Nothing Special   »   [go: up one dir, main page]

You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (827)

Search Parameters:
Keywords = map spectrum

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
13 pages, 4906 KiB  
Technical Note
An Extended Omega-K Algorithm for Automotive SAR with Curved Path
by Ping Guo, Chao Li, Haolan Li, Yuchen Luan, Anyi Wang, Rongshu Wang and Shiyang Tang
Remote Sens. 2024, 16(23), 4508; https://doi.org/10.3390/rs16234508 (registering DOI) - 1 Dec 2024
Viewed by 96
Abstract
Automotive millimeter-wave (MMW) synthetic aperture radar (SAR) systems can achieve high-resolution images of detection areas, providing environmental perceptions that facilitate intelligent driving. However, curved path is inevitable in complex urban road environments. Non-uniform spatial sampling, brought about by curved path, leads to cross-coupling [...] Read more.
Automotive millimeter-wave (MMW) synthetic aperture radar (SAR) systems can achieve high-resolution images of detection areas, providing environmental perceptions that facilitate intelligent driving. However, curved path is inevitable in complex urban road environments. Non-uniform spatial sampling, brought about by curved path, leads to cross-coupling and spatial variation deteriorates greatly, significantly impacting the imaging results. To deal with these issues, we developed an Extended Omega-K Algorithm (EOKA) for an automotive SAR with a curved path. First, an equivalent range model was constructed based on the relationship between the range history and Doppler frequency. Then, using azimuth time mapping, the echo data was reconstructed with a form similar to that of a uniform linear case. As a result, an analytical two-dimensional (2D) spectrum was easily derived without using of the method of series reversion (MSR) that could be exploited for EOKA. The results from the parking lot, open road, and obstacle experimental scenes demonstrate the performance and feasibility of an MMW SAR for environmental perception. Full article
Show Figures

Figure 1

Figure 1
<p>Geometry of automotive SAR with curved path.</p>
Full article ">Figure 2
<p>Real data of INS and fitting results. (<b>a</b>) X, (<b>b</b>) Y and (<b>c</b>) Z.</p>
Full article ">Figure 3
<p>The phase errors. (<b>a</b>) Fitting, (<b>b</b>) Equation (2).</p>
Full article ">Figure 4
<p>Range history reconstruction diagram.</p>
Full article ">Figure 5
<p>Flowchart of the imaging algorithm.</p>
Full article ">Figure 6
<p>The image scenes. (<b>a</b>) simulated scene; (<b>b</b>) experimental scene.</p>
Full article ">Figure 7
<p>The IRF of three targets. (<b>a</b>) OKA, (<b>b</b>) EOKA, (<b>c</b>) FFBPA.</p>
Full article ">Figure 8
<p>The optical image of obstacle scene.</p>
Full article ">Figure 9
<p>Obstacle focused images. (<b>a</b>) EOKA, (<b>b</b>) OKA.</p>
Full article ">Figure 10
<p>Focused image. (<b>a</b>) Parking lot scene; (<b>b</b>) Open road scene.</p>
Full article ">
21 pages, 534 KiB  
Article
Detection of Access Point Spoofing in the Wi-Fi Fingerprinting Based Positioning
by Juraj Machaj, Clément Safon, Slavomír Matúška and Peter Brída
Sensors 2024, 24(23), 7624; https://doi.org/10.3390/s24237624 (registering DOI) - 28 Nov 2024
Viewed by 271
Abstract
Indoor positioning based on Wi-Fi signals has gained a lot of attention lately. There are many advantages related to the use of Wi-Fi signals for positioning, including the availability of Wi-Fi access points in indoor environments and the integration of Wi-Fi transceivers into [...] Read more.
Indoor positioning based on Wi-Fi signals has gained a lot of attention lately. There are many advantages related to the use of Wi-Fi signals for positioning, including the availability of Wi-Fi access points in indoor environments and the integration of Wi-Fi transceivers into consumer devices. However, since Wi-Fi uses an unlicensed spectrum, anyone can create their own access points. Therefore, it is possible to affect the function of the localization system by spoofing signals from access points and thus alter positioning accuracy. Previously published works focused mainly on the evaluation of spoofing on localization systems and the detection of anomalies when updating the radio map. Spoofing mitigation solutions were proposed; however, their application to systems that use off-the-shelf items is not straightforward. In this paper filtering algorithms are proposed to minimize the impact of access point spoofing. The filtering was applied with a combination of the widely used K-Nearest Neighbours (KNN) localization algorithm and their performance is evaluated using the UJIIndoorLoc dataset. During the evaluation, the spoofing of Access Points was performed in two different scenarios and the number of spoofed access points ranged from 1 to 10. Based on the achieved results proposed SFKNN provided good detection of the spoofing and helped to reduce the mean localization error by 2–5 m, especially when the number of spoofed access points was higher. Full article
(This article belongs to the Special Issue Smart Systems and Wireless Sensor Networks for Localization)
Show Figures

