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Search Results (937)

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18 pages, 1652 KiB  
Article
Closed-Loop Auditory Stimulation (CLAS) During Sleep Augments Language and Discovery Learning
by Vincent P. Clark, Hector P. Valverde, Mason S. Briggs, Teagan Mullins, Jacqueline Ortiz, Christopher J. H. Pirrung, Olivia S. O’Keeffe, Madeline Hwang, Sidney Crowley, Marko Šarlija and Panagiotis Matsangas
Brain Sci. 2024, 14(11), 1138; https://doi.org/10.3390/brainsci14111138 - 13 Nov 2024
Viewed by 305
Abstract
Background/Objectives: Slow oscillation (SO) brainwaves observed during sleep have been shown to reflect the process of memory consolidation, that underlies the critical role of sleep in learning, memory, and other cognitive functions. Closed-loop auditory stimulation (CLAS) uses tones presented in phase with SOs [...] Read more.
Background/Objectives: Slow oscillation (SO) brainwaves observed during sleep have been shown to reflect the process of memory consolidation, that underlies the critical role of sleep in learning, memory, and other cognitive functions. Closed-loop auditory stimulation (CLAS) uses tones presented in phase with SOs to increase their amplitude and number, along with other brainwave signatures related to memory consolidation. Prior studies have found that CLAS maximizes the ability to perform rote memorization tasks, although this remains controversial. The present study examined whether CLAS affects a broader range of learning tasks than has been tested previously, including a rote language learning task requiring basic memorization and also two discovery learning tasks requiring insight, hypothesis testing, and integration of experience, all processes that benefit from memory consolidation. Methods: Twenty-eight healthy participants performed language and discovery learning tasks before sleeping in our laboratory for three continuous nights per week over two weeks, with verum or control CLAS using a prototype NeuroGevity system (NeuroGeneces, Inc., Santa Fe, NM, USA) in a crossed, randomized, double-blind manner. Results: Language learning showed a 35% better word recall (p = 0.048), and discovery learning showed a 26% better performance (p < 0.001) after three continuous nights of CLAS vs. control. EEG measures showed increased SO amplitude and entrainment, SO-spindle coupling, and other features that may underlie the learning benefits of CLAS. Conclusions: Taken together, the present results show that CLAS can alter brain dynamics and enhance learning, especially in complex discovery learning tasks that may benefit more from memory consolidation compared with rote word pair or language learning. Full article
(This article belongs to the Section Neurotechnology and Neuroimaging)
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<p>Shows sequence of procedures (<b>A</b>) and balancing of conditions across weeks (<b>B</b>).</p>
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<p>Example images presented to participants in the DARWARS task. The left of the figure contains example target-absent images and the right contains analogous target-present images. The cut-out boxes are used here for display purposes only and were not present in the actual task. The right boxes show target-present images (roadside IEDs, remote-controlled car bombs, and snipers) with the objects magnified.</p>
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<p>Example stimuli from the PRETXT task. The task began with a baseline test block (left column) without feedback, then a training block with feedback (middle column), and then a test block without feedback (right column).</p>
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<p>(<b>A</b>) Mean (±SD) 0.25–4 Hz filtered EEG signal, averaged across subjects, time-locked to the first auditory stimulus (t = 0 s) for the Stim and Control conditions. (<b>B</b>) Mean (±SD) of the 11–16 Hz filtered (spindle band) EEG signal amplitude envelope (based on the Hilbert transformation), averaged across subjects, time-locked to the first auditory stimulus (t = 0 s) for the Stim and Control conditions. For each stimulus, the mean spindle activity value in the 2 s period before the stimulus delivery was subtracted (which is then reflected in the y-axis values).</p>
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20 pages, 10441 KiB  
Article
Proto-DS: A Self-Supervised Learning-Based Nondestructive Testing Approach for Food Adulteration with Imbalanced Hyperspectral Data
by Kunkun Pang, Yisen Liu, Songbin Zhou, Yixiao Liao, Zexuan Yin, Lulu Zhao and Hong Chen
Foods 2024, 13(22), 3598; https://doi.org/10.3390/foods13223598 - 11 Nov 2024
Viewed by 524
Abstract
Conventional food fraud detection using hyperspectral imaging (HSI) relies on the discriminative power of machine learning. However, these approaches often assume a balanced class distribution in an ideal laboratory environment, which is impractical in real-world scenarios with diverse label distributions. This results in [...] Read more.
Conventional food fraud detection using hyperspectral imaging (HSI) relies on the discriminative power of machine learning. However, these approaches often assume a balanced class distribution in an ideal laboratory environment, which is impractical in real-world scenarios with diverse label distributions. This results in suboptimal performance when less frequent classes are overshadowed by the majority class during training. Thus, the critical research challenge emerges of how to develop an effective classifier on a small-scale imbalanced dataset without significant bias from the dominant class. In this paper, we propose a novel nondestructive detection approach, which we call the Dice Loss Improved Self-Supervised Learning-Based Prototypical Network (Proto-DS), designed to address this imbalanced learning challenge. The proposed amalgamation mitigates the label bias on the most frequent class, further improving robustness. We validate our proposed method on three collected hyperspectral food image datasets with varying degrees of data imbalance: Citri Reticulatae Pericarpium (Chenpi), Chinese herbs, and coffee beans. Comparisons with state-of-the-art imbalanced learning techniques, including the Synthetic Minority Oversampling Technique (SMOTE) and class-importance reweighting, reveal our method’s superiority. Notably, our experiments demonstrate that Proto-DS consistently outperforms conventional approaches, achieving the best average balanced accuracy of 88.18% across various training sample sizes, whereas the Logistic Model Tree (LMT), Multi-Layer Perceptron (MLP), and Convolutional Neural Network (CNN) approaches attain only 59.42%, 60.38%, and 66.34%, respectively. Overall, self-supervised learning is key to improving imbalanced learning performance and outperforms related approaches, while both prototypical networks and the Dice loss can further enhance classification performance. Intriguingly, self-supervised learning can provide complementary information to existing imbalanced learning approaches. Combining these approaches may serve as a potential solution for building effective models with limited training data. Full article
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Graphical abstract

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<p>Figures of the imbalanced food products in the datasets: (<b>a</b>–<b>d</b>) samples from the chenpi dataset, (<b>e</b>,<b>f</b>) samples from the coffee bean dataset, and (<b>g</b>,<b>h</b>) samples from the Chinese herbs dataset.</p>
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<p>Figures of the imbalanced food products in the datasets: (<b>a</b>–<b>d</b>) samples from the chenpi dataset, (<b>e</b>,<b>f</b>) samples from the coffee bean dataset, and (<b>g</b>,<b>h</b>) samples from the Chinese herbs dataset.</p>
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<p>Training process of Proto-DS using spectral prototypical contrastive learning and fine-tuning with Dice loss to improve the prototypical network. For simplicity, we use the coffee bean dataset as an example. Blue line: data flow of unknown new incoming samples. Red line:the data flow of the positive samples (majority class). Yellow line: the data flow of the negative samples (minority class).</p>
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<p>The prototypical network with various available samples for training. The blue color indicates that the object is labeled as an authentic sample, while the green color indicates that the object is labeled as counterfeit. The light blue and light green data points denote the training samples in the embeddings. whereas the dark blue and dark green data points indicate the prototypes for authentic <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">c</mi> <mn>1</mn> </msub> </semantics></math> and counterfeit <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">c</mi> <mn>2</mn> </msub> </semantics></math>, respectively. The white circle indicates the unknown test data, while the dashed line represent the distance to the prototype vectors.</p>
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<p>The test process of Proto-DS. Light grey box: unknown new incoming samples during testing. Yellow box: training for Arabica coffee beans (majority class). Orange box: training for Robusta coffee beans (minority class).</p>
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<p>Class distributions for the coffee bean and Chinese herb datasets; dark blue denotes the majority class, light blue denotes the minority class, and percentage indicates the imbalance rate for the specific imbalance setting. Please note that the Chenpi dataset contains multiple minority classes, which we represent using different light blue colors.</p>
