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16 pages, 3480 KiB  
Article
Evaluating the Seismic Resilience of Above-Ground Liquid Storage Tanks
by Emanuele Brunesi and Roberto Nascimbene
Buildings 2024, 14(10), 3212; https://doi.org/10.3390/buildings14103212 - 9 Oct 2024
Viewed by 407
Abstract
Historical seismic events have repeatedly highlighted the susceptibility of above-ground liquid storage steel tanks, underscoring the critical need for their proper design to minimize potential damage due to seismic forces. A significant failure mechanism in these structures, which play essential roles in the [...] Read more.
Historical seismic events have repeatedly highlighted the susceptibility of above-ground liquid storage steel tanks, underscoring the critical need for their proper design to minimize potential damage due to seismic forces. A significant failure mechanism in these structures, which play essential roles in the extraction and distribution of various raw or refined materials—many of which are flammable or environmentally hazardous—is the dynamic buckling of the tank walls. This study introduces a numerical framework designed to assess the earthquake-induced hydrodynamic pressures exerted on the walls of cylindrical steel tanks. These pressures result from the inertial forces generated during seismic activity. The computational framework incorporates material and geometric nonlinearities and models the tanks using four-node shell elements with two-point integration, specifically Belytschko shell elements. The Arbitrary Lagrangian–Eulerian (ALE) method is employed to accommodate substantial structural and fluid deformations, enabling a full simulation of fluid–structure interaction through highly nonlinear algorithms. Experimental test data are utilized to validate the proposed modeling approach, particularly in replicating sloshing phenomena and identifying stress concentrations that may lead to wall buckling. The study further presents results from a parametric analysis that varies the height-to-radius and radius-to-thickness ratios of a typical anchored flat-bottomed tank, examining the seismic performance of this common storage system. These results provide insights into the relationship between tank properties and mechanical behavior under dynamic loading conditions. Full article
(This article belongs to the Section Building Structures)
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<p>(<b>a</b>–<b>c</b>) illustrate examples of elephant’s foot buckling mechanisms, while (<b>d</b>–<b>f</b>) show instances of diamond-shaped buckling. These failure modes were commonly observed in the aftermath of the May 2012 Emilia seismic sequence.</p>
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<p>Anchoring system-related failure modes were observed in both flat-base and leg-supported storage tanks during the May 2012 Emilia seismic sequence. (<b>a</b>,<b>b</b>) demonstrate issues in flat-base tanks, including the fracture of anchor bolts and significant spalling of the concrete foundation at the anchorage points; (<b>c</b>,<b>d</b>) depict leg-supported tanks that suffered from a loss of verticality, primarily due to shear-buckling in the stocky, tapered support legs.</p>
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<p>The high-definition finite element (FE) model was meticulously developed to closely simulate the outcomes of shake-table tests. This advanced modeling approach was essential for accurately replicating the dynamic responses and structural behaviors observed during controlled seismic testing, providing vital insights into the performance of the structures under simulated earthquake conditions.</p>
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<p>The tank specimen evaluated by Manos and Clough [<a href="#B55-buildings-14-03212" class="html-bibr">55</a>] is a scaled model, specifically designed to facilitate detailed study under laboratory conditions: summary of the main geometrical properties.</p>
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<p>The comparison of pressure time histories from numerical simulations and experimental tests conducted by Manos and Clough [<a href="#B55-buildings-14-03212" class="html-bibr">55</a>] reveals a meticulous alignment of results, affirming the robustness of the numerical models used.</p>
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<p>Finite element model showcases the deformed shapes of the tank at different time instants, visually demonstrating how the structure distorts in response to seismic forces (as tested by Haroun [<a href="#B56-buildings-14-03212" class="html-bibr">56</a>]).</p>
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<p>Elastic acceleration displacement response spectra from recorded time histories at MRN station (NS and EW) and in accordance with the Italian building code [<a href="#B62-buildings-14-03212" class="html-bibr">62</a>].</p>
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<p>Total wall pressure distribution along the height for (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>/</mo> <mi>R</mi> </mrow> </semantics></math> = 1.5 and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>/</mo> <mi>R</mi> </mrow> </semantics></math> = 3.0.</p>
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<p>Elastic displacement response spectra from ground motion records selected by Maley et al. [<a href="#B63-buildings-14-03212" class="html-bibr">63</a>].</p>
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<p>Wall pressure peak profiles (individual records, mean, and mean plus one standard deviation) for (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>/</mo> <mi>R</mi> </mrow> </semantics></math> = 0.75 and <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>/</mo> <mi>t</mi> </mrow> </semantics></math> = 2000, (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>/</mo> <mi>R</mi> </mrow> </semantics></math> = 1.5 and <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>/</mo> <mi>t</mi> </mrow> </semantics></math> = 400, and (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>/</mo> <mi>R</mi> </mrow> </semantics></math> = 4 and <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>/</mo> <mi>t</mi> </mrow> </semantics></math> = 400.</p>
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<p>Comparison between wall pressure peak profiles (mean and mean plus standard deviation).</p>
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20 pages, 6774 KiB  
Article
A Driving Warning System for Explosive Transport Vehicles Based on Object Detection Algorithm
by Jinshan Sun, Ronghuan Zheng, Xuan Liu, Weitao Jiang and Mutian Jia
Sensors 2024, 24(19), 6339; https://doi.org/10.3390/s24196339 - 30 Sep 2024
Viewed by 378
Abstract
Due to the flammable and explosive nature of explosives, there are significant potential hazards and risks during transportation. During the operation of explosive transport vehicles, there are often situations where the vehicles around them approach or change lanes abnormally, resulting in insufficient avoidance [...] Read more.
Due to the flammable and explosive nature of explosives, there are significant potential hazards and risks during transportation. During the operation of explosive transport vehicles, there are often situations where the vehicles around them approach or change lanes abnormally, resulting in insufficient avoidance and collision, leading to serious consequences such as explosions and fires. Therefore, in response to the above issues, this article has developed an explosive transport vehicle driving warning system based on object detection algorithms. Consumer-level cameras are flexibly arranged around the vehicle body to monitor surrounding vehicles. Using the YOLOv4 object detection algorithm to identify and distance surrounding vehicles, using a game theory-based cellular automaton model to simulate the actual operation of vehicles, simulating the driver’s decision-making behavior when encountering other vehicles approaching or changing lanes abnormally during actual driving. The cellular automaton model was used to simulate two scenarios of explosive transport vehicles equipped with and without warning systems. The results show that when explosive transport vehicles encounter the above-mentioned dangerous situations, the warning system can timely issue warnings, remind drivers to make decisions, avoid risks, ensure the safety of vehicle operation, and verify the effectiveness of the warning system. Full article
(This article belongs to the Section Sensing and Imaging)
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<p>Framework diagram of research ideas.</p>
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<p>Schematic diagram of monocular camera ranging principle.</p>
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<p>Dimensions of freight cars.</p>
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<p>Camera layout.</p>
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<p>Camera appearance.</p>
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<p>YOLOv4 network structure [<a href="#B19-sensors-24-06339" class="html-bibr">19</a>].</p>
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<p>Example of vehicle data images.</p>
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<p>Training images and box labels.</p>
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<p>Enhanced training dataset.</p>
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<p>The results of training.</p>
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<p>PR curve.</p>
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<p>Loss function curve.</p>
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<p>Capturing vehicle image information (safe vehicle distance).</p>
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<p>Capture vehicle image information (when the current rear distance is less than 60 m or the left and right distance is less than 1.5 m).</p>
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<p>Lane-changing rules.</p>
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<p>Flow chart of simulation steps for cellular automata.</p>
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<p>Traffic flow statistics.</p>
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<p>Statistical chart of average vehicle speed.</p>
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<p>Statistical chart of average vehicle density.</p>
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<p>Simulation process of cellular automata (time step 291).</p>
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<p>Program warning interface.</p>
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<p>Collision statistics without warning system.</p>
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<p>Collision statistics equipped with warning system.</p>
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12 pages, 3361 KiB  
Article
Investigation of the Effects Caused by Current Interruption Devices of Lithium Cells at High Overvoltages
by Jan Haß, Christina Schieber, Florian Meilinger, Yash Kotak, Serkan Sevinc, Philipp Lang and Hans-Georg Schweiger
Appl. Sci. 2024, 14(18), 8238; https://doi.org/10.3390/app14188238 - 12 Sep 2024
Viewed by 651
Abstract
A faulty voltage measurement can lead to the overcharging of a Li-Ion cell, resulting in gas formation and heating inside the cell, which can trigger thermal runaway. To mitigate this risk, cylindrical cells are equipped with a Current Interrupt Device (CID), which functions [...] Read more.
