Bu makalede k\u0131z\u0131l\u00f6tesi radyasyonun ne oldu\u011fu ve bu t\u00fcr elektromanyetik radyasyonun ne i\u00e7in kullan\u0131ld\u0131\u011f\u0131 a\u00e7\u0131klanmaktad\u0131r. <\/p>\n
K\u0131z\u0131l\u00f6tesi radyasyon<\/strong> , ayn\u0131 zamanda IR radyasyonu<\/strong> olarak da adland\u0131r\u0131l\u0131r, 0,7 ila 1000 \u03bcm aras\u0131nda bir dalga boyu ile karakterize edildi\u011finden insan g\u00f6z\u00fcyle g\u00f6r\u00fclemeyen bir t\u00fcr elektromanyetik radyasyondur.<\/p>\n K\u0131z\u0131l\u00f6tesi radyasyon, s\u0131cakl\u0131\u011f\u0131 mutlak s\u0131f\u0131r\u0131n (0 K) \u00fczerinde olan herhangi bir cisim taraf\u0131ndan \u00fcretilir. Sonu\u00e7 olarak, herhangi bir v\u00fccut veya g\u00fcnl\u00fck nesne k\u0131z\u0131l\u00f6tesi radyasyon yayar. Daha spesifik olarak k\u0131z\u0131l\u00f6tesi radyasyon, elektronlar\u0131n, atomlar\u0131n ve molek\u00fcllerin titre\u015fimlerinden gelir.<\/p>\n K\u0131z\u0131l\u00f6tesi radyasyon enerjiyi ve momentumu yayar ve ayn\u0131 zamanda yoluna \u00e7\u0131kan cisimleri \u0131s\u0131t\u0131r. Bu nedenle k\u0131z\u0131l\u00f6tesi radyasyon, \u00e7ok say\u0131da insan\u0131n bulundu\u011fu kapal\u0131 bir alan\u0131n daha s\u0131cak olmas\u0131n\u0131n nedenlerinden biridir.<\/p>\n K\u0131z\u0131l\u00f6tesi radyasyon, 19. y\u00fczy\u0131lda fizik\u00e7i William Herschel taraf\u0131ndan ke\u015ffedildi. <\/p>\n K\u0131z\u0131l\u00f6tesi radyasyonun dalga boyu<\/strong> 0,7 ila 1000 \u03bcm aras\u0131ndad\u0131r. Bu nedenle elektromanyetik spektrum aral\u0131\u011f\u0131 g\u00f6r\u00fcn\u00fcr \u0131\u015f\u0131k ile mikrodalgalar aras\u0131ndad\u0131r.<\/p>\n A\u015fa\u011f\u0131da elektromanyetik spektrumun farkl\u0131 bantlar\u0131n\u0131 kar\u015f\u0131la\u015ft\u0131ran bir tablo g\u00f6rebilirsiniz. <\/p>\n Benzer \u015fekilde k\u0131z\u0131l\u00f6tesi radyasyon i\u00e7inde, dalga boyunun de\u011ferine ba\u011fl\u0131 olarak \u00fc\u00e7 t\u00fcr k\u0131z\u0131l\u00f6tesi radyasyon vard\u0131r:<\/p>\n G\u00f6r\u00fcld\u00fc\u011f\u00fc gibi s\u0131cakl\u0131\u011f\u0131 olan t\u00fcm cisimler \u00e7evrelerine k\u0131z\u0131l\u00f6tesi \u0131\u015f\u0131n\u0131m yayarlar. Ancak bir v\u00fccut ayn\u0131 zamanda k\u0131z\u0131l\u00f6tesi radyasyonu da absorbe etme kapasitesine sahiptir. Yani bir v\u00fccut k\u0131z\u0131l\u00f6tesi radyasyonu emdi\u011finde \u0131s\u0131n\u0131r. Yani bir cisim k\u0131z\u0131l\u00f6tesi radyasyon yayd\u0131\u011f\u0131nda ve bu elektromanyetik dalgalar ba\u015fka bir cisim taraf\u0131ndan emildi\u011finde, birinci cisim ikinci cismi \u0131s\u0131t\u0131r.