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24 pages, 8434 KiB  
Article
A Fast Inverse Synthetic Aperture Radar Imaging Scheme Combining GPU-Accelerated Shooting and Bouncing Ray and Back Projection Algorithm under Wide Bandwidths and Angles
by Jiongming Chen, Pengju Yang, Rong Zhang and Rui Wu
Electronics 2024, 13(15), 3062; https://doi.org/10.3390/electronics13153062 - 2 Aug 2024
Viewed by 459
Abstract
Inverse synthetic aperture radar (ISAR) imaging techniques are frequently used in target classification and recognition applications, due to its capability to produce high-resolution images for moving targets. In order to meet the demand of ISAR imaging for electromagnetic calculation with high efficiency and [...] Read more.
Inverse synthetic aperture radar (ISAR) imaging techniques are frequently used in target classification and recognition applications, due to its capability to produce high-resolution images for moving targets. In order to meet the demand of ISAR imaging for electromagnetic calculation with high efficiency and accuracy, a novel accelerated shooting and bouncing ray (SBR) method is presented by combining a Graphics Processing Unit (GPU) and Bounding Volume Hierarchies (BVH) tree structure. To overcome the problem of unfocused images by a Fourier-based ISAR procedure under wide-angle and wide-bandwidth conditions, an efficient parallel back projection (BP) imaging algorithm is developed by utilizing the GPU acceleration technique. The presented GPU-accelerated SBR is validated by comparison with the RL-GO method in commercial software FEKO v2020. For ISAR images, it is clearly indicated that strong scattering centers as well as target profiles can be observed under large observation azimuth angles, Δφ=90°, and wide bandwidths, 3 GHz. It is also indicated that ISAR imaging is heavily sensitive to observation angles. In addition, obvious sidelobes can be observed, due to the phase history of the electromagnetic wave being distorted resulting from multipole scattering. Simulation results confirm the feasibility and efficiency of our scheme by combining GPU-accelerated SBR with the BP algorithm for fast ISAR imaging simulation under wide-angle and wide-bandwidth conditions. Full article
(This article belongs to the Special Issue Microwave Imaging and Applications)
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of the multiple scattering.</p>
Full article ">Figure 2
<p>Schematic diagram of beam reflectance. The shape of the ray tube changes after each reflection, which is determined by the divergence factor <math display="inline"><semantics> <mrow> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <mi>D</mi> <mi>F</mi> </mrow> <mo>)</mo> </mrow> </mrow> <mi>m</mi> </msub> </mrow> </semantics></math>.</p>
Full article ">Figure 3
<p>The parallel calculation process of C++AMP using the Direct Compute API to send parallel instructions to the device (GPU).</p>
Full article ">Figure 4
<p>The structure of programming model for the GPU acceleration process.</p>
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<p>BVH tree structure accounting for multiple scattering between triangular surface patches.</p>
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<p>Segmentation process of scenario tuples.</p>
Full article ">Figure 7
<p>Mapping of triangular surface elements into <math display="inline"><semantics> <mrow> <mrow> <mi>u</mi> <mo>,</mo> <mi>v</mi> </mrow> </mrow> </semantics></math> plane. (<b>a</b>) The case before mapping; (<b>b</b>) The case corresponding to Equation (11); (<b>c</b>) The intersection of the ray with the unit triangular surface element after mapping.</p>
Full article ">Figure 8
<p>Overlap diagram of child nodes’ bounding boxes.</p>
Full article ">Figure 9
<p>Schematic diagram of backward projection for ISAR imaging.</p>
Full article ">Figure 10
<p>Parallel calculation process of the BP algorithm for ISAR imaging using CUDA acceleration.</p>
Full article ">Figure 11
<p>Flow chart of GPU-accelerated BP algorithm.</p>
Full article ">Figure 12
<p>CAD model of full-scale F-22 fighter.</p>
Full article ">Figure 13
<p>RCS angular distribution of a full-scale F-22 fighter: (<b>a</b>) incidence angle <math display="inline"><semantics> <mrow> <mrow> <mi>θ</mi> <mo>=</mo> </mrow> <mrow> <mn>90</mn> </mrow> <mo>°</mo> </mrow> </semantics></math>, azimuth angle <math display="inline"><semantics> <mrow> <mrow> <mi>φ</mi> <mo>=</mo> </mrow> <mn>0</mn> <mo>°</mo> <mrow> <mo>~</mo> <mn>36</mn> </mrow> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math>, VV polarization; (<b>b</b>) incidence angle <math display="inline"><semantics> <mrow> <mrow> <mi>θ</mi> <mo>=</mo> </mrow> <mn>0</mn> <mo>°</mo> <mrow> <mo>~</mo> <mn>36</mn> </mrow> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math>, azimuth angle <math display="inline"><semantics> <mrow> <mrow> <mi>φ</mi> <mo>=</mo> </mrow> <mn>0</mn> <mo>°</mo> </mrow> </semantics></math>, HH polarization.</p>
Full article ">Figure 14
<p>Computer-aided design (CAD) model and dimensions of a scaled A380 aircraft model.</p>
Full article ">Figure 15
<p>Three typical observation configurations with different azimuth angles under fixed incidence angle <math display="inline"><semantics> <mrow> <mrow> <mi>θ</mi> <mo>=</mo> </mrow> <mn>60</mn> <mo>°</mo> </mrow> </semantics></math>. (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>135</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>135</mn> <mo>°</mo> <mo>~</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 16
<p>ISAR imaging results using GPU-accelerated BP imaging algorithm under fixed incidence angle <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>60</mn> <mo>°</mo> </mrow> </semantics></math>. In (<b>a</b>–<b>c</b>), the backscattering fields are calculated by our GPU-accelerated SBR method with a ray density of <math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>/</mo> <mn>10</mn> </mrow> </semantics></math>; in (<b>d</b>–<b>f</b>), the backscattering fields are obtained by FEKO’s RL-GO method with a ray density of <math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>/</mo> <mn>10</mn> </mrow> </semantics></math>; in (<b>g</b>–<b>i</b>), the backscattering fields are obtained by RL-GO with a ray density of <math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>/</mo> <mn>100</mn> </mrow> </semantics></math>. (<b>a</b>,<b>d</b>,<b>g</b>) are results for azimuth angle <math display="inline"><semantics> <mrow> <mrow> <mi>φ</mi> <mo>=</mo> </mrow> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>135</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>,<b>e</b>,<b>h</b>) are results for azimuth angle <math display="inline"><semantics> <mrow> <mrow> <mi>φ</mi> <mo>=</mo> </mrow> <mo>−</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>c</b>,<b>f</b>,<b>i</b>) are results for azimuth angle <math display="inline"><semantics> <mrow> <mrow> <mi>φ</mi> <mo>=</mo> </mrow> <mo>−</mo> <mn>135</mn> <mo>°</mo> <mo>~</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 17
<p>Three typical observation configurations with different azimuth angles under fixed incidence angle <math display="inline"><semantics> <mrow> <mrow> <mi>θ</mi> <mo>=</mo> </mrow> <mn>120</mn> <mo>°</mo> </mrow> </semantics></math>. (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>135</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>135</mn> <mo>°</mo> <mo>~</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 18
<p>Similar to <a href="#electronics-13-03062-f016" class="html-fig">Figure 16</a> but with incidence angle <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>120</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 19
<p>CAD model of an electrically large aircraft.</p>
Full article ">Figure 20
<p>Three typical observation configurations with different azimuth angles under fixed incidence angle <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>60</mn> <mo>°</mo> </mrow> </semantics></math>. (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>135</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>135</mn> <mo>°</mo> <mo>~</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>.</p>
Full article ">Figure 21
<p>ISAR imaging results using GPU-accelerated BP imaging algorithm under fixed incidence angle <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>60</mn> <mo>°</mo> </mrow> </semantics></math> in (<b>a</b>–<b>c</b>), the backscattering fields are calculated by our GPU-accelerated SBR method; in (<b>d</b>–<b>f</b>), backscattering fields are obtained by FEKO’s RL-GO method at a ray density of <math display="inline"><semantics> <mrow> <mi>λ</mi> <mo>/</mo> <mn>10</mn> </mrow> </semantics></math>; (<b>a</b>,<b>d</b>) are results for azimuth <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>135</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>b</b>,<b>e</b>) are results for azimuth <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> <mo>~</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>; (<b>c</b>,<b>f</b>) are results for azimuth <math display="inline"><semantics> <mrow> <mi>φ</mi> <mo>=</mo> <mo>−</mo> <mn>135</mn> <mo>°</mo> <mo>~</mo> <mo>−</mo> <mn>45</mn> <mo>°</mo> </mrow> </semantics></math>, VV polarization.</p>
Full article ">
24 pages, 26274 KiB  
Article
Imaging Seafloor Features Using Multipath Arrival Structures
by Zhaohua Su, Jie Zhuo and Chao Sun
Remote Sens. 2024, 16(14), 2586; https://doi.org/10.3390/rs16142586 - 14 Jul 2024
Viewed by 629
Abstract
In this paper, we propose an imaging method for seafloor features based on multipath arrival structures. The bistatic sonar system employed consists of a vertical transmitting array and a horizontal towed array. The conventional back projection (BP) method, which considers the direct path [...] Read more.
