<?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>1409-2433</journal-id>
<journal-title><![CDATA[Revista de Matemática Teoría y Aplicaciones]]></journal-title>
<abbrev-journal-title><![CDATA[Rev. Mat]]></abbrev-journal-title>
<issn>1409-2433</issn>
<publisher>
<publisher-name><![CDATA[Centro de Investigaciones en Matemática Pura y Aplicada (CIMPA) y Escuela de Matemática, San José, Costa Rica.]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S1409-24332012000200001</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Asymptotical analysis and padé approximation in problems on diffusion controlled cracks propagation]]></article-title>
<article-title xml:lang="es"><![CDATA[Análisis asintótico y aproximación de padé en problemas de propagación de grietas con difusión controlada]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Balueva]]></surname>
<given-names><![CDATA[Alla V.]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Germanovich]]></surname>
<given-names><![CDATA[Leonid N.]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Gainesville State College Mathematics Department ]]></institution>
<addr-line><![CDATA[Gainesville Georgia]]></addr-line>
<country>U.S.A.</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Georgia Institute of Technology , Department of Civil Engineering ]]></institution>
<addr-line><![CDATA[Atlanta Georgia]]></addr-line>
<country>U.S.A.</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>07</month>
<year>2012</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>07</month>
<year>2012</year>
</pub-date>
<volume>19</volume>
<numero>2</numero>
<fpage>127</fpage>
<lpage>139</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.sa.cr/scielo.php?script=sci_arttext&amp;pid=S1409-24332012000200001&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.sa.cr/scielo.php?script=sci_abstract&amp;pid=S1409-24332012000200001&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.sa.cr/scielo.php?script=sci_pdf&amp;pid=S1409-24332012000200001&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[In this work, we consider the diffusion-controlled axisymmetric fracture in an infinite space, and half-space. An important example of diffusion-controlled fracture growth is given by hydrogen induced cracking. In metals, hydrogen is typically dissolved in the proton form. When protons reach the crack surface, they recombine with electrons and form molecular hydrogen in the crack cavity. Then, the fracture can propagate even in the absence of any external loading, that is, only under the excessive pressure of gas hydrogen accumulated inside the crack. Our results show that in the long-time asymptotic approximation (based on the quasi-static solution), the diffusion-controlled delamination propagates with constant velocity. We determine a maximum critical concentration that limits the use of the quasi-static solution. A transient solution, representing a short-time asymptotic approximation, is used when the concentration of gas exceeds the critical concentration. We then match these two end-member cases by using the method of Padé approximations and present closed-form solutions for both internal and near-surface diffusion-controlled crack propagation at different time scales.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[En este trabajo, consideramos la fractura de difución controlada axisimétrica en un espacio infinito, y en el semiespacio. Un ejemplo importante del crecimiento de una fractura de difusión controlada es dado por el hidrogeno inducido en agrietamiento. En metales, el hidrógeno es típicamente disuelto en forma de protones. Cuando los protones alcanzan la superficie de la grieta, se recombinan con electrones y forman hidrógeno molecular en la cavidad de la grieta. Entonces, la fractura puede propagar aún en ausencia de cualquier carga externa, esto es, sólo bajo presión excesiva de gas hidrogeno acumulado dentro de la grieta. Nuestros resultados muestran que en la aproximación asintótica a largo plazo (basada en la solución cuasiestática), la delaminación de difusión controlada propaga con velocidad constante. Nosotros de- terminamos una concentraci´on crítica máxima que limita el uso de la solución cuasiestática. Una solución transitoria, que representa una aproximación asintótica de corto plazo, es usada cuando la concentración del gas excede la concentración crítica. Entonces apareamos estos dos casos usando el método de aproximaciones de Padé y presentamos soluciones en forma cerrada tanto para propagación de grietas de difusión controlada internas como cercanas a la superficie, en diferentes escalas de tiempo.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[diffusion]]></kwd>
<kwd lng="en"><![CDATA[crack propagation]]></kwd>
