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Search Results (13,465)

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26 pages, 3740 KiB  
Article
Spatial–Temporal Evolution and Influencing Mechanism of Coupling Coordination Level of Social–Ecological Systems in China’s Resource-Based Cities Under the Carbon Neutrality Goal
by Yunhui Zhang, Zhong Wang, Yanran Peng, Wei Wang and Chengxi Tian
Land 2025, 14(1), 207; https://doi.org/10.3390/land14010207 - 20 Jan 2025
Abstract
Carbon emissions have a profound impact on the transformation goals and development paths of cities. In the context of carbon neutrality, it is of great significance to explore the coupling coordination level of the social–ecological systems in resource-based cities for realizing regional low-carbon [...] Read more.
Carbon emissions have a profound impact on the transformation goals and development paths of cities. In the context of carbon neutrality, it is of great significance to explore the coupling coordination level of the social–ecological systems in resource-based cities for realizing regional low-carbon and sustainable development. In this study, the entropy weighting method, coupling coordination degree model and geographical detector were used to measure the comprehensive development level and coupling coordination level of the social–ecological system in 116 resource-based cities in China from 2010 to 2020 and their spatial–temporal characteristics and influencing mechanism were analyzed. The results show the following: (1) The comprehensive development level of the social system in China’s resource-based cities has a significant upward trend, while the comprehensive development level of the ecological system has a gentle upward trend, and the coupling and coordination level of the social–ecological system has a fluctuating upward trend. (2) There is obvious spatial differentiation between the comprehensive development level and the coupling coordination level of the social–ecological systems in resource-based cities in China, and the relative difference is gradually increasing. (3) The digital economy index, urbanization level, science and education investment, and population density are important factors affecting the coupling coordination level, and the interaction between digital economy index, urbanization level, and population density has a strong explanatory power in the differentiation of the coupling coordination level. Based on the above conclusions, effective policy recommendations are put forward: formulate more refined and differentiated development paths, co-ordinate the spatial layout to give full play to the role of urban agglomeration, vigorously develop the digital economy, increase investment in science and education, rely on scientific and technological innovation to create development advantages, reasonably guide the population layout and take a new urbanization development route. Full article
(This article belongs to the Section Land Socio-Economic and Political Issues)
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<p>Study area.</p>
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<p>Mechanisms of social–ecological system interactions in the context of carbon neutrality.</p>
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<p>The temporal variation of the comprehensive score and coupling coordination level of the social–ecological systems in resource-based cities.</p>
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<p>Spatial differentiation of comprehensive development level of social systems in resource-based cities.</p>
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<p>Spatial differentiation of comprehensive development level of ecological systems in resource-based cities.</p>
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<p>Spatial differentiation of coupling coordination degree of social–ecological systems in resource-based cities.</p>
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<p>Interaction detection results in 2010, 2015 and 2020.</p>
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21 pages, 1391 KiB  
Article
Empirically Validated Method to Simulate Electric Minibus Taxi Efficiency Using Tracking Data
by Chris Joseph Abraham , Stephan Lacock , Armand André du Plessis and Marthinus Johannes Booysen
Energies 2025, 18(2), 446; https://doi.org/10.3390/en18020446 - 20 Jan 2025
Abstract
Simulation is a cornerstone of planning and facilitating the transition towards electric mobility in sub-Saharan Africa’s informal public transport. The primary objective of this study is to validate and refine the electro-kinetic model used to simulate electric versions of the sector’s minibuses. A [...] Read more.
Simulation is a cornerstone of planning and facilitating the transition towards electric mobility in sub-Saharan Africa’s informal public transport. The primary objective of this study is to validate and refine the electro-kinetic model used to simulate electric versions of the sector’s minibuses. A systematic simulation methodology is also developed to correct the simulation parameters and improve the high-frequency GPS data used with the model. A retrofitted electric minibus was used to capture high-frequency GPS mobility data and power draw from the battery. The method incorporates key refinements such as corrections for gross vehicle mass, elevation and speed smoothing, radial drag, hill-climb forces, and the calibration of propulsion and regenerative braking parameters. The refined simulation demonstrates improved alignment with measured power draw and trip energy usage, reducing error margins and enhancing model reliability. Factors such as trip characteristics and environmental conditions, including wind resistance, are identified as potential contributors to observed discrepancies. These findings highlight the importance of precise data handling and model calibration for accurate energy simulation and decision making in the transition to electric public transport. This work provides a robust framework for future studies and practical implementations, offering insights into the technical and operational challenges of electrifying informal public transport systems in resource-constrained regions. Full article
(This article belongs to the Special Issue Urban Electromobility and Electric Propulsion)
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<p>Energy expenditures from recent attempts in the literature compared to that measured in this paper [<a href="#B31-energies-18-00446" class="html-bibr">31</a>,<a href="#B35-energies-18-00446" class="html-bibr">35</a>,<a href="#B37-energies-18-00446" class="html-bibr">37</a>,<a href="#B38-energies-18-00446" class="html-bibr">38</a>,<a href="#B39-energies-18-00446" class="html-bibr">39</a>,<a href="#B40-energies-18-00446" class="html-bibr">40</a>]. Care should be taken when comparing these numbers, since different datasets and vehicles with different weights were used. The weights used for each source are reported.</p>
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<p>Methodology pipeline.</p>
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<p>Vehicles routes over 30 trips conducted over 10 days with colour indicating density of samples.</p>
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<p>Energy usage rate (kWh/km) recorded for various trips, and simulation results with the uncorrected model (measured mean of all trips = 0.342 kWh/km; measured mean of trips longer than 5 km = 0.327 kWh/km; simulated mean of all trips = 0.372 kWh/km; simulated mean of trips longer than 5 km = 0.375 kWh/km).</p>
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<p>Error in energy usage of each trip simulated before and after data correction.</p>
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<p>Measured and simulated energy and power profiles for trips before and after corrections were applied to the simulation method. Trip 3 is a normal trip with a typical error between measured and (corrected) simulated profiles. Trip 23 is the trip with the worst-case simulation error, and Trip 12 is the best-case simulation error, both after corrections were applied.</p>
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<p>Disaggregation of power components. Trip 3 (<b>a</b>,<b>b</b>) shows the disaggreated output for all the components. The simulation before corrections were applied is shown in (<b>a</b>,<b>b</b>) shows the output from the corrected simulation. Propulsion and regeneration energy components per trip after corrections are shown in (<b>c</b>), and the remaining errors are shown in (<b>d</b>).</p>
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<p>Gaussian smoothing operations on GPS altitude and speed data for Trip 3.</p>
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<p>Error in propulsion and regeneration energies for various propulsion and regeneration factors.</p>
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<p>Final propulsion and regeneration energy usage (measured mean of all trips = 0.342 kWh/km; measured mean of trips longer than 5 km = 0.327 kWh/km; simulated mean of all trips = 0.333 kWh/km; simulated mean of trips longer than 5 km = 0.331 kWh/km). The errors are shown in <a href="#energies-18-00446-f005" class="html-fig">Figure 5</a>.</p>
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23 pages, 1653 KiB  
Article
A Feature-Enhanced Small Object Detection Algorithm Based on Attention Mechanism
by Zhe Quan and Jun Sun
Sensors 2025, 25(2), 589; https://doi.org/10.3390/s25020589 - 20 Jan 2025
Abstract
With the rapid development of AI algorithms and computational power, object recognition based on deep learning frameworks has become a major research direction in computer vision. UAVs equipped with object detection systems are increasingly used in fields like smart transportation, disaster warning, and [...] Read more.
