{"id":16415,"date":"2024-07-22T18:57:49","date_gmt":"2024-07-22T16:57:49","guid":{"rendered":"https:\/\/navier-lab.fr\/?page_id=16415"},"modified":"2024-09-06T10:37:48","modified_gmt":"2024-09-06T08:37:48","slug":"bubbly-media-and-foams","status":"publish","type":"page","link":"https:\/\/navier-lab.fr\/en\/research\/rheophysics-porous-media\/bubbly-media-and-foams\/","title":{"rendered":"Bubbly Media and Foams"},"content":{"rendered":"<p><section class=\"kc-elm kc-css-584811 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-589606 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\"><div class=\"kc-elm kc-css-928072\" style=\"height: 40px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-247142 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/11\/mousse-couleur-2.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-92230\" style=\"height: 40px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-291809 kc_text_block\"><\/p>\n<p style=\"text-align: center;\">Our research group has investigated liquid foams, interfaces and soap films for over a decade. We focus on the mechanical stability of thin liquid films, granular films and <em>gas marbles<\/em>. We are also interested in the rheology, the coarsening and the stability of simple bubbly media or complex aerated materials, along with the production and the shaping of foamed coatings and foamed construction materials.<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-570058\" style=\"height: 20px; clear: both; width:100%;\"><\/div><\/div><\/div><\/div><\/div><\/section><section class=\"kc-elm kc-css-868273 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-834023 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-744178\"><figure class=\"sabbi-thumlinepost-card-figure\">\n                           <img loading=\"lazy\" decoding=\"async\" width=\"2125\" height=\"1789\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/coarsening-liquid-foam-1.png\" class=\"img-responsive img-thumpost\" alt=\"Coarsening of a liquid foam in microgravity (i.e. in the ISS !)\" srcset=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/coarsening-liquid-foam-1.png 2125w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/coarsening-liquid-foam-1-300x253.png 300w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/coarsening-liquid-foam-1-1024x862.png 1024w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/coarsening-liquid-foam-1-768x647.png 768w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/coarsening-liquid-foam-1-1536x1293.png 1536w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/coarsening-liquid-foam-1-2048x1724.png 2048w\" sizes=\"auto, (max-width: 2125px) 100vw, 2125px\" \/>\n                          <\/figure><div class=\"sabbi-thumlinepost-card-meta\">\n                        <h2 class=\"info-box-title ht-5\">Coarsening of liquid foams<\/h2><a href=\"#coarsening-liquid-foams\" title=\"\" target=\"_self\" class=\"btn btn-unsolemn btn-action read-more\">Read More<\/a><\/div>\n                <\/article><\/div><\/div><div class=\"kc-elm kc-css-118453 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-923241\"><figure class=\"sabbi-thumlinepost-card-figure\">\n                           <img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"298\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/nice-gas-marble.png\" class=\"img-responsive img-thumpost\" alt=\"A bubble-shaped granular film, also named gas marble\" srcset=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/nice-gas-marble.png 300w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/nice-gas-marble-150x150.png 150w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/>\n                          <\/figure><div class=\"sabbi-thumlinepost-card-meta\">\n                        <h2 class=\"info-box-title ht-5\">Granular films and gas marbles<\/h2><a href=\"#gas-marbles-granular-films\" title=\"Bubbly Media and Foams\" target=\"_self\" class=\"btn btn-unsolemn btn-action read-more\">Read More<\/a><\/div>\n                <\/article><\/div><\/div><div class=\"kc-elm kc-css-348157 