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Fiber Bragg-grating strain sensor interrogation using laser radio-frequency modulation

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Abstract

We demonstrate the possibility of using radio-frequency modulation spectroscopic techniques for interrogation of fiber Bragg-grating (FBG) structures. Sidebands at 2 GHz are superimposed onto the output spectrum of a 1560-nm DFB diode laser. The power reflected by an FBG is demodulated at multiples of the sideband frequency. The sideband-to-carrier beat signal is shown to be extremely sensitive to Bragg wavelength shifts due to mechanical stress. Using this method, both static and dynamic strain measurements can be performed, with a noise-equivalent sensitivity of the order of 150 nε/√Hz, in the quasi-static domain (2 Hz), and 1.6 nε/√Hz at higher frequencies (1 kHz). The measured frequency response is presently limited at 20 kHz only by the test device bandwidth. A long-term reproducibility in strain measurements within 100 nε is estimated from laser frequency drift referred to molecular absorption lines.

©2005 Optical Society of America

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Figures (7)

Fig. 1.
Fig. 1. Sketch of the experimental setup. F-P stands for Fabry-Pèrot, BS for beam-splitter, OI for optical isolator, BT for bias-tee, DBM for double-balanced mixer and PD for photodiode.
Fig. 2.
Fig. 2. Example of the signal obtained by high-frequency mixer demodulation upon FBG reflection (maximum at 1560.778 nm). The lower trace corresponds to the transmission of a 1-GHz free-spectral-range Fabry-Pérot interferometer, where RF sidebands at 2.2 GHz are visible.
Fig. 3.
Fig. 3. Response of the LRFM system to static deformations directly applied to the 50-% FBG by the PZT. The dashed line corresponds to a weighted linear fit. Vertical bars are standard errors of mean FBG shifts deriving from 10 measured values.
Fig. 4.
Fig. 4. FFT amplitude spectrum of the sensor output measured by a spectrum analyzer (resolution bandwidth of 50 mHz). The high peak corresponds to excitation of the PZT by a sine wave at 2 Hz with a strain-equivalent amplitude of 3 µε. The red line represents the background when the PZT is off.
Fig. 5.
Fig. 5. Spectrum given by a 3-µε deformation applied to the FBG at higher acoustic frequencies (1 kHz). In this case, the resolution bandwidth is 50 Hz.
Fig. 6.
Fig. 6. LRFM-system time response to excitation of an acoustic wave at 1100 Hz with 20-µε peak-to-peak amplitude (80-% FBG), compared to the output of an electrical strain gauge with 1-µε sensitivity (upper trace).
Fig. 7.
Fig. 7. Static strain values measured by the laser sensor are plotted vs. the electrical probe values. A weighted linear fit is also represented. The error bars represent the maximum uncertainty due to the electrical gauge reading.
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