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30 pages, 9485 KiB  
Article
Research on Path Planning Algorithm of Driverless Ferry Vehicles Combining Improved A* and DWA
by Zhaohong Wang and Gang Li
Sensors 2024, 24(13), 4041; https://doi.org/10.3390/s24134041 (registering DOI) - 21 Jun 2024
Abstract
In view of the fact that the global planning algorithm cannot avoid unknown dynamic and static obstacles and the local planning algorithm easily falls into local optimization in large-scale environments, an improved path planning algorithm based on the integration of A* and DWA [...] Read more.
In view of the fact that the global planning algorithm cannot avoid unknown dynamic and static obstacles and the local planning algorithm easily falls into local optimization in large-scale environments, an improved path planning algorithm based on the integration of A* and DWA is proposed and applied to driverless ferry vehicles. Aiming at the traditional A* algorithm, the vector angle cosine value is introduced to improve the heuristic function to enhance the search direction; the search neighborhood is expanded and optimized to improve the search efficiency; aiming at the problem that there are many turning points in the A* algorithm, a cubic quasi-uniform B-spline curve is used to smooth the path. At the same time, fuzzy control theory is introduced to improve the traditional DWA so that the weight coefficient of the evaluation function can be dynamically adjusted in different environments, effectively avoiding the problem of a local optimal solution. Through the fusion of the improved DWA and the improved A* algorithm, the key nodes in global planning are used as sub-target punctuation to guide the DWA for local planning, so as to ensure that the ferry vehicle avoids obstacles in real time. Simulation results show that the fusion algorithm can avoid unknown dynamic and static obstacles efficiently and in real time on the basis of obtaining the global optimal path. In different environment maps, the effectiveness and adaptability of the fusion algorithm are verified. Full article
(This article belongs to the Section Vehicular Sensing)
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<p>Raster map and raster location marker map.</p>
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<p>Vector diagram.</p>
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<p>Comparison of heuristic functions before and after the improved A* algorithm. (<b>a</b>) Traditional A*; (<b>b</b>) improved A* of the heuristic function.</p>
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<p>Search the neighborhood with 3 × 3.</p>
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<p>Search the neighborhood with 5 × 5.</p>
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<p>Schematic diagram of the planning result. The lines represent the searched paths and the circles represent the searched nodes. (<b>a</b>) Search the neighborhood with 3 × 3; (<b>b</b>) search the neighborhood with 5 × 5.</p>
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<p>Results of different searches for neighborhood planning. (<b>a</b>) Map 1; (<b>b</b>) Map 2.</p>
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<p>Smoothed path. (<b>a</b>) Map 1; (<b>b</b>) Map 2.</p>
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<p>Flow chart of DWA algorithm.</p>
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<p>The sports degree posture of the driverless ferry vehicle.</p>
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<p>Speed sampling space of ferry vehicles.</p>
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<p>Trajectory prediction map.</p>
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<p>Scene one.</p>
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<p>Scene two.</p>
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<p>Scene three.</p>
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<p>Fuzzy controller framework.</p>
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<p><math display="inline"><semantics> <mrow> <mi>O</mi> <mi>d</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>G</mi> <mi>d</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>H</mi> <mi>d</mi> </mrow> </semantics></math> membership function. (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>O</mi> <mi>d</mi> </mrow> </semantics></math> membership function; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>G</mi> <mi>d</mi> </mrow> </semantics></math> membership function; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>H</mi> <mi>d</mi> </mrow> </semantics></math> membership function.</p>
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<p>Membership function of output. (<b>a</b>) <math display="inline"><semantics> <mi>α</mi> </semantics></math>, <math display="inline"><semantics> <mi>β</mi> </semantics></math>, and <math display="inline"><semantics> <mi>ε</mi> </semantics></math> membership function; (<b>b</b>) <math display="inline"><semantics> <mi>γ</mi> </semantics></math> membership function.</p>
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<p>Directional fuzzy controller.</p>
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<p>Safety fuzzy controller.</p>
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<p>Fusion fuzzy controller.</p>
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<p>Fuzzy regular three-dimensional surface graph. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mn>1</mn> </msub> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mn>2</mn> </msub> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mn>3</mn> </msub> </mrow> </semantics></math>.</p>
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<p>The simulation results of fuzzy DWA in scene 1. (<b>a</b>) Path; (<b>b</b>) <math display="inline"><semantics> <mi>α</mi> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mi>β</mi> </semantics></math>; (<b>d</b>) <math display="inline"><semantics> <mi>γ</mi> </semantics></math>.</p>
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<p>The simulation results of fuzzy DWA in scene 2. (<b>a</b>) Path; (<b>b</b>) <math display="inline"><semantics> <mi>α</mi> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mi>β</mi> </semantics></math>; (<b>d</b>) <math display="inline"><semantics> <mi>γ</mi> </semantics></math>.</p>
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<p>The simulation results of fuzzy DWA in scene 3. (<b>a</b>) Path; (<b>b</b>) <math display="inline"><semantics> <mi>α</mi> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mi>β</mi> </semantics></math>; (<b>d</b>) <math display="inline"><semantics> <mi>γ</mi> </semantics></math>.</p>
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<p>Algorithm fusion flow chart.</p>
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<p>Simulation results of the fusion algorithm in a known static environment. (<b>a</b>) Environmental map; (<b>b</b>) Simulation results of fusion algorithm.</p>
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<p>Simulation results of the fusion algorithm in an environment with unknown dynamic and static obstacles. (<b>a</b>) Bypass the first static obstacle. (<b>b</b>) Encounter dynamic obstacles. (<b>c</b>) Bypass dynamic obstacles. (<b>d</b>) Bypass the second static obstacle and reach the target point.</p>
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<p>Change of weight coefficient of the fusion algorithm in the environment with unknown dynamic and static obstacles. (<b>a</b>) <math display="inline"><semantics> <mi>α</mi> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mi>β</mi> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mi>γ</mi> </semantics></math>.</p>
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<p>Variation in linear velocity and angular velocity of ferry vehicles. (<b>a</b>) Linear velocity variation curve; (<b>b</b>) angular velocity variation curve.</p>
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<p>Simulation experiment results of a 30 × 30 environment map. (<b>a</b>) Environment without unknown obstacles. (<b>b</b>) Encounter dynamic obstacles and turn. (<b>c</b>) Successfully circumvent dynamic obstacles. (<b>d</b>) Move the static obstacle around and reach the target point.</p>
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<p>The change in output weight coefficient in the presence of unknown dynamic and static obstacles. (<b>a</b>) <math display="inline"><semantics> <mi>α</mi> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mi>β</mi> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mi>γ</mi> </semantics></math>.</p>
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<p>Simulation and comparison results of different algorithms. (<b>a</b>) 20 × 20 environment map; (<b>b</b>) 30 × 30 environment map.</p>
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11 pages, 2788 KiB  
Article
Pinpointing Moisture: The Capacitive Detection for Standing Tree Health
by Jianan Yao, Zonglin Zhen, Huadong Xu, Liming Zhao, Yuying Duan and Xuhui Guo
Sensors 2024, 24(13), 4040; https://doi.org/10.3390/s24134040 (registering DOI) - 21 Jun 2024
Abstract
Background: the feasibility of the capacitance method for detecting the water content in standing tree trunks was investigated using capacitance-based equipment that was designed for measuring the water content of standing tree trunks. Methods: In laboratory experiments, the best insertion depth of the [...] Read more.
