Nothing Special   »   [go: up one dir, main page]

You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (10,748)

Search Parameters:
Keywords = simulation tool

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
33 pages, 2287 KiB  
Article
Hydrodynamic Modelling Techniques for Bays and Estuaries: Simulation Methodology and Practical Application
by Alfonso Arrieta-Pastrana, Oscar E. Coronado-Hernández and Vicente S. Fuertes-Miquel
Water 2025, 17(5), 623; https://doi.org/10.3390/w17050623 (registering DOI) - 20 Feb 2025
Abstract
Some countries grapple with data scarcity for calibration purposes when establishing current hydrodynamic models, which often require many parameters. In this context, this research presents a practical simulation methodology for hydrodynamic modelling suitable for application in bay and estuarine systems based on mass [...] Read more.
Some countries grapple with data scarcity for calibration purposes when establishing current hydrodynamic models, which often require many parameters. In this context, this research presents a practical simulation methodology for hydrodynamic modelling suitable for application in bay and estuarine systems based on mass and momentum equations and requiring only one parameter for calibration—bed friction. The proposed simulation methodology is applied to a linear open channel measuring 200,000 m long. A sensitivity analysis of the bed friction is conducted to assess the proposed methodology’s response to the maximum water levels achieved. The results are compared to linear theory, indicating that the proposed simulation methodology effectively represents the water phase. In all simulations, the maximum root mean square error is less than 2.1% when neglecting bed friction and 4.69% when a bed friction of 0.005 is considered. The proposed simulation methodology can be a practical tool for hydrodynamic modelling in shallow waters. Full article
13 pages, 2157 KiB  
Article
Nonvolatile Organic Floating-Gate Memory Using N2200 as Charge-Trapping Layer
by Wenting Zhang, Junliang Shang, Shuang Li, Hu Liu, Mengqi Ma and Dongping Ma
Appl. Sci. 2025, 15(5), 2278; https://doi.org/10.3390/app15052278 - 20 Feb 2025
Abstract
In this work, floating-gate organic field-effect transistor memory using the n-type semiconductor poly-{[N,N′-bis(2-octyldodecyl) naphthalene-1,4,5,8-bis (dicarbo- ximide)-2,6-dili]-alt-5,5′-(2,2′-bithiophene)} (N2200) as a charge-trapping layer is presented. With the assistance of a technology computer-aided design (TCAD) tool (Silvaco-Atlas), the storage characteristics of the device are numerically simulated [...] Read more.
In this work, floating-gate organic field-effect transistor memory using the n-type semiconductor poly-{[N,N′-bis(2-octyldodecyl) naphthalene-1,4,5,8-bis (dicarbo- ximide)-2,6-dili]-alt-5,5′-(2,2′-bithiophene)} (N2200) as a charge-trapping layer is presented. With the assistance of a technology computer-aided design (TCAD) tool (Silvaco-Atlas), the storage characteristics of the device are numerically simulated by using the carrier injection and Fower–Nordheim (FN) tunneling models. The shift in the transfer characteristic curves and the charge-trapping mechanism after programming/erasing (P/E) operations under different P/E voltages and different pulse operation times are discussed. The impacts of different thicknesses of the tunneling layer on storage characteristics are also analyzed. The results show that the memory window with a tunneling layer thickness of 8 nm is 16.1 V under the P/E voltage of ±45 V, 5 s. After 1000 cycle tests, the memory shows good fatigue resistance, and the read current on/off ratio reaches 103. Full article
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of device structure.</p>
Full article ">Figure 2
<p>(<b>a</b>) Output characteristics and (<b>b</b>) transfer characteristics of N2200 FG-OFETM with tunneling layer of 8 nm.</p>
Full article ">Figure 3
<p>(<b>a</b>) Transfer characteristics after P/E operation, <span class="html-italic">V</span><sub>P/E</sub> = ±45 V, 5 s; (<b>b</b>) energy level diagram of N2200 FG-OFETM without application of voltage; (<b>c</b>) energy band diagram during P operation; (<b>d</b>) energy band diagram during E operation.</p>
Full article ">Figure 4
<p>(<b>a</b>) Memory windows of N2200 FG-OFETM with different thickness of tunneling layer; (<b>b</b>,<b>c</b>) memory windows with different P/E voltages (tunneling layer is 8 nm); (<b>d</b>) memory windows under <span class="html-italic">V</span><sub>P/E</sub> = ±45 V: operation times are 1 s, 5 s, 10 s, and 15 s, respectively.</p>
Full article ">Figure 4 Cont.
<p>(<b>a</b>) Memory windows of N2200 FG-OFETM with different thickness of tunneling layer; (<b>b</b>,<b>c</b>) memory windows with different P/E voltages (tunneling layer is 8 nm); (<b>d</b>) memory windows under <span class="html-italic">V</span><sub>P/E</sub> = ±45 V: operation times are 1 s, 5 s, 10 s, and 15 s, respectively.</p>
Full article ">Figure 5
<p>Changes in the test transfer characteristic curve at different temperatures. (<b>a</b>) Programming; (<b>b</b>) erasing.</p>
Full article ">Figure 6
<p>(<b>a</b>) PRER cycling test of N2200 FG-OFETM; (<b>b</b>) the drain currents of the ON state and OFF state after erasing and programming.</p>
Full article ">
20 pages, 85541 KiB  
Article
Fostering Inclusion: A Virtual Reality Experience to Raise Awareness of Dyslexia-Related Barriers in University Settings
by José Manuel Alcalde-Llergo, Pilar Aparicio-Martínez, Andrea Zingoni, Sara Pinzi and Enrique Yeguas-Bolívar
Electronics 2025, 14(5), 829; https://doi.org/10.3390/electronics14050829 - 20 Feb 2025
Abstract
This work introduces the design, implementation, and validation of a virtual reality (VR) experience aimed at promoting the inclusion of individuals with dyslexia in university settings. Unlike traditional awareness methods, this immersive approach offers a novel way to foster empathy by allowing participants [...] Read more.
This work introduces the design, implementation, and validation of a virtual reality (VR) experience aimed at promoting the inclusion of individuals with dyslexia in university settings. Unlike traditional awareness methods, this immersive approach offers a novel way to foster empathy by allowing participants to experience firsthand the challenges faced by students with dyslexia. Specifically, the experience raises awareness by exposing non-dyslexic individuals to the difficulties commonly encountered by dyslexic students. In the virtual environment, participants explore a virtual campus with multiple buildings, navigating between them while completing tasks and simultaneously encountering barriers that simulate some of the challenges faced by individuals with dyslexia. These barriers include reading signs with shifting letters, following directional arrows that may point incorrectly, and dealing with a lack of assistance. The campus is a comprehensive model featuring both indoor and outdoor spaces and supporting various modes of locomotion. To validate the experience, more than 30 non-dyslexic participants from the university environment, mainly professors and students, evaluated it through ad hoc satisfaction surveys. The results indicated heightened awareness of the barriers encountered by students with dyslexia, with participants deeming the experience a valuable tool for increasing visibility and fostering understanding of dyslexic students. Full article
(This article belongs to the Special Issue Virtual Reality Applications in Enhancing Human Lives)
Show Figures

