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18 pages, 1211 KiB  
Article
Structural Optimization Based on Response Surface Methodology for the Venturi Injector Used in Fertigation System
by Pan Tang and Zhizhong Zhang
Horticulturae 2025, 11(2), 223; https://doi.org/10.3390/horticulturae11020223 (registering DOI) - 19 Feb 2025
Abstract
To enhance the hydraulic performance of the Venturi injector, the effects of the structural parameters were investigated using response surface methodology (RSM) and computational fluid dynamics (CFD) simulations. The fertilizer suction chamber diameter, contraction angle, and throat diameter ratio were chosen as variables, [...] Read more.
To enhance the hydraulic performance of the Venturi injector, the effects of the structural parameters were investigated using response surface methodology (RSM) and computational fluid dynamics (CFD) simulations. The fertilizer suction chamber diameter, contraction angle, and throat diameter ratio were chosen as variables, while the suction flow rate, suction concentration, and suction efficiency were selected as performance indicators. Multiple regression models were established, and the regression models were used for parameter optimization and experimental verification. The results showed that under the same inlet-outlet differential pressure, with the increase in the fertilizer suction chamber diameter, contraction angle, and throat diameter ratio, the suction flow rate, suction concentration, and suction efficiency showed a trend of first increasing and then decreasing, and there were peaks in suction performance. Predictive regression equations were established for the suction flow rate, concentration, and efficiency within the experimental parameter range. The determination coefficients of the three regression equations were 0.9987, 0.9961, and 0.9990, respectively, which indicated that the established regression equations could be used for performance prediction. The optimized combination of structural parameters included a fertilizer suction chamber diameter of 32 mm, a contraction angle of 35°, and a throat diameter ratio of 2.93. The error between the predicted and experimental values was less than 3%, indicating a high level of reliability in the predictive regression model. The performance indicators of the optimized Venturi injector were significantly improved, with an increase of 124.1~793.7 L h−1 in the suction flow rate, 9.52~16.42 percentage points in suction concentration, and 5.4~9.19 percentage points in suction efficiency. Full article
15 pages, 4231 KiB  
Article
Microstructure and Release Behavior of Alginate–Natural Hydrocolloid Composites: A Comparative Study
by Hatice Sıçramaz, Ali Baran Dönmez, Buse Güven, Derya Ünal and Elif Aşbay
Polymers 2025, 17(4), 531; https://doi.org/10.3390/polym17040531 - 18 Feb 2025
Viewed by 121
Abstract
This study investigated the effects of combining sodium alginate (ALG) with various natural hydrocolloids on the microstructure and release behaviors of microbeads. The encapsulation solutions were prepared at a 1:1 (w/w) ratio with ALG as the control and carrageenan [...] Read more.
This study investigated the effects of combining sodium alginate (ALG) with various natural hydrocolloids on the microstructure and release behaviors of microbeads. The encapsulation solutions were prepared at a 1:1 (w/w) ratio with ALG as the control and carrageenan (CAR), locust bean gum (LBG), acacia gum (ACA), pectin (PEC), and carboxymethyl cellulose (CMC) as experimental groups. Each formulation contained 0.2% (w/v) tartrazine and was extruded into a CaCl2 solution for bead production. Encapsulation efficiency varied across formulations, with the lowest in the control (ALG-ALG) and highest in ALG-CAR and ALG-CMC, reaching 74% and 78%, respectively. The microbead sizes ranged from 2.07 to 3.48 mm, with the lowest particle diameter observed in ALG-ACA composites. Surface analysis showed smooth and uniform microbeads in the control (ALG-ALG), while ALG-LBG microbeads were rougher. Release kinetics were assessed using various models, with the Higuchi model best describing the release for most formulations (highest R2 values). Tartrazine release followed pseudo-Fickian behavior in all formulations, with slower release in ALG-ACA and faster release in ALG-LBG microbeads. This study fills a gap in understanding how the incorporation of different natural hydrocolloids influences both the encapsulation efficiency and release dynamics of alginate-based microbeads, providing valuable insights for applications in food and pharmaceutical industries. Full article
(This article belongs to the Special Issue Development of Polymer Materials as Functional Coatings)
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<p>The optical microscopic images of alginate microparticles at a magnification of 4×.</p>
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<p>SEM images of microbeads at (<b>a</b>) 100× (except ALG-ACA, which was monitored at 250×), (<b>b</b>) 2000×, (<b>c</b>) 8000×.</p>
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<p>SEM images of microbeads at (<b>a</b>) 100× (except ALG-ACA, which was monitored at 250×), (<b>b</b>) 2000×, (<b>c</b>) 8000×.</p>
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<p>FTIR spectra of microbeads at (<b>a</b>) 1500–3900 and (<b>b</b>) 500–1500 cm<sup>−1</sup>.</p>
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<p>Chemical structure of tartrazine.</p>
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<p>DSC curves of microbeads.</p>
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<p>Encapsulation efficiencies (EEs%) of microbeads. Different letters “a–c” represent statistical differences according to Tukey’s test (<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Release profiles of tartrazine from microbeads.</p>
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25 pages, 8959 KiB  
Article
Numerical Analysis of the Characteristic Chemical Timescale of a C2H4/O2 Non-Premixed Rotating Detonation Engine
by Mohammed Niyasdeen Nejaamtheen, Bu-Kyeng Sung and Jeong-Yeol Choi
Energies 2025, 18(4), 989; https://doi.org/10.3390/en18040989 - 18 Feb 2025
Viewed by 146
Abstract
A three-dimensional numerical investigation using ethylene–oxygen was conducted to examine the characteristics of detonation waves in a non-premixed rotating detonation engine (RDE) across three equivalence ratio conditions: fuel-lean, stoichiometric, and fuel-rich. The study aims to identify the distinct timescales associated with detonation wave [...] Read more.
