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Search Results (5,684)

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Keywords = thermal transformation

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35 pages, 14202 KiB  
Article
Phase Transitions and Structural Evolution of Manganese Ores During High-Temperature Treatment
by Ruslan Z. Safarov, Yerlan A. Baikenov, Assemgul K. Zhandildenova, Eldar E. Kopishev, Ruslan M. Kamatov, Jumat B. Kargin, Henry Sanchez Cornejo, Crispin H. W. Barnes and Luis De Los Santos Valladares
Metals 2025, 15(1), 89; https://doi.org/10.3390/met15010089 (registering DOI) - 18 Jan 2025
Abstract
The aim of this research is to investigate the phase composition and structural peculiarities of complex metamorphic manganese ores from Central Kazakhstan before and after sintering in the temperature range of 600–1200 °C in an air atmosphere. X-ray diffraction, X-ray fluorescence, scanning electron [...] Read more.
The aim of this research is to investigate the phase composition and structural peculiarities of complex metamorphic manganese ores from Central Kazakhstan before and after sintering in the temperature range of 600–1200 °C in an air atmosphere. X-ray diffraction, X-ray fluorescence, scanning electron microscopy, and optical microscopy were used to analyze changes in elemental and phase composition. In their initial state, according to XRF analysis, the Bogach ore was manganese-rich, with a manganese content of 60.77 wt.%, while the Zhaksy ore contained manganese (44.88 wt.%), silicon (20.85 wt.%), and iron (6.14 wt.%) as its main components. In the Bogach ore samples, manganese content increased from 60.77% to 65.7% as the sintering temperature rose to 1100 °C, while the hausmannite phase (Mn3O4) emerged as the dominant phase, comprising 95.77% of the crystalline component at 1200 °C. Conversely, the Zhaksy ore samples displayed a sharp increase in braunite-phase (Mn7O12Si) content, reaching 83.81% at 1100 °C, alongside significant quartz amorphization. The degree of crystallinity in Bogach ore peaked at 56.2% at 900 °C but declined at higher temperatures due to amorphous phase formation. A surface morphology analysis revealed the transformation of dense, non-uniform particles into porous, granular structures with pronounced recrystallization as the temperature increased. In the Bogach samples, sintering at 900 °C resulted in elongated, needle-like crystalline formations, while at 1200 °C, tetragonal crystals of hausmannite dominated, indicating significant grain growth and recrystallization. For Zhaksy samples, sintering at 1100 °C led to a porous morphology with interconnected grains and microvoids, reflecting enhanced braunite crystallization and quartz amorphization. These findings provide quantitative insights into optimizing manganese oxide phases for industrial applications, such as catalysts and pigments, and emphasize the impact of thermal treatment on phase stability and structural properties. This research contributes to the development of efficient processing technologies for medium-grade manganese ores, aligning with Kazakhstan’s strategic goals in sustainable resource utilization. Full article
(This article belongs to the Special Issue Recent Progress in Metal Extraction and Recycling)
21 pages, 1281 KiB  
Article
Thermal Characteristics and Kinetics of the Thermal Degradation of Sugar Beet Waste Leaves and Pulp in Relation to Chemical Composition
by Sanja Ostojić, Darko Micić, Josipa Dukić, Iva Sabljak, Ayça Akyüz, Seda Ersus and Anet Režek Jambrak
Foods 2025, 14(2), 307; https://doi.org/10.3390/foods14020307 - 17 Jan 2025
Abstract
Thermal characteristics of dried sugar beet pulp, leaves and leaf fractions obtained after extraction: fibrous leaf pulp and fibre rich leaf fraction, were investigated by differential scanning calorimetry and thermogravimetry. The sugar beet samples showed a similar thermal behaviour associated with a similar [...] Read more.
Thermal characteristics of dried sugar beet pulp, leaves and leaf fractions obtained after extraction: fibrous leaf pulp and fibre rich leaf fraction, were investigated by differential scanning calorimetry and thermogravimetry. The sugar beet samples showed a similar thermal behaviour associated with a similar composition. Two endotherms are found on the differential scanning calorimetry curves. First one in the temperature range 31–153 °C and the second from 150–160 °C. Thermal degradation kinetics was studied by thermogravimetric analysis. Four degradation stages were observed within the temperature range 25–700 °C. The kinetic parameters of the degradation, obtained by Ortega and Friedman non-isothermal isoconversional methods did not significantly differ between models: Ea-activation energy at a conversion degree 0.1–0.9 ranged 50–200 kJ/mol; lnA- the natural logarithm of the pre-exponential factor 8–48; kp1-thermal degradation rate constant at a conversion extent of 0.5 ranged of 0.19–2.55 min−1. Constant rate of degradation is highest for the sugar beet leaves kp1 (2.58–2.55 min−1), and kp2 (70.1–70.4 min−1). The results obtained are valuable for sugar beet leaf industrial processing. A positive environmental impact is achieved by transforming the waste into high-value food additives. Full article
35 pages, 5025 KiB  
Article
Historical Analysis of Real Energy Consumption and Indoor Conditions in Single-Family Passive Building
by Szymon Firląg, Abdullah Sikander Baig and Dariusz Koc
Sustainability 2025, 17(2), 717; https://doi.org/10.3390/su17020717 (registering DOI) - 17 Jan 2025
Abstract
The paper includes a historical analysis of real energy consumption and indoor conditions in a single-family passive building located in Warsaw, Poland. Passive houses have emerged as a sustainable alternative to the conventional construction of houses, having advantages such as low energy consumption, [...] Read more.
The paper includes a historical analysis of real energy consumption and indoor conditions in a single-family passive building located in Warsaw, Poland. Passive houses have emerged as a sustainable alternative to the conventional construction of houses, having advantages such as low energy consumption, comfortable indoor temperatures, an environmentally friendly nature, and low carbon emissions. This research consists of indoor temperature assessments over a 5-year period (2018–2022) which include comfort assessments made in accordance with the standard EN 16798-1 and precise assessments made for extreme weather events over a two-week critical period including the heating and cooling seasons. The real energy consumption analysis, including electric heating, outdoor lighting, indoor lighting, ventilation, and domestic hot water, was compared against passive house and nearly-zero energy standards. The results of the study show that the building is thermally comfortable to live in, as it remained mainly in the first comfort category, IEQ I. There was no such issue as overheating and underheating even during extreme weather events. The energy need for heating remained very close to the passive standard, namely 15 kWh/(m2·year). The total primary energy consumption for heating, hot water, and electricity meets the standard required value of 120 kWh/(m2·year). These findings demonstrate the effectiveness of passive house design principles at achieving high levels of thermal comfort and energy efficiency in cold climates. In addition, it is demonstrated that it is possible to maintain comfortable indoor temperatures (even with outdoor air temperatures reaching 35 °C) without air conditioning or cooling systems. The integration of a photovoltaic system offers a viable pathway toward transforming the building into a zero-energy standard, contributing to sustainability goals and reducing carbon emissions. Full article
16 pages, 12395 KiB  
Article
Evaluating Oil Palm Trunk Biochar and Palm Oil as Environmentally Friendly Sustainable Additives in Green Natural Rubber Composites
by Narong Chueangchayaphan, Manop Tarasin, Wimonwan Phonjon and Wannarat Chueangchayaphan
Polymers 2025, 17(2), 223; https://doi.org/10.3390/polym17020223 - 17 Jan 2025
Viewed by 187
Abstract
This research examines the possibility of palm oil and oil palm trunk biochar (OPTB) from pyrolysis effectively serving as alternative processing oils and fillers, substituting petroleum-based counterparts in natural rubber (NR) composites. Chemical, elemental, surface and morphological analyses were used to characterize both [...] Read more.