In this paper, we propose an imaging method for seafloor features based on multipath arrival structures. The bistatic sonar system employed consists of a vertical transmitting array and a horizontal towed array. The conventional back projection (BP) method, which considers the direct path from the source to the seafloor scatterer and then to the receiver, is used in this system. However, discrepancies between the calculated delay values and the actual propagation delay result in projection deviations and offsets in the seafloor features within sound intensity images. To address this issue, we analyze the multipath structures from the source to the scatterer and then to the receiver based on ray theory. The delay at each grid is calculated using different multipaths, considering the distances from the seafloor grids to the source and the receiver. In the direct zone, the delay is determined using the direct ray and the surface reflection ray, while in the bottom bounce area, the delay is calculated using the bottom–surface reflection ray and the surface–bottom–surface reflection ray. Numerical simulations and experimental results demonstrate that the proposed method rectifies the delay calculation issues inherent in the conventional method. This adjustment enhances the accuracy of the projection, thereby improving the imaging quality of seafloor features. Full article
Show Figures

Figure 1

Figure 1
<p>Acoustic imaging scene of bistatic sonar. (<b>a</b>) Side view. (<b>b</b>) Top view.</p>
Full article ">Figure 2
<p>The multipath structures from the source to the seafloor scatterer and then to the receiver. (<b>a</b>) SR/DR-SR/DR. (<b>b</b>) SR/DR-BSR/SBSR. (<b>c</b>) BSR/SBSR-SR/DR. (<b>d</b>) BSR/SBSR-BSR/SBSR.</p>
Full article ">Figure 3
<p>The eigenray path, the exit angle of the eigenray at the source, and the grazing angle of the eigenray at the scatterer. (<b>a</b>) Eigenray path in the direct zone. (<b>b</b>) The grazing angle varies with range in the direct zone. (<b>c</b>) Eigenray path in the bottom bounce zone. (<b>d</b>) The grazing angle varies with range in the bottom bounce zone.</p>
Full article ">Figure 4
<p>Projection of the beam output onto the image of seafloor features.</p>
Full article ">Figure 5
<p>Flow chart of the MAS-BP method.</p>
Full article ">Figure 6
<p>Simulation environment. (<b>a</b>) The parameters of the simulation environment. (<b>b</b>) The Munk profile employed in the simulation. (<b>c</b>) Top view of the imaging scene.</p>
Full article ">Figure 7
<p>The delay value varies with range. (<b>a</b>) The delay value in the direct zone. (<b>b</b>) The delay difference in the direct zone. (<b>c</b>) The delay value in the bottom bounce zone. (<b>d</b>) The delay difference in the bottom bounce zone.</p>
Full article ">Figure 8
<p>The delay calculated using the MAS-BP method and the BP method. (<b>a</b>) The MAS-BP method. (<b>b</b>) The BP method. (<b>c</b>) The delay difference between the MAS-BP method and the BP method.</p>
Full article ">Figure 9
<p>Imaging results of scatterers generated using the MAS-BP method and the BP method. (<b>a</b>) The MAS-BP method. (<b>b</b>) Amplification of rectangular frame area in <a href="#remotesensing-16-02586-f009" class="html-fig">Figure 9</a>a. (<b>c</b>) The BP method. (<b>d</b>) Amplification of rectangular frame area in <a href="#remotesensing-16-02586-f009" class="html-fig">Figure 9</a>c.</p>
Full article ">Figure 9 Cont.
<p>Imaging results of scatterers generated using the MAS-BP method and the BP method. (<b>a</b>) The MAS-BP method. (<b>b</b>) Amplification of rectangular frame area in <a href="#remotesensing-16-02586-f009" class="html-fig">Figure 9</a>a. (<b>c</b>) The BP method. (<b>d</b>) Amplification of rectangular frame area in <a href="#remotesensing-16-02586-f009" class="html-fig">Figure 9</a>c.</p>
Full article ">Figure 10
<p>Images generated using the MAS-BP method at four receiving positions. (<b>a</b>) Position No.1. (<b>b</b>) Position No.10. (<b>c</b>) Position No.25. (<b>d</b>) Position No.40.</p>
Full article ">Figure 11
<p>Images generated using the BP method at four receiving positions. (<b>a</b>) Position No.1. (<b>b</b>) Position No.10. (<b>c</b>) Position No.25. (<b>d</b>) Position No.40.</p>
Full article ">Figure 12
<p>The peak offset values of four scatterers in each image in the track. (<b>a</b>) The results of the MAS-BP method. (<b>b</b>) The results of the BP method.</p>
Full article ">Figure 13
<p>Experimental environment. (<b>a</b>) Bathymetry of the experimental area. (<b>b</b>) The measured sound speed profile.</p>
Full article ">Figure 14
<p>Imaging results of experimental data processed using the MAS-BP method and the BP method. (<b>a</b>) The image generated using the MAS-BP method. (<b>b</b>) Amplification of rectangular frame area in <a href="#remotesensing-16-02586-f014" class="html-fig">Figure 14</a>a. (<b>c</b>) The image generated using the BP method. (<b>d</b>) Amplification of rectangular frame area in <a href="#remotesensing-16-02586-f014" class="html-fig">Figure 14</a>c.</p>
Full article ">Figure 15
<p>Imaging results of experimental data processed using the MAS-BP method at different receiving times. (<b>a</b>) 16 June 2021 15:10:23. (<b>b</b>) 16 June 2021 15:20:23. (<b>c</b>) 16 June 2021 15:30:23. (<b>d</b>) 16 June 2021 15:40:23.</p>
Full article ">Figure 16
<p>Imaging results of experimental data processed using the BP method at different receiving times. (<b>a</b>) 16 June 2021 15:10:23. (<b>b</b>) 16 June 2021 15:20:23. (<b>c</b>) 16 June 2021 15:30:23. (<b>d</b>) 16 June 2021 15:40:23.</p>
Full article ">Figure 17
<p>The difference between the amplitude of sound intensity in <a href="#remotesensing-16-02586-f015" class="html-fig">Figure 15</a> and that in <a href="#remotesensing-16-02586-f016" class="html-fig">Figure 16</a> at different receiving times. (<b>a</b>) 16 June 2021 15:10:23. (<b>b</b>) 16 June 2021 15:20:23. (<b>c</b>) 16 June 2021 15:30:23. (<b>d</b>) 16 June 2021 15:40:23.</p>
Full article ">Figure 18
<p>Imaging results of experimental data processed using the MAS-BP method, where (<b>a</b>–<b>d</b>) correspond to Track 2 and (<b>e</b>–<b>h</b>) correspond to Track 3. (<b>a</b>) 16 June 2021 15:56:23. (<b>b</b>) 16 June 2021 16:08:22. (<b>c</b>) 16 June 2021 16:15:43. (<b>d</b>) 16 June 2021 16:25:03. (<b>e</b>) 16 June 2021 20:01:43. (<b>f</b>) 16 June 2021 20:11:43. (<b>g</b>) 16 June 2021 20:23:43. (<b>h</b>) 16 June 2021 20:32:23.</p>
Full article ">Figure 19
<p>Imaging results of experimental data processed using the BP method, where (<b>a</b>–<b>d</b>) correspond to Track 2 and (<b>e</b>–<b>h</b>) correspond to Track 3. (<b>a</b>) 16 June 2021 15:56:23. (<b>b</b>) 16 June 2021 16:08:22. (<b>c</b>) 16 June 2021 16:15:43. (<b>d</b>) 16 June 2021 16:25:03. (<b>e</b>) 16 June 2021 20:01:43. (<b>f</b>) 16 June 2021 20:11:43. (<b>g</b>) 16 June 2021 20:23:43. (<b>h</b>) 16 June 2021 20:32:23.</p>
Full article ">Figure 20
<p>The difference between the amplitude of sound intensity in <a href="#remotesensing-16-02586-f018" class="html-fig">Figure 18</a> and that in <a href="#remotesensing-16-02586-f019" class="html-fig">Figure 19</a>, where (<b>a</b>–<b>d</b>) correspond to Track 2 and (<b>e</b>–<b>h</b>) correspond to Track 3. (<b>a</b>) 16 June 2021 15:56:23. (<b>b</b>) 16 June 2021 16:08:22. (<b>c</b>) 16 June 2021 16:15:43. (<b>d</b>) 16 June 2021 16:25:03. (<b>e</b>) 16 June 2021 20:01:43. (<b>f</b>) 16 June 2021 20:11:43. (<b>g</b>) 16 June 2021 20:23:43. (<b>h</b>) 16 June 2021 20:32:23.</p>
Full article ">
21 pages, 1880 KiB  
Review
Understanding the Transcription Factor NFE2L1/NRF1 from the Perspective of Hallmarks of Cancer
by Haomeng Zhang, Yong Liu, Ke Zhang, Zhixuan Hong, Zongfeng Liu, Zhe Liu, Guichen Li, Yuanyuan Xu, Jingbo Pi, Jingqi Fu and Yuanhong Xu
Antioxidants 2024, 13(7), 758; https://doi.org/10.3390/antiox13070758 - 22 Jun 2024
Viewed by 1278
Abstract
Cancer cells subvert multiple properties of normal cells, including escaping strict cell cycle regulation, gaining resistance to cell death, and remodeling the tumor microenvironment. The hallmarks of cancer have recently been updated and summarized. Nuclear factor erythroid 2-related factor 1 (NFE2L1, also named [...] Read more.