A three-dimensional numerical investigation using ethylene–oxygen was conducted to examine the characteristics of detonation waves in a non-premixed rotating detonation engine (RDE) across three equivalence ratio conditions: fuel-lean, stoichiometric, and fuel-rich. The study aims to identify the distinct timescales associated with detonation wave propagation within the combustor and to analyze their impact on detonation wave behavior, emphasizing the influence of equivalence ratio and injector behavior on detonation wave characteristics. The results indicate that the wave behavior varies with mixture concentration, with the ethylene injector demonstrating greater stiffness compared to the oxygen injector. In lean mixtures, characterized by excess oxidizer, waves exhibit less intensity and slower progression toward equilibrium, resulting in prolonged reaction times. Rich mixtures, with excess fuel, also show a delayed approach to equilibrium and an extended chemical reaction timescale. In contrast, the near-stoichiometric mixture achieves efficient combustion with the highest thermicity, rapidly reaching equilibrium and exhibiting the shortest chemical reaction timescale. Overall, the induction timescale is generally 2–3 times longer than its respective chemical reaction timescale, while the equilibrium timescale spans a broad range, reflecting the complex, rapid dynamics inherent in these chemical processes. This study identifies the role of the characteristic chemical timescale in influencing the progression of pre-detonation deflagration in practical RDEs. Prolonged induction times in non-ideal conditions, such as those arising from equivalence ratio variations, promote incomplete reactions, thereby contributing to pre-detonation phenomena and advancing our understanding of the underlying flow physics. Full article
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Figure 1
<p>(<b>a</b>) An ideal ZND wave structure with different shaded regions representing combustion (red), product expansion (yellow), injection (green), and mixing (blue). (<b>b</b>) Description of the primary timescale associated with a typical RDE [<a href="#B16-energies-18-00989" class="html-bibr">16</a>].</p>
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<p>The ideal ZND detonation structure for a C<sub>2</sub>H<sub>4</sub>/O<sub>2</sub> mixture at an ϕ of 1.0 and initial p of 1 atm, showing the normalized temporal evolutions of (<b>a</b>) <span class="html-italic">p</span> and <span class="html-italic">T</span>, and (<b>b</b>) <span class="html-italic">Y<sub>s</sub></span>.</p>
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<p>Comparison of ignition delay times with experimental and analytical results.</p>
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<p>(<b>a</b>) 2D computational domain for planar detonation. (<b>b</b>) Cell structure predicted by the current solver and (<b>c</b>) by Wang et al. [<a href="#B36-energies-18-00989" class="html-bibr">36</a>].</p>
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<p>Comparison of cell width with varying initial <span class="html-italic">p</span> by the present solver and Strehlow et al. [<a href="#B35-energies-18-00989" class="html-bibr">35</a>].</p>
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<p>(<b>a</b>) The computational geometry; (<b>b</b>) computational mesh in the near-injector region; (<b>c</b>) a close-up view of the inlets; and (<b>d</b>) two-injector multi-block grid system for RDE.</p>
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<p>(<b>a</b>) Probe data illustrating the temporal evolution of <span class="html-italic">p</span> and <span class="html-italic">T</span> profiles, and (<b>b</b>) error convergence of p<sub>VN</sub> and ω with grid sizing.</p>
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<p>Instantaneous p field of the RDE using different resolution meshes: (<b>a</b>) coarse, (<b>b</b>) base, (<b>c</b>) fine, and (<b>d</b>) very fine mesh cases.</p>
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<p>Three-dimensional view of a single anti-clockwise detonation wave under steady-state operation, highlighting the injection process. The illustrated isocontours are colored by pressure. The nomenclatures are (a) detonation wave, (b) moving direction, (c) discrete C<sub>2</sub>H<sub>4</sub> injector, (d) slit O<sub>2</sub> injector, and (e) unburned pockets.</p>
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<p>Instantaneous <span class="html-italic">p</span> field with different case studies; fuel-lean, near-stoichiometric, and fuel-rich. Outer wall (<b>left-column</b>), mid-channel (<b>middle-column</b>), and a cutting plane (<b>right-column</b>).</p>
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<p>Comparison of outer body wall pressure along the RDE length.</p>
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<p>2D line diagram depicting the locations of axial–azimuthal slices.</p>
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<p>Instantaneous Y<sub>O2</sub> mixture along the axial–azimuthal slices: (1) pre-detonation, (2) at the detonation front, and (3) post-detonation for (<b>left</b>) fuel-lean mixture, (<b>middle</b>) near-stoichiometric mixture, and (<b>right</b>) fuel-rich mixture.</p>
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<p>Variation in injection parameters showing (<b>a</b>) U<sub>C2H4</sub>, (<b>b</b>) U<sub>O2</sub>, (<b>c</b>) p<sub>C2H4</sub>, (<b>d</b>) p<sub>O2</sub>, (<b>e</b>) Y<sub>C2H4</sub>, and (<b>f</b>) Y<sub>O2</sub> with cycle-averaged time for (<b>left-column</b>) fuel and (<b>right-column</b>) oxidizer.</p>
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<p>Variation in τ<sub>rxn.</sub> plot across different ϕ.</p>
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<p>Variation in τ<sub>ind.</sub> plot across different ϕ.</p>
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<p>Variation in τ<sub>eq.</sub> for (<b>a</b>) Y<sub>OH</sub>, (<b>b</b>) Y<sub>CO</sub>, (<b>c</b>) Y<sub>C2H4</sub>, and (<b>d</b>) Y<sub>O2</sub> across different ϕ, ranging from lean to rich mixtures.</p>
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13 pages, 3960 KiB  
Article
Vestibular Testing Results in a World-Famous Tightrope Walker
by Alexander A. Tarnutzer, Fausto Romano, Nina Feddermann-Demont, Urs Scheifele, Marco Piccirelli, Giovanni Bertolini, Jürg Kesselring and Dominik Straumann
Clin. Transl. Neurosci. 2025, 9(1), 9; https://doi.org/10.3390/ctn9010009 - 17 Feb 2025
Viewed by 188
Abstract
Purpose: Accurate and precise navigation in space and postural stability rely on the central integration of multisensory input (vestibular, proprioceptive, visual), weighted according to its reliability, to continuously update the internal estimate of the direction of gravity. In this study, we examined both [...] Read more.
Purpose: Accurate and precise navigation in space and postural stability rely on the central integration of multisensory input (vestibular, proprioceptive, visual), weighted according to its reliability, to continuously update the internal estimate of the direction of gravity. In this study, we examined both peripheral and central vestibular functions in a world-renowned 53-year-old male tightrope walker and investigated the extent to which his exceptional performance was reflected in our findings. Methods: Comprehensive assessments were conducted, including semicircular canal function tests (caloric irrigation, rotatory-chair testing, video head impulse testing of all six canals, dynamic visual acuity) and otolith function evaluations (subjective visual vertical, fundus photography, ocular/cervical vestibular-evoked myogenic potentials [oVEMPs/cVEMPs]). Additionally, static and dynamic posturography, as well as video-oculography (smooth-pursuit eye movements, saccades, nystagmus testing), were performed. The participant’s results were compared to established normative values. High-resolution diffusion tensor magnetic resonance imaging (DT-MRI) was utilized to assess motor tract integrity. Results: Semicircular canal testing revealed normal results except for a slightly reduced response to right-sided caloric irrigation (26% asymmetry ratio; cut-off = 25%). Otolith testing, however, showed marked asymmetry in oVEMP amplitudes, confirmed with two devices (37% and 53% weaker on the left side; cut-off = 30%). Bone-conducted cVEMP amplitudes were mildly reduced bilaterally. Posturography, video-oculography, and subjective visual vertical testing were all within normal ranges. Diffusion tensor MRI revealed no structural abnormalities correlating with the observed functional asymmetry. Conclusions: This professional tightrope walker’s exceptional balance skills contrast starkly with significant peripheral vestibular (otolithic) deficits, while MR imaging, including diffusion tensor imaging, remained normal. These findings highlight the critical role of central computational mechanisms in optimizing multisensory input signals and fully compensating for vestibular asymmetries in this unique case. Full article
(This article belongs to the Section Clinical Neurophysiology)
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<p>Quantitative vestibular testing including video head impulse testing (vHIT) (panel <b>A</b>), bithermal caloric irrigation (panel <b>B</b>), cVEMPs (panel <b>C</b>), and oVEMPs (panel <b>D</b>). For the vHIT (panel <b>A</b>) eye velocity traces (in green) and head velocity traces (in red for assessing the right vestibular organ and in blue for assessing the left vestibular organ) are plotted against time for each SCC (20 trials per canal recorded). Note that eye velocity traces were inverted for better visualization and comparison with the head velocity traces. In the center of both panels average gains are provided for all six semicircular canals. In the subject presented here, the normal function of all six semicircular canals was seen, thus all canals were plotted in green. For caloric irrigation (panel <b>B</b>), applying warm (44 °C, red dots) and cold (30 °C, pink dots) water to one ear, the nystagmus slow phase velocity was plotted against time. Noteworthy, a canal paresis factor of 26% was seen (panel <b>B</b>), pointing to a mildly reduced function of the right horizontal semicircular canal. Response asymmetries on bone-conducted cVEMPs (plotted against time, three sessions shown) were within normal range (panel <b>C</b>), whereas on oVEMP-testing (panel <b>D</b>) a significant asymmetry ratio was noted with left-sided impairment of utricular function both when using the Nicolet (37%) and the Eclipse (53%) testing devices. Abbreviations: R = right; L = left.</p>
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<p>All tracts reconstructed from the high-resolution diffusion tensor imaging dataset. Data were sampled with a 1.3 mm isotropic spatial resolution and 64 encoded diffusion directions. Note the geometrical accuracy of the tracts due to the segmented image acquisition used. The quality of the data were also due to the absolute motion-less patient position during the acquisition. Overlay on a T1 weighted anatomical scan. Color encoding: blue: cranio-caudal, red: left-right, green: anterior–posterior.</p>
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<p>Rubro-spinal crossing of the motor tract, in red shown for the axial (<b>left</b>), sagittal (<b>middle</b>), and coronal (<b>right</b>) plane. The 1.3 mm isotropic resolution of the DTI data allowed the representation of such a small crossing with the depicted quality. For color coding see Legend of <a href="#ctn-09-00009-f002" class="html-fig">Figure 2</a>.</p>
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<p>Freddy Nock (1964–2024), renowned tightrope walker, captured in a moment of levity before undergoing MR imaging. Eager to participate in the study, Nock humorously remarked about his brain soon being visualized by the machine.</p>
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21 pages, 7497 KiB  
Article
An Enhanced Local Optimization Algorithm for GNSS Shadow Matching in Mobile Phones
by Xianggeng Han, Nijia Qian, Jingxiang Gao, Zengke Li, Yifan Hu, Liu Yang and Fangchao Li
Remote Sens. 2025, 17(4), 677; https://doi.org/10.3390/rs17040677 - 16 Feb 2025
Viewed by 331
Abstract
In the context of mobile phones, the local optimal global navigation satellite systems (GNSS) shadow matching algorithm, which is based on the urban three-dimensional model, can effectively reduce the error of GNSS pseudo-range single-point positioning. However, the positioning accuracy of this algorithm is [...] Read more.