A faulty voltage measurement can lead to the overcharging of a Li-Ion cell, resulting in gas formation and heating inside the cell, which can trigger thermal runaway. To mitigate this risk, cylindrical cells are equipped with a Current Interrupt Device (CID), which functions as a pressure relief valve, disconnecting the electrical circuit within the cell when internal pressure rises. However, this disconnection causes the cell to suddenly become highly resistant, posing a significant issue in series-connected cells. In such configurations, a portion or even the entire system voltage may drop across the disconnected cell, substantially increasing the likelihood of an electric arc. This arc could ignite any escaping flammable gases, leading to catastrophic failures. In a series of tests conducted on three different cell chemistries—NMC (Nickel Manganese Cobalt), NCA (Nickel Cobalt Aluminum), and LFP (Lithium Iron Phosphate)—it was found that the safe operation of the CID cannot be guaranteed for system voltages exceeding 120 V. Although comparative tests at double the nominal cell voltage did not exhibit the same behavior, these findings suggest that current safety standards, which recommend testing at double the nominal voltage, may not adequately address the risks involved. The tests further revealed that series connections of cells with CIDs are inherently dangerous, as, in the worst-case scenario, the entire system voltage can be concentrated across a single cell, leading to potential system failure. Full article
(This article belongs to the Section Energy Science and Technology)
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<p>Current Interrupt Device before opening, with a representation of the components of the part [<a href="#B6-applsci-14-08238" class="html-bibr">6</a>].</p>
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<p>Current Interrupt Device during the disconnection, with a schematic representation of degassing process [<a href="#B6-applsci-14-08238" class="html-bibr">6</a>].</p>
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<p>Example circuit for an CID opening in cell inside battery system. The complete systems voltage will drop at a cell whose internal resistance is high due to the opening of a CID or overcharge protection additive [<a href="#B15-applsci-14-08238" class="html-bibr">15</a>].</p>
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<p>CT-Scans of the different 18,650 cells, which are different in the positive active materials and CIDs.</p>
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<p>Test setup. V<sub>1</sub>–V<sub>4</sub> represent voltage sources for supplying the measuring devices.</p>
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<p>CID has correctly interrupted the current flow. This is typical behavior for the correct separation of CID. Hazard level 3 [<a href="#B21-applsci-14-08238" class="html-bibr">21</a>].</p>
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<p>The CID has partially interrupted the current flow. This is not typical behavior for separating CID. Hazard level 4 [<a href="#B21-applsci-14-08238" class="html-bibr">21</a>].</p>
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<p>The CID was not able to disconnect the current flow. The overcharging process leads to burn out or explosion of the cell. Hazard level 5 [<a href="#B21-applsci-14-08238" class="html-bibr">21</a>] or higher.</p>
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<p>Results of the abuse tests, sorted by voltage level.</p>
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<p>Illustration of the binary logistic regression, between the state safe 1 and the state unsafe 0. The blue marked area is the voltage range of currently very common electric cars.</p>
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35 pages, 3046 KiB  
Review
Chemicals from Brominated Flame Retardants: Analytical Methods, Occurrence, Transport and Risks
by Christian Ebere Enyoh, Tochukwu Oluwatosin Maduka, Md. Sohel Rana, Sochi Chinaemerem Osigwe, Stanley Chukwuemeka Ihenetu and Qingyue Wang
Appl. Sci. 2024, 14(17), 7892; https://doi.org/10.3390/app14177892 - 5 Sep 2024
Viewed by 1126
Abstract
Brominated flame retardants (BFRs) are synthetic chemicals widely used to reduce the flammability of consumer products, including electronics, textiles, and furniture. Despite their effectiveness in fire prevention, BFRs pose significant environmental and health risks due to their persistence, bioaccumulation, and potential toxicity. This [...] Read more.
Brominated flame retardants (BFRs) are synthetic chemicals widely used to reduce the flammability of consumer products, including electronics, textiles, and furniture. Despite their effectiveness in fire prevention, BFRs pose significant environmental and health risks due to their persistence, bioaccumulation, and potential toxicity. This review provides a comprehensive examination of BFRs, focusing on recent advancements in analytical methods for their detection and quantification in environmental and biological samples. The study explored the physicochemical properties that influence BFR distribution and transport in various matrices, including soil, water, air, sediments, and biota. The review also summarizes current knowledge on the occurrence and environmental fate of BFRs, highlighting their mobility and long-range transport. Furthermore, the study discusses the health risks associated with BFR exposure, emphasizing their endocrine-disrupting effects and impact on reproductive and neurological functions. By integrating findings from recent studies, this review aims to enhance the understanding of BFR behavior and inform regulatory strategies to mitigate their adverse effects on human health and the environment. Full article
(This article belongs to the Special Issue Emerging Contaminants in Environment)
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<p>The passive air sampling device (<b>A</b>) and polyurethane foam disk (<b>B</b>) used in the study and the schemes of the device assembling (<b>C</b>) and passive air sampling principle (<b>D</b>); data are from [<a href="#B54-applsci-14-07892" class="html-bibr">54</a>].</p>
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<p>Migration pathways of BFRs in the environment (modified from Wang et al. [<a href="#B87-applsci-14-07892" class="html-bibr">87</a>]).</p>
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<p>Postulated reaction mechanisms for anaerobic microbial transformation of <span class="html-italic">β</span>-TBCO (<b>A</b>) and DPTE (<b>B</b>) (Adapted from [<a href="#B56-applsci-14-07892" class="html-bibr">56</a>]).</p>
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<p>Main microbial transformation mechanisms for β-TBCO and DPTE involve β-elimination (E2) and Sn2-nucleophilic substitution (Adapted from Huang et al. [<a href="#B56-applsci-14-07892" class="html-bibr">56</a>]).</p>
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22 pages, 13498 KiB  
Article
Experimental Research on Thermal-Venting Characteristics of the Failure 280 Ah LiFePO4 Battery: Atmospheric Pressure Impacts and Safety Assessment
by Yu Wang, Yan Wang, Jingyuan Zhao, Hongxu Li, Chengshan Xu, Yalun Li, Hewu Wang, Languang Lu, Feng Dai, Ruiguang Yu and Feng Qian
Batteries 2024, 10(8), 270; https://doi.org/10.3390/batteries10080270 - 29 Jul 2024
Cited by 1 | Viewed by 1041
Abstract
With the widespread application of lithium-ion batteries (LIBs) energy storage stations in high-altitude areas, the impact of ambient pressure on battery thermal runaway (TR) behavior and venting flow characteristics have aroused wide research attention. This paper conducts a lateral heating experiment on 280 [...] Read more.
With the widespread application of lithium-ion batteries (LIBs) energy storage stations in high-altitude areas, the impact of ambient pressure on battery thermal runaway (TR) behavior and venting flow characteristics have aroused wide research attention. This paper conducts a lateral heating experiment on 280 Ah lithium iron phosphate batteries (LFPs) and proposes a method for testing battery internal pressure using an embedded pressure sensor. This paper analyzes the battery characteristic temperature, internal pressure, chamber pressure, and gas components under different chamber pressures. The experiment is carried out in a N2 atmosphere using a 1000 L insulated chamber. At 40 kPa, the battery experiences two instances of venting, with a corresponding peak in temperature on the battery’s side of 136.3 °C and 302.8 °C, and gas generation rates of 0.14 mol/s and 0.09 mol/s, respectively. The research results indicate that changes in chamber pressure significantly affect the center temperature of the battery side (Ts), the center temperature of the chamber (Tc), the opening time of the safety valve (topen), the triggering time of TR (tTR), the time difference (Δt), venting velocity, gas composition, and flammable limits. However, the internal pressure and gas content of the battery are apparently unaffected. Considering the TR characteristics mentioned above, a safety assessment method is proposed to evaluate the TR behavior and gas hazard of the battery. The results indicate that the risk at 40 kPa is much higher than the other three chamber pressures. This study provides theoretical references for the safe use and early warning of energy storage LIBs in high-altitude areas. Full article
(This article belongs to the Special Issue Thermal Safety of Lithium Ion Batteries)
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<p>(<b>a</b>) Experimental flow chart. (<b>b</b>) Experimental chamber. (<b>c</b>) Battery changes after thermal runaway experiment. (<b>d</b>) Data collection. (<b>e</b>) GC analysis.</p>
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<p>Battery embedded sensor method.</p>
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<p>TR experimental diagram.</p>
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<p>Feature temperatures at 40 kPa. (<b>a</b>) Battery safety valve temperature; (<b>b</b>) temperature rise rate of valve; (<b>c</b>) center temperature of battery side; (<b>d</b>) center temperature of chamber.</p>
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<p>Internal and chamber pressure. (<b>a</b>) Battery internal pressure and pressure difference; (<b>b</b>) chamber pressure and valve temperature.</p>
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<p>Gas composition distribution at 40 kPa.</p>
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<p>Gas venting characteristics at 40 kPa. (<b>a</b>) Molar of gas; (<b>b</b>) mass of gas; (<b>c</b>) volume of gas.</p>
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<p>Side temperature comparison. (<b>a</b>) Side center temperature; (<b>b</b>) peak temperature.</p>
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<p>Comparison of the central temperature in chamber. (<b>a</b>) Temperature in center of chamber; (<b>b</b>) peak temperature.</p>
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<p>The internal pressure. (<b>a</b>) Internal pressure change; (<b>b</b>) peak internal pressure.</p>
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<p>The chamber pressure. (<b>a</b>) Pressure changes in chamber; (<b>b</b>) peak pressure changes.</p>
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<p>The pressure difference. (<b>a</b>) Pressure difference; (<b>b</b>) Peak pressure difference.</p>
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<p>The key time of TR.</p>
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<p>Comparison of gas content.</p>
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<p>The proportion of gases at different pressures.</p>
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<p>Flammability limit of mixture. (<b>a</b>) UEL and LEL; (<b>b</b>) flammability limit range.</p>
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<p>Comparison of radar charts in different pressures.</p>
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21 pages, 9102 KiB  
Article
The Recyclability of Fire-Retarded Biobased Polyamide 11 (PA11) Composites Reinforced with Basalt Fibers (BFs): The Influence of Reprocessing on Structure, Properties, and Fire Behavior
by Mateusz Barczewski, Aleksander Hejna, Jacek Andrzejewski, Joanna Aniśko, Adam Piasecki, Adrian Mróz, Zaida Ortega, Daria Rutkowska and Kamila Sałasińska
Molecules 2024, 29(13), 3233; https://doi.org/10.3390/molecules29133233 - 8 Jul 2024
Viewed by 1165
Abstract
The growing requirements regarding the safety of using polymers and their composites are related to the emergence of more effective, sustainable, and hazardous-limited fire retardants (FRs). Significant amounts of FRs are usually required to effectively affect a polymer’s burning behavior, while the knowledge [...] Read more.