Cancer cells subvert multiple properties of normal cells, including escaping strict cell cycle regulation, gaining resistance to cell death, and remodeling the tumor microenvironment. The hallmarks of cancer have recently been updated and summarized. Nuclear factor erythroid 2-related factor 1 (NFE2L1, also named NRF1) belongs to the cap’n’collar (CNC) basic-region leucine zipper (bZIP) family. It acts as a transcription factor and is indispensable for maintaining both cellular homoeostasis and organ integrity during development and growth, as well as adaptive responses to pathophysiological stressors. In addition, NFE2L1 mediates the proteasome bounce-back effect in the clinical proteasome inhibitor therapy of neuroblastoma, multiple myeloma, and triple-negative breast cancer, which quickly induces proteasome inhibitor resistance. Recent studies have shown that NFE2L1 mediates cell proliferation and metabolic reprogramming in various cancer cell lines. We combined the framework provided by “hallmarks of cancer” with recent research on NFE2L1 to summarize the role and mechanism of NFE2L1 in cancer. These ongoing efforts aim to contribute to the development of potential novel cancer therapies that target the NFE2L1 pathway and its activity. Full article
(This article belongs to the Section Health Outcomes of Antioxidants and Oxidative Stress)
Show Figures

Figure 1

Figure 1
<p>The structural domains and isoform of human nuclear factor erythroid 2-related factor 1 (NFE2L1). (<b>A</b>) Basic structural domains and correlated function of human NFE2L1. (<b>B</b>) Schematic protein structures of different isoforms of human NFE2L1. Abbreviations: NTD, N-terminal domain; AD1, acidic domain 1; NST, Asn/Ser/Thr-rich; AD2, acidic domain 2; SR, serine-repeat; Neh6L, Neh6-like; CNC, Cap ‘n’ collar; bZIP, basic-region zipper; CTD, C-terminal domain. All the sequences are from the National Center for Biotechnology (<a href="http://www.ncbi.nlm.nih.gov" target="_blank">www.ncbi.nlm.nih.gov</a>).</p>
Full article ">Figure 2
<p>Proposed activation pathway of Long-Nuclear factor erythroid 2-related factor 1 (L-NFE2L1). NFE2L1 is inserted into the endoplasmic reticulum (ER), and its asparagine/Serine/Threonine-rich (NST) domain is N-glycosylated so as to become an inactive NFE2L1 glycoprotein. When required for induction by biological cues, the ER-protected transactivation domains of NFE2L1 are dynamically retrotranslocated via the AAA protein p97/valerian-containing casein (VCP) and repositioned from the luminal side of ER membranes into the cyto/nucleo-plasmic side, whereupon it undergoes various post-translational modifications, such as N-deglycosylation, O-GlcNAcylation, de-GlcNAcylation and phosphorylation to yield active isoforms. In this process, diverse enzymes like PNGase, O-Linked N-acetylglucosamine transferase (OGT), DNA damage inducible 1 homology 2 (DDI2), beta-transducin repeat-containing protein (β-TrCP), and ubiquitin ligase HMG-CoA reductase degradation 1 (HRD1) are involved. There are two distinct (β-TrCP- and HRD1-dependent) degradation mechanisms regulating NFE2L1 protein levels. In the cytoplasm, NFE2L1 is degraded and suppressed by the ER-associated degradation ubiquitin ligase HRD1 and VCP. NFE2L1 is also degraded in the nucleus via β-TrCP-mediated degradation. In cells with insufficient proteasome capacity, active NFE2L1 accumulates and then migrates to the nucleus, where it heterodimerizes with cofactors to bind ARE to induce gene transcription. In contrast, complete proteasomal processing of NFE2L1 may lead to decreased NFE2L1 protein levels and transcriptional activity.</p>
Full article ">Figure 3
<p>NFE2L1 regulated the hallmarks of cancer. NFE2L1 associates with cancer hallmarks traits through various biological features. The hallmarks with dashed arrow indicate the lack of scientific evidence. The illustration was regrated based on an updated review by Hanahan et al. [<a href="#B29-antioxidants-13-00758" class="html-bibr">29</a>].</p>
Full article ">Figure 4
<p>NFE2L1 regulates cancer cell malignance. In this review, we mainly focus on six hallmarks of cancer regulated by NFE2L1, including resisting cell death, enabling replicative immortality, activity invasion and metastasis, proteotoxic stress, deregulating cellular energetics and anti-oxidant/altered redox balance, as well as the underlying mechanisms.</p>
Full article ">
18 pages, 383 KiB  
Article
Assessing the Impact of COVID-19 on Capital Structure Dynamics: Evidence from GCC Economies
by Amanj Mohamed Ahmed, Deni Pandu Nugraha and István Hágen
Economies 2024, 12(5), 103; https://doi.org/10.3390/economies12050103 - 26 Apr 2024
Viewed by 1519
Abstract
This study seeks to investigate the potential effects of the recent pandemic (COVID-19) on capital structure dynamics. The Gulf Cooperation Council (GCC) is a fascinating topic for this study because of its distinct economic characteristics. The analysis draws upon a cross-country dataset covering [...] Read more.
This study seeks to investigate the potential effects of the recent pandemic (COVID-19) on capital structure dynamics. The Gulf Cooperation Council (GCC) is a fascinating topic for this study because of its distinct economic characteristics. The analysis draws upon a cross-country dataset covering 208 non-financial listed firms across five GCC countries, with data spanning the years 2010 to 2022. Capital structure is a dependent variable and is measured by total debt to equity, equity multiplier, and short-term debt ratios, while the COVID-19 pandemic, firm size growth, return on assets, tangibility, and growth were applied as independent variables. Using the generalized least squares (GLS) method, findings demonstrated that COVID-19 has a significant and positive influence on debt-to-equity and equity multiplier ratios but a negative one on short-term debt ratio. Thus, non-financial firms increased their debt financing and transferred debt from short-term to long-term funding. In addition, firm-specific factors, such as firm size, tangibility, and macroeconomic factors, such as GDP growth, positively and significantly impact capital financing. Conversely, profitability has a negative relationship with financial leverage. There is a lack of empirical research on how COVID-19 affects the financial structure of non-financial listed companies in GCC nations. Consequently, by filling the previously specified gaps, this study provides proof to support the idea of using debt financing to raise capital for economic recovery. GCC policymakers need to give priority to ensuring that firms have convenient access to inexpensive finance in light of the financial consequences caused by COVID-19. This will guarantee that companies have the resources necessary to bounce back and support economic growth. Full article
(This article belongs to the Special Issue Economics after the COVID-19)
15 pages, 5652 KiB  
Article
Numerical Investigation of Micrometer-Sensitive Particle Intrusion in Hydraulic Valve Clearances and Its Impact on Valve Performance
by Jianjun Zhang, Hong Ji, Wenjie Zhao, Qianpeng Chen and Xinqiang Liu
Processes 2024, 12(5), 864; https://doi.org/10.3390/pr12050864 - 25 Apr 2024
Cited by 1 | Viewed by 608
Abstract
The intrusion of micrometer-sensitive contaminant particles into the clearance of sliding valves within hydraulic fluids is one of the root causes of valve sticking and reliability issues in hydraulic systems. To reveal the transient process and characteristics of particle intrusion into the clearance [...] Read more.
