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Search Results (1,587)

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Keywords = fiber optic sensing

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14 pages, 6268 KiB  
Article
Analysis of Influence of Abnormal Fiber-Optical Current Transformer on Double Closed-Loop Control of Converter Valve in Flexible DC Converter Station
by Yirun Ji, Qing Huai, Xuanfei Huang, Libo Ma, Qian Yuan, Chengjie Zhou and Chen Zhao
Electronics 2025, 14(1), 141; https://doi.org/10.3390/electronics14010141 (registering DOI) - 1 Jan 2025
Viewed by 192
Abstract
The fiber-optical current transformer (FOCT) is the core measuring equipment of the flexible DC converter station, which affects the operation control of the system. In order to solve the problem of the influence of the abnormal FOCT on the operation of the converter [...] Read more.
The fiber-optical current transformer (FOCT) is the core measuring equipment of the flexible DC converter station, which affects the operation control of the system. In order to solve the problem of the influence of the abnormal FOCT on the operation of the converter valve being unclear, the common fault modes of temperature and optical path of the FOCT are analyzed in this paper. Then, based on the traditional optical current transformer (OCT) model and considering the influence of temperature parameters on the FOCT, the FOCT dynamic model considering multiple factors is constructed. Finally, the simulation analysis is carried out on the MATLAB 2021b/Simulink platform, and the results show that (1) when the FOCT temperature compensation is abnormal, the transmission power of the converter valve increases with the increase in temperature, but the increase in temperature change is small; (2) when the FOCT light source compensation is abnormal, the light source attenuates, the converter valve active power decreases, and the reactive power increases; and (3) when the optical fiber sensing ring is broken, the transmission power increases and seriously deviates from the preset value (the active power increases by about 87.5% and the reactive power increases by about 90%). It can be seen that the abnormal FOCT in the converter station has a serious influence on the operation of the converter valve. Full article
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<p>Schematic diagram of FOCT.</p>
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<p>Three-phase MMC topology.</p>
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<p>Coupled model of flexible DC converter valve and FOCT.</p>
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<p>Model and measured current values.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>Overall block diagram of the system.</p>
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<p>Detailed diagram of FOCT simulation module.</p>
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<p>Detailed diagram of outer-loop power control module.</p>
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<p>Detailed diagram of inner-loop current control module.</p>
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10 pages, 3849 KiB  
Communication
Tunable Single-Longitudinal-Mode Thulium–Holmium Co-Doped Fiber Laser with an Ultra-Narrow Linewidth by Utilizing a Triple-Ring Passive Sub-Ring Resonator
by Pengfei Wang, Fengping Yan, Qi Qin, Dandan Yang, Ting Feng, Peng Liu, Ting Li, Chenhao Yu, Xiangdong Wang, Hao Guo, Yuezhi Cai, Wenjie Ji and Youchao Jiang
Photonics 2025, 12(1), 19; https://doi.org/10.3390/photonics12010019 - 28 Dec 2024
Viewed by 294
Abstract
A low-cost, wavelength-tunable single-longitudinal-mode (SLM) thulium–holmium co-doped fiber laser (THDFL) in a 2 μm band with a simple structure is described in the present paper. To obtain a stable SLM and narrow laser linewidth, a five-coupler-based three-ring (FCTR) filter is utilized in the [...] Read more.
A low-cost, wavelength-tunable single-longitudinal-mode (SLM) thulium–holmium co-doped fiber laser (THDFL) in a 2 μm band with a simple structure is described in the present paper. To obtain a stable SLM and narrow laser linewidth, a five-coupler-based three-ring (FCTR) filter is utilized in the ring cavity of the fiber laser. Tunable SLM wavelength output from THDFLs with kHz linewidths can be achieved by designing the FCTR filter with an effective free-spectral range and a 3 dB bandwidth at the main resonant peak. The measurement results show that the laser is in the SLM lasing state, with a highly stabilized optical spectrum, a linewidth of approximately 9.45 kHz, an optical signal-to-noise ratio as high as 73.6 dB, and a relative intensity noise of less than −142.66 dB/Hz. Furthermore, the wavelength can be tuned in the range of 2.6 nm. The proposed fiber laser has a wide range of applications, including coherence optical communication, optical fiber sensing, and dense wavelength-division-multiplexing. Full article
(This article belongs to the Special Issue Advanced Fiber Laser Technology and Its Application)
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<p>(<b>a</b>) Experimental configuration of THDFL. LD: laser diode; WDM: wavelength division multiplexer; THDF: thulium–holmium co-doped fiber; CIR: circulator; FBG: fiber Bragg grating; OC: optical coupler; (<b>b</b>) schematic diagram of the proposed FCTR filter; (<b>c</b>) transmission and reflection spectra of the FBG.</p>
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<p>Signal-flow graph representation of the sub-ring cavity.</p>
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<p>Simulated spectra of the proposed FCTR filter. The inset is a zoom-in of the main resonant peak of the FCTR filter.</p>
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<p>(<b>a</b>) Spectrum of the single-wavelength at 2048.39 nm; (<b>b</b>) fluctuations in wavelength and power at 2048.39 nm.</p>
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<p>(<b>a</b>) The self-homodyne RF spectrum measured using a signal analyzer with a range of 0–100 MHz; (<b>b</b>) 0–500 MHz; and (<b>c</b>) 0–1000 MHz; (<b>d</b>) the spectrum of the main cavity without an FCTR filter.</p>
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<p>RIN spectra of the proposed SLM THDFL, in 0–5 MHz, using a RBW of 10 kHz for the signal analyzer. Insets show the same measurements in the 0–200 kHz range using a RBW of 100 Hz with relaxation oscillation peaks.</p>
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<p>Frequency noise PSD of the constructed SLM THDFL, and the linewidths at different integration times.</p>
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<p>The spectrum of the THDFL with a tunable wavelength range of ~2.6 nm.</p>
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15 pages, 4143 KiB  
Article
Digitalized Optical Sensor Network for Intelligent Facility Monitoring
by Esther Renner, Lisa-Sophie Haerteis, Joachim Kaiser, Michael Villnow, Markus Richter, Torsten Thiel, Andreas Pohlkötter and Bernhard Schmauss
Photonics 2025, 12(1), 18; https://doi.org/10.3390/photonics12010018 - 28 Dec 2024
Viewed by 275
Abstract
Due to their inherent advantages, optical fiber sensors (OFSs) can substantially contribute to the monitoring and performance enhancement of energy infrastructure. However, optical fiber sensor systems often are standalone solutions and do not connect to the main energy infrastructure control systems. In this [...] Read more.
