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Search Results (26,160)

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22 pages, 1515 KiB  
Article
Envisioning the Future of Mobility: A Well-Being-Oriented Approach
by Yousif Elsamani and Yuya Kajikawa
Sustainability 2024, 16(18), 8114; https://doi.org/10.3390/su16188114 (registering DOI) - 17 Sep 2024
Abstract
Mobility, a vital part of daily life, significantly impacts human well-being. Understanding this relationship is crucial for shaping the future trajectory of mobility, a connection often overlooked in previous research. This study explores the complex relationship between mobility and well-being and proposes a [...] Read more.
Mobility, a vital part of daily life, significantly impacts human well-being. Understanding this relationship is crucial for shaping the future trajectory of mobility, a connection often overlooked in previous research. This study explores the complex relationship between mobility and well-being and proposes a holistic framework for mobility’s future, prioritizing individual and societal well-being. The motivation for this research stems from the growing need to balance technological advancements in transportation with the well-being of diverse populations, especially as the mobility landscape evolves with innovations like autonomous vehicles and intelligent mobility solutions. We employ bibliometric methods, analyzing 53,588 academic articles to identify key themes and research trends related to mobility and well-being. This study categorizes these articles into thematic clusters using the Louvain modularity maximization algorithm, which facilitates the formation of cohesive groups based on citation patterns. Our findings underline the significant impact of mobility on physical, mental, psychological, financial, and social well-being. The proposed framework features four pillars: vehicle, infrastructure and environment, mobility stakeholders, and policy. This framework underscores the importance of collaboration between institutional and individual actions in shaping a future mobility landscape that is technologically advanced, socially responsible, and conducive to an improved quality of life. Full article
(This article belongs to the Section Sustainable Transportation)
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Figure 1

Figure 1
<p>Research clusters using direct citation network analysis showing the top 6 (in size) clusters.</p>
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<p>Heatmap of the cosine similarity analysis between the top 30 clusters.</p>
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<p>Clusters related to each stage of the vehicle life cycle.</p>
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<p>Well-being-centric mobility vision featuring four main pillars: vehicle, mobility stakeholders, infrastructure and environment, and policy.</p>
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14 pages, 13110 KiB  
Article
Auxeticity Tuning by Nanolayer Inclusion Ordering in Hard Sphere Crystals
by Jakub W. Narojczyk, Krzysztof W. Wojciechowski, Jerzy Smardzewski and Konstantin V. Tretiakov
Materials 2024, 17(18), 4564; https://doi.org/10.3390/ma17184564 (registering DOI) - 17 Sep 2024
Abstract
Designing a particular change in a system structure to achieve the desired elastic properties of materials for a given task is challenging. Recent studies of purely geometrical atomic models have shown that structural modifications on a molecular level can lead to interesting and [...] Read more.
Designing a particular change in a system structure to achieve the desired elastic properties of materials for a given task is challenging. Recent studies of purely geometrical atomic models have shown that structural modifications on a molecular level can lead to interesting and desirable elastic properties. Still, the result of such changes is usually difficult to predict. The present work concerns the impact of nanolayer inclusion ordering in hard sphere crystals on their elastic properties, with special attention devoted to their auxetic properties. Two sets of representative models, based on cubic crystals consisting of 6×6×6 unit cells of hard spheres and containing either neighboring or separated layers of spheres of another diameter, oriented orthogonally to the [001] direction, have been studied by Monte Carlo simulations in the isothermal–isobaric (NpT) ensemble. Their elastic constants have been evaluated using the Parinello–Rahman approach. The Monte Carlo simulations showed that introducing the layer inclusions into a pure face-centered cubic (FCC) structure leads to the system’s symmetry changes from cubic symmetry to tetragonal in both cases. Essential changes in the elastic properties of the systems due to layer ordering were found both for neighboring and separated inclusions. It has been found that the choice of a set of layer inclusions allows one to tune the auxetic properties in two crystallographic directions ([110][11¯0] and [101][1¯01]). In particular, this study revealed that the change in layer ordering (from six separated layers to six neighboring ones) allows for, respectively: (i) enhancing auxeticity of the system in the [101][1¯01] direction with almost loss of auxetic properties in the [110][11¯0] direction in the case of six separated layers, while (ii) in the case of six neighboring layers, keeping the auxetic properties in both auxetic directions independently of the size of spheres constituting inclusions. Full article
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Graphical abstract

Graphical abstract
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<p>The geometry of studied systems containing from one to six nanoinclusion layers in various configurations. The top in the figure represents the systems with neighboring layer inclusions. The middle part of the figure represents the systems with separated layer inclusions. The red spheres represent the inclusion ones, whereas the green spheres represent the ‘matrix’ ones. At the bottom of the figure, four selected systems in the periodic boundary conditions are presented, where supercell (bright colors) and periodic images of the supercell (pale colors) are shown. Some of the periodic images, in the line of sight, have been removed to facilitate the presentation.</p>
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<p>The comparison of diagonal periodic box matrix elements <math display="inline"><semantics> <msub> <mi>h</mi> <mrow> <mi>i</mi> <mi>i</mi> </mrow> </msub> </semantics></math> for systems with the same number of neighboring (NL) and separated (SL) nanolayers. The data are plotted against <math display="inline"><semantics> <mrow> <msup> <mi>σ</mi> <mo>′</mo> </msup> <mo>/</mo> <mi>σ</mi> </mrow> </semantics></math>, which is the ratio of diameters of the inclusion and the matrix spheres. The orange symbols, representing NLs, are slightly larger than the blue symbols, which represent SLs.</p>
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<p>The elastic constants (<math display="inline"><semantics> <msubsup> <mi>B</mi> <mrow> <mi>i</mi> <mi>j</mi> </mrow> <mo>∗</mo> </msubsup> </semantics></math>) of systems with neighboring nanolayers (NLs) as a function of <math display="inline"><semantics> <mrow> <msup> <mi>σ</mi> <mo>′</mo> </msup> <mo>/</mo> <mi>σ</mi> </mrow> </semantics></math>: (<b>a</b>) <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>11</mn> <mo>∗</mo> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>33</mn> <mo>∗</mo> </msubsup> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>12</mn> <mo>∗</mo> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>13</mn> <mo>∗</mo> </msubsup> </semantics></math>, (<b>c</b>) <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>44</mn> <mo>∗</mo> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>66</mn> <mo>∗</mo> </msubsup> </semantics></math>.</p>
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<p>The elastic constants (<math display="inline"><semantics> <msubsup> <mi>B</mi> <mrow> <mi>i</mi> <mi>j</mi> </mrow> <mo>∗</mo> </msubsup> </semantics></math>) of systems with separated nanolayers (SLs) as a function of <math display="inline"><semantics> <mrow> <msup> <mi>σ</mi> <mo>′</mo> </msup> <mo>/</mo> <mi>σ</mi> </mrow> </semantics></math>: (<b>a</b>) <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>11</mn> <mo>∗</mo> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>33</mn> <mo>∗</mo> </msubsup> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>12</mn> <mo>∗</mo> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>13</mn> <mo>∗</mo> </msubsup> </semantics></math>, (<b>c</b>) <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>44</mn> <mo>∗</mo> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>B</mi> <mn>66</mn> <mo>∗</mo> </msubsup> </semantics></math>.</p>
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<p>Poisson’s ratio in the main crystallographic directions as a function of <math display="inline"><semantics> <mrow> <msup> <mi>σ</mi> <mo>′</mo> </msup> <mo>/</mo> <mi>σ</mi> </mrow> </semantics></math> for neighboring nanolayer systems.</p>
