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Search Results (1,405)

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25 pages, 1252 KiB  
Article
Optimization of Energy Management Strategy for Series Hybrid Electric Vehicle Equipped with Dual-Mode Combustion Engine Under NVH Constraints
by Shupeng Zhang, Hongnan Wang, Chengkai Yang, Zeping Ouyang and Xiaoxin Wen
Appl. Sci. 2024, 14(24), 12021; https://doi.org/10.3390/app142412021 - 22 Dec 2024
Viewed by 290
Abstract
Energy management strategies (EMSs) are a core technology in hybrid electric vehicles (HEVs) and have a significant impact on their fuel economy. Optimal solutions for EMSs in the literature usually focus on improving fuel efficiency by operating the engine within a high efficiency [...] Read more.
Energy management strategies (EMSs) are a core technology in hybrid electric vehicles (HEVs) and have a significant impact on their fuel economy. Optimal solutions for EMSs in the literature usually focus on improving fuel efficiency by operating the engine within a high efficiency range, without considering the drivability, which is affected by noise–vibration–harshness (NVH) constraints at low vehicle speeds. In this paper, a dual-mode combustion engine was implemented in a plug-in series hybrid electric vehiclethat could operate efficiently either at low loads in homogeneous charge compression ignition (HCCI) mode or at high loads in spark ignition (SI) mode. An equivalent consumption minimization strategy (ECMS) combined with a dual-loop particle swarm optimization (PSO) algorithm was designed to solve the optimal control problem. A MATLAB/Simulink simulation was performed using a well-calibrated model of the target HEV to validate the proposed method, and the results showed that it can achieve a reduction in fuel consumption of around 1.3% to 9.9%, depending on the driving cycle. In addition, the operating power of the battery can be significantly reduced, which benefits the health of the battery. Furthermore, the proposed ECMS-PSO is computationally efficient, which guarantees fast offline optimization and enables real-time applications. Full article
(This article belongs to the Special Issue Recent Developments in Electric Vehicles)
14 pages, 3380 KiB  
Article
Drone Rider: Foot Vibration Stimuli to Enhance Immersion and Flight Sensation in VR
by Kazuya Shimato, Yuta Goto and Shogo Okamoto
Appl. Sci. 2024, 14(24), 12019; https://doi.org/10.3390/app142412019 - 22 Dec 2024
Viewed by 305
Abstract
Simulating the experience of flight is a key objective of virtual reality (VR) technology. To enhance the sense of flying and immersion, we developed Drone Rider, a VR system that simulates free-flight atop a drone. In this study, we investigated whether delivering vibratory [...] Read more.
Simulating the experience of flight is a key objective of virtual reality (VR) technology. To enhance the sense of flying and immersion, we developed Drone Rider, a VR system that simulates free-flight atop a drone. In this study, we investigated whether delivering vibratory stimuli to the user’s feet could improve these sensations. While high-frequency drone propeller vibrations typically induce sensory numbness, alternative vibration patterns were explored. In Experiment 1, participants rated 13 different vibration patterns derived from various mechanical sounds, such as those from chainsaws, motorcycles, and washing machines. The motorcycle-based vibrations were most effective in enhancing both the sense of flight and immersion. In Experiment 2, we synthesized new vibration patterns by superimposing the highest-rated vibrations from Experiment 1, but no combination outperformed the original motorcycle vibration. These findings suggest that vibrations with multiple components below 100 Hz may reduce sensory adaptation and enhance the sense of flight and immersion in VR. This work provides valuable insights for developers aiming to optimize haptic feedback in VR flight simulators. Full article
(This article belongs to the Special Issue Virtual and Augmented Reality: Theory, Methods, and Applications)
17 pages, 8063 KiB  
Article
Research on the Comparison of the Flow Evolution Mechanisms of a Water-Jet Pump Between Valley and Peak Conditions
by Min Liu, Yun Long, Yingying Zheng, Jinqing Zhong and Hong Yin
J. Mar. Sci. Eng. 2024, 12(12), 2352; https://doi.org/10.3390/jmse12122352 - 21 Dec 2024
Viewed by 284
Abstract
The pump hump significantly influences the vibration and operational stability of pumps. During the development of the mixed-flow waterjet pump, our team found that the pump performance curve had a hump phenomenon and the platform had vibration, so it was suspected that there [...] Read more.
The pump hump significantly influences the vibration and operational stability of pumps. During the development of the mixed-flow waterjet pump, our team found that the pump performance curve had a hump phenomenon and the platform had vibration, so it was suspected that there was a strong secondary flow in the hump region. The calculation model is the SST k-ω turbulence model. The impeller and diffuser use structured grids. By using high-speed photography technology, we map the cavitation flow structures, thereby demonstrating the evolution of cavitation processes. The hump curve was obtained by an experimental test. By comparing the test data and numerical simulation, the consistency of the method and the hump curve is verified. A comparative analysis is performed to investigate the variations in the distribution of internal vortex structures and the evolution of rotating stalls in the impeller. In the valley condition, the main frequency of pressure pulsation in the inlet section of the impeller is 0.75 times the shaft frequency, the main frequency in the middle and outlet sections of the impeller is 1 times the shaft frequency, and the main frequency in the diffuser basin is 1.5 times the shaft frequency, the main frequency in the peak condition at the points of Span = 0.1 and Span = 0.5 of the impeller is the diffuser frequency, the main frequency at the point of Span = 0.9 is the impeller blade frequency, and the main frequency in the diffuser basin is either the shaft frequency or the diffuser blade frequency. This research reveals the characteristics of vortex flow in the pump under hump conditions. It reveals that the evolution mechanism of the hump offers a guide value for the subsequent hydrodynamic design of the hump. Full article
(This article belongs to the Section Ocean Engineering)
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<p>Performance analysis of pumps under different operating conditions and characteristics of the flow field inside the impeller [<a href="#B1-jmse-12-02352" class="html-bibr">1</a>,<a href="#B2-jmse-12-02352" class="html-bibr">2</a>].</p>
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<p>The hydraulic model [<a href="#B1-jmse-12-02352" class="html-bibr">1</a>].</p>
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<p>Experimental loop and the model pump. (<b>a</b>) Three-dimensional model of an experimental pump [<a href="#B1-jmse-12-02352" class="html-bibr">1</a>,<a href="#B2-jmse-12-02352" class="html-bibr">2</a>]; (<b>b</b>) visual window of impeller plexiglass [<a href="#B30-jmse-12-02352" class="html-bibr">30</a>]; (<b>c</b>) experimental loop [<a href="#B1-jmse-12-02352" class="html-bibr">1</a>,<a href="#B2-jmse-12-02352" class="html-bibr">2</a>].</p>
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<p>Experimental loop and the model pump. (<b>a</b>) Three-dimensional model of an experimental pump [<a href="#B1-jmse-12-02352" class="html-bibr">1</a>,<a href="#B2-jmse-12-02352" class="html-bibr">2</a>]; (<b>b</b>) visual window of impeller plexiglass [<a href="#B30-jmse-12-02352" class="html-bibr">30</a>]; (<b>c</b>) experimental loop [<a href="#B1-jmse-12-02352" class="html-bibr">1</a>,<a href="#B2-jmse-12-02352" class="html-bibr">2</a>].</p>
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<p>Computational grid of hydraulic components [<a href="#B1-jmse-12-02352" class="html-bibr">1</a>,<a href="#B2-jmse-12-02352" class="html-bibr">2</a>].</p>
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<p>Distribution location of monitor points. (<b>a</b>) monitor points on the impeller, (<b>b</b>) monitor points on the diffuser.</p>
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<p>Time-domain plot of pressure pulsation inside the pump in the valley and peak conditions. (<b>a</b>) Valley condition (left: impeller flow channel; right: diffuser flow channel), (<b>b</b>) peak condition (left: impeller flow channel; right: diffuser flow channel).</p>
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<p>Frequency-domain plot of pressure pulsation inside the pump in the valley and peak conditions. (<b>a</b>) Valley condition (left: impeller basin; right: diffuser basin), (<b>b</b>) peak condition (left: impeller basin; right: diffuser basin).</p>
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<p>Pressure distribution inside the pump in the valley and peak conditions (multimedia available online). (<b>a</b>) Pressure distribution in the impeller basin (left: valley condition; right: peak condition), (<b>b</b>) pressure distribution in the diffuser basin (left: valley condition; right: peak condition).</p>
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<p>Streamline distribution inside the pump in the valley and peak conditions (multimedia available online). (<b>a</b>) Streamline distribution in the impeller basin (left: valley condition; right: peak condition), (<b>b</b>) streamline distribution in the diffuser basin (left: valley condition; right: peak condition).</p>
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<p>Vortex core distribution inside the pump in the valley and peak conditions. (<b>a</b>) Valley condition, (<b>b</b>) peak condition.</p>
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16 pages, 6457 KiB  
Article
Intelligent Fault Diagnosis for Rotating Mechanical Systems: An Improved Multiscale Fuzzy Entropy and Support Vector Machine Algorithm
by Yuxin Pan, Yinsheng Chen, Xihong Fei, Kang Wang, Tian Fang and Jing Wang
Algorithms 2024, 17(12), 588; https://doi.org/10.3390/a17120588 - 20 Dec 2024
Viewed by 255
Abstract
Rotating mechanical systems (RMSs) are widely applied in various industrial fields. Intelligent fault diagnosis technology plays a significant role in improving the reliability and safety of industrial equipment. A new algorithm based on improved multiscale fuzzy entropy and support vector machine (IMFE-SVM) is [...] Read more.
