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Search Results (1,131)

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19 pages, 1008 KiB  
Article
EEG-Based Mobile Robot Control Using Deep Learning and ROS Integration
by Bianca Ghinoiu, Victor Vlădăreanu, Ana-Maria Travediu, Luige Vlădăreanu, Abigail Pop, Yongfei Feng and Andreea Zamfirescu
Technologies 2024, 12(12), 261; https://doi.org/10.3390/technologies12120261 (registering DOI) - 14 Dec 2024
Viewed by 62
Abstract
Efficient BCIs (Brain-Computer Interfaces) harnessing EEG (Electroencephalography) have shown potential in controlling mobile robots, also presenting new possibilities for assistive technologies. This study explores the integration of advanced deep learning models—ASTGCN, EEGNetv4, and a combined CNN-LSTM architecture—with ROS (Robot Operating System) to control [...] Read more.
Efficient BCIs (Brain-Computer Interfaces) harnessing EEG (Electroencephalography) have shown potential in controlling mobile robots, also presenting new possibilities for assistive technologies. This study explores the integration of advanced deep learning models—ASTGCN, EEGNetv4, and a combined CNN-LSTM architecture—with ROS (Robot Operating System) to control a two-wheeled mobile robot. The models were trained using a published EEG dataset, which includes signals from subjects performing thought-based tasks. Each model was evaluated based on its accuracy, F1-score, and latency. The CNN-LSTM architecture model exhibited the best performance on the cross-subject strategy with an accuracy of 88.5%, demonstrating significant potential for real-time applications. Integration with ROS was facilitated through a custom middleware, enabling seamless translation of neural commands into robot movements. The findings indicate that the CNN-LSTM model not only outperforms existing EEG-based systems in terms of accuracy but also underscores the practical feasibility of implementing such systems in real-world scenarios. Considering its efficacy, CNN-LSTM shows a great potential for assistive technology in the future. This research contributes to the development of a more intuitive and accessible robotic control system, potentially enhancing the quality of life for individuals with mobility impairments. Full article
(This article belongs to the Special Issue Advanced Autonomous Systems and Artificial Intelligence Stage)
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<p>Overall system Architecture.</p>
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<p>Model architecture for CNN-LSTM.</p>
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<p>Confusion matrix for ASTGCN in the cross-subject evaluation.</p>
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<p>Training accuracy for Cross-Subject Strategy: (<b>a</b>) EEGNetv4, ASTGCN, and CNNLSTM (100 epochs); (<b>b</b>) EEGNetv4, and CNNLSTM (300 epochs).</p>
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<p>Comparison between Adam and RAdam.</p>
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18 pages, 4209 KiB  
Article
Validity Analysis of Monocular Human Pose Estimation Models Interfaced with a Mobile Application for Assessing Upper Limb Range of Motion
by Rayele Moreira, Silmar Teixeira, Renan Fialho, Aline Miranda, Lucas Daniel Batista Lima, Maria Beatriz Carvalho, Ana Beatriz Alves, Victor Hugo Vale Bastos and Ariel Soares Teles
Sensors 2024, 24(24), 7983; https://doi.org/10.3390/s24247983 (registering DOI) - 14 Dec 2024
Viewed by 145
Abstract
Human Pose Estimation (HPE) is a computer vision application that utilizes deep learning techniques to precisely locate Key Joint Points (KJPs), enabling the accurate description of a person’s pose. HPE models can be extended to facilitate Range of Motion (ROM) assessment by leveraging [...] Read more.
Human Pose Estimation (HPE) is a computer vision application that utilizes deep learning techniques to precisely locate Key Joint Points (KJPs), enabling the accurate description of a person’s pose. HPE models can be extended to facilitate Range of Motion (ROM) assessment by leveraging patient photographs. This study aims to evaluate and compare the performance of HPE models for assessing upper limbs ROM. A physiotherapist evaluated the degrees of ROM in shoulders (flexion, extension, and abduction) and elbows (flexion and extension) for fifty-two participants using both Universal Goniometer (UG) and five HPE models. Participants were instructed to repeat each movement three times to obtain measurements with the UG, then positioned while photos were captured using the NLMeasurer mobile application. The paired t-test, bias, and error measures were employed to evaluate the difference and agreement between measurement methods. Results indicated that the MoveNet Thunder INT16 model exhibited superior performance. Root Mean Square Errors obtained through this model were <10° in 8 of 10 analyzed movements. HPE models demonstrated better performance in shoulder flexion and abduction movements while exhibiting unsatisfactory performance in elbow flexion. Challenges such as image perspective distortion, environmental lighting conditions, images in monocular view, and complications in the pose may influence the models’ performance. Nevertheless, HPE models show promise in identifying KJPs and facilitating ROM measurements, potentially enhancing convenience and efficiency in assessments. However, their current accuracy for this application is unsatisfactory, highlighting the need for caution when considering automated upper limb ROM measurement with them. The implementation of these models in clinical practice does not diminish the crucial role of examiners in carefully inspecting images and making adjustments to ensure measurement reliability. Full article
(This article belongs to the Special Issue e-Health Systems and Technologies)
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<p><span class="html-italic">NLMeasurer</span> screenshots (texts in Brazilian Portuguese (PT-BR) language) with application screen with (<b>a</b>) participant records to start an assessment and buttons with two types of assessment (postural and goniometry); and (<b>b</b>) a list of all captured images of the one participant.</p>
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<p>Angle between two body segments.</p>
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<p>Virtual goniometer showing degrees (i.e., values for ROM) drawn on the device screen: (<b>a</b>) VG in left shoulder abduction; and (<b>b</b>) VG in left shoulder extension.</p>
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<p>Bland Altman plot showing the level of agreement between <span class="html-italic">MNT16Q</span> and <span class="html-italic">UG</span> when assessing shoulders. The centered red line shows bias, and the two outer dotted lines represent the upper and lower 95% confidence intervals. The trend line illustrates the correlation between the mean and the difference between the model and UG, serving as a parameter to analyze heteroscedasticity.</p>
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<p>Bland Altman plot showing the level of agreement between <span class="html-italic">MNT16Q</span> and UG when assessing elbows. The centered red line shows bias, and the two outer dotted lines represent the upper and lower 95% confidence intervals.The trend line illustrates the correlation between the mean and the difference between the model and UG, serving as a parameter to analyze heteroscedasticity.</p>
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<p>ROM measurements significantly deviating from those expected for healthy individuals by: <span class="html-italic">MNL8Q</span> (<b>a</b>)—right shoulder flexion and <span class="html-italic">MNT8Q</span>; (<b>b</b>)—right elbow flexion; (<b>c</b>)—left elbow flexion and (<b>d</b>)—right elbow extension).</p>
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28 pages, 5556 KiB  
Review
MXenes in Perovskite Solar Cells: Emerging Applications and Performance Enhancements
by Bin Luo, Xiaodan Wang, Kamale Tuokedaerhan, Shuying Wang, Chen Wang, Xiaohao Shi, Zhiqiang Yu and Xiangqian Shen
Coatings 2024, 14(12), 1564; https://doi.org/10.3390/coatings14121564 - 13 Dec 2024
Viewed by 290
Abstract
Perovskite solar cells (PSCs) have emerged as promising candidates for next-generation photovoltaic technology due to their remarkable power-conversion efficiencies (PCEs). Since their introduction, the PCE of PSCs has advanced from 3.8% to over 26%. Nonetheless, challenges pertaining to stability and reliability continue to [...] Read more.
