{"id":532,"date":"2021-12-01T15:55:31","date_gmt":"2021-12-01T14:55:31","guid":{"rendered":"http:\/\/measline.com\/\/?page_id=532"},"modified":"2022-04-13T08:42:42","modified_gmt":"2022-04-13T06:42:42","slug":"metodyka-pomiarow-optycznych","status":"publish","type":"page","link":"https:\/\/measline.com\/index.php\/pl\/measline\/605-2\/metodyka-pomiarow-optycznych\/","title":{"rendered":"Metodyka pomiar\u00f3w optycznych"},"content":{"rendered":"\n\n\n\n\n[et_pb_section fb_built=”1″ _builder_version=”4.14.2″ _module_preset=”default” hover_enabled=”0″ global_colors_info=”{}” sticky_enabled=”0″][et_pb_row column_structure=”1_2,1_2″ _builder_version=”4.14.1″ _module_preset=”default” global_colors_info=”{}”][et_pb_column type=”1_2″ _builder_version=”4.14.1″ _module_preset=”default” global_colors_info=”{}”][et_pb_text admin_label=”tytu\u0142” _builder_version=”4.14.2″ _module_preset=”default” custom_margin=”0px||0px||false|false” custom_padding=”0px||||false|false” hover_enabled=”0″ global_colors_info=”{}” sticky_enabled=”0″]

Metodyka pomiar\u00f3w optycznych<\/h2>[\/et_pb_text][et_pb_divider color=”#225600″ divider_weight=”2px” admin_label=”Separator” _builder_version=”4.14.1″ _module_preset=”default” global_colors_info=”{}”][\/et_pb_divider][et_pb_text admin_label=”Tekst” _builder_version=”4.14.2″ _module_preset=”default” custom_margin=”||-13px||false|false” hover_enabled=”0″ global_colors_info=”{}” sticky_enabled=”0″]

Typowymi parametrami optycznymi charakteryzuj\u0105cymi cia\u0142a sta\u0142e i ciecze s\u0105 odbicie, transmisja, absorpcja \u015bwiat\u0142a i fluoroscencja. Pomiary tych parametr\u00f3w wykonywane nastepuj\u0105ca metod\u0105:<\/p>\n

1. Wi\u0105zka \u015bwiat\u0142a o d\u0142ugo\u015bci fali z wybranego przedzia\u0142u widma, emitowana\u00a0ze \u017ar\u00f3d\u0142a \u015bwiat\u0142a jest doprowadzana \u015bwiat\u0142owodem do mierzonej pr\u00f3bki.<\/p>\n

2. W wyniku oddzia\u0142ywania z pr\u00f3bk\u0105 \u015bwiat\u0142o padaj\u0105ce ulega cz\u0119\u015bciowej absorpcji, interferencji i dyfrakcji.<\/p>\n

3. Nast\u0119pnie \u015bwiat\u0142o przesy\u0142ane jest do spektrometru \u015bwiat\u0142owodem, gdzie podlega pomiarowi a nast\u0119pnie analizie za pomoc\u0105 w\u0142a\u015bciwego algorytmu.<\/p>[\/et_pb_text][\/et_pb_column][et_pb_column type=”1_2″ _builder_version=”4.14.1″ _module_preset=”default” global_colors_info=”{}”][et_pb_divider show_divider=”off” _builder_version=”4.14.1″ _module_preset=”default” custom_margin=”21px||21px||true|false” global_colors_info=”{}”][\/et_pb_divider][et_pb_image src=”http:\/\/measline.com\/\/wp-content\/uploads\/2021\/12\/xpomiar20ogolny-1.jpg.pagespeed.ic_.MF-aslR0nG-1.jpg” title_text=”xpomiar20ogolny.jpg.pagespeed.ic.MF-aslR0nG” _builder_version=”4.14.2″ _module_preset=”default” hover_enabled=”0″ global_colors_info=”{}” sticky_enabled=”0″][\/et_pb_image][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=”4.14.1″ _module_preset=”default” custom_margin=”-1px||-1px||false|false” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.14.1″ _module_preset=”default” global_colors_info=”{}”][et_pb_text _builder_version=”4.14.2″ _module_preset=”default” custom_margin=”-25px||||false|false” hover_enabled=”0″ global_colors_info=”{}” sticky_enabled=”0″]

W zwi\u0105zku z nieliniowo\u015bci\u0105 intensywno\u015bci \u017ar\u00f3d\u0142a \u015bwiat\u0142a i szumem t\u0142a spektrometru w pomiarach konieczne s\u0105 dwa dodatkowe widma:<\/p>\n

a) referencyjne,<\/p>\n

b) ciemne<\/p>\n

Opieraj\u0105c si\u0119 na zebranych widmach oraz konfiguracji sprz\u0119tu pomiarowego mo\u017cliwe s\u0105 do wykonania nast\u0119puj\u0105ce pomiary absorpcji i transmisji.<\/p>\n