Rotating mechanical systems (RMSs) are widely applied in various industrial fields. Intelligent fault diagnosis technology plays a significant role in improving the reliability and safety of industrial equipment. A new algorithm based on improved multiscale fuzzy entropy and support vector machine (IMFE-SVM) is proposed for the automatic diagnosis of various fault types in elevator rotating mechanical systems. First, the empirical mode decomposition (EMD) method is utilized to construct a decomposition model of the vibration data for the extraction of relevant parameters related to the fault feature. Secondly, the improved multiscale fuzzy entropy (IMFE) model is employed, where the scale factor of the multiscale fuzzy entropy (MFE) is extended to multiple subsequences to resolve the problem of insufficient coarse granularity in the traditional MFE. Subsequently, linear discriminant analysis (LDA) is applied to reduce the dimensionality of the extracted features in order to overcome the problem of feature redundancy. Finally, a support vector machine (SVM) model is utilized to construct the optimal hyperplane for the diagnosis of fault types. Experimental results indicate that the proposed method outperforms other state-of-the-art methods in the fault diagnosis of elevator systems. Full article
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<p>EMD of the signal.</p>
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<p>An improved coarse-graining method for a scale factor of 3.</p>
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<p>The design of the IMFE algorithm.</p>
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<p>Overall framework of the proposed method.</p>
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<p>The specific forms of the four signals. (<b>a</b>) <math display="inline"><semantics> <msub> <mi>x</mi> <mn>1</mn> </msub> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <msub> <mi>x</mi> <mn>2</mn> </msub> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <msub> <mi>x</mi> <mn>3</mn> </msub> </semantics></math>; (<b>d</b>) <math display="inline"><semantics> <msub> <mi>x</mi> <mn>4</mn> </msub> </semantics></math>.</p>
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<p>The results using FE, MFE, and IMFE methods for different lengths of four experimental signals.</p>
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<p>The variance and standard deviation results of entropy values for four signals at different lengths.</p>
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<p>Visualization of clustering effects of different signal features based on EMD and IMFE.</p>
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<p>Time-domain waveforms of the nine types of working fault.</p>
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<p>Detailed diagnosis results of different methods.</p>
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26 pages, 8232 KiB  
Review
3D/4D Printing in Advanced Robotics Systems—Recent Developments and Applications
by Slawomir Blasiak, Jerzy Bochnia, Jakub Takosoglu, Tomasz Kozior, Lukasz Nowakowski, Michal Skrzyniarz, Izabela Krzysztofik, Malgorzata Blasiak, Ryszard Dindorf and Piotr Wos
Sustainability 2024, 16(24), 11174; https://doi.org/10.3390/su162411174 - 20 Dec 2024
Viewed by 377
Abstract
3D/4D printing technologies are currently among the fastest growing cutting-edge fabrication technologies. The scale of their applications is vast and applicable to nearly all industries. Three-dimensional printing technologies are particularly popular in robotics and especially in advanced design innovative solutions for areas such [...] Read more.
3D/4D printing technologies are currently among the fastest growing cutting-edge fabrication technologies. The scale of their applications is vast and applicable to nearly all industries. Three-dimensional printing technologies are particularly popular in robotics and especially in advanced design innovative solutions for areas such as manufacturing, space technology, and medicine. The development of robotics, and, in particular, of the precision of manufactured components, such as actuators, pneumatic muscles, power transmission units, etc., means that new prototypes are still being made, and the use of 3D printers reduces the production time severalfold, allowing for the completion of necessary simulations and tests. In addition, the use of 3D printers allows for the production of thin-walled and cellular structures, which is a great advantage compared to conventional fabrication technologies. In the range of 3D printers available on the market, only a few selected technologies allow for actual use in the construction of advanced robot elements (muscles, vibration dampers, etc.). In an era of rapid growth in the precision of available 3D printers and modern materials, 3D printing may soon become a major tool in robotics. This article presents an overview of 3D printing technologies and materials in terms of their application in robotics and provides examples of the use of 3D and 4D printing in prototyping and fabricating robotic elements with particular emphasis on the current state of the art. The study considered the possibilities of using 3D/4D printing in robotics with the use of polymeric materials. Three-dimensional and 4D printing technologies can have a major impact on achieving sustainable development goals by providing appropriate strategies to minimise health risks and promote environmentally friendly production processes. The review of the literature and the research work currently being carried out in this area is very promising and it seems that 3D/4D printing in robotics is widely used and is still developing, which allows us to conclude that in the near future the number of research works in this field will increase rapidly. Full article
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<p>Sales of professional and personal robots.</p>
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<p>Reachy in its standard version. (<b>A</b>) Architectural diagram describing the software stack, from the high-level software interface to the motors. Dashed lines indicate the joints’ rotation axes. (<b>B</b>) Currently available end-effectors. From top to bottom: spherical, conical, hand-shaped, and articulated clamp [<a href="#B3-sustainability-16-11174" class="html-bibr">3</a>]. Note: Dashed lines indicate the joints’ rotation axes.</p>
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<p>Bolt connector and thick finger 3D model, (<b>A</b>) two test beds, (<b>B</b>) and small test bed with Nadine robot’s forearm (<b>C</b>) [<a href="#B5-sustainability-16-11174" class="html-bibr">5</a>].</p>
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<p>Synergy of fingers for performing pinch grasp [<a href="#B6-sustainability-16-11174" class="html-bibr">6</a>].</p>
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<p>(<b>A</b>) 3D transoesophageal echocardiogram of mitral valve in mid systole used to generate preliminary 3D volume. (<b>B</b>) Manually drawn mitral valve model generated from 3D volume with computer-aided design software. (<b>C</b>) Computer-aided design rendering of fillable one-piece mould and internal structure. These moulds were created for both morphologies [<a href="#B7-sustainability-16-11174" class="html-bibr">7</a>].</p>
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<p>SEM images of the indirect 4D printed microstructures: array of stent-like microstructures (<b>a</b>), acute-angle (<b>b</b>), and obtuse (<b>c</b>), the microstent strut (<b>d</b>), the acute microstent hook (<b>e</b>), and magnification of the obtuse microstent (<b>f</b>) [<a href="#B19-sustainability-16-11174" class="html-bibr">19</a>].</p>
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<p>Real snake robot (Serpens) [<a href="#B22-sustainability-16-11174" class="html-bibr">22</a>].</p>
