[go: up one dir, main page]
More Web Proxy on the site http://driver.im/
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

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (2,183)

Search Parameters:
Keywords = drive losses

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
25 pages, 13628 KiB  
Article
Gradient Enhancement Techniques and Motion Consistency Constraints for Moving Object Segmentation in 3D LiDAR Point Clouds
by Fangzhou Tang, Bocheng Zhu and Junren Sun
Remote Sens. 2025, 17(2), 195; https://doi.org/10.3390/rs17020195 - 8 Jan 2025
Viewed by 234
Abstract
The ability to segment moving objects from three-dimensional (3D) LiDAR scans is critical to advancing autonomous driving technology, facilitating core tasks like localization, collision avoidance, and path planning. In this paper, we introduce a novel deep neural network designed to enhance the performance [...] Read more.
The ability to segment moving objects from three-dimensional (3D) LiDAR scans is critical to advancing autonomous driving technology, facilitating core tasks like localization, collision avoidance, and path planning. In this paper, we introduce a novel deep neural network designed to enhance the performance of 3D LiDAR point cloud moving object segmentation (MOS) through the integration of image gradient information and the principle of motion consistency. Our method processes sequential range images, employing depth pixel difference convolution (DPDC) to improve the efficacy of dilated convolutions, thus boosting spatial information extraction from range images. Additionally, we incorporate Bayesian filtering to impose posterior constraints on predictions, enhancing the accuracy of motion segmentation. To handle the issue of uneven object scales in range images, we develop a novel edge-aware loss function and use a progressive training strategy to further boost performance. Our method is validated on the SemanticKITTI-based LiDAR MOS benchmark, where it significantly outperforms current state-of-the-art (SOTA) methods, all while working directly on two-dimensional (2D) range images without requiring mapping. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Visualization of 2D image.</p>
Full article ">Figure 2
<p>Details of improved convolution methods.</p>
Full article ">Figure 3
<p>An overview of our method. The upper part illustrates the overall workflow of the network, while the lower part details the specific implementation of each submodule.</p>
Full article ">Figure 4
<p>Details of Depth Pixel Difference Convolution (DPDC).</p>
Full article ">Figure 5
<p>Qualitative comparisons of various methods for LiDAR-MOS in different scenes on the SemanticKITTI-MOS validation set are presented. Blue circles emphasize mispredictions and indistinct boundaries. For optimal viewing, refer to the images in color and zoom in for finer details.</p>
Full article ">Figure 6
<p>Qualitative comparisons of various methods for LiDAR-MOS between consecutive frames on the SemanticKITTI-MOS validation set are presented. Blue circles emphasize mispredictions and indistinct boundaries. For optimal viewing, refer to the images in color and zoom in for finer details.</p>
Full article ">
20 pages, 10880 KiB  
Article
Gate Driver for High-Frequency Power Converter
by Liron Cohen, Joseph B. Bernstein and Ilan Aharon
Electronics 2025, 14(2), 224; https://doi.org/10.3390/electronics14020224 - 7 Jan 2025
Viewed by 219
Abstract
This work explores the principle of utilizing gallium nitride devices as a gate driver for silicon carbide power devices. As silicon has long reached its performance limits, Wide Bandgap semiconductors such as gallium nitride and silicon carbide have emerged as promising alternatives due [...] Read more.
This work explores the principle of utilizing gallium nitride devices as a gate driver for silicon carbide power devices. As silicon has long reached its performance limits, Wide Bandgap semiconductors such as gallium nitride and silicon carbide have emerged as promising alternatives due to their superior characteristics. However, few publications suggest using a gallium nitride-based gate driver for silicon carbide, high-voltage power devices. Unlike standard voltage source gate drivers, this paper proposes a novel bi-polar current source resonant gate driver topology using gallium nitride transistors as a gate drive circuit for silicon carbide power switching. The driver receives a single input supply and pulsed width modulation signal, producing a high current bi-polar gate driving signal. The gate driver is validated by employing the proposed gate driver to a high-power silicon carbide transistor in a resonant boost converter. The experimental results show that the new gate driver recovers the gate charge wasted energy and provides high performances in varying high voltage loads at a 2.5 MHz switching frequency while reducing the gate losses by 26%. Full article
(This article belongs to the Special Issue New Trends in Power Electronics for Microgrids)
Show Figures

Figure 1

Figure 1
<p>Switching V–I characteristics of the power switch.</p>
Full article ">Figure 2
<p>Conventional voltage source gate driver.</p>
Full article ">Figure 3
<p>Basic resonant gate driver topology: (<b>a</b>) resonance during the gate-on transient [<a href="#B25-electronics-14-00224" class="html-bibr">25</a>] and (<b>b</b>) resonance in both the gate-on and the gate-off transient [<a href="#B26-electronics-14-00224" class="html-bibr">26</a>].</p>
Full article ">Figure 4
<p>RO-based converter.</p>
Full article ">Figure 5
<p>Timing circuit: (<b>a</b>) charge and (<b>b</b>) discharge.</p>
Full article ">Figure 6
<p>Elmore Delay ladder equivalent circuit.</p>
Full article ">Figure 7
<p>Inductor current curve.</p>
Full article ">Figure 8
<p>The mode of operation for driving the gate in all intervals: (<b>a</b>) t<sub>1</sub>, (<b>b</b>) t<sub>d</sub>, (<b>c</b>) t<sub>2</sub>, and (<b>d</b>) t<sub>c</sub>.</p>
Full article ">Figure 9
<p>The power losses in the resonant gate drive circuits.</p>
Full article ">Figure 10
<p>Principle of the gate drive circuit.</p>
Full article ">Figure 11
<p>Plan for full GaN driver on a chip.</p>
Full article ">Figure 12
<p>The photo of the proposed gate driver prototype.</p>
Full article ">Figure 13
<p>The RO output signal and gate driving signal.</p>
Full article ">Figure 14
<p>The standard gate driver turns ON at 2 MHz.</p>
Full article ">Figure 15
<p>The standard gate driver turns OFF at 2 MHz.</p>
Full article ">Figure 16
<p>The RO resonant gate driver turns OFF at 2 MHz.</p>
Full article ">Figure 17
<p>The RO resonant gate driver turns ON at 2 MHz.</p>
Full article ">Figure 18
<p>Measuring rise and fall times driving the RO resonant gate from the gate to the source: (<b>a</b>) turn ON transition and (<b>b</b>) turn OFF transition.</p>
Full article ">Figure 19
<p>RO Gate driving voltage and current signals with a SiC power switch drain to the source voltage and a drain current at 1.5 MHz.</p>
Full article ">Figure 20
<p>SiC running at 1000 V and 7.32 A peak—no load at 2 MHz.</p>
Full article ">Figure 21
<p>SiC running at 980 V and 8.6 A, with a peak at 2.54 MHz.</p>
Full article ">Figure 22
<p>SiC running at 522 V and 4.44 A, with a peak at 2.49 MHz.</p>
Full article ">
30 pages, 13622 KiB  
Article
Performance Simulation and Experimental Verification of a Low-Temperature Differential Free-Piston Stirling Air Conditioner Under Multi-Harmonic Drive
by Yajuan Wang, Junan Zhang, Junde Guo, Gao Zhang and Jianhua Zhang
Processes 2025, 13(1), 134; https://doi.org/10.3390/pr13010134 - 6 Jan 2025
Viewed by 344
Abstract
This study seeks to improve the performance of a low-temperature differential free-piston Stirling air conditioner (FPSAC). To achieve this, a novel approach is proposed, which replaces the conventional simple harmonic drive with a multi-harmonic drive. This modification aims to optimize the motion of [...] Read more.
This study seeks to improve the performance of a low-temperature differential free-piston Stirling air conditioner (FPSAC). To achieve this, a novel approach is proposed, which replaces the conventional simple harmonic drive with a multi-harmonic drive. This modification aims to optimize the motion of the driving piston, bringing it closer to the ideal movement pattern. The research involves both thermodynamic and dynamic coupling simulations of the FPSAC, complemented by experimental verification of its key performance parameters. A thermodynamic model for the gas medium, employing a quasi-one-dimensional dynamic approach for compressible fluids, and a nonlinear two-dimensional vibration dynamic model for the solid piston are developed, focusing on the low-temperature differential FPSAC physical model. The finite difference method is employed to numerically simulate the entire system, including the electromagnetic thrust of the multi-harmonic-driven linear oscillating motor, fluid transport equations, and the nonlinear dynamic equations of the power and gas control pistons. Variations in displacement, velocity, and pressure for each control volume at any given time are obtained, along with the indicator and temperature–entropy diagrams after the system stabilizes. The simulation results show that, in cooling mode, assuming no heat loss or mechanical friction, the Stirling cooler operates at a frequency of 80 Hz. Using the COPsin value for the simple harmonic drive as a baseline, performance is improved by altering the driving method. Under the multi-harmonic drive, the COPc5 increased by 10.03% and COPc7 by 14.23%. In heating mode, the COP under the multi-harmonic drive improved by 0.51% for COPh5 and 2.61% for COPh7. Performance experiments were conducted on the low-temperature differential FPSAC, and the key parameter test results showed good agreement with the simulation outcomes. The maximum deviation at the trough was found to be less than 2.45%, while at the peak, the maximum error did not exceed 3.61%. When compared to the simple harmonic drive, the application of the multi-harmonic drive significantly enhances the overall efficiency of the FPSAC, demonstrating its superior performance. The simulation analysis and experimental results indicate a significant improvement in the coefficient of performance of the Stirling cooler under the multi-harmonic drive at the same power level, demonstrating that the multi-harmonic drive is an effective approach for enhancing FPSAC performance. Furthermore, it should be noted that the method proposed in this study is applicable to other types of low-temperature differential free-piston Stirling air conditioners. Full article
(This article belongs to the Section Energy Systems)
Show Figures

