<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>0012-7353</journal-id>
<journal-title><![CDATA[DYNA]]></journal-title>
<abbrev-journal-title><![CDATA[Dyna rev.fac.nac.minas]]></abbrev-journal-title>
<issn>0012-7353</issn>
<publisher>
<publisher-name><![CDATA[Universidad Nacional de Colombia]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0012-73532014000300011</article-id>
<article-id pub-id-type="doi">10.15446/dyna.v81n185.36469</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Straight-Line Conventional Transient Pressure Analysis for Horizontal Wells with Isolated Zones]]></article-title>
<article-title xml:lang="es"><![CDATA[Análisis Convencional de Pruebas de Presión en Pozos Horizontales con Zonas Aisladas]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Escobar]]></surname>
<given-names><![CDATA[Freddy Humberto]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Meneses]]></surname>
<given-names><![CDATA[Alba Rolanda]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Losada]]></surname>
<given-names><![CDATA[Liliana Marcela]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Surcolombiana/CENIGAA Facultad de Ingeniería ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
<country>Colombia</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>06</month>
<year>2014</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>06</month>
<year>2014</year>
</pub-date>
<volume>81</volume>
<numero>185</numero>
<fpage>78</fpage>
<lpage>85</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_arttext&amp;pid=S0012-73532014000300011&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_abstract&amp;pid=S0012-73532014000300011&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_pdf&amp;pid=S0012-73532014000300011&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[It is common in the oil industry to complete horizontal wells selectively. Even, this selection is performed naturally since reservoir heterogeneity may cause segmented well performance. Segmentation may be partially open to flux due to high skin factor or low permeability bands. They can be treated as a nonuniform skin distribution. A few models have been introduced to capture these special details. Existing interpretation methodologies use non-linear regression analysis and the TDS technique; but, there is an absence of equations for the conventional technique. In this study, the conventional methodology is developed for the analysis of pressure transient tests in horizontal wells with isolated zones so directional permeabilities and skin factors can be obtained. The developed expressions were tested successfully with several examples reported in the literature and compared to results from other sources.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Es común en la industria petrolera completar los pozos en forma selectiva. Incluso, dicha selección se efectúa de forma natural ya que la heterogeneidad del yacimiento podría causar comportamiento segmentado del pozo. La segmentación podría estar parcialmente abierto al flujo en virtud a la alto factor de daño bajas vetas de permeabilidad. Ellas pueden tratarse como una distribución no uniforme del factor de daño. Algunos pocos modelos se han introducido para capturar estos detalles especiales. Las metodologías de interpretación existentes usan análisis de regresión no lineal y la técnica TDS; pero, se adolece de ecuaciones para el método convencional. En este estudio se desarrolla la metodología convencional para la interpretación de pruebas de presión en pozos horizontales con zonas aisladas de modo que se puedan estimar las permeabilidades y los factores de daño. Las expresiones desarrolladas se probaron satisfactoriamente con varios problemas encontrados en la literatura y se compararon con los resultados procedentes de otras fuentes.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Horizontal well]]></kwd>
<kwd lng="en"><![CDATA[isolation zones]]></kwd>
<kwd lng="en"><![CDATA[partial completion]]></kwd>
<kwd lng="en"><![CDATA[flow regimes]]></kwd>
<kwd lng="es"><![CDATA[Pozo horizontal]]></kwd>
<kwd lng="es"><![CDATA[zonas aisladas]]></kwd>
<kwd lng="es"><![CDATA[completamiento parcial]]></kwd>
