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Search Results (217)

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Keywords = residual magnetic field

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22 pages, 9528 KiB  
Article
Novel Mesoporous Cetyltrimethylammonium Bromide-Modified Magnetic Nanomaterials for Trace Extraction and Analysis of Bisphenol Endocrine Disruptors in Diverse Liquid Matrices
by Yichao Gong, Yajing Guo, Qizhi Sun and Pengyan Liu
Molecules 2025, 30(3), 628; https://doi.org/10.3390/molecules30030628 - 31 Jan 2025
Viewed by 307
Abstract
In this study, Fe3O4 was used as a magnetic core, combined with the characteristics of mesoporous adsorbents, to prepare a novel magnetic mesoporous composite material named MMC. Cetyltrimethylammonium bromide (CTAB) and tetraethyl orthosilicate (TEOS) were used as functional monomers, and [...] Read more.
In this study, Fe3O4 was used as a magnetic core, combined with the characteristics of mesoporous adsorbents, to prepare a novel magnetic mesoporous composite material named MMC. Cetyltrimethylammonium bromide (CTAB) and tetraethyl orthosilicate (TEOS) were used as functional monomers, and a simple etching method was employed. The resulting MMC was used as an effective adsorbent for the magnetic solid-phase extraction of trace residues of six bisphenol endocrine disruptors (bisphenol A, bisphenol B, bisphenol C, bisphenol F, bisphenol AF, and bisphenol AP) from environmental water and food samples. Characterization results indicated that the surface of MMC exhibited a distinct wormhole-like mesoporous structure, with the successful incorporation of CTAB functional groups and Si-OH. The crystal structure of Fe3O4 remained stable throughout the preparation process. Mapping analysis confirmed the uniform distribution of CTAB functional groups without aggregation and demonstrated high magnetic intensity, enabling rapid separation and collection under an external magnetic field. Extraction and elution conditions were optimized, and tests were conducted for interfering substances such as humic acid, glucose, fructose, and sucrose under optimal parameters. The results showed that recovery rates were not significantly affected. The quality evaluation of the method demonstrated good linearity, a broad linear range, low limits of detection and quantification, and satisfactory recovery rates. Blank and spiked analyses were conducted for seven real samples, including environmental water (rivers and lakes) and food samples (dairy, juice, and carbonated beverages), with satisfactory spiked recovery rates achieved. Thus, the developed analytical method enables the analysis and detection of trace residues of various bisphenol pollutants in complex matrices, such as environmental water and food samples, providing a valuable reference for trace analysis of similar contaminants in complex matrices. Full article
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14 pages, 4236 KiB  
Communication
Catalytic and Tribological Performances of a Novel Bi-Functional Ionic Liquid in Lubricating Ester Oil
by Yanan Wang, Huaigang Su, Jun Yin, Cheng Jiang, Qilong Zhao, Wenjing Lou and Qian Jia
Lubricants 2025, 13(2), 45; https://doi.org/10.3390/lubricants13020045 - 22 Jan 2025
Viewed by 586
Abstract
To address the detrimental effects of the residue of catalysts on the tribological performances of ester lubricants, a novel and efficient bi-functional ionic liquid 1-(3,5-di-tert-butyl-4-hydroxybenzyl)-3-methylimidazole di(2-ethylhexyl) phosphate ([(BHT-1)MIM][DEHP]) was prepared. The catalyst not only facilitates the synthesis of pentaerythritol tetra-hexanoate (PETH) through the [...] Read more.
To address the detrimental effects of the residue of catalysts on the tribological performances of ester lubricants, a novel and efficient bi-functional ionic liquid 1-(3,5-di-tert-butyl-4-hydroxybenzyl)-3-methylimidazole di(2-ethylhexyl) phosphate ([(BHT-1)MIM][DEHP]) was prepared. The catalyst not only facilitates the synthesis of pentaerythritol tetra-hexanoate (PETH) through the catalytic esterification reaction—achieving up to 96% conversion with a 94% yield—but also enhances the tribological performance of ester oil PETH when used as a lubricant additive. The tribological property has been improved remarkably: the mean friction coefficient for PETH + [(BHT-1)MIM][DEHP] is notably lower, at 0.110, compared to the PETH, which has a coefficient of 0.180. Meanwhile, the wear scar diameter of the steel ball, when lubricated with PETH + [(BHT-1)MIM][DEHP], is notably smaller than that of a steel ball lubricated solely with PETH. Especially, the reduction in the wear volume at 100 °C is up to 81.46% compared with the base oil PETH. [(BHT-1)MIM][DEHP], PETH + [(BHT-1)MIM][DEHP], and the worn track of the upper running ball and lower disc were systematically characterized by using Nuclear Magnetic Resonance (NMR) spectra, a Fourier Transform Infrared Spectrometer (FT-IR), a field emission scanning electron microscope (FESEM), Thermal gravity analysis (TG), X-ray photoelectron spectroscopy (XPS), and an optical microscope (OM). The wear mechanism of the tailored lubricant oil was discussed in terms of the chemical composition of the worn surface. Full article
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<p>The scheme for the synthesis of 2,6-di-tert-butyl-4-bromomethylphenol.</p>
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<p>The scheme for the synthesis of 1-(3,5-di-tert-butyl-4-hydroxybenzyl)-3-methyl imidazole bromide.</p>
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<p>The scheme for the synthesis of 1-(3,5-di-tert-butyl-4-hydroxybenzyl)-3-methylimidazole di(2-ethylhexyl) phosphate.</p>
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<p>The catalytic reaction of pentaerythritol with caproic acid.</p>
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<p>The HR-MS of [(BHT-1)MIM][DEHP].</p>
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<p>The TG characterization of ionic liquid [(BHT-1)MIM][DEHP].</p>
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<p>FT–IR spectra of [(BHT-1)MIM][DEHP] and PETH + [(BHT-1)MIM][DEHP].</p>
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<p>Friction coefficient variation over time for PETH and PETH + [(BHT-1)MIM][DEHP]. (The SRV test was conducted with a load of 50 N, frequency of 25 Hz, temperature of 100 °C, and a stroke length of 1 mm).</p>
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<p>Optical images of the wear scars on the upper running ball lubricated with (<b>a</b>) PETH and (<b>b</b>) PETH + [(BHT-1)MIM][DEHP]. (The SRV test was conducted with a load of 50 N, frequency of 25 Hz, temperature of 100 °C, and stroke length of 1 mm).</p>
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<p>FESEM images showing the worn surfaces of steel discs: (<b>a</b>) lubricated with PETH at 80× magnification, (<b>b</b>) lubricated with PETH at 700× magnification, (<b>c</b>) lubricated with PETH + [(BHT-1)MIM][DEHP] at 80× magnification, and (<b>d</b>) lubricated with PETH + [(BHT-1)MIM][DEHP] at 700× magnification. (The SRV test was conducted with a load of 50 N, frequency of 25 Hz, temperature of 100 °C, and a stroke length of 1 mm).</p>
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<p>The XPS spectra (<b>a</b>) the worn surface lubricated by PETH + [(BHT-1)MIM][DEHP], (<b>b</b>) pure [(BHT-1)MIM][DEHP] and (<b>c</b>) pure PETH.</p>
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16 pages, 4414 KiB  
Article
Effect of Alternating Magnetic Field Treatment on the Friction/Wear Resistance of 20Cr2Ni4A Under Lubricated Conditions
by Sufyan Akram, Mose Bevilacqua, Anatolii Babutskyi and Andreas Chrysanthou
Metals 2025, 15(1), 69; https://doi.org/10.3390/met15010069 - 14 Jan 2025
Viewed by 391
Abstract
High-strength nickel–chromium steel (20Cr2Ni4A) is typically used in bearing applications. Alternating magnetic field treatment, which is based on the use of a magnetiser, and which is fast and cost-effective in comparison to conventional processes, was applied to the material to improve its wear [...] Read more.
