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Search Results (2,972)

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18 pages, 5908 KiB  
Article
Microemulsion-Based Synthesis of Highly Efficient Ag-Doped Fibrous SiO2-TiO2 Photoanodes for Photoelectrochemical Water Splitting
by Samia Arain, Muhammad Usman, Faiq Saeed, Shouzhong Feng, Waheed Rehman, Xianhua Liu and Haitao Dai
Catalysts 2025, 15(1), 66; https://doi.org/10.3390/catal15010066 (registering DOI) - 13 Jan 2025
Viewed by 98
Abstract
Fibrous SiO2-TiO2 (FST) is one of the most promising materials for advancing photoelectrochemical water-splitting technology due to its cost-effectiveness and environmental friendliness. However, FST faces intrinsic limitations, including its low conductivity and wide bandgap. In this study, significant progress was [...] Read more.
Fibrous SiO2-TiO2 (FST) is one of the most promising materials for advancing photoelectrochemical water-splitting technology due to its cost-effectiveness and environmental friendliness. However, FST faces intrinsic limitations, including its low conductivity and wide bandgap. In this study, significant progress was made in modifying FST to overcome some of these limitations. This work involved synthesizing a new photoanode made of Ag-doped FST utilizing the microemulsion process. The Ag-doped FST was characterized using XRD, FTIR, UV–Vis, DRS, N2 adsorption–desorption, FESEM, TEM, and XPS. The results confirmed the formation of a continuous concentric lamellar structure with a large surface area. The addition of Ag species into the FST matrix caused interactions that reduced the bandgap. The Ag-doped FST photoanode exhibited an impressive photocurrent density of 13.98 mA/cm2 at 1.2 V (vs. RHE). This photocurrent density was notably higher than that of FST photoanodes, which was 11.65 mA/cm2 at 1.2 V (vs. RHE). Furthermore, the conduction band of Ag-doped FST is positioned closer to the reduction potential of hydrogen compared to that of FST, SiO2, and TiO2, facilitating rapid charge transfer and enabling the spontaneous generation of H2. The fabrication of Ag-doped FST provides valuable insights into the development of high-performance photoanodes for PEC water splitting. Full article
(This article belongs to the Special Issue Catalytic Properties of Hybrid Catalysts)
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Graphical abstract

Graphical abstract
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<p>XRD patterns of Ag-doped FST and those of the standard JCPDS cards (FST, SiO<sub>2</sub>, and TiO<sub>2</sub>).</p>
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<p>Adsorption–desorption isotherms of Ag-doped FST.</p>
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<p>FTIR spectra of TiO<sub>2</sub>, SiO<sub>2</sub>, FST, and Ag-doped FST.</p>
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<p>XPS spectra of Ag-doped FST: (<b>a</b>) Ti 2p, (<b>b</b>) Si 2p, (<b>c</b>) O 1s, (<b>d</b>) Ag 3d.</p>
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<p>FESEM images of (<b>a</b>) Ag-doped FST and (<b>b</b>) FST at 500 nm; TEM image of (<b>c</b>) Ag-doped FST at 100 nm and (<b>d</b>) Ag-doped FST at 50 nm; (<b>e</b>,<b>f</b>) HR-TEM of Ag-doped FST and FST; (<b>g</b>) SAED pattern of Ag-doped FST; (<b>h</b>) STEM; (<b>i</b>) Combined mapping and (<b>j</b>–<b>m</b>) elemental mapping of Si, O, Ti, and Ag.</p>
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<p>UV–visible spectra of Ag-doped FST, FST, SiO<sub>2</sub>, and TiO<sub>2</sub> photoanodes.</p>
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<p>(<b>a</b>) Tauc plot and (<b>b</b>) Mott–Schottky plot analysis of TiO<sub>2</sub>, SiO<sub>2</sub>, FST, and Ag-doped FST.</p>
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<p>(<b>a</b>) LSV curve, (<b>b</b>) CV curve, and (<b>c</b>) photocurrent density curves of Ag-doped FST at different applied potentials.</p>
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<p>EIS Nyquist plot of Ag-doped FST, FST, SiO<sub>2</sub>, and TiO<sub>2</sub> photoanodes.</p>
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<p>(<b>a</b>) Long-term stability of Ag-doped FST, FST, SiO<sub>2</sub>, and TiO<sub>2</sub> photoanode; (<b>b</b>) XRD spectrum of Ag-doped FST before and after use.</p>
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<p>Schematic illustration of a plausible mechanism of FST and Ag-doped FST.</p>
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<p>Schematic diagram of fabrication of FST and Ag-doped FST.</p>
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15 pages, 3138 KiB  
Article
Large-Area Clay Composite Membranes with Enhanced Permeability for Efficient Dye/Salt Separation
by Yixuan Fu, Shuai Wang, Huiquan Liu, Ke Zhang, Lunxiang Zhang, Yongchen Song and Zheng Ling
Membranes 2025, 15(1), 25; https://doi.org/10.3390/membranes15010025 - 13 Jan 2025
Viewed by 107
Abstract
The escalating discharge of textile wastewater with plenty of dye and salt has resulted in serious environmental risks. Membranes assembled from two-dimensional (2D) nanomaterials with many tunable interlayer spacings are promising materials for dye/salt separation. However, the narrow layer spacing and tortuous interlayer [...] Read more.
The escalating discharge of textile wastewater with plenty of dye and salt has resulted in serious environmental risks. Membranes assembled from two-dimensional (2D) nanomaterials with many tunable interlayer spacings are promising materials for dye/salt separation. However, the narrow layer spacing and tortuous interlayer transport channels of 2D-material-based membranes limit the processing capacity and the permeability of small salt ions for efficient dye/salt separation. In this work, a novel sepiolite/vermiculite membrane was fabricated using Meyer rod-coating and naturally occurring clay. The intercalation of sepiolite Nanofibers between vermiculite Nanosheets provides additional transport nanochannels and forms looser permeable networks, producing composite membranes with remarkably enhanced flux. As a result, the optimized membranes with 80% sepiolite exhibit remarkable flux as high as 78.12 LMH bar−1, outstanding dye rejection (Congo Red~98.26%), and excellent selectivity of dye/salt of 10.41. In addition, this novel all-clay composite membrane demonstrates stable separation performance under acidity, alkalinity and prolonged operation conditions. The large-scale sepiolite/vermiculite membranes made by the simple proposed method using low-cost materials provide new strategies for efficient and environmentally-friendly dye/salt separation. Full article
(This article belongs to the Section Membrane Applications for Water Treatment)
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Figure 1
<p>SEM images of (<b>a</b>) VNSs and (<b>b</b>) SNFs. (<b>c</b>) Viscosity of dispersion of different mass ratios of SNFs. (<b>d</b>) Digital image of large-area SVM-80 (size: 20 cm × 30 cm; load: 0.15 mg cm<sup>−2</sup>). (<b>e</b>) A diagram illustrating the fabrication processes of the SVM−<span class="html-italic">x</span>s.</p>
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<p>(<b>a</b>–<b>d</b>) Top-view SEM images of SVM−20, SVM−40, SVM−60, and SVM−80. (<b>e</b>–<b>h</b>) Cross-section SEM images of SVM−20, SVM−40, SVM−60, and SVM−80.</p>
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<p>(<b>a</b>) The XRD patterns, (<b>b</b>) water contact angles, (<b>c</b>) FT-IR spectra, and (<b>d</b>) pH and composition-dependent zeta potential of the SVM−<span class="html-italic">x</span>s.</p>
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<p>Rejection and flux of the SVM−<span class="html-italic">x</span>s: Rejection varied with the (<b>a</b>) type of feed solution, (<b>b</b>) different dye (MB) content, and (<b>c</b>) different salt (NaCl) content. Flux varied with the (<b>d</b>) type of feed solution, (<b>e</b>) different dye (MB) content, and (<b>f</b>) different salt (NaCl) content.</p>
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<p>The filtration performance of dye/salt mixtures using the SVM−<span class="html-italic">x</span>s (all dye contents are 10 mg L<sup>−1</sup>, all NaCl contents are 1 g L<sup>−1</sup>). (<b>a</b>,<b>b</b>) NaCl concentration-dependent dye and salt rejections. (<b>c</b>) Flux of dye/salt mixtures of the SVM−<span class="html-italic">x</span>s. (<b>d</b>) The UV-vis spectra of the MB/NaCl solutions before and after treatment using the SVM−<span class="html-italic">x</span>s.</p>
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<p>The influence of pH on dye/salt separation. The pH-dependent (<b>a</b>) rejection and (<b>b</b>) flux data of SVM−80, used for the separation.</p>
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<p>(<b>a</b>) The long-term stability and dye/salt separation of SVM−80. The simulated wastewater used in testing contained 1 g L<sup>−1</sup> NaCl and 10 mg L<sup>−1</sup> MB. The insets show the outstanding stability of SVM-80 after long-term separation. (<b>b</b>) The UV−vis spectra of MB/NaCl solutions before and after long−term filtration using SVM-80. The inset shows a digital image of the scalable MB removal using SVM-80 and a positive−pressure filter. (<b>c</b>) The XRD patterns of the recovered salts after filtration and evaporative crystallization. (<b>d</b>) A diagram illustrating the dye/salt separation processes of the SVM−<span class="html-italic">x</span>s.</p>
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50 pages, 5137 KiB  
Review
Combustion Behaviour of ADN-Based Green Solid Propellant with Metal Additives: A Comprehensive Review and Discussion
by Rushikesh Kore and Ashish Vashishtha
Aerospace 2025, 12(1), 46; https://doi.org/10.3390/aerospace12010046 - 12 Jan 2025
Viewed by 330
Abstract
Solid propellants play a crucial role in various civil, scientific, and defence-related aerospace propulsion applications due to their efficient energy release, high energy density, low fabrication cost, and ease of operation. Ammonium dinitramide (ADN) has gained considerable attention as a potential oxidizer for [...] Read more.