The growing requirements regarding the safety of using polymers and their composites are related to the emergence of more effective, sustainable, and hazardous-limited fire retardants (FRs). Significant amounts of FRs are usually required to effectively affect a polymer’s burning behavior, while the knowledge of their recycling potential is still insufficient. At the same time, concerns are related not only to the reduced effectiveness of flame retardancy but also, above all, to the potential deterioration of mechanical properties caused by the degradation of temperature-affected additives under processing conditions. This study describes the impact of the four-time reprocessing of bio-based polyamide 11 (PA11) modified with an intumescent flame-retardant (IFR) system composed of ammonium polyphosphate (APP), melamine cyanurate (MC), and pentaerythritol (PER) and its composites containing additional short basalt fibers (BFs). Composites manufactured via twin-screw extrusion were subjected to four reprocessing cycles using injection molding. A comprehensive analysis of their structural, mechanical, and fire behavior changes in each cycle was conducted. The obtained results confirmed the safety of using the proposed fire-retarded polyamide and its composites while reprocessing under the recommended process parameters without the risk of significant changes in the structure. The partial increase in flammability of reprocessed PA-based materials caused mainly by polymer degradation has been described. Full article
(This article belongs to the Special Issue Recent Advances in Flame Retardant Polymeric Materials)
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<p>Cooling (<b>a</b>) and second heating (<b>b</b>); DSC thermograms measured for PA and its composites subjected to multiple reprocessing.</p>
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<p>SEM images of brittle fractured injection-molded samples in two magnifications after 1st and 4th processing.</p>
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<p>FTIR spectra of PA11 (<b>a</b>); IFR (<b>b</b>); and IFR+BF (<b>c</b>) after reprocessing.</p>
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<p>FTIR spectra of PA11 (<b>a</b>); IFR (<b>b</b>); and IFR+BF (<b>c</b>) after reprocessing.</p>
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<p>Mechanical properties of reprocessed polyamide, tensile (<b>a</b>,<b>c</b>,<b>e</b>), flexural (<b>b</b>,<b>d</b>), Izod impact (<b>f</b>), and ball indentation hardness (<b>g</b>) tests.</p>
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<p>Thermomechanical properties of reprocessed polyamide; VST (<b>a</b>) and HDT (<b>b</b>).</p>
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<p>HRR vs. time curves (<b>a</b>–<b>c</b>) and relative changes in pHRR and THR caused by successive reprocessing cycles (<b>d</b>).</p>
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<p>TG and DTG curves for PA11 (<b>a,b</b>), IFR (<b>c,d</b>), and IFR+BF (<b>e,f</b>) after the first and fourth processing.</p>
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<p>The Gram–Schmidt profile obtained from an analysis of the gases emitted during the TGA of PA11, IFR, and IFR+BF after the first and fourth reprocessing.</p>
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<p>FTIR spectra of gases for each set of materials at the temperatures at which the most significant thermal events were recorded.</p>
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30 pages, 5344 KiB  
Review
Bio-Sourced Flame Retardants for Textiles: Where We Are and Where We Are Going
by Giulio Malucelli
Molecules 2024, 29(13), 3067; https://doi.org/10.3390/molecules29133067 - 27 Jun 2024
Cited by 1 | Viewed by 775
Abstract
After the period of halogenated compounds, the period of nano-structured systems, and that of phosphorus (and nitrogen)-based additives (still in progress), following the increasingly demanding circular economy concept, about ten years ago the textile flame retardant world started experiencing the design and exploitation [...] Read more.
After the period of halogenated compounds, the period of nano-structured systems, and that of phosphorus (and nitrogen)-based additives (still in progress), following the increasingly demanding circular economy concept, about ten years ago the textile flame retardant world started experiencing the design and exploitation of bio-sourced products. Indeed, since the demonstration of the potential of such bio(macro)molecules as whey proteins, milk proteins (i.e., caseins), and nucleic acids as effective flame retardants, both natural and synthetic fibers and fabrics can take advantage of the availability of several low-environmental impact/“green” compounds, often recovered from wastes or by-products, which contain all the elements that typically compose standard flame-retardant recipes. The so-treated textiles often exhibit flame-retardant features that are similar to those provided by conventional fireproof treatments. Further, the possibility of using the same deposition techniques already available in the textile industry makes these products very appealing, considering that the application methods usually do not require hazardous or toxic chemicals. This review aims to present an overview of the development of bio-sourced flame retardants, focusing attention on the latest research outcomes, and finally discussing some current challenging issues related to their efficient application, paving the way toward further future implementations. Full article
(This article belongs to the Section Materials Chemistry)
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Graphical abstract

Graphical abstract
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<p>The number of publications (from 2015 to 2024) in peer-reviewed journals, dealing with “Bio-based AND Flame retardants AND textiles” (AND is the Boolean operator; data collected from the Web of Science<sup>TM</sup> database, <a href="http://www.webofscience.com" target="_blank">www.webofscience.com</a>, accessed on 19 June 2024).</p>
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<p>Classification of bio-sourced flame retardants.</p>
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<p>Chemical structure of β-cyclodextrin. Reprinted with permission from [<a href="#B33-molecules-29-03067" class="html-bibr">33</a>]. Copyright 2007, Elsevier.</p>
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<p>Chemical structure of chitin and chitosan. Reprinted from [<a href="#B34-molecules-29-03067" class="html-bibr">34</a>] under CC-BY license.</p>
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<p>Chemical structure of tea saponin. Reprinted with permission from [<a href="#B43-molecules-29-03067" class="html-bibr">43</a>]. Copyright Elsevier, 2019.</p>
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<p>Structure of DNA. Adapted with permission from [<a href="#B45-molecules-29-03067" class="html-bibr">45</a>]. Copyright American Chemical Society, 2016.</p>
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<p>Intumescent features of DNA, as assessed through cone calorimetry tests performed at different irradiative heat fluxes (from 25 to 75 kW/m<sup>2</sup>). Reprinted with permission from [<a href="#B46-molecules-29-03067" class="html-bibr">46</a>]. Copyright Elsevier, 2014.</p>
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<p>Chemical structure of lignin. Reprinted from [<a href="#B63-molecules-29-03067" class="html-bibr">63</a>] under CC-BY license.</p>
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<p>Chemical structure of phloroglucinol.</p>
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<p>Chemical structures of cardanol, cardol, and 2-methylcardol, the constituents of technical-grade cashew nutshell liquid. Reprinted from [<a href="#B73-molecules-29-03067" class="html-bibr">73</a>] under CC-BY License.</p>
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<p>Chemical structure of levulinic acid (4-oxopentanoic acid).</p>
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<p>Chemical structure of phytic acid. Reprinted from [<a href="#B83-molecules-29-03067" class="html-bibr">83</a>] under CC-BY License.</p>
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<p>Results from vertical flame spread tests (<b>A</b>) and forced combustion tests performed at 35 kW/m<sup>2</sup> irradiative heat flux (<b>B</b>) for cotton and the fabrics treated with ammonium starch phosphate (ASP) at different loadings, before and after 50 laundry cycles. Legend: 1 = untreated cotton; 2, 3, 4 = cotton treated with ammonium starch phosphate at different loadings (24.1, 26.9, and 33.1 wt.%, respectively); 5, 6, 7 = samples 2, 3 and 4 tested after 50 laundry cycles. Adapted with permission from [<a href="#B86-molecules-29-03067" class="html-bibr">86</a>]. Copyright Elsevier, 2022.</p>
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<p>Results from forced combustion tests carried out at 35 kW/m<sup>2</sup> on neat cotton (COT), cotton treated with 5 bilayers of chitosan/Biochar (7.5 wt.% concentration) and phytic acid (PA/CH/BC (7.5%)-COT), and on the treated fabric after 10 laundry cycles (PA/CH/BC (7.5%)-COT washed). Reprinted with permission from [<a href="#B79-molecules-29-03067" class="html-bibr">79</a>]. Copyright Elsevier, 2022.</p>