Perovskite solar cells (PSCs) have emerged as promising candidates for next-generation photovoltaic technology due to their remarkable power-conversion efficiencies (PCEs). Since their introduction, the PCE of PSCs has advanced from 3.8% to over 26%. Nonetheless, challenges pertaining to stability and reliability continue to impede their commercial viability. Recent progress in interface engineering and materials science has underscored the potential of two-dimensional (2D) materials, particularly MXenes, in mitigating these challenges. MXenes represent a class of two-dimensional materials with significant potential for application in PSCs, attributed to their exceptional electrical conductivity, high carrier mobility, remarkable optical transparency, chemical stability, and tunable surface chemical properties. When employed as electron transport layers, MXenes enhance charge transfer and extraction efficiency, leading to substantial improvements in PCEs. Furthermore, their integration into hole transport layers and use as interfacial modifiers contribute to the mitigation of degradation pathways, thereby enhancing device longevity. The unique structural and electronic characteristics of MXenes facilitate their application as transparent electrodes, presenting opportunities for cost reduction and improved optical properties. This review provides a comprehensive overview of the current advancements in MXene-based PSCs, emphasizing significant accomplishments and exploring future research directions aimed at enhancing the efficiency and stability of these devices. Full article
12 pages, 3766 KiB  
Article
The Trapping Mechanism at the AlGaN/GaN Interface and the Turn-On Characteristics of the p-GaN Direct-Coupled FET Logic Inverters
by Junfeng Yu, Jihong Ding, Tao Wang, Yukai Huang, Wenzhang Du, Jiao Liang, Hongping Ma, Qingchun Zhang, Liang Li, Wei Huang and Wei Zhang
Nanomaterials 2024, 14(24), 1984; https://doi.org/10.3390/nano14241984 - 11 Dec 2024
Viewed by 227
Abstract
The trapping mechanism at the AlGaN/GaN interface in the p-GaN high electron mobility transistors (HEMTs) and its impact on the turn-on characteristics of direct-coupled FET logic (DCFL) inverters were investigated across various supply voltages (VDD) and test frequencies (f [...] Read more.
The trapping mechanism at the AlGaN/GaN interface in the p-GaN high electron mobility transistors (HEMTs) and its impact on the turn-on characteristics of direct-coupled FET logic (DCFL) inverters were investigated across various supply voltages (VDD) and test frequencies (fm). The frequency-conductance method identified two trap states at the AlGaN/GaN interface (trap activation energy Ec-ET ranges from 0.345 eV to 0.363 eV and 0.438 eV to 0.47 eV). As VDD increased from 1.5 V to 5 V, the interface traps captured more electrons, increasing the channel resistance (Rchannel) and drift-region resistance (Rdrift) of the p-GaN HEMTs and raising the low-level voltage (VOL) from 0.56 V to 1.01 V. At fm = 1 kHz, sufficient trapping and de-trapping led to a delay of 220 µs and a VOL instability of 320 mV. Additionally, as fm increased from 1 kHz to 200 kHz, a positive shift in the threshold voltage of p-GaN HEMTs occurred due to the dominance of trapping. This shift caused VOL to rise from 1.02 V to 1.40 V and extended the fall time (tfall) from 153 ns to 1 µs. This investigation enhances the understanding of DCFL GaN inverters’ behaviors from the perspective of device physics on power switching applications. Full article
(This article belongs to the Special Issue Advanced Studies in Wide-Bandgap Nanomaterials and Devices)
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<p>(<b>a</b>) Cross-sectional schematic of the monolithic integrated E/D-mode HEMT. (<b>b</b>) The fabrication process of E/D HEMTs.</p>
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<p>(<b>a</b>) C-V curve for 1 kHz &lt; <span class="html-italic">f</span><sub>m</sub> &lt; 5 MHz. (<b>b</b>) Schematic diagram of the mechanism of the C-V curve shift.</p>
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<p>(<b>a</b>) <span class="html-italic">G</span><sub>p</sub>/<span class="html-italic">w</span> is a function of <span class="html-italic">w</span> at selected voltages; the inset in (<b>a</b>) shows the schematic of the p-GaN gate stack and the equivalent circuit model. (<b>b</b>) <span class="html-italic">D</span><sub>it</sub> is a function of <span class="html-italic">E</span><sub>C</sub>-<span class="html-italic">E</span><sub>T</sub> and <span class="html-italic">τ</span><sub>t</sub> is a function of <span class="html-italic">V</span><sub>G.</sub></p>
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<p>Transfer characteristics of p-GaN HEMT.</p>
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<p>(<b>a</b>) The circuit of the DCFL inverter. (<b>b</b>) The equivalent discharge circuit of the DCFL inverter, (<b>c</b>) The microscope image of the DCFL inverter.</p>
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<p>(<b>a</b>) Output voltage <span class="html-italic">V</span><sub>out</sub> waveforms diagram under different <span class="html-italic">V</span><sub>DD</sub>. (<b>b</b>) Low-level voltage (<span class="html-italic">V</span><sub>OL</sub>) and <span class="html-italic">K</span> value under different <span class="html-italic">V</span><sub>DD.</sub></p>
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<p>(<b>a</b>) Simulated channel electric field density under different <span class="html-italic">V</span><sub>DD;</sub> (<b>b</b>) impact of trapping location on resistance degradation.</p>
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<p>(<b>a</b>) Oscilloscope screenshot of <span class="html-italic">V</span><sub>out</sub> waveforms at different frequencies. (<b>b</b>) Comparison diagram of falling edge at time t<sub>1.</sub></p>
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<p>(<b>a</b>) Numerical fitting of the output waveform of the inverter at fm = 1 kHz and the interface state ionization rate after turn-on. (<b>b</b>) The impact of trap parameters on the inverter’s performance.</p>
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23 pages, 2719 KiB  
Article
An Implementation of Web-Based Answer Platform in the Flutter Programming Learning Assistant System Using Docker Compose
by Lynn Htet Aung, Soe Thandar Aung, Nobuo Funabiki, Htoo Htoo Sandi Kyaw and Wen-Chung Kao
Electronics 2024, 13(24), 4878; https://doi.org/10.3390/electronics13244878 - 11 Dec 2024
Viewed by 315
Abstract
Programming has gained significant importance worldwide as societies increasingly rely on computer application systems. To support novices in learning various programming languages, we have developed the Programming Learning Assistant System (PLAS). It offers several types of exercise problems with different learning goals [...] Read more.
Programming has gained significant importance worldwide as societies increasingly rely on computer application systems. To support novices in learning various programming languages, we have developed the Programming Learning Assistant System (PLAS). It offers several types of exercise problems with different learning goals and levels for step-by-step self-study. As a personal answer platform in PLAS, we have implemented a web application using Node.js and EJS for Java and Python programming. Recently, the Flutter framework with Dart programming has become popular, enabling developers to build applications for mobile, web, and desktop environments from a single codebase. Thus, we have extended PLAS by implementing the Flutter environment with Visual Studio Code to support it. Additionally, we have developed an image-based user interface (UI) testing tool to verify student source code by comparing its generated UI image with the standard one using the ORB and SIFT algorithms in OpenCV. For efficient distribution to students, we have generated Docker images of the answer platform, Flutter environment, and image-based UI testing tool. In this paper, we present the implementation of a web-based answer platform for the Flutter Programming Learning Assistant System (FPLAS) by integrating three Docker images using Docker Compose. Additionally, to capture UI images automatically, an Nginx web application server is adopted with its Docker image. For evaluations, we asked 10 graduate students at Okayama University, Japan, to install the answer platform on their PCs and solve five exercise problems. All the students successfully completed the problems, which confirms the validity and effectiveness of the proposed system. Full article
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<p>Software architecture of the web-based answer platform for the FPLAS.</p>
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<p>Client-side code structure (<b>left</b>) and home page (<b>right</b>) for the <span class="html-italic">FPLAS</span>.</p>
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<p>Exercise 5 assignment for the proposed answer platform.</p>
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<p>Highlighting differences with red boxes for incorrect answers in Exercise 5.</p>
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<p>Server-side code structures for the FPLAS.</p>
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<p>Analysis of feedback on <span class="html-italic">mobile application development</span> and <span class="html-italic">Flutter</span>.</p>
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<p>Analysis of students’ feedback based on <span class="html-italic">Docker</span>.</p>
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7 pages, 2576 KiB  
Proceeding Paper
The Design of a Mobile Sensing Framework for Road Surfaces Based on Multi-Modal Sensors
by Haiyang Lyu, Yu Huang, Jianchun Hua, Wenmei Li, Tianju Wu, Hanru Zhang and Wangta Ma
Proceedings 2024, 110(1), 21; https://doi.org/10.3390/proceedings2024110021 - 11 Dec 2024
Viewed by 272
Abstract
Road surface information, encompassing aspects like road surface damages and facility distributions, is vital for maintaining and updating roads in smart cities. The proposed mobile sensing framework uses multi-modal sensors, including a GPS, gyroscope, accelerometer, camera, and Wi-Fi, integrated into a Jetson Nano [...] Read more.
