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	<title>GRASP &#124; Soft Matter &#124; University of Liège</title>
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	<link>http://grasp-lab.org</link>
	<description>frequent updates on our research</description>
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		<title>GRASP &#124; Soft Matter &#124; University of Liège</title>
		<link>http://grasp-lab.org</link>
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		<item>
		<title>Spin-Leidenfrost</title>
		<link>http://grasp-lab.org/2013/04/01/spin-leidenfrost/</link>
		<comments>http://grasp-lab.org/2013/04/01/spin-leidenfrost/#comments</comments>
		<pubDate>Sun, 31 Mar 2013 22:00:01 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[From the lab]]></category>
		<category><![CDATA[droplet]]></category>

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		<description><![CDATA[The ESA ‘Spin Your Thesis!’ programme gives university students the opportunity to perform a scientific or technology experiment which is linked to their project, by participating in a centrifuge campaign that provides hypergravity conditions. The experiments are carried out in the &#8230; <a href="http://grasp-lab.org/2013/04/01/spin-leidenfrost/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=799&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://nicovdw.files.wordpress.com/2013/03/ldc.jpg"><img class="alignleft size-medium wp-image-800" alt="LDC" src="http://nicovdw.files.wordpress.com/2013/03/ldc.jpg?w=300&#038;h=199" width="300" height="199" /></a>The ESA ‘Spin Your Thesis!’ programme gives university students the opportunity to perform a scientific or technology experiment which is linked to their project, by participating in a centrifuge campaign that provides hypergravity conditions. The experiments are carried out in the ESA Large Diameter Centrifuge facility at ESTEC in Noordwijk, the Netherlands.</p>
<p><span style="color:#ff0000;">Our PhD students have been selected for their project on Leidenfrost droplets</span> !</p>
<p>See <a href="http://www.esa.int/Education/Spin_Your_Thesis!_2013_teams_selected">the ESA web pages</a>.</p>
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		<title>Quandrops website</title>
		<link>http://grasp-lab.org/2013/03/26/quandrops/</link>
		<comments>http://grasp-lab.org/2013/03/26/quandrops/#comments</comments>
		<pubDate>Tue, 26 Mar 2013 07:49:44 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[From the lab]]></category>
		<category><![CDATA[bouncing]]></category>
		<category><![CDATA[droplet]]></category>

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		<description><![CDATA[The website dedicated to our project &#8220;QUANDROPS&#8221; (2012-2017) is now open. This project aims to study the particle-wave association of bouncing droplets. In recent experiments, such droplets have indeed displayed a number of surprising analogies with quantum particles, including tunneling and &#8230; <a href="http://grasp-lab.org/2013/03/26/quandrops/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=783&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://nicovdw.files.wordpress.com/2013/02/quandrops_logo_small.jpg"><img class="alignleft size-thumbnail wp-image-784" alt="quandrops_logo_small" src="http://nicovdw.files.wordpress.com/2013/02/quandrops_logo_small.jpg?w=150&#038;h=129" width="150" height="129" /></a>The <a href="http://www.quandrops.ulg.ac.be">website</a> dedicated to our project &#8220;QUANDROPS&#8221; (2012-2017) is now open. This project aims to study the particle-wave association of bouncing droplets. In recent experiments, such droplets have indeed displayed a number of surprising analogies with quantum particles, including tunneling and double-slit interference. Those droplets can therefore be considered as a classical manifestation of quantum wave-particle duality in the spirit of Bohm&#8217;s interpretation of quantum mechanics.</p>
<p>Please also note the beautiful logo of this new project !</p>
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		<item>
		<title>Pulses in a vertical granular column</title>
		<link>http://grasp-lab.org/2013/02/21/column/</link>
