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Machines, Volume 11, Issue 1 (January 2023) – 124 articles

Cover Story (view full-size image): In robot-assisted oral surgery, the tool needs to be fed into the target position to perform surgery. However, the manual operation of the surgeon can cause limited accuracy and misoperation. Moreover, the random movements of the patient’s head can cause difficulties with the task. To achieve the task, a motion strategy based on a new conical virtual fixture (VF) was proposed. The VF is formed using a geometry design, two-point adjustment model, and velocity conversion. Meanwhile, a binocular vision system corrects the VF to compensate for the random movement of the patient’s head. As an auxiliary framework for surgical operation, the proposed strategy has the advantages of safety, accuracy, and dynamic adaptability. Both simulations and experiments are conducted, verifying the feasibility of the proposed strategy. View this paper
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19 pages, 2893 KiB  
Article
A Surface Defect Inspection Model via Rich Feature Extraction and Residual-Based Progressive Integration CNN
by Guizhong Fu, Wenwu Le, Zengguang Zhang, Jinbin Li, Qixin Zhu, Fuzhou Niu, Hao Chen, Fangyuan Sun and Yehu Shen
Machines 2023, 11(1), 124; https://doi.org/10.3390/machines11010124 - 16 Jan 2023
Cited by 4 | Viewed by 2744
Abstract
Surface defect inspection is vital for the quality control of products and the fault diagnosis of equipment. Defect inspection remains challenging due to the low level of automation in some manufacturing plants and the difficulty in identifying defects. To improve the automation and [...] Read more.
Surface defect inspection is vital for the quality control of products and the fault diagnosis of equipment. Defect inspection remains challenging due to the low level of automation in some manufacturing plants and the difficulty in identifying defects. To improve the automation and intelligence levels of defect inspection, a CNN model is proposed for the high-precision defect inspection of USB components in the actual demands of factories. First, the defect inspection system was built, and a dataset named USB-SG, which contained five types of defects—dents, scratches, spots, stains, and normal—was established. The pixel-level defect ground-truth annotations were manually marked. This paper puts forward a CNN model for solving the problem of defect inspection tasks, and three strategies are proposed to improve the model’s performance. The proposed model is built based on the lightweight SqueezeNet network, and a rich feature extraction block is designed to capture semantic and detailed information. Residual-based progressive feature integration is proposed to fuse the extracted features, which can reduce the difficulty of model fine-tuning and improve the generalization ability. Finally, a multi-step deep supervision scheme is proposed to supervise the feature integration process. The experiments on the USB-SG dataset prove that the model proposed in this paper has better performance than that of other methods, and the running speed can meet the real-time demand, which has broad application prospects in the industrial inspection scene. Full article
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<p>The defect inspection system and dataset generation process.</p>
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<p>The sample images and ground truth of the five types of defects.</p>
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<p>The architecture of the modelling approach via rich feature extraction and residual-based progressive integration.</p>
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<p>Comparison of the proposed feature extraction strategy and the two existing structures. (<b>a</b>) Extraction of features by using the last layer in the deep stage [<a href="#B24-machines-11-00124" class="html-bibr">24</a>,<a href="#B25-machines-11-00124" class="html-bibr">25</a>]. (<b>b</b>) Extraction of features by using the last layer in all stages [<a href="#B36-machines-11-00124" class="html-bibr">36</a>,<a href="#B37-machines-11-00124" class="html-bibr">37</a>]. (<b>c</b>) Proposed: Extraction of features by using all of the layers in all stages.</p>
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<p>The details of the generative process of the <span class="html-italic">i</span>th rich feature extraction block.</p>
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<p>A detailed structural diagram of the residual-based progressive integration scheme.</p>
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<p>A diagram of the predicted results and ground truth.</p>
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<p>Visual comparisons of different predictions. Four types of defects (dents, scratches, spots, and stains) are shown in order.</p>
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<p>Visual comparisons of different defect/object localization models.</p>
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20 pages, 10234 KiB  
Article
Strength Analysis and Structure Optimization of the Crankshaft of an Opposed-Power Reciprocating Pump
by Chuan Liu, Xiuting Wei, Zuyao Yi, Zhiqin Li, Changhao Zhu and Ze Ma
Machines 2023, 11(1), 123; https://doi.org/10.3390/machines11010123 - 16 Jan 2023
Cited by 3 | Viewed by 2665
Abstract
The opposed-power reciprocating pump has the characteristics of high pressure, large flow, and high efficiency and energy saving. However, due to the special structure of the opposed-power reciprocating pump, existing theoretical methods cannot analyze its dynamic performance. Therefore, this paper proposes a method [...] Read more.
The opposed-power reciprocating pump has the characteristics of high pressure, large flow, and high efficiency and energy saving. However, due to the special structure of the opposed-power reciprocating pump, existing theoretical methods cannot analyze its dynamic performance. Therefore, this paper proposes a method of analyzing the power end of the opposed-power reciprocating pump. Firstly, according to the working principle and structural characteristics of the traditional plunger pump, the novel and complex structure of the opposed-power reciprocating pump is analyzed by analogy, and the force analysis model of the crankshaft is established. The dynamic analysis model of the Matlab program is used to solve the dynamic load and section stress in the working process, and the variation law of crankshaft load is obtained. The 25 most critical working conditions are selected for analysis, and the most critical station and section of the crankshaft are obtained. With the connection between ANSYS Workbench and Solidworks, the model is imported into ANSYS Workbench, the load on the crank pin is loaded by APDL command flow, and the static analysis of the crankshaft is carried out to obtain the stress and strain of the crankshaft. Finally, the static and fatigue strength of the dangerous section is checked, and it is proven that the strength and stiffness of the crankshaft meet the design requirements. The results show that the dynamic analysis results of the crankshaft under critical working conditions are consistent with the finite element analysis, verifying the rationality of the method and providing a reference for the improvement and optimized design of the crankshaft of the opposed-power reciprocating pump. Full article
(This article belongs to the Section Electromechanical Energy Conversion Systems)
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<p>Opposed-power reciprocating pump mechanism structure: 1. Extension rod, 2. Crosshead, 3. Rear bearing, 4. Fore bearing, 5. Left join segment, 6. Box, 7. Rod, 8. Crankshaft, 9. Upper box, 10. Right join segment, 11. Lower box.</p>
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<p>Opposed-power reciprocating pump in a separate column: 1. Plunger, 2. Manger, 3. Extension rod, 4. Crosshead, 5. Rod, 6. Crankshaft.</p>
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<p>Schematic diagram of the motion and force of the Crank double-slider mechanism.</p>
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<p>Force analysis of the crankshaft.</p>
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<p>Diagram of the crankshaft driving torque.</p>
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<p>Diagram of the tangential force of the gear.</p>
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<p>Diagram of the radial force of the gear.</p>
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<p>Diagram of force analysis on support 1 of the crankshaft.</p>
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<p>Diagram of force analysis on middle support 3 of the crankshaft.</p>
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<p>(<b>a</b>) Diagram of the x-direction support reaction force <span class="html-italic">N<sub>kx</sub></span> of each support seat of the crankshaft, (<b>b</b>) Diagram of the y-direction support reaction force <span class="html-italic">N<sub>ky</sub></span> of each support seat of the crankshaft.</p>
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<p>Crankshaft critical sections.</p>
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<p>(<b>a</b>) Diagram of the rod force changing with the first angle, (<b>b</b>) Diagram of the torque changing with the first angle.</p>
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<p>Diagram of stress variation in Section 17.</p>
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<p>SOLID187 unit figure.</p>
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<p>Crankshaft grid mode.</p>
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<p>Diagram of load distribution on the crank pin.</p>
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<p>Schematic diagram of the load on the crank pin and the change curve of the first crankshaft angle.</p>
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<p>(<b>a</b>) Diagram of maximum equivalent stress of crankshaft under 25 working conditions. (<b>b</b>) Diagram of maximum shape variable of the crankshaft under 25 working conditions.</p>
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<p>(<b>a</b>) Diagram of the maximum equivalent stress of the crankshaft when the first crankshaft angle was 90°, (<b>b</b>) Diagram of the maximum shape variable of the crankshaft when the first crankshaft angle was 90°.</p>
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<p>Diagram of the crankshaft automatic meshing.</p>
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<p>Diagram of maximum equivalent stress under automatic meshing.</p>
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<p>Diagram of the refined crankshaft meshing.</p>
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<p>Diagram of the maximum equivalent stress under mesh refinement.</p>
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12 pages, 53808 KiB  
Article
Research on Edge Detection Model of Insulators and Defects Based on Improved YOLOv4-tiny
by Boqiang Li, Liang Qin, Feng Zhao, Haofeng Liu, Jinyun Yu, Min He, Jing Wang and Kaipei Liu
Machines 2023, 11(1), 122; https://doi.org/10.3390/machines11010122 - 16 Jan 2023
Cited by 2 | Viewed by 2554
Abstract
Edge computing can avoid the long-distance transmission of massive data and problems with large-scale centralized processing. Hence, defect identification for insulators with object detection models based on deep learning is gradually shifting from cloud servers to edge computing devices. Therefore, we propose a [...] Read more.
Edge computing can avoid the long-distance transmission of massive data and problems with large-scale centralized processing. Hence, defect identification for insulators with object detection models based on deep learning is gradually shifting from cloud servers to edge computing devices. Therefore, we propose a detection model for insulators and defects designed to deploy on edge computing devices. The proposed model is improved on the basis of YOLOv4-tiny, which is suitable for edge computing devices, and the detection accuracy of the model is improved on the premise of maintaining a high detection speed. First, in the neck network, the inverted residual module is introduced to perform feature fusion to improve the positioning ability of the insulators. Then, a high-resolution detection output head is added to the original model to enhance its ability to detect defects. Finally, the prediction boxes are post-processed to incorporate split object boxes for large-scale insulators. In an experimental evaluation, the proposed model achieved an mAP of 96.22% with a detection speed of 10.398 frames per second (FPS) on an edge computing device, which basically meets the requirements of insulator and defect detection scenarios in edge computing devices. Full article
(This article belongs to the Section Robotics, Mechatronics and Intelligent Machines)
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<p>YOLOv4-tiny network structure.</p>
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<p>Structure of the inverted residual module.</p>
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<p>Structure of SE.</p>
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<p>Overall network structure of improved YOLOv4-tiny.</p>
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<p>Flowchart of the post-processing of prediction boxes.</p>
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15 pages, 9123 KiB  
Article
A 4D-Printed Self-Folding Spatial Mechanism with Pre-Stressed Response Properties
by Wencai Zhang and Duanling Li
Machines 2023, 11(1), 121; https://doi.org/10.3390/machines11010121 - 16 Jan 2023
Viewed by 1745
Abstract
Exploring the transformation of spatial mechanisms from their unfolded to controlled folding states to meet the requirements of various application scenarios has long been a hot topic in mechanical structure research. Although conventional spatial mechanisms can be designed to meet almost any application [...] Read more.
Exploring the transformation of spatial mechanisms from their unfolded to controlled folding states to meet the requirements of various application scenarios has long been a hot topic in mechanical structure research. Although conventional spatial mechanisms can be designed to meet almost any application scenario, the design’s complex and excessive combinations of structural components, kinematic pairs, and drive units are unavoidable. It introduces many problems, such as poor reliability, drive complexity, and control difficulties. Based on 4D printing technology, the design of self-folding spatial mechanisms that use pre-stressed response properties under predetermined thermal excitation to achieve different shrinkage ratios integrates the control and drive system and the structural components and kinematic pairs. It brings novel features of self-folding while effectively avoiding many problems associated with conventional mechanical design. Further, the pre-stressed response model introduces the self-folding spatial mechanisms’ excitation, morphing, and driving investigation. Self-folding spatial mechanisms with different shrinkage ratios were prepared via fused deposition modeling, which verified the theoretical analysis and pre-stress response model and the design’s correctness and feasibility by experiments. The existing 4D printing technology lacks a paradigmatic design method in the application field. Contrarily, this work organically combined the conventional mechanical structure design with materials and fabrication via fused deposition modeling. A systematic study of self-folding spatial mechanisms from structural design to morphing control was carried out. This design is expected to introduce a novel paradigm of 4D printing technology in conventional mechanical design and has considerable application prospects in spherical radar calibration mechanisms. Full article
(This article belongs to the Special Issue Recent Advances in Smart Design and Manufacturing Technology)
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<p>Schematic of the design and operating mode of the SFSM.</p>
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<p>Schematic of the construction process of the SFSM: (<b>a</b>) the SFR and the ASR, (<b>b</b>) construct of the SFRM, (<b>c</b>) construct of the SFSM (left to right by order of appearance).</p>
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<p>Schematic of the rectangular coordinate system of the ASRs and SFRs.</p>
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<p>Plane kinetic chain with <span class="html-italic">m</span> value of 12.</p>
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<p>Schematic of self-folding: (<b>a</b>) SFR and ASR self-folding, (<b>b</b>) SFRM self-folding, (<b>c</b>) SFSM self-folding.</p>
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<p>DMA test results: Storage modulus and dielectric loss angle of PLA (<b>left</b>) and storage modulus of TPU (<b>right</b>).</p>
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<p>Schematic of the manufacturing process of the SFR.</p>
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<p>Experiments on the effect of different filling patterns of TPU layer on bending: (<b>a</b>) TPU material 90° cross alignment, (<b>b</b>) TPU 90° side-by-side alignment, (<b>c</b>) TPU material 45° cross alignment, (<b>d</b>) TPU 180° side-by-side alignment.</p>
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<p>Experiment on the influence of TPU layer pre-stressed restricting capability on the change in folding angle <span class="html-italic">τ</span>.</p>
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<p>The 3D optical scanning processes.</p>
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<p>Experiment on the influence of PLA pre-stress storage capability on the change in folding angle <span class="html-italic">τ</span>.</p>
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<p>The self-folding experiment with the SFSM.</p>
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21 pages, 4474 KiB  
Article
Numerical Investigation on the Combustion and Emission Characteristics of Diesel Engine with Flexible Fuel Injection
by Qihao Mei, Intarat Naruemon, Long Liu, Yue Wu and Xiuzhen Ma
Machines 2023, 11(1), 120; https://doi.org/10.3390/machines11010120 - 16 Jan 2023
Cited by 3 | Viewed by 2310
Abstract
As the main engineering power plant, diesel engines are irreplaceable in the future. However, the stringent emission regulations impose many tough requirements to their developments. Recently, flexible fuel injection strategy has been recognized as an effective technology in creating an advanced spray and [...] Read more.