The intrusion of micrometer-sensitive contaminant particles into the clearance of sliding valves within hydraulic fluids is one of the root causes of valve sticking and reliability issues in hydraulic systems. To reveal the transient process and characteristics of particle intrusion into the clearance process, this paper proposes a numerical method for fluid–particle one-way coupling and verifies it through experimentation. Furthermore, a numerical simulation of the motion trajectory of spherical iron particles inside the valve chamber was conducted in a two-dimensional flow model. It was discovered that in a steady-state flow field with a certain valve opening, micrometer-sized particles in the valve chamber’s hydraulic fluid mainly move with the valve flow stream, and the number of micron particles invading the slide valve clearance and the probability of invasion is related to the slide valve opening and differential pressure. When the slide valve opening decreases, especially in the small opening state, the probability of particles invading the slide valve clearance will increase dramatically, and the probability of invading the clearance is as high as 27% in a valve opening of 50 μm; the larger the pressure difference between the valve ports, the more the number of particles invading the slide valve clearance increases; the particles in the inlet of the slide valve clearance are more prone to invade the slide valve clearance, and invade in an inclined way, touching the wall and then bouncing back. These findings are of great value for the design of highly reliable hydraulic control valves and the understanding of the mechanism of slide valve stalls and provide an important scientific basis for the optimization and improvement in the reliability of hydraulic systems. Full article
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<p>Schematic diagram of the structure of the slide valve.</p>
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<p>Three-dimensional diagram of the experimental model.</p>
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<p>Structure of bottom plate and size of main channel (unit: mm).</p>
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<p>High-speed visualization experimental platform for particle trajectory in valve chamber.</p>
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<p>Micrograph of spherical iron particles with a diameter of 0.5 mm.</p>
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<p>Meshing of the enlarged clearance model.</p>
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<p>Influence of the number of grids on the inlet flow rate and the maximum flow velocity at the left clearance outlet.</p>
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<p>High-speed photographic image of particle movement in the enlarged model.</p>
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<p>Flow field pressure distribution and flow line diagram.</p>
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<p>Particle motion trajectory.</p>
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<p>Two-dimensional model of slide valve chamber (unit: mm).</p>
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<p>Mesh division of the valve cavity basin of the 20 μm slide valve with clearance.</p>
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<p>Flow diagram of particle motion trajectory and local flow field of particles in valve chamber: (<b>a</b>) particle motion trajectory in valve chamber flow field; (<b>b</b>) particle movement path at the entrance of clearance 1; (<b>c</b>) gClearance 1 inlet fluid flow diagram; (<b>d</b>) flow line and pressure distribution of the flow field in the valve chamber; The areas in (<b>b</b>,<b>c</b>) are the areas shown by the red square in (<b>a</b>).</p>
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<p>Change in the number of particles in the clearance of the invading slide valve with the opening of the valve port.</p>
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<p>The change in the number of particles in the clearance of the invading slide valve with the pressure difference at the valve port.</p>
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23 pages, 8730 KiB  
Article
The Lattice Boltzmann Method Using Parallel Computation: A Great Potential Solution for Various Complicated Acoustic Problems
by Pranowo, Djoko Budiyanto Setyohadi and Agung Tri Wijayanta
Math. Comput. Appl. 2024, 29(1), 12; https://doi.org/10.3390/mca29010012 - 4 Feb 2024
Cited by 1 | Viewed by 1542
Abstract
This paper proposes the D2Q5 Lattice Boltzmann method (LBM) method, in two dimensions with five discrete lattice velocities, for simulating linear sound wave propagation in closed rooms. A second-order linear acoustic equation obtained from the LBM method was used as the model equation. [...] Read more.
This paper proposes the D2Q5 Lattice Boltzmann method (LBM) method, in two dimensions with five discrete lattice velocities, for simulating linear sound wave propagation in closed rooms. A second-order linear acoustic equation obtained from the LBM method was used as the model equation. Boundary conditions at the domain boundary use the bounce-back scheme. The LBM numerical calculation algorithm in this paper is relatively simpler and easy to implement. Parallelization with the GPU CUDA was implemented to speed up the execution time. The calculation results show that the use of parallel GPU CUDA programming can accelerate the proposed simulation 27.47 times faster than serial CPU programming. The simulation results are validated with analytical solutions for acoustic pulse reflected by the flat and oblique walls, the comparisons show very good concordance, and the D2Q5 LBM has second-order accuracy. In addition, the simulation results in the form of wavefront propagation images in complicated shaped rooms are also compared with experimental photographs, and the comparison also shows excellent concordance. The numerical results of the D2Q5 LBM are promising and also demonstrate the great capability of the D2Q5 LBM for investigating room acoustics in various complexities. Full article
(This article belongs to the Section Engineering)
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<p>The two-dimensional lattice D2Q5 model.</p>
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<p>Illustration of the streaming step.</p>
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<p>Illustration of kernel execution and thread organization.</p>
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<p>The convergence rate of the D2Q5 LBM.</p>
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<p>Closed rectangle domain and the location of source and receiver.</p>
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<p>Snapshots of reflected waves by the flat bottom wall: (<b>a</b>) at <span class="html-italic">t</span> = 3 ms; (<b>b</b>) at <span class="html-italic">t</span> = 9 ms; (<b>c</b>) at <span class="html-italic">t</span> = 15 ms; (<b>d</b>) at <span class="html-italic">t</span> = 21 ms.</p>
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<p>Signal recorded at the receiver of the first example (<b>a</b>) comparing numerical pressure and analytical solutions of pressure at the receiver; (<b>b</b>) discrepancies of numerical and analytical solutions.</p>
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<p>Closed five-sided polygonal domain and the location of source and receiver.</p>
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<p>Snapshots of reflected waves by oblique wall: (<b>a</b>) at <span class="html-italic">t</span> = 1.25 ms; (<b>b</b>) at <span class="html-italic">t</span> = 5.00 ms; (<b>c</b>) at <span class="html-italic">t</span> = 8.75 ms; (<b>d</b>) at <span class="html-italic">t</span> = 12.50 ms.</p>
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<p>Snapshots of reflected waves by oblique wall: (<b>a</b>) at <span class="html-italic">t</span> = 1.25 ms; (<b>b</b>) at <span class="html-italic">t</span> = 5.00 ms; (<b>c</b>) at <span class="html-italic">t</span> = 8.75 ms; (<b>d</b>) at <span class="html-italic">t</span> = 12.50 ms.</p>
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<p>Signal recorded at the receiver of the second example (<b>a</b>) comparison between numerical pressure and analytical solutions of pressure at the receiver; (<b>b</b>) discrepancies of numerical and analytical solutions.</p>
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<p>Complex room geometry: (<b>a</b>) Type 1; (<b>b</b>) Type 2 [<a href="#B38-mca-29-00012" class="html-bibr">38</a>].</p>
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<p>Snapshots of the acoustic pulse propagation in complex room Type 1: (<b>a</b>) at <span class="html-italic">t</span> = 2 ms; (<b>b</b>) at <span class="html-italic">t</span> = 7 ms; (<b>c</b>) at <span class="html-italic">t</span> = 19.333 ms; (<b>d</b>) at <span class="html-italic">t</span> = 31.667 ms.</p>
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<p>Two successive sound photographs in architectural models for room Type 1 [<a href="#B38-mca-29-00012" class="html-bibr">38</a>].</p>
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<p>Snapshots of the acoustic pulse propagation in complex room Type 1: (<b>a</b>) at <span class="html-italic">t</span> = 2.4 ms; (<b>b</b>) at <span class="html-italic">t</span> = 6.4 ms; (<b>c</b>) at <span class="html-italic">t</span> = 18.8 ms; (<b>d</b>) at <span class="html-italic">t</span> = 36 ms.</p>
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<p>Two successive sound photographs in architectural models for room Type 2 [<a href="#B38-mca-29-00012" class="html-bibr">38</a>].</p>
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<p>Pressure fluctuation recorded at the room receiver: (<b>a</b>) Type 1; (<b>b</b>) Type 2.</p>
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<p>Staggered grids.</p>
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<p>Staircase boundary.</p>
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<p>Comparisons of signal recorded at the receiver (<b>a</b>) comparison between numerical (LBM and FDTD) pressure and analytical solutions of pressure at the receiver; (<b>b</b>) discrepancies of numerical (LBM and FDTD) and analytical solutions.</p>
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<p>Comparisons of signal recorded at the receiver (<b>a</b>) comparison between numerical (LBM and FDTD) pressure and analytical solutions of pressure at the receiver; (<b>b</b>) discrepancies of numerical (LBM and FDTD) and analytical solutions.</p>
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18 pages, 1329 KiB  
Article
Adaptive Kalman Filter for Real-Time Visual Object Tracking Based on Autocovariance Least Square Estimation
by Jiahong Li, Xinkai Xu, Zhuoying Jiang and Beiyan Jiang
Appl. Sci. 2024, 14(3), 1045; https://doi.org/10.3390/app14031045 - 25 Jan 2024
Viewed by 1042
Abstract
Real-time visual object tracking (VOT) may suffer from performance degradation and even divergence owing to inaccurate noise statistics typically engendered by non-stationary video sequences or alterations in the tracked object. This paper presents a novel adaptive Kalman filter (AKF) algorithm, termed AKF-ALS, based [...] Read more.
