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14 pages, 3247 KiB  
Article
Validating Structural Predictions of Conjugated Macromolecules in Espaloma-Enabled Reproducible Workflows
by Madilyn E. Paul, Chris D. Jones and Eric Jankowski
Int. J. Mol. Sci. 2025, 26(2), 478; https://doi.org/10.3390/ijms26020478 - 8 Jan 2025
Abstract
We incorporated Espaloma forcefield parameterization into MoSDeF tools for performing molecular dynamics simulations of organic molecules with HOOMD-Blue. We compared equilibrium morphologies predicted for perylene and poly-3-hexylthiophene (P3HT) with the ESP-UA forcefield in the present work against prior work using the OPLS-UA forcefield. [...] Read more.
We incorporated Espaloma forcefield parameterization into MoSDeF tools for performing molecular dynamics simulations of organic molecules with HOOMD-Blue. We compared equilibrium morphologies predicted for perylene and poly-3-hexylthiophene (P3HT) with the ESP-UA forcefield in the present work against prior work using the OPLS-UA forcefield. We found that, after resolving the chemical ambiguities in molecular topologies, ESP-UA is similar to GAFF. We observed the clustering/melting phase behavior to be similar between ESP-UA and OPLS-UA, but the base energy unit of OPLS-UA was found to better connect to experimentally measured transition temperatures. Short-range ordering measured by radial distribution functions was found to be essentially identical between the two forcefields, and the long-range ordering measured by grazing incidence X-ray scattering was qualitatively similar, with ESP-UA matching experiments better than OPLS-UA. We concluded that Espaloma offers promise in the automated screening of molecules that are from more complex chemical spaces. Full article
(This article belongs to the Special Issue Molecular Modelling in Material Science)
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Figure 1

Figure 1
<p>Depictions of our generalized molecular dynamics workflow. Step 1 shows the creation of an <tt>mBuild Compound</tt> from a SMILES string. In Step 2, we create our simulation object using <tt>flowerMD</tt> and <tt>PACKMOL</tt>. We employed <tt>Espaloma</tt>to parameterize our molecules in Step 3 and write the forcefield file. In Step 4, we initialized the <tt>HOOMD-Blue</tt> simulation and predicted the morphology of our molecules.</p>
Full article ">Figure 2
<p>Diagram of the perylene molecule (<b>left</b>) and poly-3-hexylthiophene (P3HT) monomer (<b>right</b>).</p>
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<p>Temperature vs. density clustering in an order parameter (<math display="inline"><semantics> <mo>Ψ</mo> </semantics></math>) phase diagram of perylene at 12 statepoints.</p>
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<p>Snapshot of the perylene taken from the most ordered morphology at a density of 0.5 g/cm<sup>3</sup> and temperature of 248.8 K.</p>
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<p>(<b>A</b>) Radial distribution function (RDF) of perylene at various temperatures at a density of 0.5 g/cm<sup>3</sup>, which were generated from an <tt>ESP-UA</tt>-predicted morphology. (<b>B</b>) The RDF of perylene in various phases, which was generated from an <tt>OPLS-UA</tt>-predicted morphology. The <tt>OPLS-UA</tt> RDF published by Miller et al. in Ref. [<a href="#B19-ijms-26-00478" class="html-bibr">19</a>].</p>
Full article ">Figure 6
<p>(<b>A</b>) The grazing incident X-ray scattering pattern of perylene generated from an <tt>ESP-UA</tt> morphology. (<b>B</b>) The GIXS pattern of the perylene generated from an <tt>OPLS-UA</tt> morphology. The <tt>OPLS-UA</tt> GIXS pattern published by Miller et. al. in Ref. [<a href="#B19-ijms-26-00478" class="html-bibr">19</a>]. (<b>C</b>) The experimental XRD pattern for <math display="inline"><semantics> <mrow> <mi>β</mi> </mrow> </semantics></math>−perylene, which was reproduced with permission from Ishii et al. from Ref. [<a href="#B26-ijms-26-00478" class="html-bibr">26</a>]. Copyright 2014 AIP Publishing LLC. (Melville, NY, USA).</p>
Full article ">Figure 7
<p>Temperature vs. density clustering in an order parameter (<math display="inline"><semantics> <mo>Ψ</mo> </semantics></math>) phase diagram of P3HT at 12 statepoints.</p>
Full article ">Figure 8
<p>(<b>A</b>) The radial distribution function (RDF) of P3HT at a temperature of 304 K and a density of 0.5 g/cm<sup>3</sup>, which was generated from an <tt>ESP-UA</tt>-predicted morphology. (<b>B</b>) The RDF of P3HT generated from an <tt>OPLS-UA</tt>-predicted morphology. The <tt>OPLS-UA</tt> RDF published by Miller et al. in Ref. [<a href="#B20-ijms-26-00478" class="html-bibr">20</a>].</p>
Full article ">Figure 9
<p>(<b>A</b>) The grazing incident X-ray scattering pattern of P3HT at 0.5 g/cm<sup>3</sup> and 304 K generated using <tt>ESP-UA</tt>. (<b>B</b>) The corresponding experimental scattering pattern of P3HT. Reprinted (adapted) with permission from Ko et al., as shown in Ref. [<a href="#B28-ijms-26-00478" class="html-bibr">28</a>]. Copyright 2012 American Chemical Society.</p>
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<p>Snapshot of the P3HT’s most ordered morphology at a density of 0.5 g/cm<sup>3</sup> and a temperature of 304 K.</p>
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<p>Blue spheres represent the center-of-geometry positions used for RDFs and clustering criteria. Perylene (<b>a</b>), and P3HT (<b>b</b>).</p>
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<p>Overall <tt>Espaloma</tt>-<tt>MosDeF</tt> workflow. (1) <tt>mBuild</tt> compounds were used to create the topology of an <tt>openMM</tt> molecule, (2) <tt>BondWalker</tt> used octet rules to determine the double bonds in the <tt>openMM</tt> molecule. (3) <tt>Espaloma</tt> generated forcefield parameters for the <tt>openMM</tt> molecule. (4) The <tt>ESP-UA</tt> forcefield was used to re-type the <tt>mBuild</tt> compound for use in <tt>HOOMD-Blue</tt> simulations.</p>
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<p>The double- and triple-bond information that is missing from the <tt>mBuild</tt> compounds is retrieved via <tt>BondWalker</tt> by iteratively checking whether the octet rules can be satisfied for all atoms after incrementing the bond character adjacent to atoms with unsatisfied octets. Highlighted ring in the lower left shows correct double-bond assignment after application of <tt>Bondwalker</tt>.</p>
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28 pages, 10411 KiB  
Review
Porosity Tunable Metal-Organic Framework (MOF)-Based Composites for Energy Storage Applications: Recent Progress
by Huddad Laeim, Vandana Molahalli, Pongthep Prajongthat, Apichart Pattanaporkratana, Govind Pathak, Busayamas Phettong, Natthawat Hongkarnjanakul and Nattaporn Chattham
Polymers 2025, 17(2), 130; https://doi.org/10.3390/polym17020130 - 8 Jan 2025
Viewed by 195
Abstract
To solve the energy crisis and environmental issues, it is essential to create effective and sustainable energy conversion and storage technologies. Traditional materials for energy conversion and storage however have several drawbacks, such as poor energy density and inadequate efficiency. The advantages of [...] Read more.
