[go: up one dir, main page]
More Web Proxy on the site http://driver.im/
You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (1,202)

Search Parameters:
Keywords = network lifetime

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
22 pages, 4303 KiB  
Article
Extending WSN Lifetime with Enhanced LEACH Protocol in Autonomous Vehicle Using Improved K-Means and Advanced Cluster Configuration Algorithms
by Cheolhee Yoon, Seongsoo Cho and Yeonwoo Lee
Appl. Sci. 2024, 14(24), 11720; https://doi.org/10.3390/app142411720 - 16 Dec 2024
Viewed by 331
Abstract
In this paper, we propose an enhanced clustering protocol that integrates an improved K-means with a Mobility-Aware Cluster Head-Election Scored (IK-MACHES) algorithm, designed for extending the lifetime and operational efficiency of Wireless Sensor Network (WSN) with mobility. Variety approaches applying Low Energy Adaptive [...] Read more.
In this paper, we propose an enhanced clustering protocol that integrates an improved K-means with a Mobility-Aware Cluster Head-Election Scored (IK-MACHES) algorithm, designed for extending the lifetime and operational efficiency of Wireless Sensor Network (WSN) with mobility. Variety approaches applying Low Energy Adaptive Clustering Hierarchy (LEACH) often struggle to manage optimal energy distribution due to their static clustering and limited cluster head (CH) selection criteria, primarily focusing on the proximity of residual energy or distance. Thus, this paper proposes an algorithm that takes into account both the residual energy of sensor nodes and the distance between the cluster’s central point to the base station (BS), which ultimately enhances the network’s lifetime. Additionally, our approach incorporates mobility considerations, enhancing the adaptability of the mobility environments, such as autonomous vehicular networks. Our proposed method first constructs the cluster’s configuration and then elects the CH applying an improved K-means clustering algorithm—one of the machine learning methods—integrated with a proposed IK-MACHES mechanism. Three CH scoring strategies in the proposed IK-MACHES protocol evaluate the residual energy of the nodes, their distance to the BS and the cluster central point, and relative node’s mobility. The simulation results demonstrate that the proposed approach improves performance in terms of the first node dead (FND) and 80% alive nodes metrics with mobility, compared to other LEACH protocols such as classical LEACH, LEACH-B, Improved-LEACH, LEACH with K-means, Particle Swarm Optimization (PSO), and LEACH-GK protocol, thereby enhancing network lifetime through optimal CH selection. Full article
Show Figures

Figure 1

Figure 1
<p>The formation for the cluster round in the LEACH protocol and the architecture of LEACH for the WSN.</p>
Full article ">Figure 2
<p>An illustration of the 200 <math display="inline"><semantics> <mrow> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math> network area simulation setup with distributed sensor nodes, the CH, and the BS and the autonomous vehicle with a sensor node for each scenario; the BS location at (100 m, 300 m) for Scenario 1 and at (100 m, 100 m) for Scenario 2.</p>
Full article ">Figure 3
<p>Clustering results with distributed sensor nodes, CHs, and BS, after initial K-means clustering simulation for each scenario; BS location at (100 m, 300 m) for Scenario 1 and at (100 m, 100 m) for Scenario 2, respectively.</p>
Full article ">Figure 4
<p>Clustering and alive sensor nodes’ map for a BS located at (100 m, 300 m) scenario; showing the decline to 80, 50, and 20 active nodes at rounds 262, 569, and 1003, respectively.</p>
Full article ">Figure 5
<p>Clustering and alive sensor nodes’ map for a BS located at (100 m, 100 m) scenario; showing the decline to 80, 50, and 20 active nodes at rounds 1443, 1621, and 1702, respectively.</p>
Full article ">Figure 6
<p>Simulation result of network lifetime with alive nodes graph for each round with no mobility: (<b>a</b>) Scenario 1 (BS = 100 m, 300 m), (<b>b</b>) Scenario 2 (BS = 100 m, 100 m).</p>
Full article ">Figure 7
<p>The simulation result of the network lifetime with an alive node graph for each round, with a maximum mobility range of up to 10 m/round: (<b>a</b>) Scenario 1 (BS = 100 m, 300 m), (<b>b</b>) Scenario 2 (BS = 100 m, 100 m).</p>
Full article ">Figure 8
<p>Comparison of residual energy of nodes after 100 rounds, 500 rounds, and 1000 rounds for Scenario 1 (BS = 100 m, 300 m) with mobility: (<b>a</b>) no mobility and (<b>b</b>) maximum mobility range (10 m/round), depicting how energy sustainability varies by scenario.</p>
Full article ">Figure 9
<p>Comparison of residual energy of nodes after 100 rounds, 500 rounds, and 1000 rounds for Scenario 2 (BS = 100 m, 100 m) with mobility: (<b>a</b>) no mobility and (<b>b</b>) maximum mobility range (10 m/round), depicting how energy sustainability varies by scenario.</p>
Full article ">
19 pages, 3900 KiB  
Article
Contrastive Clustering-Based Patient Normalization to Improve Automated In Vivo Oral Cancer Diagnosis from Multispectral Autofluorescence Lifetime Images
by Kayla Caughlin, Elvis Duran-Sierra, Shuna Cheng, Rodrigo Cuenca, Beena Ahmed, Jim Ji, Mathias Martinez, Moustafa Al-Khalil, Hussain Al-Enazi, Javier A. Jo and Carlos Busso
Cancers 2024, 16(23), 4120; https://doi.org/10.3390/cancers16234120 - 9 Dec 2024
Viewed by 537
Abstract
Background: Multispectral autofluorescence lifetime imaging systems have recently been developed to quickly and non-invasively assess tissue properties for applications in oral cancer diagnosis. As a non-traditional imaging modality, the autofluorescence signal collected from the system cannot be directly visually assessed by a clinician [...] Read more.
Background: Multispectral autofluorescence lifetime imaging systems have recently been developed to quickly and non-invasively assess tissue properties for applications in oral cancer diagnosis. As a non-traditional imaging modality, the autofluorescence signal collected from the system cannot be directly visually assessed by a clinician and a model is needed to generate a diagnosis for each image. However, training a deep learning model from scratch on small multispectral autofluorescence datasets can fail due to inter-patient variability, poor initialization, and overfitting. Methods: We propose a contrastive-based pre-training approach that teaches the network to perform patient normalization without requiring a direct comparison to a reference sample. We then use the contrastive pre-trained encoder as a favorable initialization for classification. To train the classifiers, we efficiently use available data and reduce overfitting through a multitask framework with margin delineation and cancer diagnosis tasks. We evaluate the model over 67 patients using 10-fold cross-validation and evaluate significance using paired, one-tailed t-tests. Results: The proposed approach achieves a sensitivity of 82.08% and specificity of 75.92% on the cancer diagnosis task with a sensitivity of 91.83% and specificity of 79.31% for margin delineation as an auxiliary task. In comparison to existing approaches, our method significantly outperforms a support vector machine (SVM) implemented with either sequential feature selection (SFS) (p = 0.0261) or L1 loss (p = 0.0452) when considering the average of sensitivity and specificity. Specifically, the proposed approach increases performance by 2.75% compared to the L1 model and 4.87% compared to the SFS model. In addition, there is a significant increase in specificity of 8.34% compared to the baseline autoencoder model (p = 0.0070). Conclusions: Our method effectively trains deep learning models for small data applications when existing, large pre-trained models are not suitable for fine-tuning. While we designed the network for a specific imaging modality, we report the development process so that the insights gained can be applied to address similar challenges in other non-traditional imaging modalities. A key contribution of this paper is a neural network framework for multi-spectral fluorescence lifetime-based tissue discrimination that performs patient normalization without requiring a reference (healthy) sample from each patient at test time. Full article
(This article belongs to the Section Cancer Causes, Screening and Diagnosis)
Show Figures

