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Search Results (922)

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39 pages, 9178 KiB  
Article
Transitioning Ridehailing Fleets to Zero Emission: Economic Insights for Electric Vehicle Acquisition
by Mengying Ju, Elliot Martin and Susan Shaheen
World Electr. Veh. J. 2025, 16(3), 149; https://doi.org/10.3390/wevj16030149 - 4 Mar 2025
Viewed by 207
Abstract
Under California’s Clean Miles Standard (or SB 1014), transportation network companies (TNCs) must transition to zero-emission vehicles by 2030. One significant hurdle for TNC drivers is the electric vehicle (EV) acquisition and operating costs versus an internal combustion engine (ICE) vehicle. This study [...] Read more.
Under California’s Clean Miles Standard (or SB 1014), transportation network companies (TNCs) must transition to zero-emission vehicles by 2030. One significant hurdle for TNC drivers is the electric vehicle (EV) acquisition and operating costs versus an internal combustion engine (ICE) vehicle. This study therefore evaluates net TNC driving earnings through EV acquisition pathways—financing, leasing, and renting—along with EV-favoring policy options. Key metrics assessed include (1) total TNC income when considering service fees, fuel costs, monthly vehicle payments, etc., and (2) the time EVs take to reach parity with their ICE counterparts. Monthly comparisons illustrate the earning differentials between new/used EVs and gas-powered vehicles. Our analyses employing TNC data from 2019 to 2020 suggest that EV leasing is optimal for short-term low-mileage drivers; EV financing is more feasible for those planning to drive for TNCs for over two years; EV rentals are only optimal for higher mileages, and they are not an economical pathway for longer-term driving. Sensitivity analyses further indicate that EV charging price discounts are effective in shortening the time for EVs to reach cost parity over ICEs. Drivers may experience a total asset gain when reselling their TNC vehicle after two to three years. Full article
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<p>Driver identification criteria applied to each TNC trip.</p>
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<p>Annual driver earnings in the top 30 counties ranked by driver earnings (2019 to 2020, N = 32,359 drivers included).</p>
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<p>Monthly TNC net earnings in the first month, financing (<b>left</b>) vs. leasing (<b>right</b>).</p>
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<p>Net TNC driver monthly earnings after 84 months, financing (<b>left</b>) vs. leasing (<b>right</b>).</p>
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<p>Monthly TNC net earnings for renting (<b>left</b>) and minimum miles per week needed to reach a positive net income (<b>right</b>).</p>
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<p>Cumulative net driver earnings (<span class="html-italic">CNDEs</span>) of EVs incorporating total assets when driving 100 miles/week (<b>left</b>) and 1100 miles/week (<b>right</b>).</p>
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<p>Same-vehicle time-to-parity between financing and leasing by TNC miles driven per week across different fuel types (<b>left</b>) with total asset incorporated (<b>right</b>) (in months).</p>
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<p>Cross-comparison of net TNC driver earnings (<span class="html-italic">NDMEs</span>) difference using EV vs. ICE vehicle (<span class="html-italic">Diff</span>).</p>
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<p>Line charts of net TNC driver monthly earnings (<span class="html-italic">NDMEs</span>) comparison (<span class="html-italic">Diff</span>), new vehicle (<b>left</b>) vs. used vehicle (<b>right</b>).</p>
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<p>Net difference in net monthly TNC income across financing-to-financing comparison of EV vs. ICE vehicle (electricity rate variation).</p>
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<p>Net difference in net monthly TNC income across financing-to-financing comparison of EV vs. ICE vehicle (purchase price deduction variation).</p>
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<p>Net difference in net monthly TNC income across financing-to-financing comparison of EV vs. ICE vehicle (annual incentive variation).</p>
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<p>Dominant vehicle acquisition pathways for EVs (<b>left</b>) and ICE vehicles (<b>right</b>).</p>
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<p>Net difference in monthly earnings between an EV and an ICE assuming dominant EV and ICE pathways.</p>
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24 pages, 399 KiB  
Review
Intelligent Monitoring Systems for Electric Vehicle Charging
by Jaime A. Martins and João M. F. Rodrigues
Appl. Sci. 2025, 15(5), 2741; https://doi.org/10.3390/app15052741 - 4 Mar 2025
Viewed by 311
Abstract
The growing adoption of electric vehicles (EVs) presents new challenges for managing parking infrastructure, particularly concerning charging station utilization and user behavior patterns. This review examines the current state-of-the-art in intelligent monitoring systems for EV charging stations in parking facilities. We specifically focus [...] Read more.
The growing adoption of electric vehicles (EVs) presents new challenges for managing parking infrastructure, particularly concerning charging station utilization and user behavior patterns. This review examines the current state-of-the-art in intelligent monitoring systems for EV charging stations in parking facilities. We specifically focus on two key inefficiencies: vehicles occupying charging spots beyond the optimal fast-charging range (80% state-of-charge) and remaining connected even after reaching full capacity (100%). We analyze the theoretical and practical foundations of these systems, summarizing existing research on intelligent monitoring architectures and commercial implementations. Building on this analysis, we also propose a novel monitoring framework that integrates Internet of things (IoT) sensors, edge computing, and cloud services to enable real-time monitoring, predictive maintenance, and adaptive control. This framework addresses both the technical aspects of monitoring systems and the behavioral factors influencing charging station management. Based on a comparative analysis and simulation studies, we propose performance benchmarks and outline critical research directions requiring further experimental validation. The proposed architecture aims to offer a scalable, adaptable, and secure solution for optimizing EV charging infrastructure utilization while addressing key research gaps in the field. Full article
(This article belongs to the Special Issue Feature Review Papers in "Computing and Artificial Intelligence")
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<p>System architecture overview of the intelligent EV charging monitoring system. Colors differentiate layers and their components. Solid lines indicate data flow, while dotted lines represent component relationships.</p>
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28 pages, 288 KiB  
Article
We Are Not One, We Are Legion—Secular State in Mexico, Local Dynamics of a Federal Issue
by Felipe Gaytan Alcala
Religions 2025, 16(3), 304; https://doi.org/10.3390/rel16030304 - 27 Feb 2025
Viewed by 173
Abstract
The management of laicity in Mexico, legally and politically, is a federal issue that involves regulating the activities of Churches and religious communities in the public space, in their practices, rituals, and relations with the organs of the state. However, in recent years, [...] Read more.
