<?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>0035-001X</journal-id>
<journal-title><![CDATA[Revista mexicana de física]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. mex. fis.]]></abbrev-journal-title>
<issn>0035-001X</issn>
<publisher>
<publisher-name><![CDATA[Sociedad Mexicana de Física]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0035-001X2006000900021</article-id>
<title-group>
<article-title xml:lang="es"><![CDATA[Efecto de la interacción hidrodinámica en la velocidad de floculación de partículas brownianas]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Toro-Mendoza]]></surname>
<given-names><![CDATA[J]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Urbina-Villalba]]></surname>
<given-names><![CDATA[G]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[García-Sucre]]></surname>
<given-names><![CDATA[M]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Instituto Venezolano de Investigaciones Científicas Centro de Física Laboratorio de Fisicoquímica de Coloides]]></institution>
<addr-line><![CDATA[Caracas ]]></addr-line>
<country>Venezuela</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>05</month>
<year>2006</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>05</month>
<year>2006</year>
</pub-date>
<volume>52</volume>
<fpage>72</fpage>
<lpage>75</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0035-001X2006000900021&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0035-001X2006000900021&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0035-001X2006000900021&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[Se muestra el efecto del fluido sobre el movimiento de partículas Brownianas supendidas. Con el fin de estudiar la velocidad de floculación de una suspensión, se hace uso del algoritmo de Ermak y McCammon [J. Chem. Phys. 69 (1978) 1352] para simular sistemas a varias fracciones de volumen con el mismo número inicial de partículas. Normalmente, la interacción hidrodinámica (IH) se introduce en los algoritmos de dinámica Browniana por medio de tensores de difusión calculados mediante interacciones entre pares de partículas. Estas formulaciones, además de ser computacionalmente costosas, fallan en sistemas densos debido a la sobrestimación de la IH. En este trabajo se emplea una constante de difusión efectiva [Phys. Rev. E 68 (2003) 061408] que incorpora una corrección de la constante de difusión debida a la fracción de volumen local de partículas dispersas, conjuntamente con una formulación exacta de dicha constante para distancias cortas de aproximación. A concentraciones suficientemente diluidas, nuestros resultados reproducen aquellos de la formulación tensorial, corrigiendo las anomalías observadas a concentraciones mayores. Este procedimiento permite la evaluación adecuada de las constantes de floculación en sistemas densos.]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[The effect of the fluid on the movement of suspended Brownian particles is shown. In order to study the flocculation rate of a suspension, Ermak and McCammon's algorithm [J. Chem. Phys. 69 (1978) 1352] is used to simulate systems containing a fixed initial number of particles but different volume fractions. Commonly, Brownian dynamics algorithms introduce hydrodynamic interactions (HI) through two-body diffusion tensors. These formulations are highly demanding in computer time and fail in dense systems due to an overestimation of HI. In this work, an effective diffusion constant is used. It is evaluated at each time from the local volume fraction of particles and an exact formulae valid at short inter particle distances [Phys. Rev. E 68 (2003) 061408]. For very dilute concentrations, our results are in good agreement with those for tensorial formulations, correcting the anomalous coalescence at higher concentrations. This procedure allows an adecuate evaluation of flocculation rates in dense systems.]]></p></abstract>
<kwd-group>
<kwd lng="es"><![CDATA[Floculación]]></kwd>
<kwd lng="es"><![CDATA[interacción hidrodinámica]]></kwd>
<kwd lng="es"><![CDATA[dinámica Browniana]]></kwd>
<kwd lng="es"><![CDATA[suspensiones]]></kwd>
<kwd lng="es"><![CDATA[emulsiones]]></kwd>
<kwd lng="en"><![CDATA[Flocculation]]></kwd>
<kwd lng="en"><![CDATA[hydrodynamic interactions]]></kwd>
<kwd lng="en"><![CDATA[Brownian dynamics]]></kwd>
<kwd lng="en"><![CDATA[suspensions]]></kwd>
