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Search Results (2,082)

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Keywords = multi-physical simulation

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13 pages, 3006 KiB  
Article
Microfluidic Biosensors for the Detection of Motile Plant Zoospores
by Peikai Zhang, David E. Williams, Logan Stephens, Robert Helps, Irene Patricia Shamini Pushparajah, Jadranka Travas-Sejdic and Marion Wood
Biosensors 2025, 15(3), 131; https://doi.org/10.3390/bios15030131 (registering DOI) - 21 Feb 2025
Abstract
Plant pathogen zoospores play a vital role in the transmission of several significant plant diseases, with their early detection being important for effective pathogen management. Current methods for pathogen detection involve labour-intensive specimen collection and laboratory testing, lacking real-time feedback capabilities. Methods that [...] Read more.
Plant pathogen zoospores play a vital role in the transmission of several significant plant diseases, with their early detection being important for effective pathogen management. Current methods for pathogen detection involve labour-intensive specimen collection and laboratory testing, lacking real-time feedback capabilities. Methods that can be deployed in the field and remotely addressed are required. In this study, we have developed an innovative zoospore-sensing device by combining a microfluidic sampling system with a microfluidic cytometer and incorporating a chemotactic response as a means to selectively detect motile spores. Spores of Phytophthora cactorum were guided to swim up a detection channel following a gradient of attractant. They were then detected by a transient change in impedance when they passed between a pair of electrodes. Single-zoospore detection was demonstrated with signal-to-noise ratios of ~17 when a carrying flow was used and ~5.9 when the zoospores were induced to swim into the channel following the gradient of the attractants. This work provides an innovative solution for the selective, sensitive and real-time detection of motile zoospores. It has great potential to be further developed into a portable, remotely addressable, low-cost sensing system, offering an important tool for field pathogen real-time detection applications. Full article
(This article belongs to the Special Issue Biosensors Based on Microfluidic Devices—2nd Edition)
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<p>(<b>A</b>) Schematic illustration of life cycle of zoospores. (<b>B</b>–<b>D</b>) Optical microscope images of <span class="html-italic">Phytophthora cactorum</span> H78. (<b>B</b>) Mature sporangia harbouring zoospores (►). (<b>C</b>) Individual sporangium highlighting membrane-engaged zoospores prior to release (►). (<b>D</b>) Motile zoospores released from sporangia into water (►).</p>
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<p>Schematic of sensing setup.</p>
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<p>The finite element (COMSOL) simulation of the electrical field, with AC potential applied between the electrodes. The <span class="html-italic">X</span>-axis lies in the plane of the electrodes, and the <span class="html-italic">Z</span>-axis perpendicular to this (Z = 0 at the electrode surface). (<b>A</b>) A schematic of the equivalent circuit. (<b>B</b>) The distribution of the current densities at different positions in the channel (blue to red: low current density to high current density). (<b>C</b>) The distribution of the local electrical potential inside the channel (blue to red: low potential to high potential). (<b>D</b>) The calculated current density along the <span class="html-italic">X</span>-axis inside the channel with the Z position of zoospores at 10 µm (middle of the channel). (<b>E</b>) The calculated current density along the <span class="html-italic">Z</span>-axis inside the channel with the X position of zoospores at 100 µm (middle of the electrode gap). (<b>F</b>) The calculated impedance and current between the two electrodes with the zoospores at different X positions in the channel and Z = 10 µm. Blue and green lines are the impedance and current between the two electrodes, respectively. (<b>G</b>) The calculated impedance and current between the two electrodes with the zoospores at different Z positions in the channel, with X = 100 µm, the middle of the electrode gap. Blue and green lines are the impedance and current between the two electrodes, respectively.</p>
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<p>The sensing response from zoospores passing the electrodes, carried in a flow. (<b>A</b>) The recorded real-time signal at different AC frequencies. The frequencies presented here are 5 kHz, 30 kHz, 50 kHz, 80 kHz, and 100 kHz from top to bottom. (<b>B</b>) A zoomed version of the response recorded at 50 kHz. (<b>C</b>,<b>D</b>) The statistical analyses of the signal amplitude and signal-to-noise ratio at different frequencies. (<b>E</b>) The signal from the two different pairs of electrodes, 1 mm apart in the flow direction.</p>
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<p>(<b>A</b>) Proof-of-concept design for sampling zoospores from a flow. (<b>B</b>) The simulation result of the attractant gradient. (<b>C</b>) The simulation result of the flow rate distribution inside the microfluidic channel. (<b>D</b>) The enlarged flow simulation result showing the eddies into the stub near the entrance of the sensing channel. The numbered features are discussed in the text.</p>
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<p>(<b>A</b>) Overlap view of sensing signal received from 6 individual zoospores using Tier 2 sensor. Different lines are different individual zoospores. (<b>B</b>) Microscope image showing zoospore swimming inside the channel.</p>
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16 pages, 636 KiB  
Article
A Frequency-Domain Estimation Scheme for Frequency Offset with Large Range in OFDM Systems
by Tao Wang, Dejin Kong, Hao Jiang and Hongming Chen
Electronics 2025, 14(5), 859; https://doi.org/10.3390/electronics14050859 - 21 Feb 2025
Abstract
With the development of 5G new radio (NR) applications in high-speed scenarios, such as 5G non-terrestrial networks (NTN), the Doppler shift in the systems is significant. In this paper, an estimation scheme for frequency offset with large range in orthogonal frequency division multiplexing [...] Read more.
With the development of 5G new radio (NR) applications in high-speed scenarios, such as 5G non-terrestrial networks (NTN), the Doppler shift in the systems is significant. In this paper, an estimation scheme for frequency offset with large range in orthogonal frequency division multiplexing (OFDM) systems is proposed. The proposed scheme firstly takes advantage of the 2π-periodicity of the phase offset between two pilot OFDM symbols to estimate a set of candidate frequency offsets. It then uses the autocorrelation of the pilot sequence to determine the final estimated frequency offset. This method allows for a large estimation range, independent of the symbol gap between the two pilot OFDM symbols. Moreover, the low-complexity implementation of the scheme is provided. The simulation results based on 5G NR physical uplink shared channel (PUSCH) show the effectiveness of the proposed scheme in both single-user and multi-user scenarios, where various Doppler shifts and numbers of configured resource blocks (RB) are considered. The simulation results also show that the proposed frequency-domain method outperforms the conventional time-domain method with additional computation complexity. Full article
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<p>The baseband transmitter and receiver structure of an OFDM system with pilot-based frequency offset estimation.</p>
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<p>A frame structure with two pilot OFDM symbols.</p>
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<p>The modulus of <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold-italic">Z</mi> <mi>l</mi> </msub> <mrow> <mo>(</mo> <mi>k</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> with different values of <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>ϵ</mi> <mo stretchy="false">^</mo> </mover> <mrow> <mo>(</mo> <mi>l</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>.</p>
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<p>An NR subframe with twelve data OFDM symbols and two DMRS OFDM symbols.</p>
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<p>The MSE performance with different <math display="inline"><semantics> <mi>ϵ</mi> </semantics></math> and <span class="html-italic">M</span>.</p>
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<p>The MSE performance with different <math display="inline"><semantics> <msub> <mi>N</mi> <mrow> <mi>r</mi> <mi>b</mi> </mrow> </msub> </semantics></math>.</p>
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<p>The MSE performance of Algorithm 1 combined with the IFO estimation.</p>
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<p>The MSE performance of proposed Algorithm 1 and the conventional time domain estimation.</p>
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<p>The MSE performance of Algorithm 1 in multi-user and single-user scenarios.</p>
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20 pages, 5819 KiB  
Article
Research on the DC Ice-Melting Model and Its Influencing Factors on the Overhead Contact Systems of an Electrification Railway
by Guosheng Huang, Mingli Wu, Jieyi Liang, Songping Fu, Fuqiang Tian, Xiaojuan Pei, Qiujiang Liu and Teng Li
Energies 2025, 18(5), 1028; https://doi.org/10.3390/en18051028 - 20 Feb 2025
Abstract
The overhead contact system of the electrification railway is exposed to the natural environment throughout the year and is liable to encounter the problem of line icing. The icing on the line will reduce the current-collection performance of the pantograph, resulting in a [...] Read more.
