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Search Results (478)

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13 pages, 2875 KiB  
Article
A Comprehensive Life Cycle Carbon Footprint Assessment Model for Electric Power Material Warehouses
by Yongjun Luo, Xinyi Tang, Lei Geng, Xiang Yao, Feihong Li, Xudong Li and Qingrui Wang
Energies 2024, 17(24), 6352; https://doi.org/10.3390/en17246352 - 17 Dec 2024
Viewed by 347
Abstract
Electric power material warehouses are critical to optimizing power grid supply chains and reducing carbon emissions, aiding the power sector’s decarbonization and climate goals. Nevertheless, to our knowledge, there are no comprehensive assessments of the life cycle carbon emissions associated with storage warehouses, [...] Read more.
Electric power material warehouses are critical to optimizing power grid supply chains and reducing carbon emissions, aiding the power sector’s decarbonization and climate goals. Nevertheless, to our knowledge, there are no comprehensive assessments of the life cycle carbon emissions associated with storage warehouses, so the emission reduction potential of the ever-increasing number of automated technologies is still unknown. This study presents an extensive life cycle carbon footprint assessment model tailored for electric power material warehouses, and it encompasses both traditional and automated frameworks. Utilizing a process-based life cycle assessment (LCA) methodology, carbon emissions across five distinct stages are examined: storage buildings and facilities, loading and unloading, transportation, packaging, and information management systems. For this purpose, warehouses in Jiangsu Province, China, are employed as a case study. The results show that automating warehouses can achieve a reduction in total carbon emissions of 42.85% compared with traditional warehouses, with total life cycle emissions of 39,531.26 tCO2, and the transportation stage is identified as the predominant contributor. This research not only offers actionable recommendations for strategies, including renewable energy integration, intelligent control systems, and standardized packaging protocols, but also establishes a framework for future investigations of refining carbon accounting methodologies—particularly in underexplored domains such as packaging. Full article
(This article belongs to the Section B: Energy and Environment)
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Figure 1
<p>Definition of the scope of an electric power material warehouse.</p>
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<p>Workflow of the carbon emission reduction calculation.</p>
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<p>Carbon emission composition of automated and traditional warehouses.</p>
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<p>Carbon emission factors for storage buildings and facilities.</p>
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<p>Carbon emission factors of the operation and maintenance stage.</p>
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<p>Carbon emission factors of different carbon emission scopes in the transportation stage.</p>
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<p>The impact of transportation distance on the carbon emission factor and the overall proportion of the transportation stage.</p>
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<p>Carbon emission factors of the information management platform.</p>
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20 pages, 2638 KiB  
Article
Estimating Carbon Emissions of Northeast Brazil Railway System
by Diogo da Fonseca Soares, Sayonara Andrade Eliziário, Josicleda Domiciano Galvíncio and Angel Fermin Ramos-Ridao
Buildings 2024, 14(12), 3986; https://doi.org/10.3390/buildings14123986 - 16 Dec 2024
Viewed by 367
Abstract
This article addresses the developing of a framework to obtain specific GHG emissions for the railway system and proposes mitigation strategies. To achieve this purpose, a comprehensive life cycle assessment (LCA) method was employed with input data from various sources to analyze the [...] Read more.
This article addresses the developing of a framework to obtain specific GHG emissions for the railway system and proposes mitigation strategies. To achieve this purpose, a comprehensive life cycle assessment (LCA) method was employed with input data from various sources to analyze the contribution of energy consumption and the emissions of the railway system. This paper included gathering data from an infrastructure operation and maintenance for detailed GHG emissions impact. This study also presents a comparative analysis of the GHG emissions in different urban railway transportation systems in Northeast Brazil, providing valuable contextual insights. As a result of the combination of total GHG emissions analysis from the states of the Northeast Brazil railway system, a total of 11,996.11 metric tons of CO2 equivalent (tCO2e) was estimated. The main line traction was a prominent source of the greenhouse gas footprint, especially for the diesel traction systems at Paraiba. The proposed framework shows that significant environmental benefits can be realized with proper decision-making to increase the number of passengers–kilometer transported by rail. Full article
(This article belongs to the Special Issue Urban Climatic Suitability Design and Risk Management)
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Figure 1
<p>Location map of the northeastern railway system, Brazil.</p>
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<p>Flowchart of greenhouse gas emissions methodology for LCA railway.</p>
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<p>Composition of consumption and emissions in 2021.</p>
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<p>Composition of consumption and GHG emissions of rail system. (<b>A</b>) Rail system of Pernambuco. (<b>B</b>) Rail system of Paraiba. (<b>C</b>) Rail system of Alagoas. (<b>D</b>) Rail system of Rio Grande do Norte.</p>
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<p>GHG emissions of main line traction (diesel).</p>
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<p>GHG emission (gCO<sub>2</sub>/PKT).</p>
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33 pages, 6495 KiB  
Review
A Review of Transparent Conducting Films (TCFs): Prospective ITO and AZO Deposition Methods and Applications
by Jessica Patel, Razia Khan Sharme, Manuel A. Quijada and Mukti M. Rana
Nanomaterials 2024, 14(24), 2013; https://doi.org/10.3390/nano14242013 - 14 Dec 2024
Viewed by 491
Abstract
This study offers a comprehensive summary of the current states as well as potential future directions of transparent conducting oxides (TCOs), particularly tin-doped indium oxide (ITO), the most readily accessible TCO on the market. Solar cells, flat panel displays (FPDs), liquid crystal displays [...] Read more.