Road surface information, encompassing aspects like road surface damages and facility distributions, is vital for maintaining and updating roads in smart cities. The proposed mobile sensing framework uses multi-modal sensors, including a GPS, gyroscope, accelerometer, camera, and Wi-Fi, integrated into a Jetson Nano to collect comprehensive road surface information. The collected data are processed, stored, and analyzed on the server side, with results accessible via RESTful APIs. This system enables the detection of road conditions, which are visualized through the web mapping technique. Based on this concept, the Mobile Sensor Framework for Road Surface analysis (MSF4RS) is designed, and its use significantly enhances road surface data acquisition and analysis. Key contributions include (1) the integration of multi-modal IoT sensors to capture comprehensive road surface data; (2) the development of a software environment that facilitates robust data processing; and (3) the execution of experiments using the MSF4RS, which synergistically combines hardware and software components. The framework leverages advanced sensor technologies and server-based computational methods and offers a user-friendly web interface for the dynamic visualization and interactive exploration of road surface conditions. Experiments confirm the framework’s effectiveness in capturing and visualizing road surface data, demonstrating significant potential for smart city applications. Full article
(This article belongs to the Proceedings of The 31st International Conference on Geoinformatics)
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<p>The overall design of the framework.</p>
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<p>Sensor configuration in the vehicle: (<b>a</b>) Jetson Nano with Wi-Fi module; (<b>b</b>) GPS; (<b>c</b>) IMU; (<b>d</b>) camera.</p>
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<p>Data processing for different sensors: (<b>a</b>) detection result of camera; (<b>b</b>) spatially transformed acceleration.</p>
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<p>Interaction and visualization of BFRS detection results: (<b>a</b>) interactive layer controls; (<b>b</b>) dynamic visualization based on selected filter values (labeled by the blue bubble with white circle). The non-English annotations in the base map are automatically generated based on the geographic location by the map data provider, and it doesn’t affect the interaction and visualization of the Web page.</p>
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17 pages, 4663 KiB  
Article
Remote Water Quality Monitoring System for Use in Fairway Applications
by Marek Staude, Piotr Brożek, Ewelina Kostecka, Dariusz Tarnapowicz and Jan Wysocki
Appl. Sci. 2024, 14(23), 11406; https://doi.org/10.3390/app142311406 - 7 Dec 2024
Viewed by 543
Abstract
In the context of climate change, there is a growing need for accurate, real-time data on water quality in river waterways. This results in the development of advanced monitoring systems. This article presents a remote water quality monitoring system designed specifically for use [...] Read more.
In the context of climate change, there is a growing need for accurate, real-time data on water quality in river waterways. This results in the development of advanced monitoring systems. This article presents a remote water quality monitoring system designed specifically for use in inland waterways, the basic elements of which are placed in a buoy with an IoT unit. The proposed system uses a network of sensors strategically placed along the waterway to continuously measure critical parameters: temperature, pH, dissolved oxygen, and conductivity. Various compatibility, efficiency, and ease-of-use tests have been conducted to verify each aspect of the monitoring system. It has been shown that the sensors operate within the intended accuracy ranges. The central unit equipped with a GSM (Global System for Mobile Communications) module can wirelessly transmit data to a main server, enabling remote access and analysis via a user-friendly interface of the developed application. The paper details the technical architecture of the system, the integration of GSM technology to ensure reliable data transmission, and the results of the monitoring studies of the proposed parameters. The remote monitoring system offers significant benefits in terms of early detection of pollution events, ensuring the safety of aquatic life, and supporting sustainable navigation practices. The research results highlight the potential of GSM-based remote monitoring systems to revolutionize water quality management in waterways in various regions. Full article
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<p>Schematic diagram of the remote water quality monitoring system.</p>
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<p>A damaged buoy taken from the waterway: (<b>a</b>) made of metal; (<b>b</b>) made of composites.</p>
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<p>Time course of the discharge voltage of a LiFePO<sub>4</sub> 20Ah battery with a discharge current of 400 mA.</p>
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<p>Central unit topology.</p>
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<p>Examples of data on the main server.</p>
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<p>Sample visualization of water parameters measured.</p>
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<p>Dissolved oxygen levels in water as a function of time.</p>
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<p>Conductivity of water as a function of time (unit: mS/m).</p>
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<p>pH levels of water as a function of time.</p>
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<p>Temperature variation over time.</p>
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24 pages, 5123 KiB  
Article
An Empirical Model-Based Algorithm for Removing Motion-Caused Artifacts in Motor Imagery EEG Data for Classification Using an Optimized CNN Model
by Rajesh Kannan Megalingam, Kariparambil Sudheesh Sankardas and Sakthiprasad Kuttankulangara Manoharan
Sensors 2024, 24(23), 7690; https://doi.org/10.3390/s24237690 - 30 Nov 2024
Viewed by 538
Abstract
Electroencephalography (EEG) is a non-invasive technique with high temporal resolution and cost-effective, portable, and easy-to-use features. Motor imagery EEG (MI-EEG) data classification is one of the key applications within brain–computer interface (BCI) systems, utilizing EEG signals from motor imagery tasks. BCI is very [...] Read more.
