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Search Results (15,697)

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10 pages, 2890 KiB  
Article
A Novel Method to Represent the Three-Dimensional Inclination of the Distal Radius Joint Surface
by Akira Ikumi, Reo Asai, Yusuke Eda, Tooru Uchida, Sho Kohyama, Takeshi Ogawa and Yuichi Yoshii
Diagnostics 2025, 15(3), 345; https://doi.org/10.3390/diagnostics15030345 (registering DOI) - 1 Feb 2025
Viewed by 53
Abstract
Objectives: This study aims to define three-dimensional (3D) parameters for the inclination of the distal radius joint surface. The goal is to develop standardized parameters for fracture reduction through comprehensive 3D evaluations of the joint surfaces. Methods: We analyzed 112 CT scans of [...] Read more.
Objectives: This study aims to define three-dimensional (3D) parameters for the inclination of the distal radius joint surface. The goal is to develop standardized parameters for fracture reduction through comprehensive 3D evaluations of the joint surfaces. Methods: We analyzed 112 CT scans of unaffected wrists (56 males and 56 females) to construct 3D models of the distal radius. Using 3D coordinates, the normal vectors and angles were calculated based on three reference points on the distal radius joint surface. These normal vector components were then converted into unit vector components A, B, and C for the x, y, and z axes, respectively. Additionally, the angles of these unit vectors were assessed in the xy, yz, and xz planes. The 3D measurements were compared between males and females and against traditional two-dimensional (2D) parameters such as palmar tilt and radial inclination. Results: For males, the unit vector components were as follows: A: −0.14 ± 0.09, B: −0.92 ± 0.02, and C: −0.36 ± 0.07; for females, A: −0.21 ± 0.08, B: −0.90 ± 0.03, and C: −0.36 ± 0.05. Significant differences were found between males and females for the A and B vector components (representing the palmar–dorsal and proximal–distal axes, p < 0.01). The angles of the unit vectors in the xy, yz, and xz planes were 8.9 ± 5.4°/12.9 ± 5.0°, 21.3 ± 4.1°/22.1 ± 3.2°, and 22.2 ± 14.8°/28.8 ± 10.1° for males and females, respectively. There were significant differences between males and females in the angles of the xy and xz planes (sagittal and axial planes, p < 0.01). Strong correlations were observed between the xy-plane vectors and palmar tilt (r = 0.96), as well as between the yz-plane vectors and radial inclination (r = 0.88). Conclusions: This study evaluated the 3D inclination of the distal radius joint surface, revealing significant gender differences. This method, which also allows for the assessment of rotational alignment—difficult with conventional techniques—is expected to be a key 3D parameter in treating distal radius fractures. Full article
(This article belongs to the Special Issue Recent Advances in Bone and Joint Imaging—2nd Edition)
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Figure 1
<p>Representative images for each reference point and normal vector. (1) Radial styloid process, (2) Volar edge of the sigmoid notch, (3) Dorsal edge of the sigmoid notch.</p>
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<p>Angles of vectors in the xy, yz, and xz planes. (<b>a</b>) Angle of vector in the yz-plane. (<b>b</b>) Angle of vector in the xy-plane. (<b>c</b>) Angle of vector in the xz-plane.</p>
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<p>Coordinates of three reference points in the axial plane (yz-plane). (<b>a</b>) Results of coordinates for males. (<b>b</b>) Results of coordinates for females. Orange dots indicate the radial styloid process: reference point (1). Gray dots indicate the sigmoid notch volar edge: reference point (2). Yellow dots indicate the sigmoid notch dorsal edge: reference point (3). Blue dots indicate the barycenter.</p>
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<p>Coordinates of three reference points in the sagittal plane (xy-plane). (<b>a</b>) Results of coordinates for males. (<b>b</b>) Results of coordinates for females. Orange dots indicate the radial styloid process: reference point (1). Gray dots indicate the sigmoid notch volar edge: reference point (2). Yellow dots indicate the sigmoid notch dorsal edge: reference point (3). Blue dots indicate the barycenter.</p>
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<p>The area of the plane enclosed by the three reference points. The area was significantly larger in males than in females (*: <span class="html-italic">p</span> &lt; 0.01).</p>
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<p>Correlation between the vector angles of the xy, yz, and xz planes. (<b>a</b>) Correlation between the vector angles of the xy-plane and yz-plane. (<b>b</b>) Correlation between the vector angles of the yz-plane and xz-plane. (<b>c</b>) Correlation between the vector angles of the xy-plane and xz-plane.</p>
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<p>Correlations between the vector angles of the xy and yz planes and 3D-PT and 3D-RI. (<b>a</b>) Correlation between the vector angle of the xy-plane and 3D-PT. (<b>b</b>) Correlation between the vector angle of yz-plane and 3D-RI.</p>
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15 pages, 3775 KiB  
Article
An Environmental Engineering Study Case: Constructing Cataluminescence Sensors Based on Octahedral Nanocomposites for Isovaleraldehyde Detection
by Bai Sun, Mao Cai, Guoji Shi, Yun Wang, Lining Bao, Qiang Zhao, Mingjian Yi and Shuguang Zhu
Molecules 2025, 30(3), 646; https://doi.org/10.3390/molecules30030646 (registering DOI) - 1 Feb 2025
Viewed by 110
Abstract
Isovaleraldehyde is an important chemical raw material for the production of flavors, which is volatile and flammable and poses a health risk to humans. It is, therefore, essential to develop a rapid assay for the identification of isovaleraldehyde. In this study, octahedral NiCo [...] Read more.