High-strength nickel–chromium steel (20Cr2Ni4A) is typically used in bearing applications. Alternating magnetic field treatment, which is based on the use of a magnetiser, and which is fast and cost-effective in comparison to conventional processes, was applied to the material to improve its wear resistance. The results of pin-on-disc wear testing using a AISI 52100 alloy counter pin revealed a decrease in the specific wear rate of the treated samples by 58% and a reduction in the value of the coefficient of friction by 28%. X-ray diffraction analysis showed a small increase in the amount of martensite and higher surface compressive residual stresses by 28% leading to improved hardness. The observed changes were not induced thermally. The volume expansion by the formation of martensite was achieved at near room temperature and led to a further increase in compressive residual stresses. The significance of this study is that the improvement in the properties was achieved at a current density value that was two orders of magnitude higher than the threshold for phase transformation and dislocation movement. The reasons for the effect of the alternating magnetic field treatment on the friction and wear properties are discussed in terms of the contribution of the magnetic field to the austenite-to-martensite phase transformation and the interaction between the magnetic domain walls and dislocations. Full article
(This article belongs to the Special Issue Advances in Electromagnetic Processing of Metallic Materials)
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<p>Schematic diagrams of (<b>a</b>) the AMF treatment for the pin-on-disc sample and (<b>b</b>) a plot of the magnetic flux density against time during AMF treatment.</p>
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<p>Diagram of POD 2 pin-on-disc tester: (A) balance weight, (B) load beam, (C) sample, (D) load cell, (E) wear pin (ball) and holder, (F) wear track radius micrometre adjustment, and (G) rotating sample table.</p>
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<p>Schematic representation of the model employed in the simulation: 1, spacer; 2, air; 3, windings (comprising 70 turns); 4, air magnetizer core; and 5, disc sample.</p>
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<p>(<b>a</b>) Variation in the coefficient of friction for untreated and AMF-treated disc specimens of high-strength Ni-Cr steel; (<b>b</b>) specific wear rate and the average coefficient of friction for the untreated and AMF-treated conditions.</p>
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<p>SEM wear tracks of the surface of untreated (<b>a</b>,<b>b</b>) and treated (<b>c</b>,<b>d</b>) high-strength Ni-Cr steel after 1 h of pin-on-disc testing.</p>
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<p>AFM surface topographic micrograph of the worn surface for untreated (<b>a</b>) and treated (<b>b</b>) high-strength Ni-Cr steel.</p>
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<p>Nanoindentation results of (<b>a</b>) hardness and H/E<sup>2</sup> and (<b>b</b>) loading–unloading curves of treated and untreated high-strength Ni-Cr steel.</p>
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<p>X-ray diffraction patterns of untreated (black) and AMF-treated (red) specimens of high-strength Ni-Cr steel.</p>
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<p>Calculation using QuickField 6 software of the eddy current density at the cylindrical surface of the sample.</p>
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12 pages, 2828 KiB  
Article
An Aptamer Sensor Based on Alendronic Acid-Modified Upconversion Nanoparticles Combined with Magnetic Separation for Rapid and Sensitive Detection of Thiamethoxam
by Qian Huang, Lu Han, Hui Ma, Weijie Lan, Kang Tu, Jing Peng, Jing Su and Leiqing Pan
Foods 2025, 14(2), 182; https://doi.org/10.3390/foods14020182 - 9 Jan 2025
Viewed by 512
Abstract
The widespread use of thiamethoxam has led to pesticide residues that have sparked global concerns regarding ecological and human health risks. A pressing requirement exists for a detection method that is both swift and sensitive. Herein, we introduced an innovative fluorescence biosensor constructed [...] Read more.
The widespread use of thiamethoxam has led to pesticide residues that have sparked global concerns regarding ecological and human health risks. A pressing requirement exists for a detection method that is both swift and sensitive. Herein, we introduced an innovative fluorescence biosensor constructed from alendronic acid (ADA)-modified upconversion nanoparticles (UCNPs) linked with magnetic nanoparticles (MNPs) via aptamer recognition for the detection of thiamethoxam. Through base pairing, thiamethoxam-specific aptamer-functionalized MNPs (apt-MNPs) were integrated with complementary DNA-functionalized UCNPs (cDNA-UCNPs) to create the MNPs@UCNPs fluorescence biosensor. Thiamethoxam specifically attached to apt-MNPs, leading to their separation from cDNA-UCNPs, which in turn led to a reduction in fluorescence intensity at 544 nm following separation by an external magnetic field. The change in fluorescence intensity (ΔI) was directly correlated with the concentration of thiamethoxam, enabling the quantitative analysis of the pesticide. With optimized detection parameters, the biosensor was capable of quantifying thiamethoxam within a concentration span of 0.4–102.4 ng·mL−1, and it achieved a detection limit as minute as 0.08 ng·mL−1. Moreover, leveraging the swift magnetic concentration properties of MNPs, the assay duration could be abbreviated to 25 min. The research exhibited a swift and precise sensing platform that yielded promising results in samples of cucumber, cabbage, and apple. Full article
(This article belongs to the Special Issue Development and Application of Biosensors in the Food Field)
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<p>Characterization of UCNPs: (<b>A</b>) TEM image of OA-UCNPs, (<b>B</b>) TEM image of ADA-UCNPs, (<b>C</b>) XRD of UCNPs, and (<b>D</b>) FT-IR spectra of OA-UCNPs and ADA-UCNPs.</p>
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<p>Characterization of MNPs: (<b>A</b>) TEM image of MNPs, (<b>B</b>) XRD of MNPs, (<b>C</b>) FT-IR spectrum of MNPs, and (<b>D</b>) magnetization curve of MNPs.</p>
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<p>Optimization of (<b>A</b>) volume of apt-MNPs, (<b>B</b>) incubation time, and (<b>C</b>) response time.</p>
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<p>(<b>A</b>) Upconversion fluorescence spectrum of thiamethoxam at different concentrations. (<b>B</b>) Standard curve of thiamethoxam. (<b>C</b>) Specificity evaluation of the MNPs@UCNPs fluorescence biosensor for thiamethoxam (a: 2,4-D; b: dinotefuran; c: deltamethrin; d: imidaclothiz; e: acetamiprid; f: imidacloprid; g: thiamethoxam). The error bars represent the standard deviations based on three independent measurements.</p>
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<p>Schematic illustration of the strategy to form the MNPs@UCNPs fluorescence biosensor for thiamethoxam detection.</p>
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14 pages, 4767 KiB  
Article
Experimental Assessment of Magnetic Nanofluid Injection in High-Salinity and Heavy-Crude-Saturated Sandstone: Mitigation of Formation Damage
by Jimena Lizeth Gómez-Delgado, Nelson Gutierrez-Niño, Luis Felipe Carrillo-Moreno, Raúl Andres Martínez-López, Nicolás Santos-Santos and Enrique Mejía-Ospino
Energies 2025, 18(1), 212; https://doi.org/10.3390/en18010212 - 6 Jan 2025
Viewed by 470
Abstract
The depletion of conventional oil reserves has intensified the search for enhanced oil recovery (EOR) techniques. Recently, nanoparticle research has focused on graphene oxide-based materials, revealing a critical challenge in their practical application. Laboratory investigations have consistently demonstrated that these nanoparticles have significant [...] Read more.