Figure 1

Figure 1
<p>Maps.</p>
Full article ">Figure 2
<p>Different elements included in the virtual campus.</p>
Full article ">Figure 3
<p>Locomotion modes using the controllers. (<b>a</b>) Continuous locomotion. (<b>b</b>) Teleportation.</p>
Full article ">Figure 4
<p>Simulation of reading difficulties. (<b>a</b>) Letter movement. (<b>b</b>) Word swapping.</p>
Full article ">Figure 5
<p>Simulation of orientation barriers. (<b>a</b>) Scaled dimension of the virtual campus. (<b>b</b>) Help option providing right and wrong directions.</p>
Full article ">Figure 6
<p>(<b>a</b>) Campus render indicating the locations of the main stages of the experience. (<b>b</b>) Flow of experience stages. (<b>c</b>) Legend representing the different types of levels.</p>
Full article ">Figure 7
<p>Responses to the questions measuring the quality of the VR application. (<b>a</b>) Have you ever tried VR before the experience? (<b>b</b>) Did you experience nausea, loss of balance, or discomfort during the experience? (<b>c</b>) How much did the visual aspects of the environment engage you? (<b>d</b>) How compelling was your sense of moving around and interacting within the virtual environment?</p>
Full article ">Figure 8
<p>Responses to the questions measuring the effectiveness of the application in simulating barriers. (<b>a</b>) How challenging did you find navigating among the buildings? (<b>b</b>) How challenging did you find locating the classroom for the exam?</p>
Full article ">Figure 9
<p>Responses to the questions about participants’ dyslexia awareness. (<b>a</b>) How would you rate your understanding of dyslexia? (<b>b</b>) How useful do you consider the VR experience in raising awareness about dyslexia?</p>
Full article ">
26 pages, 1133 KiB  
Article
Adaptive CT XIGA Using LR B-Splines for Efficient Fracture Modeling
by Fei Gao, Cancan Ge, Zhuochao Tang, Jiming Gu and Rui Meng
Materials 2025, 18(5), 920; https://doi.org/10.3390/ma18050920 - 20 Feb 2025
Abstract
This paper presents a novel adaptive crack-tip extended isogeometric analysis (adaptive CT XIGA) framework based on locally refined B-splines (LR B-splines) for efficient and accurate fracture modeling in two-dimensional solids. The XIGA method facilitates crack modeling without requiring the specific locations of crack [...] Read more.
This paper presents a novel adaptive crack-tip extended isogeometric analysis (adaptive CT XIGA) framework based on locally refined B-splines (LR B-splines) for efficient and accurate fracture modeling in two-dimensional solids. The XIGA method facilitates crack modeling without requiring the specific locations of crack faces and enables crack propagation simulation without remeshing by employing localized enrichment functions. LR B-splines, as an advanced extension of B-splines and NURBS, offer high-order continuity, precise geometric representation, and local refinement capabilities, thereby enhancing computational accuracy and efficiency. Various local mesh refinement strategies, designed based on crack and crack-tip locations, are investigated. Among these strategies, the crack-tip topological refinement strategy is adopted for local refinement in the adaptive CT XIGA framework. Stress intensity factors (SIFs) are evaluated using the contour interaction integral technique, while the maximum circumferential stress criterion is adopted to predict the crack growth direction. Numerical examples demonstrate the accuracy, efficiency, and robustness of adaptive CT XIGA. The results confirm that the proposed framework achieves superior error convergence rates and significantly reduces computational costs compared to a-posteriori-error-based adaptive XIGA methods, particularly in crack propagation simulations. These advantages establish adaptive CT XIGA as a powerful and efficient tool for addressing complex fracture problems in solid mechanics. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Schematic representation of an infinite plate with a central crack under remote uniform tensile loading. (<b>b</b>) Initial computational mesh and control points. The blue dots represent the control points, while the red line depicts the crack. The red square symbols mark control points enriched with crack-tip enrichment functions, whereas the red cross symbols denote control points enriched with the Heaviside function.</p>
Full article ">Figure 2
<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT XIGA.</p>
Full article ">Figure 3
<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT2 XIGA.</p>
Full article ">Figure 4
<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT3 XIGA.</p>
Full article ">Figure 5
<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CTCF XIGA.</p>
Full article ">Figure 6
<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT2CF XIGA.</p>
Full article ">Figure 7
<p>Meshes at the first (<b>a</b>), second (<b>b</b>), and third (<b>c</b>) refinement steps obtained by adaptive CT3CF XIGA.</p>
Full article ">Figure 8
<p>Convergence of the relative error in the H1 norm as a function of the number of DOFs for adaptive XIGA using various refinement strategies.</p>
Full article ">Figure 9
<p>Convergence of the relative error in the energy norm as a function of the number of DOFs for adaptive XIGA using various refinement strategies.</p>
Full article ">Figure 10
<p>Comparison of computation times of adaptive XIGA using various refinement strategies.</p>
Full article ">Figure 11
<p>Schematic representation of a circular plate with a central crack subjected to a constant normal traction along the circumference.</p>
Full article ">Figure 12
<p>Initial computational mesh (<b>a</b>) and the meshes of local refinement at first (<b>b</b>), second (<b>c</b>), and third (<b>d</b>) steps in adaptive CT XIGA.</p>
Full article ">Figure 13
<p>Convergence of the relative error of the Mode-I SIF as a function of the number of DOFs.</p>
Full article ">Figure 14
<p>Comparison of computation times as a function of the number of refinement steps.</p>
Full article ">Figure 15
<p>Comparison of Mode-I SIFs for different crack lengths <math display="inline"><semantics> <mrow> <mn>2</mn> <mi>a</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 16
<p>Schematic representation of a square plate with a central curved crack under uniaxial tension.</p>
Full article ">Figure 17
<p>Initial computational mesh (<b>a</b>) and the meshes of local refinement at first (<b>b</b>), third (<b>c</b>), and fifth (<b>d</b>) steps in adaptive CT XIGA.</p>
Full article ">Figure 18
<p>Convergence of the mixed-mode SIFs as a function of the number of DOFs for the square plate with a center curved crack: <math display="inline"><semantics> <msub> <mi>K</mi> <mi>I</mi> </msub> </semantics></math> (<b>a</b>) and <math display="inline"><semantics> <msub> <mi>K</mi> <mrow> <mi>I</mi> <mi>I</mi> </mrow> </msub> </semantics></math> (<b>b</b>).</p>
Full article ">Figure 19
<p>Comparison of computation times as a function of the number of refinement steps.</p>
Full article ">Figure 20
<p>Comparison of the mixed-mode SIFs at different values of <math display="inline"><semantics> <mi>ω</mi> </semantics></math>: <math display="inline"><semantics> <msub> <mi>K</mi> <mi>I</mi> </msub> </semantics></math> (<b>a</b>) and <math display="inline"><semantics> <msub> <mi>K</mi> <mrow> <mi>I</mi> <mi>I</mi> </mrow> </msub> </semantics></math> (<b>b</b>).</p>
Full article ">Figure 21
<p>Schematic representation and loading conditions of a cantilever beam with an edge crack.</p>
Full article ">Figure 22
<p>The locally refined meshes of adaptive CT XIGA applying three local refinement steps for crack growth at step 0 (<b>a</b>), step 4 (<b>b</b>), step 7 (<b>c</b>), and step 9 (<b>d</b>).</p>
Full article ">Figure 23
<p>Comparison of crack growth paths of the cantilever beam with an edge crack.</p>
Full article ">Figure 24
<p>Comparison of computation times as a function of the number of crack growth steps.</p>
Full article ">Figure 25
<p>Schematic representation and loading conditions of a square plate with a center-inclined crack.</p>
Full article ">Figure 26
<p>The locally refined meshes of adaptive CT XIGA applying three local refinement steps for crack growth at step 0 (<b>a</b>), step 1 (<b>b</b>), and step 2 (<b>c</b>) when <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 27
<p>Comparison of crack growth paths of the square plate with a center-inclined crack when <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 28
<p>Comparison of computation times as a function of the number of crack growth steps.</p>
Full article ">Figure 29
<p>Crack growth paths of the center-inclined crack in the square plate by adaptive CT XIGA using three local refinement steps for different crack inclination angles.</p>
Full article ">Figure 30
<p>Schematic representation and loading conditions of a square plate with two edge cracks.</p>
Full article ">Figure 31
<p>The locally refined meshes of adaptive CT XIGA applying four local refinement steps for crack growth at step 0 (<b>a</b>), step 8 (<b>b</b>), and step 17 (<b>c</b>).</p>
Full article ">Figure 32
<p>Comparison of crack growth paths of the square plate with two edge cracks.</p>
Full article ">Figure 33
<p>Comparison of computation times as a function of the number of crack growth steps.</p>
Full article ">
16 pages, 2526 KiB  
Article
Network Architecture of a Fog–Cloud-Based Smart Farming System
by Alain Biheng, Chunling Tu, Pius Adewale Owolawi, Deon Du Plessis and Shengzhi Du
IoT 2025, 6(1), 17; https://doi.org/10.3390/iot6010017 - 20 Feb 2025
Abstract
With the rapid increase in the human population and urbanization worldwide, the demand for food production has played a significant role in driving the integration of technology into agriculture. Various Cloud-based systems, such as livestock tracking systems, have been proposed. In those systems, [...] Read more.
With the rapid increase in the human population and urbanization worldwide, the demand for food production has played a significant role in driving the integration of technology into agriculture. Various Cloud-based systems, such as livestock tracking systems, have been proposed. In those systems, data were collected by the sensors and sent to the Cloud for processing. However, significant issues with those systems were noted, such as high bandwidth utilization and security concerns, such as a high volume of row data traveling from the data collection devices (such as sensors) to the Cloud through the Internet. Additionally, the long distance between the Cloud and the data collection devices makes it unsuitable for latency-sensitive livestock disease monitoring and tracking systems. Therefore, this paper proposes a Fog–Cloud-based approach, where the processing is conducted at the Fog layer, closer to the data collection devices, and only the result is sent to the Cloud for remote viewing. The proposed method aims to reduce power consumption and latency in communication. To validate the proposed method, both the Cloud-based and Fog–Cloud-based scenarios are simulated using iFogSim (a novel simulation tool for IoT and Cloud computing), and the result shows that there is less than twice the power consumption in some scenarios and that the time consumed in the proposed Fog–Cloud-based system, depending on the number of sensors, is five to ten times lower. This study further supports the point that the Fog–Cloud-based is suitable for latency-dependent farming systems such as livestock tracking systems. Full article
Show Figures