The management of laicity in Mexico, legally and politically, is a federal issue that involves regulating the activities of Churches and religious communities in the public space, in their practices, rituals, and relations with the organs of the state. However, in recent years, the growing presence and activity of Churches at the local level has called into question the need to observe how laicity is managed by subnational governments, both state and municipal. Are there mechanisms at the local level to regulate the presence of religion in the public space? How are religious traditions presented as culturally managed? What are the demands of Churches on local authorities and what is their political relationship with them? How is the demand for religious freedom resolved locally without violating citizens’ other freedoms, such as the freedom of conscience in issues such as education, health, traffic, and freedom of expression? All this has put into perspective whether laicity and the secular state should continue to be a national dimension or whether it is necessary to rethink legal and political forms at the local level, building new frameworks of governance and governability. This text reviews the public management of laicity in eight entities of the country, which in turn is representative of the rest of the entities with their local variations. However, they generally move in the constant dimensions of religious diversity, interreligious councils, offices, or those in charge of religious affairs, and levels of municipal participation. The construction of a new laicity is then proposed, which does not exclude religion from the public agenda but rather a new secular perspective on the participation of religious communities in public affairs. From a Latin American perspective, Mexico is seen as an effective government regime that separates religion from politics, restricting the participation of religious organizations in the public agenda. However, at the local level, this regime is changing with the inclusion of faith-based organizations in politics. This will undoubtedly lead to a change in the historical concept, a reference point in the region. The term management of laicity refers to the regulation and administration of governments (services, legal support, spaces, and dialogues) with religious communities. Management (control, regulation, permits, sanctions, and recognition) is defined by law and in public policy towards religion from the federal government, but not in local governments that lack clear regulatory frameworks, intervention guidelines, and support, hence the emphasis on the term. Full article
20 pages, 7453 KiB  
Article
Hydrogen Embrittlement of a T95 Low-Alloy Steel Charged by Electrochemical Method
by Luca Paterlini, Laura Vergani, Marco Ormellese, Arianna Curia, Giorgio Re and Fabio Bolzoni
Materials 2025, 18(5), 1047; https://doi.org/10.3390/ma18051047 - 27 Feb 2025
Viewed by 265
Abstract
The hydrogen embrittlement of a typical Oil Country Tubular Good (OCTG) steel, API 5CT T95, was investigated through electrochemical hydrogen pre-charging followed by mechanical testing. J-integral and tensile tests were performed on electrochemically pre-charged samples, with varying charging conditions to simulate different hydrogen [...] Read more.
The hydrogen embrittlement of a typical Oil Country Tubular Good (OCTG) steel, API 5CT T95, was investigated through electrochemical hydrogen pre-charging followed by mechanical testing. J-integral and tensile tests were performed on electrochemically pre-charged samples, with varying charging conditions to simulate different hydrogen environmental exposure. Hydrogen concentration profiles during the electrochemical hydrogen charging process and subsequent mechanical testing in air were calculated with the support of hydrogen permeation tests and Finite Elements Method (FEM) mass diffusion analysis. This approach enabled a deeper understanding of the actual impact of hydrogen on the assessed mechanical properties. The results were compared with tests performed in air and with data available in the literature and were critically analyzed and discussed. A toughness reduction of up to 60% was observed under the most severe charging conditions; however, the alloy retained good ductility with a critical stress intensity factor of 124 MPa√m, well above the minimum values required for pipelines in high-pressure hydrogen gas and sour service applications, 55 MPa√m and 30 MPa√m, respectively, as specified by current ASME Standard and EFC Guidelines. Tensile tests on pre-charged specimens exhibited certain limitations due to the rapid hydrogen desorption rate with respect to the time required to conduct proper slow strain-rate tests. Full article
(This article belongs to the Special Issue Corrosion and Mechanical Behavior of Metal Materials (3rd Edition))
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<p>API 5CT T95 steel. Microstructure, 5% Nital etching, Optical Microscope x500.</p>
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<p>API 5CT T95 steel. Microstructure on the three principal planes, Optical Microscope x200.</p>
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<p>Drawings of the cylindrical specimens for monotonic tensile tests (<b>left</b>) and SEB pre-cracked specimens for J-integral tests (<b>right</b>). Dimensions in mm.</p>
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<p>API 5CT T95 hydrogen permeation transients measured with Devanathan-Stachurski permeation cell. Time normalized with respect to thickness on X axis, normalized current density on Y axis.</p>
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<p>Preliminary hydrogen uptake tests, 0.5 mA/cm<sup>2</sup> and 5 mA/cm<sup>2</sup>. Samples dimension: 60 × 13 × 10 mm.</p>
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<p>Normalized hydrogen concentration during the electrochemical hydrogen charge and desorption phase, calculated with FEM analysis. The vertical black lines identify the tensile and SEB samples actual pre-charge duration and the onset of the desorption simulation. <span class="html-italic">D<sub>H</sub></span> = 5.9 × 10<sup>−11</sup> m<sup>2</sup>/s.</p>
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<p>Normalized hydrogen concentration in SEB and tensile samples exposed to electrochemical charge for 1 h, 6 h, 24 h, 48 h and 72 h. <span class="html-italic">D<sub>H</sub></span> = 5.9 × 10<sup>−11</sup> m<sup>2</sup>/s. The applied pre-charge durations are highlighted in red boxes.</p>
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<p>Normalized hydrogen concentration in SEB and tensile samples exposed, respectively, to 48 h and 24 h of electrochemical charge. Hydrogen concentration after 30′, 1 h, 2 h and 4 h desorption. <span class="html-italic">D<sub>H</sub></span> = 5.9 × 10<sup>−11</sup> m<sup>2</sup>/s.</p>
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<p><span class="html-italic">K<sub>Jc</sub></span> measured by three-point bending tests on uncharged samples and pre-charged samples with two different hydrogen contents. Horizontal grey line indicates the minimum <span class="html-italic">K<sub>Jc</sub></span> value required by ASME B31-12 [<a href="#B7-materials-18-01047" class="html-bibr">7</a>] for pipeline applications.</p>
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<p>Load-crack mouth displacement plots acquired during the J-integral testing of hydrogen charged samples; Uncharged condition, 0.4 ppm hydrogen concentration and 3.1 ppm hydrogen concentration.</p>
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<p>Fractographic analysis of cylindrical tensile samples: (<b>a</b>) uncharged sample, 100X; (<b>b</b>) charged sample, 100X; (<b>c</b>) dimples on uncharged sample, 1000X, (<b>d</b>) dimples on charged sample, 1000X.</p>
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<p>Fractographic analysis of uncharged SEB: (<b>a</b>) fatigue-tearing region interface, 200X; (<b>b</b>) tearing region, 500X; SEB, 0.4 ppm hydrogen: (<b>c</b>) fatigue-tearing region interface, 200X; (<b>d</b>) mixed ductile and quasi-cleavage region, 500X; SEB, 3.1 ppm hydrogen: (<b>e</b>) fatigue-tearing region interface, 200X; (<b>f</b>) prevalent quasi cleavage region, 500X. Red arrows highlight brittle quasi cleavage regions.</p>
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<p>Fractographic analysis of uncharged SEB: (<b>a</b>) fatigue-tearing region interface, 200X; (<b>b</b>) tearing region, 500X; SEB, 0.4 ppm hydrogen: (<b>c</b>) fatigue-tearing region interface, 200X; (<b>d</b>) mixed ductile and quasi-cleavage region, 500X; SEB, 3.1 ppm hydrogen: (<b>e</b>) fatigue-tearing region interface, 200X; (<b>f</b>) prevalent quasi cleavage region, 500X. Red arrows highlight brittle quasi cleavage regions.</p>
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24 pages, 2490 KiB  
Article
Combining MAMBA and Attention-Based Neural Network for Electric Ground-Handling Vehicles Scheduling
by Jiawei Li, Weigang Fu, Gangjin Huang, Kai Liu, Jiewei Zhang and Yaoming Fu
Systems 2025, 13(3), 155; https://doi.org/10.3390/systems13030155 - 26 Feb 2025
Viewed by 255
Abstract
To reduce airport operational costs and minimize environmental pollution, an increasing number of airports are transitioning from fuel-powered to electric ground-handling vehicles. However, the limited battery capacity of electric vehicles and the need for charging make the scheduling of these vehicles more complex. [...] Read more.