The depletion of conventional oil reserves has intensified the search for enhanced oil recovery (EOR) techniques. Recently, nanoparticle research has focused on graphene oxide-based materials, revealing a critical challenge in their practical application. Laboratory investigations have consistently demonstrated that these nanoparticles have significant potential for formation damage, a critical limitation that substantially constrains their potential field implementation. This research addresses a critical challenge in EOR: developing magnetic graphene oxide nanoparticles (MGONs) that can traverse rock formations without causing formation damage. MGONs were synthesized and stabilized in formation brine with a high total dissolved solids (TDS) content with a xanthan gum polymer. Two coreflooding experiments were conducted on sandstone cores. The first experiment on high-permeability sandstone (843 mD) showed no formation damage; instead, permeability increased to 935 mD after MGON injection. Irreducible water saturation (Swirr) and residual oil saturation (Sor) were 25.1% and 31.5%, respectively. The second experiment on lower-permeability rock (231.3 mD) evaluated nanoparticle retention. The results showed that 0.09511 mg of MGONs was adsorbed per gram of rock under dynamic conditions. Iron concentration in effluents stabilized after 3 pore volumes, indicating steady-state adsorption. The successful synthesis, stability in high-TDS brine, favorable interfacial properties, and positive effects observed in coreflooding experiments collectively highlight MGONs’ potential as a viable solution for enhancing oil recovery in challenging reservoirs, without causing formation damage. Full article
(This article belongs to the Special Issue Failure and Multiphysical Fields in Geo-Energy)
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<p>FTIR spectra of graphene oxide (GO) and magnetic graphene oxide (Fe<sub>3</sub>O<sub>4</sub>@GO).</p>
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<p>Micrographs of GO on the <b>left</b> and Fe<sub>3</sub>O<sub>4</sub>@GO on the <b>right</b>.</p>
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<p>Size distribution of magnetic graphene oxide Fe<sub>3</sub>O<sub>4</sub>@GO.</p>
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<p>Compatibility test (formation brine and Fe<sub>3</sub>O<sub>4</sub>@GO magnetic nanofluid).</p>
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<p>Coreflooding Stage 1.</p>
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<p>Iron concentration in effluents.</p>
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23 pages, 7423 KiB  
Article
Crystal Plasticity Finite Element Study on Orientation Evolution and Deformation Inhomogeneity of Island Grain During the Ultra-Thin Strips Rolling of Grain Oriented Electrical Steel
by Huanzhu Wang, Ping Yang, Qingge Xie and Xinfu Gu
Materials 2024, 17(24), 6276; https://doi.org/10.3390/ma17246276 - 22 Dec 2024
Viewed by 560
Abstract
The presence of island grains in the initial finished sheets of grain-oriented electrical steel is inevitable in the preparation of ultra-thin strips. Owing to their distinctive shape and size effects, their deformation behavior during rolling differs from that of grain-oriented electrical steels of [...] Read more.
The presence of island grains in the initial finished sheets of grain-oriented electrical steel is inevitable in the preparation of ultra-thin strips. Owing to their distinctive shape and size effects, their deformation behavior during rolling differs from that of grain-oriented electrical steels of conventional thickness. This study focuses on the orientation evolution and deformation heterogeneity of island grains during rolling. Four types of island grains with orientations of {210}<001>, {110}<112>, {114}<481>, and {100}<021> were selected and modeled within the Goss-oriented matrix using full-field crystal plasticity finite element (CPFEM) simulation under plane strain compression. The results are then compared with corresponding experimental measurements. The results reveal that orientation rotation and grain fragmentation vary among the island grains of different orientations, with the first two orientations exhibiting more significant deformation heterogeneity compared to the latter two. Additionally, the orientations of the island grains significantly affect the distribution of residual Goss orientations within the surrounding matrix. Pancake-like island grains exhibit a higher degree of orientation scatter and greater deformation heterogeneity in the central layer compared to their spherical counterparts. The initial {210}<001> island grains can form a cube orientation, which can be optimized by subsequent process control to enhance magnetic properties. Full article
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<p>IPF-Z maps, ODF section and (001) pole figures of pancake-like {210}&lt;001&gt; island grain embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of the XY section with pancake-like {210}&lt;001&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5, (<b>g</b>,<b>h</b>) z = 0.75, (<b>i</b>,<b>j</b>) z = 1.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of the spherical {210}&lt;001&gt; island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of the XY section with the spherical {210}&lt;001&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5.</p>
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<p>IPF-Z maps of XZ center section of pancake-like and spherical {210}&lt;001&gt; island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>(001) pole figures of the pancake-like and spherical {210}&lt;001&gt;-oriented island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of pancake-like {110}&lt;112&gt;-oriented island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of XY section with {110}&lt;112&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5, (<b>g</b>,<b>h</b>) z = 0.75, (<b>i</b>,<b>j</b>) z = 1.</p>
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<p>IPF-Z maps of the XY center section, ODF section and (001) pole figures of the spherical {110}&lt;112&gt;-oriented island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps of XZ center section of pancake-like and spherical {110}&lt;112&gt; island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>(001) pole figures of pancake-like and spherical {110}&lt;112&gt; island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of {114}&lt;481&gt; island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of XY section with {114}&lt;481&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of {100}&lt;021&gt; island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 70%.</p>
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<p>IPF-Z maps and (001) pole figures of XY section with {100}&lt;021&gt;-oriented island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5.</p>
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<p>Evolution of {210}&lt;001&gt; island grains during cold rolling at 70% and annealing (930 °C, 3 min): (<b>a</b>,<b>d</b>,<b>e</b>) the original EBSD data of the island grain, (<b>b</b>,<b>f</b>,<b>g</b>) EBSD data after cold rolling, (<b>c</b>,<b>h</b>,<b>i</b>) EBSD data after recrystallization. Reproduced with permission from Ping Yang, Materials Chemistry and Physics; published by Elsevier, 2022 Reference [<a href="#B12-materials-17-06276" class="html-bibr">12</a>].</p>
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<p>Evolution of {110}&lt;112&gt; island grains during cold rolling to 70% and annealing (930 °C, 3 min): (<b>a</b>,<b>d</b>,<b>e</b>) the original EBSD data of island grain, (<b>b</b>,<b>f</b>,<b>g</b>) EBSD data after cold rolling, (<b>c</b>,<b>h</b>,<b>i</b>) EBSD data after recrystallization. Reproduced with permission from Ping Yang, Materials Chemistry and Physics; published by Elsevier, 2022 in Reference [<a href="#B12-materials-17-06276" class="html-bibr">12</a>].</p>
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<p>IPF-Z maps and ODF section of samples with lower initial magnetic inductions after annealing at 850 °C for 5 min at different reductions: (<b>a</b>,<b>b</b>) 60%, (<b>c</b>,<b>d</b>) 65%, (<b>e</b>,<b>f</b>) 70%, (<b>g</b>,<b>h</b>) 75%. Reproduced with permission from Ping Yang, Journal of Materials Engineering; published by Journal of Materials Engineering Editorial Department, 2017 [<a href="#B8-materials-17-06276" class="html-bibr">8</a>].</p>
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12 pages, 2135 KiB  
Article
Effects of Long-Term Fertilization on Phosphorus Form and Availability in Black Soil
by Enjia Lu, Cuilan Li, Yidan Geng, Tianfeng Liang and Jinjing Zhang
Appl. Sci. 2024, 14(24), 11673; https://doi.org/10.3390/app142411673 - 13 Dec 2024
Viewed by 789
Abstract
This study explored the effect of the combined application of chemical and organic fertilizers on phosphorus morphology and its conversion to an active state. A long-term field positioning experiment comprising five treatments was conducted in black soil. The results concluded that the soil [...] Read more.