This study offers a comprehensive summary of the current states as well as potential future directions of transparent conducting oxides (TCOs), particularly tin-doped indium oxide (ITO), the most readily accessible TCO on the market. Solar cells, flat panel displays (FPDs), liquid crystal displays (LCDs), antireflection (AR) coatings for airbus windows, photovoltaic and optoelectronic devices, transparent p–n junction diodes, etc. are a few of the best uses for this material. Other conductive metals that show a lot of promise as substitutes for traditional conductive materials include copper, zinc oxide, aluminum, silver, gold, and tin. These metals are also utilized in AR coatings. The optimal deposition techniques for creating ITO films under the current conditions have been determined to be DC (direct current) and RF (radio frequency) MS (magnetron sputtering) deposition, both with and without the introduction of Ar gas. When producing most types of AR coatings, it is necessary to obtain thicknesses of at least 100 nm and minimum resistivities on the order of 10−4 Ω cm. For AR coatings, issues related to less-conductive materials than ITO have been considered. Full article
(This article belongs to the Section Nanophotonics Materials and Devices)
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Figure 1

Figure 1
<p>Schematic diagram of the e-beam evaporation system used to deposit ITO films. Reproduced from with permission from the copyright clearance center.</p>
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<p>The XRD patterns for the phase analysis of the ITO on Si films (<b>A</b>) as deposited and post-annealed at (<b>B</b>) 500 °C, (<b>C</b>) 600 °C, and (<b>D</b>) 700 °C. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>Transmittance spectra for the ITO thin films as deposited and after annealing are displayed. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>ITO’s electrical resistivity was measured, and its relationship to the post-annealing temperature was determined. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>At three distinct post-annealing temperatures, surface roughness was measured for ITO thin films on Si using 3D AFM: (<b>a</b>) as deposited, (<b>b</b>) 500 °C, (<b>c</b>) 600 °C, and (<b>d</b>) 700 °C. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>At three distinct post-annealing temperatures, surface roughness was measured for ITO thin films on Si using 3D AFM: (<b>a</b>) as deposited, (<b>b</b>) 500 °C, (<b>c</b>) 600 °C, and (<b>d</b>) 700 °C. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>ITO films’ XRD patterns after being deposited and heated to various temperatures (<b>a</b>) in air and (<b>b</b>) under vacuum. Reproduced from [<a href="#B2-nanomaterials-14-02013" class="html-bibr">2</a>] with permission from the copyright clearance center.</p>
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<p>The transmittance spectra of the ITO thin films under diverse environmental conditions, including (<b>a</b>) in air and (<b>b</b>) under vacuum, at different temperatures during deposition and annealing. Reproduced from [<a href="#B2-nanomaterials-14-02013" class="html-bibr">2</a>] with permission from the copyright clearance center.</p>
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<p>Transmittances (%T) and resistivities (%R) of (<b>a</b>) Asahi ITO film and (<b>b</b>) conventional sol–gel ITO film (were measured and fitted. Reproduced from [<a href="#B45-nanomaterials-14-02013" class="html-bibr">45</a>] with permission from the copyright clearance center.</p>
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<p>Electrical resistivity and mobility (μ) spectra were calculated from the fit of the optical data in <a href="#nanomaterials-14-02013-f010" class="html-fig">Figure 10</a>b. Reproduced from [<a href="#B45-nanomaterials-14-02013" class="html-bibr">45</a>] with permission from the copyright clearance center.</p>
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<p>The heated ITO films’ XRD patterns, which were made from an aqueous solution with r = 0.030–0.15, are as follows: (<b>a</b>) from 20 to 60° and (<b>b</b>) from 28 to 33°. Reproduced from [<a href="#B44-nanomaterials-14-02013" class="html-bibr">44</a>] with permission from the copyright clearance center.</p>
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<p>Optical transmittance (%T) spectra (<b>a</b>) and annealing-temperature-dependent optical transmittance and bandgap (<b>b</b>,<b>c</b>) of inkjet-printed ITO thin films annealed at various temperatures. Reproduced from [<a href="#B47-nanomaterials-14-02013" class="html-bibr">47</a>] with permission from the copyright clearance center.</p>
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<p>XRD patterns of glass, ITO/NP–glass samples, and ITO/glass. Reproduced from [<a href="#B48-nanomaterials-14-02013" class="html-bibr">48</a>] with permission from the copyright clearance center.</p>
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<p>Variations in resistivity with substrate temperature for ITO films. Reproduced from [<a href="#B43-nanomaterials-14-02013" class="html-bibr">43</a>] with permission from copyright clearance center.</p>
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<p>XRD patterns of the AZO/Ag/AZO multilayer stacks on mica sheets at different annealing temperatures. Reproduced from [<a href="#B38-nanomaterials-14-02013" class="html-bibr">38</a>] with permission from the copyright clearance center.</p>
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<p>The AZO/Ag/AZO films’ optical transmittance (%T) spectra recorded at various annealing temperatures and for the as-deposited sample. Reproduced from [<a href="#B55-nanomaterials-14-02013" class="html-bibr">55</a>] with permission from the copyright clearance center.</p>
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<p>Resistivity and FOM values of AZO/Ag/AZO films for the as-deposited sample and different annealing temperatures. Reproduced from [<a href="#B55-nanomaterials-14-02013" class="html-bibr">55</a>] with permission from the copyright clearance center.</p>
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<p>Resistivity spatial distribution as a function of the film thickness for AZO thin films produced by RF-DC with H2 injection. Reproduced from [<a href="#B49-nanomaterials-14-02013" class="html-bibr">49</a>] with permission from the copyright clearance center.</p>
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<p>Resistivities of AZO films, made with different thicknesses via PLD, as a function of the exposure duration. Reproduced from [<a href="#B49-nanomaterials-14-02013" class="html-bibr">49</a>] with permission from the copyright clearance center.</p>
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31 pages, 441 KiB  
Review
The Emerging Role of Artificial Intelligence in Enhancing Energy Efficiency and Reducing GHG Emissions in Transport Systems
by Tymoteusz Miller, Irmina Durlik, Ewelina Kostecka, Adrianna Łobodzińska and Marcin Matuszak
Energies 2024, 17(24), 6271; https://doi.org/10.3390/en17246271 - 12 Dec 2024
Viewed by 611
Abstract
The global transport sector, a significant contributor to energy consumption and greenhouse gas (GHG) emissions, requires innovative solutions to meet sustainability goals. Artificial intelligence (AI) has emerged as a transformative technology, offering opportunities to enhance energy efficiency and reduce GHG emissions in transport [...] Read more.
The global transport sector, a significant contributor to energy consumption and greenhouse gas (GHG) emissions, requires innovative solutions to meet sustainability goals. Artificial intelligence (AI) has emerged as a transformative technology, offering opportunities to enhance energy efficiency and reduce GHG emissions in transport systems. This study provides a comprehensive review of AI’s role in optimizing vehicle energy management, traffic flow, and alternative fuel technologies, such as hydrogen fuel cells and biofuels. It explores AI’s potential to drive advancements in electric and autonomous vehicles, shared mobility, and smart transportation systems. The economic analysis demonstrates the viability of AI-enhanced transport, considering Total Cost of Ownership (TCO) and cost-benefit outcomes. However, challenges such as data quality, computational demands, system integration, and ethical concerns must be addressed to fully harness AI’s potential. The study also highlights the policy implications of AI adoption, underscoring the need for supportive regulatory frameworks and energy policies that promote innovation while ensuring safety and fairness. Full article
24 pages, 5781 KiB  
Article
Co-Design Optimization and Total Cost of Ownership Analysis of an Electric Bus Depot Microgrid with Photovoltaics and Energy Storage Systems
by Boud Verbrugge, Thomas Geury and Omar Hegazy
Energies 2024, 17(24), 6233; https://doi.org/10.3390/en17246233 - 11 Dec 2024
Viewed by 361
Abstract
Due to the increasing share of battery electric buses (BEBs) in cities, depots need to be adapted to the increasing load demand. The integration of renewable energy sources (RESs) into a depot can increase the self-consumption, but optimal sizing is required for a [...] Read more.