<kwd lng="es"><![CDATA[regímenes de flujo]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="left"><a href="http://dx.doi.org/10.15446/dyna.v81n185.36469" target="_blank">http://dx.doi.org/10.15446/dyna.v81n185.36469</a></p>      <p align="center"><font size="4" face="Verdana"><b>Straight-Line  Conventional Transient Pressure Analysis for Horizontal Wells with Isolated  Zones</b></font></p>     <p align="center"><i><font size="3"><b><font face="Verdana">An&aacute;lisis  Convencional de Pruebas de Presi&oacute;n en Pozos Horizontales con Zonas Aisladas</font></b></font></i></p>     <p align="center">&nbsp;</p>     <p align="center"><b><font size="2" face="Verdana">Freddy Humberto Escobar <sup>a</sup>,  Alba Rolanda Meneses <sup>b</sup> &amp; Liliana Marcela Losada <sup>c</sup></font></b><font size="2" face="Verdana"></font></p>     <p align="center">&nbsp;</p>     <p align="center"><font size="2" face="Verdana"><sup><i>a</i></sup><i> Facultad de Ingenier&iacute;a.,Universidad Surcolombiana/CENIGAA, Colombia, <a href="mailto:fescobar@usco.edu.co">fescobar@usco.edu.co</a>    <br>  <sup>b</sup> Facultad de Ingenier&iacute;a, Universidad Surcolombiana/CENIGAA,  Colombia, <a href="mailto:albita_meneses@hotmail.com">albita_meneses@hotmail.com</a>    <br>  <sup>c</sup> Facultad de Ingenier&iacute;a, Universidad Surcolombiana/CENIGAA, <a href="mailto:lilianalosada@outlook.com">lilianalosada@outlook.com</a></i></font></p>     <p align="center">&nbsp;</p>     ]]></body>
<body><![CDATA[<p align="center"><font size="2" face="Verdana"><b>Received: January  22<sup>th</sup>, 2013. Received in revised form: January 23<sup>th</sup>, 2014. Accepted: January  30<sup>th</sup>, 2014</b></font></p>     <p>&nbsp;</p> <hr>     <p><font size="2" face="Verdana"><b>Abstract    <br>  </b></font><font size="2" face="Verdana">It is common in  the oil industry to complete horizontal wells selectively. Even, this selection  is performed naturally since reservoir heterogeneity may cause segmented well  performance. Segmentation may be partially open to flux due to high skin factor  or low permeability bands. They can be treated as a nonuniform skin  distribution. A few models have been introduced to capture these special  details. Existing interpretation methodologies use non-linear regression  analysis and the <i>TDS</i> technique; but,  there is an absence of equations for the conventional technique. In this study,  the conventional methodology is developed for the analysis of pressure  transient tests in horizontal wells with isolated zones so directional  permeabilities and skin factors can be obtained. The developed expressions were  tested successfully with several examples reported in the literature and  compared to results from other sources. </font></p>     <p><font size="2" face="Verdana"><i>Key Words</i>: Horizontal well, isolation zones,  partial completion, flow regimes.</font></p>     <p><font size="2" face="Verdana"><b>Resumen    <br>  </b></font><font size="2" face="Verdana">Es com&uacute;n en la industria petrolera completar los pozos  en forma selectiva. Incluso, dicha selecci&oacute;n se efect&uacute;a de forma natural ya que  la heterogeneidad del yacimiento podr&iacute;a causar comportamiento segmentado del  pozo. La segmentaci&oacute;n podr&iacute;a estar parcialmente abierto al flujo en virtud a la alto factor de da&ntilde;o bajas vetas de  permeabilidad. Ellas pueden tratarse como una distribuci&oacute;n no uniforme del  factor de da&ntilde;o. Algunos pocos modelos se han introducido para capturar estos  detalles especiales. Las metodolog&iacute;as de interpretaci&oacute;n existentes usan  an&aacute;lisis de regresi&oacute;n no lineal y la t&eacute;cnica <i>TDS</i>; pero, se adolece de ecuaciones para el m&eacute;todo convencional. En  este estudio se desarrolla la metodolog&iacute;a convencional para la interpretaci&oacute;n  de pruebas de presi&oacute;n en pozos horizontales con zonas aisladas de modo que se  puedan estimar las permeabilidades y los factores de da&ntilde;o. Las expresiones  desarrolladas se probaron satisfactoriamente con varios problemas encontrados  en la literatura y se compararon con los resultados procedentes de otras  fuentes. </font></p>     <p><font size="2" face="Verdana"><i>Palabras  clave</i>: Pozo horizontal, zonas aisladas, completamiento  parcial, reg&iacute;menes de flujo.</font></p> <hr>     <p>&nbsp;</p>     <p><font size="3" face="Verdana"><b>1. Introduction</b></font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana">Selective completion is  a current operation performed on horizontal wells. Reservoir heterogeneity may  also cause segmentation due to low permeability bands &#91;1&#93;. As indicated by &#91;1&#93;,  &#91;2&#93; and &#91;3&#93; the existence of an intermediate late radial or pseudorradial flow regime is the most important  feature of the transient-pressure response of segmented horizontal wells. They  found that the semilog slope of the late radial flow regime is affected by the  number of equal-length segments. </font></p>     <p><font size="2" face="Verdana">Horizontal wells