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12 pages, 12643 KiB  
Communication
Power Testing of Aspheric Lenses Based on Transmission Phase Deflectometric Method
by Qiong Wu, Xiaokun Wang, Shuangshuang Zhang, Wenhan Li, Yingjing Zhao, Chengchen Zhou, Donglin Xue and Xuejun Zhang
Photonics 2024, 11(8), 756; https://doi.org/10.3390/photonics11080756 - 13 Aug 2024
Abstract
Traditional methods for testing aspheric optical lenses struggle to achieve point-by-point testing across the full aperture of the lens. To facilitate the full-aperture, high-precision, and rapid testing of aspheric optical lenses, a power testing method of lenses based on the transmission phase deflectometric [...] Read more.
Traditional methods for testing aspheric optical lenses struggle to achieve point-by-point testing across the full aperture of the lens. To facilitate the full-aperture, high-precision, and rapid testing of aspheric optical lenses, a power testing method of lenses based on the transmission phase deflectometric technique was employed. This method determines the phase deviation of light caused by the lens, thereby fitting the transmission wavefront and quickly detecting the power distribution information of the lens. This paper constructs a power testing model based on the phase deflectometric technique, proposes a calibration method that combines DLT (direct linear transformation) and pinhole models to reduce system errors, and combines phase extraction and wavefront fitting for experimental verification. The experimental results are compared with those obtained from the commercial visual lens mapper (VM-2000). The central errors of spherical power and cylindrical power are 1% and 0.7%, respectively. This provides a reliable method for the full-aperture, high-precision, and rapid testing of aspheric optical lenses. Full article
(This article belongs to the Special Issue Optical Precision Manufacturing and Testing: Technologies and Trends)
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Figure 1

Figure 1
<p>A schematic diagram of the principle of the transmitted phase deflectometric system for testing the lens refractive power.</p>
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<p>A schematic diagram of the DLT principle used to obtain the external reference matrix.</p>
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<p>A picture of the experimental setup of the transmission phase deflection measurement system.</p>
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<p>Phase map differences obtained with fringe orientations: (<b>a</b>) x direction; (<b>b</b>) y direction.</p>
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<p>(<b>a</b>,<b>c</b>) The spherical power map of the design theoretical value 1 D and 2 D lenses, respectively, obtained using our technique for the lens; (<b>b</b>,<b>d</b>) the cylindrical power map of the design theoretical value −1 D and 0 D lenses, respectively, using our technique.</p>
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<p>(<b>a</b>,<b>c</b>) The spherical power map of the design theoretical value 1 D and 2 D lenses, respectively, obtained using the commercial profilometer VM-2500; (<b>b</b>,<b>d</b>) the cylindrical power map of the design theoretical value −1 D and 0 D lenses, obtained using the commercial profilometer VM-2500 from ANCIENTO in Liaoning, China.</p>
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<p>A schematic diagram of the error optical path introduced when the lens placement is (<b>a</b>) translational, (<b>b</b>) eccentric, and (<b>c</b>) tilted.</p>
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<p>A schematic diagram of the error optical path introduced when the lens placement is (<b>a</b>) translational, (<b>b</b>) eccentric, and (<b>c</b>) tilted.</p>
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<p>The power map obtained when the lens was translated (<b>left</b>: spherical power map; <b>right</b>: cylindrical power map).</p>
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<p>The power map obtained when the lens was placed 5 mm off-center (<b>left</b>: spherical power map; <b>right</b>: cylindric power map).</p>
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<p>The power map obtained when the lens was placed at tilt of 3° (<b>left</b>: spherical power map; <b>right</b>: cylindrical power map).</p>
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28 pages, 4668 KiB  
Article
Visual Reasoning and Multi-Agent Approach in Multimodal Large Language Models (MLLMs): Solving TSP and mTSP Combinatorial Challenges
by Mohammed Elhenawy, Ahmad Abutahoun, Taqwa I. Alhadidi, Ahmed Jaber, Huthaifa I. Ashqar, Shadi Jaradat, Ahmed Abdelhay, Sebastien Glaser and Andry Rakotonirainy
Mach. Learn. Knowl. Extr. 2024, 6(3), 1894-1921; https://doi.org/10.3390/make6030093 (registering DOI) - 13 Aug 2024
Abstract
Multimodal Large Language Models (MLLMs) harness comprehensive knowledge spanning text, images, and audio to adeptly tackle complex problems. This study explores the ability of MLLMs in visually solving the Traveling Salesman Problem (TSP) and Multiple Traveling Salesman Problem (mTSP) using images that portray [...] Read more.
Multimodal Large Language Models (MLLMs) harness comprehensive knowledge spanning text, images, and audio to adeptly tackle complex problems. This study explores the ability of MLLMs in visually solving the Traveling Salesman Problem (TSP) and Multiple Traveling Salesman Problem (mTSP) using images that portray point distributions on a two-dimensional plane. We introduce a novel approach employing multiple specialized agents within the MLLM framework, each dedicated to optimizing solutions for these combinatorial challenges. We benchmarked our multi-agent model solutions against the Google OR tools, which served as the baseline for comparison. The results demonstrated that both multi-agent models—Multi-Agent 1, which includes the initializer, critic, and scorer agents, and Multi-Agent 2, which comprises only the initializer and critic agents—significantly improved the solution quality for TSP and mTSP problems. Multi-Agent 1 excelled in environments requiring detailed route refinement and evaluation, providing a robust framework for sophisticated optimizations. In contrast, Multi-Agent 2, focusing on iterative refinements by the initializer and critic, proved effective for rapid decision-making scenarios. These experiments yield promising outcomes, showcasing the robust visual reasoning capabilities of MLLMs in addressing diverse combinatorial problems. The findings underscore the potential of MLLMs as powerful tools in computational optimization, offering insights that could inspire further advancements in this promising field. Full article
12 pages, 3848 KiB  
Article
Current Measurement of Three-Core Cables via Magnetic Sensors
by Jingang Su, Peng Zhang, Xingwang Huang, Xianhai Pang, Xun Diao and Yan Li
Energies 2024, 17(16), 4007; https://doi.org/10.3390/en17164007 (registering DOI) - 13 Aug 2024
Abstract
Due to their compact structure and low laying cost, three-core power cables are widely used for power distribution networks. The three-phases of such cables are distributed symmetrically with a 120° shift to each other. Phase current is an important parameter to reflect the [...] Read more.