Due to the increasing share of battery electric buses (BEBs) in cities, depots need to be adapted to the increasing load demand. The integration of renewable energy sources (RESs) into a depot can increase the self-consumption, but optimal sizing is required for a cost-efficient and reliable operation. Accordingly, this paper introduces a co-design optimization framework for a depot microgrid, equipped with photovoltaics (PVs) and an energy storage system (ESS). Three European cities are considered to evaluate the effect of different environmental conditions and electricity prices on the optimal microgrid design. Accurate models of the different subsystems are created to estimate the load demand and the power generation. Different energy management strategies (EMSs), developed to properly control the power flow within the microgrid, are compared in terms of operational costs reduction, one of which was also experimentally validated using a hardware-in-the-loop (HiL) test setup. In addition, the total cost of ownership (TCO) of the depot microgrid is analyzed, showing that an optimally designed depot microgrid can reduce the charging-related expenses for the public transport operator (PTO) by 30% compared to a scenario in which only the distribution grid supplies the BEB depot. Full article
(This article belongs to the Section E: Electric Vehicles)
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Figure 1
<p>Overview of the architecture of the depot microgrid.</p>
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<p>Single-diode model of a PV module.</p>
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<p>Equivalent circuit diagram of a first-order Thevenin model.</p>
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<p>Overview of the control signals of the simple EMS (all, except tariff) and the advanced EMS (all).</p>
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<p>Flowchart of the advanced rule-based EMS.</p>
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<p>Simulation results illustrating the operation of the depot microgrid in Brussels with the simple EMS with (<b>a</b>) electricity tariff, (<b>b</b>) current of each subsystem, and (<b>c</b>) SoC of the ESS.</p>
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<p>Simulation results illustrating the operation of the depot microgrid in Barcelona with the simple EMS with (<b>a</b>) electricity tariff, (<b>b</b>) current of each subsystem, and (<b>c</b>) SoC of the ESS.</p>
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<p>Simulation results illustrating the operation of the depot microgrid in Gothenburg with the simple EMS with (<b>a</b>) electricity tariff, (<b>b</b>) current of each subsystem, and (<b>c</b>) SoC of the ESS.</p>
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<p>Simulation results illustrating the operation of the depot microgrid in Brussels with the advanced EMS with (<b>a</b>) electricity tariff, (<b>b</b>) current of each subsystem, and (<b>c</b>) SoC of the ESS.</p>
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<p>Simulation results illustrating the operation of the depot microgrid in Barcelona with the advanced EMS with (<b>a</b>) electricity tariff, (<b>b</b>) current of each subsystem, and (<b>c</b>) SoC of the ESS.</p>
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<p>Simulation results illustrating the operation of the depot microgrid in Gothenburg with the advanced EMS with (<b>a</b>) electricity tariff, (<b>b</b>) current of each subsystem, and (<b>c</b>) SoC of the ESS.</p>
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<p>TCO comparison of different depot configurations in the considered cities.</p>
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<p>Overview of the power devices included in the HiL test setup to represent the depot microgrid.</p>
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<p>HiL test setup of a depot microgrid.</p>
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<p>Experimental test results of the EMS for the DC microgrid with (<b>a</b>) electricity tariff and (<b>b</b>) current of each subsystem.</p>
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13 pages, 1499 KiB  
Article
Study of the Total Ownership Cost of Electric Vehicles in Romania
by Lucian-Ioan Dulău
World Electr. Veh. J. 2024, 15(12), 569; https://doi.org/10.3390/wevj15120569 - 11 Dec 2024
Viewed by 398
Abstract
Due to the significant increase in the number of EVs, this manuscript presents a study of the total ownership cost of electric vehicles in Romania. The total cost of ownership (TCO) includes the initial purchase price, maintenance costs, power prices, and government incentives [...] Read more.
Due to the significant increase in the number of EVs, this manuscript presents a study of the total ownership cost of electric vehicles in Romania. The total cost of ownership (TCO) includes the initial purchase price, maintenance costs, power prices, and government incentives or subsidies unique to the market in Romania. The TCO was calculated for battery electric vehicles (BEVs) and internal combustion vehicles (ICEs). Several vehicles were selected for the study, representing the models with the highest sales in Romania and a similar price range. The results show that EVs have a lower TCO compared with internal combustion vehicles if the battery replacement cost for EVs is not considered in the analysis. If this cost is considered, the TCO for the BEVs has a significant increase due to the high cost of the battery. Another analysis performed regards the CO2 emissions. These are higher for ICEs compared to BEVs, so the BEVs help reduce emissions. Full article
(This article belongs to the Special Issue Impact of Electric Vehicles on Power Systems and Society)
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Figure 1
<p>Price of EVs [<a href="#B50-wevj-15-00569" class="html-bibr">50</a>,<a href="#B51-wevj-15-00569" class="html-bibr">51</a>,<a href="#B52-wevj-15-00569" class="html-bibr">52</a>].</p>
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<p>Power consumption of EVs [<a href="#B53-wevj-15-00569" class="html-bibr">53</a>,<a href="#B54-wevj-15-00569" class="html-bibr">54</a>,<a href="#B55-wevj-15-00569" class="html-bibr">55</a>,<a href="#B56-wevj-15-00569" class="html-bibr">56</a>].</p>
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<p>Price of ICEs [<a href="#B59-wevj-15-00569" class="html-bibr">59</a>,<a href="#B60-wevj-15-00569" class="html-bibr">60</a>].</p>
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<p>Fuel consumption of ICEs [<a href="#B59-wevj-15-00569" class="html-bibr">59</a>,<a href="#B60-wevj-15-00569" class="html-bibr">60</a>,<a href="#B61-wevj-15-00569" class="html-bibr">61</a>].</p>
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<p>TCO for EVs (charging at dedicated station).</p>
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<p>TCO for EVs (charging at home).</p>
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<p>TCO for ICEs.</p>
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<p>CO<sub>2</sub> emissions for BEVs and ICEs.4.</p>
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22 pages, 4654 KiB  
Article
Synthesis, Characterization and Antimicrobial Activity of Trimethylantimony(V) Biscyanoximates, a New Family of Antimicrobials
by Seth A. Amankrah, Tarosha Salpadoru, Kaitlyn Cotton, Marianna A. Patrauchan, Karen L. Wozniak and Nikolay Gerasimchuk
Molecules 2024, 29(23), 5779; https://doi.org/10.3390/molecules29235779 - 6 Dec 2024
Viewed by 625
Abstract
Antimicrobial compounds play a critical role in combating microbial infections. However, the emergence of antibiotic and antifungal resistance and the scarcity of new antibiotic developments pose a significant threat and demand the discovery of new antimicrobials for both bacterial and fungal pathogens. Our [...] Read more.