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<p>Poisson’s ratio in the main crystallographic directions as a function of <math display="inline"><semantics> <mrow> <msup> <mi>σ</mi> <mo>′</mo> </msup> <mo>/</mo> <mi>σ</mi> </mrow> </semantics></math> for separated nanolayer systems.</p>
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<p>The comparison of Poisson’s ratio in auxetic directions <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">[</mo> <mn>110</mn> <mo stretchy="false">]</mo> </mrow> <mrow> <mo stretchy="false">[</mo> <mn>1</mn> <mover accent="true"> <mn>1</mn> <mo>¯</mo> </mover> <mn>0</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">[</mo> <mn>101</mn> <mo stretchy="false">]</mo> </mrow> <mrow> <mo stretchy="false">[</mo> <mover accent="true"> <mn>1</mn> <mo>¯</mo> </mover> <mn>01</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </semantics></math> (the results corresponding to <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">[</mo> <mn>011</mn> <mo stretchy="false">]</mo> </mrow> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mover accent="true"> <mn>1</mn> <mo>¯</mo> </mover> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </semantics></math> are the same as for <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">[</mo> <mn>101</mn> <mo stretchy="false">]</mo> </mrow> <mrow> <mo stretchy="false">[</mo> <mover accent="true"> <mn>1</mn> <mo>¯</mo> </mover> <mn>01</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </semantics></math>) for six nanolayer systems (NL6 vs. SL6). The inserts in the figures present the absolute value of minimal negative Poisson’s ratio in all crystallographic directions plotted in spherical coordinates for both systems at <math display="inline"><semantics> <mrow> <msup> <mi>σ</mi> <mo>′</mo> </msup> <mo>/</mo> <mi>σ</mi> <mo>=</mo> <mn>1.06</mn> </mrow> </semantics></math>. The solid line in the inserts shows the considered crystallographic direction.</p>
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20 pages, 2250 KiB  
Article
Optical Investigation of Sparks to Improve Ignition Simulation Models in Spark-Ignition Engines
by Saraschandran Kottakalam, Ahmad Anas Alkezbari, Gregor Rottenkolber and Christian Trapp
Energies 2024, 17(18), 4640; https://doi.org/10.3390/en17184640 (registering DOI) - 17 Sep 2024
Abstract
The use of renewable fuels in place of fossil fuels in internal combustion engines is regarded as a viable method for achieving zero-impact-emission powertrains. However, to achieve the best performance with these fuels, these engines require further optimization, which is achieved through new [...] Read more.
The use of renewable fuels in place of fossil fuels in internal combustion engines is regarded as a viable method for achieving zero-impact-emission powertrains. However, to achieve the best performance with these fuels, these engines require further optimization, which is achieved through new combustion strategies and the use of advanced ignition systems such as prechambers. Since simulations greatly accelerate this development, accurate simulation models are needed to accurately predict the combustion phenomenon, which requires a deep understanding of the ignition phenomenon as it significantly affects combustion. This work presents a comprehensive experimental methodology to study sparks under engine conditions, providing quantitative data to improve and validate ignition simulation models. The goal was to determine the volume generated by sparks under engine conditions that can initiate combustion and use this information to improve simulation results to match the experimental results. The visible sparks were observed with high-speed cameras to understand their time-resolved evolution and interaction with the flow. The heat transfer from the plasma was also visualized using a modified Background-Oriented Schlieren technique. The information gained from the experimental observations was used to improve an ignition simulation model. Since the velocity of the plasma was found to be slower than the surrounding flow, a user-defined parameter was included to calibrate the velocity of the simulated plasma particles. This parameter was calibrated to match the simulated spark length to the experimental spark length. In addition, since the previous simulation model did not take the heat transfer from the plasma into account, the simulated plasma particles were coupled to have heat transfer to the surroundings. Based on a comparison of the simulation results with the experimental results, the improved approach was found to provide a better physical representation of the spark ignition phenomenon. Full article
(This article belongs to the Section I: Energy Fundamentals and Conversion)
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Figure 1

Figure 1
<p>The spark windtunnel testbed: (<b>a</b>) Top view (schematic). (<b>b</b>) View from the camera.</p>
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<p>The processing steps used by the Matlab algorithm.</p>
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<p>The experimental setup for FPBOS.</p>
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<p>Heat transfer visualization with FPBOS and post-processing. (<b>a</b>) Displacement vector magnitude with an applied false color map. (<b>b</b>) Normalized grayscale image of the Integrated displacement vectors. (<b>c</b>) Projected density gradient detected by the algorithm shown in pink (conditions: 6 bar, 15 m/s, 0.06 ms after breakdown).</p>
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<p>Illustration of two consecutive time steps showing the spark precursor and the subsequent development of an initial flame kernel (red sphere).</p>
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<p>A cross-sectional view of the CFD mesh, with the central and mass electrodes clearly visible.</p>
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<p>Spark parameter detection by the algorithm for a single spark event. The image series shows the following phenomena: (<b>a</b>) spark elongation, (<b>b</b>) shortcut, and (<b>c</b>) restrike (test conditions: 6 bar pressure and 15 m/s flow velocity).</p>
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<p>Spark length and first restrike detected by the algorithm for a single spark event (test conditions: 6 bar pressure and 15 m/s flow velocity).</p>
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<p>Mean spark length (100 spark events) obtained using the Matlab algorithm with the mean and standard deviation of the time of the occurrence of the first restrike (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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<p>Simulated spark length (CADIM) compared to the experimental data (averaged over 100 cycles) till the first restrike (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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<p>Spark tip velocity from the simulated and experimental (averaged over 100 events) results (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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<p>Velocity flow field in a cross-section along the middle of the electrodes (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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<p>The simulated spark length compared to the averaged experimental data (100 events) till the first restrike location (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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<p>Simulated spark tip velocity compared to the average experimental data (100 events) (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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<p>Spark shape comparison of the simulated (VM = 0.675) and average experimental (bottom row) results (100 events) (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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<p>Simulated spark length compared to the average experimental data (100 events) till the first restrike location (test conditions: absolute pressure = 11 bar, flow velocity = 15 m/s).</p>
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<p>Simulated spark length compared to the averaged experimental data (100 events) till the first restrike (test conditions: absolute pressure = 6 bar, flow velocity = 10 m/s).</p>
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<p>Heat transfer from the spark: comparison of average experimental results (10 events) and the 300 K iso-volume projections obtained from the CADIM-VM-TWP simulation (test conditions: absolute pressure = 6 bar, flow velocity = 15 m/s).</p>
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13 pages, 4512 KiB  
Article
Development of a Robotic Platform with Autonomous Navigation System for Agriculture
by Jamil de Almeida Baltazar, André Luiz de Freitas Coelho, Domingos Sárvio Magalhães Valente, Daniel Marçal de Queiroz and Flora Maria de Melo Villar
AgriEngineering 2024, 6(3), 3362-3374; https://doi.org/10.3390/agriengineering6030192 (registering DOI) - 17 Sep 2024
Abstract
The development of autonomous agricultural robots using a global navigation satellite system aided by real-time kinematics and an inertial measurement unit for position and orientation determination must address the accuracy, reliability, and cost of these components. This study aims to develop and evaluate [...] Read more.