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<p>Visualisation spectra of each dataset. The straight lines are the averaged spectra among the particular classes, while the shaded area indicates the standard deviation of each class.</p>
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<p>Comparison with other state-of-the-art competitors in terms of balanced accuracy (B.Acc), M.F score (Macro-F score), macro-AUROC (M.AUROC), and macro-average precision (M.AP). <b>Proto-DS</b>: proposed method; <b>Conv-W</b>: CNN with class-reweighted cross entropy loss; <b>Conv-S</b>: CNN with SMOTE; <b>MLP-W</b>: MLP with class-reweighted cross entropy loss; <b>MLP-S</b>: MLP with SMOTE; <b>LMT-S</b>: logistic model tree with SMOTE and Adaboost.</p>
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<p>Comparison with state-of-the-art competitors in terms of sensitivity and specificity. Each figure summarizes the class-wise performance for all algorithms, while the rows corresponding to the different datasets.</p>
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<p>Results of the ablation study comparing different components in terms of balanced accuracy (B.Acc), M.F score (M.F1-score), macro-AUROC (M.AUROC), and macro-average precision (M.AP): <b>Proto-DS</b>, proposed method (blue straight line); <b>w/o D</b>, without applying Dice loss (blue dashed line); <b>w/o SSL</b>, without applying self-supervised learning (red straight line); <b>w/o SSL + D</b>, without self-supervised pretraining or Dice loss (red dashed line).</p>
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<p>Results of the ablation study comparing different components in terms of sensitivity (Sens.) and specificity (Spec.): <b>Proto-DS</b>, proposed method; <b>w/o D</b>, without applying Dice loss <b>w/o SSL</b>, without applying self-supervised learning; <b>w/o SSL + D</b>, without self-supervised pretraining or Dice loss.</p>
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<p>Visualization of the proposed model’s pixel-level probability for the corresponding class on various datasets. (<b>a</b>) Robusta (<b>b</b>) Arisaema (<b>c</b>) 5-Year-old Chenpi (<b>d</b>) 10-Year-old Chenpi (<b>e</b>) 15-Year-Old Chenpi. The rows represent particular samples from the minority class, while the columnsrepresent the raw image (Ground Truth), proposed method with all components (Proto-DS), and Proto-DS without particular components (w/o D, w/o SSL., w/o SSL + D). Brighter pixels indicate high probability on the corresponding class, while <b>darker pixels</b> indicate low probability on the corresponding class.</p>
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<p>Two-dimensional visualization of the learned feature space for the chenpi dataset with multiple settings: the rowsrepresent various minority training sample sizes (5/10/15/20), while the columns represent the proposed method with all components (Proto-DS) or without particular components (w/o S., w/o F. + S., w/o SSL + S., w/o SSL + F. + S.).</p>
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<p>Two-dimensional visualization of the learned feature space for the chenpi dataset with multiple settings: the rowsrepresent various minority training sample sizes (5/10/15/20), while the columns represent the proposed method with all components (Proto-DS) or without particular components (w/o S., w/o F. + S., w/o SSL + S., w/o SSL + F. + S.).</p>
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<p>Two-dimensional visualization of the learned feature space for the coffee bean dataset with multiple settings: the rows represent various minority training sample sizes (5/10/15/20), while the columns represents the proposed method with all components (Proto-DS) or without particular components (w/o S., w/o F. + S., w/o SSL + S., w/o SSL + F. + S.).</p>
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<p>Two-dimensional visualization of the learned feature space for the Chinese herbs dataset with multiple settings: the rows represent various minority training sample sizes (5/10/15/20), while the columns represent the proposed method with all components (Proto-DS) or without particular components (w/o S., w/o F. + S., w/o SSL + S., w/o SSL + F. + S.).</p>
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29 pages, 2679 KiB  
Article
Fault Diagnosis in a Four-Arm Delta Robot Based on Wavelet Scattering Networks and Artificial Intelligence Techniques
by Claudio Urrea and Carlos Domínguez
Technologies 2024, 12(11), 225; https://doi.org/10.3390/technologies12110225 - 8 Nov 2024
Viewed by 468
Abstract
This paper presents a comprehensive fault diagnosis approach for a delta robot utilizing advanced feature extraction and classification techniques. A four-arm delta robot prototype is designed in SolidWorks for realistic fault analysis. Two case studies investigate faults through control effort and vibration signals, [...] Read more.
This paper presents a comprehensive fault diagnosis approach for a delta robot utilizing advanced feature extraction and classification techniques. A four-arm delta robot prototype is designed in SolidWorks for realistic fault analysis. Two case studies investigate faults through control effort and vibration signals, with control effort detecting motor and encoder faults, while vibration signals identify bearing faults. This study compares time-domain signal features and wavelet scattering networks, applied by classification algorithms including wide neural networks (WNNs), efficient linear support vector machine (ELSVM), efficient logistic regression (ELR), and kernel naive Bayes (KNB). Results indicate that a WNN, using wavelet scattering features ranked by one-way anova, is optimal due to its consistency and reliability, while these features enhance computational efficiency by reducing classifier size. Sensitivity analysis demonstrates the classifier’s capacity to detect untrained faults, highlighting the importance of effective feature extraction and classification methods for fault diagnosis in complex robotic systems. This research significantly contributes to fault diagnosis in delta robots and lays the groundwork for future studies on fault tolerance control and predictive maintenance planning. Future work will focus on the physical implementation of the delta robot in laboratory settings, aiming to improve operational efficiency and reliability in industrial applications. Full article
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<p>Delta robot design exported to Simscape.</p>
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<p>Final assembly of the delta robot exported from SolidWorks.</p>
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<p>Outputs of the joints in case of failure in actuator 4.</p>
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<p>Control effort outputs in case of failure in actuator 4.</p>
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<p>Control effort in the event of medium magnitude sensor failure.</p>
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<p>Bearings at actuated joint of the Delta robot.</p>
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<p>Elements susceptible to failure in a bearing.</p>
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<p>Vibration without faults.</p>
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<p>BPFI fault.</p>
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<p>BPFO fault.</p>
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<p>BSF fault.</p>
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<p>FTF fault.</p>
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<p>Vibration with BPFI fault.</p>
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<p>Vibration with BPFO fault.</p>
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<p>Vibration with BSF fault.</p>
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<p>Vibration with FTF fault.</p>
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<p>Scaling function and wavelets for Case 1.</p>
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<p>Scaling function and wavelets for Case 2.</p>
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<p>Logarithmic distance analysis of the delta robot under initial condition perturbation.</p>
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<p>Logarithmic distance analysis of the delta robot under fault condition.</p>
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<p>Classification of Case 1 training for WNN using wavelet scattering networks features ranked with one-way anova.</p>
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<p>Classification of Case 1 test for WNN using wavelet scattering networks features ranked with one-way anova.</p>
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<p>Classification of training and test data in Case 2 for WNN using wavelet scattering networks features ranked with one-way anova.</p>
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<p>Algorithm size for Case 1.</p>
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<p>Algorithm size for Case 2.</p>
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<p>Untrained fault classification with WNN using wavelet scattering networks features ranked with one-way anova.</p>
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15 pages, 5623 KiB  
Article
Reverse-Bent Modular Coil Structure with Enhanced Output Stability in DWPT for Arbitrary Linear Transport Systems
by Jia Li, Chong Zhu, Junyi Ji, Jianquan Ma and Xi Zhang
Sensors 2024, 24(22), 7171; https://doi.org/10.3390/s24227171 - 8 Nov 2024
Viewed by 311
Abstract
Dynamic wireless power transfer (DWPT) systems with segmented transmitters suffer from output pulsations during the moving process. Although numerous coil structures have been developed to mitigate this fluctuation, the parameter design process is complicated and restricted by specific working conditions (e.g., air gaps). [...] Read more.
