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Search Results (1,843)

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12 pages, 1782 KiB  
Review
Combining Neural Networks and Genetic Algorithms to Understand Composition–Microstructure–Property Relationships in Additively Manufactured Metals
by Sooraj Patel, Anvesh Nathani, Amin Poozesh, Shuozhi Xu, Pejman Kazempoor and Iman Ghamarian
J. Manuf. Mater. Process. 2024, 8(6), 269; https://doi.org/10.3390/jmmp8060269 - 28 Nov 2024
Viewed by 82
Abstract
Additive manufacturing (AM) has revolutionized the production of complex metallic components by enabling the direct fabrication of intricate geometries from 3D model data. Despite its advantages in reducing material waste and customization of mechanical properties, AM faces challenges related to microstructural heterogeneity and [...] Read more.
Additive manufacturing (AM) has revolutionized the production of complex metallic components by enabling the direct fabrication of intricate geometries from 3D model data. Despite its advantages in reducing material waste and customization of mechanical properties, AM faces challenges related to microstructural heterogeneity and mechanical property variability. This review highlights the structure–property relationships in additively manufactured metals, emphasizing how heterogeneous microstructure influences yield strength and fracture toughness. Phenomenological equations are provided based on the integration of neural networks and genetic algorithm-based models to predict mechanical properties from composition and microstructural features. We also outline key considerations such as acquiring high-fidelity datasets and understanding mathematical correlations within the data needed to formulate phenomenological equations. Full article
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<p>Considerable variations in microstructure can be a reason for location-dependent properties. (<b>a</b>) A schematic representing columnar grains formed across multiple deposited layers; (<b>b</b>) hardness variation within the deposited layers in an additively printed α/β titanium part.</p>
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<p>Schematic representation of neural network model of composition–structure–property relationships. C<sub>1</sub>, C<sub>2</sub>, and C<sub>3</sub> refer to the concentration of alloying elements in a multicomponent material.</p>
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<p>Procedure to develop phenomenological equations from an experimental dataset.</p>
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<p>Virtual experiment results for the NN and GA analyses of the composition and microstructure variables in α + β titanium alloy Ti-6Al-4V [<a href="#B73-jmmp-08-00269" class="html-bibr">73</a>]. Reproduced with permission from Springer Nature (2015).</p>
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29 pages, 3720 KiB  
Article
Modeling, Simulation, and Control of a Rotary Inverted Pendulum: A Reinforcement Learning-Based Control Approach
by Ruben Hernandez, Ramon Garcia-Hernandez and Francisco Jurado
Modelling 2024, 5(4), 1824-1852; https://doi.org/10.3390/modelling5040095 (registering DOI) - 27 Nov 2024
Viewed by 202
Abstract
In this paper, we address the modeling, simulation, and control of a rotary inverted pendulum (RIP). The RIP model assembled via the MATLAB (Matlab 2021a)®/Simulink (Simulink 10.3) Simscape (Simscape 7.3)™ environment demonstrates a high degree of fidelity in its capacity to [...] Read more.
In this paper, we address the modeling, simulation, and control of a rotary inverted pendulum (RIP). The RIP model assembled via the MATLAB (Matlab 2021a)®/Simulink (Simulink 10.3) Simscape (Simscape 7.3)™ environment demonstrates a high degree of fidelity in its capacity to capture the dynamic characteristics of an actual system, including nonlinear friction. The mathematical model of the RIP is obtained via the Euler–Lagrange approach, and a parameter identification procedure is carried out over the Simscape model for the purpose of validating the mathematical model. The usefulness of the proposed Simscape model is demonstrated by the implementation of a variety of control strategies, including linear controllers as the linear quadratic regulator (LQR), proportional–integral–derivative (PID) and model predictive control (MPC), nonlinear controllers such as feedback linearization (FL) and sliding mode control (SMC), and artificial intelligence (AI)-based controllers such as FL with adaptive neural network compensation (FL-ANC) and reinforcement learning (RL). A design methodology that integrates RL with other control techniques is proposed. Following the proposed methodology, a FL-RL and a proportional–derivative control with RL (PD-RL) are implemented as strategies to achieve stabilization of the RIP. The swing-up control is incorporated into all controllers. The visual environment provided by Simscape facilitates a better comprehension and understanding of the RIP behavior. A comprehensive analysis of the performance of each control strategy is conducted, revealing that AI-based controllers demonstrate superior performance compared to linear and nonlinear controllers. In addition, the FL-RL and PD-RL controllers exhibit improved performance with respect to the FL-ANC and RL controllers when subjected to external disturbance. Full article
(This article belongs to the Topic Agents and Multi-Agent Systems)
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<p>Simscape model of the RIP. The control input is denoted by <span class="html-italic">u</span>; the angular displacement of the horizontal arm is denoted by <math display="inline"><semantics> <msub> <mi>q</mi> <mn>1</mn> </msub> </semantics></math>, and the angular position of the pendulum is denoted by <math display="inline"><semantics> <msub> <mi>q</mi> <mn>2</mn> </msub> </semantics></math>.</p>
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<p>Simulink blocks of the RIP system: (<b>a</b>) main subsystem, (<b>b</b>) elements of the main subsystem: <span class="html-italic">Configuration block</span> components (box-dashed lines), <span class="html-italic">Support_base</span>, <span class="html-italic">Actuated_arm</span> and <span class="html-italic">Pendulum</span> subsystems.</p>
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<p>(<b>a</b>) Simulink block of the support base and (<b>b</b>) components of the support base.</p>
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<p>(<b>a</b>) Simulink block of the <span class="html-italic">Actuated_arm</span> subsystem and (<b>b</b>) elements of the subsystem.</p>
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<p>Elements of the <span class="html-italic">Actuator</span> subsystem Simulink block.</p>
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<p>Elements of the <span class="html-italic">Pendulum</span> subsystem Simulink block.</p>
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<p>(<b>a</b>) Rotational friction torque and (<b>b</b>) components of the friction subsystem.</p>
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<p>Evolution of the estimated parameters <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>p</mi> <mo>^</mo> </mover> <mi>i</mi> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>.</p>
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<p>Time evolution of angular positions of the Simscape and mathematical model for (<b>a</b>) arm position and (<b>b</b>) pendulum position.</p>
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<p>Block diagram of the elements of an RL framework.</p>
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<p>Flowchart of the proposed methodology.</p>
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<p>Block diagram of the DDPG algorithm.</p>
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<p>Simulink diagram of the RL controller.</p>
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<p>Curve of the RL agent learning process.</p>
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<p>Block diagram of implemented controllers.</p>
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<p>Simulink diagram of the FL controller: (<b>a</b>) control scheme implementation, (<b>b</b>) control law implementation.</p>
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<p>Simulink diagram of the FL-ANC controller: (<b>a</b>) control scheme implementation, (<b>b</b>) adaptive neural network controller subsystem block.</p>
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<p>Simulink block diagram of swing-up controller.</p>
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<p>Time evolution of controller signals. Left-hand side upper plot: arm position <math display="inline"><semantics> <msub> <mi>q</mi> <mn>1</mn> </msub> </semantics></math>. Left-hand side bottom plot: control signal <span class="html-italic">u</span>. Right-hand side plot: pendulum position <math display="inline"><semantics> <msub> <mi>q</mi> <mn>2</mn> </msub> </semantics></math>.</p>
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<p>Time evolution of controller signals under an external force. Left-hand side upper plot: arm position <math display="inline"><semantics> <msub> <mi>q</mi> <mn>1</mn> </msub> </semantics></math>. Left-hand side bottom plot: control signal <span class="html-italic">u</span>. Right-hand side plot: pendulum position <math display="inline"><semantics> <msub> <mi>q</mi> <mn>2</mn> </msub> </semantics></math>.</p>
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18 pages, 4818 KiB  
Article
Embedded 3D Printing for Microchannel Fabrication in Epoxy-Based Microfluidic Devices
by Cheng Zhang, Wenyu Ning, Ding Nan, Jiangtao Hao, Weiliang Shi, Yang Yang, Fei Duan, Wenbo Jin, Lei Liu and Danyang Zhao
Polymers 2024, 16(23), 3320; https://doi.org/10.3390/polym16233320 - 27 Nov 2024
Viewed by 194
Abstract
Microfluidic devices offer promising solutions for automating various biological and chemical procedures. Epoxy resin, known for its excellent mechanical properties, chemical resistance, and thermal stability, is widely used in high-performance microfluidic devices. However, the poor printability of epoxy has limited its application in [...] Read more.
