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Search Results (538)

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Keywords = permanent magnet synchronous machine

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35 pages, 2572 KiB  
Review
A Review of Condition Monitoring of Permanent Magnet Synchronous Machines: Techniques, Challenges and Future Directions
by Alexandros Sergakis, Marios Salinas, Nikolaos Gkiolekas and Konstantinos N. Gyftakis
Energies 2025, 18(5), 1177; https://doi.org/10.3390/en18051177 - 27 Feb 2025
Viewed by 323
Abstract
This paper focuses on the latest advancements in diagnosing faults in Permanent Magnet Synchronous Machines (PMSMs), with particular attention paid to demagnetization, inter-turn short circuits (ITSCs), and eccentricity faults. As PMSMs play an important role in electric vehicles, renewable energy systems and aerospace [...] Read more.
This paper focuses on the latest advancements in diagnosing faults in Permanent Magnet Synchronous Machines (PMSMs), with particular attention paid to demagnetization, inter-turn short circuits (ITSCs), and eccentricity faults. As PMSMs play an important role in electric vehicles, renewable energy systems and aerospace applications, ensuring their reliability is more important than ever. This work examines widely applied methods like Motor Current Signature Analysis (MCSA) and flux monitoring, alongside more recent approaches such as time-frequency analysis, observer-based techniques and machine learning strategies. These methods are discussed in terms of strengths/weaknesses, challenges and suitability for different operating conditions. The review also highlights the importance of experimental validations to connect theoretical research with real-world applications. By exploring potential synergies between these diagnostic methods, the paper outlines ways to improve fault detection accuracy and machine reliability. It concludes by identifying future research directions, such as developing real-time diagnostics, enhancing predictive maintenance and refining sensor and computational technologies, aiming to make PMSMs more robust and fault-tolerant in demanding environments. In addition, the discussion highlights how partial demagnetization or ITSC faults may propagate if not diagnosed promptly, necessitating scalable and efficient multi-physics approaches. Finally, emphasis is placed on bridging theoretical advancements with industrial-scale implementations to ensure seamless integration into existing machine drive systems. Full article
(This article belongs to the Section A: Sustainable Energy)
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<p>(<b>a</b>) Demagnetization Curve and Recoil Lines of Permanent Magnet and (<b>b</b>) Major and Minor B−H curve [<a href="#B16-energies-18-01177" class="html-bibr">16</a>].</p>
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<p>Equivalent circuit of series connected PMSM under ITSC [<a href="#B71-energies-18-01177" class="html-bibr">71</a>].</p>
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<p>Equivalent circuit of parallel connected PMSM under ITSC [<a href="#B84-energies-18-01177" class="html-bibr">84</a>].</p>
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<p>Phase A current of the parallel branches under ITSC [<a href="#B84-energies-18-01177" class="html-bibr">84</a>].</p>
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<p>Phase C current of the parallel branches under ITSC [<a href="#B84-energies-18-01177" class="html-bibr">84</a>].</p>
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<p>Block diagram of PMSG monitoring by using Kalman Filter [<a href="#B78-energies-18-01177" class="html-bibr">78</a>].</p>
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<p>Diagram of Eccentricity Faults (<b>a</b>) SE, (<b>b</b>) DE and (<b>c</b>) ME [<a href="#B98-energies-18-01177" class="html-bibr">98</a>].</p>
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25 pages, 5587 KiB  
Article
Enhanced Dynamic Control for Flux-Switching Permanent Magnet Machines Using Integrated Model Predictive Current Control and Sliding Mode Control
by Mohammadreza Mamashli and Mohsin Jamil
Energies 2025, 18(5), 1061; https://doi.org/10.3390/en18051061 - 21 Feb 2025
Viewed by 207
Abstract
Enhancing the dynamic response of Flux-Switching Permanent Magnet Synchronous Machines (FSPMSMs) is crucial for high-performance applications such as electric vehicles, renewable energy systems, and industrial automation. Conventional Proportional Integral (PI) controllers within model predictive current control (MPCC) frameworks often struggle to meet the [...] Read more.
Enhancing the dynamic response of Flux-Switching Permanent Magnet Synchronous Machines (FSPMSMs) is crucial for high-performance applications such as electric vehicles, renewable energy systems, and industrial automation. Conventional Proportional Integral (PI) controllers within model predictive current control (MPCC) frameworks often struggle to meet the demands of rapid transient response and precise speed tracking, particularly under dynamic operating conditions. To address these challenges, this paper presents a hybrid control strategy that integrates Sliding Mode Control (SMC) into the speed loop of MPCC, aiming to significantly improve the dynamic response and control robustness of FSPMSMs. The feasibility and effectiveness of the proposed approach are validated through high-fidelity real-time simulations using OPAL-RT Technologies’ OP5707XG simulator. Two control schemes are compared: MPCC with a PI controller in the speed loop (MPCC-PI) and MPCC with SMC in the speed loop (MPCC-SMC). Testing was conducted under various operating scenarios, including starting tests, load variations, speed ramping, and speed reversals. The results demonstrate that the MPCC-SMC strategy achieves superior dynamic performance, faster settling times, smoother transitions, and enhanced steady-state precision compared to the MPCC-PI scheme. The comparative results confirm that the MPCC-SMC method outperforms conventional MPCC strategies, making it a compelling solution for advanced motor drive applications requiring enhanced dynamic control. Full article
(This article belongs to the Section F3: Power Electronics)
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<p>Model of two-level voltage source inverter. (<b>a</b>) (VSI) circuit; (<b>b</b>) switching state.</p>
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<p>Prediction algorithm.</p>
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<p>MPCC with PI in speed loop.</p>
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<p>Sliding Mode Control.</p>
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<p>Speed response under load change.</p>
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<p>Speed change. (<b>a</b>) Speed increase. (<b>b</b>) Speed reversal.</p>
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<p>The OPAL-RT simulator.</p>
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<p>Steady-state performance of the motor at rated speed and load for (<b>a</b>) MPCC-PI and (<b>b</b>) MPCC-SMC methods.</p>
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<p>FFT analysis of the phase current for (<b>a</b>) MPCC-PI and (<b>b</b>) MPCC-SMC methods.</p>
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<p>Speed, torque, and current response during starting testing. (<b>a</b>). Scheme 1. (<b>b</b>) Scheme 2.</p>
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<p>Speed, torque, and current response under loading and unloading conditions. (<b>a</b>) Scheme 1. (<b>b</b>) Scheme 2.</p>
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<p>Stability analysis of speed, torque, and current during speed change. (<b>a</b>) Scheme 1. (<b>b</b>) Scheme 2.</p>
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<p>Speed, torque, and current oscillations during speed reversal. (<b>a</b>) Scheme 1. (<b>b</b>) Scheme 2.</p>
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<p>Speed, torque, and current oscillations during speed c. (<b>a</b>) Scheme 1. (<b>b</b>) Scheme 2.</p>
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<p>Impact of parameter mismatches on Total Harmonic Distortion (THD) and torque ripple for MPCC-PI and MPCC-SMC methods: (<b>a</b>) resistance mismatch, (<b>b</b>) PM flux linkage mismatch, and (<b>c</b>) inductance mismatch.</p>
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24 pages, 3724 KiB  
Review
Towards Digital Twin Modeling and Applications for Permanent Magnet Synchronous Motors
by Grace Firsta Lukman and Cheewoo Lee
Energies 2025, 18(4), 956; https://doi.org/10.3390/en18040956 - 17 Feb 2025
Viewed by 391
Abstract
This paper explores the potential of Digital Twin (DT) technology for Permanent Magnet Synchronous Motors (PMSMs) and establishes a foundation for its modeling and applications. While DTs have been widely applied in complex systems and simulation software, their use in electric motors, especially [...] Read more.