With the rapid development of AI algorithms and computational power, object recognition based on deep learning frameworks has become a major research direction in computer vision. UAVs equipped with object detection systems are increasingly used in fields like smart transportation, disaster warning, and emergency rescue. However, due to factors such as the environment, lighting, altitude, and angle, UAV images face challenges like small object sizes, high object density, and significant background interference, making object detection tasks difficult. To address these issues, we use YOLOv8s as the basic framework and introduce a multi-level feature fusion algorithm. Additionally, we design an attention mechanism that links distant pixels to improve small object feature extraction. To address missed detections and inaccurate localization, we replace the detection head with a dynamic head, allowing the model to route objects to the appropriate head for final output. We also introduce Slideloss to improve the model’s learning of difficult samples and ShapeIoU to better account for the shape and scale of bounding boxes. Experiments on datasets like VisDrone2019 show that our method improves accuracy by nearly 10% and recall by about 11% compared to the baseline. Additionally, on the AI-TODv1.5 dataset, our method improves the mAP50 from 38.8 to 45.2. Full article
(This article belongs to the Section Remote Sensors)
26 pages, 23275 KiB  
Article
A Cause Analysis Model of Nuclear Accidents in Marine Nuclear Power Plants Based on the Perspective of a Socio-Technical System
by Fang Zhao, Ruihua Shu, Shoulong Xu and Shuliang Zou
Safety 2025, 11(1), 10; https://doi.org/10.3390/safety11010010 - 20 Jan 2025
Abstract
Marine nuclear power plants (MNPPs) represent items of forward-looking high-end engineering equipment combining nuclear power and ocean engineering, with unique advantages and broad application prospects. When a nuclear accident occurs, it causes considerable economic losses and casualties. The traditional accident analysis of nuclear [...] Read more.
Marine nuclear power plants (MNPPs) represent items of forward-looking high-end engineering equipment combining nuclear power and ocean engineering, with unique advantages and broad application prospects. When a nuclear accident occurs, it causes considerable economic losses and casualties. The traditional accident analysis of nuclear power plants only considers the failure of a single system or component, without considering the coupling between the system and the operator, the environment, and other factors. In this study, the cause mechanism of nuclear accidents in MNPPs is analyzed from the perspective of a social technology system. The causal analysis model is constructed by using the internal core causal analysis (e.g., technical control) and external stimulation causal analysis (e.g., social intervention) of accidents, after which the mechanism of the coupled evolution of each influencing factor is analyzed. A Bayesian network inference model is used to quantify the coupling relationship between the factors that affect the deterioration of nuclear accidents. The results show that the main influencing factors are pump failure, valve failure, insufficient response time, poor psychological state, unfavorable sea conditions, unfavorable offshore operating environments, communication failure, inappropriate organizational procedures, inadequate research and design institutions, inadequate regulatory agencies, and inadequate policies. These 12 factors have a high degree of causality and are the main factors influencing the deterioration of the small break loss of coolant accident (SBLOCA). In addition, the causal chain that is most likely to influence the development of SBLOCA into a severe accident is obtained. This provides a theoretical basis for preventing the occurrence of marine nuclear power accidents. Full article
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<p>Characteristic analysis diagram of socio-technical system.</p>
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<p>Analyzing perspectives of nuclear accident causation model.</p>
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<p>Relationship model of influencing factors in nuclear technology system.</p>
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<p>Relationship model of ship-influencing factors.</p>
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<p>Relationship model of the crew-influencing factors.</p>
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<p>Internal core cause mechanism of nuclear accidents in a marine reactor.</p>
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<p>Relationship model of intervention factors of government and other departments.</p>
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<p>Relationship model of the organizational factors.</p>
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<p>Relationship model of social factors.</p>
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<p>External core cause mechanism of nuclear accidents in a marine reactor.</p>
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<p>Causal analysis model for nuclear accidents in marine reactors.</p>
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<p>Logical block diagram of safety injection system.</p>
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<p>Failure factor relationship model of low-pressure safety injection system.</p>
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<p>Causality model of internal inherent factors and accident scenario factors.</p>
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<p>Causal relationship model of external intervening factors.</p>
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<p>Causal modeling of nuclear accidents in marine reactors.</p>
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<p>State probabilities of node variables for low-pressure safety injection system.</p>
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<p>State probabilities of node variables for accident scenario factors.</p>
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<p>State probabilities of node variables for internal intrinsic factors.</p>
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<p>State probabilities of node variables for external intervening factors.</p>
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<p>Input modeling of nuclear accidents in marine reactors.</p>
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<p>Reverse reasoning for SBLOCA in marine reactors.</p>
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<p>Comparison of prior and posterior probability of each node variable.</p>
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<p>Percentage change of each node variable.</p>
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<p>Maximum possible causal chain of a nuclear accident.</p>
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17 pages, 6525 KiB  
Article
Impact Assessment of Grid-Connected Solar Photovoltaic Systems on Power Distribution Grid: A Case Study on a Highly Loaded Feeder in Ulaanbaatar Ger District
by Turmandakh Bat-Orgil, Battuvshin Bayarkhuu, Bayasgalan Dugarjav and Insu Paek
Energies 2025, 18(2), 440; https://doi.org/10.3390/en18020440 - 20 Jan 2025
Abstract
Adopting and widely implementing solar photovoltaic (PV) systems are regarded as a promising solution to address energy crises by providing a sustainable and independent electricity supply while significantly reducing greenhouse gas emissions to combat climate change. This encourages households, organizations, and enterprises to [...] Read more.
