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Appl. Sci., Volume 11, Issue 4 (February-2 2021) – 621 articles

Cover Story (view full-size image): Polymeric bioresorbable stents (BRS) are designed to mitigate the side effects of traditional inert metallic stents, such as chronic inflammation and late thrombosis, but are not bioactive. To improve their biointegration, it is crucial that stents undergo autologous luminal endothelialization. Moreover, the current fabrication techniques of stents, extrusion of tubes and laser cutting, do not allow performing customizable stents addressed to patients with special needs. This article investigates the effect of different functionalization strategies onto solvent-cast poly(L-lactic acid) surfaces with the capacity to accelerate the surface endothelialization and the fabrication of 3D-printed BRS via the solvent-cast direct writing technique. View this paper
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18 pages, 468 KiB  
Article
An Empirical Investigation of Software Customization and Its Impact on the Quality of Software as a Service: Perspectives from Software Professionals
by Abdulrazzaq Qasem Ali, Abu Bakar Md Sultan, Abdul Azim Abd Ghani and Hazura Zulzalil
Appl. Sci. 2021, 11(4), 1677; https://doi.org/10.3390/app11041677 - 26 Feb 2021
Cited by 3 | Viewed by 3686
Abstract
Although customization plays a significant role in the provision of software as a service (SaaS), delivering a customizable SaaS application that reflects the tenant’s specific requirements with acceptable level of quality is a challenge. Drawing on a pr-developed software customization model for SaaS [...] Read more.
Although customization plays a significant role in the provision of software as a service (SaaS), delivering a customizable SaaS application that reflects the tenant’s specific requirements with acceptable level of quality is a challenge. Drawing on a pr-developed software customization model for SaaS quality, two fundamental objectives of this study were to determine whether different software customization approaches have direct impacts on SaaS quality, and also to assess the construct reliability and construct validity of the model. A questionnaire-based survey was used to collect data from 244 software professionals with experience in SaaS development. Structural equation modeling was employed to test the construct reliability, construct validity, and research hypotheses. The measurement model assessment suggested that the six-construct model with 39 items exhibited good construct reliability and construct validity. The findings of the structural model assessment show that all customization approaches other than the integration approach significantly influence the quality of SaaS applications. The findings also indicate that both configuration and composition approaches have positive impacts on SaaS quality, while the impacts of the other approaches are negative. The empirical assessment and evaluation of this model, which features a rich set of information, provides considerable benefits to both researchers and practitioners. Full article
(This article belongs to the Special Issue Requirements Engineering: Practice and Research)
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<p>Research model.</p>
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<p>Model fit evaluation steps in this study.</p>
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<p>Results of structural model assessment.</p>
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14 pages, 1475 KiB  
Article
Plume Divergence and Discharge Oscillations of an Accessible Low-Power Hall Effect Thruster
by Matthew Baird, Thomas Kerber, Ron McGee-Sinclair and Kristina Lemmer
Appl. Sci. 2021, 11(4), 1973; https://doi.org/10.3390/app11041973 - 23 Feb 2021
Cited by 4 | Viewed by 2664
Abstract
Hall effect thrusters (HETs) are an increasingly utilized proportion of electric propulsion devices due to their high thrust-to-power ratio. To enable an accessible research thruster, our team used inexpensive materials and simplified structures to fabricate the 44-mm-diameter Western Hall Thruster (WHT44). Anode flow, [...] Read more.
Hall effect thrusters (HETs) are an increasingly utilized proportion of electric propulsion devices due to their high thrust-to-power ratio. To enable an accessible research thruster, our team used inexpensive materials and simplified structures to fabricate the 44-mm-diameter Western Hall Thruster (WHT44). Anode flow, discharge voltage, magnet current, and cathode flow fraction (CFF) were independently swept while keeping all other parameters constant. Simultaneously, a Faraday probe was used to test plume properties at a variety of polar coordinate distances, and an oscilloscope was used to capture discharge oscillation behavior. Plasma plume divergence angle at a fixed probe distance of 4.5 thruster diameters increased with increasing anode flow, varying from 36.7° to 37.4°. Moreover, divergence angle decreased with increasing discharge voltage, magnet current, and CFF, by 0.3°, 0.2°, and 8°, respectively, over the span of the swept parameters. Generally, the thruster exhibited a strong oscillation near 90 kHz, which is higher than a similarly sized HET (20–60 kHz). The WHT44 noise frequency spectra became more broadband and the amplitude increased at a CFF of less than 1.5% and greater than 26%. Only the low flow and low voltage operating conditions showed a quiescent sinusoidal discharge current; otherwise, the discharge current probability distribution was Gaussian. This work demonstrates that the WHT44 thruster, designed for simplicity of fabrication, is a viable tool for research and academic purposes. Full article
(This article belongs to the Special Issue Plasmas for Space Propulsion)
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<p>Langmuir probe I-V traces for 44-mm-diameter Western Hall Thruster (WHT44) at 200 W and several plume locations.</p>
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<p>Experimental setup.</p>
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<p>Photograph of the (<b>a</b>) WHT44 post-test and (<b>b</b>) the WHT44 operating at the nominal operating point.</p>
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<p>Sample Faraday probe current density measurements at 10 different thruster diameters downstream (TDD) distances plotted together for the nominal 200-V, 215-W operating condition.</p>
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<p>Total ion beam current as a function of TDD at the nominal 200-V, 215-W operating condition.</p>
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<p>Divergence angle as a function of (<b>a</b>) discharge voltage, (<b>b</b>) magnet current at 4.5 TDD, (<b>c</b>) probe distance downstream at nominal operating conditions, and (d) of cathode flow fraction (CFF) at 4 TDD.</p>
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<p>Current utilization, mass utilization, and beam utilization efficiencies at a probe distance 4.5 TDD as a function of (<b>a</b>) discharge voltage, (<b>b</b>) magnet current, (<b>c</b>) CFF at 4 TDD.</p>
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<p>The mean and peak-to-peak discharge current as a function of (<b>a</b>) discharge voltage, (<b>b</b>) magnet current, and (<b>c</b>) cathode flow fraction.</p>
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<p>Discharge current as a function of time at 170 V for mass flow rates of (<b>a</b>) 1.27 mg/s, and (<b>c</b>) 1.08 mg/s. Histograms of discharge current at (<b>b</b>) 1.27 mg/s setting, and (<b>d</b>) 1.08 mg/s setting.</p>
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<p>Thruster discharge power spectral behavior for a CFF of 20.7% and: (<b>a</b>) <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>m</mi> <mo>˙</mo> </mover> <mi>a</mi> </msub> <mo>=</mo> </mrow> </semantics></math> 1.27 mg/s and <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>g</mi> </mrow> </msub> <mo>=</mo> </mrow> </semantics></math> 200 mA, (<b>b</b>) <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>m</mi> <mo>˙</mo> </mover> <mi>a</mi> </msub> <mo>=</mo> </mrow> </semantics></math> 1.08 mg/s and <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>g</mi> </mrow> </msub> <mo>=</mo> </mrow> </semantics></math> 200 mA, and (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>m</mi> <mo>˙</mo> </mover> <mi>a</mi> </msub> <mo>=</mo> </mrow> </semantics></math> 1.27 mg/s at a 200 V discharge.</p>
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<p>Thruster discharge power spectral behavior for the 170 V discharge, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>m</mi> <mo>˙</mo> </mover> <mi>a</mi> </msub> <mo>=</mo> </mrow> </semantics></math> 1.27 mg/s, and <math display="inline"><semantics> <mrow> <msub> <mi>I</mi> <mrow> <mi>m</mi> <mi>a</mi> <mi>g</mi> </mrow> </msub> <mo>=</mo> </mrow> </semantics></math> 200 mA condition as a function of CFF.</p>
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17 pages, 1571 KiB  
Article
An Immersive Serious Game for the Behavioral Assessment of Psychological Needs
by Irene Alice Chicchi Giglioli, Lucia A. Carrasco-Ribelles, Elena Parra, Javier Marín-Morales and Mariano Alcañiz Raya
Appl. Sci. 2021, 11(4), 1971; https://doi.org/10.3390/app11041971 - 23 Feb 2021
Cited by 5 | Viewed by 3411
Abstract
Motivation is an essential component in mental health and well-being. In this area, researchers have identified four psychological needs that drive human behavior: attachment, self-esteem, orientation and control, and maximization of pleasure and minimization of distress. Various self-reported scales and interviews tools have [...] Read more.
Motivation is an essential component in mental health and well-being. In this area, researchers have identified four psychological needs that drive human behavior: attachment, self-esteem, orientation and control, and maximization of pleasure and minimization of distress. Various self-reported scales and interviews tools have been developed to assess these dimensions. Despite the validity of these, they are showing limitations in terms of abstractation and decontextualization and biases, such as social desirability bias, that can affect responses veracity. Conversely, virtual serious games (VSGs), that are games with specific purposes, can potentially provide more ecologically valid and objective assessments than traditional approaches. Starting from these premises, the aim of this study was to investigate the feasibility of a VSG to assess the four personality needs. Sixty subjects participated in five VSG sessions. Results showed that the VSG was able to recognize attachment, self-esteem, and orientation and control needs with a high accuracy, and to a lesser extent maximization of pleasure and minimization of distress need. In conclusion, this study showed the feasibility to use a VSG to enhance the assessment of psychological behavioral-based need, overcoming biases presented by traditional assessment. Full article
(This article belongs to the Special Issue Applications of Virtual, Augmented, and Mixed Reality)
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<p>Consistency model.</p>
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<p>Example of a virtual agent with a secureattachment style.</p>
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<p>Crew mood state according to valence and arousal dimensions that participant could improve at the end of each session.</p>
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<p>Main study variables and their outputs.</p>
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<p>Machine learning strategy followed for each algorithm in <a href="#applsci-11-01971-t005" class="html-table">Table 5</a> and each subscale to predict. Feature selection was made and validated by cross-validation (CV). When the best features were obtained, hyperparameter tuning was carried out, also validated with CV. With the best features and hyperparameters, modelling was done, and metrics were obtained by CV.</p>
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19 pages, 31780 KiB  
Article
Impact of the Sub-Grid Scale Turbulence Model in Aeroacoustic Simulation of Human Voice
by Martin Lasota, Petr Šidlof, Manfred Kaltenbacher and Stefan Schoder
Appl. Sci. 2021, 11(4), 1970; https://doi.org/10.3390/app11041970 - 23 Feb 2021
Cited by 10 | Viewed by 2699
Abstract
In an aeroacoustic simulation of human voice production, the effect of the sub-grid scale (SGS) model on the acoustic spectrum was investigated. In the first step, incompressible airflow in a 3D model of larynx with vocal folds undergoing prescribed two-degree-of-freedom oscillation was simulated [...] Read more.
In an aeroacoustic simulation of human voice production, the effect of the sub-grid scale (SGS) model on the acoustic spectrum was investigated. In the first step, incompressible airflow in a 3D model of larynx with vocal folds undergoing prescribed two-degree-of-freedom oscillation was simulated by laminar and Large-Eddy Simulations (LES), using the One-Equation and Wall-Adaptive Local-Eddy (WALE) SGS models. Second, the aeroacoustic sources and the sound propagation in a domain composed of the larynx and vocal tract were computed by the Perturbed Convective Wave Equation (PCWE) for vowels [u:] and [i:]. The results show that the SGS model has a significant impact not only on the flow field, but also on the spectrum of the sound sampled 1 cm downstream of the lips. With the WALE model, which is known to handle the near-wall and high-shear regions more precisely, the simulations predict significantly higher peak volumetric flow rates of air than those of the One-Equation model, only slightly lower than the laminar simulation. The usage of the WALE SGS model also results in higher sound pressure levels of the higher harmonic frequencies. Full article
(This article belongs to the Special Issue Computational Methods and Engineering Solutions to Voice II)
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<p>CFD computational domain in mid–coronal section and details of the CFD mesh near the vocal and ventricular folds. The z-normal boundaries are denoted <math display="inline"><semantics> <msub> <mi mathvariant="sans-serif">Γ</mi> <mrow> <mi>f</mi> <mi>r</mi> <mi>o</mi> <mi>n</mi> <mi>t</mi> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi mathvariant="sans-serif">Γ</mi> <mrow> <mi>b</mi> <mi>a</mi> <mi>c</mi> <mi>k</mi> </mrow> </msub> </semantics></math>.</p>
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<p>Flow rates during four oscillation cycles and glottal surface.</p>
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<p>Velocity magnitude (<b>left</b>) and pressure distribution (<b>right</b>) along the glottal mid–line in three time instants <math display="inline"><semantics> <msub> <mi>t</mi> <mi>N</mi> </msub> </semantics></math> (<b>top</b>), <math display="inline"><semantics> <msub> <mi>t</mi> <mi>C</mi> </msub> </semantics></math> (<b>middle</b>) and <math display="inline"><semantics> <msub> <mi>t</mi> <mi>O</mi> </msub> </semantics></math> (<b>bottom</b>). Gray background denotes the region of the moving vocal folds.</p>
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<p>Velocity fields [<math display="inline"><semantics> <mrow> <mi mathvariant="normal">m</mi> <mspace width="0.166667em"/> <msup> <mi mathvariant="normal">s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>] in mid–sagittal plane in three time instants.</p>
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<p>Vorticity fields <math display="inline"><semantics> <mfenced open="|" close="|"> <mi mathvariant="bold">ω</mi> </mfenced> </semantics></math> in mid–coronal plane in range (0, 30,000) [<math display="inline"><semantics> <msup> <mi mathvariant="normal">s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </semantics></math>].</p>
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<p>Turbulent viscosity <math display="inline"><semantics> <msub> <mi>ν</mi> <mi>t</mi> </msub> </semantics></math> [<math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">m</mi> <mn>2</mn> </msup> <mspace width="0.166667em"/> <msup> <mi mathvariant="normal">s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>] in mid–coronal plane.</p>
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<p>Turbulent viscosity <math display="inline"><semantics> <msub> <mi>ν</mi> <mi>t</mi> </msub> </semantics></math> [<math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">m</mi> <mn>2</mn> </msup> <mspace width="0.166667em"/> <msup> <mi mathvariant="normal">s</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math>] in mid–coronal plane.</p>
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<p>Geometry, mesh and probe location for computational aeroacoustic (CAA) simulations—vocal tracts [u:] (<b>top</b>) and [i:] (<b>bottom</b>). Red—larynx, purple—vocal tract, green—PML.</p>
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<p>Spatial distribution of sound sources [<math display="inline"><semantics> <mrow> <mi>kg</mi> <mspace width="0.166667em"/> <msup> <mi mathvariant="normal">m</mi> <mrow> <mo>−</mo> <mn>6</mn> </mrow> </msup> <mspace width="0.166667em"/> <msup> <mi mathvariant="normal">s</mi> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math>] in mid–coronal plane at four frequencies (as a result of Fast Fourier Transform).</p>
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<p>Acoustic sound spectra from the numerical simulation of vocalization of [u:] (<b>left</b>) and [i:] (<b>right</b>) at monitoring point “MIC 1”.</p>
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19 pages, 6203 KiB  
Article
Climate Change Impacts on Salt Marsh Blue Carbon, Nitrogen and Phosphorous Stocks and Ecosystem Services
by Bernardo Duarte, João Carreiras and Isabel Caçador
Appl. Sci. 2021, 11(4), 1969; https://doi.org/10.3390/app11041969 - 23 Feb 2021
Cited by 15 | Viewed by 4187
Abstract
Salt marshes are valuable ecosystems, as they provide food, shelter, and important nursery areas for fish and macroinvertebrates, and a wide variety of ecosystem services for human populations. These ecosystem services heavily rely on the floristic composition of the salt marshes with different [...] Read more.