Dynamic wireless power transfer (DWPT) systems with segmented transmitters suffer from output pulsations during the moving process. Although numerous coil structures have been developed to mitigate this fluctuation, the parameter design process is complicated and restricted by specific working conditions (e.g., air gaps). To solve these problems, a novel reverse-bent modular transmitter structure is proposed for DWPT in industrial automatic application scenarios such as linear transport systems. Considering the heterogeneous current density distribution in the adjacent region between two coils which causes a drop in magnetic field, the proposed coil structure attempts to eliminate the effects of the adjacent region by bending the terminal parts of each coil reversely to the ferrite layer for shielding. Compared to traditional planar couplers, this structure array can generate a uniform magnetic field over various air gaps. A 100 W laboratory prototype was built to verify the feasibility of the proposed system. The experimental results show that the proposed system achieved a constant output voltage, and the output pulsation was within ±2.3% in the dynamic powering process. The average efficiency was about 88.29%, with a 200 mm transfer distance. When the air gap varied from 20 mm to 30 mm, the system could still retain constant voltage output characteristics. Full article
(This article belongs to the Topic Advanced Wireless Charging Technology)
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<p>Schematic diagram of magnetically levitated transport systems [<a href="#B12-sensors-24-07171" class="html-bibr">12</a>].</p>
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<p>Magnetic field for traditional planar coils.</p>
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<p>Mutual inductance for traditional planar coils.</p>
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<p>Proposed coil structure.</p>
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<p>Layout of the proposed magnetic couplers.</p>
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<p>Magnetic field simulated by Maxwell. (<b>a</b>) For proposed transmitters when <span class="html-italic">h</span><sub>m</sub> = 20 mm. (<b>b</b>) For long-track-type transmitter when <span class="html-italic">h</span><sub>m</sub> = 20 mm.</p>
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<p>Coupling coefficient when the transmitter length varies.</p>
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<p>Curves of mutual inductance fluctuation with transmitter length by simulation.</p>
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<p>Simulated mutual inductances between the receiver and transmitters (<b>a</b>) when <span class="html-italic">h</span><sub>m</sub> = 20 mm; (<b>b</b>) when <span class="html-italic">h</span><sub>m</sub> = 25 mm; (<b>c</b>) when <span class="html-italic">h</span><sub>m</sub> = 30 mm.</p>
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<p>Magnetic field simulated by Maxwell when <span class="html-italic">l</span><sub>m</sub> = 400 mm for proposed transmitters. (<b>a</b>) With one layer in bent parts. (<b>b</b>) With two layers in bent parts. (<b>c</b>) With another ferrite layer.</p>
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<p>Topology of <span class="html-italic">LCC-S</span> DWPT system.</p>
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<p>Simplified resonant circuit.</p>
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<p>Prototype of the proposed DWPT system.</p>
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<p>Experimental waveforms when <span class="html-italic">R</span><sub>L</sub> = 5 Ω. (<b>a</b>) Outputs of the inverter and rectifier when <span class="html-italic">h</span><sub>m</sub> = 20 mm. (<b>b</b>) Outputs of the inverter when <span class="html-italic">h</span><sub>m</sub> = 25 (left) and 30 mm (right).</p>
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<p>Experimental waveforms when <span class="html-italic">R</span><sub>L</sub> = 5 Ω. (<b>a</b>) Outputs of the inverter when <span class="html-italic">l</span><sub>m</sub> = 300 (left) and 350 mm (right) and (<b>b</b>) when <span class="html-italic">l</span><sub>m</sub> = 400 (left) and 500 mm (right).</p>
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<p>Curves of the output voltage and efficiency measured at different positions. (<b>a</b>) When <span class="html-italic">h</span><sub>m</sub> = 20 mm. (<b>b</b>) When <span class="html-italic">h</span><sub>m</sub> = 25 mm. (<b>c</b>) When <span class="html-italic">h</span><sub>m</sub> = 30 mm.</p>
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<p>The power losses of the system when <span class="html-italic">h</span><sub>m</sub> = 20 mm.</p>
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<p>Comparison of various methods in [<a href="#B21-sensors-24-07171" class="html-bibr">21</a>,<a href="#B24-sensors-24-07171" class="html-bibr">24</a>,<a href="#B25-sensors-24-07171" class="html-bibr">25</a>,<a href="#B27-sensors-24-07171" class="html-bibr">27</a>].</p>
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19 pages, 6105 KiB  
Article
Robotized Mobile Platform for Non-Destructive Inspection of Aircraft Structures
by Rafał Toman, Tomasz Rogala, Piotr Synaszko and Andrzej Katunin
Appl. Sci. 2024, 14(22), 10148; https://doi.org/10.3390/app142210148 - 6 Nov 2024
Viewed by 472
Abstract
The robotization of the non-destructive inspection of aircraft is essential for improving the accuracy and duration of performed inspections, being an integral part of inspection and data management systems within the currently developed NDT 4.0 concept. In this paper, the authors presented the [...] Read more.
The robotization of the non-destructive inspection of aircraft is essential for improving the accuracy and duration of performed inspections, being an integral part of inspection and data management systems within the currently developed NDT 4.0 concept. In this paper, the authors presented the design and testing of a universal mobile platform with interchangeable sensing systems for the non-destructive inspection of aircraft structures with various angles of inclination. As a result of the performed studies, a low-cost approach of automation of existing measurement devices used for inspection was proposed. The constructed prototype of the mobile platform was equipped with eddy current testing probe and successfully passed both laboratory and environmental tests, demonstrating its performance in various conditions. The presented approach confirms the effectiveness of the automation of the inspection process using climbing robots and defining the directions of possible development of automation in non-destructive testing in aviation. Full article
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<p>Relations between thrust force and angle of inclination for the considered friction coefficients.</p>
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<p>The design (<b>a</b>) and hardware implementation (<b>b</b>) of the printed circuit of the main system for the MP.</p>
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<p>The electrical scheme of the MP: M1–M4—wheel drive motors, SM—probe lifting servo, MW—propeller drive motor, R—engine speed controller, ZI—switching power supply.</p>
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<p>The design of the printed circuit (<b>a</b>), its hardware implementation (<b>b</b>), and the front panel (<b>c</b>) of the remote control for the MP.</p>
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<p>The algorithms for controlling the operation of MP (<b>a</b>) and for the remote control application (<b>b</b>).</p>
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<p>Top and side view of structural design of the MP.</p>
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<p>Front (<b>a</b>) and back (<b>b</b>) views of the assembled MP.</p>
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<p>The thrust of the propeller in function of the consumed power for the MP.</p>
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<p>The MP climbing on a vertical wall during preliminary tests.</p>
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<p>The MP on MiG-29 rudder during laboratory tests.</p>
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<p>The MP climbing on Mil series helicopter during outdoor tests.</p>
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<p>The result obtained during the tests on MiG-29 rudder. Thickness changes are visible. Black dashed lines indicate places where the MP speed was too high.</p>
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<p>The result obtained during the tests on PZL-130 wing.</p>
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15 pages, 4252 KiB  
Article
Analysis and Design of a Recyclable Inductive Power Transfer System for Sustainable Multi-Stage Rocket Microgrid with Multi-Constant Voltage Output Characteristics—Theoretical Considerations
by Peng Gu, Shibo Wang and Bowen Zhou
Sustainability 2024, 16(22), 9640; https://doi.org/10.3390/su16229640 - 5 Nov 2024
Viewed by 531
Abstract
After a traditional one-time rocket is launched, most of its parts will fall into the atmosphere and burn or fall into the ocean. The parts cannot be recycled, so the cost is relatively high. Multi-stage rockets can be recovered after launch, which greatly [...] Read more.