This study explored the effect of the combined application of chemical and organic fertilizers on phosphorus morphology and its conversion to an active state. A long-term field positioning experiment comprising five treatments was conducted in black soil. The results concluded that the soil total phosphorus (TP), available phosphorus (AP), inorganic phosphorus, and organic phosphorus contents of all treatments ranked as follows: 1.5M1NPK > M2NPK > M1NPK > NPK > CK. The long-term application of chemical and organic fertilizers increased the proportion of soil reactive phosphorus and moderately reactive phosphorus but decreased the proportion of mildly active phosphorus and residual phosphorus. A phosphorus-31 nuclear magnetic resonance (31P NMR) spectral analysis showed that the contents of orthophosphate, pyrophosphate, phosphoric acid diesters, and orthophosphate acid monoesters increased with the application of chemical and organic fertilizers, of which 1.5M1NPK usually resulted in the highest increases. In conclusion, the long-term application of chemical fertilizers could promote the conversion of soil phosphorus into active phosphorus and improve the effectiveness of soil phosphorus, and the long-term use of organic and chemical fertilizers was more effective than the use of chemical fertilizers only, with 1.5M1NPK providing the best effects. Full article
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<p>Soil total and available phosphorus content under long-term fertilizer application. Note: Different lowercase letters indicate significant differences among treatments at the <span class="html-italic">p</span> &lt; 0.05 level.</p>
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<p>Phosphorus content in various forms of soil under long-term fertilizer application (mg-kg<sup>−1</sup>). Note: Different lower case letters in the figure indicate significant differences among soil inorganic phosphorus treatments at the <span class="html-italic">p</span> &lt; 0.05 level, and different upper case letters indicate significant differences among soil organic phosphorus treatments at the <span class="html-italic">p</span> &lt; 0.05 level.</p>
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<p>Proportion of distribution of various forms of phosphorus in soil under long-term fertilization (%). Note: Different lowercase letters indicate significant differences among treatments at the <span class="html-italic">p</span> &lt; 0.05 level.</p>
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<p><sup>31</sup>P NMR spectra of soil under long-term fertilization (displacement: δ, ×10<sup>−6</sup>).</p>
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<p>Correlation analysis among soil phosphorus forms under long-term fertilization. Note: * indicates significant correlation at the <span class="html-italic">p</span> &lt; 0.05 level; ** indicates highly significant correlation at the <span class="html-italic">p</span> &lt; 0.01 level. The hue of the ellipse corresponds to the positive or negative correlation, the colour corresponds to the size of the correlation coefficient, the redder the correlation coefficient, the larger the correlation coefficient, and the shape of the ellipse corresponds to the size of the correlation coefficient, by default the more flattened the correlation coefficient is, the larger it is.</p>
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12 pages, 1121 KiB  
Article
Modeling the Bending of a Bi-Layer Cantilever with Shape Memory Controlled by Magnetic Field and Temperature
by Olga S. Stolbova and Oleg V. Stolbov
Modelling 2024, 5(4), 1924-1935; https://doi.org/10.3390/modelling5040100 - 5 Dec 2024
Viewed by 651
Abstract
This paper presents a model of the bending behavior of a bi-layer cantilever composed of titanium nickelide and a magnetoactive elastomer embedded with magnetically hard particles. The cantilever is initially subjected to an external magnetic field in its high-temperature state, followed by cooling [...] Read more.
This paper presents a model of the bending behavior of a bi-layer cantilever composed of titanium nickelide and a magnetoactive elastomer embedded with magnetically hard particles. The cantilever is initially subjected to an external magnetic field in its high-temperature state, followed by cooling to a low-temperature state before the magnetic field is removed. This sequence results in residual bending deformation. Basic relations describing the material behavior of titanium nickelide and the magnetoactive elastomer are presented. A variational formulation for the problem under consideration is written down. The problem is solved numerically using the finite element method. The influence of the applied magnetic field magnitude and the thickness of the titanium nickelide layer on the cantilever deflection magnitude is studied. The dependence of the residual cantilever deflection on the applied magnetic field is obtained. The possibility of this structure as a controllable gripping element for applications in robotics and micro-manipulation is demonstrated. Full article
(This article belongs to the Special Issue Finite Element Simulation and Analysis)
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<p>Cross-section of the bi-layer plate made of titanium nickelide (red area) and MAE (blue area).</p>
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<p>Fragments of the finite element mesh (<b>left</b> and <b>right</b> ends) with thickening in the titanium nickelide region.</p>
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<p>Loading diagram: dependence of magnetic field and temperature on step number <span class="html-italic">k</span>.</p>
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<p>Configurations of the bi-layer plate: 1—initial configuration, 2—after application of the magnetic field, 3—after cooling under a constant magnetic field, and 4—after removal of the magnetic field.</p>
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<p>Stress intensity distribution (<b>a</b>) and phase strain distribution (<b>b</b>) in the left part of the sample.</p>
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<p>Dependence of the displacement of the right end of the cantilever on step number <span class="html-italic">k</span> for different values of the thickness of the titanium nickelide layer.</p>
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<p>Dependence of the plate deflection magnitude on the thickness of the titanium nickelide layer.</p>
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<p>Dependence of the plate deflection magnitude on the applied magnetic field.</p>
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<p>Dependence of the displacement vector norm on the number of mesh nodes.</p>
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<p>Working scheme of the gripper: element position in the absence of a magnetic field (<b>a</b>) and element position in a magnetic field (<b>b</b>).</p>
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10 pages, 1925 KiB  
Article
Efficient Approximation Procedure for Magnetization Characteristics Used in Performance Analysis of Highly Saturated Electrical Machines
by Miralem Hadžiselimović, Tine Marčič and Ivan Zagradišnik
Energies 2024, 17(23), 6073; https://doi.org/10.3390/en17236073 - 2 Dec 2024
Viewed by 511
Abstract
The analytical and especially the numerical calculations of the magnetic fields of highly saturated electrical machines require a correctly given magnetizing curve. In practice, professional software may use many points of the magnetizing curve (sometimes 50 or more points). There is a high [...] Read more.