Microfluidic devices offer promising solutions for automating various biological and chemical procedures. Epoxy resin, known for its excellent mechanical properties, chemical resistance, and thermal stability, is widely used in high-performance microfluidic devices. However, the poor printability of epoxy has limited its application in 3D printing technologies for fabricating epoxy-based microfluidic devices. In this study, fumed silica is introduced into epoxy resin to formulate a yield-stress fluid suspension as a support bath for embedded 3D printing (e-3DP). The study demonstrates that increasing the fumed silica concentration from 3.0% to 9.0% (w/v) enhances the yield stress from 9.46 Pa to 56.41 Pa, the compressive modulus from 19.79 MPa to 36.34 MPa, and the fracture strength from 148.16 MPa to 168.78 MPa, while reducing the thixotropic time from 6.58 s to 1.32 s, albeit with a 61.3% decrease in the transparency ratio. The 6.0% (w/v) fumed silica–epoxy suspension is selected based on a balance between yield stress, transparency, and mechanical performance, enabling high-fidelity filament formation. Two representative microfluidic devices are successfully fabricated, demonstrating the feasibility of a fumed silica–epoxy suspension for the customizable e-3DP of epoxy-based microfluidic devices. Full article
(This article belongs to the Special Issue Biopolymers for 3D Printing)
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<p>Schematic of the e-3DP mechanism assisted by FS–ER suspension for microfluidic device fabrication. (<b>a</b>) Printing of Pluronic F127 ink in FS–ER suspension: (<b>a-1</b>) three-dimensional network structure of fumed silica with freely moving epoxy polymer chains, (<b>a-2</b>) disordered fumed silica structure, under stress, with freely moving epoxy polymer chains, and (<b>a-3</b>) core-corona micelles structure of Pluronic F127. (<b>b</b>) Crosslinked FS–ER microfluidic device with hollow channels, formed after the removal of liquefied Pluronic F127: (<b>b-1</b>) freely moving triblock polymer chains of Pluronic F127 at 4 °C, and (<b>b-2</b>) interpenetrating network structure within the fully solidified FS–ER composite.</p>
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<p>Rheological properties of FS–ER suspensions with different fumed silica concentrations: (<b>a</b>) shear stress as a function of shear rate, and (<b>b</b>) thixotropy tests on the FS–ER suspensions.</p>
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<p>Shear moduli as a function of frequency for FS–ER suspensions.</p>
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<p>Mechanical properties of crosslinked FS–ER samples: (<b>a</b>) fracture strength as a function of fumed silica concentration and (<b>b</b>) compression modulus as a function of fumed silica concentration.</p>
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<p>Transparency of crosslinked FS–ER samples with different fumed silica concentrations. Scale bar: 10 mm.</p>
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<p>Filament formation in FS–ER suspension: (<b>a</b>) filament diameter as a function of time at different path speeds and extrusion pressures, and (<b>b</b>) filament diameter as a function of resting time after printing.</p>
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<p>Rheological properties of 40.0% (<span class="html-italic">w</span>/<span class="html-italic">v</span>) Pluronic F127: (<b>a</b>) viscosity as a function of temperature and (<b>b</b>) viscosity as a function of shear rate.</p>
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<p>Shear moduli as a function of frequency for 40% <span class="html-italic">w</span>/<span class="html-italic">v</span> Pluronic F127.</p>
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<p>Printed microfluidic devices: (<b>a-1</b>) 3D model of the designed cross-channel microfluidic device, (<b>a-2</b>) printed cross-channel microstructure, and (<b>a-3</b>) cross-channel microfluidic device infused with black dye after the removal of the sacrificial ink. (<b>a-4</b>,<b>a-5</b>) Cross-sectional views of the microchannels at corresponding positions in the cross-channel microfluidic device. (<b>b-1</b>) A 3D model of the designed circular-channel microfluidic device, (<b>b-2</b>) printed circular-channel microstructure, and (<b>b-3</b>) circular-channel microfluidic device infused with black dye after the removal of the sacrificial ink. (<b>b-4</b>) Cross-sectional view of the microchannel in the circular-channel microfluidic device. The scale bars in (<b>a-2</b>,<b>a-3</b>,<b>b-2</b>,<b>b-3</b>) represent 10 mm, while the scale bars in (<b>a-4</b>,<b>a-5</b>,<b>b-4</b>) represent 0.5 mm.</p>
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16 pages, 2045 KiB  
Article
An Optimized SVR Algorithm for Pulse Pile-Up Correction in Pulse Shape Discrimination
by Xianghe Liu, Bingqi Liu, Mingzhe Liu, Yufeng Tang, Haonan Li and Yao Huang
Sensors 2024, 24(23), 7545; https://doi.org/10.3390/s24237545 - 26 Nov 2024
Viewed by 235
Abstract
Pulse pile-up presents a significant challenge in nuclear radiation measurements, particularly in neutron-gamma pulse shape discrimination, as it causes pulse distortion and diminishes identification accuracy. To address this, we propose an optimized Support Vector Regression (SVR) algorithm for correcting pulse pile-up. Initially, the [...] Read more.
Pulse pile-up presents a significant challenge in nuclear radiation measurements, particularly in neutron-gamma pulse shape discrimination, as it causes pulse distortion and diminishes identification accuracy. To address this, we propose an optimized Support Vector Regression (SVR) algorithm for correcting pulse pile-up. Initially, the Dung Beetle Optimizer (DBO) and Whale Optimization Algorithm (WOA) are integrated to refine the correction process, with performance evaluated using charge comparison methods (CCM) for pulse shape discrimination. Leveraging prior knowledge from simulated data, we further analyze the relationships between various types of pulse pile-ups, including their combinations, inter-peak distances, and the accuracy of corrections. Extensive experiments conducted in a mixed neutron-gamma radiation field using plastic scintillators demonstrate that the proposed method effectively corrects pulse pile-up and accurately discriminates between neutron and gamma. Moreover, our approach significantly improves the fidelity of pulse shape discrimination and enhances the overall reliability of radiation detection systems in high-interference environments. Full article
(This article belongs to the Section Electronic Sensors)
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<p>Schematic diagram of charge comparison method.</p>
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<p>Different pile-up pulses of simulated data.</p>
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<p>Acquisition of experimental data, (<b>a</b>) Pulse discrimination scatter plot obtained through CCM, (<b>b</b>) Neutron source chamber measurement, (<b>c</b>) Schematic diagram of pulse acquisition experiment.</p>
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<p>Flowcharts for SVR, DBO-SVR, and WOA-SVR.</p>
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<p>Pulse pile-up correction results for different SVR algorithms based on simulated data.</p>
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<p>CCM values and error bars for the test dataset, (<b>a</b>) Randomly selected 10 pulses and predicted using three methods to compare CCM values, (<b>b</b>) The CCM error bars of three predicted method.</p>
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<p>Scatter CCM values and FoM values for three methods based on simulated data. (<b>a</b>) Scatter plots of the three methods and the training data, (<b>b</b>) FoM values for three methods.</p>
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<p>Restoration of pulse pile-up by three methods, error counts, and error rates.</p>
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<p>Pulse pile-up correction results based on plastic scintillators using different SVR methods.</p>
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<p>Scatter CCM values and FoM values for three methods after correction based on experimental data. (<b>a</b>) Scatter plots of the three methods and the training data, (<b>b</b>) FoM values for three methods.</p>
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<p>Comparison of scatter plots before and after correction, (<b>a</b>) simulated data, (<b>b</b>) Experimental data.</p>
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27 pages, 2703 KiB  
Review
Indoor Air Quality Control for Airborne Diseases: A Review on Portable UV Air Purifiers
by Shriram Sankurantripati and Florent Duchaine
Fluids 2024, 9(12), 281; https://doi.org/10.3390/fluids9120281 - 26 Nov 2024
Viewed by 381
Abstract
The spread of airborne diseases such as COVID-19 underscores the need for effective indoor air quality control. This review focuses on ventilation strategies and portable air purifiers as key mitigation solutions. Ventilation systems, including natural and mechanical approaches, can reduce pathogen concentrations by [...] Read more.
The spread of airborne diseases such as COVID-19 underscores the need for effective indoor air quality control. This review focuses on ventilation strategies and portable air purifiers as key mitigation solutions. Ventilation systems, including natural and mechanical approaches, can reduce pathogen concentrations by improving airflow. However, combining ventilation with portable air purifiers, particularly those using HEPA filters, ESP filters, and UV-C radiation, can enhance Indoor air quality. While HEPA and ESP filters focus on trapping airborne particles, UV-C radiation can inactivate pathogens by disrupting their RNA. A review of UV air purifiers reveals a lack of studies on their efficacy and effectiveness in real-world settings. A thorough investigation into the performance of this mitigation solution is necessary, focusing on varying key factors, such as purifier placement, airflow dynamics, and UV dosage, to ensure optimal effectiveness. High-fidelity computational methods are essential in accurately assessing these factors, as informed by the physics of airborne transmission. Such advanced computations are necessary to determine the viability of portable UV air purifiers in mitigating airborne transmission in enclosed environments such as hospitals and public spaces. Integrating advanced air purification technologies with proper ventilation can improve safety in indoor environments and prevent future disease-related outbreaks. Full article
(This article belongs to the Special Issue Recent Advances in Fluid Mechanics: Feature Papers, 2024)
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<p>Evolution of global infected cases and the World Health Organization’s corresponding declarations during the COVID-19 pandemic.</p>
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<p>Transmission routes for SARS-CoV-2 virus to travel from an infected source to a susceptible individual [<a href="#B54-fluids-09-00281" class="html-bibr">54</a>].</p>
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<p>Factors influencing the evolution of expelled droplets during disease transmission from an infected source to a susceptible individual.</p>
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<p>Illustrations of different mechanical ventilation systems [<a href="#B88-fluids-09-00281" class="html-bibr">88</a>].</p>
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<p>Illustrations of different mechanical ventilation systems [<a href="#B88-fluids-09-00281" class="html-bibr">88</a>].</p>
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<p>General representation of an upper-room UVGI (UR-UVGI) setup.</p>
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<p>General representation of an array of UV lamps installed inside a ventilation duct.</p>
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<p>Flow chart explaining the review process for UV air purifiers.</p>
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<p>General representation of a UVGI portable air cleaner.</p>
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17 pages, 7035 KiB  
Article
Characterization and PCR Application of Family B DNA Polymerases from Thermococcus stetteri
by Aleksandra A. Kuznetsova, Marina A. Soloveva, Elena S. Mikushina, Anastasia A. Gavrilova, Artemiy S. Bakman and Nikita A. Kuznetsov
Life 2024, 14(12), 1544; https://doi.org/10.3390/life14121544 - 25 Nov 2024
Viewed by 299
Abstract
DNA polymerases from the hyperthermophilic Archaea have attracted considerable attention as PCR enzymes due to their high thermal stability and proofreading 3′ → 5′ exonuclease activity. This study is the first to report data concerning the purification and biochemical characteristics of the Tst [...] Read more.