To reduce airport operational costs and minimize environmental pollution, an increasing number of airports are transitioning from fuel-powered to electric ground-handling vehicles. However, the limited battery capacity of electric vehicles and the need for charging make the scheduling of these vehicles more complex. To address this scheduling problem, this paper proposes an electric ground-handling vehicle scheduling algorithm that combines the MAMBA model with an attention-based neural network. The MAMBA model is designed to process multi-dimensional features such as flight information, vehicle locations, service demands, and time window constraints. Subsequently, an attention mechanism-based neural network is developed to dynamically integrate vehicle states, service records, and operational and charging constraints, in order to select the most suitable flights for electric ground-handling vehicles to service. The experiments use flight data from Xiamen Gaoqi International Airport and compare the proposed method with CPLEX solvers, existing heuristic algorithms, and custom heuristic algorithms. The results demonstrate that the proposed method not only effectively solves the electric ground-handling vehicle scheduling problem and provides high-quality solutions, but also exhibits good scalability in different parameter settings and real-time scheduling scenarios. Full article
(This article belongs to the Special Issue Scheduling and Optimization in Production and Transportation Systems)
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<p>The primary service processes of ground-handling vehicles.</p>
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<p>Electric ground-handling vehicles serving civil aircraft.</p>
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<p>Flowchart of the scheduling procedure.</p>
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<p>Main procedure of the algorithm training and solving.</p>
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<p>The architecture of the proposed scheduling algorithm.</p>
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<p>Comparison of Obj (total travel distance) and Gap (algorithmic performance deviation) among algorithms across flight numbers.</p>
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<p>Computational time analysis heatmap for different algorithms across flight numbers.</p>
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<p>Comparison of Obj (total travel distance) and Gap (algorithmic performance deviation) among algorithms across distributions.</p>
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<p>Computational time analysis heatmap for different algorithms across distributions.</p>
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18 pages, 3166 KiB  
Article
A Study on Analyzing Travel Characteristics of Micro Electric Vehicles by Using GPS Data
by Sunhoon Kim, Sooncheon Hwang and Dongmin Lee
Appl. Sci. 2025, 15(4), 2113; https://doi.org/10.3390/app15042113 - 17 Feb 2025
Viewed by 282
Abstract
A micro electric vehicle (micro-EV) is a small electric car with one or two seats designed for short-to-medium-distance trips. Micro-EVs produce relatively less pollution during operation and, due to their compact size, offer greater mobility in narrow areas compared to conventional transportation. These [...] Read more.
A micro electric vehicle (micro-EV) is a small electric car with one or two seats designed for short-to-medium-distance trips. Micro-EVs produce relatively less pollution during operation and, due to their compact size, offer greater mobility in narrow areas compared to conventional transportation. These advantages have led to a continuous increase in the number of micro-EVs. However, their small battery capacity results in a limited driving range per charge, and restrictions on power and speed lead to lower driving performance. Due to these drawbacks, micro-EVs still hold a small share of the overall vehicle market. Therefore, it is necessary to evaluate the strengths of micro-EVs and analyze how they should be utilized to promote their widespread adoption. Therefore, this study analyzed the strengths of micro-EVs and identified the types of services where they can be effectively utilized to promote the use of micro-EVs as a smart mobility option. This study focused on micro-EVs used as a shared transport service, delivery service, and in public service, as part of an R&D project on micro-EVs conducted by the Ministry of Trade, Industry, and Energy. A total of 106 micro-EVs were deployed for each service type: 57 for shared transport, 13 for delivery, and 36 for public service. Each micro-EV was equipped with a GPS device, and the analysis was conducted using GPS data collected from January 2021 to October 2021. Micro-EVs with missing data due to GPS device malfunctions were excluded from the analysis. As a result, two micro-EVs from the shared transport service and one from the public service were excluded. The study compared the travel characteristics of micro-EVs across the three different service types. Additionally, a comparative analysis of the driving characteristics of micro-EVs and conventional vehicles was conducted to assess the advantages of micro-EVs over traditional vehicles. The results of the analyses showed that micro-EVs were more utilized for the delivery service type than other service types in terms of daily usage time and travel distance (3.5 h/day and 38.5 km/day, respectively), trip amounts (24.1 trips/day), and number of trips per trip chain (9.4 trips/trip chain). Moreover, micro-EVs have their strengths compared to other modes of transportation when traveling narrow roads. Analysis of the roads around the areas where micro-EVs were located showed that the micro-EVs were exposed to narrow roads with a width of under 5 m (among the total road link extensions, 57% consisted of road links with a width of less than 5 m), especially the micro-EVs used for delivery service. It is expected that the findings of this study will serve as a foundational resource for developing strategies to promote the adoption of micro electric vehicles. Full article
(This article belongs to the Section Transportation and Future Mobility)
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<p>Example of collected micro-EV GPS data (delivery service).</p>
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<p>Concept of trip and trip chain classification.</p>
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<p>Experimental sites for driving performance comparison of micro-EVs and conventional vehicles.</p>
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<p>Travel behavior characteristics of micro-EVs used for each service type.</p>
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23 pages, 2398 KiB  
Article
Energy Saving in Permanent Cardiac Pacing: Pulse Waveform and Charge Balancing Deserve Consideration
by Franco Di Gregorio, Lina Marcantoni, Aldo Mozzi, Alberto Barbetta and Francesco Zanon
Bioengineering 2025, 12(2), 194; https://doi.org/10.3390/bioengineering12020194 - 17 Feb 2025
Viewed by 235
Abstract
The pacing pulse produced by implantable stimulators can be described as a truncated exponential decay from the starting peak amplitude, corresponding to the discharge of the output stage capacitance (reservoir and isolation capacitors, in series) along the application time. Pulse decay and charge [...] Read more.