		<comments>http://grasp-lab.org/2013/02/21/column/#comments</comments>
		<pubDate>Thu, 21 Feb 2013 08:43:24 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[Article]]></category>
		<category><![CDATA[chaos]]></category>
		<category><![CDATA[collision]]></category>
		<category><![CDATA[granular matter]]></category>

		<guid isPermaLink="false">http://grasp-lab.org/?p=739</guid>
		<description><![CDATA[We investigated the dynamics of a vertical column of 12 beads submitted to a series of taps. Impulses are strong enough to eject beads. The motion of the beads are recorded using a high-speed camera. Depending on the frequency of taps, &#8230; <a href="http://grasp-lab.org/2013/02/21/column/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=739&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://grasp-lab.org/2013/02/21/column/trajectories_beads/" rel="attachment wp-att-741"><img class="alignleft size-full wp-image-741" alt="trajectories_beads" src="http://nicovdw.files.wordpress.com/2012/12/trajectories_beads.png?w=640&#038;h=232" width="640" height="232" /></a></p>
<p>We investigated the dynamics of a vertical column of 12 beads submitted to a series of taps. Impulses are strong enough to eject beads. The motion of the beads are recorded using a high-speed camera. Depending on the frequency of taps, complex trajectories are obtained as illustrated in the front picture. The trajectories are analyzed in our last article [1].</p>
<p>For low tap frequencies, the pulses travel through the pile and expel a few beads from the surface. After a few bounces, the system relaxes to the chain of contacting grains. When the tap frequency increases, fluidization is obtained. In the fluidized part of the pile, adjacent beads are bouncing in opposition of phase (see top picture). <span style="color:#3366ff;">This phase locking of the top beads is observed even when the bottom beads experience chaotic motions</span>. While the mechanical energy increases monotically with the bead vertical position, <span style="color:#3366ff;">heterogeneous patterns in the kinetic energy distribution</span> are found when the system becomes fluidized.</p>
<p>[1] G. Lumay, S. Dorbolo, O. Gerasymov and N. Vandewalle, <span style="color:#3366ff;"><em>Experimental study of a vertical column of grains submitted to a series of impulses</em></span>, Eur. Phys. J. E <span style="text-decoration:underline;">36</span> , 16 (2013) &#8211; <a href="http://www.grasp.ulg.ac.be/article/2013_lumay_EPJE.pdf">PDF</a></p>
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		<title>Self-assembled microswimmers</title>
		<link>http://grasp-lab.org/2013/01/30/microswimmers/</link>
		<comments>http://grasp-lab.org/2013/01/30/microswimmers/#comments</comments>
		<pubDate>Wed, 30 Jan 2013 20:08:56 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[Article]]></category>
		<category><![CDATA[locomotion]]></category>
		<category><![CDATA[magnetism]]></category>
		<category><![CDATA[microfluidics]]></category>
		<category><![CDATA[self-assembly]]></category>

		<guid isPermaLink="false">http://grasp-lab.org/?p=695</guid>
		<description><![CDATA[Locomotion at low Reynolds number is a key physical mechanism [1] for microscopic living organisms, but has lots of technological applications like nanomachines and microrobots [2]. Our last paper [3] proposes a tricky experiment for generating low Reynolds swimming of &#8230; <a href="http://grasp-lab.org/2013/01/30/microswimmers/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=695&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://grasp-lab.org/2013/01/30/microswimmers/assemblies/" rel="attachment wp-att-698"><img class="alignleft size-medium wp-image-698" alt="self-assembly" src="http://nicovdw.files.wordpress.com/2012/12/assemblies.jpg?w=300&#038;h=129" width="300" height="129" /></a><a href="http://brodylab.eng.uci.edu/~jpbrody/reynolds/lowpurcell.html"><span style="color:#ff0000;">Locomotion at low Reynolds number</span></a> is a key physical mechanism [1] for microscopic living organisms, but has lots of technological applications like <span style="color:#ff0000;">nanomachines and microrobots</span> [2]. Our last paper [3] proposes a tricky experiment for generating low Reynolds swimming of microscopic particles along a liquid-air interface.</p>
