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Search Results (184)

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16 pages, 7520 KiB  
Article
On the Development of Embroidered Reconfigurable Dipole Antennas: A Textile Approach to Mechanical Reconfiguration
by Sofia Bakogianni, Aris Tsolis, Chrysanthi Angelaki and Antonis A. Alexandridis
Electronics 2024, 13(18), 3649; https://doi.org/10.3390/electronics13183649 - 13 Sep 2024
Viewed by 226
Abstract
A design framework for developing full-textile reconfigurable dipole antennas is proposed for wearable applications. To this end, a precise embroidery process using conductive threads is applied to properly manage the antenna structure. Further, mechanical reconfiguration to enhance antenna operation by using solely clothing [...] Read more.
A design framework for developing full-textile reconfigurable dipole antennas is proposed for wearable applications. To this end, a precise embroidery process using conductive threads is applied to properly manage the antenna structure. Further, mechanical reconfiguration to enhance antenna operation by using solely clothing components is outlined. As a proof-of-concept, we present a full-textile embroidered dipole antenna with mechanical frequency reconfiguration. Specifically, reconfiguration is achieved by folding the dipole arms through a triangular formation. Conductive Velcro strips are employed to guide the necessary dipole arrangement. As shown, the proposed design methodology enables frequency tunability that ranges from 780 to 1330 MHz for UHF and L bands, with satisfactory radiation performance. The measured and simulated results are in good agreement, in terms of achieving similar frequency reconfiguration concept, as predicted by the electromagnetic simulation models. Full article
(This article belongs to the Section Microwave and Wireless Communications)
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<p>Embroidery machine while fabricating Shieldex 100 mm TL samples.</p>
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<p>(<b>a</b>) Magnitude, and (<b>b</b>) phase of transmission coefficient S<sub>21</sub> frequency response of fabricated transmission lines made of copper tape and embroidered patterns with a stitch density of 4 threads/mm single layer (SL_d4), 2 threads/mm-double layer (DL_d2), and 4 threads/mm double layer (DL_d4).</p>
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<p>Numerical model of the proposed dipole antenna under different folding states: States I, II, III and IV.</p>
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<p>Fully textile reconfigurable dipole: (<b>a</b>) flat prototype, and (<b>b</b>) folded prototype (State III) back-supported by non-conductive Velcro strips.</p>
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<p>Simulated and measured reflection coefficient frequency response (|S<sub>11</sub>|) of the proposed dipole antenna under folding states: (<b>a</b>) I, (<b>b</b>) II, (<b>c</b>) III, and (<b>d</b>) IV.</p>
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<p>Measured VSWR frequency response of the proposed prototype dipole reconfigurable antenna under all four folding states.</p>
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<p>Fabricated dipole antenna mounted on far-field roll/azimuth positioner at state I.</p>
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<p>Normalized in dB: simulated and measured radiation patterns of the proposed dipole antenna under folding states (<b>a</b>) I, (<b>b</b>) II, (<b>c</b>) III and (<b>d</b>) IV in E- and H-plane.</p>
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<p>Normalized in linear form: Simulated and measured radiation patterns of the proposed dipole antenna under folding states (<b>a</b>) I, (<b>b</b>) II, (<b>c</b>) III and (<b>d</b>) IV in E- and H-Plane.</p>
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<p>Simulated (<b>a</b>) S<sub>11</sub> results for different antenna–phantom distances and (<b>b</b>) SAR-1g distribution for 1 W input power at 945 MHz for folding state II.</p>
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<p>(<b>a</b>) Simulated normalized radiation patterns of dipole antenna on arm of a tissue phantom under folding state II at 945 MHz in <span class="html-italic">xy</span>-plane (E) and <span class="html-italic">xz</span>-plane (H), (<b>b</b>) simulated normalized radiation patterns of dipole antenna in free space under folding state II at 945 MHz in <span class="html-italic">xy</span>-plane (E) and <span class="html-italic">xz</span>-plane (H).</p>
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18 pages, 4812 KiB  
Article
On the Exploration of Temporal Fusion Transformers for Anomaly Detection with Multivariate Aviation Time-Series Data
by Bulent Ayhan, Erik P. Vargo and Huang Tang
Aerospace 2024, 11(8), 646; https://doi.org/10.3390/aerospace11080646 - 9 Aug 2024
Viewed by 713
Abstract
In this work, we explored the feasibility of using a transformer-based time-series forecasting architecture, known as the Temporal Fusion Transformer (TFT), for anomaly detection using threaded track data from the MITRE Corporation’s Transportation Data Platform (TDP) and digital flight data. The TFT architecture [...] Read more.
In this work, we explored the feasibility of using a transformer-based time-series forecasting architecture, known as the Temporal Fusion Transformer (TFT), for anomaly detection using threaded track data from the MITRE Corporation’s Transportation Data Platform (TDP) and digital flight data. The TFT architecture has the flexibility to include both time-varying multivariate data and categorical data from multimodal data sources and conduct single-output or multi-output predictions. For anomaly detection, rather than training a TFT model to predict the outcomes of specific aviation safety events, we train a TFT model to learn nominal behavior. Any significant deviation of the TFT model’s future horizon forecast for the output flight parameters of interest from the observed time-series data is considered an anomaly when conducting evaluations. For proof-of-concept demonstrations, we used an unstable approach (UA) as the anomaly event. This type of anomaly detection approach with nominal behavior learning can be used to develop flight analytics to identify emerging safety hazards in historical flight data and has the potential to be used as an on-board early warning system to assist pilots during flight. Full article
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<p>Temporal Fusion Transformer (TFT) architecture. Reproduced from [<a href="#B19-aerospace-11-00646" class="html-bibr">19</a>].</p>
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<p>Forecasting-based anomaly detection via nominal behavior learning with the TFTs.</p>
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<p>Averaged RMSE profiles as a function of “time before touchdown” resulting from various TFT models for the nominal flight data in the test split with speed as the target output.</p>
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<p>Feature importance rankings for the three TFT models trained with different input feature combinations with speed as the target (<b>a</b>) TFT-1, (<b>b</b>) TFT-2, and (<b>c</b>) TFT-3.</p>
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<p>Averaged RMSE profiles for TFT-2 and TFT-select.</p>
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<p>Averaged RMSE profiles from speed predictions for the TFTs trained to jointly predict speed and altitude (multi-output) in comparison to the single-output TFT model (speed).</p>
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<p>Averaged RMSE profiles from altitude predictions for the TFTs trained to jointly predict speed and altitude (multi-output) in comparison to the single-output TFT model (altitude).</p>
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<p>Averaged RMSE profiles for speed and altitude using the TFT-2 single-output models (speed and altitude modeled separately).</p>
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<p>Fisher’s score for various TFT models as a function of time before touchdown.</p>
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<p>RMSE values of the test split (nominal and UA flight data) for the single output TFT models (speed and altitude outputs) at the 26 timesteps before touchdown—zoomed in for better visualization.</p>
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<p>ROC curve for visualizing the detection performance of the RMSE-threshold-based anomaly detection at the identified time point when used with single outputs and two outputs together.</p>
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18 pages, 446 KiB  
Article
Skip-Gram and Transformer Model for Session-Based Recommendation
by Enes Celik and Sevinc Ilhan Omurca
Appl. Sci. 2024, 14(14), 6353; https://doi.org/10.3390/app14146353 - 21 Jul 2024
Viewed by 779
Abstract
Session-based recommendation uses past clicks and interaction sequences from anonymous users to predict the next item most likely to be clicked. Predicting the user’s subsequent behavior in online transactions becomes a problem mainly due to the lack of user information and limited behavioral [...] Read more.
