“…During manufacture of the panels, optical fibres containing the CFBG sensors were embedded near the first 0/90 interface, and therefore approximately 0.5 mm from the adhesive bondline. The adherends containing the sensors were cut so that the low-wavelength end of the sensor was adjacent to the cut end of one adherend (further fabrication details can be found in previous papers [15,16]). For this work, CFBG sensors with a range of sensor lengths have been used (15,30,45 and 60 mm), although all sensors had the same spectral bandwidth, having a full width at the half-maximum of the reflected spectrum of 20 nm (i.e.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…Figure 1 shows a schematic diagram of the single-lap joint and the position of the embedded CFBG sensor. The optical fibre containing the sensor was spliced to the optical arrangement which consisted of a broadband light source, coupler and optical spectrum analyser (details are provided in [14][15][16]). The bonded joints were subjected to fatigue loading using a computer-controlled servohydraulic fatigue machine (Instron 1341) with a peak load of 8 kN, an R-value (R= min / max ) of 0.1, and a sinusoidal waveform with a frequency of 3 Hz.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…Earlier work using a CFBG sensor with a length of 45 mm [16] produced a reflected spectrum which showed a perturbation at the position of the disbond front that was significantly more symmetrical in shape compared to the perturbation shown in Figure 4 for a 15 mm sensor. To investigate the effect of sensor length on the reflected spectrum in the presence of a disbond, spectra for sensors with the same spectral bandwidth of 20 nm, but different sensor lengths (15 mm, 30 mm, 45 mm and 60 mm) have been predicted.…”
Section: Effect Of Sensor Length and Chirp Ratementioning
confidence: 99%
“…In addition to uniform fibre Bragg gratings, chirped fibre Bragg grating (CFBG) sensors have been investigated more recently for damage monitoring in composite materials, bonded joints and sandwich structures (e.g. [12][13][14][15][16][17]), following the initial demonstration by Takeda, Okabe and colleagues [e.g. 18] that such sensors could both detect and locate damage development in composite materials.…”
Section: Introductionmentioning
confidence: 99%
“…In previous work [15,16] it was shown that a CFBG sensor could be used to monitor disbond initiation from one end of the overlap of a composite-composite bonded joint. In the present paper, the work is extended (a) to show that disbond monitoring at both ends of the overlap is possible with a single embedded sensor, and (b) to determine the effect of using different sensor lengths.…”
Adhesively bonded composite-composite single-lap joints, with cross-ply GFRP adherends, have been cyclically loaded to initiate disbonding at either end of the overlap length. Disbond initiation and growth have been monitored using a combination of in situ photography (the joint is transparent) and a single chirped fibre Bragg grating (CFBG) sensor embedded within one composite adherend (with the low-wavelength end of the sensor adjacent to the cut end) and not in the adhesive bondline. Sensors having the same spectral bandwidth (20 nm), and lengths in the range 15 mm to 60 mm have been tested. The experimental results have been modelled using a combination of finite-element analysis and commercial software for predicting FBG spectra, and the predictions are in very good agreement with the experimental results. In all cases, it has been shown that the position of the disbond front can be located using the CFBG sensors with a precision of about 2 mm.
“…During manufacture of the panels, optical fibres containing the CFBG sensors were embedded near the first 0/90 interface, and therefore approximately 0.5 mm from the adhesive bondline. The adherends containing the sensors were cut so that the low-wavelength end of the sensor was adjacent to the cut end of one adherend (further fabrication details can be found in previous papers [15,16]). For this work, CFBG sensors with a range of sensor lengths have been used (15,30,45 and 60 mm), although all sensors had the same spectral bandwidth, having a full width at the half-maximum of the reflected spectrum of 20 nm (i.e.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…Figure 1 shows a schematic diagram of the single-lap joint and the position of the embedded CFBG sensor. The optical fibre containing the sensor was spliced to the optical arrangement which consisted of a broadband light source, coupler and optical spectrum analyser (details are provided in [14][15][16]). The bonded joints were subjected to fatigue loading using a computer-controlled servohydraulic fatigue machine (Instron 1341) with a peak load of 8 kN, an R-value (R= min / max ) of 0.1, and a sinusoidal waveform with a frequency of 3 Hz.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…Earlier work using a CFBG sensor with a length of 45 mm [16] produced a reflected spectrum which showed a perturbation at the position of the disbond front that was significantly more symmetrical in shape compared to the perturbation shown in Figure 4 for a 15 mm sensor. To investigate the effect of sensor length on the reflected spectrum in the presence of a disbond, spectra for sensors with the same spectral bandwidth of 20 nm, but different sensor lengths (15 mm, 30 mm, 45 mm and 60 mm) have been predicted.…”
Section: Effect Of Sensor Length and Chirp Ratementioning
confidence: 99%
“…In addition to uniform fibre Bragg gratings, chirped fibre Bragg grating (CFBG) sensors have been investigated more recently for damage monitoring in composite materials, bonded joints and sandwich structures (e.g. [12][13][14][15][16][17]), following the initial demonstration by Takeda, Okabe and colleagues [e.g. 18] that such sensors could both detect and locate damage development in composite materials.…”
Section: Introductionmentioning
confidence: 99%
“…In previous work [15,16] it was shown that a CFBG sensor could be used to monitor disbond initiation from one end of the overlap of a composite-composite bonded joint. In the present paper, the work is extended (a) to show that disbond monitoring at both ends of the overlap is possible with a single embedded sensor, and (b) to determine the effect of using different sensor lengths.…”
Adhesively bonded composite-composite single-lap joints, with cross-ply GFRP adherends, have been cyclically loaded to initiate disbonding at either end of the overlap length. Disbond initiation and growth have been monitored using a combination of in situ photography (the joint is transparent) and a single chirped fibre Bragg grating (CFBG) sensor embedded within one composite adherend (with the low-wavelength end of the sensor adjacent to the cut end) and not in the adhesive bondline. Sensors having the same spectral bandwidth (20 nm), and lengths in the range 15 mm to 60 mm have been tested. The experimental results have been modelled using a combination of finite-element analysis and commercial software for predicting FBG spectra, and the predictions are in very good agreement with the experimental results. In all cases, it has been shown that the position of the disbond front can be located using the CFBG sensors with a precision of about 2 mm.
Herein, we present a novel approach for damage sensing in adhesively bonded joints using a carbon nanotube single layer web (CNT-SLW) which marks a significant departure from the approach of dispersing CNTs within epoxy resins. In this work, a very thin, highly aligned CNT-SLW (densified thickness ~ 50 nm) with aerial density of 2.0 µg/cm 2 was horizontally drawn from a vertically aligned CNT forest, positioned over an adhesive film, which was, in turn, placed between two non-conductive composite adherents. This was followed by the application of heat and pressure to cure the adhesive. These joints were subjected to quasi-static and cyclic loading to investigate the damage sensing performance of a CNT-SLW. The CNT-SLW sensor, placed parallel to the load direction, exhibits remarkably high cyclic stability as well as exceptionally high sensitivity to damage initiation and accumulation. The resistance increase (∆R/R o % ∼1633%) is significantly higher than that of adhesive sensors with dispersed CNTs/graphene, reported in the literature. Morphological studies help to explain the sensing mechanism through interactions of the CNT-SLW with the evolution of micro-cracks. These results demonstrate the potential of
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