Figure 1

Figure 1
<p>FPSAC model.</p>
Full article ">Figure 2
<p>Illustration of the one-dimensional discretization scheme applied to working space of FPSAC.</p>
Full article ">Figure 3
<p>Different waveforms. They should be listed as: (<b>a</b>)multi-harmonic; (<b>b</b>)ideal waveform.</p>
Full article ">Figure 4
<p>Cold-/hot-end heat exchanger structure.</p>
Full article ">Figure 5
<p>Energy balance of the regenerator matrix.</p>
Full article ">Figure 6
<p>Gradient-based counter flow boundary temperature.</p>
Full article ">Figure 7
<p>Top-level flow diagram of the simulation program.</p>
Full article ">Figure 8
<p>Displacement curves of the power piston and the displacer under harmonic drive. They should be listed as follows: (<b>a</b>) the displacement changes in the displacer and the power piston from startup to steady-state operation; (<b>b</b>) displacement diagrams of the power piston and the displacer over three cycles.</p>
Full article ">Figure 9
<p>Volume diagram of the expansion, compression, and total working chamber under harmonic drive. They should be listed as follows: (<b>a</b>) volume changes from startup to steady operation; (<b>b</b>) volume changes over three cycles.</p>
Full article ">Figure 10
<p>Pressure curve diagram of the expansion and compression chamber under harmonic drive. They should be listed as follows: (<b>a</b>) pressure changes from startup to steady operation; (<b>b</b>) pressure changes over three cycles.</p>
Full article ">Figure 11
<p>The <span class="html-italic">p–v</span> diagram of the expansion and compression chambers under harmonic drive. They should be listed as follows: (<b>a</b>) the <span class="html-italic">p–v</span> diagram of the compression chamber from startup to steady operation; (<b>b</b>) the <span class="html-italic">p–v</span> diagram of the expansion chamber from startup to steady operation.</p>
Full article ">Figure 12
<p>The <span class="html-italic">p–v</span> diagram of the indicated work for one cycle under harmonic drive. They should be listed as follows: (<b>a</b>) the <span class="html-italic">p–v</span> diagram of the indicated work for the compression chamber and expansion chamber; (<b>b</b>) the <span class="html-italic">p–v</span> diagram of the indicated work for the total working chamber.</p>
Full article ">Figure 13
<p>Temperature–entropy (<span class="html-italic">T–s</span>) diagram of the working chamber for one cycle under harmonic drive.</p>
Full article ">Figure 14
<p>Displacement diagrams under different harmonic drives.</p>
Full article ">Figure 15
<p>Pressure diagrams under different harmonic drives.</p>
Full article ">Figure 16
<p><span class="html-italic">p–v</span> diagram of the indicated work for the compression chamber over one cycle.</p>
Full article ">Figure 17
<p><span class="html-italic">p–v</span> diagram of the indicated work for the expansion chamber over one cycle.</p>
Full article ">Figure 18
<p><span class="html-italic">P–v</span> diagram of the indicated work for the total working chamber.</p>
Full article ">Figure 19
<p><span class="html-italic">T–s</span> diagram of temperature and entropy for one cycle.</p>
Full article ">Figure 20
<p><span class="html-italic">p–v</span> diagram of the indicated work for the total working chamber in heating mode.</p>
Full article ">Figure 21
<p><span class="html-italic">T–s</span> diagram for one cycle in heating mode.</p>
Full article ">Figure 22
<p>Experimental setup for pressure performance testing of FPSAC.</p>
Full article ">Figure 23
<p>Test bench for pressure performance testing of FPSAC.</p>
Full article ">Figure 24
<p>The pressure sensor (Hongmu Technology Co., Ltd., Nanjing, China).</p>
Full article ">Figure 25
<p>Comparison of experimental and simulation results for expansion chamber <span class="html-italic">p<sub>e</sub></span> and compression chamber <span class="html-italic">p<sub>c</sub></span>. They should be listed as follows: (<b>a</b>) harmonic drive; (<b>b</b>) third multi-harmonic drive; (<b>c</b>) fifth harmonic wave drive; (<b>d</b>) seventh harmonic wave drive.</p>
Full article ">
11 pages, 2717 KiB  
Article
The Pre-Polarization and Concentration of Cells near Micro-Electrodes Using AC Electric Fields Enhances the Electrical Cell Lysis in a Sessile Drop
by Kishor Kaphle and Dharmakeerthi Nawarathna
Biosensors 2025, 15(1), 22; https://doi.org/10.3390/bios15010022 - 6 Jan 2025
Viewed by 346
Abstract
Cell lysis is the starting step of many biomedical assays. Electric field-based cell lysis is widely used in many applications, including point-of-care (POC) applications, because it provides an easy one-step solution. Many electric field-based lysis methods utilize micro-electrodes to apply short electric pulses [...] Read more.
Cell lysis is the starting step of many biomedical assays. Electric field-based cell lysis is widely used in many applications, including point-of-care (POC) applications, because it provides an easy one-step solution. Many electric field-based lysis methods utilize micro-electrodes to apply short electric pulses across cells. Unfortunately, these cell lysis devices produce relatively low cell lysis efficiency as electric fields do not reach a significant portion of cells in the sample. Additionally, the utility of syringe pumps for flow cells in and out of the microfluidics channel causes cell loss and low throughput cell lysis. To address these critical issues, we suspended the cells in a sessile drop and concentrated on the electrodes. We used low-frequency AC electric fields (1 Vpp, 0–100 kHz) to drive the cells effectively towards electrodes and lysed using a short pulse of 10 V. A post-lysis analysis was performed using a hemocytometer, UV-vis spectroscopy, and fluorescence imaging. The results show that the pre-electric polarization of cells, prior to applying short electrical pulses, enhances the cell lysis efficiency. Additionally, the application of AC electric fields to concentrate cells on the electrodes reduces the assay time to about 4 min. In this study, we demonstrated that low-frequency AC electric fields can be used to pre-polarize and concentrate cells near micro-electrodes and improve cell lysis efficiency. Due to the simplicity and rapid cell lysis, this method may be suitable for POC assay development. Full article
(This article belongs to the Special Issue Lab-on-a-Chip Devices for Point-of-Care Diagnostics)
Show Figures

