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Search Results (412)

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Keywords = fibre sensors

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11 pages, 8257 KiB  
Article
Fibre Optic Method for Detecting Oil Fluorescence in Marine Sediments
by Emilia Baszanowska, Zbigniew Otremba and Maria Kubacka
Sensors 2025, 25(1), 173; https://doi.org/10.3390/s25010173 - 31 Dec 2024
Viewed by 163
Abstract
The aim of this study is to verify the possibility of detecting oil in the bottom sediment using a fibre optic system. The presence of oil is assessed on excitation–emission spectra obtained from spectral fluorescence signals of the sediment sample. A factory spectrofluorometer [...] Read more.
The aim of this study is to verify the possibility of detecting oil in the bottom sediment using a fibre optic system. The presence of oil is assessed on excitation–emission spectra obtained from spectral fluorescence signals of the sediment sample. A factory spectrofluorometer coupled with an experimental fibre optic measurement system was used. During the determination of spectra, the fibre optic system is set at a 45° angle to the sediment surface and placed above its surface. The light exciting the fluorescence and the light emitted by the sediment are transmitted in a combined bundle of fibre optic threads. The analysis of excitation–emission spectra of sediments contaminated with oil shows variability of the shapes of fluorescence spectra depending on the type and degree of oil contamination, which indicates the feasibility of the sensor design for detecting oil in the sediment in situ. Full article
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Figure 1
<p>An optical fibre used to detect oil in sediments: the outside connection with the spectrofluorometer (<b>a</b>); the front view of the optical fibre head (<b>b</b>).</p>
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<p>Excitation–emission fluorescence spectra of oil-free sediment (<b>a</b>) and the same sediment artificially polluted with two types of oil (<b>b</b>,<b>c</b>).</p>
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<p>Excitation-emission spectra (EEMs) of two types of oil (upper graphs) and spectra of oil-polluted sediment (the same as in <a href="#sensors-25-00173-f002" class="html-fig">Figure 2</a> but more polluted). The graphs on the left have the same scale relative to the HFO graph, those on the right to the crude oil graph. The cross in the graph (<b>f</b>) indicates the peak location.</p>
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<p>The height of the main fluorescence peaks for sediment artificially polluted with an oil of the chosen types: heavy fuel oil (HFO) (<b>a</b>), crude oil (<b>b</b>).</p>
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<p>Normalised EEM spectra for sediments polluted with two different oils at various oil concentrations, respectively: HFO 0.1% (<b>a</b>), HFO 1% (<b>b</b>), HFO 10% (<b>c</b>), crude oil 0.1% (<b>d</b>), crude oil 1% (<b>e</b>), and crude oil 10% (<b>f</b>). Normalisation was performed for both types of oil and each predetermined amount.</p>
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<p>A general scheme of the operation of an oil detector in seabed sediments.</p>
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17 pages, 5804 KiB  
Communication
Low-Coherence Integrated Optical Interferometer for Fibre Optic Sensors
by Petr Volkov, Alexander Bobrov, Oleg Vyazankin, Alexey Gorshkov, Alexander Goryunov, Glafira Lemeshevskaya, Andrey Lukyanov, Aleksey Nezhdanov, Daniil Semikov and Kirill Sidorenko
Sensors 2025, 25(1), 116; https://doi.org/10.3390/s25010116 - 27 Dec 2024
Viewed by 164
Abstract
This paper proposes and implements a novel scheme for recording signals from fibre optic sensors based on tandem low-coherence interferometry with an integrated optical reference interferometer. The circuit allows precision control of the phase shift. Additionally, the paper illustrates the potential for detecting [...] Read more.
This paper proposes and implements a novel scheme for recording signals from fibre optic sensors based on tandem low-coherence interferometry with an integrated optical reference interferometer. The circuit allows precision control of the phase shift. Additionally, the paper illustrates the potential for detecting vibration and object deformation using fibre optic Fabry–Perot sensors connected to the registration system. Full article
(This article belongs to the Section Optical Sensors)
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<p>Tandem low-coherence interferometry. SLD—superluminescent diode; Δ<sub>1</sub> and Δ<sub>2</sub>—optical arm length differences; PD—photodetector.</p>
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<p>The intensity at the output of TLCI.</p>
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<p>The scheme of the passive MZI.</p>
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<p>The scheme of the active MZI.</p>
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<p>Temperature distribution: cross section.</p>
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<p>Temperature distribution: along section.</p>
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<p>Temperature difference between hot and cold waveguides (100 um length) with a fixed heating power of 14 mW.</p>
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<p>Temperature difference between the hot and cold waveguides as a function of the power supplied to the heater for waveguides of different lengths.</p>
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<p>The photograph of an optical chip with integrated MZIs.</p>
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<p>Y-splitter.</p>
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<p>X-splitter.</p>
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<p>X-splitter splitting ratio.</p>
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<p>MZI transmission spectra for varied arm length differences.</p>
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<p>MZI transmission spectra shift due to temperature change.</p>
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<p>The relationship between the temperature of the heating element and the temperature value obtained from the shift of spectral bands.</p>
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<p>The optical power at the MZI output (heater length 60 microns) when the voltage applied to the heater changes.</p>
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<p>The optical power at the MZI output (heater length 140 microns) when the voltage applied to the heater changes.</p>
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<p>The time dynamic of the optical power at the MZI output while changing the voltage applied to the heater. The phase in the arms of the MZI was shifted from 0 to π.</p>
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<p>The scheme for vibration measurements.</p>
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<p>The scheme of the sensing interferometer.</p>
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<p>The scheme for acoustic modulator calibration. LD—laser diode.</p>
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<p>The signal recorded by the scheme from the vibrated mirror. (<b>A</b>) The blue line is the measured signal with the amplitude of the mirror as <math display="inline"><semantics> <mrow> <mo>±</mo> <mi>λ</mi> <mo>/</mo> <mn>8</mn> </mrow> </semantics></math>. (<b>B</b>) The orange line is the noise of the system in the case of the absence of mirror movement.</p>
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31 pages, 6215 KiB  
Review
Emerging Trends in the Integration of Smart Sensor Technologies in Structural Health Monitoring: A Contemporary Perspective
by Arvindan Sivasuriyan, Dhanasingh Sivalinga Vijayan, Parthiban Devarajan, Anna Stefańska, Saurav Dixit, Anna Podlasek, Wiktor Sitek and Eugeniusz Koda
Sensors 2024, 24(24), 8161; https://doi.org/10.3390/s24248161 - 21 Dec 2024
Viewed by 617
Abstract
In recent years, civil engineering has increasingly embraced communication tools for automation, with sensors playing a pivotal role, especially in structural health monitoring (SHM). These sensors enable precise data acquisition, measuring parameters like force, displacement, and temperature and transmit data for timely interventions [...] Read more.
In recent years, civil engineering has increasingly embraced communication tools for automation, with sensors playing a pivotal role, especially in structural health monitoring (SHM). These sensors enable precise data acquisition, measuring parameters like force, displacement, and temperature and transmit data for timely interventions to prevent failures. This approach reduces reliance on manual inspections, offering more accurate outcomes. This review explores various sensor technologies in SHM, such as piezoelectric, fibre optic, force, MEMS devices, GPS, LVDT, electromechanical impedance techniques, Doppler effect, and piezoceramic sensors, focusing on advancements from 2019 to 2024. A bibliometric analysis of 1468 research articles from WOS and Scopus databases shows a significant increase in publications, from 15 in 2019 to 359 in 2023 and 52 in 2024 (and still counting). This analysis identifies emerging trends and applications in smart sensor integration in civil and structural health monitoring, enhancing safety and efficiency in infrastructure management. Full article
(This article belongs to the Special Issue Recent Advances in Structural Health Monitoring and Damage Detection)
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<p>Depiction of the system setup and signal flow within the structural health monitoring (SHM) system. The components include PZT (lead zirconate titanate) sensors and a personal computer (PC). Adapted from Ref. [<a href="#B18-sensors-24-08161" class="html-bibr">18</a>].</p>
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<p>Sequence of SHM in multi-story buildings.</p>
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<p>Depiction of the sensors and communication in various industries.</p>
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<p>Illustration of the yearly scientific publications on integrating smart sensor technologies in SHM.</p>
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<p>An example of the most frequently referenced nations is an article on integrating smart sensor technologies in SHM.</p>
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<p>Illustration demonstrating the nation’s scientific output of papers on integrating smart sensor technologies in SHM.</p>
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<p>Illustration of the nations where the corresponding author researches integrating smart sensor technologies in SHM.</p>
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<p>An illustration of the key terms from the publications on integrating smart sensor technologies in SHM.</p>
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<p>An example of how frequently the most pertinent terms are used in publications about integrating smart sensor technologies in SHM.</p>
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<p>Illustration of the most pertinent keywords in bibliometric research on integrating smart sensor technologies in SHM.</p>
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<p>Fibre optic sensor for SHM application.</p>
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<p>Piezoceramic sensors in concrete.</p>
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<p>Force sensors and their components for SHM application.</p>
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<p>MEMS for acceleration monitoring.</p>
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<p>Concrete beam experiment using LVDT.</p>
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<p>EMI techniques to measure cracks in beams.</p>
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<p>Doppler effect techniques in SHM.</p>
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11 pages, 6054 KiB  
Article
A Novel Demodulation Algorithm for Micro-Displacement Measurement Based on FMCW Sinusoidal Modulation
by Zhen Xu, Yongjie Wang, Zhenqiang Li, Gaochao Li, Ke Li, Hongtao Zhang and Fang Li
Photonics 2024, 11(12), 1196; https://doi.org/10.3390/photonics11121196 - 20 Dec 2024
Viewed by 393
Abstract
Frequency-modulated continuous wave (FMCW) interferometry, an emerging laser interferometry technology, can be applied in the field of fibre-optic sensing to achieve high-precision micro-displacement measurements. To address nonlinearity issues in laser frequency modulation and localisation deviations of feature points in traditional algorithms, this paper [...] Read more.
