光谱学与光谱分析
光譜學與光譜分析
광보학여광보분석
SPECTROSCOPY AND SPECTRAL ANALYSIS
2015年
8期
2159-2163
,共5页
张凯华%于坤%张峰%刘玉芳
張凱華%于坤%張峰%劉玉芳
장개화%우곤%장봉%류옥방
铜%光谱发射率%温度%加热时间
銅%光譜髮射率%溫度%加熱時間
동%광보발사솔%온도%가열시간
Copper%Spectral emissivity%Temperature%Heating time
基于基尔霍夫定律,利用砷化镓(GaAs)半导体激光器作为标准光源研制了一种能够准确实时测量不透明物体光谱发射率的反射式测量装置。利用该装置在300~1123 K之间对黄铜和紫铜两种样品在波长1.55μm处的光谱发射率进行了系统的研究,探讨了温度、氧化、加热时间等因素对两种铜样品光谱发射率的影响。实验结果表明:黄铜和紫铜的光谱发射率均随温度的升高而增大,并且紫铜的光谱发射率始终大于黄铜的光谱发射率,两种样品随温度的光谱发射率曲线均出现了峰值和谷值。通过分析有氧化膜时金属表面的反射模型,得到了金属表面氧化膜厚度的计算公式,并利用该公式估算了紫铜发射率出现峰值和谷值时氧化膜的厚度。恒温长时间测量结果表明:光谱发射率随加热时间出现小幅增大,2 h后,由于样品表面氧化达到一定程度,氧化速率开始变缓,样品表面的光谱发射率也随之开始趋于稳定。样品在较高温度处的光谱发射率数值始终大于较低温度处的发射率数值。该研究进一步丰富了铜的光谱发射率数据,并为其光谱发射率的应用提供了实验依据。
基于基爾霍伕定律,利用砷化鎵(GaAs)半導體激光器作為標準光源研製瞭一種能夠準確實時測量不透明物體光譜髮射率的反射式測量裝置。利用該裝置在300~1123 K之間對黃銅和紫銅兩種樣品在波長1.55μm處的光譜髮射率進行瞭繫統的研究,探討瞭溫度、氧化、加熱時間等因素對兩種銅樣品光譜髮射率的影響。實驗結果錶明:黃銅和紫銅的光譜髮射率均隨溫度的升高而增大,併且紫銅的光譜髮射率始終大于黃銅的光譜髮射率,兩種樣品隨溫度的光譜髮射率麯線均齣現瞭峰值和穀值。通過分析有氧化膜時金屬錶麵的反射模型,得到瞭金屬錶麵氧化膜厚度的計算公式,併利用該公式估算瞭紫銅髮射率齣現峰值和穀值時氧化膜的厚度。恆溫長時間測量結果錶明:光譜髮射率隨加熱時間齣現小幅增大,2 h後,由于樣品錶麵氧化達到一定程度,氧化速率開始變緩,樣品錶麵的光譜髮射率也隨之開始趨于穩定。樣品在較高溫度處的光譜髮射率數值始終大于較低溫度處的髮射率數值。該研究進一步豐富瞭銅的光譜髮射率數據,併為其光譜髮射率的應用提供瞭實驗依據。
기우기이곽부정률,이용신화가(GaAs)반도체격광기작위표준광원연제료일충능구준학실시측량불투명물체광보발사솔적반사식측량장치。이용해장치재300~1123 K지간대황동화자동량충양품재파장1.55μm처적광보발사솔진행료계통적연구,탐토료온도、양화、가열시간등인소대량충동양품광보발사솔적영향。실험결과표명:황동화자동적광보발사솔균수온도적승고이증대,병차자동적광보발사솔시종대우황동적광보발사솔,량충양품수온도적광보발사솔곡선균출현료봉치화곡치。통과분석유양화막시금속표면적반사모형,득도료금속표면양화막후도적계산공식,병이용해공식고산료자동발사솔출현봉치화곡치시양화막적후도。항온장시간측량결과표명:광보발사솔수가열시간출현소폭증대,2 h후,유우양품표면양화체도일정정도,양화속솔개시변완,양품표면적광보발사솔야수지개시추우은정。양품재교고온도처적광보발사솔수치시종대우교저온도처적발사솔수치。해연구진일보봉부료동적광보발사솔수거,병위기광보발사솔적응용제공료실험의거。
In this study ,a new reflective experimental apparatus ,which can measure the spectral emissivity of opaque materials accurately and real timely ,has been developed based on the Kirchhoff’s law by using the GaAs semiconductor laser as the stand‐ard radiation source .The spectral emissivity of brass and red copper at wavelength λ=1.55 μm were investigated systematically with the temperatures range from 300 up to 1 123 K by using this apparatus and the influence of temperature ,oxidation and heating time on the spectral emissivity of two kinds of specimens were also discussed .The experimental data showed that the spectral emissivity increased with increase of temperature and appeared its peak value and valley value when the thickness of ox ‐ide film was at some degree .The spectral emissivity of red copper was always greater than that of brass .The formula for calcu‐lating the thickness of oxide film was derived from the reflection model composed of a metal and oxide film ,then the peak and valley thickness of the red copper were estimated according to this model .The experimental data of constant temperature meas‐urements showed that the spectral emissivity had a slight increase with heating time increasing .Two hours later ,the spectral emissivity of two kinds of samples trended to be stable when the thickness of oxide film was at some degree .The values of spec‐tral emissivity at high temperatures were always larger than that of low temperatures .The results of this study will further en‐rich spectral emissivity data of copper and provide experimental basis for its application .