Session-based recommendation uses past clicks and interaction sequences from anonymous users to predict the next item most likely to be clicked. Predicting the user’s subsequent behavior in online transactions becomes a problem mainly due to the lack of user information and limited behavioral information. Existing methods, such as recurrent neural network (RNN)-based models that model user’s past behavior sequences and graph neural network (GNN)-based models that capture potential relationships between items, miss different time intervals in the past behavior sequence and can only capture certain types of user interest patterns due to the characteristics of neural networks. Graphic models created to improve the current session reduce the model’s success due to the addition of irrelevant items. Moreover, attention mechanisms in recent approaches have been insufficient due to weak representations of users and products. In this study, we propose a model based on the combination of skip-gram and transformer (SkipGT) to solve the above-mentioned drawbacks in session-based recommendation systems. In the proposed method, skip-gram both captures chained user interest in the session thread through item-specific subreddits and learns complex interaction information between items. The proposed method captures short-term and long-term preference representations to predict the next click with the help of a transformer. The transformer in our proposed model overcomes many limitations in turn-based models and models longer contextual connections between items more effectively. In our proposed model, by giving the transformer trained item embeddings from the skip-gram model as input, the transformer has better performance because it does not learn item representations from scratch. By conducting extensive experiments with three real-world datasets, we confirm that SkipGT significantly outperforms state-of-the-art solutions with an average MRR score of 5.58%. Full article
(This article belongs to the Section Computing and Artificial Intelligence)
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<p>Overview of the proposed SkipGT Model.</p>
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<p>The results of ablation study: (<b>a</b>) Ablation results according to the precision values of the datasets. (<b>b</b>) Ablation results according to the mean reciprocal rank values of the datasets.</p>
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<p>Effect of layer number: (<b>a</b>) Effect of number layers on the precision value for datasets. (<b>b</b>) Effect of number layers on the mean reciprocal rank value for datasets.</p>
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<p>Effect of learning rate: (<b>a</b>) Effect of learning rate on the precision value for datasets. (<b>b</b>) Effect of learning rate on the mean reciprocal rank value for datasets.</p>
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<p>Effect of hidden layer number: (<b>a</b>) Effect of hidden number layers on the precision value for datasets. (<b>b</b>) Effect of hidden number layers on the mean reciprocal rank value for datasets.</p>
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23 pages, 16873 KiB  
Article
Performance-Degradation Analysis of the Planetary Roller Screw Mechanism under Multi-Factor Coupling Effects
by Kui Chen, Yongsheng Zhao, Jigui Zheng, Wei Shi and Zhaojing Zhang
Sensors 2024, 24(14), 4460; https://doi.org/10.3390/s24144460 - 10 Jul 2024
Viewed by 526
Abstract
The performance-degradation pattern of the planetary roller screw mechanism (PRSM) is difficult to predict and evaluate due to a variety of factors. Load-carrying capacity, transmission accuracy, and efficiency are the main indicators for evaluating the performance of the PRSM. In this paper, a [...] Read more.
The performance-degradation pattern of the planetary roller screw mechanism (PRSM) is difficult to predict and evaluate due to a variety of factors. Load-carrying capacity, transmission accuracy, and efficiency are the main indicators for evaluating the performance of the PRSM. In this paper, a testing device for the comprehensive performance of the PRSM is designed by taking into account the coupling relationships among temperature rise, vibration, speed, and load. First, the functional design and error calibration of the testing device were conducted. Secondly, the PRSM designed in the supported project was taken as the research object to conduct degradation tests on its load-bearing capacity and transmission accuracy and analyze the changes in transmission efficiency. Third, the thread profile and wear condition were scanned and inspected using a universal tool microscope and an optical microscope. Finally, based on the monitoring module of the testing device, the vibration status during the PRSM testing process was collected in real time, laying a foundation for the subsequent assessment of the changes in the performance state of the PRSM. The test results reveal the law of performance degradation of the PRSM under the coupled effects of temperature, vibration, speed, and load. Full article
(This article belongs to the Section Physical Sensors)
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<p>Structure of planetary roller screw mechanism. 1. Elastic retaining ring; 2. cage; 3. internal ring; 4. roller; 5. nut; 6. screw.</p>
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<p>Design scheme for the loading test device of the PRSM.</p>
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<p>Design scheme of precision measuring device for the PRSM.</p>
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<p>Structure and stress analysis of double-ended hinge.</p>
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<p>Torque test results of the first PRSM loading experiment.</p>
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<p>Torque test results of the second PRSM.</p>
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<p>Torque test results of the second PRSM.</p>
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<p>Assembly debugging and straightness test of the guide rail.</p>
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<p>The testing process of the initial transmission accuracy of the PRSM.</p>
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<p>The results of the initial transmission-accuracy test for the PRSMs.</p>
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<p>Measurement results of positioning error of the PRSM.</p>
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<p>Arrangement of vibration sensors.</p>
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<p>Axial load spectrum.</p>
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<p>Loading test process of the PRSM.</p>
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<p>The test results of the degradation in bearing performance of the PRSM.</p>
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<p>The test results of the degradation in bearing performance of the PRSM.</p>
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<p>Variation trend of driving torque of the PRSM.</p>
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<p>Changing trend of transmission efficiency of PRSM.</p>
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<p>Wear condition of screw threads.</p>
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<p>Wear condition of roller threads and nut threads.</p>
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<p>Temperature trend at the outer circle of the nut.</p>
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<p>Test results of vibration sensor #1.</p>
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<p>Test results of vibration sensor #2.</p>
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<p>Test results of vibration sensor #3.</p>
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<p>Test results of vibration sensor #4.</p>
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<p>Trend of maximum magnitude of vibration sensors.</p>
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<p>Test results of vibration sensor #1.</p>
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<p>Test results of vibration sensor #2.</p>
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<p>Test results of vibration sensor #3.</p>
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<p>Test results of vibration sensor #4.</p>
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<p>Test results of vibration sensor #1.</p>
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<p>Test results of vibration sensor #2.</p>
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<p>Test results of vibration sensor #3.</p>
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<p>Test results of vibration sensor #4.</p>
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16 pages, 2852 KiB  
Article
Indigenous Fire Data Sovereignty: Applying Indigenous Data Sovereignty Principles to Fire Research
by Melinda M. Adams
Fire 2024, 7(7), 222; https://doi.org/10.3390/fire7070222 - 28 Jun 2024
Viewed by 1958
Abstract
Indigenous Peoples have been stewarding lands with fire for ecosystem improvement since time immemorial. These stewardship practices are part and parcel of the ways in which Indigenous Peoples have long recorded and protected knowledge through our cultural transmission practices, such as oral histories. [...] Read more.