Antimicrobial compounds play a critical role in combating microbial infections. However, the emergence of antibiotic and antifungal resistance and the scarcity of new antibiotic developments pose a significant threat and demand the discovery of new antimicrobials for both bacterial and fungal pathogens. Our previous work described the first generation (G1) of organoantimony-based compounds that showed antimicrobial activity against several bacterial and fungal pathogens. Here, we present our efforts in modifying these compounds by replacing the tetraphenyl backbone in G1 compounds with a trimethyl group, thereby generating a new series of compounds we refer to as “generation 2”, G2. In addition to the novel backbone structure, we introduced three new anionic chloro-cyanoxime ligand groups, namely 2,4-diCl-PhCO, 2,6-diCl-PhCO and 2Cl-PhCO, which were found to be biologically active in the past. Nine new compounds of SbMe3L2 composition were obtained in high yields and characterized by NMR, IR spectroscopies, thermogravimetric TG/DSC and X-ray single crystal analyses. The antibacterial activity of the cyanoximates was tested against three bacterial (Pseudomonas aeruginosa PAO1, Escherichia coli S17 and methicillin-resistant Staphylococcus aureus (MRSA) NRS70) and two fungal (Candida albicans strain SC5314 and Cryptococcus neoformans strain H99) pathogens. Two compounds, SbMe3(MCO)2 and SbMe3(2,4-diClPhCO)2, were active against bacterial strains and inhibited the growth of PAO1 and MRSA with MICs of 50 and 100 µg/mL, respectively. Three compounds, SbMe3(MCO)2, SbMe3(ECO)2 and SbMe3(TCO)2, were active against fungal strains and inhibited either one of or both C. albicans and C. neoformans at MICs of 2.6–66.67 μg/mL. In addition, SbMe3(TCO)2 and SbMe3(MCO)2 were fungicidal at MFC 33.33–66.67 μg/mL. Ultra-thin-layer TEM imaging suggested that SbMe3(MCO)2 targets the integrity of bacterial membranes. Overall, four of the studied G2 series compounds possess antimicrobial activity against a broad range of microbial pathogens, with particular potential against fungal pathogens, which will be explored in further studies. Full article
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Graphical abstract

Graphical abstract
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<p>(<b>A</b>)—schematic depiction of the <b><span class="html-italic">G1</span></b> and <b><span class="html-italic">G2</span></b> families of organoantimony(V) cyanoximates where L is the cyanoxime anion; (<b>B</b>)—choice of ligands for the <b><span class="html-italic">G2</span></b> series. Highlighted in red are the most active compounds found in studies of the <b><span class="html-italic">G1</span></b> family of organoantimonials [<a href="#B34-molecules-29-05779" class="html-bibr">34</a>].</p>
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<p>Molecular structures and numbering schemes of SbMe<sub>3</sub>L<sub>2</sub> compounds with (<b>A</b>) ester-cyanoxime ECO<sup>−</sup>, and halogenated arylcyanoximes such as (<b>B</b>) 4Cl-PhCO<sup>−</sup>, (<b>C</b>) 2,4-diCl-PhCO<sup>−</sup> and (<b>D</b>) 2,6-diCl-PhCO<sup>−</sup>. Assignment of geometry of anions is shown.</p>
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<p>Molecular structures of trimetylantimony(V) bis-cyanoximates such as the amide/thioamide-cyanoximes: (<b>A</b>) ACO<sup>−</sup>, (<b>B</b>) TCO<sup>−</sup>, (<b>C</b>) MCO<sup>−</sup> and (<b>D</b>) TDCO<sup>−</sup>. Geometry of O-bound anions is shown.</p>
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<p>Fragment of <sup>13</sup>C{<sup>1</sup>H} NMR spectrum of SbMe<sub>3</sub>(TDCO)<sub>2</sub> in <span class="html-italic">sp</span><sup>2</sup> carbon atom region in DMSO-d<sub>6</sub> at room temperature. Red asterisks and numbers show signals of minor <span class="html-italic">cis</span>-anti stereoisomer.</p>
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<p>Thermal properties of SbMe<sub>3</sub>(TDCO)<sub>2</sub>: (<b>A</b>)—fragment of TG/DSC traces with clear melting at 175 °C while green arrow indicates point of crucible response on melting; (<b>B</b>)—yellow initial powder of the compound; (<b>C</b>)—final crucible content with sheets of elemental Sb.</p>
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<p>Fragment of TG/DSC traces for SbMe<sub>3</sub>(4Cl-PhCO)<sub>2</sub> showing clear melting at 161.46 °C followed by decomposition after ~190 °C. Green arrow shows crucible weight response at beginning of melting.</p>
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<p>Representative ultra-thin TEM images of <span class="html-italic">P. aeruginosa</span> PAO1 treated with SbMe<sub>3</sub>(MCO)<sub>2</sub> at the MIC or the solvent control, DMSO, for 1 h at 37 °C. The black arrows point to the separation of the cytoplasmic material from the cellular envelope observed upon treatment. In contrast, fully intact cells were observed in the control DMSO-treated group.</p>
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<p>General route for preparation of antimony cyanoximates using the heterogeneous metathesis reaction.</p>
Full article ">Scheme 1
<p>Principal geometrical stereoisomers of cyanoximes (<b>A</b>) and observed isomerism of protonated HL in amide-/ester-/keto-cyanoximes (<b>B</b>) [<a href="#B20-molecules-29-05779" class="html-bibr">20</a>].</p>
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<p>Redistribution of electron density in cyanoxime anions.</p>
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19 pages, 9531 KiB  
Article
Interannual and Seasonal Variability of CO2 Parameters in the Tropical Atlantic Ocean
by Frederic Bonou, A. Nathanael Dossa, Adeola M. Dahunsi and Zacharie Sohou
J. Mar. Sci. Eng. 2024, 12(12), 2248; https://doi.org/10.3390/jmse12122248 - 6 Dec 2024
Viewed by 574
Abstract
This study examined the carbon cycling dynamics in the tropical Atlantic Ocean from 1985 to 2023, focusing on factors influencing the surface partial pressure of CO2 (pCO2), freshwater input, total alkalinity (ALK), total dissolved carbon (TCO2), and pH [...] Read more.
