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Topic Editors

Institute of Mechanical Engineering, Faculty of Mechanical Engineering, Bialystok University of Technology, 15-351 Bialystok, Poland
Institute of Robotics and Machine Intelligence, Faculty of Control, Robotics and Electrical Engineering, Poznan University of Technology, 60-965 Poznan, Poland
Department of Automatic Control and Robotics, Faculty of Electrical Engineering, Bialystok University of Technology, Wiejska 45D street, 15-351 Bialystok, Poland
Faculty of Mechanical Engineering, Lublin University of Technology, Nadbystrzycka 36, 20-618 Lublin, Poland
Department of Computer-Aided Design Systems, Lviv Polytechnic National University, 5 Mytropolyta Andreya St., building 4, 79013 Lviv, Ukraine

Design, Simulation and New Applications of Unmanned Aerial Vehicles

Abstract submission deadline
closed (31 May 2023)
Manuscript submission deadline
closed (31 August 2023)
Viewed by
160754

Topic Information

Dear Colleagues,

As the Editor of the Special Issue “Design, Simulation and New Applications of Unmanned Aerial Vehicles”, I would like to invite you to submit a paper on this subject. Recently, we have experienced a huge increase in the development of unmanned aerial vehicles (UAVs). Every month brings new scientific papers pertaining to UAVs, which have become an even stronger accelerator for research in this field. This Special Issue aims to contribute to the development of unmanned aerial vehicles in many areas. Particular attention will be given to high-quality papers that address significant advances in the design, modeling, and control of UAVs, as well as novel applications. Potential topics include, but are not limited to, the following:

  • UAV design;
  • CAx systems in UAV design;
  • Efficiency of UAV platform;
  • FEA in UAV design;
  • CFD analysis of UAV;
  • Fiber composites in UAV;
  • MEMS in UAS;
  • Sensors in UAV;
  • UGV and UAV collaboration;
  • Multirotor UAV;
  • UAV navigation;
  • Machine learning for UAV autonomous control;
  • UAV dynamics, control and simulation;
  • New applications for UAVs;
  • Embedded systems design for UAVs;
  • UAS electronics design;
  • Algorithms and software for UAV/UAS.

Dr. Andrzej Łukaszewicz
Prof. Dr. Wojciech Giernacki
Prof. Dr. Zbigniew Kulesza
Prof. Dr. Jaroslaw Alexander Pytka
Dr. Andriy Holovatyy
Topic Editors

Keywords

  • UAV design
  • UAV airframe
  • UAV strength analysis
  • CAx systems in UAV design
  • efficiency of UAV platform
  • FEA in UAV design
  • CFD analysis of UAV
  • smart materials in UAV
  • fiber composites in UAV
  • MEMS in UAS
  • sensors in UAV
  • UGV and UAV collaboration
  • multirotor UAV
  • UAV navigation
  • dynamics of UAVs
  • machine learning for UAV autonomous control
  • UAV control and simulation
  • new application for UAVs
  • MEMS sensors design for UAVs
  • embedded systems design for UAVs
  • UAS electronics design
  • algorithms and software for UAV/UAS

Participating Journals

Journal Name Impact Factor CiteScore Launched Year First Decision (median) APC
Applied Sciences
applsci
2.7 4.5 2011 16.9 Days CHF 2400
Drones
drones
4.8 6.1 2017 17.9 Days CHF 2600
Energies
energies
3.2 5.5 2008 16.1 Days CHF 2600
Machines
machines
2.6 2.1 2013 15.6 Days CHF 2400
Materials
materials
3.4 5.2 2008 13.9 Days CHF 2600
Sensors
sensors
3.9 6.8 2001 17 Days CHF 2600

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Published Papers (50 papers)

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27 pages, 2317 KiB  
Review
Power Sources for Unmanned Aerial Vehicles: A State-of-the Art
by Yavinaash Naidu Saravanakumar, Mohamed Thariq Hameed Sultan, Farah Syazwani Shahar, Wojciech Giernacki, Andrzej Łukaszewicz, Marek Nowakowski, Andriy Holovatyy and Sławomir Stępień
Appl. Sci. 2023, 13(21), 11932; https://doi.org/10.3390/app132111932 - 31 Oct 2023
Cited by 2 | Viewed by 2725
Abstract
Over the past few years, there has been an increasing fascination with electric unmanned aerial vehicles (UAVs) because of their capacity to undertake demanding and perilous missions while also delivering advantages in terms of flexibility, safety, and expenses. These UAVs are revolutionizing various [...] Read more.
Over the past few years, there has been an increasing fascination with electric unmanned aerial vehicles (UAVs) because of their capacity to undertake demanding and perilous missions while also delivering advantages in terms of flexibility, safety, and expenses. These UAVs are revolutionizing various public services, encompassing real-time surveillance, search and rescue operations, wildlife assessments, delivery services, wireless connectivity, and precise farming. To enhance their efficiency and duration, UAVs typically employ a hybrid power system. This system integrates diverse energy sources, such as fuel cells, batteries, solar cells, and supercapacitors. The selection of an appropriate hybrid power arrangement and the implementation of an effective energy management system are crucial for the successful functioning of advanced UAVs. This article specifically concentrates on UAV platforms powered by batteries, incorporating innovative technologies, like in-flight recharging via laser beams and tethering. It provides an all-encompassing and evaluative examination of the current cutting-edge power supply configurations, with the objective of identifying deficiencies, presenting perspectives, and offering recommendations for future consideration in this domain. Full article
Show Figures

Figure 1

Figure 1
<p>Two types of drones: (<b>a</b>) fixed-wing drone, (<b>b</b>) rotary-wing drone.</p>
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<p>A typical UAV block diagram [<a href="#B64-applsci-13-11932" class="html-bibr">64</a>].</p>
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<p>UAV propulsion system block diagram.</p>
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<p>The swapping and hot swapping algorithms.</p>
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<p>A laser-powered UAV inflight charging system [<a href="#B54-applsci-13-11932" class="html-bibr">54</a>,<a href="#B58-applsci-13-11932" class="html-bibr">58</a>,<a href="#B68-applsci-13-11932" class="html-bibr">68</a>].</p>
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<p>The fuel cell system auxiliaries.</p>
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17 pages, 5197 KiB  
Article
Curved-Line Path-Following Control of Fixed-Wing Unmanned Aerial Vehicles Using a Robust Disturbance-Estimator-Based Predictive Control Approach
by Weiwei Qi, Mingbo Tong, Qi Wang, Wei Song and Hunan Ying
Appl. Sci. 2023, 13(20), 11577; https://doi.org/10.3390/app132011577 - 23 Oct 2023
Viewed by 840
Abstract
In this research, the design of a robust curved-line path-following control system for fixed-wing unmanned aerial vehicles (FWUAVs) affected by uncertainties on the latitude plane is studied. This is undertaken to enhance closed-loop system robustness under unknown uncertainties and derive the control surface [...] Read more.
In this research, the design of a robust curved-line path-following control system for fixed-wing unmanned aerial vehicles (FWUAVs) affected by uncertainties on the latitude plane is studied. This is undertaken to enhance closed-loop system robustness under unknown uncertainties and derive the control surface deflection angle directly used to control FWUAVs, which has rarely been studied in previous works. The system is formed through the mass center position control (MCPC) and yaw angle control (YAC) subsystems. In the MCPC, the desired yaw angle, which is treated as the reference signal for the YAC subsystem, is calculated analytically using path-following errors, current flow angles, and the yaw angle. In the YAC, a disturbance estimator is designed to estimate uncertainties such as nonlinearities, couplings, time variations, model parameter perturbations, and unmodeled dynamics. Predictive functional controllers are designed to target nominal systems in the absence of uncertainties, such that the estimations of the uncertainties can be incorporated through feedback for closed-loop system robustness enhancement. The simulation results show that higher path-following precision and stronger robustness for the FWUAVs based on the proposed approach can be achieved using only rough model parameters compared with the conventional nonlinear dynamic inversion, which requires detailed model information. Full article
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Figure 1

Figure 1
<p>Path following on the latitude plane.</p>
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<p>Path−following effect.</p>
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<p>Path−following errors.</p>
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<p>Control laws.</p>
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<p>Uncertainty estimation and estimation error <math display="inline"><semantics> <mrow> <msub> <mi>e</mi> <mi>r</mi> </msub> <mo>=</mo> <msub> <mi>f</mi> <mi>r</mi> </msub> <mo>−</mo> <msub> <mrow> <mover accent="true"> <mi>f</mi> <mo stretchy="true">^</mo> </mover> </mrow> <mi>r</mi> </msub> </mrow> </semantics></math>.</p>
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<p>Yaw angles: proposed approach.</p>
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<p>Yaw angles: the NDI approach.</p>
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<p>Yaw rates.</p>
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<p>Path−following effects.</p>
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<p>Path−following errors.</p>
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<p>Control laws.</p>
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<p>Uncertainty estimation: +30% and estimation error <math display="inline"><semantics> <mrow> <msub> <mi>e</mi> <mi>r</mi> </msub> <mo>=</mo> <msub> <mi>f</mi> <mi>r</mi> </msub> <mo>−</mo> <msub> <mrow> <mover accent="true"> <mi>f</mi> <mo stretchy="true">^</mo> </mover> </mrow> <mi>r</mi> </msub> </mrow> </semantics></math>.</p>
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<p>Uncertainty estimations: −30% and estimation error <math display="inline"><semantics> <mrow> <msub> <mi>e</mi> <mi>r</mi> </msub> <mo>=</mo> <msub> <mi>f</mi> <mi>r</mi> </msub> <mo>−</mo> <msub> <mrow> <mover accent="true"> <mi>f</mi> <mo stretchy="true">^</mo> </mover> </mrow> <mi>r</mi> </msub> </mrow> </semantics></math>.</p>
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<p>Yaw angles: +30%.</p>
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<p>Yaw angles: −30%.</p>
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<p>Yaw rates.</p>
Full article ">
21 pages, 8997 KiB  
Article
Rapid Deployment Method for Multi-Scene UAV Base Stations for Disaster Emergency Communications
by Rui Gao and Xiao Wang
Appl. Sci. 2023, 13(19), 10723; https://doi.org/10.3390/app131910723 - 27 Sep 2023
Viewed by 1174
Abstract
The collaborative deployment of multiple UAVs is a crucial issue in UAV-supported disaster emergency communication networks, as utilizing these UAVs as air base stations can greatly assist in restoring communication networks within disaster-stricken areas. In this paper, the problem of rapid deployment of [...] Read more.
The collaborative deployment of multiple UAVs is a crucial issue in UAV-supported disaster emergency communication networks, as utilizing these UAVs as air base stations can greatly assist in restoring communication networks within disaster-stricken areas. In this paper, the problem of rapid deployment of randomly distributed UAVs in disaster scenarios is studied, and a distributed rapid deployment method for UAVs´ emergency communication network is proposed; this method can cover all target deployment points while maintaining connectivity and provide maximum area coverage for the emergency communication network. To reduce the deployment complexity, we decoupled the three-dimensional UAV deployment problem into two dimensions: vertical and horizontal. For this small-area deployment scenario, a small area UAVs deployment improved-Broyden–Fletcher–Goldfarb–Shanno (SAIBFGS) algorithm is proposed via improving the Iterative step size and search direction to solve the high computational complexity of the traditional Broyden–Fletcher–Goldfarb–Shanno (BFGS) algorithm. In a large area deployment scenario, aiming at the problem of the premature convergence of the standard genetic algorithm (SGA), the large-area UAVs deployment elitist strategy genetic algorithm (LAESGA) is proposed through the improvement of selection, crossover, and mutation operations. The adaptation function of connectivity and coverage is solved by using SAIBFGS and LAESGA, respectively, in the horizontal dimension to obtain the optimal UAV two-dimensional deployment coordinates. Then, the transmitting power and height of the UAV base station are dynamically adjusted according to the channel characteristics and the discrete coefficients of the ground users to be rescued in different environments, which effectively improves the power consumption efficiency of the UAV base station and increases the usage time of the UAV base station, realizing the energy-saving deployment of the UAV base station. Finally, the effectiveness of the proposed method is verified via data transmission rate simulation results in different environments. Full article
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Figure 1

Figure 1
<p>Communication network model of UAV base stations.</p>
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<p>Plot of path loss versus horizontal distance.</p>
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<p>Schematic of the selected operation.</p>
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<p>Fitness curve of iteration number and the Euclid distance between UAVs and target deployment points. (<b>a</b>) Fitness curve for 500 m × 500 m area UAV deployment (eight UAVs); (<b>b</b>) fitness curve for 1500 m × 1500 m area UAV deployment (eight UAVs); (<b>c</b>) fitness curve for 2500 m × 2500 m area UAV deployment (eight UAVs); (<b>d</b>) fitness curve for 4000 m × 4000 m area UAV deployment (10 UAVs).</p>
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<p>Comparison of average computing time.</p>
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<p>A simulated representation of the deployment of small area UAVs. (<b>a</b>) UAVs initial deployment of small area; (<b>b</b>) UAVs final deployment results under the small area LAESGA algorithm; (<b>c</b>) UAVs final deployment results under the small area SAIBFGS algorithm; (<b>d</b>) UAVs final deployment results under the small area SGA algorithm.</p>
Full article ">Figure 7
<p>A simulated representation of the deployment of large-area UAVs. (<b>a</b>) UAVs´ initial deployment in the large area; (<b>b</b>) UAVs´ final deployment results under the large area LAESGA algorithm; (<b>c</b>) UAVs´ final deployment results under the large area SAIBFGS algorithm; (<b>d</b>) UAVs´ final deployment results under the large area SGA algorithm.</p>
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<p>The relationship between the height of the UAV base station and the discrete coefficient of ground users to be rescued.</p>
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<p>The relationship between the launch power of UAVs base station and the discrete coefficient of ground users to be rescued.</p>
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<p>The data transmission rate of UAVs base station in urban environment: (<b>a</b>) 100 m hover height deployment and 40 dBm launch power; (<b>b</b>) 200 m hover height deployment and 60 dBm launch power.</p>
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<p>The data transmission rate of UAVs base station in suburban environment: (<b>a</b>) 160 m hover height deployment and 30 dBm launch power; (<b>b</b>) 200 m hover height deployment and 60 dBm launch power.</p>
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<p>The data transmission rate of UAVs base station in rural environment: (<b>a</b>) 200 m hover height deployment and 20 dBm launch power; (<b>b</b>) 200 m hover height deployment and 60 dBm launch power.</p>
Full article ">
20 pages, 12294 KiB  
Article
Research on Scenario Modeling for V-Tail Fixed-Wing UAV Dynamic Obstacle Avoidance
by Peihao Huang, Yong Tang, Bingsan Yang and Tao Wang
Drones 2023, 7(10), 601; https://doi.org/10.3390/drones7100601 - 25 Sep 2023
Cited by 1 | Viewed by 3517
Abstract
With the advantages of long-range flight and high payload capacity, large fixed-wing UAVs are often used in anti-terrorism missions, disaster surveillance, and emergency supply delivery. In the existing research, there is little research on the 3D model design of the V-tail fixed-wing UAV [...] Read more.
With the advantages of long-range flight and high payload capacity, large fixed-wing UAVs are often used in anti-terrorism missions, disaster surveillance, and emergency supply delivery. In the existing research, there is little research on the 3D model design of the V-tail fixed-wing UAV and 3D flight environment modeling. The study focuses on designing a comprehensive simulation environment using Gazebo and ROS, referencing existing large fixed-wing UAVs, to design a V-tail aircraft, incorporating realistic aircraft dynamics, aerodynamics, and flight controls. Additionally, we present a simulation environment modeling approach tailored for obstacle avoidance in no-fly zones, and have created a 3D flight environment in Gazebo, generating a large-scale terrain map based on the original grayscale heightmap. This terrain map is used to simulate potential mountainous terrain threats that a fixed-wing UAV might encounter during mission execution. We have also introduced wind disturbances and other specific no-fly zones. We integrated the V-tail fixed-wing aircraft model into the 3D flight environment in Gazebo and designed PID controllers to stabilize the aircraft’s flight attitude. Full article
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Figure 1

Figure 1
<p>A 3D model of a V-tail fixed-wing UAV created using SolidWorks. The aircraft model has 8 moving parts, which are ① right aileron, ② left aileron, ③ right tail, ④ left tail, ⑤ propeller, ⑥ front wheel, ⑦ right wheel, and ⑧ left wheel.</p>
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<p>Flowchart of converting a SolidWorks model to SDF format. In SolidWorks, individual 3D models of different components of the aircraft are created separately. These components are then assembled to form a complete aircraft. A model format conversion plugin is used to convert this model into URDF format. Finally, the model is converted to the SDF format recommended by Gazebo using the format conversion command in the terminal.</p>
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<p>Add aerodynamic plugin to the SDF aircraft model description file. Using the official aerodynamics plugin provided by Gazebo, the figure displays the aerodynamic parameters of the left wing. In the aircraft model description file used in this study, the same plugin is also employed for the right wing and tails.</p>
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<p>V-tail aircraft in Gazebo. After successfully launching the simulation program, the aircraft model will appear on the runway scene in Gazebo.</p>
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<p>Multiple V-tail aircraft in Gazebo. Gazebo supports the simultaneous simulation of multiple aircraft models, which facilitates the research of multi-UAV formation flight algorithms.</p>
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<p>Add wind plugin to the SDF aircraft model description file. Using the officially provided wind disturbance plugin, you can set the wind direction and magnitude for both constant wind and gusts.</p>
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<p>Original heightmap. Different grayscale values represent different altitudes, where higher grayscale values (whiter pixels) indicate higher elevations.</p>
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<p>Terrain model in Gazebo. Different textures are applied to different altitudes: blue texture represents ocean areas, green texture represents grassland regions, and brown texture represents mountainous areas.</p>
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<p>Terrain model in Gazebo (local zoom). The image displays details from <a href="#drones-07-00601-f008" class="html-fig">Figure 8</a>, where the red dashed box highlights mountains at different altitudes. These mountains pose a threat to low-altitude aircraft flight.</p>
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<p>Hemisphere models in Gazebo. On the foundation of the terrain model, some custom semi-transparent red hemisphere regions are added as no-fly zones.</p>
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<p>Cylinder models in Gazebo. On the foundation of the terrain model, some custom semi-transparent purple cylindrical regions are added as no-fly zones.</p>
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<p>The comprehensive simulation system flowchart.</p>
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<p>The block diagram for the V-tail aircraft controller design.</p>
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<p>ROS node graph. Using the official ROS tool, “rqt_graph” generates a ROS node graph, where ellipses represent individual nodes and arrows indicate the direction of data transmission.</p>
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<p>Comprehensive simulation flight scenario. The flight environment consists of two parts: one is the runway scene used for taxiing and takeoff of the aircraft, and the other is the terrain model used to simulate obstacles encountered by the aircraft during flight.</p>
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<p>Keyboard control. The figure displays an aircraft control program we designed, which allows controlling the aircraft’s attitude and throttle through keyboard inputs. It also prints the desired and actual values in real time.</p>
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<p>Attitude angle data of the aircraft. During flight testing, a segment of attitude angle data is recorded. Through configuring different desired attitude angles, the attitude angle controller steers the aircraft to reach the desired angles.</p>
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<p>Pitch angle data of the aircraft. Pitch angle data during the aircraft’s takeoff phase is recorded. At the moment of takeoff, the desired pitch angle is set to −0.3 radians. After a period of angular fluctuations, the pitch angle eventually stabilizes at −0.3 radians.</p>
Full article ">Figure 19
<p>Aircraft is in the climbing phase. The aircraft’s V-tail control surface is set to rotate within the range of −0.52 radians to 0.52 radians. At takeoff, the pitch angle is set to −0.3 radians, at which point the V-tail control surface is at its maximum deflection.</p>
Full article ">Figure 20
<p>The pitch angle of the aircraft is stable at −0.3 radians. When the aircraft’s pitch angle stabilizes at −0.3 radians, due to excessive lift, the V-tail control surface needs to rotate downward by a certain angle to maintain pitch stability.</p>
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<p>Roll angle data of the aircraft. During the stable flight phase, multiple desired roll angles for the aircraft are set to evaluate the performance of the roll angle controller.</p>
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<p>The roll angle of the aircraft is stable at 0.42 radians. A screenshot of the aircraft maintaining a roll angle of 0.42 radians is taken. At this moment, the aileron control surface is essentially not deflected. Due to excessive lift generated by the high aircraft speed, the V-tail control surface rotates downward by a certain angle to maintain pitch stability.</p>
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19 pages, 10216 KiB  
Article
Dynamic Analysis and Numerical Simulation of Arresting Hook Engaging Cable in Carried-Based UAV Landing Process
by Haoyuan Shao, Zi Kan, Yifeng Wang, Daochun Li, Zhuoer Yao and Jinwu Xiang
Drones 2023, 7(8), 530; https://doi.org/10.3390/drones7080530 - 13 Aug 2023
Cited by 1 | Viewed by 1605
Abstract
Carrier-based unmanned aerial vehicles (UAVs) require precise evaluation methods for their landing and arresting safety due to their high autonomy and demanding reliability requirements. In this paper, an efficient and accurate simulation method is presented for studying the arresting hook engaging arresting cable [...] Read more.
Carrier-based unmanned aerial vehicles (UAVs) require precise evaluation methods for their landing and arresting safety due to their high autonomy and demanding reliability requirements. In this paper, an efficient and accurate simulation method is presented for studying the arresting hook engaging arresting cable process. The finite element method and multibody dynamics (FEM-MBD) approach is employed. By establishing a rigid–flexible coupling model encompassing the UAV and arresting gear system, the simulation model for the engagement process is obtained. The model incorporates multiple coordinate systems to effectively capture the relative motion between the rigid and flexible components. The model considers the material properties, arresting gear system characteristics, and UAV state during engagement. Verification is conducted by comparing simulation results with experimental data from a referenced arresting hook rebound. Finally, simulations are performed under different touchdown points and roll angles of the UAV to analyze the stress distribution of the hook, center of gravity variations, and the tire touch and rollover cable response. The proposed rigid–flexible coupling arresting dynamics model in this paper enables the effective analysis of the dynamic behavior during the arresting hook engaging arresting cable process. Full article
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Figure 1