To solve the energy crisis and environmental issues, it is essential to create effective and sustainable energy conversion and storage technologies. Traditional materials for energy conversion and storage however have several drawbacks, such as poor energy density and inadequate efficiency. The advantages of MOF-based materials, such as pristine MOFs, also known as porous coordination polymers, MOF composites, and their derivatives, over traditional materials, have been thoroughly investigated. These advantages stem from their high specific surface area, highly adjustable structure, and multifunctional nature. MOFs are promising porous materials for energy storage and conversion technologies, according to research on their many applications. Moreover, MOFs have served as sacrificial materials for the synthesis of different nanostructures for energy applications and as support substrates for metals, metal oxides, semiconductors, and complexes. One of the most intriguing characteristics of MOFs is their porosity, which permits space on the micro- and meso-scales, revealing and limiting their functions. The main goals of MOF research are to create high-porosity MOFs and develop more efficient activation techniques to preserve and access their pore space. This paper examines the porosity tunable mixed and hybrid MOF, pore architecture, physical and chemical properties of tunable MOF, pore conditions, market size of MOF, and the latest development of MOFs as precursors for the synthesis of different nanostructures and their potential uses. Full article
(This article belongs to the Section Polymer Applications)
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Graphical abstract

Graphical abstract
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<p>The development of metal–organic frameworks and their prospects for high-performance supercapacitors [<a href="#B5-polymers-17-00130" class="html-bibr">5</a>].</p>
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<p>The Web of science data of MOF-based material for energy applications (typing keyword MOF, Energy) and number of documents published by type, subject area and the year.</p>
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<p>Utilization of metal–organic frameworks and their derivatives in supercapacitors [<a href="#B10-polymers-17-00130" class="html-bibr">10</a>].</p>
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<p>Development of MOF materials for upcoming generation rechargeable energy sources [<a href="#B14-polymers-17-00130" class="html-bibr">14</a>]. Figure (<b>a</b>) Structure of Ni –MOF, (<b>b</b>) Crystal structure of Ni<sub>3</sub>(HITP)<sub>2</sub>. (<b>c</b>) crystal structure of MOF-199.</p>
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<p>Perfect MOF and covalent organic framework (COF) components for cutting-edge batteries [<a href="#B19-polymers-17-00130" class="html-bibr">19</a>].</p>
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<p>Metal oxide composites produced from MOFs and their potential uses in energy storage [<a href="#B19-polymers-17-00130" class="html-bibr">19</a>].</p>
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<p>Methods for pore architecturing MOFs (<b>a</b>) Structural features and design directions of MOFs. (<b>b</b>–<b>e</b>) General strategies for manipulating pores, including (<b>b</b>) molecular design, (<b>c</b>) templating, (<b>d</b>) controlled assembly, and (<b>e</b>) defect engineering. [<a href="#B22-polymers-17-00130" class="html-bibr">22</a>].</p>
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<p>Strategies for pore architecturing materials generated from MOFs.</p>
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<p>The production of Ni-MOF@PPy and its application in the construction of the asymmetric supercapacitor Ni-MOF@PPy/AC [<a href="#B24-polymers-17-00130" class="html-bibr">24</a>].</p>
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<p>The electrochemical properties of Ni-MOF@PPy//AC ASC are demonstrated by the following: (<b>a</b>) specific capacitance curve at various current densities; (<b>b</b>) CV curves under varying scan rates; (<b>c</b>) GCD curves at various current densities; and (<b>d</b>) CV curves at various voltage windows [<a href="#B23-polymers-17-00130" class="html-bibr">23</a>].</p>
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<p>Substrate materials for high-performance supercapattery devices based on co-MOF and polyaniline. (<b>a</b>). Pictorial illustration of the ASC device, AC//MOF/PANI; CV profiles of AC anode and MOF/PANI cathode (<b>b</b>); GCD curves at various current density (<b>c</b>); specific capacity vs. current density plot (<b>d</b>); specific capacity and columbic efficiency plot (<b>e</b>); and EIS of before stability test, after 3000 GCD cycles and one month later (<b>f</b>) [<a href="#B25-polymers-17-00130" class="html-bibr">25</a>].</p>
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<p>A combination of Ni/Co-MOF-rGO composite as electrode material for high-performance supercapacitors [<a href="#B26-polymers-17-00130" class="html-bibr">26</a>].</p>
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<p>Most commonly employed methods of synthesis of MOFs [<a href="#B30-polymers-17-00130" class="html-bibr">30</a>].</p>
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<p>Schematic pathway of 2D Ni-MOF/C-CNTs [<a href="#B38-polymers-17-00130" class="html-bibr">38</a>].</p>
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<p>Illustration of synthesis process for composite NC/Ni-Ni<sub>3</sub>S<sub>4</sub>/CNTs.</p>
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<p>Modifiable rare-earth fcu-MOFs. An integrated framework to boost CO<sub>2</sub> adsorption energetics and uptake [<a href="#B40-polymers-17-00130" class="html-bibr">40</a>].</p>
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<p>MOFs serve as adaptable carriers for NE encapsulation. NE@MOF composites can be categorized into four groups according to their structural features [<a href="#B43-polymers-17-00130" class="html-bibr">43</a>].</p>
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<p>Pore size contraction-based adsorption kinetics-driven gas/vapor separations using modifiable rare-earth fcu-MOF platform [<a href="#B47-polymers-17-00130" class="html-bibr">47</a>].</p>
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<p>Building MXene @Ce-MOF composites rich in oxygen vacancies for improved energy conversion and storage [<a href="#B48-polymers-17-00130" class="html-bibr">48</a>].</p>
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<p>Composites for structural energy storage that are based on improved carbon fiber electrodes with layered double hydroxide metal–organic frame enhancement [<a href="#B49-polymers-17-00130" class="html-bibr">49</a>].</p>
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<p>An assessment of both redox-active Cu-MOF and Co-MOF as materials for electrodes for hybrid energy storage devices of battery–supercapacitor type [<a href="#B50-polymers-17-00130" class="html-bibr">50</a>].</p>
Full article ">Figure 22
<p>Effective use and storage of solar thermal energy based on phase change substances stabilized by MOF@CuO composites [<a href="#B51-polymers-17-00130" class="html-bibr">51</a>].</p>
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<p>Global MOF for marketing field with various applications.</p>
Full article ">
18 pages, 1759 KiB  
Article
Comparative Analysis of Chemical Composition and Antibacterial Activity of Essential Oils from Five Varieties of Lavender Extracted via Supercritical Fluid Extraction
by Lijing Lin, Zhencheng Lv, Meiyu Wang, Ankang Kan, Songling Zou, Bin Wu, Limin Guo, Salamet Edirs, Jiameng Liu and Lin Zhu
Molecules 2025, 30(2), 217; https://doi.org/10.3390/molecules30020217 - 7 Jan 2025
Viewed by 216
Abstract
This study aimed to determine the chemical composition of five Lavender essential oils (LEOs) using the gas chromatography–mass spectroscopy technique and to assess their antibacterial activity against four marine Vibrio species, including Shewanella algae, Shewanella maridflavi, Vibrio harveyi, and Vibrio [...] Read more.
This study aimed to determine the chemical composition of five Lavender essential oils (LEOs) using the gas chromatography–mass spectroscopy technique and to assess their antibacterial activity against four marine Vibrio species, including Shewanella algae, Shewanella maridflavi, Vibrio harveyi, and Vibrio alginolyticus. Sensitivity tests were performed using the disk diffusion and serial dilution methods. The results showed that all five LEOs exhibited antibacterial activity against the four tested marine Vibrio species. The antibacterial activities of all five LEOs were above moderate sensitivity. The five LEOs from French blue, space blue, eye-catching, and true Lavender showed high sensitivity, particularly against Shewanella maridflavi. The compounds of LEOs from different varieties of Lavender were similar and mainly comprised linalool, linalyl acetate, eucalyptol, and isoborneol. Different varieties of LEOs possessed unique components besides common components, and the percentage of each one was different, which led to different fragrance loads. The major fragrances were lily of the valley, an aromatic compound fragrance, and an herbal fragrance. The antibacterial activity of LEO from eye-catching Lavender was better than that of others, which could provide a reference for its application in the prevention and control of marine Vibrio spp. and the development of antibacterial products. Full article
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Figure 1
<p>(<b>a</b>) Bacteriostatic effect of five <span class="html-italic">Lavender</span> essential oils against <span class="html-italic">Shewanella maridflavi</span>. (<b>b</b>) Inhibition zone effect of five LEOs against <span class="html-italic">Shewanella algae</span>. (<b>c</b>) Inhibition zone effect of five LEOs against <span class="html-italic">Vibrio alginolyticus</span>. (<b>d</b>) Inhibition zone effect of five LEOs against <span class="html-italic">Vibrio harveyi</span>.</p>
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<p>Total ion chromatogram of volatile components in LEOs ((<b>a</b>) French blue LEO; (<b>b</b>) 701 LEO; (<b>c</b>) space blue LEO; (<b>d</b>) eye-catching LEO; (<b>e</b>) true LEO).</p>
Full article ">Figure 3
<p>Radar chart of aroma distribution for each essential oil. Note: (<b>a</b>) French blue <span class="html-italic">Lavender</span>; (<b>b</b>) 701 <span class="html-italic">Lavender</span>; (<b>c</b>) space blue <span class="html-italic">Lavender</span>; (<b>d</b>) eye-catching <span class="html-italic">Lavender</span>; (<b>e</b>) true <span class="html-italic">Lavender</span>; each letter represents a different aroma: A—fatty; B—cool; C—citrus; D—frankincense; E—food; F—fruity; G—green; H—herbaceous; I—iris; J—jasmine; K—pine; L—aromatic compounds; M—lily of the valley; N—narcotic; O—orchid; P—phenolic; R—rose; S—spicy; T—toasted; Ve—vegetable; W—woody; Y—earthy; Z—organic solvent; Ca—camphor.</p>
Full article ">
18 pages, 2058 KiB  
Article
Multi-Criteria Decision Analysis in Drug Discovery
by Rafał A. Bachorz, Michael S. Lawless, David W. Miller and Jeremy O. Jones
Appl. Biosci. 2025, 4(1), 2; https://doi.org/10.3390/applbiosci4010002 - 6 Jan 2025
Viewed by 332
Abstract
Drug discovery is inherently a multi-criteria optimization problem. In the first instance, it involves a tremendously large chemical space, where each compound can be characterized by multiple molecular and biological properties. Modern computational approaches try to efficiently explore the chemical space in search [...] Read more.
