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Appl. Sci., Volume 13, Issue 4 (February-2 2023) – 725 articles

Cover Story (view full-size image): Growing consumer demand for high-quality products coupled with minimally processed products and minor use of synthetic food additives have increased the need to search for new sources of natural antimicrobials to ensure product safety. This study aimed to evaluate the antimicrobial activity of extracts from the brown algae Ericaria selaginoides against Bacillus cereus in typical Catalan fresh cheese (“mató”) by means of testing. Three concentrations of a crude extract and its corresponding two subfractions (non-polar and mid-polar) obtained after purification showed an antimicrobial dose-dependent effect on B. cereus, from inhibition to inactivation. The results showed an improvement in the antimicrobial effect after purification compared with the effect observed when the crude extract was tested. Moreover, compounds of different chemical natures may be involved in this antimicrobial. View this paper
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23 pages, 6339 KiB  
Article
A Novel Deep Reinforcement Learning Approach to Traffic Signal Control with Connected Vehicles
by Yang Shi, Zhenbo Wang, Tim J. LaClair, Chieh (Ross) Wang, Yunli Shao and Jinghui Yuan
Appl. Sci. 2023, 13(4), 2750; https://doi.org/10.3390/app13042750 - 20 Feb 2023
Cited by 8 | Viewed by 4611
Abstract
The advent of connected vehicle (CV) technology offers new possibilities for a revolution in future transportation systems. With the availability of real-time traffic data from CVs, it is possible to more effectively optimize traffic signals to reduce congestion, increase fuel efficiency, and enhance [...] Read more.
The advent of connected vehicle (CV) technology offers new possibilities for a revolution in future transportation systems. With the availability of real-time traffic data from CVs, it is possible to more effectively optimize traffic signals to reduce congestion, increase fuel efficiency, and enhance road safety. The success of CV-based signal control depends on an accurate and computationally efficient model that accounts for the stochastic and nonlinear nature of the traffic flow. Without the necessity of prior knowledge of the traffic system’s model architecture, reinforcement learning (RL) is a promising tool to acquire the control policy through observing the transition of the traffic states. In this paper, we propose a novel data-driven traffic signal control method that leverages the latest in deep learning and reinforcement learning techniques. By incorporating a compressed representation of the traffic states, the proposed method overcomes the limitations of the existing methods in defining the action space to include more practical and flexible signal phases. The simulation results demonstrate the convergence and robust performance of the proposed method against several existing benchmark methods in terms of average vehicle speeds, queue length, wait time, and traffic density. Full article
(This article belongs to the Special Issue Transportation Planning, Management and Optimization)
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<p>Proposed data-driven optimization framework for traffic signal control.</p>
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<p>The simulated intersection.</p>
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<p>An example of traffic state matrix.</p>
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<p>A typical signal cycle with four phases.</p>
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<p>The structure of the proposed convolutional autoencoder (CAE) for traffic state representation.</p>
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<p>Training history of the proposed convolutional autoencoder.</p>
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<p>Proposed deep reinforcement learning model.</p>
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<p>Convergence of the proposed DRL network.</p>
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<p>Training history of a reference DRL-based traffic signal controller.</p>
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<p>Performance comparisons with baselines.</p>
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<p>Simulation comparisons with baselines.</p>
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<p>Performance estimation of the proposed method in each lane.</p>
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<p>Traffic flow simulated by the proposed method in each lane.</p>
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<p>Traffic flow simulated by the referenced method in each lane.</p>
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<p>Simulation comparisons with the DRL-based controller trained using symmetric SPaT.</p>
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<p>Robustness analysis by comparing the performance of DRL-based controller.</p>
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17 pages, 537 KiB  
Article
Estimating the Energy Savings of Energy Efficiency Actions with Ensemble Machine Learning Models
by Elissaios Sarmas, Evangelos Spiliotis, Nikos Dimitropoulos, Vangelis Marinakis and Haris Doukas
Appl. Sci. 2023, 13(4), 2749; https://doi.org/10.3390/app13042749 - 20 Feb 2023
Cited by 13 | Viewed by 2445
Abstract
Energy efficiency financing is considered among the top priorities in the energy sector among several stakeholders. In this context, accurately estimating the energy savings achieved by energy efficiency actions before being approved and implemented is of major importance to ensure the optimal allocation [...] Read more.
Energy efficiency financing is considered among the top priorities in the energy sector among several stakeholders. In this context, accurately estimating the energy savings achieved by energy efficiency actions before being approved and implemented is of major importance to ensure the optimal allocation of the available financial resources. This study aims to provide a machine-learningbased methodological framework for a priori predicting the energy savings of energy efficiency renovation actions. The proposed solution consists of three tree-based algorithms that exploit bagging and boosting as well as an additional ensembling level that further mitigates prediction uncertainty. The proposed models are empirically evaluated using a database of various, diverse energy efficiency renovation investments. Results indicate that the ensemble model outperforms the three individual models in terms of forecasting accuracy. Also, the generated predictions are relatively accurate for all the examined project categories, a finding that supports the robustness of the proposed approach. Full article
(This article belongs to the Section Energy Science and Technology)
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<p>The structure of the random forest algorithm, which is based on bootstrap aggregating (or bagging) the predictions of multiple decision tree models.</p>
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<p>The general structure of the gradient boosting algorithm, which is based on boosting the predictions of multiple decision tree models.</p>
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<p>Comparative analysis of the 8 investment categories in terms of cost, energy savings, and investment efficiency (defined as investment cost per energy savings). (<b>a</b>) Investment cost per category. (<b>b</b>) Energy savings per category. (<b>c</b>) Investment efficiency per category.</p>
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<p>Structure of the experimental application.</p>
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<p>Scatter plot visualization of the real and the predicted values based on the EW ensemble model for the EE renovation projects of the test set.</p>
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17 pages, 3162 KiB  
Article
Visual Exploration of Cycling Semantics with GPS Trajectory Data
by Xuansu Gao, Chengwu Liao, Chao Chen and Ruiyuan Li
Appl. Sci. 2023, 13(4), 2748; https://doi.org/10.3390/app13042748 - 20 Feb 2023
Cited by 3 | Viewed by 2262
Abstract
Cycling—as a sustainable and convenient exercise and travel mode—has become increasingly popular in modern cities. In recent years, with the proliferation of sport apps and GPS mobile devices in daily life, the accumulated cycling trajectories have opened up valuable opportunities to explore the [...] Read more.
Cycling—as a sustainable and convenient exercise and travel mode—has become increasingly popular in modern cities. In recent years, with the proliferation of sport apps and GPS mobile devices in daily life, the accumulated cycling trajectories have opened up valuable opportunities to explore the underlying cycling semantics to enable a better cycling experience. In this paper, based on large-scale GPS trajectories and road network data, we mainly explore cycling semantics from two perspectives. On one hand, from the perspective of the cyclists, trajectories could tell their frequently visited sequences of streets, thus potentially revealing their hidden cycling themes, i.e., cyclist behavior semantics. On the other hand, from the perspective of the road segments, trajectories could show the cyclists’ fine-grained moving features along roads, thus probably uncovering the moving semantics on roads. However, the extraction and understanding of such cycling semantics are nontrivial, since most of the trajectories are raw data and it is also difficult to aggregate the dynamic moving features from trajectories into static road segments. To this end, we establish a new visual analytic system called VizCycSemantics for pervasive computing, in which a topic model (i.e., LDA) is used to extract the topics of cyclist behavior semantics and moving semantics on roads, and a clustering method (i.e., k-means ++) is used to further capture the groups of similar cyclists and road segments within the city; finally, multiple interactive visual interfaces are implemented to facilitate the interpretation for analysts. We conduct extensive case studies in the city of Beijing to demonstrate the effectiveness and practicability of our system and also obtain various insightful findings and pieces of advice. Full article
(This article belongs to the Special Issue New Insights into Pervasive and Mobile Computing)
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<p>Overview of the system framework.</p>
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<p>Workflow of backend algorithms.</p>
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<p>The processes of trajectory data transformation. (<b>a</b>) Textualization for trajectories to street names. (<b>b</b>) Textualization for moving features.</p>
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<p>Illustration of heading direction and turning angle calculation.</p>
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<p>The interfaces of VizCycSemantics system. (<b>a</b>) Cycling map. (<b>b</b>) Cycling groups and topics. (<b>c</b>) Size of cycling groups. (<b>d</b>) Street cloud of cycling topics. (<b>e</b>) Temporal evolution of cycling topics. (<b>f</b>) Moving topic distribution. (<b>g</b>) Moving topics.</p>
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<p>(<b>a</b>) Cycling groups and topics. (<b>b</b>) Street cloud of cycling topics. (<b>c</b>) Size of cycling groups. (<b>d</b>) Temporal evolution of cycling topics at different time granularity values.</p>
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<p>(<b>a</b>,<b>b</b>) Topics of recreational cycling distributed on the map. (<b>c</b>,<b>d</b>) Topics of connected cycling distributed on the map. (<b>e</b>–<b>i</b>) Topics of daily commuting cycling distributed on the map. (<b>j</b>) Topic of exercising cycling distributed on the map.</p>
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<p>Moving semantics profiling. (<b>a</b>) The most important topics of velocity. (<b>b</b>) The most important topics of acceleration. (<b>c</b>) The most important topics of turning angle. (<b>d</b>) The topic distribution of a selected road segment. (<b>e</b>,<b>f</b>) Grouping of road segments with velocity, acceleration and turning angle in two local areas, respectively.</p>
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<p>The grouping of moving attributes and the corresponding inference and suggestion.</p>
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11 pages, 6856 KiB  
Communication
Robot Assisted THz Imaging with a Time Domain Spectrometer
by Dominik Bachmann, Rolf Brönnimann, Luis Nicklaus Caceres, Sofie L. Gnannt, Erwin Hack, Elena Mavrona, Daniel Sacré and Peter Zolliker
Appl. Sci. 2023, 13(4), 2747; https://doi.org/10.3390/app13042747 - 20 Feb 2023
Cited by 2 | Viewed by 1917
Abstract
THz-Time domain spectroscopic imaging is demonstrated combining a robotic scanning method with continuous signal acquisition and holographic reconstruction of the object to improve the imaging resolution. We apply the method to a metallic Siemens star in order to quantify resolution and to wood [...] Read more.
THz-Time domain spectroscopic imaging is demonstrated combining a robotic scanning method with continuous signal acquisition and holographic reconstruction of the object to improve the imaging resolution. We apply the method to a metallic Siemens star in order to quantify resolution and to wood samples to demonstrate the technique on a non-metallic object with an unknown structure. Full article
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<p>Schematic representation of the THz-TDS setup for measurements using a robot arm for sample scanning (PM: off-axis parabolic mirror, P1, P2: polarizer).</p>
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<p>Synchronization using timestamps of TDS and robot: (<b>a</b>) a scan speed of 5 <math display="inline"><semantics> <mi mathvariant="normal">m</mi> </semantics></math><math display="inline"><semantics> <mi mathvariant="normal">m</mi> </semantics></math>/<math display="inline"><semantics> <mi mathvariant="normal">s</mi> </semantics></math> and a total scanning time of 6 <math display="inline"><semantics> <mi>min</mi> </semantics></math>; (<b>b</b>) a scan speed of 2 <math display="inline"><semantics> <mi mathvariant="normal">m</mi> </semantics></math><math display="inline"><semantics> <mi mathvariant="normal">m</mi> </semantics></math>/<math display="inline"><semantics> <mi mathvariant="normal">s</mi> </semantics></math> and a total scanning time of 20 <math display="inline"><semantics> <mi>min</mi> </semantics></math>.</p>
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<p>Resolution sample (<b>left</b>), wood sample #1; LR spruce (<b>middle</b>), wood sample #2; RT spruce from branch (<b>right</b>), scale in cm; wood directions R, T, and L are shown in the figure.</p>
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<p>Simulation scheme of TDS experiments (not to scale).</p>
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<p>Resolution target images without mask for selected frequencies. Measurement (top) and simulation (bottom); (<b>a</b>) 0.5 THz; (<b>b</b>) 1.0 THz; (<b>c</b>) 1.5 THz; (<b>d</b>) 2.0 THz.</p>
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<p>Resolution target images for selected frequencies taken with a 0.5 mm mask at a distance of 0.5 mm. Measurement (top row) and simulation (bottom row): (<b>a</b>) 0.5 THz; (<b>b</b>) 1.0 THz; (<b>c</b>) 1.5 THz; (<b>d</b>) 2.0 THz.</p>
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<p>Resolution target images at distance <math display="inline"><semantics> <mrow> <mo>Δ</mo> <mi>z</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math> mm from mask: measurement: (first row), and simulations (second row); holographic reconstruction of measurements (third row) and holographic reconstruction of simulations (fourth row); (<b>a</b>) 0.5 THz; (<b>b</b>) 1.0 THz; (<b>c</b>) 1.5 THz; (<b>d</b>) 2.0 THz.</p>
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<p>Intensity (gray scale) and phase images (color scale) of the wood sample #1. Sample orientation of annual rings with respect to polarization: <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <msup> <mn>0</mn> <mo>∘</mo> </msup> </mrow> </semantics></math> (top two rows) and <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <msup> <mn>90</mn> <mo>∘</mo> </msup> </mrow> </semantics></math> (bottom two rows): (<b>a</b>) 0.5 THz; (<b>b</b>) 1.0 THz; (<b>c</b>) 1.5 THz; (<b>d</b>) 2.0 THz.</p>
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<p>Intensity (top row) and phase images (bottom row) at 0.5 THz for wood sample #2 for measurements at different polarizer orientations [<math display="inline"><semantics> <msub> <mi>P</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>P</mi> <mn>2</mn> </msub> </semantics></math>]: (<b>a</b>) [<math display="inline"><semantics> <msup> <mn>45</mn> <mo>∘</mo> </msup> </semantics></math>, <math display="inline"><semantics> <msup> <mn>45</mn> <mo>∘</mo> </msup> </semantics></math>]; (<b>b</b>) [<math display="inline"><semantics> <msup> <mn>135</mn> <mo>∘</mo> </msup> </semantics></math>, <math display="inline"><semantics> <msup> <mn>135</mn> <mo>∘</mo> </msup> </semantics></math>]; (<b>c</b>) [<math display="inline"><semantics> <msup> <mn>135</mn> <mo>∘</mo> </msup> </semantics></math>, <math display="inline"><semantics> <msup> <mn>45</mn> <mo>∘</mo> </msup> </semantics></math>]; (<b>d</b>) [<math display="inline"><semantics> <msup> <mn>45</mn> <mo>∘</mo> </msup> </semantics></math>, <math display="inline"><semantics> <msup> <mn>135</mn> <mo>∘</mo> </msup> </semantics></math>].</p>
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15 pages, 4411 KiB  
Article
Underwater Object Detection Method Based on Improved Faster RCNN
by Hao Wang and Nanfeng Xiao
Appl. Sci. 2023, 13(4), 2746; https://doi.org/10.3390/app13042746 - 20 Feb 2023
Cited by 29 | Viewed by 4746
Abstract
In order to better utilize and protect marine organisms, reliable underwater object detection methods need to be developed. Due to various influencing factors from complex and changeable underwater environments, the underwater object detection is full of challenges. Therefore, this paper improves a two-stage [...] Read more.
