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Search Results (5,058)

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Keywords = dynamic strength

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20 pages, 11411 KiB  
Article
Modeling and Nonlinear Dynamic Characteristics Analysis of Fault Bearing Time-Varying Stiffness-Flexible Rotor Coupling System
by Renzhen Chen, Jingyi Lv, Jing Tian, Yanting Ai, Fengling Zhang and Yudong Yao
Mathematics 2024, 12(22), 3591; https://doi.org/10.3390/math12223591 (registering DOI) - 16 Nov 2024
Viewed by 101
Abstract
There is a complex dynamic interaction between the aero-engine bearing and the rotor, and the resulting time-varying system parameters have an impact on the nonlinear dynamic characteristics of the rolling bearing-flexible rotor system. In this study, the interaction between the time-varying stiffness of [...] Read more.
There is a complex dynamic interaction between the aero-engine bearing and the rotor, and the resulting time-varying system parameters have an impact on the nonlinear dynamic characteristics of the rolling bearing-flexible rotor system. In this study, the interaction between the time-varying stiffness of the rolling bearing and the transient response of the flexible rotor is considered. The Newmark-β integral method is used to solve the dynamic equation, and the relationship between the time-varying characteristics of bearing stiffness and load and the dynamic characteristics of the rotor is studied. The relationship between bearing stiffness and vibration strength is analyzed, and the influence of damage size on the time domain signal energy of the disc is analyzed. The results show that the model established in this paper can accurately reflect the dynamic interaction between the bearing and the rotor. With the extension of the bearing damage, the dynamic stiffness of the bearing attenuates, the intensity of the excitation force increases, and the vibration is transmitted to the disc, which affects the motion stability and vibration response of the disc. Full article
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Figure 1
<p>Full-text research process.</p>
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<p>Six-node rotor-bearing system model.</p>
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<p>Damage bearing model diagram.</p>
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<p>Contact between the rolling element and damage pit.</p>
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<p>Bearing damage description function. (<b>a</b>,<b>c</b>,<b>d</b>) represent the states when the rolling body passes through defects of different sizes, and (<b>b</b>,<b>d</b>,<b>f</b>) show the relationship between <span class="html-italic">h</span> and <span class="html-italic">Φ</span> in the three states, respectively.</p>
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<p>Rotor system dynamics differential equation solving process.</p>
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<p>Bifurcation diagram of healthy bearing-rotor system.</p>
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<p>Time-varying stiffness of bearing and system response.</p>
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<p>Disc bifurcation diagrams under different damage widths.</p>
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<p>Three-dimensional spectrum of the disc under different damage widths.</p>
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<p>Bifurcation diagram of the disc under different damage lengths.</p>
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<p>The three-dimensional spectrum of the disc under different damage lengths.</p>
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<p>Axis orbit of 1500 rad/s disc (<b>a</b>) <span class="html-italic">B</span> = 0.7 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>b</b>) <span class="html-italic">B</span> = 1.4 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>c</b>) <span class="html-italic">B</span> = 2.1 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>d</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>e</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 1.9145 mm; (<b>f</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>g</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 9.572 mm; and (<b>h</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 11.4872 mm.</p>
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<p>Axis orbit of 1800 rad/s disc (<b>a</b>) <span class="html-italic">B</span> = 0.7 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>b</b>) <span class="html-italic">B</span> = 1.4 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>c</b>) <span class="html-italic">B</span> = 2.1 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>d</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>e</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 1.9145 mm; (<b>f</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>g</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 9.572 mm; and (<b>h</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 11.4872 mm.</p>
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<p>The root mean square relationship between the vibration energy of the disc and the bearing stiffness under different damage degrees.</p>
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<p>Bearing-rotor test bench.</p>
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<p>Comparison of vibration energy between simulation signal and experimental signal under different damage degrees.</p>
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17 pages, 11465 KiB  
Article
The Catastrophic Failure Mechanisms and the Prevention of Dynamic Pressure-Related Hazards During Mining Under an Interval Goaf Through an Isolated Coal Pillar in Shallow and Closely Spaced Coal Seams
by Bin Wang, Jie Zhang, Haifei Lin, Hui Liu, Shoushi Gao and Yifeng He
Appl. Sci. 2024, 14(22), 10554; https://doi.org/10.3390/app142210554 (registering DOI) - 15 Nov 2024
Viewed by 268
Abstract
Given the potential for dynamic load-induced support crushing that may occur during mining under an interval goaf through an isolated coal pillar (ICP) in shallow closely spaced coal seams, this paper systematically explored this issue through a case study of the 30,103 working [...] Read more.
Given the potential for dynamic load-induced support crushing that may occur during mining under an interval goaf through an isolated coal pillar (ICP) in shallow closely spaced coal seams, this paper systematically explored this issue through a case study of the 30,103 working face at the Nanliang Coal Mine. We employed a combined approach of similarity simulations, theoretical analyses, numerical simulations, and field measurements to investigate the catastrophic failure mechanisms and prevention strategies for dynamic pressure-related hazards encountered when mining a lower coal seam that passes through an ICP. The findings indicated that the synchronous cutting instability of the interlayer effective bearing stratum (IEBS) and double-arch bridge structure of the ICP roof were the primary causes of dynamic load-induced support crushing at the working face. A mechanical model was developed to characterize the IEBS instability during mining under an interval goaf. The sources and transmission pathways of dynamic mining pressure during mining passing through the ICP were clarified. The linked instability of the double-arch bridge structure of the ICP roof was induced by IEBS failure. The UDEC numerical model was utilized to elucidate the instability of the IEBS during mining in the lower coal seam and to analyze the vertical stress distribution patterns in the floor rock strata of the interval goaf. A comprehensive prevention and control strategy for roof dynamic pressure, which includes pre-releasing concentrated stress in the ICP, strengthening the support strength of the working face, and accelerating the advancement speed was proposed. The effectiveness of this prevention and control strategy was validated through actually monitoring the characteristics of mining pressure data from the 30,103 working face following pressure relief. The findings provide valuable insights for rock stratum control of shallow and closely spaced coal seam mining under similar conditions. Full article
(This article belongs to the Special Issue Advances in Green Coal Mining Technologies)
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<p>Coal pillar distribution plan of the overlying interval goaf at the 30,103 working face. (<b>a</b>) Local plan of the 30,103 working face. (<b>b</b>) Local sectional view of the 30,103 working face.</p>
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<p>Comprehensive cylindrical map of the OR in the No. 30,103 working face.</p>
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<p>Model design.</p>
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<p>Instability characteristics of the OR in the interval mining goaf [<a href="#B33-applsci-14-10554" class="html-bibr">33</a>].</p>
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<p>Fracture of the LKS.</p>
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<p>Fracture of the UKS.</p>
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<p>Mining under the ICP.</p>
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<p>The working face left the ICP for 7 m.</p>
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<p>Schematic diagram of the IEBS in closely spaced coal seams.</p>
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<p>Fracture characteristics of the IEBS during mining under the stress release zone. (<b>a</b>) Fracture of the interlayer lower bearing stratum. (<b>b</b>) Fracture of the interlayer upper bearing stratum.</p>
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<p>Fracture characteristics of IRS during mining under stress concentration zone. (<b>a</b>) Working face under the ICP. (<b>b</b>) Working face exiting the ICP.</p>
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<p>Fracture mechanics model for the IEBS. (<b>a</b>) Instability simulation of the IEBS under the double-arch bridge structure. (<b>b</b>) A diagram of the instability movement of the IEBS.</p>
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<p>Diagram of the overburden load on the ICP.</p>
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<p>Model for the rock column fracture instability structure in the CKS.</p>
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<p>Caving displacement nephogram of the OR.</p>
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<p>The overburden rock caving of the working face through the ICP. (<b>a</b>) The sixth periodic weighting. (<b>b</b>) The seventh periodic weighting.</p>
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<p>Variation curve of working resistance for support No. 75.</p>
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18 pages, 14275 KiB  
Article
Method of Forming Road Surface Replicas Using 3D Printing Technology
by Wojciech Owczarzak, Sławomir Sommer and Grzegorz Ronowski
Coatings 2024, 14(11), 1455; https://doi.org/10.3390/coatings14111455 - 15 Nov 2024
Viewed by 188
Abstract
Rolling resistance is a critical factor that influences vehicle energy consumption, emissions, and overall performance. It directly impacts fuel efficiency, tire longevity, and driving dynamics. Traditional rolling resistance tests are conducted on smooth steel drums, which fail to replicate real-world road surface textures, [...] Read more.
