[go: up one dir, main page]

 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (1,796)

Search Parameters:
Keywords = microsphere

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
12 pages, 3779 KiB  
Article
A Silver Modified Nanosheet Self-Assembled Hollow Microsphere with Enhanced Conductivity and Permeability
by Fangmin Wang, Xue Dong, Yuzhen Zhao, Zemin He, Wenqi Song, Chunsheng Li, Jiayin Li, Jianfeng Huang and Zongcheng Miao
Molecules 2024, 29(18), 4384; https://doi.org/10.3390/molecules29184384 (registering DOI) - 15 Sep 2024
Viewed by 179
Abstract
The utilization of sheet structure composites as a viable conductive filler has been implemented in polymer-based electromagnetic shielding materials. However, the development of an innovative sheet structure to enhance electromagnetic shielding performance remains a significant challenge. Herein, we propose a novel design incorporating [...] Read more.
The utilization of sheet structure composites as a viable conductive filler has been implemented in polymer-based electromagnetic shielding materials. However, the development of an innovative sheet structure to enhance electromagnetic shielding performance remains a significant challenge. Herein, we propose a novel design incorporating silver-modified nanosheet self-assembled hollow spheres to optimize their performance. The unique microporous structure of the hollow composite, combined with the self-assembled surface nanosheets, facilitates multiple reflections of electromagnetic waves, thereby enhancing the dissipation of electromagnetic energy. The contribution of absorbing and reflecting electromagnetic waves in hollow nanostructures could be attributed to both the inner and outer surfaces. When multiple reflection attenuation is implemented, the self-assembled stack structure of nanosheets outside the composite material significantly enhances the occurrence of multiple reflections, thereby effectively improving its shielding performance. The structure also facilitates multiple reflections of incoming electromagnetic waves at the internal and external interfaces of the material, thereby enhancing the shielding efficiency. Simultaneously, the incorporation of silver particles can enhance conductivity and further augment the shielding properties. Finally, the optimized Ag/NiSi-Ni nanocomposites can demonstrate superior initial permeability (2.1 × 10−6 H m−1), saturation magnetization (13.2 emu g−1), and conductivity (1.2 × 10−3 Ω•m). This work could offer insights for structural design of conductive fillers with improved electromagnetic shielding performance. Full article
(This article belongs to the Section Nanochemistry)
Show Figures

Figure 1

Figure 1
<p>XRD patterns of NiSi-Ni (OH)<sub>2</sub>, NiSi-Ni, and Ag/NiSi-Ni.</p>
Full article ">Figure 2
<p>The SEM images of NiSi–Ni(OH)<sub>2</sub> (<b>a</b>,<b>b</b>), NiSi–Ni (<b>c</b>,<b>d</b>), and Ag/NiSi-Ni (<b>e</b>,<b>f</b>).</p>
Full article ">Figure 3
<p>The TEM and HRTEM images of NiSi–Ni(OH)<sub>2</sub> (<b>a</b>–<b>c</b>); NiSi–Ni (<b>d</b>–<b>f</b>); and Ag/NiSi-Ni (<b>g</b>–<b>i</b>).</p>
Full article ">Figure 4
<p>Nitrogen adsorption, desorption isotherms (<b>a</b>), and pore diameter distributions (<b>b</b>) of NiSi-Ni (OH)<sub>2</sub>, NiSi-Ni, and Ag/NiSi-Ni.</p>
Full article ">Figure 5
<p>Hysteresis loops (<b>a</b>) and initial magnetization curves (<b>b</b>) of NiSi-Ni and Ag/NiSi-Ni.</p>
Full article ">Figure 6
<p>The SEM images of Ag/NiSi–Ni-1 (<b>a</b>), Ag/NiSi–Ni-2 (<b>b</b>), and Ag/NiSi–Ni-3 (<b>c</b>).</p>
Full article ">Figure 7
<p>Volume resistivity of Ag/NiSi–Ni–1, Ag/NiSi–Ni–2, and Ag/NiSi–Ni–3.</p>
Full article ">Figure 8
<p>Absorption, reflection, and transmission mechanisms of high-frequency electromagnetic waves in nanosheet self-assembled hollow sphere structure particles.</p>
Full article ">Figure 9
<p>Schematic illustration of the preparation process of Ag/NiSi-Ni.</p>
Full article ">
24 pages, 11084 KiB  
Review
Recent Applications of PLGA in Drug Delivery Systems
by Jie Yang, Huiying Zeng, Yusheng Luo, Ying Chen, Miao Wang, Chuanbin Wu and Ping Hu
Polymers 2024, 16(18), 2606; https://doi.org/10.3390/polym16182606 (registering DOI) - 14 Sep 2024
Viewed by 147
Abstract
Poly(lactic-co-glycolic acid) (PLGA) is a widely used biodegradable and biocompatible copolymer in drug delivery systems (DDSs). In this article, we highlight the critical physicochemical properties of PLGA, including its molecular weight, intrinsic viscosity, monomer ratio, blockiness, and end caps, that significantly influence drug [...] Read more.
Poly(lactic-co-glycolic acid) (PLGA) is a widely used biodegradable and biocompatible copolymer in drug delivery systems (DDSs). In this article, we highlight the critical physicochemical properties of PLGA, including its molecular weight, intrinsic viscosity, monomer ratio, blockiness, and end caps, that significantly influence drug release profiles and degradation times. This review also covers the extensive literature on the application of PLGA in delivering small-molecule drugs, proteins, peptides, antibiotics, and antiviral drugs. Furthermore, we discuss the role of PLGA-based DDSs in the treating various diseases, including cancer, neurological disorders, pain, and inflammation. The incorporation of drugs into PLGA nanoparticles and microspheres has been shown to enhance their therapeutic efficacy, reduce toxicity, and improve patient compliance. Overall, PLGA-based DDSs holds great promise for the advancement of the treatment and management of multiple chronic conditions. Full article
14 pages, 2997 KiB  
Article
Lactic Acid Bacterial Fermentation of Esterified Agave Fructans in Simulated Physicochemical Colon Conditions for Local Delivery of Encapsulated Drugs
by Carmen Miramontes-Corona, Abraham Cetina-Corona, María Esther Macías-Rodríguez, Alfredo Escalante, Rosa Isela Corona-González and Guillermo Toriz
Fermentation 2024, 10(9), 478; https://doi.org/10.3390/fermentation10090478 (registering DOI) - 14 Sep 2024
Viewed by 179
Abstract
Understanding drug release in the colon is fundamental to developing efficient treatments for colon-related diseases, while unraveling the relationship between the colonic microbiota and excipients is crucial to unveiling the effect of biomaterials on the release of drugs. In this contribution, the bio-release [...] Read more.
Understanding drug release in the colon is fundamental to developing efficient treatments for colon-related diseases, while unraveling the relationship between the colonic microbiota and excipients is crucial to unveiling the effect of biomaterials on the release of drugs. In this contribution, the bio-release of ibuprofen (encapsulated in acetylated and palmitoylated agave fructans) was evaluated by fermentation with lactic acid bacteria in simulated physicochemical (pH and temperature) colon conditions. It was observed that the size of the acyl chain (1 in acetyl and 15 in palmitoyl) was critical both in the growth of the microorganisms and in the release of the drug. For example, both the bacterial growth and the release of ibuprofen were more favored with acetylated fructan microspheres. Among the microorganisms evaluated, Bifidobacterium adolescentis and Lactobacillus brevis showed great potential as probiotics useful to release drugs from modified fructans. The production of short-chain fatty acids (lactic, acetic, and propionic acids) in the course of fermentations was also determined, since such molecules have a positive effect both on colon-related diseases and on the regulation of the intestinal microbiota. It was found that a higher concentration of acetate is related to a lower growth of bacteria and less release of ibuprofen. Full article
(This article belongs to the Special Issue Fermentation: 10th Anniversary)
Show Figures