Solid propellants play a crucial role in various civil, scientific, and defence-related aerospace propulsion applications due to their efficient energy release, high energy density, low fabrication cost, and ease of operation. Ammonium dinitramide (ADN) has gained considerable attention as a potential oxidizer for green solid propellants due to its high oxygen content, significant energy density, non-toxicity, and non-polluting combustion products, leading to lower environmental impact. As ADN is a new desirable oxidizer in the field of solid propellants, understanding the practicality and viability of the use of ADN in composite solid propellants necessitates a thorough understanding of its chemical and thermal decomposition pathways in addition to its combustion characteristics in the presence of other ingredients. ADN is being explored as an alternative to the traditionally used ammonium perchlorate (AP), a toxic oxidizer containing chlorine (Cl). Additionally, AP monopropellants often suffer from moderate burning rates and poor mechanical strength. To address these limitations, researchers have explored the incorporation of metal additives, such as aluminium (Al), magnesium (Mg), and metalloid boron (B), to enhance the combustion performance and burn rate of AP. These metals not only act as energy-rich additives but also influence the combustion process through various mechanisms. The incorporation of metal additives into ADN has shown promising enhancements in the overall energetic performance of green solid propellants. This review aims to provide an in-depth analysis of the thermal decomposition of ADN and its combustion behaviour, along with the combustion of ADN-based solid propellants with metal additives. Finally, based on an extensive review of the existing literature, various research pathways for focused future collaborative efforts are identified to further advance ADN-based “green” solid propellants. Full article
(This article belongs to the Section Astronautics & Space Science)
18 pages, 9211 KiB  
Article
Cu0-Functionalized, ZIF-8-Derived, Nitrogen-Doped Carbon Composites for Efficient Iodine Elimination in Solution
by Jiuyu Chen, Chensheng Gao, Jingwen Chen, Fei Liu and Zhiwen Liu
Nanomaterials 2025, 15(2), 105; https://doi.org/10.3390/nano15020105 - 12 Jan 2025
Viewed by 228
Abstract
The development of copper-based materials with a high efficiency and low cost is desirable for use in iodine (I2) remediation. Herein, Cu0-nanoparticles-functionalized, ZIF-8 (Zeolite Imidazole Framework-8)-derived, nitrogen-doped carbon composites (Cu@Zn-NC) were synthesized by ball milling and pyrolysis processes. The [...] Read more.
The development of copper-based materials with a high efficiency and low cost is desirable for use in iodine (I2) remediation. Herein, Cu0-nanoparticles-functionalized, ZIF-8 (Zeolite Imidazole Framework-8)-derived, nitrogen-doped carbon composites (Cu@Zn-NC) were synthesized by ball milling and pyrolysis processes. The as-prepared composites were characterized using SEM, BET, XRD, XPS, and FT-IR analyses. The results showed that the morphology of ZIF-8 changed from a leaf-like structure into an irregular structure after the introduction of a copper salt and carbonization. The copper in the pyrolysis samples was mainly in the form of Cu0 particles. The presence of an appropriate amount of Cu0 particles could increase the specific surface area of Cu@Zn-NC. The subsequent batch adsorption results demonstrated that the as-fabricated composites showed high I2 adsorption amounts (1204.9 mg/g) and relatively fast dynamics in an iodine–cyclohexane solution when the Cu content was 30% and the pyrolysis temperature was 600 °C, outperforming the other Cu-based materials. The isothermal adsorption followed both Langmuir and Dubinin–Radushkevich isotherm models, while the kinetics of I2 adsorption followed a pseudo-second-order kinetic model. The activation energy (Eα) of the adsorbent was determined to be 47.2 kJ/mol, according to the Arrhenius equation. According to the experimental and DFT analyses, I2-Zn interactions and I2-Cu0 chemisorption jointly promoted the elimination of iodine. In general, this study provided an operative adsorbent for the highly effective capture of iodine in solution, which might be worth applying on a large scale. Full article
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Figure 1
<p>Schematic illustration of the synthesis procedure of xCu@Zn-NC samples.</p>
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<p>(<b>a</b>–<b>c</b>) SEM images of ZIF-8 (<b>a</b>), 20%Cu@ZIF-8 (<b>b</b>), and 30%Cu@ZIF-8 (<b>c</b>); (<b>d</b>–<b>i</b>) SEM images of Zn-NC (<b>d</b>,<b>g</b>), 20%Cu@Zn-NC (<b>e</b>,<b>h</b>), and 30%Cu@Zn-NC (<b>f</b>,<b>i</b>) in different magnifications.</p>
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<p>N<sub>2</sub> adsorption–desorption isotherms (<b>a</b>) and pore size distributions (<b>b</b>) of xCu@Zn-NC samples. (Gray area: the zoom position in the diagram).</p>
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<p>XRD patterns of xCu@ZIF-8 (<b>a</b>) and xCu@Zn-NC (<b>b</b>).</p>
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<p>XPS patterns of Zn-NC and 30%Cu@Zn-NC. (<b>a</b>) Survey spectra; (<b>b</b>) Zn 2p spectra; (<b>c</b>) C 1s spectra; (<b>d</b>) N 1s spectra; (<b>e</b>) O 1s spectra; (<b>f</b>) Cu 2p spectra.</p>
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<p>FT-IR spectra of xCu@Zn-NC samples.</p>
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<p>(<b>a</b>) The effect of Cu content and pyrolysis temperature on the I<sub>2</sub> adsorption capacity; (<b>b</b>) adsorption isotherms of various samples for I<sub>2</sub>.</p>
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<p>(<b>a</b>) Kinetic adsorption of I<sub>2</sub> by xCu@Zn-NC samples, (<b>b</b>) UV–vis absorption spectra of I<sub>2</sub> solution (900 mg/L) in different contact time.</p>
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<p>The effect of temperature on the I<sub>2</sub> adsorption capacity of 30%Cu@Zn-NC sample. (Inset: Plot of ln <span class="html-italic">K<sub>ads</sub></span> versus 1/<span class="html-italic">T</span>).</p>
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<p>Reusability performance of 30%Cu@Zn-NC sample toward I<sub>2</sub>.</p>
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<p>(<b>a</b>) XRD patterns of I<sub>2</sub>-NC and I<sub>2</sub>-x%Cu@Zn-NC. (<b>b</b>–<b>f</b>) XPS patterns of I<sub>2</sub>-Zn-NC and I<sub>2</sub>-30%Cu@Zn-NC. (<b>b</b>) C 1s spectra, (<b>c</b>) O 1s spectra, (<b>d</b>) Zn 2p spectra, (<b>e</b>) Cu 2p spectra, (<b>f</b>) I 3d spectra.</p>
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<p>Configuration and charge density difference of I<sub>2</sub> adsorption on different models of Cu@Zn-NC.</p>
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19 pages, 6100 KiB  
Article
Research on the Performance of a Liquid–Solid Triboelectric Nanogenerator Prototype Based on Multiphase Liquid
by Wei Wang, Jin Yan, Xianzhang Wang, Hongchen Pang, Chengqi Sun, Yin Sun, Lijun Wang and Dapeng Zhang
Micromachines 2025, 16(1), 78; https://doi.org/10.3390/mi16010078 (registering DOI) - 11 Jan 2025
Viewed by 517
Abstract
In recent years, liquid–solid triboelectric nanogenerators (L-S TENGs) have been rapidly developed in the field of liquid energy harvesting and self-powered sensing. This is due to a number of advantages inherent in the technology, including the low cost of fabricated materials, structural diversity, [...] Read more.