Drug discovery is inherently a multi-criteria optimization problem. In the first instance, it involves a tremendously large chemical space, where each compound can be characterized by multiple molecular and biological properties. Modern computational approaches try to efficiently explore the chemical space in search of molecules with the desired combination of properties. For example, Pareto optimizers identify a so-called “Pareto front”, a set of non-dominated solutions. From a qualitative perspective, all solutions on the front are potentially equally desirable, each expressing a trade-off between the goals. However, often there is a need to weight the objectives differently, depending on their perceived importance. To address this, we recently implemented a new Multi-Criteria Decision Analysis (MCDA) method as part of the AI-powered Drug Design (AIDDTM) technology initiative. This allows the user to weight various objective functions differently, which, in turn, efficiently directs the generative chemistry process toward the desired areas in chemical space. Full article
(This article belongs to the Special Issue Neural Networks and Deep Learning for Biosciences)
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Figure 1
<p>Illustration of multiple Pareto fronts based on two criteria. Each point represents an alternative in the two-dimensional space of both criteria, with the lowest Pareto front (1st Pareto front) containing non-dominated alternatives, and each subsequent front containing points that are dominated by all alternatives in the previous fronts. All alternatives on the same Pareto front are considered qualitatively equivalent among all the alternatives on that front. This highlights a limitation of the Pareto approach, i.e., the lack of the ability to distinguish between alternatives on a given front.</p>
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<p>A set of alternatives evaluated across two differently weighted criteria: Criterion 1 (weight 0.85) and Criterion 2 (weight 0.15). Each numbered point represents an alternative uniquely ranked by the VIKOR method. By incorporating criterion weights and calculating a combined <span class="html-italic">Q</span> score, VIKOR enables differentiation among alternatives that might otherwise appear equally optimal on the same Pareto front, providing a more refined decision-making framework.</p>
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<p>The seed structure (benzimidazole), target, and rediscovered structures resulting from the calculation in which MCDA pruning was applied to the 5a86 ligand rediscovery.</p>
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<p>Histogram showing the distribution of 3D similarity scores for compounds generated using MCDA and Pareto pruning applied within the AIDD<sup>TM</sup> module.</p>
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<p>Overlay of candidate and reference (green) compounds, illustrating the structural similarity achieved. The upper image shows the best match obtained with MCDA pruning, with a high 3D similarity score (Sim3D = 0.875). The lower image displays one of the worst matches, with a lower Sim3D score (Sim3D = 0.81), reflecting a less favorable alignment between the candidate and reference compounds.</p>
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<p>The reference 5a86 ligand structure in its native experimental conformation, serving as a baseline for 3D similarity assessments in compound optimization.</p>
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<p>Distribution of pEC50 biological activity values for the PXR receptor, obtained from the ChEMBL database. The training data are shown in dark blue, while the test data are represented in light blue.</p>
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<p>Plot of predicted vs. observed pIC50 values, illustrating the quality of the QSAR regression model for agonistic biological activity toward the PXR receptor. On the test set, the model achieved an RMSE of 0.468 and an MAE of 0.380, indicating satisfactory predictive capability.</p>
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<p>The optimized ligands aim to reduce activation of the PXR receptor while maintaining 3D similarity to the crystal structure reference. At the top is the initial structure from the 5a86 crystal structure, and at the bottom are four proposed analogs exhibiting low PXR activity and high 3D similarity.</p>
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<p>Overlay of the reference ligand reference structure (in green) with the selected optimized compound.</p>
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<p>Histogram showing the distribution of 3D similarity scores for compounds generated using VIKOR, TOPSIS, and Pareto pruning in the ciprofloxacin molecular optimization.</p>
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<p>Histogram showing the distribution of fraction bioavailable (%Fb) for compounds generated using VIKOR, TOPSIS, and Pareto pruning in the ciprofloxacin molecular optimization.</p>
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<p>Histogram showing the distribution of 3D similarity (Sim3D) for compounds generated using VIKOR, TOPSIS, and Pareto pruning in ciprofloxacin molecular optimization. For each pruning scheme, the data were narrowed down to the top 500 compounds with respect to the %Fb objective. This enables a quantitative estimation of the quality of the trade-offs made by each pruning scheme.</p>
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<p>Predicted plasma concentration curves for ciprofloxacin (orange) and the optimized compound (blue). The molecular optimization, supported by the VIKOR pruning scheme, resulted in a structure with significantly improved pharmacokinetic (PK) characteristics while retaining the key structural features of ciprofloxacin.</p>
Full article ">
12 pages, 2636 KiB  
Article
MoTe2 Photodetector for Integrated Lithium Niobate Photonics
by Qiaonan Dong, Xinxing Sun, Lang Gao, Yong Zheng, Rongbo Wu and Ya Cheng
Nanomaterials 2025, 15(1), 72; https://doi.org/10.3390/nano15010072 - 5 Jan 2025
Viewed by 275
Abstract
The integration of a photodetector that converts optical signals into electrical signals is essential for scalable integrated lithium niobate photonics. Two-dimensional materials provide a potential high-efficiency on-chip detection capability. Here, we demonstrate an efficient on-chip photodetector based on a few layers of MoTe [...] Read more.