Figure 1

Figure 1
<p>(<b>A</b>) A model of agave fructan according to [<a href="#B33-fermentation-10-00478" class="html-bibr">33</a>]; in native fructan, R is OH; in palmitoylated fructan, 4 Rs are substituted with palmitoyl moieties; for acetylated fructan, about 62 Rs should be acetyl groups. (<b>B</b>) <sup>1</sup>H NMR spectra: (<b>a</b>) native fructan analyzed in D<sub>2</sub>O; H-C* denotes the proton at the anomeric carbon in glucose (<b>b</b>) palmitoylated fructan obtained in CDCl<sub>3</sub>; (<b>c</b>) acetylated fructans analyzed in <sup>d6</sup>DMSO.</p>
Full article ">Figure 2
<p>Scanning Electron Micrographs of (<b>a</b>) acetylated (7920X) and (<b>b</b>) palmitoylated fructan (1750X).</p>
Full article ">Figure 3
<p>Growth profile of strains and their consortium obtained by optical density of (<b>a</b>) acetylated fructan microspheres and (<b>b</b>) palmitoylated fructan microspheres: <span class="html-italic">B. adolescentis</span> (●); <span class="html-italic">Weisella paramesenteroides</span> (◆); <span class="html-italic">Enterococcus mundtii</span> (◼); <span class="html-italic">Lactobacillus brevis</span> (▲); <span class="html-italic">consortium</span> (∗).</p>
Full article ">Figure 4
<p>Percentage of ibuprofen release as function of fermentation time from (<b>a</b>) acetylated and (<b>b</b>) palmitoylated fructan microspheres with <span class="html-italic">B. adolescentis</span> (●); <span class="html-italic">Weisella paramesenteroides</span> (◆); <span class="html-italic">Enterococcus mundtii</span> (◼); <span class="html-italic">Lactobacillus brevis</span> (▲); and <span class="html-italic">consortium</span> (∗).</p>
Full article ">Figure 5
<p>Production of SCFA (g/L) by lactic acid bacteria at 48 h of fermentation: (<b>a</b>) acetylated fructan microspheres and (<b>b</b>) palmitoylated fructan microspheres, (■) lactic acid, (□) acetic acid, and (<span class="html-fig-inline" id="fermentation-10-00478-i001"><img alt="Fermentation 10 00478 i001" src="/fermentation/fermentation-10-00478/article_deploy/html/images/fermentation-10-00478-i001.png"/></span>) propionic acid. BA: <span class="html-italic">B. adolescentis</span>; WP: <span class="html-italic">Weisella paramesenteroides</span>; EL: <span class="html-italic">Enterococcus mundtii</span>; LB: <span class="html-italic">Lactobacillus brevis</span>; C: <span class="html-italic">consortium</span>.</p>
Full article ">Scheme 1
<p>Phylogenetic tree for identification of <span class="html-italic">Weissella paramesenteroides</span> (Jal1), <span class="html-italic">Enterococcus mundtii</span> (BT5inv), and <span class="html-italic">Lactobacillus brevis</span> (Col18) isolated from carposphere of tomato. The red boxes indicate the identified strains in the phylogenetic tree.</p>
Full article ">
17 pages, 13288 KiB  
Article
Multi-Scale Visualization Study of Water and Polymer Microsphere Flooding through Horizontal Wells in Low-Permeability Oil Reservoir
by Liang Cheng, Yang Xie, Jie Chen, Xiao Wang, Zhongming Luo and Guo Chen
Energies 2024, 17(18), 4597; https://doi.org/10.3390/en17184597 - 13 Sep 2024
Viewed by 244
Abstract
Our target USH reservoir in the D oilfield is characterized by “inverse rhythm” deposition with the noticeable features of “high porosity and low permeability”. The reservoir has been developed with waterflooding using horizontal wells. Due to the strong heterogeneity of the reservoir, water [...] Read more.
Our target USH reservoir in the D oilfield is characterized by “inverse rhythm” deposition with the noticeable features of “high porosity and low permeability”. The reservoir has been developed with waterflooding using horizontal wells. Due to the strong heterogeneity of the reservoir, water channeling is severe, and the water cut has reached 79%. Considering the high temperature and high salinity reservoir conditions, polymer microspheres (PMs) were selected to realize conformance control. In this study, characterization of the polymer microsphere suspension was achieved via morphology, size distribution, and viscosity measurement. Furthermore, a multi-scale visualization study of the reservoir development process, including waterflooding, polymer microsphere flooding, and subsequent waterflooding, was conducted using macro-scale coreflooding and calcite-etched micromodels. It was revealed that the polymer microspheres could swell in the high salinity brine (170,000 ppm) by 2.7 times if aged for 7 days, accompanied by a viscosity increase. This feature is beneficial for the injection at the wellbore while swelled to work as a profile control agent in the deep formation. The macro-scale coreflood with a 30 cm × 30 cm × 4.5 cm layer model with 108 electrodes installed enabled the oil distribution visualization from different perpendicular cross sections. In this way, the in situ conformance control ability of the polymer microsphere was revealed both qualitatively and quantitatively. Furthermore, building on the calcite-etched visible micro-model, the pore-scale variation of the residual oil when subjected to waterflooding, polymer microsphere waterflooding, and subsequent waterflooding was collected, which revealed the oil displacement efficiency increase by polymer microspheres directly. The pilot test in the field also proves the feasibility of conformance control by the polymer microspheres, i.e., more than 40,000 bbls of oil increase was observed in the produces, accompanied by an obvious water reduction. Full article
Show Figures

Figure 1

Figure 1
<p>Illustration of the stratigraphic distribution and well-logging curves of the USH reservoir in D oilfield.</p>
Full article ">Figure 2
<p>Illustration of the horizontal well deployment in the USH reservoir of D oilfield.</p>
Full article ">Figure 3
<p>Artificial rock samples used in the macro-coreflooding tests: (<b>a</b>) picture of the real rock sample; (<b>b</b>) schematic of the layered structure of the rock sample and well placements.</p>
Full article ">Figure 4
<p>Top view (Pro. 1# and Pro. 2# are two producers; Inj. 1#, Inj. 2# and Inj. 3# are three injecteors.) (<b>a</b>), cross-sectional view of A-A’ (<b>b</b>) and B-B’ (<b>c</b>) of the artificial rock sample.</p>
Full article ">Figure 5
<p>Experimental setup of the macro-corefloods.</p>
Full article ">Figure 6
<p>Schematic of the calcite-etched micromodel.</p>
Full article ">Figure 7
<p>Setup of the displacement experiment.</p>
Full article ">Figure 8
<p>Microscopic morphology and size distribution of the polymer microsphere dispersion system after being aged for different times.</p>
Full article ">Figure 9
<p>SEM imaging of the 3D internal structure of the polymer microsphere.</p>
Full article ">Figure 10
<p>Apparent viscosity of the polymer microsphere dispersion system under different aging times.</p>
Full article ">Figure 11
<p>Oil saturation distribution variation on the A-A’ cross section in the process of macro-coreflooding.</p>
Full article ">Figure 12
<p>Oil saturation distribution variation on the B-B’ cross section in the process of macro-coreflooding.</p>
Full article ">Figure 13
<p>Oil saturation distribution variation on the four layers from top view in the process of macro-coreflooding.</p>
Full article ">Figure 14
<p>Oil recovery factors and water cuts response of two producers (<b>a</b>); and injection pressure response of three injections in the process of macro-coreflooding (<b>b</b>).</p>
Full article ">Figure 15
<p>Results of the micro-model displacement experiments.</p>
Full article ">Figure 16
<p>Microscopic residual oil morphology at the end of the water drive and PM drive stage.</p>
Full article ">
14 pages, 8908 KiB  
Article
Construction of Patterned Cu2O Photonic Crystals on Textile Substrates for Environmental Dyeing with Excellent Antibacterial Properties
by Zhen Yin, Chunxing Zhou, Yiqin Shao, Zhan Sun, Guocheng Zhu and Parpiev Khabibulla
Nanomaterials 2024, 14(18), 1478; https://doi.org/10.3390/nano14181478 - 11 Sep 2024
Viewed by 285
Abstract
Structural dyeing has attracted much attention due to its advantages such as environmental friendliness, vivid color, and resistance to fading. Herein, we propose an alternative strategy for fabric coloring based on Cu2O microspheres. The strong Mie scattering effect of Cu2 [...] Read more.
Structural dyeing has attracted much attention due to its advantages such as environmental friendliness, vivid color, and resistance to fading. Herein, we propose an alternative strategy for fabric coloring based on Cu2O microspheres. The strong Mie scattering effect of Cu2O microspheres enables the creation of vibrant structural colors on fabric surfaces. These colors are visually striking and can potentially be adjusted by tuning the diameter of the microspheres. Importantly, the Cu2O spheres were firmly bonded to the fabrics by using the industrial adhesive PDMS, and the Cu2O structural color fabrics exhibited excellent color fastness to washing, rubbing, and bending. Cu2O structural color fabrics also demonstrated excellent antimicrobial properties against bacteria such as Escherichia coli (E. coli) and Staphylococcus aureus (S. aureus). The bactericidal rates of Cu2O structural color textiles after washing for E. coli and S. aureus reached 92.40% and 94.53%, respectively. This innovative approach not only addresses environmental concerns associated with traditional dyeing processes but also enhances fabric properties by introducing vibrant structural colors and antimicrobial functionality. Full article
Show Figures