<p>First, identical soft ferromagnetic particles are placed on a liquid-air interface. Capillary attraction is prevented by applying a vertical magnetic field which provides a repulsive interaction between the particles.<span style="color:#ff0000;"> <a title="Magnetic Cheerios Effect" href="http://grasp-lab.org/2012/04/23/magnetic-cheerios-effect-self-assembly-driven-by-a-magnetic-field/"><span style="color:#ff0000;">The balance of capillary attraction and magnetic repulsion creates a self-assembly</span></a> </span>[4] as shown in the front picture. These structures are then perturbed by applying an oscillating horizontal field. The resulting cooperative dance of the particles provides a net propulsion of the particles along the liquid surface (see trajectories on the picture below). <span style="color:#ff0000;">The self-assembly is swimming ! <span style="color:#333333;">See the movies below :</span></span></p>
<ul>
<li><span style="line-height:16px;"><a href="http://www.grasp.ulg.ac.be/article/movieSwimmers1.mov" target="_blank">Movie 1</a> - An efficient swimmer of N=3 beads. </span></li>
<li><a href="http://www.grasp.ulg.ac.be/article/movieSwimmers2.mov" target="_blank">Movie 2</a> - The horizontal field is switched off. The swimmer is seen to stop its motion. Then the field is switched on but in another direction. The motion resumes but in a different pulsating mode (with a different swimming speed).</li>
<li><a href="http://www.grasp.ulg.ac.be/article/movieSwimmers3.mov" target="_blank">Movie 3</a> - The complex motion of a swimming (pentagonal) assembly made of N=6 beads.</li>
</ul>
<p><a href="http://grasp-lab.org/2013/01/30/microswimmers/traj/" rel="attachment wp-att-700"><img class="size-medium wp-image-700 alignright" alt="swimming" src="http://nicovdw.files.wordpress.com/2012/12/traj.jpg?w=300&#038;h=105" width="300" height="105" /></a></p>
<p>This work opens new perspectives in mesoscopic physics. <span style="color:#ff0000;">The most important feature of our system is that both self-assembling and periodic deformations can be rescaled to smaller sizes.</span></p>
<p><strong>References</strong></p>
<p>[1] E.Lauga, Soft Matter <span style="text-decoration:underline;">7</span>, 3060 (2011)<br />
[2] P.Tierno, R.Golestanian, I.Pagonabarraga, and F.Sagués, Phys. Rev. Lett. <span style="text-decoration:underline;">101</span>, 218304 (2008)<br />
[3] G.Lumay, N.Obara, F.Weyer, N.Vandewalle, Soft Matter <span style="text-decoration:underline;">9</span>, 2420 (2013) - <a href="http://www.grasp.ulg.ac.be/article/2013_lumay_SM.pdf">PDF</a><br />
[4] N.Vandewalle et al., Phys. Rev. E <span style="text-decoration:underline;">85</span>, 041402 (2012) - <a href="http://www.grasp.ulg.ac.be/article/2012_vandewalle_PRE2.pdf">PDF</a> - <a title="Magnetic Cheerios Effect" href="http://nicovdw.wordpress.com/2012/04/23/magnetic-cheerios-effect-self-assembly-driven-by-a-magnetic-field/">Post</a></p>
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			<media:title type="html">swimming</media:title>
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		<title>Faraday instability at foam/water interface</title>
		<link>http://grasp-lab.org/2013/01/10/faraday/</link>
		<comments>http://grasp-lab.org/2013/01/10/faraday/#comments</comments>
		<pubDate>Thu, 10 Jan 2013 19:34:41 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[Article]]></category>
		<category><![CDATA[foam]]></category>
		<category><![CDATA[instability]]></category>
		<category><![CDATA[soap film]]></category>

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		<description><![CDATA[Foams are common fluid entities of our everyday life. Our group is, among others, involved in ESA projects on the foam generation and stability under microgravity [1]. On Earth, the gravitational drainage dries the foam such that an interface between &#8230; <a href="http://grasp-lab.org/2013/01/10/faraday/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=760&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://nicovdw.files.wordpress.com/2013/01/im000039.jpg"><img class="alignleft size-large wp-image-770" alt="foam" src="http://nicovdw.files.wordpress.com/2013/01/im000039.jpg?w=640&#038;h=181" width="640" height="181" /></a><br />