The pacing pulse produced by implantable stimulators can be described as a truncated exponential decay from the starting peak amplitude, corresponding to the discharge of the output stage capacitance (reservoir and isolation capacitors, in series) along the application time. Pulse decay and charge balancing have relevant implications on the ideal setting of a pacing device, as demonstrated by mathematical predictions based on well-acknowledged theoretical statements. Successful stimulation is achieved with minimum energy expense at a pulse duration shorter than the chronaxie time, which represents the upper border of the advisable duration interval. With any start amplitude, the stimulation safety margin can be improved by a duration increase beyond the chronaxie only up to an absolute limit (longest useful duration), which depends on the chronaxie and the pulse time-constant. At the longest useful duration, the threshold start amplitude is at the minimum and cannot decrease any further, though it and the corresponding pulse mean amplitude largely exceed the rheobase. The overall pacing performance is affected, in addition, by the load resistance and the electrode capacitance. Pulse amplitude decay limits the effectiveness of extended duration in implantable stimulators, making short pulses preferable whenever possible. Proper pulse settings based on actual waveform properties can prevent energy waste and reduce pacing consumption, thus prolonging the service life of the stimulator. Full article
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Graphical abstract

Graphical abstract
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<p>Different outcomes in excitability assessment considering or ignoring the exponential pulse decay. The simulation assumes <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>I</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">A</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> <mo>=</mo> <mn>0.4</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">s</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>=</mo> <mn>500</mn> <mo> </mo> <mi mathvariant="normal">O</mi> <mi mathvariant="normal">h</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>o</mi> <mi>u</mi> <mi>t</mi> </mrow> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi mathvariant="normal">µ</mi> <mi mathvariant="normal">F</mi> </mrow> </semantics></math>. (<b>a</b>) Mean voltage of the threshold pulse as a function of pulse duration (Lapicque’s law, solid curve) and corresponding start voltage, derived from the exponential decay model (dashed curve). (<b>b</b>) Linear regression of threshold charge on duration based on the mean or the start pulse voltage (thick and light lines, respectively).</p>
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<p>Time-course of pulse voltage <math display="inline"><semantics> <mrow> <mfenced separators="|"> <mrow> <mi>V</mi> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mfenced> </mrow> </semantics></math> normalized to the start value <math display="inline"><semantics> <mrow> <mfenced separators="|"> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>p</mi> </mrow> </msub> </mrow> </mfenced> </mrow> </semantics></math> in an implantable pacemaker featuring 4 µF output capacitance and 500 or 400 Ohm load resistance (solid and dashed curves, respectively). The voltage declines exponentially during the stimulus at a rate that increases if the product of output capacitance and load resistance decreases. Though the amplitude ratio is positive, it must be pointed out that the pacing stimulus is actually a cathodal pulse (the tip electrode is negative with respect to either the ring electrode or the pacemaker case).</p>
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<p>Energy expense per cardiac cycle to pace at threshold in an implant with <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>I</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math> = 1 mA, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> = 0.4 ms, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>o</mi> <mi>u</mi> <mi>t</mi> </mrow> </msub> </mrow> </semantics></math> = 4 µF, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>a</mi> <mo>,</mo> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> = 5 µF, <math display="inline"><semantics> <mrow> <mi>R</mi> </mrow> </semantics></math> = 500 Ohm, considering the pulse energy alone (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>W</mi> </mrow> <mrow> <mi>p</mi> <mo>_</mo> <mi>t</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math>: dashed curve) or the total energy released to the load by spike emission and charge balancing (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>W</mi> </mrow> <mrow> <mi>l</mi> <mo>_</mo> <mi>t</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math>: solid curve). The latter is minimized at a pulse duration shorter than the chronaxie (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math>: vertical line).</p>
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<p>The same simulation as in <a href="#bioengineering-12-00194-f003" class="html-fig">Figure 3</a>, assuming a load resistance of either 500 Ohm (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> <mo>=</mo> <mn>0.5</mn> <mo> </mo> <mi mathvariant="normal">V</mi> <mo>;</mo> <mo> </mo> <mi>τ</mi> </mrow> </semantics></math> = 2 ms) or 400 Ohm (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> <mo>=</mo> <mn>0.4</mn> <mo> </mo> <mi mathvariant="normal">V</mi> <mo>;</mo> <mo> </mo> <mi>τ</mi> </mrow> </semantics></math> = 1.6 ms) and variable chronaxie. (<b>a</b>) The pulse duration implying minimum energy expense to pace at threshold, normalized to the chronaxie time, is plotted versus the chronaxie, considering the pulse energy alone (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>W</mi> </mrow> <mrow> <mi>p</mi> <mo>_</mo> <mi>t</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math>: open symbols) or the total energy released to the load per cardiac cycle (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>W</mi> </mrow> <mrow> <mi>l</mi> <mo>_</mo> <mi>t</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math>: full symbols). Both are minimized at a pulse duration shorter than the chronaxie, though the difference is much more prominent for the released energy. (<b>b</b>) Percent increase in energy released to the load to pace at threshold, if the pulse duration is set at the chronaxie instead of the optimal value.</p>
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<p>Same simulation as in <a href="#bioengineering-12-00194-f003" class="html-fig">Figure 3</a>, comparing the energy released to the load per cardiac cycle at threshold (th) and in the presence of a relative (1.25×) or additive safety margin (+0.2 V; +0.4 V). A relative margin increases the energy without affecting its relation with the pulse duration. In contrast, an additive margin progressively shortens the duration that entails minimum energy consumption, and shrinks the advisable duration range. The vertical dotted line indicates the chronaxie time (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math>).</p>
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<p>Effect of an additive safety margin (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>S</mi> </mrow> <mrow> <mi>a</mi> <mi>d</mi> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math>) on the energy released to the load. Same simulation as in <a href="#bioengineering-12-00194-f004" class="html-fig">Figure 4</a>, with 0.4 ms chronaxie (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math>). Threshold pacing is represented as <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>S</mi> </mrow> <mrow> <mi>a</mi> <mi>d</mi> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math> = 0. (<b>a</b>) Pulse duration minimizing the released energy (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mn>1</mn> <mo>_</mo> <mi>W</mi> <mi>m</mi> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math>), normalized to the chronaxie and plotted as a function of the additive safety margin. (<b>b</b>) Difference between the energy released to the load at the chronaxie and at the optimal duration reported in panel (<b>a</b>), expressed as percent of the minimum energy.</p>
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<p>Predictions referring to an implant with 0.4 V rheobase, 0.4 ms chronaxie, and 1.6 ms time-constant. (<b>a</b>) Threshold mean voltage as a function of pulse duration according to Lapicque (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>m</mi> <mo>_</mo> <mi>t</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math>: solid curve) compared with the mean voltage of decaying pulses with a start amplitude of 1.25 V (wide dashed curve), 1 V (narrow dashed curve), or 0.75 V (minimum threshold start amplitude, dotted curve). The vertical segments indicate the duration of maximum additive margin with 1.25 V or 1 V start amplitude. The highest vertical line indicates the longest useful duration, entailing maximum relative margin with any start amplitude. (<b>b</b>) Pulse duration required to reach the threshold (solid curve), or to pace with maximum relative or additive safety margin (dashed line and crosses, respectively), as a function of the ratio between start and rheobase voltage.</p>