Background: the feasibility of the capacitance method for detecting the water content in standing tree trunks was investigated using capacitance-based equipment that was designed for measuring the water content of standing tree trunks. Methods: In laboratory experiments, the best insertion depth of the probe for standing wood was determined by measurement experiments conducted at various depths. The bark was to be peeled when specimens and standing wood were being measured. The actual water content of the test object was obtained by specimens being weighed and the standing wood being weighed after the wood core was extracted. Results: A forecast of the moisture content of standing wood within a range of 0 to 180% was achieved by the measuring instrument. The feasibility of the device for basswood and fir trees is preliminarily studied. When compared to the drying method, the average error of the test results was found to be less than 8%, with basswood at 7.75%, and fir at 7.35%. Conclusions: It was concluded that the measuring instrument has a wide measuring range and is suitable for measuring wood with low moisture content, as well as standing timber with high moisture content. The measuring instrument, being small in size, easy to carry, and capable of switching modes, is considered to have a good application prospect in the field of forest precision monitoring and quality improvement. Full article
(This article belongs to the Topic Advances in Non-Destructive Testing Methods, 2nd Volume)
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<p>Plane−parallel capacitor.</p>
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<p>Block diagram of the system of standing tree trunk moisture content measurement.</p>
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<p>555 multiple resonant swing circuit diagram.</p>
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<p>Key schematic diagram.</p>
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<p>Standing tree trunk moisture meter. (<b>a</b>): front view of the instrument. (<b>b</b>) field measurement of tree moisture content.</p>
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<p>Relation diagram of insertion depth and electromagnetic wave period in water medium test. (<b>a</b>) Distilled water medium test; (<b>b</b>) fitted curve of the average of six experiments.</p>
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<p>Fitting diagram of electromagnetic wave period and water content of basswood and fir. (<b>a</b>) Basswood; (<b>b</b>) fir.</p>
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<p>Comparison diagram of water content fitting curve between capacitive method and drying method of basswood and fir. (<b>a</b>) Basswood; (<b>b</b>) fir.</p>
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<p>Comparison of basswood and fir measurements with real data. (<b>a</b>) Basswood; (<b>b</b>) fir.</p>
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37 pages, 6754 KiB  
Article
SC-AOF: A Sliding Camera and Asymmetric Optical-Flow-Based Blending Method for Image Stitching
by Jiayi Chang, Qin Li, Yanju Liang and Liguo Zhou
Sensors 2024, 24(13), 4035; https://doi.org/10.3390/s24134035 (registering DOI) - 21 Jun 2024
Abstract
Parallax processing and structure preservation have long been important and challenging tasks in image stitching. In this paper, an image stitching method based on sliding camera to eliminate perspective deformation and asymmetric optical flow to solve parallax is proposed. By maintaining the viewpoint [...] Read more.
Parallax processing and structure preservation have long been important and challenging tasks in image stitching. In this paper, an image stitching method based on sliding camera to eliminate perspective deformation and asymmetric optical flow to solve parallax is proposed. By maintaining the viewpoint of two input images in the mosaic non-overlapping area and creating a virtual camera by interpolation in the overlapping area, the viewpoint is gradually transformed from one to another so as to complete the smooth transition of the two image viewpoints and reduce perspective deformation. Two coarsely aligned warped images are generated with the help of a global projection plane. After that, the optical flow propagation and gradient descent method are used to quickly calculate the bidirectional asymmetric optical flow between the two warped images, and the optical-flow-based method is used to further align the two warped images to reduce parallax. In the image blending, the softmax function and registration error are used to adjust the width of the blending area, further eliminating ghosting and reducing parallax. Finally, by comparing our method with APAP, AANAP, SPHP, SPW, TFT, and REW, it has been proven that our method can not only effectively solve perspective deformation, but also gives more natural transitions between images. At the same time, our method can robustly reduce local misalignment in various scenarios, with higher structural similarity index. A scoring method combining subjective and objective evaluations of perspective deformation, local alignment and runtime is defined and used to rate all methods, where our method ranks first. Full article
(This article belongs to the Section Sensing and Imaging)
17 pages, 21254 KiB  
Article
A Two-Axis Orthogonal Resonator for Variable Sensitivity Mode Localization Sensing
by Yuta Nagasaka, Alessia Baronchelli, Shuji Tanaka and Takashiro Tsukamoto
Sensors 2024, 24(13), 4038; https://doi.org/10.3390/s24134038 (registering DOI) - 21 Jun 2024
Abstract
This paper experimentally demonstrates a mode localization sensing approach using a single two-axis orthogonal resonator. The resonator consists of concentric multi-rings connected by elliptic springs that enable two orthogonal oscillation modes. By electrostatically tuning the anisotropic stiffness between the two axes, the effective [...] Read more.