Rolling resistance is a critical factor that influences vehicle energy consumption, emissions, and overall performance. It directly impacts fuel efficiency, tire longevity, and driving dynamics. Traditional rolling resistance tests are conducted on smooth steel drums, which fail to replicate real-world road surface textures, potentially skewing results. This article presents the process of designing surface replicas using 3D printing technology, which consisted of selecting the internal structure, material, and print parameters of the surface sample. In order to verify the designed structures, an original mechanical strength test was performed. The test was based on pressing the tire onto the test sample with an appropriate force that corresponded to typical conditions during rolling resistance measurements. The test results included surface texture profiles before and after the application of load, which were then superimposed to detect any possible sample deformation. The obtained strength test results confirmed the validity of using 3D printing technology in the process of obtaining road surface replicas. Full article
(This article belongs to the Special Issue Surface Engineering and Mechanical Properties of Building Materials)
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<p>Texture ranges and their impact on tire-road interaction [<a href="#B5-coatings-14-01455" class="html-bibr">5</a>].</p>
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<p>Interface between tire and road surface for pavements with different texture [<a href="#B9-coatings-14-01455" class="html-bibr">9</a>].</p>
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<p>A running machine, which belongs to the equipment of the Mechanical Vehicles and Military Techniques Department of the Gdańsk University of Technology, drum with a diameter of 2 m.</p>
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<p>Road surface replica (PERS surface).</p>
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<p>The process of creating an elastic layer that is a negative representation of the road surface.</p>
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<p>Diagram showing the method of forming a replica of a road surface for running machines with an external drum (1, 2—mold halves; 3—elastic coating constituting a negative reproduction of the road surface; 4—top layer of the replica (gelcoat layer mixed with finely cut glass fiber); 5—leveling layer of epoxy resin; 6—layer of epoxy casting resin; 7—layer consisting of glass fiber mats immersed in epoxy resin).</p>
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<p>Flowchart showing the research stages.</p>
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<p>“Grid” geometry of pavement replica fillings (5%, 10%, and 15% of infill density).</p>
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<p>“Concentric” geometry of pavement replica fillings (5%, 10%, and 15% of infill density).</p>
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<p>“Triangles” geometry of pavement replica fillings (5%, 10%, and 15% of infill density).</p>
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<p>“Trihexagon” geometry of pavement replica fillings (5%, 10%, and 15% of infill density).</p>
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<p>“Cross” geometry of pavement replica fillings (5%, 10%, and 15% of infill density).</p>
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<p>APS4 surface 3D model.</p>
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<p>A stand for carrying out strength tests.</p>
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<p>Road replica sample scanned by laser profilometer.</p>
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<p>Graphs showing the strength test results for individual samples: (<b>a</b>) Grid; (<b>b</b>) Trihexagon; (<b>c</b>) Cross.</p>
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<p>Graphs showing the strength test results for individual samples: (<b>a</b>) Grid; (<b>b</b>) Trihexagon; (<b>c</b>) Cross.</p>
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<p>APS4 surface profile changes for specific loads (concentric, 5% infill).</p>
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<p>APS4 surface profile changes for specific loads (concentric, 10% infill).</p>
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<p>APS4 surface profile changes for specific loads (concentric, 15% infill).</p>
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<p>APS4 surface profile changes for specific loads (triangle, 5% infill).</p>
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<p>APS4 surface profile changes for specific loads (triangle, 10% infill).</p>
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19 pages, 5030 KiB  
Article
Microstructural Evolution and Damage Mechanism of Water-Immersed Coal Based on Physicochemical Effects of Inorganic Minerals
by Xuexi Chen, Zijian Liu, Tao Li, Jingyi Ma and Jiaying Hu
Materials 2024, 17(22), 5579; https://doi.org/10.3390/ma17225579 - 15 Nov 2024
Viewed by 305
Abstract
Coal seam water injection technology enables seam permeability enhancement and facilitates outburst risk reduction. This study investigated the microscale effects of water infiltration on coal and the evolution mechanisms of its mechanical properties. To this end, we systematically analyzed dynamic changes (such as [...] Read more.
Coal seam water injection technology enables seam permeability enhancement and facilitates outburst risk reduction. This study investigated the microscale effects of water infiltration on coal and the evolution mechanisms of its mechanical properties. To this end, we systematically analyzed dynamic changes (such as mineral composition, pore structure, and mechanical performance) in coal soaked for various durations using X-ray diffraction, low-field nuclear magnetic resonance (NMR), and uniaxial compression testing. The results indicate: (1) the coal NMR T2 spectrum displays three characteristic peaks, corresponding to rapid water absorption, uniform transition, and stabilization stages of soaking traditionally divided according to peak area variation trends. (2) The coal strength decreases with progressive soaking, influenced by water content, pore volume, mineral composition, etc. Its compressive strength and elastic modulus drop by 22.4% and 19.5%, respectively, compared to the initial values. (3) The expansion of clay minerals during immersion reduces average pore size. In contrast, quartz particle displacement, pore water movement, and soluble mineral dissolution increase pore volume, reducing the overall structure strength. (4) The dominant factors driving the degradation of mechanical properties vary across immersion stages, including water content and specific mineral concentration. This work offers new insights into how hydraulic technology alters coal seams, providing theoretical support for optimizing water injection strategies in the seam. Full article
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<p>Changes in moisture content of coal samples under various soaking duration conditions.</p>
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<p>Graphical representation of Experimental Methodology.</p>
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<p>XRD analysis of coal samples at different soaking durations.</p>
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<p>XRD analysis of coal samples at different soaking durations.</p>
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<p>T<sub>2</sub> Spectra of Coal at Different Soaking Durations.</p>
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<p>Variations in T<sub>2</sub> Spectrum Area and Proportion of Coal Samples at Different Soaking Durations.</p>
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<p>Stress–strain curves of coal samples with different soaking durations.</p>
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<p>Variation in compressive strength (<b>a</b>) and elastic modulus (<b>b</b>) with soaking duration.</p>
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<p>Failure modes of coal samples with different soaking durations.</p>
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<p>Evolution of coal pore structure at different soaking times.</p>
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17 pages, 4507 KiB  
Article
Simplified Gravity Load Collapse Dynamic Analysis of Old-Type Reinforced Concrete Frames
by Konstantinos G. Megalooikonomou
Constr. Mater. 2024, 4(4), 704-720; https://doi.org/10.3390/constrmater4040038 - 14 Nov 2024
Viewed by 471
Abstract
The results of shaking table tests from previous studies on a one-story, two-bay reinforced concrete frame—exhibiting both shear and axial failures—were compared with nonlinear dynamic analyses using simplified models intended to evaluate the collapse potential of older reinforced concrete structures. To replicate the [...] Read more.
