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H2O温度二维分布的滤波反投影重建
引用本文:宋俊玲, 洪延姬, 王广宇. H2O温度二维分布的滤波反投影重建[J]. 强激光与粒子束, 2012, 24: 2073-2078. doi: 10.3788/HPLPB20122409.2073
作者姓名:宋俊玲  洪延姬  王广宇
作者单位:1.装备学院 激光推进及其应用国家重点实验室, 北京 1 01 41 6
摘    要:利用可调谐半导体吸收光谱技术实现燃烧场温度二维分布重建。设计H2O模型温度分布范围为300~1300 K,高斯型分布,利用Radon变换模拟实验测量结果。采用滤波反投影算法重建了两条吸收谱线强度场,进而得到气体温度二维分布,重建结果与模型符合较好。研究了不同投影数目和随机噪声对重建结果的影响,结果表明:随着投影数目的减少和噪声幅值的增加,重建温度分布均方误差增大,图像重建效果变差。当投影数目减小到4个,重建温度场已不能完全反映原始温度场信息。

关 键 词:激光吸收光谱   气体温度二维重建   滤波反投影   谱线强度   投影数目
收稿时间:2011-10-25
修稿时间:2011-12-16

Two-dimensional water temperature reconstruction by filtered back-projection method
Song Junling, Hong Yanji, Wang Guangyu. Two-dimensional water temperature reconstruction by filtered back-projection method[J]. High Power Laser and Particle Beams, 2012, 24: 2073-2078. doi: 10.3788/HPLPB20122409.2073
Authors:Song Junling  Hong Yanji  Wang Guangyu
Affiliation:1. National Key Laboratory of Laser Propulsion and Application,Academy of Equipment,Beijing 101416,China
Abstract:The reconstruction of water temperature in combustion is realized by the tunable diode laser absorption spectroscopy technique. The model for H2O temperature distribution is assumed as a Gaussian function, ranging from 300 K to 1300 K. Radon transform is used to simulate the experimental results. The reconstruction of temperature distribution is achieved by reconstruction of two temperature-dependent line strengths based on the filtered back-projection method. The temperature reconstruction result agrees well with the original model. Moreover, the influences of the number of projections and random errors in projections on reconstruction are also studied. The simulation results indicate that the decrease in projection number or the increase in noise increases the mean square error of the reconstructed temperature, deteriorating the reconstructed image. The temperature reconstruction can not reveal the original temperature distribution when the projection number reduces to four.
Keywords:laser absorption spectroscopy  two dimensional temperature reconstruction  filtered back-projection  spectral intensity  projection number
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