The analytical and especially the numerical calculations of the magnetic fields of highly saturated electrical machines require a correctly given magnetizing curve. In practice, professional software may use many points of the magnetizing curve (sometimes 50 or more points). There is a high probability that a point will be entered or measured incorrectly. We have therefore set ourselves three objectives. The first is to reduce the number of points given. The second is to ensure that the curve is given analytically (in the form of orthogonal polynomials) and is as smooth as possible. This means that the derivatives of the reluctance are also as smooth as possible. Therefore, the Newton–Raphson iteration procedure in numerical calculations converges rapidly. The third objective was to make the magnetizing curve continue beyond a magnetic field density of 2 T up to about 3 T. Most professional programs simply limit the magnetizing curve to about 2.2 T. This limitation makes it impossible to calculate accurately the magnetic field in the bridges, especially when the slots in the rotor are closed. Local fields can exceed values of 2.2 T. A solution has been found. It uses higher order orthogonal polynomials. It has been shown that 12 given points of the magnetizing curve is enough to give a good approximation of the measured curve. However, one polynomial function is not enough. We need three functions and another exponential function for magnetic field densities above around 2 T up to a value of relative permeability equal to 1. In the numerical calculation of the field, we thus achieve the desired error (residual) vector of the Newton–Raphson iterative procedure in 10 ÷ 15 steps for semi-closed slots and 20 ÷ 30 steps for closed slots. Full article
(This article belongs to the Special Issue Advances in Electrical Machines Design and Control)
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<p>Closed rotor slot of (<b>a</b>) single- and (<b>b</b>) three-phase motors.</p>
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<p>Magnetic flux density around closed rotor slots (<span class="html-italic">B</span><sub>max</sub> = 2.635 T).</p>
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<p>Measured B–H curve.</p>
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<p>Approximated B–H curve and measured data.</p>
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<p>Modeled relative reluctivity.</p>
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<p>Derivative of relative reluctivity.</p>
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<p>Approximated B–H curve–quality M800-50A from [<a href="#B2-energies-17-06073" class="html-bibr">2</a>].</p>
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14 pages, 4008 KiB  
Article
Structural, Magnetic, and Mössbauer Study on Nb and Heat Treatment of Fe-Si-B-P-Cu-Nb Ribbons
by Hyunkyung Lee, Hyunkyung Choi, Young Rang Uhm and Haein Choi-Yim
Metals 2024, 14(12), 1381; https://doi.org/10.3390/met14121381 - 2 Dec 2024
Viewed by 687
Abstract
This study aims to enhance the amorphous formation ability and magnetic properties that are crucial for the production of high-quality nanocrystalline alloys. The structural, thermal, and magnetic characteristics of the alloy ribbons were analyzed through a systematic adjustment of Nb content, and, including [...] Read more.
This study aims to enhance the amorphous formation ability and magnetic properties that are crucial for the production of high-quality nanocrystalline alloys. The structural, thermal, and magnetic characteristics of the alloy ribbons were analyzed through a systematic adjustment of Nb content, and, including Nb, significantly improved the amorphous formation ability and thermal stability of the alloy, which is vital for nanocrystalline production. By varying the Nb content within Fe85-xSi2B8P4Cu1Nbx (x = 0.0, 0.5, 1.0, and 1.5), we explored finer adjustments to achieve homogeneous amorphousness during the melt spinning process. Careful control over the Nb content facilitated the production of amorphous ribbons with consistent homogeneity, which was critical for the subsequent fabrication of nanocrystalline structures through heat treatment. As a result, the amorphous ribbon of Fe85.5Si2B8P4Cu1Nb0.5 showed a low coercivity of 7 A/m. The heat treatment showed a remarkably high saturation magnetic flux density of 1.94 T. Additionally, the grain size (D) decreased as the Nb content increased, with D values ranging from 25.09 nm to 24.29 nm, as calculated by the Scherrer formula. Mössbauer spectroscopy confirmed the formation of nanocrystalline and residual amorphous phases. The hyperfine magnetic field values (Beff) decreased from 25.7 T to 24.7 T in the amorphous samples and reached 33.0 T in the nanocrystalline phases. This study highlights Nb’s positive impact on thermal stability and amorphous formation capacity in Fe-Si-B-P-Cu alloys, culminating in the successful fabrication of nanocrystalline ribbons with superior structural and magnetic properties. Full article
(This article belongs to the Special Issue Metallic Magnetic Materials: Manufacture, Properties and Applications)
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<p>XRD patterns of as-spun Fe<sub>85-<span class="html-italic">x</span></sub>Si<sub>2</sub>B<sub>8</sub>P<sub>4</sub>Cu<sub>1</sub>Nb<span class="html-italic"><sub>x</sub></span> (<span class="html-italic">x</span> = 0.0, 0.5, 1.0, and 1.5) alloy ribbons.</p>
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<p>Hysteresis loops of as-spun Fe<sub>85-<span class="html-italic">x</span></sub>Si<sub>2</sub>B<sub>8</sub>P<sub>4</sub>Cu<sub>1</sub>Nb<span class="html-italic"><sub>x</sub></span> (<span class="html-italic">x</span> = 0.0, 0.5, 1.0, and 1.5) alloy ribbons. Insert shows the saturation magnetization part measured by VSM.</p>
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<p>Enlarged B-H loop near coercivity (H<sub>C</sub>), measured by the DC B-H tracer.</p>
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<p>DSC curves of as-spun Fe<sub>85-<span class="html-italic">x</span></sub>Si<sub>2</sub>B<sub>8</sub>P<sub>4</sub>Cu<sub>1</sub>Nb<span class="html-italic"><sub>x</sub></span> (<span class="html-italic">x</span> = 0.0, 0.5, 1.0, and 1.5) alloy ribbons.</p>
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<p>XRD patterns of the Fe<sub>85-<span class="html-italic">x</span></sub>Si<sub>2</sub>B<sub>8</sub>P<sub>4</sub>Cu<sub>1</sub>Nb<span class="html-italic"><sub>x</sub></span> (<span class="html-italic">x</span> = 0.0, 0.5, 1.0, and 1.5) ribbons annealed at 420 °C and 460 °C for 10 min and the grain size calculated by the Scherrer formula.</p>
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<p>Mösbauer spectroscopy spectra of amorphous and nanocrystalline ribbons of Fe<sub>85-<span class="html-italic">x</span></sub>Si<sub>2</sub>B<sub>8</sub>P<sub>4</sub>Cu<sub>1</sub>Nb<span class="html-italic"><sub>x</sub></span> (<span class="html-italic">x</span> = 0.0, 0.5, 1.0): (<b>a</b>–<b>c</b>) as-spun state; (<b>d</b>–<b>f</b>) annealed at 420 °C or 460 °C.</p>
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<p>Trends of B<sub>S</sub> and H<sub>C</sub> on the annealing temperature of the composition Fe<sub>85-<span class="html-italic">x</span></sub>Si<sub>2</sub>B<sub>8</sub>P<sub>4</sub>Cu<sub>1</sub>Nb<span class="html-italic"><sub>x</sub></span> (<span class="html-italic">x</span> = 0. 0, 0.5, 1.0, 1.5) after annealing at 380 °C to 480 °C for 10 min.</p>
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12 pages, 1933 KiB  
Article
Metallacrown of CeIIICuII5: Synthesis, Structural Characterization and Insights for Nanoparticles
by Jésio D. Tempesta, Fábio Faria Paiva, Leonildo A. Ferreira, Rafaela M. R. da Silva, Luckerman D. G. Botelho, Iara M. L. Rosa, Caio Cesar Candido, Angelo Marcio Gomes, Wallace C. Nunes, Guilherme P. Guedes and Maria Vanda Marinho
Magnetochemistry 2024, 10(12), 96; https://doi.org/10.3390/magnetochemistry10120096 - 30 Nov 2024
Viewed by 849
Abstract
The heterobimetallic 15-MC-5 metallacrown of formula [CeCu5(5mpzHA)5(NO3)(H2O)7]·2NO3·7H2O, designated MC-Ce, was synthesized using 5-methyl-2-pyrazinehydroxamic acid (5mpzHA) as a linker, reacting with CeIII and CuII salts under mild [...] Read more.
