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Search Results (4,302)

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11 pages, 4630 KiB  
Article
A Study on the Mechanisms and Performance of a Polyvinyl Alcohol-Based Nanogenerator Based on the Triboelectric Effect
by Wuliang Sun, Junhui Dong, Xiaobo Gao, Baodong Chen and Ding Nan
Materials 2024, 17(18), 4514; https://doi.org/10.3390/ma17184514 (registering DOI) - 14 Sep 2024
Abstract
Polyvinyl alcohol (PVA), a versatile polymer, is extensively used across many industries, such as chemicals, food, healthcare, textiles, and packaging. However, research on applying PVA to triboelectric nanogenerators (TENGs) remains limited. Consequently, we chose PVA as the primary material to explore its contact [...] Read more.
Polyvinyl alcohol (PVA), a versatile polymer, is extensively used across many industries, such as chemicals, food, healthcare, textiles, and packaging. However, research on applying PVA to triboelectric nanogenerators (TENGs) remains limited. Consequently, we chose PVA as the primary material to explore its contact electrification mechanisms at the molecular level, alongside materials like Polyethylene (PE), Polyvinylidene fluoride (PVDF), and Polytetrafluoroethylene (PTFE). Our findings show that PVA has the highest band gap, with the smallest band gap occurring between the HOMO of PVA and the LUMO of PTFE. During molecular contact, electron transfer primarily occurs in the outermost layers of the molecules, influenced by the functional groups of the polymers. The presence of fluorine atoms enhances the electron transfer between PVA and PTFE to maximum levels. Experimental validation confirmed that PVA and PTFE contact yields the highest triboelectric performance: VOC of 128 V, ISC of 2.83 µA, QSC of 82 nC, and an output power of 384 µW. Moreover, P-TENG, made of PVA and PTFE, was successfully applied in self-powered smart devices and monitored human respiration and bodily movements effectively. These findings offer valuable insights into using PVA in triboelectric nanogenerator technologies. Full article
(This article belongs to the Special Issue Nanotechnology and Nanomaterials for Energy Applications)
Show Figures

Figure 1

Figure 1
<p>Electron density isosurface diagrams of PVA (<b>A</b>), PE (<b>B</b>), PVDF (<b>C</b>), and PTFE (<b>D</b>). (<b>E</b>) Simulated frontier orbital energy levels and calculated HOMO–LUMO energy gaps for PVA, PE, PVDF, and PTFE. (<b>F</b>) Orbital energy difference diagrams for PVA, PE, PVDF, and PTFE.</p>
Full article ">Figure 2
<p>(<b>A</b>) Atomic charge transfer at the PVA–PE interface. (<b>B</b>) Atomic charge transfer at the PVA–PVDF interface. (<b>C</b>) Atomic charge transfer at the PVA–PTFE interface. (<b>D</b>) Charge transfer of different atoms in PVA–PE. (<b>E</b>) Charge transfer of different atoms in PVA–PVDF. (<b>F</b>) Charge transfer of different atoms in PVA–PTFE. Note that the columns represent the total transferred charge of the atoms in the polymers. (Note: The atoms marked by the red dashed circles match the charges given in the figure).</p>
Full article ">Figure 3
<p>(<b>A</b>) Structure of the P-TENG. (<b>B</b>) Three-dimensional topography of PE film. (<b>C</b>) Three-dimensional topography of PVDF film. (<b>D</b>) Three-dimensional topography of PTFE film. (<b>E</b>) Three-dimensional topography of PVA film, corresponding electron microscopy images, and fiber diameters. (<b>F</b>) Phase image of PE film. (<b>G</b>) Phase image of PVDF film. (<b>H</b>) Phase image of PTFE film. (<b>I</b>) Phase image of PVA film.</p>
Full article ">Figure 4
<p>(<b>A</b>) Schematic diagram of the working principle of the P-TENG. (<b>B</b>) Contact–separation process of P-TENGs and corresponding electric potential distribution. (<b>C</b>) Schematic diagram of an atomic-level electron cloud/potential well model describing the contact electrification process of P-TENGs.</p>
Full article ">Figure 5
<p>Electric output performance of different polymers in contact–separation with PVA fiber membrane, including voltage (<b>A</b>), current (<b>B</b>), and transferred charge (<b>C</b>). Measurement of the voltage of the P-TENG under different external load resistances at a frequency of 3 Hz and 5 N force, with PVA–PE (<b>D</b>), PVA–PVDF (<b>E</b>), and PVA–PTFE (<b>F</b>). Measurement of the peak power of the P-TENG under different external load resistances at a frequency of 3 Hz and 5 N force, with PVA–PE (<b>G</b>), PVA–PVDF (<b>H</b>), and PVA–PTFE (<b>I</b>).</p>
Full article ">Figure 6
<p>(<b>A</b>) Durability test of the P-TENG, first 5 s (<b>B</b>), last 5 s (<b>C</b>). (<b>D</b>) Capacitive charging curve for the P-TENG. (<b>E</b>) Working circuit diagram of the TENG supplying power to a thermometer. (<b>F</b>) Temperature gauge charging curve of the P-TENG. (<b>G</b>) Respiratory monitoring by the P-TENG. (<b>H</b>) Finger bending monito by the P-TENG. (<b>I</b>) Motion state monitoring by the P-TENG.</p>
Full article ">
32 pages, 16650 KiB  
Article
Hierarchical Structure-Based Wireless Active Balancing System for Power Batteries
by Jia Xie, Huipin Lin, Jifeng Qu, Luhong Shi, Zuhong Chen, Sheng Chen and Yong Zheng
Energies 2024, 17(18), 4602; https://doi.org/10.3390/en17184602 - 13 Sep 2024
Abstract
This paper conducts an in-depth study of a wireless, hierarchical structure-based active balancing system for power batteries, aimed at addressing the rapid advancements in battery technology within the electric vehicle industry. The system is designed to enhance energy density and the reliability of [...] Read more.
This paper conducts an in-depth study of a wireless, hierarchical structure-based active balancing system for power batteries, aimed at addressing the rapid advancements in battery technology within the electric vehicle industry. The system is designed to enhance energy density and the reliability of the battery system, developing a balancing system capable of managing cells with significant disparities in characteristics, which is crucial for extending the lifespan of lithium-ion battery packs. The proposed system integrates wireless self-networking technology into the battery management system and adopts a more efficient active balancing approach, replacing traditional passive energy-consuming methods. In its design, inter-group balancing at the upper layer is achieved through a soft-switching LLC resonant converter, while intra-group balancing among individual cells at the lower layer is managed by an active balancing control IC and a bidirectional buck–boost converter. This configuration not only ensures precise control but also significantly enhances the speed and efficiency of balancing, effectively addressing the heat issues caused by energy dissipation. Key technologies involved include lithium-ion batteries, battery management systems, battery balancing systems, LLC resonant converters, and wireless self-networking technology. Tests have shown that this system not only reduces energy consumption but also significantly improves energy transfer efficiency and the overall balance of the battery pack, thereby extending battery life and optimizing vehicle performance, ensuring a safer and more reliable operation of electric vehicle battery systems. Full article
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Figure 1

Figure 1
<p>Switching waveforms of ZVS and ZCS in resonant converters.</p>
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<p>Full-bridge structure (<b>a</b>) vs. half-bridge structure (<b>b</b>).</p>
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<p>Full-bridge rectification (<b>a</b>) vs. full-wave rectification structure (<b>b</b>).</p>
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<p>Top-level LLC equalization structure diagram.</p>
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<p>Full-bridge LLC converter.</p>
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<p>Initial resonant current in the resonant tank.</p>
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<p>Three operating states of the converters.</p>
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<p>Timing diagram for key mode analysis.</p>
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<p>Schematic diagram of mode 1 current transformer.</p>
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<p>Schematic diagram of mode 2 current transformer.</p>
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<p>Schematic diagram of mode 3 current transformer.</p>
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<p>Flowchart of LLC parameter design process.</p>
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<p>State transition diagram of the LLC equalizer.</p>
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<p>Interrupt execution flow. (<b>a</b>) 20 μs interrupt execution flow. (<b>b</b>) 5 ms interrupt execution flow.</p>
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<p>Hierarchical equalization system scheduling flowchart.</p>
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<p>Star network topology.</p>
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<p>Mesh network topology.</p>
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<p>Top-level central wireless node operational flowchart.</p>
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<p>Physical circuit image of LLC equalization converter.</p>
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<p>LLC equalization digital control board.</p>
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<p>Actual resonant frequency in quasi-resonant state testing.</p>
Full article ">Figure 22
<p>Key waveforms at 10% load. (<b>a</b>) Resonant tank waveform. (<b>b</b>) Secondary-side diode waveforms. (<b>c</b>) Gate drive and drain–source waveforms of switch S₂. (<b>d</b>) Gate drive and drain–source waveforms of switch S₄.</p>
Full article ">Figure 22 Cont.