Frequency-modulated continuous wave (FMCW) interferometry, an emerging laser interferometry technology, can be applied in the field of fibre-optic sensing to achieve high-precision micro-displacement measurements. To address nonlinearity issues in laser frequency modulation and localisation deviations of feature points in traditional algorithms, this paper proposes a demodulation algorithm suitable for sinusoidal frequency modulation schemes, incorporating the principle of orthogonal phase-locked amplification. The algorithm includes signal preprocessing, phase-locked amplification, error correction, and phase calculation. Experimental results show that the system achieves a measurement error standard deviation of 3.23 nanometres for static targets. The displacement measurement error at 100 μm is 0.057% F.S., and the linearity between the measured values and the actual displacement values is 0.99997. Compared with conventional methods, the approach introduced in this paper eliminates the need for separate nonlinear corrections of the current-to-optical frequency relationship and minimises the issue of feature point localization deviations, showing significant potential for practical applications. Full article
(This article belongs to the Special Issue Editorial Board Members’ Collection Series: Photonics Sensors)
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<p>Frequency relationship between the reference wave, signal wave, and beat signal during sinusoidal wave modulation.</p>
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<p>Waveforms of beat signals from a real optical sinusoidalwave FMCW interferometer.</p>
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<p>Signal processing flow, consisting of four parts: signal preprocessing, lock-in amplification, ellipse fitting and error correction, and phase calculation.</p>
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<p>Diagram of the displacement measurement system structure.</p>
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<p>Physical diagram of the displacement measurement system structure.</p>
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<p>Static displacement error test results: (<b>a</b>) scatter plot of error variation over time; (<b>b</b>) error distribution histogram.</p>
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<p>Displacement demodulation results for the displacement stage when the preset value is 100 μm on the basis of 40 measurements: (<b>a</b>) linear displacement; (<b>b</b>) error distribution.</p>
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<p>Results of 20 steps of 5 μm for the target: (<b>a</b>) relationship between measurement values and time during the stepping process; (<b>b</b>) linear fit between the measurement values of 20 steps and the actual displacement.</p>
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<p>Plots of uncorrected (<b>a</b>) and corrected (<b>b</b>) experimental datasets.</p>
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<p>(<b>a</b>) Distribution of static displacement errors within one hour; (<b>b</b>) relationship between static standard deviation and time.</p>
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15 pages, 5476 KiB  
Article
ZnO–Polyaniline Nanocomposite Functionalised with Laccase Enzymes for Electrochemical Detection of Cetyltrimethylammonuium Bromide (CTAB)
by Hilda Dinah Kyomuhimbo, Usisipho Feleni, Nils Hendrik Haneklaus and Hendrik Gideon Brink
J. Xenobiot. 2024, 14(4), 1988-2002; https://doi.org/10.3390/jox14040106 - 16 Dec 2024
Viewed by 491
Abstract
The direct discharge of cationic surfactants into environmental matrices has exponentially increased due to their wide application in many products. These compounds and their degraded products disrupt microbial dynamics, hinder plant survival, and affect human health. Therefore, there is an urgent need to [...] Read more.
The direct discharge of cationic surfactants into environmental matrices has exponentially increased due to their wide application in many products. These compounds and their degraded products disrupt microbial dynamics, hinder plant survival, and affect human health. Therefore, there is an urgent need to develop electroanalytical assessment techniques for their identification, determination, and monitoring. In our study, ZnO-PANI nanocomposites were electrodeposited on a glassy carbon electrode (GCE), followed by the immobilization of laccase enzymes and the electrodeposition of polypyrrole (PPy), to form a biosensor that was used for the detection of CTAB. A UV-Vis analysis showed bands corresponding to the π-π* transition of benzenoid and quinoid rings, π-polaron band transition and n-π*polaronic transitions associated with the extended coil chain conformation of PANI, and the presence and interaction of ZnO with PANI and type 3 copper in the laccase enzymes. The FTIR analysis exhibited peaks corresponding to N-H and C-N stretches and bends for amine, C=C stretches for conjugated alkenes, and a C-H bend for aromatic compounds. A high-resolution scanning electron microscopy (HRSEM) analysis proved that PANI and ZnO-PANI were deposited as fibres with hairy topography resulting from covalent bonding with the laccase enzymes. The modified electrode (PPy-6/GCE) was used as a platform for the detection of CTAB with three linear ranges of 0.5–100 µM, 200–500 µM, and 700–1900 µM. The sensor displayed a high sensitivity of 0.935 μA μM−1 cm−2, a detection limit of 0.0116 µM, and acceptable recoveries of 95.02% and 87.84% for tap water and wastewater, respectively. Full article
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Graphical abstract

Graphical abstract
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<p>A graph of (<b>A</b>) UV-Vis analysis and (<b>B</b>) Tauc plots for PANI and ZnO-PANI and PPy-Lac-ZnO-PANI composites.</p>
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<p>FTIR spectra for (<b>A</b>) PANI and (<b>B</b>) ZnO-PANI and (<b>C</b>) PPy-Lac-ZnO-PANI composites.</p>
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<p>SEM and EDS for (<b>A</b>,<b>B</b>) blank SPCE and (<b>C</b>,<b>D</b>) PANI-, (<b>E</b>,<b>F</b>) ZnO-PANI-, and (<b>G</b>,<b>H</b>) PPy-Lac-ZnO-PANI-modified SPCEs.</p>
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<p>Graphs showing electrochemical deposition of (<b>A</b>) PANI, (<b>B</b>) ZnO-PANI, and (<b>C</b>) PPy; (<b>D</b>,<b>E</b>) effect of ZnO loading on the conductivity of PANI; CV of (<b>F</b>) PANI and (<b>G</b>) ZnO-PANI at varying scan rates; and (<b>H</b>) Randles–Ševčík plot for PANI and ZnO-PANI composites.</p>
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<p>Cyclic voltammograms of different electrodes in the (<b>A</b>) absence and (<b>B</b>) presence of 20 µM CTAB in 0.1 M PBS. (<b>C</b>) A graph of electrode activity (peak current) at varying pH of the solution. (<b>D</b>) Effect of pH on conductivity of electrode and peak current vs. concentration of CTAB in 0.1 M PBS. (<b>E</b>) DPV of CTAB at different concentrations in PBS.</p>
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<p>(<b>A</b>) Cyclic voltammogram of PPy-Lac-ZnO-PANI/GCE electrode in 0.01 M ABTS in 0.1 M PBS and (<b>B</b>) Randles–Ševčík plot for PPy-Lac-ZnO-PANI/GCE in 0.01 M ABTS in 0.1 M PBS.</p>
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<p>Performance of the PPy/Lac-ZnO-PANI/GCE in presence of (<b>A</b>) interferants and (<b>B</b>) in real water samples and reusability of the biosensor in (<b>C</b>) PBS and (<b>D</b>) in tap water and wastewater.</p>
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<p>Performance of the PPy/Lac-ZnO-PANI/GCE in presence of (<b>A</b>) interferants and (<b>B</b>) in real water samples and reusability of the biosensor in (<b>C</b>) PBS and (<b>D</b>) in tap water and wastewater.</p>
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<p>Suggested mechanism for electrochemical oxidation of CTAB [<a href="#B70-jox-14-00106" class="html-bibr">70</a>,<a href="#B71-jox-14-00106" class="html-bibr">71</a>].</p>
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9 pages, 13511 KiB  
Communication
Polarization-Independent Focusing Vortex Beam Generation Based on Ultra-Thin Spiral Diffractive Lens on Fiber End-Facet
by Luping Wu, Zhiyong Bai, Rui Liu, Yuji Wang, Jian Yu, Jianjun Ran, Zikai Chen, Zilun Luo, Changrui Liao, Ying Wang, Jun He, George Y. Chen and Yiping Wang
Photonics 2024, 11(12), 1167; https://doi.org/10.3390/photonics11121167 - 11 Dec 2024
Viewed by 563
Abstract
An ultra-thin spiral diffractive lens (SDL) was fabricated by using focused ion beam milling on a fiber end-facet coated with a 100 nm thick Au film. Focusing vortex beams (FVBs) were successfully excited by the SDLs due to the coherent superposition of diffracted [...] Read more.
