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Search Results (569)

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Keywords = switch machine

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22 pages, 627 KiB  
Article
Fitness Approximation Through Machine Learning with Dynamic Adaptation to the Evolutionary State
by Itai Tzruia, Tomer Halperin, Moshe Sipper and Achiya Elyasaf
Information 2024, 15(12), 744; https://doi.org/10.3390/info15120744 - 21 Nov 2024
Viewed by 421
Abstract
We present a novel approach to performing fitness approximation in genetic algorithms (GAs) using machine learning (ML) models, focusing on dynamic adaptation to the evolutionary state. We compare different methods for (1) switching between actual and approximate fitness, (2) sampling the population, and [...] Read more.
We present a novel approach to performing fitness approximation in genetic algorithms (GAs) using machine learning (ML) models, focusing on dynamic adaptation to the evolutionary state. We compare different methods for (1) switching between actual and approximate fitness, (2) sampling the population, and (3) weighting the samples. Experimental findings demonstrate significant improvement in evolutionary runtimes, with fitness scores that are either identical or slightly lower than those of the fully run GA—depending on the ratio of approximate-to-actual-fitness computation. Although we focus on evolutionary agents in Gymnasium (game) simulators—where fitness computation is costly—our approach is generic and can be easily applied to many different domains. Full article
(This article belongs to the Special Issue Machine Learning and Data Mining: Innovations in Big Data Analytics)
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Graphical abstract

Graphical abstract
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<p>Gymnasium environments (or custom modifications of them) that we use for actual fitness-score evaluation.</p>
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<p>Flowchart of proposed method. In evolution mode, the algorithm functions as a regular GA. When the switch condition is met, the algorithm shifts to prediction mode: actual (in-simulator) fitness values are calculated only for a sampled subset of the population, while the rest are assigned approximate fitnesses from the ML model. This latter is retrained before moving to the next generation.</p>
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19 pages, 6424 KiB  
Article
Research into Energy-Saving Control Strategies of a Bulldozer Driven by a Torque Converter Based on the Minimum Fuel Consumption Rate of the Whole Machine
by Hongbin Qiang, He Li, Shaopeng Kang, Kailei Liu, Jing Yang and Lian Wang
Sustainability 2024, 16(22), 10111; https://doi.org/10.3390/su162210111 - 20 Nov 2024
Viewed by 281
Abstract
In order to address the issue of poor fuel efficiency in hydraulic bulldozers during operation, this paper proposes a speed–load control strategy aimed at minimizing the overall fuel consumption rate of the machine. First, input–output models of the engine, hydraulic torque converter and [...] Read more.
In order to address the issue of poor fuel efficiency in hydraulic bulldozers during operation, this paper proposes a speed–load control strategy aimed at minimizing the overall fuel consumption rate of the machine. First, input–output models of the engine, hydraulic torque converter and the entire vehicle were established. Then, based on the bulldozer’s output power and fuel consumption rate, a performance metric for the overall fuel consumption rate was proposed to reflect the machine’s working efficiency. The characteristics of the overall fuel consumption rate were analyzed under different load, speed, and gear conditions. Next, a work point optimization control strategy was proposed for the whole machine energy-saving mode and constant power mode, aiming to minimize the overall fuel consumption rate while using the load, speed, and gear as control variables. To verify the feasibility of the work point optimization control strategy, simulations were conducted for both the energy-saving and constant power modes. The simulation results showed that in the whole machine energy-saving mode, this control strategy resulted in the lowest fuel consumption compared to constant speed control strategies at 1500, 1700, and 2000 rpm, with significant reductions in most cases. In the constant power mode, a comparison between four optimal operating points and the whole machine energy-saving mode revealed that while the former had slightly higher fuel consumption, it ensured a stable power output. Finally, experimental testing demonstrated that the proposed control strategy reduced the overall fuel consumption rate by 12.5% compared to the constant speed mode, verifying the effectiveness of the strategy. The study concludes that the energy-saving control strategy, through the coordinated switching between the two modes in complex operating conditions, not only ensures a stable power output for the bulldozer but also significantly improves fuel efficiency, providing an important reference for optimizing the efficiency of transmission systems in construction machines. Full article
(This article belongs to the Section Energy Sustainability)
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<p>The powertrain of the bulldozer.</p>
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<p>The engine characteristics: (<b>a</b>) the engine performance curve; (<b>b</b>) the engine speed control characteristic curve.</p>
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<p>The engine characteristic curve.</p>
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<p>The characteristic curve of the torque converter.</p>
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<p>The input characteristic of the engine and the torque converter.</p>
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<p>The output characteristics of the engine and the torque converter.</p>
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<p>The EFC of the engine and torque converter system.</p>
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<p>The torque percentage of the engine: (<b>a</b>) the no-load torque percentage of the engine at different speeds; (<b>b</b>) the engine torque percentage at different speeds in first gear.</p>
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<p>The thrust required for no-load traveling of the whole machine.</p>
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<p>The FCWM at different speeds and thrusts.</p>
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<p>The FCWM at different thrusts.</p>
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<p>The FCWM and rotation at different thrusts.</p>
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<p>The FCWM at different speeds.</p>
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<p>The control strategy of minimum FCWM.</p>
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<p>The optimization control strategy simulation model.</p>
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<p>The set load thrust of the bulldozer.</p>
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<p>The FCWM of the whole machine energy-saving mode.</p>
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<p>The whole machine energy-saving mode: (<b>a</b>) the thrust of the bulldozer; (<b>b</b>) the parameters of the four working points.</p>
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<p>The FCWM of the constant power mode.</p>
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<p>Comparison of the performance of the optimum operating points in different modes.</p>
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<p>The test system for the bulldozer.</p>
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<p>The test data of the bulldozer.</p>
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18 pages, 6972 KiB  
Article
The Design and Experimental Research on a High-Frequency Rotary Directional Valve
by Shunming Hua, Siqiang Liu, Zhuo Qiu, Xiaojun Wang, Xuechang Zhang and Huijuan Zhang
Processes 2024, 12(11), 2600; https://doi.org/10.3390/pr12112600 - 19 Nov 2024
Viewed by 279
Abstract
A directional valve is a core component of the electro-hydraulic shakers in fatigue testing machines, controlling the cylinder or motor that drives the piston for reciprocating linear or rotary motion. In this article, a high-speed rotating directional valve with a symmetrical flow channel [...] Read more.
