{"id":1334,"date":"2014-07-01T11:19:02","date_gmt":"2014-07-01T09:19:02","guid":{"rendered":"https:\/\/hylab.infinitodesign.net\/services\/numeric\/development-of-meshless-numerical-schemes\/"},"modified":"2014-07-01T11:19:02","modified_gmt":"2014-07-01T09:19:02","slug":"development-of-meshless-numerical-schemes","status":"publish","type":"page","link":"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/development-of-meshless-numerical-schemes\/","title":{"rendered":"Development of Meshless numerical schemes"},"content":{"rendered":"\n<p class=\"has-ast-global-color-0-color has-text-color has-medium-font-size\">Both development of 3D meshless numerical scheme and their use to simulate fluid\/structure interaction problem, and free \u2013 surface flow where the assumption of Shallow Water Equations are no longer valid.<\/p>\n\n<p>In this framework the development of variable resolution Smoothed Particle Hydrodynamics numerical schemes is conducted.<\/p>\n\n<figure class=\"wp-block-embed is-type-rich is-provider-handler-delloggetto-incorporato wp-block-embed-handler-delloggetto-incorporato wp-embed-aspect-16-9 wp-has-aspect-ratio\"><div class=\"wp-block-embed__wrapper\">\n<div class=\"ast-oembed-container\" style=\"height: 100%;\"><iframe loading=\"lazy\" title=\"3D SPH numerical simulation of the wave generated by the Vajont rockslide explanation.\" width=\"500\" height=\"281\" src=\"https:\/\/www.youtube.com\/embed\/NK2T_ICe8v8?feature=oembed\" frameborder=\"0\" allow=\"accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture\" allowfullscreen><\/iframe><\/div>\n<\/div><figcaption><em>A 3D numerical modeling of the wave generated by the Vajont slide, obtained by the meshless SPH technique \u2013 dualsphysics (<a href=\"http:\/\/dual.sphysics.org\">dual.sphysics.org<\/a>) software.<\/em><\/figcaption><\/figure>\n\n<div style=\"height:1em\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n<figure class=\"wp-block-embed is-type-rich is-provider-handler-delloggetto-incorporato wp-block-embed-handler-delloggetto-incorporato wp-embed-aspect-16-9 wp-has-aspect-ratio\"><div class=\"wp-block-embed__wrapper\">\n<div class=\"ast-oembed-container\" style=\"height: 100%;\"><iframe loading=\"lazy\" title=\"Variable Resolution SPH flow past a cylinder (Renato Vacondio)\" width=\"500\" height=\"375\" src=\"https:\/\/www.youtube.com\/embed\/Ifj-EDhlRkQ?feature=oembed\" frameborder=\"0\" allow=\"accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture\" allowfullscreen><\/iframe><\/div>\n<\/div><figcaption><em>Variable resolution simulations of flow past a cylinder (Re=100) obtained by SPH numerical scheme SPHysics.<\/em><\/figcaption><\/figure>\n","protected":false},"excerpt":{"rendered":"<p>Both development of 3D meshless numerical scheme and their use to simulate fluid\/structure interaction problem, and free \u2013 surface flow where the assumption of Shallow Water Equations are no longer valid. In this framework the development of variable resolution Smoothed Particle Hydrodynamics numerical schemes is conducted.<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":1190,"menu_order":0,"comment_status":"closed","ping_status":"open","template":"","meta":{"site-sidebar-layout":"default","site-content-layout":"default","ast-global-header-display":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":""},"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v19.9 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Development of Meshless numerical schemes - HyLab<\/title>\n<meta name=\"robots\" content=\"noindex, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Development of Meshless numerical schemes - HyLab\" \/>\n<meta property=\"og:description\" content=\"Both development of 3D meshless numerical scheme and their use to simulate fluid\/structure interaction problem, and free \u2013 surface flow where the assumption of Shallow Water Equations are no longer valid. In this framework the development of variable resolution Smoothed Particle Hydrodynamics numerical schemes is conducted.