An ultra-thin spiral diffractive lens (SDL) was fabricated by using focused ion beam milling on a fiber end-facet coated with a 100 nm thick Au film. Focusing vortex beams (FVBs) were successfully excited by the SDLs due to the coherent superposition of diffracted waves and their azimuth dependence of the phase accumulated from the spiral aperture to the beam axis. The polarization and phase characteristics of the FVBs were experimentally investigated. Results show that the input beams with various polarization states were converted to FVBs, whose polarization states were the same as those of the input beams. Furthermore, the focal length of the SDL and the in-tensity and phase distribution at the focus spot of the FVBs were numerically simulated by the FDTD method in the ultra-wide near-infrared waveband from 1300 nm to 1800 nm. The focal length was tuned from 21.8 μm to 14.7 μm, the intensity profiles exhibited a doughnut-like shape, and the vortex phase was converted throughout the broadband range. The devices are expected to be candidates for widespread applications including optical communications, optical imaging, and optical tweezers. Full article
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<p>(<b>a</b>) The schematic diagram of SDL with <span class="html-italic">l</span> = 1; (<b>b</b>) simulated intensity distribution at the focal spot for <span class="html-italic">l</span> = 1; (<b>c</b>) the phase distribution at the focal spot for <span class="html-italic">l</span> = 1; (<b>d</b>) The schematic diagram of SDL with <span class="html-italic">l</span> = 2; (<b>e</b>) simulated intensity distribution at the focal spot for <span class="html-italic">l</span> = 2; (<b>f</b>) the phase distribution at the focal spot for <span class="html-italic">l</span> = 2.</p>
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<p>(<b>a</b>) Schematic diagram of the structure of the SDL fabricated on the multimode fiber end-facet; (<b>b</b>) calculation and experimental measurement of divergence angles <span class="html-italic">θ</span> of output beams from the GIF with different lengths; (<b>c</b>) intensity distribution of outputting beam from the GIF about 400 μm long.</p>
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<p>(<b>a</b>,<b>b</b>) SEM images of SDLs fabricated with <span class="html-italic">l</span> = 1 and 2 on the fiber end-facet, respectively; (<b>c</b>) schematic diagram of the measurement system to characterize the outputting beam; (<b>d</b>) measured intensity distribution at the focal spot for <span class="html-italic">l</span> = 1; (<b>e</b>) measured interference patterns between the focal spot and an extended Gaussian beam for <span class="html-italic">l</span> = 1; (<b>f</b>) measured intensity distribution at the focal spot for <span class="html-italic">l</span> = 2; (<b>g</b>) measured interference patterns between the focal spot and an extended Gaussian beam for <span class="html-italic">l</span> = 2.</p>
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<p>Measured intensity distribution and the interference patterns with different polarization state beams injected into the hybrid fiber. (<b>a</b>) <span class="html-italic">l</span> = 1; (<b>b</b>) <span class="html-italic">l</span> = 2.</p>
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<p>Simulated results for the focusing characteristics of the SDL with <span class="html-italic">l</span> = 2, under different wavelengths: (<b>a</b>) 1300 nm, (<b>b</b>) 1400 nm, (<b>c</b>) 1500 nm, (<b>d</b>) 1600 nm, (<b>e</b>) 1700, and (<b>f</b>) 1800 nm. The panels in the first two rows depict the phase distribution and intensity distribution at the focal spot, respectively; the panels in the bottom row illustrate the intensity distributions in the (<span class="html-italic">x</span>, <span class="html-italic">z</span>) plane.</p>
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14 pages, 4820 KiB  
Article
Digital Twin for a Frequency Mixer Used as a Phase Sensor
by Carlos Pires, Manuel Abreu, Isabel Godinho, Rui Agostinho and João A. Sousa
Sensors 2024, 24(23), 7574; https://doi.org/10.3390/s24237574 - 27 Nov 2024
Viewed by 483
Abstract
The Portuguese Institute for Quality is responsible for the realization and dissemination of the frequency standard in Portugal. There are several techniques for frequency transfer, but we use a frequency mixer to detect phase variations between two light signals with different wavelengths, traveling [...] Read more.
The Portuguese Institute for Quality is responsible for the realization and dissemination of the frequency standard in Portugal. There are several techniques for frequency transfer, but we use a frequency mixer to detect phase variations between two light signals with different wavelengths, traveling along an optical fibre. In this paper, we present the development of a digital twin (DT) that replicates the use of a frequency mixer to improve the frequency transfer problem. A setup was built to train and validate the technique: a frequency mixer was used to determine the phase difference between the two signals, which are caused by temperature gradients in the fibre, together with real-time temperature data from sensors placed along the fibre and on the mixer itself. The DT was trained with two machine learning algorithms, in particular, ARIMA and LSTM networks. To estimate the accuracy of the frequency mixer working as a phasemeter, several sources of uncertainty were considered and included in the DT model, with the goal of obtaining a phase value measurement and its uncertainty in real time. The JCGM 100:2008 and JCGM 101:2008 approaches were used for the estimation of the uncertainty budget. With this work, we merge DT technology with a frequency mixer used for phase detection to provide its value and uncertainty in real time. Full article
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<p>Representation of the physical system for phase measurement, which includes two lasers to transform the signal from UTC(IPQ) into light, two wavelength multiplexers (MUX and DMUX), two photodetectors to detect light, a frequency mixer, and a multimeter to measure voltage.</p>
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<p>Schema for the calculation of the theoretical phase and experimental phase.</p>
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<p>(<b>a</b>) Voltage values on the left axis and temperature values on the right axis. (<b>b</b>) Experimental and theoretical phase values on the left axis and temperature of the lasers, optical fibre, detectors, and mixer on the right axis.</p>
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<p>Determination of uncertainty budget using Ishikawa diagram.</p>
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<p>Chart of the comparison of uncertainty distribution. In blue is the Monte Carlo approach and in red is the GUM approach.</p>
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<p>Chart of measured phase values, modelled values, and estimated values (digital twin) using a NN.</p>
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<p>Chart for measured phase values, modelled values, and estimated values (digital twin) using LSTM network.</p>
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<p>Schema for the digital twin.</p>
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<p>Five-day sequence of measurement data.</p>
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<p>Trained model applied to theoretical data.</p>
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<p>Trained model applied to experimental data.</p>
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16 pages, 5102 KiB  
Article
Machine Learning-Based Structural Health Monitoring Technique for Crack Detection and Localisation Using Bluetooth Strain Gauge Sensor Network
by Tahereh Shah Mansouri, Gennady Lubarsky, Dewar Finlay and James McLaughlin
J. Sens. Actuator Netw. 2024, 13(6), 79; https://doi.org/10.3390/jsan13060079 - 23 Nov 2024
Viewed by 1126
Abstract
Within the domain of Structural Health Monitoring (SHM), conventional approaches generally are complicated, destructive, and time-consuming. It also necessitates an extensive array of sensors to effectively evaluate and monitor the structural integrity. In this research work, we present a novel, non-destructive SHM framework [...] Read more.