Due to their compact structure and low laying cost, three-core power cables are widely used for power distribution networks. The three-phases of such cables are distributed symmetrically with a 120° shift to each other. Phase current is an important parameter to reflect the operation state of the power system and three-core cable. Three-core symmetrical power cables use a common shield, leading to magnetic field cancelation outside the cable during steady operation. Thus, traditional magnetic-based current transformers cannot measure the phase current on three-core cable non-invasively. In order to measure the phase current more conveniently, a phase current measurement method for three-core cables based on a magnetic sensor is proposed in this paper. Nonlinear equations of a phase current and the magnetic field of a measuring point are constructed. The calculated magnetic field distribution of the three-core cable is verified using a finite element simulation. The effectiveness of the measurement method is further validated through experiments. This proposed method is able to conveniently detect the phase current of three-core power cables, which can help cable maintenance. Full article
(This article belongs to the Special Issue Power Cables in Energy Systems)
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<p>Three-core cable structure.</p>
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<p>Schematic of surface magnetic field-sensing model for three-core cable.</p>
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<p>Mesh diagram of finite element simulation for cable magnetic field.</p>
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<p>Finite element simulation result of magnetic field profile.</p>
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<p>Simulation result of magnetic flux density along radian.</p>
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<p>Finite element simulation of magnetic field without steel wire armor.</p>
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<p>Set values and deduced values and errors of current.</p>
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<p>Laboratory test picture for three-core cable current measurement with magnetic sensors.</p>
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<p>Schematic drawing of the laboratory test.</p>
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<p>Part of the data collected by the experiment.</p>
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<p>Experiment to derive the three-phase cable current. (<b>a</b>) Comparison between the calculated value and the reference value when the current is 20 A. (<b>b</b>) Comparison between the calculated value and the reference value when the current is 30 A. (<b>c</b>) Comparison between the calculated value and the reference value when the current is 60 A.</p>
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<p>Experiment to derive the three-phase cable current. (<b>a</b>) Comparison between the calculated value and the reference value when the current is 20 A. (<b>b</b>) Comparison between the calculated value and the reference value when the current is 30 A. (<b>c</b>) Comparison between the calculated value and the reference value when the current is 60 A.</p>
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25 pages, 23704 KiB  
Article
PE-SLAM: A Modified Simultaneous Localization and Mapping System Based on Particle Swarm Optimization and Epipolar Constraints
by Cuiming Li, Zhengyu Shang, Jinxin Wang, Wancai Niu and Ke Yang
Appl. Sci. 2024, 14(16), 7097; https://doi.org/10.3390/app14167097 - 13 Aug 2024
Abstract
Due to various typical unstructured factors in the environment of photovoltaic power stations, such as high feature similarity, weak textures, and simple structures, the motion model of the ORB-SLAM2 algorithm performs poorly, leading to a decline in tracking accuracy. To address this issue, [...] Read more.
Due to various typical unstructured factors in the environment of photovoltaic power stations, such as high feature similarity, weak textures, and simple structures, the motion model of the ORB-SLAM2 algorithm performs poorly, leading to a decline in tracking accuracy. To address this issue, we propose PE-SLAM, which improves the ORB-SLAM2 algorithm’s motion model by incorporating the particle swarm optimization algorithm combined with epipolar constraint to eliminate mismatches. First, a new mutation strategy is proposed to introduce perturbations to the pbest (personal best value) during the late convergence stage of the PSO algorithm, thereby preventing the PSO algorithm from falling into local optima. Then, the improved PSO algorithm is used to solve the fundamental matrix between two images based on the feature matching relationships obtained from the motion model. Finally, the epipolar constraint is applied using the computed fundamental matrix to eliminate incorrect matches produced by the motion model, thereby enhancing the tracking accuracy and robustness of the ORB-SLAM2 algorithm in unstructured photovoltaic power station scenarios. In feature matching experiments, compared to the ORB algorithm and the ORB+HAMMING algorithm, the ORB+PE-match algorithm achieved an average accuracy improvement of 19.5%, 14.0%, and 6.0% in unstructured environments, respectively, with better recall rates. In the trajectory experiments of the TUM dataset, PE-SLAM reduced the average absolute trajectory error compared to ORB-SLAM2 by 29.1% and the average relative pose error by 27.0%. In the photovoltaic power station scene mapping experiment, the dense point cloud map constructed has less overlap and is complete, reflecting that PE-SLAM has basically overcome the unstructured factors of the photovoltaic power station scene and is suitable for applications in this scene. Full article
(This article belongs to the Special Issue Autonomous Vehicles and Robotics)
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<p>Photovoltaic power plant scene images.</p>
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<p>PE-SLAM system framework diagram.</p>
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<p>Schematic diagram of motion model.</p>
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<p>Schematic diagram of epipolar constraint.</p>
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<p>Schematic diagram of matching point pairs for pole constraint verification.</p>
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<p>Improved mutation strategy for particle perturbation.</p>
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<p>Particle update schematic.</p>
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<p>Optical images of OxfordVGG dataset.</p>
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<p>Influence of important parameters on accuracy and time consuming.</p>
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<p>Influence of important parameters on accuracy and time consuming.</p>
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<p>Line chart of fitness change.</p>
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<p>Matching accuracy based on the data.</p>
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<p>The recall rate of matching results based on the dataset.</p>
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<p>Unstructured scenarios for datasets.</p>
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<p>Trajectory error plot of the structure_notexture sequence.</p>
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<p>Trajectory error plot of the nostructure_texture sequence.</p>
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<p>Trajectory error plot of the structure_texture sequence.</p>
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<p>The 3D map generated from the structure_notexture sequence.</p>
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<p>The 3D map generated from the nostructure_texture sequence.</p>
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<p>The 3D map generated from the structure_texture sequence.</p>
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<p>Robot model based on Gazebo.</p>
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<p>Photovoltaic power station simulation scene based on Gazebo.</p>
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<p>Trajectory error plot of the Si.</p>
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<p>The 3D map generated from the Si.</p>
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<p>Partial images of indoor scenes.</p>
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<p>Partial images of outdoor scenes.</p>
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<p>The 3D map generated from In sequence.</p>
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<p>The 3D map generated from Real sequence.</p>
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14 pages, 293 KiB  
Article
Extensions of Orders to a Power Set vs. Scores of Hesitant Fuzzy Elements: Points in Common of Two Parallel Theories
by Esteban Induráin, Ana Munárriz and M. Sergio Sara
Axioms 2024, 13(8), 549; https://doi.org/10.3390/axioms13080549 - 13 Aug 2024
Abstract
We deal with two apparently disparate theories. One of them studies extensions of orderings from a set to its power set. The other one defines suitable scores on hesitant fuzzy elements. We show that both theories have the same mathematical substrate. Thus, important [...] Read more.
