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Search Results (10,696)

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24 pages, 20801 KiB  
Article
Four-Dimensional Generalized AMS Optimization Considering Critical Engine Inoperative for an eVTOL
by Jiannan Zhang, Max Söpper, Florian Holzapfel and Shuguang Zhang
Aerospace 2024, 11(12), 990; https://doi.org/10.3390/aerospace11120990 (registering DOI) - 29 Nov 2024
Abstract
In this paper, we present a method to optimize the attainable moment set (AMS) to increase the control authority for electrical vertical take-off and landing vehicles (eVTOLs). As opposed to 3D AMSs for conventional airplanes, the hover control of eVTOLs requires vertical thrust [...] Read more.
In this paper, we present a method to optimize the attainable moment set (AMS) to increase the control authority for electrical vertical take-off and landing vehicles (eVTOLs). As opposed to 3D AMSs for conventional airplanes, the hover control of eVTOLs requires vertical thrust produced by the powered lift system in addition to three moments. The limits of the moments and vertical thrust are coupled due to input saturation, and, as a result, the concept of the traditional AMS is extended to the 4D generalized moment set to account for this coupling effect. Given a required moment set (RMS) derived from system requirements, the optimization is formulated as a 4D convex polytope coverage problem, i.e., the AMS coverage over the RMS, such that the system’s available control authority is maximized to fulfill the prescribed requirements. The optimization accounts for not only nominal flight, but also for one critical engine inoperative situation. To test the method, it is applied to an eVTOL with eight rotors to optimize for the rotors’ orientation with respect to the body axis. The results indicate highly improved coverage of the RMS for both failure-free and one-engine-inoperative situations. Closed-loop simulation tests are performed for both optimal and non-optimal configurations to further validate the results. Full article
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<p>Two-dimensional example of AMS, RMS, and the margin in between.</p>
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<p>(<b>a</b>) Model of the airframe under discussion. The figure directly refers to <a href="#aerospace-11-00990-f001" class="html-fig">Figure 1</a> in Ref. [<a href="#B25-aerospace-11-00990" class="html-bibr">25</a>]; (<b>b</b>) top view of the airframe under discussion.</p>
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<p>Rotor tilt layout according to initial design parameters.</p>
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<p>Comparison of AMS with different rotor tilt angles and the RMS.</p>
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<p>Test 1 optimized rotor layout.</p>
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<p>Test 1 comparison: Optimized AMS, initial AMS, and RMS.</p>
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<p>Test 1 comparison: Cumulative count of margin factors.</p>
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<p>Test 1 cost function over optimization variables.</p>
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<p>Test 2 optimized rotor layout.</p>
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<p>Test 2 comparison: Optimized AMS, initial AMS, and RMS.</p>
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<p>Test 2 comparison: Cumulative count of margin factors.</p>
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<p>Test 3 optimized rotor layout.</p>
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<p>Test 3 comparison: Optimized AMS, initial AMS, and RMS. The AMSs are degraded by removing the critical rotor from the control set.</p>
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<p>Test 3 comparison: Cumulative count of margin factors.</p>
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<p>Test 3 cost function over optimization variables.</p>
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<p>Test 4 optimized rotor layout.</p>
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<p>Test 4 comparison: Optimized AMS, initial AMS, and RMS. The AMSs are degraded by removing the critical rotor from the control set.</p>
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<p>Test 4 comparison: Cumulative count of margin factors.</p>
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<p>Tracking performance for the initial configuration.</p>
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<p>Control efforts (as rotor speeds in rad/s) of the initial configuration.</p>
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<p>Tracking performance of the initial configuration. Failure injected @ t = 10 s; failure known to the flight control system @ t = 11 s.</p>
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<p>Control efforts (as rotor speeds in rad/s) of the initial configuration. Failure to L01 injected @ t = 10 s; failure known to the flight control system @ t = 11 s.</p>
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<p>Tracking performance of the non-failure-optimized configuration. Failure injected @ t = 10 s; failure known to the flight control system @ t = 11 s.</p>
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<p>Control efforts (as rotor speeds in rad/s) of the non-failure-optimized configuration. Failure to L01 injected @ t = 10 s; failure known to the flight control system @ t = 11 s.</p>
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<p>Tracking performance of the critical-failure-optimized configuration. Failure injected @ t = 10 s; failure known to the flight control system @ t = 11 s.</p>
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<p>Control efforts (as rotor speeds in rad/s) of the critical-failure-optimized configuration. Failure to L01 injected @ t = 10 s; failure known to the flight control system @ t = 11 s.</p>
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17 pages, 2066 KiB  
Article
Extending Conflict-Based Search for Optimal and Efficient Quadrotor Swarm Motion Planning
by Zihao Wang, Zhiwei Zhang, Wenying Dou, Guangpeng Hu, Lifu Zhang and Meng Zhang
Drones 2024, 8(12), 719; https://doi.org/10.3390/drones8120719 (registering DOI) - 29 Nov 2024
Abstract
Multi-agent pathfinding has been extensively studied by the robotics and artificial intelligence communities. The classical algorithm, conflict-based search (CBS), is widely used in various real-world applications due to its ability to solve large-scale conflict-free paths. However, classical CBS assumes discrete time–space planning and [...] Read more.
Multi-agent pathfinding has been extensively studied by the robotics and artificial intelligence communities. The classical algorithm, conflict-based search (CBS), is widely used in various real-world applications due to its ability to solve large-scale conflict-free paths. However, classical CBS assumes discrete time–space planning and overlooks physical constraints in actual scenarios, making it unsuitable for direct application in unmanned aerial vehicle (UAV) swarm. Inspired by the decentralized planning and centralized conflict resolution ideas of CBS, we propose, for the first time, an optimal and efficient UAV swarm motion planner that integrates state lattice with CBS without any underlying assumption, named SL-CBS. SL-CBS is a two-layer search algorithm: (1) The low-level search utilizes an improved state lattice. We design emergency stop motion primitives to ensure complete UAV dynamics and handle spatio-temporal constraints from high-level conflicts. (2) The high-level algorithm defines comprehensive conflict types and proposes a motion primitive conflict detection method with linear time complexity based on Sturm’s theory. Additionally, our modified independence detection (ID) technique is applied to enable parallel conflict processing. We validate the planning capabilities of SL-CBS in classical scenarios and compare these with the latest state-of-the-art (SOTA) algorithms, showing great improvements in success rate, computation time, and flight time. Finally, we conduct large-scale tests to analyze the performance boundaries of SL-CBS+ID. Full article
(This article belongs to the Section Drone Design and Development)
30 pages, 2645 KiB  
Article
An Innovative Applied Control System of Helicopter Turboshaft Engines Based on Neuro-Fuzzy Networks
by Serhii Vladov, Oleksii Lytvynov, Victoria Vysotska, Viktor Vasylenko, Petro Pukach and Myroslava Vovk
Appl. Syst. Innov. 2024, 7(6), 118; https://doi.org/10.3390/asi7060118 (registering DOI) - 29 Nov 2024
Abstract
This study focuses on helicopter turboshaft engine innovative fault-tolerant fuzzy automatic control system development to enhance safety and efficiency in various flight modes. Unlike traditional systems, the proposed automatic control system incorporates a fuzzy regulator with an adaptive control mechanism, allowing for dynamic [...] Read more.
