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18 pages, 9884 KiB  
Article
The Far-Infrared Absorption Spectrum of HD16O: Experimental Line Positions, Accurate Empirical Energy Levels, and a Recommended Line List
by Semen N. Mikhailenko, Ekaterina V. Karlovets, Aleksandra O. Koroleva and Alain Campargue
Molecules 2024, 29(23), 5508; https://doi.org/10.3390/molecules29235508 - 21 Nov 2024
Abstract
The far-infrared absorption spectrum of monodeuterated water vapor, HD16O, is analyzed using three high-sensitivity absorption spectra recorded by high-resolution Fourier transform spectroscopy at the SOLEIL synchrotron facility. The gas sample was obtained using a 1:1 mixture of H2O and [...] Read more.
The far-infrared absorption spectrum of monodeuterated water vapor, HD16O, is analyzed using three high-sensitivity absorption spectra recorded by high-resolution Fourier transform spectroscopy at the SOLEIL synchrotron facility. The gas sample was obtained using a 1:1 mixture of H2O and D2O leading to a HDO abundance close to 50%. The room temperature spectra recorded in the 50–720 cm−1 range cover most of the rotational band. The sensitivity of the recordings allows for lowering by three orders of magnitude the detectivity threshold of previous absorption studies in the region. Line centers are determined with a typical accuracy of 5 × 10−5 cm−1 for well-isolated lines. The combined line list of 8522 water lines is assigned to 9186 transitions of the nine stable water isotopologues (H2XO, HDXO, and D2XO with X = 16, 17, and 18). Regarding the HD16O isotopologue, a total of 2443 transitions are presently assigned while about 530 absorption transitions were available prior to our SOLEIL recordings. The comparison with the HITRAN list of HD16O transitions is discussed in detail. The obtained set of accurate HD16O transition frequencies is merged with literature sources to generate a set of 1121 accurate empirical rotation–vibration energies for the first five vibrational states (000), (010), (100), (020), and (001). The comparison to the previous dataset from an IUPAC task group illustrates a gain in the average energy accuracy by more than one order of magnitude. Based on these levels, a recommended list of transitions between the first five vibrational states is proposed for HD16O in the 0–4650 cm−1 frequency range. Full article
(This article belongs to the Special Issue Molecular Spectroscopy and Molecular Structure in Europe)
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<p>Successive zooms of the FTS spectrum #19 of deuterated water recorded at the SOLEIL synchrotron with a pressure of 4 mbar between 50 and 700 cm<sup>−1</sup>.</p>
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<p>Line parameter retrieval from the FTS spectra #19–21 of deuterated water near 356.4 cm<sup>−1</sup>. The line profile fit was performed in narrow spectral intervals around the lines that were not too saturated. <b>Upper panel</b><span class="html-italic">:</span> Recorded spectra at about 10 µbar, 0.3 mbar, and 4 mbar (#21, #20, and #19, respectively) with corresponding best-fit spectra (blue, red, and green, respectively). <b>Lower panel</b><span class="html-italic">:</span> Corresponding (obs. − calc.) residuals in %.</p>
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<p>Overview of the HD<sup>16</sup>O lines retrieved from spectra #19–21 of deuterated water between 50 and 720 cm<sup>−1</sup>. The global experimental line list was obtained by combining the lists at about 10 µbar (#21), 0.3 mbar (#20), and 4 mbar (#19) (green, orange, and yellow dots, respectively). Note that the strongest lines retrieved from the lowest pressure spectrum are measured with strongly underestimated intensities (see text). The gray dots correspond to the SP variational list [<a href="#B8-molecules-29-05508" class="html-bibr">8</a>,<a href="#B9-molecules-29-05508" class="html-bibr">9</a>].</p>
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<p>Overview of the HD<sup>16</sup>O transitions observed by absorption and by emission below 720 cm<sup>−1</sup> [<a href="#B23-molecules-29-05508" class="html-bibr">23</a>]. The line intensities from Schwenke and Partridge [<a href="#B8-molecules-29-05508" class="html-bibr">8</a>,<a href="#B9-molecules-29-05508" class="html-bibr">9</a>] were attached to the transition wavenumbers.</p>
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<p>Differences between the HD<sup>16</sup>O line positions measured from the SOLEIL spectra in the present study and in Ref. [<a href="#B3-molecules-29-05508" class="html-bibr">3</a>] (24MiKaKoCa) (red dots) and differences between the present and HITRAN2020 values [<a href="#B5-molecules-29-05508" class="html-bibr">5</a>] (cyan dots).</p>
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<p>Comparison between the FTS spectrum (black line) of HD<sup>16</sup>O transitions to the spectra simulations (red line) based on the HITRAN2020 database in four spectral intervals showing significant differences.</p>
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<p>Histograms of the uncertainties of the present and IUPAC-TG [<a href="#B25-molecules-29-05508" class="html-bibr">25</a>] energy levels of HD<sup>16</sup>O (red and green, respectively). The blue histogram corresponds to the differences in the energy values obtained in this work (TW) and those recommended by the IUPAC-TG.</p>
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<p>Energy differences, <span class="html-italic">E</span><sup>TW</sup>–<span class="html-italic">E</span><sup>IUPAC</sup>, of the energy levels of the ground, (010), and (001) vibrational states of HD<sup>16</sup>O determined in this work (TW) and recommended by the IUPAC-TG [<a href="#B25-molecules-29-05508" class="html-bibr">25</a>].</p>
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<p>Overview of the HD<sup>16</sup>O line list provided in the HITRAN2020 database (gray dots) [<a href="#B5-molecules-29-05508" class="html-bibr">5</a>] and of the lines with <span class="html-italic">J</span> &gt; 20 predicted by Schwenke and Partridge (red circles) [<a href="#B8-molecules-29-05508" class="html-bibr">8</a>,<a href="#B9-molecules-29-05508" class="html-bibr">9</a>]. The HITRAN list is limited to <span class="html-italic">J</span> ≤ 20 transitions.</p>
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<p>Overview of the HD<sup>16</sup>O recommended line lists based on the variational calculations by Schwenke and Partridge [<a href="#B8-molecules-29-05508" class="html-bibr">8</a>,<a href="#B9-molecules-29-05508" class="html-bibr">9</a>]. Except those corresponding to the black stars, the transition frequencies have been empirically corrected, using either presently determined or IUPAC-TG energy levels (cyan and red symbols, respectively).</p>
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33 pages, 2260 KiB  
Article
A Five-Axis Toolpath Corner-Smoothing Method Based on the Space of Master–Slave Movement
by Song Gao, Haiming Zhang, Jianzhong Yang, Jiejun Xie and Wanqiang Zhu
Machines 2024, 12(12), 834; https://doi.org/10.3390/machines12120834 - 21 Nov 2024
Abstract
The smoothing of linear toolpaths plays is critical in improving machining quality and efficiency in five-axis CNC machining. Existing corner-smoothing methods often overlook the impact of spline curvature fluctuations, which may lead to acceleration variations, hindering surface quality improvements. The paper presents a [...] Read more.