Indigenous Peoples have been stewarding lands with fire for ecosystem improvement since time immemorial. These stewardship practices are part and parcel of the ways in which Indigenous Peoples have long recorded and protected knowledge through our cultural transmission practices, such as oral histories. In short, our Peoples have always been data gatherers, and as this article presents, we are also fire data gatherers and stewards. Given the growing interest in fire research with Indigenous communities, there is an opportunity for guidance on data collection conducted equitably and responsibly with Indigenous Peoples. This Special Issue of Fire presents fire research approaches and data harvesting practices with Indigenous communities as we “Reimagine the Future of Living and Working with Fire”. Specifically, the article provides future-thinking practices that can achieve equitable, sustainable, and just outcomes with and for stakeholders and rightholders (the preferred term Indigenous Peoples use in partnerships with academics, agencies, and NGOs). This research takes from the following key documents to propose an “Indigenous fire data sovereignty” (IFDS) framework: (1) Articles declared in the United Nations Declaration on the Rights of Indigenous Peoples (UNDRIP) as identified by the author and specified in Indigenous-led and allied Indigenous fire research in Australia, Canada, and the U.S.; (2) recommendations specific to cultural fire policy and calls for research in the 2023 Wildland Fire Mitigation and Management Commission report; (3) research and data barriers and opportunities produced in the 2024 Good Fire II report; and threads from (4) the Indigenous Fire Management conceptual model. This paper brings together recommendations on Indigenous data sovereignty, which are principles developed by Indigenous researchers for the protection, dissemination, and stewardship of data collected from Tribal/Nation/Aboriginal/First Nations Indigenous communities. The proposed IFDS framework also identifies potential challenges to Indigenous fire data sovereignty. By doing so, the framework serves as an apparatus to deploy fire research and data harvesting practices that are culturally informed, responsible, and ethically demonstrated. The article concludes with specific calls to action for academics and researchers, allies, fire managers, policymakers, and Indigenous Peoples to consider in exercising Indigenous fire data sovereignty and applying Indigenous data sovereignty principles to fire research. Full article
(This article belongs to the Special Issue Reimagining the Future of Living and Working with Fire)
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<p><span class="html-italic">Indigenous fire data sovereignty</span> framework informed by the scholarship of Indigenous fire scholars and allies working in Indigenous-centered or Indigenous-informed cultural burning research in Australia, Canada, and the U.S.; and Indigenous-identified Indigenous data sovereignty scholars adopting IDS FAIR and CARE principles into research, institutional, and governmental partnerships with Indigenous Peoples. The IFDS framework is informed by the following key documents: (1) Articles of the United Nations Declaration on the Rights of Indigenous Peoples (UNDRIP) as identified by the author and specified in Indigenous-led and allied Indigenous fire research in Australia, Canada, and the U.S; (2) recommendations specific to cultural fire policy and calls for research in the 2023 Wildland Fire Mitigation and Management Commission report [<a href="#B33-fire-07-00222" class="html-bibr">33</a>]; (3) research and data barriers and opportunities produced in the 2024 Good fire II report [<a href="#B32-fire-07-00222" class="html-bibr">32</a>]; and threads from (4) the Indigenous Fire Management conceptual model [<a href="#B19-fire-07-00222" class="html-bibr">19</a>].</p>
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20 pages, 9420 KiB  
Article
Assessment of Adhesion in Woven Fabric-Reinforced Laminates (FRLs) Using Novel Yarn Pullout in Laminate Test
by Feyi Adekunle, Ang Li, Rahul Vallabh and Abdel-Fattah M. Seyam
J. Compos. Sci. 2024, 8(7), 242; https://doi.org/10.3390/jcs8070242 - 26 Jun 2024
Viewed by 1006
Abstract
Fiber-reinforced laminates with flexibility (FRLs) are becoming increasingly crucial across diverse sectors due to their adaptability and outstanding mechanical attributes. Their ability to deliver high performance relative to their weight makes them indispensable in lighter-than-air (LTA) applications, such as aerostats, inflatable antennas, surge [...] Read more.
Fiber-reinforced laminates with flexibility (FRLs) are becoming increasingly crucial across diverse sectors due to their adaptability and outstanding mechanical attributes. Their ability to deliver high performance relative to their weight makes them indispensable in lighter-than-air (LTA) applications, such as aerostats, inflatable antennas, surge bladders, gas storage balloons, life rafts, and other related uses. This research delved into employing woven fabrics as the reinforcement material and explored how their specific parameters, like fiber type, fabric count (warp thread density × weft thread density), fabric areal density, and fabric cover influence the bonding and mechanical properties of laminates. A thorough analysis encompassing standard T-peel (ASTM standard D1876) and a newly proposed yarn pullout in laminate test were conducted on laminates fabricated with various woven reinforcements, each with its unique specifications. The T-peel test was utilized to gauge the adhesive strength between FRL components, offering crucial insights into interfacial bonding within the laminates. Nevertheless, challenges exist with the T-peel test, including instances where the adherents lack the strength to withstand rupture, resulting in unsuccessful peel propagation and numerous outliers that necessitate costly additional trials. Thus, our research group introduced a novel yarn pullout in laminate test to accurately assess adhesion in FRLs. This study uncovered correlations between both adhesion tests (T-peel and yarn pullout in laminate), indicating that the innovative yarn pullout in laminate test could effectively substitute for characterizing adhesion in FRLs. Furthermore, the findings unveiled a complex relationship between woven fabric specifications and laminate properties. We noted that variations in fiber type, yarn linear density, and adhesive type significantly impacted adhesion strength. For instance, Kevlar exhibited markedly superior adhesion compared to Ultra-High Molecular Weight Polyethylene (UHMWPE) when paired with Thermoplastic Polyurethane (TPU) adhesive, whereas UHMWPE demonstrated better adhesion with Ethylene Vinyl Acetate (EVA). Moreover, the adhesion quality lessened as fabric count increased for the same adhesive quantity. These discoveries carry practical implications for material selection and design across industries, from automotive to aerospace, offering avenues to enhance FRL performance. Full article
(This article belongs to the Special Issue Discontinuous Fiber Composites, Volume III)
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<p>Laminate structure.</p>
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<p>Bonding high-performance fibers with adhesives: (<b>a</b>) Kevlar and TPU, (<b>b</b>) Kevlar and EVA, and (<b>c</b>) Kevlar and EVOH [<a href="#B9-jcs-08-00242" class="html-bibr">9</a>].</p>
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<p>UHMWPE atomic structure showing strong covalent C-C bonds and weak hydrogen bonds between the molecules [<a href="#B13-jcs-08-00242" class="html-bibr">13</a>].</p>
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<p>Microscopic images (X80) of UHMWPE woven fabrics: (<b>a</b>) UP66 and (<b>b</b>) UP80 showing different tightness levels.</p>
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<p>Test panel and specimen for T-peel test [<a href="#B19-jcs-08-00242" class="html-bibr">19</a>].</p>
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<p>Typical load-displacement curve for T-peel test for FRLs.</p>
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<p>Yarn pullout in laminate sample specifications.</p>
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<p>Typical load-displacement curve for yarn pullout in laminate test.</p>
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<p>Comparison of adhesion using T-peel test in Kevlar and UHMWPE woven fabrics with analogous areal density.</p>
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<p>Correlation between pullout force and peel strength for (<b>a</b>) weft samples and (<b>b</b>) warp samples.</p>
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<p>Comparison of peel and yarn pullout in laminate values.</p>
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<p>Microscopic images of yarn pullout in laminate test: (<b>a</b>) KP60_EVOH before testing in X20 mag, (<b>b</b>) KP60_EVOH before testing in X40 mag, (<b>c</b>) KP60_EVOH after testing in X40 mag, (<b>d</b>) KP60_EVOH after testing in X80 mag, (<b>e</b>) UP66_TPU after testing in X20 mag, and (<b>f</b>) UP66_TPU after testing in X40 mag.</p>
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<p>Pullout force of Kevlar samples in weft and warp directions.</p>
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<p>Microscopic images of yarn after being pulled out of laminate: (<b>a</b>) Kevlar yarn in 40× mag, (<b>b</b>) Kevlar yarn in 100× mag, (<b>c</b>) UHMWPE yarn in 40× mag, and (<b>d</b>) UHMWPE yarn in 100× mag.</p>
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<p>Microscopic images of yarn after being pulled out of laminate: (<b>a</b>) Kevlar yarn in 40× mag, (<b>b</b>) Kevlar yarn in 100× mag, (<b>c</b>) UHMWPE yarn in 40× mag, and (<b>d</b>) UHMWPE yarn in 100× mag.</p>
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<p>Pullout force of UHMWPE samples in weft and warp directions.</p>
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<p>Microscopic image of UP60 showing number of yarns in warp and weft directions.</p>
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<p>Yarn pullout in laminates KP36, KP60, KP140, and KP170, graphs for: (<b>a</b>) EVA, (<b>b</b>) TPU, and (<b>c</b>) EVOH.</p>
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<p>Yarn pullout in laminates KP36, KP60, KP140, and KP170, graphs for: (<b>a</b>) EVA, (<b>b</b>) TPU, and (<b>c</b>) EVOH.</p>
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<p>Box plot of pullout force (N).</p>
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31 pages, 4853 KiB  
Review
Advances in Polyvinyl Alcohol-Based Membranes for Fuel Cells: A Comprehensive Review on Types, Synthesis, Modifications, and Performance Optimization
by Chandra Mouli R. Madhuranthakam, Weam S. K. Abudaqqa and Michael Fowler
Polymers 2024, 16(13), 1775; https://doi.org/10.3390/polym16131775 - 23 Jun 2024
Viewed by 947
Abstract
Fuel cell technology is at the forefront of sustainable energy solutions, and polyvinyl alcohol (PVA) membranes play an important role in improving performance. This article thoroughly investigates the various varieties of PVA membranes, their production processes, and the numerous modification tactics used to [...] Read more.