DNA polymerases from the hyperthermophilic Archaea have attracted considerable attention as PCR enzymes due to their high thermal stability and proofreading 3′ → 5′ exonuclease activity. This study is the first to report data concerning the purification and biochemical characteristics of the Tst DNA polymerase from Thermococcus stetteri. Both the wild type Tst(wt) DNA polymerase and its chimeric form containing the P36H substitution—which reduces the enzyme’s affinity for the U-containing template and dUTP—and the DNA-binding domain Sso7d from S. solfataricus were obtained and analyzed. It was shown that Tst(wt) could effectively amplify up to 6-kb DNA fragments, whereas TstP36H–Sso7d could amplify DNA fragments up to 15 kb. It was found that TstP36H–Sso7d has superior PCR efficiency compared to the commonly used DNA polymerase PfuV93Q–Sso7d. For the amplification of a 2-kb DNA fragment, TstP36H–Sso7d required less than 10 s of extension time, whereas for PfuV93Q–Sso7d, the extension time was no less than 30 s. Steady-state kinetic assays revealed that the dNTP-binding affinity KdNTPm was the same for TstP36H–Sso7d and PfuV93Q–Sso7d, whereas the maximum rate of dNTP incorporation, kcat, was two orders of magnitude higher for TstP36H–Sso7d. Moreover, the incorporation of incorrect dNTP was not observed for TstP36H–Sso7d up to 56 °C, whereas for PfuV93Q–Sso7d, the extension of primer with incorrect dNTP was observed at 37 °C, supporting higher fidelity of TstP36H–Sso7d. The obtained data suggest that TstP36H–Sso7d may be a good candidate for high-fidelity DNA amplification. Full article
(This article belongs to the Special Issue Advances in Research in Biocatalysis: 2nd Edition)
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<p>Expression and purification assay of Tst DNA polymerases. (<b>A</b>) Expression analysis of Tst(wt) and the TstP36H–Sso7d DNA polymerase gene in <span class="html-italic">E. coli</span> Rosetta 2(DE3) pLysS cells containing the recombinant plasmids. A. Lane M, protein molecular mass markers; Lane N, sonicated pellet (N<sup>P</sup>) and lysate (N<sup>L</sup>) of uninduced cells; Lane I, sonicated pellet (I<sup>P</sup>) and lysate (I<sup>L</sup>) of induced cells. (<b>B</b>) Purification of Tst(wt) and TstP36H–Sso7d DNA polymerases. Lines 1–3 indicate protein-containing fractions from chromatographies in a HiTrap Heparin™ column, Line 4, resulting in the Heparin-purified Tst(wt) DNA polymerase, Line 5, resulting in the phenyl-purified TstP36H–Sso7d DNA polymerase.</p>
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<p>Characterization of the Tst(wt) DNA polymerase. DNA polymerase activity of the purified Tst(wt) DNA polymerase assayed under the indicated conditions. The TstP36H–Sso7d DNA polymerase showed the same results; therefore, these results are presented as one. Effects on Tst(wt) DNA polymerase activity in terms of (<b>A</b>) pH; (<b>B</b>) MgCl<sub>2</sub>; (<b>C</b>) KCl; (<b>D</b>) (NH<sub>4</sub>)<sub>2</sub>SO<sub>4</sub>; and (<b>E</b>) elongation temperature. (<b>F</b>) Thermostability of Tst(wt) DNA polymerase; the purified enzyme was incubated at 95 °C. (<b>G</b>) The DSF profile, black trace represents experimental data, red curve is theoretically fitted.</p>
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<p>Comparison of PCR efficiency in amplifying a 2-kb fragment from λ DNA using Tst(wt), TstP36H–Sso7d, and PfuV93Q–Sso7d DNA polymerases with various extension times. The enzymes used and extension times are indicated at the top of the figure. PCR products were resolved using 1.0% agarose gel electrophoresis. Lane M, Sky-High DNA ladder (Biolabmix LLC, Novosibirsk, Russia).</p>
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<p>Comparison of PCR amplification of 2–10 kb from λ DNA using Tst(wt), TstP36H–Sso7d, and PfuV93Q–Sso7d DNA polymerases with various extension times. Amplicon sizes are indicated at the top of the figure. Lane M contains DNA molecular-sized markers (SkyHigh DNA ladder, Biolabmix, LLC, Novosibirsk, Russia). The cycling protocol consisted of one initial denaturation step at 94 °C for 30 s; 30 cycles of 94 °C for 30 s, 60 °C for 30 s, 72 °C for 1 min (<b>A</b>), 1.5 min (<b>B</b>), 2 min (<b>C</b>), and 1 cycle of 72 °C for 10 min.</p>
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<p>Comparison of PCR amplification of 2–10 kb from λ DNA using Tst(wt), TstP36H–Sso7d, and PfuV93Q–Sso7d DNA polymerases with various extension times. Amplicon sizes are indicated at the top of the figure. Lane M contains DNA molecular-sized markers (SkyHigh DNA ladder, Biolabmix, LLC, Novosibirsk, Russia). The cycling protocol consisted of one initial denaturation step at 94 °C for 30 s; 30 cycles of 94 °C for 30 s, 60 °C for 30 s, 72 °C for 1 min (<b>A</b>), 1.5 min (<b>B</b>), 2 min (<b>C</b>), and 1 cycle of 72 °C for 10 min.</p>
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<p>Comparison of PCR amplification of 10–20-kb from λ DNA using Tst(wt), TstP36H–Sso7d, and PfuV93Q–Sso7d DNA polymerases. Amplicon sizes are indicated at the top of the figure. Lane M contains DNA molecular-sized markers (SkyHigh DNA ladder, Biolabmix, LLC, Novosibirsk, Russia). The cycling protocol consists of one initial denaturation step at 94 °C for 30 s; 30 cycles of 94 °C for 30 s, 60 °C for 30 s, 72 °C 5 min, and 1 cycle of 72 °C for 10 min.</p>
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<p>Primer–template elongation using TstP36H–Sso7d and PfuV93Q–Sso7d DNA polymerases under 20 °C. Representative single-nucleotide (dTTP) primer strand extension PAAG analysis with 10 µM dTTP. The nonlinear regression fit of the single-nucleotide extension experiments by the Michaelis–Menten equation for TstP36H–Sso7d (blue) and PfuV93Q–Sso7d (black) DNA polymerases.</p>
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<p>Primer–template elongation by TstP36H–Sso7d and PfuV93Q–Sso7d DNA polymerases at different temperatures with incorrect dNTP. Representative nucleotide (dNTP) primer strand extension PAAG analysis was conducted with 5 mM of dNTP (PfuV93Q–Sso7d DNA polymerase) and 10 mM of dNTP (TstP36H–Sso7d DNA polymerase).</p>
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<p>Primer–template elongation by TstP36H–Sso7d and PfuV93Q–Sso7d DNA polymerases at different temperatures with incorrect dNTP. Representative nucleotide (dNTP) primer strand extension PAAG analysis was conducted with 5 mM of dNTP (PfuV93Q–Sso7d DNA polymerase) and 10 mM of dNTP (TstP36H–Sso7d DNA polymerase).</p>
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23 pages, 4058 KiB  
Article
Improving Flood Streamflow Estimation of Ungauged Small Reservoir Basins Using Remote Sensing and Hydrological Modeling
by Fangrong Zhou, Nan Wu, Yuning Luo, Yuhao Wang, Yi Ma, Yifan Wang and Ke Zhang
Remote Sens. 2024, 16(23), 4399; https://doi.org/10.3390/rs16234399 - 24 Nov 2024
Viewed by 545
Abstract
Small- and medium-sized reservoirs significantly alter natural flood processes, making it essential to understand their impact on runoff for effective water resource management. However, the lack of measured data for most small reservoirs poses challenges for accurately simulating their behavior. This study proposes [...] Read more.
Small- and medium-sized reservoirs significantly alter natural flood processes, making it essential to understand their impact on runoff for effective water resource management. However, the lack of measured data for most small reservoirs poses challenges for accurately simulating their behavior. This study proposes a novel method that utilizes readily available satellite observation data, integrating hydraulic, hydrological, and mathematical formulas to derive outflow coefficients. Based on the Grid-XinAnJiang (GXAJ) model, the enhanced GXAJ-R model accounts for the storage and release effects of ungauged reservoirs and is applied to the Tunxi watershed. Results show that the original GXAJ model achieved a stable performance with an average NSE of 0.88 during calibration, while the NSE values of the GXAJ and GXAJ-R models during validation ranged from 0.78 to 0.97 and 0.85 to 0.99, respectively, with an average improvement of 0.03 in the GXAJ-R model. This enhanced model significantly improves peak flow simulation accuracy, reduces relative flood peak error by approximately 10%, and replicates the flood flow process with higher fidelity. Additionally, the area–volume model derived from classified small-scale data demonstrates high accuracy and reliability, with correlation coefficients above 0.8, making it applicable to other ungauged reservoirs. The OTSU-NDWI method, which improves the NDWI, effectively enhances the accuracy of water body extraction from remote sensing, achieving overall accuracy and kappa coefficient values exceeding 0.8 and 0.6, respectively. This study highlights the potential of integrating satellite data with hydrological models to enhance the understanding of reservoir behavior in data-scarce regions. It also suggests the possibility of broader applications in similarly ungauged basins, providing valuable tools for flood management and risk assessment. Full article
(This article belongs to the Special Issue Remote Sensing for Terrestrial Hydrologic Variables)
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<p>Geographical location and reservoir distribution map of Tunxi basin; the upper right corner shows the Xinanjiang Reservoir catchment area, located in the north of the Tunxi River Basin, as an example of water extraction.</p>
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<p>Flowchart of this study.</p>
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<p>Schematic diagram of flow over a practical weir without gate control, 1-1 and 2-2 are sections used to calculate the energy equation.</p>
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<p>GXAJ-R model framework diagram.</p>
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<p>Schematic of grid–reservoir classification, where (<b>a</b>–<b>c</b>) represent Case a to Case c respectively.</p>
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<p>Water body extraction results for the Dongfanghong Reservoir catchment area in 2017.</p>
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<p>Comparison of water body extraction accuracy for the Dongfanghong Reservoir area between NDWI and OTSU-NDWI methods from 2014 to 2017, (<b>a</b>) is the box plot of OA and KC, and (<b>b</b>) is the relationship between the reservoir water area extracted by remote sensing and the measured value.</p>
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<p>Simulated hourly streamflow at the Tunxi basin outlet for the GXAJ and GXAJ-R models.</p>
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<p>Model performance indicators. (<b>a</b>) NSE, (<b>b</b>) RTE, (<b>c</b>) RRE, (<b>d</b>) RPE.</p>
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14 pages, 2506 KiB  
Article
Investigation of Nonlinear Relations Among Flow Profiles Using Artificial Neural Networks
by Shiming Yuan, Caixia Chen, Yong Yang and Yonghua Yan
Fluids 2024, 9(12), 276; https://doi.org/10.3390/fluids9120276 - 23 Nov 2024
Viewed by 196
Abstract
This study investigated the ability of artificial neural networks (ANNs) to resolve the nonlinear dynamics inherent in the behavior of complex fluid flows, which often exhibit multifaceted characteristics that challenge traditional analytical or numerical methods. By employing flow profile pairs that are generated [...] Read more.
