{"title":"中高压汞灯的原子温度和激发温度","authors":"E. Drakakis, Dimitrios Karabourniotis, G. Zissis","doi":"10.2150/JLVE.IEIJ130000514","DOIUrl":null,"url":null,"abstract":"Atomic and excitation temperatures were determined in medium-pressure (0.14 atm) mercury lamp working on square-wave current from radiance measurements of the red wing of the resonance mercury line 254 nm. The results were compared with these obtained using time resolved measurements at the maximum- and minimum current phase in a high-pressure (6 atm) mercury lamp operating with typical conventional electromagnetic ballast, and show that strong nonequilibrium phenomena occur in particular in the medium-pressure lamp. The excitation temperature was determined from the peak radiance using a non-LTE version of the Bartels method. The atomic temperature as well as the plasma pressure was then deduced from a non-LTE simulation of the line shape.","PeriodicalId":311488,"journal":{"name":"Journal of Light & Visual Environment","volume":"115 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2013-03-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Atomic and Excitation Temperatures in Medium- and High-pressure Mercury Arc Lamps\",\"authors\":\"E. Drakakis, Dimitrios Karabourniotis, G. Zissis\",\"doi\":\"10.2150/JLVE.IEIJ130000514\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Atomic and excitation temperatures were determined in medium-pressure (0.14 atm) mercury lamp working on square-wave current from radiance measurements of the red wing of the resonance mercury line 254 nm. The results were compared with these obtained using time resolved measurements at the maximum- and minimum current phase in a high-pressure (6 atm) mercury lamp operating with typical conventional electromagnetic ballast, and show that strong nonequilibrium phenomena occur in particular in the medium-pressure lamp. The excitation temperature was determined from the peak radiance using a non-LTE version of the Bartels method. The atomic temperature as well as the plasma pressure was then deduced from a non-LTE simulation of the line shape.\",\"PeriodicalId\":311488,\"journal\":{\"name\":\"Journal of Light & Visual Environment\",\"volume\":\"115 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2013-03-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Light & Visual Environment\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.2150/JLVE.IEIJ130000514\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Light & Visual Environment","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2150/JLVE.IEIJ130000514","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Atomic and Excitation Temperatures in Medium- and High-pressure Mercury Arc Lamps
Atomic and excitation temperatures were determined in medium-pressure (0.14 atm) mercury lamp working on square-wave current from radiance measurements of the red wing of the resonance mercury line 254 nm. The results were compared with these obtained using time resolved measurements at the maximum- and minimum current phase in a high-pressure (6 atm) mercury lamp operating with typical conventional electromagnetic ballast, and show that strong nonequilibrium phenomena occur in particular in the medium-pressure lamp. The excitation temperature was determined from the peak radiance using a non-LTE version of the Bartels method. The atomic temperature as well as the plasma pressure was then deduced from a non-LTE simulation of the line shape.