The results of shaking table tests from previous studies on a one-story, two-bay reinforced concrete frame—exhibiting both shear and axial failures—were compared with nonlinear dynamic analyses using simplified models intended to evaluate the collapse potential of older reinforced concrete structures. To replicate the nonlinear behavior of columns, whether shear-critical or primarily flexure-dominant, a one-component beam model was applied. This model features a linear elastic element connected in series to a rigid plastic, linearly hardening spring at each end, representing a concentrated plasticity component. To account for strength degradation through path-dependent plasticity, a negative slope model as degradation was implemented, linking points at both shear and axial failure. The shear failure points were determined through pushover analysis of shear-critical columns using Phaethon software. Although the simplified model provided a reasonable approximation of the overall frame response and lateral strength degradation, especially in terms of drift, its reduced computational demands led to some discrepancies between the calculated and measured shear forces and drifts during certain segments of the time-history response. Full article
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<p>Graphical research framework of this study (Δ<span class="html-italic"><sub>shear</sub></span> cantilever lateral displacement due to shear mechanism, Δ<span class="html-italic"><sub>slip</sub></span> cantilever lateral displacement due to pull-out slip of anchorage or lap splice, Δ<span class="html-italic"><sub>flex</sub></span> cantilever lateral displacement due to flexure, Δ<span class="html-italic"><sub>tot</sub></span> total lateral displacement, <span class="html-italic">l<sub>r</sub></span> yield penetration length in the anchorage, <span class="html-italic">f<sub>by</sub></span> local bond strength of the anchorage, <span class="html-italic">l<sub>p</sub></span> plastic hinge length, <span class="html-italic">γ<sub>e</sub></span> elastic shear strain, <span class="html-italic">γ<sub>p</sub></span> plastic shear strain. <span class="html-italic">θ</span> cantilever lateral rotation, <span class="html-italic">θ<sub>slip</sub></span> cantilever lateral rotation due to pull-out slip, <span class="html-italic">V<sub>R</sub></span> shear strength, <span class="html-italic">L<sub>s</sub></span> shear span, <span class="html-italic">d</span> column section effective depth, <span class="html-italic">V</span> seismic shear force, Δ lateral displacement, Δ<span class="html-italic"><sub>s</sub></span> lateral displacement at shear failure, Δ<span class="html-italic"><sub>a</sub></span> lateral displacement at axial failure).</p>
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<p>Beam (<b>a</b>) displacements and (<b>b</b>) forces in global, local, and basic reference systems and (<b>c</b>) one-component beam model.</p>
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<p>(<b>a</b>) Specimen 2 of shake table test [<a href="#B37-constrmater-04-00038" class="html-bibr">37</a>,<a href="#B38-constrmater-04-00038" class="html-bibr">38</a>]. (<b>b</b>) Simplified numerical model implemented in MATLAB 2024b.</p>
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<p>Capacity curve of center shear-critical column of Specimen 2 and lateral displacement contributions for each step of the pushover analysis (16 total pushover steps of 5 kN) [This is a screenshot from Phaethon Windows software’s user interface].</p>
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<p>Strain, slip, and bond distributions along the straight anchorage length of center shear-critical column of Specimen 2 for pushover step 15 of Phaethon Windows software. See also <a href="#constrmater-04-00038-f001" class="html-fig">Figure 1</a> and <a href="#constrmater-04-00038-f004" class="html-fig">Figure 4</a>.</p>
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<p>Time-history responses in terms of drift, base shear, and center column shear of Specimen 2.</p>
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<p>Absolute error time-history responses in terms of drift, base shear, and center column shear of Specimen 2.</p>
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<p>Shear hysteretic response of Specimen 2.</p>
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<p>Below beam moment–rotation hysteretic response of center column of Specimen 2.</p>
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<p>Below beam moment–rotation hysteretic response of outside column of Specimen 2.</p>
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25 pages, 3842 KiB  
Article
An Innovative Dynamic Model for Predicting Typhoon Track Deflections over Complex Terrain
by Hung-Cheng Chen
Atmosphere 2024, 15(11), 1372; https://doi.org/10.3390/atmos15111372 - 14 Nov 2024
Viewed by 403
Abstract
This study presents an innovative, dynamic model for predicting typhoon track deflections over complex terrain. Based on potential vorticity conservation, the model incorporates a topographic adjusting parameter (α) and a meridional adjusting velocity (MAV) to capture the vortex’s response to terrain variations. Simulations [...] Read more.