A directional valve is a core component of the electro-hydraulic shakers in fatigue testing machines, controlling the cylinder or motor that drives the piston for reciprocating linear or rotary motion. In this article, a high-speed rotating directional valve with a symmetrical flow channel layout is designed to optimize the force on the valve core of the directional valve. A comparative analysis is conducted on the flow capacity of valve ports with different shapes. A steady-state hydrodynamic mathematical model is established for the valve core, the theoretical analysis results of which are verified through a Computational Fluid Dynamics (CFD) simulation of the fluid domain inside the directional valve. A prototype of the rotatory directional valve is designed and manufactured, and an experimental platform is built to measure the hydraulic force acting on the valve core to verify the performance of the valve. The displacement curves at different commutation frequencies are also obtained. The experimental results show that the symmetrical flow channel layout can significantly optimize the hydraulic force during the movement of the valve core. Under a pressure of 1 MPa, the hydraulic cylinder driven by the prototype can achieve a sinusoidal curve output with a maximum frequency of 60 Hz and an amplitude of 2.5 mm. The innovation of this design lies in the creation of a directional valve with a symmetric flow channel layout. The feasibility of the design is verified through modeling, simulation, and experimentation, and it significantly optimizes the hydraulic forces acting on the spool. It provides us with the possibility to further improve the switching frequency of hydraulic valves and has important value in engineering applications. Full article
(This article belongs to the Section Manufacturing Processes and Systems)
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<p>Structure of rotary directional valve.</p>
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<p>Valve port shapes.</p>
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<p>Relationship between circular orifice area and valve core angle.</p>
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<p>Relationship between triangle orifice area and valve core angle.</p>
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<p>Relationship between square orifice area and valve core angle.</p>
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<p>The average flow area of the valve port and its ratio to the maximum flow area.</p>
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<p>Fluid domain division.</p>
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<p>Mesh quality test results.</p>
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<p>Cloud diagrams of the valve port velocity with different port openings. (<b>a</b>) The inlet I is used as the pressure inlet. (<b>b</b>) The inlet II is used as the pressure inlet.</p>
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<p>Vector diagrams of liquid flow at different valve openings. (<b>a</b>) The inlet I is used as the pressure inlet. (<b>b</b>) The inlet II is used as the pressure inlet.</p>
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<p>Jet angle and spool torque at different rotation angles. (<b>a</b>) Jet angle curves. (<b>b</b>) Spool torque curves.</p>
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<p>Hydraulic simulation system diagram.</p>
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<p>System flow rate and cylinder amplitude at different commutation frequencies.</p>
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<p>Flow rate and cylinder amplitude at different pressures.</p>
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<p>Flow rate and cylinder amplitude at different loads.</p>
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<p>Test platform. (<b>a</b>) Overview of experimental system. (<b>b</b>) Prototype and sensors.</p>
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<p>Hydraulic cylinder displacement curves at different commutation frequencies.</p>
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<p>The relationship between the steady-state hydraulic torque and the spool rotation angle.</p>
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<p>The torque of the spool at different pressures.</p>
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16 pages, 6119 KiB  
Article
Electronic Dynamic Switching Techniques for Efficient Drive of Asymmetric Three-Phase Motors with Single-Phase Supply
by Wellington do Prado, Geraldo Caixeta Guimarães and Guilherme Henrique Alves
Energies 2024, 17(22), 5769; https://doi.org/10.3390/en17225769 - 19 Nov 2024
Viewed by 344
Abstract
This article presents an analysis of the behavior of an asymmetric machine subjected to dynamic switching at different load levels. The authors herein present theoretical and practical results regarding the drive of a 2 HP asymmetric three-phase induction motor, allowing for conclusions to [...] Read more.
This article presents an analysis of the behavior of an asymmetric machine subjected to dynamic switching at different load levels. The authors herein present theoretical and practical results regarding the drive of a 2 HP asymmetric three-phase induction motor, allowing for conclusions to be drawn concerning its operation in such a configuration using capacitive dynamic switching. Previous research has demonstrated that the efficiency of single-phase powered asymmetric motors is only viable when the applied load matches the rated load of the motor. Given that this mode of operation is shown to hold practical infeasibilities for asymmetric three-phase motors, the proposal of a solution is put forward that involves varying the capacitance according to demand. This approach results in a significant improvement in efficiency regardless of whether the motor is running on a full or reduced load. Full article
(This article belongs to the Section F3: Power Electronics)
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<p>Asymmetric induction machine stator connection details.</p>
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<p>Main system screen.</p>
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<p>Machine torque with load and capacitor variation.</p>
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<p>Step load applied to the motor.</p>
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<p>Asymmetric motor speed with load and capacitor variation.</p>
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<p>Current values during the load stage applied to the motor, yellow current phase A, blue current phase B, orange current phase C.</p>
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<p>Test bench.</p>
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<p>10 hp motor used as load.</p>
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<p>Current at 20% load.</p>
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<p>Speed at 20% load.</p>
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<p>Current at 50% load.</p>
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<p>Speed at 50% load.</p>
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<p>Current at 80% load.</p>
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<p>Speed at 80% load.</p>
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<p>Current at 100% load.</p>
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<p>Speed at 100% load.</p>
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<p>Current at 120% load.</p>
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<p>Speed at 120% load.</p>
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21 pages, 14758 KiB  
Article
Hybrid Control Strategy for LLC Converter Based on Improved Fruit Fly Optimization Algorithm
by Qitong Xue, Pengfei Zhi, Wanlu Zhu, Haifeng Wei, Yi Zhang and Jia Cui
Electronics 2024, 13(22), 4526; https://doi.org/10.3390/electronics13224526 - 18 Nov 2024
Viewed by 252
Abstract
This paper presents a hybrid control strategy for the LLC resonant converter in X-ray machines, addressing the limitations of voltage gain range under Pulse Frequency Modulation (PFM) and dynamic response under Phase Shift Modulation (PSM). The strategy employs an improved fruit fly optimization [...] Read more.