This paper explores the potential of Digital Twin (DT) technology for Permanent Magnet Synchronous Motors (PMSMs) and establishes a foundation for its modeling and applications. While DTs have been widely applied in complex systems and simulation software, their use in electric motors, especially PMSMs, remains limited. This study examines physics-based, data-driven, and hybrid modeling approaches and evaluates their feasibility for real-time simulation, fault detection, and predictive maintenance. It also identifies key challenges such as computational demands, data integration, and the lack of standardized frameworks. By assessing current developments and outlining future directions, this work provides insights into how DTs can be implemented for PMSMs and drive advancements in industrial applications. Full article
(This article belongs to the Section F3: Power Electronics)
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<p>The number of publications about Industry 4.0, IoT, and Digital Twin, and the trend line of Digital Twin research.</p>
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<p>Data flow in (<b>a</b>) digital model; (<b>b</b>) digital shadow; and (<b>c</b>) Digital Twin (adapted from [<a href="#B16-energies-18-00956" class="html-bibr">16</a>]).</p>
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<p>Digital twin configuration for electric motors.</p>
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<p>PMSM key components.</p>
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<p>Physics-based motor modeling.</p>
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<p>Data-driven-based motor modeling.</p>
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<p>Physics-informed data-driven-based motor modeling.</p>
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<p>Real-life applications of PMSMs.</p>
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<p>Monitoring framework (adapted from [<a href="#B44-energies-18-00956" class="html-bibr">44</a>], Digital Twin route added).</p>
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<p>The most efficient motor selection process using Digital Twin (adapted from [<a href="#B49-energies-18-00956" class="html-bibr">49</a>]).</p>
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24 pages, 11241 KiB  
Article
Comparative Analysis of the Effect of Rotor Faults in the Performance of Low-Speed High-Torque Machines
by Carlos Madariaga-Cifuentes, Cesar Gallardo, Jose E. Ruiz-Sarrio, Juan A. Tapia and Jose A. Antonino-Daviu
Appl. Sci. 2025, 15(4), 1721; https://doi.org/10.3390/app15041721 - 8 Feb 2025
Viewed by 475
Abstract
Several studies have focused on modeling and analyzing the impact of rotor faults in conventional low-pole-count machines, while related research on low-speed high-torque (LSHT) machines with a high pole count remains limited. In these machines, the combination of low speed, high inertia, and [...] Read more.
Several studies have focused on modeling and analyzing the impact of rotor faults in conventional low-pole-count machines, while related research on low-speed high-torque (LSHT) machines with a high pole count remains limited. In these machines, the combination of low speed, high inertia, and high torque levels presents a critical application for advanced diagnosis techniques. The present paper aims to describe and quantify the impact of rotor faults on the performance of LSHT machine types during the design stage. Specifically, 10-pole and 16-pole synchronous reluctance machines (SynRMs), permanent magnet synchronous machines (PMSMs), and squirrel-cage induction machines (SCIMs) are assessed by means of detailed 2D simulations. The effects of eccentricity, broken rotor bars, and partial demagnetization are studied, with a focus on performance variations. The results show that LSHT PMSMs are not significantly affected by the partial demagnetization of a few magnets, and the same holds true for common faults in SynRMs and SCIMs. Nonetheless, a significant increase in torque ripple was observed for all evaluated faults, with different origins and diverse effects on the torque waveform, which could be hard or invasive to analyze. Furthermore, it was concluded that specialized diagnosis techniques are effectively required for detecting the usual faults in LSHT machines, as their effect on major performance indicators is mostly minimal. Full article
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<p>LSHT machines in 3D sketches: (<b>a</b>) example of LSHT PMSM with 14 poles; (<b>b</b>) example of LSHT SCIM with 16 poles; (<b>c</b>) example of LSHT SynRM with 16 poles. The three-phase windings are highlighted in red, green, and blue for phases A, B, and C, respectively.</p>
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<p>Different eccentricity types in electric machines: (<b>a</b>) faultless machine; (<b>b</b>) machine with static eccentricity; (<b>c</b>) machine with dynamic eccentricity.</p>
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<p>Different misalignment types: (<b>a</b>) reference faultless machine; (<b>b</b>) parallel misalignment; (<b>c</b>) angular misalignment.</p>
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<p>Types of demagnetization in electrical machines: (<b>a</b>) position of magnetization probes; (<b>b</b>) machine with uniform demagnetization; (<b>c</b>) machine with partial demagnetization.</p>
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<p>Flowchart of the assessment of selected machines using FE simulations.</p>
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<p>Optimized machines for 10-pole LSHT applications: (<b>a</b>) PMSM; (<b>b</b>) SynRM; (<b>c</b>) SCIM.</p>
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<p>The resulting optimized 10-pole LSHT machines in 3D sketches: (<b>a</b>) PMSM; (<b>b</b>) SynRM; (<b>c</b>) SCIM.</p>
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<p>The 2D FE model used for the evaluation of 10-pole LSHT machines: (<b>a</b>) meshed best PMSM model; (<b>b</b>) meshed best SynRM model; (<b>c</b>) meshed best SCIM model. A quad-layer airgap was considered in all FE models to enhance accuracy.</p>
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<p>Optimized LSHT 16-pole machines: (<b>a</b>) PMSM; (<b>b</b>) SynRM; (<b>c</b>) SCIM.</p>
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<p>The resulting optimized 16-pole LSHT machines in 3D sketches: (<b>a</b>) PMSM; (<b>b</b>) SynRM; (<b>c</b>) SCIM.</p>
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<p>The 2D FE model used for the evaluation of 16-pole LSHT machines: (<b>a</b>) meshed best PMSM model; (<b>b</b>) meshed best SynRM model; (<b>c</b>) meshed best SCIM model. A quad-layer airgap was considered in all FE models to enhance accuracy.</p>
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27 pages, 1802 KiB  
Article
Optimal Design of Interior Permanent Magnet Synchronous Motor Considering Various Sources of Uncertainty
by Giacomo Guidotti, Dario Barri, Federico Soresini and Massimiliano Gobbi
World Electr. Veh. J. 2025, 16(2), 79; https://doi.org/10.3390/wevj16020079 - 5 Feb 2025
Viewed by 513
Abstract
The automotive industry is experiencing a period of transition from traditional internal combustion engine (ICE) vehicles to electric vehicles. Although electric machines have always been used in many applications, they are generally designed neglecting the sources of uncertainty, even such uncertainty can lead [...] Read more.
