{"id":15896,"date":"2024-06-06T18:37:47","date_gmt":"2024-06-06T16:37:47","guid":{"rendered":"https:\/\/www.icpf.cas.cz\/?p=15896"},"modified":"2024-06-06T18:46:49","modified_gmt":"2024-06-06T16:46:49","slug":"kelvin-equation-for-bridging-transitions","status":"publish","type":"post","link":"https:\/\/www.icpf.cas.cz\/en\/kelvin-equation-for-bridging-transitions\/","title":{"rendered":"Kelvin equation for bridging transitions"},"content":{"rendered":"<p style=\"text-align: justify;\">If two solid surfaces immersed in a fluid get sufficiently close together, a local condensation between them may occur. These so-called bridging transitions, referring to the formation of a liquid film connecting the surfaces, depend sensitively on their shape. The theoretical study led by <a href=\"https:\/\/www.icpf.cas.cz\/en\/employee\/doc-mgr-malijevsky-alexandr-ph-d\/\" target=\"_blank\" rel=\"noopener\">Prof. Alexandr Malijevsk\u00fd<\/a> and published in <em>Physical Review E<\/em> formulates general conditions for bridging transitions between a pair of surfaces of arbitrary shapes. We have shown that the problem can be solved effectively by an appropriate mapping of the system to a much simpler one formed by a pair of parallel plates leading to a newly generalized Kelvin equation (see Fig. 1). The equation was utilized to examine asymptotic behavior of bridging transitions and their relation to capillary condensation for a class of fundamental walls geometries. We have shown that the gradual flattening of the confining walls leads to a critical phenomenon characterized by a diverging growth of the bridging film. Associated geometry-dependent critical exponents were determined, and a covariance law revealing a relation between the geometric and Young\u2019s contact angle for wedge-like structures was found. All the analytical predictions were confirmed numerically using appropriate molecular models.<\/p>\n<p style=\"text-align: center;\"><a href=\"https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01.jpg\" data-rel=\"lightbox-image-0\" data-rl_title=\"\" data-rl_caption=\"\" title=\"\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-15894 \" src=\"https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01.jpg\" alt=\"\" width=\"747\" height=\"227\" srcset=\"https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01.jpg 1550w, https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01-300x91.jpg 300w, https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01-1024x312.jpg 1024w, https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01-768x234.jpg 768w, https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01-1536x468.jpg 1536w, https:\/\/www.icpf.cas.cz\/wp-content\/uploads\/2024\/06\/Malijevsky-2024-01-370x113.jpg 370w\" sizes=\"auto, (max-width: 747px) 100vw, 747px\" \/><\/a><\/p>\n<p style=\"text-align: center;\"><span style=\"font-size: 10pt;\">Fig. 1. Bridging between a pair of walls of complex geometry (left) can be mapped to a system formed of planar walls of appropriate dimensions (right)<\/span><\/p>\n<ul>\n<li>Malijevsk\u00fd A.*, Posp\u00ed\u0161il M.: Kelvin equation for bridging transitions. <em>Physical Review E <\/em><strong>2024<\/strong>, <em>109 <\/em>(3 March), 034801. <a href=\"https:\/\/doi.org\/DOI:%2010.1103\/PhysRevE.109.034801\" target=\"_blank\" rel=\"noopener\">doi: 10.1103\/PhysRevE.109.034801<\/a><\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>If two solid surfaces immersed in a fluid get sufficiently close together, a local condensation between them may occur. These so-called bridging transitions, referring to the formation of a liquid film connecting the surfaces, depend sensitively on their shape. The theoretical study led by Prof. Alexandr Malijevsk\u00fd and published in Physical Review E formulates general&hellip;<\/p>\n","protected":false},"author":19,"featured_media":15894,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"footnotes":""},"categories":[83],"tags":[],"class_list":["post-15896","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-scientific-achievements"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/posts\/15896","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/users\/19"}],"replies":[{"embeddable":true,"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/comments?post=15896"}],"version-history":[{"count":4,"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/posts\/15896\/revisions"}],"predecessor-version":[{"id":15902,"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/posts\/15896\/revisions\/15902"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/media\/15894"}],"wp:attachment":[{"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/media?parent=15896"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/categories?post=15896"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.icpf.cas.cz\/en\/wp-json\/wp\/v2\/tags?post=15896"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}