In the context of mobile phones, the local optimal global navigation satellite systems (GNSS) shadow matching algorithm, which is based on the urban three-dimensional model, can effectively reduce the error of GNSS pseudo-range single-point positioning. However, the positioning accuracy of this algorithm is susceptible to noise, and its continuous signal-to-noise ratio (SNR) scoring method does not fully exploit the probability density and probability distribution information contained in the SNR. Therefore, this paper proposes two improvements for the local optimal shadow matching algorithm: (1) utilizing low-pass filtering to filter SNR, thereby reducing the influence of noise on the algorithm and (2) introducing a probability-based SNR scoring method to fully leverage the probability density and probability distribution information of SNR. In dynamic single-point positioning, the improved algorithm attains an absolute positioning accuracy of up to 3 m, representing a decimeter-level enhancement over the original algorithm. Experiments confirm that using the SNR statistical information of non-line of sight (NLOS) and line-of-sight (LOS) as prior information results in better positioning accuracy compared to when this information is distorted by multipath effects. Additionally, to address the issue of high time complexity in the shadow matching algorithm, especially when considering local optima, this paper presents a scheme to simplify the algorithm’s flow, reducing its time complexity by approximately 75%. Full article
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<p>Sky shadow map.</p>
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<p>Local candidate region and local candidate point selection.</p>
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<p>LOS/NLOS signal: (<b>a</b>) Probability density curve; (<b>b</b>) probability distribution curve.</p>
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<p>The flow chart of shadow matching algorithm considering local optimum.</p>
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<p>This is a figure. Schemes follow the same formatting. Determine local candidate region: (<b>a</b>) obtain points inside roads; (<b>b</b>) obtain local candidate points.</p>
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<p>Satellite visibility prediction reference figure: (<b>a</b>) satellite-ground connection figure; (<b>b</b>) satellite visibility figure.</p>
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<p>Scores for each candidate position: (<b>a</b>) the results of continuous SNR scoring; (<b>b</b>) the results of SNR scoring based on probability.</p>
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<p>First-order low-pass filtering smoothed SNR.</p>
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<p>Flow chart of improved shadow matching algorithm considering local optimum.</p>
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<p>Experimental scene, locations, and routes of the collected data.</p>
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<p>LOS signal (affected by multipath effects): (<b>a</b>) probability density curve; (<b>b</b>) probability distribution curve.</p>
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<p>The statistical charts of the plane error distribution: (<b>a</b>) error distribution in the E direction at point 1 in experimental group 1; (<b>b</b>) error distribution in the E direction at point 2 in experimental group 1; (<b>c</b>) error distribution in the E direction at point 3 in experimental group 1; (<b>d</b>) error distribution in the N direction at point 1 in experimental group 1; (<b>e</b>) error distribution in the N direction at point 2 in experimental group 1; (<b>f</b>) error distribution in the N direction at point 3 in experimental group 1; (<b>g</b>) error distribution in the E direction at point 1 in experimental group 2; (<b>h</b>) error distribution in the E direction at point 2 in experimental group 2; (<b>i</b>) error distribution in the E direction at point 3 in experimental group 2; (<b>j</b>) error distribution in the N direction at point 1 in experimental group 2; (<b>k</b>) error distribution in the N direction at point 2 in experimental group 2; (<b>l</b>) error distribution in the N direction at point 3 in experimental group 2.</p>
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<p>The distribution of SNR origin data of NLOS and LOS signals: (<b>a</b>) the distribution of SNR origin data; (<b>b</b>) the distribution of SNR smoothed data.</p>
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<p>Pseudo-range single-point positioning: positioning of continuous SNR scoring in the experimental group 1 and the experiment group 2.</p>
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<p>The distribution of SNR origin data of route 1 and route 2: (<b>a</b>) the distribution of SNR origin data; (<b>b</b>) the distribution of SNR smoothed data.</p>
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13 pages, 1432 KiB  
Article
Significance of Influent C/N Ratios in Mainstream Anammox Process: Nitrogen Removal and Microbial Dynamics
by Yandong Yang, Shichong Liu, Lei Liu, Yanan Long, Chao Wang and Changqing Liu
Water 2025, 17(4), 562; https://doi.org/10.3390/w17040562 - 15 Feb 2025
Viewed by 199
Abstract
Achieving simultaneous anammox and denitrification is a feasible approach for enhancing nitrogen removal in mainstream anammox processes. Nevertheless, the optimal C/N range and microbial dynamics driving this process are still not fully understood. In this study, three mainstream anammox reactors were operated with [...] Read more.