This study examined the carbon cycling dynamics in the tropical Atlantic Ocean from 1985 to 2023, focusing on factors influencing the surface partial pressure of CO2 (pCO2), freshwater input, total alkalinity (ALK), total dissolved carbon (TCO2), and pH levels. The time series data revealed significant trends, with average pCO2 concentrations rising from approximately 350 μatm in the early 1990s to over 400 μatm by 2023. The TCO2 levels increased from about 2000 μmol/kg to 2200 μmol/kg, while ALK rose from approximately 2300 μmol/kg to 2500 μmol/kg. This increase highlights the ocean’s role as a carbon sink, particularly in areas with high biological productivity and upwelling where TCO2 also rose. This study employed Empirical Orthogonal Functions (EOFs) to identify variability modes and understand spatial patterns of pCO2. Freshwater dynamics significantly affect TCO2 concentrations, particularly in coastal regions, where pH can shift from 8.2 to 7.9, exacerbating acidification. Rising sea surface temperatures have been linked to elevated pCO2 values. These findings support the need for ongoing monitoring and effective management strategies to mitigate the impacts of climate change and ensure the sustainability of marine resources. This study documented the long-term trends in tropical Atlantic CO2 parameters linked to the North Atlantic Oscillation (NAO) and Atlantic Multidecadal Oscillation (AMO). Full article
(This article belongs to the Section Chemical Oceanography)
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<p>Study area with spatial distribution of elevation from GEBCO 2024 [<a href="#B20-jmse-12-02248" class="html-bibr">20</a>]; data of main surface ocean circulation in tropical Atlantic. The arrows indicate the ocean surface circulation direction.</p>
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<p>Yearly averages of CO<sub>2</sub> parameters from 1985 to 2022. Shaded area shows minimum and maximum values each year for (<b>a</b>) pCO<sub>2</sub> (μatm), (<b>b</b>) TCO<sub>2</sub> (μmol·kg⁻<sup>1</sup>), (<b>c</b>) FCO<sub>2</sub> (mol·C·m⁻<sup>2</sup>·yr⁻<sup>1</sup>), and (<b>d</b>) pH.</p>
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<p>Spatial distribution of average (<b>a</b>) pCO<sub>2</sub>, (<b>b</b>) FGCO<sub>2</sub>, (<b>c</b>) total alkalinity (ALK), and (<b>d</b>) total inorganic carbon (TCO<sub>2</sub>) over the period 1985 to 2022.</p>
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<p>Seasonal variability of FGCO<sub>2</sub> during boreal: (<b>a</b>) winter (December–January–February: DJF), (<b>b</b>) spring (March-April-May: MAM), (<b>c</b>) summer (June–July–August: JJA), and (<b>d</b>) autumn (September–October–November: SON).</p>
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<p>Seasonal variability of pCO<sub>2</sub> during boreal (<b>a</b>) winter (December–January–February: DJF), (<b>b</b>) spring (March–April–May: MAM), (<b>c</b>) summer (June–July–August: JJA), and (<b>d</b>) autumn (September–October–November: SON).</p>
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<p>Seasonal variability of total alkalinity (ALK) during boreal (<b>a</b>) winter (December–January–February: DJF), (<b>b</b>) spring (March–April–May: MAM), (<b>c</b>) summer (June–July–August: JJA), and (<b>d</b>) autumn (September–October–November: SON).</p>
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<p>Seasonal variability of total inorganic carbon during boreal (<b>a</b>) winter (December–January–February: DJF), (<b>b</b>) spring (March–April–May: MAM), (<b>c</b>) summer (June–July–August: JJA), and (<b>d</b>) autumn (September–October–November: SON).</p>
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<p>Seasonal variability of principal component (PCs) of CO<sub>2</sub> parameters (pCO<sub>2</sub>, TCO<sub>2</sub>, FGCO<sub>2,</sub> ALK), SSS, SST, CHL, net primary production, and wind in tropical Atlantic Ocean.</p>
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<p>Spatial patterns of the first Empirical Orthogonal Function (EOF1) and corresponding normalized principal component (PC) time series for various parameters in the tropical Atlantic Ocean.</p>
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<p>Correlation matrix showing the relationships between the climate modes (NINO3.4, AMO, and NAO) and CO<sub>2</sub>-related parameters (FGCO<sub>2</sub>, PCO<sub>2</sub>, and TCO<sub>2</sub>) in the study region. The colors indicate the strength and direction of correlations, with blue for positive and red for negative. The significant correlations (95% of significance level) highlight the interplay between climate variability and carbon cycle dynamics. The cross means, there is no significance.</p>
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22 pages, 6085 KiB  
Article
Technical–Economic Analyses of Electric Energy Generation by Biogas from Anaerobic Digestion of Sewage Sludge from an Aerobic Reactor with the Addition of Charcoal
by Cornélio Ribeiro Garcia, Michael Danilo Vargas Hincapie, Regina Mambeli Barros, Maxi Estefany Huamán Córdova, Hellen Luisa de Castro e Silva, Ivan Felipe Silva dos Santos, Electo Eduardo Silva Lora, Geraldo Lucio Tiago Filho, João Victor Rocha de Freitas, Adriele Maria de Cássia Crispim and Aylla Joani Mendonça de Oliveira Pontes
Methane 2024, 3(4), 595-616; https://doi.org/10.3390/methane3040034 - 2 Dec 2024
Viewed by 746
Abstract
This study aimed to obtain the energy recovery potential of the biogas produced from anaerobic digestion (AD) of the sludge from a wastewater treatment plant (WWTP), including the use of biochar as an additive for substrate co-digestion and catalyst for methane production. We [...] Read more.