The automotive industry is experiencing a period of transition from traditional internal combustion engine (ICE) vehicles to electric vehicles. Although electric machines have always been used in many applications, they are generally designed neglecting the sources of uncertainty, even such uncertainty can lead to significant deterioration of the motor performance. The aim of this paper is to compare the results obtained from the multi-objective optimization of an interior permanent magnet synchronous motor (IPMSM) using a robust approach versus a deterministic one. Unlike other studies in the literature, this research simultaneously considers different sources of uncertainty, such as geometric parameters, magnet properties, and operating temperature, to assess the variability of electric motor performance. Different designs of a 48 slot–8 pole motor are simulated with finite element analysis, then the outputs are used to train artificial neural networks that are employed to find the optimal design with different approaches. The method incorporates an innovative use of the neural network-based variance estimation (NNVE) technique to efficiently calculate the standard deviation of the objective functions. Finally, the results of the robust optimization are compared with those of the deterministic optimization. Due to the small margin of improvement in robustness, both methods lead to similar results. Full article
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<p>Flow chart of the proposed method.</p>
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<p>Structure of a neuron in a neural network.</p>
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<p>Structure of the feedforward artificial neural networks used in this paper. They receive as input the design variables, the operating conditions, and their standard deviation. The output is constituted by the average value and standard deviation of objective and constraint functions.</p>
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<p>Example of the optimisation of an objective function f(x). The black line represents a generic function f(x) to be optimised, the green and blue points are two local maxima and the dashed red lines are used to highlight the uncertainty interval of the green and blue points.</p>
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<p>Cross-section of the motor used in the case study. White, green, red, yellow, grey and light blue are respectively the colors associated with air, magnets, stator material, slots, shaft and rotor material.</p>
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<p>Radial section of the motor in which the following design variables are highlighted: (<b>a</b>) slot opening, (<b>b</b>) magnet thickness, (<b>c</b>) web thickness, (<b>d</b>) tooth width, (<b>e</b>) magnet width, (<b>f</b>) pole V angle, (<b>g</b>) airgap, (<b>h</b>) bridge thickness. White, green, red, yellow, light blue and grey are respectively the colors associated with air, magnets, stator material, slots, rotor material and slot opening.</p>
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<p>Structure of the neural network used to evaluate the performance indexes and the peak voltage.</p>
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<p>Structure of the neural network used to evaluate the peak temperatures of magnets and windings.</p>
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<p>Correlation plot of the neural network trained with the mechanical simulations.</p>
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<p>Correlation plot of the neural network trained with the thermal simulations.</p>
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<p>Comparison of the computational effort of the Monte Carlo method and the proposed approach.</p>
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<p>Average fitness of the population during the optimization using non-dominated sorting genetic algorithm with a population of <math display="inline"><semantics> <msup> <mn>10</mn> <mn>4</mn> </msup> </semantics></math> individuals.</p>
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<p>Comparison of the deterministic and MOMSD optimal solutions in terms of expected values. Red and black lines represent the uncertainty range for deterministic and MOMSD solutions, respectively. These lines are centered on three distinct points, each representing the best performance for torque, torque ripple, or efficiency, with an extension of <math display="inline"><semantics> <mrow> <mn>6</mn> <mi>σ</mi> </mrow> </semantics></math> in each direction.</p>
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<p>Average performance of the optimal deterministic and MOMSD designs.</p>
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<p>Utopia points of the deterministic and MOMSD optimal solutions.</p>
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<p>Nadir points of the deterministic and MOMSD optimal solutions.</p>
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<p>Comparison between the expected values of the objective functions obtained with the deterministic approach and with the <math display="inline"><semantics> <mi>β</mi> </semantics></math>-efficient approach (<math display="inline"><semantics> <mi>β</mi> </semantics></math> = 95% and <math display="inline"><semantics> <mi>β</mi> </semantics></math> = 99%).</p>
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<p>Comparison between the standard deviations of the objective functions obtained with the deterministic approach and with the <math display="inline"><semantics> <mi>β</mi> </semantics></math>-efficient approach (<math display="inline"><semantics> <mi>β</mi> </semantics></math> = 95% and <math display="inline"><semantics> <mi>β</mi> </semantics></math> = 99%).</p>
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<p>Average performance of the optimal deterministic and <math display="inline"><semantics> <mi>β</mi> </semantics></math>-efficient designs.</p>
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<p>Utopia points of the deterministic and <math display="inline"><semantics> <mi>β</mi> </semantics></math>-efficient (<math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>95</mn> <mo>%</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>99</mn> <mo>%</mo> </mrow> </semantics></math>) optimal solutions.</p>
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<p>Nadir points of the deterministic and <math display="inline"><semantics> <mi>β</mi> </semantics></math>-efficient (<math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>95</mn> <mo>%</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>99</mn> <mo>%</mo> </mrow> </semantics></math>) optimal solutions.</p>
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25 pages, 9084 KiB  
Article
Real-Time Modeling of Static, Dynamic and Mixed Eccentricity in Permanent Magnet Synchronous Machines
by Ramón Pérez, Jérôme Cros and Mathieu Picard
Machines 2025, 13(2), 120; https://doi.org/10.3390/machines13020120 - 4 Feb 2025
Viewed by 531
Abstract
Eccentricity faults are one of the main causes that significantly affect the performance of permanent magnet synchronous machines (PMSMs). Monitoring eccentricity in real time could prevent failures by adapting operation conditions and maintenance schedule when early signs of deterioration are detected. This article [...] Read more.
Eccentricity faults are one of the main causes that significantly affect the performance of permanent magnet synchronous machines (PMSMs). Monitoring eccentricity in real time could prevent failures by adapting operation conditions and maintenance schedule when early signs of deterioration are detected. This article proposes making a circuit-type model of a permanent magnet machine with an easily configurable eccentricity for simulations and real-time analysis of signals under different operating conditions. The basis for the construction of the circuit model will be the simulation of the PMSM with 49 different coordinates of the rotor center, using the finite element analysis (FEA). The presence of eccentricity causes a variation in the inductances, the no-load flux and the expansion torque depending on the position of the rotor. The model proposes the use of bilinear interpolation (BI) to estimate the inductance matrix, the no-load flux vector captured by the stator winding and the cogging torque due to the presence of the magnets in the rotor, all of them for each rotor position. The validation is done by comparing the precision in the results of the machine’s self-inductances, the torque and the voltage waveform at the PMSM terminals and the static torque of the PMSM. The circuit model results are validated in two ways: (1) through experimental simulation, comparing the same results obtained using FEA and (2) through practical experimentation, producing a dynamic eccentricity in the machine of 0.3 mm. The results show that the proposed model is capable of accurately reproducing the behavior of the PMSM against eccentricity faults and presents computational time savings close to 99% compared to the response time obtained using FEA. This rapid PMSM model, parameterizable according to the degree of eccentricity, is the basis for the real-time simulation of the main machine waveforms, such as voltage, current and torque. Full article
(This article belongs to the Special Issue Fault Diagnostics and Fault Tolerance of Synchronous Electric Drives)
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<p>Graphic representation of eccentricity on the machine. (<b>a</b>) Healthy machine; (<b>b</b>) Static eccentricity; (<b>c</b>) Dynamic eccentricity.</p>
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<p>Graphical representation of bilinear interpolation.</p>
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<p>Procedure for the identification of <math display="inline"><semantics> <mrow> <mfenced open="[" close="]" separators="|"> <mrow> <mi mathvariant="bold-italic">L</mi> <mfenced separators="|"> <mrow> <mi>θ</mi> </mrow> </mfenced> </mrow> </mfenced> </mrow> </semantics></math> of given machine excentricity <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>x</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>y</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> with FE model.</p>
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<p>Procedure for the identification of <math display="inline"><semantics> <mrow> <mfenced open="[" close="]" separators="|"> <mrow> <msub> <mrow> <mi mathvariant="bold-italic">λ</mi> </mrow> <mrow> <mi>m</mi> </mrow> </msub> <mfenced separators="|"> <mrow> <mi>θ</mi> </mrow> </mfenced> </mrow> </mfenced> </mrow> </semantics></math> of given machine excentricity <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>x</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>y</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> with FE model.</p>
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<p>(<b>a</b>) PMSM used for the study and (<b>b</b>) the rotor center coordinates.</p>
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<p>Geometry and meshing of the PMSM with an FEA model.</p>
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<p>Parameters of phase A in the presence of static eccentricity as a function of the rotor position for 3 different CR positions. (<b>a</b>) Self-inductance; (<b>b</b>) no-load flow captured by the winding.</p>
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<p>Block diagram of command method implemented in MATLAB/Simulink.</p>
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<p>Bilinear interpolation carried out in the Simulink environment.</p>
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<p>Detail of the PMSM command diagram.</p>
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<p>PMSM coupled circuit model in Simulink block diagram.</p>
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<p>Self-inductance variations for (<b>a</b>) SE with <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> = −0.15 mm and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> = 0.1 mm, (<b>b</b>) DE = 0.3 mm, (<b>c</b>) ME: SE with <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> = −0.15 mm and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> = 0.1 mm + DE = 0.3 mm.</p>
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<p>No-load flux captured by the stator winding results: (<b>a</b>) SE with <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> = −0.15 mm and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> = 0.1 mm, (<b>b</b>) DE = 0.3 mm, (<b>c</b>) ME: SE with <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> = −0.15 mm and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> = 0.1 mm + DE = 0.3 mm.</p>
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<p>No-load flux captured by the stator winding results: (<b>a</b>) SE with <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> = −0.15 mm and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> = 0.1 mm, (<b>b</b>) DE = 0.3 mm, (<b>c</b>) ME: SE with <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> = −0.15 mm and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> = 0.1 mm + DE = 0.3 mm.</p>
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<p>Voltage in phase A of the PMSM for a DE = 0.3 mm.</p>
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<p>Torque developed by the PMSM for (<b>a</b>) SE with x = −0.15 mm and y = 0.1 mm. (<b>b</b>) Relative error for SE; (<b>c</b>) DE = 0.3 mm and (<b>d</b>) relative error for DE.</p>
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<p>Bushings to produce static eccentricity. (<b>a</b>) Front view, (<b>b</b>) side view and dynamic eccentricity (<b>c</b>) front view, (<b>d</b>) side view.</p>
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<p>Bearing for the study of eccentricity.</p>
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<p>Production of a dynamic eccentricity of 0.3 mm in the PMSM.</p>
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<p>(<b>a</b>) Rotor bushings and (<b>b</b>) stator bushings producing a dynamic eccentricity of 0.3 mm.</p>
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<p>PMSM with a 0.3 mm dynamic eccentricity fault.</p>
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<p>Block diagram of the experiment carried out.</p>
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<p>PMSM speed during the experiment carried out.</p>
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<p>Measured rotor angular position and rotor angular position estimated by the proposed model.</p>
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<p>Comparison between the static torque measured experimentally and the static torque obtained from the model proposed.</p>
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<p>Measured static torque and estimated static torque by the proposed model.</p>
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44 pages, 3781 KiB  
Review
Fault Detection of Permanent Magnet Synchronous Machines: An Overview
by Henghui Li, Zi-Qiang Zhu, Ziad Azar, Richard Clark and Zhanyuan Wu
Energies 2025, 18(3), 534; https://doi.org/10.3390/en18030534 - 24 Jan 2025
Viewed by 636
Abstract
These days, as the application of permanent magnet synchronous machines (PMSMs) and drive systems becomes popular, the reliability issue of PMSMs gains more and more attention. To improve the reliability of PMSMs, fault detection is one of the practical techniques that enables the [...] Read more.
