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12 pages, 7217 KiB  
Article
Temperature-Induced Phase Transformations in Tutton Salt K2Cu(SO4)2(H2O)6: Thermoanalytical Studies Combined with Powder X-Ray Diffraction
by João G. de Oliveira Neto, Ronilson S. Santos, Kamila R. Abreu, Luzeli M. da Silva, Rossano Lang and Adenilson O. dos Santos
Physchem 2024, 4(4), 458-469; https://doi.org/10.3390/physchem4040032 (registering DOI) - 16 Nov 2024
Abstract
Tutton salts have received considerable attention due to their potential applications in thermochemical energy storage (TCHS) systems. This technology requires high-purity materials that exhibit reversible dehydration reactions, significant variations in dehydration enthalpy, and high-temperature melting points. In this study, K2Cu(SO4 [...] Read more.
Tutton salts have received considerable attention due to their potential applications in thermochemical energy storage (TCHS) systems. This technology requires high-purity materials that exhibit reversible dehydration reactions, significant variations in dehydration enthalpy, and high-temperature melting points. In this study, K2Cu(SO4)2(H2O)6 Tutton salt in the form of single crystals was grown using the slow solvent evaporation method. Their structural, morphological, and thermal characteristics are presented and discussed, as well as temperature-induced phase transformations. At room temperature, the salt crystallizes in a monoclinic structure belonging to the P21/a space group, which is typical for Tutton salts. The lack of precise control over the solvent evaporation rate during crystal growth introduced structural disorder, resulting in defects on the crystal surface, including layer discontinuities, occlusions, and pores. Thermoanalytical analyses revealed two stages of mass loss, corresponding to the release of 4 + 2 coordinated H2O molecules — four weakly coordinated and two strongly coordinated to the copper. The estimated dehydration enthalpy was ≈ 80.8 kJ/mol per mole of H2O. Powder X-ray diffraction measurements as a function of temperature showed two phase transformations associated with the complete dehydration of the starting salt occurring between 28 and 160 °C, further corroborating the thermal results. The total dehydration up to ≈ 160 °C, high enthalpy associated with this process, and high melting point temperature make K2Cu(SO4)2(H2O)6 a promising candidate for TCHS applications. Full article
(This article belongs to the Section Solid-State Chemistry and Physics)
25 pages, 20123 KiB  
Article
EDWNet: A Novel Encoder–Decoder Architecture Network for Water Body Extraction from Optical Images
by Tianyi Zhang, Wenbo Ji, Weibin Li, Chenhao Qin, Tianhao Wang, Yi Ren, Yuan Fang, Zhixiong Han and Licheng Jiao
Remote Sens. 2024, 16(22), 4275; https://doi.org/10.3390/rs16224275 (registering DOI) - 16 Nov 2024
Abstract
Automated water body (WB) extraction is one of the hot research topics in the field of remote sensing image processing. To address the challenges of over-extraction and incomplete extraction in complex water scenes, we propose an encoder–decoder architecture semantic segmentation network for high-precision [...] Read more.
Automated water body (WB) extraction is one of the hot research topics in the field of remote sensing image processing. To address the challenges of over-extraction and incomplete extraction in complex water scenes, we propose an encoder–decoder architecture semantic segmentation network for high-precision extraction of WBs called EDWNet. We integrate the Cross-layer Feature Fusion (CFF) module to solve difficulties in segmentation of WB edges, utilizing the Global Attention Mechanism (GAM) module to reduce information diffusion, and combining with the Deep Attention Module (DAM) module to enhance the model’s global perception ability and refine WB features. Additionally, an auxiliary head is incorporated to optimize the model’s learning process. In addition, we analyze the feature importance of bands 2 to 7 in Landsat 8 OLI images, constructing a band combination (RGB 763) suitable for algorithm’s WB extraction. When we compare EDWNet with various other semantic segmentation networks, the results on the test dataset show that EDWNet has the highest accuracy. EDWNet is applied to accurately extract WBs in the Weihe River basin from 2013 to 2021, and we quantitatively analyzed the area changes of the WBs during this period and their causes. The results show that EDWNet is suitable for WB extraction in complex scenes and demonstrates great potential in long time-series and large-scale WB extraction. Full article
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Figure 1
<p>Spatial location and scope of the Weihe River Basin study area in the People’s Republic of China: (<b>a</b>) is the administrative divisions of China, (<b>b</b>) is the true color Landsat 8 OLI image of the study area, (<b>c</b>) is the image before pansharpening in a randomly selected area, and (<b>d</b>) is the image after pansharpening in a randomly selected area.</p>
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<p>EDWNet model structure.</p>
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<p>CFF module structure.</p>
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<p>DAM module structure.</p>
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<p>GAM module structure.</p>
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<p>SHAP values of bands 2 to 7 in Landsat 8 OLI images.</p>
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<p>Validation loss of EDWNet in different band combination images.</p>
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<p>Classification results of WBs using different methods: (<b>a</b>–<b>c</b>) the scenario with small WBs, (<b>d</b>,<b>e</b>) the scenario with a reservoir, (<b>f</b>) the scenario with a wide river channel, (<b>g</b>) the scenario with shadows of hills. The yellow dotted line indicates WBs misclassified as background, while the red dotted line indicates pixels misclassified as WBs.</p>
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<p>Spatial distribution of the main stream of the “Xi’an-Xianyang” section in the Weihe River Basin.</p>
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<p>Results of river width extraction using different methods in the Weihe River “Xi’an-Xianyang” section: (<b>a</b>) line graph of river width extracted using different methods at different longitudes, and (<b>b</b>) difference between river width extracted using different methods and true width.</p>
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<p>Results of river width extraction using different methods in the Weihe River “Xi’an-Xianyang” section: (<b>a</b>) line graph of river width extracted using different methods at different longitudes, and (<b>b</b>) difference between river width extracted using different methods and true width.</p>
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<p>Scatter plot of label river width and extracted river width in different methods.</p>
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<p>Extraction maps of the Weihe River Basin in 2014, 2016, 2018, and 2020. The left side are the original images, and the right side are the WB extraction results. The yellow color represents the background, the blue color represents the extracted WB. The area inside the yellow rectangle is a local magnified view of a certain section of the Weihe River mainstream.</p>
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<p>Long time-series WB extraction results in the Weihe River Basin from 2013 to 2021: (<b>a</b>) WB extraction accuracy and (<b>b</b>) WB area changes.</p>
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<p>Average high temperature days in the Weihe River Basin from 2013 to 2020.</p>
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<p>NINO 3.4 index from 2013 to 2021.</p>
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16 pages, 4235 KiB  
Article
Mobile Accelerometer Applications in Core Muscle Rehabilitation and Pre-Operative Assessment
by Aleš Procházka, Daniel Martynek, Marie Vitujová, Daniela Janáková, Hana Charvátová and Oldřich Vyšata
Sensors 2024, 24(22), 7330; https://doi.org/10.3390/s24227330 (registering DOI) - 16 Nov 2024
Abstract
Individual physiotherapy is crucial in treating patients with various pain and health issues, and significantly impacts abdominal surgical outcomes and further medical problems. Recent technological and artificial intelligent advancements have equipped healthcare professionals with innovative tools, such as sensor systems and telemedicine equipment, [...] Read more.