<kwd lng="en"><![CDATA[asymptotic analysis]]></kwd>
<kwd lng="en"><![CDATA[Padé approximation]]></kwd>
<kwd lng="es"><![CDATA[difusión]]></kwd>
<kwd lng="es"><![CDATA[propagación de grietas]]></kwd>
<kwd lng="es"><![CDATA[análisis asintótico]]></kwd>
<kwd lng="es"><![CDATA[aproximación de Padé]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  <font 2="" size=""></font>     <div  style="text-align: center; font-family: verdana; font-weight: bold;"><font  2="" size="+1">Asymptotical analysis and pad&eacute; approximation in problems on diffusion controlled cracks propagation    <br>     <br> An&aacute;lisis asint&oacute;tico y aproximaci&oacute;n de pad&eacute; en problemas de propagaci&oacute;n de grietas con difusi&oacute;n controlada    <br> </font></div> <font 2="" size=""><br style="font-family: verdana;"> </font><font 2="" size=""><font size="-1"><span  style="font-family: verdana;">Alla V. Balueva<a href="#Afiliacion1">*</a><a name="Afiliacion3"></a>+</span></font></font><br  style="font-family: verdana;"> <font 2="" size=""><font size="-1"><span style="font-family: verdana;">Leonid N. Germanovich<a href="#Afiliacion2">&#8224;</a><a name="Afiliacion4"></a>*</span></font></font>    <br> <font 2="" size=""><font size="-1"><span style="font-family: verdana;"></span></font></font><font  2="" size=""><font size="-1"><span style="font-family: verdana;"><a  href="mailto:leonid@ce.gatech.edu"></a><a href="#correspondencia">    <br> </a><a name="Correspondencia2"></a>*<a href="#Correspondencia1">Direcci&oacute;n para correspondencia</a><br style="font-family: verdana;"> </span></font></font><font 2="3"><span  style="font-family: verdana; font-weight: bold;"></span></font> <hr  style="width: 100%; height: 2px; margin-left: 0px; margin-right: 0px;"><font  2="3"><span style="font-family: verdana; font-weight: bold;">Abstract</span></font><br  style="font-family: verdana;"> <br style="font-family: verdana;">     <div style="text-align: justify;"><font 2="" size=""><font size="-1"><span  style="font-family: verdana;">In this work, we consider the diffusion-controlled axisymmetric fracture in an infinite space, and half-space. An important example of diffusion-controlled fracture growth is given by hydrogen induced cracking. In metals, hydrogen is typically dissolved in the proton form. When protons reach the crack surface, they recombine with electrons and form molecular hydrogen in the crack cavity.&nbsp; Then, the fracture can propagate even in the absence of any external loading, that is, only under the excessive pressure of gas hydrogen accumulated inside the crack. </span></font></font><br  style="font-family: verdana;"> </div> <br style="font-family: verdana;">     <div style="text-align: justify;"><font 2="" size=""><font size="-1"><span  style="font-family: verdana;">Our results show that in the long-time asymptotic approximation (based on the quasi-static solution), the diffusion-controlled delamination propagates with constant velocity. We determine a maximum critical concentration that limits the use of the quasi-static solution. A transient solution, representing a short-time asymptotic approximation, is used when the concentration of gas exceeds the critical concentration. We then match these two end-member cases by using the method of Pad&eacute; approximations and present closed-form solutions for both internal and near-surface diffusion-controlled crack propagation at different time scales.</span></font></font><br style="font-family: verdana;"> </div> <br style="font-family: verdana;">     <div style="text-align: justify;"><font 2="" size=""><font size="-1"><span  style="font-family: verdana;"><span style="font-weight: bold;">Keywords:</span> diffusion, crack propagation, asymptotic analysis, Pad&eacute; approximation.</span></font></font><br  style="font-family: verdana;"> </div> <br style="font-family: verdana;"> <font 2=""><span style="font-family: verdana; font-weight: bold;">Resumen</span></font><br  style="font-family: verdana; font-weight: bold;"> <br style="font-family: verdana;">     ]]></body>
<body><![CDATA[<div style="text-align: justify;"><font 2="" size=""><font size="-1"><span  style="font-family: verdana;">En este trabajo, consideramos la fractura de difuci&oacute;n controlada axisim&eacute;trica en un espacio infinito, y en el semiespacio. Un ejemplo importante del crecimiento de una fractura de difusi&oacute;n controlada es dado por el hidrogeno inducido en agrietamiento. En metales, el hidr&oacute;geno es t&iacute;picamente disuelto en forma de protones. Cuando los protones alcanzan la superficie de la grieta, se recombinan con electrones y forman hidr&oacute;geno molecular en la cavidad de la grieta. Entonces, la fractura puede propagar a&uacute;n en ausencia de cualquier carga externa, esto es, s&oacute;lo bajo presi&oacute;n excesiva de gas hidrogeno acumulado dentro de la grieta.