Figure 1
<p>Schematic diagram of element contact.</p>
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<p>Schematic diagram of UAV and arresting gear system.</p>
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<p>Main parts of UAV model: (<b>a</b>) Side view of carrier-based UAV; (<b>b</b>) Top view of carrier-based UAV.</p>
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<p>FEM model of landing gear. (<b>a</b>) MLG; (<b>b</b>) NLG.</p>
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<p>Schematic of tire assemblies. (<b>a</b>) Internal structure of tire; (<b>b</b>) FEM model of tire and constraint.</p>
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<p>Schematic diagram of arresting hook.</p>
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<p>Diagram of arresting gear system.</p>
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<p>Diagram of arresting cable and wire rope supports.</p>
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<p>FEM model of pendant.</p>
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<p>FEM model of wire rope support.</p>
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<p>Diagram of simulation test of arresting hook bounce. (<b>a</b>) Left-side view (<b>b</b>); top-side view.</p>
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<p>Comparison of bounce height of arresting hook between experiment and simulation. Sinking velocity = (<b>a</b>) 3.6 m/s; (<b>b</b>) 4 m/s; (<b>c</b>) 5 m/s [<a href="#B13-drones-07-00530" class="html-bibr">13</a>].</p>
Full article ">Figure 12 Cont.
<p>Comparison of bounce height of arresting hook between experiment and simulation. Sinking velocity = (<b>a</b>) 3.6 m/s; (<b>b</b>) 4 m/s; (<b>c</b>) 5 m/s [<a href="#B13-drones-07-00530" class="html-bibr">13</a>].</p>
Full article ">Figure 13
<p>Carrier-based UAV model and parameters. (<b>a</b>) Configuration of UAV; (<b>b</b>) diagram of distance between touchdown point and cable <span class="html-italic">d</span>; (<b>c</b>) diagram of UAV roll angle, <math display="inline"><semantics> <mi>φ</mi> </semantics></math>.</p>
Full article ">Figure 14
<p>Stress distribution of the arresting hook at the moment the hook engages the cable. (<b>a</b>) <span class="html-italic">d</span> = 1 m; (<b>b</b>) <span class="html-italic">d</span> = 2 m; (<b>c</b>) <span class="html-italic">d</span> = 4 m; (<b>d</b>) <span class="html-italic">d</span> = 6 m; (<b>e</b>) <span class="html-italic">d</span> = 8 m; (<b>f</b>) <span class="html-italic">d</span> = 10 m.</p>
Full article ">Figure 14 Cont.
<p>Stress distribution of the arresting hook at the moment the hook engages the cable. (<b>a</b>) <span class="html-italic">d</span> = 1 m; (<b>b</b>) <span class="html-italic">d</span> = 2 m; (<b>c</b>) <span class="html-italic">d</span> = 4 m; (<b>d</b>) <span class="html-italic">d</span> = 6 m; (<b>e</b>) <span class="html-italic">d</span> = 8 m; (<b>f</b>) <span class="html-italic">d</span> = 10 m.</p>
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<p>Engagement process after tire rolling cable.</p>
Full article ">Figure 15 Cont.
<p>Engagement process after tire rolling cable.</p>
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<p>Time history of the height of the center of gravity after the landing gear touches the deck under different roll angles.</p>
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<p>Stress distribution of the arresting hook at the moment the hook engages the cable: (<b>a</b>) <math display="inline"><semantics> <mi>φ</mi> </semantics></math> = 0; (<b>b</b>) <math display="inline"><semantics> <mi>φ</mi> </semantics></math> = 2°; (<b>c</b>) <math display="inline"><semantics> <mi>φ</mi> </semantics></math> = 4°; (<b>d</b>) <math display="inline"><semantics> <mi>φ</mi> </semantics></math> = 6°; (<b>e</b>) <math display="inline"><semantics> <mi>φ</mi> </semantics></math> = 8°.</p>
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<p>Hook engaging cable after one side of the tire touches the cable.</p>
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<p>Hook engaging cable after one side of the tire rolls over the cable.</p>
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<p>Hook engaging cable after one side of the tire rolls over the cable.</p>
Full article ">
19 pages, 13632 KiB  
Article
An Approach to the Implementation of a Neural Network for Cryptographic Protection of Data Transmission at UAV
by Ivan Tsmots, Vasyl Teslyuk, Andrzej Łukaszewicz, Yurii Lukashchuk, Iryna Kazymyra, Andriy Holovatyy and Yurii Opotyak
Drones 2023, 7(8), 507; https://doi.org/10.3390/drones7080507 - 2 Aug 2023
Cited by 1 | Viewed by 1378
Abstract
An approach to the implementation of a neural network for real-time cryptographic data protection with symmetric keys oriented on embedded systems is presented. This approach is valuable, especially for onboard communication systems in unmanned aerial vehicles (UAV), because of its suitability for hardware [...] Read more.
An approach to the implementation of a neural network for real-time cryptographic data protection with symmetric keys oriented on embedded systems is presented. This approach is valuable, especially for onboard communication systems in unmanned aerial vehicles (UAV), because of its suitability for hardware implementation. In this study, we evaluate the possibility of building such a system in hardware implementation at FPGA. Onboard implementation-oriented information technology of real-time neuro-like cryptographic data protection with symmetric keys (masking codes, neural network architecture, and matrix of weighting coefficients) has been developed. Due to the pre-calculation of matrices of weighting coefficients and tables of macro-partial products and the use of tabular-algorithmic implementation of neuro-like elements and dynamic change of keys, it provides increased cryptographic stability and hardware–software implementation on FPGA. The table-algorithmic method of calculating the scalar product has been improved. By bringing the weighting coefficients to the greatest common order, pre-computing the tables of macro-partial products, and using operations of memory read, fixed-point addition, and shift operations instead of floating-point multiplication and addition operations, it provides a reduction in hardware costs for its implementation and calculation time as well. Using a processor core supplemented with specialized hardware modules for calculating the scalar product, a system of neural network cryptographic data protection in real-time has been developed, which, due to the combination of universal and specialized approaches, software, and hardware, ensures the effective implementation of neuro-like algorithms for cryptographic encryption and decryption of data in real-time. The specialized hardware for neural network cryptographic data encryption was developed using VHDL for equipment programming in the Quartus II development environment ver. 13.1 and the appropriate libraries and implemented on the basis of the FPGA EP3C16F484C6 Cyclone III family, and it requires 3053 logic elements and 745 registers. The execution time of exclusively software realization of NN cryptographic data encryption procedure using a NanoPi Duo microcomputer based on the Allwinner Cortex-A7 H2+ SoC was about 20 ms. The hardware–software implementation of the encryption, taking into account the pre-calculations and settings, requires about 1 msec, including hardware encryption on the FPGA of four 2-bit inputs, which is performed in 160 nanoseconds. Full article
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<p>Structure of NN technology for cryptographic data protection: (<b>a</b>) the process of data encryption; (<b>b</b>) the process of decrypting data.</p>
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<p>The structure of the data encryption NN.</p>
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<p>The NN architecture for decryption of encrypted data.</p>
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<p>Structure of the stationary part of the system of NN cryptographic data protection and transmission.</p>
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<p>Structure of the UAV onboard part of the system of NN cryptographic data protection and transmission.</p>
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<p>Structure of the component of NN cryptographic encryption of data.</p>
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<p>Structure of the component of NN cryptographic decryption of data.</p>
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<p>A circuit of the specialized hardware components of NN cryptographic data encryption.</p>
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<p>The timing chart of the specialized hardware of NN cryptographic data encryption.</p>
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22 pages, 12295 KiB  
Article
Experimental Characterization of Composite-Printed Materials for the Production of Multirotor UAV Airframe Parts
by Tomislav Šančić, Marino Brčić, Denis Kotarski and Andrzej Łukaszewicz
Materials 2023, 16(14), 5060; https://doi.org/10.3390/ma16145060 - 18 Jul 2023
Cited by 3 | Viewed by 1610
Abstract
In this paper, the characterization of 3D-printed materials that are considered in the design of multirotor unmanned aerial vehicles (UAVs) for specialized purposes was carried out. The multirotor UAV system is briefly described, primarily from the aspect of system dynamics, considering that the [...] Read more.
In this paper, the characterization of 3D-printed materials that are considered in the design of multirotor unmanned aerial vehicles (UAVs) for specialized purposes was carried out. The multirotor UAV system is briefly described, primarily from the aspect of system dynamics, considering that the airframe parts connect the UAV components, including the propulsion configuration, into a functional assembly. Three additive manufacturing (AM) technologies were discussed, and a brief overview was provided of selective laser sintering (SLS), fused deposition modeling (FDM), and continuous fiber fabrication (CFF). Using hardware and related software, 12 series of specimens were produced, which were experimentally tested utilizing a quasi-static uniaxial tensile test. The results of the experimental tests are provided graphically with stress–strain diagrams. In this work, the focus is on CFF technology and the testing of materials that will be used in the production of mechanically loaded airframe parts of multirotor UAVs. The experimentally obtained values of the maximum stresses were compared for different technologies. For the considered specimens manufactured using FDM and SLS technology, the values are up to 40 MPa, while for the considered CFF materials and range of investigated specimens, it is shown that it can be at least four times higher. By increasing the proportion of fibers, these differences increase. To be able to provide a wider comparison of CFF technology and investigated materials with aluminum alloys, the following three-point flexural and Charpy impact tests were selected that fit within this framework for experimental characterization. Full article
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<p>Multirotor UAV platform: (<b>a</b>) quadrotor heavy-lift prototype; (<b>b</b>) hexarotor 3D model.</p>
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<p>Examples of 3D-printed airframe parts.</p>
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<p>SLS technology—schematic overview.</p>
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<p>AM technologies—schematic overview: (<b>a</b>) FDM; (<b>b</b>) CFF.</p>
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<p>Test specimen (ISO 527-2 [<a href="#B45-materials-16-05060" class="html-bibr">45</a>] standard test specimen for uniaxial quasi-static tensile testing)—G-code generation in a slicer.</p>
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<p>Additive manufacturing and experimental measurements flow chart.</p>
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<p>Experimental equipment: (<b>a</b>) SHIMADZU AG-X; (<b>b</b>) performing quasi-static uniaxial tensile stress on the test specimen.</p>
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<p>S09 test specimen with concentric fiber reinforcement.</p>
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<p>CFF—fiber reinforcement angles.</p>
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<p>Integrated experimental procedure for material characterization.</p>
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<p>Stress–strain diagram for specimen 1 (S01) series experimental measurements.</p>
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<p>Stress–strain diagram for S02 experimental measurements.</p>
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<p>Stress–strain diagram for S03 experimental measurements.</p>
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<p>Stress–strain diagram for S04 experimental measurements.</p>
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<p>Stress–strain diagram for S05 experimental measurements.</p>
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<p>Stress–strain diagram for S06 experimental measurements.</p>
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<p>Stress–strain diagram for S07 experimental measurements.</p>
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<p>Stress–strain diagram for S08 experimental measurements.</p>
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<p>Stress–strain diagram for S09 experimental measurements.</p>
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<p>Stress–strain diagram for S10 experimental measurements.</p>
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<p>Stress–strain diagram for S11 experimental measurements.</p>
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<p>Stress–strain diagram for S12 experimental measurements.</p>
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<p>Mean values of the maximum stress regarding PLA and PETG materials.</p>
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<p>Mean values of the maximum stress regarding default print parameters for PLA, PETG, PA 12, and Onyx materials.</p>
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<p>Mean values of the maximum stress regarding CFF technology using Onyx and fiberglass reinforcement.</p>
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<p>Three-point flexural test—equipment and test execution.</p>
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22 pages, 6640 KiB  
Article
Analysis of Aerodynamic Characteristics of Propeller Systems Based on Martian Atmospheric Environment
by Wangwang Zhang, Bin Xu, Haitao Zhang, Changle Xiang, Wei Fan and Zhiran Zhao
Drones 2023, 7(6), 397; https://doi.org/10.3390/drones7060397 - 15 Jun 2023
Cited by 4 | Viewed by 2110
Abstract
Compared to detection methods employed by Mars rovers and orbiters, the employment of Mars UAVs presents clear advantages. However, the unique atmospheric conditions on Mars pose significant challenges to the design and operation of such UAVs. One of the primary difficulties lies in [...] Read more.
Compared to detection methods employed by Mars rovers and orbiters, the employment of Mars UAVs presents clear advantages. However, the unique atmospheric conditions on Mars pose significant challenges to the design and operation of such UAVs. One of the primary difficulties lies in the impact of the planet’s low air density on the aerodynamic performance of the UAV’s rotor system. In order to determine the aerodynamic characteristics of the rotor system in the Martian atmospheric environment, a rotor system suitable for the Martian environment was designed under the premise of fully considering the special atmospheric environment of Mars, and the aerodynamic characteristics of the rotor system in the compressible and ultra-low Reynolds number environment were numerically simulated by means of a numerical calculation method. Additionally, a bench experiment was conducted in a vacuum chamber simulating the Martian atmospheric environment, and the aerodynamic characteristics of the UAV rotor system in the Martian environment were analyzed by combining theory and experiments. The feasibility of the rotor system applied to the Martian atmospheric environment was verified, and the first generation of Mars unmanned helicopters was developed and validated via hovering experiments, which thereby yielded crucial data support for the design of subsequent Mars UAV models. Full article
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<p>General Mach–Reynolds number research areas.</p>
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<p>Maximum section lift-to-drag ratio versus Reynolds number.</p>
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<p>Force analysis of blade element.</p>
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<p>Torsion angle and chord length distribution of different parts of propeller: (<b>a</b>) twist angle distribution; (<b>b</b>) chord length distribution.</p>
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<p>Propeller model.</p>
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<p>Mars propeller three-dimensional mesh: (<b>a</b>) static zone; (<b>b</b>) rotating zone; (<b>c</b>) blade tip area mesh.</p>
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<p>Diagram of propeller vorticity structure on the iso−surface of the Q−criterion = 5000 in Martian: (<b>a</b>) 2000 RPM; (<b>b</b>) 2400 RPM; (<b>c</b>) 2600 RPM; (<b>d</b>) 3000 RPM.</p>
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<p>Propeller structure and the finite element model: (<b>a</b>) structure diagram of the foam sandwich of the Mars propeller; (<b>b</b>) finite element model of the Mars propeller.</p>
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<p>Finite element analysis results of Mars Propeller: (<b>a</b>) axial direction deformation of the Mars propeller; (<b>b</b>) failure factors of the Mars propeller.</p>
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<p>Mars unmanned helicopter model.</p>
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<p>A vacuum chamber simulating the atmospheric environment of Mars.</p>
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<p>The test system of the Mars propeller in the vacuum chamber.</p>
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<p>Data collection system of the test bench.</p>
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<p>Thrust coefficient at different rotating speeds and angles of attack.</p>
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<p>Power coefficient at different speeds and angles of attack.</p>
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<p>Merit factors at different speeds and angles of attack.</p>
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<p>Hovering experiment of mars unmanned helicopter in vacuum chamber.</p>
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16 pages, 4490 KiB  
Article
Noise Impact Assessment of UAS Operation in Urbanised Areas: Field Measurements and a Simulation
by Filip Škultéty, Erik Bujna, Michal Janovec and Branislav Kandera
Drones 2023, 7(5), 314; https://doi.org/10.3390/drones7050314 - 9 May 2023
Cited by 1 | Viewed by 2069
Abstract
This article’s main topic is an assessment of unmanned aircraft system (UAS) noise pollution in several weight categories according to Regulation (EU) 2019/947 and its impact on the urban environment during regular operation. The necessity of solving the given problem is caused by [...] Read more.
This article’s main topic is an assessment of unmanned aircraft system (UAS) noise pollution in several weight categories according to Regulation (EU) 2019/947 and its impact on the urban environment during regular operation. The necessity of solving the given problem is caused by an increasing occurrence of UASs in airspace and the prospect of introducing unmanned aircraft into broader commercial operations. This work aims to provide an overview of noise measurements of two UAS weight categories under natural atmospheric conditions to assess their impact on the surrounding environment. On top of that, modelling and simulations were used to observe and assess the noise emission characteristics. The quantitative results contain an assessment of the given noise restrictions based on the psychoacoustic impact and actual measured values inserted into the urban simulation scenario of the Zilina case study located in northwest Slovakia. It was preceded by a study of noise levels in certain areas to evaluate the variation level after UAS integration into the corresponding airspace. Following a model simulation of the C2 category, it was concluded that there was a marginal rise in the level of noise exposure, which would not exceed the prescribed standards of the Environmental Noise Directive. Full article
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<p>Conical area without obstructions during measurement.</p>
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<p>Microphone array on a hemispherical measurement surface for measurement.</p>
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<p>Microphone array at the airstrip.</p>
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<p>Equivalent sound pressure levels in time of DJI Inspire during hovering.</p>
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<p>Equivalent sound pressure levels in time of DJI Inspire during the overflight.</p>
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<p>Comparison of L<sub>WA</sub> for the two drones during overflight at a speed of 10 kmh<sup>−1</sup> at 0.5 m height.</p>
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<p>Comparison of L<sub>WA</sub> for the two drones during hovering at 0.5 m height.</p>
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<p>Noise load around flight corridor at 2D visualisation.</p>
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<p>Noise load around flight corridor at 3D visualisation.</p>
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22 pages, 8949 KiB  
Article
Design and Experiment of Ecological Plant Protection UAV Based on Ozonated Water Spraying
by Hang Xu, Lili Yi, Chuanyong Li, Yuemei Sun, Liangchen Hou, Jingbo Bai, Fanxia Kong, Xin Han and Yubin Lan
Drones 2023, 7(5), 291; https://doi.org/10.3390/drones7050291 - 26 Apr 2023
Cited by 2 | Viewed by 1849
Abstract
With the development of pesticide substitution technology, ozonated water has been gradually applied in agricultural plant protection. This paper describes our development of an ecological plant protection unmanned aerial vehicle (UAV) that can produce and spray ozonated water while flying. Firstly, this paper [...] Read more.
With the development of pesticide substitution technology, ozonated water has been gradually applied in agricultural plant protection. This paper describes our development of an ecological plant protection unmanned aerial vehicle (UAV) that can produce and spray ozonated water while flying. Firstly, this paper carries out the design of the ozonated water system, including the selection of the ozone generator and the gas-liquid mixing method. Secondly, the conceptual design method of the ecological plant protection UAV is introduced, including total weight estimation, propulsion system selection, layout and structure design, battery modeling, center of gravity evaluation, and control system. Then, static analysis was computed in ANSYS Workbench on the UAV fuselage. Finally, the field test verified that the hovering time of the UAV could reach the design requirement of 10 min when it was fully loaded. The effective spraying width (with a height of 2 m and a speed of 3 m/s) is 5.25 m. The UAV was used to spray ozonated water with a concentration of 17 ppm continuously once a day; on day 7, the control effect could reach 76.4% and the reduction rate of the larvae population was 59.3%. Therefore, spraying ozonated water with a concentration of 17 ppm every day by using the ecological plant protection UAV can effectively control broccoli diamondback moth larvae and achieve the control effect of traditional pesticides (Chlorantraniliprole SC). Full article
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<p>The design process for ecological plant protection UAV.</p>
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<p>The UAV composition and each system’s workflow.</p>
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<p>Statistics of the hovering time of plant protection UAV. Green balls represent the projection on the plane composed of the “Hover time” axis and the “Total weight” axis, and blue balls represent the projection on the plane composed of the “Total weight” axis and the “Battery weight” axis.</p>
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<p>The ozone generator’s working concept.</p>
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<p>Variation of ozonated water concentration in different production modes: (<b>a</b>) generation of ozonated water concentration; (<b>b</b>) attenuation of ozonated water concentration.</p>
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<p>Statistics of workload weight and the total weight of plant protection UAV.</p>
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<p>The load performance diagram of the propulsion system.</p>
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<p>The 3D model and the layout design of the ecological plant protection UAV.</p>
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<p>The 3D model and the layout design of the ecological plant protection UAV.</p>
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<p>(<b>a</b>) The direction of motor rotation; (<b>b</b>) The layout of the flight control system.</p>
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<p>Control block diagram of the ozonated water system.</p>
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<p>(<b>a</b>) Mesh model of the UAV; (<b>b</b>) the boundary conditions.</p>
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<p>The results of UAV statics analysis: (<b>a</b>) total deformation of the UAV; (<b>b</b>) equivalent stress of the UAV.</p>
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<p>The hovering time test of the ecological plant protection UAV: (<b>a</b>) install the power meter; (<b>b</b>) the UAV stays in hover.</p>
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<p>Comparison of hover times at different weights.</p>
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<p>The effective spraying width test: (<b>a</b>) the layout plan; (<b>b</b>) the test site.</p>
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<p>The effective spraying width of the UAV in two flights (a total of four rows).</p>
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<p>(<b>a</b>) The ecological plant protection UAV; (<b>b</b>) X8 large-load plant protection UAV.</p>
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<p>Ecological plant protection UAV spraying operation.</p>
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<p>During the testing period, mean number (±SE) of diamondback moth larvae collected from four treatments.</p>
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12 pages, 2100 KiB  
Article
Optimum Flight Height for the Control of Desert Locusts Using Unmanned Aerial Vehicles (UAV)
by Violet Ochieng’, Ivan Rwomushana, George Ong’amo, Paul Ndegwa, Solomon Kamau, Fernadis Makale, Duncan Chacha, Kush Gadhia and Morris Akiri
Drones 2023, 7(4), 233; https://doi.org/10.3390/drones7040233 - 28 Mar 2023
Cited by 4 | Viewed by 2925
Abstract
Desert locust is one of the most destructive migratory pest in the world. Current methods of control rely on conventional chemical insecticides during invasion. Some environmentally friendly biopesticides based on Metarhizium acridum and insect growth regulators have also been deployed in preventive control [...] Read more.
Desert locust is one of the most destructive migratory pest in the world. Current methods of control rely on conventional chemical insecticides during invasion. Some environmentally friendly biopesticides based on Metarhizium acridum and insect growth regulators have also been deployed in preventive control operations. They have been tested in sprayers mounted on commonly used platforms such as vehicles, aircraft, and human. However, despite being used successfully, these tools present many challenges, hence the need to supplement them with suitable alternatives. The successful use of drones to control pests such as fall armyworm, planthoppers, aphids, among others, makes it an attractive technology that has the potential to improve locust management, especially in inaccessible areas. However, key parameters for the safe and optimal use of drones in desert locust control are not documented. This study established the key parameters for spraying desert locusts with a drone. To test the optimum height for spraying Metarhizium acridum on the locusts, the drone was flown at five different heights: 2.5, 5, 7.5, 10, and 12.5 m. At each height, the drone sprayed the ink mixture on spray cards pinned to the ground to approximate the droplet density and compare it to the standard droplet density recommended for desert locust control. To assess the efficacy of M. acridum and the effectiveness of drones in its application, 50 g of spores were mixed in 1 L of diesel and sprayed on caged live locusts of different stages (3rd and 4th instars, as well as the adults); they were monitored for twenty-one days in a controlled room, and their mortality was determined. Variation in droplet density between the tested heights was significant. A height of 10 m agrees with the recommended standard droplet density within the 45 droplets/cm2 range. Mortality varied among the locusts’ developmental stages within and between heights. Survival probability varied between heights for 3rd instar, 4th instar, and adults. All the developmental stages of the desert locust were susceptible to Novacrid and the recommended target stage is the 3rd instar. Management of desert locusts by the use of drone technology appears promising when the pesticides are applied at an optimum height and standard operating procedures are followed. Further research could explore the gap in the effects of environmental parameters on flight application efficiency. Full article
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<p>Illustration of the experimental layout of spray cards for establishing optimum droplet density by spraying at different heights using an Agras T20 drone fitted with a Micronair 12 ultra-low volume (ULV) spraying boom.</p>
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<p>Samples of papers with droplets.</p>
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<p>Wire mesh cages (objects arranged within the yellow circle) with live locusts arranged parallel to the drone flight path (object within the red circle).</p>
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<p>Kaplan—Meier survival curves for different stages of desert locusts sprayed with Novacrid<sup>®</sup> at different drone flight heights. The same small letters adjacent to the legend indicate no significant difference in the survival distribution curve at <italic>p</italic> &gt; 0.05. (<bold>A</bold>) Survival curve of the 3rd instar, (<bold>B</bold>) survival curve of the 4th instar, and (<bold>C</bold>) survival curve of adults. “+” indicates right censorship.</p>