We deal with two apparently disparate theories. One of them studies extensions of orderings from a set to its power set. The other one defines suitable scores on hesitant fuzzy elements. We show that both theories have the same mathematical substrate. Thus, important possibility/impossibility results concerning criteria for extensions can be transferred to new results on scores. And conversely, conditions imposed a priori on scores can give rise to new extension criteria. This enhances and enriches both theories. We show examples of translations of classical results on extensions in the context of scores. Also, we state new results concerning the impossibility of finding a utility function representing some kind of extension order if some restrictions are imposed on the utility function considered as a score. Full article
22 pages, 7639 KiB  
Article
Evaluation of the Effectiveness of Solar Array Simulators in Reproducing the Characteristics of Photovoltaic Modules
by Valdemar Moreira Cavalcante Junior, Rafael C. Neto, Eduardo José Barbosa, Fabrício Bradaschia, Marcelo Cabral Cavalcanti and Gustavo Medeiros de Souza Azevedo
Sustainability 2024, 16(16), 6932; https://doi.org/10.3390/su16166932 - 13 Aug 2024
Abstract
The search for energy alternatives in the face of growing global demand highlights solar energy as a promising and sustainable option that is fundamental in reducing carbon emissions and mitigating climate change. In this context, inverters play a key role in connecting and [...] Read more.
The search for energy alternatives in the face of growing global demand highlights solar energy as a promising and sustainable option that is fundamental in reducing carbon emissions and mitigating climate change. In this context, inverters play a key role in connecting and distributing solar energy, requiring certification through specific tests. Given environmental unpredictability and economic challenges, the use of Solar Array Simulators (SASs) is recommended to accurately replicate the behavior of photovoltaic modules under various conditions. This study analyzes the static and dynamic performances of SASs with the aim of ensuring a faithful reproduction of module behavior in real situations under both steady-state and transient conditions. The primary focus is to ensure that experimental results are reliable and representative, promoting the implementation of more efficient energy solutions. Additionally, this study discusses the importance of optimizing inverter controllers to reflect the more realistic dynamics provided by SASs. Full article
(This article belongs to the Section Energy Sustainability)
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Figure 1
<p>Examples of PV curve-generating elements for inverter and MPPT algorithm testing: (<b>a</b>) PV module; (<b>b</b>) SAS.</p>
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<p>Standard structure of an SAS.</p>
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<p>Graphic interfaces of SAS systems: (<b>a</b>) Chroma [<a href="#B21-sustainability-16-06932" class="html-bibr">21</a>]; (<b>b</b>) Ecosense [<a href="#B22-sustainability-16-06932" class="html-bibr">22</a>]; (<b>c</b>) Keysight [<a href="#B23-sustainability-16-06932" class="html-bibr">23</a>]; (<b>d</b>) Regatron [<a href="#B24-sustainability-16-06932" class="html-bibr">24</a>].</p>
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<p>Configuration 1—Schematic for the experiments related to the behavior of the sources (SAS + RC load).</p>
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<p>Configuration 2—Schematic of the experiments related to the behavior of the sources (SAS + buck–boost converter).</p>
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<p>Evaluation of the steady-state behavior of SASs: obtaining I–V curves with the buck–boost converter for the configuration of a module with irradiance ranging from 200 to 1000 W/m<sup>2</sup>.</p>
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<p>Evaluation of the steady-state behavior of SASs: obtaining PV Curves with the buck–boost converter for the configuration of a module with irradiance ranging from 200 to 1000 W/m<sup>2</sup>.</p>
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<p>Evaluation of the steady-state behavior of emulated sources: obtaining I–V Curves with the buck–boost converter for the configuration of six modules with irradiance ranging from 200 to 1000 W/m<sup>2</sup>.</p>
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<p>Evaluation of the steady-state behavior of emulated sources: obtaining I–V curves with the buck–boost converter for the configuration of six modules with irradiance ranging from 200 to 1000 W/m<sup>2</sup>.</p>
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<p>Behavior of the evaluated sources for a transient in the I–V curve from 1000 to 600 W/m<sup>2</sup>. Results obtained for sources connected in a fixed duty cycle buck–boost converter.</p>
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<p>Behavior of SAS A in response to an RC load step, applying loads with different time constants (<math display="inline"><semantics> <mi>τ</mi> </semantics></math>): 12.53 ms (configuration 1), 125.30 ms (configuration 10), and 376.00 ms (configuration 13). (<b>a</b>) Path on the I–V curve; (<b>b</b>) voltage variation; (<b>c</b>) current variation.</p>
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<p>Behavior of SAS B in response to an RC load step, applying loads with different time constants (<math display="inline"><semantics> <mi>τ</mi> </semantics></math>): 12.53 ms (configuration 1), 125.30 ms (configuration 10), and 376.00 ms (configuration 13). (<b>a</b>) Path on the I–V curve; (<b>b</b>) voltage variation; (<b>c</b>) current variation.</p>
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<p>Transient behavior of current and voltage of the evaluated SAS for shaded curves using the GCCMP technique (case 1). (<b>a</b>) voltage variation; (<b>b</b>) current variation.</p>
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<p>Trajectory followed by the evaluated SAS regarding the PV curves, considering shaded curves and using the GCCMP technique (case 1).</p>
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<p>Trajectory followed by the evaluated SAS regarding the PV curves, considering shaded curves and using the GCCMP technique (case 2).</p>
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16 pages, 18233 KiB  
Article
Electromagnetic–Structural Finite Element Analysis of Copper and Aluminum Windings in Power Transformers under Short-Circuit Conditions
by Richard Gonçalves Cornelius, Betina Luísa Lenhard, Leonardo Hautrive Medeiros, Herber Cuadro Fontoura, Cristian Hans Correa, Rodinei Carraro, Rafael Concatto Beltrame, Tiago dos Santos, Tiago Bandeira Marchesan and Vitor Cristiano Bender
Energies 2024, 17(16), 3994; https://doi.org/10.3390/en17163994 - 12 Aug 2024
Viewed by 200
Abstract
Electromagnetic forces can lead to the structural failure of power transformers due to extreme loading conditions, vibration, and/or fatigue. Therefore, studying the nature and the magnitude of these forces is a key task in the design and failure analysis of such important equipment. [...] Read more.