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<p>Synthesis of 2,6-dimethoxy polysaccharide ammonium phosphate. Reprinted with permission from [<a href="#B89-molecules-29-03067" class="html-bibr">89</a>]. Copyright Elsevier, 2023.</p>
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<p>Heat release Rate (<b>a</b>), Total Smoke Release (<b>b</b>), and Total Smoke Production (<b>c</b>) curves of untreated cotton (cotton) and the fabric treated with the zeolitic imidazolate framework-8 modified with chitosan and Zn<sup>2+</sup> (CZIF-8@CF). Adapted with permission from [<a href="#B90-molecules-29-03067" class="html-bibr">90</a>]. Copyright Elsevier, 2023.</p>
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<p>Results from vertical flame spread tests performed on cotton fabrics treated with a 3-(2-aminoethylamino)-propyltrimethoxysilane sol containing 14 wt.% phytic acid, after different laundry cycles. Reprinted with permission from [<a href="#B93-molecules-29-03067" class="html-bibr">93</a>]. Copyright Elsevier, 2024.</p>
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<p>Grafting reaction of ammonium phytate onto wool fabrics. Reprinted with permission from [<a href="#B98-molecules-29-03067" class="html-bibr">98</a>]. Copyright Elsevier, 2022.</p>
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<p>Results of vertical flame spread tests performed on wool fabrics treated with ammonium phytate (dry add-on: 14.2 wt.%) before and after laundry cycles. Reprinted with permission from [<a href="#B98-molecules-29-03067" class="html-bibr">98</a>]. Copyright Elsevier, 2022.</p>
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<p>Synthesis of phytate urea salt and its covalent crosslinking with silk fabrics. Adapted with permission from [<a href="#B99-molecules-29-03067" class="html-bibr">99</a>]. Copyright Elsevier, 2021.</p>
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<p>Synthesis of glycidyl phytate isocyanurate (<b>a</b>) and its covalent crosslinking with silk fabrics (<b>b</b>). Reprinted with permission from [<a href="#B100-molecules-29-03067" class="html-bibr">100</a>]. Copyright Elsevier, 2023.</p>
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<p>Typical SEM micrographs and EDS analysis of coated silk samples. Legend: Control = untreated silk; Silk-1 = the fabric treated with the reactive bio-based FR (11.8% dry add-on); Silk-2 = the fabric treated with the reactive bio-based FR (14.2% dry add-on). Reprinted with permission from [<a href="#B102-molecules-29-03067" class="html-bibr">102</a>]. Copyright Elsevier, 2023.</p>
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<p>Heat Release Rate (HRR) vs. temperature curves for pristine kapok (KF) and the phosphorylated fabrics (KFPA-X, where X represents the phytic acid dosage in g). Reprinted from [<a href="#B105-molecules-29-03067" class="html-bibr">105</a>] under CC-BY License.</p>
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19 pages, 10325 KiB  
Article
Study on Liquid Hydrogen Leakage and Diffusion Behavior in a Hydrogen Production Station
by Xiang Fu, Guodong Li, Shiyu Chen, Chunyan Song, Zhili Xiao, Hao Luo, Jiaqi Wan, Tianqi Yang, Nianfeng Xu and Jinsheng Xiao
Fire 2024, 7(7), 217; https://doi.org/10.3390/fire7070217 - 26 Jun 2024
Viewed by 1301
Abstract
Liquid hydrogen storage is an important way of hydrogen storage and transportation, which greatly improves the storage and transportation efficiency due to the high energy density but at the same time brings new safety hazards. In this study, the liquid hydrogen leakage in [...] Read more.
Liquid hydrogen storage is an important way of hydrogen storage and transportation, which greatly improves the storage and transportation efficiency due to the high energy density but at the same time brings new safety hazards. In this study, the liquid hydrogen leakage in the storage area of a hydrogen production station is numerically simulated. The effects of ambient wind direction, wind speed, leakage mass flow rate, and the mass fraction of gas phase at the leakage port on the diffusion behavior of the liquid hydrogen leakage were investigated. The results show that the ambient wind direction directly determines the direction of liquid hydrogen leakage diffusion. The wind speed significantly affects the diffusion distance. When the wind speed is 6 m/s, the diffusion distance of the flammable hydrogen cloud reaches 40.08 m, which is 2.63 times that under windless conditions. The liquid hydrogen leakage mass flow rate and the mass fraction of the gas phase have a greater effect on the volume of the flammable hydrogen cloud. As the leakage mass flow rate increased from 5.15 kg/s to 10 kg/s, the flammable hydrogen cloud volume increased from 5734.31 m3 to 10,305.5 m3. The installation of a barrier wall in front of the leakage port can limit the horizontal diffusion of the flammable hydrogen cloud, elevate the diffusion height, and effectively reduce the volume of the flammable hydrogen cloud. This study can provide theoretical support for the construction and operation of hydrogen production stations. Full article
(This article belongs to the Special Issue Hydrogen Safety: Challenges and Opportunities)
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<p>Modeling (<b>a</b>) and meshing (<b>b</b>) for validation.</p>
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<p>Hydrogen concentration distribution at 20.94 s of leakage in experiment [<a href="#B2-fire-07-00217" class="html-bibr">2</a>] (<b>a</b>) and simulation (<b>b</b>).</p>
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<p>Experimental [<a href="#B2-fire-07-00217" class="html-bibr">2</a>] and simulated values of hydrogen concentration at monitoring point.</p>
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<p>Hydrogen production station layout.</p>
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<p>Geometric model (<b>a</b>) and meshing (<b>b</b>) of hydrogen production station.</p>
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<p>Volume of flammable hydrogen cloud with different numbers of meshes.</p>
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<p>Liquid hydrogen distribution at different moments.</p>
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<p>Hydrogen concentration (<b>a</b>) and temperature distribution (<b>b</b>) at different moments.</p>
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<p>Flammable hydrogen clouds at different moments during the leakage process.</p>
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<p>Variation in flammable hydrogen clouds with time for different wind speeds.</p>
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<p>Volume (<b>a</b>) and diffusion distance (<b>b</b>) of flammable hydrogen clouds under different wind speed conditions.</p>
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<p>Liquid hydrogen flow with different leakage mass flow rates.</p>
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<p>Variation in flammable hydrogen clouds with time under different leakage mass flow rate conditions.</p>
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<p>Diffusion distance (<b>a</b>) and volume (<b>b</b>) of flammable hydrogen clouds at different leakage mass flow rates.</p>
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<p>Liquid hydrogen flow at different leakage gas phase mass fractions.</p>
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<p>Hydrogen concentration distribution at different leakage gas phase mass fractions.</p>
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<p>Diffusion distances (<b>a</b>) and volumes (<b>b</b>) of flammable hydrogen clouds for different leakage gas phase mass fractions.</p>
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<p>Barrier walls at different locations.</p>
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<p>Hydrogen concentration distribution with time at different barrier wall locations.</p>
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<p>Volume of flammable hydrogen cloud at different barrier wall locations.</p>
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<p>Hydrogen concentration distribution with time for different barrier wall heights.</p>
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<p>Volume of flammable hydrogen cloud at different barrier wall heights.</p>
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17 pages, 5685 KiB  
Article
Harnessing Enhanced Flame Retardancy in Rigid Polyurethane Composite Foams through Hemp Seed Oil-Derived Natural Fillers
by Mansi Ahir, Chandan Bodhak and Ram K. Gupta
Polymers 2024, 16(11), 1584; https://doi.org/10.3390/polym16111584 - 3 Jun 2024
Cited by 2 | Viewed by 604
Abstract
Over the past few decades, polymer composites have received significant interest and become protagonists due to their enhanced properties and wide range of applications. Herein, we examined the impact of filler and flame retardants in hemp seed oil-based rigid polyurethane foam (RPUF) composites’ [...] Read more.