Figure 1

Figure 1
<p>Preparation of Cu<sub>2</sub>O microspheres and simulation effect of Cu<sub>2</sub>O microspheres on fabrics.</p>
Full article ">Figure 2
<p>SEM images corresponding to Cu<sub>2</sub>O microspheres with different particle sizes: (<b>A</b>) 165 nm, (<b>B</b>) 210 nm, (<b>C</b>) 240 nm, (<b>D</b>) 275 nm.</p>
Full article ">Figure 3
<p>SEM images of (<b>A</b>) fiber surface sprayed with 210 nm Cu<sub>2</sub>O microspheres (×2000); (<b>B</b>) fabric surface sprayed with 210 nm Cu<sub>2</sub>O microspheres (×20,000); (<b>C</b>) EDS elemental analysis.</p>
Full article ">Figure 4
<p>(<b>A</b>) XRD profiles of Cu<sub>2</sub>O microspheres. (<b>B</b>) Size distribution by intensity.</p>
Full article ">Figure 5
<p>Structural color schematic.</p>
Full article ">Figure 6
<p>Photographs of structural colored fabrics: (<b>A</b>) 165 nm, (<b>B</b>) 210 nm, (<b>C</b>) 240 nm, (<b>D</b>) 275 nm.</p>
Full article ">Figure 7
<p>Reflectance curves of structural colored fabrics with different particle sizes of Cu<sub>2</sub>O microspheres: (<b>A</b>) 165 nm, (<b>B</b>) 210 nm, (<b>C</b>) 240 nm, (<b>D</b>) 275 nm.</p>
Full article ">Figure 8
<p>Comparison after rubbing fastness tests: (<b>A</b>) original fabric, (<b>B</b>) fabric in friction, (<b>C</b>) fabric after friction.</p>
Full article ">Figure 9
<p>Comparison after fast light fastness tests: (<b>A</b>) original fabric, (<b>B</b>) fabric after fast light fastness tests, (<b>C</b>) original fabric, (<b>D</b>) fabric after fast light fastness tests.</p>
Full article ">Figure 10
<p>Comparison after washing fastness tests: (<b>A</b>) original fabric, (<b>B</b>) fabric in washing fastness tests, (<b>C</b>) fabric after washing fastness tests.</p>
Full article ">Figure 11
<p>Comparison after rubbing bending tests: (<b>A</b>) fabric in rubbing bending tests, (<b>B</b>) fabric after rubbing bending tests.</p>
Full article ">Figure 12
<p><span class="html-italic">E. coli</span> colony (<b>A</b>), control plate (<b>B</b>), and Cu<sub>2</sub>O structural colored fabric (<b>C</b>) after washes; <span class="html-italic">S. aureus</span> colony (<b>D</b>), control plate (<b>E</b>), and Cu<sub>2</sub>O structural colored fabric (<b>F</b>) after washes.</p>
Full article ">
23 pages, 12483 KiB  
Article
Development of Resorbable Phosphate-Based Glass Microspheres as MRI Contrast Media Agents
by Jesús Molinar-Díaz, Andi Arjuna, Nichola Abrehart, Alison McLellan, Roy Harris, Md Towhidul Islam, Ahlam Alzaidi, Chris R. Bradley, Charlotte Gidman, Malcolm J. W. Prior, Jeremy Titman, Nicholas P. Blockley, Peter Harvey, Luca Marciani and Ifty Ahmed
Molecules 2024, 29(18), 4296; https://doi.org/10.3390/molecules29184296 - 10 Sep 2024
Viewed by 954
Abstract
In this research, resorbable phosphate-based glass (PBG) compositions were developed using varying modifier oxides including iron (Fe2O3), copper (CuO), and manganese (MnO2), and then processed via a rapid single-stage flame spheroidisation process to manufacture dense (i.e., solid) [...] Read more.
In this research, resorbable phosphate-based glass (PBG) compositions were developed using varying modifier oxides including iron (Fe2O3), copper (CuO), and manganese (MnO2), and then processed via a rapid single-stage flame spheroidisation process to manufacture dense (i.e., solid) and highly porous microspheres. Solid (63–200 µm) and porous (100–200 µm) microspheres were produced and characterised via SEM, XRD, and EDX to investigate their surface topography, structural properties, and elemental distribution. Complementary NMR investigations revealed the formation of Q2, Q1, and Q0 phosphate species within the porous and solid microspheres, and degradation studies performed to evaluate mass loss, particle size, and pH changes over 28 days showed no significant differences among the microspheres (63–71 µm) investigated. The microspheres produced were then investigated using clinical (1.5 T) and preclinical (7 T) MRI systems to determine the R1 and R2 relaxation rates. Among the compositions investigated, manganese-based porous and solid microspheres revealed enhanced levels of R2 (9.7–10.5 s−1 for 1.5 T; 17.1–18.9 s−1 for 7 T) and R1 (3.4–3.9 s−1 for 1.5 T; 2.2–2.3 s−1 for 7 T) when compared to the copper and iron-based microsphere samples. This was suggested to be due to paramagnetic ions present in the Mn-based microspheres. It is also suggested that the porosity in the resorbable PBG porous microspheres could be further explored for loading with drugs or other biologics. This would further advance these materials as MRI theranostic agents and generate new opportunities for MRI contrast-enhancement oral-delivery applications. Full article
(This article belongs to the Special Issue Advanced Magnetic Resonance Methods in Materials Chemistry Analysis)
Show Figures

