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

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

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

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

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (1,103)

Search Parameters:
Keywords = resolving set

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
17 pages, 1473 KiB  
Case Report
Tact Training with Augmentative Gestural Support for Language Disorder and Challenging Behaviors: A Case Study in an Italian Community-Based Setting
by Laura Turriziani, Rosa Vartellini, Maria Grazia Barcello, Marcella Di Cara and Francesca Cucinotta
J. Clin. Med. 2024, 13(22), 6790; https://doi.org/10.3390/jcm13226790 - 11 Nov 2024
Viewed by 306
Abstract
Background: Gestures or manual signing are valid options for augmentative and alternative communication. However, the data in the literature are limited to a few neurodevelopmental disorders, and less is known about its application in the community setting. Objectives: This case report explores the [...] Read more.
Background: Gestures or manual signing are valid options for augmentative and alternative communication. However, the data in the literature are limited to a few neurodevelopmental disorders, and less is known about its application in the community setting. Objectives: This case report explores the feasibility and preliminary efficacy of tact training with augmentative gestural support intervention for a child affected by a language disorder with challenging behaviors in a community setting. Methods: Baseline assessments were conducted using the Verbal Behavior Milestone Assessment and Placement Program (VB-MAPP) and Griffiths Mental Developmental Scale-III (GMDS-III). The patient received six months of standard treatment, consisting of neuropsychomotor and speech therapy each twice a week, with improved cooperation in proposed activities, but no improvement in language. Afterward, a total of 24 sessions of tact training with augmentative gestural support interventions were performed. Data were collected by two independent observers and analyzed to measure language and behavioral outcomes. Results: VB-MAPP scores increased form minimal communication and social interaction at T0 (baseline) to improved compliance but unchanged language skills at T1 (after standard therapy). After tack training with augmentative gestural support (T2), VB-MAPP scores showed significant improvements, with notable increases in verbal operants, independence in communication, and intersubjectivity skills. GMDS-III scores at T2 also demonstrated growth in social, communicative, and cognitive skills. Additionally, challenging behaviors were reduced by more than 70% and nearly resolved by the end of the intervention. Conclusions: Personalized approaches appear to be essential for interventions tailored to developmental age. Further research is needed to determine the effectiveness of these approaches for other neurodevelopmental disorders, identify patient characteristics that may be predictors of outcomes to tailor the intervention, and explore the generalization of the results obtained with these strategies. Full article
(This article belongs to the Special Issue Diagnosis, Treatment, and Prognosis of Neuropsychiatric Disorders)
Show Figures

Figure 1

Figure 1
<p>Barriers assessment. VB-MAPP at baseline (T0), after six months (T1), and after twelve months (T2). The barriers assessment determines the presence of 24 learning and language acquisition barriers frequently faced by children with Autism or developmental delays.</p>
Full article ">Figure 1 Cont.
<p>Barriers assessment. VB-MAPP at baseline (T0), after six months (T1), and after twelve months (T2). The barriers assessment determines the presence of 24 learning and language acquisition barriers frequently faced by children with Autism or developmental delays.</p>
Full article ">Figure 2
<p>VB-MAPP at T0-T1-T2. This figure illustrates the progression of the child’s performance based on the VB-MAPP assessment over three key time points.</p>
Full article ">Figure 3
<p>Griffiths Mental Developmental Scale-III at T1 and T2. In the GMDS-III assessment, the child obtains an equivalent age (AE) in months for each skill. In the bar graph, the AE values for each subscale obtained at six months and after twelve months have been placed side by side.</p>
Full article ">Figure 4
<p>Challenging behaviors measured at baseline (T0), after six months (T1) and after twelve months (T2). The duration was measured as they were persistent, and it was not possible to measure their frequency.</p>
Full article ">
25 pages, 10287 KiB  
Article
Multi-Objective Optimization for Controlling Conflicts in Roadway Surrounding Rock Induced by Floor Stress-Relief Groove
by Yanting Qin, Yuantian Sun, Guichen Li, Jinghua Li, Sen Yang, Enqing Chen and Cheng Zhang
Appl. Sci. 2024, 14(22), 10178; https://doi.org/10.3390/app142210178 - 6 Nov 2024
Viewed by 321
Abstract
This paper studies the effectiveness of the stress-relief groove on the floor of deep coal roadway and determines the influence of the stress-relief groove parameters on the surrounding rock through qualitative analysis. Based on the displacement conflict problem, evaluation indicators were established, and [...] Read more.
This paper studies the effectiveness of the stress-relief groove on the floor of deep coal roadway and determines the influence of the stress-relief groove parameters on the surrounding rock through qualitative analysis. Based on the displacement conflict problem, evaluation indicators were established, and the optimal solution set was obtained. The innovations of this research include: 1. For geotechnical numerical simulations, novel stress monitoring and plastic zone monitoring techniques have been introduced to accurately reflect the condition of the surrounding rock; 2. The effects of floor relief grooves in deep roadway on surrounding rock have been analyzed, and the advantages and utilities of central and corner relief grooves have been determined; 3. The usability of small datasets has been enhanced by applying SEGA to optimize machine learning models with data augmentation techniques; 4. Multi-objective optimization algorithms have been applied to geotechnical engineering, providing valuable references for decision making. The results demonstrate that multi-objective optimization can significantly enhance the effectiveness of surrounding rock control, resolve conflicts, and achieve more reasonable construction plans. This research provides new theoretical foundations and practical guidance for deep mine roadway-surrounding rock control. Full article
Show Figures

Figure 1

Figure 1
<p>Integrated geological histogram.</p>
Full article ">Figure 2
<p>1305 working face roadway support scheme.</p>
Full article ">Figure 3
<p>Numerical model.</p>
Full article ">Figure 4
<p>Peak point monitoring schematic.</p>
Full article ">Figure 5
<p>Cyclometric stress lines.</p>
Full article ">Figure 6
<p>Data set distribution.</p>
Full article ">Figure 7
<p>Experimental flow.</p>
Full article ">Figure 8
<p>Recessive frontier and dominance relationships.</p>
Full article ">Figure 9
<p>SEGA algorithm flow.</p>
Full article ">Figure 10
<p>Stress-relief effect of central grooving.</p>
Full article ">Figure 11
<p>Peak stress changes in center grooving.</p>
Full article ">Figure 12
<p>Stress-relief effect of floor-side corners grooving.</p>
Full article ">Figure 13
<p>Stress changes in floor-side corner grooving.</p>
Full article ">Figure 14
<p>Center backfill—floor-side grooving displacement comparison.</p>
Full article ">Figure 15
<p>2 m × 2 m Stress-relief groove plastic volume.</p>
Full article ">Figure 16
<p>SEGA optimization of SVR iterative process.</p>
Full article ">Figure 17
<p>Predicted value—real value.</p>
Full article ">Figure 18
<p>Iterative process.</p>
Full article ">Figure 19
<p>Pareto front.</p>
Full article ">Figure 20
<p>Filtering the dominant solution.</p>
Full article ">Figure 21
<p>Theoretical values—simulated values.</p>
Full article ">Figure 22
<p>Field Implementation.</p>
Full article ">Figure 23
<p>Later investigation of roadway site conditions.</p>
Full article ">Figure 24
<p>Layout of measuring points of roadway displacement.</p>
Full article ">Figure 25
<p>Deformation diagram of surrounding rock in roadway field.</p>
Full article ">Figure A1
<p>Distribution of plastic zones in the center groove.</p>
Full article ">Figure A2
<p>Floor-side grooving plastic zone.</p>
Full article ">
19 pages, 9100 KiB  
Article
Deep Ultraviolet Excitation Photoluminescence Characteristics and Correlative Investigation of Al-Rich AlGaN Films on Sapphire
by Zhe Chuan Feng, Ming Tian, Xiong Zhang, Manika Tun Nafisa, Yao Liu, Jeffrey Yiin, Benjamin Klein and Ian Ferguson
Nanomaterials 2024, 14(21), 1769; https://doi.org/10.3390/nano14211769 - 4 Nov 2024
Viewed by 507
Abstract
AlGaN is attractive for fabricating deep ultraviolet (DUV) optoelectronic and electronic devices of light-emitting diodes (LEDs), photodetectors, high-electron-mobility field-effect transistors (HEMTs), etc. We investigated the quality and optical properties of AlxGa1−xN films with high Al fractions (60–87%) grown on [...] Read more.
AlGaN is attractive for fabricating deep ultraviolet (DUV) optoelectronic and electronic devices of light-emitting diodes (LEDs), photodetectors, high-electron-mobility field-effect transistors (HEMTs), etc. We investigated the quality and optical properties of AlxGa1−xN films with high Al fractions (60–87%) grown on sapphire substrates, including AlN nucleation and buffer layers, by metal–organic chemical vapor deposition (MOCVD). They were initially investigated by high-resolution X-ray diffraction (HR-XRD) and Raman scattering (RS). A set of formulas was deduced to precisely determine x(Al) from HR-XRD data. Screw dislocation densities in AlGaN and AlN layers were deduced. DUV (266 nm) excitation RS clearly exhibits AlGaN Raman features far superior to visible RS. The simulation on the AlGaN longitudinal optical (LO) phonon modes determined the carrier concentrations in the AlGaN layers. The spatial correlation model (SCM) analyses on E2(high) modes examined the AlGaN and AlN layer properties. These high-x(Al) AlxGa1−xN films possess large energy gaps Eg in the range of 5.0–5.6 eV and are excited by a DUV 213 nm (5.8 eV) laser for room temperature (RT) photoluminescence (PL) and temperature-dependent photoluminescence (TDPL) studies. The obtained RTPL bands were deconvoluted with two Gaussian bands, indicating cross-bandgap emission, phonon replicas, and variation with x(Al). TDPL spectra at 20–300 K of Al0.87Ga0.13N exhibit the T-dependences of the band-edge luminescence near 5.6 eV and the phonon replicas. According to the Arrhenius fitting diagram of the TDPL spectra, the activation energy (19.6 meV) associated with the luminescence process is acquired. In addition, the combined PL and time-resolved photoluminescence (TRPL) spectroscopic system with DUV 213 nm pulse excitation was applied to measure a typical AlGaN multiple-quantum well (MQW). The RT TRPL decay spectra were obtained at four wavelengths and fitted by two exponentials with fast and slow decay times of ~0.2 ns and 1–2 ns, respectively. Comprehensive studies on these Al-rich AlGaN epi-films and a typical AlGaN MQW are achieved with unique and significant results, which are useful to researchers in the field. Full article
Show Figures

