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14 pages, 6056 KiB  
Article
Centrifugal Test Study on the Vertical Uplift Capacity of Single-Cylinder Foundation in High-Sensitivity Marine Soil
by Mingzhe Wei, Yanghui Ye, Wei Zhao, Zehao Wang, Fuhao Ge and Tingkai Nian
J. Mar. Sci. Eng. 2024, 12(12), 2152; https://doi.org/10.3390/jmse12122152 - 25 Nov 2024
Abstract
Offshore wind power is a new type of clean energy with broad development prospects. Accurate analysis of the uplift capacity of offshore wind turbine foundations is a crucial prerequisite for ensuring the safe operation of wind turbines under complex hydrodynamic conditions. However, current [...] Read more.
Offshore wind power is a new type of clean energy with broad development prospects. Accurate analysis of the uplift capacity of offshore wind turbine foundations is a crucial prerequisite for ensuring the safe operation of wind turbines under complex hydrodynamic conditions. However, current research on the uplift capacity of suction caissons often neglects the high-sensitivity characteristics of marine soils. Therefore, this paper first employs the freeze–thaw cycling procedure to prepare high-sensitivity saturated clay. Subsequently, a single−tube foundation for wind turbines is constructed within a centrifuge through a penetration approach. Ten sets of centrifuge model tests with vertical cyclic pullout are conducted. Through comparative analysis, this study explores the pullout capacity and its variation patterns of suction caisson foundations in clay with different sensitivities under cyclic loading. This research indicates the following: (1) The preparation of high-sensitivity soil through the freeze−thaw procedure is reliable; (2) the uplift capacity of suction caissons in high−sensitivity soil rapidly decreases with increasing numbers of cyclic loads and then tends to stabilize. The cumulative displacement rate of suction caissons in high-sensitivity soil is fast, and the total number of pressure–pullout cycles required to reach non-cumulative displacement is significantly smaller than that in low-sensitivity soil; (3) the vertical cyclic loading times and stiffness evolution patterns of single-tube foundations, considering the influence of sensitivity, have been analyzed. It was found that the secant stiffness exhibits a logarithmic function relationship with both the number of cycles and sensitivity. The findings of this study provide assistance and support for the design of suction caissons in high-sensitivity soils. Full article
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Figure 1

Figure 1
<p>Microscopic images of kaolin and ball clay before and after freeze–thaw cycles: (<b>a</b>) microscopic image of ball clay before freeze–thaw; (<b>b</b>) microscopic image of kaolin before freeze–thaw; (<b>c</b>) microscopic image of ball clay after freeze–thaw; (<b>d</b>) microscopic image of kaolin after freeze–thaw.</p>
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<p>Centrifuge test: (<b>a</b>) centrifugal model test device; (<b>b</b>) photo of test model box and suction cylinder; (<b>c</b>) point layout drawing; (<b>d</b>) schematic diagram of penetration, monotonic, and cyclic loading.</p>
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<p>The experimental relationship between the normalized vertical displacement <span class="html-italic">w</span>/<span class="html-italic">L</span> and the cycle number <span class="html-italic">N</span>: (<b>a</b>) normalized vertical displacements versus number of cycles for low-sensitivity soil at <span class="html-italic">V<sub>C</sub></span> /<span class="html-italic">V</span><sub>0</sub> = 0.39, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; <span class="html-italic">V<sub>C</sub></span> /<span class="html-italic">V</span><sub>0</sub> = 0.425, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.03; <span class="html-italic">V<sub>C</sub></span> /<span class="html-italic">V</span><sub>0</sub> = 0.45 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.05 condition; (<b>b</b>) normalized vertical displacements versus number of cycles for low-sensitivity soil at <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.35, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.325, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.02; <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.3 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01 condition; (<b>c</b>) normalized vertical displacements versus number of cycles for highly sensitive soils at <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.4, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.425, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01 conditions; (<b>d</b>) normalized vertical displacements versus number of cycles for highly sensitive soils at <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.3, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.32, <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01 conditions.</p>