The overhead contact system of the electrification railway is exposed to the natural environment throughout the year and is liable to encounter the problem of line icing. The icing on the line will reduce the current-collection performance of the pantograph, resulting in a decrease in the safety and reliability of the overhead contact system. It is an effective way to solve the icing problem by using the Joule heat generated by the DC in the conductor to melt the ice. In this paper, the multi-physics simulation software COMSOL is used to construct the finite element simulation model of the overhead contact system unit composed of a contact line, catenary wire and dropper. The model covers the physical processes such as convective heat transfer between conductor and air, heat conduction between overhead contact system and ice layer during ice melting, and considers the latent heat factor of ice melting. Under the condition of no icing, the actual data of several temperature points are measured under the applied current state of the overhead contact system, and the validity of the model is verified by comparing the simulated temperature data with the measured data. On this basis, the effects of ambient temperature, ice thickness and current on ice melting were studied using simulations. The results show that the ambient temperature has a significant effect on the ice-melting speed. Under 10 mm ice thickness and 2 m/s wind speed conditions, the time to start melting ice increases from 2 to 60 min until the ice cannot be melted as the ambient temperature decreases from −1 °C to −25 °C. Various initial conditions for ice thickness and wind speed were analyzed. Under the condition of no ice, the temperature rise of the contact wire and the catenary wire increases significantly with the current increase. When the current increases from 500 A to 2000 A, the temperature rise of the contact wire increases from 9.08–9.25 °C to 214.07–218.59 °C, and the temperature rise of the catenary wire increases from 6.88–7.01 °C to 173.43–177.13 °C. In addition, there is an optimal ice thickness range for the ice-melting process. When melting ice at −1 °C and −5 °C, the optimal ice thickness ranges are 4–8 mm and 1–4 mm, respectively. Full article
(This article belongs to the Section F: Electrical Engineering)
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<p>Experimental circuit diagram of full-scale measurement of overhead contact system.</p>
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<p>The schematic diagram of the line connection between the overhead contact system and the negative power supply.</p>
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<p>The power supply connection diagram of the overhead contact system and the wiring diagram of the electrical connection wire. (<b>a</b>) Positive and negative electrodes; (<b>b</b>) connection wire.</p>
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<p>Temperature measurement point and measurement equipment. (<b>a</b>,<b>b</b>) Temperature measurement point, (<b>c</b>) measurement equipment.</p>
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<p>Temperature measurement point and measurement equipment. (<b>a</b>,<b>b</b>) Temperature measurement point, (<b>c</b>) measurement equipment.</p>
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<p>The cross-sectional diagrams of various wires and the cross-sectional diagram considered in the modeling. (<b>a</b>) Simulation, (<b>b</b>) catenary wire, (<b>c</b>) contact wire, (<b>d</b>) dropper.</p>
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<p>Direct suspension and catenary suspension diagram in overhead contact system. (<b>a</b>) Direct suspension, (<b>b</b>) catenary suspension.</p>
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<p>The geometric model of the structural unit in the simulation.</p>
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<p>The boundary conditions of the Electric Currents Interface and the Heat Transfer in Solids Interface in the simulation. (<b>a</b>) Electric Currents Interface. (<b>b</b>) Heat Transfer in Solids Interface.</p>
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<p>The model diagram of the components and the whole model in validity verification simulation. (<b>a</b>) short-circuit electric connection wires; (<b>b</b>) clamps; (<b>c</b>) negative electrical connection wires; (<b>d</b>) whole model.</p>
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<p>The corresponding position of the temperature data points in the simulation, (<b>a</b>) center point, (<b>b</b>) ice layer edge point.</p>
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<p>Variation curves of maximum temperature with ice thickness in 60 min at different ambient temperatures at the center point (<b>a</b>) and edge point (<b>b</b>) of the contact wire.</p>
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<p>Variation curves of maximum temperature with ice thickness in 60 min at different ambient temperatures at the center point (<b>a</b>) and edge point (<b>b</b>) of the catenary wire.</p>
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<p>Ice-melting time simulation results of contact wire and catenary wire under different ice thicknesses and ambient temperature.</p>
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<p>The steady-state temperature–current curve of contact wire/catenary wire at 0 °C and 5 °C.</p>
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<p>Grid structure diagram.</p>
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<p>Finite element mesh convergence test results.</p>
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21 pages, 11490 KiB  
Article
Research on Disturbance Compensation Control and Parameter Identification of a Multiple Air-Bearing Planar Air-Floating Platform Based on ADRC
by Chuanxiao Xu, Guohua Kang, Junfeng Wu, Zhen Li, Xinyong Tao, Jiayi Zhou and Jiaqi Wu
Aerospace 2025, 12(2), 160; https://doi.org/10.3390/aerospace12020160 - 19 Feb 2025
Abstract
The spacecraft microgravity simulation air-bearing platform is a crucial component of the spacecraft ground testing system. Special disturbances, such as the flatness and roughness of the contact surface between the air bearings and the granite platform, increasingly affect the control accuracy of the [...] Read more.