Salt marshes are valuable ecosystems, as they provide food, shelter, and important nursery areas for fish and macroinvertebrates, and a wide variety of ecosystem services for human populations. These ecosystem services heavily rely on the floristic composition of the salt marshes with different species conferring different service values and different adaptation and resilience capacities towards ecosystem stressors. Blue carbon, nitrogen, and phosphorous stocks are no exception to this, and rely on the interspecific differences in the primary production metabolism and physiological traits. Furthermore, these intrinsic physiological characteristics also modulate the species response to any environmental stressor, such as the ones derived from ongoing global changes. This will heavily shape transitional ecosystem services, with significant changes of the ecosystem value of the salt marshes in terms of cultural, provisioning, regulating, and supporting ecosystem services, with a special emphasis on the possible alterations of the blue carbon, nitrogen, and phosphorous stocks retained in these key environments. Thus, the need to integrate plant physiological characteristics and feedbacks towards the expected climate change-driven stressors becomes evident to accurately estimate the ecosystem services of the salt marsh community, and transfer these fundamental services into economic assets, for a fluid communication of the ecosystems value to stakeholders, decision and policy makers, and environmental management entities. Full article
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<p>Atlantic and Mediterranean estuarine systems along the Portuguese coast that were analyzed.</p>
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<p>Species relative abundance in the six transitional systems.</p>
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<p>Canonical analysis of principal components of the species relative coverage in the different salt marshes evaluated in the six transitional systems.</p>
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<p>Present-day values for supporting (<b>a</b>), provisioning (<b>b</b>), regulating (<b>c</b>), and cultural (<b>d</b>) ecosystem services in the six transitional systems.</p>
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<p>Blue carbon (<b>a</b>), nitrogen (<b>b</b>), and phosphorous (<b>c</b>) annual sequestration by the most abundant species in the salt marshes of the six transitional systems.</p>
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<p>Species relative abundance (%) in the salt marshes of the transitional systems analyzed under present-day conditions and in the five climate change scenarios considered.</p>
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<p>Species relative abundance (%) in the salt marshes of the transitional systems analyzed under present-day conditions and in the five climate change scenarios considered.</p>
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<p>Blue carbon (<b>a</b>), nitrogen (<b>b</b>), and phosphorous (<b>c</b>) annual sequestration by the most abundant species in the salt marshes of the six transitional systems under present-day conditions and in the five climate change scenarios considered.</p>
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<p>Ecosystem annual values and relative change toward the present conditions under expectable climate change scenarios (CO<sub>2</sub>—rising atmospheric CO<sub>2</sub>; SLR—prolonged submersion; Temp—temperature rise; Osmotic—osmotic stress) of the salt marshes of the six transitional systems considered: (<b>a</b>)—Sado estuary, (<b>b</b>)—Mondego estuary, (<b>c</b>)—Mira estuary, (<b>d</b>)—Aveiro coastal lagoon, (<b>e</b>)—Tagus estuary, (<b>f</b>)—Ria Formosa coastal lagoon).</p>
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<p>Ecosystem annual values and relative change toward the present conditions under expectable climate change scenarios (CO<sub>2</sub>—rising atmospheric CO<sub>2</sub>; SLR—prolonged submersion; Temp—temperature rise; Osmotic—osmotic stress) of the salt marshes of the six transitional systems considered: (<b>a</b>)—Sado estuary, (<b>b</b>)—Mondego estuary, (<b>c</b>)—Mira estuary, (<b>d</b>)—Aveiro coastal lagoon, (<b>e</b>)—Tagus estuary, (<b>f</b>)—Ria Formosa coastal lagoon).</p>
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18 pages, 4346 KiB  
Article
Effects of Tooth Surface Crack Propagation on Meshing Stiffness and Vibration Characteristic of Spur Gear System
by Lan-tao Yang, Yi-min Shao, Wei-wei Jiang, Lu-ke Zhang, Li-ming Wang and Jin Xu
Appl. Sci. 2021, 11(4), 1968; https://doi.org/10.3390/app11041968 - 23 Feb 2021
Cited by 13 | Viewed by 2354
Abstract
Tooth surface cracks are considered as the early stage of the development of tooth surface spalling failure. Understanding the excitation mechanism of surface cracks has a great significance in the early diagnosis of spalling faults. However, there are few studies on the dynamic [...] Read more.
Tooth surface cracks are considered as the early stage of the development of tooth surface spalling failure. Understanding the excitation mechanism of surface cracks has a great significance in the early diagnosis of spalling faults. However, there are few studies on the dynamic modelling of surface cracks, and the influence mechanism of surface cracking on the dynamic characteristics of a gear system is also not yet clear during its propagation process. Thus, an analytical calculation model of the meshing stiffness of gear with tooth surface crack is developed. Then, a dynamic model of a spur gear system with six degrees of freedom (DOF) is established based on the proposed surface crack calculation model. The effects of surface crack propagation on the meshing stiffness and dynamic characteristics of gear system are investigated. The results show that the side frequencies of dynamic transmission error (DTE) are more sensitive than those of the acceleration responses during the surface crack propagation, which is more favorable to the surface crack fault diagnosis. Compared to the traditional spalling fault model, the proposed model can accurately characterize the dynamic characteristics of a gear system with the early spalling defect. Full article
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<p>Geometric parameters of tooth surface crack.</p>
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<p>The cantilever beam model of gear with tooth surface crack fault.</p>
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<p>Meshing positions of gear tooth with surface crack fault: (<b>a</b>) left of the fault zone, (<b>b</b>) above the fault zone, (<b>c</b>) right of the fault zone.</p>
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<p>Dynamical model of spur gear system with six DOF.</p>
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<p>Effects of surface crack length on meshing stiffness: (<b>a</b>) single-tooth pair, (<b>b</b>) double-tooth pairs.</p>
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<p>Effects of surface crack width on meshing stiffness: (<b>a</b>) single-tooth pair, (<b>b</b>) double-tooth pairs.</p>
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<p>Effects of surface crack depth on meshing stiffness: (<b>a</b>) single-tooth pair, (<b>b</b>) double-tooth pairs.</p>
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<p>Effects of crack parameters on the DTE: (<b>a</b>) length, (<b>b</b>) width, (<b>c</b>) depth.</p>
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<p>Effects of crack parameters on the acceleration responses: (<b>a</b>) length, (<b>b</b>) width, (<b>c</b>) depth.</p>
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<p>Schematic of surface crack propagation.</p>
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<p>Effects of surface crack propagation on meshing stiffness: (<b>a</b>) single-tooth pair, (<b>b</b>) double-tooth pairs.</p>
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<p>Effects of surface crack propagation on time domain of DTE.</p>
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<p>DTE spectra of different fault cases: (<b>a</b>) case #1, (<b>b</b>) case #2, (<b>c</b>) case #3, (<b>d</b>) case #4.</p>
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<p>DTE spectra of different fault cases: (<b>a</b>) case #1, (<b>b</b>) case #2, (<b>c</b>) case #3, (<b>d</b>) case #4.</p>
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<p>Effects of surface crack propagation on time domain of acceleration response.</p>
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<p>Acceleration spectra of different fault cases: (<b>a</b>) case #1, (<b>b</b>) case #2, (<b>c</b>) case #3, (<b>d</b>) case #4.</p>
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<p>BAR of different fault cases: (<b>a</b>) DTE, (<b>b</b>) acceleration.</p>
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12 pages, 1708 KiB  
Article
Diagnosis of Sepsis by AI-Aided Proteomics Using 2D Electrophoresis Images of Patient Serum Incorporating Transfer Learning for Deep Neural Networks
by Nobuhiro Hayashi, Yoshihide Sawada, Kei Ujimoto, Syunta Yamaguchi, Yoshikuni Sato, Takahiro Miki, Toru Nakada and Toshiaki Iba
Appl. Sci. 2021, 11(4), 1967; https://doi.org/10.3390/app11041967 - 23 Feb 2021
Cited by 2 | Viewed by 3061
Abstract
An accuracy of ≥98% was achieved in sepsis diagnosis using serum samples from 30 sepsis patients and 68 healthy individuals and a high-performance two-dimensional polyacrylamide gel electrophoresis (HP-2D-PAGE) method developed here with deep learning and transfer learning algorithms. In this method, small-scale target [...] Read more.
An accuracy of ≥98% was achieved in sepsis diagnosis using serum samples from 30 sepsis patients and 68 healthy individuals and a high-performance two-dimensional polyacrylamide gel electrophoresis (HP-2D-PAGE) method developed here with deep learning and transfer learning algorithms. In this method, small-scale target domain data, which are collected to achieve our objective, are inputted directly into a model constructed with source domain data which are collected from a different domain from the target; target vectors are estimated with the outputted target domain data and applied to refine the model. Recognition performance of small-scale data is improved by reusing all layers, including the output layers of the neural network. Proteomics is generally considered the ultimate bio-diagnostic technique and provides extremely high information density in its two-dimensional electrophoresis images, but extracting the data has posed a basic problem. The present study is expected to solve that problem and will be an important breakthrough for practical utilization and future perspectives of proteomics in clinics after evaluation in clinical settings. Full article
(This article belongs to the Special Issue AI Proteomics: Technologies and Their Potential)
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<p>Outline of our proposed method. (<b>A</b>): Training the deep neural network (DNN) using the source domain data, (<b>B</b>): estimating the relation vectors of each target domain label, (<b>C</b>): tuning all parameters using pairs of target domain data and relation vectors.</p>
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<p>Relationship between relation vectors and hyperplane. (<b>A</b>): The margin using the average vector as the relation vector, and (<b>B</b>) represents the margin using our method.</p>
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<p>Examples of two-dimensional gel electrophoresis (2D-GE) images. X and Y-axes represent isoelectric points (pI) and molecular weights (Da), and black regions represent protein spots. Upper left: sepsis. Upper right: non-sepsis. Lower: source domain 2D-GE images. The position of the same protein is approximately the same for each patient because each axis represents an absolute physical quantity. Our previously developing technology has incremented the accuracy<sup>1</sup>. However, as shown in this figure, it is difficult for even an expert to detect valid spots for classifying sepsis. Thus, we directly inputted 2D-GE images in the DNN.</p>
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<p>Visualization of weight. Red circles show examples of currently known valid spots. Blue frame represents the position of the weight image. 1: Transthyretin [<a href="#B21-applsci-11-01967" class="html-bibr">21</a>], 2: Ceruloplasmin [<a href="#B22-applsci-11-01967" class="html-bibr">22</a>], 3: Prothrombin [<a href="#B23-applsci-11-01967" class="html-bibr">23</a>].</p>
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15 pages, 1101 KiB  
Article
Review on Quality Control Methods in Metal Additive Manufacturing
by Jungeon Lee, Hyung Jun Park, Seunghak Chai, Gyu Ri Kim, Hwanwoong Yong, Suk Joo Bae and Daeil Kwon
Appl. Sci. 2021, 11(4), 1966; https://doi.org/10.3390/app11041966 - 23 Feb 2021
Cited by 33 | Viewed by 5313
Abstract
Metal additive manufacturing (AM) has several similarities to conventional metal manufacturing, such as welding and cladding. During the manufacturing process, both metal AM and welding experience repeated partial melting and cooling, referred to as deposition. Owing to deposition, metal AM and welded products [...] Read more.
Metal additive manufacturing (AM) has several similarities to conventional metal manufacturing, such as welding and cladding. During the manufacturing process, both metal AM and welding experience repeated partial melting and cooling, referred to as deposition. Owing to deposition, metal AM and welded products often share common product quality issues, such as layer misalignment, dimensional errors, and residual stress generation. This paper comprehensively reviews the similarities in quality monitoring methods between metal AM and conventional metal manufacturing. It was observed that a number of quality monitoring methods applied to metal AM and welding are interrelated; therefore, they can be used complementarily with each other. Full article
(This article belongs to the Special Issue Additive Manufacturing and System: From Methods to Applications)
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<p>Schematic diagram of the PBF process; (<b>a</b>) a schematic model and (<b>b</b>) a schematic side view of PBF process.</p>
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<p>Schematic diagram of the DED and welding processes using (<b>a</b>) a coaxial nozzle and (<b>b</b>) a material feed nozzle.</p>
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<p>Conceptual representation of (<b>a</b>) common anomalies and (<b>b</b>) defects in both metal AM and welding.</p>
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<p>Schematic diagram of a single-cladding track: <b><span class="html-italic">H</span></b> is track height, <b><span class="html-italic">D</span></b> is track depth, <b><span class="html-italic">W</span></b> is track width, and <b><span class="html-italic">α</span></b> is cladding angle.</p>
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11 pages, 1237 KiB  
Article
Region-of-Interest-Based Cardiac Image Segmentation with Deep Learning
by Raul-Ronald Galea, Laura Diosan, Anca Andreica, Loredana Popa, Simona Manole and Zoltán Bálint
Appl. Sci. 2021, 11(4), 1965; https://doi.org/10.3390/app11041965 - 23 Feb 2021
Cited by 16 | Viewed by 3855
Abstract
Despite the promising results obtained by deep learning methods in the field of medical image segmentation, lack of sufficient data always hinders performance to a certain degree. In this work, we explore the feasibility of applying deep learning methods on a pilot dataset. [...] Read more.