The development of autonomous agricultural robots using a global navigation satellite system aided by real-time kinematics and an inertial measurement unit for position and orientation determination must address the accuracy, reliability, and cost of these components. This study aims to develop and evaluate a robotic platform with autonomous navigation using low-cost components. A navigation algorithm was developed based on the kinematics of a differential vehicle, combined with a proportional and integral steering controller that followed a point-to-point route until the desired route was completed. Two route mapping methods were tested. The performance of the platform control algorithm was evaluated by following a predefined route and calculating metrics such as the maximum cross-track error, mean absolute error, standard deviation of the error, and root mean squared error. The strategy of planning routes with closer waypoints reduces cross-track errors. The results showed that when adopting waypoints every 3 m, better performance was obtained compared to waypoints only at the vertices, with maximum cross-track error being 44.4% lower, MAE 64.1% lower, SD 39.4% lower, and RMSE 52.5% lower. This study demonstrates the feasibility of developing autonomous agricultural robots with low-cost components and highlights the importance of careful route planning to optimize navigation accuracy. Full article
(This article belongs to the Section Agricultural Mechanization and Machinery)
16 pages, 1092 KiB  
Review
Myotube Guidance: Shaping up the Musculoskeletal System
by Aaron N. Johnson
J. Dev. Biol. 2024, 12(3), 25; https://doi.org/10.3390/jdb12030025 (registering DOI) - 17 Sep 2024
Abstract
Myofibers are highly specialized contractile cells of skeletal muscles, and dysregulation of myofiber morphogenesis is emerging as a contributing cause of myopathies and structural birth defects. Myotubes are the myofiber precursors and undergo a dramatic morphological transition into long bipolar myofibers that are [...] Read more.
Myofibers are highly specialized contractile cells of skeletal muscles, and dysregulation of myofiber morphogenesis is emerging as a contributing cause of myopathies and structural birth defects. Myotubes are the myofiber precursors and undergo a dramatic morphological transition into long bipolar myofibers that are attached to tendons on two ends. Similar to axon growth cones, myotube leading edges navigate toward target cells and form cell–cell connections. The process of myotube guidance connects myotubes with the correct tendons, orients myofiber morphology with the overall body plan, and generates a functional musculoskeletal system. Navigational signaling, addition of mass and volume, and identification of target cells are common events in myotube guidance and axon guidance, but surprisingly, the mechanisms regulating these events are not completely overlapping in myotubes and axons. This review summarizes the strategies that have evolved to direct myotube leading edges to predetermined tendon cells and highlights key differences between myotube guidance and axon guidance. The association of myotube guidance pathways with developmental disorders is also discussed. Full article
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Figure 1
<p>Myotube guidance ensures muscles are targeted to the correct tendon. (<b>A</b>) Confocal micrograph of a <span class="html-italic">Drosophila</span> embryo near the end of embryogenesis (Stage 16) labeled for Tropomyosin (myotubes, violet) and Talin (tendon cells, green). Notice the musculoskeletal pattern is precisely repeated in each hemisegment along the anterior–posterior axis. (<b>B</b>) Live Stage 16 embryo that expressed nuclear RFP and membrane-bound GFP in all tendon cells and in a subset of myotubes. Eight tendon cells (T1-T8) and one LO1 myotube were labeled (dotted white line) in two adjacent hemisegments. The LO1 myotube attached to tendon T4 in both segments despite close proximity to seven other tendon cells. Diagram shows the 30 myotubes per embryonic segment. The LO1 myotube (Longitudinal Oblique 1) is shown in green.</p>
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<p>Myotube guidance. (<b>A</b>) Live imaging of an LO1 myotube that expressed cytoplasmic GFP and nuclear RFP. Arrows highlight the dorsal myotube leading edge. At 60 min the dorsal myotube leading edge reached a choice point and navigated to a muscle attachment site on the anterior of the segment. A single myonucleus followed the leading edge throughout elongation (bottom row). Notice that myoblast fusion incorporates a second nucleus at 150 min. (<b>B</b>) Confocal images of Stage 16 embryos expressing the identity gene reporter <span class="html-italic">slouch:GFP</span> labeled for cytoplasmic GFP (green) and Tropomyosin (violet). The pattern of <span class="html-italic">slouch:GFP</span> myotubes was disrupted in <span class="html-italic">salm</span> mutant embryos. LO1 muscles often attached to the incorrect tendons.</p>
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<p>Nervous system defects in myotube guidance mutants. Confocal images of Stage 16 embryos labeled for the peripheral nervous system (PNS) protein Futsch. In wild-type embryos, multiple axons extend along a single track. Individual axons deviate from the common track (arrowheads) in <span class="html-italic">bsd</span> and <span class="html-italic">tum</span> embryos.</p>
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22 pages, 4560 KiB  
Article
Integrating System Perspectives to Optimize Ecosystem Service Provision in Urban Ecological Development
by Wenbo Cai and Chengji Shu
Systems 2024, 12(9), 375; https://doi.org/10.3390/systems12090375 (registering DOI) - 17 Sep 2024
Viewed by 54
Abstract
System-based approaches are critical for addressing the complex and interconnected nature of urban ecological development and restoration of ecosystem services. This study adopts a system perspective to investigate the spatiotemporal drivers of key ecosystem services, including carbon sequestration, water conservation, sediment reduction, pollution [...] Read more.