Electromagnetic forces can lead to the structural failure of power transformers due to extreme loading conditions, vibration, and/or fatigue. Therefore, studying the nature and the magnitude of these forces is a key task in the design and failure analysis of such important equipment. Keeping this issue in mind, this work aims at conducting a numerical analysis in order to evaluate the mechanical stresses and displacements of windings in power transformers due to the action of electromagnetic forces. With this purpose, a finite element model is developed considering electromagnetic and mechanical effects assuming short-circuit conditions. The study compares the cases employing copper and aluminum windings with header tap, in different temperatures. The model developed in this work is verified against analytical solutions. The numerical calculations allow for performing a detailed analysis in terms of the distribution of both displacements and stresses along the windings, which is of great relevance for identifying critical structural points and avoiding structural failure. Overall, the obtained results demonstrate that the finite element model is a useful tool for the structural design of power transformers that allow for investigating and optimizing key aspects before manufacturing. Full article
(This article belongs to the Special Issue Design and Optimization of Power Transformer Diagnostics II)
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Figure 1
<p>Forces in concentric windings with a tap in the head on the outer winding.</p>
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<p>Ampère-turn residual method tap located at the head of the external winding.</p>
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<p>Elastic stiffness according to temperature.</p>
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<p>Model to determine axial stresses: (<b>a</b>) Double-embedded beam model. (<b>b</b>) Disc section between radial spacers.</p>
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<p>Tilting effect due to axial forces.</p>
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<p>Model used to determine the radial stresses on the outer winding.</p>
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<p>Active part constructive characteristics.</p>
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<p>Finite element model: (<b>a</b>) Isometric view. (<b>b</b>) Side view. (<b>c</b>) Top view.</p>
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<p>Structural model for mechanical analysis.</p>
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<p>Electromagnetic forces in a high-voltage winding: (<b>a</b>) axial forces (N), (<b>b</b>) radial forces (N).</p>
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<p>Axial stress distribution along the segment.</p>
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<p>Axial displacement distribution along the segment.</p>
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<p>Axial displacement comparison considering copper and aluminum.</p>
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<p>Analysis of segment 1 of disc 57: (<b>a</b>) Axial Stress. (<b>b</b>) Axial Displacement.</p>
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<p>Radial stress distribution along the segment.</p>
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<p>Radial displacement: (<b>a</b>) Displacement distribution along the segment. (<b>b</b>) Comparison of the resulting copper and aluminum displacements.</p>
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18 pages, 4783 KiB  
Article
Designing a Hybrid Energy-Efficient Harvesting System for Head- or Wrist-Worn Healthcare Wearable Devices
by Zahra Tohidinejad, Saeed Danyali, Majid Valizadeh, Ralf Seepold, Nima TaheriNejad and Mostafa Haghi
Sensors 2024, 24(16), 5219; https://doi.org/10.3390/s24165219 - 12 Aug 2024
Viewed by 204
Abstract
Battery power is crucial for wearable devices as it ensures continuous operation, which is critical for real-time health monitoring and emergency alerts. One solution for long-lasting monitoring is energy harvesting systems. Ensuring a consistent energy supply from variable sources for reliable device performance [...] Read more.
Battery power is crucial for wearable devices as it ensures continuous operation, which is critical for real-time health monitoring and emergency alerts. One solution for long-lasting monitoring is energy harvesting systems. Ensuring a consistent energy supply from variable sources for reliable device performance is a major challenge. Additionally, integrating energy harvesting components without compromising the wearability, comfort, and esthetic design of healthcare devices presents a significant bottleneck. Here, we show that with a meticulous design using small and highly efficient photovoltaic (PV) panels, compact thermoelectric (TEG) modules, and two ultra-low-power BQ25504 DC-DC boost converters, the battery life can increase from 9.31 h to over 18 h. The parallel connection of boost converters at two points of the output allows both energy sources to individually achieve maximum power point tracking (MPPT) during battery charging. We found that under specific conditions such as facing the sun for more than two hours, the device became self-powered. Our results demonstrate the long-term and stable performance of the sensor node with an efficiency of 96%. Given the high-power density of solar cells outdoors, a combination of PV and TEG energy can harvest energy quickly and sufficiently from sunlight and body heat. The small form factor of the harvesting system and the environmental conditions of particular occupations such as the oil and gas industry make it suitable for health monitoring wearables worn on the head, face, or wrist region, targeting outdoor workers. Full article
(This article belongs to the Special Issue Wearable Sensors for Human Health Monitoring and Analysis)
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<p>(<b>a</b>) The block diagram of the hybrid energy harvesting system; (<b>b</b>) proposed development of the hybrid energy harvesting system.</p>
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<p>Comparison of several examples of commercial energy harvesting ICs used for PV/TEG energy sources.</p>
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<p>The proposed multi-port energy harvesting system.</p>
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<p>Circuit schematic of the BQ25504 ultra-low-power DC/DC boost converter.</p>
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<p>Hardware implementation of the prototype energy harvesting system on glasses as a wearable device, which are worn on the human body.</p>
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<p>Exchange of PV/TEG power, battery, and wearable sensor node power in different weather conditions.</p>
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<p>The power demand of the PV energy harvesting system under the various resistive loads.</p>
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<p>Efficiency and power losses of the PV energy harvesting system under various resistive loads.</p>
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<p>The power demand of the TEG energy harvesting system under the various resistive loads.</p>
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<p>Efficiency and power losses of the TEG energy harvesting system under various resistive loads.</p>
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<p>The contribution of hybrid energy harvesting resources in supplying the output load in shadow conditions.</p>
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<p>Power contribution of the hybrid energy harvesting system for wearable sensor node.</p>
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<p>Energy harvesting system efficiency and P<sub>loss</sub>.</p>
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25 pages, 10387 KiB  
Article
Aftermaths of COVID-19 Lockdown on Socioeconomic and Psychological Nexus of Urban Population: A Case in Hyderabad, Pakistan
by Mir Aftab Hussain Talpur, Shabir Hussain Khahro, Muhammad Saad Khan, Fahad Ahmed Shaikh and Yasir Javed
Societies 2024, 14(8), 150; https://doi.org/10.3390/soc14080150 - 12 Aug 2024
Viewed by 191
Abstract
The COVID-19 pandemic started in the last week of December, 2019. An emergency was declared throughout the globe as the virus spread over 208 counties within a short amount of time. This pandemic had significant negative impacts on common men living in densely [...] Read more.
