<?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>S1870-35422011000100009</article-id>
<title-group>
<article-title xml:lang="es"><![CDATA[La fuerza normal: ¿una fuerza conservativa?]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Díaz-Solórzano]]></surname>
<given-names><![CDATA[S.]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[González-Díaz]]></surname>
<given-names><![CDATA[L.]]></given-names>
</name>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Pedagógica Experimental Libertador (UPEL) Instituto Pedagógico de Caracas Departamento de Matemáticas y Física]]></institution>
<addr-line><![CDATA[Caracas ]]></addr-line>
<country>Venezuela</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>06</month>
<year>2011</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>06</month>
<year>2011</year>
</pub-date>
<volume>57</volume>
<numero>1</numero>
<fpage>51</fpage>
<lpage>56</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S1870-35422011000100009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S1870-35422011000100009&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S1870-35422011000100009&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[La fuerza normal es una fuerza de ligadura que surge del contacto entre un objeto y una superficie. Esta fuerza puede conservar la energía mecánica de un sistema o no. Se muestra que dicha fuerza es conservativa cuando la superficie no evoluciona en el tiempo, así como la tasa a la cual varía la energía mecánica cuando la fuerza normal es no conservativa. Para esta última situación, se propone la función energía pseudo-potencial asociada a la fuerza normal con la finalidad de obtener la ecuacion de movimiento del objeto sometido a dicha fuerza a partir de consideraciones energéticas.]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[The normal force is a constraint force that arises from the contact between an object and a surface. This force can preserve the mechanical energy of a system or not. It is shown that normal force is conservative when the surface does not evolve over time, as well as the rate to which the mechanical energy changes when the normal force is not conservative. For the latter situation, it is proposed the pseudo-potential energy function associated to normal force in order to obtain from energetic considerations the equation of movement of the object under the above mentioned force.]]></p></abstract>
<kwd-group>
<kwd lng="es"><![CDATA[Fuerza normal]]></kwd>
<kwd lng="es"><![CDATA[energía mecánica y trabajo]]></kwd>
<kwd lng="es"><![CDATA[energía pseudo-potencial]]></kwd>
<kwd lng="en"><![CDATA[Normal force]]></kwd>
<kwd lng="en"><![CDATA[mechanical energy and word]]></kwd>
<kwd lng="en"><![CDATA[pseudo-potential energy]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  	    <p align="justify"><font face="verdana" size="4">Ense&ntilde;anza</font></p> 	    <p align="center"><font face="verdana" size="2">&nbsp;</font></p> 	    <p align="center"><font face="verdana" size="4"><b>La fuerza normal: &iquest;una fuerza conservativa?</b></font></p> 	    <p align="center"><font face="verdana" size="2">&nbsp;</font></p> 	    <p align="center"><font face="verdana" size="2"><b>S. D&iacute;az&#150;Sol&oacute;rzano and L. Gonz&aacute;lez&#150;D&iacute;az</b></font></p> 	    <p align="justify"><font face="verdana" size="2">&nbsp;</font></p> 	    <p align="justify"><font face="verdana" size="2"><i>Centro de Investigaciones de Matem&aacute;tica y F&iacute;sica, Departamento de Matem&aacute;ticas y F&iacute;sica, Instituto Pedag&oacute;gico de Caracas, UPEL, Av. P&aacute;ez, Caracas 1021, Venezuela, e&#150;mail:</i> <a href="mailto:srafael@ipc.upel.edu.ve">srafael@ipc.upel.edu.ve</a>; <a href="mailto:lagdelul@gmail.com">lagdelul@gmail.com</a></font></p> 	    <p align="justify"><font face="verdana" size="2">&nbsp;</font></p> 	    <p align="justify"><font face="verdana" size="2">Recibido el 25 de octubre de 2010    ]]></body>
<body><![CDATA[<br>     Aceptado el 29 de marzo de 2011</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">La fuerza normal es una fuerza de ligadura que surge del contacto entre un objeto y una superficie. Esta fuerza puede conservar la energ&iacute;a mec&aacute;nica de un sistema o no. Se muestra que dicha fuerza es conservativa cuando la superficie no evoluciona en el tiempo, as&iacute; como la tasa a la cual var&iacute;a la energ&iacute;a mec&aacute;nica cuando la fuerza normal es no conservativa. Para esta &uacute;ltima situaci&oacute;n, se propone la funci&oacute;n energ&iacute;a pseudo&#150;potencial asociada a la fuerza normal con la finalidad de obtener la ecuacion de movimiento del objeto sometido a dicha fuerza a partir de consideraciones energ&eacute;ticas.</font></p> 	    <p align="justify"><font face="verdana" size="2"><b>Descriptores:</b> Fuerza normal; energ&iacute;a mec&aacute;nica y trabajo; energ&iacute;a pseudo&#150;potencial.</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 normal force is a constraint force that arises from the contact between an object and a surface. This force can preserve the mechanical energy of a system or not. It is shown that normal force is conservative when the surface does not evolve over time, as well as the rate to which the mechanical energy changes when the normal force is not conservative. For the latter situation, it is proposed the pseudo&#150;potential energy function associated to normal force in order to obtain from energetic considerations the equation of movement of the object under the above mentioned force.</font></p> 	    <p align="justify"><font face="verdana" size="2"><b>Keywords:</b> Normal force; mechanical energy and word; pseudo&#150;potential energy.