Over the past few decades, polymer composites have received significant interest and become protagonists due to their enhanced properties and wide range of applications. Herein, we examined the impact of filler and flame retardants in hemp seed oil-based rigid polyurethane foam (RPUF) composites’ performance. Firstly, the hemp seed oil (HSO) was converted to a corresponding epoxy analog, followed by a ring-opening reaction to synthesize hemp bio-polyols. The hemp polyol was then reacted with diisocyanate in the presence of commercial polyols and other foaming components to produce RPUF in a single step. In addition, different fillers like microcrystalline cellulose, alkaline lignin, titanium dioxide, and melamine (as a flame retardant) were used in different wt.% ratios to fabricate composite foam. The mechanical characteristics, thermal degradation behavior, cellular morphology, apparent density, flammability, and closed-cell contents of the generated composite foams were examined. An initial screening of different fillers revealed that microcrystalline cellulose significantly improves the mechanical strength up to 318 kPa. The effect of melamine as a flame retardant in composite foam was also examined, which shows the highest compression strength of 447 kPa. Significantly better anti-flaming qualities than those of neat foam based on HSO have been reflected using 22.15 wt.% of melamine, with the lowest burning time of 4.1 s and weight loss of 1.88 wt.%. All the composite foams showed about 90% closed-cell content. The present work illustrates the assembly of a filler-based polyurethane foam composite with anti-flaming properties from bio-based feedstocks with high-performance applications. Full article
(This article belongs to the Special Issue Flame-Retardant Polymer Composites II)
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<p>A schematic diagram for the synthesis of HSO-based RPUF composite.</p>
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<p>(<b>a</b>) FT-IR spectra and (<b>b</b>) GPC chromatograms of HSO, EHSO, and HSPO.</p>
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<p>The apparent density of (<b>a</b>) filler-based and (<b>b</b>) filler-encapsulated flame retardant-based RPUF composite.</p>
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<p>Closed-cell content of (<b>a</b>) filler-based and (<b>b</b>) filler-encapsulated flame retardant-based RPUF composite.</p>
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<p>Typical stress-strain curves of the HSO-RPUF composites containing (<b>a</b>) MC, (<b>b</b>) TiO<sub>2</sub>, (<b>c</b>) AL, and (<b>d</b>) melamine (MC-encapsulated) under compression, showing linear elastic and plateau regions.</p>
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<p>TGA thermograms of HSO-RPUF composites containing (<b>a</b>) AL, (<b>b</b>) TiO<sub>2</sub>, (<b>c</b>) MC, and (<b>d</b>) melamine (MC-encapsulated).</p>
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<p>SEM images of HSO-based RPUF composite with (<b>a</b>) microcrystalline cellulose filler and (<b>b</b>) MC-encapsulated melamine flame retardant.</p>
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<p>SEM images of HSO-based RPUF composite with (<b>a</b>) microcrystalline cellulose filler and (<b>b</b>) MC-encapsulated melamine flame retardant.</p>
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<p>(<b>a</b>) Burning time and (<b>b</b>) weight loss (%) content of the HSO-RPUFs with varying amounts of melamine.</p>
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<p>Optical images of horizontal burning tests of HSO-RPUF composites containing melamine flame retardant.</p>
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20 pages, 18539 KiB  
Review
Nanostructured Flame-Retardant Layer-by-Layer Architectures for Cotton Fabrics: The Current State of the Art and Perspectives
by Giulio Malucelli
Nanomaterials 2024, 14(10), 858; https://doi.org/10.3390/nano14100858 - 15 May 2024
Viewed by 1327
Abstract
Nowadays, nanotechnology represents a well-established approach, suitable for designing, producing, and applying materials to a broad range of advanced sectors. In this context, the use of well-suited “nano” approaches accounted for a big step forward in conferring optimized flame-retardant features to such a [...] Read more.
Nowadays, nanotechnology represents a well-established approach, suitable for designing, producing, and applying materials to a broad range of advanced sectors. In this context, the use of well-suited “nano” approaches accounted for a big step forward in conferring optimized flame-retardant features to such a cellulosic textile material as cotton, considering its high ease of flammability, yearly production, and extended use. Being a surface-localized phenomenon, the flammability of cotton can be quite simply and effectively controlled by tailoring its surface through the deposition of nano-objects, capable of slowing down the heat and mass transfer from and to the textile surroundings, which accounts for flame fueling and possibly interacting with the propagating radicals in the gas phase. In this context, the layer-by-layer (LbL) approach has definitively demonstrated its reliability and effectiveness in providing cotton with enhanced flame-retardant features, through the formation of fully inorganic or hybrid organic/inorganic nanostructured assemblies on the fabric surface. Therefore, the present work aims to summarize the current state of the art related to the use of nanostructured LbL architectures for cotton flame retardancy, offering an overview of the latest research outcomes that often highlight the multifunctional character of the deposited assemblies and discussing the current limitations and some perspectives. Full article
(This article belongs to the Special Issue Nanomaterials and Textiles)
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Graphical abstract

Graphical abstract
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<p>A scheme of the flaming combustion cycle for a textile material.</p>
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<p>The number of publications (from 2000 to 2024) in peer-reviewed journals, dealing with “Layer-by-Layer” (data collected from the Web of Science<sup>TM</sup> database, <a href="http://www.webofscience.com" target="_blank">www.webofscience.com</a>, accessed on 14 April 2024).</p>
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<p>A scheme of the LbL dipping process: the substrate is sequentially immersed into baths containing dilute aqueous solutions/suspensions of the “objects” (particles, rods/tubes, sheets/lamellae, polyelectrolytes, biomacromolecules) to deposit. Reprinted with permission from [<a href="#B27-nanomaterials-14-00858" class="html-bibr">27</a>]. Copyright 2018, Elsevier.</p>
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<p>A closer look at the dipping-assisted LbL process employing polyelectrolyte baths: the use of a primer layer. Reprinted from [<a href="#B49-nanomaterials-14-00858" class="html-bibr">49</a>] under BB-CY License.</p>
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<p>TEM cross-sectional images of assemblies (30 bi-layers) made with Laponite and branched poly(ethyleneimine) at pH 10 (<b>a</b>) and pH 8 (<b>b</b>) and with branched poly(ethyleneimine) and Laponite at pH 6 (<b>c</b>); all the assemblies were grown on a polystyrene (PS) film. Several light-colored round or elliptical areas appeared in the lateral view of the cross-section (<b>c</b>) (highlighted by red arrows), which correspond to the size of Laponite platelets tilted on their sides. Reprinted with permission from [<a href="#B60-nanomaterials-14-00858" class="html-bibr">60</a>]. Copyright 2009, American Chemical Society.</p>
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<p>(<b>A</b>) Heat release rate (HRR) and (<b>B</b>) total heat release (THR) curves for untreated cotton (COT) and the LbL-treated fabrics through dipping, vertical, and horizontal spray-assisted processes. Reprinted with permission from [<a href="#B63-nanomaterials-14-00858" class="html-bibr">63</a>]. Copyright 2013, Elsevier.</p>
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<p>The results from vertical flame spread tests: uncoated fabric recorded at 4 s after ignition (<b>a</b>); uncoated fabric at the end of the test (<b>b</b>); cotton fabric coated with an intumescent tri-layer made of branched poly(ethylenimine), ammonium polyphosphate, and fluorinated-decyl polyhedral oligomeric silsesquioxane recorded at 4 s after ignition (<b>c</b>); and cotton fabric coated with an intumescent tri-layer made of branched poly(ethylenimine), ammonium polyphosphate, and fluorinated-decyl polyhedral oligomeric silsesquioxane at the end of the test (<b>d</b>). Reprinted with permission from [<a href="#B69-nanomaterials-14-00858" class="html-bibr">69</a>]. Copyright 2015, American Chemical Society.</p>
