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Search Results (4,058)

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15 pages, 1992 KiB  
Article
Multi-Channel Vibration Measurements Based on a Self-Mixing Vertical-Cavity Surface-Emitting Laser Array
by Wei Xia, Jingyu Yu, Sunan Shao, Zhengyu Qian, Hui Hao, Ming Wang and Dongmei Guo
Photonics 2025, 12(3), 178; https://doi.org/10.3390/photonics12030178 - 21 Feb 2025
Abstract
This paper studied a multi-channel self-mixing interferometric vibration measurement system based on a vertical-cavity surface-emitting laser array. A 1 × 8 laser array was utilized to irradiate multiple positions of a vibrating target to establish independent measurement channels. The reflected light beams, carrying [...] Read more.
This paper studied a multi-channel self-mixing interferometric vibration measurement system based on a vertical-cavity surface-emitting laser array. A 1 × 8 laser array was utilized to irradiate multiple positions of a vibrating target to establish independent measurement channels. The reflected light beams, carrying the vibration information of each position, were redirected back into the laser and coherently mixed with the original optical field, generating the self-mixing interference. The interferometric signals were measured by monitoring the junction voltage variations across the terminals of the VCSEL array. A denoising filtering method based on the variational mode decomposition with Hausdorff distance was proposed to improve the signal-to-noise ratio. Furthermore, the vibration waveforms of different positions were reconstructed using the Hilbert transform-based orthogonal phase demodulation technology. Both simulations on synthetic signals and experiments with real datasets were conducted to validate the feasibility and stability of the proposed method. Due to the array detection configuration, the system boasted a simple and compact structure, low power consumption, and easy extensibility, laying the groundwork for high accuracy and multi-dimensional vibration detection in industrial applications. Full article
21 pages, 6412 KiB  
Article
Inverse Synthetic Aperture Radar Image Multi-Modal Zero-Shot Learning Based on the Scattering Center Model and Neighbor-Adapted Locally Linear Embedding
by Xinfei Jin, Hongxu Li, Xinbo Xu, Zihan Xu and Fulin Su
Remote Sens. 2025, 17(4), 725; https://doi.org/10.3390/rs17040725 - 19 Feb 2025
Abstract
Inverse Synthetic Aperture Radar (ISAR) images are extensively used in Radar Automatic Target Recognition (RATR) for non-cooperative targets. However, acquiring training samples for all target categories is challenging. Recognizing target classes without training samples is called Zero-Shot Learning (ZSL). When ZSL involves multiple [...] Read more.
Inverse Synthetic Aperture Radar (ISAR) images are extensively used in Radar Automatic Target Recognition (RATR) for non-cooperative targets. However, acquiring training samples for all target categories is challenging. Recognizing target classes without training samples is called Zero-Shot Learning (ZSL). When ZSL involves multiple modalities, it becomes Multi-modal Zero-Shot Learning (MZSL). To achieve MZSL, a framework is proposed for generating ISAR images with optical image aiding. The process begins by extracting edges from optical images to capture the structure of ship targets. These extracted edges are used to estimate the potential locations of the target’s scattering centers. Using the Geometric Theory of Diffraction (GTD)-based scattering center model, the edges’ ISAR images are generated from the scattering centers. Next, a mapping is established between the edges’ ISAR images and the actual ISAR images. Neighbor-Adapted Local Linear Embedding (NALLE) generates pseudo-ISAR images for the unseen classes by combining the edges’ ISAR images with the actual ISAR images from the seen classes. Finally, these pseudo-ISAR images serve as training samples, enabling the recognition of test samples. In contrast to the network-based approaches, this method requires only a limited number of training samples. Experiments based on simulated and measured data validate the effectiveness. Full article
(This article belongs to the Section Remote Sensing Image Processing)
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<p>The flowchart of the proposed algorithm.</p>
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<p>Optical image with its edges. (<b>a</b>) Optical image. (<b>b</b>) Edges of the optical image.</p>
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<p>Process of NALLE generating a patch <math display="inline"><semantics> <msubsup> <mi>y</mi> <mi>I</mi> <mi>n</mi> </msubsup> </semantics></math> from <math display="inline"><semantics> <msubsup> <mi>y</mi> <mi>O</mi> <mi>n</mi> </msubsup> </semantics></math> (with <math display="inline"><semantics> <mrow> <mi>K</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>), where the arrows indicate the process flow. To clearly distinguish between the optical and ISAR images, the left side shows patches from optical images in grayscale, while the right side shows patches from ISAR images in pseudo-color.</p>
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<p>The 3D models, ISAR images, and optical images for simulated ships. (<b>a</b>–<b>c</b>) are the 3D model, ISAR image, and optical image of Target 1; (<b>d</b>–<b>f</b>) are the 3D model, ISAR image, and optical image of Target 2; (<b>g</b>–<b>i</b>) are the 3D model, ISAR image, and optical image of Target 3.</p>
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<p>Output of each step in the proposed method for Target 3. (<b>a</b>) Optical image with an attitude similar to the ISAR image. (<b>b</b>) Grayscale image with pseudocolor after preprocessing. (<b>c</b>) ISAR image of edges generated by the scattering center models. (<b>d</b>) Pseudo-ISAR image synthesized by the NALLE algorithm. (<b>e</b>) ISAR image with an attitude similar to the optical image in (<b>a</b>).</p>
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<p>Mean and standard deviation of the accuracy for the simulated data with varying <span class="html-italic">K</span>. (<b>a</b>) Mean accuracy. (<b>b</b>) Standard deviation of accuracy.</p>
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<p>Mean and standard deviation of accuracy for the simulated data with varying patch sizes. (<b>a</b>) Mean accuracy for the unseen class. (<b>b</b>) Mean accuracy for all targets. (<b>c</b>) Standard deviation of accuracy for the unseen class. (<b>d</b>) Standard deviation of accuracy for all targets.</p>
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<p>Optical and ISAR images of the measured ships. (<b>a</b>–<b>c</b>) are the optical images of barque, geared bulk carrier, and gearless bulk carrier, respectively; (<b>d</b>–<b>f</b>) are the ISAR images of barque, geared bulk carrier, and gearless bulk carrier, respectively.</p>
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<p>Output of each step in the proposed method for the gearless bulk carrier. (<b>a</b>) Optical image with an attitude similar to the ISAR image. (<b>b</b>) Grayscale image with pseudocolor after preprocessing. (<b>c</b>) ISAR image of edges generated by the scattering center models. (<b>d</b>) Pseudo-ISAR image synthesized by the NALLE algorithm. (<b>e</b>) ISAR image with an attitude similar to the optical image in (<b>a</b>).</p>
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<p>Mean and standard deviation of the accuracy for the measured data with varying <span class="html-italic">K</span>. (<b>a</b>) Mean accuracy. (<b>b</b>) Standard deviation of accuracy.</p>
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<p>Mean and standard deviation of accuracy for the measured data with varying patch sizes. (<b>a</b>) Mean accuracy for the unseen class. (<b>b</b>) Mean accuracy for all targets. (<b>c</b>) Standard deviation of accuracy for the unseen class. (<b>d</b>) Standard deviation of accuracy for all targets.</p>
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18 pages, 307 KiB  
Article
Who Will Author the Synthetic Texts? Evoking Multiple Personas from Large Language Models to Represent Users’ Associative Thesauri
by Maxim Bakaev, Svetlana Gorovaia and Olga Mitrofanova
Big Data Cogn. Comput. 2025, 9(2), 46; https://doi.org/10.3390/bdcc9020046 - 18 Feb 2025
Abstract
Previously, it was suggested that the “persona-driven” approach can contribute to producing sufficiently diverse synthetic training data for Large Language Models (LLMs) that are currently about to run out of real natural language texts. In our paper, we explore whether personas evoked from [...] Read more.