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-353455\"><figure class=\"sabbi-thumlinepost-card-figure\">\n                           <img loading=\"lazy\" decoding=\"async\" width=\"269\" height=\"269\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/bumpy-bubbles.png\" class=\"img-responsive img-thumpost\" alt=\"Bubbly yield-stress fluid\" srcset=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/bumpy-bubbles.png 269w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/bumpy-bubbles-150x150.png 150w\" sizes=\"auto, (max-width: 269px) 100vw, 269px\" \/>\n                          <\/figure><div class=\"sabbi-thumlinepost-card-meta\">\n                        <h2 class=\"info-box-title ht-5\">Stability of aerated yield-stress fluids<\/h2><a href=\"#yield-stress-fluid-foam-stability\" title=\"Bubbly Media and Foams\" target=\"_self\" class=\"btn btn-unsolemn btn-action read-more\">Read More<\/a><\/div>\n                <\/article><\/div><\/div><div class=\"kc-elm kc-css-309234 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-823058\"><figure class=\"sabbi-thumlinepost-card-figure\">\n                           <img loading=\"lazy\" decoding=\"async\" width=\"400\" height=\"400\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/07\/mousse-ciment-400x400-1.jpg\" class=\"img-responsive img-thumpost\" alt=\"Cement foam\" srcset=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/07\/mousse-ciment-400x400-1.jpg 400w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/07\/mousse-ciment-400x400-1-300x300.jpg 300w, https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/07\/mousse-ciment-400x400-1-150x150.jpg 150w\" sizes=\"auto, (max-width: 400px) 100vw, 400px\" \/>\n                          <\/figure><div class=\"sabbi-thumlinepost-card-meta\">\n                        <h2 class=\"info-box-title ht-5\">Foamed construction materials<\/h2><a href=\"#foamed-construction-materials\" title=\"Bubbly Media and Foams\" target=\"_self\" class=\"btn btn-unsolemn btn-action read-more\">Read More<\/a><\/div>\n                <\/article><\/div><\/div><\/div><\/div><\/section><section class=\"kc-elm kc-css-779817 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-25192 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\"><div class=\"kc-elm kc-css-956917\" style=\"height: 0px; clear: both; width:100%;\"><\/div>\n<div class=\"kc-elm kc-css-237571 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=\"coarsening-liquid-foams\" class=\"kc-elm kc-css-52952 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-757147 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\"><div class=\"kc-elm kc-css-665775 kc_text_block\"><\/p>\n<h3>Coarsening of liquid foams<\/h3>\n<p>\n<\/div><div class=\"kc-elm kc-css-182074 kc_text_block\"><\/p>\n<h5>O. Pitois, N. Galvani (PhD)<\/h5>\n<h5>Collaborations : S. Cohen-Addad, R. H\u00f6hler (INSP), D. Langevin, E. Rio, A. Salonen (LPS), D. J. Durian (U. Pennsylvania), S. Vincent-Bonnieu (ESA)<\/h5>\n<p>\n<\/div><div class=\"kc-elm kc-css-389412\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-83013 kc_text_block\"><\/p>\n<p>\nIn liquid foams, we name <em>coarsening<\/em> the gas diffusion from one bubble to another through the liquid that separates them. Coarsening leads to a decrease in the number of bubbles and to an increase of their average size. While many applications deal with <em>wet<\/em> foams, i.e. with a liquid volume fraction above 20%, these foams have been seldom studied because of their instability to liquid drainage due to gravity.