{"id":283656,"date":"2010-02-02T15:31:38","date_gmt":"2010-02-02T20:31:38","guid":{"rendered":"tag:www.mentor.com:\/\/927a8aa710f17b13e152fdbde8f5cc1c"},"modified":"2010-02-02T15:31:38","modified_gmt":"2010-02-02T20:31:38","slug":"blog-posthow-much-do-%e2%80%98u-value%e2%80%99-good-thermal-insulation-part-ii","status":"publish","type":"post","link":"https:\/\/mereja.media\/index\/283656","title":{"rendered":"blog post:How much do \u2018U-Value\u2019 good thermal insulation? Part II"},"content":{"rendered":"<p>It might well be that a single U-value is quoted, in reality though that single value describes the ease by which heat can pass through various stages, from an \u2018inside\u2019, passing through a \u2018wall\/window\u2019 and going to the \u2018outside\u2019. The resistance (inverse of the ease, resistance = 1\/ease) the heat experiences as it passes from the inside air to the inner solid surface of the wall construction (and from the outer surface to the outside air)\u00a0 is due to the fact that air sticks to the solid surface. How strange is that? . <!--more--><\/p>\n<p>\u00a0 This so called \u2018no-slip\u2019 condition is due to the adhesion of the fluid molecules to a solid surface. What about if the surface was a smooth as a mirror? Nope, it still sticks I\u2019m afraid. Air speed is zero at the surface but increases away from the wall to the free stream air speed. This region between the wall surface and the free stream air speed is called the \u2018boundary layer\u2019. It\u2019s the thermal resistance of the internal and external boundary layers that can comprises the main contribution to the overall resistance and thus, although you can\u2019t really do that much about it in terms of redesign (air will always stick) it\u2019s useful to understand its nature.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignleft size-full wp-image-34\" style=\"border: 5px solid white\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff-hvac\/files\/2010\/01\/simple_room.jpg\" alt=\"simple_room\" width=\"338\" height=\"278\" \/>Let\u2019s use <a href=\"http:\/\/www.mentor.com\/products\/mechanical\/products\/flovent\" >FloVENT <\/a>to setup a basic model of \u2019slice\u2019 of a room with hot radiator, walls and outside air. We\u2019ll go for a full complex 3D model later in this blog.\u00a0 FloVENT uses numerical techniques based on Computational Fluid Dynamics (CFD) to predict what the resulting air flow patterns and temperature distribution is. OK, this is a pretty \u2018lite\u2019 application of FloVENT, purely to demonstrate some HVAC theory. FloVENT\u2019s capable of a whole lot more from cleanroom compliance to datacenter full room cooling there\u2019s a whole bunch of stuff it can do.<\/p>\n<p><!--content--><\/p>\n<p>With an assumed temperature of 2degC otuside (spring in England <img src='http:\/\/blogs.mentor.com\/robinbornoff\/wp-includes\/images\/smilies\/icon_wink.gif' alt=';)' class='wp-smiley' \/> ) FloVENT predicts the room to be hotter, this is the least you\u2019d expect from a CFD tool in terms of predictive accuracy\u2026<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-36\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff-hvac\/files\/2010\/01\/simple_room_temp.jpg\" alt=\"simple_room_temp\" width=\"414\" height=\"258\" \/><\/p>\n<p>The air moves by natural convection, that it to say by buoyancy, there are no fans or air supply terminals. Hot air rises from the radiator, drops down the inside wall as it cools, its heat passes through the wall to the outside air that then picks up that heat and rises, again due to buoyancy.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-38\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff-hvac\/files\/2010\/01\/room_flow.gif\" alt=\"room_flow\" width=\"511\" height=\"495\" \/><\/p>\n<p>Looking at the air flow \u2018vectors\u2019 up close shows the decrease in speed as the wall is approached:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-40\" src=\"http:\/\/s3-blogs.mentor.com\/robinbornoff-hvac\/files\/2010\/01\/vectors_boundary_layer.jpg\" alt=\"vectors_boundary_layer\" width=\"460\" height=\"519\" \/><\/p>\n<p>For thermal insulation air can be your best friend and worst enemy. Static air is a really good thermal insulator with a thermal conductivity of ~ 0.026 W\/mK it\u2019s about twice as good as glass wool matting and about 20 times better than brickwork. As soon as air starts moving though (as it does even when it gets a little hotter than it\u2019s surroundings) it\u2019s really good at getting rid of heat, as good as any solid material is at conducting the heat away. The boundary layer is a devil you have to live with, with inescapable stagnant air right next to the wall you have to look elsewhere to improve the thermal insulation, to reduce the U-value. Such as inside the wall itself, more on that next time\u2026<\/p>\n<p>18th January 2010, Ross-on-Wye<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/feeds.feedburner.com\/~r\/mgc_mechanical\/~4\/SRUmJr6W1pQ\" height=\"1\" width=\"1\"\/><\/p>\n","protected":false},"excerpt":{"rendered":"<p>It might well be that a single U-value is quoted, in reality though that single value describes the ease by which heat can pass through various stages, from an \u2018inside\u2019, passing through a \u2018wall\/window\u2019 and going to the \u2018outside\u2019. The resistance (inverse of the ease, resistance = 1\/ease) the heat experiences as it passes from [&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-283656","post","type-post","status-publish","format-standard","hentry","category-news"],"_links":{"self":[{"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/posts\/283656","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=283656"}],"version-history":[{"count":0,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/posts\/283656\/revisions"}],"wp:attachment":[{"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/media?parent=283656"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/categories?post=283656"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/mereja.media\/index\/wp-json\/wp\/v2\/tags?post=283656"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}