Isovaleraldehyde is an important chemical raw material for the production of flavors, which is volatile and flammable and poses a health risk to humans. It is, therefore, essential to develop a rapid assay for the identification of isovaleraldehyde. In this study, octahedral NiCo2O4/MIL-Fe53 nanocomposites were successfully fabricated for the rapid detection of isovaleraldehyde. The prepared NiCo2O4/MIL-Fe53 nanocomposites were characterized by SEM, XRD, FTIR, and XPS to analyze the material properties. The effects of temperature, carrier gas flow rate, selectivity, and stability on the cataluminescence performance of this sensor were investigated. The results showed that NiCo2O4/MIL-Fe53 nanocomposites have excellent selectivity to isovaleraldehyde with response and recovery times of 6 and 8 s, respectively. A linear relationship was found between the CTL signal and isovaleraldehyde concentration Y = 9.56X − 23.3 (R2 = 0.99) over the concentration range of 13.66 to 437.22 ppm with a detection limit of 2.44 ppm. The relative deviation RSD = 4.18% for multiple tests of the sensor indicates good stability and longevity. Mechanistic studies have shown that the heterojunction formed by NiCo2O4/MIL-Fe53 nanocomposites has the advantage of improving CTL sensing performance. This study may advance the application of cataluminescence sensors in the detection of isovaleraldehyde. Full article
(This article belongs to the Special Issue Nano-Functional Materials for Sensor Applications—2nd Edition)
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<p>(<b>A</b>) The SEM images of MIL-Fe<sub>53</sub>, (<b>B</b>) NiCo<sub>2</sub>O<sub>4</sub>, and (<b>C</b>) NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub>.</p>
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<p>(<b>A</b>) XRD patterns of NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> nanocomposites; (<b>B</b>) FTIR spectra of NiCo<sub>2</sub>O<sub>4</sub>, MIL-Fe<sub>53</sub>, and NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub>.</p>
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<p>(<b>A</b>) Adsorption isotherms of NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> nanocomposites; (<b>B</b>) pore size analysis plots of NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> nanocomposites.</p>
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<p>(<b>A</b>) XPS curves of fresh and used reaction NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub>; (<b>B</b>) high-resolution scan of O 1 s; (<b>C</b>) high-resolution scan of Fe 2p; (<b>D</b>) high-resolution scan of Co 2p; and (<b>E</b>) high-resolution scan of Ni 2p.</p>
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<p>(<b>A</b>) CTL signal intensities of NiCo<sub>2</sub>O<sub>4</sub>, NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> against isovaleraldehyde; (<b>B</b>) effect of working temperature on CTL signal intensity and S/N (concentration: 156.16 ppm; flow rate: 350 mL/min); (<b>C</b>) effect of carrier gas flow rate on CTL signal intensity and S/N (concentration: 156.16 ppm; temperature: 220 °C).</p>
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<p>(<b>A</b>) CTL response of the sensor to different compounds (temperature: 234 °C; flow rate: 300mL/min); (<b>B</b>) characterization of the response of the isovaleraldehyde sensor.</p>
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<p>(<b>A</b>) CTL intensities corresponding to different concentrations of isovaleraldehyde; (<b>B</b>) curve of isovaleraldehyde concentration versus signal intensity; (<b>C</b>) signal intensity of 10 tests of NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> sensor over 600s; and (<b>D</b>) signal intensity of NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> sensor tested over seven days.</p>
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<p>Reaction mechanism diagram of cataluminescence.</p>
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<p>Mechanism of heterojunctions in NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> nanocomposites.</p>
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<p>Diagram of the synthesized structure of NiCo<sub>2</sub>O<sub>4</sub>/MIL-Fe<sub>53</sub> and schematic diagram of the BPCL sensing device.</p>
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14 pages, 1968 KiB  
Article
Pathogenic Yersinia enterocolitica’s Contamination of Cheeks, Tongues, and Other Pork Meats at Retail in France, 2023
by Martine Denis, Arnaud Felten, Linda Ducret, Emmanuelle Houard, Manon Tasset, Delphine Novi and Marianne Chemaly
Appl. Microbiol. 2025, 5(1), 15; https://doi.org/10.3390/applmicrobiol5010015 (registering DOI) - 1 Feb 2025
Viewed by 108
Abstract
Pathogenic Y. enterocolitica’s contamination of cheeks, tongues, and other pork meats at retail was assessed in 2023, over 9 months. A total of 111 samples of cheeks, 104 of tongues, and 160 of fresh meat were taken at retail from the 13 [...] Read more.
Pathogenic Y. enterocolitica’s contamination of cheeks, tongues, and other pork meats at retail was assessed in 2023, over 9 months. A total of 111 samples of cheeks, 104 of tongues, and 160 of fresh meat were taken at retail from the 13 regions of mainland France. The level of contamination was 16.0%, with a higher contamination in tongues (39.4%), followed by cheeks (16.4%). Only one meat sample was contaminated. Of the 128 isolated strains, 97.6% were of the BT4 biotype. Depending on the method used to check the presence of the plasmid—yadA-PCR, CR-MOX testing, or sequencing—the results were not consistent for some strains, but most of the strains (≥ to 65%) had the virulent plasmid pYV. All the BT4 strains (except two strains) carried the sequence ST18; they were distributed in 54 cgMLST genotypes. The genetic diversity of the strains was very high, whatever the typing method used, including cgMLST, wgMLST, and cgSNP. There was higher contamination in tongues and cheeks, and lower contamination in meat, suggesting that the head deboning step is riskier than the evisceration step for contamination by pathogenic Y. enterocolitica. This pathogen remains a zoonotic agent of public health importance to be monitored in pigs. Full article
(This article belongs to the Special Issue Applied Microbiology of Foods, 2nd Edition)
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<p>The distribution of the samples in the 13 regions of mainland France.</p>
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<p>The strain Y23PE0281 (BT4, isolated from tongue) and strain Y23PE0341 (BT4, isolated from tongue) on CR-MOX after 28 h at 37 °C. In the absence of the plasmid, the colonies were colorless (strain Y23PE0281). The strain Y23PE0341 showed two types of colonies, colorless colonies and colonies that were orange–red pinheads, indicating the presence of the plasmid.</p>
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<p>The cgMLST tree from Enterobase of the 57 BT4 strains. The number on the branch indicates the allelic distance. Clusters were created when the allelic distance was ≤5. A total of 56 cgMLST genotypes were identified and could not all be presented on the tree.</p>
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<p>The cgSNP tree for the BT4 strains (<span class="html-italic">n</span> = 57). Strains were considered closely related when the allelic distance was ≤4 (with wgMLST, tree not shown) and the number of different SNPs was ≤10.</p>
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13 pages, 708 KiB  
Article
Halogen Bonding and Rearrangements in Complexes of N-Chlorosuccinimide with Halides
by Maison Hardin, Matthias Zeller and Sergiy V. Rosokha
Molecules 2025, 30(3), 639; https://doi.org/10.3390/molecules30030639 (registering DOI) - 31 Jan 2025
Viewed by 243
Abstract
The role of halogen bonding (HaB) in the reactions of N-chlorosuccinimide (SimCl), a versatile reagent in organic synthesis, was investigated through experimental and computational analyses of its interactions with halides. The reactions of SimCl with Br or I resulted in [...] Read more.
The role of halogen bonding (HaB) in the reactions of N-chlorosuccinimide (SimCl), a versatile reagent in organic synthesis, was investigated through experimental and computational analyses of its interactions with halides. The reactions of SimCl with Br or I resulted in the crystallization of HaB complexes of chloride with N-iodosuccinimide (SimI) or N-bromosuccinimide (SimBr). Computational analysis revealed that halogen rearrangements, which occurred even at −73 °C, were facilitated by halogen bonding. The dissociation of SimCl∙Y (Y = I or Br) complexes into a Sim + ClY pair (followed by the rotation and re-binding of the interhalogen molecules) bypassed the formation of the high-energy Sim + Cl⁺ pair and drastically (about tenfold) reduced the dissociation energy of the N–Cl bond. Furthermore, while the dissociation energy of individual SimCl is higher (and its HaB is weaker) compared to that of SimI or SimBr, the dissociation of the N-Cl bond in SimCl∙Y requires less energy than in the complexes of SimBr or SimI. The facile cleavage of such bonds in HaB complexes explains the high reactivity of SimCl and its effectiveness as a halogenating agent. Full article
19 pages, 6136 KiB  
Article
Numerical Simulation Study of the Motion Characteristics of Autonomous Underwater Vehicles During Mooring Lurking Procedure
by Yuyang Hu, Zhaoyong Mao, Bo Cheng, Bo Li and Wenlong Tian
J. Mar. Sci. Eng. 2025, 13(2), 275; https://doi.org/10.3390/jmse13020275 - 31 Jan 2025
Viewed by 233
Abstract
A two-dimensional coupled dynamics model for a moored autonomous underwater vehicle (AUV) was developed using the lumped mass method for mooring cable dynamics and the Newton-Euler method for rigid body dynamics. This model enables the integrated simulation of AUV motion, flow field interactions, [...] Read more.