Within the domain of Structural Health Monitoring (SHM), conventional approaches generally are complicated, destructive, and time-consuming. It also necessitates an extensive array of sensors to effectively evaluate and monitor the structural integrity. In this research work, we present a novel, non-destructive SHM framework based on machine learning (ML) for the accurate detection and localisation of structural cracks. This approach leverages a minimal number of strain gauge sensors linked via Bluetooth Low Energy (BLE) communication. The framework is validated through empirical data collected from 3D carbon fibre-reinforced composites, including three distinct specimens, ranging from crack-free samples to specimens with up to ten cracks of varying lengths and depths. The methodology integrates an analytical examination of the Shewhart chart, Grubbs’ test (GT), and hierarchical clustering (HC) algorithm, tailored towards the metrics of fracture measurement and classification. Our novel ML framework allows one to replace exhausting laboratory procedures with a modern and quick mechanism for the material, with unprecedented properties that could provide potential applications in the composites industry. Full article
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<p>(<b>a</b>) Ss sample cut from 3D layer-to-layer composite material and its developed length crack (red arrows show increasing cracks)—lift and drag force’s position on hydrofoil is shown in upper-right. (<b>b</b>) Schematic of the three-specimen geometry and a crack position. (<b>c</b>) Load configuration during the experiment. Please note the crack location identified via defined algorithms in framework in next sections.</p>
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<p>(<b>a</b>) Removable electronic enclosure attaches to the strain gauge electrodes using a holder permanently fixed on the sample surface. The node can be moved to a new location. (<b>b</b>,<b>c</b>) The enclosure accommodates a wireless module (BLE), a coin cell battery, supporting electronics, and a spring-loaded connector. (<b>d</b>) Spring-loaded interconnecting header in contact with copper pads deposited on the sample surface and connected to the strain gauge sensor. (<b>e</b>) Electronic module that accommodates BLE sensors, compared with a pen to evaluate the size. (<b>f</b>) The front side of the bridging board has four resistors. It is a connector between the strain gauge sensors and the transmitting board.</p>
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<p>(<b>a</b>) Measured strain vs. sensor number when crack developed through Bs—Figure illustrates the sensor outputs for various experimental configurations labelled as Exp 1–9. These configurations correspond to specific load conditions and crack positions as follows: Exp 1 represents a scenario with minimal strain applied, Exp 2–4 involve moderate strain with an incipient crack in both sides, Exp 5–8 indicate higher strain with multiple surface cracks, and Exp 9 denotes maximum load conditions under which significant crack propagation was observed after 48 h. Each experiment’s unique setup is detailed to provide insights into the strain responses across varying crack severities. (<b>b</b>) The average value of each BLE sensor when cracks developed through Bs [equivalent experiment shown in (<b>a</b>)].</p>
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<p>Machine learning-based SHM framework.</p>
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<p>(<b>a</b>) Comparing five sensors’ outputs for Ss before crack development (sensors under load but in normal phase). (<b>b</b>) Anomalous sensors after crack development through Ss. (<b>c</b>,<b>d</b>) Comparing five sensor outputs for Rs before and after crack development, respectively. As discussed above, a sensor close to cracks usually appears out of UCL/LCL interval.</p>
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<p>A dendrogram of six initial surface cracks (<b>left</b>), and equivalent Venn diagram (<b>right</b>). The dendrogram shows classificatory relationships between samples. The height of links increases when there is a progression in crack depth.</p>
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<p>(<b>a</b>) Normal probability plot of developed cracks for Rs before GT application. (<b>b</b>,<b>c</b>) The same samples after applying GT threshold (α); (0.05 % and 10%) with 90% and 99.5 % confidence, respectively. Please note: GT applied on two other forms of samples and similar results achieved.</p>
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<p>Probability density belonging to sensor 3 (square) on the left, and sensor 2 (rectangle) on the right, before and after crack development. For square, the process shift (<math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">Δ</mi> </mrow> </semantics></math>) is positive, while the rectangle shows negative variance. This is because the IoT sensors were located on the surface of the square, while the same sensors were located beneath the surface for the rectangle specimen, resulting in negative recordings.</p>
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<p>Probability Density Function (PDF) of the prediction error for R, S, and B samples. The bars represent cracks within each sample, and the curve shows PDF prediction. A better Shewhart accuracy in predicting the crack location is indicated by greater coverage of the bars by the curve.</p>
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<p>(<b>a</b>) The difference between link height for ‘ss’ using HC algorithm during crack growth. (<b>b</b>) Repetition of exp a. for ‘rs’. (<b>c</b>) Blue line shows a polynomial model adjusted to the cluster link using ‘ss’ with R<sup>2</sup> = %97 to evaluate the prediction accuracy. Each dot represents a link between developed cracks, and all can be located within 99% of prediction bounds. (<b>d</b>) Repetition of exp c. for ‘bs’ and ‘rs’. R<sup>2</sup> = %91 for prediction bounds of 95%.</p>
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<p>(<b>a</b>) Applying G-test with <math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math> = 0.5. on anomalous sensors of three different shape specimens (specimen 1: square, specimen 2: rectangle, and specimen 3: beam). Selected <math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math> will define one outlier for specimens 2 and 3 and null for specimen 1. (<b>b</b>) Equivalent experiment with <math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math> = 10; here, five outliers (shown inside the red circle) were selected via G-test from various specimens.</p>
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18 pages, 2283 KiB  
Article
Respiratory Rate Monitoring via a Fibre Bragg Grating-Embedded Respirator Mask with a Wearable Miniature Interrogator
by Nat Limweshasin, Itzel Avila Castro, Serhiy Korposh, Stephen P. Morgan, Barrie R. Hayes-Gill, Mark A. Faghy and Ricardo Correia
Sensors 2024, 24(23), 7476; https://doi.org/10.3390/s24237476 - 23 Nov 2024
Viewed by 515
Abstract
A respiration rate (RR) monitoring system was created by integrating a Fibre Bragg Grating (FBG) optical fibre sensor into a respirator mask. The system exploits the sensitivity of an FBG to temperature to identify an individual’s RR by measuring airflow temperature variation near [...] Read more.
A respiration rate (RR) monitoring system was created by integrating a Fibre Bragg Grating (FBG) optical fibre sensor into a respirator mask. The system exploits the sensitivity of an FBG to temperature to identify an individual’s RR by measuring airflow temperature variation near the nostrils and mouth. To monitor the FBG response, a portable, battery-powered, wireless miniature interrogator system was developed to replace a relatively bulky benchtop interrogator used in previous studies. A healthy volunteer study was conducted to evaluate the performance of the developed system (10 healthy volunteers). Volunteers were asked to perform normal breathing whilst simultaneously wearing the system and a reference spirometer for 120 s. Individual breaths are then identified using a peak detection algorithm. The result showed that the number of breaths detected by both devices matched exactly (100%) across all volunteer trials. Full article
(This article belongs to the Section Biosensors)
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<p>Dimension of employed respirator mask (head strap removed).</p>
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<p>Side view illustration of overall design of respirator mask after FBG placements perpendicular to breath airflow direction; sub-panel shows a magnified sketch (not to scale) at the respirator mask airway and cross-sectional diagram of FBG grating elements along with inhalation and exhalation airflow directions.</p>
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<p>System diagram of the mini-interrogator operation with WebSocket protocol.</p>
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<p>FiSpecX100 instrumentation flow chart, including ESP32, UART protocol, and parsing of FBG data/wavelength shift values.</p>
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<p>Mask System setup during volunteer study (note: FBG placement on respirator mask is as shown in <a href="#sensors-24-07476-f002" class="html-fig">Figure 2</a>; head strap included in this figure).</p>
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<p>FBG respirator mask and reference spirometer setup during volunteer experiments (sub-panel shows a photo of FBG placement in the respirator mask airway, taken from the inside of the respirator mask after spirometer attachment).</p>
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<p>Examples of data from a volunteer (<b>top</b> panel = Mask System raw data, <b>bottom</b> panel = reference spirometer data).</p>
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<p>Mask System data when placed on benchtop at experiment venue; (<b>a</b>) time domain where the X-axis is labelled as data samples and acquisition rate; (<b>b</b>) frequency domain (note: sub-panel in (<b>b</b>) shows magnification of data at 0–1 Hz).</p>
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<p>Inverted and filtered Mask System data peak detection (sub-panel shows magnification of data at the double peak).</p>
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<p>Example comparison between processed Mask System and reference spirometer normalised data and peak detection (note: the result of reference spirometer data manual breath count is shown as the peaks of the signal labelled as “Reference Spirometer Peaks”).</p>
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12 pages, 3959 KiB  
Communication
Deep Integration Between Polarimetric Forward-Transmission Fiber-Optic Communication and Distributed Sensing Systems
by George Y. Chen, Ming Chen, Xing Rao, Shangwei Dai, Runlong Zhu, Guoqiang Liu, Junhong Lu, Hanjie Liu and Yiping Wang
Sensors 2024, 24(21), 6778; https://doi.org/10.3390/s24216778 - 22 Oct 2024
Viewed by 877
Abstract
The structural health of fiber-optic communication networks has become increasingly important due to their widespread deployment and reliance in interconnected cities. We demonstrate a smart upgrade of a communication system employing a dual-polarization-state polarization shift keying (2-PolSK) modulation format to enable distributed vibration [...] Read more.