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<p>Normalized cyclic load and normalized displacement relationship diagram of low-sensitivity soil: (<b>a</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.3 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; (<b>b</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.35 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.02; (<b>c</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.45 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.05; (<b>d</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.325 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; (<b>e</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.39 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; (<b>f</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.425 and <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.03.</p>
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<p>Normalized cyclic load and normalized displacement relationship diagram of high-sensitivity soil: (<b>a</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.3; <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; (<b>b</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.32; <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; (<b>c</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.4; <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01; (<b>d</b>) normalized cyclic load versus normalized vertical displacement for <span class="html-italic">V<sub>C</sub></span>/<span class="html-italic">V</span><sub>0</sub> = 0.425; <span class="html-italic">V</span><sub>a</sub>/<span class="html-italic">V</span><sub>0</sub> = 0.01.</p>
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<p>Definition of secant stiffness.</p>
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<p>Scatter plot of secant stiffness: (<b>a</b>) scatter plot of cut-line stiffness of low-sensitivity soil; (<b>b</b>) scatter plot of stiffness of high-sensitivity earth cut line.</p>
Full article ">
38 pages, 445 KiB  
Review
Advances and Challenges in Low-Resource-Environment Software Systems: A Survey
by Abayomi Agbeyangi and Hussein Suleman
Informatics 2024, 11(4), 90; https://doi.org/10.3390/informatics11040090 - 25 Nov 2024
Abstract
A low-resource environment has limitations in terms of resources, such as limited network availability and low-powered computing devices. In such environments, it is arguably more difficult to set up new software systems, maintain existing software, and migrate between software systems. This paper presents [...] Read more.
A low-resource environment has limitations in terms of resources, such as limited network availability and low-powered computing devices. In such environments, it is arguably more difficult to set up new software systems, maintain existing software, and migrate between software systems. This paper presents a survey of software systems for low-resource environments to highlight the challenges (social and technical) and concepts. A qualitative methodology is employed, consisting of an extensive literature review and comparative analysis of selected software systems. The literature covers academic and non-academic sources, focusing on identifying software solutions that address specific challenges in low-resource environments. The selected software systems are categorized based on their ability to overcome challenges such as limited technical skills, device constraints, and socio-cultural issues. The study reveals that despite noteworthy progress, unresolved challenges persist, necessitating further attention to enable the optimal performance of software systems in low-resource environments. Full article
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<p>Low-resource software challenges and their interactions.</p>
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20 pages, 689 KiB  
Article
Study on the Minimum Operation Width of Human-Powered Bicycles for Safe and Comfortable Cycling
by Shangwen Qu, Jiangbi Hu, Ronghua Wang, Yanyan Guan, Sen Ma and Zechao Zhang
Appl. Sci. 2024, 14(23), 10928; https://doi.org/10.3390/app142310928 - 25 Nov 2024
Abstract
Chinese cities are increasingly developing exclusive bicycle paths to improve the safety and efficiency of bicycle transit. The width of bikeways is a critical factor influencing cyclists’ safety and comfort, with insufficient width identified as a major contributor to bicycle accidents. Therefore, determining [...] Read more.