In recent years, liquid–solid triboelectric nanogenerators (L-S TENGs) have been rapidly developed in the field of liquid energy harvesting and self-powered sensing. This is due to a number of advantages inherent in the technology, including the low cost of fabricated materials, structural diversity, high charge-energy conversion efficiency, environmental friendliness, and a wide range of applications. As liquid phase dielectric materials typically used in L-S TENG, a variety of organic and inorganic single-phase liquids, including distilled water, acidic solutions, sodium chloride solutions, acetone, dimethyl sulfoxide, and acetonitrile, as well as paraffinic oils, have been used in experiments. However, it is noteworthy that the function of multiphase liquids as dielectric materials is still understudied. The “Multiphase Liquid Triboelectric Nanogenerator Prototype (ML-TENG Pro)” presented in this paper takes a single-electrode solid–liquid triboelectric nanogenerator as the basic model and uses lubricating oil and deionized water as dielectric materials. After verifying the stability of single-phase liquid materials (e.g., DI water, seawater, ethanol, etc.) for power generation, the power generation performances of oil–water two-phase, gas–oil–water three-phase (with a small number of bubbles), and gas–oil–water three-phase (with many bubbles) in open space are further investigated. COMSOL Multiphysics 6.0 software was used to investigate the material transport mechanism and formation of oil–water two-phase and gas–oil–water three-phase. Finally, this study presents the power generation performance of ML-TENG Pro in the extreme state of gas–oil–water three-phase “emulsification”. This paper outlines the limitations of the ML-TENG, named PRO, and suggests avenues for future improvement. The research presented in this paper provides a theoretical basis for evaluating the quality of lubricants for mechanical power equipment. Full article
(This article belongs to the Special Issue Emerging Applications of Triboelectric Effects/Materials)
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Figure 1
<p>The working mechanism of L-S TENG. (<b>a</b>) An illustration of the EDL (electrical double-layer model [<a href="#B32-micromachines-16-00078" class="html-bibr">32</a>]; (<b>b</b>) “Wang transition” model [<a href="#B33-micromachines-16-00078" class="html-bibr">33</a>].</p>
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<p>The ML-TENG Pro and its different dielectric materials.</p>
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<p>The materials, fabrication, and experimental process of ML-TENGPro. (<b>a</b>) gives the manufacturing process for the ML-TENG Pro. (<b>b</b>) describes tests of ML-TENG Pro’s power generation performance in various types of liquids.</p>
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<p>The power generation using a single-phase liquid triboelectric material. (<b>a</b>,<b>b</b>) Illustrate the generation of electricity by DI water in low-frequency tribological processes; (<b>c</b>,<b>d</b>) depict the same phenomenon in DI water of high-frequency tribological processes. (<b>e</b>,<b>f</b>) Depict the generation of electricity by lubricant oil in the low-frequency tribological processes. (<b>g</b>,<b>h</b>) Depict the lubricant oil in the high-frequency tribological processes. (<b>i</b>,<b>j</b>) Illustrate the generation of electricity by sea water in low-frequency tribological processes; (<b>k</b>,<b>l</b>) depict the same phenomenon in sea water of high-frequency tribological processes. (<b>m</b>,<b>n</b>) Illustrate the generation of electricity by 75% ethanol in low-frequency tribological processes; (<b>o</b>,<b>p</b>) depict the same phenomenon in 75% ethanol of high-frequency tribological processes.</p>
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<p>The power generation using a single-phase liquid triboelectric material. (<b>a</b>,<b>b</b>) Illustrate the generation of electricity by DI water in low-frequency tribological processes; (<b>c</b>,<b>d</b>) depict the same phenomenon in DI water of high-frequency tribological processes. (<b>e</b>,<b>f</b>) Depict the generation of electricity by lubricant oil in the low-frequency tribological processes. (<b>g</b>,<b>h</b>) Depict the lubricant oil in the high-frequency tribological processes. (<b>i</b>,<b>j</b>) Illustrate the generation of electricity by sea water in low-frequency tribological processes; (<b>k</b>,<b>l</b>) depict the same phenomenon in sea water of high-frequency tribological processes. (<b>m</b>,<b>n</b>) Illustrate the generation of electricity by 75% ethanol in low-frequency tribological processes; (<b>o</b>,<b>p</b>) depict the same phenomenon in 75% ethanol of high-frequency tribological processes.</p>
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<p>The simulation of the rising process of a drop of pure oil carried into DI water by ML-TENGPro. (<b>a</b>) Is a real shot of the oil drop, (<b>b</b>) is the process of the oil drop rising through the 2D numerical simulation, and (<b>c</b>) is the process of the oil drop rising through the 3D numerical simulation.</p>
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<p>Bubbles carry the water phase across the oil–water interface or remain at the interface. (<b>a</b>) Is a 2D schematic diagram. (<b>b</b>) Is a 3D schematic diagram.</p>
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<p>The ML-TENG Pro-induced transverse wave. (<b>a</b>) Is the top-down angle, and (<b>b</b>) is the transparent side view angle.</p>
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<p>The power generation of ML-TENG Pro effect from the obvious oil–water interface to the fuzzy semi-emulsified interface. The image (<b>j</b>) is a genuine photograph of the three stages; (<b>a</b>–<b>c</b>) represent the voltage diagram; (<b>d</b>–<b>f</b>) are current graphs; (<b>g</b>–<b>i</b>) are the Vpp and nApp comparison charts for the three phases.</p>
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<p>Experiment on the power generation performance of fully emulsified liquid. (<b>a</b>) describes how ML-TENG Pro enters the emulsion. voltage and current diagram (<b>b</b>,<b>c</b>). The figure (<b>e</b>,<b>f</b>) demonstrate the rationale behind the constrained power generation capacity of ML-TENG Pro in a fully emulsified liquid. (<b>d</b>) photograph of emulsion used in experiment.</p>
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10 pages, 3918 KiB  
Article
Design and Fabrication of Ultrathin Metallic Phase Shifters for Visible and Near-Infrared Wavelengths
by Qing Guo, Jinkui Chu, Chuanlong Guan, Chuxiao Zhang and Ran Zhang
Micromachines 2025, 16(1), 74; https://doi.org/10.3390/mi16010074 - 10 Jan 2025
Viewed by 348
Abstract
The polarization state of light is critical for biological imaging, acousto-optics, bio-navigation, and many other optical applications. Phase shifters are extensively researched for their applications in optics. The size of optical elements with phase delay that are made from natural birefringent materials is [...] Read more.