This study aimed to obtain the energy recovery potential of the biogas produced from anaerobic digestion (AD) of the sludge from a wastewater treatment plant (WWTP), including the use of biochar as an additive for substrate co-digestion and catalyst for methane production. We carried out the following steps: chemical–physical laboratory analyses of sludge samples; the building, operation, and monitoring of an experimental prototype of a batch bioreactor of 2.5 L for the AD of the sludge (with and without the addition of charcoal); qualitative measurements of biogas; the study of charcoal morphology; and the projection of useful energy generation from the AD sludge after treatment. A study on the economic viability and avoided greenhouse gas (GHG) emissions was performed based on the experimental results. The substrate showed alterations in all the physicochemical parameters evaluated after AD, such as a reduction of 35% in the biochemical oxygen demand (BOD) analysis; the experiment carried out using biochar showed positive results regarding the speed of CH4 production and a greater potential for energy recovery. Enterprises from 2000 kW onwards would present an internal rate of return (IRR) equal to or higher than the minimum attractiveness rate (MAR) of 15%. The USD 95.28/MWh tariff presented economic feasibility for the studied scenarios. WWTPs that produce enough sludge to generate power of 2000 kW would need to process the waste of 117,200 inhabitants with charcoal addition and 136,000 without charcoal. It would be possible to avoid the emission of 2307.97 tCO2/year (2000 kW). According to the results obtained, this study revealed that using alternative energies based on anaerobic digestion and biochar can generate positive results regarding methane production, and its application as an energy source in a WWTP proved to be economically viable at a specific level of power production. Full article
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<p>Experimental units: (<b>a</b>) bottle assembled (left); and (<b>b</b>) bottles immersed in the water system for heating (right).</p>
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<p>Values for investment in biogas thermal power plants. Source: Silva et al. [<a href="#B50-methane-03-00034" class="html-bibr">50</a>].</p>
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<p>Comparative plot of the production of CH<sub>4.</sub></p>
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<p>Comparative plot of the production of H<sub>2</sub>S.</p>
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<p>SEM of (<b>a</b>) charcoal and (<b>b</b>) SEM approximation of charcoal.</p>
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<p>SEM detail of charcoal porosity.</p>
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<p>NPV (<b>a</b>) Scenario 1 (left superior); (<b>b</b>) Scenario 2 (right superior); (<b>c</b>) Scenario 3 (left inferior); (<b>d</b>) (right inferior).</p>
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<p>IRR regarding Scenario 1 and Scenario 2 related to minimum attractiveness rate.</p>
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<p>Population: (<b>a</b>) versus Scenario 1 and Scenario 2 (right); (<b>b</b>) energy generated and avoided GHG emissions versus Scenario 1 and Scenario 2 related to minimum attractiveness rate.</p>
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9 pages, 1161 KiB  
Article
An Evaluation of a Point-of-Care GEM Premier ChemSTAT Analyzer in an Emergency Department: Prevention of Contrast-Induced Nephropathy and Optimization of Patient Flow
by Marina Brailova, Marie Audin, Julien Raconnat, Jean-Baptiste Bouillon-Minois, Jeannot Schmidt, Bruno Pereira, Damien Bouvier and Vincent Sapin
J. Clin. Med. 2024, 13(23), 7174; https://doi.org/10.3390/jcm13237174 - 26 Nov 2024
Viewed by 368
Abstract
Background: Having a laboratory renal profile for medical imaging examinations requiring contrast media (CM) administration is strongly advised. Creatinine helps identify patients at risk of contrast-induced nephropathy (CIN). The GEM® Premier™ ChemSTAT (Werfen) is a point-of-care (POC) analyzer with 12 emergency parameters, [...] Read more.
Background: Having a laboratory renal profile for medical imaging examinations requiring contrast media (CM) administration is strongly advised. Creatinine helps identify patients at risk of contrast-induced nephropathy (CIN). The GEM® Premier™ ChemSTAT (Werfen) is a point-of-care (POC) analyzer with 12 emergency parameters, including a creatinine assay. This study aims to compare ChemSTAT with the central analytical solution of the University Hospital of Clermont-Ferrand and to evaluate the interest in using POC creatinine in the emergency department (ED) to optimize the flow of patients, especially when CM administration is necessary. Methods: More than 200 whole blood (WB) samples from the ED were evaluated on the ChemSTAT analyzer. As comparative methods, the plasma aliquots from the same samples were assayed on an Atellica® CH (Siemens Healthineers). The clinical concordance was assessed according to the decision cut-offs of the French Society of Radiology for the risk of CIN. The availability times of biological results between ChemSTAT and the central laboratory were studied. Results: WB results from the ChemSTAT analyzer correlated well with those from the Atellica® CH, except for tCO2 (the known bias between the Siemens and Cobas Roche methods for predicting ChemSTAT values). The results of the creatinine assay allow for identical medical decisions in comparison to the renal-risk cut-offs. The availability of the biological results was reduced by 50 min on average with ChemSTAT vs the central laboratory. Computed tomography (CT) was performed for 44.7% of patients, including the injection of the CM in 68% of cases. For these patients, the availability of creatinine results relative to imaging time is faster with the ChemSTAT by an average of 45.2 min. Conclusions: Great analytical and clinical correlations for creatinine assays allow for the safe identification of patients at risk of CIN, and improve patient flow in ED, especially for those requiring computed tomography with CM. Full article
(This article belongs to the Section Nephrology & Urology)
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<p>Correlation between the WB samples analyzed on the GEM<sup>®</sup> Premier™ ChemSTAT and the plasma samples analyzed on the Atellica<sup>®</sup> CH for creatinine: (<b>a</b>) linear regression; (<b>b</b>) Bland–Altman difference plots. The red line represents the absolute mean difference (µmol/L). The green lines represent the limit of agreement (±1.96 SD of the differences).</p>
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<p>Correlation between the Atellica<sup>®</sup> CH and the GEM<sup>®</sup> Premier™ ChemSTAT creatinine methods for the eGFR values: (<b>a</b>) linear regression; (<b>b</b>) Bland–Altman plot.</p>
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<p>Error grid analysis of concordance between eGFR risk stratification using the GEM<sup>®</sup> Premier™ ChemSTAT vs Atellica<sup>®</sup> CH creatinine methods: (<b>a</b>) comparison by a 30 mL/min/1.73 m<sup>2</sup> threshold; (<b>b</b>) comparison by a 45 mL/min/1.73 m<sup>2</sup> threshold.</p>
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14 pages, 4677 KiB  
Article
Enhanced Transparency and Resistive Switching Characteristics in AZO/HfO2/Ti RRAM Device via Post Annealing Process
by Yuseong Jang, Chanmin Hwang, Sanggyu Bang and Hee-Dong Kim
Inorganics 2024, 12(12), 299; https://doi.org/10.3390/inorganics12120299 - 21 Nov 2024
Viewed by 697
Abstract
As interest in transparent electronics increases, ensuring the reliability of transparent RRAM (T-RRAM) devices, which can be used to construct transparent electronics, has become increasingly important. However, defects and traps within these T-RRAM devices can degrade their reliability. In this study, we investigated [...] Read more.
