{"id":13,"date":"2026-07-09T08:46:45","date_gmt":"2026-07-09T08:46:45","guid":{"rendered":"http:\/\/localhost\/?page_id=13"},"modified":"2026-09-10T13:21:41","modified_gmt":"2026-09-10T13:21:41","slug":"lab","status":"publish","type":"page","link":"https:\/\/www.auriga.polimi.it\/index.php\/lab\/","title":{"rendered":"Lab"},"content":{"rendered":"\n<div class=\"wp-block-group alignfull\" style=\"padding-top:80px;padding-bottom:80px\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-container-core-group-is-layout-f538988d wp-block-group-is-layout-constrained\">\n<p class=\"is-style-eyebrow wp-block-paragraph\">The experimental campaign<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">One problem at several scales<\/h2>\n\n\n\n<p class=\"is-style-lede wp-block-paragraph\">A bubble column is designed and operated as a whole, but what it does as a whole is settled at the scale of single bubbles: how fast one rises, how it deforms, whether it drifts sideways, whether two of them merge, how much gas crosses its surface. Inside a working column those mechanisms cannot be told apart, because millions of bubbles are doing all of them at once. The campaign therefore works at two scales \u2014 isolating one mechanism at a time in small laboratory columns, then measuring the aggregate behaviour in a large-diameter one \u2014 so that what is observed at the top of the column can be traced to the physics underneath it.<\/p>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group alignfull has-surface-background-color has-background\" style=\"padding-top:80px;padding-bottom:80px\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-container-core-group-is-layout-f538988d wp-block-group-is-layout-constrained\">\n<p class=\"is-style-eyebrow wp-block-paragraph\">Small scale \u00b7 Work package b and c<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Small-scale bubble columns<\/h2>\n\n\n\n<p class=\"is-style-prose wp-block-paragraph\">Six transparent acrylic columns, they differ in the section, in the injector carried on the bottom plate \u2014 a needle, rows of needles, and  perforated plate \u2014 and in the optical access up the height, which is what decides the experiment each one can do. The working fluids range from water to the aqueous ionic-liquid mixtures the project has selected.<\/p>\n\n\n\n<div class=\"wp-block-group rig-grid\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-group rig-row\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<figure class=\"wp-block-image size-full rig-drawing\"><img loading=\"lazy\" decoding=\"async\" width=\"156\" height=\"829\" src=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-single-bubble.png\" alt=\"CAD elevation of the single-bubble column\" class=\"wp-image-342\"\/><\/figure>\n\n\n\n<div class=\"wp-block-group rig-text\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<h3 class=\"wp-block-heading\">Single-bubble column<\/h3>\n\n\n\n<p class=\"is-style-prose wp-block-paragraph\">A rectangular column releases single bubbles, tracked with a high-speed camera to study how they rise, change shape, and wobble in water and ionic liquid solutions, revealing the basic physics behind bubble behaviour in liquids.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group rig-row\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<figure class=\"wp-block-image size-full rig-drawing\"><img loading=\"lazy\" decoding=\"async\" width=\"186\" height=\"810\" src=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-bubble-swarm.png\" alt=\"CAD elevation of the rectangular bubble-swarm column\" class=\"wp-image-343\" srcset=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-bubble-swarm.png 186w, https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-bubble-swarm-69x300.png 69w\" sizes=\"auto, (max-width: 186px) 100vw, 186px\" \/><\/figure>\n\n\n\n<div class=\"wp-block-group rig-text\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<h3 class=\"wp-block-heading\">Bubble-swarm column<\/h3>\n\n\n\n<p class=\"is-style-prose wp-block-paragraph\">A rectangular column with perforated plates of different hole sizes generates a controlled bubble swarm, tracked through image analysis and gas holdup measurements to reveal flow-regime behaviour feeding into a broader theory of bubble columns.