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20 pages, 11411 KiB  
Article
Modeling and Nonlinear Dynamic Characteristics Analysis of Fault Bearing Time-Varying Stiffness-Flexible Rotor Coupling System
by Renzhen Chen, Jingyi Lv, Jing Tian, Yanting Ai, Fengling Zhang and Yudong Yao
Mathematics 2024, 12(22), 3591; https://doi.org/10.3390/math12223591 - 16 Nov 2024
Viewed by 565
Abstract
There is a complex dynamic interaction between the aero-engine bearing and the rotor, and the resulting time-varying system parameters have an impact on the nonlinear dynamic characteristics of the rolling bearing-flexible rotor system. In this study, the interaction between the time-varying stiffness of [...] Read more.
There is a complex dynamic interaction between the aero-engine bearing and the rotor, and the resulting time-varying system parameters have an impact on the nonlinear dynamic characteristics of the rolling bearing-flexible rotor system. In this study, the interaction between the time-varying stiffness of the rolling bearing and the transient response of the flexible rotor is considered. The Newmark-β integral method is used to solve the dynamic equation, and the relationship between the time-varying characteristics of bearing stiffness and load and the dynamic characteristics of the rotor is studied. The relationship between bearing stiffness and vibration strength is analyzed, and the influence of damage size on the time domain signal energy of the disc is analyzed. The results show that the model established in this paper can accurately reflect the dynamic interaction between the bearing and the rotor. With the extension of the bearing damage, the dynamic stiffness of the bearing attenuates, the intensity of the excitation force increases, and the vibration is transmitted to the disc, which affects the motion stability and vibration response of the disc. Full article
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<p>Full-text research process.</p>
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<p>Six-node rotor-bearing system model.</p>
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<p>Damage bearing model diagram.</p>
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<p>Contact between the rolling element and damage pit.</p>
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<p>Bearing damage description function. (<b>a</b>,<b>c</b>,<b>d</b>) represent the states when the rolling body passes through defects of different sizes, and (<b>b</b>,<b>d</b>,<b>f</b>) show the relationship between <span class="html-italic">h</span> and <span class="html-italic">Φ</span> in the three states, respectively.</p>
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<p>Rotor system dynamics differential equation solving process.</p>
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<p>Bifurcation diagram of healthy bearing-rotor system.</p>
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<p>Time-varying stiffness of bearing and system response.</p>
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<p>Disc bifurcation diagrams under different damage widths.</p>
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<p>Three-dimensional spectrum of the disc under different damage widths.</p>
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<p>Bifurcation diagram of the disc under different damage lengths.</p>
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<p>The three-dimensional spectrum of the disc under different damage lengths.</p>
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<p>Axis orbit of 1500 rad/s disc (<b>a</b>) <span class="html-italic">B</span> = 0.7 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>b</b>) <span class="html-italic">B</span> = 1.4 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>c</b>) <span class="html-italic">B</span> = 2.1 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>d</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>e</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 1.9145 mm; (<b>f</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>g</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 9.572 mm; and (<b>h</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 11.4872 mm.</p>
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<p>Axis orbit of 1800 rad/s disc (<b>a</b>) <span class="html-italic">B</span> = 0.7 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>b</b>) <span class="html-italic">B</span> = 1.4 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>c</b>) <span class="html-italic">B</span> = 2.1 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>d</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>e</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 1.9145 mm; (<b>f</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 5.7436 mm; (<b>g</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 9.572 mm; and (<b>h</b>) <span class="html-italic">B</span> = 2.8 mm <span class="html-italic">L</span> = 11.4872 mm.</p>
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<p>The root mean square relationship between the vibration energy of the disc and the bearing stiffness under different damage degrees.</p>
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<p>Bearing-rotor test bench.</p>
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<p>Comparison of vibration energy between simulation signal and experimental signal under different damage degrees.</p>
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16 pages, 14652 KiB  
Article
Structural Basis of Activity of HER2-Targeting Construct Composed of DARPin G3 and Albumin-Binding Domains
by Anastasia G. Konshina, Eduard V. Bocharov, Elena V. Konovalova, Alexey A. Schulga, Vladimir Tolmachev, Sergey M. Deyev and Roman G. Efremov
Int. J. Mol. Sci. 2024, 25(21), 11370; https://doi.org/10.3390/ijms252111370 - 22 Oct 2024
Viewed by 861
Abstract
Non-immunoglobulin-based scaffold proteins (SPs) represent one of the key therapeutic target-specific and high-affinity binders in modern medicine. Among their cellular targets are signaling receptors, in particular, receptor tyrosine kinases, whose dysfunction leads to the development of cancer and other serious diseases. Successful applications [...] Read more.
Non-immunoglobulin-based scaffold proteins (SPs) represent one of the key therapeutic target-specific and high-affinity binders in modern medicine. Among their cellular targets are signaling receptors, in particular, receptor tyrosine kinases, whose dysfunction leads to the development of cancer and other serious diseases. Successful applications of SPs have been reported for HER receptor type 2 (HER2), a member of the human epidermal growth factor receptor family that regulates cell growth and differentiation. To extend the blood residence of SPs and prevent their high accumulation in the kidneys, these proteins are often fused with serum albumin. Promising results for HER2-binding activity were obtained for SP G3 from the DARPins (Designed Ankyrin Repeat Proteins) family fused with an albumin-binding domain (ABD). Interestingly, the detected HER2–G3 binding strongly depended on the position of the G3 module in the sequence of the constructs. Further improvement of these constructs for biomedical applications requires deciphering the molecular mechanism responsible for this effect. Here, we investigate the structural and dynamic aspects of ABD–G3 and G3–ABD chimeras using NMR spectroscopy and molecular modeling. Based on biophysical data, we come to the conclusion that extensive inter-domain contacts form in both constructs, although their binding interfaces and complex stability are somewhat different. Also, it is shown that the domain linker plays an important role—it limits the accessibility of the detected protein–protein binding sites, depending on the order of the domains in the chimeric molecules. These results create a solid structural basis for the rational design of new effective SP constructs targeting the signaling receptors in cells. Full article
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Graphical abstract

Graphical abstract
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<p>Amino acid sequences of DARPin constructions: G3–ABD, ABD–G3, G3, and ABD. The sequence of the interdomain linker (GS<sub>3</sub>)<sub>3</sub> is underlined.</p>
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<p>Overlaid <sup>1</sup>H-NMR spectra of the DARPins G3–ABD (in blue) and ABD–G3 (in red). The characteristic regions with the signals of amide and aromatic groups (<b>A</b>) and methyl groups (<b>B</b>) are shown. (The full spectra are presented in <a href="#app1-ijms-25-11370" class="html-app">Figure S1</a>.) The separate low-field and high-field <sup>1</sup>H-signals (near 9.6 and −0.2 ppm) of the G3 subunit are zoomed, and the major and minor components of the split <sup>1</sup>H-signals are marked by asterisks.</p>