Achieving simultaneous anammox and denitrification is a feasible approach for enhancing nitrogen removal in mainstream anammox processes. Nevertheless, the optimal C/N range and microbial dynamics driving this process are still not fully understood. In this study, three mainstream anammox reactors were operated with varying influent C/N ratios. The results demonstrated a remarkable nitrogen removal of 92.6% achieved by combining partial denitrification and anammox with the C/N ratio set at 1.0. However, the nitrogen removal efficiency decreased when the C/N ratio was either 0.5 or 2.0, causing the accumulation of nitrate and ammonium in the effluent, respectively. These results suggest a narrow optimal range of the influent C/N for mainstream anammox processes. Additionally, a transition in the predominant denitrifier population from Denitratisoma to Thauera was noted when the C/N ratio increased. The denitrifying phenotype of Thauera was significantly influenced by the C/N ratio. Thauera can effectively collaborate with anammox bacteria only at a suitable C/N ratio, where it partially reduces the nitrate generated in the anammox reaction. With a high influent C/N, Thauera primarily performed nitrite reduction, notably inhibiting anammox activity. The results of this study are valuable for the optimal design of the mainstream anammox process. Full article
(This article belongs to the Special Issue ANAMMOX Based Technology for Nitrogen Removal from Wastewater)
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Graphical abstract
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<p>The TN removal performance (<b>a</b>), effluent nitrogen concentrations (<b>b</b>), and ΔNO<sub>2</sub><sup>−</sup>/ΔNH<sub>4</sub><sup>+</sup> and ΔNO<sub>3</sub><sup>−</sup>/ΔNH<sub>4</sub><sup>+</sup> ratios (<b>c</b>) of the mainstream anammox reactor at an influent C/N of 0.5.</p>
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<p>The TN removal performance (<b>a</b>), effluent nitrogen concentrations (<b>b</b>), and ΔNO<sub>2</sub><sup>−</sup>/ΔNH<sub>4</sub><sup>+</sup> and ΔNO<sub>3</sub><sup>−</sup>/ΔNH<sub>4</sub><sup>+</sup> ratios (<b>c</b>) of the mainstream anammox reactor at an influent C/N of 1.0.</p>
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<p>The TN removal performance (<b>a</b>), effluent nitrogen concentrations (<b>b</b>), and ΔNO<sub>2</sub><sup>−</sup>/ΔNH<sub>4</sub><sup>+</sup> and ΔNO<sub>3</sub><sup>−</sup>/ΔNH<sub>4</sub><sup>+</sup> ratios (<b>c</b>) of the mainstream anammox reactor at an influent C/N of 2.0.</p>
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<p>Variations in organic and nitrogen concentrations in the typical cycles of mainstream anammox reactors with influent C/N ratios of 0.5 (<b>a</b>), 1.0 (<b>b</b>), and 2.0 (<b>c</b>).</p>
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<p>Core genera of the mainstream anammox reactors with various influent C/N ratios.</p>
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24 pages, 20331 KiB  
Article
Population Dynamics of the Widespread Alien Decapod Species, Brown Shrimp (Penaeus aztecus), in the Mediterranean Sea
by Mehmet Cengiz Deval and Tomris Deniz
Animals 2025, 15(4), 561; https://doi.org/10.3390/ani15040561 - 14 Feb 2025
Viewed by 268
Abstract
This study investigated the population dynamics, growth, reproduction, and parasitism of Penaeus aztecus over a 27-month period in Antalya Bay (Eastern Mediterranean). P. aztecus was the most abundant shrimp species, comprising 53.4% of the collected shrimp specimens. Abundance varied seasonally, with peak densities [...] Read more.
This study investigated the population dynamics, growth, reproduction, and parasitism of Penaeus aztecus over a 27-month period in Antalya Bay (Eastern Mediterranean). P. aztecus was the most abundant shrimp species, comprising 53.4% of the collected shrimp specimens. Abundance varied seasonally, with peak densities in summer. Males had a smaller mean carapace length (CL) of 25.8 mm compared to females at 30.2 mm. Females dominated larger size classes, with all individuals ≥ 46 mm CL being female. The sex ratio was balanced at 1:1, with no seasonal variations. Spawning occurred year-round, peaking in June, late summer, and November. Females displayed four ovarian stages, with the first mature size (FMS) at 36 mm CL. Parasitism by Epipenaeon ingens reduced the density of mature females, with 42% of potential spawners failing to develop gonads. The prevalence of parasitism showed seasonal variation and was inversely correlated with sea surface temperature (SST). Marine recruitment occurred from June to November, with a peak between July and September. Growth analysis revealed faster rates in females, while males reached a smaller maximum size. This study also identified inefficiencies in gear selectivity, with many juvenile shrimp (below recruitment size) being retained. Trawl efficiency improved with the use of turtle excluder devices (TEDs), which reduced bycatch of nontarget species, such as loggerhead turtles and cartilaginous fishes. The instantaneous total mortality rate (Z) ranged from 0.658 to 0.026 month⁻1 for male shrimp and from 1.00 to 0.014 month⁻1 for female shrimp, with survival sharply declining after recruitment, leaving only about 3.6% of individuals surviving beyond 10 months. Full article
(This article belongs to the Section Ecology and Conservation)
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<p>Trawl sampling tracks in the Antalya Bay (eastern Mediterranean). The red dots indicate the starting point of each trawl haul.</p>
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<p>Length frequency distributions of infected and non-infected shrimp by carapace length (CL) and by sex of <span class="html-italic">Penaeus aztecus</span> sampled in Antalya Bay (a 64 mm CL female not included).</p>
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<p>The four macroscopic developmental stages of the ovary in female <span class="html-italic">Penaeus aztecus</span>.</p>
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<p>(<b>a</b>) Pooled monthly percentage distribution of the four ovarian developmental stages of <span class="html-italic">Penaeus aztecus</span> from Antalya Bay (eastern Mediterranean) during the study period, from March 2019 to November 2021. (<b>b</b>) Monthly pooled oscillation of the gonadosomatic index (GSI) for standard sizes (CL ≥ 34 mm), with extreme values indicated by “o” and high extreme values by “*”. (<b>c</b>) Overlap of GSI values across the four ovarian stages. (<b>d</b>) First maturation size (CL<sub>50%</sub>) for female specimens.</p>
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<p>(<b>a</b>) Pooled monthly percentage distribution of the four ovarian developmental stages of <span class="html-italic">Penaeus aztecus</span> from Antalya Bay (eastern Mediterranean) during the study period, from March 2019 to November 2021. (<b>b</b>) Monthly pooled oscillation of the gonadosomatic index (GSI) for standard sizes (CL ≥ 34 mm), with extreme values indicated by “o” and high extreme values by “*”. (<b>c</b>) Overlap of GSI values across the four ovarian stages. (<b>d</b>) First maturation size (CL<sub>50%</sub>) for female specimens.</p>
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<p>Monthly fluctuations in the density of recruits-of-the-year (D<sub>REC</sub>), total density (D<sub>TOT</sub>), and sea surface temperature (SST) observed during the surveys.</p>
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<p>The mean CLs of the identified modal groups of five cohorts of <span class="html-italic">Penaeus aztecus</span> on a modal progression analysis for female (<b>a</b>) and male (<b>b</b>) over a 27-month period in the Antalya Bay.</p>
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<p>(<b>a</b>) Carapace length (CL) to total weight (TW) regression slopes (b ± confidence intervals) for <span class="html-italic">Penaeus aztecus</span> by group: infected females (IF) and - male (IM), uninfected females (UIF) and - male (UIM), pooled female (F) and - male (M). (<b>b</b>) CL/TW relationships for both sex (straight line and yellow circles for male, dashed line and red circles for female).</p>
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<p>Seasonally oscillating von Bertalanffy growth curves fitted to the observed mean carapace length (CL) at relative age for both sexes of <span class="html-italic">Penaeus aztecus</span>. The pink line represents the estimated growth curve for females, with pink circles indicating the observed mean CL values (mm). The blue line represents the estimated growth curve for males, with blue circles marking the observed mean CL values (mm).</p>
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<p>The selection curve for <span class="html-italic">Penaeus aztecus</span>, represented by the thick logistic line with confidence intervals, is derived from pooled data. The observed retention values are shown as red circles, while the size structures of entered specimens are depicted by the thick line and escaped specimens by the broken line. (<b>a</b>) Retention probability of the codend. (<b>b</b>) Escapement probability of the TED grid. (<b>c</b>) Retention probability of the entire system.</p>
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10 pages, 284 KiB  
Proceeding Paper
Construction of Dimensionless Groups by Entropic Similarity
by Robert K. Niven
Phys. Sci. Forum 2023, 9(1), 27; https://doi.org/10.3390/psf2023009027 - 13 Feb 2025
Viewed by 19
Abstract
Since the early 20th century, dimensional analysis and similarity arguments have provided a critical tool for the analysis of scientific, engineering, and thermodynamic systems. Traditionally, the resulting dimensionless groups are categorized into those defined by (i) geometric similarity, involving ratios of length [...] Read more.