Real-time visual object tracking (VOT) may suffer from performance degradation and even divergence owing to inaccurate noise statistics typically engendered by non-stationary video sequences or alterations in the tracked object. This paper presents a novel adaptive Kalman filter (AKF) algorithm, termed AKF-ALS, based on the autocovariance least square estimation (ALS) methodology to improve the accuracy and robustness of VOT. The AKF-ALS algorithm involves object detection via an adaptive thresholding-based background subtraction technique and object tracking through real-time state estimation via the Kalman filter (KF) and noise covariance estimation using the ALS method. The proposed algorithm offers a robust and efficient solution to adapting the system model mismatches or invalid offline calibration, significantly improving the state estimation accuracy in VOT. The computation complexity of the AKF-ALS algorithm is derived and a numerical analysis is conducted to show its real-time efficiency. Experimental validations on tracking the centroid of a moving ball subjected to projectile motion, free-fall bouncing motion, and back-and-forth linear motion, reveal that the AKF-ALS algorithm outperforms a standard KF with fixed noise statistics. Full article
(This article belongs to the Special Issue Autonomous Vehicles and Robotics)
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<p>Flowchart of the ALS-KF based VOT algorithm.</p>
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<p>Performance of model noise covariance estimation <math display="inline"><semantics> <msub> <mi>Q</mi> <mrow> <mi>A</mi> <mi>L</mi> <mi>S</mi> </mrow> </msub> </semantics></math> using ALS algorithm over 500 Monte Carlo simulations. The blue dots denote the estimated diagonal-form model noise covariance matrix <math display="inline"><semantics> <mrow> <msub> <mi>Q</mi> <mrow> <mi>M</mi> <mi>C</mi> </mrow> </msub> <mo>=</mo> <mi>d</mi> <mi>i</mi> <mi>a</mi> <mi>g</mi> <mrow> <mo>(</mo> <msub> <mover accent="true"> <mi>Q</mi> <mo stretchy="false">^</mo> </mover> <mn>11</mn> </msub> <mo>,</mo> <msub> <mover accent="true"> <mi>Q</mi> <mo stretchy="false">^</mo> </mover> <mn>22</mn> </msub> <mo>)</mo> </mrow> </mrow> </semantics></math> over each Monte Carlo simulation, where the x-axis and y-axis represent the first and second diagonal elements respectively. The black bold dot is the model noise covariance estimate <math display="inline"><semantics> <msub> <mover accent="true"> <mi>Q</mi> <mo stretchy="false">^</mo> </mover> <mrow> <mi>A</mi> <mi>L</mi> <mi>S</mi> </mrow> </msub> </semantics></math> via the ALS algorithm. The intersection of two red dotted lines denotes the true noise covariance <math display="inline"><semantics> <msub> <mi>Q</mi> <mrow> <mi>t</mi> <mi>r</mi> <mi>u</mi> <mi>e</mi> </mrow> </msub> </semantics></math>.</p>
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<p>Performance of measurement noise covariance estimation <math display="inline"><semantics> <msub> <mi>R</mi> <mrow> <mi>A</mi> <mi>L</mi> <mi>S</mi> </mrow> </msub> </semantics></math> using ALS algorithm over 500 Monte Carlo simulations. The blue bars denote the estimated measurement noise covariance value <math display="inline"><semantics> <msub> <mi>R</mi> <mrow> <mi>M</mi> <mi>C</mi> </mrow> </msub> </semantics></math> over each Monte Carlo simulation, where the x-axis and y-axis respectively represent the measurement noise covariance value and the probabilistic density. The black bold dot is the measurement noise covariance estimate <math display="inline"><semantics> <msub> <mover accent="true"> <mi>Q</mi> <mo stretchy="false">^</mo> </mover> <mrow> <mi>A</mi> <mi>L</mi> <mi>S</mi> </mrow> </msub> </semantics></math> via the ALS algorithm. The intersection of the red dotted line and x-axis denotes the true noise covariance <math display="inline"><semantics> <msub> <mi>Q</mi> <mrow> <mi>t</mi> <mi>r</mi> <mi>u</mi> <mi>e</mi> </mrow> </msub> </semantics></math>.</p>
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<p>VOT using the proposed AKF-ALS algorithm and traditional KF algorithm. The green, blue, and red circles, respectively, represent the circle of the ball with true centroid, with estimated centroid using AKF-ALS algorithm, and with estimated centroid using KF algorithm.</p>
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<p>Bounding box-based pedestrian tracking with occlusions using AKF-ALS algorithm.</p>
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18 pages, 4770 KiB  
Article
Come and Gone! Psychological Resilience and Organizational Resilience in Tourism Industry Post COVID-19 Pandemic: The Role of Life Satisfaction
by Ibrahim A. Elshaer
Sustainability 2024, 16(2), 939; https://doi.org/10.3390/su16020939 - 22 Jan 2024
Cited by 2 | Viewed by 1646
Abstract
This research paper delves into the multifaceted relationships between psychological resilience, organizational trust, life satisfaction, and organizational resilience within the context of tourism firms in Egypt. Against the backdrop of the COVID-19 pandemic and its profound effects on the tourism industry, the study [...] Read more.
This research paper delves into the multifaceted relationships between psychological resilience, organizational trust, life satisfaction, and organizational resilience within the context of tourism firms in Egypt. Against the backdrop of the COVID-19 pandemic and its profound effects on the tourism industry, the study aims to unravel the intricate interplay of individual and organizational factors that contribute to the adaptive capacity and well-being of employees. The research employs a quantitative methodology, engaging full-time sales and marketing employees from five-star hotels and class A travel agents (660) as key participants, employing SmartPLS-SEM vs4 to analyze the collected data. Through a nuanced examination of their experiences post-pandemic, the study investigates how psychological resilience, defined as the ability to bounce back from adversity, influences both life satisfaction and organizational resilience. Additionally, the impact of organizational trust, characterized by the confidence and faith employees place in their organization, on life satisfaction and organizational resilience is explored. Preliminary findings suggest a positive association between psychological resilience and both life satisfaction and organizational resilience. Employees exhibiting higher levels of psychological resilience tend to not only experience greater life satisfaction but also contribute significantly to their organization’s resilience. Furthermore, organizational trust emerges as a critical factor, positively influencing life satisfaction and organizational resilience. The study contributes valuable insights to the evolving landscape of tourism management and lays the foundation for future research endeavors in this domain. Full article
(This article belongs to the Section Tourism, Culture, and Heritage)
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<p>Research framework. + Means positive effect.</p>
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<p>The examined research model.</p>
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15 pages, 3124 KiB  
Article
Microchannel Gas Flow in the Multi-Flow Regime Based on the Lattice Boltzmann Method
by Xiaoyu Li, Zhi Ning and Ming Lü
Entropy 2024, 26(1), 84; https://doi.org/10.3390/e26010084 - 18 Jan 2024
Viewed by 1108
Abstract
In this work, a lattice Boltzmann method (LBM) for studying microchannel gas flow is developed in the multi-flow regime. In the LBM, by comparing previous studies’ results on effective viscosity in multi-flow regimes, the values of the rarefaction factor applicable to multi-flow regions [...] Read more.
