{"id":519420,"date":"2010-04-07T05:22:23","date_gmt":"2010-04-07T09:22:23","guid":{"rendered":"tag:www.mentor.com:\/\/66822328f119bcbc19528d6bdc4526ce"},"modified":"2010-04-07T05:22:23","modified_gmt":"2010-04-07T09:22:23","slug":"blog-posthow-much-do-%e2%80%98u-value%e2%80%99-good-thermal-insulation-part-vii-ooo-shut-that-door","status":"publish","type":"post","link":"https:\/\/mereja.media\/index\/519420","title":{"rendered":"blog post:How much do \u2018U-Value\u2019 good thermal insulation? Part VII &#8211; &#8220;Ooo, shut that door&#8221;"},"content":{"rendered":"<p><a href=\"http:\/\/en.wikipedia.org\/wiki\/Larry_Grayson\" >Larry Grayson\u2019s<\/a>\u00a0famous high camp catchphrase would be well heeded by those wanting to ensure good thermal insulation. You can make it difficult for heat to leave a room, thus maintain a warm room temperature, by constructing walls and floors of sandwiched layers of various materials, restricting heat transfer to conduction and (in cavities) radiation methods only. Open a door however and cold air will rush in. Open a door just a crack and\u00a0even a\u00a0trickle of cold air can result in\u00a0a substantial decrease in U-value.<!--more--><\/p>\n<p>[Links to download and inspect the FloVENT models used in this blog can be found at the bottom of the page]<\/p>\n<p>To investigate this let\u2019s take the model we\u2019ve been using and\u00a0stick a door in the outer wall.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-976\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/room_with_door.jpg\" alt=\"room_with_door\" width=\"316\" height=\"287\" \/><\/p>\n<p>The resulting temperature distribution in the room is:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-978\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/room_temp.jpg\" alt=\"room_temp\" width=\"420\" height=\"260\" \/><\/p>\n<p>Despite the fact this is part 7 in a series about U-Value we\u2019ve done precious little U-value calculations. To derive the U-value for room as a whole,\u00a0we need to know the amount of heat that leaves the room (= the amount of heat dissipated by the radiator), the total surface area of room, the internal room temperature and the external temperature. For this model:<\/p>\n<p><!--content--><\/p>\n<p>U-value = 200W \/ (20.6 degC &#8211; 2.0 degC) x\u00a07.9 m\u00b2 =\u00a01.36 W\/m\u00b2K<\/p>\n<p>Considering UK building regs stipulate a U-value of less than 0.3 W\/m\u00b2K the value of\u00a01.36 W\/m\u00b2K is really bad, why? For this model we are effectively looking at\u00a0only a\u00a0relatively small section of a room (think of it as part of a corridor), a section that has a disproportionately large area of door in it. Compared to a 300 mm thick cavity wall, doors are really rubbish at restricting heat, it is this that is pushing up this \u2018local\u2019 U-value.<\/p>\n<p>So, let\u2019s open the door a crack, a 5mm gap to be precise. Simply a question of redefining the geometry in the model to resolve the gap between door and jam (the wall above door is hidden for clarity in this image):<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-980\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/door_gap.png\" alt=\"door_gap\" width=\"435\" height=\"282\" \/><\/p>\n<p>Whether the air can only enter\/leave the room through the door gap or whether there is another gap somewhere else in the room that allows the air to flow right through can have a large effect on the resulting U-value. To investigate this two models are simulated, one with the room sealed apart from the door gap. The\u00a0other model has a gap under another internal door leading to another room. Comparing the resulting temperature distributions for both models shows marked differences:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-1008\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/door_gaps_temp.jpg\" alt=\"door_gaps_temp\" width=\"546\" height=\"452\" \/><\/p>\n<p>\u00a0Remembering that the U-value for the room section with the door closed was\u00a01.36 W\/m\u00b2K, with\u00a0a\u00a0door gap but the rest of the room sealed the U-value is\u00a01.43 W\/m\u00b2K, an increase\u00a0 (compared to no door gap) of 5%. With an internal door gap allowing throughflow the U-value becomes\u00a01.63 W\/m\u00b2K, an increase (compared to no door gap) of 20%.<\/p>\n<p>A CFD based simulation using <a href=\"http:\/\/www.mentor.com\/products\/mechanical\/products\/flovent\" >FloVENT<\/a> provides more than just the opportunity to observe temperatures. By examining air flow patterns an understanding of why the temperatures are what they are can be gleaned. A great way of understanding the airflow patterns is to animate air flow arrows, akin to introducing smoke in the door gap to visualise the subsequent convection of air passing through the gap. The animation below shows the trickling of cold air that comes in the lower portion of the door crack:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-1000\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/gap_anim1.gif\" alt=\"gap_anim1\" width=\"480\" height=\"360\" \/><\/p>\n<p>With the rest of the room sealed, any air trickling in through the gap has to be balanced by air being pushed out. The simulation predicts, as expected, that the cold air trickles in through the bottom half of the crack and warmer air trickles back out the top portion, a double whammy.