This research examines the possibility of palm oil and oil palm trunk biochar (OPTB) from pyrolysis effectively serving as alternative processing oils and fillers, substituting petroleum-based counterparts in natural rubber (NR) composites. Chemical, elemental, surface and morphological analyses were used to characterize both carbon black (CB) and OPTB, by using Fourier transform infrared spectroscopy (FTIR), X-ray diffraction (XRD), Brunauer–Emmett–Teller (BET) gas porosimetry, and scanning electron microscopy (SEM). The influences of OPTB contents from 0 to 100 parts per hundred rubber (phr) on thermal, dielectric, dynamic mechanical, and cure characteristics, and the key mechanical properties of particulate NR-composites were investigated. OPTB enhanced the characteristics of the composites, as demonstrated by a rise in dielectric constant, thermal stability, storage modulus, glass transition temperature (Tg), hardness and modulus at 300% elongation, along with a decrease in the loss tangent (tan δ). Tear strength exhibited an increase with OPTB content up to a specific threshold, whereas tensile strength and elongation at break declined. This implies a compromise between the various mechanical properties when incorporating OPTB as a filler. This work supports the potential application of OPTB as a renewable substitute for CB in the rubber industry, particularly in tire production and other industrial rubber applications, which would also bring environmental, sustainability, and economic benefits for the palm oil-related industry. Full article
(This article belongs to the Special Issue Exploration and Innovation in Sustainable Rubber Performance)
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<p>(<b>a</b>) FTIR spectra and (<b>b</b>) XRD analyses of CB and OPTB.</p>
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<p>SEM images of CB and OPTB showing the morphologies of (<b>a</b>) CB at ×250 magnification, (<b>b</b>) CB at ×2500 magnification, (<b>c</b>) OPTB at ×250 magnification, and (<b>d</b>) OPTB at ×2500 magnification.</p>
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<p>Thermal properties of OPTB powder and NR composites: (<b>a</b>) TGA curves and (<b>b</b>) DTG curves.</p>
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<p>Dielectric constants of NR composites by frequency of excitation.</p>
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<p>(<b>a</b>) Storage modulus, (<b>b</b>) loss modulus, and (<b>c</b>) tan δ for the experimental NR composites.</p>
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<p>Storage modulus vs. strain for the NR composites.</p>
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<p>Time profiles of torque for the NR compounds.</p>
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<p>Physical and mechanical properties of NR composites: (<b>a</b>) hardness, (<b>b</b>) tear strength, (<b>c</b>) stress–strain curves, (<b>d</b>) modulus @300%, (<b>e</b>) tensile strength, and (<b>f</b>) elongation at break.</p>
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14 pages, 5173 KiB  
Article
Synthesis, Characterization, and Cytotoxicity Research of Sulfur-Containing Metal Complexes
by Yanting Yang, Danqin Li and Mei Luo
Inorganics 2025, 13(1), 26; https://doi.org/10.3390/inorganics13010026 - 17 Jan 2025
Viewed by 94
Abstract
In this experiment, the excellent coordination ability of sulfur-containing ligands was utilized. Diphenylacetyl disulfide and 3,3′-diaminodiphenyl sulfone were selected as ligands, and Cu(NO3)2·3H2O, Ni(NO3)2·6H2O and ZnCl2 were reacted under one-pot [...] Read more.
In this experiment, the excellent coordination ability of sulfur-containing ligands was utilized. Diphenylacetyl disulfide and 3,3′-diaminodiphenyl sulfone were selected as ligands, and Cu(NO3)2·3H2O, Ni(NO3)2·6H2O and ZnCl2 were reacted under one-pot conditions to synthesize three mononuclear complexes: [C4H18CuO12S2](I), [C12H18N4NiO11S](II) and [C24H24Cl2N4O4S2Zn](III). Complex (I) belongs to the orthorhombic crystal system with space group Pbca, while complexes (II) and (III) belong to the monoclinic crystal system with space groups P21/n and P2/n. The crystal structure of the complex was determined using X-ray diffraction (XRD). The structure of the complex was analyzed using infrared Fourier transform infrared spectroscopy (FT-IR), ultraviolet–visible spectroscopy (UV–Vis), nuclear magnetic resonance (NMR), and electrospray mass spectrometry (ESI-MS), and the thermal stability and composition of the complex were detected via thermogravimetry (TGA). In terms of application, the biological activity of complexes (I)–(III) in human cancer cell lines (lung cancer A549, liver cancer SMMC-7721, breast cancer MDA-MB-231, and colon cancer SW480) was tested using the MTS method. The results showed that complex (II) had a good inhibitory effect on breast cancer MDA-MB-231. Full article
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<p>Synthesis protocol of complexes (I)–(III). (<b>a</b>) for (I), (<b>b</b>) for S<sub>8</sub>, (<b>c</b>) for (II) and (<b>d</b>) for (III).</p>
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<p>ORTEP molecular structures of complexes, (<b>a</b>) for (I), (<b>b</b>) for S<sub>8</sub>, (<b>c</b>) for (II) and (<b>d</b>) for (III), with a 30% thermal ellipsoid probability.</p>
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<p>IR spectra of complexes (I) to (III) in the 4000–500 cm<sup>−1</sup> region.</p>
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<p>UV–Vis spectra of complexes (I)–(III) in the range of 200–1000 nm. ((<b>a</b>) shows the UV absorption spectra of complexes I–III at 200–800nm, while (<b>b</b>) shows the UV absorption spectra of complexes I–II at 300–1000 nm).</p>
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<p><sup>1</sup>H NMR (<b>a</b>) and <sup>13</sup>C NMR (<b>b</b>) spectra of complex (III).</p>
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<p>Electrospray ionization mass spectra of complexes (I)–(III).</p>
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<p>Thermogravimetric analysis (TGA) decomposition curves of complexes (I)–(III).</p>
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17 pages, 37474 KiB  
Article
The Deformation Mechanism of the Rings of Angular-Contact Ball Bearings During the Quenching and Tempering Process
by Ruijie Gu, Yi Tong, Qiang Wang, Liaoyuan Chen and Ziyang Shang
Machines 2025, 13(1), 64; https://doi.org/10.3390/machines13010064 - 17 Jan 2025
Viewed by 143
Abstract
During the heat treatment process, bearing rings are subjected to drastic temperature variability and complex microstructural evolution, which result in deformation, high residual stresses, operational instability and a limited operating life. However, the underlying relationship between temperature, phase transformation, and deformation has not [...] Read more.
