<?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>1870-3542</journal-id>
<journal-title><![CDATA[Revista mexicana de física E]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. mex. fís. E]]></abbrev-journal-title>
<issn>1870-3542</issn>
<publisher>
<publisher-name><![CDATA[Sociedad Mexicana de Física]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S1870-35422008000200007</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Mathematics motivated by physics: the electrostatic potential is the Coulomb integral transform of the electric charge density]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Medina]]></surname>
<given-names><![CDATA[L]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Ley Koo]]></surname>
<given-names><![CDATA[E]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Nacional Autónoma de México Facultad de Ciencias ]]></institution>
<addr-line><![CDATA[México D.F]]></addr-line>
<country>México</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Nacional Autónoma de México Instituto de Física ]]></institution>
<addr-line><![CDATA[México D.F]]></addr-line>
<country>Mexico</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>12</month>
<year>2008</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>12</month>
<year>2008</year>
</pub-date>
<volume>54</volume>
<numero>2</numero>
<fpage>153</fpage>
<lpage>159</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S1870-35422008000200007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S1870-35422008000200007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S1870-35422008000200007&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[This article illustrates a practical way to connect and coordinate the teaching and learning of physics and mathematics. The starting point is the electrostatic potential, which is obtained in any introductory course of electromagnetism from the Coulomb potential and the superposition principle for any charge distribution. The necessity to develop solutions to the Laplace and Poisson differential equations is also recognized, identifying the Coulomb potential as the generating function of harmonic functions. Correspondingly, the convenience of expressing the electrostatic potential in terms of its multipole expansion in spherical coordinates, or as integral transforms based on harmonic functions in different coordinate systems, is also established. These connections provide a motivation for teachers and students to acquire the necessary mathematics as a basic tool in the study of electromagnetic theory, optics and quantum mechanics]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Este artículo ilustra una manera práctica de conectar y coordinar la enseñanza y aprendizaje de la física y las matemáticas. El punto de partida es el potencial electroestático que se obtiene en el curso introductorio de electromagnetismo a partir del potencial de Coulomb y del principio de superposición para cualquier distribución de carga. También se reconoce la necesidad de construir soluciones de las ecuaciones diferenciales de Laplace y de Poisson, identificando al potencial de Coulomb como una función generadora de funciones armónicas. Correspondientemente, también se reconoce la conveniencia de expresar al potencial electroestático en términos de su desarrollo multipolar en coordenadas esféricas, o de transformadas integrales basadas en funciones armónicas en diferentes sistemas de coordenadas. Estas conexiones proporcionan una motivación para maestros y alumnos para adquirir las matemáticas necesarias como una herramienta básica en el estudio de la teoría electromagnética, la óptica y mecánica cuántica]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Electrostatics]]></kwd>
<kwd lng="en"><![CDATA[Laplace and Poisson equations]]></kwd>
<kwd lng="en"><![CDATA[spherical and circular cylindrical Harmonic functions]]></kwd>
<kwd lng="es"><![CDATA[Electroestática]]></kwd>
<kwd lng="es"><![CDATA[ecuaciones diferenciales de Laplace y de Poisson]]></kwd>
<kwd lng="es"><![CDATA[funciones armónicas esféricas y cilindricas circulares]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="justify"><font face="verdana" size="4">Ense&ntilde;anza</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="4"><b>Mathematics motivated by physics: the electrostatic potential is the Coulomb integral transform of the electric charge density</b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="center"><font face="verdana" size="2"><b>L. Medina&ordf; and E. Ley Koo<sup>a,b</sup></b></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><i>&ordf; Facultad de Ciencias, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Ciudad Universitaria, M&eacute;xico D.F., 04510, M&eacute;xico, </i>e&#150;mail: <a href="mailto:lumg@fciencias.unam.mx">lumg@fciencias.unam.mx</a><i>,</i></font></p>     <p align="justify"><font face="verdana" size="2"><i><sup>b </sup>Instituto de F&iacute;sica, Universidad Nacional Aut&oacute;noma de M&eacute;xico, Apartado Postal 20&#150;364, 01000 M&eacute;xico D.F., Mexico, </i>e&#150;mail: <a href="mailto:eleykoo@fisica.unam.mx">eleykoo@fisica.unam.mx</a></font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2">Recibido el 19 de octubre de 2007    ]]></body>
<body><![CDATA[<br> Aceptado el 11 de marzo de 2007</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">This article illustrates a practical way to connect and coordinate the teaching and learning of physics and mathematics. The starting point is the electrostatic potential, which is obtained in any introductory course of electromagnetism from the Coulomb potential and the superposition principle for any charge distribution. The necessity to develop solutions to the Laplace and Poisson differential equations is also recognized, identifying the Coulomb potential as the generating function of harmonic functions. Correspondingly, the convenience of expressing the electrostatic potential in terms of its multipole expansion in spherical coordinates, or as integral transforms based on harmonic functions in different coordinate systems, is also established. These connections provide a motivation for teachers and students to acquire the necessary mathematics as a basic tool in the study of electromagnetic theory, optics and quantum mechanics.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Keywords: </b>Electrostatics; Laplace and Poisson equations; spherical and circular cylindrical Harmonic functions.</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>     <p align="justify"><font face="verdana" size="2">Este art&iacute;culo ilustra una manera pr&aacute;ctica de conectar y coordinar la ense&ntilde;anza y aprendizaje de la f&iacute;sica y las matem&aacute;ticas. El punto de partida es el potencial electroest&aacute;tico que se obtiene en el curso introductorio de electromagnetismo a partir del potencial de Coulomb y del principio de superposici&oacute;n para cualquier distribuci&oacute;n de carga. Tambi&eacute;n se reconoce la necesidad de construir soluciones de las ecuaciones diferenciales de Laplace y de Poisson, identificando al potencial de Coulomb como una funci&oacute;n generadora de funciones arm&oacute;nicas. Correspondientemente, tambi&eacute;n se reconoce la conveniencia de expresar al potencial electroest&aacute;tico en t&eacute;rminos de su desarrollo multipolar en coordenadas esf&eacute;ricas, o de transformadas integrales basadas en funciones arm&oacute;nicas en diferentes sistemas de coordenadas. Estas conexiones proporcionan una motivaci&oacute;n para maestros y alumnos para adquirir las matem&aacute;ticas necesarias como una herramienta b&aacute;sica en el estudio de la teor&iacute;a electromagn&eacute;tica, la &oacute;ptica y mec&aacute;nica cu&aacute;ntica.</font></p>     <p align="justify"><font face="verdana" size="2"><b>Descriptores: </b>Electroest&aacute;tica; ecuaciones diferenciales de Laplace y de Poisson; funciones arm&oacute;nicas esf&eacute;ricas y cilindricas circulares. </font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">PACS:41.20.Cv1</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><a href="/pdf/rmfe/v54n2/v54n2a7.pdf" target="_blank">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>Acknowledgement</b></font></p>     <p align="justify"><font face="verdana" size="2">One of the authors (E.L.K.) on sabbatical leave at the University of Wisconsin&#150;Milwaukee with support from DGAPA&#150;UNAM wishes to thank Professor Hans Volkmer of the School of Mathematical Sciences for his hospitality.</font></p>     <p align="justify"><font face="verdana" size="2">&nbsp;</font></p>     <p align="justify"><font face="verdana" size="2"><b>References</b></font></p>     <!-- ref --><p align="justify"><font face="verdana" size="2">1. I.   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