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20 pages, 3556 KiB  
Article
Enhancing Real-Time Video Streaming Quality via MPT-GRE Multipath Network
by Naseer Al-Imareen and Gábor Lencse
Electronics 2025, 14(3), 497; https://doi.org/10.3390/electronics14030497 - 25 Jan 2025
Viewed by 638
Abstract
The demand for real-time 4K video streaming has introduced technical challenges due to the high bandwidth, low latency, and minimal jitter required for high-quality user experience. Traditional single-path networks often fail to meet these requirements, especially under network congestion and packet loss conditions, [...] Read more.
The demand for real-time 4K video streaming has introduced technical challenges due to the high bandwidth, low latency, and minimal jitter required for high-quality user experience. Traditional single-path networks often fail to meet these requirements, especially under network congestion and packet loss conditions, which degrade video quality and disrupt streaming stability. This study evaluates Multipath tunnel- Generic Routing Encapsulation (MPT-GRE), a technology designed to address these challenges by enabling simultaneous data transmission across multiple network paths. By aggregating bandwidth and adapting dynamically to network conditions, MPT-GRE enhances resilience, maintains quality during network disruptions, and offers throughput nearly equal to the sum of its physical paths’ throughput. This feature ensures that even if one path fails, the technology seamlessly continues streaming through the remaining path, significantly reducing interruptions. We measured key video quality metrics to assess MPT-GRE’s performance: Structural Similarity Index Measure (SSIM), Mean Squared Error (MSE), and Peak Signal-to-Noise Ratio (PSNR). Our results confirm that the MPT-GRE tunnel effectively improves SSIM, PSNR, and reduces MSE compared to single-path streaming, offering a more stable, high-quality viewing experience. Our results indicate that analyzing the SSIM, MSE, and PSNR values for 4K video streaming using the MPT tunnel demonstrates a significant performance improvement compared to a single path. The improvement percentages of the SSIM and PSNR values for the MPT tunnel are (29.05% and 29.04%) higher than that of the single path, while MSE is reduced by 81.17% compared to the single path. Full article
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<p>The conceptual architecture of MPT-GRE [<a href="#B17-electronics-14-00497" class="html-bibr">17</a>].</p>
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<p>The theoretical process of the MPT-GRE mechanism [<a href="#B17-electronics-14-00497" class="html-bibr">17</a>].</p>
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<p>A snapshot of Waterloo Database video sequences [<a href="#B21-electronics-14-00497" class="html-bibr">21</a>].</p>
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<p>MPT-GRE multipath network topology of real-time 4K video streaming.</p>
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<p>SSIM comparison for different videos streaming via the single path and MPT-GRE tunnel.</p>
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<p>MSE comparison for different videos streaming via the single path and MPT-GRE tunnel.</p>
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<p>PSNR comparison for different videos streaming via the single path and MPT-GRE tunnel.</p>
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20 pages, 4809 KiB  
Article
Design and Evaluation of Noise Simulation Algorithm Using MATLAB Ray Tracing Engine for Noise Assessment and Prediction
by Precin Kalisalvan, Mohd Sayuti Ab Karim and Siti Nurmaya Musa
Appl. Sci. 2025, 15(3), 1009; https://doi.org/10.3390/app15031009 - 21 Jan 2025
Viewed by 583
Abstract
The Malaysian Department of Occupational Safety and Health (DOSH) reported that noise-induced hearing loss (NIHL) accounted for 92% of occupational diseases in 2019. To address this, accurate risk assessment is crucial. The current noise evaluation methods are complex and time-consuming, relying on manual [...] Read more.
The Malaysian Department of Occupational Safety and Health (DOSH) reported that noise-induced hearing loss (NIHL) accounted for 92% of occupational diseases in 2019. To address this, accurate risk assessment is crucial. The current noise evaluation methods are complex and time-consuming, relying on manual calculations and field measurements. An easy-to-use, open-source noise simulator that directly compares the output with national standards would help mitigate this issue. This research aims to develop an advanced noise evaluation tool to assess and predict unregulated workplace noise, providing tailored safety recommendations. Using a representative plant layout, the Sound Pressure Level (SPL) is calculated using MATLAB’s ray tracing propagation model. The model simulates all possible transmission paths from the source to the receiver to derive the resultant SPL. A noise simulation application featuring a graphical user interface (GUI) built with MATLAB’s App Designer (version: R2024a) automates these computations. The simulation results are validated against the DOSH’s safety standards in Malaysia. Additional safety metrics, such as the recommended maximum exposure time and the required Noise Reduction Rating (NRR) for hearing protection, are calculated based on the SPLs for hazardous locations. The simulation algorithm’s functionality is validated against manual calculations, with an average deviation of just 3.06 dB, demonstrating the model’s precision. This tool can assess and predict indoor noise levels, provide information on optimal exposure limits, and recommend necessary protective measures, ultimately reducing the risk of NIHL in factory environments. It can potentially optimise plant floor operations for existing and new facilities, ensuring safer shift operations and reducing worker noise hazard exposure. Full article
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<p>Acoustic ray tracing algorithm framework [<a href="#B31-applsci-15-01009" class="html-bibr">31</a>].</p>
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<p>Overall process of noise assessment and safety recommendations.</p>
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<p>Sections in the graphical user interface (1—file upload, 2—receiver information, 3—source information, 4—safety recommendations, and 5—resultant SPL).</p>
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<p>GUI simulates safety recommendations when the resultant SPL is above the limits.</p>
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<p>Test floor plan with sources and receiver in meters.</p>
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<p>(<b>a</b>) Floor plan of the factory (Furniture Painting and Assembly factory in Klang Malaysia) with pictures (A1/A2—Painting booth, B1/B2—Sanding booth, C1—Assembly booth); (<b>b</b>) drawing of floor plan divided into grids; (<b>c</b>) 3D model of the floor plan’s outline.</p>
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<p>Three-dimensional version of ray diagram of the simulation when reflection is changed from 0, 1, 2, 3 and 4.</p>
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<p>Resultant SPL vs. max number of reflections graph.</p>
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<p>Resultant SPLs vs. surface materials.</p>
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<p>Three-dimensional version of ray diagram during simulation verification (with reflection).</p>
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<p>Recorded SPLs from collected real-world data in dB.</p>
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<p>Simulated SPLs plotted on a grid and heatmap in dB.</p>
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<p>Comparison between SPLs from site and simulation.</p>
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21 pages, 4888 KiB  
Article
Digital Twin-Assisted Lightpath Provisioning and Nonlinear Mitigation in C+L+S Multiband Optical Networks
by Sadegh Ghasrizadeh, Prasunika Khare, Nelson Costa, Marc Ruiz, Antonio Napoli, Joao Pedro and Luis Velasco
Sensors 2024, 24(24), 8054; https://doi.org/10.3390/s24248054 - 17 Dec 2024
Viewed by 801
Abstract
Multiband (MB) optical transmission targets increasing the capacity of operators’ optical transport networks. However, nonlinear impairments (NLI) affect each optical channel in the C+L+S bands differently, and, therefore, the routing and spectrum assignment (RSA) problem needs to be complemented with fast and accurate [...] Read more.