During the heat treatment process, bearing rings are subjected to drastic temperature variability and complex microstructural evolution, which result in deformation, high residual stresses, operational instability and a limited operating life. However, the underlying relationship between temperature, phase transformation, and deformation has not been fully revealed in previous research. As a result, it is difficult to accurately control the roundness of bearing rings during the heat treatment process. Therefore, a combination of numerical simulations and experimental methods was employed to analyze the heat treatment process of the rings of angular-contact ball bearings (ACBB) (7008C). Firstly, according to the multiple coupling theory of thermal, phase-transition, and stress–strain fields, a model for the numerical simulation of the quenching and tempering process was established. Secondly, the thermal–physical properties of the material were calculated using the Jmatpro 7.0 software, and the quenching and tempering processes were numerically simulated using the Deform software. Subsequently, the evolution of the stress, phase-transformation, and deformation behaviors of bearing rings during the quenching and tempering were studied in detail. Finally, the roundness errors of the bearing rings were obtained by a coordinate-measuring machine (CMM). The results showed that the axial and radial stress distributions at the surface and center of the bearing rings were significantly different. The bearing rings experienced uneven expansion and deformation. The roundness errors of the inner diameter and outer diameter of the inner ring were 0.0386 mm and 0.0423 mm, respectively. The roundness errors of the inner diameter and outer diameter of the outer ring were 0.0202 mm and 0.0180 mm, respectively. In this study, the mechanism of the effect of the temperature variation and phase transformation on deformation during the quenching and tempering process was revealed in detail. This provides a reference for controlling the roundness of bearing rings in actual production processes. Full article
(This article belongs to the Section Material Processing Technology)
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<p>The heat treatment multi-field coupling schematic.</p>
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<p>The geometric structures of the bearing rings: (<b>a</b>) inner ring; (<b>b</b>) outer ring.</p>
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<p>The schematic diagram of mesh and fixed nodes: (<b>a</b>) inner ring; (<b>b</b>) outer ring.</p>
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<p>The content of elements in bearing rings.</p>
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<p>The quenching and tempering process of the bearing rings.</p>
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<p>A schematic diagram of the controlled-atmosphere production line with the roller mesh belt.</p>
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<p>A schematic diagram of the CMM.</p>
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<p>A schematic diagram of the nodes.</p>
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<p>The variation in stress with time during quenching cooling: (<b>a</b>) effective stress; (<b>b</b>) axial stress; (<b>c</b>) radial stress; (<b>d</b>) circumferential stress.</p>
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<p>The dimensional variation during the quenching heating process of the inner ring: (<b>a</b>) a heating time of 5 s; (<b>b</b>) a heating time of 736 s; (<b>c</b>) at the end of the heating process.</p>
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<p>The dimensional variation during the quenching heating process of the outer ring: (<b>a</b>) a heating time of 5 s; (<b>b</b>) a heating time of 736 s; (<b>c</b>) at the end of the heating process.</p>
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<p>The dimensional variation during the quenching heating process of the inner ring: (<b>a</b>) A schematic diagram of the nodes; (<b>b</b>) The dimensional variation curve of the inner ring during the heating process; (<b>c</b>) The variation curve of the microstructure and dimension with temperature during the heating process at point P1.</p>
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<p>The dimensional variations during the quenching cooling process of the inner ring: (<b>a</b>) a cooling time of 3 s; (<b>b</b>) a cooling time of 14 s; (<b>c</b>) the end of cooling.</p>
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<p>The dimensional variations during the quenching cooling process of the outer ring: (<b>a</b>) a cooling time of 3 s; (<b>b</b>) a cooling time of 14 s; (<b>c</b>) the end of cooling.</p>
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<p>The dimensional variation during the quenching cooling process of the inner ring: (<b>a</b>) The schematic diagram of nodes; (<b>b</b>) The dimensional variation curve of the inner ring during the cooling process; (<b>c</b>) The variation curve of microstructure and dimension with temperature during the cooling process at point P1.</p>
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<p>The simulation results for the dimension of the bearing rings after the quenching and tempering processes: (<b>a</b>) the roundness of the inner diameter of the inner ring; (<b>b</b>) the roundness of the outer diameter of the inner ring; (<b>c</b>) the roundness of the inner diameter of the outer ring; (<b>d</b>) the roundness of the outer diameter of the outer ring.</p>
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<p>The experimental results are compared with the simulation results: (<b>a</b>) the roundness error of the inner ring; (<b>b</b>) the roundness error of the outer ring.</p>
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18 pages, 2041 KiB  
Article
A Wavelet Transform-Based Transfer Learning Approach for Enhanced Shaft Misalignment Diagnosis in Rotating Machinery
by Houssem Habbouche, Tarak Benkedjouh, Yassine Amirat and Mohamed Benbouzid
Electronics 2025, 14(2), 341; https://doi.org/10.3390/electronics14020341 - 17 Jan 2025
Viewed by 142
Abstract
Rotating machines are vital for ensuring reliability, safety, and operational availability across various industrial sectors. Among the faults that can affect these machines, shaft misalignment is particularly critical due to its impact on other components connected to the shaft, making it a key [...] Read more.
Rotating machines are vital for ensuring reliability, safety, and operational availability across various industrial sectors. Among the faults that can affect these machines, shaft misalignment is particularly critical due to its impact on other components connected to the shaft, making it a key focus for diagnostic systems. Misalignment can lead to significant energy losses, and therefore, early detection is crucial. Vibration analysis is an effective method for identifying misalignment at an early stage, enabling corrective actions before it negatively impacts equipment efficiency and energy consumption. To improve monitoring efficiency, it is essential that the diagnostic system is not only intelligent but also capable of operating in real-time. This study proposes a methodology for diagnosing shaft misalignment faults by combining wavelet transform for feature extraction and transfer learning for fault classification. The accuracy of the proposed soft real-time solution is validated through a comparison with other time-frequency transformation techniques and transfer learning networks. The methodology also includes an experimental procedure for simulating misalignment faults using a laser measurement tool. Additionally, the study evaluates the thermal impacts and vibration signature of each type of misalignment fault through multi-sensor monitoring, highlighting the effectiveness and robustness of the approach. First, wavelet transform is used to obtain a good representation of the signal in the time-frequency domain. This step allows for the extraction of key features from multi-sensor vibration signals. Then, the transfer learning network processes these features through its different layers to identify the faults and their severity. This combination provides an intelligent decision-support tool for diagnosing misalignment faults, enabling early detection and real-time monitoring. The proposed methodology is tested on two datasets: the first is a public dataset, while the second was created in the laboratory to simulate shaft misalignment using a laser alignment tool and to demonstrate the effect of this defect on other components through thermal imaging. The evaluation is carried out using various criteria to demonstrate the effectiveness of the methodology. The results highlight the potential of implementing the proposed soft real-time solution for diagnosing shaft misalignment faults. Full article
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<p>Flowchart of the proposed shaft misalignment fault diagnosis.</p>
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<p>AlexNet architecture.</p>
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<p>WT of different signals classes: (<b>a</b>) no misalignment, (<b>b</b>) horizontal misalignment with 0.5 mm, (<b>c</b>) horizontal misalignment with 1.15 mm, (<b>d</b>) vertical misalignment with 0.34 mm, (<b>e</b>) vertical misalignment with 0.8 mm, and (<b>f</b>) vertical misalignment with 1.09 mm.</p>
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<p>Statistical features evolution for normal state: (<b>a</b>) RMS, (<b>b</b>) kurtosis, (<b>c</b>) skewness, and (<b>d</b>) crest factor.</p>
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<p>Confusion matrix, the blue color represents correctly classified samples, while other colors indicate misclassified ones.</p>
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<p>Misalignment test bench: (<b>a</b>) model; (<b>b</b>) real.</p>
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<p>Misalignment control parts, (<b>a</b>) Soft foot, (<b>b</b>) Flexible coupling, and (<b>c</b>) Motor support.</p>
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<p>Experimental setup and data acquisition system for shaft misalignment fault diagnosis using shaft misalignment system Easy-Laser E540.</p>
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<p>Thermal image in the case of Defaut N°1: speed of rotation 3000 RPM using infrared camera Fluke Ti32.</p>
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<p>(<b>a</b>) Vibration signal of the misalignment fault; (<b>b</b>) spectrum of the vibration signal.</p>
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<p>Sketch of the test bench and acquisition chain.</p>
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<p>WT of signal from sensor 3: (<b>a</b>) Fault N°1; (<b>b</b>) Fault N°6.</p>
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<p>Confusion matrix of Data N°1, the blue color represents correctly classified samples, while other colors indicate misclassified ones.</p>
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<p>Confusion matrix of Data N°2, the blue color represents correctly classified samples, while other colors indicate misclassified ones.</p>
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<p>Confusion matrix of Data N°3, the blue color represents correctly classified samples, while other colors indicate misclassified ones.</p>
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17 pages, 4766 KiB  
Article
Monitoring the Maize Canopy Chlorophyll Content Using Discrete Wavelet Transform Combined with RGB Feature Fusion
by Wenfeng Li, Kun Pan, Yue Huang, Guodong Fu, Wenrong Liu, Jizhong He, Weihua Xiao, Yi Fu and Jin Guo
Agronomy 2025, 15(1), 212; https://doi.org/10.3390/agronomy15010212 - 16 Jan 2025
Viewed by 203
Abstract
To evaluate the accuracy of Discrete Wavelet Transform (DWT) in monitoring the chlorophyll (CHL) content of maize canopies based on RGB images, a field experiment was conducted in 2023. Images of maize canopies during the jointing, tasseling, and grouting stages were captured using [...] Read more.