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<p>Heat release rate (HRR) vs. time curves for untreated cotton (COT) and for the fabric treated with 5 bi-layers of phytic acid and chitosan embedding biochar at 7.5 wt.%, before (PA/CH/BC 7.5%-COT) and after 10 laundry cycles (PA/CH/BC 7.5%-COT washed). Reprinted with permission from [<a href="#B75-nanomaterials-14-00858" class="html-bibr">75</a>]. Copyright 2022, Elsevier.</p>
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<p>The results from pyrolysis–combustion flow calorimetry tests: heat release rate (HRR) vs. temperature curves for untreated cotton, for the fabric treated with 5 bi-layers of chitosan/ammonium polyphosphate (CS/APP cotton) and for the fabric treated with 5 bi-layers of chitosan/ammonium polyphosphate and silica/titania hexamethyldisilamine sol (CS/APP@TiO<sub>2</sub>-SiO<sub>2</sub> HMDS cotton) as the top layer. Reprinted from [<a href="#B78-nanomaterials-14-00858" class="html-bibr">78</a>] under CC-BY License.</p>
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<p>Heat release rate (HRR, (<b>a</b>)) and total heat release (THR, (<b>b</b>)) vs. time curves for untreated (pure cotton) and LbL-treated cotton (Cotton-XXBL, where XX stands for the number of deposited bi-layers). Reprinted with permission from [<a href="#B80-nanomaterials-14-00858" class="html-bibr">80</a>]. Copyright 2022, Elsevier.</p>
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<p>Electrical conductivity (<b>a</b>) and electromagnetic interference shielding efficiency (EMI SE, (<b>b</b>)) for untreated (pure cotton) and LbL-treated cotton (Cotton-XXBL, where XX stands for the number of deposited bi-layers). Reprinted with permission from [<a href="#B80-nanomaterials-14-00858" class="html-bibr">80</a>]. Copyright 2022, Elsevier.</p>
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<p>Sensing performances of the LbL-coated fabrics. Sensitivity fitting diagrams of the assemblies made of 1 or 2 bi-layers (<b>a</b>). I–V curves (<b>b</b>) and stability tests of 2 bi-layered assemblies (<b>c</b>). Output currents of the 2 bi-layered assemblies under different external pressures (<b>d</b>). The transient response time (<b>e</b>) and relaxation time (<b>f</b>) of the 2 bi-layered assemblies. Durability tests of the 2 bi-layered assemblies during 10,000 s (<b>g</b>). Reprinted with permission from [<a href="#B82-nanomaterials-14-00858" class="html-bibr">82</a>]. Copyright 2023, Elsevier.</p>
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<p>A scheme of the construction process for the design of LbL multifunctional coatings on cotton. Legend: CS = chitosan; PA = phytic acid; PDMS = poly(dimethyl siloxane). Reprinted with permission from [<a href="#B90-nanomaterials-14-00858" class="html-bibr">90</a>]. Copyright 2024, Elsevier.</p>
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21 pages, 9557 KiB  
Article
Cooling and Multiphase Analysis of Heated Environmentally Friendly R152A (C2H4F2) Fluid Coming from the Production Process According to Nist Indicators
by Mehmet Akif Kartal, Gürcan Atakök and Sezgin Ersoy
Appl. Sci. 2024, 14(10), 4143; https://doi.org/10.3390/app14104143 - 14 May 2024
Cited by 1 | Viewed by 769
Abstract
Cooling processes are responsible for a significant portion (20%) of global energy consumption and raise environmental concerns such as ozone depletion, the greenhouse effect, and high energy use. This study investigates the potential of R152a, a refrigerant with low global warming potential (GWP), [...] Read more.
Cooling processes are responsible for a significant portion (20%) of global energy consumption and raise environmental concerns such as ozone depletion, the greenhouse effect, and high energy use. This study investigates the potential of R152a, a refrigerant with low global warming potential (GWP), as a more sustainable alternative. The performance, safety, and operational efficiency of R152a were evaluated under various conditions. Although R152a offers high performance and low GWP, its flammability necessitates caution, especially in certain mixtures. A 12-pass tube-type heat exchanger model was simulated using computational fluid dynamics (CFD) to analyze the fluid behavior within the exchanger. The pressure, density, dynamic pressure, Prandtl number, total pressure, and temperature distributions for both R152a and H2O (water) were visualized using contour plots. The simulations comprehensively examined the fluid behavior inside and outside the heat exchanger. The results revealed the influence of the temperature on the internal dynamic pressure and density of R152a. Compared with R134a, R152a demonstrated superior performance but a lower coefficient of performance (COP) than R32. Studies also suggest that R152a exhibits lower irreversibility in Organic Rankine Cycle (ORC) systems than R245fa. These findings suggest that R152a holds promise for future refrigeration systems, as supported by existing research on its performance and compatibility. One study focused on optimizing the heat exchanger performance by maximizing the heat capacity and minimizing the pressure drop. This study employed a parallel-flow heat exchanger with R152a as the coolant for the hot process water. The temperature changes, pressure drops, and resulting energy efficiency and thermal performance of both fluids were analyzed. The results highlight the distinct energy efficiencies and thermal performance of the employed fluids. Full article
(This article belongs to the Special Issue Advances and Applications of CFD (Computational Fluid Dynamics))
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<p>Flow track of designed model.</p>
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<p>Baffle plate and side view of model.</p>
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<p>Mesh grid of model.</p>
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<p>Dimensions of model.</p>
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<p>Domain names of the model.</p>
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<p>Absolute pressure of internal fluid volume.</p>
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<p>Absolute pressure of external fluid volume.</p>
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<p>Comparison of compressibility factor and pressure [<a href="#B23-applsci-14-04143" class="html-bibr">23</a>].</p>
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<p>Compressibility factor of R152a.</p>
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<p>Contour density of internal fluid volume.</p>
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<p>Contour density of external fluid volume at Z = p00.0 [cm].</p>
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<p>(<b>a</b>) Contour density of external fluid volume at Z = p05.0 [cm], (<b>b</b>) Z = p10.0 [cm], (<b>c</b>) Z = p15.0 [cm], and (<b>d</b>) Z = p20.0 [cm].</p>
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<p>Contour dynamic pressure of R152a volume at Z = p00.0 [cm].</p>
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<p>Contour dynamic pressure of H<sub>2</sub>O volume at Z = p00.0 [cm].</p>
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<p>Contour of Prandtl number of R152a volume at Z = p00.0 [cm].</p>
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<p>Contour of Prandtl number of H<sub>2</sub>O volume at Z = p00.0 [cm].</p>
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<p>Contour of total pressure of R152a volume at Z = p00.0 [cm].</p>
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<p>Contour of total pressure of H<sub>2</sub>O volume at Z = p00.0 [cm].</p>
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<p>(<b>a</b>) Contour of velocity of R152a volume at Z = p00.0 [cm]; (<b>b</b>) contour of streamline velocity of R152a volume at Z = p00.0 [cm].</p>
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<p>(<b>a</b>) Contour of velocity of H<sub>2</sub>O volume at Z = p00.0 [cm]; (<b>b</b>) contour of streamline velocity of H<sub>2</sub>O volume at Z = p00.0 [cm].</p>
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<p>Contour of temperature of H<sub>2</sub>O and R152a in all domains at Z = p00.0 [cm].</p>
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<p>Contour of temperature of H<sub>2</sub>O external fluid volume at Z = p00.0 [cm].</p>
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<p>Contour of temperature of R152a internal fluid volume at Z = p00.0 [cm].</p>
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<p>Flowchart of methodology.</p>
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27 pages, 7953 KiB  
Article
Properties and Performance of Epoxy Resin/Boron Acid Composites
by Anna Rudawska, Mariaenrica Frigione, Antonella Sarcinella, Valentina Brunella, Ludovica Di Lorenzo and Ewa Olewnik-Kruszkowska
Materials 2024, 17(9), 2092; https://doi.org/10.3390/ma17092092 - 29 Apr 2024
Cited by 2 | Viewed by 947
Abstract
This research study focused on the effect of adding boric acid to epoxy resin in order to obtain a composite material with improved properties and performance. To this end, a fine powder of boric acid (H3BO3) was introduced into [...] Read more.