This study focuses on helicopter turboshaft engine innovative fault-tolerant fuzzy automatic control system development to enhance safety and efficiency in various flight modes. Unlike traditional systems, the proposed automatic control system incorporates a fuzzy regulator with an adaptive control mechanism, allowing for dynamic fuel flow and blade pitch angle adjustment based on changing conditions. The scientific novelty lies in the helicopter turboshaft engines distinguishing separate models and the fuel metering unit, significantly improving control accuracy and adaptability to current flight conditions. During experimental research on the TV3-117 engine installed on the Mi-8MTV helicopter, a parametric modeling system was developed to simulate engine operation in real time and interact with higher-level systems. Innovation is evident in the creation of the failure model that accounts for dynamic changes and probabilistic characteristics, enabling the prediction of failures and minimizing their impact on the system. The results demonstrate high effectiveness for the proposed model, achieving an accuracy of 99.455%, while minimizing the loss function, confirming its reliability for practical application in dynamic flight conditions. Full article
17 pages, 888 KiB  
Article
Physics-Informed Neural Networks for Unmanned Aerial Vehicle System Estimation
by Domenico Bianchi, Nicola Epicoco, Mario Di Ferdinando, Stefano Di Gennaro and Pierdomenico Pepe
Drones 2024, 8(12), 716; https://doi.org/10.3390/drones8120716 - 29 Nov 2024
Viewed by 30
Abstract
The dynamic nature of quadrotor flight introduces significant uncertainty in system parameters, such as thrust and drag factors. Consequently, operators grapple with escalating challenges in implementing real-time control actions. This study presents an approach for estimating the dynamic model of Unmanned Aerial Vehicles [...] Read more.
The dynamic nature of quadrotor flight introduces significant uncertainty in system parameters, such as thrust and drag factors. Consequently, operators grapple with escalating challenges in implementing real-time control actions. This study presents an approach for estimating the dynamic model of Unmanned Aerial Vehicles based on Physics-Informed Neural Networks (PINNs), which is of paramount importance due to the presence of uncertain data and since control actions are required in very short computation times. In this regard, by including physical laws into neural networks, PINNs offer the potential to tackle several issues, such as heightened non-linearities in low-inertia systems, elevated measurement noise, and constraints on data availability or uncertainties, while ensuring the robustness of the solution, thus ensuring effective results in short time, once the network training has been performed and without the need to be retrained. The effectiveness of the proposed method is showcased in a simulation environment with real data and juxtaposed with a state-of-the-art technique, such as the Extended Kalman Filter (EKF). The results show that the proposed estimator outperforms the EKF both in terms of the efficacy of the solution and computation time. Full article
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<p>Quadrotor orientation using Euler angles.</p>
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<p>PINNs architecture. It functions by employing its own output prediction as the initial state.</p>
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<p>Position x-axis and corresponding error.</p>
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<p>Position y-axis and corresponding error.</p>
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<p>Position z-axis and corresponding error.</p>
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<p>Roll angle <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math> and corresponding error.</p>
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<p>Pitch angle <math display="inline"><semantics> <mi>θ</mi> </semantics></math> and corresponding error.</p>
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<p>Yaw angle <math display="inline"><semantics> <mi>ψ</mi> </semantics></math> and corresponding error.</p>
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22 pages, 14750 KiB  
Article
Safety Status Prediction Model of Transmission Tower Based on Improved Coati Optimization-Based Support Vector Machine
by Xinxi Gong, Yaozhong Zhu, Yanhai Wang, Enyang Li, Yuhao Zhang and Zilong Zhang
Buildings 2024, 14(12), 3815; https://doi.org/10.3390/buildings14123815 - 28 Nov 2024
Viewed by 211
Abstract
Natural calamities have historically impacted operational mountainous power transmission towers, including high winds and ice accumulation, which can result in pole damage or diminished load-bearing capability, compromising their structural integrity. Consequently, developing a safety state prediction model for transmission towers may efficiently monitor [...] Read more.
Natural calamities have historically impacted operational mountainous power transmission towers, including high winds and ice accumulation, which can result in pole damage or diminished load-bearing capability, compromising their structural integrity. Consequently, developing a safety state prediction model for transmission towers may efficiently monitor and evaluate potential risks, providing early warnings of structural dangers and diminishing the likelihood of bending or collapse incidents. This paper presents a safety state prediction model for transmission towers utilizing improved coati optimization-based SVM (ICOA-SVM). Initially, we optimize the coati optimization algorithm (COA) through inverse refraction learning and Levy flight strategy. Subsequently, we employ the improved coati optimization algorithm (ICOA) to refine the penalty parameters and kernel function of the support vector machine (SVM), thereby developing the safety state prediction model for the transmission tower. A finite element model is created to simulate the dynamic reaction of the transmission tower under varying wind angles and loads; ultimately, wind speed, wind angle, and ice cover thickness are utilized as inputs to the model, with the safe condition of the transmission tower being the output. The predictive outcomes indicate that the proposed ICOA-SVM model exhibits rapid convergence and high prediction accuracy, with a 62.5% reduction in root mean square error, a 59.6% decrease in average relative error, and a 75.0% decline in average absolute error compared to the conventional support vector machine. This work establishes a scientific foundation for the safety monitoring and maintenance of transmission towers, effectively identifying possible dangers and substantially decreasing the likelihood of accidents. Full article
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<p>Schematic diagram of refractive inverse learning principle.</p>
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<p>(<b>a</b>) <span class="html-italic">f</span><sub>1</sub> test function; (<b>b</b>) <span class="html-italic">f</span><sub>2</sub> test function; (<b>c</b>) <span class="html-italic">f</span><sub>3</sub> test function; (<b>d</b>) <span class="html-italic">f</span><sub>4</sub> test function; (<b>e</b>) <span class="html-italic">f</span><sub>5</sub> test function; (<b>f</b>) <span class="html-italic">f</span><sub>6</sub> test function.</p>
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<p>(<b>a</b>) <span class="html-italic">f</span><sub>1</sub> test function; (<b>b</b>) <span class="html-italic">f</span><sub>2</sub> test function; (<b>c</b>) <span class="html-italic">f</span><sub>3</sub> test function; (<b>d</b>) <span class="html-italic">f</span><sub>4</sub> test function; (<b>e</b>) <span class="html-italic">f</span><sub>5</sub> test function; (<b>f</b>) <span class="html-italic">f</span><sub>6</sub> test function.</p>
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<p>ICAO-SVM model flowchart.</p>
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<p>Finite element model diagram of transmission tower.</p>
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<p>(<b>a</b>) Stress and displacement cloud diagram for a wind direction angle of 30°, wind speed of 10 m/s, and an ice thickness of 0 mm; (<b>b</b>) Stress and displacement cloud diagram for a wind direction angle of 90°, wind speed of 10 m/s, and an ice thickness of 0 mm; (<b>c</b>) Stress and displacement cloud diagram for a wind direction angle of 90°, wind speed of 30 m/s, and an ice thickness of 0 mm; (<b>d</b>) Stress and displacement cloud diagram for a wind direction angle of 90°, wind speed of 30 m/s, and an ice thickness of 0 mm.</p>
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<p>(<b>a</b>) Stress and displacement cloud diagram for a wind direction angle of 30°, wind speed of 10 m/s, and an ice thickness of 0 mm; (<b>b</b>) Stress and displacement cloud diagram for a wind direction angle of 90°, wind speed of 10 m/s, and an ice thickness of 0 mm; (<b>c</b>) Stress and displacement cloud diagram for a wind direction angle of 90°, wind speed of 30 m/s, and an ice thickness of 0 mm; (<b>d</b>) Stress and displacement cloud diagram for a wind direction angle of 90°, wind speed of 30 m/s, and an ice thickness of 0 mm.</p>
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<p>SVM prediction results.</p>
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<p>COA-SVM prediction results.</p>
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<p>ICOA-SVM prediction results.</p>
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18 pages, 2499 KiB  
Article
Intelligent Path Planning for UAV Patrolling in Dynamic Environments Based on the Transformer Architecture
by Ching-Hao Yu, Jichiang Tsai and Yuan-Tsun Chang
Electronics 2024, 13(23), 4716; https://doi.org/10.3390/electronics13234716 - 28 Nov 2024
Viewed by 237
Abstract
Due to its NP-Hard property, the Travelling Salesman Problem (TSP) has long been a prominent research topic in path planning. The goal is to design the algorithm with the fastest execution speed in order to find the path with the lowest travelling cost. [...] Read more.