Figure 1

Figure 1
<p>HR-XRD wide scans of four AlGaN samples, with the substrate sapphire (0006) peak at 41.70° for calibration.</p>
Full article ">Figure 2
<p>HR-XRD fine scans of four AlGaN/AlN/sapphire samples. (<b>a</b>) The first order with the sapphire (0006) peak at 41.70° for calibration, (<b>a1</b>) Gaussian fits for AlGaN (0002) peaks with red lines and for AlN (0002) peaks with green lines, and (<b>b</b>) the third-order scans.</p>
Full article ">Figure 3
<p>HR-XRD fine scans and Gaussian fits of the AlGaN (0006) peaks for three AlGaN samples, with high x(Al) compositions of 71.4%, 81.1%, and 87.7%, respectively.</p>
Full article ">Figure 4
<p>Typical SE psi (Ψ) and delta (∆) spectra at 60°–70° incidences from an Al<sub>x</sub>Ga<sub>1−x</sub>N sample A60 with x = 60.2%.</p>
Full article ">Figure 5
<p>DUV 266 nm excitation Raman scattering spectra for 5 AlGaN/AlN/sapphire samples with high x(Al) between 60.2% and 87.7%, respectively.</p>
Full article ">Figure 6
<p>Fitted AlGaN A<sub>1</sub>(LO) modes from DUV 266 nm excitation Raman scattering spectra of five Al<sub>x</sub>Ga<sub>1−x</sub>N/AlN/sapphire samples with high x(Al) between 60.2% and 87.7%, respectively. Fitted values and calculated results of plasmon frequency/damping constant, phonon lifetime, and carrier concentration are listed in <a href="#nanomaterials-14-01769-t003" class="html-table">Table 3</a>.</p>
Full article ">Figure 7
<p>Raman spectral data at 700–900 cm<sup>−1</sup> from the A60 (x = 60.2%) sample under the 266 nm excitation, and Voigt fittings of three modes of sapphire at 753 cm<sup>−1</sup>, AlGaN A1(LO) at 846 cm<sup>−1</sup>, and the surface optical (SO) mode between them (at 822 cm<sup>−1</sup>).</p>
Full article ">Figure 8
<p>Experimental Raman (ex. 266 nm) data and Voigt mode fittings for AlGaN and AlN E<sub>2</sub>(high) modes in five Al<sub>x</sub>Ga<sub>1−x</sub>N/AlN/sapphire samples with x(Al) of 60.2%, 71.4%, 75.3%, 81.1%, and 87.7%, respectively.</p>
Full article ">Figure 9
<p>DUV 266 nm excitation Raman spectral information of AlN E<sub>2</sub>(high) modes, with experimental data (fitted from Voigt contours at <a href="#nanomaterials-14-01769-f008" class="html-fig">Figure 8</a>) in blue symbols and SCM fits by red lines, for our five Al<sub>x</sub>Ga<sub>1−x</sub>N/AlN/sapphire samples. The calculated parameters based upon SCM are listed in <a href="#nanomaterials-14-01769-t002" class="html-table">Table 2</a>.</p>
Full article ">Figure 10
<p>DUV 266 nm excitation Raman spectral information of AlGaN E<sub>2</sub>(high) modes, with experimental data (fitted from Voigt contours at <a href="#nanomaterials-14-01769-f008" class="html-fig">Figure 8</a>) in blue symbols and SCM fits by red lines, for five Al<sub>x</sub>Ga<sub>1−x</sub>N/AlN/sapphire samples. The calculated parameters based upon SCM are listed in <a href="#nanomaterials-14-01769-t005" class="html-table">Table 5</a>.</p>
Full article ">Figure 11
<p>RT photoluminescence (PL) spectra under 213 nm excitation for five Al<sub>x</sub>Ga<sub>1−x</sub>N/AlN/sapphire samples with x(Al) between 60.2 and 87.7%, respectively.</p>
Full article ">Figure 12
<p>Relationships of the PL peak energy and full width at half maximum (FWHM, i.e., w in <a href="#nanomaterials-14-01769-f011" class="html-fig">Figure 11</a>) values vs. x(Al) for Al<sub>x</sub>Ga<sub>1−x</sub>N/AlN/sapphire, in which an E peak point of x = 1.0 is from previously measured AlN/sapphire under 193 nm excitation [<a href="#B29-nanomaterials-14-01769" class="html-bibr">29</a>]. Red open circles are for PL peaks and black stars are for FWHM. Red line and blue dashed line are guides for eye.</p>
Full article ">Figure 13
<p>(<b>a</b>) Variable temperature (20–300 K) PL spectra of the Al<sub>0.87</sub>Ga<sub>0.13</sub>N/AlN/sapphire sample. (<b>b</b>) Normalized integrated PL intensity vs. 1/T, fitted with Arrhenius formulism, obtaining the activation energy of E<sub>act</sub> = 19.6 meV.</p>
Full article ">Figure 14
<p>Gaussian fits on the main PL bands at 20, 50, 100, 200, 250, and 300 K, respectively, for the Al<sub>0.87</sub>Ga<sub>0.13</sub>N/AlN/sapphire sample. Each spectrum is deconvoluted to two bands, with the strong one at 5.60–5.59 eV and a weaker one at 5.49–5.48 eV for 20–250 K and at ~5.44 eV for 300 K, respectively.</p>
Full article ">Figure 15
<p>(<b>a</b>) RT PL of an AlGaN MQW with MQW emission peak at 350 nm, AlGaN-barrier peak at 295 nm, and a broad band over 400–580 nm. (<b>b</b>) RT TRPL decay spectra from the 213 nm pulse laser (red) and the AlGaN MQW sample W10, detected at 440 nm (blue). (<b>c</b>) RT TRPL detected at four wavelengths for AlGaN MQW sample W10.</p>
Full article ">
19 pages, 4437 KiB  
Article
Adaptive Weighted Particle Swarm Optimization for Controlling Multiple Switched Reluctance Motors with Enhanced Deviatoric Coupling Control
by Tianyu Zhang, Xianglian Xu, Fangqing Zhang, Yifeng Gu, Kaitian Deng, Yuli Xu, Tunzhen Xie and Yuanqing Song
Electronics 2024, 13(21), 4320; https://doi.org/10.3390/electronics13214320 - 3 Nov 2024
Viewed by 490
Abstract
Switched reluctance motors (SRMs) are widely used in industrial applications due to their advantages. Multi-motor synchronous control systems are crucial in modern industry, as their control strategies significantly impact synchronization performance. Traditional deviation coupling control structures face limitations during the startup phase, leading [...] Read more.
Switched reluctance motors (SRMs) are widely used in industrial applications due to their advantages. Multi-motor synchronous control systems are crucial in modern industry, as their control strategies significantly impact synchronization performance. Traditional deviation coupling control structures face limitations during the startup phase, leading to excessive tracking errors and exacerbated by uneven load distribution, resulting in desynchronized motor acceleration and increased speed synchronization errors. This study proposes a modified deviation coupling control method based on an adaptive weighted particle swarm optimization (PSO) algorithm to enhance multi-motor synchronization performance. Traditional deviation coupling control applies equal reference torque inputs to each motor’s current loop, failing to address uneven load distribution and causing inconsistent accelerations. To resolve this, a gain equation based on speed deviation is introduced, incorporating self-tracking error and gain coefficients for dynamic synchronization error compensation. The gain coefficients are optimized using the adaptive weighted PSO algorithm to improve system adaptability. A simulation model of a synchronization control system for three SRMs was developed in the Matlab/Simulink R2023b environment. This model compares the synchronization performance of traditional deviation coupling, Fuzzy-PID improved structure, and adaptive PSO improved structure during motor startup, sudden speed increases, and load disturbances. The validated deviation coupling control structure achieved the initial set speed in approximately 0.236 s, demonstrating faster convergence and a 6.35% reduction in settling time. In both the motor startup and sudden speed increase phases, the two optimized methods outperformed the traditional structure in dynamic performance and synchronization accuracy, with the adaptive PSO structure improving synchronization accuracy by 54% and 37.17% over the Fuzzy-PID structure, respectively. Therefore, the PSO-optimized control system demonstrates faster convergence, improved stability, and enhanced synchronization performance. Full article
(This article belongs to the Section Power Electronics)
Show Figures

