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Search Results (2,860)

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19 pages, 11059 KiB  
Article
VividWav2Lip: High-Fidelity Facial Animation Generation Based on Speech-Driven Lip Synchronization
by Li Liu, Jinhui Wang, Shijuan Chen and Zongmei Li
Electronics 2024, 13(18), 3657; https://doi.org/10.3390/electronics13183657 (registering DOI) - 14 Sep 2024
Viewed by 250
Abstract
Speech-driven lip synchronization is a crucial technology for generating realistic facial animations, with broad application prospects in virtual reality, education, training, and other fields. However, existing methods still face challenges in generating high-fidelity facial animations, particularly in addressing lip jitter and facial motion [...] Read more.
Speech-driven lip synchronization is a crucial technology for generating realistic facial animations, with broad application prospects in virtual reality, education, training, and other fields. However, existing methods still face challenges in generating high-fidelity facial animations, particularly in addressing lip jitter and facial motion instability issues in continuous frame sequences. This study presents VividWav2Lip, an improved speech-driven lip synchronization model. Our model incorporates three key innovations: a cross-attention mechanism for enhanced audio-visual feature fusion, an optimized network structure with Squeeze-and-Excitation (SE) residual blocks, and the integration of the CodeFormer facial restoration network for post-processing. Extensive experiments were conducted on a diverse dataset comprising multiple languages and facial types. Quantitative evaluations demonstrate that VividWav2Lip outperforms the baseline Wav2Lip model by 5% in lip sync accuracy and image generation quality, with even more significant improvements over other mainstream methods. In subjective assessments, 85% of participants perceived VividWav2Lip-generated animations as more realistic compared to those produced by existing techniques. Additional experiments reveal our model’s robust cross-lingual performance, maintaining consistent quality even for languages not included in the training set. This study not only advances the theoretical foundations of audio-driven lip synchronization but also offers a practical solution for high-fidelity, multilingual dynamic face generation, with potential applications spanning virtual assistants, video dubbing, and personalized content creation. Full article
(This article belongs to the Section Artificial Intelligence)
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<p>Speech-driven facial animation generation illustration.</p>
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<p>Partial dataset sample illustration.</p>
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<p>The architecture of VividWav2Lip. The network architecture primarily consists of three core components: Generator, Pre-trained Lip-Sync Expert and Facial Restoration module. The Generator encompasses four key elements: Facial Encoder, Audio Encoder, our proposed Cross Attention mechanism module and Additional Residual Blocks.</p>
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<p>Cross-Attention mechanism architecture diagram.</p>
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<p>SE residual mechanism architecture diagram.</p>
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<p>Training loss curve diagram.</p>
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<p>Performance comparison across leading lip synchronization approaches. The first four terms in the ‘Audio’ row are text in Chinese used for driven the model.</p>
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<p>Subjective evaluation results across four different tasks.</p>
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<p>Qualitative analysis. The Wav2Lip model suffers from jitter issues, which VividWav2Lip effectively addresses. The incorporation of a facial restoration network further enhances the output, resulting in high-fidelity images. The arrows and boxes indicate the lip regions of interest.</p>
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26 pages, 7340 KiB  
Article
Versatile Video Coding-Post Processing Feature Fusion: A Post-Processing Convolutional Neural Network with Progressive Feature Fusion for Efficient Video Enhancement
by Tanni Das, Xilong Liang and Kiho Choi
Appl. Sci. 2024, 14(18), 8276; https://doi.org/10.3390/app14188276 - 13 Sep 2024
Viewed by 356
Abstract
Advanced video codecs such as High Efficiency Video Coding/H.265 (HEVC) and Versatile Video Coding/H.266 (VVC) are vital for streaming high-quality online video content, as they compress and transmit data efficiently. However, these codecs can occasionally degrade video quality by adding undesirable artifacts such [...] Read more.
Advanced video codecs such as High Efficiency Video Coding/H.265 (HEVC) and Versatile Video Coding/H.266 (VVC) are vital for streaming high-quality online video content, as they compress and transmit data efficiently. However, these codecs can occasionally degrade video quality by adding undesirable artifacts such as blockiness, blurriness, and ringing, which can detract from the viewer’s experience. To ensure a seamless and engaging video experience, it is essential to remove these artifacts, which improves viewer comfort and engagement. In this paper, we propose a deep feature fusion based convolutional neural network (CNN) architecture (VVC-PPFF) for post-processing approach to further enhance the performance of VVC. The proposed network, VVC-PPFF, harnesses the power of CNNs to enhance decoded frames, significantly improving the coding efficiency of the state-of-the-art VVC video coding standard. By combining deep features from early and later convolution layers, the network learns to extract both low-level and high-level features, resulting in more generalized outputs that adapt to different quantization parameter (QP) values. The proposed VVC-PPFF network achieves outstanding performance, with Bjøntegaard Delta Rate (BD-Rate) improvements of 5.81% and 6.98% for luma components in random access (RA) and low-delay (LD) configurations, respectively, while also boosting peak signal-to-noise ratio (PSNR). Full article
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<p>Enhancing video quality with CNN based post-processing in conventional VVC coding workflow.</p>
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<p>MP4 to YUV conversion and reconstruction using VVenC and VVdeC.</p>
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<p>Illustration of video-to-image conversion process: (<b>a</b>) original videos converted to original images using FFmpeg, and (<b>b</b>) reconstructed videos converted to reconstructed images using FFmpeg.</p>
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<p>Illustration of the conversion process from YUV 4:2:0 format to YUV 4:4:4 format before feeding data into the deep learning network.</p>
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<p>Illustration of down-sampling process of neural network output from YUV 4:4:4 to YUV 4:2:0 format.</p>
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<p>Architecture of the proposed CNN-based post-filtering method, integrating multiple feature extractions for enhanced output refinement.</p>
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<p>Comparative visualization of (<b>b</b>) reconstructed frames from anchor VVC and (<b>c</b>) proposed methods for DaylightRoad2 sequence at QP 42 for RA configuration, alongside the (<b>a</b>) original uncompressed reference frame.</p>
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<p>Comparative visualization of (<b>b</b>) reconstructed frames from anchor VVC and (<b>c</b>) proposed methods for FourPeople sequence at QP 42 for LD configuration, alongside the (<b>a</b>) original uncompressed reference frame.</p>
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<p>RD curve performance comparison for five different test sequences in RA configuration.</p>
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<p>RD curve performance comparison for four different test sequences in LD configuration.</p>
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<p>Visual quality comparison of proposed method with 8 feature extraction blocks for RA and LD scenarios at QP 42: (<b>a</b>) MarketPlace Sequence and (<b>b</b>) PartyScene Sequence.</p>
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<p>Visual quality comparison of proposed method with 12 feature extraction blocks for RA and LD scenarios at QP 42: (<b>a</b>) RitualDance Sequence and (<b>b</b>) Cactus Sequence.</p>
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27 pages, 6340 KiB  
Article
Design and Evaluation of Real-Time Data Storage and Signal Processing in a Long-Range Distributed Acoustic Sensing (DAS) Using Cloud-Based Services
by Abdusomad Nur and Yonas Muanenda
Sensors 2024, 24(18), 5948; https://doi.org/10.3390/s24185948 - 13 Sep 2024
Viewed by 279
Abstract
In cloud-based Distributed Acoustic Sensing (DAS) sensor data management, we are confronted with two primary challenges. First, the development of efficient storage mechanisms capable of handling the enormous volume of data generated by these sensors poses a challenge. To solve this issue, we [...] Read more.
