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18 pages, 9706 KiB  
Article
Dynamics Study of Hybrid Support Flywheel Energy Storage System with Damping Ring Device
by Mingming Hu, Kun Liu, Jingbo Wei, Eryong Hou, Duhe Liu and Xi Zhao
Actuators 2024, 13(12), 532; https://doi.org/10.3390/act13120532 (registering DOI) - 23 Dec 2024
Abstract
The flywheel energy storage system (FESS) of a mechanical bearing is utilized in electric vehicles, railways, power grid frequency modulation, due to its high instantaneous power and fast response. However, the lifetime of FESS is limited because of significant frictional losses in mechanical [...] Read more.
The flywheel energy storage system (FESS) of a mechanical bearing is utilized in electric vehicles, railways, power grid frequency modulation, due to its high instantaneous power and fast response. However, the lifetime of FESS is limited because of significant frictional losses in mechanical bearings and challenges associated with passing the critical speed. To suppress the unbalanced response of FESS at critical speed, a damping ring (DR) device is designed for a hybrid supported FESS with mechanical bearing and axial active magnetic bearing (AMB). Initially, the dynamic model of the FESS with DR is established using Lagrange’s equation. Moreover, the dynamic parameters of the DR are obtained by experimental measurements using the method of free vibration attenuation. Finally, the influence of the DR device on the critical speed and unbalanced response of FESS is analyzed. The results show that the designed DR device can effectively reduce the critical speed of FESS, and increase the first and second mode damping ratio. The critical speed is reduced from 13,860 rpm to 5280 rpm. Compared with FESS of the mechanical bearing, the unbalanced response amplitude of the FESS with DR is reduced by more than 87.8%, offering promising technical support for the design of active and passive control systems in FESS. Full article
(This article belongs to the Special Issue Actuator Technology for Active Noise and Vibration Control)
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Figure 1

Figure 1
<p>Schematic of FESS structure.</p>
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<p>Simplified model of FESS rotor–bearing system.</p>
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<p>FESS.</p>
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<p>Unfilled DR.</p>
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<p>Cross-section of the DR measuring device.</p>
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<p>Experimental procedure of DR.</p>
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<p>Experimental platform of DR.</p>
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<p>Curve fitting of free decay data.</p>
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<p>Modal shapes of FESS with DR at 0 rpm: (<b>a</b>) first modal, (<b>b</b>) second modal, (<b>c</b>) third modal, (<b>d</b>) fourth modal.</p>
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<p>Modal shapes of FESS with DR at 12,000 rpm: (<b>a</b>) first modal, (<b>b</b>) second modal, (<b>c</b>) third modal, (<b>d</b>) fourth modal.</p>
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<p>Variation of 1st- to 4th-order modal damping ratio with damping coefficients: (<b>a</b>) <math display="inline"><semantics> <msub> <mi>c</mi> <mn>1</mn> </msub> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <msub> <mi>c</mi> <mn>4</mn> </msub> </semantics></math>.</p>
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<p>Campbell diagram of the FESS: (<b>a</b>) REB + DR, (<b>b</b>) REB.</p>
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<p>Variation of unbalanced response with stiffness: (<b>a</b>) upper bearing, (<b>b</b>) upper end face of flywheel.</p>
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<p>Variation of unbalanced response with damping: (<b>a</b>) upper bearing, (<b>b</b>) upper end face of flywheel.</p>
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<p>Comparison of unbalanced response: (<b>a</b>) upper bearing, (<b>b</b>) upper flywheel end face, (<b>c</b>) lower flywheel end face, (<b>d</b>) lower bearing.</p>
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15 pages, 8029 KiB  
Article
Study on Length–Diameter Ratio of Axial–Radial Flux Hybrid Excitation Machine
by Mingyu Guo, Jiakuan Xia, Qimin Wu, Wenhao Gao and Hongbo Qiu
Processes 2024, 12(12), 2942; https://doi.org/10.3390/pr12122942 - 23 Dec 2024
Abstract
To improve the flux regulation range of the Axial–Radial Flux Hybrid Excitation Machine (ARFHEM) and the utilization rate of permanent magnets (PMs), the effects of different length–diameter ratios (LDRs) on the ARFHEM performance are studied. Firstly, the principle of the flux regulation of [...] Read more.
To improve the flux regulation range of the Axial–Radial Flux Hybrid Excitation Machine (ARFHEM) and the utilization rate of permanent magnets (PMs), the effects of different length–diameter ratios (LDRs) on the ARFHEM performance are studied. Firstly, the principle of the flux regulation of the ARFHEM is introduced by means of the structure and equivalent magnetic circuit method. Then, based on the principle of the bypass effect, the analytical formulas of LDRs, the number of pole-pairs, and the flux regulation ability are derived, and then the restrictive relationship between the air-gap magnetic field, LDR, and the number of pole-pairs is revealed. On this basis, the influence of an electric LDR on motor performance is studied. By comparing and analyzing the air-gap magnetic density and no-load back electromotive force (EMF) of motors with different LDRs, the variation in the magnetic flux regulation ability of motors with different LDRs is obtained and its influence mechanism is revealed. In addition, the torque regulation ability and loss of motors with different LDRs are compared and analyzed, and the influence mechanism of the LDR on torque and loss is determined. Finally, the above analysis is verified by experiments. Full article
(This article belongs to the Section Manufacturing Processes and Systems)
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Figure 1

Figure 1
<p>Structure of ARFHEM.</p>
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<p>The flux path and equivalent magnetic circuit of ARFHEM in different excitation current working conditions. (<b>a</b>) Only PM working state. (<b>b</b>) Negative excitation current working state. (<b>c</b>,<b>d</b>) Positive current excitation working state.</p>
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<p>Schematic diagram of bypass structure.</p>
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<p>Air-gap flux regulation characteristic curve with LDRs. (<b>a</b>) The radial air-gap flux density varies with the excitation current. (<b>b</b>) Variation of the multiple of air-gap magnetic flux regulation with LDRs.</p>
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<p>Relation between no-load back EMF and LDR. (<b>a</b>) No-load back EMF. (<b>b</b>) Total harmonic distortion.</p>
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<p>The output torque of a motor with different LDRs varies with the excitation current.</p>
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<p>Influence of different LDRs on motor loss.</p>
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<p>The ARFHEM prototypes.</p>
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<p>The test platform of prototypes.</p>
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<p>The back EMF varies with the excitation currents. (<b>a</b>) 0A. (<b>b</b>) 1A. (<b>c</b>) 3A. (<b>d</b>) 5A.</p>
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<p>The back EMF varies with the excitation currents. (<b>a</b>) 0A. (<b>b</b>) 1A. (<b>c</b>) 3A. (<b>d</b>) 5A.</p>
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19 pages, 5387 KiB  
Article
Cytotoxic Natural Products from Cryptomeria japonica (Thunb. ex L.) D.Don
by Bjørn Tobiassen Heieren, Anja Strandvoll Dyrdal, Lars Herfindal, Bjarte Holmelid, Cato Brede, Heidi Lie Andersen and Torgils Fossen
Int. J. Mol. Sci. 2024, 25(24), 13735; https://doi.org/10.3390/ijms252413735 - 23 Dec 2024
Abstract
Cryptomeria japonica is a commercially important tree native to Japan. The tree belongs to the ancient genus Cryptomeria and has found important uses as a medicinal plant, as well as a main source of timber in Japan. In recent years, there has been [...] Read more.