This paper presents a hybrid control strategy for the LLC resonant converter in X-ray machines, addressing the limitations of voltage gain range under Pulse Frequency Modulation (PFM) and dynamic response under Phase Shift Modulation (PSM). The strategy employs an improved fruit fly optimization algorithm (IFOA) to optimize PI control and integrate Hybrid Phase-Shifted and Frequency-Modulated control. It dynamically adjusts the switching frequency and phase shift angle to maintain output stability and efficiency, ensuring optimal operation under rated conditions. A Matlab-based system simulation model confirmed the stability and accuracy of the IFOA in controlling the converter. Subsequent prototype testing validated the strategy’s effectiveness in reducing conduction losses, enhancing overall efficiency, and demonstrating practical feasibility and superiority. Full article
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<p>The overall system framework.</p>
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<p>Hybrid control based on IFOA.</p>
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<p>Full-bridge LLC resonant converter.</p>
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<p>Simplified circuit diagram of LLC resonant converter.</p>
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<p>Gain curves corresponding to different Q values.</p>
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<p>Simulation results of IFOA, FOA, GA, and PSO.</p>
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<p>Flowchart of the IFOA.</p>
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<p>Step response of the system under different methods.</p>
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<p>PSM realizes 360 V buck to 330 V.</p>
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<p>PFM realizes 360 V buck to 330 V.</p>
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<p>Realization of ZVS at PSM buck.</p>
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<p>Realization of ZVS at PFM buck.</p>
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<p>PFM realizes 360 V boost to 390 V.</p>
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<p>PSM realizes 360 V boost to 390 V.</p>
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<p>PFM boost does not realize ZVS.</p>
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<p>PSM boost realizes ZVS.</p>
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<p>Switching from phase shift mode to inverter mode.</p>
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<p>Sub-side rectifier diode realizes ZCS.</p>
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<p>Output 390 V in PFM.</p>
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<p>Comparison of driving waveforms at 420 V and 390 V.</p>
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<p>Output 300 V in PSM.</p>
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<p>Comparison of driving waveforms at 330 V and 300 V.</p>
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<p>Comparison between PI regulation alone and algorithmic optimized PI regulation.</p>
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<p>Test environment.</p>
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<p>Block diagram of a test connection structure.</p>
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<p>Efficiency of LLC converter with hybrid control added vs. efficiency of LLC converter without hybrid control added.</p>
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<p>X-ray machine three-stage boost waveforms.</p>
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<p>X-ray metrology stability test results.</p>
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21 pages, 8877 KiB  
Article
The Effect of the Number of Parallel Winding Paths on the Fault Tolerance of a Switched Reluctance Motor
by Mariusz Korkosz, Jan Prokop and Piotr Bogusz
Energies 2024, 17(22), 5701; https://doi.org/10.3390/en17225701 - 14 Nov 2024
Viewed by 336
Abstract
Achieving increased fault tolerance in an electric motor requires decisions to be made about the type and specifications of the motor machine and its appropriate design. Depending on the type of motor, there are generally three ways to achieve an increased resistance of [...] Read more.
Achieving increased fault tolerance in an electric motor requires decisions to be made about the type and specifications of the motor machine and its appropriate design. Depending on the type of motor, there are generally three ways to achieve an increased resistance of the drive system to tolerate resulting faults. The simplest way is to select the right motor and design it appropriately. Switched reluctance motors (SRMs) have a high tolerance for internal faults (in the motor windings). Failure tolerance can be improved by using parallel paths. The SRM 24/16 solution has been proposed, which allows for operation with four parallel paths. In this paper, a mathematical model designed to analyse the problem under consideration is provided. Based on numerical calculations, the influence of typical faults (open and partial short circuit in one of the paths) on the electromagnetic torque generated as well as its ripple and (source and phase) currents were determined. The higher harmonics of the source current (diagnostic signal) were determined. Laboratory tests were performed to verify the various configurations for the symmetric and emergency operating states. The feasibility of SRM correct operation monitoring was determined from an FFT analysis of the source current. Full article
(This article belongs to the Special Issue Reliability and Condition Monitoring of Electric Motors and Drives)
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<p>SRM 24/16: (<b>a</b>) cross section; (<b>b</b>) physical prototype.</p>
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<p>Winding configuration (<b>a</b>) <span class="html-italic">a</span> = 1, (<b>b</b>) <span class="html-italic">a</span> = 2, (<b>c</b>) <span class="html-italic">a</span> = 4.</p>
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<p>Power converter for SRM.</p>
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<p>Waveforms of the electromagnetic torque at <span class="html-italic">a</span> = 1.</p>
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<p>Waveforms of phase and SC current at <span class="html-italic">a</span> = 1.</p>
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<p>Waveforms of the electromagnetic torque at <span class="html-italic">a</span> = 2.</p>
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<p>Waveforms of phase current at <span class="html-italic">a</span> = 2.</p>
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<p>Waveforms of the branch and SC current at <span class="html-italic">a</span> = 2.</p>
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<p>Waveforms of electromagnetic torque at <span class="html-italic">a</span> = 4.</p>
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<p>Waveforms of the phase current at <span class="html-italic">a</span> = 4.</p>
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<p>Waveforms of the winding path and the SC current at <span class="html-italic">a</span> = 4.</p>
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<p>Waveforms of the DC current at <span class="html-italic">a</span> = 1.</p>
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<p>FFT of the DC current at <span class="html-italic">a</span> = 1.</p>
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<p>Waveforms of the DC current at <span class="html-italic">a</span> = 2.</p>
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<p>FFT of the DC current at <span class="html-italic">a</span> = 2.</p>
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<p>Waveforms of the DC current at <span class="html-italic">a</span> = 4.</p>
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<p>FFT of the DC current at <span class="html-italic">a</span> = 4.</p>
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<p>Laboratory test stand.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 1 SYM in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 1 SC in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 1 OC in the laboratory test.</p>
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<p>FFT of the DC currents for <span class="html-italic">a</span> = 1 in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 2 SYM in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 2 SC in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 2 OC in the laboratory test.</p>
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<p>FFT of DC currents for <span class="html-italic">a</span> = 2 in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 4 SYM in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 4 SC in the laboratory test.</p>
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<p>Waveforms of phase and DC currents for <span class="html-italic">a</span> = 4 OC in the laboratory test.</p>
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<p>Waveforms of the winding path currents Ph1 for <span class="html-italic">a</span> = 4 SC in the laboratory test.</p>
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<p>Waveforms of the winding path currents Ph2 for <span class="html-italic">a</span> = 4 SC in the laboratory test.</p>
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<p>Waveforms of the winding path currents Ph3 for <span class="html-italic">a</span> = 4 SC in the laboratory test.</p>
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<p>FFT of DC currents for <span class="html-italic">a</span> = 4 in the laboratory test.</p>
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18 pages, 4159 KiB  
Article
Preclinical Implementation of matRadiomics: A Case Study for Early Malformation Prediction in Zebrafish Model
by Fabiano Bini, Elisa Missori, Gaia Pucci, Giovanni Pasini, Franco Marinozzi, Giusi Irma Forte, Giorgio Russo and Alessandro Stefano
J. Imaging 2024, 10(11), 290; https://doi.org/10.3390/jimaging10110290 - 14 Nov 2024
Viewed by 438
Abstract
Radiomics provides a structured approach to support clinical decision-making through key steps; however, users often face difficulties when switching between various software platforms to complete the workflow. To streamline this process, matRadiomics integrates the entire radiomics workflow within a single platform. This study [...] Read more.