The structural health of fiber-optic communication networks has become increasingly important due to their widespread deployment and reliance in interconnected cities. We demonstrate a smart upgrade of a communication system employing a dual-polarization-state polarization shift keying (2-PolSK) modulation format to enable distributed vibration monitoring. Sensing can be conducted without hardware changes or occupying additional communication bandwidth. Experimental results demonstrate that forward transmission-based distributed vibration sensing can coexist with PolSK data transmission without significant deterioration in performance. This proof-of-concept study achieved a sensitivity of 0.4141 μV/με with a limit of detection (LoD) of 563 pε/Hz1/2@100 Hz. The single-span sensing distance can reach up to 121 km (no optical amplification) with a positioning accuracy as small as 874 m. The transmission rate is 300 Mb/s, the QdB is 16.78 dB, and the corresponding BER is 5.202 × 10−12. For demonstration purposes, the tested vibration frequency range is between 100 and 200 Hz. Full article
(This article belongs to the Special Issue Distributed Sensors: Development and Applications)
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<p>Concept of PolSK communication and sensing deep integration. (<b>a</b>) PolSK transmitter module; (<b>b</b>) optical transmission with vibration influence; (<b>c</b>) PolSK receiver module. AM: amplitude modulator; PBS: polarization beam splitter; PBC: polarization beam combiner; PD: photodetector.</p>
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<p>Schematic of the integrated system. PC: polarization controller; EOM: electro-optic modulator; OC: optical coupler; Cir: circulator; SMF: single-mode fiber; BPD: balanced photodetector.</p>
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<p>Relationship between applied strain and differential voltage.</p>
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<p>Single-point vibration positioning processing sequence. (<b>a</b>) Differential voltage signal; (<b>b</b>) cross-correlation results, red square: indicates area for magnification; (<b>c</b>) local magnification around the highest peak; (<b>d</b>) corresponding vibration position. The PZT was driven with a 200 Hz sinusoidal signal.</p>
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<p>Multi-point vibration positioning processing sequence. (<b>a</b>) Differential voltage signal; (<b>b</b>) time-delay spectrum showing corresponding positions associated with signal frequencies (identified from amplitude spectrum); (<b>c</b>) 3D relationship between vibration position, frequency, and amplitude.</p>
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<p>Vibration positioning accuracy from 100 repeated measurements. Inset: histogram of the positioning results with a Gaussian fitting.</p>
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<p>PolSK communication bit recovery under the influence of vibrations. (<b>a</b>) BPD1 signal (01011 sequence); (<b>b</b>) BPD2 signal (10100 sequence). Red line: recovery of original communication signal; blue line: BPD signal; black dashed line: decision threshold.</p>
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<p>Eye diagram of PolSK communication–sensing system under the influence of vibrations.</p>
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<p>Communication–sensing crosstalk analysis. (<b>a</b>) No data transmission and vibration; (<b>b</b>) data transmission only; (<b>c</b>) vibration only; (<b>d</b>) data transmission with vibration. The vibration amplitude applied was 26.7 με. Red line: minimum to maximum value.</p>
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19 pages, 51632 KiB  
Article
Three-Dimensional Printing Limitations of Polymers Reinforced with Continuous Stainless Steel Fibres and Curvature Stiffness
by Alison J. Clarke, Andrew N. Dickson, Vladimir Milosavljević and Denis P. Dowling
J. Compos. Sci. 2024, 8(10), 410; https://doi.org/10.3390/jcs8100410 - 6 Oct 2024
Viewed by 1183
Abstract
This study investigates the printability limitations of 3D-printed continuous 316L stainless steel fibre-reinforced polymer composites obtained using the Materials Extrusion (MEX) technique. The objective was to better understand the geometric printing limitations of composites fabricated using continuous steel fibres, based on a combination [...] Read more.
This study investigates the printability limitations of 3D-printed continuous 316L stainless steel fibre-reinforced polymer composites obtained using the Materials Extrusion (MEX) technique. The objective was to better understand the geometric printing limitations of composites fabricated using continuous steel fibres, based on a combination of bending stiffness testing and piezoresistive property studies. The 0.5 mm composite filaments used in this study were obtained by co-extruding polylactic acid (PLA), with a 316 L stainless steel fibre (SSF) bundle. The composite printability limitations were evaluated by the printing of a series of ’teardrop’ shaped geometries with angles in the range from 5° to 90° and radii between 2 and 20 mm. The morphology and dimensional measurements of the resulting PLA-SSF prints were evaluated using μCT scanning, optical microscopy, and calliper measurements. Sample sets were compared and statistically examined to evaluate the repeatability, turning ability, and geometrical print limitations, along with dimensional fluctuations between designed and as-printed structures. Comparisons of the curvature bending stiffness were made with the PLA-only polymer and with 3D-printed nylon-reinforced short and long carbon fibre composites. It was demonstrated that the stainless steel composites exhibited an increase in bending stiffness at smaller radii. The change in piezoresistance response of the PLA-SSF with load applied during the curvature bending stiffness testing demonstrated that the 3D-printed composites may have the potential for use as structural health monitoring sensors. Full article
(This article belongs to the Special Issue Polymer Composites and Fibers, 3rd Edition)
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<p>Teardrop geometry designs investigated.</p>
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<p>Teardrop plan and elevation CAD designs, including geometry dimensions with an angle of 70° and a 15 mm radius.</p>
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<p>(<b>a</b>) The piezoresistive response of a PLA-SSF filament attached to a plastic moving between straight or bent configuration; (<b>b</b>) schematic of the curvature bend test testing jig; and (<b>c</b>) photograph the curvature bend test equipment during composite sample testing.</p>
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<p>Three-dimensional printed PLA-SSF composites: (<b>a</b>) teardrop geometries investigated along with the (<b>b</b>) curvature bend test semi-circle samples.</p>
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<p>Planer CT scans of the middle sections of PLA-SSF teardrop geometries: (<b>a</b>) 20° angle with a radius of 4 mm and (<b>b</b>) 70° with a radius of 15 mm. Note the differences in the scale bars for the two scan images.</p>
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<p>Close up view of the apex angle section illustrating cornering material deposition: (<b>a</b>) 20° and a radius of 4 mm; (<b>b</b>) 70° and a radius of 15 mm; and (<b>c</b>) differences between the design dimensions and as-printed geometries obtained at the teardrop apex for prints with angles from 5° to 90°.</p>
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<p>Radius dimensions of teardrop geometries: (<b>a</b>) teardrop with a 20° angle and radius of 4 mm; (<b>b</b>) teardrop with a 70° angle and radius of 15 mm; and (<b>c</b>) average wall width around semi-circular sections.</p>
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<p>Overview of the difference between the design and as-printed dimensional results: (<b>a</b>) dimensional evaluation between the difference between the estimated marginal mean dimensions vs. the design dimensions; and (<b>b</b>) average resulting internal lengths.</p>
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<p>Curvature bending stiffness (CBS) (<b>a</b>) results for the printed materials shown. Note that the CBS testing was carried out using two test rigs (depending on the composite geometry), as described in <a href="#sec2dot4-jcs-08-00410" class="html-sec">Section 2.4</a>; (<b>b</b>) PLA-SSF CBS samples cross section; and (<b>c</b>) Onyx-cCF CBS samples cross section.</p>
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<p>Curvature bending stiffness testing force against resistance for semi-circle sample set with a radius of 10 mm (seven specimens).</p>
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9 pages, 3152 KiB  
Article
Fibre Refractometry for Minimally Invasive Sugar Content Measurements within Produce
by Mark A. Zentile, Peter Offermans, David Young and Xu U. Zhang
Sensors 2024, 24(19), 6336; https://doi.org/10.3390/s24196336 - 30 Sep 2024
Viewed by 964
Abstract
A minimally invasive needle refractometer is presented for sugar content measurements within produce. A passive sampling cap structure was developed that improves the reliability of the device by avoiding interfering back reflections from the flesh of the produce. It is explained that factory [...] Read more.