Figure 1

Figure 1
<p>Visualization of spoofing detection principle implemented in SFKNN on localization request with spoofed APs.</p>
Full article ">Figure 2
<p>Localization errors achieved by proposed solutions without spoofing of APs.</p>
Full article ">Figure 3
<p>Localization request drop rate for different numbers of spoofed APs in Scenario 1.</p>
Full article ">Figure 4
<p>Localization request drop rate for different numbers of spoofed APs in Scenario 2.</p>
Full article ">Figure 5
<p>Localization errors achieved in both scenarios with five spoofed APs.</p>
Full article ">Figure 6
<p>Localization errors achieved in both scenarios with 10 spoofed APs.</p>
Full article ">
15 pages, 16548 KiB  
Article
Short-Wave Infrared (SWIR) Imaging for Robust Material Classification: Overcoming Limitations of Visible Spectrum Data
by Hanbin Song, Sanghyeop Yeo, Youngwan Jin, Incheol Park, Hyeongjin Ju, Yagiz Nalcakan and Shiho Kim
Appl. Sci. 2024, 14(23), 11049; https://doi.org/10.3390/app142311049 - 27 Nov 2024
Viewed by 364
Abstract
This paper presents a novel approach to material classification using short-wave infrared (SWIR) imaging, aimed at applications where differentiating visually similar objects based on material properties is essential, such as in autonomous driving. Traditional vision systems, relying on visible spectrum imaging, struggle to [...] Read more.
This paper presents a novel approach to material classification using short-wave infrared (SWIR) imaging, aimed at applications where differentiating visually similar objects based on material properties is essential, such as in autonomous driving. Traditional vision systems, relying on visible spectrum imaging, struggle to distinguish between objects with similar appearances but different material compositions. Our method leverages SWIR’s distinct reflectance characteristics, particularly for materials containing moisture, and demonstrates a significant improvement in accuracy. Specifically, SWIR data achieved near-perfect classification results with an accuracy of 99% for distinguishing real from artificial objects, compared to 77% with visible spectrum data. In object detection tasks, our SWIR-based model achieved a mean average precision (mAP) of 0.98 for human detection and up to 1.00 for other objects, demonstrating its robustness in reducing false detections. This study underscores SWIR’s potential to enhance object recognition and reduce ambiguity in complex environments, offering a valuable contribution to material-based object recognition in autonomous driving, manufacturing, and beyond. Full article
21 pages, 16398 KiB  
Article
Assessing the Effect of Water on Submerged and Floating Plastic Detection Using Remote Sensing and K-Means Clustering
by Lenka Fronkova, Ralph P. Brayne, Joseph W. Ribeiro, Martin Cliffen, Francesco Beccari and James H. W. Arnott
Remote Sens. 2024, 16(23), 4405; https://doi.org/10.3390/rs16234405 - 25 Nov 2024
Viewed by 547
Abstract
Marine and freshwater plastic pollution is a worldwide problem affecting ecosystems and human health. Although remote sensing has been used to map large floating plastic rafts, there are research gaps in detecting submerged plastic due to the limited amount of in situ data. [...] Read more.
Marine and freshwater plastic pollution is a worldwide problem affecting ecosystems and human health. Although remote sensing has been used to map large floating plastic rafts, there are research gaps in detecting submerged plastic due to the limited amount of in situ data. This study is the first to collect in situ data on submerged and floating plastics in a freshwater environment and analyse the effect of water submersion on the strength of the plastic signal. A large 10 × 10 m artificial polymer tarpaulin was deployed in a freshwater lake for a two-week period and was captured by a multi-sensor and multi-resolution unmanned aerial vehicle (UAV) and satellite. Spectral analysis was conducted to assess the attenuation of individual wavelengths of the submerged tarpaulin in UAV hyperspectral and Sentinel-2 multispectral data. A K-Means unsupervised clustering algorithm was used to classify the images into two clusters: plastic and water. Additionally, we estimated the optimal number of clusters present in the hyperspectral dataset and found that classifying the image into four classes (water, submerged plastic, near surface plastic and buoys) significantly improved the accuracy of the K-Means predictions. The submerged plastic tarpaulin was detectable to ~0.5 m below the water surface in near infrared (NIR) (~810 nm) and red edge (~730 nm) wavelengths. However, the red spectrum (~669 nm) performed the best with ~84% true plastic positives, classifying plastic pixels correctly even to ~1 m depth. These individual bands outperformed the dedicated Plastic Index (PI) derived from the UAV dataset. Additionally, this study showed that in neither Sentinel-2 bands, nor the derived indices (PI or Floating Debris Index (FDI), it is currently possible to determine if and how much of the tarpaulin was under the water surface, using a plastic tarpaulin object of 10 × 10 m. Overall, this paper showed that spatial resolution was more important than spectral resolution in detecting submerged tarpaulin. These findings directly contributed to Sustainable Development Goal 14.1 on mapping large marine plastic patches of 10 × 10 m and could be used to better define systems for monitoring submerged and floating plastic pollution. Full article
(This article belongs to the Section Environmental Remote Sensing)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>A composite figure showing the (<b>A</b>) location of the area of interest; (<b>B</b>) the tarpaulin taken after it was installed on 5 August 2021; (<b>C</b>) the tarpaulin after it had sunk on 10 August 2021, and; (<b>D</b>) a summary of the datasets collected on 19 August 2021 (including RGB, thermal, hyperspectral, multispectral and Sentinel-2 MSI). * ESRI Satellite basemap was sourced from: <a href="https://qms.nextgis.com/geoservices/1300/" target="_blank">https://qms.nextgis.com/geoservices/1300/</a> (accessed on 18 November 2023).</p>
Full article ">Figure 2
<p>A diagram of the K-Means classification process and the plastic versus non-plastic hyperspectral mask created using the visible spectrum.</p>
Full article ">Figure 3
<p>This figure shows the number of plastic pixels detected for two K-Means classes, plastic versus water (<b>A</b>). The bottom figure (<b>B</b>) shows the results of the same K-Means predictions after removing the highly reflective buoy pixels. The percentage of true plastic pixels predicted were extracted from confusion matrices for individual hyperspectral bands.</p>
Full article ">Figure 4
<p>UAV collected imagery of the tarpaulin using: (<b>A</b>) a true colour composite from hyperspectral data; (<b>B</b>) a testing mask derived from hyperspectral data; (<b>C</b>) thermal camera data; (<b>D</b>) predictions for the band 187 at 810 nm (NIR); (<b>E</b>) band 187 at 810 nm in greyscale which performs the best at the predictions of submerged tarpaulin before removing buoy pixels for two clusters, and; (<b>F</b>) RGB image showing the colour coded crosses where the reflectance was extracted for <a href="#remotesensing-16-04405-f005" class="html-fig">Figure 5</a>.</p>
Full article ">Figure 5
<p>Reflectance extracted for specific points across the tarpaulin imagery (marked in <a href="#remotesensing-16-04405-f004" class="html-fig">Figure 4</a>F), showing an average reflectance across the electromagnetic spectrum for buoys, near-surface tarpaulin, submerged tarpaulin, and water. Buoys act almost as perfect reflectors, with an average reflectance of ~1.</p>
Full article ">Figure 6
<p>Reflectance across 400 to 1000 nm extracted from the point locations depicted in <a href="#remotesensing-16-04405-f004" class="html-fig">Figure 4</a>F (excluding buoys) for near-surface and submerged tarpaulin and water, as well as the results of the K-Means predictions for two clusters (plastic versus water). The K-Means plastic predictions showed the number of correctly classified pixels peaked at ~810 nm (NIR), and gradually dropped after exhibiting a strong salt and pepper noise from 900 nm onwards.</p>
Full article ">Figure 7
<p>K-Means plastic predictions for four clusters peaked at the red band spectrum ~669, followed by the red edge and NIR. These individual wavelengths outperformed predictions of the dedicated PI. PI predicted most of the near-surface and submerged tarpaulin pixels. However, it also predicted a lot of false positives in the water class, creating distinct salt and pepper noise.</p>
Full article ">Figure 8
<p>This image shows reflectance of submerged and floating tarpaulin and water pixels extracted from hyperspectral UAV data and multispectral Sentinel-2 satellite data.</p>
Full article ">Figure 9
<p>Sentinel-2 bands for water and partially submerged tarpaulin (visible in the zoomed red rectangle) in Whitlingham Great Broad area of interest (LAKE AOI), as well as derived PI and FDI from 11 August 2021.</p>
Full article ">Figure 10
<p>Boxplots showed that water and submerged and floating plastic tarpaulin have a small spread/variation in FDI, but their means overlapped. The distribution of the two classes differed from each other in PI, distinguishing tarpaulin better from water than FDI.</p>
Full article ">Figure 11
<p>This image showed the K-Means predictions with two clusters for Sentinel-2 imagery from 11/08/2021. The Sentinel-2 bands were chosen for a comparison with the best-performing UAV-collected hyperspectral wavelengths and the bands used for the floating litter indices calculations (<a href="#sec2dot3-remotesensing-16-04405" class="html-sec">Section 2.3</a>).</p>
Full article ">
18 pages, 2663 KiB  
Article
Improved RT-DETR for Infrared Ship Detection Based on Multi-Attention and Feature Fusion
by Chun Liu, Yuanliang Zhang, Jingfu Shen and Feiyue Liu
J. Mar. Sci. Eng. 2024, 12(12), 2130; https://doi.org/10.3390/jmse12122130 - 22 Nov 2024
Viewed by 435
Abstract
Infrared cameras form images by capturing the thermal radiation emitted by objects in the infrared spectrum, making them complex sensors widely used in maritime surveillance. However, the broad spectral range of the infrared band makes it susceptible to environmental interference, which can reduce [...] Read more.
Infrared cameras form images by capturing the thermal radiation emitted by objects in the infrared spectrum, making them complex sensors widely used in maritime surveillance. However, the broad spectral range of the infrared band makes it susceptible to environmental interference, which can reduce the contrast between the target and the background. As a result, detecting infrared targets in complex marine environments remains challenging. This paper presents a novel and enhanced detection model developed from the real-time detection transformer (RT-DETR), which is designated as MAFF-DETR. The model incorporates a novel backbone by integrating CSP and parallelized patch-aware attention to enhance sensitivity to infrared imagery. Additionally, a channel attention module is employed during feature selection, leveraging high-level features to filter low-level information and enabling efficient multi-level fusion. The model’s target detection performance on resource-constrained devices is further enhanced by incorporating advanced techniques such as group convolution and ShuffleNetV2. The experimental results show that, although the enhanced RT-DETR algorithm still experiences missed detections under severe object occlusion, it has significantly improved overall performance, including a 1.7% increase in mAP, a reduction in 4.3 M parameters, and a 5.8 GFLOPs decrease in computational complexity. It can be widely applied to tasks such as coastline monitoring and maritime search and rescue. Full article
(This article belongs to the Special Issue AI-Empowered Marine Energy)
Show Figures