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<p>Kaplan—Meier survival curves for different stages of desert locusts sprayed with Novacrid<sup>®</sup> at different drone flight heights. The same small letters adjacent to the legend indicate no significant difference in the survival distribution curve at <italic>p</italic> &gt; 0.05. (<bold>A</bold>) Survival curve of the 3rd instar, (<bold>B</bold>) survival curve of the 4th instar, and (<bold>C</bold>) survival curve of adults. “+” indicates right censorship.</p>
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24 pages, 5384 KiB  
Article
Acoustic SLAM Based on the Direction-of-Arrival and the Direct-to-Reverberant Energy Ratio
by Wenhao Qiu, Gang Wang and Wenjing Zhang
Drones 2023, 7(2), 120; https://doi.org/10.3390/drones7020120 - 9 Feb 2023
Cited by 1 | Viewed by 1679
Abstract
This paper proposes a new method that fuses acoustic measurements in the reverberation field and low-accuracy inertial measurement unit (IMU) motion reports for simultaneous localization and mapping (SLAM). Different from existing studies that only use acoustic data for direction-of-arrival (DoA) estimates, the source’s [...] Read more.
This paper proposes a new method that fuses acoustic measurements in the reverberation field and low-accuracy inertial measurement unit (IMU) motion reports for simultaneous localization and mapping (SLAM). Different from existing studies that only use acoustic data for direction-of-arrival (DoA) estimates, the source’s distance from sensors is calculated with the direct-to-reverberant energy ratio (DRR) and applied to eliminate the nonlinear noise from motion reports. A particle filter is applied to estimate the critical distance, which is key for associating the source’s distance with the DRR. A keyframe method is used to eliminate the deviation of the source position estimation toward the robot. The proposed DoA-DRR acoustic SLAM (D-D SLAM) is designed for three-dimensional motion and is suitable for drones. The method is the first acoustic SLAM algorithm that has been validated on a real-world drone dataset that contains only acoustic data and IMU measurements. Compared with previous methods, D-D SLAM has acceptable performance in locating the drone and building a source map from a real-world drone dataset. The average location accuracy is 0.48 m, while the source position error converges to less than 0.25 m within 2.8 s. These results prove the effectiveness of D-D SLAM in real-world scenes. Full article
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<p>World frame and robot frame.</p>
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<p>Extensive simulation of the origin method when the robot and the source remain still for (<b>a</b>) beginning (3 time steps), (<b>b</b>) 10 time steps, and (<b>c</b>) 17 time steps.</p>
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<p><span class="html-italic">T</span><sub>60</sub> = 0.15 s, Trajectory estimation on simulations for aSLAM with true speed plus noise (orange dash-dotted line), aSLAM with IMU data (blue dashed line), and the D-D SLAM with IMU data (red dotted line).</p>
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<p><span class="html-italic">T</span><sub>60</sub> = 0.15 s, Trajectory and source estimations on simulations for D-D SLAM with and without the keyframe method.</p>
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<p><span class="html-italic">T</span><sub>60</sub> = 0.5 s, Trajectory and source estimations on simulations for D-D SLAM under the condition of different SNRs.</p>
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<p>Simulation results for (<b>a</b>) the trajectory errors and (<b>b</b>) the source position errors over time steps.</p>
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<p>The state of different critical distance particles and the weighted critical distance with simulation data under the condition of <span class="html-italic">T</span><sub>60</sub> = 0.15 s.</p>
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<p>The estimation of trajectory and the source position using aSLAM and D-D SLAM with and without the keyframe method.</p>
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<p>Dataset result for (<b>a</b>) the trajectory error and (<b>b</b>) the source position estimation error over time steps.</p>
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<p>The state of different critical distance particles and the weighted critical distance with real data.</p>
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<p>The positional error and the critical distance estimation with (<b>a</b>) different numbers of particles and (<b>b</b>) the max number of GM components.</p>
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<p>The robot-source distance and the trajectory error of D-D SLAM.</p>
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15 pages, 8814 KiB  
Article
Semantic Scene Understanding with Large Language Models on Unmanned Aerial Vehicles
by J. de Curtò, I. de Zarzà and Carlos T. Calafate
Drones 2023, 7(2), 114; https://doi.org/10.3390/drones7020114 - 8 Feb 2023
Cited by 17 | Viewed by 5591
Abstract
Unmanned Aerial Vehicles (UAVs) are able to provide instantaneous visual cues and a high-level data throughput that could be further leveraged to address complex tasks, such as semantically rich scene understanding. In this work, we built on the use of Large Language Models [...] Read more.
Unmanned Aerial Vehicles (UAVs) are able to provide instantaneous visual cues and a high-level data throughput that could be further leveraged to address complex tasks, such as semantically rich scene understanding. In this work, we built on the use of Large Language Models (LLMs) and Visual Language Models (VLMs), together with a state-of-the-art detection pipeline, to provide thorough zero-shot UAV scene literary text descriptions. The generated texts achieve a GUNNING Fog median grade level in the range of 7–12. Applications of this framework could be found in the filming industry and could enhance user experience in theme parks or in the advertisement sector. We demonstrate a low-cost highly efficient state-of-the-art practical implementation of microdrones in a well-controlled and challenging setting, in addition to proposing the use of standardized readability metrics to assess LLM-enhanced descriptions. Full article
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<p>RYZE Tello Microdrones and the NXP Hover Games Drone Kit.</p>
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<p>UAV real-time literary storytelling.</p>
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<p>UAV captured frame processing and GPT-3. Very good GPT-3 descriptions of the scene.</p>
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<p>UAV captured frame processing and GPT-3. Adequate literary GPT-3 descriptions.</p>
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<p>UAV captured frame processing and GPT-3. Adequate literary GPT-3 descriptions.</p>
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<p>UAV captured frame processing and GPT-3. Somewhat good descriptions, but the CLIP captioning module and the YOLOv7 produce inaccurate outputs.</p>
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<p>UAV captured frame processing and GPT-3. Somewhat good descriptions, but the CLIP captioning module and the YOLOv7 produce inaccurate outputs.</p>
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<p>UAV captured frame processing and GPT-3. Failure cases.</p>
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15 pages, 8977 KiB  
Article
A Computational Investigation of the Hover Mechanism of an Innovated Disc-Shaped VTOL UAV
by Samia Shahrin Ahmed Snikdha and Shih-Hsiung Chen
Drones 2023, 7(2), 105; https://doi.org/10.3390/drones7020105 - 3 Feb 2023
Cited by 1 | Viewed by 3003
Abstract
Inventive approaches are constantly being revealed in the field of vertical take-off and landing (VTOL) unmanned aerial vehicle (UAV) configuration concepts and designs. To date, a body-associated configuration of UAVs for augmented lift remains unclear among other approached designs. The current paper investigates [...] Read more.
Inventive approaches are constantly being revealed in the field of vertical take-off and landing (VTOL) unmanned aerial vehicle (UAV) configuration concepts and designs. To date, a body-associated configuration of UAVs for augmented lift remains unclear among other approached designs. The current paper investigates the mechanism of a high-lift ducted fan mounted in the central body for VTOL UAV designs. We report an unresolved design of a disc-shaped UAV with a single rotor that aims to enhance the cost-effectiveness of fuel consumption with a substantial contribution of body lift to hover thrust. The convex upper surface curvature was applied to generate a significant lift contribution from the body during hover. The computational fluid dynamics (CFD) approach based on unstructured discretization followed by three-dimensional steady Reynolds-averaged Navier–Stokes (RANS) flow was applied in ANSYS CFX to mechanistically investigate the underlying design considerations. The disc-shaped UAV uses the lip curvature on the duct inlet to generate a vertical force that demonstrates a significant contribution of 95% of the rotor thrust during hovering. The UAV’s upper surface generates prolonged flow entrainment free from momentum losses in swirling flows. This phenomenon is followed by reduced power consumption in hovering and vertical flight, making the UAV aerodynamically stable and environmentally safe. Full article
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<p>Design parameters of the lifting UAV; (<b>a</b>) isometric view, (<b>b</b>) bottom view, (<b>c</b>) side view, and (<b>d</b>) top view.</p>
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<p>(<b>a</b>) Surface mesh on the UAV body inside the stationary domain, (<b>b</b>) duct, (<b>c</b>) lower surface, (<b>d</b>) lip curvature, and (<b>e</b>) upper surface.</p>
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<p>(<b>a</b>) Surface mesh on the UAV parts in the rotating domain, (<b>b</b>) zoomed-in view of the mesh on the blades.</p>
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<p>(<b>a</b>) Hub showing the blade section, (<b>b</b>) volume mesh through the mid-section of the UAV in the density zone.</p>
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<p>(<b>a</b>) Computational domain interpreting boundary conditions; (<b>b</b>) interface between the rotational and stationary domains.</p>
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<p>Mesh sensitivity analysis in hovering.</p>
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<p>Pressure contour at hovering, <math display="inline"><semantics> <mrow> <msub> <mi>U</mi> <mo>∞</mo> </msub> <mo>=</mo> <mn>0</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mo>/</mo> <mi mathvariant="normal">s</mi> </mrow> </semantics></math>. (<b>a</b>) XY, Z = 0 mid-plane, (<b>b</b>) YZ, X = −0.5 upper surface, and (<b>c</b>) YZ, X = 0.5 lower surface cross-sectional plane.</p>
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<p>Velocity contour at hovering, <math display="inline"><semantics> <mrow> <msub> <mi>U</mi> <mo>∞</mo> </msub> <mo>=</mo> <mn>0</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mo>/</mo> <mi mathvariant="normal">s</mi> </mrow> </semantics></math>. (<b>a</b>) XY, Z = 0 mid-plane, (<b>b</b>) YZ, X = −0.5 upper surface, and (<b>c</b>) YZ, X = 0.5 lower surface cross-sectional plane.</p>
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<p>Mid-section plane plots of (<b>a</b>) surface streamlines, and (<b>b</b>) velocity vector in hovering, at <math display="inline"><semantics> <mrow> <msub> <mi>U</mi> <mo>∞</mo> </msub> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> m/s.</p>
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<p>(<b>a</b>) Extra lift contribution from the body delineating the UAV hover efficiency, (<b>b</b>) discrete hover and vertical flight thrust with body lift, (<b>c</b>) percentage generation of body lift and rotor thrust in hover and vertical flight, and (<b>d</b>) thrust coefficient of the UAV with increasing vertical wind speed.</p>
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<p>(<b>a</b>) The percentage of extra lift generated by the body compared to the rotor thrust, (<b>b</b>) lift distribution of the body from hover with 0 m/s to the vertical flight with increasing wind velocity.</p>
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37 pages, 15518 KiB  
Article
Research on Aerodynamic Characteristics of Trans-Media Vehicles Entering and Exiting the Water in Still Water and Wave Environments
by Jun Wei, Yong-Bai Sha, Xin-Yu Hu, Zhe Cao, De-Ping Chen, Da Zhou and Yan-Li Chen
Drones 2023, 7(2), 69; https://doi.org/10.3390/drones7020069 - 18 Jan 2023
Cited by 2 | Viewed by 2365
Abstract
The problem of aircraft entering and exiting water is a complex, nonlinear, strongly disturbed, and multi-coupled multiphase flow problem, which involves the precise capture of the air/water interface and the multi-coupling interaction between aircraft, water, and air. Moreover, due to the large difference [...] Read more.
The problem of aircraft entering and exiting water is a complex, nonlinear, strongly disturbed, and multi-coupled multiphase flow problem, which involves the precise capture of the air/water interface and the multi-coupling interaction between aircraft, water, and air. Moreover, due to the large difference in medium properties during the crossing, the load on the body will suddenly change. In this paper, the VOF (volume of fluid) algorithm is used to capture the liquid surface at the air/water interface, and since body movement is involved in this process, the overset grid technology is used to avoid the traditional dynamic grid deformation problem. In the process of this numerical simulation prediction, the effects of different water-entry angles and different water-entry heights on the body load and attitude of the trans-medium aircraft, as well as the cavitation evolution law of the body water entry are analyzed. On this basis, to simulate the authenticity and complexity of the water-entry environment, numerical wave-making technology was introduced to analyze the water-entry load, posture, and cavitation evolution law of the body under different wave environments. The numerical parameters under the condition of wave and no wave are compared, and the difference in water-entry performance under the condition of wave and no wave is analyzed. Full article
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<p>Schematic diagram of the overall structure of the water–air dual-power ducted trans-medium aircraft.</p>
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<p>Schematic diagram of thruster type and its arrangement.</p>
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<p>Schematic diagram of the working principle of the power system of the trans-medium aircraft: (<b>a</b>–<b>d</b>) translation, roll, pitch, yaw (air layout); (<b>e</b>–<b>h</b>) translation, roll, pitch, yaw (underwater layout).</p>
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<p>Schematic diagram of the working principle of the power system of the trans-medium aircraft: (<b>a</b>–<b>d</b>) translation, roll, pitch, yaw (air layout); (<b>e</b>–<b>h</b>) translation, roll, pitch, yaw (underwater layout).</p>
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<p>Schematic diagram of the cross-sectional structure of the duct body.</p>
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<p>Schematic diagram of the frame structure design of the trans-media aircraft: (<b>a</b>) air quadcopter support frame; (<b>b</b>) cross frame structure; (<b>c</b>) underwater propeller support rack; (<b>d</b>) aircraft overall rack layout design.</p>
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<p>Spatial distribution of phase fraction and its interface reconstruction by VOF method.</p>
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<p>Schematic diagram of the force on the surface microelement at the interface of two phases.</p>
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<p>Schematic diagram of the assembly principle of overset grid.</p>
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<p>Schematic diagram of the numerical wave-making calculation domain.</p>
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<p>Schematic diagram of variable curves under different grid levels: (<b>a</b>) rotor thrust curve; (<b>b</b>) the tip speed curve when R/r = 1.1; (<b>c</b>) the tip speed curve when R/r = 1.2.</p>
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<p>Residual curve.</p>
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<p>Schematic diagram of grid generation for numerical prediction of water inflow and outflow.</p>
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<p>Water flow phase change and body motion streamline diagram of the inflow flow field.</p>
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<p>Q-value cloud chart when entering the water at 40°.</p>
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<p>Q-value cloud chart when entering the water at 40°.</p>
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<p>Variation curve of water load impact at different heights.</p>
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<p>Velocity curves of the body entering the water at different heights.</p>
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<p>Phase transition diagram of water flows cavitation at different heights: (<b>a</b>) 0.2 m high into the water; (<b>b</b>) 0.3 m high into the water; (<b>c</b>) 0.5 m high into the water.</p>
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<p>Phase transition diagram of water flows cavitation at different heights: (<b>a</b>) 0.2 m high into the water; (<b>b</b>) 0.3 m high into the water; (<b>c</b>) 0.5 m high into the water.</p>
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<p>Velocity flow line diagram of the calculation domain under different altitude conditions.</p>
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<p>Body water load change curve.</p>
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<p>Angular velocity variation curve of aircraft out of water attitude.</p>
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<p>Schematic diagram of cavitation phase transition of water flow in water-outlet process (portrait).</p>
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<p>Schematic diagram of cavitation phase transition of water flow in water-outlet process (overlook).</p>
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<p>Schematic diagram of shock wave generation.</p>
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<p>Schematic diagram of wave height curve changes under different water-entry angles.</p>
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<p>Schematic diagram of cavitation evolution of water phase volume fraction at different angles: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Schematic diagram of cavitation evolution of water phase volume fraction at different angles: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Schematic diagram of cavitation evolution of water phase volume fraction at different angles: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Schematic diagram of the angular velocity change curve of entering the water at different angles: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Schematic diagram of the change curve of the mechanical parameters of the body: (<b>a</b>) body load impact; (<b>b</b>) body movement speed; (<b>c</b>) body motion displacement.</p>
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<p>Phase volume fraction binary map: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Phase volume fraction binary map: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Schematic diagram of vertical velocity streamlines in the computational domain flow field: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Schematic diagram of vertical velocity streamlines in the computational domain flow field: (<b>a</b>–<b>e</b>) are, respectively, 0°, 10°, 20°, 30°, and 40° into the water.</p>
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<p>Variation curves of wave height at the central axis position under different wave intensities.</p>
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<p>Schematic diagram of cavitation evolution: (<b>a</b>) 0.3 m; (<b>b</b>) 0.4 m.</p>
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<p>Schematic diagram of cavitation evolution: (<b>a</b>) 0.3 m; (<b>b</b>) 0.4 m.</p>
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<p>The mechanical characteristic curves of the body: (<b>a</b>) load curve; (<b>b</b>) speed curve; (<b>c</b>) displacement curve.</p>
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<p>The mechanical characteristic curves of the body: (<b>a</b>) load curve; (<b>b</b>) speed curve; (<b>c</b>) displacement curve.</p>
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<p>Phase volume fraction binary map: (<b>a</b>) 0.3 m; (<b>b</b>) 0.4 m.</p>
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18 pages, 4130 KiB  
Article
Path Planning of Unmanned Aerial Vehicle in Complex Environments Based on State-Detection Twin Delayed Deep Deterministic Policy Gradient
by Danyang Zhang, Zhaolong Xuan, Yang Zhang, Jiangyi Yao, Xi Li and Xiongwei Li
Machines 2023, 11(1), 108; https://doi.org/10.3390/machines11010108 - 13 Jan 2023
Cited by 3 | Viewed by 2145
Abstract
This paper investigates the path planning problem of an unmanned aerial vehicle (UAV) for completing a raid mission through ultra-low altitude flight in complex environments. The UAV needs to avoid radar detection areas, low-altitude static obstacles, and low-altitude dynamic obstacles during the flight [...] Read more.
This paper investigates the path planning problem of an unmanned aerial vehicle (UAV) for completing a raid mission through ultra-low altitude flight in complex environments. The UAV needs to avoid radar detection areas, low-altitude static obstacles, and low-altitude dynamic obstacles during the flight process. Due to the uncertainty of low-altitude dynamic obstacle movement, this can slow down the convergence of existing algorithm models and also reduce the mission success rate of UAVs. In order to solve this problem, this paper designs a state detection method to encode the environmental state of the UAV’s direction of travel and compress the environmental state space. In considering the continuity of the state space and action space, the SD-TD3 algorithm is proposed in combination with the double-delayed deep deterministic policy gradient algorithm (TD3), which can accelerate the training convergence speed and improve the obstacle avoidance capability of the algorithm model. Further, to address the sparse reward problem of traditional reinforcement learning, a heuristic dynamic reward function is designed to give real-time rewards and guide the UAV to complete the task. The simulation results show that the training results of the SD-TD3 algorithm converge faster than the TD3 algorithm, and the actual results of the converged model are better. Full article
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<p>Schematic of battlefield environment.</p>
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<p>Probability model of radar detection.</p>
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<p>Schematic diagram of status detection code.</p>
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<p>The combination of the state probing method and the TD3 model.</p>
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<p>Training result of TD3 algorithm model in environment 1.</p>
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<p>Training result of TD3 algorithm model in environment 2.</p>
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<p>Training result of SD-TD3 (6) algorithm model in environment 1.</p>
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<p>Training results of SD-TD3 (6) algorithm model in Environment 2.</p>
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<p>Training result of SD-TD3 (12) algorithm model in environment 1.</p>
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<p>Training result of SD-TD3 (12) algorithm model in environment 2.</p>
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<p>The best training results of the three algorithmic models. (<b>a</b>) Best training results of the model in environment 1; (<b>b</b>) Best training results of the model in environment 2.</p>
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<p>Success rate of all algorithmic models in both environments.</p>
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17 pages, 2932 KiB  
Article
Strapdown Celestial Attitude Estimation from Long Exposure Images for UAV Navigation
by Samuel Teague and Javaan Chahl
Drones 2023, 7(1), 52; https://doi.org/10.3390/drones7010052 - 12 Jan 2023
Cited by 2 | Viewed by 1995
Abstract
Strapdown celestial imaging sensors provide a compact, lightweight alternative to their gimbaled counterparts. Strapdown imaging systems typically require a wider field of view, and consequently longer exposure intervals, leading to significant motion blur. The motion blur for a constellation of stars results in [...] Read more.
Strapdown celestial imaging sensors provide a compact, lightweight alternative to their gimbaled counterparts. Strapdown imaging systems typically require a wider field of view, and consequently longer exposure intervals, leading to significant motion blur. The motion blur for a constellation of stars results in a constellation of trails on the image plane. We present a method that extracts the path of these star trails, and uses a linearized weighted least squares approach to correct noisy inertial attitude measurements. We demonstrate the validity of this method through its application to synthetically generated images, and subsequently observe its relative performance by using real images. The findings of this study indicate that the motion blur present in strapdown celestial imagery yields an a posteriori mean absolute attitude error of less than 0.13 degrees in the yaw axis, and 0.06 degrees in the pitch and roll axes (3 σ) for a calibrated wide-angle camera lens. These findings demonstrate the viability of low-cost, wide-angle, strapdown celestial attitude sensors on lightweight UAV hardware. Full article
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<p>A region of interest containing a single star trail, captured from a strapdown celestial imaging sensor (Pi Camera HQ, 500 ms exposure interval). The shape of the star trail indicates that the camera was subjected to significant changes in attitude throughout the exposure interval.</p>
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<p>Flow diagram of image processing chain, with example images (black and white images converted to a perceptually uniform colour scale).</p>
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<p>An example of attitude correction, displaying a region of interest for a single star. Greyscale images are overlaid onto a three-channel image. <b>Left</b>: mean-only alignment, <b>Right</b>: fine attitude alignment. Green, real image; blue, synthetic image from INS; red, reprojection after corrections.</p>
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<p>Zeta Science FX61 airframe used for capturing in-flight imagery.</p>
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<p>An example of Perlin gradient-based noise generation across various octaves (frequencies).</p>
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<p>Histogram of mean absolute errors from each simulated image containing <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>14</mn> </mrow> </semantics></math> attitude references. (<b>a</b>) Yaw. (<b>b</b>) Pitch. (<b>c</b>) Roll.</p>
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<p>An example of simulation attitude correction, displaying superimposed regions of interest. Green channel, baseline simulation image; blue channel, synthetic image from noisy INS; red channel, synthetic image after corrections. Max yaw error: 0.0727<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math>, max pitch error: 0.0286<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math>, max roll error: 0.0226<math display="inline"><semantics> <msup> <mrow/> <mo>∘</mo> </msup> </semantics></math>.</p>
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<p>ROIs of stars used for attitude correction on a real image. Green channel, real image; blue channel, synthetic image from raw INS data; red channel, synthetic image from corrected INS data. The intensity of each ROI is amplified such that the peak pixel intensity is 255.</p>
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<p>ROIs of stars used for attitude correction on a real image. Green channel, real image; blue channel, synthetic image from raw INS data; red channel, synthetic image from corrected INS data. The intensity of each ROI is amplified such that the peak pixel intensity is 255.</p>
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31 pages, 9975 KiB  
Article
Energy Autonomy Simulation Model of Solar Powered UAV
by Krzysztof Mateja, Wojciech Skarka, Magdalena Peciak, Roman Niestrój and Maik Gude
Energies 2023, 16(1), 479; https://doi.org/10.3390/en16010479 - 1 Jan 2023
Cited by 9 | Viewed by 2523
Abstract
The energy autonomy of UAVs is an important direction in the field of aerospace. Long-endurance aerial vehicles allow for continuous flight; however, to meet the guidelines, the power supply system has to be able to harvest energy from outside. Solar cells allow the [...] Read more.
The energy autonomy of UAVs is an important direction in the field of aerospace. Long-endurance aerial vehicles allow for continuous flight; however, to meet the guidelines, the power supply system has to be able to harvest energy from outside. Solar cells allow the production of electricity during the day when the sun shines on their surface. Depending on the location, time, weather, and other external factors, the energy produced by PV panels will change. In order to calculate as accurately as possible the energy obtained by solar cells, we developed a simulation model that took into account all of the external restrictions and the UAV’s limits during flight. The conducted analysis made it possible to obtain information for the specific input data on whether the UAV is able to fly for 24 h in a specific flight scenario. The UAV powered by solar cells developed by us and the performed aviation missions have shown that the UAV is capable of continuous flight without the need to land. Full article
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<p>Explanation of air mass notion.</p>
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<p>Energy balance general diagram.</p>
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<p>Efficiency decrease in solar cells.</p>