Since the early 20th century, dimensional analysis and similarity arguments have provided a critical tool for the analysis of scientific, engineering, and thermodynamic systems. Traditionally, the resulting dimensionless groups are categorized into those defined by (i) geometric similarity, involving ratios of length scales; (ii) kinematic similarity, involving ratios of velocities or accelerations, and (iii) dynamic similarity, involving ratios of forces. This study considers an additional category based on entropic similarity, with three variants defined by the following: (i) ratios of global or local entropy production terms Π entrop = σ ˙ 1 / σ ˙ 2 or Π ^ entrop = σ ˙ ^ 1 / σ ˙ ^ 2 ; (ii) ratios of entropy flow rates Π entrop = F S , 1 / F S , 2 or magnitudes of entropy fluxes Π ^ entrop = | | j S 1 | | / | | j S 2 | | ; and (iii) the ratio of a fluid velocity to that of a carrier of information Π info = U / c . Given that all phenomena involving work against friction, dissipation, spreading, chemical reaction, mixing, separation, or the transmission of information are governed by the second law of thermodynamics, these are more appropriately analyzed directly in terms of competing entropic phenomena and the dominant entropic regime, rather than indirectly using ratios of forces. This work presents the entropic dimensionless groups derived for a wide range of diffusion, chemical reaction, dispersion, and wave phenomena, revealing an entropic interpretation for many known dimensionless groups and many new dimensionless groups. Full article
17 pages, 2829 KiB  
Article
Comparative Patterns of Sex Expression and Sex Ratios in Island and Continental Bryophyte Populations
by Anabela Martins, Jairo Patiño and Manuela Sim-Sim
Plants 2025, 14(4), 573; https://doi.org/10.3390/plants14040573 - 13 Feb 2025
Viewed by 639
Abstract
Reproductive biology patterns are crucial for understanding the dynamics and evolution of plants. This is particularly relevant in bryophytes, where sex expression and reproductive success can vary significantly with environmental conditions. Islands, with their isolated and diverse environments, provide natural laboratories to explore [...] Read more.
Reproductive biology patterns are crucial for understanding the dynamics and evolution of plants. This is particularly relevant in bryophytes, where sex expression and reproductive success can vary significantly with environmental conditions. Islands, with their isolated and diverse environments, provide natural laboratories to explore these dynamics. In this study, we investigate sex expression, the phenotypic sex ratio, and sporophyte production in one moss (Exsertotheca intermedia) and three liverwort species (Frullania polysticta, Frullania teneriffae, Porella canariensis) across their entire distribution range. Depending on the species, the geographic range includes the Canary Islands, Madeira, the Azores, the Iberian Peninsula, the British Isles, and the Faroe Islands. For the non-Macaronesian endemic species (F. teneriffae, P. canariensis) higher levels of sex expression and males were found in the Macaronesian archipelagos. In leafy liverworts, females appear to be correlated with lower temperatures and higher precipitation levels, while males seem to be associated with higher temperatures and relatively lower precipitation levels. In this study, we demonstrated that bryophyte populations from Macaronesia exhibited higher levels of sex expression compared to their continental counterparts, suggesting that the distinct environmental conditions of these islands play a crucial role in shaping their reproductive patterns. Full article
(This article belongs to the Section Plant Ecology)
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<p>(<b>A</b>,<b>B</b>) Box plots with Kruskal–Wallis and Wilcoxon tests, displaying sex expression (SE) results for each species and region. Horizontal black lines denote median values, and the mean value is represented by a black dot the respective number displayed on the left. (<b>C</b>,<b>D</b>) Bean plots with Kruskal–Wallis and Wilcoxon tests, displaying phenotypic sex ratio (PSR) results for each species and region (*** <span class="html-italic">p</span> &lt; 0.001, ** <span class="html-italic">p</span> &lt; 0.01, * <span class="html-italic">p</span> &lt; 0.05, ns indicates a non-significant difference). N, number of samples analyzed per locality. (<b>A</b>,<b>C</b>) <span class="html-italic">Exsertotheca intermedia</span>. (<b>B</b>,<b>D</b>) <span class="html-italic">Frullania polysticta</span>.</p>
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<p>(<b>A</b>,<b>B</b>) Box plots with Wilcoxon tests, displaying sex expression (SE) results for each species and region (**** <span class="html-italic">p</span> &lt; 0.0001, ns indicates a non-significant difference). Horizontal black lines denote median values, and the mean value is represented by a black dot the respective number displayed on the left. (<b>C</b>,<b>D</b>) Bean plots with Kruskal–Wallis and Wilcoxon tests, displaying phenotypic sex ratio (PSR) results for each species and region (**** <span class="html-italic">p</span> &lt; 0.0001, ns indicates a non-significant difference). N, number of samples analyzed per locality. (<b>A</b>,<b>C</b>) <span class="html-italic">Frullania teneriffae</span>. (<b>B</b>,<b>D</b>) <span class="html-italic">Porella canariensis</span>.</p>
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<p>Forest plot depicting the effect of elevation, temperature and precipitation (coefficient, with 95% confidence interval) on sex expression (SE) and phenotypic female-to-male sex ratio (PSR♀ and PSR♂) for each species, derived from Generalized Linear Mixed Models (GLMMs) (*** <span class="html-italic">p</span> &lt; 0.001, * <span class="html-italic">p</span> &lt; 0.05, ns indicates a non-significant difference).</p>
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<p>A binomial plot showing the phenotypic male sex ratio (PSR♂) of each studied species across regions and the frequency of sporophytes (FSP). The red line separates the samples with PSR♂ lower or higher than 0.5. (<b>A</b>) <span class="html-italic">Exsertotheca intermedia</span>. (<b>B</b>) <span class="html-italic">Frullania polysticta</span>. (<b>C</b>) <span class="html-italic">Frullania teneriffae</span>. (<b>D</b>) <span class="html-italic">Porella canariensis</span>.</p>
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<p>Maps showing the location of the samples of our studied species (yellow circle: <span class="html-italic">Exsertotheca intermedia</span>, green triangle: <span class="html-italic">Frullania polysticta</span>, pink triangle: <span class="html-italic">Frullania teneriffae</span>, blue square: <span class="html-italic">Porella canariensis</span>) across the five regions. (<b>A</b>) An overall view of the sampling area, including the Macaronesia (Oceanic islands), which contains (<b>B</b>) the Canary Islands; (<b>C</b>) Madeira Island; (<b>D</b>) and the Azores archipelago, as well as the European Atlantic fringe (continental areas): (<b>E</b>) the Iberian Peninsula; (<b>F</b>) the British Isles; and the Faroe Islands.</p>
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11 pages, 9499 KiB  
Communication
A Complementary Metal-Oxide Semiconductor (CMOS) Analog Optoelectronic Receiver with Digital Slicers for Short-Range Light Detection and Ranging (LiDAR) Systems
by Yunji Song and Sung-Min Park
Micromachines 2025, 16(2), 215; https://doi.org/10.3390/mi16020215 - 13 Feb 2025
Viewed by 340
Abstract
This paper introduces an analog differential optoelectronic receiver (ADOR) integrated with digital slicers for short-range LiDAR systems, consisting of a spatially modulated P+/N-well on-chip avalanche photodiode (APD), a cross-coupled differential transimpedance amplifier (CCD-TIA) with cross-coupled active loads, a continuous-time linear equalizer [...] Read more.