In this work, a lattice Boltzmann method (LBM) for studying microchannel gas flow is developed in the multi-flow regime. In the LBM, by comparing previous studies’ results on effective viscosity in multi-flow regimes, the values of the rarefaction factor applicable to multi-flow regions were determined, and the relationship between relaxation time and Kn number with the rarefaction factor is given. The Kn number is introduced into the second-order slip boundary condition together with the combined bounce-back/specular-reflection (CBBSR) scheme to capture the gas flow in the multi-flow regime. Sensitivity analysis of the dimensionless flow rate to adjustable parameters using the Taguchi method was carried out, and the values of adjustable parameters were determined based on the results of the sensitivity analysis. The results show that the dimensionless flow rate is more sensitive to j than h. Numerical simulations of Poiseuille flow and pulsating flow in a microchannel with second-order slip boundary conditions are carried out to validate the method. The results show that the velocity profile and dimensionless flow rate simulated by the present numerical simulation method in this work are found in the multi-flow regime, and the phenomenon of annular velocity profile in the microchannel is reflected in the phases. Full article
(This article belongs to the Special Issue Mesoscopic Fluid Mechanics)
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<p>Dimensionless effective viscosity with <span class="html-italic">Kn</span>. The black line, the red line and the blue line are rarefied gas coefficient of 1.5 and 1.7 and 2, respectively. Triangle is the IP method by Roohi and Darbbandi [<a href="#B39-entropy-26-00084" class="html-bibr">39</a>], square is the DSMC method by Michalis et al. [<a href="#B20-entropy-26-00084" class="html-bibr">20</a>], and circle is the theoretical method by Stops [<a href="#B30-entropy-26-00084" class="html-bibr">30</a>].</p>
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<p>Comparison between the simulated dimensionless flow rate with different <span class="html-italic">j</span> and linearized BE solutions by Cercignani et al. [<a href="#B50-entropy-26-00084" class="html-bibr">50</a>].</p>
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<p>Comparison between the simulated dimensionless flow rate with different <span class="html-italic">h</span> and linearized BE solutions by Cercignani et al. [<a href="#B50-entropy-26-00084" class="html-bibr">50</a>].</p>
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<p>Relative deviation with <span class="html-italic">Kn</span>.</p>
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<p>Velocity profile of Poiseuille flow in a microchannel. From figure (<b>a</b>–<b>h</b>) are velocity profile with different <span class="html-italic">Kn</span>. (<b>a</b>,<b>b</b>) N-S by Bahukudumbi and Beskok [<a href="#B47-entropy-26-00084" class="html-bibr">47</a>]. (<b>c</b>–<b>e</b>) N-S by Hadjiconstantinou [<a href="#B42-entropy-26-00084" class="html-bibr">42</a>], CLB by Liu and Feng [<a href="#B17-entropy-26-00084" class="html-bibr">17</a>], MRTLB by Guo et al. [<a href="#B28-entropy-26-00084" class="html-bibr">28</a>], LB by Ohwada [<a href="#B51-entropy-26-00084" class="html-bibr">51</a>]. (<b>f</b>–<b>h</b>) CLB by Liu and Feng [<a href="#B17-entropy-26-00084" class="html-bibr">17</a>], MRTLB by Guo et al. [<a href="#B28-entropy-26-00084" class="html-bibr">28</a>], FMLB by Zhou and Zhong [<a href="#B41-entropy-26-00084" class="html-bibr">41</a>], LB by Ohwada [<a href="#B51-entropy-26-00084" class="html-bibr">51</a>].</p>
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<p>Velocity profile of Poiseuille flow in a microchannel. From figure (<b>a</b>–<b>h</b>) are velocity profile with different <span class="html-italic">Kn</span>. (<b>a</b>,<b>b</b>) N-S by Bahukudumbi and Beskok [<a href="#B47-entropy-26-00084" class="html-bibr">47</a>]. (<b>c</b>–<b>e</b>) N-S by Hadjiconstantinou [<a href="#B42-entropy-26-00084" class="html-bibr">42</a>], CLB by Liu and Feng [<a href="#B17-entropy-26-00084" class="html-bibr">17</a>], MRTLB by Guo et al. [<a href="#B28-entropy-26-00084" class="html-bibr">28</a>], LB by Ohwada [<a href="#B51-entropy-26-00084" class="html-bibr">51</a>]. (<b>f</b>–<b>h</b>) CLB by Liu and Feng [<a href="#B17-entropy-26-00084" class="html-bibr">17</a>], MRTLB by Guo et al. [<a href="#B28-entropy-26-00084" class="html-bibr">28</a>], FMLB by Zhou and Zhong [<a href="#B41-entropy-26-00084" class="html-bibr">41</a>], LB by Ohwada [<a href="#B51-entropy-26-00084" class="html-bibr">51</a>].</p>
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<p>Dimensionless flow rate of Poiseuille flow in a microchannel. Chain line is the N-S method by Hadjiconstantinou [<a href="#B42-entropy-26-00084" class="html-bibr">42</a>], dotted line is the MRTLB method by Guo et al. [<a href="#B28-entropy-26-00084" class="html-bibr">28</a>], and circle is the Experimental method by Dong [<a href="#B52-entropy-26-00084" class="html-bibr">52</a>].</p>
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<p>Velocity profile of pulsating flow in a microchannel.</p>
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32 pages, 8581 KiB  
Article
Structure Design of Bionic PDC Cutter and the Characteristics of Rock Breaking Processes
by Zebing Wu, Ruofei Yuan, Wenxi Zhang, Jiale Liu and Shiyao Hu
Processes 2024, 12(1), 66; https://doi.org/10.3390/pr12010066 - 27 Dec 2023
Cited by 2 | Viewed by 1010
Abstract
The rational structural design of polycrystalline diamond compact (PDC) cutters effectively enhances the performance of drill bits in rock fragmentation and extends their service life. Inspired by bionics, a bionic PDC cutter was designed, taking the mole claw toe, shark tooth, and microscopic [...] Read more.