The polarization state of light is critical for biological imaging, acousto-optics, bio-navigation, and many other optical applications. Phase shifters are extensively researched for their applications in optics. The size of optical elements with phase delay that are made from natural birefringent materials is limited; however, fabricating waveplates from dielectric metamaterials is very complex and expensive. Here, we present an ultrathin (14 nm) metallic phase shifter developed using nanoimprinting technology and the oxygen plasma ashing technique for visible and near-infrared wavelengths. The fabrication process can produce desirable metallic phase shifters with high efficiency, large area, and low cost. We demonstrate through a numerical simulation and experiment that the metallic phase shifter exhibits phase delay performance. Our results highlight the simplicity of the fabrication process for a metallic phase shifter with phase delay performance and offer important opportunities for creating high-efficiency, ultrathin polarizing elements, which can be used in miniaturized devices, such as integrated circuits. Full article
(This article belongs to the Special Issue Nanostructured Optoelectronic and Nanophotonic Devices)
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Figure 1
<p>Structural schematics of double-layer and single-layer aluminum nanowire gratings.</p>
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<p>Transmittance and phase of double-layer and single-layer aluminum nanowire gratings.</p>
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<p>Effect of thickness, width, and period on transmittance and phase. (<b>a</b>) Effect of thickness on transmittance of <span class="html-italic">x</span>-polarized light. (<b>b</b>) Effect of thickness on transmittance of <span class="html-italic">y</span>-polarized light. (<b>c</b>) Effect of thickness on phase. (<b>d</b>) Effect of width on transmittance of <span class="html-italic">x</span>-polarized light. (<b>e</b>) Effect of width on transmittance of <span class="html-italic">y</span>-polarized light. (<b>f</b>) Effect of width on phase. (<b>g</b>) Effect of period on transmittance of <span class="html-italic">x</span>-polarized light. (<b>h</b>) Effect of period on transmittance of <span class="html-italic">y</span>-polarized light. (<b>i</b>) Effect of period on phase.</p>
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<p>Near-field distribution. (<b>a</b>) Incident polarization is along the length of the nanowire gratings. (<b>b</b>) Incident polarization is along the width of the nanowire gratings. The wavelength used in the simulation is 427 nm.</p>
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<p>Schematic diagram of fabrication process: (<b>a</b>) preparation of flexible IPS by NIL; (<b>b</b>) transfer patterns of IPS to UV-curable resist layer using UV-NIL; (<b>c</b>) aluminum thermal evaporation process; (<b>d</b>) oxygen plasma ashing process; (<b>e</b>) desirable ultrathin metallic phase shifter.</p>
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<p>Manufacturing process of ultrathin metallic phase shifter: (<b>a</b>) SEM surface view of flexible IPS; (<b>b</b>) SEM cross-sectional image and (<b>c</b>) SEM surface view of feature patterns of UV-curable resist layer; (<b>d</b>) SEM cross-sectional image of double-layer aluminum nanowire gratings; (<b>e</b>) AFM surface view and (<b>f</b>) AFM cross-sectional image of double-layer aluminum nanowire gratings; (<b>g</b>) SEM cross-sectional image and (<b>h</b>) SEM surface view of ultrathin metallic phase shifter.</p>
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<p>Test results of transmittance and phase of ultrathin metallic phase shifter: test system schemes of (<b>a</b>) transmittance and (<b>b</b>) phase; (<b>c</b>) test results of transmittance and phase difference.</p>
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18 pages, 11743 KiB  
Article
The Design and Validation of an Open-Palm Data Glove for Precision Finger and Wrist Tracking
by Olivia Hosie, Mats Isaksson, John McCormick, Oren Tirosh and Chrys Hensman
Sensors 2025, 25(2), 367; https://doi.org/10.3390/s25020367 - 9 Jan 2025
Viewed by 354
Abstract
Wearable motion capture gloves enable the precise analysis of hand and finger movements for a variety of uses, including robotic surgery, rehabilitation, and most commonly, virtual augmentation. However, many motion capture gloves restrict natural hand movement with a closed-palm design, including fabric over [...] Read more.
Wearable motion capture gloves enable the precise analysis of hand and finger movements for a variety of uses, including robotic surgery, rehabilitation, and most commonly, virtual augmentation. However, many motion capture gloves restrict natural hand movement with a closed-palm design, including fabric over the palm and fingers. In order to alleviate slippage, improve comfort, reduce sizing issues, and eliminate movement restrictions, this paper presents a new low-cost data glove with an innovative open-palm and finger-free design. The new design improves usability and overall functionality by addressing the limitations of traditional closed-palm designs. It is especially beneficial in capturing movements in fields such as physical therapy and robotic surgery. The new glove incorporates resistive flex sensors (RFSs) at each finger and an inertial measurement unit (IMU) at the wrist joint to measure wrist flexion, extension, ulnar and radial deviation, and rotation. Initially the sensors were tested individually for drift, synchronisation delays, and linearity. The results show a drift of 6.60°/h in the IMU and no drift in the RFSs. There was a 0.06 s delay in the data captured by the IMU compared to the RFSs. The glove’s performance was tested with a collaborate robot testing setup. In static conditions, it was found that the IMU had a worst case error across three trials of 7.01° and a mean absolute error (MAE) averaged over three trials of 4.85°, while RFSs had a worst case error of 3.77° and a MAE of 1.25° averaged over all five RFSs used. There was no clear correlation between measurement error and speed. Overall, the new glove design proved to accurately measure joint angles. Full article
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<p>Images of the glove.</p>
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<p>Block diagram of the system electronics.</p>
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<p>Robotic testing setup.</p>
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<p>Hand in testing setup showing the glove placement. The red line shows the alignment of the fourth robot axis with the wrist joint.</p>
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<p>Start and end angles of linear mapping of RFSs.</p>
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<p>Calibration positions of hand.</p>
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<p>Mapping of the resistance (k<math display="inline"><semantics> <mo>Ω</mo> </semantics></math>) to the angle of deflection (°). Each curve represents a different RFS used in the glove: dotted for thumb, solid for index, dashed for middle, dash-dotted for ring, and solid with stars for little finger. The graph shows the calibration of resistance to deflection angles, essential for accurate motion tracking.</p>
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<p>Comparison of measured wrist angle and real wrist angle as measured by IMU. The data points (o) represent the average value at each angle, with standard deviations across each trial shown by error bars. The dotted trendline shows the linearity of the relationship between measured and real angles. The close alignment of the data points with the trendline suggests minimal deviation, reinforcing the reliability of the IMU for wrist angle measurements.</p>
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<p>The comparison of the measured finger angle and real finger angle as measured by RFS. Data points (o) represent the average value at each angle, with standard deviations across each trial shown by error bars. The coloured dotted trendline shows the linearity of the relationship between measured and real angles for all the fingers: blue for index, yellow for middle, green for ring, and red for little finger.</p>
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<p>The comparison of measured thumb angle and real thumb angle as measured by RFS. Data points (o) represent the average value at each angle, with standard deviations across each trial shown by error bars. The dotted trendline shows the linearity of the relationship between measured and real angles.</p>
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<p>Progression of IMU angles (°) over a 6 s period, showing the change in angle as a function of time. The plot highlights the sensor’s responsiveness and consistency during continuous motion. Non-continuous motion at the start and end of the trial is included in this graph to demonstrate why it is excluded from further calculations.</p>
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42 pages, 3563 KiB  
Review
A Review of Sulfate Removal from Water Using Polymeric Membranes
by Jamal Al Mehrate, Sadek Shaban and Amr Henni
Membranes 2025, 15(1), 17; https://doi.org/10.3390/membranes15010017 - 9 Jan 2025
Viewed by 217
Abstract
Access to clean and reliable water has become a critical concern due to the global water crisis. High sulfate levels in drinking water raise health concerns for humans and animals and can cause serious corrosion in industrial systems. Sulfated waters represent a major [...] Read more.
Access to clean and reliable water has become a critical concern due to the global water crisis. High sulfate levels in drinking water raise health concerns for humans and animals and can cause serious corrosion in industrial systems. Sulfated waters represent a major challenge on the Canadian prairies, leading to many cattle deaths. While reverse osmosis (RO) membranes effectively remove sulfates, they are costly due to high-pressure requirements. Nanofiltration (NF) membranes present a more affordable alternative, outperforming traditional methods like adsorption, desalination, and ion exchange. Developing low-pressure ultrafiltration (UF) and microfiltration (MF) membranes could also reduce costs. This review explores advancements in polymeric materials and membrane technology to enhance sulfate removal, focusing on methods used to reduce fouling and improve permeate flux. Techniques discussed include phase inversion (PI), thin-film composite (TFC), and thin-film nanocomposite (TFN) membranes. The review also highlights recent fabrication methods for pristine and nanomaterial-enhanced membranes, acknowledging both benefits and limitations. Continued innovations in polymer-based membranes are expected to drive further performance and cost-efficiency improvements. This review found that studies in the literature dealt mainly with sulfate concentrations below 2000 mg/L, indicating a need to address higher concentrations in future studies. Full article
(This article belongs to the Special Issue Membrane Separation and Water Treatment: Modeling and Application)
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<p>Number of publications per year, from 2011 to 2024, for treating sulfated waters using polymeric membranes; based on Web of Science research using these main keywords: sulfate removal, polymer membrane, and water.</p>
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<p>The general process for the fabrication and modification of polymeric membranes (adapted from [<a href="#B101-membranes-15-00017" class="html-bibr">101</a>]).</p>
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<p>Four membrane module types (adapted from [<a href="#B108-membranes-15-00017" class="html-bibr">108</a>]).</p>
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<p>Description of how membranes work (Green bubbles: oil, Blue bubbles: water) (adapted from [<a href="#B110-membranes-15-00017" class="html-bibr">110</a>]).</p>
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<p>Filtration process in different membranes.</p>
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<p>Different types of phase-inversion processes (adapted from [<a href="#B149-membranes-15-00017" class="html-bibr">149</a>]).</p>
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<p>Description of the dip-coating process (adapted from [<a href="#B56-membranes-15-00017" class="html-bibr">56</a>]).</p>
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<p>Description of the spin-coating process: (<b>a</b>) applying a polymer solution to a substrate; (<b>b</b>) spinning (adapted from [<a href="#B56-membranes-15-00017" class="html-bibr">56</a>]).</p>
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<p>Concept of surface modifications: (<b>A</b>) TFC membrane; (<b>B</b>) TFN membrane (adapted from [<a href="#B165-membranes-15-00017" class="html-bibr">165</a>]).</p>
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<p>Process of ion-exchange treatment (adapted from [<a href="#B195-membranes-15-00017" class="html-bibr">195</a>]).</p>
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<p>Hollow fiber membrane contactor (adapted from [<a href="#B198-membranes-15-00017" class="html-bibr">198</a>]).</p>
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<p>Process of ZLD system (adapted from [<a href="#B204-membranes-15-00017" class="html-bibr">204</a>]).</p>
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<p>Diagram of the process of ED (adapted from [<a href="#B223-membranes-15-00017" class="html-bibr">223</a>]).</p>
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34 pages, 12218 KiB  
Review
Significance of the Powder Metallurgy Approach and Its Processing Parameters on the Mechanical Behavior of Magnesium-Based Materials
by Sachin Kumar Sharma, Sandra Gajević, Lokesh Kumar Sharma, Dhanesh G. Mohan, Yogesh Sharma, Mladen Radojković and Blaža Stojanović
Nanomaterials 2025, 15(2), 92; https://doi.org/10.3390/nano15020092 - 9 Jan 2025
Viewed by 379
Abstract
Magnesium-based materials, which are known for their light weight and exceptional strength-to-weight ratio, hold immense promise in the biomedical, automotive, aerospace, and military sectors. However, their inherent limitations, including low wear resistance and poor mechanical properties, have driven the development of magnesium-based metal [...] Read more.