To evaluate the accuracy of Discrete Wavelet Transform (DWT) in monitoring the chlorophyll (CHL) content of maize canopies based on RGB images, a field experiment was conducted in 2023. Images of maize canopies during the jointing, tasseling, and grouting stages were captured using unmanned aerial vehicle (UAV) remote sensing to extract color, texture, and wavelet features and to construct a color and texture feature dataset and a fusion of wavelet, color, and texture feature datasets. Backpropagation neural network (BP), Stacked Ensemble Learning (SEL), and Gradient Boosting Decision Tree (GBDT) models were employed to develop CHL monitoring models for the maize canopy. The performance of these models was evaluated by comparing their predictions with measured CHL data. The results indicate that the dataset integrating wavelet features achieved higher monitoring accuracy compared to the color and texture feature dataset. Specifically, for the integrated dataset, the BP model achieved an R2 value of 0.728, an RMSE of 3.911, and an NRMSE of 15.24%; the SEL model achieved an R2 value of 0.792, an RMSE of 3.319, and an NRMSE of 15.34%; and the GBDT model achieved an R2 value of 0.756, an RMSE of 3.730, and an NRMSE of 15.45%. Among these, the SEL model exhibited the highest monitoring accuracy. This study provides a fast and reliable method for monitoring maize growth in field conditions. Future research could incorporate cross-validation with hyperspectral and thermal infrared sensors to further enhance model reliability and expand its applicability. Full article
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<p>Overview of experimental site location and density settings. Note: D1–D3 represent different densities: 5.7, 6.3, and 6.9 plants/m<sup>2</sup>.</p>
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<p>Flow chart for remote sensing data processing.</p>
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<p>Workflow for removing image background.</p>
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<p>The decomposition procedure of the image. Note: H denotes a high-pass filter, L denotes a low-pass filter, LL denotes the proximate feature, HL denotes the longitudinal edge feature, LH denotes the lateral edge feature, and HH denotes the diagonal feature.</p>
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<p>Stacking ensemble learning implementation process integrating SVR and LightGBM.</p>
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<p>Heatmap of correlation between color and texture features and CHL content.</p>
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<p>Heat map of correlation between wavelet features and CHL content.</p>
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<p>Scatterplot of predicted chlorophyll content of BP, SEL, and GBDT models based on different data.</p>
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<p>Distribution of R<sup>2</sup>, RMSE, and NRMSE at different growth stages of maize.</p>
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<p>Ranking the importance of color, texture, and wavelet features.</p>
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<p>Schematic diagram of discrete wavelet decomposition.</p>
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23 pages, 1277 KiB  
Review
The Role of Ionic Liquids in Textile Processes: A Comprehensive Review
by Anastasia Anceschi, Claudia Riccardi and Alessia Patrucco
Molecules 2025, 30(2), 353; https://doi.org/10.3390/molecules30020353 - 16 Jan 2025
Viewed by 222
Abstract
Thanks to their unique physicochemical properties, ionic liquids (ILs) have moved from niche academic interest to critical components in various industrial applications. The textile industry, facing significant environmental and economic pressures, has begun to explore ILs as sustainable alternatives to traditional solvents and [...] Read more.
Thanks to their unique physicochemical properties, ionic liquids (ILs) have moved from niche academic interest to critical components in various industrial applications. The textile industry, facing significant environmental and economic pressures, has begun to explore ILs as sustainable alternatives to traditional solvents and chemicals. This review summarizes research on the use of ILs in various textile processes, including dyeing, finishing, and fiber recycling, where their high thermal stability, tunable solubility, and low volatility are exploited to reduce resource consumption and environmental impact. The discussion also extends to the integration of ILs in textile waste recycling, highlighting innovative approaches to fiber dissolution and regeneration aimed at circular economy goals. Despite these advances, challenges such as high production costs and scalability remain barriers to the widespread adoption of ILs in the textile sector. Addressing these barriers through continued research and development is essential to fully realize the potential of ILs for sustainable transformation in textiles. Full article
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<p>Ionic liquid generations.</p>
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<p>Common cations and anions that are present in ionic liquids.</p>
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<p>Common properties of ionic liquids.</p>
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<p>Sectors of the textile industry where ionic liquids are used.</p>
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<p>Schematic representation and example of gemini ionic liquids.</p>
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<p>Example of applications of ionic liquids in textile finishing.</p>
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<p>Schematic representation of cotton/PET separation and recovery.</p>
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<p>Schematic representation of the use of ionic liquids in dyed textile and wastewater treatment. In particular, the figure illustrates the dual role of ionic liquids as effective extraction agents for dye removal from wastewater and textiles. Key mechanisms include dye adsorption, solubilization, and ionic exchange. Applications depicted range from the removal of acid dyes and reactive dyes from aqueous solutions to the recovery of colorants and reuse of treated textiles. The process highlights the potential of ILs for sustainable wastewater treatment and recycling in the textile industry.</p>
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<p>Benefits associated with the use of ionic liquids in the textile sector.</p>
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<p>Potential obstacles to the use of ionic liquids in the textile industry.</p>
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19 pages, 4024 KiB  
Article
Spectroscopic and Morphological Examination of Co0.9R0.1MoO4 (R = Ho, Yb, Gd) Obtained by Glycine Nitrate Procedure
by Milena Rosić, Maja Milošević, Maria Čebela, Vladimir Dodevski, Vesna Lojpur, Uroš Čakar and Srecko Stopic
Materials 2025, 18(2), 397; https://doi.org/10.3390/ma18020397 - 16 Jan 2025
Viewed by 234
Abstract
The glycine nitrate procedure (GNP) is a method that proved to be the easiest and most effective method for controlling the composition and morphology during the synthesis of Co0.9R0.1MoO4 (R = Ho, Yb, Gd). This method of the [...] Read more.