Due to its NP-Hard property, the Travelling Salesman Problem (TSP) has long been a prominent research topic in path planning. The goal is to design the algorithm with the fastest execution speed in order to find the path with the lowest travelling cost. In particular, new generative AI technology is continually emerging. The question of how to exploit algorithms from this realm to perform TSP path planning, especially in dynamic environments, is an important and interesting problem. The TSP application scenario investigated by this paper is that of an Unmanned Aerial Vehicle (UAV) that needs to patrol all specific ship-targets on the sea surface before returning to its origin. Hence, during the flight, we must consider real-time changes in wind velocity and direction, as well as the dynamic addition or removal of ship targets due to mission requirements. Specifically, we implement a Deep Reinforcement Learning (DRL) model based on the Transformer architecture, which is widely used in Generative AI, to solve the TSP path-planning problem in dynamic environments. Finally, we conduct numerous simulation experiments to compare the performance of our DRL model and the traditional heuristic algorithm, the Simulated Annealing (SA) method, in terms of operation time and path distance in solving the ordinary TSP, to verify the advantages of our model. Notably, traditional heuristic algorithms cannot be applied to dynamic environments, in which wind velocity and direction can change at any time. Full article
(This article belongs to the Special Issue Parallel, Distributed, Edge Computing in UAV Communication)
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<p>The Transformer model architecture diagram.</p>
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<p>Inference process of the transformer model in static environment.</p>
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<p>Inference process of the transformer model in dynamic environment.</p>
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<p>Hybrid training flow chart.</p>
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<p>Dynamic nodes removal with varying numbers of nodes: (<b>a</b>) TSP 10, (<b>b</b>) TSP 20, and (<b>c</b>) TSP 50.</p>
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<p>Node addition process.</p>
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<p>Dynamic node addition and removal with different node counts: (<b>a</b>) TSP 10, (<b>b</b>) TSP 20, and (<b>c</b>) TSP 50.</p>
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31 pages, 3335 KiB  
Article
Unified Ecosystem for Data Sharing and AI-Driven Predictive Maintenance in Aviation
by Igor Kabashkin and Vitaly Susanin
Computers 2024, 13(12), 318; https://doi.org/10.3390/computers13120318 - 28 Nov 2024
Viewed by 190
Abstract
The aviation industry faces considerable challenges in maintenance management due to the complexities of data standardization, data sharing, and predictive maintenance capabilities. This paper introduces a unified ecosystem for data sharing and AI-driven predictive maintenance designed to address these challenges by integrating real-time [...] Read more.
The aviation industry faces considerable challenges in maintenance management due to the complexities of data standardization, data sharing, and predictive maintenance capabilities. This paper introduces a unified ecosystem for data sharing and AI-driven predictive maintenance designed to address these challenges by integrating real-time and historical data from diverse sources, including aircraft sensors, maintenance logs, and operational records. The proposed ecosystem enables predictive analytics and anomaly detection, enhancing decision-making processes for airlines, maintenance, repair, and overhaul providers, and regulatory bodies. Key elements of the ecosystem include a modular design with feedback loops, scalable AI models for predictive maintenance, and robust data-sharing frameworks. This paper outlines the architecture of a unified aviation maintenance ecosystem built around multiple data sources, including aircraft sensors, maintenance logs, flight data, weather data, and manufacturer specifications. By integrating various components and stakeholders, the system achieves its full potential through several key use cases: monitoring aircraft component health, predicting component failures, receiving maintenance alerts, performing preventive maintenance, and generating compliance reports. Each use case is described in detail and supported by illustrative dataflow diagrams. The findings underscore the transformative impact of such an ecosystem on aviation maintenance practices, marking a significant step toward safer, more efficient, and sustainable aviation operations. Full article
(This article belongs to the Special Issue Emerging Trends in Machine Learning and Artificial Intelligence)
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<p>Unified aviation maintenance ecosystem.</p>
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<p>Integrated AI-driven use cases for aircraft health monitoring and compliance.</p>
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<p>Dataflow diagram for the monitor aircraft component health use case.</p>
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<p>Color-coding scheme for architectural components and priority indicators.</p>
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<p>Dataflow diagram for the predict component failure use case.</p>
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<p>Dataflow diagram for the receive maintenance alerts use case.</p>
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<p>Dataflow diagram for the perform preventive maintenance use case.</p>
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<p>Dataflow diagram for the generate compliance reports use case.</p>
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<p>AI engine architecture for the predictive maintenance system.</p>
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15 pages, 4566 KiB  
Article
Informative Path Planning Using Physics-Informed Gaussian Processes for Aerial Mapping of 5G Networks
by Jonas F. Gruner, Jan Graßhoff, Carlos Castelar Wembers, Kilian Schweppe, Georg Schildbach and Philipp Rostalski
Sensors 2024, 24(23), 7601; https://doi.org/10.3390/s24237601 - 28 Nov 2024
Viewed by 237
Abstract
The advent of 5G technology has facilitated the adoption of private cellular networks in industrial settings. Ensuring reliable coverage while maintaining certain requirements at its boundaries is crucial for successful deployment yet challenging without extensive measurements. In this article, we propose the leveraging [...] Read more.