This study presents an innovative, dynamic model for predicting typhoon track deflections over complex terrain. Based on potential vorticity conservation, the model incorporates a topographic adjusting parameter (α) and a meridional adjusting velocity (MAV) to capture the vortex’s response to terrain variations. Simulations using an idealized bell-shaped mountain and Taiwan’s realistic topography reveal that steeper terrain gradients consistently deflect typhoon tracks southward. This steering effect intensifies with increasing vortex strength due to a larger α, leading to enhanced MAV. Shallower approach angles also amplify deflections due to prolonged terrain interaction. Results highlight the significant role of Taiwan’s Central Mountain Range in shaping typhoon trajectories. This model offers a refined approach for predicting typhoon behavior near complex terrain, advancing forecasting capabilities, and enhancing disaster preparedness strategies. Full article
(This article belongs to the Special Issue Typhoon/Hurricane Dynamics and Prediction (2nd Edition))
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<p>Schematic of the dynamic model that illustrates the interaction between a cyclonic vortex and isolated topography. (<b>a</b>) The vortex approaches the terrain at an impinging angle <math display="inline"><semantics> <mrow> <mi>γ</mi> </mrow> </semantics></math>. The vortex has a radius of maximum winds <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>R</mi> </mrow> <mrow> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> and a maximum azimuthal velocity <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math>, interacting with a bell-shaped mountain of maximum height <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>h</mi> </mrow> <mrow> <mi>M</mi> </mrow> </msub> </mrow> </semantics></math> and base height <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>h</mi> </mrow> <mrow> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math>. (<b>b</b>) Cross-sectional profile of the topography along the vortex path. <math display="inline"><semantics> <mrow> <mi>D</mi> </mrow> </semantics></math> represents the unperturbed fluid depth, and <math display="inline"><semantics> <mrow> <mi>H</mi> </mrow> </semantics></math> is the total fluid depth accounting for topography and surface effects. <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>η</mi> </mrow> <mrow> <mi>v</mi> </mrow> </msub> </mrow> </semantics></math> denotes the maximum free surface depression caused by the vortex. <math display="inline"><semantics> <mrow> <mi>θ</mi> </mrow> </semantics></math> is the inclined angle of topography.</p>
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<p>(<b>a</b>) The 3D bell-shaped mountain’s topography shows the latitudinal cross sections AA’ to EE’. Solid contour lines represent 100-m intervals, whereas dashed lines mark 1000-m elevations. (<b>b</b>) Cross-sectional topographic profiles along each of the five latitudes. These profiles illustrate the steep elevation of the CMR, peaking above 3000 m, with the highest elevations near the CC’ and DD’ sections, showing strong variation in terrain across the island.</p>
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<p>Tracks of vortex M passing over isolated topography for different impinging angles: (<b>a</b>) 195°, (<b>b</b>) 170°, (<b>c</b>) 145°, and (<b>d</b>) 120°. The corresponding track deflections (<span class="html-italic">δ</span>) are also shown. Numbers 1–12 represent the name of cases, respectively. The dashed lines represent the tracks and deflections for the northern landfall cases (1, 4, 7, and 10). The solid lines show the tracks and deflections for the central landfall cases (2, 5, 8, and 11). The dashed-dotted lines correspond to the tracks and deflections for the southern landfall cases (3, 6, 9, and 12).</p>
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<p>(<b>a</b>) Topography of Taiwan: Contour lines representing elevations of 100 m (solid lines) and 1000 m (dashed lines) are shown. Five latitudinal cross-sections (AA’, BB’, CC’, DD’, and EE’) are marked. (<b>b</b>) Elevational profiles: Topographic profiles along the five cross-sections indicated in panel (<b>a</b>) are displayed.</p>
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<p>Simulated tracks (scanned trajectories) of vortices interacting with the realistic topography of Taiwan at varying initial latitudes but fixed impinging angles. Each panel represents a different vortex central relative vorticity (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>ζ</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math>): (<b>a</b>) S1 (<math display="inline"><semantics> <mrow> <mn>2</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>−</mo> <mn>4</mn> </mrow> </msup> <msup> <mrow> <mi>s</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>), (<b>b</b>) S2 (<math display="inline"><semantics> <mrow> <mn>4</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>−</mo> <mn>4</mn> </mrow> </msup> <msup> <mrow> <mi>s</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>), (<b>c</b>) S3 (<math display="inline"><semantics> <mrow> <mn>6</mn> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>−</mo> <mn>4</mn> </mrow> </msup> <msup> <mrow> <mi>s</mi> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>). The impinging angle (γ) for the panels (<b>a</b>–<b>c</b>) is 195°. Panels (<b>d</b>–<b>f</b>) use the same vortex intensities as (<b>a</b>–<b>c</b>), respectively, but with an impinging angle of 170°. Numbers 1–5 are scanned tracks of vortices impinging from north to south latitudes. S1, S2 and S3 are names of vortices.</p>
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<p>The figure is similar to <a href="#atmosphere-15-01372-f005" class="html-fig">Figure 5</a> but illustrates tracks for shallower impinging angles. Panels (<b>a</b>–<b>c</b>) display the tracks for vortices S1, S2, and S3, respectively, with a fixed impinging angle of 145°. Panels (<b>d</b>–<b>f</b>) present the corresponding tracks for the same vortices, but with an impinging angle of 120°. Numbers 1-5 are scanned tracks of vortices impinging from north to south latitudes. S1, S2 and S3 are names of vortices.</p>
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<p>Comparison of the dynamic model’s simulated track with the observed track of Typhoon Soudelor (2015). (<b>a</b>) Simulated track (red solid line) and observed typhoon center positions (open pink stars) overlaid on the topography of Taiwan. (<b>b</b>) Elevational profile (black solid line) along the simulated track and the corresponding track deflection (red solid line). Track deflection is defined as the southward deviation of the simulated track from a straight westward path.</p>
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18 pages, 4818 KiB  
Article
Investigation of In Situ Gelation Behavior and Enhanced Oil Recovery Ability of Polymer Gel Used for Controlling CO2 Channeling in Tight Fractured Reservoir
by Hong He, Yibo Liu, Guang Zhao, Yifei Liu, Haihua Pei and Wei Zhou
Gels 2024, 10(11), 741; https://doi.org/10.3390/gels10110741 - 14 Nov 2024
Viewed by 273
Abstract
Polymer gels are one of the most common plugging agents used for controlling CO2 channeling and improving sweep efficiency and oil recovery in tight fractured reservoirs. However, the in situ gelation behavior and enhanced oil recovery ability of polymer gel in fractured [...] Read more.
Polymer gels are one of the most common plugging agents used for controlling CO2 channeling and improving sweep efficiency and oil recovery in tight fractured reservoirs. However, the in situ gelation behavior and enhanced oil recovery ability of polymer gel in fractured porous media is still unclear. Thus, in this study, the bulk and in situ gelation behavior of crosslinked phenolic resin gel in a long stainless microtube as the fractured porous media was investigated. The enhanced oil recovery ability of phenolic resin gel used for CO2 channeling was investigated by means of a fractured core model. Results show that, with the increase of polymer and crosslinker concentrations, the bulk gelation time shortens and gel strength improves during the static gelation process. With the increase of polymer concentration and temperature, the in situ static gelation time and dynamic gelation time of the gel system in the microtube are shortened, and the breakthrough pressure gradient increases after gelation. Compared with the in situ static gelation behavior, the in situ dynamic gelation time is prolonged and the breakthrough pressure gradient decreases after gelation. The in situ static gelation time in the microtube is 1.2 times that of bulk gelation time in an ampoule bottle, and the in situ dynamic gelation time is nearly 3 times that of ampoule bottles. When the injected slug volume was 1.0 FV (fracture volume), as the polymer concentration increased from 3000 mg·L−1 to 4000 mg·L−1, the incremental oil recovery increased from 3.53% to 4.73%. Full article
(This article belongs to the Special Issue Polymer Gels for the Oil and Gas Industry)
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<p>The effect of polymer and crosslinker concentration on the bulk gelation process at 70 °C.</p>
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<p>The effect of temperature on bulk gelation behavior (70 °C and 90 °C).</p>
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<p>Comparisons of gel appearance varying with time at 70 °C and 90 °C.</p>
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<p>Breakthrough pressure and pressure gradient versus time at 70 °C and 90 °C.</p>
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<p>Breakthrough pressure and pressure gradient of different polymer concentrations versus time at 90 °C.</p>
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<p>Change of injection pressure with time at 70 °C and 90 °C (injection rate v = 0.05 mL·min<sup>−1</sup>).</p>
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<p>Change of injection pressure as a function of time during flow of gelant solution in the microtube (90 °C, 0.25 mL·min<sup>−1</sup>).</p>
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<p>Change of injection pressure as a function of time during flow of gelant solution in the microtube at different injection rates (90 °C).</p>
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<p>Gas flooding performance curve of an injected gel system with different polymer and crosslinker concentrations.</p>
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<p>Gas flooding performance curve of an injected gel system with different polymer and crosslinker concentrations.</p>
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<p>Incremental histogram of oil recovery of different injected gel system concentrations.</p>
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<p>Design and physical image of complex fracture core model.</p>
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<p>Apparatus of the microtube flow experiment.</p>
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<p>Schematic diagram of core flooding experiment.</p>
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20 pages, 17248 KiB  
Article
Experimental Study on the Dynamic Mechanical Properties and Crashing Behaviors of Limestone Under High Temperatures in Real-Time
by Lianying Zhang, Bing Li, Peng Wu, Shiru Guo, Yadong Zheng, Ming Li and Fuqiang Zhu
Appl. Sci. 2024, 14(22), 10486; https://doi.org/10.3390/app142210486 - 14 Nov 2024
Viewed by 244
Abstract
In this study, a split Hopkinson pressure bar (SHPB) test system with real-time temperature control was developed, and dynamic tests on limestone taken from deep coal mines within real-time temperatures of 25 to 800 °C were carried out. Additionally, the scanning electron microscope [...] Read more.
