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23 pages, 9009 KiB  
Article
Four-Dimensional Trajectory Optimization for CO2 Emission Benchmarking of Arrival Traffic Flow with Point Merge Topology
by Chao Wang, Chenyang Xu, Wenqing Li, Shanmei Li and Shilei Sun
Aerospace 2024, 11(8), 673; https://doi.org/10.3390/aerospace11080673 - 16 Aug 2024
Viewed by 502
Abstract
The benchmarking of CO2 emissions serves as the foundation for the accurate assessment of the environmental impact of air traffic. To calculate the environmental benchmarks of arrival traffic flows with Point Merge System (PMS) patterns, this study proposes a 4D trajectory optimization [...] Read more.
The benchmarking of CO2 emissions serves as the foundation for the accurate assessment of the environmental impact of air traffic. To calculate the environmental benchmarks of arrival traffic flows with Point Merge System (PMS) patterns, this study proposes a 4D trajectory optimization method that combines data-driven and optimal control models. First, the predominant arrival routes of traffic flows are identified using the trajectory spectral clustering method, which provides the horizontal reference for 4D trajectory optimization. Second, an optimal control model for vertical profiles with point merging topology is established, with the objective of minimizing the fuel–time cost. Finally, considering the complex structure of the PMS, a flexible and adaptable genetic algorithm-based vertical profile nonlinear optimization model is created. The experimental results demonstrate that the proposed method is adaptable to variations in aircraft type and cost index parameters, enabling the generation of different 4D trajectories. The results also indicate an environmental efficiency gap of approximately 10% between the actual CO2 emissions of the arrival traffic flow example and the obtained benchmark. With this benchmark trajectory generation methodology, the environmental performance of PMSs and associated arrival aircraft scheduling designs can be assessed on the basis of reliable data. Full article
(This article belongs to the Section Aeronautics)
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<p>The framework of the proposed method.</p>
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<p>Spherical segment–path distance between trajectories: (<b>a</b>) the distance from point <span class="html-italic">O</span> to trajectory <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>T</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math>; (<b>b</b>) the spherical segment–path distance from <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>T</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> to <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>T</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>Route structure of point merge system.</p>
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<p>Typical CDO process of point merge procedure.</p>
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<p>Arrival CAS profile model, represented by seven decision variables.</p>
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<p>PVG airspace configuration and arrival trajectories.</p>
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<p>Five arrival traffic flows identified using spectral clustering.</p>
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<p>Comparison of core trajectories generated by <span class="html-italic">k</span>-medoids and AP clustering.</p>
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<p>The optimized 4D trajectory with <span class="html-italic">CI</span> = 30: (<b>a</b>) vertical profile; and (<b>b</b>) optimized trajectory.</p>
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<p>Fuel flow comparison: (<b>a</b>) real trajectory; and (<b>b</b>) optimized trajectory.</p>
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<p>Comparison of results between actual trajectory and optimized trajectories.</p>
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<p>Comparison of glide path angles derived from GACDO, GPOPS, and the actual trajectory.</p>
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<p>Trajectory optimization results for different <span class="html-italic">CI</span> values: (<b>a</b>) altitude profile; and (<b>b</b>) CAS profile.</p>
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<p>Comparison of actual and optimized altitude profiles in arrival traffic flow <span class="html-italic">F</span><sub>4</sub>.</p>
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28 pages, 11615 KiB  
Article
Identifying the Nonlinear Impacts of Road Network Topology and Built Environment on the Potential Greenhouse Gas Emission Reduction of Dockless Bike-Sharing Trips: A Case Study of Shenzhen, China
by Jiannan Zhao, Changwei Yuan, Xinhua Mao, Ningyuan Ma, Yaxin Duan, Jinrui Zhu, Hujun Wang and Beisi Tian
ISPRS Int. J. Geo-Inf. 2024, 13(8), 287; https://doi.org/10.3390/ijgi13080287 - 16 Aug 2024
Viewed by 489
Abstract
Existing studies have limited evidence about the complex nonlinear impact mechanism of road network topology and built environment on bike-sharing systems’ greenhouse gas (GHG) emission reduction benefits. To fill this gap, we examine the nonlinear effects of road network topological attributes and built [...] Read more.
Existing studies have limited evidence about the complex nonlinear impact mechanism of road network topology and built environment on bike-sharing systems’ greenhouse gas (GHG) emission reduction benefits. To fill this gap, we examine the nonlinear effects of road network topological attributes and built environment elements on the potential GHG emission reduction of dockless bike-sharing (DBS) trips in Shenzhen, China. Various methods are employed in the research framework of this study, including a GHG emission reduction estimation model, spatial design network analysis (sDNA), gradient boosting decision tree (GBDT), and partial dependence plots (PDPs). Results show that road network topological variables have the leading role in determining the potential GHG emission reduction of DBS trips, followed by land use variables and transit-related variables. Moreover, the nonlinear impacts of road network topological variables and built environment variables show certain threshold intervals for the potential GHG emission reduction of DBS trips. Furthermore, the impact of built environment on the potential GHG emission reduction of DBS trips is moderated by road network topological indicators (closeness and betweenness). Compared with betweenness, closeness has a greater moderating effect on built environment variables. These findings provide empirical evidence for guiding bike-sharing system planning, bike-sharing rebalancing strategy optimization, and low-carbon travel policy formulation. Full article
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<p>Research framework. (<b>a</b>) Estimating the potential GHG emission reduction of DBS trips which is utilized as dependent variable; (<b>b</b>) Extracting the independent variables, including road network topological variables and built environment variables; (<b>c</b>) Identifying the nonlinear impacts of road network topology and built environment on the potential GHG emission reduction of DBS trips.</p>
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<p>Study area and analysis grids.</p>
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<p>Spatial distribution of the potential GHG emission reduction of DBS trips in Shenzhen.</p>
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<p>Road networks and their topological measurements in Shenzhen: (<b>a</b>) NQPDA5000; (<b>b</b>) TPBtA5000.</p>
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<p>The city centers of Shenzhen.</p>
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<p>Nonlinear and threshold effects of road network topological variables and built environment variables on the potential GHG emission reduction of DBS trips: (<b>a</b>) NQPDA5000; (<b>b</b>) TPBtA5000; (<b>c</b>) Distance to the nearest metro station; (<b>d</b>) Distance to the nearest bus stop; (<b>e</b>) Population density; (<b>f</b>) Distance to the nearest city center; (<b>g</b>) Enterprise density; (<b>h</b>) POI mix entropy.</p>
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<p>Nonlinear and threshold effects of road network topological variables and built environment variables on the potential GHG emission reduction of DBS trips: (<b>a</b>) NQPDA5000; (<b>b</b>) TPBtA5000; (<b>c</b>) Distance to the nearest metro station; (<b>d</b>) Distance to the nearest bus stop; (<b>e</b>) Population density; (<b>f</b>) Distance to the nearest city center; (<b>g</b>) Enterprise density; (<b>h</b>) POI mix entropy.</p>
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<p>Interaction effects of road network topological variables and built environment variables on the potential GHG emission reduction of DBS trips: (<b>a1</b>–<b>a6</b>) represent the moderate effects of NQPDA5000 on the other six most important built environment variables; (<b>b1</b>–<b>b6</b>) represent the moderate effects of TPBtA5000 on the other six most important built environment variables.</p>
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17 pages, 3403 KiB  
Article
Innovative Tools for DNA Topology Probing in Human Cells Reveal a Build-Up of Positive Supercoils Following Replication Stress at Telomeres and at the FRA3B Fragile Site
by Claire Ghilain, Olivia Vidal-Cruchez, Aurélia Joly, Michelle Debatisse, Eric Gilson and Marie-Josèphe Giraud-Panis
Cells 2024, 13(16), 1361; https://doi.org/10.3390/cells13161361 - 15 Aug 2024
Viewed by 552
Abstract
Linear unconstrained DNA cannot harbor supercoils since these supercoils can diffuse and be eliminated by free rotation of the DNA strands at the end of the molecule. Mammalian telomeres, despite constituting the ends of linear chromosomes, can hold supercoils and be subjected to [...] Read more.
