{"id":13632,"date":"2021-02-03T14:03:44","date_gmt":"2021-02-03T13:03:44","guid":{"rendered":"https:\/\/navier-lab.fr\/?page_id=13632"},"modified":"2024-08-01T15:51:36","modified_gmt":"2024-08-01T13:51:36","slug":"granular-and-particulate-media","status":"publish","type":"page","link":"https:\/\/navier-lab.fr\/en\/research\/rheophysics-porous-media\/granular-and-particulate-media\/","title":{"rendered":"Granular and Particulate Media"},"content":{"rendered":"<p><section class=\"kc-elm kc-css-876247 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-262865 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\"><div class=\"kc-elm kc-css-401606\" style=\"height: 40px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-997152 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/unsaturated-wet-granular-flow.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-453720\" style=\"height: 40px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-114368 kc_text_block\"><\/p>\n<p style=\"text-align: center;\">We conduct research on dense granular material rheology &#8212; notably wet and unsaturated media &#8212; and we also investigate their acoustic properties. We use inclined planes, rheometers and more recently a rotating cell allowing us to trigger avalanches in quasistatic conditions. We also study these materials through numerical simulations with over twenty years of experience in the domain.<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-355312\" style=\"height: 20px; clear: both; width:100%;\"><\/div><\/div><\/div><\/div><\/div><\/section><section class=\"kc-elm kc-css-180138 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-240345 kc_col-sm-3 kc_column kc_col-sm-3\"><div class=\"kc-col-container\"><\/div><\/div><div class=\"kc-elm kc-css-952946 kc_col-sm-3 kc_column kc_col-sm-3\"><div class=\"kc-col-container\"> <article class=\"sabbi-thumlinepost-card solitude-bg__x kc-elm kc-css-685315\"><figure class=\"sabbi-thumlinepost-card-figure\">\n                           <img loading=\"lazy\" decoding=\"async\" width=\"522\" height=\"221\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2021\/02\/slices_tomo.png\" class=\"img-responsive img-thumpost\" alt=\"Tomography slices of a wet granular materials showing interstitial liquid\" srcset=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2021\/02\/slices_tomo.png 522w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2021\/02\/slices_tomo-300x127.png 300w\" sizes=\"auto, (max-width: 522px) 100vw, 522px\" \/>\n                          <\/figure><div class=\"sabbi-thumlinepost-card-meta\">\n                        <h2 class=\"info-box-title ht-5\">Unsaturated wet granular materials<\/h2><a href=\"#unsaturated-wet-granular-materials\" title=\"Unsaturated Wet Granular Materials\" target=\"_self\" class=\"btn btn-unsolemn btn-action read-more\">Read More<\/a><\/div>\n                <\/article><\/div><\/div><div class=\"kc-elm kc-css-416010 kc_col-sm-3 kc_column kc_col-sm-3\"><div class=\"kc-col-container\"> <article class=\"sabbi-thumlinepost-card solitude-bg__x kc-elm kc-css-119333\"><figure class=\"sabbi-thumlinepost-card-figure\">\n                           <img loading=\"lazy\" decoding=\"async\" width=\"184\" height=\"245\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/rearrangements-immersed-granular.png\" class=\"img-responsive img-thumpost\" alt=\"Probing rearrangements in an immersed granular suspension using acoustic diffusion.\" \/>\n                          <\/figure><div class=\"sabbi-thumlinepost-card-meta\">\n                        <h2 class=\"info-box-title ht-5\">Acoustic wave diffusion in immersed granular media<\/h2><a href=\"#acoustic-diffusion-granular-materials\" title=\"Acoustic Diffusion in Granular Materials\" target=\"_self\" class=\"btn btn-unsolemn btn-action read-more\">Read More<\/a><\/div>\n                <\/article><\/div><\/div><div class=\"kc-elm kc-css-274335 kc_col-sm-3 kc_column kc_col-sm-3\"><div class=\"kc-col-container\"><\/div><\/div><\/div><\/div><\/section><section class=\"kc-elm kc-css-176460 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-844478 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\"><div class=\"kc-elm kc-css-206708\" style=\"height: 0px; clear: both; width:100%;\"><\/div>\n<div class=\"kc-elm kc-css-333388 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<\/div><\/div><\/div><\/div><\/section><section id=\"unsaturated-wet-granular-materials\" class=\"kc-elm kc-css-108737 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-965042 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\"><div class=\"kc-elm kc-css-121036 kc_text_block\"><\/p>\n<h3>Structure and Rheology of Wet, Unsaturated Granular Media<\/h3>\n<p>\n<\/div><div class=\"kc-elm kc-css-348480 kc_text_block\"><\/p>\n<h5>A. Fall, J.