Electroencephalography (EEG) is a non-invasive technique with high temporal resolution and cost-effective, portable, and easy-to-use features. Motor imagery EEG (MI-EEG) data classification is one of the key applications within brain–computer interface (BCI) systems, utilizing EEG signals from motor imagery tasks. BCI is very useful for people with severe mobility issues like quadriplegics, spinal cord injury patients, stroke patients, etc., giving them the freedom to a certain extent to perform activities without the need for a caretaker, like driving a wheelchair. However, motion artifacts can significantly affect the quality of EEG recordings. The conventional EEG enhancement algorithms are effective in removing ocular and muscle artifacts for a stationary subject but not as effective when the subject is in motion, e.g., a wheelchair user. In this research study, we propose an empirical error model-based artifact removal approach for the cross-subject classification of motor imagery (MI) EEG data using a modified CNN-based deep learning algorithm, designed to assist wheelchair users with severe mobility issues. The classification method applies to real tasks with measured EEG data, focusing on accurately interpreting motor imagery signals for practical application. The empirical error model evolved from the inertial sensor-based acceleration data of the subject in motion, the weight of the wheelchair, the weight of the subject, and the surface friction of the terrain under the wheelchair. Three different wheelchairs and five different terrains, including road, brick, concrete, carpet, and marble, are used for artifact data recording. After evaluating and benchmarking the proposed CNN and empirical model, the classification accuracy achieved is 94.04% for distinguishing between four specific classes: left, right, front, and back. This accuracy demonstrates the model’s effectiveness compared to other state-of-the-art techniques. The comparative results show that the proposed approach is a potentially effective way to raise the decoding efficiency of motor imagery BCI. Full article
(This article belongs to the Section Biomedical Sensors)
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<p>Overall architecture of the proposed empirical model-based artifacts removal and LM-CNN-based classification.</p>
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<p>The proposed LM-CNN architecture.</p>
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<p>(<b>a</b>) Image of the ultra-cortex ‘Mark IV’; (<b>b</b>) Cyton Board.</p>
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<p>Order and duration of motor actions during a recording session.</p>
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<p>The electrode positions used during the recordings.</p>
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<p>The image shows a sample reference EEG recording session.</p>
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<p>Empirical error model creation and the flow chart.</p>
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<p>The three different wheelchairs that were built for the EEG data recording purpose.</p>
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<p>The above images show the recording sessions we performed in the artifact EEG recording: (<b>a</b>) wheelchair-2 on concrete surface, (<b>b</b>) wheelchair-3 on a brick surface, (<b>c</b>) wheelchair-2 on the road, (<b>d</b>) wheelchair-2 on the marble surface, (<b>e</b>) wheelchair-2 on the carpet surface.</p>
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<p>The model performance comparison for a subject in the same wheelchair but on different surfaces without the empirical model.</p>
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<p>The model performance comparison for a subject on the same surface but using different wheelchairs without the empirical model.</p>
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<p>The proposed model performance comparison of a subject in the same wheelchair but on different surfaces.</p>
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<p>The proposed model performance comparison of a subject in the same wheelchair but on different surfaces.</p>
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<p>(<b>a</b>) The confusion matrix for a subject’s data without empirical error removal and (<b>b</b>) the confusion matrix for a subject’s data with empirical error removal. The confusion matrix represents the classification results for a single subject’s data, not an average across multiple subjects.</p>
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20 pages, 2772 KiB  
Article
Activities of Daily Living Object Dataset: Advancing Assistive Robotic Manipulation with a Tailored Dataset
by Md Tanzil Shahria and Mohammad H. Rahman
Sensors 2024, 24(23), 7566; https://doi.org/10.3390/s24237566 - 27 Nov 2024
Viewed by 395
Abstract
The increasing number of individuals with disabilities—over 61 million adults in the United States alone—underscores the urgent need for technologies that enhance autonomy and independence. Among these individuals, millions rely on wheelchairs and often require assistance from another person with activities of daily [...] Read more.
The increasing number of individuals with disabilities—over 61 million adults in the United States alone—underscores the urgent need for technologies that enhance autonomy and independence. Among these individuals, millions rely on wheelchairs and often require assistance from another person with activities of daily living (ADLs), such as eating, grooming, and dressing. Wheelchair-mounted assistive robotic arms offer a promising solution to enhance independence, but their complex control interfaces can be challenging for users. Automating control through deep learning-based object detection models presents a viable pathway to simplify operation, yet progress is impeded by the absence of specialized datasets tailored for ADL objects suitable for robotic manipulation in home environments. To bridge this gap, we present a novel ADL object dataset explicitly designed for training deep learning models in assistive robotic applications. We curated over 112,000 high-quality images from four major open-source datasets—COCO, Open Images, LVIS, and Roboflow Universe—focusing on objects pertinent to daily living tasks. Annotations were standardized to the YOLO Darknet format, and data quality was enhanced through a rigorous filtering process involving a pre-trained YOLOv5x model and manual validation. Our dataset provides a valuable resource that facilitates the development of more effective and user-friendly semi-autonomous control systems for assistive robots. By offering a focused collection of ADL-related objects, we aim to advance assistive technologies that empower individuals with mobility impairments, addressing a pressing societal need and laying the foundation for future innovations in human–robot interaction within home settings. Full article
(This article belongs to the Special Issue Vision Sensors for Object Detection and Tracking)
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<p>Examples of mislabeled or ignored data from the COCO dataset: (<b>a</b>) incorrect class label; (<b>b</b>) incorrect class label; (<b>c</b>) incorrect class label; (<b>d</b>) incorrect class label.</p>
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<p>Examples of mislabeled or ignored data from the LVIS dataset: (<b>a</b>) missing annotation for one class; (<b>b</b>) missing annotations for multiple classes; (<b>c</b>) incorrect class label; (<b>d</b>) incorrect bounding box information.</p>
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<p>Examples of mislabeled or ignored data from the Open Images dataset: (<b>a</b>) incorrect class label; (<b>b</b>) incorrect class label; (<b>c</b>) missing annotations; (<b>d</b>) incorrect class label.</p>
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15 pages, 10219 KiB  
Article
Effect of Alkyl Side Chain Length on Electrical Performance of Ion-Gel-Gated OFETs Based on Difluorobenzothiadiazole-Based D-A Copolymers
by Han Zhou, Zaitian Cheng, Guoxing Pan, Lin Hu and Fapei Zhang
Polymers 2024, 16(23), 3287; https://doi.org/10.3390/polym16233287 - 26 Nov 2024
Viewed by 376
Abstract
The performance of organic field-effect transistors (OFETs) is highly dependent on the dielectric–semiconductor interface, especially in ion-gel-gated OFETs, where a significantly high carrier density is induced at the interface at a low gate voltage. This study investigates how altering the alkyl side chain [...] Read more.
The performance of organic field-effect transistors (OFETs) is highly dependent on the dielectric–semiconductor interface, especially in ion-gel-gated OFETs, where a significantly high carrier density is induced at the interface at a low gate voltage. This study investigates how altering the alkyl side chain length of donor–acceptor (D-A) copolymers impacts the electrical performance of ion-gel-gated OFETs. Two difluorobenzothiadiazole-based D-A copolymers, PffBT4T-2OD and PffBT4T-2DT, are compared, where the latter features longer alkyl side chains. Although PffBT4T-2DT shows a 2.4-fold enhancement of charge mobility in the SiO2-gated OFETs compared to its counterpart due to higher crystallinity in the film, PffBT4T-2OD outperforms PffBT4T-2DT in the ion-gel-gated OFETs, manifested by an extraordinarily high mobility of 17.7 cm2/V s. The smoother surface morphology, as well as stronger interfacial interaction between the ion-gel dielectric and PffBT4T-2OD, enhances interfacial charge accumulation, which leads to higher mobility. Furthermore, PffBT4T-2OD is blended with a polymeric elastomer SEBS to achieve ion-gel-gated flexible OFETs. The blend devices exhibit high mobility of 8.6 cm2/V s and high stretchability, retaining 45% of initial mobility under 100% tensile strain. This study demonstrates the importance of optimizing the chain structure of polymer semiconductors and the semiconductor–dielectric interface to develop low-voltage and high-performance flexible OFETs for wearable electronics applications. Full article
(This article belongs to the Section Polymer Chemistry)
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<p>(<b>a</b>) Chemical structure of PffBT4T-2OD and PffBT4T-2DT. (<b>b</b>) The normalized UV-visible absorption spectra of the PffBT4T-2OD and PffBT4T-2DT film.</p>
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<p>(<b>a</b>,<b>b</b>) Two-dimensional GIXRD patterns of the PffBT4T-2OD film (<b>a</b>) and PffBT4T-2DT film (<b>b</b>), respectively; (<b>c</b>,<b>d</b>) Cross-section profiles along the <span class="html-italic">q<sub>xy</sub></span> (<b>c</b>) and <span class="html-italic">q<sub>z</sub></span> (<b>d</b>) directions of the GIXRD patterns shown in (<b>a</b>,<b>b</b>).</p>
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<p>(<b>a</b>) The molecular structure of [EMIM]<sup>+</sup>[TFSI]<sup>−</sup> and P(VDF-HFP). (<b>b</b>) The photograph of prepared ion-gel films. (<b>c</b>) The specific capacitance–frequency curve of ion-gel film. The inset shows the schematic of an Au/ion-gel/Au capacitor structure.</p>
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<p>(<b>a</b>,<b>b</b>) Typical transfer curves of the ion-gel-gated OFETs (W = 2 mm/L = 50 μm) based on PffBT4T-2OD films (<b>a</b>) and PffBT4T-2DT films (<b>b</b>). The inset of (<b>a</b>) illustrates the schematic of ion-gel-gated OFETs on the TG/BC structure. (<b>c</b>,<b>d</b>) Corresponding output curves of the ion-gel-gated OFETs of PffBT4T-2OD films (<b>c</b>) and PffBT4T-2DT films (<b>d</b>), respectively.</p>
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<p>AFM height images (<b>a</b>,<b>b</b>) and phase images (<b>c</b>,<b>d</b>) of PffBT4T-2OD films (<b>a</b>,<b>c</b>) and PffBT4T-2DT films (<b>b</b>,<b>d</b>) in tapping mode.</p>
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<p>(<b>a</b>) Photograph illustration of stretching polymer films at the strain of 25%, 50%, and 100%. (<b>b</b>,<b>c</b>) OM images of the stretched PffBT4T-2OD films (<b>b</b>) and blended films (PffBT4T-2DT/SEBS = 7:3) (<b>c</b>) under various strains, where the white arrow denotes the strain direction.</p>
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<p>Typical transfer curves of the ion-gated OFETs based on pure PffBT4T-2OD films (<b>a</b>,<b>c</b>) and PffBT4T-2OD/SEBS (7:3) blend films (<b>b</b>,<b>d</b>) before tensile strain (<b>a</b>,<b>b</b>) and under the strain of 100% (<b>c</b>,<b>d</b>), respectively. The strain direction is parallel to the direction of channel current. The channel length (L) and channel width (W) are 200 μm and 2 mm, respectively.</p>
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28 pages, 4190 KiB  
Article
Know Your Grip: Real-Time Holding Posture Recognition for Smartphones
by Rene Hörschinger, Marc Kurz and Erik Sonnleitner
Electronics 2024, 13(23), 4596; https://doi.org/10.3390/electronics13234596 - 21 Nov 2024
Viewed by 453
Abstract
This paper introduces a model that predicts four common smartphone-holding postures, aiming to enhance user interface adaptability. It is unique in being completely independent of platform and hardware, utilizing the inertial measurement unit (IMU) for real-time posture detection based on sensor data collected [...] Read more.