Despite the promising results obtained by deep learning methods in the field of medical image segmentation, lack of sufficient data always hinders performance to a certain degree. In this work, we explore the feasibility of applying deep learning methods on a pilot dataset. We present a simple and practical approach to perform segmentation in a 2D, slice-by-slice manner, based on region of interest (ROI) localization, applying an optimized training regime to improve segmentation performance from regions of interest. We start from two popular segmentation networks, the preferred model for medical segmentation, U-Net, and a general-purpose model, DeepLabV3+. Furthermore, we show that ensembling of these two fundamentally different architectures brings constant benefits by testing our approach on two different datasets, the publicly available ACDC challenge, and the imATFIB dataset from our in-house conducted clinical study. Results on the imATFIB dataset show that the proposed approach performs well with the provided training volumes, achieving an average Dice Similarity Coefficient of the whole heart of 89.89% on the validation set. Moreover, our algorithm achieved a mean Dice value of 91.87% on the ACDC validation, being comparable to the second best-performing approach on the challenge. Our approach provides an opportunity to serve as a building block of a computer-aided diagnostic system in a clinical setting. Full article
(This article belongs to the Special Issue Soft Computing in Applied Sciences and Industrial Applications)
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<p>The flow-diagram that supports our approach. Before the training process starts, two scaling steps and a cropping step are performed: each original image slice is resized to <math display="inline"><semantics> <mrow> <mn>512</mn> <mo>×</mo> <mn>512</mn> </mrow> </semantics></math> and, from this enlarged image, a ROI is cropped (by using the corresponding ground-truth) and resized to <math display="inline"><semantics> <mrow> <mn>224</mn> <mo>×</mo> <mn>224</mn> </mrow> </semantics></math>. The segmentation model is trained on these processed images and a set of masks are predicted for each input. Finally, the masks are re-scaled to the original dimensions and re-inserted in the original image.</p>
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<p>Sample results from the imATFIB validation set (Red—ground truth, Yellow—model prediction). (<b>A</b>) Input image, (<b>B</b>) Label mask, (<b>C</b>) All Ensemble model (<math display="inline"><semantics> <msub> <mi>M</mi> <mn>9</mn> </msub> </semantics></math>), (<b>D</b>) U-net model (<math display="inline"><semantics> <msub> <mi>M</mi> <mn>4</mn> </msub> </semantics></math>).</p>
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13 pages, 4798 KiB  
Article
Design and Validation of an Adjustable Large-Scale Solar Simulator
by Daniele Colarossi, Eleonora Tagliolini, Paolo Principi and Roberto Fioretti
Appl. Sci. 2021, 11(4), 1964; https://doi.org/10.3390/app11041964 - 23 Feb 2021
Cited by 15 | Viewed by 2673
Abstract
This work presents an adjustable large-scale solar simulator based on metal halide lamps. The design procedure is described with regards to the construction and spatial arrangement of the lamps and the designed optical system. Rotation and translation of the lamp array allow setting [...] Read more.
This work presents an adjustable large-scale solar simulator based on metal halide lamps. The design procedure is described with regards to the construction and spatial arrangement of the lamps and the designed optical system. Rotation and translation of the lamp array allow setting the direction and the intensity of the luminous flux on the horizontal plane. To validate the built model, irradiance nonuniformity and temporal instability tests were carried out assigning Class A, B, or C for each test, according to the International Electrotechnical Commission (IEC) standards requirements. The simulator meets the Class C standards on a 200 × 90 cm test plane, Class B on 170 × 80 cm, and Class A on 80 × 40 cm. The temporal instability returns Class A results for all the measured points. Lastly, a PV panel is characterized by tracing the I–V curve under simulated radiation, under outdoor natural sunlight, and with a numerical method. The results show a good approximation. Full article
(This article belongs to the Section Energy Science and Technology)
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<p>Metal halide lamp structure (mm).</p>
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<p>Detail of a lamp mounted under the parabolic mirror (<b>a</b>) and the theoretical representation (<b>b</b>).</p>
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<p>Lamp array size. CAD reconstruction (mm) (<b>a</b>) and real image (<b>b</b>).</p>
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<p>3D view of the whole system: vertical flux configuration (<b>a</b>) and horizontal flux configuration (<b>b</b>).</p>
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<p>Detail of a side box.</p>
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<p>Nonuniformity test (the shadows are due to the photo).</p>
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<p>Layout of the test area.</p>
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<p>Spatial distribution of irradiation values on the test surface (W/m<sup>2</sup>).</p>
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<p>Long-term instability test results.</p>
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<p>Variable resistor scheme [<a href="#B24-applsci-11-01964" class="html-bibr">24</a>].</p>
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<p>Procedure for the determination of the shape S parameter [<a href="#B25-applsci-11-01964" class="html-bibr">25</a>].</p>
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<p>Comparison of indoor, outdoor, and numerical I–V curve.</p>
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15 pages, 3193 KiB  
Article
Robust Long-Term Visual Object Tracking via Low-Rank Sparse Learning for Re-Detection
by Shanshan Luo, Baoqing Li, Xiaobing Yuan and Huawei Liu
Appl. Sci. 2021, 11(4), 1963; https://doi.org/10.3390/app11041963 - 23 Feb 2021
Cited by 2 | Viewed by 2136
Abstract
The Discriminative Correlation Filter (DCF) has been universally recognized in visual object tracking, thanks to its excellent accuracy and high speed. Nevertheless, these DCF-based trackers perform poorly in long-term tracking. The reasons include the following aspects—first, they have low adaptability to significant appearance [...] Read more.
The Discriminative Correlation Filter (DCF) has been universally recognized in visual object tracking, thanks to its excellent accuracy and high speed. Nevertheless, these DCF-based trackers perform poorly in long-term tracking. The reasons include the following aspects—first, they have low adaptability to significant appearance changes in long-term tracking and are prone to tracking failure; second, these trackers lack a practical re-detection module to find the target again after tracking failure. In our work, we propose a new long-term tracking strategy to solve these issues. First, we make the best of the static and dynamic information of the target by introducing the motion features to our long-term tracker and obtain a more robust tracker. Second, we introduce a low-rank sparse dictionary learning method for re-detection. This re-detection module can exploit a correlation among these training samples and alleviate the impact of occlusion and noise. Third, we propose a new reliability evaluation method to model an adaptive update, which can switch expediently between the tracking module and the re-detection module. Massive experiments demonstrate that our proposed approach has an obvious improvement in precision and success rate over these state-of-the-art trackers. Full article
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<p>The framework of our proposed tracker. Our method mainly consists of tracking and re-detection modules. After the tracking module has processed the input frames, we perform a reliability estimation for the tracking result, update the tracking model adaptively, and decide whether re-detection is needed for the current result. If the re-detection process is adopted, we perform a reliability estimation for the re-detection result and decide whether the re-detected result can replace the originally detected result re-detection is needed for the current result.</p>
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<p>Illustration of the MBH. (<b>a</b>,<b>b</b>) Reference images at time t − 1 and t. (<b>c</b>) Horizontal motion boundary histograms. (<b>d</b>) Vertical motion boundary histograms.</p>
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<p>Peak sidelobe ratio (PSR) values significantly decrease when tracking results become less reliable (the green box represents the ground-truth target location, and the red color denotes the tracker outputs).</p>
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<p>The values of <math display="inline"><semantics> <mrow> <mi>S</mi> <mi>m</mi> <mi>o</mi> <mi>o</mi> <mi>t</mi> <msub> <mi>h</mi> <mi>t</mi> </msub> </mrow> </semantics></math> significantly decrease when tracking results become less reliable (the green box represents the ground-truth target location, and the red color denotes the tracker outputs).</p>
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<p>Precision plots (<b>left</b>) and Success plots (<b>right</b>) of OPE on OTB-2013 dataset. The values in the legend indicate the quantitative comparisons of distance precision at the threshold of 20 pixels and overlap success rate at the conventional thresholds of 0.5 <math display="inline"><semantics> <mfenced separators="" open="(" close=")"> <mi>I</mi> <mi>O</mi> <mi>U</mi> <mo>&gt;</mo> <mn>0.5</mn> </mfenced> </semantics></math>.</p>
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<p>Precision plots (<b>left</b>) and Success plots (<b>right</b>) of OPE on OTB-2013 dataset. The values in the legend indicate the quantitative comparisons of distance precision at the threshold of 20 pixels and overlap success rate at the conventional thresholds of 0.5 <math display="inline"><semantics> <mfenced separators="" open="(" close=")"> <mi>I</mi> <mi>O</mi> <mi>U</mi> <mo>&gt;</mo> <mn>0.5</mn> </mfenced> </semantics></math>.</p>
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<p>Precision plots (<b>left</b>) and Success plots (<b>right</b>) of OPE on OTB-2013 dataset. The values in the legend indicate the quantitative comparisons of distance precision at the threshold of 20 pixels and overlap success rate at the conventional thresholds of 0.5 <math display="inline"><semantics> <mfenced separators="" open="(" close=")"> <mi>I</mi> <mi>O</mi> <mi>U</mi> <mo>&gt;</mo> <mn>0.5</mn> </mfenced> </semantics></math>.</p>
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<p>Success plots over 11 challenging attributes on OTB-2013 dataset. The values in the legend indicate the overlap success rate at the conventional thresholds of 0.5 <math display="inline"><semantics> <mfenced separators="" open="(" close=")"> <mi>I</mi> <mi>O</mi> <mi>U</mi> <mo>&gt;</mo> <mn>0.5</mn> </mfenced> </semantics></math>.</p>
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<p>Qualitative comparison of our proposed tracker with state-of-the-art trackers on the box, freeman, singer, ironman and panda videos, under out of view, occlusion, scale variation, out-of-plane rotation and low resolution, respectively.</p>
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<p>Precision plots (<b>left</b>) and Success plots (<b>right</b>) of OPE on OTB-2015 dataset. The values in the legend indicate the quantitative comparisons of distance precision at the threshold of 20 pixels and overlap success rate at the conventional thresholds of 0.5 <math display="inline"><semantics> <mfenced separators="" open="(" close=")"> <mi>I</mi> <mi>O</mi> <mi>U</mi> <mo>&gt;</mo> <mn>0.5</mn> </mfenced> </semantics></math>.</p>
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<p>Precision plots (<b>left</b>) and success plots (<b>right</b>) of OPE on Temple color-128 dataset. The values in the legend indicate the quantitative comparisons of distance precision at the threshold of 20 pixels and overlap success rate at the conventional thresholds of 0.5 <math display="inline"><semantics> <mfenced separators="" open="(" close=")"> <mi>I</mi> <mi>O</mi> <mi>U</mi> <mo>&gt;</mo> <mn>0.5</mn> </mfenced> </semantics></math>.</p>
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11 pages, 3128 KiB  
Article
Formulation and Thermomechanical Characterization of Functional Hydrogels Based on Gluten Free Matrices Enriched with Antioxidant Compounds
by Vanesa Sanz, Herminia Domínguez and María Dolores Torres
Appl. Sci. 2021, 11(4), 1962; https://doi.org/10.3390/app11041962 - 23 Feb 2021
Cited by 3 | Viewed by 2060
Abstract
Native starch from potatoes and hybrid carrageenans from the red alga Mastocarpus stellatus have been used as gluten-free gelling matrices to obtain functional hydrogels. The enrichment of gelling matrices with antioxidant compounds from natural sources is an increasing market trend. In this context, [...] Read more.
Native starch from potatoes and hybrid carrageenans from the red alga Mastocarpus stellatus have been used as gluten-free gelling matrices to obtain functional hydrogels. The enrichment of gelling matrices with antioxidant compounds from natural sources is an increasing market trend. In this context, this work is aimed at the formulation and thermo-rheological characterization of functional hydrogels using potato starch from agro-industrial waste and kappa–iota hybrid carrageenans extracted from the above seaweed, enriched with antioxidant compounds from different agro-industrial products, such as waste coming from the pruning of green tea and two varieties of hops used in the brewing industry. Environmentally friendly technologies such as microwave hydrodiffusion and gravity, microwave-assisted extraction, ultrasounds and autohydrolysis were used for the recovery of antioxidant compounds. The results point out that functional hydrogels based on potato starch and hybrid carrageenans with a wide range of viscoelastic features can be achieved, with the particularity of being suitable for people with celiac disease. The incorporation of selected antioxidant extracts from vegetable by-products involved the drop (about tenfold) of the viscous and elastic properties of the formulated gels. The sequential combination of the above treatments could even further expand the thermo-rheological properties of formulated hydrogels, with potential application in functional foodstuffs and novel gluten-free goods. Full article
(This article belongs to the Special Issue Gluten-Free Foods)
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<p>General scheme of gluten-free hydrogel production. T = temperature; t = time; CSB = <span class="html-italic">Camellia sinensis</span> branches; CSL = <span class="html-italic">Camellia sinensis</span> leaves; PH and NH = industrial hops; MAE = microwave-assisted extraction; AH = autohydrolysis); MHG = microwave hydrodiffusion and gravity; US = ultrasounds.</p>
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<p>Cooling profiles for (<b>a</b>) the control matrices prepared with the hybrid carrageenan (C1) or potato starch (S1), as well as (<b>b</b>) the corresponding gelling temperatures (<span class="html-italic">Tg</span>) for all formulated matrices. Note that in this and subsequent plots, error bars were not presented when they were smaller than the symbol size.</p>
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<p>Viscoelastic features of the proposed matrices, prepared with (<b>a</b>–<b>c</b>) hybrid carrageenan or (<b>d</b>) potato starch in the presence of extract from <span class="html-italic">Camellia sinensis</span> agricultural wastes and industrial hops (see <a href="#applsci-11-01962-t001" class="html-table">Table 1</a> for coding). Note here that C1 and S1 are the controls prepared with hybrid carrageenan and potato starch, respectively.</p>
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<p>Viscoelastic features of the proposed matrices, prepared with (<b>a</b>–<b>c</b>) hybrid carrageenan or (<b>d</b>) potato starch in the presence of extract from <span class="html-italic">Camellia sinensis</span> agricultural wastes and industrial hops (see <a href="#applsci-11-01962-t001" class="html-table">Table 1</a> for coding). Note here that C1 and S1 are the controls prepared with hybrid carrageenan and potato starch, respectively.</p>
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<p>Heating profiles for (<b>a</b>) control matrices prepared with the hybrid carrageenan (C1) or potato starch (S1), as well as (<b>b</b>) the corresponding melting temperatures T<sub>m</sub> for all formulated matrices. Note than in this and subsequent plots, error bars were not presented whenever they were smaller than the symbol size.</p>
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<p>Texture parameters in terms of (<b>a</b>) firmness, (<b>b</b>) adhesiveness, (<b>c</b>) cohesiveness and (<b>d</b>) springiness for the proposed matrices prepared with hybrid carrageenan or potato starch in the presence of selected extracts (E1–E7; see <a href="#applsci-11-01962-t001" class="html-table">Table 1</a>). The controls prepared with hybrid carrageenan (C1) and potato starch (S1) were also included.</p>
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<p>Texture parameters in terms of (<b>a</b>) firmness, (<b>b</b>) adhesiveness, (<b>c</b>) cohesiveness and (<b>d</b>) springiness for the proposed matrices prepared with hybrid carrageenan or potato starch in the presence of selected extracts (E1–E7; see <a href="#applsci-11-01962-t001" class="html-table">Table 1</a>). The controls prepared with hybrid carrageenan (C1) and potato starch (S1) were also included.</p>
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<p>Color parameters for proposed matrices prepared with (<b>a</b>) hybrid carrageenan or potato starch in the presence of the selected extracts (E1–E7; see <a href="#applsci-11-01962-t001" class="html-table">Table 1</a>) compared with the controls (C1 and S1). The gray and black bars in the plot (<b>b</b>) correspond to the a* and b* parameters, respectively.</p>
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18 pages, 27429 KiB  
Article
Vibration Isolation of a Surveillance System Equipped in a Drone with Mode Decoupling
by Yun-Ho Shin, Donggeun Kim, Seho Son, Ji-Wan Ham and Ki-Yong Oh
Appl. Sci. 2021, 11(4), 1961; https://doi.org/10.3390/app11041961 - 23 Feb 2021
Cited by 3 | Viewed by 3199
Abstract
Vibration isolation with mode decoupling plays a crucial role in the design of an intelligent robotic system. Specifically, a coupled multi-degree-of-freedom (multi-DOF) model accurately predicts responses of system dynamics; hence, it is useful for vibration isolation and control with mode decoupling. This study [...] Read more.
