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Search Results (654)

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16 pages, 2295 KiB  
Article
Aberrant Responding in Hypothesis Testing: A Threat to Validity or Source of Insight?
by Georgios Sideridis and Mohammed H. Alghamdi
Behav. Sci. 2025, 15(3), 319; https://doi.org/10.3390/bs15030319 - 6 Mar 2025
Viewed by 27
Abstract
Aberrant responding poses a significant challenge in measurement and validity, often distorting well-established relationships between psychological and educational constructs. This study examines how aberrant response patterns influence the relationship between student–teacher relations and students’ perceptions of school safety. Using data from 6617 students [...] Read more.
Aberrant responding poses a significant challenge in measurement and validity, often distorting well-established relationships between psychological and educational constructs. This study examines how aberrant response patterns influence the relationship between student–teacher relations and students’ perceptions of school safety. Using data from 6617 students from the Saudi Arabia Kingdom from the 2022 Programme for International Student Assessment (PISA), we employed the cusp catastrophe model to evaluate the nonlinear dynamics introduced by aberrant responses, as measured by the U3 person-fit index and the number of Guttman errors. Theoretical and empirical support for the cusp model suggests that aberrance functions as a bifurcation parameter, shifting the relationship between student–teacher relations and perceived school safety from predictable linearity to chaotic instability when exceeding a critical threshold in aberrant responding. Results indicate that both the U3 index and the number of Guttman errors significantly contribute to response distortions, confirming the cusp model’s superiority over traditional linear and logistic alternatives. These findings suggest that ignoring aberrant responding risks misinterpreting data structures, while properly accounting for it through catastrophe models provides a more nuanced understanding of nonlinear system behavior in educational assessment. The study highlights the importance of person-fit statistics in psychometric evaluations and reinforces the predictive utility of nonlinear models in handling response distortions in large-scale assessments. Full article
(This article belongs to the Section Psychiatric, Emotional and Behavioral Disorders)
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<p>Thom’s theoretical formulation of the cusp catastrophe model.</p>
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<p>Density of outcome variable with dashed lines pointing to identified modes.</p>
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<p>Densities per area of the lower surface for the model using U3 as the bifurcation term. The respective estimates when the bifurcation term was the number of Guttman errors are shown in <a href="#app1-behavsci-15-00319" class="html-app">Appendix A</a>. The colored area indicates the densities within and outside the parts of the lower surface.</p>
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<p>Densities per area of the lower surface for the model using U3 as the bifurcation term. The respective estimates when the bifurcation term was the number of Guttman errors are shown in <a href="#app1-behavsci-15-00319" class="html-app">Appendix A</a>. The colored area indicates the densities within and outside the parts of the lower surface.</p>
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<p>Observations in the lower surface within and outside the bifurcation area for the cusp model with the U3 index. Darker colors point to observations that are present closer to the upper surface and the opposite.</p>
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<p>Oscillation of observations between upper and lower surfaces with U3 as the splitting factor.</p>
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<p>Densities for Model Using the Number of Guttman Errors as the Bifurcation Term. Color indicates part of the lower surface.</p>
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17 pages, 4359 KiB  
Article
Research on Fourier Transform Spectral Phase Correction Algorithm Based on CTKB-NCM
by Xiong Wang, Chunhui Yan, Zimin Huo, Pengzhang Dai and Dong Yao
Photonics 2025, 12(3), 219; https://doi.org/10.3390/photonics12030219 - 28 Feb 2025
Viewed by 158
Abstract
In Fourier Transform Spectrometers, phase errors in spectral measurement induce distortion in reconstructed spectra. Existing phase correction algorithms demonstrate insufficient precision in addressing both linear phase and instrumental phase components, resulting in limited applications for the restored spectra in the field of precision [...] Read more.
In Fourier Transform Spectrometers, phase errors in spectral measurement induce distortion in reconstructed spectra. Existing phase correction algorithms demonstrate insufficient precision in addressing both linear phase and instrumental phase components, resulting in limited applications for the restored spectra in the field of precision measurement. This paper proposes an algorithm called the Cross-Teager–Kaiser ψB Energy Operator–Nonlinear Calibration Model (CTKB-NCM) for phase error correction. The algorithm first uses the cross-Teager–Kaiser ψB energy operator (CTKB) method to correct linear phase errors, then applies the Nonlinear Calibration Model (NCM) to solve for the instrument phase correction parameters at each wavenumber, and finally uses the instrument phase correction parameters to correct the residual phase after the linear phase error has been corrected. The Rao algorithm is used to determine the optimal instrument phase correction parameters. Simulation experiments demonstrate that the CTKB-NCM method achieves an order-of-magnitude improvement in normalized reconstructed spectral accuracy for SO2 gas compared to the conventional Mertz method. Full article
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<p>The schematic of a Michelson-type time-modulated Fourier Transform Spectrometer.</p>
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<p>A block diagram of the CTKB-NCM phase correction algorithm structure.</p>
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<p>The linear phase error correction process of the CTKB method.</p>
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<p>A flowchart of the Rao algorithm.</p>
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<p>(<b>a</b>) A comparison of the normalized restored spectra after linear phase error correction using the CTKB method and the Mertz method; (<b>b</b>,<b>c</b>) comparisons of the local spectra after linear phase error correction by the two methods; (<b>d</b>) the difference between the normalized restored spectra of the two methods.</p>
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<p>The convergence curve of the objective function of the Rao algorithm.</p>
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<p>(<b>a</b>,<b>b</b>) Comparisons of the normalized restored spectra obtained from the SO<sub>2</sub> measurement spectrum after linear phase error correction using the CTKB method, with the instrument phase correction parameters calculated using the least squares method and the Rao algorithm, respectively. (<b>c</b>) A comparison of the normalized spectral reconstruction errors for the two methods mentioned above.</p>
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<p>The phase correction process of the CTKB-NMPRC algorithm.</p>
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<p>(<b>a</b>) Comparison of spectral restoration using CTKB-NCM, Mertz, and Forman Methods. (<b>b</b>,<b>c</b>) Local spectral restoration comparisons. (<b>d</b>) Comparison of restoration spectral errors among three methods.</p>
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20 pages, 15946 KiB  
Article
DVF-NET: Bi-Temporal Remote Sensing Image Registration Network Based on Displacement Vector Field Fusion
by Mingliang Xue, Yiming Zhang, Shucai Jia, Chong Cao, Lin Feng and Wanquan Liu
Sensors 2025, 25(5), 1380; https://doi.org/10.3390/s25051380 - 24 Feb 2025
Viewed by 232
Abstract
Accurate image registration is essential for various remote sensing applications, particularly in multi-temporal image analysis. This paper introduces DVF-NET, a novel deep learning-based framework for dual-temporal remote sensing image registration. DVF-NET integrates two displacement vector fields to address nonlinear distortions caused by significant [...] Read more.
