• Photonics Research
  • Vol. 10, Issue 11, 2599 (2022)
Huicong Li1、2, Wenzhu Huang1、3, Wentao Zhang1、2、*, and Jianxiang Zhang1、2
Author Affiliations
  • 1State Key Laboratory of Transducer Technology, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 2College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Shenzhen Academy of Disaster Prevention and Reduction, Shenzhen 518003, China
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    DOI: 10.1364/PRJ.468283 Cite this Article Set citation alerts
    Huicong Li, Wenzhu Huang, Wentao Zhang, Jianxiang Zhang. Fiber optic strain rate sensor based on a differentiating interferometer[J]. Photonics Research, 2022, 10(11): 2599 Copy Citation Text show less

    Abstract

    Strain rate is an important basic physical parameter in the fields of deformation observation, geodetic measurement, and geophysical monitoring. This paper proposes a novel fiber optic strain rate sensor (FOSRS) that can directly measure the strain rate through a differentiating interferometer that converts the strain rate to the optical phase. The sensing principle, sensitivity, resolution, and dynamic range of the proposed FOSRS are theoretically analyzed and verified by experiment. The experimental results show that the developed FOSRS with a 12.1 m sensing fiber has a flat sensitivity of 69.50 dB, a nanostrain rate (nε/s) resolution, and a dynamic range of better than 95 dB. An ultrahigh static resolution of 17.07 /s can be achieved by using a 25.277 km sensing fiber for long baseline measurements. The proposed method significantly outperforms existing indirect measurement methods and has potential applications in geophysical monitoring and crustal deformation observation.
    ε˙(t)=dε(t)dt=ddt(dlL)=dvL,

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    ΔLopt(t)={1n22[(1σ)p12σp11]}nΔL(t)=ξnΔL(t),

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    φ(t)=4πξnLλ0ε(t),

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    T=n(LDL0)c,

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    ψ=φ(t)φ(t+T)=Tdφ(t)dt.

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    ε˙(t)=cλ04πn2ξL(LDL0)ψ.

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    I(lopt)=|E1(t)+E2(t+lopt/c)|2=I1+I2+2I1I2Re[γ(lopt/c)],

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    lopt=2[ΔLopt(t)ΔLopt(t+T)],

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    I(lopt)=I1+I2+2I1I2G(lopt)exp(j2πlopt/λ0)=I1+I2+2I1I2G(lopt)exp(jψ).

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    I=I+I1+I2+2I1I2G(lopt)cos(ψ)=D+Acos(ψ),

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    P1=D1+A1cos(ψ),P2=D2+A2cos(ψ+θ),P3=D3+A3cos(ψθ),

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    H(s)=ψ(s)ε(s)s=4πn2ξL(LDL0)cλ0.

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    ε˙min(RIN)=10ψRIN/20cλ04πn2ξL(LDL0),

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    ε˙max<cλ022ξn2(LDL0)LΔλ.

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    DR=20lg(2πλ010ψRIN/20Δλ).

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    ε˙=0.14×106U12.1·2πfsin(2πft).

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    P1=D1+A1cos(θ0),P2=D2+A2cos(θ0+θ1),P3=D3+A3cos(θ0+θ2),(A1)

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    nRIN=[10RIN12010RIN22010RIN320]T.(A2)

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    σRIN2=pθ0TPnRINnRINTPpθ0.(A3)

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    P=[P1000P2000P3],(A4)

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    pθ0T=pTcosθ0qTsinθ0,(A5)

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    [qTpT]=[A3A1D2D1sinθ2A2A1D3D1sinθ1A3A1sinθ2A2A1sinθ1A3A1D2D1cosθ2A2A1D3D1cosθ1D3D1A3A1cosθ2A2A1cosθ1D2D1]D2D1A3sinθ2D3D1A2sinθ1+A2A1A3sin(θ1θ2).(A6)

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    ψRIN=10lg(pθ012P1210RIN110+pθ022P2210RIN210+pθ032P3210RIN310+2pθ01pθ02P1P210RIN1+RIN220+2pθ02pθ03P2P310RIN2+RIN320+2pθ03pθ01P3P110RIN3+RIN120).(A7)

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    Huicong Li, Wenzhu Huang, Wentao Zhang, Jianxiang Zhang. Fiber optic strain rate sensor based on a differentiating interferometer[J]. Photonics Research, 2022, 10(11): 2599
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