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17 pages, 14357 KiB  
Article
Model Test of Dynamic Response of Living Poles Slope Under Train Loads
by Xueliang Jiang, Zihao Wang, Hui Yang and Haodong Wang
Appl. Sci. 2024, 14(23), 11355; https://doi.org/10.3390/app142311355 - 5 Dec 2024
Viewed by 470
Abstract
Live stump-supported slopes are an environmentally friendly form of support that utilizes the powerful anchoring and reinforcing effects of deep-rooted plants to enhance slope stability. In order to ensure the safety and stability of embankment slopes during their service life, it is necessary [...] Read more.
Live stump-supported slopes are an environmentally friendly form of support that utilizes the powerful anchoring and reinforcing effects of deep-rooted plants to enhance slope stability. In order to ensure the safety and stability of embankment slopes during their service life, it is necessary to carry out research on the dynamic characteristics and stability of live stump slopes under train vibration loading. In this study, a large-scale indoor dynamic loading model test with a geometry of 1:7 was carried out on the live stump slope of a ballasted passenger railroad track to explore the attenuation characteristics of additional dynamic stresses, the dynamic displacement response law of the slope surface and the stress response characteristics of the live stumps, and to further investigate the influence of the live stumps on the stability of the slope under the dynamic loading. The results are as follows. (i) Additional dynamic stresses decayed at the bed surface and bed floor at a greater rate than the embankment body, and were significantly affected by dynamic loading when the vertical depth was less than 0.89 m. (ii) The dynamic displacement of the foundation bed is larger than that of the embankment body. The displacement response of the slope near the top and about 1/4 of the elevation of slope is the largest. (iii) The taproot of the living poles has many reverse bending points, and the bending moment of the taproot between the lateral roots shows the law of being larger on the top and smaller on the bottom. (iv) The slope facing has an amplifying effect on the vibration load of the train, and the farther away from the track, the smaller the amplifying effect. The research results have reference significance for the theoretical research and engineering application of living poles. Full article
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<p>Profile of prototype slope.</p>
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<p>Model of the stump and rail: (<b>a</b>) Stump; (<b>b</b>) Rail.</p>
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<p>Construction of model box and layout of energy absorbing foam board: (<b>a</b>) construction of model box; (<b>b</b>) energy absorbing foam board.</p>
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<p>Layout of monitoring points in physical model.</p>
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<p>Layout of strain measuring points of living pole.</p>
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<p>Photo of slope model under excitation force.</p>
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<p>The curve of inspire force.</p>
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<p>Vertical dynamic pressure response data at different depths.</p>
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<p>Variation curve of peak pressure response with depth: (<b>a</b>) frequency; (<b>b</b>) axle load; (<b>c</b>) amplitude.</p>
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<p>Displacement distribution of slope under different axial loads.</p>
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<p>Time curve of strain of Z2 on pole A under working condition 1.</p>
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<p>Peak bending moment of the living poles under different axial loads: (<b>a</b>) bending moment of living poles A; (<b>b</b>) bending moment of living poles B; (<b>c</b>) bending moment of living poles C.</p>
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<p>The curve of stress of the lateral roots under working condition 2: (<b>a</b>) axial force of living poles A; (<b>b</b>) axial force of living poles B; (<b>c</b>) axial force of living poles C.</p>
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23 pages, 13815 KiB  
Article
Vibration Measurement and Numerical Simulation of the Effect of Non-Structural Elements on Dynamic Properties of Large-Span Structures
by Jialiang Chen, Wei He, Congbo Sun, Sen Hou, Junjie Chen and Zhe Wang
Buildings 2024, 14(11), 3589; https://doi.org/10.3390/buildings14113589 - 12 Nov 2024
Viewed by 640
Abstract
Non-structural elements have been demonstrated to be essential for the dynamic performance of large-span structures. However, how to quantify their effect has not yet been fully understood. In this study, the contribution of non-structural elements to dynamic properties of large-span structures is systematically [...] Read more.
Non-structural elements have been demonstrated to be essential for the dynamic performance of large-span structures. However, how to quantify their effect has not yet been fully understood. In this study, the contribution of non-structural elements to dynamic properties of large-span structures is systematically investigated via both field measurement and numerical simulation methods. Modal testing of an indoor stadium and an elevated highway bridge was conducted during different construction phases, and the corresponding modal characteristics were identified. Results show that the traditional capacity-based models are incapable of reflecting the actual dynamic characteristics of in-service structures since neglecting the effect of non-structural elements would result in remarkable discrepancies in modal properties. A general modeling framework incorporating the contribution of slab/deck pavement, infill walls (or crash barriers), and joints/connections for large-span structures is developed to quantitatively consider the effect of non-structural elements based on the principle of equivalence of stiffness and mass to the actual structure. The effectiveness of the method is validated by vibration measurement results. Full article
(This article belongs to the Special Issue Vibration Prediction and Noise Assessment of Building Structures)
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<p>BU Stadium. (<b>a</b>) Elevated view, (<b>b</b>) interior of 2nd floor (before decoration), (<b>c</b>) interior of 2nd floor (after decoration), and (<b>d</b>) impacting test.</p>
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<p>(<b>a</b>) Cross section of bridge L7, (<b>b</b>) plane view of bridge L7 with the layout of bearings (arrows denote possible movement directions), (<b>c</b>) side view (in construction), and (<b>d</b>) deck view (deck pavement). All dimensions in m.</p>
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<p>Construction method for bridge deck pavement.</p>
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<p>Data acquisition system and test instruments. (<b>a</b>) Bruel &amp; Kjaer DAQ system, (<b>b</b>) 4507B accelerometers, and (<b>c</b>) VSE-15-D1 accelerometer.</p>
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<p>Plan view of slab B4 and sensor arrangements. All dimensions in mm.</p>
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<p>Measured floor responses with single-person impacting.</p>
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<p>Measured floor responses with single-person impacting. (<b>a</b>) Time history; (<b>b</b>) frequency sepectrum.</p>
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<p>Test grid and sensors deployment of L7 bridge. Note: 1. All dimensions are in m; TP: test point; 2. △ Fixed reference TP, in three orthogonal directions; <span class="html-fig-inline" id="buildings-14-03589-i001"><img alt="Buildings 14 03589 i001" src="/buildings/buildings-14-03589/article_deploy/html/images/buildings-14-03589-i001.png"/></span> mobile TP, in vertical and transverse directions; <span class="html-fig-inline" id="buildings-14-03589-i002"><img alt="Buildings 14 03589 i002" src="/buildings/buildings-14-03589/article_deploy/html/images/buildings-14-03589-i002.png"/></span> mobile TP, in vertical direction.</p>
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<p>Stabilization diagram at reference point: (<b>a</b>) vertical direction; (<b>b</b>) transverse direction. Note: ☆ represents stable points for frequency, * denotes stable points for frequency and damping ratio, ○ denotes stable points for frequency, damping ratio, and mode shape.</p>
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<p>The first few mode shapes of the L7 bridge based on the SSI method.</p>
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<p>The first few mode shapes of the L7 bridge based on the SSI method.</p>
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<p>Infill walls under horizontal load: (<b>a</b>) actual system, (<b>b</b>) simplified model.</p>
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<p>Schematic of boundary conditions to be processed.</p>
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<p>First three bending modes of large-span floors in BU stadium (Phase 2) by the FE method.</p>
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<p>(<b>a</b>) cross section and (<b>b</b>) FE model of the L7 bridge.</p>
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<p>First 12 mode shapes of the L7 bridge (Phase 3) based on the initial FE model.</p>
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<p>First 12 mode shapes of the L7 bridge (Phase 3) based on the initial FE model.</p>
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16 pages, 2157 KiB  
Article
Motion Target Localization Method for Step Vibration Signals Based on Deep Learning
by Rui Chen, Yanping Zhu, Qi Chen and Chenyang Zhu
Appl. Sci. 2024, 14(20), 9361; https://doi.org/10.3390/app14209361 - 14 Oct 2024
Viewed by 788
Abstract
To address the limitations of traditional footstep vibration signal localization algorithms, such as limited accuracy, single feature extraction, and cumbersome parameter adjustment, a motion target localization method for step vibration signals based on deep learning is proposed. Velocity vectors are used to describe [...] Read more.