Individual physiotherapy is crucial in treating patients with various pain and health issues, and significantly impacts abdominal surgical outcomes and further medical problems. Recent technological and artificial intelligent advancements have equipped healthcare professionals with innovative tools, such as sensor systems and telemedicine equipment, offering groundbreaking opportunities to monitor and analyze patients’ physical activity. This paper investigates the potential applications of mobile accelerometers in evaluating the symmetry of specific rehabilitation exercises using a dataset of 1280 tests on 16 individuals in the age range between 8 and 75 years. A comprehensive computational methodology is introduced, incorporating traditional digital signal processing, feature extraction in both time and transform domains, and advanced classification techniques. The study employs a range of machine learning methods, including support vector machines, Bayesian analysis, and neural networks, to evaluate the balance of various physical activities. The proposed approach achieved a high classification accuracy of 90.6% in distinguishing between left- and right-side motion patterns by employing features from both the time and frequency domains using a two-layer neural network. These findings demonstrate promising applications of precise monitoring of rehabilitation exercises to increase the probability of successful surgical recovery, highlighting the potential to significantly enhance patient care and treatment outcomes. Full article
(This article belongs to the Special Issue Robust Motion Recognition Based on Sensor Technology)
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<p>Principle of data processing during rehabilitation exercises presenting (<b>a</b>) mobile Matlab initialization, (<b>b</b>) data acquisition using accelerometric sensors inside the smartphone, (<b>c</b>) export of recorded signals to the remote drive, and (<b>d</b>) processing of data on the remote drive in time and frequency domains to extract motion features and evaluate the coefficient of symmetry.</p>
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<p>Selected rehabilitation exercises used for accelerometric data acquisition recorded by wearable sensors (red squares) located on the left and right sides of the body used for data acquisition and processing in the computational and visualization environment of the mobile Matlab system.</p>
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<p>Principle of data processing during rehabilitation exercises presenting (<b>a</b>) animation of motion exercises to train individuals and data acquisition using a smartphone, (<b>b</b>) data import into the proposed web-page, (<b>c</b>) frequency domain remote signal processing including symmetry coefficient estimation, and (<b>d</b>) extraction and analysis of motion features.</p>
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<p>Symmetry criteria for 8 rehabilitation exercises evaluated by (<b>a</b>) time domain and (<b>b</b>) mixed-domain features presenting mean values by 16 tests of different individuals with 10 repetitions of each rehabilitation exercise.</p>
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<p>Comparison of symmetry criteria for 16 tests involving different individuals and eight rehabilitation exercises, evaluated using time domain and spectral domain features.</p>
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<p>Comparison of distribution of the time and spectral domain features for selected exercises of (<b>a</b>) prevailing asymmetric motion (individual 6, exercise 6) and (<b>b</b>) prevailing symmetric motion (individual 10, exercise 5) with centers of the right and left side positions and <span class="html-italic">c</span> multiples of standard deviations for <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>0.2</mn> <mo>,</mo> <mn>0.5</mn> <mo>,</mo> <mn>1</mn> </mrow> </semantics></math>.</p>
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<p>Classification of symmetry features of the body cross-motion by mixed features using (<b>a</b>) support vector machine, (<b>b</b>) the Bayes method, and (<b>c</b>) the two-layer neural network for a selected individual 6-DH.</p>
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17 pages, 5937 KiB  
Article
Advancing Sustainable Transportation Equity for Older Adults: A Geospatial Analysis of Mobility Gaps in Florida
by Soowoong Noh
Sustainability 2024, 16(22), 10013; https://doi.org/10.3390/su162210013 (registering DOI) - 16 Nov 2024
Abstract
As older adults face increasing mobility challenges due to diminished driving ability, they encounter heightened risks of social exclusion, impacting their mental, social, and physical well-being. This study investigates spatial gaps in the availability of sustainable transportation options—including public transit, paratransit, and specialized [...] Read more.
As older adults face increasing mobility challenges due to diminished driving ability, they encounter heightened risks of social exclusion, impacting their mental, social, and physical well-being. This study investigates spatial gaps in the availability of sustainable transportation options—including public transit, paratransit, and specialized senior services—and examines their alignment with the distribution of older adults segmented by age group (65–74, 75–84, and 85+). Using Florida as a case study, Geographic Information System (GIS) was employed to conduct a geospatial analysis, identifying statistically significant clusters of low transportation availability alongside high concentrations of older adults. The primary contribution of this research lies in its innovative methodology, which integrates precise transportation service boundaries with age-segmented demographic data, offering a nuanced assessment of transportation equity as a crucial aspect of sustainability. Findings provide a comprehensive framework for policymakers, enabling targeted resource allocation and planning that enhance mobility, accessibility, and quality of life for older adults. This study contributes to advancing sustainable development goals by addressing transportation disparities, supporting equitable, age-sensitive transportation solutions, and informing broader discussions on sustainable urban planning. Full article
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<p>Overview of Find-a-Ride website data structure (adapted from [<a href="#B27-sustainability-16-10013" class="html-bibr">27</a>]). Modifications include updates to route types.</p>
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<p>Conceptual process of the research.</p>
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<p>Comprehensive alternative transportation availability in Florida.</p>
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<p>Cluster and outlier analysis of older adult population spatial distribution.</p>
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<p>Spatial gaps between transportation availability and older adults by age group.</p>
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22 pages, 42906 KiB  
Article
Monitoring the Subsidence in Wan’an Town of Deyang Based on PS-InSAR Technology (Sichuan, China)
by Hongyi Guo, Antonio Miguel Martínez-Graña and José Angel González-Delgado
Sustainability 2024, 16(22), 10010; https://doi.org/10.3390/su162210010 (registering DOI) - 16 Nov 2024
Abstract
In recent years, land subsidence has become a crucial factor affecting urban safety and sustainable development, especially in Wan’an Town. To accurately monitor and analyze the land subsidence in Wan’an Town, this study uses the PS-InSAR technique combined with an improved DEM for [...] Read more.