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<p>Pulse decay implications on the threshold strength–duration curve in an implant featuring <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>I</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">A</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mi>c</mi> </mrow> </msub> <mo>=</mo> <mn>0.4</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">s</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>R</mi> <mo>=</mo> <mn>400</mn> <mo> </mo> <mi mathvariant="normal">O</mi> <mi mathvariant="normal">h</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>o</mi> <mi>u</mi> <mi>t</mi> </mrow> </msub> <mo>=</mo> <mn>4</mn> <mo> </mo> <mi mathvariant="normal">µ</mi> <mi mathvariant="normal">F</mi> </mrow> </semantics></math>. (<b>a</b>) The threshold mean voltage decreases as a function of pulse duration (thick solid curve), tending to the rheobase <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> <mo>=</mo> <mn>0.4</mn> <mo> </mo> <mi mathvariant="normal">V</mi> <mo>)</mo> </mrow> </semantics></math>. The corresponding start voltage (light solid curve) decreases with a lower slope and stops declining at a value much higher than the rheobase (0.75 V with 1.01 ms duration). Beyond this point, the actual threshold start amplitude is constant (dotted line). (<b>b</b>) The experimental relation between threshold charge and duration is linear and consistent with the assumed rheobase and chronaxie only in the duration range where the threshold start amplitude decreases (solid line).</p>
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<p>Effect of pulse decay on the threshold parameters in implants with time-constant of 1.6 or 2 ms (circles and crosses, respectively). (<b>a</b>) Longest useful pulse duration as a function of the chronaxie. Beyond this limit, the threshold start amplitude is independent of duration, and Lapicque’s law does not apply. (<b>b</b>) Lowest threshold start voltage (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>p</mi> <mo>_</mo> <mi>t</mi> <mi>h</mi> <mo>_</mo> <mi>m</mi> <mi>i</mi> <mi>n</mi> </mrow> </msub> </mrow> </semantics></math>) and corresponding mean voltage (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>m</mi> <mo>_</mo> <mi>t</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math>) at the longest useful duration, normalized to the rheobase and plotted as a function of the chronaxie.</p>
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<p>Effect of a change in load resistance (<math display="inline"><semantics> <mrow> <mi>R</mi> <mo>/</mo> <msub> <mrow> <mi>R</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math>) on the released energy (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>W</mi> </mrow> <mrow> <mi>l</mi> </mrow> </msub> <mo>/</mo> <msub> <mrow> <mi>W</mi> </mrow> <mrow> <mi>l</mi> <mo>_</mo> <mi>r</mi> <mi>e</mi> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math>), calculated by assuming that pulse mean current and duration are constant, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>a</mi> <mo>,</mo> <mi>c</mi> </mrow> </msub> </mrow> </semantics></math> = 5 µF, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>o</mi> <mi>u</mi> <mi>t</mi> </mrow> </msub> </mrow> </semantics></math> = 4 µF, and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>R</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math> = 500 Ohm (from which <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math> = 2 ms). The relation is virtually linear in the resistance range of ±30%, with slope decreasing for increasing ratio of pulse duration to reference time-constant (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> <mo>/</mo> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math>). The solid line represents a pulse duration approaching 0, featuring 1:1 correspondence between relative resistance and released energy. Dotted and dashed lines indicate, respectively, a pulse duration of 0.2 and 0.4 <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>t</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> <mo>/</mo> <msub> <mrow> <mi>τ</mi> </mrow> <mrow> <mi>r</mi> <mi>e</mi> <mi>f</mi> </mrow> </msub> </mrow> </semantics></math>. Since the pacing impedance is generally lower in unipolar than bipolar stimulation, the former is better suited to pacing energy reduction.</p>
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33 pages, 866 KiB  
Article
Secure Electric Vehicle Charging Infrastructure in Smart Cities: A Blockchain-Based Smart Contract Approach
by Abdullahi Chowdhury, Sakib Shahriar Shafin, Saleh Masum, Joarder Kamruzzaman and Shi Dong
Smart Cities 2025, 8(1), 33; https://doi.org/10.3390/smartcities8010033 - 15 Feb 2025
Viewed by 403
Abstract
Increasing adoption of electric vehicles (EVs) and the expansion of EV charging infrastructure present opportunities for enhancing sustainable transportation within smart cities. However, the interconnected nature of EV charging stations (EVCSs) exposes this infrastructure to various cyber threats, including false data injection, man-in-the-middle [...] Read more.
Increasing adoption of electric vehicles (EVs) and the expansion of EV charging infrastructure present opportunities for enhancing sustainable transportation within smart cities. However, the interconnected nature of EV charging stations (EVCSs) exposes this infrastructure to various cyber threats, including false data injection, man-in-the-middle attacks, malware intrusions, and denial of service attacks. Financial attacks, such as false billing and theft of credit card information, also pose significant risks to EV users. In this work, we propose a Hyperledger Fabric-based blockchain network for EVCSs to mitigate these risks. The proposed blockchain network utilizes smart contracts to manage key processes such as authentication, charging session management, and payment verification in a secure and decentralized manner. By detecting and mitigating malicious data tampering or unauthorized access, the blockchain system enhances the resilience of EVCS networks. A comparative analysis of pre- and post-implementation of the proposed blockchain network demonstrates how it thwarts current cyberattacks in the EVCS infrastructure. Our analyses include performance metrics using the benchmark Hyperledger Caliper test, which shows the proposed solution’s low latency for real-time operations and scalability to accommodate the growth of EV infrastructure. Deployment of this blockchain-enhanced security mechanism will increase user trust and reliability in EVCS systems. Full article
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<p>Cybersecurity threat targeting EVCS.</p>
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<p>Overview of key components in the blockchain-aided EV charging network.</p>
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<p>EVCS transactions using Hyperledger Fabric. EV = electric vehicle, EVSE = electric vehicle supply equipment, CM = charging management, CP = charging provider, BP = billing provider.</p>
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<p>Firmware update flow for electric vehicle supply equipment (EVSE).</p>
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<p>Comparison of average and maximum CPU and memory usage across different transaction volumes for Org1. (<b>a</b>) Average CPU and memory usage, (<b>b</b>) maximum CPU and memory usage.</p>
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18 pages, 2164 KiB  
Article
Comprehensive Investigation of the Durability of Lithium-Ion Batteries Under Frequency Regulation Conditions
by Yuxin Tian, Liye Wang, Chenglin Liao and Guifu Yan
Batteries 2025, 11(2), 75; https://doi.org/10.3390/batteries11020075 - 14 Feb 2025
Viewed by 275
Abstract
Due to the large-scale use of renewable energy generation and its lack of inertia, the frequency of the grid is extremely unstable. At the same time, with the vigorous development of new energy vehicles, large-scale power batteries have huge potential for renewable energy [...] Read more.
Due to the large-scale use of renewable energy generation and its lack of inertia, the frequency of the grid is extremely unstable. At the same time, with the vigorous development of new energy vehicles, large-scale power batteries have huge potential for renewable energy consumption. In this context, the Vehicle-to-Grid (V2G) method is proposed. Electric vehicles are used as energy storage systems to provide frequency regulation services as flexible power grid resources. However, when electric vehicles are invested in large-scale frequency regulation, their own power battery durability will also be affected. Based on this problem, the pseudo-two-dimensions (P2D) model of the battery was established in this paper, and the effects of temperature, state of charge (SOC), reported power, and frequency regulation conditions on battery capacity attenuation and negative potential distribution were explored through experiments and simulations. Full article
(This article belongs to the Special Issue Towards a Smarter Battery Management System: 2nd Edition)
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<p>Research framework.</p>
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<p>Battery internal structure diagram.</p>
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<p>P2D model in COMSOL.</p>
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<p>The superposition of different pulse conditions.</p>
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<p>The <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>K</mi> </mrow> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> </mrow> </semantics></math> of each level of the factor within first, second, and third rounds.</p>
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<p>Negative potential distribution results.</p>
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40 pages, 12596 KiB  
Review
A Review on the Additive Manufacturing of W-Cu Composites
by Muhammad Hussain, Bosheng Dong, Zhijun Qiu, Ulf Garbe, Zengxi Pan and Huijun Li
Metals 2025, 15(2), 197; https://doi.org/10.3390/met15020197 - 13 Feb 2025
Viewed by 475
Abstract
In recent years, W-Cu composite systems have become very interesting subjects due to good electrical and thermal conductivity, high-temperature strength, certain plasticity, and excellent radiation resistance. W-Cu composites are a very important class of materials in applications like PFM (plasma facing materials), functional [...] Read more.