Radiomics provides a structured approach to support clinical decision-making through key steps; however, users often face difficulties when switching between various software platforms to complete the workflow. To streamline this process, matRadiomics integrates the entire radiomics workflow within a single platform. This study extends matRadiomics to preclinical settings and validates it through a case study focused on early malformation differentiation in a zebrafish model. The proposed plugin incorporates Pyradiomics and streamlines feature extraction, selection, and classification using machine learning models (linear discriminant analysis—LDA; k-nearest neighbors—KNNs; and support vector machines—SVMs) with k-fold cross-validation for model validation. Classifier performances are evaluated using area under the ROC curve (AUC) and accuracy. The case study indicated the criticality of the long time required to extract features from preclinical images, generally of higher resolution than clinical images. To address this, a feature analysis was conducted to optimize settings, reducing extraction time while maintaining similarity to the original features. As a result, SVM exhibited the best performance for early malformation differentiation in zebrafish (AUC = 0.723; accuracy of 0.72). This case study underscores the plugin’s versatility and effectiveness in early biological outcome prediction, emphasizing its applicability across biomedical research fields. Full article
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<p>The workflow of the extended version of matRadiomics for preclinical studies.</p>
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<p>Mean relative error for each feature for the two different preprocessing methods.</p>
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<p>Mean relative error for bin count equal to one and equal to sixty-four.</p>
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<p>Mean relative error on features for the first and the second zebrafish dataset.</p>
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<p>Example of all_fish (<b>a</b>), heart (<b>b</b>), head (<b>c</b>), eye (<b>d</b>), yolk (<b>e</b>), and length (<b>f</b>) masks used in the study.</p>
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<p>(<b>a</b>) The window that appears to manually assign the name of the mask for the analysis of the first image. (<b>b</b>) The window with the list of masks used after the extraction of the features of the first image.</p>
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<p>Example of bar plot for selected features for all masks without all_fish mask. In red, the feature selected using the PBC method.</p>
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<p>Example of performance of the predictive model for the all_fish mask based on the ROC curve, precision and confusion matrix.</p>
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<p>The best results obtained for each mask, together with the corresponding image, the selected features, and the predictive ML model that achieves the highest performance.</p>
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17 pages, 37894 KiB  
Article
High-Precision Rotor Position Fitting Method of Permanent Magnet Synchronous Machine Based on Hall-Effect Sensors
by Kaining Qu, Pengfei Pang and Wei Hua
Energies 2024, 17(22), 5625; https://doi.org/10.3390/en17225625 - 10 Nov 2024
Viewed by 571
Abstract
The high-performance vector control technology of permanent magnet synchronous machines (PMSMs) relies on high-precision rotor position. The Hall-effect sensor has the advantages of low cost, simple installation, and strong anti-interference ability. However, it can only provide six discrete rotor angles in an electrical [...] Read more.
The high-performance vector control technology of permanent magnet synchronous machines (PMSMs) relies on high-precision rotor position. The Hall-effect sensor has the advantages of low cost, simple installation, and strong anti-interference ability. However, it can only provide six discrete rotor angles in an electrical cycle, which makes high-precision vector control of PMSMs difficult. Hence, to obtain the necessary rotor position of PMSMs, a rotor position fitting method combining the Hall signal and machine flux information is proposed. Firstly, the rotor position signal output by the Hall-effect sensors is used to calibrate and update the stator flux obtained under pure integration. Then, based on the corrected stator flux and its relationship with current and angle, the rotor position and speed are obtained. Experimental verification shows that the rotor position observer combining Hall signal and flux information can reduce the initial value bias and integral drift caused by traditional average speed method hysteresis and pure integration method calculation of flux and can quickly and accurately track and estimate the rotor position, achieving high-performance vector control of PMSMs. Full article
(This article belongs to the Special Issue Designs and Control of Electrical Machines and Drives)
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<p>Hall-effect Sensors.</p>
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<p>Hall installation mode and output signals (<b>a</b>) 120° Hall-effect installation, (<b>b</b>) Hall-effect output signals.</p>
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<p>Relation of Hall signal and rotor position.</p>
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<p>Estimation principle by average velocity method.</p>
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<p>Hall signal delay under digital control system.</p>
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<p>Structure of position vector tracking observer.</p>
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<p>Bode diagram of position vector tracking observer based on back EMF.</p>
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<p>Stator flux observer combined with flux linkage information and Hall signal.</p>
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<p>Input voltage calculation for the flux observer.</p>
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<p>Rotor position observer combined with flux linkage information and Hall signal.</p>
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<p>The experiment platform.</p>
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<p>Flux linkage waveforms under three conditions (<b>a</b>) Flux linkage before correction, (<b>b</b>) Flux linkage at discrete Hall points, (<b>c</b>) Flux linkage under Hall signal correction.</p>
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<p>Comparison of no-load starting rotor positions (<b>a</b>) Average speed, (<b>b</b>) Vector tracking, (<b>c</b>) Flux-Hall.</p>
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<p>Comparison of on-rated-load starting rotor positions.</p>
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<p>Estimated rotor angle errors under three initial positions (<b>a</b>) The Hall intermediate angle, (<b>b</b>) 25° advanced, (<b>c</b>) 25° delayed.</p>
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<p>Comparison of <math display="inline"><semantics> <mrow> <mi>d</mi> <mi>q</mi> </mrow> </semantics></math>-frame currents waveforms. Comparison of <math display="inline"><semantics> <mrow> <mi>d</mi> <mi>q</mi> </mrow> </semantics></math>-frame currents waveforms (<b>a</b>) Average speed, (<b>b</b>) Flux-Hall.</p>
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<p>Comparison of rotor positions under a speed change from 300/min to 1800/min (<b>a</b>) Average speed, (<b>b</b>) Flux-Hall, (<b>c</b>) Angle error.</p>
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<p>Rotor position during forward and reverse switching (<b>a</b>) Average speed, (<b>b</b>) Flux-Hall.</p>
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<p>Stator current and rotor position at 750/min (<b>a</b>) Average speed, (<b>b</b>,<b>c</b>) Flux-Hall.</p>
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<p>Rotor position under different inductance (<b>a</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>L</mi> </mrow> <mo stretchy="false">^</mo> </mover> <mo>=</mo> <mn>0.8</mn> <mi>L</mi> </mrow> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>L</mi> </mrow> <mo stretchy="false">^</mo> </mover> <mo>=</mo> <mn>1.2</mn> <mi>L</mi> </mrow> </semantics></math>, (<b>c</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>L</mi> </mrow> <mo stretchy="false">^</mo> </mover> <mo>=</mo> <mi>L</mi> </mrow> </semantics></math>.</p>
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<p>Rotor position under different resistance (<b>a</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>R</mi> </mrow> <mo stretchy="false">^</mo> </mover> <mo>=</mo> <mn>0.8</mn> <mi>R</mi> </mrow> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>R</mi> </mrow> <mo stretchy="false">^</mo> </mover> <mo>=</mo> <mn>1.2</mn> <mi>R</mi> </mrow> </semantics></math>, (<b>c</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>R</mi> </mrow> <mo stretchy="false">^</mo> </mover> <mo>=</mo> <mi>R</mi> </mrow> </semantics></math>.</p>
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22 pages, 7935 KiB  
Article
Cycle Time-Based Fault Detection and Localization in Pneumatic Drive Systems
by Vladimir Boyko and Jürgen Weber
Actuators 2024, 13(11), 447; https://doi.org/10.3390/act13110447 - 7 Nov 2024
Viewed by 517
Abstract
Compressed air ranks among the most expensive forms of energy. In recent decades, increased efforts have been made to enhance the overall energy efficiency of pneumatic actuator systems and develop reliable fault detection methods for preventing energy losses. However, most of the methods [...] Read more.