These days, as the application of permanent magnet synchronous machines (PMSMs) and drive systems becomes popular, the reliability issue of PMSMs gains more and more attention. To improve the reliability of PMSMs, fault detection is one of the practical techniques that enables the early interference and mitigation of the faults and subsequently reduces the impact of the faults. In this paper, the state-of-the-art fault detection methods of PMSMs are systematically reviewed. Three typical faults, i.e., the inter-turn short-circuit fault, the PM partial demagnetization fault, and the eccentricity fault, are included. The existing methods are firstly classified into signal-, model-, and data-based methods, while the focus of this paper is laid on the signal sources and the signatures utilized in these methods. Based on this perspective, this paper intends to provide a new insight into the inherent commonalities and differences among these detection methods and thus inspire further innovation. Furthermore, comparison is conducted between methods based on different signatures. Finally, some issues in the existing methods are discussed, and future work is highlighted. Full article
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<p>Classification of faults in the PMSM drive system. The detailed explanation of inter-turn short-circuit fault, partial demagnetization fault, and rotor eccentricity fault is shown in <a href="#sec2dot1-energies-18-00534" class="html-sec">Section 2.1</a>, <a href="#sec3dot1-energies-18-00534" class="html-sec">Section 3.1</a> and <a href="#sec4dot1-energies-18-00534" class="html-sec">Section 4.1</a>.</p>
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<p>Classification of detection methods for ITSC, PD, and eccentricity faults.</p>
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<p>Illustration of fault detection procedure of signal-, model-, and data-based methods.</p>
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<p>Illustration of ITSC fault. (<b>a</b>) Illustration; (<b>b</b>) equivalent circuit.</p>
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<p>Classification of signal-based methods for ITSC detection.</p>
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<p>Illustration of typical mounting placing of flux sensors for fault detection. (<b>a</b>) Invasive methods; (<b>b</b>) less-invasive methods.</p>
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<p>Classification of model-based methods for ITSC detection.</p>
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<p>Classification of data-based methods for ITSC detection.</p>
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<p>Illustration of demagnetization curve of a PM.</p>
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<p>Classification of signal-based methods for PD detection.</p>
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<p>Classification of model-based methods for PD detection.</p>
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<p>Classification of data-based methods for PD detection.</p>
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<p>Illustration of eccentricity. (<b>a</b>) SE; (<b>b</b>) DE.</p>
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<p>Classification of signal-based methods for eccentricity detection.</p>
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<p>Classification of data-based methods for eccentricity detection.</p>
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<p>Illustration of existing challenges and future work.</p>
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22 pages, 9823 KiB  
Article
HIL-Based Fault-Tolerant Vector Space Decomposition Control for a Six-Phase PMSM Fed by a Five-Level CHB Converter
by Mona Shayeghan, Marco Di Benedetto, Alessandro Lidozzi and Luca Solero
Energies 2025, 18(3), 507; https://doi.org/10.3390/en18030507 - 23 Jan 2025
Viewed by 818
Abstract
The growing demand for higher reliability and efficiency in modern electric drives, coupled with the increasing adoption of multi-phase machines, has necessitated advancements in fault-tolerant control strategies. This paper presents a fault tolerance analysis for a six-phase permanent magnet synchronous machine (PMSM) connected [...] Read more.
The growing demand for higher reliability and efficiency in modern electric drives, coupled with the increasing adoption of multi-phase machines, has necessitated advancements in fault-tolerant control strategies. This paper presents a fault tolerance analysis for a six-phase permanent magnet synchronous machine (PMSM) connected to a five-level cascaded H-bridge converter, employing a level-shift pulse width modulation (LSPWM) technique. Unlike existing strategies, this work integrates a unique combination of three key innovations: first, a fault detection mechanism capable of identifying faults in both machine phases and inverter legs with high precision; second, an open-circuit fault compensation strategy that dynamically reconfigures the faulty inverter phase leg into a two-level topology to reduce losses and preserve healthy switches; and third, a modified closed-loop control method designed specifically to mitigate the adverse effects of short-circuit faults while maintaining system stability. The proposed approach is validated through rigorous simulations in Simulink and Hardware-in-the-Loop (HIL) tests, demonstrating its robustness and applicability in high-reliability applications. Full article
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<p>Configuration of a symmetrical six-phase (A–F) PMSM.</p>
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<p>Topology of a six-phase (A–F), five-level cascade H-bridge inverter.</p>
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<p>Fault in MCI CHB modules in 6 phase inverter (A–F).</p>
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<p>Coordinate of six-phase (A–F) PMSM in rotating frame.</p>
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<p>Control structure of the six-phase (A–F) PMSM with a five-level CHB inverter.</p>
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<p>Waveforms at a steady state, from top to bottom: phase-to-neutral switching voltage A, line-to-line switching voltage AB, and six-phase (A–F) currents.</p>
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<p>Waveforms at a steady state, from top to bottom: mechanical speed, <span class="html-italic">id</span> and <span class="html-italic">iq</span> currents, <span class="html-italic">iα</span> and <span class="html-italic">iβ</span> currents, and electrical angle.</p>
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<p>Equivalent circuit of the converter under fault of S<sub>1</sub> in the HB1 in phase A.</p>
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<p>Waveforms at steady state under open-circuit fault of S<sub>1</sub> in HB1, from top to bottom: phase-to-neutral switching voltage A, line-to-line switching voltage AB, and six-phase currents.</p>
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<p>Waveforms at steady state under open-circuit fault of S<sub>1</sub> in the HB1, from top to bottom: mechanical speed, <span class="html-italic">i<sub>d</sub></span> and <span class="html-italic">i<sub>q</sub></span> currents, <span class="html-italic">i<sub>α</sub></span> and <span class="html-italic">i<sub>β</sub></span> currents, and electrical angle.</p>
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<p>Waveforms at steady state under a short-circuit fault of S<sub>1</sub> in the HB1, from top to bottom: mechanical speed, <span class="html-italic">i<sub>d</sub></span> and <span class="html-italic">i<sub>q</sub></span> currents, <span class="html-italic">i<sub>α</sub></span> and <span class="html-italic">i<sub>β</sub></span> currents, six-phase currents and electrical angle.</p>
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<p>HIL test bench for the six-phase PMSM supplied by a 5-level CHB converter.</p>
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<p>Six-phase currents waveform at steady state: <span class="html-italic">i<sub>A</sub></span> (yellow line), <span class="html-italic">i<sub>B</sub></span> (green line), <span class="html-italic">i<sub>C</sub></span> (magenta line), <span class="html-italic">i<sub>D</sub></span> (red line), <span class="html-italic">i<sub>E</sub></span> (orange line) and <span class="html-italic">i<sub>F</sub></span> (cyan line); 10 A/div, 1 ms/div.</p>