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<p>Example 3D-printed IPMC soft crawling robot inspired by a caterpillar: (<b>a1</b>) biological caterpillar showing body and leg segments that were modelled in the design of the crawling robot; (<b>a2</b>) assembled robot with two legs and two body sections, with electrical connections; (<b>b1</b>) back leg actuator closing and front leg actuator opening while body is contracted; (<b>b2</b>) extension of body actuators while back leg actuator is closed and front leg actuator is open propelling the robot forward; (<b>b3</b>) back leg actuator opening and front leg actuator closing while body is extended; (<b>b4</b>) contraction of body actuators while back leg actuator is open and front leg actuator is closed drawing up the back of the robot [<a href="#B28-sustainability-16-11174" class="html-bibr">28</a>].</p>
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<p>Three-dimensional model and stl recording: (<b>a</b>) CAD, (<b>b</b>) coarse–stl Ld–0.01, Ad–30 degrees, (<b>c</b>) fine–stl Ld–0.006, Ad–10 degrees, (<b>d</b>) adjusted–stl Ld–0.001, Ad–5 degrees.</p>
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<p>Complex search results for 3D printing, additive technology, and robotics.</p>
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<p>Number of search results for particular issues, divided into scientific categories: (<b>a</b>) 3D printing, (<b>b</b>) additive technology, (<b>c</b>) robotics.</p>
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<p>Number of search results for particular issues, divided into scientific categories: (<b>a</b>) 3D printing, (<b>b</b>) additive technology, (<b>c</b>) robotics.</p>
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<p>Prototype of the electric motor housing: (<b>a</b>) view on the build platform, (<b>b</b>) view after installation [own source].</p>
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<p>Prototype of the electric motor housing with engine printed in SLS technology: (<b>a</b>) Impuls Mars Rover, (<b>b</b>) motor housing [own source].</p>
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<p>A hand exoskeleton for rehabilitation [<a href="#B89-sustainability-16-11174" class="html-bibr">89</a>].</p>
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19 pages, 5980 KiB  
Article
Study on the Transient Extraction Transform Algorithm for Defect Detection in Welded Plates Based on Laser Vibrometer
by Yu Du, Xinke Xu, Longbiao Zhao, Dijian Yuan and Jinwen Wang
Photonics 2024, 11(12), 1193; https://doi.org/10.3390/photonics11121193 - 19 Dec 2024
Viewed by 347
Abstract
This paper addresses the issue of detecting welding defects in steel plates during the welding process by proposing a method that combines the laser vibrometer with transient feature extraction technology. The method employs a high-resolution laser vibrometer to collect vibration signals from excited [...] Read more.
This paper addresses the issue of detecting welding defects in steel plates during the welding process by proposing a method that combines the laser vibrometer with transient feature extraction technology. The method employs a high-resolution laser vibrometer to collect vibration signals from excited weld plates, followed by feature extraction and analysis for defect detection and identification. The focus of the research is on the optimization and application of the transient extraction transform algorithm, which plays a crucial role in signal feature extraction for defect recognition. By optimizing the short-time Fourier transform, we further propose the use of the transient extraction transform algorithm to effectively characterize and extract transient components from defect signals. To validate the proposed algorithm, we compare the defect recognition performance of several algorithms using quantitative metrics such as Rényi entropy and kurtosis. The results indicate that the proposed method yields a more centralized time–frequency representation and significantly increases the kurtosis of transient components, providing a new approach for detecting welding defects in steel plates. Full article
(This article belongs to the Special Issue Advances and Applications of Laser Measurements)
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<p>Schematic diagram of the laser vibrometer.</p>
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<p>Preparation and defect classification of experimental welded plates.</p>
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<p>(<b>a</b>) Signal time-domain diagram; (<b>b</b>) STFT transformation result; (<b>c</b>) WT transformation result.</p>
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<p>Simulation results under the ideal model based on the Dirac function: (<b>a</b>) dirac function signal at <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math> s; (<b>b</b>) spectrum; (<b>c</b>) STFT spectrogram; (<b>d</b>) slice of the spectrogram at <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>50</mn> </mrow> </semantics></math> Hz, i.e., <math display="inline"><semantics> <mrow> <mfenced close="|" open="|"> <mrow> <mi>G</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <msub> <mi>ω</mi> <mn>0</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mfenced> </mrow> </semantics></math>; (<b>e</b>) GD <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mn>0</mn> </msub> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>; (<b>f</b>) slice of the GD at <math display="inline"><semantics> <mrow> <msub> <mi>ω</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>50</mn> </mrow> </semantics></math> Hz, i.e., <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mn>0</mn> </msub> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>; (<b>g</b>) TEO; and (<b>h</b>) results of the TET Test.</p>
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<p>Digital signals and scaling for TET representation.</p>
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<p>Preparation and defect classification of experimental welded plates.</p>
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<p>Vibrometer measurement field calibration chart.</p>
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<p>Comparison of WT transformation results: (<b>a</b>) normal plate; (<b>b</b>) the plate containing arc pit defects; and (<b>c</b>) the plate containing porous defects.</p>
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<p>Comparison of signal processing at the same location across different plates: (<b>a</b>) time-domain signal; (<b>b</b>) STFT transformation results.</p>
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<p>(<b>a</b>) Normal ban111 waveform; (<b>b</b>) STFT results; (<b>c</b>) TET results; (<b>d</b>) WT results; (<b>e</b>) SST results.</p>
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<p>Rényi entropy of TF results obtained by different TFA methods at different noise levels (S/N ratios of 1–30 dB).</p>
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<p>Kurtosis at different noise levels (signal-to-noise ratio of 1–30 dB).</p>
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<p>(<b>a</b>) Raw signal; (<b>b</b>) transient component extraction using the TET method.</p>
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<p>STFT effect diagram: (<b>a</b>) ban121; (<b>b</b>) ban221; (<b>c</b>) ban331; (<b>d</b>) ban431; and (<b>e</b>) ban641.</p>
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<p>TET effect diagram: (<b>a</b>) ban121; (<b>b</b>) ban221; (<b>c</b>) ban331; (<b>d</b>) ban431; and (<b>e</b>) ban641.</p>
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18 pages, 9492 KiB  
Article
Noise Reduction in CWRU Data Using DAE and Classification with ViT
by Jun-gyo Jang, Soon-sup Lee, Se-yun Hwang and Jae-chul Lee
Appl. Sci. 2024, 14(24), 11771; https://doi.org/10.3390/app142411771 - 17 Dec 2024
Viewed by 290
Abstract
With the Fourth Industrial Revolution unfolding worldwide, technologies including the Internet of Things, sensors, and artificial intelligence are undergoing rapid development. These technological advancements have played a significant role in the dramatic growth of the predictive maintenance market for mechanical equipment, prompting active [...] Read more.