Figure 1

Figure 1
<p>SEM images of flame spheroidised-processed solid microspheres (SMS) P45 (63–200 µm) with modified compositions: Fe–(<b>a</b>) 2.5%, (<b>d</b>) 5%; Cu–(<b>b</b>) 2.5%, (<b>e</b>) 5%; and Mn–(<b>c</b>) 2.5%, (<b>f</b>) 5%.</p>
Full article ">Figure 2
<p>SEM images of flame spheroidised-processed porous microspheres (PMS) P45, in the ranges of (<b>a</b>–<b>f</b>) 150–200 µm and (<b>g</b>–<b>l</b>) 100–150 µm, with modified compositions: Fe–(<b>a</b>,<b>g</b>) 2.5%, (<b>d</b>,<b>j</b>) 5%; Cu–(<b>b</b>,<b>h</b>) 2.5%, (<b>e</b>,<b>k</b>) 5%; and Mn–(<b>c</b>,<b>i</b>) 2.5%, (<b>f</b>,<b>l</b>) 5%.</p>
Full article ">Figure 3
<p>XRD patterns for flame spheroidised-processed solid glass microspheres (SMS) P45 with modified Fe, Cu, and Mn compositions.</p>
Full article ">Figure 4
<p>XRD patterns for flame spheroidised-processed porous microspheres (PMS) P45 with modified Fe, Cu, and Mn compositions.</p>
Full article ">Figure 5
<p>BSE images and EDX elemental mapping of flame spheroidised-processed solid glass microspheres (SMS) P45, following sectioning, illustrating modified Fe, Cu, and Mn compositions. (The colours represent: purple for phosphate, red for sodium, green for calcium, light blue for oxygen, blue for copper, and dark blue for manganese).</p>
Full article ">Figure 6
<p>BSE images and EDX elemental mapping of flame spheroidised-processed porous glass microspheres (PMS) P45 (100–200 µm), following sectioning, illustrating the modified Fe, Cu, and Mn compositions and revealing good levels of interconnected porosity among the samples. (The colours represent: purple for phosphate, red for sodium, green for calcium, light blue for oxygen, blue for copper, and dark blue for manganese).</p>
Full article ">Figure 7
<p>Degradation studies on: (<b>a</b>,<b>b</b>) Mass loss (%), (<b>c</b>,<b>d</b>) pH change, and (<b>e</b>,<b>f</b>) microsphere size (µm), as a function of immersion time (day 1, 3, 7, 14, 21, and 28) for (<b>a</b>,<b>c</b>,<b>e</b>) solid, and (<b>b</b>,<b>d</b>,<b>f</b>) porous microspheres of Fe2.5, Fe5, Cu2.5, Cu5, Mn2.5, and Mn5 over 28 days. SMS (solid microspheres); PMS (porous microspheres).</p>
Full article ">Figure 8
<p>Transverse relaxivity (<span class="html-italic">R</span><sub>2</sub>) measurements and associated MRI relaxation images showing hydroxymethyl cellulose suspension of solid microspheres (SMS) and porous microspheres (PMS) loaded with iron (Fe), copper (Cu), and manganese (Mn) assessed via 1.5 T (<b>a</b>,<b>c</b>) and 7 T (<b>b</b>,<b>d</b>,<b>e</b>) MRI systems. (<b>a</b>,<b>b</b>) highlight <span class="html-italic">R</span><sub>2</sub> measurements as a function of molar concentration; (<b>c</b>,<b>d</b>) <span class="html-italic">R</span><sub>2</sub> relaxation times for SMS and PMS. 7 T MRI measurements are compared with s hydroxymethyl cellulose solution as a way of control; and (<b>e</b>) 7 T MRI system <span class="html-italic">R</span><sub>2</sub> relaxation MRI mappings for SMS and PMS suspensions.</p>
Full article ">Figure 9
<p>Longitudinal relaxivity (<span class="html-italic">R</span><sub>1</sub>) measurements and associated MRI relaxation images showing hydroxymethyl cellulose suspensions of solid microspheres (SMS) and porous microspheres (PMS) loaded with iron (Fe), copper (Cu), and manganese (Mn) assessed via 1.5 T (<b>a</b>,<b>c</b>) and 7 T (<b>b</b>,<b>d</b>,<b>e</b>) MRI systems. (<b>a</b>,<b>b</b>) highlight <span class="html-italic">R</span><sub>1</sub> measurements as a function of molar concentration; (<b>c</b>,<b>d</b>) <span class="html-italic">R</span><sub>1</sub> relaxation times for SMS and PMS. 7 T measurements are compared with hydroxymethyl cellulose solution as way of control; and (<b>e</b>) 7 T MRI system <span class="html-italic">R</span><sub>1</sub> relaxation MRI images for SMS and PMS suspensions.</p>
Full article ">Figure 10
<p>High-magnification SEM images of flame spheroidised-processed porous microspheres (PMS), in the range of 150–200 µm, with modified compositions: Fe–(<b>a</b>) 2.5%, (<b>d</b>) 5%; Cu–(<b>b</b>) 2.5%, (<b>e</b>) 5%; and Mn–(<b>c</b>) 2.5%, (<b>f</b>) 5%, extracted from the sample sets presented in <a href="#molecules-29-04296-f002" class="html-fig">Figure 2</a>.</p>
Full article ">
21 pages, 6611 KiB  
Article
Shear Behavior of High-Strength and Lightweight Cementitious Composites Containing Hollow Glass Microspheres and Carbon Nanotubes
by Dongmin Lee, Seong-Cheol Lee, Oh-Sung Kwon and Sung-Won Yoo
Buildings 2024, 14(9), 2824; https://doi.org/10.3390/buildings14092824 - 7 Sep 2024
Viewed by 479
Abstract
In this study, an experimental program was conducted to investigate the shear behavior of beams made of high-strength and lightweight cementitious composites (HS-LWCCs) containing hollow glass microspheres and carbon nanotubes. The compressive strength and dry density of the HS-LWCCs were 87.8 MPa and1.52 [...] Read more.
In this study, an experimental program was conducted to investigate the shear behavior of beams made of high-strength and lightweight cementitious composites (HS-LWCCs) containing hollow glass microspheres and carbon nanotubes. The compressive strength and dry density of the HS-LWCCs were 87.8 MPa and1.52 t/m3, respectively. To investigate their shear behavior, HS-LWCC beams with longitudinal rebars were fabricated. In this test program, the longitudinal and shear reinforcement ratios were considered as the test variables. The HS-LWCC beams were compared with ordinary high-strength concrete (HSC) beams with a compressive strength of 89.3 MPa to determine their differences; the beams had the same reinforcement configuration. The test results indicated that the initial stiffness and shear capacity of the HS-LWCC beams were lower than those of the HSC beams. These results suggested that the low shear resistance of the HS-LWCC beams led to brittle failure. This was attributed to the beams’ low elastic modulus under compression and the absence of a coarse aggregate. Furthermore, the difference in the shear capacity of the HSC and HS-LWCC beams slightly decreased as the shear reinforcement ratio increased. The diagonal compression strut angle and diagonal crack angle of the HS-LWCC beams with shear reinforcement were more inclined than those of the HSC beams. This indicated that the lower shear resistance of the HS-LWCCs could be more effectively compensated for when shear reinforcement is provided and the diagonal crack angle is more inclined. The ultimate shear capacities measured in the tests were compared with various shear design provisions, including those of ACI-318, EC2, and CSA A23.3. This comparison showed that the current shear design provisions considerably overestimate the contribution of concrete to the shear capacity of HS-LWCC beams. Full article
(This article belongs to the Special Issue Study on the Durability of Construction Materials and Structures)
Show Figures

Figure 1

Figure 1
<p>Compression test results. (<b>a</b>) Compression test setup. (<b>b</b>) Compressive stress–strain responses.</p>
Full article ">Figure 2
<p>Design of specimens (unit: mm). (<b>a</b>) Details of specimens. (<b>b</b>) Cross section of specimens.</p>
Full article ">Figure 2 Cont.
<p>Design of specimens (unit: mm). (<b>a</b>) Details of specimens. (<b>b</b>) Cross section of specimens.</p>
Full article ">Figure 3
<p>Designation of specimens.</p>
Full article ">Figure 4
<p>Test setup and LVDTs configuration. (<b>a</b>) Test setup. (<b>b</b>) Location of LVDTs (unit: mm). (<b>c</b>) LVDT rosette.</p>
Full article ">Figure 5
<p>Crack patterns at failure. (<b>a</b>) N-L1.2. (<b>b</b>) L-L1.2. (<b>c</b>) N-L1.7. (<b>d</b>) L-L1.7. (<b>e</b>) N-L2.3. (<b>f</b>) L-L2.3. (<b>g</b>) N-L2.9. (<b>h</b>) L-L2.9. (<b>i</b>) N-V.18. (<b>j</b>) L-V.18. (<b>k</b>) N-V.27. (<b>l</b>) L-V.27. (<b>m</b>) N-V.36. (<b>n</b>) L-V.36.</p>
Full article ">Figure 5 Cont.
<p>Crack patterns at failure. (<b>a</b>) N-L1.2. (<b>b</b>) L-L1.2. (<b>c</b>) N-L1.7. (<b>d</b>) L-L1.7. (<b>e</b>) N-L2.3. (<b>f</b>) L-L2.3. (<b>g</b>) N-L2.9. (<b>h</b>) L-L2.9. (<b>i</b>) N-V.18. (<b>j</b>) L-V.18. (<b>k</b>) N-V.27. (<b>l</b>) L-V.27. (<b>m</b>) N-V.36. (<b>n</b>) L-V.36.</p>
Full article ">Figure 6
<p>Load–deflection responses of specimens. (<b>a</b>) HSC beams without shear reinforcement. (<b>b</b>) HS-LWCC beams without shear reinforcement. (<b>c</b>) HSC beams with shear reinforcement. (<b>d</b>) HS-LWCC beams with shear reinforcement.</p>
Full article ">Figure 7
<p>Effect of shear parameters on shear capacity. (<b>a</b>) Longitudinal reinforcement ratio. (<b>b</b>) Shear reinforcement ratio.</p>
Full article ">Figure 8
<p>Effect of shear parameters on shear capacity reduction ratio. (<b>a</b>) Longitudinal reinforcement ratio. (<b>b</b>) Shear reinforcement ratio.</p>
Full article ">Figure 9
<p>Effect of shear parameters on deflection at maximum load. (<b>a</b>) Longitudinal reinforcement ratio. (<b>b</b>) Shear reinforcement ratio.</p>
Full article ">Figure 10
<p>Load–average strain relationship in web.</p>
Full article ">Figure 11
<p>Principal and shear strains in web.</p>
Full article ">Figure 12
<p>Diagonal compression strut angles. (<b>a</b>) HSC beams. (<b>b</b>) HS-LWCC beams.</p>
Full article ">Figure 13
<p>Comparison of shear capacity between test results and design provisions. (<b>a</b>) ACI 318-19. (<b>b</b>) CSA A23.3:19. (<b>c</b>) Eurocode 2.</p>
Full article ">
16 pages, 5675 KiB  
Article
A Facile and Efficient Protocol for Phospholipid Enrichment in Synovial Joint Fluid: Monodisperse-Mesoporous SiO2 Microspheres as a New Metal Oxide Affinity Sorbent
by Serhat Aladağ, İlayda Demirdiş, Burcu Gökçal Kapucu, Emine Koç, Ozan Kaplan, Batuhan Erhan Aktaş, Mustafa Çelebier, Ali Tuncel and Feza Korkusuz
Separations 2024, 11(9), 262; https://doi.org/10.3390/separations11090262 - 5 Sep 2024
Viewed by 444
Abstract
Phospholipids (PLs), essential components of cell membranes, play significant roles in maintaining the structural integrity and functionality of joint tissues. One of the main components of synovial joint fluid (SJF) is PLs. Structures such as PLs that are found in low amounts in [...] Read more.
Phospholipids (PLs), essential components of cell membranes, play significant roles in maintaining the structural integrity and functionality of joint tissues. One of the main components of synovial joint fluid (SJF) is PLs. Structures such as PLs that are found in low amounts in biological fluids may need to be selectively enriched to be analyzed. Monodisperse-mesoporous SiO2 microspheres were synthesized by a multi-step hydrolysis condensation method for the selective enrichment and separation of PLs in the SJF. The microspheres were characterized by SEM, XPS, XRD, and BET analyses. SiO2 microspheres had a 161.5 m2/g surface area, 1.1 cm3/g pore volume, and 6.7 nm pore diameter, which were efficient in the enrichment of PLs in the SJF. The extracted PLs with sorbents were analyzed using Q-TOF LC/MS in a gradient elution mode with a C18 column [2.1 × 100 mm, 2.5 μM, Xbridge Waters (Milford, MA, USA)]. An untargeted lipidomic approach was performed, and the phospholipid enrichment was successfully carried out using the proposed solid-phase extraction (SPE) protocol. Recovery of the SPE extraction of PLs using sorbents was compared to the classical liquid–liquid extraction (LLE) procedure for lipid extraction. The results showed that monodisperse-mesoporous SiO2 microspheres were eligible for selective enrichment of PLs in SJF samples. These microspheres can be used to identify PLs changes in articular joint cartilage (AJC) in physiological and pathological conditions including osteoarthritis (OA) research. Full article
Show Figures

