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13 pages, 3469 KiB  
Article
Design of Composite N-Doped Carbon Nanofiber/TiO2/Diatomite Separator for Lithium–Sulfur Batteries
by Wenjie Xiao, Xiaoyu Wu, Yang Shu, Yitao Zha and Sainan Liu
Materials 2024, 17(22), 5615; https://doi.org/10.3390/ma17225615 - 17 Nov 2024
Viewed by 316
Abstract
Lithium–sulfur batteries (LSBs) exhibit high theoretical specific capacities, abundant resource reserves, and low costs, making them promising candidates for next-generation lithium-ion batteries (LIBs). However, significant challenges, such as the shuttle effect and volume expansion, hinder their practical applications. To address these issues, this [...] Read more.
Lithium–sulfur batteries (LSBs) exhibit high theoretical specific capacities, abundant resource reserves, and low costs, making them promising candidates for next-generation lithium-ion batteries (LIBs). However, significant challenges, such as the shuttle effect and volume expansion, hinder their practical applications. To address these issues, this study introduces a unique intermediate layer comprising N-doped carbon nanofiber/TiO2/diatomite (NCNF/TiO2/DE) from the perspective of membrane modification. The intermediate layer comprises nitrogen-doped titanium dioxide/carbon nanofiber (NCNF/TiO2) materials, with diatomite filling the fiber gaps. This forms a three-dimensional (3D) conductive network that provides ample space for sulfur volume expansion and numerous adsorption active sites, thereby accelerating electrolyte penetration and lithium-ion diffusion. These features collectively contribute to the outstanding electrochemical performance of the battery. At 0.1 C, the NCNF/TiO2/DE-800-coated separator battery achieved a first-cycle discharge specific capacity of 1311.1 mAh g−1, significantly higher than the uncoated lithium–sulfur battery (919.6 mAh g−1). Under varying current densities, the NCNF/TiO2/DE-800 material demonstrates good electrochemical reversibility and exhibits high lithium-ion diffusion rates and low charge-transfer resistance. Therefore, this study provides an advanced intermediate layer material that enhances the electrochemical performance of lithium–sulfur batteries. Full article
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<p>Schematic illustration of the synthesis process of NCNF/TiO<sub>2</sub>/DE.</p>
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<p>(<b>a</b>–<b>c</b>) SEM micrographs of NCNF/TiO<sub>2</sub>/DE at different magnifications, (<b>d</b>) TEM image, (<b>e</b>,<b>f</b>) high-resolution TEM images, (<b>g</b>–<b>l</b>) elemental mapping images of C, O, N, Ti, and Si.</p>
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<p>(<b>a</b>) XRD patterns of NCNF/TiO<sub>2</sub>/DE at 600 °C, 700 °C, and 800 °C. (<b>b</b>) Raman spectra of NCNF/TiO<sub>2</sub>/DE at 600 °C, 700 °C, and 800 °C. (<b>c</b>) Nitrogen adsorption/desorption isotherms and pore size distribution (PSD) curves of NCNF/TiO<sub>2</sub>/DE-800.</p>
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<p>(<b>a</b>) XPS spectra of NCNF/TiO<sub>2</sub>/DE-800. (<b>b</b>) High-resolution XPS spectra of C 1s, N 1s, Ti 2p, and Si 2p.</p>
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<p>(<b>a</b>) CV curves of batteries with different intermediate layers at a scan rate of 0.1 mV s<sup>−1</sup>. (<b>b</b>) CV curve of the battery with NCNF/TiO<sub>2</sub>/DE-800 intermediate layer. (<b>c</b>) CV curves of the battery with NCNF/TiO<sub>2</sub>/DE-800 intermediate layer at scan rates ranging from 0.1 to 0.5 mV s<sup>−1</sup>. (<b>d</b>) Relationship between peak current values for anodic and cathodic processes and the square root of the scan rate obtained from CV measurements. (<b>e</b>) Initial charge–discharge curves of batteries with different intermediate layers at 0.5 C. (<b>f</b>) Constant current charge–discharge curves of the battery with NCNF/TiO<sub>2</sub>/DE-800 intermediate layer at 0.1 C over 1, 5, 10, 25, 50, and 100 cycles. (<b>g</b>) Cycling performance of batteries with different intermediate layers at 0.1 C over 100 cycles. (<b>h</b>) Charge–discharge curves of the battery with NCNF/TiO<sub>2</sub>/DE-800 intermediate layer at different current densities.</p>
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<p>Nyquist plots of batteries with different intermediate layers.</p>
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16 pages, 3143 KiB  
Article
A Low-Power 5-Bit Two-Step Flash Analog-to-Digital Converter with Double-Tail Dynamic Comparator in 90 nm Digital CMOS
by Reena George and Nagesh Ch
J. Low Power Electron. Appl. 2024, 14(4), 53; https://doi.org/10.3390/jlpea14040053 - 4 Nov 2024
Viewed by 576
Abstract
Low-power portable devices play a major role in IoT applications, where the analog-to-digital converters (ADCs) are very important components for the processing of analog signals. In this paper, a 5-bit two-step flash ADC with a low-power double-tail dynamic comparator (DTDC) using the control [...] Read more.
Low-power portable devices play a major role in IoT applications, where the analog-to-digital converters (ADCs) are very important components for the processing of analog signals. In this paper, a 5-bit two-step flash ADC with a low-power double-tail dynamic comparator (DTDC) using the control switching technique is presented. The most significant bit (MSB) in the proposed design is produced by only one low-power DTDC in the first stage, and the remaining bits are generated by the flash ADC in the second stage with the help of an auto-control circuit. A control circuit produced reference voltages with respect to the control input and mid-point voltage (Vk). The proposed design and simulations are carried out using 90 nm CMOS technology. The result shows that the peak differential non-linearity (DNL) and integral non-linearity (INL) are +0.60/−0.69 and +0.66/−0.40 LSB, respectively. The signal-to-noise and distortion ratio (SNDR) for an input signal having a frequency of 1.75 MHz is found to be 30.31 dB. The total power consumption of the proposed design is significantly reduced, which is 439.178 μW for a supply voltage of 1.2 V. The figure of merit (FOM) is about 0.054 pJ/conversion step at 250 MS/s. The present design provides low power consumption and occupies less area compared to the existing works. Full article
(This article belongs to the Special Issue Analog/Mixed-Signal Integrated Circuit Design)
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<p>Block diagram of proposed N-bit two-step flash ADC.</p>
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<p>Schematic diagram of proposed 5-bit flash ADC.</p>
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<p>Schematic diagram of double tail dynamic comparator.</p>
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<p>Circuit diagram of control circuit.</p>
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<p>Circuit diagram of mux-based encoder.</p>
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<p>Transient simulation of low-power DTDC.</p>
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<p>Transient simulation of control circuit.</p>
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<p>DC simulation of control circuit.</p>
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<p>Post-layout simulation of 5-bit proposed two-step flash ADC.</p>
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<p>Spectral plot of low input frequency 1.75 MHz at 250 MS/s after post-layout simulation.</p>
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<p>Spectral plot of Nyquist frequency 121.09 MHz at 250 MS/s after post-layout simulation.</p>
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<p>Monte-Carlo simulation of (<b>a</b>) SNR and (<b>b</b>) SINAD for low input 1.75 MHz at 250 MS/s after post-layout simulation for 200 runs.</p>
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<p>Monte-Carlo simulation of (<b>a</b>) SFDR and (<b>b</b>) SNDR for input 1.75 MHz at 250 MS/s after post-layout simulation.</p>
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<p>Post-layout simulations: (<b>a</b>) DNL and (<b>b</b>) INL.</p>
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<p>Monte-Carlo simulation: (<b>a</b>) DNL and (<b>b</b>) INL after post-layout simulation for 200 runs.</p>
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<p>Post-layout of (<b>a</b>) control circuit and (<b>b</b>) double-tail dynamic comparator.</p>
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<p>Layout of proposed 5-bit two-step flash ADC.</p>
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<p>Monte-Carlo simulation of total power consumption with 200 runs.</p>
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<p>(<b>a</b>) SNDR and (<b>b</b>) SFDR of proposed ADC versus temperatures (T = −40 °C to 120 °C) with process corner variations (TT, SF, FS, SS, FF) after post-layout simulation.</p>
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<p>Average power of proposed ADC versus (<b>a</b>) temperatures (T = −40 °C to 120 °C) and (<b>b</b>) supply voltage (VDD = 1 V to 1.3 V) with process corner variations (TT, SF, FS, SS, FF) after post-layout simulation.</p>
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17 pages, 1877 KiB  
Article
High Consistency Ramp Design Method for Low Noise Column Level Readout Chain
by Zhongjie Guo, Lin Li, Ruiming Xu, Suiyang Liu, Ningmei Yu, Yuan Yang and Longsheng Wu
Sensors 2024, 24(21), 7057; https://doi.org/10.3390/s24217057 - 1 Nov 2024
Viewed by 538
Abstract
In order to address the inconsistency problem caused by parasitic backend wiring among multiple ramp generators and among multiple columns in large-array CMOS image sensors (CIS), this paper proposes a high-precision compensation technology combining average voltage technology, adaptive negative feedback dynamic adjustment technology, [...] Read more.