In recent years, W-Cu composite systems have become very interesting subjects due to good electrical and thermal conductivity, high-temperature strength, certain plasticity, and excellent radiation resistance. W-Cu composites are a very important class of materials in applications like PFM (plasma facing materials), functional graded materials (FGM), electronic packaging materials, high-voltage electrical contacts, sweating materials, shaped charge liners, electromagnetic gun-rail materials, kinetic energy penetrators, and radiation shielding/protection. There is no possibility of forming a crystalline structure between these two materials. However, due to the unique properties these materials possess, they can be used by preparing them as a composite. Generally, W-Cu composites are prepared via the conventional powder metallurgy routes, i.e., sintering, hot pressing, hot isostatic pressing, isostatic cold pressing, sintering and infiltration, and microwave sintering. However, these processes have certain limitations, like the inability to produce bulk material, they are expensive, and their adoptability is limited. Here, in this review, we will discuss in detail the fabrication routes of additive manufacturing, and its current progress, challenges, trends, and associated properties obtained. We will also explain the challenges for the additive manufacturing of the composite. We will also compare W-Cu composites to other materials that can challenge them in terms of specific applications or service conditions. The solidification mechanism will be explained for W-Cu composites in additive manufacturing. Finally, we will conclude the progress of additive manufacturing of W-Cu composites to date and suggest future recommendations based on the current challenges in additive manufacturing. Full article
(This article belongs to the Section Welding and Joining)
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<p>Phase diagram of W and Cu. Reprinted with permission from Ref. [<a href="#B45-metals-15-00197" class="html-bibr">45</a>].</p>
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<p>Gibbs free energy vs. alloy composition, Reprinted with permission from Ref. [<a href="#B46-metals-15-00197" class="html-bibr">46</a>]. 1985, AIP Publishing.</p>
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<p>Formation enthalpy calculated vs. compositional ratios using MD simulations, reprinted with permission from ref. [<a href="#B48-metals-15-00197" class="html-bibr">48</a>], 2017, Elsevier.</p>
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<p>Surface energy of different materials studied in the research, reprinted from [<a href="#B49-metals-15-00197" class="html-bibr">49</a>].</p>
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<p>Surface energy of different transition metals and W (The dotted line shows results based on FCD-LMTO calculations), reprinted with permission from ref. [<a href="#B50-metals-15-00197" class="html-bibr">50</a>], 2018, Elsevier.</p>
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<p>Effect of nano-sized particles on the formation enthalpy for W50Cu50 system, reprinted from Ref. [<a href="#B47-metals-15-00197" class="html-bibr">47</a>].</p>
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<p>(<b>a</b>) Discontinuous FGM and (<b>b</b>) continuous FGM, (<b>c</b>–<b>e</b>) schematic diagrams showing discontinuous FGMs that contain interfaces with gradual change in composition, grain orientation and volume fractions of two types of second-phase particles, respectively. (<b>f</b>–<b>h</b>) schematic diagrams showing continuous FGMs in absence of interfaces and with gradual change in grain size, fiber orientation and volume fraction of second-phase particles. Reprinted with permission from Ref. [<a href="#B62-metals-15-00197" class="html-bibr">62</a>], 2019, Elsevier.</p>
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<p>Shift (red arrow) in Ductile-to-brittle transition temperature (DBTT) of W tested in cold-rolled, hot-rolled, and annealed conditions in LS and TS orientations. Reprinted with permission from Ref. [<a href="#B65-metals-15-00197" class="html-bibr">65</a>], 2016, Elsevier.</p>
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<p>Effect of Re addition on DBTT in W, reprinted with permission from Ref. [<a href="#B66-metals-15-00197" class="html-bibr">66</a>], 2018, Elsevier.</p>
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<p>Mechanistic models of heat and mass transfer and fluid flow in AM. reprinted with permission from Ref. [<a href="#B70-metals-15-00197" class="html-bibr">70</a>].</p>
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<p>(<b>a</b>) Infiltration method for W-Cu production. (<b>b</b>) W-Cu microstructure obtained, reprinted with permission from Ref. [<a href="#B25-metals-15-00197" class="html-bibr">25</a>], 2018, Elsevier.</p>
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<p>Liquid-phase sintering mechanism, reprinted with permission from Ref. [<a href="#B78-metals-15-00197" class="html-bibr">78</a>], 2009, Springer Nature.</p>
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<p>(<b>a</b>) Vacuum and (<b>b</b>) microwave heating (the intensity of color represents the heat energy), reprinted with permission from Ref. [<a href="#B82-metals-15-00197" class="html-bibr">82</a>], 2024, Wiley.</p>
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<p>Schematic of hot-pressing process, reprinted with permission from Ref. [<a href="#B60-metals-15-00197" class="html-bibr">60</a>], 2008, Elsevier.</p>
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<p>Spark plasma sintering setup and the heating mechanism, reprinted with permission from Ref. [<a href="#B82-metals-15-00197" class="html-bibr">82</a>], 2024, Wiley.</p>
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<p>Schematic of injection molding, reprinted with permission from Ref. [<a href="#B25-metals-15-00197" class="html-bibr">25</a>], 2018, Elsevier.</p>
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<p>Schematic of mechanical alloying: (<b>a</b>) process and (<b>b</b>) mechanism. Reprinted with permission from Ref. [<a href="#B92-metals-15-00197" class="html-bibr">92</a>], 2013, Elsevier.</p>
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<p>A schematic of fabrication of W-Cu composite using laser technology, reprinted with permission from Ref. [<a href="#B93-metals-15-00197" class="html-bibr">93</a>], 2020, Elsevier.</p>
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<p>W-Cu composite prepared by laser additive manufacturing technology with different scanning and laser-power levels, reprinted with permission from Ref. [<a href="#B94-metals-15-00197" class="html-bibr">94</a>], 2018, Elsevier.</p>
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<p>Schematic of electron beam melting, reprinted from Ref. [<a href="#B96-metals-15-00197" class="html-bibr">96</a>].</p>
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<p>SEM surface morphology of the W-(Ni)-Cu composites. (<b>a</b>) W-Cu40 wt.%; (<b>b</b>) W-Cu30 wt.%; (<b>c</b>) W-Cu25 wt.%; and (<b>d</b>) W-Ni5 wt.%–Cu15 wt.%, reprinted with permission from Ref. [<a href="#B42-metals-15-00197" class="html-bibr">42</a>], 2016, Elsevier.</p>
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<p>Surface SEM images of Cu-15W sample before and after HCPEB irradiation. (<b>a</b>) Initial, (<b>b</b>) 5 pulses, (<b>c</b>) 10 pulses, and (<b>d</b>) BSE image of 10-pulsed sample, reprinted with permission from Ref. [<a href="#B43-metals-15-00197" class="html-bibr">43</a>], 2018, Elsevier.</p>
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<p>Cross-sections of three-layer W–Cu cladding on a steel substrate: (<b>a</b>) one layer (75% W), (<b>b</b>) two layers (75% + 95% W), and (<b>c</b>) three layers (75% + 95% + 98% W), reprinted from Ref. [<a href="#B44-metals-15-00197" class="html-bibr">44</a>].</p>
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<p>Typical (<b>a</b>,<b>b</b>) microstructure and (<b>c</b>) XRD of W and Cu system, reprinted with permission from Ref. [<a href="#B19-metals-15-00197" class="html-bibr">19</a>], 2022, Elsevier.</p>
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<p>TEM observations at W/Cu interface: (<b>a</b>) HAADF image; (<b>b</b>) EDX line-scanning profile along the red arrow marked in (<b>a</b>); (<b>c</b>,<b>d</b>) element mapping; (<b>e</b>) HAADF image of the W/Cu interface; and (<b>f</b>) HR-TEM image of the interface, reprinted with permission from Ref. [<a href="#B151-metals-15-00197" class="html-bibr">151</a>], 2022, Elsevier.</p>
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<p>Colling rate on (<b>a</b>) Cu substrate; and (<b>b</b>) Cu, Al, and SS substrate, reprinted with permission from Ref. [<a href="#B172-metals-15-00197" class="html-bibr">172</a>], 1995, Elsevier.</p>
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<p>Schematic of laser welding and molten pool formation, reprinted from Ref. [<a href="#B178-metals-15-00197" class="html-bibr">178</a>].</p>
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<p>Schematic of electron beam melting, reprinted with permission from Ref. [<a href="#B179-metals-15-00197" class="html-bibr">179</a>], 2016, Elsevier.</p>
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<p>(<b>a</b>) Schematic of the welding principle, (<b>b</b>) Material states, fluid flow and four types of forces involved during the welding process, reprinted from Ref. [<a href="#B181-metals-15-00197" class="html-bibr">181</a>].</p>
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<p>The degree of undercooling explained (<b>a</b>) Hypocooling, (<b>b</b>) Critical undercooling, (<b>c</b>) Hypercooling, reprinted with permission from Ref. [<a href="#B185-metals-15-00197" class="html-bibr">185</a>], 2010, Springer.</p>
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<p>Geometrically necessary dislocations (GNDs) and statistically stored dislocations (SSDs), reprinted with permission from Ref. [<a href="#B187-metals-15-00197" class="html-bibr">187</a>], 2019, Elsevier.</p>
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<p>Solidification mechanism of W-Cu system explained in four steps, reprinted with permission from Ref. [<a href="#B19-metals-15-00197" class="html-bibr">19</a>], 2022, Elsevier.</p>
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16 pages, 2531 KiB  
Article
Modeling and Simulation of Electric Vehicles Charging Services by a Time Colored Petri Net Framework
by Agostino Marcello Mangini, Maria Pia Fanti, Bartolomeo Silvestri, Luigi Ranieri and Michele Roccotelli
Energies 2025, 18(4), 867; https://doi.org/10.3390/en18040867 - 12 Feb 2025
Viewed by 650
Abstract
The transport sector is responsible for about 60% of emissions in the atmosphere due to the exhaust-polluting gases of internal combustion engine (ICE) vehicles. An effective solution to this issue is the electrification of the transport means, which can significantly reduce pollution, especially [...] Read more.