This paper introduces an analog differential optoelectronic receiver (ADOR) integrated with digital slicers for short-range LiDAR systems, consisting of a spatially modulated P+/N-well on-chip avalanche photodiode (APD), a cross-coupled differential transimpedance amplifier (CCD-TIA) with cross-coupled active loads, a continuous-time linear equalizer (CTLE), a limiting amplifier (LA), and dual digital slicers. A key feature is the integration of an additional on-chip dummy APD at the differential input node, which enables the proposed ADOR to outperform a traditional single-ended TIA in terms of common-mode noise rejection ratio. Also, the CCD-TIA utilizes cross-coupled PMOS-NMOS active loads not only to generate the symmetric output waveforms with maximized voltage swings, but also to provide wide bandwidth characteristics. The following CTLE extends the receiver bandwidth further, allowing the dual digital slicers to operate efficiently even at high sampling rates. The LA boosts the output amplitudes to suitable levels for the following slicers. Then, the inverter-based slicers with low power consumption and a small chip area produce digital outputs. The fabricated ADOR chip using a 180 nm CMOS process demonstrates a 20 dB dynamic range from 100 μApp to 1 mApp, 2 Gb/s data rate with a 490 fF APD capacitance, and 22.7 mW power consumption from a 1.8 V supply. Full article
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<p>Block diagrams of the proposed ADOR.</p>
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<p>(<b>a</b>) Cross-sectional view of the P<sup>+</sup>/N-well APD integrated on-chip; (<b>b</b>) its layout.</p>
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<p>Schematic diagram of the CCD-TIA.</p>
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<p>Schematic diagram of the 3-bit CTLE.</p>
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<p>Schematic diagram of the LA.</p>
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<p>Layout of the proposed ADOR.</p>
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<p>Simulated frequency responses of the CCD-TIA, CTLE, and LA circuits.</p>
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<p>Simulated output waveforms of the ADOR corresponding to varying input current levels.</p>
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<p>Photograph of the fabricated ADOR chip and its corresponding test setup (inc. optical test).</p>
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<p>Measured eye diagrams of the ADOR with a 500 μA<sub>pp</sub> input current at various data rates of (<b>a</b>) 500 Mb/s, (<b>b</b>) 1 Gb/s, and (<b>c</b>) 2 Gb/s, respectively.</p>
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<p>Measured eye-diagrams of the ADOR at 500-M/bs for various input currents of (<b>a</b>) 100 μA<sub>pp</sub>, (<b>b</b>) 500 μA<sub>pp</sub>, and (<b>c</b>) 1 mA<sub>pp</sub>, respectively.</p>
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<p>Measured output noise voltage of the ADOR.</p>
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19 pages, 19542 KiB  
Article
A Programmable Gain Amplifier Featuring a High Power Supply Rejection Ratio for a 20-Bit Sigma-Delta ADC
by Wenhui Li, Daishi Tian, Hao Zhu and Qingqing Sun
Electronics 2025, 14(4), 720; https://doi.org/10.3390/electronics14040720 - 12 Feb 2025
Viewed by 451
Abstract
A programmable gain amplifier (PGA) is commonly used to optimize the input dynamic range of high-performance systems such as headphones and biomedical sensors. But PGA is rather sensitive to electromagnetic interference (EMI), which limits the precision of these systems. Many capacitor-less low-dropout regulator [...] Read more.
A programmable gain amplifier (PGA) is commonly used to optimize the input dynamic range of high-performance systems such as headphones and biomedical sensors. But PGA is rather sensitive to electromagnetic interference (EMI), which limits the precision of these systems. Many capacitor-less low-dropout regulator (LDO) schemes with high power supply rejection have been proposed to act as the independent power supply for PGA, which consumes additional power and area. This paper proposed a PGA with a high power supply rejection ratio (PSRR) and low power consumption, which serves as the analog front-end amplifier in the 20-bit sigma-delta ADC. The PGA is a two-stage amplifier with hybrid compensation. The first stage is the recycling folded cascode amplifier with the gain-boost technique, while the second stage is the class-AB output stage. The PGA was implemented in the 0.18 μm CMOS technology and achieved a 9.44 MHz unity-gain bandwidth (UGBW) and a 57.8° phase margin when driving the capacitor of 5.9 pF. An optimum figure-of-merit (FoM) value of 905.67 has been achieved with the proposed PGA. As the front-end amplifier of a high-precision ADC, it delivers a DC gain of 162.1 dB, the equivalent input noise voltage of 301.6 nV and an offset voltage of 1.61 μV. Within the frequency range below 60 MHz, the measured PSRR of ADC is below −70 dB with an effective number of bits (ENOB), namely 20 bits. Full article
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<p>Block diagram of a 20-bit sigma-delta ADC with the front-end PGA.</p>
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<p>Proposed two-stage amplifier (RFC1) using hybrid compensation.</p>
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<p>An AC small-signal model for RFC1.</p>
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<p>The final proposed two-stage amplifier (RFC2) applied in the 20-bit sigma-delta ADC: (<b>a</b>) the detailed amplifier circuit with the gain-boost and chopper circuits; (<b>b</b>) the CMOS switch used in the input end; (<b>c</b>) the CH<sub>p</sub> and CH<sub>n</sub> used in the amplifier and the non-overlapping clock at the gate.</p>
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<p>The final proposed two-stage amplifier (RFC2) applied in the 20-bit sigma-delta ADC: (<b>a</b>) the detailed amplifier circuit with the gain-boost and chopper circuits; (<b>b</b>) the CMOS switch used in the input end; (<b>c</b>) the CH<sub>p</sub> and CH<sub>n</sub> used in the amplifier and the non-overlapping clock at the gate.</p>
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<p>Die micrographs of RFC1 and RFC2: (<b>a</b>) RFC1; (<b>b</b>) PGA consisting of RFC2 in the 20-bit sigma-delta ADC.</p>
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<p>Frequency characteristics of amplifiers (RFC1 and RFC2): (<b>a</b>) AC frequency response of RFC1 and RFC2; (<b>b</b>) the variation in UGBW of RFC1 and RFC2 with temperature.</p>
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<p>The large-signal step response of RFC1.</p>
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<p>PSRR simulation: (<b>a</b>) PSRR simulation schematic diagram; (<b>b</b>) PSRR simulation results of RFC1 and RFC2.</p>
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<p>The noise spectral power density of RFC1 and RFC2: (<b>a</b>) the noise spectral power density of RFC1 without the chopper circuit; (<b>b</b>) the noise spectral power density of RFC2 with the chopper circuit on and down.</p>
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<p>The Monte Carol simulation results of RFC1 and RFC2 under different conditions: (<b>a</b>) the process simulation result of RFC1; (<b>b</b>)the mismatch simulation result of RFC1; (<b>c</b>) the process simulation result of RFC2 with the chopper circuit on; (<b>d</b>) the mismatch simulation result of RFC2 with the chopper circuit on; (<b>e</b>) the process simulation result of RFC2 with the chopper circuit off; (<b>f</b>) the mismatch simulation result of RFC2 with the chopper circuit off.</p>
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<p>The measurement circuit of GBW.</p>
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<p>The UGBW testing result of RFC1.</p>
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<p>The measurement circuit of slew rate.</p>
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<p>The measured result of slew rate.</p>
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<p>PSRR measurement: (<b>a</b>) the measurement system diagram of PSRR; (<b>b</b>) the measured result of PSRR. The peak-to-peak values of the sine waves applied to AVDD are 33 mV and 66 mV, respectively.</p>
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<p>The comprehensive comparison results of FoM<sub>s</sub> and DC gain with prior works [<a href="#B6-electronics-14-00720" class="html-bibr">6</a>,<a href="#B16-electronics-14-00720" class="html-bibr">16</a>,<a href="#B23-electronics-14-00720" class="html-bibr">23</a>,<a href="#B24-electronics-14-00720" class="html-bibr">24</a>,<a href="#B25-electronics-14-00720" class="html-bibr">25</a>].</p>
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13 pages, 6452 KiB  
Communication
A Complementary Metal-Oxide-Semiconductor Optoelectronic Analog Front-End Preamplifier with Cross-Coupled Active Loads for Short-Range LiDARs
by Yunji Song, Yejin Choi, Dukyoo Jung, Seonhan Choi and Sung-Min Park
Sensors 2025, 25(4), 1040; https://doi.org/10.3390/s25041040 - 10 Feb 2025
Viewed by 388
Abstract
In this paper, a CMOS optoelectronic analog front-end (AFE) preamplifier with cross-coupled active loads for short range LiDAR applications is presented, which consists of a spatially modulated P+/N-well on-chip avalanche photodiode (APD), the differential input stage with cross-coupled active loads, and [...] Read more.