As the main engineering power plant, diesel engines are irreplaceable in the future. However, the stringent emission regulations impose many tough requirements to their developments. Recently, flexible fuel injection strategy has been recognized as an effective technology in creating an advanced spray and mixture formation and improving combustion efficiency indirectly. However, the detailed combustion and emission behaviors under flexible fuel injection are still unknown. Therefore, this paper aims to investigate the combustion and emission characteristics under flexible fuel injection and explore an optimal injection strategy for high-efficiency combustion. A numerical simulation method is conducted by coupling the large-eddy simulation (LES) model and the SAGE combustion model. Then, the spray mixing, combustion flame propagation and emissions formation under various multiple-injection strategies are investigated. Results reveal that initial an ultrahigh injection pressure has a significant influence on the spray’s axial penetration while dwell time mainly affects the spray’s radial expansion. Under an initial ultrahigh injection pressure, the turbulence kinetic energy (TKE) becomes larger, and the vortex motions are stronger, contributing to a better spray turbulent mixing. Meanwhile, a snatchier flame structure with a favorable level of equivalence ratio and a homogeneous temperature distribution is obtained. In this way, the peak heat release rate (HRR) could increase by 46.7% with a 16.7% reduction in soot formation and a 31.4% reduction in NOx formation. Full article
(This article belongs to the Special Issue Advances in Combustion Science for Future IC Engines)
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<p>Geometric structure of CVCC and computational domain.</p>
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<p>Evolution process of spray combustion flame in different cases: (<b>a</b>) case 1; (<b>b</b>) case 2.</p>
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<p>Comparison of simulation results of HRR and experimental data in different cases.</p>
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<p>Injection rate shapes of various multiple-injection strategies.</p>
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<p>Variations of spray angle and spray boundaries in different multiple-injection strategies.</p>
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<p>Spray characteristics distribution history in different multiple-injection strategies: (<b>a</b>) TKE; (<b>b</b>) equivalence ratio.</p>
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<p>Spray characteristics distribution history in different multiple-injection strategies: (<b>a</b>) TKE; (<b>b</b>) equivalence ratio.</p>
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<p>Variation of combustion chamber pressure and flame temperature.</p>
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<p>Variation of HRR in different multiple-injection strategies.</p>
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<p>Formation history of soot and NO<sub>x</sub> emissions in different multiple-injection strategies: (<b>a</b>) macroscopic variations; (<b>b</b>) microscopic distributions.</p>
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<p>Formation history of soot and NO<sub>x</sub> emissions in different multiple-injection strategies: (<b>a</b>) macroscopic variations; (<b>b</b>) microscopic distributions.</p>
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20 pages, 6770 KiB  
Article
Early Fault Diagnosis of Rolling Bearing Based on Threshold Acquisition U-Net
by Dongsheng Zhang, Laiquan Zhang, Naikang Zhang, Shuo Yang and Yuhao Zhang
Machines 2023, 11(1), 119; https://doi.org/10.3390/machines11010119 - 15 Jan 2023
Cited by 2 | Viewed by 2233
Abstract
Considering the problem that the early fault signal of rolling bearing is easily interfered with by background information, such as noise, and it is difficult to extract fault features, a method of rolling bearing early fault diagnosis based on the threshold acquisition U-Net [...] Read more.
Considering the problem that the early fault signal of rolling bearing is easily interfered with by background information, such as noise, and it is difficult to extract fault features, a method of rolling bearing early fault diagnosis based on the threshold acquisition U-Net (TA-UNet) is proposed. First, to improve the feature extraction ability of U-Net, the channel spatial threshold acquisition network (CS-TAN) and the dilated convolution module (DCM) based on different dilated rate combinations are introduced into the U-Net to construct the TA-UNet. Among them, the CS-TAN can adaptively learn the threshold, reduce the interference of noise in the signal, and the DCM can improve the multi-scale feature extraction ability of the network. Then, the TA-UNet is used for early fault diagnosis, and the method is divided into two steps: The model training phase and the vibration signal fault feature extraction phase. In the first step, additive gaussian white noise is added to the vibration signal to obtain the noise-added vibration signal, and the TA-UNet is trained to learn how to denoise the noise-added vibration signal. In the second step, the trained TA-UNet is used to extract the fault features of vibration signals and diagnose the early fault types of rolling bearing. The two-step method solves the problem that U-Net, as a supervised neural network, needs corresponding labeled data to be trained, as it realizes the fault diagnosis of unlabeled data. The feature extraction capability of the TA-UNet is evaluated by denoising the simulated signal of rolling bearing. The effectiveness of the proposed diagnostic method is demonstrated by the early fault diagnosis of open-source datasets. Full article
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<p>Structure of channel threshold acquisition network (C-TAN) and channel spatial threshold acquisition network (CS-TAN). (<b>a</b>) Structure of C-TAN; (<b>b</b>) Structure of CS-TAN.</p>
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<p>Dilated convolution module with exponentially increasing dilated rate (<span class="html-italic">r</span> = 1, 2, 4), stride = 1, kernel size = 3.</p>
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<p>Structure of the proposed TA-UNet.</p>
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<p>t-SNE reduces the dimension of the vibration signal and the implicit feature of the vibration signal. (<b>a</b>) t-SNE reduces the dimension of the vibration signal; (<b>b</b>) t-SNE reduces the dimension of the implicit feature of the vibration signal.</p>
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<p>Early fault diagnosis method of rolling bearing based on TA-UNet.</p>
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<p>TA-UNet noise reduction results for simulation signal with SNR = −45 dB. (<b>a</b>) Simulation signal with SNR = −45 dB; (<b>b</b>) Noise reduction results of simulation signal by TA-UNet; (<b>c</b>) Impulse signal.</p>
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<p>Noise reduction results of different networks for different SNRs.</p>
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<p>Training Process of TA-UNet for SNR = −45 dB simulation signal noise reduction. (<b>a</b>) outer fault impulse signal; (<b>b</b>) simulation signal with SNR = −45 dB; (<b>c</b>) training process of TA-UNet, epochs are 10 in turn, 20, 30, 40, 60, 80, 100 (from left to right).</p>
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<p>The layout of the bearing accelerated degradation test rig of Case 1.</p>
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<p>The RMS trend of bearing vibration signal in Case 1.</p>
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<p>Waveform and envelope spectrum of vibration signal and noise-reduced vibration signal in Case 1. (<b>a</b>) Waveform of vibration signal and noise-reduced vibration signal; (<b>b</b>) Envelope spectrum of vibration signal; (<b>c</b>) Envelope spectrum of noise reduction signal.</p>
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<p>The envelope spectrum of the noise reduction vibration signal obtained by EEMD, VMD, WPD, and the proposed method in Case 1. (<b>a</b>) EEMD; (<b>b</b>) VMD; (<b>c</b>) WPD; (<b>d</b>) The proposed method.</p>
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<p>Envelope spectrum of vibration signal and different noise-reduced vibration signals in Case 1. (<b>a</b>) Envelope spectrum of vibration signal; (<b>b</b>) Envelope spectrum of noise-reduced vibration signal by AG-UNet; (<b>c</b>) Envelope spectrum of noise-canceling vibration signal by U-Net; (<b>d</b>) Envelope spectrum of noise-canceling vibration signal by TA-UNet.</p>
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<p>The layout of the bearing accelerated degradation test rig of Case 2.</p>
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<p>The RMS trend of vibration signal in Case 2.</p>
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<p>Waveform and envelope spectrum of vibration signal and noise reduction signal in Case 2. (<b>a</b>) Waveform of vibration signal and noise reduction signal; (<b>b</b>) Envelope spectrum of vibration signal; (<b>c</b>) Envelope spectrum of noise reduction signal.</p>
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<p>The envelope spectrum of the noise reduction vibration signal obtained by EEMD, VMD, WPD, and the proposed method in Case 2. (<b>a</b>) EEMD; (<b>b</b>) VMD; (<b>c</b>) WPD; (<b>d</b>) The proposed method.</p>
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<p>Envelope spectrum of vibration signal and different noise reduction signals in Case 2. (<b>a</b>) Envelope spectrum of vibration signal; (<b>b</b>) Envelope spectrum of noise reduction signal by AG-UNet; (<b>c</b>) Envelope spectrum of noise reduction signal by U-Net; (<b>d</b>) Envelope spectrum of noise reduction signal by TA-UNet.</p>
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22 pages, 6534 KiB  
Article
Modification and Validation of 1D Loss Models for the Off-Design Performance Prediction of Centrifugal Compressors with Splitter Blades
by Xiuxin Yang, Yan Liu and Guang Zhao
Machines 2023, 11(1), 118; https://doi.org/10.3390/machines11010118 - 15 Jan 2023
Cited by 2 | Viewed by 2246
Abstract
One-dimensional (1D) aerodynamic performance predictions are very often conducted by researchers and designers during the preliminary design of centrifugal compressors. This paper focuses on a 1D prediction method for centrifugal compressors with splitter blades, which is rarely seen in the open literature. One-dimensional [...] Read more.
One-dimensional (1D) aerodynamic performance predictions are very often conducted by researchers and designers during the preliminary design of centrifugal compressors. This paper focuses on a 1D prediction method for centrifugal compressors with splitter blades, which is rarely seen in the open literature. One-dimensional prediction of aerodynamic overall performance is made for centrifugal compressors with different technical design specifications. However, the aerodynamic overall prediction accuracy relies on the accuracy of the 1D-loss-models used. Therefore, an optimum combination of loss models is proposed by summarizing a variety of loss models presented in the public literature. In addition, an optimization method is utilized to optimize some coefficients involved in loss models in order to improve the generality of the combined model. The modified models obtained in this study are proved to have good predictive accuracy. Full article
(This article belongs to the Section Turbomachinery)
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<p>Meridional channel of the computational domain.</p>
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<p>Different types of impellers: (<b>a</b>) Impeller without splitter blades; (<b>b</b>) Impeller with one row of splitter blades; (<b>c</b>) Impeller with two rows of splitter blades.</p>
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<p>Decomposition of the impeller with splitter blades: (<b>a</b>) Impeller with one row of splitter blades; (<b>b</b>) Impeller with two rows of splitter blades.</p>
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<p>Aerodynamic calculation process for an impeller with splitter blades.</p>
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<p>Performance comparison for: (<b>a</b>) Krain impeller; (<b>b</b>) Eckardt-O impeller.</p>
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<p>Performance comparison for two methods for the SRV2-O impeller: (<b>a</b>) Total pressure ratio; (<b>b</b>) Isentropic efficiency.</p>
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<p>Performance comparison for two methods for Impeller R: (<b>a</b>) Total pressure ratio; (<b>b</b>) Isentropic efficiency.</p>
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<p>Performance comparison for two methods for Impeller J: (<b>a</b>) Total pressure ratio; (<b>b</b>) Isentropic efficiency.</p>
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<p>Eckardt-O performance comparison: (<b>a</b>) Total pressure ratio comparison; (<b>b</b>) Efficiency comparison.</p>
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<p>Pareto front for the Eckardt-O impeller.</p>
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<p>Comparisons of 1D predicted performance before and after optimization for the Krain impeller: (<b>a</b>) Total pressure ratio before optimization; (<b>b</b>) Total pressure ratio after optimization; (<b>c</b>) Efficiency before optimization; (<b>d</b>) Efficiency after optimization.</p>
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<p>Comparisons of the 1D predicted performance before and after optimization for the Eckardt-O impeller: (<b>a</b>) Total pressure ratio before optimization; (<b>b</b>) Total pressure ratio after optimization; (<b>c</b>) Efficiency before optimization; (<b>d</b>) Efficiency after optimization.</p>
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<p>Comparisons of different 1D prediction for the Eckardt-O impeller: (<b>a</b>) Total pressure ratio; (<b>b</b>) Isentropic efficiency.</p>
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<p>Comparisons of the 1D predicted performance before and after optimization for the SRV2-O impeller: (<b>a</b>) Total pressure ratio before optimization; (<b>b</b>) Total pressure ratio after optimization; (<b>c</b>) Efficiency before optimization; (<b>d</b>) Efficiency after optimization.</p>
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<p>Comparisons of the 1D predicted performance before and after optimization for the R impeller: (<b>a</b>) Total pressure ratio before optimization; (<b>b</b>) Total pressure ratio after optimization; (<b>c</b>) Efficiency before optimization; (<b>d</b>) Efficiency after optimization.</p>
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<p>Comparisons of the 1D predicted performance before and after optimization for the impeller J: (<b>a</b>) Total pressure ratio before optimization; (<b>b</b>) Total pressure ratio after optimization; (<b>c</b>) Efficiency before optimization; (<b>d</b>) Efficiency after optimization.</p>
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18 pages, 4462 KiB  
Article
Anti-Rollover Control and HIL Verification for an Independently Driven Heavy Vehicle Based on Improved LTR
by Lufeng Zheng, Yongjie Lu, Haoyu Li and Junning Zhang
Machines 2023, 11(1), 117; https://doi.org/10.3390/machines11010117 - 14 Jan 2023
Cited by 6 | Viewed by 2753
Abstract
The rollover evaluation index provides an important threshold basis for the anti-rollover control system of vehicle. Regarding the rollover risk of independently driven heavy-duty vehicles, a new rollover evaluation index is proposed, and the feasibility of the improved index was verified through hierarchical [...] Read more.