In recent years, land subsidence has become a crucial factor affecting urban safety and sustainable development, especially in Wan’an Town. To accurately monitor and analyze the land subsidence in Wan’an Town, this study uses the PS-InSAR technique combined with an improved DEM for detailed research on land subsidence in Wan’an Town. PS-InSAR, or Permanent Scatterer Interferometric SAR, is suitable for high-precision monitoring of surface deformation. The natural neighbor interpolation method optimizes DEM data, improving its spatial resolution and accuracy. In this study, multiple periods of SAR imagery data of Wan’an Town were collected and preprocessed through radiometric calibration, phase unwrapping, and other steps. Using the PS-InSAR technique, the phase information of permanent scatterers (PS points) on the surface was extracted to establish a deformation model and preliminarily analyze the land subsidence in Wan’an Town. Concurrently, the DEM data were optimized using the natural neighbor interpolation method to enhance its accuracy. Finally, the optimized DEM data were combined with the surface deformation information extracted through the PS-InSAR technique for a detailed analysis of the land subsidence in Wan’an Town. The research results indicate that the DEM data optimized by the natural neighbor interpolation method have higher accuracy and spatial resolution, providing a more accurate reflection of the topographical features of Wan’an Town. The research found that the optimized DEM provided a more accurate reflection of Wan’an Town’s topographical features. By combining PS-InSAR data, subsidence information from 2016 to 2024 was calculated. The study area showed varying degrees of subsidence, with rates ranging from 6 mm/year to 10 mm/year. Four characteristic deformation areas were analyzed for causes and influencing factors. The findings contribute to understanding urban land subsidence, guiding urban planning, and providing data support for geological disaster warning and prevention. Full article
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<p>Digital elevation model of the study area.</p>
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<p>Topography of the study area and radar image coverage area.</p>
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<p>Geology map of the study area.</p>
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<p>Elevation contrast chart.</p>
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<p>Workflow of PS processing.</p>
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<p>Spatial and temporal baseline distribution map.</p>
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<p>Differential interferogram.</p>
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<p>Spatial distribution of the average subsidence rate in the study area from 2016 to 2024.</p>
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<p>Settlement comparison diagram.</p>
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<p>Total subsidence in the study area from 2016 to 2024.</p>
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<p>Natural neighbor interpolation.</p>
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<p>Time-series deformation map of the study area from 2016 to 2024.</p>
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<p>GPS survey map. (<b>A</b>) Field survey map of target A, (<b>B</b>) field survey map of target B, (<b>C</b>) field survey map of target C, (<b>D</b>) field survey map of target D.</p>
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<p>(<b>A</b>) Deformation analysis of Deformation Target Area A. (<b>B</b>) Deformation analysis of Deformation Target Area B. (<b>C</b>) Deformation analysis of Deformation Target Area C. (<b>D</b>) Deformation analysis of Deformation Target Area D.</p>
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<p>(<b>A</b>) Deformation analysis of Deformation Target Area A. (<b>B</b>) Deformation analysis of Deformation Target Area B. (<b>C</b>) Deformation analysis of Deformation Target Area C. (<b>D</b>) Deformation analysis of Deformation Target Area D.</p>
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14 pages, 4897 KiB  
Article
Novel Dynamic Behaviors in Fractional Chaotic Systems: Numerical Simulations with Caputo Derivatives
by Mohamed A. Abdoon, Diaa Eldin Elgezouli, Borhen Halouani, Amr M. Y. Abdelaty, Ibrahim S. Elshazly, Praveen Ailawalia and Alaa H. El-Qadeem
Axioms 2024, 13(11), 791; https://doi.org/10.3390/axioms13110791 (registering DOI) - 16 Nov 2024
Abstract
Over the last several years, there has been a considerable improvement in the possible methods for solving fractional-order chaotic systems; however, achieving high accuracy remains a challenge. This work proposes a new precise numerical technique for fractional-order chaotic systems. Through simulations, we obtain [...] Read more.
Over the last several years, there has been a considerable improvement in the possible methods for solving fractional-order chaotic systems; however, achieving high accuracy remains a challenge. This work proposes a new precise numerical technique for fractional-order chaotic systems. Through simulations, we obtain new types of complex and previously undiscussed dynamic behaviors.These phenomena, not recognized in prior numerical results or theoretical estimations, underscore the unique dynamics present in fractional systems. We also study the effects of the fractional parameters β1, β2, and β3 on the system’s behavior, comparing them to integer-order derivatives. It has been demonstrated via the findings that the suggested technique is consistent with conventional numerical methods for integer-order systems while simultaneously providing an even higher level of precision. It is possible to demonstrate the efficacy and precision of this technique through simulations, which demonstrates that this method is useful for the investigation of complicated chaotic models. Full article
(This article belongs to the Special Issue Fractional Calculus and the Applied Analysis)
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Figure 1
<p>Time series plots of the systems (1) under parameters <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> . Left: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>1.1</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>1</mn> <mo>]</mo> </mrow> </semantics></math>, right: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>1</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>1</mn> <mo>]</mo> </mrow> </semantics></math>.</p>
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<p>Time series plots of the systems (1) under different parameters. Left: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>2.1</mn> <mo>,</mo> <mn>1.18</mn> <mo>,</mo> <mn>1.1</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>1.19</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>19</mn> </mrow> </semantics></math>. Right: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>1.2</mn> <mo>,</mo> <mn>2.02</mn> <mo>,</mo> <mn>2.1</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>18</mn> </mrow> </semantics></math>.</p>
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<p>Time series plots of the systems (1) under different parameters. Left: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>2.1</mn> <mo>,</mo> <mn>1.18</mn> <mo>,</mo> <mn>0.95</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>15</mn> </mrow> </semantics></math>. Right: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>2.12</mn> <mo>,</mo> <mn>1.18</mn> <mo>,</mo> <mn>1.1</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2.12</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>1.9</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>30</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with parameters <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>0.95</mn> <mo>,</mo> <mn>0.93</mn> <mo>,</mo> <mn>0.98</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>0.95</mn> <mo>,</mo> <mn>1.03</mn> <mo>,</mo> <mn>1.08</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>20</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>2.95</mn> <mo>,</mo> <mn>2.93</mn> <mo>,</mo> <mn>2.98</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>9</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>11</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>1.5</mn> <mo>,</mo> <mn>1.3</mn> <mo>,</mo> <mn>1.8</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>9.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>0.9</mn> <mo>,</mo> <mn>1.23</mn> <mo>,</mo> <mn>1.28</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>1.95</mn> <mo>,</mo> <mn>1.93</mn> <mo>,</mo> <mn>1.98</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>1.5</mn> <mo>,</mo> <mn>1.9</mn> <mo>,</mo> <mn>0.98</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>7</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>9</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>1.99</mn> <mo>,</mo> <mn>1.98</mn> <mo>,</mo> <mn>0.93</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>.</p>
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<p>Numerical simulations for the systems (1) with varied parameters: <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mo>[</mo> <mn>2.95</mn> <mo>,</mo> <mn>2.98</mn> <mo>,</mo> <mn>2.93</mn> <mo>]</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>9</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>.</p>
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16 pages, 29569 KiB  
Article
Assessing Weed Canopy Cover in No-Till and Conventional Tillage Plots in Winter Wheat Production Using Drone Data
by Judith N. Oppong, Clement E. Akumu and Sam Dennis
Agronomy 2024, 14(11), 2706; https://doi.org/10.3390/agronomy14112706 (registering DOI) - 16 Nov 2024
Abstract
Weed canopy cover assessment, particularly using drone-acquired data, plays a vital role in precision agriculture by providing accurate, timely, and spatially detailed information, enhancing weed management decision-making in response to environmental and management variables. Despite the significance of this approach, few studies have [...] Read more.