</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: 01.55+b; 45.20.D&#150;; 45.20dg; 45.20dh</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/v57n1/v57n1a9.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>Referencias</b></font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">1. A. French,<i> Mec&aacute;nica Newtoniana</i> Ed. 1ra <i>Tomo 1</i> (Editorial Reverte, Espa&ntilde;a, 1974).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456055&pid=S1870-3542201100010000900001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <p align="justify"><font face="verdana" size="2">2. Un v&iacute;nculo hol&oacute;nomo es un v&iacute;nculo geom&eacute;trico que no depende de las velocidades. Se escribe como <img src="/img/revistas/rmfe/v57n1/a9e1.jpg">, donde las <i>N</i> variables corresponden a los vectores posici&oacute;n de cada una de las part&iacute;culas que conforman el sistema f&iacute;sico en consideraci&oacute;n y la variable <i>t</i> representa el tiempo &#91;15&#93;.</font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">3. L.A. Pars, <i>A treatise on analytical dynamics</i> Ed. 1ra, (Heinemann, London, 1965);    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456058&pid=S1870-3542201100010000900002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --> L. Meirovitch, <i>Methods of analytical dynamics</i> (McGraw&#150;Hill, New York, 1970).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456059&pid=S1870-3542201100010000900003&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">4. R. Serway y J. Jewett, <i>F&iacute;sica para ciencias e ingenier&iacute;a</i> Vol. 1 (International Thomson, M&eacute;xico, 2005);    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456061&pid=S1870-3542201100010000900004&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --> M. Alonso y E. Finn, <i>F&iacute;sica: Mec&aacute;nica</i> Vol 1. (Fondo Educativo Interamericano, 1976).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456062&pid=S1870-3542201100010000900005&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">5. D. Keeports, <i>Phys. Educ.</i> <b>41</b> (2006) 219.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456064&pid=S1870-3542201100010000900006&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">6. T. Chow, <i>Classical mechanincs</i> (John Wiley &amp; Sons, New York, 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=8456066&pid=S1870-3542201100010000900007&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --> H. Goldstein, <i>Classical Mechanincs</i> Ed. 2da, (Addison&#150;Wesley Publishing Company, Philippines, 1980);    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456067&pid=S1870-3542201100010000900008&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --> J. Jr. Norwood, <i>Mecanica Clasica a nivel intermedio,</i> (Editorial Dossat, Espa&ntilde;a, 1981);    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456068&pid=S1870-3542201100010000900009&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --> H.J.W. M&uuml;ller&#150;Kirsten, <i>Classical Mechanics and Relativity,</i> (World Scientific, Singapur, 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=8456069&pid=S1870-3542201100010000900010&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">7. J.R. Gaskill and M. Arenstein, <i>Amer. Jour. Phys</i> <b>37</b> (1969) 93.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456071&pid=S1870-3542201100010000900011&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">8. J. Jos&eacute; y E. Saletan, <i>Classical Dynamics: A contemporary approach</i> (Cambridge University Press, New York, 1998).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456073&pid=S1870-3542201100010000900012&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">9. I.V. Sav&eacute;liev, <i>Curso de f&iacute;sica general: Mec&aacute;nica y F&iacute;sica Molecular</i> Tomo 1 (Mir, Mosc&uacute;, 1984).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456075&pid=S1870-3542201100010000900013&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    <p align="justify"><font face="verdana" size="2">10. Un v&iacute;nculo reh&oacute;nomo es un v&iacute;nculo que depende expl&iacute;citamente del tiempo &#91;16&#93;.</font></p> 	    <!-- ref --><p align="justify"><font face="verdana" size="2">11 . L.A. Santal&oacute;, <i>Vectores y tensores con sus aplicaciones</i> Ed. 10ma, (Editorial Universitaria de Buenos Aires, Argentina, 1976).    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=8456078&pid=S1870-3542201100010000900014&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></font></p> 	    ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">12. Una situaci&oacute;n f&iacute;sica en la cual el multiplicador depende del tiempo y el v&iacute;nculo no, surge al considerar fuerzas externas dependientes del tiempo.</font></p> 	    <p align="justify"><font face="verdana" size="2">13. Un v&iacute;nculo escler&oacute;nomo o estacionario es un v&iacute;nculo que no depende expl&iacute;citamente del tiempo &#91;15&#93;.</font></p> 	    <p align="justify"><font face="verdana" size="2">14. S. D&iacute;az&#150;Solorzano y L. Gonz&aacute;lez&#150;D&iacute;az, en preparaci&oacute;n.</font></p>      ]]></body><back>
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<given-names><![CDATA[L.A.]]></given-names>
</name>
</person-group>
<source><![CDATA[Vectores y tensores con sus aplicaciones]]></source>
<year>1976</year>
<edition>Ed. 10ma</edition>
<publisher-name><![CDATA[Editorial Universitaria de Buenos Aires]]></publisher-name>
</nlm-citation>
</ref>
</ref-list>
</back>
</article>