<\/p>\n<p>We have joined a European consortium led by Dominique Langevin in the framework of a MAP Contract (Hydrodynamics of Wet Foams) with the European Space Agency to study liquid foam coarsening <em>on the International Space Station <\/em>(!). The first round of experiments conducted in 2020 have yielded precious results related to the bubble growth dynamics for a broad range of liquid volume fractions from wet foams to bubbly liquids (50 %). We have observed a change in the coarsening regime from a growth with <em>t<\/em><sup>1\/2<\/sup> for small liquid fractions to <em>t<\/em><sup>1\/3<\/sup> for the larger liquid fractions. One of our main results is that the volume fraction for which the change of regime occurs (0.39) is laregly above the Random Close Packing volume fraction (0.31 as the foams are not monodisperse). We have shown that this deviation is caused by small adhesion forces that keep the average contact area between bubbles to a non-zero value beyond Random Close Packing. We have also highlighted an excess of small bubbles (named <em>roaming bubbles<\/em>) in the bubble size distribution compared to theoretical models. We have shown that these bubbles have lost contact with the foam bubbles, which impedes their dissolution. These <em>roaming bubbles<\/em> had never been seen before.<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-614013\" style=\"height: 20px; clear: both; width:100%;\"><\/div>\n\t<div class=\"kc-elm kc-css-482284 kc_shortcode kc_video_play kc_video_wrapper\" data-video=\"https:\/\/vimeo.com\/1006563329\" data-width=\"600\" data-height=\"338.98305084746\" data-fullwidth=\"\" data-autoplay=\"\" data-loop=\"yes\" data-control=\"yes\" data-related=\"\" data-showinfo=\"\" data-kc-video-mute=\"\">\n\t\t\t<\/div>\n\n<div class=\"kc-elm kc-css-884208 kc_text_block\"><\/p>\n<p style=\"text-align: center;\"><em>Credits : ENPC, Ingenius<br \/><\/em><\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-867361\" style=\"height: 20px; clear: both; width:100%;\"><\/div>\n<div class=\"kc-elm kc-css-496967 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-842909 kc_text_block\"><\/p>\n<h4>References<\/h4>\n<ul>\n<li><a href=\"https:\/\/doi.org\/10.1073\/pnas.2306551120\">Hierarchical bubble size distributions in coarsening wet liquid foams<\/a>, N. Galvani, M. Pasquet, A. Mukherjee, A. Requier, S. Cohen-Addad, O. Pitois, R. H\u00f6hler, E. Rio, A. Salonen, D. J. Durian and D. Langevin, <em>PNAS<\/em> <strong>120<\/strong> (38), e2306551120 (2023)<\/li>\n<\/ul>\n<div>\n<ul>\n<li><a href=\"https:\/\/doi.org\/10.1039\/D3SM00535F\">Coarsening transitions of wet liquid foams under microgravity conditions<\/a>, M. Pasquet, N. Galvani, A. Requier, S. Cohen-Addad, R. H\u00f6hler, O. Pitois, E. Rio, A. Salonen and D. Langevin, <em>Soft Matter <\/em><span id=\"top\"><strong>19<\/strong>, 6267-6279 (2023)<\/span><\/li>\n<\/ul>\n<\/div>\n<p>\n<\/div><\/div><\/div><\/div><\/div><\/section><section id=\"gas-marbles-granular-films\" class=\"kc-elm kc-css-382583 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-795684 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\">\n<div class=\"kc-elm kc-css-496211 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-738551 kc_text_block\"><\/p>\n<h3>Granular Films and Gas Marbles<\/h3>\n<p>\n<\/div><div class=\"kc-elm kc-css-24637 kc_text_block\"><\/p>\n<h5>F. Rouyer, Y. Khidas, P. Gauthier (PhD)<\/h5>\n<h5>Collaboration : A. Seguin, G. Gauthier (FAST)<\/h5>\n<p>\n<\/div><div class=\"kc-elm kc-css-527885\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-883194 kc_text_block\"><\/p>\n<p>\nThere are multiple, important applications for systems presenting liquid interfaces containing adsorbed solid particles : decreased surfactant usage, reinforcement of bubbles in aerated construction materials, and froth floatation or encapsulation for environmental remediation processes.<\/p>\n<p>The ANR project PhyGaMa (2020-2024, in collaboration with Laboratoire FAST) is dedicated to studying <em>gas marbles<\/em>, a new object discovered in the laboratory. <em>Gas marbles <\/em>are pockets of gas surrounded by a closed envelope of liquid and adsorbed solid particles which are a few tens of micrometers in diameter. In this object, the liquid is under a slight depression, which confers capillary cohesion to the grains and an unexpected mechanical resistance. We coined the term <em>gas marble<\/em> in reference to <a href=\"https:\/\/www.nature.com\/articles\/35082026\"><em>liquid marbles<\/em><\/a> that were discovered in 2001.<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-312804\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-652793 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/11\/Armored-soap-films.