Weed canopy cover assessment, particularly using drone-acquired data, plays a vital role in precision agriculture by providing accurate, timely, and spatially detailed information, enhancing weed management decision-making in response to environmental and management variables. Despite the significance of this approach, few studies have investigated weed canopy cover through drone-based imagery. This study aimed to fill this gap by evaluating the effects of conventional tillage (CT) and no-till (NT) practices on weed canopy cover in a winter wheat field over two growing seasons. Results indicated that in the 2022–2023 season, weed populations were similar between tillage systems, with a high mean weed cover of 1.448 cm2 ± 0.241 in CT plots. In contrast, during the 2023–2024 season, NT plots exhibited a substantially higher mean weed cover (1.784 cm2 ± 0.167), with a significant overall variation (p < 0.05) in weed distribution between CT and NT plots. These differences suggest that, while CT practices initially mask weed emergence by burying seeds and disrupting root systems, NT practices encourage greater weed establishment over time by leaving seeds near the soil surface. These findings provide valuable insights for optimizing weed management practices, emphasizing the importance of comprehensive approaches to improve weed control and overall crop productivity. Full article
(This article belongs to the Special Issue Weed Ecology, Evolution and Management)
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<p>Location of the study area with an insert of the study field.</p>
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<p>Schematic illustration of the methodology used for this study.</p>
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<p>No-till and conventional tillage plot layout for winter wheat production.</p>
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<p>West-to-east drone flight path for field image acquisition.</p>
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<p>Classified weed canopy cover map derived from the 2022–2023 tillering growth stage.</p>
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<p>Classified weed canopy cover map derived from the 2022–2023 jointing growth stage.</p>
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<p>Classified weed canopy cover map derived from the 2022–2023 booting growth stage.</p>
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<p>Classified weed canopy cover map derived from the 2022–2023 mature growth stage.</p>
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<p>Classified weed canopy cover map derived from the 2023–2024 tillering growth stage.</p>
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<p>Classified weed canopy cover map derived from the 2023–2024 jointing growth stage.</p>
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<p>Classified weed canopy cover map derived from the 2023–2024 booting growth stage.</p>
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<p>Classified weed canopy cover map derived from the 2023–2024 mature growth stage.</p>
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<p>Mean canopy cover of weeds for conventional tillage and no-till over the study period. Error bars = standard error of mean (SE).</p>
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17 pages, 2760 KiB  
Article
Hyperspectral Image Classification Method Based on Morphological Features and Hybrid Convolutional Neural Networks
by Tonghuan Ran, Guangfeng Shi, Zhuo Zhang, Yuhao Pan and Haiyang Zhu
Appl. Sci. 2024, 14(22), 10577; https://doi.org/10.3390/app142210577 (registering DOI) - 16 Nov 2024
Abstract
The exploitation of the spatial and spectral characteristics of hyperspectral remote sensing images (HRSIs) for the high-precision classification of earth observation targets is crucial. Convolutional neural networks (CNNs) have good classification performance and are widely used neural networks. Herein, a morphological processing (MP)-based [...] Read more.
The exploitation of the spatial and spectral characteristics of hyperspectral remote sensing images (HRSIs) for the high-precision classification of earth observation targets is crucial. Convolutional neural networks (CNNs) have good classification performance and are widely used neural networks. Herein, a morphological processing (MP)-based HRSI classification method and a 3D–2D CNN are proposed to improve HRSI classification accuracy. Principal component analysis is performed to reduce the dimensionality of the HRSI cube, and MP is implemented to extract the spectral–spatial features of the low-dimensional HRSI cube. The extracted features are concatenated with the low-dimensional HRSI cube, and the designed 3D–2D CNN framework completes the classification task. Residual connections and an attention mechanism are added to the CNN structure to prevent gradient vanishing, and the scale of the control parameters of the model structure is optimized to guarantee the model’s feature extraction ability. The CNN structure uses multiscale convolution, involving depthwise separable convolution, which can effectively reduce the amount of parameter calculation. Two classic datasets (Indian Pines and Pavia University) and a self-made dataset (My Dataset) are used to compare the performance of this method with existing classification techniques. The proposed method effectively improved classification accuracy despite its short classification time. Full article
10 pages, 535 KiB  
Article
Validating the Precision and Accuracy of Coral Fragment Photogrammetry
by Spencer Miller, Carlo Caruso and Crawford Drury
Remote Sens. 2024, 16(22), 4274; https://doi.org/10.3390/rs16224274 (registering DOI) - 16 Nov 2024
Abstract
Photogrammetry is a common tool for evaluating ecosystem-scale questions on coral reefs due to the ability to measure complex structures in situ. This technique is also increasingly being used at smaller scales to collect growth and morphometric data about individual coral fragments in [...] Read more.