Magnesium-based materials, which are known for their light weight and exceptional strength-to-weight ratio, hold immense promise in the biomedical, automotive, aerospace, and military sectors. However, their inherent limitations, including low wear resistance and poor mechanical properties, have driven the development of magnesium-based metal matrix composites (Mg-MMCs). The pivotal role of powder metallurgy (PM) in fabricating Mg-MMCs was explored, enhancing their mechanical and corrosion resistance characteristics. The mechanical characteristics depend upon the fabrication methodology, composition, processing technique, and reinforcement added to the magnesium. PM is identified as the most efficient due to its ability to produce near-net shape composites with high precision, cost-effectiveness, and minimal waste. Furthermore, PM enables precise control over critical processing parameters, such as compaction pressure, sintering temperature, and particle size, which directly influence the composite’s microstructure and properties. This study highlights various reinforcements, mainly carbon nanotubes (CNTs), graphene nanoparticles (GNPs), silicon carbide (SiC), and hydroxyapatite (HAp), and their effects on improving wear, corrosion resistance, and mechanical strength. Among these, CNTs emerge as a standout reinforcement due to their ability to enhance multiple properties when used at optimal weight fractions. Further, this study delves into the interaction between reinforcement types and matrix materials, emphasizing the importance of uniform dispersion in preventing porosity and improving durability. Optimal PM conditions, such as a compaction pressure of 450 MPa, sintering temperatures between 550 and 600 °C, and sintering times of 2 h, are recommended for achieving superior mechanical performance. Emerging trends in reinforcement materials, including nanostructures and bioactive particles, are also discussed, underscoring their potential to widen the application spectrum of Mg-MMCs. Full article
(This article belongs to the Section Nanofabrication and Nanomanufacturing)
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<p>Comparative study of powder metallurgy with other processes [<a href="#B30-nanomaterials-15-00092" class="html-bibr">30</a>].</p>
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<p>Primary processing parameters and secondary operations of powder metallurgy.</p>
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<p>SEM image of Mg-based alloy formed at different compaction pressures: (<b>a</b>) 100 MPa, (<b>b</b>) 200 MPa, (<b>c</b>) 300 MPa, (<b>d</b>) 400 MPa, and (<b>e</b>) 500 MPa. (<b>f</b>) Variation in density of composite with compaction pressure [<a href="#B67-nanomaterials-15-00092" class="html-bibr">67</a>].</p>
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<p>SEM micrograph of the composite (<b>a</b>) Mg-1wt.%Al-1wt.%Sn-0.18wt.%GNP, (<b>b</b>–<b>f</b>) X-ray mapping of Mg-1wt.%Al-1wt.%Sn-0.18wt.%GNP, and (<b>g</b>,<b>h</b>) fracture image of Mg-1wt.%Al-1wt.%Sn-0.18wt.%GNP [<a href="#B82-nanomaterials-15-00092" class="html-bibr">82</a>].</p>
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<p>TEM image relating the grain distribution for (<b>a</b>,<b>b</b>) 5 wt.%, (<b>c</b>,<b>d</b>) 7.5 wt.%, and (<b>e</b>,<b>f</b>) 10 wt.% of vanadium. (<b>g</b>–<b>l</b>) SEM image and EDS mapping for 5 wt.% of vanadium in the AZ31 alloy, revealing the uniform dispersion of the reinforcing agent, along with the other elements, such as Al, Mn, and Zn [<a href="#B83-nanomaterials-15-00092" class="html-bibr">83</a>].</p>
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<p>(<b>A</b>) FESEM image and EDS mapping for (<b>a</b>) 2 wt.% of Al<sub>2</sub>O<sub>3</sub> and (<b>b</b>) 8 wt.% Al<sub>2</sub>O<sub>3</sub> of Mg composites. (<b>B</b>) XRD analysis of the composite depicting (X = 0 wt.%, I = 2 wt.%, II = 4 wt.%, III = 6 wt.%, IV = 8 wt.%). (<b>C</b>(<b>a</b>–<b>c</b>)) shows the EDS analysis of the samples after immersion, showcasing the different elemental components in the composite and showing that pitting corrosion is found in the presence of a high Al<sub>2</sub>O<sub>3</sub> content [<a href="#B100-nanomaterials-15-00092" class="html-bibr">100</a>].</p>
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<p>Variation in microhardness of composites subject to reinforcement.</p>
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<p>SEM micrograph of worn-out surfaces of Mg /SiC (<b>a</b>) Mg/SiC for 0.4 m/s at 5 N, (<b>b</b>) Mg/SiC for 0.4 m/s at 10 N, (<b>c</b>) Mg/SiC for 0.6 m/s at 5 N, (<b>d</b>) Mg/SiC for 0.6 m/s at 10 N, (<b>e</b>) Mg/SiC for 0.8 m/s at 5 N, and (<b>f</b>) Mg/SiC for 0.8 m/s at 10 N [<a href="#B109-nanomaterials-15-00092" class="html-bibr">109</a>]. (<b>g</b>–<b>i</b>) Optical characterization of TiC-reinforced (3 wt.%, 6 wt.%, and 9 wt.%) magnesium composites [<a href="#B111-nanomaterials-15-00092" class="html-bibr">111</a>].</p>
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<p>Surface morphology of worn-out sample of Mg/0.5 wt.% BN composites at a normal load of 5 N and a sliding velocity of (<b>a</b>) 0.6 m/s, (<b>d</b>) 0.9 m/s, and (<b>g</b>) 1.2 m/s; composites at a normal load of 7 N and a sliding velocity of (<b>b</b>) 0.6 m/s, (<b>e</b>) 0.9 m/s, and (<b>h</b>) 1.2 m/s; and composites at a normal load of 10 N and a sliding velocity of (<b>c</b>) 0.6 m/s, (<b>f</b>) 0.9 m/s, (<b>i</b>), 1.2 m/s [<a href="#B143-nanomaterials-15-00092" class="html-bibr">143</a>].</p>
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<p>Compressive strength of composites with reinforcement.</p>
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<p>Mechanical properties of Mg-based material composites formed using different reinforcements (vol.%) in MMCs.</p>
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<p>Variation in compressive strength of composites with different particle sizes of reinforcement in MMCs.</p>
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<p>Variation in microhardness of composites at different sintering temperatures in MMCs.</p>
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<p>Variation in the mechanical properties of composites via different sintering times in MMCs.</p>
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18 pages, 1697 KiB  
Article
Reputation-Based Leader Selection Consensus Algorithm with Rewards for Blockchain Technology
by Munir Hussain, Amjad Mehmood, Muhammad Altaf Khan, Rabia Khan and Jaime Lloret
Computers 2025, 14(1), 20; https://doi.org/10.3390/computers14010020 - 8 Jan 2025
Viewed by 408
Abstract
Blockchain technology is an emerging decentralized and distributed technology that can maintain data security. It has the potential to transform many sectors completely. The core component of blockchain networks is the consensus algorithm because its efficiency, security, and scalability depend on it. A [...] Read more.