The integration of a photodetector that converts optical signals into electrical signals is essential for scalable integrated lithium niobate photonics. Two-dimensional materials provide a potential high-efficiency on-chip detection capability. Here, we demonstrate an efficient on-chip photodetector based on a few layers of MoTe2 on a thin film lithium niobate waveguide and integrate it with a microresonator operating in an optical telecommunication band. The lithium-niobate-on-insulator waveguides and micro-ring resonator are fabricated using the femtosecond laser photolithography-assisted chemical–mechanical etching method. The lithium niobate waveguide-integrated MoTe2 presents an absorption coefficient of 72% and a transmission loss of 0.27 dB µm−1 at 1550 nm. The on-chip photodetector exhibits a responsivity of 1 mA W−1 at a bias voltage of 20 V, a low dark current of 1.6 nA, and a photo–dark current ratio of 108 W−1. Due to effective waveguide coupling and interaction with MoTe2, the generated photocurrent is approximately 160 times higher than that of free-space light irradiation. Furthermore, we demonstrate a wavelength-selective photonic device by integrating the photodetector and micro-ring resonator with a quality factor of 104 on the same chip, suggesting potential applications in the field of on-chip spectrometers and biosensors. Full article
(This article belongs to the Section Nanofabrication and Nanomanufacturing)
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Figure 1
<p>(<b>a</b>) Schematic diagram of the MoTe<sub>2</sub>-based on-chip photodetector. (<b>b</b>) Raman spectrum of 2H-MoTe<sub>2</sub> (20 layers) on the LNOI platform under 532 nm laser excitation. Insert schematic of the MoTe<sub>2</sub> structure: Mo (purple) and Te (yellow), the arrows indicate the direction of atom vibration. (<b>c</b>) AFM image of 2H-MoTe<sub>2</sub> covering the LNOI waveguide (WG). (<b>d</b>) The thickness of the 2H-MoTe<sub>2</sub> layer corresponds to the region of the solid line (red color) marked in (<b>c</b>).</p>
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<p>Simulation of the light field distribution in the LNOI waveguide without 2H-MoTe<sub>2</sub> (<b>a</b>) and with 2H-MoTe<sub>2</sub> (<b>b</b>). (<b>c</b>) The simulation of the electric field intensity |E<sup>2</sup>| in the coupling section for TE polarization. (<b>d</b>) Measured transmission loss of the waveguide without and with 2H-MoTe<sub>2</sub>.</p>
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<p>(<b>a</b>) Schematic band diagrams of the Au-2H-MoTe<sub>2</sub>-Au structure: (<b>top</b>) in thermal equilibrium; (<b>bottom</b>) under illumination and applied bias voltage. (<b>b</b>) Comparison of the I-V curves under dark and in-coupled light intensity with 190 μW. (<b>c</b>) I–V curves at varying light intensities. (<b>d</b>) Photocurrent as a function of light intensity within the waveguide at different bias voltages. (<b>e</b>) Responsivity and EQE as functions of bias voltage. (<b>f</b>) Impulse response curve of the photodetector.</p>
Full article ">Figure 4
<p>(<b>a</b>) I–V curves at a constant in-coupled light intensity of 300 μW with different wavelengths. (<b>b</b>) Comparison of the responsivity of the photodetector under in-coupled light via waveguide and spatial illumination. (<b>c</b>) Simulated absorption rate of 2H-MoTe<sub>2</sub> at varying thicknesses. (<b>d</b>) 2H-MoTe<sub>2</sub> thickness-dependent responsivity of on-chip photodetectors.</p>
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<p>(<b>a</b>) Schematic diagram of the PD on a waveguide-coupled ring resonant cavity, the arrows indicate the direction of light propagation. (<b>b</b>) Optical micrograph of the micro-ring resonator (MRR) and the corresponding waveguide-integrated photodetector. (<b>c</b>) Output energy of the waveguide with and without 2H-MoTe<sub>2</sub>. (<b>d</b>) Comparison of transmission spectrum measured using commercial detectors and photocurrent measured using on-chip integrated PD, and Lorentz fitting curve.</p>
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13 pages, 1052 KiB  
Article
Physico-Chemical Characteristics of Rosa canina L. Seeds and Determining Their Potential Use
by Małgorzata Stryjecka, Anna Kiełtyka-Dadasiewicz and Monika Michalak
Appl. Sci. 2025, 15(1), 168; https://doi.org/10.3390/app15010168 - 28 Dec 2024
Viewed by 350
Abstract
Rosa canina is well-known plant, and its fruits have been used for centuries. The seeds have been less utilized and remain untested. The objective of this study was to examine the physico-chemical properties of rosehip seeds and to identify potential applications based on [...] Read more.
Rosa canina is well-known plant, and its fruits have been used for centuries. The seeds have been less utilized and remain untested. The objective of this study was to examine the physico-chemical properties of rosehip seeds and to identify potential applications based on their properties. The physico-chemical properties of the seeds were determined, including swelling index (2.51), color in the CIE L * a * b * space (b * = 26.2), as well as carbohydrate (79.2 g/100 g), soluble dietary fiber (71.6 g/100 g), protein (7.67 g/100 g), fat (6.23 g/100 g), and ash (1.96 g/100 g) content. Among the amino acids, glutamic acid dominated (1.58 mg/100 g), while among the fatty acids, linoleic acid (53.19%), linolenic acid (20.24%), and oleic acid (17.63%) were the most dominant. In addition, rosehip seeds contained large amounts of calcium (3851 mg/kg), potassium (2732 mg/kg), and phosphorus (991 mg/kg), as well as vitamin C (1783 μg/g). It was found that the content of other valuable phytochemicals, such as phenolic compounds (2633 μg/g) and carotenoids (3.13 μg/g) influenced the antioxidant properties of the tested raw material. This activity examined by the ferric-reducing antioxidant power (FRAP) and DPPH radical scavenging activity methods was assessed at a level of 191 and 229 μmol TE/g, respectively. The results indicate the potential use of rosehip seed, a by-product of the food processing industry, as a new high-value ingredient for health products, such as nutraceuticals, pharmaceuticals, and cosmeceuticals. Full article
(This article belongs to the Special Issue Advances in Bioactive Compounds from Plants and Their Applications)
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<p>Diagram of a rosehip fruit with a cross-section showing the seeds (drawn by Małgorzata Gorzel).</p>
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<p>Rosehip seeds used for research (photographed by Marcin Dadasiewicz).</p>
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21 pages, 6120 KiB  
Communication
Identifying Crystal Structure of Halides of Strontium and Barium Perovskite Compounds with EXPO2014 Software
by Jorge A. Perez Franco, Antonieta García Murillo, Felipe de J. Carrillo Romo, Issis C. Romero Ibarra and Arturo Cervantes Tobón
Materials 2025, 18(1), 58; https://doi.org/10.3390/ma18010058 - 26 Dec 2024
Viewed by 392
Abstract
The synthesis of ethylamine-based perovskites has emerged to attempt to replace the lead in lead-based perovskites for the alkaline earth elements barium and strontium, introducing chloride halide to prepare the perovskites in solar cell technology. X-ray diffraction studies were conducted, and EXPO2014 software [...] Read more.
The synthesis of ethylamine-based perovskites has emerged to attempt to replace the lead in lead-based perovskites for the alkaline earth elements barium and strontium, introducing chloride halide to prepare the perovskites in solar cell technology. X-ray diffraction studies were conducted, and EXPO2014 software was utilized to resolve the structure. Chemical characterization was performed using Fourier transform infrared spectroscopy, photophysical properties were analyzed through ultraviolet–visible spectroscopy, and photoluminescence properties were determined to confirm the perovskite characteristics. The software employed can determine new crystal structures, as follows: orthorhombic for barium perovskite CH3CH2NH3BaCl3 and tetragonal for strontium perovskite CH3CH2NH3SrCl3. The ultraviolet–visible spectroscopy data demonstrated that a temperature increase (90–110 °C) contributed to reducing the band gap from 3.93 eV to 3.67 eV for barium perovskite and from 4.05 eV to 3.84 eV for strontium perovskite. The results exhibited that new materials can be obtained through gentle chemistry and specialized software like EXPO2014, both of which are capable of conducting reciprocal and direct space analyses for identifying crystal structures using powder X-ray diffraction. Full article
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Graphical abstract

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<p>Steps for synthesizing the strontium and barium ethylamine chloride perovskites.</p>
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<p>Crystal structure visualization by EXPO2014 of barium perovskite (CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>BaCl<sub>3</sub>) at different temperatures: (<b>a</b>) at 90 °C, (<b>b</b>) at 100 °C, and (<b>c</b>) at 110 °C, with an orthorhombic structure. The structural models shown were drawn with VESTA software (Ver. 3.5.8).</p>
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<p>Crystal structure visualization by EXPO2014 of strontium perovskite (CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>SrCl<sub>3</sub>) at different temperatures: (<b>a</b>) at 90 °C, (<b>b</b>) at 100 °C, and (<b>c</b>) at 110 °C, with a tetragonal structure. The structural models shown were drawn with VESTA software.</p>
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<p>Experimental X-ray powder diffraction pattern of barium perovskite with an orthorhombic structure at 90, 100, and 110 °C.</p>
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<p>Experimental X-ray powder diffraction pattern of strontium perovskite with a tetragonal structure at 90, 100, and 110 °C.</p>
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<p>FTIR spectra for the barium perovskites (CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>BaCl<sub>3</sub>) at different temperatures.</p>
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<p>FTIR spectra for the strontium perovskites (CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>SrCl<sub>3</sub>) at different temperatures.</p>
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<p>Absorption spectra of CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>BaCl<sub>3</sub> at 90, 100, and 110 °C.</p>
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<p>Absorption spectra of CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>SrCl<sub>3</sub> at 90, 100, and 110 °C.</p>
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<p>PL emission spectra of CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>BaCl<sub>3</sub> at 90, 100, and 110 °C.</p>
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<p>PL emission spectra of CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>SrCl<sub>3</sub> at 90, 100, and 110 °C.</p>
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<p>Normalized UV–Visible spectra of CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>BaCl<sub>3</sub> perovskite at 90, 100, and 110 °C. Inset: corresponding Tauc plots.</p>
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<p>Normalized UV–Visible spectra of CH<sub>3</sub>CH<sub>2</sub>NH<sub>3</sub>SrCl<sub>3</sub> perovskite at 90, 100, and 110 °C. Inset: corresponding Tauc plots.</p>
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<p>Band gap structure and energy levels of barium perovskite.</p>
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<p>Band gap structure and energy levels of strontium perovskite.</p>
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16 pages, 2405 KiB  
Article
Generation of Rational Drug-like Molecular Structures Through a Multiple-Objective Reinforcement Learning Framework
by Xiangying Zhang, Haotian Gao, Yifei Qi, Yan Li and Renxiao Wang
Molecules 2025, 30(1), 18; https://doi.org/10.3390/molecules30010018 - 24 Dec 2024
Viewed by 395
Abstract
As an appealing approach for discovering novel leads, the key advantage of de novo drug design lies in its ability to explore a much broader dimension of chemical space, without being confined to the knowledge of existing compounds. So far, many generative models [...] Read more.