Figure 1

Figure 1
<p>Approach overview. Step 1 (<b>A</b>–<b>C</b>)—input pixel-level training data (see example pixel panels (<b>B</b>,<b>F</b>)) into the encoder and train using contrastive loss. After step 1 pre-training, the bottleneck representation shows the clustering of each class (see bottleneck representation Panel (<b>G</b>)). Step 2 (<b>D</b>,<b>E</b>)—add pixel-level classifiers and train with categorical cross-entropy losses. Aggregate all pixel-level labels from a single image using a 50% threshold to label each image.</p>
Full article ">Figure 2
<p>The network structure of the proposed architecture.</p>
Full article ">Figure 3
<p>Contrastive training with synthetic data. The clustering and separation losses work together to separate the classes. Each component functions alone as expected when batch normalization is used. (<b>a</b>) Synthetic 2 class training data. (<b>b</b>) After: Clust. and Sep. losses with batch norm. (<b>c</b>) Single class clustering result. (<b>d</b>) Single class clustering loss. (<b>e</b>) Sep. loss collapse w/o batch norm. (<b>f</b>) Sep. loss training curve w/o batch norm. (<b>g</b>) Sep. loss only training w/batch norm. (<b>h</b>) Separation loss curve with batch norm.</p>
Full article ">Figure 4
<p>Contrastive training with three classes. All three classes were separable after using the adaptive weighting scheme. (<b>a</b>) Synthetic 3 class training data. (<b>b</b>) Final result using clustering and separation losses without adaptive weighting. (<b>c</b>) Final result using clustering and separation losses with adaptive weighting.</p>
Full article ">Figure 5
<p>Loss functions for contrastive training with three classes. Each component of the loss function is more stable with the adaptive weighting. (<b>a</b>) Training losses without adaptive weighting. (<b>b</b>) Training losses with adaptive weighting.</p>
Full article ">Figure 6
<p>Two-dimensional (2D) contrastive feature space representation and silhouette scores during pre-training. The shapes represent each class. The stars represent healthy samples. The circles represent malignant samples. The squares represent benign samples. The cool colors represent samples from patients with benign lesions, while the warm colors represent samples from patients with malignant lesions. The shades of warm and cool colors help differentiate between tightly clustered patients, but have no additional meaning.</p>
Full article ">
24 pages, 2735 KiB  
Article
Research on High-Efficiency Routing Protocols for HWSNs Based on Deep Reinforcement Learning
by Yu Song, Zhigui Liu, Kunran Li, Xiaoli He and Weizhuo Zhu
Electronics 2024, 13(23), 4746; https://doi.org/10.3390/electronics13234746 - 30 Nov 2024
Viewed by 445
Abstract
In heterogeneous wireless sensor networks (HWSNs), optimizing energy efficiency presents significant challenges due to variations in node energy levels and the complexity of the network environment. This paper introduces an energy efficiency optimization algorithm for HWSNs based on the Deep Q-Network (HDQN). The [...] Read more.
In heterogeneous wireless sensor networks (HWSNs), optimizing energy efficiency presents significant challenges due to variations in node energy levels and the complexity of the network environment. This paper introduces an energy efficiency optimization algorithm for HWSNs based on the Deep Q-Network (HDQN). The algorithm aims to address these challenges by selecting the optimal information transmission path. The HDQN leverages energy differences between nodes and real-time environmental data to enhance network efficiency. Its reward function takes into account node distance, remaining energy, and relay node count to balance node participation and minimize overall energy consumption. The Deep Q-Network (DQN) uses the mean squared error for precise reward estimation, and an improved packet header structure supports effective routing decisions. Simulation results show that the HDQN significantly outperforms existing algorithms—EEHCHR, 2L-HMGEAR, NCOGA, DEEC, and SEP—in terms of energy efficiency, network lifetime, and robustness, demonstrating its potential to advance the performance of HWSNs. The research results of the paper provide a theoretical basis for future energy efficiency research in wireless communication and contribute to the study of the new generation of wireless networks. Full article
(This article belongs to the Special Issue Applications of Sensor Networks and Wireless Communications)
Show Figures

Figure 1

Figure 1
<p>Application scenario of HWSNs in smart agriculture.</p>
Full article ">Figure 2
<p>System model of HWSNs.</p>
Full article ">Figure 3
<p>Deep reinforcement learning process.</p>
Full article ">Figure 4
<p>HWSNs system model for clustering data transmission based on DQN.</p>
Full article ">Figure 5
<p>Flowchart of HDQN algorithm.</p>
Full article ">Figure 6
<p>Improved HDQN algorithm packet header.</p>
Full article ">Figure 7
<p>Comparison of simulation experiments on the number of surviving nodes in HWSNs.</p>
Full article ">Figure 8
<p>Comparison of average remaining energy of nodes in HWSNs.</p>
Full article ">Figure 9
<p>Comparison of total energy consumption in HWSNs.</p>
Full article ">Figure 10
<p>Comparative chart of total energy consumption in HWSNs with varying BS positions.</p>
Full article ">Figure 11
<p>Simulation experiment of remaining energy with varying node numbers in HWSNs.</p>
Full article ">Figure 12
<p>Simulation of transmission counts with free-space energy model in HWSNs.</p>
Full article ">
23 pages, 5895 KiB  
Article
Energy-Efficient Data Fusion in WSNs Using Mobility-Aware Compression and Adaptive Clustering
by Emad S. Hassan, Marwa Madkour, Salah E. Soliman, Ahmed S. Oshaba, Atef El-Emary, Ehab S. Ali and Fathi E. Abd El-Samie
Technologies 2024, 12(12), 248; https://doi.org/10.3390/technologies12120248 - 28 Nov 2024
Viewed by 830
Abstract
To facilitate energy-efficient information dissemination from multiple sensors to the sink within Wireless Sensor Networks (WSNs), in-network data fusion is imperative. This paper presents a new WSN topology that incorporates the Mobility-Efficient Data Fusion (MEDF) algorithm, which integrates a data-compression protocol with an [...] Read more.
To facilitate energy-efficient information dissemination from multiple sensors to the sink within Wireless Sensor Networks (WSNs), in-network data fusion is imperative. This paper presents a new WSN topology that incorporates the Mobility-Efficient Data Fusion (MEDF) algorithm, which integrates a data-compression protocol with an adaptive-clustering mechanism. The primary goals of this topology are, first, to determine a dynamic sequence of cluster heads (CHs) for each data transmission round, aiming to prolong network lifetime by implementing an adaptive-clustering mechanism resilient to network dynamics, where CH selection relies on residual energy and minimal communication distance; second, to enhance packet delivery ratio (PDR) through the application of a data-compression technique; and third, to mitigate the hot-spot issue, wherein sensor nodes nearest to the base station endure higher relay burdens, consequently influencing network longevity. To address this issue, mobility models provide a straightforward solution; specifically, a Random Positioning of Grid Mobility (RPGM) model is employed to alleviate the hot-spot problem. The simulation results show that the network topology incorporating the proposed MEDF algorithm effectively enhances network longevity, optimizes average energy consumption, and improves PDR. Compared to the Energy-Efficient Multiple Data Fusion (EEMDF) algorithm, the proposed algorithm demonstrates enhancements in PDR and energy efficiency, with gains of 5.2% and 7.7%, respectively. Additionally, it has the potential to extend network lifetime by 13.9%. However, the MEDF algorithm increases delay by 0.01% compared to EEMDF. The proposed algorithm is also evaluated against other algorithms, such as the tracking-anchor-based clustering method (TACM) and Energy-Efficient Dynamic Clustering (EEDC), the obtained results emphasize the MEDF algorithm’s ability to conserve energy more effectively than the other algorithms. Full article
(This article belongs to the Special Issue Perpetual Sensor Nodes for Sustainable Wireless Network Applications)
Show Figures