<p>Key waveforms at 10% load. (<b>a</b>) Resonant tank waveform. (<b>b</b>) Secondary-side diode waveforms. (<b>c</b>) Gate drive and drain–source waveforms of switch S₂. (<b>d</b>) Gate drive and drain–source waveforms of switch S₄.</p>
Full article ">Figure 23
<p>Key waveforms at 50% load. (<b>a</b>) Resonant tank waveform. (<b>b</b>) Diode waveforms. (<b>c</b>) Gate drive and drain–source waveforms of switch S₂. (<b>d</b>) Gate drive and drain–source waveforms of switch S₄.</p>
Full article ">Figure 24
<p>Key waveforms at 100% load. (<b>a</b>) Resonant tank waveform. (<b>b</b>) Diode waveforms. (<b>c</b>) Gate drive and drain–source waveforms of switch S₂. (<b>d</b>) Gate drive and drain–source waveforms of switch S₄.</p>
Full article ">Figure 25
<p>Efficiency curve of the converter.</p>
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<p>State of charge (SOC) variation in static equalization.</p>
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<p>State of charge (SOC) variation process in charging equalization.</p>
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<p>Physical image of intra-module ETA3000 equalization interposer.</p>
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<p>Schematic diagram of equalization interposer insertion.</p>
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<p>Curve of intra-module static equalization at lower level.</p>
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<p>Curve of intra-module charging equalization at lower level.</p>
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<p>Charging equalization current curve.</p>
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<p>Balancing efficiency comparison.</p>
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<p>Energy consumption comparison.</p>
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<p>Cooling power requirement.</p>
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<p>System reliability comparison.</p>
Full article ">
16 pages, 4720 KiB  
Article
Dynamics of a New Four-Thirds-Degree Sub-Quadratic Lorenz-like System
by Guiyao Ke, Jun Pan, Feiyu Hu and Haijun Wang
Axioms 2024, 13(9), 625; https://doi.org/10.3390/axioms13090625 - 12 Sep 2024
Viewed by 105
Abstract
Aiming to explore the subtle connection between the number of nonlinear terms in Lorenz-like systems and hidden attractors, this paper introduces a new simple sub-quadratic four-thirds-degree Lorenz-like system, where x˙=a(yx), [...] Read more.
Aiming to explore the subtle connection between the number of nonlinear terms in Lorenz-like systems and hidden attractors, this paper introduces a new simple sub-quadratic four-thirds-degree Lorenz-like system, where x˙=a(yx), y˙=cxx3z, z˙=bz+x3y, and uncovers the following property of these systems: decreasing the powers of the nonlinear terms in a quadratic Lorenz-like system where x˙=a(yx), y˙=cxxz, z˙=bz+xy, may narrow, or even eliminate the range of the parameter c for hidden attractors, but enlarge it for self-excited attractors. By combining numerical simulation, stability and bifurcation theory, most of the important dynamics of the Lorenz system family are revealed, including self-excited Lorenz-like attractors, Hopf bifurcation and generic pitchfork bifurcation at the origin, singularly degenerate heteroclinic cycles, degenerate pitchfork bifurcation at non-isolated equilibria, invariant algebraic surface, heteroclinic orbits and so on. The obtained results may verify the generalization of the second part of the celebrated Hilbert’s sixteenth problem to some degree, showing that the number and mutual disposition of attractors and repellers may depend on the degree of chaotic multidimensional dynamical systems. Full article
(This article belongs to the Section Mathematical Analysis)
Show Figures

Figure 1

Figure 1
<p>For <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>4</mn> <mo>,</mo> <mn>1</mn> <mo>)</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>∈</mo> <mo>[</mo> <mn>0</mn> <mo>,</mo> <mn>5</mn> <mo>]</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>1</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>1</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>1</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>0.13</mn> <mo>,</mo> <mn>1.3</mn> <mo>,</mo> <mn>1.6</mn> <mo>)</mo> </mrow> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>7</mn> </mrow> </msup> </mrow> </semantics></math>; (<b>a</b>–<b>c</b>) bifurcation diagrams; (<b>d</b>) Lyapunov exponents versus <span class="html-italic">c</span> of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>). In contrast to system (<a href="#FD2-axioms-13-00625" class="html-disp-formula">2</a>) [<a href="#B22-axioms-13-00625" class="html-bibr">22</a>] (Figure 3, p. 363), these figures suggest that the solutions for the system in (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) display stable equilibria and period orbits, rather than the self-excited and hidden attractors shown in the system in (<a href="#FD2-axioms-13-00625" class="html-disp-formula">2</a>).</p>
Full article ">Figure 2
<p>For <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>3</mn> <mo>,</mo> <mn>1.5</mn> <mo>)</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>∈</mo> <mo>[</mo> <mn>0.1</mn> <mo>,</mo> <mn>599.1</mn> <mo>]</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>1.314</mn> <mo>,</mo> <mn>2.236</mn> <mo>,</mo> <mn>4.669</mn> <mo>)</mo> </mrow> </mrow> </semantics></math>; (<b>a</b>–<b>c</b>) bifurcation diagrams; (<b>d</b>) Lyapunov exponents versus <span class="html-italic">c</span> of system (<a href="#FD2-axioms-13-00625" class="html-disp-formula">2</a>). The subfigures (<b>a</b>–<b>c</b>) are consistent with the subfigure (<b>d</b>), showing that system (<a href="#FD2-axioms-13-00625" class="html-disp-formula">2</a>) mainly experiences periodic behaviors.</p>
Full article ">Figure 3
<p>For <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>3</mn> <mo>,</mo> <mn>1.5</mn> <mo>)</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>∈</mo> <mo>[</mo> <mn>0.1</mn> <mo>,</mo> <mn>599.1</mn> <mo>]</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>1.314</mn> <mo>,</mo> <mn>2.236</mn> <mo>,</mo> <mn>4.669</mn> <mo>)</mo> </mrow> </mrow> </semantics></math>; (<b>a</b>–<b>c</b>) bifurcation diagrams; (<b>d</b>) Lyapunov exponents versus <span class="html-italic">c</span> of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>). In contrast with <a href="#axioms-13-00625-f002" class="html-fig">Figure 2</a>, the four subfigures show that system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) mainly behaves in a similar way to self-excited attractors, verifying the introduced property, i.e., a decrease in powers of nonlinear terms of the quadratic Lorenz-like system (<a href="#FD2-axioms-13-00625" class="html-disp-formula">2</a>) may narrow or even eliminate the range of the parameter <span class="html-italic">c</span> for hidden attractors, but enlarge it for self-excited attractors.</p>
Full article ">Figure 4
<p>Phase portraits of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) for <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>c</mi> <mo>,</mo> <mi>b</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>3</mn> <mo>,</mo> <mn>100</mn> <mo>,</mo> <mn>1.5</mn> <mo>)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>1.314</mn> <mo>,</mo> <mn>2.236</mn> <mo>,</mo> <mn>4.669</mn> <mo>)</mo> </mrow> </mrow> </semantics></math> illustrating the existence of two-scroll self-excited attractor suggested in <a href="#axioms-13-00625-f003" class="html-fig">Figure 3</a>.</p>
Full article ">Figure 4 Cont.