In order to better utilize and protect marine organisms, reliable underwater object detection methods need to be developed. Due to various influencing factors from complex and changeable underwater environments, the underwater object detection is full of challenges. Therefore, this paper improves a two-stage algorithm of Faster RCNN (Regions with Convolutional Neural Network Feature) to detect holothurian, echinus, scallop, starfish and waterweeds. The improved algorithm has better performance in underwater object detection. Firstly, we improved the backbone network of the Faster RCNN, replacing the VGG16 (Visual Geometry Group Network 16) structure in the original feature extraction module with the Res2Net101 network to enhance the expressive ability of the receptive field of each network layer. Secondly, the OHEM (Online Hard Example Mining) algorithm is introduced to solve the imbalance problem of positive and negative samples of the bounding box. Thirdly, GIOU (Generalized Intersection Over Union) and Soft-NMS (Soft Non-Maximum Suppression) are used to optimize the regression mechanism of the bounding box. Finally, the improved Faster RCNN model is trained using a multi-scale training strategy to enhance the robustness of the model. Through ablation experiments based on the improved Faster RCNN model, each improved part is disassembled and then the experiments are carried out one by one, which can be known from the experimental results that, based on the improved Faster RCNN model, [email protected] reaches 71.7%, which is 3.3% higher than the original Faster RCNN model, and the average accuracy reaches 43%, and the F1-score reaches 55.3%, a 2.5% improvement over the original Faster RCNN model, which shows that the proposed method in this paper is effective in underwater object detection. Full article
(This article belongs to the Section Robotics and Automation)
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<p>Network structure diagram of the Faster RCNN.</p>
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<p>The network structure of the improved Faster RCNN.</p>
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<p>The effect of dataset preprocessing.</p>
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<p>Mosaic data enhancement, (<b>a</b>) four randomly entered pictures (from left to right, they are respectively a starfish, water plants, a scallop, a sea cucumber), (<b>b</b>) data augmentation results.</p>
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<p>Results of different methods for underwater object detection. (<b>a</b>–<b>e</b>) are respectively the detection results based on Fast RCNN, Faster RCNN, YOLOV3, SSD, the improved Faster RCNN. The black creatures are sea cucumbers, the blue five-pointed creatures are starfishes, the green round creatures are scallops, and the black slander creatures are seaweeds in the images.</p>
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<p>The precision-recall curves.</p>
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<p>Underwater detection results between the Faster RCNN and our method.</p>
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25 pages, 12305 KiB  
Article
Evaluation of Engineering Site and Subsurface Structures Using Seismic Refraction Tomography: A Case Study of Abydos Site, Sohag Governorate, Egypt
by Abdelbaset M. Abudeif, Gamal Z. Abdel Aal, Nessreen F. Abdelbaky, Ahmed M. Abdel Gowad and Mohammed A. Mohammed
Appl. Sci. 2023, 13(4), 2745; https://doi.org/10.3390/app13042745 - 20 Feb 2023
Cited by 2 | Viewed by 2712
Abstract
Because of the strategic importance of the Abydos archaeological site in Egypt as a source of wealth for Egyptian tourism, this study was concerned with carrying out geophysical measurements to detect subsurface succession and measure variations in the geotechnical engineering features of the [...] Read more.
Because of the strategic importance of the Abydos archaeological site in Egypt as a source of wealth for Egyptian tourism, this study was concerned with carrying out geophysical measurements to detect subsurface succession and measure variations in the geotechnical engineering features of the soils/rocks in order to protect this significant area. The findings will assist geologists and seismologists in collaborating with archaeologists for future site development, revitalization, and investment. The primary objectives of this work were to determine the subsurface lithology, evaluate the engineering geotechnical properties of soils/rocks, identify the layer thicknesses, and identify the site class by calculating Vs30. To achieve these goals, seventeen (17) seismic refraction tomography (SRT) P- and S-wave measurements were executed in front of the Osirion location. SeisImager Software was used for the processing and interpretation of the outcomes. The results were the travel time–distance curves, which were used for building the 2D seismic models that exhibited the velocity and the depth of the layered models. These models were validated by our previous works using electric resistivity tomography and borehole data. The results indicated that this site consisted of three geoseismic subsurface layers. The first layer was the surface that was made up of wadi deposits, which were a mixture of gravel, sand, and silt and were characterized by incompetent to slightly competent materials. The second layer corresponded to the sand and muddy sand deposits of competent rock that was of fair to moderate quality. The third layer (clay deposits) had a higher velocity and was more compact and may be employed as a bedrock layer. The elastic moduli, Vs30, petrophysical, and geotechnical properties of the three geoseismic layers were appraised as essential parameters. Integration of petrophysical and geotechnical parameters and elastic moduli revealed that the third layer was composed of competent clays, which were characterized by low values of porosity, void ratio, Poisson ratio, and stress ratio. It also had a high rigidity, Young’s and bulk moduli, concentration and material indexes, N-value, ultimate bearing capacities, and high density values, and vice versa for the first layer. The standard NEHRP site class was B (rocks). These parameters are ordinarily used as key indications and serve as significant inputs for any future work. Full article
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<p>Location map for the Abydos site, with (<b>a</b>) a map of Egypt and (<b>b</b>) a more comprehensive map of the Abydos temple that depicts the Osirion site and nearby boreholes.</p>
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<p>(<b>A</b>) A geological map of the Sohag district, including the investigated area, emphasizing the major surface geologic units and a cross-section through the study site passing by the Osirion location [<a href="#B14-applsci-13-02745" class="html-bibr">14</a>]. (<b>B</b>) From the three drilled wells (1, 2, and 3) that were situated in the research site, the stratigraphic sequence west of the Abydos area was determined [<a href="#B18-applsci-13-02745" class="html-bibr">18</a>].</p>
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<p>The configuration of the seismic refraction lines for P- and S-waves in the current investigation.</p>
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<p>Examples of the obtained picked refraction seismic data for profile 1, which involved two segments. In segment 1, there was (<b>A</b>) a P-wave shooting forward at a distance of −2.5 m, (<b>B</b>) a P-wave shooting at the mid-point between geophones 6 and 7 at a distance of 27.5 m, (<b>C</b>) a P-wave shooting at the mid-point of the profile at a distance of 57.5 m, (<b>D</b>) a P-wave shooting at the mid-point between geophones 18 and 19 at a distance of 87.5 m, and (<b>E</b>) a P-wave shooting at a distance of 117.5 m. In segment 2, there was (<b>F</b>) a P-wave shooting forward at a distance of 82.5 m, (<b>G</b>) a P-wave shooting at a distance of 112.5 m, (<b>H</b>) a P-wave shooting at a distance of 142.5 m, (<b>I</b>) a P-wave shooting at a distance of 172.5 m, and (<b>J</b>) a P-wave shooting at a distance of 202.5 m.</p>
Full article ">Figure 4 Cont.
<p>Examples of the obtained picked refraction seismic data for profile 1, which involved two segments. In segment 1, there was (<b>A</b>) a P-wave shooting forward at a distance of −2.5 m, (<b>B</b>) a P-wave shooting at the mid-point between geophones 6 and 7 at a distance of 27.5 m, (<b>C</b>) a P-wave shooting at the mid-point of the profile at a distance of 57.5 m, (<b>D</b>) a P-wave shooting at the mid-point between geophones 18 and 19 at a distance of 87.5 m, and (<b>E</b>) a P-wave shooting at a distance of 117.5 m. In segment 2, there was (<b>F</b>) a P-wave shooting forward at a distance of 82.5 m, (<b>G</b>) a P-wave shooting at a distance of 112.5 m, (<b>H</b>) a P-wave shooting at a distance of 142.5 m, (<b>I</b>) a P-wave shooting at a distance of 172.5 m, and (<b>J</b>) a P-wave shooting at a distance of 202.5 m.</p>
Full article ">Figure 4 Cont.
<p>Examples of the obtained picked refraction seismic data for profile 1, which involved two segments. In segment 1, there was (<b>A</b>) a P-wave shooting forward at a distance of −2.5 m, (<b>B</b>) a P-wave shooting at the mid-point between geophones 6 and 7 at a distance of 27.5 m, (<b>C</b>) a P-wave shooting at the mid-point of the profile at a distance of 57.5 m, (<b>D</b>) a P-wave shooting at the mid-point between geophones 18 and 19 at a distance of 87.5 m, and (<b>E</b>) a P-wave shooting at a distance of 117.5 m. In segment 2, there was (<b>F</b>) a P-wave shooting forward at a distance of 82.5 m, (<b>G</b>) a P-wave shooting at a distance of 112.5 m, (<b>H</b>) a P-wave shooting at a distance of 142.5 m, (<b>I</b>) a P-wave shooting at a distance of 172.5 m, and (<b>J</b>) a P-wave shooting at a distance of 202.5 m.</p>
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<p>The observed and calculated travel time–distance curves of the seismic refraction profile 1 (<b>A</b>) for the P-wave and (<b>B</b>) for the S-wave.</p>
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<p>Example of the seismic refraction profile 1: (<b>A</b>) travel time–distance curve derived from the P-wave profile; (<b>B</b>) 2D depth–velocity model derived from P-wave profile; (<b>C</b>) travel time–distance curve derived from the S-wave profile; and (<b>D</b>) 2D depth–velocity model derived from the S-wave profile.</p>
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<p>The 2D depth–velocity models for the P-wave and associated S-wave profiles along the NW–SE direction were produced.</p>
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<p>The 2D depth–velocity models for the P-wave and associated S-wave profiles along the NW–SE and SW–NE directions were produced.</p>
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<p>The 2D depth–velocity models for the P-wave and associated S-wave profiles along the NW–SE and SW–NE directions were produced.</p>
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<p>The 2D electrical resistivity model of profile 1. This model emphasized the distinctive geoelectric zones that were identified using the borehole and resistivity data that were available and it also showed the depth of the groundwater level.</p>
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<p>(<b>A</b>) Three-dimensional fence diagrams depicting the velocity variations for the P-wave and (<b>B</b>) S-wave along the surveyed profiles. The three interpreted geoseismic layers are shown in this figure. They were all differentiated using the vertical and horizontal velocity distributions.</p>
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<p>Zonation maps showing the spatial variation of seismic P- and S-wave velocities for three layers along the study site, as shown in the (<b>a</b>) V<sub>p</sub> of the first layer, (<b>b</b>) V<sub>p</sub> of the second layer, (<b>c</b>) V<sub>p</sub> of the third layer, (<b>d</b>) V<sub>s</sub> of the first layer, (<b>e</b>) V<sub>s</sub> of the second layer, and (<b>f</b>) V<sub>s</sub> of the third layer.</p>
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<p>The depths to the top of the second (<b>a</b>) and third (<b>b</b>) layers are depicted on a shaded color relief map using the seismic results.</p>
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17 pages, 10440 KiB  
Article
Gap and Force Adjustment during Laser Beam Welding by Means of a Closed-Loop Control Utilizing Fixture-Integrated Sensors and Actuators
by Klaus Schricker, Leander Schmidt, Hannes Friedmann and Jean Pierre Bergmann
Appl. Sci. 2023, 13(4), 2744; https://doi.org/10.3390/app13042744 - 20 Feb 2023
Cited by 3 | Viewed by 2667
Abstract
The development of adaptive and intelligent clamping devices allows for the reduction of rejects and defects based on weld discontinuities in laser-beam welding. The utilization of fixture-integrated sensors and actuators is a new approach, realizing adaptive clamping devices that enable in-process data acquisition [...] Read more.