Figure 1

Figure 1
<p>The main steps of MEDF algorithm.</p>
Full article ">Figure 2
<p>Proposed cluster-formation algorithm.</p>
Full article ">Figure 3
<p>Data fusion steps.</p>
Full article ">Figure 4
<p>LWT procedures.</p>
Full article ">Figure 5
<p>Multi-level LWT procedures.</p>
Full article ">Figure 6
<p>Visual representation of distributed encoding.</p>
Full article ">Figure 7
<p>Visual representation of joint encoding.</p>
Full article ">Figure 8
<p>Multi-path routing from source at CH4 to BS.</p>
Full article ">Figure 9
<p>PDR of MEDF and EEMDF [<a href="#B27-technologies-12-00248" class="html-bibr">27</a>] algorithms using RW mobility technique.</p>
Full article ">Figure 10
<p>PDR of MEDF and EEMDF [<a href="#B27-technologies-12-00248" class="html-bibr">27</a>] algorithms using RPGM mobility technique.</p>
Full article ">Figure 11
<p>Network lifetime using RW mobility technique.</p>
Full article ">Figure 12
<p>Network lifetime using RPGM mobility technique.</p>
Full article ">Figure 13
<p>AEC using RW mobility technique.</p>
Full article ">Figure 14
<p>AEC using the RPGM mobility technique.</p>
Full article ">Figure 15
<p>Average delay using RW mobility technique.</p>
Full article ">Figure 16
<p>Average delay using RPGM mobility technique.</p>
Full article ">Figure 17
<p>Average residual energy versus number of rounds for the considered algorithms.</p>
Full article ">Figure 18
<p>Network lifetime versus number of nodes: (<b>a</b>) First Dead Node, (<b>b</b>) Half Dead Node, and (<b>c</b>) Last Dead Node.</p>
Full article ">
21 pages, 2310 KiB  
Article
K-Means Based Bee Colony Optimization for Clustering in Heterogeneous Sensor Network
by Prince Modey, Gaddafi Abdul-Salaam, Emmanuel Freeman, Patrick Acheampong, William Leslie Brown-Acquaye, Israel Edem Agbehadji and Richard C. Millham
Sensors 2024, 24(23), 7603; https://doi.org/10.3390/s24237603 - 28 Nov 2024
Viewed by 507
Abstract
In Wireless Sensor Networks (WSNs), an efficient clustering technique is critical in optimizing the energy level of networked sensors and prolonging the network lifetime. While the traditional bee colony optimization technique has been widely used as a clustering technique in WSN, it mostly [...] Read more.
In Wireless Sensor Networks (WSNs), an efficient clustering technique is critical in optimizing the energy level of networked sensors and prolonging the network lifetime. While the traditional bee colony optimization technique has been widely used as a clustering technique in WSN, it mostly suffers from energy efficiency and network performance. This study proposes a Bee Colony Optimization that synergistically combines K-mean algorithms (referred to as K-BCO) for efficient clustering in heterogeneous sensor networks. This is to develop a robust and efficient clustering algorithm that addresses the challenges of energy consumption and network performance in WSNs. The K-BCO algorithm outperformed comparative clustering algorithms such as H-LEACH, DBCP, and ABC-ACO in average error rate (AER), average data delivery rate (ADDR), and average energy consumption (AEC) for transmitting data packets from sensors to cluster heads. The K-BCO outperformed other algorithms in terms of ADDR at 95.00% against H-LEACH (75.86%), DBCP (72.07%) and ABC-ACO (90.08%). The findings indicate that the K-BCO not only optimizes energy consumption but also guarantees more stable and robust solutions, thereby extending the network lifetime of WSNs. Thus, K-BCO is recommended to practitioners in wireless sensor networks as it paves the way for more efficient and sustainable wireless communication. Full article
(This article belongs to the Special Issue Advanced Applications of WSNs and the IoT—2nd Edition)
Show Figures

Figure 1

Figure 1
<p>The Flowchart of the Proposed K-BCO Algorithm.</p>
Full article ">Figure 2
<p>Simulation of sensors, cluster heads, cluster centers and base stations within the 400-m square area.</p>
Full article ">Figure 3
<p>Data delivery rates of K-BCO over 20 iterations.</p>
Full article ">Figure 4
<p>Energy consumption of K-BCO over 20 iterations.</p>
Full article ">Figure 5
<p>Average execution time of K-BCO over 20 iterations.</p>
Full article ">Figure 6
<p>Average data delivery rates of the proposed K-BCO comparison with H-LEACH, DBCP and ABC-ACO.</p>
Full article ">Figure 7
<p>Average energy cost of the proposed K-BCO comparison with H-LEACH, DBCP and ABC-ACO.</p>
Full article ">Figure 8
<p>Execution time of the proposed K-BCO comparison with H-LEACH, DBCP and ABC-ACO.</p>
Full article ">
20 pages, 4101 KiB  
Article
IEEE 802.15.6 and LoRaWAN for WBAN in Healthcare: A Comparative Study on Communication Efficiency and Energy Optimization
by Soleen Jaladet Al-Sofi, Salih Mustafa S. Atroshey and Ismail Amin Ali
Computers 2024, 13(12), 313; https://doi.org/10.3390/computers13120313 - 26 Nov 2024
Viewed by 656
Abstract
Wireless body area networks (WBANs), which continually gather and transmit patient health data in real time, are essential for improving healthcare administration. Patient outcomes can be improved by sending these data to medical professionals for prompt review and treatment. For the effective deployment [...] Read more.
Wireless body area networks (WBANs), which continually gather and transmit patient health data in real time, are essential for improving healthcare administration. Patient outcomes can be improved by sending these data to medical professionals for prompt review and treatment. For the effective deployment of WBANs, communication solutions are necessary to maximize critical performance parameters, such as low power consumption, minimal delay, and acceptable data rates, while guaranteeing dependable transmission. Two prominent technologies in this field are LoRaWAN, which is renowned for its long-range capabilities and energy efficiency, and IEEE 802.15.6, which was created especially for short-range medical applications with high data throughput. This study provides a comparative evaluation of these two technologies to determine their suitability for diverse WBAN healthcare scenarios. By using the NS3, a simulation was performed to calculate six key performance metrics: throughput, arrival rate, delay, energy consumption, packet delivery ratio (PDR), and network lifetime. The study analyzed each technology’s performance under varying node counts. At a density of 50 nodes, IEEE 802.15.6 demonstrated superior throughput, with 45 kbps, compared to LoRaWAN, and a higher PDR of 30%. Additionally, IEEE 802.15.6 showed a higher arrival rate, of 0.33%, than LoRaWAN. On the other hand, LoRaWAN showed notable strengths in energy consumption, with only 42 J, compared to IEEE 802.15.6, and significantly lower delay, with a delay of 7 s. Additionally, LoRaWAN offered an extended network lifetime, of 18 h, compared to IEEE 802.15.6. Full article