Figure 1

Figure 1
<p>Structure of the proposed Fog–Cloud-based livestock farming system.</p>
Full article ">Figure 2
<p>Basic structure of a data collection module.</p>
Full article ">Figure 3
<p>Signal flow graph of the proposed system.</p>
Full article ">Figure 4
<p>Cloud-based design.</p>
Full article ">Figure 5
<p>Fog–Cloud-based design.</p>
Full article ">Figure 6
<p>Cloud-based and Fog–Cloud-based overall system delay.</p>
Full article ">Figure 7
<p>Cloud-based and Fog–Cloud-based energy consumption.</p>
Full article ">
18 pages, 2368 KiB  
Article
Design of a Remanufacturing Line Applying Lean Manufacturing and Supply Chain Strategies
by Rosa Hilda Félix-Jácquez, Óscar Hernández-Uribe, Leonor Adriana Cárdenas-Robledo and Zaida Antonieta Mora-Alvarez
Logistics 2025, 9(1), 33; https://doi.org/10.3390/logistics9010033 - 20 Feb 2025
Abstract
Background: Remanufacturing products for sustainability involves layout and production planning, tools and equipment, material arrangement and handling, inventory management, technology integration, and more. This study presents an empirical vision through a discrete event simulation (DES) model integrating lean manufacturing (LM) and supply [...] Read more.
Background: Remanufacturing products for sustainability involves layout and production planning, tools and equipment, material arrangement and handling, inventory management, technology integration, and more. This study presents an empirical vision through a discrete event simulation (DES) model integrating lean manufacturing (LM) and supply chain (SC) strategies with industry 4.0 (I4.0) technologies, applied to a case in a railway company. Methods: The work presents scenarios following a methodology with an incremental approach to implement strategies of lean manufacturing (LM) and supply chain (SC) in the context of I4.0 and their effects represented in DES models with applicability in remanufacturing and production line management. Five simulation scenarios were analyzed according to strategies layered incrementally. Results: Behaviors and outcomes were compared across the scenarios considering the remanufactured engines, percentage of process time, human labor occupation, and the statistical analysis of the process capability. Scenario five achieved the objective of remanufacturing 40 engines in one year with a cycle time of 214.45 h. Conclusions: The purpose was to design an engine remanufacturing line incorporating LM and SC strategies via a DES model, highlighting the importance of their gradual adoption toward I4.0 implementation. The integration of previous strategies improves flexibility and productivity in manufacturing processes. Full article
Show Figures

Figure 1

Figure 1
<p>Description of the research methodology.</p>
Full article ">Figure 2
<p>Flow chart remanufacturing process.</p>
Full article ">Figure 3
<p>Object flow diagram of the remanufacturing line.</p>
Full article ">Figure 4
<p>Scenario 5 with the LM, SC, and I4.0 strategies integrated.</p>
Full article ">Figure 5
<p>Percentage of the human labor occupation by scenario.</p>
Full article ">Figure 6
<p>Process capability by scenario: (<b>a</b>) Scenario 1; (<b>b</b>) Scenario 2; (<b>c</b>) Scenario 3; (<b>d</b>) Scenario 4; (<b>e</b>) Scenario 5.</p>
Full article ">Figure 6 Cont.
<p>Process capability by scenario: (<b>a</b>) Scenario 1; (<b>b</b>) Scenario 2; (<b>c</b>) Scenario 3; (<b>d</b>) Scenario 4; (<b>e</b>) Scenario 5.</p>
Full article ">
16 pages, 14946 KiB  
Article
Ocean Target Electric Field Signal Analysis and Detection Using LOFAR Based on Basis Pursuit
by Huiwen Hu, Xuepeng Sun, Guocheng Wang and Lintao Liu
J. Mar. Sci. Eng. 2025, 13(2), 387; https://doi.org/10.3390/jmse13020387 - 19 Feb 2025
Abstract
An ocean target electric field signal is an effective approach for analyzing the ocean environment and is widely used for detecting ocean targets, extracting their features, and tracking them. Low-frequency analysis and recording (LOFAR) is a commonly used time–frequency analysis tool that provides [...] Read more.
An ocean target electric field signal is an effective approach for analyzing the ocean environment and is widely used for detecting ocean targets, extracting their features, and tracking them. Low-frequency analysis and recording (LOFAR) is a commonly used time–frequency analysis tool that provides the time–frequency spectrum of a signal; however, its reliance on the Fourier transform (FT) results in a low frequency resolution and signal-to-noise ratio (SNR), which limits its target detection capabilities. To address this problem, we propose a method called low-frequency analysis and recording based on basis pursuit (LOFAR-BP) for analyzing and detecting ocean target electric field signals. LOFAR-BP uses basis pursuit (BP) with the L1 norm for frequency analysis, whereas LOFAR utilizes the FT. We demonstrate that the FT is the L2 norm mathematically. LOFAR-BP generates the time–frequency spectrum in the same way that LOFAR does. By extracting characteristic values from the time–frequency spectrum, targets can be detected using an appropriate threshold. Both simulation and ocean experiments showed that LOFAR-BP effectively enhances target signals and suppresses noise. Compared with LOFAR, LOFAR-BP improved the frequency resolution by 60% in both experiments and increased the SNR by 54.82 dB in the simulation experiment and by 39.59 dB in the ocean experiment. When applied to target detection, LOFAR-BP can detect targets 6 s earlier than LOFAR can. Full article
(This article belongs to the Section Ocean Engineering)
Show Figures