This research study focused on the effect of adding boric acid to epoxy resin in order to obtain a composite material with improved properties and performance. To this end, a fine powder of boric acid (H3BO3) was introduced into epoxy resin in different amounts, i.e., 0.5 g, 1.0 g, and 1.5 g. As the matrix of the epoxy composites, styrene-modified epoxy resin based on bisphenol A (BPA) (Epidian 53) was used. It was cross-linked with two types of curing agents, i.e., an amine (ET) and a polyamide (PAC). The mechanical properties of the obtained epoxy composites (in terms of compressive strength, compressive modulus, and compressive strain) were determined at room temperature in order to assess the effect of the addition of boron acid and of the type of curing agent employed to cure the epoxy on these characteristics. Calorimetric measurements were made to highlight any changes in the glass transition temperature (Tg) as a result of the addition of boric acid to epoxy resin. Finally, flammability tests were performed on both Epidian 53/PAC and Epidian 53/ET epoxy composites to analyze their fire behavior and consequently establish the effectiveness of the selected additive as a flame retardant. Full article
(This article belongs to the Special Issue Mechanical Properties and Application of Adhesive Materials)
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<p>Schemes of (<b>a</b>) bisphenolic epoxy resin [<a href="#B56-materials-17-02092" class="html-bibr">56</a>]; (<b>b</b>) polyaminoamide curing agent [<a href="#B56-materials-17-02092" class="html-bibr">56</a>]; (<b>c</b>) ortho form of boric acid [<a href="#B48-materials-17-02092" class="html-bibr">48</a>].</p>
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<p>Samples of boron acid/epoxy resin composites: (<b>a</b>) type 1; (<b>b</b>) type 2.</p>
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<p>Compressive strengths calculated on the boron acid/epoxy resin composites.</p>
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<p>Correlation coefficient r (X, Y) of (<b>a</b>) E53/ET boron acid/epoxy resin composites; (<b>b</b>) E53/PAC boron acid/epoxy resin composites (results are reported in <a href="#materials-17-02092-t003" class="html-table">Table 3</a>).</p>
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<p>Compressive modulus measured on the boron acid/epoxy resin composites.</p>
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<p>Correlation coefficient r (X, Y) of (<b>a</b>) E53/ET boron acid/epoxy resin composites; (<b>b</b>) E53/PAC boron acid/epoxy resin composites (results are reported in <a href="#materials-17-02092-t004" class="html-table">Table 4</a>).</p>
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<p>Compressive strain calculated on the boron acid/epoxy resin composites.</p>
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<p>Correlation coefficient r (X, Y) of (<b>a</b>) E53/ET boron acid/epoxy resin composites; (<b>b</b>) E53/PAC boron acid/epoxy resin composites (<a href="#materials-17-02092-t005" class="html-table">Table 5</a>).</p>
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<p>Linear burning rate depending on the content of the flame retardant (boron acid).</p>
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<p>Views of E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.0 sample of epoxy resin composites: (<b>a</b>) immediately after removing the flame source, (<b>b</b>) after combustion.</p>
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<p>Maximum temperature in the burning area of E53/ET epoxy resin composite samples depending on burning time.</p>
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<p>Thermal images of E53/ET epoxy resin composite samples recorded immediately after subtraction of the ignition source (time 0): (<b>a</b>) E53/ET; (<b>b</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Thermal images of E53/ET epoxy resin composite samples recorded immediately after subtraction of the ignition source (time 0): (<b>a</b>) E53/ET; (<b>b</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Thermal images of E53/ET epoxy resin composite samples recorded 60 s after ignition source subtraction: (<b>a</b>) E53/ET; (<b>b</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Thermal images of E53/ET epoxy resin composite samples recorded 60 s after ignition source subtraction: (<b>a</b>) E53/ET; (<b>b</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/ET/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Maximum temperature in the burning area of E53/PAC epoxy resin composite samples depending on burning time.</p>
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<p>Thermal images of E53/PAC epoxy resin composite samples recorded immediately after the subtraction of the ignition source (time 0): (<b>a</b>) E53/PAC; (<b>b</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Thermal images of E53/PAC epoxy resin composite samples recorded immediately after the subtraction of the ignition source (time 0): (<b>a</b>) E53/PAC; (<b>b</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Thermal images of E53/PAC epoxy resin composite samples recorded 40 s after ignition source subtraction: (<b>a</b>) E53/PAC; (<b>b</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Thermal images of E53/PAC epoxy resin composite samples recorded 40 s after ignition source subtraction: (<b>a</b>) E53/PAC; (<b>b</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/0.5; (<b>c</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.0; (<b>d</b>) E53/PAC/H<sub>3</sub>BO<sub>3</sub>/1.5.</p>
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<p>Average compressive strength calculated on boron acid/epoxy composites containing solvent-free resin (i.e., Epidian 5) and solvent-modified resin (i.e., Epidian 53), cured using amine or polyamide curing agents.</p>
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<p>Temperature recorded along the axis of the E53/ET epoxy resin composite samples: (<b>a</b>) immediately after removing the ignition source; (<b>b</b>) 60 s after removing the ignition source.</p>
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<p>Temperature recorded along the axis of the E53/PAC epoxy resin composite sample: (<b>a</b>) immediately after removing the ignition source; (<b>b</b>) 40 s after removing the ignition source.</p>
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13 pages, 2673 KiB  
Article
Fire Behavior of Wood–Glass and Jute–Glass Hybrid Laminates Manufactured by Vacuum Infusion
by Letícia Zimermann Pires, Ohayna Lisboa Santos, Agnė Kairytė, Jurga Šeputytė-Jucikė, Sylwia Makowska, Daniele Battegazzore, Alberto Frache, Rafael de Avila Delucis, Pedro Henrique Gonzalez de Cademartori and Andrey Pereira Acosta
Appl. Sci. 2024, 14(8), 3450; https://doi.org/10.3390/app14083450 - 19 Apr 2024
Cited by 1 | Viewed by 759
Abstract
This study explores the fire behavior of wood–glass and jute–glass hybrid laminates, with a focus on the influence of jute and wood veneers as new materials for composite production. Five-layer hybrid laminates were manufactured using the vacuum infusion process (VIP). Combustion and carbonization [...] Read more.
This study explores the fire behavior of wood–glass and jute–glass hybrid laminates, with a focus on the influence of jute and wood veneers as new materials for composite production. Five-layer hybrid laminates were manufactured using the vacuum infusion process (VIP). Combustion and carbonization performances were assessed using a cone calorimeter based on the ISO 5660 method. This study evaluates flammability through key parameters including ignition time, heat release rate, and smoke production. The results indicated that the ignition time was significantly longer (ca. 64 s) for the glass–jute laminate (GJGJG), compared to the wood–glass laminate (WGWGW) (ca. 53 s). The heat release rate of laminates containing organic components was higher than the sample composed only of glass mat (G5) but their rates were all lower than the polyester reference resin. WGWGW, compared to the GJGJG sample, was able to produce a good-quality protective shield and, therefore, postpone the occurrence of the heat release peak. In this way, the fire growth rate index (FIGRA) best performance was accomplished by the WGWGW sample (2.7 ± 0.3 kW/m2 × s), which was even better than that of the G5 sample. The total-smoke-released value was highest for polyester, 7361 ± 839 m2/m2, followed by WGWGW, 2873 ± 188 m2/m2, and J5, 2484 ± 216 m2/m2. Among the hybrid laminates, the best performance was obtained by GJGJG, 1860 ± 49 m2/m2, but compared to the G5 laminates, it was only ~36% higher. The specific extinction area (SEA) is a smoke parameter related to the mass of the samples; the best result was obtained by WGWGW with 697 ± 31 m2/kg. Finally, the neat polyester and all laminates achieved UL 94HB classification, with firing rates below 40 mm/min. Full article
(This article belongs to the Special Issue New Challenges in Civil Structure for Fire Response Volume II)
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<p>Representation of the VIP for manufacturing the laminates and their different stacking sequences.</p>
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<p>Heat release rate as a function of time for each group analyzed (<b>A</b>) and the average values of the heat release rate and confidence interval of 95% (<b>B</b>). Different letters above the errors in each group represent a statistical difference.</p>
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<p>Appearance of the samples before and after the cone calorimeter tests.</p>
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<p>Total heat release (THR) as a function of time for each group analyzed (<b>A</b>) and average maximum values for THR (<b>B</b>). Different letters above the errors in each group represent a statistical difference.</p>
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<p>Total smoke release as a function of time for each group analyzed (<b>A</b>) and average values for total smoke release at the end of the test (<b>B</b>). Different letters above the errors in each group represent a statistical difference.</p>
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<p>Percentage of reduction in transmittance of the laser in the exhaust air flow as a function of time for each group analyzed.</p>
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<p>Carbon monoxide and carbon dioxide as functions of time for each group analyzed (<b>A</b>,<b>C</b>) and average values for carbon monoxide and carbon dioxide (<b>B</b>,<b>D</b>). Different letters above the errors in each group indicate a statistical difference.</p>
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<p>Appearance of the samples during the horizontal firing test in accordance with UL 94.</p>
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18 pages, 5698 KiB  
Article
Effect of Amino Silicone Oil-Phosphorylation Hybrid Modification on the Properties of Microcellulose Fibers
by Quan Yuan, Guimei Zhang, Chunxuan Li, Shiwei Xu and Liping He
Polymers 2024, 16(8), 1123; https://doi.org/10.3390/polym16081123 - 17 Apr 2024
Viewed by 1018
Abstract
Microcellulose materials are increasingly considered multifunctional candidates for emerging energy applications. Microcellulose fibers (MCF) are a kind of bio-based reinforcement in composites, and their hydrophilic character hinders their wide application in industry. Thus, in the present work, MCF was hybrid-modified by amino silicone [...] Read more.