Fuel cell technology is at the forefront of sustainable energy solutions, and polyvinyl alcohol (PVA) membranes play an important role in improving performance. This article thoroughly investigates the various varieties of PVA membranes, their production processes, and the numerous modification tactics used to solve inherent problems. Various methods were investigated, including chemical changes, composite blending, and the introduction of nanocomposites. The factors impacting PVA membranes, such as proton conductivity, thermal stability, and selectivity, were investigated to provide comprehensive knowledge. By combining various research threads, this review aims to completely investigate the current state of PVA membranes in fuel cell applications, providing significant insights for both academic researchers and industry practitioners interested in efficient and sustainable energy conversion technologies. The transition from traditional materials such as Nafion to PVA membranes has been prompted by limitations associated with the former, such as complex synthesis procedures, reduced ionic conductivity at elevated temperatures, and prohibitively high costs, which have hampered their widespread adoption. As a result, modern research efforts are increasingly focused on the creation of alternative membranes that can compete with conventional technical efficacy and economic viability in the context of fuel cell technologies. Full article
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<p>Two-dimensional diagram of a fuel cell membrane. Redrawn from [<a href="#B26-polymers-16-01775" class="html-bibr">26</a>].</p>
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<p>Chemical Structure of PVA. (<b>a</b>) Fully hydrolyzed PVA structure. (<b>b</b>) Partially hydrolyzed PVA. Redrawn from [<a href="#B44-polymers-16-01775" class="html-bibr">44</a>].</p>
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<p>SEM Micrographs of PVA Membrane: (<b>a</b>) top surface and (<b>b</b>) cross-section. Reproduced with permission from [<a href="#B65-polymers-16-01775" class="html-bibr">65</a>].</p>
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<p>Research Trends in Publications on Polyvinyl Alcohol (PVA)-Based Membranes for Fuel Cells (2014–2024). Extracted from ScienceDirect on 1 June 2024.</p>
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<p>Progression of PEM Technologies. Extracted from [<a href="#B69-polymers-16-01775" class="html-bibr">69</a>,<a href="#B75-polymers-16-01775" class="html-bibr">75</a>].</p>
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<p>Schematic representation of PEM. Redrawn from [<a href="#B79-polymers-16-01775" class="html-bibr">79</a>].</p>
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<p>Solution Casting Method for Synthesizing SPEEK/PVA Blend Membranes with Colloidal Silica Additives. Adopted from [<a href="#B86-polymers-16-01775" class="html-bibr">86</a>].</p>
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<p>Schematic representation of AEMFC. Redrawn from [<a href="#B128-polymers-16-01775" class="html-bibr">128</a>].</p>
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<p>Schematic representation of phase inversion of PVA-based membrane. Redrawn from [<a href="#B143-polymers-16-01775" class="html-bibr">143</a>,<a href="#B144-polymers-16-01775" class="html-bibr">144</a>].</p>
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<p>Illustration of the Electrospinning Process for PVA-based membrane fabrication. Redrawn from [<a href="#B152-polymers-16-01775" class="html-bibr">152</a>].</p>
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<p>Approaches to enhance the performance of PVA membranes in fuel cell technology. Extracted from [<a href="#B157-polymers-16-01775" class="html-bibr">157</a>,<a href="#B176-polymers-16-01775" class="html-bibr">176</a>,<a href="#B188-polymers-16-01775" class="html-bibr">188</a>,<a href="#B189-polymers-16-01775" class="html-bibr">189</a>,<a href="#B190-polymers-16-01775" class="html-bibr">190</a>,<a href="#B191-polymers-16-01775" class="html-bibr">191</a>,<a href="#B192-polymers-16-01775" class="html-bibr">192</a>].</p>
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<p>Cross-linking Methods in Polymers with Carboxyl Groups: Ionic Cross-linking via Metal Ion Complexation and Covalent Cross-linking via Thermal or Photochemical Processes. Reproduced from [<a href="#B193-polymers-16-01775" class="html-bibr">193</a>].</p>
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18 pages, 6156 KiB  
Article
Modern Electromagnetic-Radiation-Shielding Materials Made Using Different Knitting Techniques
by Zbigniew Mikołajczyk, Iwona Nowak, Łukasz Januszkiewicz, Monika Szewczyk and Joanna Junak
Materials 2024, 17(13), 3052; https://doi.org/10.3390/ma17133052 - 21 Jun 2024
Viewed by 630
Abstract
This paper summarizes the possibility of employing knitted textile barriers as a shield against electromagnetic fields to protect the human body from their negative impact. Ten variants of knitted fabrics made of electrically conductive yarns, steel, and copper wire that differed in stitch [...] Read more.
