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Search Results (1,743)

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Keywords = Matlab-Simulink model

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16 pages, 4716 KiB  
Article
Research on Water Flow Control Strategy for PEM Electrolyzer Considering the Anode Bubble Effect
by Liheng An, Yizhi Tian and Haikun Zhao
Energies 2025, 18(2), 273; https://doi.org/10.3390/en18020273 - 9 Jan 2025
Viewed by 267
Abstract
At higher current densities, the bubble effect in the anode flow field of the PEM electrolyzer (PEM EL) worsens mass transfer losses and energy consumption. This study employs a moderate increase in the water flow rate to remove accumulated bubbles under fluctuating electrical [...] Read more.
At higher current densities, the bubble effect in the anode flow field of the PEM electrolyzer (PEM EL) worsens mass transfer losses and energy consumption. This study employs a moderate increase in the water flow rate to remove accumulated bubbles under fluctuating electrical input, thereby improving PEM EL system efficiency. An enhanced PEM EL equivalent circuit model incorporating bubble over-potential based on the oxygen volume fraction is developed. Considering the energy consumption of auxiliary equipment and the reduction in losses from mitigating the bubble effect, a numerical simulation evaluates the impact of flow rate variations on overall electrolysis energy consumption, leading to a comprehensive energy consumption model for the PEM EL system, incorporating electrical, chemical, and thermal energy conversions. The control objective is to maximize system efficiency by optimizing the water flow rate, with a performance-preset-based controller implemented in MATLAB/Simulink. The simulation results show that the controller can accurately track the target flow rate, and the dynamic regulation time improved by 1.5 s compared to the traditional performance constraint function, better matching the rate of change in electrical energy. Under the water flow control mode, hydrogen production increased by 6.6 L within 130 s of the simulation, available energy increased by 8.32 × 106 J, and the efficiency of the PEM EL system improved by 2.79%. Full article
(This article belongs to the Section A5: Hydrogen Energy)
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<p>PEM EL geometric model.</p>
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<p>Comparison of simulation and literature experimental results [<a href="#B15-energies-18-00273" class="html-bibr">15</a>].</p>
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<p>The impact of water flow rate in the anode CL (2 V, 338.15 K). (<b>a</b>) Oxygen volume fraction; (<b>b</b>) volumetric current density.</p>
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<p>Temperature in the anode CL.</p>
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<p>Revised Equivalent Circuit Diagram of the PEM EL.</p>
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<p>Schematic of the PEM EL System Structure.</p>
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<p>Process of operating point variation in the PEM EL under changing power conditions.</p>
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<p>Control flowchart of the PEM EL.</p>
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<p>Racking error during water flow rate increase under two performance functions. (<b>a</b>) Under <span class="html-italic">P</span>(<span class="html-italic">t</span>). (<b>b</b>) Under <span class="html-italic">P</span><sub>new</sub>(<span class="html-italic">t</span>).</p>
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<p>Comparison of flow-tracking error.</p>
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<p>Input power of the PEM EL System.</p>
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<p>Performance comparison of the PEM EL system under variable power input. (<b>a</b>) Comparison: operating voltage. (<b>b</b>) Comparison: operating current. (<b>c</b>) Comparison: hydrogen production. (<b>d</b>) Comparison: hydrogen high heat value.</p>
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<p>Energy consumption and efficiency analysis: (<b>a</b>) comparison of system efficiency in the two modes. (<b>b</b>) energy consumption of each device in flow control mode.</p>
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22 pages, 6085 KiB  
Article
A Sliding Mode Approach to Vector Field Path Following for a Fixed-Wing UAV
by Luca Pugi, Lorenzo Franchi, Samuele Favilli and Giuseppe Mattei
Robotics 2025, 14(1), 7; https://doi.org/10.3390/robotics14010007 - 9 Jan 2025
Viewed by 241
Abstract
Unmanned aerial vehicle (UAV) technology has recently experienced increasing development, leading to the creation of a wide variety of autonomous solutions. In this paper, a guidance strategy for straight and orbital paths following fixed-wing small UAVs is presented. The proposed guidance algorithm is [...] Read more.
Unmanned aerial vehicle (UAV) technology has recently experienced increasing development, leading to the creation of a wide variety of autonomous solutions. In this paper, a guidance strategy for straight and orbital paths following fixed-wing small UAVs is presented. The proposed guidance algorithm is based on a reference vector field as desired, with 16 courses for the UAV to follow. A sliding mode approach is implemented to improve the robustness and effectiveness, and the asymptotic convergence of the aircraft to the desired trajectory in the presence of constant wind disturbances is proved according to Lyapunov. The algorithm exploits the banking dynamics and generates reference signals for the inner-loop aileron control. A MATLAB&Simulink® simulation environment is used to verify the performance and robustness of the compared guidance algorithms. This high-fidelity model considers the six-degrees-of-freedom (DoF) whole-flight dynamics of the UAV and it is based on experimental flight test data to implement the aerodynamic behavior. Full article
(This article belongs to the Section Aerospace Robotics and Autonomous Systems)
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<p>Guidance, Navigation and Control scheme of the proposed UAV.</p>
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<p>Definition of flight angles and speed relations.</p>
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<p>Straight line guidance problem.</p>
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<p>Orbit path guidance problem.</p>
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<p>Calculated vector fields of <span class="html-italic">χ<sub>des</sub></span> for an example of straight path (<b>a</b>) and for an example of orbit path (<b>b</b>).</p>
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<p>Propulsion (<b>a</b>), power management layout (<b>b</b>) [<a href="#B17-robotics-14-00007" class="html-bibr">17</a>] and corresponding Matlab-Simulink simulation model (<b>c</b>).</p>
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<p>Efficiency of installed ICE [<a href="#B17-robotics-14-00007" class="html-bibr">17</a>].</p>
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<p>Comparison of vector field algorithms, (<b>a</b>) without wind disturbance, (<b>b</b>) with a fixed crosswind disturbance of 9 [m/s].</p>
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<p>Comparison of heading (<b>a</b>) and course VF control (<b>b</b>) in the presence of wind disturbances.</p>
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<p>Comparison of course-based control algorithms in a high-wind scenario.</p>
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<p>Different closed paths with polygonal shape (<b>a</b>), example of simulation performed with an octagonal one (<b>b</b>).</p>
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<p>Max transversal error <span class="html-italic">d</span> measured after the turn on different waypoints with various path control algorithms (<b>a</b>–<b>c</b>), and corresponding poles approximating residual oscillations after each turn (<b>d</b>).</p>
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<p>Orbit geometry and path planning in transition scenario.</p>
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<p>Comparison of transition techniques.</p>
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12 pages, 18318 KiB  
Article
Performance Analysis of a Synchronous Reluctance Generator with a Slitted-Rotor Core for Off-Grid Wind Power Generation
by Samuel Adjei-Frimpong and Mbika Muteba
Electricity 2025, 6(1), 2; https://doi.org/10.3390/electricity6010002 - 8 Jan 2025
Viewed by 278
Abstract
In this paper, the performance of a Dual-Stator Winding Synchronous Reluctance Generator (SynRG) suitability for off-grid wind power generation is analyzed. The rotor of the SynRG has a slitted-rotor core to improve selected vital performance parameters. The SynRG with a slitted-rotor core was [...] Read more.