In cloud-based Distributed Acoustic Sensing (DAS) sensor data management, we are confronted with two primary challenges. First, the development of efficient storage mechanisms capable of handling the enormous volume of data generated by these sensors poses a challenge. To solve this issue, we propose a method to address the issue of handling the large amount of data involved in DAS by designing and implementing a pipeline system to efficiently send the big data to DynamoDB in order to fully use the low latency of the DynamoDB data storage system for a benchmark DAS scheme for performing continuous monitoring over a 100 km range at a meter-scale spatial resolution. We employ the DynamoDB functionality of Amazon Web Services (AWS), which allows highly expandable storage capacity with latency of access of a few tens of milliseconds. The different stages of DAS data handling are performed in a pipeline, and the scheme is optimized for high overall throughput with reduced latency suitable for concurrent, real-time event extraction as well as the minimal storage of raw and intermediate data. In addition, the scalability of the DynamoDB-based data storage scheme is evaluated for linear and nonlinear variations of number of batches of access and a wide range of data sample sizes corresponding to sensing ranges of 1–110 km. The results show latencies of 40 ms per batch of access with low standard deviations of a few milliseconds, and latency per sample decreases for increasing the sample size, paving the way toward the development of scalable, cloud-based data storage services integrating additional post-processing for more precise feature extraction. The technique greatly simplifies DAS data handling in key application areas requiring continuous, large-scale measurement schemes. In addition, the processing of raw traces in a long-distance DAS for real-time monitoring requires the careful design of computational resources to guarantee requisite dynamic performance. Now, we will focus on the design of a system for the performance evaluation of cloud computing systems for diverse computations on DAS data. This system is aimed at unveiling valuable insights into performance metrics and operational efficiencies of computations on the data in the cloud, which will provide a deeper understanding of the system’s performance, identify potential bottlenecks, and suggest areas for improvement. To achieve this, we employ the CloudSim framework. The analysis reveals that the virtual machine (VM) performance decreases significantly the processing time with more capable VMs, influenced by Processing Elements (PEs) and Million Instructions Per Second (MIPS). The results also reflect that, although a larger number of computations is required as the fiber length increases, with the subsequent increase in processing time, the overall speed of computation is still suitable for continuous real-time monitoring. We also see that VMs with lower performance in terms of processing speed and number of CPUs have more inconsistent processing times compared to those with higher performance, while not incurring significantly higher prices. Additionally, the impact of VM parameters on computation time is explored, highlighting the importance of resource optimization in the DAS system design for efficient performance. The study also observes a notable trend in processing time, showing a significant decrease for every additional 50,000 columns processed as the length of the fiber increases. This finding underscores the efficiency gains achieved with larger computational loads, indicating improved system performance and capacity utilization as the DAS system processes more extensive datasets. Full article
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<p>Experimental setup of a distributed vibration sensor using a <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math>-OTDR scheme in direct detection [<a href="#B8-sensors-24-05948" class="html-bibr">8</a>].</p>
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<p>Intrusion detection using a <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math>-OTDR sensor [<a href="#B16-sensors-24-05948" class="html-bibr">16</a>].</p>
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<p>Block diagram of the developed system.</p>
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<p>Schematic representation of the connection of the DAS sensor system to DynamoDB.</p>
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<p>Steps to use CloudSim.</p>
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<p>Block diagram of simulation flow for the basic scenario.</p>
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<p>Schematic representation of the implementation of processing of DAS data in CloudSim.</p>
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<p>Latency per batch of DynamoDB access for sample number of batches used to write trace samples.</p>
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<p>Latency per batch of DynamoDB access used to write trace samples with number of batches scaling with <math display="inline"><semantics> <msup> <mn>2</mn> <mi>n</mi> </msup> </semantics></math> for each index n.</p>
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<p>(<b>a</b>) Total latency of DynamoDB access (<b>b</b>) Latency per sample for varying trace sample sizes in the range of 5000–550,000 samples corresponding to 1–110 km sensing distances.</p>
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<p>Analysis of processing time and cloudlet utilization for differential operations in DAS sensing system: a study on single cycle versus multiple cycles. The study focuses on two distinct scenarios: (<b>a</b>) a single cycle of measurement, and (<b>b</b>) a series of 10 consecutive cycles of measurement. The measurements are conducted in a 110 km long optical sensing fiber. Note that the number of cloudlets increases for each cloudlet ID in the horizontal axis.</p>
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<p>Processing time versus cloudlets for FFT operation for (<b>a</b>) a single cycle, and (<b>b</b>) 10 cycles, of measurement in a 110 km fiber. Note that the number of cloudlets increases for each cloudlet ID in the horizontal axis.</p>
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<p>Evaluation of the mean processing time for each virtual machine in differential operations: a comparative study on a single cycle versus multiple cycles in a 110 km optical fiber. The investigation is conducted under two distinct conditions: (<b>a</b>) a single cycle of measurement, and (<b>b</b>) a series of 10 consecutive cycles of measurement. The measurements are performed in a 110 km long optical fiber. This research aims to understand the computational efficiency of cloud services in DAS sensing systems.</p>
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<p>Mean processing time for each VM for FFT operation for (<b>a</b>) a single cycle, and (<b>b</b>) 10 cycles, of measurement in a 110 km fiber.</p>
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<p>Statistical analysis of processing time for virtual machines in differential operations: an examination of standard deviation and variance across single and multiple cycles in a 110 km optical fiber. The analysis is conducted under two different scenarios: (<b>a</b>) a single cycle of measurement, and (<b>b</b>) a sequence of 10 cycles of measurement. The measurements are carried out in a 110 km long optical fiber. This study provides a deeper understanding of the variability and consistency in the performance of VMs during differential operations in DAS sensing systems.</p>
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<p>Standard deviation and variance for vms based on processing time-for differential operation for (<b>a</b>) a single cycle, and (<b>b</b>) 10 cycles, of measurement in a 110 km fiber.</p>
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<p>Evaluation of processing time for incremental data in optical fiber measurements (for each additional 50,000 rows) during two distinct operations: (<b>a</b>) the differential operation, and (<b>b</b>) the Fast Fourier Transform (FFT) operation. The measurements are conducted in a 110 km long optical fiber. This examination aims to understand the computational scalability of these operations in the context of increasing data volume.</p>
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<p>Analysis of processing time and cloudlet utilization for differential operations in optical fiber measurements with a specific focus on two distinct scenarios: (<b>a</b>) varying only the Million Instructions Per Second (MIPS) of the virtual machines (VMs), and (<b>b</b>) varying only the Processing Elements (PE) of the VMs. The measurements are conducted during a single cycle in a 110 km long optical fiber. This study aims to understand the influence of MIPS and PE variations on the performance and efficiency of VMs during differential operations in DAS sensing systems.</p>
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<p>Processing time versus cloudlets for differential operation for (<b>a</b>) varying only the MIPS of the VMs, and (<b>b</b>) varying only the PE of the VMs, for a 10 cycle of measurements in a 110 km fiber.</p>
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<p>Processing time versus cost for (<b>a</b>) differential, and (<b>b</b>) FFT operation for 10 cycles of measurement in a 110 km fiber.</p>
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<p>Cost of processing versus cloudlets for differential operation for (<b>a</b>) a single cycle, and (<b>b</b>) 10 cycles, of measurement in a 110 km fiber.</p>
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<p>Cost of processing versus cloudlets for FFT operation for (<b>a</b>) a single cycle, and (<b>b</b>) 10 cycles, of measurement in a 110 km fiber.</p>
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20 pages, 4413 KiB  
Article
Design and Manufacturing of Dielectric Resonators via 3D Printing of Composite Polymer/Ceramic Filaments
by Paris Sofokleous, Eva Paz and Francisco Javier Herraiz-Martínez
Polymers 2024, 16(18), 2589; https://doi.org/10.3390/polym16182589 - 13 Sep 2024
Viewed by 378
Abstract
Rapid technological advancements in recent years have opened the door to innovative solutions in the field of telecommunications and wireless systems; thus, new materials and manufacturing methods have been explored to satisfy this demand. This paper aims to explore the application of low-cost, [...] Read more.
Rapid technological advancements in recent years have opened the door to innovative solutions in the field of telecommunications and wireless systems; thus, new materials and manufacturing methods have been explored to satisfy this demand. This paper aims to explore the application of low-cost, commercially available 3D-printed ceramic/polymer composite filaments to design dielectric resonators (DRs) and check their suitability for use in high-frequency applications. Three-dimensional printing was used to fabricate the three-dimensional dielectric resonant prototypes. The filaments were characterized in terms of their thermal and mechanical properties and quality of printability. Additionally, the filaments’ dielectric properties were analyzed, and the prototypes were designed and simulated for a target frequency of ~2.45 GHz. Afterward, the DRs were successfully manufactured using the 3D printing technique, and no post-processing techniques were used in this study. A simple and efficient feeding method was used to finalize the devices, while the printed DRs’ reflection coefficient (S11) was measured. Results on prototype size, manufacture ease, printability, cost per volume, and bandwidth (BW) were used to evaluate the materials’ suitability for high-frequency applications. This research presents an easy and low-cost manufacturing process for DRs, opening a wide range of new applications and revolutionizing the manufacturing of 3D-printed high-frequency devices. Full article
(This article belongs to the Section Polymer Processing and Engineering)
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<p>DR prototypes: (<b>a</b>) side view; (<b>b</b>) top view. DR’s radius (r<sub>DR</sub>); DR’s height (h<sub>DR</sub>); ground plane’s length (l<sub>GP</sub>); ground plane’s height (h<sub>GP</sub>); feeding point distance (d<sub>fp</sub>); feed height (h<sub>f</sub>); coaxial radius (r<sub>c</sub>).</p>
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<p>DSC curves for (<b>a</b>) ABS, PLA, PLA50ZrO<sub>2</sub>, and PLA20HA; and (<b>b</b>) PO, PO30TiO, and PO40TiO.</p>
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<p>Stress–Strain curves for (<b>a</b>) ABS, PLA, PLA50ZrO<sub>2</sub>, and PLA20HA; and (<b>b</b>) PO, PO30TiO, and PO40TiO.</p>
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<p>Stress–Strain curves for (<b>a</b>) ABS, PLA, PLA50ZrO<sub>2</sub>, and PLA20HA; and (<b>b</b>) PO, PO30TiO, and PO40TiO.</p>
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<p>Top and side view images of 3D-printed bricks: PLA (<b>a</b>,<b>d</b>), PLA50ZrO<sub>2</sub> (<b>b</b>,<b>e</b>), and PLA20HA (<b>c</b>,<b>f</b>), respectively. Arrows indicate the most notable defects.</p>
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<p>Theoretical (simulation)–Experimental (VNA) resonant frequency of the prototypes.</p>
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<p>The 3D-printed prototypes. From top left to bottom right: PLA50ZrO<sub>2</sub>; PLA20HA; PO30TiO; PO40TiO; PLA; and ABS.</p>
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<p>Frequency response—Minimum of reflection coefficient (|S<sub>11</sub>|) between PLA50ZrO<sub>2</sub> and PLA prototypes.</p>
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<p>PLA50ZrO<sub>2</sub> prototype on the GP, fed by the coaxial connector.</p>
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<p>Simulated and measured frequency response and reflection coefficient (|S<sub>11</sub>|) of PLA50ZrO<sub>2</sub> prototype.</p>
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17 pages, 7100 KiB  
Article
Effects of Fuel Penetration on the RDE Performance with JISC Injector Configuration
by Gyeong-Ui Mo, In-Hoi Koo, Keon-Hyeong Lee, Su-Wan Choi and Jeong-Yeol Choi
Aerospace 2024, 11(9), 752; https://doi.org/10.3390/aerospace11090752 - 13 Sep 2024
Viewed by 192
Abstract
This study investigates the operational characteristics of the Rotating Detonation Engine (RDE), with a focus on fuel injector design. Inspired by the similarity between the fuel injection structure of RDE and the Jet in Supersonic Crossflow (JISC) of a scramjet, experimental research on [...] Read more.