Chinese cities are increasingly developing exclusive bicycle paths to improve the safety and efficiency of bicycle transit. The width of bikeways is a critical factor influencing cyclists’ safety and comfort, with insufficient width identified as a major contributor to bicycle accidents. Therefore, determining the minimum operational width for human-powered bicycles is essential for bikeway design. While some countries’ design manuals consider speed as a factor in determining width, there is a lack of field experiments to validate these specifications from the perspective of cyclists’ safety and comfort. This study addresses this gap by conducting a field experiment to measure cycling workload, which reflects safety and comfort under different widths and cycling speeds. The experiment involved 12 cyclists on a test road, where cycling workload was measured at various preset widths and cycling speeds for a single human-powered cyclist. The results were further validated using conventional lateral distance measurement techniques, which are used in the existing literature to determine the cycling width. The results show that wider bikeway widths lead to a lower cycling workload, enhancing comfort and safety. However, both very high (over 20 km/h) and very low (under 5 km/h) speeds significantly increase cyclists’ workload, which in turn requires a wider path to maintain a safe and comfortable cycling experience. The study found that a minimum width of 0.90 m may be adequate for cyclists traveling at speeds between 10 and 15 km/h, while a width of 1.0 m is sufficient for speeds ranging from 5 km/h to 25 km/h, provided the bicycle width does not exceed 0.62 m. Given that cyclists typically progress from slower to faster speeds, a minimum operational width of 1.0 m is recommended for most cases. This study highlights the importance of considering cyclists’ workload in determining appropriate bikeway widths. It provides valuable insights for designing safer, more comfortable bike paths and reducing bicycle accidents, contributing to the sustainable development of urban cycling infrastructure. Full article
(This article belongs to the Special Issue Sustainable Urban Mobility)
16 pages, 4008 KiB  
Article
Low-Power 8T SRAM Compute-in-Memory Macro for Edge AI Processors
by Hye-Ju Shin and Sung-Hun Jo
Appl. Sci. 2024, 14(23), 10924; https://doi.org/10.3390/app142310924 - 25 Nov 2024
Abstract
The traditional Von Neumann architecture creates bottlenecks due to data movement. The compute-in-memory (CIM) architecture performs computations within memory bit-cell arrays, enhancing computational performance. Edge devices utilizing artificial intelligence (AI) address real-time problems and have established themselves as groundbreaking technology. The 8T structure [...] Read more.
The traditional Von Neumann architecture creates bottlenecks due to data movement. The compute-in-memory (CIM) architecture performs computations within memory bit-cell arrays, enhancing computational performance. Edge devices utilizing artificial intelligence (AI) address real-time problems and have established themselves as groundbreaking technology. The 8T structure proposed in this paper has strengths over other existing structures in that it better withstands environmental changes within the SRAM and consumes lower power during memory operation. This structure minimizes reliance on complex ADCs, instead utilizing a simplified voltage differential approach for multiply-and-accumulate (MAC) operations, which enhances both power efficiency and stability. Based on these strengths, it can achieve higher battery efficiency in AI edge devices and improve system performance. The proposed integrated circuit was simulated in a 90 nm CMOS process and operated on a 1 V supply voltage. Full article
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Figure 1
<p>Proposed 8T SRAM-CIM bit-cell schematic.</p>
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<p>Overall SRAM-CIM architecture.</p>
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<p>(<b>a</b>) Read operation and (<b>b</b>) write operation.</p>
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<p>Bit-cell internal multiplication output process.</p>
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<p>(<b>a</b>) Body voltage effect and (<b>b</b>) threshold voltage variation.</p>
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<p>(<b>a</b>) Voltage difference before body voltage effect and (<b>b</b>) after body voltage effect.</p>
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<p>Word line driver simulation result.</p>
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<p>Write driver schematic.</p>
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<p>Write driver simulation result.</p>
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<p>Static body biasing schematic.</p>
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<p>(<b>a</b>) Conventional 8T SRAM and (<b>b</b>) ultra-low power (ULP) 8T SRAM.</p>
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<p>(<b>a</b>) Power comparison in read operation and (<b>b</b>) power comparison in write operation.</p>
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<p>(<b>a</b>) Read noise margin and (<b>b</b>) write noise margin comparison graph.</p>
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24 pages, 9843 KiB  
Article
Study of AC Conductivity and Relaxation Times Depending on Moisture Content in Nanocomposites of Insulation Pressboard–Innovative Bio-Oil–Water Nanodroplets
by Pawel Zukowski, Konrad Kierczynski, Pawel Okal, Marek Zenker, Rafal Pajak, Marek Szrot, Pawel Molenda and Tomasz N. Koltunowicz
Materials 2024, 17(23), 5767; https://doi.org/10.3390/ma17235767 - 25 Nov 2024
Abstract
The aim of this study was to determine the frequency–temperature dependence of the AC conductivity and relaxation times in humid electrical pressboard used in the insulation of power transformers, impregnated with the innovative NYTRO® BIO 300X bio-oil produced from plant raw materials. [...] Read more.