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<p>Voltage waveform at steady state: phase-to-neutral switching voltages <span class="html-italic">V<sub>AN(sw)</sub></span> (magenta line) and line-to-line switching voltage <span class="html-italic">V<sub>AB(sw)</sub></span> (green trace). 200 V/div, 1 ms/div.</p>
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<p>Three-phase currents waveform at steady state: <span class="html-italic">i<sub>A</sub></span> (yellow line), <span class="html-italic">i<sub>B</sub></span> (green line) and <span class="html-italic">i<sub>C</sub></span> (magenta line) 10 A/div. (<b>a</b>) Mechanical speed <span class="html-italic">ω<sub>m</sub></span> (orange line) 500 rpm/div and electrical angle <span class="html-italic">ϑ</span> (red line) 5 rad/div; (<b>b</b>) d-axis <span class="html-italic">i<sub>d</sub> </span>(red line) and q-axis current <span class="html-italic">i<sub>q</sub></span> (orange line) 10 A/div; and 1 ms/div.</p>
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<p>Six-phase current waveforms under OC fault: <span class="html-italic">i<sub>A</sub></span> (yellow line), <span class="html-italic">i<sub>B</sub></span> (green line), <span class="html-italic">i<sub>C</sub></span> (magenta line), <span class="html-italic">i<sub>D</sub></span> (red line), <span class="html-italic">i<sub>E</sub></span> (orange line) and <span class="html-italic">i<sub>F</sub></span> (cyan line); 10 A/div, 1 ms/div.</p>
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<p>Voltage waveforms under OC fault: phase-to-neutral switching voltages V<sub>AN(sw)</sub> (magenta line) and line-to-line switching voltage V<sub>AB(sw)</sub> (green trace). 200 V/div, 1 ms/div.</p>
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<p>Waveforms at a steady state under OC fault: three-phase currents <span class="html-italic">i<sub>A</sub></span> (yellow line), <span class="html-italic">i<sub>B</sub></span> (green line), <span class="html-italic">i<sub>C</sub></span> (magenta line), mechanical speed <span class="html-italic">ω<sub>m</sub></span> (red line) and q-axis current <span class="html-italic">i<sub>q</sub></span> (orange line); 10 A/div, 500 rpm/div, 1 ms/div.</p>
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<p>Six-phase current waveforms under SC fault: <span class="html-italic">i<sub>A</sub></span> (yellow line), <span class="html-italic">i<sub>B</sub></span> (green line), <span class="html-italic">i<sub>C</sub></span> (magenta line), <span class="html-italic">i<sub>D</sub></span> (red line), <span class="html-italic">i<sub>E</sub></span> (orange line) and <span class="html-italic">i<sub>F</sub></span> (cyan line); 10 A/div, 1 ms/div.</p>
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<p>Waveforms at a steady state under SC fault: three-phase currents <span class="html-italic">i<sub>A</sub></span> (yellow line), <span class="html-italic">i<sub>B</sub></span> (green line), <span class="html-italic">i<sub>C</sub></span> (magenta line), mechanical speed <span class="html-italic">ω<sub>m</sub></span> (red line) and q-axis current <span class="html-italic">i<sub>q</sub></span> (orange line); 10 A/div, 500 rpm/div, 1 ms/div.</p>
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16 pages, 8559 KiB  
Article
Transmission Line Modeling-Based Position Sensorless Control for Permanent Magnet Synchronous Machines
by Dianxun Xiao, Kun Hu and Chengrui Li
Electronics 2025, 14(2), 271; https://doi.org/10.3390/electronics14020271 - 10 Jan 2025
Viewed by 529
Abstract
Position sensorless control has been widely used in permanent magnet synchronous motor (PMSM) drives in low-cost applications or in the fault-tolerance control of position sensors. Conventional sensorless control methods often adopt a back electromagnetic force (EMF)-based position observer, which results in bandwidth reduction [...] Read more.
Position sensorless control has been widely used in permanent magnet synchronous motor (PMSM) drives in low-cost applications or in the fault-tolerance control of position sensors. Conventional sensorless control methods often adopt a back electromagnetic force (EMF)-based position observer, which results in bandwidth reduction in signal processing and lower estimation accuracy. This paper introduces a numerical solution based on transmission line modeling (TLM) to obtain the back EMF. The TLM method is used for the numerical calculation of electromagnetics due to the clear algorithm structure, robust convergence and stability, and easy implementation in dynamic circuit analyses. This paper first analyzes the 2D TLM method techniques. Then, a new application of TLM theory in position sensorless control of PMSMs is put forward. The proposed TLM-based sensorless control scheme can estimate the back EMF without decreasing the bandwidth, thereby enhancing the dynamic performance of the sensorless control. All numerical results are implemented using the proposed approach, which validates the effectiveness of the proposed method. Full article
(This article belongs to the Special Issue Power Electronics Controllers for Power System)
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<p>Structure of 2D TLM. (<b>a</b>) Nodes; (<b>b</b>) inductance and capacitance branch.</p>
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<p>Simplified structure of 2D TLM.</p>
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<p>Structure of the OPLL observer.</p>
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<p>Voltage equations of PMSMs expressed as the circuit. (<b>a</b>) Equivalent circuit of the voltage equations. (<b>b</b>) Replacing the inductance to the short circuit. (<b>c</b>) Circuit of (<b>b</b>) considering the impedance and equivalent voltage.</p>
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<p>Voltage equations of PMSMs expressed as the circuit. (<b>a</b>) Equivalent circuit of the voltage equations. (<b>b</b>) Replacing the inductance to the short circuit. (<b>c</b>) Circuit of (<b>b</b>) considering the impedance and equivalent voltage.</p>
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<p>The overall control block of the proposed PMSM sensorless control.</p>
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<p>Voltage distortion caused by inverter nonlinearity.</p>
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<p>Non-ideal simulation current considering real-world disturbances and nonlinearity.</p>
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<p>Position estimation results of the proposed method. (<b>a</b>) At 2000 r/min and 5 N·m load. (<b>b</b>) At 2000 r/min and 30 N·m load.</p>
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<p>Comparative position estimation results under the rated 30 N·m load disturbance at 2000 r/min. (<b>a</b>) Proposed method. (<b>b</b>) Conventional method.</p>
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<p>Comparative position estimation results with the speed change from 500 r/min to 2000 r/min with the rated 30 N·m load. (<b>a</b>) Proposed method. (<b>b</b>) Conventional method.</p>
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<p>Comparative position estimation results when the OPLL parameter increases at 2000 r/min speed with the rated 30 N·m load. (<b>a</b>) Proposed method. (<b>b</b>) Conventional method.</p>
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<p>Position estimation results of the proposed method with larger OPLL parameter values under the rated 30 N·m load disturbance at 2000 r/min.</p>
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18 pages, 8696 KiB  
Article
Traction Synchronous Machine with Rotor Field Winding and Two-Phase Harmonic Field Exciter
by Vladimir Prakht, Vladimir Dmitrievskii, Vadim Kazakbaev, Aleksey Paramonov and Victor Goman
World Electr. Veh. J. 2025, 16(1), 25; https://doi.org/10.3390/wevj16010025 - 6 Jan 2025
Viewed by 733
Abstract
Many modern electric drives for cars, trucks, ships, etc., use permanent magnet synchronous motors because of their compact size. At the same time, permanent magnets are expensive, and their uncontrolled flux is a problem when it is necessary to provide a wide constant [...] Read more.