</span></font></font><br  style="font-family: verdana;"> </div> <br style="font-family: verdana;">     <div style="text-align: justify;"><font 2="" size=""><font size="-1"><span  style="font-family: verdana;">Nuestros resultados muestran que en la aproximaci&oacute;n asint&oacute;tica a largo plazo (basada en la soluci&oacute;n cuasiest&aacute;tica), la delaminaci&oacute;n de difusi&oacute;n controlada propaga con velocidad constante. Nosotros de- terminamos una concentraci&oacute;n cr&iacute;tica m&aacute;xima que limita el uso de la </span></font></font><font 2=""  size=""><font size="-1"><span style="font-family: verdana;">soluci&oacute;n cuasiest&aacute;tica. Una soluci&oacute;n transitoria, que representa una aproximaci&oacute;n asint&oacute;tica de corto plazo, es usada cuando la concentraci&oacute;n del gas excede la concentraci&oacute;n cr&iacute;tica.&nbsp; Entonces apareamos estos dos casos usando el m&eacute;todo de aproximaciones de Pad&eacute; y presentamos soluciones en forma cerrada tanto para propagaci&oacute;n de grietas de difusi&oacute;n controlada internas como cercanas a la superficie, en diferentes escalas de tiempo.</span></font></font><br  style="font-family: verdana;"> </div> <br style="font-family: verdana;">     <div style="text-align: justify;"><font 2="" size=""><font size="-1"><span  style="font-family: verdana;"><span style="font-weight: bold;">Palabras clave:</span> difusi&oacute;n, propagaci&oacute;n de grietas, an&aacute;lisis asint&oacute;tico, aproximaci&oacute;n de Pad&eacute;.</span></font></font><br  style="font-family: verdana;"> </div> <br style="font-family: verdana;">     <div style="text-align: justify;"><font 2="" size=""><font size="-1"><span  style="font-family: verdana;"><span style="font-weight: bold;">Mathematics Subject Classification:</span> 74A45, 74N25, 41A21.</span></font></font><br  style="font-family: verdana;"> </div> <font 2=""><span style="font-family: verdana; font-weight: bold;"></span></font> <hr  style="width: 100%; height: 2px; margin-left: 0px; margin-right: 0px;"><font  2=""><span style="font-family: verdana;"></span></font>    <br> <font 2=""><span style="font-family: verdana;"><font size="-1">Ver contenido disponible en pdf</font></span><span  style="font-family: verdana; font-weight: bold;"></span></font>    <br> <font 2=""><span style="font-family: verdana; font-weight: bold;"></span></font>    <br> <font 2=""><span style="font-family: verdana; font-weight: bold;"></span></font> <hr  style="width: 100%; height: 2px; margin-left: 0px; margin-right: 0px;"><font  2=""><span style="font-family: verdana; font-weight: bold;"></span></font>    <!-- ref --><br> <font 2=""><span style="font-family: verdana; font-weight: bold;">References</span></font><br  style="font-family: verdana; font-weight: bold;"> <br style="font-family: verdana;"> <font 2="" size=""><font size="-1"><span style="font-family: verdana;">[1] Balueva, A.V; Dashevski, I.D. 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E-Mail: a<a href="mailto:balueva@gsc.edu">balueva@gsc.edu</a></font><font  size="-1"><br style="font-family: verdana;"> </font><font style="font-family: verdana;" 2="" size="-1">Leonid N. Germanovich. </font><font style="font-family: verdana;" 2=""  size="-1">Georgia Institute of Technology, Department of Civil Engineering, Atlanta, Georgia, U.S.A. E-Mail: <a href="mailto:leonid@ce.gatech.edu">leonid@ce.gatech.edu</a>    <br> </font><font 2="" size=""><font size="-1"><span  style="font-family: verdana;">    <br> <a name="Afiliacion1"></a><a href="#Afiliacion3">*</a>Gainesville State College, Mathematics Department, P.O. Box 1358, Gainesville, Georgia, U.S.A. E-Mail: <a href="mailto:abalueva@gsc.edu">abalueva@gsc.edu</a></span></font></font><br  style="font-family: verdana;"> <font 2="" size=""><font size="-1"><span style="font-family: verdana;"><a  name="Afiliacion2"></a><a href="#Afiliacion4">&#8224;</a>Georgia Institute of Technology, Department of Civil Engineering, Atlanta, Georgia, U.S.A. E-Mail: <a href="mailto:leonid@ce.gatech.edu">leonid@ce.gatech.edu</a></span></font></font>    <br> <font 2="" size=""><font size="-1"><span style="font-family: verdana;"></span></font></font><font  2="" size=""><font size="-1"><span style="font-family: verdana;"></span></font></font><font  2="" size="-1"><span style="font-family: verdana;"></span></font> <hr style="width: 100%; height: 2px;">     <div style="text-align: center;"><font style="font-weight: bold;" 2=""  size="-1"><span style="font-family: verdana;">Received: 18 Feb 2010; Revised: 28 Jun 2012; Accepted: 29 Jun 2012</span></font>    <br> </div>      ]]></body><back>
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