Due to their inherent advantages, optical fiber sensors (OFSs) can substantially contribute to the monitoring and performance enhancement of energy infrastructure. However, optical fiber sensor systems often are standalone solutions and do not connect to the main energy infrastructure control systems. In this paper, we propose a solution for the digitalization of an optical fiber sensor system realized by the Open Platform Communications Unified Architecture (OPC UA) protocol and the Internet of Things (IoT) platform Insights Hub. The optical fiber sensor system is based on bidirectional incoherent optical frequency domain reflectometry (biOFDR) and is used for the interrogation of fiber Bragg grating (FBG) arrays. To allow for an automated sensor identification and thus measurement procedure, an optical sensor identification marker based on a unique combination of fiber Bragg gratings (FBGs) is established. To demonstrate the abilities of the digitalized sensor network, a field test was performed in a power plant test facility of Siemens Energy. Temperature measurements of a packaged FBG sensor fiber were performed with a portable demonstrator, illustrating the system’s robustness and the comprehensive data processing stream from sensor value formation to the cloud. The realized network services promote sensor data quality, fusion, and modeling, expanding opportunities using digital twin technology. Full article
(This article belongs to the Special Issue Advanced Optical Fiber Sensors for Harsh Environment Applications)
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<p>Optical sensor system based on the bidirectional incoherent optical frequency domain (biOFDR): (<b>a</b>) Schematic of the biOFDR setup; (<b>b</b>) image of the portable demonstrator.</p>
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<p>Optical sensor identification markers (ID markers) based on three FBGs with different wavelength combinations: (<b>a</b>) measurement results of marker 1-1-1 from the biOFDR; (<b>b</b>) different wavelength and position combinations with applied markers 1-1-1 and 1-1-2 in blue and red, respectively.</p>
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<p>Digital sensor network architecture. Data flow from left (DigiMonet biOFDR system) to right (cloud applications). The different communication paths are marked by type.</p>
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<p>Measurement value Open Platform Communications Unified Architecture (OPC UA) node with properties, exemplarily shown for the full-width half-maximum (FWHM) bandwidth of FBG 1.</p>
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<p>Automated cloud onboarding based on the Siemens MindSphere Digital Service Platform (MDSP).</p>
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<p>Power plant generator mockup at Siemens Energy AG with installed fiber sensor arrays. The black dots on the sensor strip mark the position of the FBG. Each sensor strip consists of a standard single-mode fiber with 10 FBGs.</p>
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<p>Configuration scheme of the OPC UA service structure. Service connections are depicted in grey, OPC UA connections in yellow, and file transfers in green.</p>
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<p>Measurement results acquired with the bidirectional iOFDR setup: (<b>a</b>) FBG sensor elements and marker configuration; (<b>b</b>) temperature measurements for all 10 FBGs over the whole measurement time (each color represents the temperature measurement of one FBG).</p>
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<p>Screenshot of the ThingsBoard during the field test. The measured temperature values (as depicted in <a href="#photonics-12-00018-f008" class="html-fig">Figure 8</a>) are transferred from the biOFDR demonstrator unit to the cloud via the OPC UA data servers.</p>
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<p>Insights Hub Monitor dashboard (simplified screenshot). The calculated temperature values (Max, Mean, Min) are derived from the Statistics µ-service.</p>
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14 pages, 9635 KiB  
Article
Monitoring a Railway Bridge with Distributed Fiber Optic Sensing Using Specially Installed Fibers
by Kinzo Kishida, Thein Lin Aung and Ruiyuan Lin
Sensors 2025, 25(1), 98; https://doi.org/10.3390/s25010098 - 27 Dec 2024
Viewed by 277
Abstract
This article explores the use of distributed fiber optic sensing (DFOS) technology in monitoring civil infrastructure, with a concrete example of an elevated railway bridge in Taiwan. The field test utilized multiple strain-sensing fibers attached to a 1 km span of a bullet [...] Read more.
This article explores the use of distributed fiber optic sensing (DFOS) technology in monitoring civil infrastructure, with a concrete example of an elevated railway bridge in Taiwan. The field test utilized multiple strain-sensing fibers attached to a 1 km span of a bullet train railway bridge, which were combined to calculate the 3-dimensional bridge deformation. The installed sensing system and continuous measurements enabled quick safety confirmation after earthquakes of Richter scale 6.4 and 6.8 magnitudes occurred. Finally, the dynamic monitoring of a bullet train using Distributed Acoustic Sensing (DAS) demonstrated the merits of fiber optic sensing for both static and dynamic measurements. The empirical data gathered through this work aid in the evaluation of DFOS technology for structural-monitoring applications. Full article
(This article belongs to the Special Issue Optical Sensors for Industrial Applications)
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<p>Installation of optical fiber cables on the bridge girder.</p>
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<p>Box girder (<b>a</b>) side view, (<b>b</b>) isometric view and coordinate system, (<b>c</b>) cross-section view and designation of fiber strains, (<b>d</b>) with pier.</p>
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<p>Brillouin frequency shift of four fibers between 7 A.M. 24 October and 2 P.M. 26 October, for (<b>a</b>) fibers on top half and (<b>b</b>) fibers on bottom half of box girder.</p>
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<p>The deformation of the bridge structure in the entire monitoring interval. (<b>left</b>) Horizontal and vertical bending deformations and (<b>right</b>) each component of displacement.</p>
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<p>The deformation of the bridge structure in the entire monitoring interval.</p>
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<p>(<b>above</b>) An example display of the entire monitoring section by the SCADA system. (<b>below</b>) A display of a section of interest and the warning values for safety management and inspection implementation standards.</p>
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<p>Strain changes over one-month interval (4-quadrant comparison at 700 m). Each tick on X-axis corresponds to start of day (00:00).</p>
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<p>The horizontal bending strain in the upper part of the bridge girder after the earthquake on 18 September 2022. The green shaded region shows the normal range of strains before the earthquake.</p>
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<p>The vertical bending strain on the left side of the bridge girder after the earthquake on 18 September 2022. The green shaded region shows the normal range of strains before the earthquake.</p>
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<p>Conceptual diagram of dynamic measurement; fiber is U-turned at end of monitoring section.</p>
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<p>(<b>a</b>) The dynamic signal (strain rate) due to a passing train, measured by the DAS system, (<b>b</b>) the time snapshot along the vertical dotted line, (<b>c</b>) the time trace along the horizontal dotted line.</p>
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<p>(<b>a</b>) The dynamic strain of the bridge due to a passing train, (<b>b</b>) the time snapshot along the vertical dotted line, (<b>c</b>) 13 peaks from the bogies of 12 train cars can be seen in the time trace.</p>
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20 pages, 7404 KiB  
Review
Fiber-Optic Distributed Acoustic Sensing for Smart Grid Application
by Xiaofeng Zhang, Jun Qi, Xiao Liang, Zhen Guan, Zeguang Liu, Chang Zhang, Dabin Chen, Weifeng Deng, Changzhi Xu, Xinwei Wang and Huanhuan Liu
Photonics 2025, 12(1), 7; https://doi.org/10.3390/photonics12010007 - 25 Dec 2024
Viewed by 315
Abstract
Fiber-optic distributed acoustic sensing (DAS) promises great application prospects in smart grids due to its superior capabilities, including resistance to electromagnetic interference, long-distance coverage, high sensitivity and real-time monitoring. In this paper, we review the research progress and application status of DAS technology [...] Read more.