Figure 1

Figure 1
<p>Architecture of the MAFF-DETR Network.</p>
Full article ">Figure 2
<p>Comparison between the Original CSP Module and the CPPA Module in MAFF-DETR: (<b>a</b>) Architecture of the CSP module. (<b>b</b>) Architecture of the CPPA module.</p>
Full article ">Figure 3
<p>Structure overview of the parallelized patch-aware attention module.</p>
Full article ">Figure 4
<p>Detailed structure of the SFF and CA modules.</p>
Full article ">Figure 5
<p>Detailed structure of the multi-layer dynamic shuffle transformer module.</p>
Full article ">Figure 6
<p>Dataset analysis: (<b>a</b>) Bar graph of the number of ship types. (<b>b</b>) Bounding box overlay.</p>
Full article ">Figure 7
<p>Examples of bounding box visualizations of infrared ship detections for different scenarios: (<b>a</b>) Detection results of adjacent fishing boats. (<b>b</b>) Detection results of extremely small targets. (<b>c</b>) Detection results at the image edges. (<b>d</b>) Detection results in complex nearshore scenarios. The red box indicates the false negatives and false positives issues of RT-DETR.</p>
Full article ">Figure 8
<p>Examples of heat maps Illustrating infrared ship detection for different scenarios: (<b>a</b>) Heat map of adjacent fishing boats. (<b>b</b>) Heat map of extremely small targets. (<b>c</b>) Heat map at the image edges. (<b>d</b>) Heat map in complex nearshore scenarios.</p>
Full article ">
16 pages, 5245 KiB  
Article
Ball-on-Disk Wear Maps for Bearing Steel–Hard Anodized EN AW-6082 Aluminum Alloy Tribocouple in Dry Sliding Conditions
by Enrico Baroni, Annalisa Fortini, Lorenzo Meo, Chiara Soffritti, Mattia Merlin and Gian Luca Garagnani
Coatings 2024, 14(11), 1469; https://doi.org/10.3390/coatings14111469 - 19 Nov 2024
Viewed by 434
Abstract
In recent years, Golden Hard Anodizing (G.H.A.®) has been developed as a variant of the traditional hard anodizing process with the addition of Ag+ ions in the nanoporous structure. The tribological properties of this innovative surface treatment are still not [...] Read more.
In recent years, Golden Hard Anodizing (G.H.A.®) has been developed as a variant of the traditional hard anodizing process with the addition of Ag+ ions in the nanoporous structure. The tribological properties of this innovative surface treatment are still not well understood. In this study, ball-on-disk tests were conducted in dry sliding conditions using 100Cr6 (AISI 52100) bearing steel balls as a counterbody and GHA®-anodized EN AW-6082 aluminum alloy disks. The novelty of this work lies in the mapping of the wear properties of the tribocouple under different test conditions for a better comparison of the results. Three different normal loads (equal to 5, 10, and 15 N) and three different reciprocating frequencies (equal to 2, 3, and 4 Hz) were selected to investigate a spectrum of operating conditions for polished and unpolished G.H.A.®-anodized EN AW-6082 aluminum alloy. Quantitative wear maps were built based on the resulting wear rate values to define the critical operating limits of the considered tribocouple. The results suggest that the coefficient of friction (COF) was independent of test conditions, while different wear maps were found for polished and non-polished surfaces. Polishing before anodizing permitted the acquisition of lower wear for the anodized disks and the steel balls. Full article
Show Figures