Figure 1

Figure 1
<p>Calculated electric field (<b>a</b>) and electric field gradients (<b>b</b>) in the vicinity of the interdigitated electrodes used for cell lysis experiments. Scale bars indicate 5 µm.</p>
Full article ">Figure 2
<p>Variation in cell lysis efficiency and cell count (after application lysis electric field) with experimental conditions used in the study. Control: cells from the tube left at room temperature; Immediate: immediately after pipetting cells on the electrodes; Gravity: settling cells under gravity; nDEP: after applying negative DEP and pDEP: after applying positive DEP.</p>
Full article ">Figure 3
<p>The quantification of nucleic acid (<b>a</b>) and protein molecules (<b>b</b>) in the buffer after concentrating cells on the electrodes using gravity settling, immediately after pipetting cell sample on the electrodes, applying nDEP, pDEP. For all these conditions, the cell samples were lysed applying 10 V pulse for 2 s.</p>
Full article ">Figure 4
<p>Concentration of cellular DNA on T-electrodes using AC electric fields. (<b>a</b>) Picture of interdigitated T-electrodes. (<b>b</b>–<b>d</b>) fluorescence images of T-electrodes after applying no electric potential, 10 Vpp (1 MHz), 10 Vpp (500 kHz), respectively. Scale bars show 10 µm.</p>
Full article ">Figure 5
<p>Concentration of cellular DNA on T-electrodes using AC electric fields (10 Vpp, 1 MHz). (<b>a</b>) Image of T-electrodes (from concentrated cells) without cell lysis. (<b>b</b>) Image of T-electrodes (from concentrated cells) on T-electrodes after electrical cell lysis. White circles show the concentrated DNA molecules on the electrodes. Scale bars show 20 µm.</p>
Full article ">
27 pages, 4210 KiB  
Article
Magnetic Field Distribution and Energy Losses in a Permanent Magnet Linear Synchronous Motor Under Stick-Slip Friction
by Paweł Olejnik, Yared D. Desta and Marcin Mydłowski
Energies 2025, 18(1), 191; https://doi.org/10.3390/en18010191 - 4 Jan 2025
Viewed by 551
Abstract
This study investigates the modeling and dynamic analysis of three coupled electromechanical systems, emphasizing interactions between a magnetic linear drive and frictional contact with flat springs. The experimental setup includes a table driven by a three-phase permanent magnet linear synchronous motor (PMLSM) using [...] Read more.
This study investigates the modeling and dynamic analysis of three coupled electromechanical systems, emphasizing interactions between a magnetic linear drive and frictional contact with flat springs. The experimental setup includes a table driven by a three-phase permanent magnet linear synchronous motor (PMLSM) using an LMCA4 inductor, LMCAS3 magnetic track, and Xenus XTL controller. Mechanical phenomena such as stick-slip friction and impulsive loads are observed, particularly due to the rapid buckling of flat springs. These springs transition between sliding friction and fixation, impacting the motor’s operation during reciprocating velocity trajectories and generating acoustic emissions. Numerical simulations using COMSOL Multiphysics evaluate the magnetic field and system geometry in two- and three-dimensional spaces. Key findings include mechanical stick-slip vibrations, numerical modeling of the linear drive, and comparative analysis of experimental and simulated inductor current variations. Additionally, energy loss mechanisms under irregular loading conditions are assessed. The results highlight the coupling between friction-induced current changes and magnetic field variations, elucidating their impact on motor efficiency, vibration propagation, and acoustic emissions. The study provides insights into optimizing the design and reliability of coreless linear motors for precision applications under discontinuous loading. Full article
Show Figures

Figure 1

Figure 1
<p>The dynamical coupling between the linear motor driving the table in a frictional contact with flexible flat springs. The following contact forces can be distinguished: <math display="inline"><semantics> <msub> <mi>R</mi> <mi>n</mi> </msub> </semantics></math>—normal reaction, <math display="inline"><semantics> <msub> <mi>F</mi> <mi>t</mi> </msub> </semantics></math>—tangential force, <math display="inline"><semantics> <msub> <mi>F</mi> <mi>f</mi> </msub> </semantics></math>—friction force. The table is subjected to a quasi periodic forcing generated by the motor. Two opposing laser sensors (L) measure the vibrations of both flat springs.</p>
Full article ">Figure 2
<p>Experimental dynamic response of the double-spring system in frictional contact governed by a stick-slip phenomenon with a table driven by a magnetic linear motor, with two different normal loads <math display="inline"><semantics> <msubsup> <mi>F</mi> <mi>e</mi> <mrow> <mo>(</mo> <mi>I</mi> <mo>,</mo> <mi>I</mi> <mi>I</mi> <mo>)</mo> </mrow> </msubsup> </semantics></math> applied to the table.</p>
Full article ">Figure 3
<p>Schematics of the control system of the LMCAS3 Ironless Linear Motor.</p>
Full article ">Figure 4
<p>Variation of actual coil current <math display="inline"><semantics> <msubsup> <mi>I</mi> <mi>m</mi> <mrow> <mo>(</mo> <mi>E</mi> <mo>)</mo> </mrow> </msubsup> </semantics></math> measured on the experimental stand.</p>
Full article ">Figure 5
<p>Variation of actual velocity of the forcer <span class="html-italic">v</span> measured on the experimental stand under the following conditions: (i) no external load, (ii) the first level external load <math display="inline"><semantics> <msubsup> <mi>R</mi> <mi>e</mi> <mrow> <mo>(</mo> <mn>1</mn> <mo>)</mo> </mrow> </msubsup> </semantics></math>, (iii) the second level external load <math display="inline"><semantics> <msubsup> <mi>F</mi> <mi>e</mi> <mrow> <mo>(</mo> <mi>I</mi> <mi>I</mi> <mo>)</mo> </mrow> </msubsup> </semantics></math>.</p>
Full article ">Figure 6
<p>Simple configuration of the LMCAS3 ironless linear motor.</p>
Full article ">Figure 7
<p>3-D model view of constant distribution of magnets implemented in COMSOL.</p>
Full article ">Figure 8
<p>Magnetic flux density in the stator, inductor and around the linear motor.</p>
Full article ">Figure 9
<p>Time-varying magnetic flux density norm distribution along a horizontal line.</p>
Full article ">Figure 10
<p>Variation of numerically simulated coil current <math display="inline"><semantics> <msubsup> <mi>I</mi> <mi>m</mi> <mrow> <mo>(</mo> <mi>Num</mi> <mo>)</mo> </mrow> </msubsup> </semantics></math> (blue line) with reference to measurement <math display="inline"><semantics> <msubsup> <mi>I</mi> <mi>m</mi> <mrow> <mo>(</mo> <mi>Exp</mi> <mo>)</mo> </mrow> </msubsup> </semantics></math> (black line) on the experimental stand for various levels of extra loads (I and II) exerted by the flat springs in stick-slip frictional contact between the table and ends of the springs.</p>
Full article ">Figure 11
<p>Numerical distribution of the 3-D magnetic field <math display="inline"><semantics> <mi mathvariant="bold-italic">B</mi> </semantics></math> of the investigated linear motor.</p>
Full article ">Figure 12
<p>Two-dimensional numerical distribution of induced eddy currents as streamlines and losses (W m<sup>−2</sup>) in the linear motor subjected to mechanical loading from the plate in stick-slip frictional contact at <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mi>m</mi> </msub> <mo>=</mo> </mrow> </semantics></math> 5 Hz.</p>
Full article ">
33 pages, 3394 KiB  
Review
Mechanisms of Rhodopsin-Related Inherited Retinal Degeneration and Pharmacological Treatment Strategies
by Maria Azam and Beata Jastrzebska
Cells 2025, 14(1), 49; https://doi.org/10.3390/cells14010049 - 4 Jan 2025
Viewed by 439
Abstract
Retinitis pigmentosa (RP) is a hereditary disease characterized by progressive vision loss ultimately leading to blindness. This condition is initiated by mutations in genes expressed in retinal cells, resulting in the degeneration of rod photoreceptors, which is subsequently followed by the loss of [...] Read more.
Retinitis pigmentosa (RP) is a hereditary disease characterized by progressive vision loss ultimately leading to blindness. This condition is initiated by mutations in genes expressed in retinal cells, resulting in the degeneration of rod photoreceptors, which is subsequently followed by the loss of cone photoreceptors. Mutations in various genes expressed in the retina are associated with RP. Among them, mutations in the rhodopsin gene (RHO) are the most common cause of this condition. Due to the involvement of numerous genes and multiple mutations in a single gene, RP is a highly heterogeneous disease making the development of effective treatments particularly challenging. The progression of this disease involves complex cellular responses to restore cellular homeostasis, including the unfolded protein response (UPR) signaling, autophagy, and various cell death pathways. These mechanisms, however, often fail to prevent photoreceptor cell degradation and instead contribute to cell death under certain conditions. Current research focuses on the pharmacological modulation of the components of these pathways and the direct stabilization of mutated receptors as potential treatment strategies. Despite these efforts, the intricate interplay between these mechanisms and the diverse causative mutations involved has hindered the development of effective treatments. Advancing our understanding of the interactions between photoreceptor cell death mechanisms and the specific genetic mutations driving RP is critical to accelerate the discovery and development of therapeutic strategies for this currently incurable disease. Full article
(This article belongs to the Special Issue New Advances in Neuroinflammation)
Show Figures