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group rig-row\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<figure class=\"wp-block-image size-full rig-drawing\"><img loading=\"lazy\" decoding=\"async\" width=\"108\" height=\"812\" src=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-swarm-cylindrical.png\" alt=\"CAD elevation of the cylindrical bubble-swarm column\" class=\"wp-image-344\" srcset=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-swarm-cylindrical.png 108w, https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-swarm-cylindrical-40x300.png 40w\" sizes=\"auto, (max-width: 108px) 100vw, 108px\" \/><\/figure>\n\n\n\n<div class=\"wp-block-group rig-text\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<h3 class=\"wp-block-heading\">Circular bubble-swarm column<\/h3>\n\n\n\n<p class=\"is-style-prose wp-block-paragraph\">The circular counterpart of the swarm column: a cylindrical body flanged at both ends, with a perforated distributor across the bottom flange and access fittings at six heights. This column has three different spargers and it main purpose is to study the operating curve.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group rig-row\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<figure class=\"wp-block-image size-full rig-drawing\"><img loading=\"lazy\" decoding=\"async\" width=\"401\" height=\"590\" src=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-coalescence.png\" alt=\"CAD view of the coalescence cell\" class=\"wp-image-345\" srcset=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-coalescence.png 401w, https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-coalescence-204x300.png 204w\" sizes=\"auto, (max-width: 401px) 100vw, 401px\" \/><\/figure>\n\n\n\n<div class=\"wp-block-group rig-text\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<h3 class=\"wp-block-heading\">Coalescence cell<\/h3>\n\n\n\n<p class=\"is-style-prose wp-block-paragraph\">A short rectangular cell with two capillaries entering through opposite walls and meeting at the centre, so that two bubbles can be brought together under controlled conditions. It measures the coalescence of bubbles, recorded by high-speed imaging against a backlight.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group rig-row\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<figure class=\"wp-block-image size-full rig-drawing\"><img loading=\"lazy\" decoding=\"async\" width=\"182\" height=\"849\" src=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-cfd-grade.png\" alt=\"CAD elevation of the CFD-grade column\" class=\"wp-image-346\" srcset=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-cfd-grade.png 182w, https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-cfd-grade-64x300.png 64w\" sizes=\"auto, (max-width: 182px) 100vw, 182px\" \/><\/figure>\n\n\n\n<div class=\"wp-block-group rig-text\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<h3 class=\"wp-block-heading\">CFD-grade column<\/h3>\n\n\n\n<p class=\"is-style-prose wp-block-paragraph\">A rectangular column with a controlled injection sparger where each hole can be operated independently, giving measurements clean and repeatable enough to serve as a validation case for the project&#8217;s numerical work.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group rig-row\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<figure class=\"wp-block-image size-full rig-drawing\"><img loading=\"lazy\" decoding=\"async\" width=\"204\" height=\"849\" src=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-mass-transfer.png\" alt=\"CAD elevation of the mass-transfer column\" class=\"wp-image-347\" srcset=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-mass-transfer.png 204w, https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/rig-mass-transfer-72x300.png 72w\" sizes=\"auto, (max-width: 204px) 100vw, 204px\" \/><\/figure>\n\n\n\n<div class=\"wp-block-group rig-text\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<h3 class=\"wp-block-heading\">Mass-transfer column<\/h3>\n\n\n\n<p class=\"is-style-prose wp-block-paragraph\">A circular column enclosed by a square enclosure to remove refraction effects in image analysis, dedicated to the interfacial mass transfer between the gas and the liquid \u2014 the step that connects the bubble-scale work to the CO\u2082 absorption the project is aiming at.