Figure 1

Figure 1
<p>Curve of winding inductance as a function of the relative position between the stator and rotor.</p>
Full article ">Figure 2
<p>Block diagram of SRM speed control system.</p>
Full article ">Figure 3
<p>Conventional deviation coupling structures.</p>
Full article ">Figure 4
<p>Tracking error controller.</p>
Full article ">Figure 5
<p>Structure of the speed compensator for the first motor.</p>
Full article ">Figure 6
<p>Improved velocity compensator.</p>
Full article ">Figure 7
<p>Flowchart of standard PSO algorithm.</p>
Full article ">Figure 8
<p>Improved deviation coupling simulation model.</p>
Full article ">Figure 9
<p>Single SRM control system simulation model.</p>
Full article ">Figure 10
<p>Speed differential between SRM1 and SRM2.</p>
Full article ">Figure 11
<p>Speed differential between SRM1 and SRM3.</p>
Full article ">Figure 12
<p>Speed differential between SRM2 and SRM3.</p>
Full article ">Figure 13
<p>Global synchronization error.</p>
Full article ">Figure 14
<p>Local enlargement.</p>
Full article ">
11 pages, 1730 KiB  
Case Report
Nitroglycerin (NTG) Infusion for Intraprocedural Vasospasm in Transarterial Microembolization (TAME): A Case Series
by Kuan-Wei Li, Keng-Wei Liang, Wen-Ying Liao, Chien-Kuo Wang, Yi-Sheng Liu, Tai-Hua Yang, Chun-Hsin Wu and Bow Wang
Life 2024, 14(11), 1413; https://doi.org/10.3390/life14111413 - 1 Nov 2024
Viewed by 581
Abstract
Transarterial microembolization (TAME) is an innovative approach to treating chronic musculoskeletal pain. During the procedure, intraprocedural vasospasm, presenting juxta-catheter stenosis, and poor distal artery perfusion and flow through the anastomosis commonly pose challenges. Difficulty of the catheter reaching the target vessel and restricted [...] Read more.
Transarterial microembolization (TAME) is an innovative approach to treating chronic musculoskeletal pain. During the procedure, intraprocedural vasospasm, presenting juxta-catheter stenosis, and poor distal artery perfusion and flow through the anastomosis commonly pose challenges. Difficulty of the catheter reaching the target vessel and restricted drug delivery are possible consequences. To address these issues, transcatheter nitroglycerin (NTG) infusion at the extremity’s small-sized artery has been introduced. We investigated patients who underwent the TAME procedure wherein NTG was employed and sourced from two institutional settings. Transcatheter NTG infusion was administered in seven instances of chronic musculoskeletal pain manifesting with intraprocedural vasospasm during TAME procedures. Patient profiles, preprocedural imaging, fluoroscopic findings, adverse events, and Numerical Rating Scale (NRS) scores were evaluated. As a result, all seven cases experiencing intraprocedural vasospasm exhibited rapid responses to transcatheter NTG infusion. Angiography conducted pre- and post-infusion demonstrated increased vessel size, resolved proximal catheter stenosis, and improved distal perfusion. One case presented an adverse effect of self-limited transient hypotension. The NRS scores decreased following the procedure. Transcatheter NTG infusion at the extremity’s small-sized muscular artery can be an effective technique for resolving intraprocedural vasospasm in TAME procedures, irrespective of the target diseases and approach vessels. Full article
(This article belongs to the Special Issue A Paradigm Shift in Airway and Pain Management—2nd Edition)
Show Figures