This study investigates the operational characteristics of the Rotating Detonation Engine (RDE), with a focus on fuel injector design. Inspired by the similarity between the fuel injection structure of RDE and the Jet in Supersonic Crossflow (JISC) of a scramjet, experimental research on fuel injectors with jet penetration was conducted. Five injectors were designed, each with a fixed fuel injection area or injection hole diameter. Experiments determined practical injection areas, and an empirical correlation was used to calculate jet penetration heights. Under conditions of a total mass flow rate of 105 ± 5 g/s and an equivalence ratio of 1.05 ± 0.1, combustion modes were analyzed. Initial detonation occurrence was assessed through pressure history, with a detailed analysis via image post-processing. The results indicated that the injector D4N15, with the highest jet penetration height, exhibited deflagration, while D4N23 showed chaotic propagation. The injector D2N60 demonstrated relatively unstable behavior in sustained detonation cases. Thrust comparisons revealed that D4N30, with wider hole spacing and higher jet penetration height, exhibited approximately 12.5% higher specific impulse compared to D1N240. These outcomes confirm the significant impact of jet penetration height and hole spacing on detonation propagation and engine performance. Full article
(This article belongs to the Special Issue Aerospace Combustion Engineering (2nd Edition))
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<p>Schematics of experimental RDE model: (<b>a</b>) Schematic of annular RDE and instrumentation installation. (<b>b</b>) Schematic of propellant injection structure.</p>
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<p>Schematic of the pre-detonator installed tangentially to the RDE combustion channel.</p>
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<p>Five manufactured fuel injectors (part of center-body in RDE).</p>
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<p>Theoretical mass flow rate and experimental mass flow rate reflecting production error: (<b>a</b>) Mass flow rate of oxidizer and D4 fuel injectors. (<b>b</b>) D1N24 and D2N60 fuel injectors’ mass flow rate.</p>
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<p>Calculated jet penetration heights for the five manufactured injectors.</p>
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<p>Load cell calibration result.</p>
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<p>Experimental sequence of the RDE hot fire test: time sequence of each valve and ignition.</p>
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<p>Comparison of thrust and specific impulse results: (<b>a</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>m</mi> </mrow> <mo>˙</mo> </mover> </mrow> </semantics></math> = 107 g/s with <math display="inline"><semantics> <mrow> <mi>Φ</mi> <mo>=</mo> </mrow> </semantics></math> 1.01, (<b>b</b>) <math display="inline"><semantics> <mrow> <mover accent="true"> <mrow> <mi>m</mi> </mrow> <mo>˙</mo> </mover> </mrow> </semantics></math> = 160 ± 0.9 g/s with <math display="inline"><semantics> <mrow> <mi>Φ</mi> </mrow> </semantics></math> = 0.471 ± 0.005, and (<b>c</b>) various conditions.</p>
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<p>The history of thrust and pressure: (<b>a</b>) Exptl.03, D4N15 without back-pressure and (<b>b</b>) Exptl.05, D4N30 with back-pressure.</p>
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<p>High-speed-camera pictures and image-processing images for combustion-mode verification: (<b>a</b>) high-speed-camera snapshots and image-processing coordinate; (<b>b</b>) 2-wave detonation of Exptl.01, D1N240; (<b>c</b>) 3-wave detonation with counter-rotating of Exptl.02, D2N60; (<b>d</b>) deflagration with D4N15 of Exptl.03; (<b>e</b>) Exptl.04, chaotic propagation with D4N23 fuel injector; and (<b>f</b>) 3 detonation waves with D4N30 of Exptl.05.</p>
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<p>Detonation propagation analysis based on STFT and FFT results: (<b>a</b>) wave mode with D1N240 of Exptl.01, (<b>b</b>) relatively unstable propagation with D2N60, and (<b>c</b>) 3-wave mode with D4N30 of Exptl.06.</p>
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<p>Wall pressure of D4 fuel injectors.</p>
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<p>Combustion mode and specific impulse according to injector parameters.</p>
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10 pages, 2956 KiB  
Article
Preparation and Properties Study of CsPbX3@PMMA Luminescent Resin
by Xinqiang Ma, Shengying Fan, Wenwen Yang, Jiajie Wei, Xiaolei Wang, Jincheng Ni, Wei Cheng and Qinhe Zhang
Micromachines 2024, 15(9), 1150; https://doi.org/10.3390/mi15091150 - 13 Sep 2024
Viewed by 247
Abstract
Perovskite as an emerging semiconductor luminescent material has attracted widespread attention due to its simple preparation, high luminescence quantum yield, high color purity, tunable spectrum, and ability to cover the entire visible light band. However, due to the influence of water or other [...] Read more.
Perovskite as an emerging semiconductor luminescent material has attracted widespread attention due to its simple preparation, high luminescence quantum yield, high color purity, tunable spectrum, and ability to cover the entire visible light band. However, due to the influence of water or other highly polar solvents, oxygen, temperature, and radiation, perovskite nanocrystals will aggregate or collapse in the lattice, eventually leading to luminescence quenching. This study starts from the postprocessing of perovskite, uses methyl methacrylate as the monomer and TPO as the photoinitiator, and encapsulates the perovskite powder prepared by the hot injection method through ultraviolet light initiation. A method is proposed to improve the luminescence and crystal structure stability of perovskite. By eliminating the influence of environmental factors on perovskite nanocrystals through the dense structure formed by organic polymers, the resistance of perovskite to strong polar solvents such as water will be greatly improved, and it has great potential in the protection of perovskite. Finally, by changing the proportion of halogen elements in the perovskite resin to change the color of the luminescent resin, a fluorescent coating emitting light in all visible light bands is prepared. Fluorescent coatings are widely used in life and industry fields such as plastics, sol, and paper. Full article
(This article belongs to the Special Issue Optical and Laser Material Processing)
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<p>Structural characterization of CsPbBr<sub>3</sub>@PMMA: (<b>a</b>) Fourier transform infrared spectrum of perovskite in toluene solution and resin, (<b>b</b>) X−ray diffraction pattern of perovskite nanocrystals and perovskite resin (perovskite−PMMA bulk: black thin solid line (top), perovskite−PMMA powder: red thin solid line (middle), perovskite nanocrystal powder: black thick solid line (bottom)), (<b>c</b>) thermogravimetric analysis diagram of perovskite nanocrystals and perovskite resin.</p>
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<p>Photophysical properties of CsPbBr<sub>3</sub>@PMMA: (<b>a</b>) perovskite nanocrystals with different luminescence by changing halogen elements, (<b>b</b>) fluorescence spectra of CsPbX<sub>3</sub>–toluene solution, (<b>c</b>) fluorescence spectra of CsPbX<sub>3</sub>@PMMA resin, (<b>d</b>) perovskite luminescent resin under day light (upper) and ultraviolet light (lower), (<b>e</b>) ultraviolet absorption spectra of CsPbX<sub>3</sub>–toluene solution, (<b>f</b>) ultraviolet absorption spectra of CsPbX<sub>3</sub>@PMMA luminescent resin.</p>
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<p>Temperature response and stability test of CsPbX<sub>3</sub>@PMMA luminescent resin: (<b>a</b>–<b>g</b>) luminescence change diagrams of the effect of temperature on perovskite, (<b>a</b>) 30 °C, (<b>b</b>) 60 °C, (<b>c</b>) 90 °C, (<b>d</b>) 120 °C, (<b>e</b>) 150 °C, (<b>f</b>) 180 °C, (<b>g</b>) 210 °C; (<b>h</b>) luminescence diagram of perovskite resin under UV lamp irradiation upon return to room temperature after heating; (<b>i</b>) perovskite resin under day light; (<b>j</b>) perovskite resin under ultraviolet light in water (left) and ethanol (right) solutions; (<b>k</b>) perovskite resin under day light in water (left) and ethanol (right) solutions.</p>
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<p>Application of CsPbX<sub>3</sub>@PMMA luminescent resin: (<b>a</b>) schematic diagram of dissolution and recasting of perovskite luminescent resin, (<b>b</b>) mixing diagram of two different color luminescent resins, (<b>c</b>) fluorescence spectrum diagram of the two resins mixed in (<b>b</b>), (<b>d</b>) after the three resins are overlapped, a white light source is prepared using ultraviolet light as the excitation light.</p>
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12 pages, 7802 KiB  
Article
Influence of Printing Strategies on the Microstructure and Mechanical Properties of Additively Manufactured Alloy 625 Using Directed Energy Deposition (DED-LB-p)
by Florian Scherm, Haneen Daoud and Uwe Glatzel
Metals 2024, 14(9), 1041; https://doi.org/10.3390/met14091041 - 13 Sep 2024
Viewed by 196
Abstract
Directed energy deposition (DED-LB-p) is used for the production of large components due to the high deposition rates. The large number of process parameters and printing strategies makes it difficult to optimize this process to achieve the optimal properties. Intensive post-processing is still [...] Read more.