With the Fourth Industrial Revolution unfolding worldwide, technologies including the Internet of Things, sensors, and artificial intelligence are undergoing rapid development. These technological advancements have played a significant role in the dramatic growth of the predictive maintenance market for mechanical equipment, prompting active research on noise removal techniques and classification algorithms for the accurate determination of the causes of equipment failure. In this study, time series data were preprocessed using the denoising autoencoder technique, a deep learning-based noise removal method, to improve the accuracy of failure classification from mechanical equipment data. To convert the preprocessed time series data into frequency components, the short-time Fourier transform technique was employed. The fault types of mechanical equipment were classified using the vision transformer (ViT) technique, a deep learning technique that has been actively used in recent image analysis research. Additionally, the classification performance of the ViT-based technique for vibration time series data was comparatively validated against existing classification algorithms. The accuracy of failure classification was the highest when the data, preprocessed using a Denoising Autoencoder (DAE), were classified by a Vision Transformer (ViT). Full article
(This article belongs to the Section Applied Industrial Technologies)
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<p>The importance of data preprocessing.</p>
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<p>Research flowchart.</p>
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<p>Short−time Fourier transform theory.</p>
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<p>Result of STFT ((<b>a</b>) normal; (<b>b</b>) ball; (<b>c</b>) inner; (<b>d</b>) outer).</p>
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<p>Learning method of the Denoising Autoencoder.</p>
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<p>Image division for ViT learning.</p>
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<p>Structure of the vision transformer (* New learnable parameters) [<a href="#B31-applsci-14-11771" class="html-bibr">31</a>].</p>
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<p>Experiment device [<a href="#B34-applsci-14-11771" class="html-bibr">34</a>].</p>
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<p>DAE model structure.</p>
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<p>Result of normal data ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>Result of ball fault data ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>Result of inner-race data ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>Result of outer-race data ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>Result of normal-data STFT ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>Result of ball-fault-data STFT ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>Result of inner-race-data STFT ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>Result of outer-race-data STFT ((<b>a</b>) raw data; (<b>b</b>) DAE data).</p>
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<p>The result of classifying raw data by applying it to ViT.</p>
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<p>The result of classification by applying DAE data to ViT.</p>
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<p>Configuring data for K-fold cross-validation.</p>
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<p>Classification result based on CNN—1.</p>
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<p>Classification result based on CNN—2 ((<b>a</b>) CNN channel-wise accuracy; (<b>b</b>) confusion matrix of 3 Channel CNN).</p>
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17 pages, 325 KiB  
Review
Diagnosis, Pathophysiology and Management of Microvascular Dysfunction in Diabetes Mellitus
by Yih-Kuen Jan, Nicolas Kelhofer, Tony Tu, Owaise Mansuri, Kingsley Onyemere, Shruti Dave and Suguna Pappu
Diagnostics 2024, 14(24), 2830; https://doi.org/10.3390/diagnostics14242830 - 16 Dec 2024
Viewed by 363
Abstract
Microcirculation is an essential system that regulates oxygen and nutrients to cells and tissues in response to various environmental stimuli and pathophysiological conditions. Diabetes mellitus can cause microvascular complications including nephropathy, neuropathy, and retinopathy. The pathogenesis of microvascular dysfunction in diabetes is associated [...] Read more.
Microcirculation is an essential system that regulates oxygen and nutrients to cells and tissues in response to various environmental stimuli and pathophysiological conditions. Diabetes mellitus can cause microvascular complications including nephropathy, neuropathy, and retinopathy. The pathogenesis of microvascular dysfunction in diabetes is associated with hyperglycemia and the result of an interplay of various factors. Research studies have demonstrated that functional microvascular dysfunction appears much earlier than structural alterations in vasculature in diabetes. This finding of the progression from microvascular dysfunction to macrovascular disease establishes a foundation for the screening and early diagnosis of diabetes by assessing the microvascular function. This comprehensive review discusses technologies (laser Doppler, transcutaneous oximetry, infrared thermography and near-infrared spectroscopy) with computational methods (linear (time and frequency domains), nonlinear and machine learning approaches) for diagnosing microvascular dysfunction in diabetes. Pathophysiological changes of microvascular dysfunction leading to impaired vasomotion and blood flow oscillations in diabetes are reviewed. Recent findings in managing microvascular dysfunction using lifestyle modifications and force-based modulations are evaluated. A consensus endorsed by the American Diabetes Association has been reached that an effective exercise program would greatly slow down the progression of microvascular dysfunction and its impact on diabetic foot ulcers, muscle fatigue and weakness and peripheral neuropathy. However, it is imperative to determine the dose–response relationship of exercise and microvascular responses in patients with diabetes. Research studies have demonstrated that local vibration and whole-body vibration can improve microcirculation in various pathological conditions, including diabetes. Due to the complex nature of microvascular regulation, various computational methods have been developed to shed light on the influence of diabetes on microvascular dysfunction. This comprehensive review will contribute to the diagnosis and management of microvascular dysfunction in diabetes. Full article
(This article belongs to the Special Issue Vascular Malformations: Diagnosis and Management)
15 pages, 8380 KiB  
Article
Design and Analysis of a Low Torque Ripple Permanent Magnet Synchronous Machine for Flywheel Energy Storage Systems
by Yubo Sun, Zhenghui Zhao and Qian Zhang
Energies 2024, 17(24), 6337; https://doi.org/10.3390/en17246337 - 16 Dec 2024
Viewed by 381
Abstract
Flywheel energy storage systems (FESS) are technologies that use a rotating flywheel to store and release energy. Permanent magnet synchronous machines (PMSMs) are commonly used in FESS due to their high torque and power densities. One of the critical requirements for PMSMs in [...] Read more.
Flywheel energy storage systems (FESS) are technologies that use a rotating flywheel to store and release energy. Permanent magnet synchronous machines (PMSMs) are commonly used in FESS due to their high torque and power densities. One of the critical requirements for PMSMs in FESS is low torque ripple. Therefore, a PMSM with eccentric permanent magnets is proposed and analyzed in this article to reduce torque ripple. Cogging torque, a significant contributor to torque ripple, is investigated by a combination of finite element analysis and the analytical method. An integer-slot distribution winding structure is adopted to reduce vibration and noise. Moreover, the effects of eccentric permanent magnets and harmonic injection on the cogging torque are analyzed and compared. In addition, the electromagnetic performance is analyzed, and the torque ripple is found to be 3.1%. Finally, a prototype is built and tested, yielding a torque ripple of 3.9%, to verify the theoretical analysis. Full article
(This article belongs to the Special Issue Energy, Electrical and Power Engineering: 3rd Edition)
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<p>Topology of proposed PMSM.</p>
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<p>Winding connection.</p>
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<p>Analysis model of surface-mounted PMSM.</p>
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<p>Bread-type eccentric permanent magnet.</p>
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<p>Influence of eccentricity on torque performance.</p>
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<p>Cogging torque of PMSM with different permanent magnets.</p>
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<p>Air gap magnetic densities of PMSM with different permanent magnets. (<b>a</b>) Radial air gap magnetic densities. (<b>b</b>) Tangential air gap magnetic densities. (<b>c</b>) Harmonic order.</p>
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<p>Cogging torque contribution of different harmonics. (<b>a</b>) PMSM with original permanent magnets. (<b>b</b>) PMSM with eccentric permanent magnets.</p>
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<p>Permanent magnet with third harmonic injection.</p>
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<p>Cogging torque of PMSM with harmonic injection. (<b>a</b>) Effect of harmonic injection. (<b>b</b>) Contribution of harmonics.</p>
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<p>Load electromagnetic performance. (<b>a</b>) Magnetic field line. (<b>b</b>) Magnetic flux density.</p>
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<p>Back electromotive force of PMSM.</p>
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<p>Torque performance of PMSM. (<b>a</b>) Cogging torque. (<b>b</b>) Torque.</p>
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<p>Vibration acceleration of PMSM with different permanent magnets.</p>
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<p>Prototype.</p>
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<p>Experimental platform.</p>
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<p>Vibration and noise test platform.</p>
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<p>Comparison of experimental and simulated results. (<b>a</b>) Back electromotive force of prototype. (<b>b</b>) Comparison of back electromotive force coefficient.</p>
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<p>Experimental results. (<b>a</b>) Torque. (<b>b</b>) Vibration acceleration.</p>
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20 pages, 5421 KiB  
Article
A Miniaturized and Ultra-Low-Power Wireless Multi-Parameter Monitoring System with Self-Powered Ability for Aircraft Smart Skin
by Chongqi Wang, Yu Wang, Wei Pu and Lei Qiu
Sensors 2024, 24(24), 7993; https://doi.org/10.3390/s24247993 - 14 Dec 2024
Viewed by 301
Abstract
The aircraft smart skin (ASS) with structural health monitoring capabilities is a promising technology. It enables the real-time acquisition of the aircraft’s structural health status and service environment, thereby improving the performance of the aircraft and ensuring the safety of its operation, which [...] Read more.