The COVID-19 pandemic started in the last week of December, 2019. An emergency was declared throughout the globe as the virus spread over 208 counties within a short amount of time. This pandemic had significant negative impacts on common men living in densely populated countries, including Pakistan. Hence, this research aimed to record people’s perception of the 7th largest settlement in Pakistan, namely Hyderabad. This study mainly focused on socioeconomic and psychological parameters. The close-ended questionnaire was designed concerning the Depression, Anxiety, and Stress Scale (DASS-21). The DASS-21 is an optimal tool for recording the emotional values of depression, anxiety, and stress. A total of 400 questionnaires were filled out; they used a 5-point Likert scale. Significant socioeconomic issues were noted, such as lower household income, economic recession, job cuts, inaccessible Internet services during online teaching or working from home, etc. The primary challenges in the lockdown situation were Internet access (4.06) and anxiety (4.86) in the female population. There were higher levels of depression (N = 200), anxiety (N = 341), and stress (N = 125) in the local inhabitants. Other notable problems were illuminated, such as restrictions on social gatherings, electricity load shedding, and lower incomes. This study concludes that the degree of psychological problems varied according to the typology of gender. Based on study findings, this study recommends the prompt execution of policies considering possible future pandemics to restrain anxiety and depression in the female population. The local government is also advised to revitalize infrastructure to provide uninterrupted power supplies and Internet facilities. The income-generating channels should be open for lower-income households concerning future lockdowns. Full article
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<p>The number of students impacted by Pakistan’s educational institutions closing due to COVID-19 [<a href="#B30-societies-14-00150" class="html-bibr">30</a>].</p>
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<p>Economic growth in South Asian countries from 2014 to 2021 [<a href="#B32-societies-14-00150" class="html-bibr">32</a>].</p>
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<p>Urban land-use map of District Hyderabad, Pakistan.</p>
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<p>Research design diagram.</p>
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<p>COVID-19’s theoretical framework.</p>
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<p>Barriers to remote working.</p>
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<p>Disturbance factors regarding online education.</p>
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<p>Identification of main factors during a pandemic.</p>
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<p>Public perception about the government’s role during the pandemic.</p>
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<p>Factors of public perception about the government’s stability.</p>
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<p>Lockdown affected students’ ability to learn.</p>
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<p>Social issues during lockdown.</p>
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<p>Poverty statistics during lockdown.</p>
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<p>Role of non-governmental social welfare organizations during the lockdown.</p>
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<p>Levels of depression.</p>
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<p>Level of anxiety.</p>
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<p>Level of stress.</p>
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31 pages, 6910 KiB  
Article
An MPPT Control Strategy Based on Current Constraint Relationships for a Photovoltaic System with a Battery or Supercapacitor
by Guohong Lai, Guoping Zhang and Shaowu Li
Energies 2024, 17(16), 3982; https://doi.org/10.3390/en17163982 - 11 Aug 2024
Viewed by 383
Abstract
When the battery or supercapacitor is connected to the output of a PV system, the conventional voltage equation expressing its mathematical model usually must be replaced by the current relationship to study the maximum power point tracking (MPPT) control theory. However, hitherto, there [...] Read more.
When the battery or supercapacitor is connected to the output of a PV system, the conventional voltage equation expressing its mathematical model usually must be replaced by the current relationship to study the maximum power point tracking (MPPT) control theory. However, hitherto, there is a lack of an attempt to disclose the current constraint relationships at the maximum power point (MPP), which leads to the potential risk of MPPT failure. To solve this problem, in this paper, the MPPT constraint conditions on the basis of currents are built and then a new MPPT control strategy is proposed. In this strategy, a linearized model parameter of a PV cell is used as the bridge to find the current relationships. On the basis of them, some expressions involving the duty cycle are built to directly calculate the control signal of the MPPT controller. Meanwhile, an implementation method is designed to match this proposed MPPT strategy. Finally, some simulation experiments are conducted. The simulation results verify that the proposed MPPT constraint expressions are accurate and workable and that the proposed MPPT strategy and its implementation process are feasible and available. In addition, the simulation results also show that the proposed MPPT strategy has a better MPPT speed and the same MPPT accuracy when the P&O method and fuzzy algorithm are compared. By this work, the MPPT constraint conditions based on current relationships are first found, representing a breakthrough in disclosing the inherent relationships between different currents when the PV system is operating around the MPP. Full article
(This article belongs to the Section A2: Solar Energy and Photovoltaic Systems)
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<p>Configuration of PV system with battery or supercapacitor.</p>
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<p>Linear equivalent model of PV cell at the MPP.</p>
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<p>Equivalent model of PV system with battery.</p>
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<p>Equivalent model of PV system with supercapacitor.</p>
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<p>Structure of the whole system.</p>
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<p>Flow chart of the main control process.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves with 400 W/m<sup>2</sup> and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> values.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves with 600 W/m<sup>2</sup> and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> values.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves with 800 W/m<sup>2</sup> and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> values.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves with 1000 W/m<sup>2</sup> and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> values.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves under 0 °C and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> conditions.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves under 15 °C and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> conditions.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves under 30 °C and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> conditions.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mi>o</mi> </msub> <mo>−</mo> <mi>D</mi> </mrow> </semantics></math> curves under 45 °C and various <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> conditions.</p>
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<p>Curve of <span class="html-italic">S</span> in first group.</p>
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<p>Compared curves of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>o</mi> </msub> </mrow> </semantics></math> in first group.</p>
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<p>Curve of <span class="html-italic">D</span> in first group.</p>
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<p>Curves of three currents in first group.</p>
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<p>Curve of <span class="html-italic">T</span> in second group.</p>
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<p>Curves of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>o</mi> </msub> </mrow> </semantics></math> in second group.</p>
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<p>Curve of <span class="html-italic">D</span> in second group.</p>
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<p>Curves of three currents in second group.</p>
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<p>Curve of <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mi>S</mi> <mi>u</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> in third group.</p>
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<p>Curves of <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>o</mi> </msub> </mrow> </semantics></math> in third group.</p>
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<p>Curve of <span class="html-italic">D</span> in third group.</p>
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<p>Curves of three currents in third group.</p>
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<p>Curve of the varying irradiance.</p>
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<p>Curve of the varying temperature.</p>
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<p>Compared duty cycle curves of three MPPT methods.</p>
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<p>Compared power curves of three MPPT methods.</p>
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<p>Compared output current curves of three MPPT methods.</p>
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<p>Compared curves of <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>s</mi> <mi>M</mi> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mn>2</mn> <msub> <mi>I</mi> <mrow> <mi>o</mi> <mi>M</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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12 pages, 1531 KiB  
Article
Blistering Behavior of Beryllium and Beryllium Alloy under High-Dose Helium Ion Irradiation
by Ping-Ping Liu, Qi-Cong Wang, Yu-Mei Jia, Wen-Tuo Han, Xiao-Ou Yi, Qian Zhan and Fa-Rong Wan
Materials 2024, 17(16), 3997; https://doi.org/10.3390/ma17163997 - 11 Aug 2024
Viewed by 267
Abstract
Beryllium (Be) has been selected as the solid neutron multiplier material for a tritium breeding blanket module in ITER, which is also the primary option of the Chinese TBM program. But the irradiation swelling of beryllium is severe under high temperature, high irradiation [...] Read more.