The rational structural design of polycrystalline diamond compact (PDC) cutters effectively enhances the performance of drill bits in rock fragmentation and extends their service life. Inspired by bionics, a bionic PDC cutter was designed, taking the mole claw toe, shark tooth, and microscopic biomaterial structures as the bionic prototypes. To verify its rock-breaking effectiveness, the finite element method was employed to compare the rock-breaking processes of the bionic cutter, triangular prism cutter, and axe cutter. The study also investigated the influence of different back rake angles, cutting depths, arc radii, and hydrostatic pressures on rock breaking using the bionic cutter. Prior to this, the accuracy of the finite element model was validated through laboratory tests. Subsequently, a drill bit incorporating all three types of cutters was constructed, and simulations of rock breaking were conducted on a full-sized drill bit. The results demonstrate that the bionic cutter exhibits superior load concentration on the rock compared to the triangular prism cutter and the axe cutter. Additionally, its arc structure facilitates the “shoveling” of the rock, making it more susceptible to breakage under tensile stress. As a result, the efficiency of the bionic cutter surpasses that of the triangular prism and axe cutters. Similarly, it exhibits minimal fluctuations and values in cutting force. As the back rake angle and cutting depth increase, the MSE and cutting force of all three cutters also increase. However, the bionic cutter consistently maintains the lowest MSE and cutting force, confirming the superiority of its bionic structural design. The MSE and cutting force of the bionic cutter fluctuate with the increase of the arc radius, and the optimal arc radius falls within the simulation range, between 21 mm and 23 mm. Compared to the other two types of cutters, bionic cutters possess a unique structure that allows for better release of internal stress within the rock, thereby ensuring higher efficiency in rock-breaking, particularly in deep geological formations. The rock breaking simulation results of full-sized drill bits show that the use of a bionic cutter can improve the drill bit’s ability to penetrate the formation, reduce the possibility of drill bit bounce during the rock breaking process, prevent the occurrence of stick-slip, improve the drilling stability, effectively improve the efficiency and service life of the drill bit during the rock breaking process, and reduce the drilling cost. It is concluded that the research results of bionic PDC cutters are helpful to the development of high-performance drill bits and the reduction of drilling costs. Full article
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<p>Mole’s claws and toes.</p>
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<p>Arc structure design.</p>
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<p>Signs of teeth crunching.</p>
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<p>Shark’s teeth.</p>
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<p>Saw structure design.</p>
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<p>Microscopic material structure: (<b>a</b>) grain boundary structure; (<b>b</b>) grain boundary structure amplification.</p>
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<p>Structural design: (<b>a</b>) design of the junction structure; (<b>b</b>) overall structure.</p>
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<p>Assembly model.</p>
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<p>Cutter structure: (<b>a</b>) triangular prism cutter; (<b>b</b>) axe-shaped cutter.</p>
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<p>Stress–strain curve of rock.</p>
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<p>Mesh model: (<b>a</b>) equiaxial view; (<b>b</b>) side view.</p>
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<p>Three-dimensional model of the cutting structure of the bit.</p>
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<p>Finite element model.</p>
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<p>Cutting forces for testing and simulation of triangular prism cutters.</p>
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<p>Cutting force and specific mechanical energy for three cutters: (<b>a</b>) cutting force; (<b>b</b>) MSE.</p>
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<p>Stress contours at the beginning of the cutter breaking: (<b>a</b>) triangular prism cutter; (<b>b</b>) axe cutter; (<b>c</b>) bionic cutter.</p>
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<p>Stress contours during rock breaking by three different cutters.</p>
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<p>Displacement and shear stress contours during rock breaking by three different cutters: (<b>a</b>) displacement; (<b>b</b>) shear stress.</p>
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<p>Contact stress contours during rock breaking with different cutters.</p>
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<p>Relationship between the back rake angle and the mean value of cutting force for three types of cutters: (<b>a</b>) triangular prism cutter; (<b>b</b>) axe cutter; (<b>c</b>) bionic cutter.</p>
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<p>Relationship between the angle of back rake angle and the MSE for three types of cutters: (<b>a</b>) triangular prism cutter; (<b>b</b>) axe cutter; (<b>c</b>) bionic cutter.</p>
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<p>Contact stress distribution of bionic cutters with different back rake angles.</p>
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<p>Stress contours of bionic cutters with different back rack angles on rocks.</p>
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<p>Rock-breaking displacement contours of bionic cutter under different back rake angles.</p>
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<p>Variation of cutting forces at different depths of cut for three types of cutters: (<b>a</b>) triangular prism cutter; (<b>b</b>) axe cutter; (<b>c</b>) bionic cutter.</p>
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<p>Depth of cut vs. MSE for three cutters: (<b>a</b>) triangular prism cutter; (<b>b</b>) axe cutter; (<b>c</b>) bionic cutter.</p>
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<p>Cutting force and MSE of rock breaking by bionic cutters with different arc radii: (<b>a</b>) mean cutting force; (<b>b</b>) MSE.</p>
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<p>Contact stress distribution of bionic cutters with different arc radii during the rock-breaking process.</p>
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<p>Diagram of applying hydrostatic pressure.</p>
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<p>Rock-breaking stress contour of three kinds of cutters under different hydrostatic pressures.</p>
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<p>The mean cutting force and MSE change of three cutters under different hydrostatic pressure: (<b>a</b>) Mean cutting force; (<b>b</b>) MSE.</p>
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<p>Wellbore stress contours at different moments for the three drill bits.</p>
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<p>Rock-breaking footage for three drill bits.</p>
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<p>Counter torque for three drill bits.</p>
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16 pages, 1844 KiB  
Article
A Co-Adaptation Method for Resilience Rebound in Unmanned Aerial Vehicle Swarms in Surveillance Missions
by Kunlun Wei, Tao Zhang and Chuanfu Zhang
Drones 2024, 8(1), 4; https://doi.org/10.3390/drones8010004 - 26 Dec 2023
Viewed by 1703
Abstract
An unmanned aerial vehicle (UAV) swarm is a fast-moving system where self-adaption is necessary when conducting a mission. The major causative factors of mission failures are inevitable disruptive events and uncertain threats. Given the unexpected disturbances of events and threats, it is important [...] Read more.
An unmanned aerial vehicle (UAV) swarm is a fast-moving system where self-adaption is necessary when conducting a mission. The major causative factors of mission failures are inevitable disruptive events and uncertain threats. Given the unexpected disturbances of events and threats, it is important to study how a UAV swarm responds and enable the swarm to enhance resilience and alleviate negative influences. Cooperative adaptation must be established between the swarm’s structure and dynamics, such as communication links and UAV states. Thus, based on previous structural adaptation and dynamic adaptation models, we provide a co-adaptation model for UAV swarms that combines a swarm’s structural characteristics with its dynamic characteristics. The improved model can deal with malicious events and contribute to a rebound in the swarm’s performance. Based on the proposed co-adaptation model, an improved resilience metric revealing the discrepancy between the minimum performance and the standard performance is proposed. The results from our simulation experiments show that the surveillance performance of a UAV swarm bounces back to its initial state after disruptions happen in co-adaptation cases. This metric demonstrates that our model can contribute towards the swarm’s overall systemic resiliency by withstanding and resisting unpredictable threats and disruptions. The model and metric proposed in this article can help identify best practices in improving swarm resilience. Full article
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<p>A sketch map of a UAV swarm.</p>
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<p>Static model.</p>
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<p>Structural adaptation model.</p>
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<p>Dynamic adaptation model.</p>
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<p>Co-adaptation model.</p>
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<p>A collaborative surveillance mission utilizing a UAV swarm.</p>
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<p>The overlap surveillance area of two adjacent UAVs.</p>
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<p>Schematic of single UAV performance curve.</p>
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<p>Surveillance mission over a specified battlefield.</p>
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<p><math display="inline"><semantics> <mrow> <mi>y</mi> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </semantics></math> as total messages under different communication links numbers.</p>
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<p><math display="inline"><semantics> <mrow> <mi>y</mi> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </semantics></math> as surveillance area under different disturbance programs.</p>
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<p><math display="inline"><semantics> <mrow> <mi>y</mi> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </semantics></math> as surveillance area under different models.</p>
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<p>Resilience value obtained via Tran et al. [<a href="#B4-drones-08-00004" class="html-bibr">4</a>] (<b>a</b>) and our for proposed method (<b>b</b>) for each event.</p>
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<p>Contrast between total resilience value of our proposed method and Tran.</p>
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18 pages, 1182 KiB  
Review
Urban in Question: Recovering the Concept of Urban in Urban Resilience
by Shomon Shamsuddin
Sustainability 2023, 15(22), 15907; https://doi.org/10.3390/su152215907 - 14 Nov 2023
Cited by 1 | Viewed by 1826
Abstract
Existential threats from climate change, weather-related disasters, and other crises have drawn increasing attention to urban resilience. Prior work has focused on explicating resilience and proposing various definitions of it. But the emphasis on describing resilience might overlook what urban means in discussions [...] Read more.
Existential threats from climate change, weather-related disasters, and other crises have drawn increasing attention to urban resilience. Prior work has focused on explicating resilience and proposing various definitions of it. But the emphasis on describing resilience might overlook what urban means in discussions of urban resilience. This paper investigates how urban resilience scholarship conceptualizes and defines the term urban. I conduct a literature review and content analysis of recently published urban resilience articles. The results reveal how urban is prominently featured, but its conceptual use is not identified, and the term is left undefined. The findings suggest serious concerns about the applicability and generalizability of urban resilience to different contexts. The paper contributes to the literature by showing how conceptualizing urban alternately as a shared subject of study, influential condition, or measurement category has far-reaching implications for urban resilience planning, implementation, and assessment. Drawing upon the idea of simulated annealing, the paper suggests that taking a few conceptual steps backward may help our understanding of urban resilience—and cities to bounce back better. Full article
(This article belongs to the Section Sustainable Urban and Rural Development)
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<p>Depiction of urban growth process.</p>
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<p>Article selection process.</p>
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<p>Hill climbing with error.</p>
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11 pages, 324 KiB  
Article
Investigation of Nurses’ Wellbeing towards Errors in Clinical Practice—The Role of Resilience
by Despoina Pappa, Ioannis Koutelekos, Eleni Evangelou, Evangelos Dousis, Polyxeni Mangoulia, Georgia Gerogianni, Afroditi Zartaloudi, Georgia Toulia, Martha Kelesi, Nikoletta Margari, Eftychia Ferentinou, Areti Stavropoulou and Chrysoula Dafogianni
Medicina 2023, 59(10), 1850; https://doi.org/10.3390/medicina59101850 - 18 Oct 2023
Cited by 2 | Viewed by 1999
Abstract
Background and Objectives: The fatigue, stress, and burnout of nurses lead to them frequently making mistakes, which have a negative impact not only on the safety of the patients but also on their psychology. The ability to bounce back from mistakes is [...] Read more.