Vibration isolation with mode decoupling plays a crucial role in the design of an intelligent robotic system. Specifically, a coupled multi-degree-of-freedom (multi-DOF) model accurately predicts responses of system dynamics; hence, it is useful for vibration isolation and control with mode decoupling. This study presents a vibration isolation method with mode decoupling based on system identification, including a coupled multi-DOF model to design intelligent robotic systems. Moreover, the entire procedure is described, including the derivation of the governing equation of the coupled multi-DOF model, estimation of the frequency response function, and parameter estimation using least squares approximation. Furthermore, the suggested methods were applied for a mobile surveillance system suffering from resonances with mode coupling; it made the monitoring performance of the surveillance camera deteriorate. The resonance problem was mitigated by installing vibration isolators, but limited to eliminate the coupling effects of natural frequency deterioration performances of vibration isolation. More seriously, system identification with a simple decoupled model limits the prediction of this phenomenon. Hence, it is difficult to enhance the performance of vibration isolators. In contrast, the presented method can accurately predict the vibration phenomenon and plays a critical role in vibration isolation. Therefore, dynamic characteristics were predicted based on a vibration isolator using the coupled three-DOF model, and a final suggestion is presented here. The experiments demonstrated that the suggested configuration decreased vibration up to 98.3%, 94.0%, and 94.5% in the operational frequency range, i.e., 30–85 Hz, compared to the original surveillance system in the fore-after, side-by-side, and vertical directions, respectively. The analysis suggests that the present method and procedure effectively optimize the vibration isolation performances of a drone containing a surveillance system. Full article
(This article belongs to the Special Issue Noise Reduction and Vibration Isolation)
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<p>A free body diagram of (<b>a</b>) general and (<b>b</b>) coupled two-degree-of-freedom system.</p>
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<p>Experimental set-up for the transmissibility measurement.</p>
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<p>Measured transmissibility with modal testing: (<b>a</b>) fore-after direction, (<b>b</b>) side-by-side direction, and (<b>c</b>) vertical direction.</p>
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<p>Vibration pathway of a surveillance system in a drone: (<b>a</b>) original pathway and (<b>b</b>) proposed pathway.</p>
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<p>Configuration of selected mounts for the gimbal system.</p>
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<p>Comparison of transmissibility before and after applying mount elements: (<b>a</b>) fore-after direction, (<b>b</b>) side-by-side direction, and (<b>c</b>) vertical direction.</p>
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<p>Simulation results of the coupled three‒DOF mathematical model in (<b>a</b>) the time domain and (<b>b</b>) in the frequency domain.</p>
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<p>Optimal design of vibration isolators.</p>
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<p>Comparison of transmissibility before and after the mount design modification in (<b>a</b>) fore-after, (<b>b</b>) side-by-side, and (<b>c</b>) vertical directions.</p>
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<p>Mode shape of rigid body modes for (<b>a</b>) initial and (<b>b</b>) optimal designs from measurement and prediction.</p>
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<p>Simulation results of the coupled three‒DOF mathematical model between initial and optimal designs in (<b>a</b>) the time domain and (<b>b</b>) the frequency domain.</p>
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13 pages, 4332 KiB  
Article
Theoretical Analysis and Design of an Innovative Coil Structure for Transcranial Magnetic Stimulation
by Naming Zhang, Ziang Wang, Jinhua Shi, Shuya Ning, Yukuo Zhang, Shuhong Wang and Hao Qiu
Appl. Sci. 2021, 11(4), 1960; https://doi.org/10.3390/app11041960 - 23 Feb 2021
Cited by 1 | Viewed by 2531
Abstract
Previous research showed that pulsed functional magnetic stimulation can activate brain tissue with optimum intensity and frequency. Conventional stimulation coils are always set as a figure-8 type or Helmholtz. However, the magnetic fields generated by these coils are uniform around the target, and [...] Read more.
Previous research showed that pulsed functional magnetic stimulation can activate brain tissue with optimum intensity and frequency. Conventional stimulation coils are always set as a figure-8 type or Helmholtz. However, the magnetic fields generated by these coils are uniform around the target, and their magnetic stimulation performance still needs improvement. In this paper, a novel type of stimulation coil is proposed to shrink the irritative zone and strengthen the stimulation intensity. Furthermore, the electromagnetic field distribution is calculated and measured. Based on numerical simulations, the proposed coil is compared to traditional coil types. Moreover, the influential factors, such as the diameter and the intersection angle, are also analyzed. It was demonstrated that the proposed coil has a better performance in comparison with the figure-8 coil. Thus, this work suggests a new way to design stimulation coils for transcranial magnetic stimulation. Full article
(This article belongs to the Section Electrical, Electronics and Communications Engineering)
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<p>Principle of the transcranial magnetic stimulation (TMS).</p>
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<p>Circuit diagram of the signal generator.</p>
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<p>Framework of the TMS system including insulated gate bipolar translator (IGBT).</p>
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<p>3D model of the proposed coil and the human head.</p>
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<p>(<b>a</b>) Structures of the measurement coil and (<b>b</b>) prototype of the measurement coil.</p>
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<p>(<b>a</b>) Front view of the proposed coil, (<b>b</b>) top view of the proposed coil, and (<b>c</b>) the location of the compared plane (8 cm beyond the coil plane).</p>
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<p>The prototype of the proposed coil for TMS.</p>
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<p>Structures of the human head with multilayers.</p>
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<p>Comparison of the measurements and the simulated calculations of the magnetic flux density.</p>
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<p>Comparison of the magnetic flux density distribution between the proposed coil and the typical coils. (<b>a</b>) The proposed coil, (<b>b</b>) figure-8 quad coil, (<b>c</b>) figure-8 coil, and (<b>d</b>) round coil.</p>
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<p>Comparison of the electrical field between the four coils.</p>
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<p>Comparison of the magnetic flux density between the four coils.</p>
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<p>Comparison of the full width at half maximum (FWHM) between the four coils.</p>
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<p>Comparison of the electric fields at different stimulation depths.</p>
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<p>Comparison of FHWM between the different diameters of the little coil.</p>
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<p>Simulation of FWHM at 7 cm beyond the coil plane.</p>
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<p>Simulation of FWHM at 9 cm beyond the coil plane.</p>
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<p>Comparison of FHWM between the different intersection angles of the big-little coils.</p>
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18 pages, 16876 KiB  
Article
Data Assimilation of AOD and Estimation of Surface Particulate Matters over the Arctic
by Kyung M. Han, Chang H. Jung, Rae-Seol Park, Soon-Young Park, Sojin Lee, Markku Kulmala, Tuukka Petäjä, Grzegorz Karasiński, Piotr Sobolewski, Young Jun Yoon, Bang Young Lee, Kiyeon Kim and Hyun S. Kim
Appl. Sci. 2021, 11(4), 1959; https://doi.org/10.3390/app11041959 - 23 Feb 2021
Cited by 4 | Viewed by 3350
Abstract
In this study, more accurate information on the levels of aerosol optical depth (AOD) was calculated from the assimilation of the modeled AOD based on the optimal interpolation method. Additionally, more realistic levels of surface particulate matters over the Arctic were estimated using [...] Read more.
In this study, more accurate information on the levels of aerosol optical depth (AOD) was calculated from the assimilation of the modeled AOD based on the optimal interpolation method. Additionally, more realistic levels of surface particulate matters over the Arctic were estimated using the assimilated AOD based on the linear relationship between the particulate matters and AODs. In comparison to the MODIS observation, the assimilated AOD was much improved compared with the modeled AOD (e.g., increase in correlation coefficients from −0.15–0.26 to 0.17–0.76 over the Arctic). The newly inferred monthly averages of PM10 and PM2.5 for April–September 2008 were 2.18–3.70 μg m−3 and 0.85–1.68 μg m−3 over the Arctic, respectively. These corresponded to an increase of 140–180%, compared with the modeled PMs. In comparison to in-situ observation, the inferred PMs showed better performances than those from the simulations, particularly at Hyytiala station. Therefore, combining the model simulation and data assimilation provided more accurate concentrations of AOD, PM10, and PM2.5 than those only calculated from the model simulations. Full article
(This article belongs to the Special Issue Air Pollution II)
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<p>Bottom–up emissions of (<b>a</b>) SO<sub>2</sub>, (<b>b</b>) NO<sub>x</sub>, (<b>c</b>) EC, (<b>d</b>) OC, (<b>e</b>) PM<sub>10</sub>, and (<b>f</b>) PM<sub>2.5</sub> for the CMAQ simulations over the Arctic. The red triangles (▲) in the panel of (<b>a</b>) represent the locations of five AERONET stations of Thule, Hornsund, Andenes, Hyytiala, and Kuopio.</p>
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<p>Scatter plots between hourly <span class="html-italic">τ<sub>AERONET</sub></span> and <span class="html-italic">τ<sub>MODIS</sub></span> for (<b>a</b>) April, (<b>b</b>) May, (<b>c</b>) June, (<b>d</b>) July, (<b>e</b>) August, (<b>f</b>) September, and (<b>g</b>) all months. Their statistical analysis of R (correlation coefficient), S (slope), N (number of data), MB (mean bias), NMB (normalized mean bias, %), and IOA (index of agreement) was presented.</p>
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<p>Scatter plots and statistical analysis between <span class="html-italic">τ<sub>MODIS</sub></span> and <span class="html-italic">τ<sub>CMAQ</sub></span> and <span class="html-italic">τ<sub>assimilated</sub></span> over the entire domain for (<b>a</b>) April, (<b>b</b>) May, (<b>c</b>) June, (<b>d</b>) July, (<b>e</b>) August, and (<b>f</b>) September 2008. The statistical analysis of R (correlation coefficient), IOA (index of agreement), MB (mean bias), NMB (normalized mean bias, %), S (slope), and N (number of data) was presented.</p>
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<p>Daily mean variations of <span class="html-italic">τ<sub>AERONET</sub></span> (black closed square), <span class="html-italic">τ<sub>MODIS</sub></span> (blue open circles), <span class="html-italic">τ<sub>CMAQ</sub></span> (green lines), and <span class="html-italic">τ<sub>Assim</sub></span> (red lines) at several stations of (<b>a</b>) Thule, (<b>b</b>) Hornsund, (<b>c</b>) Andenes, (<b>d</b>) Hyytiala, and (<b>e</b>) Kuopio. Their mean values with standard deviations for April–September.</p>
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<p>Spatial maps of monthly average PMs calculated from CMAQ simulation and estimated from the linear relationship between assimilated AODs and PMs for May. (<b>a</b>) PM<sub>10</sub> and (<b>c</b>) PM<sub>2.5</sub> calculated from the CMAQ simulations. (<b>b</b>) PM<sub>10</sub> and (<b>d</b>) PM<sub>2.5</sub> estimated from the Equations (11) and (12). Daily mean variations of observed (black closed squares), modeled (green lines), and estimated (red lines) PM<sub>10</sub> at (<b>e</b>) Hyytiala and (<b>g</b>) Vindeln stations and PM<sub>2.5</sub> at (<b>f</b>) Hyytiala and (<b>h</b>) Virolahi stations. Mean values (M, μg m<sup>−3</sup>), mean bias (MB, μg m<sup>−3</sup>), Index of Agreement (IOA), and slope (S) from the observation (M<sub>in-situ</sub>), CMAQ simulation (M<sub>CMAQ</sub>), and linear estimation (M<sub>Assim</sub>) for April–September. The closed triangles in Figure (a) and (c) indicate the locations of the monitoring stations.</p>
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<p>Temporal variations of the modeled (bright and dark green lines) and estimated (red and purple lines) PM<sub>10</sub> and PM<sub>2.5</sub> at (<b>a</b>) Thule, (<b>b</b>) Hyytiala, (<b>c</b>) Hornsund, (<b>d</b>) Kuopio, (<b>e</b>) Andenes, and (<b>f</b>) the North Pole. The RD (relative differences) of PM<sub>10</sub> and PM<sub>2.5</sub> were also calculated at each station from following equations of RD<sub>PM10</sub> = (PM<sub>10,CMAQw/OI</sub>–PM<sub>10,CMAQ</sub>)/ PM<sub>10,CMAQ</sub> and RD<sub>PM2.5</sub> = (PM<sub>2.5,CMAQw/OI</sub>–PM<sub>2.5,CMAQ</sub>)/ PM<sub>2.5,CMAQ</sub>).</p>
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17 pages, 5344 KiB  
Article
Performances Assessment of Tricalcium Aluminate as an Innovative Material for Thermal Energy Storage Applications
by Fabrizio Alvaro, Elpida Piperopoulos, Luigi Calabrese, Emanuele La Mazza, Maurizio Lanza and Candida Milone
Appl. Sci. 2021, 11(4), 1958; https://doi.org/10.3390/app11041958 - 23 Feb 2021
Cited by 2 | Viewed by 2431
Abstract
In this paper, tricalcium aluminate hexahydrate (Ca3Al2O6·6H2O), thanks to its appropriate features, was assessed as an innovative, low-cost and nontoxic material for thermochemical energy storage applications. The high dehydration heat and the occurring temperature (200–300 [...] Read more.
