{"id":410,"date":"2024-01-18T22:44:30","date_gmt":"2024-01-19T03:44:30","guid":{"rendered":"https:\/\/research.gsd.harvard.edu\/grg\/?page_id=410"},"modified":"2024-02-23T12:32:26","modified_gmt":"2024-02-23T17:32:26","slug":"thin-film-cooling","status":"publish","type":"page","link":"https:\/\/research.gsd.harvard.edu\/grg\/thin-film-cooling\/","title":{"rendered":"Thin Film Cooling"},"content":{"rendered":"\n<p>                                  <\/p>\n\n\n\n<div class=\"wp-block-group alignwide\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-columns alignwide is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<div class=\"wp-block-group is-vertical is-layout-flex wp-container-core-group-is-layout-8cf370e7 wp-block-group-is-layout-flex\">\n<p class=\"has-medium-font-size\" style=\"font-style:normal;font-weight:500\">Grinham Research Group<\/p>\n\n\n\n<p class=\"has-small-font-size\" style=\"font-style:normal;font-weight:300\">Harvard University Graduate School of Design<\/p>\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator alignwide has-alpha-channel-opacity\" \/>\n<\/div><\/div>\n\n\n\n<h1 class=\"wp-block-heading alignwide has-large-font-size\" id=\"h-thin-film-cooling\" style=\"font-style:normal;font-weight:300\">Thin Film Cooling<\/h1>\n\n\n\n<h1 class=\"wp-block-heading alignwide has-small-font-size\" style=\"font-style:normal;font-weight:300\">Cooling<\/h1>\n\n\n\n<div style=\"height:25px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<div class=\"wp-block-columns alignwide is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<h2 class=\"wp-block-heading has-medium-font-size\" id=\"h-project-overview\">Project Overview<\/h2>\n\n\n\n<div style=\"height:10px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<p class=\"has-small-font-size\" style=\"font-style:normal;font-weight:400\">In this study, we report a paradigmatic shift in bioinspired microchannel heat exchanger design towards its integration into thin film wearable devices, thermally active surfaces in buildings, photovoltaic devices, and other thermoregulating devices whose typical cooling fluxes are below 1 kW\/m2. The transparent thermoregulation device is fabricated by bonding a thin corrugated elastomeric film to the surface of a substrate to form a microchannel water-circuit with bioinspired unit cell geometry. <\/p>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<p class=\"has-small-font-size\" style=\"font-style:normal;font-weight:400\"><\/p>\n<\/div>\n<\/div>\n\n\n\n<figure class=\"wp-block-image alignwide size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"575\" src=\"https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_1-1024x575.jpg\" alt=\"Prototype of thin film cooling with diamond grid channels\" class=\"wp-image-411\" srcset=\"https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_1-1024x575.jpg 1024w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_1-300x169.jpg 300w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_1-768x432.jpg 768w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_1.jpg 1500w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<div style=\"height:25px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h2 class=\"wp-block-heading alignwide has-medium-font-size\" id=\"h-innovation\">Innovation<\/h2>\n\n\n\n<div class=\"wp-block-columns alignwide is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<h3 class=\"wp-block-heading has-small-font-size\" id=\"h-project-team\" style=\"font-style:normal;font-weight:400\">Project Team<\/h3>\n\n\n\n<div style=\"height:10px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<p class=\"color: #f542f5 has-black-color has-text-color has-small-font-size\" style=\"font-style:normal;font-weight:300\">Jonathan Grinham<br>Matthew J. Hancock<br>Kitty Kumar<br>Martin Bechthold<br>Donald E. Ingber<br>Joanna Aizenberg<\/p>\n\n\n\n<p><\/p>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.67%\">\n<p class=\"has-small-font-size\" style=\"font-style:normal;font-weight:400\">Inspired by the dynamic scaling of flow systems in nature, empirically derived sizing<br>rules and a novel numerical optimization method implemented in MATLAB\u00ae with COMSOL Multiphysics\u00ae are used to maximize the thermoregulation performance of the<br>microchannel network by enhancing the uniformity of flow distribution. The optimized network design results in a 25% to 37% increase in the heat flux compared to non-optimized designs. The study demonstrates the versatility of the presented device design and architecture by fabricating and testing a scaled-up numerically optimized heat exchanger design for building-scale and wearable applications.<\/p>\n<\/div>\n<\/div>\n\n\n\n<figure class=\"wp-block-image alignwide size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"768\" src=\"https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_2-1024x768.jpg\" alt=\"Chart showing relationship between surface area and cooling flux\" class=\"wp-image-412\" srcset=\"https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_2-1024x768.jpg 1024w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_2-300x225.jpg 300w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_2-768x576.jpg 768w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_2-1536x1152.jpg 1536w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_2-2048x1536.jpg 2048w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<figure class=\"wp-block-image alignwide size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"455\" src=\"https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_3-1024x455.jpg\" alt=\"Comparison of simulation and experimental results\" class=\"wp-image-413\" srcset=\"https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_3-1024x455.jpg 1024w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_3-300x133.jpg 300w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_3-768x341.jpg 768w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_3-1536x683.jpg 1536w, https:\/\/research.gsd.harvard.edu\/grg\/files\/2024\/01\/ThinFilmCooling_web_3-2048x911.jpg 2048w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<hr class=\"wp-block-separator alignwide has-alpha-channel-opacity\" \/>\n","protected":false},"excerpt":{"rendered":"<p>Grinham Research Group Harvard University Graduate School of Design Thin Film Cooling Cooling Project Overview In this study, we report [&hellip;]<\/p>\n","protected":false},"author":178,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"_mi_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"class_list":["post-410","page","type-page","status-publish","hentry"],"acf":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO Premium plugin v20.10 (Yoast SEO v26.7) - 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