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<p>Flow chart of choosing the parameters of the power supply system.</p>
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<p>TwinStratos 17 prototype.</p>
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<p>The simulation model and the flow of data.</p>
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<p>Solar cells samples: (<b>a</b>) Non-laminated solar cell in the test stand table; (<b>b</b>) Laminated solar cell coated with 100 μm PVC film.</p>
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<p>Samsung INR18650-35E tested in the insulation layer.</p>
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<p>General diagram of the TwinStratos power supply system.</p>
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<p>Flow chart of the energy balance of the UAV.</p>
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<p>Flight scenarios for TS17.</p>
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<p>Flight scenarios for TS12.</p>
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<p>Irradiation for Gliwice for different days beginning seasons of the year.</p>
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<p>Irradiation for different location in the Vernal equinox.</p>
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<p>Irradiation for Gliwice in vernal equinox for different altitude.</p>
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<p>I-V and P-V characteristics of the SunPower Maxeon Ne3.</p>
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<p>P-V and I-V characteristics of the laminated SunPower Maxeon Ne3 for different irradiance.</p>
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<p>P-V and I-V characteristics of the laminated SunPower Maxeon Ne3 for different temperatures.</p>
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<p>Power consumption of TS17 electric motors during climbing.</p>
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<p>Power consumption of TS12 electric motors during climbing.</p>
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<p>Power consumption of TS17 electric motors for cruise speed.</p>
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<p>Power consumption of TS12 electric motors for cruise speed.</p>
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<p>Tuned characteristics of the Samsung INR18650-35E battery simulation model.</p>
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<p>TwinStratos 17 5 km scenario in the vernal equinox.</p>
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<p>TwinStratos 17 5 km scenario in the summer solstice.</p>
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<p>TwinStratos 17 8 km scenario in the summer solstice.</p>
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<p>TwinStratos 12 10 km scenario in the vernal equinox.</p>
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<p>TwinStratos 12 15 km scenario in the vernal equinox.</p>
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<p>TwinStratos 12 20 km scenario in the vernal equinox.</p>
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<p>TwinStratos 12 20 km scenario in the summer solstice.</p>
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19 pages, 5650 KiB  
Article
An Aeromagnetic Compensation Algorithm Based on Radial Basis Function Artificial Neural Network
by Shuai Zhou, Changcheng Yang, Zhenning Su, Ping Yu and Jian Jiao
Appl. Sci. 2023, 13(1), 136; https://doi.org/10.3390/app13010136 - 22 Dec 2022
Cited by 6 | Viewed by 2141
Abstract
Aeromagnetic exploration is a magnetic exploration method that detects changes of the earth’s magnetic field by loading a magnetometer on an aircraft. With the miniaturization of magnetometers and the development of unmanned aerial vehicles (UAV) technology, UAV aeromagnetic surveying plays an increasingly important [...] Read more.
Aeromagnetic exploration is a magnetic exploration method that detects changes of the earth’s magnetic field by loading a magnetometer on an aircraft. With the miniaturization of magnetometers and the development of unmanned aerial vehicles (UAV) technology, UAV aeromagnetic surveying plays an increasingly important role in mineral exploration and other fields due to its advantages of low cost and safety. However, in the process of aeromagnetic measurement data, due to the ferromagnetic material of the aircraft itself and the change of flight direction and attitude, magnetic field interference will occur and affect the measurement of the geomagnetic field by the magnetometer. The work of aeromagnetic compensation is to compensate for this part of the magnetic interference and improve the magnetic measurement accuracy of the magnetometer. This paper focused on the problems of UAV aeromagnetic survey data processing and improved the accuracy of UAV based aeromagnetic data measurement. Based on the Tolles–Lawson model, a numerical simulation experiment of magnetic interference of UAV-based aeromagnetic data was carried out, and a radial basis function (RBF) artificial neural network (ANN) algorithm was proposed for the first time to compensate the aeromagnetic data. Compared with classical backpropagation (BP) ANN, the test results of the synthetic data and real measured magnetic data showed that the RBF-ANN has higher compensation accuracy and stronger generalization ability. Full article
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<p>Coordinate system conversion relationship.</p>
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<p>Structure diagram of BP-ANN.</p>
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<p>Structure diagram of RBF-ANN.</p>
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<p>Gaussian radial basis function.</p>
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<p>Simulation model of a three-axis fluxgate: (<b>a</b>) flight A; and (<b>b</b>) flight B.</p>
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<p>Aeromagnetic interference model corresponding to FOM flight.</p>
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<p>Simulation data compensation results: (<b>a</b>) test set flight A; and (<b>b</b>) test set flight B.</p>
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<p>UAV detection platform.</p>
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<p>Aeromagnetic measurement equipment.</p>
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<p>Flight C and Flight D flight paths.</p>
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<p>Aeromagnetic interference model: (<b>a</b>) Flight C; (<b>b</b>) Flight D.</p>
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<p>Flight C compensation results: (<b>a</b>) BP-ANN and BRF-ANN compensation results; and (<b>b</b>) compensation for the resulting sampling points 1000 to 1500.</p>
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<p>Flight D compensation results: (<b>a</b>) BP-ANN and BRF-ANN compensation results; and (<b>b</b>) compensation for the resulting sampling points 1000 to 1500.</p>
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20 pages, 13552 KiB  
Article
Exploring the Feasibility of Mitigating Flood Hazards by an Existing Pond System in Taoyuan, Taiwan
by Kuo-Hsin Tseng, Tsun-Hua Yang, Pei-Yuan Chen, Hwa Chien, Chi-Farn Chen and Yi-Chan Hung
Drones 2023, 7(1), 1; https://doi.org/10.3390/drones7010001 - 20 Dec 2022
Cited by 1 | Viewed by 1881
Abstract
Changes in the global climate have induced densified rainfall and caused natural hazards across the world in recent years. Formed by a central mountain range and a corridor of alluvial plains to the west, Taiwan is at risk of flood hazards owing to [...] Read more.
Changes in the global climate have induced densified rainfall and caused natural hazards across the world in recent years. Formed by a central mountain range and a corridor of alluvial plains to the west, Taiwan is at risk of flood hazards owing to its low-lying lands as well as the distinct seasonality of rainfall patterns. The rapid discharge of surface runoff and a growing number of impervious surfaces have also increased flood hazards during recent typhoon landfalls. A century ago, ancestors in Taoyuan City constructed a system of water channels composed of thousands of ponds to fulfill the needs of agriculture and aquaculture. During the expansion of urban areas, land reformation replaced a majority of earlier ponds with residential and industrial zones. However, the remaining ponds could potentially serve as on-site water detention facilities under the increasing risk of floods. In this research, we first renewed an outdated pond database by deploying a novel unmanned aerial vehicle (UAV) system with a micro-sonar to map the bathymetry of 80 ponds. Next, a simplified inundation model (SPM) was used to simulate the flood extent caused by different scenarios of rainfall in Bade District of Taoyuan City. Assuming that extremely that heavy rainfalls at 25, 50, 75, and 100 mm occurred in a very short period, the flood area would decrease by 96%, 75%, 52%, and 37%, respectively, when the ponds were preparatorily emptied. Full article
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<p>(Overview map) Taoyuan city in the red box is located in northern Taiwan. (Main) The pond system in Taoyuan City (blue) is a multipurpose water facility for various applications, for example: (<b>a</b>) irrigation; (<b>b</b>) fish farming; and (<b>c</b>) ecology parks.</p>
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<p>Bade District in Taoyuan City is the demonstration site for flood detention simulation: (<b>a</b>) an overview of Bade District and pond locations (black polygon); (<b>b</b>) a blow-up view of the orange box in panel (<b>a</b>). The 20-m resolution elevation model from MOI does not appropriately reveal bathymetry in pond locations (red); and (<b>c</b>) The DEM is modified within ponds by depth information from the government database or our fieldwork.</p>
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<p>Workflow for pond measurements and to build an integrated digital elevation model with neighboring terrain.</p>
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<p>(<b>a</b>) A sample of micro-sonar that can measure water depth in 0.6–40 m; and (<b>b</b>) the entire module combines a DJI-P3A UAV, a micro-sonar, and an Android phone in a waterproof bag.</p>
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<p>A schematic diagram of surveying parameters in the target pond, where <span class="html-italic">d</span> is the depth from sonar, O<sub>1</sub> is the highest water level without a water gate, and O<sub>2</sub> is the highest water level when a water gate exists. The slope along the pond edge is assumed a constant <span class="html-italic">S</span>.</p>
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<p>Two examples of the integrated pond model in YM145 (<b>left</b>) and BD033 (<b>right</b>). Color code indicates water depth based on the highest water level.</p>
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<p>A schematic of SPM redrawn from [<a href="#B22-drones-07-00001" class="html-bibr">22</a>,<a href="#B30-drones-07-00001" class="html-bibr">30</a>]: (<b>a</b>) the terrain is illustrated as nine cells with varying elevations; (<b>b</b>) the flood occurs at cell #5 and the steepest slope in this region is shown as the red arrow, between two (cell #1 and #2) out of eight possible flowing directions (orange arrows); the planar angles between the red arrow and directions to cell #1 and #2 (angle a and b) are used as weights to allocate water accumulated in cell #5; and (<b>c</b>) the allocation process is iterated among cells until reaching a balanced water level.</p>
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<p>(<b>a</b>) The Otter Unmanned Surface Vehicle (USV) and a Norbit iWBMS multibeam echosounder scanning bathymetry; (<b>b</b>) Our UAV and a micro-sonar measurement (14 points), and the IDW-interpolated bathymetry; and (<b>c</b>) Scatterplot of depth values over 14 points.</p>
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<p>The 80 selected pond models. Each pond has an area greater than 2500 m<sup>2</sup> and at least 10 measurement points.</p>
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<p>A log scale comparison of: (<b>a</b>) water extent; and and (<b>b</b>) water storage in 80 selected ponds.</p>
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<p>SPM flood simulation under 75 mm rainfall scenario by using pre-emptied ponds: (<b>a</b>) flood patches (blue) and their links to the unfilled ponds (black line); (<b>b</b>) reduced flood patches (red) after floodwater redistribution; and (<b>c</b>) three main routes of water redirection to reduce flood hazard.</p>
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<p>Simulation of the flooded area in Bade District (north up). The terrain declined from south to north. Four panels represent rainfall simulations from 25 mm to 100 mm. The base map adopts Sentinel-2 natural color composite on 17 November 2019.</p>
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<p>The percentage of the reduced flood area and volume based on the TYWR database and the ones based on our fieldwork.</p>
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<p>Land use map of Bade District. (modified from Taiwan MAP Service, National Land Surveying and Mapping Center, <a href="https://maps.nlsc.gov.tw" target="_blank">https://maps.nlsc.gov.tw</a> (accessed on 1 July 2022)).</p>
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12 pages, 3205 KiB  
Article
RF Source Localization Using Multiple UAVs through a Novel Geometrical RSSI Approach
by Nurbanu Güzey
Drones 2022, 6(12), 417; https://doi.org/10.3390/drones6120417 - 15 Dec 2022
Cited by 3 | Viewed by 1782
Abstract
In this paper, a novel geometrical localization scheme based on the Received Signal Strength Indicator (RSSI) is developed for a group of unmanned aerial vehicles (UAVs). Since RSSI-based localization does not require complicated hardware, it is the correct choice for RF target localization. [...] Read more.
In this paper, a novel geometrical localization scheme based on the Received Signal Strength Indicator (RSSI) is developed for a group of unmanned aerial vehicles (UAVs). Since RSSI-based localization does not require complicated hardware, it is the correct choice for RF target localization. In this promising work, unlike the other techniques given in the literature, transmit power or path loss exponent information is not needed. The procedure depends on the received power difference of each receiver in UAVs. In the developed scheme, four UAVs forming two groups fly in perpendicular planes. Each UAV in the group moves in a circle, keeping its distance from the plane’s center until it gets equal power with the other members of its group. Using this movement rate, lines passing through the source position are calculated. The intersection of these lines gives the position of the RF target. However, in a noisy environment, the lines do not intersect at one point. Therefore, the algorithm given in the manuscript finds a point that has a minimum distance to all lines and is also developed. Simulation results are provided at the end of the manuscript to verify our theoretical claims. Full article
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<p>Initial and desired locations of the UAVs.</p>
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<p>UAVs fly in the desired initial location with different received signal strengths.</p>
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<p>UAVs move in a circular formation to receive the same RSSI value.</p>
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<p>Flowchart of proposed localization method.</p>
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<p>Rotation of UAVs and a line passing through augmented point and formation center.</p>
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<p>Intersection of multiple lines, which gives the source location.</p>
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<p>(<b>a</b>) Received power by D1 and D3, (<b>b</b>) received power by D2 and D4, and (<b>c</b>) power differences of each group.</p>
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<p>Source localization in a noisy environment.</p>
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24 pages, 592 KiB  
Article
Sensorless and Coordination-Free Lane Switching on a Drone Road Segment—A Simulation Study
by Zhouyu Qu and Andreas Willig
Drones 2022, 6(12), 411; https://doi.org/10.3390/drones6120411 - 14 Dec 2022
Cited by 1 | Viewed by 1634
Abstract
Copter-type UAVs (unmanned aerial vehicles) or drones are expected to become more and more popular for deliveries of small goods in urban areas. One strategy to reduce the risks of drone collisions is to constrain their movements to a drone road system as [...] Read more.
Copter-type UAVs (unmanned aerial vehicles) or drones are expected to become more and more popular for deliveries of small goods in urban areas. One strategy to reduce the risks of drone collisions is to constrain their movements to a drone road system as far as possible. In this paper, for reasons of scalability, we assume that path-planning decisions for drones are not made centrally but rather autonomously by each individual drone, based solely on position/speed/heading information received from other drones through WiFi-based communications. We present a system model for moving drones along a straight road segment or tube, in which the tube is partitioned into lanes. We furthermore present a cost-based algorithm by which drones make lane-switching decisions, and evaluate the performance of differently parameterized versions of this algorithm, highlighting some of the involved tradeoffs. Our algorithm and results can serve as a baseline for more advanced algorithms, for example, including more elaborate sensors. Full article
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<p>Lane layout when looking along the tube in the <span class="html-italic">y</span>-direction.</p>
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<p>Beacon contents.</p>
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<p>Pseudocode of the GreedyLS algorithm.</p>
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<p>Average number of collisions per kilometre for varying drone generation rate <math display="inline"><semantics> <mi>λ</mi> </semantics></math> and beaconing rate <math display="inline"><semantics> <mi>β</mi> </semantics></math>. <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> km. With the Blind algorithm.</p>
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<p>Average number of collisions per kilometre for varying drone generation rate <math display="inline"><semantics> <mi>λ</mi> </semantics></math> and beaconing rate <math display="inline"><semantics> <mi>β</mi> </semantics></math>, without the Blind algorithm. <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> km.</p>
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<p>Average number of lane switching operations per drone per kilometre for selected algorithms.</p>
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<p>Average number of collisions per kilometre for varying drone generation rate <math display="inline"><semantics> <mi>λ</mi> </semantics></math> and different choices for <math display="inline"><semantics> <mrow> <mo>(</mo> <msubsup> <mi>ϵ</mi> <mn>1</mn> <mo>*</mo> </msubsup> <mo>,</mo> <msubsup> <mi>ϵ</mi> <mn>2</mn> <mo>*</mo> </msubsup> <mo>)</mo> </mrow> </semantics></math>, for Crowded, PreferOutside and PreferInside algorithms. <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> km.</p>
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<p>Average number of packet losses per kilometre for selected algorithms at a 20 Hz beaconing rate.</p>
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<p>Average speed per kilometre for selected algorithms.</p>
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<p>Average speed for varying drone generation rate <math display="inline"><semantics> <mi>λ</mi> </semantics></math> and different choices for <math display="inline"><semantics> <mrow> <mo>(</mo> <msubsup> <mi>ϵ</mi> <mn>1</mn> <mo>*</mo> </msubsup> <mo>,</mo> <msubsup> <mi>ϵ</mi> <mn>2</mn> <mo>*</mo> </msubsup> <mo>)</mo> </mrow> </semantics></math>, for Crowded, PreferOutside and PreferInside algorithms. <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> km.</p>
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<p>Average speed for varying drone generation rate <math display="inline"><semantics> <mi>λ</mi> </semantics></math> and different choices for <math display="inline"><semantics> <mrow> <mo>(</mo> <msubsup> <mi>ϵ</mi> <mn>1</mn> <mo>*</mo> </msubsup> <mo>,</mo> <msubsup> <mi>ϵ</mi> <mn>2</mn> <mo>*</mo> </msubsup> <mo>)</mo> </mrow> </semantics></math>, for Crowded, PreferOutside and PreferInside algorithms. <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> km.</p>
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<p>Average out-of-tube tier per kilometre for selected algorithms.</p>
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<p>Average number of collisions for selected algorithms under “stressed” and “normal” settings, for a low drone generation rate of 0.1 Hz.</p>
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16 pages, 6671 KiB  
Article
Efficiency Decreases in a Laminated Solar Cell Developed for a UAV
by Krzysztof Mateja, Wojciech Skarka and Aleksandra Drygała
Materials 2022, 15(24), 8774; https://doi.org/10.3390/ma15248774 - 8 Dec 2022
Cited by 5 | Viewed by 1577
Abstract
Achieving energy autonomy in a UAV (unmanned aerial vehicle) is an important direction for aerospace research. Long endurance flights allow for continuous observations, taking of measurements and control of selected parameters. To provide continuous flight, a UAV must be able to harvest energy [...] Read more.
Achieving energy autonomy in a UAV (unmanned aerial vehicle) is an important direction for aerospace research. Long endurance flights allow for continuous observations, taking of measurements and control of selected parameters. To provide continuous flight, a UAV must be able to harvest energy externally. The most popular method to achieve this is the use of solar cells on the wings and structure of the UAV. Flexible solar cells mounted on the surface of the wings can be damaged and contaminated. To prevent these negative changes, it is necessary to apply a protective coating to the solar cells. One of the more promising methods is lamination. To properly carry out this process, some parameters have to be appropriately adjusted. The appropriate selection of temperature and feed speed in the laminator allows a PV (photovoltaic) panel to be coated with film, minimizing any defects in the structure. Covering PV panels with film reduces the performance of the solar cells. By measuring the current–voltage characteristics, data were obtained showing the change in the performance of solar cells before and after lamination. In the case of testing flexible PV panels, the efficiency decreased from 24.29 to 23.33%. This informed the selection of the appropriate number of solar cells for the UAV, considering the losses caused by the lamination process. Full article
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<p>The first prototype of TwinStratos.</p>
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<p>Samples tests: (<b>a</b>) incision test of a film with a thickness of 250 μm with a burst gap; (<b>b</b>) incision test of a film with a thickness of 100 μm, which does not enlarge the damage.</p>
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<p>Laminated solar cells: (<b>a</b>) without defects; (<b>b</b>) adhesive stains on the surface caused by too fast feed; (<b>c</b>,<b>d</b>) damp patches from the adhesive caused by too low temperature of lamination.</p>
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<p>Laminated solar cells: (<b>a</b>) without defects; (<b>b</b>) adhesive stains on the surface caused by too fast feed; (<b>c</b>,<b>d</b>) damp patches from the adhesive caused by too low temperature of lamination.</p>
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<p>Test stand: (<b>a</b>) solar simulator with a xenon flash lamp, measuring table, and computer for downloading current–voltage characteristics; (<b>b</b>) research conducted on flexible solar cells placed on the measuring table.</p>
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<p>Characteristics of: (<b>a</b>) spectral response of Maxeon Ne3; (<b>b</b>) 100 μm film absorption; (<b>c</b>) 100 μm film reflection; (<b>d</b>) 100 μm film transmission.</p>
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<p>Characteristics of: (<b>a</b>) spectral response of Maxeon Ne3; (<b>b</b>) 100 μm film absorption; (<b>c</b>) 100 μm film reflection; (<b>d</b>) 100 μm film transmission.</p>
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<p>SEM textured surface topography of the N-type monocrystalline silicon solar cell.</p>
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<p>Rear surface of Maxeon Ne3 with visible connectors in the lower part.</p>
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<p>Topography of the electric contact surfaces of a monocrystalline silicon photovoltaic cell of the N-type: (<b>a</b>) contact of fingers (grid lines) with connectors; (<b>b</b>) finger (grid line).</p>
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<p>I–V and P–V characteristics of the SunPower Maxeon Ne3 cells.</p>
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<p>I–V curve at different irradiation levels for SunPower Maxeon Ne3 cells.</p>
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<p>P–V curve at different irradiation levels for SunPower Maxeon Ne3 cells.</p>
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<p>I–V curve at different temperatures for a SunPower Maxeon Ne3 cell.</p>
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<p>P–V curve at different temperatures for a SunPower Maxeon Ne3 cell.</p>
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27 pages, 10809 KiB  
Article
Aerodynamic Performance Analysis of VTOL Arm Configurations of a VTOL Plane UAV Using a Computational Fluid Dynamics Simulation
by Gesang Nugroho, Yoshua Dwiyanson Hutagaol and Galih Zuliardiansyah
Drones 2022, 6(12), 392; https://doi.org/10.3390/drones6120392 - 2 Dec 2022
Cited by 2 | Viewed by 6959
Abstract
A vertical take-off and landing plane (VTOL plane) is a fixed-wing unmanned aerial vehicle (FWUAV) configuration with the ability to take off and land vertically. It combines the benefits of fixed-wing and multirotor configurations, which gives it a high cruising range and independence [...] Read more.
A vertical take-off and landing plane (VTOL plane) is a fixed-wing unmanned aerial vehicle (FWUAV) configuration with the ability to take off and land vertically. It combines the benefits of fixed-wing and multirotor configurations, which gives it a high cruising range and independence from a runway. This configuration requires arms as mountings for the VTOL’s motors. This study discusses the design of a VTOL Plane with various VTOL arm configurations, and a computational fluid dynamics (CFD) simulation was conducted to find out which configuration performs the best aerodynamically. The VTOL arm configurations analyzed were a quad-plane, a twin-tail boom, a tandem wing, and a transverse arm. The interpreted performances were the lift and drag performances, stall conditions, flight efficiency, stability, and maneuverability. The relative wind directions toward the longitudinal axis of the UAV, which are the sideslip angle and the angle of attack, were varied to simulate various flying conditions. The results showed that the twin tail-boom is the most advantageous based on the interpreted performances. Full article
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<p>Definition of angle of attack and angle of sideslip.</p>
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<p>VTOL plane mission profile. Note: 1—ground test; 2—engine start and warm up; 3—VTOL take-off preparation; 4—VTOL take-off; 5—VTOL transition to forward flight; 6—Climb; 7—cruise; 8—loiter and cruise back; 9—descent; 10—forward flight transition to VTOL; 11—VTOL landing; 12—engine shutdown and ground test.</p>
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<p>Performance sizing graph.</p>
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<p>Wing planform design in mm.</p>
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<p>Schematic drawing of the VTOL motors’ position.</p>
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<p>Three-dimensional model of the VTOL plane with a twin-tail boom configuration.</p>
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<p>Three-dimensional model of the VTOL plane with a quad-plane configuration.</p>
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<p>Schematic drawing of the tandem wing configuration.</p>
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<p>Three-dimensional model of the VTOL plane with the tandem wing configuration.</p>
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<p>Schematic drawing of the transverse arm configuration.</p>
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<p>Three-dimensional model of the VTOL lane with a transverse arm configuration.</p>
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<p>Free-body diagram of the aircraft.</p>
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<p>Mesh results visualization.</p>
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<p>Orthogonal quality distribution.</p>
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<p>Skewness quality distribution.</p>
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<p>Pressure contours; (<b>a</b>) bottom view at 0° AoA, (<b>b</b>) top view at 0°AoA, (<b>c</b>) bottom view at 16° AoA, and (<b>d</b>) top view at 16° AoA.</p>
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<p>C<sub>L</sub> and C<sub>D</sub> in headwind conditions; (<b>a</b>) C<sub>L</sub> vs. AoA, and (<b>b</b>) C<sub>D</sub> vs. AoA.</p>
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<p>C<sub>L</sub> vs. AoA; sideslip angle: (<b>a</b>) 15°, and (<b>b</b>) 30°.</p>
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<p>L/D vs. AoA; sideslip angle: (<b>a</b>) 0°, (<b>b</b>) 15°, and (<b>c</b>) 30°.</p>
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<p>The stall phenomenon visualized by the airflow over the wing at (<b>a</b>) 0° AoA and (<b>b</b>) 24° AoA.</p>
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<p>Stall speed vs. AoA; sideslip angle: (<b>a</b>) 0°, (<b>b</b>) 15°, (<b>c</b>) 30°.</p>
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<p>Stall speed vs. AoA; sideslip angle: (<b>a</b>) 0°, (<b>b</b>) 15°, (<b>c</b>) 30°.</p>
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<p>C<sub>p</sub> vs. AoA; sideslip angle: (<b>a</b>) 0°, (<b>b</b>) 15°, and (<b>c</b>) 30°.</p>
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<p>C<sub>p</sub> vs. AoA; sideslip angle: (<b>a</b>) 0°, (<b>b</b>) 15°, and (<b>c</b>) 30°.</p>
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<p>C<sub>r</sub> vs. AoA; sideslip angle: (<b>a</b>) 15°, and (<b>b</b>) 30°.</p>