As interest in transparent electronics increases, ensuring the reliability of transparent RRAM (T-RRAM) devices, which can be used to construct transparent electronics, has become increasingly important. However, defects and traps within these T-RRAM devices can degrade their reliability. In this study, we investigated the improvement of transparency and reliability of T-RRAM devices with an AZO/HfO2/Ti structure through rapid thermal annealing (RTA) at 450 °C for 60 s in a nitrogen atmosphere. The device without RTA exhibited a low transmittance of 30%, whereas the device with RTA showed a significantly higher transmittance of over 75%. Furthermore, the device operated at lower current levels after RTA, which resulted in a reduction in its operating voltages, and the forming, setting, and reset voltages changed from 3.3, 2.4, and −5.1 V, respectively, to 2, 1, and −2.7 V. This led to an improvement in the endurance characteristics of the device, which thereby suggests that these improvements can be attributed to a reduction in the defects and trap density within the T-RRAM device caused by RTA. Full article
(This article belongs to the Special Issue Optical and Quantum Electronics: Physics and Materials)
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<p>(<b>a</b>) Schematic structure, (<b>b</b>) cross-section FE-SEM images, and (<b>c</b>) transmittance at wavelengths of 200 nm to 1100 nm of the proposed T-RRAM.</p>
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<p>Resistive switching characteristics of proposed T-RRAM (<b>a</b>) without RTA and (<b>b</b>) after RTA at 450 °C for 60 s in a nitrogen atmosphere. (<b>c</b>) Retention and (<b>d</b>) endurance characteristics of T-RRAM without RTA and after RTA.</p>
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<p>XPS spectra of the Ti 2p region of the Ti top electrode without RTA and after RTA.</p>
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<p>XRD patterns of as-deposited HfO<sub>2</sub> and Ti films and HfO<sub>2</sub> and Ti films after RTA, and (inset) average grain size of the HfO<sub>2</sub> and Ti films.</p>
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<p>SCLC mechanism at the positive bias of proposed T-RRAM (<b>a</b>) without RTA and (<b>b</b>) after RTA.</p>
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<p>Band diagram of proposed T-RRAM (<b>a</b>) in the low-voltage region, (<b>b</b>) medium-voltage region and (<b>c</b>) high-voltage region. (The orange arrows indicate the direction of the electric field).</p>
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<p>Nyquist plot of proposed T-RRAM at (<b>a</b>) HRS and (<b>b</b>) LRS.</p>
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<p>Equivalent circuit of proposed T-RRAM at (<b>a</b>) HRS and (<b>b</b>) LRS.</p>
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11 pages, 2765 KiB  
Article
Eco-Friendly Castor Oil-Based Composite with High Clam Shell Powder Content
by Fangqing Weng, Kui Jian, Yazhou Yi, Peirui Zhang, Ernest Koranteng, Qing Huang, Jiahui Liu and Guoping Zeng
Polymers 2024, 16(23), 3232; https://doi.org/10.3390/polym16233232 - 21 Nov 2024
Viewed by 498
Abstract
Eco-friendly castor oil-based composites with a high content of clam shell powder were prepared in this study. Biomass composites were prepared by blending castor-oil-based polyurethane prepolymer (COPU) with a filler consisting of high-content clam shell powder (CSP), named CSP-COPU. The structure, microstructure, mechanical [...] Read more.
Eco-friendly castor oil-based composites with a high content of clam shell powder were prepared in this study. Biomass composites were prepared by blending castor-oil-based polyurethane prepolymer (COPU) with a filler consisting of high-content clam shell powder (CSP), named CSP-COPU. The structure, microstructure, mechanical properties, and thermal stability of the composites were investigated. The results showed that even at a loading as high as 75 wt.% of the CSP filler, the composite still exhibited good tensile strength and elongation at break. Furthermore, compared with the CSP-COPU composites, TCOS-50 synthesized through blending OH-terminated castor oil-based polyurethane prepolymer (TCOPU) and CSP filler proved that the chemical bond between COPU containing terminal -NCO groups and CSP containing active -OH groups was the key reason to obtaining the composite material with desirable properties. These findings provide prospects for applying biomass-loaded CSP-COPU composites in the packaging industry while contributing to carbon peak achievement and carbon neutrality. Full article
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<p>(<b>a</b>) Composite samples of COPU, COS-25,.COS-50, COS-75; (<b>b</b>) Composite samples of TCOS-50.</p>
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<p>(<b>a</b>) IR image of clam shell powder; IR image of COS composite material (<b>b</b>) placed for 24 h and (<b>c</b>) placed for 16 days.</p>
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<p>SEM images of (<b>A1</b>) COS-25 (×500), (<b>A2</b>) COS-25 (×3000), (<b>B1</b>) COS-50 (×500), (<b>B2</b>) (×3000), and (<b>C1</b>) COS-75 (×500), (<b>C2</b>) COS-75 (×3000).</p>
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<p>XRD pattern of (<b>a</b>) CSP and (<b>b</b>) COPU and composites.</p>
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<p>TG diagram of COPU and COS composites.</p>
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<p>Contact angle diagram of COS composites.</p>
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<p>Interface structure of COS-50 composite material.</p>
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13 pages, 5261 KiB  
Article
A High-Performance Micro Differential Pressure Sensor
by Xutao Fan, Lei Wang and Songsong Zhang
Micromachines 2024, 15(11), 1396; https://doi.org/10.3390/mi15111396 - 20 Nov 2024
Viewed by 538
Abstract
With the development of the micro electromechanical system (MEMS), which widely adopts micro differential pressure sensors (MDPSs), the demand for high-performance MDPSs had continuously increased. Pressure sensors realized using MEMS technology integrated with biomedical catheters are of significant importance in the detection and [...] Read more.