After a traditional one-time rocket is launched, most of its parts will fall into the atmosphere and burn or fall into the ocean. The parts cannot be recycled, so the cost is relatively high. Multi-stage rockets can be recovered after launch, which greatly reduces the cost of space launches. Moreover, recycling rockets can reduce the generation of waste and reduce pollution and damage to the environment. With the reduction in rocket launch costs and technological advances, space exploration and development can be carried out more frequently and economically. It provides technical support for the sustainable use of space resources. It not only promotes the sustainable development of the aerospace field but also has a positive impact on global environmental protection, resource utilization, and economic development. In order to adapt to the stage-by-stage separation structure of the rocket, this paper proposes a new multi-stage rocket inductive power transfer (IPT) system to power the rocket microgrid. The planar coil structure is used to form wireless power transfer between each stage of the rocket, reducing the volume of the magnetic coupling structure. The volume of the circuit topology structure is reduced by introducing an auxiliary coil. An equivalent three-stage S/T topology is proposed, and the constant voltage output characteristics of multiple loads are analyzed. A multi-stage coil structure is proposed to supply power to multiple loads simultaneously. In order to eliminate undesired magnetic coupling between coils, ferrite cores are added between coils for effective electromagnetic shielding. The parameters of the magnetic coupling structure are optimized based on the finite element method (FEM). A prototype of the proposed IPT system is built to simulate a multi-stage rocket. A series of experiments are conducted to verify the advantages of the proposed IPT system, and the three-stage rocket system efficiency reached 88.5%. This project is theoretical. Its verification was performed only in the laboratory conditions. Full article
(This article belongs to the Special Issue Recent Advances in Smart Grids for a Sustainable Energy System)
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<p>Conceptual image of an IPT system powering a multi-stage rocket microgrid.</p>
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<p>Circuit model of IPT system.</p>
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<p>Ideal AC circuit of the IPT system.</p>
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<p>Circuit model after mutual inductance <span class="html-italic">M</span><sub>AS</sub> is ignored.</p>
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<p>Illustration of the reflection impedance.</p>
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<p>Structure of three-stage magnetic coupler. (<b>a</b>) Coupler structure. (<b>b</b>) Structure of the litz coil part. (<b>c</b>) Structure of the ferrite core part.</p>
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<p>Distribution of space magnetic field in 2D view.</p>
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<p>The mutual inductance value between coils is affected by the simulation results of the ferrite core position and the ferrite core side length. (<b>a</b>) Effect on <span class="html-italic">M</span><sub>AP</sub>. (<b>b</b>) Effect on <span class="html-italic">M</span><sub>AS</sub>.</p>
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<p>Effect of <span class="html-italic">R</span><sub>A</sub> and <span class="html-italic">L</span><sub>F</sub> on Mutual Inductance. (<b>a</b>) Effect on <span class="html-italic">M</span><sub>AP</sub>/<span class="html-italic">M</span><sub>AS</sub>. (<b>b</b>) Effect on <span class="html-italic">M</span><sub>AP</sub>.</p>
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<p>Mutual inductance after changing the thickness of the ferrite core.</p>
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<p>Curves of voltage transformation ratio of the system under different auxiliary coil radius.</p>
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<p>Prototype of the system.</p>
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<p>Output voltage curves of the IPT system.</p>
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<p>Output power and efficiency of the IPT system. (<b>a</b>) <span class="html-italic">R</span><sub>2</sub> = 40 Ω, <span class="html-italic">R</span><sub>3</sub> = 40 Ω. (<b>b</b>) <span class="html-italic">R</span><sub>1</sub> = 40 Ω, <span class="html-italic">R</span><sub>3</sub> = 40 Ω. (<b>c</b>) <span class="html-italic">R</span><sub>1</sub> = 40 Ω, <span class="html-italic">R</span><sub>2</sub> = 3 Ω.</p>
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<p>Waveform of the IPT system. When <span class="html-italic">U</span><sub>in</sub> = 72 V, <span class="html-italic">R</span><sub>L1</sub> = 20 Ω, <span class="html-italic">R</span><sub>L2</sub> = 40 Ω, <span class="html-italic">R</span><sub>L3</sub> = 40 Ω: (<b>a</b>) <span class="html-italic">U</span><sub>mn1</sub>, AC. (<b>b</b>) <span class="html-italic">U</span><sub>mn2</sub>, AC. (<b>c</b>) <span class="html-italic">U</span><sub>mn3</sub>, AC. (<b>d</b>) <span class="html-italic">U</span><sub>out1</sub>, DC. (<b>e</b>) <span class="html-italic">U</span><sub>out2</sub>, DC. (<b>f</b>) <span class="html-italic">U</span><sub>out3</sub>, DC. When <span class="html-italic">U</span><sub>in</sub> = 72 V, <span class="html-italic">R</span><sub>L1</sub> = 40 Ω, <span class="html-italic">R</span><sub>L2</sub> = 250 Ω, <span class="html-italic">R</span><sub>L3</sub> = 40 Ω: (<b>g</b>) <span class="html-italic">U</span><sub>mn1</sub>, AC. (<b>h</b>) <span class="html-italic">U</span><sub>mn2</sub>, AC. (<b>i</b>) <span class="html-italic">U</span><sub>mn3</sub>, AC. (<b>j</b>) <span class="html-italic">U</span><sub>out1</sub>, DC. (<b>k</b>) <span class="html-italic">U</span><sub>out2</sub>, DC. (<b>l</b>) <span class="html-italic">U</span><sub>out3</sub>, DC.</p>
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26 pages, 10736 KiB  
Article
Experimental Evaluation of Under Slab Mats (USMs) Made from End-of-Life Tires for Ballastless Tram Track Applications
by Cezary Kraśkiewicz, Piotr Majnert, Anna Al Sabouni-Zawadzka, Przemysław Mossakowski and Marcin Zarzycki
Materials 2024, 17(21), 5388; https://doi.org/10.3390/ma17215388 - 4 Nov 2024
Viewed by 403
Abstract
The growing population of urban areas results in the need to deal with the noise pollution from the transportation system. This study presents experimental test results of static and dynamic elastic characteristics of under slab mats (USMs) according to the procedure of DIN [...] Read more.
The growing population of urban areas results in the need to deal with the noise pollution from the transportation system. This study presents experimental test results of static and dynamic elastic characteristics of under slab mats (USMs) according to the procedure of DIN 45673-7. Prototype USMs based on recycled elastomeric materials, i.e., SBR granules and fibres produced from waste car tires, are analysed. Vibration isolation mats with different thicknesses (10, 15, 20, 25, 30, and 40 mm), densities (500 and 600 kg/m3), and different degrees of space filling (no holes, medium holes, large holes) are considered. Moreover, a practical application of the laboratory test results of USMs in the design of ballastless track structures of two different types (with a concrete slab and longitudinal beams) is presented. Deflections of the rail and the floating slab system, as well as stresses acting on the mat, are determined according to EN 16432-2. The use of shredded rubber from recycled car tires as a material component of sustainable and environmentally friendly tram track structures may be one of the most effective ways to manage rubber waste within the current trend toward a circular economy, and this study intends to introduce methods for experimental identification and analytical selection of basic static and dynamic parameters of prototype USMs. Full article
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<p>Tram track structure in a mass–spring system: 1—Vignoles rail with rail support and rail fastening system, 2—discrete or strip support with USM, 3—concrete track base plate, 4—tunnel invert slab. Elements of the mass–spring system are marked in orange.</p>
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<p>Tram track structure in a mass–spring system: 1—grooved rail with rail fastening system, 2—wooden sleeper, 3—ballast, 4—reinforced concrete trough, 5—discrete or strip support with USM, 6—tunnel invert slab. Elements of the mass–spring system are marked in orange.</p>
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<p>Tram track structure in a mass–spring system: 1—grooved rail, 2—rail web filler block, 3—embedded rail system (ERS) grouting, 4—reinforced concrete track base plate, 5—concrete filling, 6—kerbstone with concrete bench, 7—continuous support with USM, 8—consolidated formation. Elements of the mass–spring system are marked in orange.</p>
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<p>Recycling of end-of-life tires: (<b>a</b>) mechanically removed steel (for recycling) against the background of a pile of tires at the storage yard; (<b>b</b>) mechanically shredded tires (left side of the photograph); (<b>c</b>) SBR granulate; (<b>d</b>) SBR fibres.</p>
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<p>Photographs of selected USM samples with varying hole sizes: (<b>a</b>) Sample no. 175.1; (<b>b</b>) Sample no. 178.1; (<b>c</b>) Sample no. 179.1.</p>
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<p>Test stand for the determination of static and dynamic elastic characteristics of USMs: (<b>a</b>) Sample no. 169.1 (10 mm); (<b>b</b>) Sample no. 175.1 (25 mm).</p>
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<p>Static elastic characteristics of three samples of USM no. 175.</p>
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<p>Dynamic elastic characteristics of USM sample no. 175.1 at various load frequencies (initial static load of 0.02 N/mm<sup>2</sup>).</p>
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<p>Comparison of the static elastic characteristics of four samples with a density of 600 kg/m<sup>3</sup>.</p>
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<p>Influence of USM thickness on its static bedding modulus at varying load ranges (for samples with a density of 600 kg/m<sup>3</sup>).</p>
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<p>Comparison of the dynamic elastic characteristics at 5 Hz of four samples with a density of 600 kg/m<sup>3</sup> (initial static load of 0.02 N/mm<sup>2</sup>).</p>
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<p>Influence of USM thickness on its dynamic bedding modulus tested at various frequencies (for samples with a density of 600 kg/m<sup>3</sup>).</p>
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<p>Influence of load frequency on the dynamic bedding modulus of USMs with varying thicknesses and a density of 600 kg/m<sup>3</sup> (initial static load of 0.02 N/mm<sup>2</sup>).</p>
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<p>Comparison of the static elastic characteristics of five samples with a density of 500 kg/m<sup>3</sup>.</p>
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<p>Influence of USM thickness on its static bedding modulus at varying load ranges (for samples with a density of 500 kg/m<sup>3</sup>).</p>
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<p>Comparison of the dynamic elastic characteristics at 5 Hz of five samples with a density of 500 kg/m<sup>3</sup> (initial static load of 0.02 N/mm<sup>2</sup>).</p>
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<p>Influence of USM thickness on its dynamic bedding modulus tested at various frequencies (for samples with a density of 500 kg/m<sup>3</sup>).</p>