The aircraft smart skin (ASS) with structural health monitoring capabilities is a promising technology. It enables the real-time acquisition of the aircraft’s structural health status and service environment, thereby improving the performance of the aircraft and ensuring the safety of its operation, which in turn reduces maintenance costs. In this paper, a miniaturized and ultra-low-power wireless multi-parameter monitoring system (WMPMS) for ASS is developed, which is capable of monitoring multiple parameters of an aircraft, including random impact events, vibration, temperature, humidity, and air pressure. The system adopts an all-digital monitoring method and a low-power operating mechanism, and it is integrated into a low-power hardware design. In addition, considering the airborne resources limitations, an energy self-supply module based on a thermoelectric generator (TEG) is developed to continuously power the system during flight. Based on the above design, the system has a size of only 45 mm × 50 mm × 30 mm and an average power consumption of just 7.59 mW. Through experimental validation, the system has excellent performance in multi-parameter monitoring and operating power consumption, and it can realize the self-supply of energy. Full article
(This article belongs to the Section Fault Diagnosis & Sensors)
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<p>Architecture of ASS-based multi-parameter monitoring of an aircraft.</p>
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<p>Basic principle of the digital sequence-based impact region localization method.</p>
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<p>Overall hardware architecture of the WMPMS.</p>
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<p>The developed WMPMS.</p>
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<p>Software architecture of the system.</p>
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<p>The thermoelectric conversion unit.</p>
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<p>Experimental setup of impact monitoring.</p>
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<p>Example of impact monitoring: (<b>a</b>) impact occurring in region 1; (<b>b</b>) digital sequences.</p>
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<p>Experimental setup of environmental monitoring verification.</p>
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<p>Vibration monitoring results: (<b>a</b>) WMPMS; (<b>b</b>) accelerometer.</p>
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<p>Temperature monitoring results.</p>
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<p>Humidity monitoring results.</p>
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<p>Air pressure monitoring results.</p>
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<p>Schematic diagram of the energy self-supply verification setup.</p>
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<p>Physical diagram of the energy self-supply verification setup.</p>
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<p>Verification results of the thermoelectric generator.</p>
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<p>Energy recovery results.</p>
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<p>Multi-parameter monitoring of the composite UAV wing.</p>
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<p>PZT placement on the impact monitoring regions.</p>
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22 pages, 3758 KiB  
Review
Laser Cladding In Situ Carbide-Reinforced Iron-Based Alloy Coating: A Review
by Junli Tang, Kaiming Wang and Hanguang Fu
Metals 2024, 14(12), 1419; https://doi.org/10.3390/met14121419 - 11 Dec 2024
Viewed by 449
Abstract
Laser cladding, as an advanced surface modification technology, has the advantages of a high energy density, controlled dilution rate and good metallurgical bonding between the coating and the substrate. Its rapid heating and cooling properties help to form a dense and fine coating [...] Read more.
Laser cladding, as an advanced surface modification technology, has the advantages of a high energy density, controlled dilution rate and good metallurgical bonding between the coating and the substrate. Its rapid heating and cooling properties help to form a dense and fine coating structure on the surface of the substrate, thus enhancing wear and corrosion resistance. In recent years, the in situ generation of carbide-reinforced iron-based composite coatings has gradually become a research hotspot because it combines the high hardness values of carbide with the high toughness values of iron-based alloys, which significantly improves the comprehensive performance of the coatings. This paper reviews the research progress of laser cladding in situ carbide-reinforced iron-based alloy coatings and explores the role of different types of in situ synthesized carbides (TiC, NbC, WC, etc.) in the coatings and their effects on their wear resistance and mechanical properties. The distribution of carbides in the coatings and their morphological characteristics are also discussed, and the effects of laser power, scanning speed and auxiliary treatments (ultrasonic vibration, induction heating, etc.) on the microstructure and properties of the coatings are analyzed. Finally, the problems and future directions of development in this field are envisioned. Full article
(This article belongs to the Special Issue Laser Additive Manufacturing of Alloys)
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<p>Laser cladding process. (<b>a</b>) Components of the laser cladding system; (<b>b</b>) Melt pool reaction. Reprinted from Ref. [<a href="#B10-metals-14-01419" class="html-bibr">10</a>].</p>
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<p>The effect of varying nano-WC contents on the wear rate of Fe-based coatings. Reprinted from Ref. [<a href="#B13-metals-14-01419" class="html-bibr">13</a>].</p>
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<p>SEM cross-sectional images of in situ synthesized 316L stainless steel reinforced with different TiC contents: (<b>a</b>) 3.6% TiC; (<b>b</b>) 3.6% TiC; (<b>c</b>) 3.6% TiC. Reprinted with permission from Ref. [<a href="#B18-metals-14-01419" class="html-bibr">18</a>]. Copyright 2024 Elsevier.</p>
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<p>Mechanism of in situ synthesized WC in iron-based alloys: (<b>a</b>) above 1340 °C; (<b>b</b>) 1340 °C; (<b>c</b>) 1190 °C; (<b>d</b>) 640 °C; (<b>e</b>) 600 °C; (<b>f</b>) 450 °C. Reprinted with permission from Ref. [<a href="#B22-metals-14-01419" class="html-bibr">22</a>]. Copyright 2024 TRIBOLOGY.</p>
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<p>Phase evolution process of in situ synthesized NbC: (<b>a</b>) Phase distribution of the Fe-based coating, (<b>b</b>) Phase distribution of the composite coating. Reprinted with permission from Ref. [<a href="#B26-metals-14-01419" class="html-bibr">26</a>]. Copyright 2024 Elsevier.</p>
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<p>Variation in microhardness of coatings along the depth direction at different CeO<sub>2</sub> contents. Reprinted with permission from Ref. [<a href="#B40-metals-14-01419" class="html-bibr">40</a>]. Copyright 2024 Elsevier.</p>
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<p>Effect of process parameters on clad height (<b>H</b>): (<b>a</b>) variation in H with shielding gas flow rate (G) at different scanning speeds (v); (<b>b</b>) variation in H with v at different laser power values (P); (<b>c</b>) variation in H with P at different G values. Reprinted with permission from Ref. [<a href="#B41-metals-14-01419" class="html-bibr">41</a>]. Copyright 2024 Elsevier.</p>
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<p>Pareto front solution set under different process parameters. Reprinted with permission from Ref. [<a href="#B45-metals-14-01419" class="html-bibr">45</a>]. Copyright 2024 Elsevier.</p>
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<p>Size and distribution of enhanced phases of coatings at different ultrasonic vibration powers: (<b>a</b>) 0 W; (<b>b</b>) 100 W; (<b>c</b>) 200 W; (<b>d</b>) 300 W. Reprinted with permission from Ref. [<a href="#B53-metals-14-01419" class="html-bibr">53</a>]. Copyright 2024 Elsevier.</p>
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<p>Thermal imaging photograph of the molten pool taken by an infrared camera. (<b>a</b>) Using an induction heater; (<b>b</b>) Without using an induction heater. Reprinted with permission from Ref. [<a href="#B57-metals-14-01419" class="html-bibr">57</a>]. Copyright 2024 Elsevier.</p>
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36 pages, 7199 KiB  
Review
Electric Vehicle Battery Technologies: Chemistry, Architectures, Safety, and Management Systems
by Dmitrii K. Grebtsov, Mikhail K. Kubasov, Egor R. Bernatskii, Pavel A. Beliauski, Andrey A. Kokorenko, Shakhboz Sh. Isokjanov, Sergey P. Kazikov, Alexey M. Kashin, Daniil M. Itkis and Sofia M. Morozova
World Electr. Veh. J. 2024, 15(12), 568; https://doi.org/10.3390/wevj15120568 - 10 Dec 2024
Viewed by 1352
Abstract
Electric and hybrid vehicles have become widespread in large cities due to the desire for environmentally friendly technologies, reduction of greenhouse gas emissions and fuel, and economic advantages over gasoline and diesel vehicles. In electric vehicles, overheating, vibration, or mechanical damage due to [...] Read more.