Linear unconstrained DNA cannot harbor supercoils since these supercoils can diffuse and be eliminated by free rotation of the DNA strands at the end of the molecule. Mammalian telomeres, despite constituting the ends of linear chromosomes, can hold supercoils and be subjected to topological stress. While negative supercoiling was previously observed, thus proving the existence of telomeric topological constraints, positive supercoils were never probed due to the lack of an appropriate tool. Indeed, the few tools available currently could only investigate unwound (Trioxsalen) or overwound (GapR) DNA topology (variations in twist) but not the variations in writhe (supercoils and plectonemes). To address this question, we have designed innovative tools aimed at analyzing both positive and negative DNA writhe in cells. Using them, we could observe the build-up of positive supercoils following replication stress and inhibition of Topoisomerase 2 on telomeres. TRF2 depletion caused both telomere relaxation and an increase in positive supercoils while the inhibition of Histone Deacetylase I and II by TSA only caused telomere relaxation. Moving outside telomeres, we also observed a build-up of positive supercoils on the FRA3B fragile site following replication stress, suggesting a topological model of DNA fragility for this site. Full article
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<p>In vitro topological properties of Topotools. (<b>a</b>) Schematics of Topotools proteins. For purification purposes, recombinant Topotools were fused to an N-terminal (His)6 tag. (<b>b</b>) 2D Gels of Topo assays where 1 µM Topotools were incubated with a relaxed circular plasmid in the presence of wheat germ Topoisomerase I. Note the appearance of topoisomers and their inverse orientation. Chloroquine, which creates (+) supercoils, increases migration for RFP-GyrA CTD topoisomers, indicating that RFP-GyrA CTD also creates (+) supercoils. In contrast, chloroquine slows down migration for RFP-HMfB topoisomers, indicating that RFP-HMfB creates (−) supercoils.</p>
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<p>Topotools bind chromatin all along mitosis. Representative images of fixed Topotools-expressing HT1080 ST cells synchronized by treatment with RO-3306 and then released. Images were taken at different time points, allowing observation of different stages of mitosis. Cells were fixed and no labeling or IF were performed. DAPI and Topotools RFP signals were monitored.</p>
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<p>Topoisomerase 2 inhibition and replication stress cause a build-up of positive supercoils on telomeres. (<b>a</b>) Representative images of Hela-38 cells transduced by Topotools-expressing lentiviruses and treated with ICRF-193 at 35 µM for 5 h. Topotools were detected by IF using a rat anti-HA antibody and telomeres by PNA FISH using a telomeric probe. Circles indicate co-localizations. (<b>b</b>) Quantification of the co-localizations between Topotools and telomeres observed in the experiment shown in (<b>a</b>). Statistics were performed compared to control condition using Kruskal–Wallis followed by Dunn tests. **** <span class="html-italic">p</span> &lt; 0.0001. (<b>c</b>) Representative Slot blot of ChIP experiments performed with HT1080 ST transduced by Topotools-expressing or Empty lentiviruses. Cells were treated using 150 nM of Aphidicolin and 10 µM of ICRF-193 for 24 h. Topotools-bound chromatin was immuno-precipitated using an anti-HA antibody. (<b>d</b>) Quantification of the ChIP experiment. Error bars represent maximal values obtained between two biological replicates.</p>
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<p>Inhibition of HDAC I and II by Trichostatin-A (TSA) causes telomere relaxation. Quantification of the co-localizations between Topotools and telomeres observed in Hela-38 cells transduced by Topotools-expressing lentiviruses and treated with 2.5 µM of TSA for 5 h. Topotools were detected by IF using a rat anti-HA antibody and telomeres by PNA FISH using a telomeric probe. Statistics were performed compared to control condition using Kruskal–Wallis tests followed by Dunn tests. *** <span class="html-italic">p</span> &lt; 0.001.</p>
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<p>Knockdown of TRF2 causes supercoil build-up on telomeres. (<b>a</b>) Representative images of HCT116 cells expressing the corresponding Topotools and transfected with vectors expressing either a siRNA targeting <span class="html-italic">TERF2</span> mRNA or a siRNA of identical composition but with a random sequence (siCtrl). Topotools were detected by IF using a rat anti-HA antibody and telomeres by PNA FISH using a telomeric probe (Telo). Circles indicate co-localizations. (<b>b</b>) Quantification of the co-localizations between Topotools and telomeres observed in the experiment shown in (<b>a</b>). Statistics were performed compared to control conditions using Kruskal–Wallis tests followed by Dunn tests. **** <span class="html-italic">p</span> &lt; 0.0001. (<b>c</b>) QPCR analysis of TRF2 expression in the HCT116 cells used in (<b>a</b>). (<b>d</b>) Western blot showing Topotools and Actin expression in the experiment shown in Figure (<b>a</b>). Anti-tRFP and anti-Actin antibodies were used.</p>
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<p>Mild replication stress causes topological changes in the <span class="html-italic">FHIT</span> gene. Top: graphical representation of the <span class="html-italic">FHIT</span> gene and position of primers pairs used to analyze ChIP samples. Bottom: quantitative analysis of ChIP samples by qPCR using primers pairs A to F and performed on HCT116 cells expressing the Topotools and the RFP control. Three conditions were analyzed: DMSO (− DOX), Doxycyclin induction of Topotool expression (+ DOX), and Doxycyclin induction and treatment with Aphidicolin (150 nM for 24 h, + DOX + APH). Antibodies used were rat anti-HA and rat IgG.</p>
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17 pages, 60730 KiB  
Article
Topology Optimization with Explicit Components Considering Stress Constraints
by Yubao Ma, Zhiguo Li, Yuxuan Wei and Kai Yang
Appl. Sci. 2024, 14(16), 7171; https://doi.org/10.3390/app14167171 - 15 Aug 2024
Viewed by 556
Abstract
Topology optimization focuses on the conceptual design of structures, characterized by a large optimization space and a significant impact on structural performance, and has been widely applied in industrial fields such as aviation and aerospace. However, most topology optimization methods prioritize structural stiffness [...] Read more.