This paper experimentally demonstrates a mode localization sensing approach using a single two-axis orthogonal resonator. The resonator consists of concentric multi-rings connected by elliptic springs that enable two orthogonal oscillation modes. By electrostatically tuning the anisotropic stiffness between the two axes, the effective coupling stiffness between the modes can be precisely controlled down to near-zero values. This allows the sensitivity of mode localization sensing to be tuned over a wide range. An order of magnitude enhancement in sensitivity is experimentally achieved by reducing the coupling stiffness towards zero. The resonator’s simple single-mass structure offers advantages over conventional coupled resonator designs for compact, tunable mode localization sensors. Both positive and negative values of coupling stiffness are demonstrated, enabling maximum sensitivity at the point where coupling crosses through zero. A method for decomposing overlapping resonance peaks is introduced to accurately measure the amplitude ratios of the localized modes even at high sensitivities. The electrostatic tuning approach provides a new option for realizing variable sensitivity mode localization devices using a simplified resonator geometry. Full article
(This article belongs to the Special Issue MEMS and NEMS Sensors: 2nd Edition)
18 pages, 6098 KiB  
Article
Photovoltaic Power Injection Control Based on a Virtual Synchronous Machine Strategy
by Miguel Albornoz, Jaime Rohten, José Espinoza, Jorge Varela, Daniel Sbarbaro and Yandi Gallego
Sensors 2024, 24(13), 4039; https://doi.org/10.3390/s24134039 (registering DOI) - 21 Jun 2024
Abstract
The increasing participation of photovoltaic sources in power grids presents the challenge of enhancing power quality, which is affected by the intrinsic characteristics of these sources, such as variability and lack of inertia. This power quality degradation mainly generates variations in both voltage [...] Read more.
The increasing participation of photovoltaic sources in power grids presents the challenge of enhancing power quality, which is affected by the intrinsic characteristics of these sources, such as variability and lack of inertia. This power quality degradation mainly generates variations in both voltage magnitude and frequency, which are more pronounced in microgrids. In fact, the magnitude problem is particularly present in the distribution systems, where photovoltaic sources are spread along the grid. Due to the power converter’s lack of inertia, frequency problems can be seen throughout the network. Grid-forming control strategies in photovoltaic systems have been proposed to address these problems, although most proposed solutions involve either a direct voltage source or energy storage systems, thereby increasing costs. In this paper, a photovoltaic injection system is designed with a virtual synchronous machine control strategy to provide voltage and frequency support to the grid. The maximum power point tracking algorithm is adapted to provide the direct voltage reference and inject active power according to the droop frequency control. The control strategy is validated through simulations and key experimental setup tests. The results demonstrate that it is possible to inject photovoltaic power and provide voltage and frequency support. Full article
(This article belongs to the Special Issue Advances in Sensor Technologies for Microgrid and Energy Storage)
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<p>(<b>a</b>) Inverter and (<b>b</b>) synchronous machine connected to the infinite bus.</p>
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<p>DC voltage control loop.</p>
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<p>(<b>a</b>) Root locus and (<b>b</b>) step response of the DC controller.</p>
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<p>Small-signal model.</p>
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<p>Simulation of the nonlinear fifth-order model and the reduced linear model, (<b>a</b>) rotor angular speed, (<b>b</b>) power angle, and (<b>c</b>) magnetic flux.</p>
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<p>Step response of active power transfer functions considering torque droop coefficient variation.</p>
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<p>Step response of active power transfer functions considering inertia variation.</p>
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<p>Step response of reactive power transfer functions considering torque droop coefficient variation.</p>
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<p>Step response of reactive power transfer functions considering inertia variation.</p>
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<p>Root locus of synchronverter considering parameters variations, (<b>a</b>) torque droop coefficient varies, (<b>b</b>) inertia varies, and (<b>c</b>) gain <math display="inline"><semantics> <msub> <mi>K</mi> <mi>q</mi> </msub> </semantics></math> varies.</p>
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<p>Single diode solar cell model.</p>
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<p>Solar cell curves, (<b>a</b>) power of the solar cell considering irradiance variation and (<b>b</b>) power of the solar cell considering temperature variation.</p>
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<p>MPPT based on measurement cells.</p>
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<p>Proposed strategy control and power system.</p>
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<p>Simulation results, (<b>a</b>) irradiance step change, (<b>b</b>) active power and frequency, (<b>c</b>) reactive power and grid voltage magnitude, and (<b>d</b>) DC voltage.</p>
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<p>Simulation of synchronverter including frequency droop correction, (<b>a</b>) active power and frequency change, and (<b>b</b>) DC voltage and voltage reference.</p>
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<p>(<b>a</b>) PV modules and (<b>b</b>) experimental setup.</p>
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<p>Experimental results, (<b>a</b>) synchronverter injecting PV power, (<b>b</b>) frequency increment of 1 Hz, (<b>c</b>) sag of 5%, and (<b>d</b>) swell of 5%.</p>
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17 pages, 10021 KiB  
Article
Extraction of Moso Bamboo Parameters Based on the Combination of ALS and TLS Point Cloud Data
by Suying Fan, Sishuo Jing, Wenbing Xu, Bin Wu, Mingzhe Li and Haochen Jing
Sensors 2024, 24(13), 4036; https://doi.org/10.3390/s24134036 (registering DOI) - 21 Jun 2024
Abstract
Extracting moso bamboo parameters from single-source point cloud data has limitations. In this article, a new approach for extracting moso bamboo parameters using airborne laser scanning (ALS) and terrestrial laser scanning (TLS) point cloud data is proposed. Using the field-surveyed coordinates of plot [...] Read more.