Figure 1

Figure 1
<p>Schematic rod photoreceptor and rhodopsin structure. (<b>A</b>) The schematic representation of the rod photoreceptor cell (left panel) and a close-up of rod outer segment disc membranes with rhodopsin (Rho) molecules. (<b>B</b>) The structure of bovine Rho. The PDB ID:1GZM was used to show the side view of bovine Rho in the dark state. Transmembrane helices are labeled TM1–7. Cytoplasmic helix 8 is labeled H8. Extracellular (intradiscal) loops connecting TM helices on the ligand-binding site of the receptor are labeled ECL1, ECL2, and ECL3. Intracellular (cytoplasmic) loops, connecting TM helices on the effector binding site of the receptor are labeled ICL1, ICL2, and ICL3. 11-<span class="html-italic">cis</span>-retinal is shown as red sticks. The location of residues mutated in retinitis pigmentosa (RP) is shown in orange. (<b>C</b>) Two-dimensional representation of human Rho structure. Residues mutated in RP are indicated with orange circles. The Lys296, which covalently binds the 11-<span class="html-italic">cis</span>-retinal, is shown with a yellow circle filled with orange. The P23H mutation is shown with a red circle filled with orange.</p>
Full article ">Figure 2
<p>Unfolded protein response. The unfolded protein response (UPR) involves three primary sensor receptors within the ER membranes: protein kinase RNA-like ER kinase (PERK), inositol-requiring enzyme 1 (IRE1), and activating transcription factor 6 (ATF6). PERK phosphorylates eIF2α, which reduces protein translation and upregulates ATF4 transcription factor, which activates the expression of antioxidants and components of the ER-associated degradation ERAD signaling. Activated by unfolded proteins, IRE1 activates transcription factor sXBP1 which stimulates the synthesis of protein folding regulators, ERAD, and lipid biosynthesis. ATF6 (P90), upon activation, translocates to the Golgi apparatus, where it is cleaved to P50 form by proteases S1P and S2P. Cleaved ATF6 stimulates the expression of ERAD and folding regulators.</p>
Full article ">Figure 3
<p>Schematic interplay between oxidative stress, inflammation, and photoreceptor cell death. Oxidative radicals are generated during respiration in mitochondria. Under normal physiological conditions, superoxide dismutase (SOD) catalyzes superoxide radicals (<sup>1</sup>O<sub>2</sub>) into hydrogen peroxide (H<sub>2</sub>O<sub>2</sub>) and oxygen (O<sub>2</sub>), while catalase breaks down hydroxyl radicals ·OH to water (H<sub>2</sub>O) and O<sub>2</sub>. H<sub>2</sub>O<sub>2</sub> is converted by glutathione peroxidase to H<sub>2</sub>O. During this reaction, GSH is converted to its reduced form GSSH. The back conversion of GSSH → GSH involves NADPH → NAD<sup>+</sup> change. Excess of reactive oxygen species (ROS) accumulated under chronic conditions of genetic mutation leads to damage of cellular content and release of pro-inflammatory markers that aggravate inflammation, ultimately leading to cell death.</p>
Full article ">Figure 4
<p>Classical inflammation and pyroptosis signaling. In classical inflammation, damage-associated molecular patterns (DAMPs) activate phosphorylation of IκB kinase (IKK), which degrades IκB from the IκB/NFκB complex leading to the activation of NFκB. Activated NFκB stimulates the expression of proinflammatory cytokines, including IL-1β, IL-18, and TNF-α, as well as the expression of NLRP3, which leads to the formation of inflammasome. In addition, chemokine receptor CX3CR1 activated by CX3CL1 stimulates NFκB through G protein signaling. Pyroptosis is activated by DAMPs through death receptors; for example, tumor necrosis factor receptors (TNFR1 and TNRF2), which stimulate the expression of NOD-like receptor protein 3 (NLRP3) and inflammasome formation that activates caspase-1, which activates IL-1β and IL-18. Alternatively, pyroptosis is activated through Toll-like receptor 4 (TLR4) stimulated by bacterial lipopolysaccharides (LPS). Caspase-4 and -5 are activated in this pathway leading to the activation of gasdermin (GSDMD), which inserts into the membrane forming a pore that allows for the release of pro-inflammatory cytokines activated by caspase-1.</p>
Full article ">Figure 5
<p>Apoptosis pathway. Extrinsic apoptosis is activated by extrinsic signals through death receptors (TNFRs), which recruit adaptor proteins like the Fas-associated death domain (FADD), followed by pro-caspase-8 activation. Active caspase-8 directly stimulates executioner caspase-3 and -7, leading to apoptosis. Caspase-8 can also stimulate BID, which activates BAX and BAK to permeabilize the mitochondrial membrane, linking the extrinsic and intrinsic pathways. The intrinsic pathway is activated by cellular stressors like damaged DNA or oxidative stress, which activates BAX and BAK. Permeabilized mitochondria release cytochrome c, which binds to apoptotic protease activating factor APAF1 and triggers activation of caspase-9 followed by activation of executioner caspase-3 and -7.</p>
Full article ">Figure 6
<p>Necroptosis signaling. Necroptosis is triggered by the activation of death receptors, particularly tumor necrosis factor receptor 1 (TNFR1) upon binding of TNF-α. It could also be activated by Toll-receptor 4 (TLR4). TNFR1 recruits adaptor proteins TRADD, TRAF2, and RIPK1. In apoptosis, receptor-interacting protein kinase-1 (RIPK1) is polyubiquitinated and promotes cell survival. When caspase-8 is blocked, RIPK1 interacts with RIPK3, forming a necrosome complex. RIPK3 autophosphorylates and then phosphorylates mixed-lineage kinase domain-like protein (MLKL), a necroptosis key effector, which isomerizes and translocates to the membrane where it forms a pore enabling the release of cellular content. This can further lead to the activation of inflammatory response through released DAMPs.</p>
Full article ">Figure 7
<p>Ferroptosis signaling. Cellular iron is imported via the transferrin receptor (TFR1), which binds Fe<sup>3+</sup> (ferric iron)-loaded transferrin. Inside the cell, Fe<sup>3+</sup> became reduced to Fe<sup>2+</sup> (ferrous iron). Free Fe<sup>2+</sup> can catalyze the Fenton reaction leading to the generation of reactive oxygen species (ROS) production, which oxidizes unsaturated membrane phospholipids. Under normal physiological conditions, an antioxidant system involving glutathione peroxidase (GPx) prevents lipid peroxidation using its cofactor GSH, which is generated in exchange for glutamate transported out of the cell through the antiporter SLC7A11. Under chronic stress of pathogenic mutations, unchecked lipid peroxidation disrupts membrane integrity and leads to photoreceptor cell death.</p>
Full article ">
18 pages, 1166 KiB  
Review
The Role of Fractalkine in Diabetic Retinopathy: Pathophysiology and Clinical Implications
by Cheng-Yung Lee and Chang-Hao Yang
Int. J. Mol. Sci. 2025, 26(1), 378; https://doi.org/10.3390/ijms26010378 - 4 Jan 2025
Viewed by 309
Abstract
Diabetic retinopathy (DR) is a complication of diabetes, characterized by progressive microvascular dysfunction that can result in vision loss. Chronic hyperglycemia drives oxidative stress, endothelial dysfunction, and inflammation, leading to retinal damage and complications such as neovascularization. Current treatments, including anti-VEGF agents, have [...] Read more.
Diabetic retinopathy (DR) is a complication of diabetes, characterized by progressive microvascular dysfunction that can result in vision loss. Chronic hyperglycemia drives oxidative stress, endothelial dysfunction, and inflammation, leading to retinal damage and complications such as neovascularization. Current treatments, including anti-VEGF agents, have limitations, necessitating the exploration of alternative therapeutic strategies. Fractalkine (CX3CL1), a chemokine with dual roles as a membrane-bound adhesion molecule and a soluble chemoattractant, has emerged as a potential therapeutic target. Its receptor, CX3CR1, is expressed on immune cells and mediates processes such as immune cell recruitment and microglial activation through intracellular signaling pathways. In DR, soluble fractalkine plays critical roles in retinal inflammation, angiogenesis, and neuroprotection, balancing tissue damage and repair. In DR, elevated fractalkine levels are associated with retinal inflammation and endothelial dysfunction. Experimental studies suggest that fractalkine deficiency exacerbates the severity of diabetic retinopathy (DR), whereas exogenous fractalkine appears to reduce inflammation, oxidative stress, and neuronal damage. However, its role in pathological angiogenesis within DR remains unclear and warrants further investigation. Preclinical evidence indicates that fractalkine may hold therapeutic potential, particularly in mitigating tissue injury and inflammation associated with early-stage DR. Full article
Show Figures