Figure 1

Figure 1
<p>Steps of LOFAR and LOFAR-BP.</p>
Full article ">Figure 2
<p>Simulated signal.</p>
Full article ">Figure 3
<p>Time–frequency spectra of simulated signal. (<b>a</b>) LOFAR. (<b>b</b>) LOFAR-BP.</p>
Full article ">Figure 4
<p>Frequency spectrum.</p>
Full article ">Figure 5
<p>Frequency resolution of simulated signal.</p>
Full article ">Figure 6
<p>Electric field signal.</p>
Full article ">Figure 7
<p>Time–frequency spectra of electric field signal. (<b>a</b>) LOFAR. (<b>b</b>) LOFAR-BP.</p>
Full article ">Figure 8
<p>Frequency resolution of electric field signal.</p>
Full article ">Figure 9
<p>Characteristic value.</p>
Full article ">Figure 10
<p>Detection result.</p>
Full article ">
24 pages, 8996 KiB  
Article
Design of a Three-Input, Single-Output DC–DC Converter for Electric Charging Station
by Sivaram Natarajan Vijayanathan, Lavanya Anbazhagan, Jagabar Sathik Mohamed Ali, Divya Navamani Jayachandran, Pradeep Vishnuram, CH. Naga Sai Kalyan, Mustafa Abdullah and Rajkumar Singh Rathore
Energies 2025, 18(4), 1005; https://doi.org/10.3390/en18041005 - 19 Feb 2025
Abstract
This article presents a novel four-port DC–DC converter designed to integrate photovoltaics, fuel cells, and supercapacitors with one DC charging single-output port with a reduced component count. The proposed converter ensures an efficient power management strategy to manage the load power demand and [...] Read more.
This article presents a novel four-port DC–DC converter designed to integrate photovoltaics, fuel cells, and supercapacitors with one DC charging single-output port with a reduced component count. The proposed converter ensures an efficient power management strategy to manage the load power demand and optimize the power flow from the sources. The power management controller helps enhance the performance of the system by dynamically prioritizing the sources based on their availability and the demand of the load. A comprehensive reliability analysis is conducted to measure the converter’s robustness under varying load conditions, proving its suitability for real-world applications. The proposed topology’s performance was validated in three different scenarios for 1 kW using a simulation tool, and experiments in the laboratory were conducted. The failure rate and efficiency of the system are analyzed, and the converter promises a 96.5% efficiency for 1 kW and a failure rate of 4.6216 × 106 failures per hour. The simulation and experimental results validate the converter’s performance, highlighting its superior efficiency, reliability, and scalability. Full article
Show Figures

Figure 1

Figure 1
<p>The model and characteristics of PV.</p>
Full article ">Figure 2
<p>Model and characteristics of PEM fuel cell.</p>
Full article ">Figure 3
<p>Model of supercapacitor.</p>
Full article ">Figure 4
<p>Proposed topology.</p>
Full article ">Figure 5
<p>Different scenarios and modes of operation: (<b>a</b>) Mode 1, (<b>b</b>) Mode 2, (<b>c</b>) Mode 3, (<b>d</b>) Mode 4, (<b>e</b>) Mode 5, (<b>f</b>) Mode (6).</p>
Full article ">Figure 6
<p>Predicted waveform for the proposed configuration.</p>
Full article ">Figure 7
<p>Proposed EMCS Flowchart of CS.</p>
Full article ">Figure 8
<p>Detailed schematic of PV–FC–SC fed charging station.</p>
Full article ">Figure 9
<p>Simulation waveform for the proposed topology during Scenario 1.</p>
Full article ">Figure 10
<p>Simulation waveform for the proposed topology during Scenario 2.</p>
Full article ">Figure 11
<p>Simulation waveform for the proposed topology during Scenario 3.</p>
Full article ">Figure 12
<p>Simulation waveform for the supercapacitor: (<b>a</b>) % SOC, (<b>b</b>) supercapacitor current, (<b>c</b>) supercapacitor voltage, (<b>d</b>) DC link voltage Vdc, (<b>e</b>) DC link current Idc.</p>
Full article ">Figure 13
<p>Experimental setup of proposed topology.</p>
Full article ">Figure 14
<p>Voltage, current, and switching pulse waveforms for Scenario 1.</p>
Full article ">Figure 15
<p>Voltage, current, and switching pulse waveforms for Scenario 2.</p>
Full article ">Figure 16
<p>Voltage, current, and switching pulse waveforms for Scenario 3.</p>
Full article ">Figure 17
<p>Comparison of efficiency between theoretical and measured values.</p>
Full article ">Figure 18
<p>Failure rate during Scenario 1 for (<b>a</b>) switch S<sub>A</sub>, (<b>b</b>) diode D<sub>A</sub>, (<b>c</b>) inductor L<sub>A</sub>, and (<b>d</b>) capacitor C<sub>A</sub>.</p>
Full article ">Figure 19
<p>Failure rate during Scenario 2 for (<b>a</b>) switch S<sub>B</sub>, (<b>b</b>) inductor L<sub>B</sub>, (<b>c</b>) diode D<sub>B</sub>, (<b>d</b>) diode D<sub>D</sub>, (<b>e</b>) capacitor C<sub>A</sub>, and (<b>f</b>) capacitor C<sub>B</sub>.</p>
Full article ">Figure 20
<p>Failure rate during Scenario 3 for (<b>a</b>) switch S<sub>A</sub>, (<b>b</b>) switch S<sub>B</sub>, (<b>c</b>) diode D<sub>B</sub>, (<b>d</b>) diode D<sub>C</sub>, (<b>e</b>) inductor L<sub>A</sub>, (<b>f</b>) inductor L<sub>A</sub>, (<b>g</b>) capacitor C<sub>A</sub>, and (<b>h</b>) capacitor C<sub>B</sub>.</p>
Full article ">Figure 21
<p>Reliability curve of all three scenarios.</p>
Full article ">
18 pages, 17324 KiB  
Article
Design and Performance Testing Analysis of Underground Electromagnetic Coupling Electro-Hydraulic Signal Wet Joint Scheme
by Min Wen, Renjun Xie, Hao Qiu, Yanfeng Cao, Zening Hou, Zhiyuan Qi, Hao Pan, Hui Huang and Gang Bi
Processes 2025, 13(2), 592; https://doi.org/10.3390/pr13020592 - 19 Feb 2025
Abstract
The electro-hydraulic composite intelligent completion technology is one of the most effective ways to solve the efficient development of oil and gas. The development of an electro-hydraulic composite wet joint tool that is compatible with the electro-hydraulic composite intelligent completion system can achieve [...] Read more.
The electro-hydraulic composite intelligent completion technology is one of the most effective ways to solve the efficient development of oil and gas. The development of an electro-hydraulic composite wet joint tool that is compatible with the electro-hydraulic composite intelligent completion system can achieve intelligent control between the upper and lower pipe columns of deepwater oil and gas wells and the pluggable transmission of monitoring signals. This article proposes a new type of electromagnetic coupling electro-hydraulic composite wet joint designed to address the defects of friction damage and poor contact in current wet joint direct contact power transmission. The joint uses claw docking and wireless energy transmission to achieve the composite transmission of hydraulic and electric power. Firstly, we independently designed a DC power supply inverter circuit, rectification circuit, and wireless power transmission coil assembly to form a wireless power transmission system. We also conducted testing and analysis on the wireless power transmission efficiency, which exceeded 60%. When the input voltage was above 80 V, the output power was greater than 60 W, meeting the design requirements. Secondly, the mechanical structure of the new electro-hydraulic signal wet joint tool was optimized and its strength was verified. The simulation results showed that the maximum stress was 891.8 MPa, and the maximum deformation of the wet joint docking overall structure was 0.123 mm. The strength and deformation met the design requirements. The hydraulic and electrical connectivity indoor tests were conducted on the electromagnetic coupling wet joint, and all aspects of transmission were normal, thus forming a design scheme for the underground electromagnetic coupling electro-hydraulic signal wet joint. The wireless transmission type electro-hydraulic signal wet joint designed in this article is of great significance for accelerating the promotion and application process of deepwater intelligent completion systems. Full article
(This article belongs to the Section Automation Control Systems)
Show Figures