Show Figures

Figure 1

Figure 1
<p>Bandwidth-range characteristics of different wireless technologies.</p>
Full article ">Figure 2
<p>Three-tier architecture for WBAN.</p>
Full article ">Figure 3
<p>Network topology of the IEEE 802.15.6 network.</p>
Full article ">Figure 4
<p>IEEE 802.15.6 flowchart using CSMA/CA.</p>
Full article ">Figure 5
<p>Network topology of LoRaWAN.</p>
Full article ">Figure 6
<p>Flowchart of the LoRaWAN transmitter module.</p>
Full article ">Figure 7
<p>Average throughput changes across the number of nodes.</p>
Full article ">Figure 8
<p>Average arrival rate changes across the number of nodes.</p>
Full article ">Figure 9
<p>Average delay changes across the number of nodes.</p>
Full article ">Figure 10
<p>Average energy consumption changes across the number of nodes.</p>
Full article ">Figure 11
<p>Average packet delivery ratio changes across the number of nodes.</p>
Full article ">Figure 12
<p>Average network lifetime changes across the number of nodes.</p>
Full article ">
17 pages, 403 KiB  
Article
Enhancing Stability and Efficiency in Mobile Ad Hoc Networks (MANETs): A Multicriteria Algorithm for Optimal Multipoint Relay Selection
by Ayoub Abdellaoui, Yassine Himeur, Omar Alnaseri, Shadi Atalla, Wathiq Mansoor, Jamal Elmhamdi and Hussain Al-Ahmad
Information 2024, 15(12), 753; https://doi.org/10.3390/info15120753 - 26 Nov 2024
Viewed by 497
Abstract
Mobile ad hoc networks (MANETs) are autonomous systems composed of multiple mobile nodes that communicate wirelessly without relying on any pre-established infrastructure. These networks operate in highly dynamic environments, which can compromise their ability to guarantee consistent link lifetimes, security, reliability, and overall [...] Read more.
Mobile ad hoc networks (MANETs) are autonomous systems composed of multiple mobile nodes that communicate wirelessly without relying on any pre-established infrastructure. These networks operate in highly dynamic environments, which can compromise their ability to guarantee consistent link lifetimes, security, reliability, and overall stability. Factors such as mobility, energy availability, and security critically influence network performance. Consequently, the selection of paths and relay nodes that ensure stability, security, and extended network lifetimes is fundamental in designing routing protocols for MANETs. This selection is pivotal in maintaining robust network operations and optimizing communication efficiency. This paper introduces a sophisticated algorithm for selecting multipoint relays (MPRs) in MANETs, addressing the challenges posed by node mobility, energy constraints, and security vulnerabilities. By employing a multicriteria-weighted technique that assesses the mobility, energy levels, and trustworthiness of mobile nodes, the proposed approach enhances network stability, reachability, and longevity. The enhanced algorithm is integrated into the Optimized Link State Routing Protocol (OLSR) and validated through NS3 simulations, using the Random Waypoint and ManhattanGrid mobility models. The results indicate superior performance of the enhanced algorithm over traditional OLSR, particularly in terms of packet delivery, delay reduction, and throughput in dynamic network conditions. This study not only advances the design of routing protocols for MANETs but also significantly contributes to the development of robust communication frameworks within the realm of smart mobile communications. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Multipoint relays illustration.</p>
Full article ">Figure 2
<p>Modified multipoint relays illustration.</p>
Full article ">Figure 3
<p>Mean Delay comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 4
<p>Mean Jitter comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 5
<p>PLR comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 6
<p>PDR comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 7
<p>Lost Packets comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 8
<p>Throughput comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 9
<p>Mean Delay comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 10
<p>Mean Jitter comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 11
<p>PLR comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 12
<p>PDR comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 13
<p>Lost Packets comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">Figure 14
<p>Throughput comparison between MCW_OLSR, OLSR, DSDV, and SR_OLSR.</p>
Full article ">
24 pages, 1660 KiB  
Article
Performance Study of FSO/THz Dual-Hop System Based on Cognitive Radio and Energy Harvesting System
by Jingwei Lu, Rongpeng Liu, Yawei Wang, Ziyang Wang and Hongzhan Liu
Electronics 2024, 13(23), 4656; https://doi.org/10.3390/electronics13234656 - 26 Nov 2024
Viewed by 445
Abstract
In order to address the problems of low spectrum efficiency in current communication systems and extend the lifetime of energy-constrained relay devices, this paper proposes a novel dual-hop free-space optical (FSO) system that integrates cognitive radio (CR) and energy harvesting (EH). In this [...] Read more.
In order to address the problems of low spectrum efficiency in current communication systems and extend the lifetime of energy-constrained relay devices, this paper proposes a novel dual-hop free-space optical (FSO) system that integrates cognitive radio (CR) and energy harvesting (EH). In this system, the source node communicates with two users at the terminal via FSO and terahertz (THz) hard-switching links, as well as a multi-antenna relay for non-orthogonal multiple access (NOMA). There is another link whose relay acts as both the power beacon (PB) in the EH system and the primary network (PN) in the CR system, achieving the double function of auxiliary transmission. In addition, based on the three possible practical working scenarios of the system, three different transmit powers of the relay are distinguished, thus enabling three different working modes of the system. Closed-form expressions are derived for the interruption outage probability per user for these three operating scenarios, considering the Gamma–Gamma distribution for the FSO link, the αμ distribution for the THz link, and the Rayleigh fading distribution for the radio frequency (RF) link. Finally, the numerical results show that this novel system can be adapted to various real-world scenarios and possesses unique advantages. Full article
(This article belongs to the Section Microwave and Wireless Communications)
Show Figures