Topology optimization focuses on the conceptual design of structures, characterized by a large optimization space and a significant impact on structural performance, and has been widely applied in industrial fields such as aviation and aerospace. However, most topology optimization methods prioritize structural stiffness and often overlook stress levels, which are critical factors in engineering design. In recent years, explicit topology optimization methods have been extensively developed due to their ability to produce clear boundaries and their compatibility with CAD/CAE systems. Nevertheless, research on incorporating stress constraints within the explicit topology optimization framework remains scarce. This paper is dedicated to investigating stress constraints within the explicit topology optimization framework. Due to the clear boundaries and absence of intermediate density elements in the explicit topology optimization framework, this approach avoids the challenge of stress calculation for intermediate density elements encountered in the traditional density method. This provides a natural advantage in solving topology optimization problems considering stress constraints, resulting in more accurate stress calculations. Compared with existing approaches, this paper proposes a novel component topology description function that enhances the deformability of components, improving the representation of geometric boundaries. The lower-bound Kreisselmeier–Steinhauser aggregation function is employed to manage the stress constraint, reducing the solution scale and computational burden. The effectiveness of the proposed method is demonstrated through two classic examples of topology optimization. Full article
(This article belongs to the Special Issue Structural Optimization Methods and Applications, 2nd Edition)
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<p>Comparison of two types of topology optimization methods applied to the short beam example. (<b>a</b>) Optimization results obtained using the implicit topology optimization method. (<b>b</b>) Optimization results obtained using the explicit topology optimization method.</p>
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<p>Schematic diagram illustrating the SIMP-MMC hybrid algorithm. (<b>a</b>) The initial force path, derived from the SIMP method, is extracted and mapped onto the component layout. (<b>b</b>) The final optimized result obtained using the MMC method [<a href="#B8-applsci-14-07171" class="html-bibr">8</a>].</p>
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<p>The designs of the L-shape beam in recent research. (<b>a</b>) Optimized result obtained by Dixiong Yang et al. using the implicit topology optimization method in 2018 [<a href="#B15-applsci-14-07171" class="html-bibr">15</a>]. (<b>b</b>) Optimized result obtained by Senhora et al. using the implicit topology optimization method in 2020 [<a href="#B16-applsci-14-07171" class="html-bibr">16</a>]. (<b>c</b>) Optimized result obtained by Xiaoya Zhai et al. using the implicit topology optimization method in 2021 [<a href="#B17-applsci-14-07171" class="html-bibr">17</a>]. (<b>d</b>) Optimized result obtained by Gustavo Assis da Silva et al. using the implicit topology optimization method in 2021 [<a href="#B18-applsci-14-07171" class="html-bibr">18</a>]. (<b>e</b>) Optimized result obtained by Shanglong Zhang et al. using the explicit topology optimization method in 2017 [<a href="#B19-applsci-14-07171" class="html-bibr">19</a>]. (<b>f</b>) Optimized result obtained by Weisheng Zhang et al. using the explicit topology optimization method in 2018 [<a href="#B20-applsci-14-07171" class="html-bibr">20</a>]. (<b>g</b>) Optimized result obtained by Pooya Rostami et al. using the explicit topology optimization method in 2021 [<a href="#B21-applsci-14-07171" class="html-bibr">21</a>].</p>
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<p>Schematic diagram of topology optimization of the short beam example based on the MMC method. (<b>a</b>) Initial layout of the components. (<b>b</b>) Movement and deformation of the components during the early stages of the optimization process. (<b>c</b>) Movement and deformation of the components during the later stages of the optimization process. (<b>d</b>) Optimized layout of the components.</p>
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<p>Schematic diagram of component connection at the end of a straight line.</p>
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<p>Parametric description of the variability of the shape of the components.</p>
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<p>Component deformation diagrams with different parameters.</p>
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<p>The design area and the initial layout of the components of the L-shaped beam.</p>
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<p>Comparison of the optimization results before and after adding stress constraints, including the finite-element mesh and stress distribution calculated from ABAQUS.</p>
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<p>The iterative convergence curves of the objective function and the constraint function of the L-shaped beam.</p>
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<p>Some key iterative steps in the optimization process of the L-shaped beam.</p>
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<p>The design area and the initial layout of the components of the T-shaped beam.</p>
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<p>Comparison of the optimization results before and after adding stress constraints, including the finite-element mesh and stress distribution calculated from ABAQUS.</p>
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<p>The iterative convergence curves of the objective function and the constraint function of the T-shaped beam.</p>
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<p>Some key iterative steps in the optimization process of the T-shaped beam.</p>
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19 pages, 4270 KiB  
Article
Neural Network-Based Aggregated Equivalent Modeling of Distributed Photovoltaic External Characteristics of Faults
by Kuan Li, Qiang Huang, Rongqi Fan, Shuai Gao, Anning Wang, Tao Huang and Ruichen Sun
Electronics 2024, 13(16), 3232; https://doi.org/10.3390/electronics13163232 - 15 Aug 2024
Viewed by 388
Abstract
Distributed power networks have a large number of photovoltaic power sources. The bidirection of power flow, different transient control strategies, and installation locations make the transient characteristics highly complex and unpredictable. The vast network of the distribution system makes it almost impossible to [...] Read more.
Distributed power networks have a large number of photovoltaic power sources. The bidirection of power flow, different transient control strategies, and installation locations make the transient characteristics highly complex and unpredictable. The vast network of the distribution system makes it almost impossible to predict the electrical quantities of each branch. Reasonable aggregation modeling of the distribution network can greatly simplify the network topology, facilitating transient control and the setting of relay protection settings. An aggregated equivalent modeling method based on the LSTM neural network for distributed PV fault external characteristics is proposed. This method equates the complex distribution network to a highly nonlinear but controllable current source. The method can output the IV curves of equivalent PV system parallel points under any output power and is able to predict the fault characteristics of the equivalent system after a voltage drop at the parallel point. Compared to traditional mechanistic modeling, this method does not require specific modeling of complex physical systems and is able to accurately map the strong nonlinear inputs and outputs of distribution networks. The established LSTM model first uses a one-dimensional convolutional layer for feature extraction of the PV power coefficients (input), and then two hidden layers are utilized to process the sequence data; the vectors are mapped into a sequence of external characteristic curves (output) in a fully connected layer. A typical distribution network is built based on the traditional PV power model, and a large number of different output combinations are selected for simulation to provide an effective training set and validation set data for LSTM model training. By using the training set data, the weights and offset coefficients of each layer of the LSTM are continuously optimized until the model with the smallest overall error is obtained, which is the optimal model. Finally, the optimal model is utilized to establish an equivalent distribution network system, different degrees of voltage drops are set up at the grid-connected points, the fault characteristics are compared with those of the complete model, and the simulation results can prove the reliability and practicality of the proposed method. Full article
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<p>PV module equivalent circuit.</p>
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<p>PV inverter main circuit structure.</p>
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<p>A simplified flowchart of closed-loop control principle of inverter.</p>
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<p>Block diagram of DC voltage and current double closed-loop control principle of inverter.</p>
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<p>Requirements for LVRT capability of PV power plants.</p>
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<p>LSTM fundamentals.</p>
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<p>LSTM-based training process.</p>
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<p>Distributed power output aggregation modeling logic.</p>
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<p>Distributed power network topology diagram.</p>
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<p>Variation curves of line current RMS for different PV outputs.</p>
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<p>Line current phase variation curves for different PV outputs.</p>
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<p>Comparison of current RMS values of LSTM model and simulation model.</p>
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<p>Comparison of current phase between LSTM model and simulation model.</p>
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<p>Simulink simulation system based on LSTM training models.</p>
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<p>Comparison of current RMS values of LSTM model and simulation model. (<b>a</b>) Output coefficients of [1.0, 0.8, 0.4, 0.9, 0.7]; (<b>b</b>) output coefficients of [0.3, 0.2, 0.1, 0.6, 0.5].</p>
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10 pages, 2009 KiB  
Brief Report
Challenges and Solutions for Secure Key Management and Monitoring: Review of the Cerberis3 Quantum Key Distribution System
by Ints Meijers
Quantum Rep. 2024, 6(3), 426-435; https://doi.org/10.3390/quantum6030027 - 13 Aug 2024
Viewed by 443
Abstract
Quantum Key Distribution (QKD) offers a revolutionary approach to secure communication, leveraging the principles of quantum mechanics to generate and distribute cryptographic keys that are immune to eavesdropping. As QKD systems become more widely adopted, the need for robust monitoring and management solutions [...] Read more.