Fiber-optic distributed acoustic sensing (DAS) promises great application prospects in smart grids due to its superior capabilities, including resistance to electromagnetic interference, long-distance coverage, high sensitivity and real-time monitoring. In this paper, we review the research progress and application status of DAS technology in power systems, focusing on its applications in areas such as the wind-induced vibration detection of transmission lines, partial discharge monitoring, transformer condition monitoring, and underwater cable and renewable energy transmission monitoring, as well as in the safety and protection of surrounding power facilities. Addressing the challenges currently faced by DAS technology in the smart grid, including detection accuracy, system cost, and data processing capability, this paper analyzes its major technical bottlenecks and proposes future research directions. Full article
(This article belongs to the Special Issue Advanced Optical Fiber Sensors for Harsh Environment Applications)
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<p>Application scenario of DAS technology in smart grid.</p>
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<p>DAS system principle: (<b>a</b>) DAS system architecture; (<b>b</b>) vibration causing changes in RBS; (<b>c</b>) RBS microphysical model.</p>
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<p>Structure diagram of different demodulation methods: (<b>a</b>) 3 × 3 structure; (<b>b</b>) PGC; (<b>c</b>) coherent detection; (<b>d</b>) 90° hybrid.</p>
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<p>Recent progress of DAS system in terms of (<b>a</b>,<b>b</b>) extending sensing distance [<a href="#B36-photonics-12-00007" class="html-bibr">36</a>]; (<b>c</b>,<b>d</b>) suppressing noise [<a href="#B38-photonics-12-00007" class="html-bibr">38</a>]; (<b>e</b>,<b>f</b>) improving acoustic wave sensitivity [<a href="#B39-photonics-12-00007" class="html-bibr">39</a>]; (<b>g</b>,<b>h</b>) reducing the data size and computation time [<a href="#B40-photonics-12-00007" class="html-bibr">40</a>].</p>
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<p>Recent progress of DAS system in discharge detection: (<b>a</b>–<b>c</b>) single-mode fiber wound around an elastic cylindrical base for GIS [<a href="#B66-photonics-12-00007" class="html-bibr">66</a>]; (<b>d</b>–<b>f</b>) 3D-printed sensing elements integrated in φ-OTDR for breakdown discharge detection [<a href="#B19-photonics-12-00007" class="html-bibr">19</a>]; (<b>g</b>–<b>i</b>) machine learning method for DAS systems in PD classification [<a href="#B67-photonics-12-00007" class="html-bibr">67</a>].</p>
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<p>Recent progress of DAS system in transmission line monitoring: (<b>a</b>,<b>b</b>) power cable vibration measurement [<a href="#B84-photonics-12-00007" class="html-bibr">84</a>]; (<b>c</b>,<b>d</b>) tension towers and tangent towers [<a href="#B87-photonics-12-00007" class="html-bibr">87</a>].</p>
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17 pages, 4769 KiB  
Article
Intelligent Pattern Recognition Using Distributed Fiber Optic Sensors for Smart Environment
by Brian Pamukti, Shofuro Afifah, Shien-Kuei Liaw, Jiun-Yu Sung and Daping Chu
Sensors 2025, 25(1), 47; https://doi.org/10.3390/s25010047 - 25 Dec 2024
Viewed by 264
Abstract
Distributed fiber optic sensors (DFOSs) have become increasingly popular for intrusion detection, particularly in outdoor and restricted zones. Enhancing DFOS performance through advanced signal processing and deep learning techniques is crucial. While effective, conventional neural networks often involve high complexity and significant computational [...] Read more.
Distributed fiber optic sensors (DFOSs) have become increasingly popular for intrusion detection, particularly in outdoor and restricted zones. Enhancing DFOS performance through advanced signal processing and deep learning techniques is crucial. While effective, conventional neural networks often involve high complexity and significant computational demands. Additionally, the backscattering method requires the signal to travel twice the normal distance, which can be inefficient. We propose an innovative interferometric sensing approach utilizing a Mach–Zehnder interferometer (MZI) combined with a time forest neural network (TFNN) for intrusion detection based on signal patterns. This method leverages advanced sensor characterization techniques and deep learning to improve accuracy and efficiency. Compared to the conventional one-dimensional convolutional neural network (1D-CNN), our proposed approach achieves an 8.43% higher accuracy, demonstrating the significant potential for real-time signal processing applications in smart environments. Full article
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<p>Illustration of the environment in restricted zones.</p>
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<p>Experimental setup with interferometric sensing.</p>
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<p>Model comparison experimental workflow.</p>
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<p>The convolutional neural network (CNN) architecture for intrusion detection.</p>
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<p>The dense neural network (DNN) architecture for intrusion detections.</p>
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<p>The dense neural network (RNN) architecture for intrusion detections.</p>
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<p>Sample signals obtained by the DAQ system: demonstrating various physical interactions for (<b>a</b>) crawling, (<b>b</b>) knocking, (<b>c</b>) touching, and (<b>d</b>) noise.</p>
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<p>Visual comparison of voltage distributions across four different types of vibrations using violin plots.</p>
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<p>Trend of training accuracy and time vs. number of estimators for (<b>a</b>) TFNN and epochs for (<b>b</b>) CNN, (<b>c</b>) DNN, and (<b>d</b>) RNN.</p>
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<p>Evaluation of intrusion signal classification using a confusion matrix representation for (<b>a</b>) proposed method, (<b>b</b>) CNN, (<b>c</b>) DNN, and (<b>d</b>) RNN.</p>
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<p>Evaluation of intrusion signal classification using a confusion matrix representation for (<b>a</b>) proposed method, (<b>b</b>) CNN, (<b>c</b>) DNN, and (<b>d</b>) RNN.</p>
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<p>Comparing t-SNE visualizations (<b>a</b>) before and (<b>b</b>) after applying proposed models.</p>
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10 pages, 2316 KiB  
Article
Enhanced Vernier Effect in Cascaded Fiber Loop Interferometers for Improving Temperature Sensitivity
by Jianming Zhou, Yanyan Zhi, Junyi Zhang, Jianping Yao, Junkai Zhang and Jiejun Zhang
Sensors 2025, 25(1), 38; https://doi.org/10.3390/s25010038 - 25 Dec 2024
Viewed by 242
Abstract
This work presents a high-sensitivity temperature sensing system utilizing an enhanced Vernier effect implemented in cascaded fiber loop interferometers. High-sensitivity temperature sensors based on the Vernier effect have broad application prospects, but the sensitivity of traditional measurement schemes is difficult to improve further [...] Read more.