The glycine nitrate procedure (GNP) is a method that proved to be the easiest and most effective method for controlling the composition and morphology during the synthesis of Co0.9R0.1MoO4 (R = Ho, Yb, Gd). This method of the combustion process achieves control of stoichiometry, homogeneity, and purity. Metal nitrates and glycine were mixed in the appropriate stoichiometric ratios to produce Co0.9R0.1MoO4 (R = Ho, Yb, Gd). The samples obtained by the mentioned method were further subjected to different characterization methods such as differential thermal analyses (DTA), X-ray diffraction (XRD), Fourier transform infrared spectrum (FTIR), spectroscopy, field emission scanning electron microscopy (FESEM), and nitrogen adsorption method. A high level of anisotropy of the shape and size of particles in the form of agglomerates was found. Also, there are noticeable differences in the microstructure and plate crystals. The color of the synthesized sample changes from darker to lighter shades after thermal treatments. There are pronounced changes in the dominant wavelength (nm) and color purity between the initial sample and the sample after heating (1100 °C) due to the concentration of Co. Full article
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<p>DTA curve for the synthesized powder of Co<sub>0.9</sub>R<sub>0.1</sub>MoO<sub>4</sub> (R = Ho, Yb, Gd): (<b>a</b>,<b>b</b>) Co<sub>0.9</sub>Ho<sub>0.1</sub>MoO<sub>4</sub>; (<b>c</b>,<b>d</b>) Co<sub>0.9</sub>Yb<sub>0.1</sub>MoO<sub>4</sub>; (<b>e</b>) Co<sub>0.9</sub>Gd<sub>0.1</sub>MoO<sub>4</sub>; (<b>b</b>,<b>d</b>) Application Gaussian peak functions from OriginPro 8.5 (green lines).</p>
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<p>XRD pattern of Co<sub>0.9</sub>R<sub>0.1</sub>MoO<sub>4</sub> (R = Ho, Yb, Gd) powder sample after combustion reaction: (<b>a</b>) Co<sub>0.9</sub>Ho<sub>0.1</sub>MoO<sub>4</sub> (<b>b</b>) Co<sub>0.9</sub>Yb<sub>0.1</sub>MoO<sub>4</sub> (<b>c</b>) Co<sub>0.9</sub>Gd<sub>0.1</sub>MoO<sub>4</sub>; * undoped CoMoO<sub>4</sub> [<a href="#B30-materials-18-00397" class="html-bibr">30</a>]; (<b>d</b>) comparison of undoped synthesized CoMoO<sub>4</sub> with doped synthesized Co<sub>0.9</sub>R<sub>0.1</sub>MoO<sub>4</sub> (R = Ho, Yb, Gd) samples; (<b>e</b>) comparison of undoped CoMoO<sub>4</sub> at 450 °C with doped Co<sub>0.9</sub>R<sub>0.1</sub>MoO<sub>4</sub> (R = Ho, Yb, Gd) samples at 450 °C; (<b>f</b>) comparison of undoped CoMoO<sub>4</sub> at 1000 °C with doped Co<sub>0.9</sub>R<sub>0.1</sub>MoO<sub>4</sub> (R = Ho, Yb, Gd) samples at 1100 °C.</p>
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<p>The FTIR spectra of the as-prepared Co<sub>0.9</sub>R<sub>0.1</sub>MoO<sub>4</sub> (R = Ho, Yb, Gd) samples: (<b>a</b>) Co<sub>0.9</sub>Ho<sub>0.1</sub>MoO<sub>4</sub> (<b>b</b>) Co<sub>0.9</sub>Yb<sub>0.1</sub>MoO<sub>4</sub> (<b>c</b>) Co<sub>0.9</sub>Gd<sub>0.1</sub>MoO<sub>4</sub>.</p>
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<p>FE-SEM micrographs of Co<sub>0.9</sub>Ho<sub>0.1</sub>MoO<sub>4</sub> as-prepared sample (<b>a</b>); (<b>b</b>) at 450 °C; (<b>c</b>) at 1100 °C; (<b>d</b>) one representative EDS spectrum of Co<sub>0.9</sub>Ho<sub>0.1</sub>MoO<sub>4</sub>; (<b>e</b>) one representative EDS spectrum of Co<sub>0.9</sub>Gd<sub>0.1</sub>MoO<sub>4</sub>; (<b>f</b>) one representative EDS spectrum of Co<sub>0.9</sub>Yb<sub>0.1</sub>MoO<sub>4</sub>.</p>
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<p>Chromatic diagram of Co<sub>0.9</sub>R<sub>0.1</sub>MoO<sub>4</sub> (R = Ho, Yb, Gd) samples.</p>
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<p>Nitrogen adsorption isotherms, as the amount of N<sub>2</sub> adsorbed as a function of relative pressure for: (<b>a</b>) Co<sub>0.9</sub>Ho<sub>0.1</sub>MoO<sub>4</sub> samples synthesized and at 450 °C; (<b>b</b>) Co<sub>0.9</sub>Yb<sub>0.1</sub>MoO<sub>4</sub> samples synthesized; (<b>c</b>) Co<sub>0.9</sub>Gd<sub>0.1</sub>MoO<sub>4</sub> samples synthesized and at 450 °C.</p>
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39 pages, 7831 KiB  
Article
Integrated Renewable Energy Systems for Buildings: An Assessment of the Environmental and Socio-Economic Sustainability
by Hossam A. Gabbar and A. Ramadan
Sustainability 2025, 17(2), 656; https://doi.org/10.3390/su17020656 - 16 Jan 2025
Viewed by 441
Abstract
Developing a green energy strategy for municipalities requires creating a framework to support the local production, storage, and use of renewable energy and green hydrogen. This framework should cover essential components for small-scale applications, including energy sources, infrastructure, potential uses, policy backing, and [...] Read more.
Developing a green energy strategy for municipalities requires creating a framework to support the local production, storage, and use of renewable energy and green hydrogen. This framework should cover essential components for small-scale applications, including energy sources, infrastructure, potential uses, policy backing, and collaborative partnerships. It is deployed as a small-scale renewable and green hydrogen unit in a municipality or building demands meticulous planning and considering multiple elements. Municipality can promote renewable energy and green hydrogen by adopting policies such as providing financial incentives like property tax reductions, grants, and subsidies for solar, wind, and hydrogen initiatives. They can also streamline approval processes for renewable energy installations, invest in hydrogen refueling stations and community energy projects, and collaborate with provinces and neighboring municipalities to develop hydrogen corridors and large-scale renewable projects. Renewable energy and clean hydrogen have significant potential to enhance sustainability in the transportation, building, and mining sectors by replacing fossil fuels. In Canada, where heating accounts for 80% of building energy use, blending hydrogen with LPG can reduce emissions. This study proposes a comprehensive approach integrating renewable energy and green hydrogen to support small-scale applications. The study examines many scenarios in a building as a case study, focusing on economic and greenhouse gas (GHG) emission impacts. The optimum scenario uses a hybrid renewable energy system to meet two distinct electrical needs, with 53% designated for lighting and 10% for equipment with annual saving CAD$ 87,026.33. The second scenario explores utilizing a hydrogen-LPG blend as fuel for thermal loads, covering 40% and 60% of the total demand, respectively. This approach reduces greenhouse gas emissions from 540 to 324 tCO2/year, resulting in an annual savings of CAD$ 251,406. This innovative approach demonstrates the transformative potential of renewable energy and green hydrogen in enhancing energy efficiency and sustainability across sectors, including transportation, buildings, and mining. Full article
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<p>Five-phase diagram illustrating the progression of energy efficiency and renewable energy integration in buildings [<a href="#B4-sustainability-17-00656" class="html-bibr">4</a>].</p>
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<p>Annual growth for renewable electricity generation by source, 2018–2020 [<a href="#B10-sustainability-17-00656" class="html-bibr">10</a>].</p>
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<p>Hydrogen (H<sub>2</sub>) with its uses for fuel, heat, and feedstock.</p>
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<p>The Block Diagram for The Workflow.</p>
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<p>Algorithm for Electric Power and Heat Energy in Buildings.</p>
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<p>Algorithm of the Building Electric Power and Heat Energy.</p>
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<p>Schematic of the renewable energy and the hydrogen system in TRNSYS software.</p>
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<p>The power Curve for the Wind Turbine with cut-off power.</p>
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<p>Annually hour solar irradiance data for Oshawa City, located within the Durham zone.</p>
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<p>Annual wind speed data for Oshawa City, located within the Durham zone.</p>
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<p>Annually PV Power output data for Oshawa City, located within the Durham zone Sc 4-1 and Sc 4-2.</p>
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<p>Annually Wind Turbines Power output data for Oshawa City, located within the Durham zone Sc 4-1 and Sc 4-2.</p>
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<p>Annually PV Power output data for Oshawa City, located within the Durham zone Sc 4-3 and Sc 4-4.</p>
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<p>Annually Wind Turbines Power output data for Oshawa City, located within the Durham zone Sc 4-3 and Sc 4-4.</p>
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<p>Electric Loads (Light) Summary.</p>
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<p>Electric Loads (Equipment) Summary.</p>
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<p>Cost Saving Analysis Yearly Summary.</p>
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<p>Building Roof Layout with PV and Wind turbines Installed.</p>
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<p>Annually Hydrogen Production.</p>
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<p>Fuel Consumption for Different Scenarios with and Without Propane -H<sub>2</sub> mixture.</p>
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<p>Running Cost and Saving for Different Scenarios.</p>
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<p>GHG Emissions for Different Scenarios.</p>
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<p>The Definition of the Risk Scenarios.</p>
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<p>Fault tree Analysis of hydrogen hazard.</p>
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16 pages, 3454 KiB  
Article
Utilization of Thermal-Activated Coal Gangue to Enhance the Properties of Sandy Soil Composites
by Wangtao Fan, Ruofan Liu, Runxia Zhang, Xiaoguang Chen, Jin Li, Aochen Zhang, Jing Qian, Zhaolin Gu and Jianyun Wang
Appl. Sci. 2025, 15(2), 817; https://doi.org/10.3390/app15020817 - 15 Jan 2025
Viewed by 399
Abstract
To effectively solve the problem of land sanding and improve the water- and element-retaining properties of sandy soil, a thermal-activated coal gangue (TACG) was used as an ameliorating material to prepare a composite soil mixed with sandy soil to enhance the water-retaining and [...] Read more.