The aim of this study was to determine the frequency–temperature dependence of the AC conductivity and relaxation times in humid electrical pressboard used in the insulation of power transformers, impregnated with the innovative NYTRO® BIO 300X bio-oil produced from plant raw materials. Tests were carried out for a composite of cellulose–bio-oil–water nanodroplets with a moisture content of 0.6% by weight to 5% by weight in the frequency range from 10−4 Hz to 5·103 Hz. The measurement temperatures ranged from 20 °C to 70 °C. The current conductivity in percolation channels in cellulose–bio insulating oil–water nanodroplets nanocomposites was analyzed. In such nanocomposites, DC conduction takes place via electron tunneling between the potential wells formed by the water nanodroplets. It was found that the value of the percolation channel resistance is lowest in the case of a regular arrangement of the nanodroplets. As disorder increases, characterized by an increase in the standard deviation value, the percolation channel resistance increases. It was found that the experimental values of the activation energy of the conductivity and the relaxation time of the composite of cellulose–bio-oil–water nanodroplets are the same within the limits of uncertainty and do not depend on the moisture content. The value of the generalized activation energy is ΔE ≈ (1.026 ± 0.0160) eV and is constant over the frequency and temperature ranges investigated. This study shows that in the lowest frequency region, the conductivity value does not depend on frequency. As the frequency increases further, the relaxation time decreases; so, the effect of moisture on the conductivity value decreases. The dependence of the DC conductivity on the moisture content was determined. For low moisture contents, the DC conductivity is practically constant. With a further increase in water content, there is a sharp increase in DC conductivity. Such curves are characteristic of the dependence of the DC conductivity of composites and nanocomposites on the content of the conducting phase. A percolation threshold value of xc ≈ (1.4 ± 0.3)% by weight was determined from the intersection of flat and steeply sloping sections. The frequency dependence of the values of the relative relaxation times was determined for composites with moisture contents from 0.6% by weight to 5% by weight for a measurement temperature of 60 °C. The highest relative values of the relaxation time τref occur for direct current and for the lowest frequencies close to 10−4 Hz. As the frequency increases further, the relaxation time decreases. The derivatives d(logτref)/d(logf) were calculated, from the analysis of which it was determined that there are three stages of relaxation time decrease in the nanocomposites studied. The first occurs in the frequency region from 10−4 Hz to about 3·10−1 Hz, and the second from about 3·10−1 Hz to about 1.5·101 Hz. The beginning of the third stage is at a frequency of about 1.5·101 Hz. The end of this stage is above the upper range of the Frequency Domain Spectroscopy (FDS) meter, which is 5·103 Hz. It has been established that the nanodroplets are in the cellulose and not in the bio-oil. The occurrence of three stages on the frequency dependence of the relaxation time can be explained when the fibrous structure of the cellulose is taken into account. Nanodroplets, found in micelles, microfibrils and in the fibers of which cellulose is composed, can have varying distances between nanodroplets, determined by the dimensions of these cellulose components. Full article
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Figure 1

Figure 1
<p>Schematic representation of the rate of decay of the square of the wave function outside a potential well with nanometer dimensions, the distance between which is <span class="html-italic">r<sub>h</sub></span>.</p>
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<p><span class="html-italic">a</span>—tunneling of the electron from the first well to the second well in the direction opposite to the electric field; <span class="html-italic">p</span>—tunneling of the electron with a probability <span class="html-italic">p</span> from the second well to the third well; 1 − <span class="html-italic">p</span>—back tunneling of the electron with a probability of 1 − <span class="html-italic">p</span> from the second well to the first well.</p>
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<p>Diagram of the setup for AC measurements of the electrical properties of insulating materials: 1—FDS-PDC Dielectric Response Analyzer; 2—temperature meter; 3—climate chamber; 4—hermetic vessel; 5—voltage electrode; 6—tested sample; 7—guard electrode; 8—PT 1000 temperature sensor; 9—measurement electrode.</p>