The spacecraft microgravity simulation air-bearing platform is a crucial component of the spacecraft ground testing system. Special disturbances, such as the flatness and roughness of the contact surface between the air bearings and the granite platform, increasingly affect the control accuracy of the simulation experiment as the number of air bearings increases. To address this issue, this paper develops a novel compensation control system based on Active Disturbance Rejection Control (ADRC), which estimates and compensates for the disturbing forces and moments caused by the roughness and levelness of the contact surface, thereby improving the control precision of the spacecraft ground simulation system. A dynamic model of the multi-air-bearing platform under disturbance is established. A cascade ADRC algorithm based on the Linear Extended State Observer (LESO) is designed. The Gauss–Newton iteration method is used to identify the parameters of the sliding friction coefficient and the tilt angle of the air-bearing platform. A full-physics simulation experimental platform for spacecraft with rotor-based propulsion is constructed, and the proposed algorithm is validated. The experimental results show that on a marble surface with a flatness of grade 00, an overall tilt angle of 0–1 degrees, and a surface friction coefficient of 0–0.01, the position control accuracy for the simulated spacecraft can reach 1.5 cm, and the attitude control accuracy can reach 1°. Under ideal conditions, the identification accuracy for the contact surface friction coefficient is 2 × 10−4, and the recognition accuracy for the overall levelness of the marble surface can reach 1 × 10−3, laying the foundation for high-precision ground simulation experiments of spacecraft in multi-air-bearing scenarios. Full article
(This article belongs to the Section Astronautics & Space Science)
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<p>Main structure of this paper.</p>
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<p>Coordinate system representation.</p>
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<p>Conversion of inertial force systems.</p>
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<p>Controller structure.</p>
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<p>Gauss–Newton method solution process.</p>
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<p>Virtual plane friction coefficient distribution.</p>
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<p>Numerical simulation results for circular trajectory tracking.</p>
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<p>Control outputs.</p>
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<p>Friction coefficient calibration results.</p>
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<p>Marble plane inclination calibration results.</p>
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<p>Floating microgravity simulation experiment system structure.</p>
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<p>Spacecraft simulator.</p>
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<p>Experiment platform hardware and software communication flow chart.</p>
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<p>Observer parameter tuning and parameterization results.</p>
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<p>Calibration result of thrust curve.</p>
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<p>Circular trajectory tracking experiment.</p>
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<p>Experimental results of trajectory tracking.</p>
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<p>Position and attitude control errors.</p>
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<p>Parameter identification experiment.</p>
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<p>Three-axis perturbation identification results.</p>
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<p>Friction coefficient identification results.</p>
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<p>Results of marble inclination identification.</p>
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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)
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<p>PRISMA flow diagram of the review process.</p>
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<p>Basic results of the review: (<b>a</b>) by year, (<b>b</b>) by discipline.</p>
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<p>The most common current use of AI-supported AM in rehabilitation and physiotherapy (authors’ own elaboration).</p>
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<p>Possible future customization of AI–supported 3D printed assistive technologies in rehabilitation and physiotherapy (authors’ own elaboration).</p>
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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)
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<p>A schematic representation of ATES operation (adapted from Bloemendal et al. [<a href="#B7-energies-18-01001" class="html-bibr">7</a>]).</p>
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<p>Prisma flow diagram.</p>
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<p>Number of articles uploaded per year.</p>
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<p>Number of articles per country.</p>
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<p>Locations of ATES systems from <a href="#energies-18-01001-t007" class="html-table">Table 7</a>.</p>
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9 pages, 3854 KiB  
Proceeding Paper
The Mechanical Characterization of a Gyroid-Based Metamaterial by Compression Testing
by Andrea Ciula, Gianluca Rubino and Pierluigi Fanelli
Eng. Proc. 2025, 85(1), 17; https://doi.org/10.3390/engproc2025085017 - 18 Feb 2025
Abstract
Gyroid-based mechanical metamaterials have garnered increasing attention for their unique mechanical properties, particularly in applications involving complex stress environments. This study focuses on the mechanical characterization of the gyroid cell, a member of the Triply Periodic Minimal Surfaces (TPMS) family, through both experimental [...] Read more.
Gyroid-based mechanical metamaterials have garnered increasing attention for their unique mechanical properties, particularly in applications involving complex stress environments. This study focuses on the mechanical characterization of the gyroid cell, a member of the Triply Periodic Minimal Surfaces (TPMS) family, through both experimental and numerical analyses. Three different gyroid morphologies were generated by varying a single parameter in the parametric equation of the gyroid surface. Specimens were fabricated by 3D printing based on Liquid Crystal Display (LCD) technology, and compression tests were conducted to measure the equivalent Young’s modulus. Numerical models developed using Finite Element Method (FEM) analysis were validated through the experimental findings. The results indicate a good correlation between the experimental and numerical data, particularly in the linear elastic region, confirming the suitability of FEM simulations in predicting the mechanical response of these cellular structures. The study serves as a foundational step towards a broader multi-physical characterization of TPMS-based metamaterials and paves the way for the future development of tailored metamaterials for specific applications, including sacrificial limiters in plasma-facing components of Tokamaks. Full article
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<p>Isometric view (<b>top</b>) and top view along z axis (<b>bottom</b>) of isometric gyroid cell (<b>left</b>) and two manipulated cell morphologies (<b>center</b> and <b>right</b>).</p>
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<p>Isotropic gyroid cell (cyan) and offset surfaces obtained with a non-zero constant term d (blue and yellow).</p>
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<p>Top, side, and isometric views and 3D-printed samples of the three examined cell morphologies with different values of parameter <span class="html-italic">a</span>.</p>
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<p>Force–displacement curves for all the compression tests. The dotted line is associated with a specimen printed in a different batch than all the others. The thick line indicates a specimen that has been previously lapped. In this figure, the settling zone (<b>a</b>) and the linear zone (<b>b</b>) are clearly distinguishable. The ranges in which the peak load values for cells of the same morphology fall are rather wide compared to their absolute value (<b>c</b>).</p>
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<p>Force–displacement curves of tested specimens with <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math> obtained from experimental tests compared with numerical result from a model with the same morphology. The slope of the linear zone and the peak load are shown for each experimental curve.</p>
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<p>Force–displacement curves of tested specimens with <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> obtained from experimental tests compared with the numerical result from a model with the same morphology. The slope of the linear zone and the peak load are shown for each experimental curve.</p>
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<p>Force–displacement curves of tested specimens with <math display="inline"><semantics> <mrow> <mi>a</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math> obtained from experimental tests compared with the numerical result from a model with the same morphology. The slope of the linear zone and the peak load are shown for each experimental curve.</p>
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<p>Trends derived from experimental analysis and confirmed by the FEM model of equivalent Young’s modulus <math display="inline"><semantics> <msub> <mi>E</mi> <mrow> <mi>e</mi> <mi>q</mi> </mrow> </msub> </semantics></math>, maximum load <math display="inline"><semantics> <msub> <mi>L</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math>, and maximum displacement <math display="inline"><semantics> <msub> <mi>d</mi> <mrow> <mi>L</mi> <mi>m</mi> <mi>a</mi> <mi>x</mi> </mrow> </msub> </semantics></math> as gyroid cell parameter <span class="html-italic">a</span> changes.</p>
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<p>Typical Von Mises equivalent stress distribution on the three gyroid cells investigated.</p>
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17 pages, 12589 KiB  
Article
Analysis of the Influence of Process Parameters on Transverse Flux Induction Heating of Endless-Rolling Strip
by Lin Gao, Fang-Zhou Shi, Meng Yan, Yi-Ping He, Jian Xiang, Xiao-Hu Qi and Hua-Gui Huang
Metals 2025, 15(2), 218; https://doi.org/10.3390/met15020218 - 18 Feb 2025
Abstract
This study focuses on the effect of an induction heating device on the entry of a thin strip continuous casting and rolling line. A finite element model for the electromagnetic–thermal coupling of transverse magnetic flux induction heating was developed by adopting COMSOL software [...] Read more.