Figure 1

Figure 1
<p>Working principle of electromagnetic induction wireless power transmission.</p>
Full article ">Figure 2
<p>Schematic diagram of inverter circuit.</p>
Full article ">Figure 3
<p>Principles of circuit design.</p>
Full article ">Figure 4
<p>Schematic diagram of rectification circuit.</p>
Full article ">Figure 5
<p>Fourth-generation wireless power transmission coil assembly.</p>
Full article ">Figure 6
<p>Wireless signal transmission experiment process (medium: air).</p>
Full article ">Figure 7
<p>Wireless signal transmission experiment process (medium: 5 wt% NaCl).</p>
Full article ">Figure 8
<p>Wireless signal transmission oscilloscope (medium: drilling fluid).</p>
Full article ">Figure 9
<p>Wireless signal transmission experiment process (medium: rock debris + sand).</p>
Full article ">Figure 10
<p>Schematic diagram of wet joint female head structure.</p>
Full article ">Figure 11
<p>Schematic diagram of wet joint male structure.</p>
Full article ">Figure 12
<p>Wet joint docking assembly.</p>
Full article ">Figure 13
<p>Electro-hydraulic composite wet joint locking and disengagement mechanism.</p>
Full article ">Figure 14
<p>Electric hydraulic signal wet joint power transmission structure.</p>
Full article ">Figure 15
<p>Electro-hydraulic composite wet joint hydraulic transmission structure.</p>
Full article ">Figure 16
<p>Simulation results of single load and composite load on the upper shell.</p>
Full article ">Figure 17
<p>Simulation results of single load and composite load on the lower shell.</p>
Full article ">Figure 18
<p>Simulation results of single load and composite load on valve core.</p>
Full article ">Figure 19
<p>Simulation results of single load and composite load of claw.</p>
Full article ">Figure 20
<p>Hydraulic transmission test in air and saltwater wet environments. (<b>a</b>) Hydraulic transmission test in air; (<b>b</b>) Hydraulic transmission test in saltwater wet environment.</p>
Full article ">Figure 21
<p>Electricity and signal transmission testing in humid environments with air and salt water. (<b>a</b>) Testing of electrical energy and signal transmission in the air; (<b>b</b>) Salt water wet environment electrical energy and signal transmission testing.</p>
Full article ">Figure 22
<p>Sealing test of wet joint local prototype.</p>
Full article ">
20 pages, 1619 KiB  
Systematic Review
A Breakthrough in Producing Personalized Solutions for Rehabilitation and Physiotherapy Thanks to the Introduction of AI to Additive Manufacturing
by Emilia Mikołajewska, Dariusz Mikołajewski, Tadeusz Mikołajczyk and Tomasz Paczkowski
Appl. Sci. 2025, 15(4), 2219; https://doi.org/10.3390/app15042219 - 19 Feb 2025
Abstract
The integration of artificial intelligence (AI) with additive manufacturing (AM) is driving breakthroughs in personalized rehabilitation and physical therapy solutions, enabling precise customization to individual patient needs. This article presents the current state of knowledge and perspectives of using personalized solutions for rehabilitation [...] Read more.
The integration of artificial intelligence (AI) with additive manufacturing (AM) is driving breakthroughs in personalized rehabilitation and physical therapy solutions, enabling precise customization to individual patient needs. This article presents the current state of knowledge and perspectives of using personalized solutions for rehabilitation and physiotherapy thanks to the introduction of AI to AM. Advanced AI algorithms analyze patient-specific data such as body scans, movement patterns, and medical history to design customized assistive devices, orthoses, and prosthetics. This synergy enables the rapid prototyping and production of highly optimized solutions, improving comfort, functionality, and therapeutic outcomes. Machine learning (ML) models further streamline the process by anticipating biomechanical needs and adapting designs based on feedback, providing iterative refinement. Cutting-edge techniques leverage generative design and topology optimization to create lightweight yet durable structures that are ideally suited to the patient’s anatomy and rehabilitation goals .AI-based AM also facilitates the production of multi-material devices that combine flexibility, strength, and sensory capabilities, enabling improved monitoring and support during physical therapy. New perspectives include integrating smart sensors with printed devices, enabling real-time data collection and feedback loops for adaptive therapy. Additionally, these solutions are becoming increasingly accessible as AM technology lowers costs and improves, democratizing personalized healthcare. Future advances could lead to the widespread use of digital twins for the real-time simulation and customization of rehabilitation devices before production. AI-based virtual reality (VR) and augmented reality (AR) tools are also expected to combine with AM to provide immersive, patient-specific training environments along with physical aids. Collaborative platforms based on federated learning can enable healthcare providers and researchers to securely share AI insights, accelerating innovation. However, challenges such as regulatory approval, data security, and ensuring equity in access to these technologies must be addressed to fully realize their potential. One of the major gaps is the lack of large, diverse datasets to train AI models, which limits their ability to design solutions that span different demographics and conditions. Integration of AI–AM systems into personalized rehabilitation and physical therapy should focus on improving data collection and processing techniques. Full article
(This article belongs to the Special Issue Additive Manufacturing in Material Processing)
Show Figures

Figure 1

Figure 1
<p>PRISMA flow diagram of the review process.</p>
Full article ">Figure 2
<p>Basic results of the review: (<b>a</b>) by year, (<b>b</b>) by discipline.</p>
Full article ">Figure 3
<p>The most common current use of AI-supported AM in rehabilitation and physiotherapy (authors’ own elaboration).</p>
Full article ">Figure 4
<p>Possible future customization of AI–supported 3D printed assistive technologies in rehabilitation and physiotherapy (authors’ own elaboration).</p>
Full article ">
25 pages, 3614 KiB  
Review
Challenges and Opportunities for Aquifer Thermal Energy Storage (ATES) in EU Energy Transition Efforts—An Overview
by Katarina Marojević, Tomislav Kurevija and Marija Macenić
Energies 2025, 18(4), 1001; https://doi.org/10.3390/en18041001 - 19 Feb 2025
Abstract
Aquifer Thermal Energy Storage (ATES) systems are a promising solution for sustainable energy storage, leveraging underground aquifers to store and retrieve thermal energy for heating and cooling. As the global energy sector faces rising energy demands, climate change, and the depletion of fossil [...] Read more.
Aquifer Thermal Energy Storage (ATES) systems are a promising solution for sustainable energy storage, leveraging underground aquifers to store and retrieve thermal energy for heating and cooling. As the global energy sector faces rising energy demands, climate change, and the depletion of fossil fuels, transitioning to renewable energy sources is imperative. ATES systems contribute to these efforts by reducing greenhouse gas (GHG) emissions and improving energy efficiency. This review uses the PRISMA (Preferred Reporting Items for Systematic Reviews and Meta-Analysis) methodology as a systematic approach to collect and analyze relevant literature. It highlights trends, gaps, and advancements in ATES systems, focusing on simulation methods, environmental impacts, and economic feasibility. Tools like MODFLOW, FEFLOW, and COMSOL Multiphysics are emphasized for optimizing design and system performance. Europe is identified as a continent with the most favorable predispositions for ATES implementation due to its diverse and abundant aquifer systems, strong policy frameworks supporting renewable energy, and advancements in subsurface energy technologies. Full article
(This article belongs to the Special Issue Development and Utilization in Geothermal Energy)
Show Figures