The advent of 5G technology has facilitated the adoption of private cellular networks in industrial settings. Ensuring reliable coverage while maintaining certain requirements at its boundaries is crucial for successful deployment yet challenging without extensive measurements. In this article, we propose the leveraging of unmanned aerial vehicles (UAVs) and Gaussian processes (GPs) to reduce the complexity of this task. Physics-informed mean functions, including a detailed ray-tracing simulation, are integrated into the GP models to enhance the extrapolation performance of the GP prediction. As a central element of the GP prediction, a quantitative evaluation of different mean functions is conducted. The most promising candidates are then integrated into an informative path-planning algorithm tasked with performing an efficient UAV-based cellular network mapping. The algorithm combines the physics-informed GP models with Bayesian optimization and is developed and tested in a hardware-in-the-loop simulation. The quantitative evaluation of the mean functions and the informative path-planning simulation are based on real-world measurements of the 5G reference signal received power (RSRP) in a cellular 5G-SA campus network at the Port of Lübeck, Germany. These measurements serve as ground truth for both evaluations. The evaluation results demonstrate that using an appropriate mean function can result in an enhanced prediction accuracy of the GP model and provide a suitable basis for informative path planning. The subsequent informative path-planning simulation experiments highlight these findings. For a fixed maximum travel distance, a path is iteratively computed, reducing the flight distance by up to 98% while maintaining an average root-mean-square error of less than 6 dBm when compared to the measurement trials. Full article
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<p>5G mMeasurement unit mounted below a DJI Matrice 300 UAV.</p>
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<p>Flight planning for the measurement flight in UgCS ground control software by SPH Engineering (Riga, Latvia). The green lines depict the flight routes, and the red transparent areas mark no-fly zones around higher structures like light poles.</p>
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<p>Scatter plot of the received reference signal strength (RSRP) measurements, together with the antenna pattern of the base station, on a geospatial map. The base station is marked with a drop pin. Created using the MATLAB Antenna Toolbox. Background: © OpenStreetMap contributors, CC BY-SA.</p>
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<p>Visualization of the processes of acquiring the simulation data. Background: © OpenStreetMap contributors, CC BY-SA.</p>
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<p>Evaluation setups with different means to separate the test set from the training set. Training point (candidates) are labeled in green, test points are labeled in blue, and discarded points are labeled in red. The base station is marked with a drop pin. (<b>a</b>) Height separation. (<b>b</b>) Cluster separation. (<b>c</b>) Distance separation. (<b>d</b>) Random split (example). Background: © OpenStreetMap contributors, CC BY-SA.</p>
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<p>Root-mean-square error (RMSE) between the measurement from the test set and the predicted value of the utilized GP with the indicated mean function (<math display="inline"><semantics> <msub> <mi>m</mi> <mrow> <mn>3</mn> <mi>GPP</mi> <mo>−</mo> <mi>UMi</mi> </mrow> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>m</mi> <mi>CD</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>m</mi> <mrow> <mn>3</mn> <mi>GPP</mi> </mrow> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>m</mi> <mi>SIM</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>m</mi> <mi>ZERO</mi> </msub> </semantics></math>) or the simulation without a GP (“<math display="inline"><semantics> <mrow> <mi>only</mi> <mspace width="0.166667em"/> <mi>SIM</mi> </mrow> </semantics></math>”) on a logarithmic axis.</p>
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<p>Simplified 2D visualization of the candidate points.</p>
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<p>Root-mean-square error (RMSE) between the measurement from the test set and the predicted value of the utilized GP with the indicated mean function (<math display="inline"><semantics> <msub> <mi>m</mi> <mi>ZERO</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>m</mi> <mi>CD</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>m</mi> <mi>SIM</mi> </msub> </semantics></math>) and the tuning parameters of the IPP algorithm (<math display="inline"><semantics> <mi>α</mi> </semantics></math> and <math display="inline"><semantics> <mi>κ</mi> </semantics></math>) plotted using a logarithmic color scale.</p>
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25 pages, 11917 KiB  
Article
Multi-Phase Trajectory Planning for Wind Energy Harvesting in Air-Launched UAV Swarm Rendezvous and Formation Flight
by Xiangsheng Wang, Tielin Ma, Ligang Zhang, Nanxuan Qiao, Pu Xue and Jingcheng Fu
Drones 2024, 8(12), 709; https://doi.org/10.3390/drones8120709 - 28 Nov 2024
Viewed by 202
Abstract
Small air-launched unmanned aerial vehicles (UAVs) face challenges in range and endurance due to their compact size and lightweight design. To address these issues, this paper introduces a multi-phase wind energy harvesting trajectory planning method designed to optimize the onboard electrical energy consumption [...] Read more.
Small air-launched unmanned aerial vehicles (UAVs) face challenges in range and endurance due to their compact size and lightweight design. To address these issues, this paper introduces a multi-phase wind energy harvesting trajectory planning method designed to optimize the onboard electrical energy consumption during rendezvous and formation flight of air-launched fixed-wing swarms. This method strategically manages gravitational potential energy from air-launch deployments and harvests wind energy that aligns with the UAV’s flight speed. We integrate wind energy harvesting strategies for single vehicles with the spatial–temporal coordination of the swarm system. Considering the wind effects into the trajectory planning allows UAVs to enhance their operational capabilities and extend mission duration without changes on the vehicle design. The trajectory planning method is formalized as an optimal control problem (OCP) that ensures spatial–temporal coordination, inter-vehicle collision avoidance, and incorporates a 3-degree of freedom kinematic model of UAVs, extending wind energy harvesting trajectory optimization from an individual UAV to swarm-level applications. The cost function is formulized to comprehensively evaluate electrical energy consumption, endurance, and range. Simulation results demonstrate significant energy savings in both low- and high-altitude mission scenarios. Efficient wind energy utilization can double the maximum formation rendezvous distance and even allow for rendezvous without electrical power consumption when the phase durations are extended reasonably. The subsequent formation flight phase exhibits a maximum endurance increase of 58%. This reduction in electrical energy consumption directly extends the range and endurance of air-launched swarm, thereby enhancing the mission capabilities of the swarm in subsequent flight. Full article
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<p>Diagram illustrating the optimal two-phase wind energy harvesting trajectory of air-launched UAV swarms from different mother planes.</p>
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<p>Typical wind profile of the altitude range [<a href="#B39-drones-08-00709" class="html-bibr">39</a>].</p>
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<p>Three views and an axonometric view of the air-launched UAV.</p>
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<p>Aerodynamic and thrust forces acting on the UAV and the aerodynamic angles.</p>
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<p>Joint wind energy harvesting trajectories of fixed-wing swarms. (<b>a</b>) Closed-loop trajectories in loiter mode; (<b>b</b>) Open-loop trajectories for rendezvous.</p>
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<p>Transformation process of the multi-phase trajectory OCP for air-launched swarms in the hp-adaptive pseudo-spectral method, <math display="inline"><semantics> <mrow> <mi>l</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mi>L</mi> <mo stretchy="false">]</mo> </mrow> </semantics></math> is the phase number.</p>
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<p>The numerical solution procedure of the hp-adaptive pseudo-spectral method in the multi-phase trajectory optimization of fixed-wing swarm, <math display="inline"><semantics> <mrow> <mi>l</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mi>L</mi> <mo stretchy="false">]</mo> </mrow> </semantics></math> is the phase number.</p>
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<p>Framework of two-phase OCP in the low-altitude mission scenario.</p>
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<p>Trajectory for the low-altitude mission scenarios without wind energy harvesting in an altitude range of 1.1–0.5 km.</p>
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<p>Trajectory for the low-altitude mission scenarios with wind energy harvesting in an altitude range of 1.1–0.5 km.</p>
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<p>The potential, electrical, and kinetic energy in the low-altitude mission scenario.</p>
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<p>Framework of two-phase OCP in the high-altitude mission scenario.</p>
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<p>Three-dimensional spatial trajectory and energy diagram of the five cost functions in a high-altitude mission in an altitude range of 8.3–6 km.</p>
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<p>Three-dimensional spatial trajectory and energy diagram of the five cost functions in a high-altitude mission in an altitude range of 8.3–6 km.</p>
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25 pages, 6785 KiB  
Article
Intelligent QLFEKF Integrated Navigation for the SSBE Cruise Phase Based on X-Ray Pulsar/Solar and Target Planetary Doppler Information Fusion
by Wenjian Tao, Jinxiu Zhang, Jianing Song, Qin Lin, Zebin Chen, Hui Wang, Jikun Yang and Jihe Wang
Remote Sens. 2024, 16(23), 4465; https://doi.org/10.3390/rs16234465 - 28 Nov 2024
Viewed by 179
Abstract
The Solar System Boundary Exploration (SSBE) mission is the focal point for future far-reaching space exploration. Due to the SSBE having many scientific difficulties that need to be studied, such as a super long space exploratory distance, a super long flight time in [...] Read more.