This study investigated the ability of artificial neural networks (ANNs) to resolve the nonlinear dynamics inherent in the behavior of complex fluid flows, which often exhibit multifaceted characteristics that challenge traditional analytical or numerical methods. By employing flow profile pairs that are generated through high-fidelity numerical simulations, encompassing both the one-dimensional benchmark problems and the more intricate three-dimensional boundary layer transition problem, this research convincingly demonstrates that neural networks possess a remarkable capacity to effectively capture the discontinuities and the subtle wave characteristics that occur at small scales within complex fluid flows, thereby showcasing their robustness in handling intricate fluid dynamics phenomena. Furthermore, even in the context of challenging three-dimensional problems, this study reveals that the average velocity profiles can be predicted with a high degree of accuracy, utilizing a limited number of input profiles during the training phase, which underscores the efficiency and efficacy of the model in understanding complex systems. The findings of this study significantly underscore the immense potential that artificial neural networks, along with deep learning methodologies, hold in advancing our comprehension of the fundamental physics that govern complex fluid dynamics systems, while concurrently demonstrating their applicability across a variety of flow scenarios and their capacity to yield insightful revelations regarding the nonlinear relationships that exist among diverse flow parameters, thus paving the way for future research in this critical area of study. Full article
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<p>A schematic of the simulation domain.</p>
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<p>Pressure–density profile pairs (1000 pairs).</p>
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<p>Comparison of predicted and exact solutions at (<b>a</b>) time step = 742; (<b>b</b>) time step = 851.</p>
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<p>Pressure–density profile pairs (1800 pairs).</p>
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<p>Comparison of predicted and exact solutions at (<b>a</b>) time step = 52; (<b>b</b>) time step = 176; (<b>c</b>) time step = 426.</p>
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<p>Comparison of predicted and numerical solutions at (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mn>128</mn> <mo> </mo> <mi>d</mi> <mi>x</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mn>176</mn> <mo> </mo> <mi>d</mi> <mi>x</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mn>516</mn> <mo> </mo> <mi>d</mi> <mi>x</mi> </mrow> </semantics></math>.</p>
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<p>Comparison of predicted and numerical solutions at (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mn>130</mn> <mo> </mo> <mi>d</mi> <mi>x</mi> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mn>205</mn> <mo> </mo> <mi>d</mi> <mi>x</mi> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>=</mo> <mn>516</mn> <mo> </mo> <mi>d</mi> <mi>x</mi> </mrow> </semantics></math>.</p>
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24 pages, 3781 KiB  
Article
Enhancing Building-Integrated Photovoltaic Power Forecasting with a Hybrid Conditional Generative Adversarial Network Framework
by Dong Ha Choi, Wei Li and Albert Y. Zomaya
Energies 2024, 17(23), 5877; https://doi.org/10.3390/en17235877 - 23 Nov 2024
Viewed by 349
Abstract
This paper presents a novel framework that integrates Conditional Generative Adversarial Networks (CGANs) and TimeGAN to generate synthetic Building-Integrated Photovoltaic (BIPV) power data, addressing the challenge of data scarcity in this domain. By incorporating time-related attributes as conditioning information, our method ensures the [...] Read more.
This paper presents a novel framework that integrates Conditional Generative Adversarial Networks (CGANs) and TimeGAN to generate synthetic Building-Integrated Photovoltaic (BIPV) power data, addressing the challenge of data scarcity in this domain. By incorporating time-related attributes as conditioning information, our method ensures the preservation of chronological order and enhances data fidelity. A tailored learning scheme is implemented to capture the unique characteristics of solar power generation, particularly during sunrise and sunset. Comprehensive evaluations demonstrate the framework’s effectiveness in generating high-quality synthetic data, evidenced by a 79.58% improvement in the discriminative score and a 13.46% improvement in the predictive score compared to TimeGAN. Moreover, integrating the synthetic data into forecasting models resulted in up to 23.56% improvement in mean absolute error (MAE) for BIPV power generation predictions. These results highlight the potential of our framework to enhance prediction accuracy and optimize data utilization in renewable energy applications. Full article
(This article belongs to the Section A2: Solar Energy and Photovoltaic Systems)
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<p>Block diagram of the components and loss functions in the proposed framework.</p>
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<p>Learning flow of the proposed framework.</p>
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<p>PCA and t-SNE visualization of the original and synthetic data.</p>
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<p>Comparison of BIPV forecasting accuracy using synthetic data and original data.</p>
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<p>Discriminative score and predictive score by condition set.</p>
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<p>BIPV forecasting accuracy by condition set.</p>
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<p>Comparison of BIPV forecasting accuracy with TimeGAN.</p>
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<p>Comparison of power data generated by GAN framework with original data.</p>
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<p>Discriminative and predictive score of the synthetic data with and without <math display="inline"><semantics> <msub> <mi>L</mi> <mi>off</mi> </msub> </semantics></math>.</p>
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<p>Forecasting accuracy with and without <math display="inline"><semantics> <msub> <mi>L</mi> <mi>off</mi> </msub> </semantics></math>.</p>
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<p>The effect of <math display="inline"><semantics> <msub> <mi>L</mi> <mi>off</mi> </msub> </semantics></math> on the synthetic power data.</p>
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<p>Discriminative and predictive score of the synthetic data with and without learning scheme.</p>
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<p>Forecasting accuracy with and without learning scheme.</p>
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40 pages, 15913 KiB  
Review
Photocrosslinkable Biomaterials for 3D Bioprinting: Mechanisms, Recent Advances, and Future Prospects
by Yushang Lai, Xiong Xiao, Ziwei Huang, Hongying Duan, Liping Yang, Yuchu Yang, Chenxi Li and Li Feng
Int. J. Mol. Sci. 2024, 25(23), 12567; https://doi.org/10.3390/ijms252312567 - 22 Nov 2024
Viewed by 588
Abstract
Constructing scaffolds with the desired structures and functions is one of the main goals of tissue engineering. Three-dimensional (3D) bioprinting is a promising technology that enables the personalized fabrication of devices with regulated biological and mechanical characteristics similar to natural tissues/organs. To date, [...] Read more.
Constructing scaffolds with the desired structures and functions is one of the main goals of tissue engineering. Three-dimensional (3D) bioprinting is a promising technology that enables the personalized fabrication of devices with regulated biological and mechanical characteristics similar to natural tissues/organs. To date, 3D bioprinting has been widely explored for biomedical applications like tissue engineering, drug delivery, drug screening, and in vitro disease model construction. Among different bioinks, photocrosslinkable bioinks have emerged as a powerful choice for the advanced fabrication of 3D devices, with fast crosslinking speed, high resolution, and great print fidelity. The photocrosslinkable biomaterials used for light-based 3D printing play a pivotal role in the fabrication of functional constructs. Herein, this review outlines the general 3D bioprinting approaches related to photocrosslinkable biomaterials, including extrusion-based printing, inkjet printing, stereolithography printing, and laser-assisted printing. Further, the mechanisms, advantages, and limitations of photopolymerization and photoinitiators are discussed. Next, recent advances in natural and synthetic photocrosslinkable biomaterials used for 3D bioprinting are highlighted. Finally, the challenges and future perspectives of photocrosslinkable bioinks and bioprinting approaches are envisaged. Full article
(This article belongs to the Special Issue Bioprinting: Progress and Challenges)
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<p>Schematic illustration of (<b>a</b>) extrusion, (<b>b</b>) inkjet, (<b>c</b>) stereolithography, and (<b>d</b>) light-assisted 3D bioprinting (The figures were created with BioRender).</p>
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<p>A schematic illustration of the mechanism of free radical chain-growth polymerization. (<b>a</b>) The mechanism of free radical chain-growth polymerization. (<b>b</b>) A schematic of polymer chains containing reactive groups crosslinking through free radical chain-growth polymerization.</p>
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<p>Schematic illustrations of the mechanism of thiol-ene-mediated polymerization. (<b>a</b>) A schematic illustration of the mechanism of thiol-ene crosslinking. (<b>b</b>) A schematic of polymer chains containing reactive groups crosslinking through thiol-ene polymerization. (<b>c</b>) Kinetic modeling of photoinitiated thiol-ene click chemistry based on alkene conversion and a summary of the reactivity of the alkene group (Copyright 2012 American Chemical Society [<a href="#B122-ijms-25-12567" class="html-bibr">122</a>]).</p>
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<p>The mechanism of redox crosslinking. (<b>a</b>) A schematic illustration of the mechanism of redox polymerization. (<b>b</b>) A schematic of polymer chains containing reactive groups crosslinking through redox reactions.</p>