Foams are common fluid entities of our everyday life. Our group is, among others, involved in ESA projects on the <a title="News from the ISS" href="http://grasp-lab.org/2012/07/12/news-from-the-iss/">foam generation and stability under microgravity</a> [1]. On Earth, the gravitational drainage dries the foam such that an interface between the foam and the liquid pool is observed.</p>
<p>In a recent paper [2], the dynamics of this foam/liquid interface has been investigated. The idea of this research is to see this interface as a separation between two fluids, characterized by a given (effective) surface tension. By vertically shaking the system, the forcing acceleration faces this effective surface tension and, above a critical threshold, causes the emergence of Faraday waves. Different threshold values have been observed as a function of the foam properties. A phenomenological model has been proposed.</p>
<p>[1] N.Vandewalle, H.Caps, G.Delon, A.Saint-Jalmes, E.Rio, L.Saulnier, M.Adler, A.L.Biance, O.Pitois, S.Cohen-Addad, R.Hohler, D.Weaire, S.Hutzler, D.Langevin, <em>Foam Stability in Microgravity</em>, J. Phys. Conf. Series <span style="text-decoration:underline;">327</span>, 012024 (2011) – <a href="http://www.grasp.ulg.ac.be/article/2011_vandewalle_JPCS.pdf">PDF</a><br />
[2] A.Bronfort and H.Caps, Phys. Rev. E <span style="text-decoration:underline;">86</span>, 066313 (2012) &#8211; <a href="http://www.grasp.ulg.ac.be/article/2012_bronfort_PRE.pdf">PDF</a></p>
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		<title>Antibubble as an interfacial shear rheometer</title>
		<link>http://grasp-lab.org/2012/12/28/abb/</link>
		<comments>http://grasp-lab.org/2012/12/28/abb/#comments</comments>
		<pubDate>Fri, 28 Dec 2012 11:04:23 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[Article]]></category>
		<category><![CDATA[antibubble]]></category>
		<category><![CDATA[rheology]]></category>
		<category><![CDATA[soap film]]></category>

		<guid isPermaLink="false">http://grasp-lab.org/?p=684</guid>
		<description><![CDATA[As described in a recent post, antibubbles are surprising fluid objects [1,2]. An antibubble is a spherical air film that is immersed in a surfactant mixture.  Since no stabilization process exists for the air film, the antibubble must die. Its &#8230; <a href="http://grasp-lab.org/2012/12/28/abb/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=684&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://nicovdw.files.wordpress.com/2012/11/abbsite.jpg"><img class="alignleft size-full wp-image-688" title="antibubble" alt="" src="http://nicovdw.files.wordpress.com/2012/11/abbsite.jpg?w=640"   /></a>As described in <a title="Review on Antibubbles" href="http://grasp-lab.org/2012/07/04/review-on-antibubbles/">a recent post</a>, antibubbles are surprising fluid objects [1,2]. An antibubble is a spherical air film that is immersed in a surfactant mixture.  Since no stabilization process exists for the air film, the antibubble must die. Its lifetime is fixed by the drainage time of the air from the South pole to the North pole of the antibubble under the action of the hydrostatic pressure. When the air film thickness  at the bottom of the antibubble reaches a critical point, it (anti-)explodes. The front picture is an antibubble seen with a monochromatic light. Fringes emphasize thickness gradients along the air film.</p>
<p>In a letter [3], a dynamical model of the air drainage is proposed  that accounts for the particular geometry of the air flow and for the physical properties of the wall. Indeed, we show that according to the used surfactant, the lifetime is modified as predicted by the model. It is demonstrated that the antibubble constitutes a smart tool in order to get fine surface properties of a surfactant mixture as for example the <a href="http://www.ksvnima.com/interfacial-shear-rheometry">surface shear viscosity</a>.</p>
<p>[1] S.Dorbolo, H.Caps and N.Vandewalle, New J. Phys. <span style="text-decoration:underline;">5</span>, 66.1-66.9 (2003) &#8211; <a href="http://www.grasp.ulg.ac.be/article/2003_dorbolo_NJP.pdf">PDF</a><br />