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<p>C<sub>r</sub> vs. AoA; sideslip angle: (<b>a</b>) 15°, and (<b>b</b>) 30°.</p>
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<p>C<sub>y</sub> vs. AoA; sideslip angle: (<b>a</b>) 15°, and (<b>b</b>) 30°.</p>
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<p>C<sub>y</sub> vs. AoA; sideslip angle: (<b>a</b>) 15°, and (<b>b</b>) 30°.</p>
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<p>Maneuverability in headwind conditions; bank angles: (<b>a</b>) 10°, (<b>b</b>) 20°, (<b>c</b>) 30°, and (<b>d</b>) 40°.</p>
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<p>Maneuverability in headwind conditions; bank angles: (<b>a</b>) 10°, (<b>b</b>) 20°, (<b>c</b>) 30°, and (<b>d</b>) 40°.</p>
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<p>Maneuverability in crosswind conditions; bank angle: (<b>a</b>) 10°, (<b>b</b>) 20°, (<b>c</b>) 30°, and (<b>d</b>) 40°.</p>
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<p>Maneuverability in crosswind conditions; bank angle: (<b>a</b>) 10°, (<b>b</b>) 20°, (<b>c</b>) 30°, and (<b>d</b>) 40°.</p>
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17 pages, 2882 KiB  
Article
Sliding Mode Path following and Control Allocation of a Tilt-Rotor Quadcopter
by Chih-Chen Yih and Shih-Jeh Wu
Appl. Sci. 2022, 12(21), 11088; https://doi.org/10.3390/app122111088 - 1 Nov 2022
Viewed by 1521
Abstract
A tilt-rotor quadcopter (TRQ) equipped with four tilt-rotors is more agile than its under-actuated counterpart and can fly at any path while maintaining the desired attitude. To take advantage of this additional control capability and enhance the quadrotor system’s robustness and capability, we [...] Read more.
A tilt-rotor quadcopter (TRQ) equipped with four tilt-rotors is more agile than its under-actuated counterpart and can fly at any path while maintaining the desired attitude. To take advantage of this additional control capability and enhance the quadrotor system’s robustness and capability, we designed two sliding mode controls (SMCs): the typical SMC exploits the properties of the rotational dynamics, and the modified SMC avoids undesired chattering. Our simulation studies show that the proposed SMC scheme can follow the planned flight path and keep the desired attitude in the presence of variable deviations and external perturbations. We demonstrate from the Lyapunov stability theorem that the proposed control scheme can guarantee the asymptotic stability of the TRQ in terms of position and attitude following via control allocation. Full article
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<p>The schematic diagram of the TRQ for modeling.</p>
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<p>The TRQ control scheme.</p>
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<p>The attitude path with variable deviations.</p>
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<p>The position path with variable deviations.</p>
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<p>The propelling force with variable deviations.</p>
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<p>The turning torque with variable deviations.</p>
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<p>The tilt angle path with variable deviations.</p>
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<p>The rotor velocity with variable deviations.</p>
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<p>The attitude path with variable deviations and perturbations.</p>
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<p>The position path with variable deviations and perturbations.</p>
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<p>The propelling force with variable deviations and perturbations.</p>
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<p>The turning torque with variable deviations and perturbations.</p>
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<p>The tilt angle path with variable deviations and perturbations.</p>
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<p>The rotor velocity with variable deviations and perturbations.</p>
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23 pages, 2254 KiB  
Article
Minimum Energy Control of Quadrotor UAV: Synthesis and Performance Analysis of Control System with Neurobiologically Inspired Intelligent Controller (BELBIC)
by Wojciech Giernacki
Energies 2022, 15(20), 7566; https://doi.org/10.3390/en15207566 - 13 Oct 2022
Cited by 5 | Viewed by 1832
Abstract
There is a strong trend in the development of control systems for multi-rotor unmanned aerial vehicles (UAVs), where minimization of a control signal effort is conducted to extend the flight time. The aim of this article is to shed light on the problem [...] Read more.
There is a strong trend in the development of control systems for multi-rotor unmanned aerial vehicles (UAVs), where minimization of a control signal effort is conducted to extend the flight time. The aim of this article is to shed light on the problem of shaping control signals in terms of energy-optimal flights. The synthesis of a UAV autonomous control system with a brain emotional learning based intelligent controller (BELBIC) is presented. The BELBIC, based on information from the feedback loop of the reference signal tracking system, shows a high learning ability to develop an appropriate control action with low computational complexity. This extends the capabilities of commonly used fixed-value proportional–integral–derivative controllers in a simple but efficient manner. The problem of controller tuning is treated here as a problem of optimization of the cost function expressing control signal effort and maximum precision flight. The article introduces several techniques (bio-inspired metaheuristics) that allow for quick self-tuning of the controller parameters. The performance of the system is comprehensively analyzed based on results of the experiments conducted for the quadrotor model. Full article
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<p>Block diagram of the BEL model (briefly characterized in <a href="#sec1dot4-energies-15-07566" class="html-sec">Section 1.4</a>), proposed by Moren and Balkenius [<a href="#B29-energies-15-07566" class="html-bibr">29</a>], where: SI—sensory input, ES—emotional signal, OC—orbitofrontal cortex, A—amygdala, MO—memory output.</p>
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<p>Block diagram for autonomous control of the UAV (thrust and torques <math display="inline"><semantics> <msub> <mi>u</mi> <mi>i</mi> </msub> </semantics></math> for <span class="html-italic">i</span> = <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mn>4</mn> </mrow> </semantics></math> are defined in Equation (<a href="#FD15-energies-15-07566" class="html-disp-formula">15</a>).</p>
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<p>Reference frames related to the X4-flyer II simplified graphics. Left (4) and right (2) propulsion units rotate clockwise, while the front (1) and rear (3) counterclockwise.</p>
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<p>(<b>a</b>) BEL computational model, (<b>b</b>) SISO closed-loop control system with BELBIC controller.</p>
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<p>MATLAB-based block diagram of the UAV autonomous control system with BELBIC controllers (inputs: UAV’s desired position in <math display="inline"><semantics> <msub> <mi>x</mi> <mi>d</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>y</mi> <mi>d</mi> </msub> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>z</mi> <mi>d</mi> </msub> </semantics></math> axis and desired yaw angle <math display="inline"><semantics> <msub> <mi>ψ</mi> <mi>d</mi> </msub> </semantics></math>; while output: UAV state vector of current position and orientation).</p>
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<p>The CFA algorithm [<a href="#B51-energies-15-07566" class="html-bibr">51</a>].</p>
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<p>Experiment No. 1: An exemplary test of the effectiveness of square-shaped path tracking for the X-4 Flyer II drone model in a system with BELBIC controllers tuned by trial and error: (<b>a</b>–<b>c</b>) reference (desired) and actual (measured) positions of the UAV on the <span class="html-italic">X</span>, <span class="html-italic">Y</span>, and <span class="html-italic">Z</span> axes, (<b>d</b>) flight trajectory in 3D.</p>
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<p>Experiment No. 2: Function <math display="inline"><semantics> <mrow> <mi>I</mi> <mi>A</mi> <mi>E</mi> <mo>=</mo> <mi>f</mi> <mo>(</mo> <msub> <mi>K</mi> <mi>i</mi> </msub> <mo>)</mo> </mrow> </semantics></math> (for <math display="inline"><semantics> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mn>3</mn> </mrow> </semantics></math>).</p>
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<p>Experiment No. 2: Function <math display="inline"><semantics> <mrow> <mi>I</mi> <mi>A</mi> <mi>E</mi> <mo>=</mo> <mi>f</mi> <mo>(</mo> <msub> <mi>K</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>K</mi> <mn>2</mn> </msub> <mo>,</mo> <msub> <mi>K</mi> <mn>3</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for gains limited to the value of 400 and <math display="inline"><semantics> <mi>α</mi> </semantics></math> = <math display="inline"><semantics> <mrow> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mi>β</mi> </semantics></math> = <math display="inline"><semantics> <mrow> <mn>0.01</mn> </mrow> </semantics></math>.</p>
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<p>Experiment No. 2: Test of the performance of circle-shaped path tracking for the X-4 Flyer II drone model in a system with BELBIC altitude controller: (<b>a</b>) reference (desired) and actual (measured) positions of the UAV in the <span class="html-italic">Z</span> axes and (<b>b</b>) flight trajectory in 3D.</p>
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<p>Experiment No. 3: (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>Z</mi> <mo>=</mo> <mi>f</mi> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </semantics></math> [m] of the X-4 Flyer II drone model in a system with BELBIC altitude controller in 5 s flight time horizon for <math display="inline"><semantics> <mi mathvariant="sans-serif">Ψ</mi> </semantics></math> = <math display="inline"><semantics> <mrow> <mi>v</mi> <mi>a</mi> <mi>r</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">Γ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, (<b>b</b>) IAE and IAU values.</p>
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28 pages, 17076 KiB  
Article
Aerodynamic Numerical Simulation Analysis of Water–Air Two-Phase Flow in Trans-Medium Aircraft
by Jun Wei, Yong-Bai Sha, Xin-Yu Hu, Jin-Yan Yao and Yan-Li Chen
Drones 2022, 6(9), 236; https://doi.org/10.3390/drones6090236 - 3 Sep 2022
Cited by 4 | Viewed by 2795
Abstract
A trans-medium aircraft is a new concept aircraft that can both dive in the water and fly in the air. In this paper, a new type of water–air multi-medium span vehicle is designed based on the water entry and exit structure model of [...] Read more.
A trans-medium aircraft is a new concept aircraft that can both dive in the water and fly in the air. In this paper, a new type of water–air multi-medium span vehicle is designed based on the water entry and exit structure model of a multi-rotor UAV. Based on the designed structural model of the cross-media aircraft, the OpenFOAM open source numerical platform is used to analyze the single-medium aerodynamic characteristics and the multi-medium spanning flow analysis. The rotating flow characteristics of single-medium air rotor and underwater propeller are calculated by sliding mesh. In order to prevent the numerical divergence caused by the deformation of the grid movement, the overset grid method and the multiphase flow technology are used for the numerical simulation of the water entry and exit of the cross-medium aircraft. Through the above analysis, the flow field characteristics of the trans-medium vehicle in different media are verified, and the changes in the body load and attitude at different water entry angles are also obtained during the process of medium crossing. Full article
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<p>Flight control rigid body model for trans-media aircraft.</p>
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<p>Schematic diagram of the coordinate system of the trans-media aircraft.</p>
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<p>Schematic diagram of the multi-medium spanning force of a trans-medium aircraft (<b>a</b>) Free entry; (<b>b</b>) Out of water.</p>
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<p>Schematic diagram of the force of a trans-medium aircraft entering water at a certain attitude angle.</p>
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<p>Vertical access to water: (<b>a</b>) vertical into the water; (<b>b</b>) vertical out of water.</p>
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<p>Enter and exit the water at a certain attitude angle: (<b>a</b>) water entry process; (<b>b</b>) out of water process.</p>
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<p>APC1047SF air rotor: (<b>a</b>) physical map; (<b>b</b>) model diagram.</p>
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<p>Flow computation domain: (<b>a</b>) computational domain scale modeling; (<b>b</b>) computational domain division and boundary setting.</p>
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<p>Schematic diagram of computational domain meshing results: (<b>a</b>) outer domain meshing situation; (<b>b</b>) air rotor meshing; (<b>c</b>) inner domain meshing; (<b>d</b>) meshing of the interface between the inner and outer domains.</p>
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<p>Schematic diagram of computational domain meshing results: (<b>a</b>) outer domain meshing situation; (<b>b</b>) air rotor meshing; (<b>c</b>) inner domain meshing; (<b>d</b>) meshing of the interface between the inner and outer domains.</p>
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<p>Numerical thrust and experimental thrust at different rotational speeds.</p>
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<p>Cloud map of aerodynamic characteristics of a single propeller of an air rotor. (<b>a</b>) RPM = <math display="inline"><semantics> <mrow> <mn>2</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>b</b>) RPM = <math display="inline"><semantics> <mrow> <mn>3</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>c</b>) RPM = <math display="inline"><semantics> <mrow> <mn>5</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>d</b>) RPM = <math display="inline"><semantics> <mrow> <mn>7</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>e</b>) RPM = <math display="inline"><semantics> <mrow> <mn>8</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math> (unit <math display="inline"><semantics> <mrow> <mi>r</mi> <mi>o</mi> <mi>u</mi> <mi>n</mi> <mi>d</mi> <mo>×</mo> <mi>m</mi> <mi>i</mi> <msup> <mi>n</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>).</p>
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<p>Cloud map of aerodynamic characteristics of a single propeller of an air rotor. (<b>a</b>) RPM = <math display="inline"><semantics> <mrow> <mn>2</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>b</b>) RPM = <math display="inline"><semantics> <mrow> <mn>3</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>c</b>) RPM = <math display="inline"><semantics> <mrow> <mn>5</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>d</b>) RPM = <math display="inline"><semantics> <mrow> <mn>7</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math>; (<b>e</b>) RPM = <math display="inline"><semantics> <mrow> <mn>8</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>3</mn> </msup> </mrow> </semantics></math> (unit <math display="inline"><semantics> <mrow> <mi>r</mi> <mi>o</mi> <mi>u</mi> <mi>n</mi> <mi>d</mi> <mo>×</mo> <mi>m</mi> <mi>i</mi> <msup> <mi>n</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>).</p>
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<p>Schematic diagram of the tip vortex.</p>
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<p>Schematic diagram of wake vortex structure.</p>
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<p>Curve diagram of physical quantities changing with time and space: (<b>a</b>) graph of pressure versus position; (<b>b</b>) graph of pressure change with time; (<b>c</b>) graph of velocity versus position; (<b>d</b>) graph of speed change with time.</p>
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<p>Schematic diagram of grid and computational domain division: (<b>a</b>) fluid computational domain size; (<b>b</b>) computational domain boundary conditions; (<b>c</b>) internal and external computational domain division; (<b>d</b>) blade meshing.</p>
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<p>Hover state tip vortex.</p>
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<p>Numerical cloud map in hover state: (<b>a</b>) pressure cloud map; (<b>b</b>) axial velocity contour.</p>
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<p>Forward flight wakes at different forward flight speeds.</p>
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<p>Numerical contour of flow field under different forward flight speeds: (<b>a</b>) longitudinal pressure contour; (<b>b</b>) longitudinal velocity contour; (<b>c</b>) axial velocity contour.</p>
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<p>Numerical contour of flow field under different forward flight speeds: (<b>a</b>) longitudinal pressure contour; (<b>b</b>) longitudinal velocity contour; (<b>c</b>) axial velocity contour.</p>
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<p>Variation diagram of the force characteristics of each blade of the aircraft: (<b>a</b>) forward flight speed is 1.5 <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>•</mo> <msup> <mi>s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; (<b>b</b>) forward flight speed is 5 <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>•</mo> <msup> <mi>s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; (<b>c</b>) forward flight speed is 10 <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>•</mo> <msup> <mi>s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>.</p>
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<p>Variation diagram of the force characteristics of each blade of the aircraft: (<b>a</b>) forward flight speed is 1.5 <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>•</mo> <msup> <mi>s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; (<b>b</b>) forward flight speed is 5 <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>•</mo> <msup> <mi>s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>; (<b>c</b>) forward flight speed is 10 <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>•</mo> <msup> <mi>s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>.</p>
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<p>Schematic diagram of single propeller meshing: (<b>a</b>) computational domain model parameters; (<b>b</b>) boundary conditions and division of internal and external domains.</p>
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<p>Propeller hydrodynamic performance curve.</p>
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<p>(<b>a</b>) Flow field area grid; (<b>b</b>) background mesh and overset mesh; (<b>c</b>) background grid and overset grid area marker map (1 for overset grid, 0 for background grid).</p>
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<p>(<b>a</b>) Pressure curve; (<b>b</b>) speed curve.</p>
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<p>Attitude change curve of entering water at different angles.</p>
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<p>The physical evolution process of cavitation entering water from different angles: (<b>a</b>) vertical into the water; (<b>b</b>–<b>e</b>) inclined angle into the water (10°, 20°, 30°, 40°).</p>
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20 pages, 1664 KiB  
Article
Fast Terminal Sliding Mode Fault-Tolerant Control for Markov Jump Nonlinear Systems Based on an Adaptive Observer
by Pu Yang, Ziwei Shen, Yu Ding and Kejia Feng
Drones 2022, 6(9), 233; https://doi.org/10.3390/drones6090233 - 2 Sep 2022
Cited by 3 | Viewed by 1933
Abstract
In this paper, a new adaptive observer is proposed to estimate the actuator fault and disturbance of a quadrotor UAV system with actuator failure and disturbance. Based on this, a nonsingular fast terminal sliding mode controller is designed. Firstly, according to the randomness [...] Read more.
In this paper, a new adaptive observer is proposed to estimate the actuator fault and disturbance of a quadrotor UAV system with actuator failure and disturbance. Based on this, a nonsingular fast terminal sliding mode controller is designed. Firstly, according to the randomness of faults and disturbances, the UAV system under faults and disturbances is regarded as one of the Markov jump nonlinear systems (MJNSs). Secondly, an adaptive observer is designed to simultaneously observe the system state, fault, and disturbance. In order to improve the precision, the fast adaptive fault estimation (FAFE) algorithm is adopted in the adaptive observer. In addition, a quasi-one-sided Lipschitz condition is used to deal with the nonlinear term, which relaxes the condition and contains more nonlinear information. Finally, a nonsingular fast terminal sliding mode controller is designed for fault-tolerant control of the system. The simulation results show that the faults and disturbances can be observed successfully, and that the system is stochastic stable. Full article
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<p>Model of a quadrotor.</p>
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<p>Qdrone.</p>
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<p>OptiTrack Flex-3 motion capture cameras.</p>
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<p>The ground station.</p>
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<p>System mode.</p>
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<p>Estimated fault and disturbance from observer.</p>
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<p>State response of attitude angle.</p>
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<p>State response of angular velocity.</p>
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<p>State response of the attitude angle by the method in [<a href="#B43-drones-06-00233" class="html-bibr">43</a>].</p>
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<p>State response of the angular velocity by the method in [<a href="#B43-drones-06-00233" class="html-bibr">43</a>].</p>
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19 pages, 638 KiB  
Article
Factors Associated with the Adoption of Drones for Product Delivery in the Context of the COVID-19 Pandemic in Medellín, Colombia
by Alejandro Valencia-Arias, Paula Andrea Rodríguez-Correa, Juan Camilo Patiño-Vanegas, Martha Benjumea-Arias, Jhony De La Cruz-Vargas and Gustavo Moreno-López
Drones 2022, 6(9), 225; https://doi.org/10.3390/drones6090225 - 27 Aug 2022
Cited by 9 | Viewed by 3942
Abstract
This study aims to identify the factors associated with the adoption of drone delivery in Medellín, Colombia, in the context of the COVID-19 pandemic. For that purpose, it implemented the Diffusion of Innovation (DOI) theory and the Technology Acceptance Model (TAM), which have [...] Read more.
This study aims to identify the factors associated with the adoption of drone delivery in Medellín, Colombia, in the context of the COVID-19 pandemic. For that purpose, it implemented the Diffusion of Innovation (DOI) theory and the Technology Acceptance Model (TAM), which have constructs that complement each other to determine the decision to accept a given technology. A survey was administered to 121 participants in order to validate the model proposed here, which is based on variables that reflect the perceived attributes and risks of this innovation and individuals’ characteristics. The results indicate that the factors Performance Risk, Compatibility, Personal Innovativeness, and Relative Advantage of Environmental Friendliness have the greatest influence on Intention to Use Drone Delivery (mediated by Attitude Towards Drone Delivery). This paper offers relevant information for the academic community and delivery companies because few other studies have investigated this topic. Additionally, the proposed technology adoption model can be a benchmark for other emerging economies in similar social, economic, and technological conditions. Full article
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<p>Model of adoption of drone delivery in Medellín.</p>
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21 pages, 13617 KiB  
Article
Design and Analysis of a Deployment Mechanism with Clearance Compensation for High Stiffness Missile Wings
by Yong Zhao, Shang Chen, Yimeng Gao, Honghao Yue, Xiaoze Yang, Tongle Lu and Fei Yang
Drones 2022, 6(8), 211; https://doi.org/10.3390/drones6080211 - 17 Aug 2022
Cited by 2 | Viewed by 4081
Abstract
The deployment performance of the unfolded wing determines whether the winged missiles can fly normally after being launched, infecting the attack performance of the winged missiles. The paper proposes a new deployment mechanism with clearance eliminator. Based on the slider-crank principle, the proposed [...] Read more.
The deployment performance of the unfolded wing determines whether the winged missiles can fly normally after being launched, infecting the attack performance of the winged missiles. The paper proposes a new deployment mechanism with clearance eliminator. Based on the slider-crank principle, the proposed deployment mechanism achieves fast and low-impact deployment of the wings. The proposed clearance eliminator with shape memory alloy (SMA) effectively eliminates the clearance of the sliding pair and improves the support stiffness and stability of the deployed wing. The collision characteristics and the clearance elimination are studied for the deployment mechanism. The influence of the collision force on the motion state of the wing during the deployment is analyzed. The static stiffness of the wing under the clearance state and the deformation is analyzed. The dynamic stiffness under the catapult clearance elimination state is modeled based on the fractal geometry and contact stress theory. The relationship between the locking force and the support stiffness is revealed. The kinetic simulation is used to analyze the motion response during the action of the deployment mechanism. Modal analysis, harmonic response analysis, and random vibration analysis were conducted for the whole wings. A prototype was developed to verify the ejection performance of the wing according to the input load characteristics. The dynamic stiffness of the unfolded wings is tested by the fundamental frequency experiments to verify the performance of the clearance elimination assembly. The experimental results show that the designed deployment mechanism with clearance compensation achieves fast ejection and high stiffness retention of the missile wing. Full article
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<p>Deployment mechanism for the missile wings.</p>
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<p>The principle of wing ejection and locking.</p>
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<p>Structure of drive actuator.</p>
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<p>Working principle of drive actuator.</p>
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<p>Configuration of clearance eliminator.</p>
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<p>Configuration of SMA driver.</p>
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<p>Working principle of the clearance eliminator.</p>
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<p>Simplified model of the wing deployment mechanism.</p>
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<p>Collision force at the driving joint.</p>
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<p>Collision force at the wing joint.</p>
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<p>The effect of clearance on the displacement of the wing.</p>
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<p>The effect of clearance on the velocity of the wing.</p>
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<p>Static stiffness analysis of the missile wing.</p>
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<p>Schematic of the wing subjected to normal load.</p>
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<p>Deflection angle–load relationship.</p>
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<p>Deflection–load relationship.</p>
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<p>Relationship between <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mrow> <mi>S</mi> <mi>M</mi> <mi>A</mi> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mi>f</mi> </semantics></math>.</p>
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<p>Equivalent diagram of the support part.</p>
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<p>Vibration frequency versus locking force.</p>
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<p>The relationship between the intrinsic frequency of the wing and the locking force.</p>
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<p>Displacement versus time.</p>
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<p>Velocity versus time.</p>
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<p>Mesh division and modal analysis under docking condition.</p>
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<p>Modal analysis with deployment: (<b>a</b>) Pre-stress loading; (<b>b</b>) Results of modal analysis.</p>
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<p>Amplitude–frequency response characteristics.</p>
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<p>Schematic diagram of maximum deformation of the wing during resonance.</p>
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<p>Loaded power spectral density.</p>
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<p>Displacement response spectrum.</p>
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<p>Acceleration response.</p>
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<p>Principle prototype of deployment mechanism.</p>
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<p>High-speed camera test system.</p>
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<p>Testing results of the high-speed camera.</p>
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<p>Wing load test.</p>
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<p>Modal test experiment.</p>
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<p>The amplitude–frequency of the wing vibration.</p>
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<p>The mode of wing vibration.</p>
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14 pages, 2456 KiB  
Article
A Neural Network Approach to Estimate Transient Aerodynamic Properties of a Flapping Wing System
by Bluest Lan, You-Jun Lin, Yu-Hsiang Lai, Chia-Hung Tang and Jing-Tang Yang