Accurate image registration is essential for various remote sensing applications, particularly in multi-temporal image analysis. This paper introduces DVF-NET, a novel deep learning-based framework for dual-temporal remote sensing image registration. DVF-NET integrates two displacement vector fields to address nonlinear distortions caused by significant variations between images, enabling more precise image alignment. A key innovation of this method is the incorporation of a Structural Attention Module (SAT), which enhances the model’s ability to focus on structural features, improving the feature extraction process. Additionally, we propose a novel loss function design that combines multiple similarity metrics, ensuring more comprehensive supervision during training. Experimental results on various remote sensing datasets indicate that the proposed DVF-NET outperforms the existing methods in both accuracy and robustness, particularly when handling images with substantial geometric distortions such as tilted buildings. The results validate the effectiveness of our approach and highlight its potential for various remote sensing tasks, including change detection, land cover classification, and environmental monitoring. DVF-NET provides a promising direction for the advancement of remote sensing image registration techniques, offering both high precision and robustness in complex real-world scenarios. Full article
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<p>Illustration of some inconsistent factors. The area within the red box shows significant deformation. (<b>A</b>) Different image shadow contours caused by different shooting times; (<b>B</b>) building tilt caused by different shooting angles; (<b>C</b>) obstruction due to rain and fog causes the loss of features.</p>
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<p>The accuracy of registration varies severely with different building heights. This figure demonstrates the registration results of low, higher, and very high buildings, which are marked by different colors.</p>
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<p>The overall framework of the proposed network, consisting primarily of three parts: the backbone and two displacement vector field prediction modules. These output an affine matrix with 6 degrees of freedom and a projection matrix with 8 degrees of freedom, respectively. <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mi>a</mi> </msub> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>H</mi> <mo>×</mo> <mi>W</mi> <mo>×</mo> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mi>p</mi> </msub> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>H</mi> <mo>×</mo> <mi>W</mi> <mo>×</mo> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math> correspond to displacement vector fields for these matrices. STN (Spatial Transformer Network) [<a href="#B25-sensors-25-01380" class="html-bibr">25</a>] represents the specific spatial transformation network.</p>
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<p>The affine matrix prediction phase. Given the source image feature <math display="inline"><semantics> <msub> <mi>F</mi> <mi>S</mi> </msub> </semantics></math>, and the target image feature <math display="inline"><semantics> <msub> <mi>F</mi> <mi>T</mi> </msub> </semantics></math>, along with their respective structural image features, the process outputs an affine matrix <math display="inline"><semantics> <msub> <mi>T</mi> <mi>a</mi> </msub> </semantics></math> with 6 degrees of freedom.</p>
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<p>The projection matrix prediction phase. Given the source image feature <math display="inline"><semantics> <msub> <mi>F</mi> <mi>S</mi> </msub> </semantics></math> and the target image feature <math display="inline"><semantics> <msub> <mi>F</mi> <mi>T</mi> </msub> </semantics></math>, along with their respective structural image features, the process outputs a projection matrix <math display="inline"><semantics> <msub> <mi>T</mi> <mi>a</mi> </msub> </semantics></math> with 8 degrees of freedom.</p>
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<p>An overview of image pair generation is shown, with the blue section representing dataset construction and the yellow section indicating keypoint extraction.</p>
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<p>Registration visualization results: (<b>a</b>) source; (<b>b</b>) target; (<b>c</b>) SIFT; (<b>d</b>) Lofter; (<b>e</b>) Roma; (<b>f</b>) DAM-NET; (<b>g</b>) DVF-NET. SIFT encountered global misalignment, while the other methods could all complete the registration.</p>
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<p>Local comparison of feature-based and region-based models with DVF-NET on Google Earth dataset. The solid red box shows the stitching effect of the converted image and the target image: (<b>a</b>) Roma; (<b>b</b>) DAM-NET; (<b>c</b>) DNF-NET.</p>
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<p>Local comparison of feature-based and region-based models with DVF-NET in S2looking. Tthe solid red box shows the stitching effect of the converted image and the target image: (<b>a</b>) DAM-NET; (<b>b</b>) Roma; (<b>c</b>) DNF-NET.</p>
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<p>Comparison of reverse registration results in two datasets, where the blue part represents the corresponding section of the source image, and the solid red box shows the stitching effect of the converted image and the target image. The first two are from the Google Earth dataset, and the last one is from the S2looking dataset: (<b>a</b>) Roma; (<b>b</b>) DAM-NET; (<b>c</b>) DVF-NET.</p>
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<p>Semantic comparison results of the three methods for low-rise buildings. The red part of the figure represents the semantic map of the converted source image, and the blue part represents the difference between the semantic map of the converted source image and the target image. The smaller the proportion of the white area, the better the registration effect; the results of the percentage of white areas are shown below. (<b>A</b>) DAM-NET: 21.49%; (<b>B</b>) Roma: 19.26%; (<b>C</b>) DVF-NET: 16.30%.</p>
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<p>Semantic comparison results of the three methods for tall buildings. The red part of the figure represents the semantic map of the converted source image, and the blue part represents the difference between the semantic map of the converted source image and the target image. The smaller the proportion of the white area, the better the registration effect; the results of the percentage of white areas are shown below. (<b>a</b>) DAM-NET: 22.09%; (<b>b</b>) Roma: 20.34%; (<b>c</b>) DVF-NET: 16.89%.</p>
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<p>The effect of the number of keypoints on the model’s convergence speed is shown. It can be observed that the green line (<span class="html-italic">n</span> = 300) in the diagram converges to the lowest point first.</p>
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23 pages, 8186 KiB  
Article
How Does Land Finance Influence Vegetation Dynamics in China?
by Siqi Yan and Jian Wang
Land 2025, 14(3), 466; https://doi.org/10.3390/land14030466 - 23 Feb 2025
Viewed by 263
Abstract
Land-based financing plays an essential role in urbanization in the developing world, and it is widely recognized to have profound environmental effects. However, there have been relatively few research endeavors on the impact of land finance on vegetation dynamics. This study applies fixed [...] Read more.
Land-based financing plays an essential role in urbanization in the developing world, and it is widely recognized to have profound environmental effects. However, there have been relatively few research endeavors on the impact of land finance on vegetation dynamics. This study applies fixed effects models and an instrumental variable approach to examine the impact of land finance on vegetation status and mechanisms of influence, using data for 286 Chinese cities between 2011 and 2022. The nonlinear relationship between land finance and vegetation conditions at different levels of economic development is investigated by estimating panel threshold models. The findings show that land finance exerts an inhibiting impact on vegetation conditions. The restraining effect of land finance on vegetation status tends to be more pronounced in western China or in secondary industry-led cities. The analysis of mechanisms of influence indicates that land finance negatively affects vegetation conditions by speeding up urban expansion, suppressing innovation, reducing land use efficiency, and distorting the fiscal expenditure structure. The analysis of the threshold effect suggests that land finance exerts a stronger curbing effect on vegetation status as the economic development level rises. The findings have significant policy implications for deepening reform of the fiscal system and promoting vegetation protection and restoration. Full article
(This article belongs to the Special Issue Land Development and Investment)
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<p>Mechanisms through which land finance affects vegetation dynamics.</p>
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<p>Spatial patterns of the extent of local governments’ dependence on land finance in China between 2011 and 2022.</p>
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<p>Spatial patterns of the vegetation status in China between 2011 and 2022.</p>
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<p>Kernel density estimation for the extent of local governments’ dependence on land finance and vegetation status.</p>
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<p>LR statistics.</p>
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18 pages, 1858 KiB  
Article
The Design of a Low-Power Pipelined ADC for IoT Applications
by Junkai Zhang, Tao Sun, Zunkai Huang, Wei Tao, Ning Wang, Li Tian, Yongxin Zhu and Hui Wang
Sensors 2025, 25(5), 1343; https://doi.org/10.3390/s25051343 - 22 Feb 2025
Viewed by 375
Abstract
This paper proposes a low-power 10-bit 20 MS/s pipelined analog-to-digital converter (ADC) designed for the burgeoning needs of low-data-rate communication systems, particularly within the Internet of Things (IoT) domain. To reduce power usage, multiple power-saving techniques are combined, such as sample-and-hold amplifier-less (SHA-less) [...] Read more.