-N. Roux, F. Chevoir, A. Awdi (PhD), C. Chateau (ME)<\/h5>\n<h5>Collaborations : S. Deb\u0153uf (d&#8217;Alembert)<\/h5>\n<p>\n<\/div><div class=\"kc-elm kc-css-453758\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-614506 kc_text_block\"><\/p>\n<p>\nExperiments on the rheology of granular materials wetted by a silicone oil are in good agreement with <em>discrete element<\/em> numerical simulations conducted in-house. Both follow rheological models of <em>\u00b5<\/em>(<em>I<\/em>)-type, generalised to include a characteristic pressure <em>P<sup>*<\/sup><\/em> defined as :<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-523119\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-104312 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/08\/equation_typical_adhesion_pressure-1.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-424529\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-190199 kc_text_block\"><\/p>\n<p>\nWith <em>P<\/em> the confinement pressure, <em>d<\/em> the grain diameter and <em>F<sub>0<\/sub> <\/em>the inter-granular, attractive force (here proportional to the surface tension). More recently, the experimental study of the rheology of these materials has been extended to inclined plane experiments in collaboration with S. Deboeuf from <em>Institut Jean le Rond d&#8217;Alembert.<\/em> The micromorphology of these materials is observed by Discrete Element method in numerical simulations and by&nbsp;X-ray microtomography in a tailor-made experimental setup allowing us to measure the microstructure dynamics.<\/p>\n<p>We have used advanced image segmentation algorithms leveraging Articifial Intelligence tools to precisely analyse the microstructure (grain arrangement, liquid bridge morphology evolution under shear) that can go beyond the pendular regime of isolated liquid bridges (PhD thesis of Ahmad Awdi, co-supervised with C. Chateau of the Multi-\u00c9chelle group). Another recent development is the study of the viscous effects in these liquid bridges for steady shear and large amplitude oscillatory shear (LAOS). The rheological properties of these systems are then characterised by a visco-inertial number <em>J <\/em>combining the classical inertial number <em>I <\/em>from granular matter rheology and the viscous number <em>I<sub>v <\/sub><\/em>characteristic of suspensions in the Stokes regime :<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-110299\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-430574 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/08\/J-relation-wet-granular-materials.jpg\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-261827\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div data-kc-equalheight=\"true\" data-kc-row-action=\"true\" data-kc-equalheight-align=\"middle\" class=\"kc-elm kc-css-705913 kc_row kc_row_inner\"><div class=\"kc-elm kc-css-269297 kc_col-sm-6 kc_column_inner kc_col-sm-6\"><div class=\"kc_wrapper kc-col-inner-container\"><div class=\"kc-elm kc-css-687147 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/tomo-rheoscopy-experimental-setup.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-737171 kc_text_block\"><\/p>\n<p style=\"text-align: center;\"><em>Measuring the water content in an insaturated granular material using X-ray microtomography. (a) Microtomograph and the in-place experimental setup (b) Cross-sectional view of the shear cell. (c) Translation and rotation stage at the bottom of the shear cell, hidden from view in Panel (a).<br \/>\n<\/em><\/p>\n<p>\n<\/div><\/div><\/div><div class=\"kc-elm kc-css-880572 kc_col-sm-6 kc_column_inner kc_col-sm-6\"><div class=\"kc_wrapper kc-col-inner-container\"><div class=\"kc-elm kc-css-820967 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/heat-maps-phi_L.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-722131 kc_text_block\"><\/p>\n<p style=\"text-align: center;\"><em>Water content in a slice of an unsaturated wet granular material (left) in the initial state (right) after 10 minutes under shear.<br \/>\n<\/em><\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-148457\" style=\"height: 100px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-331903 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/liquid-morphologies.