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<p>Collagen-based photocrosslinking bioinks. (<b>a</b>) Schematic representation of methacrylate- [<a href="#B171-ijms-25-12567" class="html-bibr">171</a>,<a href="#B172-ijms-25-12567" class="html-bibr">172</a>], maleic- [<a href="#B173-ijms-25-12567" class="html-bibr">173</a>], norbornene- [<a href="#B170-ijms-25-12567" class="html-bibr">170</a>], and thiol-modified [<a href="#B174-ijms-25-12567" class="html-bibr">174</a>] collagen synthesis. (<b>b</b>) The relative solubility of NorCol and collagen at different pH values. (<b>c</b>) The miscibility of NorCol with gelatin and alginate. (<b>d</b>) Temperature-sensitive extrusion bioprinting of NorCol bioinks. (<b>d</b>) (i) Schematic of temperature-sensitive extrusion bioprinting of NorCol bio-inks. (ii) Printed NorCol hydrogels (12 layers, 3 mm) after 1 day of culture. Fluorescence micrographs showing cell (iii) viability (day 1) and (iv) spreading (day 5) within NorCol hydrogels (Copyright 2021 American Chemical Society [<a href="#B170-ijms-25-12567" class="html-bibr">170</a>]).</p>
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<p>Schematic illustration of collagen hydrolysis and representative routes to synthesize methacrylate, norbornene, vinyl, and tyrosine-modified gelatin.</p>
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<p>The bioprinting performance of photocrosslinkable gelatin bioinks. (<b>a</b>) The cell viability within the printed scaffold is affected by the methacrylate degree of GelMA. (i) Photocrosslinking for solidification. (ii) Evaluation of live and dead cells encapsulating in 7.5% GM-30/60/90 on day 5. (iii) Semiquantitative analysis of cell viability, (<span class="html-italic">** p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001) (Copyright 2023 Wiley [<a href="#B52-ijms-25-12567" class="html-bibr">52</a>]). (<b>b</b>) An illustrative scheme of cell-laden bioprinting using GelMA and GelNB/HepSH bioinks. (<b>c</b>) HUVEC-laden constructs are built from GelNB/HepSH and GelMA bioinks. (i) Fluorescence micrographs showing the bioprinted constructs after 1 and 7 days of culture. (ii) Semiquantitative analysis of cell viability. Fluorescence micrographs showing HUVEC cytoskeleton in both bioinks after cell culture for 7 days, using (iii) an inverted fluorescence microscope and (iv) a laser scanning confocal microscope, scale bars = 500 μm. (v,vi) 3D-printed canine peripheral-nerve-like constructs using the GelNB/HepSH bioink, scale bars = 4 mm (Copyright 2021 American Chemical Society [<a href="#B112-ijms-25-12567" class="html-bibr">112</a>]). (<b>d</b>) GelNB/GelS bioinks can undergo superfast gelation at extremely low photoinitiator concentrations. (i) Water-based synthesis of GelNB and GelS from gelatin. (ii) Photocrosslinked thiol-ene click hydrogel. (iii) Comparison of the two thiol-ene hydrogel systems GelNB/DTT and GelNB/GelS. <span class="html-italic">*** p</span> &lt; 0.001. (<b>e</b>) The 3D bioprinting of an NHDF-laden hydrogel grid structure (i) 3D bioprinting of a hydrogel grid structure (1 cm × 1 cm) consisting of four layers on a glass slide. Post-printing cell viability analysis of 3D bioprinted NHDF at day 1 using (ii) GelMA and (iii) GelNB/GelS bioinks. (iv) Distribution of NHDF within the hydrogel, (i) Live/dead staining and (ii) distribution of NHDF, scale bars = 100 μm, (<span class="html-italic">** p &lt;</span> 0.01) (Copyright 2021 Wiley [<a href="#B180-ijms-25-12567" class="html-bibr">180</a>]). (<b>f</b>) A schematic comparison of GelNB synthesized by (i) 5-norbornene-2-carboxylic acid and (ii) CA.</p>
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<p>Hyaluronic acid-based photocrosslinking bioinks. (<b>a</b>) Synthesis route of light-cured hyaluronic acid. (<b>b</b>) Modification of sodium HA with CA to form NorHA<sub>CA</sub>. (i) Reaction scheme for NorHA<sub>CA</sub> synthesis. (ii) Degree of modification of HA with norbornene is tuned by changing the molar ratio of CA to HA repeat units. (iii) Schematic representation of network formation by visible light-induced thiol-ene step-growth reaction between NorHA<sub>CA</sub> and DTT in the presence of photoinitiator (LAP), (<span class="html-italic">** p &lt;</span> 0.01, <span class="html-italic">**** p &lt;</span> 0.0001). (<b>c</b>) Biocompatibility and DLP-based 3D bioprinting of NorHA<sub>CA</sub> bioinks. (i) Representative fluorescence micrographs of bMSCs encapsulated in NorHA<sub>CA</sub> (5wt%, 40%mod.) bulk hydrogels over time (1, 3, and 7 days), scale bars = 200 μm. (ii) Semiquantitative analysis of cell viability, (<span class="html-italic">* p &lt;</span> 0.05). (iii) Schematic representation of DLP-based 3D printing of NorHACA hydrogels with bMSCs. (iv) Representative maximum projection image of bMSCs encapsulated in a NorHA<sub>CA</sub> macroporous lattice at day 1, scale bars = 1 mm and 500 μm (Copyright 2023 American Chemical Society [<a href="#B204-ijms-25-12567" class="html-bibr">204</a>]). (<b>d</b>) HA-TBA mediates the synthesis of NorHA.</p>
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<p>Alginate-based bioinks. (<b>a</b>) The (i) structure and (ii) gelation mechanism of alginate. (<b>b</b>) The norbornene alginate bioink (Alg-norb) was functionalized by light-mediated RGD grafting for building L929 cell-embedded constructs. (i) Schematic overview of the strategy employed to develop photoactive Alg-norb for bioprinting. (ii) Photoinitiated thiol−ene reactions of Alg-norb with RGD Peptide Sequence (CGGGRGDS). (iii) Images of 3D bioprinted hydrogels loaded with cells at (a) day 0 and (b) day 7. Green and red cell tracker labeled L929 as two different bioinks printed as alternating fibers (c) in the X-Y plane and (d) in the Z direction (Copyright 2018 American Chemical Society [<a href="#B218-ijms-25-12567" class="html-bibr">218</a>]). (<b>c</b>) The synthesis of Alg-RGD through a thiol-ene click reaction to promote the cell growth and vascularization of HUVECs. (i) Design of the HA/Alg-RGD hydrogel. (ii) Schematic diagram of the 3D printing process. (iii) Fluorescent images of GFP-HUVECs cultured in the hydrogel at intervals of 3, 7, and 14 days post-3D printing, along with magnified images of selected regions (scale bar = 1 mm and 200 μm, respectively) (Copyright 2023 American Chemical Society [<a href="#B219-ijms-25-12567" class="html-bibr">219</a>]).</p>
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<p>SF-based photocrosslinkable bioink. (<b>a</b>) Production, structure, and modification of SF (Copyright 2023 Elsevier [<a href="#B228-ijms-25-12567" class="html-bibr">228</a>]). (<b>b</b>) The design and printing performance of the redox-crosslinkable SF/CG bioink. (i) Schematic of the printing process of SF/CG bioink. (ii) CAD images depicting the ear, nose, and hand and printed images at various angles (Copyright 2024 Elsevier [<a href="#B237-ijms-25-12567" class="html-bibr">237</a>]). (<b>c</b>) Methacrylate-group-functionalized SF for recapitulating human skin models through 3D bioprinting (Copyright 2024 Wiely [<a href="#B243-ijms-25-12567" class="html-bibr">243</a>]).</p>
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<p>dECM-based photocrosslinkable bioinks. (<b>a</b>) The production and modification of dECM (Copyright 2023 Ivyspring [<a href="#B252-ijms-25-12567" class="html-bibr">252</a>]). (<b>b</b>) The Ru/SPS-induced visible light crosslinking of dECM. (i) The crosslinking mechanism. (ii) The gelled dECM hydrogel (Copyright 2023 Wiely [<a href="#B253-ijms-25-12567" class="html-bibr">253</a>]). (<b>c</b>) The light-activated dityrosine crosslinking reaction in dECM bioink to realize centimeter-scale 3D bioprinting. (i) A schematic of visible-light active dityrosine synthesis. (ii) Extrusion-based printing of dECM. (iii) DLP photopatterning with 100 µm step-size constructs, scale bars = 100 μm for white represent printed fiber, 500 μm for live/dead images, (Copyright 2021 Wiely [<a href="#B124-ijms-25-12567" class="html-bibr">124</a>]). (<b>d</b>) Liver dECM was functionalized by glycidyl methacrylate and methacrylic anhydride for the systematic comparison of different type of methacrylate dECM bioinks. The (i) preparation and (ii) modification of live dECM (Copyright 2024 Elsevier [<a href="#B254-ijms-25-12567" class="html-bibr">254</a>]). (<b>e</b>) The decellularized small intestine submucosa (dSIS) was functionalized by norbornene to create an orthogonally crosslinked dSIS hydrogel for cancer and vascular tissue engineering. (i) 1H NMR spectra of dSIS and dSIS-NB. Peak a: alkene protons (HC=CH), Peak b: ethyl protons (CH<sub>2</sub>), Peaks c and d: methine protons (C<sub>3</sub>CH). (ii) Schematic of thiol-norbornene photo-crosslinking. (iii) Schematic of DLP bioprinting. (iv) In situ, photo rheometry of dSIS-NB gelation with tartrazine added as a photo absorber to improve printing fidelity, dotted line indicate light on. (v) A CAD image of astar-shaped object for DLP bioprinting and the DLP printed dSIS-NB gel. (vi) A representative live/dead confocal image of interconnected microvascular HUVEC network within the printed hydrogel on day 3 (Copyright 2024 Wiely [<a href="#B255-ijms-25-12567" class="html-bibr">255</a>]).</p>
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<p>PEG-based photocrosslinkable bioinks. (<b>a</b>) A schematic of the structures of modified photocrosslinkable PEG derivatives for 3D bioprinting. (<b>b</b>) A schematic diagram of the process for preparing a hydrogel with cell adhesion properties. (A) Schematic representation of the ink design and the hydrogel manufacturing process. (B) Synthetic approach toward labelled RGD peptides (Copyright 2024 Wiley [<a href="#B266-ijms-25-12567" class="html-bibr">266</a>]). (<b>c</b>) A schematic illustration of the fabrication of enzymatically degradable PEG hydrogels to mimic matrix remodeling. (A) Components used in the development of the bioinspired pseudo-reversible stiffening and softening hydrogels include PEG-4-Nb (Mn∼ 5, 10, or 20 kDa), PEG-8-Nb (Mn∼40 kDa), di-thiol nondegradable linkers (PEG-2-SH; Mn∼ 2 or 3.4 kDa), di-thiol MMP degradable linker, a di-thiol MMP PEG-conjugate (PEG<sub>8</sub>MMP), and an MMP-thrombin degradable peptide linker (MMP+Thb). (B) Hydrogel tools were designed to mimic aspects of matrix degradation or matrix deposition that occurs during matrix remodeling of the cellular microenvironment through incorporation of PEG<sub>8</sub>MMP and MMP+Thb linkers, respectively. (C) A reduction of matrix density was achieved by photopolymerization of PEG hydrogels in the presence of a combination of MMP and MMP+Thb linkers, enabling triggered softening through a reduction of crosslink density upon incubation with thrombin. (D) For triggered stiffening, hydrogels were formed by photopolymerization of PEG hydrogels in the presence of MMP crosslinkers followed by secondary photopolymerization of excess reactive handles with PEG or peptide linkers (Copyright 2022 Wiley [<a href="#B267-ijms-25-12567" class="html-bibr">267</a>]). (<b>d</b>) A schematic representation of MSN bioinks for extrusion-based in situ bioprinting applications (Copyright 2023 Elsevier [<a href="#B268-ijms-25-12567" class="html-bibr">268</a>]).</p>