A minimally invasive needle refractometer is presented for sugar content measurements within produce. A passive sampling cap structure was developed that improves the reliability of the device by avoiding interfering back reflections from the flesh of the produce. It is explained that factory calibration may not be needed for this type of refractometer, potentially reducing production costs. Also demonstrated is an iterative method to correct for temperature variations without the need for an integrated model for how the refractive index changes with temperature for different levels of sugar concentration. The sensor showed a typical standard deviation of 0.4 °Bx for a 10-s-long measurement and was validated against a prism refractometer, showing an average offset of (0.0±0.1) °Bx. In addition, the potential for using the device to investigate sugar distributions within a single fruit sample is demonstrated. Full article
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<p>The schematic and design of the experimental apparatus. (<b>a</b>) The schematic of the sensing system. A laser launches light into a single-mode optical fibre. The laser intensity is modulated with a sine wave generator. A fibre circulator directs the light to the needle probe, and reflected light is directed by the circulator to a photodetector. (<b>b</b>) A rendering of the probe cap design. (<b>c</b>) A cutout rendering showing the location of the needle probe when mounted in the cap. (<b>d</b>) A photo of the needle probe within the probe cap after insertion into a sample fruit.</p>
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<p>Soluble solid content derived from fibre-based refractive index measurements over time whilst varying the sample temperature. The dashed purple lines show the sample temperature. The solid green lines give the results when using only Equation (<a href="#FD4-sensors-24-06336" class="html-disp-formula">4</a>), while the solid dark blue line is the result of applying the iterative temperature correction method. The top panel shows the results for a 15.1 °Bx solution, while the bottom panel shows the results for pure water. The data presented in this figure are available in the <a href="#app1-sensors-24-06336" class="html-app">Supplementary Material</a>.</p>
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<p>(<b>Top panel</b>) Plotted are the SSCs of whole fruit samples measured by the fibre refractometer against measurements by a prism refractometer. (<b>Bottom panel</b>) Fibre refractometer response minus the reference prism refractometer plotted against the prism refractometer response. In both panels, the green points, red squares and blue crosses correspond to green grapes, strawberries and blueberries, respectively. The dashed blue line is the line of equivalence. The data presented in this figure are available in the <a href="#app1-sensors-24-06336" class="html-app">Supplementary Material</a>.</p>
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<p>A photograph of a strawberry segment after measurement with the fibre refractometer at five locations. After measurement, the probe cap was left in the fruit to show the location of the measurement. The overlaid numbers are the measured SSC values in °Bx.</p>
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17 pages, 10452 KiB  
Article
Experimental Study of Sinkhole Propagation Induced by a Leaking Pipe Using Fibre Bragg Grating Sensors
by Josué Yumba, Maria Ferentinou and Michael Grobler
Sensors 2024, 24(19), 6215; https://doi.org/10.3390/s24196215 - 25 Sep 2024
Cited by 1 | Viewed by 1097
Abstract
Sinkhole formation caused by leaking pipes in karst soluble rocks is a significant concern, leading to infrastructure damage and safety risks. In this paper, an experiment was conducted to investigate sinkhole formation in dense sand induced by a leaking pipe. Fibre Bragg grating [...] Read more.
Sinkhole formation caused by leaking pipes in karst soluble rocks is a significant concern, leading to infrastructure damage and safety risks. In this paper, an experiment was conducted to investigate sinkhole formation in dense sand induced by a leaking pipe. Fibre Bragg grating (FBG) sensors were used to record the strain. A balloon was gradually deflated within a bed of wet silica sand to create an underground cavity. Eighteen FBG sensors, with a wavelength range between 1550 nm and 1560 nm, were embedded horizontally and vertically in the physical model at different levels to monitor deformation at various locations. A leaking pipe was installed to induce the collapse of the formed arch above the cavity. The strain measurements suggested the following four phases in the sinkhole formation process: (1) cavity formation, (2) progressive weathering and erosion, (3) catastrophic collapse, and (4) subsequent equilibrium conditions. The results showed differences in the strain signatures and distributions between the horizontal and vertical measurements. During the critical phase of the sinkhole collapse, the horizontal measurements primarily showed tension, while the vertical measurements indicated compression. This investigation demonstrates the effectiveness of FBGs as advanced monitoring tools for sinkhole precursor identification. The study also suggests using FBGs in geotechnical monitoring applications to improve the understanding and mitigation of sinkholes and related geohazards. Full article
(This article belongs to the Special Issue Optical Fiber Sensors Used for Civil Engineering)
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<p>Depiction of a single-mode optical fibre.</p>
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<p>Working principle of an FBG sensor.</p>
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<p>Model preparation: (<b>a</b>) Isolation of temperature cable with three printed FBGs and T1, T2, T3 in red show the locations of temperature sensors isolation tube, (<b>b</b>) vertical support design of the optical fibre sensors mounted in the modelling box with S1, S2, S3 in red show the locations of the strain sensors, and (<b>c</b>) container with optical fibre sensors mounted.</p>
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<p>Horizontal and vertical positions of FBG sensors in the sinkhole model. The green-dotted layers represent the dyed soil, visually illustrating the collapse pattern. ’H’ with a number indicates the horizontal positioning of a specific FBG sensor, while ’V’ with a number denotes the vertical placement of the sensor.</p>
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<p>Experimental setup consisting of water supply system, physical small-scale model of the sinkhole, and data acquisition system.</p>
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<p>Development of the sinkhole: (<b>a</b>) The balloon is inflated with water to create a cavity in the soil mass. (<b>b</b>) The ballon is deflated, and the cavity is created. (<b>c</b>) Water leaks into the soil mass to induce the collapse and form the sinkhole. (<b>d</b>) The sinkhole develops and is propagated upward toward the ground surface.</p>
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<p>The horizontal strain was measured in different layers by three optic fibre sensor cables: (<b>a</b>) Strain induced by leaking water, (<b>b</b>) optic fibre cable 1, (<b>c</b>) optic fibre cable 2, and (<b>d</b>) optic fibre cable 3.</p>
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<p>Horizontal strain variation during the four identified phases in the failure process of the sinkhole: (<b>a</b>) Cavity formation process, (<b>b</b>) weathering or erosion process, (<b>c</b>) collapsing process, and (<b>d</b>) equilibrium process.</p>
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<p>Vertical strains were measured in different layers by the three optic fibre sensor cables: (<b>a</b>) Strain induced by leaking water, (<b>b</b>) optic fibre cable 1, (<b>c</b>) optic fibre cable 2, and (<b>d</b>) optic fibre cable 3.</p>
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<p>Vertical strains were measured in different layers by the three optic fibre sensor cables: (<b>a</b>) Strain induced by leaking water, (<b>b</b>) optic fibre cable 1, (<b>c</b>) optic fibre cable 2, and (<b>d</b>) optic fibre cable 3.</p>
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<p>Vertical strain variation during the four identified phases in the failure process of a sinkhole, (<b>a</b>) cavity formation process, (<b>b</b>) weathering or erosion process, (<b>c</b>) collapsing process, and (<b>d</b>) equilibrium process.</p>
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<p>Vertical strain variation during the four identified phases in the failure process of a sinkhole, (<b>a</b>) cavity formation process, (<b>b</b>) weathering or erosion process, (<b>c</b>) collapsing process, and (<b>d</b>) equilibrium process.</p>
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30 pages, 3954 KiB  
Article
Investigation of the Robust Integration of Distributed Fibre Optic Sensors in Structural Concrete Components
by Johannes Wimmer and Thomas Braml
Sensors 2024, 24(18), 6122; https://doi.org/10.3390/s24186122 - 22 Sep 2024
Viewed by 1037
Abstract
In recent times, the value of data has grown. This tendency is also observeable in the construction industry, where research and digitalisation are increasingly oriented towards the collection, processing and analysis of different types of data. In addition to planning data, measurement data [...] Read more.