This paper introduces a model that predicts four common smartphone-holding postures, aiming to enhance user interface adaptability. It is unique in being completely independent of platform and hardware, utilizing the inertial measurement unit (IMU) for real-time posture detection based on sensor data collected around tap gestures. The model identifies whether the user is holding and operating the smartphone with one hand or using both hands in different configurations. For model training and validation, sensor time series data undergo extensive feature extraction, including statistical, frequency, magnitude, and wavelet analyses. These features are incorporated into 74 distinct sets, tested across various machine learning frameworks—k-nearest neighbors (KNN), support vector machine (SVM), and random forest (RF)—and evaluated for their effectiveness using metrics such as cross-validation scores, test accuracy, Kappa statistics, confusion matrices, and ROC curves. The optimized model demonstrates a high degree of accuracy, successfully predicting the holding hand with a 95.7% success rate. This approach highlights the potential of leveraging sensor data to improve mobile user experiences by adapting interfaces to natural user interactions. Full article
(This article belongs to the Special Issue Applied Machine Learning in Intelligent Systems)
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<p>Thumb coverage during one-handed interaction with the right thumb, showing different holding postures [<a href="#B1-electronics-13-04596" class="html-bibr">1</a>].</p>
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<p>Defined holding postures used for the experiment, from left to right: left-single, left-double, right-double, and right-single [<a href="#B5-electronics-13-04596" class="html-bibr">5</a>].</p>
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<p>(<b>a</b>) Number of samples for each holding posture in the dataset. (<b>b</b>) Number of samples each user contributed to the final dataset.</p>
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<p>(<b>a</b>) Actual X and Y coordinates of all tap gestures in the dataset. (<b>b</b>) Number of samples per location (dataset split into nine different locations categorized by the labels displayed in the app).</p>
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<p>The whole dataset visualized and grouped by sensor axis, location, and holding posture, with a rolling median filter and a window size of 25.</p>
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<p>Flowchart explaining the different steps from an unmodified dataset up to the final model evaluation.</p>
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<p>Comparison of the raw time series data from the accelerometer’s <span class="html-italic">Z</span>-axis with the scaled time series data using a custom scaling implementation, as well as the scaled and filtered data.</p>
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<p>Comparison of the mean values of a time series (accelerometer <span class="html-italic">z</span>-axis) after being scaled with different scaling implementations.</p>
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<p>(<b>a</b>) Visualization of positive and negative skewness in time series data [<a href="#B13-electronics-13-04596" class="html-bibr">13</a>]. (<b>b</b>) Comparison between positive and negative kurtosis [<a href="#B14-electronics-13-04596" class="html-bibr">14</a>].</p>
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<p>Visualization of a filter bank structure used for extracting up to level-three coefficients by applying several high-pass (h[n]) and low-pass (g[n]) filters [<a href="#B21-electronics-13-04596" class="html-bibr">21</a>].</p>
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<p>Visualization of the approximation coefficients as well as the detailed coefficients for the accelerometer <span class="html-italic">x</span>-axis.</p>
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<p>Correlation matrix of all combined features (370).</p>
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<p>Correlation matrix of all combined features, but features with a correlation between each other that is greater than 0.9 or lower than <math display="inline"><semantics> <mrow> <mo>−</mo> <mn>0.9</mn> </mrow> </semantics></math> according to the Pearson correlation coefficient have been removed.</p>
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<p>Cumulative variance plotted in relation to the number of PCs used. (<b>a</b>) The total amount of PCs, accumulating in a variance of 1.0. (<b>b</b>,<b>c</b>) Using as many PCs as necessary to achieve a cumulative variance of 0.95 with 59 PCs and 0.9 with 38 PCs, respectively.</p>
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<p>Distribution of total samples per holding posture after combining the left-double and right-double postures into a single two-handed holding posture.</p>
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<p>Comparison of sensor data from a single axis (gyroscope <span class="html-italic">Y</span>-axis) at a specific location (middle of the touchscreen), grouped by holding posture and averaged across all samples. It includes (<b>a</b>) the raw data, (<b>b</b>) data trimmed by 0.1 s on both ends, and (<b>c</b>) data trimmed by 0.2 s on both ends to shorten the time series.</p>
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<p>Confusion matrix and ROC curves for three different models: The baseline model with raw time series scaled and filtered (<b>a</b>,<b>d</b>), the RF with wavelet features from the IMU (<b>b</b>,<b>e</b>), and the RF with all wavelet features and a 0.9 correlation filter (<b>c</b>,<b>f</b>). All models used the dataset with four holding postures.</p>
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<p>Confusion matrix and ROC curves for three different models: The SVM with combined features and a 0.8 correlation filter (<b>a</b>,<b>d</b>), the SVM with PCA features and a 0.9 correlation filter (<b>b</b>,<b>e</b>), and the RF with all wavelet features, a 0.9 correlation filter, and a 100 ms cutoff (<b>c</b>,<b>f</b>). All models used the dataset with three holding postures.</p>
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40 pages, 8690 KiB  
Review
Recent Advances and Remaining Challenges in Perovskite Solar Cell Components for Innovative Photovoltaics
by Pari Baraneedharan, Sankar Sekar, Silambarasan Murugesan, Djaloud Ahamada, Syed Ali Beer Mohamed, Youngmin Lee and Sejoon Lee
Nanomaterials 2024, 14(23), 1867; https://doi.org/10.3390/nano14231867 - 21 Nov 2024
Viewed by 938
Abstract
This article reviews the latest advancements in perovskite solar cell (PSC) components for innovative photovoltaic applications. Perovskite materials have emerged as promising candidates for next-generation solar cells due to their exceptional light-absorbing capabilities and facile fabrication processes. However, limitations in their stability, scalability, [...] Read more.