Electric and hybrid vehicles have become widespread in large cities due to the desire for environmentally friendly technologies, reduction of greenhouse gas emissions and fuel, and economic advantages over gasoline and diesel vehicles. In electric vehicles, overheating, vibration, or mechanical damage due to collision with an object or another vehicle can lead to the failure of lithium-ion batteries up to thermal runaway and fire. Therefore, the development of battery safety control systems is one of the most important factors contributing to the large-scale electrification of public and private transport. This review examines the design features of the location and management of the battery pack to achieve maximum safety and operational efficiency when using an electric vehicle. The power characteristics and life-cycles of various types of lithium-ion batteries depending on the chemical nature of their electrodes are considered, using the example of commercial vehicles’—Tesla, Nissan Leaf, Porsche Taycan, Zeekr, and Chevrolet Volt—strategic technologies for the placement and packaging of batteries, and battery cooling and monitoring systems (State of Health and State of Charge) are also discussed. In conclusion, the current challenges in the field are summarized and promising research directions are proposed. Full article
(This article belongs to the Special Issue Intelligent Electric Vehicle Control, Testing and Evaluation)
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Graphical abstract
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<p>Crystallographic structure and electrochemical reaction for three main types of cathode materials for EVs: (<b>a</b>) LFP; (<b>b</b>) NMC; (<b>c</b>) NCA. (1) The process of lithium extraction in the cathode; (2) the process of lithium insertion into graphite planes at the anode; (3) the general intercalation/deintercalation reaction occurring in the battery cell (image produced using VESTA [<a href="#B25-wevj-15-00568" class="html-bibr">25</a>]).</p>
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<p>Components of EV batteries.</p>
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<p>The form factor of batteries, their features, and applications.</p>
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<p>“Floor” and “T-Shape” arrangement of modules in an electric vehicle.</p>
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<p>Diagram of the number of new electric vehicle models according to the form factors of the cells used (data up to 2021 are adapted with permission from Ref. [<a href="#B87-wevj-15-00568" class="html-bibr">87</a>]; data of 2022–2023 are based on this work).</p>
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<p>Various EVB architectures.</p>
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<p>Scheme of BMS main components architecture.</p>
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<p>Classification of methods for assessing the state of charge, SOC.</p>
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<p>The principle of operation of adaptive filters for SOC estimation (adapted with permission from Ref. [<a href="#B108-wevj-15-00568" class="html-bibr">108</a>], Copyright 2018 Elsevier).</p>
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<p>Methods for assessing the degree of degradation of LIBs.</p>
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<p>Classification of battery thermal management systems (adapted with permission from Ref. [<a href="#B127-wevj-15-00568" class="html-bibr">127</a>], Copyright 2018 Elsevier).</p>
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<p>(<b>a</b>) Schematic of battery module using the air distribution pipe (adapted with permission from Ref. [<a href="#B139-wevj-15-00568" class="html-bibr">139</a>] Copyright 2019 Elsevier). (<b>b</b>) Three-dimensional view of the parallel air-cooled BTMS with U-type flow (adapted with permission from Ref. [<a href="#B140-wevj-15-00568" class="html-bibr">140</a>]). (<b>c</b>) J-type cooling channel (combined Z-type and U-type) (adapted with permission from Ref. [<a href="#B141-wevj-15-00568" class="html-bibr">141</a>] Copyright 2019 Elsevier).</p>
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<p>Scheme of single-phase (<b>a</b>) and two-phase (<b>b</b>) immersion cooling for LIBs (adapted with permission from Ref. [<a href="#B134-wevj-15-00568" class="html-bibr">134</a>] Copyright 2024 Elsevier).</p>
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<p>(<b>a</b>) LIB by Xing. (<b>b</b>) LIB by Kreisel.</p>
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<p>(<b>a</b>) Dimensions and structure of mini-channel cooling plate (adapted with permission from Ref. [<a href="#B149-wevj-15-00568" class="html-bibr">149</a>] Copyright 2021 Elsevier). (<b>b</b>) Cooling plates with microchannel slots (adapted with permission from Ref. [<a href="#B150-wevj-15-00568" class="html-bibr">150</a>] Copyright 2021 Elsevier). (<b>c</b>) Cooling pipes in Tesla Model S (adapted with permission from Ref. [<a href="#B138-wevj-15-00568" class="html-bibr">138</a>]).</p>
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<p>(<b>a</b>) Scheme of the heat pipe device (adapted with permission from Ref. [<a href="#B161-wevj-15-00568" class="html-bibr">161</a>]). (<b>b</b>) Scheme of the cooling system based thermoelectric converter with copper plates. (<b>c</b>) Scheme of the cooling system based thermoelectric converter with aluminum.</p>
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<p>(<b>a</b>) The scheme with zigzag cooling channels and PCM (adapted with permission from Ref. [<a href="#B172-wevj-15-00568" class="html-bibr">172</a>]). (<b>b</b>) Microchannel cooling plate with PCM elements (adapted with permission from Ref. [<a href="#B173-wevj-15-00568" class="html-bibr">173</a>]). (<b>c</b>) Scheme with side cooling plates and PCM (adapted with permission from Ref. [<a href="#B131-wevj-15-00568" class="html-bibr">131</a>] Copyright 2021 Elsevier).</p>
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48 pages, 6986 KiB  
Review
Fluid Flow-Based Vibration Energy Harvesters: A Critical Review of State-of-the-Art Technologies
by Sadia Bakhtiar, Farid Ullah Khan, Hailing Fu, Amal Z. Hajjaj and Stephanos Theodossiades
Appl. Sci. 2024, 14(23), 11452; https://doi.org/10.3390/app142311452 - 9 Dec 2024
Viewed by 1109
Abstract
Energy harvesting technology plays an important role in converting ambient energy into useful electrical energy to power wireless sensing and system monitoring, especially for systems operating in isolated, abandoned or embedded locations where battery replacement or recharging is not a feasible solution. This [...] Read more.