The smoothing of linear toolpaths plays is critical in improving machining quality and efficiency in five-axis CNC machining. Existing corner-smoothing methods often overlook the impact of spline curvature fluctuations, which may lead to acceleration variations, hindering surface quality improvements. The paper presents a five-axis toolpath corner-smoothing method based on the space of master–slave movement (SMM), aiming to minimize curvature fluctuations in five-axis machining and improve surface quality. The concept of movement space in master–slave cooperative motion is introduced, where the tool tip position and tool orientation are decoupled into a main motion trajectory and two master–slave movement space trajectories. By deriving the curvature monotony conditions of a dual Bézier spline, a G2-continuous tool tip corner-smoothing curve with minimal curvature fluctuations is constructed in real-time. Subsequently, using the SMM and the asymmetric dual Bézier spline, a high-order continuous synchronization relationship between the tool tip position and tool orientation is established. Simulation tests and machining experiments show that with our smoothing algorithm, maximum acceleration values for each axis were reduced by 21.05%, while jerk was lowered by 22.31%. These results indicate that trajectory smoothing significantly reduces mechanical vibrations and improves surface quality. Full article
(This article belongs to the Section Advanced Manufacturing)
10 pages, 2220 KiB  
Article
Prediction of Blast Vibration Velocity of Buried Steel Pipe Based on PSO-LSSVM Model
by Hongyu Zhang, Shengwu Tu, Senlin Nie and Weihua Ming
Sensors 2024, 24(23), 7437; https://doi.org/10.3390/s24237437 - 21 Nov 2024
Abstract
In order to ensure the safe operation of adjacent buried pipelines under blast vibration, it is of great practical engineering significance to accurately predict the peak vibration velocity ofburied pipelines under blasting loads. Relying on the test results of the buried steel pipe [...] Read more.
In order to ensure the safe operation of adjacent buried pipelines under blast vibration, it is of great practical engineering significance to accurately predict the peak vibration velocity ofburied pipelines under blasting loads. Relying on the test results of the buried steel pipe blast model test, a sensitivity analysis of relevant influencing factors was carried out by using the gray correlation analysis method. A least squares support vector machine (LS-SVM) model was established to predict the peak vibration velocity of the pipeline and determine the best parameter combination in the LS-SVM model through a local particle swarm optimization (PSO), and the results of the PSO-LSSVM model were predicted. These were compared with BP neural network model and Sa’s empirical formula. The results show that the fitting correlation coefficient (R2), root mean square error (RMSE), average relative error (MRE), and Nash coefficient (NSE) of the PSO-LSSVM model for the prediction of pipeline peak vibration velocity are 91.51%, 2.95%, 8.69%, and 99.03%, showing that the PSO-LSSVM model has a higher prediction accuracy and better generalization ability, which provides a new idea for the vibration velocity prediction of buried pipelines under complex blasting conditions. Full article
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<p>Processing flow of PSO-LSSVM model.</p>
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<p>Model test layout diagram.</p>
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<p>Installation diagram of blast vibration meter.</p>
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<p>Fitness curve of PSO-LSSVM model.</p>
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<p>A comparison between the true value and the predicted value of the training sample of the PSO-LSSVM model.</p>
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<p>Comparison of prediction results of different models.</p>
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14 pages, 8918 KiB  
Article
Molecular Energy of Metamorphic Coal and Methane Adsorption Based on Gaussian Simulation
by Tao Yang, Jingyan Hu, Tao Li, Heng Min and Shuchao Zhang
Processes 2024, 12(12), 2621; https://doi.org/10.3390/pr12122621 - 21 Nov 2024
Abstract
Effectively controlling the adsorption and desorption of coal and mine gas is crucial to preventing harm to the environment. Therefore, this paper investigated the adsorption of coal and methane molecules from the perspective of microscopic energy through Gaussian simulation. Gaussian 09W and GaussView [...] Read more.
Effectively controlling the adsorption and desorption of coal and mine gas is crucial to preventing harm to the environment. Therefore, this paper investigated the adsorption of coal and methane molecules from the perspective of microscopic energy through Gaussian simulation. Gaussian 09W and GaussView 5.0 software were used to construct and optimize the molecular model of four different metamorphic coals, namely lignite, sub-bituminous coal, bituminous coal, and anthracite, and their adsorption structure with methane as well as the energy, bond length, vibration frequency, infrared spectrum, and other data on the optimal structure were obtained. The binding energy of coal molecules and methane from large to small was as follows: sub-bituminous coal (7.3696 KJ/mol), lignite (6.6149 KJ/mol), bituminous coal (5.2170 KJ/mol), and anthracite (4.9510 KJ/mol). The equilibrium distance was negatively correlated with the binding energy, and the molecular structure and position of coal largely determined the binding energy. Additionally, adsorption was more likely to occur between methane molecules and hydroxyl groups. Many new vibration modes were observed during the adsorption of coal and methane molecules. This paper is of practical significance, as studying the adsorption of coal and mine gas can prevent and control mine gas outbursts and ensure safe production. Full article
(This article belongs to the Topic Energy Extraction and Processing Science)
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<p>Gaussian simulation operation interface. (<b>a</b>) Energy change trend. (<b>b</b>) Vibration frequency.</p>
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<p>Molecular structure diagram of different metamorphic coals: (<b>a</b>) lignite (<b>b</b>) sub-bituminous coal, (<b>c</b>) bituminous coal, (<b>d</b>) anthracite.</p>
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<p>Optimal structure model of different metamorphic coal molecules: (<b>a</b>) lignite (<b>b</b>) sub-bituminous coal, (<b>c</b>) bituminous coal, (<b>d</b>) anthracite.</p>
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<p>Molecular energy values of different metamorphic coals.</p>
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<p>Infrared spectra of different metamorphic coal molecules. (<b>a</b>) Lignite. (<b>b</b>) Sub-bituminous coal. (<b>c</b>) Bituminous coal. (<b>d</b>) Anthracite.</p>
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<p>Infrared spectra of different metamorphic coal molecules. (<b>a</b>) Lignite. (<b>b</b>) Sub-bituminous coal. (<b>c</b>) Bituminous coal. (<b>d</b>) Anthracite.</p>
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<p>Binding energy of different adsorption positions of lignite.</p>
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<p>Binding energy of different adsorption positions of sub-bituminous coal.</p>
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<p>Binding energy of different adsorption positions of bituminous coal.</p>
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<p>Binding energy of different adsorption positions of anthracite.</p>
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<p>Optimal structure model of methane molecules adsorbed by different metamorphic coal molecules. (<b>a</b>) lignite, (<b>b</b>) sub-bituminous coal, (<b>c</b>) bituminous coal, (<b>d</b>) anthracite.</p>
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<p>Adsorption equilibrium distance of different metamorphic coal molecules.</p>
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<p>Binding energy of different metamorphic coal molecules after adsorption.</p>
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<p>Infrared spectra of the optimal configuration of methane adsorbed by different metamorphic coal molecules. (<b>a</b>) Lignite. (<b>b</b>) Sub-bituminous coal. (<b>c</b>) Bituminous coal. (<b>d</b>) Anthracite.</p>
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13 pages, 5425 KiB  
Article
Highly Sensitive SnS2/rGO-Based Gas Sensor for Detecting Chemical Warfare Agents at Room Temperature: A Theoretical Study Based on First-Principles Calculations
by Ting Liang, Huaizhang Wang, Huaning Jiang, Yelin Qi, Rui Yan, Jiangcun Li and Yanlei Shangguan
Crystals 2024, 14(12), 1008; https://doi.org/10.3390/cryst14121008 - 21 Nov 2024
Abstract
Chemical warfare agents (CWAs) are known as poor man’s bombs because of their small lethal dose, cheapness, and ease of production. Therefore, the highly sensitive and rapid detection of CWAs at room temperature (RT = 25 °C) is essential. In this paper, we [...] Read more.