The Solar System Boundary Exploration (SSBE) mission is the focal point for future far-reaching space exploration. Due to the SSBE having many scientific difficulties that need to be studied, such as a super long space exploratory distance, a super long flight time in orbit, and a significant communication data delay between the ground and the probe, the probe must have sufficient intelligence to realize intelligent autonomous navigation. Traditional navigation schemes have been unable to provide high-accuracy autonomous intelligent navigation for the probe independent of the ground. Therefore, high-accuracy intelligent astronomical integrated navigation would provide new methods and technologies for the navigation of the SSBE probe. The probe of the SSBE is disturbed by multiple sources of solar light pressure and a complex, unknown environment during its long cruise operation while in orbit. In order to ensure the high-accuracy position state and velocity state error estimation for the probe in the cruise phase, an autonomous intelligent integrated navigation scheme based on the X-ray pulsar/solar and target planetary Doppler velocity measurements is proposed. The reinforcement Q-learning method is introduced, and the reward mechanism is designed for trial-and-error tuning of state and observation noise error covariance parameters. The federated extended Kalman filter (FEKF) based on the Q-learning (QLFEKF) navigation algorithm is proposed to achieve high-accuracy state estimations of the autonomous intelligence navigation system for the SSBE probe cruise phase. The main advantage of the QLFEKF is that Q-learning combined with the conventional federated filtering method could optimize the state parameters in real-time and obtain high position and velocity state estimation (PVSE) accuracy. Compared with the conventional FEKF integrated navigation algorithm, the PVSE navigation accuracy of the federated filter integrated based the Q-learning navigation algorithm is improved by 55.84% and 37.04%, respectively, demonstrating the higher accuracy and greater capability of the raised autonomous intelligent integrated navigation algorithm. The simulation results show that the intelligent integrated navigation algorithm based on QLFEKF has higher navigation accuracy and is able to satisfy the demands of autonomous high accuracy for the SSBE cruise phase. Full article
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<p>The fundamental principle of the X-ray pulsar measurement pulse TOA.</p>
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<p>The basic principle of the solar/target planetary object Doppler velocity measurement.</p>
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<p>Intelligent information interaction with the flight environment for the PA.</p>
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<p>Collections of states and corresponding collections for actions for the QLFEKF. The shaded areas denote various combinations of the state and observation noise error covariance matrices <b><span class="html-italic">Q</span></b><span class="html-italic"><sub>k</sub></span> and <b><span class="html-italic">R</span></b><span class="html-italic"><sub>k</sub></span><sub>.</sub> The arrows represent the transitions between different states, and it means choosing different actions.</p>
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<p>Structure diagram of the <span class="html-italic">Q</span>-learning-based FEKF intelligent integrated navigation.</p>
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<p>Comparison of the position estimate RMSEs between STD/XP-QLFEKF and other integrated navigation algorithms.</p>
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<p>Comparison of the position estimate RMSEs for three axes between STD/XP-QLFEKF and other integrated navigation algorithms.</p>
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<p>Comparison of the velocity estimate RMSEs between STD/XP-QLFEKF and other integrated navigation algorithms.</p>
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<p>Comparison of the velocity estimate RMSEs based on three axes between STD/XP-QLFEKF and other integrated navigation algorithms.</p>
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<p>The PVSE RMSE errors (3<span class="html-italic">σ</span>) of the cruise phase as a function of the learning rate.</p>
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<p>The PVSE RMSE errors (3<span class="html-italic">σ</span>) of the cruise phase as a function of the discount factor.</p>
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<p>The PVSE RMSE errors (3<span class="html-italic">σ</span>) for the cruise phase as s function of the action selection probability.</p>
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<p>The influence of different iteration cycles of the reinforcement <span class="html-italic">Q</span>-learning on the precision of the PVSE errors in the probe’s cruise phase.</p>
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14 pages, 3419 KiB  
Article
Multievent Correlation with Neutron Volume Detectors
by Noah Nachtigall, Andreas Houben and Richard Dronskowski
Quantum Beam Sci. 2024, 8(4), 30; https://doi.org/10.3390/qubs8040030 - 28 Nov 2024
Viewed by 290
Abstract
The development of advanced volume detectors for neutron time-of-flight diffractometers offers exciting new possibilities. This work takes advantage of these advances by implementing a novel data preprocessing algorithm, exemplified for the first time with data acquired during the operation of a singular mounting [...] Read more.