Figure 1

Figure 1
<p>Optical micrographs in cross-section of the anodized layers before wear tests for (<b>a</b>) UP. (<b>b</b>) P.</p>
Full article ">Figure 2
<p>COF evolution during distance for UP (unpolished substrate) and P (previously polished substrate) anodic layers at the different investigated loads: (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N.</p>
Full article ">Figure 3
<p>Representative VPSEM micrographs of wear tracks of the G.H.A.<sup>®</sup>-anodized disk (<b>a</b>) after 50 m, (<b>b</b>) after 100 m, (<b>c</b>) after 150 m, and (<b>d</b>) after 200 m. The orange arrow indicates the direction of reciprocating sliding.</p>
Full article ">Figure 4
<p>VPSEM micrograph at high magnification of the wear tracks of the disk together with semi-quantitative EDS spectra (<b>a</b>). The solid red arrow indicates the area of revelation for the semi-quantitative EDS analysis (<b>b</b>). The red-edged arrow indicates the new deposition of material, while the yellow-edged arrow indicates the removal of a part of the anodic layer with its corresponding EDS spectra (<b>c</b>).</p>
Full article ">Figure 5
<p>Contact pressure evolution during sliding distance for the different applied loads: (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N. <span class="html-italic">Y</span>-axis is reported in logarithmic scale.</p>
Full article ">Figure 6
<p>Worn volume of material from both the counterbodies at the different investigated loads in the case of sliding against UP samples together with a shape factor for the wear scar diameters on the 100Cr6 steel balls at (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N.</p>
Full article ">Figure 7
<p>Quantitative wear maps for 100Cr6 ball and UP anodized disks.</p>
Full article ">Figure 8
<p>Worn volume of material from both the counterbodies at the different investigated loads in the case of sliding against P samples together with a shape factor for the wear scar diameters on the 100Cr6 steel balls at (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N.</p>
Full article ">Figure 9
<p>Quantitative wear maps for 100Cr6 ball and P anodized disks.</p>
Full article ">
15 pages, 3454 KiB  
Article
Soliton Solutions and Chaotic Dynamics of the Ion-Acoustic Plasma Governed by a (3+1)-Dimensional Generalized Korteweg–de Vries–Zakharov–Kuznetsov Equation
by Amjad E. Hamza, Mohammed Nour A. Rabih, Amer Alsulami, Alaa Mustafa, Khaled Aldwoah and Hicham Saber
Fractal Fract. 2024, 8(11), 673; https://doi.org/10.3390/fractalfract8110673 - 19 Nov 2024
Viewed by 403
Abstract
This study explores the novel dynamics of the (3+1)-dimensional generalized Korteweg–de Vries–Zakharov–Kuznetsov (KdV-ZK) equation. A Galilean transformation is employed to derive the associated system of equations. Perturbing this system allows us to investigate the presence and characteristics of chaotic behavior, including return maps, [...] Read more.
This study explores the novel dynamics of the (3+1)-dimensional generalized Korteweg–de Vries–Zakharov–Kuznetsov (KdV-ZK) equation. A Galilean transformation is employed to derive the associated system of equations. Perturbing this system allows us to investigate the presence and characteristics of chaotic behavior, including return maps, fractal dimension, power spectrum, recurrence plots, and strange attractors, supported by 2D and time-dependent phase portraits. A sensitivity analysis is demonstrated to show how the system behaves when there are small changes in initial values. Finally, the planar dynamical system method is used to derive anti-kink, dark soliton, and kink soliton solutions, advancing our understanding of the range of solutions admitted by the model. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>,<b>b</b>) Visualization of the dynamics of the proposed perturbed system by setting specific parameter values as <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mn>0.7</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 2
<p>(<b>a</b>,<b>b</b>) Visualization of the dynamics of the proposed perturbed system by setting specific parameter values as <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mn>0.7</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 3
<p>(<b>a</b>–<b>d</b>) Chaotic behavior by assuming the parameters <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 4
<p>(<b>a</b>–<b>d</b>) Chaotic behavior by assuming the parameters <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 5
<p>(<b>a</b>–<b>d</b>) Visualizations based on numerical simulations of the various state variables over time <span class="html-italic">t</span> assuming <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mn>0.7</mn> </mrow> </semantics></math> with various initial values.</p>
Full article ">Figure 6
<p>(<b>a</b>–<b>f</b>) Visualizations based on numerical simulations of the given equation with parameters assumed to be <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi>ϱ</mi> <mo>=</mo> <mn>0.7</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>1</mn> <mo>.</mo> </mrow> </semantics></math> with various initial values.</p>
Full article ">Figure 7
<p>Visualizations of the Lyapunov spectrum for <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi>ϱ</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> with various initial values.</p>
Full article ">Figure 8
<p>(<b>a</b>–<b>d</b>) Visualizations of the return maps and power spectra for <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi>ϱ</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>1.8</mn> </mrow> </semantics></math> with various initial values.</p>
Full article ">Figure 9
<p>(<b>a</b>–<b>d</b>) Visualizations of the return map and fractal dimensions for <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi>ϱ</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>1.8</mn> </mrow> </semantics></math> with various initial values.</p>
Full article ">Figure 10
<p>(<b>a</b>–<b>c</b>) Visualizations of the behavior of strange attractors for <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi>ϱ</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>1.8</mn> </mrow> </semantics></math> with various initial values.</p>
Full article ">Figure 11
<p>(<b>a</b>–<b>c</b>) Visualizations of the behavior of strange attractors for <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> <mo>,</mo> <mspace width="3.33333pt"/> <mi>ϱ</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mi mathvariant="sans-serif">M</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">u</mi> <mo>=</mo> <mn>1.8</mn> </mrow> </semantics></math> with various initial values.</p>
Full article ">Figure 12
<p>(<b>a</b>,<b>b</b>) Numerical demonstration of the obtained solution <math display="inline"><semantics> <msub> <mi mathvariant="script">Z</mi> <mn>2</mn> </msub> </semantics></math> with <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mo>−</mo> <mn>1</mn> </mrow> </semantics></math>; green t = −4, blue t = 0, and red t = 4.</p>
Full article ">Figure 13
<p>(<b>a</b>,<b>b</b>) Graphical behavior of <math display="inline"><semantics> <msub> <mi mathvariant="script">Z</mi> <mn>4</mn> </msub> </semantics></math> for <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mo>−</mo> <mn>1</mn> </mrow> </semantics></math>; green t = −5, blue t = 0, and red t = 5.</p>
Full article ">Figure 14
<p>(<b>a</b>,<b>b</b>) Numerical demonstration of the obtained solution <math display="inline"><semantics> <msub> <mi mathvariant="script">Z</mi> <mn>7</mn> </msub> </semantics></math> with parameters used as <math display="inline"><semantics> <mrow> <mi>z</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <msub> <mi>λ</mi> <mn>1</mn> </msub> <mo>=</mo> <mo>−</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>λ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>ζ</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>0.4</mn> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>ϱ</mi> <mo>=</mo> <mo>−</mo> <mn>1</mn> </mrow> </semantics></math>; green t = −10, blue t = 0, and red t = 10.</p>
Full article ">
19 pages, 4171 KiB  
Article
FastSLAM-MO-PSO: A Robust Method for Simultaneous Localization and Mapping in Mobile Robots Navigating Unknown Environments
by Xu Bian, Wanqiu Zhao, Ling Tang, Hong Zhao and Xuesong Mei
Appl. Sci. 2024, 14(22), 10268; https://doi.org/10.3390/app142210268 - 8 Nov 2024
Viewed by 567
Abstract
In the realm of mobile robotics, the capability to navigate and map uncharted territories is paramount, and Simultaneous Localization and Mapping (SLAM) stands as a cornerstone technology enabling this capability. While traditional SLAM methods like Extended Kalman Filter (EKF) and FastSLAM have made [...] Read more.
In the realm of mobile robotics, the capability to navigate and map uncharted territories is paramount, and Simultaneous Localization and Mapping (SLAM) stands as a cornerstone technology enabling this capability. While traditional SLAM methods like Extended Kalman Filter (EKF) and FastSLAM have made strides, they often struggle with the complexities of non-linear dynamics and non-Gaussian noise, particularly in dynamic settings. Moreover, these methods can be computationally intensive, limiting their applicability in real-world scenarios. This paper introduces an innovative enhancement to the FastSLAM framework by integrating Multi-Objective Particle Swarm Optimization (MO-PSO), aiming to bolster the robustness and accuracy of SLAM in mobile robots. We outline the theoretical underpinnings of FastSLAM and underscore its significance in robotic autonomy for mapping and exploration. Our approach innovates by crafting a specialized fitness function within the MO-PSO paradigm, which is instrumental in optimizing the particle distribution and addressing the challenges inherent in traditional particle filtering methods. This strategic fusion of MO-PSO with FastSLAM not only circumvents the pitfalls of particle degeneration, but also enhances the overall robustness and precision of the SLAM process across a spectrum of operational environments. Our empirical evaluation involves testing the proposed method on three distinct simulation benchmarks, comparing its performance against four other algorithms. The results indicate that our MO-PSO-enhanced FastSLAM method outperforms the traditional particle filtering approach by significantly reducing particle degeneration and ensuring more reliable and precise SLAM performance in challenging environments. This research demonstrates that the integration of MO-PSO with FastSLAM is a promising direction for improving SLAM in mobile robots, providing a robust solution for accurate mapping and localization even in complex and unknown settings. Full article
Show Figures