Directed energy deposition (DED-LB-p) is used for the production of large components due to the high deposition rates. The large number of process parameters and printing strategies makes it difficult to optimize this process to achieve the optimal properties. Intensive post-processing is still the main obstacle to the widespread use of this process. In this work, the influence of different printing strategies and process parameters on the microstructural and tensile mechanical performance at room temperature is investigated. The porosity is measured in both printing directions. The grain orientation and size are analyzed by EBSD. A very low porosity of less than 0.4% is found in all the printed samples. The samples printed with the optimized offset printing strategy show a significant improvement in tensile strength of 1000 MPa without heat treatment compared to the other processing routes. Full article
(This article belongs to the Special Issue Laser Processing Technology and Principles of Metal Materials)
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<p>Principle of directed energy deposition with powder as the feedstock material: (<b>a</b>) overview, and (<b>b</b>) detail.</p>
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<p>(<b>a</b>) SEM micrograph of Alloy625 powder, overview; (<b>b</b>) SEM micrograph of Alloy625 powder, spherical shaped particles with tiny satellites.</p>
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<p>(<b>a</b>) Robot and positioner; (<b>b</b>) coaxial three jet powder feeding nozzle; and (<b>c</b>) pneumatic powder feeder.</p>
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<p>(<b>a</b>) Light optical micrograph; and (<b>b</b>) corresponding binarized image.</p>
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<p>(<b>a</b>) Different scan strategies for the deposition of larger volume samples; and (<b>b</b>) optical micrograph of a cross-section from the offset unidirectional scan strategy.</p>
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<p>(<b>a</b>) Specimen geometry for the tensile tests; and (<b>b</b>) specimens after tensile test.</p>
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<p>Samples obtained within the parameter study: (<b>a</b>) laser power increases, (<b>b</b>) powder feed rate increases, and (<b>c</b>,<b>d</b>) scan speed increases while laser power and energy density, respectively, remain constant, standard parameter set marked with boxes.</p>
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<p>(<b>a</b>) SEM micrograph of Alloy625, overview, backscattered electron (BSE) detector; and (<b>b</b>) SEM micrograph of Alloy625, detail, dendritic microstructure (BSE).</p>
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<p>SEM BSE micrograph and corresponding element distribution of nickel, chromium, iron, niobium and molybdenum.</p>
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<p>Stress–strain curves for different scan strategies: (<b>a</b>–<b>c</b>) load normal to scan direction; and (<b>d</b>–<b>f</b>) load in scan direction, five samples for each scan strategy tested.</p>
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<p>Grain orientation maps obtained from samples deposited with different scan strategies: (<b>a</b>–<b>c</b>) normal to build direction, (<b>d</b>–<b>f</b>) in build direction (BD), blue arrow indicates load direction in tensile tests.</p>
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24 pages, 8434 KiB  
Article
Computational Modeling Approach to Profile Hemodynamical Behavior in a Healthy Aorta
by Ahmed M. Al-Jumaily, Mohammad Al-Rawi, Djelloul Belkacemi, Radu Andy Sascău, Cristian Stătescu, Florin-Emilian Țurcanu and Larisa Anghel
Bioengineering 2024, 11(9), 914; https://doi.org/10.3390/bioengineering11090914 - 12 Sep 2024
Viewed by 274
Abstract
Cardiovascular diseases (CVD) remain the leading cause of mortality among older adults. Early detection is critical as the prognosis for advanced-stage CVD is often poor. Consequently, non-invasive diagnostic tools that can assess hemodynamic function, particularly of the aorta, are essential. Computational fluid dynamics [...] Read more.
Cardiovascular diseases (CVD) remain the leading cause of mortality among older adults. Early detection is critical as the prognosis for advanced-stage CVD is often poor. Consequently, non-invasive diagnostic tools that can assess hemodynamic function, particularly of the aorta, are essential. Computational fluid dynamics (CFD) has emerged as a promising method for simulating cardiovascular dynamics efficiently and cost-effectively, using increasingly accessible computational resources. This study developed a CFD model to assess the aorta geometry using tetrahedral and polyhedral meshes. A healthy aorta was modeled with mesh sizes ranging from 0.2 to 1 mm. Key hemodynamic parameters, including blood pressure waveform, pressure difference, wall shear stress (WSS), and associated wall parameters like relative residence time (RRT), oscillatory shear index (OSI), and endothelial cell activation potential (ECAP) were evaluated. The performance of the CFD simulations, focusing on accuracy and processing time, was assessed to determine clinical viability. The CFD model demonstrated clinically acceptable results, achieving over 95% accuracy while reducing simulation time by up to 54%. The entire simulation process, from image construction to the post-processing of results, was completed in under 120 min. Both mesh types (tetrahedral and polyhedral) provided reliable outputs for hemodynamic analysis. This study provides a novel demonstration of the impact of mesh type in obtaining accurate hemodynamic data, quickly and efficiently, using CFD simulations for non-invasive aortic assessments. The method is particularly beneficial for routine check-ups, offering improved diagnostics for populations with limited healthcare access or higher cardiovascular disease risk. Full article
(This article belongs to the Section Biomechanics and Sports Medicine)
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<p>The current processes used for CFD simulation.</p>
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<p>(<b>a</b>) The aortic geometry showing the lateral and medial views with the boundary conditions and the computational domain; (<b>b</b>) the location of the points considered for investigation (adapted from [<a href="#B2-bioengineering-11-00914" class="html-bibr">2</a>]).</p>
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<p>The mesh for the inlet face shows the inflation used for (<b>a</b>) tetrahedral and (<b>b</b>) polyhedral meshes.</p>
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<p>(<b>a</b>) The systolic pressure values for the different meshes; (<b>b</b>) the diastolic pressure values for the different meshes.</p>
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<p>The computational fluid dynamics result was validated against the clinical data for the mesh element size of 0.2 mm for both polyhedral and tetrahedral meshes.</p>
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<p>The pressure waveforms at the aortic arch for the different meshes: (<b>a</b>) tetrahedral; (<b>b</b>) polyhedral; (<b>c</b>) the ΔP2 at the aortic arch, showing that the difference between the meshes is minimal; and (<b>d</b>) the normal central aortic pressure waveform.</p>
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<p>TAWSS for the different meshes to see the development of high contours for healthy aorta. (Tetrahedral = Tetra; polyhedral = Poly).</p>
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<p>The threshold values for the TAWSS for the different meshes (blue for values below the threshold of 5 Pa and red for values above 5 Pa) are used to visualize areas higher and lower than the threshold value. (Tetra = tetrahedral; Poly = polyhedral).</p>
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<p>The OSI for the different meshes to see the development of high contours for healthy aorta. (Tetrahedral = Tetra; polyhedral = Poly).</p>
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<p>The RRT for the different meshes to see the development of high contours for healthy aorta. (Tetrahedral = Tetra; polyhedral = Poly).</p>
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<p>The ECAP for the different meshes to see the development of high contours for healthy aorta. (Tetrahedral = Tetra; polyhedral = Poly).</p>
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<p>The TAWSS for the three-time steps (0.005, 0.001, and 0.0005 s) for 0.4 mm mesh element size: (<b>a</b>) polyhedral mesh; and (<b>b</b>) tetrahedral mesh.</p>
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<p>The OSI for the three-time steps (0.005, 0.001, and 0.0005 s) for 0.4 mm mesh element size: (<b>a</b>) polyhedral mesh; and (<b>b</b>) tetrahedral mesh.</p>
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<p>The RRT for the three-time steps (0.005, 0.001, and 0.0005 s) for 0.4 mm mesh element size: (<b>a</b>) polyhedral mesh; and (<b>b</b>) tetrahedral mesh.</p>
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<p>The ECAP for the three-time steps (0.005, 0.001, and 0.0005 s) for 0.4 mm mesh element size: (<b>a</b>) polyhedral mesh; and (<b>b</b>) tetrahedral mesh.</p>
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<p>The threshold values of OSI for the different meshes presented in this study illustrate the high and low mechanical shear oscillation WSS per cardiac cycle on the aortic wall. (Tetrahedral = Tetra; polyhedral = Poly).</p>
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<p>The threshold contours for the RRT for the different meshes illustrate the relative residence time based on the mechanical oscillation during a cardiac cycle and WSS values on the aortic wall. (Tetrahedral = Tetra; polyhedral = Poly).</p>
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<p>The threshold for the ECAP for the different meshes illustrates the degree of thrombogenic susceptibility of the endothelial cell to localize the possible location for high mechanical oscillation. (Tetrahedral = Tetra; polyhedral = Poly).</p>
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13 pages, 12554 KiB  
Article
Wettability Behaviour of Metal Surfaces after Sequential Nanosecond and Picosecond Laser Texturing
by Yin Tang, Zheng Fang, Yang Fei, Shuai Wang, Walter Perrie, Stuart Edwardson and Geoff Dearden
Micromachines 2024, 15(9), 1146; https://doi.org/10.3390/mi15091146 - 12 Sep 2024
Viewed by 344
Abstract
This study examines the wettability behaviour of 304 stainless steel (304SS) and Ti-6Al-4V (Ti64) surfaces after sequential nanosecond (ns) and picosecond (ps) laser texturing; in particular, how the multi-scale surface structures created influence the lifecycle of surface hydrophobicity. The effect of different post-process [...] Read more.