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<p>Frequency dependence of the conductivity of a pressboard with a moisture content of 2% by weight impregnated with bio-oil for temperatures: 1—20 °C; 2—30 °C; 3—40 °C; 4—50 °C; 5—60 °C; 6—70 °C.</p>
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<p>Arrhenius plots for the conductivity of pressboard with a moisture content of 2% by weight for 18 selected measurement frequencies <span class="html-italic">f</span><sub>i</sub> from 1—frequency 10<sup>−4</sup> Hz—to 18—frequency 5·10<sup>3</sup> Hz.</p>
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<p>Frequency dependence of the activation energy of the conductivity of the bio-oil-impregnated pressboard with a moisture content of 2% by weight. Negative values are shown in red.</p>
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<p>Frequency dependence of the conductivity of the composite pressboard—bio-oil—moisture for a water content of 4% by weight. Measurement temperatures: 1—20 °C; 2—30 °C; 3—40 °C; 4—50 °C; 5—60 °C; 6—70 °C.</p>
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<p>Shift in the σ(<span class="html-italic">f</span>, <span class="html-italic">T</span>) dependence along the X and Y axes using the generalized activation energy for moisture content of 4% by weight: 1—reference temperature 20 °C [<a href="#B61-materials-17-05767" class="html-bibr">61</a>]; 2—reference temperature 60 °C. Every third point is marked on the graphs for each temperature.</p>
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<p>Frequency dependences of conductivity for water contents: 1—0.6% by weight; 2—1% by weight; 3—2% by weight; 4—3% by weight; 5—4% by weight; 6—5% by weight. Temperature of 60 °C.</p>
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<p>The dependencies of the conductivity of the pressboard–bio-oil–water nanodroplets composite on the distance between water molecules, according to Formula (32), for 16 selected frequencies ranging from (1)—10<sup>−4</sup> Hz to (16)—5·10<sup>3</sup> Hz. Measurement temperature: 60 °C.</p>
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<p>Frequency dependence of the coefficient value <span class="html-italic">B</span>(<span class="html-italic">f</span>), as shown in Formula (34).</p>
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<p>Frequency-dependent relationship of the relative relaxation time. 1—water content 2% by weight; 2—3% by weight; 3—4% by weight; 4—5% by weight.</p>
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<p>The frequency-dependent derivative of the logarithm of the relaxation time with respect to the logarithm of frequency: 1—<span class="html-italic">X</span> = 2% by weight; 2—3% by weight; 3—4% by weight; 4—5% by weight.</p>
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<p>Frequency-dependent distances over which electrons tunnel. 1—water content 2% by weight; 2—3% by weight; 3—4% by weight; 4—5% by weight.</p>
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<p>The dependencies of the distances over which electrons tunnel with respect to moisture content for stages I, II, and III are as follows: 1—the upper boundary of stage I is defined at a frequency of 10<sup>−4</sup> Hz. 2—the upper boundary of stage II and the lower boundary of stage I are defined at a frequency of 3·10<sup>−1</sup> Hz. 3—the upper boundary of stage III and the lower boundary of stage II are defined at a frequency of 1.5·10<sup>1</sup> Hz.</p>
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<p>Schematic representation of the percolation channel for direct current flow: 1—electrodes; 2—nanodroplets; 3—vector of the electric field under direct voltage.</p>
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<p>Schematic representation of alternating current flow in clusters with increased frequency—(<b>a</b>–<b>c</b>). 1—electrodes; 2—nanodroplets; 3—electric field vector in the first half-cycle; 4—electric field vector in the second half-cycle.</p>
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30 pages, 4423 KiB  
Article
Watermarking Tiny MLCommons Image Applications Without Extra Deployability Costs
by Alessandro Carra, Dilan Ece Durmuskaya, Beatrice Di Giulio, Laura Falaschetti, Claudio Turchetti and Danilo Pietro Pau
Electronics 2024, 13(23), 4644; https://doi.org/10.3390/electronics13234644 - 25 Nov 2024
Viewed by 32
Abstract
The tasks assigned to neural network (NN) models are increasingly challenging due to the growing demand for their applicability across domains. Advanced machine learning programming skills, development time, and expensive assets are required to achieve accurate models, and they represent important assets, particularly [...] Read more.