Multiband (MB) optical transmission targets increasing the capacity of operators’ optical transport networks. However, nonlinear impairments (NLI) affect each optical channel in the C+L+S bands differently, and, therefore, the routing and spectrum assignment (RSA) problem needs to be complemented with fast and accurate tools to consider the quality of transmission (QoT) within the provisioning process. This paper proposes a digital twin-assisted approach for lightpath provisioning to provide a complete solution for the RSA problem that ensures the required QoT in MB optical networks. The OCATA time domain digital twin is proposed, not only to estimate the QoT of a selected path but also to support the QoT-based channel assignment process. OCATA is based on a Deep Neural Network (DNN) to model the propagation of the optical signal. However, because of the different impacts of nonlinear noise on each channel and the large number of channels that need to be considered in C+L+S MB scenarios, OCATA needs to be adapted to make it scalable, while keeping its high accuracy and fast QoT estimation characteristics. In consequence, a complete methodology is proposed in this work that limits the number of channels being modeled to just a few. Moreover, OCATA-MB helps to mitigate NLI noise by programming the receiver at the provisioning time and thus with very little complexity compared to its equivalent implemented during the operation. NLI noise mitigation can be applied in the case when a lightpath cannot be provisioned because none of the available channels can provide the required QoT, making it an advantageous tool for reducing connection blocking. Exhaustive simulation results demonstrate the remarkable accuracy of OCATA-MB in estimating the QoT for any channel. Interestingly, by utilizing the proposed OCATA-MB-assisted lightpath provisioning approach, a reduction of the blocking ratio exceeding 50% when compared to traditional approaches is shown when NLI noise mitigation is not applied. If NLI mitigation is implemented, an additional over 50% blocking reduction is achieved. Full article
(This article belongs to the Special Issue Sensing Technologies and Optical Communication)
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<p>Overview of the considered MB scenario (<b>a</b>) and illustrative performance of MB optical transmission (<b>b</b>).</p>
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<p>Main building blocks of the OCATA-MB time domain digital twin.</p>
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<p>Example of <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi mathvariant="sans-serif">Φ</mi> </mrow> <mrow> <mi>o</mi> <mi>u</mi> <mi>t</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msubsup> </mrow> </semantics></math> feature and regular (<b>a</b>) (reproduced from [<a href="#B20-sensors-24-08054" class="html-bibr">20</a>]) and optimized (<b>b</b>) detection area for CP <span class="html-italic">i</span> = [<a href="#B20-sensors-24-08054" class="html-bibr">20</a>].</p>
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<p>Proposed DT-assisted MB-RSA procedure.</p>
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<p>Definition grid for 16-QAM signal constellations.</p>
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<p>Value of selected σ features and CPs vs. channel index and piecewise linear fitting with 1, 4, and 6 segments. (<b>a</b>) <span class="html-italic">σ<sup>I</sup></span>, (−3 + 3i), (<b>b</b>) <span class="html-italic">σ<sup>Q</sup></span>, (−3 + 3i), and (<b>c</b>) <span class="html-italic">σ<sup>I</sup></span>, (3 − 3i).</p>
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<p>Pre-FEC BER vs. number of piecewise linear segments.</p>
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<p>Pre-FEC BER vs. number of piecewise linear segments.</p>
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<p>Reconstructed constellations for an RCh (<b>a</b>) and a non-RCh (<b>b</b>). Details of two CPs, one exterior and one interior (<b>c</b>).</p>
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<p>Evolution of pre-FEC BER as a function of the number of spans for several channels.</p>
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<p>Estimated pre-FEC BER for different number of areas.</p>
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<p>Real and estimated pre-FEC BER with squared and optimized detection areas vs. # spans for ch. 1 (<b>a</b>), 150 (<b>b</b>), and 337 (<b>c</b>).</p>
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<p>Optimal detection areas (k = 10,000) for QAM-16 signals for five spans. (<b>a</b>) Ch. 1 in the S band, (<b>b</b>) Ch. 150 in the C band, and (<b>c</b>) Ch. 337 in the L band.</p>
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<p>Spanish core optical network topology (<b>a</b>). Number of demands blocked (<b>b</b>) and blocking ratio evolution (<b>c</b>) vs. demand number.</p>
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22 pages, 3464 KiB  
Article
Mechanisms of Noise Transmission in Velocity Broad-Band Seismometers: Modeling and Analysis
by Yini Sun, Zhongkun Zhang, Zhijuan Zhu, Bin Chen and Lingyun Ye
Appl. Sci. 2024, 14(23), 11393; https://doi.org/10.3390/app142311393 - 6 Dec 2024
Viewed by 618
Abstract
This paper focuses on the noise transmission process, presenting a comprehensive noise transfer model for velocity broad-band seismometers, which elucidate the transmission mechanisms of five distinct noise sources. We analyzed the spectral characteristics of the noise transfer functions across the forward path, feedback [...] Read more.
This paper focuses on the noise transmission process, presenting a comprehensive noise transfer model for velocity broad-band seismometers, which elucidate the transmission mechanisms of five distinct noise sources. We analyzed the spectral characteristics of the noise transfer functions across the forward path, feedback path, and data acquisition stages, with a focus on gains, corner frequencies, and the 0 dB point. Numerical simulations and experiments using the CS60 seismometer showed excellent agreement with theoretical predictions, validating the proposed model and associated noise optimization strategies. This study identified effective methods to reduce noise transfer gains, including optimizing the input and feedback mechanical constants and refining gains at various stages. Full article
(This article belongs to the Section Mechanical Engineering)
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<p>Median self-noise models for some typical VBB seismometers [<a href="#B19-applsci-14-11393" class="html-bibr">19</a>].</p>
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<p>Two approaches to optimizing sensor noise: noise source or transmission path.</p>
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<p>VBB seismometer system block diagram and noise sources.</p>
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<p>Equivalent circuit model for feedback path analysis.</p>
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<p>Theoretical amplitude–frequency curves of the noise transfer functions for the CS60.</p>
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<p>EIN caused by suspension pendulum noise.</p>
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<p>EIN caused by white noise in forward path.</p>
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<p>EIN caused by white noise of integrator.</p>
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<p>EIN caused by force transducer noise.</p>
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<p>EIN caused by white noise of differential amplifier.</p>
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<p>EIN from different noise sources: Solid lines denote the theoretical values, while corresponding simulation results are represented with symbols such as rectangles, circles, triangles, and diamonds in matching colors.</p>
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<p>Experimental setup.</p>
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<p>Measured, theoretical, and simulated self-noise values. NLNM and NHNM curves represent Peterson’s Earth noise model [<a href="#B2-applsci-14-11393" class="html-bibr">2</a>].</p>
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14 pages, 4275 KiB  
Article
Physical Layer Security Based on Non-Orthogonal Communication Technique with Coded FTN Signaling
by Myung-Sun Baek and Hyoung-Kyu Song
Mathematics 2024, 12(23), 3800; https://doi.org/10.3390/math12233800 - 30 Nov 2024
Viewed by 696
Abstract
In recent years, ensuring communication security at the physical layer has become increasingly important due to the transmission of sensitive information over various networks. Traditional approaches to physical layer security often rely on artificial noise generation, which may not offer robust solutions against [...] Read more.