Previously, it was suggested that the “persona-driven” approach can contribute to producing sufficiently diverse synthetic training data for Large Language Models (LLMs) that are currently about to run out of real natural language texts. In our paper, we explore whether personas evoked from LLMs through HCI-style descriptions could indeed imitate human-like differences in authorship. For this end, we ran an associative experiment with 50 human participants and four artificial personas evoked from the popular LLM-based services: GPT-4(o) and YandexGPT Pro. For each of the five stimuli words selected from university websites’ homepages, we asked both groups of subjects to come up with 10 short associations (in Russian). We then used cosine similarity and Mahalanobis distance to measure the distance between the association lists produced by different humans and personas. While the difference in the similarity was significant for different human associators and different gender and age groups, neither was the case for the different personas evoked from ChatGPT or YandexGPT. Our findings suggest that the LLM-based services so far fall short at imitating the associative thesauri of different authors. The outcome of our study might be of interest to computer linguists, as well as AI/ML scientists and prompt engineers. Full article
9 pages, 1545 KiB  
Proceeding Paper
The Influence of Mechanochemical Synthesis Method on Photodegradability Characteristics of Hydroxyapatite/Zinc Oxide Composite
by Cristina Rodica Dumitrescu, Florina-Diana Gheorghe, Monica Matei, Larisa-Mădălina Ștefan and Elena Holban
Environ. Earth Sci. Proc. 2025, 33(1), 3; https://doi.org/10.3390/eesp2025033003 - 18 Feb 2025
Abstract
The ZnO/hydroxyapatite nanocomposite was prepared by attrition in a planetary mill from hydroxyapatite (HA) and ZnO nanopowders. The photocatalytic degradation of synthetic dye, methyl orange (MO), was evaluated under stirring and UV irradiations by measuring the spectroscopically UV-VIS absorbance of the solution in [...] Read more.
The ZnO/hydroxyapatite nanocomposite was prepared by attrition in a planetary mill from hydroxyapatite (HA) and ZnO nanopowders. The photocatalytic degradation of synthetic dye, methyl orange (MO), was evaluated under stirring and UV irradiations by measuring the spectroscopically UV-VIS absorbance of the solution in order to determine the remanent dye concentration. The samples CZH3 (75% ZnO) and CZH4 (25% ZnO) highlighted the best MO retention from aqueous solution by adsorption and photodegradation effects. The high absorbance of the proposed nanocomposites showed their potential to be used as photocatalysts for wastewater treatment to enable the retention of organic pollutants. Full article
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<p>The variation in the MO concentration in the residual aqueous solution during the irradiation time.</p>
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<p>First-order kinetics of the photocatalytic degradation of MO.</p>
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<p>Thermogravimetric and differential scanning calorimetry variation for composite samples after 4 h of UV irradiation time.</p>
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<p>X-Ray Diffraction plot (<b>a</b>,<b>d</b>) and comparative XRD patterns for composite samples CHZ1-CHZ5 after immersion in MO aq. sol. for 4 h irradiation time, MO dye powder, HA, and ZnO powders before UV treatment; (<b>b</b>) insert detail for 2<span class="html-italic">θ</span> 19–35°; (<b>c</b>) XRD plot for HA powder before and after immersion for 4 h irradiation time.</p>
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22 pages, 645 KiB  
Article
Comparative Analysis of Servitization in European Union Countries Using Hellwig’s Synthetic Measure of Development
by Małgorzata Kołodziejczak
Sustainability 2025, 17(4), 1683; https://doi.org/10.3390/su17041683 - 18 Feb 2025
Abstract
The purpose of this paper is to evaluate and compare the degree of servitization of the economies of European Union countries and to assess the importance of servitization for sustainable development. This study used Eurostat data from the years 2000 and 2023. Using [...] Read more.
The purpose of this paper is to evaluate and compare the degree of servitization of the economies of European Union countries and to assess the importance of servitization for sustainable development. This study used Eurostat data from the years 2000 and 2023. Using Hellwig’s synthetic measure of development, four groups of countries differing in the degree of servitization in each of the years studied were created and then compared in the context of the differences between them, including population density, the share of the service sector in employment and gross value-added creation, and the level of gross value added created by the service sector per capita. The results showed that a high degree of servitization characterizes mainly the rich countries of the EU-15, while a lower one applies mainly to the countries of Central and Eastern Europe. The service sector increased its share in employment, structure, and gross value-added creation during the period under review. High population density was also a factor conducive to the development of services, but its increase did not always coexist with an increase in the degree of servitization of the economy. Servitization drives development and facilitates optimal use of resources. However, high levels of servitization are not always reflected in good values of sustainable development. Servitization processes can be stimulated by adequate economic development policies, but the methods and actions taken in this regard should be adapted to the level of economic development and the specifics of each country. Full article
(This article belongs to the Special Issue Advanced Studies in Economic Growth, Environment and Sustainability)
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<p>Types of countries by degree of servitization in 2023.</p>
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12 pages, 426 KiB  
Review
Corneal Allogenic Intrastromal Ring Segments: A Literature Review
by Issac Levy, Ritika Mukhija and Mayank A. Nanavaty
J. Clin. Med. 2025, 14(4), 1340; https://doi.org/10.3390/jcm14041340 - 18 Feb 2025
Abstract
Background: Corneal allogenic intrastromal ring segments (CAIRSs) offer a novel, biocompatible alternative to synthetic intracorneal ring segments (ICRSs). This review aims to evaluate the clinical outcomes of CAIRS. Methods: Inclusion criteria were studies with a minimum of 20 eyes and six months of [...] Read more.