Figure 1

Figure 1
<p>Hard-switched FSO/THz-RF dual-hop NOMA link with CR and EH.</p>
Full article ">Figure 2
<p>The comparison between different beamwidth and jitter standard deviations versus OPs.</p>
Full article ">Figure 3
<p>The comparison between <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>R</mi> </mrow> </semantics></math> link transmission distances and THz frequency cases versus OP. The first row represent <math display="inline"><semantics> <msub> <mi>U</mi> <mn>1</mn> </msub> </semantics></math>, and the second row represent <math display="inline"><semantics> <msub> <mi>U</mi> <mn>2</mn> </msub> </semantics></math>, respectively.</p>
Full article ">Figure 4
<p>SNR versus OP under the comparison between different visibility.</p>
Full article ">Figure 5
<p>SNR versus OP for different turbulence conditions and pointing errors when <math display="inline"><semantics> <mrow> <mi>L</mi> <mi>F</mi> </mrow> </semantics></math> = <math display="inline"><semantics> <mrow> <mi>D</mi> <mi>T</mi> </mrow> </semantics></math> = 350 m among three working scenarios.</p>
Full article ">Figure 6
<p>OP versus <span class="html-italic">N</span> among three working scenarios.</p>
Full article ">Figure 7
<p>OP versus <math display="inline"><semantics> <mrow> <msub> <mi>g</mi> <mi>u</mi> </msub> <mn>1</mn> </mrow> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mi>ξ</mi> </semantics></math> = 1, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>B</mi> </msub> <mo>/</mo> <msub> <mi>N</mi> <mn>0</mn> </msub> </mrow> </semantics></math> = 2 dB, <math display="inline"><semantics> <mrow> <mi>η</mi> <mo>/</mo> <msub> <mi>P</mi> <mi>B</mi> </msub> </mrow> </semantics></math> =-1.9 dB, <math display="inline"><semantics> <msub> <mi>g</mi> <mrow> <mi>R</mi> <mi>n</mi> <msub> <mi>U</mi> <mn>1</mn> </msub> </mrow> </msub> </semantics></math> = 3 dB, <math display="inline"><semantics> <msub> <mi>g</mi> <mrow> <mi>R</mi> <mi>n</mi> <msub> <mi>U</mi> <mn>2</mn> </msub> </mrow> </msub> </semantics></math> = 5 dB, <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math> = 0.77, and <math display="inline"><semantics> <msub> <mi>γ</mi> <mrow> <mi>S</mi> <mi>R</mi> </mrow> </msub> </semantics></math> = 15 dB.</p>
Full article ">Figure 8
<p>OP versus <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ξ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>B</mi> </msub> <mo>/</mo> <msub> <mi>N</mi> <mn>0</mn> </msub> </mrow> </semantics></math> = 2 dB, <math display="inline"><semantics> <mrow> <mi>η</mi> <mo>/</mo> <msub> <mi>P</mi> <mi>B</mi> </msub> </mrow> </semantics></math> = -1.9 dB, <math display="inline"><semantics> <msub> <mi>g</mi> <mrow> <mi>R</mi> <mi>n</mi> <msub> <mi>U</mi> <mn>1</mn> </msub> </mrow> </msub> </semantics></math> = 3 dB, <math display="inline"><semantics> <msub> <mi>g</mi> <mrow> <mi>R</mi> <mi>n</mi> <msub> <mi>U</mi> <mn>2</mn> </msub> </mrow> </msub> </semantics></math> = 5 dB, <math display="inline"><semantics> <mi>α</mi> </semantics></math> = 2.902, <math display="inline"><semantics> <mi>β</mi> </semantics></math> = 2.510, and <math display="inline"><semantics> <msub> <mi>γ</mi> <mrow> <mi>S</mi> <mi>R</mi> </mrow> </msub> </semantics></math> = 8 dB.</p>
Full article ">Figure 9
<p>OP versus <math display="inline"><semantics> <mrow> <mi>η</mi> <mo>/</mo> <msub> <mi>P</mi> <mi>B</mi> </msub> </mrow> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ξ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>B</mi> </msub> <mo>/</mo> <msub> <mi>N</mi> <mn>0</mn> </msub> </mrow> </semantics></math> = 2 dB, <math display="inline"><semantics> <msub> <mi>g</mi> <mrow> <mi>R</mi> <mi>n</mi> <msub> <mi>U</mi> <mn>1</mn> </msub> </mrow> </msub> </semantics></math> = 3 dB, <math display="inline"><semantics> <msub> <mi>g</mi> <mrow> <mi>R</mi> <mi>n</mi> <msub> <mi>U</mi> <mn>2</mn> </msub> </mrow> </msub> </semantics></math> = 5 dB, <math display="inline"><semantics> <mi>α</mi> </semantics></math>= 2.902, <math display="inline"><semantics> <mi>β</mi> </semantics></math> = 2.510, <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math> = 0.77, and <math display="inline"><semantics> <msub> <mi>γ</mi> <mrow> <mi>S</mi> <mi>R</mi> </mrow> </msub> </semantics></math> = 15 dB.</p>
Full article ">Figure 10
<p>A comparison of the power of the SN network and OP at different <span class="html-italic">I</span>.</p>
Full article ">
15 pages, 3696 KiB  
Article
Impact of Alkali Metals on CeO2-WO3/TiO2 Catalysts for NH3-Selective Catalytic Reduction and Lifetime Prediction of Catalysts
by Mutao Xu, Yuhang Deng, Xingxiu Gao, Qijie Jin, Wei Yan, Liguo Chen, Jian Yang, Jing Song, Changcheng Zhou and Haitao Xu
Molecules 2024, 29(23), 5570; https://doi.org/10.3390/molecules29235570 - 25 Nov 2024
Viewed by 378
Abstract
Ce-based catalysts have been widely used in the removal of nitrogen oxides from industrial flue gas because of their good catalytic performance and environmental friendliness. However, the mechanism of alkali metal poisoning in Ce-based catalysts remains to be further studied. This work involves [...] Read more.
Ce-based catalysts have been widely used in the removal of nitrogen oxides from industrial flue gas because of their good catalytic performance and environmental friendliness. However, the mechanism of alkali metal poisoning in Ce-based catalysts remains to be further studied. This work involves the preparation of the K/Na-poisoned CeWTi catalyst via the impregnation method for assessing its performance in NO removal. Experiments show that both K and Na exhibit detrimental effects on the CeWTi catalyst, and the loading of alkali metal reduces the specific surface area and pore volume of the catalyst. Furthermore, the presence of alkaline metals results in a notable decline in the CeWTi acid concentration, particularly in Lewis acid sites. Concurrently, the levels of Ce3+, oxygen vacancies, and reducing agents on the catalyst surface decrease, leading to diminished reduction capability and eventual catalyst deactivation. The application of a BP neural network for catalyst activity prediction yielded an average relative error of approximately 0.73%, indicating enhanced accuracy in prediction outcomes. This work explored the cause of alkali metal poisoning of the CeWTi catalyst and provided an effective prediction method for the lifetime of CeWTi catalyst, which provided theoretical guidance for the engineering application of Ce-based catalysts. Full article
(This article belongs to the Special Issue Advances in Nano-Catalyst and Single-Atom Catalyst)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) NO conversion over K-CeWTi catalysts, (<b>b</b>) NO conversion of Na-CeWTi catalysts.</p>
Full article ">Figure 2
<p>Fitting deactivation curve of K-poisoned CeWTi catalysts.</p>
Full article ">Figure 3
<p>(<b>a</b>) XRD patterns of as-prepared catalysts, and (<b>b</b>) comparison of XRD patterns of 0.39K-CeWTi and 0.39Na-CeWTi at 20~40°.</p>
Full article ">Figure 4
<p>SEM image of as-prepared catalysts, (<b>a</b>) CeWTi, (<b>b</b>) 0.39K-CeWTi, (<b>c</b>) 0.39Na-CeWTi; TEM image of as-prepared catalysts, (<b>d</b>,<b>g</b>) CeWTi, (<b>e</b>,<b>h</b>) 0.39K-CeWTi, (<b>f</b>,<b>i</b>) 0.39Na-CeWTi.</p>
Full article ">Figure 5
<p>(<b>a</b>) NH<sub>3</sub>-TPD patterns of the as-prepared catalysts, (<b>b</b>) comparison of NH<sub>3</sub>-TPD patterns of 0.39K-CeWTi and 0.39Na-CeWTi, and (<b>c</b>) acid quantity of as-prepared catalysts.</p>
Full article ">Figure 6
<p>(<b>a</b>) H<sub>2</sub>-TPR patterns of the as-prepared catalysts, (<b>b</b>) comparison of H<sub>2</sub>-TPR patterns of 0.39K-CeWTi and 0.39Na-CeWTi, and (<b>c</b>) H<sub>2</sub> consumption of as-prepared catalysts.</p>
Full article ">Figure 7
<p>XPS spectra of the prepared catalysts, (<b>a</b>) Ce 3<span class="html-italic">d</span>, (<b>b</b>) W 4<span class="html-italic">f</span>, and (<b>c</b>) O 1<span class="html-italic">s</span>.</p>
Full article ">Figure 8
<p>Comparison of predicted values and true values of BP neural network test.</p>
Full article ">
23 pages, 6739 KiB  
Article
A Novel Energy Replenishment Algorithm to Increase the Network Performance of Rechargeable Wireless Sensor Networks
by Tariq, Vishwanath Eswarakrishnan, Adil Hussain, Zhu Wei and Muhammad Uzair
Sensors 2024, 24(23), 7491; https://doi.org/10.3390/s24237491 - 24 Nov 2024
Viewed by 504
Abstract
The emerging wireless energy transfer technology enables sensor nodes to maintain perpetual operation. However, maximizing the network performance while preserving short charging delay is a great challenge. In this work, a Wireless Mobile Charger (MC) and a directional charger (DC) were deployed to [...] Read more.
The emerging wireless energy transfer technology enables sensor nodes to maintain perpetual operation. However, maximizing the network performance while preserving short charging delay is a great challenge. In this work, a Wireless Mobile Charger (MC) and a directional charger (DC) were deployed to transmit wireless energy to the sensor node to improve the network’s throughput. To the best of our knowledge, this is the first work to optimize the data sensing rate and charging delay by the joint scheduling of an MC and a DC. We proved we could transmit maximum energy to each sensor node to obtain our optimization objective. In our proposed work, a DC selected a total horizon of 360° and then selected the horizon of each specific 90 area based on its antenna orientation. The DC’s orientation was scheduled for each time slot. Furthermore, multiple MCs were used to transmit energy for sensor nodes that could not be covered by the DC. We divided the rechargeable wireless sensor network into several zones via a Voronoi diagram. We deployed a static DC and one MC charging location in each zone to provide wireless charging service jointly. We obtained the optimal charging locations of the MCs in each zone by solving Mix Integral Programming for energy transmission. The optimization objective of our proposed research was to sense maximum data from each sensor node with the help of maximum energy. The lifetime of each sensor network could increase, and the end delay could be maximized, with joint energy transmission. Extensive simulation results demonstrated that our RWSNs were designed to significantly improve network lifetime over the baseline method. Full article
(This article belongs to the Topic Advances in Wireless and Mobile Networking)
Show Figures