In this study, a split Hopkinson pressure bar (SHPB) test system with real-time temperature control was developed, and dynamic tests on limestone taken from deep coal mines within real-time temperatures of 25 to 800 °C were carried out. Additionally, the scanning electron microscope (SEM), X-ray diffraction (XRD), and energy dispersion spectrum (EDS) tests were conducted to analyze the fracture mechanism of limestone at real-time temperatures. The results reveal that the dynamic compressive strength of limestone linearly declines with increasing temperatures; due to not being affected by thermal shock damage, its strength degradation is not significant after cooling to room temperature, whereas the dynamic elastic modulus exhibits a negative exponential nonlinear decrease with the increase in temperatures. The average strain rate has a positive correlation with the dynamic compressive strength of limestone, while the dynamic elastic modulus exhibits variations in accordance with the Boltzmann function and its relationship with the strain rate. The combined influence of strain rate and temperature on the dynamic compressive strength of limestone can be accurately described by a binary quadratic function. The mechanism of real-time action on limestone can be divided into three stages: when the temperature is between 25 and 200 °C, crystal micro-expansion leads to the densification of micropores, which leads to the increase in limestone strength. When the temperature is between 200 °C and 600 °C, the formation of microcracks induced by thermal stress and intergranular expansion results in a reduction in limestone strength. When the temperature is between 600 and 800 °C, in addition to the continued expansion of the intergranular resulting in the increase in the number of micro-cracks, the decomposition of dolomite at high temperatures leads to chemical deterioration and further reduction in the strength of limestone. Full article
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<p>Micro-mineral characteristics of dolomite (Ca·Mg (CO<sub>3</sub>)<sub>2</sub>) and calcite (CaCO<sub>3</sub>) at a temperature of 25 °C. (<b>a</b>) investigated limestone specimen; (<b>b</b>) microstructure of the investigated limestone specimen; (<b>c</b>) energy spectra of point a; (<b>d</b>) energy spectra of point b.</p>
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<p>Schematic of the SHPB with real-time temperature control system.</p>
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<p>Dynamic stress–strain curves of the limestone specimen under the coupling effect of the real-time temperature and impact loading.</p>
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<p>Variation in the dynamic compressive strength <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mi mathvariant="normal">d</mi> </msub> </mrow> </semantics></math> with the temperature <span class="html-italic">T</span>.</p>
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<p>Variation in the dynamic compressive stress <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mi mathvariant="normal">d</mi> </msub> </mrow> </semantics></math> with the strain rate <math display="inline"><semantics> <mover accent="true"> <mi>ε</mi> <mo>˙</mo> </mover> </semantics></math>.</p>
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<p>Variation in the temperature sensitivity coefficient <span class="html-italic">η</span> with the temperature <span class="html-italic">T</span>.</p>
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<p>Variation in the dynamic, comprehensive stress <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mi mathvariant="normal">d</mi> </msub> </mrow> </semantics></math> with the temperature <span class="html-italic">T</span> and strain rate <math display="inline"><semantics> <mover accent="true"> <mi>ε</mi> <mo>˙</mo> </mover> </semantics></math>.</p>
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<p>Variation in the dynamic elastic modulus <span class="html-italic">E</span><sub>d</sub> with the temperature <span class="html-italic">T</span>.</p>
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<p>Variation in the dynamic elastic modulus <span class="html-italic">E</span><sub>d</sub> with the strain rate <math display="inline"><semantics> <mover accent="true"> <mi>ε</mi> <mo>˙</mo> </mover> </semantics></math>.</p>
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<p>Variation in the dynamic elastic modulus <span class="html-italic">E</span><sub>d</sub> with the temperature <span class="html-italic">T</span> and strain rate <math display="inline"><semantics> <mover accent="true"> <mi>ε</mi> <mo>˙</mo> </mover> </semantics></math>.</p>
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<p>XRD analysis of the mineral composition in the specimens at different temperatures.</p>
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<p>Micro-structural characteristics of dolomite in the limestone at 800 °C.</p>
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<p>Micro-structural characteristics of dolomite in the limestone at 800 °C.</p>
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<p>Micro-structural characteristics of calcite in the limestone at 800 °C.</p>
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<p>Micro-fracture characteristics of the limestone specimen after impact loading under different real-time temperatures.</p>
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<p>Micro-fracture characteristics of the limestone specimen after impact loading under different real-time temperatures.</p>
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<p>Variation in the microfracture patterns under different strain rates and at a temperature of 800 °C.</p>
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16 pages, 1366 KiB  
Article
The Value of Community Capitals in Sustainable Urban Development: A Qualitative Exploration of Urban Informal Workers
by Ivy Chumo, Blessing Mberu and Caroline Kabaria
Challenges 2024, 15(4), 44; https://doi.org/10.3390/challe15040044 - 14 Nov 2024
Viewed by 230
Abstract
Urban informality, often viewed negatively, is not solely the product of the urban poor but also reflects the failure of formal systems to adapt. Informal workers, who make up about 61% of the global workforce, operate outside formal labor laws and significantly contribute [...] Read more.
Urban informality, often viewed negatively, is not solely the product of the urban poor but also reflects the failure of formal systems to adapt. Informal workers, who make up about 61% of the global workforce, operate outside formal labor laws and significantly contribute to urban development. Understanding and harnessing community capitals are vital for sustainable urban development. This qualitative study explored the community capitals framework (CCF) in an urban context, addressing the limitations of quantitative data on CCF, which often overlooks critical social factors. This study team conducted in-depth interviews with 36 informal service providers from the education, healthcare, water, sanitation, and solid waste management sectors. Additionally, four local leaders from two urban informal settlements in Nairobi, Kenya, were interviewed. The data from the transcripts were analyzed using thematic framework analysis, guided by the community capitals framework. We identified seven forms of community capital that benefit informal workers: natural, cultural, human, social, political, financial, and built. Human capital, which focuses on skills and qualities, was the most frequently utilized, followed by social capital, which centers on connections and relationships. Next in importance were financial and political capital. Although cultural capital was the least implemented, it was described as important for reflecting community knowledge and traditions. Examples of these capitals in action included solid waste workers, manual pit emptiers, education providers, health workers, and water service providers, who all contributed to urban development and well-being through waste management, sanitation, education, healthcare, and access to clean water. In conclusion, service providers use community capitals as a planning tool to understand dynamics, refine strategies, and build trust for urban development. Each capital functions like a community bank account, containing strengths and opportunities. Although cultural capital was ranked last, it warrants further research to explore its drivers. Additional research is needed to fully grasp the relationships among the various capitals and their impact on service delivery. Full article
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<p>Community capitals framework.</p>
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<p>Study sites (source: authors, 2022).</p>
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<p>Type and frequency of capitals reflected in service delivery.</p>
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11 pages, 4314 KiB  
Article
Mechanistic Study of Atomic Oxygen Erosion on Polyimide Under Electric Fields: A Molecular Dynamics and Density Functional Theory Approach
by Shengrui Zhou, Li Zhang, Liang Zou, Bilal Iqbal Ayubi and Yiwei Wang
Molecules 2024, 29(22), 5353; https://doi.org/10.3390/molecules29225353 - 14 Nov 2024
Viewed by 250
Abstract
Polyimide (PI) is widely used in aerospace applications due to its superior insulating properties. However, the high concentration of atomic oxygen (AO) in low Earth orbit leads to significant performance degradation in PI, and the underlying mechanism of AO erosion under an electric [...] Read more.