This study examines the wettability behaviour of 304 stainless steel (304SS) and Ti-6Al-4V (Ti64) surfaces after sequential nanosecond (ns) and picosecond (ps) laser texturing; in particular, how the multi-scale surface structures created influence the lifecycle of surface hydrophobicity. The effect of different post-process treatments is also examined. Surfaces were analysed using Scanning Electron Microscopy (SEM), a white light interferometer optical profiler, and Energy Dispersive X-ray (EDX) spectroscopy. Wettability was assessed through sessile drop contact angle (CA) measurements, conducted at regular intervals over periods of up to 12 months, while EDX scans monitored elemental chemical changes. The results show that sequential (ns + ps) laser processing produced multi-scale surface texture with laser-induced periodic surface structures (LIPSS). Compared to the ns laser case, the (ns + ps) laser processed surfaces transitioned more rapidly to a hydrophobic state and maintained this property for much longer, especially when the single post-process treatment was ultrasonic cleaning. Some interesting features in CA development over these extended timescales are revealed. For 304SS, hydrophobicity was reached in 1–2 days, with the CA then remaining in the range of 120 to 140° for up to 180 days; whereas the ns laser-processed surfaces took longer to reach hydrophobicity and only maintained the condition for up to 30 days. Similar results were found for the case of Ti64. The findings show that such multi-scale structured metal surfaces can offer relatively stable hydrophobic properties, the lifetime of which can be extended significantly through the appropriate selection of laser process parameters and post-process treatment. The addition of LIPSS appears to help extend the longevity of the hydrophobic property. In seeking to identify other factors influencing wettability, from our EDX results, we observed a significant and steady rate of increase in the carbon content at the surface over the study period. Full article
(This article belongs to the Special Issue Ultrafast Laser Micro- and Nanoprocessing, 2nd Edition)
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<p>Schematic of optical setup used for ps laser processing (Created with BioRender.com). The beam was attenuated by a λ/2 plate and a Glan-Laser Calcite Polarizer transmitting horizontal polarization. The beam passes through a diffraction-limited beam expander (Rodenstock; M = x3) and is then modulated by a reflective phase-only SLM and input to a galvo scanner after passing through a 4f optical system. An aperture allows the shaped zero-order light to pass through for laser processing.</p>
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<p>Schematic of the experimental process: laser process and surface property analysis methods (Created with BioRender.com). Four groups (1–4) of polished samples were processed with the ns laser to form the underlying micron-scale doubly periodic structure, while groups 3 and 4 were then also exposed to ps laser processing for LIPSS overlaying. For comparison, groups 1 and 3 were subjected to wettability tests twice a week, while groups 2 and 4 were measured for elemental concentration by EDX once a week. All samples were stored in ambient air during ageing.</p>
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<p>(Answer for question 2, reviewer 1). SEM images of ns laser processed 304SS and Ti64 surfaces. (<b>a</b>,<b>c</b>) are ×150 magnification, while (<b>b</b>,<b>d</b>) are ×1000 magnification.</p>
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<p>SEM image of LIPSS on 304SS and Ti64 surfaces: (<b>a</b>,<b>c</b>) ×1000 magnification and (<b>b</b>,<b>d</b>) ×5000 magnification.</p>
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<p>Surface topography 2D analyses, microscope images, and topography Fourier transform analyses of laser-textured functional surfaces before and after adding ps laser-generated LIPSS.</p>
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<p>Long-term wettability behaviour of ns laser ablated 304SS surfaces, for different post-process treatments: CA measured during the period up to 257 days after exposure.</p>
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<p>Wettability behaviour of ns laser processed Ti64 surfaces over a period of 141 days.</p>
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<p>Wettability behaviour of ns + ps laser processed 304SS and Ti64 surfaces over a period of 141 days.</p>
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<p>Comparison of time-dependent variation in carbon composition at the surface of samples processed by ns and (ns + ps) lasers, followed by ultrasonic cleaning: (<b>a</b>) 304SS and (<b>b</b>) Ti64.</p>
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<p>Comparison of time-dependent variation in oxygen composition at the surface of samples processed by ns and (ns + ps) lasers, followed by ultrasonic cleaning: (<b>a</b>) 304SS and (<b>b</b>) Ti64.</p>
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<p>EDX element-layered distribution map on ns (<b>a</b>) 304SS and (<b>d</b>) Ti64 and ns + ps (<b>b</b>) 304SS and (<b>e</b>) Ti64 laser processed surface structure ×500 magnification and (<b>c</b>) 304SS and (<b>f</b>) Ti64 ×1000 magnification Ns laser processed structure has obvious wider and stronger carbon absorption and oxidises around the peak of the structure compared to the ns + ps laser processed structure.</p>
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<p>SEM images of 304SS on (<b>a</b>) day 2 and (<b>b</b>) day 142. ns (<b>a-1</b>,<b>b-1</b>) and ns + ps (<b>a-2</b>,<b>b-2</b>) laser processed surface structure ×1000 magnification and (<b>a-3</b>,<b>b-3</b>) ×5000 magnification.</p>
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<p>SEM images of Ti64 on (<b>a</b>) day 2 and (<b>b</b>) day 142. ns (<b>a-1</b>,<b>b-1</b>) and ns + ps (<b>a-2</b>,<b>b-2</b>) laser-processed surface structure ×1000 magnification and (<b>a-3</b>,<b>b-3</b>) ×5000 magnification.</p>
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24 pages, 2183 KiB  
Review
A Comprehensive Review on Studying and Developing Guidelines to Standardize the Inspection of Properties and Production Methods for Mycelium-Bound Composites in Bio-Based Building Material Applications
by Worawoot Aiduang, Praween Jinanukul, Wandee Thamjaree, Tanongkiat Kiatsiriroat, Tanut Waroonkun and Saisamorn Lumyong
Biomimetics 2024, 9(9), 549; https://doi.org/10.3390/biomimetics9090549 - 11 Sep 2024
Viewed by 529
Abstract
Mycelium-bound composites (MBCs) represent a promising advancement in bio-based building materials, offering sustainable alternatives for engineering and construction applications. This review provides a comprehensive overview of the current research landscape, production methodologies, and standardization ideas related to MBCs. A basic search on Scopus [...] Read more.