The rollover evaluation index provides an important threshold basis for the anti-rollover control system of vehicle. Regarding the rollover risk of independently driven heavy-duty vehicles, a new rollover evaluation index is proposed, and the feasibility of the improved index was verified through hierarchical control and HIL (hardware-in-the-loop) experiments. Based on an 18-DOF spatial dynamics model of a heavy-duty vehicle, the improved LTR (load transfer rate) index was obtained to describe the dynamic change in the tire’s vertical load. It replaces the suspension force and the vertical inertia force of the unsprung load mass. It avoids the problem of directly measuring or estimating the vertical load in the LTR index. Under the conditions of fishhooking and angle stepping, three types of rollover indicators were compared, and the proposed index can more sensitively identify the likelihood of rollover. In order to apply the improved rollover index to a rollover control well, a hierarchical controller based on the identification of the slip rate of the road surface, ABS control with sliding mode, variable structure and differential braking was designed. Simulations and HIL tests proved that the designed controller can accurately predict the rollover risk and avoid the rollover in time. Under the condition of J-turning, the yaw rate, slip angle and maximum lateral acceleration are reduced by 9%, 16% and 3%, respectively; under the condition of fishhooking, the maximum yaw rate, slip angle and lateral acceleration are reduced by 12%, 18% and 3%, respectively. Full article
(This article belongs to the Special Issue Advanced Modeling, Analysis and Control for Electrified Vehicles)
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<p>Vehicle model diagram.</p>
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<p>Algorithmic flow of the new rollover evaluation index.</p>
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<p>Comparison of three types of rollover indicators in time domain.</p>
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<p>Comparison of three types of rollover indicators.</p>
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<p>Anti-rollover control strategy based on the NLTR index.</p>
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<p>Differential braking control logic diagram.</p>
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<p>Steering wheel angle.</p>
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<p>J-turn.</p>
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<p>Fishhook.</p>
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<p>HIL flowchart.</p>
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<p>J-turn.</p>
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<p>Fishhook.</p>
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18 pages, 4867 KiB  
Article
The Graph Neural Network Detector Based on Neighbor Feature Alignment Mechanism in LIDAR Point Clouds
by Xinyi Liu, Baofeng Zhang and Na Liu
Machines 2023, 11(1), 116; https://doi.org/10.3390/machines11010116 - 14 Jan 2023
Cited by 3 | Viewed by 2349
Abstract
Three-dimensional (3D) object detection has a vital effect on the environmental awareness task of autonomous driving scenarios. At present, the accuracy of 3D object detection has significant improvement potential. In addition, a 3D point cloud is not uniformly distributed on a regular grid [...] Read more.
Three-dimensional (3D) object detection has a vital effect on the environmental awareness task of autonomous driving scenarios. At present, the accuracy of 3D object detection has significant improvement potential. In addition, a 3D point cloud is not uniformly distributed on a regular grid because of its disorder, dispersion, and sparseness. The strategy of the convolution neural networks (CNNs) for 3D point cloud feature extraction has the limitations of potential information loss and empty operation. Therefore, we propose a graph neural network (GNN) detector based on neighbor feature alignment mechanism for 3D object detection in LiDAR point clouds. This method exploits the structural information of graphs, and it aggregates the neighbor and edge features to update the state of vertices during the iteration process. This method enables the reduction of the offset error of the vertices, and ensures the invariance of the point cloud in the spatial domain. For experiments performed on the KITTI public benchmark, the results demonstrate that the proposed method achieves competitive experimental results. Full article
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<p>Framework overview.</p>
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<p>The dynamic sparsification-based point cloud processing. Firstly, we define the expression of the voxel grid as <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>i</mi> </msub> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>×</mo> <msub> <mi>C</mi> <mn>1</mn> </msub> </mrow> </msup> </mrow> </semantics></math>. Secondly, to ensure the invariance of the point cloud structure in the spatial domain, the local voxel feature <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>l</mi> <mi>o</mi> <mi>c</mi> </mrow> </msub> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>×</mo> <msub> <mi>C</mi> <mn>2</mn> </msub> </mrow> </msup> </mrow> </semantics></math> is obtained by mapping the voxel feature <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>i</mi> </msub> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>×</mo> <msub> <mi>C</mi> <mn>1</mn> </msub> </mrow> </msup> </mrow> </semantics></math> using MLP. This feature includes the number of voxel grids and the number of points contained in the grid. Then, according to the number of points contained in the grid sort the voxel grid, the binary mask <math display="inline"><semantics> <mover accent="true"> <mi>D</mi> <mo stretchy="false">^</mo> </mover> </semantics></math> is obtained. Finally, the local voxel feature expression <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mi>l</mi> </msub> <mi>o</mi> <mi>c</mi> </mrow> </semantics></math> and the binary mask <math display="inline"><semantics> <mover accent="true"> <mi>D</mi> <mo stretchy="false">^</mo> </mover> </semantics></math> are aggregated to obtain the global voxel feature <math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>g</mi> <mi>l</mi> <mi>o</mi> <mi>b</mi> <mi>a</mi> <mi>l</mi> </mrow> </msub> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>×</mo> <msub> <mi>C</mi> <mn>2</mn> </msub> </mrow> </msup> </mrow> </semantics></math>.</p>
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<p>Construction strategy for edge features in the graph. Red indicates the vertex, and blue indicates its neighbors.</p>
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<p>GNN based on neighbor feature alignment mechanism in a single iteration.</p>
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<p>The classical GNN.</p>
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<p>The encoding neighbor method.</p>
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<p>The feature aggregation method.</p>
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<p>The neighbor feature alignment mechanism.</p>
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<p>The message passing and state updating process of our method.</p>
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<p>The parameterization of the bounding box.</p>
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<p>Qualitative results for cyclist and pedestrian categories on the KITTI dataset.</p>
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<p>The qualitative results on the KITTI dataset.</p>
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32 pages, 2644 KiB  
Article
Ensemble Classifier for Recognition of Small Variation in X-Bar Control Chart Patterns
by Waseem Alwan, Nor Hasrul Akhmal Ngadiman, Adnan Hassan, Syahril Ramadhan Saufi and Salwa Mahmood
Machines 2023, 11(1), 115; https://doi.org/10.3390/machines11010115 - 14 Jan 2023
Cited by 5 | Viewed by 1888
Abstract
Manufacturing processes have become highly accurate and precise in recent years, particularly in the chemical, aerospace, and electronics industries. This has attracted researchers to investigate improved procedures for monitoring and detection of small process variations to remain in line with such advances. Among [...] Read more.
Manufacturing processes have become highly accurate and precise in recent years, particularly in the chemical, aerospace, and electronics industries. This has attracted researchers to investigate improved procedures for monitoring and detection of small process variations to remain in line with such advances. Among these techniques, statistical process controls (SPC), in particular the control chart pattern (CCP), have become a popular choice for monitoring process variance, being utilized in numerous industrial and manufacturing applications. This study provides an improved control chart pattern recognition (CCPR) method focusing on X-bar chart patterns of small process variations using an ensemble classifier comprised of five complementing algorithms: decision tree, artificial neural network, linear support vector machine, Gaussian support vector machine, and k-nearest neighbours. Before advancing to the classification step, Nelson’s Rus Rules were utilized as a monitoring rule to distinguish between stable and unstable processes. The study’s findings indicate that the proposed method improves classification performance for patterns with mean changes of less than 1.5 sigma, and confirm that the performance of the ensemble classifier is superior to that of the individual classifier. The ensemble classifier can distinguish unstable pattern types with a classification accuracy of 99.55% and an ARL1 of 11.94. Full article
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<p>Flowchart of the models using normal shift and small shift datasets.</p>
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<p>Structure of an Ensemble Classifier with Majority Voting.</p>
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<p>The training flowchart for the fully developed patterns model using normal shift and small shift datasets.</p>
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<p>Testing flowchart for the fully developed patterns model using normal shift and small shift datasets.</p>
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<p>The training flowchart for the developing patterns model using normal shift and small shift datasets.</p>
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<p>Testing flowchart for the developing patterns model using normal shift and small shift datasets.</p>
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20 pages, 6489 KiB  
Article
Fault Prediction of On-Board Train Control Equipment Using a CGAN-Enhanced XGBoost Method with Unbalanced Samples
by Jiang Liu, Kangzhi Xu, Baigen Cai and Zhongbin Guo
Machines 2023, 11(1), 114; https://doi.org/10.3390/machines11010114 - 14 Jan 2023
Cited by 8 | Viewed by 2595
Abstract
On-board train control equipment is an important component of the Train Control System (TCS) of railway trains. In order to guarantee the safe and efficient operation of the railway system, Predictive Maintenance (PdM) is significantly required. The operation data of the on-board equipment [...] Read more.
On-board train control equipment is an important component of the Train Control System (TCS) of railway trains. In order to guarantee the safe and efficient operation of the railway system, Predictive Maintenance (PdM) is significantly required. The operation data of the on-board equipment allow us to build fault prediction models using a data-driven approach. However, the problem of unbalanced fault samples makes it difficult to achieve the expected modeling performance. In this paper, a Conditional Generative Adversarial Network (CGAN) is adopted to solve the unbalancing problem by generating synthetic samples corresponding to specific fault labels that belong to the minority classes. With this basis, a CGAN-enhanced eXtreme Gradient Boosting (XGBoost) solution is presented for training the fault prediction models. From the pre-processing to the field data, artificial fault samples are generated and integrated into the training sample sets, and the XGBoost models can be derived with multiple decision trees. Both the feature importance sequence list and the knowledge graph are derived to describe the characteristics obtained by the models. Filed data sets from practical operation are utilized to validate the proposed solution. By comparison with conventional machine learning algorithms, it can be found that higher accuracy, precision, recall, and F1 scores, which are up to 99.76%, can be achieved by the proposed solution. By involving the CGAN strategy, the maximum enhancement to the F1 score with the XGBoost approach reaches 6.13%. The advantages of the proposed solution show great potential in implementing equipment health management and intelligent condition-based maintenance. Full article
(This article belongs to the Special Issue Advances in Fault Diagnosis and Anomaly Detection)
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<p>Structure of the CTCS2-200H on-board train control equipment.</p>
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<p>Structure diagram of CGAN-enhanced XGBoost method for fault prediction.</p>
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<p>Procedures of raw data processing for training sample extraction.</p>
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<p>Work low of the CGAN augmentation process.</p>
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<p>Procedures of fault prediction model training by CGAN and XGBoost.</p>
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<p>Comparison of the generated and real sample features at different epochs.</p>
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<p>Comparison of the data distribution corresponding to six main features.</p>
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<p>Results of XGBoost training using CGAN-enhanced 2018-T(A) sample set.</p>
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<p>Results of XGBoost training using CGAN-enhanced 2018-T(B) sample set.</p>
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<p>Results of XGBoost training using CGAN-enhanced 2018-T(C) sample set.</p>
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<p>Typical sub-model (tree) of the ensemble by the training with 2018-T(A).</p>
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<p>Typical sub-model (tree) of the ensemble by the training with 2018-T(B).</p>
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<p>Typical sub-model (tree) of the ensemble by the training with 2018-T(C).</p>
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<p>XGBoost performance using raw sample sets with different iteration numbers.</p>
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<p>XGBoost performance using CGAN-enhanced sets with different iteration numbers.</p>
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32 pages, 4482 KiB  
Article
Common Noninteracting Control with Simultaneous Common Partial Zeroing with Application to a Tracked UGV
by Fotis N. Koumboulis and Nikolaos D. Kouvakas
Machines 2023, 11(1), 113; https://doi.org/10.3390/machines11010113 - 14 Jan 2023
Viewed by 1712
Abstract
In several MIMO system applications, the deviations of some output performance variables from their nominal values are required to be controlled independently, while the other performance variables are required to remain at their nominal value. This problem, named noninteracting control with simultaneous partial [...] Read more.
In several MIMO system applications, the deviations of some output performance variables from their nominal values are required to be controlled independently, while the other performance variables are required to remain at their nominal value. This problem, named noninteracting control with simultaneous partial output zeroing, is important in the case of the common design of multi-model systems. To this end, the problem of a common noninteracting control with simultaneous common partial output zeroing is formulated. The present paper aims to develop a solution to the problem of multi-model normal linear time-invariant systems via regular and static measurement output feedback. The present approach follows the method developed for the solution of the common I/O decoupling problem. The main results of the paper are the introduction and the formulation of the problem at hand, the establishment of the necessary and sufficient conditions for its solvability, and the derivation of the respective general solution of the controller matrices. For the resulting closed-loop system, the additional design requirement of approximate command following a simultaneous I/O stabilizability is studied using a composite norm 2 type cost function and a metaheuristic algorithm for the derivation of the free parameters of the controller. The present results are illustrated through a numerical example of a nonlinear process with two operating points. Moreover, all the above results are successfully applied to the two-model description of a robot-tracked UGV, using a common controller feeding back measurements of the motor currents and the orientation of the vehicle. Full article
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<p>Modified logistic function.</p>
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<p>Forward velocity of the vehicle.</p>
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<p>Angular velocity of the vehicle.</p>
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<p>Heading angle of the vehicle.</p>
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<p>Motor currents.</p>
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<p>Motor angular velocities.</p>
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<p>Track forces.</p>
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<p>Voltage supplies.</p>
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<p>Forward velocity of the vehicle.</p>
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<p>Heading angle of the vehicle.</p>
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43 pages, 7755 KiB  
Review
Influence of Preparation Characteristics on Stability, Properties, and Performance of Mono- and Hybrid Nanofluids: Current and Future Perspective
by Humaira Yasmin, Solomon O. Giwa, Saima Noor and Hikmet Ş. Aybar
Machines 2023, 11(1), 112; https://doi.org/10.3390/machines11010112 - 13 Jan 2023
Cited by 13 | Viewed by 2987
Abstract
Nanofluids (NFs) synthesized via the suspension of diverse nanoparticles into conventional thermal fluids are known to exhibit better thermal, optical, tribological, and convective properties, photothermal conversion, and heat transfer performance in comparison with traditional thermal fluids. Stability is pivotal to NF preparation, properties, [...] Read more.