In order to address the inconsistency problem caused by parasitic backend wiring among multiple ramp generators and among multiple columns in large-array CMOS image sensors (CIS), this paper proposes a high-precision compensation technology combining average voltage technology, adaptive negative feedback dynamic adjustment technology, and digital correlation double sampling technology to complete the design of an adaptive ramp signals inconsistency calibration scheme. The method proposed in this article has been successfully applied to a CIS with a pixel array of 8192(H) × 8192(V), based on the 55 nm 1P4M CMOS process, with a pixel size of 10×10μm2. The chip area is 88(H) × 89(V) mm2, and the frame rate is 10 fps. The column-level analog-to-digital converter is a 12-bit single-slope analog-to-digital converter (SS ADC). The experimental results show that the ramp generation circuit proposed in this paper can reduce the inconsistency among the ramp signals to 0.4% LSB, decreases the column fixed pattern noise (CFPN) caused by inconsistent ramps of each column to 0.000037% (0.15 e), and increases the overall chip area and power consumption by only 0.6% and 0.5%, respectively. This method provides an effective solution to the influence of non-ideal factors on the consistency of ramp signals in large area array CIS. Full article
(This article belongs to the Section Sensing and Imaging)
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<p>The schematic diagram of CMOS image sensor architecture.</p>
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<p>The metal wire distributed RC parasitic model.</p>
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<p>The error curves of different column numbers driven by global ramp circuit.</p>
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<p>The error curve of the distortion of the non-constant gate capacitance of the comparator input stage to the ramp signal.</p>
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<p>Circuit diagram and working sequence of integral ramp generator: (<b>a</b>) circuit diagram; (<b>b</b>) sequence diagram.</p>
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<p>The voltage averaging principle diagram of distributed multiple ramp signal generator.</p>
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<p>Column level inconsistency error caused by ramp inconsistency between the average voltage scheme and the traditional global ramp scheme.</p>
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<p>The high consistency adaptive ramp circuit for a large area CMOS image sensor.</p>
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<p>The sequence diagram of adaptive ramp circuit.</p>
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<p>The schematic diagram of the overall layout.</p>
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<p>Overall layout design.</p>
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<p>The adaptive calibration waveform of the ramp signal generator.</p>
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<p>The relative error diagram of slope between adaptive ramp and ideal ramp.</p>
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<p>The error diagram among the ramp signals of each column.</p>
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<p>Nonlinear error diagram of ramp signal of 12 bit adaptive ramp generator: (<b>a</b>) DNL; (<b>b</b>) INL.</p>
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21 pages, 6757 KiB  
Article
Study of Hydrofoil Boundary Layer Prediction with Two Correlation-Based Transition Models
by Changliang Ye, Yang Wang, Dongsen An, Jun Chen, Hongyeyu Yan, Yuan Zheng, Kan Kan and Bart P. M. van Esch
J. Mar. Sci. Eng. 2024, 12(11), 1965; https://doi.org/10.3390/jmse12111965 - 1 Nov 2024
Viewed by 526
Abstract
In the realm of marine science and engineering, hydrofoils play a pivotal role in the efficiency and performance of marine turbines and water-jet pumps. In this investigation, the boundary layer characteristics of an NACA0009 hydrofoil with a blunt trailing edge are focused on. [...] Read more.
In the realm of marine science and engineering, hydrofoils play a pivotal role in the efficiency and performance of marine turbines and water-jet pumps. In this investigation, the boundary layer characteristics of an NACA0009 hydrofoil with a blunt trailing edge are focused on. The effectiveness of both the two-equation gamma theta (γ-Reθt) transition model and the one-equation intermittency (γ) transition model in forecasting boundary layer behavior is evaluated. When considering natural transition, these two models outperform the shear stress transport two-equation (SST k-ω) turbulence model, notably enhancing the accuracy of predicting boundary layer flow distribution for chord-length Reynolds numbers (ReL) below 1.6 × 106. However, as ReL increases, both transition models deviate from experimental values, particularly when ReL is greater than 2 × 106. The results indicate that the laminar separation bubble (LSB) is sensitive to changes in angles of attack (AOA) and ReL, with its formation observed at AOA greater than 2°. The dimensions of the LSB, including the initiation and reattachment points, are found to contract as ReL increases while maintaining a constant AOA. Conversely, an increase in AOA at similar ReL values leads to a reduced size of the LSB. The findings are essential for the design and performance optimization of water-jet pumps, particularly in predicting and flow separation and transition phenomena. Full article
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<p>NACA0009 blunt trailing edge hydrofoil computational domain.</p>
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<p>Grid diagram.</p>
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<p>Iterative convergence diagrams of two models.</p>
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<p>Distribution of wall friction coefficient (<span class="html-italic">Re<sub>L</sub></span> = 2 × 10<sup>6</sup>).</p>
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<p>Boundary layer shape factor distribution (<span class="html-italic">Re<sub>L</sub></span> = 2 × 10<sup>6</sup>).</p>
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<p>Distribution of <span class="html-italic">y</span>-direction velocities over time in the wake region (<span class="html-italic">Re<sub>L</sub></span> = 2 × 10<sup>6</sup>).</p>
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<p>Tangential time-averaged velocity distribution under different turbulence models.</p>
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<p>Distribution of relative thickness <span class="html-italic">δ</span>/<span class="html-italic">h</span> under various models.</p>
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<p>Distribution of the shape factor <span class="html-italic">H</span><sub>12</sub> for the hydrofoil boundary layer for various models.</p>
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<p>Distribution of the intermittent factor <span class="html-italic">γ</span> for the hydrofoil boundary layer.</p>
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<p>Complete transition position of the boundary layer at different Reynolds numbers.</p>
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<p>Turbulence intensity development along the flow direction.</p>
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<p>Layout of LSB on the surface at different AOA.</p>
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<p>Laminar separation bubble length distributions of hydrofoil.</p>
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21 pages, 5750 KiB  
Article
Remote Sensing of Residential Landscape Irrigation in Weber County, Utah: Implications for Water Conservation, Image Analysis, and Drone Applications
by Annelise M. Turman, Robert B. Sowby, Gustavious P. Williams and Neil C. Hansen
Sustainability 2024, 16(21), 9356; https://doi.org/10.3390/su16219356 - 28 Oct 2024
Viewed by 1299
Abstract
Analyzing irrigation patterns to promote efficient water use in urban areas is challenging. Analysis of irrigation by remote sensing (AIRS) combines multispectral aerial imagery, evapotranspiration data, and ground-truth measurements to overcome these challenges. We demonstrate AIRS on eight neighborhoods in Weber County, Utah, [...] Read more.