Background: Corneal allogenic intrastromal ring segments (CAIRSs) offer a novel, biocompatible alternative to synthetic intracorneal ring segments (ICRSs). This review aims to evaluate the clinical outcomes of CAIRS. Methods: Inclusion criteria were studies with a minimum of 20 eyes and six months of follow up. The primary outcome measure was uncorrected distance visual acuity (UDVA). The secondary outcomes were a change in corrected distance visual acuity (CDVA), spherical equivalent (SE), mean keratometry (K-mean), maximum keratometry (K-max), K1, K2, and pachymetry. Results: The primary outcome UDVA improved from 0.83 ± 0.15 to 0.40 ± 0.08 logMAR (p = 0.01), while CDVA improved from 0.52 ± 0.22 to 0.19 ± 0.09 logMAR (p = 0.01). K-max decreased from 57.8 ± 1.09 D to 53.57 ± 2.66 D (p < 0.01), and K-mean reduced from 49.27 ± 0.28 D to 45.30 ± 1.46 D (p < 0.01). An average of 84.92% ± 11.4% of eyes had an improvement in UDVA. No major complications or significant visual acuity deterioration were reported. Conclusions: CAIRSs serve as an alternative to synthetic ICRSs and even corneal transplantation in some cases. They represent a safe, effective, and biocompatible promising advancement in corneal ectasia management to improve visual acuity and corneal topography with minimal complications. Full article
(This article belongs to the Section Ophthalmology)
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<p>Study Flowchart.</p>
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13 pages, 3133 KiB  
Article
Lippia sidoides Cham. Compounds Induce Biochemical Defense Mechanisms Against Curvularia lunata sp. in Maize Plants
by Bruna Leticia Dias, Talita Pereira de Souza Ferreira, Mateus Sunti Dalcin, Dalmarcia de Souza Carlos Mourão, Paulo Ricardo de Sena Fernandes, Taila Renata Neitzke, João Victor de Almeida Oliveira, Tiago Dias, Luis Oswaldo Viteri Jumbo, Eugênio Eduardo de Oliveira and Gil Rodrigues dos Santos
J 2025, 8(1), 7; https://doi.org/10.3390/j8010007 - 17 Feb 2025
Abstract
Corn (Zea mays L.) productivity is often compromised by phytosanitary challenges, with fungal disease like Curvularia leaf spot being particularly significant. While synthetic fungicides are commonly used, there is growing interest in exploring alternative compounds that are effective against pathogens, ensure food [...] Read more.
Corn (Zea mays L.) productivity is often compromised by phytosanitary challenges, with fungal disease like Curvularia leaf spot being particularly significant. While synthetic fungicides are commonly used, there is growing interest in exploring alternative compounds that are effective against pathogens, ensure food safety, and have low toxicity to non-target organisms. In this study, we examined the biochemical changes in corn plants treated with Lippia sidoides essential oil and its major compound, thymol. Both treatments serve as preventive measures for inoculated plants and induced resistance. We tested five concentrations of each product in in vivo experiments. After evaluating the area under the disease progress curve, we analyzed leaf samples for enzymatic activities, including superoxide dismutase, catalase, ascorbate peroxidase, and chitinase. Phytoalexin induction was assessed using soybean cotyledons and sorghum mesocotyls. Cytotoxicity tests revealed lower toxicity at concentrations below 50 µL/mL. Both essential oil and thymol stimulated the production of reactive oxygen species, with thymol primarily activating catalase and L. sidoides oil increasing ascorbate peroxidase levels. Both thymol and L. sidoides were also key activators of chitinase. These findings suggest that L. sidoides essential oil and thymol are promising candidates for developing biological control products to enhance plant defense against pathogens. Full article
(This article belongs to the Special Issue Feature Papers of J—Multidisciplinary Scientific Journal in 2024)
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<p>Area under the disease progress curve (AUDPC) for maize plants treated with <span class="html-italic">Lippia sidoides</span> essential oil and thymol at different concentrations (<b>A</b>), and the AUDPC over the time in the promissory concentration (50 µL/mL) in maize treated plants and untreated plants (<b>B</b>). Each symbol shows the mean (±SD) of three replicates.</p>
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<p>Induction of phytoalexins in soybeans and sorghum treated with <span class="html-italic">Lippia sidoides</span> essential oil and thymol at different concentrations; production of glyceollin in soybean cotyledons (<b>A</b>) and production of 3-deoxyanthocyanin in sorghum mesocotyls (<b>B</b>). Each symbol shows the mean (±SD) of three replicates.</p>
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<p>Enzymatic activity of superoxide dismutase (<b>A</b>), catalase (<b>B</b>), ascorbate peroxidase (<b>C</b>), and chitinase (<b>D</b>) in maize plants treated with essential oil (<span class="html-italic">Lippia sidoides</span>) and thymol. The comparison includes plants inoculated only with the pathogen (<span class="html-italic">Curvularia lunata)</span> or those that received preventive treatments with essential oil (<span class="html-italic">L. sidoides</span> + <span class="html-italic">C. lunata</span>) and thymol (Thymol + <span class="html-italic">C. lunata</span>). Bars represent the mean (±SD) of three replicates. Different letters indicate statistical differences according to Tukey’s test (<span class="html-italic">p</span> &lt; 0.050).</p>
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<p>In vitro analysis of cytotoxicity in peripheral blood mononuclear cells (PBMC) at different concentrations of <span class="html-italic">L. sidoides</span> and thymol. The bars represent the mean (±SD) of five replicates. Connecting lines indicate a statistical difference in Tukey’s test (<span class="html-italic">p</span> &lt; 0.05).</p>
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24 pages, 11822 KiB  
Article
Electricity Data Quality Enhancement Strategy Based on Low-Rank Matrix Recovery
by Guo Xu, Xinliang Teng, Lei Zhang and Jianjun Xu
Energies 2025, 18(4), 944; https://doi.org/10.3390/en18040944 - 16 Feb 2025
Abstract
Electricity consumption data form the foundation for the efficient and reliable operation of smart grids and are a critical component for ensuring effective data mining. However, due to factors such as meter failures and extreme weather conditions, anomalies frequently occur in the data, [...] Read more.
