I\u015f\u0131\u011f\u0131n polarizasyonu, polarize olmayan \u0131\u015f\u0131\u011f\u0131n polarize \u0131\u015f\u0131\u011fa d\u00f6n\u00fc\u015ft\u00fc\u011f\u00fc s\u00fcre\u00e7tir.<\/strong> Basit\u00e7e s\u00f6ylemek gerekirse, \u0131\u015f\u0131k polarizasyonu, farkl\u0131 y\u00f6nlerde sal\u0131nan bir \u0131\u015f\u0131k \u0131\u015f\u0131n\u0131n\u0131n tek bir d\u00fczlemde sal\u0131nan bir \u0131\u015f\u0131k \u0131\u015f\u0131n\u0131na d\u00f6n\u00fc\u015ft\u00fcr\u00fclmesini i\u00e7erir.<\/p>\n Bu nedenle polarize edici \u0131\u015f\u0131k, yay\u0131lma y\u00f6n\u00fcn\u00fc s\u0131n\u0131rlayarak onu y\u00f6nlendirmek anlam\u0131na gelir. Yani polarize \u0131\u015f\u0131\u011f\u0131n sal\u0131nd\u0131\u011f\u0131 y\u00f6ne polarizasyon y\u00f6n\u00fc denir. <\/p>\n Polarize olmayan \u0131\u015f\u0131k, bir elektrik alan\u0131 ve farkl\u0131 y\u00f6nlerde sal\u0131nan bir manyetik alandan olu\u015fur; b\u00f6ylece iki alan birbirine ve dalgan\u0131n yay\u0131lma y\u00f6n\u00fcne dik olur. B\u00f6ylece \u0131\u015f\u0131k polarize oldu\u011funda yaln\u0131zca tek y\u00f6nde sal\u0131nan bir elektromanyetik dalga elde ederiz.<\/p>\n I\u015f\u0131\u011f\u0131n veya herhangi bir elektromanyetik dalgan\u0131n \u00fc\u00e7 t\u00fcr polarizasyonu vard\u0131r:<\/p>\n Bu b\u00f6l\u00fcmde polarize \u0131\u015f\u0131k elde etmek i\u00e7in en yayg\u0131n prosed\u00fcrler a\u00e7\u0131klanmaktad\u0131r. T\u00fcm polarizasyon i\u015flemlerinin ayn\u0131 \u00e7al\u0131\u015fma prensibine dayand\u0131\u011f\u0131n\u0131 unutmay\u0131n: elektrik alan\u0131, polarizasyon d\u00fczlemi ad\u0131 verilen tek bir d\u00fczlemde titre\u015fmeye zorlan\u0131r. <\/p>\n Bu polarizasyon i\u015flemi, belirli malzemelerin bir elektromanyetik dalgan\u0131n elektrik alan\u0131n\u0131n bile\u015fenlerinden birini absorbe edebilmesi ger\u00e7e\u011finden yararlan\u0131r. Bu fiziksel \u00f6zelli\u011fe dikroizm denir.<\/p>\n Elektrik alan\u0131n\u0131n bile\u015fenlerinden birinin emilmesiyle yay\u0131lma y\u00f6n\u00fc de\u011fi\u015ftirilir ve sonu\u00e7 olarak \u0131\u015f\u0131k polarize olur.<\/p>\n \u00d6rne\u011fin turmalin gibi baz\u0131 kristaller bu polarizasyon \u00f6zelliklerine sahiptir. <\/p>\n I\u015f\u0131k bir y\u00fczeyden yans\u0131d\u0131\u011f\u0131nda polarize olabilir. B\u00f6ylece, yans\u0131yan \u0131\u015f\u0131k, elektrik alan\u0131n\u0131n geli\u015f d\u00fczlemine do\u011fru olan bile\u015feni yans\u0131t\u0131lmad\u0131\u011f\u0131 i\u00e7in k\u0131smi polarizasyona u\u011frar, dolay\u0131s\u0131yla bu bile\u015fen ortadan kald\u0131r\u0131l\u0131r.<\/p>\n Bu olay, yans\u0131yan \u0131\u015f\u0131k \u0131\u015f\u0131n\u0131 k\u0131r\u0131lan \u0131\u015f\u0131k \u0131\u015f\u0131n\u0131na (y\u00fczeyden ge\u00e7en) dik oldu\u011funda meydana gelir. <\/p>\n \u00c7ift k\u0131r\u0131lma polarizasyonu olarak da adland\u0131r\u0131lan \u00e7ift k\u0131r\u0131lma polarizasyonu, belirli cisimlerin \u00e7ok \u00f6zel bir optik \u00f6zelli\u011fi sayesinde meydana gelir. Bu \u00f6zellik, gelen \u0131\u015f\u0131k \u0131\u015f\u0131n\u0131n\u0131 birbirine dik iki do\u011frusal polarize \u0131\u015f\u0131na b\u00f6lmekten olu\u015fur.<\/p>\n Polariz\u00f6r<\/strong> , \u0131\u015f\u0131\u011f\u0131 polarize eden optik bir ara\u00e7t\u0131r. Basit\u00e7e s\u00f6ylemek gerekirse, polariz\u00f6r, polarize olmayan do\u011fal \u0131\u015f\u0131\u011f\u0131 polarize \u0131\u015f\u0131\u011fa d\u00f6n\u00fc\u015ft\u00fcren bir cihazd\u0131r.