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<p>MD/MC-data analysis: difference in binding interfaces of the G3 domain for G3–ABD and ABD–G3 molecules. (<b>A</b>) The molecular surfaces of both DARPin (G3) domain and experimentally-derived model of the HER2 (subdomain IV)–G3 complex (4hrn, D) are colored according to the values of the molecular hydrophobicity potential (MHP). The main hydrophobic pattern on the DARPin surface is shown (<b>A</b>). The molecular surfaces of G3 module of G3–ABD (<b>B</b>) and ABD–G3 (<b>C</b>) are colored according to the high or low degree of involvement of the corresponding residues in contact with the ABD module during w-MD-runs (starts from non-interacting domains). Spatial arrangement of ABD domain relative to G3 in MD complexes of G3–ABD (<b>B</b>) and ABD–G3 (<b>C</b>) chimeras is given in cartoon representation. The corresponding representatives of the most populated MD-clusters are colored in green/cyan and light blue for hydrophobic interfaces (np-site) and a number of “polar” interfaces (p-sites), respectively. The key interface residues of G3 found in MD trajectories starting from complexes with hydrophobic interface (<b>B</b>), in low-energy MC states (colored in magenta, (<b>B</b>)), and in experimental 3D model of HER2–G3 (<b>A</b>) are indicated.</p>
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<p>Difference in binding interfaces of the ABD domain for G3–ABD and ABD–G3 molecules. The molecular surfaces of ABD modules of G3–ABD (<b>A</b>) and ABD–G3 (<b>B</b>) are colored according to the high or low degree of involvement of the corresponding residues in contact with the G3 domain during w-MD runs. The corresponding scale is given with the spectral band. Data are averaged over all w-MD-trajectories, color intensity reflects the population degree. HSA-binding residues found in HSA–ABD complex (PDB ID: 2vdb) are represented by stick lines. The residues from inter-helical loops of HSA motif involved in electrostatic interactions (including H-bonds) with HSA are designated (see <a href="#app1-ijms-25-11370" class="html-app">Figure S3</a>). The HSA residues found at the G3–ABD interfaces of MD complexes obtained from MD simulations of non-interacting (at start) domains are colored by atom type.</p>
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<p>Results of MD simulations started from non-interacting G3 and ABD domains: difference in interaction interfaces of the domain linker for G3–ABD and ABD–G3 molecules. The molecular surface of G3 module of G3–ABD (<b>A</b>) and ABD–G3 (<b>B</b>) is colored according to the high or low degree of involvement of the corresponding residues in contact with the inter-domain linker during w-MD runs. Data are averaged over all w-MD trajectories, and color intensity reflects the population degree. Location of the linker (backbone atoms) in the complexes with the hydrophobic domain interface (ABD domain is given as green helix) is shown relative to the area of its most probable contact with the G3 surface observed in w-MD starts.</p>
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<p>A hypothetical diagram illustrating the most likely protein–protein interactions predicted based on NMR and modeling experiments. (<b>A</b>) ABD-binding sites (p- and np-sites) on the surface of G3 domain of the chimeras G3-ABD and ABD-G3: p-sites have different localizations depending on the type of construct. Location of p-site near HER2-binding interface of G3 can lead to a loss of HER2-activity of the ABD-G3 in HSA-free environment. (<b>B</b>) Types of HSA/chimera complexes (with or without dissociation of G3/ABD domains) upon addition of HSA to the medium. (<b>C</b>) HER2-binding activity of the chimeras upon addition of HER2 to HSA-containing medium.</p>
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14 pages, 1115 KiB  
Article
Practical Stability of Observer-Based Control for Nonlinear Caputo–Hadamard Fractional-Order Systems
by Rihab Issaoui, Omar Naifar, Mehdi Tlija, Lassaad Mchiri and Abdellatif Ben Makhlouf
Fractal Fract. 2024, 8(9), 531; https://doi.org/10.3390/fractalfract8090531 - 11 Sep 2024
Cited by 1 | Viewed by 509
Abstract
This paper investigates the problem of observer-based control for a class of nonlinear systems described by the Caputo–Hadamard fractional-order derivative. Given the growing interest in fractional-order systems for their ability to capture complex dynamics, ensuring their practical stability remains a significant challenge. We [...] Read more.
This paper investigates the problem of observer-based control for a class of nonlinear systems described by the Caputo–Hadamard fractional-order derivative. Given the growing interest in fractional-order systems for their ability to capture complex dynamics, ensuring their practical stability remains a significant challenge. We propose a novel concept of practical stability tailored to nonlinear Hadamard fractional-order systems, which guarantees that the system solutions converge to a small ball containing the origin, thereby enhancing their robustness against perturbations. Furthermore, we introduce a practical observer design that extends the classical observer framework to fractional-order systems under an enhanced One-Sided Lipschitz (OSL) condition. This extended OSL condition ensures the convergence of the proposed practical observer, even in the presence of significant nonlinearities and disturbances. Notably, the novelty of our approach lies in the extension of both the practical observer and the stability criteria, which are innovative even in the integer-order case. Theoretical results are substantiated through numerical examples, demonstrating the feasibility of the proposed method in real-world control applications. Our contributions pave the way for the development of robust observers in fractional-order systems, with potential applications across various engineering domains. Full article
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<p>The actual state <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>x</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> and its corresponding estimate for Example 1.</p>
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<p>The actual state <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>x</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math> and its corresponding estimate for Example 1.</p>
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<p>Actual states <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>x</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo> </mo> <msub> <mrow> <mi>x</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math> and their estimates for Example 2.</p>
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15 pages, 331 KiB  
Review
An Overview of Model-Free Adaptive Control for the Wheeled Mobile Robot
by Chen Zhang, Chen Cen and Jiahui Huang
World Electr. Veh. J. 2024, 15(9), 396; https://doi.org/10.3390/wevj15090396 - 29 Aug 2024
Cited by 1 | Viewed by 997
Abstract
Control technology for wheeled mobile robots is one of the core focuses in the current field of robotics research. Within this domain, model-free adaptive control (MFAC) methods, with their advanced data-driven strategies, have garnered widespread attention. The unique characteristic of these methods is [...] Read more.
Control technology for wheeled mobile robots is one of the core focuses in the current field of robotics research. Within this domain, model-free adaptive control (MFAC) methods, with their advanced data-driven strategies, have garnered widespread attention. The unique characteristic of these methods is their ability to operate without relying on prior model information of the control system, which showcases their exceptional capability in ensuring closed-loop system stability. This paper extensively details three dynamic linearization techniques of MFAC: compact form dynamic linearization, partial form dynamic linearization and full form dynamic linearization. These techniques lay a solid theoretical foundation for MFAC. Subsequently, the article delves into some advanced MFAC schemes, such as dynamic event-triggered MFAC and iterative learning MFAC. These schemes further enhance the efficiency and intelligence level of control systems. In the concluding section, the paper briefly discusses the future development potential and possible research directions of MFAC, aiming to offer references and insights for future innovations in control technology for wheeled mobile robots. Full article
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<p>Tracking performance with PID.</p>
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<p>Control input with PID.</p>
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<p>Tracking performance with MFAC.</p>
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<p>Tracking performance of the WMR with MFAC under disturbance.</p>
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19 pages, 3608 KiB  
Article
Genome-Wide Association Study of Cuticle and Lipid Droplet Properties of Cucumber (Cucumis sativus L.) Fruit
by Stephanie Rett-Cadman, Yiqun Weng, Zhangjun Fei, Addie Thompson and Rebecca Grumet
Int. J. Mol. Sci. 2024, 25(17), 9306; https://doi.org/10.3390/ijms25179306 - 28 Aug 2024
Viewed by 999
Abstract
The fruit surface is a critical first line of defense against environmental stress. Overlaying the fruit epidermis is the cuticle, comprising a matrix of cutin monomers and waxes that provides protection and mechanical support throughout development. The epidermal layer of the cucumber ( [...] Read more.