The development of adaptive and intelligent clamping devices allows for the reduction of rejects and defects based on weld discontinuities in laser-beam welding. The utilization of fixture-integrated sensors and actuators is a new approach, realizing adaptive clamping devices that enable in-process data acquisition and a time-dependent adjustment of process conditions and workpiece position by means of a closed-loop control. The present work focused on sensor and actuator integration for an adaptive clamping device utilized for laser-beam welding in a butt-joint configuration, in which the position and acting forces of the sheets to be welded can be adjusted during the process (studied welding speeds: 1 m/min, 5 m/min). Therefore, a novel clamping system was designed allowing for the integration of inductive probes and force cells for obtaining time-dependent data of the joint gap and resulting forces during welding due to the displacement of the sheets. A novel automation engineering concept allowed the communication between different sensors, actuators and the laser-beam welding setup based on an EtherCAT bus. The subsequent development of a position control and a force control and their combination was operated with a real time PC as master in the bus system and proved the feasibility of the approach based on proportional controllers. Finally, the scalability regarding higher welding speeds was demonstrated. Full article
(This article belongs to the Special Issue Laser Material Processing and Thermal Joining Process)
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<p>Schematic figure of the clamping situation and position of sensors and actuators (dimensions in millimeter): (<b>a</b>) Gap measurement via inductive probes IP1-3; (<b>b</b>) Linear actuators LA1-2 and force measurement via load cells LC1-2.</p>
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<p>Design of the adaptive clamping device in perspective and top view.</p>
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<p>Design details for integration of inductive probes and linear actuators and load cells (half section view).</p>
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<p>Realization of adaptive clamping device in laser welding setup (housings of load cells and actuators removed).</p>
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<p>Schematic figure of the bus system for sensor and actuator integration.</p>
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<p>Realized control cabinet for sensor and actuator integration and control in testing mode.</p>
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<p>Top view of an uncontrolled weld with unhindered gap formation (v<sub>w</sub> = 1 m/min, P<sub>L</sub> = 0.4 kW).</p>
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<p>Unhindered gap formation (v<sub>w</sub> = 1 m/min, P<sub>L</sub> = 0.4 kW): (<b>a</b>) Gap measurement via inductive probes; (<b>b</b>) High-speed recording of sheet edges at the end of the specimen at different times.</p>
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<p>Force measurement of a rigid clamping for an uncontrolled process (v<sub>w</sub> = 1 m/min, P<sub>L</sub> = 0.4 kW).</p>
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<p>Closed-loop position control.</p>
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<p>Closed-loop position control (v<sub>w</sub> = 1 m/min, P<sub>L</sub> = 0.4 kW): (<b>a</b>) Gap measurement via inductive probes; (<b>b</b>) Force measurement via load cells.</p>
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<p>Closed-loop force control.</p>
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<p>Closed-loop compression force control (v<sub>w</sub> = 1 m/min, P<sub>L</sub> = 0.4 kW): (<b>a</b>) unhindered gap formation; (<b>b</b>) setpoint value 0 N; (<b>c</b>) setpoint value −30 N; and (<b>d</b>) setpoint value −75 N.</p>
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<p>Closed-loop force-position control.</p>
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<p>Closed-loop force-position control (v<sub>w</sub> = 1 m/min, P<sub>L</sub> = 0.4 kW): (<b>a</b>) gap measurement via inductive probes; and (<b>b</b>) force measurement via load cells.</p>
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<p>Comparison of maximum gap width for unhindered gap formation and force-controlled process at 1 m/min and 5 m/min welding speed and examples of weld seams.</p>
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<p>Closed-loop force-position control (v<sub>w</sub> = 5 m/min, P<sub>L</sub> = 1.0 kW): (<b>a</b>) gap measurement via inductive probes; and (<b>b</b>) force measurement via load cells.</p>
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19 pages, 1852 KiB  
Review
A Comprehensive Review of Conventional, Machine Leaning, and Deep Learning Models for Groundwater Level (GWL) Forecasting
by Junaid Khan, Eunkyu Lee, Awatef Salem Balobaid and Kyungsup Kim
Appl. Sci. 2023, 13(4), 2743; https://doi.org/10.3390/app13042743 - 20 Feb 2023
Cited by 38 | Viewed by 4544
Abstract
Groundwater level (GWL) refers to the depth of the water table or the level of water below the Earth’s surface in underground formations. It is an important factor in managing and sustaining the groundwater resources that are used for drinking water, irrigation, and [...] Read more.
Groundwater level (GWL) refers to the depth of the water table or the level of water below the Earth’s surface in underground formations. It is an important factor in managing and sustaining the groundwater resources that are used for drinking water, irrigation, and other purposes. Groundwater level prediction is a critical aspect of water resource management and requires accurate and efficient modelling techniques. This study reviews the most commonly used conventional numerical, machine learning, and deep learning models for predicting GWL. Significant advancements have been made in terms of prediction efficiency over the last two decades. However, while researchers have primarily focused on predicting monthly, weekly, daily, and hourly GWL, water managers and strategists require multi-year GWL simulations to take effective steps towards ensuring the sustainable supply of groundwater. In this paper, we consider a collection of state-of-the-art theories to develop and design a novel methodology and improve modelling efficiency in this field of evaluation. We examined 109 research articles published from 2008 to 2022 that investigated different modelling techniques. Finally, we concluded that machine learning and deep learning approaches are efficient for modelling GWL. Moreover, we provide possible future research directions and recommendations to enhance the accuracy of GWL prediction models and improve relevant understanding. Full article
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<p>Arithmetic conceptualization of GWL research using AI-based model during 2008–2022.</p>
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<p>Relevant and irrelevant papers selection process.</p>
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<p>Groundwater prediction process.</p>
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<p>Different kinds of data used for prediction of GWL.</p>
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<p>A basic architecture of ANFIS model.</p>
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<p>Graphical representation of Bi-LSTM.</p>
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12 pages, 1080 KiB  
Article
The Temperature Interval of the Liquid–Glass Transition of Amorphous Polymers and Low Molecular Weight Amorphous Substances
by Migmar V. Darmaev, Michael I. Ojovan, Alexey A. Mashanov and Timur A. Chimytov
Appl. Sci. 2023, 13(4), 2742; https://doi.org/10.3390/app13042742 - 20 Feb 2023
Cited by 3 | Viewed by 2001
Abstract
We present calculation results of the temperature interval δTg characterizing the liquid–glass transition in amorphous materials obtained on the basis of available data of the empirical parameters C1 and C2 in the Williams–Landel–Ferry (WLF) viscosity equation. We consider the unambiguous [...] Read more.
We present calculation results of the temperature interval δTg characterizing the liquid–glass transition in amorphous materials obtained on the basis of available data of the empirical parameters C1 and C2 in the Williams–Landel–Ferry (WLF) viscosity equation. We consider the unambiguous dependence of the relative transition temperature interval δTg/Tg on the fraction of the fluctuation volume fg frozen at the glass transition temperature Tg utilizing Sanditov’s model of delocalized atoms. The parameter f = ΔVe/V, which determines the molecular mobility characteristic of delocalized atoms in the liquid–glass transition region, is weakly dependent on the nature of most vitreous substances and can be found as fg = 1/C1. We show that the temperature interval δTg is less than 1% of the Tg for most amorphous substances. This result conforms with Simon’s classical idea of a small temperature range in which the structure freezes. The structural relaxation time τg at Tg of polymers and chalcogenide glasses is also calculated. Full article
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<p>Temperature dependence of the viscosity of As-S glasses in coordinates corresponding to the Williams–Landel–Ferry equation. The data of [<a href="#B18-applsci-13-02742" class="html-bibr">18</a>] were used where the composition is as follows: As—32.5 mol%; S—67.5 mol%.</p>
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<p>Linear correlation between the temperature interval <span class="html-italic">δT<sub>g</sub></span> characterizing the glass transition range and the glass transition temperature <span class="html-italic">T<sub>g</sub></span> of glasses in the As-S system. The point numbers correspond to the glass order numbers in <a href="#applsci-13-02742-t001" class="html-table">Table 1</a>.</p>
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<p>Linear correlation between <span class="html-italic">δT<sub>g</sub></span> and <span class="html-italic">T<sub>g</sub></span> for Se-Ge glasses. The point numbers correspond to the glass order numbers in <a href="#applsci-13-02742-t001" class="html-table">Table 1</a>.</p>
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<p>Correlation between <span class="html-italic">δT<sub>g</sub></span> and <span class="html-italic">T<sub>g</sub></span> for As-Se glasses. The point numbers correspond to the glass order numbers in <a href="#applsci-13-02742-t001" class="html-table">Table 1</a>.</p>
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16 pages, 2535 KiB  
Article
Optimization of BP Neural Network Model for Rockburst Prediction under Multiple Influence Factors
by Chao Wang, Jianhui Xu, Yuefeng Li, Tuanhui Wang and Qiwei Wang
Appl. Sci. 2023, 13(4), 2741; https://doi.org/10.3390/app13042741 - 20 Feb 2023
Cited by 5 | Viewed by 2351
Abstract
Rockbursts are serious threats to the safe production of mining, resulting in great casualties and property losses. The accurate prediction of rockburst is an important premise that influences the safety and health of miners. As a classical machine learning algorithm, the back propagation [...] Read more.
Rockbursts are serious threats to the safe production of mining, resulting in great casualties and property losses. The accurate prediction of rockburst is an important premise that influences the safety and health of miners. As a classical machine learning algorithm, the back propagation (BP) neural network has been widely used in rockburst prediction. However, there are few reports about the influence study of different training sample sizes, optimization algorithms and index dimensionless methods on the prediction accuracy of BP neural network models. Therefore, 100 groups of typical rockburst engineering samples were collected locally and abroad, and considering the relevance, scientificity and quantifiability of the prediction indexes, the ratio of the maximum tangential stress of surrounding rock to the rock uniaxial compressive strength (σθ/σc), the ratio of the rock uniaxial compressive strength to the rock uniaxial tensile strength (σc/σt) and the elastic energy index (Wet) were chosen as the prediction indexes. When the number of samples was 40, 70 and 100, sixty improved BP models were established based on the standard gradient descent algorithm and four optimization algorithms (momentum gradient descent algorithm, quasi-Newton algorithm, conjugate gradient algorithm, Levenberg–Marquardt algorithm) and four index dimensionless methods (unified extreme value processing method, differentiated extreme value processing method, data averaging processing method, normalized processing method). The prediction performances of each improved model were compared with those of standard BP models. The comparative study results indicate that the sample size, optimization algorithm and dimensionless method have different effects on the prediction accuracy of BP models, which are described as follows: (1) The prediction accuracy value A of the BP model increases with the addition of sample size. The average value Aave of twenty improved models under three kinds of sample sizes increases from Aave (40) = 69.7% to Aave (100) = 75.3%, with a maximal value Amax from Amax (40) = 85.0% to Amax (100) = 97.0%. (2) The value A and comprehensive accuracy value C of the BP model based on four optimization algorithms are generally higher than those of the standard BP model. (3) The improved BP model based on the unified extreme value processing method combined with the Levenberg–Marquardt algorithm has the highest value Amax (100) = 97.0% and value C = 194, and the prediction results of five engineering cases are completely consistent with the actual situation at the site, so this is the best BP neural network model selected in this paper. Full article
(This article belongs to the Special Issue Mining Safety: Challenges & Prevention)
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<p>Structure of the BP neural network.</p>
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<p>Box plot of prediction indexes: (<b>a</b>) <span class="html-italic">σ</span><sub>θ</sub>/<span class="html-italic">σ</span><sub>c</sub>; (<b>b</b>) <span class="html-italic">σ</span><sub>c</sub>/<span class="html-italic">σ</span><sub>t</sub>; (<b>c</b>) <span class="html-italic">W</span><sub>et</sub>.</p>
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<p>Flow chart of model optimization.</p>
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<p>Model accuracy rate <span class="html-italic">A</span> under different dimensionless methods: (<b>a</b>) sample size 40; (<b>b</b>) sample size 70; (<b>c</b>) sample size 100.</p>
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<p>Model accuracy rate under different sample sizes.</p>
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<p>Comparison of prediction results.</p>
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25 pages, 6986 KiB  
Article
Process Optimization of Microwave-Assisted Extraction of Chlorophyll, Carotenoid and Phenolic Compounds from Chlorella vulgaris and Comparison with Conventional and Supercritical Fluid Extraction
by Ioulia Georgiopoulou, Soultana Tzima, Vasiliki Louli and Kostis Magoulas
Appl. Sci. 2023, 13(4), 2740; https://doi.org/10.3390/app13042740 - 20 Feb 2023
Cited by 26 | Viewed by 4410
Abstract
The production of bioactive products from microalgae biomass with efficient and environmentally friendly technologies is a field of great research interest. The present work focuses on the recovery of high-added value bioactive components from Chlorella vulgaris through microwave-assisted extraction (MAE) with aq. ethanol [...] Read more.
The production of bioactive products from microalgae biomass with efficient and environmentally friendly technologies is a field of great research interest. The present work focuses on the recovery of high-added value bioactive components from Chlorella vulgaris through microwave-assisted extraction (MAE) with aq. ethanol 90% v/v. The effect of extraction temperature (40–60 °C), duration (5–25 min), solvent-to-biomass ratio (20–90 mLsolv/gbiom), and microwave power (300–800 watts) was investigated regarding the extraction yield, extract’s chlorophyll, carotenoid and phenolic content, and antioxidant activity. MAE optimization at 60 °C, 300 watts, 14 min, and 22 mLsolv/gbiom led to 11.14% w/w yield, 63.36 mg/gextr total chlorophylls, 7.06 mg/gextr selected carotenoids of astaxanthin, lutein and β-carotene, 24.88 mg/gextr total carotenoids, 9.34 mgGA/gextr total phenolics, and 40.49 mgextr/mgDPPH IC50 (antioxidant activity indicator). Moreover, the conventional solid-liquid extraction (SLE) with aq. ethanol 90% v/v, the supercritical fluid extraction (SFE) with CO2, as well as SFE with cosolvent addition (10% w/w ethanol), were also performed for comparison purposes. The results revealed that SLE presented the highest yield. However, the non-conventional methods of MAE and SFE led to extracts of competitive or even better quality under significantly shorter extraction duration. Full article
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<p>The effect of extraction duration on MAE’s (<b>a</b>) extraction yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity. The extraction conditions of the single-factor experiments were maintained at 55 mL<sub>solv</sub>/g<sub>biom</sub>, 50 °C and 550 watts.</p>
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<p>The effect of extraction duration on MAE’s (<b>a</b>) extraction yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity. The extraction conditions of the single-factor experiments were maintained at 55 mL<sub>solv</sub>/g<sub>biom</sub>, 50 °C and 550 watts.</p>
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<p>The effect of solvent-to-biomass ratio on MAE’s (<b>a</b>) extraction yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) select and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity. The extraction conditions of the single-factor experiments were maintained at 50 °C, 15 min and 550 watts.</p>
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<p>The effect of solvent-to-biomass ratio on MAE’s (<b>a</b>) extraction yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) select and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity. The extraction conditions of the single-factor experiments were maintained at 50 °C, 15 min and 550 watts.</p>
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<p>The effect of extraction temperature on MAE’s (<b>a</b>) extraction yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity. The extraction conditions of the single-factor experiments were maintained at 55 mL<sub>solv</sub>/g<sub>biom</sub>, 15 min and 550 watts.</p>
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<p>The effect of microwave power on MAE’s (<b>a</b>) extraction yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity. The extraction conditions of the single-factor experiments were maintained at 50 °C, 55 mL<sub>solv</sub>/g<sub>biom</sub> and 15 min.</p>
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<p>The simultaneous effect of extraction temperature, duration, solvent-to-biomass ratio, and microwave power on MAE’s (<b>a</b>) yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity.</p>
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<p>The simultaneous effect of extraction temperature, duration, solvent-to-biomass ratio, and microwave power on MAE’s (<b>a</b>) yield, extract’s total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity.</p>
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<p>Experimental versus predicted values of (<b>a</b>) extraction yield, (<b>b</b>) total chlorophyll content, (<b>c</b>) total carotenoid content, and (<b>d</b>) antioxidant activity. The error bars refer to the experimental coefficient of deviation.</p>
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<p>Comparison between the conventional solid-liquid extraction (SLE), microwave-assisted extraction (MAE), supercritical fluid extraction (SFE) and supercritical fluid extraction with 10% <span class="html-italic">w</span>/<span class="html-italic">w</span> cosolvent addition (SFE + 10% Ethanol) of <span class="html-italic">Chlorella vulgaris</span>, regarding the (<b>a</b>) extraction yield, total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity.</p>
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<p>Comparison between the conventional solid-liquid extraction (SLE), microwave-assisted extraction (MAE), supercritical fluid extraction (SFE) and supercritical fluid extraction with 10% <span class="html-italic">w</span>/<span class="html-italic">w</span> cosolvent addition (SFE + 10% Ethanol) of <span class="html-italic">Chlorella vulgaris</span>, regarding the (<b>a</b>) extraction yield, total (<b>b</b>) phenolic and (<b>c</b>) chlorophyll content, (<b>d</b>) selected and (<b>e</b>) total carotenoid content, and (<b>f</b>) antioxidant activity.</p>
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<p>Comparison between the conventional solid-liquid extraction (SLE), microwave-assisted extraction (MAE), supercritical fluid extraction (SFE) and supercritical fluid extraction with 10% <span class="html-italic">w</span>/<span class="html-italic">w</span> cosolvent addition (SFE + 10% Ethanol) of <span class="html-italic">Chlorella vulgaris</span>, regarding the (<b>a</b>) selected and (<b>b</b>) total carotenoid content expressed in amount of bioactive component per amount of biomass.</p>
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<p>Contour plots of MAE yield as a function of extraction temperature and microwave power at the low, central and high levels of extraction duration and solvent-to-biomass ratios.</p>
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<p>Contour plots of extract’s total chlorophyll content as a function of extraction temperature and microwave power at the low, central and high levels of extraction duration and solvent-to-biomass ratios.</p>
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<p>Contour plots of extract’s total carotenoid content as a function of extraction temperature and microwave power at the low, central and high levels of extraction duration and solvent-to-biomass ratios.</p>
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<p>Contour plots of extract’s antioxidant activity indicator, IC<sub>50</sub>, as a function of extraction temperature and microwave power at the low, central and high levels of extraction duration and solvent-to-biomass ratio.</p>
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14 pages, 7893 KiB  
Article
Comparative Analysis of Partially Renewable Composite Fuels Based on Peat, Lignite and Plant Oil
by Roman Egorov, Dmitrii O. Glushkov and Maxim Belonogov
Appl. Sci. 2023, 13(4), 2739; https://doi.org/10.3390/app13042739 - 20 Feb 2023
Cited by 1 | Viewed by 1517
Abstract
The inevitable depletion of exploited fossil fuel deposits motivates the investigation of every possibility of saving them. One of the ways to do that is to combine fossil fuels with renewable plant-derived fuels. This paper studies the specific aspects of the thermochemical conversion [...] Read more.