This paper summarizes the possibility of employing knitted textile barriers as a shield against electromagnetic fields to protect the human body from their negative impact. Ten variants of knitted fabrics made of electrically conductive yarns, steel, and copper wire that differed in stitch pattern, structural parameters, and raw material, were designed, manufactured, and tested. The knitted fabrics produced differed in structural parameters, including course and wale density, surface density, thickness, thread length in the loop, wale and course take-up, volume cover factor, and surface porosity. These parameters were examined in accordance with the research methodology used in knitting. Barrier measurements were taken in the direction of the wales and in the direction of the courses for two frequencies of electromagnetic fields: 2–4 GHz and 4–7 GHz. It was observed that the shielding effectiveness of the manufactured materials depends on the structural parameters of the fabric, the stiches applied, and the type of yarn. Full article
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<p>Microscope thread images: (<b>a</b>) Shieldex, 150 dtex; (<b>b</b>) Shieldex, 340 dtex; (<b>c</b>) Amman, 120 dtex; (<b>d</b>) Shieldex, 600 dtex; (<b>e</b>) Cu wire; (<b>f</b>) steel wire, (<b>g</b>) scale for sample yarn.</p>
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<p>Single-bearing cylindrical crochet machine (cylinder diameter = 4″; needle number <span class="html-italic">NE</span> = 14; number of needles, <span class="html-italic">L</span> = 169; number of revolutions, n = 50–200/min). (<b>a</b>) Full view of the machine; (<b>b</b>) view of the cylinder.</p>
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<p>Cylindrical double-bearing crochet machine from Mayer &amp; Cie (cylinder diameter = 30″; gauge pitch = 1.27 mm; needle number, <span class="html-italic">NE</span> = 20; number of needles, <span class="html-italic">L</span> = 2 × 1872).</p>
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<p>The HKS 3 warp-knitting machine from Karl Mayer, with needle number <span class="html-italic">NE</span> = 28.</p>
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<p>(<b>a</b>) Measurement station equipped with a microscope and view system; (<b>b</b>,<b>c</b>) examples of determining the length of yarn in a stitch. (A dozen or so points lying on the yarn axis in the loop were manually marked. The program then automatically connected the dots and approximated them in the form of a curve. After determining the yarn axis, the result of the thread length in the stitch was shown).</p>
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<p>(<b>a</b>) Measuring station for determining experimental porosity; (<b>b</b>) histogram made by the TEXTIL-STUDIO program.</p>
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<p>(<b>a</b>) Actual view of the knitted fabric; (<b>b</b>) binary image of knitted fabric.</p>
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<p>Electric field orientation in waveguides: (<b>a</b>) coaxial; (<b>b</b>) rectangular in fundamental mode.</p>
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<p>Measurement setup.</p>
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<p>(<b>a</b>) The WR284 waveguide; (<b>b</b>) the WR159 waveguide.</p>
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<p>Microscope images of knitted fabrics: (<b>a</b>) knitted fabric 1 (variant 1); (<b>b</b>) knitted fabrics 2 and 3; (<b>c</b>) knitted fabric 4; (<b>d</b>) knitted fabric 5; (<b>e</b>) knitted fabric 6; (<b>f</b>) knitted fabric 7; (<b>g</b>) knitted fabric 8; (<b>h</b>) kitted fabric 9; (<b>i</b>) knitted fabric 10 (magnification 4.4×).</p>
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<p>Attenuation along courses, frequency range 2–4 GHz.</p>
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<p>Attenuation along courses, frequency range 4–7 GHz.</p>
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<p>Attenuation along wales, frequency range 2–4 GHz.</p>
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<p>Attenuation along wales, frequency range 4–7 GHz.</p>
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13 pages, 5877 KiB  
Article
Study of Leakage Current Transport Mechanisms in Pseudo-Vertical GaN-on-Silicon Schottky Diode Grown by Localized Epitaxy
by Mohammed El Amrani, Julien Buckley, Thomas Kaltsounis, David Plaza Arguello, Hala El Rammouz, Daniel Alquier and Matthew Charles
Crystals 2024, 14(6), 553; https://doi.org/10.3390/cryst14060553 - 14 Jun 2024
Viewed by 732
Abstract
In this work, a GaN-on-Si quasi-vertical Schottky diode was demonstrated on a locally grown n-GaN drift layer using Selective Area Growth (SAG). The diode achieved a current density of 2.5 kA/cm2, a specific on-resistance RON,sp of [...] Read more.
In this work, a GaN-on-Si quasi-vertical Schottky diode was demonstrated on a locally grown n-GaN drift layer using Selective Area Growth (SAG). The diode achieved a current density of 2.5 kA/cm2, a specific on-resistance RON,sp of 1.9 mΩ cm2 despite the current crowding effect in quasi-vertical structures, and an on/off current ratio (Ion/Ioff) of 1010. Temperature-dependent current–voltage characteristics were measured in the range of 313–433 K to investigate the mechanisms of leakage conduction in the device. At near-zero bias, thermionic emission (TE) was found to dominate. By increasing up to 10 V, electrons gained enough energy to excite into trap states, leading to the dominance of Frenkel–Poole emission (FPE). For a higher voltage range (−10 V to −40 V), the increased electric field facilitated the hopping of electrons along the continuum threading dislocations in the “bulk” GaN layers, and thus, variable range hopping became the main mechanism for the whole temperature range. This work provides an in-depth insight into the leakage conduction transport on pseudo-vertical GaN-on-Si Schottky barrier diodes (SBDs) grown by localized epitaxy. Full article
(This article belongs to the Special Issue Wide Bandgap Semiconductor: GaN and SiC Material and Device)
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<p>(<b>a</b>) Schematic cross-section of quasi-vertical Schottky diode using localized epitaxy. Inset: optical microscopy of the circular measured devices. (<b>b</b>) Net doping concentration (N<sub>D</sub> − N<sub>A</sub>) in the n-GaN drift layer from the C-V curve at 1MHz. Inset: (A<sup>2</sup>/C<sup>2</sup>) versus the reverse voltage (The red dotted line corresponds to the fit).</p>
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<p>Typical forward J-V curves obtained for GaN pseudo-vertical SBD in (<b>a</b>) semi-log and (<b>b</b>) linear scale, respectively.</p>
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<p>(<b>a</b>) Temperature-dependent forward J-V characteristics on a linear scale (inset: differential specific on-resistance R<sub>on,sp</sub> as a function of temperature T) and (<b>b</b>) in semi-log scale.</p>
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<p>(<b>a</b>) The extracted ideality factor n and Schottky barrier height as a function of temperature for several measured devices, and (<b>b</b>) the experimental Richardson’s plot.</p>
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<p>(<b>a</b>) Typical breakdown characteristic of the fabricated pseudo-vertical GaN and (<b>b</b>) typical temperature-dependent reverse J–V characteristics on the log scale.</p>
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<p>Schematic energy band diagram of thermionic emission in metal–semiconductor structure.</p>
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<p>(<b>a</b>) Typical reverse ln (J) versus V with the fitting model and (<b>b</b>) ln (JTE/T<sup>2</sup>) versus E<sup>½</sup> at the voltage range of 0 to −0.4 V.</p>
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<p>Schematic energy band diagram of FP emission in metal–semiconductor structure.</p>
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<p>Typical ln (J/E) versus <math display="inline"><semantics> <mrow> <msup> <mrow> <mi mathvariant="normal">E</mi> </mrow> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math> fitted with FPE model in range voltage from 0.5 to 10 V.</p>
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<p>(<b>a</b>) The slope of the ln (J/E) versus E<sup>1/2</sup> A (T) as a function of <math display="inline"><semantics> <mrow> <mfrac> <mrow> <mi mathvariant="normal">q</mi> </mrow> <mrow> <mi mathvariant="normal">k</mi> <mi mathvariant="normal">T</mi> </mrow> </mfrac> </mrow> </semantics></math>. (<b>b</b>) The intercept B (T) as a function of 1000/T.</p>
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<p>Schematic energy band diagram of VRH emission in metal–semiconductor structure.</p>
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<p>(<b>a</b>) ln (J) as a function of applied electric field, E. (<b>b</b>) ln (J) versus (1/T)<sup>1/2</sup> at reverse voltages of −10, −20, −30 and −40 V.</p>
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<p>d[log(ln(J))]/dlog(E) of GaN on Si SBD as function of applied voltage [<a href="#B25-crystals-14-00553" class="html-bibr">25</a>].</p>
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<p>Schematic depicting determined leakage processes under reverse bias for GaN-on-Si SBD grown by localized epitaxy [<a href="#B28-crystals-14-00553" class="html-bibr">28</a>,<a href="#B33-crystals-14-00553" class="html-bibr">33</a>].</p>
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15 pages, 533 KiB  
Article
Girls’ Reluctance and Intersectional Identities in STEM-Rich Makerspaces
by Priyanka Parekh
Educ. Sci. 2024, 14(6), 628; https://doi.org/10.3390/educsci14060628 - 11 Jun 2024
Viewed by 749
Abstract
Craft and e-textile circuits are technologies that bridge the gender gap in Science, Technology, Engineering, and Mathematics (STEM) learning. Acknowledging the need to study girls’ underrepresentation in STEM, this article delves into the identity negotiations of four girls aged eleven to fourteen as [...] Read more.
