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DTSTART:20150423T110000
DTEND:20150423T120000
SUMMARY:Wetting Phenomena: Competitive Effects of Surface Tension and Elasticity on Thin and/or Soft Solids
DESCRIPTION:<p style="text-align: left;">A DCAMM seminar&nbsp;will be presented by </p>\n<p style="text-align: center;"><strong>Professor Martin E.R. Shanahan<br />\n12M, CNRS 5295<br />\nUniversit&eacute; de Bordeaux, France</strong><strong>&nbsp;<br />\n<br />\n</strong></p>\n<p style="text-align: left;"><strong>Abstract</strong>: <br />\n<br />\n<span>The simple equation attributed to Young describing the equilibrium of a liquid, L, on a solid substrate, S, in the presence of a second, immiscible fluid (which we take to be vapour, V) and involving surface/interfacial tensions, <em>&gamma;</em><sub>ij</sub>, (i, j = S, L, or V) and contact angle, <em>&theta;</em>, &nbsp;is over two centuries old, yet still hides secrets! Amongst various poorly understood aspects, the role played by the component of liquid &nbsp;surface tension perpendicular to the solid surface, <em>&gamma;</em> sin<em>&theta;</em>&nbsp; (where<em> &gamma;</em><sub>LV</sub>&nbsp; = &gamma;, for brevity) has remained unknown for a very long time, or even &ldquo;forgotten&rdquo;! We consider here various situations in which &gamma; sin<em>&theta;</em> cannot be neglected, as well as some observations reported in the lite-&nbsp;&nbsp;&nbsp; rature which can thus, at least in part, be explained by the apparently unbalanced term.<br />\n<br />\n</span><span>We discuss two specific cases of the problem: that in which the solid is intrinsically &ldquo;hard&rdquo; (metal, glass, etc.) yet very thin, and that of a semi-infinite solid but of low elastic modulus (elastomer, gel, etc.).</span></p>\n<p style="text-align: left;"> <span>The problems may be approached either by variational techniques to obtain the configuration of minimal free energy, or by consideration &nbsp;&nbsp;&nbsp;of force balance. In both cases, we obtain equations describing solid deformations due to capillary forces. Some consequences of these deformations are discussed, in particular the stability or instability of solids shapes when in contact with a liquid, recently referred to as &ldquo;elastocapillary origami&rdquo;, modification of Young&rsquo;s equation, and &ldquo;viscoelastic braking&rdquo;, i.e. reduction of wetting or dewetting rates on elastomeric solids. We also consider some results to be found in the literature in the light of these studies, including in the context of metallurgy.</span>All interested persons are invited. </p>\n<p style="text-align: left;">All interested persons are invited</p>
X-ALT-DESC;FMTTYPE=text/html:<p style="text-align: left;">A DCAMM seminar&nbsp;will be presented by </p>\n<p style="text-align: center;"><strong>Professor Martin E.R. Shanahan<br />\n12M, CNRS 5295<br />\nUniversit&eacute; de Bordeaux, France</strong><strong>&nbsp;<br />\n<br />\n</strong></p>\n<p style="text-align: left;"><strong>Abstract</strong>: <br />\n<br />\n<span>The simple equation attributed to Young describing the equilibrium of a liquid, L, on a solid substrate, S, in the presence of a second, immiscible fluid (which we take to be vapour, V) and involving surface/interfacial tensions, <em>&gamma;</em><sub>ij</sub>, (i, j = S, L, or V) and contact angle, <em>&theta;</em>, &nbsp;is over two centuries old, yet still hides secrets! Amongst various poorly understood aspects, the role played by the component of liquid &nbsp;surface tension perpendicular to the solid surface, <em>&gamma;</em> sin<em>&theta;</em>&nbsp; (where<em> &gamma;</em><sub>LV</sub>&nbsp; = &gamma;, for brevity) has remained unknown for a very long time, or even &ldquo;forgotten&rdquo;! We consider here various situations in which &gamma; sin<em>&theta;</em> cannot be neglected, as well as some observations reported in the lite-&nbsp;&nbsp;&nbsp; rature which can thus, at least in part, be explained by the apparently unbalanced term.<br />\n<br />\n</span><span>We discuss two specific cases of the problem: that in which the solid is intrinsically &ldquo;hard&rdquo; (metal, glass, etc.) yet very thin, and that of a semi-infinite solid but of low elastic modulus (elastomer, gel, etc.).</span></p>\n<p style="text-align: left;"> <span>The problems may be approached either by variational techniques to obtain the configuration of minimal free energy, or by consideration &nbsp;&nbsp;&nbsp;of force balance. In both cases, we obtain equations describing solid deformations due to capillary forces. Some consequences of these deformations are discussed, in particular the stability or instability of solids shapes when in contact with a liquid, recently referred to as &ldquo;elastocapillary origami&rdquo;, modification of Young&rsquo;s equation, and &ldquo;viscoelastic braking&rdquo;, i.e. reduction of wetting or dewetting rates on elastomeric solids. We also consider some results to be found in the literature in the light of these studies, including in the context of metallurgy.</span>All interested persons are invited. </p>\n<p style="text-align: left;">All interested persons are invited</p>

URL:http://www.dcamm.dk/da/Kalender/2015/04/Seminar_No_682
DTSTAMP:20260927T042900Z
UID:{0115C4AE-74C5-4A54-89F6-74C22007771F}-20150423T110000-20150423T110000
LOCATION: Room 05.060, Aarhus University, Department of Engineering, Inge Lehmanns Gade 10, 8000  Aarhus C
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