Figure 1

Figure 1
<p>A schematic representation of ATES operation (adapted from Bloemendal et al. [<a href="#B7-energies-18-01001" class="html-bibr">7</a>]).</p>
Full article ">Figure 2
<p>Prisma flow diagram.</p>
Full article ">Figure 3
<p>Number of articles uploaded per year.</p>
Full article ">Figure 4
<p>Number of articles per country.</p>
Full article ">Figure 5
<p>Locations of ATES systems from <a href="#energies-18-01001-t007" class="html-table">Table 7</a>.</p>
Full article ">
26 pages, 9359 KiB  
Article
Experimental and Numerical Analyses of the Influence of Al2O3 Nanoparticle Supplementation in Biodiesel (Water Hyacinth) Blends with Diesel on CI Engine Responses
by Ameer Hasan Hamzah, Abdulrazzak Akroot and Hasanain A. Abdul Wahhab
Appl. Sci. 2025, 15(4), 2204; https://doi.org/10.3390/app15042204 - 19 Feb 2025
Abstract
The current work includes experimental and numerical investigations into the effects of biodiesel (Eichhornia Crassipes) blends with different aluminum oxide nanoparticle concentrations on the combustion process in diesel engines. The experiments included measuring performance parameters and emissions tests while changing the engine speed [...] Read more.
The current work includes experimental and numerical investigations into the effects of biodiesel (Eichhornia Crassipes) blends with different aluminum oxide nanoparticle concentrations on the combustion process in diesel engines. The experiments included measuring performance parameters and emissions tests while changing the engine speed and increasing loads. IC Engine Fluent, a specialist computational tool included in the ANSYS software (R19.0 version), was used to simulate internal combustion engine dynamics and combustion processes. All investigations were carried out using biodiesel blends with three concentrations of Al2O3 nanoparticles: 50, 100, and 150 ppm. The tested samples are called D100, D80B20, D80B20N50, D80B20N100, and D80B20N150, accordingly. The combustion characteristics are improved due to the catalytic effect and higher surface area of nano additives. The results showed improvements in the combustion process as the result of the nanoparticles’ addition, which led to the higher peak cylinder pressure. The increases in the peak cylinder pressures for D80B20N50, D80B20N100, and D80B20N150 about D80B20 were 3%, 5%, and 8%, respectively, at a load of 200 Nm, while the simulation found that the maximum temperature for biodiesel blends diesel was higher than that for pure diesel; this was due to the higher hydrocarbon values of D80B20. Also, nano additives caused a decrease in temperatures in the combustion of biofuels. Finally, nano additives caused an enhancement of the emissions test results for all parameters when compared to pure diesel fuel and biofuel. Full article
(This article belongs to the Special Issue Clean Combustion Technologies and Renewable Fuels)
Show Figures

Figure 1

Figure 1
<p>Experimental setup visualization.</p>
Full article ">Figure 2
<p>Numerical analysis flowchart.</p>
Full article ">Figure 3
<p>Cylinder geometry of internal combustion engine.</p>
Full article ">Figure 4
<p>CI engine domain and mesh generated.</p>
Full article ">Figure 5
<p>Variation of the BSFC with load for all fuel blend samples: D100, D80B20, D80B20N50, D80B20N100, and D80B20N150.</p>
Full article ">Figure 6
<p>Variation of the BTE with the load for all fuel blend samples: D100, D80B20, D80B20N50, D80B20N100, and D80B20N150.</p>
Full article ">Figure 7
<p>Variation in the CO emissions with the load for all fuel blend samples: D100, D80B20, D80B20N50, D80B20N100, and D80B20N150.</p>
Full article ">Figure 8
<p>Variation of the CO<sub>2</sub> emissions with the load for all fuel blend samples: D100, D80B20, D80B20N50, D80B20N100, and D80B20N150.</p>
Full article ">Figure 9
<p>Variation of the HC emissions with the load for all fuel blend samples: D100, D80B20, D80B20N50, D80B20N100, and D80B20N150.</p>
Full article ">Figure 10
<p>Variation of the NOx emissions with the load for all fuel blend samples: D100, D80B20, D80B20N50, D80B20N100, and D80B20N150.</p>
Full article ">Figure 11
<p>Contours of cylinder pressure variation with the crank angle of all tested fuels at a load of 200 Nm.</p>
Full article ">Figure 12
<p>Variation of cylinder pressure with the crank angle of all tested fuels at a load of 200 Nm.</p>
Full article ">Figure 13
<p>Peak cylinder pressure of the diesel and biodiesel blend with nano additives at different loads.</p>
Full article ">Figure 14
<p>Contours of cylinder temperature variation with the crank angle of B20N150 at a load of 200 Nm.</p>
Full article ">Figure 15
<p>Max. temperature of the diesel and biodiesel blend with nano additives at different loads.</p>
Full article ">Figure 16
<p>Contours of velocity distribution at different crank angles of D80B20N150 at a load of 200 Nm.</p>
Full article ">Figure 17
<p>The variation of the Numerical BTE with the engine load for fuel blend samples.</p>
Full article ">Figure 18
<p>Contours of CO<sub>2</sub> mass fraction of different fuel blends at a load of 200 Nm and speed of 1150 rpm.</p>
Full article ">Figure 19
<p>Contours of CO<sub>2</sub> mass fraction of different fuel blends at a load of 200 Nm and speed of 1400 rpm.</p>
Full article ">Figure 20
<p>Contours of CO<sub>2</sub> mass fraction of different fuel blends at a load of 200 Nm and speed of 1600 rpm.</p>
Full article ">Figure 21
<p>Contours of CO<sub>2</sub> mass fraction of different fuel blends at a load of 200 Nm and speed of 1800 rpm.</p>
Full article ">Figure 22
<p>Numerical results of CO<sub>2</sub> emissions with engine speed for all additives.</p>
Full article ">Figure 23
<p>Contours of NOx mass fraction of different fuel blends at a load of 200 Nm and speed of 1150 rpm.</p>
Full article ">Figure 24
<p>Contours of NOx mass fraction of different fuel blends at a load of 200 Nm and speed of 1400 rpm.</p>
Full article ">Figure 25
<p>Contours of NOx mass fraction of different fuel blends at a load of 200 Nm and speed of 1600 rpm.</p>
Full article ">Figure 26
<p>Contours of NOx mass fraction of different fuel blends at a load of 200 Nm and speed of 1800 rpm.</p>
Full article ">Figure 27
<p>Numerical results of NOx emissions with engine speed for all additives.</p>
Full article ">Figure 28
<p>Comparison of numerical and experimental results of BTE with the load for D80B20 and D80B20N150.</p>
Full article ">Figure 29
<p>The compared numerical and experimental results of peak pressure with the engine load for D80B20 and D80B20N150 blends.</p>
Full article ">
29 pages, 7576 KiB  
Article
A Flatness Error Prediction Model in Face Milling Operations Using 6-DOF Robotic Arms
by Iván Iglesias, Alberto Sánchez-Lite, Cristina González-Gaya and Francisco J. G. Silva
J. Manuf. Mater. Process. 2025, 9(2), 66; https://doi.org/10.3390/jmmp9020066 - 19 Feb 2025
Abstract
The current trend in machining with robotic arms involves leveraging Industry 4.0 technologies to propose solutions that reduce path deviation errors. This approach presents significant challenges alongside promising advancements, as well as a substantial increase in the cost of future industrial robotic cells, [...] Read more.
The current trend in machining with robotic arms involves leveraging Industry 4.0 technologies to propose solutions that reduce path deviation errors. This approach presents significant challenges alongside promising advancements, as well as a substantial increase in the cost of future industrial robotic cells, which is not always amortizable. As an alternative or complementary approach to this trend, methods encouraging the occasional use of Industry 4.0 devices for characterizing the behavior of the actual physical cell, calibration, or adjustment are proposed. One such method, called FlePFaM, predicts flatness errors in face milling operations using robotic arms. This is achieved by estimating tool path deviation errors through the integration of a simple model of the robot arm’s mechanics with the cutting forces vector of the process, thereby optimizing machining conditions. These conditions are determined through prior empirical estimations of mass, stiffness, and damping. The conducted tests enabled the selection of the most favorable combination of variables, such as the robot wrist configuration, the position and orientation of the workpiece, and the predominant milling orientation. This led to the identification of the configuration with the lowest absolute flatness error according to the model’s predictions. The results demonstrated a high degree of similarity—between 97% for the closest case and 57% for the farthest case—between simulated and experimental flatness error values. FlePFaM represents a significant step forward in adopting innovative robotic arm solutions for reliable and efficient production. FlePFaM includes dimensional flatness indicators that provide practical support for decision making. Full article
Show Figures