Figure 1

Figure 1
<p>An illustration of membrane-bound fractalkine, soluble fractalkine, and the fractalkine receptor (CX3CR1). (<b>A</b>) Membrane-bound fractalkine (mFKN) is a membrane protein consisting of 373 amino acids, structured into four distinct domains: N-terminal, mucin-like, transmembrane, and cytoplasmic domains. It is primarily expressed on vascular endothelial cells and certain immune cells, playing a critical role in recruiting immune cells to inflamed tissues. (<b>B</b>) Soluble fractalkine (sFKN) is generated by the cleavage of mFKN via the enzymes ADAM10 and ADAM17. It consists of the N-terminal and mucin-like domains. sFKN is somehow more relevant to diabetic retinopathy pathophysiology than mFKN. (<b>C</b>) The fractalkine receptor (CX3CR1) is a G-protein-coupled receptor (GPCR) characterized by seven transmembrane alpha helices. Its activation triggers downstream signaling pathways typical of GPCRs, including PLC/IP3, JAK/STAT, RAS/RAF/MEK, and PI3K/Akt, mediating immune responses, inflammation, and angiogenesis.</p>
Full article ">Figure 2
<p>The roles of fractalkine in diabetic retinopathy. (<b>A</b>) In the diabetic retina, fractalkine is expressed by injured inner retinal neurons, specifically retinal ganglion cells. Membrane-bound fractalkine is cleaved into its soluble form. Microglia are the only retinal cell type that express the fractalkine receptor, CX3CR1. In diabetic retinopathy (DR), microglia become activated, adopt an amoeboid morphology, and lose their stabilizing influence on retinal capillaries, leading to fibrin or fibrinogen extravasation. Activated microglia also secrete pro-inflammatory mediators, including IL-6, TNF-α, and IL-1β, exacerbating retinal inflammation and neuronal damage. (<b>B</b>) Exogenous soluble fractalkine (sFKN) application signals microglia via CX3CR1, inducing a homeostatic state. Microglia morphology is restored, with branched and elongated processes, and the secretion of pro-inflammatory mediators is reduced. Consequently, tissue inflammation and neuronal injury are alleviated. The connection between microglia and capillaries is re-established, decreasing fibrin and fibrinogen leakage. However, the impact of fractalkine on diabetic retinal neovascularization remains poorly understood.</p>
Full article ">
26 pages, 4452 KiB  
Article
Research on Traffic Accident Severity Level Prediction Model Based on Improved Machine Learning
by Jiming Tang, Yao Huang, Dingli Liu, Liuyuan Xiong and Rongwei Bu
Systems 2025, 13(1), 31; https://doi.org/10.3390/systems13010031 - 4 Jan 2025
Viewed by 401
Abstract
Traffic accidents occur frequently, causing significant losses to people’s lives and property safety. Accurately predicting the severity level of traffic accidents is of great significance. Based on traffic accident data, this study comprehensively considers various influencing factors such as the geographical location, road [...] Read more.
Traffic accidents occur frequently, causing significant losses to people’s lives and property safety. Accurately predicting the severity level of traffic accidents is of great significance. Based on traffic accident data, this study comprehensively considers various influencing factors such as the geographical location, road conditions, and environment. The data are divided into accident-related categories, weather-related categories, and road- and environment-related categories. The machine learning method is improved through integration for the accident level prediction. In the experiment, effective preprocessing measures were taken for problems such as data imbalance, missing values, the encoding of categorical variables, and the standardization of numerical features. The unbalanced distribution of “Severity” was improved through under-sampling and over-sampling techniques. Firstly, we adopted a multi-stage fusion strategy. A multi-layer perceptron (MLP) was used for the preliminary prediction, and then its result was combined with the original features to form a new feature. Decision tree, XGBoost, and random forest algorithms, respectively, were applied for the secondary prediction. The analysis results show that the improved machine learning model is significantly superior to a single model in the overall performance. The “MLP + random forest” model performs well in evaluation indicators such as the accuracy, recall rate, and F1 value. The accuracy rate is as high as 94%. In the prediction of different traffic accident severity levels (minor, moderate, and severe), the improved machine learning model also generally shows better performance and stability. The research results of this study have broad prospects in the field of intelligent driving. It can realize real-time accident prediction and early warnings, and provide decision support for drivers and autonomous driving systems. The research also provides a scientific basis for traffic planning and management departments to improve driving conditions and reduce the probability and losses of traffic accidents. Full article
Show Figures

Figure 1

Figure 1
<p>Method flowchart for the whole work.</p>
Full article ">Figure 2
<p>MLP structure diagram.</p>
Full article ">Figure 3
<p>Decision tree flowchart.</p>
Full article ">Figure 4
<p>XGBoost flowchart.</p>
Full article ">Figure 5
<p>Random forest principle diagram.</p>
Full article ">Figure 6
<p>Sample distribution.</p>
Full article ">Figure 7
<p>Accident-related features.</p>
Full article ">Figure 8
<p>Weather-related features.</p>
Full article ">Figure 9
<p>Road- and Environment-related features.</p>
Full article ">Figure 10
<p>Confusion matrix before and after the improvement.</p>
Full article ">Figure 11
<p>ROC curve diagram.</p>
Full article ">Figure 12
<p>PR curve comparison diagram.</p>
Full article ">Figure 13
<p>Sensitivity analysis of the features.</p>
Full article ">
22 pages, 34247 KiB  
Article
Habitat Quality Dynamics in Urumqi over the Last Two Decades: Evidence of Land Use and Land Cover Changes
by Siying Chen, Ümüt Halik, Lei Shi, Wentao Fu, Lu Gan and Martin Welp
Land 2025, 14(1), 84; https://doi.org/10.3390/land14010084 - 3 Jan 2025
Viewed by 324
Abstract
The integrity of habitat quality is a pivotal cornerstone for the sustainable advancement of local ecological systems. Rapid urbanization has led to habitat degradation and loss of biodiversity, posing severe threats to regional sustainability, particularly in extremely vulnerable arid zones. However, systematic research [...] Read more.
The integrity of habitat quality is a pivotal cornerstone for the sustainable advancement of local ecological systems. Rapid urbanization has led to habitat degradation and loss of biodiversity, posing severe threats to regional sustainability, particularly in extremely vulnerable arid zones. However, systematic research on the assessment indicators, limiting factors, and driving mechanisms of habitat quality in arid regions is notably lacking. This study takes Urumqi, an oasis city in China’s arid region, as a case study and employs the InVEST and PLUS models to conduct a dynamic evaluation of habitat quality in Urumqi from 2000 to 2022 against the backdrop of land use changes. It also simulates habitat quality under different scenarios for the year 2035, exploring the temporal and spatial dynamics of habitat quality and its driving mechanisms. The results indicate a decline in habitat quality. The habitat quality in the southern mountainous areas is significantly superior to that surrounding the northern Gurbantunggut Desert, and it exhibits greater stability. The simulation and prediction results suggest that from 2020 to 2035, habitat degradation will be mitigated under Ecological Protection scenarios, while the decline in habitat quality will be most pronounced under Business-As-Usual scenarios. The spatial distribution of habitat quality changes in Urumqi exhibits significant autocorrelation and clustering, with these patterns intensifying over time. The observed decline in habitat quality in Urumqi is primarily driven by anthropogenic activities, urban expansion, and climate change. These factors have collectively contributed to significant alterations in the landscape, leading to the degradation of ecological conditions. To mitigate further habitat quality loss and support sustainable development, it is essential to implement rigorous ecological protection policies, adopt effective ecological risk management strategies, and promote the expansion of ecological land use. These actions are crucial for stabilizing and improving regional habitat quality in the long term. Full article
Show Figures

Figure 1

Figure 1
<p>Sketch map of study area. (<b>a</b>) illustrates the geographical position of Urumqi, Xinjiang, within China; (<b>b</b>) presents the spatial distribution of different land use categories in Urumqi in 2022.</p>
Full article ">Figure 2
<p>Technology road map for land use modeling and habitat quality evaluation.</p>
Full article ">Figure 3
<p>Development probability of various types of land.</p>
Full article ">Figure 4
<p>Comparing real and simulated land use in 2020. The simulated spatial distribution of land use exhibits discrepancies primarily in the central urban area (<b>A</b>) and two ecological transition zones (<b>B</b>,<b>C</b>). Consequently, (<b>A</b>) depicts an enlarged view of the central urban area, (<b>B</b>) provides an enlarged view of the southwestern region, and (<b>C</b>) presents an enlarged view of the southeastern region.</p>
Full article ">Figure 5
<p>Conversion of land use types, 2000–2022.</p>
Full article ">Figure 6
<p>Spatial distribution of land use in different scenarios for 2035.</p>
Full article ">Figure 7
<p>Transformation of land use in 2022–2035.</p>
Full article ">Figure 8
<p>Quantitative changes in habitat quality level.</p>
Full article ">Figure 9
<p>Spatial distribution of habitat quality from 2000 to 2022.</p>
Full article ">Figure 10
<p>Spatial variation in habitat quality from 2000 to 2022. (<b>a</b>) Spatial pattern of habitat quality grade shift. (<b>b</b>) Spatial changes in habitat quality. (<b>c</b>) Spatiotemporal characterization of HQ cold spots and hot spots.</p>
Full article ">Figure 11
<p>Habitat quality in different scenarios for 2035. (<b>A</b>) represents the magnified view of the southwestern area, while (<b>B</b>) depicts the magnified view of the southeastern area.</p>
Full article ">Figure 12
<p>Contribution of driving factors by land use type.</p>
Full article ">
15 pages, 6267 KiB  
Article
Efficiency Optimization of the Main Operating Points of an EV Traction Motor
by Gi-haeng Lee and Yong-min You
Appl. Sci. 2025, 15(1), 368; https://doi.org/10.3390/app15010368 - 2 Jan 2025
Viewed by 392
Abstract
Motor efficiency presents a trade-off between low-speed and high-speed regions. Additionally, the cross-sectional area of hairpin motors employing rectangular wires is larger than that of round wires, thereby amplifying AC copper losses. As the operating speed increases, the AC copper loss also becomes [...] Read more.
Motor efficiency presents a trade-off between low-speed and high-speed regions. Additionally, the cross-sectional area of hairpin motors employing rectangular wires is larger than that of round wires, thereby amplifying AC copper losses. As the operating speed increases, the AC copper loss also becomes more pronounced; therefore, efficiently determining the optimal design point considering these characteristics is essential. This study optimizes the efficiency of an electric vehicle (EV) simulation is conducted using MATLAB 2024, and the main operating points according to the driving cycle are selected. For the EV simulation to select the main operating points, the driving cycle of the multi-cycle test method, which is used for measuring domestic driving range, is considered to enhance the validity of the operating points. The efficiency optimization of the main operating points was performed considering the AC copper loss, and essential parameters such as the torque ripple and total harmonic distortion of the back-electromotive force were incorporated as constraints. Furthermore, the predictive performances of the 11 metamodels were compared to identify the most suitable metamodel for the output and design variables. Subsequently, the selected metamodel was integrated with four optimization algorithms to optimize the design. Full article
(This article belongs to the Section Electrical, Electronics and Communications Engineering)
Show Figures