This work presents a high-sensitivity temperature sensing system utilizing an enhanced Vernier effect implemented in cascaded fiber loop interferometers. High-sensitivity temperature sensors based on the Vernier effect have broad application prospects, but the sensitivity of traditional measurement schemes is difficult to improve further due to the limited variation in the difference between two free spectrum ranges (FSRs). Our sensing system incorporates two fiber loop interferometers and a single-mode fiber to form a Vernier spectral response, characterized by two complementary optical filter responses. As the temperature of the sensing fiber changes, one FSR decreases, and the other increases, respectively, enhancing the difference value between the two FSRs to form an enhanced Vernier effect. Experimental results demonstrate that the temperature sensitivity of a traditional Vernier effect measurement is only −298.29 kHz/°C, while our proposed enhanced Vernier effect sensing system achieves a sensitivity of 618.14 kHz/°C, which is 92 times higher than that of a two-arm optical carrier-based microwave interferometry (OCMI) sensing system and 2.07 times higher than that of a traditional Vernier effect sensing system. This approach with an enhanced Vernier effect scheme based on cascaded fiber loop interferometers can be used to design high-sensitivity sensing systems for biometrics, smart cities, and the Internet of Things. Full article
(This article belongs to the Section Communications)
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<p>The schematic of the high-sensitivity temperature sensing system based on the enhanced Vernier effect and cascaded fiber loop interferometers. (BOS: broadband optical source; PC: polarization controller; EOM: electrooptical modulator; OC: optical coupler; R1: length of optical fiber loop 1; R2: length of optical fiber loop 2; PD: photodetector; and VNA: vector network analyzer).</p>
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<p>Optical Vernier effect envelope spectrum generated by superposition of different FSRs: (<b>a</b>) FSR1. (<b>b</b>) FSR2. (<b>c</b>) FSR3. (<b>d</b>) Superposition of FSR1 and FSR2. (<b>e</b>) Superposition of FSR1 and FSR3.</p>
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<p>FSR change diagram of the two-beam OCMI sensing system as a response to temperature change: (<b>a</b>) FSR1 of L0 and L1. (<b>b</b>) FSR2 of L1 and L2.</p>
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<p>Two kinds of the Vernier effect temperature sensing system of envelope spectrum shifting: (<b>a</b>) The traditional scheme. (<b>b</b>) The enhanced scheme.</p>
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<p>Envelope offset curves of the Vernier effect as the temperature changes: (<b>a</b>) Traditional test scheme. (<b>b</b>) Enhanced test scheme.</p>
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<p>Linear fittings of temperature change and frequency shifts: (<b>a</b>) Enhanced Vernier effect. (<b>b</b>) L1 and L2. (<b>c</b>) L0 and L1. (<b>d</b>) Traditional Vernier effect.</p>
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<p>Stability analysis diagram of temperature sensing system based on enhanced Vernier effect.</p>
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10 pages, 2211 KiB  
Communication
Track Deflection Monitoring for Railway Construction Based on Dynamic Brillouin Optical Time-Domain Reflectometry
by Tianfang Zhang, Liming Zhou, Weimin Liu and Linghao Cheng
Sensors 2024, 24(24), 8205; https://doi.org/10.3390/s24248205 - 23 Dec 2024
Viewed by 479
Abstract
Real-time online monitoring of track deformation during railway construction is crucial for ensuring the safe operation of trains. However, existing monitoring technologies struggle to effectively monitor both static and dynamic events, often resulting in high false alarm rates. This paper presents a monitoring [...] Read more.
Real-time online monitoring of track deformation during railway construction is crucial for ensuring the safe operation of trains. However, existing monitoring technologies struggle to effectively monitor both static and dynamic events, often resulting in high false alarm rates. This paper presents a monitoring technology for track deformation during railway construction based on dynamic Brillouin optical time-domain reflectometry (Dy-BOTDR), which effectively meets requirements in the monitoring of both static and dynamic events of track deformation. Dy-BOTDR can provide a two-dimensional spatial–temporal distribution map of track strain changes to characterize various events for better monitoring accuracy and lower false alarm rates. Full article
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<p>Schematic diagram of the beam micro-element before and after deformation.</p>
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<p>Real-time online monitoring system for track deformation of the tested railway based on dynamic BOTDR. PMC: polarization maintain coupler; SOA: semiconductor optical amplifier; EDFA: erbium-doped fiber amplifier; AWG: arbitrary waveform generator; DAQ: data acquisition.</p>
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<p>The deflection and strain curve at a specific location on the railway track.</p>
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<p>Maximum values of the deflection curve processed with different wavelet functions.</p>
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<p>Algorithm flow for calculating rail deflection from deformation.</p>
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<p>Real-time spatiotemporal two-dimensional distribution map of track strain changes as the train passes.</p>
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13 pages, 4333 KiB  
Article
Free-Space to SMF Integration and Green to C-Band Conversion Based on PPLN
by Takahiro Kodama, Kiichiro Kuwahara, Ayumu Kariya and Rikizo Ikuta
Sensors 2024, 24(24), 8162; https://doi.org/10.3390/s24248162 - 21 Dec 2024
Viewed by 370
Abstract
In this study, we experimentally demonstrate a PPLN-based free-space to SMF (single-mode fiber) conversion system capable of efficient long-wavelength down-conversion from 518 nm, optimized for minimal loss in highly turbid water, to 1540 nm, which is ideal for low-loss transmission in standard SMF. [...] Read more.
In this study, we experimentally demonstrate a PPLN-based free-space to SMF (single-mode fiber) conversion system capable of efficient long-wavelength down-conversion from 518 nm, optimized for minimal loss in highly turbid water, to 1540 nm, which is ideal for low-loss transmission in standard SMF. Leveraging the nonlinear optical properties of periodically poled lithium niobate (PPLN), we achieve a wavelength conversion efficiency of 1.6% through difference frequency generation while maintaining a received optical signal-to-noise ratio of 10.4 dB. Our findings underscore the potential of integrating PPLN-based wavelength conversion with fiber optic networks, offering a viable solution for next-generation optical sensor systems that demand real-time, low-latency, and reliable data transmission. This work represents a significant advancement in developing robust and efficient optical sensor technologies, addressing the challenges associated with long-distance transmission and broad-linewidth light sources in optical remote sensing applications. Full article
(This article belongs to the Special Issue Atmospheric Optical Remote Sensing)
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<p>Overall structure of optical remote sensing system.</p>
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<p>FSFC configuration: (<b>a</b>) no-conversion type, (<b>b</b>) O/E/O conversion type, and (<b>c</b>) O/O conversion type.</p>
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<p>Power budget diagram of overall optical remote sensing system.</p>
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<p>Schematic configuration of the FSFC.</p>
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<p>Structure of (<b>a</b>) SHG and (<b>b</b>) DFG.</p>
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<p>The acceptance bandwidth by sinc<sup>2</sup>(Δ<span class="html-italic">kl</span>/2) for a single-frequency pump laser at 780 nm.</p>
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<p>Experimental setup.</p>
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<p>External view of FSFC.</p>
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<p>Characteristics of the change in the 780 nm pump power: (<b>a</b>) insertion loss in PPLN 2, (<b>b</b>) output power relationship, and (<b>c</b>) conversion efficiency <span class="html-italic">η</span> in Equation (8) (linear scale on the vertical axis).</p>
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<p>Characteristics of change in the 518 nm input power: (<b>a</b>) output power relationship and (<b>b</b>) conversion efficiency.</p>
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<p>(<b>a</b>) Received OSNR characteristics in relation to the output power of EDFA 1, (<b>b</b>) optical spectrum with a varying center wavelength of the green band’s OOK signal, and (<b>c</b>) optical spectrum with a varying output power of EDFA 1.</p>
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<p>Correlation between the transmitted and received signals.</p>
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<p>Measured power characteristics of SMF without and with wavelength conversion.</p>
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16 pages, 4212 KiB  
Article
Ultra-High Sensitivity Methane Gas Sensor Based on Cryptophane-A Thin Film Depositing in Double D-Shaped Photonic Crystal Fiber Using the Vernier Effect
by Di Zhou, Sajid Ullah, Sa Zhang and Shuguang Li
Sensors 2024, 24(24), 8132; https://doi.org/10.3390/s24248132 - 19 Dec 2024
Viewed by 377
Abstract
Methane gas leakage can lead to pollution problems, such as rising ambient temperature. In this paper, the Vernier effect of a double D-shaped photonic crystal fiber (PCF) in a Sagnac interferometer (SI) is proposed for the accurate detection of mixed methane gas content [...] Read more.