This paper proposes a low-power 10-bit 20 MS/s pipelined analog-to-digital converter (ADC) designed for the burgeoning needs of low-data-rate communication systems, particularly within the Internet of Things (IoT) domain. To reduce power usage, multiple power-saving techniques are combined, such as sample-and-hold amplifier-less (SHA-less) architecture, capacitor scaling, and dynamic comparators. In addition, this paper presents a novel operational amplifier (op-amp) with gain boosting, featuring a dual-input differential pair that enables internal pipeline stage switching, effectively alleviating the crosstalk and memory effects inherent in conventional shared op-amp configurations, thereby further reducing power consumption. A prototype ADC was fabricated in a 180 nm CMOS process and the core size was 0.333 mm2. The ADC implemented operated at a 20 MHz sampling rate under a 1.8 V supply voltage. It achieved a spurious-free dynamic range (SFDR) of 61.83 dB and a signal-to-noise-and-distortion ratio (SNDR) of 54.15 dB while demonstrating a maximum differential non-linearity (DNL) of 0.36 least significant bit (LSB) and a maximum integral non-linearity (INL) of 0.67 LSB. Notably, the ADC consumed less than 5 mW of power at the mentioned sampling frequency, showcasing excellent power efficiency. Full article
(This article belongs to the Section Electronic Sensors)
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<p>An overview of a low-power IoT vibration sensor network. (<b>a</b>) Subsurface seismic sensor deployment for vehicle/pedestrian vibration detection in a smart city, with LoRaWAN communication to an AI node. (<b>b</b>) Signal processing flow in a sensor node, highlighting the analog front-end and proposed low-power pipelined ADC for energy-efficient data conversion.</p>
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<p>Architecture of 10-bit pipelined ADC.</p>
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<p>Structure and timing of first stage and second stage.</p>
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<p>Structure of gate-boosted switch.</p>
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<p>Dual-input, differential-pair, gain-boosted, switched operational amplifier circuit.</p>
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<p>Switched-capacitor common-mode feedback circuit.</p>
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<p>(<b>a</b>) The dynamic comparator with a pre-amplifier and (<b>b</b>) differential-pair dynamic comparator.</p>
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<p>Die photo micrograph.</p>
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<p>Measured ADC output FFT spectra under (<b>a</b>) <math display="inline"><semantics> <msub> <mi>F</mi> <mi>S</mi> </msub> </semantics></math> = 20 MHz and <math display="inline"><semantics> <msub> <mi>F</mi> <mrow> <mi>I</mi> <mi>N</mi> </mrow> </msub> </semantics></math> = 1MHz; (<b>b</b>) <math display="inline"><semantics> <msub> <mi>F</mi> <mi>S</mi> </msub> </semantics></math> = 20 MHz and <math display="inline"><semantics> <msub> <mi>F</mi> <mrow> <mi>I</mi> <mi>N</mi> </mrow> </msub> </semantics></math> = 2.4 MHz; and (<b>c</b>) <math display="inline"><semantics> <msub> <mi>F</mi> <mi>S</mi> </msub> </semantics></math> = 20 MHz and <math display="inline"><semantics> <msub> <mi>F</mi> <mrow> <mi>I</mi> <mi>N</mi> </mrow> </msub> </semantics></math> = 3.6 MHz.</p>
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<p>Measured SNR, SNDR, and SFDR versus input frequency at 20 MS/s.</p>
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<p>(<b>a</b>) The measured DNL of the proposed ADC and (<b>b</b>) measured INL of the proposed ADC.</p>
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21 pages, 5358 KiB  
Article
Deep Learning-Based Feature Matching Algorithm for Multi-Beam and Side-Scan Images
by Yu Fu, Xiaowen Luo, Xiaoming Qin, Hongyang Wan, Jiaxin Cui and Zepeng Huang
Remote Sens. 2025, 17(4), 675; https://doi.org/10.3390/rs17040675 - 16 Feb 2025
Viewed by 299
Abstract
Side-scan sonar and multi-beam echo sounder (MBES) are the most widely used underwater surveying tools in marine mapping today. The MBES offers high accuracy in depth measurement but is limited by low imaging resolution due to beam density constraints. Conversely, side-scan sonar provides [...] Read more.
Side-scan sonar and multi-beam echo sounder (MBES) are the most widely used underwater surveying tools in marine mapping today. The MBES offers high accuracy in depth measurement but is limited by low imaging resolution due to beam density constraints. Conversely, side-scan sonar provides high-resolution backscatter intensity images but lacks precise positional information and often suffers from distortions. Thus, MBES and side-scan images complement each other in depth accuracy and imaging resolution. To obtain high-quality seafloor topography images in practice, matching between MBES and side-scan images is necessary. However, due to the significant differences in content and resolution between MBES depth images and side-scan backscatter images, they represent a typical example of heterogeneous images, making feature matching difficult with traditional image matching methods. To address this issue, this paper proposes a feature matching network based on the LoFTR algorithm, utilizing the intermediate layers of the ResNet-50 network to extract shared features between the two types of images. By leveraging self-attention and cross-attention mechanisms, the features of the MBES and side-scan images are combined, and a similarity matrix of the two modalities is calculated to achieve mutual matching. Experimental results show that, compared to traditional methods, the proposed model exhibits greater robustness to noise interference and effectively reduces noise. It also overcomes challenges, such as large nonlinear differences, significant geometric distortions, and high matching difficulty between the MBES and side-scan images, significantly improving the optimized image matching results. The matching error RMSE has been reduced to within six pixels, enabling the accurate matching of multi-beam and side-scan images. Full article
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<p>Schematic diagram of the feature matching network used in this paper.</p>
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<p>Feature extraction flowchart.</p>
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<p>Flowchart of the self-attention mechanism implementation.</p>
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<p>The implementation process of the cross-attention mechanism.</p>
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<p>Symmetric epipolar distance diagram.</p>
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<p>Sample map of the study area from partial multi-beam images. Figure (<b>a</b>) represents the Multi-beam image of the city wall area. Figure (<b>b</b>) represents the highly distorted multi-beam image of the urban area. Figure (<b>c</b>) represents the Multi-beam image of the urban canal area. Figure (<b>d</b>) represents the Multi-beam image of the urban area. Figure (<b>e</b>) represents the Multi-beam image of the urban reservoir area. Figure (<b>f</b>) represents the Multi-beam image of the mountainous area near the city.</p>
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<p>Sample side-scan sonar images from the study area. Figure (<b>a</b>) represents the side-scan sonar image of the city wall area. Figure (<b>b</b>) represents the highly distorted side-scan sonar image of the urban area. Figure (<b>c</b>) represents the side-scan sonar image of the urban canal area. Figure (<b>d</b>) represents the side-scan sonar image of the urban area. Figure (<b>e</b>) represents the side-scan sonar image of the urban reservoir area. Figure (<b>f</b>) represents the side-scan sonar image of the mountainous area near the city.</p>
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<p>The challenges in matching multi-beam and side-scan sonar images, the blue, red, and yellow boxes represent different transformation relationships in the feature points.</p>
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<p>Side-scan image to be excluded.</p>
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<p>(<b>a</b>) Self-built multi-beam image dataset. (<b>b</b>) Self-built side-scan image dataset.</p>
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<p>Comparison of matching results of different algorithms, where the matching lines in different colors represent the matching status of different feature points.</p>
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<p>Registration results for different network structures on three types of images. (<b>a</b>) Without self-attention mechanism. (<b>b</b>) Without cross-attention mechanism. (<b>c</b>) Without attention mechanism. (<b>d</b>) Our method. P1 represents the city near the city wall. P2 represents urban lakes. P3 represents urban area. The matching lines in different colors represent the matching status of different feature points.</p>
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<p>Matching results of the algorithm on different areas. (<b>a</b>,<b>d</b>) Urban area feature matching results. (<b>b</b>,<b>g</b>,<b>i</b>) Feature matching results for urban areas with significant distortions. (<b>c</b>,<b>f</b>) Matching results for urban lakes and canals. (<b>e</b>,<b>j</b>) Matching results for underwater hilly areas. (<b>h</b>) Underwater farmland area feature matching results. The matching lines in different colors represent the matching status of different feature points.</p>
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22 pages, 2349 KiB  
Article
Digital Real-Time Simulation and Power Quality Analysis of a Hydrogen-Generating Nuclear-Renewable Integrated Energy System
by Sushanta Gautam, Austin Szczublewski, Aidan Fox, Sadab Mahmud, Ahmad Javaid, Temitayo O. Olowu, Tyler Westover and Raghav Khanna
Energies 2025, 18(4), 937; https://doi.org/10.3390/en18040937 - 15 Feb 2025
Viewed by 572
Abstract
This paper investigates the challenges and solutions associated with integrating a hydrogen-generating nuclear-renewable integrated energy system (NR-IES) under a transactive energy framework. The proposed system directs excess nuclear power to hydrogen production during periods of low grid demand while utilizing renewables to maintain [...] Read more.