As an appealing approach for discovering novel leads, the key advantage of de novo drug design lies in its ability to explore a much broader dimension of chemical space, without being confined to the knowledge of existing compounds. So far, many generative models have been described in the literature, which have completely redefined the concept of de novo drug design. However, many of them lack practical value for real-world drug discovery. In this work, we have developed a graph-based generative model within a reinforcement learning framework, namely, METEOR (Molecular Exploration Through multiplE-Objective Reinforcement). The backend agent of METEOR is based on the well-established GCPN model. To ensure the overall quality of the generated molecular graphs, we implemented a set of rules to identify and exclude undesired substructures. Importantly, METEOR is designed to conduct multi-objective optimization, i.e., simultaneously optimizing binding affinity, drug-likeness, and synthetic accessibility of the generated molecules under the guidance of a special reward function. We demonstrate in a specific test case that without prior knowledge of true binders to the chosen target protein, METEOR generated molecules with superior properties compared to those in the ZINC 250k data set. In conclusion, we have demonstrated the potential of METEOR as a practical tool for generating rational drug-like molecules in the early phase of drug discovery. Full article
(This article belongs to the Special Issue Computational Approaches in Drug Discovery and Design)
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<p>UMAP projection of the ZINC 250k molecules (grey) and those generated by DFM (blue) and GCPN<sub>ours</sub> (green), respectively. This plot illustrates the similarity between the chemical spaces covered by different generative models.</p>
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<p>Distribution of three desired features and the unweighted sum of rewards of the molecules generated at the last round of reinforcement learning (red lines: METEOR<sub>GCPN</sub>; blue lines: METEOR<sub>DFM</sub>; green lines: ZINC 250k).</p>
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<p>Several key features of METEOR<sub>DFM</sub> (<b>left</b>) and METEOR<sub>GCPN</sub> (<b>right</b>) observed during the reinforcement learning process. (<b>a</b>,<b>b</b>): Three property rewards; (<b>c</b>,<b>d</b>): Total and unpenalized rewards; (<b>e</b>,<b>f</b>): Three penalty factors. Here, each line plots the mean value of a certain feature computed over all molecules generated at each round of roll-out.</p>
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<p>UMAP projections of 50,000 ZINC 250k molecules (grey) and 50,000 molecules generated at certain rounds by METEOR<sub>DFM</sub> (blue) and METEOR<sub>GCPN</sub> (green), respectively. Different rounds are indicated in colors with different shades.</p>
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<p>Examples of the molecules generated by METEOR<sub>DFM</sub> and METEOR<sub>GCPN</sub> as well as the corresponding true binders of GBA.</p>
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<p>Distribution of the GLIDE docking scores computed for several sets of molecules: ZINC 250k molecules (<span class="html-italic">n</span> = 247168, green), METEOR<sub>DFM</sub> molecules (<span class="html-italic">n</span> = 279910, blue), and METEOR<sub>GCPN</sub> molecules (<span class="html-italic">n</span> = 739130, red).</p>
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<p>Illustration of graph generation process for the aspirin molecule by GCPN (<b>top</b>), DFM (<b>bottom left</b>, in a depth-first manner), and BFM (<b>bottom right</b>, in a breadth-first manner). At each step, the end atoms of new bonds are marked in red, possible focus atoms are marked in blue, and “finished atoms” are depicted in black.</p>
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17 pages, 11037 KiB  
Article
Rapid Fluid Velocity Field Prediction in Microfluidic Mixers via Nine Grid Network Model
by Qian Li, Yuwei Chen, Taotao Sun and Junchao Wang
Micromachines 2025, 16(1), 5; https://doi.org/10.3390/mi16010005 - 24 Dec 2024
Viewed by 384
Abstract
The rapid advancement of artificial intelligence is transforming the computer-aided design of microfluidic chips. As a key component, microfluidic mixers are widely used in bioengineering, chemical experiments, and medical diagnostics due to their efficient mixing capabilities. Traditionally, the simulation of these mixers relies [...] Read more.
The rapid advancement of artificial intelligence is transforming the computer-aided design of microfluidic chips. As a key component, microfluidic mixers are widely used in bioengineering, chemical experiments, and medical diagnostics due to their efficient mixing capabilities. Traditionally, the simulation of these mixers relies on the finite element method (FEM), which, although effective, presents challenges due to its computational complexity and time-consuming nature. To address this, we propose a nine-grid network (NGN) model theory with a centrally symmetric structure.The NGN uses a symmetric structure similar to a 3 × 3 grid to partition the fluid space to be predicted. Using this theory, we developed and trained an artificial neural network (ANN) to predict the fluid dynamics within microfluidic mixers. This approach significantly reduces the time required for fluid evaluation. In this study, we designed a prototype microfluidic mixer and validated the reliability of our method by comparing it with predictions from traditional FEM software. The results show that our NGN model completes fluid predictions in just 40 s compared to approximately 10 min with FEM, with acceptable error margins. This technology achieves a 15-fold acceleration, greatly reducing the time and cost of microfluidic chip design. Full article
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<p>Introduction and usage example of nine-grid network model. (<b>A</b>) Meshing of microfluidic mixer. (<b>B</b>) ANN libarary. (<b>C</b>) Dataset structure. (<b>D</b>) Example input and output for the ANN_569 model. (<b>E</b>) An example of predicting the fluid field of the target system using the nine-gride network model.</p>
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<p>(<b>A</b>) The geometric structure diagram of a microfluidic mixer, which has two inlets, two outlets, and a 500 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m × 500 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m reaction zone. (<b>B</b>) An example shows the fluid velocity field predicted by the FEM of a randomly generated mixer.</p>
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<p>The design process of a random microfluidic mixer. Within a month, 10,000 random microfluidic mixer chip designs were generated using MATLAB R2020b programs, and the performance of each chip was simulated using COMSOL <math display="inline"><semantics> <mrow> <mn>5.5</mn> </mrow> </semantics></math>. Finally, the results were saved in a MySQL <math display="inline"><semantics> <mrow> <mn>5.7</mn> <mo>.</mo> <mn>16</mn> </mrow> </semantics></math> database.</p>
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<p>(<b>A</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> of ANN_6 during 6000 epochs. (<b>B</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> of ANN_6 during 6000 epochs. (<b>C</b>) The histogram of the absolute error of <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> of 185,337 items in the test set. (<b>D</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> of ANN_8 during 6000 epochs. (<b>E</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> of ANN_8 during 6000 epochs. (<b>F</b>) The histogram of the absolute error of <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> of 185,337 items in the test set. (<b>G</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of ANN_9 during 6000 epochs. (<b>H</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of ANN_9 during 6000 epochs. (<b>I</b>) The histogram of the absolute error of <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of 185,337 items in the test set.</p>