This article reviews the latest advancements in perovskite solar cell (PSC) components for innovative photovoltaic applications. Perovskite materials have emerged as promising candidates for next-generation solar cells due to their exceptional light-absorbing capabilities and facile fabrication processes. However, limitations in their stability, scalability, and efficiency have hindered their widespread adoption. This review systematically explores recent breakthroughs in PSC components, focusing on absorbed layer engineering, electron and hole transport layers, and interface materials. In particular, it discusses novel perovskite compositions, crystal structures, and manufacturing techniques that enhance stability and scalability. Additionally, the review evaluates strategies to improve charge carrier mobility, reduce recombination, and address environmental considerations. Emphasis is placed on scalable manufacturing methods suitable for large-scale integration into existing infrastructure. This comprehensive review thus provides researchers, engineers, and policymakers with the key information needed to motivate the further advancements required for the transformative integration of PSCs into global energy production. Full article
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<p>Cubic lattice of the perovskite crystal ABX<sub>3</sub>. Reproduced with permission [<a href="#B31-nanomaterials-14-01867" class="html-bibr">31</a>], Copyright (2021) by John Wiley and Sons.</p>
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<p>Evolution of PSCs: (<b>a</b>,<b>b</b>) energy levels of PSCs and (<b>c</b>–<b>h</b>) device structures of PSCs. Reprinted from [<a href="#B37-nanomaterials-14-01867" class="html-bibr">37</a>], Copyright (2019) by Frontiers Group.</p>
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<p>Chalcogenide perovskite lattice and chemical elements at sites A and B. Reproduced with permission [<a href="#B48-nanomaterials-14-01867" class="html-bibr">48</a>], Copyright (2019) by John Wiley and Sons.</p>
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<p>Passivation engineering: (<b>a</b>) reducing trap states to improve performance, (<b>b</b>) removal of hysteresis, (<b>c</b>) enhancing stability, and (<b>d</b>) photosensitive molecule-assisted passivation to inhibit undesired defect-assisted recombination. (<b>a</b>) Reprinted from [<a href="#B54-nanomaterials-14-01867" class="html-bibr">54</a>], Copyright (2021) by Elsevier’s Group. (<b>b</b>) Reproduced with permission [<a href="#B55-nanomaterials-14-01867" class="html-bibr">55</a>], Copyright (2019) by American Chemical Society. (<b>c</b>) Reprinted from [<a href="#B56-nanomaterials-14-01867" class="html-bibr">56</a>], Copyright (2021) by RSC Group. (<b>d</b>) Reproduced with permission [<a href="#B57-nanomaterials-14-01867" class="html-bibr">57</a>], Copyright (2023) by American Chemical Society.</p>
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<p>(<b>a</b>) Oxidation parameters for Spiro-OMeTAD-based PSCs. (<b>b</b>) Band structure and energy level of an inverted organic photovoltaic device that utilizes an HTL of PEDOT:PSS doped with V<sub>2</sub>O<sub>5</sub>. (<b>c</b>) Examples of PTAA used with a perovskite and the resulting efficiency. (<b>d</b>) Doped PTAA with improved charge transport properties and a lower trap density. (<b>a</b>) Reproduced with permission [<a href="#B94-nanomaterials-14-01867" class="html-bibr">94</a>], Copyright (2022) by American Chemical Society. (<b>b</b>) Reprinted [<a href="#B95-nanomaterials-14-01867" class="html-bibr">95</a>], Copyright (2021) by John Wiley and Sons. (<b>c</b>) Reproduced with permission [<a href="#B96-nanomaterials-14-01867" class="html-bibr">96</a>], Copyright (2014) by American Chemical Society. (<b>d</b>) Reproduced with permission [<a href="#B97-nanomaterials-14-01867" class="html-bibr">97</a>], Copyright (2022) by Springer Nature Group.</p>
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<p>(<b>a</b>) Cross-sectional SEM image of PSC with M-P3HT. (<b>b</b>) Steady-state PL spectra. (<b>c</b>) TRPL spectra. (<b>d</b>) J–V curves of champion devices based on P3HT, M-P3HT, and R-P3HT. (<b>e</b>) EQE spectra and integrated photocurrent curves of device with P3HT, M-P3HT, and R-P3HT. (<b>f</b>) Steady-state <span class="html-italic">PCE</span>. Reproduced with permission [<a href="#B109-nanomaterials-14-01867" class="html-bibr">109</a>], Copyright (2022) by Springer Nature Group.</p>
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<p>Potential approaches for the HTL to enhance PSC efficiency.</p>
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<p>(<b>a</b>) Device structure and relationship between current density and brightness with respect to applied bias (inset: EQE curves) and (<b>b</b>) high crystallinity, conductivity, and hole-extraction properties of a PSC with high <span class="html-italic">PCE</span> of 17.74% using low-temperature-processed Cu-doped NiO<sub>x</sub> [<a href="#B114-nanomaterials-14-01867" class="html-bibr">114</a>,<a href="#B116-nanomaterials-14-01867" class="html-bibr">116</a>]. (<b>a</b>) Reproduced with permission [<a href="#B114-nanomaterials-14-01867" class="html-bibr">114</a>], Copyright (2013) by John Wiley and Sons. (<b>b</b>) Reproduced with permission [<a href="#B116-nanomaterials-14-01867" class="html-bibr">116</a>], Copyright (2015) by John Wiley and Sons.</p>
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<p>(<b>a</b>) Current–voltage (J-V) characteristics and steady photocurrent characteristics of PSCs based on NiCo<sub>2</sub>O<sub>4</sub> tested under AM 1.5 G illumination with an intensity of 100 mW cm<sup>−2</sup>. (<b>b</b>) p-i-n and n-i-p configurations for use of metal oxides as CTLs for both electrons and holes, leading to a higher <span class="html-italic">PCE</span>. (<b>c</b>) Inverted PSCs with a <span class="html-italic">PCE</span> of 19.91%, 14.6% higher than the control device, demonstrating promise of interfacial layer carrier transport for high-performance PSCs and expanding PSC material options. (<b>d</b>) Schematic and cross-sectional FESEM image of a device containing V<sub>2</sub>O<sub>5</sub>. (<b>e</b>) Hybrid ETLs with Cr<sub>2</sub>O<sub>3</sub>@GP and Cr<sub>2</sub>O<sub>3</sub>@CNT with an improved <span class="html-italic">PCE</span> of 18.5% and 26.8% compared to a plane ETL. (<b>a</b>) Reproduced with permission [<a href="#B129-nanomaterials-14-01867" class="html-bibr">129</a>], Copyright (2018) by John Wiley and Sons. (<b>b</b>) Reproduced with permission [<a href="#B130-nanomaterials-14-01867" class="html-bibr">130</a>], Copyright (2021) by Elsevier’s Group. (<b>c</b>) Reproduced with permission [<a href="#B131-nanomaterials-14-01867" class="html-bibr">131</a>], Copyright (2023) by Elsevier’s Group. (<b>d</b>) Reproduced with permission [<a href="#B132-nanomaterials-14-01867" class="html-bibr">132</a>], Copyright (2019) by American Chemical Society. (<b>e</b>) Reprinted [<a href="#B133-nanomaterials-14-01867" class="html-bibr">133</a>], Copyright (2017) by Royal Society of Chemistry.</p>
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<p>Use of fullerenes in PSCs as an ETL. Reproduced with permission [<a href="#B148-nanomaterials-14-01867" class="html-bibr">148</a>], Copyright (2021) by Elsevier’s Group.</p>
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<p>(<b>a</b>) Relationship between current and voltage in a DSSC with acetonitrile and an ionic liquid as electrolyte. (<b>b</b>) Structure of an FTO/TiO<sub>2</sub> compact layer/TiO<sub>2</sub> NS layer/perovskite/Spiro-OMeTAD/Au device used for the fabrication of PSCs in ambient conditions. (<b>c</b>) High levels of SnC<sub>2</sub>O<sub>4</sub> were used to produce SnO<sub>2</sub> films with an improved <span class="html-italic">PCE</span> of 21.31%. (<b>a</b>) Reproduced with permission [<a href="#B149-nanomaterials-14-01867" class="html-bibr">149</a>], Copyright (2009) by Elsevier’s Group. (<b>b</b>) Reproduced with permission [<a href="#B150-nanomaterials-14-01867" class="html-bibr">150</a>], Copyright (2023) by Elsevier’s Group. (<b>c</b>) Reproduced with permission [<a href="#B152-nanomaterials-14-01867" class="html-bibr">152</a>], Copyright (2022) by Elsevier’s Group.</p>
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<p><span class="html-italic">PCE</span> of a ZnSe-modified PSC. Reproduced with permission [<a href="#B159-nanomaterials-14-01867" class="html-bibr">159</a>], Copyright (2019) by Elsevier’s Group.</p>
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<p>Development of counter electrodes for more efficient, stable, and financially feasible PSCs for solar energy market adoption.</p>
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<p>Delocalized surface states in PSCs. Reproduced with permission [<a href="#B168-nanomaterials-14-01867" class="html-bibr">168</a>], Copyright (2019) by Elsevier’s Group.</p>
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<p>Key strategies used to enhance the stability of PSCs.</p>
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<p>Potential directions for PSC systems.</p>
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14 pages, 4501 KiB  
Article
Moisture Distribution and Ice Front Identification in Freezing Soil Using an Optimized Circular Capacitance Sensor
by Xing Hu, Qiao Dong, Bin Shi, Kang Yao, Xueqin Chen and Xin Yuan
Sensors 2024, 24(22), 7392; https://doi.org/10.3390/s24227392 - 20 Nov 2024
Viewed by 402
Abstract
As the interface between frozen and unfrozen soil, the ice front is not only a spatial location concept, but also a potentially dangerous interface where the mechanical properties of soil could change abruptly. Accurately identifying its spatial position is essential for the safe [...] Read more.