Quantum Key Distribution (QKD) offers a revolutionary approach to secure communication, leveraging the principles of quantum mechanics to generate and distribute cryptographic keys that are immune to eavesdropping. As QKD systems become more widely adopted, the need for robust monitoring and management solutions has become increasingly crucial. The Cerberis3 QKD system from ID Quantique addresses this challenge by providing a comprehensive monitoring and visualization platform. The system’s advanced features, including central configuration, SNMP integration, and the graphical visualization of key performance metrics, enable network administrators to ensure their QKD infrastructure’s reliable and secure operation. Monitoring critical parameters such as Quantum Bit Error Rate (QBER), secret key rate, and link visibility is essential for maintaining the integrity of the quantum channel and optimizing the system’s performance. The Cerberis3 system’s ability to interface with encryption vendors and support complex network topologies further enhances its versatility and integration capabilities. By addressing the unique challenges of quantum monitoring, the Cerberis3 system empowers organizations to leverage the power of QKD technology, ensuring the security of their data in the face of emerging quantum computing threats. This article explores the Cerberus3 system’s features and its role in overcoming the monitoring challenges inherent to QKD deployments. Full article
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<p>Experimental setup diagram.</p>
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<p>Key rate.</p>
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<p>QBER.</p>
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<p>Visibility.</p>
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<p>Detections.</p>
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<p>Compression.</p>
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26 pages, 2782 KiB  
Article
A Techno-Economic Assessment of DC Fast-Charging Stations with Storage, Renewable Resources and Low-Power Grid Connection
by Gurpreet Singh, Matilde D’Arpino and Terence Goveas
Energies 2024, 17(16), 4012; https://doi.org/10.3390/en17164012 - 13 Aug 2024
Viewed by 531
Abstract
The growing demand for high-power DC fast-charging (DCFC) stations for electric vehicles (EVs) is expected to lead to increased peak power demand and a reduction in grid power quality. To maximize the economic benefits and station utilization under practical constraints set by regulatory [...] Read more.
The growing demand for high-power DC fast-charging (DCFC) stations for electric vehicles (EVs) is expected to lead to increased peak power demand and a reduction in grid power quality. To maximize the economic benefits and station utilization under practical constraints set by regulatory authorities, utilities and DCFC station operators, this study explores and provides methods for connecting DCFC stations to the grid, employing low-power interconnection rules and distributed energy resources (DERs). The system uses automotive second-life batteries (SLBs) and photovoltaic (PV) systems as energy buffer and local energy resources to support EV charging and improve the station techno-economic feasibility through load shifting and charge sustaining. The optimal sizing of the DERs and the selection of the grid interconnection topology is achieved by means of a design space exploration (DSE) and exhaustive search approach to maximize the economic benefits of the charging station and to mitigate high-power demand to the grid. Without losing generality, this study considers a 150 kW DCFC station with a range of DER sizes, grid interconnection specifications and related electricity tariffs of American Electric Power (AEP) Ohio and the Public Utility Commission of Ohio (PUCO). Various realistic scenarios and strategies are defined to account for the interconnection requirements of the grid to the DCFC with DERs. The system’s techno-economic performance over a ten-year period for different scenarios is analyzed and compared using a multitude of metrics. The results of the analysis show that the the integration of DERs in DCFC stations has a positive impact on the economic value of the investment when compared to traditional installations. Full article
(This article belongs to the Special Issue Future Smart Energy for Electric Vehicle Charging)
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<p>Architecture of the proposed DCFC system.</p>
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<p>Modeling framework for the DCFC station with its subsystems.</p>
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<p>Classification of cost components for DCFC station.</p>
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<p>Design space exploration architecture.</p>
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<p>Analysis for the 10th day of year 1: EV load, PV power, grid power, SLB power, SLB SOC and temperature.</p>
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<p>Analysis for the 150th day of year 1: EV load, PV power, grid power, SLB power, SLB SOC and temperature.</p>
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<p>Residual capacity vs. time in months for different control architectures—Control B (<b>top plot</b>) and Control C (<b>bottom plot</b>).</p>
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<p>Residual capacity vs. mean SOC for different control architectures—Control B (<b>top plot</b>) and Control C (<b>bottom plot</b>).</p>
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<p>Sensitivity analysis for traditional DCFC—revenue (<b>left plot</b>) and demand charges and transformer cost (<b>right plot</b>).</p>
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<p>NPV results for all scenarios with all configurations and their selected controls.</p>
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<p>NPV (<b>left plot</b>) and cash flow (<b>right plot</b>) for the selected configurations with the highest NPV among all scenarios.</p>
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<p>Cost breakdown (<b>left plot</b> ) and OPEX cost (<b>right plot</b>) for the selected configurations with the highest NPV among all scenarios.</p>
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<p>Net grid energy (<b>left plot</b> ) and PV direct utilization expressed in % (<b>right plot</b>) for the highest and lowest NPV configurations among all scenarios.</p>
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16 pages, 6484 KiB  
Article
An Enhanced Six-Turn Multilayer Planar Inductor Interleaved Winding Design for LLC Resonant Converters with Low Current Ringing
by Qichen Liu and Zhengquan Zhang
Electronics 2024, 13(16), 3201; https://doi.org/10.3390/electronics13163201 - 13 Aug 2024
Viewed by 385
Abstract
Planar magnetic components have been widely used in high-density power converters and are suitable for various topologies. The application of planar inductors in LLC resonant converters can lead to parasitic capacitance, which causes current ringing and results in EMI issues. To mitigate the [...] Read more.
Planar magnetic components have been widely used in high-density power converters and are suitable for various topologies. The application of planar inductors in LLC resonant converters can lead to parasitic capacitance, which causes current ringing and results in EMI issues. To mitigate the impact of current ringing, the parasitic capacitance of the planar inductor needs to be reduced. This paper proposes a new six-turn interleaved winding design. Compared to the previous four-turn interleaved winding design, it maintains low parasitic capacitance while positioning both the input and output terminals of the inductor on the outer turn, further enhancing the integration of high-density power converters. The parasitic capacitance was calculated using theoretical methods and verified through finite element simulations. Experimental validation was conducted using an LLC resonant converter test platform. Compared to the previous four-turn interleaved winding design, the new six-turn interleaved winding design satisfies both the input and output terminals, using an outer turn configuration. Additionally, the new design exhibits reduced parasitic capacitance and is suitable for use in LLC resonant converters, where it also minimizes current ringing. Full article
(This article belongs to the Special Issue Compatibility, Power Electronics and Power Engineering)
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<p>The 3D schematic of the planar inductor winding structure: (<b>a</b>) previous 4-turn interleaved winding design; (<b>b</b>) proposed new 6-turn interleaved winding design.</p>
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<p>Previous 4-turn interleaved winding design for top and bottom layers: (<b>a</b>) top layer turns; (<b>b</b>) bottom layer turns.</p>
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<p>Proposed new 6-turn interleaved winding design for top and bottom layers: (<b>a</b>) top layer turns; (<b>b</b>) bottom layer turns.</p>
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<p>The 3D simulation model in Ansys Maxwell: (<b>a</b>) 4-turn interleaved winding; (<b>b</b>) 6-turn interleaved winding.</p>
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<p>Simulation results of the electric field strength on the XY plane: (<b>a</b>) 4-turn interleaved winding; (<b>b</b>) 6-turn interleaved winding.</p>
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<p>Simulation results of the electric field strength on the ZY plane: (<b>a</b>) 4-turn interleaved winding; (<b>b</b>) 6-turn interleaved winding.</p>
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<p>Planar inductor prototypes: (<b>a</b>) planar inductor with 4-turn interleaved winding; (<b>b</b>) planar inductor with 6-turn interleaved winding.</p>
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<p>Actual test platform.</p>
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<p>Schematic diagram of the LLC resonant converter test platform.</p>
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<p>Planar inductor with 4-turn interleaved winding tested waveform, time division 280 ns/div: (<b>a</b>) load set to 25 Ω; (<b>b</b>) load set to 30 Ω; (<b>c</b>) load set to 50 Ω.</p>
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<p>Planar inductor with 4-turn interleaved winding tested waveform, time division 104 ns/div: (<b>a</b>) load set to 25 Ω; (<b>b</b>) load set to 30 Ω; (<b>c</b>) load set to 50 Ω.</p>
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<p>Planar inductor with 6-turn interleaved winding tested waveform, time division 280 ns/div: (<b>a</b>) load set to 25 Ω; (<b>b</b>) load set to 30 Ω; (<b>c</b>) load set to 50 Ω.</p>
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<p>Planar inductor with 6-turn interleaved winding tested waveform, time division 104 ns/div: (<b>a</b>) load set to 25 Ω; (<b>b</b>) load set to 30 Ω; (<b>c</b>) load set to 50 Ω.</p>
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12 pages, 2111 KiB  
Article
RAAFNet: Reverse Attention Adaptive Fusion Network for Large-Scale Point Cloud Semantic Segmentation
by Kai Wang and Huanhuan Zhang
Mathematics 2024, 12(16), 2485; https://doi.org/10.3390/math12162485 - 12 Aug 2024
Viewed by 570
Abstract
Point cloud semantic segmentation is essential for comprehending and analyzing scenes. However, performing semantic segmentation on large-scale point clouds presents challenges, including demanding high memory requirements, a lack of structured data, and the absence of topological information. This paper presents a novel method [...] Read more.