Photogrammetry is a common tool for evaluating ecosystem-scale questions on coral reefs due to the ability to measure complex structures in situ. This technique is also increasingly being used at smaller scales to collect growth and morphometric data about individual coral fragments in manipulative experiments. However, there are substantial uncertainties in data quality and interpretation and limited reporting of the parameters useful for standardization across studies. There is a need to characterize the capabilities of photogrammetry as applied to coral fragments, to establish validation metrics for reporting, and to determine sources of variation in measurements to refine and improve methods. Here, we used fragments of two common reef-building corals (Montipora capitata and Porites compressa) and known size standards to evaluate accuracy and precision and present suggested validation metrics. We also used a tiered experimental design to evaluate sources of error in a photogrammetry workflow in a manipulative experiment using a purpose-built multi-camera workstation. We demonstrate extremely high accuracy (R2 > 0.999) in determining the surface area and volume of known objects, as well as very high precision (average CV < 0.01) in coral measurements during tests of reproducibility. These outcomes show the utility of fragment photogrammetry for experimental coral reef science and present suggested validation metrics and approaches that can help standardize data evaluation and interpretation in any application of photogrammetry to coral fragments. Full article
14 pages, 5811 KiB  
Article
Influence of Cold-Rolling Processes on the Dimensional Accuracy and Roughness of Small-Diameter Thick-Walled Seamless Tubes
by Xiuping Ding, Ran Li, Pengfei Jin, Weijie Wang, Cheng Zhang, Minyu Ma and Jinfeng Huang
Metals 2024, 14(11), 1297; https://doi.org/10.3390/met14111297 (registering DOI) - 16 Nov 2024
Abstract
Cold pilgering is widely utilized in high-end applications for the precise shaping of seamless tubes due to its capacity for large deformation, which reduces the number of deformation processes and shortens production cycles. However, there is a gap in the research on the [...] Read more.
Cold pilgering is widely utilized in high-end applications for the precise shaping of seamless tubes due to its capacity for large deformation, which reduces the number of deformation processes and shortens production cycles. However, there is a gap in the research on the cold pilgering of small-diameter, thick-walled seamless tubes, specifically those with an outer diameter–wall thickness ratio of ≤3. In this study, cold pilgering tests were performed on Cr-Mo-V hot-working die steel small-diameter thick-walled tubes. It was discovered that increasing the feed rate results in greater deviations in both inner diameter and wall thickness, although it has little effect on inner wall roughness. In contrast, increasing wall thickness reduction leads to higher wall thickness deviation but reduces inner surface roughness without significantly affecting inner diameter deviation. The study also found that a decrease in the initial inner wall roughness before pilgering results in improved final roughness. Under optimal conditions, the average inner surface roughness Sa can reach 0.177 μm, and small-diameter thick-walled seamless tubes with deviations in the inner diameter and wall thickness of 0.05 mm and 0.03 mm, respectively, are obtained. After tempering at 600 °C, the tensile strength (Rm) and yield strength (Rp0.2) of the cold-pilgered tube reach 1092 MPa and 947 MPa, respectively, and the elongation (δ5%) and impact energy (AkU) increase to 20.4% and 61.5 J, respectively. Full article
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<p>Picture of the LG40 pilger mill (Adapted from Ref [<a href="#B19-metals-14-01297" class="html-bibr">19</a>]).</p>
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<p>Schematic diagram of the angles and control points of the wall thickness on the cross-section.</p>
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<p>Schematic diagram of heat treatment processes for mother tubes and cold-pilgered tubes.</p>
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<p>Schematic diagram of tensile specimens.</p>
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<p>Effect of different feed rates (2, 3, and 4 mm/stroke) on the tubes<sub>WT</sub> deviation of the cold-pilgered tubes.</p>
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<p>Effect of feed rates (2, 3, and 4 mm/stroke) on the inner diameter deviation of the cold-pilgered tubes.</p>
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<p>Inner surface morphology of the cold-pilgered tubes with the feed rates of (<b>a</b>) 2 mm/stroke, (<b>b</b>) 3.5 mm/stroke, and (<b>c</b>) 4 mm/stroke, and (<b>d</b>) sample description.</p>
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<p>Effect of wall thickness reduction (2.5, 3.5, and 4 mm) on the wall thickness deviation of the cold-pilgered tubes.</p>
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<p>Effect of wall thickness reduction (2.5, 3.5, and 4 mm) on the tubes<sub>ID</sub> deviation of the cold-pilgered tubes.</p>
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<p>Inner surface morphology of the cold-pilgered tubes with the wall thickness reduction of (<b>a</b>) 2.0 mm, (<b>b</b>) 3.5 mm, and (<b>c</b>) 4.0 mm, and (<b>d</b>) at the worn region.</p>
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<p>Inner surface morphologies of the tubes with different initial inner surface roughness before and after rolling: (<b>a</b>,<b>c</b>,<b>e</b>) refer to the seamless tubes with the initial surface roughness (<span class="html-italic">S</span><sub>a</sub>) of 0.772 μm, 1.151 μm, and 1.483 μm, respectively, before rolling; (<b>b</b>,<b>d</b>,<b>f</b>) correspond to the morphology of the inner surface of the seamless tube after rolling, compared to (<b>a</b>,<b>c</b>,<b>e</b>), respectively.</p>
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<p>Room temperature mechanical properties of the cold-pilgered tubes with different tempering temperatures.</p>
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<p>Microstructures of the inner surfaces along the axial direction for (<b>a</b>) the tube before rolling, (<b>b</b>) the cold-pilgered tube, and (<b>c</b>) the tube after 600 °C tempering.</p>
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14 pages, 2691 KiB  
Article
Analysis of Mineral Composition and Isotope Ratio as Part of Chemical Profiles of Apples for Their Authentication
by Boris Krška, Martin Mészáros, Tomáš Bílek, Aleš Vávra, Jan Náměstek and Jiří Sedlák
Agronomy 2024, 14(11), 2703; https://doi.org/10.3390/agronomy14112703 (registering DOI) - 16 Nov 2024
Abstract
One of the consequences of the globalisation of food markets is the effort enabling the control of food security and its origin. This might be traced by using different chemical composition analyses. However, for Central Europe, there is a lack of knowledge about [...] Read more.
One of the consequences of the globalisation of food markets is the effort enabling the control of food security and its origin. This might be traced by using different chemical composition analyses. However, for Central Europe, there is a lack of knowledge about the original reference values as well as their heterogeneity among the lands and countries. This study focused on characterizing the mineral profiles of apple tree fruits and comparing these profiles among different districts in Central Europe. The fruits of the apple cultivars ‘Gala’ and ‘Golden Delicious’ originated in the Czech Republic and Poland. The mineral and isotopic content of the apple fruit flesh was analysed using ICP-MS. The data were processed using the ANOVA test and compositely analysed using the PCA and LDA models. The results show relatively high variation in element distribution, particularly 87Sr/86Sr, Mn, Zn, Cu, Ca, P, and B, ranging between 20.6 and67.9% for both cultivars on average. However, their high variability within particular districts complicates the resolution of the LDA model. The reasons are linked to the geomorphological and pedological heterogeneity of the analysed districts as well as the particular sensitivity of the set of chosen primers to agronomic practices and tree performance. For this region, only partial separation among districts could be obtained by P, Ca, and Cu content, as well as the isotopic ratio of 10B/11B. However, the resolution of the geographical discrimination needs to be improved by an enhanced set of primers, the use of more precise analytical techniques for the Sr isotopic ratio, or by multiple chemical analyses. Furthermore, the heterogeneity of the analysed districts could be tackled by more detailed analyses at the level of micro-regions. Full article
(This article belongs to the Section Horticultural and Floricultural Crops)
20 pages, 8203 KiB  
Article
An In Vitro Oxidative Stress Model of the Human Inner Ear Using Human-Induced Pluripotent Stem Cell-Derived Otic Progenitor Cells
by Minjin Jeong, Sho Kurihara and Konstantina M. Stankovic
Antioxidants 2024, 13(11), 1407; https://doi.org/10.3390/antiox13111407 (registering DOI) - 16 Nov 2024
Viewed by 40
Abstract
The inner ear organs responsible for hearing (cochlea) and balance (vestibular system) are susceptible to oxidative stress due to the high metabolic demands of their sensorineural cells. Oxidative stress-induced damage to these cells can cause hearing loss or vestibular dysfunction, yet the precise [...] Read more.