Electricity consumption data form the foundation for the efficient and reliable operation of smart grids and are a critical component for ensuring effective data mining. However, due to factors such as meter failures and extreme weather conditions, anomalies frequently occur in the data, which adversely impact the performance of data-driven applications. Given the near full-rank nature of low-voltage distribution area electricity consumption data, this paper employs clustering to enhance the low-rank property of the data. Addressing common issues such as missing data, sparse noise, and Gaussian noise in electricity consumption data, this paper proposes a multi-norm optimization model based on low-rank matrix theory. Specifically, the truncated nuclear norm is used as an approximation of matrix rank, while the L1-norm and F-norm are employed to constrain sparse noise and Gaussian noise, respectively. The model is solved using the Alternating Direction Method of Multipliers (ADMM), achieving a unified framework for handling missing data and noise processing within the model construction. Comparative experiments on both synthetic and real-world datasets demonstrate that the proposed method can accurately recover measurement data under various noise contamination scenarios and different distributions of missing data. Moreover, it effectively separates principal components of the data from noise contamination. Full article
(This article belongs to the Special Issue Artificial Intelligence Technologies Applied to Smart Grids)
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<p>Common data missing and noisy scenarios.</p>
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<p>Singular values of electricity consumption data matrix for different number of users in 30 days.</p>
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<p>Singular values of electricity consumption data matrix of 500 users under different time windows.</p>
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<p>Framework diagram of low-rank matrix data repair strategy based on clustering and truncation nuclear norm.</p>
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<p>Matrix element decomposition of electricity consumption data in low-voltage station area.</p>
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<p>Tuning of the regularization parameter <math display="inline"><semantics> <mi>δ</mi> </semantics></math>.</p>
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<p>(<b>a</b>) Comparison of the Root Mean Squared Error (RMSE) of different methods on the synthetic matrix under various missing rates. (<b>b</b>) Box plot of the mean and standard deviation of RMSE for TNN over 50 runs under different missing rates.</p>
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<p>(<b>a</b>) RMSE under varying matrix dimensions, <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>σ</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>. (<b>b</b>) RMSE under varying matrix ranks, <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>=</mo> <mi>n</mi> <mo>=</mo> <mn>300</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>σ</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>. (<b>c</b>) RMSE under varying noise levels, <math display="inline"><semantics> <mrow> <mi>m</mi> <mo>=</mo> <mi>n</mi> <mo>=</mo> <mn>300</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>.</p>
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<p>Recovery accuracy (RMSE and RRE) of different methods under various random missing rates without noise.</p>
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<p>Recovery performance of electricity consumption data for one user over 30 days at a 20% missing rate without noise.</p>
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<p>Recovery accuracy (RMSE and RRE) of different methods under various continuous missing intervals without noise.</p>
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<p>Noise separation performance for Gaussian and impulse noise without missing data.</p>
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<p>Comparison of Data Recovery Performance Under Mixed Noise and Different Random Missing Rates.</p>
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<p>Comparison of data recovery performance under mixed noise and different continuous missing intervals.</p>
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21 pages, 20678 KiB  
Article
Estimation of Equivalent Pore Aspect Ratio in Rock Physics Models and Validation Using Digital Rocks
by Luiz Eduardo Queiroz, Dario Grana, Celso Peres Fernandes, Tapan Mukerji, Leandro Passos de Figueiredo and Iara Frangiotti Mantovani
Geosciences 2025, 15(2), 67; https://doi.org/10.3390/geosciences15020067 - 15 Feb 2025
Abstract
Complex pore structures with multiple inclusions challenge the predictive accuracy of rock physics models. This study introduces a novel method for estimating a single equivalent pore aspect ratio that optimizes rock physics model predictions by minimizing discrepancies with experimental measurements in porous rocks [...] Read more.
Complex pore structures with multiple inclusions challenge the predictive accuracy of rock physics models. This study introduces a novel method for estimating a single equivalent pore aspect ratio that optimizes rock physics model predictions by minimizing discrepancies with experimental measurements in porous rocks with multiple inclusions with variable aspect ratios and proportions. The proposed methodology uses digital rock physics numerical simulations for validation. A comparative analysis is conducted between the equivalent aspect ratio derived from optimized rock physics models, numerical simulations, and the aspect ratio distribution estimated from digital rock samples. The approach is tested on both synthetic and real core samples, demonstrating its robustness and applicability to field data, including core samples and well log data. The validation results confirm that the method enhances predictive accuracy and offers a versatile framework for addressing pore complexity in subsurface rock formations. Full article
(This article belongs to the Section Geophysics)
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<p>Sensitivity of equivalent pore aspect ratio (EPAR) to RPM parameters. The EPAR values are obtained by optimizing the aspect ratio value of a single inclusion. The EPAR values are plotted as function of the volume fraction of the inclusions with aspect ratio <math display="inline"><semantics> <msub> <mi>α</mi> <mn>2</mn> </msub> </semantics></math>. Their variations are shown with respect to multiple values of the following parameters: porosity <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math> (<b>a</b>), matrix bulk modulus <math display="inline"><semantics> <msub> <mi>K</mi> <mi>m</mi> </msub> </semantics></math> (<b>b</b>), matrix shear modulus <math display="inline"><semantics> <msub> <mi>μ</mi> <mi>m</mi> </msub> </semantics></math> (<b>c</b>), aspect ratio of inclusion 1 <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math> (<b>d</b>), and aspect ratio of inclusion 2 <math display="inline"><semantics> <msub> <mi>α</mi> <mn>2</mn> </msub> </semantics></math> (<b>e</b>). In each plot, one parameter varies, whereas the others are kept constant and equal to the reference parameters.</p>
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<p>Equivalent pore aspect ratio (EPAR) for porous medium with inclusions of aspect ratios <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>α</mi> <mn>2</mn> </msub> </semantics></math> and variable volumetric proportions for different rock physics models. The colored lines represent predictions for different values of (<b>a</b>) porosity, (<b>b</b>) <math display="inline"><semantics> <msub> <mi>α</mi> <mn>2</mn> </msub> </semantics></math>, and (<b>c</b>) <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math>. In each plot, one parameter varies, whereas the others are kept constant and equal to the reference parameters.</p>
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<p>EPAR for porous rocks with 3 inclusion types: (<b>a</b>) EPAR variations for variable inclusion proportions and (<b>b</b>) EPAR variations in limiting cases with two inclusions only.</p>
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<p>Example of synthetic digital sample with ellipsoidal inclusions.</p>
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<p>Comparison between RPM predictions and DRP numerical simulations for synthetic digital images with constant aspect ratio for bulk and shear moduli. The stars represent the values of the numerical simulations, and the lines represent the RPM predictions.</p>
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<p>Relative error between RPM predictions and DRP numerical simulations for synthetic digital images for bulk and shear moduli.</p>
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<p>Comparison between RPM predictions and DRP numerical simulations for synthetic digital images with two inclusion types with aspect ratios <math display="inline"><semantics> <mrow> <msub> <mi>α</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.9</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>α</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math> for bulk and shear moduli. The stars represent the values of the numerical simulations, and the lines represent the RPM predictions.</p>
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<p>Bulk and shear moduli calculated using DRP numerical simulations in GeoDict. The stars represent the calculated porosity and elastic moduli of each sub-sample; the colors represent each sample type. The dashed-dotted lines represent the RPM predictions assuming different mineralogical compositions consistent with the samples for three different values of aspect ratios equal to 0.1, 0.2, and 0.3.</p>
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<p>Estimated EPAR of digital images of 80 sub-samples for four RPMs. Each color represents a different rock type.</p>
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<p>Estimated bulk and shear moduli of digital images of 80 sub-samples for four RPMs. Circles indicate values of elastic moduli numerically calculated using DRP; crosses indicate elastic moduli calculated using RPMs with the calculated EPARs. Each color represents a different rock type.</p>
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<p>Aspect ratio distribution calculated from digital image analysis: on the (<b>left</b>), we show the distribution of aspect ratios; on the (<b>right</b>), we show the volume-weighted distribution of aspect ratios for sample BVE from lower Barra Velha formation (blue histograms) and sample ITP from Itapema formation (orange histograms).</p>
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<p>Pore space separation into individual objects (3D and 2D views) or sample BVE from lower Barra Velha formation (<b>left</b>) and sample ITP from Itapema formation (<b>right</b>). Each color represents an object considered as an individual pore.</p>
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<p>Measured and computed log data. From (<b>left</b>) to (<b>right</b>): porosity, estimated EPAR, and bulk and shear moduli. Black lines represent well logs, blue lines represent RPM predictions using EPAR, and golden lines represent EPAR mean values for each formation. The background colors represent stratigraphic zones corresponding to the intervals upper and lower Barra Velha and Itapema, respectively.</p>
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<p>Crossplot of bulk modulus versus porosity for well log data. The smaller dots represent well log measurements, the larger dots represent the laboratory measurements in core samples, and the colored lines represent the rock physics model for different values of the aspect ratio. Two thin sections from core samples illustrate the different pore structure and shape in the stratigraphic zones. The colors represent three stratigraphic zones corresponding to the intervals upper and lower Barra Velha and Itapema.</p>
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26 pages, 14781 KiB  
Article
Combined Motion Compensation Method for Long Synthetic Aperture Radar Based on Subaperture Processing
by Yuan Zhang, Limin Huang, Zhichao Xu, Zihao Wang and Biao Chen
J. Mar. Sci. Eng. 2025, 13(2), 355; https://doi.org/10.3390/jmse13020355 - 14 Feb 2025
Abstract
Long synthetic aperture radar (SAR) offers the advantage of achieving higher resolution by utilizing longer synthetic aperture times, which makes it a promising technology for ocean observation in the future. However, compared to SAR systems with shorter synthetic aperture times, it suffers more [...] Read more.