Polyimide (PI) is widely used in aerospace applications due to its superior insulating properties. However, the high concentration of atomic oxygen (AO) in low Earth orbit leads to significant performance degradation in PI, and the underlying mechanism of AO erosion under an electric field remains unclear. This study utilizes molecular dynamics simulations to model AO erosion on PI under various electric field strengths and explores the corresponding degradation mechanisms. The results indicate that the presence of an electric field exacerbates the degradation of PI by AO. AO erosion elevates the polymer’s temperature, and the combined effects of thermal and electric stresses increase the polymer’s free volume, loosening its structure and accelerating degradation. The quantity of AO-induced erosion products increases with rising electric field strength, causing more large carbon chains to detach from the polymer surface. Density functional theory (DFT) calculations further reveal that the electric field reduces the frontier orbital energy gap in PI molecules, making AO erosion reactions more thermodynamically favorable. This work provides an atomic-level insight into the degradation mechanism of PI under AO erosion in electric fields and offers a theoretical basis for future studies on polymer resistance to AO erosion in space environments. Full article
(This article belongs to the Special Issue Exclusive Feature Papers in Macromolecular Chemistry)
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<p>Snapshots of the model erosion during AO exposure under electric field strengths of (<b>a</b>) E = 0.0 V/nm, (<b>b</b>) E = 0.4 V/nm, and (<b>c</b>) E = 0.8 V/nm.</p>
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<p>Normalized mass changes during AO erosion under different electric field strengths.</p>
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<p>Temperature variations in the decomposition and protected regions during AO erosion.</p>
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<p>(<b>a</b>) Free volume distribution in the PI model and (<b>b</b>) changes in free volume under different temperatures and electric field strengths.</p>
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<p>Variations in the types and quantities of products during AO erosion simulation.</p>
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<p>Snapshots of the main products generated during AO erosion.</p>
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<p>Changes in frontier orbitals and energy gap of PI molecules under electric field influence.</p>
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<p>The PI monomer structure and the relaxed equilibrium cell structure.</p>
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22 pages, 2042 KiB  
Review
Drought Dynamics in Sub-Saharan Africa: Impacts and Adaptation Strategies
by Pedro Lombe, Elsa Carvalho and Paulo Rosa-Santos
Sustainability 2024, 16(22), 9902; https://doi.org/10.3390/su16229902 - 13 Nov 2024
Viewed by 551
Abstract
The escalation in both frequency and severity of drought events has significantly amplified the vulnerability of numerous countries, particularly in developing ones, imposing substantial economic, environmental, and social pressures. This article presents a systematic review of drought occurrences in Sub-Saharan Africa (SSA), examining [...] Read more.
The escalation in both frequency and severity of drought events has significantly amplified the vulnerability of numerous countries, particularly in developing ones, imposing substantial economic, environmental, and social pressures. This article presents a systematic review of drought occurrences in Sub-Saharan Africa (SSA), examining historical trends, current impacts, and projected future implications. Through this comprehensive assessment, a clear trend of intensifying drought phenomena emerges across SSA, leading to crop failures, drying of water sources, loss of pasture, food shortages, and an increase in food prices. This review also highlights the concerning potential for worsening conditions in certain regions, resulting in consequences such as migration, food insecurity, malnutrition, family disintegration, crop losses, and increased disease prevalence, notably HIV/AIDS. This study further reveals that current adaptation measures by governments and NGOs should be improved to effectively adapt to the diverse impacts of drought, and it contributes to a deeper understanding of drought dynamics in Sub-Saharan Africa and assesses its critical impacts on food security and social well-being. It also evaluates adaptation measures across different countries, highlighting their strengths and weaknesses and enabling quick identification of areas for improvement. Additionally, it informs resilience-building efforts in vulnerable communities. Full article
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<p>Study area. Adapted from AMCOW (2018).</p>
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<p>Flow chart used for systematic review based on PRISMA 2020: <a href="https://prisma-statement.org" target="_blank">https://prisma-statement.org</a>, accessed on 4 November 2024.</p>
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<p>Drought dynamics in Sub-Saharan Africa.</p>
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<p>Drought impacts in Sub-Saharan Africa, based on Busker et al., (2023) [<a href="#B26-sustainability-16-09902" class="html-bibr">26</a>], Gebrechorkos et al., (2020) [<a href="#B21-sustainability-16-09902" class="html-bibr">21</a>], Kamali et al., (2018) [<a href="#B27-sustainability-16-09902" class="html-bibr">27</a>], Orimoloye, (2022) [<a href="#B28-sustainability-16-09902" class="html-bibr">28</a>], Von Uexkull, (2014) [<a href="#B29-sustainability-16-09902" class="html-bibr">29</a>], Orievulu et al., (2022) [<a href="#B30-sustainability-16-09902" class="html-bibr">30</a>], Bell and Keys, (2016) [<a href="#B31-sustainability-16-09902" class="html-bibr">31</a>], Treibich et al., (2022) [<a href="#B10-sustainability-16-09902" class="html-bibr">10</a>], Shukla et al., (2021) [<a href="#B32-sustainability-16-09902" class="html-bibr">32</a>], Andriano and Behrman, (2020) [<a href="#B33-sustainability-16-09902" class="html-bibr">33</a>], Haile et al., (2020) [<a href="#B34-sustainability-16-09902" class="html-bibr">34</a>], (Ajayi and Ilori, 2020) [<a href="#B35-sustainability-16-09902" class="html-bibr">35</a>].</p>
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<p>Drought projections in Sub-Saharan [<a href="#B9-sustainability-16-09902" class="html-bibr">9</a>].</p>
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19 pages, 5490 KiB  
Article
Polyurethanes Made with Blends of Polycarbonates with Different Molecular Weights Showing Adequate Mechanical and Adhesion Properties and Fast Self-Healing at Room Temperature
by Yuliet Paez-Amieva, Noemí Mateo-Oliveras and José Miguel Martín-Martínez
Materials 2024, 17(22), 5532; https://doi.org/10.3390/ma17225532 - 13 Nov 2024
Viewed by 283
Abstract
Dynamic non-covalent interactions between polycarbonate soft segments have been proposed for explaining the intrinsic self-healing of polyurethanes synthesized with polycarbonate polyols (PUs) at 20 °C. However, these self-healing PUs showed insufficient mechanical properties, and their adhesion properties have not been explored yet. Different [...] Read more.