Figure 1

Figure 1
<p>Initial model.</p>
Full article ">Figure 2
<p>Main operating point selection process.</p>
Full article ">Figure 3
<p>Vehicle dynamics.</p>
Full article ">Figure 4
<p>UDDS and HWFET driving cycles.</p>
Full article ">Figure 5
<p>Operating points EV simulation.</p>
Full article ">Figure 6
<p>Operating point density.</p>
Full article ">Figure 7
<p>Optimal design process.</p>
Full article ">Figure 8
<p>Shape of design variables.</p>
Full article ">Figure 9
<p>Efficiency in main operating points.</p>
Full article ">Figure 10
<p>Back-EMF waveforms.</p>
Full article ">Figure 11
<p>Magnetic flux lines (<b>a</b>) initial model (<b>b</b>) optimal model.</p>
Full article ">
14 pages, 6956 KiB  
Article
Enhanced Inversion of Sound Speed Profile Based on a Physics-Inspired Self-Organizing Map
by Guojun Xu, Ke Qu, Zhanglong Li, Zixuan Zhang, Pan Xu, Dongbao Gao and Xudong Dai
Remote Sens. 2025, 17(1), 132; https://doi.org/10.3390/rs17010132 - 2 Jan 2025
Viewed by 315
Abstract
The remote sensing-based inversion of sound speed profile (SSP) enables the acquisition of high-spatial-resolution SSP without in situ measurements. The spatial division of the inversion grid is crucial for the accuracy of results, determining both the number of samples and the consistency of [...] Read more.
The remote sensing-based inversion of sound speed profile (SSP) enables the acquisition of high-spatial-resolution SSP without in situ measurements. The spatial division of the inversion grid is crucial for the accuracy of results, determining both the number of samples and the consistency of inversion relationships. The result of our research is the introduction of a physics-inspired self-organizing map (PISOM) that facilitates SSP inversion by clustering samples according to the physical perturbation law. The linear physical relationship between sea surface parameters and the SSP drives dimensionality reduction for the SOM, resulting in the clustering of samples exhibiting similar disturbance laws. Subsequently, samples within each cluster are generalized to construct the topology of the solution space for SSP reconstruction. The PISOM method significantly improves accuracy compared with the SOM method without clustering. The PISOM has an SSP reconstruction error of less than 2 m/s in 25% of cases, while the SOM method has none. The transmission loss calculation also shows promising results, with an error of only 0.5 dB at 30 km, 5.5 dB smaller than that of the SOM method. A physical interpretation of the neural network processing confirms that physics-inspired clustering can bring better precision gains than the previous spatial grid. Full article
(This article belongs to the Special Issue Artificial Intelligence for Ocean Remote Sensing)
Show Figures

Figure 1

Figure 1
<p>SSP samples and background profile.</p>
Full article ">Figure 2
<p>Flow chart of the physics-inspired SOM inversion. The black italicized variable represents the input parameters extracted from the training samples; the blue italicized variable denotes the input parameters utilized for solution information; and the red italicized variable signifies the output parameters serving as the reconstruction coefficients of the SSP.</p>
Full article ">Figure 3
<p>Errors in reconstruction for different sample numbers.</p>
Full article ">Figure 4
<p>Errors in reconstruction for different depths.</p>
Full article ">Figure 5
<p>Examples of sound speed profile reconstruction.</p>
Full article ">Figure 6
<p>Transmission loss calculated using different SSPs, (<b>a</b>) SSPs, (<b>b</b>) Transmission loss.</p>
Full article ">Figure 7
<p>Spatial distribution of two sample clusters.</p>
Full article ">Figure 8
<p>Temporal distribution of two sample clusters.</p>
Full article ">
15 pages, 5913 KiB  
Article
Research on Self-Excited Inverter Rectification Method of Receiver in Wireless Power Transfer System
by Suqi Liu, Xueying Yan, Gang Wang and Yuping Liu
Processes 2025, 13(1), 89; https://doi.org/10.3390/pr13010089 - 2 Jan 2025
Viewed by 421
Abstract
To decrease the complexity and increase the efficiency of wireless power transfer (WPT) systems, this paper proposes a novel self-excited invert rectification method for the design of the invert rectifier of the receiver (Rx). The self-excited invert rectifier can perform the self-driving and [...] Read more.
To decrease the complexity and increase the efficiency of wireless power transfer (WPT) systems, this paper proposes a novel self-excited invert rectification method for the design of the invert rectifier of the receiver (Rx). The self-excited invert rectifier can perform the self-driving and soft-switching of the MOSFETs as well as the frequency-tracking function without a microcontroller. This allows us to greatly simplify the structure of the invert rectifier and increase the transfer efficiency (TE) of the WPT system. Firstly, a self-excited invert rectifier circuit is designed, and a self-excited invert rectification method is studied. Additionally, the power loss of the self-excited invert rectifier is analyzed. Finally, the self-excited invert rectifier of the WPT experimental system is designed. The self-excited invert rectification method is then verified. The key component parameters of the self-excited invert rectifier are provided and optimized. The TE of the WPT system that includes the self-excited invert rectifier is improved by more than 5% without a microcontroller. The self-excited invert rectifier of the Rx provides a practical solution for decreasing the complexity and increasing the TE of the WPT system. Full article
(This article belongs to the Section Energy Systems)
Show Figures