Point cloud semantic segmentation is essential for comprehending and analyzing scenes. However, performing semantic segmentation on large-scale point clouds presents challenges, including demanding high memory requirements, a lack of structured data, and the absence of topological information. This paper presents a novel method based on the Reverse Attention Adaptive Fusion network (RAAFNet) for segmenting large-scale point clouds. RAAFNet consists of a reverse attention encoder–decoder module, an adaptive fusion module, and a local feature aggregation module. The reverse attention encoder–decoder module is applied to extract point cloud features at different scales. The adaptive fusion module enhances fine-grained representation within multi-resolution feature maps. Furthermore, a local aggregation classifier is introduced, which aggregates the features of neighboring points to the center point in order to leverage contextual information and enhance the classifier’s perceptual capability. Finally, the predicted labels are generated. Notably, our method excels at extracting point cloud features across different dimensions and produces highly accurate segmentation results. Experimental results on the Semantic3D dataset achieved an overall accuracy of 89.9% and a mIoU of 74.4%. Full article
(This article belongs to the Topic Big Data Intelligence: Methodologies and Applications)
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<p>The diagram of the RAAFNet method.</p>
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<p>Backward attention fusion module.</p>
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<p>Adaptive fusion module.</p>
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<p>Results of different methods on the Semantic3D Dataset.</p>
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20 pages, 3270 KiB  
Article
Chemical Synthesis and Structure–Activity Relationship Studies of the Coagulation Factor Xa Inhibitor Tick Anticoagulant Peptide from the Hematophagous Parasite Ornithodoros moubata
by Vincenzo De Filippis, Laura Acquasaliente, Andrea Pierangelini and Oriano Marin
Biomimetics 2024, 9(8), 485; https://doi.org/10.3390/biomimetics9080485 - 12 Aug 2024
Viewed by 741
Abstract
Tick Anticoagulant Peptide (TAP), a 60-amino acid protein from the soft tick Ornithodoros moubata, inhibits activated coagulation factor X (fXa) with almost absolute specificity. Despite TAP and Bovine Pancreatic Trypsin Inhibitor (BPTI) (i.e., the prototype of the Kunitz-type protease inhibitors) sharing a [...] Read more.
Tick Anticoagulant Peptide (TAP), a 60-amino acid protein from the soft tick Ornithodoros moubata, inhibits activated coagulation factor X (fXa) with almost absolute specificity. Despite TAP and Bovine Pancreatic Trypsin Inhibitor (BPTI) (i.e., the prototype of the Kunitz-type protease inhibitors) sharing a similar 3D fold and disulphide bond topology, they have remarkably different amino acid sequence (only ~24% sequence identity), thermal stability, folding pathways, protease specificity, and even mechanism of protease inhibition. Here, fully active and correctly folded TAP was produced in reasonably high yields (~20%) by solid-phase peptide chemical synthesis and thoroughly characterised with respect to its chemical identity, disulphide pairing, folding kinetics, conformational dynamics, and fXa inhibition. The versatility of the chemical synthesis was exploited to perform structure–activity relationship studies on TAP by incorporating non-coded amino acids at positions 1 and 3 of the inhibitor. Using Hydrogen–Deuterium Exchange Mass Spectrometry, we found that TAP has a remarkably higher conformational flexibility compared to BPTI, and propose that these different dynamics could impact the different folding pathway and inhibition mechanisms of TAP and BPTI. Hence, the TAP/BPTI pair represents a nice example of divergent evolution, while the relative facility of TAP synthesis could represent a good starting point to design novel synthetic analogues with improved pharmacological profiles. Full article
(This article belongs to the Special Issue Biomimetic Approaches in Healthcare—Innovations Inspired by Nature)
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<p>The amino acid sequence and structural similarity of TAP and BPTI. (<b>A</b>) The amino acid sequence alignment of TAP and BPTI: Conserved residues are indicated in bold. The disulphide bond topology is conserved in the two inhibitors and indicated by plain lines (orange). The secondary structure alignment of TAP and BPTI is also reported. (<b>B</b>) The three-dimensional structure of TAP and BPTI: Ribbon drawing representations are based on the best representative NMR conformers of TAP (1tcp.pdb) and BPTI (1pit.pdb). Helical regions are coloured in red, β-strands are in cyan, while segments of irregular structure are in light grey. The regions involved in trypsin or fXa binding are shown in magenta. N- and C-termini are also indicated. (<b>C</b>) The surface electrostatic potentials of TAP and BPTI: The orientation of the two inhibitors are as in panel B. The surface is coloured according to the electrostatic potential (blue, positive; red, negative) and expressed as kJ/(mol·q), as indicated. Calculations were performed using the APBS programme, run on the coordinates of the best representative conformers in the NMR structure of TAP and BPTI. Protein structure images were generated using the PyMOL ver. 1.3 Molecular Graphics System.</p>
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<p>Purification and disulphide oxidative renaturation of TAP. (<b>A</b>) RP-HPLC analysis of crude, synthetic TAP after resin cleavage and side chain protecting group removal. (<b>B</b>) RP-HPLC analysis of reduced (R) and oxidised (N) TAP after purification by semi-preparative RP-HPLC. (<b>C</b>) Kinetics of disulphide oxidative renaturation of TAP. Purified TAP (1 mg/mL) with Cys residues in reduced state (R) was allowed to fold under air oxidation conditions, at pH 8.3 in the presence of β-mercaptoethanol (250 μM) (see text). At fixed time points, aliquots (20 μL) were taken, acid quenched, and fractionated by analytical RP-HPLC to estimate folding yields of native TAP (N).</p>
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<p>Spectroscopic characterisation of N-TAP. (<b>A</b>) Fluorescence spectra of N-TAP. Protein samples (50 µg/mL) were excited at 280 and 295 nm. (<b>B</b>,<b>C</b>) Far-UV (<b>B</b>) and near-UV (<b>C</b>) circular dichroism spectra of N-TAP. Spectra were recorded at protein concentration of 0.1 mg/mL and 1 mg/mL in far- and near-UV region, respectively. All measurements were carried out at 25 ± 0.1 °C in PBS, pH 7.4, and resulting spectra were subtracted for corresponding baselines. (<b>D</b>) Temperature dependence of the relative ellipticity (θ/θ<sub>0</sub>) of TAP (●) and BPTI (<span style="color:#A4A4A4">●</span>). Ellipticity values (θ) of TAP and BPTI (1 mg/mL) were recorded at 289 nm as a function of temperature and normalised by the initial value (θ<sub>0</sub>) measured at 2 °C.</p>
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<p>Global HDX-MS analysis of N-TAP and BPTI. (<b>A</b>,<b>B</b>) Representative traces of global deuterium uptake of N-TAP (<b>A</b>) and BPTI (<b>B</b>) at increasing H/D exchange times. Proteins (25 μg/mL) were incubated at 25 °C with 95% D<sub>2</sub>O in PBS buffer, pD 7.43, and <span class="html-italic">m</span>/<span class="html-italic">z</span> spectra were taken at increasing labelling times, as indicated. For both N-TAP (<span class="html-italic">m</span>/<span class="html-italic">z</span> = 997.875, average value) and BPTI (<span class="html-italic">m</span>/<span class="html-italic">z</span> = 931.166, average value), multiple charged species at z = +7 were selected for monitoring deuterium uptake. (<b>C</b>) Time-course analysis of %D increase in TAP and BPTI, as indicated. Experimental conditions are those reported in panels (<b>A</b>,<b>B</b>). Data points are average of three different experiments, with error bars as standard deviations (see Methods).</p>