Blockchain technology is an emerging decentralized and distributed technology that can maintain data security. It has the potential to transform many sectors completely. The core component of blockchain networks is the consensus algorithm because its efficiency, security, and scalability depend on it. A consensus problem is a difficult and significant task that must be considered carefully in a blockchain network. It has several practical applications such as distributed computing, load balancing, and blockchain transaction validation. Even though a lot of consensus algorithms have been proposed, the majority of them require many computational and communication resources. Similarly, they also suffer from high latency and low throughput. In this work, we proposed a new consensus algorithm for consortium blockchain for a leader selection using the reputation value of nodes and the voting process to ensure high performance. A security analysis is conducted to demonstrate the security of the proposed algorithm. The outcomes show that the proposed algorithm provides a strong defense against the network nodes’ abnormal behavior. The performance analysis is performed by using Hyperledger Fabric v2.1 and the results show that it performs better in terms of throughput, latency, CPU utilization, and communications costs than its rivals Trust-Varying Algo, FP-BFT, and Scalable and Trust-based algorithms. Full article
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<p>Flowchart of the proposed reputation-based consensus algorithm.</p>
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<p>Throughput of the proposed consensus algorithm.</p>
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<p>Latency of the proposed consensus algorithm.</p>
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<p>Resource consumption (CPU cycle).</p>
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<p>Communication bandwidth for the proposed consensus algorithm.</p>
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<p>Security of proposed consensus algorithm against malicious nodes.</p>
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11 pages, 10115 KiB  
Article
Numerical Simulations of Single-Step Holographic Interferometry for Split-Ring Metamaterial Fabrication
by Zhiming Qi and Wenyao Liang
Nanomaterials 2025, 15(2), 86; https://doi.org/10.3390/nano15020086 - 8 Jan 2025
Viewed by 301
Abstract
Artificial microstructures, especially metamaterials, have garnered increasing attention in numerous applications due to their rich and distinctive properties. Starting from the principle of multi-beam interference, we have theoretically devised a beam configuration consisting of six symmetrically distributed coherent beams to generate two-dimensional microstructures [...] Read more.
Artificial microstructures, especially metamaterials, have garnered increasing attention in numerous applications due to their rich and distinctive properties. Starting from the principle of multi-beam interference, we have theoretically devised a beam configuration consisting of six symmetrically distributed coherent beams to generate two-dimensional microstructures with diverse shapes of unitcells under different polarization combinations. In particular, a split-ring metamaterial template is achieved with two adjacent circularly and four linearly polarized beams with such single-step holographic interferometry. Furthermore, simulation results show that the orientation and shape of the split-ring unitcell can be accurately adjusted by controlling the polarization position, polarization degree, or power ratio of the coherent beams. The optimal parameters to produce a high-quality split-ring metamaterial with a contrast higher than 0.97 are obtained. These results provide useful guidance for the effective and low-cost fabrication of metamaterials with diverse unitcells. Full article
(This article belongs to the Special Issue 2D Materials and Metamaterials in Photonics and Optoelectronics)
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<p>(<b>a</b>) Polarization decomposition of the <span class="html-italic">m</span>th light beam. (<b>b</b>) Beam configuration of six light beams. (<b>c</b>) The projected beam configuration and reciprocal basis vectors.</p>
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<p>Simulation results for different polarization combinations. (<b>a1</b>–<b>a3</b>) and (<b>b1</b>–<b>b3</b>) are obtained under relative intensity thresholds of 40% and 64%, respectively. Purple scale bars: equal to the interference wavelength <span class="html-italic">λ</span>.</p>
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<p>Simulation results for different polarization combinations: (<b>a</b>) one, (<b>b1</b>–<b>b3</b>) two, (<b>c1</b>–<b>c3</b>) three, (<b>d1</b>–<b>d3</b>) four, (<b>e</b>) five, or (<b>f</b>) six beams are circularly polarized (<span class="html-italic">γ<sub>m</sub></span> = 1), while the left beams are kept as linearly polarized (<span class="html-italic">γ<sub>m</sub></span> = 0). The red number 1 and black number 0 in <span class="html-italic">γ<sub>m</sub></span> represent the circularly and linearly polarized beams, respectively. Purple scale bars: equal to the interference wavelength <span class="html-italic">λ</span>.</p>
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<p>Simulation results for different polarization positions of adjacent circularly polarized beams. (<b>a</b>) (1, 2) beams; (<b>b</b>) (2, 3) beams; (<b>c</b>) (3, 4) beams; (<b>d</b>) (4, 5) beams. The red number 1 and black number 0 in <span class="html-italic">γ<sub>m</sub></span> represent the circularly and linearly polarized beams, respectively. Purple scale bars: equal to the interference wavelength <span class="html-italic">λ</span>.</p>
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<p>Simulation results for different polarization degrees of adjacent beams 2 and 3: (<b>a</b>) (0.5, 0.5); (<b>b</b>) (1, 1); (<b>c</b>) (2, 2); (<b>d</b>) (5, 5). The red numbers in <span class="html-italic">γ<sub>m</sub></span> indicate the polarization degrees of beams 2 and 3; while the black number 0 in <span class="html-italic">γ<sub>m</sub></span> represents that beams 1, 4, 5, 6 are linearly polarized beams. Purple scale bars: equal to the interference wavelength <span class="html-italic">λ</span>.</p>
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<p>Simulation results for different power ratios of beams 2 to 3: (<b>a</b>) 0.8:1; (<b>b</b>) 1.2:1; (<b>c</b>) 0.8:0.8; (<b>d</b>) 1.2:1.2. The red numbers indicate the power ratios of beams 2 and 3. Purple scale bars: equal to the interference wavelength <span class="html-italic">λ</span>.</p>
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17 pages, 3310 KiB  
Article
Fully Inkjet-Printed Flexible Graphene–Prussian Blue Platform for Electrochemical Biosensing
by Željka Boček, Marko Zubak and Petar Kassal
Biosensors 2025, 15(1), 28; https://doi.org/10.3390/bios15010028 - 8 Jan 2025
Viewed by 314
Abstract
Prussian Blue (PB) is commonly incorporated into screen-printed enzymatic devices since it enables the determination of the enzymatically produced hydrogen peroxide at low potentials. Inkjet printing is gaining popularity in the development of electrochemical sensors as a substitute for screen printing. This work [...] Read more.