To address the limitations of traditional footstep vibration signal localization algorithms, such as limited accuracy, single feature extraction, and cumbersome parameter adjustment, a motion target localization method for step vibration signals based on deep learning is proposed. Velocity vectors are used to describe human motion and adapt it to the nonlinear motion and complex interactions of moving targets. In the feature extraction stage, a one-dimensional residual convolutional neural network is constructed to extract the time–frequency domain features of the signals, and a channel attention mechanism is introduced to enhance the model’s focus on different vibration sensor signal features. Furthermore, a bidirectional long short-term memory network is built to learn the temporal relationships between the extracted signal features of the convolution operation. Finally, regression operations are performed through fully connected layers to estimate the position and velocity vectors of the moving target. The dataset consists of footstep vibration signal data from six experimental subjects walking on four different paths and the actual motion trajectories of the moving targets obtained using a visual tracking system. Experimental results show that compared to WT-TDOA and SAE-BPNN, the positioning accuracy of our method has been improved by 37.9% and 24.8%, respectively, with a system average positioning error reduced to 0.376 m. Full article
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<p>Location scenario. This figure shows the experiment scene of vibration signal acquisition of a moving target, including the sensor configuration, single moving target, and one camera.</p>
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<p>Overview of our method. This paper proposes a deep learning-based method for locating moving targets using vibration signals. The approach begins by collecting vibration signal data sequences and recording the actual trajectories of pedestrians on the ground using cameras. Subsequently, supervised learning is employed, leveraging deep learning techniques to extract signal features for training the positioning model. Finally, the two-dimensional velocity vectors of pedestrians are output to estimate their motion trajectories.</p>
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<p>Architectures of our method.</p>
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<p>The real experimental conditions.</p>
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<p>Comparison of the predicted trajectory and the real trajectory.</p>
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<p>Velocity vector comparison. (<b>a</b>) Comparison of real velocity and prediction in the X-axis direction. (<b>b</b>) Comparison of real velocity and prediction in the Y-axis direction.</p>
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<p>Part of the linear path test results. (<b>a</b>) The test set results of experimenter A. (<b>b</b>) The test set results of experimenter B. (<b>c</b>) The test set results of experimenter C.</p>
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<p>Part of the test result graph around the figure-eight path. (<b>a</b>) The test set results of experimenter A. (<b>b</b>) The test set results of experimenter B. (<b>c</b>) The test set results of experimenter C.</p>
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<p>Part of the loop path test results. (<b>a</b>) The test set results of experimenter A. (<b>b</b>) The test set results of experimenter B. (<b>c</b>) The test set results of experimenter C.</p>
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<p>Part of the L-path test results. (<b>a</b>) The test set results of experimenter A. (<b>b</b>) The test set results of experimenter B. (<b>c</b>) The test set results of experimenter C.</p>
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<p>Test set experimental results.</p>
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<p>Comparison of positioning results of different methods.</p>
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14 pages, 3006 KiB  
Article
Study on the Performance Evaluation Method and Application of Drainage Nonwoven Geotextile in the Yellow River Sediment Filling Reclamation Area
by Huang Sun, Zhenqi Hu, Deyun Song, Xinran Nie and Shuai Wang
Land 2024, 13(10), 1597; https://doi.org/10.3390/land13101597 - 30 Sep 2024
Viewed by 703
Abstract
Technical challenges associated with drainage and filling efficacy confront the Yellow River sediment filling reclamation, a novel approach to reclaiming coal-mined subsided lands. This study proposes an improved geotextile performance evaluation method to address the shortcomings of current geotextile screening methodologies in the [...] Read more.
Technical challenges associated with drainage and filling efficacy confront the Yellow River sediment filling reclamation, a novel approach to reclaiming coal-mined subsided lands. This study proposes an improved geotextile performance evaluation method to address the shortcomings of current geotextile screening methodologies in the drainage of the Yellow River sediment. This method comprehensively considers essential characteristics under working conditions, such as permeability, soil conservation, and blockage prevention properties, including indicators such as the permeability coefficient and sediment retention rate of geotextiles under pressure. Indoor flume filling and drainage experiments were implemented to verify the efficacy of geotextile drainage. The improved method identified thermal-bonded nonwoven geotextiles of 200 and 250 g·m−2 as having the highest comprehensive evaluation scores. The experimental results showed that these geotextiles significantly improved their drainage efficiency and better met the specific requirements of the Yellow River sediment filling reclamation. Traditional screening methods may be unsuitable for sediment drainage conditions, necessitating sediment interception and rapid drainage due to the streaming water–sediment mixture. Therefore, the newly established performance evaluation method is more appropriate for the specific requirements. It is recommended that a simple vibrating device be installed to maintain 20 vibrations per minute to keep drainage channels clear and provide stable drainage performance in engineering applications. Full article
(This article belongs to the Section Land, Soil and Water)
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<p>(<b>a</b>) Location and basic characteristics of coal-mined subsided lands; (<b>b</b>) Location of coal-mined subsided lands and Yellow River sediment collection points; (<b>c</b>) Dredging ships clearing accumulated sediment; (<b>d</b>) The particle size distribution curve of the Yellow River sediment.</p>
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<p>Cross-section of a flume experiment device: (<b>a</b>) Left view along drainage direction of the process of filling and drainage in plastic flume; (<b>b</b>) Front view of test geotextile discharge cross-sections; and (<b>c</b>) Front view of CK discharge cross-sections.</p>
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<p>Geotextile evaluation indicator weightfvs and results: (<b>a</b>) Evaluation indicator weights; and (<b>b</b>) Geotextile evaluation results.</p>
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<p>Sediment content in drainage water of experiment treatments.</p>
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<p>(<b>a</b>–<b>c</b>) Moisture content change of the surface sediments of experiment treatments in a plastic flume at points 1, 2, 3; (<b>d</b>–<b>f</b>) Moisture content change of surface sediments of experiment treatments in a plastic flume at points 1, 2, 3.</p>
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<p>Moisture content change in surface and bottom sediments of three treatments in plastic flume: (<b>a</b>–<b>c</b>) Moisture content change of surface sediments at points 1, 2, and 3; and (<b>d</b>–<b>f</b>) Moisture content change of bottom sediments on points 1, 2, and 3. Note: ZT-250,ZT-300 EDR base on the data from ref. [<a href="#B10-land-13-01597" class="html-bibr">10</a>].</p>
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<p>Geotextile treatment drainage speed under vibration.</p>
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18 pages, 7037 KiB  
Article
Predicting the Influence of Vibration from Trains in the Throat Area of a Metro Depot on Over-Track Buildings
by Guoqing Di, Hanxin Li and Jingyi Guo
Appl. Sci. 2024, 14(19), 8598; https://doi.org/10.3390/app14198598 - 24 Sep 2024
Viewed by 512
Abstract
Urban land resources are scarce in China. To utilize land effectively and economically, many cities are developing over-track buildings above metro depots. The vibration from the entrance and exit lines of metro depots under an over-track platform would significantly impact over-track buildings. To [...] Read more.