Figure 1

Figure 1
<p>Structures of the major phospholipids [<a href="#B24-separations-11-00262" class="html-bibr">24</a>,<a href="#B25-separations-11-00262" class="html-bibr">25</a>].</p>
Full article ">Figure 2
<p>Radiographic imaging result and SJF aspiration sample of a 57-year-old patient with grade 4 OA diagnosis.</p>
Full article ">Figure 3
<p>Representation of metabolite, protein, and lipid phases from top to bottom, respectively, after the LLE protocol.</p>
Full article ">Figure 4
<p>The schematic representation of the synthesis protocol for monodisperse-mesoporous SiO<sub>2</sub> microspheres.</p>
Full article ">Figure 5
<p>Different scales SEM photographs of monodisperse-mesoporous SiO<sub>2</sub> microspheres ((<b>a</b>): 20 µm scale, (<b>b</b>): 10 µm scale, (<b>c</b>): 2 µm scale).</p>
Full article ">Figure 6
<p>Brunauer–Emmett–Teller (BET) result of monodisperse-mesoporous SiO<sub>2</sub> microspheres.</p>
Full article ">Figure 7
<p>XRD spectra of the monodisperse-mesoporous SiO<sub>2</sub> microspheres.</p>
Full article ">Figure 8
<p>(<b>A</b>) Survey XPS spectrum, (<b>B</b>) core level spectra for C1s scan, (<b>C</b>) core level spectra for O1s scan, and (<b>D</b>) core level spectra for Si 2p scan with monodisperse-mesoporous SiO<sub>2</sub> microspheres.</p>
Full article ">Figure 9
<p>The schematic representation of the phospholipid enrichment using monodisperse-mesoporous SiO<sub>2</sub> microspheres.</p>
Full article ">Figure 10
<p>Overlapped based peak chromatograms (<b>A</b>) Base peak chromatograms of the SPE fraction. (<b>B</b>) Base peak chromatograms of the LLE fraction.</p>
Full article ">Figure 11
<p>Comparative recovery for PLs using different extraction techniques (SPE: solid-phase extraction, LLE: liquid–liquid extraction).</p>
Full article ">Figure 12
<p>The enrichment rates of the sorbent for the phospholipid species predominantly found in SJF (PA: Phosphatidic acid, PC: Phosphatidylcholines, PG: Phosphatidylglycerol, PS: Phosphatidylserine).</p>
Full article ">
18 pages, 10991 KiB  
Article
The Influence of Shot Peening Media on Surface Properties and Fatigue Behaviour of Aluminium Alloy 6082 T6
by Erik Calvo-García, Jesús del Val, Antonio Riveiro, Sara Valverde-Pérez, David Álvarez, Manuel Román, César Magdalena, Aida Badaoui, Pablo Pou-Álvarez and Rafael Comesaña
J. Manuf. Mater. Process. 2024, 8(5), 192; https://doi.org/10.3390/jmmp8050192 - 3 Sep 2024
Viewed by 451
Abstract
Shot peening is generally used to improve the fatigue performance of mechanical components. However, identifying the geometrical and mechanical characteristics of the shots that improve fatigue strength is still a challenging task, as there are many variables involved in the shot peening process. [...] Read more.
Shot peening is generally used to improve the fatigue performance of mechanical components. However, identifying the geometrical and mechanical characteristics of the shots that improve fatigue strength is still a challenging task, as there are many variables involved in the shot peening process. The present work addresses the effect of different shot media on the fatigue behaviour of an aluminium alloy 6082 T6. Four different shot types were used: silica microspheres, alumina shots, aluminium cut wire and zinc cut wire. Axial fatigue tests were carried out to obtain the Wöhler curves corresponding to each shot peening treatment. The surface properties of the shot-peened specimens, such as grain size, hardness, residual stress and roughness were measured to determine their effect on the fatigue results. The fatigue results revealed that silica and zinc shots increased significantly the fatigue life of the alloy, whereas alumina and aluminium shots reduced its fatigue strength. Almen intensities have shown to correlate well with grain refinement and strain hardening. However, better fatigue results were obtained with the shots that generated higher surface compressive residual stresses. It is believed that small and smooth shots are preferable to sharp and irregular ones, regardless of the Almen intensity or surface hardness attained with the latter. Full article
(This article belongs to the Special Issue Deformation and Mechanical Behavior of Metals and Alloys)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Grain structure of the non-treated aluminium alloy 6082 T6.</p>
Full article ">Figure 2
<p>Particles used in the shot peening process: (<b>a</b>) silica microspheres, (<b>b</b>) alumina, (<b>c</b>) aluminium cut wire and (<b>d</b>) zinc cut wire.</p>
Full article ">Figure 3
<p>Dimensions and requirements of the fatigue test specimens.</p>
Full article ">Figure 4
<p>Grain structures at the surface of the aluminium alloy 6082 T6 after shot peening treatments with (<b>a</b>) silica microspheres, (<b>b</b>) alumina, (<b>c</b>) aluminium cut wire and (<b>d</b>) zinc cut wire.</p>
Full article ">Figure 5
<p>Nanohardness measurements as a function of depth for different shot peening treatments.</p>
Full article ">Figure 6
<p>Effect of Almen intensity on (<b>a</b>) grain refinement and (<b>b</b>) surface nanohardness increase.</p>
Full article ">Figure 7
<p>Surface residual stresses for different shot peening treatments.</p>
Full article ">Figure 8
<p>Surface topography of aluminium alloy 6082 T6 specimens (<b>a</b>) with no surface treatment and shot-peened with (<b>b</b>) silica microspheres, (<b>c</b>) alumina particles, (<b>d</b>) aluminium cut wire and (<b>e</b>) zinc cut wire.</p>
Full article ">Figure 9
<p>Wöhler diagrams of the 6082 T6 alloy subjected to different shot peening treatments.</p>
Full article ">Figure 10
<p>Fracture surface (front and lateral) of a non-treated specimen of 6082 aluminium alloy tested to a maximum stress of 305 MPa.</p>
Full article ">Figure 11
<p>Fracture surfaces (front and lateral) of the 6082 aluminium alloy shot-peened with (<b>a</b>) silica microspheres, (<b>b</b>) alumina particles, (<b>c</b>) aluminium cut wire and (<b>d</b>) zinc cut wire, all tested to a maximum stress of 305 MPa.</p>
Full article ">Figure 12
<p>Fatigue crack (<b>a</b>) initiation and (<b>b</b>) propagation of a non-treated specimen of 6082 aluminium alloy tested to a maximum stress of 305 MPa.</p>
Full article ">Figure 13
<p>Fatigue crack initiation sites of 6082 aluminium alloy specimens shot-peened with (<b>a</b>) silica microspheres, (<b>b</b>) alumina particles, (<b>c</b>) aluminium cut wire and (<b>d</b>) zinc cut wire, all tested to a maximum stress of 305 MPa.</p>
Full article ">
15 pages, 2210 KiB  
Article
Probiotic Encapsulation: Bead Design Improves Bacterial Performance during In Vitro Digestion (Part 2: Operational Conditions of Vibrational Technology)
by Yesica Vanesa Rojas-Muñoz, María de Jesús Perea-Flores and María Ximena Quintanilla-Carvajal
Polymers 2024, 16(17), 2492; https://doi.org/10.3390/polym16172492 - 31 Aug 2024
Viewed by 575
Abstract
The development of functional foods is a viable alternative for the prevention of numerous diseases. However, the food industry faces significant challenges in producing functional foods based on probiotics due to their high sensitivity to various processing and gastrointestinal tract conditions. This study [...] Read more.
The development of functional foods is a viable alternative for the prevention of numerous diseases. However, the food industry faces significant challenges in producing functional foods based on probiotics due to their high sensitivity to various processing and gastrointestinal tract conditions. This study aimed to evaluate the effect of the operational conditions during the extrusion encapsulation process using vibrating technology on the viability of Lactobacillus fermentum K73, a lactic acid bacterium with hypocholesterolemia probiotic potential. An optimal experimental design approach was employed to produce sweet whey–sodium alginate (SW-SA) beads with high bacterial content and good morphological characteristics. In this study, the effects of frequency, voltage, and pumping rate were optimized for a 300 μm nozzle. The microspheres were characterized using RAMAN spectroscopy, scanning electron microscopy, and confocal laser scanning microscopy. The optimal conditions for bead production were found: 70 Hz, 250 V, and 20 mL/min with a final cell count of 8.43 Log10 (CFU/mL). The mean particle diameter was 620 ± 5.3 µm, and the experimental encapsulation yield was 94.3 ± 0.8%. The INFOGEST model was used to evaluate the survival of probiotic beads under gastrointestinal tract conditions. Upon exposure to in vitro conditions of oral, gastric, and intestinal phases, the encapsulated viability of L. fermentum was 7.6 Log10 (CFU/mL) using the optimal encapsulation parameters, which significantly improved the survival of probiotic bacteria during both the encapsulation process and under gastrointestinal conditions compared to free cells. Full article
(This article belongs to the Section Polymer Applications)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Three-dimensional surface response plots for variables: (<b>A</b>) viability (Log<sub>10</sub> (CFU/mL)), (<b>B</b>) encapsulation Efficiency (%).</p>
Full article ">Figure 2
<p>Confocal laser scanning microscopy images of bacteria viability assay: (<b>A</b>) autofluorescence control (unstained sample), (<b>B</b>) <span class="html-italic">L. fermentum K73</span> unencapsulated, (<b>C</b>) <span class="html-italic">L. fermentum</span> K73 encapsulated in SW-SA beads. Right side: live cells, left side: dead cells.</p>
Full article ">Figure 3
<p>SEM Images of <span class="html-italic">L. fermentum</span> K73 freeze-dried SW-SA beads: (<b>A</b>) 100X, (<b>B</b>) 500X, (<b>C</b>) 2700X.</p>
Full article ">Figure 4
<p>Raman mapping: 2D sodium alginate intensity.</p>
Full article ">Figure 5
<p>Viability of free and encapsulated <span class="html-italic">L. fermentum</span> K73 cells during OP (oral phase: 2 min, pH 7.0), GP (gastric phase: 120 min, pH 3.0), and IP (intestinal phase: 120 min, pH 7.0) according to the INFOGEST in vitro model. Mean value ± standard deviation of at least three independent measurements is included. (A–C) Different letters within the same treatment (encapsulated or free cells) indicate statistical significance (<span class="html-italic">p</span> &lt; 0.05). (a,b) Different letters with the same in vitro digestion phase indicate statistical significance (<span class="html-italic">p</span> &lt; 0.05).</p>
Full article ">
14 pages, 5594 KiB  
Article
A Novel Device for Micro-Droplets Generation Based on the Stepwise Membrane Emulsification Principle
by Lei Lei, Sven Achenbach, Garth Wells, Hongbo Zhang and Wenjun Zhang
Micromachines 2024, 15(9), 1118; https://doi.org/10.3390/mi15091118 - 31 Aug 2024
Viewed by 499
Abstract
This paper presents a novel design of the device to generate microspheres or micro-droplets based on the membrane emulsification principle. Specifically, the novelty of the device lies in a proposed two-layer or stepwise (by generalization) membrane structure. An important benefit of the stepwise [...] Read more.
This paper presents a novel design of the device to generate microspheres or micro-droplets based on the membrane emulsification principle. Specifically, the novelty of the device lies in a proposed two-layer or stepwise (by generalization) membrane structure. An important benefit of the stepwise membrane is that it can be fabricated with the low-cost material (SU-8) and using the conventional lithography technology along with a conventional image-based alignment technique. The experiment to examine the effectiveness of the proposed membrane was conducted, and the result shows that microspheres with the size of 2.3 μm and with the size uniformity of 0.8 μm can be achieved, which meets the requirements for most applications in industries. It is noted that the traditional membrane emulsification method can only produce microspheres of around 20 μm. The main contribution of this paper is thus the new design principle of membranes (i.e., stepwise structure), which can be made by the cost-effective fabrication technique, for high performance of droplets production. Full article
Show Figures