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<p>(<b>A</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> of ANN_69 during 8000 epochs. (<b>B</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> of ANN_69 during 8000 epochs. (<b>C</b>) The histogram of the absolute error of <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> of 157,763 items in the test set. (<b>D</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of ANN_69 during 8000 epochs. (<b>E</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of ANN_69 during 8000 epochs. (<b>F</b>) The histogram of the absolute error of <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of 157,763 items in the test set.</p>
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<p>(<b>A</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> of ANN_89 during 8000 epochs. (<b>B</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> of ANN_89 during 8000 epochs. (<b>C</b>) The histogram of the absolute error of <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>8</mn> </mrow> </msub> </semantics></math> of 156,774 items in the test set. (<b>D</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of ANN_89 during 8000 epochs. (<b>E</b>) The training curve of the <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of ANN_89 during 8000 epochs. (<b>F</b>) The histogram of the absolute error of <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>x</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>y</mi> <mo>,</mo> <mn>9</mn> </mrow> </msub> </semantics></math> of 156,774 items in the test set.</p>
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<p>The step of predicting fluid velocity field of the microfluidic chip using ANN Tool.</p>
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<p>The velocity distribution in the reaction zone was predicted by COMSOL and ANN methods. The corresponding SSIM values between the two methods are listed for quantitative analysis.</p>
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<p>The COMSOL and ANN methods were used to predict the velocity distribution of 500 new microfluidic chip reaction zones, and the distribution of the corresponding SSIM values between the two methods was calculated.</p>
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<p>The SSIM for <math display="inline"><semantics> <msub> <mi>v</mi> <mi>x</mi> </msub> </semantics></math> is 0.7646, the SSIM for <math display="inline"><semantics> <msub> <mi>v</mi> <mi>y</mi> </msub> </semantics></math> is 0.7597, and the SSIM for the total velocity is 0.6459.</p>
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<p>The SSIM for <math display="inline"><semantics> <msub> <mi>v</mi> <mi>x</mi> </msub> </semantics></math> is 0.5494, the SSIM for <math display="inline"><semantics> <msub> <mi>v</mi> <mi>y</mi> </msub> </semantics></math> is 0.5489, and the SSIM for the total velocity is 0.5507.</p>
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<p>The SSIM for <math display="inline"><semantics> <msub> <mi>v</mi> <mi>x</mi> </msub> </semantics></math> is 0.5497, the SSIM for <math display="inline"><semantics> <msub> <mi>v</mi> <mi>y</mi> </msub> </semantics></math> is 0.5496, and the SSIM for the total velocity is 0.5227.</p>
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10 pages, 1262 KiB  
Perspective
Microbiota-Induced Radioprotection: A Novel Approach to Enhance Human Radioresistance with In-Situ Genetically Engineered Gut Bacteria
by Anna O. Yakimova, Anastasiia Nikolaeva, Olesya Galanova, Victoria A. Shestakova, Ekaterina I. Smirnova, Alina Levushkina, Denis S. Baranovskii, Anna N. Smirnova, Vasiliy N. Stepanenko, Dmitry A. Kudlay, Peter V. Shegay, Andrey D. Kaprin, Dmitry V. Sosin and Ilya D. Klabukov
Appl. Microbiol. 2025, 5(1), 1; https://doi.org/10.3390/applmicrobiol5010001 - 24 Dec 2024
Viewed by 559
Abstract
The high sensitivity of living organic forms to space radiation remains the critical issue during spaceflight, to which they will be chronically exposed during months of interplanetary or even decades of interstellar spaceflight. In the human body, all actively dividing and poorly differentiated [...] Read more.
The high sensitivity of living organic forms to space radiation remains the critical issue during spaceflight, to which they will be chronically exposed during months of interplanetary or even decades of interstellar spaceflight. In the human body, all actively dividing and poorly differentiated cells are always close to being damaged by radiological or chemical agents. The chronic exposure to ionizing radiation primarily causes changes in blood counts and intestinal damage such as fibrosis, obliterative vasculitis, changes in the gut microbiota, and atrophy or degeneration of muscle fibers. The project “MISS: Microbiome Induced Space Suit” was presented at the Giant Jamboree of the International Genetically Engineered Machine Competition 2021, with the aim to investigate the ability of the novel microbiota-mediated approach to enhance human resistance to ionizing radiation. The key innovative part of the project was the idea to create a novel radioprotector delivery mechanism based on human gut microbiota with the function of outer membrane vesicles (OMVs) secretion. The project concept proposed the feasibility of genetically modifying the human microbiota in situ through the delivery of genetic constructs to the host’s crypts using silicon nanoparticles with chemically modified surfaces. In this perspective, we discuss the advances in modifying microbiota-mediated secretory activity as a promising approach for radioprotection and as an alternative to hormone therapy and other health conditions that currently require continuous drug administration. Future clinical trials of in situ methods to genetic engineering the crypt microbiota may pave the way for indirect regulation of human cells. Full article
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Figure 1
<p>Bacterial-mediated Radioprotector Probiotics modulate the radioprotection of intestinal cells through the transport of bacterial outer membrane vesicles (OMVs) containing recombinant biomolecules into human cells. Created with <a href="http://Biorender.com" target="_blank">Biorender.com</a>.</p>
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<p>(<b>A</b>)—The concept of the Microbiota-Induced Space Suit project; (<b>B</b>)—Pathway of OMVs-mediated radioprotector delivery into intestine crypt cells through gene-engineered microbiota. Created with <a href="http://Biorender.com" target="_blank">Biorender.com</a>.</p>
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33 pages, 7655 KiB  
Article
Silanization of Starch and Its Effect on Cross-Linking and Mechanical, Dynamic, Hydrophobic, and Aging Properties of Polymeric Compositions Containing Natural Rubber
by Konrad Mrozowski and Aleksandra Smejda-Krzewicka
Materials 2024, 17(24), 6273; https://doi.org/10.3390/ma17246273 - 22 Dec 2024
Viewed by 477
Abstract
In recent years, the search for more sustainable fillers for elastomeric composites than silica and carbon black has been underway. In this work, silanized starch was used as an innovative filler for elastomeric composites. Corn starch was chemically modified by silanization (with n-octadecyltrimethoxysilane) [...] Read more.