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group alignfull\" style=\"padding-top:80px;padding-bottom:80px\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-container-core-group-is-layout-f538988d wp-block-group-is-layout-constrained\">\n<p class=\"is-style-eyebrow wp-block-paragraph\">Large scale \u00b7 Work package D<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Large-diameter bubble column<\/h2>\n\n\n\n<div class=\"wp-block-group large-col\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"large-col-drawing\"><img decoding=\"async\" src=\"https:\/\/www.auriga.polimi.it\/wp-content\/uploads\/2026\/09\/large-column-drawing-scaled.png\" alt=\"CAD elevation of the large-diameter bubble column\"><\/div>\n\n\n\n<div class=\"wp-block-group large-col-text\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<p class=\"is-style-lede wp-block-paragraph\">A circular large-diameter column (4.5 m height, 0.39 m inner diameter) dedicated to flow patterns, coherent structures and the local and global fluid-dynamic properties along the \u03a9-curve.<\/p>\n\n\n\n<ul class=\"wp-block-list is-style-spec-list\">\n<li><strong>Column<\/strong> \u2014 4.5 m height, 0.39 m inner diameter, 2.5 m initial liquid level, liquid recirculation, gas sparger region 0.40 m<\/li>\n\n\n\n<li><strong>Spargers<\/strong> \u2014 Interchangeable perforated plates with different hole diameters<\/li>\n\n\n\n<li><strong>Global measurements<\/strong> \u2014 Gas holdup, gas disengagement, global mass transfer<\/li>\n\n\n\n<li><strong>Local measurements<\/strong> \u2014 Three optical probes (void fraction, bubble size, velocity), wire-mesh sensors, image analysis near the sparger and at different radial\/axial positions<\/li>\n<\/ul>\n<\/div><\/div>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-group alignfull has-surface-background-color has-background\" style=\"padding-top:80px;padding-bottom:80px\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-container-core-group-is-layout-f538988d wp-block-group-is-layout-constrained\">\n<p class=\"is-style-eyebrow wp-block-paragraph\">Instrumentation<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Instruments and computing resources<\/h2>\n\n\n\n<p class=\"is-style-lede wp-block-paragraph\">The measurement chain behind the two experimental scales, and the computing resources that process what it produces.<\/p>\n\n\n\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"instrument-grid\">\n\n  <div class=\"instrument\">\n    <svg viewBox=\"0 0 48 48\" fill=\"none\" stroke=\"currentColor\" stroke-width=\"1.6\" stroke-linecap=\"round\" aria-hidden=\"true\">\n      <circle cx=\"24\" cy=\"24\" r=\"17\"><\/circle>\n      <path d=\"M16 9v30M24 7v34M32 9v30M9 16h30M7 24h34M9 32h30\"><\/path>\n      <circle cx=\"24\" cy=\"24\" r=\"1.6\" fill=\"currentColor\" stroke=\"none\"><\/circle>\n      <circle cx=\"16\" cy=\"32\" r=\"1.6\" fill=\"currentColor\" stroke=\"none\"><\/circle>\n      <circle cx=\"32\" cy=\"16\" r=\"1.6\" fill=\"currentColor\" stroke=\"none\"><\/circle>\n    <\/svg>\n    <p class=\"instrument-kind\">Measurement<\/p>\n    <h4>Wire-mesh sensor<\/h4>\n    <p>Gas fraction resolved over the whole cross-section of the column, at high acquisition rate, from the conductance between two crossing planes of wires.<\/p>\n  <\/div>\n\n  <div class=\"instrument\">\n    <svg viewBox=\"0 0 48 48\" fill=\"none\" stroke=\"currentColor\" stroke-width=\"1.6\" stroke-linecap=\"round\" aria-hidden=\"true\">\n      <circle cx=\"24\" cy=\"13\" r=\"7.5\"><\/circle>\n      <path d=\"M19 42V24M29 42V29\"><\/path>\n      <circle cx=\"19\" cy=\"22.5\" r=\"1.8\" fill=\"currentColor\" stroke=\"none\"><\/circle>\n      <circle cx=\"29\" cy=\"27.5\" r=\"1.8\" fill=\"currentColor\" stroke=\"none\"><\/circle>\n    <\/svg>\n    <p class=\"instrument-kind\">Measurement<\/p>\n    <h4>Optical probes<\/h4>\n    <p>Local measurements at a point in the flow. Dual-tip probes give void fraction, bubble chord length and bubble velocity from the time each tip spends in the gas; Doppler probes give the velocity of the dispersed phase without touching it, from the frequency shift of the backscattered light.