\" \/>\n<meta property=\"og:url\" content=\"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/development-of-meshless-numerical-schemes\/\" \/>\n<meta property=\"og:site_name\" content=\"HyLab\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<script type=\"application\/ld+json\" class=\"yoast-schema-graph\">{\"@context\":\"https:\/\/schema.org\",\"@graph\":[{\"@type\":\"WebPage\",\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/development-of-meshless-numerical-schemes\/\",\"url\":\"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/development-of-meshless-numerical-schemes\/\",\"name\":\"Development of Meshless numerical schemes - HyLab\",\"isPartOf\":{\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/#website\"},\"datePublished\":\"2014-07-01T09:19:02+00:00\",\"dateModified\":\"2014-07-01T09:19:02+00:00\",\"breadcrumb\":{\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/development-of-meshless-numerical-schemes\/#breadcrumb\"},\"inLanguage\":\"en-US\",\"potentialAction\":[{\"@type\":\"ReadAction\",\"target\":[\"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/development-of-meshless-numerical-schemes\/\"]}]},{\"@type\":\"BreadcrumbList\",\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/development-of-meshless-numerical-schemes\/#breadcrumb\",\"itemListElement\":[{\"@type\":\"ListItem\",\"position\":1,\"name\":\"Home\",\"item\":\"http:\/\/hylabnew.unipr.it\/en\/\"},{\"@type\":\"ListItem\",\"position\":2,\"name\":\"Services\",\"item\":\"http:\/\/hylabnew.unipr.it\/en\/services\/\"},{\"@type\":\"ListItem\",\"position\":3,\"name\":\"Numeric Services\",\"item\":\"http:\/\/hylabnew.unipr.it\/en\/services\/numeric\/\"},{\"@type\":\"ListItem\",\"position\":4,\"name\":\"Development of Meshless numerical schemes\"}]},{\"@type\":\"WebSite\",\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/#website\",\"url\":\"http:\/\/hylabnew.unipr.it\/en\/\",\"name\":\"HyLab\",\"description\":\"Parma Hydraulic Engineering Research Lab\",\"publisher\":{\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/#organization\"},\"potentialAction\":[{\"@type\":\"SearchAction\",\"target\":{\"@type\":\"EntryPoint\",\"urlTemplate\":\"http:\/\/hylabnew.unipr.it\/en\/?s={search_term_string}\"},\"query-input\":\"required name=search_term_string\"}],\"inLanguage\":\"en-US\"},{\"@type\":\"Organization\",\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/#organization\",\"name\":\"HyLab\",\"url\":\"http:\/\/hylabnew.unipr.it\/en\/\",\"logo\":{\"@type\":\"ImageObject\",\"inLanguage\":\"en-US\",\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/#\/schema\/logo\/image\/\",\"url\":\"https:\/\/i0.wp.com\/hylabnew.unipr.it\/wp-content\/uploads\/2022\/06\/hylab-logo-2.png?fit=635%2C200\",\"contentUrl\":\"https:\/\/i0.wp.com\/hylabnew.unipr.it\/wp-content\/uploads\/2022\/06\/hylab-logo-2.png?fit=635%2C200\",\"width\":635,\"height\":200,\"caption\":\"HyLab\"},\"image\":{\"@id\":\"http:\/\/hylabnew.unipr.it\/en\/#\/schema\/logo\/image\/\"}}]}<\/script>\n<!-- \/ Yoast SEO plugin. -->","yoast_head_json":{"title":"Development of Meshless numerical schemes - HyLab","robots":{"index":"noindex","follow":"follow","max-snippet":"max-snippet:-1","max-image-preview":"max-image-preview:large","max-video-preview":"max-video-preview:-1"},"og_locale":"en_US","og_type":"article","og_title":"Development of Meshless numerical schemes - HyLab","og_description":"Both development of 3D meshless numerical scheme and their use to simulate fluid\/structure interaction problem, and free \u2013 surface flow where the assumption of Shallow Water Equations are no longer valid. 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