Beryllium (Be) has been selected as the solid neutron multiplier material for a tritium breeding blanket module in ITER, which is also the primary option of the Chinese TBM program. But the irradiation swelling of beryllium is severe under high temperature, high irradiation damage and high doses of transmutation-induced helium. Advanced neutron multipliers with high stability at high temperature are desired for the demonstration power plant (DEMO) reactors and the China Fusion Engineering Test Reactor (CFETR). Beryllium alloys mainly composed of Be12M (M is W or Ti) phase were fabricated by HIP, which has a high melting point and high beryllium content. Beryllium and beryllide (Be12Ti and Be12W) samples were irradiated by helium ion with 30 keV and 1 × 1018 cm−2 at RT. The microstructures of Be, Be12Ti and Be12W samples were analyzed by SEM and TEM before and after ion irradiation. The average size of the first blistering on the surface of Be-W alloy is about 0.8 μm, and that of secondary blistering is about 79 nm. The surface blistering rates of the beryllium and beryllide samples were also compared. These results may provide a preliminary experimental basis for evaluating the irradiation swelling resistance of beryllium alloy. Full article
19 pages, 5543 KiB  
Article
Research on Maximum Longitudinal Slope and the Length Limit of Expressways Based on the Performance of Pure Electric Heavy-Duty Vehicles
by Yulong Pei, Lintao Hu, Sheng Pan and Yuhang Wen
Appl. Sci. 2024, 14(16), 7043; https://doi.org/10.3390/app14167043 - 11 Aug 2024
Viewed by 440
Abstract
With the global energy transition and advancements in electric vehicle technology, the use of pure electric heavy-duty vehicles in logistics is rising. However, current highway grade design standards do not fully consider their performance characteristics, making it urgent to establish appropriate grade limits. [...] Read more.
With the global energy transition and advancements in electric vehicle technology, the use of pure electric heavy-duty vehicles in logistics is rising. However, current highway grade design standards do not fully consider their performance characteristics, making it urgent to establish appropriate grade limits. This study aims to explore the maximum grade and the critical length suitable for pure electric heavy-duty vehicles on highways. A co-simulation platform for pure electric heavy-duty vehicles was built using TruckSim and MATLAB/Simulink. A comparative analysis was conducted on the climbing characteristics of pure electric heavy-duty vehicles and traditional fuel-powered vehicles. Additionally, the climbing speed decay degree (DV) was introduced to investigate the speed variation characteristics of pure electric heavy-duty vehicles under the joint influence of multiple factors. These findings serve as the basis for determining the maximum grade and the critical length applicable to pure electric heavy-duty vehicles on highways. The research findings indicate that, compared to traditional fuel-powered heavy-duty vehicles, pure electric heavy-duty vehicles exhibit smoother acceleration and deceleration processes, smaller speed fluctuations, higher travel speeds, and greater equilibrium speed values during uphill climbing. The power-to-weight ratio has a greater impact on the climbing speed of pure electric heavy-duty vehicles, while the initial vehicle speed has a relatively minor effect. It was observed that the dynamic performance of pure electric heavy-duty vehicles does not align with the maximum grade stipulated by current regulations in China. These research findings provide important reference points for road longitudinal section design and vehicle management in road freight enterprises. Full article
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<p>Road model. (<b>a</b>) Profile view; (<b>b</b>) actual effect.</p>
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<p>Vertical curve setting for experimental road.</p>
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<p>Engine speed–torque curve for fuel-powered vehicles.</p>
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<p>Motor efficiency map.</p>
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<p>External characteristic curve of the motor.</p>
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<p>Schematic diagram of power system settings for an electric vehicle model in TruckSim.</p>
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<p>The speed of heavy-duty vehicles on roads with a design speed of 80 km/h. (<b>a</b>) Traditional fuel-powered heavy-duty vehicles; (<b>b</b>) pure electric heavy-duty vehicles.</p>
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<p>The speed of heavy-duty vehicles on roads with a design speed of 100 km/h. (<b>a</b>) Traditional fuel-powered heavy-duty vehicles; (<b>b</b>) pure electric heavy-duty vehicles.</p>
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<p>The speed of heavy-duty vehicles on roads with a design speed of 120 km/h. (<b>a</b>) Traditional fuel-powered heavy-duty vehicles; (<b>b</b>) pure electric heavy-duty vehicles.</p>
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<p>Relationship between slope, load weight, and <span class="html-italic">DV</span>. (<b>a</b>) Three-dimensional plot; (<b>b</b>) Y-Z plane.</p>
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<p>Relationship between slope, power-to-weight ratio, and <span class="html-italic">DV</span>.</p>
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<p>Relationship between slope, initial climbing speed, and <span class="html-italic">DV</span>.</p>
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<p>Relationship between initial climbing speed, load weight, and <span class="html-italic">DV</span>.</p>
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<p>Relationship between initial climbing speed, power-to-weight ratio, and <span class="html-italic">DV</span>.</p>
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19 pages, 2325 KiB  
Article
A Quantitative Analysis of the Complex Response Relationship between Urban Green Infrastructure (UGI) Structure/Spatial Pattern and Urban Thermal Environment in Shanghai
by Zhenru Guan and Hao Zhang
Sustainability 2024, 16(16), 6886; https://doi.org/10.3390/su16166886 (registering DOI) - 10 Aug 2024
Viewed by 771
Abstract
The urban heat island (UHI) effect has evolved into one of the key environmental problems affecting the urban ecological environment and sustainable development. Based on 52 Urban Thermal Heat spots (UTHSs) with significant differences between land use structure and urban green infrastructure (UGI) [...] Read more.
