As described in section 1.1.6, the Brillouin scattering frequency, vb, is a function of the refractive index of the fibre core, n, the acoustic wave velocity, υa, in the fibre (~5800 m/s), and the wavelength of the incident light, λ (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 Δvb is the change in Brillouin frequency due to a simultaneous change in strain, Δε, and in temperature, ΔT. Here, Cɛ and CT are referred to as the strain coefficient and the temperature coefficient, respectively, of the Brillouin frequency shift.

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