{"id":600,"date":"2018-10-17T00:14:39","date_gmt":"2018-10-16T16:14:39","guid":{"rendered":"https:\/\/plasticmoldco.com\/?p=600"},"modified":"2018-10-17T00:14:39","modified_gmt":"2018-10-16T16:14:39","slug":"chapter-25-2-residual-stress-china-injection-mold","status":"publish","type":"post","link":"https:\/\/www.plasticmoldco.com\/cs\/2018\/10\/17\/kapitola-25-2-zbytkove-napeti-porcelanove-vstrikovaci-formy\/","title":{"rendered":"Kapitola 25-2, Zbytkov\u00e9 nap\u011bt\u00ed, vst\u0159ikovac\u00ed forma z porcel\u00e1nu"},"content":{"rendered":"

Nevyv\u00e1\u017een\u00e9 chlazen\u00ed<\/h1>\n

od st\u011bny formy do jej\u00edho st\u0159edu m\u016f\u017ee zp\u016fsobit tepeln\u011b indukovan\u00e9 zbytkov\u00e9 nap\u011bt\u00ed. Krom\u011b toho m\u016f\u017ee doj\u00edt k asymetrick\u00e9mu tepeln\u011b indukovan\u00e9mu zbytkov\u00e9mu nap\u011bt\u00ed, pokud je rychlost ochlazov\u00e1n\u00ed obou povrch\u016f nevyv\u00e1\u017een\u00e1. Takov\u00e9 nevyv\u00e1\u017een\u00e9 ochlazov\u00e1n\u00ed m\u00e1 za n\u00e1sledek asymetrick\u00fd pr\u016fb\u011bh tahu a tlaku nap\u0159\u00ed\u010d d\u00edlem, co\u017e zp\u016fsobuje ohybov\u00fd moment, kter\u00fd m\u00e1 tendenci zp\u016fsobovat deformace d\u00edlu. To je zn\u00e1zorn\u011bno na obr\u00e1zku 3 n\u00ed\u017ee. V d\u016fsledku toho jsou d\u00edly s nerovnom\u011brnou tlou\u0161\u0165kou nebo \u0161patn\u011b chlazen\u00e9 oblasti n\u00e1chyln\u00e9 k nevyv\u00e1\u017een\u00e9mu chlazen\u00ed, a t\u00edm i ke zbytkov\u00fdm tepeln\u00fdm nap\u011bt\u00edm. U st\u0159edn\u011b slo\u017eit\u00fdch d\u00edl\u016f je rozlo\u017een\u00ed zbytkov\u00fdch nap\u011bt\u00ed zp\u016fsoben\u00fdch teplem d\u00e1le komplikov\u00e1no nestejnou tlou\u0161\u0165kou st\u011bn, chlazen\u00edm formy a omezen\u00edm formy v\u016f\u010di voln\u00e9mu smr\u0161\u0165ov\u00e1n\u00ed.<\/p>\n

\"\"<\/p>\n

OBR\u00c1ZEK 3. Asymetrick\u00e9 tepeln\u011b indukovan\u00e9 zbytkov\u00e9 nap\u011bt\u00ed zp\u016fsoben\u00e9 nevyv\u00e1\u017een\u00fdm chlazen\u00edm nap\u0159\u00ed\u010d tlou\u0161\u0165kou v\u00fdlisku zp\u016fsobuje deformace v\u00fdlisku.<\/h3>\n

Prom\u011bnliv\u00e1 hustota zmrazen\u00ed<\/h2>\n

N\u00e1sleduj\u00edc\u00ed obr\u00e1zek zn\u00e1zor\u0148uje zm\u011bny hustoty zmrazen\u00e9ho materi\u00e1lu zp\u016fsoben\u00e9 pr\u016fb\u011bhem tlaku v obalu.<\/p>\n

Teplotn\u00ed profil<\/h3>\n

Na lev\u00e9m obr\u00e1zku je vykreslen teplotn\u00ed profil v jednom m\u00edst\u011b na d\u00edlu. Pro \u00fa\u010dely ilustrace je d\u00edl rozd\u011blen na osm stejn\u00fdch vrstev po cel\u00e9 tlou\u0161\u0165ce d\u00edlu. Profil ukazuje teplotu v okam\u017eiku tuhnut\u00ed (zamrznut\u00ed) pro ka\u017edou vrstvu (t1 a\u017e t8). V\u0161imn\u011bte si, \u017ee materi\u00e1l za\u010d\u00edn\u00e1 tuhnout od vn\u011bj\u0161\u00edch vrstev a zamrzl\u00e9 rozhran\u00ed se s \u010dasem posouv\u00e1 dovnit\u0159.<\/p>\n