Analyzing irrigation patterns to promote efficient water use in urban areas is challenging. Analysis of irrigation by remote sensing (AIRS) combines multispectral aerial imagery, evapotranspiration data, and ground-truth measurements to overcome these challenges. We demonstrate AIRS on eight neighborhoods in Weber County, Utah, using 0.6 m National Agriculture Imagery Program (NAIP) and 0.07 m drone imagery, reference evapotranspiration (ET), and water use records. We calculate the difference between the actual and hypothetical water required for each parcel and compare water use over three time periods (2018, 2021, and 2023). We find that the quantity of overwatering, as well as the number of customers overwatering, is decreasing over time. AIRS provides repeatable estimates of irrigated area and irrigation demand that allow water utilities to track water user habits and landscape changes over time and, when controlling for other variables, see if water conservation efforts are effective. In terms of image analysis, we find that (1) both NAIP and drone imagery are sufficient to measure irrigated area in urban settings, (2) the selection of a threshold value for the normalized difference vegetation index (NDVI) becomes less critical for higher-resolution imagery, and (3) irrigated area measurement can be enhanced by combining NDVI with other tools such as building footprint extraction, object classification, and deep learning. Full article
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<p>Approach for Analysis of Irrigation by Remote Sensing (AIRS) [<a href="#B16-sustainability-16-09356" class="html-bibr">16</a>].</p>
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<p>Eight study areas within West Haven, Utah, with metered parcels.</p>
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<p>Drone flight restrictions with our general study area (rectangle). The red region represents restricted zones, the blue region represents authorization zones, the orange region represents enhanced warning zones, and the yellow region represents warning zones.</p>
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<p>Adjusting NDVI threshold values. (<b>a</b>) Base image without NDVI pixels. (<b>b</b>) Base image with 0.10 NDVI threshold value. (<b>c</b>) Base image with 0.15 NDVI threshold value. (<b>d</b>) Base image with 0.19 NDVI threshold value.</p>
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<p>NDVI variations from shadows (top, base image; bottom, base image with NDVI overlay).</p>
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<p>(<b>a</b>) NDVI pixel count distributions for 2018, (<b>b</b>) NDVI pixel count distributions for 2021, (<b>c</b>) NDVI pixel count distributions for 2023.</p>
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<p>(<b>a</b>) NDVI value vs. pixel count distribution of Landsat (30 m resolution), (<b>b</b>) NDVI value vs. pixel count distribution for NAIP (0.6 m resolution), (<b>c</b>) NDVI value vs. pixel count distribution of drone images (0.067 m resolution).</p>
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<p>(<b>a</b>) Base image, (<b>b</b>) base image with NDVI pixels and a legend, demonstrating that roofs are being classified as irrigated area.</p>
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<p>ModelBuilder process used to measure irrigated area.</p>
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<p>Variation of irrigated area due to imagery type: (<b>a</b>) 2018 NAIP image and irrigated area, (<b>b</b>) 2021 NAIP image and irrigated area, (<b>c</b>) 2023 drone image and irrigated area.</p>
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<p>Distribution of percentage of overwatering for all parcels.</p>
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<p>Percentage of overwatering grouped by study area.</p>
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<p>(<b>a</b>) Changes in percentage of overwatering during 2018, (<b>b</b>) Changes in percentage of overwatering during 2021, (<b>c</b>) Changes in percentage of overwatering during 2023.</p>
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<p>(<b>a</b>) Irrigated area vs. percentage of overwatering for 2018, (<b>b</b>) Irrigated area vs. percentage of overwatering for 2021, (<b>c</b>) Irrigated area vs. percentage of overwatering for 2023.</p>
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<p>(<b>a</b>) Irrigated area vs. percentage of overwatering for 2018, (<b>b</b>) Irrigated area vs. percentage of overwatering for 2021, (<b>c</b>) Irrigated area vs. percentage of overwatering for 2023.</p>
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22 pages, 9440 KiB  
Review
Modification and Functionalization of Separators for High Performance Lithium–Sulfur Batteries
by Mengyu Shen, Songshi Xu, Xiuyu Wang, Yonghui Zhang, Yu Feng, Fei Xing, Yingying Yang and Qiqian Gao
Int. J. Mol. Sci. 2024, 25(21), 11446; https://doi.org/10.3390/ijms252111446 - 24 Oct 2024
Viewed by 685
Abstract
Lithium–sulfur batteries (LSB) have been recognized as a prominent potential next-generation energy storage system, owing to their substantial theoretical specific capacity (1675 mAh g−1) and high energy density (2600 Wh kg−1). In addition, sulfur’s abundance, low cost, and environmental [...] Read more.
Lithium–sulfur batteries (LSB) have been recognized as a prominent potential next-generation energy storage system, owing to their substantial theoretical specific capacity (1675 mAh g−1) and high energy density (2600 Wh kg−1). In addition, sulfur’s abundance, low cost, and environmental friendliness make commercializing LSB feasible. However, challenges such as poor cycling stability and reduced capacity, stemming from the formation and diffusion of lithium polysulfides (LiPSs), hinder LSB’s practical application. Introducing functional separators represents an effective strategy to surmount these obstacles and enhance the electrochemical performance of LSBs. Here, we have conducted a comprehensive review of recent advancements in functional separators for LSBs about various (i) carbon and metal compound materials, (ii) polymer materials, and (iii) novel separators in recent years. The detailed preparation process, morphology and performance characterization, and advantages and disadvantages are summarized, aiming to fundamentally understand the mechanisms of improving battery performance. Additionally, the development potential and future prospects of advanced separators are also discussed. Full article
(This article belongs to the Section Materials Science)
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<p>(<b>a</b>) The configuration of LSB with three layers of modified separators [<a href="#B32-ijms-25-11446" class="html-bibr">32</a>]. Copyright © 2017, with permission from John Wiley and Sons. (<b>b</b>) The schematic representation of a LSB incorporating a RGO-coated separator [<a href="#B35-ijms-25-11446" class="html-bibr">35</a>]. Copyright © 2015, with permission from IOP Publishing. (<b>c</b>) Schematic diagram of a LSB with KB/Mo<sub>2</sub>C-modified separator. (<b>d</b>) Photograph of the Li<sub>2</sub>S<sub>6</sub> adsorption test: KB-modified and KB/Mo<sub>2</sub>C-modified separators. (<b>e</b>) Cycle performance at 0.2 C; ex situ XANES of (<b>f</b>) Mo K-edge and (<b>g</b>) S K-edge for the separator at certain states of charge/discharge during the first cycle and after 50 cycles. (<b>h</b>) The corresponding discharge–charge curves [<a href="#B39-ijms-25-11446" class="html-bibr">39</a>]. Copyright © 2021, with permission from Elsevier.</p>