The urban heat island (UHI) effect has evolved into one of the key environmental problems affecting the urban ecological environment and sustainable development. Based on 52 Urban Thermal Heat spots (UTHSs) with significant differences between land use structure and urban green infrastructure (UGI) spatial layout within the influence range of UHI in Shanghai, Landsat-8/9 satellite images were used to construct a high-dimensional dataset reflecting the impact of built environment components on urban thermal environment. Descriptive statistical analysis was used to analyze the spatial difference qualitatively. Using the stepwise regression (SWR) model and partial least square regression (PLSR) model, the complex response relationship between UGI’s structure/spatial pattern differentiation and urban thermal environment in three spatial stratification ranges of UTHSs was quantitatively analyzed. Overall, the statistical explanatory power of the PLSR model is much better than the stepwise regression model. The PLSR model points out that moderately increasing the average building height, class area (CA), percentage of landscape (PLAND), landscape shape index (LSI), and largest patch index (LPI) play a positive role in inhibiting the growth of land surface temperature (LST), and the cooling effect of index weights decreases in order. However, the interaction effects of the box-cox transformed indices with underlines, e.g., CA × Cohesion × AI × LPI and PLAND × CA × Cohesion × AI × LPI, exert relatively small weight on the cooling effect. According to the results, suggestions such as optimization of the UGI structure and urban construction layout were proposed, which can effectively mitigate the UHI effect. Full article
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<p>Distribution of 52 UTHSs in the study area.</p>
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<p>Research framework diagram.</p>
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<p>LST chart of the five levels of UTHSs from 2013 to 2022 and mean value under three spatial levels. (<b>a</b>) LST chart of the five levels of UTHSs in 2013. (<b>b</b>) LST chart of the five levels of UTHSs in 2015. (<b>c</b>) LST chart of the five levels of UTHSs in 2017. (<b>d</b>) LST chart of the five levels of UTHSs in 2020. (<b>e</b>) LST chart of the five levels of UTHSs in 2022. (<b>f</b>)Average LST plot for five years. Notes: The lowercases that appear above the box plots are the result of the HSD test.</p>
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<p>Nonlinear fitting diagram of LST correlation among three spatial stratification areas (<b>a</b>) Nonlinear fitting diagram of LST correlation among the buffer area and the whole area. (<b>b</b>) Nonlinear fitting diagram of LST correlation among the core area and the whole area. (<b>c</b>) Nonlinear fitting diagram of LST correlation among the buffer area and the core area.</p>
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<p>Land use classification and LST Distribution of typical UTHSs. Notes: In this Figure, the inner frame line is the core area, the outer frame line is the overall area boundary, and the inner and outer frame line range is a 500 m buffer.</p>
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26 pages, 14290 KiB  
Article
Exploratory Analysis Using Deep Learning for Water-Body Segmentation of Peru’s High-Mountain Remote Sensing Images
by William Isaac Perez-Torres, Diego Armando Uman-Flores, Andres Benjamin Quispe-Quispe, Facundo Palomino-Quispe, Emili Bezerra, Quefren Leher, Thuanne Paixão and Ana Beatriz Alvarez
Sensors 2024, 24(16), 5177; https://doi.org/10.3390/s24165177 - 10 Aug 2024
Viewed by 439
Abstract
High-mountain water bodies represent critical components of their ecosystems, serving as vital freshwater reservoirs, environmental regulators, and sentinels of climate change. To understand the environmental dynamics of these regions, comprehensive analyses of lakes across spatial and temporal scales are necessary. While remote sensing [...] Read more.
High-mountain water bodies represent critical components of their ecosystems, serving as vital freshwater reservoirs, environmental regulators, and sentinels of climate change. To understand the environmental dynamics of these regions, comprehensive analyses of lakes across spatial and temporal scales are necessary. While remote sensing offers a powerful tool for lake monitoring, applications in high-mountain terrain present unique challenges. The Ancash and Cuzco regions of the Peruvian Andes exemplify these challenges. These regions harbor numerous high-mountain lakes, which are crucial for fresh water supply and environmental regulation. This paper presents an exploratory examination of remote sensing techniques for lake monitoring in the Ancash and Cuzco regions of the Peruvian Andes. The study compares three deep learning models for lake segmentation: the well-established DeepWaterMapV2 and WatNet models and the adapted WaterSegDiff model, which is based on a combination of diffusion and transformation mechanisms specifically conditioned for lake segmentation. In addition, the Normalized Difference Water Index (NDWI) with Otsu thresholding is used for comparison purposes. To capture lakes across these regions, a new dataset was created with Landsat-8 multispectral imagery (bands 2–7) from 2013 to 2023. Quantitative and qualitative analyses were performed using metrics such as Mean Intersection over Union (MIoU), Pixel Accuracy (PA), and F1 Score. The results achieved indicate equivalent performance of DeepWaterMapV2 and WatNet encoder–decoder architectures, achieving adequate lake segmentation despite the challenging geographical and atmospheric conditions inherent in high-mountain environments. In the qualitative analysis, the behavior of the WaterSegDiff model was considered promising for the proposed application. Considering that WatNet is less computationally complex, with 3.4 million parameters, this architecture becomes the most pertinent to implement. Additionally, a detailed temporal analysis of Lake Singrenacocha in the Vilcanota Mountains was conducted, pointing out the more significant behavior of the WatNet model. Full article
(This article belongs to the Special Issue Application of Satellite Remote Sensing in Geospatial Monitoring)
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<p>Location of the study area.</p>
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<p>Landsat-8 scenes selected for study.</p>
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<p>Combining process from B2 to B7 into a single 6-channel image.</p>
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<p>From left to right: <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>θ</mi> <mo>,</mo> <mi>ρ</mi> <mo>)</mo> </mrow> </semantics></math> parameter space, deskwed image, cropped image, and division of the image into 256 × 256 pixel patches.</p>
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<p>Mask creation process.</p>