Craft and e-textile circuits are technologies that bridge the gender gap in Science, Technology, Engineering, and Mathematics (STEM) learning. Acknowledging the need to study girls’ underrepresentation in STEM, this article delves into the identity negotiations of four girls aged eleven to fourteen as they construct craft and e-textiles at a library makerspace. Qualitative analysis of their talk at the workshop found that several factors shaped the girls’ identity work, such as their awareness of their abilities and fellow participants’ projects, their understanding of parents’ expectations, and their strengths in other STEM domains. While all four girls reluctantly participated in making circuits, the reason for their reluctance varied from an interest in craft and the messiness of working with conductive thread to the preference for familiarity and complexity within other STEM domains such as programming and engineering. Further, as the girls questioned their need to engage in circuit-making, their preference for a particular identity became apparent. Overall, this study’s findings underscore the tensions in learning in technology-rich environments such as makerspaces, highlighting maker technologies’ affordances and limitations and emphasizing the need for a deeper understanding of what shapes learners’ participation and identities. Full article
(This article belongs to the Section Technology Enhanced Education)
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<p>An illustration of maker identities as a function of structures informing STEM learning and learners’ agentic identity work in recognition of the structure.</p>
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17 pages, 10503 KiB  
Article
Wearable Loops for Dynamic Monitoring of Joint Flexion: A Machine Learning Approach
by Henry Saltzman, Rahul Rajaram, Yingzhe Zhang, Md Asiful Islam and Asimina Kiourti
Electronics 2024, 13(12), 2245; https://doi.org/10.3390/electronics13122245 - 7 Jun 2024
Cited by 1 | Viewed by 519
Abstract
We present a machine learning driven system to monitor joint flexion angles during dynamic motion, using a wearable loop-based sensor. Our approach uses wearable loops to collect transmission coefficient data and an Artificial Neural Network (ANN) with fine-tuned parameters to increase accuracy of [...] Read more.
We present a machine learning driven system to monitor joint flexion angles during dynamic motion, using a wearable loop-based sensor. Our approach uses wearable loops to collect transmission coefficient data and an Artificial Neural Network (ANN) with fine-tuned parameters to increase accuracy of the measured angles. We train and validate the ANN for sagittal plane flexion of a leg phantom emulating slow motion, walking, brisk walking, and jogging. We fabricate the loops on conductive threads and evaluate the effect of fabric drift via measurements in the absence and presence of fabric. In the absence of fabric, our model produced a root mean square error (RMSE) of 5.90°, 6.11°, 5.90°, and 5.44° during slow motion, walking, brisk walking, and jogging. The presence of fabric degraded the RMSE to 8.97°, 7.21°, 9.41°, and 7.79°, respectively. Without the proposed ANN method, errors exceeded 35.07° for all scenarios. Proof-of-concept results on three human subjects further validate this performance. Our approach empowers feasibility of wearable loop sensors for motion capture in dynamic, real-world environments. Increasing speed of motion and the presence of fabric degrade sensor performance due to added noise. Nevertheless, the proposed framework is generalizable and can be expanded upon in the future to improve upon the reported angular resolution. Full article
(This article belongs to the Special Issue Wearable Electronics for Noninvasive Sensing)
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<p>Joint flexion sensor with two planar loops.</p>
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<p>High level flowchart of experiments, data collection, data preprocessing, and machine learning reported in the paper.</p>
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<p>Flowchart describing the machine learning block in <a href="#electronics-13-02245-f002" class="html-fig">Figure 2</a> higher dimensionality, and it is well known that ANNs are best suited for high-dimensional data.</p>
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<p>Phantoms with two planar loops (one above and one below the joint) employed in this study: (<b>a</b>) sleeveless and (<b>b</b>) sleeved.</p>
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<p>Flowchart describing the data preprocessing block in <a href="#electronics-13-02245-f002" class="html-fig">Figure 2</a> noise.</p>
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<p>Graphs of |S<sub>21</sub>| vs time, (camera-measured) angle vs time, sleeveless trials (<b>a</b>), sleeved trials (<b>b</b>), and (camera-measured) angle vs. |S<sub>21</sub>| for all trials (<b>c</b>).</p>
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<p>Diagram of ANN structure: input, output and feed forward layers.</p>
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<p>Predicted (blue) vs. actual (red) angles as a function of time for all speeds: (<b>a</b>) sleeveless sensor and (<b>b</b>) sleeved sensor.</p>
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18 pages, 10650 KiB  
Article
Textronic Capacitive Sensor with an RFID Interface
by Patryk Pyt, Kacper Skrobacz, Piotr Jankowski-Mihułowicz and Mariusz Węglarski
Sensors 2024, 24(12), 3706; https://doi.org/10.3390/s24123706 - 7 Jun 2024
Viewed by 654
Abstract
This article presents an innovative combination of textile electrical circuits with advanced capabilities of electronic RFID sensors, indicating the revolutionary nature of the development of textronics, which is used in various areas of life, from fashion to medicine. A review of the literature [...] Read more.