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<p>Inhibition of FXa amidolytic activity by wild-type synthetic TAP and mutated analogues. (<b>A</b>) Progress curves of pNA release by fXa. FXa solutions were pre-incubated (30 min) with increasing concentration of TAP and reaction was started by addition of chromogenic substrate RGR-pNA. Measurements were carried out at 25 °C in TBS, pH 7.4, containing 0.2 M NaCl and steady-state velocities of pNA release were determined from increase in absorbance at 405 nm. (<b>B</b>) Plot of relative velocities (v<sub>i</sub>/v<sub>0</sub>) of pNA release as function of increasing concentrations of wild-type and synthetic TAP analogues, as indicated. Notably, v<sub>i</sub> and v<sub>0</sub> are steady-state velocities of RGR-pNA hydrolysis in presence and absence of inhibitor, respectively. Data points are average of three independent measurements, with error bars as ±SD. As relevant examples, only fXa inhibition properties of Tyr1β-naphthyl-Ala and Arg3pyridyl-Ala analogues are reported. Data points were analysed according to the competitive tight-binding inhibition model, to yield K<sub>I</sub> values reported in <a href="#biomimetics-09-00485-t001" class="html-table">Table 1</a>.</p>
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<p>The details of the TAP-fXa interaction and the molecular structure of substituting amino acid side chains. (<b>A</b>) A close-up view of the interaction of the N-terminal amino acids 1–3 with the fXa active site. The amino acids of the TAP involved in the interaction with fXa are highlighted in stick and colour coded (carbon, grey; oxygen, red; nitrogen, blue); the catalytic amino acids of fXa are in blue, while those of the substrate specificity sites are coloured magenta. The picture was generated on the crystallographic structure of the TAP-fXa complex (1kig.pdb). (<b>B</b>) The surface electrostatic potential of fXa. The stick representation of the first three residues of TAP is also shown. The surface is coloured according to the electrostatic potential (blue, positive; red, negative) and expressed as kJ/(mol·q), as indicated. Calculations were performed using the APBS programme, run on the coordinates of the TAP-fXa complex, after removing the coordinates of TAP 4–60. Images were generated using the PyMOL ver. 1.3 Molecular Graphics System. (<b>C</b>) The structure of the substituting non-coded amino acids at position 1 and 3 of TAP.</p>
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<p>Comparison of the three-dimensional structure of TAP and BPTI in the free and proteases-bound form. (<b>A</b>) Ribbon drawing representation of the superposition of the NMR solution structure of free TAP (1tcp, red) with that of TAP in the crystallographic structure of the fXa-TAP complex (1kig, light gold). Ribbon drawing representation of the superposition of the NMR solution structure of free BPTI (1pit, blue) with that of BPTI in the crystallographic structure of the trypsin-BPTI complex (4y0y, light grey). (<b>B</b>) Close-up view of the superposition of the conformation of TAP sequence Tyr1-Asn2-Arg3- in the free (1tcp, red) and fXa-bound state (1kig, light gold).</p>
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25 pages, 859 KiB  
Article
Entanglement and Generalized Berry Geometrical Phases in Quantum Gravity
by Diego J. Cirilo-Lombardo and Norma G. Sanchez
Symmetry 2024, 16(8), 1026; https://doi.org/10.3390/sym16081026 - 12 Aug 2024
Viewed by 825
Abstract
A new formalism is introduced that makes it possible to elucidate the physical and geometric content of quantum space–time. It is based on the Minimum Group Representation Principle (MGRP). Within this framework, new results for entanglement and geometrical/topological phases are found and implemented [...] Read more.
A new formalism is introduced that makes it possible to elucidate the physical and geometric content of quantum space–time. It is based on the Minimum Group Representation Principle (MGRP). Within this framework, new results for entanglement and geometrical/topological phases are found and implemented in cosmological and black hole space–times. Our main results here are as follows: (i) We find the Berry phases for inflation and for the cosmological perturbations and express them in terms of the observables, such as the spectral scalar and tensor indices, nS and nT, and the tensor-to-scalar ratio r. The Berry phase for de Sitter inflation is imaginary with the sign describing the exponential acceleration. (ii) The pure entangled states in the minimum group (metaplectic) Mp(n) representation for quantum de Sitter space–time and black holes are found. (iii) For entanglement, the relation between the Schmidt type representation and the physical states of the Mp(n) group is found: This is a new non-diagonal coherent state representation complementary to the known Sudarshan diagonal one. (iv) Mean value generators of Mp(2) are related to the adiabatic invariant and topological charge of the space–time, (matrix element of the transition <t<). (v) The basic even and odd n-sectors of the Hilbert space are intrinsic to the quantum space–time and its discrete levels (in particular, continuum for n), they do not require any extrinsic generation process such as the standard Schrodinger cat states, and are entangled. (vi) The gravity or cosmological domains on one side and another of the Planck scale are entangled. Examples: The quantum primordial trans-Planckian de Sitter vacuum and the classical late de Sitter vacuum today; the central quantum gravity region and the external classical gravity region of black holes. The classical and quantum dual gravity regions of the space–time are entangled. (vii) The general classical-quantum gravity duality is associated with the Metaplectic Mp(n) group symmetry which provides the complete full covering of the phase space and of the quantum space–time mapped from it. Full article
(This article belongs to the Section Physics)
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<p>Chiral-antichiral oscillation (zitterbebegung) giving the pattern of cat states from first principles. The asymmetry in the pattern can be seen, marking a preferential temporal evolution.</p>
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<p>3D picture of the chiral-antichiral oscillation (cat states pattern).</p>
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<p>The three images show from top to down the entangled coherent state where the degree of entaglement varies as a function of time from the highest to the lowest degree controlled by the overlap <math display="inline"><semantics> <mfenced separators="" open="&#x2329;" close="&#x232A;"> <mi>α</mi> <mspace width="0.166667em"/> <mo>|</mo> <mspace width="0.166667em"/> <mi>β</mi> </mfenced> </semantics></math>. Here <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>)</mo> </mrow> </semantics></math> correspond to <math display="inline"><semantics> <mrow> <mo form="prefix">Re</mo> <mspace width="0.166667em"/> <mover accent="true"> <mi>α</mi> <mo>˜</mo> </mover> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo form="prefix">Im</mo> <mspace width="0.166667em"/> <mover accent="true"> <mi>α</mi> <mo>˜</mo> </mover> </mrow> </semantics></math>.</p>
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28 pages, 6642 KiB  
Article
Boolean Modeling of Biological Network Applied to Protein–Protein Interaction Network of Autism Patients
by Leena Nezamuldeen and Mohsin Saleet Jafri
Biology 2024, 13(8), 606; https://doi.org/10.3390/biology13080606 - 10 Aug 2024
Cited by 1 | Viewed by 751
Abstract
Cellular molecules interact with one another in a structured manner, defining a regulatory network topology that describes cellular mechanisms. Genetic mutations alter these networks’ pathways, generating complex disorders such as autism spectrum disorder (ASD). Boolean models have assisted in understanding biological system dynamics [...] Read more.