The inner ear organs responsible for hearing (cochlea) and balance (vestibular system) are susceptible to oxidative stress due to the high metabolic demands of their sensorineural cells. Oxidative stress-induced damage to these cells can cause hearing loss or vestibular dysfunction, yet the precise mechanisms remain unclear due to the limitations of animal models and challenges of obtaining living human inner ear tissue. Therefore, we developed an in vitro oxidative stress model of the pre-natal human inner ear using otic progenitor cells (OPCs) derived from human-induced pluripotent stem cells (hiPSCs). OPCs, hiPSCs, and HeLa cells were exposed to hydrogen peroxide or ototoxic drugs (gentamicin and cisplatin) that induce oxidative stress to evaluate subsequent cell viability, cell death, reactive oxygen species (ROS) production, mitochondrial activity, and apoptosis (caspase 3/7 activity). Dose-dependent reductions in OPC cell viability were observed post-exposure, demonstrating their vulnerability to oxidative stress. Notably, gentamicin exposure induced ROS production and cell death in OPCs, but not hiPSCs or HeLa cells. This OPC-based human model effectively simulates oxidative stress conditions in the human inner ear and may be useful for modeling the impact of ototoxicity during early pregnancy or evaluating therapies to prevent cytotoxicity. Full article
(This article belongs to the Special Issue Oxidative Stress in Hearing Loss)
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<p>Derivation and characterization of OPCs from hiPSCs. (<b>a</b>) Scheme illustrating the generation of OPCs from hiPSCs and corresponding stages of human development. hiPSCs resemble the inner cell mass (ICM), while OPCs correspond to the otocyst stage. (<b>b</b>) Representative bright-field images of SK8-A hiPSCs on day 0 and derived OPCs on day 20. Scale bars, 100 µm. (<b>c</b>) qRT-PCR data showing fold changes in mRNA expression of otic-related markers (<span class="html-italic">PAX2</span>, <span class="html-italic">PAX8</span>, and <span class="html-italic">GATA3</span>) in OPCs compared to hiPSCs. The expression levels in hiPSCs were set to 1. Mean ± SD; * <span class="html-italic">p</span> &lt; 0.05; *** <span class="html-italic">p</span> &lt; 0.001. (<b>d</b>) Representative immunocytochemistry images showing protein expression of otic lineage markers in OPCs. hiPSCs were used as negative controls to verify the absence of false-positive signals. Scale bars, 100 µm. Abbreviations: <span class="html-italic">PAX2</span>, paired box 2; <span class="html-italic">PAX8</span>, paired box 8; <span class="html-italic">GATA3</span>, GATA binding protein 3. See “Statistical analysis and reproducibility” in <a href="#sec2dot6-antioxidants-13-01407" class="html-sec">Section 2.6</a> for statistics and experimental information.</p>
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<p>Effects of H<sub>2</sub>O<sub>2</sub> on cell viability and death. (<b>a</b>) Dose-response curves of H<sub>2</sub>O<sub>2</sub> in hiPSCs, HeLa cells, and OPCs. The percentages of viable hiPSCs and HeLa cells were measured after treatment with 15.625, 31.25, 62.5, 125, 250, 500, and 1000 μM H<sub>2</sub>O<sub>2</sub> for 24 h. OPCs were treated with 1.56, 3.13, 6.25, 12.5, 25, 50, and 100 mM H<sub>2</sub>O<sub>2</sub> for 24 h. * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, **** <span class="html-italic">p</span> &lt; 0.0001. (<b>b</b>) Real-time cell death measurements under control (vehicle), 12.5 mM, and 25 mM H<sub>2</sub>O<sub>2</sub> conditions are displayed as gray, light orange, and orange circles, respectively. Cell viability is expressed as the mean percentage ± SD. (<b>c</b>) Phase contrast and merged red fluorescent propidium iodide (PI)-positive images of OPCs, taken 24 h post-exposure to H<sub>2</sub>O<sub>2</sub>. Images were captured at 20× magnification using the IncuCyte<sup>®</sup> imager. Scale bars, 200 μm. See “Statistical analysis and reproducibility” in <a href="#sec2dot6-antioxidants-13-01407" class="html-sec">Section 2.6</a> for statistics and experimental information.</p>
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<p>Effects of gentamicin on cell viability and death. (<b>a</b>) Dose-response curves of the gentamicin in hiPSCs, HeLa cells, and OPCs. The percentage of viable hiPSCs, HeLa cells, and OPCs were measured after treatment with 75, 150, 300, 600, 1200, 2400, and 4800 μM gentamicin for 24 h. Cell viability is expressed as the mean percentage ± SD. * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.005, **** <span class="html-italic">p</span> &lt; 0.0001. (<b>b</b>) Real-time cell death measurements under 0 (vehicle), 150, and 600 μM gentamicin (genta) conditions are displayed as gray, light orange, and orange circles, respectively. (<b>c</b>) Phase contrast and merged red fluorescent propidium iodide (PI)-positive images of OPCs, taken 24 h post-treatment with gentamicin. Images were captured at 20× magnification using the IncuCyte<sup>®</sup> imager. Scale bars, 200 μm. See “Statistical analysis and reproducibility” in <a href="#sec2dot6-antioxidants-13-01407" class="html-sec">Section 2.6</a> for statistics and experimental information.</p>