In this paper, tricalcium aluminate hexahydrate (Ca3Al2O6·6H2O), thanks to its appropriate features, was assessed as an innovative, low-cost and nontoxic material for thermochemical energy storage applications. The high dehydration heat and the occurring temperature (200–300 °C) suggest that this material could be more effective than conventional thermochemical storage materials operating at medium temperature. For these reasons, in the present paper, Ca3Al2O6·6H2O hydration/dehydration performances, at varying synthesis procedures, were assessed. Experimentally, a co-precipitation and a solid–solid synthesis were studied in order to develop a preparation method that better provides a performing material for this specific application field. Thermal analysis (TGA, DSC) and structural characterization (XRD) were performed to evaluate the thermochemical behavior at medium temperature of the prepared materials. Furthermore, reversibility of the dehydration process and chemical stability of the obtained materials were investigated through cycling dehydration/hydration tests. The promising results, in terms of de/hydration performance and storage density (≈200 MJ/m3), confirm the potential effectiveness of this material for thermochemical energy storage applications and encourage further developments on this topic. Full article
(This article belongs to the Special Issue Materials for Thermal Energy Storage-Volume II)
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<p>Co-precipitation method flowchart.</p>
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<p>Schematized hydration procedure sequences.</p>
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<p>CA-11 diffraction patterns after 2 h calcination under static air at 500 °C, 700 °C, 900 °C and 1100 °C. (JCPDS reference cards: CaAl<sub>2</sub>O<sub>4</sub>: 01-0888; Ca<sub>12</sub>Al<sub>14</sub>O<sub>33</sub>: 09-0413; Ca<sub>3</sub>Al<sub>2</sub>O<sub>6</sub>: 38-1429; CaO: 70-4068; CaCO<sub>3</sub>: 83-1762/19-3758; AlO(OH): 78-4581).</p>
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<p>Diffraction patterns after calcination (<b>a</b>) and after hydration (<b>b</b>) for CA-32/CA-32H (red), CA-11/CA-11H (blue) and CA-S/CA-SH (orange). (JCPDS reference cards: Ca<sub>3</sub>Al<sub>2</sub>O<sub>6</sub>: 38-1429; CaO: 70-4068; Ca<sub>12</sub>Al<sub>14</sub>O<sub>33</sub>: 09-0413; Al<sub>2</sub>O<sub>3</sub>: 34-0440; Ca<sub>3</sub>Al<sub>2</sub>O<sub>6</sub>·6H<sub>2</sub>O: 24-0217; Al(OH)<sub>3</sub>: 33-0018; Ca(OH)<sub>2</sub>: 44-1481; CaCO<sub>3</sub>: 83-1762).</p>
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<p>Scanning electron microscopy (SEM) images at magnification = 100 k of calcined products CA-32 (<b>a</b>), CA-11 (<b>b</b>) and CA-S (<b>c</b>).</p>
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<p>SEM images at magnification = 100 k and punctual energy dispersive X-ray analysis (EDX) estimated Ca/Al molar ratios of hydrated products CA-32H (<b>a</b>), CA-11H (<b>b</b>) and CA-SH (<b>c</b>).</p>
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<p>CA-32H (red), CA-11H (blue) and CA-SH (orange) thermogravimetric (TG) (<b>a</b>) and differential scanning calorimetry (DSC) (<b>b</b>) curves, recorded between 150 °C and 375 °C, scan rate 10 °C/min.</p>
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<p>First dehydration/hydration cycle for CA-32H (red), CA-11H (blue) and CA-SH (orange).</p>
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<p>The 1st, 2nd, 3rd, 4th and 5th normalized dehydration/hydration curves for CA-32H (red), CA-11H (blue) and CA-SH (orange).</p>
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<p>Released heat per mass unit (<b>a</b>) and volume unit (<b>b</b>) per cycle.</p>
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<p>Diffraction pattern after the five-cycle experiment for CA-32H (red), CA-11H (blue) and CA-SH (orange). (JCPDS reference cards: Ca<sub>3</sub>Al<sub>2</sub>O<sub>6</sub>·6H<sub>2</sub>O: 24-0217; Ca<sub>12</sub>Al<sub>14</sub>O<sub>33</sub>: 09-0413; Ca(OH)<sub>2</sub>: 44-1481; Al<sub>2</sub>O<sub>3</sub>: 04-2852; CaCO<sub>3</sub>: 12-0489).</p>
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<p>SEM images, magnification = 100 k, for CA-32H (<b>a</b>), CA-11H (<b>b</b>) and CA-SH (<b>c</b>) after five dehydration-hydration cycles.</p>
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14 pages, 3866 KiB  
Article
Viability of Cupola Slag as an Alternative Eco-Binder and Filler in Concrete and Mortars
by Israel Sosa, Pablo Tamayo, Jose A. Sainz-Aja, Ana Cimentada, Juan Antonio Polanco, Jesús Setién and Carlos Thomas
Appl. Sci. 2021, 11(4), 1957; https://doi.org/10.3390/app11041957 - 23 Feb 2021
Cited by 7 | Viewed by 2356
Abstract
Obtaining new materials capable of meeting society’s demands motivates the search for new solutions that are capable of satisfying twofold requirements: respect for the environment and obtaining more durable and resistant materials. Cupola slag is a by-product generated in the process of obtaining [...] Read more.
Obtaining new materials capable of meeting society’s demands motivates the search for new solutions that are capable of satisfying twofold requirements: respect for the environment and obtaining more durable and resistant materials. Cupola slag is a by-product generated in the process of obtaining ductile iron. When the slag undergoes rapid cooling, its vitrification is favored, leaving the silica in an amorphous structure and, thus, susceptible to reacting. Through reaction, the slag can develop cementing properties and cement can consequently be partially replaced with residue, providing savings in economic and environmental costs compared to traditional hydraulic binders. In this study, the physical and chemical properties of cupola slag and its recovery process are analyzed. Mortars that incorporate traditional admixtures (fly ash and limestone filler) have been manufactured and consistency and mechanical properties have been compared with mortars that incorporate cupola slag admixture. Mortars have also been manufactured with normalized sand and with Portland cement replacements (0, 10, 20, and 30% by weight) with cupola slag, and both the consistency and the mechanical properties have been compared at 7, 28, 60, and 90 days. The results obtained show the suitability of cupola slag as a binder and as an admixture, with respect to the traditional ones, and how the mechanical properties tend to converge for all of the replacement levels characterized, for ages close to 90 days of age. Full article
(This article belongs to the Special Issue Eco-Performance of Alternative Binder Systems)
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<p>(<b>a</b>) Transport and cooling of cupola slag in trays; (<b>b</b>) detail of the stockpile at the plant.</p>
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<p>Scheme of the recovery process of cupola slag.</p>
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<p>Determination of the maximum particle size of cupola slag by SEM.</p>
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<p>Diffractogram of the cupola slag.</p>
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<p>Infrared spectrum of cupola slag.</p>
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<p>Micrograph of a cupola slag particle at two different scales: low (<b>a</b>) and high level of magnification (<b>b</b>).</p>
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<p>Mortar consistency with different cupola slag replacements.</p>
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<p>Mechanical properties of mortars with different admixtures: compressive strength (<b>a</b>); flexural strength (<b>b</b>).</p>
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<p>Compressive strength (<b>a</b>) and flexural strength (<b>b</b>) of mortars with various cement replacements by cupola slag.</p>
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3 pages, 182 KiB  
Editorial
Special Issue: The State of the Art of Thermochemical Heat Storage
by Salvatore Vasta
Appl. Sci. 2021, 11(4), 1956; https://doi.org/10.3390/app11041956 - 23 Feb 2021
Cited by 2 | Viewed by 1430
Abstract
Nowadays, thermal energy storage (TES) is gaining a crucial role in the development of highly efficient thermal energy systems [...] Full article
(This article belongs to the Section Mechanical Engineering)
22 pages, 640 KiB  
Article
Outlier Detection for Multivariate Time Series Using Dynamic Bayesian Networks
by Jorge L. Serras, Susana Vinga and Alexandra M. Carvalho
Appl. Sci. 2021, 11(4), 1955; https://doi.org/10.3390/app11041955 - 23 Feb 2021
Cited by 6 | Viewed by 3660
Abstract
Outliers are observations suspected of not having been generated by the underlying process of the remaining data. Many applications require a way of identifying interesting or unusual patterns in multivariate time series (MTS), now ubiquitous in many applications; however, most outlier detection methods [...] Read more.
Outliers are observations suspected of not having been generated by the underlying process of the remaining data. Many applications require a way of identifying interesting or unusual patterns in multivariate time series (MTS), now ubiquitous in many applications; however, most outlier detection methods focus solely on univariate series. We propose a complete and automatic outlier detection system covering the pre-processing of MTS data that adopts a dynamic Bayesian network (DBN) modeling algorithm. The latter encodes optimal inter and intra-time slice connectivity of transition networks capable of capturing conditional dependencies in MTS datasets. A sliding window mechanism is employed to score each MTS transition gradually, given the DBN model. Two score-analysis strategies are studied to assure an automatic classification of anomalous data. The proposed approach is first validated in simulated data, demonstrating the performance of the system. Further experiments are made on real data, by uncovering anomalies in distinct scenarios such as electrocardiogram series, mortality rate data, and written pen digits. The developed system proved beneficial in capturing unusual data resulting from temporal contexts, being suitable for any MTS scenario. A widely accessible web application employing the complete system is publicly available jointly with a tutorial. Full article
(This article belongs to the Collection Machine Learning in Computer Engineering Applications)
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<p>Example of a stationary first-order Markov DBN. On the left, the prior network <math display="inline"><semantics> <msup> <mi>B</mi> <mn>0</mn> </msup> </semantics></math>, for <math display="inline"><semantics> <mrow> <mi>t</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>, and on the right, the transition network <math display="inline"><semantics> <msubsup> <mi>B</mi> <mrow> <mi>t</mi> <mo>−</mo> <mn>1</mn> </mrow> <mi>t</mi> </msubsup> </semantics></math> over slices <math display="inline"><semantics> <mrow> <mi>t</mi> <mo>−</mo> <mn>1</mn> </mrow> </semantics></math> and <span class="html-italic">t</span>, for all <math display="inline"><semantics> <mrow> <mi>t</mi> <mo>≥</mo> <mn>1</mn> </mrow> </semantics></math>.</p>
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<p>Scheme of the proposed outlier detection approach comprised of four phases. Datasets formed by MTS data can be directly applied to the modeling phase when discrete; otherwise, the pre-processing phase is applied before modeling. Discrete data is delivered to the modeling phase along with parameters <span class="html-italic">p</span>, <span class="html-italic">m</span>, and <span class="html-italic">s</span> of the DBN to be modeled. Afterward, a sliding window algorithm outputs a score distribution for the data (scoring entire MTS, called subjects, or only portions of it, called transitions, depending on the user’s choice). The score-analysis phase considers two distinct strategies providing thus two possible routes for outlier disclosure.</p>
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<p>Transition networks of stationary first-order DBNs (<math display="inline"><semantics> <mrow> <mi>m</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>). The network (<b>a</b>) on the left represents the transition network of DBN <span class="html-italic">A</span> which generates normal subjects. Networks (<b>b</b>,<b>c</b>) represent DBN <span class="html-italic">B</span> and <span class="html-italic">C</span>, respectively, which generate anomalous subjects. Dashed connections represent links which are removed with respect to the normal network (<b>a</b>), while red links symbolize added dependencies. Solid black edges are connections which are common with respect to (<b>a</b>).</p>
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<p>Comparison between GMM and Tukey’s score-analysis <math display="inline"><semantics> <msub> <mi mathvariant="normal">F</mi> <mn>1</mn> </msub> </semantics></math> scores for multiple outlier ratios. Each value is an average of all 15 trials performed for each outlier ratio.</p>
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<p>Subject outlierness using METEOR (<b>a</b>) and PST approach (<b>b</b>) for a same experiment of a dataset of 10,000 subjects (<math display="inline"><semantics> <mrow> <mi>N</mi> <mo>=</mo> <mn>10</mn> <mo>,</mo> <mn>000</mn> </mrow> </semantics></math>) with 20% anomalies generated by model <span class="html-italic">C</span>. Histograms display thresholds using both score-analysis strategies. Scores below the threshold are classified as abnormal (in red) while the rest are classified as normal (in green), being the presented color representation for the Tukey’s thresholds.</p>
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<p>Mean and standard deviation of normalized ECG variables along time using a SAX alphabet <math display="inline"><semantics> <mrow> <msub> <mi>r</mi> <mi>i</mi> </msub> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> </mrow> </semantics></math>.</p>
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<p>ECG transitions arranged by subject. A non-stationary second-order tDBN (<math display="inline"><semantics> <mrow> <mi>m</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>) model with inter-slice connectivity (<math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>) is used together with Tukey’s score-analysis. Flipped subjects are associated to the highest subject ids. Data is discretized using SAX with an alphabet of 5 symbols (<math display="inline"><semantics> <mrow> <msub> <mi>r</mi> <mi>i</mi> </msub> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math> for all <span class="html-italic">i</span>). Transitions displayed in red are classified as abnormal while in green are classified as normal.</p>
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<p>Normalized values of variables <math display="inline"><semantics> <msub> <mi>X</mi> <mrow> <mi>i</mi> <mo>∈</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mn>6</mn> </mrow> </msub> </semantics></math> representing France’s mortality rates of males with ages 10, 20, 30, 40, 60 and 80, respectively, from 1841 to 1987. Each time stamp represents a year. Data is discretized with a SAX alphabet <math display="inline"><semantics> <mrow> <msub> <mi>r</mi> <mi>i</mi> </msub> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math> for all <span class="html-italic">i</span>.</p>
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<p>Transition outlierness for mortality datasets of 5 (<b>a</b>) and 6 (<b>b</b>) variables using a third-order tDBN (<math display="inline"><semantics> <mrow> <mi>m</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>) with one inter-slice connectivity per node (<math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>). Dataset (<b>a</b>) is comprised by 5 variables (<math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>5</mn> </mrow> </semantics></math>) representing mortality rates of males with ages 20, 30, 40, 60 and 80. Dataset (<b>b</b>) includes the same variables as (<b>a</b>) with the addition of a variable representing the mortality rate of males aged 10 (<math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>). Transitions are arranged by year and classified as anomalous (red) and normal (green). Major wars and epidemics which affected France in the selected years are exhibited.</p>
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13 pages, 4924 KiB  
Article
Optimal Design and Experimental Verification of Ultrasonic Cutting Horn for Ceramic Composite Material
by Mibbeum Hahn, Yeungjung Cho, Gunhee Jang and Bumcho Kim
Appl. Sci. 2021, 11(4), 1954; https://doi.org/10.3390/app11041954 - 23 Feb 2021
Cited by 6 | Viewed by 3706
Abstract
We developed and optimized a block-type ultrasonic horn that can be used for cutting hard materials. The proposed block-type sonotrode consists of an aluminum horn and a tungsten carbide blade to increase the cutting of hard materials. We designed an initial ultrasonic block [...] Read more.