Long synthetic aperture radar (SAR) offers the advantage of achieving higher resolution by utilizing longer synthetic aperture times, which makes it a promising technology for ocean observation in the future. However, compared to SAR systems with shorter synthetic aperture times, it suffers more severely from issues such as image defocusing, blurring and artifacts during the observation of maritime targets, due to motion errors. To improve the quality of SAR imaging against motion errors in long synthetic aperture time scenarios, this paper proposes a combined motion compensation (MOCO) method based on subaperture processing. The method first divides the full aperture data into several subapertures. Within each subaperture, the platform is assumed to move at approximately constant velocity. The major imaging step is then combined with two motion compensation operations, which are performed individually within each subaperture. Then, the processed subaperture data are stitched together, and finally, the residual errors are compensated by the third MOCO, resulting in the final image. By simulating maritime observation targets with point targets, simulation results demonstrate that the proposed MOCO algorithm effectively reduce the influence of motion errors, suppress the sidelobe interference to the imaging, and improve the focusing accuracy. Compared with other classical MOCO algorithms, the ISLR_r and ISLR_a metrics show improvements of 0.2662 and 0.8170 dB, respectively. Further verification of the proposed method is conducted by processing the imaging results of measured sea surface data. The proposed algorithm produces clearer wave textures and achieves better imaging performance on targets such as ships in the sea. This result validates the effectiveness and superiority of the proposed method. The proposed method effectively addresses the need for high-precision motion error compensation in high-resolution imaging within long synthetic aperture time system. Full article
(This article belongs to the Special Issue Ocean Observations)
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<p>Synthetic aperture illustration.</p>
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<p>SAR geometry model with platform motion errors.</p>
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<p>Position of four point targets.</p>
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<p>The raw echo signal of point targets with motion errors.</p>
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<p>The simulated imaging results of point targets with motion errors without motion compensation.</p>
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<p>Flowchart of SAR combined MOCO method.</p>
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<p>Subaperture processing schematic diagram.</p>
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<p>Spectral division schematic diagram.</p>
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<p>The raw echo signal after subaperture division.</p>
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<p>The subaperture data after the first range compression, envelope correction and the first MOCO.</p>
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<p>The subaperture data after the SRC.</p>
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<p>The subaperture data after RCMC.</p>
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<p>The subaperture data after the second MOCO.</p>
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<p>The data after the subaperture stitching.</p>
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<p>The data after the third MOCO.</p>
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<p>The final imaging result.</p>
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<p>The upsampling result of the point target.</p>
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<p>Flowchart of frequency-domain block-by-block algorithm.</p>
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<p>Flowchart of frequency-division algorithm.</p>
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<p>The imaging result of the two classical algorithms (<b>a</b>) the imaging result of the frequency-domain block-by-block algorithm; (<b>b</b>) the imaging result of the frequency-division algorithm.</p>
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<p>Azimuth profile of the point target.</p>
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<p>The real sea surface imaging result of the four algorithms (<b>a</b>) the imaging result of the range Doppler algorithm (without MOCO); (<b>b</b>) the imaging result of the frequency-domain block-by-block algorithm; (<b>c</b>) the imaging result of the frequency-division algorithm; (<b>d</b>) the imaging result of the proposed algorithm.</p>
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<p>The real sea surface imaging result of the four algorithms (<b>a</b>) the imaging result of the range Doppler algorithm (without MOCO); (<b>b</b>) the imaging result of the frequency-domain block-by-block algorithm; (<b>c</b>) the imaging result of the frequency-division algorithm; (<b>d</b>) the imaging result of the proposed algorithm.</p>
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15 pages, 3565 KiB  
Article
pH Measurements Using Leaky Waveguides with Synthetic Hydrogel Films
by Victoria Wensley, Nicholas J. Goddard and Ruchi Gupta
Micromachines 2025, 16(2), 216; https://doi.org/10.3390/mi16020216 - 14 Feb 2025
Abstract
Leaky waveguides (LWs) are low-refractive-index films deposited on glass substrates. In these, light can travel in the film while leaking out at the film–substrate interface. The angle at which light can travel in the film is dependent on its refractive index and thickness, [...] Read more.
Leaky waveguides (LWs) are low-refractive-index films deposited on glass substrates. In these, light can travel in the film while leaking out at the film–substrate interface. The angle at which light can travel in the film is dependent on its refractive index and thickness, which can change with pH when the film is made of pH-responsive materials. Herein, we report an LW comprising a waveguide film made of a synthetic hydrogel containing the monomers acrylamide and N-[3-(dimethylamino)propyl]methacrylamide (DMA) and a bisacrylamide crosslinker for pH measurements between 4 and 8. The response of the LW pH sensor was reversible and the response times were 0.90 ± 0.14 and 2.38 ± 0.22 min when pH was changed from low to high and high to low, respectively. The reported LW pH sensor was largely insensitive to typical concentrations of common interferents, including sodium chloride, urea, aluminum sulfate, calcium chloride, and humic acid. Compared to a glass pH electrode, the measurement range is smaller but is close to the range required for monitoring the pH of drinking water. The pH resolution of the hydrogel sensor was ~0.004, compared to ~0.01 for the glass electrode. Full article
(This article belongs to the Special Issue Manufacturing and Application of Advanced Thin-Film-Based Device)
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<p>A schematic showing the casting methods used for the fabrication of LWs.</p>
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<p>A schematic of the LW instrument.</p>
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<p>A schematic of a simplest LW (<b>a</b>) without and (<b>b</b>) with an equilateral prism where the red line with arrows show the path of light beam.</p>
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<p>Chemical structures of (<b>a</b>) acrylamide, (<b>b</b>) N-[3-(dimethylamino)propyl]methacrylamide (DMA) monomers, and (<b>c</b>) N, N-methylene bisacrylamide crosslinker.</p>
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<p>A typical (<b>a</b>) two-dimensional reflectivity curve and the corresponding (<b>b</b>) one-dimensional reflectivity curve of an LW with a hydrogel film made of 5% (<span class="html-italic">w</span>:<span class="html-italic">v</span>) total monomer solution and with a 15% molar ratio of DMA to total monomer.</p>
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<p>Time course of the response of an LW to pH where the hydrogel film was made of 5% (<span class="html-italic">w</span>:<span class="html-italic">v</span>) total monomer solution and 15% molar ratio of DMA to total monomer.</p>
