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

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (736)

Search Parameters:
Keywords = frequency selective surface

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
16 pages, 5245 KiB  
Article
Ball-on-Disk Wear Maps for Bearing Steel–Hard Anodized EN AW-6082 Aluminum Alloy Tribocouple in Dry Sliding Conditions
by Enrico Baroni, Annalisa Fortini, Lorenzo Meo, Chiara Soffritti, Mattia Merlin and Gian Luca Garagnani
Coatings 2024, 14(11), 1469; https://doi.org/10.3390/coatings14111469 - 19 Nov 2024
Viewed by 379
Abstract
In recent years, Golden Hard Anodizing (G.H.A.®) has been developed as a variant of the traditional hard anodizing process with the addition of Ag+ ions in the nanoporous structure. The tribological properties of this innovative surface treatment are still not [...] Read more.
In recent years, Golden Hard Anodizing (G.H.A.®) has been developed as a variant of the traditional hard anodizing process with the addition of Ag+ ions in the nanoporous structure. The tribological properties of this innovative surface treatment are still not well understood. In this study, ball-on-disk tests were conducted in dry sliding conditions using 100Cr6 (AISI 52100) bearing steel balls as a counterbody and GHA®-anodized EN AW-6082 aluminum alloy disks. The novelty of this work lies in the mapping of the wear properties of the tribocouple under different test conditions for a better comparison of the results. Three different normal loads (equal to 5, 10, and 15 N) and three different reciprocating frequencies (equal to 2, 3, and 4 Hz) were selected to investigate a spectrum of operating conditions for polished and unpolished G.H.A.®-anodized EN AW-6082 aluminum alloy. Quantitative wear maps were built based on the resulting wear rate values to define the critical operating limits of the considered tribocouple. The results suggest that the coefficient of friction (COF) was independent of test conditions, while different wear maps were found for polished and non-polished surfaces. Polishing before anodizing permitted the acquisition of lower wear for the anodized disks and the steel balls. Full article
Show Figures

Figure 1

Figure 1
<p>Optical micrographs in cross-section of the anodized layers before wear tests for (<b>a</b>) UP. (<b>b</b>) P.</p>
Full article ">Figure 2
<p>COF evolution during distance for UP (unpolished substrate) and P (previously polished substrate) anodic layers at the different investigated loads: (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N.</p>
Full article ">Figure 3
<p>Representative VPSEM micrographs of wear tracks of the G.H.A.<sup>®</sup>-anodized disk (<b>a</b>) after 50 m, (<b>b</b>) after 100 m, (<b>c</b>) after 150 m, and (<b>d</b>) after 200 m. The orange arrow indicates the direction of reciprocating sliding.</p>
Full article ">Figure 4
<p>VPSEM micrograph at high magnification of the wear tracks of the disk together with semi-quantitative EDS spectra (<b>a</b>). The solid red arrow indicates the area of revelation for the semi-quantitative EDS analysis (<b>b</b>). The red-edged arrow indicates the new deposition of material, while the yellow-edged arrow indicates the removal of a part of the anodic layer with its corresponding EDS spectra (<b>c</b>).</p>
Full article ">Figure 5
<p>Contact pressure evolution during sliding distance for the different applied loads: (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N. <span class="html-italic">Y</span>-axis is reported in logarithmic scale.</p>
Full article ">Figure 6
<p>Worn volume of material from both the counterbodies at the different investigated loads in the case of sliding against UP samples together with a shape factor for the wear scar diameters on the 100Cr6 steel balls at (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N.</p>
Full article ">Figure 7
<p>Quantitative wear maps for 100Cr6 ball and UP anodized disks.</p>
Full article ">Figure 8
<p>Worn volume of material from both the counterbodies at the different investigated loads in the case of sliding against P samples together with a shape factor for the wear scar diameters on the 100Cr6 steel balls at (<b>a</b>) 5 N, (<b>b</b>) 10 N, and (<b>c</b>) 15 N.</p>
Full article ">Figure 9
<p>Quantitative wear maps for 100Cr6 ball and P anodized disks.</p>
Full article ">
14 pages, 2522 KiB  
Article
Quantitative Investigation of Layer-by-Layer Deposition and Dissolution Kinetics by New Label-Free Analytics Based on Low-Q-Whispering Gallery Modes
by Mateusz Olszyna, Algi Domac, Jasmine Zimmer and Lars Dähne
Photonics 2024, 11(11), 1087; https://doi.org/10.3390/photonics11111087 - 19 Nov 2024
Viewed by 387
Abstract
A new instrument for label-free measurements based on optical Low-Q Whispering Gallery Modes (WGMs) for various applications is used for a detailed study of the deposition and release of Layer-by-Layer polymer coatings. The two selected coating pairs interact either via hydrogen bonding or [...] Read more.
A new instrument for label-free measurements based on optical Low-Q Whispering Gallery Modes (WGMs) for various applications is used for a detailed study of the deposition and release of Layer-by-Layer polymer coatings. The two selected coating pairs interact either via hydrogen bonding or electrostatic interactions. Their assembly was followed by common Quartz Crystal Microbalance (QCM) technology and the Low-Q WGMs. In contrast to planar QCM sensor chips of 1 cm, the WGM sensors are fluorescent spherical beads with diameters of 10.2 µm, enabling the detection of analyte quantities in the femtogram range in tiny volumes. The beads, with a very smooth surface and high refractive index, act as resonators for circular light waves that can revolve up to 10,000 times within the bead. The WGM frequencies are highly sensitive to changes in particle diameter and the refractive index of the surrounding medium. Hence, the adsorption of molecules shifts the resonance frequency, which is detected by a robust instrument with a high-resolution spectrometer. The results demonstrate the high potential of the new photonic measurement and its advantages over QCM technology, such as cheap sensors (billions in one Eppendorf tube), simple pre-functionalization, much higher statistic safety by hundreds of sensors for one measurement, 5–10 times faster analysis, and that approx. 25, 000 fewer analyte molecules are needed for one sensor. In addition, the deposited molecule amount is not superposed by hydrated water as for QCM. A connection between sensors and instruments does not exist, enabling application in any transparent environment, like microfluidics, drop-on slides, Petri dishes, well plates, cell culture vasculature, etc. Full article
(This article belongs to the Special Issue Fundamentals, Advances, and Applications in Optical Sensing)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Process of LbL coating of planar surfaces by dip coating; (<b>b</b>) LbL coating of colloidal templates by washing under centrifugation or filtration processes. Subsequent removal of the core leads to hollow capsules.</p>
Full article ">Figure 2
<p>(<b>a</b>) Whispering Gallery Modes detection system; (<b>b</b>) WGM chip with a microarray of 6000 wells (magnification 300×).</p>
Full article ">Figure 3
<p>(<b>a</b>) Principle of WGM measurement: (1) 405 nm laser for excitation of the fluorescence molecules; (2) some molecules in the neighborhood of the surface emit light by chance, which hits the surface by an angle larger than the critical angle and is totally reflected back; if their wavelength is in resonance after several reflections, they form the circulating WGM (3); after up to 10,000 circulations, they are scattered out (4), and their wavelengths are measured by the spectrometer (5); the spectra are sent for signal evaluation to the software (WhisperSense v1.1.3) (6). (<b>b</b>) Typical WGM spectrum of 10.2 µm polystyrene fluorescent microbeads before (black) and after adsorption of molecules (red, shifted). (<b>c</b>) Calculated mass of one polyelectrolyte layer adsorption over time.</p>
Full article ">Figure 4
<p>Deposition of one double layer of hydrogen-bonded PVPon/PMAA and electrostatically bonded PAH/PSS on a basic PVPon/PMAA or PAH/PSS coating, respectively (<b>a</b>) followed by WGM analytics; (<b>b</b>) followed by QCM analytics.</p>
Full article ">Figure 5
<p>Deposition of eight double layers of hydrogen-bonded PVPon/PMAA: (<b>a</b>) followed by WGM analytics; (<b>b</b>) followed by QCM analytics.</p>
Full article ">Figure 6
<p>Dissolution kinetics for (PVPon/PMAA)<sub>2</sub> at increasing pH values of different buffer solutions followed by WGM: the zero value corresponds to the sensor beads pre-coated with PAH/PSS/PAH/PMAA.</p>
Full article ">Figure 7
<p>(<b>a</b>) Assembling and degradation of the (PVPON/PMAA)<sub>3</sub>/(PAH/PSS)<sub>3.5</sub> salt-free assembling, followed by WGM; (<b>b</b>) assembling and degradation of the (PVPON/PMAA)<sub>3</sub>/(PAH/PSS)<sub>3.5</sub> assembled with 0.2 M salt, followed by WGM; (<b>c</b>) assembling and degradation of the (PVPON/PMAA)<sub>3</sub>/(PAH/PSS)<sub>3.5</sub> assembled with 0.2 M salt, followed by QCM; (<b>d</b>) degradation of the (PVPON/PMAA)<sub>3</sub>/(PAH-Rho/PSS)<sub>3.5</sub> assembled with 0.2 M salt on a glass slide, followed by Confocal Laser Scanning Microscopy (CLSM).</p>