The transport sector is responsible for about 60% of emissions in the atmosphere due to the exhaust-polluting gases of internal combustion engine (ICE) vehicles. An effective solution to this issue is the electrification of the transport means, which can significantly reduce pollution, especially in urban areas. Apart from the necessary technological advancements that must improve the battery performances, the diffusion of electric vehicles (EVs) must be further supported and facilitated by new dedicated services and tools for electric vehicle users and operators aiming at improving the travel and charging experience. To this goal, this paper proposes new models based on Timed Colored Petri Nets (TCPN) to simulate and manage the charge demand of the EV fleet. At first, the proposed tool must take into account the charging requests from different EV drivers with different charging need located in different geographical areas. This is possible by knowing input data such as EV current location, battery data, charge points (CPs) availability, and compatibility. In particular, EV drivers are simulated when finding and booking the preferred charge option according to the available infrastructure in the area of interest and the CPs tariff and power rate. The proposed TCPN is designed to model the multi-user charging demand in specific geographic areas, and it is evaluated in several scenarios of a case study to measure its performance in serving multiple EV users. Full article
(This article belongs to the Special Issue Smart Cities and the Need for Green Energy)
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<p>TCPN for Night and Day Cycle.</p>
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<p>Features Assignment and Sorting to the Correct Area.</p>
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<p>CP Selection.</p>
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<p>CP Management.</p>
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<p>Round Areas for CP Selection Example.</p>
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17 pages, 251 KiB  
Article
The Relationship of Socioeconomic Factors and Substance Abuse Treatment Dropout
by Wenyu Zhang and Hui Wu
Healthcare 2025, 13(4), 369; https://doi.org/10.3390/healthcare13040369 - 10 Feb 2025
Viewed by 647
Abstract
Background: Treatment dropout in substance use disorder (SUD) programs poses a significant challenge to achieving successful outcomes and leads to legal and financial issues. Socioeconomic factors have been identified as key contributors to treatment attrition; yet, the specific impact of patients’ socioeconomic [...] Read more.
Background: Treatment dropout in substance use disorder (SUD) programs poses a significant challenge to achieving successful outcomes and leads to legal and financial issues. Socioeconomic factors have been identified as key contributors to treatment attrition; yet, the specific impact of patients’ socioeconomic conditions remains underexplored. The purpose of this study is to examine the relationship between socioeconomic factors and SUD treatment dropout. Methods: We conducted a retrospective analysis of socioeconomic factors associated with treatment dropout among individuals with alcohol, marijuana, and heroin substance abuse. Logistic regression was used to examine the association between patients’ socioeconomic factors and treatment dropout. Adjusted odds ratios were calculated to quantify the strength of these associations. Results: Our findings demonstrate that demographic factors and financial status, including age (12–19 years), Black or African American race, and reliance on public assistance, correlate with an increased likelihood of treatment dropout. Black or African American patients receiving public assistance exhibit elevated dropout rates in ambulatory services, while patients of other single races without private insurance show higher dropout rates in detox services. Individuals aged 18–49 who are not part of the labor force have increased dropout rates in rehab services. Interestingly, patients in dependent living situations, who pay for services through private insurance or receive them at no charge, experience lower dropout rates as the number of arrests increases. Conversely, independently living patients with prior SUD treatments have higher dropout rates compared to those undergoing treatment for the first time. Conclusions: This study underscores the critical importance of addressing financial barriers to treatment access and retention in order to improve outcomes for individuals with substance use disorders (SUDs). Targeted interventions that support economically disadvantaged populations are essential for reducing treatment dropout rates and enhancing the effectiveness of SUD treatment programs. Full article
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<p>Correlation between gender and treatment dropout.</p>
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17 pages, 6367 KiB  
Article
Coordinated Frequency Control for Electric Vehicles and a Thermal Power Unit via an Improved Recurrent Neural Network
by Jianhua Zhang and Yongyue Wang
Energies 2025, 18(3), 533; https://doi.org/10.3390/en18030533 - 24 Jan 2025
Viewed by 418
Abstract
With the advancement of intelligent power generation and consumption technologies, an increasing number of renewable energy sources (RESs), smart loads, and electric vehicles (EVs) are being integrated into smart grids. This paper proposes a coordinated frequency control strategy for hybrid power systems with [...] Read more.