<kwd lng="en"><![CDATA[emulsions]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="justify"><font face="verdana" size="4">F&iacute;sica del Petr&oacute;lero</font></p>     <p align="center"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="4"><b>Efecto de la interacci&oacute;n hidrodin&aacute;mica en la velocidad de floculaci&oacute;n de part&iacute;culas brownianas</b></font></p>     <p align="center"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b>J. Toro&#150;Mendoza*, G. Urbina&#150;Villalba y M. Garc&iacute;a&#150;Sucre</b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><i>Laboratorio de Fisicoqu&iacute;mica de Coloides, Centro de F&iacute;sica, Instituto Venezolano de Investigaciones Cient&iacute;ficas, Apartado postal 21827, Caracas, 1020&#150;A, Venezuela, * e&#150;mail: <a href="mailto:jtorom@ivic.ve">jtorom@ivic.ve</a></i></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">Recibido el 24 de noviembre de 2003    <br> Aceptado el 2 de junio de 2004</font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>Resumen</b></font></p>     <p align="justify"><font face="verdana" size="2">Se muestra el efecto del fluido sobre el movimiento de part&iacute;culas Brownianas supendidas. Con el fin de estudiar la velocidad de floculaci&oacute;n de una suspensi&oacute;n, se hace uso del algoritmo de Ermak y McCammon &#91;<i>J. Chem. Phys. </i>69 (1978) 1352&#93; para simular sistemas a varias fracciones de volumen con el mismo n&uacute;mero inicial de part&iacute;culas. Normalmente, la interacci&oacute;n hidrodin&aacute;mica (IH) se introduce en los algoritmos de din&aacute;mica Browniana por medio de tensores de difusi&oacute;n calculados mediante interacciones entre pares de part&iacute;culas. Estas formulaciones, adem&aacute;s de ser computacionalmente costosas, fallan en sistemas densos debido a la sobrestimaci&oacute;n de la IH. En este trabajo se emplea una constante de difusi&oacute;n efectiva &#91;<i>Phys. Rev. E </i>68 (2003) 061408&#93; que incorpora una correcci&oacute;n de la constante de difusi&oacute;n debida a la fracci&oacute;n de volumen local de part&iacute;culas dispersas, conjuntamente con una formulaci&oacute;n exacta de dicha constante para distancias cortas de aproximaci&oacute;n. A concentraciones suficientemente diluidas, nuestros resultados reproducen aquellos de la formulaci&oacute;n tensorial, corrigiendo las anomal&iacute;as observadas a concentraciones mayores. Este procedimiento permite la evaluaci&oacute;n adecuada de las constantes de floculaci&oacute;n en sistemas densos.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Descriptores: </b>Floculaci&oacute;n; interacci&oacute;n hidrodin&aacute;mica; din&aacute;mica Browniana; suspensiones; emulsiones.</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>Abstract</b></font></p>     <p align="justify"><font face="verdana" size="2">The effect of the fluid on the movement of suspended Brownian particles is shown. In order to study the flocculation rate of a suspension, Ermak and McCammon's algorithm <i>&#91;J. Chem. Phys. </i>69 (1978) 1352&#93; is used to simulate systems containing a fixed initial number of particles but different volume fractions. Commonly, Brownian dynamics algorithms introduce hydrodynamic interactions (HI) through two&#150;body diffusion tensors. These formulations are highly demanding in computer time and fail in dense systems due to an overestimation of HI. In this work, an effective diffusion constant is used. It is evaluated at each time from the local volume fraction of particles and an exact formulae valid at short inter particle distances <i>&#91;Phys. Rev. E </i>68 (2003) 061408&#93;. For very dilute concentrations, our results are in good agreement with those for tensorial formulations, correcting the anomalous coalescence at higher concentrations. This procedure allows an adecuate evaluation of flocculation rates in dense systems.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Keywords: </b>Flocculation; hydrodynamic interactions; Brownian dynamics; suspensions; emulsions.</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">PACS: 05.40Jc;83.10Mj;82.70Pe</font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmf/v52s3/v52s3a21.pdf">DESCARGAR ART&Iacute;CULO EN FORMATO PDF</a></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>Referencias</b></font></p>     <!-- ref --><p align="justify"><font face="verdana" size="2">1. D.L. Ermak y J.A. McCammon, <i>J. Chem. Phys. </i><b>69</b> (1978) 1352.&nbsp; &nbsp; &nbsp; &nbsp; &nbsp;</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=8326047&pid=S0035-001X200600090002100001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p align="justify"><font face="verdana" size="2">2. J.K.G. Dhont. <i>An Introduction to Dynamics of <i>Colloids. </i>Elsevier </i>(1996).</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=8326048&pid=S0035-001X200600090002100002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p align="justify"><font face="verdana" size="2">3. G.K. Batchelor, <i>J. Fluid Mech. </i><b>119 </b>(1982) 379.</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=8326049&pid=S0035-001X200600090002100003&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p align="justify"><font face="verdana" size="2">4. J.G. 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