Full article ">
17 pages, 6624 KiB  
Article
Laser-Induced Silver Nanowires/Polymer Composites for Flexible Electronics and Electromagnetic Compatibility Application
by Il’ya Bril’, Anton Voronin, Yuri Fadeev, Alexander Pavlikov, Ilya Govorun, Ivan Podshivalov, Bogdan Parshin, Mstislav Makeev, Pavel Mikhalev, Kseniya Afanasova, Mikhail Simunin and Stanislav Khartov
Polymers 2024, 16(22), 3174; https://doi.org/10.3390/polym16223174 - 14 Nov 2024
Viewed by 506
Abstract
Nowadays, the Internet of Things (IOT), electronics, and neural interfaces are becoming an integral part of our life. These technologies place unprecedentedly high demands on materials in terms of their mechanical and electrical properties. There are several strategies for forming conductive layers in [...] Read more.
Nowadays, the Internet of Things (IOT), electronics, and neural interfaces are becoming an integral part of our life. These technologies place unprecedentedly high demands on materials in terms of their mechanical and electrical properties. There are several strategies for forming conductive layers in such composites, e.g., volume blending to achieve a percolation threshold, inkjet printing, lithography, and laser processing. The latter is a low-cost, environmentally friendly, scalable way to produce composites. In our work, we synthesized AgNW and characterized them using Ultraviolet-visible spectroscopy (UV-vis), Transmission electron microscopy (TEM), and Selective area electron diffraction (SAED). We found that our AgNW absorbed in the UV-vis range of 345 to 410 nm. This is due to the plasmon resonance phenomenon of AgNW. Then, we applied the dispersion of AgNW on the surface of the polymer substrate, dried them and we got the films of AgNW.. We irradiated these films with a 432 nm laser. As a result of the treatment, we observed two processes. The first one was the sintering and partial melting of nanowires under the influence of laser radiation, as a consequence of which, the sheet resistance dropped more than twice. The second was the melting of the polymer at the interface and the subsequent integration of AgNW into the substrate. This allowed us to improve the adhesion from 0–1 B to 5 B, and to obtain a composite capable of bending, with radius of 0.5 mm. We also evaluated the shielding efficiency of the obtained composites. The shielding efficiency for 500–600 nm thick porous film samples were 40 dB, and for 3.1–4.1 µm porous films the shielding efficiency was about 85–90 dB in a frequency range of 0.01–40 GHz. The data obtained by us are the basis for producing flexible electronic components based on AgNW/PET composite for various applications using laser processing methods. Full article
(This article belongs to the Special Issue Multifunctional Polymer Composite Materials)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>AgNW characterization. (<b>a</b>)—TEM Image, (<b>b</b>)—SAED, (<b>c</b>)—AgNW diameter, (<b>d</b>)—AgNW length, (<b>e</b>)—UV-vis absorption spectra.</p>
Full article ">Figure 2
<p>Samples preparation and characterization. (<b>a</b>)—Samples obtaining scheme, (<b>b</b>)—effect of power density on electrical parameters and morphology, (<b>c</b>)—SEM images at different power densities, (<b>d</b>)—XRD of original film, (<b>e</b>)—XRD of laser-processed film.</p>
Full article ">Figure 3
<p>Thickness effect study. (<b>a</b>)—Dependence of thickness from concentration of AgNW basic dispersion, (<b>b</b>)—SEM image of x-section of 62.5 μL/cm2 BSE (top image), (<b>c</b>)—EDX spectra.</p>
Full article ">Figure 4
<p>Electrical properties. (<b>a</b>)—Four-point probe measurements illustration, (<b>b</b>)—sheet resistance/thickness dependence and resistivity of AgNW/PET composite, (<b>c</b>)—sheet resistance/thickness comparison [<a href="#B35-polymers-16-03174" class="html-bibr">35</a>,<a href="#B36-polymers-16-03174" class="html-bibr">36</a>,<a href="#B37-polymers-16-03174" class="html-bibr">37</a>,<a href="#B38-polymers-16-03174" class="html-bibr">38</a>,<a href="#B39-polymers-16-03174" class="html-bibr">39</a>,<a href="#B40-polymers-16-03174" class="html-bibr">40</a>,<a href="#B41-polymers-16-03174" class="html-bibr">41</a>,<a href="#B42-polymers-16-03174" class="html-bibr">42</a>].</p>
Full article ">Figure 5
<p>Electromagnetic compatibility. (<b>a</b>)—Waveguide method illustration, (<b>b</b>)—S<sub>21</sub> parameter at 0.01–7 GHz range, (<b>c</b>)—S<sub>21</sub> parameter at 17–26.5 GHz range, (<b>d</b>)—S<sub>21</sub> parameter at 26.5–40 GHz range.</p>
Full article ">Figure 6
<p>Reflection, absorption, transmission (RAT) diagrams. (<b>a</b>)—RAT at 0.01–7 GHz, (<b>b</b>)—RAT at 17–26.5 GHz, (<b>c</b>)—RAT at 26.5–40 GHz, (<b>d</b>)—AgNW/PET composite EMI shielding illustration.</p>
Full article ">Figure 7
<p>AgNW/PET composite comparisons with alternative materials. (<b>a</b>)—SE comparison [<a href="#B45-polymers-16-03174" class="html-bibr">45</a>,<a href="#B46-polymers-16-03174" class="html-bibr">46</a>,<a href="#B47-polymers-16-03174" class="html-bibr">47</a>,<a href="#B48-polymers-16-03174" class="html-bibr">48</a>,<a href="#B49-polymers-16-03174" class="html-bibr">49</a>,<a href="#B50-polymers-16-03174" class="html-bibr">50</a>,<a href="#B51-polymers-16-03174" class="html-bibr">51</a>,<a href="#B52-polymers-16-03174" class="html-bibr">52</a>,<a href="#B53-polymers-16-03174" class="html-bibr">53</a>,<a href="#B54-polymers-16-03174" class="html-bibr">54</a>,<a href="#B55-polymers-16-03174" class="html-bibr">55</a>,<a href="#B56-polymers-16-03174" class="html-bibr">56</a>,<a href="#B57-polymers-16-03174" class="html-bibr">57</a>,<a href="#B58-polymers-16-03174" class="html-bibr">58</a>,<a href="#B59-polymers-16-03174" class="html-bibr">59</a>,<a href="#B60-polymers-16-03174" class="html-bibr">60</a>,<a href="#B61-polymers-16-03174" class="html-bibr">61</a>], (<b>b</b>)—SSE<sub>T</sub> comparison [<a href="#B61-polymers-16-03174" class="html-bibr">61</a>,<a href="#B62-polymers-16-03174" class="html-bibr">62</a>,<a href="#B63-polymers-16-03174" class="html-bibr">63</a>,<a href="#B64-polymers-16-03174" class="html-bibr">64</a>,<a href="#B65-polymers-16-03174" class="html-bibr">65</a>,<a href="#B66-polymers-16-03174" class="html-bibr">66</a>,<a href="#B67-polymers-16-03174" class="html-bibr">67</a>,<a href="#B68-polymers-16-03174" class="html-bibr">68</a>].</p>
Full article ">Figure 8
<p>Mechanical properties. (<b>a</b>)—Optical image of untreated film before and after the ASTM D3359 test; (<b>b</b>)—optical image of processed film with C<sub>AgNW</sub> = 12.5 μL/cm<sup>2</sup> before and after the ASTM D3359 test; (<b>c</b>)—optical image of processed film with C<sub>AgNW</sub> = 75 μL/cm<sup>2</sup> before and after the ASTMD D3359 test; (<b>d</b>)—change in resistance after a tape test; (<b>e</b>)—changing of resistance at different bending radius; (<b>f</b>)—thermoforming demonstration.</p>
Full article ">
25 pages, 36381 KiB  
Article
Delineation of Groundwater Potential Using the Bivariate Statistical Models and Hybridized Multi-Criteria Decision-Making Models
by Müsteyde Baduna Koçyiğit and Hüseyin Akay
Water 2024, 16(22), 3273; https://doi.org/10.3390/w16223273 - 14 Nov 2024
Viewed by 524
Abstract
Identifying groundwater potential zones in a basin and developing a sustainable management plan is becoming more important, especially where surface water is scarce. The main aim of the study is to prepare the groundwater potential maps (GWPMs) considering the bivariate statistical models of [...] Read more.
Identifying groundwater potential zones in a basin and developing a sustainable management plan is becoming more important, especially where surface water is scarce. The main aim of the study is to prepare the groundwater potential maps (GWPMs) considering the bivariate statistical models of frequency ratio (FR), weight of evidence (WoE), and the multi-criteria decision-making (MCDM) model of Technique for Order Preference by Similarity to an Ideal Solution (TOPSIS) hybridized with FR and WoE. Two distance measures, Euclidean and Manhattan, were used in TOPSIS to evaluate their effect on GWPMs. The research focused on the Burdur Lake catchment located in the southwest of Türkiye. In total, 74 wells with high yields were chosen randomly for the analysis, 52 (70%) for training, and 22 (30%) for testing processes. Sixteen groundwater conditioning factors were selected. The area under the receiver operating characteristic (AUROC) and true skill statistics (TSS) were utilized to examine the goodness-of-fit and prediction accuracy of approaches. The TOPSIS-WoE-Manhattan model and the FR and WoE models gave the best AUROC values of 0.915 and 0.944 for the training and testing processes, respectively. The best TSS values of 0.827 and 0.864 were obtained by the TOPSIS-FR-Euclidean and WoE models for the training and testing processes, respectively. Full article
Show Figures