[2] S.Dorbolo, E.Reyssat, N.Vandewalle and D.Quéré, Europhys. Lett. <span style="text-decoration:underline;">69</span>, 966-970 (2005) – <a href="http://www.grasp.ulg.ac.be/article/2005_dorbolo_EPL.pdf">PDF</a><br />
[3] B.Scheid, S.Dorbolo, L.R.Arriaga, and E.Rio, Phys. Rev. Lett. <span style="text-decoration:underline;">109</span>, 264502 (2012) &#8211; <a href="http://www.grasp.ulg.ac.be/article/2012_scheid_PRL.pdf">PDF</a></p>
<p><a href="http://link.aps.org/doi/10.1103/PhysRevLett.109.264502"> </a></p>
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		<title>Bouncing droplets for measuring elongational viscosity</title>
		<link>http://grasp-lab.org/2012/12/22/elongational/</link>
		<comments>http://grasp-lab.org/2012/12/22/elongational/#comments</comments>
		<pubDate>Fri, 21 Dec 2012 23:10:26 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[Article]]></category>
		<category><![CDATA[bouncing]]></category>
		<category><![CDATA[droplet]]></category>
		<category><![CDATA[rheology]]></category>

		<guid isPermaLink="false">http://grasp-lab.org/?p=721</guid>
		<description><![CDATA[When a droplet is gently deposited onto a vibrated liquid bath, the droplet could bounce repeatedly, avoiding coalescence. This peculiar behavior discovered in 2005 [1] is the starting point of an active research on pilot wave dynamics (see for example &#8230; <a href="http://grasp-lab.org/2012/12/22/elongational/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=721&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://grasp-lab.org/2012/12/22/elongational/drop_chaos/" rel="attachment wp-att-730"><img class="alignleft size-full wp-image-730" alt="drop_chaos" src="http://nicovdw.files.wordpress.com/2012/12/drop_chaos.jpg?w=640&#038;h=60" width="640" height="60" /></a></p>
<p>When a droplet is gently deposited onto a vibrated liquid bath, the droplet could bounce repeatedly, avoiding coalescence. This peculiar behavior discovered in 2005 [1] is the starting point of an active research on pilot wave dynamics (see for example our project <a href="http://www.quandrops.ulg.ac.be">QUANDROPS</a>) and droplet resonance effects [2]. <span style="color:#0000ff;">In our last article on the subject [3], we demonstrated that the bouncing behavior of polymeric droplets onto highly viscous bath allows us to study/measure the elongational viscosity of the polymeric samples</span>. It is found that large elongational viscosity of the polymer solution droplets suppressed large droplet deformations.</p>
<p>[1] Y. Couder, E. Fort, C.-H. Gautier, and A. Boudaoud, Phys. Rev. Lett. <span style="text-decoration:underline;">94</span>, 177801 (2005). [2] S.Dorbolo, D.Terwagne, N.Vandewalle, and T.Gilet, New J. Phys. <span style="text-decoration:underline;">10</span>, 113021 (2008) - <a href="http://www.grasp.ulg.ac.be/article/2008_dorbolo_NJP.pdf">PDF</a><br />
[3] S. Gier, S. Dorbolo, D. Terwagne, N. Vandewalle, and C. Wagner, <span style="color:#3366ff;"><em>Bouncing of polymeric droplets on liquid interfaces</em></span>, Phys. Rev. E <span style="text-decoration:underline;">86</span>, 066314 (2012) &#8211; <a href="http://www.grasp.ulg.ac.be/article/2012_gier_PRE.pdf">PDF</a></p>
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		<title>3d printing revolution in the lab</title>
		<link>http://grasp-lab.org/2012/11/17/3dprinting/</link>
		<comments>http://grasp-lab.org/2012/11/17/3dprinting/#comments</comments>
		<pubDate>Sat, 17 Nov 2012 20:10:59 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[From the lab]]></category>
		<category><![CDATA[droplet]]></category>
		<category><![CDATA[foam]]></category>
		<category><![CDATA[granular matter]]></category>
		<category><![CDATA[microfluidics]]></category>
		<category><![CDATA[percolation]]></category>
		<category><![CDATA[self-assembly]]></category>

		<guid isPermaLink="false">http://grasp-lab.org/?p=455</guid>