We developed and optimized a block-type ultrasonic horn that can be used for cutting hard materials. The proposed block-type sonotrode consists of an aluminum horn and a tungsten carbide blade to increase the cutting of hard materials. We designed an initial ultrasonic block horn that has double slots and an exponential stepped profile. We developed a finite element model of the initial model and analyzed the characteristics of natural frequency and displacement. We formulated a DOE table and response surface to perform sensitivity analysis and analyze the correlation between the design variables and characteristics of the proposed block horn. The optimal ultrasonic block horn was derived via a multi-objective optimal design problem to maximize the amplitude uniformity of the proposed horn and frequency separation. We fabricated the optimal block horn and verified it experimentally. An ultrasonic cutting experiment was conducted to find the ultrasonic cutting force with hard ceramic composite materials. A cutting test with a conventional cutting machine under the same condition was also conducted to compare the cutting force. The proposed optimal ultrasonic cutter requires 70% less cutting force than the conventional cutter to cut a ceramic composite material and the cutting surface with the application of the proposed optimal ultrasonic cutter is much cleaner with no crack and delamination than that with the application of the conventional cutter. Full article
(This article belongs to the Special Issue Ultrasonic Transducers and Related Apparatus and Applications)
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<p>(<b>a</b>) A block-type ultrasonic cutting machine and (<b>b</b>) a sonotrode.</p>
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<p>Finite element model of the initial sonotrode.</p>
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<p>Mode shape and natural frequency of the (<b>a</b>) one lower mode (<span class="html-italic">f</span><sub>axial−1</sub>), (<b>b</b>) axial mode (<span class="html-italic">f</span><sub>axial</sub>) and (<b>c</b>) one higher mode (<span class="html-italic">f</span><sub>axial+1</sub>).</p>
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<p>Simulated displacement at the lower face of the initial block-type horn model.</p>
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<p>Design parameters of a block-type ultrasonic cutting horn.</p>
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<p>The 1st order trend lines of the frequency isolations according to the variation of the design parameters of the ultrasonic cutting horn.</p>
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<p>The 1st order trend lines of the displacement uniformity and gain according to the variation of the design parameters of the ultrasonic cutting horn.</p>
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<p>Simulated output displacement of the optimal and initial models at the horn lower face.</p>
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<p>(<b>a</b>) Experimental set-up for a displacement measurement experiment and (<b>b</b>) fabricated optimal model and measuring points.</p>
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<p>Simulated and experimental output displacement of the optimal model.</p>
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<p>Cutting experiment set-up.</p>
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<p>SEM images of cutting surface (<b>a</b>) without the application of ultrasonic vibration and (<b>b</b>) with the application of ultrasonic vibration.</p>
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15 pages, 5709 KiB  
Article
Semantic 3D Mapping from Deep Image Segmentation
by Francisco Martín, Fernando González, José Miguel Guerrero, Manuel Fernández and Jonatan Ginés
Appl. Sci. 2021, 11(4), 1953; https://doi.org/10.3390/app11041953 - 23 Feb 2021
Cited by 3 | Viewed by 3007
Abstract
The perception and identification of visual stimuli from the environment is a fundamental capacity of autonomous mobile robots. Current deep learning techniques make it possible to identify and segment objects of interest in an image. This paper presents a novel algorithm to segment [...] Read more.
The perception and identification of visual stimuli from the environment is a fundamental capacity of autonomous mobile robots. Current deep learning techniques make it possible to identify and segment objects of interest in an image. This paper presents a novel algorithm to segment the object’s space from a deep segmentation of an image taken by a 3D camera. The proposed approach solves the boundary pixel problem that appears when a direct mapping from segmented pixels to their correspondence in the point cloud is used. We validate our approach by comparing baseline approaches using real images taken by a 3D camera, showing that our method outperforms their results in terms of accuracy and reliability. As an application of the proposed algorithm, we present a semantic mapping approach for a mobile robot’s indoor environments. Full article
(This article belongs to the Special Issue Deep Image Semantic Segmentation and Recognition)
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<p>Example of deep image segmentation.</p>
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<p>Complete process of our approach.</p>
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<p>At the bottom left, we show the segmented image in RViz <a href="https://github.com/ros-visualization/rviz" target="_blank">https://github.com/ros-visualization/rviz</a> (accessed on 21 January 2021). The rest of the figure shows the corresponding point cloud. The <span class="html-italic">Boundary point</span> problem appears at the edges of the segmented areas. As seen in the point cloud, some points belong to the book whose positions are on the back wall.</p>
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<p>Example of the application of the algorithm with a simplification in 2D.</p>
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<p>Grid map of the simulated environment.</p>
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<p>Coordinate axes connections from the map frame to the sensor frame.</p>
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<p>Instantaneous perception <math display="inline"><semantics> <msub> <mi mathvariant="script">O</mi> <mi>t</mi> </msub> </semantics></math> from the 3D segmentation process.</p>
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<p>Comparison of different methods.</p>
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<p>Differences of erosion and original with the proposed method.</p>
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<p>Processing times in seconds.</p>
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<p>Mapping of a real domestic environment.</p>
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16 pages, 4090 KiB  
Article
Analysis of the Aggregate Effect on the Compressive Strength of Concrete Using Dune Sand
by Euibae Lee, Jeongwon Ko, Jaekang Yoo, Sangjun Park and Jeongsoo Nam
Appl. Sci. 2021, 11(4), 1952; https://doi.org/10.3390/app11041952 - 23 Feb 2021
Cited by 7 | Viewed by 2883
Abstract
In this study, the compressive strengths of concrete were investigated based on water content and aggregate volume fractions, comprising dune sand (DS), crushed sand (CS), and coarse aggregate (CA), for different ages. Experimental data were used to analyze the effects of the volume [...] Read more.
In this study, the compressive strengths of concrete were investigated based on water content and aggregate volume fractions, comprising dune sand (DS), crushed sand (CS), and coarse aggregate (CA), for different ages. Experimental data were used to analyze the effects of the volume fraction changes of aggregates on the compressive strength. The compressive strength of concrete increases until the volumetric DS to fine aggregate (FA) ratio (DS/FA ratio) reaches 20%, after which it decreases. The relationship between changes in compressive strength and aggregate volume fractions was analyzed considering the effect factor of each aggregate on the compressive strength and at 2 conditions: (1) 0 < DS < CS < CA and (2) 0 < CA < CS < DS. For condition (1), when the effect factor of CA = 1, those of DS and CS were within 0.04–0.83 and 0.72–0.92, respectively, for all mixtures. For condition (2), when the effect factor of DS = 1, those of CS and CA were within 0.68–0.80 and 0.02–0.79, respectively. Full article
(This article belongs to the Special Issue Advanced Fiber-Reinforced Cementitious Composites)
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Figure 1
<p>Particle-size distributions of the FAs used in this study.</p>
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<p>Particle-size distributions of the FAs used in this study.</p>
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<p>Admixture (AD) contents of the concrete mixtures used to attain the target slump.</p>
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<p>Slump/AD ratios calculated for the different concrete mixtures used in this study.</p>
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<p>Air contents of the different concrete mixtures used in this study.</p>
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<p>Compressive strengths of the different concrete mixtures according to age; (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150.</p>
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<p>Compressive strengths of the different concrete mixtures according to age; (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150.</p>
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<p>Mean compressive strengths and standard deviations of concrete mixtures with different DS/FA ratios.</p>
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<p>Mean compressive strengths and standard deviations of concrete mixtures with different water contents.</p>
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<p>Aggregate volume fractions and compressive strengths of (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150.</p>
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<p>Aggregate volume fractions and compressive strengths of (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150.</p>
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<p>Common ranges of the effect factors for (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150 mixtures at different ages (<span class="html-italic">a &lt; b &lt; c</span>, <span class="html-italic">c</span> = 1).</p>
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<p>Common ranges of the effect factors for (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150 mixtures at different ages (<span class="html-italic">a &lt; b &lt; c</span>, <span class="html-italic">c</span> = 1).</p>
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<p>Common ranges of the effect factors for the (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150 mixtures at different ages (<span class="html-italic">a &gt; b &gt; c</span>, <span class="html-italic">a</span> = 1).</p>
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<p>Common ranges of the effect factors for the (<b>a</b>) W170, (<b>b</b>) W160, and (<b>c</b>) W150 mixtures at different ages (<span class="html-italic">a &gt; b &gt; c</span>, <span class="html-italic">a</span> = 1).</p>
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20 pages, 7589 KiB  
Article
Entropy Generation and MHD Convection within an Inclined Trapezoidal Heated by Triangular Fin and Filled by a Variable Porous Media
by Ahmad Almuhtady, Muflih Alhazmi, Wael Al-Kouz, Zehba A. S. Raizah and Sameh E. Ahmed
Appl. Sci. 2021, 11(4), 1951; https://doi.org/10.3390/app11041951 - 23 Feb 2021
Cited by 10 | Viewed by 1871
Abstract
Analyses of the entropy of a thermal system that consists of an inclined trapezoidal geometry heated by a triangular fin are performed. The domain is filled by variable porosity and permeability porous materials and the working mixture is Al2O3-Cu [...] Read more.
Analyses of the entropy of a thermal system that consists of an inclined trapezoidal geometry heated by a triangular fin are performed. The domain is filled by variable porosity and permeability porous materials and the working mixture is Al2O3-Cu hybrid nanofluids. The porosity is varied exponentially with the smallest distance to the nearest wall and the permeability is depending on the particle diameter. Because of using the two energy equations model (LTNEM), sources of the entropy are entropy due to the transfer of heat of the fluid phase, entropy due to the fluid friction and entropy due to the porous phase transfer of heat. A computational domain with new coordinates (ξ,η) is created and Finite Volume Method (FVM) in case of the non-orthogonal grids is used to solve the resulting system. Various simulations for different values of the inclination angle, Hartmann number and alumina-copper concentration are carried out and the outcomes are presented in terms of streamlines, temperature, fluid friction entropy and Bejan number. It is remarkable that the increase in the inclination angle causes a diminishing of the heat transfer rate. Additionally, the irreversibility due to the temperature gradients is dominant near the heated fins, regardless of the values of the Hartmann number. Full article
(This article belongs to the Special Issue Nanofluids Application in Heat Transfer)
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<p>Schematic diagram of the current model.</p>
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<p>Mesh generation of the current geometry.</p>
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<p>Comparisons of the streamlines, isotherms, local Bejan number and local entropy generation due to heat transfer with those of Ilis et al. [<a href="#B47-applsci-11-01951" class="html-bibr">47</a>] <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>r</mi> <mo>=</mo> <mn>0.71</mn> <mo>,</mo> <mo> </mo> <mi>R</mi> <mi>a</mi> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>5</mn> </msup> <mo>,</mo> <mo> </mo> <msub> <mi>φ</mi> <mn>1</mn> </msub> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>−</mo> <mn>4</mn> </mrow> </msup> </mrow> </semantics></math>.</p>
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<p>Features of the streamlines and temperature distributions for the fluid phase and porous phase for the variation of the inclination angle <math display="inline"><semantics> <mi>γ</mi> </semantics></math> (<math display="inline"><semantics> <mrow> <mi>γ</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mi>π</mi> <mn>6</mn> </mfrac> <mo>,</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> <mo>,</mo> <mfrac> <mi>π</mi> <mn>2</mn> </mfrac> </mrow> </semantics></math>) at <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>a</mi> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>6</mn> </msup> <mo>,</mo> <mo> </mo> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo>%</mo> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> </mrow> </semantics></math>.</p>
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<p>Features of the local entropy generation due to the fluid friction and local Bejan number for the variation of the inclination angle <math display="inline"><semantics> <mi>γ</mi> </semantics></math> (<math display="inline"><semantics> <mrow> <mi>γ</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mi>π</mi> <mn>6</mn> </mfrac> <mo>,</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> <mo>,</mo> <mfrac> <mi>π</mi> <mn>2</mn> </mfrac> </mrow> </semantics></math>) at <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>a</mi> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>6</mn> </msup> <mo>,</mo> <mo> </mo> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo>%</mo> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> <mo>.</mo> </mrow> </semantics></math></p>
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<p>Features of the streamlines and temperature distribution for the fluid phase and porous phase for the variation of the Hartmann number<math display="inline"><semantics> <mrow> <mo> </mo> <mi>H</mi> <mi>a</mi> </mrow> </semantics></math> (<math display="inline"><semantics> <mrow> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mn>15</mn> <mo>,</mo> <mn>25</mn> <mo>,</mo> <mn>50</mn> <mo>,</mo> <mn>100</mn> </mrow> </semantics></math>) at <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>a</mi> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>5</mn> </msup> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo>%</mo> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>.</p>
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<p>Features of the local entropy generation due to the fluid friction and local Bejan number for the variation of the Hartmann number<math display="inline"><semantics> <mrow> <mo> </mo> <mi>H</mi> <mi>a</mi> </mrow> </semantics></math> (<math display="inline"><semantics> <mrow> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mn>15</mn> <mo>,</mo> <mn>25</mn> <mo>,</mo> <mn>50</mn> <mo>,</mo> <mn>100</mn> </mrow> </semantics></math>) at <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>a</mi> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>5</mn> </msup> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo>%</mo> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> <mo>,</mo> <mi>γ</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>.</p>
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<p>Profiles of the Nu<sub>f</sub> for the variation of the inclination angle <math display="inline"><semantics> <mi>γ</mi> </semantics></math> (<math display="inline"><semantics> <mrow> <mi>γ</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mi>π</mi> <mn>6</mn> </mfrac> <mo>,</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> <mo>,</mo> <mfrac> <mi>π</mi> <mn>2</mn> </mfrac> </mrow> </semantics></math>) at <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>a</mi> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mn>6</mn> </msup> <mo>,</mo> <mtext> </mtext> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mtext> </mtext> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mtext> </mtext> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> <mo>=</mo> <mn>1</mn> <mo>%</mo> <mo>,</mo> <mrow> <mtext> </mtext> <mi mathvariant="sans-serif">Φ</mi> </mrow> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> </mrow> </semantics></math>.</p>
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<p>Profiles of the Nu<sub>f</sub> for the variation of the Rayleigh number and nanoparticle volume fraction <math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> </mrow> </semantics></math> at<math display="inline"><semantics> <mrow> <mo> </mo> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <mi>γ</mi> <mo>=</mo> <mi>π</mi> <mo>/</mo> <mn>6</mn> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> </mrow> </semantics></math>.</p>
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<p>Profiles of the S<sub>T</sub> of the nanofluid phase in the entire domain for the variation of the Rayleigh number and nanoparticle volume fraction <math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> </mrow> </semantics></math> at<math display="inline"><semantics> <mrow> <mo> </mo> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <mi>γ</mi> <mo>=</mo> <mi>π</mi> <mo>/</mo> <mn>6</mn> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> </mrow> </semantics></math>.</p>
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<p>Profiles of the S<sub>total</sub> in the entire domain for the variation of the Rayleigh number and nanoparticle volume fraction <math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> </mrow> </semantics></math> at<math display="inline"><semantics> <mrow> <mo> </mo> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <mi>γ</mi> <mo>=</mo> <mi>π</mi> <mo>/</mo> <mn>6</mn> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> </mrow> </semantics></math>.</p>
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<p>Profiles of the S<sub>TS</sub> of the solid phase in the entire domain for the variation of the Rayleigh number and nanoparticle volume fraction <math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> </mrow> </semantics></math> at<math display="inline"><semantics> <mrow> <mo> </mo> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <mi>γ</mi> <mo>=</mo> <mi>π</mi> <mo>/</mo> <mn>6</mn> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> </mrow> </semantics></math>.</p>
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<p>Profiles of the S<sub>f</sub> in the entire domain for the variation of the Rayleigh number and nanoparticle volume fraction <math display="inline"><semantics> <mrow> <msub> <mi>ϕ</mi> <mrow> <mi>A</mi> <mi>l</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>ϕ</mi> <mrow> <mi>C</mi> <mi>u</mi> </mrow> </msub> </mrow> </semantics></math> at<math display="inline"><semantics> <mrow> <mo> </mo> <mi>H</mi> <mi>a</mi> <mo>=</mo> <mn>15</mn> <mo>,</mo> <mo> </mo> <mi>H</mi> <mo>=</mo> <mn>0.1</mn> <mo>,</mo> <mo> </mo> <mi>γ</mi> <mo>=</mo> <mi>π</mi> <mo>/</mo> <mn>6</mn> <mo>,</mo> <mo> </mo> <mi mathvariant="sans-serif">Φ</mi> <mo>=</mo> <mfrac> <mi>π</mi> <mn>3</mn> </mfrac> </mrow> </semantics></math>.</p>
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14 pages, 3303 KiB  
Article
Automatic Identification of Peanut-Leaf Diseases Based on Stack Ensemble
by Haixia Qi, Yu Liang, Quanchen Ding and Jun Zou
Appl. Sci. 2021, 11(4), 1950; https://doi.org/10.3390/app11041950 - 23 Feb 2021
Cited by 35 | Viewed by 3592
Abstract
Peanut is an important food crop, and diseases of its leaves can directly reduce its yield and quality. In order to solve the problem of automatic identification of peanut-leaf diseases, this paper uses a traditional machine-learning method to ensemble the output of a [...] Read more.