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<p>(<b>a</b>) Schematic illustration for the preparation process of HSN-rGO; SEM images of fresh Li (<b>b</b>,<b>c</b>) and Li metal anodes of the LSBs with HSN-rGO-PP (<b>d</b>,<b>e</b>) after 250 cycles at 1 C; (<b>f</b>) CV curves at different scan rate of the LSBs and (<b>g</b>) the corresponding linear fitting based on Randles–Sevick equation of the LSBs with HSN-rGO-PP; (<b>h</b>) long-term cyclic stability over 1000 cycles at 1 C of the LSBs with PP, LSN-rGO-PP, and HSN-rGO-PP, respectively [<a href="#B42-ijms-25-11446" class="html-bibr">42</a>]. Copyright © 2021, with permission from Elsevier. (<b>i</b>) Schematic diagram of mwGMSMO synthesis process [<a href="#B43-ijms-25-11446" class="html-bibr">43</a>]. Copyright © 2021, with permission from American Chemical Society. (<b>j</b>,<b>k</b>) TEM images of CoS<sub>2</sub>/CNT materials at different magnifications; (<b>l</b>) synthesis of CoS<sub>2</sub>/CNTs; (<b>m</b>) fabrication of a separator modified with functional materials; (<b>n</b>) application diagram of CoS<sub>2</sub>/CNT separator in LSBs [<a href="#B44-ijms-25-11446" class="html-bibr">44</a>]. Copyright © 2023, with permission from Elsevier.</p>
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<p>(<b>a</b>) Schematic diagram of manufacturing methods for NSMO and SMO separators. Schematic diagram of prohibited shuttle by the (<b>b</b>) PP and (<b>c</b>) SMO separators. (<b>d</b>) Long cycle performance of LSBs with SMO separators after 500 cycles at 0.5 C [<a href="#B57-ijms-25-11446" class="html-bibr">57</a>]. Copyright © 2021, with permission from Elsevier. (<b>e</b>) Mechanism diagram of rGO/MoO<sub>2</sub>-modified PP separator [<a href="#B58-ijms-25-11446" class="html-bibr">58</a>]. Copyright © 2021, with permission from Springer Nature. (<b>f</b>) Schematic diagram of the synthesis process of the S/YSC@Fe<sub>3</sub>O<sub>4</sub> [<a href="#B59-ijms-25-11446" class="html-bibr">59</a>]. Copyright © 2017, with permission from John Wiley and Sons. (<b>g</b>) Schematic diagram of HPCA-TO. (<b>h</b>) Cycle performance and corresponding Coulombic efficiency of batteries with different separators at 1 C. (<b>i</b>) Rate capacity of the batteries with the different separators at different current rates [<a href="#B60-ijms-25-11446" class="html-bibr">60</a>]. Copyright © 2022, with permission from Elsevier.</p>
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<p>(<b>a</b>) Schematic of MoS<sub>2</sub>@MGF as an interlayer for LSBs. Schematic of LSBs with PP (<b>b</b>) and MoS<sub>2</sub>@MGF/PP (<b>c</b>) separators; (<b>e</b>) rate capabilities; and cycling performance (<b>d</b>) at 1 C for LSBs with MoS<sub>2</sub>/PP, MGF/PP, MoS<sub>2</sub>@MGF/PP, MoS<sub>2</sub>@SP/PP, and PP [<a href="#B67-ijms-25-11446" class="html-bibr">67</a>]. Copyright © 2024, with permission from John Wiley and Sons. (<b>f</b>) Schematic diagram of the synthesis process of the NiS<sub>2</sub>-MnS/MoS<sub>2</sub>-3DNGr hybrid. (<b>g</b>,<b>h</b>) TEM images of the NiS<sub>2</sub>-MnS/MoS<sub>2</sub>-3DNGr hybrid [<a href="#B70-ijms-25-11446" class="html-bibr">70</a>]. Copyright © 2022, with permission from Elsevier.</p>
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<p>Schematic illustration of the LSBs with (<b>a</b>) a regular Celgard separator and (<b>b</b>) a PPy-modified separator; cross-section SEM images of Li metal anode of the LSBs with (<b>c</b>) PPy-modified separators and (<b>d</b>) regular Celgard separators after 250 cycles at 0.5 C [<a href="#B85-ijms-25-11446" class="html-bibr">85</a>]. Copyright © 2019, with permission from Elsevier. (<b>e</b>) A schematic of the cell with PPy/ZnO interlayer [<a href="#B86-ijms-25-11446" class="html-bibr">86</a>]. Copyright © 2018, with permission from Springer Nature. (<b>f</b>) Schematic diagram of a PANI-GO interlayer inserted between cathode and separator in LSBs [<a href="#B90-ijms-25-11446" class="html-bibr">90</a>]. Copyright © 2018, with permission from Royal Society of Chemistry. (<b>g</b>) Schematic illustrating the mechanism of the high-performance battery equipped with VOH@PANI-PP separator. (<b>h</b>) Rate performance of the battery equipped with the VOH@PANI-PP separator at different current densities [<a href="#B92-ijms-25-11446" class="html-bibr">92</a>]. Copyright © 2021, with permission from John Wiley and Sons.</p>
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<p>Polymerization scheme of aniline emeraldine salt chains (<b>a</b>); schematic illustration of the MoS<sub>2</sub>/PANi assembly (<b>b</b>) [<a href="#B93-ijms-25-11446" class="html-bibr">93</a>]. Copyright © 2021, with permission from Elsevier. (<b>c</b>) Schematic illustration of the fabrication of RPM and (<b>d</b>) RPM-modified separator for the inhibition and reutilization of LiPSs. (<b>e</b>) Schematic diagram of LiPSs trapping–interception–conversion process on RPM/PP (left) and severe shuttle effect on PP separator (right). (<b>f</b>) Rate performance of the cell with different separators. (<b>g</b>) Cycling performance of the cell with RPM/PP separator at 5 C [<a href="#B94-ijms-25-11446" class="html-bibr">94</a>]. Copyright © 2022, with permission from John Wiley and Sons. (<b>h</b>) Theoretical mechanism of the battery incorporating a PEDOT:PSS-coated separator and a sulfur-infused expanded graphene cathode [<a href="#B100-ijms-25-11446" class="html-bibr">100</a>]. Copyright © 2016, with permission from Royal Society of Chemistry. (<b>i</b>) Preparation of CB/PEDOT:PSS-modified separator [<a href="#B101-ijms-25-11446" class="html-bibr">101</a>]. Copyright © 2019, with permission from John Wiley and Sons.</p>
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<p>(<b>a</b>) The structure of LSB with AAO separator and SEM image of AAO surface. (<b>b</b>) The structure of a LSB with a Celgard separator and SEM image of the surface of the Celgard 2400 [<a href="#B103-ijms-25-11446" class="html-bibr">103</a>]. Copyright © 2020, with permission from American Chemical Society. (<b>c</b>) Schematic illustration of the fabrication process of MnFe<sub>2</sub>O<sub>4</sub> and modifying separator. (<b>d</b>) The cycling performance of the batteries equipped with PP, AB, and MFO-5% separator after 500 cycles at 1 C. (<b>e</b>) The schematic of LSB configured with PP separator. (<b>f</b>) Schematic diagram of LSB with MFO-5%-modified separator configuration [<a href="#B105-ijms-25-11446" class="html-bibr">105</a>]. Copyright © 2020, with permission from Elsevier. (<b>g</b>) Schematic diagram for LLTO@Li-S battery [<a href="#B107-ijms-25-11446" class="html-bibr">107</a>]. Copyright © 2022, with permission from American Chemical Society.</p>
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<p>Various materials used for modification and functionalization of separators.</p>
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9 pages, 2681 KiB  
Communication
A 28/56 Gb/s NRZ/PAM-4 Dual-Mode Transmitter with Eye-Opening Enhancement in 28 nm CMOS
by Jonghyeok Won and Jintae Kim
Electronics 2024, 13(18), 3774; https://doi.org/10.3390/electronics13183774 - 23 Sep 2024
Viewed by 679
Abstract
This paper presents a non-return-to-zero (NRZ)/4-level pulse amplitude modulation (PAM-4) dual-mode wireline transmitter with an eye-opening enhancement technique to improve horizontal eye-opening. With the eye-enhancement pulse generator and the auxiliary pull-up device in the tail-less current-mode driver, the worst-case horizontal eye-opening increased by [...] Read more.