		<description><![CDATA[Recent articles [1-3] emphasized the interest of 3d printing for scientists. In addition to pedagogical activities, during which students experience 3d models, scientific research can benefit a lot from such a technique. Scientists may build complex structures and may dream &#8230; <a href="http://grasp-lab.org/2012/11/17/3dprinting/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=455&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://nicovdw.files.wordpress.com/2012/08/morphograin.jpg"><img class="alignleft size-full wp-image-473" title="morphograin" alt="grain morphologies" src="http://nicovdw.files.wordpress.com/2012/08/morphograin.jpg?w=640&#038;h=160" height="160" width="640" /></a></p>
<p>Recent articles [1-3] emphasized the interest of 3d printing for scientists. In addition to pedagogical activities, during which students experience 3d models, scientific research can benefit a lot from such a technique. Scientists may build complex structures and may dream about new possibilities for testing their ideas.</p>
<p>A 3d printer (Mojo, STRATASYS) is now used in our lab. Examples of 3d applications are :</p>
<ul>
<li><span style="color:#ff0000;">Granular matter</span> : to design grains (see pictures above) with spec<span style="color:#333333;">ific non-convex shapes fo</span>r <a title="Interlocking of non-convex particles" href="http://grasp-lab.org/2012/05/16/interlocking-of-non-convex-particles/">interlocking</a>, providing unusual granular properties. The morphology of grains can also be determined by measurements of real particle systems.</li>
<li><span style="color:#ff0000;">Self-assembly</span> : to produce synthetic floating bodies for testing <a title="Magnetic Cheerios Effect" href="http://grasp-lab.org/2012/04/23/magnetic-cheerios-effect-self-assembly-driven-by-a-magnetic-field/">capillary attraction between small objects suspended to a liquid interface</a>. The shape of objects will induce capillary multipoles for specific interactions.</li>
<li><span style="color:#ff0000;">Microfluidics</span> : to build complex microfluidic devices for creating encapsulated droplets or producing monodisperse bubbles.</li>
<li><span style="color:#ff0000;">Foam</span> : to create 3d complex rigid frames for trapping improbable (stable or metastable) <a title="Selected picture" href="http://grasp-lab.org/2012/04/22/soap/">soap film structures</a>.</li>
<li><span style="color:#ff0000;">Statistical Physics</span> : to design specific lattices for playing with the granular counterpart of the Maxwell&#8217;s demon.</li>
<li><span style="color:#ff0000;">Percolation</span> : to print 3d <a href="http://en.wikipedia.org/wiki/Fractal">fractal</a> structures for testing fluid invasion and other physical processes such as diffusion.</li>
<li><span style="color:#ff0000;">Complex fiber networks</span> : to create frames for connecting complex digital microfluidics fiber-based networks.</li>
</ul>
<p>Many more ideas are currently tested.</p>
<p>[1] J.N.A.Matthews, <span style="color:#339966;"><em>3D printing breaks out of its mold</em></span>, Physics Today <span style="text-decoration:underline;">64</span>, 25 (2011)<br />
[2] M.D.Symes et al, <span style="color:#339966;"><em>Integrated 3D-printed reactionware for chemical synthesis and analysis</em></span>, Nature Chemistry <span style="text-decoration:underline;">4</span>, 349 (2012)<br />
[3] N.Jones, <span style="color:#339966;"><em>Three-dimensional printers are opening up new worlds to research</em></span>, Nature <span style="text-decoration:underline;">487</span>, 22 (2012)</p>
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		<title>Building sandcastles grain by grain</title>
		<link>http://grasp-lab.org/2012/10/28/grainbygrain/</link>
		<comments>http://grasp-lab.org/2012/10/28/grainbygrain/#comments</comments>
		<pubDate>Sun, 28 Oct 2012 19:44:48 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[Article]]></category>
		<category><![CDATA[cohesion]]></category>
		<category><![CDATA[granular matter]]></category>
		<category><![CDATA[self-assembly]]></category>

		<guid isPermaLink="false">http://grasp-lab.org/?p=662</guid>
		<description><![CDATA[From sugar poured into a bowl to tons of grains discharge processes in industry, a peculiar feature of granular materials emerges : the formation of a pile. When the grains are not cohesive, only the friction and the grain geometry &#8230; <a href="http://grasp-lab.org/2012/10/28/grainbygrain/">Continue reading <span class="meta-nav">&#8594;</span></a><img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=662&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p><a href="http://nicovdw.files.wordpress.com/2012/10/suction.jpg"><img class="aligncenter size-full wp-image-668" title="sand tower" alt="" src="http://nicovdw.files.wordpress.com/2012/10/suction.jpg?w=640"   /></a></p>