In this paper, the performance of a Dual-Stator Winding Synchronous Reluctance Generator (SynRG) suitability for off-grid wind power generation is analyzed. The rotor of the SynRG has a slitted-rotor core to improve selected vital performance parameters. The SynRG with a slitted-rotor core was modeled using a two-dimensional (2D) Finite Element Method (FEM) to study the electromagnetic performance of key parameters of interest. To validate the FEA results, a prototype of the SynRG with a slitted rotor was tested in the laboratory for no-load operation and load operation for unity, lagging, and leading power factors. To evaluate the capability of the SynRG with a slitted-rotor core to operate in a wind turbine environment, the machine was modeled and simulated in Matlab/Simulink (R2023a) for dynamic responses. The FEA results reveal that the SynRG with a slitted-rotor core, compared with the conventional SynRG with the same ratings and specifications, reduces the torque ripple by 24.51%, 29.72%, and 13.13% when feeding 8 A to a load with unity, lagging, and leading power factors, respectively. The FEA results also show that the induced voltage on no-load of the SynRG with a slitted-rotor core, compared with the conventional SynRG of the same ratings and specifications, increases by 10.77% when the auxiliary winding is fed by a capacitive excitation current of 6 A. Furthermore, the same results show that with a fixed excitation capacitive current of 6 A, the effect of armature reaction of the SynRG with a slitted-rotor core is demagnetizing when operating with load currents having a lagging power factor, and magnetizing when operating with load currents having unity and leading power factors. The same patterns have been observed in the experimental results for different excitation capacitance values. The Matlab/Simulink results show that the SynRG with a slitted-rotor core has a quicker dynamic response than the conventional SynRG. However, a well-designed pitch-control mechanism for the wind turbine is necessary to account for changes in wind speeds. Full article
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<p>Synchronous Reluctance Generator with direct capacitance injection. (<b>a</b>) Off-grid wind turbine topology, (<b>b</b>) Schematic diagram of the self-excited NSynRG winding scheme.</p>
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<p>Cross-sections of the rotor of SynRG and stator with two sets of windings. (<b>a</b>) Rotor with slit-cuts on <span class="html-italic">d</span>-axis, (<b>b</b>) Conventional rotor, (<b>c</b>) Stator showing the arrangement of both main and auxiliary windings.</p>
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<p>Photographs that show the constituents of the prototype SynRG with a slitted-rotor core. (<b>a</b>) Single rotor lamination, (<b>b</b>) Complete rotor core with shaft, (<b>c</b>) Rotor core inserted in the stator bore space ready to be fastened.</p>
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<p>Photographs of the laboratory setup. (<b>a</b>) Experimental setup rig photo, (<b>b</b>) Photograph showing the inductive load scheme in the experimental setup.</p>
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<p>Flux density distribution of the SynRG with a slitted-rotor core operating with a current load of 8 A and an excitation current of 6.8 A: 1000 rpm: (<b>a</b>) Unity power factor, (<b>b</b>) Lagging power factor, (<b>c</b>) Leading power factor.</p>
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<p>Comparison of saturation characteristics between the unoptimized NSynRG with a slitted-rotor core and optimized NSynRG with a slitted-rotor core.</p>
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<p>Induced no-load voltages with excitation current of 6 A. (<b>a</b>) Conventional SynRG, (<b>b</b>) SynRG with a slitted-rotor core.</p>
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<p>Airgap flux density on no-load with excitation current of 6.8 A. (<b>a</b>) The profile, (<b>b</b>) Harmonic spectrum.</p>
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<p>FEA electromagnetic torque profiles with a load current of 8 A of the NSynRG. (<b>a</b>) Unoptimized NSynRG, (<b>b</b>) Optimized NSynRG.</p>
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<p>Generated voltage characteristics on no-load. (<b>a</b>) Excitation capacitance of 50 µF, (<b>b</b>) Excitation capacitance of 90 µF, (<b>c</b>) Excitation capacitance of 140 µF, (<b>d</b>) Harmonic components of the no-load induced voltage.</p>
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<p>Regulation characteristics at different excitation capacitance values, such as (<b>a</b>) resistive load, (<b>b</b>) inductive load, and (<b>c</b>) capacitive load.</p>
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<p>No-load dynamic response of the SynRG with a slitted-rotor core at a constant wind speed of 4 m/s with 90 µF excitation capacitance. (<b>a</b>) Electromagnetic Torque, (<b>b</b>) Speed.</p>
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<p>No-load dynamic response of the conventional SynRG rotor at a constant wind speed of 4 m/s with 90 µF excitation capacitance. (<b>a</b>) Electromagnetic Torque, (<b>b</b>) Speed.</p>
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28 pages, 7616 KiB  
Article
Boosting Solar Sustainability: Performance Assessment of Roof-Mounted PV Arrays Under Snow Considering Various Module Interconnection Schemes
by Ebrahim Mohammadi, Gerry Moschopoulos and Aoxia Chen
Sustainability 2025, 17(1), 329; https://doi.org/10.3390/su17010329 - 4 Jan 2025
Viewed by 538
Abstract
The transition to renewable energy sources is vital for achieving sustainability, and photovoltaic (PV) systems play a key role in this shift. However, their performance can be significantly affected in snowy conditions, where the irradiation and energy production are limited. This study addresses [...] Read more.
The transition to renewable energy sources is vital for achieving sustainability, and photovoltaic (PV) systems play a key role in this shift. However, their performance can be significantly affected in snowy conditions, where the irradiation and energy production are limited. This study addresses a critical gap in the literature by developing a MATLAB/Simulink model that considers the impacts of snow layering and removal on roof-mounted photovoltaic arrays. This study investigates various module interconnection schemes—including Series, Series-Parallel, Total-Cross-Tied, Bridge-Linked, and Honey-Comb—to determine their impact on energy efficiency in snowy environments. Based on the results, when the modules are fully covered by uniform snow, the power losses can increase from 38.9% to 93.2% for all interconnection schemes by increasing the accumulated snow from 1 cm to 5 cm. When the modules are covered by nonuniform snow and the snow removal is considered the TCT scheme has the minimum power losses and the maximum efficiency, depending on the accumulated snow pattern. For the worst scenario, the power loss is 70.1% for TCT, 71.7% for SP, 72% for HC, 72.3% for BL, and 76.7% for series interconnection. For the other scenarios, almost a similar trend can be observed where the TCT interconnection has the maximum efficiency, and the series interconnection has the minimum efficiency. Full article
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<p>Equivalent circuit of single-diode PV model.</p>
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<p>PV array and different configurations. (<b>a</b>) Roof-mounted photovoltaic array schematic, (<b>b</b>) series, (<b>c</b>) SP, (<b>d</b>) TCT, (<b>e</b>) HC, (<b>f</b>) BL configuration.</p>
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<p>The impacts of uniform snow coverage on the PV array performance with TCT, SP, HC, BL configurations and various snow depths in Scenario 1. (<b>a</b>) P-V curve, (<b>b</b>) I-V curve.</p>
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<p>Uniform snow coverage and snow sliding off the array for Scenario 2.</p>
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<p>The impacts of various snow sliding levels on the PV array performance considering the uniform snow coverage of h = 1 cm for all modules in Scenario 2. (<b>a</b>) P-V curve, (<b>b</b>) I-V curve.</p>
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<p>Non-uniform snow on the array for Scenario 3. (<b>a</b>) for A = 0, (<b>b</b>) for A = 0.2.</p>
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<p>Effect of different snow sliding levels on the PV array performance considering the non-uniform snow coverage for different rows of Scenario 3. (<b>a</b>) P-V curve, (<b>b</b>) I-V curve.</p>
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<p>Non-uniform snow on the array (Scenario 4). (<b>a</b>) for A = 0, (<b>b</b>) for A = 0.2.</p>
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<p>Effect of different snow sliding levels on P-V curve in Scenario 4. (<b>a</b>) A = 1 (fully snow covered (blue curve)), STC (black curve), (<b>b</b>) A = 0.2, (<b>c</b>) A = 0.4, (<b>d</b>) A = 0.8 (scenario 4).</p>
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<p>Effect of different snow sliding levels on I-V curve in Scenario 4. (<b>a</b>) A = 1 (fully snow-covered (blue curve)), STC (black curve), (<b>b</b>) A = 0.2, (<b>c</b>) A = 0.4 and (<b>d</b>) A = 0.8.</p>
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<p>The effects of different snow sliding levels (A) on the (<b>a</b>) P-V curve, (<b>b</b>) I-V curve of the PV array with series interconnection in Scenario 4.</p>
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<p>Non-uniform snow coverage on the array for Scenario 5. (<b>a</b>) pattern 1, (<b>b</b>) pattern 2.</p>
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<p>P-V curves of the PV system in scenario 5 considering SP, TCT, BL, and HC configurations: (<b>a</b>) Pattern 1, (<b>b</b>) Pattern 2.</p>
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<p>I-V curves of the PV system in scenario 5 considering SP, TCT, BL, and HC configurations: (<b>a</b>) Pattern 1, (<b>b</b>) Pattern 2.</p>
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<p>Characteristic curves of the PV system in Scenario 5 considering S configuration (<b>a</b>) P-V, (<b>b</b>) I-V curves.</p>
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<p>Non-uniform snow coverage on the array for Scenario 6.</p>
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<p>Characteristic curves of the PV system in scenario 6 considering TCT, SP, Bl, and HC configurations: (<b>a</b>) P-V, (<b>b</b>) I-V curves.</p>
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<p>Characteristic curves of the PV system in Scenario 6 considering S configuration (<b>a</b>) P-V, (<b>b</b>) I-V curves.</p>
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<p>Random snow coverage on the array (Scenario 7).</p>
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<p>Characteristic curves of the PV system in Scenario 7 considering TCT, SP, Bl, and HC configurations: (<b>a</b>) P-V, (<b>b</b>) I-V curves.</p>
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<p>Characteristic curves of the PV system in Scenario 7 considering S configuration (<b>a</b>) P-V, (<b>b</b>) I-V curves.</p>
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30 pages, 12843 KiB  
Article
Design and Optimization of the Heatsink of a Level 1 Electric Vehicle Charger
by Iheanyi Emmanuel Ebere, Ashraf Ali Khan, Samuel Ogundahunsi, Emeka Ugwuemeaju, Usman Ali Khan and Shehab Ahmed
Energies 2025, 18(1), 180; https://doi.org/10.3390/en18010180 - 3 Jan 2025
Viewed by 479
Abstract
The onboard circuits of EV chargers comprise heat-producing electronic devices such as MOSFETs and diodes for switching and power conversion operations. A heatsink must dissipate this generated heat to extend the devices’ life and prevent component thermal stress or failure. This study primarily [...] Read more.