Figure 1

Figure 1
<p>The Pareto front and dominance relationships.</p>
Full article ">Figure 2
<p>The flow chart of MO-PSO.</p>
Full article ">Figure 3
<p>Three problem scenarios in benchmark. The black areas represent obstacles that are non-negotiable, while the white areas denote traversable spaces. The red dot signifies the starting point of the simulated vehicle, and the green dot indicates its destination. As the algorithm operates, the vehicle constructs a map and verifies its trajectory along the existing path, following the blue line from the starting point to the endpoint. The SLAM algorithm is utilized to build the map and simulate the vehicle’s trajectory during this process.</p>
Full article ">Figure 4
<p>Comparative results in the small-scale scenario.</p>
Full article ">Figure 5
<p>Comparative results in the medium-scale scenario.</p>
Full article ">Figure 6
<p>Comparative results in the large-scale scenario.</p>
Full article ">Figure 7
<p>Analysis of the population parameters <span class="html-italic">N</span> in the small-scale scenario. The green represents the route estimated by the SLAM process.</p>
Full article ">
22 pages, 958 KiB  
Article
Energy Citizenship in Energy Transition: The Case of the Baltic States
by Rasa Ikstena, Ērika Lagzdiņa, Jānis Brizga, Ivars Kudrenickis and Raimonds Ernšteins
Sustainability 2024, 16(22), 9665; https://doi.org/10.3390/su16229665 - 6 Nov 2024
Viewed by 788
Abstract
The governance of energy systems is undergoing a transformative shift, vital to advancing the energy transition. Understanding the dynamics of energy citizenship and the factors that influence citizen engagement in energy matters is critical for driving social and institutional change. This paper informs [...] Read more.
The governance of energy systems is undergoing a transformative shift, vital to advancing the energy transition. Understanding the dynamics of energy citizenship and the factors that influence citizen engagement in energy matters is critical for driving social and institutional change. This paper informs on the key results of a comprehensive analysis of 54 energy citizenship cases in the Baltic states (Latvia, Estonia, and Lithuania). The study explores the role of citizens in the energy transition and characterizes the socio-economic and geopolitical factors shaping energy citizenship activities in the region. The governance of energy systems represents a significant transformational shift that is essential for energy transition. A more comprehensive understanding of the current state of energy citizenship and the factors influencing the energy transition process could inform the social and institutional changes necessary for the involvement of citizens in energy matters. This desk study represents a crucial element of the EU Horizon 2000 EnergyPROSPECTS project, which aims to map the landscape of energy citizenship in Europe. This paper presents an in-depth analysis of 54 cases from the Baltic states. The findings provide insight into the role of citizens in the transition process and the underlying factors and conditions that shape energy citizenship activities within the specific socio-economic and geopolitical context of the region. In general, energy citizenship in the Baltic states can be seen to exist on a spectrum between reformative and transformative practices. Overall, progress is being made toward systemic changes in the energy sector, with a focus on the democratization of processes. Nevertheless, additional measures to enhance and reinforce energy citizenship, coupled with the advancement of enabling conditions, are imperative at all levels of governance and across all energy transition scenarios. Full article
(This article belongs to the Section Energy Sustainability)
Show Figures

Figure 1

Figure 1
<p>Factors motivating to start an energy citizenship case (Top 5).</p>
Full article ">Figure 2
<p>What do the actors involved in the case want to achieve (Top 5).</p>
Full article ">Figure 3
<p>Distribution of cases in the scale of reformative to transformative case.</p>
Full article ">
15 pages, 9822 KiB  
Article
Phase Space Formulation of Light Propagation on Tilted Planes
by Patrick Gioia, Antonin Gilles, Anas El Rhammad and San Vũ Ngọc
Photonics 2024, 11(11), 1034; https://doi.org/10.3390/photonics11111034 - 3 Nov 2024
Viewed by 409
Abstract
The solution of the Helmholtz equation describing the propagation of light in free space from a plane to another can be described by the angular spectrum operator, which acts in the frequency domain. Many applications require this operator to be generalized to handle [...] Read more.
The solution of the Helmholtz equation describing the propagation of light in free space from a plane to another can be described by the angular spectrum operator, which acts in the frequency domain. Many applications require this operator to be generalized to handle tilted source and target planes, which has led to research investigating the implications of these adaptations. However, the frequency domain representation intrinsically limits the understanding the way the signal is transformed through propagation. Instead, studying how the operator maps the space–frequency components of the wavefield provides essential information that is not available in the frequency domain. In this work, we highlight and exploit the deep relation between wave optics and quantum mechanics to explicitly describe the symplectic action of the tilted angular spectrum in phase space, using mathematical tools that have proven their efficiency for quantum particle physics. These derivations lead to new algorithms that open unprecedented perspectives in various domains involving the propagation of coherent light. Full article
Show Figures

Figure 1

Figure 1
<p>Wavefield-recording planes for the test scenes <span class="html-italic">Dices</span>, <span class="html-italic">Piano</span> and <span class="html-italic">Woods</span>. Plane <span class="html-italic">B</span> is the image of plane <span class="html-italic">A</span> by a rigid 3D transformation. The wavefield captured in <span class="html-italic">B</span> is the image of the one captured in <span class="html-italic">A</span> by operator <math display="inline"><semantics> <mi mathvariant="script">T</mi> </semantics></math>. (<b>a</b>) <span class="html-italic">Dices</span>. (<b>b</b>) <span class="html-italic">Piano</span>. (<b>c</b>) <span class="html-italic">Woods</span>.</p>
Full article ">Figure 2
<p>Numerical reconstructions with focus on specific planes: (<b>a</b>) Hologram A (original pose). (<b>b</b>) Hologram B (target pose). (<b>c</b>) Frequency domain transform of hologram A. (<b>d</b>) Phase space transform of hologram A. (<b>e</b>) Phase space transform of hologram A without phase correction.</p>
Full article ">Figure 3
<p>Hologram editing in phase space. (<b>a</b>) Original hologram (central view). (<b>b</b>,<b>c</b>) Numerical reconstructions of the partially modified hologram A, in which the green dice has been removed and the blue dice has been shifted and rotated (central and bottom–left views, respectively).</p>
Full article ">
15 pages, 3938 KiB  
Article
Whole Blood Transcriptome Analysis in Congenital Anemia Patients
by Maria Sanchez-Villalobos, Eulalia Campos Baños, Elena Martínez-Balsalobre, Veronica Navarro-Ramirez, María Asunción Beltrán Videla, Miriam Pinilla, Encarna Guillén-Navarro, Eduardo Salido-Fierrez and Ana Belén Pérez-Oliva
Int. J. Mol. Sci. 2024, 25(21), 11706; https://doi.org/10.3390/ijms252111706 - 31 Oct 2024
Viewed by 504
Abstract
Congenital anemias include a broad range of disorders marked by inherent abnormalities in red blood cells. These abnormalities include enzymatic, membrane, and congenital defects in erythropoiesis, as well as hemoglobinopathies such as sickle cell disease and thalassemia. These conditions range in presentation from [...] Read more.
Congenital anemias include a broad range of disorders marked by inherent abnormalities in red blood cells. These abnormalities include enzymatic, membrane, and congenital defects in erythropoiesis, as well as hemoglobinopathies such as sickle cell disease and thalassemia. These conditions range in presentation from asymptomatic cases to those requiring frequent blood transfusions, exhibiting phenotypic heterogeneity and different degrees of severity. Despite understanding their different etiologies, all of them have a common pathophysiological origin with congenital defects of erythropoiesis. We can find different types, from congenital sideroblastic anemia (CSA), which is a bone marrow failure anemia, to hemoglobinopathies as sickle cell disease and thalassemia, with a higher prevalence and clinical impact. Recent efforts have focused on understanding erythropoiesis dysfunction in these anemias but, so far, deep gene sequencing analysis comparing all of them has not been performed. Our study used Quant 3′ mRNA-Sequencing to compare transcriptomic profiles of four sickle cell disease patients, ten thalassemia patients, and one rare case of SLC25A38 CSA. Our results showed clear differentiated gene map expressions in all of them with respect to healthy controls. Our study reveals that genes related to metabolic processes, membrane genes, and erythropoiesis are upregulated with respect to healthy controls in all pathologies studied except in the SLC25A38 CSA patient, who shows a unique gene expression pattern compared to the rest of the congenital anemias studied. Our analysis is the first that compares gene expression patterns across different congenital anemias to provide a broad spectrum of genes that could have clinical relevance in these pathologies. Full article
(This article belongs to the Section Molecular Genetics and Genomics)
Show Figures

