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Search Results (2,258)

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17 pages, 20814 KiB  
Article
Vision-Based Gesture-Driven Drone Control in a Metaverse-Inspired 3D Simulation Environment
by Yaseen, Oh-Jin Kwon, Jaeho Kim, Jinhee Lee and Faiz Ullah
Drones 2025, 9(2), 92; https://doi.org/10.3390/drones9020092 - 24 Jan 2025
Viewed by 535
Abstract
Unlike traditional remote control systems for controlling unmanned aerial vehicles (UAVs) and drones, active research is being carried out in the domain of vision-based hand gesture recognition systems for drone control. However, contrary to static and sensor based hand gesture recognition, recognizing dynamic [...] Read more.
Unlike traditional remote control systems for controlling unmanned aerial vehicles (UAVs) and drones, active research is being carried out in the domain of vision-based hand gesture recognition systems for drone control. However, contrary to static and sensor based hand gesture recognition, recognizing dynamic hand gestures is challenging due to the complex nature of multi-dimensional hand gesture data, present in 2D images. In a real-time application scenario, performance and safety is crucial. Therefore we propose a hybrid lightweight dynamic hand gesture recognition system and a 3D simulator based drone control environment for live simulation. We used transfer learning-based computer vision techniques to detect dynamic hand gestures in real-time. The gestures are recognized, based on which predetermine commands are selected and sent to a drone simulation environment that operates on a different computer via socket connectivity. Without conventional input devices, hand gesture detection integrated with the virtual environment offers a user-friendly and immersive way to control drone motions, improving user interaction. Through a variety of test situations, the efficacy of this technique is illustrated, highlighting its potential uses in remote-control systems, gaming, and training. The system is tested and evaluated in real-time, outperforming state-of-the-art methods. The code utilized in this study are publicly accessible. Further details can be found in the “Data Availability Statement”. Full article
(This article belongs to the Special Issue Mobile Fog and Edge Computing in Drone Swarms)
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Figure 1
<p>Gesture-Based UAVs Control: Demonstrating Human Gesture Recognition for Drone Navigation in a Simulated Environment via Sockets.</p>
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<p>RGB-camera takes hand gestures as input from the frames.</p>
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<p>Static vs dynamic hand gestures.</p>
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<p>The architecture of the V-HGR model.</p>
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<p>Shows drones in a 3D environment, being controlled by commands received from the client side. (<b>a</b>) shows a single drone ready to take off. (<b>b</b>) shows the drone takeoff after a command was received. (<b>c</b>) shows swarm of drones waiting for command. (<b>d</b>) shows a scenario where a series of commands were received and executed; 1. drone selection, followed by 2. Two (to select half of the drones) and then followed by 3. Takeoff (selected drones took off).</p>
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<p>Communication between V-HGR and the 3D simulator module via sockets.</p>
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<p>Dataset’s class distribution. Class labels are shown on the x-axis, while number of images in each category are shown on the y-axis.</p>
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<p>Confusion matrix for vision-based dynamic gesture recognition trained model based on the test data.</p>
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17 pages, 3587 KiB  
Article
Detection of Dopamine Using Hybrid Materials Based on NiO/ZnO for Electrochemical Sensor Applications
by Irum Naz, Aneela Tahira, Arfana Begum Mallah, Elmuez Dawi, Lama Saleem, Rafat M. Ibrahim and Zafar Hussain Ibupoto
Catalysts 2025, 15(2), 116; https://doi.org/10.3390/catal15020116 - 24 Jan 2025
Viewed by 322
Abstract
Dopamine is a neurotransmitter which is classified as a catecholamine. It is also one of the main metabolites produced by some tumor types (such as paragangliomas and neoblastomas). As such, determining and monitoring the level of dopamine is of the utmost importance, ideally [...] Read more.
Dopamine is a neurotransmitter which is classified as a catecholamine. It is also one of the main metabolites produced by some tumor types (such as paragangliomas and neoblastomas). As such, determining and monitoring the level of dopamine is of the utmost importance, ideally using analytical techniques that are sensitive, simple, and low in cost. Due to this, we have developed a non-enzymatic dopamine sensor that is highly sensitive, selective, and rapidly detects the presence of dopamine in the body. A hybrid material fabricated with NiO and ZnO, based on date fruit extract, was synthesized by hydrothermal methods and using NiO as a precursor material. This paper discusses the role of date fruit extracts in improving NiO’s catalytic performance with reference to ZnO and the role that they play in this process. An X-ray powder diffraction study, a scanning electron microscope study, and a Fourier transform infrared spectroscopy study were performed in order to investigate the structure of the samples. It was found that, in the composite NiO/ZnO, NiO exhibited a cubic phase and ZnO exhibited a hexagonal phase, both of which exhibited well-oriented aggregated cluster shapes in the composite. A hybrid material containing NiO and ZnO has been found to be highly electro-catalytically active in the advanced oxidation of dopamine in a phosphate buffer solution at a pH of 7.3. It has been found that this can be accomplished without the use of enzymes, and the range of oxidation used here was between 0.01 mM and 4 mM. The detection limit of non-enzymatic sensors is estimated to be 0.036 μM. Several properties of the non-enzymatic sensor presented here have been demonstrated, including its repeatability, selectivity, and reproducibility. A test was conducted on Sample 2 for the detection of banana peel and wheat grass, and the results were highly encouraging and indicated that biomass waste may be useful for the manufacture of medicines to treat chronic diseases. It is thought that date fruit extracts would prove to be valuable resources for the development of next-generation electrode materials for use in clinical settings, for energy conversion, and for energy storage. Full article
(This article belongs to the Section Electrocatalysis)
24 pages, 2460 KiB  
Article
An Unequal Clustering and Multi-Hop Routing Protocol Based on Fuzzy Logic and Q-Learning in WSNs
by Zhen Wang and Jin Duan
Entropy 2025, 27(2), 118; https://doi.org/10.3390/e27020118 - 24 Jan 2025
Viewed by 263
Abstract
Clustering-based routing techniques are key to significantly extending the lifetime of wireless sensor networks (WSNs). However, these approaches often do not address the common hotspot issue in multi-hop WSNs. To overcome this challenge and enhance network lifespan, this study presents FQ-UCR, a hybrid [...] Read more.