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<p>Influence of load frequency on the dynamic bedding modulus of USMs with varying thicknesses and a density of 500 kg/m<sup>3</sup> (initial static load of 0.02 N/mm<sup>2</sup>).</p>
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<p>Comparison of the static elastic characteristics for USM samples with corresponding thicknesses and varying densities (blue curves—density 600 kg/m<sup>3</sup>, orange curves—density 500 kg/m<sup>3</sup>): (<b>a</b>) 15 mm thick samples; (<b>b</b>) 20 mm thick samples; (<b>c</b>) 25 mm thick samples.</p>
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<p>Comparison of the dynamic elastic characteristics at 5 Hz for USM samples with corresponding thicknesses and varying densities (blue curves—density 600 kg/m<sup>3</sup>, orange curves—density 500 kg/m<sup>3</sup>): (<b>a</b>) 15 mm thick samples; (<b>b</b>) 20 mm thick samples; (<b>c</b>) 25 mm thick samples.</p>
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<p>Comparison of the static elastic characteristics for USM samples with corresponding thicknesses and varying space filling (blue curves—no holes, orange curves—medium holes, grey curves—large holes): (<b>a</b>) 20 mm thick samples; (<b>b</b>) 25 mm thick samples.</p>
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<p>Comparison of the dynamic elastic characteristics at 5 Hz for USM samples with corresponding thicknesses and varying space filling (blue curves—no holes, orange curves—medium holes, grey curves—large holes): (<b>a</b>) 20 mm thick samples; (<b>b</b>) 25 mm thick samples.</p>
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<p>Type 1 track structure: 1—Vignoles rail 49E1, 2—rail support and rail fastening system, 3—concrete slab, 4—USM, 5—protective layer of unbound aggregate mixture.</p>
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<p>Type 2 track structure: 1—Vignoles rail 49E1, 2—rail support and rail fastening system, 3—concrete beam, 4—USM, 5—protective layer of unbound aggregate mixture.</p>
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<p>Reference tram vehicle—PESA “Swing” 120Na.</p>
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<p>Static elastic characteristics of USM sample no. 175.1.</p>
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<p>Diagram of the floating slab system deflections in two types of tram track structures with USMs: (<b>a</b>) Type 1 (concrete slab); (<b>b</b>) Type 2 (concrete beams).</p>
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<p>Diagram of compressive stresses under the floating slab system in two types of tram track structures with USMs: (<b>a</b>) Type 1 (concrete slab); (<b>b</b>) Type 2 (concrete beams).</p>
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12 pages, 7286 KiB  
Article
Online Quality Control of Powder Bed Fusion with High-Resolution Eddy Current Testing Inductive Sensor Arrays
by Pedro Faria, Rodolfo L. Batalha, André Barrancos and Luís S. Rosado
Sensors 2024, 24(21), 6827; https://doi.org/10.3390/s24216827 - 24 Oct 2024
Viewed by 427
Abstract
This paper presents the development of a novel eddy current array (ECA) system for real-time, layer-by-layer quality control in powder bed fusion (PBF) additive manufacturing. The system is integrated into the recoater of a PBF machine to provide spatially resolved electrical conductivity imaging [...] Read more.
This paper presents the development of a novel eddy current array (ECA) system for real-time, layer-by-layer quality control in powder bed fusion (PBF) additive manufacturing. The system is integrated into the recoater of a PBF machine to provide spatially resolved electrical conductivity imaging of the manufactured part. The system features an array of 40 inductive sensors spaced at 1 mm pitch and is capable of performing a full array readout every 0.192 mm at 100 mm/s recoater speed. Array scalability was achieved through the careful selection of the electromagnetic configuration, miniaturized and seamlessly integrated sensor elements, and the use of advanced mixed signal processing techniques. Experimental validation was performed on stainless steel 316L parts, successfully detecting metallic structures and confirming system performance in both laboratory and real-time PBF environments. The prototype achieved a signal-to-noise ratio (SNR) of 26.5 dB, discriminating metal from air and thus demonstrating its potential for improving PBF part design, process optimization, and defect detection. Full article
(This article belongs to the Section Fault Diagnosis & Sensors)
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<p>Powder bed fusion quality control with eddy current sensors.</p>
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<p>Eddy current array monitoring system block diagram.</p>
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<p>Sensing coils and excitation element coil.</p>
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<p>Excitation driver circuit schematic.</p>
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<p>Sensor amplifier circuit schematic.</p>
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<p>Eddy current array monitoring system PCB and 3D-printed enclosure.</p>
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<p>Digital signal processing performed using the dsPIC33 microcontrollers.</p>
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<p>Data interface between the ESP32-S3 and the several dsPIC33 microcontroller instances.</p>
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<p>Eddy current array monitoring system user interface.</p>
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<p>Two-dimensional imaging result on a two-dimensional scan over part 1.</p>
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<p>Two-dimensional imaging result on a two-dimensional scan over part 2.</p>
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<p>ECA system deployed in a RenAM 500S Flex PBF machine.</p>
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<p>Real-time imaging results of several layers of the PBF-produced part.</p>
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<p>Real-time imaging results of several layers of the PBF-produced part.</p>
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17 pages, 8507 KiB  
Article
Development of an Electromyography Signal Acquisition Prototype and Statistical Validation Against a Commercial Device
by Erick Guzmán-Quezada, Santiago Lomeli-Garcia, Jorge Velazco-Garcia, Maby Jonguitud-Ceballos, Adriana Vega-Martinez, Juan Ojeda-Galvan, Francisco J. Alvarado-Rodríguez and Fernanda Reyes-Jiménez
Sensors 2024, 24(21), 6787; https://doi.org/10.3390/s24216787 - 22 Oct 2024
Viewed by 566
Abstract
Electromyography (EMG) stands out as an accessible and inexpensive method for identifying muscle contractions on the surface and within deeper muscle tissues. Using specialized electronic circuits for amplification and filtering can help develop simple but effective systems for detecting and analyzing these signals. [...] Read more.
Electromyography (EMG) stands out as an accessible and inexpensive method for identifying muscle contractions on the surface and within deeper muscle tissues. Using specialized electronic circuits for amplification and filtering can help develop simple but effective systems for detecting and analyzing these signals. However, EMG devices developed by research teams frequently lack rigorous methodologies for validating the quality of the signals they record compared to those obtained by commercial systems that have undergone extensive testing and regulatory approval for market release. This underscores the critical need for standardized validation techniques to reliably assess the performance of experimental devices relative to established commercial equipment. Hence, this study introduces a methodology for the development and statistical validation of a laboratory EMG circuit compared with a professional device available on the market. The experiment simultaneously recorded the muscle electrical activity of 18 volunteers using two biosignal acquisition devices—a prototype EMG and a commercial system—both applied in parallel at the same recording site. Volunteers performed a series of finger and wrist extension movements to elicit myoelectric activity in these forearm muscles. To achieve this, it was necessary to develop not only the EMG signal conditioning board, but also two additional interface boards: one for enabling parallel recording on both devices and another for synchronizing the devices with the task programmatically controlled in Python that the volunteers were required to perform. The EMG signals generated during these tasks were recorded simultaneously by both devices. Subsequently, 22 feature indices commonly used for classifying muscular activity patterns were calculated from two-second temporal windows of the recordings to extract detailed temporal and spatial characteristics. Finally, the Mean Absolute Percentage Error (MAPE) was computed to compare the indices from the prototype with those from the commercial device, using this method as a validation system to assess the quality of the signals recorded by the prototype relative to the commercial equipment. A concordance of 87.6% was observed between the feature indices calculated from the recordings of both devices, suggesting high effectiveness and reliability of the EMG signals recorded by the prototype compared to the commercial device. These results validate the efficacy of our EMG prototype device and provide a solid foundation for the future evaluation of similar devices, ensuring their reliability, accuracy, and suitability for research or clinical applications. Full article
(This article belongs to the Special Issue EMG Sensors and Signal Processing Technologies)
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<p>(<b>a</b>) Muscle signal processing stages implemented in the EMG prototype and (<b>b</b>) the design of the electronic board using EAGLE software; top and bottom views.</p>
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<p>(<b>a</b>) Electronic board developed for the connection between the electrodes and the forearm. This board sends raw data to the Biopac® device and the EMG prototype. (<b>b</b>) The second electronic board connects to the EMG prototype. It transmits the muscle signal information to the Biopac® through the connectors it has, which are similar to those of the previous board. These connect through the SS60L cable. (<b>c</b>) Connection diagram of the experimental elements, showing a representation of a subject with board 1 connected on the forearm, its connection to the Biopac®, and the EMG prototype. It also shows the connection of the prototype to the microcontroller and the second board, its connection to the Biopac®, and the connection between the Biopac® and a computer. The connection between the Teensy 3.2 board and the Biopac® (via the SS60L cable) functions as an analog trigger.</p>
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<p>(<b>a</b>) Representation of a volunteer during recording, showing the body posture and arm placement during the execution of the trials; (<b>b</b>) movements requested by the Python interface that participants had to perform; and (<b>c</b>) the time diagram of the recording acquired by the Biopac® device, showing the synchronization of the signals captured by the EMG prototype and the Biopac®, as well as the DAC signal used as a trigger.</p>
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<p>Stages of muscle signal processing implemented in the EMG prototype. (<b>a</b>) Diagram of signal pre-amplification using an instrumentation amplifier; (<b>b</b>) passive high-pass filter; (<b>c</b>) active low-pass filter; (<b>d</b>) the second stage of amplification; and (<b>e</b>) 60 Hz notch filter.</p>