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<p>Estimated thickness and refractive index of waveguide films made of 5% (<span class="html-italic">w</span>:<span class="html-italic">v</span>) monomer solution containing a 20% molar ratio of DMA for different pH solutions.</p>
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<p>The response of an LW comprising a 5% (<span class="html-italic">w</span>:<span class="html-italic">v</span>) hydrogel film to pH, where the molar ratio of DMA to total monomer was between 0 and 40% (where error bars show variations in response of LWs across the width of the flow cell).</p>
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<p>The response of an LW, comprising a hydrogel film made of a 5% (<span class="html-italic">w</span>:<span class="html-italic">v</span>) monomer solution containing a 20% molar ratio of DMA, to cycles of pH 4 and 8 buffers.</p>
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<p>Shift in resonance angle versus time of an LW exposed to cycles of (<b>a</b>) pH 4 to pH 8 and (<b>b</b>) pH 8 to pH 4.</p>
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<p>Time constant of an LW exposed to cycles of pH 4 to pH 8 and pH 8 to pH 4.</p>
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<p>Shits in resonance angles of an LW comprising a hydrogel film made using a 5% (<span class="html-italic">w</span>:<span class="html-italic">v</span>) total monomer solution and a 10% molar ratio of DMA for 10 mM phosphate a buffer of pH 7 containing (<b>a</b>) sodium chloride, (<b>b</b>) urea, aluminum sulfate, calcium chloride, and humic acid.</p>
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27 pages, 8424 KiB  
Article
Research on the Algorithm of Lake Surface Height Inversion in Qinghai Lake Based on Sentinel-3A Altimeter
by Chuntao Chen, Xiaoqing Li, Jianhua Zhu, Hailong Peng, Youhua Xue, Wanlin Zhai, Mingsen Lin, Yufei Zhang, Jiajia Liu and Yili Zhao
Remote Sens. 2025, 17(4), 647; https://doi.org/10.3390/rs17040647 - 14 Feb 2025
Abstract
Lakes are a crucial component of inland water bodies, and changes in their water levels serve as key indicators of global climate change. Traditional methods of lake water level monitoring rely heavily on hydrological stations, but there are problems such as regional representativeness, [...] Read more.
Lakes are a crucial component of inland water bodies, and changes in their water levels serve as key indicators of global climate change. Traditional methods of lake water level monitoring rely heavily on hydrological stations, but there are problems such as regional representativeness, data stability, and high maintenance costs. The satellite altimeter is an essential tool in lake research, with the Synthetic Aperture Radar (SAR) altimeter offering a high spatial resolution. This enables precise and quantitative observations of lake water levels on a large scale. In this study, we used Sentinel-3A SAR Radar Altimeter (SRAL) data to establish a more reasonable lake height inversion algorithm for satellite-derived lake heights. Subsequently, using this technology, a systematic analysis study was conducted with Qinghai Lake as the case study area. By employing regional filtering, threshold filtering, and altimeter range filtering techniques, we obtained effective satellite altimeter height measurements of the lake surface height. To enhance the accuracy of the data, we combined these measurements with GPS buoy-based geoid data from Qinghai Lake, normalizing lake surface height data from different periods and locations to a fixed reference point. A dataset based on SAR altimeter data was then constructed to track lake surface height changes in Qinghai Lake. Using data from the Sentinel-3A altimeter’s 067 pass over Qinghai Lake, which has spanned 96 cycles since its launch in 2016, we analyzed over seven years of lake surface height variations. The results show that the lake surface height exhibits distinct seasonal patterns, peaking in September and October and reaching its lowest levels in April and May. From 2016 to 2023, Qinghai Lake showed a general upward trend, with an increase of 2.41 m in lake surface height, corresponding to a rate of 30.0 cm per year. Specifically, from 2016 to 2020, the lake surface height rose at a rate of 47.2 cm per year, while from 2020 to 2022, the height remained relatively stable. Full article
(This article belongs to the Special Issue Remote Sensing in Monitoring Coastal and Inland Waters)
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<p>Schematic of the Qinghai Lake experimental site in 2019 (the green circle with * indicate tide gauge installation points; and the red triangle denote GPS reference station locations).</p>
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<p>Establishment of GPS reference station.</p>
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<p>Diagram of the installation of the tide gauge on the centering rod in an erect position (the red circle is level bubble, which indicates the centralization of the centering rod).</p>
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<p>Deployment strategy for the GPS buoy.</p>
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<p>Water level data measured by the pressure tide gauge installed in the air.</p>
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<p>Tide gauge measurement of water level changes in Qinghai Lake on 15 July 2019.</p>
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<p>Schematic diagram of the method for measuring lake surface height with a pressure-type tide gauge.</p>
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<p>Results of the first comparative test between the tide gauge and GPS buoy.</p>
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<p>Results of the second comparative test between the tide gauge and GPS buoy.</p>
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<p>Variation in lake water level during geoid measurement on 15 July 2019.</p>
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<p>Variation in lake water level during geoid measurement in July 2019.</p>
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<p>Distribution of Qinghai Lake water surface height derived from Sentinel-3A 067 pass with latitude.</p>
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<p>Variations in lake surface height of Qinghai Lake derived from Sentinel-3A 067 pass after regional screening.</p>
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<p>Variations in lake surface height of Qinghai Lake derived from Sentinel-3A after regional and threshold filtering.</p>
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<p>Time series of lake surface height derived from Sentinel-3A SRAL after regional and threshold filtering.</p>
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<p>Single-pass standard deviation (StD) statistics of lake surface heights derived from Sentinel-3A SRAL after regional and threshold filtering.</p>
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<p>Comparative plot of the time series of lake surface heights and the standard deviation (StD) of lake surface height in the same pass.</p>
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<p>Time series of lake surface height derived from the improved and effective satellite altimeter extraction method for Qinghai Lake.</p>
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<p>The normalized average lake surface height of Qinghai Lake obtained after normalization. (<b>a</b>) The rising trend of Qinghai Lake water level; (<b>b</b>) The distribution of residuals.</p>
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<p>Distribution of annual average lake surface height changes of Qinghai Lake.</p>
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26 pages, 5383 KiB  
Article
Characterization and Emulsifying Ability of Cassava Peels Solubilized Using Hydrothermal Treatments
by Jane Chizie Ogbonna, Mitsutoshi Nakajima and Marcos Antonio das Neves
Polymers 2025, 17(4), 496; https://doi.org/10.3390/polym17040496 - 13 Feb 2025
Abstract
Cassava peels are rich in polysaccharides but highly unexplored and underutilized, as they could be used to meet the increasing demand for clean-label foods. This study investigated the effect of temperature on the solubilization of cassava peel during hydrothermal treatment to determine the [...] Read more.