Urban land resources are scarce in China. To utilize land effectively and economically, many cities are developing over-track buildings above metro depots. The vibration from the entrance and exit lines of metro depots under an over-track platform would significantly impact over-track buildings. To study the influence of train vibration in the throat area of a metro depot on over-track buildings, a simulation model was established using a finite element method. The reasonability of the simulation method and parameter settings was verified through comparing the vibration simulation results with vibration test results in the throat area of a metro depot. Furthermore, the impact of parameters of over-track platform and building on indoor vibration induced by a train was quantitatively studied. According to simulation results, a prediction model was developed to predict the impact of train vibration on over-track buildings in metro depots. From the perspective of architectural planning and design, this study provides a theoretical and technical basis for the prevention and control of indoor vibrations in over-track buildings of urban metro depots. Full article
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<p>A simplified model of the vertical vibration of a train [<a href="#B19-applsci-14-08598" class="html-bibr">19</a>].</p>
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<p>The load of vertical vibration from trains in the straight section of the throat area.</p>
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<p>The geometric model of track, soil, and over-track platform and building.</p>
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<p>Layouts of verification points in the measured metro depot.</p>
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<p>Layouts of vibration acceleration sensors at each sampling point: (<b>a</b>) ground; (<b>b</b>) column of the over-track platform.</p>
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<p>The comparison of the measured and simulated 1/3 octave spectrum of the vertical vibration acceleration level: (<b>a</b>) ground; (<b>b</b>) column of the over-track platform.</p>
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<p>Layouts of the civil building and measurement points: (<b>a</b>) horizontal layout; (<b>b</b>) vertical layout.</p>
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<p>The measured results of vertical vibration at C1: (<b>a</b>) vibration acceleration in time domain; (<b>b</b>) frequency spectra of vibration acceleration between 0 Hz and 250 Hz.</p>
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<p>The <span class="html-italic">VL</span><sub>Zmax</sub> at each floor in the frame and shear wall buildings with 4–20 storeys: (<b>a</b>) frame structure; (<b>b</b>) shear wall structure.</p>
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<p>The influence of <span class="html-italic">N</span> on the <span class="html-italic">VL</span><sub>Zmax</sub> of the first floor.</p>
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<p>The influence of <span class="html-italic">N</span> on the Δ<span class="html-italic">VL</span><sub>Zmax</sub> in buildings.</p>
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<p>The influence of <span class="html-italic">W</span> on the <span class="html-italic">VL</span><sub>Zmax</sub> of the first floor.</p>
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<p>The influence of <span class="html-italic">R</span> on the <span class="html-italic">VL</span><sub>Zmax</sub> of the first floor.</p>
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<p>The influence of <span class="html-italic">W</span> on Δ<span class="html-italic">VL</span><sub>Zmax</sub> in buildings.</p>
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<p>The influence of <span class="html-italic">R</span> on Δ<span class="html-italic">VL</span><sub>Zmax</sub> in buildings.</p>
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<p>The influence of <span class="html-italic">D</span> on the <span class="html-italic">VL</span><sub>Zmax</sub> of the first floor.</p>
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<p>The influence of <span class="html-italic">H</span> on the <span class="html-italic">VL</span><sub>Zmax</sub> of the first floor.</p>
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<p>The influence of <span class="html-italic">T</span> on the <span class="html-italic">VL</span><sub>Zmax</sub> of the first floor.</p>
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<p>The influence of <span class="html-italic">S</span> on the <span class="html-italic">VL</span><sub>Zmax</sub> of the first floor.</p>
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19 pages, 15502 KiB  
Article
Train-Induced Vibration and Structure-Borne Noise Measurement and Prediction of Low-Rise Building
by Jialiang Chen, Sen Hou, Bokai Zheng, Xuming Li, Fangling Peng, Yingying Wang and Junjie Chen
Buildings 2024, 14(9), 2883; https://doi.org/10.3390/buildings14092883 - 12 Sep 2024
Viewed by 952
Abstract
The advancement of urban rail transit is increasingly confronted with environmental challenges related to vibration and noise. To investigate the critical issues surrounding vibration propagation and the generation of structure-borne noise, a two-story frame building was selected for on-site measurements of both vibration [...] Read more.
The advancement of urban rail transit is increasingly confronted with environmental challenges related to vibration and noise. To investigate the critical issues surrounding vibration propagation and the generation of structure-borne noise, a two-story frame building was selected for on-site measurements of both vibration and its induced structure-borne noise. The collected data were analyzed in both the time and frequency domains to explore the correlation between these phenomena, leading to the proposal of a hybrid prediction method for structural noise that was subsequently compared with measured results. The findings indicate that the excitation of structure-borne noise produces significant waveforms within sound signals. The characteristic frequency of the structure-borne noise is 25–80 Hz, as well as that of the train-induced vibration. Furthermore, there exists a positive correlation between structural vibration and structure-borne noise, whereby increased levels of vibration correspond to more pronounced structure-borne noise; additionally, indoor distribution patterns of structure-borne noise are non-uniform, with corner wall areas exhibiting greater intensity than central room locations. Finally, a hybrid prediction methodology that is both semi-analytical and semi-empirical is introduced. The approach derives dynamic response predictions of the structure through analytical solutions, subsequently estimating the secondary noise within the building’s interior using a newly formulated empirical equation to facilitate rapid predictions regarding indoor building vibrations and structure-borne noises induced by subway train operations. Full article
(This article belongs to the Special Issue Vibration Prediction and Noise Assessment of Building Structures)
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<p>Schematic representation of measurement program and spatial relationship between tunnel and building.</p>
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<p>Photographs of instrumentation utilized for measurement.</p>
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<p>Flowchart of measuring procedures.</p>
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<p>Time history and spectrogram interception of the train pass-by events.</p>
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<p>Time domain diagram of vibration acceleration of field soil and building structure.</p>
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<p>Time domain diagram of vibration acceleration of measuring point G1 on field soil.</p>
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<p>Time domain diagram of sound pressure of near tunnel on floor center.</p>
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<p>Comparison of vibration acceleration levels in frequency domain at different measuring points of the near tunnel.</p>
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<p>Comparison of vibration acceleration levels in frequency domain of near and far tunnels on field soil.</p>
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<p>Comparison of noise sound pressure in frequency domain of different measuring points of near tunnel.</p>
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<p>Comparison of noise sound pressure level in frequency domain of same measurement points of near and far tunnels.</p>
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<p>Measured transmission difference.</p>
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<p>Comparison of measured and model’s predicted results [<a href="#B22-buildings-14-02883" class="html-bibr">22</a>,<a href="#B24-buildings-14-02883" class="html-bibr">24</a>,<a href="#B29-buildings-14-02883" class="html-bibr">29</a>,<a href="#B30-buildings-14-02883" class="html-bibr">30</a>,<a href="#B33-buildings-14-02883" class="html-bibr">33</a>].</p>
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<p>Comparison of errors between measured and model’s predicted results [<a href="#B22-buildings-14-02883" class="html-bibr">22</a>,<a href="#B24-buildings-14-02883" class="html-bibr">24</a>,<a href="#B29-buildings-14-02883" class="html-bibr">29</a>,<a href="#B30-buildings-14-02883" class="html-bibr">30</a>,<a href="#B33-buildings-14-02883" class="html-bibr">33</a>].</p>
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15 pages, 4158 KiB  
Article
Experimental Investigation on Building Sound Environment: Traffic-Induced Air Noise and Structure-Borne Noise
by Jialiang Chen, Lingshan He, Xuming Li, Bokai Zheng, Teng Wang, Dongyang Wang and Chao Zou
Buildings 2024, 14(8), 2380; https://doi.org/10.3390/buildings14082380 - 1 Aug 2024
Viewed by 1138
Abstract
The impact of urban traffic on human health is significant. This research conducts field measurements in Guangzhou, China, focusing on a building situated near subgrade roads and viaducts to investigate the characteristics of airborne and structure-borne noise generated by these infrastructures. The analysis [...] Read more.