Figure 1

Figure 1
<p>Relationship between the cutting constraints and the trajectory deviation.</p>
Full article ">Figure 2
<p>Diagram of the predictive methodology.</p>
Full article ">Figure 3
<p>Linear and torsional stiffness and damping factors simplification.</p>
Full article ">Figure 4
<p>(<b>a</b>) Geometry of a shaving. (<b>b</b>) Resulting of cutting forces on the TCP.</p>
Full article ">Figure 5
<p>Flowchart of the best-fit plane calculation process.</p>
Full article ">Figure 6
<p>Programmed path using One-Way Next.</p>
Full article ">Figure 7
<p>Configuration (<b>A</b>) and (<b>B</b>) for the wrist configuration of robot.</p>
Full article ">Figure 8
<p>Locations (1 and 2) and orientations stock (L and T).</p>
Full article ">Figure 9
<p>Experimental cell with IRB 6640 robot.</p>
Full article ">Figure 10
<p>Reading of the robot encoders (<b>a</b>) and frequency spectrum of the path error (<b>b</b>).</p>
Full article ">Figure 11
<p>3D cutting force values for rotation 360° (<b>a</b>) and main direction of guiding vector (<b>b</b>).</p>
Full article ">Figure 12
<p>Face milling in aluminum test parts for five paths in case n° 6 (magnified 1:10).</p>
Full article ">Figure 13
<p>Deviation errors in Z direction for each <span class="html-italic">P</span><sub>i</sub> from points 56 to 80.</p>
Full article ">Figure 14
<p>Mean deviation errors in Z direction for each <span class="html-italic">P</span><sub>i</sub> from points 56 to 80.</p>
Full article ">Figure 15
<p>Geometric deviation errors in Z direction for each <span class="html-italic">P</span><sub>i</sub> from points 56 to 80.</p>
Full article ">Figure 16
<p>Absolute deviation errors in Z direction for each <span class="html-italic">P</span><sub>i</sub> from points 56 to 80.</p>
Full article ">Figure 17
<p>Digitalized surface with higher flatness absolute error, T orientation.</p>
Full article ">Figure 18
<p>Digitalized surface with lower flatness absolute error, L orientation.</p>
Full article ">
18 pages, 3777 KiB  
Article
Surrogate-Assisted Cost Optimization for Post-Tensioned Concrete Slab Bridges
by Lorena Yepes-Bellver, Alejandro Brun-Izquierdo, Julián Alcalá and Víctor Yepes
Infrastructures 2025, 10(2), 43; https://doi.org/10.3390/infrastructures10020043 - 18 Feb 2025
Abstract
The study uses surrogate modeling techniques to evaluate cost optimization methodologies for post-tensioned concrete slab bridges. These structures are key components in transportation infrastructure, where design efficiency can yield significant economic benefits. The research focuses on a three-span slab bridge, with spans of [...] Read more.
The study uses surrogate modeling techniques to evaluate cost optimization methodologies for post-tensioned concrete slab bridges. These structures are key components in transportation infrastructure, where design efficiency can yield significant economic benefits. The research focuses on a three-span slab bridge, with spans of 24, 34, and 28 m, optimized through the Kriging surrogate model combined with heuristic algorithms such as simulated annealing. Input variables included deck depth, base geometry, and concrete grade, with Latin Hypercube Sampling ensuring diverse design exploration. Results reveal that the optimized design achieves a 6.54% cost reduction compared to conventional approaches, primarily by minimizing material usage—concrete by 14.8% and active steel by 11.25%. Among the predictive models analyzed, the neural network demonstrated the lowest prediction error but required multiple runs for stability, while the Kriging model offered accurate local optimum identification. This work highlights surrogate modeling as a practical and efficient tool for bridge design, reducing costs while adhering to structural and serviceability criteria. The methodology facilitates better-informed decision-making in structural engineering, supporting more economical bridge designs. Full article
(This article belongs to the Section Infrastructures and Structural Engineering)
Show Figures

Figure 1

Figure 1
<p>View of the longitudinal profile of the PC slab.</p>
Full article ">Figure 2
<p>Cross-section of the lightweight PC slab bridge deck.</p>
Full article ">Figure 3
<p>Simplified flowchart of the proposed methodology.</p>
Full article ">Figure 4
<p>Response surface of cost depending on concrete grade and deck depth (<a href="#infrastructures-10-00043-t003" class="html-table">Table 3</a> and <a href="#infrastructures-10-00043-t004" class="html-table">Table 4</a>).</p>
Full article ">Figure 5
<p>Normalized measurements and costs of the optimized structure relative to the reference slab.</p>
Full article ">Figure 6
<p>Response surface for the 38 observed deck data points (<a href="#infrastructures-10-00043-t003" class="html-table">Table 3</a> and <a href="#infrastructures-10-00043-t004" class="html-table">Table 4</a>).</p>
Full article ">Figure 7
<p>Contour plot for the 38 observed deck data points (<a href="#infrastructures-10-00043-t003" class="html-table">Table 3</a> and <a href="#infrastructures-10-00043-t004" class="html-table">Table 4</a>).</p>
Full article ">Figure 8
<p>Polynomial quadratic model fitted at 30 observed slab bridge deck data points (<a href="#infrastructures-10-00043-t002" class="html-table">Table 2</a>).</p>
Full article ">Figure 9
<p>ANN cost for a 3.15 m base width and 35 MPa concrete grade as a function of deck depth.</p>
Full article ">Figure 10
<p>ANN cost for a 1.30 m depth and 35 MPa concrete grade as a function of deck depth width.</p>
Full article ">Figure 11
<p>ANN cost for a 1.30 m depth and 3.15 m base width as a function of the concrete grade.</p>
Full article ">
51 pages, 17258 KiB  
Review
A Review of Simulation Tools Utilization for the Process of Laser Powder Bed Fusion
by Ľuboš Kaščák, Ján Varga, Jana Bidulská, Róbert Bidulský and Tibor Kvačkaj
Materials 2025, 18(4), 895; https://doi.org/10.3390/ma18040895 - 18 Feb 2025
Abstract
This review describes the process of metal additive manufacturing and focuses on the possibility of correlated input parameters that are important for this process. The correlation of individual parameters in the metal additive manufacturing process is considered using simulation tools that allow the [...] Read more.
This review describes the process of metal additive manufacturing and focuses on the possibility of correlated input parameters that are important for this process. The correlation of individual parameters in the metal additive manufacturing process is considered using simulation tools that allow the prediction of various defects, thus making the real production process more efficient, especially in terms of time and costs. Special attention is paid to multiple applications using these simulation tools as an initial analysis to determine the material’s behavior when defining various input factors, including the results obtained. Based on this, further procedures were implemented, including real production parts. This review also points out the range of possible variations that simulation tools have, which helps to effectively predict material defects and determine the volume of consumed material, supports construction risk, and other information necessary to obtain a quality part in the production process. From the overview of the application of simulation tools in this process, it was found that the correlation between theoretical knowledge and the definition of individual process parameters and other variables are related and are of fundamental importance for achieving the final part with the required properties. In terms of some specific findings, it can be noted that simulation tools identify adverse phenomena occurring in the production processes and allow manufacturers to test the validity of the proposed conceptual and model solutions without making actual changes in the production system, and they have the measurable impact on the design and production of quality parts. Full article
(This article belongs to the Special Issue Plastic Deformation and Mechanical Behavior of Metallic Materials)
Show Figures