The onboard circuits of EV chargers comprise heat-producing electronic devices such as MOSFETs and diodes for switching and power conversion operations. A heatsink must dissipate this generated heat to extend the devices’ life and prevent component thermal stress or failure. This study primarily investigates the optimal heatsink geometry and pin configuration, which offers the most efficient temperature versus cost performance. MATLAB/Simulink (R2024a) was used to model a Level 1 charger using eight MOSFETs and four diodes. Various heatsink geometries were modeled using the ANSYS (2024 R1) Workbench and Fluent software to optimize the sink’s thermal performance. The analyses were performed under transient conditions using natural and forced cooling scenarios. The 2 mm wide plate fin heatsink with 44 fins yielded the best result. Further enhancement of the best-performing naturally cooled model improved the switches and diodes temperatures by 14% and 4%, respectively. The performance of the heatsink was further improved by applying a cooling fan to achieve an up to 25% diode and 40% MOSFET thermal dissipation efficiency. The results of this study show that the most efficient cooling performance and cost are realized when the optimum combination of fin spacing, proximity from the cooling fan, and fin geometry is selected. Full article
(This article belongs to the Section J: Thermal Management)
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<p>Device thermal resistances.</p>
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<p>Topology of the modeled bi-directional EV charger.</p>
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<p>MATLAB/Simulink model showing the schematic diagram of an EV charger.</p>
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<p>Grid supply waveforms.</p>
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<p>Battery waveform.</p>
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<p>(<b>a</b>). Transient thermal distribution of Model C1. (<b>b</b>). Model C1 temperature distribution.</p>
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<p>(<b>a</b>). Transient thermal distribution of Model C2. (<b>b</b>). Model C2 temperature distribution.</p>
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<p>(<b>a</b>). Transient thermal distribution of Model P1. (<b>b</b>). Model P1 temperature distribution.</p>
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<p>(<b>a</b>). Transient thermal distribution of Model P2. (<b>b</b>). Model P2 temperature distribution.</p>
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<p>Model P2-A temperature distribution.</p>
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<p>Model P2-B temperature distribution.</p>
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<p>Model P2-C temperature distribution.</p>
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<p>Model P2-D temperature distribution.</p>
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<p>Plot of temperature distribution over time for variants of Model P2.</p>
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<p>Heatsink in the computational domain.</p>
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<p>Air properties dialog from Fluent material database.</p>
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<p>Rotating domain cell zone specification.</p>
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<p>Diode power density setup.</p>
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<p>MOSFET power density setup.</p>
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<p>P2-D temperature distribution at 100 mm from fan.</p>
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<p>P2-D temperature distribution at 200 mm from fan.</p>
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<p>P2-D temperature distribution at 300 mm from fan.</p>
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<p>Thirty-three-fin variant P2-D<span class="html-italic"><sub>i</sub></span> temperature distribution.</p>
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<p>Twenty-two-fin variant P2-D<span class="html-italic"><sub>j</sub></span> temperature distribution.</p>
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<p>Eleven-fin variant P2-D<span class="html-italic"><sub>k</sub></span> temperature distribution.</p>
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<p>Six-fin variant P2-D<span class="html-italic"><sub>l</sub></span> temperature distribution.</p>
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<p>Active versus passive cooling thermal performance.</p>
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26 pages, 8196 KiB  
Article
Control Strategy for DC Micro-Grids in Heat Pump Applications with Renewable Integration
by Claude Bertin Nzoundja Fapi, Mohamed Lamine Touré, Mamadou-Baïlo Camara and Brayima Dakyo
Electronics 2025, 14(1), 150; https://doi.org/10.3390/electronics14010150 - 2 Jan 2025
Viewed by 409
Abstract
DC micro-grids are emerging as a promising solution for efficiently integrating renewable energy into power systems. These systems offer increased flexibility and enhanced energy management, making them ideal for applications such as heat pump (HP) systems. However, the integration of intermittent renewable energy [...] Read more.