Clustering-based routing techniques are key to significantly extending the lifetime of wireless sensor networks (WSNs). However, these approaches often do not address the common hotspot issue in multi-hop WSNs. To overcome this challenge and enhance network lifespan, this study presents FQ-UCR, a hybrid approach that merges unequal clustering based on fuzzy logic (FL) with routing optimized through Q-learning. In FQ-UCR, a tentative CH employs a fuzzy inference system (FIS) to compute its probability of being selected as the final CH. By using the Q-learning algorithm, the best forwarding cluster head (CH) is chosen to construct the data transmission route between the CHs and the base station (BS). The approach is extensively evaluated and compared with protocols like EEUC and CHEF. Simulation results demonstrate that FQ-UCR improves energy efficiency across all nodes, significantly extends network lifetime, and effectively alleviates the hotspot issue. Full article
(This article belongs to the Special Issue Wireless Communications: Signal Processing Perspectives)
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<p>The network model employed in this study.</p>
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<p>Radio model.</p>
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<p>Flow chart of proposed FQ-UCR protocol.</p>
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<p>Block diagram of FIS.</p>
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<p>FIS developed for selecting CHs in FQ-UCR.</p>
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<p>Membership function for residual energy.</p>
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<p>Membership function for distance to base.</p>
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<p>Membership function for number of neighbors.</p>
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<p>Membership function for node centrality.</p>
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<p>Membership function for output variables for CH selection (probability).</p>
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<p>Membership function for output variables for radius.</p>
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<p>Block diagram of Q-learning.</p>
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<p>(<b>a</b>) Node distribution for Scenario 1. (<b>b</b>) Node distribution for Scenario 2.</p>
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<p>The figure compares the residual energy (in Joules) of 100 nodes, with the BS located at (100, 100), across different protocols.</p>
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<p>The figure compares the residual energy (in Joules) of 200 nodes, with the BS located at (100, 100), across different protocols.</p>
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<p>The figure compares the residual energy (in Joules) of 400 nodes, with the BS located at (100, 100), across different protocols.</p>
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<p>Network lifetime comparison for 100 nodes in Scenario 1.</p>
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<p>Network lifetime comparison for 200 nodes in Scenario 1.</p>
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<p>Network lifetime comparison for 400 nodes in Scenario 1.</p>
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<p>Comparative analysis based on network stability period with BS located at (100, 250).</p>
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<p>Comparative analysis based on throughput in Scenario 1.</p>
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<p>The figure compares the residual energy (in Joules) of 100 nodes, with the BS located at (100, 250), across different protocols.</p>
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<p>The figure compares the residual energy (in Joules) of 200 nodes, with the BS located at (100, 250), across different protocols.</p>
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<p>The figure compares the residual energy (in Joules) of 400 nodes, with the BS located at (100, 250), across different protocols.</p>
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<p>Network lifetime comparison for 100 nodes in Scenario 2.</p>
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<p>Network lifetime comparison for 200 nodes in Scenario 2.</p>
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<p>Network lifetime comparison for 400 nodes in Scenario 2.</p>
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<p>Comparative analysis based on network stability period with BS located at (100, 250).</p>
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<p>Comparative analysis based on throughput in Scenario 2.</p>
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11 pages, 4940 KiB  
Article
Terahertz CMOS High-Sensitivity Sensor Based on Hybridized Spoof Surface Plasmon Resonator
by Ming Wan, Chenchen Li, Di Bao, Jiangpeng Wang, Kai Lu, Zhenyu Qu and Hao Gao
Photonics 2025, 12(2), 102; https://doi.org/10.3390/photonics12020102 - 23 Jan 2025
Viewed by 329
Abstract
In recent years, spoof localized surface plasmon (SLSP) have gained increasing attention due to their strong electromagnetic wave confinements. Based on the multipole resonance of SLSP, a high-Q-factor terahertz resonator based on CMOS technology is proposed. Specifically, a quadrilateral hybridized SLSP structure, composed [...] Read more.
In recent years, spoof localized surface plasmon (SLSP) have gained increasing attention due to their strong electromagnetic wave confinements. Based on the multipole resonance of SLSP, a high-Q-factor terahertz resonator based on CMOS technology is proposed. Specifically, a quadrilateral hybridized SLSP structure, composed of a core and a cavity SLSP resonator, is designed to reduce electric dimension and improve the Q-factor. The experimentally measured Q-factor reached 56.7 at 194 GHz, which is quite a high value within the terahertz frequency band, particularly given the compact electrical dimension of 0.081λ × 0.081λ. Moreover, pharmaceutical testing in the terahertz frequency range was successfully conducted, including glucose and two traditional Chinese medicines: Chuanbei and Sanqi. And three frequency shifts (4 GHz, 3.2 GHz, and 1.4 GHz) were observed. Thus, the SLSP resonator holds great potential for high-performance terahertz applications. Full article
(This article belongs to the Special Issue New Trends in Terahertz Photonics)
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Figure 1
<p>Schematic of the cavity SLSP resonator, in which D = 126 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>l</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> = 40 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>l</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math> = 34 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>l</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> </semantics></math> = 30 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>l</mi> </mrow> <mrow> <mn>4</mn> </mrow> </msub> </mrow> </semantics></math> = 23 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>l</mi> </mrow> <mrow> <mn>5</mn> </mrow> </msub> </mrow> </semantics></math> = 12 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="normal">g</mi> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">p</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> = 8 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, and L = 150 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>.</p>
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<p>Cross section of the CMOS technology.</p>
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<p>(<b>a</b>) The simulated reflection coefficient. (<b>b</b>,<b>c</b>) The <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>E</mi> </mrow> <mrow> <mi>z</mi> </mrow> </msub> </mrow> </semantics></math>−field distributions of the cavity SLSP structure.</p>
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<p>Schematic of the hybridized LSP resonator structure.</p>
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<p>(<b>a</b>) The simulation results comparison of the hybridized SLSP resonator and the cavity resonator. (<b>b</b>,<b>c</b>) The electric field distributions of modes M1 and M2.</p>
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<p>Surface current distributions of modes (<b>a</b>) m1, (<b>b</b>) m2, (<b>c</b>) M1, and (<b>d</b>) M2.</p>
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<p>(<b>a</b>) The proposed SLSP resonator under dielectric film for sensing simulation, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="normal">D</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> = 146 <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>. (<b>b</b>,<b>c</b>) S parameter obtained from changing t and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math>. (<b>d</b>) Simulation sensing performance without pass layers.</p>
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<p>Process flow of CMOS technology.</p>
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<p>(<b>a</b>) The microscopic image of the proposed SLSP. (<b>b</b>) Comparison of measured and simulated S parameter.</p>
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<p>(<b>a</b>) The microscopic image of fabricated sample during sensing experiment. (<b>b</b>) The measured results for the sensing experiment.</p>
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36 pages, 6105 KiB  
Review
An Overview of Potential Applications of Environmentally Friendly Hybrid Polymeric Materials
by Raluca Nicoleta Darie-Niță and Stanisław Frąckowiak
Polymers 2025, 17(2), 252; https://doi.org/10.3390/polym17020252 - 20 Jan 2025
Viewed by 795
Abstract
The applications of polymeric materials are being constantly reviewed and improved. In the present world, the word hybrid, and the general idea of combining two or more inherently different approaches, designs, and materials is gaining significant attention. The area of sustainable materials with [...] Read more.
The applications of polymeric materials are being constantly reviewed and improved. In the present world, the word hybrid, and the general idea of combining two or more inherently different approaches, designs, and materials is gaining significant attention. The area of sustainable materials with a low environmental impact is also rapidly evolving with many new discoveries, including the use of materials of a natural origin and countless combinations thereof. This review tries to summarize the current state of knowledge about hybrid polymeric materials and their applications with special attention to the materials that can be considered “environmentally friendly”. As the current application field is quite broad, the review was limited to the following topics: packaging, medical applications, sensors, water purification, and electromagnetic shielding. Furthermore, this review points out the new prospects and challenges for the use of the mentioned materials in terms of creating novel solutions with different nano and micro-materials of mostly natural and renewable origin. Full article