Figure 1

Figure 1
<p>The dynamics of melt pool formation in the L-PBF process [<a href="#B54-materials-18-00895" class="html-bibr">54</a>].</p>
Full article ">Figure 2
<p>Process parameters in the L-PBF method controlling residual stress characteristics [<a href="#B87-materials-18-00895" class="html-bibr">87</a>].</p>
Full article ">Figure 3
<p>Display of the multi-layer process simulation in steps [<a href="#B54-materials-18-00895" class="html-bibr">54</a>]. (<b>a</b>) powder laying on the 1st layer (<b>b</b>) powder discretizing on the 1st layer (<b>c</b>) laser scanning on the 1st layer (<b>d</b>) surface reconstruction on the 1st layer (<b>e</b>) powder laying on the 2nd layer (<b>f</b>) powder discretizing on the 2nd layer (<b>g</b>) laser scanning on the 2nd layer (<b>h</b>) surface reconstruction on the 2nd layer.</p>
Full article ">Figure 4
<p>Powder particle size: (<b>a</b>) powder settling and powder lying (<b>b</b>,<b>c</b>) powder spreading and settling to the working zone [<a href="#B158-materials-18-00895" class="html-bibr">158</a>].</p>
Full article ">Figure 5
<p>Multiphysics numerical simulations designed for modeling metal additive manufacturing [<a href="#B198-materials-18-00895" class="html-bibr">198</a>].</p>
Full article ">Figure 6
<p>Different representations of scales occurring in the L-PBF process [<a href="#B208-materials-18-00895" class="html-bibr">208</a>].</p>
Full article ">Figure 7
<p>3D simulation of hydrodynamics and the effects of recoil and Marangoni forces [<a href="#B208-materials-18-00895" class="html-bibr">208</a>].</p>
Full article ">Figure 8
<p>View of laser–powder interaction in the L-PBF process: (<b>A</b>) particle with size of 19.2 μm, (<b>B</b>) particle with size of 29.2 μm [<a href="#B210-materials-18-00895" class="html-bibr">210</a>].</p>
Full article ">Figure 9
<p>3D rendering of (<b>a</b>) fine (<b>b</b>) coarse sintered powder bed. Yellow frames show comparison of the magnified area of powder bed of both type of powder [<a href="#B211-materials-18-00895" class="html-bibr">211</a>].</p>
Full article ">Figure 10
<p>Computational modes of inherent deformation (<b>a</b>) uniform stress (<b>b</b>) scan pattern (<b>c</b>) thermal stress [<a href="#B250-materials-18-00895" class="html-bibr">250</a>].</p>
Full article ">Figure 11
<p>Simulation results in Deform software [<a href="#B251-materials-18-00895" class="html-bibr">251</a>].</p>
Full article ">Figure 12
<p>Amphyon simulation software environment.</p>
Full article ">Figure 13
<p>The environment in Netfabb Simulation software.</p>
Full article ">Figure 14
<p>Simulation software VGSTUDIO MAX.</p>
Full article ">Figure 15
<p>Example of cantilever beam simulation in the AscentAM simulation software [<a href="#B278-materials-18-00895" class="html-bibr">278</a>].</p>
Full article ">Figure 16
<p>Support generation in Inspire Print3D simulation software [<a href="#B284-materials-18-00895" class="html-bibr">284</a>].</p>
Full article ">Figure 17
<p>Individual part models, (<b>1</b>) slide cylinder model, (<b>2</b>) aircraft part, (<b>3</b>) tensile test sample, (<b>4</b>) part, (<b>5</b>) parts with circular inner channels, (<b>6</b>) clutch levers, (<b>7</b>) rocker arms for racing cars, (<b>8</b>) electric motor mounting brackets, (<b>9</b>) tibial components, (<b>10</b>) bridge-shaped geometry, (<b>11</b>) motorcycle brake pedal, (<b>12</b>) double cantilever bridge, (<b>13</b>) model.</p>
Full article ">Figure 18
<p>Images of the melting pool in the L-PBF process (<b>1a</b>) two-pass model of finite elements under laser action, (<b>1b</b>) morphology of the molten pool [<a href="#B297-materials-18-00895" class="html-bibr">297</a>], (<b>2a</b>) transient temperature distribution at the beginning of layer melting, (<b>2b</b>) temperature distribution at the end of layer melting [<a href="#B298-materials-18-00895" class="html-bibr">298</a>], (<b>3a</b>) melt development at different laser deposition rates at 542 μm density, (<b>3b</b>) melt development at laser speed 600 mm/s of the powder at 664 μm density [<a href="#B299-materials-18-00895" class="html-bibr">299</a>].</p>
Full article ">Figure 19
<p>Comparison of the display of the orientation of the part and the support material (<b>1</b>) model of the sliding cylinder [<a href="#B285-materials-18-00895" class="html-bibr">285</a>], (<b>2</b>) part [<a href="#B287-materials-18-00895" class="html-bibr">287</a>], (<b>3</b>) rocker arm for a racing car [<a href="#B290-materials-18-00895" class="html-bibr">290</a>], (<b>4</b>) clutch lever [<a href="#B289-materials-18-00895" class="html-bibr">289</a>], (<b>5a</b>) layout of the support structure of the aircraft part without optimization, (<b>5b</b>) with optimization [<a href="#B185-materials-18-00895" class="html-bibr">185</a>], (<b>6</b>) tibial component [<a href="#B292-materials-18-00895" class="html-bibr">292</a>].</p>
Full article ">Figure 20
<p>Comparison of the display of the volume fraction of the material under different input conditions and for different types of parts in the L-PBF process (<b>1</b>) model of the feed cylinder [<a href="#B285-materials-18-00895" class="html-bibr">285</a>], (<b>2</b>) tensile sample [<a href="#B286-materials-18-00895" class="html-bibr">286</a>], (<b>3a</b>) volume fraction of the material of the aircraft part without optimization, (<b>3b</b>) with optimization [<a href="#B185-materials-18-00895" class="html-bibr">185</a>], (<b>4a</b>) part with an internal circular channel with a wall thickness of 10 mm, (<b>4b</b>) part with an internal circular channel with a wall thickness of 20 mm [<a href="#B288-materials-18-00895" class="html-bibr">288</a>], (<b>5a</b>) volume fraction in case of appropriate part orientation, (<b>5b</b>) volume fraction in case of inappropriate part orientation [<a href="#B287-materials-18-00895" class="html-bibr">287</a>].</p>
Full article ">Figure 21
<p>The comparison of the deformation display under different input conditions and for different types of parts in the L-PBF process (<b>1</b>) tibial component model [<a href="#B292-materials-18-00895" class="html-bibr">292</a>], (<b>2</b>) electric motor mounting bracket [<a href="#B291-materials-18-00895" class="html-bibr">291</a>], (<b>3a</b>) comparison of simulated bridge-shaped geometry (<b>3b</b>) geometry of the original model [<a href="#B293-materials-18-00895" class="html-bibr">293</a>], (<b>4a</b>) part with an internal circular channel with a wall thickness of 10 mm, (<b>4b</b>) part with an internal circular channel with a wall thickness of 20 mm [<a href="#B288-materials-18-00895" class="html-bibr">288</a>], (<b>5a</b>) Simulated deformation field for a double cantilever beam before cutting off the supports by the self-strain method (<b>5b</b>) by the simulation method [<a href="#B295-materials-18-00895" class="html-bibr">295</a>].</p>
Full article ">Figure 22
<p>Comparison of the equivalent stress display under different input conditions and for different types of parts in the L-PBF process (<b>1</b>) rocker arm for a racing car [<a href="#B290-materials-18-00895" class="html-bibr">290</a>], (<b>2a</b>) double cantilever beam before removing the support, (<b>2b</b>) after removing the support [<a href="#B295-materials-18-00895" class="html-bibr">295</a>], (<b>3a</b>) part with an internal circular channel with a wall thickness of 10 mm, (<b>3b</b>) part with an internal circular channel with a wall thickness of 20 mm [<a href="#B288-materials-18-00895" class="html-bibr">288</a>], (<b>4</b>)—motorcycle brake pedal [<a href="#B294-materials-18-00895" class="html-bibr">294</a>], (<b>5</b>)—model [<a href="#B296-materials-18-00895" class="html-bibr">296</a>].</p>
Full article ">Figure 23
<p>Comparison of the display of the shape deviation under different input conditions and for various types of parts in the L-PBF process (<b>1</b>). part with an internal circular channel with a wall thickness of 20 and 10 mm [<a href="#B288-materials-18-00895" class="html-bibr">288</a>], (<b>2</b>). motorcycle brake pedal [<a href="#B320-materials-18-00895" class="html-bibr">320</a>], (<b>3</b>). slider cylinder model [<a href="#B285-materials-18-00895" class="html-bibr">285</a>], (<b>4</b>). clutch lever [<a href="#B289-materials-18-00895" class="html-bibr">289</a>], (<b>5</b>). aircraft part (<b>5a</b>) aircraft part shape deviation without optimization, (<b>5b</b>) with optimization [<a href="#B185-materials-18-00895" class="html-bibr">185</a>].</p>
Full article ">
Back to TopTop