In recent times, the value of data has grown. This tendency is also observeable in the construction industry, where research and digitalisation are increasingly oriented towards the collection, processing and analysis of different types of data. In addition to planning data, measurement data is a main focus. fibre optic measurements offer a highly precise and comprehensive approach to data collection. It is, however, important to note that this technology is still in research regarding concrete structures. This paper presents two methods of integrating filigree sensors into concrete structures. The first approach entails wrapping a fibre around a tendon duct and analysing the installation and associated measurements. The second method involves bonding polyimide and acrylate-coated fibres with 2K epoxy and cyanoacrylate in the grooves of rebars, exposing them to chemical environments. The resulting measurement data is evaluated qualitatively and quantitatively to ascertain its resilience to environmental factors. These developed criteria are consolidated in a decision matrix. Fibre-adhesive combinations necessitate protection from chemical and mechanical influences. The limitations of the solutions are pointed out, and alternative options are proposed. Full article
(This article belongs to the Special Issue Sensor-Based Structural Health Monitoring of Civil Infrastructure)
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<p>Components and influences on a DFOS sensor configuration.</p>
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<p>Fibre types, sketches and pictures. (<b>a</b>) Acrylate coated fibre. (<b>b</b>) Polyimide coated fibre. (<b>c</b>) Polyamide fibre optic cable [<a href="#B6-sensors-24-06122" class="html-bibr">6</a>].</p>
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<p>Different cable and fibre types in a reinforcement cage.</p>
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<p>Prestressed concrete beam, principle sketch of centric (blue, <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mi mathvariant="normal">e</mi> <mo>=</mo> <mn>0</mn> </mrow> </msub> </semantics></math>) and excentric (red, <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mi mathvariant="normal">e</mi> <mspace width="4.pt"/> <mo>≠</mo> <mspace width="4.pt"/> <mn>0</mn> </mrow> </msub> </semantics></math>).</p>
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<p>Methods of fibre attachment onto ducts: (<b>a</b>) Longitudinal direction (fibre marked by blue arrows), (<b>b</b>) Along the coil (marked by yellow arrows), (<b>c</b>) Sketches in view and longitudinal section with blue longitudinal fibre and yellow coil fibre, drawing by [<a href="#B38-sensors-24-06122" class="html-bibr">38</a>].</p>
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<p>Experimental setup: (<b>a</b>) Fixed specimen, (<b>b</b>) Load curve of test.</p>
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<p>Steps of data processing (<b>a</b>) Raw data, (<b>b</b>) Cleaned data, (<b>c</b>) Smoothed data.</p>
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<p>(<b>a</b>) Overview of the specimens configurations, (<b>b</b>) Structure of the prepared rebar.</p>
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<p>Experimental setup of rebar tensile tests (<b>a</b>) Fixed specimen, (<b>b</b>) Load curve of test, (<b>c</b>) Specimen in Zwick Z400 with measurement marks for RTSS.</p>
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<p>Steps of data processings (<b>a</b>) Raw data, (<b>b</b>) Cut out segment of interest, (<b>c</b>) Cut out period of interest, (<b>d</b>) Strain over time for one single gauge (raw and smoothed data), (<b>e</b>) Strain at the length of sensor at a single timestamp (raw and smoothed data).</p>
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<p>Comparison of strain and smoothed strain over time at a specific gauge and force and smoothed force over time in a specimen.</p>
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<p>Categories of measurement results.</p>
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<p>Qualitative results of the tensile tests T01 and T02, arranged by category and sensor configuration.</p>
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<p>Classification of measurement curves of raw data and smoothed data (<b>a</b>) linear regression with raw data, (<b>b</b>) linear regression with smoothed data, (<b>c</b>) polynomial regression with raw data, (<b>d</b>) polynomial regression with smoothed data.</p>
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<p>Classification of the smoothed measurement curves into the best fitting regression curve for the three test series.</p>
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<p>Strain ranges of the specimens for the three test series.</p>
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<p>(<b>a</b>): Mean strain differences ΔØ(T01−T02) for smoothed data, (<b>b</b>): Mean strains of T01 measurements.</p>
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<p>Relative standard deviations over time of the curves from linear regression.</p>
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<p>(<b>a</b>) Visualisation of the <math display="inline"><semantics> <msup> <mi mathvariant="normal">R</mi> <mn>2</mn> </msup> </semantics></math> vectors in space, (<b>b</b>) Euclidean distances of the <math display="inline"><semantics> <msup> <mi mathvariant="normal">R</mi> <mn>2</mn> </msup> </semantics></math> vectors to T01 with the marked WLacrEP03 (grey circle, dotted) and LLacrCA03 (red circle, full).</p>
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<p>Exemplary regression curves of two specimens (<b>a</b>) LLacrCA03, (<b>b</b>) WLacrEP03.</p>
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<p>Difference of absolute strain range—mean strain range of specimen for the three test series.</p>
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23 pages, 7922 KiB  
Article
Development of Miniaturised Fibre-Optic Laser Doppler Velocimetry for Opaque Liquid: Measurement of the Velocity Profile in the Engine Oil Flow of a Lubrication System
by Tsutomu Tajikawa, Shimpei Kohri, Taiki Mouri, Takaichi Fujimi, Hiromasa Yamaguchi and Kenkichi Ohba
Photonics 2024, 11(9), 892; https://doi.org/10.3390/photonics11090892 - 22 Sep 2024
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Abstract
This study developed a fibre-optic laser Doppler velocimetry sensor for use in opaque, high-temperature, and high-pressure fluid flows by inserting the fibre perpendicular to the main flow. The tip of the optical fibre was obliquely polished and chemically etched using a buffered hydrofluoric [...] Read more.
This study developed a fibre-optic laser Doppler velocimetry sensor for use in opaque, high-temperature, and high-pressure fluid flows by inserting the fibre perpendicular to the main flow. The tip of the optical fibre was obliquely polished and chemically etched using a buffered hydrofluoric acid solution, and a reflective mirror was deposited on the surface of the oblique fibre tip. Based on the results of the verification test using the rotating annular open channel, the fabrication conditions of the fibre tip were optimized for measuring the lubricating oil flow. The flow velocity profiles in the engine’s oil flow of the lubrication system during engine bench testing were measured. These velocity profiles were influenced by variations in the measurement position, oil temperature, and engine speed. The measurement accuracy of this sensor was compared with the volumetric flow rate obtained by cross-sectional area integration of the flow velocity profile, as measured using a Coriolis flowmeter, and the difference was within 1%. By combining computational simulation for flow and optical attenuation and particle scattering in light transmission through a working fluid, this fibre-optic sensor achieved a measurement volume of 200 microns in length and 200 microns in width at a distance of 900–1000 microns from the sensor. Full article
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Figure 1

Figure 1
<p>Design and fabrication processes for the normally inserted FO-LDV sensor. (<b>a</b>) Schematic of the FO-LDV sensor designed for normal insertion against the main flow and the fibre tip traverser for measuring the flow velocity profile. (<b>b</b>) Schematic of the oblique polishing process. The optical fibre and its holder for the stiffening of the fibre are shown in sectional views. (<b>c</b>) Schematic of the chemical etching process. (<b>d</b>) The process of forming the reflection mirror utilised direct current (DC) sputtering. By employing a mask tube, the aluminium mirror was formed on the surface of the fibre’s end.</p>
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<p>Outline of the verification and validation testing for the prototyped FO-LDV sensor. (<b>a</b>) Validation test setup using a rotating annular open channel and the optical system. By rotating the channel filled with the working fluid at a constant speed of revolution, a uniform flow velocity was generated, as calculated from both the rotating radius and the speed of revolution. (<b>b</b>) Examples of working fluids: unused lubricating oil (left) and deteriorated oil with MoS<sub>2</sub> powder after engine bench testing. (<b>c</b>) Overview of the lubricating flow system of the engine bench test and the verification test for the FO-LDV. (<b>d</b>) Measurement location of flow during the engine bench test. (<b>e</b>) The definition of the coordinate system for measurement of the velocity profile.</p>
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<p>Results of FO-LDV prototyping. (<b>a</b>) Examples of the obliquely cut fibre tip. Optical micrograph of the polished surface (left). Side view of the obliquely cut fibre tip (middle). Scanning electron micrograph of the polished fibre tip, which was coated by platinum (right), with debris caused by inadequate cleaning. (<b>b</b>) Histogram of the angle of the polished surface of the optical fibres. (<b>c</b>) Example of the reflection mirror deposited on the optical fibre tip. Optical micrograph of the mirror’s surface without the etching process (left). By masking the optical fibre, a reflection mirror did not form on the sidewall (right). (<b>d</b>) Result of simulating the relationship between the reflection mirror’s curvature and the focal length of the superimposed path of the laser from the fibre. (<b>e</b>) Relationship between the chemical etching time and the curvature of the surface of the chemically etched optical fibre tip. The plots indicate the experimental results, and the rigid line indicates a cubic function as an approximation of the experimental result. (<b>f</b>) Example of a fabricated FO-LDV sensor. Optical micrograph of the FO-LDV with a curved surface on the tip (left). The laser beam was emitted from the fibre’s sidewall after being reflected at the obliquely placed curved mirror (right). The laser’s path was visualised by the scattered particles in the fluid.</p>