Methane gas leakage can lead to pollution problems, such as rising ambient temperature. In this paper, the Vernier effect of a double D-shaped photonic crystal fiber (PCF) in a Sagnac interferometer (SI) is proposed for the accurate detection of mixed methane gas content in the gas. The optical fiber structure of the effective sensing in the sensing SI loop and the effective sensing in the reference SI loop are the same. Both of them adopt the polarization-maintaining photonic crystal fiber (PM-PCF) designed in this paper. The optical fiber structure of the effective sensing in the sensing SI loop deposited with the methane gas-sensitive film is polished to obtain a double-D structure. This operation makes it easier for methane gas to contact the sensitive film and realize the sensor’s repeated use. The sensing capability of the methane gas sensor was evaluated utilizing the finite element method (FEM). The numerical simulation results show that when the concentration of methane gas in the environment is 0~3.5%, the average sensitivity of two parallel Sagnac loops is 409.43 nm/%. Using Vernier effect cascade SI loops, the sensitivity of the sensor for detecting methane gas increased by four times. Without considering air and humidity, we provide a practical scheme for the development and design of high-sensitivity methane gas sensors. Full article
(This article belongs to the Special Issue Advances in the Design and Application of Optical Fiber Sensors)
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<p>(<b>a</b>) The end-face view after PCF truncation; (<b>b</b>) PCF cross-section after polishing; (<b>c</b>) polarization mode X-direction electric field diagram; and (<b>d</b>) polarization mode Y-direction electric field diagram.</p>
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<p>PCF methane gas-sensing principle drawing based on a single SI loop.</p>
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<p>Trend image of refractive index (<b>a</b>) in the X direction and Y direction, (<b>b</b>) in the X direction, (<b>c</b>) in the Y direction of PCF, (<b>d</b>) trend image of phase birefringence B and wavelength at 0–3.5% methane concentration in the external environment, and (<b>e</b>) trend image of phase birefringence B versus methane concentration at wavelengths of 1000 to 2000 nm.</p>
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<p>Trend image of refractive index (<b>a</b>) in the X direction and Y direction, (<b>b</b>) in the X direction, (<b>c</b>) in the Y direction of PCF, (<b>d</b>) trend image of phase birefringence B and wavelength at 0–3.5% methane concentration in the external environment, and (<b>e</b>) trend image of phase birefringence B versus methane concentration at wavelengths of 1000 to 2000 nm.</p>
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<p>(<b>a</b>) The transmission spectrum of 500 nm methane gas sensing film with the concentration of methane gas 0–3.5% in the external gas environment and (<b>b</b>) the dip wavelength is fitted by a polynomial with methane concentration of 0–3.5%.</p>
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<p>(<b>a</b>) The trend diagram of the interference inclination of the transmission spectrum and the methane concentration with the thickness of the methane-sensitive film increases from 500 nm to 900 nm and (<b>b</b>) the trend diagram of the interference inclination of the transmission spectrum and the methane concentration with the depth of polishing increases from 5 × 10<sup>3</sup> nm to 6 × 10<sup>3</sup> nm.</p>
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<p>Deposition of methane gas-sensitive film on sensing arm based on Vernier effect reference arm without any modification of methane gas-sensing principle diagram.</p>
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<p>(<b>a</b>) The transmission spectrum of the reference SI loop is 4 cm in length, (<b>b</b>) the transmission spectrum of the reference SI loop is 4.1 cm in length, and (<b>c</b>) the transmission spectrum of the reference SI loop is 4.2 cm in length between 1000 and 3000 nm in wavelength. (The red line in (<b>a</b>–<b>c</b>) is the interference valley tracking curve) (<b>d</b>) The image is a polynomial fitting of the inclination wavelength of the transmission spectrum to the content of the external methane concentration.</p>
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<p>(<b>a</b>) The transmission spectrum of SI loops, (<b>b</b>) the transmission spectrum of the sensing SI loop is 1 × 10<sup>8</sup> nm in length, and (<b>c</b>) the transmission spectrum of the reference SI loop is 4 × 10<sup>7</sup> nm in length.</p>
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<p>(<b>a</b>) The transmission spectrum of a single SI loop, and (<b>b</b>) the transmission spectrum of a parallel SI loop between 1000 and 3000 nm in wavelength. (The red line in (<b>a</b>,<b>b</b>) is the interference valley tracking curve). (<b>c</b>) The position of the two envelope wavelengths is fitted to the polynomial of the methane concentration.</p>
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21 pages, 7982 KiB  
Article
Flexural Behavior of BFRP Bar–Recycled Tire Steel Fiber-Reinforced Concrete Beams
by Jing-Hua Fu, Ao Zhang, Kai-Feng Chen, Bao-Yuan Li and Wei Wu
Materials 2024, 17(24), 6197; https://doi.org/10.3390/ma17246197 - 18 Dec 2024
Viewed by 386
Abstract
This research advocates for the use of basalt fiber-reinforced polymer (BFRP) bars and recycled tire steel fibers to reinforce concrete beams. Six concrete beams were constructed using different volume contents of recycled tire steel fibers (0, 0.5%, 1.0%, 1.5%) and BFRP reinforcement ratios [...] Read more.
This research advocates for the use of basalt fiber-reinforced polymer (BFRP) bars and recycled tire steel fibers to reinforce concrete beams. Six concrete beams were constructed using different volume contents of recycled tire steel fibers (0, 0.5%, 1.0%, 1.5%) and BFRP reinforcement ratios (0.48%, 0.75%, 1.08%). Mechanical properties tests were conducted to investigate the flexural characteristics and failure modes of beams utilizing the non-contact full-field strain displacement measuring technology–digital image (3D-DIC) technology. The recycled tire steel fiber (RTSF) improves flexural performance, which contributes to inhibiting crack propagation, reducing flexural deformation, and improving the first cracking and ultimate loading capacities. Under the same reinforcement ratio, in comparison to ordinary BFRP beams, the cracking load of BFRP-RTSF beams increased by 17.73%, 23.76%, and 42.94%, respectively, and the ultimate bearing capacity increased by 4.03%, 5.85%, and 13.21%, respectively. In addition, a modified calculation model of bearing capacity considering RTSF tensile strength is proposed. The predicted values of BFRP-RTSF beams match well with the experimental values. Full article
(This article belongs to the Special Issue Strengthening, Repair, and Retrofit of Reinforced Concrete)
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<p>RTSF used in this study.</p>
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<p>Length distribution of recycled tire steel fiber (RTSF).</p>
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<p>BFRP bar used in this study.</p>
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<p>Details for the specimens.</p>
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<p>Four-point bending configuration for BFRP-RTSF beams (unit: mm).</p>
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<p>3D digital image correlation measurement system.</p>
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<p>Crack patterns and failure of beams of BRTSC: (<b>a</b>) BRTSC-8-00; (<b>b</b>) BRTSC-8-05; (<b>c</b>) BRTSC-8-10; (<b>d</b>) BRTSC-8-15; (<b>e</b>) BRTSC-10-10; (<b>f</b>) BRTSC-12-10 (w represents crack width).</p>
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<p>Crack patterns and failure of beams of BRTSC: (<b>a</b>) BRTSC-8-00; (<b>b</b>) BRTSC-8-05; (<b>c</b>) BRTSC-8-10; (<b>d</b>) BRTSC-8-15; (<b>e</b>) BRTSC-10-10; (<b>f</b>) BRTSC-12-10 (w represents crack width).</p>
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<p>Crack development process of beams measured by 3D-DIC: (<b>a</b>) BRTSC-8-00; (<b>b</b>) BRTSC-8-05; (<b>c</b>) BRTSC-8-10; (<b>d</b>) BRTSC-8-15; (<b>e</b>) BRTSC-10-10; (<b>f</b>) BRTSC-12-10.</p>
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<p>Crack development in beam under flexural loading: (<b>a</b>) BRTSC-8-00; (<b>b</b>) BRTSC-8-05; (<b>c</b>) BRTSC-8-10; (<b>d</b>) BRTSC-8-15; (<b>e</b>) BRTSC-10-10; (<b>f</b>) BRTSC-12-10. (The numbers in the figure represent the load values and the numbers in parentheses represent the order in which the cracks appeared).</p>