Energy harvesting technology plays an important role in converting ambient energy into useful electrical energy to power wireless sensing and system monitoring, especially for systems operating in isolated, abandoned or embedded locations where battery replacement or recharging is not a feasible solution. This paper provides an integrative study of the methodologies and technologies of energy harvesting from fluid flow-induced vibration (FIV). The recent research endeavors contributing to flow-based energy harvesting have been reviewed to present the state-of-the-art issues and challenges. Several mechanisms on FIVs including vortex-induced vibrations (VIVs), flutter, galloping and wake galloping are thoroughly discussed in terms of device architecture, operating principles, energy transduction, voltage production and power generation. Additionally, advantages and disadvantages of each FIV energy harvesting mechanism are also talked about. Power enhancement methods, such as induced nonlinearities, optimized harvester’s configuration, hybridization and coupling of aerodynamic instabilities, for boosting the harvester’s output are also elucidated and categorized. Moreover, rotary wind energy harvesters are reviewed and discussed. Finally, the challenges and potential directions related to the flow-based energy harvesters (FBEHs) are also mentioned to provide an insight to researchers on the development of sustainable energy solutions for remote wireless sensing and monitoring systems. Full article
(This article belongs to the Section Mechanical Engineering)
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<p>Potential energy sources for FIV-based harvesting for powering WSNs in IoT applications.</p>
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<p>Schematic of coupling between fluid, structure and energy transduction in FBEHs.</p>
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<p>Typical trend of VIVs: (<b>a</b>) synchronization region; (<b>b</b>) Karman vortex street.</p>
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<p>Karman vortex street-based PE-FBEHs. (<b>a</b>) Schematic of energy harvesting from von Karman vortices in airflow [<a href="#B43-applsci-14-11452" class="html-bibr">43</a>]; (<b>b</b>) Direction-adaptive EH with a guide wing reproduced with permission from [<a href="#B47-applsci-14-11452" class="html-bibr">47</a>], Elsevier, 2019; (<b>c</b>) VIV energy harvester reproduced with permission from [<a href="#B48-applsci-14-11452" class="html-bibr">48</a>], Elsevier, 2018; (<b>d</b>) Schematic of VIV micro windmill with three blades reproduced with permission from [<a href="#B49-applsci-14-11452" class="html-bibr">49</a>], Elsevier, 2022.</p>
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<p>VIV-TEEHs: (<b>a</b>) TEEH with springs reproduced with permission from [<a href="#B59-applsci-14-11452" class="html-bibr">59</a>] Elsevier, 2022; (<b>b</b>) Hydrokinetic TEEH reproduced with permission from [<a href="#B61-applsci-14-11452" class="html-bibr">61</a>] Elsevier, 2023; (<b>c</b>) Y-shaped/flag-type TEEH reproduced with permission from [<a href="#B62-applsci-14-11452" class="html-bibr">62</a>] Elsevier, 2024; (<b>d</b>) Vortex-induced rolling TEEH reproduced with permission from [<a href="#B63-applsci-14-11452" class="html-bibr">63</a>] Elsevier, 2024.</p>
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<p>(<b>a</b>) Typical trend of a galloping flow energy harvester; galloping-based PE-FBEHs with different shaped bluff bodies: (<b>b</b>) bulb-like cross-sectional reproduced with permission from [<a href="#B77-applsci-14-11452" class="html-bibr">77</a>] Elsevier, 2019; (<b>c</b>) fork-shaped reproduced with permission from [<a href="#B75-applsci-14-11452" class="html-bibr">75</a>] Elsevier, 2019; (<b>d</b>) cut-corner prism reproduced with permission from [<a href="#B84-applsci-14-11452" class="html-bibr">84</a>] Elsevier, 2021; (<b>e</b>) hyper-structure corrugated [<a href="#B86-applsci-14-11452" class="html-bibr">86</a>]; (<b>f</b>) double-airfoil reproduced with permission from [<a href="#B88-applsci-14-11452" class="html-bibr">88</a>] Elsevier, 2023; (<b>g</b>) tri-section beam and square body with splitters [<a href="#B91-applsci-14-11452" class="html-bibr">91</a>].</p>
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<p>Galloping EM-FBEHs: (<b>a</b>) Halbach effect EH reproduced with permission from [<a href="#B93-applsci-14-11452" class="html-bibr">93</a>] Elsevier, 2019; (<b>b</b>) spring-coupling EH [<a href="#B94-applsci-14-11452" class="html-bibr">94</a>]; (<b>c</b>) (i) torsional galloping EH, (ii) modified design with beam elements reproduced with permission from [<a href="#B95-applsci-14-11452" class="html-bibr">95</a>] Elsevier, 2023; (<b>d</b>) elastic strips suspended EH reproduced with permission from [<a href="#B96-applsci-14-11452" class="html-bibr">96</a>] Elsevier, 2024.</p>
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<p>Piezoelectric flag tested with various bluff bodies reproduced with permission from [<a href="#B112-applsci-14-11452" class="html-bibr">112</a>] Elsevier, 2023.</p>
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<p>Flutter EM-FBEHs. (<b>a</b>) Cantilever-based EMEH [<a href="#B118-applsci-14-11452" class="html-bibr">118</a>]. (<b>b</b>) Design of wind belt EMEH reproduced with permission from [<a href="#B115-applsci-14-11452" class="html-bibr">115</a>] Elsevier, 2016.</p>
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<p>Bio-inspired FEHs: (<b>a</b>) wing-stimulated TEEH [<a href="#B130-applsci-14-11452" class="html-bibr">130</a>]; (<b>b</b>) PEH with MFC layers reproduced with permission from [<a href="#B133-applsci-14-11452" class="html-bibr">133</a>] Elsevier, 2020.</p>
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<p>(<b>a</b>) Illustration of wake galloping phenomenon reproduced with permission from [<a href="#B136-applsci-14-11452" class="html-bibr">136</a>] Elsevier, 2016. (<b>b</b>) Characteristic response of wake galloping EH. (<b>c</b>) Wake galloping with different interference cylinder cross-sections reproduced with permission from [<a href="#B144-applsci-14-11452" class="html-bibr">144</a>] Elsevier, 2019. (<b>d</b>) Schematic of iced-conductor-inspired wake galloping reproduced with permission from [<a href="#B146-applsci-14-11452" class="html-bibr">146</a>] Elsevier, 2020.</p>
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<p>Nonlinear PE-FEHs: (<b>a</b>) VIV piezo-magneto-elastic EH reproduced with permission from [<a href="#B153-applsci-14-11452" class="html-bibr">153</a>] Elsevier, 2017. (<b>b</b>) Self tunable airfoil EH [<a href="#B157-applsci-14-11452" class="html-bibr">157</a>]. (<b>c</b>) VIV-EH with nonlinear stiffness reproduced with permission from [<a href="#B159-applsci-14-11452" class="html-bibr">159</a>] Elsevier, 2024. (<b>d</b>) Y-shaped bistable PEH reproduced with permission from [<a href="#B162-applsci-14-11452" class="html-bibr">162</a>] Elsevier, 2018. (<b>e</b>) Galloping-based moving bluff body reproduced with permission from [<a href="#B166-applsci-14-11452" class="html-bibr">166</a>] Elsevier, 2021. (<b>f</b>) Tristable flutter-based PEH reproduced with permission from [<a href="#B181-applsci-14-11452" class="html-bibr">181</a>] Elsevier, 2024.</p>
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<p>Coupled fluid flow phenomena in FEHs: (<b>a</b>) circular-based PEH with attachments (circular, triangular, and square) reproduced with permission from [<a href="#B193-applsci-14-11452" class="html-bibr">193</a>] Elsevier, 2018; (<b>b</b>) interaction between VIV and galloping in FEH reproduced with permission from [<a href="#B77-applsci-14-11452" class="html-bibr">77</a>] Elsevier, 2019; (<b>c</b>) VIV and galloping PEH reproduced with permission from [<a href="#B196-applsci-14-11452" class="html-bibr">196</a>] Elsevier, 2019; (<b>d</b>) dumbbell-shaped bluff body for FEH reproduced with permission from [<a href="#B198-applsci-14-11452" class="html-bibr">198</a>] Elsevier, 2024; (<b>e</b>) cylindrical bluff body in FEH with two symmetrical airfoils [<a href="#B203-applsci-14-11452" class="html-bibr">203</a>].</p>
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<p>Rotary wind EHs: (<b>a</b>) TE-PE energy harvester reproduced with permission from [<a href="#B206-applsci-14-11452" class="html-bibr">206</a>] Elsevier, 2017; (<b>b</b>) TE-EM energy harvester reproduced with permission from [<a href="#B207-applsci-14-11452" class="html-bibr">207</a>] Elsevier, 2020; (<b>c</b>) PE-EM-TE-based RWEH reproduced with permission from [<a href="#B209-applsci-14-11452" class="html-bibr">209</a>] Elsevier 2022; (<b>d</b>) orientation adaptive EM-based RWEH reproduced with permission from [<a href="#B212-applsci-14-11452" class="html-bibr">212</a>] Elsevier 2024.</p>
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16 pages, 3898 KiB  
Article
The Influence of Changing Belt Loading Conditions on the Operational Condition of the Belt Transmission
by Jozef Mascenik and Tomas Coranic
Actuators 2024, 13(12), 506; https://doi.org/10.3390/act13120506 - 8 Dec 2024
Viewed by 460
Abstract
Given the fact that belt drives are used to transmit power to a fairly large extent, it is natural to devote scientific attention to their transmission with an effort to contribute to the constant technical and technological progress in the field of belt [...] Read more.