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<p>(<b>a</b>) The final version of the EMG prototype includes connectors compatible with the Arduino UNO model and connectors for interacting with other electronic boards; (<b>b</b>) electronic board for the communication of muscle signals after processing; (<b>c</b>) electronic circuit that interacts with the skin surface, indicating the connections of the electrodes and the U1 connector to interact with the EMG prototype; (<b>d</b>) connection of all modules; and (<b>e</b>) volunteer with the setup during the recording session.</p>
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<p>(<b>a</b>) EMG signals in the time domain: the left side shows the signal acquired by the Biopac® equipment, and the right side shows the EMG signal recorded with our prototype. The dashed lines indicate the start and end marked with the visual interface. (<b>b</b>) Frequency analysis using the Fourier transform after applying a band-pass filter from 20 to 200 Hz. (<b>c</b>) Spectrogram of each of the signals.</p>
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<p>Heatmap of feature values by subject, showing the (1 − MAPE) values for each feature and subject. Darker colors indicate better agreement between the EMG prototype and Biopac® equipment.</p>
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<p>Average (1 − MAPE) per subject, showing the agreement between the EMG prototype and Biopac® equipment for each subject.</p>
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<p>Average (1 − MAPE) per feature, showing the agreement between the EMG prototype and Biopac® equipment for each feature.</p>
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14 pages, 7209 KiB  
Article
Detection and Early Warning of Duponchelia fovealis Zeller (Lepidoptera: Crambidae) Using an Automatic Monitoring System
by Edgar Rodríguez-Vázquez, Agustín Hernández-Juárez, Audberto Reyes-Rosas, Carlos Patricio Illescas-Riquelme and Francisco Marcelo Lara-Viveros
AgriEngineering 2024, 6(4), 3785-3798; https://doi.org/10.3390/agriengineering6040216 - 18 Oct 2024
Viewed by 859
Abstract
In traditional pest monitoring, specimens are manually inspected, identified, and counted. These techniques can lead to poor data quality and hinder effective pest management decisions due to operational and economic limitations. This study aimed to develop an automatic detection and early warning system [...] Read more.
In traditional pest monitoring, specimens are manually inspected, identified, and counted. These techniques can lead to poor data quality and hinder effective pest management decisions due to operational and economic limitations. This study aimed to develop an automatic detection and early warning system using the European Pepper Moth, Duponchelia fovealis (Lepidoptera: Crambidae), as a study model. A prototype water trap equipped with an infrared digital camera controlled using a microprocessor served as the attraction and capture device. Images captured by the system in the laboratory were processed to detect objects. Subsequently, these objects were labeled, and size and shape features were extracted. A machine learning model was then trained to identify the number of insects present in the trap. The model achieved 99% accuracy in identifying target insects during validation with 30% of the data. Finally, the prototype with the trained model was deployed in the field for result confirmation. Full article
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<p>Trap body design and placement of the infrared (IR) camera module. (<b>a</b>) Dimensions of the trap body and location of the watertight box (WPB). The green box indicates the opening for accessing the study model insect, (<b>b</b>) arrangement of the IR camera within the waterproof box affixed to the trap body, providing a view of the bucket bottom, and (<b>c</b>) positioning of the IR camera within the lower section of the waterproof box.</p>
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<p>Schematic diagram of the electronic components comprising the prototype. (<b>a</b>) Controller power supply, (<b>b</b>) solar panel, (<b>c</b>) non-standard rechargeable lead-acid battery, (<b>d</b>) raspberry Pi 4B© controller, (<b>e</b>) infrared (IR) camera module, and (<b>f</b>) ESP32 microcontroller.</p>
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<p>Image processing steps by the prototype. (<b>a</b>) Original infrared (IR) image captured using the utilized software. (<b>b</b>) flowchart depicting the image processing pipeline, (<b>c</b>) binarization of the grayscale image to eliminate background noise, and (<b>d</b>) contour detection and extraction in the binarized image to quantify characteristics of identified objects.</p>
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<p>Flowchart of trap operation.</p>
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<p>System installation for field testing. (<b>a</b>) Trap installation within the strawberry plantation; and (<b>b</b>) functional inspections and screenshots of the prototype during field establishment.</p>
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<p>Optimization of the hyperparameter and input variable of the Antormelo model. (<b>a</b>) Optimizing decision tree model depth shows how model performance varies as a function of the maximum depth of the tree; (<b>b</b>) classification of objects based on the characteristics established by the decision tree model implemented in the created system.</p>
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<p>Incorporation of a decision tree model for <span class="html-italic">D. fovealis</span> detection.</p>
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<p>Detection of EPM. Within the green square the objects identified as “Insect” are shown, while in the red box the objects belonging to the “Non-insect” class are classified. (<b>a</b>) The image is displayed with the indicated identification and objects with various sizes are detected, expanding the established range; (<b>b</b>) identification of the insect and application of filter to reduce objects of no interest.</p>
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<p>(<b>a</b>) Field selectivity of the model in identifying D. fovealis; (<b>b</b>) daily insect counts monitored using the developed system; (<b>c</b>) captures of EPM recorded through manual counting.</p>
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21 pages, 6351 KiB  
Article
The Influence of Structure Optimization on Vortex Suppression and Energy Dissipation in the Draft Tube of Francis Turbine
by Xiaoxu Zhang, Cong Nie and Zhumei Luo
Processes 2024, 12(10), 2249; https://doi.org/10.3390/pr12102249 - 15 Oct 2024
Viewed by 666
Abstract
Under partial load operating conditions, vortex rope generation in the draft tube of a Francis turbine is considered one of the main reasons for hydro unit vibration. In this paper, a Francis turbine HLA551-LJ-43 in the laboratory was taken as a prototype. Numerical [...] Read more.
Under partial load operating conditions, vortex rope generation in the draft tube of a Francis turbine is considered one of the main reasons for hydro unit vibration. In this paper, a Francis turbine HLA551-LJ-43 in the laboratory was taken as a prototype. Numerical simulations of the entire flow passage were carried out. Four different hydro-turbines were chosen to analyze the effect of vortex suppression, which were named the prototype turbine (N-J), the turbine with J-grooves installed on its conical section (W-J), the one with extending runner cone (C), and the one that considered the J-grooves and the extending runner cone at the same time (J+C). Under the part load conditions in which the vortex rope is easily generated (0.4–0.8 times design flow QBEP), the spectrum characteristics of pressure fluctuation, the morphology of vortex rope, and the energy dissipation based on the entropy production theory in the draft tube were studied. The results show that the three optimized structures W-J, C, and J+C could reduce the pressure pulsation in the conical section of the draft tube, weaken the eccentricity of the vortex rope, and decrease the energy losses in the runner and draft tube. It is worth mentioning that the turbine with a J+C optimized structure had the most potent effect on vortex suppression and energy dissipation. Primarily when operating in deep partial load (DPL) conditions, the efficiency of the turbine with a J+C optimized structure was increased by 13.7% compared to the prototype turbine, and the main frequency amplitude of the pressure pulsation in the draft tube was reduced to 32% of the prototype. Full article
(This article belongs to the Section Process Control and Monitoring)
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<p>Prototype hydro turbine HLA551-LJ-43.</p>
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<p>Three-dimensional model of the prototype turbine.</p>
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<p>Grid independence verification.</p>
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<p>The y plus of the Francis turbine blade.</p>
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<p>Unstructured hexahedral grids of each flow component.</p>
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<p>The layout of the modification measures of W-J and C, the location of the monitoring points, and the monitoring surface.</p>
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<p>Pressure fluctuation at monitoring points TS2 of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
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<p>Pressure fluctuation spectrogram at monitoring points TS2 of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) Q* = 53% (DPL); (<b>b</b>) Q* = 69% (PL).</p>
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<p>The distribution of the circumferential and axial velocity of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
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<p>The vortex rope zone of the prototype and the three structural optimization measures under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
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<p>The streamlines of section TP1 of the draft tube under DPL and PL conditions, listed as: (<b>a</b>) <span class="html-italic">Q</span>* = 53% (DPL); (<b>b</b>) <span class="html-italic">Q</span>* = 69% (PL).</p>
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<p>LEPR distribution on the outlet of runner and draft tube of different modification measures under DPL operating conditions (<span class="html-italic">Q</span>* = 53%), listed as: (<b>a</b>) N-J; (<b>b</b>) W-J; (<b>c</b>) C; (<b>d</b>) C+J.</p>
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<p>Hydraulic losses of four turbine models under different operating conditions.</p>
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<p>Efficiency of four turbine models under different operating conditions.</p>
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27 pages, 5309 KiB  
Article
A Case Study on the Integration of Powerline Communications and Visible Light Communications from a Power Electronics Perspective
by Felipe Loose, Juan Ramón Garcia-Meré, Adrion Andrei Rosanelli, Carlos Henrique Barriquello, José Antonio Fernandez Alvárez, Juan Rodríguez and Diego González Lamar
Sensors 2024, 24(20), 6627; https://doi.org/10.3390/s24206627 - 14 Oct 2024
Viewed by 654
Abstract
This paper presents a dual-purpose LED driver system that functions as both a lighting source and a Visible Light Communication (VLC) transmitter integrated with a Powerline Communication (PLC) network under the PRIME G3 standard. The system decodes PLC messages from the powerline grid [...] Read more.