Mycelium-bound composites (MBCs) represent a promising advancement in bio-based building materials, offering sustainable alternatives for engineering and construction applications. This review provides a comprehensive overview of the current research landscape, production methodologies, and standardization ideas related to MBCs. A basic search on Scopus revealed over 250 publications on MBCs between 2020 and 2024, with more than 30% focusing on engineering and materials science. Key studies have investigated the physical and mechanical properties of MBCs, optimizing parameters such as substrate type, fungal species, incubation time, and post-processing to enhance material performance. Standardizing the inspection of MBC properties is crucial for ensuring quality and reliability. Various testing standards, including those from the American Society for Testing and Materials (ASTM), the International Organization for Standardization (ISO), the Japanese Industrial Standard (JIS), European Standards (EN), Deutsches Institut für Normung (DIN), and the Thai Industrial Standards Institute (TIS), are utilized to evaluate density, water absorption, compression strength, tensile strength, insulation, and other critical properties. This review highlights the distinction between lab-scale and apply-scale testing methodologies, emphasizing the need for comprehensive evaluation protocols. Additionally, the production process of MBCs involves critical steps like substrate preparation, fungal species selection, and mycelium growth, necessitating the implementation of good manufacturing practices (GMPs) to ensure consistency and quality. The internal and external structures of MBCs significantly influence their performance, necessitating standardized inspection methods using advanced techniques such as scanning electron microscopy (SEM), X-ray computed tomography (CT) scanning, and surface profilometry. By establishing robust inspection protocols and production standards, the industry can enhance the reliability and adoption of MBCs, contributing to innovations in materials science and promoting environmental sustainability. This review underscores the importance of interdisciplinary collaboration, advanced characterization tools, and regulatory frameworks to address challenges and advance the field of MBCs. Full article
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<p>Subject-specific documents related to the engineering and materials science fields of MBC manufacturing. Created by Google SketchUp program version 8 for Windows.</p>
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<p>An overall biotechnological process is generally used to produce MBCs (modified from Elsacker et al. [<a href="#B25-biomimetics-09-00549" class="html-bibr">25</a>] and Almpani-Lekka et al. [<a href="#B60-biomimetics-09-00549" class="html-bibr">60</a>]). Created by Google SketchUp program version 8 for Windows.</p>
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<p>Recommendation on good manufacturing procedure (GMP) guidelines to standardize MBC production for applications involving bio-based building materials. Created by BioRender.com (<a href="https://www.biorender.com/" target="_blank">https://www.biorender.com/</a>; access date: 5 June 2024 [<a href="#B68-biomimetics-09-00549" class="html-bibr">68</a>]).</p>
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<p>Composite models of MBCs for applications in bio-based building materials, such as boards (<b>A</b>), bricks (<b>B</b>), and floor tiles (<b>C</b>).</p>
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25 pages, 14704 KiB  
Article
Improvement of Fatigue Strength in Additively Manufactured Aluminum Alloy AlSi10Mg via Submerged Laser Peening
by Hitoshi Soyama
Coatings 2024, 14(9), 1174; https://doi.org/10.3390/coatings14091174 - 11 Sep 2024
Viewed by 288
Abstract
As the fatigue properties of as-built components of additively manufactured (AM) metals are considerably weaker than those of wrought metals because of their rougher surface, post-processing is necessary to improve the fatigue properties. To demonstrate the improvement in the fatigue properties of AM [...] Read more.
As the fatigue properties of as-built components of additively manufactured (AM) metals are considerably weaker than those of wrought metals because of their rougher surface, post-processing is necessary to improve the fatigue properties. To demonstrate the improvement in the fatigue properties of AM metals via post-processing methods, the fabrication of AlSi10Mg, i.e., PBF–LS/AlSi10Mg, through powder bed fusion (PBF) using laser sintering (LS) and its treatment via submerged laser peening (SLP), using a fiber laser and/or a Nd/YAG laser, was evaluated via plane bending fatigue tests. In SLP, laser ablation (LA) is generated by a pulsed laser and a bubble is generated after LA, which behaves like a cavitation bubble that is referred to as “laser cavitation (LC)”. In this paper, LA-dominated SLP is referred to as “laser treatment (LT)”, while LC collapse-dominated SLP is referred to as “laser cavitation peening (LCP)”, as the impact of LC collapse is used for peening. It was revealed that SLP using a fiber laser corresponded with LT rather than LCP. It was demonstrated that the fatigue strength at N = 107 was 85 MPa for LCP and 103 MPa for the combined process of blasting (B) + LT + LCP, whereas the fatigue strength of the as-built specimen was 54 MPa. Full article
(This article belongs to the Special Issue Laser Surface Engineering: Technologies and Applications)
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<p>Typical aspects of submerged laser peening (SLP), showing laser ablation (LA), laser cavitation (LC), laser treatment (LT), and laser cavitation peening (LCP). These high-speed images are reprinted from [<a href="#B12-coatings-14-01174" class="html-bibr">12</a>], with permission from Elsevier, License Number 5824671356429.</p>
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<p>Geometry of plane bending fatigue specimen manufactured via PBF–LS/AlSi10Mg: (<b>a</b>) schematic of specimen (the thickness is 3 mm), (<b>b</b>) photograph of as-built specimen.</p>
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<p>Schematic of test section of SLP system and definition of standoff distance in air <span class="html-italic">s<sub>a</sub></span> and water <span class="html-italic">s<sub>w</sub></span>.</p>
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<p>Diagonal view of SLP system using a fiber laser.</p>
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<p>Diagonal view of SLP using a Nd/YAG laser.</p>
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<p>Photograph of XRD system and coordinates for residual stress measurement [<a href="#B11-coatings-14-01174" class="html-bibr">11</a>].</p>
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<p>Aspects of LA and LC and sound pressure changing over time after irradiated pulsed laser <span class="html-italic">t<sub>L</sub></span> induced by Nd/YAG laser with a wavelength <span class="html-italic">λ</span> = 1064 nm and a pulse width <span class="html-italic">t<sub>w</sub></span> = 6 ns: (<b>a</b>) aspects of LA and LC, (<b>b</b>) sound pressure <span class="html-italic">p<sub>s</sub></span>.</p>
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<p>Aspects of LA and LC and sound pressure changes over time after irradiated pulsed laser <span class="html-italic">t<sub>L</sub></span> induced by fiber laser with a wavelength <span class="html-italic">λ</span> = 1080 nm at pulse width <span class="html-italic">t<sub>w</sub></span> = 20 μs and 300 μs: (<b>a</b>) aspect of LA and LC at <span class="html-italic">t<sub>w</sub></span> = 20 μs; (<b>b</b>) sound pressure <span class="html-italic">p<sub>s</sub></span> at <span class="html-italic">t<sub>w</sub></span> = 20 μs; (<b>c</b>) aspects of LA and LC at <span class="html-italic">t<sub>w</sub></span> = 300 μs; (<b>d</b>) sound pressure <span class="html-italic">p<sub>s</sub></span> at <span class="html-italic">t<sub>w</sub></span> = 300 μs.</p>
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<p>Aspects of LA and LC and sound pressure changes over time after irradiated pulsed laser <span class="html-italic">t<sub>L</sub></span> induced by fiber laser with a wavelength <span class="html-italic">λ</span> = 1080 nm at pulse width <span class="html-italic">t<sub>w</sub></span> = 20 μs and 300 μs: (<b>a</b>) aspect of LA and LC at <span class="html-italic">t<sub>w</sub></span> = 20 μs; (<b>b</b>) sound pressure <span class="html-italic">p<sub>s</sub></span> at <span class="html-italic">t<sub>w</sub></span> = 20 μs; (<b>c</b>) aspects of LA and LC at <span class="html-italic">t<sub>w</sub></span> = 300 μs; (<b>d</b>) sound pressure <span class="html-italic">p<sub>s</sub></span> at <span class="html-italic">t<sub>w</sub></span> = 300 μs.</p>
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<p>Effect of pulse width <span class="html-italic">t<sub>w</sub></span> on LT using fiber laser.</p>
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<p>Effect of standoff distance in water <span class="html-italic">s<sub>w</sub></span> on LT using fiber laser.</p>
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<p>Aspects of specimen observed by a digital microscope: (<b>a</b>) as-built surface; (<b>b</b>) LT (SLP with fiber laser); (<b>c</b>) blasting (B); (<b>d</b>) LCP (SLP with Nd/YAG laser); (<b>e</b>) B + LT; (<b>f</b>) LT + LCP; (<b>g</b>) B + LCP; (<b>h</b>) B + LT + LCP.</p>
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<p>Aspects of specimen observed by a SEM: (<b>a</b>) as-built surface; (<b>b</b>) LT (SLP with fiber laser); (<b>c</b>) blasting (B); (<b>d</b>) LCP (SLP with Nd/YAG laser); (<b>e</b>) B + LT; (<b>f</b>) LT + LCP; (<b>g</b>) B + LCP; (<b>h</b>) B + LT + LCP.</p>
