{"id":606,"date":"2018-10-17T00:15:56","date_gmt":"2018-10-16T16:15:56","guid":{"rendered":"https:\/\/plasticmoldco.com\/?p=606"},"modified":"2018-10-17T00:15:56","modified_gmt":"2018-10-16T16:15:56","slug":"chapter-24-cooling-system-equations","status":"publish","type":"post","link":"https:\/\/www.plasticmoldco.com\/ja\/2018\/10\/17\/\u7b2c24\u7ae0-\u51b7\u5374\u30b7\u30b9\u30c6\u30e0\u306e\u65b9\u7a0b\u5f0f\/","title":{"rendered":"\u7b2c24\u7ae0 \u51b7\u5374\u30b7\u30b9\u30c6\u30e0\u306e\u65b9\u7a0b\u5f0f"},"content":{"rendered":"<div id=\"titlep\">\n<div><\/div>\n<\/div>\n<h1>\u51b7\u5374\u6642\u9593<\/h1>\n<p>\u7406\u8ad6\u7684\u306b\u306f\u3001\u51b7\u5374\u6642\u9593\u306f\u6700\u3082\u91cd\u3044\u90e8\u5206\u306e\u8089\u539a\u306e2\u4e57\u306b\u6bd4\u4f8b\u3059\u308b\u304b\u3001\u30e9\u30f3\u30ca\u30fc\u5f84\u304c\u6700\u5927\u306e\u5834\u5408\u306f1.6\u306e\u3079\u304d\u4e57\u306b\u6bd4\u4f8b\u3059\u308b\u3002\u3064\u307e\u308a<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-1288 alignnone\" title=\"\u51b7\u5374\u6642\u9593\" src=\"https:\/\/web.archive.org\/web\/20130131102810im_\/http:\/\/www.moldchina.org\/wp-content\/uploads\/2011\/10\/Cooling-time.gif\" alt=\"\u51b7\u5374\u6642\u9593\" width=\"477\" height=\"202\" \/><\/p>\n<p>\u3053\u3053\u3067\u3001\u30dd\u30ea\u30de\u30fc\u30e1\u30eb\u30c8\u306e\u71b1\u62e1\u6563\u7387\u306f\u6b21\u306e\u3088\u3046\u306b\u5b9a\u7fa9\u3055\u308c\u308b\u3002<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-1289 alignnone\" title=\"\u51b7\u5374\u6642\u9593-2\" src=\"https:\/\/web.archive.org\/web\/20130131102810im_\/http:\/\/www.moldchina.org\/wp-content\/uploads\/2011\/10\/Cooling-time-2.gif\" alt=\"\u51b7\u5374\u6642\u9593\" width=\"453\" height=\"86\" \/><\/p>\n<p>\u3064\u307e\u308a\u3001\u8089\u539a\u30922\u500d\u306b\u3059\u308b\u3068\u51b7\u5374\u6642\u9593\u306f4\u500d\u306b\u306a\u308b\u3002<\/p>\n<h1>\u30ec\u30a4\u30ce\u30eb\u30ba\u6570\u3068\u51b7\u5374\u6c34\u306e\u6d41\u308c<\/h1>\n<p>\u51b7\u5374\u6c34\u306e\u6d41\u308c\u304c\u4e71\u6d41\u3067\u3042\u308b\u304b\u3069\u3046\u304b\u306f\u3001\u88681\u306b\u793a\u3059\u30ec\u30a4\u30ce\u30eb\u30ba\u6570\uff08Re\uff09\u306b\u3088\u3063\u3066\u5224\u65ad\u3059\u308b\u3053\u3068\u304c\u3067\u304d\u308b\u3002\u30ec\u30a4\u30ce\u30eb\u30ba\u6570\u306f\u6b21\u306e\u3088\u3046\u306b\u5b9a\u7fa9\u3055\u308c\u308b\uff1a<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-1290 alignnone\" title=\"\u51b7\u5374\u6642\u9593-3\" src=\"https:\/\/web.archive.org\/web\/20130131102810im_\/http:\/\/www.moldchina.org\/wp-content\/uploads\/2011\/10\/Cooling-time-3.gif\" alt=\"\u51b7\u5374\u6642\u9593-3\" width=\"287\" height=\"79\" \/><\/p>\n<p>\u3069\u3053\u00a0<strong>\u03c1<\/strong>\u00a0\u306f\u51b7\u5374\u6c34\u306e\u5bc6\u5ea6\u3067\u3042\u308b\u3001\u00a0<strong>U<\/strong>\u00a0\u306f\u51b7\u5374\u6c34\u306e\u5e73\u5747\u901f\u5ea6\u3067\u3042\u308b\u3001\u00a0<strong>d<\/strong>\u00a0\u306f\u51b7\u5374\u6d41\u8def\u306e\u76f4\u5f84\u3001\u305d\u3057\u3066\u00a0\u00a0<strong>\u03b7<\/strong>\u00a0\u306f\u30af\u30fc\u30e9\u30f3\u30c8\u306e\u52d5\u7c98\u5ea6\u3067\u3042\u308b\u3002<\/p>\n<p>\u88681.\u30af\u30fc\u30e9\u30f3\u30c8\u30d5\u30ed\u30fc\u306e\u7a2e\u985e\u3068\u5bfe\u5fdc<br \/>\n\u30ec\u30a4\u30ce\u30eb\u30ba\u6570\u306e\u7bc4\u56f2<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-1291\" title=\"\u51b7\u5374\u6642\u9593-4\" src=\"https:\/\/web.archive.org\/web\/20130131102810im_\/http:\/\/www.moldchina.org\/wp-content\/uploads\/2011\/10\/Cooling-time-4.gif\" alt=\"\u51b7\u5374\u6642\u9593-4\" width=\"347\" height=\"182\" \/><\/p>","protected":false},"excerpt":{"rendered":"<p>Cooling time Theoretically, cooling time is proportional to the square of the heaviest part wall thickness or the power of 1.6 for the largest runner diameter. That is: where the thermal diffusivity of polymer melt is defined as In other words, doubling the wall thickness quadruples the cooling time. Reynolds number and coolant flow Whether or not the coolant flow is turbulent can be determined by the Reynolds number (Re), as listed in Table 1. The Reynolds number is defined as: where\u00a0\u03c1\u00a0is the density of the coolant,\u00a0U\u00a0is the averaged velocity of the coolant,\u00a0d\u00a0is the diameter of the cooling channel, and\u00a0\u00a0\u03b7\u00a0is the dynamic viscosity of the coolant. TABLE 1. Coolant flow [&hellip;]<\/p>","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_et_pb_use_builder":"","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"categories":[15],"tags":[],"class_list":["post-606","post","type-post","status-publish","format-standard","hentry","category-mould-technology-blog-1"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v26.4 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Chapter 24, Cooling system equations - Plastic Mold | China Mold Maker<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.plasticmoldco.com\/ja\/2018\/10\/17\/capitulo-24-ecuaciones-del-sistema-de-refrigeracion\/\" \/>\n<meta property=\"og:locale\" content=\"ja_JP\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Chapter 24, Cooling system equations - Plastic Mold | China Mold Maker\" \/>\n<meta property=\"og:description\" content=\"Cooling time Theoretically, cooling time is proportional to the square of the heaviest part wall thickness or the power of 1.6 for the largest runner diameter. 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