Calculating strain from Brillouin frequency data
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Published:2016
Cedric Kechavarzi, MSc, PhD, FHEA, Kenichi Soga, FREng, FICE, Nicholas de Battista, BE&A (Hons), MSc, PhD, MASCE, A&CE, Loizos Pelecanos, MEng(Hons), ACGI, PhD, DIC, Mohammed Z E B Elshafie, BSc (Hons), MPhil, PhD, Robert J Mair, CBE FREng, FICE, FRS, 2016. "Calculating strain from Brillouin frequency data", Distributed Fibre Optic Strain Sensing for Monitoring Civil Infrastructure: A Practical Guide, Cedric Kechavarzi, MSc, PhD, FHEA, Kenichi Soga, FREng, FICE, Nicholas de Battista, BE&A (Hons), MSc, PhD, MASCE, A&CE, Loizos Pelecanos, MEng(Hons), ACGI, PhD, DIC, Mohammed Z E B Elshafie, BSc (Hons), MPhil, PhD, Robert J Mair, CBE FREng, FICE, FRS
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As described in section 1.1.6, the Brillouin scattering frequency, , is a function of the refractive index of the fibre core, n, the acoustic wave velocity, , in the fibre (~5800 m/s), and the wavelength of the incident light, (Equation 1.4).
This Brillouin frequency shifts linearly with changes in longitudinal strain and temperature in the fibre core/cladding so that (Horiguchi et al., 1989):
or
which is the same as Equation 1.9 where is the change in Brillouin frequency due to a simultaneous change in strain, , and in temperature, . Here, Cɛ and CT are referred to as the strain coefficient and the temperature coefficient, respectively, of the Brillouin frequency shift.