This paper presents a dual-purpose LED driver system that functions as both a lighting source and a Visible Light Communication (VLC) transmitter integrated with a Powerline Communication (PLC) network under the PRIME G3 standard. The system decodes PLC messages from the powerline grid and transmits the information via LED light to an optical receiver under a binary phase shift keying (BPSK) modulation. The load design targets a light flux of 800 lumens, suitable for LED light bulb applications up to 10 watts, ensuring practicality and energy efficiency. The Universal Asynchronous Receiver-Transmitter (UART) module enables communication between the PLC and VLC systems, allowing for an LED driver with dynamic control and real-time operation. Key signal processing stages are commented and developed, including a hybrid buck converter with modulation capabilities and a nonlinear optical receiver to regenerate the BPSK reference signal for VLC. Results show a successful prototype working under a laboratory environment. Experimental validation shows successful transmission of bit streams from the PLC grid to the VLC setup. A design guideline is presented in order to dictate the design of the electronic devices involved in the experiment. Finally, this research highlights the feasibility of integrating PLC and VLC technologies, offering an efficient and cost-effective solution for data transmission over existing infrastructure. Full article
(This article belongs to the Special Issue Challenges and Future Trends in Optical Communications)
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<p>Block diagram of the system’s architecture.</p>
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<p>Differences between AF and DF solutions.</p>
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<p>General channel model.</p>
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<p>Comparison of the AF and DF case for the BPSK BER curve.</p>
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<p>VLC system block diagram architecture.</p>
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<p>Proposed hybrid converter topology.</p>
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<p>Waveforms on the coupled coil of the converter.</p>
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<p>Circuit model of the dynamics of proposed converter.</p>
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<p>Simplified first order circuit to determine coupling capacitor.</p>
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<p>Simplified first order circuit to determine coupling capacitor.</p>
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<p>Dimensions of SMD LED for the load.</p>
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<p>Linear model approximation of IxV curve of the proposed LED load.</p>
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<p>Time diagram of the PLC network and interaction with the VLC system.</p>
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<p>Waveforms in time and frequency domains of the LED current.</p>
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<p>Schematic of receiver circuit.</p>
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<p>Frequency responses of the proposed prototype.</p>
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<p>Block diagram of experiment.</p>
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<p>Top view of prototype.</p>
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<p>Receiver prototype.</p>
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<p>Receiver prototype.</p>
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<p>Spectrum of PLC message.</p>
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<p>PLC parameters for modified PLC &amp; Go application.</p>
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<p>Bit stream (<b>top</b>) and its BPSK signal (<b>bottom</b>).</p>
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<p>BPSK signal. From top to bottom: optical receiver output (green); input BPSK signal (blue); LED current (magenta).</p>
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<p>BPSK signal on the receiver. From top to bottom: input BPSK signal (green); optical receiver output (blue); received optical signal (yellow); average value reference for comparator (magenta).</p>
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19 pages, 4480 KiB  
Article
Nonlinear Analysis and Closed-Form Solution for Overhead Line Magnetic Energy Harvester Behavior
by Alexander Abramovitz, Moshe Shwartsas and Alon Kuperman
Appl. Sci. 2024, 14(19), 9146; https://doi.org/10.3390/app14199146 - 9 Oct 2024
Viewed by 534
Abstract
Recently, much attention has been given to the development of various energy harvesting technologies to power remote electronic sensors, data loggers, and communicators that can be installed on smart grid systems. Magnetic energy harvesting is, perhaps, the most straightforward way to capture a [...] Read more.
Recently, much attention has been given to the development of various energy harvesting technologies to power remote electronic sensors, data loggers, and communicators that can be installed on smart grid systems. Magnetic energy harvesting is, perhaps, the most straightforward way to capture a significant amount of power from a current-carrying overhead line. Since the harvester is expected to have a small size, the high currents of the distribution system easily saturate its magnetic core. As a result, the operation of the magnetic harvester is highly nonlinear and makes precise analytical modeling difficult. The operation of an overhead line magnetic energy harvester (OLMEH) generating significant DC power output into a constant voltage load was investigated in this paper. The analysis method was based on the Froelich equation to analytically model the nonlinearity of the core’s BH characteristic. The main findings of this piecewise nonlinear analysis include a closed-form solution that accounts for both the core and rectifiers’ nonlinearities and provides an accurate prediction of OLMEH transfer window length, output current, and harvested power. Continuous and discontinuous operational modes are identified and the mode transition boundary is obtained quantitatively. The theoretical investigation was concluded by comparison with a computer simulation and also verified by the experimental results of a laboratory prototype harvester. A good agreement was found. Full article
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<p>Overhead line energy harvester under constant voltage load.</p>
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<p>Comparison of the measured BH curve of the silicon steel core sample (EILOR MAGNETIC CORES) to its Froelich approximation.</p>
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<p>PSIM—generated comparison plot of the simulated BH curve vs. the Froelich approximation (1) (<b>a</b>); MATHCAD—generated Froelich Equation (1) vs. <span class="html-italic">atan</span>(<span class="html-italic">*</span>) approximation, vs. the piecewise-linear approximation of the BH curve (<b>b</b>).</p>
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<p>Simplified OLMEH model (<b>a</b>) and its DCM equivalent circuits during the positive half-cycle with: rectifier OFF (State 1) (<b>b</b>); rectifier ON (State 2) (<b>c</b>).</p>
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<p>OLMEH’s key simulated waveforms in the discontinuous mode.</p>
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<p>Comparison plot of the <span class="html-italic">sin</span>(<span class="html-italic">x</span>) function vs. the linear approximation, vs. the parabolic approximation, and vs. the “mirrored Froelich equation” (15) (for <span class="html-italic">K</span><sub>1</sub> = 3.232, <span class="html-italic">K</span><sub>2</sub> = 2.861).</p>
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<p>OLMEH’s simulated waveforms in: DCM due to low current <span class="html-italic">I</span><sub>1</sub> = 50 A rms, <span class="html-italic">V<sub>b</sub></span> = 23 V (<b>a</b>); DCM due to high voltage <span class="html-italic">I</span><sub>1</sub> = 100 A rms, <span class="html-italic">V<sub>b</sub></span> = 25 V (<b>b</b>); DCM-CCM boundary <span class="html-italic">I</span><sub>1</sub> = 100 A rms, <span class="html-italic">V<sub>b</sub></span> = 22 V (<b>c</b>); CCM due to high current <span class="html-italic">I</span><sub>1</sub> = 125 A rms, <span class="html-italic">V<sub>b</sub> =</span> 23 V (<b>d</b>); CCM due to low voltage <span class="html-italic">I</span><sub>1</sub> = 100 A rms, <span class="html-italic">V<sub>b</sub></span> = 22 V (<b>e</b>).</p>
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<p>View of the experimental prototype OLMEH (<b>a</b>) and its test bench (<b>b</b>).</p>
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<p>Typical waveforms of the experimental overhead line energy harvester at: <span class="html-italic">I</span><sub>1</sub> = 100 A rms and <span class="html-italic">V<sub>b</sub></span> = 25 V (<b>a</b>); <span class="html-italic">I</span><sub>1</sub> = 100 A and <span class="html-italic">V<sub>b</sub></span> = 35 V (<b>b</b>); <span class="html-italic">I</span><sub>1</sub> = 75 A rms and <span class="html-italic">V<sub>b</sub></span> = 23 V (<b>c</b>); <span class="html-italic">I</span><sub>1</sub> = 150 A rms and <span class="html-italic">V<sub>b</sub></span> = 23 V (<b>d</b>). Vert. scale: <span class="html-italic">I</span><sub>1</sub>—200 A/div; <span class="html-italic">V<sub>in</sub></span>—20 V/div; <span class="html-italic">V</span><sub>1</sub>—2 V/div; <span class="html-italic">I<sub>in</sub></span>—5 A/div; hor. scale 5 ms/div.</p>
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<p>Measured OLMEH output power vs. the CVL voltage at a line current of 100 A rms and 180 A rms.</p>
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<p>Comparison of the calculated vs. the measured output power as a function of the line current at fixed CVL voltage <span class="html-italic">V<sub>b</sub></span> = 30 V.</p>
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<p>Comparison of the calculated power, Pocalc, vs. the measured power, Pomeas, output power (DCM) as a function of the CVL voltage at a fixed line current (100 A rms).</p>
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17 pages, 7212 KiB  
Article
Zigbee-Based Wireless Sensor Network of MEMS Accelerometers for Pavement Monitoring
by Nicky Andre Prabatama, Mai Lan Nguyen, Pierre Hornych, Stefano Mariani and Jean-Marc Laheurte
Sensors 2024, 24(19), 6487; https://doi.org/10.3390/s24196487 - 9 Oct 2024
Viewed by 1124
Abstract
In this paper, we propose a wireless sensor network for pavement health monitoring exploiting the Zigbee technology. Accelerometers are adopted to measure local accelerations linked to pavement vibrations, which are then converted into displacements by a signal processing algorithm. Each device consists of [...] Read more.