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-719176 kc_text_block\"><\/p>\n<p style=\"text-align: center;\"><em>Simple liquid bridges and more complex morphologies between particle pairs (triplets, quadruplets, &#8230;) of unsaturated wet granular materials.<br \/>\n<\/em><\/p>\n<p>\n<\/div><\/div><\/div><\/div><div class=\"kc-elm kc-css-4978\" style=\"height: 10px; clear: both; width:100%;\"><\/div>\n<div class=\"kc-elm kc-css-59231 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-793630 kc_text_block\"><\/p>\n<h4>References<\/h4>\n<ul>\n<li><a href=\"https:\/\/doi.org\/10.1122\/1.5026979\">Rheology and microstructure of unsaturated wet granular materials: Experiments and simulations<\/a>, D. Hautemayou, M. Badetti, A. Fall, S. Rodts, P. Aimedieu, J.-N. Roux, and F. Chevoir, <em>Journal of Rheology<\/em> <strong>62<\/strong>(5), 1175\u20131186 (2018).<\/li>\n<li><a href=\"https:\/\/doi.org\/10.1122\/8.0000631\"> Cohesion and aggregates in unsaturated wet granular flows down a rough incline<\/a>, S. Deboeuf and A. Fall, <em>Journal of Rheology<\/em><strong> 67<\/strong>(4), 909\u2013922 (2023)<\/li>\n<li><a href=\"https:\/\/doi.org\/10.1122\/8.0000507\">Viscous dissipation in large amplitude oscillatory shear of unsaturated wet granular matter<\/a>, A. Awdi, C. Chateau, F. Chevoir, J.-N. Roux and A. Fall, <em>Journal of Rheology<\/em> <strong>67<\/strong>(2), 365\u2013372 (2023)<\/li>\n<\/ul>\n<p>\n<\/div><\/div><\/div><\/div><\/div><\/section><section id=\"acoustic-diffusion-granular-materials\" class=\"kc-elm kc-css-883717 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-799332 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\">\n<div class=\"kc-elm kc-css-425441 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-385603 kc_text_block\"><\/p>\n<h3>Acoustic Wave Diffusion in Immersed Granular Materials<\/h3>\n<p>\n<\/div><div class=\"kc-elm kc-css-306384 kc_text_block\"><\/p>\n<h5>J. L\u00e9opold\u00e8s, V. Langlois, I. Awada (PhD), M. Bornert (ME)<\/h5>\n<p>\n<\/div><div class=\"kc-elm kc-css-588489\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-672660 kc_text_block\"><\/p>\n<p>\nWe use elastic wave propagation in a simple numerical model to characterise an immersed granular material at different time and spatial scales, and to identify potential new physical variables (e.g. particle rotation). In the PhD thesis of Ibrahim Awada, we study multiple scattering of ultrasound waves in dense granular suspensions. We have shown that correlating successive transmitted ultrasound signals allows us to estimate local strain at the grain scale down to 0.00001. This method has been applied to a granular material under plastic solid regime, with a sample located in a rotating drum oscillating below the angle of repose. We quantitatively measure the progressive compaction of the granular material and detect local, precursor events before the avalanches. We are currently writing an article on these results.<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-455785\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-211584 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/rearrangements-immersed-granular-with-graph.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-433887\" style=\"height: 10px; clear: both; width:100%;\"><\/div>\n<div class=\"kc-elm kc-css-120242 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-34238 kc_text_block\"><\/p>\n<h4>References<\/h4>\n<ul>\n<li><a href=\"https:\/\/doi.org\/10.1039\/D0SM01427C\">Probing intermittency and reversibility in a dense granular suspension under shear using multiply scattered ultrasound<\/a>, J. L\u00e9opold\u00e8s and X. Jia, <em>Soft Matter <\/em><strong>16<\/strong>, 10716-10722 (2020)<\/li>\n<\/ul>\n<p>\n<\/div><\/div><\/div><\/div><\/div><\/section><\/p>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":53,"featured_media":0,"parent":12398,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-13632","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages\/13632","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/users\/53"}],"replies":[{"embeddable":true,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/comments?post=13632"}],"version-history":[{"count":27,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages\/13632\/revisions"}],"predecessor-version":[{"id":17068,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages\/13632\/revisions\/17068"}],"up":[{"embeddable":true,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages\/12398"}],"wp:attachment":[{"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/media?parent=13632"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}