Figure 1

Figure 1
<p>A 61-year-old female with left lateral epicondylitis. (<b>A</b>) Angiography at the left brachial artery showing patent left radial recurrent artery without stenosis. (<b>B</b>) Angiography at the left radial recurrent artery showing a vasospasm with a proximal catheter stenosis point, measuring 0.99 mm at the narrowest point (black arrowhead). (<b>C</b>) Angiography after NTG infusion showing resolved stenosis (black arrowhead, measured 2.45 mm).</p>
Full article ">Figure 2
<p>A 26-year-old male with bilateral forefoot plantar side pain at the 2nd-4th toes. (<b>A</b>) Angiography at the left arcuate artery showing a vasospasm with impaired perfusion of left dorsal metatarsal arteries (white arrowheads) and proximal catheter stenosis (black arrowheads, 1.75 mm). (<b>B</b>) Angiography after NTG infusion showing improved perfusion of left dorsal metatarsal arteries (white arrowheads) and improved proximal catheter stenosis (black arrowheads, 2.46 mm).</p>
Full article ">Figure 3
<p>A 55-year-old female presented with pain and swelling at the DIP joints of their left hand for 2 years. (<b>A</b>) Angiography at the left radial artery showing a vasospasm with flow through the superficial palmar arch via anastomosis (white arrow), proximal catheter stenosis (black arrowhead, measured 1.12 mm), and impaired perfusion of the deep palmar arch with absence of blood flow at the DIP joint level (white arrowheads). (<b>B</b>) Magnification of proximal catheter stenosis (black arrowhead). (<b>C</b>) Angiography after NTG infusion showing improved perfusion toward digital arteries at the DIP joint level via the deep palmar arch (white arrowheads). The vascular stenosis was completely resolved (black arrowheads, 2.71 mm). (<b>D</b>) Magnification of resolved stenosis (black arrowhead).</p>
Full article ">Figure 4
<p>A 36-year-old female presented with left knee pain after a traffic accident for 1 year. (<b>A</b>) Angiography at the left lateral inferior genicular artery showing flow through the left medial superior genicular artery via anastomosis (white arrow), impaired perfusion (white arrowhead), and proximal catheter stenosis (black arrowhead, 0.85 mm). (<b>B</b>) Angiography after NTG infusion showing improved perfusion of left lateral inferior genicular artery territories (white arrowheads), and the vascular stenosis was resolved (black arrowhead, 1.03 mm).</p>
Full article ">Figure 5
<p>A 20-year-old male presented with bilateral foot 2nd-4th metatarsalgia for 2 years. (<b>A</b>) Angiography at the right anterior tibial artery showing vasospasm with impaired perfusion to the right dorsal metatarsal arteries (white arrowhead). (<b>B</b>) Angiography after NTG infusion showing improved perfusion to the right dorsal metatarsal arteries (white arrowheads).</p>
Full article ">Figure 6
<p>A 62-year-old female presented with right shoulder pain during elevation and put down for about 2 years post-operation. (<b>A</b>) Angiography at the right thoracoacromial artery showing vasospasm with proximal catheter stenosis (black arrowhead, measured 1.12 mm) and impaired distal perfusion distal to the stenosis point (white arrowhead). (<b>B</b>) Angiography after NTG infusion showing resolved stenosis (black arrowhead, measured 1.96 mm) and improved distal perfusion (white arrowhead).</p>
Full article ">
19 pages, 742 KiB  
Systematic Review
The Effect of Exercise Program Interventions on Frailty, Clinical Outcomes, and Biomarkers in Older Adults: A Systematic Review
by Adchara Prommaban, Sasiwimon Moonkayaow, Phichayut Phinyo, Penprapa Siviroj, Wachiranun Sirikul and Peerasak Lerttrakarnnon
J. Clin. Med. 2024, 13(21), 6570; https://doi.org/10.3390/jcm13216570 - 1 Nov 2024
Viewed by 522
Abstract
Background: Frailty is characterized by the decreased ability in older adults to handle daily or acute stressors due to age-related declines in physiological reserve and organ system performance. This condition results from the interaction of multiple physiological pathways and changes in biomarkers. Exercise [...] Read more.
Background: Frailty is characterized by the decreased ability in older adults to handle daily or acute stressors due to age-related declines in physiological reserve and organ system performance. This condition results from the interaction of multiple physiological pathways and changes in biomarkers. Exercise programs are currently recommended to promote “healthy aging” in frail older adults. Objective: This systematic review aimed to evaluate the effectiveness of exercise program interventions in improving outcomes related to frailty, physical function, cognitive performance, and biomarkers in frail older adults. Methods: This study was designed according to the PRISMA guidelines. A systematic search was conducted in PubMed, Embase, and Scopus for studies published between 2014 and 2024. Two independent reviewers extracted data, with disagreements resolved by a third reviewer. Randomized controlled trials involving pre-frail or frail older adults aged 60 and above in all settings were included. The focus was on the impact of exercise programs, especially multicomponent interventions, on frailty outcomes and biomarkers. Results: Nine studies involving a total of 2083 participants met the inclusion criteria. The age range of participants was 65.35 ± 5.15 to 86.7 ± 4.00 years, with 64.7% being female. The results demonstrated that multicomponent exercise programs significantly improved frailty status, enhanced physical and cognitive function, and improved emotional well-being. Additionally, these programs led to significant reductions in inflammatory biomarkers, such as IL-6 and TNF-α, which are associated with frailty. Conclusion: This review highlights the beneficial effects of multicomponent exercise programs on pre-frail and frail older adults, providing evidence that these interventions improve physical and cognitive functions and emotional well-being, and reduce inflammation. These findings offer valuable insights into developing targeted interventions to manage frailty in clinical practice. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>A flow diagram of the literature search and data selection.</p>
Full article ">
20 pages, 1432 KiB  
Article
An Algorithm for the Solution of Integro-Fractional Differential Equations with a Generalized Symmetric Singular Kernel
by Sameeha A. Raad and Mohammed A. Abdou
Fractal Fract. 2024, 8(11), 644; https://doi.org/10.3390/fractalfract8110644 - 30 Oct 2024
Viewed by 403
Abstract
This work studies an integro-fractional differential equation (I-FrDE) with a generalized symmetric singular kernel. The scientific approach in this study was to transform the integro-differential equation (I-DE) into a mixed integral equation (MIE) with an Able kernel [...] Read more.
This work studies an integro-fractional differential equation (I-FrDE) with a generalized symmetric singular kernel. The scientific approach in this study was to transform the integro-differential equation (I-DE) into a mixed integral equation (MIE) with an Able kernel in fractional time and a generalized symmetric singular kernel in position. Additionally, the authors first set conditions on the singular kernels, whether related to time or position, and then transform the integral equation into an integral operator. Secondly, the solution is unique, which is proven by means of fixed-point theorems. In combination with the solution rules, the convergence of the solution is studied, and the error equation resulting from the solution is a stable error-integral influencer equation. Next, to solve this MIE, the authors apply a special technique to separate the variables and produce an integral equation in position with coefficients, in the form of an integral operator in time. As the most effective technique for resolving singular integral equations, the Toeplitz matrix method (TMM) is utilized to convert the integral equation into an algebraic system for the purpose of solving the position problem. The existence of a solution to the linear algebraic system in Banach space is then demonstrated. Lastly, certain applications where the functions of the generalized symmetric kernel are cubic or exponential and it assumes the logarithmic, Cauchy, or Carleman form are discussed. In each case, Maple 18 is also used to compute the error estimate. Full article
Show Figures