Figure 1

Figure 1
<p>Location map of Burdur Lake catchment in Türkiye.</p>
Full article ">Figure 2
<p>Methodology of the study.</p>
Full article ">Figure 3
<p>Topographic-related groundwater conditioning factors: (<b>a</b>) elevation; (<b>b</b>) slope; (<b>c</b>) aspect; (<b>d</b>) curvature; (<b>e</b>) TWI; (<b>f</b>) SPI; (<b>g</b>) TPI; (<b>h</b>) TRI; (<b>i</b>) CI; (<b>j</b>) distance to stream; (<b>k</b>) distance to fault; (<b>l</b>) proximity to the lake; (<b>m</b>) drainage density; (<b>n</b>) rainfall; (<b>o</b>) LULC where (1) artificial surfaces, (2) agricultural areas, (3) forest and semi-natural areas, (4) wetlands, and (5) water bodies; and (<b>p</b>) lithology in which Qal: alluvial deposits, plk: lacustrine limestone, travertine with intermediate level, Pk: limestone, Kkr: Iimestone, chert, and radiolarite interlayers, Ok: conglomerate, plçkı: conglomerate, sandstone, Mko: conglomerate, sandstone, mudstone, Pkt: sandstone, claystone, sandy limestone, siltstone, Ek: sandstone, sandy limestone, claystone, siltstone, plm: marn, mudstone, lacustrine limestone with intermediate level, Ko: ophiolite, peridotite, harzburgite, pyroxene, dunite, Kom: ophiolitic mélange and olistostrome, Tra: recrystallized limestone, plQt: tuff, tuffite, pumice, plQ: gravelstone, sandstone, mudstone, Ok_toacm: mudstone, sandstone, shale.</p>
Full article ">Figure 3 Cont.
<p>Topographic-related groundwater conditioning factors: (<b>a</b>) elevation; (<b>b</b>) slope; (<b>c</b>) aspect; (<b>d</b>) curvature; (<b>e</b>) TWI; (<b>f</b>) SPI; (<b>g</b>) TPI; (<b>h</b>) TRI; (<b>i</b>) CI; (<b>j</b>) distance to stream; (<b>k</b>) distance to fault; (<b>l</b>) proximity to the lake; (<b>m</b>) drainage density; (<b>n</b>) rainfall; (<b>o</b>) LULC where (1) artificial surfaces, (2) agricultural areas, (3) forest and semi-natural areas, (4) wetlands, and (5) water bodies; and (<b>p</b>) lithology in which Qal: alluvial deposits, plk: lacustrine limestone, travertine with intermediate level, Pk: limestone, Kkr: Iimestone, chert, and radiolarite interlayers, Ok: conglomerate, plçkı: conglomerate, sandstone, Mko: conglomerate, sandstone, mudstone, Pkt: sandstone, claystone, sandy limestone, siltstone, Ek: sandstone, sandy limestone, claystone, siltstone, plm: marn, mudstone, lacustrine limestone with intermediate level, Ko: ophiolite, peridotite, harzburgite, pyroxene, dunite, Kom: ophiolitic mélange and olistostrome, Tra: recrystallized limestone, plQt: tuff, tuffite, pumice, plQ: gravelstone, sandstone, mudstone, Ok_toacm: mudstone, sandstone, shale.</p>
Full article ">Figure 4
<p>Weights of factors with the AHP method.</p>
Full article ">Figure 5
<p>Maps of groundwater potential classes by using the methods of (<b>a</b>) FR, (<b>b</b>) WoE, (<b>c</b>) TOPSIS-FR-Euclidean, (<b>d</b>) TOPSIS-FR-Manhattan, (<b>e</b>) TOPSIS-WoE-Euclidean, and (<b>f</b>) TOPSIS-WoE-Manhattan.</p>
Full article ">Figure 5 Cont.
<p>Maps of groundwater potential classes by using the methods of (<b>a</b>) FR, (<b>b</b>) WoE, (<b>c</b>) TOPSIS-FR-Euclidean, (<b>d</b>) TOPSIS-FR-Manhattan, (<b>e</b>) TOPSIS-WoE-Euclidean, and (<b>f</b>) TOPSIS-WoE-Manhattan.</p>
Full article ">Figure 6
<p>Validation of estimated groundwater potential maps by extraction values of (<b>a</b>) training and (<b>b</b>) testing processes.</p>
Full article ">Figure 7
<p>Variations in areal percentage of the drainage area of groundwater potential categories (VL = Very Low, L = Low, M = Medium, H = High, and VH = Very High) based on the natural break method generated by the FR, WoE, TOPSIS-FR-Euclidean, TOPSIS-FR-Manhattan, TOPSIS-WoE-Euclidean, and TOPSIS-WoE-Manhattan models.</p>
Full article ">Figure 8
<p>Variations in percent groundwater pixels at groundwater potential categories based on the natural break method generated by the FR, WoE, TOPSIS-FR-Euclidean, TOPSIS-FR-Manhattan, TOPSIS-WoE-Euclidean, and TOPSIS-WoE-Manhattan models.</p>
Full article ">
14 pages, 2271 KiB  
Article
Location Detection and Numerical Simulation of Guided Wave Defects in Steel Pipes
by Hao Liang, Junhong Zhang and Song Yang
Appl. Sci. 2024, 14(22), 10403; https://doi.org/10.3390/app142210403 - 12 Nov 2024
Viewed by 480
Abstract
At present, researchers in the field of pipeline inspection focus on pipe wall defects while neglecting pipeline defects in special situations such as welds. This poses a threat to the safe operation of projects. In this paper, a multi-node fusion and modal projection [...] Read more.
At present, researchers in the field of pipeline inspection focus on pipe wall defects while neglecting pipeline defects in special situations such as welds. This poses a threat to the safe operation of projects. In this paper, a multi-node fusion and modal projection algorithm of steel pipes based on guided wave technology is proposed. Through an ANSYS numerical simulation, research is conducted to achieve the identification, localization, and quantification of axial cracks on the surface of straight pipelines and internal cracks in circumferential welds. The propagation characteristics and vibration law of ultrasonic guided waves are theoretically solved by the semi-analytical finite element method in the pipeline. The model section is discretized in one-dimensional polar coordinates to obtain the dispersion curve of the steel pipe. The T(0,1) mode, which is modulated by the Hanning window, is selected to simulate the axial crack of the pipeline and the L(0,2) mode to simulate the crack in the weld, and the correctness of the dispersion curve is verified. The results show that the T(0,1) and L(0,2) modes are successfully excited, and they are sensitive to axial and circumferential cracks. The time–frequency diagram of wavelet transform and the time domain diagram of the crack signal of Hilbert transform are used to identify the echo signal. The first wave packet peak point and group velocity are used to locate the crack. The pure signal of the crack is extracted from the simulation data, and the variation law between the reflection coefficient and the circumferential and radial dimensions of the defect is calculated to evaluate the size of the defect. This provides a new and feasible method for steel pipe defect detection. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) The dispersion curve of group velocity. (<b>b</b>) The dispersion curve of phase velocity.</p>
Full article ">Figure 2
<p>Displacement wave structures with different longitudinal modes: (<b>a</b>) L(0,2); (<b>b</b>) L(0,1).</p>
Full article ">Figure 3
<p>Schematic diagram of different guided waves propagating in pipes: (<b>a</b>) T(0,1); (<b>b</b>) L(0,2).</p>
Full article ">Figure 4
<p>Pipeline defect: (<b>a</b>) axial defect; (<b>b</b>) inner defect of circumferential weld.</p>
Full article ">Figure 5
<p>Flow chart of steel pipe modeling.</p>
Full article ">Figure 6
<p>Hanning window modulation signal.</p>
Full article ">Figure 7
<p>2DFFT result chart.</p>
Full article ">Figure 8
<p>Axial displacement nephogram of defects in circumferential weld at different times: (<b>a</b>) t = 0.5 ms; (<b>b</b>) t = 1 ms; (<b>c</b>) t = 1.5 ms; (<b>d</b>) t = 2 ms; (<b>e</b>) t = 2.5 ms; (<b>f</b>) t = 3 ms.</p>
Full article ">Figure 9
<p>(<b>a</b>) Waveform of a crack-free pipeline; (<b>b</b>) waveform of a cracked pipeline; (<b>c</b>) fesidual signal data waveform.</p>
Full article ">Figure 10
<p>Time–frequency diagram of a wavelet transform signal.</p>
Full article ">Figure 11
<p>Time domain diagram of Hilbert transform crack signal.</p>
Full article ">Figure 12
<p>Quantitative analysis of circumferential defects in pipes with different lengths: (<b>a</b>) 30°; (<b>b</b>) 60°; (<b>c</b>) 180°; (<b>d</b>) reflection coefficient relation–circumferential dimension curve.</p>
Full article ">Figure 13
<p>Quantitative analysis of pipeline defects with different radial depths: (<b>a</b>) 2 mm; (<b>b</b>) 2.5 mm; (<b>c</b>) 3 mm; (<b>d</b>) reflection coefficient relation–radial dimension curve.</p>
Full article ">
17 pages, 3593 KiB  
Article
The Effect of the Construction of a Tillage Layer on the Infiltration of Snowmelt Water into Freeze–Thaw Soil in Cold Regions
by Ziqiao Zhou, Sisi Liu, Bingyu Zhu, Rui Wang, Chao Liu and Renjie Hou
Water 2024, 16(22), 3224; https://doi.org/10.3390/w16223224 - 9 Nov 2024
Viewed by 363
Abstract
The snow melting and runoff process in the black soil area of Northeast China has led to soil quality degradation in farmland, posing a threat to sustainable agricultural development. To investigate the regulatory effect of tillage layer construction on the infiltration characteristics of [...] Read more.
The snow melting and runoff process in the black soil area of Northeast China has led to soil quality degradation in farmland, posing a threat to sustainable agricultural development. To investigate the regulatory effect of tillage layer construction on the infiltration characteristics of snowmelt water, a typical black soil in Northeast China was selected as the research object. Based on field experiments, four protective tillage treatments (CK: control treatment; SB: sub-soiling treatment; BC: biochar regulation treatment; SB + BC: sub-soiling tillage and biochar composite treatment) were set up, and the evolution of soil physical structure, soil thawing rate, snow melting infiltration characteristics, and the feedback effect of frozen layer evolution on snowmelt infiltration were analyzed. The research results indicate that sub-soiling and the application of biochar effectively regulate soil aggregate particle size and increase soil total porosity. Among them, at the 0–10 cm soil layer, the soil mean weight diameter (MWD) values under SB, BC, and SB + BC treatment conditions increased by 6.25%, 16.67%, and 19.35%, respectively, compared to the CK treatment. Sub-soiling increases the frequency of energy exchange between the soil and the environment, while biochar enhances soil heat storage performance and accelerates the melting rate of frozen soil layers. Therefore, under the SB + BC treatment conditions, the maximum soil freezing rate increased by 21.92%, 5.67%, and 25.12% compared to the CK, SB, and BC treatments, respectively. In addition, sub-soiling and biochar treatment effectively improved the penetration performance of snowmelt water into frozen soil layers, significantly enhancing the soil’s ability to store snowmelt water. Overall, it can be concluded that biochar regulation has a good improvement effect on the infiltration capacity of surface soil snowmelt water. Sub-soiling can enhance the overall snowmelt water holding capacity, and the synergistic effect of biochar and deep tillage is the best. These research results have important guiding significance for the rational construction of a protective tillage system model and the improvement of the utilization efficiency of snowmelt water resources in black soil areas. Full article
Show Figures