Drones 2022, 6(8), 210; https://doi.org/10.3390/drones6080210 - 17 Aug 2022
Cited by 2 | Viewed by 2217
Abstract
Understanding the causal impacts among various parameters is essential for designing micro aerial vehicles (MAVs). The simulation of computational fluid dynamics (CFD) provides us with a technique to calculate aerodynamic forces precisely. However, even a single result regularly takes considerable computational time. Machine [...] Read more.
Understanding the causal impacts among various parameters is essential for designing micro aerial vehicles (MAVs). The simulation of computational fluid dynamics (CFD) provides us with a technique to calculate aerodynamic forces precisely. However, even a single result regularly takes considerable computational time. Machine learning, due to the advance in computer hardware, shows another approach that can speed up the analysis process. In this study, we introduce an artificial neural network (ANN) framework to predict the transient aerodynamic forces and the corresponding energy consumption. Instead of considering the whole transient changes of each parameter as inputs, we utilised the technique of Fourier transform to simplify the ANN structure for minimising the computation cost. Furthermore, two typical activation functions, rectified linear unit (ReLU) and sigmoid, were attempted to build the network. The validity of the method was further examined by comparing it with CFD simulation. The result shows that both functions are able to provide highly accurate estimations that can be implemented for model construction under this framework. Consequently, this novel approach makes it possible to reduce the complexity of analysis, study the flapping wing aerodynamics and enable a more efficient way to optimise parameters. Full article
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<p>Experimental setup. (<b>a</b>) Photograph of a blue tiger butterfly (<span class="html-italic">T. septentrionis</span>). (<b>b</b>) Measurement method. Two synchronised high-speed cameras were mounted onto a transparent chamber orthogonally along the y- and z-axis. By utilising the photographed images, a butterfly’s position could be determined.</p>
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<p>Angle parameters of a flying butterfly. (<b>a</b>) Definitions of angles. From the coordinates of each feature’s points, body pitching angle <math display="inline"><semantics> <mi>θ</mi> </semantics></math>, sweeping angle <math display="inline"><semantics> <mi>η</mi> </semantics></math>, rotation angle <math display="inline"><semantics> <mi>α</mi> </semantics></math> and flapping angle <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math> were obtained. (<b>b</b>) Angles measured from the experiments (<math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>15</mn> </mrow> </semantics></math>). The solid lines indicate four feature angles; the surrounding shaded areas represent the 95% confidence intervals. The abscissa axis denotes the normalised time in a flapping period; the blue area (from <math display="inline"><semantics> <mrow> <mi>T</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> to 0.6) indicates the downstroke phase, and the rest (from <math display="inline"><semantics> <mrow> <mi>T</mi> <mo>=</mo> <mn>0.6</mn> </mrow> </semantics></math> to 1) is upstroke.</p>
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<p>Conditions of the simulation. (<b>a</b>) Boundary conditions (inlet: velocity, outlet: pressure). (<b>b</b>) Grid convergence test.</p>
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<p>Generated datasets. The data were randomly separated into training (64%, blue markers, <math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>16</mn> </mrow> </semantics></math>), validation (16%, red markers, <math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math>) and testing (20%, amber markers, <math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math>) groups. The testing data were merely utilised for evaluation and did not participate in the training processes.</p>
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<p>Structure of an ANN model. The inputs were <span class="html-italic">b</span> and <span class="html-italic">w</span>, and the outputs were Fourier coefficients of <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mi>h</mi> </msub> <mo>,</mo> <msub> <mi>F</mi> <mi>v</mi> </msub> <mo>,</mo> <msub> <mi>F</mi> <mi>w</mi> </msub> </mrow> </semantics></math> and <span class="html-italic">P</span>.</p>
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<p>Two types of activation functions.</p>
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<p>Loss, the MSE of the 44 output parameters, of ReLU- (<b>a</b>) and sigmoid- (<b>b</b>) based ANN training processes.</p>
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<p><span class="html-italic">k</span>-Fold cross validation (<math display="inline"><semantics> <mrow> <mi>k</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math>).</p>
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<p>Validation of the two models in comparison with the CFD simulation. The black solid lines were calculated by CFD simulation; the blue and red dashed lines were obtained from the ReLU- and sigmoid-based ANNs, respectively.</p>
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<p>Net vertical force <math display="inline"><semantics> <msub> <mover accent="true"> <mi>F</mi> <mo>¯</mo> </mover> <mi>v</mi> </msub> </semantics></math> and corresponding efficiency <math display="inline"><semantics> <msub> <mover accent="true"> <mi>E</mi> <mo>¯</mo> </mover> <mi>v</mi> </msub> </semantics></math> in a single flapping period.</p>
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<p>Optimal aerodynamics obtained by the ANN in comparison with CFD simulated result.</p>
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17 pages, 2874 KiB  
Article
Imagery Synthesis for Drone Celestial Navigation Simulation
by Samuel Teague and Javaan Chahl
Drones 2022, 6(8), 207; https://doi.org/10.3390/drones6080207 - 15 Aug 2022
Cited by 4 | Viewed by 3153
Abstract
Simulation plays a critical role in the development of UAV navigation systems. In the context of celestial navigation, the ability to simulate celestial imagery is particularly important, due to the logistical and legal constraints of conducting UAV flight trials after dusk. We present [...] Read more.
Simulation plays a critical role in the development of UAV navigation systems. In the context of celestial navigation, the ability to simulate celestial imagery is particularly important, due to the logistical and legal constraints of conducting UAV flight trials after dusk. We present a method for simulating night-sky star field imagery captured from a rigidly mounted ‘strapdown’ UAV camera system, with reference to a single static reference image captured on the ground. Using fast attitude updates and spherical linear interpolation, images are superimposed to produce a finite-exposure image that accurately captures motion blur due to aircraft actuation and aerodynamic turbulence. The simulation images are validated against a real data set, showing similarity in both star trail path and magnitude. The outcomes of this work provide a simulation test environment for the development of celestial navigation algorithms. Full article
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<p>Celestial equatorial coordinate system.</p>
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<p>Calibration curve of image brightness using a PiCamHQ, 500 ms exposure time.</p>
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<p>Calibration of standard deviation in star brightness using a PiCamHQ, 500 ms exposure time.</p>
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<p>Pixel intensity of a measured star (red wireframe), with the simulated pixel intensity overlaid (blue solid).</p>
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<p>Phantom FX-61 with camera mounted in fuselage.</p>
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<p>Lower magnitude stars captured in-flight (4× increased brightness for display purposes).</p>
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<p>Close-up of bright stars captured in motion. Real images (left) are paired with their simulated counterpart (right). (<b>a</b>) Image captured during aerial manoeuvre; (<b>b</b>) Image captured during constant-rate turn; (<b>c</b>) Image captured with high pitch-rate; (<b>d</b>) Image captured during aerial manoeuvre.</p>
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<p>Individual stars over multiple images, comparing measured intensity to simulated intensity. Red crosses indicate the peak pixel intensity for a given observation. (<b>a</b>) Visual magnitude: 1.5, mean error: <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>23.6</mn> </mrow> </semantics></math>, mean percentage error: 37.5%; (<b>b</b>) Visual magnitude: 2.25, mean error: 12.2, mean percentage error: 82.3%; (<b>c</b>) Visual magnitude: 2.45, mean error: <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>6.3</mn> </mrow> </semantics></math>, mean percentage error: 38.0%.</p>
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<p>Histogram of absolute differences in star centroids between real and simulated images.</p>
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20 pages, 7078 KiB  
Article
Genetic Algorithm and Greedy Strategy-Based Multi-Mission-Point Route Planning for Heavy-Duty Semi-Rigid Airship
by Shaoxing Hu, Bingke Wang, Aiwu Zhang and Yiming Deng
Sensors 2022, 22(13), 4954; https://doi.org/10.3390/s22134954 - 30 Jun 2022
Cited by 2 | Viewed by 1732
Abstract
The large volume and windward area of the heavy-duty semi-rigid airship (HSA) result in a large turning radius when the HSA passes through every mission point. In this study, a multi-mission-point route planning method for HSA based on the genetic algorithm and greedy [...] Read more.
The large volume and windward area of the heavy-duty semi-rigid airship (HSA) result in a large turning radius when the HSA passes through every mission point. In this study, a multi-mission-point route planning method for HSA based on the genetic algorithm and greedy strategy is proposed to direct the HSA maneuver through every mission point along the optimal route. Firstly, according to the minimum flight speed and the maximum turning slope angle of the HSA during turning, the minimum turning radius of the HSA near each mission point is determined. Secondly, the genetic algorithm is used to determine the optimal flight sequence of the HSA from the take-off point through all the mission points to the landing point. Thirdly, based on the optimal flight sequence, the shortest route between every two adjacent mission points is obtained by using the route planning method based on the greedy strategy. By determining the optimal flight sequence and the shortest route, the optimal route for the HSA to pass through all mission points can be obtained. The experimental results show that the method proposed in this study can generate the optimal route with various conditions of the mission points using simulation studies. This method reduces the total voyage distance of the optimal route by 18.60% on average and improves the flight efficiency of the HSA. Full article
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<p>The overall flow chart of the route planning algorithm proposed. The input offline information includes HSA take-off and landing points and route mission points, the minimum flight speed, and the maximum turning slope angle of the HSA during turning.</p>
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<p>Flow chart of route planning method based on the greedy strategy. The initial input information includes the coordinates of the multi-mission points of the optimal flight sequence of the HAS and the coordinates of the circle center <math display="inline"><semantics> <mrow> <msub> <mi>O</mi> <mi>O</mi> </msub> </mrow> </semantics></math> of the take-off point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>O</mi> </msub> </mrow> </semantics></math>.</p>
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<p>Schematic diagram of route planning when the distance <math display="inline"><semantics> <mrow> <msub> <mi>D</mi> <mrow> <msub> <mi>O</mi> <mi>i</mi> </msub> <msup> <mrow/> <mo>′</mo> </msup> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> </mrow> </msub> </mrow> </semantics></math> is less than the minimum turning radius <math display="inline"><semantics> <mi>R</mi> </semantics></math>. (<b>a</b>) is the schematic diagram of route planning at <math display="inline"><semantics> <mrow> <mo>∠</mo> <msub> <mi>O</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>≤</mo> <mn>90</mn> </mrow> </semantics></math>, (<b>b</b>) is the schematic diagram of a route planning at <math display="inline"><semantics> <mrow> <mo>∠</mo> <msub> <mi>O</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>&gt;</mo> <mn>90</mn> </mrow> </semantics></math>, the red line is the calculated shortest route.</p>
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<p>Schematic diagram of route planning when the distance <math display="inline"><semantics> <mrow> <msub> <mi>D</mi> <mrow> <msub> <mi>O</mi> <mi>i</mi> </msub> <msup> <mrow/> <mo>′</mo> </msup> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> </mrow> </msub> </mrow> </semantics></math> is less than the minimum turning radius <math display="inline"><semantics> <mi>R</mi> </semantics></math>. (<b>a</b>) is the schematic diagram of route planning at <math display="inline"><semantics> <mrow> <mo>∠</mo> <msub> <mi>O</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>≤</mo> <mn>90</mn> </mrow> </semantics></math>, (<b>b</b>) is the schematic diagram of a route planning at <math display="inline"><semantics> <mrow> <mo>∠</mo> <msub> <mi>O</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>&gt;</mo> <mn>90</mn> </mrow> </semantics></math>, the red line is the calculated shortest route.</p>
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<p>Schematic diagram of route planning when the distance <math display="inline"><semantics> <mrow> <msub> <mi>D</mi> <mrow> <msub> <mi>O</mi> <mi>i</mi> </msub> <msup> <mrow/> <mo>′</mo> </msup> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> </mrow> </msub> </mrow> </semantics></math> is equal to the minimum turning radius <math display="inline"><semantics> <mi>R</mi> </semantics></math>. (<b>a</b>) is the schematic diagram of route planning at <math display="inline"><semantics> <mrow> <mo>∠</mo> <msub> <mi>O</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>≤</mo> <mn>90</mn> </mrow> </semantics></math>, (<b>b</b>) is the schematic diagram of a route planning at <math display="inline"><semantics> <mrow> <mo>∠</mo> <msub> <mi>O</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mi>i</mi> </msub> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>&gt;</mo> <mn>90</mn> </mrow> </semantics></math>, the red line is the calculated shortest route.</p>
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<p>Schematic diagram of optimal route. <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>O</mi> </msub> </mrow> </semantics></math> is the take-off and landing point of the HSA, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>P</mi> <mn>2</mn> </msub> <mo>,</mo> <msub> <mi>P</mi> <mn>3</mn> </msub> <mo>,</mo> <msub> <mi>P</mi> <mn>4</mn> </msub> </mrow> </semantics></math> are the input multi-mission points, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>O</mi> </msub> <mo>→</mo> <msub> <mi>P</mi> <mn>2</mn> </msub> <mo>→</mo> <msub> <mi>P</mi> <mn>4</mn> </msub> <mo>→</mo> <msub> <mi>P</mi> <mn>3</mn> </msub> <mo>→</mo> <msub> <mi>P</mi> <mn>1</mn> </msub> <mo>→</mo> <msub> <mi>P</mi> <mi>O</mi> </msub> </mrow> </semantics></math> is the optimal flight sequence based on the genetic algorithm, and the red line is the optimal route obtained by the route planning method based on the greedy strategy.</p>
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<p>Layout of route planning simulation software developed for multi-mission-point route planning. After selecting the “Multi-Mission Points” mode, the user can click “Set Mission”, then click on the map to set the coordinates of the multi-mission points, and finally click “Generate”. And the optimal route will be displayed on the map.</p>
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<p>Representative HSA, Zeppelin NT airship adopted in the simulation study and validation.</p>
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<p>The mission point selection diagram, where the unnumbered point represents the take-off and landing point, and the marked points numbered <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>~</mo> <mn>9</mn> </mrow> </semantics></math> represent the nine mission points selected in sequence.</p>
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<p>The partial enlarged view of the optimal route of mission points <math display="inline"><semantics> <mrow> <mn>8</mn> <mo>→</mo> <mn>3</mn> </mrow> </semantics></math>. The red line with arrows is the calculated best route, the marked points represent the mission point.</p>
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<p>Schematic diagram of the route distance of two adjacent mission points corresponding to different parameters <math display="inline"><semantics> <mi>θ</mi> </semantics></math>. (<b>a</b>) the relationship between parameter <math display="inline"><semantics> <mi>θ</mi> </semantics></math> and the route distance of the mission points <math display="inline"><semantics> <mrow> <mn>2</mn> <mo>→</mo> <mn>1</mn> </mrow> </semantics></math>, (<b>b</b>) the relationship between parameter <math display="inline"><semantics> <mi>θ</mi> </semantics></math> and the route distance of the mission points <math display="inline"><semantics> <mrow> <mn>8</mn> <mo>→</mo> <mn>3</mn> </mrow> </semantics></math>.</p>
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<p>Schematic diagram of the output result of the route planning software. The blue line with arrows is the calculated best route, and the red line is the route that the simulated airship has traveled. And the output shows that the total route distance of the optimal route is 15,139.92 m.</p>
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<p>The main types of DUBINS path. <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>S</mi> </msub> </mrow> </semantics></math> represents the beginning speed direction, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math> represents the ending speed direction,<math display="inline"><semantics> <mi>S</mi> </semantics></math> represents the straight line, <math display="inline"><semantics> <mi>R</mi> </semantics></math> represents the right turn, and <math display="inline"><semantics> <mi>L</mi> </semantics></math> represents the left turn. (<b>a</b>) LSL means that the HSA starts from the beginning point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>S</mi> </msub> </mrow> </semantics></math>, first turns left, then goes straight line, and finally turns left to the ending point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math>. (<b>b</b>) RSR means that the HSA starts from the beginning point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>S</mi> </msub> </mrow> </semantics></math>, first turns right, then goes straight line, and finally turns right to the ending point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math>. (<b>c</b>) RSL means that the HSA starts from the beginning point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>S</mi> </msub> </mrow> </semantics></math>, first turns right, then goes straight line, and finally turns left to the ending point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math>. (<b>d</b>) LSR means that the HSA starts from the beginning point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>S</mi> </msub> </mrow> </semantics></math>, first turns left, then goes straight line, and finally turns right to the ending point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math>. (<b>e</b>) RLR means that the HSA starts from the beginning point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>S</mi> </msub> </mrow> </semantics></math>, first turns right, then turns left, and finally turns right to the ending point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math>. (<b>f</b>) LRL means that the HSA starts from the beginning point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>S</mi> </msub> </mrow> </semantics></math>, first turns left, then urns right, and finally turns left to the ending point <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>E</mi> </msub> </mrow> </semantics></math>.</p>
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<p>Schematic diagram of the simulation results of the multi-mission-point route planning method based on DUBINS curve. The red line with arrows is the calculated best route, and the blue line is the route that the simulated airship has traveled. And the output shows that the total route distance of the optimal route is 18,637.87 m.</p>
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17 pages, 3408 KiB  
Article
A Reliable Merging Link Scheme Using Weighted Markov Chain Model in Vehicular Ad Hoc Networks
by Siman Emmanuel, Ismail Fauzi Bin Isnin and Mohd. Murtadha Bin Mohamad
Sensors 2022, 22(13), 4861; https://doi.org/10.3390/s22134861 - 27 Jun 2022
Cited by 1 | Viewed by 1665
Abstract
The vehicular ad hoc network (VANET) is a potential technology for intelligent transportation systems (ITS) that aims to improve safety by allowing vehicles to communicate quickly and reliably. The rates of merging collision and hidden terminal problems, as well as the problems of [...] Read more.
The vehicular ad hoc network (VANET) is a potential technology for intelligent transportation systems (ITS) that aims to improve safety by allowing vehicles to communicate quickly and reliably. The rates of merging collision and hidden terminal problems, as well as the problems of picking the best match cluster head (CH) in a merged cluster, may emerge when two or more clusters are merged in the design of a clustering and cluster management scheme. In this paper, we propose an enhanced cluster-based multi-access channel protocol (ECMA) for high-throughput and effective access channel transmissions while minimizing access delay and preventing collisions during cluster merging. We devised an aperiodic and acceptable merge cluster head selection (MCHS) algorithm for selecting the optimal merge cluster head (MCH) in centralized clusters where all nodes are one-hop nodes during the merging window. We also applied a weighted Markov chain mathematical model to improve accuracy while lowering ECMA channel data access transmission delay during the cluster merger window. We presented extensive simulation data to demonstrate the superiority of the suggested approach over existing state-of-the-arts. The implementation of a MCHS algorithm and a weight chain Markov model reveal that ECMA is distinct and more efficient by 64.20–69.49% in terms of average network throughput, end-to-end delay, and access transmission probability. Full article
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<p>Merging cluster structure.</p>
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<p>Merge collision due to node mobility [<a href="#B20-sensors-22-04861" class="html-bibr">20</a>]. Note: THSO is the ratio of a THS’s necessary time slots to the total number of time slots available for that THS.</p>
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<p>Illustrations of cluster merging phases (from M –&gt; N –&gt; L –&gt; Q).</p>
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<p>The transition process of <span class="html-italic">X</span><sub>n</sub>.</p>
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<p>(<b>a</b>): Diagram of ECMA protocol. (<b>b</b>): Merge cluster head channel access.</p>
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<p>(<b>a</b>): Diagram of ECMA protocol. (<b>b</b>): Merge cluster head channel access.</p>
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<p>Access delay at various state.</p>
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<p>CH lifetime and it influence on Mw.</p>
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<p>CM disconnection frequency and it influence on Mw.</p>
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<p>CM disconnection frequency and it influence on Mw.</p>
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<p>Average network throughput versus average velocity.</p>
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<p>Average end-to-end delay versus average velocity.</p>
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<p>Successful access transmission probability versus average velocity.</p>
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25 pages, 11863 KiB  
Article
An Autonomous Control Framework of Unmanned Helicopter Operations for Low-Altitude Flight in Mountainous Terrains
by Zibo Jin, Lu Nie, Daochun Li, Zhan Tu and Jinwu Xiang
Drones 2022, 6(6), 150; https://doi.org/10.3390/drones6060150 - 17 Jun 2022
Cited by 3 | Viewed by 2777
Abstract
Low-altitude flight in mountainous terrains is a difficult flight task applied in both military and civilian fields. The helicopter has to maintain low altitude to realize search and rescue, reconnaissance, penetration, and strike operations. It contains complex environment perception, multilevel decision making, and [...] Read more.
Low-altitude flight in mountainous terrains is a difficult flight task applied in both military and civilian fields. The helicopter has to maintain low altitude to realize search and rescue, reconnaissance, penetration, and strike operations. It contains complex environment perception, multilevel decision making, and multi-objective flight control; thus, flight is currently mainly conducted by human pilots. In this work, a control framework is implemented to realize autonomous flight for unmanned helicopter operations in an unknown mountainous environment. The identification of targets and threats is introduced using a deep neural network. A 3D vector field histogram method is adopted for local terrain avoidance based on airborne Lidar sensors. In particular, we propose an intuitive direct-viewing method to judge and change the visibilities of the helicopter. On this basis, a finite state machine is built for decision making of the autonomous flight. A highly realistic simulation environment is established to verify the proposed control framework. The simulation results demonstrate that the helicopter can autonomously complete flight missions including a fast approach, threat avoidance, cover concealment, and circuitous flight operations similar to human pilots. The proposed control framework provides an effective solution for complex flight tasks and expands the flight control technologies for high-level unmanned helicopter operations. Full article
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<p>Cascade PID controllers of the helicopter control channels: (<b>a</b>) longitude channel; (<b>b</b>) lateral channel; (<b>c</b>) altitude channel; (<b>d</b>) yaw channel.</p>
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<p>Cascade PID controllers of the helicopter control channels: (<b>a</b>) longitude channel; (<b>b</b>) lateral channel; (<b>c</b>) altitude channel; (<b>d</b>) yaw channel.</p>
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<p>Closed-loop system of the realistic simulation environment.</p>
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<p>Realistic scenario of the mountainous terrain.</p>
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<p>Structure of the YOLO Network.</p>
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<p>Precision–recall (PR) curve of the YOLO network.</p>
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<p>Circling flight around the target.</p>
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<p>Visual servo control of the circling flight.</p>
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<p>Flight path of the helicopter hovering around a static target.</p>
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<p>Helicopter linear velocities during a circling flight.</p>
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<p>Anchor box size during a circling flight.</p>
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<p>Flight path of the helicopter hovering around a moving target.</p>
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<p>Formation of the 2D primary polar histogram.</p>
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<p>Generation of point-cloud data of virtual Lidar sensor.</p>
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<p>Narrow mountainous area with additional obstacles.</p>
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<p>Flight path of the 3D VFH method.</p>
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<p>Helicopter linear velocities during the low-altitude flight.</p>
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<p>Helicopter during the low-altitude flight.</p>
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<p>Direct-viewing method of visibility judgement.</p>
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<p>Finite state machine of the decision-making framework.</p>
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<p>Simulation scene of the low-altitude flight.</p>
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<p>Flight paths of the flight tasks in the low-altitude flight: (<b>a</b>) long-range penetration; (<b>b</b>) fast approach; (<b>c</b>) fast avoidance; (<b>d</b>) circuitous flight.</p>
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<p>Diagrammatic presentation of all flight tasks.</p>
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13 pages, 807 KiB  
Article
Hybrid Quasi-Optimal PID-SDRE Quadrotor Control
by Wojciech Giernacki, Sławomir Stępień, Marcin Chodnicki and Agnieszka Wróblewska
Energies 2022, 15(12), 4312; https://doi.org/10.3390/en15124312 - 13 Jun 2022
Cited by 4 | Viewed by 1881
Abstract
In the paper, a new cascade control system for an autonomous flight of an unmanned aerial vehicle (UAV) based on Proportional–Integral–Derivative (PID) and finite-time State-Dependent Riccati Equation (SDRE) control is proposed. The PID and SDRE controllers are used in a hybrid control system [...] Read more.
In the paper, a new cascade control system for an autonomous flight of an unmanned aerial vehicle (UAV) based on Proportional–Integral–Derivative (PID) and finite-time State-Dependent Riccati Equation (SDRE) control is proposed. The PID and SDRE controllers are used in a hybrid control system for precise control and stabilization, which is necessary to increase the drone’s flight stability and maneuver precision. The hybrid PID-SDRE control system proposed for the quadrotor model is quasi-optimal, since the suboptimal control algorithm for the UAV stabilization is used. The combination of the advantages of PID and SDRE control gives a significant improvement in the quality of control while maintaining the simplicity of the control system. Furthermore, the use of the suboptimal control technique provides the UAV attitude tracking in finite time. These remarks are drawn from a series of simulation tests conducted for the drone model. Full article