A two-dimensional coupled dynamics model for a moored autonomous underwater vehicle (AUV) was developed using the lumped mass method for mooring cable dynamics and the Newton-Euler method for rigid body dynamics. This model enables the integrated simulation of AUV motion, flow field interactions, and mooring cable behavior. The study investigates the effects of varying ocean current velocities and mooring cable lengths on AUV motion responses. The results indicate that under the influence of mooring forces, the AUV stabilizes near its equilibrium position after release and undergoes periodic oscillatory motion. Specifically, when the X-direction oscillation completes two cycles and the Y-direction oscillation completes four cycles, the AUV demonstrates an 8-shaped trajectory, with maximum motion amplitudes observed. These findings provide insights into the dynamic behavior of moored AUVs in ocean environments, contributing to the design and operation of long-term underwater monitoring systems. Full article
(This article belongs to the Section Ocean Engineering)
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<p>(<b>a</b>) Physical model of anchored underwater vehicle; (<b>b</b>) cylinder system and the corresponding computational domain.</p>
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<p>Modelling of a dynamic mooring line.</p>
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<p>Grid distribution: (<b>a</b>) encrypted grid (I: static area; II: wake encrypted area; III: vibration encrypted area); (<b>b</b>) Grid of cylinder area (IV: square motion area).</p>
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<p>Solving process of the numerical solution process of the FSI.</p>
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<p>Numerical model validation: (<b>a</b>) comparison of vibration in y-direction; (<b>b</b>) comparison of cable tension in flow direction.</p>
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<p>The variation of cable force with time under different ocean current velocities. (<b>a</b>) <span class="html-italic">F<sub>cable_x</sub></span>; (<b>b</b>) <span class="html-italic">F<sub>cable_y</sub></span>.</p>
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<p>The variation of AUV position with time under different ocean current velocities. (<b>a</b>) X-position; (<b>b</b>) Y-position.</p>
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<p>Amplitude in the Y-direction at different ocean current velocities.</p>
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<p>The trajectory of the center-of-mass motion for three ocean current velocities. (<b>a</b>) <span class="html-italic">v</span> = 0.0486 m/s; (<b>b</b>) <span class="html-italic">v</span> = 0.0648 m/s; (<b>c</b>) <span class="html-italic">v</span> = 0.0809 m/s.</p>
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<p>Cloud diagrams of velocity field and vortex structure in different velocities.</p>
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<p>The variation of cable force with time under different cable lengths (<b>a</b>) <span class="html-italic">F<sub>cable_x</sub></span>; (<b>b</b>) <span class="html-italic">F<sub>cable_y</sub></span>.</p>
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<p>The variation of AUV position with time under different cable lengths. (<b>a</b>) X-position; (<b>b</b>) Y-position.</p>
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<p>Amplitude in the Y-direction at different cable lengths.</p>
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<p>The trajectory of the center-of-mass motion for three cable lengths. (<b>a</b>) <span class="html-italic">L</span> = 12 m; (<b>b</b>) <span class="html-italic">L</span> = 14 m; (<b>c</b>) <span class="html-italic">L</span> = 16 m.</p>
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<p>Cloud diagrams of velocity field and vortex structure in different cable lengths.</p>
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16 pages, 10739 KiB  
Article
Investigation of the Hysteresis Performance of Multi-Story Y-Shaped Eccentrically Bare Braced Steel Frame with Block Slit Damper (BSD)
by Chen Zhou, Haibo Wen, Jing Zhao, Lizhong Jiang, Xiaodong Xu, Hong Zheng, Yuxiao Tian, Muhua Liang, Xiyao Wang and Hai Zhang
Buildings 2025, 15(3), 451; https://doi.org/10.3390/buildings15030451 - 31 Jan 2025
Viewed by 284
Abstract
This paper investigated the hysteresis performance of multi-story Y-shaped eccentrically bare braced steel frames with block slit dampers (BSDs). After validating existing models through finite element (FE) analysis, an FE model of Y-shaped eccentrically bare braced steel frames (YEBFs) with BSD (BSD-YEBFs) was [...] Read more.
This paper investigated the hysteresis performance of multi-story Y-shaped eccentrically bare braced steel frames with block slit dampers (BSDs). After validating existing models through finite element (FE) analysis, an FE model of Y-shaped eccentrically bare braced steel frames (YEBFs) with BSD (BSD-YEBFs) was established. The influences of different types of BSDs on the hysteresis performance of YEBFs were subsequently analysed, as were the seismic performances of YEBFs with BSD (BSDF) and traditional Y-shaped eccentrically bare braced steel frames (TEBF) under cyclic loading, including the stress failure mode, hysteresis curve, stiffness, strength, and energy dissipation capacity. The results showed that: (1) compared with those of BASE-Y, the ductility coefficients of YEBFs with one level BSD (BSD-1) and two level BSD (BSD-2) increased by 59.57% and 39.47%, respectively, and the lateral bearing capacity decreased by 3.26% and 2.78%, respectively. (2) Compared with those of TEBF, the yield bearing capacity and ultimate bearing capacity of BSDF increased by 3.13% and 11.12%, respectively, and the ductility coefficient increased by 56.7%. Moreover, BSDF possesses higher initial stiffness and more sustained energy dissipation capabilities. Full article
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<p>Schematic diagram of steel frames and dampers.</p>
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<p>Dimensions of YEBF in reference [<a href="#B22-buildings-15-00451" class="html-bibr">22</a>] (unit: mm).</p>
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<p>Stress–strain relationship of steel.</p>
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<p>Boundary conditions.</p>
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<p>Loading protocol.</p>
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<p>Grid division of specimen Y-1.</p>
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<p>Failure mode of specimen Y-1.</p>
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<p>Comparison of hysteresis curves and backbone curves of specimen Y-1.</p>
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<p>Schematic diagram of BSD-YEBF (unit: mm).</p>
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<p>Schematic diagram of BSD-1 and BSD-2 (unit: mm).</p>
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<p>Grid division of BSD-YEBF structure.</p>
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<p>Force-displacement curves of specimens BASE-Y, BSD-1, and BSD-2.</p>
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<p>Grid division and boundary conditions of BSDF.</p>
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<p>Stress cloud of BSDF during cyclic loading process.</p>
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<p>Stress cloud of TEBF during cyclic loading process.</p>
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<p>Force-displacement curves for the BSDF and TEBF frames.</p>
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<p>Stiffness degradation curves.</p>
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<p>Strength degradation curves.</p>
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<p>Comparison of energy dissipation capacity.</p>
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14 pages, 13945 KiB  
Article
S-Bend and Y Waveguide Architectures in Germanate Glasses Irradiated by Femtosecond Laser
by Thiago Vecchi Fernandes, Camila Dias da Silva Bordon, Niklaus Ursus Wetter, Wagner de Rossi and Luciana Reyes Pires Kassab
Micromachines 2025, 16(2), 171; https://doi.org/10.3390/mi16020171 - 31 Jan 2025
Viewed by 281
Abstract
This study is focused on the fabrication and characterization of various dual waveguides through femtosecond (fs) laser irradiation of GeO2-based glass samples. The objective of the present work is to develop diverse waveguide configurations, namely straight, S-bend and Y-shaped waveguides within [...] Read more.