Figure 1

Figure 1
<p>Meteorological background conditions in the study area.</p>
Full article ">Figure 2
<p>Soil structure characteristics. (<b>a</b>) Soil mean weight diameter; (<b>b</b>) proportion of soil particles &gt; 0.25 mm in size; (<b>c</b>) total soil porosity; (<b>d</b>) soil three-phase structure distance. Different letters represent the variability of soil at different depths under the same treatment conditions (<span class="html-italic">p</span> &lt; 0.05).</p>
Full article ">Figure 3
<p>Characterization of thickness of soil frost layer evolution. (<b>a</b>) represents the CK treatment; (<b>b</b>) represents the SB treatment; (<b>c</b>) represents the BC treatment; and (<b>d</b>) represents the SB + BC treatment.</p>
Full article ">Figure 4
<p>Snow melting and infiltration process. (<b>a</b>) represents the CK treatment; (<b>b</b>) represents the SB treatment; (<b>c</b>) represents the BC treatment; and (<b>d</b>) represents the SB + BC treatment.</p>
Full article ">Figure 5
<p>Interaction effects of snowpack ablation infiltration and freezing depth evolution. (<b>a</b>–<b>d</b>) represent the relationship between soil thawing rate and snow melting rate under different treatments. (<b>e</b>–<b>h</b>) represent the relationship between soil frost thickness and cumulative infiltration under different treatments.</p>
Full article ">Figure 6
<p>Variation curve of cumulative soil infiltration. (<b>a</b>) Pre-freezing period; the tension is −5 cm; (<b>b</b>) pre-freezing period; the tension is −10 cm; (<b>c</b>) post-thaw period; the tension is −5 cm; and (<b>d</b>) post-thaw period; the tension is −10 cm.</p>
Full article ">Figure 7
<p>Saturated hydraulic conductivity of frozen and unfrozen soil. (<b>a</b>) 0–10 cm soil layer; (<b>b</b>) 10–20 cm soil layer; (<b>c</b>) 20–30 cm soil layer; and (<b>d</b>) 30–40 cm soil layer. Different letters represent the variability of soil at different depths under the same treatment conditions (<span class="html-italic">p</span> &lt; 0.05).</p>
Full article ">
13 pages, 4685 KiB  
Article
High-Performance SAW-Based Microfluidic Actuators Composed of Sputtered Al–Cu IDT Electrodes
by Hwansun Kim, Youngjin Lee, Peddathimula Puneetha, Sung Jin An, Jae-Cheol Park and Siva Pratap Reddy Mallem
Coatings 2024, 14(11), 1420; https://doi.org/10.3390/coatings14111420 - 8 Nov 2024
Viewed by 419
Abstract
To realize highly sensitive SAW devices, novel Al–Cu thin films were developed using a combinatorial sputtering system. The Al–Cu sample library exhibited a wide range of chemical compositions and electrical resistivities, providing valuable insights for selecting optimal materials for SAW devices. Considering the [...] Read more.
To realize highly sensitive SAW devices, novel Al–Cu thin films were developed using a combinatorial sputtering system. The Al–Cu sample library exhibited a wide range of chemical compositions and electrical resistivities, providing valuable insights for selecting optimal materials for SAW devices. Considering the significant influence of electrode resistivity and density on acoustic wave propagation, an Al–Cu film with 65 at% Al was selected as the IDT electrode material. The selected Al–Cu film demonstrated a resistivity of 6.0 × 10−5 Ω-cm and a density of 4.4 g/cm3, making it suitable for SAW-based microfluidic actuator applications. XRD analysis revealed that the Al–Cu film consisted of a physical mixture of Al and Cu without the formation of Al–Cu alloy phases. The film exhibited a fine-grained microstructure with an average crystallite size of 7.5 nm and surface roughness of approximately 6 nm. The SAW device fabricated with Al–Cu IDT electrodes exhibited excellent acoustic performance, resonating at 143 MHz without frequency shift and achieving an insertion loss of −13.68 dB and a FWHM of 0.41 dB. In contrast, the Au electrode-based SAW device showed significantly degraded acoustic characteristics. Moreover, the SAW-based microfluidic module equipped with optimized Al–Cu IDT electrodes successfully separated 5 μm polystyrene (PS) particles even at high flow rates, outperforming devices with Au IDT electrodes. This enhanced performance can be attributed to the improved resonance characteristics of the SAW device, which resulted in a stronger acoustic radiation force exerted on the PS particles. Full article
(This article belongs to the Special Issue Thin Films and Nanostructures for Electronics)
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of combinatorial sputtering to produce Al–Cu thin films with varying and uniform compositions.</p>
Full article ">Figure 2
<p>Thickness distribution and cross-section images of Al–Cu thin films [<a href="#B25-coatings-14-01420" class="html-bibr">25</a>].</p>
Full article ">Figure 3
<p>Surface and cross-sectional SEM images of Al–Cu thin films with uniform thickness and compositions.</p>
Full article ">Figure 4
<p>XRD patterns of Al–Cu thin films with uniform physical and chemical properties.</p>
Full article ">Figure 5
<p>AFM topography images of sputter-deposited Al–Cu thin films (S1, S2, S3) with different surface roughness values.</p>
Full article ">Figure 6
<p>SAW-IDT pattern design for separating 5 μm PS micro-particles. (<b>a</b>) Distribution of resonant frequency depending on IDT pattern width and (<b>b</b>) relationship between total IDT length and electrode pairs at the reference impedance of 50 Ω.</p>
Full article ">Figure 7
<p>Resonant frequency of SAW devices with Al–Cu and Au electrode.</p>
Full article ">Figure 8
<p>SAW-based microfluidic actuator module for 5 μm PS particle separation. (<b>a</b>) Picture of SAW-based microfluidic actuator module and (<b>b</b>) separation efficiency of PS particles according to the flow rate of PS suspension with a concentration of 100 μg/L.</p>
Full article ">Figure 9
<p>Optical microscope images of PS particles captured at the drain/outlet ports in the SAW actuator module consisting of two different electrodes.</p>
Full article ">
19 pages, 6416 KiB  
Article
Fourier Neural Operator Networks for Solving Reaction–Diffusion Equations
by Yaobin Hao and Fangying Song
Fluids 2024, 9(11), 258; https://doi.org/10.3390/fluids9110258 - 6 Nov 2024
Viewed by 492
Abstract
In this paper, we used Fourier Neural Operator (FNO) networks to solve reaction–diffusion equations. The FNO is a novel framework designed to solve partial differential equations by learning mappings between infinite-dimensional functional spaces. We applied the FNO to the Surface Quasi-Geostrophic (SQG) equation, [...] Read more.
In this paper, we used Fourier Neural Operator (FNO) networks to solve reaction–diffusion equations. The FNO is a novel framework designed to solve partial differential equations by learning mappings between infinite-dimensional functional spaces. We applied the FNO to the Surface Quasi-Geostrophic (SQG) equation, and we tested the model with two significantly different initial conditions: Vortex Initial Conditions and Sinusoidal Initial Conditions. Furthermore, we explored the generalization ability of the model by evaluating its performance when trained on Vortex Initial Conditions and applied to Sinusoidal Initial Conditions. Additionally, we investigated the modes (frequency parameters) used during training, analyzing their impact on the experimental results, and we determined the most suitable modes for this study. Next, we conducted experiments on the number of convolutional layers. The results showed that the performance of the models did not differ significantly when using two, three, or four layers, with the performance of two or three layers even slightly surpassing that of four layers. However, as the number of layers increased to five, the performance improved significantly. Beyond 10 layers, overfitting became evident. Based on these observations, we selected the optimal number of layers to ensure the best model performance. Given the autoregressive nature of the FNO, we also applied it to solve the Gray–Scott (GS) model, analyzing the impact of different input time steps on the performance of the model during recursive solving. The results indicated that the FNO requires sufficient information to capture the long-term evolution of the equations. However, compared to traditional methods, the FNO offers a significant advantage by requiring almost no additional computation time when predicting with new initial conditions. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) the structural framework of the complete Fourier Neural Operator; (<b>b</b>) the structure of a Fourier layer.</p>
Full article ">Figure 2
<p>The plot illustrates the training and testing loss after 500 epochs for different numbers of Fourier modes (6, 12, 18, 24).</p>
Full article ">Figure 3
<p>The <b>first row</b> of images shows the values of the solution at time steps 11, 13, 15, 17, and 19 resulting from the numerical method. The <b>second row</b> of images displays the predicted values of the FNO at these same time steps. The third row of images shows the absolute error between the numerical solution and the FNO prediction.</p>
Full article ">Figure 4
<p>Comparison of test errors across various models with different numbers of convolutional layers (y-axis: logarithmic scale of loss values).</p>
Full article ">Figure 5
<p>The above figure shows the effect of different convolutional layer variations on the experimental results: (<b>a</b>) comparison of test errors for different convolutional layers; (<b>b</b>) taking logarithms of both the test error and the number of convolutional layers.</p>
Full article ">Figure 6
<p>Numerical solutions (<b>first row</b>) and predicted values (<b>second row</b>) for the Sinusoidal Initial Condition at time steps 11, 13, 15, 17, and 19 from left to right, respectively.</p>
Full article ">Figure 7
<p>Numerical solutions (<b>first row</b>) and predicted values (<b>second row</b>) of the Vortex Initial Condition at 11, 13, 15, 17, and 19 from left to right, respectively.</p>
Full article ">Figure 8
<p>The <b>first row</b> of images shows the numerical solution, followed by the results of predicting at 11, 13, 15, 17, and 19, using input steps of 2, 4, 6, 8, and 10 from top to bottom.</p>
Full article ">Figure 9
<p>Comparison of predicted L2 errors for different input time steps.</p>
Full article ">Figure A1
<p>(<b>a</b>) the values of the solution at time steps 11, 13, 15, 17, and 19 resulting from the numerical method; (<b>b</b>) the figure shows the results of a model trained using only the Vortex Initial Conditions to predict the Sinusoidal Initial Conditions at time steps 11, 13, 15, 17, and 19.</p>
Full article ">Figure A2
<p>(<b>a</b>) the figure shows the results of a model trained using a combination of 100 Vortex Initial Conditions and five Sinusoidal Initial Conditions, to predict the Sinusoidal Initial Conditions at time steps 11, 13, 15, 17, and 19; (<b>b</b>) the error between the numerical solution and the prediction is demonstrated.</p>
Full article ">Figure A3
<p>(<b>a</b>) the figure shows the results of a model trained using a combination of 100 Vortex Initial Conditions and 15 Sinusoidal Initial Conditions, to predict the Sinusoidal Initial Conditions at time steps 11, 13, 15, 17, and 19; (<b>b</b>) the error between the numerical solution and the prediction is demonstrated.</p>
Full article ">Figure A4
<p>(<b>a</b>) the figure shows the results of a model trained using a combination of 100 Vortex Initial Conditions and 25 Sinusoidal Initial Conditions, to predict the Sinusoidal Initial Conditions at time steps 11, 13, 15, 17, and 19; (<b>b</b>) the error between the numerical solution and the prediction is demonstrated.</p>
Full article ">
27 pages, 3503 KiB  
Review
Frequency Selective Surfaces: Design, Analysis, and Applications
by Waseem Afzal, Muhammad Zeeshan Baig, Amir Ebrahimi, Md. Rokunuzzaman Robel, Muhammad Tausif Afzal Rana and Wayne Rowe
Telecom 2024, 5(4), 1102-1128; https://doi.org/10.3390/telecom5040056 - 5 Nov 2024
Viewed by 777
Abstract
This paper aims to provide a general review of the fundamental ideas, varieties, methods, and experimental research of the most advanced frequency selective surfaces available today. Frequency-selective surfaces are periodic structures engineered to work as spatial filters in interaction with electromagnetic (EM) waves [...] Read more.
This paper aims to provide a general review of the fundamental ideas, varieties, methods, and experimental research of the most advanced frequency selective surfaces available today. Frequency-selective surfaces are periodic structures engineered to work as spatial filters in interaction with electromagnetic (EM) waves with different frequencies, polarization, and incident angles in a desired and controlled way. They are usually made of periodic elements with dimensions less than the operational wavelength. The primary issue examined is the need for more efficient, compact, and adaptable electromagnetic filtering solutions. The research method involved a comprehensive review of recent advancements in FSS design, focusing on structural diversity, miniaturization, multiband operations, and the integration of active components for tunability and reconfigurability. Key findings include the development of highly selective miniaturized FSSs, innovative applications on flexible and textile substrates, and the exploration of FSSs for liquid and strain sensing. The conclusions emphasize the significant potential of FSS technology to enhance wireless communication, environmental monitoring, and defense applications. This study provides valuable insights into the design and application of FSSs, aiming to guide future research and development in this dynamic field. Full article
Show Figures