Cryptomeria japonica is a commercially important tree native to Japan. The tree belongs to the ancient genus Cryptomeria and has found important uses as a medicinal plant, as well as a main source of timber in Japan. In recent years, there has been an increased interest in discovering extended uses of C. japonica as a source of novel bioactive natural products with potential applications as lead compounds for active principles of future drugs. The compounds were isolated by a combination of two-phase extraction, XAD-7 Amberlite column chromatography, Sephadex LH-20 column chromatography and preparative High Performance Liquid Chromatography (HPLC). The structures were determined by a combination of several 1D and 2D Nuclear Magnetic Resonance (NMR) experiments and high-resolution mass spectrometry. Here, we report on the isolation and characterization of the novel biflavone glucoside hinokiflavone 7″-O-β-glucopyranoside, in addition to sixteen known compounds including the flavonols quercetin, quercetin 3-O-α-rhamnopyranoside and quercetin 3-O-β-galactopyranoside, the dihydroflavonols taxifolin 3-O-β-glucopyranoside, taxifolin 7-O-β-glucopyranoside, the flavanones naringenin, naringenin 7-O-β-galactopyranoside and eriodictyol 4′-O-β-glucopyranoside, the flavanol catechin, the biflavonoid amentoflavone, the dihydrochalcone phloretin 2′-O-β-glucopyranoside, the sesquiterpenoid roseoside, the polyphenolic compounds chlorogenic acid, methyl chlorogenate and the flavanocoumarins catechin-(7,8)-7″-(3,4 dihydroxyphenyl)-dihydro-8″(3H)-pyranone, and mururin A. The compounds exhibited low-to-moderate cytotoxic activity against MOLM-13 leukemia cells. Full article
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Figure 1
<p><span class="html-italic">Cryptomeria japonica</span> grown in the Arboretum of University of Bergen. Photo: Heidi Lie Andersen. Photo was taken on 14 November 2024.</p>
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<p>Molecular structures of quercetin (<b>1</b>), quercetin 3-<span class="html-italic">O</span>-<span class="html-italic">α</span>-rhamnopyranoside (<b>2</b>), quercetin 3-<span class="html-italic">O</span>-<span class="html-italic">β</span>-galactopyranoside (<b>3</b>), taxifolin 3-<span class="html-italic">O</span>-<span class="html-italic">β</span>-glucopyranoside (<b>4</b>), taxifolin 7-<span class="html-italic">O</span>-<span class="html-italic">β</span>-glucopyranoside (<b>5</b>), naringenin (<b>6</b>), naringenin 7-<span class="html-italic">O</span>-<span class="html-italic">β</span>-galactopyranoside (<b>7</b>), eriodictyol 4′-<span class="html-italic">O</span>-<span class="html-italic">β</span>-glucopyranoside (<b>8</b>), catechin (<b>9</b>), amentoflavone (<b>10</b>), phloretin 2′-<span class="html-italic">O</span>-<span class="html-italic">β</span>-glucopyranoside (<b>11</b>), roseoside (<b>12</b>), chlorogenic acid (<b>13</b>), and methyl chlorogenate (<b>13m</b>), in addition to the rare natural products catechin-(7,8)-7″-(3,4-dihydroxyphenyl)-dihydro-8″(3H)-pyranone (<b>14</b>), hinokiflavone 7″-<span class="html-italic">O</span>-<span class="html-italic">β</span>-glucopyranoside (<b>15</b>), and Mururin A (<b>16</b>).</p>
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<p>Expanded regions of the 2D <sup>1</sup>H-<sup>13</sup>C HMBC spectrum (<b>left</b>) and the 2D <sup>1</sup>H-<sup>1</sup>H ROESY spectrum (<b>right</b>) of hinokiflavone 7″-<span class="html-italic">O</span>-<span class="html-italic">β</span>-glucopyranoside (<b>15</b>) showing important crosspeaks for determination of linkages between the substructures of the compound. Blue arrows highlight the observed correlations in the molecular structure.</p>
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15 pages, 5042 KiB  
Article
Characterization of kHz Repetition Rate Laser-Driven Electron Beams by an Inhomogeneous Field Dipole Magnet Spectrometer
by Illia Zymak, Marco Favetta, Gabriele Maria Grittani, Carlo Maria Lazzarini, Gianfranco Tassielli, Annika Grenfell, Leonardo Goncalves, Sebastian Lorenz, Vanda Sluková, Filip Vitha, Roberto Versaci, Edwin Chacon-Golcher, Michal Nevrkla, Jiří Šišma, Roman Antipenkov, Václav Šobr, Wojciech Szuba, Theresa Staufer, Florian Grüner, Loredana Lapadula, Ezio Ranieri, Michele Piombino, Nasr A. M. Hafz, Christos Kamperidis, Daniel Papp, Sudipta Mondal, Pavel Bakule and Sergei V. Bulanovadd Show full author list remove Hide full author list
Photonics 2024, 11(12), 1208; https://doi.org/10.3390/photonics11121208 - 23 Dec 2024
Abstract
We demonstrate a method to characterize the beam energy, transverse profile, charge, and dose of a pulsed electron beam generated by a 1 kHz TW laser-plasma accelerator. The method is based on imaging with a scintillating screen in an inhomogeneous, orthogonal magnetic field [...] Read more.
We demonstrate a method to characterize the beam energy, transverse profile, charge, and dose of a pulsed electron beam generated by a 1 kHz TW laser-plasma accelerator. The method is based on imaging with a scintillating screen in an inhomogeneous, orthogonal magnetic field produced by a wide-gap magnetic dipole. Numerical simulations were developed to reconstruct the electron beam parameters accurately. The method has been experimentally verified and calibrated using a medical LINAC. The energy measurement accuracy in the 6–20 MeV range is proven to be better than 10%. The radiation dose has been calibrated by a water-equivalent phantom, RW3, showing a linear response of the method within 2% in the 0.05–0.5 mGy/pulse range. Full article
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Figure 1

Figure 1
<p>Top-view scheme of the EBDS system integrated into the ALFA accelerator. The components in vacuum and air are labeled with orange and blue colors, respectively.</p>
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<p>Map of the calculated magnetic field vector magnitude in planes crossing the center of the area between magnet poles indicated by the black dot: (<b>a</b>) plane orthogonal to the beam, (<b>b</b>) plane parallel to the beam. The distance between the magnet poles is 4 cm, and the length of the magnet is 4 cm.</p>
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<p>Theoretical electron beam trajectories calculated using the SIMION model: (<b>a</b>) for various energies in the range 1–100 MeV (electron trajectories out of the magnetic field are indicated in green, in the magnetic field in red); (<b>b</b>) beam displacement to energy for several beam pointing angles.</p>
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<p>Electron fluence map calculated using FLUKA Monte Carlo simulation for 5 MeV, 10 MeV, 20 MeV, 50 MeV, and 100 MeV beams and a 2 mm slit aperture opening: (<b>a</b>) top view; (<b>b</b>) screen plane view. The model includes electron–matter interaction processes to evaluate resolution increasing with the aperture. Blue arrows indicate the average displacement of the beam, and red indicates the minimal possible displacement for the beam of a certain energy. Green rectangular allocates non-deflected beam. The orange “ref” line refers to the slit edge and indicates a reference to calculate minimal possible energy, and <span class="html-italic">x</span> = 0 coordinates the average energy for the measured deflection using the same calibration.</p>
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<p>Theoretical dependence of the deposited dose to the beam charge density was calculated for a thin water layer using the NIST ESTAR database and for a 1 cm radius and 1 cm high water cylinder irradiated by the flattop profile beam of the same radius.</p>
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<p>FLUKA model of the 300 mrad divergent 3 MeV electron beam propagating near the partially inserted magnet (30 mm offset), slit aperture is aligned with a beam: (<b>a</b>) top view; (<b>b</b>) side view; (<b>c</b>) screen plane view. The model is used to develop sample irradiation strategies and beam artifact analysis.</p>
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<p>Experimental setup for the verification of the EBDS using the electron LINAC with, respectively, a 4 mm and 2 cm diameter round profile collimator as a reference source: (<b>a</b>) beam energy; (<b>b</b>) dose calibration. The magnet, Lanex screen, CMOS camera, mirror, and radiation shield are used as the electron detection system. The magnet or RW3 beam mediator slabs are inserted downstream from the screen for energy or dose calibration measurements.</p>
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<p>Verification of the beam energy measurement with the EBDS based on numerical models using a reference radiation source. Horizontal error bars are smaller than the markers. The linear fit is calculated using the least squares algorithm.</p>
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<p>Calibration curve relating the phosphor screen luminance with the ionization chamber dose. Screen intensity, normalized to the camera luminance range, is calibrated over the water phantom absorbed dose value. The average measurement accuracy defined by the linear fit is better than 2%. Vertical error bars are smaller than the marker size.</p>
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<p>Reconstruction of the energy spectrum for the nitrogen gas target used in the ALFA beamline: (<b>a</b>) reference beam pointing image on the LANEX phosphor screen, without the magnet; (<b>b</b>) profile of the reference beam without the magnetic field, used to determine the absolute dose and the beam fluence; (<b>c</b>) deflected beam profile image; (<b>d</b>) energy spectrum obtained from the profile of the deflected beam with energy binning. The area between pink lines is used to assess the beam profile and reconstruct the spectrum. The red line indicates the reference beam pointing used for the spectrum reconstruction.</p>
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<p>Evaluation of the energy spectrum for the gas mixture (98% Helium–2% Nitrogen) target: (<b>a</b>) profile of the beam deflected with the magnetic field; (<b>b</b>) evaluated spectrum with energy binning. The area between pink lines is used to assess the beam profile and reconstruct the spectrum. The red line indicates the reference beam pointing used for the spectrum reconstruction.</p>
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<p>MeV-range electron beam profile obtained with the partially inserted slit and magnet technique integrated over 20 shots. This enhanced contrast color scale profile was generated with a nitrogen target. The dots indicate a 1 cm scale.</p>
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29 pages, 20951 KiB  
Article
Design and SAR Analysis of an AMC-Integrated Wearable Cavity-Backed SIW Antenna
by Yathavi Thangavelu, Balakumaran Thangaraju and Rajagopal Maheswar
Micromachines 2024, 15(12), 1530; https://doi.org/10.3390/mi15121530 - 23 Dec 2024
Abstract
Wearable communication technologies necessitate antenna designs that harmonize ergonomic compatibility, reliable performance, and minimal interaction with human tissues. However, high specific absorption rate (SAR) levels, limited radiation efficiency, and challenges in integration with flexible materials have significantly constrained widespread deployment. To address these [...] Read more.