This study is focused on the fabrication and characterization of various dual waveguides through femtosecond (fs) laser irradiation of GeO2-based glass samples. The objective of the present work is to develop diverse waveguide configurations, namely straight, S-bend and Y-shaped waveguides within GeO2–PbO glasses embedded with silver nanoparticles, utilizing a double-guide platform, for photonic applications such as resonant rings and beam splitters. Enhanced guidance was observed with a larger radius of curvature (80 mm) among the two distinct S-bend waveguides produced. The maximum relative propagation loss was recorded for the S-bend waveguide with a 40 mm radius, while the minimum loss was noted for the Y-shaped waveguide. In the latter configuration, with an opening angle of 5° and a separation of 300 µm between the two arms, an output power ratio of 50.5/49.5 between the left and right arms indicated promising potential for beam splitter applications. During the study, the quality factor (M2) of the proposed architectures was measured and the 80 mm S-bend configuration presented the best symmetry between the x and y axes; in the case of the Y configuration the similarity between the M2 values in both axes, for the first and second arms, indicates comparable light guidance. Full article
(This article belongs to the Special Issue Laser Micro/Nano Fabrication, Second Edition)
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Figure 1
<p>Illustration of waveguide architectures in GeO<sub>2</sub>-PbO glass irradiated with a femtosecond laser: (<b>a</b>) straight, S-bend with (<b>b</b>) 40 mm, (<b>c</b>) 80 mm radius and (<b>d</b>) Y-shaped.</p>
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<p>Illustration of the arrangement used for writing waveguides. Microscopy images of the damage caused by the laser at the time of writing on the entry and exit faces of the glass are shown.</p>
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<p>Experimental setup used to measure (<b>a</b>) propagation loss; (<b>b</b>) M<sup>2</sup>.</p>
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<p>Experimental setup used for measurements of polarization of dual waveguides.</p>
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<p>Results for the GP sample with a straight waveguide and a 10 µm separation between the guide walls (<b>a</b>) Mx<sup>2</sup> (<b>b</b>) My<sup>2</sup>.</p>
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<p>Results for the S-bend waveguide with 40 mm radius (<b>a</b>) Mx<sup>2</sup> (<b>b</b>) My<sup>2</sup>.</p>
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<p>Results for the S-bend waveguide with 80 mm radius (<b>a</b>) Mx<sup>2</sup> (<b>b</b>) My<sup>2</sup>.</p>
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<p>Results for the first arm of the Y-shaped waveguide (<b>a</b>) Mx<sup>2</sup> (<b>b</b>) My<sup>2</sup>.</p>
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<p>Results for the second arm of the Y-shaped waveguide (<b>a</b>) Mx<sup>2</sup> (<b>b</b>) My<sup>2</sup>.</p>
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<p>(<b>a</b>) Top view of the region of curvature of the S-bend waveguide with 40 mm radius. (<b>b</b>) View of the mode of the S-bend waveguide with 40 mm radius.</p>
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<p>(<b>a</b>) Top view of the region of curvature of the S-bend waveguide with 80 mm radius. (<b>b</b>) View of the mode of the S-bend waveguide with 80 mm radius.</p>
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<p>(<b>a</b>) Top view of the region of the aperture of the Y-shaped architecture. (<b>b</b>) Simultaneous view of the Y modes.</p>
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<p>Absorbance in the visible range for GP samples with and without silver nanoparticles.</p>
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<p>(<b>a</b>,<b>b</b>) TEM images of the GP2Ag sample with silver nanoparticles. (<b>c</b>) TEM image of an isolated silver nanoparticle with the interplanar distance corresponding to the crystalline plane (1,1,1) of a face centered cubic silver. (<b>d</b>) Size distribution of silver nanoparticles.</p>
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<p>STEM images show the spatial distribution of (<b>a</b>) Ge, (<b>b</b>) Pb, (<b>c</b>) Ag and (<b>d</b>) O in the sample.</p>
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15 pages, 10612 KiB  
Article
Enhanced Performance of Austenitic Oxide Dispersion-Strengthened 316L Steel: A Study on Y2O3 Reinforcement and Corrosion Behaviour
by Jan Pokorný, Jiří Kubásek, Črtomir Donik, David Nečas, Vojtěch Hybášek, Jaroslav Fojt, Anna Dobkowska, Irena Paulin, Jaroslav Čapek and Matjaž Godec
Materials 2025, 18(3), 641; https://doi.org/10.3390/ma18030641 - 31 Jan 2025
Viewed by 313
Abstract
This study explores the mechanical and corrosion properties of yttria-reinforced 316L stainless steel. Powder precursor materials were prepared using mechanical alloying. Varying yttria (Y2O3) contents (1, 3, and 5 wt%) were used to assess its impact on the steel’s [...] Read more.