Extracting moso bamboo parameters from single-source point cloud data has limitations. In this article, a new approach for extracting moso bamboo parameters using airborne laser scanning (ALS) and terrestrial laser scanning (TLS) point cloud data is proposed. Using the field-surveyed coordinates of plot corner points and the Iterative Closest Point (ICP) algorithm, the ALS and TLS point clouds were aligned. Considering the difference in point distribution of ALS, TLS, and the merged point cloud, individual bamboo plants were segmented from the ALS point cloud using the point cloud segmentation (PCS) algorithm, and individual bamboo plants were segmented from the TLS and the merged point cloud using the comparative shortest-path (CSP) method. The cylinder fitting method was used to estimate the diameter at breast height (DBH) of the segmented bamboo plants. The accuracy was calculated by comparing the bamboo parameter values extracted by the above methods with reference data in three sample plots. The comparison results showed that by using the merged data, the detection rate of moso bamboo plants could reach up to 97.30%; the R2 of the estimated bamboo height was increased to above 0.96, and the root mean square error (RMSE) decreased from 1.14 m at most to a range of 0.35–0.48 m, while the R2 of the DBH fit was increased to a range of 0.97–0.99, and the RMSE decreased from 0.004 m at most to a range of 0.001–0.003 m. The accuracy of moso bamboo parameter extraction was significantly improved by using the merged point cloud data. Full article
(This article belongs to the Special Issue Laser Scanning and Applications)
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<p>Locations of three moso bamboo sample plots (red rectangles).</p>
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<p>Scanner and target locations in a plot.</p>
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<p>Co-registration and cropping of the TLS data in a sample plot. (<b>c</b>) Point cloud captured at the central scan position; (<b>a</b>,<b>b</b>,<b>d</b>,<b>e</b>) point clouds captured at the scan positions on the plot edges; (<b>f</b>) co-registered point cloud; (<b>g</b>) cropped point cloud.</p>
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<p>ALS point cloud. (<b>a</b>) RGB point cloud; (<b>b</b>) elevation-rendering point cloud.</p>
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<p>Alignment of TLS point cloud (red) and ALS point cloud (yellow) in a moso bamboo sample plot. (<b>a</b>) Aligned point cloud; (<b>b</b>) aligned ground point cloud.</p>
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<p>Bamboo segmentation using the PCS algorithm.</p>
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<p>A segment of a bamboo culm point cloud used for cylinder fitting and DBH estimation.</p>
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<p>Moso bamboo segmentation from (<b>a</b>) ALS point cloud, (<b>b</b>) TLS point cloud, and (<b>c</b>) ALS-TLS point cloud. Different colors distinguish the different moso bamboo plants.</p>
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<p>Moso bamboo detection results derived using (<b>a</b>) ALS data, (<b>b</b>) TLS data, and (<b>c</b>) ALS-TLS point cloud.</p>
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<p>DBH estimation by cylindrical fitting based on different data sources. (<b>a</b>,<b>b</b>) Plot A1; (<b>c</b>,<b>d</b>) plot A2; (<b>e</b>,<b>f</b>) plot A3.</p>
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<p>Bamboo height extraction based on different data sources. (<b>a</b>–<b>c</b>) Plot A1; (<b>d</b>–<b>f</b>) plot A2; (<b>g</b>–<b>i</b>) plot A3.</p>
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11 pages, 701 KiB  
Article
Development of a Dynamically Re-Configurable Radio-Frequency Interference Detection System for L-Band Microwave Radiometers
by Adrian Perez-Portero, Jorge Querol, Andreu Mas-Vinolas, Adria Amezaga, Roger Jove-Casulleras and Adriano Camps
Sensors 2024, 24(13), 4034; https://doi.org/10.3390/s24134034 (registering DOI) - 21 Jun 2024
Abstract
Real-Time RFI Detection and Flagging (RT-RDF) for microwave radiometers is a versatile new FPGA algorithm designed to detect and flag Radio-Frequency Interference (RFI) in microwave radiometers. This block utilizes computationally-efficient techniques to identify and analyze RF signals, allowing the system to take appropriate [...] Read more.
Real-Time RFI Detection and Flagging (RT-RDF) for microwave radiometers is a versatile new FPGA algorithm designed to detect and flag Radio-Frequency Interference (RFI) in microwave radiometers. This block utilizes computationally-efficient techniques to identify and analyze RF signals, allowing the system to take appropriate measures to mitigate interference and maintain reliable performance. With L-Band microwave radiometry as the main application, this RFI detection algorithm focuses on the Kurtogram and Spectrogram to detect non-Gaussian behavior. To gain further modularity, an FFT-based filter bank is used to divide the receiver’s bandwidth into several sub-bands within the band of interest of the instrument, depending on the application. Multiple blanking strategies can then be applied in each band using the provided detection flags. The algorithm can be re-configured in the field, for example with dynamic integration times to support operation in different environments, or configurable thresholds to account for variable RFI environments. A validation and testing campaign has been performed on multiple scenarios with the ARIEL commercial microwave radiometer, and the results confirm the excellent performance of the system. Full article
(This article belongs to the Special Issue Techniques and Instrumentation for Microwave Sensing)
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<p>Block diagram of the RFI Detection HDL Block. In yellow, the user inputs (data, configuration), in blue, the RT-RDF stages, and in green the outputs.</p>
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<p>High-level block diagram of the radiometer, showing the antennas and RF frontend on the left and the processing stage within the FPGA on the right.</p>
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<p>Data of the first measurements taken in an RFI-free environment. In (<b>a</b>), the power is captured without the RDDF algorithm enabled, and in (<b>b</b>) with it enabled. The antenna alternates between pointing at the microwave absorber (power closer to hot load) or the sky (power closer to cold load). (<b>c</b>) shows the kurtosis plot divided by sub-band and epoch number. (<b>a</b>) Radiometer’s output power, RFI mitigator OFF; (<b>b</b>) Radiometer’s output power, RFI mitigator ON; (<b>c</b>) Kurtosis.</p>
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<p>Data of the measurements taken in an RFI-free environment and sweeping the frequency of a narrowband interference. (<b>a</b>,<b>b</b>) depict the power detected by the radiometer when the RFI mitigator was disabled and enabled, respectively. (<b>c</b>–<b>e</b>) correspond to the power, kurtosis, and detection flag for the enabled case with respect to the epoch (i.e., duration of the test), respectively. (<b>a</b>) Radiometer’s output power, RFI mitigator OFF; (<b>b</b>) Radiometer’s output power, RFI mitigator ON; (<b>c</b>) Relative power (dB); (<b>d</b>) Kurtosis; (<b>e</b>) RFI detected.</p>
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<p>Data of the measurements taken in an RFI-free environment and decreasingly sweeping the power of a narrowband interference from −10 dBm to −80 dBm. (<b>a</b>) depicts the power detected by the radiometer when the RFI mitigator was enabled. (<b>b</b>–<b>d</b>) correspond to the power, kurtosis, and detection flag with respect to the epoch (i.e., duration of the test), respectively. (<b>a</b>) Radiometer’s output power; (<b>b</b>) Relative power (dB); (<b>c</b>) Kurtosis; (<b>d</b>) RFI detected.</p>
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13 pages, 2124 KiB  
Article
Smart Partitioned Blockchain
by Basem Assiri and Hani Alnami
Sensors 2024, 24(13), 4033; https://doi.org/10.3390/s24134033 (registering DOI) - 21 Jun 2024
Abstract
Blockchain is a developing technology that promises advancements when it is applied to other fields. Applying blockchain to other systems requires a customized blockchain model to satisfy the requirements of different application fields. One important area is to integrate blockchain with smart spaces [...] Read more.