Adopting and widely implementing solar photovoltaic (PV) systems are regarded as a promising solution to address energy crises by providing a sustainable and independent electricity supply while significantly reducing greenhouse gas emissions to combat climate change. This encourages households, organizations, and enterprises to install solar PV systems. However, there are many solar PV systems that have been connected to the power distribution grid without following the required procedures. Power distribution grid operators cannot detect the locations of these solar PV systems. Thus, it is necessary to assess the impact of solar PV systems on the power distribution grid in detail, even though there are multiple economic and environmental advantages associated with installing solar PV systems. This study analyzes the changes in an overloaded power distribution grid’s power losses and voltage deviations with solar PV systems. There are two main factors considered for assessing the impact of the solar PV system on the power distribution grid: the total installed capacity of the solar PV systems and the location of the connection. Based on a comparison between the measurement results of three feeders with higher loads in the Ulaanbaatar area, the Dambadarjaa feeder, which has the highest load, was selected. The impact of the solar PV systems on the selected feeder was analyzed by connecting eight solar PV systems at four different locations. Their total installed capacities vary between 25 and 80 percent of the highest daily load of the selected feeder. The results show that the power loss of the feeder can be greatly reduced when the total installed capacity of the solar PV systems is selected optimally, and the location of the connection is at the end of the power distribution grid. Full article
(This article belongs to the Section A2: Solar Energy and Photovoltaic Systems)
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<p>Equivalent schemes of the feeders with the highest loads in 110/35/10 kV Selbe substation: (<b>a</b>) Chingeltei feeder; (<b>b</b>) Sogoot feeder; (<b>c</b>) Dambadarjaa feeder, where symbol “/” expresses the nominal cross-section of the cable.</p>
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<p>Measured loads of the Dambadarjaa feeder shown on a monthly basis.</p>
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<p>Solar irradiance and ambient temperature in Ulaanbaatar.</p>
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<p>A developed scheme for the Dambadarjaa feeder using the PowerFactory simulation software.</p>
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<p>Dambadarjaa feeder map from 110/35/10 kV Selbe substation with solar PV systems connected at different points: (<b>a</b>) Dambadarjaa feeder map from 110/35/10 kV Selbe substation; (<b>b</b>) solar PV systems connected at the beginning of the power distribution line; (<b>c</b>) solar PV systems connected at the middle of the power distribution line; and (<b>d</b>) solar PV systems connected at the end of the power distribution line.</p>
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<p>Energy losses depend on the total installed capacity and connection points of solar PV systems with regard to the feeder load.</p>
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<p>Costs of energy losses depend on the total installed capacity and connection points of solar PV systems with regard to the feeder load.</p>
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<p>Probed voltage deviation at the beginning of the power distribution line when the solar PV systems are connected (<b>a</b>) at the beginning, (<b>b</b>) in the middle, (<b>c</b>) at the end, and (<b>d</b>) evenly distributed throughout the power distribution line.</p>
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<p>Probed voltage deviation in the middle of the power distribution line when the solar PV systems are connected (<b>a</b>) at the beginning, (<b>b</b>) in the middle, (<b>c</b>) at the end, and (<b>d</b>) evenly distributed throughout the power distribution line.</p>
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<p>Probed voltage deviation at the end of the power distribution line when the solar PV systems are connected (<b>a</b>) at the beginning, (<b>b</b>) in the middle, (<b>c</b>) at the end, and (<b>d</b>) evenly distributed throughout the power distribution line.</p>
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20 pages, 3387 KiB  
Article
A Fuzzy Inertia-Based Virtual Synchronous Generator Model for Managing Grid Frequency Under Large-Scale Electric Vehicle Integration
by Yajun Jia and Zhijian Jin
Processes 2025, 13(1), 287; https://doi.org/10.3390/pr13010287 - 20 Jan 2025
Abstract
The rapid proliferation of EVs has ushered in a transformative era for the power industry, characterized by increased demand volatility and grid frequency instability. In response to these challenges, this paper introduces a novel approach that combines fuzzy logic with adaptive inertia control [...] Read more.
The rapid proliferation of EVs has ushered in a transformative era for the power industry, characterized by increased demand volatility and grid frequency instability. In response to these challenges, this paper introduces a novel approach that combines fuzzy logic with adaptive inertia control to improve the frequency stability of grids amidst large-scale electric vehicle (EV) integration. The proposed methodology not only adapts to varying charging scenarios but also strikes a balance between steady-state and dynamic performance considerations. This research establishes a solid theoretical foundation for the inertia-adaptive virtual synchronous generator (VSG) concept and introduces a pioneering fuzzy inertia-based VSG methodology. Additionally, it incorporates adaptive output scaling factors to enhance the robustness and adaptability of the control strategy. These contributions offer valuable insights into the evolving landscape of adaptive VSG strategies and provide a pragmatic solution to the pressing challenges arising from the integration of large-scale EVs, ultimately fostering the resilience and sustainability of contemporary power systems. Finally, simulation results illustrate that the new proposed fuzzy adaptive inertia-based VSG method is effective and has superior advantages over the traditional VSG and droop control strategies. Specifically, the proposed method reduces the maximum frequency change by 25% during load transitions, with a peak variation of 0.15 Hz compared to 0.2 Hz for the traditional VSG. Full article
(This article belongs to the Special Issue Applications of Smart Microgrids in Renewable Energy Development)
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<p>Power grids highly rely on power electronic devices for rectification and inversion.</p>
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<p>Basic structure of VSG control used for power grids with large-scale EV integration.</p>
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<p>Structure of the phase-locked loop.</p>
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<p>Transfer function of frequency regulation process.</p>
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<p>Relationship between Δ<span class="html-italic">f<sub>max</sub></span> and <span class="html-italic">ξ</span>.</p>
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<p>Proposed adaptive fuzzy inertia controller.</p>
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<p>Membership functions. (<b>a</b>) Membership function for <span class="html-italic">In</span> 1; (<b>b</b>) membership function for <span class="html-italic">In</span> 2; and (<b>c</b>) membership function for <span class="html-italic">Out</span>.</p>
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<p>Steady-state control performance. (<b>a</b>) Traditional VSG with constant inertia; and (<b>b</b>) proposed fuzzy adaptive inertia-based VSG.</p>
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<p>Steady-state control performance. (<b>a</b>) Traditional VSG with constant inertia; and (<b>b</b>) proposed fuzzy adaptive inertia-based VSG.</p>
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<p>Dynamic control performance. (<b>a</b>) Traditional VSG with constant inertia; and (<b>b</b>) proposed fuzzy adaptive inertia-based VSG.</p>
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<p>Dynamic control performance. (<b>a</b>) Traditional VSG with constant inertia; and (<b>b</b>) proposed fuzzy adaptive inertia-based VSG.</p>
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<p>Dynamic control performance of proposed fuzzy adaptive inertia-based VSG when scaling coefficient <span class="html-italic">K<sub>J</sub></span> for output is 6.</p>
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<p>Control performance of droop control method.</p>
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13 pages, 5435 KiB  
Article
Design, Analysis, and Comparison of Electric Vehicle Electric Oil Pump Motor Rotors Using Ferrite Magnet
by Huai-Cong Liu
World Electr. Veh. J. 2025, 16(1), 50; https://doi.org/10.3390/wevj16010050 - 20 Jan 2025
Viewed by 101
Abstract
With the recent proliferation of electric vehicles, there is increasing attention on drive motors that are powerful and efficient, with a higher power density. To meet such high power density requirements, the cooling technology used for drive motors is particularly important. To further [...] Read more.