Chemical warfare agents (CWAs) are known as poor man’s bombs because of their small lethal dose, cheapness, and ease of production. Therefore, the highly sensitive and rapid detection of CWAs at room temperature (RT = 25 °C) is essential. In this paper, we have developed a resistive semiconductor sensor for the highly sensitive detection of CWAs at RT. The gas-sensing material is SnS2/rGO nanosheets (NSs) prepared by hydrothermal synthesis. The lower detection limits of the SnS2/rGO NSs-based gas sensor were 0.05 mg/m3 and 0.1 mg/m3 for the typical chemical weapons sarin (GB) and sulfur mustard (HD), respectively. The responsivity can reach −3.54% and −10.2% in 95 s for 1.0 mg/m3 GB, and in 47 s for 1.0 mg/m3 HD. They are 1.17 and 2.71 times higher than the previously reported Nb-MoS2 NSs-based gas sensors, respectively. In addition, it has better repeatability (RSD = 6.77%) and stability for up to 10 weeks (RSD = 20.99%). Furthermore, to simplify the work of later researchers based on the detection of CWAs by two-dimensional transition metal sulfur compounds (2D-TMDCs), we carried out calculations of the SnS2 NSs-based and SnS2/rGO NSs-based gas sensor-adsorbing CWAs. Detailed comparisons are made in conjunction with experimental results. For different materials, it was found that the SnS2/rGO NSs-based gas sensor performed better in all aspects of adsorbing CWAs in the experimental results. Adsorbed CWAs at a distance smaller than that of the SnS2 NSs-based gas sensor in the theoretical calculations, as well as its adsorption energy and transferred charge, were larger than those of the SnS2 NSs-based gas sensor. For different CWAs, the experimental results show that the sensitivity of the SnS2/rGO NSs-based gas sensor for the adsorption of GB is higher than that of HD, and accordingly, the theoretical calculations show that the adsorption distance of the SnS2/rGO NSs-based gas sensor for the adsorption of GB is smaller than that of HD, and the adsorption energy and the amount of transferred charge are larger than that of HD. This regularity conclusion proves the feasibility of adsorption of CWAs by gas sensors based on SnS2 NSs, as well as the feasibility and reliability of theoretical prediction experiments. This work lays a good theoretical foundation for subsequent rapid screenings of gas sensors with gas-sensitive materials for detecting CWAs. Full article
(This article belongs to the Special Issue Organic Photonics: Organic Optical Functional Materials and Devices)
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<p>(<b>a</b>) Sensor electrode physical picture; (<b>b</b>) SEM images of the SnS<sub>2</sub>/rGO NSs; (<b>c</b>) TEM images of the SnS<sub>2</sub>/rGO NSs; (<b>d</b>) the high-resolution TEM image.</p>
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<p>SnS<sub>2</sub>/rGO (<b>a</b>) XRD characterization; (<b>b</b>) Raman spectra; (<b>c</b>) EDS elemental mapping.</p>
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<p>The response–recovery curve of the SnS<sub>2</sub> and SnS<sub>2</sub>/rGO NSs-based gas sensor was exposed to various concentrations of (<b>a</b>) GB and (<b>b</b>) HD vapor ranging from 0.05 to 1.5 mg/m<sup>3</sup>. (<b>c</b>) Three successive sensing cycles of the SnS<sub>2</sub> NSs-based and SnS<sub>2</sub>/rGO NSs-based gas sensors were continuously exposed to 0.1 mg/m<sup>3</sup> GB. (<b>d</b>) Long-term stability of the SnS<sub>2</sub>/rGO NSs-based gas sensor was exposed to 0.5 mg/m<sup>3</sup> GB for ten weeks.</p>
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<p>Sensing schematic diagram of SnS<sub>2</sub>/rGO NSs (<b>a</b>) in air and (<b>b</b>) adsorption GB.</p>
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<p>Structural modeling of (<b>a</b>) SnS<sub>2</sub>; (<b>b</b>) SnS<sub>2</sub>/rGO; (<b>c</b>) GB; and (<b>d</b>) HD. Optimal adsorption sites of GB on (<b>e</b>) SnS<sub>2</sub> and (<b>f</b>) SnS<sub>2</sub>/rGO surfaces. Optimal adsorption sites of HD on (<b>g</b>) SnS<sub>2</sub> and (<b>h</b>) SnS<sub>2</sub>/rGO surfaces.</p>
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<p>Differential charge-density plots of SnS<sub>2</sub> adsorption on (<b>a</b>) GB and (<b>b</b>) HD; differential charge-density plots of SnS<sub>2</sub>/GO adsorption on (<b>c</b>) GB and (<b>d</b>) HD. (The isosurfaces take the value of 0.02 eV/Å. Green is the region of concentration of electrons. Light blue is the region of dissipation of electrons).</p>
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<p>(<b>a</b>) Energy band structure and (<b>b</b>) density-of-state plots for SnS<sub>2</sub>. (<b>c</b>) Energy band structure and (<b>d</b>) density-of-state plots for SnS<sub>2</sub>/rGO. (<b>e</b>) Energy band structure and (<b>f</b>) density-of-state plots of SnS<sub>2</sub>/rGO NSs-adsorbed GB. (<b>g</b>) Energy band structure and (<b>h</b>) density-of-state plots of SnS<sub>2</sub>/rGO NSs-adsorbed HD.</p>
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12 pages, 1164 KiB  
Article
The Effects of a 12-Week Training Multicomponent Exercise Program on Landing Mechanics in Recreational Athletes
by Adrián Feria-Madueño, Timothy Hewett, Thomas Dos’Santos and Borja Sañudo
Healthcare 2024, 12(23), 2327; https://doi.org/10.3390/healthcare12232327 - 21 Nov 2024
Viewed by 3
Abstract
Background/Objectives: This study investigated the impacts of a 12-week training program on kinetic parameters during landings in non-professional recreational athletes. Methods: Fifty-seven non-elite recreational athletes performed three unilateral-landing trials from a 30 cm high structure on a force platform. The following outcome measures [...] Read more.