Figure 1

Figure 1
<p>QuantSeq analysis in different congenital anemias. (<b>A</b>) General scheme of Quant 3′ mRNA–Sequencing procedure. (<b>B</b>–<b>E</b>) Heatmap and pie chart showing under- (blue) or overexpressed (red) genes between controls and transfusion-dependent thalassemia (TDT) (<b>B</b>), non-transfusion-dependent thalassemia (NTDT), (<b>C</b>), sickle cell disease (SCD), (<b>D</b>) and congenital sideroblastic anemia (CSA) patient. Heatmap is restricted to significant data according to Log2FC &lt; −2 or &gt;2, and adjusted <span class="html-italic">p</span>–value &lt; 0.05.</p>
Full article ">Figure 2
<p>The CSA patient exhibits a distinct expression pattern in genes with respect to the rest of the congenital anemias. Heatmaps showing genes, which are significantly underexpressed (blue) or overexpressed (red) across different patient groups. The intensity of the colors indicates the level of expression of each representative gene. Groups studied correlate with those indicated in <a href="#ijms-25-11706-f001" class="html-fig">Figure 1</a> and pathways have been selected considering their importance in red blood cells, including erythropoiesis, iron metabolism, glycolysis, oxidative metabolism, and genes that codified erythrocyte membrane proteins.</p>
Full article ">Figure 3
<p>The CSA patient presents a different expression pattern of genes involved in erythropoiesis and iron metabolism. (<b>A</b>) Analysis of differential expressions of genes involved in erythropoiesis and heme group formation. Increase levels of <span class="html-italic">GATA1</span>, <span class="html-italic">HEMGN</span>, <span class="html-italic">ALAS2</span>, <span class="html-italic">SLC25A38</span>, <span class="html-italic">SLC25A37</span>, <span class="html-italic">ABCB10</span>, and <span class="html-italic">FECH</span> in all congenital anemias with respect to healthy control except the CSA patient. The increase in <span class="html-italic">ERFE</span> levels in all congenital anemias studied. (<b>B</b>) The <span class="html-italic">CDAN1</span> gene expression is significantly decreased in CSA patients. All graphs are represented in fold change with respect to control samples.</p>
Full article ">Figure 4
<p>BPGM gene expression correlates with SCD patients’ severity. (<b>A</b>) Graph with the representative fold change expression compared to healthy controls for the <span class="html-italic">BPGM</span> gene in TDT, NTDT, SCD, and CSA patients. (<b>B</b>) <span class="html-italic">BPGM</span> normalized gene expression in the 4 healthy controls and the 4 SCD patients, with a clear increase in <span class="html-italic">BPGM</span> gene expression in S2 and S4 patients that correlates with patients’ disease severity.</p>
Full article ">Figure 5
<p>A high expression gene profile related to oxidative metabolism in the majority of the congenital anemias compared to healthy donors. (<b>A</b>) Genes related to oxidative metabolism, <span class="html-italic">GLRX5, GPX1, GCLC</span>, and <span class="html-italic">PRDX2</span>, are upregulated in all congenital anemias with respect to healthy controls except in the CSA patient. (<b>B</b>) Significant fold change decrease in <span class="html-italic">SLC25A39</span> gene expression in the CSA patient. All graphs represent the fold change relative to healthy control individuals.</p>
Full article ">Figure 6
<p>The genes related to structural membrane protein expression are differentially expressed in the different congenital anemias. <span class="html-italic">SCL4A1, ANK1, EPB4.1, EPB4.2, SPTB, STOM</span> and <span class="html-italic">SPTA1</span> gene expression profiles are represented for TDT, NTDT, SCD, and CSA patients. A decrease in expression in all of these genes is observed in the CSA patient. All fold changes are relative to healthy control individuals.</p>
Full article ">Figure 7
<p>Dysregulated metabolic pathways in patients with congenital anemias (<b>A</b>–<b>E</b>). STRING analysis of interactions among upregulated genes in NTDT (<b>A</b>) and SCD (<b>C</b>) patients, and downregulated genes in NTDT (<b>B</b>), SCD (<b>D</b>), and CSA (<b>E</b>), compared to healthy controls. The table highlights metabolic pathways significantly impacted, accounting for the total number of genes involved in each network, their strength (Log10(genes implicated/total number of genes in the network)), and significance (<span class="html-italic">p</span>-values corrected for multiple testing within each category using the Benjamini–Hochberg procedure).</p>
Full article ">
7 pages, 2780 KiB  
Case Report
Coronal Cementum and Reduced Enamel Epithelium on Occlusal Surface of Impacted Wisdom Tooth in a Human
by Naohiro Horie, Masaru Murata, Yasuhito Minamida, Hiroki Nagayasu, Tsuyoshi Shimo, Toshiyuki Akazawa, Hidetsugu Tsujigiwa, Youssef Haikel and Hitoshi Nagatsuka
Dent. J. 2024, 12(11), 348; https://doi.org/10.3390/dj12110348 - 30 Oct 2024
Viewed by 469
Abstract
Background: There is only limited research on the coronal cementum of a tooth, and the mechanisms of its forming process are not well-defined. This report presents a coronal cementum on the occlusal surfaces of enamel in an impacted wisdom tooth in a human, [...] Read more.
Background: There is only limited research on the coronal cementum of a tooth, and the mechanisms of its forming process are not well-defined. This report presents a coronal cementum on the occlusal surfaces of enamel in an impacted wisdom tooth in a human, which is not nearly the cervical portion. Materials and Methods: The tooth (Tooth #1) was derived from a 46-year-old female. Histological analysis, including hematoxylin and eosin (HE) and toluidine blue (TB) staining, and Scanning Electron Microscopy and Energy Dispersive X-ray Spectrometer (SEM-EDS) analysis of the extracted tooth were conducted. Radiographic examination showed that Tooth #1 was horizontally impacted in the maxilla and had the apex of a single root placed between the buccal and palatal roots of Tooth #2. Results: Coronal cementum was distributed widely on the enamel, and reduced enamel epithelium was also found with enamel matrix proteins histologically. The formation of acellular cementum was observed to be more predominant than that of the cellular cementum in Tooth #1. SEM showed that the occlusal cementum connected directly with enamel. Calcium mapping revealed an almost similar occlusal cementum and enamel. In addition, the spectrum of elements in coronal cementum resembled the primary cementum according to SEM-EDS. Discussion: Thus, coronal cementogenesis in impacted human teeth might be related to the existence of reduced enamel epithelium. Full article
Show Figures