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<p>Effects of cisplatin on cell viability and death. (<b>a</b>) Dose-response curves of the cisplatin in hiPSCs, HeLa cells, and OPCs. Cell viability of hiPSCs was measured after treatment with 1.56, 3.12, 6.25, 12.5, 25, 50, and 100 μM cisplatin for 24 h. Cell viability of HeLa cells was measured after treatment with 1.56, 3.13, 6.25, 12.5, 25, 50, 100, and 200 μM cisplatin for 24 h. OPCs were treated with 12.5, 25, 50, 100, 200, 400, and 800 μM cisplatin for 24 h. Cell viability is expressed as the mean percentage ± SD. * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.005, **** <span class="html-italic">p</span> &lt; 0.0001. (<b>b</b>) Real-time cell death measurements under 0 (vehicle), 25 and 50 μM cisplatin (cis) conditions are displayed as gray, light orange, and orange circles, respectively. (<b>c</b>) Phase contrast and merged red fluorescent propidium iodide (PI)-positive images of OPCs, taken 24 h post-treatment with cisplatin. Images were captured at 20× magnification using the IncuCyte<sup>®</sup> imager. Scale bars, 200 μm. See “Statistical analysis and reproducibility” in <a href="#sec2dot6-antioxidants-13-01407" class="html-sec">Section 2.6</a> for statistics and experimental information.</p>
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<p>Real-time detection of apoptosis in live OPCs. Apoptosis was visualized using BioTracker NucView caspase 3/7 enzyme activity as a red fluorescent signal. (<b>a</b>) OPCs were treated with vehicle, 300, and 600 μM gentamicin and observed over 24 h. Representative images of OPCs 20 h post-treatment. Top row shows merged phase contrast and red fluorescent images, bottom row shows red fluorescent images. (<b>b</b>) Red object count plotted over time, normalized to 0 h. A significant increase in caspase 3/7 enzyme activity was observed in the 600 μM gentamicin (genta) group compared to the vehicle group from 5 h. (<b>c</b>) Representative images of OPCs 20 h post-treatment with vehicle, 25, and 50 μM cisplatin. (<b>d</b>) Red object count plotted over time, normalized to 0 h. From 11 h, a significant increase in caspase 3/7 enzyme activity was observed in the 50 μM cisplatin (cis) group compared to the vehicle group. Data represent the mean of 3 independent experiments, each with 4 technical replicates per time point ± SD. Scale bars, 200 μm.</p>
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<p>Effects of gentamicin and cisplatin on OPC mitochondria. (<b>a</b>,<b>b</b>) Representative fluorescence images of OPCs stained with DAPI (nuclei in blue), Mito-Tracker (mitochondria in red), and cytochrome c (cyt c in red) at 0, 6, and 24 h after treatment with 600 μM gentamicin (<b>a</b>) and 50 μM cisplatin (<b>b</b>). Scale bars: 20 μm. (<b>c</b>,<b>d</b>) Quantification of active mitochondria by measuring the percentage of Mito-Tracker positive area, normalized to the number of DAPI-stained nuclei at 0, 6, and 24 h after treatment with 300 and 600 μM gentamicin (<b>c</b>), and 25 and 50 μM cisplatin (<b>d</b>). Mito-Tracker positivity at 0 h was set to 100%. ns, not significant, * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, **** <span class="html-italic">p</span> &lt; 0.0001. See “Statistical analysis and reproducibility” in <a href="#sec2dot6-antioxidants-13-01407" class="html-sec">Section 2.6</a> for statistics and experimental information.</p>
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<p>Real-time detection of reactive oxygen species (ROS) in live OPCs. (<b>a</b>) Intracellular ROS production was visualized using CellROX reagent as a red fluorescent signal. OPCs were treated with vehicle, 300, and 600 μM gentamicin and observed over 24 h. Representative images of OPCs 12 h post-treatment are displayed. The top row shows merged phase contrast and red fluorescent images, while the bottom row shows red fluorescent images alone. (<b>b</b>) Red mean intensity was plotted over time, normalized to 0 h. A significant increase in ROS production was observed in the 600 μM gentamicin (genta) group compared to the vehicle group from 6 h, and in the 300 μM gentamicin group from 8 h. (<b>c</b>) Representative images of OPCs 12 h post-treatment with vehicle, 25, and 50 μM cisplatin. (<b>d</b>) Red mean intensity plotted over time, normalized to 0 h. From 8 h, a significant increase in ROS production was observed in the 50 μM cisplatin (cis) group compared to the vehicle group. From 16 h, a significant increase was also observed in the 25 μM cisplatin group compared to the vehicle group. Data represent the mean of 3 independent experiments, each with 4 technical replicates per time point ± SD. * <span class="html-italic">p</span> &lt; 0.05. Scale bars, 200 μm.</p>
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10 pages, 2387 KiB  
Article
Controlled Formation of Porous Cross-Bar Arrays Using Nano-Transfer Printing
by Yu Na Kim, Eun Bin Kang, Tae Wan Park and Woon Ik Park
Materials 2024, 17(22), 5609; https://doi.org/10.3390/ma17225609 (registering DOI) - 16 Nov 2024
Viewed by 72
Abstract
Nano-transfer printing (nTP) has emerged as an effective method for fabricating three-dimensional (3D) nanopatterns on both flat and non-planar substrates. However, most transfer-printed 3D patterns tend to exhibit non-discrete and/or non-porous structures, limiting their application in high-precision nanofabrication. In this study, we introduce [...] Read more.