with isolated areas can be a practical  solution for such problems presented in different formations such as gas/water  coning, sand production and asphalt production; however, it has a great impact  in the skin factor. Currently, the  characterization of locations is important since it is a valuable tool which  allows for the determination of the best exploitation scenario. </font></p>     <p><font size="2" face="Verdana">Recently,  &#91;4&#93; introduced a new model for the type of geometry here discussed. They made a  detailed discussion of the importance and impact of selective horizontal well  completion. Also, they formulated the <i>TDS </i>methodology, initially introduced by &#91;5&#93; for horizontal wells, for  interpretation of well pressure tests in segmented horizontal wells. In this  study, the solution proposed by &#91;4&#93; is used to develop equations to be used in  the conventional straight-line methodology and successfully applied to field  examples provided by &#91;4&#93; and &#91;6&#93;. The results of the estimated permeabilities  in the <i>x</i> and <i>z</i> directions and skin factors were compared with those from &#91;4&#93;  using the <i>TDS</i> technique. Escobar et  al. &#91;7&#93; have indicated the importance of the traditional-conventional analysis  even in transient-rate tests interpretation. </font></p>     <p><font size="2" face="Verdana">So far, the only available methodology for well test interpretation  in the systems under consideration was the one presented by &#91;4&#93; following the  philosophy of the TDS technique &#91;8&#93;. However, the importance of its application  is based upon some examples recently reported in the literature. For instance, &#91;9&#93;  presented some examples for the use of zonal isolations in horizontal well  completions in a hydraulic fracturing treatment which was conducted with five  packer isolation systems so that five isolated zones were created. On the other  hand, &#91;10&#93; introduced some field examples for well testing procedures in  multi-zone openhole completion wells in which casing annulus packers, instead  of cement, were used to provide the isolations.</font></p>     <p>&nbsp;</p>     <p><font size="3" face="Verdana"><b>2 Formulation</b></font></p>     <p><b><font size="2" face="Verdana">2.1. Mathematical Model    <br>  </font></b><font size="2" face="Verdana">The model developed by &#91;1&#93; corresponds to the dimensionless  pressure governing equation based upon the following assumptions: (1)  homogeneous reservoir, with constant and uniform thickness with closed top and  bottom boundaries. (2) Anisotropic system but with constant porosity and  permeability in each direction, (3) negligible frictional and gravitational  effects, and (4) the well extends in the midpoint of the formation height.</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq01.gif"></p>     <p><font size="2" face="Verdana">In which the dimensionless  parameters are as follows:</font></p>     ]]></body>
<body><![CDATA[<p><img src="img/revistas/dyna/v81n185/v81n185a11eq0211.gif"></p>     <p><font size="2" face="Verdana"><b>2.2. General equation of horizontal wells with  isolated zones    <br>  </b></font><font size="2" face="Verdana">Flow regimes in horizontal wells depend upon several  issues mainly related to geometry. When the ratio of the wellbore length to the  reservoir thickness, LD, is less than 5 the well acts a single source/sink,  then, early spherical flow develops. As example of such case is sketched in <a href="#fig01">Fig.  1</a>. If 5 &lt; LD &lt; 20 then, vertical  early-radial flow takes places, however, if LD becomes larger than 20 then  early-radial flow cannot be seen since the formation thickness results too thin  compared to the wellbore length and the top and bottom of the formation are  quickly reached. </font></p>     <p align="center"><font size="2" face="Verdana"><a name="fig01"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig01.gif"></p>     <p><font size="2" face="Verdana">As stated before, radial flow regime develops in short  horizontal wells (L<sub>D</sub>=20) with or without isolated zones. The  governing expression presented by &#91;4&#93; is given by:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq12.gif"></p>     <p><font size="2" face="Verdana">When <i>Z</i>=0, Equation 12 becomes:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq13.gif"></p>     <p><font size="2" face="Verdana">Replacing the dimensionless quantities in Equation (13),  dividing by the natural log of 10 and solving for the well-flowing pressure, it  yields:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq14.gif"></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana">The slope, <i>m<sub>ER</sub></i>,  from a semilog plot of pressure versus time allows for the estimation of (<i>k<sub>y</sub>k<sub>z</sub></i>)<sup>0.5</sup>,</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq15.gif"></p>     <p><font size="2" face="Verdana">The sketch of <a href="#fig02">Fig. 2</a> shows the development of an  intermediate radial flow when a horizontal well possesses isolated zones  indicating that 5 &lt; <i>L<sub>D </sub></i>&lt;  20. The governing dimensionless pressure derivative equation for such flow  regime is:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq16.