This study focuses on the effect of an induction heating device on the entry of a thin strip continuous casting and rolling line. A finite element model for the electromagnetic–thermal coupling of transverse magnetic flux induction heating was developed by adopting COMSOL software 6.1 to systematically investigate the effects of process parameters on the magnetic field, eddy current field, and the transverse temperature distribution of the strip. The results show that when the gap is between 20 mm and 40 mm, the maximum value of magnetic induction in the overheating region at the edges of the strip increases from 0.28 T to 0.35 T and 0.38. When the strip width is 1000 mm, there is an approximately 29% increase in magnetic induction in comparison to a strip with a width of 800 mm, and both eddy current density and temperature exhibit abnormal fluctuations. The maximum temperature difference in the temperature uniformity region at the center of the strip is only 3 °C at different frequencies, and the temperature-rise curves almost completely overlap. With increasing current, the temperature difference between the weak temperature region and the temperature uniformity region at the center widens, indicating a deterioration in temperature uniformity. Meanwhile, the field conditions are simulated using a simplified model of continuous heating. The results indicate that the maximum temperature deviation in the overheating region at the edges of the strip is 6 °C, while the deviation in the temperature uniformity region is 2 °C. Furthermore, the simulation data reveal an average temperature rise of 1156 °C across the width of the strip, with a deviation of 1.4 °C compared to the measured results, which verifies the validity of the proposed model. The analysis results provide a reference basis for designing transverse magnetic flux induction heating devices and optimizing process parameters. Full article
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<p>Process layout diagram of an endless rolling production line.</p>
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<p>The geometric model and mesh division of the induction heating device: (<b>a</b>) geometric model; (<b>b</b>) mesh division; (<b>c</b>) geometric parameters of induction heating model.</p>
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<p>Material parameters of ASTM1045 and silicon steel: (<b>a</b>) relative permeability and resistivity of ASTM1045; (<b>b</b>) specific heat capacity and thermal conductivity of ASTM1045; (<b>c</b>) density of silicon steel; (<b>d</b>) specific heat capacity and thermal conductivity of silicon steel.</p>
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<p>Procedures of electromagnetic and thermal analysis for induction heating process.</p>
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<p>A schematic diagram of the induction heating part of an endless rolling production line.</p>
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<p>The simulation data are compared with measured data.</p>
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<p>Eddy current, magnetic field, and thermal distribution nephogram and graph: (<b>a</b>) geometric model; (<b>b</b>) magnetic field; (<b>c</b>) eddy current field; (<b>d</b>) temperature field; (<b>e</b>) distribution curves of magnetic flux density and eddy current density; (<b>f</b>) temperature distribution curve.</p>
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<p>The distribution of magnetic lines on the cross-section after the induction heating state is stable: (<b>a</b>) section 1; (<b>b</b>) section 2.</p>
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<p>The simulation results in the width direction of the strip under different gaps: (<b>a</b>) magnetic induction strength distribution curve; (<b>b</b>) eddy current density curves; (<b>c</b>) temperature distribution.</p>
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<p>The simulation results in the width direction of the strip under different strip thicknesses: (<b>a</b>) magnetic induction strength distribution curve; (<b>b</b>) eddy current density curves; (<b>c</b>) temperature distribution.</p>
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<p>The simulation results in the width direction of the strip under different plate widths: (<b>a</b>) magnetic induction strength distribution curve; (<b>b</b>) eddy current density curves; (<b>c</b>) temperature distribution.</p>
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<p>The simulation results in the width direction of the strip under different strip speeds: (<b>a</b>) magnetic induction strength distribution curve; (<b>b</b>) eddy current density curves; (<b>c</b>) temperature distribution.</p>
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<p>The simulation results in the width direction of the strip under different frequencies: (<b>a</b>) magnetic induction strength distribution curve; (<b>b</b>) eddy current density curves; (<b>c</b>) temperature distribution.</p>
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<p>The simulation results in the width direction of the strip under different current: (<b>a</b>) magnetic induction strength distribution curve; (<b>b</b>) eddy current density curves; (<b>c</b>) temperature distribution.</p>
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<p>Results of the average temperature rise and standard deviation at the center of the strip: (<b>a</b>) results under different gaps; (<b>b</b>) results under different strip thicknesses; (<b>c</b>) results under different strip widths; (<b>d</b>) results under different strip speeds; (<b>e</b>) results under different frequencies; (<b>f</b>) results under different currents.</p>
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19 pages, 3933 KiB  
Article
A Fully Coupled Electro-Vibro-Acoustic Benchmark Model for Evaluation of Self-Adaptive Control Strategies
by Thomas Kletschkowski
J 2025, 8(1), 6; https://doi.org/10.3390/j8010006 - 17 Feb 2025
Abstract
The reduction of noise and vibration is possible with passive, semi-active and active control strategies. Especially where self-adaptive control is required, it is necessary to evaluate the noise reduction potential before the control approach is applied to the real-world problem. This evaluation can [...] Read more.
The reduction of noise and vibration is possible with passive, semi-active and active control strategies. Especially where self-adaptive control is required, it is necessary to evaluate the noise reduction potential before the control approach is applied to the real-world problem. This evaluation can be based on a virtual model that contains all relevant sub-systems, transfer paths and coupling effects on the one hand. On the other hand, the complexity of such a model has to be limited to focus on principal findings such as convergence speed, power consumption, and noise reduction potential. The present paper proposes a fully coupled electro-vibro-acoustic model for the evaluation of self-adaptive control strategies. This model consists of discrete electrical and mechanical networks that are applied to model the electro-acoustic behavior of noise and anti-noise sources. The acoustic field inside a duct, terminated by these electro-acoustic sources, is described by finite elements. The resulting multi-physical model is capable of describing all relevant coupling effects and enables an efficient evaluation of different control strategies such as the local control of sound pressure or active control of acoustic absorption. It is designed as a benchmark model for the benefit of the scientific community. Full article
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<p>Topological model of system (top) and electro-vibro-acoustical model (bottom).</p>
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<p>Resonance frequencies of the uncontrolled system.</p>
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<p>Normalized mode shapes in resonance.</p>
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<p>System input and system output without self-adaptive control.</p>
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<p>IR and resonance frequencies of the uncontrolled system.</p>
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<p>Modelling of system response without active control.</p>
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<p>Active control of local sound pressure—time-history of simulation.</p>
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<p>Frequency domain illustration of active control of local sound pressure.</p>
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<p>Active control of local absorption—time-history of simulation.</p>
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<p>Frequency domain illustration of active control of local absorption.</p>
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18 pages, 5927 KiB  
Article
Design and Optimization of a Gold and Silver Nanoparticle-Based SERS Biosensing Platform
by Soumyadeep Saha, Manoj Sachdev and Sushanta K. Mitra
Sensors 2025, 25(4), 1165; https://doi.org/10.3390/s25041165 - 14 Feb 2025
Abstract
This study investigates the design and optimization of a nanoparticle-based surface-enhanced Raman scattering (SERS) biosensing platform using COMSOL Multiphysics simulations. The primary goal is to enhance the sensitivity and specificity of SERS biosensors, which are crucial for the precise detection and quantification of [...] Read more.