With the advancement of intelligent power generation and consumption technologies, an increasing number of renewable energy sources (RESs), smart loads, and electric vehicles (EVs) are being integrated into smart grids. This paper proposes a coordinated frequency control strategy for hybrid power systems with RESs, smart loads, EVs, and a thermal power unit (TPU), in which EVs and the TPU participate in short-term frequency regulation (FR) jointly. All EVs provide FR auxiliary services as controllable loads; specifically, the EV aggregations operate in charging mode when participating in FR. The proposed coordinated frequency control strategy is implemented by an improved recurrent neural network (IRNN), which combines a recurrent neural network with a functional-link layer. The weights and biases of the IRNN are trained by an improved backpropagation through time (BPTT) algorithm, in which a chaotic competitive swarm optimizer (CCSO) is proposed to optimize the learning rates. Finally, the simulation results verify the superiority of the coordinated frequency control strategy. Full article
(This article belongs to the Section E: Electric Vehicles)
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<p>Schematic view of EV-integrated hybrid power system.</p>
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<p>Equivalent battery model of EV.</p>
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<p>Coordinated frequency control strategy for EV aggregators and a TPU.</p>
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<p>General concept of CSO.</p>
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<p>The flow chart of the proposed CCSO.</p>
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<p>Distribution graph of chaotic maps.</p>
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<p>The system frequency response curve.</p>
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<p>Output power change of turbine under load disturbance.</p>
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<p>Output power change of EVs under load disturbance.</p>
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<p>Non-Gaussian disturbances from wind energy.</p>
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<p>Non-Gaussian disturbances from solar energy.</p>
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<p>System frequency response under non-Gaussian disturbances.</p>
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<p>PDF of the frequency deviation with the FLRNN + CCSO-based control strategy.</p>
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<p>Output power change of thermal turbine under non-Gaussian disturbances.</p>
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<p>Output power change of EVs under non-Gaussian disturbances.</p>
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23 pages, 2740 KiB  
Article
Comparative Study of ASTM C1202 and IBRACON/NT Build 492 Testing Methods for Assessing Chloride Ion Penetration in Concretes Using Different Types of Cement
by Wanderson Santos de Jesus, Suânia Fabiele Moitinho da Silva, Thalles Murilo Santos de Almeida, Marcelo Tramontin Souza, Eduarda Silva Leal, Ramon Santos Souza, Laio Andrade Sacramento, Ivan Bezerra Allaman and José Renato de Castro Pessôa
Buildings 2025, 15(3), 302; https://doi.org/10.3390/buildings15030302 - 21 Jan 2025
Viewed by 703
Abstract
Durability is crucial for reinforced concrete, directly influencing the service life of structures. The presence of aggressive agents, especially chloride ions, significantly impacts durability. This study investigates the differences between ASTM C1202 and IBRACON/NT Build 492 standards in concrete containing various types of [...] Read more.
Durability is crucial for reinforced concrete, directly influencing the service life of structures. The presence of aggressive agents, especially chloride ions, significantly impacts durability. This study investigates the differences between ASTM C1202 and IBRACON/NT Build 492 standards in concrete containing various types of cement designed for a characteristic compressive strength of 40 MPa. Forty-eight cylindrical samples were prepared using eight types of Portland cement, including those with blast furnace slag, filler, and pozzolanic materials. Chloride migration tests were performed according to the ASTM C1202/2022 and IBRACON/NT Build 492/1999 methodologies. At a 95% confidence level, the results indicated that concrete made with filler-containing cement (PCII F-SR and PC II F) showed the poorest chloride resistance, with charge passing values exceeding 4000 coulombs (ASTM C1202) and diffusion coefficients above 10 × 10−12 m2/s (IBRACON/NT Build 492). In contrast, concrete containing high slag cement (PC III-SR) and pozzolan cement (PC IV) demonstrated superior resistance to chloride penetration, with charge passing values below 1500 coulombs and diffusion coefficients under 5 × 10−12 m2/s. Notably, discrepancies in classification were observed, as PC II Z (fly-ash based) and PC II E-SR (slag-based) received different ratings under the two methods. ASTM C1202 was found to be more stringent than NT Build 492, highlighting significant variations in the classification criteria between these standards. Based on the findings, new interval values are proposed for classifying concrete regarding the risk of chloride ion penetration, particularly for the ASTM C1202 standard, in order to better align with performance-based durability criteria and improve classification accuracy. Full article
(This article belongs to the Section Building Materials, and Repair & Renovation)
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<p>Schematic illustrations of (<b>a</b>) sample cutting and selection and (<b>b</b>) apparatus for measuring chloride ion migration based on NT Build 492 method [<a href="#B5-buildings-15-00302" class="html-bibr">5</a>,<a href="#B12-buildings-15-00302" class="html-bibr">12</a>]. Adapted from Silva [<a href="#B26-buildings-15-00302" class="html-bibr">26</a>].</p>
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<p>Photograph highlighting the chloride migration test in progress.</p>
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<p>Photograph of a sample highlighting the measurement profile for determining the chloride penetration depth.</p>
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<p>Comparison of chloride penetration depth in different concrete groups: (<b>a</b>) concretes with slag-based cement, (<b>b</b>) concretes with fly ash-based cement, (<b>c</b>) concretes with filler-based cement, and (<b>d</b>) the average chloride penetration depth across all concretes.</p>
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<p>Comparison of Dns values between concretes according to the Scott–Knott test. Different lowercase letters indicate differences between treatments at a 5% significance level.</p>
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<p>Comparison of total charge passing values between concretes according to the Scott–Knott test. Different lowercase letters indicate differences between treatments at a 5% significance level.</p>
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<p>(<b>a</b>) Average Dns and the charge passed for all concrete samples, and (<b>b</b>) correlation between both techniques. The plot also includes risk classification based on limits of charge passed (ASTM C1202) and D<sub>ns</sub> (IBRACON/NT Build 492).</p>
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22 pages, 1818 KiB  
Article
Cooperative Service Caching and Task Offloading in Mobile Edge Computing: A Novel Hierarchical Reinforcement Learning Approach
by Tan Chen, Jiahao Ai, Xin Xiong and Guangwu Hu
Electronics 2025, 14(2), 380; https://doi.org/10.3390/electronics14020380 - 19 Jan 2025
Viewed by 694
Abstract
In the current mobile edge computing (MEC) system, the user dynamics, diversity of applications, and heterogeneity of services have made cooperative service caching and task offloading decision increasingly important. Service caching and task offloading have a naturally hierarchical structure, and thus, hierarchical reinforcement [...] Read more.
In the current mobile edge computing (MEC) system, the user dynamics, diversity of applications, and heterogeneity of services have made cooperative service caching and task offloading decision increasingly important. Service caching and task offloading have a naturally hierarchical structure, and thus, hierarchical reinforcement learning (HRL) can be used to effectively alleviate the dimensionality curse in it. However, traditional HRL algorithms are designed for short-term missions with sparse rewards, while existing HRL algorithms proposed for MEC lack delicate a coupling structure and perform poorly. This article introduces a novel HRL-based algorithm, named hierarchical service caching and task offloading (HSCTO), to solve the problem of the cooperative optimization of service caching and task offloading in MEC. The upper layer of HSCTO makes decisions on service caching while the lower layer is in charge of task offloading strategies. The upper-layer module learns policies by directly utilizing the rewards of the lower-layer agent, and the tightly coupled design guarantees algorithm performance. Furthermore, we adopt a fixed multiple time step method in the upper layer, which eliminates the dependence on the semi-Markov decision processes (SMDPs) theory and reduces the cost of frequent service replacement. We conducted numerical evaluations and the experimental results show that HSCTO improves the overall performance by 20%, and reduces the average energy consumption by 13% compared with competitive baselines. Full article
(This article belongs to the Special Issue Advanced Technologies in Edge Computing and Applications)
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<p>System model.</p>
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<p>Architecture of hierarchical reinforcement learning.</p>
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<p>Reward of service caching agent during training process.</p>
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<p>Rewards of task offloading agents during training process. (<b>a</b>–<b>c</b>) show the reward curves of the 3 agents respectively.</p>
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<p>Comparison of rewards with different <math display="inline"><semantics> <mi>η</mi> </semantics></math>.</p>
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<p>Comparison of average utility with a different <math display="inline"><semantics> <mi>η</mi> </semantics></math>.</p>
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<p>Comparison of the reward for different algorithms.</p>
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<p>Comparison of average utility for different algorithms.</p>
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