Blockchain is a developing technology that promises advancements when it is applied to other fields. Applying blockchain to other systems requires a customized blockchain model to satisfy the requirements of different application fields. One important area is to integrate blockchain with smart spaces and the Internet of Things to process, manage, and store data. Actually, smart spaces and Internet of Things systems include various types of transactions in terms of sensitivity. The sensitivity can be considered as correctness sensitivity, time sensitivity, and specialization sensitivity. Correctness sensitivity means that the systems should accept precise or approximated data in some cases, whereas time sensitivity means that there are time bounds for each type of transaction, and specialization sensitivity applies when some transactions are processed only by specialized people. Therefore, this work introduces the smart partitioned blockchain model, where we use machine learning and deep learning models to classify transactions into different pools according to their sensitivity levels. Then, each pool is mapped to a specific part of the smart partitioned blockchain model. The parts can be permissioned or permissionless. The permissioned parts can have different sub-parts if needed. Consequently, the smart partitioned blockchain can be customized to meet application-field requirements. In the experimental results, we use bank and medical datasets with a predefined sensitivity threshold for classification accuracy in each system. The bank transactions are critical, whereas the classification of the medical dataset is speculative and less critical. The Random Forest model is used for bank-dataset classification, and its accuracy reaches 100%, whereas Sequential Deep Learning is used for the medical dataset, which reaches 91%. This means that all bank transactions are correctly mapped to the corresponding parts of the blockchain, whereas accuracy is lower for the medical dataset. However, acceptability is determined based on the predefined sensitivity threshold. Full article
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<p>Shows a smart partitioned blockchain with two categories of transactions, which are sensitive and non-sensitive. Consequently, the partitioned blockchain layer has a permissioned part and a permissionless part. The last layer shows the ledger storage.</p>
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<p>Shows a smart partitioned blockchain with three categories of transactions. The partitioned blockchain layer has two sub-parts of permissioned blockchain and one permissionless blockchain part. The last layer shows the ledger.</p>
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<p>Correlation matrix of the health data; the target variable is 0 or 1, where 0 denotes a non-sensitive medical transaction, and 1 indicates a sensitive medical transaction. We classified transactions of patients experiencing a heart attack as sensitive transactions.</p>
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<p>Confusion matrix of bank-transaction-status detection.</p>
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<p>Part (<b>a</b>) shows the application of smart partitioned blockchain on the bank dataset with three categories of transactions that are mapped to three parts of the blockchain, whereas part (<b>b</b>) shows the application of a smart partitioned blockchain to the medical dataset, with two categories that are mapped to two parts of the blockchain.</p>
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26 pages, 11261 KiB  
Article
A Novel Simulation Method for 3D Digital-Image Correlation: Combining Virtual Stereo Vision and Image Super-Resolution Reconstruction
by Hao Chen, Hao Li, Guohua Liu and Zhenyu Wang
Sensors 2024, 24(13), 4031; https://doi.org/10.3390/s24134031 (registering DOI) - 21 Jun 2024
Abstract
3D digital-image correlation (3D-DIC) is a non-contact optical technique for full-field shape, displacement, and deformation measurement. Given the high experimental hardware costs associated with 3D-DIC, the development of high-fidelity 3D-DIC simulations holds significant value. However, existing research on 3D-DIC simulation was mainly carried [...] Read more.
3D digital-image correlation (3D-DIC) is a non-contact optical technique for full-field shape, displacement, and deformation measurement. Given the high experimental hardware costs associated with 3D-DIC, the development of high-fidelity 3D-DIC simulations holds significant value. However, existing research on 3D-DIC simulation was mainly carried out through the generation of random speckle images. This study innovatively proposes a complete 3D-DIC simulation method involving optical simulation and mechanical simulation and integrating 3D-DIC, virtual stereo vision, and image super-resolution reconstruction technology. Virtual stereo vision can reduce hardware costs and eliminate camera-synchronization errors. Image super-resolution reconstruction can compensate for the decrease in precision caused by image-resolution loss. An array of software tools such as ANSYS SPEOS 2024R1, ZEMAX 2024R1, MECHANICAL 2024R1, and MULTIDIC v1.1.0 are used to implement this simulation. Measurement systems based on stereo vision and virtual stereo vision were built and tested for use in 3D-DIC. The results of the simulation experiment show that when the synchronization error of the basic stereo-vision system (BSS) is within 103 time steps, the reconstruction error is within 0.005 mm and the accuracy of the virtual stereo-vision system is between the BSS’s synchronization error of 107 and 106 time steps. In addition, after image super-resolution reconstruction technology is applied, the reconstruction error will be reduced to within 0.002 mm. The simulation method proposed in this study can provide a novel research path for existing researchers in the field while also offering the opportunity for researchers without access to costly hardware to participate in related research. Full article
(This article belongs to the Section Sensing and Imaging)
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<p>Schematic diagram of reference subset and target subset.</p>
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<p>The influence of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">D</mi> <mn>0</mn> </msub> </mrow> </semantics></math> value on subset.</p>
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<p>Geometric diagram of first-order shape function.</p>
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<p>Geometric optical model of virtual stereo vision based on four planar mirrors.</p>
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<p>Schematic diagram of image preprocessing for a virtual stereo-vision system.</p>
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<p>Geometric optical model of virtual stereo vision based on a bi-prism.</p>
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<p>Virtual stereo vision diagram based on a triangular prism [<a href="#B56-sensors-24-04031" class="html-bibr">56</a>].</p>
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<p>MMRSRGAN architecture.</p>
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<p>Schematic diagram of the sample tensile simulation experiment (<b>a</b>) and simulated lens design (<b>b</b>).</p>