Figure 1

Figure 1
<p>Initial X-ray images of the 46-year-old female patient. (<b>A</b>): Panoramic image. Note: impacted wisdom teeth (#1, 16, 17, 32). (<b>B</b>): Dental image (#1, 2, 3, 4). Arrow indicates horizontally impacted tooth (#1). (<b>C</b>): CT (axial image). (<b>D</b>): CT (coronal image) showing root apex of upper right third molar (#1) placed between buccal and palatal roots of upper right second molar (#2).</p>
Full article ">Figure 2
<p>Whole image and histological views of extracted Tooth #1. (<b>A</b>): Macroscopic image of #1 showing crown covered with hard tissues. Arrows indicating hard tissues. (<b>B</b>): Non-demineralized section stained with TB. Hard tissues (blue color) and enamel (brown) in black line area. (<b>C</b>): Higher magnification of the black line area in B showing enamel surface covered directly with hard tissues. Blue-stained hard tissues over brown-stained enamel. (<b>D</b>): Demineralized section stained with HE showing lower magnification of crown region. Clear white space indicates completely demineralized enamel. (<b>E</b>): Higher magnification of black line box in (<b>D</b>) showing cementum attached with enamel. Note: Cementum distinguished from bone, including osteocytes. b: bone, c: cementum, and f: fibrous connective tissue.</p>
Full article ">Figure 3
<p>Histological views of horizontal impacted Tooth #1 in HE. (<b>A</b>): Arrows indicating reduced enamel epithelium showing thin bundle. Note: Attachment to primary cementum (PC)–enamel (white clear space) junction (arrowhead). (<b>B</b>): Occlusal cementum (c) on enamel. (<b>C</b>): Co-existence of acellular and cellular cementum matrix. Enamel protein (*) near reduced enamel epithelium (arrows). (<b>D</b>): Cross mark indicating detached cementum pearl in fibrous connective tissues. (<b>E</b>): Acellular coronal cementum contacted directly with reduced enamel epithelium on enamel. Bone with osteoblast lining. b: bone, c: cementum, f: fibrous connective tissue, pc: primary cementum, *: enamel matrix protein, ◆: cellular cementum, arrow: reduced enamel epithelium, arrowhead: primary cementum–enamel junction, cross mark: cementum pearl.</p>
Full article ">Figure 4
<p>SEM-EDS analyses. (<b>A</b>): SEM image of crown region of extracted tooth. (<b>B</b>): High-magnification image of black box area in A. (<b>C</b>): Tiny white dots indicate distribution of Ca element. Yellow dotted line shows border between coronal cementum (*) and enamel. (<b>D</b>,<b>E</b>): Spectrum of EDS analysis. (<b>D</b>): Primary cementum. (<b>E</b>): Coronal cementum pointed out by arrow in A.</p>
Full article ">
20 pages, 899 KiB  
Article
A Koopman Reachability Approach for Uncertainty Analysis in Ground Vehicle Systems
by Alok Kumar, Bhagyashree Umathe and Atul Kelkar
Machines 2024, 12(11), 753; https://doi.org/10.3390/machines12110753 - 24 Oct 2024
Viewed by 1517
Abstract
Recent progress in autonomous vehicle technology has led to the development of accurate and efficient tools for ensuring safety, which is crucial for verifying the reliability and security of vehicles. These vehicles operate under diverse conditions, necessitating the analysis of varying initial conditions [...] Read more.
Recent progress in autonomous vehicle technology has led to the development of accurate and efficient tools for ensuring safety, which is crucial for verifying the reliability and security of vehicles. These vehicles operate under diverse conditions, necessitating the analysis of varying initial conditions and parameter values. Ensuring the safe operation of the vehicle under all these varying conditions is essential. Reachability analysis is an important tool to certify the safety and stability of the vehicle dynamics. We propose a reachability analysis approach for evaluating the response of the vehicle dynamics, specifically addressing uncertainties in the initial states and model parameters. Reachable sets illustrate all the possible states of a dynamical system that can be obtained from a given set of uncertain initial conditions. The analysis is crucial for understanding how variations in initial conditions or system parameters can lead to outcomes such as vehicle collisions or deviations from desired paths. By mapping out these reachable states, it is possible to design systems that maintain safety and reliability despite uncertainties. These insights help to ensure the stability and reliability of the vehicles, even in unpredictable conditions, by reducing accidents and optimizing performance. The nonlinearity of the model complicates the computation of reachable sets in vehicle dynamics. This paper proposes a Koopman theory-based approach that utilizes the Koopman principal eigenfunctions and the Koopman spectrum. By leveraging the Koopman principal eigenfunction, our method simplifies the computational process and offers a formal approximation for backward and forward reachable sets. First, our method effectively computes backward and forward reachable sets for a nonlinear quarter-car model with fixed parameter values. Furthermore, we applied our approach to analyze the uncertainty response for cases with uncertain parameters of the vehicle model. When compared to time-domain simulations, our proposed Koopman approach provided accurate results and also reduced the computational time by half in most cases. This demonstrates the efficiency and reliability of our proposed approach in dynamic systems uncertainty analysis using the reachable sets. Full article
(This article belongs to the Section Industrial Systems)
Show Figures

Figure 1

Figure 1
<p>Nonlinear quarter-car dynamic model.</p>
Full article ">Figure 2
<p>Flowchart for the complete process of our proposed Koopman approach for uncertainty analysis.</p>
Full article ">Figure 3
<p>Diagram for (<b>a</b>) forward reachable set starting from an initial set, (<b>b</b>) backward reachable set for the given target set.</p>
Full article ">Figure 4
<p>Forward reachable sets obtained using the proposed Koopman approach at different times (shown in different colors) for the chassis displacement <math display="inline"><semantics> <msub> <mi>x</mi> <mn>1</mn> </msub> </semantics></math> and chassis velocity <math display="inline"><semantics> <msub> <mi>x</mi> <mn>2</mn> </msub> </semantics></math>. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 5
<p>Forward reachable sets obtained using the proposed Koopman approach at different times (shown in different colors) for the wheel displacement <math display="inline"><semantics> <msub> <mi>x</mi> <mn>3</mn> </msub> </semantics></math> and wheel velocity <math display="inline"><semantics> <msub> <mi>x</mi> <mn>4</mn> </msub> </semantics></math>. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 6
<p>Backward reachable sets obtained using the proposed Koopman approach at different times (shown in different colors) at different times for the chassis displacement <math display="inline"><semantics> <msub> <mi>x</mi> <mn>1</mn> </msub> </semantics></math> and chassis velocity <math display="inline"><semantics> <msub> <mi>x</mi> <mn>2</mn> </msub> </semantics></math>. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 7
<p>Backward reachable sets obtained using the proposed Koopman approach at different times (shown in different colors) at different times for the wheel displacement <math display="inline"><semantics> <msub> <mi>x</mi> <mn>3</mn> </msub> </semantics></math> and wheel velocity <math display="inline"><semantics> <msub> <mi>x</mi> <mn>4</mn> </msub> </semantics></math>. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 8
<p>Forward reachable sets at a fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for varying suspension spring coefficient. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 9
<p>Backward reachable sets at a fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for varying suspension spring coefficient. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 10
<p>Forward reachable sets at a given fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for varying suspension damping coefficient. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 11
<p>Backward reachable sets at a fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> showing the impact of varying suspension damping coefficient. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 12
<p>Forward reachable sets at a given time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for varying wheel mass. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 13
<p>Backward reachable sets at a fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for varying wheel mass. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 14
<p>Forward reachable sets at a fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity (<math display="inline"><semantics> <msub> <mi>x</mi> <mn>2</mn> </msub> </semantics></math>) for varying chassis mass. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 15
<p>Backward reachable sets shown at a fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for the case of varying chassis mass. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 16
<p>Forward reachable sets shown at a fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity (<math display="inline"><semantics> <msub> <mi>x</mi> <mn>2</mn> </msub> </semantics></math>) for varying tire spring coefficient. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">Figure 17
<p>Backward reachable sets at a given fixed time for the chassis displacement <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </semantics></math> and chassis velocity <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mn>2</mn> </msub> <mo>)</mo> </mrow> </semantics></math> for varying tire spring coefficient. The gray tube shows the trajectories obtained from the time-domain simulation with some of the trajectories shown in cyan color.</p>
Full article ">
19 pages, 5209 KiB  
Article
Fault Prediction for Rotating Mechanism of Satellite Based on SSA and Improved Informer
by Qing Lan, Ye Zhu, Baojun Lin, Yizheng Zuo and Yi Lai
Appl. Sci. 2024, 14(20), 9412; https://doi.org/10.3390/app14209412 - 15 Oct 2024
Viewed by 631
Abstract
The rotational mechanism, which plays a critical role in energy supply, payload antenna pointing, and attitude stabilization in satellites is essential for the overall functionality and performance stability of the satellite. This paper takes the space turntable of a specific satellite model as [...] Read more.
The rotational mechanism, which plays a critical role in energy supply, payload antenna pointing, and attitude stabilization in satellites is essential for the overall functionality and performance stability of the satellite. This paper takes the space turntable of a specific satellite model as an example, utilizing high-frequency and high-dimensional telemetry data. An improved informer model is used to predict and diagnose features related to the turntable’s operational health, including temperature, rotational speed, and current. In this paper, we present a forecasting method for turntable temperature data using a hybrid model that combines singular spectrum analysis with an enhanced informer model (SSA-Informer), comparing the results with threshold limits to determine if faults occur in the satellite’s rotational mechanism. First, during telemetry data processing, singular spectrum analysis (SSA) is proposed to retain the long-term and oscillatory trends in the original data while filtering out noise from interference. Next, the improved informer model predicts the turntable temperature based on the mapping relationship between the turntable subsystem’s motor current and temperature, with multiple experiments conducted to obtain optimal parameters. Finally, temperature thresholds generated from the prediction results are used to forecast faults in the rotational mechanism over different time periods. The proposed method is compared with current popular time-series prediction models. The experimental results show that the model achieves high prediction accuracy, with reductions of at least 10% in both the MAE and MSE than CNN-LSTM, DA-RNN, TCN-SE and informer, demonstrating the outstanding advantages of the SSA and improved informer-based method in predicting temperature faults in satellite rotational mechanisms. Full article
Show Figures