This article presents an innovative combination of textile electrical circuits with advanced capabilities of electronic RFID sensors, indicating the revolutionary nature of the development of textronics, which is used in various areas of life, from fashion to medicine. A review of the literature relating to the construction of textronic RFID identifiers and capacitive textronic sensors is performed. Various approaches to measuring capacity using RFID tags are discussed. This article focuses on presenting the concept of a capacitive sensor with an RFID interface, consisting of a microelectronic part and a textile part. The textile part is based on the WL4007 material, where antennas and capacitive sensors are embroidered using SPARKFUN DEV 11791 conductive thread. The antenna is a half-wave dipole designed to operate at a frequency of 860 MHZ. The microelectronic part is sewn to the textile part and consists of a microcontroller, an RFID-integrated circuit and a coupling loop, placed on the PCB. The embroidered antenna is coupled with a loop on the microelectronic module. This article focuses on presenting various designs of textronic electrodes, enabling various types of measurements. Article presents capacitance measurements of individual sensor electrodes, made using a measuring bridge and a built RFID tag. The sensors’ capacity measurement results are shown. Full article
(This article belongs to the Special Issue Sensors and Sensing Technology: RFID Devices)
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<p>Demonstrator of a textile capacitive sensor with an RFID interface: (<b>a</b>) symbolic representation of the individual components of the demonstrator; (<b>b</b>) photo of the completed demonstrator.</p>
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<p>Block diagram of a textronic capacitive sensor with an RFID interface.</p>
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<p>Diagram of the electrical connection of capacitive sensors with the channels of the TSD and the method of connecting sampling capacitors.</p>
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<p>Design of a textronic antenna, which is a half-wave dipole operating in the UHF frequency range.</p>
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<p>Textronic capacitive sensor in the shape of circles.</p>
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<p>Textronic capacitive sensor in the shape of a slider, enabling the detection of linear movement of objects.</p>
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<p>Textronic capacitive sensor in the shape of ring fragments arranged around a common axis. The sensor enables the detection of the rotational movement of an object.</p>
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<p>Ground electrode, placed under the measuring electrodes.</p>
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<p>Cross-section of an embroidered capacitive sensor.</p>
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<p>Operating algorithm of the demonstration program of a capacitive textile sensor with an RFID interface.</p>
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<p>A measuring system used to determine the capacity of a capacitive sensor, depending on the distance of the object located in front of the sensor. The red and green lines symbolize the measurement probes, attached to the mass electrode and the measuring electrode of the textronic sensor, respectively.</p>
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<p>Photo of the measuring system used to measure the capacity of the sensor depending on the distance of the object.</p>
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<p>A plot showing the results of capacitance measurements of a button-shaped electrode sensor for various object distances.</p>
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<p>A plot showing the hysteresis of a button-shaped capacitive sensor, reflecting the difference in the sensor’s capacitance as the object approaches and moves away.</p>
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<p>A plot showing the results of capacitance measurements of a sensor with a slider-shaped electrode for various object distances.</p>
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<p>A plot showing the hysteresis of a slide-shaped capacitive sensor, reflecting the difference in the sensor’s capacitance as the object approaches and moves away.</p>
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<p>A plot showing the results of capacitance measurements of a sensor with an electrode in the shape of a rotary sensor for various object distances.</p>
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<p>A plot showing the hysteresis of a rotary-shaped capacitive sensor, reflecting the difference in the sensor’s capacitance as the object approaches and moves away.</p>
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<p>ISOStart program window showing the reading of the serial number of the sensor identifier via the RFID interface.</p>
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19 pages, 4686 KiB  
Article
Experimental Behaviour of Tensioner for Rigid Hangers of Arch Bridges
by Michele Fabio Granata, Benedetta Fontana, Marco Rosone and Giovanni Culotta
Designs 2024, 8(3), 55; https://doi.org/10.3390/designs8030055 - 5 Jun 2024
Viewed by 787
Abstract
In steel tied arch bridges where the hangers are made of rigid bars, the replacement of damaged hangers is rather complex. In fact, while generally the cable hangers are already prepared with anchors at the ends and their replacement traces the initial stages [...] Read more.
In steel tied arch bridges where the hangers are made of rigid bars, the replacement of damaged hangers is rather complex. In fact, while generally the cable hangers are already prepared with anchors at the ends and their replacement traces the initial stages of construction with their prestressing, on the contrary, the rigid bars are welded to the arch and the deck, so their replacement must include the design of a new suspension system that allows the insertion of a pretension where this had never been considered. To check the reliability of this new system, a prototype of tensioner was studied for the case of a steel arch bridge in which the high level of corrosion made it necessary to replace all the original hangers with new ones. This entailed the need to test the tensioner performance with the aim of ensuring the axial force transmission between the two hanger segments without slippage in the threads, as well as to test the correct tension setting before construction and putting into service the hangers to be replaced. For this reason, a predictive experimental campaign was carried out on a prototype by means of tests for the mechanical characterization of the materials used, tensile tests of the system, and tensioning tests under load, measuring the displacements and strains of the system elements. The results of the tests, with slippage in the threads limited to the 2% of total elongation, and the turnaround-stressing curves were useful for the definition of the pieces to be assembled during on-site work and for addressing the operating procedures of the tensioning phases on-site during hanger replacement. Validation with the on-site monitoring of stressing operation was conducted at the end; the monitoring of tension through dynamic tests confirmed the agreement of on-site results with the predictive loading tests of the experimental campaign on the tensioner prototype. Full article
(This article belongs to the Topic Resilient Civil Infrastructure)
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<p>The case study bridge. (<b>a</b>) Original configuration; (<b>b</b>) original hanger with welded connections at the end; (<b>c</b>) new suspension system; (<b>d</b>) new hanger with end connections and intermediate tensioner.</p>
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<p>Replacement sequence. (<b>a</b>) Original configuration; (<b>b</b>) hanger cutting and stress release (<span class="html-italic">N<sub>0,i</sub></span>); (<b>c</b>) new hanger and imposed distortion Δ<span class="html-italic"><sub>i</sub></span> through tensioner.</p>
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<p>FE model of the bridge. (<b>a</b>) Entire model; (<b>b</b>) stress variation in the hangers for a generic stage of replacement; (<b>c</b>) axial force diagram in the new hanger and in the adjacent ones after the application of distortion Δ<span class="html-italic"><sub>i</sub></span> through the tensioner.</p>
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<p>Geometry of the tensioner prototype. (<b>a</b>) Lateral view and longitudinal cross-section (Measures in mm). (<b>b</b>) 3D view. (<b>c</b>) Real picture of the tensioner prototype.</p>
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<p>View of the whole hanger with the top (at the left side) and bottom (at the right side) connections with the central tensioner.</p>
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<p>Tensile tests on hanger bars. Stress–strain diagrams. (Colours are adopted for the three different samples).</p>
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<p>Test-setup. (<b>a</b>) Schematic layout (T<span class="html-italic"><sub>i</sub></span> transducers, SG<span class="html-italic"><sub>i</sub></span> strain gauges); (<b>b</b>) picture of the piece on the machine.</p>
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<p>Tensile test results. (<b>a</b>) Load–displacement graphs of transducers; (<b>b</b>) load–strain graphs of strain gauges.</p>
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<p>Tensile test results. Load–slip diagrams at the top and bottom threads.</p>
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<p>Tensioning tests. (<b>a</b>) Graduated area on the tensioner; (<b>b</b>) first test with rotation obtained by a universal wrench; (<b>c</b>) tensioning test carried out through a rigid specially manufactured wrench.</p>
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<p>Tensioning test results. Load–strain graphs of the four tests. The corresponding rotation of the tensioner is reported in the additional right vertical axis.</p>
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<p>Replacement of hangers. (<b>a</b>) Cutting of old hangers; (<b>b</b>) and (<b>c</b>) tensioning phases on-site of new hangers.</p>
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<p>Monitoring of stressing stages. (<b>a</b>) Strain; (<b>b</b>) axial force.</p>
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<p>Dynamic tests for validation of stressing operations.</p>
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27 pages, 9472 KiB  
Article
A GPU-Based Integration Method from Raster Data to a Hexagonal Discrete Global Grid
by Senyuan Zheng, Liangchen Zhou, Chengshuai Lu and Guonian Lv
Remote Sens. 2024, 16(11), 2022; https://doi.org/10.3390/rs16112022 - 4 Jun 2024
Viewed by 575
Abstract
This paper proposes an algorithm for the conversion of raster data to hexagonal DGGSs in the GPU by redevising the encoding and decoding mechanisms. The researchers first designed a data structure based on rhombic tiles to convert the hexagonal DGGS to a texture [...] Read more.
