scirp.77631-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.77631-ref12">12</xref>] .</p><p>Havlena-Odeh graphical method was adopted to perform material balance calculations which matched with Hurst-Everdingen Dake Radial Aquifer model [<xref ref-type="bibr" rid="scirp.77631-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.77631-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.77631-ref15">15</xref>] . An iterative non linear regression was used to automatically find the best mathematical fit for a given model showed original gas in place of 104 BSCF (<xref ref-type="fig" rid="fig6">Figure 6</xref>).</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Havlena-odeh graphical method of material balance</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x7.png"/></fig><p>Reservoir Driver Mechanism indices are also calculated and plotted (<xref ref-type="fig" rid="fig7">Figure 7</xref>) which translates current average water saturation as 56.6%, which was 48.7% at initial condition. Initial water drive index was 25% but now it is 50%, which means gas expansion within the reservoir has reduced to 50%.</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> RS gas reservoir drive indices</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x8.png"/></fig><p>Material balance estimates are also validated by history matching of production and pressures which showed good match (<xref ref-type="fig" rid="fig8">Figure 8</xref>). A simulation of production is run to check the validity of the results. Gas and water relative per- meabilities are estimated from historical WGR.</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> RS gas reservoir production and pressure simulation</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x9.png"/></fig><p>The accurate and perfect history matching is achieved through simulation which indicates the authenticity and validity of results of different parameters of reservoir as well as aquifer [<xref ref-type="bibr" rid="scirp.77631-ref16">16</xref>] . The models which are used for reservoir and aquifer are correct and the set of pressure used in this modeling also has been proved accurate. This set of pressure has been obtained through the well testing interpretation. As per the matched material balance dynamic model, the yearly water encroachment into the reservoir is given in <xref ref-type="table" rid="table2">Table 2</xref>. The cumulative water production into the reservoir is estimated 23 MMRB. The corrected P/Z Vs G<sub>p</sub> plot has been generated manually too by using Microsoft Excel as shown in <xref ref-type="fig" rid="fig9">Figure 9</xref>. In this corrected P/Z Vs G<sub>p</sub> plot volume of encroached water is incorporated and subtracted.</p><p>The Initial Gas In-Place of RS Gas Field calculated by Material Balance is also verified by Volumetric Reserve Estimation Method. Volumetric Method uses</p><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Corrected P/Z vs G<sub>p</sub> plot of RS gas reservoir</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x10.png"/></fig><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Pressure, gas production and water encroachment of RS gas field</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Year</th><th align="center" valign="middle" >Pressure/ psi</th><th align="center" valign="middle" >Z</th><th align="center" valign="middle" >G<sub>p</sub>/BSCF</th><th align="center" valign="middle" >P/Z</th><th align="center" valign="middle" >We/ MMRB</th><th align="center" valign="middle" >G<sub>p</sub>-(We/Bg) /BSCF</th></tr></thead><tr><td align="center" valign="middle" >Initial</td><td align="center" valign="middle" >2080</td><td align="center" valign="middle" >0.9732</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >2137</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >2011</td><td align="center" valign="middle" >1968</td><td align="center" valign="middle" >0.9725</td><td align="center" valign="middle" >7.2517</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >3.168</td><td align="center" valign="middle" >5.280</td></tr><tr><td align="center" valign="middle" >2012</td><td align="center" valign="middle" >1911</td><td align="center" valign="middle" >0.9723</td><td align="center" valign="middle" >12.713</td><td align="center" valign="middle" >1965</td><td align="center" valign="middle" >7.637</td><td align="center" valign="middle" >8.044</td></tr><tr><td align="center" valign="middle" >2013</td><td align="center" valign="middle" >1866</td><td align="center" valign="middle" >0.9721</td><td align="center" valign="middle" >19.242</td><td align="center" valign="middle" >1920</td><td align="center" valign="middle" >13.935</td><td align="center" valign="middle" >10.607</td></tr><tr><td align="center" valign="middle" >2015</td><td align="center" valign="middle" >1789</td><td align="center" valign="middle" >0.9720</td><td align="center" valign="middle" >27.917</td><td align="center" valign="middle" >1841</td><td align="center" valign="middle" >23.086</td><td align="center" valign="middle" >13.176</td></tr></tbody></table></table-wrap><p>static properties of the reservoir and Material Balance Method is the dynamic model of the reservoir [<xref ref-type="bibr" rid="scirp.77631-ref17">17</xref>] . The following two approaches are used to calculate the IGIP of RS Gas Field.</p><p>Firstly the reservoir is considered as rectangular in shape (<xref ref-type="fig" rid="fig1">Figure 1</xref>0) as classical Reservoir Engineering and petro-physical model employ in the following renowned equation.</p><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Rectangular reservoir</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2890027x11.png"/></fig><disp-formula id="scirp.77631-formula94"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2890027x12.png"  xlink:type="simple"/></disp-formula><p>where G means gas in place (SCF), A is reservoir area (acres), h shows reservoir thickness (feet), θ indicates porosity (fractions), S<sub>wi</sub> is water saturation (fractions) and B<sub>gi</sub> is gas formation volume factor (ft<sup>3</sup>/SCF). 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