This study investigates the design and optimization of a nanoparticle-based surface-enhanced Raman scattering (SERS) biosensing platform using COMSOL Multiphysics simulations. The primary goal is to enhance the sensitivity and specificity of SERS biosensors, which are crucial for the precise detection and quantification of biomolecules. The simulation study explores the use of gold and silver nanoparticles in various arrangements, including single, multiple, and periodic nanospheres. The effects of polarization and the phenomenon of local hotspot switching in trimer and tetramer nanosphere systems are analyzed. To validate the simulation results, a SERS biosensing platform is fabricated by self-assembling gold nanoparticles on a silicon substrate, with methylene blue used as the Raman probe molecule. The findings demonstrate the feasibility of optimizing SERS biochips through simulation, which can be extended to various nanostructures. This work contributes to the advancement of highly sensitive and specific SERS biosensors for diagnostic and analytical applications. Full article
(This article belongs to the Section Biosensors)
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<p>Geometry and mesh of single nanosphere with physical domain and perfectly matched layer.</p>
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<p>(<b>A</b>) Electrical field around a single nanosphere. Enhancement factor plots at different Raman wavelengths for single nanosphere of (<b>B</b>) silver and (<b>C</b>) gold.</p>
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<p>(<b>A</b>) Electric field of a nanodimer system. Enhancement factor plots of nanodimer system (<b>B</b>) gold at λ = 785 nm and (<b>C</b>) silver at λ = 633 nm.</p>
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<p>Electrical field of the nanodimer system at orientation (<b>A</b>) 45° and (<b>B</b>) 90° with respect to the direction of incident polarization. (<b>C</b>) Enhancement factor variation with orientation for gold nanodimers of radius 80 nm, gap 2 nm and λ = 785 nm.</p>
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<p>Polarization charge of nanodimer system at different orientations: (<b>A</b>) perfectly aligned with the direction of polarization and (<b>B</b>) perpendicular alignment with the direction of polarization.</p>
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<p>Electrical field of nanotrimer system for different orientations (<b>A</b>) nanotrimer orientation A and (<b>B</b>) nanotrimer orientation B. Here polarization is in the positive z-direction. Enhancement factor plots for nanotrimer system orientation A for (<b>C</b>) silver at λ = 633 nm and (<b>D</b>) gold at λ = 785 nm.</p>
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<p>Electric field of nanotetramer systems at different orientations (<b>A</b>–<b>C</b>). The direction of polarization is positive z.</p>
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<p>Enhancement factor plots for nanotetramer system orientation C for (<b>A</b>) silver at λ = 633 nm and (<b>B</b>) gold at λ = 785 nm.</p>
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<p>Nanotetramer system at orientation C, showing the phenomenon of hotspot switching. (<b>A</b>) Hotspot 1–4 are on, hotspot 5 is off for silver nanotetramer radius 100 nm, gap of 4 nm and λ = 633 nm. (<b>B</b>) Hotspot 1–4 are off, hotspot 5 is on for silver nanotetramer radius 40 nm, gap of 4 nm and λ = 633 nm.</p>
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<p>Enhancement factor plot of (<b>A</b>) hotspot 5 and (<b>B</b>) hotspot 1 for silver nanotetramer at λ = 532 nm. Variation of enhancement factor with orientation of silver (<b>C</b>) nanotrimer of radius 140 nm, gap 2 nm at λ = 532 nm and (<b>D</b>) nanotetramer of radius 60 nm, gap 2 nm at λ = 532 nm.</p>
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<p>(<b>A</b>) A three-dimensional view of a periodic array of nanospheres. (<b>B</b>) Unit cell of the periodic nanosphere array. (<b>C</b>) Enhancement factor of the unit cell showing an effective domain of one nanosphere only.</p>
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<p>Average enhancement factor plot of periodic silver nanospheres at (<b>A</b>) λ = 532 nm, (<b>B</b>) λ = 633 nm and for periodic gold nanospheres at (<b>C</b>) λ = 785 nm. (<b>D</b>) Variation of average enhancement factor with orientation of a periodic gold nanosphere array of radius 100 nm, gap 2 nm at λ = 785 nm.</p>
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<p>Proper functionalization scheme of gold nanoparticles by aminating the Si surface.</p>
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<p>Scanning electron microscopy images of gold nanoparticles self-assembling over (<b>A</b>) bare Si substrate without any amination after 24 h immersion, (<b>B</b>) aminated Si substrate after 11 h immersion, (<b>C</b>) aminated Si substrate after 18 h immersion and (<b>D</b>) aminated Si substrate after 24 h immersion (<b>E</b>) Higher magnified image of gold nanoparticles self-assembling over aminated Si substrate after 24 h immersion showing the formation of different nanoparticle systems—single nanosphere, nanodimer, nanotrimer, and nanotetramer (as highlighted by red circles).</p>
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<p>(<b>A</b>) Baseline corrected Raman spectrum of 1 mM methylene blue on bare SiO<sub>2</sub> surface and 1 µM methylene blue on SiO<sub>2</sub> surface self-assembled with gold nanoparticles at different immersion times. (<b>B</b>) Enhancement factor measured for two signature peaks of methylene blue at different immersion times in gold nanoparticle solution.</p>
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17 pages, 7313 KiB  
Article
Preliminary Prediction of Temperature Field and Thermal Hazards in the Water Diversion Tunnel of the “Yellow River to Xining” Project
by Hao Zhu, Yaru Wang, Wenjing Lin, Gaofan Yue, Zhining Liu, Feng Zhou and Lu Yang
Appl. Sci. 2025, 15(4), 1982; https://doi.org/10.3390/app15041982 - 14 Feb 2025
Abstract
As tunnel engineering advances towards greater depths, larger scales, and longer distances, high rock temperatures and tunnel thermal damage frequently occur, constituting some of the main geological hazards faced by transportation, water conservancy, and other tunnel engineering projects. In this study, we take [...] Read more.