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<p>Crack development in beam under flexural loading: (<b>a</b>) BRTSC-8-00; (<b>b</b>) BRTSC-8-05; (<b>c</b>) BRTSC-8-10; (<b>d</b>) BRTSC-8-15; (<b>e</b>) BRTSC-10-10; (<b>f</b>) BRTSC-12-10. (The numbers in the figure represent the load values and the numbers in parentheses represent the order in which the cracks appeared).</p>
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<p>Load versus maximum crack width: (<b>a</b>) beams with different RTSF volume fractions; (<b>b</b>) beams with different BFRP reinforcement ratios.</p>
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<p>Load–deflection response at mid-span for concrete beams: (<b>a</b>) beams with different RTSF volume fractions; (<b>b</b>) beams with different BFRP reinforcement ratios.</p>
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<p>Strains of concrete at different positions along the height of beams under various loads: (<b>a</b>) BRTSC-8-00; (<b>b</b>) BRTSC-8-05; (<b>c</b>) BRTSC-8-10; (<b>d</b>) BRTSC-8-15; (<b>e</b>) BRTSC-10-10; (<b>f</b>) BRTSC-12-10.</p>
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<p>Strains of concrete at different positions along the height of beams under various loads: (<b>a</b>) BRTSC-8-00; (<b>b</b>) BRTSC-8-05; (<b>c</b>) BRTSC-8-10; (<b>d</b>) BRTSC-8-15; (<b>e</b>) BRTSC-10-10; (<b>f</b>) BRTSC-12-10.</p>
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<p>Load–strain response at the mid-span of basalt reinforcement in beams: (<b>a</b>) beams with different RTSF volume fractions; (<b>b</b>) beams with different BFRP reinforcement ratios.</p>
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<p>The calculation diagram of the flexural capacity of the beam section: (<b>a</b>) section; (<b>b</b>) strain distribution; (<b>c</b>) stress distribution; (<b>d</b>) equivalent rectangular stress distribution.</p>
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20 pages, 9338 KiB  
Article
Application of Active Heating Tests with the Distributed Temperature Sensing to Characterize Flow Dynamics in a Tidal-Influenced Coastal Aquifer
by Yu-Huan Chang, Chuen-Fa Ni, Chi-Ping Lin, Chia-Yu Hsu, An-Yi Hsu, Nguyen Hoang Hiep and Doan Thi Thanh Thuy
Water 2024, 16(24), 3631; https://doi.org/10.3390/w16243631 - 17 Dec 2024
Viewed by 343
Abstract
Aquifer storage and recovery have gained attention as a solution that utilizes submarine groundwater discharge (SGD) as a surrogate water resource to alleviate water scarcity and fill the demand gap. Characterizing SGD is crucial for using coastal groundwater and improving understanding of the [...] Read more.
Aquifer storage and recovery have gained attention as a solution that utilizes submarine groundwater discharge (SGD) as a surrogate water resource to alleviate water scarcity and fill the demand gap. Characterizing SGD is crucial for using coastal groundwater and improving understanding of the interaction between continental water and seawater. This study employs fiber-optical distributed temperature sensing (FODTS) and the heat tracer to quantify the groundwater flux in a coastal aquifer in northern Taiwan. The fluxes in different sections along the borehole were estimated from the temperature response caused by the active heating tests and campier groundwater flux under different tidal conditions, providing information on potential water resources for water resource planning and management. According to the active heating tests, the material of the sections with high-temperature response mainly consists of a gravel–sand mixture. Based on the estimations of groundwater fluxes along the well, the sections with low sensitivity of temperature response have low hydraulic conductivity and low groundwater flux. The estimated thermal parameters at the site are consistent with those obtained from the borehole samples in the laboratory tests. The groundwater fluxes in different sections are calculated based on the temperature response observed from the FODTS. The groundwater fluxes along the well vary between 0.02 and 1.77 m/day. There are considerable differences between the estimated fluxes during the tidal cycle in a heterogeneous coastal aquifer, indicating the high uncertainty of estimated SGD along coastlines. Full article
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<p>The geological map of the study area is divided into (I) the western Hsuehshan Range belt, (II) the western foothills province, and (III) the Taoyuan–Zhongli tablelands.</p>
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<p>The borehole data and the conceptual model of the coastal aquifer at the site: (<b>a</b>) The material types of each layer were obtained from the core samples; (<b>b</b>) The conceptual model (not to scale) of the groundwater flow at the site was based on observations from the borehole drilling logs and previous investigations that showed the artesian wells in the intertidal zone.</p>
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<p>The site-specific conditions and the facilities for the study site: (<b>a</b>) The aerial shot of the study area near the coastline; (<b>b</b>) the configuration of the well field and the locations of well BW02; (<b>c</b>) the orange line is background groundwater level and the blue line is temperature measured in well BW01; and (<b>d</b>) the field configuration of the active heating test setup.</p>
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<p>The experimental periods for different cases as compared to the tidal variations. The red lines indicate the heating period, and the blue lines indicate the cooling periods during the active heating tests, and the dotted line indicates the time before and after the tests.</p>
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<p>The geological profile of BW02 obtained from the core samples and the temperature profile of BW02 during Case 1. The red dashed lines indicate the periods of different heating powers.</p>
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<p>The comparison of the results for four heating cases. The time duration of Case 2 and Case 3 is a half-tidal period, and Case 4 and Case 5 are a full-tidal period. The temperature variation with time shows the tidal condition influences groundwater flow with time. Prominent heat accumulation portions are in the well casing sections located on the top and bottom of the well.</p>
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<p>The dotted line indicates the contour of temperature variation during the heating period and the red line indicates groundwater level of Case 4 under the tidal cycle condition. The increase and decrease in groundwater water levels simultaneously reflect the tidal variations because of the short distance from the well to the coastline.</p>
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<p>Comparison between the estimated and measured temperature, the residuals, and the noise in Cases 4 and 5.</p>
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<p>Comparison between the estimated and measured temperature, the residuals, and the noise in Cases 2 and 3.</p>
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<p>Fitting parameters A and B for estimating groundwater fluxes along the observation well. The black and red lines are the groundwater flux of Cases 2 and 3, respectively.</p>
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<p>Estimation of the groundwater fluxes of BW02 under different tidal conditions. The black and green lines are the groundwater flux of Cases 2 and 3, respectively.</p>
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<p>The comparison between the geological logging, the temperature response, and the estimated groundwater flux from Case 2.</p>
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<p>The comparison between the geological loggings, the temperature response, and the estimated groundwater flux from Case 3.</p>
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14 pages, 9062 KiB  
Article
Dual-Band High-Throughput and High-Contrast All-Optical Topology Logic Gates
by Jinying Zhang, Yulin Si, Yexiaotong Zhang, Bingnan Wang and Xinye Wang
Micromachines 2024, 15(12), 1492; https://doi.org/10.3390/mi15121492 - 13 Dec 2024
Viewed by 532
Abstract
Optical computing offers advantages such as high bandwidth and low loss, playing a crucial role in signal processing, communication, and sensing applications. Traditional optical logic gates, based on nonlinear fibers and optical amplifiers, suffer from poor robustness and large footprints, hindering their on-chip [...] Read more.