The fruit surface is a critical first line of defense against environmental stress. Overlaying the fruit epidermis is the cuticle, comprising a matrix of cutin monomers and waxes that provides protection and mechanical support throughout development. The epidermal layer of the cucumber (Cucumis sativus L.) fruit also contains prominent lipid droplets, which have recently been recognized as dynamic organelles involved in lipid storage and metabolism, stress response, and the accumulation of specialized metabolites. Our objective was to genetically characterize natural variations for traits associated with the cuticle and lipid droplets in cucumber fruit. Phenotypic characterization and genome-wide association studies (GWAS) were performed using a resequenced cucumber core collection accounting for >96% of the allelic diversity present in the U.S. National Plant Germplasm System collection. The collection was grown in the field, and fruit were harvested at 16–20 days post-anthesis, an age when the cuticle thickness and the number and size of lipid droplets have stabilized. Fresh fruit tissue sections were prepared to measure cuticle thickness and lipid droplet size and number. The collection showed extensive variation for the measured traits. GWAS identified several QTLs corresponding with genes previously implicated in cuticle or lipid biosynthesis, including the transcription factor SHINE1/WIN1, as well as suggesting new candidate genes, including a potential lipid-transfer domain containing protein found in association with isolated lipid droplets. Full article
(This article belongs to the Special Issue Genetics and Molecular Breeding of Cucurbitaceous Crops)
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Figure 1
<p>Examples of the diversity of cuticle and lipid droplet traits in the cucumber core collection. Fresh tissue sections of various accessions in the collection. Scale bar represents 50 µm.</p>
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<p>Distribution of cuticle and lipid droplet traits for fruit epidermis of the cucumber core collection (<span class="html-italic">n</span> = 374). (<b>A</b>) Trait distribution using best linear unbiased estimates (BLUEs) of accessions for combined data from 2019–2021. (<b>B</b>) Distribution of epidermal trait values based on region of origin. Geographic regions were assigned as per Wang et al. [<a href="#B29-ijms-25-09306" class="html-bibr">29</a>]. Values for each accession are based on measurements from three fruits per accession per year.</p>
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<p>Manhattan, QQ, and allele effect plots for cuticle thickness for fruit from the cucumber core collection using BLUE values. (<b>A</b>) FarmCPU and BLINK models of GWAS. The blue and red lines represent Bonferroni-corrected <span class="html-italic">p</span>-values of 0.05 and 0.01, respectively; the dashed blue line represents FDR ≤ 0.05. (<b>B</b>) SNP markers with significant allelic effects. BLUE values were calculated from combined data from 2019–2021. *, **, ***, and **** represent <span class="html-italic">p</span> ≤ 0.05, 0.01, 0.001, and 0.0001, respectively. Heterozygotes were included if they were &gt;10% of the population.</p>
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<p>Chromosomal locations of significant SNPs identified by GWAS for cuticle and lipid droplet traits. Lines above the chromosomes indicate previously identified QTLs. Asterisks indicate previously identified cuticle-associated genes, and triangles indicate potential novel candidate genes.</p>
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<p>Manhattan, QQ, and allele effect plots for lipid droplet diameter for fruit from the cucumber core collection using BLUE values. (<b>A</b>) FarmCPU and BLINK models of GWAS. The blue and red lines represent Bonferroni-corrected <span class="html-italic">p</span>-values of 0.05 and 0.01, respectively; the dashed blue line represents FDR ≤ 0.05. (<b>B</b>) SNP markers with significant allelic effects. (<b>C</b>) Example of the alternate allele effect of SNP within <span class="html-italic">CsGy2G011870</span>. BLUE values were calculated from combined data from 2019–2021. **, ***, and **** represent <span class="html-italic">p</span> ≤ 0.01, 0.001, and 0.0001, respectively.</p>
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<p>Manhattan, QQ, and allele effect plots for lipid droplet number for fruit from the cucumber core collection using BLUE values. (<b>A</b>) FarmCPU and BLINK models of GWAS. The blue and red lines represent Bonferroni-corrected <span class="html-italic">p</span>-values of 0.05 and 0.01, respectively; the dashed blue line represents FDR ≤ 0.05. (<b>B</b>) SNP markers with significant allelic effects. BLUE values were calculated from combined data from 2019–2021. * and **** represent <span class="html-italic">p</span> ≤ 0.05 and 0.0001, respectively.</p>
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<p>Cross section illustrating measurement of cuticle and lipid droplet traits. Images were taken of cross sections and viewed at 200× magnification, and a uniform line of 450 µm was drawn across each sample. Within this area, the total number of lipid droplets was counted, the area of each lipid droplet was measured (yellow ellipses), and the diameter was calculated using the Nikon NIS-Elements BR software (version 5.30.03). Cuticle thickness was measured in three locations (white lines).</p>
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19 pages, 6792 KiB  
Article
Computational and ADMET Predictions of Novel Compounds as Dual Inhibitors of BuChE and GSK-3β to Combat Alzheimer’s Disease
by Saurabh G. Londhe, Vinayak Walhekar, Mangala Shenoy, Suvarna G. Kini, Marcus T. Scotti, Luciana Scotti and Dileep Kumar
Pharmaceutics 2024, 16(8), 991; https://doi.org/10.3390/pharmaceutics16080991 - 26 Jul 2024
Viewed by 1483
Abstract
Background: Alzheimer’s disease is a serious and widespread neurodegenerative illness in the modern healthcare scenario. GSK-3β and BuChE are prominent enzymatic targets associated with Alzheimer’s disease. Co-targeting GSK3β and BChE in Alzheimer’s disease helps to modify disease progression and enhance cognitive function by [...] Read more.
Background: Alzheimer’s disease is a serious and widespread neurodegenerative illness in the modern healthcare scenario. GSK-3β and BuChE are prominent enzymatic targets associated with Alzheimer’s disease. Co-targeting GSK3β and BChE in Alzheimer’s disease helps to modify disease progression and enhance cognitive function by addressing both tau pathology and cholinergic deficits. However, the treatment arsenal for Alzheimer’s disease is extremely inadequate, with present medications displaying dismal success in treating this never-ending ailment. To create novel dual inhibitors, we have used molecular docking and dynamics analysis. Our focus was on analogs formed from the fusion of tacrine and amantadine ureido, specifically tailored to target GSK-3β and BuChE. Methods: In the following study, molecular docking was executed by employing AutoDock Vina and molecular dynamics and ADMET predictions were performed using the Desmond and Qikprop modules of Schrödinger. Results: Our findings unveiled that compounds DKS1 and DKS4 exhibited extraordinary molecular interactions within the active domains of GSK-3β and BuChE, respectively. These compounds engaged in highly favorable interactions with critical amino acids, including Lys85, Val135, Asp133, and Asp200, and His438, Ser198, and Thr120, yielding encouraging docking energies of −9.6 and −12.3 kcal/mol. Additionally, through extensive molecular dynamics simulations spanning a 100 ns trajectory, we established the robust stability of ligands DKS1 and DKS4 within the active pockets of GSK-3β and AChE. Particularly noteworthy was DKS5, which exhibited an outstanding human oral absorption rate of 79.792%, transcending the absorption rates observed for other molecules in our study. Conclusion: In summary, our in silico findings have illuminated the potential of our meticulously designed molecules as groundbreaking agents in the fight against Alzheimer’s disease, capable of simultaneously inhibiting both GSK-3β and BuChE. Full article
(This article belongs to the Special Issue ADME Properties in the Drug Delivery)
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Figure 1
<p>Designing strategy of dual inhibitors DKS the chained GSK-3β and BuChE pharmacophores Tacrine and thiazole motif by the application of molecular hybridization and scaffold hopping methodology.</p>
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<p>Chemical structures of designed molecules.</p>
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<p>Molecular architecture of GSK-3β.</p>
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<p>Molecular skeleton of BuChE.</p>
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<p>Coinciding poses of the co-crystallized ligands: (<b>a</b>) docked conformation of 2WE in cyan with co-crystallized ligand in green, RMSD: 0.98 Å; (<b>b</b>) docked conformation of THA (Tacrine) in cyan with co-crystallized ligand in green, RMSD: 0.5 Å.</p>
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<p>(<b>a</b>–<b>d</b>) Docked complexes of DKS-1, -5, -6, and -8 with GSK-3β kinase.</p>
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<p>(<b>a</b>,<b>b</b>) Docked complexes of DKS-2 and -4 with BuChE. (<b>c</b>,<b>d</b>) Docked complexes of DKS-5 and -11 with BuChE.</p>
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<p>(<b>a</b>,<b>b</b>) RMSD plot of DSK1 complexed with GSK-3β and DSK4 complexed BuChE.</p>
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<p>(<b>a</b>,<b>b</b>) RMSF plot of DSK1 complexed with GSK-3β and DSK4 complexed BuChE.</p>
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<p>(<b>a</b>,<b>b</b>) RMSF plot of DSK1 complexed with GSK-3β and DSK4 complexed BuChE.</p>
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<p>(<b>a</b>–<b>d</b>) Protein–ligand contact plot of DSK1 complexed with GSK-3β and DSK4 complexed with BuChE.</p>
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<p>(<b>a</b>,<b>b</b>) Crystal structure of BuChE at 0 and 100 ns.</p>
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<p>(<b>a</b>,<b>b</b>) Crystal structure of GSK-3β at 0 and 100 ns.</p>
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<p>(<b>a</b>,<b>b</b>) Heat maps of DKS1 and DKS4.</p>
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<p>(<b>a</b>,<b>b</b>) 2D graphical notation of DKS1 and DKS4.</p>
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27 pages, 22071 KiB  
Article
FBG Sensing Data Motivated Dynamic Feature Assessment of the Complicated CFRP Antenna Beam under Various Vibration Modes
by Cong Chen, Chao Zhang, Jie Ma, Shi-Zhong He, Jian Chen, Liang Sun and Hua-Ping Wang
Buildings 2024, 14(7), 2249; https://doi.org/10.3390/buildings14072249 - 22 Jul 2024
Viewed by 907
Abstract
Carbon fiber-reinforced polymer (CFRP) components were extensively used and current studies mainly refer to CFRP laminates. The dynamic performance of the complicated CFRP antenna beams is yet to be explored. Therefore, a sensor layout based on fiber Bragg gratings (FBGs) in series was [...] Read more.