Cassava peels are rich in polysaccharides but highly unexplored and underutilized, as they could be used to meet the increasing demand for clean-label foods. This study investigated the effect of temperature on the solubilization of cassava peel during hydrothermal treatment to determine the emulsifying ability of solubilized cassava peel (SCP). Subcritical water conditions were employed via hydrothermal (120–200 °C; 2 MPa) or autoclave (127 °C; 0.2 MPa) treatments to solubilize cassava peels. The composition of the SCPs was determined, and their emulsifying ability was assessed using interfacial tension and zeta potential measurements. Under the best treatment conditions (140 °C at 2 MPa [hydrothermal]; 127 °C at 0.2 MPa [autoclave]), SCPs reduced interfacial tension against soybean oil to 12.9 mN/m and 13.4 mN/m, respectively. A strengthened co-emulsifier system was developed by incorporating SCPs with Quillaja saponins (QS) or Tween 20 to enhance the performance. Dynamic interfacial tension and zeta potential measurements revealed synergistic interactions, showing a remarkable reduction in interfacial tension from 12.94 to 5.33 mN/m. This suggests that the SCP has a surfactant-like structure owing to its amphiphilic structure and hydrophobic chains (nonpolar region) attached to the -OH functional group (polar region). Combining a second surface-active compound or co-emulsifier results in an additive effect, reducing the interfacial tension. These findings provide novel insights into carbohydrate-saponin binding and elucidate the impact of peel composition, concentration, and hydrothermal treatment conditions on co-emulsifier system performance, which will assist in the development of emulsifiers, contributing to the advancement of clean-label food technologies, effectively replacing synthetic emulsifiers in food formulations, and offering both sustainability and functionality. A systematic investigation of processing conditions and co-emulsifier interactions provides a practical framework for developing high-performance natural emulsifiers from agricultural waste. Full article
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Graphical abstract

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<p>Schematic diagram of the equipment used for hydrothermal treatment: (<b>a</b>) Hydrothermal treatment (HTS) reactor and (<b>b</b>) autoclave.</p>
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<p>Temperature, pressure, and time profile of the hydrothermal solubilization reactor at 140 °C and 2 MPa with a holding time of 15 min.</p>
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<p>Effect of thermal treatment temperature on the solubilization yield and pH of solubilized cassava peels (SCPs) obtained using an HTS reactor.</p>
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<p>Effect of hydrothermal treatment temperature on the composition (carbohydrates, protein, and ash content) of SCPs obtained using an HTS reactor.</p>
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<p>Effect of hydrothermal treatment temperature on cyanide content of SCPs obtained using an HTS reactor.</p>
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<p>Scanning electron microscope (SEM) images of (<b>a</b>) untreated cassava peel powder; (<b>b</b>) cassava peels solubilized at 140 °C and 2 MPa (HTS reactor) and freeze-dried; and (<b>c</b>) cassava peels solubilized at 127 °C and 0.2 MPa (autoclave) and freeze-dried.</p>
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<p>Droplet size distribution of oil-in-water (O/W) emulsions stabilized by SCPs and stored for 10 d at (<b>a</b>) 5 °C and (<b>b</b>) 25 °C.</p>
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<p>Mean droplet diameter (<span class="html-italic">d</span><sub>3,2</sub>) of O/W emulsions stabilized by SCPs and stored for 10 d at (<b>a</b>) 5 °C and (<b>b</b>) 25 °C.</p>
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<p>Effect of the weight ratio between SCPs and co-emulsifiers (<span class="html-italic">Quillaja</span> saponin or Tween 20) on interfacial tension: (<b>a</b>) 140 °C at 2 MPa (HTS reactor) and (<b>b</b>) 127 °C at 0.2 MPa (autoclave) (weight ratios of 10:0, 7.5:2.5, 5:5, 2.5:7.5, and 0:10 (SCP: co-emulsifier)).</p>
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<p>Effect of weight ratio of solubilized cassava peels (SCP) to co-emulsifiers (<span class="html-italic">Quillaja</span> saponin or Tween 20) on zeta potential: (<b>a</b>) 140 °C at 2 MPa (HTS reactor) and (<b>b</b>) 127 °C at 0.2 MPa (autoclave) (the weight ratios were 10:0, 7.5:2.5, 5:5, 2.5:7.5, and 0:10 (SCP: co-emulsifier)).</p>
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<p>Droplet size distribution of O/W emulsions stabilized by SCPs or <span class="html-italic">Quillaja</span> saponins at various weight ratios, and stored for 10 d: (<b>a</b>) Fresh emulsion (day 0); (<b>b</b>) stored at 5 °C for 10 days; and (<b>c</b>) stored at 25 °C for 10 days (the weight ratios were 10:0, 7.5:2.5, 5:5, 2.5:7.5, and 0:10 (SCP: co-emulsifier)).</p>
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<p>Droplet size distribution of O/W emulsions stabilized by SCPs or <span class="html-italic">Quillaja</span> saponins at various weight ratios, and stored for 10 d: (<b>a</b>) Fresh emulsion (day 0); (<b>b</b>) stored at 5 °C for 10 days; and (<b>c</b>) stored at 25 °C for 10 days (the weight ratios were 10:0, 7.5:2.5, 5:5, 2.5:7.5, and 0:10 (SCP: co-emulsifier)).</p>
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<p>Mean droplet diameter (<span class="html-italic">d</span><sub>3,2</sub>) of O/W emulsions stabilized by SCPs or <span class="html-italic">Quillaja</span> saponin at various weight ratios and stored for 10 days either at (<b>a</b>) 5 °C or (<b>b</b>) 25 °C (the weight ratios were 10:0, 7.5:2.5, 5:5, 2.5:7.5, and 0:10 (SCP: co-emulsifier)).</p>
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<p>Emulsions stabilized by solubilized cassava peels loaded with varied ratios of <span class="html-italic">Quillaja</span> saponin as a co-emulsifier.</p>
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<p>Schematic illustration of the potential synergistic interaction between SCPs and <span class="html-italic">Quillaja</span> saponins.</p>
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<p>Schematic illustration of the carbohydrates–saponin binding mechanism that leads to a reduction in interfacial tension.</p>
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18 pages, 8347 KiB  
Article
Shallow Subsurface Wavefield Data Interpolation Method Based on Transfer Learning
by Danfeng Zang, Jian Li, Chuankun Li, Hengran Zhang, Zhipeng Pei and Yixiang Ma
Appl. Sci. 2025, 15(4), 1964; https://doi.org/10.3390/app15041964 - 13 Feb 2025
Abstract
The deployment density of surface sensors can significantly impact the accuracy of subsurface shallow seismic field energy inversion. With finite budget constraints, it is often not feasible to deploy a large number of sensors, resulting in limited seismic signal acquisition that hinders accurate [...] Read more.