With the recent proliferation of electric vehicles, there is increasing attention on drive motors that are powerful and efficient, with a higher power density. To meet such high power density requirements, the cooling technology used for drive motors is particularly important. To further optimize the cooling effects, the use of direct oil-cooling technology for drive motors is gaining more attention, especially regarding the requirements for electric vehicle electric oil pumps (EOPs) in motor cooling. In such high-temperature environments, it is also necessary for the EOP to maintain its performance under high temperatures. This research explores the feasibility of using high-temperature-resistant ferrite magnets in the rotors of EOPs. For a 150 W EOP motor with the same stator size, three different rotor configurations are proposed: a surface permanent magnet (SPM) rotor, an interior permanent magnet (IPM) rotor, and a spoke-type IPM rotor. While the rotor sizes are the same, to maximize the power density while meeting the rotor’s mechanical strength requirements, the different rotor configurations make the most use of ferrite magnets (weighing 58 g, 51.8 g, and 46.3 g, respectively). Finite element analysis (FEA) was used to compare the performance of these models with that of the basic rotor design, considering factors such as the no-load back electromotive force, no-load voltage harmonics (<10%), cogging torque (<0.1 Nm), load torque, motor loss, and efficiency (>80%). Additionally, a comprehensive analysis of the system efficiency and energy loss was conducted based on hypothetical electric vehicle traction motor parameters. Finally, by manufacturing a prototype motor and conducting experiments, the effectiveness and superiority of the finite element method (FEM) design results were confirmed. Full article
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<p>A diagram of the direct cooling of the end-winding in an oil-cooling drive motor for electric vehicles, reprinted with permission from Ref [<a href="#B20-wevj-16-00050" class="html-bibr">20</a>]. Copyright 2020 Hyundai-transys.</p>
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<p>The three-phase MMF factor for the three pole–slot combinations, (<b>a</b>) 10/12, (<b>b</b>) 8/12, and (<b>c</b>) 14/12.</p>
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<p>Three different shapes of ferrite magnet rotors: (<b>a</b>) model 1 (SPM with sleeve), (<b>b</b>) model 2 (spoke-type IPM), (<b>c</b>) model 3 (IPM).</p>
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<p>(<b>a</b>) The phase B-EMF of the three models. (<b>b</b>) The FFT analysis of the three models. (<b>c</b>) The cogging torque for the three models.</p>
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<p>FEM torque value at different current angles (phase current Ia: 12 arms).</p>
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<p>Cross section and flux density distributions of three models in MPTA condition. (<b>a</b>) Model 1, load condition (Ia: 12 arms; β: 0°). (<b>b</b>) Model 2, load condition (Ia: 12 arms; β: 15°). (<b>c</b>) Model 3, load condition (Ia: 12 arms; β: 35°).</p>
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<p>Comparison of torque and power according to speed.</p>
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<p>Efficiency maps of three models: (<b>a</b>) model 1; (<b>b</b>) model 2; (<b>c</b>) model 3.</p>
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<p>(<b>a</b>) The motor speed and (<b>b</b>) absolute load torque over the WLTP class 3 driving cycle, reprinted from Ref. [<a href="#B23-wevj-16-00050" class="html-bibr">23</a>].</p>
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<p>(<b>a</b>) The EOP motor speed and (<b>b</b>) absolute EOP motor torque over the WLTP class 3 driving cycle.</p>
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<p>(<b>a</b>) EOP motor specification for peak torque versus speed characteristics (all models); (<b>b</b>) loss over WLTP class 3 for model 1 and model 2.</p>
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<p>The prototype of the SPM with a ferrite magnet for the EOP.</p>
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<p>Experiment and simulation results of no-load line induced voltage at 1000 r/min. (<b>a</b>) Experiment. (<b>b</b>) Simulation. (<b>c</b>) Experiment results of cogging torque, reprinted with permission from Ref. [<a href="#B25-wevj-16-00050" class="html-bibr">25</a>]. Copyright 2020 IEEE.</p>
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26 pages, 16943 KiB  
Article
Nu—A Marine Life Monitoring and Exploration Submarine System
by Ali A. M. R. Behiry, Tarek Dafar, Ahmed E. M. Hassan, Faisal Hassan, Abdullah AlGohary and Mounib Khanafer
Technologies 2025, 13(1), 41; https://doi.org/10.3390/technologies13010041 - 20 Jan 2025
Viewed by 163
Abstract
Marine life exploration is constrained by factors such as limited scuba diving time, depth restrictions for divers, costly expeditions, safety risks to divers’ health, and minimizing harm to marine ecosystems, where traditional diving often risks disturbing marine life. This paper introduces Nu (named [...] Read more.
Marine life exploration is constrained by factors such as limited scuba diving time, depth restrictions for divers, costly expeditions, safety risks to divers’ health, and minimizing harm to marine ecosystems, where traditional diving often risks disturbing marine life. This paper introduces Nu (named after an ancient Egyptian deity), a 3D-printed Remotely Operated Underwater Vehicle (ROUV) designed in an attempt to address these challenges. Nu employs Long Range (LoRa), a low-power and long-range communication technology, enabling wireless operation via a manual controller. The vehicle features an onboard live-feed camera with a separate communication system that transmits video to an external real-time machine learning (ML) pipeline for fish species classification, reducing human error by taxonomists. It uses Brushless Direct Current (BLDC) motors for long-distance movement and water pump motors for precise navigation, minimizing disturbance, and reducing damage to surrounding species. Nu’s functionality was evaluated in a controlled 2.5-m-deep body of water, focusing on connectivity, maneuverability, and fish identification accuracy. The fish detection algorithm achieved an average precision of 60% in identifying fish presence, while the classification model achieved 97% precision in assigning species labels, with unknown species flagged correctly. The testing of Nu in a controlled environment has met the system design expectations. Full article
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<p>ROUV system model.</p>
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<p>Three-dimensional-designed parts of the ROUV’s body: (<b>a</b>) Exterior body piece used to hold the WTC. (<b>b</b>) Component holder to house the components inside the WTC. (<b>c</b>) End-cap design to seal the WTC. (<b>d</b>) Syringe holder design.</p>
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<p>Full 3D design assembly simulation.</p>
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<p>Printing structure of FDM printers [<a href="#B35-technologies-13-00041" class="html-bibr">35</a>].</p>
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<p>Controller circuit diagram.</p>
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<p>ROUV circuit.</p>
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<p>ROUV camera system.</p>
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<p>ROUV assembled.</p>
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<p>ROUV operating underwater.</p>
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<p>Validation batch: labels and predictions. (<b>a</b>) Validation batch labels. (<b>b</b>) Validation batch predictions.</p>
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<p>Confusion matrix.</p>
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<p>Training and validation loss and accuracy curves. (<b>a</b>) Loss learning curve. (<b>b</b>) Accuracy learning curve.</p>
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<p>Pipeline classification testing: (<b>a</b>) High-quality images. (<b>b</b>) Low-quality images (tested using the onboard camera).</p>
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12 pages, 4475 KiB  
Article
High-Q Resonances Induced by Toroidal Dipole Bound States in the Continuum in Terahertz Metasurfaces
by Lincheng Guo and Yachen Gao
Crystals 2025, 15(1), 96; https://doi.org/10.3390/cryst15010096 (registering DOI) - 20 Jan 2025
Viewed by 160
Abstract
The radiation mode of the interaction between electromagnetic waves and materials has always been a research hotspot in nanophotonics, and bound states in the continuum (BICs) belong to one of the nonradiative modes. Owing to their high-quality factor characteristics, BICs are extensively employed [...] Read more.