This paper presents a non-return-to-zero (NRZ)/4-level pulse amplitude modulation (PAM-4) dual-mode wireline transmitter with an eye-opening enhancement technique to improve horizontal eye-opening. With the eye-enhancement pulse generator and the auxiliary pull-up device in the tail-less current-mode driver, the worst-case horizontal eye-opening increased by 30% in the PAM-4 eye diagram. The power efficiency of the NRZ mode was also improved by completely turning off the LSB path in the differential data path, resulting in only a 31% power efficiency degradation, which is far lower than that of the prior dual-mode transmitters. Fabricated in 28 nm CMOS, the transmitter achieves power efficiency of 1.4 pJ/bit at 56 Gb/s in PAM-4 mode and 1.84 pJ/bit at 28 Gb/s in NRZ mode, respectively. Full article
(This article belongs to the Section Microelectronics)
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<p>Overall architecture of the transmitter.</p>
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<p>1 UI data and eye-boosting pulse generator, along with its timing diagram.</p>
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<p>Schematic of TSPC flip-flop with programmable reset strength.</p>
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<p>Configuration of the transmitter (half-circuit) when the eye enhancement is: (<b>a</b>) off; and (<b>b</b>) on.</p>
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<p>The simulated rise time of the transmitter output in NRZ mode at three corner cases (TT, SF, FS) when the eye enhancement is: (<b>a</b>) off; and (<b>b</b>) on.</p>
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<p>The mode selector and the differential data path for NRZ/PAM-4 dual-mode operation.</p>
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<p>(<b>a</b>) Die photo; (<b>b</b>) power breakdown of the transmitter; and (<b>c</b>) measurement setup.</p>
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<p>Measurement result of eye diagram when the eye enhancement is (<b>top</b>) off and (<b>bottom</b>) on: (<b>a</b>) at 56 Gb/s PAM-4; and (<b>b</b>) 28 Gb/s NRZ.</p>
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14 pages, 5297 KiB  
Article
Area-Efficient Mixed-Signal Time-to-Digital Converter Integration for Time-Resolved Photon Counting
by Sergio Moreno, Victor Moro, Joan Canals and Angel Diéguez
Sensors 2024, 24(17), 5763; https://doi.org/10.3390/s24175763 - 4 Sep 2024
Viewed by 723
Abstract
Digital histogram generation for time-resolved measurements with single-photon avalanche diode (SPAD) sensors requires the storage of many timestamp signals. This work presents a mixed-signal time-to-digital converter (TDC) that uses analog storage to achieve an area-efficient design that can be integrated in large SPAD [...] Read more.
Digital histogram generation for time-resolved measurements with single-photon avalanche diode (SPAD) sensors requires the storage of many timestamp signals. This work presents a mixed-signal time-to-digital converter (TDC) that uses analog storage to achieve an area-efficient design that can be integrated in large SPAD arrays. Fabricated using a 150 nm CMOS process, the prototype occupies an area of only 18.3 µm × 36.5 µm, a notable size reduction compared to conventional designs. The experimental results demonstrated high performance, with an integral nonlinearity (INL) of 0.35/0.14 least significant bit (LSB) and a differential nonlinearity (DNL) of 0.14/−0.12 LSB. In addition, the proposed TDC can support the construction of histograms comprising up to 512 bins, making it an effective solution to accommodate a wide range of resolution requirements. Validated in a point-of-care (PoC) device for fluorescence lifetime measurements, it distinguished between lifetimes of approximately 4.1 ns, 3.6 ns and 80 ns with the Alexa Fluor (AF) 546 and 568 dyes and Quantum Dot (QD) 705, respectively. The analog storage design and area-efficient architecture offer a novel approach to integrating TDCs in SPAD-based systems, with potential applications in medical diagnostics and beyond. Full article
(This article belongs to the Section Intelligent Sensors)
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<p>Timing diagram of the TDC full operation signals, showing no event detection and random input events during a single measuring period. Block diagram of the TDC chip, which shows the digital circuit blocks and off-chip histogram generation at the bottom. Only the main connections are indicated.</p>
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<p>Schematics of the SPAD and TDC chip readouts. They show the interconnection between the chips and the basic operation timing diagram.</p>
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<p>Step size of analog counter by applying different bias injection values. The dotted black line shows the ideal step size. The vertical lines indicate the resolution expressed in number of loops. Bias<sub>res</sub> was 0.7 V.</p>
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<p>Representation of the injection step size for the purposes of the linearity study.</p>
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<p>Differential nonlinearity (DNL) and integral nonlinearity (INL) of the fine stage using a bias resolution of 1.8 V.</p>
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<p>Characterization of the bin widths for several bias resolution values.</p>
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<p>Cross-sectional view of the PoC device chamber. The laser is aligned with the camera of the SPAD chip. The fluorescence liquid is introduced into the microfluidic tubes of the µ-Slide until the microchannel is filled.</p>
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<p>Simplified view of the measurement process flow.</p>
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<p>Decay times for QD 705, AF 546 and AF568 at a concentration of 1 µM. The application of the Savitzky–Golay filter in the post-processing step proved advantageous for high-resolution signals, enabling more precise measurements despite the intrinsic noise associated with the TDC.</p>
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<p>Decay histograms of the IRF and QD 705 at concentrations ranging from 1 µM to 1/32 µM. For the purpose of ease of visualization, only three concentrations are represented.</p>
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9 pages, 2012 KiB  
Article
Scalable Ni12P5-Coated Carbon Cloth Cathode for Lithium–Sulfur Batteries
by Artur M. Suzanowicz, Thulitha M. Abeywickrama, Hao Lin, Dana Alramahi, Carlo U. Segre and Braja K. Mandal
Energies 2024, 17(17), 4356; https://doi.org/10.3390/en17174356 - 31 Aug 2024
Viewed by 673
Abstract
As a better alternative to lithium-ion batteries (LIBs), lithium–sulfur batteries (LSBs) stand out because of their multi-electron redox reactions and high theoretical specific capacity (1675 mA h g−1). However, the long-term stability of LSBs and their commercialization are significantly compromised by [...] Read more.
As a better alternative to lithium-ion batteries (LIBs), lithium–sulfur batteries (LSBs) stand out because of their multi-electron redox reactions and high theoretical specific capacity (1675 mA h g−1). However, the long-term stability of LSBs and their commercialization are significantly compromised by the inherently irreversible transition of soluble lithium polysulfides (LiPS) into solid short-chain S species (Li2S2 and Li2S) and the resulting substantial density change in S. To address these issues, we used activated carbon cloth (ACC) coated with Ni12P5 as a porous, conductive, and scalable sulfur host material for LSBs. ACC has the benefit of high electrical conductivity, high surface area, and a three-dimensional (3D) porous architecture, allowing for ion transport channels and void spaces for the volume expansion of S upon lithiation. Ni12P5 accelerates the breakdown of Li2S to increase the efficiency of active materials and trap soluble polysulfides. The highly effective Ni12P5 electrocatalyst supported on ACC drastically reduced the severity of the LiPS shuttle, affected the abundance of adsorption–diffusion–conversion interfaces, and demonstrated outstanding performance. Our cells achieved near theoretical capacity (>1611 mA h g−1) during initial cycling and superior capacity retention (87%) for >250 cycles following stabilization with a 0.05% decay rate per cycle at 0.2 C. Full article
(This article belongs to the Section D2: Electrochem: Batteries, Fuel Cells, Capacitors)
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<p>Synthetic scheme for S@ACC@Ni<sub>12</sub>P<sub>5</sub>.</p>
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<p>SEM images of (<b>A</b>) activated carbon cloth (ACC), (<b>B</b>) ACC@Ni(OH)<sub>2</sub>, and (<b>C</b>) ACC@Ni<sub>12</sub>P<sub>5</sub>.</p>
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<p>X-ray diffraction (XRD) patterns for ACC@Ni(OH)<sub>2</sub> (shown in blue) and ACC@Ni<sub>12</sub>P<sub>5</sub> (shown in red).</p>
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<p>Long-term discharge capacity and Coulombic efficiency of S@ACC@Ni<sub>12</sub>P<sub>5</sub> at 0.2 C for 350 cycles.</p>
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<p>Rate capabilities of S@ACC@Ni<sub>12</sub>P<sub>5</sub> at different rates.</p>
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13 pages, 1499 KiB  
Article
Aqua Extracts of Lyophilized Sea Buckthorn Modify Fermentation and Quality Properties of Set-Type Yogurt
by Aikaterini Silyvridou, Anastasia Bari, Theodora Georgopoulou, Catherine Baxevanou and Persephoni Giannouli
Appl. Sci. 2024, 14(17), 7634; https://doi.org/10.3390/app14177634 - 29 Aug 2024
Viewed by 691
Abstract
Sea buckthorn is a promising ingredient for the food industry because it is a good source of vitamins, polyphenols, phytosterols, etc. In this research, it is the first time that aqueous extracts of lyophilized sea buckthorn (LSB) 0%, 0.5%, 1%, 2%, and 3% [...] Read more.