Dynamic non-covalent interactions between polycarbonate soft segments have been proposed for explaining the intrinsic self-healing of polyurethanes synthesized with polycarbonate polyols (PUs) at 20 °C. However, these self-healing PUs showed insufficient mechanical properties, and their adhesion properties have not been explored yet. Different PUs with self-healing at 20 °C, acceptable mechanical properties, and high shear strengths (similar to the highest ones reported in the literature) were synthesized by using blends of polycarbonate polyols of molecular weights 1000 and 2000 Da (CD1000 + CD2000). Their structural, thermal, rheological, mechanical, and adhesion (single lap-shear tests) properties were assessed. PUs with higher CD1000 polyol contents exhibited shorter self-healing times and dominant viscous properties due to the higher amount of free carbonate groups, significant carbonate–carbonate interactions, and low micro-phase separation. As the CD2000 polyol content in the PUs increased, slower kinetics and longer self-healing times and higher mechanical and adhesion properties were obtained due to a dominant rheological elastic behavior, soft segments with higher crystallinities, and greater micro-phase separation. All PUs synthesized with CD1000 + CD2000 blends exhibited a mixed phase due to interactions between polycarbonate soft segments of different lengths which favored the self-healing and mobility of the polymer chains, resulting in increased mechanical properties. Full article
(This article belongs to the Special Issue Smart Soft Materials: From Design to Applications)
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<p>Scheme of the device employed to assess the self-healing ability and the kinetics of the self-healing of the PUs at 20 °C.</p>
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<p>(<b>A</b>) ATR-IR spectra of PUs obtained with CD1000 + CD2000 mixtures. (<b>B</b>) 3600–2600 cm<sup>−1</sup> region of the ATR-IR spectra.</p>
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<p>Variation of I<sub>C=O</sub>/I<sub>OC(O)O</sub> ratios of PUs obtained with CD1000 + CD2000 mixtures with respect to their CD2000 polyol content.</p>
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<p>Curve fitting of the carbonyl stretching region of the ATR-IR spectra of some PUs obtained with CD1000 + CD2000 mixtures.</p>
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<p>X-ray diffractograms of PUs obtained with CD1000 + CD2000 mixtures.</p>
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<p>Variation in the intensities of the crystalline peaks at different 2θ values of PUs obtained with CD1000 + CD2000 mixtures as a function of their CD2000 polyol content. X-ray diffractograms.</p>
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<p>DSC curves of PUs obtained with CD1000 + CD2000 mixtures. First heating run.</p>
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<p>TGA curves of PUs obtained with CD1000 + CD2000 mixtures.</p>
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<p>Derivatives of the TGA curves of PUs obtained with CD1000 + CD2000 mixtures. TGA experiments.</p>
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<p>Variation in the storage (E′) moduli as a function of the temperature for PUs obtained with CD1000 + CD2000 mixtures. DMA experiments.</p>
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<p>Variation in tan delta as a function of temperature for PUs obtained with CD1000 + CD2000 mixtures. DMA experiments.</p>
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<p>Stress–strain curves of PUs obtained with CD1000 + CD2000 mixtures.</p>
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<p>Self-healing kinetics at 20 °C of PUs obtained with CD1000 + CD2000 mixtures.</p>
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<p>Variation in the self-healing time at 20 °C of PUs obtained with CD1000+CD2000 mixtures as a function of their CD2000 polyol content.</p>
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<p>Scheme of the interactions among polycarbonate soft segments of different molecular weights in 60C1000-40C2000. CD1000 soft segments are shown in black and CD2000 soft segments are shown in red.</p>
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<p>Shear strength vs. displacement curves of stainless steel/PU adhesive/stainless steel joints.</p>
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<p>Variation in the shear strength of stainless steel/PU adhesive/stainless steel joints as a function of the CD2000 polyol content in the PU.</p>
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15 pages, 1293 KiB  
Article
Nonlinear Dynamics Analysis of Handgrip Strength Using the Poincaré Plot Method Through Video Processing Techniques
by Constantin Ciucurel and Elena Ioana Iconaru
J. Funct. Morphol. Kinesiol. 2024, 9(4), 234; https://doi.org/10.3390/jfmk9040234 - 13 Nov 2024
Viewed by 341
Abstract
Background/Objectives: The aim of this study was to analyze the nonlinear dynamics of handgrip strength (HGS) in young adults, focusing on hand dominance, by employing the Poincaré plot method to assess short- and long-term variability utilizing dynamometry and video motion capture during sustained [...] Read more.
Background/Objectives: The aim of this study was to analyze the nonlinear dynamics of handgrip strength (HGS) in young adults, focusing on hand dominance, by employing the Poincaré plot method to assess short- and long-term variability utilizing dynamometry and video motion capture during sustained isometric contractions. Methods: A cross-sectional exploratory study was conducted on 30 healthy subjects (mean age 21.6 ± 1.3 years, 13 males and 17 females), measuring HGS for both the dominant hand (DH) and nondominant hand (NDH) using a Saehan hydraulic dynamometer during 25-s sustained isometric contractions. A GoPro HERO11 Black camera recorded the dynamometer’s needle movements, and the video data were analyzed using Kinovea software. Angular values were converted to force using a calibration-based formula, and the Poincaré plot computed variability indices (short-term variability—SD1, long-term variability—SD2, ratio SD1/SD2, and area of the fitting ellipse) for each hand in relation to HGS and angular velocity (AV). Data analysis included descriptive and inferential statistics. Results: We demonstrated a strong correlation between mechanical and video measurements (p ≤ 0.001), confirming the reliability of the video method. The findings highlight the importance of nonlinear analysis in understanding neuromuscular function and fatigue, revealing significant correlations among HGS, AV, Poincaré indices, and fatigue levels in both hands (p ≤ 0.001). Increased maximum HGS and AV correlated with higher nonlinear variability in force production. Conclusions: This study confirms the reliability of the proposed video-based HGS assessment and demonstrates the effectiveness of Poincaré plot analysis for capturing nonlinear variability in HGS. Full article
(This article belongs to the Section Kinesiology and Biomechanics)
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<p>Flowchart of the recruitment process for participants in the study (n: number of subjects).</p>
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<p>Typical Poincaré plot for a subject’s handgrip strength data: (<b>a</b>) dominant hand; (<b>b</b>) nondominant hand.</p>
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<p>Typical Poincaré plot for a subject’s angular velocity data: (<b>a</b>) dominant hand; (<b>b</b>) nondominant hand.</p>
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14 pages, 2909 KiB  
Article
Laser-Induced Decomposition and Mechanical Degradation of Carbon Fiber-Reinforced Polymer Subjected to a High-Energy Laser with Continuous Wave Power up to 120 kW
by Sebastian Schäffer, Stefan Reich, Dominic Heunoske, Martin Lueck, Johannes Wolfrum and Jens Osterholz
J. Compos. Sci. 2024, 8(11), 471; https://doi.org/10.3390/jcs8110471 - 13 Nov 2024
Viewed by 328
Abstract
Carbon fiber-reinforced polymer (CFRP), noted for its outstanding properties including high specific strength and superior fatigue resistance, is increasingly employed in aerospace and other demanding applications. This study investigates the interactions between CFRP composites and high-energy lasers (HEL), with continuous wave laser powers [...] Read more.