Peanut is an important food crop, and diseases of its leaves can directly reduce its yield and quality. In order to solve the problem of automatic identification of peanut-leaf diseases, this paper uses a traditional machine-learning method to ensemble the output of a deep learning model to identify diseases of peanut leaves. The identification of peanut-leaf diseases included healthy leaves, rust disease on a single leaf, leaf-spot disease on a single leaf, scorch disease on a single leaf, and both rust disease and scorch disease on a single leaf. Three types of data-augmentation methods were used: image flipping, rotation, and scaling. In this experiment, the deep-learning model had a higher accuracy than the traditional machine-learning methods. Moreover, the deep-learning model achieved better performance when using data augmentation and a stacking ensemble. After ensemble by logistic regression, the accuracy of residual network with 50 layers (ResNet50) was as high as 97.59%, and the F1 score of dense convolutional network with 121 layers (DenseNet121) was as high as 90.50. The deep-learning model used in this experiment had the greatest improvement in F1 score after the logistic regression ensemble. Deep-learning networks with deeper network layers like ResNet50 and DenseNet121 performed better in this experiment. This study can provide a reference for the identification of peanut-leaf diseases. Full article
(This article belongs to the Section Food Science and Technology)
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<p>The original images of peanut leaves collected by mobile phone.</p>
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<p>Condition of leaves, from left to right: healthy, simultaneously suffering from rust and scorch disease, rust disease, leaf-spot disease, and scorch disease.</p>
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<p>A typical convolutional neural network structure.</p>
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<p>Inception module structure.</p>
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<p>Out-of-fold prediction process.</p>
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<p>(<b>a</b>) Accuracy of model ensemble; (<b>b</b>) <span class="html-italic">F</span>1 score of model ensemble.</p>
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<p>ROC curves for the model after ensemble. (<b>a</b>) ROC curve DenseNet121 + LR data augmentation; (<b>b</b>) ROC curve DenseNet121 + LR without data augmentation; (<b>c</b>) ROC curve VGG16 + SVM data augmentation; (<b>d</b>) ROC curve VGG16 + SVM without data augmentation; (<b>e</b>) ROC curve DenseNet121 + RF data augmentation; (<b>f</b>) ROC curve DenseNet121 + RF without data augmentation.</p>
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19 pages, 4843 KiB  
Article
Application of Artificial Intelligence to Determined Unconfined Compressive Strength of Cement-Stabilized Soil in Vietnam
by Huong Thi Thanh Ngo, Tuan Anh Pham, Huong Lan Thi Vu and Loi Van Giap
Appl. Sci. 2021, 11(4), 1949; https://doi.org/10.3390/app11041949 - 23 Feb 2021
Cited by 29 | Viewed by 2985
Abstract
Cement stabilized soil is one of the commonly used as ground reinforcement solutions in geotechnical engineering. In this study, the main object was to apply three machine learning (ML) methods namely gradient boosting (GB), artificial neural network (ANN) and support vector machine (SVM) [...] Read more.
Cement stabilized soil is one of the commonly used as ground reinforcement solutions in geotechnical engineering. In this study, the main object was to apply three machine learning (ML) methods namely gradient boosting (GB), artificial neural network (ANN) and support vector machine (SVM) to predict unconfined compressive strength (UCS) of cement stabilized soil. Soil samples were collected at Hai Duong city, Vietnam. A total of 216 soil–cement samples were mixed in the laboratory and compressed to determine the UCS. This data set is divided into two parts of the training data set (80%) and testing set (20%) to build and test the model, respectively. To verify the performance of ML model, various criteria named correlation coefficient (R), mean absolute error (MAE) and root mean square error (RMSE) were used. The results show that all three ML models were effective methods to predict the UCS of cement-stabilized soil. Amongst three model used in this study, optimized ANN model provided superior performance compare to two others models with performance indicator R = 0.925, RMSE = 419.82 and MAE = 292.2 for testing part. This study can provide an effective tool to quickly predict the UCS of cement stabilized soil with high accuracy. Full article
(This article belongs to the Section Civil Engineering)
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<p>Experiment location.</p>
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<p>Undisturbed samples.</p>
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<p>Unconfined compression test equipment.</p>
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<p>Axial stress–strain relation.</p>
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<p>Diagram of a fully connected artificial neural network (ANN) with one hidden layer and a single output value.</p>
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<p>Comparison between (<b>a</b>) grid search and (<b>b</b>) random search for hyper-parameter tuning [<a href="#B50-applsci-11-01949" class="html-bibr">50</a>].</p>
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<p>Flow chart of the 5-fold cross-validation technique.</p>
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<p>Density curve of the performance indicator R on 300 samplings with the: (<b>a</b>) Training set and (<b>b</b>) Testing set.</p>
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<p>Density curve of the performance indicator RMSE on 300 samplings with the: (<b>a</b>) Training set and (<b>b</b>) Testing set.</p>
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<p>Density curve of the performance indicator MAE on 300 samplings with the: (<b>a</b>) Training set and (<b>b</b>) Testing set.</p>
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<p>Measure and predicted values of unconfined compressive strength (UCS) of cement-stabilized soil using the training set: (<b>a</b>) gradient boosting (GB); (<b>c</b>) ANN and (<b>e</b>) support vector machine (SVM) and testing set: (<b>b</b>) GB; (<b>d</b>) ANN and (<b>f</b>) SVM.</p>
Full article ">Figure 11 Cont.
<p>Measure and predicted values of unconfined compressive strength (UCS) of cement-stabilized soil using the training set: (<b>a</b>) gradient boosting (GB); (<b>c</b>) ANN and (<b>e</b>) support vector machine (SVM) and testing set: (<b>b</b>) GB; (<b>d</b>) ANN and (<b>f</b>) SVM.</p>
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<p>Feature importance index of 14 variables used in this study.</p>
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<p>An example of some axial stress–strain relation curves of the soil–cement mixture.</p>
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<p>An example of some axial stress–strain relation curves of the soil–cement mixture.</p>
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19 pages, 7383 KiB  
Article
Online Intelligent Perception of Pantograph and Catenary System Status Based on Parameter Adaptation
by Yuan Shen, Xiao Pan and Luonan Chang
Appl. Sci. 2021, 11(4), 1948; https://doi.org/10.3390/app11041948 - 23 Feb 2021
Cited by 7 | Viewed by 2769
Abstract
Online autonomous perception of pantograph catenary system status is of great significance for railway autonomous operation and maintenance (RIOM). Image sensors combined with an image processing algorithm can realize the automatic acquisition of the pantograph catenary condition; however, it is difficult to meet [...] Read more.
Online autonomous perception of pantograph catenary system status is of great significance for railway autonomous operation and maintenance (RIOM). Image sensors combined with an image processing algorithm can realize the automatic acquisition of the pantograph catenary condition; however, it is difficult to meet the demand of long-term stable condition acquisition, which restricts the implementation of online contact state feedback and the realization of railway automation. This paper proposes an online intelligent perception of the pantograph and catenary system (PCS) status based on parameter adaptation to realize fast and stable state analysis when the train is in long-term operation outdoors. First, according to the feature of the contact point, we used histogram of gradient (HoG) features and one-dimensional signal combined with a KCF tracker as the baseline method. Then, a result discriminator located by L1 and hash similarity constraints was used to construct a closed-loop parameter adaptive localization framework, which retrieves and updates parameters when tracking failure occurs. After that, a pruned RefineDet method was used to detect pantograph horns and sparks, which, together with the contact points localization method, ensure the long-term stability of feature localization in PCS images. Then, based on the stereo cameras model, the three-dimensional trajectory of the whole pantograph body can be reconstructed by the image features, and we obtained pantograph catenary contact parameters including the pantograph slide posture, contact line offset, arc detection, separation detection, etc. Our method has been tested on more than 16,000 collected image pairs and the results show that the proposed method has a better positioning effect than the state-of-art method, and realizes the online acquisition of pantograph catenary contact state, representing a significant contribution to RIOM. Full article
(This article belongs to the Collection Machine Learning in Computer Engineering Applications)
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<p>Overview of the online pantograph and catenary system (PCS) intelligent perception analysis system and illustration of the four modules: data collection, feature localization, reconstruction, and data analysis.</p>
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<p>Contact points localization by template matching. Two template signals are shown in the bottom-right corner in bright pink.</p>
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<p>Hash similarity for fault tracking.</p>
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<p>The pruned RefineDet network framework.</p>
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<p>Example of pantograph pose change: (<b>a</b>) change in X-O-Z coordinates and (<b>b</b>) change in Z coordinate.</p>
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<p>The tested datasets which contains various complex situation. (<b>a</b>) Image in different illumination, (<b>b</b>) illustration of sparks in PCS images, and (<b>c</b>) an example of complex background.</p>
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<p>Illustration of tracking results in long-term datasets.</p>
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<p>Precision of the tracking results. (<b>a</b>,<b>b</b>) The precision with region of interest(ROI) threshold, and (<b>c</b>,<b>d</b>) the precision along with the dataset length. (<b>a</b>,<b>c</b>) A comparison our method compared to other tracking methods. (<b>b</b>,<b>d</b>) A comparison of our method with other tracking method in our adaptive tracking framework.</p>
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<p>Train dataset of pruned RefineDet: (<b>a</b>–<b>c</b>) illustration emphasizing the horns in double side and sparks, respectively, and (<b>d</b>) illustration of the augmented frames.</p>
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<p>Pantograph pose in frame sequence, in which the left part is the pantograph moving trajectory and the right part shows the details in 10,000–12,000 frames. The top is the lateral view and the bottle, and in below is the theta and height value of the pantograph, respectively.</p>
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9 pages, 6886 KiB  
Article
Application of the Segmented Correlation Technology in Seismic Communication with Morse Code
by Yuanjie Jiang, Yuda Chen, Ruyun Tian, Longxu Wang, Shixue Lv, Jun Lin and Xuefeng Xing
Appl. Sci. 2021, 11(4), 1947; https://doi.org/10.3390/app11041947 - 23 Feb 2021
Cited by 3 | Viewed by 2077
Abstract
Seismic communication might promise to revolutionize the theory of seismic waves. However, one of the greatest challenges to its widespread adoption is the difficulty of signal extraction because the seismic waves in the vibration environments, such as seas, streets, city centers and subways, [...] Read more.