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<p>WatNet model architecture.</p>
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<p>DeepWaterMapV2 model architecture based on 3 primary blocks.</p>
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<p>General architecture of WaterSegDiff based on a conditioning model and a diffusion model that integrate their information through two conditioning mechanisms, <math display="inline"><semantics> <mi mathvariant="script">U</mi> </semantics></math>-SA and SS-Former.</p>
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<p>SS-Former internal architecture consisting of two symmetrical cross-attention modules.</p>
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<p>Qualitative analysis of 5 selected samples that represent large lakes with compact structures. Showing the RGB image, ground truth, NDWI, WatNet, DeepWaterMapV2, and WaterSegDiff results. (<b>a</b>) Large and irregular lake, (<b>b</b>) two lakes with compact structure, (<b>c</b>) scene with river crossing, (<b>d</b>) large lake in mountainous region, (<b>e</b>) lake surrounded by dense vegetation.</p>
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<p>Qualitative analysis of 5 selected samples that represent small and dispersed lakes. Showing the RGB image, ground truth, NDWI, WatNet, DeepWaterMapV2, and WaterSegDiff results. (<b>a</b>,<b>b</b>) Snowy scene with shadows with presence of clear and turbid lakes, (<b>c</b>) completely snowy scene, (<b>d</b>,<b>e</b>) partially snowy area with scattered lakes.</p>
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<p>The edges extracted from Lake Singrenacocha based on NDWI, WatNet, DeepWaterMapV2, and WaterSegDiff. Highlights in yellow, green, blue, and red for the years 2014, 2016, 2018, and 2020, respectively.</p>
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<p>Graphical representation of the segmentation performance of Lake Singrenacocha during the years 2014, 2016, 2018, and 2020.</p>
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13 pages, 1635 KiB  
Article
Optical Biosensor Based on Porous Silicon and Tamm Plasmon Polariton for Detection of CagA Antigen of Helicobacter pylori
by Guoguang Rong, Alexey Kavokin and Mohamad Sawan
Sensors 2024, 24(16), 5153; https://doi.org/10.3390/s24165153 - 9 Aug 2024
Viewed by 180
Abstract
Helicobacter pylori (H. pylori) is a common pathogen with a high prevalence of infection in human populations. The diagnosis of H. pylori infection is critical for its treatment, eradication, and prognosis. Biosensors have been demonstrated to be powerful for the rapid [...] Read more.
Helicobacter pylori (H. pylori) is a common pathogen with a high prevalence of infection in human populations. The diagnosis of H. pylori infection is critical for its treatment, eradication, and prognosis. Biosensors have been demonstrated to be powerful for the rapid onsite detection of pathogens, particularly for point-of-care test (POCT) scenarios. In this work, we propose a novel optical biosensor, based on nanomaterial porous silicon (PSi) and photonic surface state Tamm Plasmon Polariton (TPP), for the detection of cytotoxin-associated antigen A (CagA) of H. pylori bacterium. We fabricated the PSi TPP biosensor, analyzed its optical characteristics, and demonstrated through experiments, with the sensing of the CagA antigen, that the TPP biosensor has a sensitivity of 100 pm/(ng/mL), a limit of detection of 0.05 ng/mL, and specificity in terms of positive-to-negative ratio that is greater than six. From these performance factors, it can be concluded that the TPP biosensor can serve as an effective tool for the diagnosis of H. pylori infection, either in analytical labs or in POCT applications. Full article
(This article belongs to the Special Issue Optical Biosensors and Applications)
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<p>The PSi TPP biosensor structure and its optical measurement configuration. The Au NPs embedded in the first LP PSi layer means that Au NP can infiltrate into the nanopores of porous silicon. The picture on the bottom left shows the setup of the 12 × 8 biosensor array and its sequential measurement by an in-house developed equipment mainly consisting of a two-dimensional moving stage to carry and position the sensor array and a fiber spectrometer to take the optical measurement.</p>
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<p>(<b>a</b>) Cross-sectional scanning electron microscopy image of the TPP biosensor structure. The periodic layered structure of the porous silicon DBR is clearly visible. The gold thin film is the bright layer on top of the porous silicon DBR with the thickness not to scale due to a focusing issue; (<b>b</b>) atomic force microscopy image of a Au thin film surface morphology, showing the nanoporous structure of Au due to conformal deposition onto porous silicon; (<b>c</b>) Color map of electrical field strength distribution profile of TPP biosensor simulated by COMSOL V5.5. The field peak resides in the first (or top) PSi layer close to the thin metal film. Light is incident from the left side of the TPP device in air with a power of 1 W/m; (<b>d</b>) An example of the reflection spectrum of the TPP device is that of where the resonant state manifests as the reflection minimum at a wavelength of around 730 nm; (<b>e</b>) Example of the redshift of the TPP resonance wavelength upon the specific biomolecular binding of 3 ng/mL CagA antigen with the CagA antibody immobilized on the biosensor surface beforehand. The spectrum of the TPP biosensor both before (solid curve) and after (dashed curve) binding is shown. The redshift of the resonance minimum, indicated as arrows, is around 360 pm. (<b>f</b>) Example TPP resonance spectra upon exposure to PBS buffer with CagA antibody immobilized on the biosensor surface beforehand. The spectrum of the TPP biosensor both before (solid curve) and after (dashed curve) PBS is shown. The shift of resonance minimum, indicated as arrows, is 0 pm.</p>
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<p>Response characterization of CagA antigen detection for detecting varying concentrations of CagA antigen in the PBS buffer, with both PSi TPP (black circles) and PSi DBR (grey circles) biosensors. Error bars on the experimental data points (solid circle) show a standard error from five experiments, with each experiment using a different biosensor. The linear fittings (dashed curves) are performed to match the data points. The linear equations go through the origin and the quality of the fitting is also given in the figure.</p>
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<p>Specificity test and competitivity test of the PSi TPP biosensor with the objective of CagA antigen detection. CagA has a concentration of 1 ng/mL and all other nonspecific species concentrations of 5 ng/mL. Error bars on the experimental data bars (solid rectangle) show the standard error from five experiments, with each experiment using a different biosensor.</p>
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