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<p>Schematic diagram of the measurement-systems simulation model. (<b>a</b>) BSS (<b>b</b>) MVSS (<b>c</b>) BVSS (<b>d</b>) QVSS.</p>
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<p>Accuracy-verification results for four measurement systems. (<b>a</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi mathvariant="normal">e</mi> </mrow> <mo>¯</mo> </mover> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="sans-serif">δ</mi> </mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>Bar chart of relative error between camera calibration results and true values.</p>
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<p>3D-reconstruction cloud map of the sample surface.</p>
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<p>Sample node-reconstruction error.</p>
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<p>Reconstruction (<b>a</b>) and error evaluation (<b>b</b>) of sample deformation process by BSS.</p>
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<p>The effect of the application of the MMRSRGAN model in QVSS. (<b>a</b>) ×2 scale; (<b>b</b>) ×4 scale; (<b>c</b>) ×8 scale.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi mathvariant="normal">E</mi> </mrow> <mrow> <mi mathvariant="normal">p</mi> <mi mathvariant="normal">r</mi> </mrow> </msub> </mrow> </semantics></math> index of four measurement systems after the application of the MMRSRGAN model.</p>
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<p>Schematic diagram of three-dimensional dimensions of tensile specimen (<b>a</b>) and loading curve (<b>b</b>).</p>
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<p>Simulated camera spectral curve. (<b>a</b>) Red sensitivity curve; (<b>b</b>) green sensitivity curve; (<b>c</b>) blue sensitivity curve.</p>
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<p>Surface optical parameters of simulated calibration plates (<b>a</b>) and tensile specimens (<b>b</b>).</p>
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<p>Schematic diagram of structural of BSS, MVSS, BVSS, and QVSS. See <a href="#sensors-24-04031-t0A4" class="html-table">Table A4</a> for structural-parameter values. (<b>a</b>) BSS; (<b>b</b>) BVSS; (<b>c</b>) MVSS; (<b>d</b>) QVSS.</p>
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<p>DIC parameter settings. (<b>a</b>) BSS; (<b>b</b>) BVSS; (<b>c</b>) MVSS; (<b>d</b>) QVSS.</p>
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16 pages, 2873 KiB  
Article
Robots as Mental Health Coaches: A Study of Emotional Responses to Technology-Assisted Stress Management Tasks Using Physiological Signals
by Katarzyna Klęczek, Andra Rice and Maryam Alimardani
Sensors 2024, 24(13), 4032; https://doi.org/10.3390/s24134032 (registering DOI) - 21 Jun 2024
Abstract
The current study investigated the effectiveness of social robots in facilitating stress management interventions for university students by evaluating their physiological responses. We collected electroencephalogram (EEG) brain activity and Galvanic Skin Responses (GSRs) together with self-reported questionnaires from two groups of students who [...] Read more.
The current study investigated the effectiveness of social robots in facilitating stress management interventions for university students by evaluating their physiological responses. We collected electroencephalogram (EEG) brain activity and Galvanic Skin Responses (GSRs) together with self-reported questionnaires from two groups of students who practiced a deep breathing exercise either with a social robot or a laptop. From GSR signals, we obtained the change in participants’ arousal level throughout the intervention, and from the EEG signals, we extracted the change in their emotional valence using the neurometric of Frontal Alpha Asymmetry (FAA). While subjective perceptions of stress and user experience did not differ significantly between the two groups, the physiological signals revealed differences in their emotional responses as evaluated by the arousal–valence model. The Laptop group tended to show a decrease in arousal level which, in some cases, was accompanied by negative valence indicative of boredom or lack of interest. On the other hand, the Robot group displayed two patterns; some demonstrated a decrease in arousal with positive valence indicative of calmness and relaxation, and others showed an increase in arousal together with positive valence interpreted as excitement. These findings provide interesting insights into the impact of social robots as mental well-being coaches on students’ emotions particularly in the presence of the novelty effect. Additionally, they provide evidence for the efficacy of physiological signals as an objective and reliable measure of user experience in HRI settings. Full article
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<p>The 2D arousal–valence model of emotions, adapted from [<a href="#B25-sensors-24-04032" class="html-bibr">25</a>].</p>
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<p>Physiological measurements during the stress management task. (<b>A</b>) Brain signals were recorded using a Unicorn Hybrid Black EEG cap. (<b>B</b>) The EEG signals were collected from 8 electrodes (shown in green). However, in this study, only electrodes in the frontal region (F3 and F4 marked with red circle) were used for computation of emotional valence. (<b>C</b>) Galvanic Skin Responses (GSRs) were recorded using a Shimmer3 GSR+ sensor that was placed on the wrist and fingers of the participants’ non-dominant hand.</p>
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<p>A participant completing the MIST stress induction task.</p>
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<p>Overview of the stress management task being mediated by a Pepper robot. A video of an expanding and shrinking circle was displayed on the robot’s tablet to guide the participant with the timing of the breathing exercise.</p>
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<p>Experimental procedure.</p>
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<p>Comparison of the two Robot and Laptop groups in terms of (<b>A</b>) the change in their perceived stress (PSQ), (<b>B</b>) change in emotional valence (FAA), and (<b>C</b>) change in arousal level (GSR).</p>
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<p>Empirical reconstruction of the 2D arousal–valence model of emotions using participants’ physiological signals (i.e., GSR and FAA features).</p>
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<p>Comparison of the Robot and Laptop groups with respect to their self-reported experience with the technology they used during the stress management task.</p>
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10 pages, 800 KiB  
Article
The Effect of Caffeine on Movement-Related Cortical Potential Morphology and Detection
by Mads Jochumsen, Emma Rahbek Lavesen, Anne Bruun Griem, Caroline Falkenberg-Andersen and Sofie Kirstine Gedsø Jensen
Sensors 2024, 24(12), 4030; https://doi.org/10.3390/s24124030 (registering DOI) - 20 Jun 2024
Abstract
Movement-related cortical potential (MRCP) is observed in EEG recordings prior to a voluntary movement. It has been used for e.g., quantifying motor learning and for brain-computer interfacing (BCIs). The MRCP amplitude is affected by various factors, but the effect of caffeine is underexplored. [...] Read more.