Background/Objectives: This study investigated the impacts of a 12-week training program on kinetic parameters during landings in non-professional recreational athletes. Methods: Fifty-seven non-elite recreational athletes performed three unilateral-landing trials from a 30 cm high structure on a force platform. The following outcome measures were analyzed: the ground reaction forces at initial ground contact (PF1) and the highest value (PF2), impulse (change in the moment of force during landing), stabilization time, and ankle and knee accelerations. The ground reaction forces, momentum, and accelerations were evaluated in the vertical, medio-lateral, and anteroposterior axes. Participants were randomly assigned to two groups. The experimental group (EG) underwent a 12-week intervention, three times per week, consisting of various exercises, such as strength, eccentric, proprioceptive, whole-body vibration (WBV), and neuromuscular exercises. After 12 weeks, the same outcome measures were analyzed. Results: The effects of the training program on vertical ground reaction forces were not clear (0.3% and 0.9%, respectively). Medio-lateral (64.8%, d = 0.51) and anteroposterior (43.9%, d = 1.34) forces were probably reduced due to the training program. The stabilization time was also reduced in the experimental group (44.2%). The training program most likely decreased the vertical impulse (47.3%, d = −1.56), whereas the total ankle acceleration increased (18.4%, d = 0.79). Conclusions: The findings reveal significant improvements in neuromuscular control and stability during landings, specifically demonstrating reduced medio-lateral forces, vertical momentum, and acceleration during monopodal landings. This study focuses on the importance of proper landing techniques in minimizing the risk of knee injuries, emphasizing the falling strategy’s role in injury prevention. Full article
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<p>Participant with hands on hips preparing to perform a single leg landing as part of the experimental protocol.</p>
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<p>Comparative effects of the training program in both groups in relation to kinetic variables during landings. PF1 (N/Kg) = ground reaction force at first contact with the ground. PF2 (N/Kg) = peak maximum vertical force during landing. ML− force (N/Kg) = force in the medio-lateral axis exerted in varus. ML+ force (N/Kg) = force in the medio-lateral axis exerted in valgus. Force<sub>AP−</sub> (N/Kg) = force in the anterior–posterior axis exerted backward. Force<sub>AP+</sub> (N/Kg) = force in the anterior–posterior axis exerted forward. TdEst (s) = stabilization time after landing. Bars indicate changes in means with a 90% confidence interval.</p>
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<p>Comparative effects of the training program in both groups in relation to the kinetic variables of acceleration during landings. ACC<sub>ANKLE</sub>TOTAL (g) = total localized acceleration at the ankle during ground contact. ACC<sub>ANKLE</sub>ML (g) = partial acceleration of the ankle in medio-lateral axis when GRF is maximum. ACC<sub>ANKLE</sub>AP (g) = partial acceleration of the ankle in anterior–posterior axis when GRF is maximum. ACC<sub>ANKLE</sub>Z (g) = partial acceleration of the ankle in vertical axis when GRF is maximum. ACC<sub>KNEE</sub>ML (g) = partial acceleration of the knee in medio-lateral axis when GRF is maximum. ACC<sub>ANKLE</sub>AP (g) = partial acceleration of the knee in anterior–posterior axis when GRF is maximum. ACC<sub>ANKLE</sub>Z (g) = partial acceleration of the knee in vertical axis when GRF is maximum.</p>
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19 pages, 6827 KiB  
Article
Intelligent Identification and Prediction of Roof Deterioration Areas Based on Measurements While Drilling
by Jing Wu, Zhi-Qiang Zhao, Xiao-He Wang, Yi-Qing Wang, Xiao-Xiang Wei and Zhi-Qiang You
Sensors 2024, 24(23), 7421; https://doi.org/10.3390/s24237421 - 21 Nov 2024
Viewed by 15
Abstract
During roadway excavation, the presence of roof deterioration zones, such as layered spaces and weak interlayers, significantly affects the stability of the surrounding rock. To achieve timely and effective support for roadways, it is essential to utilize drilling measurement signals obtained during the [...] Read more.
During roadway excavation, the presence of roof deterioration zones, such as layered spaces and weak interlayers, significantly affects the stability of the surrounding rock. To achieve timely and effective support for roadways, it is essential to utilize drilling measurement signals obtained during the construction of anchorage holes for the identification and prediction of these deterioration zones. This study systematically investigates the response characteristics of thrust, torque, and Y-direction vibration signals to different combinations of rock layers through theoretical analysis, laboratory experiments, ABAQUS dynamic numerical simulations, and field measurements. The results indicate that these drilling parameters effectively characterize variations in rock structure and strength, with distinct signal features observed particularly in roof deterioration zones. Based on these findings, this paper proposes a deep learning algorithm that employs Long Short-Term Memory (LSTM) recurrent neural networks for classification prediction, along with a random forest algorithm for regression prediction, aimed at the intelligent identification and prediction of roof deterioration zones. The algorithm demonstrates outstanding performance in both laboratory experiments and field tests, achieving a 100% recognition rate for layered spaces and a 96.6% accuracy for identifying deterioration zones, with high accuracy at lower values of mechanical specific energy (MSE). The proposed method provides significant insights for real-time monitoring and control of roof deterioration zones, enhancing the safety and stability of roadway excavations, and serves as a valuable reference for future research and practical applications. Full article
(This article belongs to the Section Intelligent Sensors)
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<p>Mechanical model for calculating cutting force of PDC drill bits.</p>
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<p>Drilling experiment equipment diagram.</p>
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<p>Drilling signal diagram. (<b>a</b>) Combinations of rock layer and separation; (<b>b</b>) combinations of concrete.</p>
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<p>Drilling signal complementary ensemble empirical mode decomposition diagram. (<b>a</b>) Separation layer (torque); (<b>b</b>) separation layer (thrust); (<b>c</b>) separation layer (vibration); (<b>d</b>) rock strata (torque); (<b>e</b>) rock strata (thrust); (<b>f</b>) rock strata (vibration).</p>
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<p>Drilling signal violin diagram. (<b>a</b>) Torque signal; (<b>b</b>) thrust signal; (<b>c</b>) vibration signal.</p>
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<p>Correlation index analysis diagram.</p>
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<p>Numerical simulation model diagram.</p>
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<p>Mises stress distribution of different rock strata combinations in drilling process.</p>
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<p>Drilling signal curve diagram. (<b>a</b>) Separation layer (torque); (<b>b</b>) separation layer (thrust); (<b>c</b>) tock strata (torque); (<b>d</b>) rock strata (thrust).</p>
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<p>Simulated drilling signal violin diagram. (<b>a</b>) Torque signal; (<b>b</b>) thrust signal.</p>
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<p>LSTM prediction results diagram.</p>
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<p>Confusion matrix diagram.</p>
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<p>Rock stratum histogram.</p>
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<p>Field test diagram.</p>
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<p>Field drilling signal diagram.</p>
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<p>The comparison diagram between true value and predicted value of MSE.</p>
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15 pages, 3119 KiB  
Article
Fault Detection in Harmonic Drive Using Multi-Sensor Data Fusion and Gravitational Search Algorithm
by Nan-Kai Hsieh and Tsung-Yu Yu
Machines 2024, 12(12), 831; https://doi.org/10.3390/machines12120831 - 21 Nov 2024
Viewed by 8
Abstract
This study proposes a fault diagnosis method for harmonic drive systems based on multi-sensor data fusion and the gravitational search algorithm (GSA). As a critical component in robotic arms, harmonic drives are prone to failures due to wear, less grease, or improper loading, [...] Read more.