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig02"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig02.gif"></p>     <p><font size="2" face="Verdana">Since the semilog slope is natural log of 10 times higher  than the pressure derivative value, Equation (16) allows one to find an expression to find the horizontal  permeability, (<i>k<sub>x</sub>k<sub>y</sub></i>)<sup>0.5</sup> from the semilog slope, <i>m<sub>ER</sub></i>, once the dimensionless pressure derivative  is placed in oilfield units; </font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq17.gif"></p>     <p><font size="2" face="Verdana">As described by <a href="#fig03">Fig. 3</a>, the pseudo-spherical (or two  hemispherical) flow develops when the length of the</font></p>     <p align="center"><font size="2" face="Verdana"><a name="fig03"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig03.gif"></p>     <p><font size="2" face="Verdana">perforated area is so short compared  to the formation thickness forcing the well to act as a single source/sink. The  dimensionless pressure derivative governing equation presented by &#91;4&#93; is;</font></p>     ]]></body>
<body><![CDATA[<p><img src="img/revistas/dyna/v81n185/v81n185a11eq18.gif"></p>     <p><font size="2" face="Verdana">Integration of the  Equation (18) leads us to obtain the dimensionless pressure for such flow  regime:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq19.gif"></p>     <p><font size="2" face="Verdana">Replacing the  dimensionless terms, we obtain:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq20.gif"></p>     <p><font size="2" face="Verdana">The slope  of a Cartesian plot of pressure versus the inverse square root of time, mps,  allows one to calculate (kx)0.5, knowing mps of a Cartesian graph.</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq21.gif"></p>     <p><font size="2" face="Verdana">Needless to say that the pseudo-spherical skin factor can  be obtained from the intercept of such a plot.</font></p>     <p><font size="2" face="Verdana">In long horizontal wells (LD&gt;20), the early radial flow  regime is hardly seen while early linear flow is dominant in the proximities to  the well. The governing dimensionless pressure derivative equation for this  linear flow is given by &#91;4&#93;, </font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq22.gif"></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana">Integration of  Equation 22 leads to the dimensionless pressure governing equation; </font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq23.gif"></p>     <p><font size="2" face="Verdana">After replacing the dimensionless quantities, we obtain:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq231.gif"></p>     <p><font size="2" face="Verdana">Equation (23) suggests that a plot of pressure versus the  square root of time provides a straight line whose slope <i>m<sub>EL</sub></i> can be used to estimate the square root of <i>k<sub>y</sub></i>, </font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq24.gif"></p>     <p><font size="2" face="Verdana"><a href="#fig04">Fig. 4</a> shows that once early-radial flow vanishes, the  well acts as a hydraulic fracture, then linear flow develops. A long horizontal  well (L<sub>D</sub>&gt;20) with a high number of isolated zones also exhibits  an early linear flow regime which is effective to the whole wellbore. The  dimensionless pressure derivative governing equation was presented by &#91;4&#93; as  follows:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq25.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig04"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig04.gif"></p>     <p><font size="2" face="Verdana">After integration of Equation 25, we obtain:</font></p>     ]]></body>