Figure 1

Figure 1
<p>The error according to the time <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math>, the parameter <math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math>, and a logarithmic kernel.</p>
Full article ">Figure 2
<p>The error via the time <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> and the parameters <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>,</mo> <mi>β</mi> </mrow> </semantics></math>, for the Carleman kernel.</p>
Full article ">Figure 3
<p>The error according to the time <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> and the parameter <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>,</mo> </mrow> </semantics></math> with a Cauchy kernel.</p>
Full article ">Figure 4
<p>The error over the time <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> and the parameter <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>,</mo> </mrow> </semantics></math> with a log-exponential kernel.</p>
Full article ">Figure 5
<p>The error according to the time <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> and the parameter <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>,</mo> </mrow> </semantics></math> for a Cauchy-exponential kernel.</p>
Full article ">
13 pages, 8586 KiB  
Article
Study on Mechanical Properties and Safety of Ultra-Thin Reactive Powder Concrete Prefabricated Slabs Applied to I-Beam Joints of Bridges
by Bin Liu, Xiang Liu, Buyu Jia, Quansheng Yan and Zheng Yang
Buildings 2024, 14(11), 3456; https://doi.org/10.3390/buildings14113456 - 30 Oct 2024
Viewed by 329
Abstract
Conventional methods for constructing bridge I-beam joints face several challenges, including heavy precast slabs, complicated transportation and lifting procedures, strict accuracy requirements, lengthy construction timelines, and increased safety risks. The use of ultra-thin, high-performance reactive powder concrete (RPC) prefabricated slabs can effectively resolve [...] Read more.
Conventional methods for constructing bridge I-beam joints face several challenges, including heavy precast slabs, complicated transportation and lifting procedures, strict accuracy requirements, lengthy construction timelines, and increased safety risks. The use of ultra-thin, high-performance reactive powder concrete (RPC) prefabricated slabs can effectively resolve these issues. However, research in this area is limited, leaving our understanding of the strength and feasibility of ultra-thin RPC slabs for I-beam joints incomplete. Therefore, this study conducts a thorough examination of the strength and safety aspects of these slabs to assess their practical suitability. First, 11 numerical models are generated to evaluate the bearing capacity of ultra-thin RPC slabs, determining key factors such as cracking load, ultimate load, and safety factor according to relevant codes and standards. This establishes a theoretical foundation for practical engineering applications. Next, several sets of ultra-thin RPC slabs that meet material performance criteria are prefabricated to study the mechanical properties under equivalent concentrated load. Finally, two types of in situ temporary construction loads are encountered in the safety calculations of the RPC slabs. This study aims to provide a robust theoretical framework and technical support for the application and advancement of ultra-thin RPC prefabricated slabs in bridge I-beam joints. Full article
(This article belongs to the Special Issue Innovation in Pavement Materials: 2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of joint of I-beam (unit: cm).</p>
Full article ">Figure 2
<p>Typical shape form of the RPC slab unit.</p>
Full article ">Figure 3
<p>Constitutive relation of RPC: (<b>a</b>) Compression constitutive; (<b>b</b>) tension constitutive.</p>
Full article ">Figure 4
<p>Numerical model: (<b>a</b>) Slab width 650 mm; (<b>b</b>) slab width 900 mm; (<b>c</b>) slab width 1200 mm.</p>
Full article ">Figure 5
<p><math display="inline"><semantics> <mrow> <mi>F</mi> <mo>−</mo> <mo>∆</mo> </mrow> </semantics></math> curve under concentrated load.</p>
Full article ">Figure 6
<p><math display="inline"><semantics> <mrow> <mi>F</mi> <mo>−</mo> <mo>∆</mo> </mrow> </semantics></math> curve under uniformly distributed load.</p>
Full article ">Figure 7
<p>Numerical failure process of RPC slab.</p>
Full article ">Figure 8
<p>Cracking and ultimate margin coefficients of RPC slabs: (<b>a</b>) Cracking surplus coefficient under concentrated force; (<b>b</b>) limiting coefficient of excess under concentrated force; (<b>c</b>) the cracking surplus coefficient under uniform distribution force; (<b>d</b>) the limiting surplus coefficient under uniform distribution force.</p>
Full article ">Figure 9
<p>Strength tests: (<b>a</b>) Compression test; (<b>b</b>) tensile test; (<b>c</b>) bending test.</p>
Full article ">Figure 10
<p>Loading test and test specimens: (<b>a</b>) Concentrated loading diagram; (<b>b</b>) RPC slab test site; (<b>c</b>) 650 mm slab width + C140 RPC slab; (<b>d</b>) 1200 mm slab width + C160 RPC slab.</p>
Full article ">
23 pages, 1286 KiB  
Article
Synergy as the Failure of Distributivity
by Ivan Sevostianov and Ofer Feinerman
Entropy 2024, 26(11), 916; https://doi.org/10.3390/e26110916 - 28 Oct 2024
Viewed by 358
Abstract
The concept of emergence, or synergy in its simplest form, is widely used but lacks a rigorous definition. Our work connects information and set theory to uncover the mathematical nature of synergy as the failure of distributivity. For the trivial case of discrete [...] Read more.
The concept of emergence, or synergy in its simplest form, is widely used but lacks a rigorous definition. Our work connects information and set theory to uncover the mathematical nature of synergy as the failure of distributivity. For the trivial case of discrete random variables, we explore whether and how it is possible to get more information out of lesser parts. The approach is inspired by the role of set theory as the fundamental description of part–whole relations. If taken unaltered, synergistic behavior is forbidden by the set-theoretic axioms. However, random variables are not a perfect analogy of sets: we formalize the distinction, highlighting a single broken axiom—union/intersection distributivity. Nevertheless, it remains possible to describe information using Venn-type diagrams. The proposed multivariate theory resolves the persistent self-contradiction of partial information decomposition and reinstates it as a primary route toward a rigorous definition of emergence. Our results suggest that non-distributive variants of set theory may be used to describe emergent physical systems. Full article
Show Figures