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<p>AtraxASF UAV used for drone modeling and simulation experiments.</p>
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<p>PID-SDRE control schema of the 6 DoF quadcopter model.</p>
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<p>UAV angular response—PID control mode.</p>
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<p>UAV angular speed response—PID control mode.</p>
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<p>Angular response of UAV—PID-SDRE control mode, <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math> s.</p>
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<p>UAV angular speed response—PID-SDRE control mode, <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math> s.</p>
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<p>Angular response of UAV—PID-SDRE control mode, <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math> s.</p>
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<p>UAV angular speed response—PID-SDRE control mode, <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math> s.</p>
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<p>Angular response of the UAV—PID-SDRE control mode, <math display="inline"><semantics> <msub> <mi>t</mi> <mi>f</mi> </msub> </semantics></math> = 1 s.</p>
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<p>UAV angular speed response—PID-SDRE control mode, <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> s.</p>
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22 pages, 23952 KiB  
Article
Enhanced Single Shot Small Object Detector for Aerial Imagery Using Super-Resolution, Feature Fusion and Deconvolution
by Mahdi Maktab Dar Oghaz, Manzoor Razaak and Paolo Remagnino
Sensors 2022, 22(12), 4339; https://doi.org/10.3390/s22124339 - 8 Jun 2022
Cited by 10 | Viewed by 2623
Abstract
One common issue of object detection in aerial imagery is the small size of objects in proportion to the overall image size. This is mainly caused by high camera altitude and wide-angle lenses that are commonly used in drones aimed to maximize the [...] Read more.
One common issue of object detection in aerial imagery is the small size of objects in proportion to the overall image size. This is mainly caused by high camera altitude and wide-angle lenses that are commonly used in drones aimed to maximize the coverage. State-of-the-art general purpose object detector tend to under-perform and struggle with small object detection due to loss of spatial features and weak feature representation of the small objects and sheer imbalance between objects and the background. This paper aims to address small object detection in aerial imagery by offering a Convolutional Neural Network (CNN) model that utilizes the Single Shot multi-box Detector (SSD) as the baseline network and extends its small object detection performance with feature enhancement modules including super-resolution, deconvolution and feature fusion. These modules are collectively aimed at improving the feature representation of small objects at the prediction layer. The performance of the proposed model is evaluated using three datasets including two aerial images datasets that mainly consist of small objects. The proposed model is compared with the state-of-the-art small object detectors. Experiment results demonstrate improvements in the mean Absolute Precision (mAP) and Recall values in comparison to the state-of-the-art small object detectors that investigated in this study. Full article
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<p>Objects in UAV images are usually small in size (proportional to total image size) and general purpose object detectors are not designed to cope with it [<a href="#B11-sensors-22-04339" class="html-bibr">11</a>].</p>
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<p>Poor feature representation of small objects at deeper layers of typical Convolutional Neural Networks, which are usually caused by multiple pooling and stride &gt;1 processes.</p>
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<p>Network architecture of the proposed object detection model. The SSD model is used as the baseline network and extended to include deconvolution module (orange), super-resolution module (green), and shallow layer feature fusion module (<b>+</b>).</p>
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<p>Schematic comparison of approaches used by different types of object detectors. (<b>a</b>) Single stage detectors (e.g., YOLO). (<b>b</b>) Multi-level features used at prediction layer (e.g., SSD). (<b>c</b>) Approach of supplying shallow layer features for prediction (e.g., FSSD). (<b>d</b>) Deconvolutional layers for improved feature representation (e.g., DSSD). (<b>e</b>) Network schema of our proposed approach.</p>
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<p>A deconvolutional module unit used after the SSD layers.</p>
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<p>A deconvolutional module unit merged with an SSD layer using element-wise sum operation.</p>
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<p>The super-resolution module.</p>
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<p>Concatenation of the <math display="inline"><semantics> <mrow> <mi>C</mi> <mi>o</mi> <mi>n</mi> <mi>v</mi> <mn>4</mn> <mo>_</mo> <mn>3</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>C</mi> <mi>o</mi> <mi>n</mi> <mi>v</mi> <mn>5</mn> <mo>_</mo> <mn>3</mn> </mrow> </semantics></math> feature layers.</p>
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<p>Example images of the livestock dataset. In the images, sheep are small targets for the object detectors.</p>
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<p>Comparison of small object detection between the proposed network (<b>bottom row</b>), the SSD network (<b>middle row</b>) and the FS-SSD network (<b>top row</b>) on the custom livestock dataset.</p>
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<p>Qualitative evaluation of bounding box predictions by the proposed network on custom livestock dataset. Blue boxes correspond to the ground truth label and red boxes are the predicted bounding boxes.</p>
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<p>Comparison of small object detection of our proposed network (bottom row) with the SSD network (top row) onthe <span class="html-italic">Pedestrian</span> category from the Stanford drone dataset.</p>
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<p>Comparison of small object detection of our proposed network (<b>bottom row</b>) with SSD network (<b>top row</b>) on a custom dataset acquired under MONICA project data.</p>
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<p>Speed and accuracy comparison of the proposed method with the state-of-the-art methods on the livestock dataset. It can be observed that the proposed model supersedes other approaches in terms of mAP, which makes it suitable for applications where accuracy is critically important.</p>
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<p>Comparison between the proposed model mAP with some other object detectors on the SDD dataset. Car, Bicyclist, and Pedestrian categories were considered in this comparison.</p>
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<p>Comparison of mAP with IoU of 0.5 and 0.75 on the <span class="html-italic">Pedestrian</span> category of the SDD dataset.</p>
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14 pages, 3861 KiB  
Article
Mission Chain Driven Unmanned Aerial Vehicle Swarms Cooperation for the Search and Rescue of Outdoor Injured Human Targets
by Yusen Cao, Fugui Qi, Yu Jing, Mingming Zhu, Tao Lei, Zhao Li, Juanjuan Xia, Jianqi Wang and Guohua Lu
Drones 2022, 6(6), 138; https://doi.org/10.3390/drones6060138 - 28 May 2022
Cited by 8 | Viewed by 3258
Abstract
A novel cooperative strategy for distributed unmanned aerial vehicle (UAV) swarms with different functions, namely the mission chain-driven unmanned aerial vehicle swarms cooperation method, is proposed to allow the fast search and timely rescue of injured human targets in a wide-area outdoor environment. [...] Read more.
A novel cooperative strategy for distributed unmanned aerial vehicle (UAV) swarms with different functions, namely the mission chain-driven unmanned aerial vehicle swarms cooperation method, is proposed to allow the fast search and timely rescue of injured human targets in a wide-area outdoor environment. First, a UAV-camera unit is exploited to detect the suspected human target combined with improved deep learning technology. Then, the target location information is transferred to a self-organizing network. Then, the special bio-radar-UAV unit was released to recheck the survivals through a respiratory characteristic detection algorithm. Finally, driven by the location and vital sign status of the injured, a nearby emergency-UAV unit will perform corresponding medical emergency missions, such as dropping emergency supplies. Experimental results show that this strategy can identify the human targets autonomously from the outdoor environment effectively, and the target detection, target sensing, and medical emergency mission chain is completed successfully relying on the cooperative working mode, which is meaningful for the future search-rescue mission of outdoor injured human targets. Full article
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<p>UAV swarm’s collaboration system.</p>
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<p>Collaboration between UAVs with different functions.</p>
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<p>UAV swarms for carrying real-time target detection and sensing systems.</p>
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<p>Main configuration of the outdoor first-aid kit.</p>
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<p>Schematic diagram of UAV Swarms.</p>
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<p>Yolov4-tiny feature structure diagram.</p>
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<p>Schematic diagram of sensing life.</p>
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<p>Design of the life sensing device; (<b>a</b>) Stm32F103; (<b>b</b>) Positioning module; (<b>c</b>) LoRa; (<b>d</b>) Bio-radar; (<b>e</b>) System power switch.</p>
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<p>Design of the air communication device on the UAV; (<b>a</b>) Nvidia Jetson Nano; (<b>b</b>) Usb-ttl; (<b>c</b>) Usb-ttl; (<b>d</b>) Radio module; (<b>e</b>) LoRa; (<b>f</b>) Stm32F103; (<b>g</b>) Battery.</p>
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<p>(<b>a</b>) Real-time formation test of four UAVs, (<b>b</b>) Target detection experiment based on UAV swarms with different functions.</p>
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<p>Human target detection. (<b>a</b>) Human target in the weed cover. (<b>b</b>) Human target in the gully.</p>
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<p>Respiration signal detection. (<b>a</b>) Different distances and angles. (<b>b</b>) Respiration signal waveform.</p>
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<p>Emergency UAV for emergency supply.</p>
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19 pages, 6751 KiB  
Article
An Acoustic Fault Detection and Isolation System for Multirotor UAV
by Adam Bondyra, Marek Kołodziejczak, Radosław Kulikowski and Wojciech Giernacki
Energies 2022, 15(11), 3955; https://doi.org/10.3390/en15113955 - 27 May 2022
Cited by 18 | Viewed by 2572
Abstract
With the rising popularity of unmanned aerial vehicles (UAVs) and increasing variety of their applications, the task of providing reliable and robust control systems becomes significant. An active fault-tolerant control (FTC) scheme requires an effective fault detection and isolation (FDI) algorithm to provide [...] Read more.
With the rising popularity of unmanned aerial vehicles (UAVs) and increasing variety of their applications, the task of providing reliable and robust control systems becomes significant. An active fault-tolerant control (FTC) scheme requires an effective fault detection and isolation (FDI) algorithm to provide information about the fault’s occurrence and its location. This work aims to present a prototype of a diagnostic system intended to recognize and identify broken blades of rotary wing UAVs. The solution is based on an analysis of acoustic emission recorded with an onboard microphone array paired with a lightweight yet powerful single-board computer. The standalone hardware of the FDI system was utilized to collect a wide and publicly available dataset of recordings in real-world experiments. The detection algorithm itself is a data-driven approach that makes use of an artificial neural network to classify characteristic features of acoustic signals. Fault signature is based on Mel Frequency Spectrum Coefficients. Furthermore, in the paper an extensive evaluation of the model’s parameters was performed. As a result, a highly accurate fault classifier was developed. The best models allow not only a detection of fault occurrence, but thanks to multichannel data provided with a microphone array, the location of the impaired rotor is reported, as well. Full article
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<p>Samples of rotors used in fault detection experiments and overview of the propulsion test rig.</p>
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<p>Performance comparison of faulty and undamaged rotors: thrust of a single motor–rotor unit (<b>top</b>) and achieved power efficiency (<b>bottom</b>).</p>
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<p>The <span class="html-italic">Falcon V5</span> UAV used for FDI experiments and a detailed view of the coaxial propulsion unit.</p>
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<p>The stack of <span class="html-italic">Raspberry Pi 3B+</span> SBC and microphone array module.</p>
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<p>Experimental setup to acquire acoustic data.</p>
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<p>Summary of the pretraining signal processing steps.</p>
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<p>Structure of the LSTM-based fault classifier.</p>
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<p>Structure of CNN-based fault classifier.</p>
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<p>Process of gathering samples of acoustic dataset and evaluating FDI method.</p>
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<p>Types of fault scenarios considered in experiments: (<b>1</b>) no faults, (<b>2</b>) single damaged rotor, (<b>3</b>) dual fault, adjacent, (<b>4</b>) dual fault, opposite actuators.</p>
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<p>Samples of recorded audio signals along with their PSD estimates: (<b>a</b>) all rotors healthy, (<b>b</b>) single damaged rotor, opposite microphone, (<b>c</b>) single damaged rotor, closest microphone.</p>
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<p>Samples of recorded audio signals along with their PSD estimates: (<b>a</b>) all rotors healthy, (<b>b</b>) single damaged rotor, opposite microphone, (<b>c</b>) single damaged rotor, closest microphone.</p>
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15 pages, 271 KiB  
Article
User Preferences in Drone Design and Operation
by Kyungdoh Kim
Drones 2022, 6(5), 133; https://doi.org/10.3390/drones6050133 - 23 May 2022
Cited by 3 | Viewed by 3405
Abstract
Drones, which were first used in military applications, are now widely used by civilians for various purposes such as for deliveries and as cameras. There has been a lack of research into what drone users expect in terms of drone design and operation [...] Read more.
Drones, which were first used in military applications, are now widely used by civilians for various purposes such as for deliveries and as cameras. There has been a lack of research into what drone users expect in terms of drone design and operation from a user perspective. In order to figure out what users want from drones, it is necessary to investigate the perception and design preferences of users with regard to drones. Surveys were conducted to collect data on preferences for various aspects of the design and operation of drone technology. Features relevant to the design and operation of drones were considered. We have identified the underlying factor structures of drone design and operation: outdoor mission type, user interface, military mission type, usefulness, risk, special mission type, and concern. The most important factors that contribute to all the dependent variables are the user interface and usefulness. The fact that drones will be increasingly used in the future is clear; however, the purpose of this study was to find out the areas on which to focus and pay further attention. Full article
24 pages, 17606 KiB  
Article
Flight Test of Autonomous Formation Management for Multiple Fixed-Wing UAVs Based on Missile Parallel Method
by Guang Zhan, Zheng Gong, Quanhui Lv, Zan Zhou, Zian Wang, Zhen Yang and Deyun Zhou
Drones 2022, 6(5), 99; https://doi.org/10.3390/drones6050099 - 19 Apr 2022
Cited by 4 | Viewed by 3722
Abstract
This paper reports on the formation and transformation of multiple fixed-wing unmanned aerial vehicles (UAVs) in three-dimensional space. A cooperative guidance law based on the classic missile-type parallel-approach method is designed for the multi-UAV formation control problem. Additionally, formation transformation strategies for multi-UAV [...] Read more.
This paper reports on the formation and transformation of multiple fixed-wing unmanned aerial vehicles (UAVs) in three-dimensional space. A cooperative guidance law based on the classic missile-type parallel-approach method is designed for the multi-UAV formation control problem. Additionally, formation transformation strategies for multi-UAV autonomous assembly, disbandment, and special circumstances are formed, effective for managing and controlling the formation. When formulating the management strategy for formation establishment, its process is divided into three steps: (i) selecting and allocating target points, (ii) forming loose formations, and (iii) forming short-range formations. The management of disbanding the formation is formulated through reverse thinking: the assembly process is split and recombined in reverse, and a formation disbanding strategy that can achieve a smooth transition from close to lose formation is proposed. Additionally, a strategy is given for adjusting the formation transformation in special cases, and the formation adjustment is completed using the adjacency matrix. Finally, a hardware-in-the-loop simulation and measured flight verification using a simulator show the practicality of the guidance law in meeting the control requirements of UAV formation flight for specific flight tasks. Full article
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<p>Formation control framework based on cooperative waypoint-following.</p>
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<p>Schematic for calculating the virtual dynamic tracking point.</p>
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<p>Schematic of guidance by parallel-approach method.</p>
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<p>Relationship between wingman and dynamic tracking point.</p>
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<p>Attitude control modeling of lateral-heading channel.</p>
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<p>Attitude control modeling of pitch channel.</p>
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<p>Control modeling of velocity channel.</p>
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<p>Tracking effect of wingman: (<b>a</b>) time histories of the heading angle; (<b>b</b>) time histories of the velocities.</p>
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<p>Schematic of linear formation for collaborative waypoint management.</p>
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<p>Relationship of coordinated waypoints in straight horizontal formation.</p>
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<p>Relationship of cooperating waypoints in horizontal triangular formation.</p>
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<p>Plan view of relationship among coordination waypoints for stepped formation.</p>
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<p>Side view of relationship among coordination waypoints for stepped formation.</p>
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<p>Schematic of formation transformation process.</p>
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<p>Example of formation change process.</p>
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<p>Data-link survivable network architecture.</p>
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<p>Schematic of formation reconstruction.</p>
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<p>Relationship among all systems in hardware-in-the-loop simulation.</p>
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<p>Device connection diagram for hardware-in-the-loop simulation.</p>
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<p>Hardware-in-the-loop simulation: (<b>a</b>) ground-station perspective; (<b>b</b>) Tacview software perspective.</p>
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<p>Three-dimensional view of hardware-in-the-loop simulation of formation transformation: (<b>a</b>) triangular formation; (<b>b</b>) formation in the middle of changing; (<b>c</b>) stepped formation.</p>
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<p>Changes of positions of wingmen relative to leader in formation change.</p>
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<p>Change in heading angle during formation transformation.</p>
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<p>Electric vertical takeoff and landing aircraft.</p>
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<p>UAV flight platform equipment.</p>
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<p>Connections of ground measurement and control system.</p>
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<p>Connections of formation test equipment.</p>
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<p>Photograph of four-plane coordinated formation before takeoff.</p>
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<p>Flow chart of formation flight test.</p>
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<p>Flight interface of ground-station software.</p>
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<p>Photographs of actual flight of four-machine coordinated formation: (<b>a</b>) ground view of straight formation; (<b>b</b>) aerial view of stepped formation.</p>
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<p>UAV returning after leaving formation.</p>
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<p>Control effect of actual flight-heading channels of four aircraft in cooperative formation.</p>
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<p>Three-dimensional maps of actual flight route of four-plane cooperative formation: (<b>a</b>) trajectory diagram from plotting software; (<b>b</b>) flight trajectory.</p>
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24 pages, 8816 KiB  
Article
Novel Drone Design Using an Optimization Software with 3D Model, Simulation, and Fabrication in Drone Systems Research
by Ahmed. O. MohamedZain, Huangshen Chua, Kianmeng Yap, Pavithren Uthayasurian and Teoh Jiehan
Drones 2022, 6(4), 97; https://doi.org/10.3390/drones6040097 - 14 Apr 2022
Cited by 7 | Viewed by 10011
Abstract
This paper presents the design of a small size Unmanned Aerial Vehicle (UAV) using the 3DEXPERIENCE software. The process of designing the frame parts involves many methods to ensure the parts can meet the requirements while conforming to safety and industry standards. The [...] Read more.
This paper presents the design of a small size Unmanned Aerial Vehicle (UAV) using the 3DEXPERIENCE software. The process of designing the frame parts involves many methods to ensure the parts can meet the requirements while conforming to safety and industry standards. The design steps start with the selection of materials that can be used for the drone, which are polylactic acid (PLA), acrylonitrile styrene acrylate (ASA), and acrylonitrile butadiene styrene (ABS). The drone frame consists of four main parts, which are the center top cover (50 g), the side top cover (10 g), the middle cover (30 g), and the drone’s arm (80 g). A simulation was carried out to determine the stress, displacement, and weight of the drone’s parts. Additionally, a trade-off study was conducted to finalize the shapes of the parts and the various inputs based on their priorities. The outcome of this new design can be represented in design concepts, which involve the use of the snap hook function to assemble two body parts together, namely the middle cover and the center top cover, without the need of an additional fastener. Full article
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<p>Drone hybrid H-design, H-design, and X-design Available for Development [<a href="#B8-drones-06-00097" class="html-bibr">8</a>].</p>
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<p>Original Design of the Drone using 3DEXPERIENCE.</p>
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<p>Drone’s Frame Design. (<b>a</b>) Top View of Drone. (<b>b</b>) Drone’s Arm. (<b>c</b>) Cantilever Snap Fit Design for Side Cover. (<b>d</b>) Cantilever Snap Fit Design for Middle Cover.</p>
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<p>PLA Stress Curve.</p>
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<p>ABS Stress Curve.</p>
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<p>ASA Stress Curve.</p>
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<p>Restraining of the Drone Parts. (<b>a</b>) Center Top Cover. (<b>b</b>) Side Top Cover. (<b>c</b>) Middle Cover. (<b>d</b>) Arm.</p>
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<p>Stress and Displacement of the Drone’s Parts. (<b>a</b>) Centre Top Cover. (<b>b</b>) Side Top Cover. (<b>c</b>) Drone’s Arm. (<b>d</b>) Middle Cover.</p>
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<p>Stress and Displacement of the Drone’s Parts. (<b>a</b>) Centre Top Cover. (<b>b</b>) Side Top Cover. (<b>c</b>) Drone’s Arm. (<b>d</b>) Middle Cover.</p>
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<p>Drone’s Carriage Stress and Displacement. (<b>a</b>) Leg Bereket. (<b>b</b>) Bottom Cover.</p>
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<p>KPI of Centre Top Cover.</p>
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<p>KPI of Side Top Cover.</p>
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<p>KPI of Middle Cover.</p>
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<p>KPI of Arm.</p>
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<p>KPI of Arm.</p>
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<p>KPI of Leg Bracket.</p>
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<p>KPI of Leg Bracket.</p>
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<p>KPI of Bottom Cover.</p>
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<p>Output Weight of the Drone’s Parts. (<b>a</b>) Center Top Cover. (<b>b</b>) Side Top Cover. (<b>c</b>) Middle Cover. (<b>d</b>) Drone’s Arm.</p>
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<p>Output Weight of the Drone’s Parts. (<b>a</b>) Center Top Cover. (<b>b</b>) Side Top Cover. (<b>c</b>) Middle Cover. (<b>d</b>) Drone’s Arm.</p>
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<p>Hardware of the Drone Design.</p>
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27 pages, 10942 KiB  
Article
Autonomous Unmanned Heterogeneous Vehicles for Persistent Monitoring
by Vaios Lappas, Hyo-Sang Shin, Antonios Tsourdos, David Lindgren, Sylvain Bertrand, Julien Marzat, Hélène Piet-Lahanier, Yiannis Daramouskas and Vasilis Kostopoulos
Drones 2022, 6(4), 94; https://doi.org/10.3390/drones6040094 - 10 Apr 2022
Cited by 4 | Viewed by 3415
Abstract
Swarms of unmanned vehicles (air and ground) can increase the efficiency and effectiveness of military and law enforcement operations by enhancing situational awareness and allowing the persistent monitoring of multiple hostile targets. The key focus in the development of the enabling technologies for [...] Read more.
Swarms of unmanned vehicles (air and ground) can increase the efficiency and effectiveness of military and law enforcement operations by enhancing situational awareness and allowing the persistent monitoring of multiple hostile targets. The key focus in the development of the enabling technologies for swarm systems is the minimisation of uncertainties in situational awareness information for surveillance operations supported by ‘system of systems’ composed of static and mobile heterogeneous sensors. The identified critical enabling techniques and technologies for adaptive, informative and reconfigurable operations of unmanned swarm systems are robust static sensor network design, mobile sensor tasking (including re-allocation), sensor fusion and information fusion, including behaviour monitoring. The work presented in this paper describes one of the first attempts to integrate all swarm-related technologies into a prototype, demonstrating the benefits of swarms of heterogeneous vehicles for defence applications used for the persistent monitoring of high-value assets, such as military installations and camps. The key enabling swarm system technologies are analysed here, and novel algorithms are presented that can be implemented in available COTS-based unmanned vehicles. The algorithms have been designed and optimised to require small computational power, be flexible, be reconfigurable and be implemented in a large range of commercially available unmanned vehicles (air and ground). Full article
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<p>An overview of the autonomous swarm framework building blocks.</p>
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<p>Swarm task allocation with multiple UAV agents and targets.</p>
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<p>Surveillance of a high-value military asset, where a swarm of air/ground drones serve multiple purposes, such as acquisition of completing camera angles and establishing relay chains for effective and secure communication (source FOI).</p>
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<p>Simulation scenario for monitoring a high value asset (military base).</p>
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<p>(<b>a</b>) Results for the RD dictionary using the neural network. (<b>b</b>) Results for the RD dictionary using the neural network with 100 bins.</p>
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<p>(<b>a</b>) Assessment for the normal vehicle. (<b>b</b>) Assessment for the abnormal vehicle.</p>
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<p>(<b>a</b>) Assessment for the normal vehicle. (<b>b</b>) Assessment for the abnormal vehicle.</p>