This paper investigates the challenges and solutions associated with integrating a hydrogen-generating nuclear-renewable integrated energy system (NR-IES) under a transactive energy framework. The proposed system directs excess nuclear power to hydrogen production during periods of low grid demand while utilizing renewables to maintain grid stability. Using digital real-time simulation (DRTS) in the Typhoon HIL 404 model, the dynamic interactions between nuclear power plants, electrolyzers, and power grids are analyzed to mitigate issues such as harmonic distortion, power quality degradation, and low power factor caused by large non-linear loads. A three-phase power conversion system is modeled using the Typhoon HIL 404 model and includes a generator, a variable load, an electrolyzer, and power filters. Active harmonic filters (AHFs) and hybrid active power filters (HAPFs) are implemented to address harmonic mitigation and reactive power compensation. The results reveal that the HAPF topology effectively balances cost efficiency and performance and significantly reduces active filter current requirements compared to AHF-only systems. During maximum electrolyzer operation at 4 MW, the grid frequency dropped below 59.3 Hz without filtering; however, the implementation of power filters successfully restored the frequency to 59.9 Hz, demonstrating its effectiveness in maintaining grid stability. Future work will focus on integrating a deep reinforcement learning (DRL) framework with real-time simulation and optimizing real-time power dispatch, thus enabling a scalable, efficient NR-IES for sustainable energy markets. Full article
(This article belongs to the Section B4: Nuclear Energy)
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<p>Transactive energy framework [<a href="#B8-energies-18-00937" class="html-bibr">8</a>].</p>
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<p>Simplified plot illustrating the increase in profitability of a nuclear power plant with hydrogen production [<a href="#B8-energies-18-00937" class="html-bibr">8</a>].</p>
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<p>Tightly coupled NR-IES [<a href="#B10-energies-18-00937" class="html-bibr">10</a>].</p>
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<p>DRL framework based on OpenAI Gym and Ray-RLlib [<a href="#B10-energies-18-00937" class="html-bibr">10</a>].</p>
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<p>Cumulative revenue with and without hydrogen IES [<a href="#B10-energies-18-00937" class="html-bibr">10</a>].</p>
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<p>Three-phase power conversion system with a hybrid active power filter.</p>
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<p>SCADA panel.</p>
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<p>Energy price data and load profile.</p>
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<p>Ramping factor.</p>
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<p>Circuit configuration of an active harmonic filter (AHF).</p>
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<p>(<b>a</b>) Reference current generator. (<b>b</b>) Current control.</p>
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<p>Hybrid active power filter—shunt active + shunt passive topology.</p>
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<p>Grid frequencies with and without an AHF.</p>
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<p>(<b>a</b>) Source current without a filter. (<b>b</b>) Source current with an AHF.</p>
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<p>Grid harmonic mitigation with an AHF.</p>
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<p>(<b>a</b>) Zoomed-in view of the electrolyzer profile for the first 48 h. (<b>b</b>) Power factor before and after HAPF implementation.</p>
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<p>Comparison of active filter currents.</p>
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23 pages, 6481 KiB  
Article
Nonlinear Quantization Method of SAR Images with SNR Enhancement and Segmentation Strategy Guidance
by Zijian Yao, Linlin Fang, Junxin Yang and Lihua Zhong
Remote Sens. 2025, 17(3), 557; https://doi.org/10.3390/rs17030557 - 6 Feb 2025
Viewed by 450
Abstract
The quantization process of synthetic aperture radar (SAR) images faces significant challenges due to their high dynamic range, resulting in notable quantization distortion. This not only degrades the visual quality of the quantized images but also severely impacts the accuracy of image interpretation. [...] Read more.
The quantization process of synthetic aperture radar (SAR) images faces significant challenges due to their high dynamic range, resulting in notable quantization distortion. This not only degrades the visual quality of the quantized images but also severely impacts the accuracy of image interpretation. To mitigate the distortion caused by uniform quantization and enhance visual quality, this paper introduced a novel nonlinear quantization framework via signal-to-noise ratio (SNR) enhancement and segmentation strategy guidance. This framework introduces guiding information to improve quantization performance in weak scattering regions. A histogram adjustment method is developed to incorporate the spatial information of SAR images into the quantization process to enhance the quantization performance, specifically within weak scattering regions. Additionally, the optimal quantizer is improved by refining the SNR distribution across quantization units, addressing imbalances in their allocation. Experimental results based on Gaofen-3 (GF-3) satellite data demonstrate that the proposed algorithm approaches the global quantization performance of optimal quantizers while achieving superior local quantization performance compared to existing methods. Full article
(This article belongs to the Section Remote Sensing Image Processing)
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<p>Overview of the nonlinear quantization method framework.</p>
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<p>Overall framework of the proposed method.</p>
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<p>Results of the dynamic range of SAR images and histogram proportion. (<b>a</b>) Dynamic range results of SAR images for different land cover types. (<b>b</b>) Histogram proportion of SAR images for different land cover types in the [1:1000] quantization level range.</p>
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<p>Extraction results of sparse strong scattering points. The orange regions indicate the distribution of strong scattering points, while the blue histograms represent the image histogram. (<b>a</b>) Histogram of the land scene. (<b>b</b>) Histogram of the coast scene. (<b>c</b>) Histogram of the ocean scene.</p>
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<p>Segmentation experiment results. (<b>a</b>,<b>d</b>,<b>g</b>) Original quantized images. (<b>b</b>,<b>e</b>,<b>h</b>) Histogram segmentation results. (<b>c</b>,<b>f</b>,<b>i</b>) Morphological transformation processing results.</p>
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<p>Histogram of fine-tuning experimental results. (<b>a</b>–<b>f</b>) Histogram fusion results of six different SAR coast scene images.</p>
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<p>Image quantization experimental results.</p>
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<p>Local effects of nonlinear quantization experiment. (<b>a</b>) Original image, with the selected weak scattering area indicated by a red box. (<b>b</b>) Uniform quantization. (<b>c</b>) Histogram equalization. (<b>d</b>) Logarithmic quantization. (<b>e</b>) Optimal quantization. (<b>f</b>) The algorithm proposed in this paper.</p>
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<p>Quantization distortion experimental results for each quantization levels.</p>
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<p>Q–SNR experimental results for each quantization level.</p>
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<p>Q–SNR experimental results at the quantization levels of [0, 3000].</p>
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<p>Ground truth and clustering results with different methods. (<b>a</b>) Original image. (<b>b</b>) Ground truth label. (<b>c</b>) Histogram equalization clustering. (<b>d</b>) Log quantization clustering. (<b>e</b>) Optimal quantization clustering. (<b>f</b>) Proposed method clustering.</p>
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<p>Comparisons of <math display="inline"><semantics> <msub> <mi>F</mi> <mn>1</mn> </msub> </semantics></math> score in different binary classifications with different methods. (<b>a</b>) <math display="inline"><semantics> <msub> <mi>F</mi> <mn>1</mn> </msub> </semantics></math> score curve of land classification. (<b>b</b>) <math display="inline"><semantics> <msub> <mi>F</mi> <mn>1</mn> </msub> </semantics></math> score curve of ocean classification.</p>
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14 pages, 3034 KiB  
Article
Implementation of a Current Harmonics Suppression Strategy for a Six-Phase Permanent Magnet Synchronous Motor
by Yu-Ting Lin, Jonq-Chin Hwang, Cheng-Ting Tsai and Cheng-Tsung Lin
Energies 2025, 18(3), 665; https://doi.org/10.3390/en18030665 - 31 Jan 2025
Viewed by 497
Abstract
This paper proposes a current harmonic suppression strategy that combines harmonic synchronous rotating frame (HSRF) current feedback control and back-electromotive force harmonic (BEMFH) feedforward compensation to suppress the fifth and seventh current harmonics of a six-phase permanent magnet synchronous motor (PMSM). The current [...] Read more.