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<p>PF127 and PVA for 3D bioprinting. (<b>a</b>) A schematic diagram of the structure and gel formation mechanism of PF127 (Copyright 2020 American Chemical Society [<a href="#B283-ijms-25-12567" class="html-bibr">283</a>]). (<b>b</b>) A schematic diagram of PF127 as a sacrificial material for the preparation of microvascular tissue. (i) Schematic of the manufacturing process. (ii) Perfusion of fluorescent dextran solution into a GFP-HDFs/RFP-HUVECs co-culture construct (Copyright 2021 IOP Publishing [<a href="#B282-ijms-25-12567" class="html-bibr">282</a>]). (<b>c</b>) Norbornene-modified PVA and gelatin were used to construct a cell-laden hydrogel through volumetric bioprinting (VBP) to promote cell growth and support osteogenic differentiation. (i) (a) Schematic of the set-up for VBP. (b) Illustration of VBP of a PVA bioresin. (c) Chemical structures of norbornene-modified PVA, thiolated crosslinker (PEG2SH), and photoinitiator (LAP). (d) Mechanism of radical-mediated thiol-norbornene photoclick reaction. (ii) (a) Live(green)/dead(red) stained hMSCs following 24 h after printing, scale bars = 100 µm (i, iv). Confocal images of actin-nuclei stained hMSCs in soft and stiff gels at 24 h (ii, v) and 7 days (iii, vi) after printing, scale bars = 100 µm (ii, v) and 50 µm (iii, vi). Scale bars for all inserts are 20 µm. Visualization of single cells in soft and stiff matrix using automated IMARIS dendrite tracking, scale bars = 10µm (iii-1, vi-1). (b) Quantification of cell viability of hMSCs at different time points. (c) Quantification of average cell area in soft and stiff constructs over time. (* <span class="html-italic">p</span> = 0.0485; ns, not significant; n ≥ 3) (d) Confocal image of actin-nuclei stained hMSCs showing cell-cell contacts in the soft gels following 14 days of osteogenic culture (Copyright 2023 Wiley [<a href="#B284-ijms-25-12567" class="html-bibr">284</a>]).</p>
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<p>Representative photoinitiator-free photocrosslinking strategies. (<b>a</b>) A schematic diagram of UV light crosslinking based on coumarin derivatives. (<b>b</b>) A schematic diagram of UV-light-triggered imine crosslinking (Copyright 2021 American Association for the Advancement of Science [<a href="#B337-ijms-25-12567" class="html-bibr">337</a>]). (<b>c</b>) A schematic diagram of UV-light-mediated dual crosslinking based on azide-modified chitosan (Copyright 2011 American Chemical Society [<a href="#B335-ijms-25-12567" class="html-bibr">335</a>]). (<b>d</b>) A schematic diagram of photoinitiator-free photocrosslinking with SbQ as an intermediate. (i) Synthesis of PVA-SBQ and (ii) UV-light-mediated crosslinking mechanism.</p>
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<p>The application of NIR-light-mediated photocrosslinking based on upconversion nanoparticles (UCNPs) for in vivo 3D bioprinting. (<b>a</b>) NIR photopolymerization-based 3D printing technology that enables the noninvasive in vivo 3D bioprinting of tissue constructs (Copyright 2020 American Association for the Advancement of Science [<a href="#B340-ijms-25-12567" class="html-bibr">340</a>]). (<b>b</b>) The 3D bioprinting of noninvasive fracture scaffolds in vivo by the NIR photocuring method. (i) Schematic of the noninvasive fixation of a broken bone with the UCNPs-assisted 3D bioprinting in-vivo. (ii) Fixation scaffolds for (a) oblique and (b) comminuted fractures using UCNPs-assisted NIR 3Dprinting. Images (I, II, III, and IV) show the pre-fracture, post-fracture, 3D skeleton fixation, and corresponding magnified images of the bones respectively. The shin bones of chickens were used in the experiment, scale bar = 0.65 cm. (c) Photograph and CT image with a broken rat. (d) Bioink is subcutaneously injected into the fracture area. (e) 3D in-vivo printing. (f) Images of fracture fixation positions in-vivo, scale bar = 0.6 cm (Copyright 2024 Wiley [<a href="#B339-ijms-25-12567" class="html-bibr">339</a>]).</p>
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<p>Radical generation mechanisms of type I and type II photoinitiators. * means exciting state.</p>
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16 pages, 5987 KiB  
Article
From Single Shot to Structure: End-to-End Network-Based Deflectometry for Specular Free-Form Surface Reconstruction
by M.Hadi Sepanj, Saed Moradi, Amir Nazemi, Claire Preston, Anthony M. D. Lee and Paul Fieguth
Appl. Sci. 2024, 14(23), 10824; https://doi.org/10.3390/app142310824 - 22 Nov 2024
Viewed by 348
Abstract
Deflectometry is a key component in the precise measurement of specular (mirrored) surfaces; however, traditional methods often lack an end-to-end approach that performs 3D reconstruction in a single shot with high accuracy and generalizes across different free-form surfaces. This paper introduces a novel [...] Read more.
Deflectometry is a key component in the precise measurement of specular (mirrored) surfaces; however, traditional methods often lack an end-to-end approach that performs 3D reconstruction in a single shot with high accuracy and generalizes across different free-form surfaces. This paper introduces a novel deep neural network (DNN)-based approach for end-to-end 3D reconstruction of free-form specular surfaces using single-shot deflectometry. Our proposed network, VUDNet, innovatively combines discriminative and generative components to accurately interpret orthogonal fringe patterns and generate high-fidelity 3D surface reconstructions. By leveraging a hybrid architecture integrating a Variational Autoencoder (VAE) and a modified U-Net, VUDNet excels in both depth estimation and detail refinement, achieving superior performance in challenging environments. Extensive data simulation using Blender leading to a dataset which we will make available, ensures robust training and enables the network to generalize across diverse scenarios. Experimental results demonstrate the strong performance of VUDNet, setting a new standard for 3D surface reconstruction. Full article
(This article belongs to the Special Issue Technical Advances in 3D Reconstruction)
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<p>Overview of the context faced by this paper: A known fringe pattern is reflected by some shape of interest, and the resulting reflection is captured by a camera. Our proposed method, VUDNet, reconstructs the estimated shape based on the observed image, trained on a dataset of simulated reflections.</p>
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<p>General architecture of the proposed VUDNet for end-to-end 3D reconstruction of specular free-form surfaces. The network integrates a Variational Autoencoder (VAE, <b>bottom</b>) for coarse depth estimation and a modified U-Net (<b>top</b>) for detail refinement. The ensemble approach leverages both generative and discriminative components, combining their outputs (<b>right</b>) to produce accurate depth maps from single-shot 2D images.</p>
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<p>Simulation environment setup for generating the dataset. The environment includes a fixed camera, a fixed pattern, and various surface settings to replicate realistic deflectometry scenarios. An orthogonal sinusoidal fringe pattern is projected onto specular objects, and the reflected fringes are captured by the camera. This setup ensures the generation of a robust and varied dataset, essential for training the VUDNet to accurately reconstruct 3D surfaces from single-shot 2D images. Since this image is a direct screenshot from the Blender environment, the surface is reflecting the simulated world background. The reflection of the pattern plane on the surface is visible to the camera.</p>
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<p>Mean absolute difference between the ground truth depth map and the predicted depth map from our VUDNet model for a selected sample. The error pattern demonstrates smoothness, effective regularization, and an overall minimal presence of outliers. The top region contains localized patterns of higher error values (illustrated as collection of red pixels), however despite these localized artifacts, the remainder of the image demonstrates the model’s accuracy with no visible orthogonal fringe patterns.</p>
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<p>Comparison of ground truth (<b>left</b>) and VUDNet-estimated depth maps (<b>right</b>), showing effective noise reduction and fine detail retention. The top images showcase a result for a deformation sample, while the bottom images represent an example of the geometric case.</p>
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<p>VAE representation (<b>left</b>) showcasing distinct separation of clusters in the latent space, visualized as the first and second components of t-SNE. The clustering indicates effective differentiation of surface characteristics and potent feature extraction. The four images on the right correspond to the selected points in the latent space (<b>right</b>). It is evident that images from a given cluster share related surface characteristics, highlighting the network’s ability to identify underlying similarities despite variations in surface characteristics.</p>
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<p>The image panels here are organized the same as in <a href="#applsci-14-10824-f006" class="html-fig">Figure 6</a>, with the latent space (<b>left</b>) visualized from the first and second components of t-SNE, and the images (<b>right</b>) corresponding to the selected points in the latent space. The difference is that <a href="#applsci-14-10824-f006" class="html-fig">Figure 6</a> was trained on the entire dataset, whereas here it is trained exclusively on the deformation data. It is clear that images positioned closer in the latent space share more similarities in reflection shape, while those farther apart are less similar, even though they belong to the same overall category of deformation surfaces. This emphasizes the network’s capability to capture underlying similarities despite variations in surface characteristics within the same category.</p>
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29 pages, 3406 KiB  
Article
Comparison of Prediction Models for Sonic Boom Ground Signatures Under Realistic Flight Conditions
by Jacob Jäschke, Samuele Graziani, Francesco Petrosino, Antimo Glorioso and Volker Gollnick
Aerospace 2024, 11(12), 962; https://doi.org/10.3390/aerospace11120962 - 22 Nov 2024
Viewed by 374
Abstract
This paper presents a comparative analysis of simplified and high-fidelity sonic boom prediction methods to assess their applicability in the conceptual design of supersonic aircraft. The high-fidelity approach combines Computational Fluid Dynamics (CFD) for near-field shock analysis with ray-tracing and the Augmented Burgers [...] Read more.