Figure 1

Figure 1
<p>This diagram illustrates how information in two variables <math display="inline"><semantics> <mrow> <mi>X</mi> <mo>,</mo> <mi>Y</mi> </mrow> </semantics></math> about a third variable <span class="html-italic">Z</span> can be decomposed into different information atoms. The amount of such information in <math display="inline"><semantics> <mrow> <mi>X</mi> <mo>,</mo> <mi>Y</mi> </mrow> </semantics></math> and joint variable <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>X</mi> <mo>,</mo> <mi>Y</mi> <mo>)</mo> </mrow> </semantics></math> is measured using the mutual information <math display="inline"><semantics> <mrow> <mi>I</mi> <mo>(</mo> <mi>X</mi> <mo>;</mo> <mi>Z</mi> <mo>)</mo> <mo>,</mo> <mi>I</mi> <mo>(</mo> <mi>Y</mi> <mo>;</mo> <mi>Z</mi> <mo>)</mo> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>I</mi> <mo>(</mo> <mo>(</mo> <mi>X</mi> <mo>,</mo> <mi>Y</mi> <mo>)</mo> <mo>;</mo> <mi>Z</mi> <mo>)</mo> </mrow> </semantics></math> correspondingly. Redundant information <span class="html-italic">R</span> is information that is shared between <span class="html-italic">X</span> and <span class="html-italic">Y</span> such that knowing one of them suffices in deducing this information about <span class="html-italic">Z</span>. Unique information <math display="inline"><semantics> <msub> <mi>U</mi> <mi>X</mi> </msub> </semantics></math> is found only in <span class="html-italic">X</span>, <math display="inline"><semantics> <msub> <mi>U</mi> <mi>Y</mi> </msub> </semantics></math>—only in <span class="html-italic">Y</span>. The synergistic information <span class="html-italic">S</span> that <span class="html-italic">X</span> and <span class="html-italic">Y</span> hold about <span class="html-italic">Z</span> is only contained in the joint variable, but not individual sources on their own.</p>
Full article ">Figure 2
<p>A Venn-type diagram for the XOR gate. Each variable is represented by a primary color circle (red, yellow, blue) while the outer circle outlines the whole system. Of the total 2 bits of the XOR gate, one is covered two times and is represented by the inner disk. Since it is covered twice, this area is colored by pairwise color-blends (orange, purple, and green). Since it is covered by three variables, it includes patches of all three possible blends. A critical difference between this diagram and a set-theoretic one is that even though the three variables have no pairwise intersections, the inner disk representing the mutual content of all three variables is non-empty. The remaining 1 bit is covered once and resides only inside the joint variable. Since this area is covered once, it is colored by primary colors. Patches of all three colors are used since this area does not belong to any single variable.</p>
Full article ">Figure 3
<p>A single realization of the inclusion–exclusion principle for three variables. The new region, corresponding to the distributivity-breaking difference is represented via a checkered pattern. Covering numbers are written for each sector and highlighted by the colors. This is not a full Venn-type diagram that defines the information atoms, and hence, its structure is clearly not invariant with respect to variable permutations.</p>
Full article ">Figure 4
<p>A graphical illustration for the general solution of the trivariate problem. Compared to the Venn diagram for three sets, two new regions here are the 2-covered part of triple intersection <math display="inline"><semantics> <msub> <mo>Π</mo> <mi>s</mi> </msub> </semantics></math> (synergistic atom) and a ghost atom <math display="inline"><semantics> <msub> <mo>Π</mo> <mi>g</mi> </msub> </semantics></math>, which is not a part of any single initial variable. Similarly to <a href="#entropy-26-00916-f003" class="html-fig">Figure 3</a>, colors indicate the coverings: three primary colors (red, yellow, blue, or their checkered combination) correspond to 1-covered atoms, the overlay of any two colors (orange, purple, green or their checkered combination) is 2-covered, and the overlay of all three colors (brown) is 3-covered.</p>
Full article ">
20 pages, 5007 KiB  
Article
Multi-Material Topology Optimization on Separate Tetrahedral Meshes with Explicit Design Resolution by Means of Remeshing
by Robert Renz and Albert Albers
Algorithms 2024, 17(10), 460; https://doi.org/10.3390/a17100460 - 16 Oct 2024
Viewed by 501
Abstract
As a method of lightweight design, multi-material design aims to make targeted use of materials in order to reduce CO2 emissions. In this context, it can be described as one of the product development methods used to meet the challenges of climate [...] Read more.
As a method of lightweight design, multi-material design aims to make targeted use of materials in order to reduce CO2 emissions. In this context, it can be described as one of the product development methods used to meet the challenges of climate change. However, since the design of structures in multi-material design is complex, topology optimization can be used to support the product developer. In this article, a multi-material topology optimization method is developed that combines the Velocity Field Level Set method with the Reconciled Level Set method. Furthermore, the current design is explicitly resolved in each iteration by means of multi-material remeshing. The edge collapse phase in the remeshing process is achieved by applying the producer consumer pattern. The developed method is then validated using known examples from the state of research, and the influence of the parameters of the method on the result is analyzed by means of studies. Full article
(This article belongs to the Section Analysis of Algorithms and Complexity Theory)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) A 2D level set function (blue), which represents a rectangle with two holes. The intersection between the level set function and the plane (green) results in the surface of the rectangle (orange). (<b>b</b>) Representation of the level set function and the corresponding part colored in blue.</p>
Full article ">Figure 2
<p>Reconciled level set method: The level set functions <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>1</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> (gray) and <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> (blue) each represent the boundaries of a material (<math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mi>i</mi> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>) in the design domain D. <math display="inline"><semantics> <mi mathvariant="sans-serif">Γ</mi> </semantics></math> (orange) is the interface between the two materials.</p>
Full article ">Figure 3
<p>Visualization of the MBO operator using two level set functions <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>1</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> (gray) and <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> (blue) moving towards each other based on [<a href="#B22-algorithms-17-00460" class="html-bibr">22</a>]. (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>1</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> are moving towards each other; there is no overlap. (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>1</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> overlap in the orange area. (<b>c</b>) Correction of <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>1</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>φ</mi> <mn>2</mn> </msub> <mrow> <mo>(</mo> <mi mathvariant="bold-italic">x</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> by applying the MBO operator; there is no longer any overlap.</p>
Full article ">Figure 4
<p>Structure of the optimization loop with the individual components.</p>
Full article ">Figure 5
<p>Schematic representation of the velocity extension from the zero level set (blue) to the target vertex based on [<a href="#B33-algorithms-17-00460" class="html-bibr">33</a>]. For this purpose, the pole of the target vertex is determined on the zero level set, and then, the normal velocity of the target vertex (orange) is calculated from the normal velocities of the triangle (green) using linear interpolation.</p>
Full article ">Figure 6
<p>Level set mesh (gray) and the dual mesh with corresponding cells (blue) based on [<a href="#B35-algorithms-17-00460" class="html-bibr">35</a>]. The dual mesh is used to develop an accurate upwind approximation of the Hamiltonian. A cellcorner c is shaded black.</p>
Full article ">Figure 7
<p>Five unique marching tetrahedra cases based on [<a href="#B36-algorithms-17-00460" class="html-bibr">36</a>]. The resulting discretized interface consisting of triangles is shown in orange.</p>
Full article ">Figure 8
<p>(<b>a</b>) Mesh with classification of vertices into volume and boundary vertices based on [<a href="#B38-algorithms-17-00460" class="html-bibr">38</a>]. (<b>b</b>) Invalid edge collapse since the collapse does not preserve the interface position (non-feature preserving). (<b>c</b>) Valid edge collapse since the collapse preserves the interface (feature preserving).</p>
Full article ">Figure 9
<p>Examples of cavity operations. (<b>a</b>) Edge collapse: the cavity is initialized with all adjacent elements (triangles or tetrahedra) of vertex A, and vertex B serves as the target vertex for the meshing. (<b>b</b>) Edge swap: the cavity is initialized with all elements adjacent to edge BC, and node A serves as the target node for meshing.</p>
Full article ">Figure 10
<p>Pre-processing step for remeshing the blue design area. Determination of the convex hull (orange), offset calculation of the convex hull (gray) with subsequent meshing.</p>
Full article ">Figure 11
<p>Design space of a box with chamfered edges, which is supported at four locations in the z-plane and has a load application location on the surface with a force in the negative <span class="html-italic">z</span>-direction in the amount of <span class="html-italic">F</span>.</p>
Full article ">Figure 12
<p>Symmetrical design space of the cantilever beam with a fixed support (<math display="inline"><semantics> <mrow> <msub> <mi>u</mi> <mi>x</mi> </msub> <mo>=</mo> <msub> <mi>u</mi> <mi>y</mi> </msub> <mo>=</mo> <msub> <mi>u</mi> <mi>z</mi> </msub> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>), a floating support (<math display="inline"><semantics> <mrow> <msub> <mi>u</mi> <mi>x</mi> </msub> <mo>=</mo> <msub> <mi>u</mi> <mi>y</mi> </msub> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>) and a load application point on the front side with a force in the negative <span class="html-italic">z</span>-direction in the amount of <span class="html-italic">F</span>.</p>
Full article ">Figure 13
<p>(<b>a</b>) Initial hole structure of the box in the single-material case. (<b>b</b>) Optimization result for the box at iteration 107.</p>
Full article ">Figure 14
<p>(<b>a</b>) Objective function for the single-material case of the box. (<b>b</b>) Volume constraint for the single-material case of the box.</p>
Full article ">Figure 15
<p>(<b>a</b>) Initial hole structure of the cantilever in the single-material case. (<b>b</b>) Optimization result for the cantilever at iteration 60.</p>
Full article ">Figure 16
<p>(<b>a</b>) History of the objective function for the single-material case of the cantilever. (<b>b</b>) History of the volume constraint for the single-material case of the cantilever.</p>
Full article ">Figure 17
<p>(<b>a</b>) Initial hole structure of the box in the multi-material case. Material 1 fills the entire design space except for the holes that are filled with material 2 (blue). (<b>b</b>) Optimization result for the box at iteration 293.</p>
Full article ">Figure 18
<p>(<b>a</b>) History of the objective function for the multi-material case of the box. (<b>b</b>) History of the volume constraints for the multi-material case of the box (blue material 1, brown material 2).</p>
Full article ">Figure 19
<p>(<b>a</b>) Initial hole structure of the cantilever in the multi-material case. Material 1 fills the entire design space except for the holes that are filled with material 2 (blue). (<b>b</b>) Optimization result of the cantilever at iteration 267.</p>
Full article ">Figure 20
<p>(<b>a</b>) History of the objective function for the multi-material case of the cantilever. (<b>b</b>) History of the volume constraints for the multi-material case of the cantilever (blue material 1, brown material 2).</p>
Full article ">Figure 21
<p>Optimization results of the cantilever for the multi-material case for different average edge lengths of the FE mesh with constant edge length of the LS mesh (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>e</mi> <mi>l</mi> <mi>e</mi> <mi>n</mi> <mi>g</mi> <mi>t</mi> <msub> <mi>h</mi> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> <mo>=</mo> <mn>1.5</mn> </mrow> </semantics></math> (iteration 230). (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>e</mi> <mi>l</mi> <mi>e</mi> <mi>n</mi> <mi>g</mi> <mi>t</mi> <msub> <mi>h</mi> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> <mo>=</mo> <mn>2.0</mn> </mrow> </semantics></math> (iteration 267). (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>e</mi> <mi>l</mi> <mi>e</mi> <mi>n</mi> <mi>g</mi> <mi>t</mi> <msub> <mi>h</mi> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math> (iteration 163).</p>
Full article ">Figure 22
<p>Optimization results of the cantilever for the multi-material case for different values of the Helmholtz filter parameter (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mi>r</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>0.75</mn> <mo>∗</mo> <mi>e</mi> <mi>l</mi> <mi>e</mi> <mi>n</mi> <mi>g</mi> <mi>t</mi> <msub> <mi>h</mi> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> </mrow> </semantics></math> (iteration 227). (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mi>r</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>1.25</mn> <mo>∗</mo> <mi>e</mi> <mi>l</mi> <mi>e</mi> <mi>n</mi> <mi>g</mi> <mi>t</mi> <msub> <mi>h</mi> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> </mrow> </semantics></math> (iteration 267). (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>r</mi> <mi>f</mi> </msub> <mo>=</mo> <mn>1.75</mn> <mo>∗</mo> <mi>e</mi> <mi>l</mi> <mi>e</mi> <mi>n</mi> <mi>g</mi> <mi>t</mi> <msub> <mi>h</mi> <mrow> <mi>a</mi> <mi>v</mi> <mi>g</mi> </mrow> </msub> </mrow> </semantics></math> (iteration 205).</p>
Full article ">
8 pages, 3598 KiB  
Article
Camouflage Breaking with Stereo-Vision-Assisted Imaging
by Han Yao, Libang Chen, Jinyan Lin, Yikun Liu and Jianying Zhou
Photonics 2024, 11(10), 970; https://doi.org/10.3390/photonics11100970 - 16 Oct 2024
Viewed by 524
Abstract
Camouflage is a natural or artificial process that prevents an object from being detected, while camouflage breaking is a countering process for the identification of the concealed object. We report that a perfectly camouflaged object can be retrieved from the background and detected [...] Read more.
Camouflage is a natural or artificial process that prevents an object from being detected, while camouflage breaking is a countering process for the identification of the concealed object. We report that a perfectly camouflaged object can be retrieved from the background and detected with stereo-vision-assisted three-dimensional (3D) imaging. The analysis is based on a binocular neuron energy model applied to general 3D settings. We show that a perfectly concealed object with background interference can be retrieved with vision stereoacuity to resolve the hidden structures. The theoretical analysis is further tested and demonstrated with distant natural images taken by a drone camera, processed with a computer and displayed using autostereoscopy. The recovered imaging is presented with the removal of background interference to demonstrate the general applicability for camouflage breaking with stereo imaging and sensing. Full article
(This article belongs to the Special Issue Optical Imaging Innovations and Applications)
Show Figures