Optical computing offers advantages such as high bandwidth and low loss, playing a crucial role in signal processing, communication, and sensing applications. Traditional optical logic gates, based on nonlinear fibers and optical amplifiers, suffer from poor robustness and large footprints, hindering their on-chip integration. All-optical logic gates based on topological photonic crystals have emerged as a promising approach for developing robust and monolithic optical computing systems. Expanding topological photonic crystal logic gates from a single operating band to dual bands can achieve high throughput, significantly enhancing parallel computing capabilities. This study integrates the topological protection offered by valley photonic crystals with linear interference effects to design and implement seven optical computing logic gates on a silicon substrate. These gates, based on dual-band valley photonic crystal topological protection, include OR, XOR, NOT, NAND, NOR, and AND. The robustness of the implemented OR logic gates was verified in the presence of boundary defects. The results demonstrate that multi-band parallel computing all-optical logic gates can be achieved using topological photonic crystals, and these gates exhibit high robustness. The all-optical logic gates designed in this study hold significant potential for future applications in optical signal processing, optical communication, optical sensing, and other related areas. Full article
(This article belongs to the Special Issue Photonic and Optoelectronic Devices and Systems, Second Edition)
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<p>Schematic of two-dimensional photonic crystal structure and its band structures. (<b>a</b>) Schematic of photonic crystal structure with <span class="html-italic">θ</span> = 0°; (<b>b</b>) view of the first Brillouin zone of a triangular lattice, dashed triangle marked <span class="html-italic">k</span>-path for band calculation; (<b>c</b>) photonic crystal band structure with <span class="html-italic">θ</span> = 0°; (<b>d</b>) schematic of photonic crystal rotation structure at <span class="html-italic">θ</span> = 5° (blue represents scattered body at <span class="html-italic">θ</span> = 0°, red represents scatterer at <span class="html-italic">θ</span> = 5°); (<b>e</b>) photonic crystal band structure with <span class="html-italic">θ</span> = 5°; (<b>f</b>) schematic of photonic crystal rotation structure at <span class="html-italic">θ</span> = −5° (blue represents scattered body at <span class="html-italic">θ</span> = 0°, red represents scatterer at <span class="html-italic">θ</span> = −5°); (<b>e</b>) photonic crystal band structure with <span class="html-italic">θ</span> = 5°; the curves in (<b>e</b>,<b>g</b>) represent the first band, second band, third band, fourth band, and fifth band in sequence from top to bottom.</p>
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<p>Schematic of AC-type supercell structure with zigzag-type boundary and its band structure. (<b>a</b>) Schematic diagram of AC-type supercell structure; (<b>b</b>) the band structure of the AC-type supercell structure in Gap I; (<b>c</b>) the band structure of the AC-type supercell structure in Gap II. Dashed lines represent both the intrinsic bulk and edge states of the photonic crystal. Refer to the main text for details on their differentiation based on energy and momentum.</p>
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<p>Design diagram of “OR” and “XOR” gate.</p>
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<p>The calculation results of the light field distribution in the logical states of “OR” gate and “XOR” gate. (<b>a</b>) “OR/XOR” gate logic input state 01, logic output state 1 (OR_01(XOR_01)); (<b>b</b>) “OR/XOR” gate logic input state 10, logic output state 1 (OR_10(XOR_10)); (<b>c</b>) “OR” gate logic input state 11, logic output state 1 (OR_11); (<b>d</b>) “XOR” gate logic input state 11, logic output state 0 (XOR_11). The color scale represents the magnitude of the electric field (V/m) obtained directly from simulations.</p>
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<p>Design diagram of “NOT”, “NAND”, “NOR”, and “XNOR” gates.</p>
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<p>Calculation results of the light field distribution in the logic state of the “NOT” gate. (<b>a</b>) “NOT” gate logic input state 00, logic output state 1 (NOT_00); (<b>b</b>) “NOT” gate logic input state 01, logic output state 1 (NOT_01); (<b>c</b>) “NOT” gate logic input state 10, logic output state (0NOT_10); (<b>d</b>) “NOT” gate logic input state 11, logic output state 0 (NOT_11). The color scale represents the magnitude of the electric field, and the scale is adjusted to best visualize the field distribution.</p>
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<p>The calculation result of the optical field distribution in the “NAND” gate logic state. (<b>a</b>) “NAND” gate logic input state 00, the logic output state 1 (NAND_00); (<b>b</b>) “NAND” gate logic input state 01, logic output state 1 (NAND_01); (<b>c</b>) “NAND” gate logic input state 10, logic output state 1 (NAND_10); (<b>d</b>) “NAND” gate logic input state 11, logic output state 0 (NAND_11).</p>
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<p>The calculation result of the optical field distribution in the “NOR” gate logic state. (<b>a</b>) “NOR” gate logic input state 00, the logic output state 1 (NOR_00); (<b>b</b>) “NOR” gate logic input state 01, logic output state 0 (NOR_01); (<b>c</b>) “NOR” gate logic input state 10, logic output state 0 (NOR_10); (<b>d</b>) “NOR” gate logic input state 11, logic output state 0 (NOR_11).</p>
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<p>Calculation results of optical field distribution in “XNOR” gate logic state. (<b>a</b>) “XNOR” gate logic input state 00, logic output state 1 (XNOR_00); (<b>b</b>) “XNOR” gate logic input state 01, logic output state 0 (XNOR_01); (<b>c</b>) “XNOR” gate logic input state 10, logic output state 0 (XNOR_10); (<b>d</b>) “XNOR” gate logic input state 11, logic output state 1 (XNOR_11).</p>
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<p>Design diagram of “AND” gate.</p>
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<p>Calculation results of the light field distribution in the logic state of the “AND” gate. (<b>a</b>) “AND” gate logic input state 00, logic output state 0 (AND_00); (<b>b</b>) “AND” gate logic input state 01, logic output state 0 (AND_01); (<b>c</b>) “AND” gate logic input state 10, logic output state_ 0 (AND_10); (<b>d</b>) “AND” gate logic input state 11, logic output state 1 (AND_11).</p>
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<p>The calculation results of optical field distribution for AC-type “OR/XOR” gate logic states at 281.95 THz (1064 nm). (<b>a</b>) “OR/XOR” gate logic input state 01, logic output state 1 (OR_01(XOR_01)); (<b>b</b>) “OR/XOR” gate logic input state 10, logic output state 1 (OR_10(XOR_10)); (<b>c</b>) “OR” gate logic input state 11, logic output state 1 (OR_11); (<b>d</b>) “XOR” gate logic input state 11, logic output state 0 (XOR_11).</p>
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<p>The calculation results of optical field distribution for ABC-type “OR/XOR” gate logic states at 193.54 THz (1550 nm). (<b>a</b>) “OR/XOR” gate logic input state 01, logic output state 1 (OR_01(XOR_01)); (<b>b</b>) “OR/XOR” gate logic input state 10, logic output state 1 (OR_10(XOR_10)); (<b>c</b>) “OR” gate logic input state 11, logic output state 1 (OR_11); (<b>d</b>) “XOR” gate logic input state 11, logic output state 0 (XOR_11).</p>
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<p>The calculation results of optical field distribution for ABC-type “OR/XOR” gate logic states at 281.95 THz (1064 nm). (<b>a</b>) “OR/XOR” gate logic input state 01, logic output state 1 (OR_01(XOR_01)); (<b>b</b>) “OR/XOR” gate logic input state 10, logic output state 1 (OR_10(XOR_10)); (<b>c</b>) “OR” gate logic input state 11, logic output state 1 (OR_11); (<b>d</b>) “XOR” gate logic input state 11, logic output state 0 (XOR_11).</p>