This paper presents a comparative analysis of simplified and high-fidelity sonic boom prediction methods to assess their applicability in the conceptual design of supersonic aircraft. The high-fidelity approach combines Computational Fluid Dynamics (CFD) for near-field shock analysis with ray-tracing and the Augmented Burgers Equation for far-field propagation through a non-uniform atmosphere, whereas the simplified Carlson method uses analytical approximations for rapid predictions. The comparison across selected climb, cruise, and descent conditions for a supersonic reference aircraft shows that the Carlson method captures general trends in sonic boom behavior, such as changes in peak overpressure and signal duration with varying Mach number and altitude. However, significant deviations are noted under realistic atmospheric conditions, highlighting limitations in the simplified model’s accuracy. Common psycho-acoustic metrics were evaluated to assess the potential annoyance on the ground. The results demonstrate that while the simplified method is effective for early-stage design assessments, the high-fidelity model is essential for precise sonic boom characterization under realistic conditions, particularly for regulatory and community impact evaluations. Full article
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<p>Simulation domains for state-of-the-art sonic boom prediction. The near-field domain is computed via CFD methods while the far-field domain accounts for the atmospheric variations and is modeled with a combination of ray-tracing and a non-linear wave equation. Adapted from [<a href="#B16-aerospace-11-00962" class="html-bibr">16</a>].</p>
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<p>Details of the CFD computational domain. (<b>a</b>) Unstructured and structured region of the CFD near-field mesh. (<b>b</b>) Computational domain of the CFD near-field simulation.</p>
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<p>Definition of the ray-tracing azimuth angles <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math> around an aircraft flying towards the reader. Positive azimuth angles are defined towards port side, negative azimuth angles towards starboard side.</p>
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<p>Geometry model of CS1.</p>
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<p>CS1 mission profile and associated Angle of Attack.</p>
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<p>Properties of the three reference atmospheres for the current study. The pressure profiles of both cases of SBPW3 are almost identical, such that the orange line is hidden by the green one in the pressure plot. The wind velocities in both directions are zero for the windless ISA case.</p>
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<p>Extracted near-field pressure signatures from the CFD solution at a radial distance of <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>=</mo> <mn>1</mn> <mi>L</mi> <mo>=</mo> <mn>62</mn> <mspace width="0.166667em"/> <mi mathvariant="normal">m</mi> </mrow> </semantics></math> for the three operating conditions of CS1. The azimuth angle of <math display="inline"><semantics> <mrow> <mi>ϕ</mi> <mo>=</mo> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math> shows the extracted pressure signal below the aircraft (on-track). The right plot shows an exemplary pressure signature extracted at off-track conditions for an azimuth angle of <math display="inline"><semantics> <mrow> <mi>ϕ</mi> <mo>=</mo> <mn>40</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
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<p>Computed primary sonic boom footprint for CS1 flying towards east. The marks depict the ground intersection points of the computed rays. The labels show the values of the limiting azimuth angles <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math>. <b>ISA</b> shows the footprint in the windless International Standard Atmosphere, <b>SBPW3 Case 1</b> for the realistic atmosphere from the Third Sonic Boom Prediction Workshop (SBPW3) with a wide range of azimuth angles, and <b>SBPW3 Case 2</b> the SBPW3 case for a realistic atmosphere that is intended to result in a particular wide carpet.</p>
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<p>Computed shock wave pressure signatures at ground level for the three operating conditions of CS1 in the International Standard Atmosphere. The azimuth angle of <math display="inline"><semantics> <mrow> <mi>ϕ</mi> <mo>=</mo> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math> shows the on-track sonic boom and the right plot shows an exemplary off-track sonic boom, computed for an azimuth angle of <math display="inline"><semantics> <mrow> <mi>ϕ</mi> <mo>=</mo> <mn>40</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
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<p>Computed shock wave pressure signatures at ground level for the three operating conditions of CS1 in the realistic atmospheres of the Third Sonic Boom Prediction Workshop (SBPW3). The left plot depicts case 1 and the right plot depicts case 2. The azimuth angle of <math display="inline"><semantics> <mrow> <mi>ϕ</mi> <mo>=</mo> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math> is plotted with solid lines. Dash-dotted lines show an exemplary off-track sonic boom at an azimuth angle of <math display="inline"><semantics> <mrow> <mi>ϕ</mi> <mo>=</mo> <mn>40</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
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<p>Computed acoustic sonic boom carpet as observed at ground level for the three operating conditions of CS1 flying towards east (i.e., towards the reader) in the International Standard Atmosphere. The left plot shows the distribution of peak amplitudes over the sonic boom carpet, and the right plot shows the distribution of Stevens’ Perceived Level of Noise Mk VII.</p>
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<p>Computed sonic boom carpet at ground level for the three operating conditions of CS1 flying towards east in the first realistic atmosphere of SBPW3. The left plot shows the distribution of peak amplitudes over the sonic boom carpet, and the right plot shows the distribution of Stevens’ Perceived Level of Noise Mk VII.</p>
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<p>Computed sonic boom carpet at ground level for the three operating conditions of CS1 flying towards the east in the second realistic atmosphere of SBPW3. The left plot shows the distribution of peak amplitudes over the sonic boom carpet, and the right plot shows the distribution of Stevens’ Perceived Level of Noise Mk VII.</p>
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16 pages, 30693 KiB  
Article
LM-CycleGAN: Improving Underwater Image Quality Through Learned Perceptual Image Patch Similarity and Multi-Scale Adaptive Fusion Attention
by Jiangyan Wu, Guanghui Zhang and Yugang Fan
Sensors 2024, 24(23), 7425; https://doi.org/10.3390/s24237425 - 21 Nov 2024
Viewed by 359
Abstract
The underwater imaging process is often hindered by high noise levels, blurring, and color distortion due to light scattering, absorption, and suspended particles in the water. To address the challenges of image enhancement in complex underwater environments, this paper proposes an underwater image [...] Read more.
The underwater imaging process is often hindered by high noise levels, blurring, and color distortion due to light scattering, absorption, and suspended particles in the water. To address the challenges of image enhancement in complex underwater environments, this paper proposes an underwater image color correction and detail enhancement model based on an improved Cycle-consistent Generative Adversarial Network (CycleGAN), named LPIPS-MAFA CycleGAN (LM-CycleGAN). The model integrates a Multi-scale Adaptive Fusion Attention (MAFA) mechanism into the generator architecture to enhance its ability to perceive image details. At the same time, the Learned Perceptual Image Patch Similarity (LPIPS) is introduced into the loss function to make the training process more focused on the structural information of the image. Experiments conducted on the public datasets UIEB and EUVP demonstrate that LM-CycleGAN achieves significant improvements in Structural Similarity Index (SSIM), Peak Signal-to-Noise Ratio (PSNR), Average Gradient (AG), Underwater Color Image Quality Evaluation (UCIQE), and Underwater Image Quality Measure (UIQM). Moreover, the model excels in color correction and fidelity, successfully avoiding issues such as red checkerboard artifacts and blurred edge details commonly observed in reconstructed images generated by traditional CycleGAN approaches. Full article
(This article belongs to the Collection Computational Imaging and Sensing)
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<p>Network structure of LM-CycleGAN. <math display="inline"><semantics> <mrow> <mi>X</mi> </mrow> </semantics></math> denotes the underwater degraded image domain and <math display="inline"><semantics> <mrow> <mi>Y</mi> </mrow> </semantics></math> denotes the underwater high-quality image domain.</p>
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<p>The network structure of the LM-CycleGAN generator, where the MLP is the Multi-Layer Perceptron, “n*nConv” denotes an operation that involves processing with a single convolutional kernel, and “⊕” denotes element-wise addition.</p>
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<p>Network structure of Multi-scale Adaptive Fusion Attention (MAFA), where the dilation rates are set to [<a href="#B1-sensors-24-07425" class="html-bibr">1</a>,<a href="#B2-sensors-24-07425" class="html-bibr">2</a>,<a href="#B3-sensors-24-07425" class="html-bibr">3</a>,<a href="#B4-sensors-24-07425" class="html-bibr">4</a>], and the number of ‘heads’ is set to 8.</p>
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<p>Network structure of LM-CycleGAN discriminator. Assuming the input is an RGB image with dimensions 3 × 256 × 256 pixels, the final output will be a tensor of size 1 × 30 × 30.</p>
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<p>Original image and its edge image and generated image and its edge image: (<b>a</b>) Underwater degraded image; (<b>b</b>) Edge image corresponding to the underwater degraded image; (<b>c</b>) Generated underwater high-quality image; (<b>d</b>) Edge image corresponding to the underwater high-quality image.</p>
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<p>The network structure of Learned Perceptual Image Patch Similarity (LPIPS), <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ω</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> denotes the specific weight layer corresponding to the ith output layer.</p>
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<p>Sample images from the UIEB, EUVP, and RUIE datasets: (<b>a</b>,<b>b</b>) underwater degraded images and their corresponding reference images from the UIEB dataset; (<b>c</b>,<b>d</b>) underwater degraded images and their corresponding reference images from the EUVP dataset; (<b>e</b>) underwater degraded images from the RUIE dataset.</p>
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<p>Visual comparison of image enhancement algorithms on the UIEB dataset.</p>
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<p>Visual comparison of image enhancement algorithms on the EUVP dataset.</p>
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<p>Visual comparison of image enhancement algorithms on the RUIE dataset.</p>
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<p>Comparison of enhancement effects from different strategies on the UIEB dataset, where the red box highlights local enhancement areas.</p>
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32 pages, 17378 KiB  
Article
High-Fidelity Infrared Remote Sensing Image Generation Method Coupled with the Global Radiation Scattering Mechanism and Pix2PixGAN
by Yue Li, Xiaorui Wang, Chao Zhang, Zhonggen Zhang and Fafa Ren
Remote Sens. 2024, 16(23), 4350; https://doi.org/10.3390/rs16234350 - 21 Nov 2024
Viewed by 228
Abstract
 To overcome the problems in existing infrared remote sensing image generation methods, which make it difficult to combine high fidelity and high efficiency, we propose a High-Fidelity Infrared Remote Sensing Image Generation Method Coupled with the Global Radiation Scattering Mechanism and Pix2PixGAN (HFIRSIGM_GRSMP) [...] Read more.
