红外与激光工程
紅外與激光工程
홍외여격광공정
INFRARED AND LASER ENGINEERING
2014年
3期
956-960
,共5页
潘虎%王广宇%宋俊玲%于小红
潘虎%王廣宇%宋俊玲%于小紅
반호%왕엄우%송준령%우소홍
激光吸收光谱%波长调制%谐波检测%燃烧场诊断
激光吸收光譜%波長調製%諧波檢測%燃燒場診斷
격광흡수광보%파장조제%해파검측%연소장진단
laser absorption spectroscopy%wavelength-modulation%harmonic detection%combustion field diagnosis
可调谐二极管激光吸收光谱在诸多领域有广泛的应用,但因为基线获取的困难,在高压、强干扰条件下的测量存在困难。波长调制光谱的理论显示,一次谐波信号(1f)和二次谐波信号(2f)包含了初始光强和光电探测器增益两个公共项。通过一次谐波信号归一化的二次谐波(2f/1f)信号,消除了信号强度与光强的相关性,可得到吸收光谱的绝对强度及温度等信息。通过测量激光调制参数,结合已知光谱参数可通过数值仿真得到理论的2f/1f信号。利用数值锁相算法,可以实现频分复用的免标定波长调制光谱测量,实验显示,当恒温池设定温度为600 K、700 K和800 K时,光谱测量温度与热电偶测量值偏差小于2%,该方法具有可靠性和更强适应性。
可調諧二極管激光吸收光譜在諸多領域有廣汎的應用,但因為基線穫取的睏難,在高壓、彊榦擾條件下的測量存在睏難。波長調製光譜的理論顯示,一次諧波信號(1f)和二次諧波信號(2f)包含瞭初始光彊和光電探測器增益兩箇公共項。通過一次諧波信號歸一化的二次諧波(2f/1f)信號,消除瞭信號彊度與光彊的相關性,可得到吸收光譜的絕對彊度及溫度等信息。通過測量激光調製參數,結閤已知光譜參數可通過數值倣真得到理論的2f/1f信號。利用數值鎖相算法,可以實現頻分複用的免標定波長調製光譜測量,實驗顯示,噹恆溫池設定溫度為600 K、700 K和800 K時,光譜測量溫度與熱電偶測量值偏差小于2%,該方法具有可靠性和更彊適應性。
가조해이겁관격광흡수광보재제다영역유엄범적응용,단인위기선획취적곤난,재고압、강간우조건하적측량존재곤난。파장조제광보적이론현시,일차해파신호(1f)화이차해파신호(2f)포함료초시광강화광전탐측기증익량개공공항。통과일차해파신호귀일화적이차해파(2f/1f)신호,소제료신호강도여광강적상관성,가득도흡수광보적절대강도급온도등신식。통과측량격광조제삼수,결합이지광보삼수가통과수치방진득도이론적2f/1f신호。이용수치쇄상산법,가이실현빈분복용적면표정파장조제광보측량,실험현시,당항온지설정온도위600 K、700 K화800 K시,광보측량온도여열전우측량치편차소우2%,해방법구유가고성화경강괄응성。
Tunable diode laser absorption spectroscopy is widely used in many applications,with difficulty of abstracting baseline,it is hard to be used in high-pressure and high-disturbing conditions. It′s indicated in theory of wavelength-modulation spectroscopy that the first and second order harmonic signals contain tow common terms: incident intensity and gain of detector . By normalizing 2f signal with 1f signal ( 2f/1f ), dependency of 2f/1f signal on incident intensity was eliminated, absolute strength of a spectra can be obtained subsequently. With measured laser parameter and known spectral parameters, theoretical 2f/1f signal was simulated by numerical calculation. Calibration-free wavelength-modulation spectroscopy was built based on frequency demultiplexing method, by numeric lock-in code. When a temperature stabilized cell was set at 600 K, 700 K, 800 K, precision of 2% is achieved compared with thermocouple measurement, which indicates that the method is much more reliable and adaptable.