This study explores the mechanical and corrosion properties of yttria-reinforced 316L stainless steel. Powder precursor materials were prepared using mechanical alloying. Varying yttria (Y2O3) contents (1, 3, and 5 wt%) were used to assess its impact on the steel’s properties. X-ray diffraction and scanning electron microscopy confirmed the successful dispersion of Y2O3 within the matrix, with the formation of chromium carbides during spark plasma sintering (SPS). The mechanical properties, including hardness and compressive yield strength, improved with increasing Y2O3 contents, with the highest strength observed in the 316L-5Y2O3 sample. However, corrosion resistance decreased with higher yttria concentrations. The 3 wt% Y2O3 sample exhibited the highest corrosion rate due to localized corrosion in areas enriched with oxide particles and chromium carbides. Electrochemical testing revealed that carbide formation and Cr-depleted regions from SPS processing contributed to the corrosion behaviour. These findings suggest that while yttria reinforcement enhances mechanical strength, optimizing the Y2O3 content and processing methods is crucial to balance both mechanical and corrosion performance in ODS 316L stainless steel. Full article
(This article belongs to the Section Advanced Materials Characterization)
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<p>(<b>a</b>) XRD patterns of MA powders; (<b>b</b>) particle size distribution of MA powders.</p>
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<p>SEM micrographs of mechanically alloyed powders: (<b>a</b>) 316L-1Y<sub>2</sub>O<sub>3</sub>; (<b>b</b>) 316L-3 Y<sub>2</sub>O<sub>3</sub>; (<b>c</b>) 316L-5 Y<sub>2</sub>O<sub>3</sub>.</p>
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<p>XRD patterns of consolidated samples.</p>
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<p>(<b>a</b>–<b>c</b>) General microstructure of consolidated materials (red ellipses-Y<sub>2</sub>O<sub>3</sub> bands); (<b>d</b>–<b>f</b>) close-up images of consolidated materials (red arrows—oxide particles; green arrows—Cr<sub>23</sub>C<sub>6</sub>), with varying yttria contents: (<b>a</b>,<b>d</b>) 1 wt %; (<b>b</b>,<b>e</b>) 3 wt %; (<b>c</b>,<b>f</b>) 5 wt %.</p>
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<p>(<b>a</b>–<b>c</b>) EBSD IPF maps of consolidated materials; (<b>d</b>–<b>f</b>) phase distribution maps of consolidated materials—carbides are in green, austenite in red, with varying Y<sub>2</sub>O<sub>3</sub> contents: (<b>a</b>,<b>d</b>) 1 wt %; (<b>b</b>,<b>e</b>) 3 wt %; (<b>c</b>,<b>f</b>) 5 wt %. IPF maps corresponds to the Z axis which is parallel to the vertical axis of the SPSed sample. Both austenite and carbide phase have similar fcc structure; therefore, they are not distinguished in the IPF map.</p>
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<p>Hardness chart of consolidated materials.</p>
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<p>(<b>a</b>) Stress–strain curves of austenitic ODS steel at 25 °C for varying Y<sub>2</sub>O<sub>3</sub> contents; (<b>b</b>) stress–strain curves of austenitic ODS steel at 600 °C for varying Y<sub>2</sub>O<sub>3</sub> contents.</p>
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<p>Potentiodynamic curves.</p>
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<p>EPR-SL curves of consolidated materials.</p>
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<p>SEM surface micrographs of the materials after exposure: (<b>a</b>) 316L (SPS); (<b>b</b>) 316L-1Y<sub>2</sub>O<sub>3</sub>; (<b>c</b>) 316L-3Y<sub>2</sub>O<sub>3</sub>.</p>
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12 pages, 410 KiB  
Article
Nut Consumption Is Associated with Cognitive Status in Southern Italian Adults
by Justyna Godos, Francesca Giampieri, Evelyn Frias-Toral, Raynier Zambrano-Villacres, Angel Olider Rojas Vistorte, Vanessa Yélamos Torres, Maurizio Battino, Fabio Galvano, Sabrina Castellano and Giuseppe Grosso
Nutrients 2025, 17(3), 521; https://doi.org/10.3390/nu17030521 - 30 Jan 2025
Viewed by 281
Abstract
Background: Nut consumption has been considered a potential protective factor against cognitive decline. The aim of this study was to test whether higher total and specific nut intake was associated with better cognitive status in a sample of older Italian adults. Methods: A [...] Read more.
Background: Nut consumption has been considered a potential protective factor against cognitive decline. The aim of this study was to test whether higher total and specific nut intake was associated with better cognitive status in a sample of older Italian adults. Methods: A cross-sectional analysis on 883 older adults (>50 y) was conducted. A 110-item food frequency questionnaire was used to collect information on the consumption of various types of nuts. The Short Portable Mental Status Questionnaire was used to assess cognitive status. Multivariate logistic regression analyses were performed to calculate odds ratios (ORs) and 95% confidence intervals (CIs) for the association between nut intake and cognitive status after adjusting for potential confounding factors. Results: The median intake of total nuts was 11.7 g/day and served as a cut-off to categorize low and high consumers (mean intake 4.3 g/day vs. 39.7 g/day, respectively). Higher total nut intake was significantly associated with a lower prevalence of impaired cognitive status among older individuals (OR = 0.35, CI 95%: 0.15, 0.84) after adjusting for potential confounding factors. Notably, this association remained significant after additional adjustment for adherence to the Mediterranean dietary pattern as an indicator of diet quality, (OR = 0.32, CI 95%: 0.13, 0.77). No significant associations were found between cognitive status and specific types of nuts. Conclusions: Habitual nut intake is associated with better cognitive status in older adults. Full article
(This article belongs to the Special Issue Nuts for Human: The Role of Nuts in a Healthy Diet)
20 pages, 7054 KiB  
Article
High-Pressure Hydrogen Charge Check-Valve Energy Loss-Based Correlation Analysis Affecting Internal Flow Characterizations
by Seung-Hun Oh, Sun-Min Jang and Hyun-Kyu Suh
Appl. Sci. 2025, 15(3), 1428; https://doi.org/10.3390/app15031428 (registering DOI) - 30 Jan 2025
Viewed by 283
Abstract
In this study, we analyzed changes in flow characteristics and energy-dissipation characteristics due to changes in hydrogen temperature and inlet/outlet differential pressure in a check valve, which affect the storage safety and reliability of high-pressure hydrogen refueling systems. The effects of flow separation [...] Read more.
In this study, we analyzed changes in flow characteristics and energy-dissipation characteristics due to changes in hydrogen temperature and inlet/outlet differential pressure in a check valve, which affect the storage safety and reliability of high-pressure hydrogen refueling systems. The effects of flow separation and recirculation flow generation at the back end of the valve were investigated, and the pressure, flow rate, pressure coefficient, and energy dissipation at the core part (where the hydrogen inflow is blocked) and the outlet part (where the hydrogen is discharged) were numerically analyzed. The hydrogen-inlet temperature (Tin) was selected as 233 K, 293 K, and 363 K, and the differential pressure (∆P) was selected in the range of 2 to 10 MPa in 2 MPa steps. To ensure the reliability of the numerical results, mesh dependence was performed, and the effect of the mesh geometry on the results was less than 2%. The numerical simulation results showed that the hydrogen introduced into the core part is discharged into the discharge part, and the pressure decreases by up to 6% and the velocity increases by up to 16% at the 95 mm position of the L-shaped curved tube. In addition, for the hydrogen-inlet temperature of 233 K in the L-shaped curved tube, the flow velocity decreases by up to 60% and the pressure coefficient increases at the 2.3 mm point in the Y-axis direction, indicating that the main flow area is biased towards the bottom of the valve due to the constriction of the veins caused by flow separation. The TDR results showed that the hydrogen discharge to the discharge region increased by 96% at 95 mm compared to 90 mm, and the turbulent kinetic energy of the hydrogen was dissipated, resulting in a temperature increase of up to 4.5 K. The exergy destruction was maximized in the core region where flow separation occurs, indicating that the pressure, velocity, and TDR changes due to flow separation and recombination have a significant impact on the energy loss of the flow in the check valve. Full article
23 pages, 2309 KiB  
Article
Large Losses of Pyrogenic Carbon (Biochar) and Native Soil Carbon During a 15-Month Field Study in North Florida, USA
by Jing Lyu and Andrew R. Zimmerman
Agriculture 2025, 15(3), 300; https://doi.org/10.3390/agriculture15030300 - 30 Jan 2025
Viewed by 292
Abstract
Although the application of biochar to soils has been proposed as a method of carbon sequestration for climate mitigation while improving crop yields, losses of biochar carbon (BC) through mineralization may reduce these benefits. However, few field studies have been conducted that control [...] Read more.