Figure 1

Figure 1
<p>A side view of a membrane emulsification device.</p>
Full article ">Figure 2
<p>The membrane for microspheres generation. (<b>a</b>) The single-layer structure of the pores on the membrane emulsification device; (<b>b</b>) the stepwise structure of the pores (not to scale).</p>
Full article ">Figure 3
<p>The stepwise pore structure of the new membrane emulsification device (not to scale).</p>
Full article ">Figure 4
<p>The optical image of one alignment on the first layer.</p>
Full article ">Figure 5
<p>The optical image of pores with 1 × 1 μm<sup>2</sup>.</p>
Full article ">Figure 6
<p>The membranes before and after chromium etching.</p>
Full article ">Figure 7
<p>The optical image of one alignment on the second layer.</p>
Full article ">Figure 8
<p>The optical images of (<b>a</b>) the top view and (<b>b</b>) bottom view of the pores with 20 × 20 μm<sup>2</sup>.</p>
Full article ">Figure 9
<p>The membranes glued to ABS tubes. The diameter of the tubes is 1 cm.</p>
Full article ">Figure 10
<p>The fabricated stepwise membranes for microsphere generation. (<b>a</b>) Three membranes; (<b>b</b>) the magnified optical image of the porous membrane.</p>
Full article ">Figure 11
<p>The schematic illustration of the fabrication procedure of the membrane with multilayer structure (not drawn to scale). (<b>a</b>) Sputtering with chrome; (<b>b</b>) Spin coating with SU-8; (<b>c</b>) Mask aligning; (<b>d</b>) Exposure with laser; (<b>e</b>) Post exposure bake; (<b>f</b>) Opaque region is rinsed off by developer; (<b>g</b>) O<sub>2</sub> plasma cleaning; (<b>h</b>) Chrome etching; (<b>i</b>) Spin coating with SU-8; (<b>j</b>) Mask aligning; (<b>k</b>) Exposure with laser; (<b>l</b>) Post exposure bake; (<b>m</b>) Opaque region is rinsed off by developer; (<b>n</b>) Glue to an ABS tube; (<b>o</b>) Glass and chrome removing.</p>
Full article ">Figure 12
<p>Experimental set-up for the membrane emulsification process.</p>
Full article ">Figure 13
<p>White dots are microspheres generated using the SU-8 membrane. Agitation speed: 100 rpm. Distance between the agitator and the membrane: 1 cm.</p>
Full article ">Figure 14
<p>The optical images of the microspheres generated by the SU-8 membrane with the agitation speeds of 60 rpm (<b>a</b>), 80 rpm (<b>b</b>), and 100 rpm (<b>c</b>). Microspheres are highlighted in red circles in (<b>c</b>).</p>
Full article ">Figure 15
<p>Average microsphere diameters with standard deviations for different agitation speeds.</p>
Full article ">Figure 16
<p>An optical image of the failure of the SU-8 membrane.</p>
Full article ">
17 pages, 2647 KiB  
Article
The Essential Role of Monte Carlo Simulations for Lung Dosimetry in Liver Radioembolization with 90Y Microspheres
by Edoardo d’Andrea, Nico Lanconelli, Marta Cremonesi, Vincenzo Patera and Massimiliano Pacilio
Appl. Sci. 2024, 14(17), 7684; https://doi.org/10.3390/app14177684 - 30 Aug 2024
Viewed by 563
Abstract
This study compares various methodologies for lung dosimetry in radioembolization using Monte Carlo (MC) simulations. A voxelized anthropomorphic phantom, created from a real patient’s CT scan, preserved the actual density distribution of the lungs. Lung dosimetry was evaluated for five lung-shunt (LS) cases [...] Read more.
This study compares various methodologies for lung dosimetry in radioembolization using Monte Carlo (MC) simulations. A voxelized anthropomorphic phantom, created from a real patient’s CT scan, preserved the actual density distribution of the lungs. Lung dosimetry was evaluated for five lung-shunt (LS) cases using traditional methods: the mono-compartmental organ-level approach (MIRD), local energy deposition (LED), and convolution with voxel S-values, either with local density corrections (SVOX_L) or without (SVOX_ST). Additionally, a novel voxel S-value (VSV) kernel for lung tissue with an ICRU density of 0.296 g/cm3 was developed. Calculations were performed using either the ICRU lung density (Lung_296), the average lung density of the phantom (Lung_221), or the local density (Lung_L). The comparison revealed significant underestimations in the mean absorbed dose (AD) for the classical approaches: approximately −40% for MIRD, −27% for LED, −28% for SVOX_L, and −88% for SVOX_ST. Similarly, calculations with the lung VSV kernel showed underestimations of about −62% for Lung_296, −50% for Lung_221, and −35% for Lung_L. Given the high heterogeneity of lung tissue, traditional dosimetric methods fail to provide accurate estimates of the mean AD for the lungs. Therefore, MC dosimetry based on patient images is recommended as the preferred method for precise assessment of lung AD during radioembolization. Full article
Show Figures