Wearable communication technologies necessitate antenna designs that harmonize ergonomic compatibility, reliable performance, and minimal interaction with human tissues. However, high specific absorption rate (SAR) levels, limited radiation efficiency, and challenges in integration with flexible materials have significantly constrained widespread deployment. To address these limitations, this manuscript introduces a novel wearable cavity-backed substrate-integrated waveguide (SIW) antenna augmented with artificial magnetic conductor (AMC) structures. The proposed architecture is meticulously engineered using diverse textile substrates, including cotton, jeans, and jute, to synergistically integrate SIW and AMC technologies, mitigating body-induced performance degradation while ensuring safety and high radiation efficiency. The proposed design demonstrates significant performance enhancements, achieving SAR reductions to 0.672 W/kg on the spine and 0.341 W/kg on the forelimb for the cotton substrate. Furthermore, the AMC-backed implementation attains ultra-low reflection coefficients, as low as −26.56 dB, alongside a gain improvement of up to 1.37 dB, culminating in a total gain of 7.09 dBi. The impedance bandwidth exceeds the ISM band specifications, spanning 150 MHz (2.3–2.45 GHz). The design maintains remarkable resilience and operational stability under varying conditions, including dynamic bending and proximity to human body models. By substantially suppressing back radiation, enhancing directional gain, and preserving impedance matching, the AMC integration optimally adapts the antenna to body-centric communication scenarios. This study uniquely investigates the dielectric and mechanical properties of textile substrates within the AMC-SIW configuration, emphasizing their practicality for wearable applications. This research sets a precedent for wearable antenna innovation, achieving an unprecedented balance of flexibility, safety, and electromagnetic performance while establishing a foundation for next-generation wearable systems. Full article
(This article belongs to the Topic Innovation, Communication and Engineering)
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Figure 1

Figure 1
<p>Geometry of cavity-backed SIW antenna on a wearable substrate showing (<b>a</b>) front-end view, (<b>b</b>) ground plane, (<b>c</b>) surface current distribution on the cavity-backed SIW antenna patch, and (<b>d</b>) microstrip feedline structure.</p>
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<p>SIW vias structures.</p>
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<p>Performance analysis of S-parameter characteristics of proposed cavity-backed SIW textile antenna.</p>
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<p>Performance analysis (gain) of cavity-backed SIW textile antenna.</p>
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<p>Boundary conditions for in-phase reflection characteristics.</p>
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<p>(<b>a</b>) Geometry of circular-shaped patch-type AMC array cell. (<b>b</b>) Equivalent circuit.</p>
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<p>In-phase simulation of 2.45 GHz AMC unit cells with normal plane incidence.</p>
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<p>Simulated reflection coefficient of (<b>a</b>) cotton, (<b>b</b>) jean, and (<b>c</b>) jute with varying separation distances from the AMC Plane.</p>
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<p>Isolation of AMC plane with textile antennas using a 3 mm thick layer of polyurethane foam. (<b>a</b>) Cotton, (<b>b</b>) jean, and (<b>c</b>) jute.</p>
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<p>Simulated reflection coefficient characteristics of cotton, jean, and jute textile antennas separated from the AMC plane using a 3 mm layer of polyurethane foam.</p>
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<p>Simulated gain radiation patterns of AMC-integrated cotton, jean, and jute substrate normalized radiation patterns [dBi] at 2.45 GHz.</p>
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<p>Resonant frequency and reflection coefficient for y-axis bending at 30 degrees for cotton, jean, and jute materials.</p>
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<p>Resonant frequency and reflection coefficient for x-axis bending at 30 degrees for cotton, jean, and jute materials.</p>
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<p>Three-layer test person’s body models were tested on (<b>a</b>) wearable antenna with cotton Substrate. (<b>b</b>) Antenna affixed on AMC structure.</p>
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<p>Simulated resonant frequency and reflection coefficient of all antennas affixed on three-layer test person’s body models.</p>
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<p>Simulated radiation patterns normalized to 0 dBi are shown for a frequency of 2.45 GHz affixed on three-layer test person’s body models.</p>
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<p>Fabricated cavity-backed SIW textile antenna and AMC reflector plane with cotton fabric (<b>a</b>) front and (<b>b</b>) back view.</p>
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<p>Fabricated cavity-backed SIW textile antenna and AMC reflector plane with jean fabric (<b>a</b>) front and (<b>b</b>) back view.</p>
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<p>Fabricated cavity-backed SIW textile antenna and AMC reflector plane with jute fabric (<b>a</b>) front and (<b>b</b>) back view.</p>
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<p>Fabricated cavity-backed SIW textile antenna and AMC reflector plane with jute fabric (<b>a</b>) front and (<b>b</b>) back view.</p>
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<p>Testing setup: AMC-integrated cavity-backed SIW textile antenna with cotton fabric affixed on the body of test person. (<b>a</b>) Spine and (<b>b</b>) forelimb.</p>
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<p>Testing setup: AMC-integrated cavity-backed SIW textile antenna with jean fabric affixed on the body of test person. (<b>a</b>) Spine and (<b>b</b>) forelimb.</p>
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<p>Testing setup: AMC-integrated cavity-backed SIW textile antenna with jute fabric affixed on the body of test person. (<b>a</b>) Spine and (<b>b</b>) forelimb.</p>
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<p>Snapshot of reflection coefficient S<sub>11</sub> (dB) measurement using VNA for the AMC-supported cotton antenna placed close to a test person’s (<b>a</b>) human spine. (<b>b</b>) Forelimb of radius 50 mm.</p>
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<p>Snapshot of reflection coefficient S<sub>11</sub> (dB) measurement using VNA for the AMC-supported jean antenna placed close to a test person’s (<b>a</b>) human spine. (<b>b</b>) Forelimb of radius 50 mm.</p>
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<p>Snapshot of reflection coefficient S<sub>11</sub> (dB) measurement using VNA for the AMC-supported jute antenna placed close to a test person’s (<b>a</b>) human spine. (<b>b</b>) Forelimb of radius 50 mm.</p>
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<p>Reflection coefficient S<sub>11</sub> (dB) of the AMC-supported cotton antenna placed close to a test person’s (<b>a</b>) human spine. (<b>b</b>) Forelimb of radius 50 mm. Solid red line: measured results. Solid black line: simulated results.</p>
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<p>Reflection coefficient S<sub>11</sub> (dB) of the AMC-supported jean antenna placed close to a test person’s (<b>a</b>) human spine. (<b>b</b>) Forelimb of radius 50 mm. Solid red line: measured results. Solid black line: simulated results.</p>
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<p>Reflection coefficient S<sub>11</sub> (dB) of the AMC-supported jute antenna placed close to a test person’s (<b>a</b>) human spine. (<b>b</b>) Forelimb of radius 50 mm. Solid red line: measured results. Solid black line: simulated results.</p>
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<p>Measurement setup of cotton textile antenna in a microwave-shielded far-field anechoic chamber.</p>
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<p>Tested radiation patterns (degree vs. dB) of an antenna placed close to a test person’s (<b>a</b>) human spine. (<b>b</b>) Forelimb of radius 50 mm.</p>
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<p>SAR analysis of SIW wearable antennas made of cotton, jean, and jute fabrics on (<b>a</b>) human spine and (<b>b</b>) forelimb at 2.45 GHz using 3-layer body phantoms with a mass of 10 g.</p>
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20 pages, 3373 KiB  
Review
Progress and Prospects for Titanium Extraction from Titanium-Bearing Blast Furnace Slag
by Yuxuan Qu, Lei Xing, Minglei Gao, Suxing Zhao, Qianqian Ren, Lanjie Li and Yue Long
Materials 2024, 17(24), 6291; https://doi.org/10.3390/ma17246291 (registering DOI) - 23 Dec 2024
Abstract
The composition of TBFS is complex. It is categorized into low (W(TiO2) < 5%), medium (5% < W(TiO2) < 20%), and high-titanium slag (W(TiO2) > 20%) based on Ti content. The titanium in the slag is underutilized, causing it to [...] Read more.