System-based approaches are critical for addressing the complex and interconnected nature of urban ecological development and restoration of ecosystem services. This study adopts a system perspective to investigate the spatiotemporal drivers of key ecosystem services, including carbon sequestration, water conservation, sediment reduction, pollution mitigation, and stormwater regulation, within the Yangtze River Delta Eco-Green Integrated Development Demonstration Area (YRDDA) from 2000 to 2020. We propose a novel framework for defining enhanced-efficiency ecosystem service management regions (EESMR) to guide targeted restoration. Our analysis revealed the complex interplay of 11, 9, 6, 6, and 10 driving factors for selected ecosystem services, highlighting the spatiotemporal heterogeneity of these drivers. By overlaying these key factors, we identified high-efficiency restoration priority areas for EESMR that ensure high returns on investment and the efficient restoration of ecosystem functions. This system-oriented approach provided critical spatial guidance for integrated ecological restoration, green development, and eco-planning. These findings offer valuable insights for policymakers and planners in the Yangtze River Delta and other rapidly urbanizing regions, supporting the formulation of effective land-use policies that balance environmental sustainability and urban growth. Full article
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<p>Location of the Yangtze River Delta Eco-Green Integration Demonstration Area.</p>
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<p>System-based conceptual framework of the Enhanced-Efficiency Ecosystem Service Management Region (EESMR).</p>
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<p>Single-factor detection q-values (* <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001). CDS represents carbon sequestration, RS represents reduction of sedimentation, RNSP represents reduction of non-point source pollution, SRR represents stormwater runoff regulation, and WC represents water conservation.</p>
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<p>Interaction detection results for ecosystem service drivers.</p>
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<p>Interaction detection results for ecosystem service drivers. Enhanced-Efficiency Ecosystem Service Management Region targeting ecosystem service enhancement. WC represents water conservation, SRR represents stormwater runoff regulation, CDS represents carbon sequestration, RS represents reduction of sedimentation, and RNSP represents reduction of non-point source pollution.</p>
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16 pages, 7153 KiB  
Article
Error Analysis of Non-Time-Synchronized Lightning Positioning Method
by Yanhui Wang, Lijie Yao, Yingchang Min, Yali Liu and Guo Zhao
Remote Sens. 2024, 16(18), 3443; https://doi.org/10.3390/rs16183443 (registering DOI) - 17 Sep 2024
Viewed by 121
Abstract
Since the non-time-synchronized lightning positioning method does not rely on the time synchronization of the stations in the positioning system, it eliminates the errors arising from the pursuit of time synchronization and potentially achieves higher positioning accuracy. This paper provides a comprehensive overview [...] Read more.
Since the non-time-synchronized lightning positioning method does not rely on the time synchronization of the stations in the positioning system, it eliminates the errors arising from the pursuit of time synchronization and potentially achieves higher positioning accuracy. This paper provides a comprehensive overview of the errors present in the three-dimensional lightning positioning system. It compares the results of traditional positioning methods with those of non-time-synchronized lightning positioning algorithms. Subsequently, a simulation analysis of the positioning errors is conducted specifically for the non-time-synchronized lightning positioning method. The results show that (1) the non-time-synchronized lightning positioning method exhibits greater errors when utilizing two randomly positioned radiation sources for location determination. Consequently, the resulting positioning outcomes only provide a general overview of the lightning discharge. (2) The positioning outcomes resemble those of the traditional method when employing a fixed-coordinate beacon point. However, the errors in the three-dimensional positional coordinates of these fixed-coordinate beacon points significantly impact the deviations in the positioning results. This impact is positively correlated with the positional error of the beacon point, considering both the orientation and magnitude. (3) Similarly to the traditional method, the farther away from the center of the positioning network, the larger the radial error. (4) The spatial position of the selected fixed-coordinate beacon point has little influence on the error. Full article
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<p>Schematic diagram of the non-time-synchronized lightning method of positioning.</p>
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<p>Schematic diagram of lightning signal extraction error.</p>
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<p>Comparison of positioning results between non-time-synchronized positioning method and time-difference arrival method. (TOA denotes “time difference of arrival”; DOPI denotes “difference of pulse interval”).</p>
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<p>Results of joint beacon point positioning based on non-time-synchronized method (beacon point: 192,685 m, −343,961 m, 4473 m).</p>
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<p>Plot of positioning results based on iterative computation of beacon point (beacon point: 191,864 m, −344,037 m, 4495 m).</p>
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<p>Schematic of simulated errors in non-fixed-coordinate beacon point.</p>
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<p>Schematic of simulated errors in non-time-synchronized lightning positioning with fixed-coordinate beacon point.</p>
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<p>Schematic diagram of radial error.</p>
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<p>Radial error for beacon point (−20 km, −49 km, 6 km), for (30 k, 20 k) direction.</p>
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<p>Horizontal positioning errors in a 100 km × 100 km square area with a height of 6 km, where vector errors are added to the black beacon point. The scenarios are as follows: (<b>a</b>) the beacon point is shifted by 1 km to the due east direction, (<b>b</b>) the beacon point is shifted by 1 km to the due south direction, (<b>c</b>) the beacon point is shifted by 1 km to the due west direction, and (<b>d</b>) the beacon point is shifted by 1 km to the due north direction.</p>
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<p>Horizontal positioning errors in a 100 km × 100 km square area with a height of 6 km, where vector errors are added to the black beacon point. The scenarios are as follows: (<b>a</b>) the beacon point is shifted by 3 km in the due east direction, (<b>b</b>) the beacon point is shifted by 3 km in the due south direction, (<b>c</b>) the beacon point is shifted by 3 km in the due west direction, and (<b>d</b>) the beacon point is shifted by 3 km in the due north direction.</p>
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<p>Horizontal positioning error (100 km × 100 km square area with 6 km height), transforming the quadrant where the beacon point is located: (<b>a</b>) the beacon point is located in the first quadrant with coordinates (30 km, 30 km, 6 km), (<b>b</b>) the beacon point is located in the second quadrant with coordinates (−30 km, 30 km, 6 km), (<b>c</b>) the beacon point is located in the third quadrant with coordinates (−30 km, −30 km, 6 km), (<b>d</b>) the beacon point is located in the fourth quadrant with coordinates (30 km, −30 km, 6 km).</p>
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17 pages, 6501 KiB  
Article
Enhancing Mechanical Properties of Graphene/Aluminum Nanocomposites via Microstructure Design Using Molecular Dynamics Simulations
by Zhonglei Ma, Hongding Wang, Yanlong Zhao, Zhengning Li, Hong Liu, Yizhao Yang and Zigeng Zhao
Materials 2024, 17(18), 4552; https://doi.org/10.3390/ma17184552 - 16 Sep 2024
Viewed by 264
Abstract
This study explores the mechanical properties of graphene/aluminum (Gr/Al) nanocomposites through nanoindentation testing performed via molecular dynamics simulations in a large-scale atomic/molecular massively parallel simulator (LAMMPS). The simulation model was initially subjected to energy minimization at 300 K, followed by relaxation for 50 [...] Read more.