The impact of urban traffic on human health is significant. This research conducts field measurements in Guangzhou, China, focusing on a building situated near subgrade roads and viaducts to investigate the characteristics of airborne and structure-borne noise generated by these infrastructures. The analysis involves the use of both sound pressure level and overall sound pressure level, as well as an examination of the transfer function between outdoor and indoor noise levels. The findings indicate that traffic-related airborne noise demonstrates a characteristic frequency at 1000 Hz in this scenario, while viaduct- and building-generated structure-borne noise is predominantly distributed at lower frequencies. Additionally, it is worth noting that structural vibrations generate significantly less energy compared to airborne traffic noise sources. The variation in outdoor road noise across different floors over the entire frequency range demonstrates an initial increase followed by a decrease with rising floor height due to air damping effects as well as sound barriers’ attenuation properties. These results enhance engineers’ understanding of urban traffic-induced airborne or structure-borne noise while establishing foundational data for designing layouts integrating urban buildings with roads. Full article
(This article belongs to the Special Issue Vibration Prediction and Noise Assessment of Building Structures)
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<p>Structures of the study.</p>
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<p>Photographs of buildings.</p>
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<p>Photograph and spatial layout of the measurement room.</p>
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<p>Schematic representation of indoor noise generated by road traffic.</p>
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<p>Instrumentation setup and the photos in different positions during measuring.</p>
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<p>Comparison of sound pressure level at different times. (<b>a</b>) A-weighted SPL; (<b>b</b>) A-weighted overall SPL.</p>
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<p>Comparison of the sound pressure levels with different distances from the traffic road. (<b>a</b>) A-weighted SPL; (<b>b</b>) A-weighted overall SPL.</p>
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<p>Comparison of the SPLs of indoors and outdoors. A-weighted SPL (<b>a</b>) on 6th floor; (<b>c</b>) on 10th floor; (<b>e</b>) on 14th floor. A-weighted overall SPL (<b>b</b>) on 6th floor; (<b>d</b>) on 10th floor; (<b>f</b>) on 14th floor.</p>
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<p>Comparison of the SPLs of indoors and outdoors. A-weighted SPL (<b>a</b>) on 6th floor; (<b>c</b>) on 10th floor; (<b>e</b>) on 14th floor. A-weighted overall SPL (<b>b</b>) on 6th floor; (<b>d</b>) on 10th floor; (<b>f</b>) on 14th floor.</p>
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<p>Comparison of the outdoor noise with the different building floor heights; (<b>a</b>) A-weighted SPL; (<b>b</b>) Overall A-weighted SPL.</p>
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<p>Schematic representation of the reduction effect of the sound barrier.</p>
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<p>Comparison of indoor noise with different building floor heights; (<b>a</b>) A-weighted SPL; (<b>b</b>) Overall A-weighted SPL.</p>
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<p>Comparison of the SPLs from different types of road; (<b>a</b>) A-weighted SPL; (<b>b</b>) Overall A-weighted SPL.</p>
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<p>Comparison of indoor and outdoor noise and their transfer function on the third floor; (<b>a</b>) A-weighted SPL; (<b>b</b>) Transfer function.</p>
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32 pages, 17404 KiB  
Article
A Novel Method for Full-Section Assessment of High-Speed Railway Subgrade Compaction Quality Based on ML-Interval Prediction Theory
by Zhixing Deng, Wubin Wang, Linrong Xu, Hao Bai and Hao Tang
Sensors 2024, 24(11), 3661; https://doi.org/10.3390/s24113661 - 5 Jun 2024
Cited by 1 | Viewed by 1109
Abstract
The high-speed railway subgrade compaction quality is controlled by the compaction degree (K), with the maximum dry density (ρdmax) serving as a crucial indicator for its calculation. The current mechanisms and methods for determining the ρdmax [...] Read more.
The high-speed railway subgrade compaction quality is controlled by the compaction degree (K), with the maximum dry density (ρdmax) serving as a crucial indicator for its calculation. The current mechanisms and methods for determining the ρdmax still suffer from uncertainties, inefficiencies, and lack of intelligence. These deficiencies can lead to insufficient assessments for the high-speed railway subgrade compaction quality, further impacting the operational safety of high-speed railways. In this paper, a novel method for full-section assessment of high-speed railway subgrade compaction quality based on ML-interval prediction theory is proposed. Firstly, based on indoor vibration compaction tests, a method for determining the ρdmax based on the dynamic stiffness Krb turning point is proposed. Secondly, the Pso-OptimalML-Adaboost (POA) model for predicting ρdmax is determined based on three typical machine learning (ML) algorithms, which are back propagation neural network (BPNN), support vector regression (SVR), and random forest (RF). Thirdly, the interval prediction theory is introduced to quantify the uncertainty in ρdmax prediction. Finally, based on the Bootstrap-POA-ANN interval prediction model and spatial interpolation algorithms, the interval distribution of ρdmax across the full-section can be determined, and a model for full-section assessment of compaction quality is developed based on the compaction standard (95%). Moreover, the proposed method is applied to determine the optimal compaction thicknesses (H0), within the station subgrade test section in the southwest region. The results indicate that: (1) The PSO-BPNN-AdaBoost model performs better in the accuracy and error metrics, which is selected as the POA model for predicting ρdmax. (2) The Bootstrap-POA-ANN interval prediction model for ρdmax can construct clear and reliable prediction intervals. (3) The model for full-section assessment of compaction quality can provide the full-section distribution interval for K. Comparing the H0 of 50~60 cm and 60~70 cm, the compaction quality is better with the H0 of 40~50 cm. The research findings can provide effective techniques for assessing the compaction quality of high-speed railway subgrades. Full article
(This article belongs to the Topic Advanced Risk Assessment in Geotechnical Engineering)
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<p>A framework for full-section assessment of high-speed railway subgrade compaction quality based on ML-interval prediction theory.</p>
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<p>Novel method for determining <span class="html-italic">ρ</span><sub>dmax..</sub> The progression from A to B to C represents the gradual·densification of the particles in the compacted·state. The progression from C to D represents the gradual deterioration of the particles after optimal compaction time.</p>
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<p>Large intelligent vibration compaction instrument.</p>
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<p>Evolution curve of <span class="html-italic">ρ<sub>d</sub></span>, <span class="html-italic">K<sub>rb</sub></span>, and <span class="html-italic">K</span><sub>20</sub> for grading aggregates: (<b>a</b>) <span class="html-italic">ρ<sub>d</sub>;</span> (<b>b</b>) <span class="html-italic">K<sub>rb</sub>;</span> and (<b>c</b>) <span class="html-italic">K</span><sub>20.</sub></p>
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<p><span class="html-italic">POA</span> prediction model for <span class="html-italic">ρ<sub>dmax.</sub></span></p>
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<p>Three selected ML algorithms: (<b>a</b>) BPNN; (<b>b</b>) SVR; and (<b>c</b>) RF.</p>
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<p>Sources of prediction uncertainty.</p>
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<p>Prediction interval structure.</p>
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<p>Quantification of <span class="html-italic">ρ</span><sub>dmax</sub> prediction uncertainty.</p>
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<p>Bootstrap-modification for <span class="html-italic">ρ<sub>dmax</sub></span> POA model.</p>
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<p>Illustration of pseudo-training set generation.</p>
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<p>A model for the full-section assessment of compaction quality based on ML-interval prediction theory.</p>
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<p>Three typical interpolation algorithms: (<b>a</b>) IDW; (<b>b</b>) Spline; (<b>c</b>) Kriging.</p>
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<p><span class="html-italic">ρ<sub>dmax</sub></span> prediction database: (<b>a</b>) <span class="html-italic">d</span><sub>max</sub>; (<b>b</b>) <span class="html-italic">b</span>; (<b>c</b>) <span class="html-italic">m</span>; (<b>d</b>) <span class="html-italic">EI</span>; (<b>e</b>) <span class="html-italic">LAA</span>; (<b>f</b>) <span class="html-italic">Wac</span>; (<b>g</b>) <span class="html-italic">Waf</span>.</p>
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<p><span class="html-italic">ρ<sub>dmax</sub></span> prediction database: (<b>a</b>) <span class="html-italic">d</span><sub>max</sub>; (<b>b</b>) <span class="html-italic">b</span>; (<b>c</b>) <span class="html-italic">m</span>; (<b>d</b>) <span class="html-italic">EI</span>; (<b>e</b>) <span class="html-italic">LAA</span>; (<b>f</b>) <span class="html-italic">Wac</span>; (<b>g</b>) <span class="html-italic">Waf</span>.</p>
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<p>PSO parameter optimization results and fitting results on the training set: (<b>a</b>) PSO parameter optimization; (<b>b</b>) PSO-BPNN-AdaBoost; (<b>c</b>) PSO-SVR-AdaBoost; and (<b>d</b>) PSO-RF-AdaBoost.</p>
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<p>PSO parameter optimization results and fitting results on the training set: (<b>a</b>) PSO parameter optimization; (<b>b</b>) PSO-BPNN-AdaBoost; (<b>c</b>) PSO-SVR-AdaBoost; and (<b>d</b>) PSO-RF-AdaBoost.</p>
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<p>Point prediction results: (<b>a</b>) PSO-BPNN-AdaBoost; (<b>b</b>) PSO-SVR-AdaBoost; and (<b>c</b>) PSO-RF-AdaBoost.</p>
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<p>The prediction performance of PSO-BPNN model: (<b>a</b>) fitting results on the training set for PSO-BPNN; (<b>b</b>) prediction results on the training set for PSO-BPNN.</p>
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<p>Interval prediction results: (<b>a</b>) 90% confidence level; (<b>b</b>) 95% confidence level; (<b>c</b>) 99% confidence level; and (<b>d</b>) accuracy assessment.</p>