The composition of TBFS is complex. It is categorized into low (W(TiO2) < 5%), medium (5% < W(TiO2) < 20%), and high-titanium slag (W(TiO2) > 20%) based on Ti content. The titanium in the slag is underutilized, causing it to accumulate and contribute to environmental pollution. Current methods for extracting titanium from TBFS include acid leaching, alkali fusion roasting, high-temperature carbonation–low-temperature chlorination, electrochemical molten salt electrolysis, and selective enrichment. However, these methods still face challenges such as environmental impact, high costs, low Ti recovery, and low Ti grade. This paper summarizes the mechanisms and characteristics of the above methods. Future research should focus on integrating pyrometallurgy with beneficiation processes, followed by further purification of titanium-rich phases through hydrometallurgy. Additionally, combining this with novel separation technologies (such as microwave and superconducting magnetic separation) will optimize the dissociation of titanium-bearing phases after enrichment. Full article
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<p>(<b>a</b>) Physical image of titanium slag; (<b>b</b>) SEM image of titanium slag.</p>
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<p>Crystal structures of titanium-bearing phases. (<b>a</b>) perovskite; (<b>b</b>) rutile; (<b>c</b>) anosovite.</p>
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<p>Flowchart for sulfuric acid leaching of titanium-bearing blast furnace slag.</p>
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<p>Flowchart for hydrochloric acid leaching of titanium slag.</p>
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<p>Schematic of mixed-acid leaching of TBFS.</p>
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<p>Process flowchart for TiO<sub>2</sub> production through alkali fusion and salt roasting.</p>
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<p>Process flowchart for ammonium sulfate pyrolysis and acid leaching.</p>
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<p>New process flowchart for CH<sub>4</sub>–H<sub>2</sub>–N<sub>2</sub> mixed gas reduction and low-temperature chlorination.</p>
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<p>Process flowchart for electrochemical molten salt electrolysis.</p>
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<p>Process flowchart for ultragravity metallurgy.</p>
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27 pages, 11482 KiB  
Article
Clean Self-Supervised MRI Reconstruction from Noisy, Sub-Sampled Training Data with Robust SSDU
by Charles Millard and Mark Chiew
Bioengineering 2024, 11(12), 1305; https://doi.org/10.3390/bioengineering11121305 - 23 Dec 2024
Abstract
Most existing methods for magnetic resonance imaging (MRI) reconstruction with deep learning use fully supervised training, which assumes that a fully sampled dataset with a high signal-to-noise ratio (SNR) is available for training. In many circumstances, however, such a dataset is highly impractical [...] Read more.
Most existing methods for magnetic resonance imaging (MRI) reconstruction with deep learning use fully supervised training, which assumes that a fully sampled dataset with a high signal-to-noise ratio (SNR) is available for training. In many circumstances, however, such a dataset is highly impractical or even technically infeasible to acquire. Recently, a number of self-supervised methods for MRI reconstruction have been proposed, which use sub-sampled data only. However, the majority of such methods, such as Self-Supervised Learning via Data Undersampling (SSDU), are susceptible to reconstruction errors arising from noise in the measured data. In response, we propose Robust SSDU, which provably recovers clean images from noisy, sub-sampled training data by simultaneously estimating missing k-space samples and denoising the available samples. Robust SSDU trains the reconstruction network to map from a further noisy and sub-sampled version of the data to the original, singly noisy, and sub-sampled data and applies an additive Noisier2Noise correction term upon inference. We also present a related method, Noiser2Full, that recovers clean images when noisy, fully sampled data are available for training. Both proposed methods are applicable to any network architecture, are straightforward to implement, and have a similar computational cost to standard training. We evaluate our methods on the multi-coil fastMRI brain dataset with novel denoising-specific architecture and find that it performs competitively with a benchmark trained on clean, fully sampled data. Full article
(This article belongs to the Special Issue Artificial Intelligence for Better Healthcare and Precision Medicine)
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<p>The proposed self-supervised reconstruction and denoising method, Robust SSDU, which extends the training procedure illustrated in <a href="#bioengineering-11-01305-f001" class="html-fig">Figure 1</a> of [<a href="#B25-bioengineering-11-01305" class="html-bibr">25</a>] to low-SNR data. The sub-sampled, noisy training data <math display="inline"><semantics> <msub> <mi>y</mi> <mi>t</mi> </msub> </semantics></math> are further sub-sampled by a mask <math display="inline"><semantics> <msub> <mi>M</mi> <msub> <mi mathvariant="normal">Λ</mi> <mi>t</mi> </msub> </msub> </semantics></math> and corrupted by further noise <math display="inline"><semantics> <msub> <mover accent="true"> <mi>n</mi> <mo>˜</mo> </mover> <mi>t</mi> </msub> </semantics></math>, yielding <math display="inline"><semantics> <msub> <mover accent="true"> <mi>y</mi> <mo>˜</mo> </mover> <mi>t</mi> </msub> </semantics></math>. The loss is computed between <math display="inline"><semantics> <msub> <mi>y</mi> <mi>t</mi> </msub> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mi>θ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mover accent="true"> <mi>y</mi> <mo>˜</mo> </mover> <mi>t</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math> on <math display="inline"><semantics> <msub> <mi mathvariant="normal">Ω</mi> <mi>t</mi> </msub> </semantics></math>.</p>
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<p>The refinement module for the proposed architecture Denoising VarNet, which trains two networks in parallel, removing noise and aliasing separately.</p>
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<p>The difference between the test set loss of Standard VarNet and the proposed Denoising VarNet for the benchmark training method. All differences are positive, showing that Denoising VarNet outperformed Standard VarNet, especially for a large <math display="inline"><semantics> <msub> <mi>σ</mi> <mi>n</mi> </msub> </semantics></math>.</p>
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<p>The robustness to <math display="inline"><semantics> <mi>α</mi> </semantics></math> of Noisier2Full, Robust SSDU, and their weighted versions at <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi mathvariant="normal">Ω</mi> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mi>n</mi> </msub> <mo>=</mo> <mn>0.06</mn> </mrow> </semantics></math>. The performance of the fully supervised benchmark, which did not depend on <math display="inline"><semantics> <mi>α</mi> </semantics></math>, is also shown. The weighted versions were substantially more robust, especially for small <math display="inline"><semantics> <mi>α</mi> </semantics></math>: at <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0.05</mn> </mrow> </semantics></math>, the values of the Unweighted Noisier2Full and Robust SSDU, which are excluded from the visualization, were 0.70 and 0.62, respectively.</p>
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<p>Reconstructions when fully sampled, noisy data are available for training. “Noisy” and “Noisy and sub-sampled” refer to the RSS reconstruction of <math display="inline"><semantics> <mrow> <msub> <mi>y</mi> <mrow> <mn>0</mn> <mo>,</mo> <mi>s</mi> </mrow> </msub> <mo>+</mo> <msub> <mi>n</mi> <mi>s</mi> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>M</mi> <msub> <mi mathvariant="normal">Ω</mi> <mi>s</mi> </msub> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>y</mi> <mrow> <mn>0</mn> <mo>,</mo> <mi>s</mi> </mrow> </msub> <mo>+</mo> <msub> <mi>n</mi> <mi>s</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math>, respectively. While there is clear noise in Supervised w/o denoising’s reconstruction, the proposed method, which is indicated with an asterisk, performs very similarly to the fully supervised benchmark. The red arrows show artifacts for Supervised with BM3D, and the green arrows show the improved recovery and contrast of fine features for Noisier2Full.</p>
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<p>Example reconstructions for networks trained on noisy, sub-sampled data. The proposed method, Robust SSDU, highlighted with an asterisk, performed very similarly to the fully supervised benchmark, even at <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi mathvariant="normal">Ω</mi> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>. Red arrows highlight hallucinated features in the SSDU with BM3D image, whereas green arrows highlight good recovery of edge features in the Robust SSDU reconstructions.</p>