Compressed air ranks among the most expensive forms of energy. In recent decades, increased efforts have been made to enhance the overall energy efficiency of pneumatic actuator systems and develop reliable fault detection methods for preventing energy losses. However, most of the methods developed so far require additional sensors, resulting in extra costs, and/or are not applicable during machine operation, which leads to their limited use in the industry. This article introduces a cycle time-based method for detecting faults in pneumatic actuators through the use of proximity switches, enabling cost-effective monitoring in real time without the necessity of further sensors. A systematic analysis is conducted, expanding the current state of knowledge by detailing the influence of all potential leakage points on the movement times of a pneumatic drive and taking into account the different velocity control strategies (meter-out and meter-in) and operating points expressed via the pneumatic frequency ratio. Previously unassessed specifics of internal leakage, including the impact of pressure profiles and differences between differential cylinders and cylinder with equal piston areas, are also presented. The applicability of the proposed method and its detection limits in an industrial environment are examined using pneumatic assembly machines. Full article
(This article belongs to the Section High Torque/Power Density Actuators)
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<p>Potential fault locations within a pneumatic drive (symbolic depiction): (1) external leakage in piston-side chamber A; (2) internal (interchamber) leakage; (3) external leakage in rod-side chamber B; (4 and 5) external leakages between the directional valve and the throttle valves; (6) increased friction.</p>
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<p>Test bench for investigating cycle time-based fault detection with corresponding fault locations.</p>
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<p>Influence of external leakage <span class="html-italic">Q<sub>ext</sub></span> = 20 L/min between cylinder and throttle check valve with meter-out throttling on cylinder pressure and position: (<b>a</b>) piston side A (fault location 1); (<b>b</b>) rod side B (fault location 3).</p>
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<p>Influence of external leakage <span class="html-italic">Q<sub>ext</sub></span> = 20 L/min between directional control valve and throttle check valve with meter-out throttling on cylinder pressure and position: (<b>a</b>) piston side A (fault location 4); (<b>b</b>) rod side B (fault location 5).</p>
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<p>Influence of internal leakage <span class="html-italic">Q<sub>int</sub></span> = 40 L/min in the cylinder (fault location 3) on the meter-out throttled cylinder’s pressure and position.</p>
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<p>Influence of increased piston friction <span class="html-italic">F<sub>add,fr</sub></span> = 20 N (fault location 6) on the meter-out throttled cylinder’s pressure and position.</p>
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<p>Equal delay in the extension and retraction time in case of internal leakage <span class="html-italic">Q<sub>int</sub></span> = 40 L/min in the rodless cylinder Festo DGC-18-200-G-PPV-A with meter-out throttling.</p>
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<p>Influence of external leakage <span class="html-italic">Q<sub>ext</sub></span> = 20 L/min between cylinder and throttle check valve with meter-in throttling on cylinder pressure and position: (<b>a</b>) piston side A (fault location 1); (<b>b</b>) rod side B (fault location 3).</p>
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<p>Influence of external leakage between directional control valve and throttle check valve with meter-in throttling on cylinder pressure and position: (<b>a</b>) piston side A (fault location 4); (<b>b</b>) rod side B (fault location 5).</p>
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<p>Influence of (<b>a</b>) internal leakage <span class="html-italic">Q<sub>int</sub></span> = 30 L/min in the cylinder (fault location 3) and (<b>b</b>) increased piston friction <span class="html-italic">F<sub>add,fr</sub></span> = 20 N (fault location 6) on the meter-in throttled cylinder’s pressure and position.</p>
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<p>Influence of the pneumatic frequency ratio <span class="html-italic">Ω</span> on changes in the movement time of the Ø25 × 50 Hoerbiger R6025/50 differential pneumatic cylinder for different fault locations and at constant fault values. Meter-out throttling: (<b>a</b>) fault location 1; (<b>b</b>) fault location 3; (<b>c</b>) fault location 4; (<b>d</b>) fault location 5; (<b>e</b>) fault location 2; (<b>f</b>) fault location 6. Meter-in throttling: (<b>g</b>) fault location 1; (<b>h</b>) fault location 3; (<b>i</b>) fault location 4; (<b>j</b>) fault location 5; (<b>k</b>) fault location 2; (<b>l</b>) fault location 6.</p>
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<p>(<b>a</b>) Influence of internal leakage on the extension time change of different pneumatic differential cylinders with meter-out throttling as a function of the pneumatic frequency ratio <span class="html-italic">Ω</span>, changes in pressure and position profiles, and interchamber flow direction in (<b>b</b>) well-sized cylinder with <span class="html-italic">Ω</span> &lt; 1.5; (<b>c</b>) well-sized cylinder with <span class="html-italic">Ω</span> = 1.5; (<b>d</b>) oversized cylinder with <span class="html-italic">Ω</span> &gt; 1.5.</p>
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<p>Influence of internal leakage on the extension time change of different pneumatic differential cylinders with meter-out throttling as a function of the mean piston velocity <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>x</mi> </mrow> <mo>˙</mo> </mover> </mrow> </semantics></math>.</p>
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<p>Change in the movement time of the Ø25 × 50 Hoerbiger R6025/50 differential pneumatic cylinder at <span class="html-italic">Ω</span> = 1.3 as a function of leakage rate. Meter-out throttling: (<b>a</b>) fault location 1; (<b>b</b>) fault location 3; (<b>c</b>) fault location 4; (<b>d</b>) fault location 5; (<b>e</b>) fault location 2. Meter-in throttling: (<b>f</b>) fault location 1; (<b>g</b>) fault location 3; (<b>h</b>) fault location 4; (<b>i</b>) fault location 5; (<b>j</b>) fault location 2.</p>
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<p>Algorithm for time-based fault detection and localization in pneumatic drives with well-sized, double-acting differential cylinders (PFR <span class="html-italic">Ω</span> ≤ 1.5) and meter-out throttling.</p>
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<p>Algorithm for time-based fault detection and localization in pneumatic drives with oversized, double-acting differential cylinders (PFR <span class="html-italic">Ω</span> &gt; 1.5) and meter-out throttling.</p>
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<p>Algorithm for time-based fault detection and localization in pneumatic drives with double-acting differential cylinders (all PFR values) and meter-in throttling.</p>
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<p>Handling system (<b>a</b>) and its motion sequence (<b>b</b>).</p>
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<p>Changes in cycle time of pneumatic actuators and supply pressure of the handling system as well as room temperature during fault-free operation.</p>
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<p>(<b>a</b>) Pneumatic system for fully automated assembly of a fuel cell stack by XENON Automatisierungstechnik GmbH [<a href="#B39-actuators-13-00447" class="html-bibr">39</a>]; (<b>b</b>) external leakage generation at cylinder 1 (flap actuator).</p>
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<p>Above: Changes in cycle time of pneumatic actuators of the assembly machine resulting from external piston-side leakage in chamber A before and after the throttle valve; below: corresponding fault recognition paths of the algorithms.</p>
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20 pages, 3080 KiB  
Article
Research on Active–Passive Training Control Strategies for Upper Limb Rehabilitation Robot
by Yongming Yang
Machines 2024, 12(11), 784; https://doi.org/10.3390/machines12110784 - 6 Nov 2024
Viewed by 357
Abstract
Due to accidents, upper limb movement disorders have become increasingly common. Training can help restore muscle strength and rebuild neurological function. However, the existing single mode has limitations in adapting to the training needs of different rehabilitation stages. Therefore, this paper conducts research [...] Read more.