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<p>Predicted output and variance at 95% confidence level: (<b>a</b>) predicted output; (<b>b</b>) variance of the total error; (<b>c</b>) variance of the cognitive error; (<b>d</b>) variance of the random error; and (<b>e</b>) distribution of random error variance.</p>
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<p>Test section.</p>
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<p>Results of measured <span class="html-italic">ρ<sub>d</sub></span>: (<b>a</b>) 40~50 cm thickness; (<b>b</b>) 50~60 cm thickness; and (<b>c</b>) 60~70 cm thickness.</p>
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<p>Interpolation results of <span class="html-italic">ρ</span><sub>d</sub> at 40 cm thickness using different interpolation algorithms: (<b>a</b>) Spline algorithm; (<b>b</b>) IDW algorithm; and (<b>c</b>) Kriging algorithm.</p>
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<p>Full-section distribution results of filler parameters: (<b>a</b>) <span class="html-italic">d</span><sub>max</sub>; (<b>b</b>) <span class="html-italic">b</span>; (<b>c</b>) <span class="html-italic">m</span>; (<b>d</b>) <span class="html-italic">EI</span>; (<b>e</b>) <span class="html-italic">LAA</span>; (<b>f</b>) <span class="html-italic">W</span><sub>ac</sub>; and (<b>g</b>) <span class="html-italic">W</span><sub>af.</sub></p>
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<p>Full-section distribution results of filler parameters: (<b>a</b>) <span class="html-italic">d</span><sub>max</sub>; (<b>b</b>) <span class="html-italic">b</span>; (<b>c</b>) <span class="html-italic">m</span>; (<b>d</b>) <span class="html-italic">EI</span>; (<b>e</b>) <span class="html-italic">LAA</span>; (<b>f</b>) <span class="html-italic">W</span><sub>ac</sub>; and (<b>g</b>) <span class="html-italic">W</span><sub>af.</sub></p>
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<p>Full-section distribution results of filler parameters: (<b>a</b>) <span class="html-italic">d</span><sub>max</sub>; (<b>b</b>) <span class="html-italic">b</span>; (<b>c</b>) <span class="html-italic">m</span>; (<b>d</b>) <span class="html-italic">EI</span>; (<b>e</b>) <span class="html-italic">LAA</span>; (<b>f</b>) <span class="html-italic">W</span><sub>ac</sub>; and (<b>g</b>) <span class="html-italic">W</span><sub>af.</sub></p>
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<p>Results of the interval prediction for full-section <span class="html-italic">ρ<sub>dmax</sub></span>: (<b>a</b>) 40~50 cm thickness; (<b>b</b>) 50~60 cm thickness; and (<b>c</b>) greater than 60 cm thickness.</p>
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<p>Results of the interval assessment for full-section compaction quality: (<b>a</b>) 40~50 cm thickness; (<b>b</b>) 50~60 cm thickness; and (<b>c</b>) greater than 60 cm thickness.</p>
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<p>A framework for the full-section assessment of high-speed railway subgrade service performance based on ML-interval prediction theory.</p>
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<p>A full cross-section compaction quality assessment system.</p>
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47 pages, 36235 KiB  
Article
Research on Running Performance Optimization of Four-Wheel-Driving Ackerman Chassis by the Combining Method of Quantitative Experiment with Dynamic Simulation
by Xiangyu Zhang, Bowen Xie, Yang Yang, Yongbin Liu and Pan Jiang
Machines 2024, 12(3), 198; https://doi.org/10.3390/machines12030198 - 17 Mar 2024
Viewed by 1778
Abstract
The wheeled chassis, which is the carrying device of the existing handling robot, is mostly only suitable for flat indoor environments and does not have the ability to work on outdoor rugged terrain, greatly limiting the development of chassis driven handling robots. On [...] Read more.
The wheeled chassis, which is the carrying device of the existing handling robot, is mostly only suitable for flat indoor environments and does not have the ability to work on outdoor rugged terrain, greatly limiting the development of chassis driven handling robots. On this basis, this paper innovatively designs a four-wheel-driving Ackerman chassis with strong vibration absorption and obstacle surmounting capabilities and conducts performance research and optimization on it through quantitative experiments and dynamic simulation. Firstly, based on the introduction of the working principle and structure of the four-wheel-driving Ackerman carrier chassis, a multi-sensor distributed dynamic performance test system is constructed through the analysis of the chassis performance evaluation index. Then, according to the quantitative operation experiment of the chassis, the vibration and acceleration characteristics of the chassis at different positions of the chassis, the amount of slip and straightness of the chassis under different running distance, and the operating characteristics of the chassis under different road conditions and different damping springs conditions were analyzed respectively, which verified the rationality of the chassis design. Finally, by constructing the chassis dynamics simulation model; the influence law of chassis structure; and performance parameters such as chassis wheelbase, guide rod structure, and parameters, wheel friction coefficient and assembly error on the dynamic characteristics of the chassis is studied, and the optimal structure of the four-wheel-driving Ackerman chassis is determined while it is verified based on the simulation results. The research shows that the four-wheel-driving Ackerman chassis has good vibration performance and stability and has strong adaptability to different roads. After optimization, the vibration performance, stability, amount of slip, and straightness of the chassis structure are significantly improved, and the straightness is reduced to 0.399%, which is suitable for precise carriage applications on the chassis. The research has important guiding significance for promoting the development and application of wheeled chassis. Full article
(This article belongs to the Section Vehicle Engineering)
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<p>Ackerman steering principle.</p>
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<p>Ackermann mechanism of the chassis.</p>
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<p>Installation arrangement of Ackermann steering mechanism.</p>
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<p>The rod model of the Ackerman steering mechanism.</p>
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<p>Construction of four-wheel-driving Akerman carrier chassis.</p>
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<p>The realized vehicle.</p>
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<p>Kinematic model construction of the Ackerman carrier chassis.</p>
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<p>Multi-sensor distribution characteristics.</p>
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<p>Principle of straightness test.</p>
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<p>Three-dimensional schematic of the multi-sensor information test system (the red marks are vibration sensors and the blue ones are acceleration sensors in the figure).</p>
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<p>Effects of each experiment.</p>
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<p>Vibration displacement at different positions.</p>
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<p>Acceleration of X-axis at different positions.</p>
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<p>Acceleration of Y-axis at different positions.</p>
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<p>Acceleration of Z-axis at different positions.</p>
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<p>Slipping amount of the two wheels under different operating distances.</p>
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<p>The deviation values of Experiment 1. (<b>a</b>) Calibrated distance, (<b>b</b>) Actual distance.</p>
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<p>The deviation values of Experiment 2. (<b>a</b>) Calibrated distance, (<b>b</b>) Actual distance.</p>
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<p>The deviation values of Experiment 3. (<b>a</b>) Calibrated distance, (<b>b</b>) Actual distance.</p>
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<p>The deviation values of Experiment 4.(<b>a</b>) Calibrated distance, (<b>b</b>) Actual distance.</p>
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<p>The deviation values of Experiment 5. (<b>a</b>) Calibrated distance, (<b>b</b>) Actual distance.</p>
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<p>The average offset.</p>
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<p>The average deviation proportion.</p>
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<p>Operating environment of the chassis. (<b>a</b>) Porcelain floor, (<b>b</b>) Asphalt road, (<b>c</b>) Cement road, (<b>d</b>) 15° slope.</p>
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<p>Vibration displacement.</p>
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<p>Acceleration in the X-direction.</p>
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<p>Deformation experiment of spring under loading.</p>
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<p>Spring–loading force curve.</p>
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<p>Spring vibration displacement under different spring conditions.</p>
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<p>Spring vibration displacement under different spring conditions.</p>
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<p>Motion acceleration in X direction under different spring conditions.</p>
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<p>Motion acceleration in X direction under different spring conditions.</p>
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<p>Performance optimization method combining quantitative experiment and dynamic simulation.</p>
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<p>Four-wheel-driving Ackerman chassis dynamics simulation model.</p>
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<p>Vibration displacement of different positions of the chassis under different wheelbases.</p>
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<p>Vibration displacement in different positions under different guide rod structures.</p>
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<p>Vibration displacement of different positions with different friction coefficients.</p>
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<p>Wheel slip amount under different wheel friction coefficients.</p>
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18 pages, 3187 KiB  
Article
Effects of Periodic Materials on Distance Attenuation in Wall–Slab Structures: An Experiment
by Jongwoo Cho, Kwonsik Song, Nahyun Kwon, Moonseo Park and Tae Wan Kim
Buildings 2024, 14(3), 694; https://doi.org/10.3390/buildings14030694 - 5 Mar 2024
Cited by 1 | Viewed by 1085
Abstract
This research examines the application of periodic materials in wall–slab structures to mitigate impact noise and vibration propagation, a prevalent issue in multifamily housing. Traditional methods, such as floating floors, have proven insufficient in addressing low-frequency impact noises and in facilitating the identification [...] Read more.