Widma absorpcyjne \/ transmisyjne pokazuj\u0105 oddzia\u0142ywanie \u015bwiat\u0142a z badan\u0105 pr\u00f3bk\u0105 w zale\u017cno\u015bci od d\u0142ugo\u015bci fali.\u00a0\u00a0Badana pr\u00f3bka mo\u017ce by\u0107 zar\u00f3wno w postaci ciek\u0142ej jak i cia\u0142a sta\u0142ego. Rysunek poni\u017cej pokazuje og\u00f3lny rysunek z uchwytem dla pr\u00f3bek ciek\u0142ych zamontowany w\u00a0 urz\u0105dzeniu z serii FR. Bardziej szczeg\u00f3\u0142owo opis pomiar\u00f3w znajduje si\u0119 instrukcji obs\u0142ugi urz\u0105dze\u0144 FR<\/a>.<\/p>[\/et_pb_text][et_pb_image src=”http:\/\/measline.com\/\/wp-content\/uploads\/2021\/12\/xpomiar20absorpcji.jpg.pagespeed.ic_.McGA6gsqVi.jpg” title_text=”xpomiar20absorpcji.jpg.pagespeed.ic.McGA6gsqVi” align=”center” _builder_version=”4.14.2″ _module_preset=”default” global_colors_info=”{}”][\/et_pb_image][et_pb_text _builder_version=”4.14.2″ _module_preset=”default” custom_padding=”0px||0px||true|false” global_colors_info=”{}”]

Wsp\u00f3\u0142czynnik poch\u0142aniania \u015bwiat\u0142a (absorbancja) dla okre\u015blonej d\u0142ugo\u015bci fali \u015bwietlnej\u00a0<\/span>\"A_\\lambda\" zdefiniowany jest nast\u0119puj\u0105co:<\/span><\/p>[\/et_pb_text][et_pb_image _builder_version=”4.14.2″ _module_preset=”default” hover_enabled=”0″ sticky_enabled=”0″ title_text=”row” src=”http:\/\/measline.com\/\/wp-content\/uploads\/2021\/12\/row.png” align=”center”][\/et_pb_image][et_pb_text _builder_version=”4.14.2″ _module_preset=”default” hover_enabled=”0″ sticky_enabled=”0″]

gdzie \"I_0\"\u00a0jest nat\u0119\u017ceniem \u015bwiat\u0142a przechodz\u0105cego przez pust\u0105 kuwet\u0119, a \"I_1\"\u00a0jest nat\u0119\u017ceniem \u015bwiat\u0142a przechodz\u0105cego przez kuwet\u0119 z badan\u0105 ciecz\u0105.<\/p>\n

Dla precyzyjnych bada\u0144 zar\u00f3wno od \"I_0\"\u00a0jak i od \"I_1\"\u00a0nale\u017cy odj\u0105\u0107 przyczynek pochodz\u0105cy od tzw.\u00a0pr\u0105du ciemnego \u00a0generuj\u0105cego si\u0119 w czujnikach \u015bwiat\u0142a w wyniku termicznej kreacji no\u015bnik\u00f3w pr\u0105du.<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section]\n\n\n\n\n","protected":false},"excerpt":{"rendered":"

Metodyka pomiar\u00f3w optycznychTypowymi parametrami optycznymi charakteryzuj\u0105cymi cia\u0142a sta\u0142e i ciecze s\u0105 odbicie, transmisja, absorpcja \u015bwiat\u0142a i fluoroscencja. Pomiary tych parametr\u00f3w wykonywane nastepuj\u0105ca metod\u0105: 1. Wi\u0105zka \u015bwiat\u0142a o d\u0142ugo\u015bci fali z wybranego przedzia\u0142u widma, emitowana\u00a0ze \u017ar\u00f3d\u0142a \u015bwiat\u0142a jest doprowadzana \u015bwiat\u0142owodem do mierzonej pr\u00f3bki. 2. W wyniku oddzia\u0142ywania z pr\u00f3bk\u0105 \u015bwiat\u0142o padaj\u0105ce ulega cz\u0119\u015bciowej absorpcji, interferencji i […]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":605,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"class_list":["post-532","page","type-page","status-publish","hentry"],"yoast_head":"\nMetodyka pomiar\u00f3w optycznych - Measline<\/title>\n<meta name=\"description\" content=\"Teoretyczny opis metodyki stosowanej do charakterystyki cia\u0142 sta\u0142ych i cieczy metodami optycznymi\" \/>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/measline.com\/index.php\/pl\/measline\/605-2\/metodyka-pomiarow-optycznych\/\" \/>\n<meta property=\"og:locale\" content=\"pl_PL\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Metodyka pomiar\u00f3w optycznych - 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