Although the application of biochar to soils has been proposed as a method of carbon sequestration for climate mitigation while improving crop yields, losses of biochar carbon (BC) through mineralization may reduce these benefits. However, few field studies have been conducted that control for biochar migration so that the rates and processes of BC remineralization from soils, as well as the effects of biochar on native soil organic carbon, can be accurately determined. Here, biochar made from different biomass types (oak, pine wood, and grass) and temperatures (lightly charred at 250 °C and pyrolyzed at 400 and 650 °C) were added to fine sandy Entisol in an open agricultural field and Spodosol in a shaded forested site in North Central Florida. After 15 months, BC losses, determined by the Kurth–Mackenzie–Deluca chemical–thermal oxidation method, ranged from 17.5 to 93.3% y−1 (14.0–51.5% y−1 for the 650 °C biochar). These losses were correlated with but much greater than the 0.4–3% y−1 BC losses recorded in a one-year laboratory study using the same biochars and those of several previous field studies (1–14% y−1). The losses of non-BC native carbon stocks (i.e., positive priming) also varied with biochar and soil type and ranged from 1.5 to 15.8% y−1. The high BC losses observed in this study may be attributed to the subtropical and temporally variable climate conditions at the study site. Greater efforts should be made to base BC long-term stability estimates on field studies that monitor or control for biochar migration rather than reliance only upon laboratory incubations. Full article
(This article belongs to the Section Agricultural Soils)
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<p>Biochar carbon content in agricultural soil (AS) soil–biochar treatments before (initial) and following (final) 15-month field incubation in irrigated and non-irrigated plots (means and standard deviations shown). Different letters above bars indicate treatments with significantly different means (<span class="html-italic">p</span> &lt; 0.05) within each treatment type.</p>
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<p>Biochar carbon content in forest soil (FS) soil–biochar treatments before (initial) and following (final) 15-month field incubation (means and standard deviations shown). Different letters above bars indicate treatments with significantly different means (<span class="html-italic">p</span> &lt; 0.05) within each treatment type.</p>
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<p>Boxplot of BC %Loss in agricultural soil (AS) and forest soil (FS) soil–biochar treatments with two-way ANOVA comparisons of biochars of different biomass and pyrolysis temperature. (<b>a</b>) agricultural soil (AS) biochar type and (<b>b</b>) temperature, forest soil (FS) by (<b>c</b>) biochar type and (<b>d</b>) temperature. ‘ns’ indicates a non-significant difference.</p>
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<p>Native soil C (non-BC) in agricultural soil (AS) soil–biochar treatments before (initial) and following (final) 15-month field incubation in irrigated and non-irrigated plots (means and standard deviations shown). Different letters above bars indicate treatments with significantly different means (<span class="html-italic">p</span> &lt; 0.05) within each treatment type.</p>
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<p>Native soil C (non-BC) in forest soil (FS) soil–biochar treatments before (initial) and following (final) 15-month field incubation (means and standard deviations shown). Different letters above bars indicate treatments with significantly different means (<span class="html-italic">p</span> &lt; 0.05) within each treatment type.</p>
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<p>Boxplots of native soil C (non-BC) %Loss in agricultural soil (AS) by (<b>a</b>) biochar type and (<b>b</b>) temperature, and forest soil (FS) by (<b>c</b>) biochar type and (<b>d</b>) temperature. Treatments are compared via two-way ANOVA. ‘ns’ indicates a non-significant difference.</p>
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<p>Comparison of laboratory versus field-based biochar carbon (BC) mineralization rates from this and previous studies including one [<a href="#B24-agriculture-15-00300" class="html-bibr">24</a>] using the same biochars as this study. Studies included are those that published H/C<sub>org</sub> biochar values. Raw data and sources used.</p>
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16 pages, 1607 KiB  
Article
P2Y1 and P2Y12 Receptors Mediate Aggregation of Dog and Cat Platelets: A Comparison to Human Platelets
by Reece A. Sophocleous, Stephen J. Curtis, Belinda L. Curtis, Lezanne Ooi and Ronald Sluyter
Int. J. Mol. Sci. 2025, 26(3), 1206; https://doi.org/10.3390/ijms26031206 - 30 Jan 2025
Viewed by 305
Abstract
Thrombosis is one of the most prevalent and serious health issues amongst humans. A key component of thrombotic events is the activation and aggregation of platelets, of which the P2Y1 and P2Y12 receptors play a crucial role in this process. Despite [...] Read more.
Thrombosis is one of the most prevalent and serious health issues amongst humans. A key component of thrombotic events is the activation and aggregation of platelets, of which the P2Y1 and P2Y12 receptors play a crucial role in this process. Despite a breadth of knowledge on thrombosis and its mechanisms and treatment in various disorders in humans, there is less of an understanding of the expression and exact role of these receptors in companion animals such as dogs and cats. Therefore, this study aimed to investigate P2Y1 and P2Y12 receptors on dog and cat platelets in platelet-rich plasma and compare them to human platelets. Immunoblotting revealed the presence of P2Y1 and P2Y12 receptor proteins on dog and cat platelets, although relative amounts of each receptor appeared to contrast those of human platelets, with increased amounts of P2Y1 compared to P2Y12 receptors in dogs and cats. Using a modified 384-well plate aggregation assay, designed for use with small volumes, the human P2Y1 and P2Y12 receptor agonists adenosine 5′-diphosphate and 2-methylthio-adenosine 5′-diphosphate caused aggregation of dog and cat platelets. This aggregation was near-completely inhibited by the selective P2Y12 antagonist ticagrelor. Aggregation of dog and cat platelets was partly inhibited by the human P2Y1 receptor antagonist MRS2179. The agonist and antagonist responses in dog and cat platelets were like those of human platelets. In contrast, the aggregation of dog platelets in the absence of added nucleotides was two-fold greater than that of cats and humans. This study indicates that platelets of cats and dogs possess functional P2Y1 and P2Y12 receptors that can be inhibited by human antagonists. The data presented suggest differing roles or responses of the platelet P2Y receptors in dogs and cats compared to humans but also highlight the potential of using currently available P2Y1 or P2Y12 antiplatelet drugs such as ticagrelor for the treatment of thrombosis in these companion animals. Full article
(This article belongs to the Special Issue Purinergic Signalling in Physiology and Pathophysiology 2.0)
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<p>Presence of P2Y<sub>1</sub> and P2Y<sub>12</sub> in dog, cat, and human platelets. (<b>A</b>,<b>B</b>) PRP was isolated from the whole blood of dogs, cats, or humans to obtain platelets. Whole lysates of platelets were analysed by immunoblotting using an (<b>A</b>) anti-P2Y<sub>1</sub> or (<b>B</b>) anti-P2Y<sub>12</sub> receptor antibody (top panels) or (<b>A</b>,<b>B</b>) anti-actin antibody (bottom panels). Arrows indicate (<b>A</b>) P2Y<sub>1</sub> or (<b>B</b>) P2Y<sub>12</sub> receptors. Results are representative of three independent experiments.</p>