The inevitable depletion of exploited fossil fuel deposits motivates the investigation of every possibility of saving them. One of the ways to do that is to combine fossil fuels with renewable plant-derived fuels. This paper studies the specific aspects of the thermochemical conversion of composite fuels consisting of peat or lignite with rapeseed oil. It was shown that mixtures of peat or lignite with rapeseed oil can be successfully gasified when the temperature is higher than 700–800 °C. The self-sustaining combustion of these fuels does not support such high temperatures, and thus the process requires external heating. The obtained optimal component ratio for peat-oil and lignite-oil compositions is about 1:2 and 3:2, respectively. Such mixtures allow the most efficient usage of the oxidation heat during conversion. The high calorific value of such fuels is very close to that of rapeseed oil (38.5 MJ/kg), even for the lignite-oil composition with 40 wt% lignite. Lower overall prices of fossil fuels compared to pure renewable plant-derived fuels help reduce costs and save valuable fossil fuels. Full article
(This article belongs to the Special Issue Fuel Combustion Mechanisms, Characteristics and Emission Analysis)
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<p>Scheme of the experimental setup for high-temperature gasification of the fuel under a light flow. It includes a light source (1), a parabolic mirror for light focusing (2) and a cuvette with fuel (3) placed on an electronic balance (4) platform. The gas analyzer (6) is connected to the cuvette with a quick connect fitting. The thermal imaging system is (5).</p>
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<p>TGA results for thermal decomposition of fuels. TGA dependencies (<b>a</b>), the DTG dependencies (<b>b</b>) and the thermal effect of fuel decomposition (<b>c</b>). The shaded area on the plot shows the temperature range where the maximum heat production is recorded for all the fuels.</p>
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<p>Average temperatures during conversion for P + RO (<b>a</b>) and L + RO (<b>b</b>) fuel compositions. The red zone corresponds to fuel conversion. The green and gray zones correspond to compositions with excess production of CO<sub>2</sub> and extremely low overall gas production.</p>
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<p>Characteristic temperatures (green) recorded during the allothermal conversion of composite fuels and their components (normalized to the highest temperature) and high calorific values of the fuels (normalized to the highest value). Normalization factors: <span class="html-italic">T</span><sub>max</sub> = 1350 °C, <span class="html-italic">Q</span><sub>max</sub> = 38.5 MJ/kg.</p>
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<p>Chemical composition of producer gas for different fossil fuel—renewable component ratios in the composite fuel. The gas trends are shown in subfigures: CO (<b>a</b>), CO<sub>2</sub> (<b>b</b>), CH<sub>4</sub> (<b>c</b>), SO<sub>2</sub> (<b>d</b>), NO (<b>e</b>). The optimal fuel compositions are 35 wt% peat and 65 wt% rapeseed oil; 60 wt% lignite and 40 wt% rapeseed oil.</p>
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<p>Producer gas weight per square centimeter of the irradiated fuel area versus time. The fuel compositions are P + RO (<b>a</b>) and L + RO (<b>b</b>). The weight fraction of rapeseed oil is shown on the right. The light flow intensity is 880 W/cm<sup>2</sup>.</p>
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<p>Producer gas weight per square centimeter of the irradiated fuel area versus time. The fuel compositions are P + RO (<b>a</b>) and L + RO (<b>b</b>). The weight fraction of rapeseed oil is shown on the right. The light flow intensity is 880 W/cm<sup>2</sup>.</p>
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<p>External heating source energy used to convert unit weight of fuel composition. Solid components are peat (P), lignite (L) and bituminous coal processing waste (C). The energy is shown on a log scale.</p>
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13 pages, 2401 KiB  
Article
Biomechanical Analysis of Femoral Stem Features in Hinged Revision TKA with Valgus or Varus Deformity: A Comparative Finite Elements Study
by Edoardo Bori and Bernardo Innocenti
Appl. Sci. 2023, 13(4), 2738; https://doi.org/10.3390/app13042738 - 20 Feb 2023
Cited by 1 | Viewed by 1703
Abstract
Hinged total knee arthroplasty (TKA) is a valid option to treat patients during revision of an implant; however, in case of varus/valgus deformity, the force transmission from the femur to the tibia could be altered and therefore the performance of the implant could [...] Read more.
Hinged total knee arthroplasty (TKA) is a valid option to treat patients during revision of an implant; however, in case of varus/valgus deformity, the force transmission from the femur to the tibia could be altered and therefore the performance of the implant could be detrimental. To be able to evaluate this, the goal of this study was to investigate, using a validated finite element analysis, the effect of varus/valgus load configurations in the bones when a hinged TKA is used. In detail, short and long stem lengths (50 mm, and 120 mm), were analyzed both under cemented or press-fit fixation under the following varus and valgus deformity: 5°, 10°, 20°, and 30°. The main outputs of the study were average bone stress in different regions of interest, together with tibio-femoral contact pressure and force. Results demonstrated that changes in the varus or valgus deformity degrees induce a change in the medio-lateral stress and force distribution, together with a change in the contact area. The effect of stem length and cement do not alter the tibio-femoral contact biomechanics but its effect is mainly localized in the distal femoral region, and it is negligible in the proximal regions. Full article
(This article belongs to the Special Issue Advanced Imaging in Orthopedic Biomechanics)
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<p>Load conditions applied to the model, (<b>A</b>) frontal view, reporting the direction of the forces applied; (<b>B</b>) distal view, reporting the area used for the applied force. FL = lateral force (in blue), FM = medial force (in green).</p>
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<p>Regions of interest defined for the present study. All of the regions have a height of 30 mm measured along the femoral anatomical axis.</p>
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<p>Qualitative overview of the von Mises stress distribution (in MPa) on the polyethylene insert and of the contact pressure (in MPa) and area on the polyethylene insert for the different varus/valgus configurations analyzed in the study, for a stem length of 50 mm cemented. M = medial, L = lateral.</p>
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<p>Input force, contact force and contact area relative to different varus/valgus angles for the cemented 50 mm stem.</p>
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<p>Average von Mises stresses in four regions of interest ((<b>A</b>): ROI 1, (<b>B</b>): ROI 3, (<b>C</b>): ROI 5, (<b>D</b>): ROI 7) for the different prosthesis features, according to the varus/valgus angles addressed.</p>
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15 pages, 5270 KiB  
Article
Thermomechanical Stresses in Silicon Chips for Optoelectronic Devices
by Claudia Mezzalira, Fosca Conti, Danilo Pedron and Raffaella Signorini
Appl. Sci. 2023, 13(4), 2737; https://doi.org/10.3390/app13042737 - 20 Feb 2023
Cited by 1 | Viewed by 1885
Abstract
The growing interest in improving optoelectronic devices requires continuous research of the materials and processes involved in manufacturing. From a chemical point of view, the study of this sector is crucial to optimize existing manufacturing processes or create new ones. This work focusses [...] Read more.
The growing interest in improving optoelectronic devices requires continuous research of the materials and processes involved in manufacturing. From a chemical point of view, the study of this sector is crucial to optimize existing manufacturing processes or create new ones. This work focusses on the experimental evaluation of residual stresses on samples that are intended to simulate part of the structure of an optoelectronic device. It represents an important starting point for the development of optoelectronic devices with characteristics suitable for future industrial production. Silicon chips, with a thickness of 120 μm, were soldered onto copper and alumina substrates, using different assembly parameters in terms of temperature and pressure. Using Raman spectroscopy, the stress evaluation was estimated in a wide temperature range, from −50 to 180 °C. Silicon chips soldered with AuSn alloy on copper substrates demonstrated at 22 °C a compressive stress, developed in the center of the assembly with a maximum value of −600 MPa, which reached −1 GPa at low temperatures. They present a stress distribution with a symmetric profile with respect to the central area of the chip. The silicon chip assembled on a ceramic substrate without pressure turned out to be extremely interesting. Even in the absence of pressure, the sample did not show a large shift in the Raman position, indicating a low stress. Full article
(This article belongs to the Section Applied Physics General)
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<p>Schematic illustration of an assembled device showing three main components: Si chip on top, substrate on bottom, and interconnection material in between. The cartesian axis system reflects the geometric symmetry of the Si crystal.</p>
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<p>Images of (<b>a</b>) copper and (<b>b</b>) Al<sub>2</sub>O<sub>3</sub> ceramic substrates.</p>
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<p>Temperature profile used for the soldering process with AuSn alloy as the interconnection material, without (<b>a</b>) and with (<b>b</b>) pressure. The grey regions indicate an N<sub>2</sub> atmosphere, while the light-yellow region indicates the additional presence of formic acid gas in the oven.</p>
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<p>Schematic subdivision of the surface of silicon chips (<b>a</b>). The Raman signal is acquired at the center position of each square. The diagonal points [1, 1] to [11, 11] are colored yellow in panel (<b>b</b>), while the positions [1, 1] and [6, 6] are colored yellow in panel (<b>c</b>).</p>
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<p>Raman spectrum of the silicon unmounted chip, measured using 514.5 nm radiation from an Ar laser.</p>
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<p>Raman peak, corresponding to the LO phonon mode, collected, at room temperature, along the diagonal points (from [1, 1] to [10, 10] of <a href="#applsci-13-02737-f004" class="html-fig">Figure 4</a>b) of (<b>a</b>) the Si_Unmounted chip, (<b>b</b>) sample A_AuSn, (<b>c</b>) sample A_AuSn_p and (<b>d</b>) sample B_AuSn.</p>
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<p>Raman-shift distribution at room temperature of the (<b>a</b>) Si_Unmounted chip, (<b>b</b>) A_AuSn, (<b>c</b>) A_AuSn_p, and (<b>d</b>) B_AuSn samples.</p>
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<p>Central [6, 6] (squares) and corner (triangles) [1, 1] Raman shift recorded at temperatures from −50 to 180 °C with the Si_Unmounted chip (<b>a</b>), the A_AuSn_p sample (<b>b</b>) and the A_AuSn sample (<b>c</b>).</p>
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<p>Raman shift distribution along the diagonal recorded at −50 (black points and lines), 20 (red points and lines) and 180 °C (blue points and lines), on (<b>a</b>) Si_Unmounted chip, (<b>b</b>) A_AuSn_p sample and (<b>c</b>) A_AuSn sample (C). Position <span class="html-italic">i</span> refers to the position [i,i] of <a href="#applsci-13-02737-f004" class="html-fig">Figure 4</a>b.</p>
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<p>Stress distribution along the diagonal recorded at −50 (Black points and lines), 20 (Red points and lines) and 180 °C (Blue points and lines), on the Si_Unmounted chip (<b>a</b>), the A_AuSn_p sample (<b>b</b>) and the A_AuSn sample (<b>c</b>). Position <span class="html-italic">i</span> refers to the position [x, x] of <a href="#applsci-13-02737-f004" class="html-fig">Figure 4</a>b.</p>
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<p>Stress distribution at 20 °C, on (<b>a</b>) Si_Unmounted chip, (<b>b</b>) A_AuSn_p, (<b>c</b>) A_AuS, and (<b>d</b>) B_AuSn samples.</p>
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<p>Stress distribution at −50 °C, on a Si_Unmounted chip (panel <b>a</b>), A_AuSn_p sample (<b>b</b>), and A_AuSn sample (<b>c</b>).</p>
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<p>Stress distribution at 180 °C, on Si_Unmounted chip (<b>a</b>), A_AuSn_p sample (<b>b</b>), and A_AuSn sample (<b>c</b>).</p>
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21 pages, 13258 KiB  
Article
Identification Procedure for Design Optimization of Gravitational Electromagnetic Energy Harvesters
by Mirco Lo Monaco, Caterina Russo and Aurelio Somà
Appl. Sci. 2023, 13(4), 2736; https://doi.org/10.3390/app13042736 - 20 Feb 2023
Cited by 6 | Viewed by 1898
Abstract
Energy harvesting is a promising technique for supplying low-power devices as an alternative to conventional batteries. Energy harvesters can be integrated into Autonomous Internet of Things (AIoT) systems to create a wireless network of sensor nodes for real-time monitoring of assets. This paper [...] Read more.