To effectively solve the problem of land sanding and improve the water- and element-retaining properties of sandy soil, a thermal-activated coal gangue (TACG) was used as an ameliorating material to prepare a composite soil mixed with sandy soil to enhance the water-retaining and fertilizer-fixing properties of the sandy soil and reduce the evaporation of water in the soil. The structure and thermal stability of the gangue were characterized using Fourier transform infrared spectroscopy and thermogravimetric analysis. By applying different dosages and different calcination temperatures of the TACG, the water-holding capacity of the mixed soil was determined, and changes in pore structure were observed. When the dosage was 15% and the calcination temperature was 600 °C, the mixed soil possessed the most excellent distribution of pore structure and could effectively prevent water evaporation. Meanwhile, the application of the TACG in sandy soil improved its adsorption of K+, which showed the potential application of thermally activated gangue materials in the field of soil improvement. Full article
(This article belongs to the Special Issue Sustainable and Low-Carbon Building Materials in Special Areas)
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<p>TG analytical curves of the original gangue.</p>
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<p>Gangue heating/cooling curves of the calcination process.</p>
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<p>Schematic diagram of soil column.</p>
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<p>XRD patterns of coal gangue after calcination at different temperatures.</p>
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<p>(<b>a</b>) Raw coal gangue effect on soil aggregate composition; (<b>b</b>) 600 °C gangue effect on soil aggregate composition; and (<b>c</b>) 850 °C gangue effect on soil aggregate composition.</p>
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<p>Changes in water uptake of mixed soils with different treatments.</p>
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<p>(<b>a</b>) Changes in water content of mixed soils modified with raw coal gangue. (<b>b</b>) Changes in water content of mixed soil modified with coal gangue calcined at 600 °C. (<b>c</b>) Changes in water content of mixed soil modified with coal gangue calcined at 850 °C.</p>
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<p>Water vapor isothermal adsorption curve (15% coal gangue mixed sandy soil).</p>
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<p>Pore distribution curve of mixed sandy soil.</p>
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<p>(<b>a</b>) Changes in NH<sub>4</sub><sup>+</sup> adsorption/desorption under different treatments. (<b>b</b>) Changes in PO<sub>4</sub><sup>3−</sup> adsorption/desorption under different treatments. (<b>c</b>) Changes in K<sup>+</sup> adsorption/desorption under different treatments.</p>
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34 pages, 15315 KiB  
Review
Recent Advances in the Performance and Mechanisms of High-Entropy Alloys Under Low- and High-Temperature Conditions
by Rui Xi and Yanzhou Li
Coatings 2025, 15(1), 92; https://doi.org/10.3390/coatings15010092 - 15 Jan 2025
Viewed by 320
Abstract
High-entropy alloys, since their development, have demonstrated great potential for applications in extreme temperatures. This article reviews recent progress in their mechanical performance, microstructural evolution, and deformation mechanisms at low and high temperatures. Under low-temperature conditions, the focus is on alloys with face-centered [...] Read more.
High-entropy alloys, since their development, have demonstrated great potential for applications in extreme temperatures. This article reviews recent progress in their mechanical performance, microstructural evolution, and deformation mechanisms at low and high temperatures. Under low-temperature conditions, the focus is on alloys with face-centered cubic, body-centered cubic, and multi-phase structures. Special attention is given to their strength, toughness, strain-hardening capacity, and plastic-toughening mechanisms in cold environments. The key roles of lattice distortion, nanoscale twin formation, and deformation-induced martensitic transformation in enhancing low-temperature performance are highlighted. Dynamic mechanical behavior, microstructural evolution, and deformation characteristics at various strain rates under cold conditions are also summarized. Research progress on transition metal-based and refractory high-entropy alloys is reviewed for high-temperature environments, emphasizing their thermal stability, oxidation resistance, and frictional properties. The discussion reveals the importance of precipitation strengthening and multi-phase microstructure design in improving high-temperature strength and elasticity. Advanced fabrication methods, including additive manufacturing and high-pressure torsion, are examined to optimize microstructures and improve service performance. Finally, this review suggests that future research should focus on understanding low-temperature toughening mechanisms and enhancing high-temperature creep resistance. Further work on cost-effective alloy design, dynamic mechanical behavior exploration, and innovative fabrication methods will be essential. These efforts will help meet engineering demands in extreme environments. Full article
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<p>Overview of the historical evolution and milestones in HEA research.</p>
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<p>Schematic diagram of lattice distortion in HEAs [<a href="#B90-coatings-15-00092" class="html-bibr">90</a>].</p>
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<p>Variations in (<b>a</b>) mechanical strength and (<b>b</b>) fracture strain across temperatures ranging from 113 K to 1273 K and different loading directions [<a href="#B135-coatings-15-00092" class="html-bibr">135</a>].</p>
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<p>Twin interactions in [111]-oriented CoCrFeMnNi HEA crystals subjected to 20% tensile deformation at 77 K are shown as: (<b>a</b>) a bright-field image, (<b>b</b>) a dark-field image, and (<b>c</b>) a diffraction pattern [<a href="#B136-coatings-15-00092" class="html-bibr">136</a>].</p>
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<p>(<b>a</b>) Elemental distributions of Cr, Fe, Ni, Co, and Cu in the FeNiCoCrCu0.5 HEA; (<b>b</b>) Composition variations between the FCC matrix and Cu-rich areas; (<b>c</b>) atom probe tomography reconstruction illustrating Cu distribution, enlarged cluster images, and a one-dimensional composition analysis [<a href="#B140-coatings-15-00092" class="html-bibr">140</a>].</p>
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<p>Fracture surface morphology of CrMnFeCoNi<sub>2</sub>Cu alloy under tensile deformation at various temperatures. (<b>a</b>) 300 K. (<b>b</b>) Partial enlarged view of (<b>a</b>). (<b>c</b>) 77 K. (<b>d</b>) Partial enlarged view of (<b>c</b>). (<b>e</b>) 10 K. (<b>f</b>) Partial enlarged view of (<b>e</b>). (<b>g</b>) 4.2 K. (<b>h</b>) Partial enlarged view of (<b>g</b>) [<a href="#B129-coatings-15-00092" class="html-bibr">129</a>].</p>
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<p>Tensile deformation structures of the alloy at 223 K. (<b>a</b>) Primary deformation twin formation; (<b>b</b>,<b>c</b>) secondary nanoscale twin development; (<b>d</b>) indexed results illustrating twin orientations and strain conditions [<a href="#B137-coatings-15-00092" class="html-bibr">137</a>].</p>
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<p>Fracture surface appearances under various conditions. (<b>a</b>) Entire fracture view at 293 K; (<b>b</b>) detailed fracture morphology at 293 K; (<b>c</b>) side view of the sample at 293 K; (<b>d</b>) entire fracture view at 77 K; (<b>e</b>) detailed fracture morphology at 77 K; (<b>f</b>) side view of the sample at 77 K [<a href="#B144-coatings-15-00092" class="html-bibr">144</a>].</p>