The radiation mode of the interaction between electromagnetic waves and materials has always been a research hotspot in nanophotonics, and bound states in the continuum (BICs) belong to one of the nonradiative modes. Owing to their high-quality factor characteristics, BICs are extensively employed in nonlinear harmonic generators and sensors. Here, the influence of structural parameters on radiation modes has been systematically analyzed using band theory; the mechanisms of quasi-BIC mode and BIC mode were also analyzed through multipole decomposition of scattered power and near-field distribution. Notably, this study presents the discovery that the toroidal dipole-BIC (TD-BIC) arises from the interference and cancellation of electric and toroidal dipoles. The research results indicate that the structure, which supports symmetry-protected BICs, is sensitive to variations in the concentration of NaCl solution in its surroundings, making it applicable for liquid detection in miniaturized metal sensors. The proposed scheme broadens the applicability of BIC-based sensors and provides a prospective platform for biological and chemical sensing. Full article
(This article belongs to the Special Issue Organic Photonics: Organic Optical Functional Materials and Devices)
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<p>(<b>a</b>) Schematic of the DSRR under the THz wave illumination. (<b>b</b>) Detailed diagram of the unit structure of metamaterials.</p>
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<p>(<b>a</b>) Simulated spectra of the ideal DSRR composed of PEC and realistic metallic (Al) with varying structural parameters <span class="html-italic">g</span><sub>2</sub>. (<b>b</b>) Simulated transmittance spectra map of the DSRR for various <span class="html-italic">g</span><sub>2</sub>. (<b>c</b>) The band structure and radiative Q-factor of the DSRR structure at gap sizes of 4 μm. (<b>d</b>) The curve shows the change in the radiative Q-factor with variations in the asymmetry parameter <span class="html-italic">α</span> at the Γ-point, depicted in logarithmic plots.</p>
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<p>(<b>a</b>) The total scattering power. (<b>b</b>) The scattering powers of different multipoles including ED, MD, TD, EQ, and MQ in the Cartesian coordinate system. In the cases of (<b>c</b>) <span class="html-italic">g</span><sub>2</sub> = 4 μm and (<b>d</b>) <span class="html-italic">g</span><sub>2</sub> = 10 μm, scattering direction diagrams between ED and TD and radiation power diagrams between ED<sub>x</sub>−ik<sub>0</sub>TD<sub>x</sub> were plotted, respectively.</p>
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<p>Electromagnetic field distribution of BIC (<b>a</b>,<b>b</b>) and quasi-BIC (<b>c</b>,<b>d</b>). The green, red, blue, and black arrows represent the directions of ED, MD, TD, and surface current, respectively.</p>
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<p>(<b>a</b>) Schematic diagram of NaCl concentration solution sensor. (<b>b</b>,<b>c</b>) Simulated spectra versus the refractive index of liquid. (<b>d</b>) Refractive index sensitivity curve of frequency versus surrounding liquid concentration. (<b>e</b>) Figure of merit as a function of the liquid’s refractive index.</p>
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20 pages, 3595 KiB  
Article
Integration of a Heterogeneous Battery Energy Storage System into the Puducherry Smart Grid with Time-Varying Loads
by M A Sasi Bhushan, M. Sudhakaran, Sattianadan Dasarathan and Mariappane E
Energies 2025, 18(2), 428; https://doi.org/10.3390/en18020428 - 19 Jan 2025
Viewed by 498
Abstract
A peak shaving approach in selected industrial loads helps minimize power usage during high demand hours, decreasing total energy expenses while improving grid stability. A battery energy storage system (BESS) can reduce peak electricity demand in distribution networks. Quasi-dynamic load flow analysis (QLFA) [...] Read more.
A peak shaving approach in selected industrial loads helps minimize power usage during high demand hours, decreasing total energy expenses while improving grid stability. A battery energy storage system (BESS) can reduce peak electricity demand in distribution networks. Quasi-dynamic load flow analysis (QLFA) accurately assesses the maximum loading conditions in distribution networks by considering factors such as load profiles, system topology, and network constraints. Achieving maximum peak shaving requires optimizing battery charging and discharging cycles based on real-time energy generation and consumption patterns. Seamless integration of battery storage with solar photovoltaic (PV) systems and industrial processes is essential for effective peak shaving strategies. This paper proposes a model predictive control (MPC) scheme that can effectively perform peak shaving of the total industrial load. Adopting an MPC-based algorithm design framework enables the development of an effective control strategy for complex systems. The proposed MPC methodology was implemented and tested on the Indian Utility 29 Node Distribution Network (IU29NDN) using the DIgSILENT Power Factory environment. Additionally, the analysis encompasses technical and economic results derived from a simulated storage operation and, taking Puducherry State Electricity Department tariff details, provides significant insights into the application of this method. Full article
(This article belongs to the Section F: Electrical Engineering)
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<p>Block diagram of a distribution network with PV-BESS.</p>
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<p>Proposed model predictive control.</p>
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<p>Single-line diagram of an IU29NDN model for the smart grid of Puducherry in India.</p>
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<p>Electricity load profile of IU29NDN in summer season.</p>
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<p>Electricity load profile of IU29NDN in monsoon season.</p>
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<p>Electricity load profile of IU29NDN in winter season.</p>
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<p>One-week averaged load profile of IU29NDN.</p>
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<p>Expanded peak load regions and discharge-power curves for BESS control.</p>
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<p>Flow chart of PV-BESS for control and determination.</p>
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<p>Limitation of BESS by the battery available energy for (<b>a</b>) summer, (<b>b</b>) monsoon, and (<b>c</b>) winter.</p>
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<p>Numerous experimental results of peak load shaving during (<b>a</b>) summer, (<b>b</b>) monsoon, and (<b>c</b>) winter seasons.</p>
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<p>Battery power profiles for (<b>a</b>) summer, (<b>b</b>) monsoon, and (<b>c</b>) winter.</p>
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<p>Battery power profiles for (<b>a</b>) summer, (<b>b</b>) monsoon, and (<b>c</b>) winter.</p>
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<p>Simulation Diagram of the IU29NDN Modeled in DIgSILENT Power Factory v15.1.7.</p>
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12 pages, 3649 KiB  
Article
Enhancing Thermoelectric Performance: The Impact of Carbon Incorporation in Spin-Coated Al-Doped ZnO Thin Films
by Alberto Giribaldi, Cristiano Giordani, Giovanna Latronico, Cédric Bourgès, Takahiro Baba, Cecilia Piscino, Maya Marinova, Takao Mori, Cristina Artini, Hannes Rijckaert and Paolo Mele
Coatings 2025, 15(1), 107; https://doi.org/10.3390/coatings15010107 (registering DOI) - 19 Jan 2025
Viewed by 219
Abstract
In the present study, for the first time, aluminum-doped zinc oxide (AZO) thin films with nanoinclusions of amorphous carbon have been synthesized via spin coating, and the thermoelectric performances were investigated varying the aging period of the solution, the procedure of carbon nanoparticles’ [...] Read more.