This paper proposes a current harmonic suppression strategy that combines harmonic synchronous rotating frame (HSRF) current feedback control and back-electromotive force harmonic (BEMFH) feedforward compensation to suppress the fifth and seventh current harmonics of a six-phase permanent magnet synchronous motor (PMSM). The current harmonics of six-phase PMSMs vary with the current due to manufacturing imperfections and the inverter nonlinearity effect. Using fixed-parameter BEMFH feedforward compensation cannot completely eliminate current harmonics. This paper integrates a closed-loop harmonic current control strategy, using HSRF in the differential mode of the six-phase PMSM rotor rotating frame to effectively mitigate current harmonic variations caused by load changes. The controller adapts a Texas Instrument microcontroller featuring encoder interfaces, complementary pulse width modulation (PWM), and analog–digital converters (ADC) to simplify the board design. The rotor angle feedback is provided by a 12-pole resolver in conjunction with an Analog Device resolver-to-digital converter (RDC). The specifications of the six-phase PMSM are as follows: 12 poles, 1200 rpm, 200 A (rms), and 600 V DC bus. The total harmonic distortion (THD) of the phase current for harmonics below the 21st order was reduced from 31.71% to 4.84% under the test conditions of 1200 rpm rotor speed and 200 A peak phase current. Specifically, the fifth and seventh harmonics were reduced from 29.98% and 9.72% to 2.74% and 1.21%, respectively. These results validate the feasibility of the proposed current harmonic suppression strategy. Full article
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<p>The <span class="html-italic">dq</span>-axis in the rotor rotating frame and the <math display="inline"><semantics> <mrow> <mi>α</mi> <mi>β</mi> <mi>a</mi> </mrow> </semantics></math>-axis, <math display="inline"><semantics> <mrow> <mi>α</mi> <mi>β</mi> <mi>x</mi> </mrow> </semantics></math>-axis, <span class="html-italic">abc</span>-axis and <span class="html-italic">xyz</span>-axis in the stationary frame of the six-phase PMSM.</p>
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<p>The control block diagram of the CM and DM current controllers, including the fifth and seventh HSRFCC and BEMFHFC: (<b>a</b>) the main block diagram; (<b>b</b>) expansion of HSRFCC; (<b>c</b>) flow chart.</p>
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<p>The test platform: (<b>a</b>) the dynamometer, six−phase drive, and six−phase PMSM; (<b>b</b>) inside of the six−phase drive; (<b>c</b>) electrical diagram of the drive, laptop, DC power supply, and dynamometer.</p>
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<p>The test platform: (<b>a</b>) the dynamometer, six−phase drive, and six−phase PMSM; (<b>b</b>) inside of the six−phase drive; (<b>c</b>) electrical diagram of the drive, laptop, DC power supply, and dynamometer.</p>
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<p>The comparison of measured and simulated phase currents <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>a</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>b</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>x</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>y</mi> </msub> </semantics></math> before using BEMFHFC and HSRFCC: (<b>a</b>) simulated phase currents; (<b>b</b>) measured phase currents.</p>
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<p>The comparison of measured and simulated phase currents <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>a</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>b</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>x</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>y</mi> </msub> </semantics></math> after using BEMFHFC and HSRFCC: (<b>a</b>) simulated phase currents; (<b>b</b>) measured phase currents.</p>
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<p>The harmonic spectrum and THD of measured phase currents <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>a</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>b</mi> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>x</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>y</mi> </msub> </semantics></math> after using space BEMFHFC and HSRFCC: (<b>a</b>) <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>a</mi> </msub> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>b</mi> </msub> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>x</mi> </msub> </semantics></math>; (<b>d</b>) <math display="inline"><semantics> <msub> <mover accent="true"> <mi>i</mi> <mo stretchy="false">^</mo> </mover> <mi>y</mi> </msub> </semantics></math>.</p>
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31 pages, 7960 KiB  
Article
Supraharmonic Distortion at the Grid Connection Point of a Network Comprising a Photovoltaic System
by Anthoula Menti, Pavlos Pachos and Constantinos S. Psomopoulos
Energies 2025, 18(3), 564; https://doi.org/10.3390/en18030564 - 25 Jan 2025
Viewed by 527
Abstract
Grid-connected photovoltaic (PV) systems inject nonsinusoidal currents into the grid at the point of their connection. The technology of the inverter utilized for the conversion of DC power into AC is directly associated with distortion characteristics. Even though pulse-width-modulated (PWM) converters generate considerably [...] Read more.
