• Chinese Optics Letters
  • Vol. 17, Issue 7, 070602 (2019)
Jian Li1、2, Yang Xu1、2, Mingjiang Zhang1、2、*, Jianzhong Zhang1、2, Lijun Qiao1、2, and Tao Wang1、2
Author Affiliations
  • 1Key Laboratory of Advanced Transducers and Intelligent Control System, Ministry of Education and Shanxi Province, Taiyuan 030024, China
  • 2College of Physics & Optoelectronics, Taiyuan University of Technology, Taiyuan 030024, China
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    DOI: 10.3788/COL201917.070602 Cite this Article Set citation alerts
    Jian Li, Yang Xu, Mingjiang Zhang, Jianzhong Zhang, Lijun Qiao, Tao Wang. Performance improvement in double-ended RDTS by suppressing the local external physics perturbation and intermodal dispersion[J]. Chinese Optics Letters, 2019, 17(7): 070602 Copy Citation Text show less

    Abstract

    We propose and experimentally demonstrate a novel Raman-based distributed fiber-optics temperature sensor (RDTS) for improving the temperature measurement accuracy and engineering applicability. The proposed method is based on double-ended demodulation with a reference temperature and dynamic dispersion difference compensation method, which can suppress the effect of local external physics perturbation and intermodal dispersion on temperature demodulation results. Moreover, the system can omit the pre-calibration process by using the reference temperature before the temperature measurement. The experimental results of dispersion compensation indicate that the temperature accuracy optimizes from 5.6°C to 1.2°C, and the temperature uncertainty decreases from 16.8°C to 2.4°C. Moreover, the double-ended configuration can automatically compensate the local external physics perturbation of the sensing fiber, which exhibits a distinctive improvement.
    ϕs(L)=ϕs[(L2maxL2L1maxL1)L+L2(L2L2maxL1L1max)L1],(1)

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    RBack(T,L)=ϕsBackϕaBack=KsKa(υsυa)4exp(hΔvkT)exp{0L[αa(L)αs(L)]dL},(2)

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    RFor(T,L)=ϕsForϕaFor=KsKa(υsυa)4exp(hΔvkT)exp{Ll[αa(L)αs(L)]dL}.(3)

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    RLoop(T,L)=RBack(T,L)·RFor(T,L)=KsKa(υsυa)4exp(hΔvkT)exp{0l[αa(L)αs(L)]dL}.(4)

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    RLoop(T0,L0)=RBack(T0,L0)·RFor(T0,L0)=KsKa(υsυa)4exp(hΔvkT0)exp{0l[αa(L)αs(L)]dL}.(5)

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    1T=ln[RLoop(T,L)RLoop(T0,L0)](khΔv)+1T0.(6)

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    R(Tc,L)=ϕscBackϕacBack=KsKa(υsυa)4exp(hΔvkTc)exp{0L[αa(L)αs(L)]dL}.(7)

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    R(T,L)=ϕsBackϕaBack=KsKa(υsυa)4exp(hΔvkT)E(L)exp{0L+l[αa(L)αs(L)]dL}.(8)

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    1T=ln[R(T,L)/R(Tc,L)](k/hΔv){ln[E(L)]0l[αa(L)αs(L)]dL}1+1Tc.(9)

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    Jian Li, Yang Xu, Mingjiang Zhang, Jianzhong Zhang, Lijun Qiao, Tao Wang. Performance improvement in double-ended RDTS by suppressing the local external physics perturbation and intermodal dispersion[J]. Chinese Optics Letters, 2019, 17(7): 070602
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