The heterobimetallic 15-MC-5 metallacrown of formula [CeCu5(5mpzHA)5(NO3)(H2O)7]·2NO3·7H2O, designated MC-Ce, was synthesized using 5-methyl-2-pyrazinehydroxamic acid (5mpzHA) as a linker, reacting with CeIII and CuII salts under mild conditions. Single-crystal X-ray diffraction analysis reveals a crown-like [Cu5Ce(5mpzHA)5] core, characteristic of a 15-MC-5 system, with five CuII atoms at the rim of the crown and the CeIII ion occupying the dome of the crown, with water molecules, oxygen atoms and one nitrate anion filling the nine-coordination sphere around the CeIII ion, which exhibits a distorted spherical tricapped trigonal prism geometry. The thermogravimetric analysis evidences successive mass losses due to the removal of water molecules and decomposition of the structure after 217 °C, whereas the PXRD analysis of the thermal decomposition residue reveals the presence of copper and copper/cerium oxide particles. These nanocomposite materials were also synthesized using the metallacrown MC-Ce under a hydrothermal method in the presence of multi-walled carbon nanotubes (MWCNTs), affording insights that this metallacrown can act as a source precursor for the synthesis of these mixed cerium/copper oxide nanomaterials. The experimental χMT value in MC-Ce at room temperature is 3.175 cm3 mol−1 K, which is higher than the calculated one for one magnetically isolated CeIII plus five CuII ions, probably due to the antiferromagnetic interactions among CuII ions within the metallacrown hoop plus the thermal depopulation of JZ sublevels of CeIII ground state (5/2), which exhibit a small splitting under the anisotropic ligand field effects. The χMT decreases continuously until it reaches the value of 0.80 cm3 mol−1 K at 10 K, reinforcing the presence of intramolecular antiferromagnetic interactions. Full article
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Graphical abstract

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<p>Thermal decomposition of MC-Ce under N<sub>2</sub>, showing TG (red) and DSC (black) curves.</p>
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<p>PXRD analysis of final product after thermal decomposition of <b>MC-Ce</b>.</p>
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<p>PXRD pattern in the presence of MWCNTs at 190 °C for 24 h using <b>MC-Ce</b> as a single route for nanoparticles.</p>
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<p>The asymmetric unit of MC-Ce with selected atom labeling. Hydrogen atoms and uncoordinated water molecules, and part of the disorder on the coordinated nitrate ion to Cu3, were omitted for clarity. Color codes: carbon (grey), copper (cyan), oxygen (red), nitrogen (blue), and cerium (yellow).</p>
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<p>Supramolecular dimers are formed by hydrogen bonds involving coordinated water molecules and nitrate oxygen atom (<b>top</b>), and intermolecular interactions between crystallization water molecules, water ligands, and pyrazine nitrogen atom (<b>bottom</b>).</p>
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<p>Temperature dependence of the <span class="html-italic">χ<sub>M</sub></span>T product of <b>MC-Ce</b> was measured by applying the 1 kOe dc field. The solid line is the best fit (see the main text for details). Inset: a magnified view in the temperature range of 2–50 K.</p>
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<p>Isothermal M vs. H plot for complex <b>MC-Ce</b> measured at 2, 4, and 8~K. Inset: reduced magnetization plot (M vs. H/T) measured at 2, 4, and 8 K.</p>
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12 pages, 2324 KiB  
Article
Fast Degaussing Procedure for a Magnetically Shielded Room
by Peter A. Koss, Jens Voigt, Ronja Rasser and Allard Schnabel
Materials 2024, 17(23), 5877; https://doi.org/10.3390/ma17235877 - 30 Nov 2024
Viewed by 3369
Abstract
A demagnetization study was conducted on a magnetically shielded room (MSR) at Fraunhofer IPM, designed for applications such as magnetoencephalography (MEG) and material testing. With a composite of two layers of mu-metal and an intermediate aluminum layer, the MSR must provide a residual [...] Read more.