Nanofluids (NFs) synthesized via the suspension of diverse nanoparticles into conventional thermal fluids are known to exhibit better thermal, optical, tribological, and convective properties, photothermal conversion, and heat transfer performance in comparison with traditional thermal fluids. Stability is pivotal to NF preparation, properties, performance, and application. NF preparation is not as easy as it appears, but complex in that obtaining a stable NF comes with the harnessing of different preparation parameters. These parameters include stirring duration and speed, volume, density, base fluid type, weight/volume concentration, density, nano-size, type of mono or hybrid nanoparticles used, type and quantity of surfactant used, and sonication time, temperature, mode, frequency, and amplitude. The effect of these preparation parameters on the stability of mono and hybrid NFs consequently affects the thermal, optical, rheological, and convective properties, and photothermal conversion and heat transfer performances of NFs in various applications. A comprehensive overview of the influence of these preparation characteristics on the thermal, optical, rheological, and properties, photothermal conversion, and heat transfer performance is presented in this paper. This is imperative due to the extensive study on mono and hybrid NFs and their acceptance as advanced thermal fluids along with the critical importance of stability to their properties and performance. The various preparation, characterization, and stability methods deployed in NF studies have been compiled and discussed herein. In addition, the effect of the various preparation characteristics on the properties (thermal, optical, rheological, and convective), photothermal conversion, and heat transfer performances of mono and hybrid NFs have been reviewed. The need to achieve optimum stability of NFs by optimizing the preparation characteristics is observed to be critical to the obtained results for the properties, photothermal conversion, and heat transfer performance studies. As noticed that the preparation characteristics data are not detailed in most of the published works and thus making it mostly impossible to reproduce NF experimental studies, stability, and results; future research is expected to address this gap. In addition, the research community should be concerned about the aging and reusability of NFs (mono and hybrid) in the nearest future. Full article
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<p>Overview of present study.</p>
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<p>Mono and hybrid NF formulation strategies.</p>
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<p>Ultrasonication of HNF.</p>
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<p>Thermal conductivity of MWCNT/water NF against ultrasonication time at the temperature of 35 °C and different concentrations. Adapted from [<a href="#B148-machines-11-00112" class="html-bibr">148</a>].</p>
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<p>Viscosity of MWCNT/water NF against ultrasonication time at the temperature of 40 °C and concentration of 0.5%. Adapted from [<a href="#B149-machines-11-00112" class="html-bibr">149</a>].</p>
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<p>Influence of ultrasonication duration on density of 0.5 vol% Al<sub>2</sub>O<sub>3</sub>-water NF at different temperatures. Adapted from [<a href="#B150-machines-11-00112" class="html-bibr">150</a>].</p>
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<p>Images of Wet-TEM of 1 wt% MWCNT + 0.25 wt% GA NF sonicated for: (<b>a</b>) 20 min at 0.5 μm scale, (<b>b</b>) 40 min at 0.5 μm scale, (<b>c</b>) 60 min at 0.5 μm scale, (<b>d</b>) 80 min at 0.5 μm scale, (<b>e</b>) 40 min at 200 nm scale, and (<b>f</b>) 80 min at 200 nm scale. Adapted from [<a href="#B155-machines-11-00112" class="html-bibr">155</a>].</p>
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<p>Viscosity against shear rate of Al<sub>2</sub>O<sub>3</sub> NF at different sonication time. Adapted from [<a href="#B165-machines-11-00112" class="html-bibr">165</a>].</p>
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<p>Influence of sonication time on viscosity of Al<sub>2</sub>O<sub>3</sub>–GL NF with volume fractions of (<b>a</b>) 2% and (<b>b</b>) 3%. Adapted from [<a href="#B98-machines-11-00112" class="html-bibr">98</a>].</p>
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<p>Influence of sonication time on the electrical conductivity and pH of MgO-EG NF at 20 °C: (<b>a</b>) electrical conductivity and (<b>b</b>) pH. Adapted from [<a href="#B120-machines-11-00112" class="html-bibr">120</a>].</p>
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<p>Effect of ultrasonication duration on the yield stress of the Al<sub>2</sub>O<sub>3</sub>-water NF. Adapted from [<a href="#B168-machines-11-00112" class="html-bibr">168</a>].</p>
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<p>Stability of MWCNT-water NFs formulated at different ultrasonication durations (30 days). Adapted from [<a href="#B136-machines-11-00112" class="html-bibr">136</a>].</p>
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<p>Effect of ultrasonic duration on zeta potentials of TiO<sub>2</sub>—H<sub>2</sub>O NF. Adapted from [<a href="#B124-machines-11-00112" class="html-bibr">124</a>].</p>
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<p>Effect of ultrasonication time on zeta potential of 0.5 vol% MWCNT/water NF at different storage time. Adapted from [<a href="#B148-machines-11-00112" class="html-bibr">148</a>].</p>
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<p>Comparison of the absorption spectra for the SWCNT NF dispersed using 3-mm and 6-mm sonication tips. Adapted from [<a href="#B175-machines-11-00112" class="html-bibr">175</a>].</p>
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<p>Effects of sonication amplitude (% in the parentheses) and time on ST<sub>nf</sub> of ZnO/DW NFs. Adapted from [<a href="#B176-machines-11-00112" class="html-bibr">176</a>].</p>
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<p>Influence of ultrasonication duration on pH value of TiO<sub>2</sub>–H<sub>2</sub>O NF with an isoelectric point of TiO<sub>2</sub>. Adapted from [<a href="#B124-machines-11-00112" class="html-bibr">124</a>].</p>
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<p>Effect of sonication time (pulse ratio 0.1/2.0 (s/s)) on average cluster size of alumina NF at different vibration amplitudes. Adapted from [<a href="#B179-machines-11-00112" class="html-bibr">179</a>].</p>
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<p>Axial variation of heat transfer coefficient at Re = 1200 ± 100 under varying sonication time using MNF. Adapted from [<a href="#B155-machines-11-00112" class="html-bibr">155</a>].</p>
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<p>Effect of dispersion fraction on electrical conductivity and pH of 0.5 vol% MgO-ZnO/DIW NF. Adapted from [<a href="#B77-machines-11-00112" class="html-bibr">77</a>].</p>
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<p>Effect of sonication time on electrical conductivity and pH of 0.5 vol% MgO-ZnO/DIW NF. Adapted from [<a href="#B77-machines-11-00112" class="html-bibr">77</a>].</p>
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<p>Nusselt number enhancement ratio against Reynolds number for hybrid NF at different concentrations of surfactant (SDS or PVP). Adapted from [<a href="#B65-machines-11-00112" class="html-bibr">65</a>].</p>
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<p>Thermal efficiency against Reynolds number for helical coil with hybrid NF containing SDS or PVP Adapted from [<a href="#B65-machines-11-00112" class="html-bibr">65</a>].</p>
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<p>Influence of preparation characteristics on properties (optical, thermal, and rheological) and performance of mono and hybrid NFs.</p>
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28 pages, 2619 KiB  
Review
The Expanding Role of Artificial Intelligence in Collaborative Robots for Industrial Applications: A Systematic Review of Recent Works
by Alberto Borboni, Karna Vishnu Vardhana Reddy, Irraivan Elamvazuthi, Maged S. AL-Quraishi, Elango Natarajan and Syed Saad Azhar Ali
Machines 2023, 11(1), 111; https://doi.org/10.3390/machines11010111 - 13 Jan 2023
Cited by 46 | Viewed by 25119
Abstract
A collaborative robot, or cobot, enables users to work closely with it through direct communication without the use of traditional barricades. Cobots eliminate the gap that has historically existed between industrial robots and humans while they work within fences. Cobots can be used [...] Read more.
A collaborative robot, or cobot, enables users to work closely with it through direct communication without the use of traditional barricades. Cobots eliminate the gap that has historically existed between industrial robots and humans while they work within fences. Cobots can be used for a variety of tasks, from communication robots in public areas and logistic or supply chain robots that move materials inside a building, to articulated or industrial robots that assist in automating tasks which are not ergonomically sound, such as assisting individuals in carrying large parts, or assembly lines. Human faith in collaboration has increased through human–robot collaboration applications built with dependability and safety in mind, which also enhances employee performance and working circumstances. Artificial intelligence and cobots are becoming more accessible due to advanced technology and new processor generations. Cobots are now being changed from science fiction to science through machine learning. They can quickly respond to change, decrease expenses, and enhance user experience. In order to identify the existing and potential expanding role of artificial intelligence in cobots for industrial applications, this paper provides a systematic literature review of the latest research publications between 2018 and 2022. It concludes by discussing various difficulties in current industrial collaborative robots and provides direction for future research. Full article
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<p>Global collaborative robot market in 2021.</p>
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<p>Relationship between AI, machine learning, and deep learning.</p>
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<p>The PRISMA model diagram for the systematic review.</p>
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<p>An example application of cobots in the manufacturing industry [<a href="#B21-machines-11-00111" class="html-bibr">21</a>].</p>
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<p>Robot usage in collaborative research works between 2018 and 2022.</p>
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<p>Tasks performed by the robot in collaborative research works.</p>
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17 pages, 8119 KiB  
Article
Film Cooling Performance of a Cylindrical Hole with an Upstream Crescent-Shaped Block in Linear Cascade
by Chao Zhang, Junhuai Dong, Zhan Wang, Pengfei Zhang, Zhiting Tong and Yue Zhang
Machines 2023, 11(1), 110; https://doi.org/10.3390/machines11010110 - 13 Jan 2023
Viewed by 1539
Abstract
Recent works have already demonstrated that placing a crescent-shaped block upstream of a cylindrical hole could enhance the cooling performance of flat-plate films. The flow and cooling performance of the crescent-shaped block applied over the pressure and suction sides of the blade is [...] Read more.
Recent works have already demonstrated that placing a crescent-shaped block upstream of a cylindrical hole could enhance the cooling performance of flat-plate films. The flow and cooling performance of the crescent-shaped block applied over the pressure and suction sides of the blade is investigated in this article. The Reynolds-averaged Navier-Stokes equations are solved with the Shear Stress Transport model for turbulence closure. Two optimized blocks are obtained from the flat-plate film cooling in our previous work, and two positions on the pressure and suction sides are tested. The blowing ratio varies from 0.5 to 2.0. The results show that when the block is applied on the blade surface, it yields a different cooling performance compared with the flat plate due to different geometry curvature and pressure gradient. The cooling performance on the suction side is slightly higher than on that on the pressure side, while the aerodynamic loss on the suction side is much higher. For the different blocks, the qualitative change of cooling performance vs. blowing ratios held on turbine blades is quite close to that of flat plates. The optimized smaller block in the flat plate provides better cooling performance at lower blowing ratios, while the larger block is superior when the blowing ratios are higher. Full article
(This article belongs to the Special Issue Heat Transfer and Energy Harvesting in Fluid System)
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<p>The sketch of the linear cascade.</p>
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<p>Velocity profile around the blade surfaces.</p>
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<p>The crescent-shaped block. (<b>a</b>) Layout; (<b>b</b>) Top view.</p>
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<p>Computational mesh.</p>
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<p>Variation of <span class="html-italic">Y</span><sup>+</sup> values over the pressure and suction surfaces.</p>
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<p>Comparisons with different levels of computational grid (<b>a</b>) pressure; (<b>b</b>) laterally averaged cooling effectiveness.</p>
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<p>Validation of the turbulence model [<a href="#B30-machines-11-00110" class="html-bibr">30</a>].</p>
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<p>Contours of cooling effectiveness at <span class="html-italic">M</span> = 0.5–2.0 at the pressure side. (<b>a</b>) Block 1, <span class="html-italic">X</span> = 12.5 mm; (<b>b</b>) Block 1, <span class="html-italic">X</span> = 35 mm; (<b>c</b>) Block 2, <span class="html-italic">X</span> = 12.5 mm; (<b>d</b>) Block 2, <span class="html-italic">X</span> = 35 mm.</p>
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<p>Dimensionless temperature distribution and streamlines for Block 1 at <span class="html-italic">X</span> = 35 mm. (<b>a</b>) <span class="html-italic">M</span> = 0.5; (<b>b</b>) <span class="html-italic">M</span> = 1.5.</p>
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<p>Dimensionless temperature distribution along plane <span class="html-italic">Z</span>/<span class="html-italic">D</span> = 0 at <span class="html-italic">M</span> = 1.0. (<b>a</b>) PS Block 1, <span class="html-italic">X</span> = 12.5 mm; (<b>b</b>) PS Block 1, <span class="html-italic">X</span> = 35 mm; (<b>c</b>) PS Block 2, <span class="html-italic">X</span> = 12.5 mm; (<b>d</b>) PS Block 2, <span class="html-italic">X</span> = 35 mm.</p>
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<p>Laterally averaged cooling effectiveness on the pressure side [<a href="#B22-machines-11-00110" class="html-bibr">22</a>]. (<b>a</b>) PS Block 1, <span class="html-italic">X</span> = 12.5 mm; (<b>b</b>) PS Block 1, <span class="html-italic">X</span> = 35 mm; (<b>c</b>) PS Block 2, <span class="html-italic">X</span> = 12.5 mm; (<b>d</b>) PS Block 2, <span class="html-italic">X</span> = 35 mm.</p>
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<p>Area averaged cooling effectiveness relative to blowing ratios on the pressure side.</p>
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<p>Local Cooling effectiveness distribution on the suction side. (<b>a</b>) SS Block 1, <span class="html-italic">X</span> = 8 mm; (<b>b</b>) SS Block 1, <span class="html-italic">X</span> = 17.5 mm; (<b>c</b>) SS Block 2, <span class="html-italic">X</span> = 8 mm; (<b>d</b>) SS Block 2, <span class="html-italic">X</span> = 17.5 mm.</p>
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<p>Dimensionless temperature and streamlines for Block 2 at <span class="html-italic">X</span> = 8 mm. (<b>a</b>) <span class="html-italic">M</span> = 0.5; (<b>b</b>) <span class="html-italic">M</span> = 1.5.</p>
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<p>Dimensionless temperature distribution along the plane <span class="html-italic">Z</span>/<span class="html-italic">D</span> = 0 at <span class="html-italic">M</span> = 2.0. (<b>a</b>) SS Block 1, <span class="html-italic">X</span> = 8 mm; (<b>b</b>) SS Block 1, <span class="html-italic">X</span> = 17.5 mm; (<b>c</b>) SS Block 2, <span class="html-italic">X</span> = 8 mm; (<b>d</b>) SS Block 2, <span class="html-italic">X</span> = 17.5 mm.</p>
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<p>Laterally averaged cooling effectiveness on suction sides [<a href="#B22-machines-11-00110" class="html-bibr">22</a>]. (<b>a</b>) Block 1, <span class="html-italic">X</span> = 8 mm; (<b>b</b>) Block 1, <span class="html-italic">X</span> = 17.5 mm; (<b>c</b>) Block 2, <span class="html-italic">X</span> = 8 mm; (<b>d</b>) Block 2, <span class="html-italic">X</span> = 17.5 mm.</p>
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<p>Area averaged cooling effectiveness v.s. blowing ratios on the suction side.</p>
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<p>Dimensionless temperature profile and surface streamlines along the plane <span class="html-italic">Z</span>/<span class="html-italic">D</span> = 0 at <span class="html-italic">M</span> = 0.5 (<b>a</b>) SS Block 1, <span class="html-italic">X</span> = 8 mm; (<b>b</b>) SS Block 2, <span class="html-italic">X</span> = 8 mm.</p>
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<p>Total pressure loss coefficient relative to blowing ratios. (<b>a</b>) On the pressure side; (<b>b</b>) On the suction side.</p>
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29 pages, 11741 KiB  
Article
Fault Location in Distribution Network by Solving the Optimization Problem Based on Power System Status Estimation Using the PMU
by Masoud Dashtdar, Arif Hussain, Hassan Z. Al Garni, Abdullahi Abubakar Mas’ud, Waseem Haider, Kareem M. AboRas and Hossam Kotb
Machines 2023, 11(1), 109; https://doi.org/10.3390/machines11010109 - 13 Jan 2023
Cited by 21 | Viewed by 5057
Abstract
Fault location is one of the main challenges in the distribution network due to its expanse and complexity. Today, with the advent of phasor measurement units (PMU), various techniques for fault location using these devices have been proposed. In this research, distribution network [...] Read more.