Movement-related cortical potential (MRCP) is observed in EEG recordings prior to a voluntary movement. It has been used for e.g., quantifying motor learning and for brain-computer interfacing (BCIs). The MRCP amplitude is affected by various factors, but the effect of caffeine is underexplored. The aim of this study was to investigate if a cup of coffee with 85 mg caffeine modulated the MRCP amplitude and the classification of MRCPs versus idle activity, which estimates BCI performance. Twenty-six healthy participants performed 2 × 100 ankle dorsiflexion separated by a 10-min break before a cup of coffee was consumed, followed by another 100 movements. EEG was recorded during the movements and divided into epochs, which were averaged to extract three average MRCPs that were compared. Also, idle activity epochs were extracted. Features were extracted from the epochs and classified using random forest analysis. The MRCP amplitude did not change after consuming caffeine. There was a slight increase of two percentage points in the classification accuracy after consuming caffeine. In conclusion, a cup of coffee with 85 mg caffeine does not affect the MRCP amplitude, and improves MRCP-based BCI performance slightly. The findings suggest that drinking coffee is only a minor confounder in MRCP-related studies. Full article
(This article belongs to the Special Issue Advances in Brain–Computer Interfaces and Sensors)
18 pages, 23447 KiB  
Article
An Improved YOLOv8 Network for Detecting Electric Pylons Based on Optical Satellite Image
by Xin Chi, Yu Sun, Yingjun Zhao, Donghua Lu, Yan Gao and Yiting Zhang
Sensors 2024, 24(12), 4012; https://doi.org/10.3390/s24124012 (registering DOI) - 20 Jun 2024
Abstract
Electric pylons are crucial components of power infrastructure, requiring accurate detection and identification for effective monitoring of transmission lines. This paper proposes an innovative model, the EP-YOLOv8 network, which incorporates new modules: the DSLSK-SPPF and EMS-Head. The DSLSK-SPPF module is designed to capture [...] Read more.
Electric pylons are crucial components of power infrastructure, requiring accurate detection and identification for effective monitoring of transmission lines. This paper proposes an innovative model, the EP-YOLOv8 network, which incorporates new modules: the DSLSK-SPPF and EMS-Head. The DSLSK-SPPF module is designed to capture the surrounding features of electric pylons more effectively, enhancing the model’s adaptability to the complex shapes of these structures. The EMS-Head module enhances the model’s ability to capture fine details of electric pylons while maintaining a lightweight design. The EP-YOLOv8 network optimizes traditional YOLOv8n parameters, demonstrating a significant improvement in electric pylon detection accuracy with an average [email protected] value of 95.5%. The effective detection of electric pylons by the EP-YOLOv8 demonstrates its ability to overcome the inefficiencies inherent in existing optical satellite image-based models, particularly those related to the unique characteristics of electric pylons. This improvement will significantly aid in monitoring the operational status and layout of power infrastructure, providing crucial insights for infrastructure management and maintenance. Full article
(This article belongs to the Section Sensing and Imaging)
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<p>The architecture of YOLOv8 network.</p>
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<p>Schematic diagram of the SPPF module structure.</p>
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<p>Schematic diagram of the LSK block module.</p>
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<p>Schematic diagram of the LSK module.</p>
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<p>Schematic diagram of the DSLSK-SPPF module.</p>
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<p>Sampling methods of regular convolution and deformable convolution Blue dots represent standard convolutions, while green dots represent deformable convolutions (Offset).</p>
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<p>Schematic diagram illustrating the computation of dynamic snake convolution kernel coordinates and optional receptive fields.</p>
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<p>Schematic diagram of the EMS-Conv module.</p>
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<p>Comparison of the detector head: (<b>a</b>) YOLOv8 detection head structure; (<b>b</b>) reconstructed detection head structure.</p>
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<p>Comparison of mAP@0.5 values between EP-YOLOv8 model and original model.</p>
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<p>Comparison of detection performance: (<b>a</b>) input image; (<b>b</b>) object detection result of YOLOv8n; (<b>c</b>) object detection result of EP-YOLOv8.</p>
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<p>Comparison of detection performance: (<b>a</b>) input image; (<b>b</b>) object detection result of YOLOv8n; (<b>c</b>) object detection result of EP-YOLOv8.</p>
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<p>Comparison of detection performance: (<b>a</b>) input image; (<b>b</b>) object detection result of YOLOv8n; (<b>c</b>) object detection result of EP-YOLOv8.</p>
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15 pages, 6042 KiB  
Article
A Ground-Based Electrostatically Suspended Accelerometer
by Hanxiao Liu, Xiaoxia He, Chenhui Wu and Rong Zhang
Sensors 2024, 24(12), 4029; https://doi.org/10.3390/s24124029 (registering DOI) - 20 Jun 2024
Abstract
In this study, we have developed an electrostatically suspended accelerometer (ESA) specifically designed for ground use. To ensure sufficient overload capacity and minimize noise resulting from high suspension voltage, we introduced a proof mass design featuring a hollow, thin-walled cylinder with a thin [...] Read more.