This study proposes a fault diagnosis method for harmonic drive systems based on multi-sensor data fusion and the gravitational search algorithm (GSA). As a critical component in robotic arms, harmonic drives are prone to failures due to wear, less grease, or improper loading, which can compromise system stability and production efficiency. To enhance diagnostic accuracy, the research employs wavelet packet decomposition (WPD) and empirical mode decomposition (EMD) to extract multi-scale features from vibration signals. These features are subsequently fused, and GSA is used to optimize the high-dimensional fused features, eliminating redundant data and mitigating overfitting. The optimized features are then input into a support vector machine (SVM) for fault classification, with K-fold cross-validation used to assess the model’s generalization capabilities. Experimental results demonstrate that the proposed diagnosis method, which integrates multi-sensor data fusion with GSA optimization, significantly improves fault diagnosis accuracy compared to methods using single-sensor signals or unoptimized features. This improvement is particularly notable in multi-class fault scenarios. Additionally, GSA’s global search capability effectively addresses overfitting issues caused by high-dimensional data, resulting in a diagnostic model with greater reliability and accuracy across various fault conditions. Full article
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<p>Enhanced harmonic drive fault diagnosis framework diagram.</p>
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<p>Three-layered wavelet packet decomposition process diagram.</p>
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<p>(<b>a</b>) Experimental setup; (<b>b</b>) schematic of the sixth axis; (<b>c</b>) gear wear; (<b>d</b>) bearing damage; (<b>e</b>) improper load; (<b>f</b>) gear fracture.</p>
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<p>K-fold cross-validation diagram.</p>
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<p>Accuracy comparison chart for different optimization methods. (<b>a</b>) FWPD, (<b>b</b>) FWPD+GSA, (<b>c</b>) FEMD, (<b>d</b>) FEMD+GSA.</p>
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<p>Accuracy comparison chart.</p>
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<p>Computation time comparison of different methods.</p>
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21 pages, 10351 KiB  
Article
TSViT: A Time Series Vision Transformer for Fault Diagnosis of Rotating Machinery
by Shouhua Zhang, Jiehan Zhou, Xue Ma, Susanna Pirttikangas and Chunsheng Yang
Appl. Sci. 2024, 14(23), 10781; https://doi.org/10.3390/app142310781 - 21 Nov 2024
Viewed by 65
Abstract
Efficient and accurate fault diagnosis of rotating machinery is extremely important. Fault diagnosis methods using vibration signals based on convolutional neural networks (CNNs) have become increasingly mature. They often struggle with capturing the temporal dynamics of vibration signals. To overcome this, the application [...] Read more.
Efficient and accurate fault diagnosis of rotating machinery is extremely important. Fault diagnosis methods using vibration signals based on convolutional neural networks (CNNs) have become increasingly mature. They often struggle with capturing the temporal dynamics of vibration signals. To overcome this, the application of Transformer-based Vision Transformer (ViT) methods to fault diagnosis is gaining attraction. Nonetheless, these methods typically require extensive preprocessing, which increases computational complexity, potentially reducing the efficiency of the diagnosis process. Addressing this gap, this paper presents the Time Series Vision Transformer (TSViT), tailored for effective fault diagnosis. The TSViT incorporates a convolutional layer to extract local features from vibration signals alongside a transformer encoder to discern long-term temporal patterns. A thorough experimental comparison of three diverse datasets demonstrates the TSViT’s effectiveness and adaptability. Moreover, the paper delves into the influence of hyperparameter tuning on the model’s performance, computational demand, and parameter count. Remarkably, the TSViT achieves an unprecedented 100% average accuracy on two of the test sets and 99.99% on the other, showcasing its exceptional fault diagnosis capabilities for rotating machinery. The implementation of this model will bring significant economic benefits. Full article
(This article belongs to the Special Issue Signal Acquisition and Processing for Measurement and Testing)
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<p>The architecture of the TSViT.</p>
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<p>The experimental bench of each dataset (<b>a</b>) PBR dataset (<b>b</b>) CWRU dataset (<b>c</b>) XJTU dataset.</p>
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<p>Time domain waveforms of vibration signal samples in the PBR dataset (<b>a</b>) NC (<b>b</b>) PL (<b>c</b>) BBF (<b>d</b>) RU.</p>
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<p>Time domain waveforms of vibration signal samples in the CWRU dataset (<b>a</b>) NC (<b>b</b>) F1 (<b>c</b>) F2 (<b>d</b>) F3 (<b>e</b>) F4 (<b>f</b>) F5 (<b>g</b>) F6 (<b>h</b>) F7 (<b>i</b>) F8 (<b>j</b>) F9.</p>
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<p>Time domain waveforms of vibration signal samples in the CWRU dataset (<b>a</b>) NC (<b>b</b>) F1 (<b>c</b>) F2 (<b>d</b>) F3 (<b>e</b>) F4 (<b>f</b>) F5 (<b>g</b>) F6 (<b>h</b>) F7 (<b>i</b>) F8 (<b>j</b>) F9.</p>
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<p>Time domain waveforms of vibration signal samples in the XJTU dataset (<b>a</b>) Cage (<b>b</b>) Inner race (<b>c</b>) Outer race (<b>d</b>) Composite.</p>
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<p>The training flow of the TSViT.</p>
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<p>The trend of loss changes on the PBR dataset (<b>a</b>) downward trend on the training dataset (<b>b</b>) downward trend on the test dataset (<b>c</b>) downward trend in average loss over 10 trials.</p>
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<p>The trend of accuracy changes in the PBR dataset (<b>a</b>) upward trend on the training dataset (<b>b</b>) upward trend on the test dataset (<b>c</b>) upward trend in average accuracy over 10 trials.</p>
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<p>The trend of loss changes in the CWRU dataset (<b>a</b>) downward trend on the training dataset (<b>b</b>) downward trend on the test dataset (<b>c</b>) downward trend in average loss over 10 trials.</p>
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<p>The trend of accuracy changes in the CWRU dataset (<b>a</b>) upward trend on the training dataset (<b>b</b>) upward trend on the test dataset (<b>c</b>) upward trend in average accuracy over 10 trials.</p>
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<p>The trend of loss changes on XJTU dataset (<b>a</b>) downward trend on the training dataset (<b>b</b>) downward trend on the test dataset (<b>c</b>) downward trend in average loss over 10 trials.</p>
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<p>The trend of accuracy changes on XJTU dataset (<b>a</b>) upward trend on the training dataset (<b>b</b>) upward trend on the test dataset (<b>c</b>) upward trend in average accuracy over 10 trials.</p>
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<p>Confusion matrix of the minimum optimal model of the CWRU test set.</p>
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<p>Accuracies on three noise-added test sets.</p>
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<p>Comparison of the influence of different hyperparameters on accuracy based on three datasets (<b>a</b>) patch size (<b>b</b>) dimension of time series patch embeddings (<b>c</b>) number of heads in MSA (<b>d</b>) number of blocks (<b>e</b>) dimension of linear transformation in MLP.</p>
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<p>Comparison of the influence of different hyperparameters on accuracy based on three datasets (<b>a</b>) patch size (<b>b</b>) dimension of time series patch embeddings (<b>c</b>) number of heads in MSA (<b>d</b>) number of blocks (<b>e</b>) dimension of linear transformation in MLP.</p>
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<p>Feature visualization in different TSViT layers through t-SNE on the PBR test set (<b>a</b>) raw signals (<b>b</b>) cnn (<b>c</b>) the first block (<b>d</b>) the second block (<b>e</b>) the third block (<b>f</b>) the fourth block (<b>g</b>) the fifth block (<b>h</b>) the sixth block (<b>i</b>) the seventh block (<b>j</b>) the eighth block (<b>k</b>) classification layer.</p>
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<p>Feature visualization in different TSViT layers through t-SNE on the CWRU test set (<b>a</b>) raw signals (<b>b</b>) cnn (<b>c</b>) the first block (<b>d</b>) the second block (<b>e</b>) the third block (<b>f</b>) the fourth block (<b>g</b>) the fifth block (<b>h</b>) the sixth block (<b>i</b>) the seventh block (<b>j</b>) the eighth block (<b>k</b>) classification layer.</p>
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<p>Feature visualization in different TSViT layers through t-SNE on the XJTU test set (<b>a</b>) raw signals (<b>b</b>) cnn (<b>c</b>) the first block (<b>d</b>) the second block (<b>e</b>) the third block (<b>f</b>) the fourth block (<b>g</b>) the fifth block (<b>h</b>) the sixth block (<b>i</b>) the seventh block (<b>j</b>) the eighth block (<b>k</b>) classification layer.</p>
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16 pages, 2949 KiB  
Article
Development of a Conceptual Scheme for Controlling Tool Wear During Cutting, Based on the Interaction of Virtual Models of a Digital Twin and a Vibration Monitoring System
by Lapshin Viktor, Turkin Ilya, Gvindzhiliya Valeriya, Dudinov Ilya and Gamaleev Denis
Sensors 2024, 24(22), 7403; https://doi.org/10.3390/s24227403 - 20 Nov 2024
Viewed by 209
Abstract
This article discusses the issue of the joint use of neural network algorithms for data processing and deterministic mathematical models. The use of a new approach is proposed, to determine the discrepancy between data from a vibration monitoring system of the cutting process [...] Read more.