Carbon fiber-reinforced polymer (CFRP) components were extensively used and current studies mainly refer to CFRP laminates. The dynamic performance of the complicated CFRP antenna beams is yet to be explored. Therefore, a sensor layout based on fiber Bragg gratings (FBGs) in series was designed to measure the dynamic response of the CFRP antenna beam, and various vibration tests (sweep frequency test, simulated long-life vibration test, shock vibration test, functional vibration test, and constant frequency vibration test) were conducted. The time and frequency domain analysis on FBG sensing signals was performed to check the vibration performance and assess the health condition of this novel CFRP structure. The results indicate that strain values reach a maximum of only 300 µε under different test conditions. The antenna beam exhibited clear vibration patterns, with the first four intrinsic frequencies identified at 44, 94.87, 107.1, and 193.45 Hz. It shows that strain distribution and vibration modes of the antenna beam can be characterized from the sensing data, and the dynamic feature can be much more accurately assessed. The FBG sensors attached on the surface of CFRP antenna beam can accurately and stably measure the dynamic response, which validates that the interfaces between optical fiber sensing elements and CFRP material have excellent interfacial bonding characteristics. The novel CFRP antenna beam exhibits the excellent dynamic performance and stability, offering the replacement of traditional steel antenna beams. The study can finally instruct the development of self-sensing CFRP antenna beams assembled with FBGs in series. Full article
(This article belongs to the Special Issue Recent Developments in Structural Health Monitoring)
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<p>A 3D model of the CFRP antenna beam.</p>
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<p>The layout of FBG sensors attached on the surfaces of CFRP antenna beam: (<b>a</b>) bottom B surface; (<b>b</b>) F surface; (<b>c</b>) R surface; (<b>d</b>) T surface; and (<b>e</b>) physical photo of the CFRP antenna beam.</p>
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<p>The layout of FBG sensors attached on the surfaces of CFRP antenna beam: (<b>a</b>) bottom B surface; (<b>b</b>) F surface; (<b>c</b>) R surface; (<b>d</b>) T surface; and (<b>e</b>) physical photo of the CFRP antenna beam.</p>
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<p>The major testing procedures of CFRP antenna beam.</p>
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<p>The time domain response of BH–sensor–d5 sensor: (<b>a</b>) sweep frequency test; (<b>b</b>) shock vibration test; (<b>c</b>) simulated long-life vibration test; and (<b>d</b>) constant frequency vibration test.</p>
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<p>The STFT time-frequency diagram of BH–sensor–d5 sensor: (<b>a</b>) sweep frequency test; (<b>b</b>) shock vibration test; (<b>c</b>) simulated long-life vibration test; and (<b>d</b>) constant frequency vibration test.</p>
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<p>The maximum transverse strain distribution diagram under vertical working conditions: (<b>a</b>) bottom B surface; (<b>b</b>) F surface; and (<b>c</b>) R surface.</p>
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<p>The maximum transverse strain distribution diagram under longitudinal conditions: (<b>a</b>) bottom B surface; (<b>b</b>) F surface; and (<b>c</b>) R surface.</p>
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<p>The maximum transverse strain distribution diagram under transverse working condition: (<b>a</b>) bottom B surface; (<b>b</b>) F surface; and (<b>c</b>) R surface.</p>
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<p>The strain time domain diagrams of the partial sensors at the bottom B surface of the vertical sweep frequency test: (<b>a</b>) BH–sensor–d1; (<b>b</b>) BH–sensor–d5; (<b>c</b>) BV–sensor1; and (<b>d</b>) BV–sensor3.</p>
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<p>The strain time domain diagrams of the partial sensors at the F surface of the vertical sweep frequency test: (<b>a</b>) FH–sensor–a1; (<b>b</b>) FH–sensor–a5; (<b>c</b>) FV–sensor3; and (<b>d</b>) FV–sensor4.</p>
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<p>The strain time domain diagrams of the partial sensors at the F surface of the vertical sweep frequency test: (<b>a</b>) FH–sensor–a1; (<b>b</b>) FH–sensor–a5; (<b>c</b>) FV–sensor3; and (<b>d</b>) FV–sensor4.</p>
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<p>The strain time domain diagrams of the partial sensors at the R surface of the vertical sweep frequency test: (<b>a</b>) RH–sensor–b1; (<b>b</b>) RH–sensor–b5; (<b>c</b>) RV–sensor4; and (<b>d</b>) RV–sensor6.</p>
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<p>The strain time domain diagrams of the partial sensors at the R surface of the vertical sweep frequency test: (<b>a</b>) RH–sensor–b1; (<b>b</b>) RH–sensor–b5; (<b>c</b>) RV–sensor4; and (<b>d</b>) RV–sensor6.</p>
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<p>The strain time domain diagrams of the sensors at the T surface of the vertical sweep frequency test: (<b>a</b>) TH–sensor2; (<b>b</b>) TH–sensor1; (<b>c</b>) TV–sensor2; and (<b>d</b>) TV–sensor1.</p>
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<p>The STFT time-frequency diagram of BH–sensor–d5 in the vertical sweep frequency test.</p>
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<p>The strain time domain diagrams of the partial sensors in the transverse shock vibration test: (<b>a</b>) BH–sensor–d1; (<b>b</b>) BH–sensor–d5; (<b>c</b>) BV–sensor1; (<b>d</b>) BV–sensor3; (<b>e</b>) FH–sensor–a1; and (<b>f</b>) FH–sensor–a5.</p>
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<p>The STFT time-frequency diagram of BH–sensor–d5 in transverse shock vibration test.</p>
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<p>The strain time domain diagrams of the partial sensors in the longitudinal simulated long-life vibration test: (<b>a</b>) BH–sensor–d1; (<b>b</b>) BH–sensor–d5; (<b>c</b>) BV–sensor1; (<b>d</b>) BV–sensor3; (<b>e</b>) FH–sensor–a1; (<b>f</b>) FH–sensor–a5; (<b>g</b>) RH–sensor–b1; and (<b>h</b>) RH–sensor–b5.</p>
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<p>The strain time domain diagrams of the partial sensors in the longitudinal simulated long-life vibration test: (<b>a</b>) BH–sensor–d1; (<b>b</b>) BH–sensor–d5; (<b>c</b>) BV–sensor1; (<b>d</b>) BV–sensor3; (<b>e</b>) FH–sensor–a1; (<b>f</b>) FH–sensor–a5; (<b>g</b>) RH–sensor–b1; and (<b>h</b>) RH–sensor–b5.</p>
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<p>The STFT time-frequency diagram of BH–sensor–d5 in longitudinal simulated long-life vibration test.</p>
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<p>The FDD results of the longitudinal simulated long-life vibration test.</p>
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<p>The strain time domain diagrams of partial sensors in the longitudinal functional vibration test: (<b>a</b>) BH–sensor–d1; (<b>b</b>) BH–sensor–d5; (<b>c</b>) BV–sensor1; (<b>d</b>) BV–sensor3; (<b>e</b>) FH–sensor–a1; (<b>f</b>) FH–sensor–a5; (<b>g</b>) RH–sensor–b1; and (<b>h</b>) RH–sensor–b5.</p>
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<p>The strain time domain diagrams of partial sensors in the longitudinal functional vibration test: (<b>a</b>) BH–sensor–d1; (<b>b</b>) BH–sensor–d5; (<b>c</b>) BV–sensor1; (<b>d</b>) BV–sensor3; (<b>e</b>) FH–sensor–a1; (<b>f</b>) FH–sensor–a5; (<b>g</b>) RH–sensor–b1; and (<b>h</b>) RH–sensor–b5.</p>
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<p>The STFT time-frequency diagram of BH–sensor–d5 in longitudinal functional vibration test.</p>
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<p>The FDD results of the longitudinal functional vibration test.</p>
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<p>The STFT and natural frequency extraction diagrams with load in vertical direction: (<b>a</b>) sweep frequency test; (<b>b</b>) shock vibration test; and (<b>c</b>) simulated long-life vibration test.</p>
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22 pages, 56505 KiB  
Article
Optimizing Slender Target Detection in Remote Sensing with Adaptive Boundary Perception
by Han Zhu and Donglin Jing
Remote Sens. 2024, 16(14), 2643; https://doi.org/10.3390/rs16142643 - 19 Jul 2024
Cited by 1 | Viewed by 876
Abstract
Over the past few years, target detectors that utilize Convolutional Neural Networks have gained extensive application in the domain of remote sensing (RS) imagery. Recently, optimizing bounding boxes has consistently been a hot topic in the research field. However, existing methods often fail [...] Read more.