Figure 1

Figure 1
<p>Wave interaction with FSS characteristics: (<b>a</b>) bandpass, (<b>b</b>) bandstop, (<b>c</b>) absorber, (<b>d</b>) polarization converter [<a href="#B14-telecom-05-00056" class="html-bibr">14</a>].</p>
Full article ">Figure 2
<p>Radomes at the Cryptologic Operations Center, Misawa, Japan (photo courtesy of en. Wikipedia).</p>
Full article ">Figure 3
<p>Cassini high-gain antenna (HGA) with a four-band FSS [<a href="#B2-telecom-05-00056" class="html-bibr">2</a>].</p>
Full article ">Figure 4
<p>An active LC array comprising metallic strips interrupted by gaps in a periodic fashion. The gaps can be loaded with varactor diodes to alter the gap capacitance [<a href="#B5-telecom-05-00056" class="html-bibr">5</a>].</p>
Full article ">Figure 5
<p>Classification of FSSs.</p>
Full article ">Figure 6
<p>Current distribution at the first and the second resonant modes—(<b>top</b>) shows the fundamental mode (frequency <math display="inline"><semantics> <msub> <mi>f</mi> <mn>0</mn> </msub> </semantics></math>), which is excited for any element shape irrespective of the incidence angle; (<b>bottom</b>) shows the first odd mode at about 2<math display="inline"><semantics> <msub> <mi>f</mi> <mn>0</mn> </msub> </semantics></math>, which may be excited at oblique incidence. The frequency of this mode may change slightly depending on the element shape [<a href="#B1-telecom-05-00056" class="html-bibr">1</a>].</p>
Full article ">Figure 7
<p>Typical shapes of FSSs. (<b>a</b>) N-pole or center-connected; (<b>b</b>) Loop type; (<b>c</b>) Solid interiors; (<b>d</b>) Combination of either first three [<a href="#B112-telecom-05-00056" class="html-bibr">112</a>].</p>
Full article ">Figure 8
<p>Examples of the third class of FSSs, the plate type elements [<a href="#B111-telecom-05-00056" class="html-bibr">111</a>].</p>
Full article ">Figure 9
<p>Frequency selective surface made of Jerusalem cross elements. (<b>a</b>) Jerusalem cross unit cell, (<b>b</b>) Simulated transmission and reflection coefficient [<a href="#B131-telecom-05-00056" class="html-bibr">131</a>].</p>
Full article ">Figure 10
<p>(<b>a</b>) Perspective view of 3D FSS; (<b>b</b>) cross-sectional view of FSS (<b>c</b>); side-view (Picture is taken from [<a href="#B142-telecom-05-00056" class="html-bibr">142</a>]).</p>
Full article ">Figure 11
<p>The first miniaturized element FSS. (<b>a</b>) 3D view of FSS, (<b>b</b>) the unit cell of the structure. (Picture taken from [<a href="#B112-telecom-05-00056" class="html-bibr">112</a>]).</p>
Full article ">Figure 12
<p>(<b>a</b>) Lumped-element circuit model for miniaturized elements, (<b>b</b>) Comparison between EM and circuit model simulations with <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>=</mo> <mn>1.08</mn> </mrow> </semantics></math> nH and <math display="inline"><semantics> <mrow> <mi>c</mi> <mo>=</mo> <mn>0.15</mn> </mrow> </semantics></math> pF (results are adopted from [<a href="#B112-telecom-05-00056" class="html-bibr">112</a>]).</p>
Full article ">Figure 13
<p>Scan angle performance of miniaturized-element FSS; (<b>a</b>) TE Polarization; (<b>b</b>) TM Polarization (results are adopted from [<a href="#B112-telecom-05-00056" class="html-bibr">112</a>]).</p>
Full article ">
22 pages, 14012 KiB  
Article
Towards Advancing Real-Time Railroad Inspection Using a Directional Eddy Current Probe
by Meirbek Mussatayev, Ruby Kempka and Mohammed Alanesi
Sensors 2024, 24(20), 6702; https://doi.org/10.3390/s24206702 - 18 Oct 2024
Viewed by 657
Abstract
In the field of railroad safety, the effective detection of surface cracks is critical, necessitating reliable, high-speed, non-destructive testing (NDT) methods. This study introduces a hybrid Eddy Current Testing (ECT) probe, specifically engineered for railroad inspection, to address the common issue of “lift-off [...] Read more.
In the field of railroad safety, the effective detection of surface cracks is critical, necessitating reliable, high-speed, non-destructive testing (NDT) methods. This study introduces a hybrid Eddy Current Testing (ECT) probe, specifically engineered for railroad inspection, to address the common issue of “lift-off noise” due to varying distances between the probe and the test material. Unlike traditional ECT methods, this probe integrates transmit and differential receiver (Tx-dRx) coils, aiming to enhance detection sensitivity and minimise the lift-off impact. The study optimises ECT probes employing different transmitter coils, emphasising three main objectives: (a) quantitatively evaluating each probe using signal-to-noise ratio (SNR) and outlining a real-time data-processing algorithm based on SNR methodology; (b) exploring the frequency range proximal to the electrical resonance of the receiver coil; and (c) examining sensitivity variations across varying lift-off distances. The experimental outcomes indicate that the newly designed probe with a figure-8 shaped transmitter coil significantly improves sensitivity in detecting surface cracks on railroads. It achieves an impressive SNR exceeding 100 for defects with minimal dimensions of 1 mm in width and depth. The simulation results closely align with experimental findings, validating the investigation of the optimal operational frequency and lift-off distance for selected probe performance, which are determined to be 0.3 MHz and 1 mm, respectively. The realisation of this project would lead to notable advancements in enhancing railroad safety by improving the efficiency of crack detection. Full article
(This article belongs to the Section Physical Sensors)
Show Figures

Figure 1

Figure 1
<p>Improved efficiency of current railroad inspection.</p>
Full article ">Figure 2
<p>Three eddy current probe configurations with: (<b>a</b>) singular; (<b>b</b>) +point, and (<b>c</b>) figure-8 shaped.</p>
Full article ">Figure 3
<p>Directional EC probe design: (<b>a</b>) winding method of the +Point, (<b>b</b>) figure-8 shaped, (<b>c</b>) rectangular single transmitter, (<b>d</b>) rectangular (RCT) receiver coil dimensions (top-down view) and (<b>e</b>) resonant frequencies of different transmitter coils.</p>
Full article ">Figure 4
<p>Simplified diagram of amplifier with tuning caps and drive coils.</p>
Full article ">Figure 5
<p>Exemplar plot of identification process of proposed system.</p>
Full article ">Figure 6
<p>Schematic of the virtual scanning model.</p>
Full article ">Figure 7
<p>(<b>i</b>) Simulated mesh overview: (<b>a</b>,<b>c</b>,<b>e</b>) show the mesh with the air domain, while (<b>b</b>,<b>d</b>,<b>f</b>) provide a zoomed-in view of the transmitter coils’ positioning near the rail for the “Singular”, “+Point”, and “Figure-8” configurations, respectively. (<b>ii</b>) FEM simulations of induced eddy current flow patterns for the (<b>a</b>) singular, (<b>b</b>) plus-point, and (<b>c</b>) figure-8-shaped probes.</p>
Full article ">Figure 8
<p>(<b>a</b>) Rail track sample (<b>b</b>). Experimental set-up.</p>
Full article ">Figure 9
<p>Optimal frequency selection study results depicted in rows: (<b>i</b>) experimental raw EC data; (<b>ii</b>) FEM simulations for EC probes with transmitter coils in configurations: (<b>a</b>) single, (<b>b</b>) plus-point, and (<b>c</b>) figure-8 shaped.</p>
Full article ">Figure 10
<p>Comparative analysis of probe sensitivity across various.</p>
Full article ">Figure 11
<p>Eddy current scan data and FEM simulation results are depicted as follows: (<b>i</b>) experimental raw EC data obtained using a figure-8 shaped transmitter at lift-offs of (<b>a</b>) 0.25 mm, (<b>b</b>) 0.5 mm, and (<b>c</b>) 1 mm; (<b>ii</b>) corresponding FEM simulation outputs for the same lift-offs shown in (<b>d</b>–<b>f</b>), respectively.</p>
Full article ">Figure 12
<p>Performance assessment of EC probe with a figure-8 shaped transmitter across lift-off distances of 0.25 mm, 0.5 mm, and 1.0 mm: (<b>a</b>) separate contributions of signal (S) and noise (N) and (<b>b</b>) SNR across various frequencies; (<b>c</b>) average voltage and structural noise at optimum 0.3 MHz.</p>
Full article ">Figure 13
<p>Lift-off noise insensitivity results using the initial EC probe prototype with a +Point transmitter and two differentially hand-wound meander receiver coils: (<b>a</b>) top-down view of the probe, and (<b>b</b>) side view of the probe on the sample with varying depths and EC scan results at 0.3 MHz.</p>
Full article ">Figure 14
<p>Dimensions of the specimen and artificially drilled hole: (<b>a</b>) schematic diagram; (<b>b</b>) real photo of the specimen.</p>
Full article ">Figure 15
<p>Raw EC data with lift-off distances of 0.25, 0.5, and 1 mm at (<b>a</b>) 0.25 MHz, (<b>b</b>) 0.3 MHz, and (<b>c</b>) 0.35 MHz operational frequencies.</p>
Full article ">Figure 16
<p>Selected probe signal-to-noise ratio over defect 1 and defects 2–3, with separate noise contributions as a function of lift-off distance.</p>
Full article ">Figure 17
<p>Eddy current scan results over studs using the selected probe: (<b>a</b>) inspected sample; (<b>b</b>) raw eddy current scan results from two individual scans.</p>
Full article ">
11 pages, 2054 KiB  
Article
Variants rs3804099 and rs3804100 in the TLR2 Gene Induce Different Profiles of TLR-2 Expression and Cytokines in Response to Spike of SARS-CoV-2
by Julio Flores-González, Zurisadai Monroy-Rodríguez, Ramcés Falfán-Valencia, Ivette Buendía-Roldán, Ingrid Fricke-Galindo, Rafael Hernández-Zenteno, Ricardo Herrera-Sicairos, Leslie Chávez-Galán and Gloria Pérez-Rubio
Int. J. Mol. Sci. 2024, 25(20), 11063; https://doi.org/10.3390/ijms252011063 - 15 Oct 2024
Viewed by 773
Abstract
The present study aimed to identify in patients with severe COVID-19 and acute respiratory distress syndrome (ARDS) the association between rs3804099 and rs3804100 (TLR2) and evaluate the expression of TLR-2 on the cell surface of innate and adaptive cells of patients’ [...] Read more.
The present study aimed to identify in patients with severe COVID-19 and acute respiratory distress syndrome (ARDS) the association between rs3804099 and rs3804100 (TLR2) and evaluate the expression of TLR-2 on the cell surface of innate and adaptive cells of patients’ carriers of C allele in at least one genetic variant. We genotyped 1018 patients with COVID-19 and ARDS. According to genotype, a subgroup of 12 patients was selected to stimulate peripheral blood mononuclear cells (PBMCs) with spike and LPS + spike. We evaluated soluble molecules in cell culture supernatants. The C allele in TLR2 (rs3804099, rs3804100) is not associated with a risk of severe COVID-19; however, the presence of the C allele (rs3804099 or rs3804100) affects the TLR-2 ability to respond to a spike of SARS-CoV-2 correctly. The reference group (genotype TT) downregulated the frequency of non-switched TLR-2+ B cells in response to spike stimulus; however, the allele’s C carriers group is unable to induce this regulation, but they produce high levels of IL-10, IL-6, and TNF-α by an independent pathway of TLR-2. Findings showed that TT genotypes (rs3804099 and rs3804100) affect the non-switched TLR-2+ B cell distribution. Genotype TT (rs3804099 and rs3804100) affects the TLR-2’s ability to respond to a spike of SARS-CoV-2. However, the C allele had increased IL-10, IL-6, and TNF-α by stimulation with spike and LPS. Full article
Show Figures