Figure 1

Figure 1
<p>Density distribution in lungs ROI in <math display="inline"><semantics> <mrow> <mi mathvariant="normal">g</mi> <mo>/</mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msup> </mrow> </semantics></math>. The distribution is characterized by a range of values from 0 to 1.06 <math display="inline"><semantics> <mrow> <mi mathvariant="normal">g</mi> <mo>/</mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msup> </mrow> </semantics></math>, a mean value of <math display="inline"><semantics> <mrow> <mn>0.221</mn> <mtext> </mtext> <mi mathvariant="normal">g</mi> <mo>/</mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msup> </mrow> </semantics></math>, and a median value of <math display="inline"><semantics> <mrow> <mn>0.179</mn> <mtext> </mtext> <mi mathvariant="normal">g</mi> <mo>/</mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msup> </mrow> </semantics></math>.</p>
Full article ">Figure 2
<p><span class="html-italic">AD</span> distribution (values expressed in Gy/GBq) within lungs (<b>A</b>) and the associated relative uncertainty map (<b>B</b>) for <span class="html-italic">LS</span> = 40%.</p>
Full article ">Figure 3
<p>Plot of the <span class="html-italic">AD</span> per unit decay to the target voxel (y-axis) versus the source-target voxel distance (x-axis) for the previously published ST kernel (9 × 9 × 9) [<a href="#B26-applsci-14-07684" class="html-bibr">26</a>] (data freely available on the website <a href="https://www.medphys.it/down_svoxel.htm" target="_blank">https://www.medphys.it/down_svoxel.htm</a>, accessed on 24 July 2024) and the lung kernel calculated in this work (32 × 32 × 32). The right plot reports the same data shown in the left plot up to a source-target of 20 mm.</p>
Full article ">Figure 4
<p>Correlation plot of the lungs’ <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>A</mi> <mi>D</mi> </mrow> <mo>¯</mo> </mover> </mrow> </semantics></math>, obtained from <span class="html-italic">MC</span> simulations with the Reference phantom (x-axis) with those from: mono-compartmental MIRD approach (MIRD), local energy deposition (LED), SVOX with ST kernel with corrections for tissue heterogeneities according to Equation (3) (SVOX_L), or without these corrections (SVOX_ST). For the SVOX_ST data, a previously published VSV kernel for soft tissue (ST) was used [<a href="#B26-applsci-14-07684" class="html-bibr">26</a>] (data freely available on the website <a href="https://www.medphys.it/down_svoxel.htm" target="_blank">https://www.medphys.it/down_svoxel.htm</a>, accessed on 24 July 2024). For each dataset, each point in the plot is associated with an increasing <span class="html-italic">LS</span> value (10%, 20%, 30%, and 40%), and a line representing the linear interpolation of each dataset serves as a qualitative eye guide only.</p>
Full article ">Figure 5
<p>Correlation plot of the lungs’ <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>A</mi> <mi>D</mi> </mrow> <mo>¯</mo> </mover> </mrow> </semantics></math>, obtained from <span class="html-italic">MC</span> simulations with the Reference phantom (on the x-axis), compared with those obtained using the new lung VSV kernel (referred to as Lung_296), those obtained after a global correction based on the mean lung density of the Reference phantom (Lung_221), and those obtained after correcting for tissue heterogeneities according to Equation (3) (Lung_L, using <math display="inline"><semantics> <mrow> <mn>0.296</mn> <mtext> </mtext> <mi mathvariant="normal">g</mi> <mo>/</mo> <mi mathvariant="normal">c</mi> <msup> <mrow> <mi mathvariant="normal">m</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msup> </mrow> </semantics></math> as the uniform tissue density). For comparison, the SVOX_ST data (already presented in <a href="#applsci-14-07684-f004" class="html-fig">Figure 4</a>) are also included. For each data series, each point in the plot corresponds to an increasing <span class="html-italic">LS</span> value (10%, 20%, 30%, and 40%), with a line representing the linear interpolation of each dataset, provided as a qualitative visual guide only.</p>
Full article ">Figure 6
<p>From left to right, this figure shows an example of the activity biodistribution for the <span class="html-italic">LS</span> = 20% case and the corresponding <span class="html-italic">AD</span> distribution maps for the <span class="html-italic">MC</span> simulation. Also included are the <span class="html-italic">AD</span> distribution maps obtained from several convolution approaches for visual comparison. The colors used to represent the activity biodistribution are purely illustrative, indicating that the activity was uniformly distributed within each region (for further details, see <a href="#sec2dot1-applsci-14-07684" class="html-sec">Section 2.1</a>). The <span class="html-italic">AD</span> distributions are reported as Gy per GBq of administered activity. For Lung_296 and Lung_L, the <span class="html-italic">AD</span> distribution does not display any dose in the liver region, reflecting the computational choice to crop the activity map to the lung region only. Note that the <span class="html-italic">AD</span> distribution for Lung_296 is represented with a different color scale, from 0 to 40 Gy/GBq, compared to the other methods, which are shown with a scale from 0 to 120 Gy/GBq, because using the latter scale, the dose values would not have been visible.</p>
Full article ">
15 pages, 7467 KiB  
Article
Fabrication of ZnCo2O4-Zn(OH)2 Microspheres on Carbon Cloth for Photocatalytic Decomposition of Tetracycline
by Sin-Ei Juang, Ning-Chien Chin, Yu-Cheng Chang and Chia-Man Chou
Molecules 2024, 29(17), 4054; https://doi.org/10.3390/molecules29174054 - 27 Aug 2024
Viewed by 351
Abstract
Zinc cobalt oxide-zinc hydroxide (ZnCo2O4-Zn(OH)2) microspheres were successfully fabricated on carbon cloth via a sample hydrothermal method. The surface morphology of these microspheres and their efficacy in degrading methyl violet were further modulated by varying the thermal [...] Read more.
Zinc cobalt oxide-zinc hydroxide (ZnCo2O4-Zn(OH)2) microspheres were successfully fabricated on carbon cloth via a sample hydrothermal method. The surface morphology of these microspheres and their efficacy in degrading methyl violet were further modulated by varying the thermal annealing temperatures. Adjusting the thermal annealing temperatures was crucial for controlling the porosity of the ZnCo₂O₄-Zn(OH)₂ microspheres, enhancing their photocatalytic performance. Various analytical techniques were utilized to evaluate the physical and chemical properties of the ZnCo2O4-Zn(OH)2 microspheres, including field-emission scanning electron microscopy, energy-dispersive spectroscopy, X-ray diffraction, field-emission transmission electron microscopy, X-ray photoelectron spectroscopy, and UV-vis spectroscopy. Compared to untreated ZnCo2O4-Zn(OH)2 microspheres, those subjected to thermal annealing exhibited increased specific surface area and light absorption capacity, rendering them highly effective photocatalysts under UVC light exposure. Subsequent studies have confirmed the superior performance of ZnCo2O4-Zn(OH)2 microspheres as a reusable photocatalyst for degrading methyl violet and tetracycline. Furthermore, trapping experiments during the photodegradation process using ZnCo₂O₄-Zn(OH)₂ microspheres identified hydroxyl radicals (·OH) and superoxide radicals (·O₂⁻) as the primary reactive species. Full article
(This article belongs to the Section Nanochemistry)
Show Figures