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<p>General classifications of hybrid materials, considering: the differences between the interactions of the components, class I and class II hybrid materials (<b>left</b>); the nature of the matrix and filler component, classified: I–O, O–I, I–I, and O–O types (<b>right</b>) [<a href="#B6-polymers-17-00252" class="html-bibr">6</a>]. Reprinted under Creative Common License CC-BY 4.0 of American Chemical Society.</p>
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<p>Fabrication methods of biocomposites [<a href="#B17-polymers-17-00252" class="html-bibr">17</a>].</p>
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<p>Aerogels based on chemical components. Reprinted with permission from [Jingyun Jing] (Recent Advances in the Synthesis and Application of Three-Dimensional Graphene-Based Aerogels); published by MDPI (2022) [<a href="#B36-polymers-17-00252" class="html-bibr">36</a>].</p>
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<p>Biodegradation behavior of various scaffolds in physiological fluids. SEM images representing the biodegradation behavior of various scaffolds (the 3D PLGA scaffolds and the gelatine/n-HA/PLGA scaffolds) exposed at different time intervals (1, 5, 9 weeks). Reprinted with permission from [Kankala et al.] (3D-Printing of Microfibrous Porous Scaffolds Based on Hybrid Approaches for Bone Tissue Engineering); published by MDPI (2018) [<a href="#B67-polymers-17-00252" class="html-bibr">67</a>].</p>
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<p>The preparation process of the PCN/CR/ATH nanofibers by electrospinning (<b>a</b>); the principle of the PCN/CR/ATH nanofiber in monitoring food freshness (<b>b</b>). Reprinted with permission from Elsevier 2024 [<a href="#B79-polymers-17-00252" class="html-bibr">79</a>].</p>
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<p>Main characteristics of biopolymers. Reprinted with permission from [Ocsana Opriș] (An Overview of Biopolymers for Drug Delivery Applications); published by MDPI (2024) [<a href="#B108-polymers-17-00252" class="html-bibr">108</a>].</p>
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<p>Scheme of the DN hydrogel formation comprising PITAU/Alg covalent gel as the first network and self-assembled peptides as the second network. Reprinted with permission from [Ghilan A.] (Injectable Networks Based on a Hybrid Synthetic/Natural Polymer Gel and Self-Assembling Peptides Functioning as Reinforcing Fillers.); published by MDPI (2023) [<a href="#B121-polymers-17-00252" class="html-bibr">121</a>].</p>
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<p>Schematic representation of the developed bioactive hybrid formulations and the visual aspects of the produced films. Reprinted with permission from [Darie-Nita R.N.] (Bioactive and Physico-Chemical Assessment of Innovative Poly(Lactic Acid)-Based Biocomposites Containing Sage, Coconut Oil, and Modified Nanoclay); published by MDPI (2023) [<a href="#B128-polymers-17-00252" class="html-bibr">128</a>].</p>
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<p>Synthesis and main features of chitosan (CS)-silica hybrid aerogels. Reprinted with permission from [Reyes-Peces et al.] (Chitosan-GPTMS-Silica Hybrid Mesoporous Aerogels for Bone Tissue Engineering); published by MDPI (2020) [<a href="#B138-polymers-17-00252" class="html-bibr">138</a>].</p>
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<p>(<b>a</b>) Scheme of the hierarchical structure of the silk fibers. (<b>b</b>) PGP structure. (<b>c</b>) Preparation steps for the development of PSCG bio-films. (<b>d</b>) PSCG bio-films. Reprinted with permission from Elsevier 2024 [<a href="#B141-polymers-17-00252" class="html-bibr">141</a>].</p>
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<p>Schematic illustration of the fabrication process and photographs of NFAs, CNFAs, and a CNFA-based piezoresistive sensor. Reprinted from [<a href="#B147-polymers-17-00252" class="html-bibr">147</a>] with permission from Elsevier 2024.</p>
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<p>Mechanisms of MB adsorption on agar/maltodextrin/PVA MMT membrane. Reprinted with permission from Elsevier 2024 [<a href="#B152-polymers-17-00252" class="html-bibr">152</a>].</p>
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<p>Schematic description of obtaining carbon aerogels derived from sodium lignin sulfonate embedded in carrageenan skeleton for methylene blue removal. Reprinted with permission from Elsevier 2024 [<a href="#B164-polymers-17-00252" class="html-bibr">164</a>].</p>
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<p>Development of an efficient sustainable EMI shield containing recycled EPDM from waste car bumper, a masterbatch of 40PP/60CaCO<sub>3</sub>, and a conductive CNT nanofiller. Reprinted with permission from [Moaref et al.] (From Waste to Value Added Products: Manufacturing High Electromagnetic Interference Shielding Composite from End-of-Life Vehicle (ELV) Waste); published by MDPI (2024) [<a href="#B170-polymers-17-00252" class="html-bibr">170</a>].</p>
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18 pages, 10611 KiB  
Article
Residual Life Prediction of SA-CNN-BILSTM Aero-Engine Based on a Multichannel Hybrid Network
by Yonghao He, Changjun Wen and Wei Xu
Appl. Sci. 2025, 15(2), 966; https://doi.org/10.3390/app15020966 - 20 Jan 2025
Viewed by 363
Abstract
As the core component of an airplane, the health status of the aviation engine is crucial for the safe operation of the aircraft. Therefore, predicting the remaining service life of the engine is of great significance for ensuring its safety and reliability. In [...] Read more.
As the core component of an airplane, the health status of the aviation engine is crucial for the safe operation of the aircraft. Therefore, predicting the remaining service life of the engine is of great significance for ensuring its safety and reliability. In this paper, a multichannel hybrid network is proposed; this network is a combination of the one-dimensional convolutional neural network (1D-CNN), the bidirectional long short-term memory network (BiLSTM), and the self-attention mechanism. For each sensor of the engine, an SA-CNN-BiLSTM network is established. The one-dimensional convolutional neural network and the bidirectional long short-term memory network are used to extract the spatial features and temporal features of the input data, respectively. Moreover, multichannel modeling is utilized to achieve the parallel processing of different sensors. Subsequently, the results are stitched together to establish a mapping relationship with the engine’s remaining useful life (RUL). Experimental validation was conducted on the aero-engine C-MAPSS dataset. The prediction results were compared with those of the other seven models to verify the effectiveness of this method in predicting the remaining service life. The results indicate that the proposed method significantly reduces the prediction error compared to other models. Specifically, for the two datasets, their mean absolute errors were only 11.47 and 11.76, the root-mean-square error values were only 12.26 and 12.78, and the scoring function values were only 195 and 227. Full article
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<p>Structure of a CNN.</p>
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<p>Schematic diagram of the convolution principle.</p>
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<p>Structure of bidirectional long short-term memory network.</p>
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<p>Structure of the attention mechanism.</p>
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<p>Prediction flow of multichannel SA-CNN-BiLSTM.</p>
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<p>Sensors of the first type.</p>
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<p>Sensors of the second type. (<b>a</b>) The variation in the values of three representative sensors with respect to the engine running time. (<b>b</b>) The specific values of sensor #2 as the running time of engines #1–#4 increases.</p>
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<p>Sensors of the third type. (<b>a</b>) The variation in the values of four representative sensors with respect to the engine running time. (<b>b</b>) The specific values of sensor #7 as the running time of engines #1–#4 increases.</p>
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<p>Segmented linear degradation model.</p>
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<p>Schematic of the sliding time window.</p>
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<p>Effect of sliding window size on RMSE and Score.</p>
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<p>Prediction results of FD001 test set on the model.</p>
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<p>Prediction results of FD003 test set on the model.</p>
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<p>Predicted results of the engine degradation process. (<b>a</b>) Unit #31 in FD001. (<b>b</b>) Unit #64n FD001. (<b>c</b>) Unit #57 in FD003. (<b>d</b>) Unit #70 in FD003.</p>
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<p>Predicted results of the engine degradation process. (<b>a</b>) Unit #31 in FD001. (<b>b</b>) Unit #64n FD001. (<b>c</b>) Unit #57 in FD003. (<b>d</b>) Unit #70 in FD003.</p>
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<p>Comparison of MAE results for different methods.</p>
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<p>Comparison of RMSE results for different methods.</p>
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<p>Comparison of Score results of different methods.</p>
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14 pages, 5735 KiB  
Article
Research on Fire Detection of Cotton Picker Based on Improved Algorithm
by Zhai Shi, Fangwei Wu, Changjie Han and Dongdong Song
Sensors 2025, 25(2), 564; https://doi.org/10.3390/s25020564 - 19 Jan 2025
Viewed by 283
Abstract
According to the physical characteristics of cotton and the work characteristics of cotton pickers in the field, during the picking process, there is a risk of cotton combustion. The cotton picker working environment is complex, cotton ignition can be hidden, and fire is [...] Read more.