 To overcome the problems in existing infrared remote sensing image generation methods, which make it difficult to combine high fidelity and high efficiency, we propose a High-Fidelity Infrared Remote Sensing Image Generation Method Coupled with the Global Radiation Scattering Mechanism and Pix2PixGAN (HFIRSIGM_GRSMP) in this paper. Firstly, based on the global radiation scattering mechanism, the HFIRSIGM_GRSMP model is constructed to address the problem of accurately characterizing factors that affect fidelity—such as the random distribution of the radiation field, multipath scattering, and nonlinear changes—through the innovative fusion of physical models and deep learning. This model accurately characterizes the complex radiation field distribution and the image detail-feature mapping relationship from visible-to-infrared remote sensing. Then, 8000 pairs of image datasets were constructed based on Landsat 8 and Sentinel-2 satellite data. Finally, the experiment demonstrates that the average SSIM of images generated using HFIRSIGM_GRSMP reaches 89.16%, and all evaluation metrics show significant improvement compared to the contrast models. More importantly, this method demonstrates high accuracy and strong adaptability in generating short-wave, mid-wave, and long-wave infrared remote sensing images. This method provides a more comprehensive solution for generating high-fidelity infrared remote sensing images.  Full article
(This article belongs to the Special Issue Deep Learning Innovations in Remote Sensing)
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<p>Remote sensing imaging mechanisms: (<b>a</b>) global radiation scattering mechanism, and (<b>b</b>) remote sensing imaging chain process.</p>
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<p>The overall architecture of the methodology of this paper.</p>
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<p>The process for obtaining the spectral reflectance of land cover materials includes references to the following databases: USGS, which stands for the United States Geological Survey; JHU, which represents Johns Hopkins University; and JPL, which refers to the Jet Propulsion Laboratory.</p>
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<p>Material matching results: (<b>a</b>) the matching results for classification of materials, and (<b>b</b>) the material spectral reflectance curve.</p>
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<p>Imaging radiometric feature mapping calculation results: (<b>a</b>) SWIR (1.566–1.651 μm) results, (<b>b</b>) MWIR (3.0–5.0 μm) results, (<b>c</b>) LWIR (10.6–11.19 μm) results, and (<b>d</b>) the visible image.</p>
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<p>The generator module architecture designed in this paper: (<b>a</b>) generator architecture, and (<b>b</b>) Fast Fourier Channel Spatial Attention Mechanism (FFCSAM).</p>
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<p>The generator module architecture designed in this paper: (<b>a</b>) generator architecture, and (<b>b</b>) Fast Fourier Channel Spatial Attention Mechanism (FFCSAM).</p>
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<p>The architecture of the proposed discriminator module includes (<b>a</b>) multi-scale feature fusion and (<b>b</b>) deformable convolution.</p>
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<p>Comprehensive loss components.</p>
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<p>Sample images of the dataset: (<b>a</b>) visible light, (<b>b</b>) SWIR, (<b>c</b>) MWIR, and (<b>d</b>) LWIR.</p>
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<p>Examples of SWIR remote sensing images generated using different methods: (<b>a</b>) on the Landsat 8 dataset, and (<b>b</b>) on the Sentinel-2 dataset.</p>
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<p>Examples of SWIR remote sensing images generated using different methods: (<b>a</b>) on the Landsat 8 dataset, and (<b>b</b>) on the Sentinel-2 dataset.</p>
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<p>Examples of MWIR remote sensing images generated using different methods on the Landsat 8 dataset.</p>
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<p>Examples of LWIR remote sensing images generated using different methods on the Landsat 8 dataset.</p>
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<p>Comparison of evaluation metric values obtained from HFIRSIGM_GRSMP and Pix2PixGAN: (<b>a</b>) PSNR, (<b>b</b>) SSIM, (<b>c</b>) UQI, (<b>d</b>) FID, and (<b>e</b>) LPIPS.</p>
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<p>Statistical results of the percentage of intervals corresponding to the values of the evaluation indicators for each model: (<b>a</b>) PSNR, (<b>b</b>) SSIM, (<b>c</b>) UQI, (<b>d</b>) FID, and (<b>e</b>) LPIPS. In the figure, an upward arrow indicates that the larger the metric, the better the image quality, while a downward arrow indicates that the smaller the metric, the better the image quality.</p>
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<p>Statistical results of the percentage of intervals corresponding to the values of the evaluation indicators for each model: (<b>a</b>) PSNR, (<b>b</b>) SSIM, (<b>c</b>) UQI, (<b>d</b>) FID, and (<b>e</b>) LPIPS. In the figure, an upward arrow indicates that the larger the metric, the better the image quality, while a downward arrow indicates that the smaller the metric, the better the image quality.</p>
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16 pages, 4761 KiB  
Article
Non-Uniform Turbulence Modeling in Isolated Unsteady Diffuser Computational Models for a Vaned Centrifugal Compressor
by Benjamin L. Holtmann and Nicole L. Key
Fluids 2024, 9(12), 270; https://doi.org/10.3390/fluids9120270 - 21 Nov 2024
Viewed by 292
Abstract
Recent advancements in computational fluid dynamics (CFD) enable new and more complex analysis methods to be developed for early design stages. One such method is the isolated unsteady diffuser model, which seeks to reduce the computational cost of unsteady CFD when modeling diffusion [...] Read more.
Recent advancements in computational fluid dynamics (CFD) enable new and more complex analysis methods to be developed for early design stages. One such method is the isolated unsteady diffuser model, which seeks to reduce the computational cost of unsteady CFD when modeling diffusion systems in centrifugal compressors with vaned diffusers by isolating the diffuser from the computational domain and prescribing an unsteady and periodic inlet boundary condition. An initial iteration of this computational methodology was developed and validated for the Centrifugal Stage for Aerodynamic Research (CSTAR) at the High-Speed Compressor Laboratory at Purdue University. However, that work showed discrepancies in flow structure predictions between full-stage and isolated unsteady CFD models, and it also presented a narrow scope of only a single loading condition. Thus, this work addresses the need for improvement in the modeling fidelity. The original methodology was expanded by including a more accurate, non-uniform definition of turbulence at the diffuser inlet and modeling several loading conditions ranging from choke to surge. Results from isolated unsteady diffuser models with non-uniform turbulence modeling were compared with uniform turbulence isolated unsteady diffuser models and full-stage unsteady models at four loading conditions along a speedline. Flow structure predictions by the three methodologies were compared using 1D parameters and outlet total pressure and midspan velocity contours. The comparisons indicate a significant improvement in 1D parameter and flow structure predictions by the isolated unsteady diffuser models at all four loading conditions when including more accurate non-uniform turbulence, without a corresponding increase in computational cost. Additionally, both isolated diffuser methodologies accurately track trends in 3D flow structures along the speedline. Full article
(This article belongs to the Special Issue Industrial CFD and Fluid Modelling in Engineering, 2nd Edition)
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<p>Jet-wake interaction at impeller outlet [<a href="#B1-fluids-09-00270" class="html-bibr">1</a>].</p>
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<p>CSTAR Gen 2.5 compressor cutaway [<a href="#B22-fluids-09-00270" class="html-bibr">22</a>].</p>
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<p>Compressor performance map (<b>a</b>) and efficiency map (<b>b</b>) indicating relative positions of high loading, design point, low loading, and near choke conditions.</p>
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<p>Definition of domains and interfaces for full-stage unsteady model (<b>a</b>) and isolated unsteady diffuser model (<b>b</b>).</p>
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<p>Comparison of total pressure ratio (<b>a</b>) and isentropic efficiency (<b>b</b>) from experimental data, full-stage steady state computational models and full-stage unsteady computational models at all four loading conditions.</p>
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<p>Comparison of static pressure recovery coefficient, C<sub>p</sub> (<b>a</b>), and total pressure loss coefficient, K (<b>b</b>), for full-stage unsteady, UT isolated unsteady diffuser, and NUT isolated unsteady diffuser models.</p>
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<p>Diffuser passage outlet normalized total pressure contours for full-stage unsteady, UT isolated unsteady diffuser, and NUT isolated unsteady diffuser models at high loading (HL), design point (DP), low loading (LL), and near choke (NC).</p>
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<p>Normalized midspan absolute velocity magnitude contours for full-stage unsteady, UT isolated unsteady diffuser, and NUT isolated unsteady diffuser models at high loading (HL), design point (DP), low loading (LL), and near choke (NC).</p>
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<p>Difference in midspan normalized absolute velocity magnitude predictions for full-stage unsteady, UT isolated unsteady diffuser, and NUT isolated unsteady diffuser models at high loading (HL), design point (DP), low loading (LL), and near choke (NC).</p>
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<p>Normalized total pressure differences at diffuser throat, 50% chord, and diffuser passage outlet at design point loading for UT isolated unsteady diffuser and NUT isolated unsteady diffuser models.</p>
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