This article discusses the issue of the joint use of neural network algorithms for data processing and deterministic mathematical models. The use of a new approach is proposed, to determine the discrepancy between data from a vibration monitoring system of the cutting process and the calculated data obtained by modeling mathematical models of the digital twin system of the cutting process. This approach is justified by the fact that some coordinates for the state of the cutting process cannot be measured, and the vibration signals measured by the vibration monitoring system (the vibration acceleration of the tip of the cutting tool) are subject to external disturbing influences. Both the experimental method and the Matlab 2022b simulation method were used as research methods. The experimental research method is based on the widespread use of modern analog vibration transducers, the signals from which undergo the process of digitalization and further processing in order to identify arrays of additional information required for virtual digital twin models. The results obtained allow us to formulate a new conceptual approach to the construction of systems for determining the degree of cutting tool wear, based on the joint use of computational virtual models of the digital twin system and data obtained from the vibration monitoring system of the cutting process. Full article
(This article belongs to the Section Physical Sensors)
9 pages, 230 KiB  
Article
Optimal Control of the Inverse Problem of the Burgers Equation for Representing the State of Sonic Vibration Velocity in Water
by Jiale Qin, Yiping Meng and Shichao Yi
Mathematics 2024, 12(22), 3625; https://doi.org/10.3390/math12223625 - 20 Nov 2024
Viewed by 240
Abstract
In this paper, we investigate the inverse of the set of unknown functions (v,g) of the Burgers equation in the framework of optimal theory. Firstly, we prove the existence of functional minimizers in the optimal control problem and derive [...] Read more.
In this paper, we investigate the inverse of the set of unknown functions (v,g) of the Burgers equation in the framework of optimal theory. Firstly, we prove the existence of functional minimizers in the optimal control problem and derive the necessary conditions for the optimal solution. Subsequently, the global uniqueness of the optimal solution and its stability are explored. After completing the ill-posed analysis of the Burgers equation, we can apply it to the problem of sonic vibration velocity in water. The desired result is obtained by inverse-performing an unknown initial state with known terminal vibration velocity. This is important for solving practical problems. Full article
(This article belongs to the Section Engineering Mathematics)
18 pages, 6536 KiB  
Article
Strong Interference Elimination in Seismic Data Using Multivariate Variational Mode Extraction
by Zhichao Yu, Yuyang Tan and Yiran Lv
Sensors 2024, 24(22), 7399; https://doi.org/10.3390/s24227399 - 20 Nov 2024
Viewed by 219
Abstract
Seismic data acquired in the presence of mechanical vibrations or power facilities may be contaminated by strong interferences, significantly decreasing the data signal-to-noise ratio (S/N). Conventional methods, such as the notch filter and time-frequency transform method, are usually inadequate for suppressing non-stationary interference [...] Read more.
Seismic data acquired in the presence of mechanical vibrations or power facilities may be contaminated by strong interferences, significantly decreasing the data signal-to-noise ratio (S/N). Conventional methods, such as the notch filter and time-frequency transform method, are usually inadequate for suppressing non-stationary interference noises, and may distort effective signals if overprocessing. In this study, we propose a method for eliminating mechanical vibration interferences in seismic data. In our method, we extended the variational mode extraction (VME) technique to a multivariate form, called multivariate variational mode extraction (MVME), for synchronous analysis of multitrace seismic data. The interference frequencies are determined via synchrosqueezing-based time-frequency analysis of process recordings; their corresponding modes are extracted and removed from seismic data using MVME with optimal balancing factors. We used synthetic data to investigate the effectiveness of the method and the influence of tuning parameters on processing results, and then applied the method to field datasets. The results have demonstrated that, compared with the conventional methods, the proposed method could effectively suppress the mechanical vibration interferences, improve the S/Ns and enhance polarization analysis of seismic signals. Full article
(This article belongs to the Special Issue Sensor Technologies for Seismic Monitoring)
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<p>Flowchart of the proposed method.</p>
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<p>Waveforms of (<b>a</b>) the 3-C seismic signal, (<b>b</b>) the 3-C interference noise, and (<b>c</b>) the synthetic data. (<b>d</b>) The time-frequency analysis result of the 1st component data. The red lines in (<b>c</b>) indicate the seismic arrival.</p>
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<p>The S/Ns of the residual signal after removing interference using MVME with a series of penalty parameters. Selection of optimal parameters according to the maximum value of S/N.</p>
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<p>Comparison of the processing results using MVME with different penalty parameters α. (<b>a</b>,<b>c</b>,<b>e</b>) These show the extracted interference noise using α = 2000, 124,000, 200,000, respectively. (<b>b</b>,<b>d</b>,<b>f</b>) These show the de-noised signals using α = 2000, 124,000, 200,000, respectively. The black and red lines are the real signals in the synthetic data and the processing results, respectively.</p>
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<p>Comparison of the S/Ns (<b>a</b>) and the final center frequencies (<b>b</b>) using MVME with different initial center frequencies.</p>
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<p>The processing results using the VME method with the optimal penalty parameter α = 124,000. (<b>a</b>) The extracted interference noise. (<b>b</b>) The de-noised signals. The black and red lines are the real signals in the synthetic data and the processing results via the VME method, respectively.</p>
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<p>The processing results using the notch filter and the SST method. (<b>a</b>,<b>b</b>) The removed interferences via notch filter and SST method, respectively. (<b>c</b>,<b>d</b>) The de-noised signals via notch filter and SST method, respectively. The black and red lines are the real signals in the synthetic data and the processing results, respectively.</p>
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<p>Comparison of the processing results of notch filter (grey dots), SST method (blue dots), and the proposed method (red dots). (<b>a</b>) S/Ns; (<b>b</b>) RMS; (<b>c</b>) rectilinearity; (<b>d</b>) azimuth angle; and (<b>e</b>) inclination angle.</p>
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<p>The planar view of the active seismic survey geometry. Black dots, blue triangles, and red circles represent the location of active seismic shots, 3-C receivers, and wellheads, respectively. The red lines indicate the horizontal well trajectories.</p>
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<p>The 3-C seismic data from a SAGD seismic monitoring project. (<b>a</b>) The 3-C waveforms of an active shot. (<b>b</b>) The time-frequency analysis result of 1-N component data. The red lines in (<b>a</b>) indicate the manually picked direct P-wave arrival times.</p>