The development of advanced volume detectors for neutron time-of-flight diffractometers offers exciting new possibilities. This work takes advantage of these advances by implementing a novel data preprocessing algorithm, exemplified for the first time with data acquired during the operation of a singular mounting unit of the POWTEX detector placed at the POWGEN instrument (SNS, ORNL, Oak Ridge, TN, USA). Our approach exploits the additional depth information provided by the volume detector needed to correlate multiple neutron events to neutron trajectories of similar origin and probability. By comparing the properties of these trajectories with the expected physical behavior, one may first identify, then label, and ultimately remove unwanted events due to phenomena such as secondary scattering within the sample environment. This capability has the potential to significantly improve the quality and information content of data collected with neutron diffractometers. Full article
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<p>Sketch of the single POWTEX detector mounting unit used in the POWTEX@POWGEN experiment, depicting 3D view, top view, and side view. Cartesian coordinates are also included, as well as the unique POWTEX detector coordinates dubbed <span class="html-italic">S</span>, <span class="html-italic">a</span>, <span class="html-italic">e</span>, and <span class="html-italic">N</span>. Since the detector coordinates are multiples of physical, detector-internal building blocks (cathode stripes, anode wires, modules, etc.), they are unitless in principle but geometrically linked to Cartesian or spherical coordinate systems. The important depth direction is <span class="html-italic">a</span> whereas the direction corresponding to 2<span class="html-italic">θ</span> is <span class="html-italic">S</span>. <span class="html-italic">N</span> divides each mounting unit into eight modules, and each module is internally divided into a lower and an upper side named <span class="html-italic">e</span>. This direction corresponds to the texture angle <span class="html-italic">φ</span>. The direction of the primary neutron beam from the source toward the sample is aligned with the positive <span class="html-italic">z</span> direction.</p>
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<p>(<b>a</b>) Intensity vs. <span class="html-italic">d</span> diffractogram of a diamond powder measurement from the POWTEX@POWGEN experiment (black) with added artificial secondary scatterer intensity (red-shaded area). (<b>b</b>) Top view demonstration of how this secondary scatterer might have been positioned relative to the sample (exaggerated dimensions).</p>
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<p>(<b>a</b>) Perspective view of a Debye–Scherrer cone as a ring on a conventional flat-plate detector. (<b>b</b>) Orthographic view of a Debye–Scherrer cone, illustrating the multiple pass-throughs in a volume detector (right) versus the single pass-through for a plate detector (center).</p>
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<p>(<b>a</b>) Top view of the detector (<span class="html-italic">a</span> vs. <span class="html-italic">S</span>) with different exemplary trajectories of equivalently scattered neutrons at different 2<span class="html-italic">θ</span> values (for one arbitrary wavelength). (<b>b</b>) Side view (<span class="html-italic">N</span>/<span class="html-italic">e</span> vs. <span class="html-italic">a</span>) showing a single trajectory’s flight path and how this translates into a depth–intensity expectation (<span class="html-italic">I</span> vs. <span class="html-italic">a</span>). Note that in this simplified picture, in some of the voxels the trajectory corresponding to the black arrow causes intensity, although no interaction with the boron conversion layer (thin lines) occurs, simply because the single arrow does not reflect the angular uncertainty.</p>
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<p>The color-scaled intensity plotted against the instrument’s voxel identifiers <span class="html-italic">a</span> and <span class="html-italic">S</span> illustrates how reflections “move” along the detector with λ. The two plots show the same reflections around <span class="html-italic">d</span> = 0.47 Å ± 0.05 Å but for two different wavelengths. In addition, the detector design implies that a reflection shift toward higher <span class="html-italic">S</span>-values can be observed at higher <span class="html-italic">a</span>-values.</p>
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<p>The color-scaled intensity plot against the <span class="html-italic">a</span> and <span class="html-italic">S</span>′ reveals the presence (<b>a</b>) of three straight vertical reflections with a width of two to four stripes but (<b>b</b>) one additional, extensively broadened reflection. The three straight reflections from the primary scatterer exhibit a distinct and consistent decline in intensity. In contrast, the broad contribution from the secondary scatterer is notable with clearly different nature including a markedly different intensity reduction with depth for each <span class="html-italic">S</span>′.</p>
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<p>Intensity plots showing the original unedited diffraction data (black) and the diffraction data with an added secondary scatterer (red). (<b>a</b>) Normalized intensity plotted against the depth identifier <span class="html-italic">a</span> for a select number of <span class="html-italic">S</span>′ values showing an <span class="html-italic">S</span>′ value without secondary intensity (<span class="html-italic">S</span>′ = 28) and <span class="html-italic">S</span>′ values with secondary intensity (<span class="html-italic">S</span>′ = 28–34). (<b>b</b>) Intensity plotted against the wavelength for one single <span class="html-italic">S</span>′ = 39.</p>
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<p>Color-scaled intensity plots after removing bad event data. (<b>a</b>) Intensity vs. <span class="html-italic">a</span> and <span class="html-italic">S</span>′ (see <a href="#qubs-08-00030-f006" class="html-fig">Figure 6</a> for comparison). (<b>b</b>) Intensity vs. <span class="html-italic">d</span> diffractogram with the optimized intensity in black, the original data with the secondary scatterer intensity in red and the leftover bad intensity in blue.</p>
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26 pages, 5172 KiB  
Article
Nighttime Lights and Population Variations in Cities of South/Southeast Asia: Distance-Decay Effect and Implications
by Griffin McAvoy and Krishna P. Vadrevu
Remote Sens. 2024, 16(23), 4458; https://doi.org/10.3390/rs16234458 - 27 Nov 2024
Viewed by 322
Abstract
Urbanization in South and Southeast Asia is accelerating due to economic growth, industrialization, and rural-to-urban migration, with megacities like Mumbai, Delhi, and Jakarta leading the trend. By analyzing VIIRS nighttime satellite data from 323 cities across 17 countries, we investigated the relationship between [...] Read more.
