• Journal of Infrared and Millimeter Waves
  • Vol. 39, Issue 6, 742 (2020)
Ying HE1, Yu-Jun ZHANG1、2、*, Kun YOU1, Bo-Qiang FAN1、2, Meng-Qi LI1、2, Dong-Qi YU1、2, Hao XIE1、2, Bo-En LEI1、2, Wei JIA3, Jun-Sen JING3, and Wen-Qing LIU1、2
Author Affiliations
  • 1Key Laboratory of Environmental Optics & Technology, Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei230031, China
  • 2University of Science and Technology of China, Hefei230026, China
  • 3College of Mechanical and Electrical Engineering, Anhui Jianzhu University, Hefei230601, China
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    DOI: 10.11972/j.issn.1001-9014.2020.06.012 Cite this Article
    Ying HE, Yu-Jun ZHANG, Kun YOU, Bo-Qiang FAN, Meng-Qi LI, Dong-Qi YU, Hao XIE, Bo-En LEI, Wei JIA, Jun-Sen JING, Wen-Qing LIU. Precise measurements the broadening characteristics and parameters of methane near-infrared absorption spectrum at high pressure[J]. Journal of Infrared and Millimeter Waves, 2020, 39(6): 742 Copy Citation Text show less

    Abstract

    The high-pressure absorption spectrum at 6046.96 cm-1 of methane was obtained with the measurement experimental platform. The empirical mode decomposition algorithm was used to filter out the detection noise caused by window deformation at high-pressure. Consequently, the overall root-mean-square error (RMSE) of absorbance signal was reduced by 3.87 times, and the residual error of absorbance signal fitting was lower than ±1% by using Lorentz line-type fitting algorithm. These studies showed that the absorption line width increased with the pressure increasing, and the mutual broadening coefficient of nitrogen-methane molecules at high-pressure was calculated as 0.0631 cm -1atm -1. Moreover, the absorption line appeared a "red shift" phenomenon as the pressure increasing, and the pressure shift coefficient of nitrogen-induced was calculated as -0.00848 cm -1atm -1. Therefore, a method of concentration inversion at high pressure was proposed by the linear relationship between the detection wavelength, pressure, and pressure shift coefficient. In conclusion, the research on spectrum broadening characteristics in high-pressure environment lays foundation for spectrum detecting in industrial environment.
    Aν=lnI0νItν=S(T)ϕ(v)PxL(1)

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    Δvc=PBxB2γA-B(2)

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    2γA-B(T)=2γA-B(T0)(T0T)n(3)

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    ν=ν0+P[δN2(1-x)+δselfx](4)

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    H1=X(t)-m1(5)

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    r1=Xt-IMF1(6)

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    rn=rn-1-IMFn(7)

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    X(t)=j=1nIMFj(t)+rn(t)(8)

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    kT=2γselfTxCH4+2γN2-CH4T1-xCH4(9)

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    ν=6 046.963 8-0.008 48P1-x(10)

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    x=1-6 046.963 8-ν0.008 48P(11)

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    Ying HE, Yu-Jun ZHANG, Kun YOU, Bo-Qiang FAN, Meng-Qi LI, Dong-Qi YU, Hao XIE, Bo-En LEI, Wei JIA, Jun-Sen JING, Wen-Qing LIU. Precise measurements the broadening characteristics and parameters of methane near-infrared absorption spectrum at high pressure[J]. Journal of Infrared and Millimeter Waves, 2020, 39(6): 742
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