Simultaneous distributed measurement of strain and temperature from noise-initiated Brillouin scattering in optical fibers

The simultaneous determination of strain and temperature distributions from the measurement of noise-initiated Brillouin scattering (NIBS) power and frequency shift in optical fibers is discussed. Equations governing the growth of the NIBS signal are derived and from these, we calculate the dependence of the Brillouin power on temperature and strain. We study the potential problem given by the need to normalize the nonlinear Brillouin signal and present a new technique that solves this problem by mathematically combining the values of the Stokes and anti-Stokes powers to produce a linear effective power. Experimental results are presented that support this theory and allow the verification of the coefficients governing the dependence of the Brillouin power and frequency shift on temperature and strain. The signal-to-noise ratio of the sensor is discussed, and it is found that the noise associated with the field statistics plays a limiting role in the sensor performance and that an optimum value for the Brillouin gain factor can be determined. A simultaneous distributed temperature and strain sensor is demonstrated; preliminary results show a strain resolution of 100-/spl mu/m strain, a temperature resolution of 4/spl deg/C, and a spatial resolution of 40 m, over a sensing length of 1200 m.

[1]  H. Ehrenreich,et al.  Absorption of Sound in Insulators , 1961 .

[2]  Norman M. Kroll,et al.  Excitation of Hypersonic Vibrations by Means of Photoelastic Coupling of High-Intensity Light Waves to Elastic Waves , 1965 .

[3]  C. Tang Saturation and Spectral Characteristics of the Stokes Emission in the Stimulated Brillouin Process , 1966 .

[4]  R. Glauber,et al.  Quantum Theory of Light Propagation in Amplifying Media , 1971 .

[5]  W. Louisell Quantum Statistical Properties of Radiation , 1973 .

[6]  Michael G. Raymer,et al.  Stimulated Raman scattering: Unified treatment of spontaneous initiation and spatial propagation , 1981 .

[7]  Govind P. Agrawal,et al.  Nonlinear Fiber Optics , 1989 .

[8]  E. M. Dianov,et al.  Saturation effects at backward-stimulated scattering in the single-mode regime of interaction , 1989 .

[9]  T. Horiguchi,et al.  Tensile strain dependence of Brillouin frequency shift in silica optical fibers , 1989, IEEE Photonics Technology Letters.

[10]  D. Jackson,et al.  Potential of stimulated Brillouin scattering as sensing mechanism for distributed temperature sensors , 1989 .

[11]  Boyd,et al.  Noise initiation of stimulated Brillouin scattering. , 1990, Physical review. A, Atomic, molecular, and optical physics.

[12]  Yahei Koyamada,et al.  Brillouin optical-fiber time domain reflectometry , 1993 .

[13]  L. Mandel,et al.  Optical Coherence and Quantum Optics , 1995 .

[14]  K. Shimizu,et al.  Development of a distributed sensing technique using Brillouin scattering , 1995 .

[15]  T. Newson,et al.  Landau Placzek ratio applied to distributed fibre sensing , 1996 .

[16]  M Farhadiroushan,et al.  Temperature and strain dependence of the power level and frequency of spontaneous Brillouin scattering in optical fibers. , 1997, Optics letters.

[17]  T. Parker,et al.  A fully distributed simultaneous strain and temperature sensor using spontaneous Brillouin backscatter , 1997, IEEE Photonics Technology Letters.