<p>Phase portraits of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) for <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>c</mi> <mo>,</mo> <mi>b</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>3</mn> <mo>,</mo> <mn>100</mn> <mo>,</mo> <mn>1.5</mn> <mo>)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>1.314</mn> <mo>,</mo> <mn>2.236</mn> <mo>,</mo> <mn>4.669</mn> <mo>)</mo> </mrow> </mrow> </semantics></math> illustrating the existence of two-scroll self-excited attractor suggested in <a href="#axioms-13-00625-f003" class="html-fig">Figure 3</a>.</p>
Full article ">Figure 5
<p>Poincaré cross-sections of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) for <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>c</mi> <mo>,</mo> <mi>b</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>3</mn> <mo>,</mo> <mn>100</mn> <mo>,</mo> <mn>1.5</mn> <mo>)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>2</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>1.314</mn> <mo>,</mo> <mn>2.236</mn> <mo>,</mo> <mn>4.669</mn> <mo>)</mo> </mrow> </mrow> </semantics></math> showing the geometrical structure of the Lorenz-like attractor depicted in <a href="#axioms-13-00625-f004" class="html-fig">Figure 4</a>.</p>
Full article ">Figure 6
<p>Phase portraits of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) for <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>c</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>1</mn> <mo>,</mo> <mn>36</mn> <mo>)</mo> </mrow> </semantics></math>, (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>0.07</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mn>3</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mn>3</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>3</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mo>±</mo> <mn>1.3</mn> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>8</mn> </mrow> </msup> <mo>,</mo> <mo>±</mo> <mn>1.3</mn> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>7</mn> </mrow> </msup> <mo>,</mo> <mo>−</mo> <mn>1</mn> <mo>)</mo> </mrow> </mrow> </semantics></math>. Both figures imply that collapsing singularly degenerate heteroclinic cycles in system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) create limited cycles rather than strange attractors.</p>
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<p>Phase portraits of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) for <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>c</mi> <mo>,</mo> <mi>b</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>4</mn> <mo>,</mo> <mn>1.8182</mn> <mo>,</mo> <mn>1</mn> <mo>)</mo> </mrow> </semantics></math> and (<b>a</b>) <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mn>3</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mn>3</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>4</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mo>±</mo> <mn>0.13</mn> <mo>,</mo> <mo>±</mo> <mn>1.3</mn> <mo>,</mo> <mn>1.6</mn> <mo>)</mo> </mrow> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>7</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>3</mn> <mo>,</mo> <mn>4</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>3</mn> <mo>,</mo> <mn>4</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>4</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mo>±</mo> <mn>2.4</mn> <mo>,</mo> <mo>±</mo> <mn>2.41</mn> <mo>,</mo> <mn>3.3</mn> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>5</mn> <mo>,</mo> <mn>6</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>5</mn> <mo>,</mo> <mn>6</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>5</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mo>±</mo> <mn>2.39</mn> <mo>,</mo> <mo>±</mo> <mn>2.4</mn> <mo>,</mo> <mn>3.32</mn> <mo>)</mo> </mrow> </mrow> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>3</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>3</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>4</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>2.4</mn> <mo>,</mo> <mn>2.41</mn> <mo>,</mo> <mn>3.3</mn> <mo>)</mo> </mrow> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>5</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>5</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>5</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mn>2.39</mn> <mo>,</mo> <mn>2.4</mn> <mo>,</mo> <mn>3.32</mn> <mo>)</mo> </mrow> </mrow> </semantics></math>, (<b>c</b>) <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>4</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>4</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>4</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mo>−</mo> <mn>2.4</mn> <mo>,</mo> <mo>−</mo> <mn>2.41</mn> <mo>,</mo> <mn>3.3</mn> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mn>6</mn> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mn>6</mn> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>5</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mo>−</mo> <mn>2.39</mn> <mo>,</mo> <mo>−</mo> <mn>2.4</mn> <mo>,</mo> <mn>3.32</mn> <mo>)</mo> </mrow> </mrow> </semantics></math>, showing at least five limit cycles for system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>) when Hopf bifurcation occurs at <math display="inline"><semantics> <msub> <mi>E</mi> <mo>±</mo> </msub> <mo>,</mo> </semantics></math> i.e., two around <math display="inline"><semantics> <msub> <mi>E</mi> <mo>+</mo> </msub> </semantics></math>, two around <math display="inline"><semantics> <msub> <mi>E</mi> <mo>−</mo> </msub> </semantics></math> and one around <math display="inline"><semantics> <msub> <mi>E</mi> <mo>±</mo> </msub> </semantics></math>.</p>
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<p>For <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>a</mi> <mo>,</mo> <mi>c</mi> <mo>)</mo> <mo>=</mo> <mo>(</mo> <mn>6</mn> <mo>,</mo> <mn>100</mn> <mo>)</mo> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>b</mi> <mo>=</mo> <mn>8</mn> <mo>,</mo> <mn>9</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mn>3</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>y</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mn>3</mn> </mrow> </msubsup> <mo>,</mo> <msubsup> <mi>z</mi> <mrow> <mn>0</mn> </mrow> <mn>3</mn> </msubsup> <mo>)</mo> </mrow> <mo>=</mo> <mrow> <mo>(</mo> <mo>±</mo> <mn>0.13</mn> <mo>,</mo> <mo>±</mo> <mn>1.3</mn> <mo>,</mo> <mn>1.6</mn> <mo>)</mo> </mrow> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>7</mn> </mrow> </msup> </mrow> </semantics></math>, phase portraits of system (<a href="#FD1-axioms-13-00625" class="html-disp-formula">1</a>), verifying the existence of a pair of heteroclinic orbits to unstable <math display="inline"><semantics> <msub> <mi>E</mi> <mn>0</mn> </msub> </semantics></math> and stable <math display="inline"><semantics> <msub> <mi>E</mi> <mo>±</mo> </msub> </semantics></math> when <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mn>3</mn> <mi>b</mi> <mo>≥</mo> <mn>4</mn> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </semantics></math>.</p>
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26 pages, 6368 KiB  
Review
Review of Fiber-Reinforced Composite Structures with Multifunctional Capabilities through Smart Textiles
by Birendra Chaudhary, Thomas Winnard, Bolaji Oladipo, Sumanta Das and Helio Matos
Textiles 2024, 4(3), 391-416; https://doi.org/10.3390/textiles4030023 - 12 Sep 2024
Viewed by 286
Abstract
Multifunctional composites and smart textiles are an important advancement in material science, offering a variety of capabilities that extend well beyond traditional structural functions. These advanced materials are poised to revolutionize applications across a wide range of industries, including aerospace, healthcare, military, and [...] Read more.
Multifunctional composites and smart textiles are an important advancement in material science, offering a variety of capabilities that extend well beyond traditional structural functions. These advanced materials are poised to revolutionize applications across a wide range of industries, including aerospace, healthcare, military, and consumer electronics, by embedding functionalities such as structural health monitoring, signal transmission, power transfer, self-healing, and environmental sensing. This review, which draws on insights from various disciplines, including material science, engineering, and technology, explores the manufacturing techniques employed in creating multifunctional composites, focusing on modifying textiles to incorporate conductive fibers, sensors, and functional coatings. The various multifunctional capabilities that result from these modifications and manufacturing techniques are examined in detail, including structural health monitoring, power conduction, power transfer, wireless communication, power storage, energy harvesting, and data transfer. The outlook and potential for future developments are also surveyed, emphasizing the need for improved durability, scalability, and energy efficiency. Key challenges are identified, such as ensuring material compatibility, optimizing fabrication techniques, achieving reliable performance under diverse conditions, and modeling multifunctional systems. By addressing these challenges through ongoing research and further innovation, we can significantly enhance the performance and utility of systems, driving advancements in technology and improving quality of life. Full article
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<p>(<b>a</b>) Global industry trends for multifunctional composites [<a href="#B12-textiles-04-00023" class="html-bibr">12</a>] and (<b>b</b>) recent journal articles for multifunctional composites (data collected from Scopus).</p>
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<p>Schematic illustration of reinforced composite systems.</p>
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<p>Smart textiles utilizing different configurations and techniques to achieve multifunctionality.</p>
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<p>Traditional composites manufacturing processes showing (<b>a</b>) hand lay-up, (<b>b</b>) resign transfer molding, (<b>c</b>) vacuum-assisted resin transfer molding, and (<b>d</b>) prepreg lay-up.</p>
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<p>Additive manufacturing methods.</p>
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<p>Spinning techniques. (<b>a</b>) Electrospinning and (<b>b</b>) solution blow technique.</p>
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<p>Multilevel use case of multifunctional structures and their capabilities for health monitoring, reproduced with permission from [<a href="#B64-textiles-04-00023" class="html-bibr">64</a>].</p>
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<p>Multifunctional composite system with embedded conductive yarns for shock load monitoring and damage detection.</p>
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<p>Power conduction and high-current transmission capabilities of multifunctional carbon/epoxy composites. Note: The arrow represents the transition either to manufacturing procedures or corresponding performance.</p>
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<p>A schematic representation of power transfer and wireless communication utilizing multifunctional composites and smart textiles.</p>
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<p>A schematic representation of a multifunctional structure capable of energy harvesting using thermoelectric, piezoelectric, photovoltaic, and energy storage elements.</p>
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<p>Schematic illustration of the structure and working principle of the triboelectric generator (<b>a</b>) with the structure of an integrated generator in bending and releasing process and (<b>b</b>) proposed mechanism of the triboelectric generator, reproduced with permission from [<a href="#B78-textiles-04-00023" class="html-bibr">78</a>].</p>
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<p>Recent work on smart textiles showcasing the electromechanical performance of textile fabrics with conductive yarn elements for data transfer capabilities [<a href="#B14-textiles-04-00023" class="html-bibr">14</a>].</p>
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<p>Nano- and microscales in a progressive modeling framework of woven composites, reproduced with permission from [<a href="#B101-textiles-04-00023" class="html-bibr">101</a>].</p>
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<p>A multiscale optimization scheme using neural networks, reproduced with permission from [<a href="#B104-textiles-04-00023" class="html-bibr">104</a>].</p>
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21 pages, 1123 KiB  
Article
Hallucination Reduction and Optimization for Large Language Model-Based Autonomous Driving
by Jue Wang
Symmetry 2024, 16(9), 1196; https://doi.org/10.3390/sym16091196 - 11 Sep 2024
Viewed by 296
Abstract
Large language models (LLMs) are widely integrated into autonomous driving systems to enhance their operational intelligence and responsiveness and improve self-driving vehicles’ overall performance. Despite these advances, LLMs still struggle between hallucinations—when models either misinterpret the environment or generate imaginary parts for downstream [...] Read more.