With the development of the micro electromechanical system (MEMS), which widely adopts micro differential pressure sensors (MDPSs), the demand for high-performance MDPSs had continuously increased. Pressure sensors realized using MEMS technology integrated with biomedical catheters are of significant importance in the detection and treatment of various biological diseases. Biomedical catheters used in low-Fr applications (1Fr = 0.33 mm outer diameter) require miniaturized sensors that do not compromise their performance. For instance, catheters (5Fr) used for central venous pressure (CVP) monitoring require the integration of high-performance sensors with total dimensions smaller than 1.65 mm along at least two directions (length, width, or height). In this paper, a silicon-on-insulator (SOI)-based MDPS was designed and fabricated for micro-pressure detection in the range of 0–1 kPa. The dimension of the sensor is only 1 mm × 1 mm × 0.4 mm, with a sensitivity of 3.401 mV/V/kPa at room temperature, nonlinearity of 0.376% FS (full scale), and an overall accuracy of 0.59% FS. The sensor operates normally when the temperature is even increased to 160 °C, and its temperature coefficient of zero output (TCO) and temperature coefficient of sensitivity (TCS) are 0.093% FS/°C and −0.144% FS/°C. The dimension and performance results of this MDPS demonstrate its potential to play a significant role in biomedical catheters. In addition, it is fabricated using an 8-inch MEMS process, which significantly reduces the cost. Full article
(This article belongs to the Special Issue Acoustic Transducers and Their Applications, 2nd Edition)
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<p>(<b>a</b>) Schematic diagram of a typical P-type piezoresistive resistor. (<b>b</b>) Wheatstone bridge diagram.</p>
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<p>P (N, T) coefficient of P-type silicon vs. doping concentration for different temperatures.</p>
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<p>(<b>a</b>) Schematic diagram of inductive diaphragm. (<b>b</b>) Stress distribution on the surface of a piezoresistor at 10 μm from the edge of the diaphragm under an applied pressure of 1 kPa.</p>
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<p>Distribution of doping concentration of the piezoresistor in the depth direction for different device layer thicknesses.</p>
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<p>Simulation results for different diaphragm thicknesses W: (<b>a</b>) Output vs. Pressure. (<b>b</b>) Sensitivity vs. Temperature.</p>
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<p>Three-dimensional model drawing of the sensor (values is μm).</p>
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<p>Manufacturing process flowchart and 8-inch MEMS wafer of the pressure sensor. (<b>a</b>) thermal oxidation; (<b>b</b>) boron light doping; (<b>c</b>) boron heave doping; (<b>d</b>) excess silicon; (<b>e</b>) deposition of silica and metal wiring; (<b>f</b>) back cavity release.</p>
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<p>Profiler result plot of the pressure sensor.</p>
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<p>Diagram of the pressure sensor test environment. (<b>a</b>) gas pressure source; (<b>b</b>) pressure controller; (<b>c</b>) DC power analyzer; (<b>d</b>) test sample; (<b>e</b>) semiconductor device analyzer; (<b>f</b>) digital multimeter; (<b>g</b>) temperature-controlled heating stage.</p>
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<p>(<b>a</b>) Static performance test chart of the sensor. (<b>b</b>) Enlargement of detail from <a href="#micromachines-15-01396-f010" class="html-fig">Figure 10</a>a.</p>
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<p>Temperature performance of the sensor.</p>
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11 pages, 2655 KiB  
Article
Enhanced Optical and Electrical Properties of IGZO/Ag/IGZO for Solar Cell Application via Post-Rapid Thermal Annealing
by Chanmin Hwang, Taegi Kim, Yuseong Jang, Doowon Lee and Hee-Dong Kim
Nanomaterials 2024, 14(22), 1841; https://doi.org/10.3390/nano14221841 - 18 Nov 2024
Viewed by 748
Abstract
In this paper, we optimized IGZO/Ag/IGZO (IAI) multilayer films by post-rapid thermal annealing (RTA) to enhance the electrical conductivity and optical transmittance in visible wavelengths for solar cell applications. Our optimized device showed an average transmittance of 85% in the visible range, with [...] Read more.
In this paper, we optimized IGZO/Ag/IGZO (IAI) multilayer films by post-rapid thermal annealing (RTA) to enhance the electrical conductivity and optical transmittance in visible wavelengths for solar cell applications. Our optimized device showed an average transmittance of 85% in the visible range, with a lowest sheet resistance of 6.03 Ω/□ when annealed at 500 °C for 60 s. Based on these results, we assessed our device with photo-generated short circuit current density (JSC) using a solar cell simulator to confirm its applicability in the solar cell. IAI multilayer RTA at 500 °C for 60 s showed a highest JSC of 40.73 mA/cm2. These results show that our proposed IAI multilayer film, which showed a high optical transparency and electrical conductivity optimized with post RTA, seems to be excellent transparent electrode for solar cell applications. Full article
(This article belongs to the Special Issue Nanostructured Materials for Electric Applications)
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<p>The RTA process for the IGZO/Ag/IGZO multilayer, and the right diagram describes the generated oxygen vacancies from the IGZO inside by RTA.</p>
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<p>AFM topology images of IGZO/Ag/IGZO after RTA, (<b>a</b>) RT, (<b>b</b>) 300, (<b>c</b>) 400, and (<b>d</b>) 500 °C for 60 s.</p>
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<p>The sheet resistance of (<b>a</b>) IGZO and (<b>b</b>) IGZO/Ag/IGZO multilayers after varying temperature conditions.</p>
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<p>(<b>a</b>) Impedance of IGZO/Ag/IGZO after RTA RT to 500 °C for 60 s and (<b>b</b>) equivalent circuit of IGZO/Ag/IGZO.</p>
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<p>(<b>a</b>) Transmittance, (<b>b</b>) reflectivity, and (<b>c</b>) absorption coefficient of IGZO/Ag/IGZO after RTA RT to 500 °C for 60 s, and each inset depicts the transmittance and reflectivity at 500 nm wavelength with varying annealing temperature.</p>
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<p>(<b>a</b>) Schematic structure of IGZO/Ag/IGZO-based solar cell and (<b>b</b>) the photo-generated short circuit current of IGZO/Ag/IGZO-based solar cell as a function of annealing temperature.</p>
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16 pages, 279 KiB  
Review
Driving the Future: An Analysis of Total Cost of Ownership for Electrified Vehicles in North America
by Patrycja Soszynska, Huda Saleh, Hana Kar, Lakshmi Varaha Iyer, Caniggia Viana and Narayan C. Kar
World Electr. Veh. J. 2024, 15(11), 492; https://doi.org/10.3390/wevj15110492 - 28 Oct 2024
Viewed by 2174
Abstract
As the number of electric vehicles (EVs) on North American roads continues to rise, driven by the shift toward sustainable transportation, understanding the economic implications of this transition is crucial. This review paper prioritizes an evaluation of the Total Cost of Ownership (TCO) [...] Read more.
As the number of electric vehicles (EVs) on North American roads continues to rise, driven by the shift toward sustainable transportation, understanding the economic implications of this transition is crucial. This review paper prioritizes an evaluation of the Total Cost of Ownership (TCO) for various types of EVs, providing insights into how different driving profiles align with the financial benefits of EV adoption. It demonstrates that at-home charging and government incentives are pivotal in reducing TCO. The analysis also offers a comprehensive overview of the factors driving EV growth, including declining operating and maintenance costs. Additionally, the paper explores adoption rates, charging infrastructure, and other non-monetary factors that influence consumer decisions in the shift to EVs. Conclusions emphasize that while EVs offer a financial advantage for many drivers, the success of broader adoption depends on decreasing the initial cost of EVs, developing charging infrastructure, and investing in charging networks. Full article
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