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<p>Clinical regions of interest annotated via fastMRI+ [<a href="#B47-bioengineering-11-01305" class="html-bibr">47</a>]. The top image shows a resection cavity and the bottom shows a lacunar infarct. The proposed method, Robust SSDU, highlighted with an asterisk, has improved sharpness compared to Standard SSDU, which has reconstruction errors arising from measurement noise. The arrow highlights improved recovery of infarct geometry.</p>
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<p>Example reconstruction for 2D Bernoulli sampling. For Standard SSDU, the test set’s NMSE and SSIM were 0.383 and 0.72, respectively, and for Robust SSDU, highlighted with an asterisk, the test set’s NMSE and SSIM were 0.316 and 0.75, respectively.</p>
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<p>The qualitative performance of the proposed method with the prospectively noisy, low-field dataset M4Raw. While SSDU with BM3D and Robust SSDU (highlighted with an asterisk) both demonstrate a denoising effect, Robust SSDU exhibits improved contrast and visibly sharper boundaries, highlighted by the green arrows.</p>
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<p>Poor recovery of fine details for ambitious sub-sampling and noise levels at <math display="inline"><semantics> <mrow> <msub> <mi>R</mi> <mi mathvariant="normal">Ω</mi> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mi>n</mi> </msub> <mo>=</mo> <mn>0.08</mn> </mrow> </semantics></math> for both the Fully-supervised benchmark, and Robust SSDU (highlighted with an asterisk).</p>
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19 pages, 8457 KiB  
Article
Complex Large-Deformation Multimodality Image Registration Network for Image-Guided Radiotherapy of Cervical Cancer
by Ping Jiang, Sijia Wu, Wenjian Qin and Yaoqin Xie
Bioengineering 2024, 11(12), 1304; https://doi.org/10.3390/bioengineering11121304 - 23 Dec 2024
Abstract
In recent years, image-guided brachytherapy for cervical cancer has become an important treatment method for patients with locally advanced cervical cancer, and multi-modality image registration technology is a key step in this system. However, due to the patient’s own movement and other factors, [...] Read more.
In recent years, image-guided brachytherapy for cervical cancer has become an important treatment method for patients with locally advanced cervical cancer, and multi-modality image registration technology is a key step in this system. However, due to the patient’s own movement and other factors, the deformation between the different modalities of images is discontinuous, which brings great difficulties to the registration of pelvic computed tomography (CT/) and magnetic resonance (MR) images. In this paper, we propose a multimodality image registration network based on multistage transformation enhancement features (MTEF) to maintain the continuity of the deformation field. The model uses wavelet transform to extract different components of the image and performs fusion and enhancement processing as the input to the model. The model performs multiple registrations from local to global regions. Then, we propose a novel shared pyramid registration network that can accurately extract features from different modalities, optimizing the predicted deformation field through progressive refinement. In order to improve the registration performance, we also propose a deep learning similarity measurement method combined with bistructural morphology. On the basis of deep learning, bistructural morphology is added to the model to train the pelvic area registration evaluator, and the model can obtain parameters covering large deformation for loss function. The model was verified by the actual clinical data of cervical cancer patients. After a large number of experiments, our proposed model achieved the highest dice similarity coefficient (DSC) metric compared with the state-of-the-art registration methods. The DSC index of the MTEF algorithm is 5.64% higher than that of the TransMorph algorithm. It will effectively integrate multi-modal image information, improve the accuracy of tumor localization, and benefit more cervical cancer patients. Full article
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<p>The CT and MR images of the same patient are shown in (<b>a</b>), and the large deformation can be found between the multimodality images, which also increases the difficulty of our algorithm design. (<b>a-1</b>) represents the patient’s CT image, and (<b>a-2</b>) represents the patient’s MR image. (<b>b-1</b>) shows the CT image and (<b>b-2</b>) shows the MR image. (<b>b-3</b>) shows the registration image, and (<b>b-4</b>) shows the superimposed image of the warp image and fixed image. The MTEF model can better learn the features of the fixed image, achieving high-precision multimodality image registration and fusion.</p>
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<p>The proposed model architecture diagram.</p>
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<p>(<b>a</b>) In the third stage, eight sub-images are obtained after the decomposition of the CT image. (<b>b</b>) In the second stage, eight sub-images are obtained after the decomposition of the CT image. (<b>c</b>) In the first stage, eight sub-images are obtained after the decomposition of the CT image. (<b>d</b>) The patient’s raw CT and MR images and enhanced processing of high-frequency components.</p>
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<p>The architecture of this paper’s proposed shared pyramid registration network (SPR-Net). It includes two independent Swin Transformer encoders and a shared decoder. In the decoder part, we employ a pyramid registration strategy to predict the deformation field between images with large deformations, achieving a coarse-to-fine registration process.</p>
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<p>High-precision similarity measurement by deep learning combined with bistructural morphology.</p>
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<p>Bistructural morphology algorithm principle and image effect under different structure sizes. (<b>a</b>) represents the schematic diagram of the principle of bistructural morphology. (<b>b-1</b>) represents the MR image of the patient. (<b>b-2</b>) represents the processing effect with a radius of 3. (<b>b-3</b>) represents the processing effect with a radius of 5. (<b>b-4</b>) represents the processing effect with a radius of 6. (<b>b-5</b>) represents the processing effect with a radius of 7. (<b>b-6</b>) represents the processing effect with a radius of 9.</p>
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<p>Complete process of algorithm registration: (<b>a-1</b>–<b>a-7</b>) represents the effect diagram of multi-mode registration, (<b>a-8</b>) represents the fusion image of the original CT and MR, and (<b>a-9</b>) represents the fusion image of the Warp image and CT, which shows that Warp and CT basically overlap, which will help doctors make use of different information for diagnosis. (<b>a-10</b>–<b>a-12</b>) represents a boxchart of (<b>a-1</b>–<b>a-3</b>), respectively. It can be seen that the warp image is distorted towards the fixed image. (<b>b-1</b>,<b>b-2</b>) represents the enhanced processing of the high-frequency components of CT and MR, respectively, (<b>b-3</b>) represents the local deformation field of the model during the local registration process, and (<b>c-1</b>–<b>c-4</b>) represents the deformation field during the process of level3 to level0.</p>
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<p>Comparison of registration effects of various algorithms in actual data and deformation field.</p>
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<p>Comparison boxplot of the registration effect of different organs. The second row on the horizontal axis represents different organs of the patient, including the bladder, CTV, femur, and small intestine. The first row represents different algorithms. The vertical axis represents the DSC values obtained by different algorithms.</p>
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<p><math display="inline"><semantics> <mrow> <mfenced close="|" open="|"> <mrow> <mi>J</mi> <mi>D</mi> </mrow> </mfenced> <mo>≤</mo> <mn>0</mn> </mrow> </semantics></math> curve of two advanced registration algorithms and MTEF variants.</p>
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<p>Registration results of MTEF using different similarity algorithms and the resulting deformation field and deformation mesh.</p>
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22 pages, 2819 KiB  
Systematic Review
Functional Magnetic Resonance Imaging in Research on Dog Cognition: A Systematic Review
by Katarzyna Skierbiszewska, Marta Borowska, Joanna Bonecka, Bernard Turek, Tomasz Jasiński and Małgorzata Domino
Appl. Sci. 2024, 14(24), 12028; https://doi.org/10.3390/app142412028 - 23 Dec 2024
Abstract
Canine functional magnetic resonance imaging (fMRI) neurocognitive studies represent an emerging field that is advancing more gradually compared to progress in human fMRI research. Given the potential benefits of canine fMRI for veterinary, comparative, and translational research, this systematic review highlights significant findings, [...] Read more.