Carbon fiber-reinforced polymer (CFRP), noted for its outstanding properties including high specific strength and superior fatigue resistance, is increasingly employed in aerospace and other demanding applications. This study investigates the interactions between CFRP composites and high-energy lasers (HEL), with continuous wave laser powers reaching up to 120 kW. A novel automated sample exchange system, operated by a robotic arm, minimizes human exposure while enabling a sequence of targeted laser tests. High-speed imaging captures the rapid expansion of a plume consisting of hot gases and dust particles during the experiment. The research significantly advances empirical models by systematically examining the relationship between laser power, perforation times, and ablation rates. It demonstrates scalable predictions for the effects of high-energy laser radiation. A detailed examination of the damaged samples, both visually and via micro-focused computed X-ray tomography, offers insights into heat distribution and ablation dynamics, highlighting the anisotropic thermal properties of CFRP. Compression after impact (CAI) tests further assess the residual strength of the irradiated samples, enhancing the understanding of CFRP’s structural integrity post-irradiation. Collectively, these tests improve the knowledge of the thermal and mechanical behavior of CFRP under extreme irradiation conditions. The findings not only contribute to predictive modeling of CFRP’s response to laser irradiation but enhance the scalability of these models to higher laser powers, providing robust tools for predicting material behavior in high-performance settings. Full article
(This article belongs to the Special Issue Carbon Fiber Composites, Volume III)
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<p>Experimental setup includes an automated sample exchange, operated by a robotic arm.</p>
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<p>A gas cloud expands rapidly caused by laser irradiation of a CFRP plate with 120 kW and a beam size of 20 mm. The plate is perforated after 0.4 s.</p>
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<p>Damage zones of irradiated CFRP samples of two tested materials (P = 120 kW, Ø = 20 mm, d = 4 mm). The heat affected zone (HAZ) extends to areas outside the applied laser spot.</p>
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<p>Perforation times as a function of laser power in a double-logarithmic representation for a beam diameter of 20 mm and different sample thicknesses d. In this diagram, a linear decrease of the logarithm of the perforation time with increase of the logarithm of the laser power can be observed, represented by the solid and dashed lines.</p>
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<p>Volume damage as a function of perforation time in a double-logarithmic representation for various laser powers.</p>
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<p>Volume removal rate as a function of laser power. Symbols: <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>r</mi> </mrow> <mrow> <mi>v</mi> <mi>o</mi> <mi>l</mi> </mrow> </msub> </mrow> </semantics></math> determined from experimental data and Equation (4). Lines: linear fit.</p>
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<p>µCT-scan cross-sections of irradiated CFRP samples reveal details of the heat affected zone and the delamination of fibers. The holes created have a conical shape (M18-1/G939, d = 6 mm).</p>
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<p>Residual compressive strength of laser irradiated CFRP samples determined in accordance with the compression after impact procedure.</p>
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20 pages, 6207 KiB  
Article
Egg White-Based Gels with Candelilla Wax: A Study of Rheological, Mechanical, Calorimetric and Microstructural Properties
by Iram Cisneros-García, Ma. de la Paz Salgado-Cruz, Alitzel B. García-Hernández, Gustavo F. Gutiérrez-López, Humberto Hernández-Sánchez, Brenda H. Camacho-Díaz and Liliana Alamilla-Beltrán
Gels 2024, 10(11), 733; https://doi.org/10.3390/gels10110733 - 13 Nov 2024
Viewed by 396
Abstract
Bigels (BGs) are innovative composite systems that integrate oleogel and hydrogel structures, and are gaining increasing attention for their unique textural and functional properties in food applications. This study evaluated the rheological and mechanical properties of egg white-based bigels incorporating candelilla wax (CW) [...] Read more.
Bigels (BGs) are innovative composite systems that integrate oleogel and hydrogel structures, and are gaining increasing attention for their unique textural and functional properties in food applications. This study evaluated the rheological and mechanical properties of egg white-based bigels incorporating candelilla wax (CW) as an oleogelator. The results indicate that different egg white protein (EWP) (5–10%) concentrations and hydrogel-to-oleogel ratios (20:80 to 80:20) significantly influenced the structural and functional properties of the bigels. Compression testing revealed no significant differences in strength across the tested range; however, higher EWP concentrations enhanced the stability of the BGs. Furthermore, increased candelilla wax oleogel (CWO) content (60%) markedly improved emulsion stability, resulting in superior strength, as confirmed by dynamic light scattering. Rheological studies demonstrated shear-thinning behavior, particularly at higher hydrogel content related to the oleogel (W/O), which exhibited the highest yield stress. Microstructural investigations confirmed the presence of a continuous oleogel phase within the bigels (W/O) and revealed the formation of a complex structure. These findings suggest that a reduced hydrogel-to-oleogel ratio can be utilized across various food systems, opening new possibilities for creating customized food structures with desirable textural and functional attributes. Full article
(This article belongs to the Special Issue Functionality of Oleogels and Bigels in Foods)
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<p>Comparison of compression force in bigels at different protein concentrations and H/O ratios. Means with different letters differ significantly (<span class="html-italic">p</span> &lt; 0.05, Tukey’s test). SD, Standard Deviation.</p>
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<p>Images of the surface structure of the bigels were captured using a stereoscope.</p>
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<p>Turbiscan Stability Index (TSI) (<b>a</b>) and backscattering (BS) profiles (<b>b</b>) over 143 h of storage for emulsion formulations with varying hydrogel/oleogel ratios and EWP concentrations at 25 °C. Images of the emulsions after 143 h of storage (<b>c</b>).</p>
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<p>Thermograms of emulsion formulations with varying H/O ratios and EWP concentrations: (<b>a</b>) heating and (<b>b</b>) cooling phases.</p>
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<p>Rheological analysis of emulsion formulations: shear stress vs. shear rate. The red circle highlights the initial slope observed in the early stages of each emulsion’s behavior.</p>
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<p>Rheological analysis of emulsion formulations: (<b>a</b>) heating and (<b>b</b>) cooling temperature sweeps.</p>
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<p>Amplitude sweeps, all with varying H/O ratios and EWP concentrations.</p>
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<p>Polarized light microscopy (PLM, (<b>a</b>–<b>j</b>)) and brightfield microscopy (BF, (<b>c</b>–<b>l</b>)) images from left to right of emulsions (<b>left</b>) and bigel (<b>right</b>). Scale bar: 100 μm. Micrographs were obtained with a magnification of 4×. Yellow circles and arrows highlight the crystalized CW surrounding the dispersed phase. Orange arrows indicate the oleogel droplets, while green arrows point to the bubbles.</p>
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<p>CLSM images of emulsions (left, (<b>a</b>–<b>j</b>)) and bigel (right, (<b>c</b>–<b>l</b>)). Oil staining by Nile red and EWP by FTIC from left to right. Scale bar: 20 μm. Micrographs were obtained with a magnification of 40×.</p>
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<p>Formation of the bigel involves two stages: first, the emulsification process, followed by the emulsion gelling process.</p>
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