A demagnetization study was conducted on a magnetically shielded room (MSR) at Fraunhofer IPM, designed for applications such as magnetoencephalography (MEG) and material testing. With a composite of two layers of mu-metal and an intermediate aluminum layer, the MSR must provide a residual field under 5 nT for the successful operation of optically pumped magnetometers (OPMs). The degaussing process, employing six individual coils, reached the necessary residual magnetic field within the central 1 m3 volume in under four minutes. Due to the low-frequency shielding factor of 100, the obtained average residual field is shown to be limited by environmental residual field changes after degaussing and not by the degaussing procedure. Full article
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<p>Schematic illustration of the experiment’s layout established to degauss the MSR. The identically colored coils on the edges are interconnected in a series so that the magnetic field induces a complete magnetic loop inside the shielding material around the inner volume, as indicated by the blue arrows for the blue coils.</p>
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<p>Images of the experimental setup elements: On the left: a picture of the mapping framework using an aluminum rail to adjust the xy-position of the pole, allowing the fluxgate to be positioned at different z-positions. On the right: a photo of the four-quadrant amplifier (black) that drives the degaussing current through the degaussing coil and the 7 Hz transformer (large white box) to eliminate DC offsets.</p>
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<p>Measured shielding factor (SF) curves for the three axes of the two-layer MSR with a 1µT effective excitation field strength. In the inset: dependence of the SF at 0.02 Hz on the amplitude of the excitation field.</p>
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<p>Illustration of the measured 3D field distributions for the three different degaussing configurations: <b>posI</b>, <b>negI</b>, and <b>posZ</b> (top row). Below, the difference between the respective 3D maps is shown. All maps use the same color code. <a href="#materials-17-05877-t001" class="html-table">Table 1</a>a provides characteristic values for these 3D field illustrations. Note that the scaling of the height of the cones relative to the absolute field value reveals minor differences in the maximum amplitude, attributed to a much larger base surface. The difference between <b>negI</b> and <b>posZ</b> is minimal because both fields have a similar direction, whereas <b>posI</b> and <b>negI</b> exhibit slightly different directions.</p>
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<p>Average field map (<b>ave</b>) and the differences between it and the maps <b>posI</b>, <b>negI</b>, and <b>posZ</b>. All maps share the same color code. <a href="#materials-17-05877-t001" class="html-table">Table 1</a>b provides characteristic values for these 3D field maps.</p>
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<p>Illustration of the corrections performed to the measured data (red) based on a simultaneous field measurement with an outside reference fluxgate (green) and the repeated measurement of the magnetic field at the center of the MSR at 7 different times. Blue is the difference between the red and the green curve. The yellow line is the calculated linear fit curve to the blue curve. The black dots are the 7 values of the magnetic field at the MSR center after all corrections are applied.</p>
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18 pages, 5428 KiB  
Article
C/Ni/N Nanocomposites Based on Hydrolysis Lignin: Synthesis, Study of Structural and Magnetic Properties
by Ihor Bordun, Dariusz Calus, Ewelina Szymczykiewicz, Myroslav Malovanyy, Nazar Nahurskyi, Anatoliy Borysiuk and Yuriy Kulyk
Nanomaterials 2024, 14(23), 1886; https://doi.org/10.3390/nano14231886 - 23 Nov 2024
Viewed by 1076
Abstract
A two-step method for the synthesis of C/Ni/N nanocomposites based on hydrolysis lignin from wood chemical processing waste is proposed. These nanocomposites were found to have a well-developed porous structure with a wide pore size distribution. It was shown that doping hydrolysis lignin [...] Read more.
A two-step method for the synthesis of C/Ni/N nanocomposites based on hydrolysis lignin from wood chemical processing waste is proposed. These nanocomposites were found to have a well-developed porous structure with a wide pore size distribution. It was shown that doping hydrolysis lignin with urea-derived nitrogen leads to the appearance of ferromagnetic behavior in the carbon material. When nickel chloride was added during pyrolysis, the magnetic behavior of the C/Ni/N composite was provided by superparamagnetic Ni particles less than 30 nm in size and the magnetism of the carbon matrix. The addition of urea during the synthesis of the nanocomposite further promotes better integration of nickel into the carbon structure. According to the results of magnetic studies, the nickel content in the C/Ni/N nanocomposite was 19 wt.% compared to 15 wt.% in the C/Ni nanocomposite. The synthesized nanocomposite was demonstrated to have no residual magnetization, so its particles do not agglomerate after the external magnetic field is removed. Due to this property and the well-developed porous structure, C/Ni/N composites have the potential to be used as catalysts, active electrode materials for autonomous energy sources, and in environmental technologies as magnetically sensitive adsorbents. Full article
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<p>General scheme for the synthesis of nanocomposites C/Ni/N.</p>
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<p>SEM images and EDX-mapping of the chemical element distribution of C/Ni/N (<b>a</b>), C/Ni (<b>b</b>) and C/N (<b>c</b>) samples.</p>
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<p>SEM images and EDX-mapping of the chemical element distribution of C/Ni/N (<b>a</b>), C/Ni (<b>b</b>) and C/N (<b>c</b>) samples.</p>
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<p>X-ray diffraction patterns of the synthesized nanocomposites C/Ni/N (<b>a</b>), C/Ni (<b>b</b>), and C/N (<b>c</b>).</p>
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<p>SAXS spectra of synthesized nanocomposites C/Ni/N (<b>a</b>), C/Ni (<b>b</b>) and C/N (<b>c</b>) (points—experimental data, solid line—smoothed curve).</p>
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<p>SAXS curves plotted in Porod coordinates <span class="html-italic">s</span><sup>4</sup><span class="html-italic">·I(s) = f(s</span><sup>4</sup><span class="html-italic">)</span> for C/Ni (<b>a</b>) and C/N (<b>b</b>) samples.</p>
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<p>Volume distribution functions of effective pore diameters for C/Ni/N (<b>a</b>), C/Ni (<b>b</b>) and C/N (<b>c</b>) samples.</p>
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<p>Nitrogen adsorption/desorption isotherms for the C/Ni/N (<b>a</b>), C/Ni (<b>b</b>) and C/N (<b>c</b>) samples.</p>
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<p>Pore size distribution for C/Ni/N (<b>a</b>), C/Ni (<b>b</b>) and C/N (<b>c</b>) samples calculated by the BJH method.</p>
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<p>Distribution of pores by size for C/Ni/N (<b>a</b>), C/Ni (<b>b</b>), and C/N (<b>c</b>) samples calculated by the MP method.</p>
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<p>Remagnetization curve of C/Ni/N nanocomposite. The inset shows a larger scale graph.</p>
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<p>Magnetic moment hysteresis curve of the C/Ni nanocomposite. The inset shows a larger scale graph.</p>
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<p>Temperature dependence of the saturation specific magnetization for C/Ni/N (<b>a</b>), C/Ni (<b>b</b>) and C/N (<b>c</b>) samples.</p>
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<p>Temperature dependences of the saturation specific magnetization: 1 of C/Ni/N composite, 2, 3—model temperature dependences for Ni nanoparticles and nitrogen-containing carbon C/N, respectively.</p>
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17 pages, 11736 KiB  
Article
3D Printing of New Foods Using Cellulose-Based Gels Obtained from Cerotonia siliqua L. Byproducts
by Antoni Capellà, Mónica Umaña, Esperanza Dalmau, Juan A. Cárcel and Antoni Femenia
Gels 2024, 10(12), 759; https://doi.org/10.3390/gels10120759 - 23 Nov 2024
Viewed by 675
Abstract
Carob pulp is a valuable source of cellulose-rich fraction (CRF) for many food applications. This study aimed to obtain and characterize a CRF derived from carob pulp waste after sugar removal and to evaluate its potential use in the 3D printing of cellulose-rich [...] Read more.