Figure 1

Figure 1
<p>TLR-2 expression in monocytes of patients with COVID-19 according to genotypes (rs3804099 and rs3804100). They were stimulated for 24 h with spike protein (1 µg/mL) or spike + LPS (1 µg/mL). An unstimulated condition was included as a control stimulation (Unstimulated). (<b>A</b>) Representative dot plots show the limitation of CD2-D3−, then the gate CD14+HLA-DR+. (<b>B</b>) The frequency of TLR -2+ monocytes is reported, and each dot represents an independent patient. Data are expressed as median and IQR values. The statistical comparisons were performed using the Kruskal-Wallis test. Blue squares are used for the reference group, and red circles for the allele C carriers’ group.</p>
Full article ">Figure 2
<p>Spike decreased TLR-2 frequency in non-switched B-cells subset by patients with the TT genotypes (rs3804099 and rs3804100). Mononuclear cells from two groups of patients were stimulated for 24 h with spike protein (1 µg/mL) or spike + LPS (1 µg/mL). An unstimulated condition was included as a control stimulation (Unstimulated). (<b>A</b>) Representative dot plots show the B -cells subsets distribution based on CD27 and IgD expression as naive (IgD + CD27 −), non-switched (IgD + CD27+), or switched (IgD -CD27+). Analysis of TLR-4+ B -cells subsets frequencies for (<b>B</b>) naïve, (<b>C</b>) non-switched, and (<b>D</b>) switched. Data were represented as median and IQR values. The Kruskal -Wallis test performed statistical comparisons, * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01. Blue squares are used for the reference group, and red circles for the allele C carriers’ group.</p>
Full article ">Figure 3
<p>Activated B-cell subsets do not change the frequency of TLR-2+ when stimulated. Mononuclear cells from two groups of patients were stimulated for 24 h with spike protein (1 µg/mL) or spike + LPS (1 µg/mL). An unstimulated condition was included as a control stimulation (unstimulated). (<b>A</b>) Representative dot plots show the distribution of activated B-cell subsets based on IgM and CD69 expression. The frequency of activated B-cell subsets positive to TLR-4 was analyzed; thus, TLR-4+ in (<b>B</b>) naïve, (<b>C</b>) non-switched, and (<b>D</b>) switched are shown. Data are represented as median and IQR values. The Kruskal–Wallis test performed statistical comparisons, * <span class="html-italic">p</span> &lt; 0.05. Blue squares are used for the reference group, and red circles for the allele C carriers’ group.</p>
Full article ">Figure 4
<p>The TLR-2 frequencies in activated CD8-T cells decreased in patients with the TT genotypes (rs3804099 and rs3804100). Mononuclear cells from two groups of patients were stimulated for 24 h with spike protein (1 µg/mL) or spike + LPS (1 µg/mL). An unstimulated condition was included as a control stimulation (unstimulated). (<b>A</b>) Representative dot plots show the CD8+ T-cell based on CD3 and CD8 expression. (<b>B</b>) Frequency of total CD8+ T-cell and TLR-4+CD8+ T cell. (<b>C</b>) Representative dot plots show the CD69 expression in the CD8+ T-cell gate. (<b>D</b>) Frequency of CD69+CD8+ T-cell, TLR-4+CD69+CD8+ T cell. Data were represented as median and IQR values. The Kruskal-Wallis test performed statistical comparisons, * <span class="html-italic">p</span> &lt; 0.05. Blue squares are used for the reference group, and red circles for the allele C carriers’ group.</p>
Full article ">Figure 5
<p>The C allele (rs3804099 or rs3804100) does not modify the secretion of inflammatory or cytotoxic cytokines by PBMCs. Mononuclear cells from two groups of patients were stimulated for 24 h with spike protein (1 µg/mL) or spike + LPS (1 µg/mL each one). An unstimulated condition was included as a control stimulation (unstimulated). The cytotoxic LEGENDplex<sup>TM</sup> panel assessed culture supernatants for nine protein markers. Data are represented as median and IQR values. The Kruskal–Wallis test performed statistical comparisons, * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01. Blue squares are used for the reference group, and red circles for the allele C carriers’ group.</p>
Full article ">
14 pages, 4647 KiB  
Article
Impacts of Fruit Frosting Coverage on Postharvest Softening of Prunes under Vibration Stress
by Wanting Chen, Kuanbo Cui, Lili Jin, Menghan Bai, Ohaer Pazilijiang, Rui Tian and Junjie Ma
Foods 2024, 13(19), 3197; https://doi.org/10.3390/foods13193197 - 8 Oct 2024
Viewed by 790
Abstract
The surface of prune fruit has a thick layer of frosting, which is easily damaged and lost during prunes harvest or postharvest handling, and there is no clear information on the effect of prune surface frost on postharvest storage quality. To investigate the [...] Read more.
The surface of prune fruit has a thick layer of frosting, which is easily damaged and lost during prunes harvest or postharvest handling, and there is no clear information on the effect of prune surface frost on postharvest storage quality. To investigate the effect of fruit frosting on the softening of prune fruits during storage under vibration stress, prunes were divided into three grades according to fruit frosting in this study and were vibrated for 8 h at a frequency of 5 Hz at 4 °C; then, samples were selected once every 8 d. The results showed that the heavy fruit frosting (HFF) group maintained higher hardness (21.47%), L* (20.85%), and total soluble solids (12.79%) levels at the end of storage and inhibited cell wall-modifying enzyme activities (polygalacturonase, pectin methylesterase, glycosidase, β-glucosidase, and cellulase) compared to frosting-less fruit (FF) group. This group also showed improved expression of key cell wall-modification genes (ADPG2, PME31, CESA1, BGAL3, XTH33, BGLU41) as well as chelate-soluble pectin (72.11%), Na2CO3-soluble pectin (42.83%), and cellulose (36.89%) solubilization and maintained lower water-soluble pectin (34.23%). Microscopic observations showed that the fruit frosting could delay the dissolution of pectin components and protect the cell wall structure. In summary, fruit frosting can effectively inhibit fruit softening and maintain fruit quality. Full article
(This article belongs to the Section Food Packaging and Preservation)
Show Figures

Figure 1

Figure 1
<p>Changes in fruit color (<span class="html-italic">L</span>*, <span class="html-italic">a</span>*, <span class="html-italic">b</span>*) (<b>A</b>–<b>C</b>), firmness (<b>D</b>), TSS (<b>E</b>), TA (<b>F</b>), weight loss (<b>G</b>), and cell membrane permeability (<b>H</b>) during storage in three groups with different degrees of frost. The vertical line represents the standard deviation of the mean. Within the same time period, different letters indicate statistical significance between groups <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">Figure 2
<p>Indicates changes in the cell wall polysaccharide content of prune fruit, WSP (<b>A</b>), CSP (<b>B</b>), NSP (<b>C</b>), and cellulose content (<b>D</b>). The vertical line represents the standard deviation of the mean. Within the same time period, different letters indicate statistical significance between groups; <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">Figure 3
<p>Changes in cell wall-degrading enzyme activity during storage: PG (<b>A</b>), PME (<b>B</b>), <span class="html-italic">β</span>-Glu (<b>C</b>), XET (<b>D</b>), <span class="html-italic">β</span>-GAL (<b>E</b>), CEL (<b>F</b>). The vertical line represents the standard deviation of the mean. Within the same time period, different letters indicate statistical significance between groups; <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">Figure 4
<p>Changes in cell wall-degrading enzyme-related genes during storage: <span class="html-italic">ADPG2</span> (<b>A</b>), <span class="html-italic">PME31</span> (<b>B</b>), <span class="html-italic">XTH33</span> (<b>C</b>), <span class="html-italic">BGAL3</span> (<b>D</b>), <span class="html-italic">BGLU41</span> (<b>E</b>), and <span class="html-italic">CESA1</span> (<b>F</b>). The vertical line represents the standard deviation of the mean. Within the same time period, different letters indicate statistical significance between groups; <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">Figure 5
<p>Transmission electron microscopy (TEM) images at 0 d after the end of vibration. ML: middle lamella CW: cell wall CM: cell membrane. HFF group (<b>A</b>,<b>B</b>), LFF group (<b>C</b>,<b>D</b>), FF group (<b>E</b>,<b>F</b>).</p>
Full article ">Figure 6
<p>Ultrastructure of prune tissue on day 24 of storage. ML: middle lamella. CW: cell wall. CM: cell membrane. ICS: cell gap. HFF group (<b>A</b>,<b>B</b>); LFF group (<b>C</b>,<b>D</b>); FF group (<b>E</b>,<b>F</b>).</p>
Full article ">Figure 7
<p>Ultrastructure of prune tissue on day 56 of storage. ML: middle lamella. CW: cell wall. CM: cell membrane. ICS: cell gap. HFF group (<b>A</b>,<b>B</b>); LFF group (<b>C</b>,<b>D</b>); FF group (<b>E</b>,<b>F</b>).</p>
Full article ">
26 pages, 6450 KiB  
Article
High-Gain Multi-Band Koch Fractal FSS Antenna for Sub-6 GHz Applications
by Atul Varshney and Duygu Nazan Gençoğlan
Appl. Sci. 2024, 14(19), 9022; https://doi.org/10.3390/app14199022 - 6 Oct 2024
Viewed by 932
Abstract
This study introduces a novel antenna based on the binary operation of a modified circular patch in conjunction with the Koch fractal. The antenna is intended for applications in the sub-6 GHz band, partial C-band, and X-band. The low-cost antenna is fabricated on [...] Read more.
This study introduces a novel antenna based on the binary operation of a modified circular patch in conjunction with the Koch fractal. The antenna is intended for applications in the sub-6 GHz band, partial C-band, and X-band. The low-cost antenna is fabricated on a 1.6-mm-thick FR-4 substrate. A frequency-selective surface (FSS) is used to overcome the decreased values of the gain and bandwidth due to the fractal operations. The introduced split ring resonator (SRR) and the antenna substrate dimension reduction reduce the bandwidth and antenna gain. The air gap between the FSS and the antenna not only enhances the antenna gain but also controls the frequency tuning at the design frequency. The antenna size is miniaturized to 36.67%. A monopole antenna ground loaded with an SRR results in improved closest tuning (3.44 GHz) near the design frequency. The antenna achieves a peak gain of 9.37 dBi in this band. The FSS-based antenna results in a 4.65 dBi improvement in the gain value with the FSS. The measured and simulated plots exhibit an excellent match with each other in all three frequency bands at 2.96–4.72 GHz. These bands cover Wi-MAX (3.5 GHz), sub-6 GHz n77 (3300–3800 MHz), n78 (3300–4200 MHz), and approximately n79 (4400–4990 MHz), in addition to C-band applications. Full article
(This article belongs to the Special Issue Antenna Design and Microwave Engineering)
Show Figures