This study explores the mechanical properties of graphene/aluminum (Gr/Al) nanocomposites through nanoindentation testing performed via molecular dynamics simulations in a large-scale atomic/molecular massively parallel simulator (LAMMPS). The simulation model was initially subjected to energy minimization at 300 K, followed by relaxation for 50 ps under the NPT ensemble, wherein the number of atoms (N), simulation temperature (T), and pressure (P) were conserved. After the model was fully relaxed, loading and unloading simulations were performed. This study focused on the effects of the Gr arrangement with a brick-and-mortar structure and incorporation of high-entropy alloy (HEA) coatings on mechanical properties. The findings revealed that Gr sheets (GSs) significantly impeded dislocation propagation, preventing the dislocation network from penetrating the Gr layer within the plastic zone. However, interactions between dislocations and GSs in the Gr/Al nanocomposites resulted in reduced hardness compared with that of pure aluminum. After modifying the arrangement of GSs and introducing HEA (FeNiCrCoAl) coatings, the elastic modulus and hardness of the Gr/Al nanocomposites were 83 and 9.5 GPa, respectively, representing increases of 21.5% and 17.3% compared with those of pure aluminum. This study demonstrates that vertically oriented GSs in combination with HEA coatings at a mass fraction of 3.4% significantly enhance the mechanical properties of the Gr/Al nanocomposites. Full article
(This article belongs to the Section Materials Simulation and Design)
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<p>Schematic of the nanoindentation models: pure aluminum (<b>a</b>), Gr/Al-level3 (<b>b</b>), Gr/Al-vertical3 (<b>c</b>), HEA/Gr/Al-level3 (<b>d</b>), and HEA/Gr/Al-vertical3 (<b>e</b>).</p>
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<p>Dislocation distributions observed along the x-axis for the five models, namely pure aluminum, Gr/Al-level3, Gr/Al-vertical3, HEA/Gr/Al-level3, and HEA/Gr/Al-vertical3, at indenter displacements of d = 15, 20, 25, 30, and 35 Å. Dislocations are colored according to their Burgers vector. Green: 1/6&lt;112&gt;; Dark blue: 1/2&lt;110&gt;; Pink: 1/6&lt;110&gt;; Yellow: 1/3&lt;100&gt;; Bright blue: 1/3&lt;111&gt;; Red: others.</p>
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<p>Side views of the y–z-planes of Gr/Al-level3 (<b>a</b>) and HEA/Gr/Al-level3 (<b>b</b>) at indentation depths of 0, 20, 25, and 30 Å. The viewing direction is along the x-axis.</p>
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<p>Side views of the y–z-planes of Gr/Al-vertical3 (<b>a</b>) at indentation depths of 0, 26, 27, 28, and 29 Å and HEA/Gr/Al-vertical3 (<b>b</b>) at indentation depths of 0, 9, 11, 13, and 16 Å. The viewing direction is along the x-axis.</p>
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<p>In-plane height profiles of Gr at an indentation depth of 30 Å for models Gr/Al-level3 (<b>a</b>), HEA/Gr/Al-level3 (<b>b</b>), Gr/Al-vertical3 (<b>c</b>), and HEA/Gr/Al-vertical3 (<b>d</b>).</p>
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<p>Evolution of total dislocation length (<b>a</b>) and indentation force (<b>b</b>) with indenter displacement.</p>
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<p>Hardness values vs. indentation depths.</p>
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<p>Force–displacement curves at the unloading stage.</p>
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<p>Distribution of dislocation lines and defect atoms at different indenter displacements during the unloading stage. Dislocations are colored according to their Burgers vector. Green: 1/6&lt;112&gt;; Dark blue: 1/2&lt;110&gt;; Pink: 1/6&lt;110&gt;; Yellow: 1/3&lt;100&gt;; Bright blue: 1/3&lt;111&gt;; Red: others. (<b>a</b>) pure aluminum; (<b>b</b>) Gr/Al-level3; (<b>c</b>) Gr/Al-vertical3; (<b>d</b>) HEA/Gr/Al-level3; (<b>e</b>) HEA/Gr/Al-vertical3.</p>
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<p>Reduced Young’s modulus of the five models.</p>
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<p>Dislocation length–indenter displacement curves. (<b>a</b>) pure aluminum; (<b>b</b>) Gr/Al-vertical3; (<b>c</b>) HEA/Gr/Al-level3; (<b>d</b>) HEA/Gr/Al-vertical3.</p>
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19 pages, 5307 KiB  
Article
Energy Monitoring and Analysis of a Residential House in China
by Yanzhi Wang, Shaotong Han, Qiuqi Zhang, Jing Sun, Zhibao Cheng and An Chen
Buildings 2024, 14(9), 2930; https://doi.org/10.3390/buildings14092930 - 16 Sep 2024
Viewed by 189
Abstract
The energy consumption of residential buildings plays a crucial role in overall energy consumption and environmental sustainability. This paper aims to conduct an energy analysis of a residential house located in China, with a focus on comparing the accuracy of the model, identifying [...] Read more.
The energy consumption of residential buildings plays a crucial role in overall energy consumption and environmental sustainability. This paper aims to conduct an energy analysis of a residential house located in China, with a focus on comparing the accuracy of the model, identifying areas for improvement, and proposing energy-efficient solutions. Four sets of temperature sensors were placed to monitor the ambient temperature at which the building is located and the indoor temperature of the residential building during a heating season. The energy consumption of keeping the building running at a low temperature was recorded and compared with the simulation results to verify the accuracy of the model. The monitoring results give the weekly average temperature of each zone on each floor, and the door and window positions, room layouts, and orientations are discussed to analyze the thermal response of the building. In addition, the effect of the heat transfer coefficient of the exterior walls, the heat transfer coefficient of the roof, and the solar heat gain coefficient (SHGC) of the exterior windows on the heating energy consumption of the building are further analyzed through simulations. The results show that, after adding a certain thickness of insulation to the exterior walls and roofs of a building, increasing the thickness of the insulation layer produces little extra energy saving. The use of building windows with high SHGC can effectively reduce building heating energy consumption. Full article
(This article belongs to the Special Issue Building Energy-Saving Technology—2nd Edition)
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<p>Building photo.</p>
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<p>Geographical location of the house and surrounding buildings.</p>
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<p>Wallboard configuration.</p>
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<p>Roof configuration.</p>
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<p>Floor configuration.</p>
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<p>Locations of indoor temperature sensors (unit: mm): red color denotes sensors’ locations, where the pentagram and circle indicate locations of the main unit and temperature sensor, respectively.</p>
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<p>Locations of outdoor temperature sensors (unit: mm): red color denotes sensors’ locations, where the pentagram and circle indicate locations of the main unit and temperature sensor, respectively.</p>
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<p>Building model (balconies not included).</p>
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<p>Modelling flowchart: blue dashed line represents settings and functions of each software.</p>
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<p>Outdoor temperature monitoring data.</p>
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<p>Weekly average indoor temperatures for each zone on each floor of the building.</p>
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<p>Influence of the thermal resistance of exterior walls on building heating energy consumption.</p>
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<p>Influence of heat transfer coefficients of exterior walls on building heating energy consumption.</p>
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<p>Influence of roof thermal resistance on building heating energy consumption.</p>
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<p>Influence of roof heat transfer coefficient on building heating energy consumption.</p>
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<p>Influence of exterior window solar heat gain coefficients on building heating energy consumption.</p>
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24 pages, 8798 KiB  
Article
Context-Aware DGCN-Based Ship Formation Recognition in Remote Sensing Images
by Tao Zhang, Xiaogang Yang, Ruitao Lu, Xueli Xie, Siyu Wang and Shuang Su
Remote Sens. 2024, 16(18), 3435; https://doi.org/10.3390/rs16183435 - 16 Sep 2024
Viewed by 227
Abstract
Ship detection and formation recognition in remote sensing have increasingly garnered attention. However, research remains challenging due to arbitrary orientation, dense arrangement, and the complex background of ships. To enhance the analysis of ship situations in channels, we model the ships as the [...] Read more.