Seismic communication might promise to revolutionize the theory of seismic waves. However, one of the greatest challenges to its widespread adoption is the difficulty of signal extraction because the seismic waves in the vibration environments, such as seas, streets, city centers and subways, are very complex. Here, we employ segmented correlation technology with Morse code (SCTMC), which extracts the target signal by cutting the collected data into a series of segments and makes these segments cross-correlate with the decoded signal to process the collected data. To test the effectiveness of the technology, a seismic communication system composed of vibroseis sources and geophones was built in an environment full of other vibration signals. Most notably, it improves the signal-to-noise ratio (SNR), extending the relay distance and suppressing other vibration signals by using technology to deal with seismic data generated by the system. Full article
(This article belongs to the Special Issue Advances in Applied Geophysics)
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<p>A long-distance transmission scheme about seismic signals.</p>
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<p>The comparison of hammering signals and footstep signals; (<b>a</b>) Hammer signals and footstep signals in raw data; (<b>b</b>) Hammering signals and footstep signals filtered by a 5–100 Hz band-pass filter; (<b>c</b>) The spectrum of footstep signals in raw data; (<b>d</b>) The spectrum of hammer signals in raw data.</p>
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<p>The amplitude changes of signals before and after filtering; (<b>a</b>) Vibroseis signals and footstep signals before filtering; (<b>b</b>) Vibroseis signals and footstep signals after filtering.</p>
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<p>The direct cross-correlation in signal simulation; (<b>a</b>) The 200 Hz SOS signal in the simulation diagram; (<b>b</b>) The direct cross-correlation about SOS signal in the simulation diagram.</p>
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<p>The distribution of 5 CDJ-S2C-2 geophones, 5 GEIWSR-II seismometers and a 500 N vibroseis source.</p>
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<p>The collected signal at 60 m; (<b>a</b>) The original data at 60 m; (<b>b</b>)The spectral analysis of the original data; (<b>c</b>) The target signal extraction with a band-pass filter; (<b>d</b>) The target signal extraction with the segmented correlation technology.</p>
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21 pages, 886 KiB  
Article
Optimizing a Reverse Supply Chain Network for Electronic Waste under Risk and Uncertain Factors
by Linh Thi Truc Doan, Yousef Amer, Sang-Heon Lee, Phan Nguyen Ky Phuc and Tham Thi Tran
Appl. Sci. 2021, 11(4), 1946; https://doi.org/10.3390/app11041946 - 23 Feb 2021
Cited by 2 | Viewed by 3177
Abstract
Minimizing the impact of electronic waste (e-waste) on the environment through designing an effective reverse supply chain (RSC) is attracting the attention of both industry and academia. To obtain this goal, this study strives to develop an e-waste RSC model where the input [...] Read more.
Minimizing the impact of electronic waste (e-waste) on the environment through designing an effective reverse supply chain (RSC) is attracting the attention of both industry and academia. To obtain this goal, this study strives to develop an e-waste RSC model where the input parameters are fuzzy and risk factors are considered. The problem is then solved through crisp transformation and decision-makers are given the right to choose solutions based on their satisfaction. The result shows that the proposed model provides a practical and satisfactory solution to compromise between the level of satisfaction of constraints and the objective value. This solution includes strategic and operational decisions such as the optimal locations of facilities (i.e., disassembly, repairing, recycling facilities) and the flow quantities in the RSC. Full article
(This article belongs to the Special Issue Electronic Waste: Management and Recovery Technologies)
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<p>The generic e-waste reverse supply chain (RSC) network.</p>
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30 pages, 4856 KiB  
Article
Category-Theoretic Formulation of the Model-Based Systems Architecting Cognitive-Computational Cycle
by Yaniv Mordecai, James P. Fairbanks and Edward F. Crawley
Appl. Sci. 2021, 11(4), 1945; https://doi.org/10.3390/app11041945 - 23 Feb 2021
Cited by 16 | Viewed by 4524
Abstract
We introduce the Concept→Model→Graph→View Cycle (CMGVC). The CMGVC facilitates coherent architecture analysis, reasoning, insight, and decision making based on conceptual models that are transformed into a generic, robust graph data structure (GDS). The GDS is then transformed into multiple views of the model, [...] Read more.
We introduce the Concept→Model→Graph→View Cycle (CMGVC). The CMGVC facilitates coherent architecture analysis, reasoning, insight, and decision making based on conceptual models that are transformed into a generic, robust graph data structure (GDS). The GDS is then transformed into multiple views of the model, which inform stakeholders in various ways. This GDS-based approach decouples the view from the model and constitutes a powerful enhancement of model-based systems engineering (MBSE). The CMGVC applies the rigorous foundations of Category Theory, a mathematical framework of representations and transformations. We show that modeling languages are categories, drawing an analogy to programming languages. The CMGVC architecture is superior to direct transformations and language-coupled common representations. We demonstrate the CMGVC to transform a conceptual system architecture model built with the Object Process Modeling Language (OPM) into dual graphs and a stakeholder-informing matrix that stimulates system architecture insight. Full article
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<p>(<b>a</b>) The Model⇔Concept duo extended to (<b>b</b>) Model→View→Concept trio extended as a (<b>c</b>) Concept→Model→Graph→View Cycle (CMGVC).</p>
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<p>OPM model (OPD on the left, OPL on the right) of a <b>Lane Keeping System</b>, loosely based on [<a href="#B32-applsci-11-01945" class="html-bibr">32</a>]. The system handles a <b>Lane Keeping</b> function that provides <b>Improved Safety</b>. <b>Lane Keeping</b> generates <b>Alerts</b> that inform the <b>Driving</b> process, and <b>Steering Commands</b> that affect the <b>Vehicle</b>’s <b>Propelling</b> function. The <b>Road</b> constitutes an instrument for both <b>Propelling</b> and <b>Lane Keeping</b>. <b>Driving</b> and <b>Propelling</b> affect each other regardless of the <b>Lane Keeping System</b>.</p>
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<p>Equivalent representations of relations between pairs of objects as: (<b>i</b>) a digraph, (<b>ii</b>) an adjacency matrix (cell (r,c) holds the arrow value of row object (r) to column object (c), and (<b>iii</b>) a set of tuples (triplets of source object (S), target object (T), and value (V), relating S to T.</p>
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<p>A category with three types: Type1, Type2, and Type3. The morphisms <math display="inline"><semantics> <mrow> <mi>m</mi> <mn>12</mn> <mo>:</mo> <mo> </mo> <mi>T</mi> <mi>y</mi> <mi>p</mi> <mi>e</mi> <mn>1</mn> <mo>→</mo> <mi>T</mi> <mi>y</mi> <mi>p</mi> <mi>e</mi> <mn>2</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>m</mi> <mn>23</mn> <mo>:</mo> <mo> </mo> <mi>T</mi> <mi>y</mi> <mi>p</mi> <mi>e</mi> <mn>2</mn> <mo>→</mo> <mi>T</mi> <mi>y</mi> <mi>p</mi> <mi>e</mi> <mn>3</mn> </mrow> </semantics></math> are specified. The morphism <math display="inline"><semantics> <mrow> <mi>m</mi> <mn>13</mn> </mrow> </semantics></math> is a composition of <math display="inline"><semantics> <mrow> <mi>m</mi> <mn>23</mn> </mrow> </semantics></math> after <math display="inline"><semantics> <mrow> <mi>m</mi> <mn>13</mn> </mrow> </semantics></math>—it transforms Type1 to Type3 by transforming Type1 to Type2, then Type2 to Type3.</p>
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<p>The CMGVC, as a cognitive–computational cycle of Conceptual Modeling, Model Transforming, Stakeholder-informing View Rendering, and Reasoning. The System, OPM Model, GDS, and SIM are specializations of the respective generic artifacts: Concept, Model, Generic Representation, and View.</p>
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<p>The OPM modeling language, OPML, as a category. Modeling (the morphism <span class="html-italic">m</span>) is like hopping through the instantiation of category types based on existing artifacts. For example: (a) creating a new Diagram D1 in a Model M, (b) creating an Object Ob1 in D1, (c) creating a Process P1 in D1, (d) creating a RelationRr1(Ob1,P1) from Ob1 to P1, (e) creating a new Diagram D2 from P1, (f) adding States St11 and St12 to Ob1 in D2, and so on. Every instantiation of a type also affects the Spec, and therefore all graphical elements have a mapping into Spec (the morphism <span class="html-italic">s</span>). Spec also feeds into the Rendering morphism <span class="html-italic">r</span>, which renders a Report from the Spec, currently in the form of a PDF file. Diagram created using MATLAB 2019b digraph plotting capabilities [<a href="#B85-applsci-11-01945" class="html-bibr">85</a>].</p>
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<p>A graph rendition of a subset of the Lane Keeping System (LKS) model in <a href="#applsci-11-01945-f002" class="html-fig">Figure 2</a>. The graph maps the OPM-specifiable terms “<span>$</span>Object”, and “<span>$</span>Process” to Domain entities: Object classifies Vehicle, Driver, and LKS; Process classifies Driving, Propelling, and Lane_Keeping. Domain-internal relations include the mutual invocation between Driving and Propelling, output of Alert and Steering_Command to Driving and Propelling, respectively, and exhibition of Lane_Keeping by LKS. This graph visualizes a subset of the GDS that represents the model. It is clearly difficult to comprehend, and is illustrated for intuition about the possible mapping of a model to a graph.</p>
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<p>A C-Set mapping functor schema from OPML to GDS (RSTUV tuple set) extracts <tt>ElementDictionary</tt> from the model’s <tt>ExportedReport</tt> and transforms <tt>ElementDictionary</tt> into three sets: <tt>ObjectElement</tt>, <tt>ProcessElement</tt>, and <tt>RelationSet</tt>. <tt>RelationSet</tt> is decomposed into a set of <tt>Relations</tt>. The functor computes attributes for each entity type from the report. For example, it lists the <tt>ObjectOPDs</tt> in which each <tt>Object</tt> is defined, and extracts the Source object/process and the Target object/process for each <tt>Relation</tt>. Each entity is then transformed into a set of <tt>RSTUVCandidates</tt>. Duplicate candidates are removed before the set of <tt>RSTUVTuple</tt> is compiled. Illustration created using the <a href="http://www.NomnoML.com" target="_blank">www.NomnoML.com</a>.</p>
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<p>Model Analyzer Framework V0.1—Prototype Architecture Description</p>
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<p>A JSON structure defining the required transformations of <tt>ProcessElement</tt> attributes to <tt>RSTUVCandidate</tt> items. This example does not include <tt>relationSourceTargetTriplets</tt>.</p>
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<p>OPM model with processes and onputs (<b>a</b>), shown in three additional renditions: (<b>b</b>) an onput-on-node/process-on-edge graph, (<b>c</b>) a process-on-node/onput-on-edge graph, and (<b>d</b>) a process-to-process onput exchange matrix. NULL processes and onputs (in all renditions) serve as placeholders for missing or partial relations, like an input without a source process (Ob12), a process without an input (P3) or without an output (P7), and an output without a target process (Ob11). Both graph visualizations were rendered using <a href="https://csacademy.com/app/graph_editor/" target="_blank">https://csacademy.com/app/graph_editor/</a> (accessed on 3 December 2020).</p>
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<p><span style="color:#00B050">Lane Keeping System</span> zooms into <span style="color:#00B050">Alert Mode</span>, <span style="color:#00B050">Steer-back Mode</span>, <span style="color:#00B050">Road Image</span>, <span style="color:#00B050">Alert Mode</span>, <span style="color:#00B050">Lane Crossing</span>, and <span style="color:#00B050">Steer-back Mode</span>, in that vertical sequence, as well as <span style="color:#0070C0">Alerting</span>, <span style="color:#0070C0">Analyzing Road</span>, <span style="color:#0070C0">Imaging Road</span>, <span style="color:#0070C0">Selecting Operational Mode</span>, and <span style="color:#0070C0">Steering</span> (This caption is formal OPL).</p>
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12 pages, 13355 KiB  
Article
In Situ Measurement of Sound Attenuation by Fish Schools (Japanese Horse Mackerel, Trachurus japonicus) at Mid-Frequency Bands
by Hansoo Kim and Dong-Guk Paeng
Appl. Sci. 2021, 11(4), 1944; https://doi.org/10.3390/app11041944 - 23 Feb 2021
Cited by 1 | Viewed by 2415
Abstract
Acoustic waves are attenuated by fish schools as they propagate through the ocean. The attenuation by fish schools is not currently considered in fishery acoustics and sonar applications, especially at mid-frequency bands. In this study, fish school attenuation experiments were conducted with a [...] Read more.
Acoustic waves are attenuated by fish schools as they propagate through the ocean. The attenuation by fish schools is not currently considered in fishery acoustics and sonar applications, especially at mid-frequency bands. In this study, fish school attenuation experiments were conducted with a number of individual fish in situ in a net cage at mid-frequency bands (3–7 kHz). The target fish species was the Japanese horse mackerel (Trachurus japonicus), which typically forms fish schools in the coastal ocean of northeastern Asia. The attenuated acoustic waves were measured for the cases of non-net, only net (0), 100, 200, 300, 400, and 500 individual horse mackerels in the net cage. Results showed that the acoustic signal attenuation increased with the number of horse mackerels. The mean and maximum attenuation coefficients were approximately 6.0–15.4 dB/m and 6.5–21.8 dB/m for all frequencies, respectively. The measured attenuation coefficients were compared with the ones from previous studies to propose new regression models with normalized extinction cross-sections of weight and length of fish. This study confirmed that the fish school attenuation could not be ignored and compensated at mid-frequencies in the ocean. These results would be useful for fishery acoustics, especially in the development of scientific echo-sounder, and naval applications of sonar operations and analysis. Full article
(This article belongs to the Collection Fishery Acoustics)
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<p>Schematic of the experimental system used to measure sound attenuation from the fish schools (Japanese horse mackerel) at mid-frequency bands. Transmitter, receiver, net cage, and underwater camera were set at a depth of 3.3 m below the sea surface.</p>
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<p>Representative attenuation experimental results of (<b>a</b>) Exp2 (only net, fish without in the net cage), (<b>b</b>) Exp3 (100 ind. fish in the net cage), (<b>c</b>) Exp5 (300 ind. fish in the net cage), and (<b>d</b>) Exp7 (500 ind. fish in the net cage) at 3 kHz; the top figures are the received voltage signals, middle ones are received levels (<span class="html-italic">RLs</span>), and bottom ones are the histogram of the <span class="html-italic">RL</span>s from the direct paths. The transmission losses in seawater were compensated for the <span class="html-italic">RL</span>s.</p>
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<p>(<b>a</b>) and (<b>b</b>) are mean and maximum attenuation coefficients at 3–7 kHz for the different number of individual fish, respectively (100 ind.: blue dotted line, 200 ind.: red straight line, 300 ind.: green straight line, 400 ind.: pink dashed line, and 500 ind.: black dashed line).</p>
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<p>Results of normalized extinction cross-section of (<b>a</b>) the wet weight (<math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mrow> <mi>e</mi> <mi>W</mi> </mrow> </msub> </mrow> </semantics></math>) and (<b>b</b>) the total length (<math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mrow> <mi>e</mi> <mi>L</mi> </mrow> </msub> </mrow> </semantics></math> ) of fish with frequency in previous and present studies. The black line is the previous regression model [<a href="#B6-applsci-11-01944" class="html-bibr">6</a>], the blue lines are the new quadratic regression models for mid-frequency from the present study, and the red lines are the total quadratic regression models for all-frequency.</p>
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