In the present study, for the first time, aluminum-doped zinc oxide (AZO) thin films with nanoinclusions of amorphous carbon have been synthesized via spin coating, and the thermoelectric performances were investigated varying the aging period of the solution, the procedure of carbon nanoparticles’ addition, and the annealing atmosphere. The addition of nanoparticles has been pursued to introduce phonon scattering centers to reduce thermal conductivity. All the samples showed a strong orientation along the [002] crystallographic direction, even though the substrate is amorphous silica, with an intensity of the diffraction peaks reaching its maximum in samples annealed in the presence of hydrogen, and generally decreasing by the addition of carbon nanoparticles. Absolute values of the Seebeck coefficient improve when nanoparticles are added. At the same time, electric conductivity is higher for the sample with 1 wt.% of carbon and annealed in Ar with 1% of H2, both increasing in absolute value with the temperature rise. Among all the samples, the lowest thermal conductivity value of 1.25 W/(m∙K) was found at room temperature, and the highest power factor was 111 μW/(m∙K2) at 325 °C. Thus, the introduction of carbon effectively reduced thermal conductivity, while also increasing the power factor, giving promising results for the further development of AZO-based materials for thermoelectric applications. Full article
(This article belongs to the Special Issue Advances in Novel Coatings)
22 pages, 1218 KiB  
Article
Electric Vehicles Charging Scheduling Strategy Based on Time Cost of Users and Spatial Load Balancing in Multiple Microgrids
by Jiaqi Zhang, Yongxiang Xia, Zhongyi Cheng and Xi Chen
World Electr. Veh. J. 2025, 16(1), 46; https://doi.org/10.3390/wevj16010046 - 19 Jan 2025
Viewed by 156
Abstract
In a sustainable energy system, managing the charging demand of electric vehicles (EVs) becomes increasingly critical. Uncontrolled charging behaviors of large-scale EV fleets will exacerbate loads imbalanced in a multi-microgrid (MMG). At the same time, the time cost of users will increase significantly. [...] Read more.
In a sustainable energy system, managing the charging demand of electric vehicles (EVs) becomes increasingly critical. Uncontrolled charging behaviors of large-scale EV fleets will exacerbate loads imbalanced in a multi-microgrid (MMG). At the same time, the time cost of users will increase significantly. To improve users’ charging experience and ensure stable operation of the MMG, we propose a new joint scheduling strategy that considers both time cost of users and spatial load balancing among MMGs. The time cost encompasses many factors, such as traveling time, queue waiting time, and charging time. Meanwhile, spatial load balancing seeks to mitigate the impact of large-scale EV charging on MMG loads, promoting a more equitable distribution of power resources across the MMG system. Compared to the Shortest Distance Matching Strategy (SDMS) and the Time Minimum Matching Strategy (TMMS) methods, our approach improves the average peak-to-valley ratio by 9.5% and 10.2%, respectively. Similarly, compared to the Load Balancing Matching Strategy (LBMS) and the Improved Load Balancing Matching Strategy (ILBMS) methods, our approach reduces the average time cost by 31.8% and 25% while maintaining satisfactory spatial load balancing. These results demonstrate that the proposed method achieves good results in handling electric vehicle scheduling problems. Full article
(This article belongs to the Special Issue Electric Vehicles and Smart Grid Interaction)
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<p>Schematic diagram of charging aggregator in microgrid.</p>
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<p>Multi-microgrids.</p>
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<p>The charging curve of battery.</p>
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<p>The time cost of a vehicle.</p>
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<p>MTC-SLBMS algorithm flowchart.</p>
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<p>Road network.</p>
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<p>Traffic flows at different time points.</p>
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<p>Comparison of average time cost under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Comparison of average valley-to-peak ratio under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Comparison of composite index(CI) under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Average valley-to-peak ratio under different participation (<span class="html-italic">C</span> = 50).</p>
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<p>MG load curve under different strategies (<span class="html-italic">N</span> = 1500 and <span class="html-italic">C</span> = 50).</p>
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<p>Comparison of the number of vehicles in each charging station under different strategies (<span class="html-italic">C</span> = 50).</p>
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<p>Comparison of average time cost under different charging station capacities.</p>
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<p>Comparison of average valley-to-peak ratio under different charging station capacities.</p>
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26 pages, 5499 KiB  
Article
Current Controlled AC/DC Converter and Its Performance—A Mathematical Model
by Jan Iwaszkiewicz, Piotr Mysiak and Adam Muc
Energies 2025, 18(2), 419; https://doi.org/10.3390/en18020419 - 18 Jan 2025
Viewed by 517
Abstract
This paper describes a mathematical model of the AC/DC converter. The analytic expressions define fundamental physical variables of the converter and their relations: phase current and voltage, shift angle between these quantities, power factor, and supply voltage UD. The mains voltage [...] Read more.