The tasks assigned to neural network (NN) models are increasingly challenging due to the growing demand for their applicability across domains. Advanced machine learning programming skills, development time, and expensive assets are required to achieve accurate models, and they represent important assets, particularly for small and medium enterprises. Whether they are deployed in the Cloud or on Edge devices, i.e., resource-constrained devices that require the design of tiny NNs, it is of paramount importance to protect the associated intellectual properties (IP). Neural networks watermarking (NNW) can help the owner to claim the origin of an NN model that is suspected to have been attacked or copied, thus illegally infringing the IP. Adapting two state-of-the-art NNW methods, this paper aims to define watermarking procedures to securely protect tiny NNs’ IP in order to prevent unauthorized copies of these networks; specifically, embedded applications running on low-power devices, such as the image classification use cases developed for MLCommons benchmarks. These methodologies inject into a model a unique and secret parameter pattern or force an incoherent behavior when trigger inputs are used, helping the owner to prove the origin of the tested NN model. The obtained results demonstrate the effectiveness of these techniques using AI frameworks both on computers and MCUs, showing that the watermark was successfully recognized in both cases, even if adversarial attacks were simulated, and, in the second case, if accuracy values, required resources, and inference times remained unchanged. Full article
(This article belongs to the Special Issue Towards Efficient and Reliable AI at the Edge)
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Figure 1
<p>Process to set the watermark matrix using one of the three options.</p>
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<p>Each step that has been taken to get to Equation (<a href="#FD1-electronics-13-04644" class="html-disp-formula">1</a>).</p>
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<p>Watermark extraction and detection process.</p>
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<p>Examples of GAN-generated images in the original resolution of 64 × 64. The original low-resolution images are not easily understandable beacause as desired they shall not be the same as the training dataset.</p>
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<p>Example of an abstract image generated using the pillow library.</p>
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<p>An example of the pre-selected images that are resized.</p>
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<p>Black-box NN watermarking approach workflow.</p>
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34 pages, 7043 KiB  
Review
Biofuels and Their Blends—A Review of the Effect of Low Carbon Fuels on Engine Performance
by Qian Xiong, Yulong Duan, Dezhi Liang, Tie Li, Hongliang Luo and Run Chen
Sustainability 2024, 16(23), 10300; https://doi.org/10.3390/su162310300 - 25 Nov 2024
Viewed by 77
Abstract
Energy is an important aspect concerning global economic development and environmental conservation. Economic growth has been accompanied by extensive use of fossil fuels, resulting in significant emissions of greenhouse gases and other pollutants. Therefore, researchers have turned their attention to low/zero carbon fuels. [...] Read more.
Energy is an important aspect concerning global economic development and environmental conservation. Economic growth has been accompanied by extensive use of fossil fuels, resulting in significant emissions of greenhouse gases and other pollutants. Therefore, researchers have turned their attention to low/zero carbon fuels. Among these, biofuels have attracted wide attention due to their relatively low cost, clean combustion products and renewability. This article reviews the combustion, performance and emission characteristics of internal combustion (IC) engines fueled with biofuels categorized into three generations by their raw material sources. According to most research findings, biofuels generally exhibit poorer combustion performance in IC engines compared to fossil fuels due to their high viscosity and low lower heating value. However, these biofuels, characterized by a high oxygen content, facilitate more complete combustion and reduce emissions of CO, UHC and smoke, albeit increasing NOx emission and fuel consumption. Both thermal efficiency and brake power also tend to decrease, but various optimization strategies such as advanced combustion modes or injection control methods can partially compensate for these drawbacks. In conclusion, biofuels should be a promising low-carbon fuel for IC engines in the future. Full article
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Figure 1
<p>The Initial Strategy on Reduction of Greenhouse Gas (GHG) Emission from Ships introduced by the IMO.</p>