DC micro-grids are emerging as a promising solution for efficiently integrating renewable energy into power systems. These systems offer increased flexibility and enhanced energy management, making them ideal for applications such as heat pump (HP) systems. However, the integration of intermittent renewable energy sources with optimal energy management in these micro-grids poses significant challenges. This paper proposes a novel control strategy designed specifically to improve the performance of DC micro-grids. The strategy enhances energy management by leveraging an environmental mission profile that includes real-time measurements for energy generation and heat pump performance evaluation. This micro-grid application for heat pumps integrates photovoltaic (PV) systems, wind generators (WGs), DC-DC converters, and battery energy storage (BS) systems. The proposed control strategy employs an intelligent maximum power point tracking (MPPT) approach that uses optimization algorithms to finely adjust interactions among the subsystems, including renewable energy sources, storage batteries, and the load (heat pump). The main objective of this strategy is to maximize energy production, improve system stability, and reduce operating costs. To achieve this, it considers factors such as heating and cooling demand, power fluctuations from renewable sources, and the MPPT requirements of the PV system. Simulations over one year, based on real meteorological data (average irradiance of 500 W/m2, average annual wind speed of 5 m/s, temperatures between 2 and 27 °C), and carried out with Matlab/Simulink R2022a, have shown that the proposed model predictive control (MPC) strategy significantly improves the performance of DC micro-grids, particularly for heat pump applications. This strategy ensures a stable DC bus voltage (±1% around 500 V) and maintains the state of charge (SoC) of batteries between 40% and 78%, extending their service life by 20%. Compared with conventional methods, it improves energy efficiency by 15%, reduces operating costs by 30%, and cuts CO2; emissions by 25%. By incorporating this control strategy, DC micro-grids offer a sustainable and reliable solution for heat pump applications, contributing to the transition towards a cleaner and more resilient energy system. This approach also opens new possibilities for renewable energy integration into power grids, providing intelligent and efficient energy management at the local level. Full article
(This article belongs to the Special Issue Innovative Technologies in Power Converters, 2nd Edition)
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<p>Configuration of the proposed micro-grid.</p>
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<p>Electrical architecture of PV system.</p>
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<p>Electrical design of a single diode PV cell.</p>
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<p>The P-V curves showing MPP: (<b>a</b>) fixed temperature and variable irradiance, (<b>b</b>) variable temperature and constant irradiance.</p>
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<p>Basic electrical diagram of the DC-DC boost converter.</p>
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<p>Equivalent electrical design of a single diode PV cell: (<b>a</b>) ON state of the switch, (<b>b</b>) OFF state of the switch.</p>
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<p>Flowchart of the FSCC approach.</p>
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<p>Improved FSCC-MPC algorithm.</p>
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<p>Schematic diagram of wind generator system.</p>
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<p>Schematic diagram of battery energy storage system.</p>
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<p>Wiring diagram for bidirectional DC-DC converter.</p>
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<p>Schematic diagram of the heat pump system.</p>
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<p>Control strategy of the micro-grid-based HP system.</p>
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<p>MPC block diagram of the micro-grid-based HP system.</p>
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<p>Proposed control strategy of the micro-grid-based HP system.</p>
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<p>Measured profiles during the year: (<b>a</b>) solar irradiance, (<b>b</b>) ambient temperature, (<b>c</b>) wind speed.</p>
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<p>Measured profiles over the year: (<b>a</b>) water temperature, (<b>b</b>) heat pump temperature.</p>
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<p>Simulation result of MPC performance: (<b>a</b>) DC bus voltage, (<b>b</b>) battery <span class="html-italic">SoC</span>.</p>
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<p>The different power waveforms: (<b>a</b>) power of PV, (<b>b</b>) power of wind, (<b>c</b>) power of battery, (<b>d</b>) power of heat pump.</p>
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<p>The different power waveforms: (<b>a</b>) over the year, (<b>b</b>) zooming 1, (<b>c</b>) zooming 2.</p>
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14 pages, 6268 KiB  
Article
Analysis of Influence of Abnormal Fiber-Optical Current Transformer on Double Closed-Loop Control of Converter Valve in Flexible DC Converter Station
by Yirun Ji, Qing Huai, Xuanfei Huang, Libo Ma, Qian Yuan, Chengjie Zhou and Chen Zhao
Electronics 2025, 14(1), 141; https://doi.org/10.3390/electronics14010141 - 1 Jan 2025
Viewed by 492
Abstract
The fiber-optical current transformer (FOCT) is the core measuring equipment of the flexible DC converter station, which affects the operation control of the system. In order to solve the problem of the influence of the abnormal FOCT on the operation of the converter [...] Read more.
The fiber-optical current transformer (FOCT) is the core measuring equipment of the flexible DC converter station, which affects the operation control of the system. In order to solve the problem of the influence of the abnormal FOCT on the operation of the converter valve being unclear, the common fault modes of temperature and optical path of the FOCT are analyzed in this paper. Then, based on the traditional optical current transformer (OCT) model and considering the influence of temperature parameters on the FOCT, the FOCT dynamic model considering multiple factors is constructed. Finally, the simulation analysis is carried out on the MATLAB 2021b/Simulink platform, and the results show that (1) when the FOCT temperature compensation is abnormal, the transmission power of the converter valve increases with the increase in temperature, but the increase in temperature change is small; (2) when the FOCT light source compensation is abnormal, the light source attenuates, the converter valve active power decreases, and the reactive power increases; and (3) when the optical fiber sensing ring is broken, the transmission power increases and seriously deviates from the preset value (the active power increases by about 87.5% and the reactive power increases by about 90%). It can be seen that the abnormal FOCT in the converter station has a serious influence on the operation of the converter valve. Full article
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<p>Schematic diagram of FOCT.</p>
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<p>Three-phase MMC topology.</p>
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<p>Coupled model of flexible DC converter valve and FOCT.</p>
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<p>Model and measured current values.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>Overall block diagram of the system.</p>
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<p>Detailed diagram of FOCT simulation module.</p>
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<p>Detailed diagram of outer-loop power control module.</p>
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<p>Detailed diagram of inner-loop current control module.</p>
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32 pages, 10813 KiB  
Article
Sliding Mode Backstepping Control of Excavator Bucket Trajectory Synovial in Particle Swarm Optimization Algorithm and Neural Network Disturbance Observer
by Xiangfei Tao, Kailei Liu, Jing Yang, Yu Chen, Jiayuan Chen and Haoran Zhu
Actuators 2025, 14(1), 9; https://doi.org/10.3390/act14010009 - 1 Jan 2025
Viewed by 434
Abstract
As a representative of multi-functional engineering machinery, the excavator is irreplaceable in the field of engineering construction. To autonomously control the excavator bucket, it is essential to control the position of the bucket hydraulic cylinder. As a consequence of the problem of position [...] Read more.
As a representative of multi-functional engineering machinery, the excavator is irreplaceable in the field of engineering construction. To autonomously control the excavator bucket, it is essential to control the position of the bucket hydraulic cylinder. As a consequence of the problem of position tracking control spawned from external disturbance and other factors in the self-mining servo system of excavators, a strategy of sliding mode backstepping control based on the particle swarm optimization algorithm and neural network disturbance observer (PSO-NNDO-SMBC) was recommended accordingly. Meanwhile, the complex disturbance was estimated online and compensated for by the system control input by the universal approximation property of the neural network disturbance observer (NNDO). Afterwards, the uncertainty of control parameters was optimized by the particle swarm optimization algorithm (PSO) and was fed back to the controller parameter input end. Afterwards, a co-simulation model of MATLAB/Simulink (MATLAB2023b) and AMESim (Simcenter Amesim 2304) was established for simulation analysis, and a test bench was set up for comparison and verification. As proven by the experimental results, PSO-NNDO-SMBC possessed strong anti-interference ability. In contrast to the sliding mode backstepping control based on the particle swarm optimization algorithm (PSO-SMBC), the maximum displacement tracking error was lowered by 50.5%. Furthermore, in comparison with the Proportional-Integral-Derivative (PID), the maximum displacement tracking error was decreased by 75.2%, which tremendously optimized the control accuracy of excavator bucket displacement tracking. Full article
(This article belongs to the Section Control Systems)
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<p>Hydraulic principle diagram of valve-controlled asymmetric cylinder.</p>
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<p>Multilayer feedforward neural network diagram.</p>
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<p>Radial basis function neural network diagram.</p>
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<p>PSO optimization SMBC parameter flow chart.</p>
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<p>Control system architecture diagram.</p>
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<p>AMESim simulation model. 1—Hydraulic oil; 2—Co-simulation interface; 3—Oil source; 4—Proportional valve; 5—Proportional amplifier 6—Rodless chamber pressure sensor; 7—Pressure sensor with rod chamber; 8—External load; 9—Force sensor; 10—Displacement sensor; 11—Speed sensor; 12—Hydraulic cylinder; 13—Oil tank.</p>
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<p>Simulink simulation model. 1—Command shift; 2—Instruction displacement first-order derivative; 3—Instruction displacement second-order derivative; 4—Instruction displacement third-order derivative; 5—Particle swarm optimization algorithm; 6—sliding mode backstepping controller 2; 7—Neural network disturbance observer; 8—Co-simulation interface.</p>
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<p>Iterative curve of particle swarm optimization algorithm.</p>
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<p>Extend step signal response curve.</p>
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<p>Extend step signal error curve.</p>
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<p>Retract step signal response curve.</p>
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<p>Retract step signal error curve.</p>
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<p>Control input of the three controllers for retract step signal.</p>
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<p>Simulation sinusoidal signal response curve.</p>
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<p>Simulation sinusoidal signal error curve.</p>
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<p>Control input of the three controllers for simulation sinusoidal signal.</p>
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<p>Simulation ramp signal response curve.</p>
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<p>Simulation ramp signal error curve.</p>
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<p>Control input of the three controllers for simulation ramp signal.</p>
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<p>2T hydraulic excavator test bench.</p>
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<p>Sinusoidal signal response curve.</p>
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<p>Sinusoidal signal error curve.</p>
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<p>Ramp signal response curve.</p>
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<p>Ramp signal error curve.</p>
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33 pages, 7735 KiB  
Article
Control and Optimization of Hydrogen Hybrid Electric Vehicles Using GPS-Based Speed Estimation
by Nouha Mansouri, Aymen Mnassri, Sihem Nasri, Majid Ali, Abderezak Lashab, Juan C. Vasquez and Josep M. Guerrero
Electronics 2025, 14(1), 110; https://doi.org/10.3390/electronics14010110 - 30 Dec 2024
Viewed by 662
Abstract
This paper investigates the feasibility of hydrogen-powered hybrid electric vehicles as a solution to transportation-related pollution. It focuses on optimizing energy use to improve efficiency and reduce emissions. The study details the creation and real-time performance assessment of a hydrogen hybrid electric vehicle [...] Read more.