Figure 1

Figure 1
<p>Structure ofturntable body.</p>
Full article ">Figure 2
<p>Satellite payload connection and control relationship.</p>
Full article ">Figure 3
<p>CNN-Informer architecture diagram.</p>
Full article ">Figure 4
<p>Diagram of motor current and turntable temperature data.</p>
Full article ">Figure 5
<p>SSA decomposition sub-sequence of motor current.</p>
Full article ">Figure 5 Cont.
<p>SSA decomposition sub-sequence of motor current.</p>
Full article ">Figure 6
<p>SSA reconstruction sequence of current and raw sequence.</p>
Full article ">Figure 7
<p>SSA decomposition sub-sequence of turntable temperature.</p>
Full article ">Figure 7 Cont.
<p>SSA decomposition sub-sequence of turntable temperature.</p>
Full article ">Figure 8
<p>SSA reconstruction sequence of temperature and raw sequence.</p>
Full article ">Figure 9
<p>Model loss curve.</p>
Full article ">Figure 10
<p>Comparison of predicted data and true data.</p>
Full article ">Figure 11
<p>Schematic diagram of turntable temperature threshold generation and fault prediction.</p>
Full article ">
14 pages, 6262 KiB  
Article
Degradation-Guided Multi-Modal Fusion Network for Depth Map Super-Resolution
by Lu Han, Xinghu Wang, Fuhui Zhou and Diansheng Wu
Electronics 2024, 13(20), 4020; https://doi.org/10.3390/electronics13204020 - 12 Oct 2024
Viewed by 452
Abstract
Depth map super-resolution (DSR) is a technique aimed at restoring high-resolution (HR) depth maps from low-resolution (LR) depth maps. In this process, color images are commonly used as guidance to enhance the restoration procedure. However, the intricate degradation of LR depth poses a [...] Read more.
Depth map super-resolution (DSR) is a technique aimed at restoring high-resolution (HR) depth maps from low-resolution (LR) depth maps. In this process, color images are commonly used as guidance to enhance the restoration procedure. However, the intricate degradation of LR depth poses a challenge, and previous image-guided DSR approaches, which implicitly model the degradation in the spatial domain, often fall short of producing satisfactory results. To address this challenge, we propose a novel approach called the Degradation-Guided Multi-modal Fusion Network (DMFNet). DMFNet explicitly characterizes the degradation and incorporates multi-modal fusion in both spatial and frequency domains to improve the depth quality. Specifically, we first introduce the deep degradation regularization loss function, which enables the model to learn the explicit degradation from the LR depth maps. Simultaneously, DMFNet converts the color images and depth maps into spectrum representations to provide comprehensive multi-domain guidance. Consequently, we present the multi-modal fusion block to restore the depth maps by leveraging both the RGB-D spectrum representations and the depth degradation. Extensive experiments demonstrate that DMFNet achieves state-of-the-art (SoTA) performance on four benchmarks, namely the NYU-v2, Middlebury, Lu, and RGB-D-D datasets. Full article
(This article belongs to the Special Issue Advances in Data-Driven Artificial Intelligence)
Show Figures

Figure 1

Figure 1
<p>Visual comparison example on NYU-v2 dataset [<a href="#B32-electronics-13-04020" class="html-bibr">32</a>]. (<b>a</b>) Color image input, (<b>b</b>) low-resolution depth input, (<b>c</b>) ground truth (GT) depth, (<b>d</b>) DKN [<a href="#B3-electronics-13-04020" class="html-bibr">3</a>], (<b>e</b>) DCTNet [<a href="#B6-electronics-13-04020" class="html-bibr">6</a>], and (<b>f</b>) our proposed DMFNet. The visualization and error comparison demonstrates the superior performance of our DMFNet in restoring clear and accurate depth results.</p>
Full article ">Figure 2
<p>An overview of the proposed DMFNet, which consists of the degradation learning branch and depth restoration branch. The former branch employs the Deep Degradation Regularization Module (DDRM) to gradually learn explicit degradation from the LR depth, while the latter branch restores fine-grained depth via the Multi-modal Fusion Block (MFB) and the degradation constraint.</p>
Full article ">Figure 3
<p>Scheme of the proposed multi-modal fusion block (MFB).</p>
Full article ">Figure 4
<p>Visual results on the synthetic NYU-v2 dataset (<math display="inline"><semantics> <mrow> <mo>×</mo> <mn>16</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 5
<p>Visual results on the synthetic RGB-D-D dataset (<math display="inline"><semantics> <mrow> <mo>×</mo> <mn>16</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 6
<p>Visual results on the synthetic Lu dataset (<math display="inline"><semantics> <mrow> <mo>×</mo> <mn>16</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 7
<p>Visual results on the synthetic Middlebury dataset (<math display="inline"><semantics> <mrow> <mo>×</mo> <mn>16</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 8
<p>Visual results on the real-world RGB-D-D dataset.</p>
Full article ">Figure 9
<p>Denoising visual results on the synthetic NYU-v2 dataset.</p>
Full article ">Figure 10
<p>Visual comparison of the intermediate depth features on RGB-D-D dataset (<math display="inline"><semantics> <mrow> <mo>×</mo> <mn>4</mn> </mrow> </semantics></math>).</p>
Full article ">
Back to TopTop