Ship detection and formation recognition in remote sensing have increasingly garnered attention. However, research remains challenging due to arbitrary orientation, dense arrangement, and the complex background of ships. To enhance the analysis of ship situations in channels, we model the ships as the key points and propose a context-aware DGCN-based ship formation recognition method. First, we develop a center point-based ship detection subnetwork, which employs depth-separable convolution to reduce parameter redundancy and combines coordinate attention with an oriented response network to generate direction-invariant feature maps. The center point of each ship is predicted by regression of the offset, target scale, and angle to realize the ship detection. Then, we adopt the spatial similarity of the ship center points to cluster the ship group, utilizing the Delaunay triangulation method to establish the topological graph structure of the ship group. Finally, we design a context-aware Dense Graph Convolutional Network (DGCN) with graph structure to achieve formation recognition. Experimental results on HRSD2016 and SGF datasets demonstrate that the proposed method can detect arbitrarily oriented ships and identify formations, attaining state-of-the-art performance. Full article
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<p>Examples of ship datasets in remote-sensing images. (<b>a</b>) The remote-sensing images are large in scale and require cropping during training. (<b>b</b>) Ships only occupy a small portion of the area in remote-sensing images, and the target features may be lost or obscured after multiple down-sampling operations. (<b>c</b>) The images have cluttered backgrounds (such as islands, port containers, dry docks, and other land targets), making locating the ships in complex backgrounds difficult.</p>
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<p>The overall framework of the proposed method. It adopts the center-point-based detection network to detect ships and get position information <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>c</mi> <mi>x</mi> </msub> <mo>,</mo> <msub> <mi>c</mi> <mi>y</mi> </msub> <mo>,</mo> <mi>w</mi> <mo>,</mo> <mi>h</mi> <mo>,</mo> <mi>θ</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>, while designing the context-aware DGCN to recognize the ship formation.</p>
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<p>The center-point-based detection model consists of feature extraction and center-point detection modules. The output is the position coordinates and angle information.</p>
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<p>The context-aware dense graph convolution network for ship formation recognition. The feature similarity clustering method is mainly used for ship grouping. The Delaunay triangulation serves as the graph structure of the ship formation. The DGCN aggregates and outputs features for formation classification. In the whole presentation, the graph nodes are treated as identical, and they have nothing to do with color change.</p>
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<p>Angle diagram of ship similarity calculation.</p>
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<p>The graph structure of ship formation based on the Delaunay triangulation. The input is the position coordinates of the center point within the ship formation. The output is the graph structure representation of ship formation for the downstream classification task.</p>
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<p>The illustration of a three-layer Locality Preserving GCN.</p>
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<p>Some typical samples from the HRSC2016 and SGF datasets. (<b>a</b>) Examples from the HRSC2016 dataset; (<b>b</b>) examples from the SGF dataset.</p>
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<p>The standard formation of the ship group. (<b>a</b>–<b>f</b>) are the six different ship formations arranged with different configurations, and they are named Formation1 to Formation6. CV, CG, DD, FFG, and SSN represent aircraft carriers, cruisers, destroyers, frigates, and nuclear submarines, respectively.</p>
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<p>Qualitative detection results on the HRSC2016 and SGF datasets with different methods. (<b>a</b>) The detection results of <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">R</mi> <mn>2</mn> </msup> <mi>CNN</mi> </mrow> </semantics></math>; (<b>b</b>) the detection results of <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">R</mi> <mn>3</mn> </msup> <mi>Det</mi> </mrow> </semantics></math>; (<b>c</b>) the detection results of the proposed method.</p>
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<p>The test results of center structure recognition and isolated ship detection. The (<b>a</b>–<b>f</b>) represent the different ship groups on the SGF dataset. The <b>first row</b> is the visual results of ship center point detection, and the <b>second row</b> plots the test result. Among them, each graph in the second row represents the identified group central structure and marks other isolated ship targets that do not belong to the group central structure. For example, in (<b>a</b>), the yellow dots clearly form the central point structure of the ship groups, and the blue triangles represent isolated ships.</p>
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<p>The visual test results for ship grouping based on feature similarity clustering. The <b>first row</b> shows the visual results of ship center point detection, including different ship groups and some isolated ships. The <b>second row</b> represents the distribution of ship centers. The <b>last row</b> is the distribution of the proposed grouping method. Different colors display the grouping results of the clustering change processes.</p>
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<p>The formation structure representation based on the Delaunay triangulation. The <b>first row</b> shows the visual results of ship grouping. The <b>second row</b> represents the distribution of ship centers. The <b>last row</b> is the graph structure of the different formations.</p>
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<p>The qualitative experimental results of formation recognition. (<b>a</b>) The recognition result of formation 1. (<b>b</b>) The recognition result of formation 2. (<b>c</b>) The recognition result of formation 6. (<b>d</b>) The recognition result of formation 5. (<b>e</b>) The recognition result of formations 2 and 6. (<b>f</b>) The recognition result of formations 2 and 3. The yellow circles are the center points of the ships, and the groups connected in green represent ship formations.</p>
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<p>The ship groups and its peripheral contour. (<b>a</b>–<b>c</b>) show the different identified formations, and (<b>d</b>–<b>f</b>) display the convex hull (green) and the outer quadrilateral (orange) of ship formations.</p>
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27 pages, 3853 KiB  
Article
Functionally Graded Materials and Structures: Unified Approach by Optimal Design, Metal Additive Manufacturing, and Image-Based Characterization
by Rui F. Silva, Pedro G. Coelho, Carolina V. Gustavo, Cláudia J. Almeida, Francisco Werley Cipriano Farias, Valdemar R. Duarte, José Xavier, Marcos B. Esteves, Fábio M. Conde, Filipa G. Cunha and Telmo G. Santos
Materials 2024, 17(18), 4545; https://doi.org/10.3390/ma17184545 - 16 Sep 2024
Viewed by 391
Abstract
Functionally Graded Materials (FGMs) can outperform their homogeneous counterparts. Advances in digitalization technologies, mainly additive manufacturing, have enabled the synthesis of materials with tailored properties and functionalities. Joining dissimilar metals to attain compositional grading is a relatively unexplored research area and holds great [...] Read more.