This paper investigates the feasibility of hydrogen-powered hybrid electric vehicles as a solution to transportation-related pollution. It focuses on optimizing energy use to improve efficiency and reduce emissions. The study details the creation and real-time performance assessment of a hydrogen hybrid electric vehicle (HHEV)system using an STM32F407VG board. This system includes a fuel cell (FC) as the main energy source, a battery (Bat) to provide energy during hydrogen supply disruptions and a supercapacitor (SC) to handle power fluctuations. A multi-agent-based artificial intelligence tool is used to model the system components, and an energy management algorithm (EMA) is applied to optimize energy use and support decision-making. Real Global Positioning System (GPS) data are analyzed to estimate energy consumption based on trip and speed parameters. The EMA, developed and implemented in real-time using Matlab/Simulink(2016), identifies the most energy-efficient routes. The results show that the proposed vehicle architecture and management strategy effectively select optimal routes with minimal energy use. Full article
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<p>Hydrogen hybrid electric vehicle design.</p>
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<p>Speed estimator.</p>
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<p>Road recognition by GPS.</p>
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<p>System control behavior based on decision-making.</p>
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<p>EMA state diagram.</p>
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<p>FC/BaT/SC configuration EMA.</p>
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<p>Role of supercapacitors in hybrid hydrogen–electric vehicles.</p>
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<p>Component sizing scheme.</p>
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<p>Scheme of system efficiency.</p>
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<p>Possible detected ways by Google Maps.</p>
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<p>Referential vehicle speed value per road.</p>
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<p>Referential vehicle speed value per road.</p>
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<p>Comparison of actual and predicted speed profiles with statistical evaluation across roads.</p>
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<p>Road 1 performance simulation.</p>
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<p>Road 2 performance simulation.</p>
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<p>Road 3 performance simulation.</p>
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<p>Road 3 performance simulation.</p>
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<p>HEV performances per road.</p>
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<p>Interactive real-time MATLAB interface.</p>
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33 pages, 17902 KiB  
Article
Modeling and Design of a Grid-Tied Renewable Energy System Exploiting Re-Lift Luo Converter and RNN Based Energy Management
by Kavitha Paulsamy and Subha Karuvelam
Sustainability 2025, 17(1), 187; https://doi.org/10.3390/su17010187 - 30 Dec 2024
Viewed by 412
Abstract
The significance of the Hybrid Renewable Energy System (HRES) is profound in the current scenario owing to the mounting energy requirements, pressing ecological concerns and the pursuit of transitioning to greener energy alternatives. Thereby, the modeling and design of HRES, encompassing PV–WECS–Battery, which [...] Read more.
The significance of the Hybrid Renewable Energy System (HRES) is profound in the current scenario owing to the mounting energy requirements, pressing ecological concerns and the pursuit of transitioning to greener energy alternatives. Thereby, the modeling and design of HRES, encompassing PV–WECS–Battery, which mainly focuses on efficient power conversion and advanced control strategy, is proposed. The voltage gain of the PV system is improved using the Re-lift Luo converter, which offers high efficiency and power density with minimized ripples and power losses. Its voltage lift technique mitigates parasitic effects and delivers improved output voltage for grid synchronization. To control and stabilize the converter output, a Proportional–Integral (PI) controller tuned using a novel hybrid algorithm combining Grey Wolf Optimization (GWO) with Hermit Crab Optimization (HCO) is implemented. GWO follows the hunting and leadership characteristics of grey wolves for improved simplicity and robustness. By simulating the shell selection behavior of hermit crabs, the HCO adds diversity to exploitation. Due to these features, the hybrid GWO–HCO algorithm enhances the PI controller’s capability of handling dynamic non-linear systems, generating better control accuracy, and rapid convergence to optimal solutions. Considering the Wind Energy Conversion System (WECS), the PI controller assures improved stability despite fluctuations in wind. A Recurrent Neural Network (RNN)-based battery management system is also incorporated for accurate monitoring and control of the State of Charge (SoC) and the terminal voltage of battery storage. The simulation is conducted in MATLAB Simulink 2021a, and a lab-scale prototype is implemented for real-time validation. The Re-lift Luo converter achieves an efficiency of 97.5% and a voltage gain of 1:10 with reduced oscillations and faster settling time using a Hybrid GWO–HCO–PI controller. Moreover, the THD is reduced to 1.16%, which indicates high power quality and reduced harmonics. Full article
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<p>Configuration of the PV–WECS–Battery Integrated HRES.</p>
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<p>Circuit representation of the PV system.</p>
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<p>PV curve.</p>
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<p>Re-lift Luo converter.</p>
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<p>Modes of operation. (<b>a</b>) Mode 1. (<b>b</b>) Mode 2.</p>
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<p>Operational waveform.</p>
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<p>Efficiency comparison of converters.</p>
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<p>Flowchart of the Hybrid GWO–HCO.</p>
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<p>Structure of the Hybrid GWO–HCO optimized the PI controller system.</p>
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<p>RNN for the battery modeling.</p>
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<p>Grid voltage synchronization.</p>
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<p>Simulation setup of the proposed system.</p>
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<p>Waveforms representing (<b>a</b>) Temperature and (<b>b</b>) Irradiation.</p>
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<p>PV panel waveforms represent (<b>a</b>) voltage and (<b>b</b>) current.</p>
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<p>Waveforms for output voltage of the Re-lift Luo converter using (<b>a</b>) PI controller, (<b>b</b>) GWO–PI controller, (<b>c</b>) Hybrid GWO–HCO–PI controller, and (<b>d</b>) Combined representation of the converter outputs.</p>
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<p>Output current waveform of Re-lift Luo converter.</p>
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<p>Output voltage waveform of (<b>a</b>) DFIG and (<b>b</b>) PWM rectifier.</p>
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<p>Waveforms for battery parameters.</p>
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<p>Waveforms representing grid parameters.</p>
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<p>Single-phase of grid current and voltage.</p>
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<p>Waveforms of (<b>a</b>) real power, (<b>b</b>) reactive power.</p>
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<p>Power factor waveform.</p>
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<p>THD Waveform.</p>
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<p>Hardware setup.</p>
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<p>PV system output (<b>a</b>) Voltage (<b>b</b>) Current.</p>
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<p>Converter voltage waveform using (<b>a</b>) PI controller (<b>b</b>) GWO-PI controller (<b>c</b>) GWO-HCO-PI controller.</p>
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<p>(<b>a</b>) Output voltage of DFIG (<b>b</b>) Output of PWM rectifier.</p>
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<p>(<b>a</b>) Battery SoC (<b>b</b>) DC-link voltage.</p>
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<p>Grid-side (<b>a</b>) Voltage and (<b>b</b>) Current.</p>
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<p>Grid current THD in (<b>a</b>) R-phase (<b>b</b>) Y-phase and (<b>c</b>) B-phase.</p>
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<p>RMSE convergence of optimization algorithms.</p>
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<p>Voltage gain analysis of converters.</p>
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24 pages, 10737 KiB  
Article
Experimental Design and Simulation of a Fly-Cutting Plant for Academic Environment Practices
by Diego Fernando Ramírez-Jiménez and Cristian Alejandro Torres Valencia
Machines 2025, 13(1), 15; https://doi.org/10.3390/machines13010015 - 29 Dec 2024
Viewed by 666
Abstract
Test plants or laboratory prototypes are essential for developing training activities in engineering. In the field of automation and control, simulators or high-fidelity equipment models commonly used in industrial processes are necessary. These tools allow engineering trainees to gain experience working with devices [...] Read more.