Figure 1

Figure 1
<p>WPT system with self-excited invert rectifier.</p>
Full article ">Figure 2
<p>Working mode 1 of the self-excited invert rectifier: Current flow is power and control loops; and 0 V is the same voltage level.</p>
Full article ">Figure 3
<p>Working mode 2 of the self-excited invert rectifier: Current flow of red dotted lines is the first process section; and Current flow of green dotted lines is the second process section.</p>
Full article ">Figure 4
<p>Working mode 3 of the self-excited invert rectifier: Current flow is power and control loops; and 0 V is the same voltage level.</p>
Full article ">Figure 5
<p>Working mode 4 of the self-excited invert rectifier: Current flow of red dotted lines is the first process section; and Current flow of green dotted lines is the second process section.</p>
Full article ">Figure 6
<p>Steady−state working waveform of the switching tubes in the self-excited invert rectifier.</p>
Full article ">Figure 7
<p>Equivalent circuit of the WPT system with self-excited invert rectifier.</p>
Full article ">Figure 8
<p>Block diagram of the WPT system that includes a self-excited invert rectifier.</p>
Full article ">Figure 9
<p>A self-excited invert rectifier experimental equipment able to perform the SD and SS of the MOSFETs.</p>
Full article ">Figure 10
<p>Gate drive waveform (gate−source voltage) of the <span class="html-italic">Q</span><sub>5</sub> and <span class="html-italic">Q</span><sub>6</sub> switching tubes.</p>
Full article ">Figure 11
<p>Working waveform (drain−source voltage) of the <span class="html-italic">Q</span><sub>5</sub> and <span class="html-italic">Q</span><sub>6</sub> switching tubes.</p>
Full article ">Figure 12
<p>(<b>a</b>) Circuit of the Rx and (<b>b</b>) temperature image of the self-excited invert rectifier.</p>
Full article ">Figure 13
<p>OP of the system as a function of the distance.</p>
Full article ">Figure 14
<p>TE of the system as a function of the distance.</p>
Full article ">Figure 15
<p>OP <span class="html-italic">P</span><sub>2</sub> of the system as a function of the frequency.</p>
Full article ">Figure 16
<p>TE <span class="html-italic">η</span><sub>2</sub> of the system as a function of the frequency.</p>
Full article ">
25 pages, 3292 KiB  
Article
Lane Detection Based on CycleGAN and Feature Fusion in Challenging Scenes
by Eric Hsueh-Chan Lu and Wei-Chih Chiu
Vehicles 2025, 7(1), 2; https://doi.org/10.3390/vehicles7010002 - 1 Jan 2025
Viewed by 309
Abstract
Lane detection is a pivotal technology of the intelligent driving system. By identifying the position and shape of the lane, the vehicle can stay in the correct lane and avoid accidents. Image-based deep learning is currently the most advanced method for lane detection. [...] Read more.
Lane detection is a pivotal technology of the intelligent driving system. By identifying the position and shape of the lane, the vehicle can stay in the correct lane and avoid accidents. Image-based deep learning is currently the most advanced method for lane detection. Models using this method already have a very good recognition ability in general daytime scenes, and can almost achieve real-time detection. However, these models often fail to accurately identify lanes in challenging scenarios such as night, dazzle, or shadows. Furthermore, the lack of diversity in the training data restricts the capacity of the models to handle different environments. This paper proposes a novel method to train CycleGAN with existing daytime and nighttime datasets. This method can extract features of different styles and multi-scales, thereby increasing the richness of model input. We use CycleGAN as a domain adaptation model combined with an image segmentation model to boost the model’s performance in different styles of scenes. The proposed consistent loss function is employed to mitigate performance disparities of the model in different scenarios. Experimental results indicate that our method enhances the detection performance of original lane detection models in challenging scenarios. This research helps improve the dependability and robustness of intelligent driving systems, ultimately making roads safer and enhancing the driving experience. Full article
Show Figures

Figure 1

Figure 1
<p>Illustration of the two-stage proposed method.</p>
Full article ">Figure 2
<p>The architecture of the proposed lane detection model training.</p>
Full article ">Figure 3
<p>The architecture of the proposed domain adaption model training.</p>
Full article ">Figure 4
<p>Qualitative analysis result of Grad-CAM.</p>
Full article ">Figure 5
<p>The example of challenge scenarios from the CULane test dataset. (<b>a</b>) Crowded; (<b>b</b>) Dazzle; (<b>c</b>) Shadow; (<b>d</b>) Arrow.</p>
Full article ">Figure 6
<p>The example of other challenge scenarios from the CULane test dataset. (<b>a</b>) Indoor; (<b>b</b>) wet ground.</p>
Full article ">Figure 7
<p>Visualization results of challenging scenes in the CULane test dataset. (<b>a</b>) Night; (<b>b</b>) crowded; (<b>c</b>) dazzle; (<b>d</b>) shadow; (<b>e</b>) arrow; (<b>f</b>) indoor; (<b>g</b>) wet ground.</p>
Full article ">Figure 7 Cont.
<p>Visualization results of challenging scenes in the CULane test dataset. (<b>a</b>) Night; (<b>b</b>) crowded; (<b>c</b>) dazzle; (<b>d</b>) shadow; (<b>e</b>) arrow; (<b>f</b>) indoor; (<b>g</b>) wet ground.</p>
Full article ">
20 pages, 4124 KiB  
Article
Digital Hydraulic Motor Characteristic Analysis for Heavy-Duty Vehicle Traction
by Hao Zhang, Wenshu Wei, Hong Wang, Yang Zhang and Xiaochao Liu
Actuators 2025, 14(1), 11; https://doi.org/10.3390/act14010011 - 1 Jan 2025
Viewed by 340
Abstract
Hydraulic motors have been widely used in large-scale machinery such as ground heavy equipment and heavy-duty vehicles, ships, and so on because of their high-power drive capability. However, the driving device is confronted with constraints related to its size and weight. Typically, the [...] Read more.
Hydraulic motors have been widely used in large-scale machinery such as ground heavy equipment and heavy-duty vehicles, ships, and so on because of their high-power drive capability. However, the driving device is confronted with constraints related to its size and weight. Typically, the hydraulic axial piston motor is preferred for its simplicity and efficiency. However, the oil distributor in traditional hydraulic motors faces significant challenges, such as evident oil leakage and power loss from the mating surfaces of the fixed oil distributor and rotating cylinder block. To enhance the reliability and performance of hydraulic motors employed in paper driving applications, this paper introduces a digital radial hydraulic motor used for heavy-duty vehicle traction. The motor is powered by an on-board pump station from which several on/off valves can distribute the hydraulic oil. This design effectively mitigates the performance degradation issues associated with friction and wear in traditional hydraulic motor oil distributors. The drive characteristics of the motor can be flexibly adjusted through the combination of valves. Our investigation into the motor’s design principles and parameter analysis is poised to make an indirect yet significant contribution to the optimization of heavy-duty vehicle traction systems. This paper delineates the application conditions and operational principles of the digital hydraulic motor, thoroughly analyzes the intricate topological interrelationships of its parameters, and meticulously develops a detailed component-level model. Through comprehensive calculations, it reveals the impact of configuration and flow valve parameters on motor efficiency. A simulation model is established for the purpose of verification. Furthermore, the influence of the flow allocation method on efficiency and pressure pulsation is examined, leading to the proposal of a novel flow allocation strategy, the efficacy of which is substantiated through simulation. In conclusion, this paper formulates critical insights to inform the design and selection of components for digital hydraulic motors. These findings may provide a feasible solution for heavy-duty vehicle traction application scenarios. Full article
(This article belongs to the Section High Torque/Power Density Actuators)
Show Figures