Given the fact that belt drives are used to transmit power to a fairly large extent, it is natural to devote scientific attention to their transmission with an effort to contribute to the constant technical and technological progress in the field of belt production and use. For testing and monitoring belt drives, a measuring system was designed and manufactured, which allowed the installation of various types of belt drives and, under a controlled load, to monitor selected parameters and the behavior of individual transmission elements. The presented contribution presents both the measuring system itself and experimental measurements on three V-belts of the same size manufactured by three different manufacturers. During the experimental measurements, parameters such as belt tension were changed by changing the axial distances of the pulley axes; by connecting electric motors through frequency converters, it was possible to control the change in the input speed of the transmission and, at the same time, the load on the output pulley. On the proposed specific design solution for testing belt drives, the actual speed of the input and output pulleys was measured by sensors to determine the belt slip, and the belt’s floating in one plane was monitored using high-precision distance measurement sensors. The analysis of the belt drives also included an assessment of their impact on other parts of the machine or equipment (for example, when transmitting large forces, this can have a negative impact on bearings and gearbox components) on which they are installed; therefore, vibration measurements were also performed. The results of the experimental measurements can contribute to designers choosing a belt drive, for example, even under boundary load parameters and extreme conditions. Full article
(This article belongs to the Section Control Systems)
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<p>Control panel of the new measuring system.</p>
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<p>Monitoring the tension of the belt (<b>a</b>) using a tensometric sensor (<b>b</b>) that detects the compressive (tensioning) force.</p>
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<p>Mechanism used to tension the belt in the mechanism.</p>
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<p>Three-dimensional model and real measuring and monitoring equipment.</p>
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<p>Transmission part of the device intended for testing belt transmissions.</p>
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<p>Dependence of the coefficient of elastic slip on the input speed and the load at the output of the belt transmission when the belt was tensioned at 50 N.</p>
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<p>Dependence of the coefficient of the elastic slip on the input speed and the load at the output of the belt transmission with a belt tension of 250 N.</p>
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<p>Dependence of the coefficient of elastic slip on the input speed and the load at the output of the belt transmission when the belt was tensioned at 450 N.</p>
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<p>Dependence of the belt floating in the lightened branch on the input speed and the load at the output of the belt transmission when the belt was tensioned at 250 N.</p>
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<p>Dependence of the belt float in the traction branch on the input speed and the load at the output of the belt transmission when the belt was tensioned at 250 N.</p>
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<p>Dependence of vibrations on the input speed and the load at the output of the belt transmission when the belt is tensioned at 250 N.</p>
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35 pages, 2694 KiB  
Review
Synthetic Jet Actuators for Active Flow Control: A Review
by Howard H. Ho, Ali Shirinzad, Ebenezer E. Essel and Pierre E. Sullivan
Fluids 2024, 9(12), 290; https://doi.org/10.3390/fluids9120290 - 6 Dec 2024
Viewed by 730
Abstract
A synthetic jet actuator (SJA) is a fluidic device often consisting of a vibrating diaphragm that alters the volume of a cavity to produce a synthesized jet through an orifice. The cyclic ingestion and expulsion of the working fluid leads to a zero-net [...] Read more.
A synthetic jet actuator (SJA) is a fluidic device often consisting of a vibrating diaphragm that alters the volume of a cavity to produce a synthesized jet through an orifice. The cyclic ingestion and expulsion of the working fluid leads to a zero-net mass-flux and the transfer of linear momentum to the working fluid over an actuation cycle, leaving a train of vortex structures propagating away from the orifice. SJAs are a promising technology for flow control applications due to their unique features, such as no external fluid supply or ducting requirements, short response time, low weight, and compactness. Hence, they have been the focus of many research studies over the past few decades. Despite these advantages, implementing an effective control scheme using SJAs is quite challenging due to the large parameter space involving several geometrical and operational variables. This article aims to explain the working mechanism of SJAs and provide a comprehensive review of the effects of SJA design parameters in quiescent conditions and cross-flow. Full article
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<p>(<b>a</b>) A schematic drawing of an SJA in quiescent flow (adapted from Feero [<a href="#B40-fluids-09-00290" class="html-bibr">40</a>]) and (<b>b</b>) a Murata MZB1001T02 microblower (adapted from Machado et al. [<a href="#B41-fluids-09-00290" class="html-bibr">41</a>]).</p>
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<p>Schematic drawing of an SJA in quiescent flow during expulsion and ingestion phase, (<b>a</b>) initiation of the ingestion cycle; (<b>b</b>) peak ingestion phase; (<b>c</b>) initiation of the expulsion cycle, and (<b>d</b>) peak expulsion phase.</p>
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<p>Schematic drawing of a rectangular SJA having an array of circular actuators (adapted from Feero [<a href="#B40-fluids-09-00290" class="html-bibr">40</a>]).</p>
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<p>Schematic drawing of different SJA modeling methods, red dotted line indicates where the boundary condition is applied, adapted from Ho et al. [<a href="#B52-fluids-09-00290" class="html-bibr">52</a>].</p>
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<p>A schematic showcasing the complexities in understanding the interaction between a synthetic jet and a boundary layer (based on Ramasamy et al. [<a href="#B114-fluids-09-00290" class="html-bibr">114</a>]).</p>
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<p>Q−criterion contours of hairpin vortices and vortex rings as a result of the interaction between a synthetic jet and a boundary layer, showcasing hairpin vortex (HV), vortex ring (VR), trailing vortex pair (TV), and the near-wall vortex (NV) (adapted from Ho et al. [<a href="#B130-fluids-09-00290" class="html-bibr">130</a>]).</p>
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<p>A schematic illustrating the (<b>a</b>) pitch angle <math display="inline"><semantics> <mi>γ</mi> </semantics></math> and (<b>b</b>) skew angle <math display="inline"><semantics> <mi>β</mi> </semantics></math> for a rectangular SJA in a cross-flow (based on Van Buren et al. [<a href="#B135-fluids-09-00290" class="html-bibr">135</a>]).</p>
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<p>A conceptual model of the vortical structures generated by a rectangular synthetic jet within a boundary layer, depicting the recirculation region and the streamwise vortex pair (based on Van Buren et al. [<a href="#B138-fluids-09-00290" class="html-bibr">138</a>]).</p>
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<p>Separated flow over an airfoil at low Reynolds numbers undergoing (<b>a</b>) shear layer transition without reattachment and (<b>b</b>) flow reattachment and separation bubble formation (based on Yarusevych et al. [<a href="#B146-fluids-09-00290" class="html-bibr">146</a>]).</p>
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<p>Examples showcasing the modulation of (<b>a</b>) a sinusoidal carrier signal at <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>1000</mn> <mi>Hz</mi> </mrow> </semantics></math> with (<b>b</b>) a sinusoidal envelope at <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mi>m</mi> </msub> <mo>=</mo> <mn>100</mn> <mi>Hz</mi> </mrow> </semantics></math> and (<b>c</b>) a square pulse envelope at <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mi>m</mi> </msub> <mo>=</mo> <mn>100</mn> <mi>Hz</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>DC</mi> <mo>=</mo> <mn>40</mn> <mo>%</mo> </mrow> </semantics></math>, over a duration of <math display="inline"><semantics> <mrow> <mn>0.05</mn> </mrow> </semantics></math><math display="inline"><semantics> <mi mathvariant="normal">s</mi> </semantics></math>.</p>
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<p>Schematic drawings of the SJA location for (<b>a</b>) a two-dimensional circular cylinder, studied by Amitay et al. [<a href="#B113-fluids-09-00290" class="html-bibr">113</a>], Amitay et al. [<a href="#B167-fluids-09-00290" class="html-bibr">167</a>] and Glezer et al. [<a href="#B118-fluids-09-00290" class="html-bibr">118</a>], and (<b>b</b>) an instrumented NACA 0025 airfoil model used by Feero et al. [<a href="#B168-fluids-09-00290" class="html-bibr">168</a>].</p>
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<p>Contraction of the controlled flow toward the airfoil centerline showcased by (<b>a</b>) a schematic drawing of the SJA array and the streamlines and (<b>b</b>) a smoke visualization image adapted from Ho and Machado [<a href="#B171-fluids-09-00290" class="html-bibr">171</a>].</p>
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