<body><![CDATA[<p><img src="img/revistas/dyna/v81n185/v81n185a11eq26.gif"></p>     <p><font size="2" face="Verdana">Once the dimensionless terms are replaced the expression  for the dimensionless pressure is presented:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq27.gif"></p>     <p><font size="2" face="Verdana">A plot of pressure versus the square root of time should a  straight line which slope,<i> m<sub>EL</sub></i>, <i> </i>allows  the estimation of <i>k<sub>y</sub></i><sup>0.5</sup>,</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq28.gif"></p>     <p>&nbsp;</p>     <p><font size="2" face="Verdana">At later time, the pseudorradial or late radial flow  regime develops in the horizontal plane without any influence of the vertical permeability.  See <a href="#fig05">Fig. 5</a>. The dimensionless pressure governing equation was also introduced  by &#91;4&#93; as follows:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq29.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig05"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig05.gif"></p>     <p><font size="2" face="Verdana">In oilfield units;</font></p>     ]]></body>
<body><![CDATA[<p><img src="img/revistas/dyna/v81n185/v81n185a11eq30.gif"></p>     <p><font size="2" face="Verdana">This flow regime corresponds to the radial flow regime observed  in vertical wells. The dimensionless pressure derivative equation is:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq31.gif"></p>     <p><font size="2" face="Verdana">Equation (31) is useful  to calculate the horizontal permeability (<i>k<sub>x</sub>k<sub>y</sub></i>)<sup>0.5</sup> if the semilog slope of a plot of pressure versus time, <i>m<sub>PR</sub></i>, is estimated during this flow regime, as:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eq32.gif"></p>     <p><font size="2" face="Verdana">Such later flow regimes as late linear and pseudosteady  state are similar to conventional horizontal wells.</font></p>     <p><font size="2" face="Verdana">Different expressions to estimate the skin factors are  provided in Appendix A.</font></p>     <p>&nbsp;</p>     <p><font size="3" face="Verdana"><b>3. Examples </b></font></p>     <p><font size="2" face="Verdana">Example 1 was taken from &#91;4&#93;. Examples 2 and 3 were taken  from &#91;6&#93;. In both cases the examples were worked by the <i>TDS</i> technique.</font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana"><b>3.1. Example 1    <br>  </b><a href="#fig06">Fig. 6</a> presents pressure and pressure derivative data for  a pressure drawdown test run in a horizontal well having two equal-length  isolated zones, each of 400 ft. Other known reservoir and well data are:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11par01.gif"></p>     <p><font size="2" face="Verdana">Estimate formation permeability in all directions using  the conventional technique.</font></p>     <p align="center"><font size="2" face="Verdana"><a name="fig06"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig06.gif"></p>     <p><font size="2" face="Verdana">Solution. Three flow regimes are clearly seen in <a href="#fig06">Fig. 6</a>: early radial, early linear  and pseudorradial. A semilog slope <i>m<sub>PR</sub></i> of 448 psi/cycle is found from <a href="#fig07">Fig. 7</a> during the late radial flow regime.  Equation 32 allows estimating a horizontal permeability, (<i>k<sub>x</sub>k<sub>y</sub></i>)<sup>0.5</sup> of 0.87 md. The Cartesian plot of pressure  versus the square root of time given in <a href="#fig08">Fig. 8</a> provides a slope, <i>m<sub>EL</sub></i>, of 82 psi/hr<sup>0.5</sup>.  Using Equation 24 a value of <i>k<sub>y</sub></i> of 1.57  md is found. Knowing (<i>k<sub>x</sub>k<sub>y</sub></i>)<sup>0.5 </sup>and <i>k<sub>y</sub></i>, a value of <i>k<sub>x</sub></i> of 0.49 md is readily obtained. From <a href="#fig09">Fig. 9</a>, a semilog slope, <i>m<sub>ER</sub></i>, of 23 psi/cycle during  the early radial flow regime is used to calculate a value of </font><font size="2" face="Verdana">(<i>k<sub>y</sub>k<sub>z</sub></i>)<sup>0.5</sup> of 0.88 md using Equation 17. From this, a value of 0.49 for <i>k<sub>z</sub></i> is then found.</font></p>     <p align="center"><font size="2" face="Verdana"><a name="fig07"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig07.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig08"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig08.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig09"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig09.gif"></p>     <p><font size="2" face="Verdana"><b>3.2. Example 2    ]]></body>