In recent years, the search for more sustainable fillers for elastomeric composites than silica and carbon black has been underway. In this work, silanized starch was used as an innovative filler for elastomeric composites. Corn starch was chemically modified by silanization (with n-octadecyltrimethoxysilane) via a condensation reaction to produce a hydrophobic starch. Starch/natural rubber composites were prepared by mixing the modified starch with elastomer. The morphology, hydrophobicity, and chemical structure of starch after and before modification were studied. The results showed that starch after silanization becomes hydrophobic (θw = 117.3°) with a smaller particle size. In addition, FT-IR spectrum analysis confirmed the attachment of silane groups to the starch. The modified starch dispersed better in the natural rubber matrix and obtained a more homogeneous morphology. The composite achieved the best dynamic (ΔG′ = 203.8 kPa) and mechanical properties (TSb = 11.4 MPa) for compositions with 15 phr of modified starch. In addition, the incorporation of silanized starch improved the hydrophobicity of the composite (θw = 117.8°). The higher starch content allowed the composites to achieve a higher degree of cross-linking, resulting in better resistance to swelling in organic solvents. This improvement is due to enhanced elastomer–filler interactions and reduced spaces that prevent solvent penetration into the material’s depths. The improved mechanical properties and good dynamic properties, as well as improved hydrophobicity, were mainly due to improved interfacial interactions between rubber and starch. This study highlights the potential and new approach of silane-modified starch as a sustainable filler, demonstrating its ability to enhance the mechanical, dynamic, and hydrophobic properties of elastomeric composites while supporting greener material solutions for the rubber industry. Full article
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<p>Common hydrophobic chemical modifications of starch.</p>
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<p>Scheme of corn starch silanization process.</p>
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<p>Flowchart of the order of the testing procedure.</p>
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<p>FT-IR spectra of modified and unmodified starch.</p>
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<p>SEM images of native corn starch (<b>a</b>–<b>c</b>) and silanized starch (<b>d</b>–<b>f</b>) at different magnifications: (<b>a</b>,<b>d</b>) 100×, (<b>b</b>,<b>e</b>) 1000×, (<b>c</b>,<b>f</b>) 5000×.</p>
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<p>Profile of water droplet, diiodomethane, and glycol ethylene on NCS and CS/OTMS pellets (θ<sub>W</sub>—water contact angle; θ<sub>D</sub>—diiodomethane contact angle; θ<sub>G</sub>—glycol ethylene contact angle).</p>
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<p>Impact of modification on surface free energy and water contact angle.</p>
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<p>SEM images of natural rubber composites: (<b>a</b>,<b>b</b>) natural rubber without corn starch, (<b>c</b>,<b>d</b>) containing 15 phr of native corn starch, and (<b>e</b>,<b>f</b>) silanized corn starch ((<b>a</b>,<b>c</b>,<b>e</b>)—magnification 500×; (<b>b</b>,<b>d</b>,<b>f</b>)—magnification 5000×).</p>
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<p>Vulcanization curves for tested NR composites filled with corn starch at T = 160 °C.</p>
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<p>Comparison of mechanical properties before and after aging of the tested NR composites (cross-linked at T = 160 °C for t = 5 min): (<b>a</b>) stress at 100% elongation; (<b>b</b>) tensile strength; (<b>c</b>) aging factor; (<b>d</b>) stress–strain chart for NR0, NR15S, and NR15M.</p>
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<p>Effect of corn starch amount and modification on the hardness of NR composites (cross-linked at T = 160 °C for t = 5 min).</p>
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<p>(<b>a</b>) Comparison of hysteresis loss values during first stretching cycle and Mullins effect values of tested NR samples, (<b>b</b>) NR0 stress–strain hysteresis chart, (<b>c</b>) NR15S stress–strain hysteresis chart, (<b>d</b>) NR15M stress–strain hysteresis chart (cross-linked at T = 160 °C for t = 5 min).</p>
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<p>Effect of modified corn starch on dynamic properties of NR composites (cross-linked at T = 160 °C for t = 5 min): (<b>a</b>) storage modulus, (<b>b</b>) magnifying storage modulus, (<b>c</b>) Payne effect.</p>
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<p>Effect of chemically and in situ silanized starch on tested NR composites loss tangent.</p>
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<p>Comparison of water contact angles of the tested NR compositions (cross-linked at T = 160 °C for t = 5 min). Letters above determination of samples indicate statistically homogeneous subsets (Tukey’s HSD test, α = 0.05); ANOVA F = 50.8, <span class="html-italic">p</span> &lt; 0.001.</p>
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<p>Influence of modified corn starch on the contact angle values of water, diiodomethane, and ethyl glycol (θ<sub>W</sub>—water contact angle; θ<sub>D</sub>—diiodomethane contact angle; θ<sub>G</sub>—glycol ethylene contact angle).</p>
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<p>Impact of modified corn starch on surface free energy parameters: (<b>a</b>) total, (<b>b</b>) dispersive, and (<b>c</b>) polar components.</p>
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18 pages, 4581 KiB  
Article
A Design-Oriented Model for Transmission Loss Optimization in Marine DOCs
by Jan Kašpar, Francesco Mauro, Marco Biot, Giovanni Rognoni and Giada Kyaw Oo D’Amore
J. Mar. Sci. Eng. 2024, 12(12), 2358; https://doi.org/10.3390/jmse12122358 - 22 Dec 2024
Viewed by 379
Abstract
The even more restrictive regulations imposed on chemical and acoustic emissions of ships necessitate the installation of after-treatment systems onboard. The spaces onboard are limited, and the Exhaust Gas Cleaning Systems (EGCSs) have big dimensions, so an appropriate integration and optimization of EGCSs [...] Read more.
The even more restrictive regulations imposed on chemical and acoustic emissions of ships necessitate the installation of after-treatment systems onboard. The spaces onboard are limited, and the Exhaust Gas Cleaning Systems (EGCSs) have big dimensions, so an appropriate integration and optimization of EGCSs allows to save space and comply with international regulations. Moreover, in the available literature, there is a lack of guidelines about the design of integrated EGCSs. This study aims to develop an ad hoc optimization methodology that uses combined Computational Fluid Dynamics (CFD)–Finite Element Method (FEM) simulations, surrogate models, and Genetic Algorithms to optimize the acoustic properties of EGCSs while considering the limits imposed by the efficiency of chemical reactions for the abatement of NOx and SOx. The developed methodology is applied to a Diesel Oxidation Catalyst (DOC), and the obtained results lead to a system that integrates the silencing effect into the DOC. Full article
(This article belongs to the Special Issue Novel Maritime Techniques and Technologies, and Their Safety)
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<p>GA main steps.</p>
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<p>Workflow of the combined CFD–FEM methodology.</p>
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<p>Mesh sensitivity study.</p>
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<p>Schematics of the DOC converter with a picture of the metallic honeycomb featuring narrow sinusoidal-shaped channels.</p>
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<p>Experimental mock-up (upper figure) and scheme of the experimental set-up for the TL calculations with the two-load technique (lower figure).</p>
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<p>Experimental vs. numerical TL of the DOC. The EFR and related harmonics are also shown in the figure.</p>
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<p>DOC dimensions used as predictor variables.</p>
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<p>Construction of design space: multidimensional combination and interaction of the predictor parameters and their constraints.</p>
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<p>Convergence history of the Genetic Algorithm.</p>
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<p>Geometry of the reference and optimized DOC.</p>
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<p>Comparison between the optimized and reference TL. The EFR and related harmonics are also shown in the figure.</p>
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<p>Velocity field in the optimized DOC calculated with CFD.</p>
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21 pages, 10983 KiB  
Review
Machine Learning Advances in High-Entropy Alloys: A Mini-Review
by Yibo Sun and Jun Ni
Entropy 2024, 26(12), 1119; https://doi.org/10.3390/e26121119 - 20 Dec 2024
Viewed by 423
Abstract
The efficacy of machine learning has increased exponentially over the past decade. The utilization of machine learning to predict and design materials has become a pivotal tool for accelerating materials development. High-entropy alloys are particularly intriguing candidates for exemplifying the potency of machine [...] Read more.
The efficacy of machine learning has increased exponentially over the past decade. The utilization of machine learning to predict and design materials has become a pivotal tool for accelerating materials development. High-entropy alloys are particularly intriguing candidates for exemplifying the potency of machine learning due to their superior mechanical properties, vast compositional space, and intricate chemical interactions. This review examines the general process of developing machine learning models. The advances and new algorithms of machine learning in the field of high-entropy alloys are presented in each part of the process. These advances are based on both improvements in computer algorithms and physical representations that focus on the unique ordering properties of high-entropy alloys. We also show the results of generative models, data augmentation, and transfer learning in high-entropy alloys and conclude with a summary of the challenges still faced in machine learning high-entropy alloys today. Full article
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<p>HEAs phase classification using SISSO descriptors as coordinates in Ref. [<a href="#B81-entropy-26-01119" class="html-bibr">81</a>]: (<b>a</b>) Classification of crystal and amorphous (AM). (<b>b</b>) Classification of intermetallic (IM) and solid solution (SS). (<b>c</b>) Classification of single-phase (BCC or FCC) and multi-phase (BCC and FCC). (<b>d</b>) Classification of BCC and FCC.</p>
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<p>Correlation and similarity between HEA materials obtained using HEA interaction network in Ref. [<a href="#B96-entropy-26-01119" class="html-bibr">96</a>].</p>
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<p>The framework of the ECNet model in Ref. [<a href="#B97-entropy-26-01119" class="html-bibr">97</a>]: The embedding layer serves the function of encoding the initial inputs derived from the atomic numbers. In the interaction block, a series of neural networks is employed for the purpose of transforming the crystal structures into atomic attributes. The elemental convolution operation entails the computation of the mean value of the atom-wise features, classified according to the atomic element type.</p>
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<p>Ternary diagrams predicted by the ECNet in Ref. [<a href="#B97-entropy-26-01119" class="html-bibr">97</a>]: (<b>a</b>) formation free energies in FeCoMn system; (<b>b</b>) magnetic moments in FeCoMn system; (<b>c</b>) formation free energies in FeCoPd system; (<b>d</b>) magnetic moments in FeCoPd system. Areas I, II, III represent the stability of alloys from high to low.</p>
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<p>Feature visualization using the t-SNE algorithm in Ref. [<a href="#B123-entropy-26-01119" class="html-bibr">123</a>]. The model in Ref. [<a href="#B123-entropy-26-01119" class="html-bibr">123</a>] contains a total of five hidden layers. The original inputs to the model and the output results of the five hidden layers are visualized as two-dimensional distributions using the t-SNE algorithm, respectively. The color of the points represents the phase of the alloys: blue, solid solution; red, mixed phase of solid solution and intermetallic; green, intermetallic; yellow, amorphous.</p>
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<p>Analysis of model interpretation in Ref. [<a href="#B124-entropy-26-01119" class="html-bibr">124</a>]: (<b>a</b>) the contributions of descriptors for BCC phase in the NbTaTiV system; (<b>b</b>) phase predictions when there is only one descriptor change. Line colors denote phase information: blue, mixed phases; violet, AM; cyan, FCC; orange, BCC + FCC; light blue, HCP; red, BCC; green, IM.</p>
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<p>Algorithm process and generated results in Ref. [<a href="#B128-entropy-26-01119" class="html-bibr">128</a>]: VAE and ANN work together to ensure the effectiveness of generating eutectic alloys; possible eutectic alloy components are generated by machine learning and experimentally verified.</p>
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<p>Algorithm process in Ref. [<a href="#B75-entropy-26-01119" class="html-bibr">75</a>]: (<b>a</b>) Mapping the chemical formula of materials to a two-dimensional representation that employs the periodic table structure. (<b>b</b>) Network structures of the model, containing the transferable feature extractor and separately trained regressor or classifier.</p>
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19 pages, 4401 KiB  
Article
Advanced Analysis of Clay Microporosity Using High-Resolution N2-Ar Adsorption Isotherms Coupled with the Derivative Isotherm Summation Method
by Anwar El Azrak, Denys I. Grekov, Laurent Truche and Pascaline Pré
Molecules 2024, 29(24), 6019; https://doi.org/10.3390/molecules29246019 - 20 Dec 2024
Viewed by 374
Abstract
The textural properties of synthetic and natural clays in the sodium form and exchanged with tetramethylammonium cations (TMA+) were characterized using N2 and Ar physisorption isotherms at cryogenic temperatures. Specific surface areas and micro/mesoporous volumes were determined using the BET [...] Read more.