According to the physical characteristics of cotton and the work characteristics of cotton pickers in the field, during the picking process, there is a risk of cotton combustion. The cotton picker working environment is complex, cotton ignition can be hidden, and fire is difficult to detect. Therefore, in this study, we designed an improved algorithm for multi-sensor data fusion; built a cotton picker fire detection system by using infrared temperature sensors, CO sensors, and the upper computer; and proposed a BP neural network model based on improved mutation operator hybrid gray wolf optimizer and particle swarm optimization (MGWO-PSO) algorithm based on the BP neural network model. This algorithm includes the introduction of a mutation operator in the gray wolf algorithm to improve the search ability of the algorithm, and, at the same time, we introduce the PSO algorithm idea. The improved fusion algorithm is used as a learning algorithm to optimize the BP neural network, and the optimized network is used to process and predict the data collected from temperature and gas sensors, which effectively improves the accuracy of fire prediction. The sensor measurements were compared with the actual values to verify the effectiveness of the GWO-PSO-optimized BP neural network model. Once experimentally verified, the improved GWO-PSO algorithm achieves a correlation coefficient R of 0.96929, a prediction accuracy rate of 96.10%, and a prediction error rate of only 3.9%, while the system monitors an accurate early warning rate of 96.07%, and the false alarm and omission rates are both less than 5%. This study can detect cotton picker fires in real time and provide timely warnings, which provides a new method for the accurate detection of fires during the field operation of cotton pickers. Full article
(This article belongs to the Section Smart Agriculture)
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<p>Overall system design diagram.</p>
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<p>System hardware diagram.</p>
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<p>Temperature module and CO module diagram.</p>
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<p>Software system diagram.</p>
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<p>Threshold graph.</p>
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<p>System flow chart.</p>
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<p>Data acquisition bench.</p>
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<p>Flowchart of the improved GWO-PSO-BP algorithm.</p>
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<p>Population spatial comparison.</p>
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<p>Iteration comparison chart.</p>
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<p>Display of real-time forecast data graphs.</p>
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<p>Simulation of the wind field inside the picking room.</p>
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<p>Cotton picker operation sensor location map.</p>
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15 pages, 5662 KiB  
Article
A Facile Electrode Modification Approach Based on Metal-Free Carbonaceous Carbon Black/Carbon Nanofibers for Electrochemical Sensing of Bisphenol A in Food
by Jin Wang, Zhen Yang, Shuanghuan Gu, Mingfei Pan and Longhua Xu
Foods 2025, 14(2), 314; https://doi.org/10.3390/foods14020314 - 18 Jan 2025
Viewed by 532
Abstract
Bisphenol A (BPA) is a typical environmental estrogen that is distributed worldwide and has the potential to pose a hazard to the ecological environment and human health. The development of an efficient and sensitive sensing strategy for the monitoring of BPA residues is [...] Read more.
Bisphenol A (BPA) is a typical environmental estrogen that is distributed worldwide and has the potential to pose a hazard to the ecological environment and human health. The development of an efficient and sensitive sensing strategy for the monitoring of BPA residues is of paramount importance. A novel electrochemical sensor based on carbon black and carbon nanofibers composite (CB/f-CNF)-assisted signal amplification has been successfully constructed for the amperometric detection of BPA in foods. Herein, the hybrid CB/f-CNF was prepared using a simple one-step ultrasonication method, and exhibited good electron transfer capability and excellent catalytic properties, which can be attributed to the large surface area of carbon black and the strong enhancement of the conductivity and porosity of carbon nanofibers, which promote a faster electron transfer process on the electrode surface. Under the optimized conditions, the proposed CB/f-CNF/GCE sensor exhibited a wide linear response range (0.4–50.0 × 10−6 mol/L) with a low limit of detection of 5.9 × 10−8 mol/L for BPA quantification. Recovery tests were conducted on canned peaches and boxed milk, yielding satisfactory recoveries of 86.0–102.6%. Furthermore, the developed method was employed for the rapid and sensitive detection of BPA in canned meat and packaged milk, demonstrating comparable accuracy to the HPLC method. This work presents an efficient signal amplification strategy through the utilization of carbon/carbon nanocomposite sensitization technology. Full article
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<p>Schematic illustration of the construction of the CB/f-CNF/GCE sensor. Note: Black line, red line, blue line, purple line, yellow line, green line and cyan line are the DPV curves of CB/f-CNF/GCE in bisphenol A solution of 0.4 μM, 1 μM, 2 μM, 6 μM, 10 μM, 20 μM and 50 μM, respectively.</p>
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<p>SEM images of CNF (<b>A</b>), f-CNF (<b>B</b>), CB (<b>C</b>), and CB/f-CNF (<b>D</b>). XRD patterns for the as-synthesized CB, f-CNF, and CB/f-CNF (<b>E</b>); Raman spectra of carbon black, f-CNF, and CB/f-CNF composite (<b>F</b>).</p>
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<p>The CV (<b>A</b>) and EIS (<b>B</b>) in a [Fe(CN)6]<sup>3−/4−</sup> redox probe solution response of GCE, CB/GCE, f-CNF/GCE, and CB/f-CNF/GCE. CV responses for GCE (<b>C</b>) and (<b>D</b>) The CB/f-CNF/GCE was analyzed at different scan rates, ranging from 10 to 100 mV s<sup>−1</sup>, in a 2.0 mmol·L<sup>−1</sup> [Fe(CN)6]<sup>3/4−</sup> solution. Note: Different lines from top to bottom are the CV curves of GCE and CB/f-CNF/GCE under the sweep speed of 10, 20, 30, 40, 50, 60, 70, 80, 90, 100 mv respectively.</p>
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<p>(<b>A</b>) CV curves of bare GCE, CB/GCE, f-CNF/GCE and CB/f-CNF/GCE in the BR containing 50 μmol L<sup>−1</sup> BPA and CV curves of CB/f-CNF/GCE in a BPA-free BR solution (blank). (<b>B</b>) CV curves of CB/f-CNF/GCE in the BR containing 20 μmol L<sup>−1</sup> BPA at various scan rates: 20, 40, 60, 80, and 100 mV s<sup>−1</sup>. (<b>C</b>) The linear relationship of the BPA oxidation peak currents versus the scan rates. (<b>D</b>) The relationship between the BPA oxidation peak potentials and the natural logarithm of scan rates. Note: The black, red, blue, green and purple lines are the CV curves of CB/f-CNF/GCE in BR containing 20 μmol L<sup>−1</sup> BPA at: 20, 40, 60, 80 and 100 mV s<sup>−1</sup> scanning rates, respectively.</p>
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<p>(<b>A</b>) DPV curves of CB/f-CNF/GCE for different concentrations of BPA. (<b>B</b>) The linear relationship between the peak current and the concentration of BPA was studied, along with anti-interference performance (<b>C</b>) and (<b>D</b>) repeatability experiments of CB/f-CNF/GCE. Note: In the <a href="#foods-14-00314-f005" class="html-fig">Figure 5</a>A, the DPV curves of CB/f-CNF/GCE in bisphenol A solution of 0.4 μM, 1 μM, 2 μM, 6 μM, 10 μM, 20 μM and 50 μM are shown in black lines, red lines, blue lines, purple lines, yellow lines, green lines and cyan lines respectively.</p>
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21 pages, 7219 KiB  
Article
Time Series Data Augmentation for Energy Consumption Data Based on Improved TimeGAN
by Peihao Tang, Zhen Li, Xuanlin Wang, Xueping Liu and Peng Mou
Sensors 2025, 25(2), 493; https://doi.org/10.3390/s25020493 - 16 Jan 2025
Viewed by 410
Abstract
Predicting the time series energy consumption data of manufacturing processes can optimize energy management efficiency and reduce maintenance costs for enterprises. Using deep learning algorithms to establish prediction models for sensor data is an effective approach; however, the performance of these models is [...] Read more.
Predicting the time series energy consumption data of manufacturing processes can optimize energy management efficiency and reduce maintenance costs for enterprises. Using deep learning algorithms to establish prediction models for sensor data is an effective approach; however, the performance of these models is significantly influenced by the quantity and quality of the training data. In real production environments, the amount of time series data that can be collected during the manufacturing process is limited, which can lead to a decline in model performance. In this paper, we use an improved TimeGAN model for the augmentation of energy consumption data, which incorporates a multi-head self-attention mechanism layer into the recovery model to enhance prediction accuracy. A hybrid CNN-GRU model is used to predict the energy consumption data from the operational processes of manufacturing equipment. After data augmentation, the prediction model exhibits significant reductions in RMSE and MAE along with an increase in the R2 value. The prediction accuracy of the model is maximized when the amount of generated synthetic data is approximately twice that of the original data. Full article
(This article belongs to the Section Intelligent Sensors)
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<p>The structure of the Variational Autoencoder.</p>
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<p>The structure of the Generative Adversarial Network.</p>
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<p>The research outline.</p>
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<p>The structure of the TimeGAN model.</p>
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<p>The loss functions of the TimeGAN model.</p>
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<p>The structure of the improved recovery module.</p>
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<p>The structure of the prediction model.</p>
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<p>The manufacturing production line.</p>
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<p>The energy consumption data of the board-splitting machine.</p>
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<p>The time series after removing outliers.</p>
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<p>The original data and generated data.</p>
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<p>The data segments of the original data and generated data.</p>
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<p>PCA visualization on the original data and generated data.</p>
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<p>t-SNE visualization on the original data and generated data.</p>
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<p>Results of prediction models on the training set and test set after using different amounts of generated data to expand the dataset.</p>
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<p>Results of prediction models on the training set and test set after using different data augmentation methods to expand the dataset.</p>
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12 pages, 2987 KiB  
Article
Analysis of Refractive Index Sensing Properties of a Hybrid Hollow Cylindrical Tetramer Array
by Meng Wang, Paerhatijiang Tuersun, Aibibula Abudula, Lan Jiang and Dibo Xu
Nanomaterials 2025, 15(2), 118; https://doi.org/10.3390/nano15020118 - 15 Jan 2025
Viewed by 366
Abstract
In recent years, metal surface plasmon resonance sensors and dielectric guided-mode resonance sensors have attracted the attention of researchers. Metal sensors are sensitive to environmental disturbances but have high optical losses, while dielectric sensors have low losses but limited sensitivity. To overcome these [...] Read more.