As tunnel engineering advances towards greater depths, larger scales, and longer distances, high rock temperatures and tunnel thermal damage frequently occur, constituting some of the main geological hazards faced by transportation, water conservancy, and other tunnel engineering projects. In this study, we take the alternative option to the No.1 deep-buried water diversion tunnel of the “Diversion of Yellow River to Jining” project as the study area, combined with the geological data of the field investigation, to comprehensively consider the thermodynamic properties of the rocks along the tunnel and the logging data along the tunnel, and we use the least squares method to fit the temperature of the logging wells to obtain the thermal background parameters of the earth’s heat flow as well as other regional heat background parameters to obtain the thermal background parameters of the tunnel. The COMSOL Multiphysics software established a two-dimensional steady-state geothermal field numerical model to predict the rock temperature along the tunnel. The results show that the maximum temperature along the tunnel is 51.1 °C, the length of the tunnel with thermal damage class I is 45.9 km, the length of the tunnel with thermal damage class II is 18.4 km, the length of the tunnel with thermal damage class III is 8.0 km, and the length of the tunnel with thermal damage class IV is predicted to be 0.18 km. Compared with the on-site temperature measurement data, the model prediction error is within ±1.5 °C, which validates the accuracy of the model. This study adopts numerical simulation combined with field geological and logging data to provide a theoretical basis for tunnel heat hazard prevention. Meanwhile, it offers technical support for the design and construction of similar deep-buried high-temperature tunnels. Full article
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<p>Geologic overview map of the study area. 1—Qinghai Nanshan North Marginal Fracture; 2—Daotang River Fracture; 3—Hacheng Fracture; 4—Laji Mountain South Marginal Fracture; 5—Laji Mountain North Marginal Fracture.</p>
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<p>Natural seismic observation profiles along the Gongheof Qinghai-Yushu highway.</p>
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<p>Geometric model of the hole and its surrounding rocks. 1—Qinghai Nanshan North Marginal Fracture; 2—Daotang River Methodist Fracture; 3—Hacheng Fracture; 4—Laji Mountain South Marginal Fracture; 5—Laji Mountain North Marginal Fracture.</p>
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<p>Numerical simulation flowchart.</p>
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<p>Schematic diagram of model meshing.</p>
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<p>Temperature measurement curve of the temperature measurement well.</p>
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<p>Model bottom temperature.</p>
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<p>Cloud diagram of numerical simulation field of tunnel. 1—Qinghai Nanshan North Marginal Fracture; 2—Daotang River Fracture; 3—Hacheng Fracture; 4—Laji Mountain South Marginal Fracture; 5—Laji Mountain North Marginal Fracture.</p>
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<p>Comparison of actual and simulated temperatures of probe holes.</p>
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<p>Temperature profile of surrounding rock along the tunnel and thermal damage classification.</p>
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<p>Diagram of the temperature impact of different schemes.</p>
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19 pages, 10300 KiB  
Article
Research on Simulation Analysis and Joint Diagnosis Algorithm of Transformer Core-Loosening Faults Based on Vibration Characteristics
by Chen Cao, Zheng Li, Jialin Wang, Jiayu Zhang, Ying Li and Qingli Wang
Energies 2025, 18(4), 914; https://doi.org/10.3390/en18040914 - 13 Feb 2025
Abstract
The existing methods for transformer core-loosening fault diagnosis primarily focus on fundamental frequency analysis, neglecting higher-frequency components, which limits early detection accuracy. This study proposes a comprehensive approach integrating full-band vibration analysis, including high-order harmonics, to enhance diagnostic precision. A theoretical model coupling [...] Read more.
The existing methods for transformer core-loosening fault diagnosis primarily focus on fundamental frequency analysis, neglecting higher-frequency components, which limits early detection accuracy. This study proposes a comprehensive approach integrating full-band vibration analysis, including high-order harmonics, to enhance diagnostic precision. A theoretical model coupling magnetostriction and thermodynamics was developed, combined with empirical mode decomposition (EMD) and Pearson’s correlation coefficient for fault characterization. A 10 kV transformer core vibration test platform was constructed, capturing signals under normal, partially loose, and completely loose states. The simulation results aligned with the experimental data, showing vibration accelerations of 0.01 m/s2 (Phase A) and 0.023 m/s2 (Phase B). A multi-physics coupling model incorporating Young’s modulus variations simulated core loosening, revealing increased high-frequency components (up to 1000 Hz) and vibration amplitudes (0.2757 m/s2 for complete loosening). The joint EMD–Pearson method quantified fault severity, yielding correlation values of 0.0007 (normal), 0.0044 (partial loosening), and 0.0116 (complete loosening), demonstrating a clear positive correlation with fault progression. Experimental validation confirmed the model’s reliability, with the simulations matching the test results. This approach addresses the limitations of traditional methods by incorporating high-frequency analysis and multi-physics modeling, significantly improving early fault detection accuracy and providing a quantifiable diagnostic framework for transformer core health monitoring. Full article
(This article belongs to the Special Issue Design and Optimization of Power Transformer Diagnostics: 3rd Edition)
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<p>Three-dimensional view of the transformer.</p>
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<p>A simplified transformer model.</p>
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<p>Transformer mesh profiling model.</p>
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<p>Low-side three-phase power frequency voltage.</p>
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<p>Flux density distribution of core.</p>
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<p>The diagram of point selection.</p>
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<p>Vibration diagrams of acceleration at various points of the transformer: (<b>a</b>) time-domain plot of vibrational acceleration in three directions at point A; (<b>b</b>) frequency-domain plot of vibrational acceleration in three directions at point A; (<b>c</b>) time-domain plot of vibrational acceleration in three directions at point B; (<b>d</b>) frequency-domain plot of vibrational acceleration in three directions at point B; (<b>e</b>) time-domain plot of vibrational acceleration in three directions at point C; and (<b>f</b>) frequency-domain plot of vibrational acceleration in three directions at point C.</p>
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<p>Distribution of experimental measurement points.</p>
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<p>Phase A top vibration acceleration of the core.</p>
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<p>Phase B top vibration acceleration of the core.</p>
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<p>Phase A and C top frequency histogram.</p>
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<p>Frequency-domain diagram of the transformer core: (<b>a</b>) phase A of the transformer core and (<b>b</b>) phase C of the transformer core.</p>
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<p>Time-domain comparison between simulation results and test results: (<b>a</b>) comparison of transformer phase A simulation results and test results and (<b>b</b>) comparison of transformer phase B simulation results and test results.</p>
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<p>Schematic diagram of transformer core loosening: (<b>a</b>) complete loosening of transformer core and (<b>b</b>) partial loosening of transformer core.</p>
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<p>Time-domain diagram of normal core.</p>
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<p>Time-domain diagram of partially loosened core.</p>
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<p>Time-domain diagram of completely loosened core.</p>
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<p>Spectrum of different loosening states.</p>
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<p>EMD decomposition results for different loosening states of the transformer core: (<b>a</b>) empirical mode decomposition diagram of normalcy; (<b>b</b>) empirical mode decomposition diagram of partial loosening; and (<b>c</b>) empirical mode decomposition diagram of complete loosening.</p>
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32 pages, 16584 KiB  
Article
Sustainable Strategies for Improving Humanitarian Construction Through BIM and Climate Analysis
by Mwikilwa Mukamba Gladdys, Bigirimana Gentil and Ping Cao
Sustainability 2025, 17(4), 1556; https://doi.org/10.3390/su17041556 - 13 Feb 2025
Abstract
The growing need for effective and sustainable solutions in humanitarian construction has prompted scholars and practitioners to explore technical approaches that address the challenges of natural disasters, health emergencies, armed conflicts and migratory flows. These solutions often encompass temporary shelters, durable shelters and [...] Read more.