Figure 1

Figure 1
<p>Koch fractal principle.</p>
Full article ">Figure 2
<p>Development of Koch fractal iteration 0 stage.</p>
Full article ">Figure 3
<p>Fractal antenna patch development: (<b>a</b>) iteration 0, (<b>b</b>) iteration 1, and (<b>c</b>) iteration 2.</p>
Full article ">Figure 4
<p>Frequency-selective surface: (<b>a</b>) FSS structure and (<b>b</b>) equivalent circuit of FSS.</p>
Full article ">Figure 5
<p>Step-by-step design development.</p>
Full article ">Figure 6
<p>Koch fractal antenna (<b>a</b>) with FSS; (<b>b</b>) side view; (<b>c</b>) top patch, bottom ground, and FSS view; and (<b>d</b>) antenna 3D model.</p>
Full article ">Figure 7
<p>Split ring resonator (SRR) structure designed at 3.5 GHz.</p>
Full article ">Figure 8
<p>Effects of iterations.</p>
Full article ">Figure 9
<p>Effects of reduced ground and SRR loading.</p>
Full article ">Figure 10
<p>Miniaturization process.</p>
Full article ">Figure 11
<p>FSS loading effect on miniaturized Koch fractal antenna: (<b>a</b>) frequency tuning and gain enhancement and (<b>b</b>) effect of air gap on resonance frequency and cumulative effective permittivity.</p>
Full article ">Figure 12
<p>SRR loading effect on FSS miniaturized Koch fractal antenna.</p>
Full article ">Figure 13
<p>FSS loading effect on miniaturized Koch fractal antenna: (<b>a</b>) antenna radiator (top view), (<b>b</b>) antenna ground (bottom view), (<b>c</b>) FSS structure, and (<b>d</b>) antenna prototype model.</p>
Full article ">Figure 13 Cont.
<p>FSS loading effect on miniaturized Koch fractal antenna: (<b>a</b>) antenna radiator (top view), (<b>b</b>) antenna ground (bottom view), (<b>c</b>) FSS structure, and (<b>d</b>) antenna prototype model.</p>
Full article ">Figure 14
<p>Simulated vs. measured reflection coefficients: (<b>a</b>) without FSS and (<b>b</b>) with FSS.</p>
Full article ">Figure 15
<p>Simulated vs. measured radiation patterns in E-plane and H-plane at (<b>a</b>) 3.62 GHz, (<b>b</b>) 7.82 GHz, and (<b>c</b>) 10.58 GHz.</p>
Full article ">Figure 15 Cont.
<p>Simulated vs. measured radiation patterns in E-plane and H-plane at (<b>a</b>) 3.62 GHz, (<b>b</b>) 7.82 GHz, and (<b>c</b>) 10.58 GHz.</p>
Full article ">Figure 16
<p>Simulated vs. measured antenna gains.</p>
Full article ">Figure 17
<p>Current density distribution of the proposed fractal antenna: (<b>a</b>) current density without FSS at 3.5 GHz, (<b>b</b>) current density with FSS at 3.5 GHz, (<b>c</b>) current density with FSS at 3.62 GHz, (<b>d</b>) current density with FSS at 7.82 GHz, and (<b>e</b>) current density with FSS at 10.58 GHz.</p>
Full article ">Figure 17 Cont.
<p>Current density distribution of the proposed fractal antenna: (<b>a</b>) current density without FSS at 3.5 GHz, (<b>b</b>) current density with FSS at 3.5 GHz, (<b>c</b>) current density with FSS at 3.62 GHz, (<b>d</b>) current density with FSS at 7.82 GHz, and (<b>e</b>) current density with FSS at 10.58 GHz.</p>
Full article ">Figure 17 Cont.
<p>Current density distribution of the proposed fractal antenna: (<b>a</b>) current density without FSS at 3.5 GHz, (<b>b</b>) current density with FSS at 3.5 GHz, (<b>c</b>) current density with FSS at 3.62 GHz, (<b>d</b>) current density with FSS at 7.82 GHz, and (<b>e</b>) current density with FSS at 10.58 GHz.</p>
Full article ">
17 pages, 924 KiB  
Article
Legendre Polynomial Fitting-Based Permutation Entropy Offers New Insights into the Influence of Fatigue on Surface Electromyography (sEMG) Signal Complexity
by Meryem Jabloun, Olivier Buttelli and Philippe Ravier
Entropy 2024, 26(10), 831; https://doi.org/10.3390/e26100831 - 30 Sep 2024
Viewed by 563
Abstract
In a recently published work, we introduced local Legendre polynomial fitting-based permutation entropy (LPPE) as a new complexity measure for quantifying disorder or randomness in time series. LPPE benefits from the ordinal pattern (OP) concept and incorporates a natural, aliasing-free multiscaling effect by [...] Read more.
In a recently published work, we introduced local Legendre polynomial fitting-based permutation entropy (LPPE) as a new complexity measure for quantifying disorder or randomness in time series. LPPE benefits from the ordinal pattern (OP) concept and incorporates a natural, aliasing-free multiscaling effect by design. The current work extends our previous study by investigating LPPE’s capability to assess fatigue levels using both synthetic and real surface electromyography (sEMG) signals. Real sEMG signals were recorded during biceps brachii fatiguing exercise maintained at 70% of maximal voluntary contraction (MVC) until exhaustion and were divided into four consecutive temporal segments reflecting sequential stages of exhaustion. As fatigue levels rise, LPPE values can increase or decrease significantly depending on the selection of embedding dimensions. Our analysis reveals two key insights. First, using LPPE with limited embedding dimensions shows consistency with the literature. Specifically, fatigue induces a decrease in sEMG complexity measures. This observation is supported by a comparison with the existing multiscale permutation entropy (MPE) variant, that is, the refined composite downsampling (rcDPE). Second, given a fixed OP length, higher embedding dimensions increase LPPE’s sensitivity to low-frequency components, which are notably present under fatigue conditions. Consequently, specific higher embedding dimensions appear to enhance the discrimination of fatigue levels. Thus, LPPE, as the only MPE variant that allows a practical exploration of higher embedding dimensions, offers a new perspective on fatigue’s impact on sEMG complexity, complementing existing MPE approaches. Full article
(This article belongs to the Special Issue Ordinal Pattern-Based Entropies: New Ideas and Challenges)
Show Figures