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<p>Costs and volumes for the total capacities of diesel fuel and alternative fuels for a bulk vessel.</p>
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<p>CP of microalgae biofuel with different proportions of CNG as additions [<a href="#B30-sustainability-16-10300" class="html-bibr">30</a>].</p>
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<p>HRR of traditional diesel fuel and sunflower biofuel at different EGR rates [<a href="#B32-sustainability-16-10300" class="html-bibr">32</a>].</p>
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<p>HRR of B20I, B20B and traditional diesel fuel [<a href="#B34-sustainability-16-10300" class="html-bibr">34</a>].</p>
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<p>The relationship between ID and temperature of different biofuels and traditional diesel fuel [<a href="#B36-sustainability-16-10300" class="html-bibr">36</a>].</p>
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<p>The relationship between ID and engine load of different biofuels and traditional diesel fuel [<a href="#B37-sustainability-16-10300" class="html-bibr">37</a>].</p>
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<p>The relationship between BTE and engine speed of mustard biofuel blends with different proportions [<a href="#B42-sustainability-16-10300" class="html-bibr">42</a>].</p>
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<p>The relationship between BTE and engine load of different biofuel blends with different proportions and traditional diesel fuel [<a href="#B47-sustainability-16-10300" class="html-bibr">47</a>].</p>
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<p>The relationship between BSFC and engine speed of cottonseed biofuel–ethanol blends with different proportions at 100% load [<a href="#B57-sustainability-16-10300" class="html-bibr">57</a>].</p>
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<p>The relationship between BSFC and engine load of algae oil biofuel mixtures with different proportions and traditional diesel fuel [<a href="#B63-sustainability-16-10300" class="html-bibr">63</a>].</p>
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<p>The relationship between BP, EGR rates and preheating temperatures of sunflower biofuel and traditional diesel fuel at 100% load [<a href="#B32-sustainability-16-10300" class="html-bibr">32</a>].</p>
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<p>The relationship between BP and engine speed of microalgae biofuel mixtures with different proportions and traditional diesel fuel [<a href="#B68-sustainability-16-10300" class="html-bibr">68</a>].</p>
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<p>The relationship between NO<sub>x</sub> emission and engine speed of soybean oil biofuel mixtures with different proportions and traditional diesel fuel [<a href="#B75-sustainability-16-10300" class="html-bibr">75</a>].</p>
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<p>The relationship between NO<sub>x</sub> emission and engine load of Chlorella protothecoides biofuel mixtures with different proportions and traditional diesel fuel [<a href="#B28-sustainability-16-10300" class="html-bibr">28</a>].</p>
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<p>Mode-wise percentage distribution of CO emissions for different fuels [<a href="#B95-sustainability-16-10300" class="html-bibr">95</a>].</p>
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<p>The relationship between CO emission and engine load of CSO mixtures with different proportions and traditional diesel fuel [<a href="#B99-sustainability-16-10300" class="html-bibr">99</a>].</p>
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<p>The relationship between CO<sub>2</sub> emission and engine load of Cymbopogon flexuosus biofuel mixtures with different proportions and traditional diesel fuel [<a href="#B102-sustainability-16-10300" class="html-bibr">102</a>].</p>
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<p>The relationship between CO<sub>2</sub> emission and engine load of SMB mixtures with different proportions [<a href="#B107-sustainability-16-10300" class="html-bibr">107</a>].</p>
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25 pages, 5047 KiB  
Article
Enhancing the Thermal Efficiency of Parabolic Trough Collectors by Using Annular Receivers for Low-Enthalpy Steam Generation
by Zuriel Aquino-Santiago, J. O. Aguilar, Guillermo Becerra-Núñez and O. A. Jaramillo
Processes 2024, 12(12), 2653; https://doi.org/10.3390/pr12122653 - 25 Nov 2024
Viewed by 105
Abstract
Parabolic Trough Collectors (PTCs) are a well-established technology for efficiently generating hot water and low-enthalpy steam. For instance, PTCs can be used in steam power systems to drive small Organic Rankine Cycles (ORCs). This study evaluated the thermal efficiency of a PTC equipped [...] Read more.