This research examines the application of periodic materials in wall–slab structures to mitigate impact noise and vibration propagation, a prevalent issue in multifamily housing. Traditional methods, such as floating floors, have proven insufficient in addressing low-frequency impact noises and in facilitating the identification of noise origins, leading to increased resident annoyance. Periodic materials, known for their effectiveness in controlling plane waves in civil engineering, were applied to the intermediate slab of a wall–slab experimental setup. The research involved assessing the attenuation of noise and vibration over distance before and after the application of periodic materials by measuring indoor sound pressure levels and the natural vibration amplitude of the structure’s members upon impact. The results showed that periodic materials not only facilitated distance attenuation but also significantly diminished noise and vibration throughout the structure, without the side effects of vibration amplification seen in prior civil engineering applications. This indicates a practical advancement in using these materials, offering a novel approach to sound insulation and enabling more precise impact source localization. Ultimately, this study contributes to improving urban living by suggesting a method to enhance acoustic comfort in multifamily housing, underlining the importance of further exploration in architectural applications of periodic materials. Full article
(This article belongs to the Special Issue Human Sensing and Artificial Intelligence in Buildings)
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<p>Construction process of experimental environment.</p>
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<p>(<b>a</b>) Rebar spacing constraints of experimental structure (top view), and (<b>b</b>) planned unit cell configuration based on the constraints.</p>
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<p>Vertical arrangement of exciters and sensors in experimental structure for data collection.</p>
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<p>Noise response changes according to the periodic material (PM) application.</p>
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<p>Vibration response changes according to the periodic material (PM) application.</p>
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17 pages, 7168 KiB  
Article
Fast 50 Hz Updated Static Infrared Positioning System Based on Triangulation Method
by Maciej Ciężkowski and Rafał Kociszewski
Sensors 2024, 24(5), 1389; https://doi.org/10.3390/s24051389 - 21 Feb 2024
Cited by 1 | Viewed by 1302
Abstract
One of the important issues being explored in Industry 4.0 is collaborative mobile robots. This collaboration requires precise navigation systems, especially indoor navigation systems where GNSS (Global Navigation Satellite System) cannot be used. To enable the precise localization of robots, different variations of [...] Read more.
One of the important issues being explored in Industry 4.0 is collaborative mobile robots. This collaboration requires precise navigation systems, especially indoor navigation systems where GNSS (Global Navigation Satellite System) cannot be used. To enable the precise localization of robots, different variations of navigation systems are being developed, mainly based on trilateration and triangulation methods. Triangulation systems are distinguished by the fact that they allow for the precise determination of an object’s orientation, which is important for mobile robots. An important feature of positioning systems is the frequency of position updates based on measurements. For most systems, it is 10–20 Hz. In our work, we propose a high-speed 50 Hz positioning system based on the triangulation method with infrared transmitters and receivers. In addition, our system is completely static, i.e., it has no moving/rotating measurement sensors, which makes it more resistant to disturbances (caused by vibrations, wear and tear of components, etc.). In this paper, we describe the principle of the system as well as its design. Finally, we present tests of the built system, which show a beacon bearing accuracy of Δφ = 0.51°, which corresponds to a positioning accuracy of ΔR = 6.55 cm, with a position update frequency of fupdate = 50 Hz. Full article
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<p>The earlier prototype of the Static Triangulation System.</p>
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<p>Principle of the STS triangulation system.</p>
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<p>Receiver photodiode sensitivity vs. Angular displacement.</p>
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<p>Weighted Mean of Angles vs Approximation method comparison.</p>
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<p>Beacon radiation pattern.</p>
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<p>Hardware configuration of the IR beacon transmission system.</p>
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<p>Oscilloscope diagrams of beacon IR diode currents.</p>
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<p>Analog front-end and digital part of the IR receiver.</p>
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<p>Hardware configuration of the IR receiver.</p>
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<p>Laboratory experimental set-up.</p>
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<p>Experimental results for the tripod in position 3.</p>
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15 pages, 3247 KiB  
Article
Design and Experiments of a Convex Curved Surface Type Grain Yield Monitoring System
by Yijun Fang, Zhijian Chen, Luning Wu, Sheikh Muhammad Farhan, Maile Zhou and Jianjun Yin
Electronics 2024, 13(2), 254; https://doi.org/10.3390/electronics13020254 - 5 Jan 2024
Cited by 1 | Viewed by 1191
Abstract
Precision agriculture relies heavily on measuring grain production per unit plot, and a grain flow monitoring system performs this using a combine harvester. In response to the high cost, complex structure, and low stability of the yield monitoring system for grain combine harvesters, [...] Read more.
Precision agriculture relies heavily on measuring grain production per unit plot, and a grain flow monitoring system performs this using a combine harvester. In response to the high cost, complex structure, and low stability of the yield monitoring system for grain combine harvesters, the objective of this research was to design a convex curved grain mass flow sensor to improve the accuracy and practicality of grain yield monitoring. In addition, it involves the development of a grain yield monitoring system based on a cut-and-flow combine harvester prototype. This research examined the real output signal of the convex curved grain mass flow sensor. Errors caused by variations in terrain were reduced by establishing the zero point of the sensor’s output. Measurement errors under different material characteristics, flow rates, and grain types were compared in indoor experiments, and the results were subsequently confirmed through field experiments. The results showed that a sensor with a cantilever beam-type elastic element and a well-constructed carrier plate may achieve a measurement error of less than 5%. After calibrating the sensor’s zero and factors, it demonstrated a measurement error of less than 5% during the operation of the combine harvester. These experimental results align with the expected results and can provide valuable technical support for the widespread adoption of impulse grain flow detection technology. In future work, the impact of factors such as vehicle vibration will be addressed, and system accuracy will be improved through structural design or adaptive filtering processing to promote the commercialization of the system. Full article
(This article belongs to the Special Issue Machine Vision and 3D Sensing in Smart Agriculture)
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<p>Convex Surface Grain Mass Flow Sensor. 1. Bearing plate, 2. Base, 3. Flow guide plate, 4. Frame, 5. Shock absorber, 6. Connecting body, 7. Elastic element.</p>
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<p>Hardware composition diagram. (<b>a</b>) Hardware physical combination diagram. 1. Grain mass flow sensor; 2. Grain yield tester; 3. CPR transmitter. (<b>b</b>) Hardware principal combination diagram.</p>
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<p>System program flowchart.</p>
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<p>Structural diagram of the bearing plate.</p>
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<p>Particle mass flow simulation loading experiment bench. 1. Motor; 2. Small pulley; 3. Large pulley; 4 Stirring cage; 5. Platform; 6. Grain inlet tank; 7. Elevator; 8. Grain outlet device; 9. Flow sensor.</p>
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<p>The working status of sensors in different field environment experiments. (<b>a</b>) The left side is a picture of the wheat experiment scenario, and the right side is a working picture of the system. (<b>b</b>) The left side is a picture of the rice experiment scenario and the right side is a working picture of the system.</p>
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25 pages, 9845 KiB  
Article
A Multi-Sensor Stochastic Energy-Based Vibro-Localization Technique with Byzantine Sensor Elimination
by Murat Ambarkutuk, Sa’ed Alajlouni, Pablo A. Tarazaga and Paul E. Plassmann
Sensors 2023, 23(23), 9309; https://doi.org/10.3390/s23239309 - 21 Nov 2023
Cited by 3 | Viewed by 1123
Abstract
This paper presents an occupant localization technique that determines the location of individuals in indoor environments by analyzing the structural vibrations of the floor caused by their footsteps. Structural vibration waves are difficult to measure as they are influenced by various factors, including [...] Read more.