<\/p>\n<p>By introducing another gap under an internal door in the opposite wall a through flow of air is established. In this case air trickles in through the entire gap of the outer door, dumps down to the floor, spreads and leaves through the opposing under door gap. The overall trickle rate is much larger and dumps cold air across much more of the floor area:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-1002\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/gapx2_anim.gif\" alt=\"gapx2_anim\" width=\"480\" height=\"360\" \/><\/p>\n<p>\u00a0Another great visualisation \u2018tool\u2019 is the ability to plot 2D planes of constant value, called \u2018iso-surfaces\u2019. The picture below shows iso-surfaces of where the air is at 14 degC, decidedly cold. The volume \u2018under\u2019 the iso-surface puddle is less than 14 degC. With a single door crack this cold puddle is somewhat restricted to the area near the door. For the double gap model this puddle volume extends over nearly all the floor surface:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-1010\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/door_gaps_iso_temp.jpg\" alt=\"door_gaps_iso_temp\" width=\"556\" height=\"437\" \/><\/p>\n<p>To badly corrupt an Oscar Wilde quote: \u201cTo suffer one door gap can be regarded as misfortune; to suffer two looks like carelessness\u201d<\/p>\n<p>***FREE MODEL DOWNLOAD FOR FLOVIZ***<\/p>\n<p>As described in <a href=\"http:\/\/blogs.mentor.com\/robinbornoff\/blog\/2010\/01\/27\/floviz-the-free-flothermflovent-cfd-results-viewer-try-it-its-free\/\" >this previous post<\/a>, FloVIZ is a freely available viewer to import and inspect, in real time and in 3D, the CFD simulation results from FloVENT. Below are links to the 3 models (.pack files) used in this blog. If you haven\u2019t downloaded and installed FloVIZ already, <a href=\"http:\/\/www.mentor.com\/products\/mechanical\/downloads\/floviz-viewer-evaluate\" ><strong>do it now<\/strong><\/a> then download the models, [File\/Import pack file&#8230;] and away you go <img src='http:\/\/blogs.mentor.com\/robinbornoff\/wp-includes\/images\/smilies\/icon_smile.gif' alt=':)' class='wp-smiley' \/> <\/p>\n<p><a href=\"http:\/\/s3.mentor.com\/robinbornoff\/U_Value_VII\/Room-U-Value-with-Closed-Door.pack\" ><img loading=\"lazy\" decoding=\"async\" class=\"alignleft size-full wp-image-1024\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/room_temp_s1.jpg\" alt=\"room_temp_s1\" width=\"100\" height=\"75\" \/>\u00a0Initial model with the closed door (Room-U-Value-with-Closed-Door.pack 22MB)<\/a><\/p>\n<p>\u00a0<\/p>\n<p><a href=\"http:\/\/s3.mentor.com\/robinbornoff\/U_Value_VII\/Room-U-Value-with-Door-Crack.pack\" ><img loading=\"lazy\" decoding=\"async\" class=\"alignleft size-full wp-image-1026\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/room_temp_gap_s.jpg\" alt=\"room_temp_gap_s\" width=\"100\" height=\"75\" \/>Single door crack in the outer door (Room-U-Value-with-Door-Crack.pack 33MB)<\/a><\/p>\n<p>\u00a0<\/p>\n<p><a href=\"http:\/\/s3.mentor.com\/robinbornoff\/U_Value_VII\/Room-U-Value-with-x2-Door-Cracks.pack\" ><img loading=\"lazy\" decoding=\"async\" class=\"alignleft size-full wp-image-1028\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff\/files\/2010\/04\/room_temp_gapx2_s.jpg\" alt=\"room_temp_gapx2_s\" width=\"100\" height=\"75\" \/>Door crack in outer door and under inner door (Room-U-Value-with-x2-Door-Cracks.pack 40MB)<\/a><\/p>\n<p>\u00a0<\/p>\n<p>Enjoy!<\/p>\n<p>7th April 2010 Hampton Court<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/feeds.feedburner.com\/~r\/mgc_mechanical\/~4\/LJtwlmp9ibA\" height=\"1\" width=\"1\"\/><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Larry Grayson\u2019s\u00a0famous high camp catchphrase would be well heeded by those wanting to ensure good thermal insulation. You can make it difficult for heat to leave a room, thus maintain a warm room temperature, by constructing walls and floors of sandwiched layers of various materials, restricting heat transfer to conduction and (in cavities) radiation methods [&hellip;]<\/p>\n","protected":false},"author":2981,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7],"tags":[],"class_list":["post-519420","post","type-post","status-publish","format-standard","hentry","category-news"],"_links":{"self":[{"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/posts\/519420","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/users\/2981"}],"replies":[{"embeddable":true,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/comments?post=519420"}],"version-history":[{"count":0,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/posts\/519420\/revisions"}],"wp:attachment":[{"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/media?parent=519420"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/categories?post=519420"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/tags?post=519420"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}