Energy harvesting is a promising technique for supplying low-power devices as an alternative to conventional batteries. Energy harvesters can be integrated into Autonomous Internet of Things (AIoT) systems to create a wireless network of sensor nodes for real-time monitoring of assets. This paper shows a design and optimization methodology for gravitational vibration-based electromagnetic energy harvesters (GVEHs) of different sizes considering the design constraints of its real application. The configuration, analytical model, and electro-mechanical coupling of these devices are described in detail. A numerical model is developed in the Ansys Maxwell FEM environment to derive the non-linear stiffness and damping of the asymmetric magnetic suspension. Experimental laboratory tests on three harvester prototypes are compared to numerical results of dynamic simulations in MATLAB/Simulink for the validation of the proposed model through error estimation. The fully-parametric validated model is used to perform sensitivity analyses on the device’s mechanical characteristics of natural frequency and magnet equilibrium position by varying the fixed and moving magnets dimensions. The set of magnets composing the magnetic spring is chosen complying with the application design constraints of size and resonance frequency tuning. Coil parameters of length and number of turns are optimized for maximum output power generation. The optimized device simulated performances are compared to other devices in the literature in terms of NPD, a significant index that evaluates power density under different excitation amplitudes. The optimized harvester presents the highest NPD value of 2.61, achieving an improvement of 52% with respect to the best harvester amongst the three tested prototypes. Full article
(This article belongs to the Special Issue State-of-the-Art in Energy Harvesting for IoT and WSN)
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<p>Schematic representation of the harvesters.</p>
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<p>(<b>a</b>) Scheme of harvester mechanical subsystem. (<b>b</b>) Scheme of harvester electric circuit.</p>
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<p>Simulink block scheme.</p>
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<p>(<b>a</b>) Magnetic field vectors for EH3. (<b>b</b>) Magnetic flux linkage for EH3.</p>
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<p>Magnetic force curves for EH1, EH2, and EH3.</p>
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<p>Exponential decay of viscous damping for EH1.</p>
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<p>Electromagnetic coupling coefficient and damping curves.</p>
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<p>Experimental setup logic flow.</p>
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<p>Experimental setup picture.</p>
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<p>Experimental and model FRFs comparison for EH1, EH2, and EH3.</p>
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<p>Fixed magnet sensitivity analysis.</p>
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<p>Moving magnet sensitivity analysis.</p>
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<p>Moving magnet sensitivity analysis.</p>
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<p>Coil axial length and number of turns sensitivity analyses.</p>
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11 pages, 1188 KiB  
Article
The Improvement and Application of the Geoelectrochemical Exploration Method
by Ming Kang, Huanzhao Guo, Wende Zhu, Xianrong Luo and Jianwen Yang
Appl. Sci. 2023, 13(4), 2735; https://doi.org/10.3390/app13042735 - 20 Feb 2023
Cited by 1 | Viewed by 1485
Abstract
The anionic and cationic species of elements from deeply buried deposits migrate to the near surface driven by various geological forces. The geoelectrochemical exploration method (GEM), derived from CHIM, consists of the application of an electric field to collect these active ions at [...] Read more.
The anionic and cationic species of elements from deeply buried deposits migrate to the near surface driven by various geological forces. The geoelectrochemical exploration method (GEM), derived from CHIM, consists of the application of an electric field to collect these active ions at the designated electrode. Prospecting effects have been investigated by researchers since the coming up of CHIM. However, the cumbersome technical equipment, complex techniques and low production efficiency have restricted its potential application in field geological survey. This paper presents the newly developed CHIM that is electrified by a low voltage dipole. The improved technique allows both anionic and cationic species of elements to be extracted simultaneously in an anode and in a cathode. Compared with the conventional CHIM method, the innovative techniques called dipole geoelectrochemical method are characterized by simple instrumentation, low cost and easy operation in field, and in particular enables simultaneous extraction of anionic and cationic species of elements, from which more information can be derived with higher extraction efficiency. The dipole geoelectrochemical method was proposed and applied in the experiments of the Yingezhuang gold ore from Zhaoyuan, Shandong Province, the 210 gold ore from Jinwozi, Xinjiang Province, and the Daiyinzhang gold polymetallic deposit from Wutaishan, Shanxi Province. There are clearly anomalies above the gold ore body, indicating the effectiveness and feasibility of the improved dipole geoelectrochemical method in both scientific research and mineral exploration. The results of anode extraction in several mining areas have shown good results, indicating that gold may be mainly negatively charged. In fact, many metal nanoparticles, clay minerals, or complexes of metal ions are negatively charged, so they migrate to the anode electrode and enrich. Full article
(This article belongs to the Special Issue New Advances and Illustrations in Applied Geochemistry)
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<p>The formation of geoelectrochemical ionic halos.</p>
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<p>Simplified profile of the DL-CHIM. 1—Anion collector; 2—Cation collector; 3—Current flow lines; 4—Disposable DC power supply.</p>
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<p>Results obtained by employing the DL-CHIM method over Yingezhuang gold deposit from Shandong, China. (<b>a</b>) Anion anomalies of Au (Anode extraction); (<b>b</b>) Cation anomalies of Au (Cathode extraction); (<b>c</b>) geological base map [<a href="#B13-applsci-13-02735" class="html-bibr">13</a>].</p>
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<p>Results obtained by employing the DL-CHIM method over 210 gold deposit from Xinjiang, China. 1—Quaternary System Holocene; 2—Quaternary System Pleistocene; 3—Gold ore body; (<b>a</b>) Anion anomalies of Au (Anode extraction); (<b>b</b>) Cation anomalies of Au (Cathode extraction); (<b>c</b>) geological base map [<a href="#B13-applsci-13-02735" class="html-bibr">13</a>].</p>
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<p>Results obtained by employing the DL-CHIM method and geochemical soil survey over Daiyinzhang gold deposit from Shanxi, China. 1—Chlorite schist; 2—Sericite schist; 3—Metamorphic diabase; 4—Plagioclase granite; 5—Gold mineralization; 6—Gold ore body; 7—Drill hole; (<b>a</b>) Soil geochemical anomalies; (<b>b</b>) Anion anomalies of Au (Anode extraction); (<b>c</b>) Cation anomalies of Au (Cathode extraction); (<b>d</b>) geological base map [<a href="#B35-applsci-13-02735" class="html-bibr">35</a>,<a href="#B36-applsci-13-02735" class="html-bibr">36</a>].</p>
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9 pages, 1468 KiB  
Communication
Optimal Complex Morlet Wavelet Parameters for Quantitative Time-Frequency Analysis of Molecular Vibration
by Shuangquan Li, Shangyi Ma and Shaoqing Wang
Appl. Sci. 2023, 13(4), 2734; https://doi.org/10.3390/app13042734 - 20 Feb 2023
Cited by 4 | Viewed by 3682
Abstract
When the complex Morlet function (CMOR) is used as a wavelet basis, it is necessary to select optimal bandwidth and center frequency. However, the method to select the optimal CMOR wavelet parameters for one specific frequency is still unclear. In this paper, we [...] Read more.
When the complex Morlet function (CMOR) is used as a wavelet basis, it is necessary to select optimal bandwidth and center frequency. However, the method to select the optimal CMOR wavelet parameters for one specific frequency is still unclear. In this paper, we deeply investigate the essence of CMOR wavelet transform and clearly illustrate the time-frequency resolution and edge effect. Then, the selection method of the optimal bandwidth and center frequency is proposed. We further perform the quantitative time-frequency (QTF) analysis of water molecule vibration based on our method. We find that the CMOR wavelet parameters obtained by our method can not only meet the requirement of frequency resolution but also meet the limit of edge effect. Moreover, there is an uphill energy relaxation in the vibration of the water molecule, which agrees well with the experimental results. These results demonstrate that our method can accurately find the optimal CMOR wavelet parameters for the target frequency. Full article
(This article belongs to the Topic Theoretical, Quantum and Computational Chemistry)
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<p>The essence of CMOR wavelet transform. (<b>a</b>) The real part of CMOR2-1, (<b>b</b>) The window functions corresponding to different target frequencies (<span class="html-italic">f<sub>1</sub></span>, <span class="html-italic">f<sub>2</sub></span>) in <span class="html-italic">u</span>(<span class="html-italic">t</span>), (<b>c</b>) Time resolution and edge effect of CMOR wavelet.</p>
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<p>The CMOR wavelet transform of cosine signal (O-H bending vibration): (<b>a</b>) The 3D time-frequency analysis, (<b>b</b>) The intensity variation over time for <span class="html-italic">f<sub>k</sub></span>, (<b>c</b>) Intensity of various frequencies at 0.5<span class="html-italic">T</span><sub>0</sub> (Δ<span class="html-italic">f</span> = 113 cm<sup>−1</sup>).</p>
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<p>QTF analysis of the water molecule vibration: (<b>a</b>) O-H bending vibration (<span class="html-italic">f<sub>k</sub></span> = 1560.6 cm<sup>−1</sup>, <span class="html-italic">f<sub>n</sub></span> = 3711.1 cm<sup>−1</sup>), (<b>b</b>) O-H symmetric stretching vibration (<span class="html-italic">f<sub>k</sub></span> = 3711.1 cm<sup>−1</sup>, <span class="html-italic">f<sub>n</sub></span> = 3819.3 cm<sup>−1</sup>), (<b>c</b>) O-H asymmetric stretching vibration (<span class="html-italic">f<sub>k</sub></span> = 3819.3 cm<sup>−1</sup>, <span class="html-italic">f<sub>n</sub></span> = 3711.1 cm<sup>−1</sup>).</p>
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18 pages, 4975 KiB  
Article
Trajectory Tracking of Autonomous Vehicle Using Clothoid Curve
by Jianshi Li, Jingtao Lou, Yongle Li, Shiju Pan and Youchun Xu
Appl. Sci. 2023, 13(4), 2733; https://doi.org/10.3390/app13042733 - 20 Feb 2023
Cited by 4 | Viewed by 2965
Abstract
This paper proposes a clothoid-curve-based trajectory tracking control method for autonomous vehicles to solve the problem of tracking errors caused by the discontinuous curvature of the control curve calculated by the pure pursuit tracking algorithm. Firstly, based on the Ackerman steering model, the [...] Read more.
This paper proposes a clothoid-curve-based trajectory tracking control method for autonomous vehicles to solve the problem of tracking errors caused by the discontinuous curvature of the control curve calculated by the pure pursuit tracking algorithm. Firstly, based on the Ackerman steering model, the motion model is constructed for vehicle trajectory tracking, Then, the position of the vehicle after the communication delay of the control system is predicted as the starting point of the clothoid control curve, and the optimization interval of the curve end point is determined. The clothoid control curves are calculated, and their parameters are verified by the vehicle motion and safety constraints, so as to obtain the optimal clothoid control curve satisfying the constraints. Finally, considering the servo system response delay time of the steering system, the steering angle target control value is obtained by previewing the curvature of the clothoid control curve. The field experiment is conducted on the test road, which consists of straight, right-angle turns and lane-change elements under three sets of speed limitations, and the test results show that the proposed clothoid-curve-based trajectory tracking control method greatly improved the tracking accuracy compared with the pure pursuit method; in particular, the yaw deviation is improved by more than 50%. Full article
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<p>Clothoid-curve-based trajectory tracking control method.</p>
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<p>Geometric model based on Ackerman steering configuration.</p>
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<p>Schematic diagram of vehicle position prediction.</p>
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<p>Influence of the selection of preview point on the calculation deviation of control path.</p>
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<p>Test platform.</p>
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<p>Software architecture.</p>
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<p>Test path.</p>
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<p>Speed limit 10 km/h trajectory tracking. Top first row: the curvatures along the field test road. Second row: actual speed of the vehicle during the trajectory tracking experiment under the speed limit of 10 km/h. It can be seen that the vehicle will slow down according to the curvature of the road ahead before entering the curve. Third row: steering wheel angle commands the comparison between the pure pursuit method and the method proposed in this paper. When tracking the curve, the method proposed in this paper increases the steering wheel angle control command later when entering the curve, and decreases the steering wheel angle control command in advance when leaving the curve, and the control amount given in the curve is also larger. It is because of this that the “cutting corner” problem suffered by the pure pursuit method is avoided. Fourth row: yaw angle deviation from the reference path point. The method proposed in this paper reduces the angle deviation to a large extent and avoids the problem of directional oscillation when turning, so as to improve the driving stability and riding comfort of the vehicle. Last row: lateral deviation from the reference path. The method proposed in this paper greatly reduces the reference path tracking error and improves the accuracy of vehicle path tracking control.</p>
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<p>Speed limit 15 km/h trajectory tracking. Top first row: the curvatures along the field test road. Second row: actual speed of the vehicle during the trajectory tracking experiment under the speed limit of 15 km/h. It can be seen that the vehicle will slow down according to the curvature of the road ahead before entering the curve. Third row: steering wheel angle commands the comparison between the pure pursuit method and the method proposed in this paper. It is noted that the steering wheel angle control commands given by the pure pursuit method suffer a drastic oscillation when leaving the right-angle turn, which does not occur in the previous test with a speed limit of 10 km/h. This problem might be caused by the improper selection of the preview distance. Fourth row: yaw angle deviation from the reference path point. The direction deviation generated by the pure pursuit tracking method when leaving the right-angle turn is actually caused by the violent oscillation of the steering wheel angle control command. Last row: lateral deviation from the reference path. Compared with the 10 km/h speed limit test, the tracking deviation of the method proposed in this paper in the first right-angle turn increased, which indicates a limitation that the trajectory tracking accuracy of the method proposed in this paper is sensitive to speed changes when passing the curve with a large curvature.</p>
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<p>Speed limit 20 km/h trajectory tracking. Top first row: the curvatures along the field test road. Second row: actual speed of the vehicle during the trajectory tracking experiment under the speed limit of 20 km/h. It can be seen that the vehicle will slow down according to the curvature of the road ahead before entering the curve. Third row: steering wheel angle commands the comparison between the pure pursuit method and the method proposed in this paper. It can be seen that the steering wheel angle control commands given by the pure pursuit method still suffer a drastic oscillation when leaving the right-angle turn. Fourth row: yaw angle deviation from the reference path point. The obvious direction deviation generated by the pure pursuit tracking method when leaving the right-angle turn also appears as expected. Last row: lateral deviation from the reference path. The performance of the method proposed in this paper is obviously better than the pure pursuit tracking method when passing through right-angle curves, but the accuracy is slightly lower when passing through S curves with a small curvature.</p>
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30 pages, 6905 KiB  
Review
A State-of-the-Art Review of Non-Destructive Testing Image Fusion and Critical Insights on the Inspection of Aerospace Composites towards Sustainable Maintenance Repair Operations
by Muhammet E. Torbali, Argyrios Zolotas and Nicolas P. Avdelidis
Appl. Sci. 2023, 13(4), 2732; https://doi.org/10.3390/app13042732 - 20 Feb 2023
Cited by 13 | Viewed by 6749
Abstract
Non-destructive testing (NDT) of aerospace structures has gained significant interest, given its non-destructive and economic inspection nature enabling future sustainable aerospace maintenance repair operations (MROs). NDT has been applied to many different domains, and there is a number of such methods having their [...] Read more.