Figure 1

Figure 1
<p>Wireless rechargeable sensor network.</p>
Full article ">Figure 2
<p>Methodology.</p>
Full article ">Figure 3
<p>Algorithm framework.</p>
Full article ">Figure 4
<p>Impact of hop count on tour length.</p>
Full article ">Figure 5
<p>Set of nodes with <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>180</mn> </mrow> <mrow> <mo>∘</mo> </mrow> </msup> </mrow> </semantics></math> coverage area.</p>
Full article ">Figure 6
<p>Different energy consumption levels of each node.</p>
Full article ">Figure 7
<p>Energy consumption rate from initial to final level.</p>
Full article ">Figure 8
<p>Data sensing rate of different nodes.</p>
Full article ">Figure 9
<p>Maximum energy transmission in the maximum timeslot.</p>
Full article ">Figure 10
<p>Highest energy transmission in the highest timeslot.</p>
Full article ">Figure 11
<p>Node coverage area with <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>90</mn> </mrow> <mrow> <mo>∘</mo> </mrow> </msup> </mrow> </semantics></math> angle.</p>
Full article ">Figure 12
<p>Data sensing rate from lowest to highest.</p>
Full article ">Figure 13
<p>Energy consumption rate from highest to lowest.</p>
Full article ">Figure 14
<p>Impact of hop count on tour length.</p>
Full article ">
11 pages, 1330 KiB  
Article
Simulation Studies of the Dynamics and the Connectivity Patterns of Hydrogen Bonds in Water from Ambient to Supercritical Conditions
by Dorota Swiatla-Wojcik
Molecules 2024, 29(23), 5513; https://doi.org/10.3390/molecules29235513 - 21 Nov 2024
Viewed by 544
Abstract
Pressurized high-temperature water attracts attention as a promising medium for chemical synthesis, biomass processing or destruction of hazardous waste. Adjustment to the desired solvent properties requires knowledge on the behavior of populations of hydrogen-bonded molecules. In this work, the interconnection between the hydrogen [...] Read more.
Pressurized high-temperature water attracts attention as a promising medium for chemical synthesis, biomass processing or destruction of hazardous waste. Adjustment to the desired solvent properties requires knowledge on the behavior of populations of hydrogen-bonded molecules. In this work, the interconnection between the hydrogen bond (HB) dynamics and the structural rearrangements of HB networks have been studied by molecular dynamics simulation using the modified central force flexible potential and the HB definition controlling pair interaction energy, HB length and HB angle. Time autocorrelation functions for molecular pairs bonded continuously and intermittently and the corresponding mean lifetimes have been calculated for conditions ranging from ambient to supercritical. A significant reduction in the continuous and intermittent lifetimes has been found between (293 K, 0.1 MPa) and (373 K, 25 MPa) and attributed to the decreasing size of patches embedded in the continuous HB network. The loss of global HB connectivity at ca. (573 K, 10 MPa) and the investigated supercritical conditions do not noticeably affect the HB dynamics. Over the whole temperature range studied, the reciprocal intermittent lifetime follows the transition state theory dependence on temperature with the activation energy of 10.4 kJ/mol. Calculations of the lifetime of molecules that do not form hydrogen bonds indicate that at supercritical temperatures, the role of reactions involving an unbound H2O molecule as a reactant can be enhanced by lowering system density. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Selected normalized time correlation functions of continuous hydrogen bonding calculated for the thermodynamic conditions specified in <a href="#molecules-29-05513-t001" class="html-table">Table 1</a>.</p>
Full article ">Figure 2
<p>Selected normalized time correlation functions of intermittent hydrogen bonding calculated for the thermodynamic conditions specified in <a href="#molecules-29-05513-t001" class="html-table">Table 1</a>.</p>
Full article ">Figure 3
<p>Selected normalized time correlation functions of monomer persistence calculated for the thermodynamic conditions specified in <a href="#molecules-29-05513-t001" class="html-table">Table 1</a>.</p>
Full article ">Figure 4
<p>(<b>a</b>) The reciprocal intermittent lifetime &lt;τ<sub>int</sub>&gt; versus 1000/T (squares) and the non-linear fit to the TST dependence: <math display="inline"><semantics> <mrow> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mn>1</mn> </mrow> <mrow> <mo>&lt;</mo> <msub> <mrow> <mi mathvariant="sans-serif">τ</mi> </mrow> <mrow> <mi mathvariant="normal">i</mi> <mi mathvariant="normal">n</mi> <mi mathvariant="normal">t</mi> </mrow> </msub> <mo>&gt;</mo> </mrow> </mfrac> </mstyle> <mo>=</mo> <msup> <mrow> <mi mathvariant="normal">A</mi> </mrow> <mrow> <mo>′</mo> </mrow> </msup> <mi mathvariant="normal">T</mi> <mo> </mo> <mi mathvariant="normal">e</mi> <mi mathvariant="normal">x</mi> <mi mathvariant="normal">p</mi> <mfenced separators="|"> <mrow> <mo>−</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <msup> <mrow> <mi mathvariant="normal">E</mi> </mrow> <mrow> <mo>≠</mo> </mrow> </msup> </mrow> <mrow> <mi mathvariant="normal">R</mi> <mi mathvariant="normal">T</mi> </mrow> </mfrac> </mstyle> </mrow> </mfenced> </mrow> </semantics></math> [A′ = 0.032 ps<sup>−1</sup>; E<sup>≠</sup> = 10.4 kJ/mol; Adj. R-square = 0.998] (red curve). (<b>b</b>) Temperature dependence of the average continuous lifetime of HBs &lt;τ<sub>c</sub>&gt; (squares) and the average lifetime of monomers &lt;τ<sub>nb</sub>&gt; (triangles). Lifetimes calculated for sub- and super-critical conditions are shown by blue squares and green triangles.</p>
Full article ">Figure 5
<p>The calculated HB lifetimes versus the mean number of HBs per molecule (&lt;n<sub>HB</sub>&gt;): (black points and left axis)—intermittent; (red points and right scale)—continuous. Lifetimes calculated for sub- and super-critical conditions are shown by open squares. Inset: the dependence of a degree of connectivity (P<sub>g</sub>) defined as the total fraction of molecules engaged in the clusters of at least five hydrogen-bonded molecules [<a href="#B8-molecules-29-05513" class="html-bibr">8</a>]. The dashed line at &lt;n<sub>HB</sub>&gt; ~ 1.9 indicates breakage of the continuous HB network (right) into a variety of statistically independent clusters (left).</p>
Full article ">Figure 6
<p>Persistence of non-bonded molecules (monomers) as a function of the mean number of HBs per molecule (&lt;n<sub>HB</sub>&gt;). Open squares correspond to sub- and super-critical conditions. Inset: the dependence of a degree of connectivity P<sub>g</sub> on &lt;n<sub>HB</sub>&gt; as in <a href="#molecules-29-05513-f005" class="html-fig">Figure 5</a>.</p>
Full article ">
24 pages, 33437 KiB  
Article
Global Assessment of Mesoscale Eddies with TOEddies: Comparison Between Multiple Datasets and Colocation with In Situ Measurements
by Artemis Ioannou, Lionel Guez, Rémi Laxenaire and Sabrina Speich
Remote Sens. 2024, 16(22), 4336; https://doi.org/10.3390/rs16224336 - 20 Nov 2024
Viewed by 619
Abstract
The present study introduces a comprehensive, open-access atlas of mesoscale eddies in the global ocean, as identified and tracked by the TOEddies algorithm implemented on a global scale. Unlike existing atlases, TOEddies detects eddies directly from absolute dynamic topography (ADT) without spatial filtering, [...] Read more.
The present study introduces a comprehensive, open-access atlas of mesoscale eddies in the global ocean, as identified and tracked by the TOEddies algorithm implemented on a global scale. Unlike existing atlases, TOEddies detects eddies directly from absolute dynamic topography (ADT) without spatial filtering, preserving the natural spatial variability and enabling precise, high-resolution tracking of eddy dynamics. This dataset provides daily information on eddy characteristics, such as size, intensity, and polarity, over a 30-year period (1993–2023), capturing complex eddy interactions, including splitting and merging events that often produce networks of interconnected eddies. This unique approach challenges the traditional single-trajectory perspective, offering a nuanced view of eddy life cycles as dynamically linked trajectories. In addition to traditional metrics, TOEddies identifies both the eddy core (characterized by maximum azimuthal velocity) and the outer boundary, offering a detailed representation of eddy structure and enabling precise comparisons with in situ data. To demonstrate its value, we present a statistical overview of eddy characteristics and spatial distributions, including generation, disappearance, and merging/splitting events, alongside a comparative analysis with existing global eddy datasets. Among the multi-year observations, TOEddies captures coherent, long-lived eddies with lifetimes exceeding 1.5 years, while highlighting significant differences in the dynamic properties and spatial patterns across datasets. Furthermore, this study integrates TOEddies with 23 years of colocalized Argo profile data (2000–2023), allowing for a novel examination of eddy-induced subsurface variability and the role of mesoscale eddies in the transport of global ocean heat and biogeochemical properties. This atlas aims to be a valuable resource for the oceanographic community, providing an open dataset that can support diverse applications in ocean dynamics, climate research, and marine resource management. Full article
(This article belongs to the Special Issue Recent Advances on Oceanic Mesoscale Eddies II)
Show Figures