The growing need for effective and sustainable solutions in humanitarian construction has prompted scholars and practitioners to explore technical approaches that address the challenges of natural disasters, health emergencies, armed conflicts and migratory flows. These solutions often encompass temporary shelters, durable shelters and multifunctional buildings designed to balance rapid deployment, cultural sensitivity and environmental sustainability. However, the assessment of sustainability in humanitarian construction remains insufficiently defined due to the complexities of crises, the variability of local materials and the impact of local climatic conditions. This study aims to bridge this gap by integrating Building Information Modeling (BIM) and simulation tools such as COMSOL Multiphysics 6.0 to study sustainable strategies for humanitarian housing. Using case studies aligned with IFRC, UNHCR and CRL (Red Cross of Luxembourg) family shelter standards, the research assessed a Climate and Local Skill-Centered Design (CLCD) by examining the performance of key design elements, including wall material emissivity and reflectance, natural lighting, and energy efficiency within the context of indoor thermal comfort. Simulation results revealed that wall finishing material reflectance significantly influences average daylight factors (D), with variations of 2% to 5% linked to lower reflectance values and changes in the window-to-floor ratio (WFR). Conversely, thermal comfort metrics indicated minimal variations in heat discomfort hours, maintaining indoor temperatures between 19 °C and 25 °C, consistent with ASHRAE Standard 55 thermal comfort criteria. This paper underscores the importance of integrating advanced IT tools and green local techniques and materials to optimize humanitarian housing for health, comfort and environmental performance, offering actionable insights for future humanitarian sustainable designs. Full article
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<p>Overview of study approach.</p>
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<p>The purpose of a humanitarian shelter. Source: Authors’ own work, 2025.</p>
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<p>Humanitarian shelter project location in the Great Lakes region. Source: Authors’ own work, 2025.</p>
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<p>Materials application and geometry meshing. Source: Authors’ own work.</p>
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<p>Sketches of the CLCD-based design.</p>
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<p>Comfort zone based on weather condition. Source: Authors’ own work, 2025.</p>
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<p>Design strategies from Climate Consultant.</p>
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<p>Site weather data summary.</p>
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<p><b>Out</b>door average temperature.</p>
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<p><b>In</b>door average temperature.</p>
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<p>Heat transfer. (<b>a</b>) Outdoor radiation from 1 p.m. to 2 p.m. (<b>b</b>) Outdoor radiation at 3 p.m. (<b>c</b>) Cooling effect of clay ground. (<b>d</b>) Cooling effect of wall material.</p>
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<p>Surface-to-surface heat transfer. (<b>a</b>) Indoor cooling at 2 a.m. (<b>b</b>) Indoor cooling at 4 a.m. (<b>c</b>) Indoor cooling at 8 a.m. (<b>d</b>) Indoor cooling at 10 a.m. (<b>e</b>) Indoor cooling at 11 p.m. (<b>f</b>) Indoor cooling at 1 a.m.</p>
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<p>Surface-to-surface heat transfer. (<b>a</b>) Indoor cooling at 2 a.m. (<b>b</b>) Indoor cooling at 4 a.m. (<b>c</b>) Indoor cooling at 8 a.m. (<b>d</b>) Indoor cooling at 10 a.m. (<b>e</b>) Indoor cooling at 11 p.m. (<b>f</b>) Indoor cooling at 1 a.m.</p>
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<p>Comfortable and uncomfortable times of the day. (<b>a</b>) Indoor cooling 6 a.m.–10 a.m. (<b>b</b>) Indoor cooling 6 p.m.–10 p.m. (<b>c</b>) Indoor uncomfortable time 12 p.m. onwards. (<b>d</b>) Indoor uncomfortable time 3 p.m. onwards.</p>
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<p>Illuminance under the local weather conditions. (<b>a</b>) Hot hours from 12 a.m.to 3 p.m. (<b>b</b>) Shelter illuminance. (<b>c</b>) Shelter position. (<b>d</b>) Interior sunlight influence. (<b>e</b>) Outdoor shadows. (<b>f</b>) Indoor shadows.</p>
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<p>Daylighting index. (<b>a</b>) Indoor best light (4%). (<b>b</b>) Indoor good light (2% or above). (<b>c</b>) Indoor bad light (less than 2%).</p>
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<p>Sustainable green design. Source: Authors’ own work.</p>
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33 pages, 6763 KiB  
Article
Modified Dynamic Movement Primitive-Based Closed Ankle Reduction Technique Learning and Variable Impedance Control for a Redundant Parallel Bone-Setting Robot
by Zhao Tan, Yahui Zhang, Jiahui Yuan, Xu Song, Jialong Zhang, Guilin Wen, Xiaoyan Hu and Hanfeng Yin
Machines 2025, 13(2), 145; https://doi.org/10.3390/machines13020145 - 13 Feb 2025
Abstract
Traditional fracture reduction relies heavily on the surgeon’s experience, which hinders the transmission of skills. This specialization bottleneck, coupled with the high demands on physical strength, significantly limits the efficiency of daily treatments in trauma orthopedics. Currently, most fracture surgery robots focus on [...] Read more.