Due to accidents, upper limb movement disorders have become increasingly common. Training can help restore muscle strength and rebuild neurological function. However, the existing single mode has limitations in adapting to the training needs of different rehabilitation stages. Therefore, this paper conducts research on active–passive training control strategies for an upper limb rehabilitation robot. It establishes an upper limb kinematic model based on the Lagrange method and builds a man–machine integration dynamics model for upper limb rehabilitation in MATLAB (R2016a)/Simulink. A design active controller, passive controller, and switching controller based on PI and feedforward compensation strategies are proposed to improve training control accuracy. The output moment of the system during active training is planned to ensure the safety and stability of the training process. By utilizing neural networks to train sample data during rehabilitation training, the fuzzy rules and membership functions in fuzzy intention recognition algorithm are optimized to improve the accuracy of intention recognition during training. By adopting the independently developed experimental platform for the upper limb rehabilitation robot, active–passive training, intention recognition, and training mode switching are achieved. The results show that the active and passive training processes are smooth, the training intention recognition is accurate, and the switching between active and passive training modes is steady. This verifies the feasibility and effectiveness of the established mathematical model in upper limb rehabilitation training. Full article
(This article belongs to the Special Issue Advancements in Mechanical Power Transmission and Its Elements)
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<p>Upper limb plane model.</p>
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<p>Upper limb man–machine integration model.</p>
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<p>Motor model.</p>
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<p>Upper limb man–machine integration dynamics model.</p>
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<p>Active–passive training control scheme.</p>
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<p>Active controller.</p>
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<p>Passive controller.</p>
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<p>Active–passive training switching controller.</p>
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<p>ANFIS schematic diagram.</p>
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<p>Characteristic curve of man–machine interaction moment under passive training.</p>
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<p>Neural fuzzy network structure.</p>
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<p>Neural network training error.</p>
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<p>Membership function during active training: (<b>a</b>) speed membership function and (<b>b</b>) speed change rate membership function.</p>
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<p>Membership function during passive training: (<b>a</b>) moment membership function and (<b>b</b>) moment change rate membership function.</p>
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<p>Mechanical structure diagram of the upper limb rehabilitation robot.</p>
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<p>Independently developed upper limb rehabilitation robot experimental platform.</p>
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<p>Active–passive training process: (<b>a</b>) contracted state, (<b>b</b>) intermediate state, (<b>c</b>) extended state.</p>
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<p>Training results (the training coefficient is set as 0.25): (<b>a</b>) training resistance moment and (<b>b</b>) training speed.</p>
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<p>Training results (the training coefficient is set as 0.45): (<b>a</b>) training resistance moment and (<b>b</b>) training speed.</p>
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<p>Passive training experimental data.</p>
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<p>Experimental results of speed and speed change rate (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.2, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 2 N∙m).</p>
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<p>Intention recognition results (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.2, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 2 N∙m).</p>
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<p>Experimental results of speed and speed change rate (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.5, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 5 N∙m).</p>
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<p>Intention recognition results (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.5, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 5 N∙m).</p>
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<p>Experimental results of speed and speed change rate (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.5, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 5 N∙m).</p>
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<p>Experimental results of speed and speed change rate (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.5, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 5 N∙m).</p>
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<p>Experimental results of speed and speed change rate (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.5, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 5 N∙m).</p>
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<p>Experimental results of speed and speed change rate (<math display="inline"><semantics> <mrow> <msub> <mi>C</mi> <mi>t</mi> </msub> </mrow> </semantics></math> = 0.5, <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <mi>d</mi> </msub> </mrow> </semantics></math> = 5 N∙m).</p>
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22 pages, 5486 KiB  
Article
Control of Large Wind Energy Converters for Aeroacoustic Noise Mitigation with Minimal Power Reduction
by Andrea Rivarola and Adrian Gambier
Energies 2024, 17(22), 5530; https://doi.org/10.3390/en17225530 - 5 Nov 2024
Viewed by 452
Abstract
The population is often opposed to wind turbines being erected near their homes, mainly because the machines are noisy, especially at night. In an effort to establish a compromise between the needs of the people and the fulfilment of energy demands, wind turbines [...] Read more.
The population is often opposed to wind turbines being erected near their homes, mainly because the machines are noisy, especially at night. In an effort to establish a compromise between the needs of the people and the fulfilment of energy demands, wind turbines have the ability to switch between day and night operation by reducing the rotation speed during the night, resulting in a loss of generated power. The present study investigates simple models for noise emission, propagation, and prediction, with the objective of proposing a control system configuration that continuously adjusts the rotational speed as much as necessary until it matches sound level regulations while minimising power losses. Thus, several approaches are implemented and tested with a very large reference wind turbine. The simulation results of a reference wind turbine show that the approaches provide significant improvements in sound reduction as well as in power conversion. Full article
(This article belongs to the Topic Advances in Wind Energy Technology)
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<p>Classic pitch control system [<a href="#B9-energies-17-05530" class="html-bibr">9</a>].</p>
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<p>Up/down-regulated power control system in cascade configuration [<a href="#B21-energies-17-05530" class="html-bibr">21</a>].</p>
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<p>Active sound damping control in cascade configuration [<a href="#B15-energies-17-05530" class="html-bibr">15</a>].</p>
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<p>Active sound damping control with CPC and inverse formula for setpoint calculation.</p>
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<p>Switching control scheme between up/down-regulated power and ASDC.</p>
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<p>Active sound damping control with variable reference.</p>
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<p>Control configuration for masked wind turbine noise.</p>
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<p>(<b>a</b>) Generator speed; (<b>b</b>) sound pressure level; (<b>c</b>) electrical power. All for the input space (<span class="html-italic">T<sub>g</sub></span>, <span class="html-italic">β</span>) and a defined wind speed <span class="html-italic">v<sub>w</sub></span><sub>0</sub>.</p>
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<p>Active sound damping control with CPC and inverse proportional torque control.</p>
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<p>Schematic description of the 20 MW wind turbine.</p>
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<p>(<b>a</b>) Generator torque; (<b>b</b>) generator speed; (<b>c</b>) electrical power. All variables depend on the wind speed.</p>
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<p>Results of Experiment 1. (<b>a</b>) Generator speed. (<b>b</b>) Sound pressure level. (<b>c</b>) Power output.</p>
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<p>Results of Experiment 2. (<b>a</b>) Generator speed. (<b>b</b>) Sound pressure level. (<b>c</b>) Power output.</p>
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<p>Results of Experiment 3. (<b>a</b>) Generator speed. (<b>b</b>) Sound pressure level. (<b>c</b>) Power output.</p>
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<p>Results of Experiment 3 (masked wind turbine noise). (<b>a</b>) Generator speed. (<b>b</b>) Sound pressure level. (<b>c</b>) Power output.</p>
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<p>Results of Experiment 4. (<b>a</b>) Generator speed. (<b>b</b>) Sound pressure level. (<b>c</b>) Power output.</p>
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14 pages, 4238 KiB  
Article
Influence of Opening Time Interval of Gate Signals on Suppression of Horizontally Polarized Signal of Infrared Pulsed Laser
by Xinyang Wu, Dongdong Wang, Di Song, Jiaqi Wang, Jiawei Guo, Peng Ren, He Cai, Yaqing Jin, Yonghong Yu, You Wang and Jing Liu
Materials 2024, 17(21), 5276; https://doi.org/10.3390/ma17215276 - 30 Oct 2024
Viewed by 360
Abstract
Since the beginning of the 21st century, infrared Nd:YVO4 pulsed lasers have been widely applied, especially in some actual industrial processes. In the working process of a laser-aided etching device, the “match-head” effect must be effectively controlled by suppressing the first giant [...] Read more.