Non-destructive testing (NDT) of aerospace structures has gained significant interest, given its non-destructive and economic inspection nature enabling future sustainable aerospace maintenance repair operations (MROs). NDT has been applied to many different domains, and there is a number of such methods having their individual sensor technology characteristics, working principles, pros and cons. Increasingly, NDT approaches have been investigated alongside the use of data fusion with the aim of combining sensing information for improved inspection performance and more informative structural health condition outcomes for the relevant structure. Within this context, image fusion has been a particular focus. This review paper aims to provide a comprehensive survey of the recent progress and development trends in NDT-based image fusion. A particular aspect included in this work is providing critical insights on the reliable inspection of aerospace composites, given the weight-saving potential and superior mechanical properties of composites for use in aerospace structures and support for airworthiness. As the integration of NDT approaches for composite materials is rather limited in the current literature, some examples from non-composite materials are also presented as a means of providing insights into the fusion potential. Full article
(This article belongs to the Section Materials Science and Engineering)
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<p>Basic representations of thermographic, ultrasonic, X-ray and eddy current NDT methods. (<b>a</b>) Schematic representation of pulsed thermography [<a href="#B23-applsci-13-02732" class="html-bibr">23</a>]. (<b>b</b>) Schematic representation of ultrasonic testing [<a href="#B24-applsci-13-02732" class="html-bibr">24</a>]. (<b>c</b>) Schematic representation of X-ray radiography. (<b>d</b>) Eddy current defect representation [<a href="#B25-applsci-13-02732" class="html-bibr">25</a>].</p>
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<p>The main steps of a generic fusion structure.</p>
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<p>(<b>c</b>) An example representation for signal-level combination for a noise-free defect simulation and defect-free experimental noise. (<b>a</b>) Simulated noise-free defect. (<b>b</b>) Experimentally measured defect-free noisy back wall [<a href="#B43-applsci-13-02732" class="html-bibr">43</a>].</p>
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<p>Basic projection of PCs as linear combinations of original data.</p>
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<p>Two-level wavelet decomposition structure (recursive filtering and subsampling).</p>
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<p>Basic neuron architecture, called the threshold logic unit (TLU), showing inputs (I), weights (W), bias (b), activation function (f) and output (X) [<a href="#B89-applsci-13-02732" class="html-bibr">89</a>].</p>
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<p>An example demonstration of three-step integration framework: feature extraction, selection and fusion [<a href="#B91-applsci-13-02732" class="html-bibr">91</a>].</p>
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<p>Schematic representation of D-S belief probability calculations for a random point using its local neighbourhood on the defect-free region on the global distribution of feature matrix (Positive evidence is where there is a defect, negative evidence is where it is non-defective, and doubt is where theere is a high plausibility.) [<a href="#B115-applsci-13-02732" class="html-bibr">115</a>].</p>
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<p>(<b>a</b>) Katunin-et-al. example fusion approach (block diagram). (<b>b</b>) Detected damage for fusion of X-ray CT scan (red) and UT C-Scan (blue color). (<b>c</b>) Distance calculation of boundary points to the centroid for X-ray CT and UT C-scan [<a href="#B118-applsci-13-02732" class="html-bibr">118</a>].</p>
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<p>Original and artificial source images to compare and see the effect of fusion and calculate evaluation metrics over the images from [<a href="#B122-applsci-13-02732" class="html-bibr">122</a>].</p>
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<p>Absolute difference imagesfor seeing how the corruption affected the images (with respect to original image). Images were converted to grayscale first.</p>
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<p>Montage of images with the fused version of the noisy and corrupted image versions (grayscale).</p>
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<p>Simple segmentation via the adaptive threshold of the grayscale images from <a href="#applsci-13-02732-f012" class="html-fig">Figure 12</a>.</p>
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13 pages, 704 KiB  
Article
Determination of Benefits of the Application of CMMS Database Improvement Proposals
by Ladislav Stazić, Nikola Račić, Tatjana Stanivuk and Đorđe Dobrota
Appl. Sci. 2023, 13(4), 2731; https://doi.org/10.3390/app13042731 - 20 Feb 2023
Cited by 5 | Viewed by 2360
Abstract
Computerized maintenance management systems (CMMSs) are software packages that support or organize the maintenance tasks of assets or equipment. They are found in the background of any ship maintenance operation and are an important part of maintenance planning, spare parts supply, record keeping, [...] Read more.
Computerized maintenance management systems (CMMSs) are software packages that support or organize the maintenance tasks of assets or equipment. They are found in the background of any ship maintenance operation and are an important part of maintenance planning, spare parts supply, record keeping, etc. In the marine market, there are a number of CMMSs that are competing fiercely to program a better and more modern program that will capture the market, which has been accompanied by published analyses and scientific papers. At the same time, the quality of the data entered into CMMS databases is questionable, a fact that has been ignored in practice and scientific circles; until recently, there were no published analyses and there was no way to measure the quality of the data entered. This article presents two proposals for improving the quality of CMMS databases and calculates their potential benefits. By implementing the first proposal, the evaluation methodology for the ship’s Planned Maintenance System database, between 10% and 15% of databases will have significant financial or safety benefits. This measure will also have an impact on more than 40% of the other databases that can also be improved. The second proposal will have a smaller impact of only 4%. The overall benefit of these proposals is to improve more than 60% of the databases and will result in a significant increase in safety or financial savings. Full article
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<p>DQA in practice, based on [<a href="#B25-applsci-13-02731" class="html-bibr">25</a>].</p>
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<p>CMMS database evaluation process.</p>
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14 pages, 2919 KiB  
Article
Characterization of the Superplastic Magnesium Alloy AZ31 through Free-Forming Tests and Inverse Analysis
by Gillo Giuliano and Wilma Polini
Appl. Sci. 2023, 13(4), 2730; https://doi.org/10.3390/app13042730 - 20 Feb 2023
Cited by 2 | Viewed by 1524
Abstract
This work proposes a simple procedure to characterize 1.0 mm thick sheets of superplastic magnesium alloy AZ31. The simplest mathematical function that models the behavior of a superplastic material is a power law between stress and strain rate with two parameters connected to [...] Read more.
This work proposes a simple procedure to characterize 1.0 mm thick sheets of superplastic magnesium alloy AZ31. The simplest mathematical function that models the behavior of a superplastic material is a power law between stress and strain rate with two parameters connected to the material: K and m. First, the parameter m (variable with the strain) was defined directly by carrying out free-forming experimental tests at constant pressure and using a simple expression taken from the analytical modeling of the free-forming process. In the second step, an inverse analysis was carried out through a finite element model (FEM) and based on a numerical–experimental comparison between the results of the dimensionless height–time (H–t) curve, which made it possible to identify the variation of the parameter K in the same strain range. Once the m and K parameters were evaluated, it was possible to simulate the free-forming tests at constant pressure in the pressure range used to characterize the material. The proposed procedure to estimate m and K parameters made it possible to best match the numerical with the experimental results in terms of the dimensionless height–time curve. The difference between the forming time estimated by FEM and that measured experimentally along the H–t curve was found to be less than 9%. Full article
(This article belongs to the Special Issue New Insights in Material Forming)
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<p>Scheme of the superplastic-forming process.</p>
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<p>Scheme of the free-forming process (a is the radius of the cylindrical die and h is the height of the dome).</p>
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<p>Height at failure for different temperature and pressure values in AZ31 alloy.</p>
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<p>Forming die constituting two parts.</p>
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<p>Free-forming process equipment and manufactured product.</p>
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<p>FEM representation of the free-forming process.</p>
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<p>Experimental dimensionless displacement–time H–t curves.</p>
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<p>Trend of the m–H curve.</p>
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<p>Trend of F(K) function for each adopted interval of H.</p>
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<p>Trend of the K–H curve.</p>
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<p>Comparison of H–t curves obtained numerically and experimentally for <span class="html-italic">p</span> = 0.2 and 0.4 MPa.</p>
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<p>Comparison of H–t curves obtained numerically and experimentally for <span class="html-italic">p</span> = 0.3 MPa.</p>
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21 pages, 10670 KiB  
Article
The Influence of Dome Geometry on the Results of Modal and Buckling Analysis
by Urszula Radoń, Paweł Zabojszcza and Milan Sokol
Appl. Sci. 2023, 13(4), 2729; https://doi.org/10.3390/app13042729 - 20 Feb 2023
Viewed by 2045
Abstract
The main purpose of this paper is to compare the results of modal analysis for two types of domes. The first one is a low-rise Schwedler dome. The second one is a high-rise geodesic dome. The low-rise Schwedler dome is subjected to large [...] Read more.
The main purpose of this paper is to compare the results of modal analysis for two types of domes. The first one is a low-rise Schwedler dome. The second one is a high-rise geodesic dome. The low-rise Schwedler dome is subjected to large displacement gradients and should be designed according to geometrical nonlinear analysis. In the case of high-rise geodesic dome, linear analysis is sufficient. In the modal analysis, the mass of the bars of the supporting structures was modeled as evenly distributed, while the mass of the covering and roof equipment was concentrated in the nodes. Classic calculations have been enriched with modal analysis taking into account normal forces. Normal forces affect the vibration frequency of the structure. Commonly used modal analysis does not take into account the influence of normal forces. In order to approximate the actual working conditions of the structure, calculations performed in Autodesk Robot Structure Professional 2022 can be performed in accordance with the modal analysis, taking into account the applied normal forces in the modal analysis. Additionally, stability loss was verified using linear or geometrical nonlinear buckling analysis. The exigence of including normal forces in modal analysis for low-rise domes is the novelty and main message of the work. Full article
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<p>Sign convention and degrees of freedom of frame element.</p>
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<p>Schwedler dome geometry plan view.</p>
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<p>Schwedler dome side view.</p>
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<p>Graphic illustration of eigenvectors for low-rise Schwedler dome (standard modal analysis).</p>
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<p>Graphic illustration of eigenvectors for low-rise Schwedler dome (standard modal analysis).</p>
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<p>Graphic illustration of eigenvectors for low-rise Schwedler dome (standard modal analysis).</p>
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<p>Graphic illustration of eigenvectors for low-rise Schwedler dome (modal analysis taking into account normal forces).</p>
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<p>Graphic illustration of eigenvectors for low-rise Schwedler dome (modal analysis taking into account normal forces).</p>
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<p>Geodesic dome geometry.</p>
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<p>Geodesic dome side view.</p>
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<p>Graphic illustration of eigenvectors geodesic domes.</p>
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<p>Graphic illustration of eigenvectors geodesic domes.</p>
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<p>Graphic illustration of eigenvectors geodesic domes.</p>
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21 pages, 2857 KiB  
Article
Shaping the Properties of Osmo-Dehydrated Strawberries in Fruit Juice Concentrates
by Hanna Kowalska, Magdalena Trusinska, Katarzyna Rybak, Artur Wiktor, Dorota Witrowa-Rajchert and Malgorzata Nowacka
Appl. Sci. 2023, 13(4), 2728; https://doi.org/10.3390/app13042728 - 20 Feb 2023
Cited by 9 | Viewed by 3373
Abstract
The growing interest in high-quality food leads to looking for new solutions in the production of natural fruit snacks. Osmotic dehydration is one of the processes, which can be used to obtain a minimally processed product as well as to give it specific [...] Read more.