This paper proposes an algorithm for the conversion of raster data to hexagonal DGGSs in the GPU by redevising the encoding and decoding mechanisms. The researchers first designed a data structure based on rhombic tiles to convert the hexagonal DGGS to a texture format acceptable for GPUs, thus avoiding the irregularity of the hexagonal DGGS. Then, the encoding and decoding methods of the tile data based on space-filling curves were designed, respectively, so as to reduce the amount of data transmission from the CPU to the GPU. Finally, the researchers improved the algorithmic efficiency through thread design. To validate the above design, raster integration experiments were conducted based on the global Aster 30 m digital elevation dataDEM, and the experimental results showed that the raster integration accuracy of this algorithms was around 1 m, while its efficiency could be improved to more than 600 times that of the algorithm for integrating the raster data to the hexagonal DGGS data, executed in the CPU. Therefore, the researchers believe that this study will provide a feasible method for the efficient and stable integration of massive raster data based on a hexagonal grid, which may well support the organization of massive raster data in the field of GIS. Full article
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<p>Differences in architecture between the CPU and the GPU. (The light blue rectangles represent the Control Unit, the dark blue rectangles represent the Arithmetic Logic Unit (AU), the red rectangles represent the Cache Memory, and the brown-yellow rectangles represent the Dynamic Random-Access Memory (DRAM)).</p>
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<p>Pipeline scheduling.</p>
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<p>Arrangement of hexagonal cells.</p>
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<p>Organization of hexagonal cells based on rhombic tiles. (The blue hexagonal cells are the cells attributed to this basic rhombic surface, and the gray hexagonal cells are the cells that do not belong to the current basic rhombic surface).</p>
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<p>Rhombic tile encoding structure.</p>
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<p>Encoding process for hexagonal cells.</p>
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<p>Decoding process for hexagonal cells.</p>
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<p>Raster data scheduling strategy.</p>
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<p>Spatial relationship between raster data and rhombic tile data.</p>
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<p>Raster data scheduling strategy: (<b>a</b>) Schematic diagram of the first raster data scheduling; (<b>b</b>) Update strategy for raster data.</p>
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<p>Principle of bilinear interpolation of raster data: (<b>a</b>) Principle of bilinear interpolation; (<b>b</b>) Finding the nearest raster point from the center of a hexagonal cell; (<b>c</b>) Interpolate the center of the hexagonal cell based on the coordinates of the four nearest raster center points.</p>
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<p>Grid–stride loops. (Dark blue rectangles represent Grids in threads. light blue and white rectangles represent Blocks in a Grid. orange rectangles represent data blocks).</p>
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<p>Thread buffer design.</p>
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<p>Experiment to determine the threshold of tile splitting.</p>
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<p>Comparison of efficiency of space-filling curves (times).</p>
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<p>Efficiency comparison for each thread combination block.</p>
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<p>CPU decoding efficiency vs. GPU decoding efficiency.</p>
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<p>Time consumed by each part of the algorithmic flow.</p>
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<p>Overall efficiency comparison.</p>
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<p>Comparison of bandwidth consumption.</p>
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<p>Comparison of efficiency with and without the use of encoding and decoding mechanisms.</p>
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<p>Various types of hexagonal cells on the surface of an icosahedron. (The black line represents the <span class="html-italic">q</span>2<span class="html-italic">d</span><span class="html-italic">i</span> coordinate system, the gray line represents rhombic cells, the green line represents triangular cells, the blue line represents hexagonal cells, and the red dashed line represents the projection of the center point of the cell into the <span class="html-italic">q</span>2<span class="html-italic">d</span><span class="html-italic">i</span> coordinate system).</p>
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<p>The algorithm for encoding.</p>
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<p>Decoding algorithm for rhombic tile data.</p>
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15 pages, 8811 KiB  
Article
Assessment of the Influence of Fabric Structure on Their Electro-Conductive Properties
by Magdalena Tokarska, Ayalew Gebremariam and Adam K. Puszkarz
Materials 2024, 17(11), 2692; https://doi.org/10.3390/ma17112692 - 2 Jun 2024
Viewed by 704
Abstract
Electro-conductive fabrics are key materials for designing and developing wearable smart textiles. The properties of textile materials depend on the production method, the technique which leads to high conductivity, and the structure. The aim of the research work was to determine the factors [...] Read more.
Electro-conductive fabrics are key materials for designing and developing wearable smart textiles. The properties of textile materials depend on the production method, the technique which leads to high conductivity, and the structure. The aim of the research work was to determine the factors affecting the electrical conductivity of woven fabrics and elucidate the mechanism of electric current conduction through this complex, aperiodic textile material. The chemical composition of the material surface was identified using scanning electron microscopy energy dispersion X-ray spectroscopy. The van der Pauw method was employed for multidirectional resistance measurements. The coefficient was determined for the assessment of the electrical anisotropy of woven fabrics. X-ray micro-computed tomography was used for 3D woven structure geometry analysis. The anisotropy coefficient enabled the classification of electro-conductive fabrics in terms of isotropic or anisotropic materials. It was found that the increase in weft density results in an increase in sample anisotropy. The rise in thread width can lead to smaller electrical in-plane anisotropy. The threads are unevenly distributed in woven fabric, and their widths are not constant, which is reflected in the anisotropy coefficient values depending on the electrode arrangement. The smaller the fabric area covered by four electrodes, the fewer factors leading to structure aperiodicity. Full article
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Figure 1

Figure 1
<p>Optical images of tested woven fabrics: (<b>a</b>) side A of sample L525; (<b>b</b>) side B of sample L525; (<b>c</b>) side A of sample M1; (<b>d</b>) side B of sample M1; (<b>e</b>) side A of sample M6; (<b>f</b>) side B of sample M6; (<b>g</b>) side A of sample M9; (<b>h</b>) side B of sample M9; (<b>i</b>) side A of sample M10; (<b>j</b>) side B of sample M10; (<b>k</b>) side A of sample M11; (<b>l</b>) side B of sample M11; (<b>m</b>) side A of sample M12; (<b>n</b>) side B of sample M12; (<b>o</b>) side A of sample U1; (<b>p</b>) side B of sample U1.</p>
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<p>Micro-CT cross-sections of tested fabrics.</p>
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<p>Van der Pauw configuration of electrodes on the circular sample for the direction defined by angle θ in the sample plane: (<b>a</b>) θ = 0°; (<b>b</b>) θ = 45°; (<b>c</b>) θ = 90°; (<b>d</b>) θ = 135°.</p>
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<p>Arrangement of electrodes on sample plane: (<b>a</b>) L; (<b>b</b>) M; (<b>c</b>) S.</p>
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<p>Curves representing electrical isotropy and anisotropy of fabric.</p>
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<p>Isotropy and anisotropy curves for samples (<b>a</b>) L525; (<b>b</b>) M1.</p>
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<p>Isotropy and anisotropy curves for samples (<b>a</b>) M6; (<b>b</b>) M9.</p>
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<p>Isotropy and anisotropy curves for samples (<b>a</b>) M10; (<b>b</b>) M11.</p>
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<p>Isotropy and anisotropy curves for samples (<b>a</b>) M12; (<b>b</b>) U1.</p>
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