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<p>Surface morphology of the alloy post-machining. (<b>a</b>) Cutting speed (vc) = 2000 mm/min at RT; (<b>b</b>) vc = 2200 mm/min at RT; (<b>c</b>) vc = 2000 mm/min at low temperature; (<b>d</b>) vc = 2200 mm/min at low temperature [<a href="#B125-coatings-15-00092" class="html-bibr">125</a>].</p>
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<p>The microstructure of Fe<sub>28.2</sub>Ni<sub>7</sub>Co<sub>11</sub>Al<sub>2.5</sub>Ta<sub>0.04</sub>B HEA after tensile testing at 77 K. (<b>a</b>) Martensite forms mainly in fine grains at ~7% strain. (<b>b</b>) At ~12% strain, martensite spreads to fine and coarse grains. (<b>c</b>) TEM shows thin-plate martensite in coarse grains. (<b>d</b>) High-resolution TEM shows nanotwins in martensite. (<b>e</b>) TEM shows thin-plate martensite in fine grains. (<b>f</b>) Nanotwins in fine-grain martensite [<a href="#B147-coatings-15-00092" class="html-bibr">147</a>].</p>
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<p>(<b>a</b>) The AlCoCrFeNi2.1 alloy fractured in tension at 77 K, (<b>b</b>) a SAED pattern from the area indicated by a green marker, and (<b>c</b>) an SAED pattern from the region indicated by a red marker. At higher magnifications, dislocation arrangements are clearly visible in both the (<b>d</b>) FCC and (<b>e</b>) B2 domains [<a href="#B127-coatings-15-00092" class="html-bibr">127</a>].</p>
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<p>Stress–strain relationships for the HEA under varying thermal conditions at strain rates of (<b>a</b>) 10<sup>−1</sup> s<sup>−1</sup> and (<b>b</b>) 10<sup>−2</sup> s<sup>−1</sup> [<a href="#B135-coatings-15-00092" class="html-bibr">135</a>].</p>
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<p>(<b>a</b>) The AlCoCrFeNi<sub>2.1</sub> microstructure, (<b>b</b>) compositional mappings, and (<b>c</b>) its stress–strain curve at 973 K [<a href="#B135-coatings-15-00092" class="html-bibr">135</a>].</p>
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<p>(<b>a</b>) Tensile stress–strain curves at various temperatures. (<b>b</b>) YS, UTS, and fracture elongation versus temperature [<a href="#B160-coatings-15-00092" class="html-bibr">160</a>].</p>
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<p>TEM micrographs of the Nb<sub>40</sub>Ti<sub>25</sub>Al<sub>15</sub>V<sub>10</sub>Ta<sub>5</sub>Hf<sub>3</sub>W<sub>2</sub> alloy after 120 h of aging at 923 K (<b>a</b>), 1023 K (<b>b</b>), and 1123 K (<b>c</b>), illustrating APB development and Hf-enriched segregations [<a href="#B164-coatings-15-00092" class="html-bibr">164</a>].</p>
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24 pages, 18984 KiB  
Article
Maximum-Power Stirling-like Heat Engine with a Harmonically Confined Brownian Particle
by Irene Prieto-Rodríguez, Antonio Prados and Carlos A. Plata
Entropy 2025, 27(1), 72; https://doi.org/10.3390/e27010072 - 15 Jan 2025
Viewed by 312
Abstract
Heat engines transform thermal energy into useful work, operating in a cyclic manner. For centuries, they have played a key role in industrial and technological development. Historically, only gases and liquids have been used as working substances, but the technical advances achieved in [...] Read more.
Heat engines transform thermal energy into useful work, operating in a cyclic manner. For centuries, they have played a key role in industrial and technological development. Historically, only gases and liquids have been used as working substances, but the technical advances achieved in recent decades allow for expanding the experimental possibilities and designing engines operating with a single particle. In this case, the system of interest cannot be addressed at a macroscopic level and their study is framed in the field of stochastic thermodynamics. In the present work, we study mesoscopic heat engines built with a Brownian particle submitted to harmonic confinement and immersed in a fluid acting as a thermal bath. We design a Stirling-like heat engine, composed of two isothermal and two isochoric branches, by controlling both the stiffness of the harmonic trap and the temperature of the bath. Specifically, we focus on the irreversible, non-quasi-static case—whose finite duration enables the engine to deliver a non-zero output power. This is a crucial aspect, which enables the optimisation of the thermodynamic cycle by maximising the delivered power—thereby addressing a key goal at the practical level. The optimal driving protocols are obtained by using both variational calculus and optimal control theory tools. Furthermore, we numerically explore the dependence of the maximum output power and the corresponding efficiency on the system parameters. Full article
(This article belongs to the Special Issue Control of Driven Stochastic Systems: From Shortcuts to Optimality)
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<p>Scheme of the stochastic Stirling cycle. The harmonic confining potential at the operating points of the cycle, from (<b>A</b>–<b>D</b>), is represented by the purple curves. The filled red and blue areas correspond to the probability density functions at those state points, where red (blue) refers to the hot (cold) equilibrium temperatures. The representation of the heat engine in the <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>κ</mi> <mo>,</mo> <mi>y</mi> <mo>)</mo> </mrow> </semantics></math> plane corresponds to the quasi-static version of the described cycle.</p>
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<p>Projection onto the <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>κ</mi> <mo>,</mo> <mi>y</mi> <mo>)</mo> </mrow> </semantics></math> plane of the phase trajectory in the Stirling heat engine. The left (right) panel corresponds to the reversible (irreversible) cycle. In both panels, <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mi>χ</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>; for the irreversible case, we consider ideal bounds for the temperature, i.e., <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">min</mo> </msub> <mo>→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">max</mo> </msub> <mo>→</mo> <mo>∞</mo> </mrow> </semantics></math>.</p>
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<p>Density plots of the optimal power (<b>left</b>) and the corresponding efficiency (<b>right</b>) in the <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>ν</mi> <mo>,</mo> <mi>χ</mi> <mo>)</mo> </mrow> </semantics></math> plane. We consider the loosest bounds for the temperature: <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">min</mo> </msub> <mo>→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">max</mo> </msub> <mo>→</mo> <mo>∞</mo> </mrow> </semantics></math>.</p>
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<p>Density plot of the optimal power in the <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>ν</mi> <mo>,</mo> <mi>χ</mi> <mo>)</mo> </mrow> </semantics></math> plane (<b>left</b>) and vertical sections for fixed values of the temperature ratio <math display="inline"><semantics> <mi>ν</mi> </semantics></math> (<b>right</b>). The curve <math display="inline"><semantics> <mrow> <mi>χ</mi> <mo>=</mo> <msup> <mi>χ</mi> <mo>∗</mo> </msup> <mrow> <mo>(</mo> <mi>ν</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> (dotted line) gives the compression ratio yielding optimal power for every temperature ratio. On the right, the upper panel corresponds to <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math> and the bottom one to <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <msup> <mi>ν</mi> <mo>∗</mo> </msup> </mrow> </semantics></math>. The points at which maximum power is reached in each case are also displayed (squares).</p>