The growing interest in high-quality food leads to looking for new solutions in the production of natural fruit snacks. Osmotic dehydration is one of the processes, which can be used to obtain a minimally processed product as well as to give it specific characteristics. Usually, a sucrose solution is used as an osmotic agent; however, the use of chokeberry, strawberry, or cherry juice concentrates can be beneficial in the process of the osmotic dehydration of fruits. The process of the dehydration of strawberries with the use of fruit juice concentrates (chokeberry, strawberry, or cherry) and a sucrose solution as a standard was carried out at a temperature of 30 °C for 3 h. The kinetics of the processes (weight reduction, water loss, and solid gain) were evaluated as well as physical (water activity, color parameters L*, a*, b*, ΔE, texture with maximum force and compression work, and structure) and chemical properties (dry matter content, total polyphenols content, total anthocyanin content, vitamin C, antioxidant activity with DPPH and ABTS radicals, spectral analysis with FTIR method, sucrose, glucose and fructose content, and thermal decomposition with TG analysis). The use of fruit juice concentrates positively influences the enrichment of the final product with bioactive compounds, such as anthocyanin and vitamin C. Strawberry and chokeberry juice concentrates have proven to be good hypertonic media for increasing the antioxidant activity of dehydrated fruit. Moreover, the use of fruit concentrates has a positive effect on the sugar profile of dehydrated strawberries. Full article
(This article belongs to the Special Issue Drying Technologies in Food Processing)
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<p>Effect of the type of osmotic agent (fruit concentrates) on the mass exchange kinetics of osmodehydrated strawberries: (<b>a</b>) weight reduction, (<b>b</b>) water loss (dashed lines), and solid gain (regular lines).</p>
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<p>Effect of the type of osmotic agent (sucrose and fruit concentrates) on the dry matter content and water activity of osmodehydrated strawberries. Different letters above columns show the statistical difference (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Effect of the type of osmotic agent (sucrose and fruit concentrates) on the mechanical properties of osmodehydrated strawberries. Different letters (small letters are for max force, capital letters are for compression work) above columns show the statistical difference (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Microstructure (200× magnification) of fresh strawberries osmotically dehydrated for 3 h in solutions of sucrose, chokeberry (chok juice), strawberry (straw juice), and cherry juice concentrates.</p>
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<p>Effect of the type of osmotic agent (sucrose and fruit concentrates) on the vitamin C content in osmodehydrated strawberries. Different letters above columns show the statistical difference (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Effect of the type of osmotic agent (sucrose and fruit concentrates) on the total polyphenol content and anthocyanin content in osmodehydrated strawberries. Different letters (small letters are for anthocyanin content, capital letters are for total polyphenol content) above columns show the statistical difference (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Effect of the type of osmotic agent (sucrose and fruit concentrates) on the antioxidant activity of osmodehydrated strawberries. Different letters (small letters are for antioxidant activity according to ABTS radical, capital letters are for antioxidant activity according to DPPH radical) above columns show the statistical difference (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Fourier transform infrared (FTIR) spectra of the solutions (<b>a</b>) and strawberries after osmotic dehydration (<b>b</b>) conducted in a different type of osmotic agent (sucrose and fruit concentrates).</p>
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<p>Effect of the type of osmotic agent (sucrose and fruit concentrates) on the sugar content of osmodehydrated strawberries. Different letters above columns show the statistical difference (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Effect of the type of osmotic agent (sucrose and fruit concentrates) on the sugar content in osmodehydrated strawberries.</p>
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<p>PCA analysis: (<b>a</b>) PCA loading plot of two principal components, (<b>b</b>) score plot presenting analyzed samples in term of PC1 vs. PC2. Markings: DM—dry matter content, WL—water loss, SG—solid gain, Aw—water activity; L*, a*, b*, ΔE—color parameters. Red lines indicate active data included in the PCA analysis, blue lines - additional data. The red line on (<b>b</b>) concerns the separation of a group of data with a similar effect of osmotic agent on the examined physicochemical indicators.</p>
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20 pages, 5189 KiB  
Article
A Hybrid Grey Wolf Optimization Algorithm Using Robust Learning Mechanism for Large Scale Economic Load Dispatch with Vale-Point Effect
by Tzu-Ching Tai, Chen-Cheng Lee and Cheng-Chien Kuo
Appl. Sci. 2023, 13(4), 2727; https://doi.org/10.3390/app13042727 - 20 Feb 2023
Cited by 9 | Viewed by 2377
Abstract
This paper proposes a new hybrid algorithm for grey wolf optimization (GWO) integrated with a robust learning mechanism to solve the large-scale economic load dispatch (ELD) problem. The robust learning grey wolf optimization (RLGWO) algorithm imitates the hunting behavior and social hierarchy of [...] Read more.
This paper proposes a new hybrid algorithm for grey wolf optimization (GWO) integrated with a robust learning mechanism to solve the large-scale economic load dispatch (ELD) problem. The robust learning grey wolf optimization (RLGWO) algorithm imitates the hunting behavior and social hierarchy of grey wolves in nature and is reinforced by robust tolerance-based adjust searching direction and opposite-based learning. This technique could effectively prevent search agents from being trapped in local optima and also generate potential candidates to obtain a feasible solution. Several constraints of power generators, such as generation limits, local demand, valve-point loading effect, and transmission losses, are considered in practical operation. Five test systems are used to evaluate the effectiveness and robustness of the proposed algorithm in solving the ELD problem. The simulation results clearly reveal the superiority and feasibility of RLGWO to find better solutions in terms of fuel cost and computational efficiency when compared with the previous literature. Full article
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<p>The hunting mechanism of GWO in one-dimensional minimization. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>α</mi> </msub> </mrow> </semantics></math> falls into a local optimum; and (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mi>α</mi> </msub> </mrow> </semantics></math> reaches the global optimum..</p>
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<p>Adjustment probability at different iteration periods.</p>
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<p>The convergence rate of the search mechanism.</p>
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<p>Comparative convergence characteristic of original GWO and proposed RLGWO algorithm for the 13-unit system.</p>
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<p>Results for different methods for the 13-unit system (50 trials): (<b>a</b>) boxplot of the final generation cost; (<b>b</b>) time and number of hits of the minimum solution.</p>
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<p>Comparative convergence characteristics of the original GWO and the proposed RLGWO algorithms for the 40-unit system.</p>
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<p>Results for different methods for the 40-unit system (50 trials): (<b>a</b>) boxplot of the final generation cost; (<b>b</b>) time and number of hits of the minimum solution.</p>
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<p>Comparative convergence characteristics of the original GWO and the proposed RLGWO algorithms for the 110-unit system.</p>
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<p>Results for different methods for the 110-unit system (50 trials): (<b>a</b>) boxplot of the final generation cost; (<b>b</b>) time and number of hits of the minimum solution.</p>
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<p>Comparative convergence characteristic of original GWO and proposed RLGWO algorithm for the 140-unit system.</p>
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<p>Results obtaind using different methods for the 140-unit system (50 trials): (<b>a</b>) boxplot of the final generation cost; (<b>b</b>) time and number of hits of the minimum solution.</p>
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<p>Comparative convergence characteristic of original GWO and proposed RLGWO algorithm for the 160-unit system.</p>
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<p>Results for different methods for the 160-unit system (50 trials): (<b>a</b>) boxplot of the final generation cost; (<b>b</b>) time and number of hits of the minimum solution.</p>
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18 pages, 4546 KiB  
Article
Sep-RefineNet: A Deinterleaving Method for Radar Signals Based on Semantic Segmentation
by Yongjiang Mao, Wenjuan Ren, Xipeng Li, Zhanpeng Yang and Wei Cao
Appl. Sci. 2023, 13(4), 2726; https://doi.org/10.3390/app13042726 - 20 Feb 2023
Cited by 1 | Viewed by 3310
Abstract
With the progress of signal processing technology and the emergence of new system radars, the space electromagnetic environment becomes more and more complex, which puts forward higher requirements for the deinterleaving method of radar signals. Traditional signal deinterleaving algorithms rely heavily on manual [...] Read more.
With the progress of signal processing technology and the emergence of new system radars, the space electromagnetic environment becomes more and more complex, which puts forward higher requirements for the deinterleaving method of radar signals. Traditional signal deinterleaving algorithms rely heavily on manual experience threshold and have poor robustness. To address this problem, we designed an intelligent radar signal deinterleaving algorithm that was completed by encoding the frequency characteristic matrix and semantic segmentation network, named Sep-RefineNet. The frequency characteristic matrix can well construct the semantic features of different pulse streams of radar signals. The Sep-RefineNet semantic segmentation network can complete pixel-level segmentation of the frequency characteristic matrix and finally uses position decoding and verification to obtain the position in the original pulse stream to complete radar signals deinterleaving. The proposed method avoids the processing of threshold judgment and pulse sequence search in traditional methods. The results of the experiment show that this algorithm improves the deinterleaving accuracy and has a good against-noise ability of aliasing pulses and missing pulses. Full article
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<p>Radar pulse signals deinterleaving.</p>
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<p>The system framework of radar signals deinterleaving.</p>
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<p>Encoding process of FCM: (<b>a</b>) PRI transformation matrix obtained by the self-correlation difference of the TOA sequence; (<b>b</b>) the statistical potential PRI; (<b>c</b>) generated frequency characteristic matrix.</p>
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<p>The result of label matrix: (<b>a</b>) PRI transform matrix; (<b>b</b>) generated label matrix.</p>
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<p>Visualization image of FCM and label matrix: (<b>a</b>) encoded FCM visualization image; (<b>b</b>) partial enlargement of the FCM; (<b>c</b>) visualization image of the corresponding label matrix; (<b>d</b>) partial enlargement of the label matrix.</p>
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<p>The network structure of Sep-RefineNet.</p>
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<p>Schematic diagram of the Sep-Residual unit: (<b>a</b>) original ResNet50 residual block [<a href="#B23-applsci-13-02726" class="html-bibr">23</a>]; (<b>b</b>) improved Sep-Residual unit; (<b>b</b>) multiple channels and multiple receptive fields, which can better extract the characteristics of the signal.</p>
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<p>Schematic diagram of the unit structure: (<b>a</b>) Multi-resolution Fusion; (<b>b</b>) Chained Residual Pooling [<a href="#B25-applsci-13-02726" class="html-bibr">25</a>].</p>
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<p>Radar pulse stream in presence of aliasing pulse and missing pulse.</p>
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<p>The partial enlargement of the FCM results for the test data: (<b>a</b>) FCM after pulse stream coding; (<b>b</b>) paired label matrix; (<b>c</b>) prediction result of FCM. The red arrow is the difference between label matrix and prediction result.</p>
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<p>The partial enlargement of the FCM results for the test data: (<b>a</b>) FCM after pulse stream coding; (<b>b</b>) paired label matrix; (<b>c</b>) prediction result of FCM. The red arrow is the difference between label matrix and prediction result.</p>
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<p>Comparison results of the improved Sep-residual unit and focal loss that respectively replace the original residual unit and cross entropy. The red solid line is the result of SRU and FL. Blue dotted line, black dotted line, and green dotted line are the results of ORU and FL, SRU and CE, and ORU and CE, respectively.</p>
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<p>The results of traditional SDIF algorithm sorts potential PRI. The blue line represents the potential PRI, which is estimated by the histogram statistics. The red curve represents the threshold function, and its degree of curvature and position translation are adjusted by manual parameters α and <span class="html-italic">k</span> in Equation (2). When the potential PRI exceeds the threshold function, this PRI is selected for pulse sequence search to complete signal deinterleaving. (<b>a</b>) The SDIF algorithm successfully sorts out potential PRI; (<b>b</b>) the potential PRI does not exceed the threshold, which means this potential PRI sorting failed.</p>
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<p>Comparison of Sep-RefineNet and traditional deinterleaving algorithms.</p>
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17 pages, 6056 KiB  
Article
Research on the Path Planning of Unmanned Sweepers Based on a Fusion Algorithm
by Yongjie Ma, Peng Ping and Quan Shi
Appl. Sci. 2023, 13(4), 2725; https://doi.org/10.3390/app13042725 - 20 Feb 2023
Cited by 2 | Viewed by 1838
Abstract
Path planning is one of the key technologies for unmanned driving. However, global paths are unable to avoid unknown obstacles, while local paths tend to fall into local optimality. To solve the problem of unsmooth and inefficient paths on multi-angle roads in a [...] Read more.
Path planning is one of the key technologies for unmanned driving. However, global paths are unable to avoid unknown obstacles, while local paths tend to fall into local optimality. To solve the problem of unsmooth and inefficient paths on multi-angle roads in a park which cannot avoid unknown obstacles, we designed a new fusion algorithm based on the improved A* and Open_Planner algorithms (A-OP). In order to make the global route smoother and more efficient, we first extracted the key points of the A* algorithm and improved the node search structure using heap sorting, and then improved the smoothness of the path using the minimum snap method; secondly, we extracted the key points of the A* algorithm as intermediate nodes in the planning of the Open_Planner algorithm, and used the A-OP algorithm to implement the path planning of the unmanned sweeper. The simulation results show that the improved A* algorithm significantly improved the planning efficiency, the nodes are less computed and the path is smoother. The fused A-OP algorithm not only accomplished global planning effectively, but also avoided unknown obstacles in the path. Full article
(This article belongs to the Section Computing and Artificial Intelligence)
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<p>Diagram of distance measurement methods.</p>
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<p>Minimum heap sort process.</p>
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<p>Key point extraction diagram. (The red square is the starting point, the blue square and the yellow square are the characteristic points in the path, and the green square is the ending point).</p>
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<p>Schematic diagram of the continuity constraint.</p>
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<p>Components of rollouts.</p>
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<p>Flow chart of fusion algorithm.</p>
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<p>Traditional A* algorithm and improved A* algorithm. (<b>a</b>) Case 1, (<b>b</b>) Case 2, (<b>c</b>) Case 1 (<b>d</b>) Case 2. (The red number in the figure represents the number of nodes in the path, the blue solid line is the planned route, the black grid is the obstacle, and the white grid is the driving area).</p>
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<p>Comparison of the number of nodes.</p>
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<p>Path-smoothing experiments. (<b>a</b>) traditional algorithms, (<b>b</b>) smooth processing path.</p>
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<p>Simulation experiments of A-OP fusion algorithm. (<b>a</b>) simple environment, (<b>b</b>) complex environments.</p>
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<p>Simulated vehicle status diagram.</p>
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<p>Unmanned sweeper for the experiment.</p>
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<p>Environment map. (<b>a</b>) Simple environment map (<b>b</b>) Complex environment map.</p>
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<p>Global planning route. (<b>a</b>) Simple environment map; (<b>b</b>) complex environment map.</p>
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<p>Obstacle avoidance experiments.</p>
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<p>Algorithm performance. (<b>a</b>) Planning time, (<b>b</b>) Path length.</p>
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11 pages, 1134 KiB  
Article
Document-Level Event Role Filler Extraction Using Key-Value Memory Network
by Hao Wang, Miao Li, Jianyong Duan, Li He and Qing Zhang
Appl. Sci. 2023, 13(4), 2724; https://doi.org/10.3390/app13042724 - 20 Feb 2023
Viewed by 1680
Abstract
Previous work has demonstrated that end-to-end neural sequence models work well for document-level event role filler extraction. However, the end-to-end neural network model suffers from the problem of not being able to utilize global information, resulting in incomplete extraction of document-level event arguments. [...] Read more.