This paper presents an occupant localization technique that determines the location of individuals in indoor environments by analyzing the structural vibrations of the floor caused by their footsteps. Structural vibration waves are difficult to measure as they are influenced by various factors, including the complex nature of wave propagation in heterogeneous and dispersive media (such as the floor) as well as the inherent noise characteristics of sensors observing the vibration wavefronts. The proposed vibration-based occupant localization technique minimizes the errors that occur during the signal acquisition time. In this process, the likelihood function of each sensor—representing where the occupant likely resides in the environment—is fused to obtain a consensual localization result in a collective manner. In this work, it becomes evident that the above sources of uncertainties can render certain sensors deceptive, commonly referred to as “Byzantines.” Because the ratio of Byzantines among the set sensors defines the success of the collective localization results, this paper introduces a Byzantine sensor elimination (BSE) algorithm to prevent the unreliable information of Byzantine sensors from affecting the location estimations. This algorithm identifies and eliminates sensors that generate erroneous estimates, preventing the influence of these sensors on the overall consensus. To validate and benchmark the proposed technique, a set of previously conducted controlled experiments was employed. The empirical results demonstrate the proposed technique’s significant improvement (3~0%) over the baseline approach in terms of both accuracy and precision. Full article
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<p>Illustration of the localization methodology proposed in this manuscript. Structural vibrations, resulting from the heel-strikes of an occupant, are detected by <span class="html-italic">m</span> accelerometers positioned within the environment. Utilizing the signal energy, denoted as <math display="inline"><semantics> <msub> <mi>e</mi> <mi>i</mi> </msub> </semantics></math>, the distance <math display="inline"><semantics> <msub> <mi>d</mi> <mi>i</mi> </msub> </semantics></math>—established between the sensor <span class="html-italic">i</span> and the occupant—is estimated. Following this, each sensor’s estimation, represented by a PDF, is projected onto the Cartesian localization space, symbolized as <math display="inline"><semantics> <mi mathvariant="script">S</mi> </semantics></math>. The entropies derived from the resultant PDFs play a pivotal role in identifying and subsequently excluding potential Byzantine sensors, employing an iterative sensor fusion approach. Upon achieving a consensus among the sensors, after the exclusion of the Byzantine sensors, the localization process is deemed complete.</p>
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<p>This figure visualizes some key variables frequently used in the paper. The blue and red boxes represent sensor <span class="html-italic">i</span> and sensor <span class="html-italic">j</span> which reside at <math display="inline"><semantics> <msub> <mi mathvariant="bold">t</mi> <mi>i</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi mathvariant="bold">t</mi> <mi>j</mi> </msub> </semantics></math>, respectively. When an occupant excites the floor with their footstep, which occurs at <math display="inline"><semantics> <msub> <mi mathvariant="bold">x</mi> <mrow> <mi>t</mi> <mi>r</mi> <mi>u</mi> <mi>e</mi> </mrow> </msub> </semantics></math>, <span class="html-italic">m</span> accelerometers first estimate <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>i</mi> </msub> <mo>∀</mo> <mrow> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mi>m</mi> </mrow> </mrow> </semantics></math>. Therefore, the estimated location vector of the occupant location by sensor <span class="html-italic">i</span> can be seen as the vector summation of its location vector <math display="inline"><semantics> <msub> <mi mathvariant="bold">t</mi> <mi>i</mi> </msub> </semantics></math> and the estimated <math display="inline"><semantics> <msub> <mi>d</mi> <mi>i</mi> </msub> </semantics></math> for some <math display="inline"><semantics> <msub> <mi>θ</mi> <mi>i</mi> </msub> </semantics></math>.</p>
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<p>The figure displays eight labeled images (<b>a</b>–<b>h</b>) in two rows. The first row depicts individual sensor PDFs: (<b>a</b>) Sensor <span class="html-italic">A</span> with a sharp peak showing high precision; (<b>b</b>) Sensor <span class="html-italic">B</span> with a broader curve showing accuracy and lower precision; (<b>c</b>) Sensor <span class="html-italic">C</span>, a Byzantine sensor with an offset sharp peak; and (<b>d</b>) Sensor <span class="html-italic">D</span> with a flat curve indicating low accuracy and precision. The second row illustrates fusion results: (<b>e</b>) a unimodal curve from sensors <span class="html-italic">A</span> and <span class="html-italic">B</span> showing enhanced precision; (<b>f</b>) a uniform distribution from sensors <span class="html-italic">A</span> and <span class="html-italic">C</span> indicating discord; (<b>g</b>) an offset peak from sensors <span class="html-italic">B</span> and <span class="html-italic">C</span> suggesting an alternative location hypothesis; and (<b>h</b>) a bimodal distribution from sensors <span class="html-italic">C</span> and <span class="html-italic">D</span> with peaks deviating from the true value. The figure highlights the challenges of fusing data from diverse sensors, especially with Byzantine influences.</p>
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<p>The testbed used in the controlled experiments. The green circles represent the unique step locations while the black squares mark the sensor locations used in the experiments.</p>
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<p>The differences between signal (step) detection algorithms employed by the baseline and proposed techniques. The black line (<b>—</b>) represents the noisy measurements of a second-order system. The green dash-dotted line (<span style="color:#39FD42"><b>— -</b></span>) represents the proposed “relaxed” detection results employed in this study. On the other hand, the red dash-dotted line (<span style="color:#F12F0F"><b>— -</b></span>) represents the signal detection algorithm employed by the baseline study.</p>
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<p>Localization outcomes for two distinct occupants using varying sensor counts (<math display="inline"><semantics> <mrow> <mi>m</mi> <mo>=</mo> <mn>2</mn> <mo>,</mo> <mn>6</mn> <mo>,</mo> <mn>11</mn> </mrow> </semantics></math>). The left column represents the first occupant’s result set and the right, the second occupant’s result set. Square markers indicate sensor locations, circles denote non-Byzantine sensors, while green pluses and red crosses symbolize the ground truth and estimated locations, respectively. Errors for configurations (<b>a</b>–<b>e</b>) show progressive refinement with increased sensors, highlighting the algorithm’s adaptability and precision. <b>Left:</b> An illustrative result of the 1st occupant’s data. <b>Right:</b> An illustrative result of the 2nd occupant’s data.</p>
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<p>Quartile analysis of sample localization errors against the number of sensors before the proposed BSE algorithm was employed. The plot showcases a consistent reduction in errors across all quartiles with an increasing number of sensors, highlighting improved consistency in both best- and worst-case scenarios.</p>
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<p>Entropy-based precision of the localization system for varying sensor counts. Red and black lines differentiate data for the first and second occupants. The figure underscores the reduced uncertainty with more sensors, highlighting the enhanced precision across all quartiles.</p>
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<p>Quantile–quantile plot between the precision and accuracy metrics observed in the experimental data. The figure provides evidence for the correlation between precision and accuracy for varying numbers of sensors.</p>
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<p>Empirical PDFs and CDFs of normed localization errors derived from location estimates for both occupants. Solid lines represent the empirical PDFs, with blue and brown indicating the proposed and baseline techniques, respectively. Dash-dotted lines depict the empirical CDFs. The plots demonstrate that the proposed technique generally results in lower localization errors compared to the baseline.</p>
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<p>The error characteristics of the proposed method as a function of the average sensor distance when all sensors were considered.</p>
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<p>The error characteristics of the proposed method as a function of the average sensor distance when a subset of the sensors were considered.</p>
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15 pages, 6737 KiB  
Article
Effects of Microstructure and Chemical Composition on the Visual Characteristics of Flattened Bamboo Board
by Lisheng Chen, Caiping Lian, Meiling Chen and Zhihui Wu
Forests 2023, 14(11), 2220; https://doi.org/10.3390/f14112220 - 10 Nov 2023
Viewed by 1382
Abstract
Flattened bamboo board is a new type of bamboo-based panel with various colors that maintains the natural texture of bamboo, and is gradually being used in indoor home decoration. Revealing the influence mechanism on the visual effect of flattened bamboo boards is the [...] Read more.