Fault location is one of the main challenges in the distribution network due to its expanse and complexity. Today, with the advent of phasor measurement units (PMU), various techniques for fault location using these devices have been proposed. In this research, distribution network fault location is defined as an optimization problem, and the network fault location is determined by solving it. This is done by combining PMU data before and after the fault with the power system status estimation (PSSE) problem. Two new objective functions are designed to identify the faulty section and fault location based on calculating the voltage difference between the two ends of the grid lines. In the proposed algorithm, the purpose of combining the PMU in the PSSE problem is to estimate the voltage and current quantities at the branch point and the total network nodes after the fault occurs. Branch point quantities are calculated using the PMU and the governing equations of the π line model for each network section, and the faulty section is identified based on a comparison of the resulting values. The advantages of the proposed algorithm include simplicity, step-by-step implementation, efficiency in conditions of different branch specifications, application for various types of faults including short-circuit and series, and its optimal accuracy compared to other methods. Finally, the proposed algorithm has been implemented on the IEEE 123-node distribution feeder and its performance has been evaluated for changes in various factors including fault resistance, type of fault, angle of occurrence of a fault, uncertainty in loading states, and PMU measurement error. The results show the appropriate accuracy of the proposed algorithm showing that it was able to determine the location of the fault with a maximum error of 1.21% at a maximum time of 23.87 s. Full article
(This article belongs to the Section Electromechanical Energy Conversion Systems)
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<p>Power network infrastructure.</p>
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<p>PMU connected to a bus.</p>
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<p>Model π two inputs of a branch of the power grid.</p>
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<p>Network status. (<b>a</b>) Information obtained from the PSSE before the fault, (<b>b</b>) The current direction of each network line after the fault.</p>
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<p>Changes in the direction of line current in exchange for the location of various faults in the main branch of the network.</p>
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<p>Voltage and current status of the node connected to the PMU. (<b>a</b>) Before the fault, (<b>b</b>) After the fault.</p>
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<p>Information of a sample line.</p>
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<p>Sample network of 3 lines.</p>
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<p>General space of the fault location problem.</p>
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<p>Fault between two buses <span class="html-italic">i</span>, <span class="html-italic">j</span>.</p>
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<p>Types of short-circuit and series faults, (<b>a</b>) single-phase fault to ground, (<b>b</b>) two-phase fault, (<b>c</b>) three-phase fault, (<b>d</b>) two-phase fault to ground, (<b>e</b>) One open conductor, (<b>f</b>) Two open conductors.</p>
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<p>Equivalent circuit of positive, negative, and zero sequences of single-phase fault to ground.</p>
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<p>Equivalent circuit of symmetric components for a fault (<b>a</b>) One open conductor, (<b>b</b>) Two open conductors.</p>
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<p>Flowchart of the steps of the proposed method.</p>
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<p>IEEE 123 Node Test Feeder distribution network with PMU.</p>
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<p>Voltage and current of network nodes under normal conditions.</p>
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<p>Results of the performance of the genetic algorithm to identify the fault section.</p>
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<p>Dimensions of the fault location problem.</p>
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<p>Mean EE value under the influence of various factors.</p>
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18 pages, 4130 KiB  
Article
Path Planning of Unmanned Aerial Vehicle in Complex Environments Based on State-Detection Twin Delayed Deep Deterministic Policy Gradient
by Danyang Zhang, Zhaolong Xuan, Yang Zhang, Jiangyi Yao, Xi Li and Xiongwei Li
Machines 2023, 11(1), 108; https://doi.org/10.3390/machines11010108 - 13 Jan 2023
Cited by 8 | Viewed by 2933
Abstract
This paper investigates the path planning problem of an unmanned aerial vehicle (UAV) for completing a raid mission through ultra-low altitude flight in complex environments. The UAV needs to avoid radar detection areas, low-altitude static obstacles, and low-altitude dynamic obstacles during the flight [...] Read more.
This paper investigates the path planning problem of an unmanned aerial vehicle (UAV) for completing a raid mission through ultra-low altitude flight in complex environments. The UAV needs to avoid radar detection areas, low-altitude static obstacles, and low-altitude dynamic obstacles during the flight process. Due to the uncertainty of low-altitude dynamic obstacle movement, this can slow down the convergence of existing algorithm models and also reduce the mission success rate of UAVs. In order to solve this problem, this paper designs a state detection method to encode the environmental state of the UAV’s direction of travel and compress the environmental state space. In considering the continuity of the state space and action space, the SD-TD3 algorithm is proposed in combination with the double-delayed deep deterministic policy gradient algorithm (TD3), which can accelerate the training convergence speed and improve the obstacle avoidance capability of the algorithm model. Further, to address the sparse reward problem of traditional reinforcement learning, a heuristic dynamic reward function is designed to give real-time rewards and guide the UAV to complete the task. The simulation results show that the training results of the SD-TD3 algorithm converge faster than the TD3 algorithm, and the actual results of the converged model are better. Full article
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<p>Schematic of battlefield environment.</p>
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<p>Probability model of radar detection.</p>
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<p>Schematic diagram of status detection code.</p>
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<p>The combination of the state probing method and the TD3 model.</p>
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<p>Training result of TD3 algorithm model in environment 1.</p>
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<p>Training result of TD3 algorithm model in environment 2.</p>
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<p>Training result of SD-TD3 (6) algorithm model in environment 1.</p>
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<p>Training results of SD-TD3 (6) algorithm model in Environment 2.</p>
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<p>Training result of SD-TD3 (12) algorithm model in environment 1.</p>
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<p>Training result of SD-TD3 (12) algorithm model in environment 2.</p>
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<p>The best training results of the three algorithmic models. (<b>a</b>) Best training results of the model in environment 1; (<b>b</b>) Best training results of the model in environment 2.</p>
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<p>Success rate of all algorithmic models in both environments.</p>
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16 pages, 1331 KiB  
Article
Enhanced Reaching-Law-Based Discrete-Time Terminal Sliding Mode Current Control of a Six-Phase Induction Motor
by Yassine Kali, Jorge Rodas, Jesus Doval-Gandoy, Magno Ayala and Osvaldo Gonzalez
Machines 2023, 11(1), 107; https://doi.org/10.3390/machines11010107 - 13 Jan 2023
Cited by 7 | Viewed by 4324
Abstract
This paper develops an inner stator current controller based on an enhanced reaching-law-based discrete-time terminal sliding mode. The problem of tracking stator currents with high accuracy while ensuring the robustness of a six-phase induction motor in the presence of uncertain electrical parameters and [...] Read more.
This paper develops an inner stator current controller based on an enhanced reaching-law-based discrete-time terminal sliding mode. The problem of tracking stator currents with high accuracy while ensuring the robustness of a six-phase induction motor in the presence of uncertain electrical parameters and unmeasurable states is tackled. The unknown dynamics are approximated by using a time delay estimation method. Then, an enhanced power-reaching law is used to make each stage of the convergence faster. A stability analysis and the system controller’s finite-time convergence are demonstrated in detail. Practical work was conducted on an asymmetrical six-phase induction machine to illustrate the developed discrete approach’s robustness and effectiveness. Full article
(This article belongs to the Special Issue Innovative Applications of Multiphase Machines)
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<p>Schematic of the 2L-VSCs and the six-phase IM in an asymmetrical configuration.</p>
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<p>Proposed control scheme.</p>
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<p>Experimental platform of the six-phase IM control system.</p>
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<p>Stator currents for the proposed enhanced PRL-based DTSMC in the (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>−</mo> <mi>β</mi> </mrow> </semantics></math>) and (<math display="inline"><semantics> <mrow> <mi>x</mi> <mo>−</mo> <mi>y</mi> </mrow> </semantics></math>) planes for different speed conditions <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math>. Stator currents for the proposed PRL-based DTSMC in the (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>−</mo> <mi>β</mi> </mrow> </semantics></math>) and (<math display="inline"><semantics> <mrow> <mi>x</mi> <mo>−</mo> <mi>y</mi> </mrow> </semantics></math>) planes for a speed <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math> of (<b>left</b>) 1000 or (<b>right</b>) 1500 rpm.</p>
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<p>Stator currents in the (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>−</mo> <mi>β</mi> </mrow> </semantics></math>) and (<math display="inline"><semantics> <mrow> <mi>x</mi> <mo>−</mo> <mi>y</mi> </mrow> </semantics></math>) planes for different speed conditions <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math>. Stator currents for a basic DTSMC in the (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>−</mo> <mi>β</mi> </mrow> </semantics></math>) and (<math display="inline"><semantics> <mrow> <mi>x</mi> <mo>−</mo> <mi>y</mi> </mrow> </semantics></math>) planes for a speed <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math> of (<b>left</b>) 1000 or (<b>right</b>) 1500 rpm.</p>
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<p>Transient condition of the <span class="html-italic">q</span>-plane current of a speed reversal action from 1000 to <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>500</mn> </mrow> </semantics></math> rpm from <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math> at a sampling frequency of 16 kHz. Transient condition of the <span class="html-italic">q</span>-plane current of a speed reversal action from 1000 to <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>500</mn> </mrow> </semantics></math> rpm from <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math> at a sampling frequency of 16 kHz for the proposed controller (<b>left</b>) and a basic DTSMC version (<b>right</b>).</p>
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<p>Transient behavior of stator currents of a speed reversal action from <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math>. The first results are from −500 to 1000 rpm, and then from 1000 to −500 rpm.</p>
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<p>Transient behavior of a speed reversal action from <math display="inline"><semantics> <msub> <mi>ω</mi> <mi>m</mi> </msub> </semantics></math>. The first results are from −500 to 1000 rpm, and then from 1000 to −500 rpm, with different values of <math display="inline"><semantics> <msub> <mi>τ</mi> <mi>r</mi> </msub> </semantics></math>.</p>
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18 pages, 7676 KiB  
Article
Frequency Response Analysis for Three-Phase Star and Delta Induction Motors: Pattern Recognition and Fault Analysis Using Statistical Indicators
by Salem Mgammal Al-Ameri, Zulkurnain Abdul-Malek, Ali Ahmed Salem, Zulkarnain Ahmad Noorden, Ahmed Allawy Alawady, Mohd Fairouz Mohd Yousof, Mohamed Ibrahim Mosaad, Ahmed Abu-Siada and Hammam Abdurabu Thabit
Machines 2023, 11(1), 106; https://doi.org/10.3390/machines11010106 - 13 Jan 2023
Cited by 12 | Viewed by 2626
Abstract
This paper presents a new investigation to detect various faults within the three-phase star and delta induction motors (IMs) using a frequency response analysis (FRA). In this regard, experimental measurements using FRA are performed on three IMs of ratings 1 HP, 3 HP [...] Read more.
This paper presents a new investigation to detect various faults within the three-phase star and delta induction motors (IMs) using a frequency response analysis (FRA). In this regard, experimental measurements using FRA are performed on three IMs of ratings 1 HP, 3 HP and 5.5 HP in normal conditions, short-circuit fault (SC) and open-circuit fault (OC) conditions. The SC and OC faults are applied artificially between the turns (Turn-to-Turn), between the coils (Coil-to-Coil) and between the phases (Phase-to-Phase). The obtained measurements show that the star and delta IMs result in dissimilar FRA signatures for the normal and faulty windings. Various statistical indicators are used to quantify the deviations between the normal and faulty FRA signatures. The calculation is performed in three frequency ranges: low, middle and high ones, as the winding parameters including resistive, inductive and capacitive components dominate the frequency characteristics at different frequency ranges. Consequently, it is proposed that the boundaries for the used indicators facilitate fault identification and quantification. Full article
(This article belongs to the Special Issue Fault Diagnosis and Health Management of Power Machinery)
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<p>Measurement setup in the laboratory. (<b>a</b>) SC and OC faults development. (<b>b</b>) Measurement connections.</p>
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<p>The measurement setup and results comparison process methodology.</p>
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<p>FRA measured responses for star vs. delta of 1 HP IM at (<b>a</b>) Normal vs. Turn-to-Turn, (<b>b</b>) Normal vs. Coil-to-Coil, (<b>c</b>) Normal vs. Phase-to-Phase SC fault and (<b>d</b>) Normal vs. open circuits.</p>
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<p>FRA measured responses for star vs. delta of 1 HP IM at (<b>a</b>) Normal vs. Turn-to-Turn, (<b>b</b>) Normal vs. Coil-to-Coil, (<b>c</b>) Normal vs. Phase-to-Phase SC fault and (<b>d</b>) Normal vs. open circuits.</p>
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<p>FRA measured responses for star vs. delta 3 HP IM at (<b>a</b>) Normal vs. Turn-to-Turn, (<b>b</b>) Normal vs. Coil-to-Coil, (<b>c</b>) Normal vs. Phase-to-Phase SC fault and (<b>d</b>) Normal vs. open circuit.</p>
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<p>FRA measured responses for star vs. delta 5.5-IM at (<b>a</b>) Normal vs. Turn-to-Turn, (<b>b</b>) Normal vs. Coil-to-Coil, (<b>c</b>) Normal vs. Phase-to-Phase SC fault and (<b>d</b>) Normal vs. open circuit.</p>
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<p>FRA of an equivalent IM RLC electrical circuit.</p>
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<p>RLC parameters and their contribution to the measured FRA. (<b>a</b>) LF range (from 10 Hz to 1 kHz), (<b>b</b>) MF range (from 1 kHz to 60 kHz), (<b>c</b>) HF range (from 60 kHz to 1 MHz).</p>
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<p>The proposed FRA sub-bands for IM FRA studies.</p>
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<p>The CC calculated values between the normal and other faults.</p>
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<p>ASLE calculated values between normal and other faults.</p>
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<p>SD calculated values between normal and other faults.</p>
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<p>MSE calculated values between normal and other faults.</p>
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<p>Mechanism of the OC fault and effect on FRA patterns. (<b>a</b>) Measurement connection. (<b>b</b>) FRA patterns.</p>
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35 pages, 4044 KiB  
Article
Classification of Wall Following Robot Movements Using Genetic Programming Symbolic Classifier
by Nikola Anđelić, Sandi Baressi Šegota, Matko Glučina and Ivan Lorencin
Machines 2023, 11(1), 105; https://doi.org/10.3390/machines11010105 - 12 Jan 2023
Cited by 4 | Viewed by 2037
Abstract
The navigation of mobile robots throughout the surrounding environment without collisions is one of the mandatory behaviors in the field of mobile robotics. The movement of the robot through its surrounding environment is achieved using sensors and a control system. The application of [...] Read more.