Over the past few years, target detectors that utilize Convolutional Neural Networks have gained extensive application in the domain of remote sensing (RS) imagery. Recently, optimizing bounding boxes has consistently been a hot topic in the research field. However, existing methods often fail to take into account the interference caused by the shape and orientation changes of RS targets with high aspect ratios during training, leading to challenges in boundary perception when dealing with RS targets that have large aspect ratios. To deal with this challenge, our study introduces the Adaptive Boundary Perception Network (ABP-Net), a novel two-stage approach consisting of pre-training and training phases, which enhances the boundary perception of CNN-based detectors. In the pre-training phase, involving the initialization of our model’s backbone network and the label assignment, the traditional label assignment with a fixed IoU threshold fails to fully cover the critical information of slender targets, resulting in the detector missing lots of high-quality positive samples. To overcome this drawback, we design a Shape-Sensitive (S-S) label assignment strategy that can improve the boundary shape perception by dynamically adjusting the IoU threshold according to the aspect ratios of the targets so that the high-quality samples with critical features can be divided into positive samples. Moreover, during the training phase, minor angle differences of the slender bounding box may cause a significant change in the value of the loss function, producing unstable gradients. Such drastic gradient changes make it difficult for the model to find a stable update direction when optimizing the bounding box parameters, resulting in difficulty with the model convergence. To this end, we propose the Robust–Refined loss function (R-R), which can enhance the boundary localization perception by focusing on low-error samples and suppressing the gradient amplification of difficult samples, thereby improving the model stability and convergence. Experiments on UCAS-AOD and HRSC2016 datasets validate our specialized detector for high-aspect-ratio targets, improving performance, efficiency, and accuracy with straightforward operation and quick deployment. Full article
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<p>(<b>a</b>–<b>d</b>) The process of a sharp decline in IoU for elongated objects. (<b>e</b>) Some high-quality samples with low IoU but containing essential parts. (<b>f</b>) Some labels with high IoU but missing core features.</p>
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<p>(<b>a</b>) Difficult samples (yellow boxes) and low localization error samples (red boxes). The green bounding box delineates the true position and dimensions of the vessel, serving as the Ground Truth Box for this ship.(<b>b</b>,<b>c</b>) The plots of most of the current regression loss functions and their derivatives.</p>
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<p>Structure diagram of the ABP-Net. The initial detection head may yield detections with larger bounding boxes that encapsulate the target adequately but may lack precision, especially for slender targets. The refined detection head then adjusts these bounding boxes to more tightly fit the targets. Both detection heads within our network employ the same parameters for the S-S label assignment and the R-R loss function. This uniformity ensures consistency in the way targets are processed across the two stages. The S-S module, with its adaptive IoU threshold adjustment, allows both heads to effectively capture the critical features of targets regardless of their aspect ratio. Similarly, the R-R loss function contributes to the stability and accuracy of the bounding box regression in both detection stages.</p>
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<p>(<b>a</b>) When the aspect ratio <math display="inline"><semantics> <msub> <mi>η</mi> <mi>i</mi> </msub> </semantics></math> is around 50 to 51 times, the weight factor <span class="html-italic">f</span> increases as the angle difference <math display="inline"><semantics> <mrow> <mo>Δ</mo> <mi>θ</mi> </mrow> </semantics></math> increases. (<b>b</b>) When the angle difference <math display="inline"><semantics> <mrow> <mo>Δ</mo> <mi>θ</mi> </mrow> </semantics></math> is around 4° to 5°, the weight factor <span class="html-italic">f</span> decreases as the aspect ratio <math display="inline"><semantics> <msub> <mi>η</mi> <mi>i</mi> </msub> </semantics></math> increases.</p>
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<p>Our S-S module consists of two submodules (<b>a</b>,<b>b</b>). The module (<b>a</b>) is used for preliminary sampling to select good-quality samples. Then, the (<b>b</b>) module further supplements the critical features of the sample through aspect ratio and angle difference.</p>
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<p>Our S-S module consists of two submodules (<b>a</b>,<b>b</b>). The module (<b>a</b>) is used for preliminary sampling to select good-quality samples. Then, the (<b>b</b>) module further supplements the critical features of the sample through aspect ratio and angle difference.</p>
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<p>Three kinds of anchor boxes with low IoU. Although the anchor box in (<b>A</b>) contains critical information, it is difficult to regress and is divided into negative samples by the S-S strategy. The anchor boxes in (<b>B</b>,<b>C</b>) have regression potential although they have a low IoU and are classified as positive samples.</p>
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<p>(<b>a</b>) Gradient function of R-R loss function. (<b>b</b>) Our proposed R-R loss function curve.</p>
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<p>Our anchor regression training module (R-R). The Green block represents feature extraction for ships. By suppressing the growth of the gradient of the loss function (red blocks) and increasing the gradient of the loss function (yellow blocks), the model further focuses on low-error sample (yellow anchor boxes) regression.</p>
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<p>Results on HRSC2016.</p>
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<p>Visual detection results of our ABP-Net and the S2ANet.</p>
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<p>Results on UCAS-AOD (cars).</p>
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<p>Results on UCAS-AOD (airplanes).</p>
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<p>Visual detection results of our ABP-Net and RepPoints.</p>
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<p>This figure illustrates a failure scenario in slender target detection using the ABP-Net. The red bounding boxes represent the predicted detections by the model, indicating the areas where the model successfully identified the targets.</p>
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18 pages, 3499 KiB  
Article
NMR Dynamic View of the Destabilization of WW4 Domain by Chaotropic GdmCl and NaSCN
by Liang-Zhong Lim and Jianxing Song
Int. J. Mol. Sci. 2024, 25(13), 7344; https://doi.org/10.3390/ijms25137344 - 4 Jul 2024
Cited by 2 | Viewed by 789
Abstract
GdmCl and NaSCN are two strong chaotropic salts commonly used in protein folding and stability studies, but their microscopic mechanisms remain enigmatic. Here, by CD and NMR, we investigated their effects on conformations, stability, binding and backbone dynamics on ps-ns and µs-ms time [...] Read more.