Sea buckthorn is a promising ingredient for the food industry because it is a good source of vitamins, polyphenols, phytosterols, etc. In this research, it is the first time that aqueous extracts of lyophilized sea buckthorn (LSB) 0%, 0.5%, 1%, 2%, and 3% w/w were used to enrich set-type yogurts. Therefore, fermentation kinetics, hardness, color, titratable acidity, syneresis, water holding capacity, total phenolic content microstructure, and sensory analysis were investigated. Extracts of lyophilized sea buckthorn shorten the yogurt fermentation time, change the microstructure, reduce syneresis, and increase water-holding capacity compared to plain yogurt. Also, the titratable acidity for all yogurts remained the same but the total phenolic content of yogurts increased as the concentration of extracts from lyophilized sea buckthorn increased. The color parameters of the fortified set-type yogurts were affected by the color of the sea buckthorn extract with increasing a* and b* values according to extract concentrations. Finally, yogurts fortified with 0.5% and 1.0% w/w extracts of LSB have good quality characteristics, increased total phenolic content, and higher scores of being liked compared to the rest of the enriched samples. This study could increase the knowledge of the uses of aqueous extracts of lyophilized sea buckthorn in dairy products. Full article
(This article belongs to the Special Issue Enrichment of Foods with Phytonutrients)
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<p>Titratable acidity (%) of set-type yogurts containing 0, 0.5, 1, 2, and 3% <span class="html-italic">w</span>/<span class="html-italic">w</span> extracts of lyophilized sea buckthorn. Different letters within the columns indicate significant differences (<span class="html-italic">p</span> &lt; 0.05) among the different treatments. All measurements were conducted in triplicate.</p>
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<p>Water holding capacity and syneresis of set-type yogurts containing 0, 0.5, 1, 2, and 3% <span class="html-italic">w</span>/<span class="html-italic">w</span> extracts of lyophilized sea buckthorn. Black columns indicate water holding capacity values (%); white columns indicate syneresis values (%). Different letters within the columns indicate significant differences (<span class="html-italic">p</span> &lt; 0.05) among the different treatments. All measurements were conducted in triplicate.</p>
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<p>Total phenolic content (mg GAE/100 g) of set-type yogurts containing 0, 0.5, 1, 2, and 3% <span class="html-italic">w</span>/<span class="html-italic">w</span> extracts of lyophilized sea buckthorn. Different letters within the columns indicate significant differences (<span class="html-italic">p</span> &lt; 0.05) among the different treatments. All measurements were conducted in triplicate.</p>
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<p>Hardness (N) of set-type yogurts containing 0, 0.5, 1, 2, and 3% <span class="html-italic">w</span>/<span class="html-italic">w</span> extracts of lyophilized sea buckthorn. Different letters within the columns indicate significant differences (<span class="html-italic">p</span> &lt; 0.05) among the different treatments. All measurements were conducted in triplicate.</p>
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<p>Microscopic images of set-type yogurt after a day of storage at 4 °C, containing 0, 0.5, 1, 2, and 3% <span class="html-italic">w</span>/<span class="html-italic">w</span> extracts of lyophilized sea buckthorn. The black scale bar represents 200 μm. (<b>A</b>) Yogurt sample with 0% <span class="html-italic">w</span>/<span class="html-italic">w</span> extract of lyophilized sea buckthorn; (<b>B</b>) yogurt sample with 0.5% <span class="html-italic">w</span>/<span class="html-italic">w</span> extract of lyophilized sea buckthorn; (<b>C</b>) yogurt sample with 1% <span class="html-italic">w</span>/<span class="html-italic">w</span> lyophilized sea buckthorn extract; (<b>D</b>) yogurt sample with 2% <span class="html-italic">w</span>/<span class="html-italic">w</span> extract of lyophilized sea buckthorn; (<b>E</b>) yogurt sample with 3% <span class="html-italic">w</span>/<span class="html-italic">w</span> extract of lyophilized sea buckthorn.</p>
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14 pages, 3115 KiB  
Article
Addition of a Polar, Porous Phase-Inversion-PVDF Membrane to Lithium–Sulfur Cells (LSBs) Already with a Microporous Polypropylene Separator Enhances the Battery Performance
by Irshad Mohammad, Luke D. J. Barter, Carol Crean and Robert C. T. Slade
Batteries 2024, 10(8), 293; https://doi.org/10.3390/batteries10080293 - 21 Aug 2024
Viewed by 1471
Abstract
Lithium–sulfur batteries (LSBs) are widely studied as an alternative to lithium-ion batteries, this emphasis being due to their high theoretical energy density and low cost, and to the high natural abundance of sulfur. Lithium polysulfide shuttling and lithium dendrite growth have limited their [...] Read more.
Lithium–sulfur batteries (LSBs) are widely studied as an alternative to lithium-ion batteries, this emphasis being due to their high theoretical energy density and low cost, and to the high natural abundance of sulfur. Lithium polysulfide shuttling and lithium dendrite growth have limited their commercialization. Porous polyvinylidene fluoride (PVDF) separators have shown improved performance (relative to hydrocarbon separators) in lithium-ion batteries due to faster lithium-ion migration and higher Li+ transference number. A thin polar PVDF membrane has now been fabricated via phase inversion (an immersion-precipitation method) yielding a β (polar) phase concentration of 72%. Preparation from commercial PVDF used dimethylformamide (DMF) solvent at the optimized crystallizing temperature of 70 °C, and pores in the membrane were generated by exchange of DMF with deionized water as non-solvent. The polar PVDF film produced has the advantages of being ultrathin (15 µm), lightweight (1.15 mg cm−2), of high porosity (75%) and high wettability (84%), and it shows enhanced thermal stability relative to polypropylene (PP). The porous, polar PVDF membrane was combined with a commercially available PP membrane to give a hybrid, two-layer, separator combination for LSBs. A synergy was created in the two-layer separator, providing high sulfur utilization and curbing polysulfide shuttling. The electrochemical performance with the hybrid separator (PP–β-PVDF) was evaluated in LSB cells and showed good cyclability and rate capability: those LSB cells showed a stable capacity of 750 mA h g−1 after 100 cycles at 0.1 C, much higher than that for otherwise-identical cells using a commercial PP-only separator (480 mA h g−1). Full article
(This article belongs to the Special Issue Energy-Dense Metal–Sulfur Batteries)
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<p>SEM images of the surface of β-PVDF membrane (<b>a</b>,<b>b</b>) prepared by phase inversion and of commercial PP membranes (<b>c</b>,<b>d</b>). The red-circled regions are discussed in the text.</p>
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<p>(<b>a</b>) Raman and (<b>b</b>) FTIR spectra of β-PVDF film (<b>top spectra</b>) and of commercial PVDF powder (<b>bottom spectra</b>). (<b>c</b>) Digital photographs of <span class="html-italic">β</span>-PVDF and PP membranes before and after heating (the latter at 150 °C, 1 h). (<b>d</b>) Electrolyte uptake percentage versus time curves for <span class="html-italic">β</span>-PVDF and PP membranes. (<b>e</b>) Contact angle test results as a function of time; electrolyte drops were placed on the surface of the β-PVDF (<b>top row</b>) and PP (<b>bottom row</b>) membranes.</p>
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<p>Color testing of polysulfide-crossover at increasing permeation times with PP separator (top layer) and with PP–β-PVDF (bottom layer) separator.</p>
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<p>Electrochemical tests on an LSB cell incorporating a hybrid PP–β-PVDF separator: (<b>a</b>) CV traces for the first five cycles; (<b>b</b>) CV traces at various voltage scan rates; C1 and A1 are the first cathodic and anodic peak currents, respectively; (<b>c</b>) corresponding linearized fits of the peak currents as a function of scan rate; (<b>d</b>) initial charge–discharge curves of Li-S batteries with PP and PP–β-PVDF separators at 0.05 C.</p>
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<p>Electrochemical investigation of LSB cells: (<b>a</b>) the first four discharge–charge voltage curves with PP–β-PVDF separator; (<b>b</b>) the first four discharge–charge voltage curves with PP-only separator; (<b>c</b>) comparison of galvanostatic cycling performance at 0.1 C with PP–β-PVDF separator with that for PP-only separator; (<b>d</b>) rate performance at various currents for cells with PP–β-PVDF.</p>
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<p>Nyquist plots of cell with PP–β-PVDF separator (<b>a</b>) before and (<b>b</b>) after 100 cycles. Before cycling, the components of the equivalent circuit are: R1 = electrolyte resistance, R2 and CPE2 are resistance and constant phase element for the charge-transfer process, R3 and CPE3 are related to intercalation of Li<sup>+</sup>. After cycling, the components are: R1 = electrolyte resistance, R2 and CPE2 are related to the solid electrolyte interphase, R3 and CPE3 are associated with the charge-transfer process, and R4 and CPE3 are related to intercalation of Li<sup>+</sup>.</p>
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13 pages, 3050 KiB  
Article
Boosting the Performance of Lithium-Sulfur Batteries with PY−DHBD−COF-Enhanced Separators
by Hong He, Wei Wang and Xiaobei Guo
Inorganics 2024, 12(8), 218; https://doi.org/10.3390/inorganics12080218 - 14 Aug 2024
Viewed by 791
Abstract
Lithium–sulfur batteries (LSBs) hold promise for use in next-generation high-energy-density energy storage systems. However, the commercial application of LSBs is hindered by the shuttle effect of polysulfides. In this study, we synthesized a covalent organic framework material (PY−DHBD−COF) and employed it to modify [...] Read more.
