In-fiber Bragg gratings exhibit dual sensitivity since their output relative wavelength shift (ΔλB/λB) depends on either the applied strain variation or the temperature difference, as shown by the sensing equation [8]:
where λB is the Bragg wavelength, pe the photo-elastic constant of the optical fiber, ξ the thermo-optic constant, αf the thermal expansion coefficient, ΔT the temperature interval (defined as the difference between the actual temperature T and the reference one Tref at which λB has been measured) and Δε the total strain variation along the grating due to the combined action of external forces and apparent strain induced by differential thermal expansion of the optical fiber relative to the host structure. These constants can be condensed into two coefficients, Kε and KT, which represent the strain sensitivity and the temperature sensitivity, respectively. If the two wavelength contributions of Equation (1) can be discriminated, it is then possible to measure simultaneously both temperature and strain.
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