Large language models (LLMs) are widely integrated into autonomous driving systems to enhance their operational intelligence and responsiveness and improve self-driving vehicles’ overall performance. Despite these advances, LLMs still struggle between hallucinations—when models either misinterpret the environment or generate imaginary parts for downstream use cases—and taxing computational overhead that relegates their performance to strictly non-real-time operations. These are essential problems to solve to make autonomous driving as safe and efficient as possible. This work is thus focused on symmetrical trade-offs between the reduction of hallucination and optimization, leading to a framework for these two combined and at least specifically motivated by these limitations. This framework intends to generate a symmetry of mapping between real and virtual worlds. It helps in minimizing hallucinations and optimizing computational resource consumption reasonably. In autonomous driving tasks, we use multimodal LLMs that combine an image-encoding Visual Transformer (ViT) and a decoding GPT-2 with responses generated by the powerful new sequence generator from OpenAI known as GPT4. Our hallucination reduction and optimization framework leverages iterative refinement loops, RLHF—reinforcement learning from human feedback (RLHF)—along with symmetric performance metrics, e.g., BLEU, ROUGE, and CIDEr similarity scores between machine-generated answers specific to other human reference answers. This ensures that improvements in model accuracy are not overused to the detriment of increased computational overhead. Experimental results show a twofold improvement in decision-maker error rate and processing efficiency, resulting in an overall decrease of 30% for the model and a 25% improvement in processing efficiency across diverse driving scenarios. Not only does this symmetrical approach reduce hallucination, but it also better aligns the virtual and real-world representations. Full article
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<p>Hallucination reduction model framework. In this model, for the evaluation part, we use Visual Translator (ViT) as an encoder for image captioning and the GPT-2 model as a decoder. This encoder–decoder architecture enables the model to accurately capture the relationships between visual elements and their textual representations, thus minimizing the potential for misidentifications or erroneous outputs due to hallucination artifacts that can stem from limitations in sensory data interpretation. Then, we use the GPT-4 model to handle both text and image inputs, ensuring that the generated answer more closely aligns with the visual content presented to it. Meanwhile, in each iteration, we use RLFH to reduce the hallucination. By using RLHF, the model can learn to adjust its responses based on the inputs provided from human evaluations. This training loop not only strengthens the model’s ability to produce accurate outputs but also enhances its overall reasoning and understanding of complex queries. After that, we combine the old and new answers and use ChatGPT to evaluate.</p>
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<p>These examples show how the RLHF helps us reduce the hallucination for the text. All the pictures are from HAD [<a href="#B28-symmetry-16-01196" class="html-bibr">28</a>], and in the answer generated by our model, we use yellow color to highlight the hallucination part. Firstly, the question–answer pairs and pictures will be combined as inputs to send to our multi-model. Then, our model will generate an original answer. After that, based on this original answer, we use RLHF to reduce the hallucinations in the answer. Comparing these two answers, we find that the hallucination, highlighted in yellow, was reduced in the answer after applying RLHF.</p>
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<p>Example of hallucination reduction. This is an example to show the process of our model. Firstly, we initialize our model, creating the RewardModel class and the EvaluationSuit class. Secondly, we load the prediction and test files. Thirdly, process the evaluation and record the score. Finally, apply reinforcement learning optimization into each iteration and record the new score.</p>
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<p>Partial result of resource optimization.These are partial experiment results; these results are based on four evaluation metrics <math display="inline"><semantics> <mrow> <msub> <mi>BLEU</mi> <mn>2</mn> </msub> <mspace width="3.33333pt"/> <mo>(</mo> <mi mathvariant="bold">a</mi> <mo>)</mo> <mo>,</mo> <msub> <mi>BLEU</mi> <mn>1</mn> </msub> <mspace width="3.33333pt"/> <mo>(</mo> <mi mathvariant="bold">b</mi> <mo>)</mo> <mo>,</mo> <msub> <mi>ROUGE</mi> <mi>L</mi> </msub> <mspace width="3.33333pt"/> <mo>(</mo> <mi mathvariant="bold">c</mi> <mo>)</mo> <mo>,</mo> <mi>CIDEr</mi> <mspace width="3.33333pt"/> <mo>(</mo> <mi mathvariant="bold">d</mi> <mo>)</mo> </mrow> </semantics></math> from our hallucination reduction model. Optimal theta is the final model parameters, and Lambda and Mu are the final Lagrange multiplier parameters.</p>
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21 pages, 3913 KiB  
Article
Cotton Disease Recognition Method in Natural Environment Based on Convolutional Neural Network
by Yi Shao, Wenzhong Yang, Jiajia Wang, Zhifeng Lu, Meng Zhang and Danny Chen
Agriculture 2024, 14(9), 1577; https://doi.org/10.3390/agriculture14091577 - 11 Sep 2024
Viewed by 198
Abstract
As an essential component of the global economic crop, cotton is highly susceptible to the impact of diseases on its yield and quality. In recent years, artificial intelligence technology has been widely used in cotton crop disease recognition, but in complex backgrounds, existing [...] Read more.
As an essential component of the global economic crop, cotton is highly susceptible to the impact of diseases on its yield and quality. In recent years, artificial intelligence technology has been widely used in cotton crop disease recognition, but in complex backgrounds, existing technologies have certain limitations in accuracy and efficiency. To overcome these challenges, this study proposes an innovative cotton disease recognition method called CANnet, and we independently collected and constructed an image dataset containing multiple cotton diseases. Firstly, we introduced the innovatively designed Reception Field Space Channel (RFSC) module to replace traditional convolution kernels. This module combines dynamic receptive field features with traditional convolutional features to effectively utilize spatial channel attention, helping CANnet capture local and global features of images more comprehensively, thereby enhancing the expressive power of features. At the same time, the module also solves the problem of parameter sharing. To further optimize feature extraction and reduce the impact of spatial channel attention redundancy in the RFSC module, we connected a self-designed Precise Coordinate Attention (PCA) module after the RFSC module to achieve redundancy reduction. In the design of the classifier, CANnet abandoned the commonly used MLP in traditional models and instead adopted improved Kolmogorov Arnold Networks-s (KANs) for classification operations. KANs technology helps CANnet to more finely utilize extracted features for classification tasks through learnable activation functions. This is the first application of the KAN concept in crop disease recognition and has achieved excellent results. To comprehensively evaluate the performance of CANnet, we conducted extensive experiments on our cotton disease dataset and a publicly available cotton disease dataset. Numerous experimental results have shown that CANnet outperforms other advanced methods in the accuracy of cotton disease identification. Specifically, on the self-built dataset, the accuracy reached 96.3%; On the public dataset, the accuracy reached 98.6%. These results fully demonstrate the excellent performance of CANnet in cotton disease identification tasks. Full article
(This article belongs to the Section Digital Agriculture)
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<p>Image display of self-built cotton disease dataset.</p>
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<p>Data preprocessing image display: (<b>a</b>) Self-built cotton disease dataset. (<b>b</b>) Public Cotton Disease Dataset.</p>
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<p>CANnet network architecture diagram. The feature extraction part mainly comprises the RFSC and PCA modules, and the KANs in the classifier part are the main innovations.</p>
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<p>RFSC module diagram.</p>
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<p>(<b>a</b>) The overall architecture of the PCA module. (<b>b</b>) The specific architecture of the SRU module. (<b>c</b>) The specific architecture of the CRU module.</p>
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<p>The confusion matrix diagram of CANnet on two datasets.</p>
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<p>(<b>a</b>) t-SNE plots of ResNet, MobileNetV2, and CANnet on self-built cotton disease datasets. (<b>b</b>) T-sne plots of ResNet, Mobile-Former, and CANnet on publicly available cotton disease datasets.</p>
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<p>(<b>a</b>) t-SNE plots of ResNet, MobileNetV2, and CANnet on self-built cotton disease datasets. (<b>b</b>) T-sne plots of ResNet, Mobile-Former, and CANnet on publicly available cotton disease datasets.</p>
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<p>Bar chart of specific species recognition accuracy using CANnet, ResNet18, and MobileNetV2 on a self-built cotton disease dataset.</p>
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<p>Bar chart of specific species recognition accuracy using CANnet, ResNet18, and Mobile-Former on a public cotton disease dataset.</p>
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<p>Attention visualization maps of ResNet, MobileNetV2, and CANnet on self-built cotton disease datasets. The darker the yellow, the better the attention effect.</p>
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<p>Attention visualization of ResNet, Mobile-Former, and CANnet on a public cotton disease dataset. The darker the yellow, the better the attention effect.</p>
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14 pages, 5783 KiB  
Article
Laser-Melted Wc/Ni-Based Coating Remelting Study on Q235 Steel Surface
by Xianglin Wu, Junhao Chen, Jiang Huang, Wenqing Shi, Qingheng Wang, Fenju An and Jingquan Wu
Coatings 2024, 14(9), 1172; https://doi.org/10.3390/coatings14091172 - 11 Sep 2024
Viewed by 219
Abstract
In order to study the effect of laser remelting on the properties of Q235 steel, WC-enhanced nickel-based remelted layers at different powers were prepared on the surface of Q235 steel using laser cladding technology. Their micro-morphologies were observed using scanning electron microscopy, and [...] Read more.