<body><![CDATA[<br>  </b>The pressure and  pressure derivative data for a drawdown test of a horizontal well are given in <a href="#fig10">Fig. 10</a>. Other relevant data are given as follows:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11par02.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig10"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig10.gif"></p>     <p><font size="2" face="Verdana">Solution. Early radial, early linear,  intermediate radial and pseudorradial flow regimes are clearly seen in the  pressure derivative curve of <a href="#fig10">Fig. 10</a>. A slope, <i>m<sub>IR</sub></i>, of 80.92 psi/cycle is obtained from the semilog  plot given in <a href="#fig11">Fig. 11</a> which allows to estimate a (<i>k<sub>y</sub>k<sub>z</sub></i>)<sup>0.5</sup> value of 2.82 md using  Equation 15. Then, using a slope of 100.68 psi/hr<sup>0.5</sup> read from <a href="#fig12">Fig. 12</a>, a <i>y</i>-direction permeability of 4.12 md is obtained by means of  Equation 24. <i>k<sub>z</sub></i> is readily  found from (<i>k<sub>y</sub>k<sub>z</sub></i>)<sup>0.5 </sup>and <i>k<sub>y</sub></i> to be 1.94  md.</font></p>     <p align="center"><font size="2" face="Verdana"><a name="fig11"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig11.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig12"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig12.gif"></p>     <p><font size="2" face="Verdana"><b>3.3. Example 3    <br>  </b><a href="#fig13">Figure 13</a> contains the  pressure and pressure derivative data form a drawdown test of a horizontal  well presented by &#91;6&#93;. </font></p>     <p align="center"><font size="2" face="Verdana"><a name="fig13"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig13.gif"></p>     <p><font size="2" face="Verdana">Reservoir, fluid and well parameters  are given below:</font></p>     ]]></body>
<body><![CDATA[<p><img src="img/revistas/dyna/v81n185/v81n185a11par03.gif"></p>     <p><font size="2" face="Verdana">Solution. From the pressure and pressure derivative log-log  plot of <a href="#fig13">Fig. 13</a> the early linear and pseudorradial flow regimes are clearly observed. The semilog slope during  the pseudorradial flow regime, <a href="#fig14">Figure 14</a>, mPR = 54.08 psi/cycle, leads to the  estimation of a horizontal permeability value (kxky)0.5 of 17.73 md. A  Cartesian slope during linear flow, mEL = 30.71 psi/hr0.5, obtained from <a href="#fig15">Fig. 15</a> is used to estimate a  ky = 15.04 md from Equation 24. kx is then estimated to be 20.9 md. </font></p>     <p align="center"><font size="2" face="Verdana"><a name="fig14"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig14.gif"></p>     <p align="center"><font size="2" face="Verdana"><a name="fig15"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11fig15.gif"></p>     <p>&nbsp;</p>     <p><font size="3" face="Verdana"><b>4. Comments on the  Result</b></font></p>     <p><font size="2" face="Verdana"><a href="#tab01">Table 1</a> presents the results obtained from  this work and compared to the values reported by &#91;1&#93; and &#91;2&#93;. Notice that the  deviation errors of the results obtained in this work are acceptable indicating  that the equations developed work well.</font></p>     <p align="center"><font size="2" face="Verdana"><a name="tab01"></a></font><img src="img/revistas/dyna/v81n185/v81n185a11tab01.gif"></p>     <p>&nbsp;</p>     <p><b><font size="3" face="Verdana">5. CONCLUSION</font></b></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana">The  straight-line conventional method for pressure-transient analysis was  complemented with new equations for horizontal wells with isolated zones. The  equations were successfully applied to examples reported in the literature and  provided similar results to the <i>TDS</i> technique. </font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11nom01.gif"></p>     <p><font size="2" face="Verdana">Apendix A. Skin factor Equations</font></p>     <p><font size="2" face="Verdana">The mechanical skin  factor from Equation 14 is:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eqA1.gif"></p>     <p><font size="2" face="Verdana">The pseudo-spherical skin factor from Equation 20 is:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eqA2.gif"></p>     <p><font size="2" face="Verdana">The total skin factor from Equation 23 is:</font></p>     <p><img src="img/revistas/dyna/v81n185/v81n185a11eqA3.gif"></p>     <p><font size="2" face="Verdana">The total skin factor from Equation 30 is:</font></p> <img src="img/revistas/dyna/v81n185/v81n185a11eqA4.gif">     ]]></body>