Urbanization in South and Southeast Asia is accelerating due to economic growth, industrialization, and rural-to-urban migration, with megacities like Mumbai, Delhi, and Jakarta leading the trend. By analyzing VIIRS nighttime satellite data from 323 cities across 17 countries, we investigated the relationship between nighttime light (NTL) brightness and population density at varying distances from city centers. Our findings reveal a significant distance-decay effect, with both the intensity of NTL brightness and the strength of the NTL-population density relationship decreasing as the distance from city centers increases. A clear negative exponential relationship with the highest R2 was observed between NTL brightness and the distance from the city center. Our analysis indicates that a 105 km radius most effectively captures the extent of major metropolitan areas, showing a peak correlation between NTL brightness and population density. Cities like Delhi and Bangkok exhibit high NTL brightness, reflecting advanced infrastructure, while mountainous or desert cities such as Kabul and Thimphu show lower brightness due to geographical constraints. These results highlight the importance of adaptive urban planning, infrastructure development, and sustainability practices in managing urbanization challenges in South and Southeast Asia. Full article
(This article belongs to the Special Issue Nighttime Light Remote Sensing Products for Urban Applications)
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<p>Countries and cities in South/Southeast Asia. A total of 323 cities spread across 17 different countries were studied to analyze population and nighttime light brightness patterns. Map lines delineate study areas and do not necessarily depict accepted national boundaries.</p>
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<p>The average nighttime light brightness of the corrected cities at different buffer sizes, before and after AOD correction was applied.</p>
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<p>Flowchart summarizing the data processing workflow.</p>
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<p>The top ten most populous cities in South and Southeast Asian countries within 30 km (<b>a</b>) and 60 km (<b>b</b>) radii from the city center.</p>
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<p>Top ten cities in nighttime light brightness in South and Southeast Asian countries at 30 (<b>a</b>) and 60 km (<b>b</b>) radii from the city center.</p>
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<p>Landscape heterogeneity in different cities of South/Southeast Asia with a 60 km radius from the city center. Significant variations in city size and green cover are evident. The mountainous cities of Kabul (<b>a</b>) and Thimpu (<b>b</b>) are typically much smaller than the other cities, due to the external limitations of the surrounding harsh terrain. An uneven distribution of green space can be seen in Delhi (<b>c</b>), Dhaka (<b>d</b>), and Ho Chi Minh City (<b>e</b>). The cities of Singapore (<b>f</b>), Kuala Lumpur (<b>g</b>), and Bangkok (<b>h</b>) border the ocean within a 60 km radius.</p>
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<p>Nighttime light brightness variations with buffer radius from the city center in different capital cities of South/Southeast Asia as retrieved from the VIIRS instrument on the Suomi-NPP satellite. New Delhi, Singapore, and Bangkok had the highest NTL brightness, and Timor-Leste and Bhutan had the lowest NTL brightness.</p>
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<p>(<b>a</b>–<b>h</b>) Nighttime light brightness variations from the city center in different countries of South Asia, as retrieved from the VIIRS Suomi-NPP. The original data are shown as a black dotted line. A relatively higher brightness can be observed for India (<b>d</b>) and Pakistan (<b>g</b>) compared to other countries. A clear negative exponential relationship can be observed in the nighttime light brightness with the increase in the distance from the city center (fitted line in dark red). In the equation, * denotes multiplication. The plot also shows confidence (dark red) and prediction (light red) bands of the data with 95% confidence.</p>
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<p>(<b>a</b>–<b>i</b>) Nighttime light brightness variations with buffer radius from the city center in different countries of Southeast Asia, as retrieved from the VIIRS Suomi-NPP. The original data are shown as a black dotted line. Relatively higher brightness can be observed in Malaysia (<b>d</b>), the Philippines (<b>e</b>), and Singapore (<b>f</b>) compared to other countries. A clear negative exponential relationship can be seen in the nighttime light brightness with the increase in the distance from the city center (fitted line in dark red). In the equation, * denotes multiplication. The plot also shows confidence (dark red) and prediction (light red) bands of the data with 95% confidence.</p>
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<p>(<b>a</b>–<b>j</b>) Nighttime light brightness versus total population correlations at different buffer radii from the city center for all South/Southeast Asian countries. The original data are shown as blue dots and the linear fit as a red line. A relatively higher correlation can be found at a 60 km radius. The plot also shows confidence (light red) and prediction (light green) bands of the data with 95% confidence.</p>
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<p>Changing proportion of land cover types as buffer radius increases. The forest includes all evergreen, deciduous, broadleaf, needle leaf, and mixed forests; other natural vegetation includes shrublands, savannahs, grasslands, and wetlands; agricultural area designates cropland and mosaics of cropland and natural vegetation; urban refers to built areas; and other denotes permanent snow/ice, barren land, and/or open water.</p>
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33 pages, 5587 KiB  
Article
Full Envelope Control of Over-Actuated Fixed-Wing Vectored Thrust eVTOL
by Emmanuel Enenakpogbe, James F. Whidborne and Linghai Lu
Aerospace 2024, 11(12), 979; https://doi.org/10.3390/aerospace11120979 - 27 Nov 2024
Viewed by 251
Abstract
A novel full-envelope controller for an over-actuated fixed-wing vectored thrust eVTOL aircraft is presented. It proposes a generic control architecture, which is applicable to piloted, semi-automatic, and fully automated flight, consisting of an aircraft-level controller (high-level controller) and a control allocation scheme. The [...] Read more.
A novel full-envelope controller for an over-actuated fixed-wing vectored thrust eVTOL aircraft is presented. It proposes a generic control architecture, which is applicable to piloted, semi-automatic, and fully automated flight, consisting of an aircraft-level controller (high-level controller) and a control allocation scheme. The aircraft-level controller consists of a main inner loop classical nonlinear dynamic inversion controller and an outer loop proportional–integral linear controller. The inner loop nonlinear dynamic inversion controller is a velocity controller that cancels the nonlinear bare airframe dynamics, while the outer loop proportional–integral linear controller is an attitude and navigation position controller. Together, they are used for hover/low-speed control and forward flight. The control allocation scheme uses a novel architecture, which transfers the nonlinearity in the vectored thrust effector model formulation to the computation of the actuator limits by converting the effector model from polar to rectangular form, thus allowing the use of classical control allocation linear optimisation technique. The linear optimisation technique is an active set linear quadratic programming constrained optimisation algorithm with a weighted least squares formulation. The control allocation allocates the overall control demand (virtual controls) to individual redundant effectors while performing control error minimisation, control channel prioritisation and control effort minimisation. Simulation results show the transition from hover to cruise, climb and descent, and coordinated turn clearly demonstrate that the controller can handle actuator saturation (position or rate). Full article
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<p>Aircraft planform showing EDF set distribution.</p>
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<p>Aerodynamic blending coefficient.</p>
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<p>Generic flight controller architecture for piloted, semi-automatic, and automated flight [<a href="#B49-aerospace-11-00979" class="html-bibr">49</a>].</p>
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<p>Command generator and outer loop controller.</p>
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<p>NDI problem formulation.</p>
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<p>The 6DoF CA functional architecture.</p>
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<p>Plan view of Lilium-style fixed-wing over-actuated vectored thrust eVTOL aircraft configuration showing EDF set distribution, control groupings, and real controls.</p>
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<p>Vectored thrust actuator limit illustration.</p>
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<p>Thrust (T) and tilting mechanism (<math display="inline"><semantics> <mo>Γ</mo> </semantics></math>) actuator dynamics.</p>
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<p>VTO, forward transition—attitude.</p>
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<p>VTO, forward transition—velocity.</p>
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<p>VTO, forward transition—effector commands.</p>
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<p>VTO, forward transition—acceleration.</p>
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<p>VTO, forward transition—control limitation status.</p>
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<p>Cruise, reverse transition, and VL with heading change—attitude.</p>
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<p>Cruise, reverse transition, and VL with heading change—velocity.</p>
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<p>Cruise, reverse transition, and VL with heading change—effector commands.</p>
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<p>Cruise, reverse transition, and VL with heading change—acceleration.</p>
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<p>Cruise, reverse transition, and VL with heading change—control limitation status.</p>
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<p>Climb, descend—attitude.</p>
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<p>Climb, descend—velocity.</p>
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<p>Climb, descend—effector commands.</p>
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<p>Climb, Descend—Acceleration.</p>
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<p>Climb, descend—control limitation status.</p>
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<p>Cruise and coordinated turn—attitude.</p>
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<p>Cruise and coordinated turn—velocity.</p>
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<p>Cruise and coordinated turn—effector commands.</p>
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<p>Cruise and coordinated turn—acceleration.</p>
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<p>Cruise and coordinated turn—control limitation status.</p>
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27 pages, 2988 KiB  
Article
UAV Mission Computer Operation Mode Optimization Focusing on Computational Energy Efficiency and System Responsiveness
by Oleksandr Liubimov, Ihor Turkin, Valeriy Cheranovskiy and Lina Volobuieva
Computation 2024, 12(12), 235; https://doi.org/10.3390/computation12120235 - 27 Nov 2024
Viewed by 294
Abstract
The rising popularity of UAVs and other autonomous control systems coupled with real-time operating systems has increased the complexity of developing systems with the proper robustness, performance, and reactivity. The growing demand for more sophisticated computational tasks, proportionally larger payloads, battery limitations, and [...] Read more.