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<p>The processed results using the proposed method. (<b>a</b>,<b>b</b>) The de-noised signals and the removed interferences, respectively. The amplitude ranges of waveforms are the same. The red lines in (<b>a</b>) indicate the manually picked direct P-wave arrival times.</p>
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<p>The processing results using the notch filter and SST method. (<b>a</b>,<b>b</b>) The de-noised signals and the removed interferences via notch filter, respectively. (<b>c</b>,<b>d</b>) The de-noised signals and the removed interferences via the SST method, respectively. The red lines in (<b>a</b>,<b>c</b>) indicate the manually picked direct P-wave arrival times.</p>
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<p>The 3D view of the survey geometry. The wellhead of the monitoring well was near to that of the treatment.</p>
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<p>The 3-C microseismic data from a hydraulic fracturing downhole monitoring. (<b>a</b>) The 3-C waveforms of a microseismic event. (<b>b</b>) The time-frequency analysis of N-component data. The red and blue lines in (<b>a</b>) represent the manually picked P-wave and S-wave arrival times, respectively.</p>
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<p>The processing results using different methods. (<b>a</b>,<b>b</b>) The de-noised signals and the removed interferences via the proposed methods, respectively. (<b>c</b>,<b>d</b>) The de-noised signals and the removed interferences via notch filter, respectively. (<b>e</b>,<b>f</b>) The de-noised signals and the removed interferences via the SST method, respectively. The red and blue lines in (<b>a</b>,<b>c</b>,<b>e</b>) represent the manually picked P-wave and S-wave arrival times, respectively.</p>
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22 pages, 4687 KiB  
Article
Study on the Thermodynamic–Kinetic Coupling Characteristics of Free-Piston Stirling Air Conditioning
by Yajuan Wang, Kang Zhao and Jun’an Zhang
Energies 2024, 17(22), 5795; https://doi.org/10.3390/en17225795 - 20 Nov 2024
Viewed by 193
Abstract
Unlike traditional free-piston Stirling heat engines or heat pumps, the free piston Stirling air conditioning (FPSAC) is specifically designed for electric vehicle air conditioning under ambient room temperature conditions. In the FPSAC system, the displacer and the power piston are coupled through gas [...] Read more.
Unlike traditional free-piston Stirling heat engines or heat pumps, the free piston Stirling air conditioning (FPSAC) is specifically designed for electric vehicle air conditioning under ambient room temperature conditions. In the FPSAC system, the displacer and the power piston are coupled through gas forces, emphasizing the importance of investing the thermodynamic–kinetic coupling characteristics. This study analyzed the damping terms within the dynamic equations of the FPSAC model and solved these equations to reveal system dynamics. By linearizing the working chamber’s pressure, the study examined the machine’s dynamic behavior, presenting solutions for amplitude and phase angle. Derived expressions for the displacement and acceleration of both the power piston and the displacer further support this analysis. The research evaluates the influence of driving force on amplitude and phase angle, alongside the impact of damping coefficients, thereby isolating thermodynamic–dynamic coupling characteristics. Control equations integrating dynamics and thermodynamics were developed, and a comprehensive system model was constructed using MATLAB(2020a)/Simulink to simulate acceleration and displacement variation in the pistons. Key findings include: (1) a positive correlation between driving force and displacer, where increased force leads to higher amplitudes; (2) a frequency of 65 Hz reveals a singularity occurs in displacer amplitude, resulting in system instability; (3) phase angle between pistons reduces to below 10° when the driving force exceeds 150 N; and (4) the power piston’s amplitude decreases with an increase in damping C1, while changes in damping C2 primarily affect the displacer’s singularity position around 65 Hz, with higher C2 values shifting the singularity to lower frequencies. Full article
(This article belongs to the Section J: Thermal Management)
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<p>Structure diagram of FPSAC.</p>
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<p>Simplified dynamics model. (<b>a</b>) Vibration system physical model. (<b>b</b>) Mechanical model of FPSAC.</p>
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<p>Force diagram for the power piston and displacer. (<b>a</b>) Power piston. (<b>b</b>) Displacer.</p>
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<p>The relationship of amplitude and frequency between the power piston and displacer. (<b>a</b>) F<sub>E</sub> = 50. (<b>b</b>) Different F<sub>E</sub>.</p>
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<p>The relationship of the phase angle and frequency between the power piston and displacer. (<b>a</b>) F<sub>E</sub> = 50. (<b>b</b>) Different F<sub>E</sub>.</p>
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<p>Changes in the amplitude of the power piston and the displacer (<span class="html-italic">C</span><sub>2</sub> = 1.5). (<b>a</b>) When C<sub>1</sub> = 6~16, changes in the amplitude of the power piston (C<sub>2</sub> = 1.5). (<b>b</b>) When C<sub>1</sub> = 6~16, changes in the amplitude of the displacer (C<sub>2</sub> = 1.5). (<b>c</b>) When C<sub>1</sub> = 6~16, changes in the amplitude of the power piston and the displacer.</p>
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<p>When <span class="html-italic">C</span><sub>1</sub> remains and <span class="html-italic">C</span><sub>2</sub> = 0~3, changes in the amplitude of the power piston and the displacer (<span class="html-italic">C</span><sub>1</sub> = 10). (<b>a</b>) Overall view. (<b>b</b>) A<sub>2</sub>.</p>
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<p>Flowchart.</p>
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<p>Matlab/Simulink model of FPSAC.</p>
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<p>The working chamber pressure diagram. (<b>a</b>) The pressure chart of the working chamber from startup to stabilization. (<b>b</b>) The working chamber pressure diagram of stabilization.</p>
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<p>Acceleration diagram of power piston and displacer. (<b>a</b>) Acceleration diagram from startup to stable operation. (<b>b</b>) Acceleration diagram of steady state.</p>
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<p>Displacement diagram of power piston and displacer. (<b>a</b>) Displacement diagram from startup to stable operation. (<b>b</b>) Displacement diagram of steady state.</p>
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<p>Comparison between the displacer and the power piston. (<b>a</b>) Acceleration diagram (φ = π/2 vs. φ = 0) (<b>b</b>) Displacement diagram (φ = π/2 vs. φ = 0).</p>
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20 pages, 12180 KiB  
Article
Computer Vision-Based Research on the Mechanism of Stick–Slip Vibration Suppression and Wear Reduction in Water-Lubricated Rubber Bearing by Surface Texture
by Anbang Zhu, Ao Ji, Longyang Sheng, Dequan Zhu, Quan Zheng, Xincong Zhou, Jun Wang and Fuming Kuang
Lubricants 2024, 12(11), 402; https://doi.org/10.3390/lubricants12110402 - 20 Nov 2024
Viewed by 180
Abstract
Water-lubricated rubber bearings are a critical component of the propulsion systems in underwater vehicles. Particularly under conditions of low speed and high load, friction-induced vibration and wear often occur. Surface texturing technology has been proven to improve lubrication performance and reduce friction and [...] Read more.