Since the beginning of the 21st century, infrared Nd:YVO4 pulsed lasers have been widely applied, especially in some actual industrial processes. In the working process of a laser-aided etching device, the “match-head” effect must be effectively controlled by suppressing the first giant pulse for a solid-state Q-switched laser. In the process of optimizing the infrared Nd:YVO4 pulsed laser by adjusting the slope parameters of the radio frequency (RF) modulation to suppress the first giant pulse, it has been found that an abnormal horizontally polarized emission with a very short time appears before the formal vertically polarized emission when the gate signal is artificially started. Actually, abnormal horizontally polarized emissions will bring some unexpected machining traces during the production process and even greater dangers. The experimental results show that with the increase in the slope duration of an RF signal, the existence time of abnormal output horizontally polarized light will be shortened, and the horizontal giant pulse and vertical giant pulse are well suppressed. When the slope duration is greater than 0.18 ms, both horizontal and vertical giant pulses will disappear. The horizontally polarized light can be thoroughly suppressed when the slope duration is greater than 13.7 ms. Compared with the method of adding a polarizer to eliminate abnormal output horizontally polarized light, this method does not add elements in the laser, ensuring that the laser volume is relatively small, and does not affect the quality of the normal output laser. The research conclusion is thought to be of great practical significance, especially for processing transparent materials. Full article
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<p>The energy level structure of the Nd:YVO<sub>4</sub> crystal (v: the energy of each sub-level; f<sub>i</sub>: the proportion of the sub-level in the main level).</p>
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<p>The axial structure of the Nd:YVO<sub>4</sub> crystal in our study.</p>
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<p>Schematic illustration of the experimental setup.</p>
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<p>Gate signal and RF signal in our experiment.</p>
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<p>(<b>a</b>) When slope duration = 5.0 μs, a vertical polarizer is added to the output end of the laser. (<b>b</b>) Slope duration adjusted to 16.0 μs. (<b>c</b>) Slope duration adjusted to 28.0 μs. (<b>d</b>) Slope duration adjusted to 100.0 μs. (<b>e</b>) Slope duration adjusted to 0.18 ms. (<b>f</b>) Slope duration adjusted to 0.75 ms (red line: gate signal; blue line: RF signal; yellow line: vertically polarized light).</p>
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<p>Slope duration of RF signals versus the giant pulse intensity along the vertical polarized direction.</p>
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<p>(<b>a</b>) When slope duration = 5.0 μs, a horizontal polarizer is added to the output end of the laser. (<b>b</b>) Slope duration adjusted to 28.0 μs. (<b>c</b>) Slope duration adjusted to 0.18 ms. (<b>d</b>) Slope duration adjusted to 2.0 ms. (<b>e</b>) Slope duration adjusted to 5.0 ms. (<b>f</b>) Slope duration adjusted to 13.7 ms. (<b>e</b>,<b>f</b>) are 50 times magnification (red line: gate signal; blue line: RF signal; yellow line: horizontally polarized light).</p>
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<p>Giant pulse and abnormal output lasing emission along the horizontally polarized direction versus the slope duration of RF signals.</p>
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<p>Relationship between focal length of thermal lens and average pump power.</p>
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<p>Schematic diagram of Nd:YVO<sub>4</sub> laser resonator.</p>
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<p>Radius of a fundamental beam at the RM versus the focal length of a Thermally Induced Lens of the Nd:YVO<sub>4</sub> crystal in our study.</p>
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<p>Relationship between the slope duration of the RF signal and the generation of the giant pulse and horizontally polarized emission.</p>
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18 pages, 7643 KiB  
Article
Intelligent Control Framework for Improving Energy System Stability Through Deep Learning-Based Modal Optimization Scheme
by Arman Fathollahi
Sustainability 2024, 16(21), 9392; https://doi.org/10.3390/su16219392 - 29 Oct 2024
Viewed by 595
Abstract
Ensuring the stability of power systems is essential to promote energy sustainability. The integrated operation of these systems is critical in sustaining modern societies and economies, responding to the increasing demand for electricity and curbing environmental consequences. This study focuses on the optimization [...] Read more.