As the interface between frozen and unfrozen soil, the ice front is not only a spatial location concept, but also a potentially dangerous interface where the mechanical properties of soil could change abruptly. Accurately identifying its spatial position is essential for the safe and efficient execution of large-scale frozen soil engineering projects. Electrical capacitance tomography (ECT) is a promising method for the visualization of frozen soil due to its non-invasive nature, low cast, and rapid response. This paper presents the design and optimization of a mobile circular capacitance sensor (MCCS). The MCCS was used to measure frozen soil samples along the depth direction to obtain moisture distribution and three-dimensional images of the ice front. Finally, the experimental results were compared with the simulation results from COMSOL Multiphysics to analyze the deviations. It was found that the fuzzy optimization design based on multi-criteria orthogonal experiments makes the MCCS meet various performance requirements. The average permittivity distribution was proposed to reflect moisture distribution along the depth direction and showed good correlation. Three-dimensional reconstructed images could provide the precise position of the ice front. The simulation results indicate that the MCCS has a low deviation margin in identifying the position of the ice front. Full article
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<p>Schematic diagram of ECT’s forward and inverse problems [<a href="#B17-sensors-24-07392" class="html-bibr">17</a>].</p>
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<p>Compaction curve of loess.</p>
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<p>The diagram of the testing procedure.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>s</mi> </mrow> </msub> </mrow> </semantics></math> and moisture content variation in different specimens: (<b>a</b>) 10% initial moisture content; (<b>b</b>) 15% initial moisture content; (<b>c</b>) 20% initial moisture content.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> and moisture content variation in different specimens: (<b>a</b>) 10% initial moisture content; (<b>b</b>) 15% initial moisture content; (<b>c</b>) 20% initial moisture content.</p>
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<p>Ice fronts of different specimens: (<b>a</b>) 10% initial moisture content; (<b>b</b>) 15% initial moisture content; (<b>c</b>) 20% initial moisture content.</p>
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<p>2D image of the relative permittivity distribution at different specimen heights with 10% initial moisture content.</p>
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<p>Three-dimensional interpolated cloud plot of relative permittivity: (<b>a</b>) 10% initial moisture content; (<b>b</b>) 15% initial moisture content; (<b>c</b>) 20% initial moisture content.</p>
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<p>Simulation results of temperature field after 24 h of freezing: (<b>a</b>) 10% initial moisture content; (<b>b</b>) 15% initial moisture content; (<b>c</b>) 20% initial moisture content.</p>
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<p>Normalized simulation results of moisture content compared with measured <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> after 24 h of freezing: (<b>a</b>) 10% initial moisture content; (<b>b</b>) 15% initial moisture content; (<b>c</b>) 20% initial moisture content.</p>
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24 pages, 12729 KiB  
Article
Experimental Investigation on the Permeability and Fine Particle Migration of Debris-Flow Deposits with Discontinuous Gradation: Implications for the Sustainable Development of Debris-Flow Fans in Jiangjia Ravine, China
by Pu Li, Kaiheng Hu and Jie Yu
Sustainability 2024, 16(22), 10066; https://doi.org/10.3390/su162210066 - 19 Nov 2024
Viewed by 518
Abstract
The particle size distribution (PSD) is a crucial parameter used to characterize the material composition of debris-flow deposits which determines their hydraulic permeability, affecting the mobility of debris flows and, hence, the sustainable development of debris-flow fans. Three types of graded bedding structures—normal, [...] Read more.