<\/p>\n \u00d6rne\u011fin G\u00fcne\u015f’in yayd\u0131\u011f\u0131 enerjinin yar\u0131dan fazlas\u0131 k\u0131z\u0131l\u00f6tesi \u0131\u015f\u0131n\u0131md\u0131r. G\u00fcne\u015f \u00f6zellikle g\u00f6r\u00fcn\u00fcr \u0131\u015f\u0131k, ultraviyole \u0131\u015f\u0131k ve k\u0131z\u0131l\u00f6tesi radyasyon yayar; en \u00e7ok yay\u0131lanlar ikincisidir.<\/p>\n K\u0131z\u0131l\u00f6tesi kameralar\u0131n, di\u011fer radyasyon t\u00fcrlerinin yan\u0131 s\u0131ra v\u00fccutlar\u0131n s\u0131cakl\u0131klar\u0131n\u0131 hesaplamak i\u00e7in yayd\u0131\u011f\u0131 k\u0131z\u0131l\u00f6tesi radyasyonu da kulland\u0131\u011f\u0131 unutulmamal\u0131d\u0131r. <\/p>\n Bu son b\u00f6l\u00fcmde k\u0131z\u0131l\u00f6tesi radyasyonun uygulamalar\u0131n\u0131n neler oldu\u011funu g\u00f6rece\u011fiz. Mant\u0131ksal olarak, bir\u00e7ok kullan\u0131m alan\u0131 oldu\u011fundan k\u0131z\u0131l\u00f6tesi radyasyonun t\u00fcm kullan\u0131mlar\u0131 sunulmam\u0131\u015ft\u0131r, ancak ana kullan\u0131m alanlar\u0131 sunulmu\u015ftur.<\/p>\n M\u00fchendislikte k\u0131z\u0131l\u00f6tesi kameralar, bir odan\u0131n veya t\u00fcm binan\u0131n farkl\u0131 s\u0131cakl\u0131klar\u0131n\u0131 analiz etmek i\u00e7in kullan\u0131l\u0131r. Bu, s\u0131z\u0131nt\u0131lar\u0131, enerji kay\u0131plar\u0131n\u0131, makinelerin a\u015f\u0131r\u0131 \u0131s\u0131nmas\u0131n\u0131 vb. tespit etmeyi m\u00fcmk\u00fcn k\u0131lar. Ek olarak k\u0131z\u0131l\u00f6tesi kameralar, bir nesnenin s\u0131cakl\u0131\u011f\u0131n\u0131 fiziksel temas kurmaya gerek kalmadan belirleyebilme avantaj\u0131na sahiptir.<\/p>\n End\u00fcstriyel sekt\u00f6rde k\u0131z\u0131l\u00f6tesi radyasyonun bir\u00e7ok uygulamas\u0131 vard\u0131r. Baz\u0131 boyalar\u0131n kurutulmas\u0131, cam\u0131n laminasyonu veya baz\u0131 imalat s\u00fcre\u00e7leri gibi i\u015flemler bu t\u00fcr radyasyondan yararlan\u0131r.<\/p>\n G\u00fcnl\u00fck ya\u015famda k\u0131z\u0131l\u00f6tesi radyasyon kullanan nesneler olduk\u00e7a yayg\u0131nd\u0131r. \u00d6rne\u011fin k\u0131z\u0131l\u00f6tesi lazer bu tip elektromanyetik dalgay\u0131 kullan\u0131r. Benzer \u015fekilde, uzaktan kumandalar da TV’ye sinyal g\u00f6ndermek i\u00e7in genellikle k\u0131z\u0131l\u00f6tesini kullan\u0131r.