In recent years, metal surface plasmon resonance sensors and dielectric guided-mode resonance sensors have attracted the attention of researchers. Metal sensors are sensitive to environmental disturbances but have high optical losses, while dielectric sensors have low losses but limited sensitivity. To overcome these limitations, hybrid resonance sensors that combine the advantages of metal and dielectric were proposed to achieve a high sensitivity and a high Q factor at the same time. In this paper, a hybrid hollow cylindrical tetramer array was designed, and the effects of the hole radius, external radius, height, period, incidence angle, and polarization angle of the hollow cylindrical tetramer array on the refractive index sensing properties were quantitatively analyzed using the finite difference time domain method. It is found that the position of the resonance peaks can be freely tuned in the visible and near-infrared regions, and a sensitivity of up to 542.8 nm/RIU can be achieved, with a Q factor of 1495.1 and a figure of merit of 1103.3 RIU−1. The hybrid metal–dielectric nanostructured array provides a possibility for the realization of high-performance sensing devices. Full article
(This article belongs to the Special Issue Modeling, Simulation and Optimization of Nanomaterials)
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<p>The unit structure, (<b>a</b>) Three-dimensional diagram and (<b>b</b>) <span class="html-italic">xoy</span> plane diagram of the hybrid hollow cylindrical tetrameric array.</p>
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<p>The reflectance spectrum of the hybrid hollow cylindrical tetramer array varies with (<b>a</b>) hole radius <span class="html-italic">r</span> and (<b>b</b>) environmental refractive index <span class="html-italic">n</span> and their corresponding values of (<b>c</b>) <span class="html-italic">S</span><sub>bulk</sub>, (<b>d</b>) <span class="html-italic">Q</span> factor, and (<b>e</b>) <span class="html-italic">FOM</span>. In the simulation, the external radius <span class="html-italic">R</span><sub>1</sub> of the large hollow cylinder is 140 nm, the external radius <span class="html-italic">R</span><sub>2</sub> of the small hollow cylinder is 100 nm, the period <span class="html-italic">P</span> is 800 nm, the height <span class="html-italic">h</span> of Si<sub>3</sub>N<sub>4</sub> is 225 nm, and the thickness <span class="html-italic">t</span> of the Au layer is 100 nm.</p>
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<p>Electric field distributions in the (<b>a</b>–<b>c</b>) <span class="html-italic">xoy</span> plane and (<b>d</b>–<b>f</b>) <span class="html-italic">xoz</span> plane at the resonance wavelengths of 679.0 nm, 736.3 nm, and 868.9 nm, respectively.</p>
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<p>The variation in (<b>a</b>) reflectance spectrum with the external radius <span class="html-italic">R</span><sub>2</sub> of the small hollow cylinder and the corresponding (<b>b</b>) <span class="html-italic">S</span><sub>bulk</sub>, (<b>c</b>) <span class="html-italic">Q</span> factor, and (<b>d</b>) <span class="html-italic">FOM</span> of the hybrid hollow cylindrical tetramer array. In the simulation, the external radius <span class="html-italic">R</span><sub>1</sub> of the large hollow cylinder is 140 nm, the hole radius <span class="html-italic">r</span> of the hollow cylinder is 40 nm, the period <span class="html-italic">P</span> is 800 nm, the height <span class="html-italic">h</span> of Si<sub>3</sub>N<sub>4</sub> is 225 nm, the thickness <span class="html-italic">t</span> of the Au layer is 100 nm, and the environmental refractive index <span class="html-italic">n</span> is 1.3.</p>
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<p>The variation in (<b>a</b>) reflectance spectrum with the cylindrical height <span class="html-italic">h</span> and the corresponding (<b>b</b>) <span class="html-italic">S</span><sub>bulk</sub>, (<b>c</b>) <span class="html-italic">Q</span> factor, and (<b>d</b>) <span class="html-italic">FOM</span> of the hybrid hollow cylindrical tetramer array. In the simulation, the external radius <span class="html-italic">R</span><sub>1</sub> of the large hollow cylinder is 140 nm, the external radius <span class="html-italic">R</span><sub>2</sub> of the small hollow cylinder is 100 nm, the hole radius <span class="html-italic">r</span> of the hollow cylinder is 40 nm, the period <span class="html-italic">P</span> is 800 nm, the thickness <span class="html-italic">t</span> of the Au layer is 100 nm, and the environmental refractive index <span class="html-italic">n</span> is 1.3.</p>
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<p>The variation in (<b>a</b>) reflectance spectrum with the period <span class="html-italic">P</span> and the corresponding (<b>b</b>) <span class="html-italic">S</span><sub>bulk</sub>, (<b>c</b>) <span class="html-italic">Q</span> factor, and (<b>d</b>) <span class="html-italic">FOM</span> of the hybrid hollow cylindrical tetramer array. In the simulation, the external radius <span class="html-italic">R</span><sub>1</sub> of the large hollow cylinder is 140 nm, the external radius <span class="html-italic">R</span><sub>2</sub> of the small hollow cylinder is 100 nm, the hole radius <span class="html-italic">r</span> of the hollow cylinder is 40 nm, the height <span class="html-italic">h</span> of Si<sub>3</sub>N<sub>4</sub> is 225 nm, the thickness <span class="html-italic">t</span> of the Au layer is 100 nm, and the environmental refractive index <span class="html-italic">n</span> is 1.3.</p>
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<p>The variation in reflectance spectrum of the hybrid hollow cylindrical tetramer array with (<b>a</b>) incidence angle <span class="html-italic">θ</span> and (<b>b</b>) polarization angle of the incident light.</p>
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26 pages, 21796 KiB  
Article
Design of a Cost-Effective Ultrasound Force Sensor and Force Control System for Robotic Extra-Body Ultrasound Imaging
by Yixuan Zheng, Hongyuan Ning, Eason Rangarajan, Aban Merali, Adam Geale, Lukas Lindenroth, Zhouyang Xu, Weizhao Wang, Philipp Kruse, Steven Morris, Liang Ye, Xinyi Fu, Kawal Rhode and Richard James Housden
Sensors 2025, 25(2), 468; https://doi.org/10.3390/s25020468 - 15 Jan 2025
Viewed by 592
Abstract
Ultrasound imaging is widely valued for its safety, non-invasiveness, and real-time capabilities but is often limited by operator variability, affecting image quality and reproducibility. Robot-assisted ultrasound may provide a solution by delivering more consistent, precise, and faster scans, potentially reducing human error and [...] Read more.