In recent years, ensuring communication security at the physical layer has become increasingly important due to the transmission of sensitive information over various networks. Traditional approaches to physical layer security often rely on artificial noise generation, which may not offer robust solutions against advanced interception techniques. This study addresses these limitations by proposing a novel security technique based on non-orthogonal signaling using Faster-than-Nyquist (FTN) signaling. Unlike conventional FTN methods that utilize fixed symbol intervals, the proposed technique employs variable symbol intervals encoded as secure information, shared only with legitimate receivers. This encoding enables effective interference cancellation and symbol detection at the receiver, while preventing eavesdroppers from deciphering transmitted signals. The performance of the proposed technique was evaluated using the DVB-S2X system, a practical digital video broadcasting standard. Simulation results demonstrated that the proposed method maintains smooth communication with minimal performance degradation compared to traditional methods. Furthermore, eavesdroppers were unable to decode the transmitted signals, confirming the enhanced security. This research presents a new approach to physical layer security that does not depend on generating artificial noise, offering a path to more secure and efficient communication systems. Full article
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<p>Signal wave comparison between general communication and FTN signaling.</p>
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<p>Comparison between general FTN signaling and coded FTN signaling.</p>
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<p>Conceptual diagram for block-wise coded FTN and variable-length block-wise coded FTN signaling.</p>
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<p>Block/flow diagram of the proposed technique.</p>
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<p>DVB-S2X System with Coded FTN signaling.</p>
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<p>BER performances of symbol-wise coded FTN signaling and block-wise coded FTN signaling in DVB-S2X system with 16-QAM.</p>
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<p>BER performances of symbol-wise coded FTN signaling and block-wise coded FTN signaling in DVB-S2X system with QPSK.</p>
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<p>BER performance of variable-length block-wise coded FTN signaling in DVB-S2X system with 16-QAM.</p>
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<p>BER performance of variable-length block-wise coded FTN signaling in DVB-S2X system with QPSK.</p>
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<p>PAPR performance of DVB-S2 system with 16QAM according to <span class="html-italic">τ</span> values.</p>
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21 pages, 6144 KiB  
Article
Unbalanced Position Recognition of Rotor Systems Based on Long and Short-Term Memory Neural Networks
by Yiming Cao, Changzhi Shi, Xuejun Li, Mingfeng Li and Jie Bian
Machines 2024, 12(12), 865; https://doi.org/10.3390/machines12120865 - 28 Nov 2024
Viewed by 607
Abstract
Rotor unbalance stands as one of the primary causes of vibration and noise in rotating equipment. Accurate identification of unbalanced positions enables targeted measures for balance correction, thereby reducing vibration and noise levels and enhancing the operational efficiency and stability of the equipment. [...] Read more.
Rotor unbalance stands as one of the primary causes of vibration and noise in rotating equipment. Accurate identification of unbalanced positions enables targeted measures for balance correction, thereby reducing vibration and noise levels and enhancing the operational efficiency and stability of the equipment. However, the complexity of rotor structures may lead to a diversity of vibration transmission paths, which complicates the identification of unbalanced positions. In this paper, an experimental platform for rotor systems is established to analyze the change patterns of vibration displacement in rotor systems at four unbalanced positions. Additionally, a rotor dynamics model is developed based on the finite element method and verified through experiments. Furthermore, an unbalanced rotor position identification method based on Long Short-Term Memory (LSTM) neural networks is proposed. This method utilizes multiple sets of measured response data and simulated data from unbalanced rotor positions to train the LSTM network, achieving precise identification of unbalanced positions at various rotational speeds. The research results indicate that under subcritical, critical, and supercritical speeds, the identification accuracy based on measured data reaches 95.5%, while the accuracy based on simulated data remains at a high level of 90.5%. These results fully validate the effectiveness and accuracy of the proposed model and identification method, providing new insights and technical means for identifying unbalanced rotor positions. Full article
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<p>Schematic of element: (<b>a</b>) shaft element; (<b>b</b>) disk element.</p>
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<p>Diagram of a coupling with loose clearance: (<b>a</b>) structure diagram; (<b>b</b>) equivalent model.</p>
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<p>Turbine rotor system test bench and simplified structure diagram.</p>
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<p>Geometric structure diagram of turbine rotor system.</p>
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<p>Rotor vibration test bench: (<b>a</b>) sensor layout; (<b>b</b>) data acquisition system.</p>
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<p>Comparisons between experimental results and simulation results of rotor system at a sub-critical speed of 5600 rpm: (<b>a</b>) boss 1 unbalanced; (<b>b</b>) boss 2 unbalanced; (<b>c</b>) boss 3 unbalanced; and (<b>d</b>) boss 4 unbalanced.</p>
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<p>Comparisons between experimental results and simulation results of rotor system at a critical speed of 7260 rpm: (<b>a</b>) boss 1 unbalanced; (<b>b</b>) boss 2 unbalanced; (<b>c</b>) boss 3 unbalanced; and (<b>d</b>) boss 4 unbalanced.</p>
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<p>Comparisons between experimental results and simulation results of rotor system at an over-critical speed of 8400 rpm: (<b>a</b>) boss 1 unbalanced; (<b>b</b>) boss 2 unbalanced; (<b>c</b>) boss 3 unbalanced; and (<b>d</b>) boss 4 unbalanced.</p>
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<p>LSTM structure diagram.</p>
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<p>The LSTM neural network: (<b>a</b>) structure diagram; (<b>b</b>) identification process.</p>
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<p>Loss curve of LSTM model.</p>
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<p>Identification results of unbalanced rotor position at subcritical speed based on LSTM: (<b>a</b>) based on experiment; (<b>b</b>) based on simulation.</p>
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<p>Identification results of unbalanced rotor position at a critical speed based on LSTM: (<b>a</b>) based on experiment; (<b>b</b>) based on simulation.</p>
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<p>Identification results of unbalanced rotor position at supercritical speed based on the LSTM: (<b>a</b>) based on experiment; (<b>b</b>) based on simulation.</p>
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14 pages, 7240 KiB  
Article
A 23–29 GHz GaN Low-Noise Amplifier with Drain-to-Source Coupling Feedback
by Fengyuan Mao, Zhijian Chen, Bin Li, Zhaohui Wu, Xinhuang Chen and Quansheng Guan
Electronics 2024, 13(21), 4154; https://doi.org/10.3390/electronics13214154 - 23 Oct 2024
Viewed by 999
Abstract
In this paper, a four-stage gallium nitride (GaN) low noise amplifier (LNA) using coupled-line (CL) feedback in a 0.15-μm GaN-on-SiC process is proposed. The electromagnetic coupling feedback between the drain and source of each transistor is employed to generate an additional signal path [...] Read more.