Figure 1

Figure 1
<p>The vision neuron energy model explains how the human brain perceives depth.</p>
Full article ">Figure 2
<p>The architecture of stereoacuity measurement with respect to the observer’s interocular separation.</p>
Full article ">Figure 3
<p>Camouflage breaking with a car concealed under trees: (<b>a</b>) the planar image by the left eye; (<b>b</b>) the planar image by the right eye; (<b>c</b>) the recovered car based on the disparity estimation.</p>
Full article ">Figure 4
<p>Left- (<b>a</b>) and right (<b>b</b>)-eye images and stereo anaglyph (<b>c</b>) synthesized by drone images taken at an altitude of 90 m above the ground. The baseline distance between the left and right views is approximately 7 m. The tree leaves obscured in 2D are made prominent with 3D.</p>
Full article ">Figure 5
<p>The energy response for the scene with two eyes focusing on the ground (<b>a</b>) and focusing on the tree (<b>b</b>). (<b>c</b>,<b>d</b>) are structures recovered, respectively, corresponding to (<b>a</b>,<b>b</b>) based on the disparity estimation.</p>
Full article ">Figure 6
<p>(<b>a</b>) The perceived 2D image pattern and (<b>b</b>,<b>c</b>) the sectioning image patterns focused on the ground and on the top of the trees.</p>
Full article ">
22 pages, 2753 KiB  
Article
Two-Stage Satellite Combined-Task Scheduling Based on Task Merging Mechanism
by Jing Yu, Jiawei Guo, Lining Xing, Yanjie Song and Zhaohui Liu
Mathematics 2024, 12(19), 3107; https://doi.org/10.3390/math12193107 - 4 Oct 2024
Viewed by 676
Abstract
Satellites adopt a single-task observation mode in traditional patterns. Although this mode boasts high imaging accuracy, it is accompanied by a limited number of observed tasks and a low utilization rate of satellite resources. This limitation becomes particularly pronounced when dealing with extensive [...] Read more.
Satellites adopt a single-task observation mode in traditional patterns. Although this mode boasts high imaging accuracy, it is accompanied by a limited number of observed tasks and a low utilization rate of satellite resources. This limitation becomes particularly pronounced when dealing with extensive and densely populated observation task sets because the inherent mobility of satellites often leads to conflicts among numerous tasks. To address this issue, this paper introduces a novel multi-task merging mechanism aimed at enhancing the observation rate of satellites by resolving task conflicts. Initially, this paper presents a task merging method based on the proposed multitask merging mechanism, referred to as the constrained graph (CG) task merging approach. This method can merge tasks while adhering to the minimal requirements specified by users. Subsequently, a multi-satellite merging scheduling model is established based on the combined task set. Considering the satellite combined-task scheduling problem (SCTSP), an enhanced fireworks algorithm (EFWA) is proposed that incorporates the CG task synthesis mechanism. This algorithm incorporates local search strategies and a population disturbance mechanism to enhance both the solution quality and convergence speed. Finally, the efficacy of the CG algorithm was validated through a multitude of simulation experiments. Moreover, the effectiveness of the EFWA is confirmed via extensive comparisons with other algorithms, including the basic ant colony optimization (ACO) algorithm, enhanced ant colony optimization (EACO) algorithm, fireworks algorithm (FWA), and EFWA. When the number of tasks in the observation area are dense, such as in the case where the number of tasks is 700, the CG + EFWA (CG is adopted in the task merging stage and EFWA is adopted in the satellite combined-task scheduling stage) method improves observation benefits by 70.35% (compared to CG + EACO, CG is adopted in the task merging stage and EACO is adopted in the satellite combined-task scheduling stage), 78.93% (compared to MS + EFWA, MS is adopted in the task merging stage and EFWA is adopted in the satellite combined-task scheduling stage), and 39.03% (compared to MS + EACO, MS is adopted in the task merging stage and EACO is adopted in the satellite combined-task scheduling stage). Full article
(This article belongs to the Special Issue The Application of Optimization Algorithm in Mathematical Model)
Show Figures

Figure 1

Figure 1
<p>The illustration of satellite sensor transition time.</p>
Full article ">Figure 2
<p>Satellite observation with task merging.</p>
Full article ">Figure 3
<p>The diagram of transforming single-task sequences into a CG model.</p>
Full article ">Figure 4
<p>The framework of the two-stage satellite combined-task scheduling algorithm.</p>
Full article ">Figure 5
<p>Observation benefit value of satellites under different task merging modes: (<b>a</b>) observation benefit value obtained by ACO; (<b>b</b>) observation benefit value obtained by FWA.</p>
Full article ">Figure 6
<p>Observation benefit value of satellites under different algorithms: (<b>a</b>) the observation area contains 100 single tasks; (<b>b</b>) the observation area contains 200 single tasks; (<b>c</b>) the observation area contains 300 single tasks; (<b>d</b>) the observation area contains 400 single tasks; (<b>e</b>) the observation area contains 500 single tasks; (<b>f</b>) the observation area contains 700 single tasks.</p>
Full article ">Figure 6 Cont.
<p>Observation benefit value of satellites under different algorithms: (<b>a</b>) the observation area contains 100 single tasks; (<b>b</b>) the observation area contains 200 single tasks; (<b>c</b>) the observation area contains 300 single tasks; (<b>d</b>) the observation area contains 400 single tasks; (<b>e</b>) the observation area contains 500 single tasks; (<b>f</b>) the observation area contains 700 single tasks.</p>
Full article ">
18 pages, 2442 KiB  
Article
Cytotoxic Potencies of Zinc Oxide Nanoforms in A549 and J774 Cells
by Nazila Nazemof, Dalibor Breznan, Yasmine Dirieh, Erica Blais, Linda J. Johnston, Azam F. Tayabali, James Gomes and Premkumari Kumarathasan
Nanomaterials 2024, 14(19), 1601; https://doi.org/10.3390/nano14191601 - 3 Oct 2024
Viewed by 1029
Abstract
Zinc oxide nanoparticles (NPs) are used in a wide range of consumer products and in biomedical applications, resulting in an increased production of these materials with potential for exposure, thus causing human health concerns. Although there are many reports on the size-related toxicity [...] Read more.
Zinc oxide nanoparticles (NPs) are used in a wide range of consumer products and in biomedical applications, resulting in an increased production of these materials with potential for exposure, thus causing human health concerns. Although there are many reports on the size-related toxicity of ZnO NPs, the toxicity of different nanoforms of this chemical, toxicity mechanisms, and potency determinants need clarification to support health risk characterization. A set of well-characterized ZnO nanoforms (e.g., uncoated ca. 30, 45, and 53 nm; coated with silicon oil, stearic acid, and (3-aminopropyl) triethoxysilane) were screened for in vitro cytotoxicity in two cell types, human lung epithelial cells (A549), and mouse monocyte/macrophage (J774) cells. ZnO (bulk) and ZnCl2 served as reference particles. Cytotoxicity was examined 24 h post-exposure by measuring CTB (viability), ATP (energy metabolism), and %LDH released (membrane integrity). Cellular oxidative stress (GSH-GSSG) and secreted proteins (targeted multiplex assay) were analyzed. Zinc oxide nanoform type-, dose-, and cell type-specific cytotoxic responses were seen, along with cellular oxidative stress. Cell-secreted protein profiles suggested ZnO NP exposure-related perturbations in signaling pathways relevant to inflammation/cell injury and corresponding biological processes, namely reactive oxygen species generation and apoptosis/necrosis, for some nanoforms, consistent with cellular oxidative stress and ATP status. The size, surface area, agglomeration state and metal contents of these ZnO nanoforms appeared to be physicochemical determinants of particle potencies. These findings warrant further research on high-content “OMICs” to validate and resolve toxicity pathways related to exposure to nanoforms to advance health risk-assessment efforts and to inform on safer materials. Full article
Show Figures