Many modern electric drives for cars, trucks, ships, etc., use permanent magnet synchronous motors because of their compact size. At the same time, permanent magnets are expensive, and their uncontrolled flux is a problem when it is necessary to provide a wide constant power speed range in the field weakening region. An alternative to permanent magnet motors is synchronous motors with field windings. This article presents a novel design of a traction brushless synchronous motor with a field winding and a two-phase harmonic exciter winding on the rotor and zero-sequence signal injection. The two-phase harmonic exciter winding increases the electromotive force on the field winding compared to a single-phase one and makes it possible to start the motor at any rotor position. This article discusses the advantages of the proposed design over conventional solutions. A simplified mathematical model based on the finite element method for steady state simulation is presented. The machine performance of a hysteresis current controller and a field-oriented PI current controller are compared using the model. Full article
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<p>HESM design [<a href="#B18-wevj-16-00025" class="html-bibr">18</a>]: (<b>a</b>) aligned rotor position; (<b>b</b>) misaligned rotor position. The letters A, −A (red), B, −B (blue), C, −C (green) indicate the phase zones of the stator winding.</p>
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<p>Sketch of the novel electric machine design (the size ratios do not correspond to the sizes adopted during modeling). The letters a, −a (light blue), b, −b (yellow) indicate the phase zones of the harmonic winding.</p>
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<p>Sketch of rotor harmonic exciter winding layout. The coils are indicated by thick rounded lines at the top. The intercoil connections are shown below as thin lines. The letters a+, a− (light blue), b+, b− (yellow) indicate the phase zones of the harmonic winding.</p>
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<p>Motor winding connection: (<b>a</b>) stator; (<b>b</b>) rotor circuit and rotor voltages and currents, voltage levels <span class="html-italic">U<sub>a</sub></span>, <span class="html-italic">U<sub>b</sub></span>, <span class="html-italic">U<sub>c</sub></span>, and <span class="html-italic">U<sub>sh</sub></span> are shown relative to the lower negative rectifier bus.</p>
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<p>Control system diagram.</p>
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<p>Rectifier condition calculation block-diagram.</p>
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<p>Some of the main dimensions of the rotor.</p>
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<p>Motor simulation with hysteresis controller: (<b>a</b>) flux density; (<b>b</b>) magnetic vector potential.</p>
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<p>Motor simulation with FOC controller: (<b>a</b>) flux density; (<b>b</b>) magnetic vector potential.</p>
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<p>Excitation flux transient process.</p>
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<p>Excitation current: (<b>a</b>) hysteresis controller; (<b>b</b>) FOC controller.</p>
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<p>Motor torque: (<b>a</b>) hysteresis controller; (<b>b</b>) FOC controller.</p>
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<p>Phase current: (<b>a</b>) hysteresis controller; (<b>b</b>) FOC controller. The waveforms of currents of different phases are shown in different colors.</p>
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<p>Neutral wire current: (<b>a</b>) hysteresis controller; (<b>b</b>) FOC controller.</p>
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<p>Phase voltage: (<b>a</b>) hysteresis controller; (<b>b</b>) FOC controller. The waveforms of voltages of different phases are shown in different colors.</p>
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<p>Line-to-line voltage: (<b>a</b>) hysteresis controller; (<b>b</b>) FOC controller. The voltage waveforms between different lines are shown in different colors.</p>
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<p>Neutral voltage relative to the arithmetic mean phase voltage: (<b>a</b>) hysteresis controller; (<b>b</b>) FOC controller.</p>
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23 pages, 5302 KiB  
Article
A Novel Method for Automatically and Accurately Diagnosing Demagnetization Fault in Direct-Drive PMSMs Using Three PNNs
by Yiyong Xiong, Jinghong Zhao, Sinian Yan, Kun Wei and Haiwen Zhou
Appl. Sci. 2024, 14(24), 11943; https://doi.org/10.3390/app142411943 - 20 Dec 2024
Viewed by 584
Abstract
Direct-drive permanent magnet synchronous machines (DDPMSMs) have recently become an ideal candidate for applications such as military, robotics, electric vehicles, etc. These machines eliminate the need for a transmission mechanism and excitation coil circuits, which enhances the system’s overall efficiency and decreases the [...] Read more.
Direct-drive permanent magnet synchronous machines (DDPMSMs) have recently become an ideal candidate for applications such as military, robotics, electric vehicles, etc. These machines eliminate the need for a transmission mechanism and excitation coil circuits, which enhances the system’s overall efficiency and decreases the likelihood of failures. However, it may incur demagnetization faults. Due to the characteristic of having a large number of pole pairs, this type of machine exhibits numerous demagnetization fault modes, which poses a challenge in locating demagnetization faults. This paper proposed a probabilistic neural network (PNN)-based diagnostic system to detect and locate demagnetization faults in DDPMSMs, using information obtained through three toroidal-yoke-type search coils arranged at the bottom of the stator slot. A rotor partition method is proposed to solve the problem of demagnetization fault location difficulty caused by various fault modes. Demagnetization fault location is achieved by sequentially diagnosing the condition of each partition of permanent magnets. Three demagnetization fault identified signals (DFISs) are constructed by the voltage of the three toroidal-yoke coils, which are used as inputs of PNNs. Three PNNs have been designed to map the extracted features and their corresponding types of demagnetization faults. The database for training and testing the PNNs is generated from a DDPMSM with different demagnetization conditions and different operating conditions, which are established through an experimentally validated mathematical model, an FEM model, and experiments. The simulation and experimental test results showed that the accuracy in diagnosing the location of the demagnetization fault is 99.2% when the demagnetization severity is 10%, which demonstrates the effectiveness of the proposed three PNN-based diagnostic approach. Full article
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<p>Placement scheme of toroidal-yoke-search coil.</p>
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<p>The waveforms of <span class="html-italic">SI</span><sub>m−2</sub>. (<b>a</b>) Mode 1 to 6. (<b>b</b>) Modes 6, 7, and 8.</p>
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<p>The waveforms of <span class="html-italic">SI</span><sub>m−2</sub> under Mode 7 with 100% demagnetization and Mode 8 with 50% demagnetization.</p>
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<p>Normalized <span class="html-italic">SI</span><sub>m</sub> under six different demagnetization fault modes.</p>
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<p>The waveforms of normalized <span class="html-italic">SI</span><sub>a1-2</sub>. (<b>a</b>) Mode 6H, Mode 7H, Mode 6D, Mode 8H, and Mode 8D. (<b>b</b>) Mode 7D and Mode 8H.</p>
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<p>The waveforms of <span class="html-italic">SI</span><sub>a2-2</sub> under Cas 7D or Mode 8H.</p>
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<p>Corresponding relationship between the pole pair number and the electric cycle number of DFISs.</p>
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<p><span class="html-italic">SI</span><sub>m</sub> under different loading conditions of the machine.</p>
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<p><span class="html-italic">SI</span><sub>m</sub> under various speeds of the machine.</p>
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<p>The process for automatically diagnosing demagnetization faults using three PNNs.</p>
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<p>Architecture of the PNN.</p>
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<p>The training results of the three PNNs. (<b>a</b>) The first PNN. (<b>b</b>) The second PNN. (<b>c</b>) The third PNN.</p>
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<p>The testing results of the three PNNs. (<b>a</b>) The first PNN. (<b>b</b>) The second PNN. (<b>c</b>) The third PNN.</p>
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<p>Experimental setup.</p>
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<p>The experimental results of the voltage of TYC1, TYC2, and SI<sub>m</sub> under healthy conditions. (<b>a</b>) The voltage waveform of TYC1 and TYC2. (<b>b</b>) The voltage waveform of <span class="html-italic">SI</span><sub>m</sub>.</p>
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<p>The experimental results of residual voltage of under fault3. (<b>a</b>) The residual voltage of TYC1, TYC2, and TYC3. (<b>b</b>) The residual voltage waveform of <span class="html-italic">S</span><sub>m</sub> and <span class="html-italic">S</span><sub>a1</sub>.</p>
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18 pages, 1356 KiB  
Article
Permanent Magnets in Sustainable Energy: Comparative Life Cycle Analysis
by Svetlana Orlova and Anton Rassõlkin
Energies 2024, 17(24), 6384; https://doi.org/10.3390/en17246384 - 18 Dec 2024
Viewed by 1504
Abstract
This study addresses the environmental challenges associated with high-performance rare-earth magnets, particularly NdFeB, which are essential in green and digital technologies. By employing Life Cycle Assessment (LCA) with openLCA software, we evaluate the environmental impacts across the life cycles of ferrite, NdFeB, and [...] Read more.