Figure 1

Figure 1
<p>Normalised sEMG PSDs: (<b>a</b>) Simulated PSDs calculated using (<a href="#FD6-entropy-26-00831" class="html-disp-formula">6</a>) and parameter pairs <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>f</mi> <mi>l</mi> </msub> <mo>;</mo> <msub> <mi>f</mi> <mi>h</mi> </msub> <mo>)</mo> </mrow> </semantics></math> in Hz: (49;146.5) denoted as <math display="inline"><semantics> <msub> <mi>w</mi> <mn>1</mn> </msub> </semantics></math>, (49;117) as <math display="inline"><semantics> <msub> <mi>w</mi> <mn>2</mn> </msub> </semantics></math>, (39;98) as <math display="inline"><semantics> <msub> <mi>w</mi> <mn>3</mn> </msub> </semantics></math>, and (29;58.5) as <math display="inline"><semantics> <msub> <mi>w</mi> <mn>4</mn> </msub> </semantics></math>; 50 Monte Carlo realisations of synthetic sEMG signals based on filtered white Gaussian noise are generated for each parameter pair. (<b>b</b>) Average normalised PSD estimates of sEMG signals acquired under fatigue conditions <math display="inline"><semantics> <msub> <mi>W</mi> <mn>1</mn> </msub> </semantics></math> to <math display="inline"><semantics> <msub> <mi>W</mi> <mn>4</mn> </msub> </semantics></math>, as described in <a href="#sec3dot2-entropy-26-00831" class="html-sec">Section 3.2</a>, and subsampled by a factor of 10. (<b>c</b>) Average normalised PSD estimates of these same sEMG signals after mean removal. All PSD estimates were calculated using an AR model of order 30 [<a href="#B55-entropy-26-00831" class="html-bibr">55</a>].</p>
Full article ">Figure 2
<p>LPPE with (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math> and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math>, applied to synthetic sEMG signals generated as described in <a href="#sec3dot1-entropy-26-00831" class="html-sec">Section 3.1</a>. (<b>c</b>,<b>d</b>) show a zoom performed on (<b>a</b>) and (<b>b</b>), respectively. The sampling frequency is 1000 Hz.</p>
Full article ">Figure 3
<p>Mean rcDPE with (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math> and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math> applied to real sEMG signals acquired as described in <a href="#sec3dot2-entropy-26-00831" class="html-sec">Section 3.2</a>. The rcDPE is insensitive to the mean removal of the acquired sEMG signals.</p>
Full article ">Figure 4
<p>LPPE with <math display="inline"><semantics> <mrow> <mi>d</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math> applied to real sEMG signals, acquired under fatigue condition from 10 subjects as described in <a href="#sec3dot2-entropy-26-00831" class="html-sec">Section 3.2</a> and subsampled by a factor <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>. The sampling frequency is <math display="inline"><semantics> <msub> <mi>F</mi> <mi>s</mi> </msub> </semantics></math> = 1000 Hz.</p>
Full article ">Figure 5
<p>LPPE with <span class="html-italic">d</span> = 5 applied to centred (mean removal) real sEMG signals acquired under fatigue condition from 10 subjects as described in <a href="#sec3dot2-entropy-26-00831" class="html-sec">Section 3.2</a>. The sampling frequency is <math display="inline"><semantics> <msub> <mi>F</mi> <mi>s</mi> </msub> </semantics></math> = 1000 Hz.</p>
Full article ">Figure 6
<p>Mean LPPE with (<b>a</b>) <span class="html-italic">d</span> = 4 and (<b>b</b>) <span class="html-italic">d</span> = 5 using the 10 real sEMG signals acquired as described in <a href="#sec3dot2-entropy-26-00831" class="html-sec">Section 3.2</a>, after mean removal and subsampling by <span class="html-italic">M</span> = 10. (<b>c</b>,<b>d</b>) are a zoom of (<b>a</b>) and (<b>b</b>), respectively. The sampling frequency is <math display="inline"><semantics> <msub> <mi>F</mi> <mi>s</mi> </msub> </semantics></math> = 1000 Hz.</p>
Full article ">Figure 7
<p>Oscillations in detrended LPPE of real sEMG signals obtained using the data-driven decomposition method, VMD, and their respective spectra with <span class="html-italic">d</span> = 4. The sampling frequency is <math display="inline"><semantics> <msub> <mi>F</mi> <mi>s</mi> </msub> </semantics></math> = 1000 Hz.</p>
Full article ">Figure 8
<p>Relative absolute difference of (<b>a</b>) LPPEs and (<b>b</b>) rcDPE of real sEMG signals using pairwise comparisons of the fatigue steps <math display="inline"><semantics> <msub> <mi>W</mi> <mn>1</mn> </msub> </semantics></math>-<math display="inline"><semantics> <msub> <mi>W</mi> <mn>2</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>W</mi> <mn>2</mn> </msub> </semantics></math>-<math display="inline"><semantics> <msub> <mi>W</mi> <mn>3</mn> </msub> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>W</mi> <mn>3</mn> </msub> </semantics></math>-<math display="inline"><semantics> <msub> <mi>W</mi> <mn>4</mn> </msub> </semantics></math>. The sampling frequency is 1000 Hz. The relative absolute difference is calculated using <math display="inline"><semantics> <mrow> <mn>100</mn> <mo>×</mo> <mstyle scriptlevel="0" displaystyle="true"> <mfrac> <mrow> <mrow> <mo>|</mo> </mrow> <msub> <mi>y</mi> <mi>i</mi> </msub> <mo>−</mo> <msub> <mi>y</mi> <mi>j</mi> </msub> <mrow> <mo>|</mo> </mrow> </mrow> <mrow> <mrow> <mo>|</mo> </mrow> <msub> <mi>y</mi> <mi>i</mi> </msub> <mo>+</mo> <msub> <mi>y</mi> <mi>j</mi> </msub> <mrow> <mo>|</mo> </mrow> </mrow> </mfrac> </mstyle> </mrow> </semantics></math>, where <math display="inline"><semantics> <msub> <mi>y</mi> <mi>i</mi> </msub> </semantics></math> is LPPE or rcDPE of step <math display="inline"><semantics> <msub> <mi>W</mi> <mi>i</mi> </msub> </semantics></math>.</p>
Full article ">Figure A1
<p>LPPE of pure tones: (<b>a</b>) LPPE shapes are shown for two sinusoids of frequencies 20 Hz and 110 Hz, with <span class="html-italic">d</span> = 5. (<b>b</b>) Segment length <span class="html-italic">L</span> corresponding to LPPE maxima represented as a function of the frequency of the pure tone. Two additional curves are provided: (-.) the inverse of the frequency, and (:) this curve scaled by a factor of 0.57 as an approximation. The sampling frequency is 1000 Hz.</p>
Full article ">Figure A2
<p>LPPE of sinusoids embedded in an additive Gaussian noise: (<b>a</b>) rcDPE and (<b>b</b>) LPPE with SNR = 0 dB. (<b>c</b>,<b>d</b>) are LPPE plotted as a function of embedding dimension × the sinusoid frequency at SNR 0 and 5 dB.</p>
Full article ">
27 pages, 10763 KiB  
Article
Cascaded Frequency Selective Surfaces with Matryoshka Geometry for Ultra-Wideband Bandwidth
by Ianes Coutinho, Francisco Madeiro and Wamberto Queiroz
Appl. Sci. 2024, 14(19), 8603; https://doi.org/10.3390/app14198603 - 24 Sep 2024
Viewed by 512
Abstract
The purpose of this paper is to present cascaded frequency selective surfaces (FSSs) with matryoshka geometry to increase the effective bandwidth. We carry out an analysis of the influence of the spacing between the surfaces on the FSSs frequency response. The application involves [...] Read more.
The purpose of this paper is to present cascaded frequency selective surfaces (FSSs) with matryoshka geometry to increase the effective bandwidth. We carry out an analysis of the influence of the spacing between the surfaces on the FSSs frequency response. The application involves a two-layer cascaded FSS, one as a band-stop filter with a matryoshka geometry and the other as a band-pass filter with inverted or negative matryoshka geometry. With this framework, it is possible to extend an ultra-wideband (UWB) of a bandwidth up to 2 GHz in the 1.8 GHz to 3.8 GHz range with just two layers and an air gap of 12 mm, in addition to a bandwidth of 2 GHz to 3.2 GHz with a smaller 4 mm gap between layers. Full article
Show Figures

Figure 1

Figure 1
<p>Example of frequency selective surface.</p>
Full article ">Figure 2
<p>Development of a matryoshka geometry from (<b>a</b>) a pair of concentric square loops to (<b>b</b>) the opened and patched square loops to (<b>c</b>) the matryoshka geometry.</p>
Full article ">Figure 3
<p>Matryoshka geometries and equivalent circuits for (<b>a</b>) a pair of concentric square loop geometry and (<b>b</b>) a square matryoshka geometry.</p>
Full article ">Figure 4
<p>Matryoshka geometry independent of polarization with three square rings.</p>
Full article ">Figure 5
<p>Fabricated FSSs: (<b>a</b>) shows the FSSs with matryoshka geometry, and (<b>b</b>) shows the FSS with inverted matryoshka geometry.</p>
Full article ">Figure 6
<p>Cascaded FSS on measurement window.</p>
Full article ">Figure 7
<p>Acrylic supports used for spacing between FSSs.</p>
Full article ">Figure 8
<p>Photograph of the experimental setup.</p>
Full article ">Figure 9
<p>Setup spatial coordinates on the FSS to identify the horizontal and vertical polarizations.</p>
Full article ">Figure 10
<p>Cascaded FSS with different gaps. (<b>a</b>) The FSSs with a spacing of one acrylic support, 2 mm wide. (<b>b</b>) Spacing of 8 mm using two supports of 3 mm and one of 2 mm. (<b>c</b>) Spacing of 20 mm using 6 acrylic supports: two of 5 mm, two of 3 mm, and two of 2 mm.</p>
Full article ">Figure 11
<p>Simulated frequency response of the FSS with band-reject matryoshka geometry for incident horizontal and vertical polarizations.</p>
Full article ">Figure 12
<p>Simulated frequency response of the FSS with band-pass matryoshka geometry for incident horizontal and vertical polarizations.</p>
Full article ">Figure 13
<p>Electric current distribution of the FSS with band-pass matryoshka geometry.</p>
Full article ">Figure 14
<p>Electric current distribution of the FSS with band-reject matryoshka geometry.</p>
Full article ">Figure 15
<p>Experimental frequency response of the FSS with band-reject matryoshka geometry for incident horizontal polarization.</p>
Full article ">Figure 16
<p>Experimental frequency response of the FSS with band-reject matryoshka geometry for incident vertical polarization.</p>
Full article ">Figure 17
<p>Experimental frequency response of the FSS with band-pass matryoshka geometry for incident horizontal <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> polarization.</p>
Full article ">Figure 18
<p>Experimental frequency response of the FSS with band-pass matryoshka geometry for incident wave with <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> polarization and different values for the incidence angle.</p>
Full article ">Figure 19
<p>Simulated frequency response of a cascaded FSS with matryoshka geometry and different values of spacing between the layers.</p>
Full article ">Figure 20
<p>Electric current distribution of the cascaded FSS with 12 mm spacing between layers.</p>
Full article ">Figure 21
<p>Experimental frequency response of a cascade FSS with matryoshka geometry, <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> polarization for the incident wave and different spacing between the layers.</p>
Full article ">Figure 22
<p>Experimental frequency response of a cascaded matryoshka geometry for different values of spacing between the layers and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> polarization for the incident wave.</p>
Full article ">Figure 23
<p>Experimental frequency response of a cascaded matryoshka FSS with spacing between the layers equal to 4 mm and different values of the angle of incidence φ.</p>
Full article ">Figure 24
<p>Experimental frequency response of a cascaded matryoshka FSS, spacing between the layers equal to 12 mm, <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math> polarization for incident wave, and different values of the incidence angle.</p>
Full article ">Figure 25
<p>Comparison of experimental and simulated frequency responses for single layer FSS with matryoshka geometry, band-reject mode, and incident wave polarizations <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 26
<p>Comparison of experimental and simulated frequency responses for single layer FSS with matryoshka geometry, band-pass mode, and incident wave polarizations <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 27
<p>Comparison of experimental and simulated frequency responses for cascaded FSS with matryoshka geometry, gap of 4 mm between layers, and incident wave polarizations <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 28
<p>Comparison of experimental and simulated frequency responses for cascaded FSS with matryoshka geometry, gap of 8 mm between layers, and incident wave polarizations <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math>.</p>
Full article ">Figure 29
<p>Comparison of experimental and simulated frequency responses for cascaded FSS with matryoshka geometry, gap of 12 mm between layers, and incident wave polarizations <math display="inline"><semantics> <mrow> <mi>x</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>y</mi> </mrow> </semantics></math>.</p>
Full article ">
Back to TopTop