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<p>ADP and 2MeSADP activate platelets from dogs, cats, or humans in a concentration-dependent manner. PRP and PPP, isolated from the whole blood of (<b>A</b>) dogs, (<b>B</b>) cats, or (<b>C</b>) humans, were incubated in the absence (Tyrode’s buffer) or presence of ADP or 2MeSADP (as indicated), and platelet aggregation was determined. Concentration–response curves were plotted based on the percent of nucleotide-induced aggregation calculated for each PRP sample, relative to the percent of nucleotide-induced aggregation in the corresponding PPP sample after a 10 min incubation. Data are mean ± SEM from three independent experiments.</p>
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<p>Ticagrelor inhibits ADP- and 2MeSADP-induced aggregation of dog, cat, or human platelets in a concentration-dependent manner. PRP and PPP, isolated from (<b>A</b>) dog, (<b>B</b>) cat, or (<b>C</b>) human whole blood, were pre-incubated in the absence (control; 0.1% DMSO in Tyrode’s buffer) or presence of ticagrelor (as indicated) for 15 min then incubated in the absence (Tyrode’s buffer) or presence of 3 µM ADP or 10–30 nM 2MeSADP (approximate EC<sub>80</sub> as determined for each species), and platelet aggregation was measured. Concentration–response curves were plotted using nucleotide-induced percent of aggregation calculated for each PRP sample relative to the percent of nucleotide-induced aggregation in the corresponding PPP sample after 10 min incubation and then normalised to the percent of nucleotide-induced aggregation in the absence of ticagrelor. Data shown for each species are mean ± SEM from three independent experiments.</p>
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<p>MRS2179 partly inhibits ADP- and 2MeSADP-induced aggregation of dog, cat, or human platelets in a concentration-dependent manner. PRP and PPP, isolated from (<b>A</b>) dog, (<b>B</b>) cat, or (<b>C</b>) human whole blood, were pre-incubated in the absence (control; Tyrode’s buffer) or presence of MRS2179 (as indicated) for 15 min then incubated in the absence (Tyrode’s buffer) or presence of 3 µM ADP or 10–30 nM 2MeSADP (approximate EC<sub>80</sub> as determined for each species), and platelet aggregation was measured. Concentration–response curves were plotted using nucleotide-induced percent of aggregation calculated for each PRP sample relative to the percent of nucleotide-induced aggregation in the corresponding PPP sample after 10 min incubation and then normalised to the percent of nucleotide-induced aggregation in the absence of MRS2179. Data shown for each species are mean ± SEM from three independent experiments.</p>
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<p>Variation in aggregation between dog, cat, and human platelets. Percent aggregation data in the absence (basal) or presence of (<b>A</b>,<b>C</b>) 3 µM ADP or (<b>B</b>,<b>D</b>) 10 nM (dog and cat) or 30 nM (human) 2MeSADP. Data were compared (<b>A</b>,<b>B</b>) after 10 min of aggregation and (<b>C</b>,<b>D</b>) after 45 min of aggregation (used throughout to plot concentration–response curves) using a two-way ANOVA with Bonferroni multiple comparisons test; ** <span class="html-italic">p</span> &lt; 0.01 and *** <span class="html-italic">p</span> &lt; 0.001 compared to corresponding basal, <sup>†††</sup> <span class="html-italic">p</span> &lt; 0.001 compared to dog basal, <sup>#</sup> <span class="html-italic">p</span> &lt; 0.05 and <sup>###</sup> <span class="html-italic">p</span> &lt; 0.001 compared to dog ADP or 2MeSADP, <sup>‡</sup> <span class="html-italic">p</span> &lt; 0.05 and <sup>‡‡‡</sup> <span class="html-italic">p</span> &lt; 0.001 compared to cat ADP or 2MeSADP. Data shown for each species are mean percent of platelet aggregation relative to PPP ± SEM from nine independent experiments, where data are derived from samples studied in <a href="#ijms-26-01206-f002" class="html-fig">Figure 2</a>, <a href="#ijms-26-01206-f003" class="html-fig">Figure 3</a> and <a href="#ijms-26-01206-f004" class="html-fig">Figure 4</a>.</p>
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19 pages, 5606 KiB  
Article
Static Calibration of a New Three-Axis Fiber Bragg Grating-Based Optical Accelerometer
by Abraham Perez-Alonzo, Luis Alvarez-Icaza and Gabriel E. Sandoval-Romero
Sensors 2025, 25(3), 835; https://doi.org/10.3390/s25030835 - 30 Jan 2025
Viewed by 255
Abstract
Optical sensors are a promising technology in structural and health monitoring due to their high sensitivity and immunity to electromagnetic interference. Because of their high sensitivity, they can register the responses of buildings to a wide range of motions, including those induced by [...] Read more.
Optical sensors are a promising technology in structural and health monitoring due to their high sensitivity and immunity to electromagnetic interference. Because of their high sensitivity, they can register the responses of buildings to a wide range of motions, including those induced by ambient noise, or detect small structural changes caused by aging or environmental factors. In previous work, an FBG-based accelerometer was introduced that is suitable for use as an autonomous unit since it does not make use of any interrogator equipment. In this paper, we present the results of the characterization of this device, which yielded the best precision and accuracy. The results show the following: (i) improvements in the orthogonality of the sensor axes, which impact their cross-axis sensitivity; (ii) reductions in the electronic noise, which increase the signal-to-noise ratio. The results of our static characterization show that, in the worst case, we can obtain a correlation coefficient R2 of 0.9999 when comparing the output voltage with the input acceleration for the X- and Y-axes of the sensor. We developed an analytical, non-iterative, 12-parameter matrix calibration approach based on the least-squares method, which allows compensation for different gains in its axes, offset, and cross-axis. To improve the accuracy of our sensor, we propose a table with correction terms that can be subtracted from the estimated acceleration. The mean error of each estimated acceleration component of the sensor is zero, with a maximum standard deviation of 0.018 m/s2. The maximum RMSE for all tested positions is 6.7 × 10−3 m/s2. Full article
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<p>Tilting platform in pitch and roll rotations. The optical sensor is placed on top of the platform. The coordinate system is shown on the right of the figure.</p>
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<p>Dependence of the FBGs of our prototype on temperature: (<b>a</b>) apart from an offset, the sensitivity in all FBGs is different; (<b>b</b>) the Bragg wavelength of sensing FBGs is adjusted by a factor and an offset; now all FBGs show the same trend.</p>
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<p>Changes in Bragg wavelength due to temperature over 17 h at laboratory room temperature. Measurements were made with a sampling period of 0.1 s, and a simple moving average with a window size of 5 was applied to the data.</p>
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<p>Vibration is applied to the tilting platform to which our sensor is attached; it can be noted that the reference FBG is not affected by such vibration: (<b>a</b>) vibration applied in a preferred direction; the X-, Y-, or Z-axis; (<b>b</b>) vibration applied in arbitrary directions.</p>
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<p>Response in wavelength of the FBGs used in our prototype with respect to tilt. The tilt is referenced to the horizontal plane; two sweeps were performed: one forward and one backward. (<b>a</b>) The sensor is rotated about its X-axis; (<b>b</b>) the sensor is rotated about its Y-axis.</p>