Flattened bamboo board is a new type of bamboo-based panel with various colors that maintains the natural texture of bamboo, and is gradually being used in indoor home decoration. Revealing the influence mechanism on the visual effect of flattened bamboo boards is the key to improving the processing of such boards for household materials. This study employed visual physical quantity measurement methods, field emission scanning electron microscopy, FTIR spectroscopy, and XPS to investigate the visual physical quantities, morphology, and chemical composition of flattened bamboo boards. The results showed that compared with the control samples, the bamboo outer layer boards were dark brown, with the largest ΔE* (38.55), while the outer boards were reddish-brown, with the largest a* (8.82). The inner boards were yellow-red and showed a lower ΔE* (6.55). Due to the elevated density, abundant inclusion, and wax, the bamboo outer layer board exhibited the highest glossiness and darkest color, followed by the outer board and the inner board. The FTIR spectroscopy revealed that hemicellulose decomposed, and the relative content of lignin increased, leading to color changes in the flattened bamboo boards. The bamboo outer layer board was the darkest due to changes in C=C bonds at 1600 cm−1 and 1509 cm−1. The surface color of the outer board was mainly red, which may be caused by C–O bonds at 1239 cm−1. The surface of the inner board was mainly yellow, which may be caused by the C–H stretching vibration of lignin at 1108 cm−1. XPS analysis showed that the proportion of C1 and O1 increased, while C2, C3, and O2 decreased, indicating that hemicellulose degraded at high temperatures, which increased the relative lignin content. Changes in the relative content of oxygen-containing functional groups and SiO2 in the flattened bamboo board were important factors responsible for the change in visual physical quantities. Full article
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Figure 1
<p>The appearance of the flattened bamboo boards and natural bamboo. (<b>a</b>) The control samples included bamboo outer layer Ct1, the outer board Ct2, and the inner board Ct3. (<b>b</b>) The flattened bamboo boards included bamboo outer layer board F1, the outer board F2, and the inner board F3.</p>
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<p>The change trend and difference of visual physical quantities between flattened bamboo boards and control samples.</p>
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<p>SEM images of the cross-section of the flattened bamboo boards (<b>a</b>) and control samples (<b>b</b>).</p>
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<p>SEM images of the longitudinal section of the flattened bamboo boards and control samples. (<b>a</b>) The surface of the bamboo outer layer board; (<b>b</b>) enlarged image of (<b>a</b>); (<b>c</b>) the surface characteristics of parenchyma cells in the bamboo outer layer board; (<b>c1</b>,<b>c2</b>) inclusions in the parenchyma cell cavity of the bamboo outer layer board; (<b>d</b>) the surface of the outer board; (<b>e</b>) enlarged image of (<b>d</b>); (<b>f</b>) the surface characteristics of parenchyma cells in the outer board; (<b>f1</b>,<b>f2</b>) inclusions in the parenchyma cell cavity of the outer board; (<b>g</b>) the surface of the inner board; (<b>h</b>) enlarged image of (<b>g</b>); (<b>i</b>) the surface characteristics of parenchyma cells in the inner board; (<b>i1</b>,<b>i2</b>) inclusions in the parenchyma cell cavity of the inner board; and (<b>j</b>–<b>l</b>) the longitudinal characteristics of the control samples. The red arrows refer to inclusions.</p>
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<p>Comparison of FTIR spectra between flattened bamboo boards and control samples on radial surface. (<b>a</b>) Bamboo outer layer board; (<b>b</b>) the outer board; (<b>c</b>) the inner board.</p>
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<p>Comparison of FTIR spectra of three different flattened bamboo boards. (<b>a</b>) Three types of flattened bamboo boards; (<b>b</b>) enlarged image of (<b>a</b>).</p>
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<p>XPS curve of three chemical states of C element in flattened bamboo boards and control samples.</p>
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<p>XPS curve of two chemical states of O element in flattened bamboo boards and control samples.</p>
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15 pages, 3123 KiB  
Article
Research on the Accumulated Pore Pressure of Expansive Soil under Subway Loading
by Lin Qing, Lei Zhu, Ying Guo and Gan Cheng
Buildings 2023, 13(10), 2596; https://doi.org/10.3390/buildings13102596 - 14 Oct 2023
Viewed by 1016
Abstract
Taking the expansive soil near Hefei Xinqiao International Airport as the research subject, indoor dynamic triaxial tests were conducted to investigate the influence of different loading methods on the dynamic pore pressure of saturated remolded expansive soil on the basis of maximally simulating [...] Read more.
Taking the expansive soil near Hefei Xinqiao International Airport as the research subject, indoor dynamic triaxial tests were conducted to investigate the influence of different loading methods on the dynamic pore pressure of saturated remolded expansive soil on the basis of maximally simulating the real characteristics of subway loading. Furthermore, the action laws of three factors, namely intermittent loading ratio, static deviator stress, and cyclic stress ratio, on the accumulated pore pressure of saturated remolded expansive soil under intermittent subway cyclic loading were analyzed. The research results indicate that the loading method significantly affects the development trend of the accumulated pore pressure. Under similar conditions, a larger intermittent loading ratio leads to smaller accumulated pore pressure values and a slower initial development rate of pore pressure under the same cycle vibration. Increasing static deviatoric stress promotes the accumulation of pore pressure. The influence of the cyclic stress ratio is dependent on the intermittent loading ratio and does not follow a consistent pattern. Full article
(This article belongs to the Special Issue Problematic Soils in Building Construction)
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Figure 1
<p>Dynamic triaxial testing system (DYNTTS).</p>
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<p>Samples of undisturbed expansive soil.</p>
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<p>Schematic diagram of continuous cyclic loading waveform in dynamic triaxial test.</p>
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<p>Schematic diagram of intermittent cyclic loading waveform in dynamic triaxial test.</p>
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<p>Time course curve of dynamic pore pressure under continuous loading conditions. (<b>a</b>) Dynamic pore pressure time course curve; and (<b>b</b>) accumulated pore pressure time course curve.</p>
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<p>Time course curve of dynamic pore pressure under intermittent loading conditions. (<b>a</b>) Dynamic pore pressure time course curve; and (<b>b</b>) accumulated pore pressure time course curve.</p>
Full article ">Figure 7
<p>Development curve of accumulated pore pressure with the number of cycles at different intermittent loading ratios. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="sans-serif">η</mi> </mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </msub> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="sans-serif">σ</mi> </mrow> <mrow> <mi mathvariant="normal">s</mi> </mrow> </msub> <mo>=</mo> <mn>15</mn> <mo> </mo> <mi mathvariant="normal">k</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> </mrow> </semantics></math>; and (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="sans-serif">η</mi> </mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </msub> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="sans-serif">σ</mi> </mrow> <mrow> <mi mathvariant="normal">s</mi> </mrow> </msub> <mo>=</mo> <mn>30</mn> <mo> </mo> <mi mathvariant="normal">k</mi> <mi mathvariant="normal">P</mi> <mi mathvariant="normal">a</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>Development curve of accumulated pore pressure with the number of cycles under different static deviator stress. (<b>a</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 1; (<b>b</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 5; (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 10; and (<b>d</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 50.</p>
Full article ">Figure 8 Cont.
<p>Development curve of accumulated pore pressure with the number of cycles under different static deviator stress. (<b>a</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 1; (<b>b</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 5; (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 10; and (<b>d</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 50.</p>
Full article ">Figure 9
<p>Development curve of accumulated pore pressure with the number of cycles at different cyclic stress ratios. (<b>a</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 1, σ<sub>s</sub> = 15 kPa; (<b>b</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 1, σ<sub>s</sub> = 30 kPa; (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 5, σ<sub>s</sub> = 15 kPa; (<b>d</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 5, σ<sub>s</sub> = 30 kPa; (<b>e</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 10, σ<sub>s</sub> = 15 kPa; (<b>f</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 10, σ<sub>s</sub> = 30 kPa; (<b>g</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 50, σ<sub>s</sub> = 15 kPa; and (<b>h</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 50, σ<sub>s</sub> = 30 kPa.</p>
Full article ">Figure 9 Cont.
<p>Development curve of accumulated pore pressure with the number of cycles at different cyclic stress ratios. (<b>a</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 1, σ<sub>s</sub> = 15 kPa; (<b>b</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 1, σ<sub>s</sub> = 30 kPa; (<b>c</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 5, σ<sub>s</sub> = 15 kPa; (<b>d</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 5, σ<sub>s</sub> = 30 kPa; (<b>e</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 10, σ<sub>s</sub> = 15 kPa; (<b>f</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 10, σ<sub>s</sub> = 30 kPa; (<b>g</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 50, σ<sub>s</sub> = 15 kPa; and (<b>h</b>) <math display="inline"><semantics> <mrow> <mo>∆</mo> <mi>T</mi> <mo>/</mo> <mi>T</mi> </mrow> </semantics></math> = 50, σ<sub>s</sub> = 30 kPa.</p>
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