• Laser & Optoelectronics Progress
  • Vol. 60, Issue 17, 1712006 (2023)
Junyan Zhuang1, Yunyun Chen1,2,3,*, and Yayi Chen1,2,3
Author Affiliations
  • 1School of Physics and Optoelectronic Engineering, Nanjing University of Information Science & Technology, Nanjing 210044, Jiangsu , China
  • 2Jiangsu Key Laboratory for Optoelectronic Detection of Atmosphere and Ocean, Nanjing University of Information Science & Technology, Nanjing 210044, Jiangsu , China
  • 3Jiangsu International Joint Laboratory on Meteorological Photonics and Optoelectronic Detection, Nanjing University of Information Science & Technology, Nanjing 210044, Jiangsu , China
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    DOI: 10.3788/LOP221975 Cite this Article Set citation alerts
    Junyan Zhuang, Yunyun Chen, Yayi Chen. Double-Temperature Measurements of Arc Plasmas by Integrating Two-Wavelength Moiré and Emission Tomography[J]. Laser & Optoelectronics Progress, 2023, 60(17): 1712006 Copy Citation Text show less

    Abstract

    In this paper, a double-temperature refractive index model, which can be used to simultaneously obtain the temperatures of the electron and gas for plasma, is introduced. In addition, the rationality and superiority of the proposed model are theoretically discussed. Furthermore, argon arc plasmas with different injected pressures are selected as practical examples for experiments. During the experiments, refractive index measurements are performed using two-wavelength moiré tomography with probe wavelengths of 532 nm and 808 nm. The region division of the measured argon plasmas is achieved using emission tomography. Finally, the temperatures of the electron and gas are reconstructed to verify the feasibility of the double-temperature refractive index model, and the factors that might cause imprecision are analyzed. The findings of this study will be valuable for expanding the applicable region of optical computerized tomography methods and facilitating optical diagnosis in plasma flow fields .
    n-1=1LA+Bλ2Nn+δ1LA+Bλ2Ni-4.46×10-14λ2Ne=1LA+Bλ2(Nn+δNi)-4.46×10-14λ2Ne
    α121-α22=1PK1(Te)
    K1(Te)=2Z1Z02πmeh23/2κTe52exp-E1κTe
    α1=1PK1(Te)1+1PK1(Te)12
    N1=Ne=α1Na0
    Na=1-α1Na0
    P=NaκTg+N1κTg+NeκTe=1-α1Na0κTg+α1Na0κTg+α1Na0κTe=1-α1κTg+α1κTg+α1κTeNa0=Tg+α1TeκNa0,
    Na0=PTg+α1Teκ
    n-1=1LA+Bλ21-α1Na0+δα1Na0-4.46×10-14λ2α1Na0=1LA+Bλ21-α1+δα1-4.46×10-14λ2α1Na0=1LA+Bλ21-1-δα1-4.46×10-14λ2α1PTg+α1Teκ
    1LA+Bλ21-1-δα1-4.46×10-14λ2α1P1+α1Teκ,Tg~Te1LA+Bλ21-1-δα1-4.46×10-14λ2α1PTg/Te+α1κ,Tg~α1Te1LA+Bλ21-1-δα1-4.46×10-14λ2α1Pα1Teκ,Tgα1Te
    n1λ1-1=1LA+Bλ121-1-δα1-4.46×10-14λ12α1PTg+α1Teκ
    n2λ2-1=1LA+Bλ221-1-δα1-4.46×10-14λ22α1PTg+α1Teκ
    n1λ1-1n2λ2-1=1LA+Bλ121-1-δα1-4.46×10-14λ12α11LA+Bλ221-1-δα1-4.46×10-14λ22α1
    α1=11-δ+4.46×10-14λ12n2λ2-1-λ22n1λ1-11Ln2λ2-1A+Bλ12-n1λ1-1A+Bλ22
    Tg1=1LA+Bλ121-1-δα1-4.46×10-14λ12α1Pn1λ1-1κ-α1Te
    Tg2=1LA+Bλ221-1-δα1-4.46×10-14λ22α1Pn2λ2-1κ-α1Te
    Tg=Tg1+Tg2/2
    f(Te)=α1-1PK1(Te)1+1PK1(Te)12
    n-1=1LA+Bλ21-0.33α1-4.46×10-14λ2α1+α1α2P1+α1+α1α2κT
    Junyan Zhuang, Yunyun Chen, Yayi Chen. Double-Temperature Measurements of Arc Plasmas by Integrating Two-Wavelength Moiré and Emission Tomography[J]. Laser & Optoelectronics Progress, 2023, 60(17): 1712006
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