GdmCl and NaSCN are two strong chaotropic salts commonly used in protein folding and stability studies, but their microscopic mechanisms remain enigmatic. Here, by CD and NMR, we investigated their effects on conformations, stability, binding and backbone dynamics on ps-ns and µs-ms time scales of a 39-residue but well-folded WW4 domain at salt concentrations ≤200 mM. Up to 200 mM, both denaturants did not alter the tertiary packing of WW4, but GdmCl exerted more severe destabilization than NaSCN. Intriguingly, GdmCl had only weak binding to amide protons, while NaSCN showed extensive binding to both hydrophobic side chains and amide protons. Neither denaturant significantly affected the overall ps-ns backbone dynamics, but they distinctively altered µs-ms backbone dynamics. This study unveils that GdmCl and NaSCN destabilize a protein before the global unfolding occurs with differential binding properties and µs-ms backbone dynamics, implying the absence of a simple correlation between thermodynamic stability and backbone dynamics of WW4 at both ps-ns and µs-ms time scales. Full article
(This article belongs to the Special Issue Structure, Function and Dynamics in Proteins: 2nd Edition)
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<p>CD characterization of the tertiary packing and thermal stability. (<b>A</b>) Hofmeister series of common cations and anions. (<b>B</b>) Near-UV CD spectra of the WW4 domain under five different conditions. (<b>C</b>) Near-UV CD spectra of WW4 at 25 °C and 90 °C as well as at 25 °C, cooled down after the thermal unfolding in the absence and in the presence of GdmCl and NaSCN at 200 mM. (<b>D</b>) Thermal unfolding curves of ellipticity at 280 nm under five different conditions.</p>
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<p>NMR characterization of the binding/perturbation to WW4. One-dimensional <sup>1</sup>H NMR spectra showing resonance peaks of Ile10 and Val22 methyl groups without (black) and with GdmCl (<b>A</b>) or NaSCN (<b>D</b>) at 20 mM (red) and 200 mM (green). Two-dimensional <sup>1</sup>H-<sup>15</sup>N NMR HSQC spectra without (blue) and with GdmCl (<b>B</b>) or NaSCN (<b>E</b>) at 20 mM (red) and 200 mM (green). (<b>C</b>) WW4 structure with residues having significant shifts (CSD &gt;  average  +  STD) of backbone amide protons in the presence of 200 mM GdmCl, colored in green. (<b>F</b>) WW4 structure with residues having significant shifts of backbone amide protons in the presence of 200 mM NaSCN, colored in red. Ile10 and Val22 side chains are also displayed in spheres.</p>
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<p>NMR quantification of the perturbations of GdmCl and NaSCN to WW4. (<b>A</b>) Chemical shift differences (CSDs) of WW4 in the presence of GdmCl at 20 (blue), 150 (cyan) and 200 (purple) mM. (<b>B</b>) Chemical shift differences (CSDs) of WW4 in the presence of NaSCN at 20 (blue), 150 (cyan) and 200 (purple) mM. The red line has a value of 0.14, which is the sum of the average and STD of CSDs in the presence of NaSCN at 200 mM. (<b>C</b>) WW4 structure with four residues having CSDs &gt;0.14, displayed in sticks. (<b>D</b>) Fitting of residue-specific dissociation constant (Kd) for Arg27 (red), Thr28 (blue), Thr29 (green) and Thr30 (cyan); experimental (dots) and simulated (lines) values for CSDs induced by additions of NaSCN at 3, 6, 10, 15, 20, 30, 40, 60, 80, 100, 125, 150 and 200 mM.</p>
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<p>Model-free analysis. (<b>A</b>) Squared generalized order parameters (S<sup>2</sup>) of WW4 without denaturant. (<b>B</b>) WW4 structure colored based on S<sup>2</sup> values without denaturant: blue—absence of S<sup>2</sup> due to the overlap of HSQC peaks or relaxation data of poor quality; green—Proline residues; red—S<sup>2</sup> &gt; 0.7; and yellow—S<sup>2</sup> &lt; 0.7. The locations of His24 and Thr26 are also indicated. (<b>C</b>) Differences in S<sup>2</sup> of WW4 with GdmCl at 20 mM (brown) and 200 mM (cyan) or NaSCN at 20 mM (purple) and 200 mM (red) from those without denaturant. (<b>D</b>) Residue-specific Rex of WW4 without (blue) and with GdmCl at 20 mM (brown), 200 mM (cyan), or NaSCN at 20 mM (purple) and 200 mM (red).</p>
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<p><sup>15</sup>N backbone CPMG relaxation dispersion. Differences in effective transverse relaxation rates (ΔR<sub>2</sub><sup>eff</sup>) at 80 and 960 Hz, for WW4 without (<b>A</b>) and with GdmCl at 200 mM (<b>B</b>) or NaSCN at 200 mM (<b>C</b>). For WW4 without denaturant, blue bars are for data at 500 MHz while red are for data at 800 MHz. For WW4 with 200 mM GdmCl or NaSCN, blue bars are for data at 500 MHz while red are for data at 800 MHz. (<b>D</b>) WW4 structure colored based on ΔR<sub>2</sub>(τ<sub>cp</sub>) without denaturant; red is for residues with ΔR<sub>2</sub><sup>eff</sup> &gt; 4 Hz. Glu10 and Tyr20 are specifically colored in yellow as their ΔR<sub>2</sub><sup>eff</sup> became &gt;4 Hz upon adding 200 mM NaSCN.</p>
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15 pages, 5478 KiB  
Article
Preparation and Properties of PA10T/PPO Blends Compatibilized with SEBS-g-MAH
by Housheng Xia, Zhen Jiang, Jiaxiang Tang, Jiao Tang, Jianping Zhou, Zize Yang, Rongbo Zheng and Junfeng Niu
Polymers 2024, 16(11), 1598; https://doi.org/10.3390/polym16111598 - 5 Jun 2024
Viewed by 1668
Abstract
Plant-derived PA10T is regarded as one of the most promising semi-aromatic polyamides; however, shortcomings, including low dimensional accuracy, high moisture absorption, and relatively high dielectric constant and loss, have impeded its extensive utilization. Polymer blending is a versatile and cost-effective method to fabricate [...] Read more.
Plant-derived PA10T is regarded as one of the most promising semi-aromatic polyamides; however, shortcomings, including low dimensional accuracy, high moisture absorption, and relatively high dielectric constant and loss, have impeded its extensive utilization. Polymer blending is a versatile and cost-effective method to fabricate new polymeric materials with excellent comprehensive performance. In this study, various ratios of PA10T/PPO blends were fabricated via melt blending with the addition of a SEBS-g-MAH compatibilizer. Molau test and scanning electron microscopy (SEM) were employed to study the influence of SEBS-g-MAH on the compatibility of PA10T and PPO. These studies indicated that SEBS-g-MAH effectively refines the domain size of the dispersed PPO phase and improves the dispersion stability of PPO particles within a hexafluoroisopropanol solvent. This result was attributed to the in situ formation of the SEBS-g-PA10T copolymer, which serves as a compatibilizer. Differential scanning calorimetry (DSC) and thermogravimetric analysis (TGA) results showed that the melting–crystallization behavior and thermal stability of blends closely resembled that of pure PA10T. Dynamic mechanical analysis (DMA) revealed that as the PPO content increased, there was a decrease in the glass transition temperature and storage modulus of PA10T. The water absorption rate, injection molding shrinkage, dielectric properties, and mechanical strength of blends were also systematically investigated. As the PPO content increased from 10% to 40%, the dielectric loss at 2.5 GHz decreased significantly from 0.00866 to 0.00572, while the notched Izod impact strength increased from 7.9 kJ/m2 to 13.7 kJ/m2. Full article
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<p>ATR/FT-IR spectra of pure PA10T and the PA10T/PPO blends.</p>
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<p>Molau test solutions in HFIP for pure PA10T, PPO, and the PA10T/PPO blends.</p>
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<p>A possible mechanism of the formation of SEBS-g-PA10T macromolecules.</p>
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<p>Melt flow index of pure PA10T and the PA10T/PPO blends.</p>
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<p>SEM micrographs of the tetrahydrofuran-etched fracture surface of the compatibilized PA10T/PPO blends containing 10%, 20%, 30%, and 40% PPO.</p>
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<p>TGA curves of pure PA10T and the PA10T/PPO blends.</p>
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<p>DSC curves of pure PA10T and the PA10T/PPO blends: (<b>A</b>) second heating run; and (<b>B</b>) cooling from the melt.</p>
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<p>(<b>A</b>) Storage modulus and (<b>B</b>) damping coefficient of pure PA10T and the PA10T/PPO blends.</p>
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<p>Water absorption rates of pure PA10T and the PA10T/PPO blends.</p>
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<p>Shrinkage rates of pure PA10T and the PA10T/PPO blends.</p>
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<p>The D<sub>k</sub> and D<sub>f</sub> values of pure PA10T and the PA10T/PPO blends.</p>
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<p>Tension stress–strain of pure PA10T and the PA10T/PPO blends.</p>
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23 pages, 2979 KiB  
Article
Hybrid Intelligent Control System for Adaptive Microgrid Optimization: Integration of Rule-Based Control and Deep Learning Techniques
by Osman Akbulut, Muhammed Cavus, Mehmet Cengiz, Adib Allahham, Damian Giaouris and Matthew Forshaw
Energies 2024, 17(10), 2260; https://doi.org/10.3390/en17102260 - 8 May 2024
Cited by 6 | Viewed by 1724
Abstract
Microgrids (MGs) have evolved as critical components of modern energy distribution networks, providing increased dependability, efficiency, and sustainability. Effective control strategies are essential for optimizing MG operation and maintaining stability in the face of changing environmental and load conditions. Traditional rule-based control systems [...] Read more.