Ultrasound imaging is widely valued for its safety, non-invasiveness, and real-time capabilities but is often limited by operator variability, affecting image quality and reproducibility. Robot-assisted ultrasound may provide a solution by delivering more consistent, precise, and faster scans, potentially reducing human error and healthcare costs. Effective force control is crucial in robotic ultrasound scanning to ensure consistent image quality and patient safety. However, existing robotic ultrasound systems rely heavily on expensive commercial force sensors or the integrated sensors of commercial robotic arms, limiting their accessibility. To address these challenges, we developed a cost-effective, lightweight, 3D-printed force sensor and a hybrid position–force control strategy tailored for robotic ultrasound scanning. The system integrates patient-to-robot registration, automated scanning path planning, and multi-sensor data fusion, allowing the robot to autonomously locate the patient, target the region of interest, and maintain optimal contact force during scanning. Validation was conducted using an ultrasound-compatible abdominal aortic aneurysm (AAA) phantom created from patient CT data and healthy volunteer testing. For the volunteer testing, during a 1-min scan, 65% of the forces were within the good image range. Both volunteers reported no discomfort or pain during the whole procedure. These results demonstrate the potential of the system to provide safe, precise, and autonomous robotic ultrasound imaging in real-world conditions. Full article
(This article belongs to the Special Issue Multi-sensor Fusion in Medical Imaging, Diagnosis and Therapy)
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<p>Patient-to-robot base registration process, along with three transformations utilized in this study shown with red arrows, relative marker transformation calculation with the help of the camera with blue arrows, and final patient-to-robot base transformation with the green arrow [<a href="#B19-sensors-25-00468" class="html-bibr">19</a>].</p>
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<p>Workflow for automatic ultrasound image acquisition of the current system. The colorful path in the ’Correct Target Points’ section represents the corrected path plan, with blue indicating the start and red indicating the stop point. For detailed explanation, see Figure 20.</p>
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<p>Custom-made force sensor mechanical structure design. (<b>a</b>) Left and right parts are separate to fit the ultrasound probe; (<b>b</b>) upper and lower parts are separate for easy replacement of the load cells; (<b>c</b>) complete sensor structure with probe and load cells; (<b>d</b>) special design on the supporting cylinders.</p>
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<p>Force sensor signal processing setup. (<b>a</b>) Front view of the force sensor with integrated load cells. (<b>b</b>) Back view of the force sensor showing the custom-designed printed circuit board (PCB) for signal integration and zero calibration, along with two 4-pin input cables (each carrying signals from two load cells) and a 6-pin output cable connected to the Teensy 4.1. (<b>c</b>) Bottom view of the 3D-printed box for the Teensy 4.1 board, with sensor signal and robot master cables. (<b>d</b>) Top view of the Teensy 4.1 box, highlighting the USB cable used for direct sensor signal access when needed for debugging.</p>
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<p>User interface for two path planning methods: (<b>a</b>) direct path planning method; (<b>b</b>) area coverage path planning method.</p>
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<p>Ultrasound-compatible abdominal aortic aneurysm phantom: (<b>a</b>) external appearance and (<b>b</b>) ultrasound visualization of internal structures. The vertical dotted line in (<b>b</b>) represent a depth scale bar, with each segment indicating 1 cm.</p>
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<p>Sensor calibration and performance assessment: (<b>a</b>) on its own with known weights; (<b>b</b>) on the robot with an ultrasound probe and commercial force sensor.</p>
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<p>Experimental setup for validating the surface force-following algorithm in the Z-direction using an ATI force sensor, a 3D-printed framework, and two AprilTag markers used for position registration.</p>
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<p>Selected area on abdominal phantom in simulation window.</p>
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<p>Automated ultrasound image acquisition on phantom experiment setup.</p>
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<p>Setup for automated ultrasound image acquisition in healthy volunteer tests: (<b>a</b>) Volunteer 1 with BMI = 21, (<b>b</b>) Volunteer 2 with BMI = 33.</p>
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<p>Abdominal aorta and iliac artery localization in volunteer testing: (<b>a</b>) B−mode image of the abdominal aorta annotated by a clinical vascular scientist (Volunteer 1) and (<b>b</b>) pulsed wave Doppler of the iliac artery (Volunteer 2).</p>
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<p>Ultrasound images acquired by the robot at different force levels: Volunteer 1’s abdominal aorta (yellow border) and Volunteer 2’s iliac artery (blue border). The vertical dotted line in all the ultrasound images represent a depth scale bar.</p>
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<p>Performance testing of the force sensor using known weights: (<b>a</b>) linearity and calibration equation relating sensor raw data to ground truth and (<b>b</b>) hysteresis evaluation over five loading–unloading cycles, comparing input and measured weights. The five colored lines overlap, resulting in a single visible black line. Detailed zoomed-in graphs are provided in <a href="#sensors-25-00468-f015" class="html-fig">Figure 15</a>.</p>
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<p>Separate hysteresis maps for five cycles with zoomed-in largest hysteresis points highlighted in the orange rectangle.</p>
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<p>Correlation between the ATI commercial force sensor readings (<span class="html-italic">x</span>-axis) and our custom-made ultrasound force sensor readings (<span class="html-italic">y</span>-axis). Each blue point represents a measurement instance where the same force was applied to both sensors. The red solid line indicates the linear fit of these data points, while the blue dashed line represents the ideal 1:1 correspondence (y = x) between these two sensors.</p>
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<p>Force comparison between custom-made force sensor and ATI force sensor.</p>
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<p>Force sensor data, platform position, and robot position over time.</p>
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<p>Force values and distributions in the combined path-planning and force-control experiment on phantom without adipose layer. The top subfigure shows force variation over time, with 3 N and 6 N thresholds marked; the middle subfigure depicts the force value distribution, highlighting ranges below 3 N, 3–6 N, and above 6 N; and the bottom subfigure displays the time proportion within each force range. Red, green and blue colours in the middle and buttom graphs match with each other.</p>
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<p>Probe’s 3D trajectory and the phantom surface visualization in the real-world coordinate system. The abdominal phantom surface is represented as a black grid and the probe centre’s 3D trajectory during the scanning process is colour-coded by time, transitioning from blue (start) to red (end).</p>
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<p>Force values and distributions in automated ultrasound image acquisition experiment on phantom with adipose layer. The top subfigure shows force variation over time, with 3 N and 6 N thresholds marked; the middle subfigure depicts the force value distribution, highlighting ranges below 3 N, 3–6 N, and above 6 N; and the bottom subfigure displays the time proportion within each force range. Red, green and blue colours in the middle and buttom graphs match with each other.</p>
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<p>Ultrasound images acquired by robot at varying force levels on AAA phantom.</p>
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<p>Abdominal aorta ultrasound images acquired by the robotic system: (<b>a</b>) Volunteer 1’s original image; (<b>b</b>) Volunteer 1’s images annotated by registered clinical vascular scientist; (<b>c</b>) Volunteer 2’s original image; (<b>d</b>) Volunteer 2’s images annotated by registered clinical vascular scientist.</p>
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<p>Force values and distributions in automated ultrasound image acquisition experiment on two volunteers. Red, green and blue colours in the middle and buttom graphs match with each other.</p>
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<p>Force values and distributions in automated ultrasound image acquisition experiment on two volunteers. Red, green and blue colours in the middle and buttom graphs match with each other.</p>
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33 pages, 8797 KiB  
Article
Hybrid Plant Growth: Integrating Stochastic, Empirical, and Optimization Models with Machine Learning for Controlled Environment Agriculture
by Nezha Kharraz and István Szabó
Agronomy 2025, 15(1), 189; https://doi.org/10.3390/agronomy15010189 - 14 Jan 2025
Viewed by 474
Abstract
Controlled Environment Agriculture (CEA) offers a viable solution for sustainable crop production, yet the optimization of the latter requires precise modeling and resource management. This study introduces a novel hybrid plant growth model integrating stochastic, empirical, and optimization approaches, using Internet of Things [...] Read more.