<\/p>\n  <\/div>\n\n  <div class=\"instrument\">\n    <svg viewBox=\"0 0 48 48\" fill=\"none\" stroke=\"currentColor\" stroke-width=\"1.6\" stroke-linecap=\"round\" aria-hidden=\"true\">\n      <rect x=\"6\" y=\"14\" width=\"29\" height=\"22\" rx=\"3\"><\/rect>\n      <path d=\"M15 14l2.5-4h7L27 14\" stroke-linejoin=\"round\"><\/path>\n      <circle cx=\"20.5\" cy=\"25\" r=\"6.5\"><\/circle>\n      <circle cx=\"20.5\" cy=\"25\" r=\"2\" fill=\"currentColor\" stroke=\"none\"><\/circle>\n      <path d=\"M35 21l7-4v16l-7-4z\" stroke-linejoin=\"round\"><\/path>\n    <\/svg>\n    <p class=\"instrument-kind\">Measurement<\/p>\n    <h4>High-speed cameras<\/h4>\n    <p>Phantom and FLIR cameras record the flow at high frame rate \u2014 the images behind Particle Shadow Velocimetry, bubble tracking, and the size, shape and velocity statistics drawn from them.<\/p>\n  <\/div>\n\n    <div class=\"instrument\">\n    <svg viewBox=\"0 0 48 48\" fill=\"none\" stroke=\"currentColor\" stroke-width=\"1.6\" stroke-linecap=\"round\" aria-hidden=\"true\">\n      <path d=\"M12 14v20a5 5 0 0 0 5 5h14a5 5 0 0 0 5-5V14\" stroke-linejoin=\"round\"><\/path>\n      <path d=\"M19 6v24M29 6v24\"><\/path>\n      <path d=\"M22 17h4M22 22h4M22 27h4\"><\/path>\n    <\/svg>\n    <p class=\"instrument-kind\">Measurement<\/p>\n    <h4>Conductivity meter<\/h4>\n    <p>For the measurements of the electrical conductivity of the liquid phase, which is related to the CO\u2082 uptake and impurity content.<\/p>\n  <\/div>\n\n  <div class=\"instrument\">\n    <svg viewBox=\"0 0 48 48\" fill=\"none\" stroke=\"currentColor\" stroke-width=\"1.6\" stroke-linecap=\"round\" aria-hidden=\"true\">\n      <path d=\"M24 6c0 0-10 12-10 20a10 10 0 0 0 20 0C34 18 24 6 24 6z\" stroke-linejoin=\"round\"><\/path>\n      <path d=\"M10 42h28\"><\/path>\n      <path d=\"M14 42v-3M24 42v-3M34 42v-3\"><\/path>\n    <\/svg>\n    <p class=\"instrument-kind\">Measurement<\/p>\n    <h4>pH meter<\/h4>\n    <p>pH of the liquid phase, monitored alongside conductivity while the solvent mixtures are prepared and while they take up CO\u2082.<\/p>\n  <\/div>\n\n  <div class=\"instrument\">\n    <svg viewBox=\"0 0 48 48\" fill=\"none\" stroke=\"currentColor\" stroke-width=\"1.6\" stroke-linecap=\"round\" aria-hidden=\"true\">\n      <rect x=\"12\" y=\"12\" width=\"24\" height=\"24\" rx=\"3\"><\/rect>\n      <rect x=\"19\" y=\"19\" width=\"10\" height=\"10\" rx=\"1.5\"><\/rect>\n      <path d=\"M18 12V7M24 12V7M30 12V7M18 41v-5M24 41v-5M30 41v-5M12 18H7M12 24H7M12 30H7M41 18h-5M41 24h-5M41 30h-5\"><\/path>\n    <\/svg>\n    <p class=\"instrument-kind\">Computing<\/p>\n    <h4>NVIDIA H200 GPU<\/h4>\n    <p>The compute behind the numerical side of the project: simulations and the image-analysis pipelines that turn recordings into bubble statistics.<\/p>\n  <\/div>\n\n<\/div>\n<\/div><\/div>\n<\/div><\/div>\n","protected":false},"excerpt":{"rendered":"<p>The experimental campaign One problem at several scales A bubble column is designed and operated as a whole, but what it does as a whole is settled at the scale of single bubbles: how fast one rises, how it deforms, whether it drifts sideways, whether two of them merge, how much gas crosses its surface. [&hellip;]<\/p>\n","protected":false},"author":6,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-13","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/pages\/13","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/users\/6"}],"replies":[{"embeddable":true,"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/comments?post=13"}],"version-history":[{"count":40,"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/pages\/13\/revisions"}],"predecessor-version":[{"id":439,"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/pages\/13\/revisions\/439"}],"wp:attachment":[{"href":"https:\/\/www.auriga.polimi.it\/index.php\/wp-json\/wp\/v2\/media?parent=13"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}