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-613599 kc_text_block\"><\/p>\n<p style=\"text-align: center;\"><em>Anatomy of a <\/em>gas marble<em>, and geometry of the liquid films at its surface<br \/>\n<\/em><\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-442970\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-319227 kc_text_block\"><\/p>\n<p>\nWe have developed an experimental setup for which we control the liquid film pressure to study the cohesion properties of the particle-laden liquid film. We have shown that the capillary underpressure determines the response of the envelope when it is being punctured. Under a critical underpressure, we observe a total opening of the envelope similar to traditional soap films; however, the opening dynamics is much overall much slower than simple soap films (Taylor-Culick opening) due to inertia. For higher liquid underpressure, the envelope has a solid behaviour and the puncture hole remains stable. Between the two regimes, we note the presence of an <em>intermittent<\/em> opening regime. Numerical simulations conducted using <em>Surface Evolver<\/em> have shown that the cohesive <em>Mohr-Coulomb <\/em>failure criterion characteristic of granular media explains the observed transition, which sheds a new light on the mechanical stability of <em>gas marbles.<\/em><\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-524328\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-663999 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/granular-film-opening.jpg\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-659492 kc_text_block\"><\/p>\n<p style=\"text-align: center;\"><em>Intermittent opening of a granular film for a liquid underpressure <\/em><em>\u0394P \u2245 &#8211; 100 Pa<\/em><\/p>\n<p>\n<\/div>\n<div class=\"kc-elm kc-css-965839 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-332957 kc_text_block\"><\/p>\n<h4>References<\/h4>\n<ul>\n<li><a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.118.228001\">Gas Marbles: Much Stronger than Liquid Marbles<\/a>, Y. Timounay, O. Pitois and F. Rouyer, <em>Physical Review Letters<\/em> Phys. Rev. Lett. <strong>118,<\/strong> 228001 (2017) | <span class=\"BxUVEf ILfuVd\" lang=\"en\"><span class=\"hgKElc\">\u2766<\/span><\/span> <strong>Editor&#8217;s Suggestion &amp; Featured in <a href=\"https:\/\/physics.aps.org\/articles\/v10\/62\"><em>Physics<\/em><\/a><\/strong><\/li>\n<li><a href=\"https:\/\/doi.org\/10.1039\/D3RA04938H\">Pressure threshold for inhibition of dense granular film opening<\/a>, N. Retailleau, Y. Khidas and F. Rouyer, <em>RSC Advances, <\/em><span id=\"top\"><strong>13<\/strong>, 30905-30914 (2023)<\/span><\/li>\n<\/ul>\n<p>\n<\/div><\/div><\/div><\/div><\/div><\/section><section id=\"yield-stress-fluid-foam-stability\" class=\"kc-elm kc-css-965569 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-20303 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\">\n<div class=\"kc-elm kc-css-103918 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-114755 kc_text_block\"><\/p>\n<h3>Stability of Foamed Yield-Stress Fluids<\/h3>\n<p>\n<\/div><div class=\"kc-elm kc-css-766476 kc_text_block\"><\/p>\n<h5>O. Pitois, B. Saint-Michel, N. Galvani (PhD)<\/h5>\n<h5>Collaboration : S. Cohen-Addad (INSP)<\/h5>\n<p>\n<\/div><div class=\"kc-elm kc-css-200653\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-548604 kc_text_block\"><\/p>\n<p>\n[Under construction]<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-753306\" style=\"height: 20px; clear: both; width:100%;\"><\/div>\n<div class=\"kc-elm kc-css-598363 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-286279 kc_text_block\"><\/p>\n<h4>References<\/h4>\n<p>\n<\/div><\/div><\/div><\/div><\/div><\/section><section id=\"foamed-construction-materials\" class=\"kc-elm kc-css-938686 kc_row\"><div class=\"kc-row-container  kc-container\"><div class=\"kc-wrap-columns\"><div class=\"kc-elm kc-css-836320 kc_col-sm-12 kc_column kc_col-sm-12\"><div class=\"kc-col-container\">\n<div class=\"kc-elm kc-css-481686 