Functionally Graded Materials (FGMs) can outperform their homogeneous counterparts. Advances in digitalization technologies, mainly additive manufacturing, have enabled the synthesis of materials with tailored properties and functionalities. Joining dissimilar metals to attain compositional grading is a relatively unexplored research area and holds great promise for engineering applications. Metallurgical challenges may arise; thus, a theoretical critical analysis is presented in this paper. A multidisciplinary methodology is proposed here to unify optimal design, multi-feed Wire-Arc Additive Manufacturing (WAAM), and image-based characterization methods to create structure-specific oriented FGM parts. Topology optimization is used to design FGMs. A beam under pure bending is used to explore the layer-wise FGM concept, which is also analytically validated. The challenges, limitations, and role of WAAM in creating FGM parts are discussed, along with the importance of numerical validation using full-field deformation data. As a result, a conceptual FGM engineering workflow is proposed at this stage, enabling digital data conversion regarding geometry and compositional grading. This is a step forward in processing in silico data, with a view to experimentally producing parts in future. An optimized FGM beam, revealing an optimal layout and a property gradient from iron to copper along the build direction (bottom–up) that significantly reduces the normal pure bending stresses (by 26%), is used as a case study to validate the proposed digital workflow. Full article
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<p>(<b>a</b>) Experimental and simulated Al-Cu phase diagram [<a href="#B59-materials-17-04545" class="html-bibr">59</a>]. (<b>b</b>) Influence of Ni equivalents on hot crack susceptibility. A, AF, FA, and F denote transitions in solidification modes (austenitic, austenitic–ferritic, ferritic–austenitic, and ferritic, respectively), depending on the composition. The blue circles indicate the susceptibility to hot cracking. As susceptibility increases, the weldability and printability of the alloys decrease.</p>
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<p>Theoretical variation in the Young’s modulus for the Fe-Cu system based on the HS bounds.</p>
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<p>Two-dimensional (half) beam numerical model. The distributed loads <math display="inline"><semantics> <mrow> <mi>Q</mi> </mrow> </semantics></math> generate a torque such that the beam is subject to pure bending. Representation of the FGMTO density-based material interpolation scheme.</p>
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<p>FGM result for the beam example solving the optimization problem (4): (<b>a</b>) Young’s modulus distribution (<b>left</b>) and von Mises stress map (<b>right</b>). (<b>b</b>) Density fields.</p>
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<p>Suggested experimental workflow to address challenges when producing an FGM by WAAM.</p>
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<p>Digital workflow converting digital data from TO to the AM system.</p>
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<p>Surface plot of the interpolation function “Surffit1” from two different angles.</p>
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<p>Comparative analysis of results between structured (<b>top</b>) and unstructured (<b>bottom</b>) meshes for the beam example: (<b>a</b>) Young’s modulus distribution [GPa]. (<b>b</b>) Von Mises stress map [MPa]. (<b>c</b>) Detailed representation of the mesh called Unstructured I.</p>
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<p>Element centroid coordinate <span class="html-italic">y</span> against the respective von Mises stress <math display="inline"><semantics> <mrow> <msup> <mrow> <mi>σ</mi> </mrow> <mrow> <mi>V</mi> <mi>M</mi> </mrow> </msup> </mrow> </semantics></math> in the region of the beam subject to pure bending. Stress results are given for the different meshes studied, structured (original) and unstructured (I, II and III).</p>
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11 pages, 1951 KiB  
Article
Optimization of Non-Alloyed Backside Ohmic Contacts to N-Face GaN for Fully Vertical GaN-on-Silicon-Based Power Devices
by Youssef Hamdaoui, Sofie S. T. Vandenbroucke, Sondre Michler, Katir Ziouche, Matthias M. Minjauw, Christophe Detavernier and Farid Medjdoub
Micromachines 2024, 15(9), 1157; https://doi.org/10.3390/mi15091157 - 15 Sep 2024
Viewed by 392
Abstract
In the framework of fully vertical GaN-on-Silicon device technology development, we report on the optimization of non-alloyed ohmic contacts on the N-polar n+-doped GaN face backside layer. This evaluation is made possible by using patterned TLMs (Transmission Line Model) through direct laser writing [...] Read more.
In the framework of fully vertical GaN-on-Silicon device technology development, we report on the optimization of non-alloyed ohmic contacts on the N-polar n+-doped GaN face backside layer. This evaluation is made possible by using patterned TLMs (Transmission Line Model) through direct laser writing lithography after locally removing the substrate and buffer layers in order to access the n+-doped backside layer. As deposited non-alloyed metal stack on top of N-polar orientation GaN layer after buffer layers removal results in poor ohmic contact quality. To significantly reduce the related specific contact resistance, an HCl treatment is applied prior to metallization under various time and temperature conditions. A 3 min HCl treatment at 70 °C is found to be the optimum condition to achieve thermally stable high ohmic contact quality. To further understand the impact of the wet treatment, SEM (Scanning Electron Microscopy) and XPS (X-ray Photoelectron Spectroscopy) analyses were performed. XPS revealed a decrease in Ga-O concentration after applying the treatment, reflecting the higher oxidation susceptibility of the N-polar face compared to the Ga-polar face, which was used as a reference. SEM images of the treated samples show the formation of pyramids on the N-face after HCl treatment, suggesting specific wet etching planes of the GaN crystal from the N-face. The size of the pyramids is time-dependent; thus, increasing the treatment duration results in larger pyramids, which explains the degradation of ohmic contact quality after prolonged high-temperature HCl treatment. Full article
(This article belongs to the Section D1: Semiconductor Devices)
17 pages, 3315 KiB  
Article
Application of the Gradient-Boosting with Regression Trees to Predict the Coefficient of Friction on Drawbead in Sheet Metal Forming
by Sherwan Mohammed Najm, Tomasz Trzepieciński, Salah Eddine Laouini, Marek Kowalik, Romuald Fejkiel and Rafał Kowalik
Materials 2024, 17(18), 4540; https://doi.org/10.3390/ma17184540 - 15 Sep 2024
Viewed by 368
Abstract
Correct design of the sheet metal forming process requires knowledge of the friction phenomenon occurring in various areas of the drawpiece. Additionally, the friction at the drawbead is decisive to ensure that the sheet flows in the desired direction. This article presents the [...] Read more.