In this paper, a four-stage gallium nitride (GaN) low noise amplifier (LNA) using coupled-line (CL) feedback in a 0.15-μm GaN-on-SiC process is proposed. The electromagnetic coupling feedback between the drain and source of each transistor is employed to generate an additional signal path for neutralization, which enhances gain and improves stability performance. A series transmission line-capacitor-transmission line (TL-C-TL) network is introduced between stages of the LNA for wider band interstage matching. The measured results show that the designed LNA achieves a 3-dB bandwidth of 23.6 to 29.8 GHz, a peak gain of 23.7 dB at 25.8 GHz, and a minimum noise figure (NF) of 2.2 dB at 27.8 GHz. The output-referred 1-dB compression point (OP1dB) is 13 dBm. The total power consumption of the LNA is 200 mW. Full article
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<p>Schematic of the proposed LNA.</p>
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<p>(<b>a</b>) Schematic of the 4-port CL coupler. (<b>b</b>) CL unit with two ports being grounded.</p>
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<p>(<b>a</b>) The equivalent self-inductance and mutual inductance. (<b>b</b>) Q-factor. (<b>c</b>) Coupling coefficient.</p>
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<p>(<b>a</b>) Single stage with drain-to-source CL feedback. (<b>b</b>) Three-dimensional view of the CL in a single stage.</p>
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<p>Small signal model of single stage.</p>
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<p>(<b>a</b>) Gain enhancement with coupling. (<b>b</b>) Isolation enhancement with coupling. (<b>c</b>) Stability improvement with coupling. (<b>d</b>) Comparison of NF<sub>min</sub> before and after coupling.</p>
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<p>Traditional matching networks (<b>a</b>) First-order LC network. (<b>b</b>) π-type network. (<b>c</b>) High-order network.</p>
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<p>The proposed interstage matching network.</p>
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<p>Input reflection coefficient of the transistor using the proposed ISMN with different lengths of series TL. (<b>a</b>) On the Smith Chart. (<b>b</b>) The same S11 is expressed in decibels versus gigahertz.</p>
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<p>Chip microphoto of the proposed LNA.</p>
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<p>Measurement configuration.</p>
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<p>Simulated and measured S-parameters of the LNA.</p>
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<p>Simulated and measured NF of the LNA.</p>
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<p>Simulated and measured OP1dB of the LNA.</p>
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<p>Simulated and measured μ-factor of the LNA.</p>
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11 pages, 18597 KiB  
Article
Demodulating Optical Wireless Communication of FBG Sensing with Turbulence-Caused Noise by Stacked Denoising Autoencoders and the Deep Belief Network
by Shegaw Demessie Bogale, Cheng-Kai Yao, Yibeltal Chanie Manie, Amare Mulatie Dehnaw, Minyechil Alehegn Tefera, Wei-Long Li, Zi-Gui Zhong and Peng-Chun Peng
Electronics 2024, 13(20), 4127; https://doi.org/10.3390/electronics13204127 - 20 Oct 2024
Cited by 1 | Viewed by 1414
Abstract
Free-space optics communication (FSO) can be used as a transmission medium for fiber optic sensing signals to make fiber optic sensing easier to implement; however, interference with the sensing signals caused by the optical turbulence and scattering of airborne particles in the FSO [...] Read more.
Free-space optics communication (FSO) can be used as a transmission medium for fiber optic sensing signals to make fiber optic sensing easier to implement; however, interference with the sensing signals caused by the optical turbulence and scattering of airborne particles in the FSO path is a potential problem. This work aims to deep denoise sensed signals from fiber Bragg grating (FBG) sensors based on FSO link transmission using advanced denoising deep learning techniques, such as stacked denoising autoencoders (SDAE). Furthermore, it will demodulate the sensed wavelength of FBGs by applying the deep belief network (DBN) technique. This is the first time the real FBG sensing experiment has utilized the actual noise interference caused by the environmental turbulence from an FSO link rather than adding noise through numerical processing. Consequently, the spectrum of the FBG sensors is clearly modulated by the noise and the issue with peak power variation. This complicates the determination of the center wavelengths of multiple stacked FBG spectra, requiring the use of machine learning techniques to predict these wavelengths. The results indicate that SDAE is efficient in denoising from the FBG spectrum, and DBN is effective in demodulating the central wavelength of the overlapped FBG spectrum. Thus, it is beneficial to implement an FSO link-based FBG sensing system in adverse weather conditions or atmospheric turbulence. Full article
(This article belongs to the Special Issue Advances in Deep Learning-Based Wireless Communication Systems)
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<p>Experimental framework for FBG array sensing based on FSO transmission with incidental particle scattering. The sensed data are used for AI model training and testing. (BLS: broadband light source; Cir.: circulator; OSA: optical spectrum analyzer; PC: personal computer).</p>
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<p>The corresponding values of the three FBG reflected wavelengths in each strain step.</p>
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<p>(<b>a</b>) Comparison of some FBG spectra before and after denoising; (<b>b</b>) Presentation of all FBG spectra (step 1 to step 16 in order) before and after denoising.</p>
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<p>Signal-to-noise ratio analysis (<b>a</b>) before SDAE denoising; (<b>b</b>) after SDAE denoising.</p>
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<p>The peak power of FBGs for each of the 19 spectra collected under strain steps 1, 8, and 16.</p>
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<p>Flowchart of wavelength demodulation by DBN.</p>
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<p>Parameters of the proposed SDAE and DBN models.</p>
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<p>Training efficiency of the DBN model in terms of accuracy and loss.</p>
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<p>Performance comparison with different machine learning models.</p>
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<p>(<b>a</b>) FBG peak wavelength prediction after applying SDAE and DBN models. (<b>b</b>) FBG peak wavelength prediction after applying the DBN model only.</p>
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19 pages, 9136 KiB  
Article
A Novel Ultrasonic Leak Detection System in Nuclear Power Plants Using Rigid Guide Tubes with FCOG and SNR
by You-Rak Choi, Doyeob Yeo, Jae-Cheol Lee, Jai-Wan Cho and Sangook Moon
Sensors 2024, 24(20), 6524; https://doi.org/10.3390/s24206524 - 10 Oct 2024
Viewed by 1436
Abstract
Leak detection in nuclear reactor coolant systems is crucial for maintaining the safety and operational integrity of nuclear power plants. Traditional leak detection methods, such as acoustic emission sensors and spectroscopy, face challenges in sensitivity, response time, and accurate leak localization, particularly in [...] Read more.