Canine functional magnetic resonance imaging (fMRI) neurocognitive studies represent an emerging field that is advancing more gradually compared to progress in human fMRI research. Given the potential benefits of canine fMRI for veterinary, comparative, and translational research, this systematic review highlights significant findings, focusing on specific brain areas activated during task-related and resting state conditions in dogs. The review addresses the following question: “What brain areas in dogs are activated in response to various stimuli?”. Following PRISMA 2020 guidelines, a comprehensive search of PUBMED, Scopus, and Web of Knowledge databases identified 1833 studies, of which 46 met the inclusion criteria. The studies were categorized into themes concerning resting state networks and visual, auditory, olfactory, somatosensory, and multi-stimulations studies. In dogs, resting state networks and stimulus-specific functional patterns were confirmed as vital for brain function. These findings reveal both similarities and differences in the neurological mechanisms underlying canine and human cognition, enhance the understanding of neural activation pathways in dogs, expand the knowledge of social bonding patterns, and highlight the potential use of fMRI in predicting the suitability of dogs for assistance roles. Further studies are needed to further map human–canine similarities and identify the unique features of canine brain function. Additionally, implementing innovative human methods, such as combined fMRI–magnetic resonance spectroscopy (MRS), into canine neurocognitive research could significantly advance the field. Full article
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<p>PRISMA flow diagram depicting research articles on dog cognition investigated using functional magnetic resonance imaging (fMRI) included and excluded from this systematic review.</p>
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<p>Traffic light plot of risk of bias in randomized controlled trials on (<b>A</b>) visual stimuli, (<b>B</b>) auditory stimuli, (<b>C</b>) olfactory stimuli, and (<b>D</b>) somatosensory stimuli and multi-stimuli.</p>
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<p>Traffic light plot of risk of bias in non-randomized trials and observational studies on (<b>A</b>) resting state networks, (<b>B</b>) visual stimuli, (<b>C</b>) auditory stimuli, and (<b>D</b>) somatosensory stimuli and multi–stimuli.</p>
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23 pages, 9787 KiB  
Article
Monitoring Ionospheric and Atmospheric Conditions During the 2023 Kahramanmaraş Earthquake Period
by Serkan Doğanalp and İrem Köz
Atmosphere 2024, 15(12), 1542; https://doi.org/10.3390/atmos15121542 - 22 Dec 2024
Viewed by 313
Abstract
Recent advancements have led to a growing prevalence of studies examining ionospheric and atmospheric anomalies as potential precursors to earthquakes. In this context, the study involved analyzing variations in ionospheric total electron content (TEC), investigating anomalies, assessing space weather conditions, and examining changes [...] Read more.
Recent advancements have led to a growing prevalence of studies examining ionospheric and atmospheric anomalies as potential precursors to earthquakes. In this context, the study involved analyzing variations in ionospheric total electron content (TEC), investigating anomalies, assessing space weather conditions, and examining changes in atmospheric parameters to evaluate potential precursors and post-seismic effects related to the Mw 7.7 and Mw 7.6 earthquakes that struck Kahramanmaraş consecutively in 2023. To compute the total electron content (TEC) values, data from 29 GNSS receivers covering a period of approximately 49 days were processed. In addition, since identical code signals were not available among all receiver stations, the study conducted an analysis of TEC estimations applying different GPS codes. To analyze space weather conditions, which are considered the main source of changes in the ionosphere, variations in sunspot number, solar activity index, magnetic activity indices (Kp and Dst), and geomagnetic field components were examined across the relevant period. To assess the potential presence of a distinct relationship between seismic activity at the Earth’s surface and ionospheric conditions, atmospheric parameters including temperature, relative humidity, and pressure were meticulously monitored and evaluated. As a result of the study, it was determined that TEC anomalies that could be evaluated as earthquake precursors independent of space weather conditions were observed starting from the 3rd day before the earthquake, and high positive TEC anomalies occurred immediately after the earthquakes. In atmospheric parameters, the change in behavior, particularly in temperature value, 10 days before the earthquake, is noteworthy. Full article
(This article belongs to the Special Issue Observations and Analysis of Upper Atmosphere)
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<p>Study area and GNSS stations.</p>
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<p>CORS-TR stations and LTAU sounding station.</p>
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<p>EKZ1 station GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs.</p>
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<p>MAR1 station GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs.</p>
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<p>ANTE station GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs.</p>
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<p>ONIY station GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs.</p>
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<p>Space weather conditions during the earthquake period.</p>
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<p>Temporal cross–correlation patterns between TEC anomalies and space weather conditions. Dark blue lines represent the confidence bounds and red points indicate the value of correlation.</p>
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<p>Atmospheric data from LTAU sounding station (2020–2023).</p>
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<p>Temporal cross–correlation patterns between TEC anomalies and atmospheric parameters. Dark blue lines represent the confidence bounds and red points indicate the value of correlation.</p>
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<p>GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs for the stations (MGOS, SILF, MRSI, ADN2, HAT2, BSHM).</p>
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<p>GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs for the stations (RAMO, POZA, NIGD, KAY1, FEEK, TUF1).</p>
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<p>GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs for the stations (TUBI, GURU, ADY1, MLY1, SIV1, ELAZ).</p>
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<p>GPS–VTEC variation (<b>top</b>) and anomaly (<b>bottom</b>) graphs for the stations (ERGN, ARUC, ZECK, KLS1, AKLE, VIR2, BHR4).</p>
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13 pages, 2451 KiB  
Article
Impact of the STFT Window Size on Classification of Grain-Oriented Electrical Steels from Barkhausen Noise Time–Frequency Spectrograms via Deep CNNs
by Michal Maciusowicz and Grzegorz Psuj
Appl. Sci. 2024, 14(24), 12018; https://doi.org/10.3390/app142412018 - 22 Dec 2024
Viewed by 350
Abstract
The Magnetic Barkhausen Noise (MBN) is a non-destructive testing method, which, due to its high sensitivity to changes in the microstructure of the material, is increasingly being applied with success as a tool for evaluation of magnetic material state and properties. However, it [...] Read more.
The Magnetic Barkhausen Noise (MBN) is a non-destructive testing method, which, due to its high sensitivity to changes in the microstructure of the material, is increasingly being applied with success as a tool for evaluation of magnetic material state and properties. However, it is no less difficult to analyze the measurement signals and their correct interpretation due to the complex, non-deterministic and stochastic nature of the Barkhausen phenomenon. Depending on the material to be examined, a signal with different characteristics can be observed. Frequently, a signal with multi-phase Barkhausen activity characteristics is obtained, like in the case of grain-oriented electrical steels. Due to the increased computational capabilities of computers, more and more advanced signal analysis methods are being used and artificial intelligence is being involved as well. Recently, the time–frequency (TF) approach for MBN signal analysis was introduced and discussed in several papers, where short-time Fourier Transform (STFT) found frequent application with promising results. Due to the automation of the search for diagnostic patterns, the stage of selecting transformation parameters becomes extremely important in the process of preparing training data for evaluation algorithms. This paper investigates the influence of the STFT computational window size on the material state evaluation results obtained using convolutional neural network (CNN). The studies were performed for MBN signals obtained from grain-oriented electrical steel with anisotropic properties. The carried out work made it possible to draw connections on the importance of the choice of the window during the implementation of CNN network training. Full article
(This article belongs to the Special Issue Progress in Nondestructive Testing and Evaluation (NDT&E))
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<p>Example of MBN signal obtained during the examination of an GO electrical steel sheet: α = 0° is the transverse direction of steel, while α = 90° is the rolling direction of steel.</p>
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<p>Time–frequency representation space depending on the size of the window.</p>
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<p>View of the transducer and schematics illustration of the measuring procedure; RD—rolling direction of steel; TD—transverse direction of the steel.</p>
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<p>Schematic of the measurement system.</p>
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<p>Exemplary spectrograms for a sample H<sub>23#1</sub> obtained for various alignments of the transducer and sizes of the computational window.</p>
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<p>Exemplary spectrograms obtained for various sizes of the computational window: before and after the dimension-fitting procedure.</p>
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<p>Figure the accuracy of the trained CNNs verified with various versions of the test set according to <a href="#applsci-14-12018-t005" class="html-table">Table 5</a>.</p>
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18 pages, 5439 KiB  
Review
Advanced Imaging Techniques for Atherosclerosis and Cardiovascular Calcification in Animal Models
by Lifang Ye, Chih-Chiang Chang, Qian Li, Yin Tintut and Jeffrey J. Hsu
J. Cardiovasc. Dev. Dis. 2024, 11(12), 410; https://doi.org/10.3390/jcdd11120410 (registering DOI) - 22 Dec 2024
Viewed by 213
Abstract
The detection and assessment of atherosclerosis and cardiovascular calcification can inform risk stratification and therapies to reduce cardiovascular morbidity and mortality. In this review, we provide an overview of current and emerging imaging techniques for assessing atherosclerosis and cardiovascular calcification in animal models. [...] Read more.