Figure 1

Figure 1
<p>Digital hydraulic motor drive system.</p>
Full article ">Figure 2
<p>Hydraulic motor digital distribution schematic.</p>
Full article ">Figure 3
<p>Working quadrants.</p>
Full article ">Figure 4
<p>Variable displacement-driven system schematic.</p>
Full article ">Figure 5
<p>Cross-sectional diagram and circumferential view of digital hydraulic motor. (<b>a</b>) Digital motor cutaway schematic. (<b>b</b>) Circumferential expansion schematic.</p>
Full article ">Figure 6
<p>Schematic diagram and the piston.</p>
Full article ">Figure 7
<p>Velocity and force decomposition.</p>
Full article ">Figure 8
<p>Motor flow of different motor configuration. (<b>a</b>) n = 8, m = 3. (<b>b</b>) n = 6, m = 3.</p>
Full article ">Figure 9
<p>The relationship between the distribution phase and piston unit power. (<b>a</b>) Ideal distribution. (<b>b</b>) Distribution with phase deviation.</p>
Full article ">Figure 10
<p>Distributing method 1: simultaneous switching commands.</p>
Full article ">Figure 11
<p>Simulation model and result of a piston. (<b>a</b>) Simulation model of a piston. (<b>b</b>) Piston displacement.</p>
Full article ">Figure 12
<p>Simulation results of distributing method 1. (<b>a</b>) Piston chamber pressure. (<b>b</b>) Valve opening. (<b>c</b>) Valve opening at 0.05 s. (<b>d</b>) Valve opening at 0.1 s. (<b>e</b>) Flow of distributing valves. (<b>f</b>) Motor power.</p>
Full article ">Figure 13
<p>Distributing method 2: avoid simultaneous switching commands.</p>
Full article ">Figure 14
<p>Simulation results of distributing method 2. (<b>a</b>) Piston chamber pressure. (<b>b</b>) Valve opening. (<b>c</b>) Valve opening at 0.05 s. (<b>d</b>) Valve opening at 0.1 s. (<b>e</b>) Flow of distributing valves. (<b>f</b>) Motor power.</p>
Full article ">Figure 15
<p>Work cycle of the piston in the discharge cycle.</p>
Full article ">Figure 16
<p>Influence of switching time and flow coefficient on motor efficiency.</p>
Full article ">Figure 17
<p>Motor efficiency envelope of on-off valve and servo valve.</p>
Full article ">
26 pages, 14553 KiB  
Article
Advancing the Classification and Attribution Method for Alpine Wetlands: A Case Study of the Source Region of Three Rivers, Tibetan Plateau
by Xiankun Zheng, Sihai Liang, Xingxing Kuang, Li Wan and Kuo Zhang
Remote Sens. 2025, 17(1), 97; https://doi.org/10.3390/rs17010097 - 30 Dec 2024
Viewed by 339
Abstract
Alpine wetlands are highly vulnerable to changes caused by global warming. Rapidly and accurately mapping alpine wetlands and analyzing the driving factors of their spatiotemporal changes are crucial for protecting and managing these resources. However, few studies have investigated classification methods and attribution [...] Read more.
Alpine wetlands are highly vulnerable to changes caused by global warming. Rapidly and accurately mapping alpine wetlands and analyzing the driving factors of their spatiotemporal changes are crucial for protecting and managing these resources. However, few studies have investigated classification methods and attribution analyses for alpine wetlands. To address this gap, a novel classification method has been developed, integrating the Google Earth Engine, alpine wetland features, and a random forest classifier, named GAWRF, to delineate wetlands in alpine regions. Additionally, an improved Partial Least Squares Structural Equation Model (PLS-SEM) was utilized to explore the mechanisms of spatiotemporal changes in wetlands of the Source Region of Three Rivers (SRTR) from 1990 to 2020. The results indicate (1) the high accuracy of the SRTR land cover maps from 1990 to 2020, with an overall accuracy of above 92.48% and a Kappa coefficient of over 0.91, satisfying the subsequent analysis of wetland spatiotemporal changes; (2) a net loss of 3.8% in the SRTR alpine wetlands, with a notable 7.9% net loss in marsh wetlands and nearly 32,010 km2 lost by 2015; and (3) topography and permafrost change as key drivers (as identified by the PLS-SEM), with permafrost contributing 52% to the significant marsh wetland loss from 2010 to 2015. This study aims to provide fundamental information that is essential for the monitoring and conservation of alpine wetlands. Full article
(This article belongs to the Special Issue Remote Sensing for the Study of the Changes in Wetlands)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Geographical map of the study area. The boundaries of the study area were obtained from the National Tibetan Plateau Data Center (<a href="https://data.tpdc.ac.cn/" target="_blank">https://data.tpdc.ac.cn/</a> (accessed on 10 December 2023)). Yangtze River Source Protected Zone: Yangtze PZ. Yellow River Source Protected Zone: Yellow PZ. Lancang River Source Protected Zone: Lancang PZ.</p>
Full article ">Figure 2
<p>Workflow for mapping the SRTR alpine wetlands.</p>
Full article ">Figure 3
<p>Alpine wetland feature collection.</p>
Full article ">Figure 4
<p>Characteristics of alpine wetlands. (<b>a</b>,<b>b</b>) show the phenological characteristics of alpine vegetation, with (<b>a</b>) representing the interannual variation in the start of the growing season (SOS) and (<b>b</b>) the interannual variation in the end of the growing season (EOS). Detailed information regarding the 7 phenological characteristics data is in the <a href="#app1-remotesensing-17-00097" class="html-app">Supporting Information Text S1</a>. (<b>c</b>,<b>d</b>) represent the start of thawing (SOT) and the start of freezing (SOF), respectively. QT, Qiangtang Plateau. WSET, western Sichuan and the eastern Tibet Plateau. ALL, QT, and WSET merged regions. (<b>e</b>) demonstrates the seasonal dynamics of the suprapermafrost groundwater level (SGL), divided into four periods: rapid falling period (RF, October to mid-November), stable low water period (SL, late November to May), rapid rising period (RR, around June), and stable high water period (SH, July to September). (<b>f</b>) represents the hydrological characteristics of alpine wetlands. DOY, day of year.</p>
Full article ">Figure 5
<p>Top five features in the assessment of the importance of alpine wetland classification features for 1990, 1995, 2000, 2005, 2010, 2015, and 2020.</p>
Full article ">Figure 6
<p>Spatial distribution map of alpine wetlands in the SRTR. (<b>a</b>) distribution of wetlands in 1990. (<b>b</b>) distribution of wetlands in 1995. (<b>c</b>) distribution of wetlands in 2000. (<b>d</b>) distribution of wetlands in 2005. (<b>e</b>) distribution of wetlands in 2010. (<b>f)</b> distribution of wetlands in 2015. (<b>g</b>) distribution of wetlands in 2020. On the sides are the meridional (<b>right panel</b>) and zonal (<b>top panel</b>) distributions of wetland area fractions over 1990, 1995, 2000, 2005, 2010, 2015, and 2020 at a resolution of 0.02°.</p>
Full article ">Figure 7
<p>Alpine wetland distributions along altitude.</p>
Full article ">Figure 8
<p>Temporal changes in alpine wetlands and other land cover types. (<b>a</b>), (<b>b</b>), (<b>c</b>), and (<b>d</b>), respectively, show the annual changes in alpine wetland area within the SRTR, Yangtze PZ, Yellow PZ, and Lancang PZ. (<b>e</b>) presents the annual changes in the area of all the land cover types within the SRTR.</p>
Full article ">Figure 9
<p>Sankey diagram for conversions among land cover types from 1990 to 2020. (<b>a</b>) Sankey map of the conversion of alpine wetlands to other land cover types. (<b>b</b>) Sankey map of the conversion of other land cover types to alpine wetlands.</p>
Full article ">Figure 10
<p>The relationships between various factors and wetland changes from 1990 to 2020 are presented as follows: (<b>a</b>) the impacts of different driving factors on alpine wetlands during the periods 1990–1995 and 1995–2000; (<b>b</b>) the impacts during the periods 2000–2005 and 2005–2010; and (<b>c</b>) the impacts during the periods 2010–2015 and 2015–2020. Solid lines indicate positive impacts, while dashed lines indicate negative impacts. The five direct paths are (1) anthropogenic change→wetland change; (2) terrain factors→wetland change; (3) soil factors→wetland change; (4) hydrological change→wetland change; and (5) permafrost change→wetland change. The four indirect paths are (1) energy change→permafrost change→wetland change; (2) energy change→hydrological change→wetland change; (3) hydrological change→permafrost change→wetland change; and (4) hydrological change→soil factors→wetland change. *** indicates a significance level of <span class="html-italic">p</span> &lt; 0.001; ** indicates a significance level of <span class="html-italic">p</span> &lt; 0.01; * indicates a significance level of <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">Figure 10 Cont.
<p>The relationships between various factors and wetland changes from 1990 to 2020 are presented as follows: (<b>a</b>) the impacts of different driving factors on alpine wetlands during the periods 1990–1995 and 1995–2000; (<b>b</b>) the impacts during the periods 2000–2005 and 2005–2010; and (<b>c</b>) the impacts during the periods 2010–2015 and 2015–2020. Solid lines indicate positive impacts, while dashed lines indicate negative impacts. The five direct paths are (1) anthropogenic change→wetland change; (2) terrain factors→wetland change; (3) soil factors→wetland change; (4) hydrological change→wetland change; and (5) permafrost change→wetland change. The four indirect paths are (1) energy change→permafrost change→wetland change; (2) energy change→hydrological change→wetland change; (3) hydrological change→permafrost change→wetland change; and (4) hydrological change→soil factors→wetland change. *** indicates a significance level of <span class="html-italic">p</span> &lt; 0.001; ** indicates a significance level of <span class="html-italic">p</span> &lt; 0.01; * indicates a significance level of <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">Figure 11
<p>Spatial distribution and attribution analysis of marsh wetland conversion to grassland in SRTR from 2010 to 2015. (<b>a</b>) illustrates the area change of marsh wetlands converted to grasslands from 2010 to 2015, along with changes in the active layer thickness of permafrost; this figure also depicts the variations in precipitation and runoff during the same period. (<b>b</b>) shows the correlation between various factors and changes in marsh wetlands. *** indicates a significance level of <span class="html-italic">p</span> &lt; 0.001; ** indicates a significance level of <span class="html-italic">p</span> &lt; 0.01.</p>
Full article ">Figure 11 Cont.
<p>Spatial distribution and attribution analysis of marsh wetland conversion to grassland in SRTR from 2010 to 2015. (<b>a</b>) illustrates the area change of marsh wetlands converted to grasslands from 2010 to 2015, along with changes in the active layer thickness of permafrost; this figure also depicts the variations in precipitation and runoff during the same period. (<b>b</b>) shows the correlation between various factors and changes in marsh wetlands. *** indicates a significance level of <span class="html-italic">p</span> &lt; 0.001; ** indicates a significance level of <span class="html-italic">p</span> &lt; 0.01.</p>
Full article ">Figure 12
<p>Comparison of alpine marsh wetland mapping results from our results with other classified products. (<b>a</b>), (<b>b</b>), and (<b>c</b>) are typical sample areas of alpine marsh wetlands within the Yangtze PZ, Yellow PZ, and Lancang PZ, respectively. CAS: A national-scale wetland dataset using object-oriented methods and multi-layer decision tree techniques. CLCD: Annual land cover data of China from 1985 to 2020, generated using random forest algorithms. GLC: Global annual land cover data from 2000 to 2015, created using change detection and random forest classification.</p>
Full article ">
Back to TopTop