• Infrared and Laser Engineering
  • Vol. 49, Issue 6, 20190575 (2020)
Tao Xiong1, Ming Gao1, Gibson Des2, and Hutson David2
Author Affiliations
  • 1西安工业大学 光电工程学院,陕西 西安 710021
  • 2西苏格兰大学 薄膜、传感器、成像学院,英国 佩斯利 PA12BE
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    DOI: 10.3788/IRLA20190575 Cite this Article
    Tao Xiong, Ming Gao, Gibson Des, Hutson David. Mainstream NDIR breathing CO2 monitoring system based on new light chamber structure[J]. Infrared and Laser Engineering, 2020, 49(6): 20190575 Copy Citation Text show less
    CPC longitudinal cross section[12]
    Fig. 1. CPC longitudinal cross section[12]
    (a) Optimization results of the CPC focusing system; (b) Aluminum CPC
    Fig. 2. (a) Optimization results of the CPC focusing system; (b) Aluminum CPC
    (a) Signal acquisition system (gas chamber) with CPC; (b) Respiratory CO2 monitoring system; (c) Schematic diagram of the main parts of the monitoring system
    Fig. 3. (a) Signal acquisition system (gas chamber) with CPC; (b) Respiratory CO2 monitoring system; (c) Schematic diagram of the main parts of the monitoring system
    (a) Straight cylinder concentrator; (b) Cone concentrator; (c) compound parabolic concentrator ray trace using ZEMAX, and samples of them; (d) Photoconductive infrared detector of the chamber
    Fig. 4. (a) Straight cylinder concentrator; (b) Cone concentrator; (c) compound parabolic concentrator ray trace using ZEMAX, and samples of them; (d) Photoconductive infrared detector of the chamber
    (a) CMOS detector(Point Grey Research, Inc) (left) and IR source EMIRS200(Axetris)(right); (b) Environment of CPC verification experiment
    Fig. 5. (a) CMOS detector(Point Grey Research, Inc) (left) and IR source EMIRS200(Axetris)(right); (b) Environment of CPC verification experiment
    Calibration experiment environment diagram
    Fig. 6. Calibration experiment environment diagram
    When the CPC and the detector are at different distances, (a) Spot pattern on the detector obtained by ZEMAX simulation; (b)Spot pattern captured by the CMOS detector in the verification experiment;(c) Comparison of the normalized light spot cross-section brightness distribution between the simulation results (silver) and experimental results (orange) at different distances between the CPC and the detector
    Fig. 7. When the CPC and the detector are at different distances, (a) Spot pattern on the detector obtained by ZEMAX simulation; (b)Spot pattern captured by the CMOS detector in the verification experiment;(c) Comparison of the normalized light spot cross-section brightness distribution between the simulation results (silver) and experimental results (orange) at different distances between the CPC and the detector
    (a)Straight cylinder concentrator, (b)cone concentrator , (c)light distribution of compound parabolic concentrator on the signal channel detector
    Fig. 8. (a)Straight cylinder concentrator, (b)cone concentrator , (c)light distribution of compound parabolic concentrator on the signal channel detector
    Relationship between the output signals of three systems corresponding to the CO2 concentration in the range of 10 000 ppm to 73 000 ppm CO2 concentration
    Fig. 9. Relationship between the output signals of three systems corresponding to the CO2 concentration in the range of 10 000 ppm to 73 000 ppm CO2 concentration
    CO2 waveform
    Fig. 10. CO2 waveform
    ParametersValue
    Power of the source/W1
    Type of IR sourceThermal infrared emitters (Lambertian source)
    Detector size/mm27.2×5.6
    Number of analyzing rays10 000 000
    IR source size/mm22.1×1.8
    Distance from light source to CPC/mm0.5
    Distance from CPC to detector/mm20
    Table 1. Input parameters in ZEMAX
    ParametersValue
    Radial aperture/mm1.79
    Angle/(°)22.86
    Length/mm9.99
    Table 2. Optimized parameters of CPC
    TypeLight efficiency
    Straight cylinder concentrator0.047%
    Cone concentrator1.2%
    Compound parabolic concentrator4.3%
    Table 3. Optical efficiency simulation results of three structures
    TypeabcdR2
    Straight cylinder0.000 70–0.148 710.49424.9430.969 9
    Cone0.001 5–0.314 822.86652.9630.978 1
    CPC0.001 1–0.262 324.03368.7790.985 3
    Table 4. Third-order polynomial fitting coefficient and calibration coefficient of system output and CO2 concentration
    TypeSNR
    Straight cylinder12.8
    Cone17.2
    CPC24.65
    Table 5. Signal-to-noise ratio of the monitoring system after installing three structures
    Tao Xiong, Ming Gao, Gibson Des, Hutson David. Mainstream NDIR breathing CO2 monitoring system based on new light chamber structure[J]. Infrared and Laser Engineering, 2020, 49(6): 20190575
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