Grid-connected photovoltaic (PV) systems inject nonsinusoidal currents into the grid at the point of their connection. The technology of the inverter utilized for the conversion of DC power into AC is directly associated with distortion characteristics. Even though pulse-width-modulated (PWM) converters generate considerably lower harmonic distortion than their predecessors, they are responsible for the emergence of a new power quality issue in distribution grids known as supraharmonics, which can cause problems such as overheating and malfunctions of equipment. PV systems are known sources of supraharmonics, but their impact has not yet been thoroughly researched. Due to the multitude of parameters affecting their performance, a more rigorous treatment is required compared to more common nonlinear devices. In this paper, emissions from a three-phase grid-connected PV system are examined by means of a dedicated simulation tool taking into account the specifics of inverter switching action without overly increasing computational cost. The impact of environmental parameters as well as factors affecting the switch control of the converter is investigated. The dependence of the supraharmonic emission of the PV system on the converter characteristics rather than environmental conditions is demonstrated. Furthermore, simulation studies on a network comprising the PV system and an additional supraharmonic-emitting system in simultaneous operation are conducted. Their combined effect on the distortion at the connection point of the network to the grid is assessed by means of a power flow-based approach, capable of quantifying interactions within this network. From the viewpoint of the grid, an increase of supraharmonic-related disturbance at low irradiance conditions is revealed. Full article
(This article belongs to the Section A2: Solar Energy and Photovoltaic Systems)
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<p>Equivalent circuit for the system under consideration.</p>
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<p>Approximation of daily variation of solar irradiance.</p>
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<p>Current waveforms at the output of the PV system (phases A, B and C) and associated frequency spectra, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>(<b>a</b>) Current (phase A) at the output of the PV inverter and its frequency spectrum, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>; (<b>b</b>) voltage (phase A) at the output of the PV system and its frequency spectrum, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>Current waveform (phase A) at PV system output and associated frequency spectrum at (<b>a</b>) 991 W/m<sup>2</sup>, (<b>b</b>) 924 W/m<sup>2</sup>, (<b>c</b>) 793 W/m<sup>2</sup>, (<b>d</b>) 609 W/m<sup>2</sup>, (<b>e</b>) 383 W/m<sup>2</sup>, and (<b>f</b>) 131 W/m<sup>2</sup>.</p>
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<p>Current waveform (phase A) at PV system output and associated frequency spectrum at (<b>a</b>) 991 W/m<sup>2</sup> and 30 °C, (<b>b</b>) 991 W/m<sup>2</sup> and 40 °C, (<b>c</b>) 609 W/m<sup>2</sup> and 30 °C, (<b>d</b>) 609 W/m<sup>2</sup> and 40 °C.</p>
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<p>PWM signal generation in the case of (<b>a</b>) natural sampling, (<b>b</b>) symmetrical regular sampling, and (<b>c</b>) asymmetrical regular sampling.</p>
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<p>Current (phase A) at the output of the PV inverter and its frequency spectrum in the case of (<b>a</b>) natural sampling, (<b>b</b>) symmetrical regular sampling, and (<b>c</b>) asymmetrical regular sampling, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>Current (phase A) at the output of the PV inverter and its frequency spectrum in the case of (<b>a</b>) symmetrical regular sampling with <span class="html-italic">T<sub>sample</sub></span> = <span class="html-italic">T<sub>c</sub></span>, (<b>b</b>) symmetrical regular sampling with <span class="html-italic">T<sub>sample</sub></span> = 4<span class="html-italic">T<sub>c</sub></span>, (<b>c</b>) asymmetrical regular sampling with <span class="html-italic">T<sub>sample</sub></span> = 7<span class="html-italic">T<sub>c</sub></span>/2, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>Current (phase A) at the output of the PV inverter and its frequency spectrum for (<b>a</b>) <span class="html-italic">t<sub>d</sub></span> = 0.005 <span class="html-italic">T<sub>c</sub></span>, (<b>b</b>) <span class="html-italic">t<sub>d</sub></span> = 0.010 <span class="html-italic">T<sub>c</sub></span> and (<b>c</b>) <span class="html-italic">t<sub>d</sub></span> = 0.015 <span class="html-italic">T<sub>c</sub></span>, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>(<b>a</b>) Current (phase A) at the output of the PV system and its frequency spectrum, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>, increased output filter resistance; (<b>b</b>) current (phase A) at the output of the PV inverter and its frequency spectrum, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>, increased output filter resistance.</p>
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<p>Current (phase A) at the output of the PV system and its frequency spectrum, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>, alternative <span class="html-italic">C<sub>f</sub></span>, <span class="html-italic">R<sub>f</sub></span> combination.</p>
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<p>Current (phase A) at the output of the inverter and its frequency spectrum with a load of (<b>a</b>) <span class="html-italic">R<sub>d</sub></span> = 20 Ω per phase, (<b>b</b>) <span class="html-italic">R<sub>d</sub></span> = 20 Ω, <span class="html-italic">L<sub>d</sub></span> = 0.03 H per phase connected in series, (<b>c</b>) no load, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>(<b>a</b>) Measurement results of the current of phase A at the PV system output at <span class="html-italic">G</span> = 927 W/m<sup>2</sup>; (<b>b</b>) simulated waveform of the current of phase A at the PV system output at <span class="html-italic">G</span> = 927 W/m<sup>2</sup>.</p>
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<p>Equivalent circuit for the extended system under consideration.</p>
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<p>Current waveform (phase A) and its frequency spectrum (<b>a</b>) at the output of the PV system inverter, (<b>b</b>) at the AC side of the rectifier of System 2, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>Current waveform (phase A) and its frequency spectrum (<b>a</b>) at the point of connection of the PV system, (<b>b</b>) at the point of connection of System 2, (<b>c</b>) at line segment 3, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>Voltage waveform (phase A) and its frequency spectrum (<b>a</b>) at the point of connection of the PV system, (<b>b</b>) at the point of connection of System 2, and (<b>c</b>) at the point of connection of the linear load, <span class="html-italic">G</span> = <span class="html-italic">G<sub>max</sub></span>.</p>
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<p>Current waveform (phase A) and its frequency spectrum (<b>a</b>) at the point of connection of the PV system, (<b>b</b>) at the point of connection of System 2, (<b>c</b>) at line segment 3, <span class="html-italic">G</span> = 609 W/m<sup>2</sup>.</p>
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20 pages, 11324 KiB  
Article
Power Quality Improvement with Three-Phase Shunt Active Power Filter Prototype Based on Harmonic Component Separation Method with Low-Pass Filter
by Marian Gaiceanu, Silviu Epure, Razvan Constantin Solea and Razvan Buhosu
Energies 2025, 18(3), 556; https://doi.org/10.3390/en18030556 - 24 Jan 2025
Viewed by 557
Abstract
This work contributes to both Romania’s and the European Union’s energy policies by highlighting the research results obtained within the Dunarea de Jos University of Galati, but also through the technological transfer of this knowledge to the industry. In order to improve the [...] Read more.
This work contributes to both Romania’s and the European Union’s energy policies by highlighting the research results obtained within the Dunarea de Jos University of Galati, but also through the technological transfer of this knowledge to the industry. In order to improve the power quality of the nonlinear loads connected to the electrical grid, a three-phase shunt active power filter prototype based on the Harmonic Component Separation Method with a Low-Pass Filter was used. The active power filter is connected at the Point of Common Coupling to compensate for individual loads or even all of them simultaneously. Therefore, active power filters can be used to compensate for the power factor and reduce the harmonic distortion of power supplies, or for processes subsequently connected to additional nonlinear loads, thus improving the energy efficiency. The shunt active power filter prototype is composed of the power side (three-phase insulated gate bipolar transistor bridge, DC link capacitor precharge system, inductive filter) and the control side (gate drive circuits, control subsystems, signal acquisition system). The filter control strategy is based on the principle of separating harmonic components with a low-pass filter, implemented by the authors on the industrial prototype. In this paper, the main technical features of the industrial shunt active power filter prototype are specified. The authors of this paper involved three cascaded control loops: the DC link voltage control loop, the shunt active power filter current control loop and the phase-locked loop. Both simulation and experimental results for the shunt-type active power filter prototype were obtained. By analyzing the obtained waveforms of the power supply source in two cases (with and without an active power filter), a decrease in the total harmonic distortion was demonstrated, both the voltage harmonic distortion factor THDu and the current harmonic distortion factor THDi in the case of the active power filter connection. By using the Field-Programmed Gate Array processing platform, the powerful computational speed features were exploited to implement the active shunt power filter control on an experimental test bench. Conducting source current harmonics mitigation increased the efficiency of the power system by decreasing the respective harmonic Joule losses. The energy-saving feature led to the increased added value of the parallel active power filter. Through the performed laboratory tests, the authors demonstrated the feasibility of the proposed control solution for the industrial prototype. In accordance with the European Union’s Research and Technological Development Policy, the development of an innovation ecosystem was taken into consideration. The unified and efficient integration of all the specific actors (enterprises, research institutes, universities and entrepreneurs) in innovation was achieved. Full article