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-965208 kc_text_block\"><\/p>\n<h3>Foamed Construction Materials<\/h3>\n<p>\n<\/div><div class=\"kc-elm kc-css-236804 kc_text_block\"><\/p>\n<h5>O. Pitois, V. Langlois, A. Kaddami (PhD), M. Ceccaldi (PhD)<\/h5>\n<h5>Collaborations : M. Gu\u00e9guen (CPDM), Y. P\u00e9chaud (LGE)<\/h5>\n<p>\n<\/div><div class=\"kc-elm kc-css-118913\" style=\"height: 10px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-489333 kc_text_block\"><\/p>\n<h4>Cementitious Foams<\/h4>\n<p>Cementitious foams offer many advantages compared to traditional concrete considering its low density &#8212; and then its small carbon and material footprint &#8212; and its remarkable thermal and <a href=\"https:\/\/navier-lab.fr\/en\/research\/rheophysics-porous-media\/transport-in-porous-media\/\">acoustical damping<\/a> properties. We have produced several samples of cementitious foam with a controlled structure to better understand how the cement morphology affects the resulting foam properties. To do so, we have met the following challenges:<\/p>\n<ol>\n<li>Formulate a fresh cementitious foam with a controlled structure. We need a good understanding of the interaction between the surfactants required to produce the foam and the cement paste. Some surfactants do not stabilise the foam under very alkaline (basic) conditions. Other surfactant, notably <em>anionic<\/em> surfactants, adsorb onto the grain surface and alter their interactions: they eventually modify the yield stress of the cement paste. When the surfactant concentration is low, the cement grains become hydrophobic and induce attractive interactions between cement particles, resulting in an increase of the yield stress of the material. In contrast, at higher surfactant concentration, the micelles adsorbed onto the grains induce steric repulsion and the yield stress of the material drops. We have then studied the mechanical resistance of fresh cementitious foams for an air content of 83%. For each data series, we have modified the cement paste yield stress through the addition of superplasticisers or large amounts of anionic surfactants. Surprisingly, the most stable formulations are also the ones with the lowest yield stresses. Meticulous rheology measurements have shown that this stability originates from a collective reorganisation of cement grains towards denser arrangements between the bubbles.<\/li>\n<li>Maintain the produced structure when the cementitious foam is setting and curing.\u00a0 This part has been studied during the PhD thesis of Blandine Feneuil (2015-2018). We have studied the influence of the bubble size, the water\/cement ratio and the surfactant content on this stability. We have then formulated a stability criterion for these materials based on the bubble size and the yield stress of the interstitial cement paste.<\/li>\n<\/ol>\n<p>\n<\/div><div class=\"kc-elm kc-css-540092\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-830055 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/11\/mousse-ciment-1.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-614679\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-808290 kc_text_block\"><\/p>\n<h4>Geopolymer Foams<\/h4>\n<p>Geopolymer foams are promising materials since they combine excellent isolation efficiency, good fire resistance and mechanical loads, whereas their carbon, material footprint and overall density are <em>very<\/em> low. Controlling the pore size in these media remains challenging since the foam ages before the geopolymer sets. During the PhD thesis of Asmaa Kaddami (2016-2019), we have studied a mixture of metakaolin suspension with an aqueous foam precursor. We have presented a physical approach to limit aging phenomena in fresh geopolymer foams and maintain the pore morphology that was initially formed. We have shown that ripening arrest is achieved when the particle concentration in the continuous phase exceeds a critical value that depends on the bubble size and the gas volume fraction. We have explained this value in the framework of the <em>jamming transition<\/em> which occurs in the metakaolin suspension when it is confined in the foam network. Confinement effects confer a finite elasticity to these granular packings against bubble movement. This very general result allows us to master the morphology of geopolymer foams of industrial interest.