Controlled Environment Agriculture (CEA) offers a viable solution for sustainable crop production, yet the optimization of the latter requires precise modeling and resource management. This study introduces a novel hybrid plant growth model integrating stochastic, empirical, and optimization approaches, using Internet of Things sensors for real-time data collection. Unlike traditional methods, the hybrid model systematically captures environmental variability, simulates plant growth dynamics, and optimizes resource inputs. The prototype growth chamber, equipped with IoT sensors for monitoring environmental parameters such as light intensity, temperature, CO2, humidity, and water intake, was primarily used to provide accurate input data for the model and specifically light intensity, water intake and nutrient intake. While experimental tests on lettuce were conducted to validate initial environmental conditions, this study was focused on simulation-based analysis. Specific tests simulated plant responses to varying levels of light, water, and nutrients, enabling the validation of the proposed hybrid model. We varied light durations between 6 and 14 h/day, watering levels between 5 and 10 L/day, and nutrient concentrations between 3 and 11 g/day. Additional simulations modeled different sowing intervals to capture internal plant variability. The results demonstrated that the optimal growth conditions were 14 h/day of light, 9 L/day of water, and 5 g/day of nutrients; maximized plant biomass (200 g), leaf area (800 cm2), and height (90 cm). Key novel metrics developed in this study, the Growth Efficiency Ratio (GER) and Plant Growth Index (PGI), provided solid tools for evaluating plant performance and resource efficiency. Simulations showed that GER peaked at 0.6 for approximately 200 units of combined inputs, beyond which diminishing returns were observed. PGI increased to 0.8 to day 20 and saturated to 1 by day 30. The role of IoT sensors was critical in enhancing model accuracy and replicability by supplying real-time data on environmental variability. The hybrid model’s adaptability in the future may offer scalability to diverse crop types and environmental settings, establishing a foundation for its integration into decision-support systems for large-scale indoor farming. Full article
(This article belongs to the Special Issue Application of Internet of Things in Agroecosystems)
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<p>Side view of the protype showing the electronic part for monitoring.</p>
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<p>IoT-integrated growing chamber from inside.</p>
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<p>Early growth stage of lettuce taken from the inside of the growth chamber.</p>
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<p>Processed image of the growing chamber for lettuce seedling analysis.</p>
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<p>Image of threshold segmentation of lettuce seedling.</p>
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<p>Plant growth prediction and resource efficiency.</p>
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<p>Combined Resource Use vs. GER for one head of lettuce.</p>
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<p>GER heatmap: light vs. water.</p>
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<p>Cooling Load Ratio and COP of cooling fans.</p>
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<p>Analysis of COP performance in response to temperature differences.</p>
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<p>Biomass yield and GER comparison across conditions.</p>
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<p>Biomass yield and GER comparison across water conditions per head of lettuce.</p>
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<p>Biomass yield and GER across nutrient conditions per head of lettuce.</p>
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<p>Fertilizer input vs. plant growth with watering rates and <math display="inline"><semantics> <mrow> <msup> <mi>R</mi> <mn>2</mn> </msup> </mrow> </semantics></math> values.</p>
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<p>Light consumption vs. plant growth with watering rates and <math display="inline"><semantics> <mrow> <msup> <mi>R</mi> <mn>2</mn> </msup> </mrow> </semantics></math> values.</p>
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<p>Logistic growth model simulation of leaf area per leaf in lettuce.</p>
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<p>Leaf area vs. water levels.</p>
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<p>Leaf area vs. nutrient intake.</p>
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<p>Leaf area vs. light intensity.</p>
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<p>User input data workflow.</p>
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<p>PGI (Plant Growth Index) over 30 Days.</p>
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17 pages, 2598 KiB  
Article
Anti-Tissue-Transglutaminase IgA Antibodies Presence Determination Using Electrochemical Square Wave Voltammetry and Modified Electrodes Based on Polypyrrole and Quantum Dots
by Angela Gabriela Pãun, Simona Popescu, Alisa Ioana Ungureanu, Roxana Trusca, Alina Popp, Cristina Dumitriu and George-Octavian Buica
Biosensors 2025, 15(1), 42; https://doi.org/10.3390/bios15010042 - 13 Jan 2025
Viewed by 545
Abstract
A novel electrochemical detection method utilizing a cost-effective hybrid-modified electrode has been established. A glassy carbon (GC) modified electrode was tested for its ability to measure electrochemical tTG antibody levels, which are essential for diagnosing and monitoring Celiac disease (CD). Tissue transglutaminase protein [...] Read more.
A novel electrochemical detection method utilizing a cost-effective hybrid-modified electrode has been established. A glassy carbon (GC) modified electrode was tested for its ability to measure electrochemical tTG antibody levels, which are essential for diagnosing and monitoring Celiac disease (CD). Tissue transglutaminase protein biomolecules are immobilized on a quantum dots-polypyrrole nanocomposite in the improved electrode. Initial, quantum dots (QDs) were obtained from Bombyx mori silk fibroin and embedded in polypyrrole film. Using carbodiimide coupling, a polyamidoamine (PAMAM) dendrimer was linked with GQDs-polypyrrole film to improve sensor sensitivity. The tissue transglutaminase (tTG) antigen was cross-linked onto PAMAM using N-(3-dimethylaminopropyl)-N′-ethylcarbodiimide hydrochloride (EDC)-N-hydroxy succinimide (NHS) chemistry to develop a nanoprobe that can detect human serum anti-tTG antibodies. The physicochemical characteristics of the synthesized nanocomposite were examined by FTIR, UV-visible, FE-SEM, EDX, and electrochemical studies. The novel electrode measures anti-tissue antibody levels in real time using human blood serum samples. The modified electrode has great repeatability and an 8.7 U/mL detection limit. Serum samples from healthy people and CD patients were compared to standard ELISA kit assays. SPSS and Excel were used for statistical analysis. The improved electrode and detection system can identify anti-tissue antibodies up to 80 U/mL. Full article
(This article belongs to the Special Issue Feature Paper in Biosensor and Bioelectronic Devices 2024)
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<p>Spectra for QdsSF solution: (<b>a</b>) UV-Vis absorption, (<b>b</b>) Florescence, (<b>c</b>) FT-IR.</p>
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<p>SEM images of modified electrodes after each step, at different magnifications: (<b>a</b>) GC/PPy, (<b>b</b>) GC/PPy-QDsSF, (<b>c</b>) GC/PPy-QDsSF-PAMAM, (<b>d</b>) GC/PPy-QDsSF-PAMAM-tTG.</p>
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<p>(<b>a</b>) Kubelka-Munk transformed reflectance spectra of GC/PPy (black line) and GC/PPy-QDsSf (olive line); (<b>b</b>) FT-IR images corresponding to the samples: QDsSF (blue line); GC/PPy-QDsSF (olive line); GC/PPy-QDsSF-PAMAM (magenta line) and GC/PPy-QDsSF-PAMAM-tTG (violet line).</p>
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<p>(<b>a</b>) EIS for modified electrodes (Nyquist diagram) recorded vs. Ag/AgCl 3 M KCl in PBS + Fe<sup>2+</sup>/Fe<sup>3+</sup> (<b>b</b>) equivalent circuit to fit the data, (<b>c</b>) SWV curves corresponding to modified electrodes vs. Ag/AgCl 3 M KCl in PBS + Fe<sup>2+</sup>/Fe<sup>3+</sup>.</p>
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<p>CVs (2nd cycle) recorded in PBS with Fe<sup>2+</sup>/Fe<sup>3+</sup> vs. Ag/AgCl 3M KCl, at different scan rates corresponding to (<b>a</b>) GC/PPyQDsSF, (<b>b</b>) GC/PPy-QDsSF-PAMAM and (<b>c</b>) GC/PPy-QDsSF-PAMAM-tTG.</p>
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<p>Calibration curve using GC/PPy-QDsSF-PAMAM-tTG electrode and standard ready to use anti tissue antibody solution.</p>
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<p>Schematic illustration for preparation of GC/PPy-QDsSF-PAMAM-tTG electrode and the detection strategy for anti-tissue antibody detection.</p>
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19 pages, 11145 KiB  
Article
Image-Driven Hybrid Structural Analysis Based on Continuum Point Cloud Method with Boundary Capturing Technique
by Kyung-Wan Seo, Junwon Park, Sang I. Park, Jeong-Hoon Song and Young-Cheol Yoon
Sensors 2025, 25(2), 410; https://doi.org/10.3390/s25020410 - 11 Jan 2025
Viewed by 575
Abstract
Conventional approaches for the structural health monitoring of infrastructures often rely on physical sensors or targets attached to structural members, which require considerable preparation, maintenance, and operational effort, including continuous on-site adjustments. This paper presents an image-driven hybrid structural analysis technique that combines [...] Read more.