This study addresses the environmental challenges associated with high-performance rare-earth magnets, particularly NdFeB, which are essential in green and digital technologies. By employing Life Cycle Assessment (LCA) with openLCA software, we evaluate the environmental impacts across the life cycles of ferrite, NdFeB, and MnAlC magnets, focusing on extraction, processing, and recycling. Various studies have explored different aspects of the LCA of NdFeB magnets, focusing on production methods, recycling processes, and the environmental impacts of different rare-earth sources. A comparative LCA highlights the significant environmental footprint of rare-earth magnets, underscoring the role of functional unit selection: when assessed per unit of energy density, the environmental impact of NdFeB magnets aligns more closely with alternatives. Methodological issues such as data quality, choice of functional units, and system complexity affect LCA accuracy, as inconsistencies in data or scope led to potential distortions in environmental assessments. This research also explores manganese-based magnets as viable alternatives to reduce reliance on rare-earth materials. Legislative initiatives, including the EU’s Ecodesign Directive and Critical Raw Materials Act, support sustainable management practices to ensure reliable material supply while promoting environmental protection. This paper highlights the importance of sustainable magnetic materials, emphasizing the need for interdisciplinary research to balance technological efficiency and environmental impact, especially as rare-earth magnet demand rises with the transition to renewable energy sources. Full article
(This article belongs to the Section A: Sustainable Energy)
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<p>Projected NdFeB magnet consumption by application segment (2022–2032) [<a href="#B12-energies-17-06384" class="html-bibr">12</a>].</p>
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<p>Magnetic parameters of permanent magnets (Nd<sub>2</sub>Fe<sub>14</sub>B [<a href="#B14-energies-17-06384" class="html-bibr">14</a>] AlNiCo [<a href="#B15-energies-17-06384" class="html-bibr">15</a>] SrFe<sub>12</sub>O<sub>19</sub> [<a href="#B16-energies-17-06384" class="html-bibr">16</a>], BaFe<sub>12</sub>O<sub>19</sub> [<a href="#B17-energies-17-06384" class="html-bibr">17</a>], SmCo<sub>5</sub>, [<a href="#B18-energies-17-06384" class="html-bibr">18</a>] Sm<sub>2</sub>Co<sub>17</sub> [<a href="#B19-energies-17-06384" class="html-bibr">19</a>], and MnAlC [<a href="#B20-energies-17-06384" class="html-bibr">20</a>]).</p>
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<p>Ferrite permanent magnet production process [<a href="#B21-energies-17-06384" class="html-bibr">21</a>].</p>
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<p>NdFeB permanent magnet production process [<a href="#B25-energies-17-06384" class="html-bibr">25</a>].</p>
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<p>Environmental, resource depletion, and human health impact comparison of NdFeB, ferrite, and MnAlC across various impact categories for functional unit 1 kg of mass.</p>
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<p>Environmental, resource depletion, and human health impact comparison of NdFeB, ferrite, and MnAlC across various impact categories for functional unit 1 kJ/m<sup>3</sup> of maximum energy product.</p>
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15 pages, 8380 KiB  
Article
Design and Analysis of a Low Torque Ripple Permanent Magnet Synchronous Machine for Flywheel Energy Storage Systems
by Yubo Sun, Zhenghui Zhao and Qian Zhang
Energies 2024, 17(24), 6337; https://doi.org/10.3390/en17246337 - 16 Dec 2024
Viewed by 711
Abstract
Flywheel energy storage systems (FESS) are technologies that use a rotating flywheel to store and release energy. Permanent magnet synchronous machines (PMSMs) are commonly used in FESS due to their high torque and power densities. One of the critical requirements for PMSMs in [...] Read more.
Flywheel energy storage systems (FESS) are technologies that use a rotating flywheel to store and release energy. Permanent magnet synchronous machines (PMSMs) are commonly used in FESS due to their high torque and power densities. One of the critical requirements for PMSMs in FESS is low torque ripple. Therefore, a PMSM with eccentric permanent magnets is proposed and analyzed in this article to reduce torque ripple. Cogging torque, a significant contributor to torque ripple, is investigated by a combination of finite element analysis and the analytical method. An integer-slot distribution winding structure is adopted to reduce vibration and noise. Moreover, the effects of eccentric permanent magnets and harmonic injection on the cogging torque are analyzed and compared. In addition, the electromagnetic performance is analyzed, and the torque ripple is found to be 3.1%. Finally, a prototype is built and tested, yielding a torque ripple of 3.9%, to verify the theoretical analysis. Full article
(This article belongs to the Special Issue Energy, Electrical and Power Engineering: 3rd Edition)
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<p>Topology of proposed PMSM.</p>
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<p>Winding connection.</p>
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<p>Analysis model of surface-mounted PMSM.</p>
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<p>Bread-type eccentric permanent magnet.</p>
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<p>Influence of eccentricity on torque performance.</p>
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<p>Cogging torque of PMSM with different permanent magnets.</p>
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<p>Air gap magnetic densities of PMSM with different permanent magnets. (<b>a</b>) Radial air gap magnetic densities. (<b>b</b>) Tangential air gap magnetic densities. (<b>c</b>) Harmonic order.</p>
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<p>Cogging torque contribution of different harmonics. (<b>a</b>) PMSM with original permanent magnets. (<b>b</b>) PMSM with eccentric permanent magnets.</p>
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<p>Permanent magnet with third harmonic injection.</p>
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<p>Cogging torque of PMSM with harmonic injection. (<b>a</b>) Effect of harmonic injection. (<b>b</b>) Contribution of harmonics.</p>
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<p>Load electromagnetic performance. (<b>a</b>) Magnetic field line. (<b>b</b>) Magnetic flux density.</p>
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<p>Back electromotive force of PMSM.</p>
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<p>Torque performance of PMSM. (<b>a</b>) Cogging torque. (<b>b</b>) Torque.</p>
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<p>Vibration acceleration of PMSM with different permanent magnets.</p>
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<p>Prototype.</p>
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<p>Experimental platform.</p>
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<p>Vibration and noise test platform.</p>
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<p>Comparison of experimental and simulated results. (<b>a</b>) Back electromotive force of prototype. (<b>b</b>) Comparison of back electromotive force coefficient.</p>
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<p>Experimental results. (<b>a</b>) Torque. (<b>b</b>) Vibration acceleration.</p>
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27 pages, 13815 KiB  
Article
Unconventional Structures of Asynchronous Motors with Two Stators and Single-Rotor Radial Air Gaps in the Context of Their Applicability Assessment
by Mihail-Florin Stan, Iulian Bancuta, Elena-Otilia Virjoghe, Adela-Gabriela Husu and Cosmin Cobianu
Energies 2024, 17(24), 6237; https://doi.org/10.3390/en17246237 - 11 Dec 2024
Viewed by 567
Abstract
The fundamental idea underlying the research presented in this paper was the desire to use less magnetically charged areas of the general construction of induction machines by increasing the active working surface by interposing a new internal stator armature. This results in a [...] Read more.
The fundamental idea underlying the research presented in this paper was the desire to use less magnetically charged areas of the general construction of induction machines by increasing the active working surface by interposing a new internal stator armature. This results in a new air gap and foreshadows the advantage of increasing the torques developed by the motor considered, compared to the equivalent standard motor, at the same volume of iron. The following research-validation methods were followed: theoretical studies (analytical simulation and FEM), an experimental model (prototype), and testing on the experimental platform. We recall obtaining solid conclusions on the technological construction, functional and energy characteristics, as well as superior performances of over 50% regarding electromagnetic torques compared to the equivalent classic version. The prototype of this type of machine was surprising due to the ease with which the rotor can be rotated, highlighting the reduced inertia. In conclusion, concerning the problem addressed and the objectives pursued, the research had, in essence, an applied and experimental nature. The recent development of permanent-magnet synchronous motor constructions has led to the concept of creating such motors in the constructive configuration specified in the paper (two stators and two radial air gaps). Full article
(This article belongs to the Section F: Electrical Engineering)
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<p>(<b>a</b>) Intermediate rotor with a three-phase winding; (<b>b</b>) Intermediate rotor with cage windings; (<b>c</b>) Tandem motor with two rotors.</p>
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<p>The connection scheme of the stator windings in the asynchronous version.</p>
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<p>The rotor cage. (<b>a</b>) The solution with a row of bars with semi-open rotor notches; (<b>b</b>) The solution with two cages separated by an isthmus, with closed notches.</p>
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<p>The variant with closed notches. (<b>a</b>) Distribution of equipotential in geometry with closed notches and rotor isthmus; (<b>b</b>) Effect of notch closure on machine reactance.</p>
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<p>Constructive variants with different numbers of bars: (<b>a</b>) Variant with 20 bars; (<b>b</b>) Variant with 28 bars.</p>
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<p>Arrangement of rotor notches: (<b>a</b>) The case of the 7 mm bar; (<b>b</b>) The case of the 9 mm bar.</p>
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<p>Examples of two types of notches: small (<b>A</b>) and large (<b>B</b>).</p>