Test plants or laboratory prototypes are essential for developing training activities in engineering. In the field of automation and control, simulators or high-fidelity equipment models commonly used in industrial processes are necessary. These tools allow engineering trainees to gain experience working with devices similar to those they will encounter in their professional contexts. This paper presents the design and simulation of a fly-cutting plant for academic use. A 3D model was developed in SketchUp, incorporating features typical of industrial plants. The system’s simulation was carried out in MATLAB R2023b using mathematical modeling. The primary contribution of this work is the design of a low-cost, compact industrial prototype that includes a conveyor belt and a continuous cutting mechanism, enabling the understanding and operation of large-scale industrial processes. Performance tests were conducted using MATLAB, Simulink, and Code Composer Studio. Subsequently, operational and cutting tests were performed using classical control techniques. Additionally, the design features of the fly-cutting plant, which can be easily implemented for process control training activities, are detailed. Full article
(This article belongs to the Special Issue Recent Developments in Machine Design, Automation and Robotics)
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<p>Industrial flying cutting plants: (<b>a</b>) T1 type and (<b>b</b>) T3 type. Source: The authors.</p>
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<p>Graphical user interface for MATLAB PIDTuner. Source: [<a href="#B31-machines-13-00015" class="html-bibr">31</a>].</p>
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<p>Graphical user interface for SketchUp desktop version. Source: [<a href="#B32-machines-13-00015" class="html-bibr">32</a>].</p>
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<p>Block diagram of the structure of the fly-cutting plant. Source: The authors.</p>
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<p>Structure designed for the conveyor belt. Source: The authors.</p>
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<p>Fixed drum roller with bearings and pulley. Source: The authors.</p>
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<p>Free drum roller. Source: The authors.</p>
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<p>Motion coordinates for the cutting system. Source: The authors.</p>
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<p>Design and 3D modeling of the cutting system using SketchUp software. Source: The authors.</p>
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<p>Pulleys’ and rollers’ relationship for the movement of the conveyor belt. Source: The authors.</p>
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<p>Maximum angular speed achieved by the conveyor belt motor. Source: The authors.</p>
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<p>Movement of the pulley P2 on the X-axis. Source: The authors.</p>
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<p>Maximum speed reached by the X-axis motor in the cutting system. Source: The authors.</p>
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<p>PWM signals for motor operation in the cutting system: (<b>a</b>) Motor for motion on the y-axis. (<b>b</b>) Motor for motion on the z-axis. Source: The authors.</p>
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<p>Power circuit for DRV8825 drivers (bottom) and L298N (top). Source: The authors.</p>
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<p>Tx and Rx circuits for high-speed optocouplers. Source: The authors.</p>
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<p>Three-dimensional (3D) design made in ARES for the power circuit. Source: The authors.</p>
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<p>Proposed signal switching circuit. Source: The authors.</p>
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<p>Three-dimensional (3D) model for the commutation circuit in <a href="#machines-13-00015-f020" class="html-fig">Figure 20</a>. Source: The authors.</p>
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<p>Proposed 3D model for the control circuit. Source: The authors.</p>
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<p>Workspace for the CCS desktop application. Source: The authors.</p>
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<p>The programming structure developed for the simulation of the fly-cutting plant. Source: The authors.</p>
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<p>Controller parameters from PIDTuner. Source: The authors.</p>
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<p>Continuous-time block diagram for the proposed controller. Source: The authors.</p>
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<p>PI controller structure in discrete time for the fly-cutting plant. Source: The authors.</p>
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<p>The programming structure developed for the simulation of the fly-cutting plant. Source: The authors.</p>
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16 pages, 4012 KiB  
Article
Dynamic Response of a Single-Rotor Wind Turbine with Planetary Speed Increaser and Counter-Rotating Electric Generator in Starting Transient State
by Radu Saulescu and Mircea Neagoe
Appl. Sci. 2025, 15(1), 191; https://doi.org/10.3390/app15010191 - 29 Dec 2024
Viewed by 573
Abstract
The paper addresses the dynamic modeling and numerical simulation of a novel single-rotor wind system with a planetary speed increaser and counter-rotating direct current (DC) generator, patented by authors, during the transient stage from rest. The proposed analytical dynamic algorithm involves the decomposition [...] Read more.
The paper addresses the dynamic modeling and numerical simulation of a novel single-rotor wind system with a planetary speed increaser and counter-rotating direct current (DC) generator, patented by authors, during the transient stage from rest. The proposed analytical dynamic algorithm involves the decomposition of the wind system into its component rigid bodies, followed by the description of their dynamic equations using the Newton–Euler method. The linear mechanical characteristics of the DC generator and wind rotor are added to these dynamic equations. These equations allow for the establishment of the close-form equation of motion of the wind system and, implicitly, the time variation of the mechanical power parameters. Numerical simulations of the obtained analytical dynamic model were performed in MATLAB-Simulink in start-up mode from rest for the case study of a 100 kW wind turbine. These results allowed highlighting the time variation of angular velocities and accelerations, torques, and powers for all system shafts, both in the transient regime and steady-state. The implementation, in this case, of the counter-rotating generator indicates a 6.4% contribution of the mobile stator to the generator’s total power. The paper’s results are useful in the design, virtual prototyping, and optimization processes of modern wind energy conversion systems. Full article
(This article belongs to the Section Energy Science and Technology)
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<p>Single-rotor wind turbine with counter-rotating electric generator: (<b>a</b>) conceptual scheme; (<b>b</b>) block scheme.</p>
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<p>(<b>a</b>) Block scheme of the wind turbine and its decomposition into components: (<b>b</b>) wind rotor; (<b>c</b>) intermediate shaft; (<b>d</b>) planetary units; and (<b>e</b>) generator rotor and stator.</p>
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<p>The mechanical characteristic of a wind rotor modeled by four linearized zones.</p>
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<p>The wind system dynamic response: (<b>a</b>) input vs. output angular speeds; (<b>b</b>) input vs. output angular accelerations; (<b>c</b>) wind rotor vs. generator torques; (<b>d</b>) wind rotor vs. generator powers.</p>
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<p>The dynamic response at the wind rotor side: (<b>a</b>) wind rotor vs. input torques; (<b>b</b>) wind rotor vs. input powers.</p>
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<p>The dynamic response at the generator side: (<b>a</b>) generator angular speeds; (<b>b</b>) generator angular accelerations; (<b>c</b>) generator rotor vs. output 1 torques; (<b>d</b>) generator rotor vs. output 1 powers; (<b>e</b>) generator stator vs. output 2 torques; (<b>f</b>) generator stator vs. output 2 powers; (<b>g</b>) mechanical powers.</p>
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33 pages, 19067 KiB  
Article
Modelling and Simulation of Pico- and Nano-Grids for Renewable Energy Integration in a Campus Microgrid
by Kuan Tak Tan, Sivaneasan Bala Krishnan and Andy Yi Zhuang Chua
Energies 2025, 18(1), 67; https://doi.org/10.3390/en18010067 - 27 Dec 2024
Viewed by 339
Abstract
Research in renewable energy sources and microgrid systems is critical for the evolving power industry. This paper examines the operational behavior of both pico- and nano-grids during transitions between grid-connected and islanded modes. Simulation results demonstrate that both grids effectively balance the power [...] Read more.