The detection and assessment of atherosclerosis and cardiovascular calcification can inform risk stratification and therapies to reduce cardiovascular morbidity and mortality. In this review, we provide an overview of current and emerging imaging techniques for assessing atherosclerosis and cardiovascular calcification in animal models. Traditional imaging modalities, such as computed tomography (CT) and magnetic resonance imaging (MRI), offer non-invasive approaches of visualizing atherosclerotic calcification in vivo; integration of these techniques with positron emission tomography (PET) imaging adds molecular imaging capabilities, such as detection of metabolically active microcalcifications with 18F-sodium fluoride. Photoacoustic imaging provides high contrast that enables in vivo evaluation of plaque composition, yet this method is limited by optical penetration depth. Light-sheet fluorescence microscopy provides high-resolution, three-dimensional imaging of cardiovascular structures and has been used for ex vivo assessment of atherosclerotic calcification, but its limited tissue penetration and requisite complex sample preparation preclude its use in vivo to evaluate cardiac tissue. Overall, with these evolving imaging tools, our understanding of cardiovascular calcification development in animal models is improving, and the combination of traditional imaging techniques with emerging molecular imaging modalities will enhance our ability to investigate therapeutic strategies for atherosclerotic calcification. Full article
(This article belongs to the Special Issue Advances in the Diagnosis of Cardiovascular Diseases)
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23 pages, 7423 KiB  
Article
Crystal Plasticity Finite Element Study on Orientation Evolution and Deformation Inhomogeneity of Island Grain During the Ultra-Thin Strips Rolling of Grain Oriented Electrical Steel
by Huanzhu Wang, Ping Yang, Qingge Xie and Xinfu Gu
Materials 2024, 17(24), 6276; https://doi.org/10.3390/ma17246276 (registering DOI) - 22 Dec 2024
Viewed by 277
Abstract
The presence of island grains in the initial finished sheets of grain-oriented electrical steel is inevitable in the preparation of ultra-thin strips. Owing to their distinctive shape and size effects, their deformation behavior during rolling differs from that of grain-oriented electrical steels of [...] Read more.
The presence of island grains in the initial finished sheets of grain-oriented electrical steel is inevitable in the preparation of ultra-thin strips. Owing to their distinctive shape and size effects, their deformation behavior during rolling differs from that of grain-oriented electrical steels of conventional thickness. This study focuses on the orientation evolution and deformation heterogeneity of island grains during rolling. Four types of island grains with orientations of {210}<001>, {110}<112>, {114}<481>, and {100}<021> were selected and modeled within the Goss-oriented matrix using full-field crystal plasticity finite element (CPFEM) simulation under plane strain compression. The results are then compared with corresponding experimental measurements. The results reveal that orientation rotation and grain fragmentation vary among the island grains of different orientations, with the first two orientations exhibiting more significant deformation heterogeneity compared to the latter two. Additionally, the orientations of the island grains significantly affect the distribution of residual Goss orientations within the surrounding matrix. Pancake-like island grains exhibit a higher degree of orientation scatter and greater deformation heterogeneity in the central layer compared to their spherical counterparts. The initial {210}<001> island grains can form a cube orientation, which can be optimized by subsequent process control to enhance magnetic properties. Full article
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<p>IPF-Z maps, ODF section and (001) pole figures of pancake-like {210}&lt;001&gt; island grain embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of the XY section with pancake-like {210}&lt;001&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5, (<b>g</b>,<b>h</b>) z = 0.75, (<b>i</b>,<b>j</b>) z = 1.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of the spherical {210}&lt;001&gt; island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of the XY section with the spherical {210}&lt;001&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5.</p>
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<p>IPF-Z maps of XZ center section of pancake-like and spherical {210}&lt;001&gt; island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>(001) pole figures of the pancake-like and spherical {210}&lt;001&gt;-oriented island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of pancake-like {110}&lt;112&gt;-oriented island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of XY section with {110}&lt;112&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5, (<b>g</b>,<b>h</b>) z = 0.75, (<b>i</b>,<b>j</b>) z = 1.</p>
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<p>IPF-Z maps of the XY center section, ODF section and (001) pole figures of the spherical {110}&lt;112&gt;-oriented island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps of XZ center section of pancake-like and spherical {110}&lt;112&gt; island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>(001) pole figures of pancake-like and spherical {110}&lt;112&gt; island grains with different reductions: (<b>a</b>,<b>b</b>) 0%, (<b>c</b>,<b>d</b>) 20%, (<b>e</b>,<b>f</b>) 40%, (<b>g</b>,<b>h</b>) 60%, (<b>i</b>,<b>j</b>) 80%.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of {114}&lt;481&gt; island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 80%.</p>
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<p>IPF-Z maps and (001) pole figures of XY section with {114}&lt;481&gt; island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5.</p>
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<p>IPF-Z maps, ODF section and (001) pole figures of {100}&lt;021&gt; island grains embedded in the Goss matrix with different reductions: (<b>a</b>–<b>c</b>) 0%, (<b>d</b>–<b>f</b>) 20%, (<b>g</b>–<b>i</b>) 40%, (<b>j</b>–<b>l</b>) 60%, (<b>m</b>–<b>o</b>) 70%.</p>
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<p>IPF-Z maps and (001) pole figures of XY section with {100}&lt;021&gt;-oriented island grains at 60% reduction: (<b>a</b>,<b>b</b>) z = 0, (<b>c</b>,<b>d</b>) z = 0.25, (<b>e</b>,<b>f</b>) z = 0.5.</p>
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<p>Evolution of {210}&lt;001&gt; island grains during cold rolling at 70% and annealing (930 °C, 3 min): (<b>a</b>,<b>d</b>,<b>e</b>) the original EBSD data of the island grain, (<b>b</b>,<b>f</b>,<b>g</b>) EBSD data after cold rolling, (<b>c</b>,<b>h</b>,<b>i</b>) EBSD data after recrystallization. Reproduced with permission from Ping Yang, Materials Chemistry and Physics; published by Elsevier, 2022 Reference [<a href="#B12-materials-17-06276" class="html-bibr">12</a>].</p>
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<p>Evolution of {110}&lt;112&gt; island grains during cold rolling to 70% and annealing (930 °C, 3 min): (<b>a</b>,<b>d</b>,<b>e</b>) the original EBSD data of island grain, (<b>b</b>,<b>f</b>,<b>g</b>) EBSD data after cold rolling, (<b>c</b>,<b>h</b>,<b>i</b>) EBSD data after recrystallization. Reproduced with permission from Ping Yang, Materials Chemistry and Physics; published by Elsevier, 2022 in Reference [<a href="#B12-materials-17-06276" class="html-bibr">12</a>].</p>
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<p>IPF-Z maps and ODF section of samples with lower initial magnetic inductions after annealing at 850 °C for 5 min at different reductions: (<b>a</b>,<b>b</b>) 60%, (<b>c</b>,<b>d</b>) 65%, (<b>e</b>,<b>f</b>) 70%, (<b>g</b>,<b>h</b>) 75%. Reproduced with permission from Ping Yang, Journal of Materials Engineering; published by Journal of Materials Engineering Editorial Department, 2017 [<a href="#B8-materials-17-06276" class="html-bibr">8</a>].</p>
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23 pages, 2201 KiB  
Article
Effects of Extremely Low-Frequency Electromagnetic Field Treatment on ASD Symptoms in Children: A Pilot Study
by Kierra Pietramala, Alessandro Greco, Alberto Garoli and Danielle Roblin
Brain Sci. 2024, 14(12), 1293; https://doi.org/10.3390/brainsci14121293 - 22 Dec 2024
Viewed by 415
Abstract
Background/Objectives: Autism Spectrum Disorder (ASD) are neurodevelopmental disorders marked by challenges in social interaction, communication, and repetitive behaviors. People with ASD may exhibit repetitive behaviors, unique ways of learning, and different ways of interacting with the world. The term “spectrum” reflects the wide [...] Read more.
