2021
DOI: 10.1016/j.compstruct.2021.114087
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A simultaneous dual-parameter optical fibre single sensor embedded in a glass fibre/epoxy composite

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Cited by 15 publications
(14 citation statements)
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“…At the same time, the cladding resonances undergo a wavelength shift and amplitude change when the external RI is varying. Hence, by performing a preliminary calibration, both the Bragg and the Ghost peaks can be used to measure simultaneously and separately the temperature and the strain variation of the material where the sensor is embedded [8]. At the same time, the envelope area of the upper and lower cladding resonance peaks can be used to detect independently the RI variation of the medium surrounding the TFBG sensor [7,[14][15][16].…”
Section: Tfbg Sensing Theorymentioning
confidence: 99%
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“…At the same time, the cladding resonances undergo a wavelength shift and amplitude change when the external RI is varying. Hence, by performing a preliminary calibration, both the Bragg and the Ghost peaks can be used to measure simultaneously and separately the temperature and the strain variation of the material where the sensor is embedded [8]. At the same time, the envelope area of the upper and lower cladding resonance peaks can be used to detect independently the RI variation of the medium surrounding the TFBG sensor [7,[14][15][16].…”
Section: Tfbg Sensing Theorymentioning
confidence: 99%
“…Each single TFBG sensor has been theoretically demonstrated to be able to measure simultaneously and separately strain, temperature and refractive index (RI) of the surrounding material [7]. While, in a real application, it was proven that this single sensor may be used to determine the thermomechanical state of a glass-fibre/epoxy composite when embedded inside [8].…”
Section: Introductionmentioning
confidence: 99%
“…Specifically n eff,core and n eff,clad,i are respectively referred to as the core and cladding modes. The wavelengths of the Bragg (λ Bragg ) and cladding (λ clad,i ) resonance peaks can be then obtained using the following fundamental equations [15]:…”
Section: Tfbg Theory and Influence Of The Surrounding Rimentioning
confidence: 99%
“…Figure 2 shows the internal structure of a weak where the tilt angle θ, the grating period ΛG along the OF axis and the no period Λ = ΛGcosθ are defined. By considering the effective refractive inde mode, the nominal wavelength can be calculated for each peak in the spec cally neff,core and neff,clad,i are respectively referred to as the core and claddin wavelengths of the Bragg ( Bragg) and cladding ( clad,i) resonance peaks can be using the following fundamental equations [15]: Once the Bragg structure is defined, if no mechanical perturbations are appli OF, then the grating period and the tilt angle are constant, then neff,core is also fixed the RI of the core and cladding OF layers are defined. As neff,clad,i is sensitive to rounding RI variations, each cladding mode has to fit with a new propagating c so that the phase-matching condition (represented by Equation ( 2)) is satisfied nominal wavelength changes for each external RI.…”
Section: Tfbg Theory and Influence Of The Surrounding Rimentioning
confidence: 99%
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