Research in renewable energy sources and microgrid systems is critical for the evolving power industry. This paper examines the operational behavior of both pico- and nano-grids during transitions between grid-connected and islanded modes. Simulation results demonstrate that both grids effectively balance the power flow, regulate the state of charge (SOC), and stabilize the voltage during dynamic operational changes. Specific scenarios, including grid disconnection, load sharing, and weather-based energy fluctuations, were tested and validated. This paper models both pico-grids and nano-grids at the Singapore Institute of Technology Punggol Campus, incorporating solar PVs, energy storage systems (ESSs), power electronic converters, and both DC and AC loads, along with utility grid connections. The pico-grid includes a battery storage system, a single-phase inverter linked to a single-phase grid, and DC and AC loads. The nano-grid comprises solar PV panels, a boost converter, a battery storage system, a three-phase inverter connected to a three-phase grid, and AC loads. Both the pico-grid and nano-grid are configurable in standalone or grid-connected modes. This configuration flexibility allows for a detailed operational analysis under various conditions. This study conducted subsystem-level modelling before integrating all components into a simulation environment. MATLAB/Simulink version R2024b was utilized to model, simulate, and analyze the power flow in both the pico-grid and nano-grid under different operating conditions. Full article
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<p>Overview of a pico-grid in a building at SIT Punggol Campus.</p>
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<p>Proposed topology used in BESS.</p>
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<p>Proposed control algorithm used to control BESS.</p>
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<p>Proposed topology used in single-phase inverter.</p>
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<p>Proposed control algorithm used to control single-phase inverter.</p>
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<p>Overview of nano-grid system of a building at SIT Punggol Campus.</p>
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<p>Proposed topology used in solar PV boost converter.</p>
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<p>Proposed control algorithm used to control boost converter.</p>
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<p>Proposed topology used in three-phase inverter.</p>
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<p>Proposed control algorithm used to control three-phase inverter.</p>
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<p>Simulation model of BESS integration with single-phase inverter.</p>
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<p>Load demand estimation of DC (top) and AC (bottom) loads for pico-grid system.</p>
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<p>The SOC level of the BESS during discharging in pico-grid system.</p>
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<p>The battery voltage of the BESS during discharging in pico-grid system.</p>
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<p>Battery current of BESS during discharging in pico-grid system.</p>
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<p>Battery capacity of BESS during discharging in pico-grid system.</p>
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<p>Voltage level at DC busbar in pico-grid system.</p>
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<p>Surplus power delivered to the grid in pico-grid system.</p>
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<p>SOC level of the BESS during charging in pico-grid system.</p>
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<p>Battery voltage of the BESS during charging in pico-grid system.</p>
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<p>DC bus voltage of the BESS during charging in pico-grid system.</p>
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<p>Battery current of BESS during charging in pico-grid system.</p>
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<p>Battery capacity of BESS during charging in pico-grid system.</p>
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<p>Supplying power from the grid to charge the battery in pico-grid system.</p>
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<p>Two parallel pico-grids connected to the single-phase grid.</p>
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<p>DC (<b>top</b>) and AC loads (<b>bottom</b>) of two pico-grids system.</p>
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<p>Surplus power from the system sent to the grid for two pico-grids system.</p>
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<p>Simulation model of integration of solar PV and BESS with three-phase inverter.</p>
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<p>Solar PV array waveform.</p>
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<p>Load demand estimation of AC loads in nano-grid system.</p>
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<p>SOC of battery during discharging in nano-grid system.</p>
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<p>Battery voltage of the BESS during discharging in nano-grid system.</p>
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<p>Battery current of BESS during discharging in nano-grid system.</p>
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<p>Power supplied by battery of BESS during discharging in nano-grid system.</p>
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<p>Voltage level at DC busbar in nano-grid system.</p>
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<p>Surplus power delivered to the grid in nano-grid system.</p>
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<p>Simulation model to demonstrate charging of battery.</p>
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<p>SOC of battery during charging in nano-grid system.</p>
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<p>Battery voltage of the BESS during charging in nano-grid system.</p>
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<p>Voltage level at DC busbar in nano-grid system (Test Condition 1).</p>
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<p>Battery current of BESS during charging in nano-grid system.</p>
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<p>Battery capacity of BESS during charging in nano-grid system.</p>
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<p>Drawing power from the grid to charge the battery in nano-grid system.</p>
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<p>Simulation model to demonstrate a rainy-day operation.</p>
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<p>Solar PV power in nano-grid system.</p>
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<p>Load demand of AC loads in nano-grid system.</p>
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<p>Power supplied by the grid to the load in nano-grid system.</p>
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<p>Simulation model to demonstrate a sunny-day operation.</p>
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<p>Load demand estimation of AC loads in nano-grid system (Test Condition 3).</p>
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<p>Solar PV power generated in nano-grid system.</p>
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<p>SOC of battery during charging in nano-grid system (Test Condition 3).</p>
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<p>Battery capacity of BESS during charging in nano-grid system (Test Condition 3).</p>
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<p>Surplus power delivered to the grid in nano-grid system (Test Condition 3).</p>
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<p>Two parallel nano-grids connected to the three-phase grid.</p>
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<p>AC loads before an increase for two nano-grids system.</p>
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<p>Surplus power from the system sent to the grid for a two-nano-grid system.</p>
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18 pages, 5737 KiB  
Article
A Semiconductor Current-Limiting Device Based on a DC Converter
by Evgeniy P. Safonov, Vladimir Ya. Frolov, Anton V. Boeshko and Ruslan S. Dautov
Energies 2025, 18(1), 58; https://doi.org/10.3390/en18010058 - 27 Dec 2024
Viewed by 306
Abstract
Short-circuit currents in autonomous and isolated electrical complexes today are approaching the switching capacity of operated circuit breakers. Since the existing equivalents cannot ensure the necessary reliability of power supply to consumers in emergency situations, it is pertinent to assess the need for [...] Read more.