Previous work has demonstrated that end-to-end neural sequence models work well for document-level event role filler extraction. However, the end-to-end neural network model suffers from the problem of not being able to utilize global information, resulting in incomplete extraction of document-level event arguments. This is because the inputs to BiLSTM are all single-word vectors with no input of contextual information. This phenomenon is particularly pronounced at the document level. To address this problem, we propose key-value memory networks to enhance document-level contextual information, and the overall model is represented at two levels: the sentence-level and document-level. At the sentence-level, we use BiLSTM to obtain key sentence information. At the document-level, we use a key-value memory network to enhance document-level representations by recording information about those words in articles that are sensitive to contextual similarity. We fuse two levels of contextual information by means of a fusion formula. We perform various experimental validations on the MUC-4 dataset, and the results show that the model using key-value memory networks works better than the other models. Full article
(This article belongs to the Special Issue Natural Language Processing (NLP) and Applications)
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<p>Document-level event fill argument element-extraction task.</p>
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<p>Hierarchical model diagram based on the key-value memory network.</p>
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19 pages, 4002 KiB  
Article
The Modular Gait Design of a Soft, Earthworm-like Locomotion Robot Driven by Ultra-Low Frequency Excitation
by Zhifeng Qi and Xiuting Sun
Appl. Sci. 2023, 13(4), 2723; https://doi.org/10.3390/app13042723 - 20 Feb 2023
Cited by 4 | Viewed by 2027
Abstract
In complex and extreme environments, such as pipelines and polluted waters, gait programming has great significance for multibody segment locomotion robots. The earthworm-like locomotion robot is a representative multibody bionic robot, which has the characteristics of low weight, multibody segments, and excellent movement [...] Read more.
In complex and extreme environments, such as pipelines and polluted waters, gait programming has great significance for multibody segment locomotion robots. The earthworm-like locomotion robot is a representative multibody bionic robot, which has the characteristics of low weight, multibody segments, and excellent movement performance under the designed gait. The body segment cell can realize large deformation under ultra-low frequency excitation. The multibody segment robot can locomote under ultra-low frequency excitation with appropriate shifts. In this paper, a modular gait design principle for a soft, earthworm-like locomotion robot is proposed. The driven modules defined by modular gait generation correspond to the peristaltic wave transmissions of the excitation in the robot for different modular gait modes. A locomotion algorithm is presented to simulate the locomotion of the earthworm-like robot under different locomotion gaits. Moreover, the locomotion speeds are obtained for different modular gait modes. The results show that locomotion speed is related to the original state of the body segments and modular gaits. As the initial actuated segments and driven modules (which correspond to the excitation frequency and shift) increase, faster movement speeds can be realized, which resolves the speed saturation of the earthworm-like robot. The proposed modular gait design method gives a new gait generation principle for the improvement of the locomotion performance of soft, earthworm-like robots. Full article
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<p>A model schematic diagram and the deformation response of a body segment from the earthworm-like robot driven by a dielectric elastomer actuator. (<b>a</b>) A diagram of the body segment deformation. <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mrow> <mi>d</mi> <mi>r</mi> <mi>i</mi> <mi>v</mi> <mi>e</mi> <mi>n</mi> </mrow> </msub> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> is the ultra-low frequency excitation. Gray represents the initial state of the segment, and blue represents the actuation state of the segment. “A” indicates the actuator; gray indicates the inactive state, and red indicates the active state. (<b>b</b>) A dynamic model of the body segment. (<b>c</b>) The response of the body segment under excitation by sinusoidal excitation voltage. The yellow line represents the simulated body segment length deformation, and the blue line represents the excitation voltage.</p>
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<p>The kinematic state definition of the body segment of the earthworm and the earthworm-like robot. A schematic diagram of the earthworm muscles contracting the segment (<b>a</b>). The initial state of the bionic segment represents “0” in (<b>b</b>). A schematic diagram of the earthworm muscle elongating segment is shown in (<b>c</b>). The final state “1” of the bionic segment with actuation, is shown in (<b>d</b>).</p>
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<p>The initial distribution of the U-DM for a 12-segment earthworm-like locomotion robot. (<b>a</b>) The initial distribution of the U-DM with three actuated segments. (<b>b</b>) The initial distribution of the U-DM with four actuated segments.</p>
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<p>The initial distribution of the B-DM with four segments for a 12-segment earthworm-like locomotion robot. (<b>a</b>) A broken, nonactuated body segment exists in the driven module (“1011”). (<b>b</b>) The nonactuated body segment is located at the boundary of the driven module (“0111”).</p>
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<p>Routine of the generation algorithm for MG-I.</p>
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<p>A gait generation demonstration for a 12-segment earthworm-like robot with two different drive modules for MG-I. A gait generation demonstration for a 12-segment robot with U-DM is shown in (<b>a</b>). The frequency of receding peristaltic wave is 1/3. The amplitude of the receding peristaltic wave is 4. A gait generation demonstration for a 12-segment robot under B-DM (“0111”) is shown in (<b>b</b>). The frequency of receding peristaltic wave is 1/3. The amplitude of the receding peristaltic wave is 3.</p>
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<p>Routine of the generation algorithm for MG-II.</p>
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<p>The gait generation demonstrations for a 12-segment robot with two different driven modules with MG-II. The “K” indicates keeping the previous state segments. A gait generation demonstration for a 12-segment robot under U-DM is shown in (<b>a</b>). The frequency of the receding peristaltic wave is 1/4. The amplitude of the receding peristaltic wave is 3. A gait generation demonstration for a 12-segment robot under B-DM (“0111”) is shown in (<b>b</b>). The frequency of the receding peristaltic wave is 1/6. The amplitude of the receding peristaltic wave is 2.</p>
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<p>Routine of locomotion simulation of the earthworm-like robot driven by ultra-low frequency excitation.</p>
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<p>Locomotion simulations of a 12-segment earthworm-like robot based on U-DM under MG-I. The line located in the number is the locomotion tracks of the body segments. (<b>a</b>) The U-DM contains three actuated segments. (<b>b</b>) The U-DM consists of four actuated segments.</p>
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<p>Locomotion simulations of a 12-segment earthworm-like robot based on U-DM with MG-II. The line located in the number is the locomotion tracks of the body segments. The driven module consists of four actuated segments. (<b>a</b>) The transmission segments contain two segments. (<b>b</b>) The transmission segments contain three segments.</p>
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<p>Locomotion simulations of a 12-segment earthworm-like robot based on B-DM with MG-I. The line located in the number is the locomotion tracks of the body segments. (<b>a</b>) The B-DM for four body segments has two actuated segments (“1001”). (<b>b</b>) The B-DM for four body segments has three actuated segments (“1011”).</p>
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<p>Locomotion simulations of a 12-segment earthworm-like robot based on B-DM with MG-II. The line located in the number is the locomotion tracks of body segments. Three actuated segments in the B-DM of four body segments (“1011”). (<b>a</b>) The transmission segments consist of two segments. (<b>b</b>) The transmission segments consist of three segments.</p>
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18 pages, 6034 KiB  
Article
Error Similarity Analysis and Error Compensation of Industrial Robots with Uncertainties of TCP Calibration
by Yufei Li, Bo Li, Xidong Zhao, Simiao Cheng, Wei Zhang and Wei Tian
Appl. Sci. 2023, 13(4), 2722; https://doi.org/10.3390/app13042722 - 20 Feb 2023
Cited by 7 | Viewed by 2590
Abstract
The machining system based on an industrial robot is a new type of equipment to meet the requirements of high quality, high efficiency and high flexibility for large and complex components of aircraft and spacecraft. The error compensation technology is widely used in [...] Read more.
The machining system based on an industrial robot is a new type of equipment to meet the requirements of high quality, high efficiency and high flexibility for large and complex components of aircraft and spacecraft. The error compensation technology is widely used in robotic machining to improve the positioning accuracy of an industrial robot with the intention of meeting the precision requirements of aerospace manufacturing. However, the robot’s positioning accuracy decreases significantly when the orientation of the tool changes dramatically. This stems from the fact that the existing robot compensation methods ignore the uncertainties of Tool Center Point (TCP) calibration. This paper presents a novel regionalized compensation method for improving the positioning accuracy of the robot with calibration uncertainties and large orientation variation of the TCP. The method is experimentally validated through the drilling of curved surface parts of plexiglass using a KUKA KR2830MT robot. Compared with a published error compensation method, the proposed approach improves the positioning accuracy of the robot under the large orientation variation to 0.235 mm. This research can broaden the field of robot calibration technology and further improve the adaptability of robotic machining. Full article
(This article belongs to the Section Robotics and Automation)
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<p>Working scenarios of existing robotic drilling systems. (<b>a</b>) NUAA robotic drilling system (<b>b</b>) NUAA dual-robot cooperative drilling and riveting system.</p>
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<p>DH model of KUKA KR500-2830.</p>
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<p>Error similarity analysis without TCP calibration error. (<b>a</b>) Similarity in the x-axis; (<b>b</b>) similarity in the y-axis; (<b>c</b>) similarity in the z-axis.</p>
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<p>Error similarity analysis with TCP calibration error within ±1 mm. (<b>a</b>) Similarity in the x-axis; (<b>b</b>) similarity in the y-axis; (<b>c</b>) similarity in the z-axis.</p>
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<p>Error similarity analysis with TCP calibration error within ±5 mm (<b>a</b>) Similarity in the x-axis; (<b>b</b>) similarity in the y-axis; (<b>c</b>) similarity in the z-axis.</p>
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<p>Regionalized error similarity compensation method.</p>
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<p>Robot error compensation process.</p>
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<p>Experimental setup of the robotic drilling system.</p>
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<p>Robotic drilling task. (<b>a</b>) Region division of robotic drilling task; (<b>b</b>) Sampling area division of robotic drilling task.</p>
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<p>Experimental results of robot compensation. (<b>a</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math> (<b>b</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>2</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>3</mn> </msub> </mrow> </semantics></math>; (<b>d</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>4</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Experimental results of robot compensation. (<b>a</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math> (<b>b</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>2</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>3</mn> </msub> </mrow> </semantics></math>; (<b>d</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>4</mn> </msub> </mrow> </semantics></math>.</p>
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<p>Spatial correlation analysis of residual error. (<b>a</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math> vs. distance; (<b>b</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>1</mn> </msub> </mrow> </semantics></math> vs. angle deviation; (<b>c</b>) Positioning error of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="italic">Ω</mi> <mn>2</mn> </msub> </mrow> </semantics></math> vs. distance and angle deviation.</p>
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26 pages, 12961 KiB  
Article
Multi-Robot Collaborative Flexible Manufacturing and Digital Twin System Design of Circuit Breakers
by Linghao Wang, Liang Shu and Hao Zhou
Appl. Sci. 2023, 13(4), 2721; https://doi.org/10.3390/app13042721 - 20 Feb 2023
Cited by 3 | Viewed by 3334
Abstract
Circuit breakers (CBs) are mainly designed to interrupt current flow when faults are detected and have been widely used in industrial applications. The existing CBs manufacturing method is semi-automatic and requires a lot of labor. To realize flexible manufacturing, a multi-robot cooperative CBs [...] Read more.
Circuit breakers (CBs) are mainly designed to interrupt current flow when faults are detected and have been widely used in industrial applications. The existing CBs manufacturing method is semi-automatic and requires a lot of labor. To realize flexible manufacturing, a multi-robot cooperative CBs flexible manufacturing system (CBFMS) is presented in this study. Aiming at the efficiency of the multi-robot cooperative CBFMS key units, a two-arm cooperation robot approach is proposed. The reinforcement learning algorithm is developed to optimize the manufacturing trajectory of the two-arm cooperation robot. To build and optimize the multi-robot cooperative CBFMS, a digital twin (DT) system describing all physical properties of the physical manufacturing plant is constructed for simulation. In the developed DT system, a kinematic control model of the collaboration robot is established. A real-time display of the robot’s trajectory, manufacturing status, and process manufacturing is provided by the data interaction with the physical cell flow between the units. Following this design, a synchronous mapping between the flexible manufacturing DT system of the CBs and the physical workshop is realized, which enables real-time monitoring and management of the physical production line. The experiments’ results show that the manufacturing efficiency, compared with traditional CBs production, is improved by 22%. Moreover, the multi-robot cooperative CBFMS can make process changes according to the production requirements, which can improve the stability of production. Full article
(This article belongs to the Topic Virtual Reality, Digital Twins, the Metaverse)
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<p>Internal structure and parts composition of a CB.</p>
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<p>Traditional CBs semi-automatic production line.</p>
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<p>Single-robot flexible manufacturing system: (<b>a</b>) Crucial unit of parts’ posture adjustment; (<b>b</b>) Individual part attitude adjustment process.</p>
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<p>The construction of the multi-robot collaborative CBs flexible manufacturing system.</p>
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<p>Robot’s flexible multi-gripper claw construction.</p>
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<p>The assembly mode of two-arm cooperation robot.</p>
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<p>Framework of the DT flexible manufacturing system.</p>
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<p>Two-arm cooperation robot’s D-H coordinate system.</p>
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<p>Monte Carlo method collaborative spatial point cloud map.</p>
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<p>Key points in collaborative manufacturing of two-arm cooperation robot.</p>
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<p>Reinforcement learning mechanism.</p>
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<p>DDPG algorithm framework.</p>
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<p>Two-arm cooperation robot in Unity environment.</p>
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<p>Convergence iteration curve during training.</p>
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<p>The success rate of the robot in completing the task.</p>
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<p>Two-arm cooperation robots working together to grip parts.</p>
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<p>Deviation between actual position and ideal target position.</p>
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<p>Logical relation construction of robot model.</p>
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<p>Comparison before and after model optimization.</p>
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<p>Kinematic control algorithm for robot model: (<b>a</b>) Digital twin model; (<b>b</b>) Kinematic algorithm; (<b>c</b>) Animator control.</p>
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<p>Model bounding volume handling: (<b>a</b>) The directional bounding volume; (<b>b</b>) The double-layer construction bounding volume; (<b>c</b>) The axis-aligned bounding volume.</p>
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<p>Principle of the collision detection algorithm: (<b>a</b>) Status one; (<b>b</b>) Status two; (<b>c</b>) Status three.</p>
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<p>Logic judgment detection algorithm flowchart.</p>
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<p>Twin system data communication mechanisms.</p>
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<p>Two-arm cooperation robot physical prototype.</p>
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<p>Main interface of DT system of multi-robot cooperative CBFMS.</p>
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<p>DT system unit interface of multi-robot cooperative CBFMS.</p>
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<p>System display in the event of a fault.</p>
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