{"id":396,"date":"2018-11-16T03:02:15","date_gmt":"2018-11-16T02:02:15","guid":{"rendered":"http:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/?page_id=396"},"modified":"2018-11-16T04:36:02","modified_gmt":"2018-11-16T03:36:02","slug":"dense-suspensions-and-colloids","status":"publish","type":"page","link":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/research\/dense-suspensions-and-colloids\/","title":{"rendered":"Dense suspensions and colloids"},"content":{"rendered":"<h1>Brownian diffusion in a dilute field of traps is Fickean but non-Gaussian<\/h1>\n<h6 class=\"authors \">Serge Mora and Yves Pomeau<\/h6>\n<p>Motivated by experimental observations, we look for the diffusion of Brownian particles in a medium where they can be either trapped in randomly disposed deep traps or where they diffuse by the regular Fick&#8217;s law outside of the traps. This process can be represented by two coupled equations\u2014one valid inside the traps and another one outside \u2014yielding the probability distribution of the distance run as a function of time. This probability depends on a unique dimensionless parameter <span id=\"MathJax-Element-1-Frame\" class=\"mjx-chtml MathJax_CHTML\"><span id=\"MJXc-Node-1\" class=\"mjx-math\"><span id=\"MJXc-Node-2\" class=\"mjx-mrow\"><span id=\"MJXc-Node-3\" class=\"mjx-mi\"><span class=\"mjx-char MJXc-TeX-math-I\">\u03bb<\/span><\/span><\/span><\/span><\/span>which is proportional to the product of the (small) density of the traps times the long time of staying in the traps. The mean-square displacement is proportional to the lag time, and for finite or large <span id=\"MathJax-Element-2-Frame\" class=\"mjx-chtml MathJax_CHTML\"><span id=\"MJXc-Node-4\" class=\"mjx-math\"><span id=\"MJXc-Node-5\" class=\"mjx-mrow\"><span id=\"MJXc-Node-6\" class=\"mjx-mi\"><span class=\"mjx-char MJXc-TeX-math-I\">\u03bb<\/span><\/span><\/span><\/span><\/span> the probability density is no longer Gaussian but exponential on intermediate time scales.<\/p>\n<h1>Viscoinertial regime of immersed granular flows<\/h1>\n<p>Lhassan Amarsid, J-Y Delenne, Patrick Mutabaruka, Yann Monerie, Fr\u00e9d\u00e9ric Perales, Farhang Radjai<\/p>\n<p>By means of extensive coupled molecular dynamics\u2013lattice Boltzmann simulations, accounting for grain dynamics and subparticle resolution of the fluid phase, we analyze steady inertial granular flows sheared by a viscous fluid. We show that, for a broad range of system parameters (shear rate, confining stress, fluid viscosity, and relative fluid-grain density), the frictional strength and packing fraction can be described by a modified inertial number incorporating the fluid effect. In a dual viscous description, the effective viscosity diverges as the inverse square of the difference between the packing fraction and its jamming value, as observed in experiments. We also find that the fabric and force anisotropies extracted from the contact network are well described by the modified inertial number, thus providing clear evidence for the role of these key structural parameters in dense suspensions.<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Brownian diffusion in a dilute field of traps is Fickean but non-Gaussian Serge Mora and Yves Pomeau Motivated by experimental observations, we look for the diffusion of Brownian particles in a medium where they can be either trapped in randomly disposed deep traps or where they diffuse by the regular Fick&#8217;s law outside of the &hellip; <a href=\"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/research\/dense-suspensions-and-colloids\/\" class=\"more-link\">Continue reading<span class=\"screen-reader-text\"> &#8220;Dense suspensions and colloids&#8221;<\/span><\/a><\/p>\n","protected":false},"author":25,"featured_media":0,"parent":321,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-396","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/pages\/396","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/users\/25"}],"replies":[{"embeddable":true,"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/comments?post=396"}],"version-history":[{"count":4,"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/pages\/396\/revisions"}],"predecessor-version":[{"id":465,"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/pages\/396\/revisions\/465"}],"up":[{"embeddable":true,"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/pages\/321"}],"wp:attachment":[{"href":"https:\/\/www.lmgc.univ-montp2.fr\/perso\/pmmd\/wp-json\/wp\/v2\/media?parent=396"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}