Leak detection in nuclear reactor coolant systems is crucial for maintaining the safety and operational integrity of nuclear power plants. Traditional leak detection methods, such as acoustic emission sensors and spectroscopy, face challenges in sensitivity, response time, and accurate leak localization, particularly in complex piping systems. In this study, we propose a novel leak detection approach that incorporates a rigid guide tube into the insulation layer surrounding reactor coolant pipes and combines this with an advanced detection criterion based on Frequency Center of Gravity shifts and Signal-to-Noise Ratio analysis. This dual-method strategy significantly improves the sensitivity and accuracy of leak detection by providing a stable transmission path for ultrasonic signals and enabling robust signal analysis. The rigid guide tube-based system, along with the integrated criteria, addresses several limitations of existing technologies, including the detection of minor leaks and the complexity of installation and maintenance. By enhancing the early detection of leaks and enabling precise localization, this approach contributes to increased reactor safety, reduced downtime, and lower operational costs. Experimental evaluations demonstrate the system’s effectiveness, focusing on its potential as a valuable addition to the current array of nuclear power plant maintenance technologies. Future research will focus on optimizing key parameters, such as the threshold frequency shift (Δf) and the number of randomly selected frequencies (N), using machine learning techniques to further enhance the system’s accuracy and reliability in various reactor environments. Full article
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<p>Concept of leak detection with rigid guide tubes for piping covered with insulation.</p>
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<p>Cross-sectional view of the insulation-sheathed pipe connected to an M/P sensor via a rigid guide tube.</p>
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<p>Experimental setup of leak detection with rigid guide tubes for piping covered with insulation.</p>
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<p>Side view of the experimental setup shown in <a href="#sensors-24-06524-f003" class="html-fig">Figure 3</a>, illustrating the arrangement of the rigid guide tube, M/P sensors, and insulation sheath.</p>
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<p>Power spectrum comparison between 0.5 mm leak at LN #2 and leak-off measured by ULD #2 at a gauge pressure of 200 kPa.</p>
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<p>FCOG measured at three different ULD points with a 0.5 mm leak at LN #2 and leak-off at a gauge pressure of 200 kPa; (<b>a</b>) ΔFCOG = 0.68 kHz @ ULD #1; (<b>b</b>) ΔFCOG = 3.44 kHz @ ULD #2; (<b>c</b>) ΔFCOG = 1.7 kHz @ ULD #3.</p>
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<p>SNR analysis across ULD sensors for 0.5 mm leak at LN #2.</p>
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<p>FCOG measured at three different ULD points with a 1.0 mm leak at LN #3 and leak-off at a gauge pressure of 200 kPa; (<b>a</b>) ΔFCOG = 1.54 kHz @ ULD #1; (<b>b</b>) ΔFCOG = 5.17 kHz @ ULD #2; (<b>c</b>) ΔFCOG = 6.09 kHz @ ULD #3.</p>
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<p>FCOG measured at three different ULD points with a 1.0 mm leak at LN #3 and leak-off at a gauge pressure of 200 kPa; (<b>a</b>) ΔFCOG = 1.54 kHz @ ULD #1; (<b>b</b>) ΔFCOG = 5.17 kHz @ ULD #2; (<b>c</b>) ΔFCOG = 6.09 kHz @ ULD #3.</p>
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<p>SNR analysis across ULD sensors for 1.0 mm leak at LN #3.</p>
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21 pages, 5770 KiB  
Article
Comparative Evaluation of Neural Network Models for Optimizing ECG Signal in Non-Uniform Sampling Domain
by Pratixita Bhattacharjee and Piotr Augustyniak
Appl. Sci. 2024, 14(19), 8772; https://doi.org/10.3390/app14198772 - 28 Sep 2024
Viewed by 1032
Abstract
Electrocardiographic signals (ECG) are ubiquitous, which justifies the research of their optimal storage and transmission. However, proposals for non-uniform signal sampling must take into account the priority of diagnostic data accuracy and record integrity, as well as robustness to noise and interference. In [...] Read more.
Electrocardiographic signals (ECG) are ubiquitous, which justifies the research of their optimal storage and transmission. However, proposals for non-uniform signal sampling must take into account the priority of diagnostic data accuracy and record integrity, as well as robustness to noise and interference. In this study, two novel methods are introduced, each utilizing a distinct neural network architecture for optimizing non-uniform sampling of ECG signal. A transformer model refines each time point selection through an iterative process using gradient descent optimization, with the goal of minimizing the mean squared error between the original and resampled signals. It adaptively modifies time points, which improves the alignment between both signals. In contrast, the Temporal Convolutional Network model trains on the original signal, and gradient descent optimization is utilized to improve the selection of time points. Evaluation of both strategies’ efficacy is performed by calculating signal distances at lower and higher sampling rates. First, a collection of synthetic data points that resembled the P-QRS-T wave was used to train the model. Then, the ECG-ID database for real data analysis was used. Filtering to remove baseline wander followed by evaluation and testing were carried out in the real patient data. The results, in particular MSE = 0.0005, RMSE = 0.0216, and Pearson’s CC = 0.9904 for 120 sps in the case of the transformer patient data model, provide viable paths for maintaining the precision and dependability of ECG-based diagnostic systems at much lower sampling rate. Outcomes indicate that both techniques are effective at improving the fidelity between the original and modified ECG signals. Full article
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<p>Raw ECG signal from the database (original signal).</p>
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<p>Filtered ECG signal (modified signal).</p>
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<p>Architectural diagram of TCN model.</p>
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<p>Architectural diagram of transformer model.</p>
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<p>Block diagram of the proposed sampling and validation process.</p>
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<p>Workflow of the proposed models—a programming viewpoint.</p>
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<p>Synthetic signal output for TCN model.</p>
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<p>Synthetic signal output for transformer model.</p>
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<p>ECG optimization using TCN Model at 18 sps for Person_30 in the database.</p>
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<p>ECG optimization using TCN Model at 120 sps for Person_30 in the database.</p>
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<p>ECG optimization using the transformer model at 18 sps for Person_30 in the database.</p>
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<p>ECG optimization using the transformer model at 120 sps for Person_30 in the database.</p>
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<p>Scatter plot for TCN model showing actual outcome: (<b>a</b>) MSE vs. number of samples; (<b>b</b>) RMSE vs. number of samples; (<b>c</b>) Pearson’s r vs. number of samples.</p>
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<p>Scatter plot for transformer model showing actual outcome: (<b>a</b>) MSE vs. number of samples; (<b>b</b>) RMSE vs. number of samples; (<b>c</b>) Pearson’s r vs. number of samples.</p>
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24 pages, 6241 KiB  
Article
Evaluation of LoRa Network Performance for Water Quality Monitoring Systems
by Syarifah Nabilah Syed Taha, Mohamad Sofian Abu Talip, Mahazani Mohamad, Zati Hakim Azizul Hasan and Tengku Faiz Tengku Mohmed Noor Izam
Appl. Sci. 2024, 14(16), 7136; https://doi.org/10.3390/app14167136 - 14 Aug 2024
Cited by 1 | Viewed by 1591
Abstract
Conserving water resources from scarcity and pollution is the basis of water resource management and water quality monitoring programs. However, due to industrialization and population growth in Malaysia, which have resulted in poor water quality in many areas, this program needs to be [...] Read more.