In order to study the effect of laser remelting on the properties of Q235 steel, WC-enhanced nickel-based remelted layers at different powers were prepared on the surface of Q235 steel using laser cladding technology. Their micro-morphologies were observed using scanning electron microscopy, and their hardness and corrosion resistance were tested using a Vickers hardness tester and an electrochemical workstation. The results show that when the laser power reached 1600 W, the number of WC particles was reduced, the fragments of the broken reinforcement particles were more evenly distributed, the fused layer had the highest uniformity, and the microhardness was more average. Additionally, the corrosion current density reached 2.397 × 10−5 A/cm2, the self-corrosion potential Ecorr of the remelted coatings was positive relative to the substrate, the corrosion resistance was the highest, the coating was uniformly flat, and its hardness was the highest. Full article
(This article belongs to the Special Issue Recent Development in Post-processing for Additive Manufacturing)
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<p>Powder morphology and size distribution. (<b>a</b>) Ni60 powder morphology distribution. (<b>b</b>) WC powder morphology distribution. (<b>c</b>) Ni60 powder size. (<b>d</b>) WC powder size.</p>
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<p>Macroscopic morphology of cladding layer before and after remelting. (<b>a</b>) Macroscopic appearance of non-remelted coating. (<b>b</b>) Macroscopic appearance of remelted layer at 1200 W of power. (<b>c</b>) Macroscopic appearance of remelted layer at 1400 W of power. (<b>d</b>) Macroscopic appearance of remelted layer at 1600 W of power.</p>
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<p>XRD diffraction pattern analysis. (<b>a</b>) Diffractograms of laser cladding layers at different levels of power. (<b>b</b>) Localized enlargement of diffraction patterns of laser cladding layers.</p>
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<p>Fe<sub>3</sub>W<sub>3</sub>C compounds appeared. The generation of Fe<sub>3</sub>W<sub>3</sub>C compounds not only changes the chemical composition of the coating but also has an effect on its properties, improving its hardness and wear resistance.</p>
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<p>Microstructure changes in WC under remelting using different powers.</p>
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<p>EDS analysis of the laser-remelted cross-sections. (<b>a</b>) Laser power of 1400 W. (<b>b</b>) Laser power of 1600 W.</p>
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<p>Hardness distribution of cladding layer section. (<b>a</b>) Cross-section hardness distribution of cladding layer. (<b>b</b>) Average hardnesses of remelting layers at different powers.</p>
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<p>Polarization curve.</p>
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13 pages, 278 KiB  
Article
Biopsychosocial Associates of Psychological Distress and Post-Traumatic Growth among Canadian Cancer Patients during the COVID-19 Pandemic
by Karen M. Zhang, Som D. Mukherjee, Gregory Pond, Michelle I. Roque, Ralph M. Meyer, Jonathan Sussman, Peter M. Ellis and Denise Bryant-Lukosius
Curr. Oncol. 2024, 31(9), 5354-5366; https://doi.org/10.3390/curroncol31090395 - 10 Sep 2024
Viewed by 266
Abstract
Objective: Understanding both the positive and negative psychological outcomes among cancer patients during the pandemic is critical for planning post-pandemic cancer care. This study (1) examined levels of psychological distress and post-traumatic growth (PTG) among Canadian cancer patients during the COVID-19 pandemic and [...] Read more.
Objective: Understanding both the positive and negative psychological outcomes among cancer patients during the pandemic is critical for planning post-pandemic cancer care. This study (1) examined levels of psychological distress and post-traumatic growth (PTG) among Canadian cancer patients during the COVID-19 pandemic and (2) explored variables that were associated with psychological distress and PTG during the pandemic using a biopsychosocial framework. Method: A cross-section survey was undertaken of patients receiving ongoing care at a regional cancer centre in Ontario, Canada, between February and December 2021. Self-reported questionnaires assessing sociodemographic information, social difficulties, psychological distress (depression, anxiety fear of recurrence, and emotional distress), PTG, illness perceptions, and behavioural responses to the pandemic were administered. Disease-related information was extracted from patient health records. Results: Prevalences of moderate to severe levels of depression, anxiety, fear of recurrence and emotional distress were reported by 26.0%, 21.2%, 44.2%, and 50.0% of the sample (N = 104), respectively. Approximately 43% of the sample reported experiencing high PTG, and these positive experiences were not associated with levels of distress. Social factors, including social difficulties, being female, lower education, and unemployment status were prominent associative factors of patient distress. Perceptions of the pandemic as threatening, adopting more health safety behaviours, and not being on active treatment also increased patient likelihood to experience severe psychological distress. Younger age and adopting more health safety behaviours increased the likelihood of experiencing high PTG. The discriminatory power of the predictive models was strong, with a C-statistic > 0.80. Conclusions: Examining both the positive and negative psychological patient outcomes during the pandemic has highlighted the complex range of coping responses. Interventions that adopt a multi-pronged approach to screen and address social distress, as well as to leverage health safety behaviours, may improve the adjustments in the pandemic aftermath. Full article
24 pages, 359 KiB  
Article
Didier Eribon vs. ‘The People’—A Critique of Chantal Mouffe’s Left Populism
by Pascal Oliver Omlin
Philosophies 2024, 9(5), 143; https://doi.org/10.3390/philosophies9050143 - 9 Sep 2024
Viewed by 402
Abstract
In this article, I develop a critique of Chantal Mouffe’s leftist populism and its construction of ‘the people’ against an opposed ‘them’, from a perspective informed by the thought of Didier Eribon. I draw on both his public interventions and his theoretical work, [...] Read more.
In this article, I develop a critique of Chantal Mouffe’s leftist populism and its construction of ‘the people’ against an opposed ‘them’, from a perspective informed by the thought of Didier Eribon. I draw on both his public interventions and his theoretical work, employing his concepts of return, society as verdict, and his two principles of critical thinking to question the desirability of crafting ‘the people’ in the first place. I contend that Eribon’s critique renders Mouffe’s proposal problematic on three accounts. First, her approach is too politically volatile; its instability leaves it devoid of a critical analysis of the differences between concrete social positions, struggles, and subjectivities within ‘the people’. Consequently, the political becomes merely a function of the social. Yet, the social and its determining power remain mostly unaddressed by her framework. Second, its simplistic opposition of an overly generalised ‘the people’ against ‘the oligarchy’ is susceptible to right-wing populist appropriations. Third, for a shot at hegemony and a general appeal, it eclipses plurality and dissensus within ‘the people’. In contrast, Eribon encourages a connection between the social and the political by suggesting that a self-critical analysis be mutually intertwined with social analysis. Instead of merely mobilising affects, they must be critically interrogated. Instead of summoning ‘the people’, a return to their respective genesis must be attempted. Unless both principles of critical thinking, the insights of return, and societal verdicts are deployed to come to terms with the social determinisms at hand, the ‘people’s’ mobilisation against an opposed ‘them’ risks sacrificing pluralism and equality alike and neglecting the criteria of the desirability of specific changes in favour of a “whatever it costs” attempt at hegemony. Full article
(This article belongs to the Special Issue Theories of Plurality and the Democratic We)
13 pages, 5845 KiB  
Review
Graphene–Liquid Crystal Synergy: Advancing Sensor Technologies across Multiple Domains
by Mohammad A. Adeshina, Abdulazeez M. Ogunleye, Hakseon Lee, Bharathkumar Mareddi, Hyunmin Kim and Jonghoo Park
Materials 2024, 17(17), 4431; https://doi.org/10.3390/ma17174431 - 9 Sep 2024
Viewed by 356
Abstract
This review explores the integration of graphene and liquid crystals to advance sensor technologies across multiple domains, with a focus on recent developments in thermal and infrared sensing, flexible actuators, chemical and biological detection, and environmental monitoring systems. The synergy between graphene’s exceptional [...] Read more.