Tlakov\u00e1 stopa<\/h3>\n

Na prost\u0159edn\u00edm obr\u00e1zku je zn\u00e1zorn\u011bn typick\u00fd pr\u016fb\u011bh tlaku, kter\u00fd ukazuje \u00farovn\u011b tlaku (P1 a\u017e P8) p\u0159i tuhnut\u00ed jednotliv\u00fdch vrstev. Obecn\u011b lze \u0159\u00edci, \u017ee tlak b\u011bhem pln\u011bn\u00ed postupn\u011b roste a dosahuje maxima v po\u010d\u00e1te\u010dn\u00ed f\u00e1zi balen\u00ed, pot\u00e9 za\u010dne klesat v d\u016fsledku ochlazov\u00e1n\u00ed a zamrz\u00e1n\u00ed hradla. V souladu s t\u00edm materi\u00e1l ve vn\u011bj\u0161\u00edch a st\u0159edn\u00edch vrstv\u00e1ch tuhne p\u0159i n\u00edzk\u00e9 \u00farovni tlaku, zat\u00edmco st\u0159edn\u00ed vrstvy tuhnou p\u0159i vysok\u00e9m tlaku p\u0159i pln\u011bn\u00ed.<\/p>\n

Specifick\u00fd objem zmrazen\u00e9ho materi\u00e1lu<\/h3>\n

Na prav\u00e9m obr\u00e1zku je zn\u00e1zorn\u011bna stopa specifick\u00e9ho objemu pro vrstvu 5 na grafu pvT a kone\u010dn\u00e9 specifick\u00e9 objemy zmrazen\u00e9 ve v\u0161ech vrstv\u00e1ch, ozna\u010den\u00e9 o\u010d\u00edslovan\u00fdmi pln\u00fdmi kruhy.<\/p>\n

\"\"<\/p>\n

OBR\u00c1ZEK 4. Faktory, kter\u00e9 ovliv\u0148uj\u00ed v\u00fdvoj specifick\u00e9ho objemu \"zamrzl\u00e9ho v\"
\nDiferenci\u00e1ln\u00ed smr\u0161\u0165ov\u00e1n\u00ed<\/h3>\n

Vzhledem k m\u011brn\u00fdm objem\u016fm zmrazen\u00fdch materi\u00e1l\u016f se jednotliv\u00e9 vrstvy smr\u0161\u0165uj\u00ed r\u016fzn\u011b, a to podle k\u0159ivek pvT, kter\u00fdmi se \u0159\u00edd\u00ed chov\u00e1n\u00ed materi\u00e1lu p\u0159i smr\u0161\u0165ov\u00e1n\u00ed. Hypoteticky, pokud by se jednotliv\u00e9 vrstvy odd\u011blily od ostatn\u00edch (jak je zn\u00e1zorn\u011bno na obr\u00e1zku 5), pak by se materi\u00e1lov\u00e9 prvky na lev\u00e9m obr\u00e1zku n\u00ed\u017ee smr\u0161tily stejn\u011b jako prvky na prost\u0159edn\u00edm obr\u00e1zku. V tomto p\u0159\u00edpad\u011b maj\u00ed mezivrstvy tendenci smr\u0161\u0165ovat se m\u00e9n\u011b ne\u017e ostatn\u00ed, proto\u017ee maj\u00ed ni\u017e\u0161\u00ed m\u011brn\u00fd objem po zamrznut\u00ed (nebo ekvivalentn\u011b vy\u0161\u0161\u00ed hustotu po zamrznut\u00ed). Ve skute\u010dnosti jsou v\u0161echny vrstvy v\u00e1z\u00e1ny dohromady. Proto bude kone\u010dn\u00fdm v\u00fdsledkem kompromisn\u00ed rozlo\u017een\u00ed smr\u0161t\u011bn\u00ed, p\u0159i kter\u00e9m budou mezivrstvy stla\u010deny a vn\u011bj\u0161\u00ed a st\u0159edn\u00ed vrstvy rozta\u017eeny.<\/p>","protected":false},"excerpt":{"rendered":"

Nerovnom\u011brn\u00e9 chlazen\u00ed od st\u011bny formy sm\u011brem do jej\u00edho st\u0159edu m\u016f\u017ee zp\u016fsobit tepeln\u011b indukovan\u00e9 zbytkov\u00e9 nap\u011bt\u00ed. Nav\u00edc m\u016f\u017ee doj\u00edt k asymetrick\u00e9mu tepeln\u011b indukovan\u00e9mu zbytkov\u00e9mu nap\u011bt\u00ed, pokud je rychlost ochlazov\u00e1n\u00ed obou povrch\u016f nevyv\u00e1\u017een\u00e1. Takov\u00e9 nevyv\u00e1\u017een\u00e9 ochlazov\u00e1n\u00ed m\u00e1 za n\u00e1sledek asymetrick\u00fd pr\u016fb\u011bh tahu a tlaku nap\u0159\u00ed\u010d d\u00edlem, co\u017e zp\u016fsobuje ohybov\u00fd moment, kter\u00fd m\u00e1 tendenci zp\u016fsobovat deformace d\u00edlu. To [...]<\/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-600","post","type-post","status-publish","format-standard","hentry","category-mould-technology-blog-1"],"yoast_head":"\nChapter 25-2, Residual stress, china injection mold - 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\/cs\/2018\/10\/17\/25-2-fejezet-marado-feszultseg-porcelan-froccsontoforma\/\" \/>\n<meta property=\"og:locale\" content=\"cs_CZ\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Chapter 25-2, Residual stress, china injection mold - Plastic Mold | China Mold Maker\" \/>\n<meta property=\"og:description\" content=\"Unbalanced cooling from the mold wall to its center can cause thermal-induced residual stress. 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