<\/p>\n I\u015f\u0131\u011f\u0131 polarize etmek i\u00e7in polariz\u00f6rler genellikle yukar\u0131daki b\u00f6l\u00fcmde a\u00e7\u0131klanan polarizasyon s\u00fcre\u00e7lerinden baz\u0131lar\u0131n\u0131 kullan\u0131r.<\/p>\n Fizikte, \u00e7ok daha geli\u015fmi\u015f optik aletlerin mekanizmalar\u0131 genellikle bir polariz\u00f6r i\u00e7erir, b\u00f6ylece aletin i\u00e7indeki \u0131\u015f\u0131k onu i\u015fleyebilmek i\u00e7in polarize edilir. \u00d6rne\u011fin bir polarimetre bir polariz\u00f6r i\u00e7erir. <\/p>\n Son olarak \u0131\u015f\u0131\u011f\u0131n polarizasyonunun ne i\u015fe yarad\u0131\u011f\u0131n\u0131 g\u00f6rece\u011fiz, \u00e7\u00fcnk\u00fc polarize \u0131\u015f\u0131k elde etme i\u015flemleri bu kadar karma\u015f\u0131ksa, bu t\u00fcr \u0131\u015f\u0131\u011f\u0131n bir\u00e7ok kullan\u0131m alan\u0131 olmas\u0131 gerekir.<\/p>\n I\u015f\u0131\u011f\u0131n polarizasyonunun bir\u00e7ok uygulamas\u0131 vard\u0131r. \u00d6rne\u011fin, muhtemelen zaten polarize g\u00fcne\u015f g\u00f6zl\u00fc\u011f\u00fc kullanm\u0131\u015fs\u0131n\u0131zd\u0131r; gelen \u0131\u015f\u0131\u011f\u0131 polarize ederek kullan\u0131c\u0131n\u0131n daha iyi g\u00f6rmesini sa\u011flar.<\/p>\n Benzer \u015fekilde, \u0131\u015f\u0131\u011f\u0131n polarizasyonu da foto\u011fraf\u00e7\u0131l\u0131kta faydal\u0131d\u0131r \u00e7\u00fcnk\u00fc bu fiziksel s\u00fcre\u00e7 foto\u011fraf\u0131n kontrast\u0131n\u0131 artt\u0131rmak i\u00e7in kullan\u0131l\u0131r.<\/p>\n Ayr\u0131ca polarize \u0131\u015f\u0131k biz fark\u0131nda olmasak da g\u00fcnl\u00fck ya\u015famda fazlas\u0131yla mevcuttur. B\u00f6ylece radyolar\u0131n bilgi iletmek i\u00e7in kulland\u0131\u011f\u0131 elektromanyetik dalgalar polarize olur.<\/p>\n Bununla birlikte, \u0131\u015f\u0131\u011f\u0131n polarizasyonunun ba\u015fka bir\u00e7ok bilimsel kullan\u0131m\u0131 da vard\u0131r; \u00f6rne\u011fin astronomide, bu disipline \u00f6zg\u00fc olaylar\u0131 incelemek i\u00e7in polarize \u0131\u015f\u0131k kullan\u0131l\u0131r.<\/p>\n","protected":false},"excerpt":{"rendered":" Bu makale fizikte \u0131\u015f\u0131\u011f\u0131n polarizasyonunun ne oldu\u011funu a\u00e7\u0131kl\u0131yor. B\u00f6ylece polarize \u0131\u015f\u0131\u011f\u0131n ne oldu\u011funu, farkl\u0131 \u0131\u015f\u0131k polarizasyon t\u00fcrlerini ve \u0131\u015f\u0131\u011f\u0131n nas\u0131l polarize edilece\u011fini ke\u015ffedeceksiniz. I\u015f\u0131\u011f\u0131n polarizasyonu nedir? I\u015f\u0131\u011f\u0131n polarizasyonu, polarize olmayan \u0131\u015f\u0131\u011f\u0131n polarize \u0131\u015f\u0131\u011fa d\u00f6n\u00fc\u015ft\u00fc\u011f\u00fc s\u00fcre\u00e7tir. Basit\u00e7e s\u00f6ylemek gerekirse, \u0131\u015f\u0131k polarizasyonu, farkl\u0131 y\u00f6nlerde sal\u0131nan bir \u0131\u015f\u0131k \u0131\u015f\u0131n\u0131n\u0131n tek bir d\u00fczlemde sal\u0131nan bir \u0131\u015f\u0131k \u0131\u015f\u0131n\u0131na d\u00f6n\u00fc\u015ft\u00fcr\u00fclmesini i\u00e7erir. …<\/p>\n![\"\u0131\u015f\u0131\u011f\u0131n](\"https:\/\/physigeek.com\/wp-content\/uploads\/2023\/09\/polarisation-de-la-lumiere.png\")
<\/figure>\n<\/span> Polarizasyon t\u00fcrleri<\/span><\/h2>\n
\n
![\"\u0131\u015f\u0131k](\"https:\/\/physigeek.com\/wp-content\/uploads\/2023\/09\/types-de-polarisation-de-la-lumiere.png\")
<\/figure>\n<\/span> I\u015f\u0131k polarizasyon s\u00fcreci<\/span><\/h2>\n
<\/span> Se\u00e7ici absorpsiyonla polarizasyon<\/span><\/h3>\n
<\/span> Yans\u0131ma polarizasyonu<\/span><\/h3>\n
<\/span> \u00c7ift k\u0131r\u0131lma polarizasyonu<\/span><\/h3>\n
<\/span> Polarizasyon<\/span><\/h2>\n
<\/span> I\u015f\u0131k polarizasyonunun uygulamalar\u0131<\/span><\/h2>\n