The navigation of mobile robots throughout the surrounding environment without collisions is one of the mandatory behaviors in the field of mobile robotics. The movement of the robot through its surrounding environment is achieved using sensors and a control system. The application of artificial intelligence could potentially predict the possible movement of a mobile robot if a robot encounters potential obstacles. The data used in this paper is obtained from a wall-following robot that navigates through the room following the wall in a clockwise direction with the use of 24 ultrasound sensors. The idea of this paper is to apply genetic programming symbolic classifier (GPSC) with random hyperparameter search and 5-fold cross-validation to investigate if these methods could classify the movement in the correct category (move forward, slight right turn, sharp right turn, and slight left turn) with high accuracy. Since the original dataset is imbalanced, oversampling methods (ADASYN, SMOTE, and BorderlineSMOTE) were applied to achieve the balance between class samples. These over-sampled dataset variations were used to train the GPSC algorithm with a random hyperparameter search and 5-fold cross-validation. The mean and standard deviation of accuracy (ACC), the area under the receiver operating characteristic (AUC), precision, recall, and F1score values were used to measure the classification performance of the obtained symbolic expressions. The investigation showed that the best symbolic expressions were obtained on a dataset balanced with the BorderlineSMOTE method with ACC¯±SD(ACC), AUC¯macro±SD(AUC), Precision¯macro±SD(Precision), Recall¯macro±SD(Recall), and F1score¯macro±SD(F1score) equal to 0.975×1.81×103, 0.997±6.37×104, 0.975±1.82×103, 0.976±1.59×103, and 0.9785±1.74×103, respectively. The final test was to use the set of best symbolic expressions and apply them to the original dataset. In this case the ACC¯±SD(ACC), AUC¯±SD(AUC), Precision¯±SD(Precision), Recall¯±SD(Recall), and F1score¯±SD(F1Score) are equal to 0.956±0.05, 0.9536±0.057, 0.9507±0.0275, 0.9809±0.01, 0.9698±0.00725, respectively. The results of the investigation showed that this simple, non-linearly separable classification task could be solved using the GPSC algorithm with high accuracy. Full article
(This article belongs to the Special Issue Modeling, Sensor Fusion and Control Techniques in Applied Robotics)
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<p>The flowchart of the research methodology used in this paper.</p>
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<p>The Pearson’s correlation analysis of the dataset variables.</p>
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<p>Correlation between the input variables and the class variable.</p>
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<p>The number of samples per each class.</p>
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<p>The <math display="inline"><semantics> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> <mo>(</mo> <msub> <mi>X</mi> <mn>1</mn> </msub> <mo>+</mo> <msub> <mi>X</mi> <mn>3</mn> </msub> <mo>,</mo> <msub> <mi>X</mi> <mn>4</mn> </msub> <mo>−</mo> <msub> <mi>X</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math>.</p>
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<p>The GPSC algorithm with random hyperparameter search with 5-fold cross-validation.</p>
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<p>The mean and standard deviation (error bars) values of <math display="inline"><semantics> <mrow> <mi>A</mi> <mi>C</mi> <mi>C</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>A</mi> <mi>U</mi> <mi>C</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>p</mi> <mi>r</mi> <mi>e</mi> <mi>c</mi> <mi>i</mi> <mi>s</mi> <mi>i</mi> <mi>o</mi> <mi>n</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>r</mi> <mi>e</mi> <mi>c</mi> <mi>a</mi> <mi>l</mi> <mi>l</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>F</mi> <mn>1</mn> <mo>−</mo> <mi>s</mi> <mi>c</mi> <mi>o</mi> <mi>r</mi> <mi>e</mi> </mrow> </semantics></math> achieved for different dataset variations.</p>
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<p>The flowchart of the model application on a theoretical mobile robot that uses the developed system.</p>
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11 pages, 2456 KiB  
Article
A Simplified Method for Inverse Kinematics of a Flexible Panel Continuum Robot for Real-Time Shape Morphing
by Wenbin Wang, Xiangping Yu, Yinjun Zhao, Long Li, Yuwen Li, Yingzhong Tian and Fengfeng Xi
Machines 2023, 11(1), 104; https://doi.org/10.3390/machines11010104 - 12 Jan 2023
Cited by 2 | Viewed by 1699
Abstract
Continuum robots are good candidates for shape morphing. However, due to the coupled problem between kinematics and statics, the inverse kinematics of continuum robots is highly nonlinear, posing a challenging problem for real-time applications. This paper presents a simplified approach to solving the [...] Read more.
Continuum robots are good candidates for shape morphing. However, due to the coupled problem between kinematics and statics, the inverse kinematics of continuum robots is highly nonlinear, posing a challenging problem for real-time applications. This paper presents a simplified approach to solving the inverse kinematics of a flexible panel continuum robot efficiently. Through an experiment, two approximate relationships are discovered. First, the arc length of the middle backbone can be estimated from the arc lengths of the two panels; second, the length difference between the two panels can be related to the tip angle of the end-effector. Based on these two discovered relationships, a simplified inverse kinematics method is proposed based on a constant curvature model. This method has been validated by the experimental data with high accuracy of less than 2% error, thereby demonstrating the effectiveness of the proposed method for real-time applications. Full article
(This article belongs to the Section Robotics, Mechatronics and Intelligent Machines)
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<p>Structure of the flexible panel continuum robot.</p>
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<p>Analysis model without gravity (<span class="html-italic">Fx</span> is the pushing force constrained along the <span class="html-italic">X</span><sub>1</sub> axis and imposed at point <span class="html-italic">C</span>, <math display="inline"><semantics> <mrow> <msub> <mrow> <msub> <mrow> <mi>M</mi> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mi>L</mi> </mrow> </msub> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <msub> <mrow> <mi>M</mi> </mrow> <mrow> <mn>2</mn> <mo>,</mo> <mi>L</mi> </mrow> </msub> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math> are moments generated by the bending of top panel <span class="html-italic">A</span> and <span class="html-italic">M<sub>C</sub></span> and <span class="html-italic">M<sub>D</sub></span> are the reaction moments).</p>
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<p>A simplified model of the flexible panel continuum mechanism.</p>
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<p>Planar parallel continuum robot and static analysis of the moving platform: (<b>a</b>) A virtual backbone that runs through the middle axis of the two panels; (<b>b</b>) A pushing force at point A and a pulling force at point B.</p>
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<p>Tip angle vs. change in length.</p>
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<p>Error analysis of the method.</p>
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15 pages, 15285 KiB  
Article
4D Printing of Hydrogels Controlled by Hinge Structure and Spatially Gradient Swelling for Soft Robots
by Masanari Kameoka, Yosuke Watanabe, MD Nahin Islam Shiblee, Masaru Kawakami, Jun Ogawa, Ajit Khosla, Hidemitsu Furukawa, Shengyang Zhang, Shinichi Hirai and Zhongkui Wang
Machines 2023, 11(1), 103; https://doi.org/10.3390/machines11010103 - 12 Jan 2023
Cited by 10 | Viewed by 3015
Abstract
In 4D printing, structures with gradients in physical properties are 3D printed in order to dramatically increase deformation. For example, printing bilayer structures with passive and active layers has been proposed, however, these methods have the disadvantages that the material of each layer [...] Read more.
In 4D printing, structures with gradients in physical properties are 3D printed in order to dramatically increase deformation. For example, printing bilayer structures with passive and active layers has been proposed, however, these methods have the disadvantages that the material of each layer is mixed, and the modeling process is complicated. Herein, we present a method of creating gradient gels with different degrees of polymerization on the UV-exposed side and the other side using a single material by simply increasing the amount of initiator. This gel is the first example in which the differential swelling ratio between two sides causes the gradient to curl inward toward the UV-exposed side. The mechanical properties (swelling ratio and Young’s modulus) were measured at different material concentrations and structures, and the effects of each on deformation were analyzed and simulated. The results show that adding an initiator concentration of 0.2 (mol/L) or more causes deformation, that increasing the crosslinker concentration by a factor of three or more increases deformation, and that adding a hinge structure limits the gradient gel to deformation up to 90°. Thus, it was found that the maximum deformation can be predicted to some extent by simulation. In the future, we will be able to create complex structures while utilizing simulation. Full article
(This article belongs to the Special Issue Advance in Additive Manufacturing)
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<p>The process of 3D printing of the ICN gels with the hinge structure. (<b>a</b>) The side cross sectional view of the silicone mold placed on the platform of GelPiPer. Pre-gel solution is sandwiched with the picture-flame shape of 2 mm or 5 mm thickness silicone spacer (outer size: 8 cm × 8 cm, inner size: 7 cm × 7 cm) in the couple of 2 mm thickness glass plates, whose surfaces are covered with 0.5 mm thickness PET films. (<b>b</b>) The molding process of the 3D printed bilayer hydrogels with hinge structure. The scanning numbers can be increased in some areas, and the areas where the scanning numbers are increased will increase in thickness, and polymerization will progress. (<b>c</b>) Deformation of printed modeling objects. The upper figure shows deformation before being placed in water, and the lower figure shows it after being placed in water. Gels with different swelling on the top and bottom layers were printed. (<b>d</b>) The SEM image of the cross section of the dried ICN gels indicates the existence of the bilayer structure. The left side, which seems white, is the UV-exposed side. This part is the upper, thinner layer. The right side is the lower, thicker layer, where the particles of photoinitiator TPO crystals precipitated during the 3D printing process are observed.</p>
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<p>Schematic illustration of fabrication process of the gradient ICN gels. When the ICN gel solution is scanned with the UV laser from one direction, the UV-exposed side has a higher crosslink density, and the other side has a lower crosslink density.</p>
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<p>The photos of 3D printed bilayer gels of the hydrogel sheet without/with the hinge structure during swelling process. The left half side of all the gels is bonded on glass plate. The right half side in not bonded and then can lift up in the swelling process. The red angles indicate the degree of bending deformation.</p>
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<p>(<b>a</b>) The swelling ratio measurement as a function of time, in the various concentrations of the initiator TPO and in the one or three scanning numbers of UV irradiation in 3D printing. (<b>b</b>) The Young’s modulus measurement as a function of the concentration of the initiator TPO in the one or three scanning numbers of UV irradiation in 3D printing. (<b>c</b>) The bending angle with the various concentrations of the initiator TPO. The inset photographs indicate the final states of deformation. (<b>d</b>) The bending angle vs. the concentration of the initiator TPO.</p>
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<p>(<b>a</b>) The swelling ratio measurement as a function of time, in the various crosslinker concentrations and in the one or three scanning numbers of UV irradiation in 3D printing. (<b>b</b>) Young’s modulus measurement as a function of the crosslinker concentration, in the one or three scanning numbers of UV irradiation in 3D printing. (<b>c</b>) The degree of deformation measurement as a function of time in the various crosslinker concentrations. The inset photographs indicate the final states of deformation. (<b>d</b>) The bending angle vs. the concentration of the crosslinker Karenz MOI-EG.</p>
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<p>(<b>a</b>) The swelling ratio measurement as a function of time, in the one, two, three, and five scanning numbers of UV irradiation in 3D printing. (<b>b</b>) Young’s modulus measurement as a function of the scanning number of UV irradiation in 3D printing. (<b>c</b>) The bending angle as a function of time, in the various scanning numbers, without hinge structure. The inset photographs indicate the final states of deformation. (<b>d</b>) The bending angle as a function of the scanning number, without hinge structure. (<b>e</b>) The bending angle as a function of time, in the various scanning numbers, with/without hinge structure. The inset photographs indicate the final states of deformation. (<b>f</b>) The bending angle as a function of the scanning number, with/without hinge structure.</p>
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<p>The before and after photographs of 4D printing of hydrogels controlled by hinge structure and spatially gradient swelling at 0 min and 30 min. (<b>a</b>) Jellyfish model (without hinge structure). (<b>b</b>) Cubic origami. (<b>c</b>) Warm models with two different hinge structures. (<b>d</b>) Scorpion model.</p>
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<p>The 4D printing of worm models with two different hinge structures. (<b>a</b>) The design of the two different hinge structures. Type 1 is a transverse hinge, whose angle between the hinge direction and the longitudinal direction of the worm is 90 degrees. Type 2 is a tilted hinge, whose angle between the hinge direction and the longitudinal direction of the worm is 120 degrees. (<b>b</b>) The before and after photographs of the two different worms. Type 1 is the transverse hinge bent until it came around. Type 2 is the tilted hinge twisted until it formed an S shape.</p>
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<p>The 4D printing of the scorpion model. (<b>a</b>) The two-step method of 3D printing of the scorpion. In the first step, the body and scissor parts are 3D printed. In the second step, the previously printed body and scissors are flipped over and then the eight legs are 3D printed. (<b>b</b>) The actual 3D printing process. After the first step of 3D printing, the silicone mold is turned over and the part to be made in the second step is 3D printed from the opposite side. This enables the 4D printing of both valley and mountain folds as in origami.</p>
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<p>FE simulation results of: (<b>a</b>) the two identical layer model, (<b>b</b>) the model with a hinge structure, and (<b>c</b>) the bending deformation in different time periods.</p>
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15 pages, 11343 KiB  
Article
A Lightweight CNN for Wind Turbine Blade Defect Detection Based on Spectrograms
by Yuefan Zhu and Xiaoying Liu
Machines 2023, 11(1), 99; https://doi.org/10.3390/machines11010099 - 11 Jan 2023
Cited by 8 | Viewed by 2462
Abstract
Since wind turbines are exposed to harsh working environments and variable weather conditions, wind turbine blade condition monitoring is critical to prevent unscheduled downtime and loss. Realizing that common convolutional neural networks are difficult to use in embedded devices, a lightweight convolutional neural [...] Read more.