This paper describes a mathematical model of the AC/DC converter. The analytic expressions define fundamental physical variables of the converter and their relations: phase current and voltage, shift angle between these quantities, power factor, and supply voltage UD. The mains voltage is defined as a digitalized sine wave while the current’s wave takes the form of a line segment defined in an appropriate time interval. The model permits the description of two modes of operation: inverter and rectifier. The assumed control method of the converter depends on the successive switching of selected vectors. They are qualified according to the principle of the lowest error between the reference and measured phase current value. The control method is realized by using hysteresis algorithms. Five different algorithm solutions and comparative results are implemented. Several examples of current, voltage, and vectors taken during the simulation and experimental works are executed. Full article
(This article belongs to the Special Issue Measurement Systems for Electric Machines and Motor Drives)
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<p>Model of PWM mains converter.</p>
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<p>Control system with three analog error comparators.</p>
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<p>Control system with three error comparators activated periodically.</p>
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<p>Control system for Algorithm A3 implementation.</p>
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<p>Waveforms of inverter phase currents and voltage vectors for hysteresis Algorithms A1 (<b>a</b>) and A2 (<b>b</b>).</p>
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<p>Waveforms of inverter phase currents and voltage vectors for hysteresis Algorithms A1 (<b>a</b>) and A2 (<b>b</b>).</p>
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<p>Waveforms of inverter phase currents and voltage vectors for hysteresis Algorithms A3 (<b>a</b>) and A4 (<b>b</b>).</p>
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<p>Waveforms of inverter phase currents and voltage vectors for hysteresis Algorithms A3 (<b>a</b>) and A4 (<b>b</b>).</p>
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<p>Waveforms of inverter phase currents and voltage vectors for hysteresis Algorithm A5.</p>
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<p>Phase current <span class="html-italic">i<sub>a</sub></span>, electromotive force <span class="html-italic">e<sub>a</sub></span>, inverter output phase voltage <span class="html-italic">U<sub>ak</sub></span> (<b>a</b>), and inverter voltage vectors <span class="html-italic">V<sub>k</sub></span><sub>,</sub> (<b>b</b>) obtained for the control model according to the discretized Algorithm A5; the assumed sampling period <span class="html-italic">T<sub>p</sub></span> = 100 µs. (Zero vectors <span class="html-italic">V<sub>k</sub></span> = 7(111) marked with number −1).</p>
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<p>Illustration of dynamic properties of the inverter controlled according to the hysteresis Algorithm A1 based on the phase current waveforms obtained at step change of the set value of the current (<b>a</b>), inverter voltage vectors <span class="html-italic">V<sub>k</sub></span>, (<b>b</b>) (zero vectors <span class="html-italic">V<sub>k</sub></span> = 7(111) marked with number −1).</p>
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<p>Three modes of converter operation are controlled according to Algorithm A5: inverter operation, synchronous operation (the set current frequency <span class="html-italic">f</span> = 0), and rectifier operation: (<b>a</b>) three-phase currents, (<b>b</b>) average current value <span class="html-italic">i<sub>D</sub></span>.</p>
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<p>System for experimental tests.</p>
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<p>AC-DC-AC converter connected to the network.</p>
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<p>Illustration of rectifier operation of the mains converter controlled according to the hysteresis algorithm: waveforms of phase currents <span class="html-italic">i<sub>f</sub></span>, the average value of intermediate circuit current <span class="html-italic">i<sub>D</sub></span>, network voltage <span class="html-italic">e<sub>f</sub></span> (<b>a</b>), and vector <span class="html-italic">V<sub>k</sub></span> (<b>b</b>).</p>
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<p>Illustration of inverter operation of the mains converter controlled according to the hysteresis algorithm: waveforms of phase currents <span class="html-italic">i<sub>f</sub></span>, average value of intermediate circuit current <span class="html-italic">i<sub>D</sub></span>, network voltage <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>e</mi> </mrow> <mrow> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math> (<b>a</b>), and vector <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>k</mi> </mrow> </msub> </mrow> </semantics></math> (<b>b</b>).</p>
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<p>Simulated waveforms of AC-DC-AC converter: MR converter works as a rectifier, while MI converter as an inverter. For both converters, the power factor |<span class="html-italic">cosφ</span>| = 1.</p>
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<p>Simulated waveforms of AC-DC-AC converter in situation when the machine converter FM works as an inverter with phase shift <span class="html-italic">ϕ</span> = <span class="html-italic">π</span>/2.</p>
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<p>Three converter structures of the laboratory model used for experimental tests: (<b>a</b>) frequency converter, (<b>b</b>) mains converter, (<b>c</b>) intermediate converter.</p>
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<p>Mains converter phase currents and voltages and spectrum of current harmonics for phase shift angle <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>π</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo> </mo> </mrow> </semantics></math> (<b>a</b>) and 0 (<b>b</b>).</p>
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<p>Mains converter phase currents and voltages and spectrum of current harmonics for phase shift angle <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mi>π</mi> </mrow> <mrow> <mn>2</mn> </mrow> </mfrac> </mstyle> <mo> </mo> </mrow> </semantics></math> (<b>a</b>) and <span class="html-italic">π</span> (<b>b</b>).</p>
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21 pages, 651 KiB  
Article
A Comparative Study of Incremental ΔΣ Analog-to-Digital Converter Architectures with Extended Order and Resolution
by Monica Aziz, Paul Kaesser, Sameh Ibrahim and Maurits Ortmanns
Electronics 2025, 14(2), 372; https://doi.org/10.3390/electronics14020372 - 18 Jan 2025
Viewed by 298
Abstract
Incremental Delta-Sigma (I-DS) analog-to-digital converters (ADCs) are one of the best candidates for integrated sensor interface systems when it comes to high resolution and power efficiency. Advanced architectures such as Multistage noise shaping (MASH) or extended counting (EC) I-DS ADCs can be used [...] Read more.
Incremental Delta-Sigma (I-DS) analog-to-digital converters (ADCs) are one of the best candidates for integrated sensor interface systems when it comes to high resolution and power efficiency. Advanced architectures such as Multistage noise shaping (MASH) or extended counting (EC) I-DS ADCs can be used to achieve a high resolution and fast conversion times and avoid stability issues. Different architectures have been proposed in the state of the art (SoA), but there exists no extensive quantitative or qualitative comparison between them. This manuscript fills this gap by providing a detailed system-level comparison between MASH, EC, and other architectural options in I-DS ADCs, where different performances between these architectures are realized depending on the employed oversampling ratio (OSR) and the chosen number of quantizer bits. Also, for specific MASH designs, the appropriate choice of the digital filter improves the SQNR. The advantages, disadvantages, and limitations of the different architectures are presented including non-idealities such as coefficient mismatch showing that 2-1 MASH-LI is less sensitive to mismatch and provides a high maximum stable amplitude (MSA) relative to the simulated architectures. Furthermore, the 2-1 EC achieves good results and comes with the advantage of a lower noise penalty factor compared to the MASH architectures. This work is intended to assist designers in selecting the most appropriate enhanced I-DS MASH architecture for their specific requirements and applications. Full article
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<p>(<b>a</b>) Multi-stage/-step I-DS ADC with three variants of requantization and (<b>b</b>) its timing diagram including the reset.</p>