Nano-transfer printing (nTP) has emerged as an effective method for fabricating three-dimensional (3D) nanopatterns on both flat and non-planar substrates. However, most transfer-printed 3D patterns tend to exhibit non-discrete and/or non-porous structures, limiting their application in high-precision nanofabrication. In this study, we introduce a simple and versatile approach to produce highly ordered, porous 3D cross-bar arrays through precise control of the nTP process parameters. By selectively adjusting the polymer solution concentration and spin-coating conditions, we successfully generated discrete, periodic line patterns, which were then stacked at a 90-degree angle to form a porous 3D cross-bar structure. This technique enabled the direct transfer printing of PMMA line patterns with well-defined, square-arrayed holes, without requiring additional deposition of functional materials. This method was applied across diverse substrates, including planar Si wafers, flexible PET, metallic copper foil, and transparent glass, demonstrating its adaptability. These well-defined 3D cross-bar patterns enhance the versatility of nTP and are anticipated to find broad applicability in various nano-to-microscale electronic devices, offering high surface area and structural precision to support enhanced functionality and performance. Full article
(This article belongs to the Special Issue Advances in Materials Processing (3rd Edition))
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Graphical abstract
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<p>Schematic illustration of the pattern formation process for PMMA cross-bar structures using pattern-transfer printing. Step 1: PMMA pattern replication—the spin-coated PMMA layer is peeled off from the Si master mold using PI tape. Step 2: transfer printing—the discretized PMMA patterns are transferred onto the target substrate.</p>
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<p>Control of the spin-coated PMMA thickness on the Si mold as a function of PMMA concentration. (<b>a</b>) Si master mold with a space width of 2 µm and a line width of 250 nm, fabricated via conventional photolithography. Scale bar: 1 cm. (<b>b</b>) SEM image of the Si master mold. Scale bars: 4 µm, 2 µm. (<b>c</b>) Filling level of the Si mold as influenced by PMMA concentration. Scale bar: 1 µm. The thickness of the PMMA film increases proportionally with the weight percentage of the PMMA solution.</p>
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<p>The effect of spin-coating rotational speed on the thickness of the PMMA film. (<b>a</b>) Tilted SEM images showing PMMA thin films on the Si line/space mold at different spin-coating speeds. Scale bar: 1 µm. (<b>b</b>) Graph illustrating the thickness of the coated PMMA film on the Si mold with lines and spaces, as a function of rotational speed. As the spin-coating speed increases, the thickness of the PMMA film decreases.</p>
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<p>Well-defined, discrete PMMA line patterns after the nTP process. (<b>a</b>) Photographs of the replicated PMMA line pattern from the Si mold (upper) and the transfer-printed PMMA line pattern on a planar Si substrate (lower). (<b>b</b>) Top-view SEM image showing the periodic PMMA line/space pattern (3.0 wt% solution) transferred at a spin speed of 5000 rpm. Scale bar: 4 µm. (<b>c</b>) Tilted SEM image of the discrete PMMA line pattern with a 2 µm width, tilted from the top-view shown in (<b>b</b>). Scale bar: 2 µm. The SEM images highlight the well-defined, discrete PMMA line array, with a thickness of approximately 105 nm.</p>
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<p>Multi-layer stacking of well-ordered PMMA line patterns on various substrates by the repeated nTP process. PMMA cross-bar patterns were successfully transfer-printed onto several substrates, including (<b>a</b>) Si wafer, (<b>d</b>) PET, copper foil, and glass. (<b>a</b>) PMMA cross-bar structure stacked on a Si wafer using the nTP process. (<b>b</b>) Surface plot of a 3D image of the PMMA cross-bar structure, clearly showing the well-organized nanoporous pattern with open areas. (<b>c</b>) SEM image of the multi-layered PMMA pattern across a large area. (<b>d</b>) Photographs (left) and SEM images (right) of PMMA cross-bar patterns, showing well-defined PMMA nanoporous structures on PET, copper foil, and glass.</p>
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17 pages, 996 KiB  
Article
Geographically-Informed Modeling and Analysis of Platform Attitude Jitter in GF−7 Sub-Meter Stereo Mapping Satellite
by Haoran Xia, Xinming Tang, Fan Mo, Junfeng Xie and Xiang Li
ISPRS Int. J. Geo-Inf. 2024, 13(11), 413; https://doi.org/10.3390/ijgi13110413 (registering DOI) - 15 Nov 2024
Viewed by 227
Abstract
The GF−7 satellite, China’s inaugural sub-meter-level stereoscopic mapping satellite, has been deployed for a wide range of applications, including natural resource investigation, environmental monitoring, fundamental surveying, and the development of global geospatial information resources. The satellite’s stable platform and reliable imaging systems are [...] Read more.
The GF−7 satellite, China’s inaugural sub-meter-level stereoscopic mapping satellite, has been deployed for a wide range of applications, including natural resource investigation, environmental monitoring, fundamental surveying, and the development of global geospatial information resources. The satellite’s stable platform and reliable imaging systems are crucial for achieving high-quality imaging and precise attitude measurements. However, the satellite’s operation is affected by both internal and external factors, which induce vibrations in the satellite platform, thereby affecting image quality and mapping accuracy. To address this challenge, this paper proposes a novel method for constructing a satellite platform vibration model based on geographic location information. The model is developed by integrating composite data from star sensors and gyroscopes (gyro) with subsatellite point location data. The experimental methodology involves the composite processing of gyro data and star sensor optical axis angles, integration of the processed data through time-matching and normalization, and denoising of the integrated data, followed by trigonometric fitting to capture the periodic characteristics of platform vibrations. The positions of the satellite substellar points are determined from the satellite orbit data. A rigorous geometric imaging model is then used to construct a vibration model with geographic location correlation in combination with the satellite subsatellite point positions. The experimental results demonstrate the following: (1) Over the same temporal range, there is a significant convergence in the waveform similarities between the gyro data and the star sensor optical axis angles, indicating a strong correlation in the jitter information; (2) The platform vibration exhibits a robust correlation with the satellite’s geographic location along its orbit. Specifically, the model reveals that the GF−7 satellite experiences the maximum vibration amplitude between 5° S and 20° S latitude during its ascending phase, and the minimum vibration amplitude between 5° N and 20° N latitude during the descending phase. The model established in this study offers theoretical support for optimizing satellite attitude and mitigating platform vibrations. Full article
20 pages, 2331 KiB  
Article
Reconstruction of Hourly Gap-Free Sea Surface Skin Temperature from Multi-Sensors
by Qianguang Tu, Zengzhou Hao, Dong Liu, Bangyi Tao, Liangliang Shi and Yunwei Yan
Remote Sens. 2024, 16(22), 4268; https://doi.org/10.3390/rs16224268 (registering DOI) - 15 Nov 2024
Viewed by 215
Abstract
The sea surface skin temperature (SSTskin) is of critical importance with regard to air–sea interactions and marine carbon circulation. At present, no single remote sensor is capable of providing a gap-free SSTskin. The use of data fusion techniques is [...] Read more.
The sea surface skin temperature (SSTskin) is of critical importance with regard to air–sea interactions and marine carbon circulation. At present, no single remote sensor is capable of providing a gap-free SSTskin. The use of data fusion techniques is therefore essential for the purpose of filling these gaps. The extant fusion methodologies frequently fail to account for the influence of depth disparities and the diurnal variability of sea surface temperatures (SSTs) retrieved from multi-sensors. We have developed a novel approach that integrates depth and diurnal corrections and employs advanced data fusion techniques to generate hourly gap-free SST datasets. The General Ocean Turbulence Model (GOTM) is employed to model the diurnal variability of the SST profile, incorporating depth and diurnal corrections. Subsequently, the corrected SSTs at the same observed time and depth are blended using the Markov method and the remaining data gaps are filled with optimal interpolation. The overall precision of the hourly gap-free SSTskin generated demonstrates a mean bias of −0.14 °C and a root mean square error of 0.57 °C, which is comparable to the precision of satellite observations. The hourly gap-free SSTskin is vital for improving our comprehension of air–sea interactions and monitoring critical oceanographic processes with high-frequency variability. Full article
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