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<p>Breakdown of the target tracking components. Sensors were used with sensor-attached detectors that propagated target detections in terms of coordinates to a local fusion node.</p>
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<p>(<b>a</b>) Screenshot of simulated targets and sensor motions, where the sensor is a UAV-borne camera trained for the (red) person in the centre (<b>b</b>) full view.</p>
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<p>Simulated swarm navigation errors from UAV sensors.</p>
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<p>Simulation of target tracking. The continuous curve (blue) is the true track, and the dashed curve (red) is the EKF estimate. The corresponding tracking RMSE is 1.2 m.</p>
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<p>Simulation as in <a href="#drones-06-00094-f015" class="html-fig">Figure 15</a> but with implementation of the collaborative positioning algorithm. The corresponding tracking is significantly reduced to &lt;0.5 m.</p>
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<p>Tracking RMSE resulting from the Monte Carlo simulation.</p>
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<p>Tracking RMSE using a collaborative positioning algorithm. The corresponding tracking is significantly reduced by up to 50%.</p>
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<p>Definition of virtual trajectory and ball for navigation cost.</p>
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<p>Monitoring mission—nominal scenario.</p>
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<p>Monitoring mission—faulty scenario 1 (faulty sensors in red).</p>
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<p>Monitoring mission—faulty scenario 2 (faulty sensors in red).</p>
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<p>Swarm structure for (<b>a</b>) guidance, navigation and control system; (<b>b</b>) network.</p>
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<p>(<b>a</b>) Mission trajectory for the EuroSWARM outdoor experiment. (<b>b</b>) Time history of target detection probability.</p>
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18 pages, 3571 KiB  
Article
Research on UAV Robust Adaptive Positioning Algorithm Based on IMU/GNSS/VO in Complex Scenes
by Jun Dai, Xiangyang Hao, Songlin Liu and Zongbin Ren
Sensors 2022, 22(8), 2832; https://doi.org/10.3390/s22082832 - 7 Apr 2022
Cited by 12 | Viewed by 2294
Abstract
As an important component of autonomous intelligent systems, the research on autonomous positioning algorithms used by UAVs is of great significance. In order to resolve the problem whereby the GNSS signal is interrupted, and the visual sensor lacks sufficient feature points in complex [...] Read more.
As an important component of autonomous intelligent systems, the research on autonomous positioning algorithms used by UAVs is of great significance. In order to resolve the problem whereby the GNSS signal is interrupted, and the visual sensor lacks sufficient feature points in complex scenes, which leads to difficulties in autonomous positioning, this paper proposes a new robust adaptive positioning algorithm that ensures the robustness and accuracy of autonomous navigation and positioning in UAVs. On the basis of the combined navigation model of vision/inertial navigation and satellite/inertial navigation, based on ESKF, a multi-source fusion model based on a federated Kalman filter is here established. Furthermore, a robust adaptive localization algorithm is proposed, which uses robust equivalent weights to estimate the sub-filters, and then uses the sub-filter state covariance to adaptively assign information sharing coefficients. After simulation experiments and dataset verification, the results show that the robust adaptive algorithm can effectively limit the impact of gross errors in observations and mathematical model deviations and can automatically update the information sharing coefficient online according to the sub-filter equivalent state covariance. Compared with the classical federated Kalman algorithm and the adaptive federated Kalman algorithm, our algorithm can meet the real-time requirements of navigation, and the accuracy of position, velocity, and attitude measurement is improved by 2–3 times. The robust adaptive localization algorithm proposed in this paper can effectively improve the reliability and accuracy of autonomous navigation systems in complex scenes. Moreover, the algorithm is general—it is not intended for a specific scene or a specific sensor combination– and is applicable to individual scenes with varied sensor combinations. Full article
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<p>Federated Kalman filter.</p>
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<p>Robust adaptive multi-source model.</p>
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<p>Comparison of information sharing coefficients of three schemes: (<b>a</b>) Scheme 1; (<b>b</b>) Scheme 2; and (<b>c</b>) Scheme 3.</p>
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<p>Comparison of state estimation of different combined systems. Asterisk indicates the starting position, the dotted line indicates the position of the enlarged area, and the arrow indicates the specific enlarged area (<b>a</b>,<b>b</b>).</p>
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<p>Comparison of trajectories of different schemes. Asterisk indicates the starting position, the dotted line indicates the position of the enlarged area, and the arrow indicates the specific enlarged area (<b>a</b>,<b>b</b>).</p>
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<p>Comparison of attitude errors.</p>
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<p>Speed error comparison chart.</p>
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<p>Comparison of position errors.</p>
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<p>The MAEs of position errors (m) in the 20 experiment groups.</p>
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<p>UAV sensor configuration (different sensors and mounting locations for UAV) and “OutBuilding”.</p>
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<p>Location estimation for different scenarios.</p>
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<p>Information sharing coefficient of different schemes (Scheme 1, Scheme 2, Scheme 3).</p>
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<p>Position estimation for different scenarios.</p>
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<p>Comparison of position, speed, and attitude errors of different schemes.</p>
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19 pages, 11479 KiB  
Article
Investigation of Rotor Efficiency with Varying Rotor Pitch Angle for a Coaxial Drone
by Knut Erik Teigen Giljarhus, Alessandro Porcarelli and Jørgen Apeland
Drones 2022, 6(4), 91; https://doi.org/10.3390/drones6040091 - 4 Apr 2022
Cited by 10 | Viewed by 5405
Abstract
Coaxial rotor systems are appealing for multirotor drones, as they increase thrust without increasing the vehicle’s footprint. However, the thrust of a coaxial rotor system is reduced compared to having the rotors in line. It is of interest to increase the efficiency of [...] Read more.
Coaxial rotor systems are appealing for multirotor drones, as they increase thrust without increasing the vehicle’s footprint. However, the thrust of a coaxial rotor system is reduced compared to having the rotors in line. It is of interest to increase the efficiency of coaxial systems, both to extend mission time and to enable new mission capabilities. While some parameters of a coaxial system have been explored, such as the rotor-to-rotor distance, the influence of rotor pitch is less understood. This work investigates how adjusting the pitch of the lower rotor relative to that of the upper one impacts the overall efficiency of the system. A methodology based on blade element momentum theory is extended to coaxial rotor systems, and in addition blade-resolved simulations using computational fluid dynamics are performed. A coaxial rotor system for a medium-sized drone with a rotor diameter of 71.12 cm is used for the study. Experiments are performed using a thrust stand to validate the methods. The results show that there exists a peak in total rotor efficiency (thrust-to-power ratio), and that the efficiency can be increased by 2% to 5% by increasing the pitch of the lower rotor. The work contributes to furthering our understanding of coaxial rotor systems, and the results can potentially lead to more efficient drones with increased mission time. Full article
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<p>Illustration of parameters and forces for blade element momentum theory. (<b>a</b>) Momentum theory control volume. (<b>b</b>) Blade element.</p>
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<p>Twist angle and chord length of the rotor blade.</p>
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<p>Comparison of A18 airfoil against airfoils along the commercial T-MOTOR G28x9.2” blade at four radial stations. From the bottom: <math display="inline"><semantics> <mrow> <mn>0.3</mn> <mi>R</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mn>0.5</mn> <mi>R</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mn>0.7</mn> <mi>R</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mn>0.9</mn> <mi>R</mi> </mrow> </semantics></math>.</p>
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<p>Top view (<b>top</b>) and front view (<b>bottom</b>) of the computational 3D rotor geometry for a pitch of 9.2”.</p>
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<p>Aerodynamic drag and lift coefficients for the A18 airfoil, calculated using XFOIL at Re = 175,000.</p>
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<p>Illustration of mesh arrangements. (<b>a</b>) Rotor surface mesh. (<b>b</b>) Close-up of mesh near rotor with layers generated using 3D T-Rex extrusion. (<b>c</b>) Mesh around rotors. The yellow rectangles indicate the AMI blocks.</p>
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<p>Non-dimensional wall distance along rotor surface at radius <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>0.7</mn> <mi>R</mi> </mrow> </semantics></math> for RPM = 2200.</p>
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<p>Picture of experimental setup showing the thrust stand in coaxial configuration and a close-up view of the load cell and motor. (<b>a</b>) Thrust stand. (<b>b</b>) Load cell and motor.</p>
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<p>Comparison between experiments, BEMT simulations and CFD simulations for a single rotor. (<b>a</b>) Thrust. (<b>b</b>) Efficiency.</p>
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<p>Magnitude of velocity vector for single-rotor setup at varying RPM. The grey line indicated in (<b>a</b>) shows the position of the second rotor for the coaxial setup. (<b>a</b>) RPM = 1600. (<b>b</b>) RPM = 1900. (<b>c</b>) RPM = 2200. (<b>d</b>) RPM = 2500.</p>
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<p>Vertical velocity at a vertical distance 0.115 m from the rotor (indicated by the grey line in <a href="#drones-06-00091-f010" class="html-fig">Figure 10</a>), estimating inflow velocity for the lower rotor in the coaxial setup. The dashed lines are the values predicted from the coaxial BEMT model.</p>
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<p>Comparison between experiments, BEMT simulations and CFD simulations for the coaxial rotor setup. (<b>a</b>) Thrust. (<b>b</b>) Efficiency.</p>
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<p>Magnitude of velocity vector for coaxial rotor setup at varying RPM. (<b>a</b>) RPM = 1600. (<b>b</b>) RPM = 1900. (<b>c</b>) RPM = 2200. (<b>d</b>) RPM = 2500.</p>
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<p>Total efficiency relative to total efficiency at pitch 9.2″ for the coaxial rotor system as a function of lower rotor pitch.</p>
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<p>Comparison of BETM and CFD for thrust along blade for pitch 14.2″.</p>
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<p>BEMT results along the blade for the lower rotor for three different pitches. (<b>a</b>) Thrust along blade. (<b>b</b>) Aerodynamic efficiency along blade.</p>
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<p>Pressure coefficient and flow pattern (as seen from the rotor) for the lower rotor at radius <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>0.3</mn> <mi>R</mi> </mrow> </semantics></math> for two different pitches. (<b>a</b>) Pitch 9.2″. (<b>b</b>) Pitch 14.2″.</p>
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<p>Pressure coefficient over the lower rotor blade at radius <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>0.3</mn> <mi>R</mi> </mrow> </semantics></math> for two different pitches.</p>
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18 pages, 9293 KiB  
Article
Automatic Air-to-Ground Recognition of Outdoor Injured Human Targets Based on UAV Bimodal Information: The Explore Study
by Fugui Qi, Mingming Zhu, Zhao Li, Tao Lei, Juanjuan Xia, Linyuan Zhang, Yili Yan, Jianqi Wang and Guohua Lu
Appl. Sci. 2022, 12(7), 3457; https://doi.org/10.3390/app12073457 - 29 Mar 2022
Cited by 6 | Viewed by 1947
Abstract
The rapid air-to-ground search of injured people in the outdoor environment has been a hot spot and a great challenge for public safety and emergency rescue medicine. Its crucial difficulties lie in the fact that small-scale human targets possess a low target-background contrast [...] Read more.
The rapid air-to-ground search of injured people in the outdoor environment has been a hot spot and a great challenge for public safety and emergency rescue medicine. Its crucial difficulties lie in the fact that small-scale human targets possess a low target-background contrast to the complex outdoor environment background and the human attribute of the target is hard to verify. Therefore, an automatic recognition method based on UAV bimodal information is proposed in this paper. First, suspected targets were accurately detected and separated from the background based on multispectral feature information only. Immediately after, the bio-radar module would be released and would try to detect their corresponding physiological information for accurate re-identification of the human target property. Both the suspected human target detection experiments and human target property re-identification experiments show that our proposed method could effectively realize accurate identification of ground injured in outdoor environments, which is meaningful for the research of rapid search and rescue of injured people in the outdoor environment. Full article
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<p>The overall architecture of the bimodal information collection system.</p>
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<p>The diagram of the bimodal information collection system.</p>
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<p>Suspected target detection and human nature re-identification based on UAV bio-modal information from multispectral camera and bio-radar.</p>
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<p>The spectral relative reflectivity of green vegetation and green camouflage.</p>
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<p>The flowchart of bimodal-information-based human targets recognition method.</p>
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<p>Flow chart of multispectral imagery preprocessing.</p>
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<p>Two kinds of features for 3 typical subjects. (<b>a</b>) Reflectivity of six bands, (<b>b</b>) Spectral indexes.</p>
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<p>The DT for identification of suspected target.</p>
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<p>Block diagram of ALE.</p>
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<p>Illustration of experimental settings for two scenarios. (<b>a</b>) <span class="html-italic">Scenario 1</span>: 12 sets of green camouflage clothes in a homogeneous grassland background, (<b>b</b>) 11 sets of green camouflage clothes, and one real personnel in green camouflage clothing in a complex background.</p>
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<p>Local multispectral remote sensing images in <span class="html-italic">Scenario 1</span> acquired by MS600 (one exposure): (<b>a</b>) 450 nm; (<b>b</b>) 555 nm; (<b>c</b>) 660 nm; (<b>d</b>) 710 nm; (<b>e</b>) 840 nm; (<b>f</b>) 940 nm.</p>
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<p>The complete reflectance panorama in <span class="html-italic">Scenario 1</span>.</p>
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<p>Suspected target recognition result in <span class="html-italic">Scenario 1</span> (<span class="html-italic">green for vegetation, yellow for soil, red for suspected target, blue for noise spot</span>).</p>
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<p>The complete reflectance panorama in <span class="html-italic">Scenario 2</span>.</p>
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<p>Suspected target recognition result in <span class="html-italic">Scenario 2</span> (<span class="html-italic">green for vegetation, yellow for soil, red for suspected target, blue for noise spot</span>).</p>
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<p>Radar echo of human target T<sub>12</sub> from 8 m and corresponding frequency analysis, (<b>a</b>) original signal and normalized frequency spectrum, (<b>b</b>) noise cancellation signal and normalized frequency spectrum, (<b>c</b>) human target reconfirmation result.</p>
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23 pages, 2610 KiB  
Review
Ice Accretion on Fixed-Wing Unmanned Aerial Vehicle—A Review Study
by Manaf Muhammed and Muhammad Shakeel Virk
Drones 2022, 6(4), 86; https://doi.org/10.3390/drones6040086 - 28 Mar 2022
Cited by 16 | Viewed by 5038
Abstract
Ice accretion on commercial aircraft operating at high Reynolds numbers has been extensively studied in the literature, but a direct transformation of these results to an Unmanned Aerial Vehicle (UAV) operating at low Reynolds numbers is not straightforward. Changes in Reynolds number have [...] Read more.
Ice accretion on commercial aircraft operating at high Reynolds numbers has been extensively studied in the literature, but a direct transformation of these results to an Unmanned Aerial Vehicle (UAV) operating at low Reynolds numbers is not straightforward. Changes in Reynolds number have a significant impact on the ice accretion physics. Previously, only a few researchers worked in this area, but it is now gaining more attention due to the increasing applications of UAVs in the modern world. As a result, an attempt is made to review existing scientific knowledge and identify the knowledge gaps in this field of research. Ice accretion can deteriorate the aerodynamic performance, structural integrity, and aircraft stability, necessitating optimal ice mitigation techniques. This paper provides a comprehensive review of ice accretion on fixed-wing UAVs. It includes various methodologies for studying and comprehending the physics of ice accretion on UAVs. The impact of various environmental and geometric factors on ice accretion physics is reviewed, and knowledge gaps are identified. The pros and cons of various ice detection and mitigation techniques developed for UAVs are also discussed. Full article
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<p>Ice accretion on fixed-wing UAV [<a href="#B13-drones-06-00086" class="html-bibr">13</a>,<a href="#B14-drones-06-00086" class="html-bibr">14</a>].</p>
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<p>Experimental ice shapes on RG-15 airfoil [<a href="#B56-drones-06-00086" class="html-bibr">56</a>].</p>
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<p>Ice shape predicted by (<b>a</b>) experiments and (<b>b</b>) numerical codes on NREL S826 airfoil [<a href="#B57-drones-06-00086" class="html-bibr">57</a>]. These simulated ice shapes are marked with an asterisk to distinguish them from the experimental shapes.</p>
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<p>Index visualization for the aerodynamic performance of RG-15 airfoil [<a href="#B68-drones-06-00086" class="html-bibr">68</a>].</p>
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<p>Formation of Laminar Separation Bubble (LSB) and Induced Separation Bubble (ISB): (<b>a</b>) 0° clean, (<b>b</b>) 0° iced, (<b>c</b>) 6° clean, (<b>d</b>) 6° iced [<a href="#B81-drones-06-00086" class="html-bibr">81</a>].</p>
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<p>Conventional (<b>a</b>) and Parting Strip (<b>b</b>) de-icing methods [<a href="#B120-drones-06-00086" class="html-bibr">120</a>].</p>
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36 pages, 2000 KiB  
Review
A Review of Counter-UAS Technologies for Cooperative Defensive Teams of Drones
by Vittorio Ugo Castrillo, Angelo Manco, Domenico Pascarella and Gabriella Gigante
Drones 2022, 6(3), 65; https://doi.org/10.3390/drones6030065 - 1 Mar 2022
Cited by 38 | Viewed by 14547
Abstract
In recent years, the drone market has had a significant expansion, with applications in various fields (surveillance, rescue operations, intelligent logistics, environmental monitoring, precision agriculture, inspection and measuring in the construction industry). Given their increasing use, the issues related to safety, security and [...] Read more.
In recent years, the drone market has had a significant expansion, with applications in various fields (surveillance, rescue operations, intelligent logistics, environmental monitoring, precision agriculture, inspection and measuring in the construction industry). Given their increasing use, the issues related to safety, security and privacy must be taken into consideration. Accordingly, the development of new concepts for countermeasures systems, able to identify and neutralize a single (or multiples) malicious drone(s) (i.e., classified as a threat), has become of primary importance. For this purpose, the paper evaluates the concept of a multiplatform counter-UAS system (CUS), based mainly on a team of mini drones acting as a cooperative defensive system. In order to provide the basis for implementing such a system, we present a review of the available technologies for sensing, mitigation and command and control systems that generally comprise a CUS, focusing on their applicability and suitability in the case of mini drones. Full article
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<p>NATO’s UAS classification system [<a href="#B4-drones-06-00065" class="html-bibr">4</a>].</p>
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<p>SWADAR concept for assessing swarming metrics (<b>a</b>) and for multi-UAV cooperative tracking (<b>b</b>) [<a href="#B27-drones-06-00065" class="html-bibr">27</a>]. The left part shows some examples of useful metrics to measure the swarm behavior of intruder drones. Some of these metrics are: the cohesion, the segregation, the presence of hierarchical structures and clusters and the f-divergence (i.e., the temporal variation of the spatial distributions of the swarm).</p>
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<p>Functional architecture of the planning logic for the C2 system. Such logic is divided into team logic and vehicle logic. The former contributes to the planning of the actions of the overall team. Starting from the team plan, the latter performs the planning and the execution for the single vehicle.</p>
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14 pages, 393 KiB  
Article
Robust Resource Allocation and Trajectory Planning of UAV-Aided Mobile Edge Computing in Post-Disaster Areas
by Peng Cao, Yi Liu and Chao Yang
Appl. Sci. 2022, 12(4), 2226; https://doi.org/10.3390/app12042226 - 21 Feb 2022
Cited by 1 | Viewed by 1804
Abstract
When natural disasters strike, users in the disaster area may be isolated and unable to transmit disaster information to the outside due to the damage of communication facilities. Unmanned aerial vehicles can be exploited as mobile edge servers to provide emergency service for [...] Read more.
When natural disasters strike, users in the disaster area may be isolated and unable to transmit disaster information to the outside due to the damage of communication facilities. Unmanned aerial vehicles can be exploited as mobile edge servers to provide emergency service for ground users due to its mobility and flexibility. In this paper, a robust UAV-aided wireless-powered mobile edge computing (MEC) system in post disaster areas is proposed, where the UAV provides charging and computing service for users in the disaster area. Considering the estimation error of users’ locations, our target is to maximize the energy acquisition of each user by jointly optimizing the computing offloading process and the UAV trajectory. Due to the strongly coupled connectionbetween optimization variables and the non-convex nature for trajectory optimization, the problem is difficult to solve. Furthermore, the semi-infinity of the users’ possible location makes the problem even more intractable. To tackle these difficulties, we ignore the estimation error of users’ location firstly, and propose an iterative algorithm by using Lagrange dual method and successive convex approximation (SCA) technology. Then, we propose a cutting-set method to deal with the uncertainty of users’ location. In this method, we degrade the influence of location uncertainty by alternating between optimization step and pessimization step. Finally, simulation results show that the proposed robust algorithm can effectively improve the user energy acquisition. Full article
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<p>The UAV-enabled wireless-powered MEC system in post-disaster area.</p>
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<p>The optimized UAV trajectories under different schemes and battery capacity.</p>
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<p>Energy gain of users under different schemes and battery capacity of UAV.</p>
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<p>Energy gain of users under different schemes and estimation errors of users.</p>
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<p>Energy gain of users under different schemes and flight altitude of UAV.</p>
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<p>Energy gain of users under different schemes and WPT transmit power of UAV.</p>
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18 pages, 6187 KiB  
Article
Application of Filters to Improve Flight Stability of Rotary Unmanned Aerial Objects
by Maciej Salwa and Izabela Krzysztofik
Sensors 2022, 22(4), 1677; https://doi.org/10.3390/s22041677 - 21 Feb 2022
Cited by 1 | Viewed by 3091
Abstract
The most common filters used to determine the angular position of quadrotors are the Kalman filter and the complementary filter. The problem of angular position estimation consist is a result of the absence of direct data. The most common sensors on board UAVs [...] Read more.
The most common filters used to determine the angular position of quadrotors are the Kalman filter and the complementary filter. The problem of angular position estimation consist is a result of the absence of direct data. The most common sensors on board UAVs are micro electro mechanical system (MEMS) type sensors. The data acquired from the sensors are processed using digital filters. In the literature, the results of research conducted on the effectiveness of Kalman and complementary filters are known. A significant problem in evaluating the performance of the studied filters was the lack of an arbitrarily determined UAV position. The authors of this paper undertook the task of determining the best filter for a real object. The main objective of this research was to improve the stability of the physical quadrotor. For this purpose, we developed a research method using a laboratory station for testing quadrotor drones. Moreover, using the MATLAB environment, they determined the optimal parameters for the real filter applied using the PX4 software, which is new and has not been considered before in the available scientific literature. It should be mentioned that the authors of this work focused on the analysis of filters most commonly used for flight stabilization, without modifying the structure of these filters. By not modifying the filter structure, it is possible to optimize the existing flight controllers. The main contribution of this study lies in finding the most optimal filter, among those available in flight controllers, for angular position estimation. The special emphasis of our work was to develop a procedure for selecting the filter coefficients for a real object. The algorithm was designed so that other researchers could use it, provided they collected arbitrary data for their objects. Selected results of the research are presented in graphical form. The proposed procedure for improving the embedded filter can be used by other researchers on their subjects. Full article
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<p>Test-bench for drones.</p>
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<p>The position of the test-bench sensors in relation to the axis of the drone system.</p>
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<p>Block diagram of the filter optimization algorithm for a real flight controller.</p>
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<p>Drone mounted on the test-bench.</p>
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<p>Summation of individual component signals.</p>
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<p>Processing of the IMU sensor data by the complementary filter.</p>
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<p>Cut-off frequency for complementary filter.</p>
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<p>Two steps Kalman filter algorithm.</p>
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<p><span class="html-italic">x</span>-axis rotation readings from accelerometer and gyroscope.</p>
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<p><span class="html-italic">y</span>-axis rotation readings from accelerometer and gyroscope.</p>
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<p>Position estimation using the complementary filter.</p>
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<p>Position estimation using the EKF.</p>
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<p>Comparison of the angular position obtained from the filters with the physical position for the <span class="html-italic">x</span>-axis.</p>
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<p>Comparison of the angular position obtained from the filters with the physical position for the <span class="html-italic">y</span>-axis.</p>
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<p>Comparison of angular position for <span class="html-italic">x</span>-axis.</p>
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<p>Comparison of angular position for <span class="html-italic">y</span>-axis.</p>
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