<\/p>\n K\u0131z\u0131l\u00f6tesi radyasyon kavram\u0131 askeri veya g\u00fcvenlik g\u00f6revlerinde de kullan\u0131l\u0131r. Gece g\u00f6r\u00fc\u015f ekipman\u0131, insan g\u00f6z\u00fcn\u00fcn g\u00f6r\u00fcn\u00fcr \u0131\u015f\u0131\u011f\u0131 alg\u0131layamad\u0131\u011f\u0131 durumlarda g\u00f6r\u00fcn\u00fcrl\u00fc\u011f\u00fc art\u0131rmak i\u00e7in k\u0131z\u0131l\u00f6tesi kullan\u0131r.<\/p>\n Son olarak, k\u0131z\u0131l\u00f6tesi radyasyonun ba\u015fka bir uygulamas\u0131 fizik tedavidir, \u00e7\u00fcnk\u00fc baz\u0131 rehabilitasyon s\u00fcre\u00e7leri iyile\u015fmeyi h\u0131zland\u0131rmak i\u00e7in bu t\u00fcr dalgalar\u0131 i\u00e7erir.<\/p>\n","protected":false},"excerpt":{"rendered":" Bu makalede k\u0131z\u0131l\u00f6tesi radyasyonun ne oldu\u011fu ve bu t\u00fcr elektromanyetik radyasyonun ne i\u00e7in kullan\u0131ld\u0131\u011f\u0131 a\u00e7\u0131klanmaktad\u0131r. K\u0131z\u0131l\u00f6tesi radyasyon nedir? K\u0131z\u0131l\u00f6tesi radyasyon , ayn\u0131 zamanda IR radyasyonu olarak da adland\u0131r\u0131l\u0131r, 0,7 ila 1000 \u03bcm aras\u0131nda bir dalga boyu ile karakterize edildi\u011finden insan g\u00f6z\u00fcyle g\u00f6r\u00fclemeyen bir t\u00fcr elektromanyetik radyasyondur. K\u0131z\u0131l\u00f6tesi radyasyon, s\u0131cakl\u0131\u011f\u0131 mutlak s\u0131f\u0131r\u0131n (0 K) \u00fczerinde olan …<\/p>\n<\/span> K\u0131z\u0131l\u00f6tesi radyasyonun dalga boyu<\/span><\/h2>\n
\n\n
\n \n isim<\/th>\n Dalga boyu<\/th>\n S\u0131kl\u0131k<\/th>\n<\/tr>\n<\/thead>\n \n Gama \u0131\u015f\u0131nlar\u0131<\/td>\n <0,01nm<\/td>\n > 30Hz<\/td>\n<\/tr>\n \n X \u0131\u015f\u0131nlar\u0131<\/td>\n 0,01nm \u2013 10nm<\/td>\n 30Hz \u2013 30PH<\/td>\n<\/tr>\n \n Ultraviyole<\/td>\n 10 nm \u2013 400 nm<\/td>\n 30PHZ \u2013 790THZ<\/td>\n<\/tr>\n \n g\u00f6r\u00fclebilir \u0131\u015f\u0131k<\/td>\n 400 nm \u2013 700 nm<\/td>\n 790THZ \u2013 430THZ<\/td>\n<\/tr>\n \n k\u0131z\u0131l\u00f6tesi<\/td>\n 700 nm \u2013 1 mm<\/td>\n 430 THz \u2013 300 GHz<\/td>\n<\/tr>\n \n Mikrodalga<\/td>\n 1mm \u2013 1m<\/td>\n 300GHz \u2013 300MHz<\/td>\n<\/tr>\n \n Radyo<\/td>\n 1m \u2013 10000km<\/td>\n 300MHz \u2013 30Hz<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/figure>\n \n
<\/span> Do\u011fal k\u0131z\u0131l\u00f6tesi radyasyon<\/span><\/h2>\n
<\/span> K\u0131z\u0131l\u00f6tesi radyasyonun uygulamalar\u0131<\/span><\/h2>\n