<\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-574843\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-568400 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2020\/11\/mousse-geopolymere.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-170463\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-949392 kc_text_block\"><\/p>\n<h4>Bio-calcifying foams<\/h4>\n<p>The PhD thesis work of M. Ceccaldi has focused on the formulation of bacterial, bio-calcifying liquid foams to induce Calcium Carbonate (CaCO3) precipitation (MICP). The best-performing formulations are based on the <em>Sporosarcina pasteurii<\/em> bacterium strain and surfactants of the <em>APG <\/em>(Alkyl Poly Glucosides) family bearing two glucose (maltosides) functions. We have shown that pumping such a foam in a granular packing indeed results in CaCO3 precipitation around the contacts between grains, whereas the impact on the material porosity remains limited. We still have to evaluate the mechanical performance of materials produced using this process that we named <em>FoamMICP.<\/em><\/p>\n<p>\n<\/div><div class=\"kc-elm kc-css-712164\" style=\"height: 20px; clear: both; width:100%;\"><\/div><div class=\"kc-elm kc-css-420571 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/biocalcified-foam-schematic.jpg\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-678567 kc_shortcode kc_single_image\">\n\n        <img decoding=\"async\" src=\"https:\/\/navier-lab.fr\/wp-content\/uploads\/2024\/07\/biocalcified-foam-microscope-1.png\" class=\"\" alt=\"\" \/>    <\/div>\n<div class=\"kc-elm kc-css-641336 kc_text_block\"><\/p>\n<p style=\"text-align: center;\"><em>(Upper panel) : bio-calcification setup of a particle stack. We pump a bio-calcifying foam loaded with bacteria in this geometry before waiting. (Lower panel):\u00a0<\/em>CaCO3 formation between particle pairs after four bio-calcifying rounds. <em><br \/>\n<\/em><\/p>\n<p>\n<\/div>\n<div class=\"kc-elm kc-css-479279 divider_line\">\n\t<div class=\"divider_inner divider_line1\">\n\t\t\t<\/div>\n<\/div>\n<div class=\"kc-elm kc-css-932087 kc_text_block\"><\/p>\n<h4>References<\/h4>\n<ul>\n<li><span lang=\"EN-US\"><a href=\"https:\/\/doi.org\/10.1016\/j.cemconres.2017.04.015\">Effect of surfactants on the yield stress of cement paste<\/a>, B. Feneuil, O. Pitois, N. Roussel, <em>Cement and Concrete Research<\/em>\u00a0 <strong>100<\/strong>, 32\u201339 (2017)<\/span><\/li>\n<li><span lang=\"EN-US\"><a href=\"https:\/\/doi.org\/10.1016\/j.cemconres.2019.105865\">Stability criterion for fresh cement foams<\/a>, B. Feneuil, P. Aimedieu, M. <\/span><span lang=\"EN-US\">Scheel, J. Perrin, N. Roussel, O. Pitois, Cement and Concrete Research<\/span><span lang=\"EN-US\"><strong> 125<\/strong>, 105865 <\/span><span lang=\"EN-US\">(2019)<\/span><\/li>\n<li><a href=\"https:\/\/theses.hal.science\/tel-04438221\/\">Formulation de mousses bio-calcifiantes pour la production de mat\u00e9riaux poreux<\/a>, M. Ceccaldi, <em>Th\u00e8se de Doctorat<\/em> (2023)<\/li>\n<\/ul>\n<p>\n<\/div><\/div><\/div><\/div><\/div><\/section><\/p>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":162,"featured_media":0,"parent":12398,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-16415","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages\/16415","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\/162"}],"replies":[{"embeddable":true,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/comments?post=16415"}],"version-history":[{"count":13,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages\/16415\/revisions"}],"predecessor-version":[{"id":17262,"href":"https:\/\/navier-lab.fr\/en\/wp-json\/wp\/v2\/pages\/16415\/revisions\/17262"}],"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=16415"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}