Carob pulp is a valuable source of cellulose-rich fraction (CRF) for many food applications. This study aimed to obtain and characterize a CRF derived from carob pulp waste after sugar removal and to evaluate its potential use in the 3D printing of cellulose-rich foods. Thus, the extraction of the CRF present in carob pulp (by obtaining the alcohol-insoluble residue) was carried out, accounting for nearly 45% dm (dry matter) of this byproduct. The CRF contained about 24% dm of cellulose. The functional properties (swelling capacity, water retention, and fat adsorption) related to this fraction were determined, showing a value of 5.9 mL/g of CRF and 4.0 and 6.5 g/g of CRF, respectively. Different gels were formulated with a total solids content of 15% wm (wet matter), using potato peel flour as a base and partially substituting with CRF (0% to 8% wm). The cellulose-based gels were characterized in terms of viscosity, water distribution (low-field Nuclear Magnetic Resonance), and printability, while the 3D printed samples were assessed for their textural properties. As the percentage of added CRF increased, the viscosity decreased while the water retention increased. Printability improved when small proportions of CRF (2% to 4%) were used, while it deteriorated for higher percentages (6% to 8%). The textural properties (hardness, adhesiveness, cohesiveness, and gumminess) showed significant changes caused by the addition of CRF, with gels containing 3% to 4% CRF exhibiting the most suitable printing values. In summary, this study demonstrates the significant potential of carob cellulose-based gel as an ingredient in the 3D printing of novel fiber-rich foods, contributing to reducing food waste and promoting sustainable practices within the framework of the circular economy. Full article
(This article belongs to the Special Issue Cellulose-Based Gels: Synthesis, Properties, and Applications)
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<p>Apparent viscosity of the cellulose-based gels formulated with 0%, 2%, 3%, 4%, 6%, and 8% CRF. Different lowercase letters indicate significant differences (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Distributions of the relaxation time after inverse Laplace transform analysis of the LF-NMR spectra of the cellulose-based gels formulated with 0%, 2%, 3%, 4%, 6%, and 8% CRF.</p>
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<p>Textural properties: hardness (<b>a</b>), adhesiveness (<b>b</b>), cohesiveness (<b>c</b>), and gumminess (<b>d</b>) of the printed gels (shape-stable) formulated with 0%, 2%, 3%, 4%, 6%, and 8% CRF. Different lowercase letters indicate significant differences (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Percentages of porosity for the printed samples across the different formulations. Different lowercase letters indicate significant differences (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Photograph of the carob pulp and seeds of the <span class="html-italic">Bugadera</span> variety.</p>
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20 pages, 11752 KiB  
Article
Characteristics of Supercritical CO2 Non-Mixed Phase Replacement in Intraformational Inhomogeneous Low-Permeability Reservoirs
by Mingxi Liu, Kaoping Song, Longxin Wang, Hong Fu and Tianhao Wang
Energies 2024, 17(22), 5608; https://doi.org/10.3390/en17225608 - 9 Nov 2024
Viewed by 640
Abstract
Under the influence of the sedimentation process, the phenomenon of intraformational non-homogeneity is widely observed in low-permeability reservoirs. In the development process of water and gas replacement (WAG), the transport law of water and gas and the distribution of residual oil are seriously [...] Read more.
Under the influence of the sedimentation process, the phenomenon of intraformational non-homogeneity is widely observed in low-permeability reservoirs. In the development process of water and gas replacement (WAG), the transport law of water and gas and the distribution of residual oil are seriously affected by the non-homogeneity of reservoir properties. In this paper, a study on two types of reservoirs with certain lengths and thicknesses is carried out, and a reasonable development method is proposed according to the characteristics of each reservoir. Firstly, through indoor physical simulation experiments combined with low-field nuclear magnetic resonance scanning (NMR), this study investigates the influence of injection rate and core length on the double-layer low-permeability inhomogeneous core replacement and pore throat mobilization characteristics. Then, a two-layer inhomogeneous low-permeability microscopic model is designed to investigate the model’s replacement and pore throat mobilization characteristics under the combined influence of rhythmites, gravity, the injection rate, etc. Finally, based on the results of the core replacement and numerical simulation, a more reasonable development method is proposed for each type of reservoir. The results show that for inhomogeneous cores of a certain length, the WAG process can significantly increase the injection pressure and effectively seal the high-permeability layer through the Jamin effect to improve the degree of recovery. Moreover, for positive and reverse rhythm reservoirs of a certain thickness, the injection rate can be reduced according to the physical properties of the reservoir, and the gravity overburden phenomenon of the gas is used to achieve the effective development of the upper layers. The effect of the development of a positive rhythm reservoir therefore improved significantly. These findings provide data support for improving the development effectiveness of CO2 in low-permeability inhomogeneous reservoirs and emphasize the importance of the influence of multiple factors, such as injection flow rate, gravity, and rhythm, in CO2 replacement. Full article
(This article belongs to the Section H: Geo-Energy)
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<p>Core cross-section physical diagram.</p>
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<p>Flowchart of CO<sub>2</sub> and water displacement experiments.</p>
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<p>Original image and cropped results of low-permeability inhomogeneous model.</p>
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<p>Diagram of different injection modes and injection speeds.</p>
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<p>Comparison of recovery degree and resistance factor at two injection flow rates (the experimental temperature is 150 °C, and the experimental minimum pressure is 40 MPa).</p>
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<p>Comparison of recovery degree and resistance factors of WAG in inhomogeneous cores of different lengths.</p>
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<p>Comparison of T<sub>2</sub> maps after displacement at different injection rates.</p>
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<p>Comparison diagram of post-displacement pore throat utilization at different injection rates.</p>
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<p>Comparison of the final displacement results of low-in/low-out and low-in/high-out with the reverse rhythm model (where ‘injection’ is the injection end and ‘extraction’ is the production end; ‘180 s/180 μm’ is the injection time/volume; ‘reverse/low-in/low-out 1 μm/s’ is the model and injection method; the blue part of the picture is CO<sub>2</sub>; the red part is crude oil; and the colored part is the oil–gas transition zone).</p>
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<p>Comparison of the final displacement results of low-in/high-out and high-in/high out with the positive rhythm model.</p>
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<p>Comparison of the final displacement results of same-in/same-out with the positive and reverse rhythm model.</p>
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<p>When 180 μm is injected, the final displacement state diagram of the positive rhythm and reverse rhythm same-in/same-out models can be obtained (The difference in oil and gas distribution in yellow borders in the figure reflects the effect of gravity.).</p>
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<p>Comparison of overall and low-permeability layers with positive and reverse rhythm models at different injection rates.</p>
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<p>Low-permeability layer and overall recovery degree of each injection method in reverse rhythm (“1” refers to the ”reverse low-speed groups”, “2” refers to the ”reverse high-speed groups”. the red box represents the grouping situation).</p>
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<p>Reverse-rhythm low-speed group gas flow pattern diagram (“1” refers to the ”reverse low-speed groups”).</p>
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<p>Reverse-rhythm high-speed group gas flow pattern diagram ( “2” refers to the ”reverse high-speed groups”).</p>
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<p>Low-permeability layer and overall recovery degree of each injection method in positive rhythm (“1” refers to the ”category 1”, “2” refers to the ”category 2” “3” refers to the ”category 3” “4” refers to the ”category 4”, the red box represents the grouping situation).</p>
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<p>Category 1 gas flow pattern diagram (The green arrow in the figure represents the direction of CO2 flow).</p>
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<p>Category 3 gas flow pattern diagram.</p>
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<p>Category 2 and Category 4 gas flow pattern diagrams.</p>
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