This review explores the integration of graphene and liquid crystals to advance sensor technologies across multiple domains, with a focus on recent developments in thermal and infrared sensing, flexible actuators, chemical and biological detection, and environmental monitoring systems. The synergy between graphene’s exceptional electrical, optical, and thermal properties and the dynamic behavior of liquid crystals leads to sensors with significantly enhanced sensitivity, selectivity, and versatility. Notable contributions of this review include highlighting key advancements such as graphene-doped liquid crystal IR detectors, shape-memory polymers for flexible actuators, and composite hydrogels for environmental pollutant detection. Additionally, this review addresses ongoing challenges in scalability and integration, providing insights into current research efforts aimed at overcoming these obstacles. The potential for multi-modal sensing, self-powered devices, and AI integration is discussed, suggesting a transformative impact of these composite sensors on various sectors, including health, environmental monitoring, and technology. This review demonstrates how the fusion of graphene and liquid crystals is pushing the boundaries of sensor technology, offering more sensitive, adaptable, and innovative solutions to global challenges. Full article
(This article belongs to the Special Issue Structural and Physical Properties of Liquid Crystals)
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<p>Three phases of a thermotropic liquid crystal.</p>
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<p>General classification of most popular liquid crystal phases.</p>
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<p>General strategies for the synthesis of graphene and its derivatives. Ref. [<a href="#B25-materials-17-04431" class="html-bibr">25</a>] reproduced with permission from Springer Nature.</p>
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<p>Graphene–liquid crystal composites for IR detection and temperature sensing. (<b>a</b>) Schematic of IR detector setup: LC-rGO cell, polarized optical microscope (POM), and IR source. (<b>b</b>) LC-rGO cell structure. (<b>c</b>) Diagram illustrating photothermal effect on LC-rGO orientational disorder under IR irradiation. (<b>d</b>) Time-lapse POM images of LC-rGO cells at 0–40 s (<b>i</b>–<b>iv</b>) during IR exposure. (<b>e</b>) RGB time-evolution and temperature rise analysis of LC-rGO cell [<a href="#B26-materials-17-04431" class="html-bibr">26</a>]. (<b>f</b>) Microscopic temperature visualization in porous graphene using cholesteric liquid crystal microcapsules (CLCMs), showing heat transfer from lower right corner. (<b>g</b>) Comparative thermal response data for various LC configurations [<a href="#B27-materials-17-04431" class="html-bibr">27</a>] reproduced with permission.</p>
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<p>(<b>a</b>) Preparation and characterization of LCE-rGO composites, showing precursor reactants, cross-linked matrix network formation, monodomain state formation in nematic phase polymer network, and optical images of partially and fully cross-linked LCE-rGO. (<b>b</b>) Reversible memory deformation of LCE-rGO by microwave irradiation. (<b>c</b>) Thermal infrared images of LC-rGO during whole microwave drive. Ref. [<a href="#B29-materials-17-04431" class="html-bibr">29</a>] reproduced with permission. (<b>d</b>) Schematic of reversible photomechanical actuation and actuation stress response in graphene/LCE nanocomposites under NIR light. Ref. [<a href="#B30-materials-17-04431" class="html-bibr">30</a>] reproduced with permission. (<b>e</b>) Thermo-elastic behavior of modified liquid crystal elastomers. Ref. [<a href="#B31-materials-17-04431" class="html-bibr">31</a>] reproduced with permission. (<b>f</b>) LCE micropillar in 118 °C silicon oil with laser on/off and length change in LCE pillars with temperature, with POM insets at different temperatures. Ref. [<a href="#B32-materials-17-04431" class="html-bibr">32</a>] reproduced with permission. (<b>g</b>) Shape-memory characteristics of liquid-crystalline elastomer/graphene oxide nanocomposites. Ref. [<a href="#B33-materials-17-04431" class="html-bibr">33</a>] reproduced with permission. (<b>h</b>) Schematic of light-driven deformation in bilayer films, with isotropic shrinkage in GO layer and anisotropic contraction in ALCN layer. (<b>i</b>) Crawling robot with ALCN outer layer and GO inner layer, responding to UV light. Soft robot and foot-shaped actuator move along UV laser direction, indicated by black arrows. (<b>j</b>) Biomimetic behaviors of GO-ALCN microrobots with concentric and leaf-like GO layers under UV/NIR light, showing real-time light-controlled deformations. Ref. [<a href="#B34-materials-17-04431" class="html-bibr">34</a>] reproduced with permission. Copyright 2020 American Chemical Society.</p>
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<p>(<b>a</b>) Schematic of the setup for inducing lipid liquid-crystal phase change through near-infrared irradiation of graphene particles. (<b>b</b>) Polarized optical microscopy images showing the orientation disruption of liquid crystals due to graphene oxide interaction. Ref. [<a href="#B35-materials-17-04431" class="html-bibr">35</a>] reproduced with permission. (<b>c</b>) Diagram illustrating the synthesis of graphene oxide/double-stranded DNA composite liquid crystals and hydrogels. (<b>d</b>) Optical and SEM images depicting the structural characteristics of these hydrogels. Ref. [<a href="#B36-materials-17-04431" class="html-bibr">36</a>] reproduced with permission. (<b>e</b>) Setup for graphene-induced photothermal liquid crystal transitions and (<b>f</b>) the corresponding temperature–time response graph showing different phases during IR exposure. Ref. [<a href="#B37-materials-17-04431" class="html-bibr">37</a>] reproduced with permission Copyright 2015 American Chemical Society. (<b>g</b>) Chemical structures of doxorubicin and its electrochemical derivatives. (<b>h</b>) Time-dependent current response for detecting doxorubicin, highlighting the sensor’s sensitivity. (<b>i</b>) Cyclic voltammetry graphs demonstrating the electrochemical detection capabilities of doxorubicin using graphene quantum dots and Cu(I) liquid crystals. Ref. [<a href="#B38-materials-17-04431" class="html-bibr">38</a>] reproduced with permission under Creative Commons license.</p>
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<p>(<b>a</b>) Schematic of the graphene-based system showing the effect of temperature and electric fields for smart window application. (<b>b</b>) Phase transitions of a chiral liquid crystal mixture observed with POM, from isotropic to N* and SmA* phases ranging from 25.0 °C to 45.0 °C. Ref. [<a href="#B39-materials-17-04431" class="html-bibr">39</a>] reproduced with permission. (<b>c</b>) Diagram of light transmission and scattering in graphene and cholesteric liquid crystal (ChLC) composites, showing adaptive transparency: planar texture when off and focal conic texture when on, indicating potential for environmental monitoring. (<b>d</b>) Optical image demonstrating environmental clarity changes through a graphene-based filter system and structural and domain analysis of graphene/ChLC composites under polarized light. Ref. [<a href="#B40-materials-17-04431" class="html-bibr">40</a>] reproduced with permission Copyright 2018 American Chemical Society. (<b>e</b>) Device showing hue and saturation changes in transmitted light with varying heating voltages and polarizations, applicable as visual indicators for environmental monitoring. (<b>f</b>) Diagram and differential scanning calorimetry (DSC) graph showing temperature range and phase transitions in ChLC/graphene systems. Sequential images depicting color change in the ChLC/graphene system at various temperatures, ranging from −45 °C to −82 °C, indicating different environmental conditions. Ref. [<a href="#B41-materials-17-04431" class="html-bibr">41</a>] reproduced with permission Copyright 2023 American Chemical Society.</p>
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10 pages, 266 KiB  
Article
Anxiety and Depression in Advanced and Metastatic Lung Cancer Patients—Correlations with Performance Status and Type of Treatment
by Roxana-Andreea Rahnea-Nita, Laura-Florentina Rebegea, Mihaela Dumitru, Radu-Iulian Mitrica, Alexandru Nechifor, Dorel Firescu, Adrian-Cornel Maier, Georgiana Bianca Constantin, Valentin-Titus Grigorean and Gabriela Rahnea-Nita
Medicina 2024, 60(9), 1472; https://doi.org/10.3390/medicina60091472 - 9 Sep 2024
Viewed by 249
Abstract
Background and Objectives: The treatment of advanced and metastatic lung cancer is multimodal, and it is coordinated by a multidisciplinary team. Anxiety and depression occur frequently in patients with lung cancer, creating considerable discomfort in therapeutic management. At the same time, these [...] Read more.