Prussian Blue (PB) is commonly incorporated into screen-printed enzymatic devices since it enables the determination of the enzymatically produced hydrogen peroxide at low potentials. Inkjet printing is gaining popularity in the development of electrochemical sensors as a substitute for screen printing. This work presents a fully inkjet-printed graphene–Prussian Blue platform, which can be paired with oxidase enzymes to prepare a biosensor of choice. The graphene electrode was inkjet-printed on a flexible polyimide substrate and then thermally and photonically treated with intense pulsed light, followed by inkjet printing of a PB nanoparticle suspension. The optimization of post-printing treatment and electrode deposition conditions was performed to yield a platform with minimal sheet resistance and peak potential differences. A thorough study of PB deposition was conducted: the fully inkjet-printed system was compared against sensors with PB deposited chemically or by drop casting the PB suspension on different kinds of carbon electrodes (glassy carbon, commercial screen-printed, and in-house inkjet-printed electrodes). For hydrogen peroxide detection, the fully inkjet-printed platform exhibits excellent sensitivity, a wider linear range, better linearity, and greater stability towards higher concentrations of peroxide than the other tested electrodes. Finally, lactate oxidase was immobilized in a chitosan matrix, and the prepared biosensor exhibited analytical performance comparable to other lactate sensors found in the literature in a wide, physiologically relevant linear range for measuring lactate concentration in sweat. The development of mediator-modified electrodes with a single fabrication technology, as demonstrated here, paves the way for the scalable production of low-cost, wearable, and flexible biosensors. Full article
(This article belongs to the Special Issue Flexible Electronics for Biosensing)
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<p>Schematic representation of the inkjet-printed electrode assembly and modification.</p>
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<p>PBNP suspension characterization. (<b>a</b>) Photo of a freshly prepared PBNP suspension, (<b>b</b>) UV/Vis spectrum of the suspension, (<b>c</b>) stability of the suspension during 4 h, (<b>d</b>) size distribution obtained by DLS, (<b>e</b>) ζ-potential obtained by ELS, and (<b>f</b>) fully inkjet-printed graphene–PBNP platform.</p>
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<p>IPL treatment optimization of inkjet-printed graphene electrodes. (<b>a</b>) Sheet resistance measurements via four point probe measurements (inset shows the significant drop of sheet resistance of the electrode after treatment compared to the unprocessed electrode); (<b>b</b>) peak separation in cyclic voltammograms (PW↔PB) at 10 mV/s recorded on an inkjet-printed electrode chemically modified after corresponding treatment.</p>
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<p>Electrochemical characterization results for optimized deposition methods on inkjet-printed electrodes (top row: chemical deposition 20 min; bottom row: drop-cast PBNP, 10 μL). (<b>a</b>) Activation in 0.1 M KCl (scan rate 50 mV/s); (<b>b</b>) scan rate dependence recorded in 0.1 M KCl (10–100 mV/s); (<b>c</b>) pH stability of deposited films shown as cathodic peak current value extracted from cyclic voltammograms recorded in buffers (pH 5.4, 6.4 and 7.4).</p>
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<p>SEM images of optimized PB-modified inkjet-printed electrodes: (<b>a</b>–<b>c</b>) chemically deposited PB ((<b>a</b>)—6k magnification, (<b>b</b>)—20k magnification, (<b>c</b>)—EDS mapping at lower magnification); (<b>d</b>–<b>f</b>) drop-cast PB nanoparticles ((<b>d</b>)—6k magnification, (<b>e</b>)—20k magnification, (<b>f</b>)—EDS mapping at lower magnification).</p>
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<p>H<sub>2</sub>O<sub>2</sub> detection with chronoamperometry ((<b>1</b>)—chronoamperograms and (<b>2</b>)—calibration curves) on electrodes modified by (<b>a</b>) 20 min chemical deposition, (<b>b</b>) drop casting 10 µL of PBNP suspension, (<b>c</b>) fully inkjet printing the PBNP suspension.</p>
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<p>Lactate detection with chronoamperometry on fully assembled inkjet-printed sensor ((<b>1</b>)—chronoamperograms and (<b>2</b>)—calibration curves for electrodes modified by (<b>a</b>) 20 min chemical deposition, (<b>b</b>) drop casting 10 µL of PBNP suspension, (<b>c</b>) fully inkjet printing the PBNP suspension).</p>
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17 pages, 3662 KiB  
Article
Superhydrophilic Titania Coatings on Glass Substrates via the Hydrosol Approach
by George V. Theodorakopoulos, Michalis K. Arfanis, Nafsika Mouti, Andreas Kaidatzis, Christian Mitterer, Konstantinos Giannakopoulos and Polycarpos Falaras
Surfaces 2025, 8(1), 5; https://doi.org/10.3390/surfaces8010005 - 6 Jan 2025
Viewed by 372
Abstract
This study presents a comprehensive investigation into the synthesis and characterization of TiO2 coatings on glass substrates, focusing on the development of superhydrophilic, self-cleaning titania coatings using the hydrosol approach. Stringent cleaning protocols were accurately followed to ensure the pristine condition of [...] Read more.
This study presents a comprehensive investigation into the synthesis and characterization of TiO2 coatings on glass substrates, focusing on the development of superhydrophilic, self-cleaning titania coatings using the hydrosol approach. Stringent cleaning protocols were accurately followed to ensure the pristine condition of glass surfaces prior to deposition. Various organic precursor solutions were precisely prepared and applied to the glass substrate via dip-coating, followed by subsequent thermal treatment. A range of characterization techniques, including Raman spectroscopy, UV/Vis spectroscopy, scanning and atomic force microscopy, X-ray photoelectron spectroscopy, and contact angle measurements, were employed to assess the properties of the coatings. The results revealed that the samples were influenced by precursor concentration and withdrawal rate, with slow speed leading to minimal alteration of transmittance. The coatings show superhydrophilic properties, as evidenced by contact angle values below 3 degrees for the thinnest films. Their thickness is approximately 13 nm with very low roughness, indicative of a smooth and uniform surface. Optimization of the deposition conditions permits the fabrication of uniform and transparent TiO2 coatings on glass substrates, offering promising opportunities for the practical use of photoinduced self-cleaning surfaces in real-life applications. Finally, a cost analysis of scaling up the coating and mirror fabrication processes confirmed the economic feasibility of this approach for concentrated solar power (CSP) applications. Full article
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Graphical abstract
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<p>Transmittance spectra of glass slides after TiO<sub>2</sub> deposition using different TTIP concentrations: (<b>a</b>) Co; (<b>b</b>) Co/2; (<b>c</b>) Co/4; and (<b>d</b>) Co/8 and for various withdrawal speeds (0.5 to 50 mm/s).</p>
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<p>SEM images of a reference glass slide (<b>a</b>); and TiO<sub>2</sub> coatings prepared using sols with TTIP concentration of Co (<b>b</b>); Co/2 (<b>c</b>); Co/4 (<b>d</b>); and Co/8 (<b>e</b>), for a withdrawal speed of 5 mm/s.</p>
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<p>Dependence of film thickness on TTIP precursor concentration (Co = 1× precursor concentration, Co/2 = 1/2×, Co/4 = 1/4×) at medium withdrawal speed (5 mm/s).</p>
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<p>Representative Raman spectra for sol-gel samples.</p>
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<p>High-resolution XPS spectra of the Co/4 sample in the Ti 2p (<b>a</b>); and O 1s region (<b>b</b>).</p>
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<p>Contact angle measurements of the coated samples produced from organic sols with varying TTIP concentration and withdrawal speeds. The software of the instrument is unable to accurately calculate angles below 3°.</p>
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<p>Indicative contact angle images of a super-hydrophilic sample: within detection limits (sample Co-m) (<b>a</b>); below the detection limits of the software (sample Co/4-m) (<b>b</b>).</p>
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<p>2D AFM images of the (<b>a</b>) bare substrate, and (<b>b</b>) Co/4 sample; (<b>c</b>) corresponding height profiles. The vertical scale is 5 nm in (<b>a</b>) and 60 nm in (<b>b</b>).</p>
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21 pages, 20668 KiB  
Article
Inverted Pyramid Nanostructures Coupled with a Sandwich Immunoassay for SERS Biomarker Detection
by Wen-Huei Chang, Shao-Quan Zhang, Zi-Yi Yang and Chun-Hung Lin
Nanomaterials 2025, 15(1), 64; https://doi.org/10.3390/nano15010064 - 2 Jan 2025
Viewed by 492
Abstract
Cancer diagnostics often faces challenges, such as invasiveness, high costs, and limited sensitivity for early detection, emphasizing the need for improved approaches. We present a surface-enhanced Raman scattering (SERS)-based platform leveraging inverted pyramid SU-8 nanostructured substrates fabricated via nanoimprint lithography. These substrates, characterized [...] Read more.