Background/Objectives: Autism Spectrum Disorder (ASD) are neurodevelopmental disorders marked by challenges in social interaction, communication, and repetitive behaviors. People with ASD may exhibit repetitive behaviors, unique ways of learning, and different ways of interacting with the world. The term “spectrum” reflects the wide variability in how ASD manifests in individuals, including differences in abilities, symptoms, and support needs, and conditions characterized by difficulties in social interactions, communication, restricted interests, and repetitive behaviors. Inflammation plays a crucial role in the pathophysiology, with increased pro-inflammatory cytokines in cerebrospinal fluid. Previous studies with transcranial magnetic stimulation have shown promising results, suggesting nervous system susceptibility to electromagnetic fields, with evidence indicating that extremely low-frequency electromagnetic field (ELF-EMF) treatment may modulate inflammatory responses through multiple pathways, including the reduction of pro-inflammatory cytokines like IL-6 and TNF-α, and the enhancement of anti-inflammatory mediators. Methods: This pilot study included 20 children (ages 2–13) with a confirmed diagnosis of ASD. A 15-week protocol involved ELF-EMF treatments using the SEQEX device, with specific day and night programs. Assessment was conducted through standardized pre- and post-treatment tests: Achenbach Child Behavior Checklist, Peabody Picture Vocabulary Test-4, Expressive One Word Picture Vocabulary Test-4, and Conner’s 3GI. Results: Statistically significant improvements were observed in receptive language (PPVT-4: from 74.07 to 90.40, p = 0.002) and expressive language (EOWPVT-4: from 84.17 to 90.50, p = 0.041). Notable reductions, with statistical significance, were found in externalizing problems across both age groups (1.5–5 years: p = 0.028; 6–18 years: p = 0.027), with particular improvement in attention and behavioral problems. The results were observed over a short period of 15 weeks, therefore excluding the possibility of coincidental age-related gains, that would typically occur during a normal developmental timeframe. Parent evaluations showed significant reduction in ASD symptoms, particularly in the 1.5–5 years group (p = 0.046). Conclusions: ELF-EMF treatment demonstrated a high safety profile and efficacy in mitigating ASD-related symptoms. The observed improvements suggest both direct effects on central and autonomic nervous systems and indirect effects through inflammatory response modulation. Further studies are needed to confirm these promising results through broader demographics and randomized control designs. Full article
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<p>The Peabody Picture Vocabulary Test-4 shows significant difference between Pre- and Post-test t = −3.809, <span class="html-italic">p</span> = 0.002.</p>
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<p>The Expressive One Word Picture Vocabulary Test-4th Edition shows significant difference between Pre- and Post-Test t = −2.312, <span class="html-italic">p</span> = 0.041.</p>
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<p>Cumulative graph for areas with significant results in the Achenbach Teacher Data for participants from 1.5 to 5 years.</p>
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<p>Cumulative graph for areas with significant results in the Achenbach Teacher Data for participants aged 6–18.</p>
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<p>The DSM−5 Oriented Scales showed significant changes in the areas of anxiety disorders (<span class="html-italic">p</span> = 0.027) and attention disorders (<span class="html-italic">p</span> = 0.042).</p>
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<p>In the 1.5–5 age group, the Achenbach Parent Data DMS-5 Oriented Scale showed significant improvement in the ASD item.</p>
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<p>Achenbach Parent Data shows significant difference between Pre- and Post-Test in Thought Problems (t = −2.201, <span class="html-italic">p</span> = 0.028).</p>
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19 pages, 11955 KiB  
Article
Structural Design and Electromagnetic Performance Analysis of Octupole Active Radial Magnetic Bearing
by Qixuan Zhu, Yujun Lu and Zhongkui Shao
Sensors 2024, 24(24), 8200; https://doi.org/10.3390/s24248200 (registering DOI) - 22 Dec 2024
Viewed by 337
Abstract
This study addresses the challenges of magnetic circuit coupling and control complexity in active radial magnetic bearings (ARMBs) by systematically investigating the electromagnetic performance of four magnetic pole configurations (NNSS, NSNS, NNNN, and SSSS). Initially, equivalent magnetic circuit modeling and finite element analysis [...] Read more.
This study addresses the challenges of magnetic circuit coupling and control complexity in active radial magnetic bearings (ARMBs) by systematically investigating the electromagnetic performance of four magnetic pole configurations (NNSS, NSNS, NNNN, and SSSS). Initially, equivalent magnetic circuit modeling and finite element analysis (FEA) were employed to analyze the magnetic circuit coupling phenomena and their effects on the magnetic flux density distribution for each configuration. Subsequently, the air gap flux density and electromagnetic force were quantified under rotor eccentricity caused by unbalanced disturbances, and the dynamic performances of the ARMBs were evaluated for eccentricity along the x-axis and at 45°. Finally, experiments measured the electromagnetic forces acting on the rotor under the NNSS and NSNS configurations during eccentric conditions. The results indicate that the NNSS configuration significantly reduces magnetic circuit coupling, improves the uniformity of electromagnetic force distribution, and offers superior stability and control efficiency under asymmetric conditions. Experimental results deviated by less than 10% from the simulations, confirming the reliability and practicality of the proposed design. These findings provide valuable insights for optimizing ARMB pole configurations and promote their application in high-speed, high-precision industrial fields such as aerospace and power engineering. Full article
(This article belongs to the Section Electronic Sensors)
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<p>Structure of the octupole ARMB. 1—stator core, 2—fixed bracket for coil winding, 3—control coil windings, 4—rotor core, 5—shaft, 6—protective bearing.</p>
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<p>The working principle of the ARMB.</p>
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<p>The control magnetic flux loop of the ARMB.</p>
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<p>Equivalent magnetic circuit of the ARMB in the NNSS pole distribution.</p>
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<p>Schematic diagram of the ARMB and coil fixing bracket assembly.</p>
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<p>The finite element simulation model of the ARMB. 1—stator, 2—coil windings, 3—rotor, 4—shaft.</p>
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<p>Magnetic field lines and magnetic flux density distribution of four magnetic pole forms.</p>
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<p>The magnetic density distribution of different disturbance offsets along the <span class="html-italic">x</span>-axis and 45° direction of the NNSS-type ARMB rotor.</p>
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<p>The magnetic density distribution of different disturbance offsets along the <span class="html-italic">x</span>-axis and 45° direction of the NSNS-type ARMB rotor.</p>
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<p>Unbalanced disturbance of the rotor–magnetic field strength at air gap relationship. (<b>a</b>) NSNS rotor offset along the x-axis in the ARMB in the form of magnetic poles. (<b>b</b>) NNSS rotor offset along the x-axis in the ARMB in the form of magnetic poles. (<b>c</b>) NSNS rotor offset along the 45° angle in the ARMB in the form of magnetic poles. (<b>d</b>) NNSS rotor offset along the 45° angle in the ARMB in the form of magnetic poles.</p>
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<p>Unbalanced disturbance of the rotor–magnetic field strength at air gap relationship. (<b>a</b>) NSNS rotor offset along the x-axis in the ARMB in the form of magnetic poles. (<b>b</b>) NNSS rotor offset along the x-axis in the ARMB in the form of magnetic poles. (<b>c</b>) NSNS rotor offset along the 45° angle in the ARMB in the form of magnetic poles. (<b>d</b>) NNSS rotor offset along the 45° angle in the ARMB in the form of magnetic poles.</p>
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<p>Comparison of the electromagnetic force between two different magnetic pole distribution forms.</p>
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<p>Experimental model composition of the ARMB.</p>
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<p>Current flow in the form of two magnetic poles. (<b>a</b>) NNSS. (<b>b</b>) NSNS.</p>
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<p>The process of experimental testing.</p>
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<p>Plot of the data comparison between the experiment and simulation.</p>
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