<body><![CDATA[<p>&nbsp;</p>     <p><font size="3" face="Verdana"><b>References </b></font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;1&#93;</b> Kamal, M.M., Buhidma, I.M., Smith, S.A., and Jones, W.R., Pressure Transient Analysis for a Well with Multiple Horizontal Sections. Paper SPE 26444, SPE Annual Technical Conference and Exhibition, Houston, 3-6 October. 1993</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000135&pid=S0012-7353201400030001100001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p> <font size="2" face="Verdana"><b>&#91;2&#93;</b> Ozkan, E., Analysis of Horizontal Well-Responses: Contemporary vs. Conventional. SPEREE 4 (4). pp. 260-269, 2001.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000136&pid=S0012-7353201400030001100002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;3&#93;</b> Yildiz, T. And Oskan, E., Transient Pressure Behavior of Selectively Completed Horizontal Wells. Paper SPE 28388, SPE Annual Technical Conference and Exhibition, New Orleans, USA, pp. 25-28 Sep., 1994.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000138&pid=S0012-7353201400030001100003&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;4&#93;</b> Al Rbeawi, S. And D. Tiab, D., Effect of the Number and Length of Zonal Isolations on Pressure Behavior of Horizontal Wells. Paper SPE 142177, SPE production and operations Symposium held in Oklahoma City, Oklahoma, USA, pp. 27-29 March. 2011.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000140&pid=S0012-7353201400030001100004&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;5&#93;</b> Engler, T. W. And Tiab, D., Analysis of Pressure and Pressure Derivatives without Type-Curve Matching. 6- Horizontal Well Tests in Anisotropic Reservoirs. Journal of Petroleum Science and Engineering, 15, pp. 153-168, 1996.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000142&pid=S0012-7353201400030001100005&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;6&#93;</b> Al Rbeawi, S., Interpretation of Pressure Transient Tests of Horizontal Wells With Multiple Hydraulic Fractures and Zonal Isolations. &#91;PhD Thesis&#93;. Norman, OK: The University of Oklahoma, 2012.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000144&pid=S0012-7353201400030001100006&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;7&#93;</b> Escobar, F.H., Rojas, M.M. and Cantillo, J.H., Straight-Line Conventional Transient Rate Analysis for Long Homogeneous and Heterogeneous Reservoirs. Dyna. year 79, (172), pp. 153-163, 2012</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000146&pid=S0012-7353201400030001100007&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p> <font size="2" face="Verdana"><b>&#91;8&#93;</b> Tiab, D., 1995, Analysis of Pressure and Pressure Derivative without Type-Curve Matching: 1- Skin and Wellbore Storage&quot;. Journal of Petroleum Science and Engineering, Vol 12, pp. 171-181. 1995.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000147&pid=S0012-7353201400030001100008&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;9&#93;</b> Maddox, B., Wahrton, M., Hinkie, R., Farabee, M. and Ely, J., Cementless Multi-Zone Horizontal Completion Yields Three-Fold Increase&quot;. Paper IADC/SPE 112774 presented at the IADC/SPE Drilling Conference in Orlando, FL. March, pp. 4-6, 2008.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000149&pid=S0012-7353201400030001100009&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p>     <!-- ref --><p> <font size="2" face="Verdana"><b>&#91;10&#93;</b> Brooks, R.T. and Scott, S., Improvement and Testing Multi-Zone Open-Hole Carbonate Formations. Paper SPE 119426 presented at the Middle East Oil and Gas Conference. Bahrain. March, pp. 15-18, 2009.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000151&pid=S0012-7353201400030001100010&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </font></p>     ]]></body>
<body><![CDATA[<p>&nbsp;</p>     <p><font size="2" face="Verdana"><b>Freddy Humberto  Escobar</b>, received a BSc degree from Universidad de America in 1989, both the  MSc received in 1995 and the PhD in 2002 were obtained from the University of  Oklahoma. All his degrees are in Petroleum Engineering. Dr. Escobar joined  Universidad Surcolombiana in 1996 and is the director of the Research Group on  Transient Well Testing and the president of Cenigaa (Research Center for  Sciences and geo-agro-environmental resources).</font></p>     <p><font size="2" face="Verdana"><b>Alba Rolanda  Meneses</b>, received her BSc in Petroleum Engineering from Universidad  Surcolombiana in 2013. She has recently joined Schlumberger Limited as a field  engineer.</font></p>     <p><font size="2" face="Verdana"><b>Liliana Marcela  Losada</b>, received her BSc in Petroleum Engineering from Universidad  Surcolombiana in 2013.</font></p>      ]]></body><back>
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