Short-circuit currents in autonomous and isolated electrical complexes today are approaching the switching capacity of operated circuit breakers. Since the existing equivalents cannot ensure the necessary reliability of power supply to consumers in emergency situations, it is pertinent to assess the need for developing new types of current-limiting devices (CLDs). This paper proposes an electrical circuit of a semiconductor current-limiting device based on a step-down DC-DC converter, where the main switch is a thyristor with an artificially switched circuit. Transient processes during the operation of the device are considered in detail. A mathematical model of the device is also provided. This model was verified by modeling the CLD circuit in MATLAB Simulink. In turn, the validity of the computer model used was proven experimentally. During the experiments, the current-limiting efficiency of the circuit was demonstrated, and its proposed mathematical model was also confirmed. This research was carried out as part of the project within the State Assignment FSEG-2023-0012. Full article
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<p>Sample diagram of a power system section for clarification of the principle of the selective operation of switching equipment.</p>
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<p>A diagram of the power system of a prospective vessel equipped with electric propulsion.</p>
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<p>Electrical diagram of a semiconductor current-limiting device.</p>
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<p>Oscillograms of transient processes during various stages of CLD operation.</p>
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<p>The stages of operation of the current-limiting device. (<b>a</b>) Nominal operation mode (time interval 0–T<sub>0</sub> in <a href="#energies-18-00058-f004" class="html-fig">Figure 4</a>). (<b>b</b>) The occurrence of a short circuit or the activation of the main thyristor (time intervals T<sub>0</sub>–T<sub>1</sub> or T<sub>2</sub>–T<sub>3</sub>, respectively, in <a href="#energies-18-00058-f004" class="html-fig">Figure 4</a>). (<b>c</b>) The artificial switching of the thyristor (time moment T<sub>1</sub> in <a href="#energies-18-00058-f004" class="html-fig">Figure 4</a>). (<b>d</b>) The current pause of the CLD (time intervals T<sub>1</sub>–T<sub>2</sub> and T<sub>3</sub>–T<sub>2</sub> in <a href="#energies-18-00058-f004" class="html-fig">Figure 4</a>).</p>
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<p>Current-limiting device equivalent circuit.</p>
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<p>The transients of the current-limiting device: (<b>a</b>) the main thyristor is on; (<b>b</b>) the main thyristor is off; and (<b>c</b>) the current at the output of the current limiter/converter.</p>
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<p>The transients of the CB discharge: (<b>a</b>) an approximate view of the substitution scheme and the oscillogram of the current at the output of the CLD, transients of the first stage; (<b>b</b>) transients of the second stage.</p>
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<p>The transients of the CB discharge: (<b>a</b>) an approximate view of the substitution scheme and the oscillogram of the current at the output of the CLD, transients of the first stage; (<b>b</b>) transients of the second stage.</p>
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<p>A more detailed picture describing the transient processes of the CB discharge. The black dashed curve is the current in the SC circuit; the red curve is the current of the main thyristor; and the blue curve is the current of the CB discharge.</p>
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<p>Appearance of the created prototype of the current-limiting device. (<b>a</b>) Photograph, view 1. (<b>b</b>) Photograph, view 2.</p>
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<p>An electrical diagram of the experimental setup.</p>
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<p>The current oscillograms at the CLD output (black solid line denotes experimental results; red dotted line is the average value) at a C<sub>PCSB</sub> precharge voltage of 500 V. The CLD operating frequency is (<b>a</b>) 36 Hz; (<b>b</b>) 48 Hz; and (<b>c</b>) 81 Hz.</p>
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<p>The current waveforms at the CLD output (the black solid line denotes the experimental results; the red dotted line is the average value) for the CLD operating at 81 Hz. The C<sub>PCSB</sub> precharge voltage is indicated directly at the waveforms.</p>
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<p>The equivalent circuit of the electromagnetic reactor of the DC circuit: (<b>a</b>) excluding the influence of skin effect and proximity effect; (<b>b</b>) taking into account the influence of the skin effect and the proximity effect.</p>
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<p>A comparison of the computer simulation and experimental results. (<b>a</b>) The output current of the current-limiting device. (<b>b</b>) The transients in the CLD at the time of artificial switching of the thyristor and the CB discharge.</p>
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<p>The simulation results of a powerful prototype of a current-limiting device. (<b>a</b>) The output current of the current-limiting device. (<b>b</b>) The transients in the CLD at the time of artificial switching of the thyristor and the CB discharge.</p>
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29 pages, 10283 KiB  
Article
Multi-Fault-Tolerant Operation of Grid-Interfaced Photovoltaic Inverters Using Twin Delayed Deep Deterministic Policy Gradient Agent
by Shyamal S. Chand, Branislav Hredzak and Maurizio Cirrincione
Energies 2025, 18(1), 44; https://doi.org/10.3390/en18010044 - 26 Dec 2024
Viewed by 429
Abstract
The elevated penetration of renewable energy has seen a significant increase in the integration of inverter-based resources (IBRs) into the electricity network. According to various industrial standards on interconnection and interoperability, IBRs should be able to withstand variability in grid conditions. Positive sequence [...] Read more.
The elevated penetration of renewable energy has seen a significant increase in the integration of inverter-based resources (IBRs) into the electricity network. According to various industrial standards on interconnection and interoperability, IBRs should be able to withstand variability in grid conditions. Positive sequence voltage-oriented control (PSVOC) with a feed-forward decoupling approach is often adopted to ensure closed-loop control of inverters. However, the dynamic response of this control scheme deteriorates during fluctuations in the grid voltage due to the sensitivity of proportional–integral controllers, the presence of the direct- and quadrature-axis voltage terms in the cross-coupling, and predefined saturation limits. As such, a twin delayed deep deterministic policy gradient-based voltage-oriented control (TD3VOC) is formulated and trained to provide effective current control of inverter-based resources under various dynamic conditions of the grid through transfer learning. The actor–critic-based reinforcement learning agent is designed and trained using the model-free Markov decision process through interaction with a grid-connected photovoltaic inverter environment developed in MATLAB/Simulink® 2023b. Using the standard PSVOC method results in inverter input voltage overshoots of up to 2.50 p.u., with post-fault current restoration times of as high as 0.55 s during asymmetrical faults. The designed TD3VOC technique confines the DC link voltage overshoot to 1.05 p.u. and achieves a low current recovery duration of 0.01 s after fault clearance. In the event of a severe symmetric fault, the conventional control method is unable to restore the inverter operation, leading to integral-time absolute errors of 0.60 and 0.32 for the currents of the d and q axes, respectively. The newly proposed agent-based control strategy restricts cumulative errors to 0.03 and 0.09 for the d and q axes, respectively, thus improving inverter regulation. The results indicate the superior performance of the proposed control scheme in maintaining the stability of the inverter DC link bus voltage, reducing post-fault system recovery time, and limiting negative sequence currents during severe asymmetrical and symmetrical grid faults compared with the conventional PSVOC approach. Full article
(This article belongs to the Special Issue Advances in Electrical Power System Quality)
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<p>Single line diagram of the IEEE 13 bus network with an interconnected solar system.</p>
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<p>Dual-stage photovoltaic power conversion circuit.</p>
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<p>Conventional positive sequence voltage oriented control (PSVOC).</p>
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<p>Twin delayed deep deterministic voltage-oriented control (TD3VOC) for inverter.</p>
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<p>General reinforcement learning workflow.</p>
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<p>Critic and actor deep neural network architecture.</p>
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<p>Training process of TD3PG RL agent incorporating data flow and environment interactions.</p>
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<p>(<b>a</b>) Cumulative reward obtained and (<b>b</b>) Q-value progression at each successive iteration.</p>
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<p>(<b>a</b>) Grid voltages, three-phase current waveform with (<b>b</b>) PSVOC and (<b>c</b>) TD3VOC, (<b>d</b>) DC link voltage, (<b>e</b>) active power, (<b>f</b>) reactive power, and negative sequence current on (<b>g</b>) direct and (<b>h</b>) quadrature axis response during asymmetrical short circuit fault between phases B and C.</p>
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<p>(<b>a</b>) Grid voltages, three-phase current waveform with (<b>b</b>) PSVOC and (<b>c</b>) TD3VOC, (<b>d</b>) DC link voltage, (<b>e</b>) active power, (<b>f</b>) reactive power, and negative sequence current on (<b>g</b>) direct and (<b>h</b>) quadrature axis response during phases A and B to ground fault.</p>
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<p>(<b>a</b>) Grid voltages, three-phase current waveform with (<b>b</b>) PSVOC and (<b>c</b>) TD3VOC, (<b>d</b>) DC link voltage, (<b>e</b>) active power, (<b>f</b>) reactive power, and negative sequence current on (<b>g</b>) direct and (<b>h</b>) quadrature axis response to a symmetrical short-circuit fault between phases A, B, and C.</p>
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<p>Integral-time error visualization for <span class="html-italic">d</span> and <span class="html-italic">q</span> axes currents using (<b>a</b>,<b>c</b>,<b>e</b>) PSVOC and (<b>b</b>,<b>d</b>,<b>f</b>) TD3VOC for (<b>a</b>,<b>b</b>) asymmetric fault between phases B and C, (<b>c</b>,<b>d</b>) asymmetric phases A and B to ground fault, and (<b>e</b>,<b>f</b>) symmetric short-circuit fault between phases A, B and C.</p>
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