The particle size distribution (PSD) is a crucial parameter used to characterize the material composition of debris-flow deposits which determines their hydraulic permeability, affecting the mobility of debris flows and, hence, the sustainable development of debris-flow fans. Three types of graded bedding structures—normal, reverse, and mixed graded bedding structures—are characterized by discontinuous gradation within a specific deposit thickness. A series of permeability tests were conducted to study the effects of bed sediment composition, particularly coarse grain sizes and fine particle contents, on the permeability and migration of fine particles in discontinuous debris-flow deposits. An increase in fine particles within the discontinuously graded bed sediment led to a power-law decrease in the average permeability coefficient. With fine particle contents of 10% and 15% in the bed sediments, the final permeability coefficient consistently exceeded the initial value. However, this trend reversed when the fine particle contents were increased to 20%, 25%, and 30%. Lower fine particle contents indicated enhanced permeability efficiency due to more interconnected voids within the coarse particle skeleton. Conversely, an increase in fine particle content reduced the permeability efficiency, as fine particles tended to aggregate at the lower section of the seepage channel. An increase in coarse particle size decreased the formation of flow channels at the coarse–fine particle interface, causing fine particles to move slowly along adjacent or clustered slow flow channels formed by fine particles, resulting in decreased permeability efficiency. Three formulae are proposed to calculate the permeability coefficients of discontinuously graded bed sediments, which may aid in understanding the initiation mechanism of channel deposits. Based on experimental studies and field investigations, it is proposed that achieving sustainable development of debris-flow fans requires a practical approach that integrates three key components: spatial land-use planning, in situ monitoring of debris flows and the environment, and land-use adjustment and management. This comprehensive and integrated approach is essential for effectively managing and mitigating the risks associated with debris flows, ensuring sustainable development in vulnerable areas. Full article
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<p>(<b>a</b>) Three gradings of bedding structures within debris-flow deposits: normal, reverse, and mixed gradation. (<b>b</b>) Reverse grading bedding structure observed in Jiangjia Ravine, China. (<b>c</b>) Particle size distribution curves of debris-flow deposits with reverse and mixed gradation. The green dotted rectangle denotes a horizontal segment in the middle of the curves.</p>
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<p>(<b>a</b>) Photograph of the experimental apparatus. (<b>b</b>) Diagram of the constant-head permeability test.</p>
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<p>Particle size distribution of continuous grading bed sediment with a natural PSD in Jiangjia Ravine, China.</p>
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<p>Grain size distribution of the bed sediments with different fine particle contents: (<b>a</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 10%; (<b>b</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 15%; (<b>c</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 20%; (<b>d</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 25%; (<b>e</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 30%. The continuous bed sediments with a fixed coarse grain size (<math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>c</mi> </msub> </mrow> </semantics></math> = 2–25) but different fine particle contents are denoted by corresponding test IDs with suffix asterisks.</p>
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<p>Permeability coefficients of discontinuous and discontinuous gradation debris-flow deposits with varying coarse particle size distributions and fine particle contents: (<b>a</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 10%; (<b>b</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 15%; (<b>c</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 20%; (<b>d</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 25%; (<b>e</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 30%. The continuous bed sediments with a fixed coarse grain size (<math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>c</mi> </msub> </mrow> </semantics></math> = 2–25) but different fine particle contents are denoted by corresponding test IDs with suffix asterisks.</p>
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<p>Relationships between coarse particle sizes and average permeability coefficients of discontinuous grading debris-flow deposits.</p>
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<p>Relationships between fine particle content and average permeability coefficients of discontinuous grading debris-flow deposits.</p>
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<p>Variation trend in the permeability coefficients of discontinuous grading bed sediments with different compositions: (<b>a</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 10%; (<b>b</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 15%; (<b>c</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 20%; (<b>d</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 25%; (<b>e</b>) <math display="inline"><semantics> <mi>P</mi> </semantics></math> = 30%.</p>
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<p>Changes in fine particle contents in experimental bed sediments with discontinuous gradation before and after the experiment: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>c</mi> </msub> </mrow> </semantics></math> = 2–5 mm; (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>c</mi> </msub> </mrow> </semantics></math> = 5–10 mm; (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>c</mi> </msub> </mrow> </semantics></math> = 10–15 mm; (<b>d</b>) <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>c</mi> </msub> </mrow> </semantics></math> = 15–20 mm; (<b>e</b>) <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mi>c</mi> </msub> </mrow> </semantics></math> = 20–25 mm. (<b>f</b>) A logarithmic relationship between the maximum fine particle content among four sampling areas and the kurtosis coefficient <math display="inline"><semantics> <mi>B</mi> </semantics></math>. The blue dotted lines denote the variations of post-test fine particle contents in areas a, b, c and d for different experimental conditions. The blue solid line signifies the fitted curve representing the relationship between the post-test peak fine particle content <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mi>p</mi> <mi>e</mi> <mi>a</mi> <mi>k</mi> </mrow> </msub> </mrow> </semantics></math> and the Kurtosis coefficient <math display="inline"><semantics> <mi>B</mi> </semantics></math>.</p>
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<p>Schematic diagram of the underlying mechanism that governs the temporal variations in permeability coefficients with (<b>a</b>,<b>b</b>) high and (<b>c</b>,<b>d</b>) low fine particle contents within discontinuous grading bed sediments. The large yellow irregular gravels with black edges depict the coarse grains, and the small yellow irregular sands without edges depict the fine particles. The red solid lines indicate connective seepage pathways, and the dashed black box denotes the aggregated fine particles. The downward blue arrows denote the seepage flows.</p>
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<p>Schematic diagram of the underlying mechanism that governs the temporal variations in permeability coefficients with (<b>a</b>,<b>b</b>) small, (<b>c</b>,<b>d</b>) medium, and (<b>e</b>,<b>f</b>) large coarse grain sizes within discontinuous grading bed sediments. The yellow solid lines denote the slow seepage channels shaped by adjacent or clustered fine particles. Other markings are the same as in <a href="#sustainability-16-10066-f010" class="html-fig">Figure 10</a>.</p>
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<p>Relationship between the measured and calculated permeability coefficients for discontinuous grading debris-flow deposits with varying fine particle contents and kurtosis coefficients: average permeability coefficients during (<b>a</b>) the entire experiment (<math display="inline"><semantics> <mi>k</mi> </semantics></math>), (<b>b</b>) the initial stage of infiltration (<math display="inline"><semantics> <mrow> <msub> <mi>k</mi> <mrow> <mi>i</mi> <mi>n</mi> <mi>i</mi> <mo>−</mo> <mn>9</mn> </mrow> </msub> </mrow> </semantics></math>), and (<b>c</b>) the final stage of infiltration (<math display="inline"><semantics> <mrow> <msub> <mi>k</mi> <mrow> <mi>f</mi> <mi>i</mi> <mi>n</mi> <mo>−</mo> <mn>9</mn> </mrow> </msub> </mrow> </semantics></math>).</p>
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<p>A schematic depicting the location and background of the Jiangjia Ravine.</p>
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<p>(<b>a</b>) A Google Earth satellite image (taken on 5 February 2022) showing the Jiangjia Ravine in Yunnan Province, China. (<b>b</b>–<b>f</b>) Several satellite images showing the locations of human activities on debris-flow fans.</p>
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<p>Schematic diagram of a practical approach to achieve the sustainable development of debris-flow fans.</p>
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10 pages, 3587 KiB  
Proceeding Paper
On the Performance Comparison of Fuzzy-Based Obstacle Avoidance Algorithms for Mobile Robots
by José Zúñiga, William Chamorro, Jorge Medina, Pablo Proaño, Renato Díaz and César Chillán
Eng. Proc. 2024, 77(1), 23; https://doi.org/10.3390/engproc2024077023 - 18 Nov 2024
Viewed by 288
Abstract
One of the critical challenges in mobile robotics is obstacle avoidance, ensuring safe navigation in dynamic environments. In this sense, this work presents a comparative study of two intelligent control approaches for mobile robot obstacle avoidance based on a fuzzy architecture. The first [...] Read more.
One of the critical challenges in mobile robotics is obstacle avoidance, ensuring safe navigation in dynamic environments. In this sense, this work presents a comparative study of two intelligent control approaches for mobile robot obstacle avoidance based on a fuzzy architecture. The first approach is a neuro-fuzzy interface that combines neural networks’ learning capabilities with fuzzy logic’s rule-based reasoning, offering a flexible and adaptable control strategy. The second is a classic Mamdani fuzzy system that relies on human-defined fuzzy rules, providing an intuitive approach to control. A key contribution of this work is the development of a fast comprehensive, model-based dataset for neural network training generated without the need for real sensor data. The results show the evaluation of these two systems’ performance, robustness, and computational efficiency using low-cost ultrasonic sensors on a Pioneer 3DX robot within the Coppelia Sim environment. Full article
(This article belongs to the Proceedings of The XXXII Conference on Electrical and Electronic Engineering)
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Figure 1

Figure 1
<p>Fuzzy systems architecture: (<b>a</b>) Sugeno membership functions. (<b>b</b>) Neuro-fuzzy membership functions. (<b>c</b>) Sugeno clustering architecture. (<b>d</b>) Mandami architecture. (<b>e</b>) Neuro-Fuzzy architecture. (<b>f</b>) Mandami input membership functions. (<b>g</b>) Mandami output membership functions.</p>
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<p>Tools for the dataset generation: (<b>a</b>) Robot geometry. (<b>b</b>) Avoidance rules visualization.</p>
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<p>Training data distributions.</p>
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<p>ANFIS training results: (<b>a</b>) Correlation Matrix. (<b>b</b>) Training error.</p>
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<p>Experiments in scenario A: (<b>a</b>) ANFIS performance. (<b>b</b>) Mandami performance.</p>
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<p>Experiments in scenario B: (<b>a</b>) ANFIS performance; (<b>b</b>) Mandami performance.</p>
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<p>Velocity and Acceleration performance results: (<b>a</b>) Mandami; (<b>b</b>) ANFIS.</p>
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