Conventional approaches for the structural health monitoring of infrastructures often rely on physical sensors or targets attached to structural members, which require considerable preparation, maintenance, and operational effort, including continuous on-site adjustments. This paper presents an image-driven hybrid structural analysis technique that combines digital image processing (DIP) and regression analysis with a continuum point cloud method (CPCM) built on a particle-based strong formulation. Polynomial regressions capture the boundary shape change due to the structural loading and precisely identify the edge and corner coordinates of the deformed structure. The captured edge profiles are transformed into essential boundary conditions. This allows the construction of a strongly formulated boundary value problem (BVP), classified as the Dirichlet problem. Capturing boundary conditions from the digital image is novel, although a similar approach was applied to the point cloud data. It was shown that the CPCM is more efficient in this hybrid simulation framework than the weak-form-based numerical schemes. Unlike the finite element method (FEM), it can avoid aligning boundary nodes with regression points. A three-point bending test of a rubber beam was simulated to validate the developed technique. The simulation results were benchmarked against numerical results by ANSYS and various relevant numerical schemes. The technique can effectively solve the Dirichlet-type BVP, yielding accurate deformation, stress, and strain values across the entire problem domain when employing a linear strain model and increasing the number of CPCM nodes. In addition, comparative analysis with conventional displacement tracking techniques verifies the developed technique’s robustness. The proposed technique effectively circumvents the inherent limitations of traditional monitoring methods resulting from the reliance on physical gauges or target markers so that a robust and non-contact solution for remote structural health monitoring in real-scale infrastructures can be provided, even in unfavorable experimental environments. Full article
(This article belongs to the Special Issue Digital Image Processing and Sensing Technologies—Second Edition)
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<p>Dirichlet-type BVP configuration modeled with interior and boundary nodes.</p>
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<p>Configuration of three-point bending test for rubber beam.</p>
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<p>Experimental setup for digital image acquisition of the 3-point bending test: (<b>a</b>) specimen setup; (<b>b</b>) device setup.</p>
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<p>The procedure of estimation and assignment of the essential boundary value from the digital image to the CPCM simulation.</p>
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<p>DIP-based boundary capturing results by the steps outlined in <a href="#sensors-25-00410-f004" class="html-fig">Figure 4</a>: (<b>a</b>) the initial state image (step 1); (<b>b</b>) the deformed shape image (step 1); (<b>c</b>) 2D edge pixels (step 2 for the initial state); (<b>d</b>) 2D edge pixels (step 2 for the deformed specimen); (<b>e</b>) 2D edge pixels (step 3 for the initial state); (<b>f</b>) 2D edge pixels (step 3 for the deformed specimen); (<b>g</b>) captured essential boundary (step 3 for the initial state boundary nodes); (<b>h</b>) captured essential boundary (step 3 for boundary nodes after loading simulation); (<b>i</b>) total CPCM model for initial state; (<b>j</b>) total CPCM model after loading simulation.</p>
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<p>Edge displacement interpolation along the boundary nodes based on linear strain model with zero strain at <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>x</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msup> </mrow> </semantics></math> and end deformations <math display="inline"><semantics> <mrow> <mi>u</mi> <mo>(</mo> <msup> <mrow> <mi>x</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msup> <mo>)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>u</mi> <mfenced separators="|"> <mrow> <msup> <mrow> <mi>x</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msup> </mrow> </mfenced> </mrow> </semantics></math>.</p>
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<p>Essential boundary configuration for the rubber beam specimen (edge and corner point numbering).</p>
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<p>Surface plots for computed displacements obtained by different simulation methods and boundary capturing schemes for 3-point rubber beam bending test: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>f</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>g</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4), (<b>h</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4).</p>
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<p>Surface plots for computed displacements obtained by different simulation methods and boundary capturing schemes for 3-point rubber beam bending test: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>f</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>g</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4), (<b>h</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4).</p>
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<p>Surface plots for computed Cauchy stresses by different simulation methods and boundary capturing methods for 3-point rubber beam bending test: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>f</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>g</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4), (<b>h</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4).</p>
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<p>Surface plots for computed Cauchy stresses by different simulation methods and boundary capturing methods for 3-point rubber beam bending test: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 1), (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>f</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>g</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>x</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4), (<b>h</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>y</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4).</p>
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<p>Surface plots for computed Cauchy and von Mises stress by different simulation methods and boundary capturing methods for 3-point rubber beam bending test: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> <mo> </mo> <mo> </mo> </mrow> </semantics></math> (Method 1), (<b>b</b>) von Mises stress (Method 1), (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>d</b>) von Mises stress (Method 2), (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>f</b>) von Mises stress (Method 3), (<b>g</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4), (<b>h</b>) von Mises stress (Method 4).</p>
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<p>Surface plots for computed Cauchy and von Mises stress by different simulation methods and boundary capturing methods for 3-point rubber beam bending test: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> <mo> </mo> <mo> </mo> </mrow> </semantics></math> (Method 1), (<b>b</b>) von Mises stress (Method 1), (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 2), (<b>d</b>) von Mises stress (Method 2), (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 3), (<b>f</b>) von Mises stress (Method 3), (<b>g</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>x</mi> <mi>y</mi> </mrow> </msub> </mrow> </semantics></math> (Method 4), (<b>h</b>) von Mises stress (Method 4).</p>
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<p>Convergence behavior of <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>L</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math> norms error (semi-log scale) for 3-point bending BVP according to various boundary capturing options such as strain model, regression function degree, and boundary capturing data source: (<b>a</b>) ANSYS-model-based boundary capturing (Methods 1 and 2); (<b>b</b>) digital-image-based boundary capturing (Method 3 and 4).</p>
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20 pages, 1495 KiB  
Article
A Distributed Energy-Throughput Efficient Cross-Layer Framework Using Hybrid Optimization Algorithm
by Pratap Singh, Nitin Mittal, Vikas Mittal, Tapankumar Trivedi, Ashish Singh, Szymon Łukasik and Rohit Salgotra
Mathematics 2025, 13(2), 224; https://doi.org/10.3390/math13020224 - 10 Jan 2025
Viewed by 444
Abstract
Magnetic induction (MI)-operated wireless sensor networks (WSNs), due to their similar performance in air, underwater, and underground mediums, are rapidly emerging networks that offer a wide range of applications, including mine prevention, power grid maintenance, underground pipeline monitoring, and upstream oil monitoring. MI-based [...] Read more.
Magnetic induction (MI)-operated wireless sensor networks (WSNs), due to their similar performance in air, underwater, and underground mediums, are rapidly emerging networks that offer a wide range of applications, including mine prevention, power grid maintenance, underground pipeline monitoring, and upstream oil monitoring. MI-based wireless underground sensor networks (WUSNs), utilizing small antenna coils, offer a viable solution by providing consistent channel conditions. The cross-layer protocols address the specific challenges of WUSNs, leading to improved network performance and enhanced operational capabilities in real-world applications. This work proposes a distributed cross-layer solution, leveraging the hybrid marine predator naked mole rat algorithm (MPNMRA) for MI-operated WUSNs. The solution, called DECMN (distributed energy-throughput efficient cross-layer network using MPNMRA), is designed to optimize the MI communication channels, MI relay coils (MI waveguide), and MI waveguide with 3D coils to fulfill quality of service (QoS) parameters, while achieving energy savings and throughput gains. DECMN utilizes the interactions between various layers to develop cross-layer protocols based on MPNMRA. Simulation results demonstrate the effectiveness of DECMN, offering energy savings, increased throughput, and reliable transmissions within the performance limits. Full article
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<p>Flowchart of MPNMRA algorithm.</p>
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<p>Structure of direct MI communication [<a href="#B22-mathematics-13-00224" class="html-bibr">22</a>].</p>
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<p>Structure of MI waveguide technique [<a href="#B22-mathematics-13-00224" class="html-bibr">22</a>].</p>
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<p>Structure of MI waveguide with 3D coils [<a href="#B22-mathematics-13-00224" class="html-bibr">22</a>].</p>
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