Background and Objectives: The treatment of advanced and metastatic lung cancer is multimodal, and it is coordinated by a multidisciplinary team. Anxiety and depression occur frequently in patients with lung cancer, creating considerable discomfort in therapeutic management. At the same time, these psychoemotional symptoms affect the patients’ quality of life. Objective: This research seeks to identify correlations both between anxiety and depression and the patients’ performance statuses, as well as between anxiety and depression and the type of treatment: radiotherapy, chemotherapy, tyrosine kinase inhibitors (TKI), immunotherapy and palliative care. Materials and Methods: The study evaluated 105 patients with lung cancer from two oncologic centers. Patients were assessed for anxiety and depression using the questionnaire Hospital Anxiety and Depression Scale (HADS). The HADS is a self-report rating scale of 14 items. It measures anxiety and depression, and has two subscales. There are seven items for each subscale. There are 4-point Likert scale ranging from 0 to 3. For each subscale, the score is the sum of the seven items, ranging from 0 to 21. Results: The most powerful correlation with statistical significance was observed between the IT type of treatment (immunotherapy) and the normal level of anxiety, PC = 0.82 (p < 0.001) as well as the normal level of depression. Palliative treatment was correlated with anxiety and depression, both borderline and abnormal. For ECOG 3–4 performance status and abnormal anxiety, respectively, abnormal depression was significantly associated. Also, continuous hospitalization was associated with abnormal anxiety and depression. Conclusions: Early assessments of anxiety and depression are necessary in patients with advanced and metastatic lung cancer, with unfavorable performance status, who have been admitted to continuous hospitalization, and who require palliative care. Full article
(This article belongs to the Section Psychiatry)
35 pages, 28009 KiB  
Article
Optoelectronics Interfaces for a VLC System for UHD Audio-Visual Content Transmission in a Passenger Van: HW Design
by Carlos Iván del Valle Morales, Juan Sebastián Betancourt Perlaza, Juan Carlos Torres Zafra, Iñaki Martinez-Sarriegui and José Manuel Sánchez-Pena
Sensors 2024, 24(17), 5829; https://doi.org/10.3390/s24175829 - 8 Sep 2024
Viewed by 472
Abstract
This work aims to provide the hardware (HW) design of the optoelectronics interfaces for a visible-light communication (VLC) system that can be employed for several use cases. Potential applications include the transmission of ultra-high-definition (UHD) streaming video through existing reading lamps installed in [...] Read more.
This work aims to provide the hardware (HW) design of the optoelectronics interfaces for a visible-light communication (VLC) system that can be employed for several use cases. Potential applications include the transmission of ultra-high-definition (UHD) streaming video through existing reading lamps installed in passenger vans. In this use case, visible light is employed for the downlink, while infrared light is used for the uplink channel, acting as a remote controller. Two primary components -a Light Fidelity (LiFi) router and a USB dongle—were designed and implemented. The ‘LiFi Router’, handling the downlink channel, comprises components such as a visible Light-Emitting Diode (LED) and an infrared receiver. Operating at a supply voltage of 12 V and consuming current at 920 mA, it is compatible with standard voltage buses found in transport vehicles. The ‘USB dongle’, responsible for the uplink, incorporates an infrared LED and a receiver optimized for visible light. The USB dongle works at a supply voltage of 5 V and shows a current consumption of 1.12 A, making it well suited for direct connection to a universal serial bus (USB) port. The bandwidth achieved for the downlink is 11.66 MHz, while the uplink’s bandwidth is 12.27 MHz. A system competent at streaming UHD video with the feature of being single-input multiple-output (SIMO) was successfully implemented via the custom hardware design of the optical transceivers and optoelectronics interfaces. To ensure the system’s correct performance at a distance of 110 cm, the minimum signal-to-noise ratio (SNRmin) for both optical links was maintained at 10.74 dB. We conducted a proof-of-concept test of the VLC system in a passenger van and verified its optimal operation, effectively illustrating its performance in a real operating environment. Exemplifying potential implementations possible with the hardware system designed in this work, a bit rate of 15.2 Mbps was reached with On–Off Keying (OOK), and 11.25 Mbps was obtained with Quadrature Phase Shift Keying (QPSK) using Orthogonal Frequency-Division Multiplexing (OFDM) obtaining a bit-error rate (BER) of 3.3259 × 10−5 in a passenger van at a distance of 72.5 cm between the LiFi router and the USB dongle. As a final addition, a solar panel was installed on the passenger van’s roof to power the user’s laptop and the USB dongle via a power bank battery. It took 13.4 h to charge the battery, yielding a battery life of 22.3 h. This characteristic renders the user’s side of the system entirely self-powered. Full article
(This article belongs to the Special Issue Sensing Technologies and Optical Communication)
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<p>The LiFi router, located on the vehicle’s interior roof, connects to the content server via a wireless Internet connection. The USB dongle, connected to the user’s portable device, receives and plays the audio-visual content as described.</p>
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<p>Block diagram of the VLC proposed system.</p>
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<p>Equivalent simplified circuit of the LUW-CN7N-KYLX-EMKM OSRAM LED for AC.</p>
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<p>LED driver based on a division voltage for n-type MOSFET.</p>
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<p>Phase-advance equalizer.</p>
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<p>Phase-advance equalizer implemented for (<b>a</b>) the first stage for a pole located at 1.8 MHz, and (<b>b</b>) the second stage for a pole located at 9 MHz.</p>
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<p>LED driver implemented with 2 equalization and 2 amplification stages.</p>
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<p>Simulated frequency response of the proposed LED driver based on two amplification and two equalization stages.</p>
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<p>(<b>a</b>) Set-up implemented to take the frequency response measurement of the LUW-CN7N-KYLX-EMKM OSRAM LED and its LED driver based on 2 equalization and 2 amplification stages; (<b>b</b>) frequency response measurement of the LUW-CN7N-KYLX-EMKM OSRAM LED and its LED driver based on 2 equalization and 2 amplification stages.</p>
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<p>Frequency response measurement of the IR HSDL-4250 LED and its LED driver based on 2 equalization and 2 amplification stages.</p>
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<p>PD driver implemented with three amplifier stages.</p>
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<p>Simulated frequency response of the PD driver implemented with three amplifier stages.</p>
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<p>(<b>a</b>) Set-up of the frequency response of the PD driver implemented with three amplifier stages using the LUW-CN7N-KYLX-EMKM OSRAM LED; (<b>b</b>) frequency response of the PD driver implemented with three amplifier stages using the LUW-CN7N-KYLX-EMKM OSRAM LED.</p>
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<p>Frequency response of the PD driver implemented with three amplifier stages using the IR HSDL-4250 LED.</p>
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<p>Block diagram of the FPGA/LED driver interface.</p>
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<p>Block diagram of the PD driver/FPGA interface.</p>
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<p>Schematic design of the FPGA/LED driver connection.</p>
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<p>Schematic design of the PD driver/FPGA connection.</p>
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<p>TE0720 SoC includes the FPGA Xilinx XA7z020-1CLG484Q.</p>
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<p>Diagram of the interaction between external interface, TE0720 SoC, and internal interface.</p>
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<p>Internal interface PCB: (<b>a</b>) top view; (<b>b</b>) bottom view.</p>
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<p>(<b>a</b>) LiFi router external interface PCB; (<b>b</b>) USB dongle external interface PCB.</p>
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<p>Block diagram of all PCBs that are part of the system.</p>
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<p>Schematic connection of the components of the system for LiFi router and USB dongle.</p>
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<p>(<b>a</b>) PCBs stack of TE0720 SoC, internal and external interfaces; (<b>b</b>) LiFi router.</p>
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<p>(<b>a</b>) PCBs stack of TE0720 SoC, internal and external interfaces; (<b>b</b>) USB dongle.</p>
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<p>Set-up carried out to test every module of the system.</p>
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<p>Scheme of the testing procedure for the transmitter block.</p>
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<p>Tests carried out in the transmitter block utilizing a (<b>a</b>) visible LED and (<b>b</b>) IR LED.</p>
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<p>Implemented test to validate the receiver block.</p>
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<p>ILA captured at the ADC’s outputs.</p>
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<p>Test carried out to validate the Tx block and Rx block working in closed loop.</p>
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<p>LiFi router and USB dongle packed in boxes.</p>
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<p>The VLC system developed was deployed using a Ford Transit model van.</p>
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<p>The user’s laptop playing a UHD video streaming due to the implemented USB dongle.</p>
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Article
Design and Experimental Testing of Extended-Range Power Supply System for 15 Horsepower Electric Tractor
by Baochao Wang, Yanshi Lv, Xianggang Chu, Dongwei Wang and Shuqi Shang
Agriculture 2024, 14(9), 1551; https://doi.org/10.3390/agriculture14091551 - 7 Sep 2024
Viewed by 467
Abstract
Electric tractors have many advantages, including high torque, excellent controllability, energy efficiency, a simple structure, and an electric interface for expansion. However, a significant limitation lies in their endurance. This study presents the design of an extended-range power supply system to ensure continuous [...] Read more.