Microgrids (MGs) have evolved as critical components of modern energy distribution networks, providing increased dependability, efficiency, and sustainability. Effective control strategies are essential for optimizing MG operation and maintaining stability in the face of changing environmental and load conditions. Traditional rule-based control systems are extensively used due to their interpretability and simplicity. However, these strategies frequently lack the flexibility for complex and changing system dynamics. This paper provides a novel method called hybrid intelligent control for adaptive MG that integrates basic rule-based control and deep learning techniques, including gated recurrent units (GRUs), basic recurrent neural networks (RNNs), and long short-term memory (LSTM). The main target of this hybrid approach is to improve MG management performance by combining the strengths of basic rule-based systems and deep learning techniques. These deep learning techniques readily enhance and adapt control decisions based on historical data and domain-specific rules, leading to increasing system efficiency, stability, and resilience in adaptive MG. Our results show that the proposed method optimizes MG operation, especially under demanding conditions such as variable renewable energy supply and unanticipated load fluctuations. This study investigates special RNN architectures and hyperparameter optimization techniques with the aim of predicting power consumption and generation within the adaptive MG system. Our promising results show the highest-performing models indicating high accuracy and efficiency in power prediction. The finest-performing model accomplishes an R2 value close to 1, representing a strong correlation between predicted and actual power values. Specifically, the best model achieved an R2 value of 0.999809, an MSE of 0.000002, and an MAE of 0.000831. Full article
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<p>The adaptive MG structure.</p>
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<p>Flow chart of hybrid intelligent control method for adaptive MG optimization (blue colour: calculation of <span class="html-italic">SOC</span>, green colour: charging of <span class="html-italic">SOC</span> of the <math display="inline"><semantics> <mrow> <mi>E</mi> <mi>S</mi> <mi>S</mi> </mrow> </semantics></math> and pink colour: discharging of <span class="html-italic">SOC</span> of the <math display="inline"><semantics> <mrow> <mi>E</mi> <mi>S</mi> <mi>S</mi> </mrow> </semantics></math>).</p>
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<p>The correlation matrix of the power flows.</p>
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<p>All monthly power trend data.</p>
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<p>Results of power flows for (<b>a</b>) the load demand, (<b>b</b>) the <math display="inline"><semantics> <mrow> <mi>E</mi> <mi>S</mi> <mi>S</mi> </mrow> </semantics></math>, and (<b>c</b>) the <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>O</mi> <mi>C</mi> </mrow> </semantics></math> of the <math display="inline"><semantics> <mrow> <mi>E</mi> <mi>S</mi> <mi>S</mi> </mrow> </semantics></math> during the rule-based control.</p>
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<p>Power flows among the components of the adaptive MG system for (<b>a</b>) the load and (<b>b</b>) the <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>V</mi> </mrow> </semantics></math>.</p>
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35 pages, 7945 KiB  
Article
Mathematical Patterns in Fuzzy Logic and Artificial Intelligence for Financial Analysis: A Bibliometric Study
by Ionuț Nica, Camelia Delcea and Nora Chiriță
Mathematics 2024, 12(5), 782; https://doi.org/10.3390/math12050782 - 6 Mar 2024
Cited by 8 | Viewed by 2792
Abstract
In this study, we explored the dynamic field of fuzzy logic and artificial intelligence (AI) in financial analysis from 1990 to 2023. Utilizing the bibliometrix package in RStudio and data from the Web of Science, we focused on identifying mathematical models and the [...] Read more.
In this study, we explored the dynamic field of fuzzy logic and artificial intelligence (AI) in financial analysis from 1990 to 2023. Utilizing the bibliometrix package in RStudio and data from the Web of Science, we focused on identifying mathematical models and the evolving role of fuzzy information granulation in this domain. The research addresses the urgent need to understand the development and impact of fuzzy logic and AI within the broader scope of evolving technological and analytical methodologies, particularly concentrating on their application in financial and banking contexts. The bibliometric analysis involved an extensive review of the literature published during this period. We examined key metrics such as the annual growth rate, international collaboration, and average citations per document, which highlighted the field’s expansion and collaborative nature. The results revealed a significant annual growth rate of 19.54%, international collaboration of 21.16%, and an average citation per document of 25.52. Major journals such as IEEE Transactions on Fuzzy Systems, Fuzzy Sets and Systems, the Journal of Intelligent & Fuzzy Systems, and Information Sciences emerged as significant contributors, aligning with Bradford’s Law’s Zone 1. Notably, post-2020, IEEE Transactions on Fuzzy Systems showed a substantial increase in publications. A significant finding was the high citation rate of seminal research on fuzzy information granulation, emphasizing its mathematical importance and practical relevance in financial analysis. Keywords like “design”, “model”, “algorithm”, “optimization”, “stabilization”, and terms such as “fuzzy logic controller”, “adaptive fuzzy controller”, and “fuzzy logic approach” were prevalent. The Countries’ Collaboration World Map indicated a strong pattern of global interconnections, suggesting a robust framework of international collaboration. Our study highlights the escalating influence of fuzzy logic and AI in financial analysis, marked by a growth in research outputs and global collaborations. It underscores the crucial role of fuzzy information granulation as a mathematical model and sets the stage for further investigation into how fuzzy logic and AI-driven models are transforming financial and banking analysis practices worldwide. Full article
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<p>Yearly research publication dynamics.</p>
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<p>Three-field diagram (middle field—authors, left field—KeyWords Plus, right field—keywords).</p>
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<p>Principal source publications.</p>
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<p>Mainly cited regional publications.</p>
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<p>Core sources by Bradford’s Law.</p>
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<p>Temporal patterns in source production.</p>
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<p>Key contributors.</p>
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<p>Authors’ publication trends over time.</p>
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<p>Key academic affiliations.</p>
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<p>Evolution of affiliation productivity.</p>
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<p>Corresponding Authors’ Countries.</p>
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<p>Countries’ impact on scientific production.</p>
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<p>Evolution of research production by country.</p>
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<p>Reference Spectroscopy.</p>
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<p>Word cloud of KeyWords Plus.</p>
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<p>Word cloud based on trigrams.</p>
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<p>Trend Topics.</p>
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<p>Thematic map based on KeyWords Plus.</p>
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<p>Thematic map based on authors’ keywords.</p>
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<p>Thematic evolution based on KeyWords Plus.</p>
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<p>Thematic Evolution based on authors’ keywords.</p>
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<p>Factorial Analysis.</p>
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15 pages, 5441 KiB  
Article
Identification of Novel Non-Nucleoside Inhibitors of Zika Virus NS5 Protein Targeting MTase Activity
by Diego Fiorucci, Micaela Meaccini, Giulio Poli, Maria Alfreda Stincarelli, Chiara Vagaggini, Simone Giannecchini, Priscila Sutto-Ortiz, Bruno Canard, Etienne Decroly, Elena Dreassi, Annalaura Brai and Maurizio Botta
Int. J. Mol. Sci. 2024, 25(4), 2437; https://doi.org/10.3390/ijms25042437 - 19 Feb 2024
Cited by 1 | Viewed by 1818
Abstract
Zika virus (ZIKV) is a positive-sense single-stranded virus member of the Flaviviridae family. Among other arboviruses, ZIKV can cause neurological disorders such as Guillain Barré syndrome, and it can have congenital neurological manifestations and affect fertility. ZIKV nonstructural protein 5 (NS5) is essential [...] Read more.
Zika virus (ZIKV) is a positive-sense single-stranded virus member of the Flaviviridae family. Among other arboviruses, ZIKV can cause neurological disorders such as Guillain Barré syndrome, and it can have congenital neurological manifestations and affect fertility. ZIKV nonstructural protein 5 (NS5) is essential for viral replication and limiting host immune detection. Herein, we performed virtual screening to identify novel small-molecule inhibitors of the ZIKV NS5 methyltransferase (MTase) domain. Compounds were tested against the MTases of both ZIKV and DENV, demonstrating good inhibitory activities against ZIKV MTase. Extensive molecular dynamic studies conducted on the series led us to identify other derivatives with improved activity against the MTase and limiting ZIKV infection with an increased selectivity index. Preliminary pharmacokinetic parameters have been determined, revealing excellent stability over time. Preliminary in vivo toxicity studies demonstrated that the hit compound 17 is well tolerated after acute administration. Our results provide the basis for further optimization studies on novel non-nucleoside MTase inhibitors. Full article
(This article belongs to the Special Issue Cutting-Edge Research on Antiviral Therapy)
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<p>(<b>A</b>) Analysis of protein dynamics and ligand–protein interactions. (<b>B</b>) Key interactions between SAM (green sticks) and NS5 MTase. (<b>C</b>) Pharmacophore model used to perform virtual screening of compounds into the SAM-binding pocket.</p>
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<p>Binding mode of ligand <b>1</b>. The hydrogen bonds are represented by yellow dotted lines.</p>
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<p>Design of experiment scheme.</p>
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<p>Kaplan–Meier survival rate curve for compound <b>17</b> after a single dose administration at the dose of 150 mg/kg.</p>
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33 pages, 12225 KiB  
Article
Coordinated Control for the Trajectory Tracking of Four-Wheel Independent Drive–Four-Wheel Independent Steering Electric Vehicles Based on the Extension Dynamic Stability Domain
by Yiran Qiao, Xinbo Chen and Dongxiao Yin
Actuators 2024, 13(2), 77; https://doi.org/10.3390/act13020077 - 16 Feb 2024
Cited by 2 | Viewed by 2144
Abstract
In order to achieve multi-objective chassis coordination control for 4WID-4WIS (four-wheel independent drive–four-wheel independent steering) electric vehicles, this paper proposes a coordinated control strategy based on the extension dynamic stability domain. The strategy aims to improve trajectory tracking performance, handling stability, and economy. [...] Read more.