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<p>Efficiency at maximum power in our approach (black solid line), Carnot efficiency (red dotted line), Curzon–Ahlborn efficiency (blue dashed line) and <math display="inline"><semantics> <msub> <mi>η</mi> <mo>+</mo> </msub> </semantics></math> (green dash-dotted line), defined in Equation (<a href="#FD70-entropy-27-00072" class="html-disp-formula">70</a>), as a function of the temperature ratio <math display="inline"><semantics> <mi>ν</mi> </semantics></math>.</p>
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<p>Optimal compression ratio <math display="inline"><semantics> <msup> <mi>χ</mi> <mo>∗</mo> </msup> </semantics></math> as a function of the Carnot efficiency <math display="inline"><semantics> <mrow> <msub> <mi>η</mi> <mi>C</mi> </msub> <mo>=</mo> <mn>1</mn> <mo>−</mo> <mi>ν</mi> </mrow> </semantics></math>. We compare numerical results (black circles) with the theoretical expansion in <math display="inline"><semantics> <msub> <mi>η</mi> <mi>C</mi> </msub> </semantics></math> up to cubic order, as given by Equations (<a href="#FD71-entropy-27-00072" class="html-disp-formula">71</a>) and (<a href="#FD72-entropy-27-00072" class="html-disp-formula">72</a>) (blue solid line). The inset shows the difference between the numerical results and the first-order approximation <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>+</mo> <msub> <mi>a</mi> <mn>1</mn> </msub> <msub> <mi>η</mi> <mi>C</mi> </msub> </mrow> </semantics></math>, which is very small, of the order of <math display="inline"><semantics> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>3</mn> </mrow> </msup> </semantics></math>, up to <math display="inline"><semantics> <mrow> <msub> <mi>η</mi> <mi>C</mi> </msub> <mo>≃</mo> <mn>0.4</mn> </mrow> </semantics></math>.</p>
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<p>Optimal power <math display="inline"><semantics> <mover accent="true"> <mi mathvariant="script">P</mi> <mo>˜</mo> </mover> </semantics></math> as a function of the compression ratio <math display="inline"><semantics> <mi>χ</mi> </semantics></math> for fixed temperature ratio <math display="inline"><semantics> <mi>ν</mi> </semantics></math> and different values of the temperature bounds <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">min</mo> </msub> <mo>,</mo> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">max</mo> </msub> <mo>)</mo> </mrow> </semantics></math>. In the four panels, we consider two values of <math display="inline"><semantics> <mi>ν</mi> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math> (<b>top</b>) and <math display="inline"><semantics> <mrow> <mi>ν</mi> <mo>=</mo> <msubsup> <mi>ν</mi> <mi>id</mi> <mo>∗</mo> </msubsup> </mrow> </semantics></math> (<b>bottom</b>) together with <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">max</mo> </msub> <mo>→</mo> <mo>+</mo> <mo>∞</mo> </mrow> </semantics></math> (<b>left</b>) and <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">min</mo> </msub> <mo>→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </semantics></math> (<b>right</b>). In this way, we have the ideal upper (lower) bound of the temperature in the left (right) panels, whereas several different values of the other, non-ideal, temperature bound are considered. The optimal power corresponding to the ideal limit of both bounds is also displayed in all the panels (dotted black line), which is reached when the non-ideal temperature bound approaches its ideal value.</p>
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<p>Density plots of the temperature and compression ratios (<b>top panels</b>) yielding optimal power (<b>bottom-left panel</b>), and the corresponding efficiency (<b>bottom-right panel</b>) in the <math display="inline"><semantics> <mfenced separators="" open="(" close=")"> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">min</mo> </msub> <mo>,</mo> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">max</mo> </msub> </mfenced> </semantics></math> plane. We consider the region defined by intervals <math display="inline"><semantics> <mrow> <mn>0</mn> <mo>&lt;</mo> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">min</mo> </msub> <mo>&lt;</mo> <mn>0.4</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mn>1.15</mn> <mo>&lt;</mo> <msub> <mi>θ</mi> <mo movablelimits="true" form="prefix">max</mo> </msub> <mo>&lt;</mo> <mn>2.50</mn> </mrow> </semantics></math>.</p>
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23 pages, 15619 KiB  
Article
Methodology for Surface Reconstruction and Prediction Based on the Electrical Discharge Machining Removal Mechanism of Cf-UHTC Materials
by Sirui Gong, Yizhou Hu, Leheng Zhang, Zhenlong Wang and Yukui Wang
Materials 2025, 18(2), 371; https://doi.org/10.3390/ma18020371 - 15 Jan 2025
Viewed by 246
Abstract
Cf-UHTC is an ideal aerospace material because of its exceptional properties, but its machinability is facing great challenges. Electrical discharge machining (EDM) offers a potential solution, but its removal mechanism remains unclear, lacking reliable prediction tools to guide the actual production. [...] Read more.
Cf-UHTC is an ideal aerospace material because of its exceptional properties, but its machinability is facing great challenges. Electrical discharge machining (EDM) offers a potential solution, but its removal mechanism remains unclear, lacking reliable prediction tools to guide the actual production. This paper deeply explores the EDM removal mechanism of Cf-ZrB2-SiC through single-pulse experiments, high-speed camera observations, and thermal–fluid coupling simulations, revealing key processes like heat transfer, phase transformation, molten pool dynamics, crater formation, and reinforcing phase effects. And the prediction of single-pulse removal with different parameters is also realized. Based on experimental and simulation results, a random continuous discharge model is developed, which deeply studies the dynamic erosion process, reconstructs EDM surfaces, and accurately predicts surface roughness. Furthermore, the thickness of the recast layer can be predicted based on the equivalent temperature method. Undoubtedly, this model provides an ideal approach for efficient production. Full article
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Figure 1

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<p>The research contents and relations.</p>
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<p>Material and machine tool.</p>
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<p>Crater dimension statistics and SEM images at various pulse widths.</p>
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<p>The correlation between the diameter and depth of craters.</p>
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<p>High-speed camera observation of the EDM process on C<sub>f</sub>-ZrB<sub>2</sub>-SiC.</p>
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<p>Schematic diagram of the removal mechanism.</p>
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<p>Schematic diagram of the model boundary conditions.</p>
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<p>Thermal–fluid coupling simulation for ceramic phase removal.</p>
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<p>Thermal–flow coupling simulation results with C<sub>f</sub> influence.</p>
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<p>The comparison between the simulation results and experimental results.</p>
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<p>Simulation results of the discharge crater with various currents.</p>
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<p>Reconstruction and prediction based on the continuous discharge model.</p>
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<p>Simulation of the continuous discharge process and the as-machined surface.</p>
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<p>Dynamic erosion characteristics of the continuous discharge process.</p>
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<p>Surface reconstruction and roughness prediction.</p>
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<p>Prediction of the recast layer thickness and experimental verification.</p>
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