Microcellulose materials are increasingly considered multifunctional candidates for emerging energy applications. Microcellulose fibers (MCF) are a kind of bio-based reinforcement in composites, and their hydrophilic character hinders their wide application in industry. Thus, in the present work, MCF was hybrid-modified by amino silicone oil-phosphorylated to fabricate hydrophobic, thermal stability, and flame-retardant microcellulose fibers for potential application in vehicle engineering. The results showed that the amino silicone oil-phosphorylated (ASOP) hybrid modification could transform the surface property of microcellulose from hydrophilic to hydrophobic and improve the compatibility between MCF and resin matrix. Meanwhile, the ASOP treatment led to the formation of an amino silicone oil film layer on the surface of the microcellulose, which improved the thermal stability of the MCF. Furthermore, the ASOP hybrid modification microcellulose fibers paper (100% microcellulose fibers paper) was transformed from flammable to flame-retardant and showed self-extinguishing behavior after burning under flame for 2 s. The flame-retardant mechanism was attributed to the formation of the char layer in the condensed phase and the production of non-combustible gases in the gaseous phase. Full article
(This article belongs to the Section Polymer Fibers)
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<p>ASOP-MCF modification process.</p>
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<p>FTIR spectra of unmodified and modified microcellulose fibers.</p>
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<p>XRD pattern of microcellulose fibers before and after modification.</p>
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<p>XPS spectra of microcellulose fibers: (<b>a</b>) full spectrum; MCF of (<b>b</b>) O1s, (<b>e</b>) C1s; (<b>d</b>) Si2p; ASOP-MCF of (<b>c</b>) O1s, (<b>f</b>) C1s.</p>
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<p>SEM image of microcellulose fibers: (<b>a</b>) MCF; (<b>b</b>) PMCF; (<b>c</b>) ASO-MCF; (<b>d</b>) ASOP-MCF; (<b>e</b>–<b>h</b>) are partially enlarged views.</p>
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<p>EDX of microcellulose fibers: (<b>a</b>) MCF; (<b>b</b>) ASOP-MCF.</p>
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<p>TGA (<b>a</b>,<b>c</b>) and DTG (<b>b</b>,<b>d</b>) curves of unmodified and modified microcellulose fibers under N<sub>2</sub> and air atmosphere.</p>
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<p>Burning of (<b>a</b>) MCF paper and (<b>b</b>) ASOP-MCF paper.</p>
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<p>(<b>a</b>) Microcellulose fibers contact angle, (<b>b</b>) contact angle versus time.</p>
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<p>Comparison of thermal stability of ASOP-MCF in this work with other phosphorylated cellulose in the literature (Blilid et al. [<a href="#B15-polymers-16-01123" class="html-bibr">15</a>], Blilid et al. [<a href="#B16-polymers-16-01123" class="html-bibr">16</a>], Khakalo et al. [<a href="#B20-polymers-16-01123" class="html-bibr">20</a>],Wang et al. [<a href="#B26-polymers-16-01123" class="html-bibr">26</a>], Benhamous et al. [<a href="#B33-polymers-16-01123" class="html-bibr">33</a>], Ghanadpour et al. [<a href="#B43-polymers-16-01123" class="html-bibr">43</a>], Costes et al. [<a href="#B44-polymers-16-01123" class="html-bibr">44</a>], Espinosa et al. [<a href="#B45-polymers-16-01123" class="html-bibr">45</a>], Kassab et al. [<a href="#B46-polymers-16-01123" class="html-bibr">46</a>], El-Shafei et al. [<a href="#B47-polymers-16-01123" class="html-bibr">47</a>], Sirvio et al. [<a href="#B48-polymers-16-01123" class="html-bibr">48</a>]).</p>
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<p>The synergistic effect of ASOP hybrid modification: (<b>a</b>) ASOP hybrid modification mechanism; (<b>b</b>) flame-retardant mechanism diagram of ASOP-MCF during burning.</p>
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21 pages, 9940 KiB  
Article
Phosphorus-Based Flame-Retardant Acrylonitrile Butadiene Styrene Copolymer with Enhanced Mechanical Properties by Combining Ultrahigh Molecular Weight Silicone Rubber and Ethylene Methyl Acrylate Copolymer
by Farnaz Ghonjizade-Samani, Laia Haurie, Ramón Malet, Marc Pérez and Vera Realinho
Polymers 2024, 16(7), 923; https://doi.org/10.3390/polym16070923 - 27 Mar 2024
Cited by 1 | Viewed by 1226
Abstract
The present work proposes to investigate the effect of an ultrahigh molecular weight silicone rubber (UHMW-SR) and two ethylene methyl acrylate copolymers (EMA) with different methyl acrylate (MA) content on the mechanical and fire performance of a fireproof acrylonitrile butadiene styrene copolymer (ABS) [...] Read more.
The present work proposes to investigate the effect of an ultrahigh molecular weight silicone rubber (UHMW-SR) and two ethylene methyl acrylate copolymers (EMA) with different methyl acrylate (MA) content on the mechanical and fire performance of a fireproof acrylonitrile butadiene styrene copolymer (ABS) composite, with an optimum amount of ammonium polyphosphate (APP) and aluminum diethyl phosphinate (AlPi). ABS formulations with a global flame retardant weight content of 20 wt.% (ABS P) were melt-compounded, with and without EMA and UHMW-SR, in a Brabender mixer. During this batch process, ABS P formulations with UHMW-SR and/or EMA registered lower torque values than those of ABS P. By means of scanning electron microscopy (SEM), it was possible to observe that all ABS composites exhibited a homogenous structure without phase separation or particle agglomeration. Slightly improved interfacial interaction between the well-dispersed flame-retardant particles in the presence of EMA and/or UHMW-SR was also noticed. Furthermore, synergies in mechanical properties by adding both EMA and UHMW-SR into ABS P were ascertained. An enhancement of molecular mobility that contributed to the softening of ABS P was observed under dynamic mechanical thermal analysis (DMTA). An improvement of its flexibility, ductility and toughness were also registered under three-point-bending trials, and even more remarkable synergies were noticed in Charpy notched impact strength. Particularly, a 212% increase was achieved when 5 wt.% of EMA with 29 wt.% of MA and 2 wt.% of UHMW-SR in ABS P (ABS E29 S P) were added. Thermogravimetric analysis (TGA) showed that the presence of EMA copolymers in ABS P formulations did not interfere with its thermal decomposition, whereas UHMW-SR presence decreased its thermal stability at the beginning of the decomposition. Although the addition of EMA or UHMW-SR, as well as the combination of both in ABS P increased the pHRR in cone calorimetry, UL 94 V-0 classification was maintained for all flame-retarded ABS composites. In addition, through SEM analysis of cone calorimetry sample residue, a more cohesive surface char layer, with Si-O-C network formation confirmed by Fourier transform infrared (FTIR), was shown in ABS P formulations with UHMW-SR. Full article
(This article belongs to the Special Issue Synthesis and Processing of Functional Polymer Materials)
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<p>Effect of UHMW-SR and EMA on ABS P torque vs. time of melt-compounding.</p>
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<p>SEM micrographs of ABS P, ABS S P, ABS E24 P, ABS E29 P, ABS E24 S P and ABS E29 S P, at 500× and 2500×, with a scale bar of 50 and 10 µm, respectively.</p>
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<p>SEM micrographs of ABS P, ABS S P, ABS E24 P, ABS E29 P, ABS E24 S P and ABS E29 S P, at 500× and 2500×, with a scale bar of 50 and 10 µm, respectively.</p>
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<p>Storage modulus (E′) and tan δ vs. temperature curves of ABS and ABS formulations.</p>
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<p>Cole–Cole plots of different samples.</p>
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<p>Stress–strain curves of (<b>a</b>) ABS and ABS with EMA and/or UHMW-SR, and (<b>b</b>) ABS P and ABS P with EMA and/or UHMW-SR, obtained from flexural test.</p>
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<p>TG curves of E24, E29 and UHMW-SR obtained at 10 °C/min under N<sub>2</sub> atmosphere.</p>
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<p>TG curves of ABS with E24 and E29 with or without UHMW-SR.</p>
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<p>(<b>a</b>) TG and (<b>b</b>) dTG of curves of flame-retardant ABS formulations.</p>
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<p>Heat release rate of ABS with either EMA (E24 or E29) copolymers or UHMW-SR and with both of them, (E24/UHMW-SR) or (E29/UHMW-SR).</p>
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<p>Heat release rate of ABS P formulations.</p>
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<p>Digital photographs of ABS, ABS S, ABS P, ABS S P, ABS E24 P, ABS E24 S P, ABS E29 P and ABS E29 S P after CC, respectively.</p>
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<p>SEM micrographs of the upper (from left), lower and lateral surfaces of the ABS P, ABS S P, ABS E24 P, ABS E24 S P, ABS E29 P and ABS E29 S P after the cone calorimeter tests (at 1000× with a scale bar of 10 µm).</p>
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<p>SEM micrographs of the upper (from left), lower and lateral surfaces of the ABS P, ABS S P, ABS E24 P, ABS E24 S P, ABS E29 P and ABS E29 S P after the cone calorimeter tests (at 1000× with a scale bar of 10 µm).</p>
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<p>FTIR spectra of flame-retardant ABS residues after cone calorimeter test.</p>
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