The deployment density of surface sensors can significantly impact the accuracy of subsurface shallow seismic field energy inversion. With finite budget constraints, it is often not feasible to deploy a large number of sensors, resulting in limited seismic signal acquisition that hinders accurate inversion of the shallow subsurface explosions. To address the challenge of insufficient sensor signals needed for inversion, we conducted a study on a subsurface shallow wavefield data interpolation method based on transfer learning. This method is designed to increase the overall signal acquisition by interpolating signals at target locations from limited measurement points. Our research employs neural networks to interpolate real seismic data, supplementing the sampled signals. Given the lack of extensive samples from actual data collection, we devised a training approach that combines numerically simulated signals with real collected signals. Initially, we performed conventional interpolation training using a deep interpolation network with complete synthetic gather images obtained from numerical simulations. Subsequently, the feature extraction part was frozen, and the interpolation network was transferred to real datasets, where it was trained using incomplete gather images. Finally, these incomplete gather images were re-input into the trained network to obtain interpolated results at the target locations. Our study demonstrates the superiority of our method by comparing it with two other interpolation networks and validating the effectiveness of transfer learning through four sets of ablation experiments in the actual test. This method can also be applied to other shallow geological structures to generate a large number of seismic signals for energy inversion. Full article
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<p>Overall schematic of transfer learning.</p>
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<p>Overall schematic of the depth interpolation model.</p>
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<p>Schematic diagram of the down-sampling block.</p>
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<p>Haar wavelet experimental results: (<b>a</b>) original data (1024 × 64); (<b>b</b>) the approximation (low-low) component (512 × 32); (<b>c</b>) the horizontal detail (low-high) component (512 × 32); (<b>d</b>) the vertical detail (high-low) component (512 × 32); (<b>e</b>) the diagonal detail (high-high) component (512 × 32).</p>
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<p>Schematic diagram of the multi-scale convolution block.</p>
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<p>Schematic diagram of the up-sampling block.</p>
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<p>Target domain training framework.</p>
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<p>Simulation of layout diagrams (the dashed line represents the location of the seismic source that needs to be deployed in the text).</p>
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<p>Two of the signaling effects: (<b>a</b>) the fifth signal; (<b>b</b>) the 121st signal.</p>
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<p>Experimental results: (<b>a</b>) complete data; (<b>b</b>) missing 60% of data; (<b>c</b>) results obtained from migration learning; (<b>d</b>) Method 1: Results of migration learning without wavelet up- and down-sampling; (<b>e</b>) Method 2: Results of migration learning without multi-scale convolutional module; (<b>f</b>) Method 3: Results obtained from training in source domain only; (<b>g</b>) Method 4: Results obtained from training in target domain only.</p>
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<p>The <span class="html-italic">f-k</span> spectrum of the experimental results: (<b>a</b>) complete data; (<b>b</b>–<b>f</b>) represent the above five training modalities in turn.</p>
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<p>The <span class="html-italic">f-k</span> spectrum of the experimental results: (<b>a</b>) complete data; (<b>b</b>–<b>f</b>) represent the above five training modalities in turn.</p>
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<p>Comparison of extracted signals (the blue curve represents the original signal, and the red curve represents the interpolated signal): (<b>a</b>) transfer learning; (<b>b</b>) Method 2: transfer learning without multi-scale convolutional modules.</p>
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<p>Experimental results: (<b>a</b>) complete data; (<b>b</b>) missing 60% of data; (<b>c</b>) results from our network; (<b>d</b>) results from U-resnet; (<b>e</b>) results from CAE; (<b>f</b>) results from MWCNN.</p>
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<p>The <span class="html-italic">f-k</span> spectrum of the experimental results (the red ellipse indicates areas different from the original image): (<b>a</b>) complete data; (<b>b</b>–<b>e</b>) represent the above five training modalities in turn.</p>
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33 pages, 2250 KiB  
Review
Unconventional Fossil Energy Carrier Assessment of the Influence of the Gas Permeability Coefficient on the Structure of Porous Materials: A Review
by Jakub T. Hołaj-Krzak, Barbara Dybek, Jan Szymenderski, Adam Koniuszy and Grzegorz Wałowski
Energies 2025, 18(4), 870; https://doi.org/10.3390/en18040870 - 12 Feb 2025
Abstract
The issue of gas permeability of porous beds is important for the development of a new generation of clean energy sources, especially in the context of unconventional energy storage. Detailed experimental studies were carried out to demonstrate the gas permeability of porous materials: [...] Read more.
The issue of gas permeability of porous beds is important for the development of a new generation of clean energy sources, especially in the context of unconventional energy storage. Detailed experimental studies were carried out to demonstrate the gas permeability of porous materials: in situ karbonizat and natural and synthetic pumice. The measure of gas permeability was the volumetric gas flow velocity resulting from the permissible pressure difference forcing the gas flow in a given axis (X, Y, Z) on a sample of a cube-shaped porous material. A novelty is the indication of correlation with selected materials exhibiting features of unconventional energy storage. Assessment of the gas permeability coefficient for selected material features shows an increasing trend for epoxy resin, dacite, in situ carbonizate and pumice. On the other hand, for carbonate rocks, mudstones and shales, there is a decrease in gas permeability. The indicated porous materials can be storage tanks of unconventional energy carriers. In an innovative way, a material (halloysite) was indicated that has the ability to store and be a source of transport in the form of a cylindrical model (nanotube) for future implementation of isotropic features of porous materials. Full article
(This article belongs to the Special Issue Energy Geotechnics and Geostructures—2nd Edition)
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Figure 1

Figure 1
<p>Scheme of flows through a porous bed [<a href="#B12-energies-18-00870" class="html-bibr">12</a>]: (<b>a</b>) layer of grains with winding channels; (<b>b</b>) rigid skeletal structure with open flows channels and blind pores and closed to flows.</p>
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<p>Scheme of flows through a porous bed [<a href="#B12-energies-18-00870" class="html-bibr">12</a>]—Darcy’s model.</p>
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<p>Sample of test material, porous material 20 × 20 × 20 mm: (<b>a</b>) karbonizat (coal char) in situ [photo from G. Wałowski]; (<b>b</b>) natural pumice [photo from G. Wałowski]; (<b>c</b>) synthetic pumice [photo from G. Wałowski]; (<b>d</b>) diagram of gas flow through the sample depending on the X, Y, Z axis [prepared by G. Wałowski].</p>
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<p>Summary of test results for gas flow resistance ΔP<sub>zm</sub> through a granular and porous bed acc. to <a href="#energies-18-00870-t001" class="html-table">Table 1</a> (prepared by G. Wałowski).</p>
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<p>Summary of test results for gas flow resistance ΔP<sub>zm</sub> through a granular and porous bed acc. to <a href="#energies-18-00870-t001" class="html-table">Table 1</a> (prepared by G. Wałowski).</p>
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<p>Gas permeability coefficient K<sub>V</sub> = f(ΔP)—selected material characteristics: epoxy resin- Gajda and Lutyński [<a href="#B62-energies-18-00870" class="html-bibr">62</a>]; dacite—Jiang and co-workers [<a href="#B25-energies-18-00870" class="html-bibr">25</a>]; carbonate rocks—Rabbani and co-workers [<a href="#B63-energies-18-00870" class="html-bibr">63</a>]; mudstone—Wu and co-workers [<a href="#B64-energies-18-00870" class="html-bibr">64</a>]; shales—Afagwu and co-workers [<a href="#B65-energies-18-00870" class="html-bibr">65</a>]—related to karbonizat (coal char) in situ (Wałowski’s own research); synthetic pumice (Wałowski’s own research); natural pumice (Wałowski’s own research)—acc. to <a href="#energies-18-00870-t002" class="html-table">Table 2</a> (prepared by G. Wałowski).</p>
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