Cellular molecules interact with one another in a structured manner, defining a regulatory network topology that describes cellular mechanisms. Genetic mutations alter these networks’ pathways, generating complex disorders such as autism spectrum disorder (ASD). Boolean models have assisted in understanding biological system dynamics since Kauffman’s 1969 discovery, and various analytical tools for regulatory networks have been developed. This study examined the protein–protein interaction network created in our previous publication of four ASD patients using the SPIDDOR R package, a Boolean model-based method. The aim is to examine how patients’ genetic variations in INTS6L, USP9X, RSK4, FGF5, FLNA, SUMF1, and IDS affect mTOR and Wnt cell signaling convergence. The Boolean network analysis revealed abnormal activation levels of essential proteins such as β-catenin, MTORC1, RPS6, eIF4E, Cadherin, and SMAD. These proteins affect gene expression, translation, cell adhesion, shape, and migration. Patients 1 and 2 showed consistent patterns of increased β-catenin activity and decreased MTORC1, RPS6, and eIF4E activity. However, patient 2 had an independent decrease in Cadherin and SMAD activity due to the FLNA mutation. Patients 3 and 4 have an abnormal activation of the mTOR pathway, which includes the MTORC1, RPS6, and eIF4E genes. The shared mTOR pathway behavior in these patients is explained by a shared mutation in two closely related proteins (SUMF1 and IDS). Diverse activities in β-catenin, MTORC1, RPS6, eIF4E, Cadherin, and SMAD contributed to the reported phenotype in these individuals. Furthermore, it unveiled the potential therapeutic options that could be suggested to these individuals. Full article
(This article belongs to the Section Bioinformatics)
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<p>Schematic representation of the mutated proteins in four patients colored with red, green, cyan, and brown with arrangements of their roles on Wnt and mTOR signaling pathways [<a href="#B33-biology-13-00606" class="html-bibr">33</a>].</p>
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<p>Schematic representation of the algorithm developed in SPIDDOR library in R using the asynchronous method. (<b>A</b>) The output of the dynamic evolution function. The rows represent the nodes, and the columns represent the 100 iterations. (<b>B</b>) The output of the average simulation function. The probability of each node to be ON calculated from 2500 (N) simulations.</p>
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<p>The oscillation of the proteins involved in cell adhesion or DNA transcription and translation in the Boolean system for 2500 simulations in every 100 time steps. The blue color shows when all the proteins are at 100% of their functional effect. The green color when the mutation-like effect was introduced to proteins with variants in each patient to delay their activation by 50%. The red color when the mutation-like effect was introduced to proteins with variants in each patient to knock out their activation.</p>
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<p>The averages of the datapoints that represent the curves in the Boolean system (<a href="#biology-13-00606-f004" class="html-fig">Figure 4</a>): (<b>A</b>) Showing the oscillation average of each protein in each patient; (<b>B</b>) Showing the oscillation average of each protein combined by patients.</p>
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<p>The knockout heatmap representing the perturbation indexes PIs as a result of knocking out each node in the system (columns) and their effect on the other nodes in the network (rows). The heatmap is scaled and colored as follows: PI values close to 1 are taking the value of 0 and colored in gray, PI values between 1.25 and 2 are taking the value of 1 and colored in light orange, PI values greater than 2 are taking the value of 2 and colored in dark orange, PI values between 0.5 and 0.8 are taking the value of −1 and colored in light blue, and PI values less than 0.5 are taking the value of −2 and colored in dark blue.</p>
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<p>Multiple sequence alignment of the residues around beta strands 1 and 2 in the ligand FGF1-19 identified in [<a href="#B59-biology-13-00606" class="html-bibr">59</a>] using NCBI COBALT and visualized with alignment viewer. The colored symbols are to ease comparison of same amino acid residue down the columns (yellow was recolored to black using onlinepngtools.com—accessed on 28 June 2024). The mutated residue (red box) in FGF5 is adjacent to the conserved domain. All sequences come from human cells, except FGF15, which is from mouse brain cells.</p>
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19 pages, 6004 KiB  
Article
An Evaluation Model for Node Influence Based on Heuristic Spatiotemporal Features
by Sheng Jin, Yuzhi Xiao, Jiaxin Han and Tao Huang
Entropy 2024, 26(8), 676; https://doi.org/10.3390/e26080676 - 10 Aug 2024
Viewed by 619
Abstract
The accurate assessment of node influence is of vital significance for enhancing system stability. Given the structural redundancy problem triggered by the network topology deviation when an empirical network is copied, as well as the dynamic characteristics of the empirical network itself, it [...] Read more.
The accurate assessment of node influence is of vital significance for enhancing system stability. Given the structural redundancy problem triggered by the network topology deviation when an empirical network is copied, as well as the dynamic characteristics of the empirical network itself, it is difficult for traditional static assessment methods to effectively capture the dynamic evolution of node influence. Therefore, we propose a heuristic-based spatiotemporal feature node influence assessment model (HEIST). First, the zero-model method is applied to optimize the network-copying process and reduce the noise interference caused by network structure redundancy. Second, the copied network is divided into subnets, and feature modeling is performed to enhance the node influence differentiation. Third, node influence is quantified based on the spatiotemporal depth-perception module, which has a built-in local and global two-layer structure. At the local level, a graph convolutional neural network (GCN) is used to improve the spatial perception of node influence; it fuses the feature changes of the nodes in the subnetwork variation, combining this method with a long- and short-term memory network (LSTM) to enhance its ability to capture the depth evolution of node influence and improve the robustness of the assessment. Finally, a heuristic assessment algorithm is used to jointly optimize the influence strength of the nodes at different stages and quantify the node influence via a nonlinear optimization function. The experiments show that the Kendall coefficients exceed 90% in multiple datasets, proving that the model has good generalization performance in empirical networks. Full article
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<p>Study overview.</p>
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<p>Node influence assessment process diagram.</p>
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<p>Nodal spatiotemporal feature construction maps.</p>
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<p>Plot of the scale of impact on the network when the HEIST model is compared to other models with high-impact nodes selected as propagation sources.</p>
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<p>Analysis of propagation in a small network.</p>
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<p>Visualization of different network structures.</p>
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<p>Graph of the effect of different training network training tests.</p>
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20 pages, 8984 KiB  
Article
Numerical Study on the Heat Dissipation Performance of Diamond Microchannels under High Heat Flux Density
by Jiwen Zhao, Kunlong Zhao, Xiaobin Hao, Yicun Li, Sen Zhang, Benjian Liu, Bing Dai, Wenxin Cao and Jiaqi Zhu
Processes 2024, 12(8), 1675; https://doi.org/10.3390/pr12081675 - 9 Aug 2024
Viewed by 809
Abstract
Heat dissipation significantly limits semiconductor component performance improvement. Thermal management devices are pivotal for electronic chip heat dissipation, with the enhanced thermal conductivity of materials being crucial for their effectiveness. This study focuses on single-crystal diamond, renowned for its exceptional natural thermal conductivity, [...] Read more.