Conserving water resources from scarcity and pollution is the basis of water resource management and water quality monitoring programs. However, due to industrialization and population growth in Malaysia, which have resulted in poor water quality in many areas, this program needs to be improved. A smart water quality monitoring system based on the internet of things (IoT) paradigm was designed to analyze water conditions in real time and enable effective water management. Long-range (LoRa) application of the low-power, wide-area networking concept has become a phenomenon in IoT smart monitoring applications. This study proposes the implementation of a LoRa network in a water quality monitoring system-based IoT approach. The LoRa nodes were embedded with measuring sensors pH, turbidity, temperature, total dissolved solids, and dissolved oxygen, in the designated water stations. They operate at a transmission power of 14 dB and a bandwidth of 125 kHz. The network properties were tested with two different antenna gains of 2.1 dBi and 3 dBi, with three different spread factors of 7, 9, and 12. The water stations were located on the Sungai Pantai and Sungai Anak Air Batu rivers on the Universiti Malaya campus, Malaysia. Following a dashboard display and K-means analysis of the water quality data received by the LoRa gateway, it was determined that both rivers are Class II B rivers. The results from the evaluation of LoRa performance on the received strength signal indicator, signal noise ratio, loss packet, and path loss at best were −83 dBm, 7 dB, <0%, and 64.41 dB, respectively, with a minimum received sensitivity of −129.1 dBm. LoRa has demonstrated its efficiency in an urban environment for smart river monitoring purposes. Full article
(This article belongs to the Section Environmental Sciences)
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<p>Process of developing a water quality monitoring system with LoRa integration.</p>
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<p>Prototype of a water quality monitoring station.</p>
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<p>Sungai Pantai and Sungai Anak Air Batu in Universiti Malaya.</p>
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<p>Location of the water stations and the gateway at Universiti Malaya.</p>
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<p>LoRa gateway positioned on the rooftop.</p>
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<p>Water quality monitoring dashboard in Android view.</p>
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<p>Thing Speak Interface: Field 1 Chart–pH (<b>a</b>), Field 2 Chart–Turbidity (<b>b</b>), Field 3 Chart–Temperature (<b>c</b>), Field 4 Chart–TDS (<b>d</b>), and Field 5 Chart–Dissolved Oxygen (<b>e</b>).</p>
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<p>Water quality status at Station 1 (<b>a</b>), Station 2 (<b>b</b>), and Station 3 (<b>c</b>).</p>
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<p>Mean, maximum, and minimum of RSSI trend based on antenna gain of 2.1 dBi.</p>
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<p>Mean, maximum, and minimum of RSSI trend based on antenna gain of 3 dBi.</p>
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<p>Mean, maximum, and minimum of SNR trend based on antenna gain of 2.1 dBi.</p>
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<p>Mean, maximum, and minimum of SNR trend based on antenna gain of 3 dBi.</p>
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<p>Integration K-means trend on water quality data and packet loss at Water Station 1.</p>
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<p>Integration K-means trend on water quality data and packet loss at Water Station 2.</p>
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<p>Integration K-means trend on water quality data and packet loss at Water Station 3.</p>
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19 pages, 16336 KiB  
Article
Advancing the Diagnosis of Aero-Engine Bearing Faults with Rotational Spectrum and Scale-Aware Robust Network
by Jin Li, Zhengbing Yang, Xiang Zhou, Chenchen Song and Yafeng Wu
Aerospace 2024, 11(8), 613; https://doi.org/10.3390/aerospace11080613 - 26 Jul 2024
Cited by 2 | Viewed by 1615
Abstract
The precise monitoring of bearings is crucial for the timely detection of issues in rotating mechanical systems. However, the high complexity of the structures makes the paths of vibration signal transmission exceedingly intricate, posing significant challenges in diagnosing aero-engine bearing faults. Therefore, a [...] Read more.
The precise monitoring of bearings is crucial for the timely detection of issues in rotating mechanical systems. However, the high complexity of the structures makes the paths of vibration signal transmission exceedingly intricate, posing significant challenges in diagnosing aero-engine bearing faults. Therefore, a Rotational-Spectrum-informed Scale-aware Robustness (RSSR) neural network is proposed in this study to address intricate fault characteristics and significant noise interference. The RSSR algorithm amalgamates a scale-aware feature extraction block, a non-activation convolutional network, and an innovative channel attention block, striking a balance between simplicity and efficacy. We provide a comprehensive analysis by comparing traditional CNNs, transformers, and their respective variants. Our strategy not only elevates diagnostic precision but also judiciously moderates the network’s parameter count and computational intensity, mitigating the propensity for overfitting. To assess the efficacy of our proposed network, we performed rigorous testing using two complex, publicly available datasets, with additional artificial noise introductions to simulate challenging operational environments. On the noise-free dataset, our technique increased the accuracy by 5.11% on the aero-engine dataset compared with the current mainstream methods. Even under maximal noise conditions, it enhances the average accuracy by 4.49% compared with other contemporary approaches. The results demonstrate that our approach outperforms other techniques in terms of diagnostic performance and generalization ability. Full article
(This article belongs to the Special Issue Aircraft Structural Health Monitoring and Digital Twin)
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<p>Illustration of the proposed fault classification method (B: batch size; ADP: adaptive pooling).</p>
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<p>Illustration of signal domain transformation method (<span class="html-italic">CS</span>: constant sampling, <math display="inline"><semantics> <msub> <mi>G</mi> <mi>t</mi> </msub> </semantics></math>: grand total, <span class="html-italic">s</span>: sum, <span class="html-italic">I</span>: interpolation, <math display="inline"><semantics> <msub> <mi>R</mi> <mi>s</mi> </msub> </semantics></math>: record and splice).</p>
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<p>Illustration of Scale-Aware Robust Block.</p>
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<p>Illustration of channel attention.</p>
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<p>Illustration of the XJ-SQV dataset experimental bench.</p>
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<p>Illustration of the HIT-dataset experimental bench.</p>
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<p>Illustration of the accuracy results on two noise-free data sets.</p>
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<p>Illustration of the accuracy results of adding noise to the XJ-SQV.</p>
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<p>Illustration of the accuracy results of adding noise to the HIT-dataset.</p>
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<p>Illustration of the t-SNE visualization result of the test set on XJ-SQV.</p>
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<p>Illustration of the t-SNE visualization result of the test set on HIT-dataset.</p>
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<p>Illustration of the t-SNE diagram of the output results of all models on XJ-SQV.</p>
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<p>Illustration of the t-SNE diagram of the output results of all models on HIT-dataset.</p>
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<p>Illustration of the t-SNE visualization of the ablation result.</p>
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16 pages, 2412 KiB  
Article
Fragmentation and ISRS-Aware Survivable Routing, Band, Modulation, and Spectrum Allocation Algorithm in Multi-Band Elastic Optical Networks
by Yunxuan Liu, Nan Feng, Lingfei Shen, Jingjing Lv, Dan Yan and Jijun Zhao
Appl. Sci. 2024, 14(11), 4755; https://doi.org/10.3390/app14114755 - 31 May 2024
Viewed by 924
Abstract
The C+L band elastic optical networks (C+L-EONs) increase the network capacity significantly. However, the introduction of an L band enhances the inter-channel stimulated Raman scattering effect (ISRS), consequently deteriorating the quality of transmission (QoT) of the signal. Furthermore, spectrum allocation leads to spectrum [...] Read more.