<p>From sugar poured into a bowl to tons of grains discharge processes in industry, a peculiar feature of granular materials emerges : the formation of a pile. When the grains are not cohesive, only the friction and the grain geometry determine the shape of the assembly which resembles a conical pyramid. <span style="color:#3366ff;">As known by any sandcastle architect, the addition of some liquid induces </span><span style="color:#3366ff;"><a title="Relative Humidity matters" href="http://grasp-lab.org/2012/04/22/rhmatters/"><span style="color:#3366ff;">cohesion between the grains due to the surface tension and capillary effects</span></a>.</span> During the last years, different groups studied the mechanical properties of wet granular piles, finding a remarkably insensitivity on the liquid content. This unexpected result is explained by a particular organization of the liquid between the grains. Although a significant progress has been achieved, all these experiments only consider wet granular piles with a low percentage of liquid. <span style="color:#0000ff;">In our last paper, we report what occurs when dry sand is poured on a highly humid granular bed. Above a threshold humidity, an interesting phenomenon appears: instead of a wet pile, stable sand towers emerge.</span> The impacting grains have a non-zero probability to stick on the wet grains, due to instantaneous liquid bridges created during their impact. The growth velocity of this self-assembled structures is determined by the flux of grains and the liquid content of the bed. We found that the higher the humidity the greater the probability of the grains to stick, but the smaller the final height of the tower, which falls when the cohesive stress at its base is surpassed.<span style="color:#000080;"> Beyond an artistic technique to sculpt sandcastles, this experimental method represents a new alternative to study the mechanical properties of wet granular materials.</span></p>
<p>F.Pacheco-Vazquez, F.Moreau, N.Vandewalle and S.Dorbolo, <span style="color:#333399;"><em>Sculpting sandcastles grain by grain: Self-assembled sand towers</em></span>, Phys. Rev. E <span style="text-decoration:underline;">86</span>, 051303 (2012) &#8211; <a href="http://www.grasp.ulg.ac.be/article/2012_pacheco_PRE.pdf">PDF</a><a href="http://pre.aps.org/accepted/b3074YccFfd1073cd91e1e403c40649bc9540e56f"><br />
</a></p>
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		<title>Leidenfrost droplet explosion</title>
		<link>http://grasp-lab.org/2012/10/22/leidenfrost/</link>
		<comments>http://grasp-lab.org/2012/10/22/leidenfrost/#comments</comments>
		<pubDate>Mon, 22 Oct 2012 20:26:11 +0000</pubDate>
		<dc:creator>nicovdw</dc:creator>
				<category><![CDATA[Fun]]></category>
		<category><![CDATA[droplet]]></category>

		<guid isPermaLink="false">http://grasp-lab.org/?p=643</guid>
		<description><![CDATA[See below our latest movie about our research on Leidenfrost droplets. This movie, emphasizing the conditions for Leidenfrost droplet explosion, will be presented at the next DFD APS meeting.<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=grasp-lab.org&#038;blog=35262626&#038;post=643&#038;subd=nicovdw&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p>See below our latest movie about our research on <a href="http://en.wikipedia.org/wiki/Leidenfrost_effect">Leidenfrost droplets</a>. This movie, emphasizing the conditions for Leidenfrost droplet explosion, will be presented at the next <a href="http://apsdfd2012.ucsd.edu">DFD APS meeting</a>.</p>
<p><span class='embed-youtube' style='text-align:center; display: block;'><iframe class='youtube-player' type='text/html' width='640' height='390' src='http://www.youtube.com/embed/z0sp3AjgUy4?version=3&#038;rel=1&#038;fs=1&#038;showsearch=0&#038;showinfo=1&#038;iv_load_policy=1&#038;wmode=transparent' frameborder='0'></iframe></span></p>
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