In this paper, a CMOS optoelectronic analog front-end (AFE) preamplifier with cross-coupled active loads for short range LiDAR applications is presented, which consists of a spatially modulated P+/N-well on-chip avalanche photodiode (APD), the differential input stage with cross-coupled active loads, and an output buffer. Particularly, another on-chip dummy APD is inserted at the differential input node to improve the common-mode noise rejection ratio significantly better than conventional single-ended TIAs. Moreover, the cross-coupled active loads are exploited at the output nodes of the preamplifier not only to help generate symmetric output waveforms, but also to enable the limiting operations even without the following post-amplifiers. In addition, the inductive behavior of the cross-coupled active loads extends the bandwidth further. The proposed AFE preamplifier implemented in a 180-nm CMOS process demonstrate the measured results of 63.5 dB dynamic range (i.e., 1 µApp~1.5 mApp input current recovery), 67.8 dBΩ transimpedance gain, 1.6 GHz bandwidth for the APD capacitance of 490 fF, 6.83 pA⁄√Hz noise current spectral density, 85 dB power supply rejection ratio, and 32.4 mW power dissipation from a single 1.8 V supply. The chip core occupies the area of 206 × 150 µm2. Full article
(This article belongs to the Special Issue Optoelectronic Functional Devices for Sensing Applications)
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<p>Block diagrams of (<b>a</b>) a typical short-range LiDAR system and (<b>b</b>) the proposed AFE preamplifiers for short-range LiDAR system.</p>
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<p>Cross-section of the on-chip P<sup>+</sup>/N-well APD.</p>
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<p>Schematic diagrams of (<b>a</b>) the proposed preamplifier and (<b>b</b>) the f<sub>T</sub>-doubler as an output buffer.</p>
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<p>Simplified schematic diagram of the AFE preamplifier.</p>
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<p>Layout of the proposed AFE preamplifier.</p>
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<p>Simulated frequency response of the AFE preamplifier.</p>
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<p>Simulated phase margin of the AFE preamplifier.</p>
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<p>Simulated eye diagrams of the AFE preamplifier for 100 μ<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>A</mi> </mrow> <mrow> <mi>p</mi> <mi>p</mi> </mrow> </msub> </mrow> </semantics></math> input currents at different data rates of (<b>a</b>) 100 Mb/s, (<b>b</b>) 500 Mb/s, and (<b>c</b>) 1 Gb/s.</p>
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<p>Simulated output pulses of the AFE preamplifier for different input currents.</p>
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<p>Chip photo of the proposed AFE preamplifier and its test setup (inc. optical test).</p>
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<p>Measured frequency response of the AFE preamplifier.</p>
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<p>Measured output noise voltage of the AFE preamplifier.</p>
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<p>Simulated vs. measured PSRR of the AFE preamplifier.</p>
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<p>Optically measured pulses of the AFE preamplifier for (<b>a</b>) 15 μA<sub>pp</sub> and (<b>b</b>) 1.5 mA<sub>pp</sub> input currents (pulse width: 10 ns).</p>
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18 pages, 11067 KiB  
Article
Influence of Load Variation on the Flow Field and Stability of the Francis Turbine
by Shenhui Li, Jiayang Pang, Chengmei Dan, Wenping Xiang, Xutao Yi and Xiaobing Liu
J. Mar. Sci. Eng. 2025, 13(2), 316; https://doi.org/10.3390/jmse13020316 - 9 Feb 2025
Viewed by 393
Abstract
With the development of a power system predominantly reliant on new energy sources, turbine generator sets are increasingly required to operate under wide load conditions, resulting in numerous unstable flow phenomena and substantial economic losses for power stations. This study employs the Shear [...] Read more.
With the development of a power system predominantly reliant on new energy sources, turbine generator sets are increasingly required to operate under wide load conditions, resulting in numerous unstable flow phenomena and substantial economic losses for power stations. This study employs the Shear Stress Transport (SST) k-ω turbulence model to combine numerical simulations with experimental methods. It calculates the guide vane opening at the rated head of a Francis turbine and examines the internal flow field characteristics and pressure pulsations under various operating conditions. The findings indicate that the entropy production ratio in the draft tube is the highest among all load conditions, ranging from about 72.7% to 95.9%. Energy dissipation in the vaneless zone and the runner increases with greater opening. At 45% and 100% load conditions, the draft tube is mainly influenced by dynamic and static interference, single and double frequencies induced by runner rotation, and low-frequency fluctuations of the vortex and. Under 60% load conditions, pressure fluctuations in the draft tube are primarily caused by the eccentric vortex band, characterized by higher intensity and a frequency of 0.2 fn. Numerical results closely align with experimental observations. The findings provide essential guidance for ensuring the stable operation of power plant units. Full article
(This article belongs to the Section Ocean Engineering)
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<p>The 3D water body model of the hydraulic turbine.</p>
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<p>Component grid.</p>
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<p>Verification of Grid Independence.</p>
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<p>Comparison of test results with numerical results.</p>
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<p>Distribution of Turbulent Entropy Production for Each Component.</p>
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<p>Distribution of Entropy Production of the Guide Vane under Different Loads and Blade Heights.</p>
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<p>Entropy Production of the Runner under Different Loads.</p>
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<p>Runner section local flow diagram.</p>
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<p>Entropy Production within the Draft tube.</p>
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<p>Inner section of draft tube.</p>
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<p>Flow Lines of Each Section of the Draft tube.</p>
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<p>Monitoring Point for the Francis Turbine.</p>
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<p>Pressure Pulsation in Vaneless space under Different Loads.</p>
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<p>Pressure Pulsation of Runner under Different Loads.</p>
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<p>Pressure Pulsation of Draft Tube under Different Loads.</p>
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<p>Principle of test measurement.</p>
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<p>Mounting Position of the Sensor.</p>
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<p>Pressure Pulsation within the Vaneless Area under Various Working Conditions.</p>
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<p>Pressure Pulsation of the Draft Tube under Various Working Conditions.</p>
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22 pages, 4590 KiB  
Article
Modelling Pollutant Dispersion in Urban Canyons to Enhance Air Quality and Urban Planning
by Francisco Ruda Sarria, MCarmen Guerrero Delgado, Rafael Monge Palma, Teresa Palomo Amores, José Sánchez Ramos and Servando Álvarez Domínguez
Appl. Sci. 2025, 15(4), 1752; https://doi.org/10.3390/app15041752 - 9 Feb 2025
Viewed by 405
Abstract
Air pollution in urban street canyons presents a serious health risk, especially in densely populated areas. While previous research has explored airflow characteristics in these canyons, it often lacks detailed data on pollutant dispersion and the effects of wind speed on airflow patterns [...] Read more.