Background and Objectives: The fatigue, stress, and burnout of nurses lead to them frequently making mistakes, which have a negative impact not only on the safety of the patients but also on their psychology. The ability to bounce back from mistakes is crucial for nurses. Nursing staff members’ physical and mental health, particularly their depression, is far from ideal, and this ill health is directly correlated with the frequency of self-reported medical errors. The nurses’ mental and physical health are also positively correlated with their perception of wellness support at work. This cross-sectional study aimed to investigate the status of nurses’ mental and physical health regarding clinical errors and the impact of resilience on coping with these situations. Materials and Methods: A total of 364 healthcare professionals participated in this research; 87.5% of them were females and 12.5% of them were males. Most of the participants were 22–35 years old. The median number of years of employment was nine. Clinical nurses anonymously and voluntarily completed a special structured questionnaire that included questions from different validated tools in order to assess their state of physical and mental wellbeing after events of stress and errors made during their practice. Results: In total, 49.4% of the nurses had made an error on their own, and 73.2% had witnessed an error that someone else had made. At the time of the error, 29.9% of the participants were in charge of more than 20 patients, while 28.9% were responsible for a maximum of three patients. Participants who were 36–45 years old had more resilience (p = 0.049) and experienced fewer negative emotions than participants who were 22–35 years old. The participants who mentioned more positive feelings according to their mental state had greater resilience (p > 0.001). Conclusions: Errors were likely to happen during clinical practice due to nurses’ negative experiences. The level of resilience among the nursing population was found to play a very important role not only in making mistakes but also in coping with errors during their daily routine. Wellness and prevention must be given top priority in all healthcare systems across the country in order to promote nurses’ optimal health and wellbeing, raise the standard of care, and reduce the likelihood of expensive, avoidable medical errors. Healthcare administrations should promote prevention programs for stress occurrence in order to support nurses’ wellbeing maintenance. Full article
(This article belongs to the Section Epidemiology & Public Health)
15 pages, 316 KiB  
Entry
Research Trends in Resilience and Vulnerability Studies
by Christopher L. Atkinson
Encyclopedia 2023, 3(4), 1208-1222; https://doi.org/10.3390/encyclopedia3040088 - 30 Sep 2023
Cited by 1 | Viewed by 2251
Definition
While the definition of resilience is disputed or even fuzzy, due in no small part to the diversity of its applications, the concept generally involves the ability to withstand and bounce back from shocks; vulnerability as a related concept involves the tendency to [...] Read more.
While the definition of resilience is disputed or even fuzzy, due in no small part to the diversity of its applications, the concept generally involves the ability to withstand and bounce back from shocks; vulnerability as a related concept involves the tendency to suffer from shocks, given existing characteristics that may prevent resilient responses. Vulnerabilities put individuals, groups, and societies at greater risk and disadvantage, suggesting a need not only for disaster response and recovery, but mitigation and preparedness. Resilience and vulnerability research has recently focused on the role of government, the COVID-19 pandemic, and flood hazards; topics of interest have also included resilience of rural and urban areas, development and sustainability, and displacement and migration. Full article
(This article belongs to the Section Social Sciences)
23 pages, 1482 KiB  
Review
Role of NFE2L1 in the Regulation of Proteostasis: Implications for Aging and Neurodegenerative Diseases
by Aswathy Chandran, Haley Jane Oliver and Jean-Christophe Rochet
Biology 2023, 12(9), 1169; https://doi.org/10.3390/biology12091169 - 25 Aug 2023
Cited by 2 | Viewed by 2097
Abstract
A hallmark of aging and neurodegenerative diseases is a disruption of proteome homeostasis (“proteostasis”) that is caused to a considerable extent by a decrease in the efficiency of protein degradation systems. The ubiquitin proteasome system (UPS) is the major cellular pathway involved in [...] Read more.
A hallmark of aging and neurodegenerative diseases is a disruption of proteome homeostasis (“proteostasis”) that is caused to a considerable extent by a decrease in the efficiency of protein degradation systems. The ubiquitin proteasome system (UPS) is the major cellular pathway involved in the clearance of small, short-lived proteins, including amyloidogenic proteins that form aggregates in neurodegenerative diseases. Age-dependent decreases in proteasome subunit expression coupled with the inhibition of proteasome function by aggregated UPS substrates result in a feedforward loop that accelerates disease progression. Nuclear factor erythroid 2- like 1 (NFE2L1) is a transcription factor primarily responsible for the proteasome inhibitor-induced “bounce-back effect” regulating the expression of proteasome subunits. NFE2L1 is localized to the endoplasmic reticulum (ER), where it is rapidly degraded under basal conditions by the ER-associated degradation (ERAD) pathway. Under conditions leading to proteasome impairment, NFE2L1 is cleaved and transported to the nucleus, where it binds to antioxidant response elements (AREs) in the promoter region of proteasome subunit genes, thereby stimulating their transcription. In this review, we summarize the role of UPS impairment in aging and neurodegenerative disease etiology and consider the potential benefit of enhancing NFE2L1 function as a strategy to upregulate proteasome function and alleviate pathology in neurodegenerative diseases. Full article
(This article belongs to the Section Neuroscience)
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<p>Mechanism of NFE2L1 activation. (<b>Top</b>) Under basal conditions, ER-associated NFE2L1 is retrotranslocated to the cytosolic side and undergoes deglycosylation by the N-glycanase NGLY1, followed by ERAD-dependent proteasomal degradation. (<b>Bottom</b>) Under conditions of proteasome impairment, NFE2L1 is deglycosylated by NGLY1 and N-terminally cleaved by the protease DDI-2. The cleaved fragment is translocated to the nucleus, where it modulates the transcription of ARE-dependent genes. Figure created with BioRender.com, accessed on 19 June 2023.</p>
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<p>Schematic showing the domain architectures of three NFE2L1 isoforms (NFE2L1/Nrf1, TCF11, LCR-F1), Nrf2, and Nrf3. The domains are as follows: N-terminal domain (NTD); Nrf2-ECH Homology Like (Neh2L, Neh5L, Neh6L, Neh3L) domains; Acidic Domain 1 (AD1); Asparagine/Serine/Threonine (NST) domain; Acidic Domain 2 (AD2); Serine Repeat (SR) domain; CNC-bZIP domain. Potential sites of post-translational modifications including N-glycosylation [<a href="#B122-biology-12-01169" class="html-bibr">122</a>,<a href="#B123-biology-12-01169" class="html-bibr">123</a>], phosphorylation [<a href="#B124-biology-12-01169" class="html-bibr">124</a>,<a href="#B125-biology-12-01169" class="html-bibr">125</a>,<a href="#B126-biology-12-01169" class="html-bibr">126</a>], O-GlcNAcylation [<a href="#B127-biology-12-01169" class="html-bibr">127</a>,<a href="#B128-biology-12-01169" class="html-bibr">128</a>,<a href="#B129-biology-12-01169" class="html-bibr">129</a>], and N-terminal truncation [<a href="#B93-biology-12-01169" class="html-bibr">93</a>] are also indicated. Figure created with BioRender.com, accessed on 30 July 2023.</p>
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<p>Model illustrating the neuroprotective function of NFE2L1: (<b>Left</b>) The UPS plays a major role in the degradation of amyloidogenic proteins such as α-synuclein in healthy neurons. (<b>Middle</b>) In neurons from patients with NDs such as PD, α-synuclein undergoes self-assembly to form oligomers and fibrils, a process that is facilitated by age- or aggregate-dependent inhibition of the proteasome. (<b>Right</b>) Upregulation of proteasome function via NFE2L1 activation should promote the clearance of monomeric α-synuclein, in turn leading to a decrease in α-synuclein aggregate burden and a slowing of PD progression. Figure created with BioRender.com, accessed on 30 July 2023.</p>
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