Lithium–sulfur batteries (LSBs) hold promise for use in next-generation high-energy-density energy storage systems. However, the commercial application of LSBs is hindered by the shuttle effect of polysulfides. In this study, we synthesized a covalent organic framework material (PY−DHBD−COF) and employed it to modify the separators of LSBs in order to buffer the shuttle effect of polysulfides. A modified separator, involving PY−DHBD−COF coating of the commercial Celgard 2500 PP separator, is prepared via a vacuum-assisted self-assembly method. The PY−DHBD−COF features hydroxyl and imine bonds, which can adsorb lithium polysulfides (LiPSs) and buffer the shuttle effect. The PY−DHBD−COF coating exhibits a thin thickness and oriented nanochannels, facilitating electrolyte wetting and Li+ transport. As a result, the LSBs with PY−DHBD−COF-modified separators exhibit a high specific capacity of 373 mAh g−1 at 4 C with only 0.005% capacity decay per cycle after 450 cycles at 2 C, demonstrating an excellent cycling performance. Full article
(This article belongs to the Section Inorganic Materials)
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<p>The synthesis of PY−DHBD−COF by 2,2′-bipyridine-5,5′-dicarbaldehyde and 4,4′,4″,4‴-(pyrene-1,3,6,8-tetrayl) tetraaniline and the top view of the relaxed structure.</p>
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<p>(<b>a</b>) Stacking unit cell structure of PY−DHBD−COF. (<b>b</b>) Fourier transform infrared (FT−IR) spectrum of PY−DHBD−COF. (<b>c</b>) Experimental and simulated PXRD patterns of PY−DHBD−COF. (<b>d</b>) SEM images and the corresponding elemental mapping images of PY−DHBD−COF. (<b>e</b>) C 1s and (<b>f</b>) N 1s XPS spectra of PY−DHBD−COF.</p>
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<p>Optical images and contact angles with the electrolytes of (<b>a</b>) the PY−DHBD−COF-modified separator and (<b>d</b>) the bare Celgard 2500 PP separator. Top-view SEM images of (<b>b</b>) the PY−DHBD−COF-modified separator and (<b>e</b>) the bare Celgard 2500 PP separator. Cross-sectional SEM images of (<b>c</b>) the PY−DHBD−COF-modified separator and (<b>f</b>) the bare Celgard 2500 PP separator.</p>
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<p>(<b>a</b>) Optical pictures of Li<sub>2</sub>S<sub>6</sub> adsorption experiments and corresponding UV-vis spectra of Li<sub>2</sub>S<sub>6</sub> solution after adsorption. (<b>b</b>) Polysulfide diffusions in H-type cells based on different separators. (<b>c</b>) CV curves and (<b>d</b>) chronoamperometric curves of different symmetric cells. (<b>e</b>) Potentiostatic discharge profiles of Li<sub>2</sub>S<sub>8</sub> solution at 2.05 V on (<b>e</b>) PY−DHBD−COF and (<b>f</b>) control (Super P) electrodes.</p>
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<p>(<b>a</b>) CV curves of LSBs based on different separators at 0.1 mV s<sup>−1</sup> sweep speed. (<b>b)</b> Charge and discharge voltage curve at 0.1 C current and (<b>c</b>) corresponding median-capacity voltage polarization and capacity comparison of two discharge plateaus at 0.1 C (Q<sub>H</sub> stands for high plateau, Q<sub>L</sub> stands for low plateau). (<b>d</b>) Rate performance of LSBs with different separators at current density ranging from 0.1 C to 4 C. (<b>e</b>) Cycling stability of LSBs with different separators at a rate of 0.2 C. (<b>f</b>) Long-cycle life tests of LSBs with different separators at a rate of 2 C (activated at 0.1 C in the first 5 cycles). (<b>g</b>) Self-discharge test (0.2 C cycle to the 10th cycle start; stand 72 h; continue cycle). (<b>h</b>) Comparison of capacity changes after 3 days of standing (from 10th to 12th turn of the voltage curve color from dark to light, where 11th turn is dotted line).</p>
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<p>CV profiles at different scan rates with (<b>a</b>) PY−DHBD−COF-modified separators and (<b>b</b>) PP separator-based LSBs. Plot of peak current versus square root of scan speed (v<sup>1/2</sup>) for different separator-based LSBs at (<b>c</b>) oxidative peak A, (<b>d</b>) reductive peak C1, and (<b>e</b>) reductive peak C2, with dashed lines indicating the fitted results. (<b>f</b>) D<sub>Li+,</sub> calculated by the linear relationship between peak current and square root of scan rates.</p>
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21 pages, 13609 KiB  
Article
Image-to-Image Steganography with Josephus Permutation and Least Significant Bit (LSB) 3-3-2 Embedding
by Muhammad Rafly Yanuar, Suryadi MT, Catur Apriono and Muhammad Firdaus Syawaludin
Appl. Sci. 2024, 14(16), 7119; https://doi.org/10.3390/app14167119 - 14 Aug 2024
Viewed by 992
Abstract
In digital image security, the Josephus permutation is widely used in cryptography to enhance randomness. However, its application in steganography is underexplored. This study introduces a novel method integrating the Josephus permutation into the LSB 3-3-2 embedding technique for image steganography. This approach [...] Read more.