Air pollution in urban street canyons presents a serious health risk, especially in densely populated areas. While previous research has explored airflow characteristics in these canyons, it often lacks detailed data on pollutant dispersion and the effects of wind speed on airflow patterns and vortex formation. This study uses Computational Fluid Dynamics (CFD) to deliver quantitative measurements of pollutant dispersion rates and qualitative insights into airflow patterns across various street canyon morphologies. The analysis examines a range of aspect ratios (ARs), from wide (AR = 0.75) to narrow (AR = 4.5), and different wind speeds to evaluate their effects on pollutant dispersion. Findings indicate that purging flow rates decline as the AR increases, with a more pronounced decrease at lower AR values. In narrower streets, airflow patterns are particularly sensitive to wind velocity, leading to unexpected vortices that hinder effective pollutant dispersion. By incorporating these insights into urban design strategies, cities can enhance street ventilation, thereby reducing pollutant concentrations and improving public health. This study also tests a specific street layout in Seville to predict pollutant accumulation under various conditions, assessing health risks based on World Health Organization guidelines. Ultimately, this research aids in developing healthier, more sustainable urban environments. Full article
(This article belongs to the Section Green Sustainable Science and Technology)
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<p>Overview of the method.</p>
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<p>Numerical domain of the street canyon.</p>
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<p>The meshing of the numerical domain.</p>
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<p>Air pattern for different <math display="inline"><semantics> <mrow> <mi mathvariant="bold-italic">A</mi> <mi mathvariant="bold-italic">R</mi> </mrow> </semantics></math>s of street canyons with <math display="inline"><semantics> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">e</mi> </mrow> </semantics></math> = 676,796.</p>
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<p>Air pattern for different <math display="inline"><semantics> <mrow> <mi mathvariant="bold-italic">A</mi> <mi mathvariant="bold-italic">R</mi> </mrow> </semantics></math>s of street canyons with <math display="inline"><semantics> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">e</mi> </mrow> </semantics></math> = 2,030,387.</p>
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<p>Air pattern for different <math display="inline"><semantics> <mrow> <mi mathvariant="bold-italic">A</mi> <mi mathvariant="bold-italic">R</mi> </mrow> </semantics></math>s of street canyons with <math display="inline"><semantics> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">e</mi> </mrow> </semantics></math> = 507,597.</p>
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<p>Classification of the number of recirculations depending on the Reynolds number and the aspect ratio.</p>
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<p>Purging flow rate results for different ARs and Reynolds numbers.</p>
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<p>Purging flow rate results between subvolumes when there are two recirculations.</p>
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<p>Purging flow rate results in the bottom subvolume when there are three recirculations.</p>
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<p>Map of the chosen streets with the level of health risk. Green is for risk-free streets, and yellow is for streets in risk level one.</p>
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16 pages, 2151 KiB  
Article
Anaerobic Digestion of Cattle Manure Contaminated with an Antibiotic Mixture: A Nature-Based Solution for Environmental Management
by Giulia Massini, Anna Barra Caracciolo, Jasmin Rauseo, Francesca Spataro, Giulia Scordo, Luisa Patrolecco, Gian Luigi Garbini, Andrea Visca, Paola Grenni, Ludovica Rolando and Valentina Mazzurco Miritana
Land 2025, 14(2), 353; https://doi.org/10.3390/land14020353 - 8 Feb 2025
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Abstract
Anaerobic digestion (AD) is a waste-to-energy strategy that leverages natural microbiological processes. It is increasingly used in farms to treat manure, resulting in biogas for energy production and digestate as fertiliser. However, animal manure often contains antibiotic (AB) residues, raising concerns about their [...] Read more.
Anaerobic digestion (AD) is a waste-to-energy strategy that leverages natural microbiological processes. It is increasingly used in farms to treat manure, resulting in biogas for energy production and digestate as fertiliser. However, animal manure often contains antibiotic (AB) residues, raising concerns about their impact on AD efficiency and their potential spread through digestate use. This multidisciplinary study evaluated the effects of an AB mixture (enrofloxacin, ciprofloxacin and sulfamethoxazole) on CH4 production, microbial community (Fungi, Bacteria and Archaea) dynamics and antibiotic resistance gene (ARG) presence. The experiment used a cattle manure/digestate ratio of 1:35, typical of real digesters, with AB concentrations set at low (2.5 mg kg−1 each) and high (7.5 mg kg−1 each) levels. The ABs affected cumulative CH4 production (ranging from 5939 to 6464 mL) only at the highest concentration. After 51 days, sulfamethoxazole reached residual levels, while enrofloxacin and ciprofloxacin were only partially degraded (<50%), but ARGs were significantly reduced. The microbial community, particularly prokaryotes, exhibited resilience, maintaining efficient CH4 production. Overall findings strongly suggest that AD is an effective treatment for producing energy and good fertiliser, also reducing AB and ARG content as well as mitigating CH4 emissions into the atmosphere. Full article
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Figure 1

Figure 1
<p>Cumulative CH<sub>4</sub> production in the three experimental conditions; (<b>a</b>) ENR, (<b>b</b>) Mix_L and (<b>c</b>) Mix_H. In each graph, the condition of addition of ABs is compared with the Control. Vertical bars represent the standard errors.</p>
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<p>Antibiotic residual concentrations (expressed as percentages) in the ENR, Mix_L and Mix_H conditions at different sampling times. The dotted lines in the ENR condition represent the residual concentrations of ABs already existing in the cattle manure and digestate mixture used to set up the experiment (not added by the spiking process).</p>
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<p>(<b>A</b>) Total microbial abundance determined by the direct count method using DAPI staining. The vertical bars represent the standard deviations. (<b>B</b>) Micrograph of the microbial community visualised under an epifluorescence microscope (Axioskop 40, Carl Zeiss).</p>
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<p>(<b>A</b>) Microbial community composition (%) at the start of the experiment and day 51 using fluorescence in situ hybridisation. <span class="html-italic">Fungi</span> (blue bars), <span class="html-italic">Bacteria</span> (green bars) and <span class="html-italic">Archaea</span> (red bars). The vertical bars represent the standard deviations. (<b>B</b>) Micrographs visualised by epifluorescence microscopy: <span class="html-italic">Fungi</span> (Calcofluor staining), <span class="html-italic">Bacteria</span> and <span class="html-italic">Archaea</span> detected using different probes with the FISH technique (FAM-labelled Eub, II and III and Cy3-labeled ARCH915 probes, respectively).</p>
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<p>Relative gene abundances (ARGs/16S) in the Control, ENR, Mix_L and Mix_H conditions at 1 and 51 days. The vertical bars represent the standard errors.</p>
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