Correct design of the sheet metal forming process requires knowledge of the friction phenomenon occurring in various areas of the drawpiece. Additionally, the friction at the drawbead is decisive to ensure that the sheet flows in the desired direction. This article presents the results of experimental tests enabling the determination of the coefficient of friction at the drawbead and using a specially designed tribometer. The test material was a DC04 carbon steel sheet. The tests were carried out for different orientations of the samples in relation to the sheet rolling direction, different drawbead heights, different lubrication conditions and different average roughnesses of the countersamples. According to the aim of this work, the Features Importance analysis, conducted using the Gradient-Boosted Regression Trees algorithm, was used to find the influence of several parameter features on the coefficient of friction. The advantage of gradient-boosted decision trees is their ability to analyze complex relationships in the data and protect against overfitting. Another advantage is that there is no need for prior data processing. According to the best of the authors’ knowledge, the effectiveness of gradient-boosted decision trees in analyzing the friction occurring in the drawbead in sheet metal forming has not been previously studied. To improve the accuracy of the model, five MinLeafs were applied to the regression tree, together with 500 ensembles utilized for learning the previously learned nodes, noting that the MinLeaf indicates the minimum number of leaf node observations. The least-squares-boosting technique, often known as LSBoost, is used to train a group of regression trees. Features Importance analysis has shown that the friction conditions (dry friction of lubricated conditions) had the most significant influence on the coefficient of friction, at 56.98%, followed by the drawbead height, at 23.41%, and the sample width, at 11.95%. The average surface roughness of rollers and sample orientation have the smallest impact on the value of the coefficient of friction at 6.09% and 1.57%, respectively. The dispersion and deviation observed for the testing dataset from the experimental data indicate the model’s ability to predict the values of the coefficient of friction at a coefficient of determination of R2 = 0.972 and a mean-squared error of MSE = 0.000048. It was qualitatively found that in order to ensure the optimal (the lowest) coefficient of friction, it is necessary to control the friction conditions (use of lubricant) and the drawbead height. Full article
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<p>3D surface topography and selected roughness parameters of DC04 steel sheet.</p>
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<p>(<b>a</b>) Diagram and (<b>b</b>) view of the testing device: 1, 2, 3—working rollers; 4—support roller; 5—body; 6—sample; 7—nut; 8—horizontal tension cell; 9—upper tension cell; 10, 11—load cells.</p>
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<p>Scheme of force parameters for the test carried out with (<b>a</b>) fixed and (<b>b</b>) freely rotating rollers.</p>
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<p>Model performance of the training and testing iterations.</p>
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<p>SHAP value plot influence on COF.</p>
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<p>Relative importance of input parameters on COF; (<b>a</b>) ordered bar chart and (<b>b</b>) pie chart with percentage.</p>
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<p>Actual and predicted values; (<b>a</b>) training COF dataset and (<b>b</b>) testing COF dataset.</p>
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<p>Actual and predicted values of training COF dataset with 0.1 adjusting.</p>
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<p>Actual and predicted values of COF; (<b>a</b>) training dataset and (<b>b</b>) testing dataset.</p>
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16 pages, 12097 KiB  
Article
Insight into the Structural and Performance Correlation of Photocatalytic TiO2/Cu Composite Films Prepared by Magnetron Sputtering Method
by Kun Lu, Miao Sun, Yaohong Jiang, Xinmeng Wu, Lijun Zhao and Junhua Xu
Catalysts 2024, 14(9), 621; https://doi.org/10.3390/catal14090621 - 14 Sep 2024
Viewed by 342
Abstract
Photocatalysis technology, as an efficient and safe environmentally friendly purification technique, has garnered significant attention and interest. Traditional TiO2 photocatalytic materials still face limitations in practical applications, hindering their widespread adoption. The research prepared TiO2/Cu films with different Cu contents [...] Read more.
Photocatalysis technology, as an efficient and safe environmentally friendly purification technique, has garnered significant attention and interest. Traditional TiO2 photocatalytic materials still face limitations in practical applications, hindering their widespread adoption. The research prepared TiO2/Cu films with different Cu contents using a magnetron sputtering multi-target co-deposition technique. The incorporation of Cu significantly enhances the antibacterial properties and visible light response of the films. The effects of different Cu contents on the microstructure, surface morphology, wettability, antibacterial properties, and visible light response of the films were investigated using an X-ray diffractometer, X-ray photoelectron spectrometer, field emission scanning electron microscope, confocal laser scanning microscope, Ultraviolet–visible spectrophotometer, and contact angle goniometer. The results showed that the prepared TiO2/Cu films were mainly composed of the rutile TiO2 phase and face-center cubic Cu phase. The introduction of Cu affected the crystal orientation of TiO2 and refined the grain size of the films. With the increase in Cu content, the surface roughness of the films first decreased and then increased. The water contact angle of the films first increased and then decreased, and the film exhibited optimal hydrophobicity when the Cu target power was 10 W. The TiO2/Cu films showed good antibacterial properties against Escherichia coli and Staphylococcus aureus. The introduction of Cu shifted the absorption edge of the films to the red region, significantly narrowed the band gap width to 2.5 eV, and broadened the light response range of the films to the visible light region. Full article
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<p>XRD patterns of TiO<sub>2</sub>/Cu composite films with different Cu target powers.</p>
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<p>XPS spectra of TiO<sub>2</sub>/Cu composite films with Cu target power of 15 W (<b>a</b>) full spectra. (<b>b</b>) Ti 2p. (<b>c</b>) Cu 2p and (<b>d</b>) O 1s.</p>
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<p>Surface morphology of TiO<sub>2</sub>/Cu composite films after annealing at 500 °C (<b>a</b>) TiO<sub>2</sub>; (<b>b</b>) Cu10; (<b>c</b>) Cu15; (<b>d</b>) Cu20.</p>
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<p>Laser confocal spectra of TiO<sub>2</sub>/Cu composite films with different Cu target powers (<b>a</b>) TiO<sub>2</sub>; (<b>b</b>) Cu10; (<b>c</b>) Cu15; (<b>d</b>) Cu20.</p>
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<p>Contact angle of TiO<sub>2</sub>/Cu films with different Cu target power (<b>a</b>) TiO<sub>2</sub>; (<b>b</b>) Cu10; (<b>c</b>) Cu15; (<b>d</b>) Cu20.</p>
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<p>Contact angle of TiO<sub>2</sub>/Cu films with different Cu target power.</p>
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<p>Antibacterial effect of TiO<sub>2</sub>/Cu composite film (<b>a</b>,<b>b</b>) <span class="html-italic">Escherichia coli</span>, (<b>c</b>,<b>d</b>) <span class="html-italic">Staphylococcus aureus</span>.</p>
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<p>(<b>a</b>) UV–Vis diffuse reflectance spectra and (<b>b</b>) optical band gap of TiO<sub>2</sub>/Cu composite films with different Cu target power.</p>
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<p>The antibacterial mechanism of TiO<sub>2</sub>/Cu composite film.</p>
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<p>Three-dimensional model of magnetron sputtering system.</p>
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<p>The schematic diagram of antibacterial test by coating plate method.</p>
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10 pages, 3451 KiB  
Article
Hunting for Monolayer Black Phosphorus with Photoluminescence Microscopy
by Chenghao Pan, Yixuan Ma, Quan Wan, Boyang Yu, Shenyang Huang and Hugen Yan
Photonics 2024, 11(9), 866; https://doi.org/10.3390/photonics11090866 (registering DOI) - 14 Sep 2024
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Abstract
Monolayer black phosphorus (BP) holds great promise for naturally hyperbolic polaritons and correlated states in rectangular moiré superlattices. However, preparing and identifying high-quality monolayer BP are challenging due to its instability and high transparency, which limits extensive studies. In this study, we developed [...] Read more.
Monolayer black phosphorus (BP) holds great promise for naturally hyperbolic polaritons and correlated states in rectangular moiré superlattices. However, preparing and identifying high-quality monolayer BP are challenging due to its instability and high transparency, which limits extensive studies. In this study, we developed a method for rapidly and nondestructively identifying monolayer BP and its crystal orientation simultaneously using modified photoluminescence (PL) microscopy. The optical contrast of monolayer BP has been significantly increased by at least twenty times compared to previous reports, making it visible even on a transparent substrate. The polarization dependence of optical contrast also allows for the in situ determination of crystal orientation. Our study facilitates the identification of monolayer BP, expediting more extensive research on and potential industrial applications of this material. Full article
(This article belongs to the Special Issue Recent Advances in Infrared Photodetection and Imaging)
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