Since wind turbines are exposed to harsh working environments and variable weather conditions, wind turbine blade condition monitoring is critical to prevent unscheduled downtime and loss. Realizing that common convolutional neural networks are difficult to use in embedded devices, a lightweight convolutional neural network for wind turbine blades (WTBMobileNet) based on spectrograms is proposed, reducing computation and size with a high accuracy. Compared to baseline models, WTBMobileNet without data augmentation has an accuracy of 97.05%, a parameter of 0.315 million, and a computation of 0.423 giga floating point operations (GFLOPs), which is 9.4 times smaller and 2.7 times less computation than the best-performing model with only a 1.68% decrease in accuracy. Then, the impact of difference data augmentation is analyzed. The WTBMobileNet with augmentation has an accuracy of 98.1%, and the accuracy of each category is above 95%. Furthermore, the interpretability and transparency of WTBMobileNet are demonstrated through class activation mapping for reliable deployment. Finally, WTBMobileNet is explored in drones image classification and spectrogram object detection, whose accuracy and mAP@[0.5, 0.95] are 89.55% and 70.7%, respectively. This proves that WTBMobileNet not only has a good performance in spectrogram classification, but also has good application potential in drone image classification and spectrogram object detection. Full article
(This article belongs to the Special Issue Machine Learning for Fault Diagnosis of Wind Turbines)
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<p>The framework of wind turbine blade defect detection based on CNN.</p>
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<p>The diagram of short-time Fourier transform.</p>
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<p>Principle and structure diagram of lightweight module.</p>
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<p>Schematic of: (<b>a</b>) inception; (<b>b</b>) depth-wise convolution; (<b>c</b>) standard convolution.</p>
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<p>The spectrogram of (<b>a</b>) normal (CUBE, Dawu); (<b>b</b>) Defect 1 (DR-60D, Dawu); (<b>c</b>) Defect 2 (DR-60D, Dawu); and (<b>d</b>) Defect 3 (CUBE, Diaoyutai).</p>
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<p>The error of WTBMobileNet with the epochs increasing.</p>
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<p>Confusion matrix of WTBMobileNet: (<b>a</b>) without data augmentation; (<b>b</b>) with data augmentation.</p>
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<p>Class activation mapping for: (<b>a</b>) Normal (CUBE, Dawu); (<b>b</b>) Defect 1 (DR-60D, Dawu); (<b>c</b>) Defect 2 (DR-60D, Dawu); and (<b>d</b>) Defect 3 (CUBE, Diaoyutai).</p>
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<p>Examples of object detection results on the spectrograms using the Faster R-CNN based on WTBMobileNet. The red is the ground-truth box, and the yellow is the predicted box.</p>
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18 pages, 4340 KiB  
Article
Research on the High Precision Synchronous Control Method of the Fieldbus Control System
by Lingyu Chen, Jieji Zheng, Dapeng Fan and Ning Chen
Machines 2023, 11(1), 98; https://doi.org/10.3390/machines11010098 - 11 Jan 2023
Cited by 2 | Viewed by 2211
Abstract
The synchronization control performance of the Fieldbus control system (FCS) is an important guarantee for the completion of multi-axis collaborative machining tasks, and its synchronization control accuracy is one of the decisive factors for the machining quality. To improve the synchronization control accuracy [...] Read more.
The synchronization control performance of the Fieldbus control system (FCS) is an important guarantee for the completion of multi-axis collaborative machining tasks, and its synchronization control accuracy is one of the decisive factors for the machining quality. To improve the synchronization control accuracy of FCS, this paper first makes a comprehensive analysis of the factors affecting synchronization in FCS. Secondly, by analyzing the communication model of linear Ethernet, a distributed clock compensation method based on timestamps is proposed to solve the asynchronous problem of communication data transmission in the linear ethernet bus topology. Then, based on the CANopen application layer protocol, the FCS communication and device control task collaboration method is proposed to ensure the synchronous control of multiple devices by FCS. Finally, an experimental platform is built for functional verification and performance testing of the proposed synchronization method. The results show that the proposed synchronization method can achieve a communication synchronization accuracy of 50 ns and a device control synchronization accuracy of 150 ns. Full article
(This article belongs to the Special Issue Social Manufacturing on Industrial Internet)
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<p>Schematic diagram of the FCS architecture.</p>
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<p>Schematic diagram of the communication structure of FCS.</p>
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<p>Schematic diagram of a typical FCS task timing sequence.</p>
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<p>Schematic diagram of the communication transmission delay in a linear network.</p>
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<p>Communication transmission delay model for the linear network.</p>
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<p>Schematic Diagram of Distributed Clock Compensation: (<b>a</b>) actual curve of local time and reference time slave; (<b>b</b>) curve of local time and reference time after compensation.</p>
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<p>Schematic diagram of the Ethernet frame data structure.</p>
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<p>Schematic diagram of CANopen frames integrated with the mapping message.</p>
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<p>Schematic diagram of system communication timing sequence in the pre-operation state.</p>
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<p>Schematic diagram of system communication timing sequence in operation.</p>
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<p>Slave control task timing sequence diagram in operation state.</p>
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<p>Slave control task timing sequence diagram in operation state.</p>
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<p>FCS experimental platform diagram.</p>
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<p>System distributed clock synchronization test result diagram: (<b>a</b>) SYNC signal waveform of each slave under a 400 μs time scale; (<b>b</b>) SYNC signal waveform of each slave under a 20 ns time scale.</p>
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<p>System device control synchronization test result diagram: (<b>a</b>) pulse output waveform of each slave under a 200 μs time scale; (<b>b</b>) pulse output waveform of each slave under a 80 ns time scale.</p>
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16 pages, 5775 KiB  
Article
On the Dynamics of an Enhanced Coaxial Inertial Exciter for Vibratory Machines
by Volodymyr Gurskyi, Vitaliy Korendiy, Pavlo Krot, Radosław Zimroz, Oleksandr Kachur and Nadiia Maherus
Machines 2023, 11(1), 97; https://doi.org/10.3390/machines11010097 - 11 Jan 2023
Cited by 14 | Viewed by 1946
Abstract
Theoretical investigations into the capabilities of a coaxial inertial drive with various operating modes for vibratory conveyors and screens are conducted in the paper. The coaxial inertial exciter is designed with one asynchronous electric motor and the kinematically synchronized rotation of two unbalanced [...] Read more.
Theoretical investigations into the capabilities of a coaxial inertial drive with various operating modes for vibratory conveyors and screens are conducted in the paper. The coaxial inertial exciter is designed with one asynchronous electric motor and the kinematically synchronized rotation of two unbalanced masses. Three variants of angular speeds ratios, namely ω21 = 1, ω21 = –1, and ω21 = 2, are considered. Based on these relations, the circular, elliptical, and complex motion trajectories of the working members are implemented. In the first two cases, single-frequency harmonic oscillations take place. In the latter case, the double-frequency periodic oscillations are excited. The dynamic behavior of the motor’s shaft during its running-up and running-out is considered. The influence of the inertial parameters of the unbalanced rotors and the relative phase shift angle between them on the elliptical trajectories of the vibratory system’s mass center motion is investigated. The use of forced kinematic synchronization provides the motion stability of the vibratory system for all considered working regimes. Full article
(This article belongs to the Special Issue Dynamics Control and Vibration Monitoring in Industrial Machines)
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<p>Vibration conveyor with three inertial drives (“GEA Group AG”).</p>
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<p>Kinematic diagram of the inertial vibration exciter with a single asynchronous electric motor, as follows: 1, 2—internal and external unbalanced rotors, respectively; 3—exciter’s body; 4—bearings; 5, 6—belt transmissions; 7—electric motor.</p>
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<p>Schemes of kinematic synchronization of the unbalanced rotors of the inertial vibration exciter. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Time series of the electric motor’s shaft angular speeds under different synchronization conditions of the unbalanced rotors.</p>
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<p>Time dependence of the electric motor’s shaft torque at different synchronization conditions of the unbalanced rotors. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math></p>
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<p>Trajectories of the mass center motion at different ratios between the angular speeds of the unbalanced rotors.</p>
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<p>Time dependencies of the disturbing force of the inertial vibration exciter at different ratios between the angular speeds of the unbalanced rotors.</p>
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<p>Time dependencies of the working member displacements at different synchronization conditions of the unbalanced rotors. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math></p>
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<p>Time dependencies of the working member displacements at different synchronization conditions of the unbalanced rotors. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math></p>
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<p>Trajectories of the working member’s mass center motion at different values of the phase shift angle <math display="inline"><semantics> <mi>φ</mi> </semantics></math> and static moments of the unbalanced rotors <math display="inline"><semantics> <mrow> <msub> <mi>m</mi> <mn>1</mn> </msub> <msub> <mi>r</mi> <mn>1</mn> </msub> <mo>/</mo> <msub> <mi>m</mi> <mn>2</mn> </msub> <msub> <mi>r</mi> <mn>2</mn> </msub> </mrow> </semantics></math> under their counter-rotation conditions, as follows: <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Amplitude–frequency characteristics of the vibratory system at the phase-shift angle <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>90</mn> <mo>°</mo> </mrow> </semantics></math> and under different synchronization conditions of (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Amplitude–frequency characteristics of the vibratory system for under synchronization condition <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> <msub> <mi>ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math> at the phase-shift angles of (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math> and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>180</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
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19 pages, 3616 KiB  
Review
Recent Development for Ultra-Precision Macro–Micro Dual-Drive System: A Review
by Manzhi Yang, Haochen Gui, Chuanwei Zhang, Shuanfeng Zhao, Feiyan Han, Meng Dang and Bin Zhang
Machines 2023, 11(1), 96; https://doi.org/10.3390/machines11010096 - 11 Jan 2023
Cited by 9 | Viewed by 3022
Abstract
Macro–micro dual-drive technology uses a micro-drive system to compensate for motion errors of a macro-drive system, solving the contradiction between large travel and high-precision motion. Additionally, it has a wide range of applications in the ultra-precision field. Therefore, it is necessary to analyze [...] Read more.