(This article belongs to the Section F: Electrical Engineering)
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<p>The Harmonic Component Separation Method with a Low-Pass Filter.</p>
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<p>The MATLAB-Simulink implementation of the harmonic improvement power system (HCSLPF).</p>
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<p>Block diagram of the generation of current references for the active power filter using Harmonic Component Extraction.</p>
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<p>The MATLAB-Simulink implementation of the harmonic improvement control system by using the HCSLPF control method.</p>
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<p>The operation of the DC voltage loop of the SAPF.</p>
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<p>The power supply waveforms: three phase voltages (blue) and three phase currents (red).</p>
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<p>The nonlinear three-phase load currents.</p>
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<p>The three-phase reference currents generated by the HCSLPF.</p>
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<p>The measured three-phase SAPF currents.</p>
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<p>The selected FFT window (red line) from the power supply phase current analysis (blue line) without an SAPF connection (red marked signal).</p>
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<p>The FFT analyses of the power supply phase current without an SAPF connection.</p>
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<p>The selected FFT window (red line) from the power supply phase current (blue line) analysis with an SAPF connection (red marked signal).</p>
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<p>The FFT analyses of the power supply phas1 current with an SAPF connection.</p>
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<p>Comparative side-by-side THD analyses of the power supply phase current (<b>a</b>) without an SAPF connection and (<b>b</b>) with an SAPF connection.</p>
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<p>The FPGA control loop implementation of the SAPF industrial prototype.</p>
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<p>The implemented three-phase FPGA PWM signal generator.</p>
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<p>The implemented FPGA PLL circuit.</p>
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<p>The grid three-phase voltage with a nonlinear load.</p>
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<p>The grid phasor harmonics.</p>
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<p>The grid phase voltage and phase current without an SAPF connection.</p>
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<p>The nonlinear three-phase load current system.</p>
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<p>The harmonics content of the load current, THD<sub>i</sub> = 29.1%.</p>
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<p>The harmonics content of the power supply voltage, THD<sub>u</sub> = 0.9%, without an SAPF connection.</p>
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<p>The grid three-phase voltage system with an SAPF connection.</p>
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<p>The harmonics content of the grid phase current with an SAPF connection: THD<sub>i</sub> = 5.6%.</p>
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<p>The harmonics content of the grid phase voltage with an SAPF connection: THD<sub>u</sub> = 0.2%.</p>
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<p>The grid phase voltage and current with an SAPF connection.</p>
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<p>Comparative experimental results of the harmonic distortion (without the SAPF and with the SAPF) for grid current signals.</p>
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<p>Comparative experimental results of the harmonic distortion (without the SAPF and with the SAPF) for grid voltage signals.</p>
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<p>The Human Machine Interface on the front of the SAPF prototype (<b>a</b>) and the Point of Common Coupling (<b>b</b>).</p>
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12 pages, 6137 KiB  
Article
520 μJ Microsecond Burst-Mode Pulse Fiber Amplifier with GHz-Tunable Intra-Burst Pulse and Flat-Top Envelope
by Yanran Gu, Xinyue Niu, Muyu Yi, Jinmei Yao, Langning Wang, Tao Xun and Jinliang Liu
Photonics 2025, 12(2), 97; https://doi.org/10.3390/photonics12020097 - 22 Jan 2025
Viewed by 766
Abstract
We present a 520 μJ microsecond burst-mode pulse fiber amplifier with a GHz-tunable intra-burst repetition rate and a nearly flat-top pulse envelope. The amplifier architecture comprises a microsecond pulse seed, a high-bandwidth electro-optic modulator (EOM), two pre-amplifier stages, a waveform-compensated acoustic-optic modulator (AOM), [...] Read more.
We present a 520 μJ microsecond burst-mode pulse fiber amplifier with a GHz-tunable intra-burst repetition rate and a nearly flat-top pulse envelope. The amplifier architecture comprises a microsecond pulse seed, a high-bandwidth electro-optic modulator (EOM), two pre-amplifier stages, a waveform-compensated acoustic-optic modulator (AOM), and two main amplifier stages. To address amplified spontaneous emission (ASE) and nonlinear effects, a multistage synchronous pumping scheme that achieved a maximum energy output of 520 μJ and has a peak power of 160 W was used. To produce a flat-topped burst pulse envelope, the AOM generates an editable waveform with a leading edge and a high trailing edge to compensate for waveform distortion, resulting in a 5 μs nearly flat-top pulse envelope at maximum energy. The laser provides an adjustable intra-burst pulse repetition rate range of 1–5 GHz through the high-bandwidth EOM modulation. The intra-burst pulse jitter time of the laser remains below 4.31 ps at different frequencies. Moreover, the beam quality of the amplifier is M2x = 1.04 and M2y = 1.1. This amplifier exhibits promising potential and can be further amplified as an optical drive source for high-power, large-bandwidth microwave photon (MWP) radar applications. Meanwhile, it is also potentially applicable as a pulse source for high-speed optical communications, the high-precision processing of special materials, and LIDAR ranging. Full article
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<p>Schematic diagram of high-power microwave photon radar, DC: direct-current, PCSS: photoconductive semiconductor switch, RF: radio frequency.</p>
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<p>(<b>a</b>) Schematic diagram of microsecond burst-mode GHz-tunable fiber laser system. ISO: isolator, EOM: electro-optic modulator, TWDM: taper/wavelength division multiplexing, IBPTWDM: isolator/bandpass/taper/wavelength division multiplexing, IBP: isolator and bandpass filter hybrid, YSF: ytterbium-doped single-mode fiber, YDF: ytterbium-doped fiber; AOM: acousto-optic modulator, LD: laser diode, AWG: arbitrary waveform generator, SG: signal generator, (<b>b</b>) schematic diagram of the synchronously triggered time sequence for each stage.</p>
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<p>(<b>a</b>) The characteristics of the single pulse seed, (<b>b</b>) the spectrum of the microsecond pulse seed, (<b>c</b>) the AWG pre-compensation signal waveform, (<b>d</b>) pre-compensated temporal waveform of the burst-mode pulse seed. The pre-compensated temporal shape of the burst-mode laser is depicted in (<b>d</b>), where the temporal shape aligns with the AWG compensation signal. The FWHM of the pre-compensated envelope is 4.2 μs. The secondary pre-amplifier achieves a maximum energy of 26.6 μJ.</p>
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<p>(<b>a</b>) The output energy in relation to the input pump energy of the amplifier, (<b>b</b>) the spectrum of the amplifier at different output energy levels, (<b>c</b>) the temporal envelope evolution of the burst-mode pulse at different energy levels, (<b>d</b>) the long-term stability of the burst-mode laser measured over 10 min.</p>
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<p>(<b>a</b>) The adjustability of the burst-mode laser frequency within the range of 1–5 GHz, (<b>b</b>) intra-burst pulse period of 200 ps—1 ns is tunable at various intra-burst repetition rates of 1–5 GHz with a sinusoidal waveform.</p>
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<p>(<b>a</b>) Schematic diagram of TIE measurement method, (<b>b</b>) TIE at different frequencies of 1–5 GHz at different stages of the amplifier.</p>
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<p>(<b>a</b>) Experimental configuration of beam quality analysis for the burst-mode laser, (<b>b</b>) the beam quality test results.</p>
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17 pages, 1899 KiB  
Article
Deep Learning-Based Gain Estimation for Multi-User Software-Defined Radios in Aircraft Communications
by Viraj K. Gajjar and Kurt L. Kosbar
Signals 2025, 6(1), 3; https://doi.org/10.3390/signals6010003 - 22 Jan 2025
Viewed by 502
Abstract
It may be helpful to integrate multiple aircraft communication and navigation functions into a single software-defined radio (SDR) platform. To transmit these multiple signals, the SDR would first sum the baseband version of the signals. This outgoing composite signal would be passed through [...] Read more.