The textural properties of synthetic and natural clays in the sodium form and exchanged with tetramethylammonium cations (TMA+) were characterized using N2 and Ar physisorption isotherms at cryogenic temperatures. Specific surface areas and micro/mesoporous volumes were determined using the BET and the t-plot models. The t-plot analysis requires the use of reference isotherms measured at the same temperature on the surface of non-porous materials with an identical chemical composition. In order to better assess the effects of chemical heterogeneities in the clay particles, reference isotherms representative of silica surfaces were taken into account in the analysis of the t-curve and corrected to account for variations in curvature at the interface of the film adsorbed in the micropores. In addition, high-resolution Ar adsorption isotherms at 87 K were analyzed using the Derivative Isotherm Summation (DIS) method to quantify the energy contributions of adsorption sites and determine the fractions of basal and lateral surfaces of clay particles. The high-energy adsorption sites, identified in the low-pressure range, were attributed to intra-particle microporosity due to stacking defects and/or open inter-layer spaces. These sites were differentiated from those on the lateral and basal surfaces of the particles. A modification of the DIS method was proposed to measure these contributions and improve the fit with the experimental data. The results show that TMA+ cation exchange significantly increases the microporosity of clays compared to their sodic form, which can be attributed to the increased contribution of intra-particle adsorption sites due to interlayer expansion. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Physical Chemistry, 2nd Edition)
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<p>Key characteristics of clay texture at the particle scale.</p>
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<p>Theoretical surface areas of ordered clay crystallite as a function of dimensions of phyllosilicate sheets (<span class="html-italic">d</span>) and their stacking number (<span class="html-italic">n</span>) changing from 1 to 100.</p>
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<p>Nitrogen adsorption and desorption isotherms at 77 K for natural (upper) and synthetic (lower) clays exchanged with Na<sup>+</sup> and TMA<sup>+</sup>.</p>
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<p>Ar adsorption isotherms (<b>left</b>) and their derivatives (<b>right</b>) at 77 K and 87 K for IdP-Na. The symbols in the form of circles and triangles correspond to two different series to evaluate the reproducibility of the results.</p>
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<p>Raw Ar adsorption isotherms (<b>top</b>) and their derivatives (<b>bottom</b>) for SA-Na (<b>left</b>) and SA-TMA materials (<b>right</b>) at 77 K and 87 K. The symbols in the form of circles and asterisks correspond to two different series to evaluate the data reproducibility.</p>
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<p>Raw Ar adsorption isotherms (<b>top</b>) and their derivatives (<b>bottom</b>) for SA-Na (<b>left</b>) and SA-TMA materials (<b>right</b>) at 77 K and 87 K. The symbols in the form of circles and asterisks correspond to two different series to evaluate the data reproducibility.</p>
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<p><span class="html-italic">t-plot</span> micropore volumes of the clay materials as determined from N<sub>2</sub> physisorption data at 77 K using the Harkins–Jura equation [<a href="#B46-molecules-29-06019" class="html-bibr">46</a>] compared with the ones derived from the corrected reference thickness curve as proposed by Galarneau et al. [<a href="#B45-molecules-29-06019" class="html-bibr">45</a>]. Solid symbols represent clays in their sodium form, while empty symbols represent clays exchanged with TMA<sup>+</sup>.</p>
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<p>Derivatives of high-resolution Ar adsorption isotherms measured at 87K for SA-Na and SAz-1-Na (blue symbols) and best-fit simulations (black line) according to a conventional (<b>a</b>,<b>b</b>) and modified (<b>c</b>) DIS analysis. Individual components are assigned to adsorption on the basal (grey dashed line) and lateral (grey continuous line) faces of clay particles, and monolayer adsorption onto particle defective sites at the edges and within intra-particle microporosity (red lines). The effect of the position of the component related to intra-particle microporosity (red arrow) on the intensity of the components corresponding to the basal and lateral faces (grey arrows) is shown for the SAz-1-Na system in (<b>d</b>).</p>
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<p>Derivatives of high-resolution Ar adsorption isotherms at 87 K (blue circles) for SA-Na (<b>a</b>), SWy2-Na (<b>b</b>), SWF-Na (<b>c</b>), and SWN-Na (<b>d</b>) together with their best-fit simulation with the modified DIS method (black line) and individual components attributed to adsorption on the basal (grey dashed line) and lateral (grey continuous line) faces of clay particles and monolayer adsorption onto defectives sites at the edges including micropores (red line).</p>
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<p>Derivative of high-resolution Ar adsorption isotherms at 87 K for IdP-Na (blue symbols) with its best-fit simulation (black line) and individual components attributed to adsorption on the basal (III, IV-grey dashed line) and lateral (II-grey continuous line) faces of clay particles and monolayer adsorption onto defective sites at the edges (I-red line).</p>
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21 pages, 751 KiB  
Article
Operational Calculus of the Quantum Statistical Fermi–Dirac and Bose–Einstein Functions Leading to the Novel Fractional Kinetic Equations
by Asifa Tassaddiq, Carlo Cattani, Rabab Alharbi, Ruhaila Md Kasmani and Sania Qureshi
Fractal Fract. 2024, 8(12), 749; https://doi.org/10.3390/fractalfract8120749 - 19 Dec 2024
Viewed by 506
Abstract
The sun is a fundamental element of the natural environment, and kinetic equations are crucial mathematical models for determining how quickly the chemical composition of a star like the sun is changing. Taking motivation from these facts, we develop and solve a novel [...] Read more.
The sun is a fundamental element of the natural environment, and kinetic equations are crucial mathematical models for determining how quickly the chemical composition of a star like the sun is changing. Taking motivation from these facts, we develop and solve a novel fractional kinetic equation containing Fermi–Dirac (FD) and Bose–Einstein (BE) functions. Several distributional properties of these functions and their proposed new generalizations are investigated in this article. In fact, it is proved that these functions belong to distribution space D while their Fourier transforms belong to Z. Fourier and Laplace transforms of these functions are computed by using their distributional representation. Thanks to them, we can compute various new fractional calculus formulae and a new relation involving the Fox–Wright function. Some fractional kinetic equations containing the FD and BE functions are also formulated and solved. Full article
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