The rising popularity of UAVs and other autonomous control systems coupled with real-time operating systems has increased the complexity of developing systems with the proper robustness, performance, and reactivity. The growing demand for more sophisticated computational tasks, proportionally larger payloads, battery limitations, and smaller take-off mass requires higher energy efficiency for all avionics and mission computers. This paper aims to develop a technique for experimentally studying the indicators of reactivity and energy consumption in a computing platform for unmanned aerial vehicles (UAVs). The paper provides an experimental assessment of the `Boryviter 0.1’ computing platform, which is implemented on the ATSAMV71 microprocessor and operates under the open-source FreeRTOS operating system. The results are the basis for developing algorithms and energy-efficient design strategies for the mission computer to solve the optimization problem. This paper provides experimental results of measurements of the energy consumed by the microcontroller and estimates of the reduction in system energy consumption due to additional time costs for suspending and resuming the computer’s operation. The results show that the `Boryviter 0.1’ computing platform can be used as a UAV mission computer for typical flight control tasks requiring real-time computing under the influence of external factors. As a further work direction, we plan to investigate the proposed energy-saving algorithms within the planned NASA F’Prime software flight framework. Such an investigation, which should use the mission computer’s actual flight computation load, will help to qualify the obtained energy-saving methods and their implementation results. Full article
18 pages, 8007 KiB  
Article
Spectral Response Function Retrieval of Spaceborne Fourier Transform Spectrometers: Application to Metop-IASI
by Pierre Dussarrat, Guillaume Deschamps and Dorothee Coppens
Remote Sens. 2024, 16(23), 4449; https://doi.org/10.3390/rs16234449 - 27 Nov 2024
Viewed by 300
Abstract
In the past decades, satellite hyperspectral remote sensing instruments have been providing key measurements for environmental monitoring, such as the analysis of water and air quality, soil usage, weather forecasting, or climate change. The success of this technology, however, relies on an accurate [...] Read more.
In the past decades, satellite hyperspectral remote sensing instruments have been providing key measurements for environmental monitoring, such as the analysis of water and air quality, soil usage, weather forecasting, or climate change. The success of this technology, however, relies on an accurate knowledge of the instrument’s spectral response functions (SRFs). Usually, the SRFs are assessed on-ground and then monitored on-flight using tedious analysis of the acquired radiances coupled with instrumental models; nonetheless, the complete retrieval of the SRFs is generally out of reach. In this context, EUMETSAT has developed a novel SRF retrieval methodology, with the intention of applying it routinely to the current Metop IASI instruments and soon to Metop-SG IASI-NG, and MTG-S IRS. By making use of spatiotemporal colocations of different detectors within a single instrument or between different platforms, relative SRFs may be retrieved on-flight without any a priori knowledge. The presented methodology is suited for instruments acquiring radiances with contiguous sampling over large spectral bands as the SRFs are retrieved by analyzing the neighboring channels’ correlations. This article focuses on Fourier transform spectrometers (FTS) in the far infrared as they possess these characteristics per design, but it is believed that the method could be extended to other technology and spectral bands. The SRFs are further processed to evaluate the relative self-apodization functions (SAFs), as they represent the discrepancies between the detectors at the interferograms level, the primary measurements of FTS. The following article presents both simulations and applications of the SRF retrieval for the three IASI instruments aboard the Metop platforms of the EPS program. We analyze both IASI sensors aboard Metop-B and C as well as the evolution of Metop-A IASI over 13 years of operation. Full article
(This article belongs to the Special Issue Remote Sensing Satellites Calibration and Validation)
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<p>Example of a few spectral radiances <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>y</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> <mo> </mo> </mrow> </semantics></math>acquired by Metop-C IASI (<b>left</b>) as a function of the wavenumber (one over the wavelength) and associated covariance matrix <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo> </mo> </mrow> </semantics></math>(<b>right</b>).</p>
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<p>Example of covariance matrix <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo> </mo> </mrow> </semantics></math>(<b>left</b>) and its subset version <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>11</mn> <mo>,</mo> <mi>s</mi> <mi>u</mi> <mi>b</mi> </mrow> </msub> </mrow> </semantics></math> (<b>right</b>) with <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>N</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> <mo>=</mo> <mn>2167</mn> <mo> </mo> </mrow> </semantics></math>and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>N</mi> </mrow> <mrow> <mi>c</mi> <mo>,</mo> <mi>s</mi> <mi>u</mi> <mi>b</mi> </mrow> </msub> <mo>=</mo> <mn>21</mn> </mrow> </semantics></math> (not at scale).</p>
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<p>Example of conversion from the retrieved SRF matrix (<b>left</b>) to a single SRF vector by extraction of its central line (<b>right</b>), with <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>N</mi> </mrow> <mrow> <mi>c</mi> <mo>,</mo> <mi>s</mi> <mi>u</mi> <mi>b</mi> </mrow> </msub> <mo>=</mo> <mn>21</mn> </mrow> </semantics></math>.</p>
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<p>SAF retrieval and simulation using IASI data without colocation errors. Average radiance per sub-band (<b>top</b>), real part of the SAF (<b>middle</b>), and imaginary part of the SAF (<b>bottom</b>).</p>
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<p>SAF retrieval and simulation using IASI data with colocation errors (~24 km). Average radiance per sub-band (<b>top</b>), real part of the SAF (<b>middle</b>), and imaginary part of the SAF (<b>bottom</b>).</p>
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<p>Metop-B IASI relative SAF of each of the 4 FOVs with respect to the 3 others (blue, red, gold, purple). Average radiance per sub-band (<b>top</b>), real part of the SAF (<b>middle</b>), and imaginary part of the SAF (<b>bottom</b>).</p>
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<p>Metop-C IASI relative SAF of each of the 4 FOVs with respect to the 3 others (blue, red, gold, purple). Average radiance per sub-band (<b>top</b>), real part of the SAF (<b>middle</b>), and imaginary part of the SAF (<b>bottom</b>).</p>
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<p>Metop-B and C IASI average radiometric error induced by the SAF discrepancies expressed in Kelvin for each FOV of view (blue, red, gold, purple). The dashed lines delimit the 6 sub-bands used in the computations.</p>
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<p>Relative SAF retrieval of Metop-A IASI over 13 years of operation, real and imaginary parts for 6 sub-bands (from 2017: blue to 2020: red), FOV#1 to 4 (top to bottom).</p>
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<p>SAF standard deviation of Metop-A IASI over 13 years of operation for each FOV with respect to the others and 6 spectral sub-bands, from 2007 to 2020.</p>
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<p>Relative SAF between IASI-B and C instruments (Metop-C is taken as the reference). Average radiance per sub-band (<b>top</b>), real part of the SAF (<b>middle</b>), and imaginary part of the SAF (<b>bottom</b>).</p>
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