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<p>The calculation results of field distribution when introducing impurity defect in the “OR” logic gate (rectangular area represents SiO<sub>2</sub> impurity defect). (<b>a</b>) Calculation results of AC-type optical field distribution at 193.54 THz (1550 nm); (<b>b</b>) calculation results of ABC-type optical field distribution at 193.54 THz (1550 nm); (<b>c</b>) calculation results of AC-type optical field distribution at 281.95 THz (1064 nm); (<b>d</b>) calculation results of ABC-type optical field distribution at 281.95 THz (1064 nm).</p>
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15 pages, 4777 KiB  
Article
Multipoint Thermal Sensing System for Power Semiconductor Devices Utilizing Fiber Bragg Gratings
by Ridwanullahi Isa, Naveed Iqbal, Mohammad Abido, Jawad Mirza and Khurram Karim Qureshi
Appl. Sci. 2024, 14(23), 11328; https://doi.org/10.3390/app142311328 - 4 Dec 2024
Viewed by 624
Abstract
This study investigates the feasibility of using fiber Bragg grating (FBG) sensors for multipoint thermal monitoring of several power semiconductor devices (PSDs), such as insulated gate bipolar transistors (IGBTs), and rectifiers assembled on a common heatsink in a three-phase inverter. A novel approach [...] Read more.
This study investigates the feasibility of using fiber Bragg grating (FBG) sensors for multipoint thermal monitoring of several power semiconductor devices (PSDs), such as insulated gate bipolar transistors (IGBTs), and rectifiers assembled on a common heatsink in a three-phase inverter. A novel approach is proposed to integrate FBG sensors beneath the baseplates of the IGBT modules, avoiding the need for invasive modifications to the device structure. By strategically positioning multiple FBG sensors, accurate temperature profiles of critical components can be obtained. The experimental results demonstrate the effectiveness of the proposed method, with the temperature measurements from FBG sensors closely matching those obtained using thermal infrared (IR) cameras within ±1.1 °C. This research highlights the potential of FBG sensors for reliable and precise thermal management in power electronic systems, contributing to improved performance and reliability. Full article
(This article belongs to the Special Issue Recent Advances and Applications of Optical and Acoustic Measurements)
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<p>Schematic of a three-phase inverter.</p>
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<p>Thermal network of a single IGBT module referenced to FBG sensor.</p>
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<p>Thermal resistance network of multiple IGBTs.</p>
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<p>Schematic of the calibration setup.</p>
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<p>Temperature–wavelength correlation of FBG sensors.</p>
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<p>(<b>a</b>) FBG array in a single optical fiber. (<b>b</b>) Installation settings of the sensors in the inverter circuit (<b>c</b>) FIBER1; vertical sensor configuration along the rectifier/IGBT baseplate. (<b>d</b>) FIBER2; horizontal sensor configuration along the rectifier/IGBTs baseplate.</p>
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<p>(<b>a</b>) Tabletop experimental setup. (<b>b</b>) Thermal imaging of the IGBT.</p>
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<p>Observed reflection spectra for the FBG sensors on the optical spectrum analyzer.</p>
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<p>FBG temperature response to varying load power.</p>
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<p>FBG temperature response to varying load power with minimized airgap effect.</p>
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<p>(<b>a</b>) Thermal imaging of IGBT at time T1. (<b>b</b>) Thermal imaging of IGBT at time T2 (where T2 &gt; T1).</p>
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<p>Predictions of hotspots using neural networks.</p>
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14 pages, 3995 KiB  
Article
An Intensity-Variation RI Sensor for Multi-Variant Alcohol Detection with Twisted Structure Using Polymer Optical Fiber
by Abdul Ghaffar, Rehan Mehdi, Irfan Mehdi, Bhagwan Das, Vicky Kumar, Sadam Hussain, Gul Sher, Kamran Ali Memon, Sikandar Ali, Mujahid Mehdi and Khurram Karim Qureshi
Chemosensors 2024, 12(12), 252; https://doi.org/10.3390/chemosensors12120252 - 3 Dec 2024
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Abstract
This research introduces an RI sensor for detecting various alcohol species with a designed twisted polymer optical fiber (POF) sensor. The sensor is developed via a straightforward twisting technique to form an effective coupling mechanism. The sensor works on intensity variation where coupled [...] Read more.
This research introduces an RI sensor for detecting various alcohol species with a designed twisted polymer optical fiber (POF) sensor. The sensor is developed via a straightforward twisting technique to form an effective coupling mechanism. The sensor works on intensity variation where coupled intensity varies when different types of alcohol are added. The structure relies on the twisting of two fibers, where one fiber is used as the illuminating fiber and the other fiber is used as the receiving fiber. Five different types of alcohol are tested (methanol, ethanol, propanol, butanol, and pentanol) as a substant. The experimental results reveal that the sensor is able to detect all five distinct substants effectively by optical power intensity variation. Moreover, the sensor’s sensitivity is analyzed with different factors such as the influence of the bending radius and the coupling length, which reveals that the sensing parameters could be customized depending on specific requirements. The sensor demonstrated consistent responses in repeatability tests, with minimal variation across multiple measurements, highlighting its stability. Additionally, the study explores temperature’s influence, revealing a sensitivity shift for every degree Celsius of change. This POF-based alcohol sensor represents a significant leap forward in optical sensing technology. Full article
(This article belongs to the Special Issue Advanced Chemical Sensors for Gas Detection)
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<p>(<b>a</b>) Sensing mechanism and (<b>b</b>) illustration of sensor fabrication and experimental setup.</p>
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<p>(<b>a</b>) Sensing mechanism and (<b>b</b>) illustration of sensor fabrication and experimental setup.</p>
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<p>Intensity response of the sensor at the end of both fibers over time: (<b>a</b>) illuminating fiber and (<b>b</b>) receiving fiber.</p>
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<p>Response of the transmission spectra in the transmitted port and in the coupled port.</p>
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<p>Measured output power of the twisted sensor under various alcohols.</p>
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<p>Demonstrated alcohol-sensing capabilities configured with an illuminated fiber and a receiving fiber.</p>
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<p>Effect of different bend radii on sensor measurement response.</p>
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<p>Influence of the twisted region’s length on the alcohol sensor’s performance.</p>
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<p>Repeatability sensor response.</p>
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<p>Influence of temperature on the sensor’s performance.</p>
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