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<p>(<b>a</b>) Block diagram of an exemplary incremental 2-1 MASH modulator with digital cancellation logic and reconstruction filter. The red dashed line indicates QE extraction from the first-stage quantizer (MASH-QE). The blue dashed line indicates the extraction of the QE from the last integrator output (MASH-LI) and (<b>b</b>) its timing diagram, including the reset.</p>
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<p>(<b>a</b>) Block diagram of an incremental 2-1 EC (Extended Counting) modulator with reconstruction filters and (<b>b</b>) its timing diagram, including the reset.</p>
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<p>Simulated SQNR of 2-0 and 2-1 MASH-QE, LI and EC at an OSR of 60. First stage: 3-bit quantizer. Second stage: 8-bit quantizer (2-0) or 4-bit quantizer (2-1).</p>
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<p>Simulated SQNR of 2-0 and 2-1 MASH-QE, LI and EC at an OSR of 60 including limiter blocks after each integrator and after the adder. First stage: 3-bit quantizer. Second stage: 8-bit quantizer (2-0) or 4-bit quantizer (2-1).</p>
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<p>Histogram of the swing at the output of the adder (before the limiter) at an input of −6 dBFS and at an input of −3 dBFS, respectively.</p>
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<p>Histogram of the swing at the last integrator output and the last sample of the last integrator output at an input amplitude of −3 dBFS, respectively.</p>
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<p>Simulated SQNR of 2-0 and 2-1 MASH-QE, LI and EC at an OSR of 60. An inter-stage gain of 6 is used for all the architectures. First stage: 3-bit quantizer. Second stage: 8-bit quantizer (2-0) or 4-bit quantizer (2-1).</p>
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<p>Simulated SQNR of 2-0 and 2-1 MASH-QE, LI, and EC at an input amplitude of −6 dBFS sinusoidal signal. An inter-stage gain of 6 is used for all the architectures. First stage: 3-bit quantizer. Second stage: 8-bit quantizer (2-0) or 4-bit quantizer (2-1).</p>
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<p>Simulated SQNR of 2-0 and 2-1 MASH-QE, LI and EC at an OSR of 100 and with limiter blocks included. First stage: 1-bit quantizer. Second stage: 8-bit quantizer (2-0) or 4-bit quantizer (2-1). The inter-stage gain is 1 for all architectures.</p>
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<p>NTFs of the exemplary 2-0 MASH-LI for the two different versions of the error cancellation logic <span class="html-italic">ECL</span><sub>LI,1</sub> and <span class="html-italic">ECL</span><sub>LI,2</sub>. Solid: single-bit quantizer in first stage and OSR = 100. Dashed: 3-bit quantizer in first stage and OSR = 60. The second stage is an 8-bit quantizer.</p>
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<p>Digital filter weights of the output of the second stage (<math display="inline"><semantics> <mrow> <msub> <mi>H</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <mi>z</mi> <mo>)</mo> </mrow> <mo>·</mo> <mrow> <msub> <mi>H</mi> <mrow> <mi>rec</mi> </mrow> </msub> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math>) in the case of the 2-0 MASH-LI at an OSR of 100. The first stage is scaled with the single-bit coefficients of <a href="#electronics-14-00372-t001" class="html-table">Table 1</a>. (<b>a</b>) shows the weights when <math display="inline"><semantics> <mrow> <msub> <mi>H</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> is designed after <span class="html-italic">ECL</span><sub>LI,1</sub> and (<b>b</b>) for <span class="html-italic">ECL</span><sub>LI,2</sub>.</p>
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<p>Simulated mean and distribution of SQNR of the exemplary 2-0 MASH-QE, 2-0 MASH-LI and 2-0 EC architectures over the variation of the analog coefficients <math display="inline"><semantics> <msub> <mi>σ</mi> <mi>c</mi> </msub> </semantics></math> in percent at an input amplitude of −6 dBFS sinusoidal signal. OSR = 60, 3-bit first-stage and 8-bit second-stage quantizers, g = 6.</p>
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<p>Simulated mean and distribution of SQNR of the exemplary 2-1 MASH-QE, 2-1 MASH-LI, and 2-1 EC architectures at −6 dBFS sinusoidal input signal over the variation of analog coefficients with standard deviation <math display="inline"><semantics> <msub> <mi>σ</mi> <mi>c</mi> </msub> </semantics></math>. OSR = 60, 3-bit first stage and 4-bit second stage quantizers, g = 6.</p>
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<p>Simulated SQNR of 2-0 and 2-1 MASH-QE, LI and EC at an OSR of 60. First stage: 3-bit quantizer. Second stage: 8-bit quantizer (2-0) or 4-bit quantizer (2-1). The input is −6 dBFS sinusoidal signal and g = 6.</p>
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14 pages, 7813 KiB  
Article
Effects of Two-Stage Injection on Combustion and Particulate Emissions of a Direct Injection Spark-Ignition Engine Fueled with Methanol–Gasoline Blends
by Miaomiao Zhang and Jianbin Cao
Energies 2025, 18(2), 415; https://doi.org/10.3390/en18020415 - 18 Jan 2025
Viewed by 282
Abstract
Methanol is widely recognized as a promising alternative fuel for achieving carbon neutrality in internal combustion engines. Its use in direct injection spark-ignition (DISI) engines, either as pure methanol or blended fuels, has demonstrated improvements in thermal efficiency and reductions in certain gaseous [...] Read more.
Methanol is widely recognized as a promising alternative fuel for achieving carbon neutrality in internal combustion engines. Its use in direct injection spark-ignition (DISI) engines, either as pure methanol or blended fuels, has demonstrated improvements in thermal efficiency and reductions in certain gaseous pollutants. However, due to the complex influencing factors and the great harm to human health, its particulate emissions need to be further explored and controlled, which is also an inevitable requirement for the development of energy conservation and carbon reduction in internal combustion engines. This study explores the effects of two-stage injection strategies combined with fuel blending on the combustion characteristics, stability, and particulate emissions of DISI engines. By testing four methanol blending ratios and four injection ratios, the presented study identifies that M20 fuel with an 8:2 injection ratio achieves optimal combustion performance, stability, and increased indicated mean effective pressure. Furthermore, under low methanol blending ratios, the 8:2 injection ratio can reduce particulate number concentrations by approximately 20%. These findings suggest that a well-designed two-stage injection strategy combined with methanol–gasoline blends can effectively control particulate emissions while maintaining the power, efficiency, and combustion stability of DISI engines. Full article
(This article belongs to the Special Issue Optimization of Efficient Clean Combustion Technology)
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<p>Schematic of experimental setup [<a href="#B27-energies-18-00415" class="html-bibr">27</a>].</p>
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<p>Effects of two-stage injection on the flame development (<b>a</b>) and combustion duration (<b>b</b>) for methanol–gasoline blends.</p>
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<p>Effects of two-stage injection on the combustion center for methanol–gasoline blends.</p>
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<p>Changes in in-cylinder pressure and temperature under M20 (<b>a</b>) and 8:2 (<b>b</b>) conditions. The solid lines represent in-cylinder pressure and the dot lines represent in-cylinder temperature.</p>
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<p>Effects of two-stage injection on exhaust temperature for methanol–gasoline blends.</p>
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<p>Effects of two-stage injection on BSFC for methanol–gasoline blends.</p>
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<p>Box plots of peak in-cylinder pressure (<b>a</b>) and the corresponding crank angle (<b>b</b>) under M20 conditions.</p>
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<p>Box plots of peak in-cylinder pressure (<b>a</b>) and the corresponding crank angle (<b>b</b>) under 8:2 condition.</p>
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<p>Return maps between IMEP(i) and IMEP(i + 1) under M20 (<b>a</b>) and 8:2 (<b>b</b>) conditions.</p>
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<p>Effects of two-stage injection on COV<sub>IMEP</sub> for methanol–gasoline blends.</p>
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<p>Effects of two-stage injection on particulate emissions: (<b>a</b>) PN-Total; (<b>b</b>) PN-Nucleation mode; (<b>c</b>) PN-Accumulation mode.</p>
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<p>Effects of two-stage injection on particle size distribution under M20 (<b>a</b>) and 8:2 (<b>b</b>) conditions.</p>
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