The C+L band elastic optical networks (C+L-EONs) increase the network capacity significantly. However, the introduction of an L band enhances the inter-channel stimulated Raman scattering effect (ISRS), consequently deteriorating the quality of transmission (QoT) of the signal. Furthermore, spectrum allocation leads to spectrum fragmentation inevitably, which escalates the bandwidth blocking rate. In addition, in C+L-EONs, a single fiber carries more services, and once one of the links fails, a huge number of requests will be interrupted, resulting in huge economic losses. Therefore, this paper proposes a survivability routing, band, modulation, and spectrum allocation (RBMSA) algorithm that effectively guarantees service survivability and reduces the impact of ISRS and spectrum fragmentation. The algorithm employs shared backup path protection and a band partitioning method, whereby the spectrum resource of the primary path is assigned in the L band and the backup path is assigned in the C band in order to minimize the impact of ISRS on the QoT of the request while ensuring the survivability of the network. Furthermore, a fragmentation metric accounting for both the free and shared spectrum resource is proposed to mitigate both free and shared spectrum fragmentation. The simulation results reveal that the proposed RBMSA algorithm reduces the bandwidth blocking probability (BBP) and the fragmentation rate (FR) by 47.7% and 21.3%, respectively, and improves the optical signal-to-noise ratio (OSNR) by 4.17 dB in NSFNET. In COST239, the BBP, FR, and OSNR are 22.1%, 21.5%, and 4.71 dB, respectively. Full article
(This article belongs to the Section Optics and Lasers)
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<p>The example of calculating the weight of the route. (<b>a</b>) The network topology with 4 nodes and 5 links. (<b>b</b>) The occupancy of the spectrum resource in the network. (<b>c</b>) The alternative routes and corresponding parameters.</p>
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<p>The network topologies: (<b>a</b>) NSFNET network and (<b>b</b>) COST239 network.</p>
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<p>The bandwidth blocking probability in (<b>a</b>) NSFNET network and (<b>b</b>) COST239 network.</p>
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<p>The resource utilization in (<b>a</b>) the NSFNET network and (<b>b</b>) the COST239 network.</p>
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<p>The OSNR in (<b>a</b>) the NSFNET network and (<b>b</b>) the COST239 network.</p>
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<p>The fragmentation ratio in (<b>a</b>) the NSFNET network and (<b>b</b>) the COST239 network.</p>
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13 pages, 5830 KiB  
Article
Determination of Highly Transient Electric Field in Water Using the Kerr Effect with Picosecond Resolution
by Petr Hoffer, Václav Prukner, Garima Arora, Radek Mušálek and Milan Šimek
Plasma 2024, 7(2), 316-328; https://doi.org/10.3390/plasma7020018 - 22 Apr 2024
Cited by 1 | Viewed by 1808
Abstract
This study utilizes the Kerr effect in the analysis of a pulsed electric field (intensity ~108 V/m, limited by the liquid dielectric strength) in deionized water at the sub-nanosecond time scale. The results provide information about voltage waveforms at the field-producing anode [...] Read more.
This study utilizes the Kerr effect in the analysis of a pulsed electric field (intensity ~108 V/m, limited by the liquid dielectric strength) in deionized water at the sub-nanosecond time scale. The results provide information about voltage waveforms at the field-producing anode (160 kV peak, du/dt > 70 kV/ns). The analysis is based on detecting the phase shifts between measured and reference pulsed laser beams (pulse width, 35 ps; wavelength, 532 nm) using a Mach–Zehnder interferometer. The signal-to-noise ratio of the detected phase shift is maximized by an appropriate geometry of the field-producing anode, which creates a correctly oriented strong electric field along the interaction path and simultaneously does not electrically load the feeding transmission line. The described method has a spatial resolution of ~1 μm, and its time resolution is determined by the laser pulse duration. Full article
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<p>Simplified sketch of (<b>a</b>) the reactor chamber composed of a grounded stainless-steel body, windows for optical diagnostics, and a water inlet/outlet, and (<b>b</b>) the coax-based HV electrode (plate anode). Images (<b>c</b>,<b>d</b>) show examples of interferograms near the plate anode (visible as the dark silhouette) captured at zero voltage (<b>c</b>) and at 160 kV (<b>d</b>).</p>
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<p>Block scheme of the interferometric (Mach–Zehnder) setup: P—polarizer; A—analyzer; M1 and M2—mirrors; RB—reference beam; PB—probing beam; ChD—delay chamber; ChM—measurements chamber with the plate anode; BS1 and BS2—beam splitters; PMT—photomultiplier; L1 and L2—objective lenses; FID—high-voltage pulsed source; <span class="html-italic">CP</span>—signal from the capacitive probe.</p>
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<p>Typical waveforms of voltage acquired by the capacitive probe and the photomultiplier detecting the laser pulse.</p>
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<p>Orientation of axes with respect to the plate anode (<b>a</b>) and <span class="html-italic">z</span>–component of electric field in the <span class="html-italic">y</span>–<span class="html-italic">z</span> plane calculated at a voltage of 150 kV and corresponding ∆<span class="html-italic">n</span> determined by Equation (1) (<b>b</b>). The position of the electrode apex corresponds to <span class="html-italic">z</span> = 0, and vertical axes of symmetry correspond to <span class="html-italic">x</span> = 0 and <span class="html-italic">y</span> = 0.</p>
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<p>Estimation of contribution to the total phase shift of the probing beam at a voltage of 150 kV in the areas where the electric field is appreciable. Distribution of electric field around the anode plate in the <span class="html-italic">y–z</span> plane is indicated by the red arrows.</p>
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<p>Spectrum of the voltage pulse generated by the FID.</p>
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<p>Description of fringe pattern in a typical interferogram: fringe deviation at zero field due to optical system distortion (<b>a</b>) and fringe pattern destruction and shift due to electric field (time delay from the voltage pulse onset and voltage are 3 ns/154 kV) (<b>b</b>). The anode plate edge is outlined for better visibility. Vertical laser polarization.</p>
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<p>Examples of (<b>a</b>) single-corner discharge and (<b>b</b>) two-corner discharge. Peak electrode voltage is ~175 kV and time delay from the voltage pulse onset and laser is approximately 3 ns.</p>
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<p>Morphology of the electrode tip in the central area and edges. Macroscopic views (<b>a</b>–<b>c</b>,<b>g</b>–<b>i</b>) and detail (<b>d</b>–<b>f</b>). Yellow arrows in (<b>a</b>,<b>c</b>,<b>g</b>,<b>i</b>) point to the path on which the discharge was evidently preferentially formed.</p>
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<p>Series of interferograms demonstrating fringe distortion at different voltages and laser polarizations. The images do not preserve the original aspect ratio (larger horizontal scale) for better fringe shift visibility. The interferometer is set up such that the fringes always shift in the presence of electric field towards the electrode at the axis of symmetry.</p>
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<p>Time dependence of phase shift in both laser polarizations (<b>a</b>,<b>c</b>) and corresponding reconstructed electric field waveforms together with the voltage waveforms gained from the HV probe (<b>b</b>,<b>d</b>). The voltage amplitude was 128 kV (<b>a</b>,<b>b</b>) and 160 kV (<b>c</b>,<b>d</b>).</p>
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<p>Numerical simulations of the <span class="html-italic">z</span>-component of the electric field (full blue line) with the calculated rise in the phase shift (dashed black line) due to the Kerr effect along the path (of the laser beam) perfectly aligned with the <span class="html-italic">y</span>-axis (<b>a</b>), and along the path that slightly leaned in the <span class="html-italic">z</span>-direction causing apparent field distortion (<b>b</b>). The electrode voltage in the simulation is 160 kV.</p>
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28 pages, 10836 KiB  
Article
Fuzzy Entropy-Assisted Deconvolution Method and Its Application for Bearing Fault Diagnosis
by Di Pei, Jianhai Yue and Jing Jiao
Entropy 2024, 26(4), 304; https://doi.org/10.3390/e26040304 - 29 Mar 2024
Viewed by 1200
Abstract
Vibration signal analysis is an important means for bearing fault diagnosis. Affected by the vibration of other machine parts, external noise and the vibration transmission path, the impulses induced by a bearing defect in the measured vibrations are very weak. Blind deconvolution (BD) [...] Read more.