Figure 1

Figure 1
<p>Describe the reaction mechanism and how to prepare ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres with the ratio of Zn/Co 1:2 on the carbon cloth.</p>
Full article ">Figure 2
<p>The FESEM images of (<b>a</b>) carbon cloth (without etching), (<b>b</b>) carbon cloth (etching), and ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres grown on the carbon cloth (<b>c</b>) without etching and (<b>d</b>) etching.</p>
Full article ">Figure 3
<p>The (<b>a</b>) FESEM and (<b>b</b>–<b>d</b>) FESEM-EDS mapping images of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres grown on the carbon cloth (etching).</p>
Full article ">Figure 4
<p>The FESEM images of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres grown on the carbon cloth under the different annealing temperatures. The annealing temperatures are (<b>a</b>) without, (<b>b</b>) 450 °C, (<b>c</b>) 550 °C, and (<b>d</b>) 650 °C, respectively.</p>
Full article ">Figure 5
<p>The XRD patterns of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres grown on the carbon cloth (<b>a</b>) without thermal annealing and (<b>b</b>) thermal annealing at 550 °C for 2 h, respectively.</p>
Full article ">Figure 6
<p>The (<b>a</b>) FETEM image, (<b>b</b>) SAED pattern, (<b>c</b>) HRTEM image, (<b>d</b>) EDS-mapping images of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres grown on the carbon cloth under the annealing temperature of 550 °C.</p>
Full article ">Figure 7
<p>XPS (<b>a</b>) survey, (<b>b</b>) Zn 2p, (<b>c</b>) Co 2p, and (<b>d</b>) O 1s spectra of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres under the annealing temperature of 550 °C.</p>
Full article ">Figure 8
<p>(<b>a</b>) Photocatalytic efficiency and (<b>b</b>) kinetic plot of as-prepared photocatalysts for MV solution under the UVC light irradiation.</p>
Full article ">Figure 9
<p>(<b>a</b>) Photocatalytic efficiency and (<b>b</b>) kinetic plot of the photocatalysts in treating TC solution under UVC light irradiation.</p>
Full article ">Figure 10
<p>Recycle experiments of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres for (<b>a</b>) MV and (<b>b</b>) TC solution under UVC light irradiation.</p>
Full article ">Figure 11
<p>XRD patterns of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres (550 °C) before (blue line) and after (purple line) four cycles of TC degradation.</p>
Full article ">Figure 12
<p>(<b>a</b>) UV-vis spectra and (<b>b</b>) Tauc plot of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres and ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres (550 °C).</p>
Full article ">Figure 13
<p>Photocatalytic activities of ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres (550 °C) for (<b>a</b>) MV (blue bar) and (<b>b</b>) TC (teal bar) solutions with four scavengers under UVC light irradiation. (<b>c</b>) Describe in detail the reaction mechanism for photocatalytic degradation of MV and TC using ZnCo<sub>2</sub>O<sub>4</sub>-Zn(OH)<sub>2</sub> microspheres.</p>
Full article ">
29 pages, 1862 KiB  
Review
Molecularly Imprinted Microspheres in Active Compound Separation from Natural Product
by Husna Muharram Ahadi, Firghi Muhammad Fardhan, Driyanti Rahayu, Rimadani Pratiwi and Aliya Nur Hasanah
Molecules 2024, 29(17), 4043; https://doi.org/10.3390/molecules29174043 - 26 Aug 2024
Viewed by 337
Abstract
Molecularly Imprinted Microspheres (MIMs) or Microsphere Molecularly Imprinted Polymers represent an innovative design for the selective extraction of active compounds from natural products, showcasing effectiveness and cost-efficiency. MIMs, crosslinked polymers with specific binding sites for template molecules, overcome irregularities observed in traditional Molecularly [...] Read more.
Molecularly Imprinted Microspheres (MIMs) or Microsphere Molecularly Imprinted Polymers represent an innovative design for the selective extraction of active compounds from natural products, showcasing effectiveness and cost-efficiency. MIMs, crosslinked polymers with specific binding sites for template molecules, overcome irregularities observed in traditional Molecularly Imprinted Polymers (MIPs). Their adaptability to the shape and size of target molecules allows for the capture of compounds from complex mixtures. This review article delves into exploring the potential practical applications of MIMs, particularly in the extraction of active compounds from natural products. Additionally, it provides insights into the broader development of MIM technology for the purification of active compounds. The synthesis of MIMs encompasses various methods, including precipitation polymerization, suspension polymerization, Pickering emulsion polymerization, and Controlled/Living Radical Precipitation Polymerization. These methods enable the formation of MIPs with controlled particle sizes suitable for diverse analytical applications. Control over the template-to-monomer ratio, solvent type, reaction temperature, and polymerization time is crucial to ensure the successful synthesis of MIPs effective in isolating active compounds from natural products. MIMs have been utilized to isolate various active compounds from natural products, such as aristolochic acids from Aristolochia manshuriensis and flavonoids from Rhododendron species, among others. Based on the review, suspension polymerization deposition, which is one of the techniques used in creating MIPs, can be classified under the MIM method. This is due to its ability to produce polymers that are more homogeneous and exhibit better selectivity compared to traditional MIP techniques. Additionally, this method can achieve recovery rates ranging from 94.91% to 113.53% and purities between 86.3% and 122%. The suspension polymerization process is relatively straightforward, allowing for the effective control of viscosity and temperature. Moreover, it is cost-effective as it utilizes water as the solvent. Full article
Show Figures

Figure 1

Figure 1
<p>Principle of MIP.</p>
Full article ">Figure 2
<p>General flow of MIP synthesis.</p>
Full article ">Figure 3
<p>Illustration of the ATRPP mechanism.</p>
Full article ">Figure 4
<p>Process of suspension polymerization.</p>
Full article ">
15 pages, 19396 KiB  
Article
Advancing Antimony(III) Adsorption: Impact of Varied Manganese Oxide Modifications on Iron–Graphene Oxide–Chitosan Composites
by Huinan Mo, Huimei Shan, Yuqiao Xu, Haimin Liao and Sanxi Peng
Molecules 2024, 29(17), 4021; https://doi.org/10.3390/molecules29174021 - 25 Aug 2024
Viewed by 428
Abstract
Antimony (Sb) is one of the most concerning toxic metals globally, making the study of methods for efficiently removing Sb(III) from water increasingly urgent. This study uses graphene oxide and chitosan as the matrix (GOCS), modifying them with FeCl2 and four MnO [...] Read more.
Antimony (Sb) is one of the most concerning toxic metals globally, making the study of methods for efficiently removing Sb(III) from water increasingly urgent. This study uses graphene oxide and chitosan as the matrix (GOCS), modifying them with FeCl2 and four MnOx to form iron–manganese oxide (FM/GC) at a Fe/Mn molar ratio of 4:1. FM/GC quaternary composite microspheres are prepared, showing that FM/GC obtained from different MnOx exhibits significant differences in the ability to remove Sb(III) from neutral solutions. The order of Sb(III) removal effectiveness is MnSO4 > KMnO4 > MnCl2 > MnO2. The composite microspheres obtained by modifying GOCS with FeCl2 and MnSO4 are selected for further batch experiments and characterization tests to analyze the factors and mechanisms influencing Sb(III) removal. The results show that the adsorption capacity of Sb(III) decreases with increasing pH and solid–liquid ratio, and gradually increases with the initial concentration and reaction time. The Langmuir model fitting indicates that the maximum adsorption capacity of Sb(III) is 178.89 mg/g. The adsorption mechanism involves the oxidation of the Mn-O group, which converts Sb(III) in water into Sb(V). This is followed by ligand exchange and complex formation with O-H in FeO(OH) groups, and further interactions with C-OH, C-O, O-H, and other functional groups in GOCS. Full article
Show Figures

Figure 1

Figure 1
<p>XRD (<b>a</b>), FTIR (<b>b</b>), and SEM (<b>c</b>) images of Fe@GC modified with different MnOx, and a comparison of adsorption capacities for Sb(III); comparison of removal effects for different MnO<sub>x</sub>-modified FM@GC on Sb (III) (<b>d</b>).</p>
Full article ">Figure 2
<p>Effects of solution pH (<b>a</b>), <span class="html-italic">m</span>/<span class="html-italic">v</span> ratio (<b>b</b>), initial solution concentration (<b>c</b>), reaction time (<b>d</b>), and coexisting ions (<b>e</b>) on the adsorption of Sb(III) by FM@GC.</p>
Full article ">Figure 3
<p>Fitting of adsorption kinetics models for FM@GC adsorption of Sb(III): (<b>a</b>) pseudo-first-order kinetics model; (<b>b</b>) pseudo-second-order kinetics model; (<b>c</b>) Weber–Morris intraparticle diffusion model; and (<b>d</b>) isothermal adsorption model fitting.</p>
Full article ">Figure 4
<p>FTIR (<b>a</b>), XRD (<b>b</b>) and SEM patterns of FM@GC before (<b>c</b>) and after (<b>d</b>) adsorption of Sb(III).</p>
Full article ">
Back to TopTop