Figure 1

Figure 1
<p>Frequency maps of first (<b>a</b>–<b>d</b>) and last (<b>e</b>–<b>h</b>) detection points of mesoscale eddies per year derived from TOEddies, META3.2, TIAN, and GOMEAD datasets, respectively. The data are aggregated into <math display="inline"><semantics> <mrow> <msup> <mn>1</mn> <mo>∘</mo> </msup> <mo>×</mo> <msup> <mn>1</mn> <mo>∘</mo> </msup> </mrow> </semantics></math> bins and normalized by the number of observation years for each dataset. The mean dynamic topography (MDT; in cm) is shown by black contours.</p>
Full article ">Figure 2
<p>Scatter plot representing the distribution of eddy occurrences for (<b>a</b>) merging and (<b>b</b>) splitting events based on TOEddies atlas for eddies with lifetimes longer than 4 weeks in each <math display="inline"><semantics> <mrow> <msup> <mn>1</mn> <mo>∘</mo> </msup> <mo>×</mo> <msup> <mn>1</mn> <mo>∘</mo> </msup> </mrow> </semantics></math> region. Bathymetric contours at −500 m, −1000 m, −2000 m, and −4000 m are indicated by gray lines.</p>
Full article ">Figure 3
<p>Histograms of eddy lifetimes (weeks) (<b>a</b>,<b>b</b>) and histograms of eddy characteristic radius <math display="inline"><semantics> <msub> <mi>R</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math> (km) (<b>c</b>,<b>d</b>) and velocity <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math> (m/s) (<b>e</b>,<b>f</b>) of anticyclonic (first column) and cyclonic eddies (second column) for the TOEddies, META3.2, TIAN, and GOMEAD datasets. We consider only mesoscale eddies having lifetimes ≥ 16 weeks, as indicated by the dashed lines in panels (<b>a</b>–<b>d</b>), and characteristic radii larger than <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> <mo>≥</mo> </mrow> </semantics></math> 30 km.</p>
Full article ">Figure 4
<p>Maps of the speed-based radius scale <math display="inline"><semantics> <msub> <mi>R</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math> (km) for eddies with lifetimes ≥ 16 weeks for each <math display="inline"><semantics> <mrow> <msup> <mn>1</mn> <mo>∘</mo> </msup> <mo>×</mo> <msup> <mn>1</mn> <mo>∘</mo> </msup> </mrow> </semantics></math> region from the (<b>a</b>) TOEddies, (<b>b</b>) META3.2, (<b>c</b>) TIAN, and (<b>d</b>) GOMEAD datasets. Zonal averages of the eddy characteristic radius are illustrated in panel (<b>e</b>). The dashed line indicates the estimated first baroclinic Rossby radius of deformation <math display="inline"><semantics> <msub> <mi>R</mi> <mi>d</mi> </msub> </semantics></math> (km) [<a href="#B10-remotesensing-16-04336" class="html-bibr">10</a>].</p>
Full article ">Figure 5
<p>Cyclonic (blue) and anticyclonic (red) eddy trajectories as detected from the TOEddies algorithm having lifetimes of at least (<b>a</b>) ≥52 weeks, (<b>b</b>) ≥78 weeks, and (<b>c</b>) ≥104 weeks. The numbers of detected eddies are labeled at the top of each panel for each polarity.</p>
Full article ">Figure 6
<p>Trajectories of long-lived (≥78 weeks) cyclonic (blue) and anticyclonic (red) eddies from the (<b>a</b>) TOEddies, (<b>b</b>) META3.2, (<b>c</b>) TIAN, and (<b>d</b>) GOMEAD datasets. The numbers of eddies are labeled at the top of each panel for each polarity.</p>
Full article ">Figure 7
<p>Trajectories of long-propagating (≥1100 km) eddies of both types from the (<b>a</b>) TOEddies, (<b>b</b>) META3.2, (<b>c</b>) TIAN, and (<b>d</b>) GOMEAD datasets tracked for ≥26 weeks.</p>
Full article ">Figure 8
<p>Eddy-network example of anticyclonic (first column) and cyclonic (second column) trajectories for the (<b>a</b>,<b>b</b>) California Upwelling System, (<b>c</b>,<b>d</b>) western Australian boundary, and (<b>e</b>,<b>f</b>) extended South Benguela System. Each eddy trajectory is colored according to its assigned order.</p>
Full article ">Figure 9
<p>Temporal evolution of dynamical characteristics of anticyclone A0 and cyclone C0, as tracked by all considered datasets. The evolution of the eddy characteristic radius <math display="inline"><semantics> <msub> <mi>R</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math> (km) and outermost radius <math display="inline"><semantics> <msub> <mi>R</mi> <mrow> <mi>o</mi> <mi>u</mi> <mi>t</mi> </mrow> </msub> </semantics></math> (km) as tracked by TOEddies is shown in panel (<b>a</b>,<b>b</b>) for A0 and C0, respectively in black. The TOEddies network reconstruction composed of all detected trajectories, anticyclonic (red) and cyclonic (blue, that have merged and splitted with the main trajectories is shown in panels (<b>c</b>,<b>d</b>). The evolutions of the eddy radii and characteristic velocity <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math> (m/s) from the different datasets are shown in panels (<b>e</b>–<b>h</b>). Panels (<b>i</b>,<b>j</b>) depict the equivalent A0 and C0 trajectories as tracked from the META3.2, TIAN, and GOMEAD datasets. Bathymetric contours at −500 m, −1000 m, −2000 m, and −4000 m are indicated by gray lines.</p>
Full article ">Figure 10
<p>Snapshots along the temporal evolution of anticyclone A0 (panels <b>a</b>–<b>f</b>) propagating westward in the Southern Ocean. The background colors correspond to the ADT (m) fields while the gray arrows correspond to surface geostrophic velocities. The characteristic and outer contours as detected by TOEddies are shown in the black solid and dashed lines. The Argo floats trapped in the eddies are shown with the magenta diamond points.</p>
Full article ">Figure 11
<p>Snapshots along the temporal evolution of cyclone C0 (panels <b>a</b>–<b>f</b>) propagating westward in the Indian Ocean. The background colors correspond to the ADT (m) fields while the gray arrows correspond to surface geostrophic velocities. The characteristic and outer contours as detected by TOEddies are shown in the black solid and dashed lines. The Argo floats trapped in the eddies are shown with magenta diamond points.</p>
Full article ">Figure 12
<p>Temporal evolution of anticyclone A0 and cyclone C0 vertical structures as obtained by Argo floats trapped inside the eddy core (<math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mrow> <mi>A</mi> <mi>R</mi> <mi>G</mi> <mi>O</mi> </mrow> </msub> <mo>≤</mo> <mi>R</mi> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </semantics></math>) (shown as magenta points in panels (<b>a</b>,<b>b</b>). Vertical profiles of temperature <math display="inline"><semantics> <mrow> <mi>T</mi> <msup> <mo>(</mo> <mo>∘</mo> </msup> <mi mathvariant="normal">C</mi> <mo>)</mo> </mrow> </semantics></math> and temperature anomalies <math display="inline"><semantics> <mrow> <msub> <mi>T</mi> <mi>A</mi> </msub> <mi> </mi> <mrow> <msup> <mo>(</mo> <mo>∘</mo> </msup> <mi mathvariant="normal">C</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> are shown in panels (<b>c</b>,<b>e</b>) for anticyclone A0, and in panels (<b>d</b>,<b>f</b>) for cyclone C0.</p>
Full article ">
22 pages, 1988 KiB  
Article
Assessing the Performance of Deep Learning Predictions for Dynamic Aperture of a Hadron Circular Particle Accelerator
by Davide Di Croce, Massimo Giovannozzi, Carlo Emilio Montanari, Tatiana Pieloni, Stefano Redaelli and Frederik F. Van der Veken
Instruments 2024, 8(4), 50; https://doi.org/10.3390/instruments8040050 - 19 Nov 2024
Viewed by 616
Abstract
Understanding the concept of dynamic aperture provides essential insights into nonlinear beam dynamics, beam losses, and the beam lifetime in circular particle accelerators. This comprehension is crucial for the functioning of modern hadron synchrotrons like the CERN Large Hadron Collider and the planning [...] Read more.
Understanding the concept of dynamic aperture provides essential insights into nonlinear beam dynamics, beam losses, and the beam lifetime in circular particle accelerators. This comprehension is crucial for the functioning of modern hadron synchrotrons like the CERN Large Hadron Collider and the planning of future ones such as the Future Circular Collider. The dynamic aperture defines the extent of the region in phase space where the trajectories of charged particles are bounded over numerous revolutions, the actual number being defined by the physical application. Traditional methods for calculating the dynamic aperture depend on computationally demanding numerical simulations, which require tracking over multiple turns of numerous initial conditions appropriately distributed in phase space. Prior research has shown the efficiency of a multilayer perceptron network in forecasting the dynamic aperture of the CERN Large Hadron Collider ring, achieving a remarkable speed-up of up to 200-fold compared to standard numerical tracking tools. Building on recent advancements, we conducted a comparative study of various deep learning networks based on BERT, DenseNet, ResNet and VGG architectures. The results demonstrate substantial enhancements in the prediction of the dynamic aperture, marking a significant advancement in the development of more precise and efficient surrogate models of beam dynamics. Full article
Show Figures