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<p>Aspects of the fractured specimen: (<b>a</b>) as-built surface; (<b>b</b>) LT (SLP with fiber laser); (<b>c</b>) blasting (B); (<b>d</b>) LCP (SLP with Nd/YAG laser); (<b>e</b>) B + LT; (<b>f</b>) LT + LCP; (<b>g</b>) B + LCP; (<b>h</b>) B + LT + LCP.</p>
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<p>Mechanical properties of as-built, LT, B, LCP, B + LT, B + LCP, LT + LCP, and B + LT + LCP specimens: (<b>a</b>) fatigue life at <span class="html-italic">σ<sub>a</sub></span> = 110 MPa; (<b>b</b>) surface roughness <span class="html-italic">R<sub>a</sub></span>; (<b>c</b>) residual stress <span class="html-italic">σ<sub>R</sub></span>; (<b>d</b>) Rockwell hardness <span class="html-italic">H<sub>R15T</sub></span>; (<b>e</b>) full width at half the maximum of X-ray diffraction pattern <span class="html-italic">FWHM</span>; (<b>f</b>) amplitude of initial angle in the plane bending fatigue test <span class="html-italic">θ<sub>a</sub></span>.</p>
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<p>Mechanical properties of as-built, LT, B, LCP, B + LT, B + LCP, LT + LCP, and B + LT + LCP specimens: (<b>a</b>) fatigue life at <span class="html-italic">σ<sub>a</sub></span> = 110 MPa; (<b>b</b>) surface roughness <span class="html-italic">R<sub>a</sub></span>; (<b>c</b>) residual stress <span class="html-italic">σ<sub>R</sub></span>; (<b>d</b>) Rockwell hardness <span class="html-italic">H<sub>R15T</sub></span>; (<b>e</b>) full width at half the maximum of X-ray diffraction pattern <span class="html-italic">FWHM</span>; (<b>f</b>) amplitude of initial angle in the plane bending fatigue test <span class="html-italic">θ<sub>a</sub></span>.</p>
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<p>Improvement of fatigue strength in as-built PBF–LS/AlSi10Mg specimens via B, LT, and LCP.</p>
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<p>Estimated fatigue life <span class="html-italic">N<sub>f est</sub></span> from fatigue life obtained via experiment <span class="html-italic">N<sub>f exp</sub></span> at <span class="html-italic">σ<sub>a</sub></span> = 110 MPa using mechanical surface properties: (<b>a</b>) Equation (6)—surface roughness <span class="html-italic">R<sub>a</sub></span> and residual stress <span class="html-italic">σ<sub>R</sub></span>, (<b>b</b>) Equation (7)—surface roughness <span class="html-italic">R<sub>a</sub></span>, residual stress <span class="html-italic">σ<sub>R</sub></span>, and Rockwell hardness <span class="html-italic">H<sub>R 15T</sub></span>.</p>
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16 pages, 4516 KiB  
Article
Left Atrial Wall Thickness Estimated by Cardiac CT: Implications for Catheter Ablation of Atrial Fibrillation
by Pedro Silva Cunha, Sérgio Laranjo, Sofia Monteiro, Inês Grácio Almeida, Tiago Mendonça, Iládia Fontes, Rui Cruz Ferreira, Ana G. Almeida, Maxim Didenko and Mário Martins Oliveira
J. Clin. Med. 2024, 13(18), 5379; https://doi.org/10.3390/jcm13185379 - 11 Sep 2024
Viewed by 325
Abstract
Atrial wall thickness (AWT) is a significant factor in understanding the pathological physiological substrate of atrial fibrillation, with a potentially substantial impact on the outcomes of catheter ablation procedures. Precise measurements of the AWT may provide valuable insights for categorising patients with AF [...] Read more.
Atrial wall thickness (AWT) is a significant factor in understanding the pathological physiological substrate of atrial fibrillation, with a potentially substantial impact on the outcomes of catheter ablation procedures. Precise measurements of the AWT may provide valuable insights for categorising patients with AF and planning targeted interventions. Objectives: The purpose of this study was to evaluate the characteristics of the left atrium (LA) using non-invasive multidetector computed tomography (MDCT) scans and subsequent three-dimensional (3D) image post-processing using novel software designed to calculate atrial thickness dimensions and mass. Methods: We retrospectively analysed 128 consecutive patients (33.6% females; mean age 55.6 ± 11.2 years) referred for AF ablation (37 with persistent AF and 91 with paroxysmal AF) who underwent preprocedural MDCT. The images were post-processed and analysed using the ADAS software (Galgo Medical), automatically calculating the LA volume and regional wall thickness. In addition, the software employed a regional semi-automatic LA parcellation feature that divided the atrial wall into 12 segments, generating atrial wall thickness (AWT) maps per segment for each patient. Results: This study demonstrated considerable variability in the average thickness of LA walls, with the anterior segments being the thickest across the cohort. Distinct sex-specific differences were observed, with males exhibiting greater anterior and septal wall thickness than females. No significant associations were identified between the average AWT and body mass index, LA volume, or sphericity. Survival analysis conducted over 24 months revealed a meaningful relationship between mean anterior wall thickness and recurrence-free survival, with increased thickness associated with a lower likelihood of AF-free survival. No such relationship was observed for the indexed LA volume. Conclusions: The variability in AWT and its association with recurrence-free survival following AF ablation suggest that AWT should be considered when stratifying patients for AF management and ablation strategies. These findings underscore the need for personalised treatment approaches and further research on the interplay of the structural properties of the left atrium as factors that can serve as important prognostic markers in AF treatment. Full article
(This article belongs to the Special Issue State of the Art: Catheter Ablation of Atrial Fibrillation)
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<p>Software reconstruction using multidetector computed tomography images and analysis using ADAS 3D™ software generated a 3D map of the atrial wall thickness. Thickness colour map: thickness &lt;1 mm, red; 1–2 mm, yellow; 2–3 mm, green; 3–4 mm, blue; &gt;4 mm, purple.</p>
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<p>Schematic illustration of 14 locations where the wall thickness was measured in the left atrium. Posterior (<b>left panel</b>), anterior (<b>middle panel</b>), and left lateral views (<b>right panel</b>) are presented. Legend: Segments 1–4, superior wall; 5–6, posterior wall; 7, septal wall; 8–11, anterior wall; 12, left lateral wall; and 13–14, between superior and inferior pulmonary veins. LIPV, left inferior pulmonary vein; LSPV, left superior pulmonary vein; MITRAL, mitral annulus; RIPV, right inferior pulmonary vein; RSPV, right superior pulmonary vein.</p>
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<p>Example of LA wall thickness measurement (posterior view). The bar on the right shows the colour code assigned to the thickness variations.</p>
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<p>Boxplot of left atrial wall thickness distribution according to region.</p>
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<p>Box plot with comparison by sex of the left atrial volume index to the body surface. Legend: LAVI, left atrial volume index; SD, standard deviation.</p>
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<p>Mean left atrial wall thickness by region.</p>
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<p>Illustration of the 14 locations in the left atrium and corresponding topographic colour maps showing thickness differences. Posterior and anterior views (<b>A</b>,<b>B</b>), right anterior oblique view (<b>C</b>), and left lateral view (<b>D</b>) are shown. Legend: LIPV, left inferior pulmonary vein; RIPV, right inferior pulmonary vein; RSPV, right superior pulmonary vein; MITRAL, mitral annulus; LAA, left atrial appendage ostium.</p>
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<p>Log-rank test estimates of recurrence-free survival according to mean anterior wall thickness (optimal cutpoint → 1.69 mm).</p>
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<p>Survival curve estimates of arrhythmia recurrence-free survival according to left atrial index volume. Legend: The optimal cut-off point obtained by maximising the sum of sensitivity and specificity was 58.6 mL/m<sup>2</sup>.</p>
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<p>Illustration of left anterior wall thickness in different patients. The areas with the highest thickness corresponded to the Bachmann bundle region. Legend: LIPV = left inferior pulmonary vein, LSPV = left superior pulmonary vein, RIPV = right inferior pulmonary vein, RSPV = right superior pulmonary vein, MITRAL = mitral annulus, LAA = left atrial appendage ostium.</p>
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19 pages, 7149 KiB  
Article
Continuous High-Precision Positioning in Smartphones by FGO-Based Fusion of GNSS–PPK and PDR
by Amjad Hussain Magsi, Luis Enrique Díez and Stefan Knauth
Micromachines 2024, 15(9), 1141; https://doi.org/10.3390/mi15091141 - 11 Sep 2024
Viewed by 320
Abstract
The availability of raw Global Navigation Satellites System (GNSS) measurements in Android smartphones fosters advancements in high-precision positioning for mass-market devices. However, challenges like inconsistent pseudo-range and carrier phase observations, limited dual-frequency data integrity, and unidentified hardware biases on the receiver side prevent [...] Read more.
