<?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>0185-1101</journal-id>
<journal-title><![CDATA[Revista mexicana de astronomía y astrofísica]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. mex. astron. astrofis]]></abbrev-journal-title>
<issn>0185-1101</issn>
<publisher>
<publisher-name><![CDATA[Universidad Nacional Autónoma de México, Instituto de Astronomía]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0185-11012007000100015</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[A Simple Accretion Model of a Rotating Gas Sphere onto a Schwarzschild Black Hole]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Huerta]]></surname>
<given-names><![CDATA[E. A.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Mendoza]]></surname>
<given-names><![CDATA[S]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Nacional Autónoma de México Instituto de Astronomía ]]></institution>
<addr-line><![CDATA[México D. F.]]></addr-line>
<country>Mexico</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>00</month>
<year>2007</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>00</month>
<year>2007</year>
</pub-date>
<volume>43</volume>
<numero>1</numero>
<fpage>191</fpage>
<lpage>202</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0185-11012007000100015&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0185-11012007000100015&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0185-11012007000100015&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[Construimos un modelo simple de acreción para una esfera de gas que cae hacia un agujero negro de Schwarzschild. Mostramos cómo construir soluciones analíticas en términos de las funciones elípticas de Jacobi. Esta construcción representa una generalización relativista del modelo de acreción Newtoniano primeramente propuesto por Ulrich (1976). De la misma manera en que ocurre para el caso Newtoniano, el flujo predice naturalmente la existencia de un disco de acreción ecuatorial alrededor del agujero. Sin embargo, el radio del disco se incrementa monotónicamente sin límite a medida que el flujo alcanza su mínimo momento angular para este caso en particular.]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[We construct a simple accretion model of a rotating gas sphere onto a Schwarzschild black hole. We show how to build analytic solutions in terms of Jacobi elliptic functions. This construction represents a general relativistic generalisation of the Newtonian accretion model first proposed by Ulrich (1976). In exactly the same form as it occurs for the Newtonian case, the flow naturally predicts the existence of an equatorial rotating accretion disc about the hole. However, the radius of the disc increases monotonically without limit as the flow reaches its minimum allowed angular momentum for this particular model.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[ACCRETION, ACCRETION DISKS]]></kwd>
<kwd lng="en"><![CDATA[HYDRODYNAMICS]]></kwd>
<kwd lng="en"><![CDATA[RELATIVITY]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="center"><font face="verdana" size="4"><b>A SIMPLE ACCRETION MODEL OF A ROTATING GAS SPHERE ONTO A SCHWARZSCHILD BLACK HOLE</b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b>E. A. Huerta &amp; S. Mendoza</b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><i>Instituto de Astronom&iacute;a, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Apdo. Postal 70&#150;264, 04510 M&eacute;xico, D. F., Mexico (<a href="mailto:eahuerta@astroscu.unam.mx">eahuerta@astroscu.unam.mx</a>, <a href="mailto:eahuerta@astroscu.unam.mx">sergio@astroscu.unam.mx</a>)</i></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">Received 2006 October 18    <br>   Accepted 2007 January 17</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>RESUMEN</b></font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">Construimos un modelo simple de acreci&oacute;n para una esfera de gas que cae hacia un agujero negro de Schwarzschild. Mostramos c&oacute;mo construir soluciones anal&iacute;ticas en t&eacute;rminos de las funciones el&iacute;pticas de Jacobi. Esta construcci&oacute;n representa una generalizaci&oacute;n relativista del modelo de acreci&oacute;n Newtoniano primeramente propuesto por Ulrich (1976). De la misma manera en que ocurre para el caso Newtoniano, el flujo predice naturalmente la existencia de un disco de acreci&oacute;n ecuatorial alrededor del agujero. Sin embargo, el radio del disco se incrementa monot&oacute;nicamente sin l&iacute;mite a medida que el flujo alcanza su m&iacute;nimo momento angular para este caso en particular.</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">We construct  a simple accretion model of a rotating gas sphere onto a Schwarzschild black hole. We show how to build analytic solutions in terms of Jacobi elliptic functions. This construction represents a general relativistic generalisation of the Newtonian accretion model first proposed by Ulrich (1976). In exactly the same form as it occurs for the Newtonian case, the flow naturally predicts the existence of an equatorial rotating accretion disc about the hole. However,  the radius of the disc increases monotonically without limit as the flow reaches its minimum allowed angular momentum for this particular model.</font></p>     <p align="justify"><font face="verdana" size="2"><b><i>Key Words:</i></b> ACCRETION, ACCRETION DISKS &#151;         HYDRODYNAMICS       &#151; RELATIVITY</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmaa/v43n1/v43n1a15.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>ACKNOWLEDGEMENTS</b></font></p>     <p align="justify"><font face="verdana" size="2">We dedicate the present article to the vivid memory of Sir Hermann Bondi who pioneered the studies of spherical accretion. We would like to thank William Lee for providing his numerical Paczynsky &amp; Wiita pseudo&#150;Newtonian results in order to make comparisons with the exact analytic solution presented in this article. The authors gratefully acknowledge financial support from DGAPA&#150;Universidad Nacional Aut&oacute;noma de M&eacute;xico (IN119203).</font></p>     ]]></body>
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