Figure 1

Figure 1
<p>Cell morphology observed after exposure of A549 and J774 to the different doses of ZnO nanoparticles (e.g., (<b>A</b>) UC-2 and (<b>B</b>) AM): light microscopy images (40× magnification).</p>
Full article ">Figure 2
<p>Cytotoxicity in A549 cells (mean ± SEM) after exposure (24 h) to ZnO nanoforms and the reference particles. Exposure experiments were conducted three times (n = 3), with duplicate samples per treatment group in each exposure experiment. (<b>A</b>) LDH Release, (<b>B</b>) CTB (Resazurin) Reduction, (<b>C</b>) Cellular ATP Levels.</p>
Full article ">Figure 3
<p>Cytotoxicity in J774 cells (mean ± SEM) after exposure (24 h) to ZnO nanoforms and reference particles. Exposure experiments were conducted three times (n = 3), with duplicate samples per treatment group in each exposure experiment. (<b>A</b>) LDH Release, (<b>B</b>) CTB (Resazurin) Reduction, (<b>C</b>) Cellular ATP Levels.</p>
Full article ">Figure 4
<p>Cellular oxidative stress status in (<b>A</b>) A549 and (<b>B</b>) J774 cells after exposure to ZnO NPs, as well as to the reference particles (30 µg/cm<sup>2</sup>).</p>
Full article ">Figure 5
<p>Heatmap and hierarchical clustering of secreted protein fold changes normalized to control (24 h post exposure of cells to ZnO nanoforms and reference particles: (<b>A</b>) A549 and (<b>B</b>) J774). Red—increased; green—decreased.</p>
Full article ">Figure 6
<p>Pathway analysis results for in vitro cellular exposure (24 h) to ZnO nanoforms and the reference particles ((<b>A</b>) A549 and (<b>B</b>) J774). Orange—increased; blue—decreased.</p>
Full article ">
23 pages, 533 KiB  
Review
Application of the Hub-and-Spoke Model in Antimicrobial Stewardship Programmes: A Scoping Review
by Ayesha Iqbal, Yuhashinee Kumaradev, Gizem Gülpinar, Claire Brandish, Maxencia Nabiryo, Frances Garraghan, Helena Rosado and Victoria Rutter
BioMed 2024, 4(4), 372-394; https://doi.org/10.3390/biomed4040030 - 1 Oct 2024
Viewed by 947
Abstract
Background: The hub-and-spoke model (HSM) offers a framework for efficient healthcare service delivery. This scoping review seeks to explore the implementation and effectiveness of the HSM in antimicrobial stewardship (AMS) programmes. Methods: The Preferred Reporting Items for Systematic Reviews and Meta-Analyses Extension for [...] Read more.
Background: The hub-and-spoke model (HSM) offers a framework for efficient healthcare service delivery. This scoping review seeks to explore the implementation and effectiveness of the HSM in antimicrobial stewardship (AMS) programmes. Methods: The Preferred Reporting Items for Systematic Reviews and Meta-Analyses Extension for Scoping Reviews (PRISMA-ScR) reporting guideline was followed. A systematic search was conducted in four electronic databases (PubMed, Medline, Cochrane Library, and Google Scholar) from inception until January 2024. Studies where the HSM was used for delivering any AMS activity, intervention, or action, were included. No study-specific filters were applied and all populations, study designs, and health settings were included. Data screening and selection were achieved using Rayyan. Three authors independently screened studies, with conflicts resolved by a fourth author. Data were narratively synthesised. Standard appraisal tools were impractical; however, critical evaluation of data collection and outcome reporting was ensured. Results: Out of 1438 articles, three were included in the scoping review. The primary interventions utilising the HSM in AMS involved reducing antibiotic misuse, training healthcare professionals, case-based learning, establishing AMS programmes, developing antibiograms, and formulating policies or guidelines pertinent to AMS. The studies demonstrated significant clinical improvements in AMS. Clinical outcomes from the studies include a significant reduction in antimicrobial usage and improved antibiotic management, with a notable decrease in days on antimicrobial therapy and increased antibiotic de-escalation. Key facilitators for AMS programme success were tailored education, collaborative learning, strong leadership, strategic practices, and data-driven decisions. Key barriers were leadership challenges, change resistance, knowledge gaps, inadequate data systems, resource limitations, and technological constraints. Conclusions: The review identified a literature gap in HSM use in AMS programmes. Further studies are needed to assess HSM’s effectiveness, feasibility, and cost-effectiveness in AMS contexts. Full article
Show Figures

Figure 1

Figure 1
<p>PRISMA diagram on the identification and selection of articles.</p>
Full article ">
7 pages, 1266 KiB  
Communication
Unusual Unsatisfactory Treatment in Two Patients with Imported Cutaneous Leishmaniasis
by Anna Kuna, Romuald Olszański, Beata Szostakowska, Natalia Kulawiak, Ravi Kant and Maciej Grzybek
Trop. Med. Infect. Dis. 2024, 9(10), 227; https://doi.org/10.3390/tropicalmed9100227 - 30 Sep 2024
Viewed by 757
Abstract
Cutaneous leishmaniasis is one of the most commonly diagnosed dermatological condition in travel medicine after diarrhoeal diseases and febrile status. The disease is transmitted by Phlebotomus and Lutzomyia sandflies. It appears in various clinical forms, the most common of which is a painless [...] Read more.
Cutaneous leishmaniasis is one of the most commonly diagnosed dermatological condition in travel medicine after diarrhoeal diseases and febrile status. The disease is transmitted by Phlebotomus and Lutzomyia sandflies. It appears in various clinical forms, the most common of which is a painless ulcer with raised edges, usually present on exposed parts of the body on the side where the insect bite occurred. Annually, over a million new cutaneous leishmaniasis (CL) cases are reported globally. We present two cases of affliction, the first occurring in Patient 1, who attempted treatment through the Kambo cleanse in South America, which is considered a toxic, even life-threatening, procedure. It involves the subcutaneous application of a substance dangerous to humans derived from the surface mucus of a frog. Patient 2 applied caustic ointments, a fruitarian diet, and hyperbaric oxygen therapy in a private setting. After initial therapeutic failures caused by the patients’ unconventional treatment ideas, the causal treatment effect was satisfactory, demonstrating the efficacy of these treatments in resolving the infection when applied appropriately. Despite the typical CL presentation in both patients, their self-treatment course was unusual. It is worth noting that alternative, sometimes harmful, self-treatment initiatives by patients may be surprising and ineffective. Promoting knowledge about tropical diseases among travellers and medical staff is crucial to improving treatment outcomes. Full article
(This article belongs to the Section Neglected and Emerging Tropical Diseases)
Show Figures

Figure 1

Figure 1
<p>(<b>A</b>) Dermatologic issues after Kambo cleansing. (<b>B</b>) Typical presentation of CL in Patient 1.</p>
Full article ">Figure 2
<p>Leishmania amastigotes in a Giemsa-stained tissue scraping. The red arrow indicates amastigotes within a macrophage.</p>
Full article ">Figure 3
<p>(<b>A</b>) Skin changes in Patient 2 before admission to the hospital. (<b>B</b>) The effect of antimonial therapy. (<b>C</b>) The caustic herbal cream used by Patient 2.</p>
Full article ">
Back to TopTop