Cancer diagnostics often faces challenges, such as invasiveness, high costs, and limited sensitivity for early detection, emphasizing the need for improved approaches. We present a surface-enhanced Raman scattering (SERS)-based platform leveraging inverted pyramid SU-8 nanostructured substrates fabricated via nanoimprint lithography. These substrates, characterized by sharp apices and edges, are further functionalized with (3-aminopropyl)triethoxysilane (APTES), enabling the uniform self-assembly of AuNPs to create a highly favorable configuration for enhanced SERS analysis. Performance testing of the substrates using malachite green (MG) as a model analyte demonstrated excellent detection capabilities, achieving a limit of detection as low as 10−12 M. Building on these results, the SERS platform was adapted for the sensitive and specific detection of hyaluronic acid (HA), a key biomarker associated with inflammation and cancer progression. The system employs a sandwich immunoassay configuration, with substrates functionalized with antibodies to capture HA molecules and 4-MBA-labeled SERS tags for detection. This setup achieved an ultra-sensitive detection limit of 10−11 g/mL for HA. Comprehensive characterization confirmed the uniformity and reproducibility of the SERS substrates, while validation in complex biological matrices demonstrated their robustness and reliability, highlighting their potential in cancer diagnostics and biomarker detection. Full article
(This article belongs to the Special Issue Synthesis and Applications of Gold Nanoparticles: 2nd Edition)
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Graphical abstract

Graphical abstract
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<p>Fabrication of inverted pyramid nanostructures. (<b>a</b>) Cr hole array mask with 400 nm period and 265 nm hole size remains on the substrate after lift-off. (<b>b</b>) Inverted pyramid Si structures, approximately 285 nm in size, formed through KOH anisotropic wet etching. (<b>c</b>) SU-8 inverted pyramid nanostructures imprinted on a Si substrate using a PFPE mold replicated from the Si master in (<b>b</b>). Scale bars in (<b>a</b>–<b>c</b>) represent 500 nm.</p>
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<p>Functionalization and AuNP attachment on SU-8 inverted pyramid nanostructures. (<b>a</b>) SEM image of synthesized AuNPs with an average size of approximately 24.6 nm, self-assembled on an APTES-functionalized SU-8 film. (<b>b</b>) Absorption spectrum of the AuNP solution, displaying a peak near 521 nm, alongside Mie scattering simulation results that indicate a corresponding AuNP size of 25.1 nm for the same absorption peak wavelength. (<b>c</b>) Top-view and (<b>d</b>) cross-sectional SEM images of AuNPs self-assembled on the APTES-functionalized SU-8 inverted pyramids. Scale bars in (<b>a</b>,<b>c</b>,<b>d</b>) represent 50 nm and 200 nm, respectively.</p>
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<p>Evaluation of SERS substrate performance using MG as the test analyte. (<b>a</b>) SERS spectra of MG at concentrations of 10<sup>−7</sup> to 10<sup>−11</sup> M, with the average intensity from five locations per sample. (<b>b</b>) SERS spectra of MG on an F<sub>13</sub>-TCS-treated hydrophobic substrate, ranging from 10<sup>−7</sup> to 10<sup>−12</sup> M, with an inset showing spectra at 10<sup>−11</sup> and 10<sup>−12</sup> M. (<b>c</b>) SERS spectra of 10<sup>−7</sup> M MG measured at 10 different locations along the coffee ring on a single substrate. (<b>d</b>) Signal intensities at 1170, 1365, and 1613 cm<sup>−1</sup> for these points, with RSDs of 7.26%, 6.49%, and 6.30%. (<b>e</b>) SERS spectra at 10<sup>−7</sup> M MG from five different substrates. (<b>f</b>) Signal intensities at the same peaks across substrates, with RSDs of 8.37%, 7.11%, and 7.27%.</p>
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<p>(<b>a</b>,<b>b</b>) DLS measurements of particle size and zeta potential variations after sequential modifications with 4-MBA and anti-HA antibodies. (<b>c</b>,<b>d</b>) TEM images showing morphological changes in AuNPs before and after conjugation with 4-MBA and anti-HA antibodies. (<b>e</b>) Absorption spectrum showing a redshift of 3.8 nm after anti-HA modification.</p>
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<p>SERS-based detection of HA molecules. (<b>a</b>) Raman spectra of 4-MBA at HA concentrations ranging from 10<sup>−7</sup> to 10<sup>−11</sup> g/mL. (<b>b</b>,<b>c</b>) The relationship between the Raman intensity and HA concentration at 1074 cm<sup>−1</sup> and 1581 cm<sup>−1</sup>, respectively. (<b>d</b>) Raman peak intensities at 1074 and 1581 cm<sup>−1</sup> for the anti-HA-functionalized SERS substrate tested with HA, CFH, and NMP22 antigens in deionized water, as well as HA antigen in a simulated complex environment containing 10% FBS, each at a concentration of 10<sup>−7</sup> g/mL. (<b>e</b>) Raman spectra of HA detection at 10<sup>−7</sup> g/mL in a simulated complex environment containing 10% FBS, compared to HA detection in deionized water. Measurements were taken at five distinct locations for each condition.</p>
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<p>Schematic representation of key processes: (<b>a</b>) fabrication of inverted pyramid nanostructures on a Si substrate, (<b>b</b>) preparation of an antibody-functionalized SERS substrate for antigen capture, and (<b>c</b>) preparation of SERS tags by conjugating 4-MBA and antibodies to AuNPs for signal detection.</p>
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14 pages, 9705 KiB  
Article
ZnO Nanoparticles by Hydrothermal Method: Synthesis and Characterization
by Juan Carlos Anaya-Zavaleta, Antonio Serguei Ledezma-Pérez, Carlos Gallardo-Vega, Joelis Rodríguez-Hernández, Carmen Natividad Alvarado-Canché, Perla Elvia García-Casillas, Arxel de León and Agustín Leobardo Herrera-May
Technologies 2025, 13(1), 18; https://doi.org/10.3390/technologies13010018 - 1 Jan 2025
Viewed by 725
Abstract
The synthesis of reliable, cost-effective, and eco-friendly ZnO piezoelectric nanoparticles (NPs) can contribute to nanotechnology applications in electronics, sensors, and energy harvesting. Herein, ZnO NPs were synthesized using a hydrothermal method under varied reaction times and adding ammonium hydroxide, which provided an advantage [...] Read more.
The synthesis of reliable, cost-effective, and eco-friendly ZnO piezoelectric nanoparticles (NPs) can contribute to nanotechnology applications in electronics, sensors, and energy harvesting. Herein, ZnO NPs were synthesized using a hydrothermal method under varied reaction times and adding ammonium hydroxide, which provided an advantage of a low-cost, scalable, low-temperature, and environmentally friendly process. Characterization through UV–Vis spectroscopy revealed absorption peaks between 374 and 397 nm, showing a blue shift compared to bulk ZnO (400 nm) attributable to nanoscale dimensions. Transmission Electron Microscopy (TEM) analysis indicated particle dimensions with length and width ranges from 150 to 341 nm and from 83 to 120 nm, respectively. X-ray diffraction (XRD) confirmed high-crystalline quality, with crystallite sizes calculated using the Scherrer equation. In addition, the effective mass model provided an estimated band gap that matched with the reported data. Also, the lattice parameters, interplanar distances, and Zn-O bond lengths were consistent with Joint Committee on Powder Diffraction Standards (JCPDS). Finally, a ZnO NP film was deposited on a steel substrate, which generated a displacement of 150 nm under a square wave voltage of 10 V. The piezoelectric behavior of the synthesized ZnO NPs can be useful for fabrication of piezoelectric nanogenerators. The proposed synthesis can allow ZnO NPs with potential application in electronic devices, energy harvesters, and transducers. Full article
(This article belongs to the Special Issue Technological Advances in Science, Medicine, and Engineering 2024)
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<p>Reaction methodology: (<b>a</b>) solution on a magnetic stirring, (<b>b</b>) completely dissolved solution, (<b>c</b>) solution into a Teflon-lined stainless steel autoclave in a muffle, and (<b>d</b>) washed and centrifuged.</p>
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<p>Normalized UV–Vis absorbance from each ZnO nanoparticle reaction. Note: For reactions with (*), the ammonium hydroxide was used.</p>
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<p>TEM images and histograms for each ZnO nanoparticle reaction of length and width: (<b>a</b>) ZnO-1, (<b>b</b>) *ZnO-1, (<b>c</b>) ZnO-2, (<b>d</b>) *ZnO-2, and (<b>e</b>) ZnO-3. For reactions with (*), the ammonium hydroxide was used.</p>
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<p>XRD patterns from each reaction.</p>
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<p>Bond length parallel to c, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="normal">L</mi> </mrow> <mrow> <mi mathvariant="normal">C</mi> </mrow> </msub> </mrow> </semantics></math>—for ab, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="normal">L</mi> </mrow> <mrow> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">b</mi> </mrow> </msub> </mrow> </semantics></math>—in a tetrahedral <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="normal">Z</mi> <mi mathvariant="normal">n</mi> </mrow> <mrow> <mn>4</mn> </mrow> </msub> <mi mathvariant="normal">O</mi> </mrow> </semantics></math> structural unit. Red is oxygen and yellow is zinc.</p>
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<p>(<b>a</b>) ZnO powder before being compressed into a pill; (<b>b</b>) ZnO pill into a hysteresis characterization.</p>
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<p>Measured polarization field hysteresis loops of ZnO powder pill.</p>
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<p>Displacement of a beam composed of a ZnO NPs film which was generated by square wave voltages at 1 Hz. Supplied voltages from (<b>a</b>) 1 to 10 and 1 V and (<b>b</b>) 1 to 10 V.</p>
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<p>Displacement of a beam composed of a ZnO NPs film, which was generated by square wave voltages at 50 Hz. Supplied voltages from (<b>a</b>) 1 to 10 V and (<b>b</b>) 10 to 1 V.</p>
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<p>Measurements of the thickness of the ZnO NPs film.</p>
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