Traditional fracture reduction relies heavily on the surgeon’s experience, which hinders the transmission of skills. This specialization bottleneck, coupled with the high demands on physical strength, significantly limits the efficiency of daily treatments in trauma orthopedics. Currently, most fracture surgery robots focus on open or minimally invasive reduction techniques, which inherently carry the risk of iatrogenic damage due to surgical incisions or bone pin insertions. However, research in closed reduction-oriented robotic systems is remarkably limited. Addressing this gap, our study introduces a novel bone-setting robot for the closed reduction of ankle fractures designed with a redundant parallel platform. The parallel robot’s design incorporates three sliding redundancy actuators that enhance its tilt flexibility while maintaining load performance. Moreover, a singularity-free redundant kinematic solver has been developed, optimizing the robot’s operational efficacy. Building upon the demonstrations from professional closed reduction techniques, we propose the use of a multivariate Student-t process as a multi-output regression model within dynamic movement primitive for accurately learning stable reduction maneuvers. Additionally, we develop an anthropomorphic variable impedance controller based on inverse dynamics. The simulation results demonstrate convincingly that the developed ankle bone-setting robot is proficient in effectively replicating and learning the nuanced closed reduction techniques. Full article
(This article belongs to the Section Robotics, Mechatronics and Intelligent Machines)
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<p>Framework diagram of the bone-setting robot system. The blue dashed box outlines the experimental setup for the redundant parallel bone-setting robot. The red dashed box represents the learning process for the closed ankle reduction utilizing a modified dynamic movement primitive (DMP) algorithm. The purple dashed box highlights the variable impedance control framework proposed in this study.</p>
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<p>Ankle illustration. (<b>a</b>) The anatomical and physiological structure of the ankle complex. (<b>b</b>) The movements of the ankle.</p>
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<p>Classic closed reduction maneuvers. (<b>a</b>) Traction. (<b>b</b>) Inversion and lift.</p>
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<p>Schematic diagram of the bone-setting robot system. The red arrow points to the core component of the bone-setting robot system, while the blue arrow indicates the core component of the redundant parallel bone-setting robot.</p>
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<p>Process of robot bone-setting.</p>
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<p>Schematic diagram of redundant parallel platform. (<b>a</b>) Diagram of overall. (<b>b</b>) Moving platform. (<b>c</b>) Base. (<b>d</b>) Three-dimensional model.</p>
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<p>Flow chart of MV-TP-DMP.</p>
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<p>Effects of different coefficients on the variable stiffness function. (<b>a</b>) <span class="html-italic">c<sub>a</sub></span>. (<b>b</b>) <span class="html-italic">c<sub>b</sub></span>.</p>
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<p>Process of the bone-setting. (<b>a</b>) Pre-reduction. (<b>b</b>) Traction. (<b>c</b>) Inversion. (<b>d</b>) Lift. (<b>e</b>) End of reduction.</p>
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<p>Preoperative simulation for the process of bone-setting. (<b>a</b>) Pre-reduction. (<b>b</b>) Traction. (<b>c</b>) Inversion. (<b>d</b>) Lift. (<b>e</b>) End of reduction.</p>
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<p>Reproducing and generalizing tests of position and orientation trajectory for MV-TP-DMP. The gray lines represent the demo trajectories used for training, which are processed by DTW and denoised. The green lines denote the reference trajectories used for the reproduction test. The blue lines indicate the trajectories generated by the MV-TP-DMP algorithm during the reproduction test, while the red lines represent the trajectories produced by the algorithm in the generalization test. The reduction process is divided by using three phases, which correspond to “Traction”, “Inversion”, and “Lift”, respectively. (<b>a</b>–<b>c</b>) represent the position along the X, Y and Z axes, respectively. (<b>d</b>–<b>f</b>) are respectively three Euler angles.</p>
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<p>Additional disturbance forces.</p>
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<p>End-effector position and orientation trajectory under the control of constant impedance controller and variable impedance controller. The closed reduction process is divided using three phases, which correspond to “Traction”, “Inversion”, and “Lift”, respectively. (<b>a</b>–<b>c</b>) represent the position along the X, Y and Z axes, respectively. (<b>d</b>–<b>f</b>) are respectively three Euler angles.</p>
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<p>Variable impedance control test under disturbance. (<b>a</b>) Diagram of variable stiffness coefficient. (<b>b</b>) Tracking error diagram of position trajectory.</p>
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<p>Actual contact force <span class="html-italic">F<sub>I</sub></span> and torque <span class="html-italic">M<sub>I</sub></span> between humans and robots. (<b>a</b>) Actual contact force. (<b>b</b>) Actual contact torque.</p>
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<p>Trajectories of the actuators. (<b>a</b>) Prismatic actuators. (<b>b</b>) Sliding actuators.</p>
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<p>Forces in the actuators. (<b>a</b>) Forces of the prismatic actuators. (<b>b</b>) Forces of the sliding actuators.</p>
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17 pages, 1674 KiB  
Article
Optimizing Rice Field Yield with Deficit Irrigation to Support Fish Populations in River Ecosystems
by Mahdi Sedighkia and Bithin Datta
Water 2025, 17(4), 535; https://doi.org/10.3390/w17040535 - 13 Feb 2025
Abstract
This study presents a simulation–optimization framework that integrates deficit irrigation strategies with ecological considerations to mitigate the impact of water abstraction on potential fish populations in river ecosystems. The framework addresses two primary objectives: minimizing fish population loss, an ecological index reflecting environmental [...] Read more.
This study presents a simulation–optimization framework that integrates deficit irrigation strategies with ecological considerations to mitigate the impact of water abstraction on potential fish populations in river ecosystems. The framework addresses two primary objectives: minimizing fish population loss, an ecological index reflecting environmental impacts, and minimizing the yield reduction of rice crops caused by deficit irrigation. Regression models and adaptive neuro-fuzzy inference systems were employed to simulate the physical and water quality parameters of the river. Additionally, a multivariate linear regression model was developed to estimate potential fish populations using combined physical and water quality indices as inputs. Multi-objective particle swarm optimization was applied to achieve the defined objectives. Results from the case study demonstrate the model’s ability to balance ecological requirements with rice production through deficit irrigation. The ecological degradation of river ecosystems was found to be comparable during dry and normal years, while rice yield decreased by approximately 10% in dry years. Comparisons with unsustainable practices, where ecological flow was disregarded, revealed that significant reductions in rice production are inevitable to sustain river ecosystems. The proposed method provides a practical approach for achieving a fair balance between agricultural benefits and environmental sustainability in river basins, making it a valuable tool for water resource management. Full article
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Figure 1

Figure 1
<p>Workflow of the proposed method (in this workflow, V/D means flow velocity to depth, and IRWQI is a combined water quality index).</p>
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<p>Location of the water diversion project and rice fields, stream network, and land use (ST means hydrometric stations, Urban means urban point, Con sites means construction sites, Div dam means diversion dam, AG1 means agricultural area 1, AG2 means agricultural area 2, DFR means dense forests, LFR means low-density forests, MFR means medium-density forests, RG1 means potential grazing areas 1, GR2 means potential grazing areas 2, HU means lands related to residential areas). The name of non-translated region from upstream to downstream are Polsefid, Zirab, Shirgah, Ghameshahr, Kiakola, Behshahr and Arabkhil.</p>
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<p>Deficit irrigation function in the study area—yield (Kg/Ha). Triangles are observed/estimated irrigation/yield in practice.</p>
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<p>A description of the Iranian River Water Quality Index (IRWQI).</p>
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<p>Multi-objective particle swarm optimization (MOPSO) flowchart [<a href="#B19-water-17-00535" class="html-bibr">19</a>].</p>
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<p>Training and testing process of DO model.</p>
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<p>The multivariate linear regression model of the potential fish population (blue: observations; orange: simulations).</p>
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<p>Pareto front according to MOPSO (Blue circles with red line are dominant solutions).</p>
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<p>Pareto front according to MOPSO (Blue circles with red line are dominant solutions).</p>
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<p>Water use per unit and yield of production in two statuses (dry years).</p>
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<p>Water use per unit and yield of production in two statuses (normal years).</p>
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