Figure 1

Figure 1
<p>Stability time for a distribution of initial conditions in <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>−</mo> <mi>y</mi> </mrow> </semantics></math> space for one of the LHC configurations that are part of the data set used for constructing the DL surrogate models. The reduction in the extent of the stable region for an increasing number of turns is clearly visible. This information is then used to determine the value of the angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math>. As an example, the angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> for 1 × 10<sup>5</sup> turns is shown in red.</p>
Full article ">Figure 2
<p>Distribution of the angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> before (blue) and after (red) the augmentation and unbiasing pre-processing.</p>
Full article ">Figure 3
<p>Architecture of the designed MLP for the <math display="inline"><semantics> <mi>DA</mi> </semantics></math> regressor, featuring a fully connected structure.</p>
Full article ">Figure 4
<p>Architecture of the designed BERT for the <math display="inline"><semantics> <mi>DA</mi> </semantics></math> regressor.</p>
Full article ">Figure 5
<p>Architecture of the designed DenseNet-121 for the <math display="inline"><semantics> <mi>DA</mi> </semantics></math> regressor.</p>
Full article ">Figure 6
<p>Architecture of the designed ResNet-18 for the <math display="inline"><semantics> <mi>DA</mi> </semantics></math> regressor.</p>
Full article ">Figure 7
<p>Architecture of the designed VGG-16 for the <math display="inline"><semantics> <mi>DA</mi> </semantics></math> regressor.</p>
Full article ">Figure 8
<p>Architecture of the designed Hybrid network for the <math display="inline"><semantics> <mi>DA</mi> </semantics></math> regressor.</p>
Full article ">Figure 9
<p>Training and validation performance over epochs. The blue line represents the training loss (MAE), while the orange line shows the validation loss. The green line tracks the learning rate adjustments throughout the training. The vertical dashed line indicates the epoch at which the model was saved.</p>
Full article ">Figure 10
<p>Predicted angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> as a function of the computed angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> values for the test data set for: (<b>a</b>) BERT, (<b>b</b>) DenseNet-121, (<b>c</b>) ResNet-18, (<b>d</b>) MLP (baseline), (<b>e</b>) Hybrid and (<b>f</b>) VGG-16 architectures. The Pearson correlation coefficient is also shown.</p>
Full article ">Figure 10 Cont.
<p>Predicted angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> as a function of the computed angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> values for the test data set for: (<b>a</b>) BERT, (<b>b</b>) DenseNet-121, (<b>c</b>) ResNet-18, (<b>d</b>) MLP (baseline), (<b>e</b>) Hybrid and (<b>f</b>) VGG-16 architectures. The Pearson correlation coefficient is also shown.</p>
Full article ">Figure 11
<p>Computed (blue) and predicted (red) angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> distribution for the test data set for: (<b>a</b>) BERT, (<b>b</b>) DenseNet-121, (<b>c</b>) ResNet-18, (<b>d</b>) MLP (baseline), (<b>e</b>) Hybrid and (<b>f</b>) VGG-16 architectures. The outcome of the Kolmogorov–Smirnov test, used to compare the two distributions, is also reported.</p>
Full article ">Figure 11 Cont.
<p>Computed (blue) and predicted (red) angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> distribution for the test data set for: (<b>a</b>) BERT, (<b>b</b>) DenseNet-121, (<b>c</b>) ResNet-18, (<b>d</b>) MLP (baseline), (<b>e</b>) Hybrid and (<b>f</b>) VGG-16 architectures. The outcome of the Kolmogorov–Smirnov test, used to compare the two distributions, is also reported.</p>
Full article ">Figure 12
<p>The true angular <math display="inline"><semantics> <mi>DA</mi> </semantics></math> (<b>left</b>) and the BERT prediction (<b>right</b>) for four different machine configurations present on the test data set. The colours indicate the stability time in turns.</p>
Full article ">Figure 13
<p>Box plot of the MAE as a function of the number of turns for the machine configurations tracked up to 5 × 10<sup>5</sup> turns in the test data set. The box limits indicate the range of the central 50% of the data with a central line marking the mean value.</p>
Full article ">
18 pages, 1428 KiB  
Article
The EUPEMEN (EUropean PErioperative MEdical Networking) Protocol for Acute Appendicitis: Recommendations for Perioperative Care
by Orestis Ioannidis, Elissavet Anestiadou, Jose M. Ramirez, Nicolò Fabbri, Javier Martínez Ubieto, Carlo Vittorio Feo, Antonio Pesce, Kristyna Rosetzka, Antonio Arroyo, Petr Kocián, Luis Sánchez-Guillén, Ana Pascual Bellosta, Adam Whitley, Alejandro Bona Enguita, Marta Teresa-Fernandéz, Stefanos Bitsianis and Savvas Symeonidis
J. Clin. Med. 2024, 13(22), 6943; https://doi.org/10.3390/jcm13226943 - 18 Nov 2024
Viewed by 648
Abstract
Background/Objectives: Acute appendicitis (AA) is one of the most common causes of emergency department visits due to acute abdominal pain, with a lifetime risk of 7–8%. Managing AA presents significant challenges, particularly among vulnerable patient groups, due to its association with substantial morbidity [...] Read more.
Background/Objectives: Acute appendicitis (AA) is one of the most common causes of emergency department visits due to acute abdominal pain, with a lifetime risk of 7–8%. Managing AA presents significant challenges, particularly among vulnerable patient groups, due to its association with substantial morbidity and mortality. Methods: The EUPEMEN (European PErioperative MEdical Networking) project aims to optimize perioperative care for AA by developing multidisciplinary guidelines that integrate theoretical knowledge and clinical expertise from five European countries. This study presents the key elements of the EUPEMEN protocol, which focuses on reducing surgical stress, optimizing perioperative care, and enhancing postoperative recovery. Results: Through this standardized approach, the protocol aims to lower postoperative morbidity and mortality, shorten hospital stays, and improve overall patient outcomes. The recommendations are tailored to address the variability in clinical practice across Europe and are designed to be widely implementable in diverse healthcare settings. Conclusions: The conclusions drawn from this study highlight the potential for the EUPEMEN protocol to significantly improve perioperative care standards for AA, demonstrating its value as a practical, adaptable tool for clinicians. Full article
(This article belongs to the Special Issue New Insights into Acute Care and Emergency Surgery)
Show Figures

Figure 1

Figure 1
<p>The EUPEMEN protocol in surgery for AA.</p>
Full article ">
24 pages, 2020 KiB  
Article
Enhanced Long-Range Network Performance of an Oil Pipeline Monitoring System Using a Hybrid Deep Extreme Learning Machine Model
by Abbas Kubba, Hafedh Trabelsi and Faouzi Derbel
Future Internet 2024, 16(11), 425; https://doi.org/10.3390/fi16110425 - 17 Nov 2024
Viewed by 4407
Abstract
Leak detection in oil and gas pipeline networks is a climacteric and frequent issue in the oil and gas field. Many establishments have long depended on stationary hardware or traditional assessments to monitor and detect abnormalities. Rapid technological progress; innovation in engineering; and [...] Read more.
Leak detection in oil and gas pipeline networks is a climacteric and frequent issue in the oil and gas field. Many establishments have long depended on stationary hardware or traditional assessments to monitor and detect abnormalities. Rapid technological progress; innovation in engineering; and advanced technologies providing cost-effective, rapidly executed, and easy to implement solutions lead to building an efficient oil pipeline leak detection and real-time monitoring system. In this area, wireless sensor networks (WSNs) are increasingly required to enhance the reliability of checkups and improve the accuracy of real-time oil pipeline monitoring systems with limited hardware resources. The real-time transient model (RTTM) is a leak detection method integrated with LoRaWAN technology, which is proposed in this study to implement a wireless oil pipeline network for long distances. This study will focus on enhancing the LoRa network parameters, e.g., node power consumption, average packet loss, and delay, by applying several machine learning techniques in order to optimize the durability of individual nodes’ lifetimes and enhance total system performance. The proposed system is implemented in an OMNeT++ network simulator with several frameworks, such as Flora and Inet, to cover the LoRa network, which is used as the system’s network infrastructure. In order to implement artificial intelligence over the FLoRa network, the LoRa network was integrated with several programming tools and libraries, such as Python script and the TensorFlow libraries. Several machine learning algorithms have been applied, such as the random forest (RF) algorithm and the deep extreme learning machine (DELM) technique, to develop the proposed model and improve the LoRa network’s performance. They improved the LoRa network’s output performance, e.g., its power consumption, packet loss, and packet delay, with different enhancement ratios. Finally, a hybrid deep extreme learning machine model was built and selected as the proposed model due to its ability to improve the LoRa network’s performance, with perfect prediction accuracy, a mean square error of 0.75, and an exceptional enhancement ratio of 39% for LoRa node power consumption. Full article
(This article belongs to the Topic Advances in Wireless and Mobile Networking)
Show Figures

Figure 1

Figure 1
<p>Description of a LoRa network: (<b>a</b>) LoRa network architecture; (<b>b</b>) LoRa stack protocol.</p>
Full article ">Figure 2
<p>The network design of the proposed system. (a) RTTM-based LoRaWAN monitoring system; (<b>b</b>) LoRa network design based on OMNet++.</p>
Full article ">Figure 3
<p>Deep extreme learning machine architecture.</p>
Full article ">Figure 4
<p>Workflow of the LoRa-network-based hybrid DELM model.</p>
Full article ">Figure 5
<p>Comparative analysis of LoRa performance: (<b>a</b>) power consumption representation; (<b>b</b>) packet delay representation; (<b>c</b>) packet loss representation.</p>
Full article ">
Back to TopTop