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<p>Results of FO-LDV prototyping. (<b>a</b>) Examples of the obliquely cut fibre tip. Optical micrograph of the polished surface (left). Side view of the obliquely cut fibre tip (middle). Scanning electron micrograph of the polished fibre tip, which was coated by platinum (right), with debris caused by inadequate cleaning. (<b>b</b>) Histogram of the angle of the polished surface of the optical fibres. (<b>c</b>) Example of the reflection mirror deposited on the optical fibre tip. Optical micrograph of the mirror’s surface without the etching process (left). By masking the optical fibre, a reflection mirror did not form on the sidewall (right). (<b>d</b>) Result of simulating the relationship between the reflection mirror’s curvature and the focal length of the superimposed path of the laser from the fibre. (<b>e</b>) Relationship between the chemical etching time and the curvature of the surface of the chemically etched optical fibre tip. The plots indicate the experimental results, and the rigid line indicates a cubic function as an approximation of the experimental result. (<b>f</b>) Example of a fabricated FO-LDV sensor. Optical micrograph of the FO-LDV with a curved surface on the tip (left). The laser beam was emitted from the fibre’s sidewall after being reflected at the obliquely placed curved mirror (right). The laser’s path was visualised by the scattered particles in the fluid.</p>
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<p>Examples of the spectral waveform of the validation test using a rotating annular open channel flow. (<b>a</b>) Typical spectral waveform without flow conditions, which exhibited pedestal noise and other noises (blue dashed lines). (<b>b</b>–<b>f</b>) Examples of spectral waveforms using the FO-LDV sensor with estimated mirror curvatures (<span class="html-italic">MC</span>) of (<b>b</b>) 0.3 mm<sup>−1</sup>, (<b>c</b>) 1.5 mm<sup>−1</sup>, (<b>d</b>) 2.2 mm<sup>−1</sup>, (<b>e</b>) 4.3 mm<sup>−1</sup>, and (<b>f</b>) 8.1 mm<sup>−1</sup>. The red rigid line indicates the actual Doppler frequency (<span class="html-italic">f<sub>D</sub></span>) of the flow.</p>
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<p>Examples from the verification test via the engine bench test. (<b>a</b>) Influence of different positions of the sensor in the cross-section of the oil gallery on the spectral waveforms as measured at the oil filter location under an engine speed <span class="html-italic">N</span> = 2000 rpm and an oil temperature <span class="html-italic">T</span> = 80 °C. The sensor’s positions were <span class="html-italic">z</span> = −5 mm (left), <span class="html-italic">z</span> = 0 mm (middle), and <span class="html-italic">z</span> = 6 mm (right). (<b>b</b>) Influence of varying engine speeds on the spectral waveforms measured at <span class="html-italic">z</span> = 0 mm at the oil filter position and under <span class="html-italic">T</span> = 80 °C. (<b>c</b>) Measured velocity profiles during the engine bench test under <span class="html-italic">N</span> = 2000 rpm and <span class="html-italic">T</span> = 80 °C: results at the filter port (left) and main gallery (right), indicating that the flow profiles were influenced by the measurement location and the oil temperature. (<b>d</b>) Influence of engine speed on velocity profiles in the main gallery under constant oil temperature conditions.</p>
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<p>Examples from the verification test via the engine bench test. (<b>a</b>) Influence of different positions of the sensor in the cross-section of the oil gallery on the spectral waveforms as measured at the oil filter location under an engine speed <span class="html-italic">N</span> = 2000 rpm and an oil temperature <span class="html-italic">T</span> = 80 °C. The sensor’s positions were <span class="html-italic">z</span> = −5 mm (left), <span class="html-italic">z</span> = 0 mm (middle), and <span class="html-italic">z</span> = 6 mm (right). (<b>b</b>) Influence of varying engine speeds on the spectral waveforms measured at <span class="html-italic">z</span> = 0 mm at the oil filter position and under <span class="html-italic">T</span> = 80 °C. (<b>c</b>) Measured velocity profiles during the engine bench test under <span class="html-italic">N</span> = 2000 rpm and <span class="html-italic">T</span> = 80 °C: results at the filter port (left) and main gallery (right), indicating that the flow profiles were influenced by the measurement location and the oil temperature. (<b>d</b>) Influence of engine speed on velocity profiles in the main gallery under constant oil temperature conditions.</p>
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<p>Evaluation of the laser beam emitted from the FO-LDV sensor. (<b>a</b>) Outline of the experimental apparatus for observation of the emitting laser’s path via the laser-induced fluorescence method. (<b>b</b>) Examples of laser-induced fluorescence images by the laser beam emitted from the sensor, recorded without the fluorescence filter. The green light was the source light from the laser, whereas the orange light is the fluorescence. The path of the laser emitted from the normally cut fibre (left). The path of the laser from the obliquely cut fibre with a flat mirror (middle). The path of the laser from the obliquely cut fibre with a curved mirror (right). (<b>c</b>) Results of image analysis of the emitted laser beam’s profiles, width, and path corresponding to <a href="#photonics-11-00892-f006" class="html-fig">Figure 6</a>b. (<b>d</b>) Comparison of the emitted beam’s divergence from the FO-LDV sensor. The horizontal axis of the graph exhibits the transmitted distance from the fibre tip, and the vertical axis exhibits the diverged beam’s diameter from each fibre tip.</p>
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<p>Evaluation of the laser beam emitted from the FO-LDV sensor. (<b>a</b>) Outline of the experimental apparatus for observation of the emitting laser’s path via the laser-induced fluorescence method. (<b>b</b>) Examples of laser-induced fluorescence images by the laser beam emitted from the sensor, recorded without the fluorescence filter. The green light was the source light from the laser, whereas the orange light is the fluorescence. The path of the laser emitted from the normally cut fibre (left). The path of the laser from the obliquely cut fibre with a flat mirror (middle). The path of the laser from the obliquely cut fibre with a curved mirror (right). (<b>c</b>) Results of image analysis of the emitted laser beam’s profiles, width, and path corresponding to <a href="#photonics-11-00892-f006" class="html-fig">Figure 6</a>b. (<b>d</b>) Comparison of the emitted beam’s divergence from the FO-LDV sensor. The horizontal axis of the graph exhibits the transmitted distance from the fibre tip, and the vertical axis exhibits the diverged beam’s diameter from each fibre tip.</p>
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<p>CFD analysis for the flow field around the FO-LDV sensor in a steady and uniform oil flow. (<b>a</b>) Fluid domain and boundary conditions for the CFD analysis (left). The model of the FO-LDV sensor (right). (<b>b</b>) Examples of the results of CFD analysis. The coloured contour maps reveal the magnitude of the flow velocity in the main flow direction. (<b>c</b>) Distribution of the flow speed approaching the FO-LDV sensor on the streamline through the forward stagnation point of the sensor. (<b>d</b>) Relationship between the Reynolds number of the flow around the FO-LDV sensor and the thickness of the stagnant layer formed in front of the sensor.</p>
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<p>CFD analysis for the flow field around the FO-LDV sensor in a steady and uniform oil flow. (<b>a</b>) Fluid domain and boundary conditions for the CFD analysis (left). The model of the FO-LDV sensor (right). (<b>b</b>) Examples of the results of CFD analysis. The coloured contour maps reveal the magnitude of the flow velocity in the main flow direction. (<b>c</b>) Distribution of the flow speed approaching the FO-LDV sensor on the streamline through the forward stagnation point of the sensor. (<b>d</b>) Relationship between the Reynolds number of the flow around the FO-LDV sensor and the thickness of the stagnant layer formed in front of the sensor.</p>
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<p>Optical simulation of the FO-LDV measurements was conducted using the results of the CFD analysis for the flow field around the FO-LDV sensor in a steady and uniform oil flow. (<b>a</b>) Conceptual diagram of the optical and physical phenomena influencing the accuracy of FO-LDV measurements. (<b>b</b>) Setting of the region of interest (ROI) in the fluid domain of the CFD analysis for the optical simulation. (<b>c</b>) Extracted CFD result of the <span class="html-italic">x</span>-direction component of the flow velocities in the ROI under <span class="html-italic">U</span> = 1.0 m/s. The coloured contour maps reveal the magnitude of the flow velocity in the main flow direction. (<b>d</b>) Distribution of the flow speed approaching the FO-LDV sensor under <span class="html-italic">U</span> = 1.0 m/s. (<b>e</b>) Distribution of laser’s intensity for a Gaussian beam emitted from the FO-LDV sensor when it reached each position in the ROI. (<b>f</b>) Relationship between the backscattered light’s intensity due to particles received by the FO-LDV sensor and the particles’ position in the ROI. (<b>g</b>) Example of the simulated spectral waveform by spatiotemporally integrating the signal/laser intensity-weighted probability of the existence of the flow velocities. (<b>h</b>) Example of an experimentally obtained spectral waveform under the same flow condition (<span class="html-italic">U</span> = 1.0 m/s) as the simulation.</p>
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