• Acta Physica Sinica
  • Vol. 68, Issue 23, 233301-1 (2019)
Bu-Qiang Zhang1,2, Zhen-Yu Xu1, Jian-Guo Liu1, Lu Yao1..., Jun Ruan1, Jia-Yi Hu1, Hui-Hui Xia1, Wei Nie1,2, Feng Yuan1,2 and Rui-Feng Kan3,*|Show fewer author(s)
Author Affiliations
  • 1Key Laboratory of Environmental Optics and Technology, Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei 230031, China
  • 2University of Science and Technology of China, Hefei 230026, China
  • 3Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, China
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    DOI: 10.7498/aps.68.20190515 Cite this Article
    Bu-Qiang Zhang, Zhen-Yu Xu, Jian-Guo Liu, Lu Yao, Jun Ruan, Jia-Yi Hu, Hui-Hui Xia, Wei Nie, Feng Yuan, Rui-Feng Kan. Temperature measurement method of high temperature and high pressure flow field based on wavelength modulation spectroscopy technology[J]. Acta Physica Sinica, 2019, 68(23): 233301-1 Copy Citation Text show less
    Simulated absorbance at different pressures: (a) Line1; (b) line2; (c) line3.模拟不同压强下的吸光度 (a) Line1; (b) line2; (c) line3
    Fig. 1. Simulated absorbance at different pressures: (a) Line1; (b) line2; (c) line3. 模拟不同压强下的吸光度 (a) Line1; (b) line2; (c) line3
    The peak ratio of 2f/1f of the two pairs of absorption lines obtained by simulation varies with temperature and concentration: (a) Line2& Line1; (b) Line2& Line3.模拟两对吸收线2f/1f峰值比随温度和浓度变化 (a) Line2& Line1; (b) Line2& Line3
    Fig. 2. The peak ratio of 2f/1f of the two pairs of absorption lines obtained by simulation varies with temperature and concentration: (a) Line2& Line1; (b) Line2& Line3. 模拟两对吸收线2f/1f峰值比随温度和浓度变化 (a) Line2& Line1; (b) Line2& Line3
    Process of temperature inversion.温度反演流程
    Fig. 3. Process of temperature inversion.温度反演流程
    Device diagram of field test.现场实验装置图
    Fig. 4. Device diagram of field test.现场实验装置图
    Calibration result of .的标定结果
    Fig. 5. Calibration result of . 的标定结果
    Original absorption signal (top) and harmonic signal (bottom).原始吸收信号(上)和谐波信号(下)
    Fig. 6. Original absorption signal (top) and harmonic signal (bottom).原始吸收信号(上)和谐波信号(下)
    Temperature measurement results of three different working conditions.三种不同工况温度测量结果
    Fig. 7. Temperature measurement results of three different working conditions.三种不同工况温度测量结果
    ${\upsilon _0}$/cm–1$S({T_0})$@296 K/cm–2·atm–1E''/cm–1γair0/cm–1·atm–1γself/cm–1·atm–1
    7185.601.91 × 10–21045.060.0410.198
    6807.836.03 × 10–63319.450.0980.183
    7444.35/371.10 × 10–31774/18060.019/0.01530.2/0.23
    Table 1.

    Spectroscopic parameters of three absorption lines.

    三条吸收线谱线参数

    StatePressure/atmFlow/kg·s–1Average temperature/K
    13.490.511958
    27.040.9971420
    310.581.481512
    Table 2. Parameters of different operating conditions
    State & illustrateState 1State 2State 3
    First groupAverage temperature/K975.411481.291596.33
    Absolute error/K17.4161.2984.33
    Relative error/%1.824.325.58
    Second groupAverage temperature/K980.571473.661595.77
    Absolute error/K22.5753.6683.77
    Relative error/%2.363.785.54
    Third groupAverage temperature/K982.911481.461601.50
    Absolute error/K24.9161.4689.50
    Relative error/%2.604.335.92
    TotalAverage temperature/K979.631478.801597.87
    Absolute error/K21.6358.8085.87
    Relative error/%2.264.145.68
    Table 3. Measurement result.
    Bu-Qiang Zhang, Zhen-Yu Xu, Jian-Guo Liu, Lu Yao, Jun Ruan, Jia-Yi Hu, Hui-Hui Xia, Wei Nie, Feng Yuan, Rui-Feng Kan. Temperature measurement method of high temperature and high pressure flow field based on wavelength modulation spectroscopy technology[J]. Acta Physica Sinica, 2019, 68(23): 233301-1
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