Vibration signal analysis is an important means for bearing fault diagnosis. Affected by the vibration of other machine parts, external noise and the vibration transmission path, the impulses induced by a bearing defect in the measured vibrations are very weak. Blind deconvolution (BD) methods can counteract the effect of the transmission path and enhance the fault impulses. Most BD methods highlight fault features of the filtered signals by impulse-featured objective functions (OFs). However, residual noise in the filtered signals has not been well tackled. To overcome this problem, a fuzzy entropy-assisted deconvolution (FEAD) method is proposed. First, FEAD takes advantage of the high noise sensitivity of fuzzy entropy (FuzzyEn) and constructs a weighted FuzzyEn–kurtosis OF to enhance the fault impulses while suppressing noise interference. Then, the PSO algorithm is used to iteratively solve the optimal inverse deconvolution filter. Finally, envelope spectrum analysis is performed on the filtered signal to realize bearing fault diagnosis. The feasibility of FEAD was first verified by the bearing fault simulation signals at constant and variable speeds. The bearing test signals from Case Western Reserve University (CWRU), the railway wheelset and the test bench validated the good performance of FEAD in fault feature enhancement. A comparison with and quantitative results for the other state-of-the-art BD methods indicated the superiority of the proposed method. Full article
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<p>The components and the mixed signals from bearing vibration models. (<b>a</b>,<b>b</b>) Fault impulses at CS and VS; (<b>c</b>,<b>d</b>) discrete harmonics at CS and VS; (<b>e</b>) random impulse; (<b>f</b>) white noise with <span class="html-italic">std</span> = 0.35; (<b>g</b>,<b>h</b>) mixed signals at CS and VS.</p>
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<p>The change rate of kurtosis and entropy indicators at different noise levels.</p>
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<p>Flowchart of the proposed FEAD bearing fault diagnosis method.</p>
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<p>The envelope spectrum of the CS simulation signal (the red dots mark the fault feature peaks herein and after).</p>
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<p>The process and results of FEAD for the CS simulation signal. (<b>a</b>) The fitness curve; (<b>b</b>,<b>c</b>) the optimal filter coefficients and its spectrum; and (<b>d</b>,<b>e</b>) the filtered signal and its envelope spectrum.</p>
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<p>The process and results of FEAD for the CS simulation signal. (<b>a</b>) The fitness curve; (<b>b</b>,<b>c</b>) the optimal filter coefficients and its spectrum; and (<b>d</b>,<b>e</b>) the filtered signal and its envelope spectrum.</p>
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<p>The order envelope spectrum of the VS simulation signal.</p>
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<p>The process and results of FEAD for the VS simulation signal. (<b>a</b>) The fitness curve; (<b>b</b>,<b>c</b>) the optimal filter coefficients and its spectrum; and (<b>d</b>,<b>e</b>) the filtered signal in the angular domain and its order envelope spectrum.</p>
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<p>The filtered signals and their envelope spectra from the CS simulation signal using comparison methods. (<b>a</b>,<b>b</b>) MEDA; (<b>c</b>,<b>d</b>) PSO-MEDA; (<b>e</b>,<b>f</b>) MCKD; and (<b>g</b>,<b>h</b>) MOMEDA.</p>
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<p>The filtered signals in the angular domain and their envelope spectra from the VS simulation signal using comparison methods. (<b>a</b>,<b>b</b>) MEDA; (<b>c</b>,<b>d</b>) PSO-MEDA; (<b>e</b>,<b>f</b>) MCKD; and (<b>g</b>,<b>h</b>) MOMEDA.</p>
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<p>The filtered signals in the angular domain and their envelope spectra from the VS simulation signal using comparison methods. (<b>a</b>,<b>b</b>) MEDA; (<b>c</b>,<b>d</b>) PSO-MEDA; (<b>e</b>,<b>f</b>) MCKD; and (<b>g</b>,<b>h</b>) MOMEDA.</p>
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<p>The vibration waveform and the envelope spectrum of the CWRU bearing ball fault data. (<b>a</b>) Time domain waveform and (<b>b</b>) envelope spectrum.</p>
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<p>The filtered signals and their envelope spectra from the CWRU bearing ball fault signal using different BD methods. (<b>a</b>,<b>b</b>) FEAD; (<b>c</b>,<b>d</b>) MEDA; (<b>e</b>,<b>f</b>) PSO-MEDA; (<b>g</b>,<b>h</b>) MCKD; and (<b>i</b>,<b>j</b>) MOMEDA.</p>
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<p>The filtered signals and their envelope spectra from the CWRU bearing ball fault signal using different BD methods. (<b>a</b>,<b>b</b>) FEAD; (<b>c</b>,<b>d</b>) MEDA; (<b>e</b>,<b>f</b>) PSO-MEDA; (<b>g</b>,<b>h</b>) MCKD; and (<b>i</b>,<b>j</b>) MOMEDA.</p>
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<p>The wheelset bearing detection device.</p>
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<p>The wheelset bearing with spalling on the inner race.</p>
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<p>The vibration waveform and the envelope spectrum of the faulty wheelset bearing. (<b>a</b>) Time domain waveform and (<b>b</b>) envelope spectrum.</p>
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<p>The filtered signals and their envelope spectra from the faulty wheelset bearing signal using different BD methods. (<b>a</b>,<b>b</b>) FEAD; (<b>c</b>,<b>d</b>) MEDA; (<b>e</b>,<b>f</b>) PSO-MEDA; (<b>g</b>,<b>h</b>) MCKD; and (<b>i</b>,<b>j</b>) MOMEDA.</p>
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<p>The EMU transmission test bench.</p>
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<p>The test bench bearing with a fault on the outer race.</p>
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<p>The speed curve (<b>a</b>), the vibration waveform in the angular domain (<b>b</b>), and the order envelope spectrum (<b>c</b>) of the test bench faulty bearing.</p>
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<p>The filtered signals in the angular domain and their envelope spectra from the test bench bearing signal using different BD methods. (<b>a</b>,<b>b</b>) FEAD; (<b>c</b>,<b>d</b>) MEDA; (<b>e</b>,<b>f</b>) PSO-MEDA; (<b>g</b>,<b>h</b>) MCKD; and (<b>i</b>,<b>j</b>) MOMEDA.</p>
Full article ">Figure 19 Cont.
<p>The filtered signals in the angular domain and their envelope spectra from the test bench bearing signal using different BD methods. (<b>a</b>,<b>b</b>) FEAD; (<b>c</b>,<b>d</b>) MEDA; (<b>e</b>,<b>f</b>) PSO-MEDA; (<b>g</b>,<b>h</b>) MCKD; and (<b>i</b>,<b>j</b>) MOMEDA.</p>
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