Ensuring the stability of power systems is essential to promote energy sustainability. The integrated operation of these systems is critical in sustaining modern societies and economies, responding to the increasing demand for electricity and curbing environmental consequences. This study focuses on the optimization of energy system stability through the coordination of power system stabilizers (PSSs) and power oscillation dampers (PODs) in a single-machine infinite bus energy grid configuration that has flexible AC alternating current transmission system (FACTS) devices. Intelligent control strategies using PSS and POD techniques are suggested to increase power system stability and generate supplementary control signals for both the generator excitation system and FACTS device switching control. An intelligent optimal modal control framework equipped with deep learning methods is introduced to control the generator excitation system and thyristor-controlled series capacitor (TCSC). By optimally choosing the weighting matrix Q and implementing close-loop pole shifting, an optimal modal control approach is formulated. To harness its adaptive potential in fine-tuning controller parameters, an auxiliary deep learning-based optimization algorithm with actor–critic architecture is implemented. This comprehensive technique provides a promising path to effectively reduce electromechanical oscillations, thereby enhancing voltage regulation and transient stability in power systems. Full article
(This article belongs to the Section Energy Sustainability)
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<p>Power system configuration with TCSC integration.</p>
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<p>The Heffron–Phillips conversion of the proposed power system with multi-band PSS2B and TCSC integration.</p>
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<p>Multi-band PSS2B stabilizer’s speed converter block representation.</p>
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<p>TCSC circuit structure and its voltage–current relationship.</p>
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<p>The eigenvalue operation area for <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="script">l</mi> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="script">l</mi> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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<p>The basic procedures of the QL algorithm.</p>
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<p>The framework of the auxiliary deep learning optimization algorithm with an actor–critic architecture.</p>
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<p>Schematic block diagram including a CPSS and an AVR.</p>
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<p>Schematic block diagram including conventional POD.</p>
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<p>Rotor angular deviation, rotor speed deviation, and transient <span class="html-italic">q</span>-axis voltage deviation responses of the power system to a 10% shift in the mechanical input power.</p>
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<p>Rotor angular deviation and rotor speed deviation responses of the power system to a 15% shift in the terminal voltage of the synchronous generator.</p>
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<p>Rotor angular deviation and rotor speed deviation responses of the power system to a 30% and 50% shift in the mechanical input power.</p>
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<p>Rotor angular deviation and rotor speed deviation responses of the power system to a 50% shift in the mechanical input power and a change in <math display="inline"><semantics> <mrow> <msub> <mrow> <mover> <mi>X</mi> <mo>´</mo> </mover> </mrow> <mi>d</mi> </msub> </mrow> </semantics></math>.</p>
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15 pages, 535 KiB  
Article
Thought-Controlled Computer Applications: A Brain–Computer Interface System for Severe Disability Support
by Kais Belwafi and Fakhreddine Ghaffari
Sensors 2024, 24(20), 6759; https://doi.org/10.3390/s24206759 - 21 Oct 2024
Viewed by 859
Abstract
This study introduces an integrated computational environment that leverages Brain–Computer Interface (BCI) technology to enhance information access for individuals with severe disabilities. Traditional assistive technologies often rely on physical interactions, which can be challenging for this demographic. Our innovation focuses on creating new [...] Read more.
This study introduces an integrated computational environment that leverages Brain–Computer Interface (BCI) technology to enhance information access for individuals with severe disabilities. Traditional assistive technologies often rely on physical interactions, which can be challenging for this demographic. Our innovation focuses on creating new assistive technologies that use novel Human–Computer interfaces to provide a more intuitive and accessible experience. The proposed system offers four key applications to users controlled by four thoughts: an email client, a web browser, an e-learning tool, and both command-line and graphical user interfaces for managing computer resources. The BCI framework translates ElectroEncephaloGraphy (EEG) signals into commands or events using advanced signal processing and machine learning techniques. These identified commands are then processed by an integrative strategy that triggers the appropriate actions and provides real-time feedback on the screen. Our study shows that our framework achieved an 82% average classification accuracy using four distinct thoughts of 62 subjects and a 95% recognition rate for P300 signals from two users, highlighting its effectiveness in translating brain signals into actionable commands. Unlike most existing prototypes that rely on visual stimulation, our system is controlled by thought, inducing brain activity to manage the system’s Application Programming Interfaces (APIs). It switches to P300 mode for a virtual keyboard and text input. The proposed BCI system significantly improves the ability of individuals with severe disabilities to interact with various applications and manage computer resources. Our approach demonstrates superior performance in terms of classification accuracy and signal recognition compared to existing methods. Full article
(This article belongs to the Special Issue Advanced Non-Invasive Sensors: Methods and Applications)
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<p>General overview of the proposed framework.</p>
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<p>Finite state machine of the proposed framework.</p>
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<p>The proposed MI-EEG signal processing chain.</p>
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<p>Confusion Matrices for Different Models.</p>
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17 pages, 6972 KiB  
Article
Knowledge Graph Completion for High-Speed Railway Turnout Switch Machine Maintenance Based on the Multi-Level KBGC Model
by Haixiang Lin, Jijin Bao, Nana Hu, Zhengxiang Zhao, Wansheng Bai and Dong Li
Actuators 2024, 13(10), 410; https://doi.org/10.3390/act13100410 - 11 Oct 2024
Viewed by 453
Abstract
The incompleteness of the existing knowledge graphs in the railway domain creates information gaps, impacting their quality and effectiveness in the operation and maintenance of high-speed railway turnout switch machines. To address this, we propose a multi-layer model (KBGC) that combines KG-BERT, graph [...] Read more.
The incompleteness of the existing knowledge graphs in the railway domain creates information gaps, impacting their quality and effectiveness in the operation and maintenance of high-speed railway turnout switch machines. To address this, we propose a multi-layer model (KBGC) that combines KG-BERT, graph attention network (GAT), and Convolutional Embedding Network (ConvE) for knowledge graph completion in railway maintenance. KG-BERT fine-tunes a pre-trained BERT model to extract deep semantic features from entities and relationships, converting them into graph structures. GAT captures key structural relationships between nodes using an attention mechanism, producing enriched semantic and structural embeddings. Finally, ConvE reshapes and convolves these embeddings to learn complex entity interactions, enabling accurate link prediction. Extensive experiments on the HRTOM dataset, containing triplet data from high-speed railway turnout switch machines, demonstrate the model’s effectiveness, achieving an MRR of 50.8% and a Hits@10 of 60.7%. These findings show that the KBGC model significantly improves knowledge graph completion, aiding railway maintenance personnel in decision making and preventive maintenance, and providing new tools for railway maintenance applications. Full article
(This article belongs to the Section Actuators for Land Transport)
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<p>High-speed railway turnout switch machine operation and maintenance specialized dictionary.</p>
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<p>High-speed rail turnout switch machine maintenance knowledge graph.</p>
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<p>KBGC multi-level high-speed rail turnout switch machine maintenance knowledge graph completion model.</p>
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<p>BERT model based on high-speed rail turnout switch machine maintenance triplets.</p>
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<p>(<b>a</b>) The attention mechanism <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mi>W</mi> <msub> <mi>h</mi> <mi>i</mi> </msub> <mo>,</mo> <mi>W</mi> <msub> <mi>h</mi> <mi>j</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math> utilized by our model is parameterized by a weight vector and applies a LeakyReLU activation function; (<b>b</b>) a depiction of multi-head attention (with <span class="html-italic">K</span> = 3 heads) performed by node 1 on its neighborhood. The distinct arrow styles and colors represent independent attention calculations. Features aggregated by each head are concatenated or averaged, resulting in <math display="inline"><semantics> <mrow> <msubsup> <mi>h</mi> <mi>i</mi> <mrow> <mi>l</mi> <mo>+</mo> <mn>1</mn> </mrow> </msubsup> </mrow> </semantics></math>.</p>
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<p>ConvE Model.</p>
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<p>Model comparison chart.</p>
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<p>Partial model completion comparison example.</p>
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<p>Ablation experiment results.</p>
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<p>Knowledge graph completion example.</p>
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<p>High-speed railway turnout switch machine maintenance knowledge completion system.</p>
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