It may be helpful to integrate multiple aircraft communication and navigation functions into a single software-defined radio (SDR) platform. To transmit these multiple signals, the SDR would first sum the baseband version of the signals. This outgoing composite signal would be passed through a digital-to-analog converter (DAC) before being up-converted and passed through a radio frequency (RF) amplifier. To prevent non-linear distortion in the RF amplifier, it is important to know the peak voltage of the composite. While this is reasonably straightforward when a single modulation is used, it is more challenging when working with composite signals. This paper describes a machine learning solution to this problem. We demonstrate that a generalized gamma distribution (GGD) is a good fit for the distribution of the instantaneous voltage of the composite waveform. A deep neural network was trained to estimate the GGD parameters based on the parameters of the modulators. This allows the SDR to accurately estimate the peak of the composite voltage and set the gain of the DAC and RF amplifier, without having to generate or directly observe the composite signal. Full article
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<p>Typical communication links of an aircraft [<a href="#B3-signals-06-00003" class="html-bibr">3</a>].</p>
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<p>SDR-based implementation of an aircraft’s communication links [<a href="#B3-signals-06-00003" class="html-bibr">3</a>]. An SDR generates and sums multiple baseband waveforms, and the resulting composite signal is then amplified and up-converted for transmission.</p>
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<p>Time domain representation of a composite signal. Its peak amplitude, <span class="html-italic">u</span>, is key to selecting the DAC’s input gain, <span class="html-italic">G</span>, so that the waveform uses the DAC’s full range.</p>
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<p>Frequency domain representation of a composite signal [<a href="#B3-signals-06-00003" class="html-bibr">3</a>].</p>
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<p>Four common distributions that closely fit composite signals [<a href="#B3-signals-06-00003" class="html-bibr">3</a>].</p>
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<p>DNN used to estimate GGD’s parameters.</p>
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<p>Average MAE training and validation loss trends across 10-fold cross-validation.</p>
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<p><math display="inline"><semantics> <msup> <mi>R</mi> <mn>2</mn> </msup> </semantics></math> plot for each of the individual parameters of the GGD, estimated using the DNN.</p>
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<p>Trend in MAE on the hold-out test set with increasing amounts of training data, expressed as a percentage of the total dataset used for training.</p>
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<p>Trends in MAE as more component signals are added to the composite signal.</p>
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<p>Trends in <math display="inline"><semantics> <msup> <mi>R</mi> <mn>2</mn> </msup> </semantics></math> score as more component signals are added to the composite signal.</p>
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<p><math display="inline"><semantics> <msup> <mi>R</mi> <mn>2</mn> </msup> </semantics></math> score comparison for S-DNN and DNN.</p>
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<p>CDF of the combined signal estimated using the DNN.</p>
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14 pages, 3064 KiB  
Article
Ring Beam Modulation-Assisted Laser Welding on Dissimilar Materials for Automotive Battery
by Se-Hoon Choi, Jong-Hyun Kim and Hae-Woon Choi
J. Manuf. Mater. Process. 2025, 9(2), 28; https://doi.org/10.3390/jmmp9020028 - 21 Jan 2025
Viewed by 776
Abstract
This paper investigates Ring Beam Modulation-assisted Laser (RBML) welding as a novel approach for joining dissimilar materials, specifically aluminum and copper, which are essential in high-performance applications such as electric vehicle batteries and aerospace components. The study aims to address challenges such as [...] Read more.
This paper investigates Ring Beam Modulation-assisted Laser (RBML) welding as a novel approach for joining dissimilar materials, specifically aluminum and copper, which are essential in high-performance applications such as electric vehicle batteries and aerospace components. The study aims to address challenges such as thermal mismatches, brittle intermetallic compounds, and structural defects that hinder traditional welding methods. The research combines experimental and computational analyses to evaluate the impact of heat input distributions and laser modulation parameters on weld quality and strength. Three welding cases are compared: fixed center beam with variable ring beam outputs, variable center beam with fixed ring outputs, and a wobble-mode beam to enhance interfacial bonding. Computational modeling supports the optimization process by simulating heat flows and material responses, exploring various shape factors, and guiding parameter selection. Key findings include a nonlinear relationship between heat input and welding strength across the cases. Case 1 demonstrates improved weld strength with higher ring beam input, while Case 2 achieves excellent reliability with relatively lower inputs. Case 3 introduces wobble welding, yielding superior resolution and consistent weld quality. These results confirm that precise ring beam modulation enhances weld reliability, minimizes thermal distortions, and optimizes energy consumption. The manuscript advances the state of knowledge in laser welding technology by demonstrating a scalable, energy-efficient method for joining dissimilar materials. This contribution supports the fabrication of lightweight, high-reliability assemblies, paving the way for innovative applications in the automotive, medical, aerospace, and shipbuilding industries. Full article
(This article belongs to the Special Issue Advances in Dissimilar Metal Joining and Welding)
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<p>Principle of the idea (<b>a</b>) dual-beam laser welding for dissimilar materials (<b>b</b>) Energy propagation of the Ring Beam Modulation-assisted Laser Welding (<b>c</b>) Weld reliability improvement through ring laser.</p>
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<p>Experimental setup (<b>a</b>) Robot arm-based laser welding (<b>b</b>) Jig for placing target specimen (<b>c</b>) Scanning head aligned to the target (<b>d</b>) Laser variation.</p>
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<p>(<b>a</b>) Cross-sections of ring beam modulation-assisted laser welding (<b>b</b>) Tensile load and bead width vs. heat input for Case 1 (<b>c</b>) Tensile load and bead width vs. heat input for Case 2.</p>
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<p>(<b>a</b>) Cross-sections of wobble welding (<b>b</b>) Unit tensile load (kgf/mm) and bead width vs. wobble amplitude for case 3 (<b>c</b>) Welding surfaces with various wobbling amplitudes.</p>
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<p>(<b>a</b>) Simulated thermal distribution (<b>b</b>) Summary of tensile load vs. heat input for each case.</p>
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13 pages, 3880 KiB  
Article
Remote Sensing Target Tracking Method Based on Super-Resolution Reconstruction and Hybrid Networks
by Hongqing Wan, Sha Xu, Yali Yang and Yongfang Li
J. Imaging 2025, 11(2), 29; https://doi.org/10.3390/jimaging11020029 - 21 Jan 2025
Viewed by 1160
Abstract
Remote sensing images have the characteristics of high complexity, being easily distorted, and having large-scale variations. Moreover, the motion of remote sensing targets usually has nonlinear features, and existing target tracking methods based on remote sensing data cannot accurately track remote sensing targets. [...] Read more.
Remote sensing images have the characteristics of high complexity, being easily distorted, and having large-scale variations. Moreover, the motion of remote sensing targets usually has nonlinear features, and existing target tracking methods based on remote sensing data cannot accurately track remote sensing targets. And obtaining high-resolution images by optimizing algorithms will save a lot of costs. Aiming at the problem of large tracking errors in remote sensing target tracking by current tracking algorithms, this paper proposes a target tracking method combined with a super-resolution hybrid network. Firstly, this method utilizes the super-resolution reconstruction network to improve the resolution of remote sensing images. Then, the hybrid neural network is used to estimate the target motion after target detection. Finally, identity matching is completed through the Hungarian algorithm. The experimental results show that the tracking accuracy of this method is 67.8%, and the recognition identification F-measure (IDF1) value is 0.636. Its performance indicators are better than those of traditional target tracking algorithms, and it can meet the requirements for accurate tracking of remote sensing targets. Full article
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<p>Overall system framework.</p>
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<p>Residual module network structure.</p>
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<p>Hybrid neural network structure.</p>
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<p>Gated cycle unit, GRU.</p>
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<p>Target tracking effect without overshoot reconstruction.</p>
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<p>Target tracking effect after overshoot reconstruction.</p>
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<p>Target tracking effect after overshoot reconstruction.</p>
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