The availability of raw Global Navigation Satellites System (GNSS) measurements in Android smartphones fosters advancements in high-precision positioning for mass-market devices. However, challenges like inconsistent pseudo-range and carrier phase observations, limited dual-frequency data integrity, and unidentified hardware biases on the receiver side prevent the ambiguity resolution of smartphone GNSS. Consequently, relying solely on GNSS for high-precision positioning may result in frequent cycle slips in complex conditions such as deep urban canyons, underpasses, forests, and indoor areas due to non-line-of-sight (NLOS) and multipath conditions. Inertial/GNSS fusion is the traditional common solution to tackle these challenges because of their complementary capabilities. For pedestrians and smartphones with low-cost inertial sensors, the usual architecture is Pedestrian Dead Reckoning (PDR)+ GNSS. In addition to this, different GNSS processing techniques like Precise Point Positioning (PPP) and Real-Time Kinematic (RTK) have also been integrated with INS. However, integration with PDR has been limited and only with Kalman Filter (KF) and its variants being the main fusion techniques. Recently, Factor Graph Optimization (FGO) has started to be used as a fusion technique due to its superior accuracy. To the best of our knowledge, on the one hand, no work has tested the fusion of GNSS Post-Processed Kinematics (PPK) and PDR on smartphones. And, on the other hand, the works that have evaluated the fusion of GNSS and PDR employing FGO have always performed it using the GNSS Single-Point Positioning (SPP) technique. Therefore, this work aims to combine the use of the GNSS PPK technique and the FGO fusion technique to evaluate the improvement in accuracy that can be obtained on a smartphone compared with the usual GNSS SPP and KF fusion strategies. We improved the Google Pixel 4 smartphone GNSS using Post-Processed Kinematics (PPK) with the open-source RTKLIB 2.4.3 software, then fused it with PDR via KF and FGO for comparison in offline mode. Our findings indicate that FGO-based PDR+GNSS–PPK improves accuracy by 22.5% compared with FGO-based PDR+GNSS–SPP, which shows smartphones obtain high-precision positioning with the implementation of GNSS–PPK via FGO. Full article
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<p>Inertial+GNSS fusion architectures.</p>
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<p>PDR mechanism.</p>
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<p>Factor graph for PDR+GNSS–SPP fusion architecture.</p>
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<p>Data collection setup.</p>
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<p>Difference between the ground truth, SPP-GNSS, and PPK-GNSS data.</p>
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<p>RTKLIB settings.</p>
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<p>Two-dimensional horizontal positioning errors in PDR+GNSS–SPP fusion architecture.</p>
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<p>Combined overall CDF from both fusion architectures using FGO and KF.</p>
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<p>Comparison of trajectories in PDR+GNSS–SPP fusion architectures.</p>
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<p>Two-dimensional horizontal positioning errors in PDR+GNSS–PPK fusion architecture.</p>
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<p>Comparison of trajectories in PDR+GNSS–PPK fusion architecture.</p>
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<p>Computational time consumed by FGO-based PDR+GNSS–PPK fusion architecture.</p>
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<p>Cumulative computational time consumed by FGO-based PDR+GNSS–PPK fusion.</p>
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<p>Google Pixel 4 raw GNSS observartions.</p>
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22 pages, 9684 KiB  
Article
Techniques and Instruments for Assessing and Reducing Risk of Exposure to Nanomaterials in Construction, Focusing on Fire-Resistant Insulation Panels Containing Nanoclay
by Romeo Cristian Ciobanu and Mihaela Aradoaei
Nanomaterials 2024, 14(18), 1470; https://doi.org/10.3390/nano14181470 - 10 Sep 2024
Viewed by 272
Abstract
The paper explains how nano exposure is assessed in the construction field and focuses on the production of fire-resistant insulation panels with nanoclay. Utilizing the commercial ANSYS CFX® software, a preliminary theoretical simulation was conducted on nano exposure in the workplace, which [...] Read more.
The paper explains how nano exposure is assessed in the construction field and focuses on the production of fire-resistant insulation panels with nanoclay. Utilizing the commercial ANSYS CFX® software, a preliminary theoretical simulation was conducted on nano exposure in the workplace, which revealed that particle dispersion is primarily driven by diffusion. Panel post-processing through drilling results in the highest inhalation exposure, followed by mixing and grinding activities. Compared to a state of ‘no activity’, each activity resulted in an exposure increase by a factor of min. 1000. An overall assessment suggests that the use of nanoparticles in construction materials may not significantly heighten workers’ exposure to nanopowders when considering particle concentration alone as opposed to using traditional micro-scale materials. However, the issue persists when it comes to blending powders or performing finishing tasks on panels, with concentration levels being significantly higher for drilling, grinding, and mixing powders at 2.4 times above the standard reference value (40,000 particles/cm3); this is unacceptable, even for brief durations. Examination of dermal contact with gloves and masks worn by workers revealed no nanoparticle penetration. Safety measures were proposed for workers based on decision trees to enhance their safety. Ten categories of protection strategies have been devised to combat the impact of nanoparticles, which are tailored to specific technical situations, but they must be modified for various types of nanoparticles despite potential shared health implications. Full article
(This article belongs to the Special Issue Advances in Toxicity of Nanoparticles in Organisms (2nd Edition))
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<p>SEM image and particle size of bentonite nanoclay.</p>
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<p>Composition of bentonite nanoclay.</p>
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<p>The simplified geometry of chamber (<b>a</b>), related grid (<b>b</b>), and streamlines of the air field within chamber (<b>c</b>).</p>
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<p>Concentrations of nanomaterials over time in the median plane of the space.</p>
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<p>Raw material preparation.</p>
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<p>Manufacture of fire-resistant panel.</p>
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<p>Finishing of panel and storage.</p>
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<p>Panel post-processing by drilling and cutting; Recycling.</p>
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<p>Example of commercial fire-resistant insulation panels containing nanoclay.</p>
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<p>Size distribution of particles vs. test scenarios.</p>
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<p>Placement of points for measuring particle parameters in the working area.</p>
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<p>SEM analysis of powder samples.</p>
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<p>Decision tree for the nanoparticle contents that are less than 5%.</p>
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<p>Decision tree for the nanoparticle contents that are more than 5%.</p>
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15 pages, 5121 KiB  
Article
Regional Spatial Mean of Ionospheric Irregularities Based on K-Means Clustering of ROTI Maps
by Yenca Migoya-Orué, Oladipo E. Abe and Sandro Radicella
Atmosphere 2024, 15(9), 1098; https://doi.org/10.3390/atmos15091098 - 9 Sep 2024
Viewed by 243
Abstract
In this paper, we investigate and propose the application of an unsupervised machine learning clustering method to characterize the spatial and temporal distribution of ionospheric plasma irregularities over the Western African equatorial region. The ordinary Kriging algorithm was used to interpolate the rate [...] Read more.
In this paper, we investigate and propose the application of an unsupervised machine learning clustering method to characterize the spatial and temporal distribution of ionospheric plasma irregularities over the Western African equatorial region. The ordinary Kriging algorithm was used to interpolate the rate of change of the total electron content (TEC) index (ROTI) over gridded 0.5° by 0.5° latitude and longitude regional maps in order to simulate the level of ionospheric plasma irregularities in a quasi-real-time scenario. K-means was used to obtain a spatial mean index through an optimal stratification of regional post-processed ROTI maps. The results obtained could be adapted by appropriate K-means algorithms to a real-time scenario, as has been performed for other applications. This method could allow us to monitor plasma irregularities in real time over the African region and, therefore, lead to the possibility of mitigating their effects on satellite-based location systems in the said region. Full article
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<p>Map of geographic locations of GNSS ground-based stations used.</p>
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<p>Solar wind plasma speed, IMF-Bz, and Dst parameters for days enclosing 2nd October 2013 storm.</p>
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<p>An example of irregularities during disturbed conditions on 2 October 2013 (DOY 275), as indicated by ROT/ROTI in FUTY (<b>left</b>) and NKLG (<b>right</b>) stations. The different colors lines represent the different visible satellites.</p>
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<p>ROTI values at IPP (<b>left</b>) during disturbed conditions on 2 October 2013 (DOY 275) at 2000 UT and ROTI map after Kriging interpolation (<b>right</b>). Empty red circles in both maps represent the GNSS ground-based stations used.</p>
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<p>Hourly regional ROTI maps (<b>left</b>) and Kriging variance maps (<b>right</b>) during a geomagnetically disturbed day (DOY 275 of the year 2013). The yellow–red areas in the maps on the left indicate the presence of nighttime irregularities at 1900, 2000, 2100, and 2200 UT.</p>
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<p>Hourly regional ROTI maps (<b>left</b>) and Kriging variance maps (<b>right</b>) during a geomagnetic quiet day (DOY 301 of the year 2013). The yellow–red areas in the maps on the left indicate the presence of nighttime irregularities at 1900, 2000, 2100, and 2200 UT.</p>
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<p>Histogram of the ROTI variance values after Kriging interpolation corresponding to all maps every 15 min on day 301, 2013. The mean, standard deviation, and 99% and 75% percentile values are included.</p>
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<p>ROTI maps projected on West African map on DOY 275 (disturbed day) at 20:20 UT (<b>left</b>) and its stratification in clusters (<b>right</b>).</p>
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<p>ROTI projected over African map for a quiet day (DOY 301, 2013) at 22:20 UT (<b>left</b>) and its stratification in clusters (<b>right</b>).</p>
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