In digital image security, the Josephus permutation is widely used in cryptography to enhance randomness. However, its application in steganography is underexplored. This study introduces a novel method integrating the Josephus permutation into the LSB 3-3-2 embedding technique for image steganography. This approach improves the randomness of the keystream generated by the chaotic logistic map, addressing vulnerabilities in basic logistic maps susceptible to steganalysis. Our algorithm is tested on RGB images as secret data, presenting higher complexity compared to grayscale images used in previous studies. Comparative analysis shows that the proposed algorithm offers higher payload capacity while maintaining image quality, outperforming traditional LSB techniques. This research advances the field of image steganography by demonstrating the effectiveness of the Josephus permutation in creating more secure and robust steganographic images. Full article
(This article belongs to the Special Issue Information Security and Cryptography)
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<p>Josephus permutation of the number sequence 1, 2, 3, 4, 5 with a fixed key of one produces a new sequence 2, 4, 1, 5, 3.</p>
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<p>The embedding (<b>a</b>) and extraction algorithm (<b>b</b>).</p>
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<p>Lyapunov exponent graph of the logistic map growth rate for the range <math display="inline"><semantics> <mrow> <mn>0</mn> <mo>≤</mo> <mi>r</mi> <mo>≤</mo> <mn>4</mn> </mrow> </semantics></math>.</p>
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<p>Bifurcation diagram of the logistic map growth rate for the range <math display="inline"><semantics> <mrow> <mn>0</mn> <mo>≤</mo> <mi>r</mi> <mo>≤</mo> <mn>4</mn> </mrow> </semantics></math>.</p>
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<p>Time graph of keystream calculation with precision levels from 16 digits to 60 digits for a secret image of size 512 × 512 pixels.</p>
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<p>Keystream generation using logistic map.</p>
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<p>(<b>a</b>) Red channel of a pixel in the secret image, (<b>b</b>) composition of an RGB pixel in the cover image, (<b>c</b>) new RGB pixel resulting from embedding (<b>a</b>) into (<b>b</b>) using LSB 3-3-2.</p>
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<p>MSE and PSNR values for brute force experiment.</p>
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13 pages, 5484 KiB  
Article
A 14-Bit Digital to Analog Converter for a Topmetal-CEE Pixel Readout Chip
by Yunqi Deng, Ping Yang, Guangming Huang, Jun Liu, Zhongguang Ren, Yan Fan and Zixuan Song
Electronics 2024, 13(15), 3074; https://doi.org/10.3390/electronics13153074 - 3 Aug 2024
Viewed by 738
Abstract
The Lanzhou Heavy Ion Research Facility (LIRF) is the largest heavy ion research facility in China, providing a substantial volume of experimental data for fundamental research in nuclear physics. The Topmetal-CEE is a pixel readout chip specifically designed for tracking detectors. Within the [...] Read more.
The Lanzhou Heavy Ion Research Facility (LIRF) is the largest heavy ion research facility in China, providing a substantial volume of experimental data for fundamental research in nuclear physics. The Topmetal-CEE is a pixel readout chip specifically designed for tracking detectors. Within the Topmetal-CEE framework, the front-end amplifier and comparator necessitate precisely adjustable bias voltages. Hence, in this paper, a 14-bit resolution DAC with an R-2R resistor network structure is designed, along with an amplifier featuring high driving capabilities as the DAC driver, thus preventing potential impedance issues when driving large pixel arrays. Test results demonstrate that the DAC module, operating under a 3.3 V supply voltage, can consistently output voltages ranging from 0 to 1.8 V. Furthermore, the differential non-linearity error is less than 1.07 LSB, and the integral non-linearity error is less than 1.57 LSB. Full article
(This article belongs to the Special Issue Machine Learning in Network-on-Chip Architectures)
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<p>Topmetal-CEE chip architecture block diagram.</p>
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<p>Binary-weighted resistive DAC diagram.</p>
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<p>The segmented DAC structure diagram.</p>
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<p>The schematic of the proposed DAC overall structure diagram.</p>
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<p>The schematic of the proposed bandgap.</p>
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<p>Structure of the proposed R-2R resistor network.</p>
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<p>ACBC three-stage amplifier schematic.</p>
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<p>ACBC three-stage amplifier structure.</p>
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<p>Simulation results of reference voltage at TT, SS, and FF process corners.</p>
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<p>Simulation results of operational amplifier gain.</p>
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<p>(<b>a</b>) DNL analysis results for post-simulation of DAC; (<b>b</b>) INL analysis results for post-simulation of DAC.</p>
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<p>(<b>a</b>) Die micrograph of the Topmetal_CEE; (<b>b</b>) die micrograph of the DAC; (<b>c</b>) layout of the DAC.</p>
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<p>(<b>a</b>) DNL analysis of DAC test results; (<b>b</b>) INL analysis of DAC test results.</p>
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14 pages, 1734 KiB  
Article
Rotorcraft Airfoil Performance in Martian Environment
by Enrico Giacomini and Lars-Göran Westerberg
Aerospace 2024, 11(8), 628; https://doi.org/10.3390/aerospace11080628 - 1 Aug 2024
Viewed by 860
Abstract
In 2021, the Ingenuity helicopter performed the inaugural flight on Mars, heralding a new epoch of exploration. However, the aerodynamics on Mars present unique challenges not found on Earth, such as low chord-based Reynolds number flows, which pose significant hurdles for future missions. [...] Read more.
In 2021, the Ingenuity helicopter performed the inaugural flight on Mars, heralding a new epoch of exploration. However, the aerodynamics on Mars present unique challenges not found on Earth, such as low chord-based Reynolds number flows, which pose significant hurdles for future missions. The Ingenuity’s design incorporated a Reynolds number of approximately 20,000, dictated by the rotor’s dimensions. This paper investigates the implications of flows at a Reynolds number of 50,000, conducting a comparative analysis with those at 20,000 Re. The objective is to evaluate the feasibility of using larger rotor dimensions or extended airfoil chord lengths. An increase in the Reynolds number alters the size and position of Laminar Separation Bubbles (LSBs) on the airfoil, significantly impacting performance. This study leverages previous research on the structure and dynamics of LSBs to examine the flow around a cambered plate with 6% camber and 1% thickness in Martian conditions. This paper details the methods and mesh used for analysis, assesses airfoil performance, and provides a thorough explanation of the results obtained. Full article
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<p>Maximum Lift-to-drag ratio vs. Reynolds number [<a href="#B5-aerospace-11-00628" class="html-bibr">5</a>].</p>
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<p>Different views of the mesh. (<b>a</b>) Mesh dimensions and boundaries. (<b>b</b>) Mesh grid. (<b>c</b>) Close-up of the mesh near the airfoil.</p>
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<p>Comparison of pressure coefficient distribution for three different mesh resolutions at 0 degrees (Re = 20,000): (<b>a</b>) 300 k elements; (<b>b</b>) 400 k elements; (<b>c</b>) 500 k elements.</p>
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<p>(<b>a</b>) Laminar Separation Bubble (LSB) on an airfoil surface, highlighting different regions [<a href="#B29-aerospace-11-00628" class="html-bibr">29</a>]. (<b>b</b>) Pressure coefficient distribution on an airfoil with and without an LSB [<a href="#B30-aerospace-11-00628" class="html-bibr">30</a>].</p>
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<p>Velocity profiles in <math display="inline"><semantics> <mrow> <mi mathvariant="normal">m</mi> <mo>/</mo> <mi mathvariant="normal">s</mi> </mrow> </semantics></math> for (<b>a</b>) −3°, (<b>b</b>) 0°, (<b>c</b>) 6°, and (<b>d</b>) 8° angles of attack with travel of separation bubble with Re = 20,000.</p>
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<p>Velocity profiles in <math display="inline"><semantics> <mrow> <mi mathvariant="normal">m</mi> <mo>/</mo> <mi mathvariant="normal">s</mi> </mrow> </semantics></math> for (<b>a</b>) −3°, (<b>b</b>) 0°, (<b>c</b>) 6°, and (<b>d</b>) 8° angles of attack with travel of separation bubble with Re = 50,000.</p>
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<p>(<b>a</b>) Laminar separation (LS) and turbulent reattachment (TR) positions (<b>b</b>) and LSB extension for 20,000 and 50,000 Re on the suction surface.</p>
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<p>(<b>a</b>) Laminar separation (LS) and turbulent reattachment (TR) positions (<b>b</b>) and LSB extension for 20,000 and 50,000 Re on the pressure surface.</p>
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<p>Skin fraction coefficient distribution for (<b>a</b>) 0° at 20,000 and (<b>b</b>) 8° at 50,000 Re.</p>
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<p>(<b>a</b>) Lift coefficient with respect to the angle of attack. (<b>b</b>) Drag coefficient with respect to the angle of attack. (<b>c</b>) Lift-to-drag ratio with respect to the angle of attack. (<b>d</b>) Drag coefficient with respect to the lift coefficient.</p>
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