In order to achieve multi-objective chassis coordination control for 4WID-4WIS (four-wheel independent drive–four-wheel independent steering) electric vehicles, this paper proposes a coordinated control strategy based on the extension dynamic stability domain. The strategy aims to improve trajectory tracking performance, handling stability, and economy. Firstly, expert PID and model predictive control (MPC) are used to achieve longitudinal speed tracking and lateral path tracking, respectively. Then, a sliding mode controller is designed to calculate the expected yaw moment based on the desired vehicle states. The extension theory is applied to construct the extension dynamic stability domain, taking into account the linear response characteristics of the vehicle. Different coordinated allocation strategies are devised within various extension domains, providing control targets for direct yaw moment control (DYC) and active rear steering (ARS). Additionally, a compound torque distribution strategy is formulated to optimize driving efficiency and tire adhesion rate, considering the vehicle’s economy and stability requirements. The optimal wheel torque is calculated based on this strategy. Simulation tests using the CarSim/Simulink co-simulation platform are conducted under slalom test and double-lane change to validate the control strategy. The test results demonstrate that the proposed control strategy not only achieves good trajectory tracking performance but also enhances handling stability and economy during driving. Full article
(This article belongs to the Special Issue Integrated Intelligent Vehicle Dynamics and Control)
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<p>The 4WID-4WIS vehicle dynamic model.</p>
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<p>Model validation results: (<b>a</b>) results of yaw rate; (<b>b</b>) results of sideslip angle.</p>
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<p>In-wheel motor efficiency map.</p>
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<p>The chassis coordinated control architecture.</p>
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<p>The extension phase portrait.</p>
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<p>The relationship between yaw rate and front wheel angle.</p>
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<p>Lateral tire force curve.</p>
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<p>The critical angle under different speeds and adhesion coefficients.</p>
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<p>The process of torque distribution control.</p>
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<p>Optimal front axle distribution coefficient.</p>
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<p>The 4WID-4WIS simulation model.</p>
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<p>Velocity tracking results under slalom test.</p>
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<p>Path tracking results under slalom test: (<b>a</b>) results of lateral displacement; (<b>b</b>) results of heading angle; (<b>c</b>) results of lateral offset; (<b>d</b>) results of heading angle error.</p>
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<p>Path tracking results under slalom test: (<b>a</b>) results of lateral displacement; (<b>b</b>) results of heading angle; (<b>c</b>) results of lateral offset; (<b>d</b>) results of heading angle error.</p>
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<p>Side slip angle under slalom test.</p>
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<p>Yaw rate results under slalom test: (<b>a</b>) results of yaw rate; (<b>b</b>) results of yaw rate error.</p>
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<p>Coordinated control results under slalom test: (<b>a</b>) results of correlation function; (<b>b</b>) results of control weights.</p>
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<p>Economic simulation results under slalom test: (<b>a</b>) results of system comprehensive efficiency; (<b>b</b>) results of battery energy consumption.</p>
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<p>Velocity tracking results under double-lane change.</p>
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<p>Path tracking results under double-lane change: (<b>a</b>) results of lateral displacement; (<b>b</b>) results of heading angle; (<b>c</b>) results of lateral offset; (<b>d</b>) results of heading angle error.</p>
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<p>Side slip angle under double-lane change.</p>
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<p>Yaw rate results under double-lane change: (<b>a</b>) results of yaw rate; (<b>b</b>) results of yaw rate error.</p>
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<p>Coordinated control results under double-lane change: (<b>a</b>) results of correlation function; (<b>b</b>) results of control weights.</p>
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<p>Economic simulation results under double-lane change: (<b>a</b>) results of system comprehensive efficiency; (<b>b</b>) results of battery energy consumption.</p>
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27 pages, 8623 KiB  
Article
Robust Speed Control of a Multi-Mass System: Analytical Tuning and Sensitivity Analysis
by Muhammed Alhanouti and Frank Gauterin
Appl. Sci. 2023, 13(24), 13268; https://doi.org/10.3390/app132413268 - 15 Dec 2023
Cited by 1 | Viewed by 964
Abstract
The regeneration of highly dynamic driving maneuvers on vehicle test benches is challenging due to several influences, such as power losses, vibrations in the overall system that involves the vehicle with the test bench, uncertainties in the model parameterization, and time delays from [...] Read more.
The regeneration of highly dynamic driving maneuvers on vehicle test benches is challenging due to several influences, such as power losses, vibrations in the overall system that involves the vehicle with the test bench, uncertainties in the model parameterization, and time delays from both the test bench and the measurement systems. In order to improve the dynamic response of the vehicle test bench and to overcome system disturbances, we employed different types of control algorithms for a mechanical multi-mass model. First, those controllers are extensively investigated in the frequency domain to analyze their stability and evaluate the noise rejection quality. Then, the expectations from the frequency analysis are confirmed in a time-domain simulation. Furthermore, sensitivity analysis tests were conducted to evaluate each controller’s robustness against the modeling parameters’ uncertainty. The linear quadratic controller with integral action demonstrated the best compromise between performance and robustness. Full article
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<p>VEhicle-in-the-Loop. <a href="https://www.fast.kit.edu/lff/4667.php" target="_blank">https://www.fast.kit.edu/lff/4667.php</a>, accessed on 18 March 2023.</p>
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<p>Complete simulation model of VEL mechanical power transmission system and a front-wheel-drive.</p>
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<p>Three mass models.</p>
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<p>Poles of the system plant.</p>
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<p>Block diagram of the plant system and the full-state controller.</p>
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<p>Block diagram representation of the plant system and the I-SS controller.</p>
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<p>Closed-loop system poles associated with all controllers.</p>
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<p>Closed-loop system dominant poles associated with all controllers.</p>
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<p>Nyquist plot in logarithmic scale [<a href="#B38-applsci-13-13268" class="html-bibr">38</a>] for PI-controlled system.</p>
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<p>Nyquist plot in logarithmic scale for LQ-controlled system.</p>
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<p>Nyquist plot in logarithmic scale for LQI-controlled system.</p>
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<p>Measurement noise amplification magnitude of all types of controllers with time delay.</p>
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<p>Desired reference signal and powertrain moment.</p>
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<p>Time response of the PI-controlled system: (<b>Left</b>) without time delay, (<b>Right</b>) with time delay.</p>
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<p>Time response of the optimal LQ-controlled system: (<b>Left</b>) without time delay, (<b>Right</b>) with time delay.</p>
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<p>Time response of the optimal LQI-controlled system: (<b>Left</b>) without time delay, (<b>Right</b>) with time delay.</p>
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<p>Influence of the time delay on the angular speed error: (<b>Top</b>) PI-controlled, (<b>Middle</b>) LQ-controlled, (<b>Bottom</b>) LQI-controlled.</p>
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<p>Measurement noise amplification of PI controller: (<b>Left</b>) without time delay, (<b>Right</b>) with time delay.</p>
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<p>Measurement noise amplification of LQ controller: (<b>Left</b>) without time delay, (<b>Right</b>) with time delay.</p>
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<p>Measurement noise amplification of LQI controller: (<b>Left</b>) without time delay, (<b>Right</b>) with time delay.</p>
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<p>Time response of LQ-controlled system at different T<sub>m</sub> values.</p>
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<p>Time response of LQI-controlled system at different T<sub>m</sub> values.</p>
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<p>Time response of LQ-controlled system at different M<sub>drive</sub> values.</p>
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<p>Time response of LQI-controlled system at different M<sub>drive</sub> values.</p>
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<p>Time response of LQ-controlled system at different J<sub>Pt2W</sub> values.</p>
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<p>Time response of LQI-controlled system at different J<sub>Pt2W</sub> values.</p>
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<p>Time response of LQ-controlled system at different K<sub>Ax</sub> values.</p>
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<p>Time response of LQI-controlled system at different values.</p>
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<p>Time response of LQ-controlled system at different J<sub>Pt2W</sub> and K<sub>Ax</sub> values.</p>
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<p>Time response of LQI-controlled system at different J<sub>Pt2W</sub> and K<sub>Ax</sub> values.</p>
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