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<p>(<b>a</b>) Transverse geometry; (<b>b</b>) The discretization network.</p>
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<p>(<b>a</b>) Magnetic flux at idle operation; (<b>b</b>) Magnetic induction at idle operation.</p>
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<p>(<b>a</b>) Magnetic induction in the outer space; (<b>b</b>) Magnetic induction in the inner space.</p>
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<p>(<b>a</b>) Magnetic flux at idle operation; (<b>b</b>) Magnetic induction at idle operation.</p>
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<p>(<b>a</b>) Magnetic induction in the outer space; (<b>b</b>) Magnetic induction in the inner space.</p>
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<p>(<b>a</b>) Magnetic flux at idle operation; (<b>b</b>) Magnetic induction at idle operation.</p>
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<p>(<b>a</b>) Magnetic induction in the outer space; (<b>b</b>) Magnetic induction in the inner space.</p>
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<p>Connection diagram for Test Report 1.</p>
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<p>Line voltage at idle [V]—No load current [A] characteristic.</p>
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<p>Power absorbed at idle [W]—Line voltage at idle [V] characteristic.</p>
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<p>Power factor at idle—Line voltage at idle [V] characteristic.</p>
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<p>Short-circuit phase current [A]—Line voltage at short-circuit operation [V] characteristic.</p>
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<p>Power absorbed at short circuit [W]—Line voltage at short-circuit [V] characteristic.</p>
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<p>Short circuit current calculated [A]—Line voltage at short-circuit [V] characteristic.</p>
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<p>Connection diagram for Test Report 2.</p>
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<p>Power factor at idle—Line voltage at idle [V] characteristic.</p>
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<p>Power absorbed at idle [W]—Line voltage at idle [V] characteristic.</p>
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<p>Line voltage at idle [V]—No-load current [A] characteristic.</p>
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<p>Short circuit current calculated [A]—Line voltage at short-circuit operation [V] characteristic.</p>
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<p>Power absorbed at short-circuit [W]—Line voltage at short-circuit [V] characteristic.</p>
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<p>Short-circuit phase current [A]—Line voltage at short-circuit [V] characteristic.</p>
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<p>The connection diagram develops torques in the same direction.</p>
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<p>The connection diagram develops torques in the opposite direction.</p>
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<p>Power factor at idle—Line voltage at idle [V] characteristic.</p>
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<p>Power absorbed at idle [W]—Line voltage at idle [V] characteristic.</p>
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<p>Line voltage at idle [V]—No-load current [A] characteristic.</p>
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<p>Short circuit current calculated [A]—Line voltage at short-circuit operation [V] characteristic.</p>
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<p>Power absorbed at short-circuit [W]—Line voltage at short-circuit [V] characteristic.</p>
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<p>Short circuit current calculated [A]—Line voltage at short-circuit [V] characteristic.</p>
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<p>The connection diagram in load operation.</p>
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<p>Power factor—Useful power [W] characteristic.</p>
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<p>Slip [%]—Useful power [W] characteristic.</p>
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<p>Yield [%]—Useful power [W] characteristic.</p>
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<p>Absorbed current [A]—Useful power [W] characteristic.</p>
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35 pages, 15787 KiB  
Review
Recent Developments and Trends in High-Performance PMSM for Aeronautical Applications
by Chendong Liao, Nicola Bianchi and Zhuoran Zhang
Energies 2024, 17(23), 6199; https://doi.org/10.3390/en17236199 - 9 Dec 2024
Viewed by 1108
Abstract
Permanent magnet synchronous machines (PMSMs) have been widely used in various applications such as robotics, electric vehicles, and aerospace due to their fast dynamic response, high-power/torque density, and high efficiency. These features make them attractive candidates for aeronautical applications, where the weight and [...] Read more.
Permanent magnet synchronous machines (PMSMs) have been widely used in various applications such as robotics, electric vehicles, and aerospace due to their fast dynamic response, high-power/torque density, and high efficiency. These features make them attractive candidates for aeronautical applications, where the weight and volume of onboard systems are critically important. This paper aims to provide an overview of recent developments in PMSMs. Key design considerations for aeronautical PMSMs across different applications are highlighted based on the analysis of industrial cases and research literature. Additionally, emerging techniques that are vital in enhancing the performance of aeronautical PMSMs are discussed. Full article
(This article belongs to the Special Issue Energy, Electrical and Power Engineering: 3rd Edition)
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<p>The No-bleed architecture of the MEA Boeing 787 Dreamliner [<a href="#B4-energies-17-06199" class="html-bibr">4</a>].</p>
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<p>E-fan developed by Airbus.</p>
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<p>Classification of aircraft electric propulsion architectures [<a href="#B4-energies-17-06199" class="html-bibr">4</a>].</p>
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<p>Full-scale 1 MW motor drive demonstrator for turbo-electric propulsion developed by MIT [<a href="#B12-energies-17-06199" class="html-bibr">12</a>].</p>
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<p>Different PMSM topologies (<b>a</b>) interior PM (<b>b</b>) PM-assisted synchronous reluctance (<b>c</b>) interior PM outer rotor (OR) (<b>d</b>) surface-mounted PM linear (<b>e</b>) surface-mounted PM (<b>f</b>) surface-inset PM (<b>g</b>) surface-mounted Halbach PM array (<b>h</b>) surface-mounted PM OR (<b>i</b>) consequent pole surface-inset PM (<b>j</b>) surface-mounted PM axial flux.</p>
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<p>Different PMSM topologies (<b>a</b>) interior PM (<b>b</b>) PM-assisted synchronous reluctance (<b>c</b>) interior PM outer rotor (OR) (<b>d</b>) surface-mounted PM linear (<b>e</b>) surface-mounted PM (<b>f</b>) surface-inset PM (<b>g</b>) surface-mounted Halbach PM array (<b>h</b>) surface-mounted PM OR (<b>i</b>) consequent pole surface-inset PM (<b>j</b>) surface-mounted PM axial flux.</p>
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<p>Maximum rotor linear velocity of PM motors for electric vehicles [<a href="#B31-energies-17-06199" class="html-bibr">31</a>,<a href="#B32-energies-17-06199" class="html-bibr">32</a>,<a href="#B33-energies-17-06199" class="html-bibr">33</a>,<a href="#B34-energies-17-06199" class="html-bibr">34</a>,<a href="#B35-energies-17-06199" class="html-bibr">35</a>,<a href="#B36-energies-17-06199" class="html-bibr">36</a>,<a href="#B37-energies-17-06199" class="html-bibr">37</a>,<a href="#B38-energies-17-06199" class="html-bibr">38</a>,<a href="#B39-energies-17-06199" class="html-bibr">39</a>,<a href="#B40-energies-17-06199" class="html-bibr">40</a>].</p>
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<p>Radial-axial magnetic flux path in hybrid excited PM machine [<a href="#B50-energies-17-06199" class="html-bibr">50</a>].</p>
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<p>Structure of electric-driven actuators (<b>a</b>) EHA [<a href="#B60-energies-17-06199" class="html-bibr">60</a>] (<b>b</b>) EMA [<a href="#B57-energies-17-06199" class="html-bibr">57</a>].</p>
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<p>The architecture of the three-stage wound-field synchronous SG.</p>
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<p>Typical dual-spool turbofan engine with integrated drive generator (IDG) [<a href="#B105-energies-17-06199" class="html-bibr">105</a>].</p>
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<p>Mechanically failed doubly-salient SG (airgap length = 0.7 mm) (<b>a</b>) rotor (<b>b</b>) stator.</p>
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<p>N3-X Aircraft with a Turboelectric Distributed Propulsion [<a href="#B130-energies-17-06199" class="html-bibr">130</a>].</p>
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<p>Evolution of the hybrid winding configuration [<a href="#B129-energies-17-06199" class="html-bibr">129</a>].</p>
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<p>Temperature dependence of (BH)max for (<b>a</b>) established permanent magnet (PM) materials compared with (<b>b</b>) emerging PM materials [<a href="#B136-energies-17-06199" class="html-bibr">136</a>].</p>
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<p>Temperature-dependent magnetic properties of Fe<sub>16</sub>N<sub>2</sub> low-temperature nitride foil and NdFeB magnets N40 and N52 [<a href="#B139-energies-17-06199" class="html-bibr">139</a>].</p>
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<p>Tested hysteresis loop of high-performance CoFe alloy 1j22.</p>
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<p>Core losses dependency on sheet thickness.</p>
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<p>Lightweight PM rotor made of composites [<a href="#B164-energies-17-06199" class="html-bibr">164</a>].</p>
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<p>Different heat sink designs realized by AM [<a href="#B177-energies-17-06199" class="html-bibr">177</a>].</p>
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<p>Cooling fins integrated with the stator core.</p>
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<p>Typical cooling techniques for high-power density electric machines.</p>
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<p>Schematic representation of Copper-Water heat pipe together with alternative wick constructions [<a href="#B194-energies-17-06199" class="html-bibr">194</a>].</p>
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