Heat dissipation significantly limits semiconductor component performance improvement. Thermal management devices are pivotal for electronic chip heat dissipation, with the enhanced thermal conductivity of materials being crucial for their effectiveness. This study focuses on single-crystal diamond, renowned for its exceptional natural thermal conductivity, investigating diamond microchannels using finite element simulations. Initially, a validated mathematical model for microchannel flow heat transfer was established. Subsequently, the heat dissipation performance of typical microchannel materials was analyzed, highlighting the diamond’s impact. This study also explores diamond microchannel topologies under high-power conditions, revealing unmatched advantages in ultra-high heat flux density dissipation. At 800 W/cm2 and inlet flow rates of 0.4–1 m/s, diamond microchannels exhibit lower maximum temperatures compared to pure copper microchannels by 7.0, 7.2, 7.4, and 7.5 °C, respectively. Rectangular cross-section microchannels demonstrate superior heat dissipation, considering diamond processing costs. The exploration of angular structures with varying parameters shows significant temperature reductions with increasing complexity, such as a 2.4 °C drop at i = 4. The analysis of shape parameter ki indicates optimal heat dissipation performance at ki = 1.1. This research offers crucial insights for developing and optimizing diamond microchannel devices under ultra-high-heat-flux-density conditions, guiding future advancements in thermal management technology. Full article
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<p>Boundary conditions set in the model.</p>
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<p>Grid division: (<b>a</b>) overall grid division and (<b>b</b>) microchannel region grid division.</p>
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<p>Grid division with different densities: (<b>a</b>) Plan A, (<b>b</b>) Plan B, (<b>c</b>) Plan C, and (<b>d</b>) Plan D.</p>
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<p>Calculation model validation: (<b>a</b>) geometric structure of microchannels; (<b>b</b>) comparison of experimental and simulated average wall temperatures along the channel direction (normal direction from the inlet to the outlet) [<a href="#B38-processes-12-01675" class="html-bibr">38</a>].</p>
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<p>Relationship between maximum temperature and heat flux density of microchannels under different flow rate conditions: (<b>a</b>) silicon, (<b>b</b>) copper, (<b>c</b>) LTCC, and (<b>d</b>) aluminum.</p>
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<p>Comparison of maximum temperatures of different substrate materials at various heat flux densities.</p>
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<p>Comparison of heat dissipation performance of diamonds with different thermal conductivities.</p>
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<p>Heat dissipation performance of diamond microchannels with varying thermal conductivity.</p>
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<p>Influence of cross-sectional shape on heat dissipation performance: (<b>a</b>) schematic of microchannel model and (<b>b</b>) impact of cross-sectional variation on heat dissipation performance.</p>
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<p>The effect of microchannel expansion on heat dissipation performance: (<b>a</b>) microchannel model and (<b>b</b>) influence of <span class="html-italic">k</span><sub>1</sub> on the heat dissipation performance of microchannels.</p>
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<p>Temperature distribution of microchannels under different <span class="html-italic">k</span><sub>1</sub> values.</p>
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<p>Flow velocity distributions of microchannels under different <span class="html-italic">k</span><sub>1</sub> values.</p>
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<p>Pressure distribution of microchannels under different <span class="html-italic">k</span><sub>1</sub> values.</p>
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<p>The influence of different numbers of diamond-shaped (hourglass-shaped) microchannels on heat dissipation performance: (<b>a1</b>–<b>c1</b>) models of diamond-shaped (hourglass-shaped) microchannels with different numbers and (<b>a2</b>–<b>c2</b>) heat dissipation performance of diamond-shaped (hourglass-shaped) microchannels with different numbers.</p>
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<p>Effects of different numbers of diamond-shaped (hourglass-shaped) microchannels on maximum flow velocity and pressure: (<b>a1</b>–<b>c1</b>) effects on flow velocity; (<b>a2</b>–<b>c2</b>) effects on maximum pressure.</p>
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19 pages, 3142 KiB  
Article
Dynamic Radiant Barrier for Modulating Heat Transfer and Reducing Building Energy Usage
by Tyler R. Stevens, Behzad Parsi, Rydge B. Mulford and Nathan B. Crane
Energies 2024, 17(16), 3959; https://doi.org/10.3390/en17163959 - 9 Aug 2024
Viewed by 684
Abstract
Buildings consume significant energy, much of which is used for heating and cooling. Insulation reduces undesired heat transfer to save on heating and cooling energy usage. Radiant barriers are a type of insulation technology that reduces radiant heat absorbed by a structure. Applying [...] Read more.
Buildings consume significant energy, much of which is used for heating and cooling. Insulation reduces undesired heat transfer to save on heating and cooling energy usage. Radiant barriers are a type of insulation technology that reduces radiant heat absorbed by a structure. Applying radiant barriers to buildings reduces costs and improves both energy efficiency and occupant comfort. However, homes often have favorable thermal gradients that could also be used to reduce energy usage if the insulation properties were switched dynamically. This article introduces two dynamic radiant barriers intended for residential attics, which can switch between reflecting and transmitting states as needed. These radiant barriers are manufactured as a single deformable assembly using sheet materials and are compatible with various actuation mechanisms. The efficacy of these radiant barriers is reported based on a hotbox experiment and numerical calculations. The experimental results demonstrate that both proposed dynamic radiant barrier designs increase effective thermal resistance by factors of approximately 2 when comparing insulating to conducting states, and by approximately 4 when comparing the insulating state to the case without a radiant barrier. Additionally, the dynamic radiant barriers achieve heat flux reductions up to 41.9% in the insulating state compared to tests without a dynamic radiant barrier. Full article
(This article belongs to the Section G: Energy and Buildings)
Show Figures

Figure 1

Figure 1
<p>Conceptual designs of the two dynamic radiant barrier designs: Accordion and S-Curve.</p>
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<p>Two dynamic radiant barrier designs: Accordion fold and S-Curve. The DRBs in this image are made from polyethylene and metalized polyester.</p>
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<p>(<b>a</b>) Manufactured and exploded views of Accordion and S-Curve DRBs. Black represents the LDPE, while blue and teal are used to differentiate the segments formed by cutting each reflective sheet. (<b>b</b>) Dimensions for LDPE and aluminum components, with units in mm.</p>
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<p>A conceptual design of the simplified Accordion DRB which uses a single folded reflective sheet instead of multiple bonded sheets.</p>
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<p>The manufactured, simplified Accordion DRB using LDPE and ten aluminum sheets in the manufactured (insulating) and deployed (conducting) states. Blue tape is used to hold down the DRB.</p>
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<p>Isometric view and cross-section of the hotbox used to measure the effective transmissivity of the proposed DRBs. Thermocouples are placed on each side of both particleboard layers to estimate the heat fluxes. The insulation has a reflective layer, and the representation of the insulating DRB is scaled to emphasize its location.</p>
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<p>Labeled cross-section of hotbox setup for corresponding dimensions listed in <a href="#energies-17-03959-t001" class="html-table">Table 1</a>. Shades of grey indicate the distinct sections of insulation.</p>
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<p>Schematic figures of the FEA hotbox and boundary conditions of the system for the 2D simulation.</p>
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<p>Averaged temperature distribution across particleboards in the control group (No DRB) during testing.</p>
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<p>A comparison of the experimental data, between the control test (without DRB) and the Accordion and S-Curve DRB configurations. Plots represent (<b>a</b>) the heat flux measurements, (<b>b</b>) ratio of heat flux across the lower particleboard, (<b>c</b>) the thermal resistance measurements, and (<b>d</b>) ratios of thermal resistance. Ins and Con refer to the insulating (manufactured) and conducting (deployed) states of the DRB.</p>
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<p>Steady–state temperature profiles of the hotbox without DRB.</p>
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<p>Heat flux from simulation and experiment through the bottom particleboard (between surfaces 3 and 4).</p>
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