Electric tractors have many advantages, including high torque, excellent controllability, energy efficiency, a simple structure, and an electric interface for expansion. However, a significant limitation lies in their endurance. This study presents the design of an extended-range power supply system to ensure continuous endurance for an electric tractor. The objective is to provide a continuous power source for our self-developed electric tractor while preserving the benefits of electric propulsion. Extended-range power systems utilize a primary mover, typically an oil-fueled internal combustion engine, to drive the generator for electricity generation, and the generated AC-form electricity is subsequently converted into stable DC bus voltage by a power electronic converter. The hardware and control design of an extended-range power supply system are finalized and validated through experimental trials. The results demonstrate the system’s capability to sustain stable DC bus voltage amidst disruptions such as sudden load shifts and fluctuations in the prime mover’s speed. Even with a 50% sudden load change, the voltage drop is within 12% and can recover to ±3% within 4 s. The extended-range can be used alone without a battery to power the electric tractor, or it can used in parallel with other extended ranges or batteries for power sharing thanks to the droop control ability. Full article
(This article belongs to the Section Agricultural Technology)
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<p>Power block diagram of the extended-range electric tractor system.</p>
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<p>Power block diagram of the extended-range electric tractor system.</p>
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<p>Block diagram of an extended-range power supply system.</p>
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<p>Current control equivalent structure diagram.</p>
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<p>Open-loop Bode diagram of current loop.</p>
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<p>Response characteristics simulated curve of <math display="inline"><semantics> <msub> <mi>i</mi> <mi>q</mi> </msub> </semantics></math>.</p>
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<p>Equivalent structure diagram of voltage loop.</p>
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<p>Equivalent structure diagram of voltage loop.</p>
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<p>Simulation results of voltage control.</p>
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<p>Characteristic curve of voltage droop control.</p>
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<p>Extended-range power supply system experiment bench.</p>
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<p>Bench experiment results of current control: (<b>a</b>) dynamic performance; (<b>b</b>) steady-state generator current waveform.</p>
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<p>Starting procedure at different initial speeds of prime mover: (<b>a</b>) 1400 r/min; (<b>b</b>) 1800 r/min; (<b>c</b>) 2200 r/min; (<b>d</b>) 2600 r/min.</p>
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<p>Bench experiment results of the voltage loop: (<b>a</b>) 3 kW power loads; (<b>b</b>) 5 kW power loads; (<b>c</b>) 10 kW power loads; (<b>d</b>) DC current.</p>
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<p>Bench experiment results of droop control: (<b>a</b>) bus voltage with varying load; (<b>b</b>) DC current.</p>
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20 pages, 1148 KiB  
Article
Beyond the Classroom: Integrating the ORID Model for In-Depth Reflection and Assessment in Service-Learning
by Fatma Kayan Fadlelmula and Saba Mansoor Qadhi
Educ. Sci. 2024, 14(9), 987; https://doi.org/10.3390/educsci14090987 - 7 Sep 2024
Viewed by 314
Abstract
Service-learning is a community-based learning approach that bridges academic knowledge with practical application through purposeful exploration, action, and reflection. In addition to enhancing academic learning in various disciplines, service-learning cultivates students’ self-awareness, personal values, and social responsibility, preparing them with essential skills for [...] Read more.
Service-learning is a community-based learning approach that bridges academic knowledge with practical application through purposeful exploration, action, and reflection. In addition to enhancing academic learning in various disciplines, service-learning cultivates students’ self-awareness, personal values, and social responsibility, preparing them with essential skills for life beyond the classroom. However, due to its experiential nature, service-learning presents challenges for effective assessment. This study provides a concrete example of student reflections structured by the Objective, Reflective, Interpretive, and Decisional (ORID) model in practice. Content analysis was implemented by examining undergraduate students’ end-of-semester reflection papers while volunteering during the 2022 FIFA World Cup in Qatar. The results showed that the model provided a guided and structured format for students to reflect on their service-learning, going beyond reporting on factual details to engaging in profound reflections on the emotional, cognitive, and prospective aspects. Moreover, with the solution aspect added to the model, students could express their creativity, articulating on innovative solutions they proposed to overcome challenges and how they turned the challenges into favorable outcomes. Clearly, the model stands as a powerful tool for educators, offering deeper insights into students’ authentic experiences, fostering comprehensive, critical, and insightful reflection, and thereby facilitating the effective assessment of experiential learning. Full article
(This article belongs to the Special Issue The Role of Reflection in Teaching and Learning)
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<p>Challenges faced during volunteering.</p>
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<p>Feelings about volunteering experience.</p>
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<p>Information and skills learned during volunteering.</p>
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<p>Plans for the future.</p>
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<p>Opportunities for the future.</p>
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14 pages, 6765 KiB  
Article
Conceptual Piezoelectric-Based Energy Harvester from In Vivo Heartbeats’ Cyclic Kinetic Motion for Leadless Intracardiac Pacemakers
by Majid Khazaee, Sam Riahi and Alireza Rezania
Micromachines 2024, 15(9), 1133; https://doi.org/10.3390/mi15091133 - 6 Sep 2024
Viewed by 385
Abstract
This paper studies the development of piezoelectric energy harvesting for self-powered leadless intracardiac pacemakers. The energy harvester fit inside the battery compartment, assuming that the energy harvester would replace the battery with a smaller rechargeable battery capacity. The power output analysis was derived [...] Read more.
This paper studies the development of piezoelectric energy harvesting for self-powered leadless intracardiac pacemakers. The energy harvester fit inside the battery compartment, assuming that the energy harvester would replace the battery with a smaller rechargeable battery capacity. The power output analysis was derived from the three-dimensional finite element analysis and in vivo heart measurements. A Doppler laser at the anterior basal in the right ventricle directly measured the heart’s kinetic motion. Piezoceramics in the cantilevered configuration were studied. The heart motion was periodic but not harmonic and shock-based. This study found that energy can be harvested by applying periodic bio-movements (cardiac motion). The results also showed that the energy harvester can generate 1.1 V voltage. The effect of various geometrical parameters on power generation was studied. This approach offers potential for self-powered implantable medical devices, with the harvested energy used to power devices such as pacemakers. Full article
(This article belongs to the Section A:Physics)
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<p>Intracardiac leadless pacemaker and the heart kinetic-energy-based harvesting concept.</p>
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<p>(<b>a</b>) ECG signal from a 69-year-old male patient with normal sinus rhythm [<a href="#B27-micromachines-15-01133" class="html-bibr">27</a>] with zoomed-in views at two 1.5 s time intervals (I) and (II) are zoomed-in ECG signals, and (<b>b</b>) Fourier transform of the ECG and (i–iv) zoomed-in view of typical heart rate frequencies.</p>
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<p>Kinetic heart motion during heart beating and respiration: (<b>a</b>) direct laser measurement of the lower point of the heart in the midline, and (<b>b</b>) zoomed-in shock-based cardiac cycle motion.</p>
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<p>The measurements of in vivo heart displacement at two points on the heart surface.</p>
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<p>(<b>a</b>) The experimental setup; (<b>b</b>) measured impact force, acceleration, and piezoelectric voltage under the impact; and (<b>c</b>) fast Fourier transform of voltage.</p>
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<p>(<b>a</b>) Intracardiac leadless pacemaker: concept of an energy-harvesting beam, rectifier, and energy storage; (<b>b</b>) dimensions of the energy harvester and study parameters.</p>
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<p>The piezoelectric cantilevered beam mechanical response under heart kinetic motion versus different tip masses: (<b>a</b>) open-circuit piezoelectric voltage; (<b>b</b>) piezoelectric beam tip deformation; (<b>c</b>) axial strain for t = 0.97 s, where the voltage is maximum; (<b>d</b>) surface electrical potential for t = 0.97 s, where the voltage is maximum.</p>
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<p>The piezoelectric cantilevered beam mechanical response under heart kinetic motion versus different piezoelectric layer thicknesses: (<b>a</b>) open-circuit piezoelectric voltage; (<b>b</b>) piezoelectric beam tip deformation; (<b>c</b>) axial strain with <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>p</mi> </msub> </mrow> </semantics></math> = 0.2 mm for t = 0.97 s, where the voltage is maximum; and (<b>d</b>) axial strain with <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>p</mi> </msub> </mrow> </semantics></math> = 0.4 mm for t = 0.97 s, where the voltage is maximum.</p>
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<p>The piezoelectric cantilevered beam’s mechanical response under heart kinetic motion with different orientations of the intracardiac leadless pacemaker; (<b>a</b>) open-circuit piezoelectric voltage; (<b>b</b>) piezoelectric beam tip deformation; (<b>c</b>) axial strain with <math display="inline"><semantics> <mi>θ</mi> </semantics></math> = 90° for t = 0.97 s, where the voltage is maximum; and (<b>d</b>) axial strain with <math display="inline"><semantics> <mi>θ</mi> </semantics></math> = 45°mm for t = 0.97 s, where the voltage is maximum.</p>
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<p>The investigation of variable-thickness piezoelectric layers, (<b>a</b>) open-circuit voltage for two parameters with different thickness, (<b>b</b>) axial strain for <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>p</mi> </msub> </mrow> </semantics></math> = 0.2 mm and <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>t</mi> </mrow> </msub> </mrow> </semantics></math> = 0.7 mm (<math display="inline"><semantics> <mi>η</mi> </semantics></math> = 0.71), and (<b>c</b>) axial strain for <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mi>p</mi> </msub> </mrow> </semantics></math> = 0.1 mm and <math display="inline"><semantics> <mrow> <msub> <mi>t</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>t</mi> </mrow> </msub> </mrow> </semantics></math> = 0.35 mm (<math display="inline"><semantics> <mi>η</mi> </semantics></math> = 0.71).</p>
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<p>The electrical performance of a five-stage Dickson charge pump (MDCP) with an AC voltage source of 1.1 V and 1 Hz.</p>
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