Water-lubricated rubber bearings are a critical component of the propulsion systems in underwater vehicles. Particularly under conditions of low speed and high load, friction-induced vibration and wear often occur. Surface texturing technology has been proven to improve lubrication performance and reduce friction and wear; however, research on how different texture parameters affect friction-induced vibration and wear mechanisms remains insufficient. In this study, various texture patterns with different area ratios and aspect ratios were designed on the surface of water-lubricated rubber bearings. By combining these designs with an in situ observation system based on computer vision technology, the effects of texture parameters on bearing friction, vibration, and wear were thoroughly investigated. The experimental results show that surface textures play a critical role in improving hydrodynamic effects and stabilizing the lubrication film at the friction interface. Specifically, textures with a high area ratio (15%) and aspect ratio (3:1) exhibited the best vibration suppression effect, primarily due to the reduction in actual contact area. However, excessively high area ratios may lead to increased surface wear. This study concludes that a reasonable selection of texture area and aspect ratios can significantly reduce frictional force fluctuations and vibration amplitude, minimize surface wear, and extend bearing life. Full article
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<p>Water-lubricated bearing friction interface visualization test rig (KMZ-2).</p>
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<p>Schematic diagram of the dimensions of the experimental disc and rubber test block.</p>
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<p>Schematic diagram of surface texture structures and single texture unit, along with a super-depth three-dimensional microscopic image.</p>
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<p>The acquisition diagram of force, vibration, and high-speed image signals.</p>
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<p>Schematic diagram of the water film distribution observation system.</p>
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<p>Vibration, friction force, and displacement signals of the non-textured test block at different rotational speeds.</p>
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<p>The Effect of texture parameters and rotational speed on vibration response.</p>
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<p>The effect of rotational speed and texture parameters on friction force.</p>
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<p>The effect of rotational speed and texture parameters on test block displacement.</p>
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<p>The effect of load and texture parameters on the worn surface of the test block.</p>
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<p>Schematic diagram of lubricating water distribution for test blocks with different texture parameters.</p>
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<p>Schematic diagram of the effect of surface texture on lubricating film formation and hydrodynamic pressure effects.</p>
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<p>Variation in vibration and displacement amplitude of test blocks with different texture parameters at different rotational speeds.</p>
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<p>Fluorescence images of test blocks with different area ratios of texture.</p>
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<p>Fluorescence images of test blocks with different aspect ratios of texture.</p>
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<p>Surface roughness distribution and contact area analysis of test blocks with different texture parameters.</p>
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27 pages, 6232 KiB  
Review
A Review of Unmanned Aerial Vehicle Based Antenna and Propagation Measurements
by Venkat R. Kandregula, Zaharias D. Zaharis, Qasim Z. Ahmed, Faheem A. Khan, Tian Hong Loh, Jason Schreiber, Alexandre Jean René Serres and Pavlos I. Lazaridis
Sensors 2024, 24(22), 7395; https://doi.org/10.3390/s24227395 - 20 Nov 2024
Viewed by 264
Abstract
This paper presents a comprehensive survey of state-of-the-art UAV–based antennas and propagation measurements. Unmanned aerial vehicles (UAVs) have emerged as powerful tools for in situ electromagnetic field assessments due to their flexibility, cost-effectiveness, and ability to operate in challenging environments. This paper highlights [...] Read more.
This paper presents a comprehensive survey of state-of-the-art UAV–based antennas and propagation measurements. Unmanned aerial vehicles (UAVs) have emerged as powerful tools for in situ electromagnetic field assessments due to their flexibility, cost-effectiveness, and ability to operate in challenging environments. This paper highlights various UAV applications, from testing large–scale antenna arrays, such as those used in the square kilometer array (SKA), to evaluating channel models for 5G/6G networks. Additionally, the review discusses technical challenges, such as positioning accuracy and antenna alignment, and it provides insights into the latest advancements in portable measurement systems and antenna designs tailored for UAV use. During the UAV–based antenna measurements, key contributors to the relatively small inaccuracies of around 0.5 to 1 dB are identified. In addition to factors such as GPS positioning errors and UAV vibrations, ground reflections can significantly contribute to inaccuracies, leading to variations in the measured radiation patterns of the antenna. By minimizing ground reflections during UAV–based antenna measurements, errors in key measured antenna parameters, such as HPBW, realized gain, and the front-to-back ratio, can be effectively mitigated. To understand the source of propagation losses in a UAV to ground link, simulations were conducted in CST. These simulations identified scattering effects caused by surrounding buildings. Additionally, by simulating a UAV with a horn antenna, potential sources of electromagnetic coupling between the antenna and the UAV body were detected. The survey concludes by identifying key areas for future research and emphasizing the potential of UAVs to revolutionize antenna and propagation measurement practices to avoid the inaccuracies of the antenna parameters measured by the UAV. Full article
(This article belongs to the Special Issue New Methods and Applications for UAVs)
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<p>Organization of the paper.</p>
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<p>Measurement configuration of the UAV system.</p>
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<p>Conventional elevated slant test range.</p>
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<p>UAV–based in situ measurement for a parabolic reflector antenna system.</p>
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<p>UAV–based measurement for a parabolic reflector antenna system placed on a ship.</p>
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<p>Vertical radiation pattern of a BASTA using a UAV.</p>
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<p>Horizontal radiation pattern of a BASTA using a UAV.</p>
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<p>Common errors in broadcasting systems.</p>
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<p>SixArms airborne measurements for broadcasting systems.</p>
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<p>(<b>a</b>) UAV–based measurements at 720 m and (<b>b</b>) UAV–based measurements at 2025 m.</p>
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<p>UAV–based measurements in radiating near field.</p>
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<p>UAV–based measurements for an array of HF wire biconical antennas.</p>
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<p>UAV with monopole flying over the LPDA array.</p>
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<p>Scattering effect in a semi–urban area simulated in CST.</p>
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<p>Hexacopter carrying cloverleaf wire antenna.</p>
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<p>Scattering effect in an urban area simulated in CST Studio Suite.</p>
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<p>Fields scattered by the UAV body.</p>
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