In this paper, we propose a wireless sensor network for pavement health monitoring exploiting the Zigbee technology. Accelerometers are adopted to measure local accelerations linked to pavement vibrations, which are then converted into displacements by a signal processing algorithm. Each device consists of an on-board unit buried in the roadway and a roadside unit. The on-board unit comprises a microcontroller, an accelerometer and a Zigbee module that transfers acceleration data wirelessly to the roadside unit. The roadside unit consists of a Raspberry Pi, a Zigbee module and a USB Zigbee adapter. Laboratory tests were conducted using a vibration table and with three different accelerometers, to assess the system capability. A typical displacement signal from a five-axle truck was applied to the vibration table with two different displacement peaks, allowing for two different vehicle speeds. The prototyped system was then encapsulated in PVC packaging, deployed and tested in a real-life road situation with a fatigue carousel featuring rotating truck axles. The laboratory and on-road measurements show that displacements can be estimated with an accuracy equivalent to that of a reference sensor. Full article
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<p>(<b>a</b>) System Architecture; (<b>b</b>) prototype tested in the laboratory.</p>
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<p>(<b>a</b>) Block diagram of the embedded unit; (<b>b</b>) embedded unit prototype.</p>
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<p>(<b>a</b>) Block diagram of the roadside unit; (<b>b</b>) roadside unit system.</p>
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<p>Five-axle truck displacement signals used for the vibrating table.</p>
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<p>(<b>a</b>) Vibrating pot test; (<b>b</b>) vibrating table test.</p>
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<p>Description of the five steps adopted to extract the displacement time histories from raw acceleration data.</p>
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<p>Vibrating table tests: (<b>a</b>) example of raw acceleration signal; (<b>b</b>) velocity history after the first integration; (<b>c</b>) displacement history after the second time integration; (<b>d</b>) final displacement history provided by the Hilbert transform.</p>
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<p>Vibrating table tests featuring a peak displacement of 0.25 mm and a vehicle speed of 45 km/h: (<b>a</b>) exemplary raw ADXL355 acceleration signal; (<b>b</b>–<b>d</b>) displacement histories obtained with the adopted signal processing procedure applied to measurements collected with the three MEMS accelerometers.</p>
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<p>Vibrating table tests featuring a peak displacement of 0.5 mm and a vehicle speed of 45 km/h: (<b>a</b>) exemplary raw MS1002 acceleration signal; (<b>b</b>–<b>d</b>) displacement histories obtained with the adopted signal processing procedure applied to measurements collected with the three MEMS accelerometers.</p>
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<p>Vibrating table tests featuring a peak displacement of 0.25 mm and a vehicle speed of 18 km/h: (<b>a</b>) raw ADXL355 acceleration signal; (<b>b</b>–<b>d</b>) displacement histories obtained with measurements collected with the three MEMS accelerometers.</p>
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<p>Vibrating table tests featuring a peak displacement of 0.25 mm and a vehicle speed of 92 km/h: (<b>a</b>) raw ADXL355 acceleration signal; (<b>b</b>–<b>d</b>) displacement histories obtained with measurements collected with the three MEMS accelerometers.</p>
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<p>Designed and fabricated PVC packaging, and assembly of the embedded unit.</p>
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<p>(<b>a</b>) Device installation scheme; (<b>b</b>) installation of the device in the pavement.</p>
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<p>(<b>a</b>) Position of the roadside unit on the test track; (<b>b</b>) accelerated pavement testing setup.</p>
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<p>(<b>a</b>) Raw acceleration, and (<b>b</b>) displacement time history obtained with the reported signal processing strategy.</p>
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16 pages, 7326 KiB  
Article
A Lyapunov Theory-Based SEIG–STATCOM Voltage Regulation Control Strategy
by Zeyu Zhang, Pingping Gong and Ziguang Lu
Energies 2024, 17(19), 4992; https://doi.org/10.3390/en17194992 - 7 Oct 2024
Viewed by 642
Abstract
To improve the voltage regulation of asynchronous generators during load switching, a Lyapunov-based control strategy has been proposed to stabilize the generator’s voltage by connecting a static synchronous compensator. By constructing a Lyapunov function from the mathematical model, the error tracking problem is [...] Read more.
To improve the voltage regulation of asynchronous generators during load switching, a Lyapunov-based control strategy has been proposed to stabilize the generator’s voltage by connecting a static synchronous compensator. By constructing a Lyapunov function from the mathematical model, the error tracking problem is transformed into a global asymptotic stability problem of the Lyapunov function at the equilibrium point. The outer loop linearizes the direct current (DC) voltage control process, while the inner loop replaces integral terms with differential terms. The proposed Lyapunov method achieves linearized voltage control with a quadratic outer loop structure and the inner loop differential structure exhibits a shorter transient process, outperforming traditional methods. Simulation and experimental tests were then used, where the latter was a down-scale laboratory prototype experiment. Compared to traditional (voltage-oriented control) VOC, the outer loop (Lyapunov-function-based control) LBC reduces the DC voltage transient processes by approximately 9.4 milliseconds, while the inner loop LBC reduces both alternating current (AC) and DC voltage transient processes by approximately 2.6 ms and 8.7 ms, respectively. Full article
(This article belongs to the Special Issue Advanced Control in Power Electronics, Drives and Generators)
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<p>Flowchart of Lyapunov function and control law.</p>
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<p>Schematic diagram of SEIG–STATCOM.</p>
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<p>Outer–inner loop of controller: (<b>a</b>) VOC (traditional control method); (<b>b</b>) LBC.</p>
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<p>Inner loop control block diagram.</p>
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<p>The Bode plot of logarithmic sensitivity: (<b>a</b>) sensitivity to <span class="html-italic">L<sub>c</sub></span>; (<b>b</b>) sensitivity to <span class="html-italic">R<sub>c</sub></span>.</p>
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<p>The zero-pole distribution of the current closed-loop transfer function.</p>
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<p>The mathematical model of the SEIG–STATCOM in Simulink.</p>
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<p>The dynamic performance of the <span class="html-italic">d</span>-axis PI controller.</p>
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<p>The dynamic performance of the proposed and VOC.</p>
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<p>Prototype experiment: (<b>a</b>) experimental platform of power generation system; (<b>b</b>) experiment block diagram of voltage regulation for SEIG.</p>
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<p>The performance of terminal voltage without STATCOM.</p>
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<p>The dynamic performance of the LBC (inner controller) and VOC.</p>
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<p>The dynamic performance of the LBC (outer controller) and VOC.</p>
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