Macro–micro dual-drive technology uses a micro-drive system to compensate for motion errors of a macro-drive system, solving the contradiction between large travel and high-precision motion. Additionally, it has a wide range of applications in the ultra-precision field. Therefore, it is necessary to analyze and research the ultra-precision macro–micro dual-drive system. Firstly, this paper analyzes the history of ultra-precision technology development and summarizes the research status of ultra-precision technology processing and application. Secondly, the micro-drive mechanism design and macro–micro-drive mode of macro–micro dual-drive technology, which can solve the contradiction of large stroke and high precision, are reviewed, and the application of macro–micro dual-drive technology in an ultra-precision system is summarized. Finally, the challenges and development trends of the ultra-precision macro–micro dual-drive system are analyzed. The research in this paper will play an important role in promoting the development of the ultra-precision system and macro–micro dual-drive technology. Full article
(This article belongs to the Special Issue Recent Progress of Thin Wall Machining)
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<p>(<b>a</b>) Nanotech 500FG. Reprinted with permission from ref. [<a href="#B5-machines-11-00096" class="html-bibr">5</a>] Copyright 2005 Elsevier; (<b>b</b>) Pico Ace. Reprinted with permission from ref. [<a href="#B5-machines-11-00096" class="html-bibr">5</a>] Copyright 2005 Elsevier; (<b>c</b>) Fanuc Robonano α-0Ia. Reprinted with permission from ref. [<a href="#B5-machines-11-00096" class="html-bibr">5</a>] Copyright 2005 Elsevier; (<b>d</b>) Aerostatic bearing spindle. Reprinted with permission from ref. [<a href="#B7-machines-11-00096" class="html-bibr">7</a>] Copyright 2018 Elsevier.</p>
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<p>(<b>a</b>) Corner smoothing scheme. Reprinted with permission from ref. [<a href="#B31-machines-11-00096" class="html-bibr">31</a>] Copyright 2015 Elsevier; (<b>b</b>) Adjustable handle design [<a href="#B32-machines-11-00096" class="html-bibr">32</a>]; (<b>c</b>) FTS and mass dampers [<a href="#B33-machines-11-00096" class="html-bibr">33</a>]; (<b>d</b>) SEM image of grinding prop. Reprinted with permission from ref. [<a href="#B34-machines-11-00096" class="html-bibr">34</a>] Copyright 2009 Elsevier; (<b>e</b>) Surface roughness of molded Pt/C multilayer mirror. Reprinted with permission from ref. [<a href="#B35-machines-11-00096" class="html-bibr">35</a>] Copyright 2008 Elsevier; (<b>f</b>) Microfluidic chip manufactured by low-temperature micromachining. Reprinted with permission from ref. [<a href="#B36-machines-11-00096" class="html-bibr">36</a>] Copyright 2012 Elsevier.</p>
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<p>In situ DPA 3D measurement system. (<b>a</b>) Reprinted with permission from ref. [<a href="#B42-machines-11-00096" class="html-bibr">42</a>] © 2015 The Optical Society; (<b>b</b>) Experimental equipment of dimethyl ether for gravure roller [<a href="#B43-machines-11-00096" class="html-bibr">43</a>]; (<b>c</b>) Free-form micro-lens array. Reprinted with permission from [<a href="#B44-machines-11-00096" class="html-bibr">44</a>] © 2015 The Optical Society.</p>
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<p>Working principle diagram of macro–micro dual-drive system.</p>
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<p>Flexure hinge with different shapes: (<b>a</b>) straight circular flexure; (<b>b</b>) circular flexure hinge; (<b>c</b>) parabolic flexure hinge; (<b>d</b>) straight beam flexure.</p>
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<p>(<b>a</b>) Clamping mechanism. Reprinted with permission from ref. [<a href="#B66-machines-11-00096" class="html-bibr">66</a>] Copyright 2009 Elsevier; (<b>b</b>) ultra-precision fiber alignment mechanism. Reprinted with permission from ref. [<a href="#B69-machines-11-00096" class="html-bibr">69</a>] Copyright 2004 Elsevier; (<b>c</b>) micro-drive reduction mechanism [<a href="#B70-machines-11-00096" class="html-bibr">70</a>]; (<b>d</b>) micro-drive amplification mechanism.</p>
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<p>(<b>a</b>) Macro–micro-positioning system [<a href="#B76-machines-11-00096" class="html-bibr">76</a>]; (<b>b</b>) prototype of a linear piezoelectric motor. Reprinted with permission from ref. [<a href="#B86-machines-11-00096" class="html-bibr">86</a>] Copyright 2016 Elsevier.</p>
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<p>(<b>a</b>) Three degrees of freedom parallel micro/nano flexible mechanical system. Reprinted with permission from ref. [<a href="#B88-machines-11-00096" class="html-bibr">88</a>] Copyright 2008 Elsevier; (<b>b</b>) The overall structure of a miniature gripper system [<a href="#B89-machines-11-00096" class="html-bibr">89</a>]. (<b>c</b>) Solid models for the 6-degree-of-freedom mechanism employing oars and fine actuation. Reprinted with permission from ref. [<a href="#B92-machines-11-00096" class="html-bibr">92</a>] Copyright 2010 Elsevier.</p>
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<p>(<b>a</b>) Rotary linear precision motion platform [<a href="#B94-machines-11-00096" class="html-bibr">94</a>]; (<b>b</b>) XY plane motion platform. Reprinted with permission from ref. [<a href="#B95-machines-11-00096" class="html-bibr">95</a>] Copyright 2004 Elsevier; (<b>c</b>) a conceptual design of SMG. Reprinted with permission from ref. [<a href="#B97-machines-11-00096" class="html-bibr">97</a>] Copyright 2018 Elsevier.</p>
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<p>The experimental setup. Reprinted with permission from ref. [<a href="#B106-machines-11-00096" class="html-bibr">106</a>] Copyright 2005 IEEE.</p>
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21 pages, 1538 KiB  
Article
Optimization of Selective Laser Sintering/Melting Operations by Using a Virus-Evolutionary Genetic Algorithm
by Nikolaos A. Fountas, John D. Kechagias and Nikolaos M. Vaxevanidis
Machines 2023, 11(1), 95; https://doi.org/10.3390/machines11010095 - 11 Jan 2023
Cited by 18 | Viewed by 2336
Abstract
This work presents the multi-objective optimization results of three experimental cases involving the laser sintering/melting operation and obtained by a virus evolutionary genetic algorithm. From these three experimental cases, the first one is formulated as a single-objective optimization problem aimed at maximizing the [...] Read more.
This work presents the multi-objective optimization results of three experimental cases involving the laser sintering/melting operation and obtained by a virus evolutionary genetic algorithm. From these three experimental cases, the first one is formulated as a single-objective optimization problem aimed at maximizing the density of Ti6Al4V specimens, with layer thickness, linear energy density, hatching space and scanning strategy as the independent process parameters. The second one refers to the formulation of a two-objective optimization problem aimed at maximizing both the hardness and tensile strength of Ti6Al4V samples, with laser power, scanning speed, hatch spacing, scan pattern angle and heat treatment temperature as the independent process parameters. Finally, the third case deals with the formulation of a three-objective optimization problem aimed at minimizing mean surface roughness, while maximizing the density and hardness of laser-melted L316 stainless steel powder. The results obtained by the proposed algorithm are statistically compared to those obtained by the Greywolf (GWO), Multi-verse (MVO), Antlion (ALO), and dragonfly (DA) algorithms. Algorithm-specific parameters for all the algorithms including those of the virus-evolutionary genetic algorithm were examined by performing systematic response surface experiments to find the beneficial settings and perform comparisons under equal terms. The results have shown that the virus-evolutionary genetic algorithm is superior to the heuristics that were tested, at least on the basis of evaluating regression models as fitness functions. Full article
(This article belongs to the Special Issue Design and Manufacturing: An Industry 4.0 Perspective)
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<p>(<b>a</b>) Transduction operation for the generation of a virus individual. (<b>b</b>) Reverse transcription operation for infecting selected individuals with a virus. (<b>c</b>) Infected individual after the reverse transcription operation performed by a virus.</p>
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<p>Partial transduction operation for changing the virus scheme.</p>
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<p>Flow chart of viral infection after the evaluation of main population’s individuals.</p>
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<p>Convergence speed exhibited by VEGA, GWO, MVO, ALO and DA algorithms for maximizing mean density, with 200 iterations.</p>
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<p>Pareto fronts for the non-dominated solutions obtained from the best simulation experiment exhibited by: (<b>a</b>) MOVEGA, (<b>b</b>) MOGWO, (<b>c</b>) MOMVO, (<b>d</b>) MOALO, (<b>e</b>) MODA and (<b>f</b>) Comparison of Pareto fronts algorithms for case 2, with 20 individuals and 200 iterations.</p>
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<p>Pareto fronts of non-dominated solutions for the best simulation experiment exhibited by: (<b>a</b>) MOVEGA, (<b>b</b>) MOGWO, (<b>c</b>) MOMVO, (<b>d</b>) MOALO and (<b>e</b>) MODA algorithms for case 3, with 20 individuals and 200 iterations.</p>
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19 pages, 4241 KiB  
Article
Intelligent Tool-Wear Prediction Based on Informer Encoder and Bi-Directional Long Short-Term Memory
by Xingang Xie, Min Huang, Yue Liu and Qi An
Machines 2023, 11(1), 94; https://doi.org/10.3390/machines11010094 - 11 Jan 2023
Cited by 11 | Viewed by 3150
Abstract
Herein, to accurately predict tool wear, we proposed a new deep learning network—that is, the IE-Bi-LSTM—based on an informer encoder and bi-directional long short-term memory. The IE-Bi-LSTM uses the encoder part of the informer model to capture connections globally and to extract long [...] Read more.
Herein, to accurately predict tool wear, we proposed a new deep learning network—that is, the IE-Bi-LSTM—based on an informer encoder and bi-directional long short-term memory. The IE-Bi-LSTM uses the encoder part of the informer model to capture connections globally and to extract long feature sequences with rich information from multichannel sensors. In contrast to methods using CNN and RNN, this model could achieve remote feature extraction and the parallel computation of long-sequence-dependent features. The informer encoder adopts the attention distillation layer to increase computational efficiency, thereby lowering the attention computational overhead in comparison to that of a transformer encoder. To better collect location information while maintaining serialization properties, a bi-directional long short-term memory (Bi-LSTM) network was employed. After the fully connected layer, the tool-wear prediction value was generated. After data augmentation, the PHM2010 basic dataset was used to check the effectiveness of the model. A comparison test revealed that the model could learn more full features and had a strong prediction accuracy after hyperparameter tweaking. An ablation experiment was also carried out to demonstrate the efficacy of the improved model module. Full article
(This article belongs to the Special Issue Tool Wear in Machining)
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<p>The scaled dot-product attention architecture.</p>
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<p>The prob-sparse self-attention architecture.</p>
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<p>Illustration of the informer encoder.</p>
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<p>Illustration of the multi-head attention layer.</p>
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<p>Illustration of the distilling layer.</p>
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<p>Graphical illustration of the LSTM.</p>
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<p>Graphical illustration of the Bi-LSTM layers used in the IE-Bi-LSTM model.</p>
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<p>Illustration of the proposed method.</p>
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<p>Illustration of the experimental setup.</p>
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<p>Data preprocessing program.</p>
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<p>Comparisons between the predicted tool wear and the ground-truth tool wear: (<b>a</b>) C1 cutter, (<b>b</b>) C4 cutter, and (<b>c</b>) C6 cutter.</p>
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<p>Estimation performance of different models using the PHM2010 testing dataset.</p>
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<p>Estimation performance of different models using the PHM2010 testing dataset.</p>
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18 pages, 5911 KiB  
Article
Tribodynamic Modelling of High-Speed Rolling Element Bearings in Flexible Multi-Body Environments
by Harry Questa, Mahdi Mohammadpour, Stephanos Theodossiades, Colin P. Garner, Stephen R. Bewsher and Günter Offner
Machines 2023, 11(1), 93; https://doi.org/10.3390/machines11010093 - 11 Jan 2023
Cited by 1 | Viewed by 2097
Abstract
This study presents a new flexible dynamic model for drive systems comprising lubricated bearings operating under conditions representative of electrified vehicle powertrains. The multi-physics approach importantly accounts for the tribological phenomena at the roller–race conjunction and models their effect on shaft-bearing system dynamics. [...] Read more.
This study presents a new flexible dynamic model for drive systems comprising lubricated bearings operating under conditions representative of electrified vehicle powertrains. The multi-physics approach importantly accounts for the tribological phenomena at the roller–race conjunction and models their effect on shaft-bearing system dynamics. This is achieved by embedding a non-linear lubricated bearing model within a flexible system level model; this is something which has not, to the authors’ knowledge, been reported on hitherto. The elastohydrodynamic (EHL) film is shown to increase contact deflection, leading to increased contact forces and total bearing stiffness as rotational speeds increase. Results show that for a 68 Nm hub motor operating up to 21,000 rpm, the input bearing EHL film reaches a thickness of 4.15 μm. The lubricant entrainment increases the roller–race contact deflection, causing the contact stiffness to increase non-linearly with speed. The contribution of the lubricant film leads to a 16.6% greater bearing stiffness at 21,000 rpm when compared to conventional dry-bearing modelling methods used in current multi-body dynamic software. This new methodology leads to more accurate dynamic response of high-speed systems necessary for the next generation of electrified vehicles. Full article
(This article belongs to the Special Issue Friction and Lubrication of Rolling Element Bearings)
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<p>Flowchart of Models.</p>
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<p>System Level Model Schematic.</p>
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<p>Bearing Schematic.</p>
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<p>Dry vs. Lubricated Roller–Race Contact.</p>
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<p>Contact Level Validation.</p>
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<p>PMSM Torque Profile and Maximum and Minimum Torque Fluctuation.</p>
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<p>Rolling Element Contact Stiffness—Dry vs. Lubricated Maximum Values.</p>
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<p>Rolling Element Contact Force—Dry vs. Lubricated Percentage Increase.</p>
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<p>Inner Race Stiffness—Dry vs. Lubricated Operating Envelope.</p>
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<p>Inner Race Displacement—Dry vs. Lubricated Operating Envelope.</p>
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<p>Inner Race Acceleration—Dry vs. Lubricated Operating Envelope.</p>
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<p>Rolling Element Contact Stiffness—Dry vs. Lubricated Minimum Values.</p>
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<p>Film Thickness vs. Contact Force 21,000 rpm.</p>
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<p>Film Thickness vs. Contact Force 12,500 rpm.</p>
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15 pages, 3521 KiB  
Article
ShuffleNet v2.3-StackedBiLSTM-Based Tool Wear Recognition Model for Turbine Disc Fir-Tree Slot Broaching
by Shenshun Ying, Yicheng Sun, Fuhua Zhou and Lvgao Lin
Machines 2023, 11(1), 92; https://doi.org/10.3390/machines11010092 - 11 Jan 2023
Cited by 1 | Viewed by 2791
Abstract
At present, deep learning technology shows great market potential in broaching tool wear state recognition based on vibration signals. However, traditional single neural network structure is difficult to extract a variety of different features simultaneously and has low robustness, so the accuracy of [...] Read more.
At present, deep learning technology shows great market potential in broaching tool wear state recognition based on vibration signals. However, traditional single neural network structure is difficult to extract a variety of different features simultaneously and has low robustness, so the accuracy of wear status recognition is not high. In view of the above problems, a broaching tool wear recognition model based on ShuffleNet v2.3-StackedBiLSTM is proposed in this paper. The model integrates ShuffleNet v2.3, which has been channel shuffling, and StackedBiLSTM, a long and short-term memory network, to effectively extract spatial and temporal features for tool wear state recognition. Based on the innovative recognition model, the turbine disc fir-tree slot broaching experiment is designed, and the performance index system based on confusion matrix is adopted. The experimental research and results show that the model has outstanding accuracy, precision, recall, and F1 value, and the accuracy rate reaches 99.37%, which is significantly better than ShuffleNet v2.3 and StackedBiLSTM models. The recognition speed of a single sample was improved to 8.67 ms, which is 90.32% less than that of the StackedBiLSTM model. Full article
(This article belongs to the Special Issue Tool Wear in Machining)
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Graphical abstract

Graphical abstract
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<p>ShuffleNet v2.3 network structure.</p>
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<p>The StackedBiLSTM structure.</p>
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<p>ShuffleNet v2.3-StackedBiLSTM tool wear state recognition model.</p>
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<p>Data pre-processing before training: (<b>a</b>) Original signal; (<b>b</b>) normalized signal.</p>
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<p>Test device diagram of tool wear experiment.</p>
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<p>Loss value and accuracy change curve of each model: (<b>a</b>) Loss value curve; (<b>b</b>) accuracy curve.</p>
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<p>Confusion matrix for different models:(<b>a</b>) ShuffleNet v2.3-StackedBiLSTM classification model confusion matrix test results; (<b>b</b>) ShuffleNet v2.3 classification model confusion matrix test results; (<b>c</b>) StackedBiLSTM classification model confusion matrix test results.</p>
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