In this study, we have developed an electrostatically suspended accelerometer (ESA) specifically designed for ground use. To ensure sufficient overload capacity and minimize noise resulting from high suspension voltage, we introduced a proof mass design featuring a hollow, thin-walled cylinder with a thin flange fixed at the center, offering the highest surface-area-to-mass ratio compared to various typical proof mass structures. Preload voltage is directly applied to the proof mass via a golden wire, effectively reducing the maximum supply voltage for suspension. The arrangement of suspension electrodes, offering five degrees of freedom and minimizing cross-talk, was designed to prioritize simplicity and maximize the utilization of electrode area for suspension purposes. The displacement detection and electrostatic suspension force were accurately modeled based on the structure. A controller incorporating an inverse winding mechanism was developed and simulated using Simulink. The simulation results unequivocally demonstrate the successful completion of the stable initial levitation process and suspension under ±1g overload. Full article
(This article belongs to the Special Issue Advanced Inertial Sensors: Advances, Challenges and Applications)
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<p>Schematic sketch of electrostatic suspension system overview and operation principle in one DOF.</p>
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<p>Typical proof mass structural diagrams: (<b>a</b>) hollow sphere; (<b>b</b>) hollow hexahedron; (<b>c</b>) six thin hollow plates; (<b>d</b>) hollow cylinder; (<b>e</b>) hollow cylinder with outer flange; (<b>f</b>) hollow cylinder with inner flange.</p>
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<p>Schematic Diagram of the Proof Mass Structure.</p>
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<p>Schematic Diagram of Electrode Structure.</p>
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<p>The numbering definition pf electrodes: (<b>a</b>) Numbering definition of planar electrodes in disk direction; (<b>b</b>). The numbering definition of cylindrical electrodes in the cylinder direction.</p>
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<p>Schematic diagram of displacement detection: (<b>a</b>) displacement detection in <math display="inline"><semantics> <mi>Z</mi> </semantics></math> DOF; (<b>b</b>) displacement detection in <math display="inline"><semantics> <mrow> <mi>X</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>Y</mi> </mrow> </semantics></math> DOF. (<b>c</b>) displacement detection in <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>ϕ</mi> </mrow> </semantics></math> DOF.</p>
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<p>Schematic diagram suspension control principle: (<b>a</b>) voltage load and electrostatic force suspension scheme in <math display="inline"><semantics> <mi>Z</mi> </semantics></math> DOF; (<b>b</b>) voltage load and electrostatic force suspension scheme in <math display="inline"><semantics> <mrow> <mi>X</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>Y</mi> </mrow> </semantics></math> DOF. (<b>c</b>) voltage load and electrostatic force suspension scheme in <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>ϕ</mi> </mrow> </semantics></math> DOF.</p>
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<p>Schematic diagram of a single-degree-of-freedom electrostatic suspension.</p>
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<p>Bode diagram of the open-loop system.</p>
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<p>Controller with inverse “winding”.</p>
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<p>Simulink model of system structure.</p>
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<p>Simulink simulation results of the initial levitation process: (<b>a</b>) PIDPL alone; (<b>b</b>) PIDPL with inverse “winding”.</p>
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<p>Simulink simulation results of the suspension stage: (<b>a</b>) result in <math display="inline"><semantics> <mi>Z</mi> </semantics></math> DOF; (<b>b</b>) result in <math display="inline"><semantics> <mrow> <mi>X</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>Y</mi> </mrow> </semantics></math> DOF. (<b>c</b>) result in <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>ϕ</mi> </mrow> </semantics></math> DOF.</p>
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<p>Step response simulation results in a robust analysis: (<b>a</b>) result in <math display="inline"><semantics> <mi>Z</mi> </semantics></math> DOF; (<b>b</b>) result in <math display="inline"><semantics> <mrow> <mi>X</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>Y</mi> </mrow> </semantics></math> DOF. (<b>c</b>) result in <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>ϕ</mi> </mrow> </semantics></math> DOF.</p>
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<p>Initial levitation simulation results in a robust analysis: (<b>a</b>) result in <math display="inline"><semantics> <mi>Z</mi> </semantics></math> DOF; (<b>b</b>) result in <math display="inline"><semantics> <mrow> <mi>X</mi> <mo> </mo> <mo>&amp;</mo> <mo> </mo> <mi>Y</mi> </mrow> </semantics></math> DOF.</p>
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15 pages, 5903 KiB  
Article
Determinants of Maximum Magnetic Anomaly Detection Distance
by Hangcheng Li, Jiaming Luo, Jiajun Zhang, Jing Li, Yi Zhang, Wenwei Zhang and Mingji Zhang
Sensors 2024, 24(12), 4028; https://doi.org/10.3390/s24124028 (registering DOI) - 20 Jun 2024
Abstract
The maximum detection distance is usually the primary concern of magnetic anomaly detection (MAD). Intuition tells us that larger object size, stronger magnetization and finer measurement resolution guarantee a further detectable distance. However, the quantitative relationship between detection distance and the above determinants [...] Read more.
The maximum detection distance is usually the primary concern of magnetic anomaly detection (MAD). Intuition tells us that larger object size, stronger magnetization and finer measurement resolution guarantee a further detectable distance. However, the quantitative relationship between detection distance and the above determinants is seldom studied. In this work, unmanned aerial vehicle-based MAD field experiments are conducted on cargo vessels and NdFeB magnets as typical magnetic objects to give a set of visualized magnetic field flux density images. Isometric finite element models are established, calibrated and analyzed according to the experiment configuration. A maximum detectable distance map as a function of target size and measurement resolution is then obtained from parametric sweeping on an experimentally calibrated finite element analysis model. We find that the logarithm of detectable distance is positively proportional to the logarithm of object size while negatively proportional to the logarithm of resolution, within the ranges of 1 m~500 m and 1 pT~1 μT, respectively. A three-parameter empirical formula (namely distance-size-resolution logarithmic relationship) is firstly developed to determine the most economic sensor configuration for a given detection task, to estimate the maximum detection distance for a given magnetic sensor and object, or to evaluate minimum detectable object size at a given magnetic anomaly detection scenario. Full article
(This article belongs to the Special Issue Advances in Magnetic Anomaly Sensing Systems)
22 pages, 4086 KiB  
Article
Experimental and Numerical Investigation of Bogie Hunting Instability for Railway Vehicles Based on Multiple Sensors
by Biao Zheng, Lai Wei, Jing Zeng and Dafu Zhang
Sensors 2024, 24(12), 4027; https://doi.org/10.3390/s24124027 (registering DOI) - 20 Jun 2024
Abstract
Bogie hunting instability is one of the common faults in railway vehicles. It not only affects ride comfort but also threatens operational safety. Due to the lower operating speed of metro vehicles, their bogie hunting stability is often overlooked. However, as wheel tread [...] Read more.
Bogie hunting instability is one of the common faults in railway vehicles. It not only affects ride comfort but also threatens operational safety. Due to the lower operating speed of metro vehicles, their bogie hunting stability is often overlooked. However, as wheel tread wear increases, metro vehicles with high conicity wheel–rail contact can also experience bogie hunting instability. In order to enhance the operational safety of metro vehicles, this paper conducts field tests and simulation calculations to study the bogie hunting instability behavior of metro vehicles and proposes corresponding solutions from the perspective of wheel–rail contact relationships. Acceleration and displacement sensors are installed on metro vehicles to collect data, which are processed in real time in 2 s intervals. The lateral acceleration of the frame is analyzed to determine if bogie hunting instability has occurred. Based on calculated safety indicators, it is determined whether deceleration is necessary to ensure the safety of vehicle operation. For metro vehicles in the later stages of wheel wear (after 300,000 km), the stability of their bogies should be monitored in real time. To improve the stability of metro vehicle bogies while ensuring the longevity of wheelsets, metro vehicle wheel treads should be reprofiled regularly, with a recommended reprofiling interval of 350,000 km. Full article
(This article belongs to the Special Issue Sensors for Real-Time Condition Monitoring and Fault Diagnosis)
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