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<p>Response in wavelength of the FBGs used in our prototype with temperature compensation. The tilt is referenced to the horizontal plane; the temperature compensation was performed with respect to the reference FBG: (<b>a</b>) the sensor is rotated about its X-axis; (<b>b</b>) the sensor is rotated about its Y-axis.</p>
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<p>Response of the sensing FBG of our sensor, the horizontal axis of the plot was converted to acceleration by using the sine function of the tilt angle for the X- and Y-axes and the cosine function for the Z-axis. In the Z-axis, the magnitude of the gravity vector is subtracted from the measurements: (<b>a</b>) the sensor is rotated about its X-axis; (<b>b</b>) the sensor is rotated about its Y-axis.</p>
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<p>Sensor output in voltage at the final sensor stage with respect to the input acceleration: (<b>a</b>) rotation about the X-axis; (<b>b</b>) rotation about the Y-axis.</p>
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<p>Absolute acceleration error comparing the theoretical acceleration due to each tilt angle with the estimated acceleration using the sensor output voltages: (<b>a</b>) the sensor is rotated about its X-axis; (<b>b</b>) the sensor is rotated about its Y-axis.</p>
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<p>Absolute acceleration error after subtracting the mean error for each sensor orientation: (<b>a</b>) X-axis response to roll rotation; (<b>b</b>) X-axis response to pitch rotation; (<b>c</b>) Y-axis response to roll rotation; (<b>d</b>) Y-axis response to pitch rotation; (<b>e</b>) Z-axis response to roll rotation; (<b>f</b>) Z-axis response to pitch rotation.</p>
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<p>Absolute acceleration error after subtracting the mean error for each sensor orientation: (<b>a</b>) X-axis response to roll rotation; (<b>b</b>) X-axis response to pitch rotation; (<b>c</b>) Y-axis response to roll rotation; (<b>d</b>) Y-axis response to pitch rotation; (<b>e</b>) Z-axis response to roll rotation; (<b>f</b>) Z-axis response to pitch rotation.</p>
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<p>Absolute acceleration error, between the magnitude of the calibrated output of the accelerometer and the magnitude of the gravity field, and their respective RMSEs: (<b>a</b>) errors before subtracting the correction term; (<b>b</b>) errors after subtracting the correction term.</p>
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<p>Electrical noise present at the output of the accelerometer electronic stage in a 60 s window.</p>
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48 pages, 1898 KiB  
Essay
The Code Underneath
by Julio Rives
Axioms 2025, 14(2), 106; https://doi.org/10.3390/axioms14020106 - 30 Jan 2025
Viewed by 189
Abstract
An inverse-square probability mass function (PMF) is at the Newcomb–Benford law (NBL)’s root and ultimately at the origin of positional notation and conformality. PrZ=2Z2, where ZZ+. Under its tail, we find information [...] Read more.
An inverse-square probability mass function (PMF) is at the Newcomb–Benford law (NBL)’s root and ultimately at the origin of positional notation and conformality. PrZ=2Z2, where ZZ+. Under its tail, we find information as harmonic likelihood Ls,t=Ht1Hs1, where Hn is the nth harmonic number. The global Q-NBL is Prb,q=Lq,q+1L1,b=qHb11, where b is the base and q is a quantum (1q<b). Under its tail, we find information as logarithmic likelihood i,j=lnji. The fiducial R-NBL is Prr,d=d,d+11,r=logr1+1d, where rb is the radix of a local complex system. The global Bayesian rule multiplies the correlation between two numbers, s and t, by a likelihood ratio that is the NBL probability of bucket s,t relative to b’s support. To encode the odds of quantum j against i locally, we multiply the prior odds Prb,jPrb,i by a likelihood ratio, which is the NBL probability of bin i,j relative to r’s support; the local Bayesian coding rule is o˜j:i|r=ijlogrji. The Bayesian rule to recode local data is o˜j:i|r=o˜j:i|rlnrlnr. Global and local Bayesian data are elements of the algebraic field of “gap ratios”, ABCD. The cross-ratio, the central tool in conformal geometry, is a subclass of gap ratio. A one-dimensional coding source reflects the global Bayesian data of the harmonic external world, the annulus xQ|1x<b, into the local Bayesian data of its logarithmic coding space, the ball xQ|x<11b. The source’s conformal encoding function is y=logr2x1, where x is the observed Euclidean distance to an object’s position. The conformal decoding function is x=121+ry. Both functions, unique under basic requirements, enable information- and granularity-invariant recursion to model the multiscale reality. Full article
(This article belongs to the Special Issue Mathematical Modelling of Complex Systems)
12 pages, 228 KiB  
Article
Statin Use and Major Adverse Cardiovascular Events Among Patients with Ischemic Heart Diseases: A Multi-Center Retrospective Study
by Awatif Hafiz, Sarah Aljohani, Hussam Kutbi, Nayyara Fatani, Lama Alkhathran, Majd Alyaqub, Meshal S. Alhamed, Abdulrhaman O. Alhaqbani, Abdulrahman A. Alhadlaq, Mohammed A. Alsalman, Majed S. Al Yami and Omar A. Almohammed
J. Clin. Med. 2025, 14(3), 908; https://doi.org/10.3390/jcm14030908 - 30 Jan 2025
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Abstract
Objective: The objective of this study was to evaluate the effects of adherence to the ACC/AHA 2018 dyslipidemia guidelines on patient management of lipid-lowering therapy in patients with ischemic heart diseases (IHD) and its correlation with major adverse cardiovascular events (MACEs), including [...] Read more.
Objective: The objective of this study was to evaluate the effects of adherence to the ACC/AHA 2018 dyslipidemia guidelines on patient management of lipid-lowering therapy in patients with ischemic heart diseases (IHD) and its correlation with major adverse cardiovascular events (MACEs), including non-fatal MI, stroke, death, hospitalization for revascularization, and peripheral arterial disease. Methods: A multi-center retrospective observational study was conducted in patients with IHD between January 2019 and December 2020, who were followed for two years. The primary objective was to assess statin utilization and adherence to the 2018 ACC/AHA guidelines and the associated influence on MACE outcomes. Inferential statistical analyses, including chi-square tests and the Mann–Whitney test, were conducted to assess the associations between adherence to the guidelines, MACE rates, and LDL-C goal achievement. Results: The study included 1011 patients with ischemic heart disease (IHD), predominantly male (78.2%), with a mean age of 59 ± 10.9 years. Non-adherent patients had higher baseline LDL-C levels (3.0 ± 1.1 mmol/L vs. 2.7 ± 1.2 mmol/L; p = 0.0005), while adherent patients were more likely to be on cardiovascular medications, including statins (78.4% vs. 57.4%), aspirin (74.2% vs. 56.3%), and P2Y12 inhibitors (69.5% vs. 48.4%), compared to non-adherent patients. Adherence was associated with lower non-fatal MI rates (9.3% vs. 21.1%, p < 0.0001) and fewer revascularizations (9.3% vs. 16.8%; p = 0.0024). Additionally, 49.2% of adherent patients achieved target LDL-C goals, compared to 30.5% of the non-adherent patients (p < 0.0001). Notably, there were no significant differences in stroke, peripheral arterial disease, or mortality rates. Conclusions: The achievement of target LDL-C goals and reduced MACEs was observed with adherence to the 2018 ACC/AHA dyslipidemia guidelines. However, lipid management in IHD patients remains sub-optimal, highlighting opportunities for further enhancement. Full article
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