Parabolic Trough Collectors (PTCs) are a well-established technology for efficiently generating hot water and low-enthalpy steam. For instance, PTCs can be used in steam power systems to drive small Organic Rankine Cycles (ORCs). This study evaluated the thermal efficiency of a PTC equipped with a receiver tube featuring a concentric annular cross-section. This receiver design consists of a tube with a concentric rod inside, forming an annular gap through which the working fluid flows. A thermodynamic model was developed to assess the PTC’s thermal efficiency in hot water and low-enthalpy steam applications. The evaluation considered the First and Second Laws of Thermodynamics, factoring in environmental losses. The model included a bare receiver tube with three-rod diameters—3/8, 1/2, and 3/4 inches—and a range of volumetric flow rates from 1 to 6 L per minute. The results showed improved heat transfer with the annular cross-section receiver compared to a conventional circular one, particularly at lower flow rates of 1 and 2 L per minute. The highest increase in thermal efficiency was observed with the 3/4-inch rod at a flow rate of 1 L per minute, where the maximum efficiency reached 40%. Full article
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Figure 1
<p>Types of receiver tubes used; (<b>a</b>) Hollow tube and (<b>b</b>) concentric annular tube.</p>
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<p>Energy balance in a δ<sub>y</sub> tube element.</p>
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<p>Parabolic trough collector.</p>
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<p>Heat removal factor, (<math display="inline"><semantics> <msub> <mi>F</mi> <mi>r</mi> </msub> </semantics></math>) vs. mass flow (<math display="inline"><semantics> <mover accent="true"> <mi>m</mi> <mo>˙</mo> </mover> </semantics></math>).</p>
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<p>Thermal efficiency at constant mass flow of 1 <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>p</mi> <mi>m</mi> </mrow> </semantics></math>.</p>
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<p>Thermal efficiency at constant mass flow of 2 lpm.</p>
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<p>Thermal efficiency at constant mass flow of 3 lpm.</p>
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<p>Thermal efficiency at constant mass flow of 4 lpm.</p>
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<p>Thermal efficiency at constant mass flow of 5 <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>p</mi> <mi>m</mi> </mrow> </semantics></math>.</p>
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<p>Second Law thermal efficiency at constant mass flow of 1 <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>p</mi> <mi>m</mi> </mrow> </semantics></math>.</p>
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<p>Second Law thermal efficiency at constant mass flow of 2 <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>p</mi> <mi>m</mi> </mrow> </semantics></math>.</p>
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<p>Second Law thermal efficiency at constant mass flow of 3 <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>p</mi> <mi>m</mi> </mrow> </semantics></math>.</p>
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<p>Second Law thermal efficiency at constant mass flow of 4 <math display="inline"><semantics> <mrow> <mi>l</mi> <mi>p</mi> <mi>m</mi> </mrow> </semantics></math>.</p>
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<p>Second Law thermal efficiency at constant mass flow of 5 lpm.</p>
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36 pages, 8468 KiB  
Article
A Novel Magnetic Integration High-Efficiency Converter with Low Ripple and High Dynamic Response for the Hybrid Power Supply Systems of All-Electric Aircraft
by Li Chen, Haifeng Gao, Fengjie Shen, Yiyi Zhang, Liangjie Qiu and Lei Wang
Aerospace 2024, 11(12), 965; https://doi.org/10.3390/aerospace11120965 - 25 Nov 2024
Viewed by 166
Abstract
With the continuous improvement of battery energy density and converter power density, as well as the miniaturization and lightweighting of related airborne electrical equipment, all-electric aircraft with hybrid power supply systems provide more trade-off space and possibilities for the design of future aircraft. [...] Read more.
With the continuous improvement of battery energy density and converter power density, as well as the miniaturization and lightweighting of related airborne electrical equipment, all-electric aircraft with hybrid power supply systems provide more trade-off space and possibilities for the design of future aircraft. It is indispensable to search for a more valuable topology and apply it to airborne power supply. This paper proposes an airborne high-gain unidirectional DC-DC converter suitable for between low-voltage unit and high-voltage bus, which consists of interleaved magnetic integrated switched coupled inductor units and improved switch capacitor units. This paper first analyzes the steady-state operating characteristics under different modes; the new topology has higher voltage gain and lower stress. Secondly, in response to the challenges of high efficiency and high power density, we propose a magnetic integration design method and comprehensive experimental scheme based on the EIE-type magnetic core structure. This successfully integrates multiple discrete inductors into a single magnetic core. Furthermore, based on the comprehensive consideration of steady-state, transient performance and power density, the general design criteria for a high-gain switched coupled inductor are summarized through the equivalent mathematical model of reverse flux coupling. Additionally, by adjusting the coupling coefficient, the converter can achieve zero-voltage switching under light load conditions, demonstrating versatility and scalability and better meeting the application requirements of electric aircraft. The proposed prototype can provide voltage gain in the range of 12–22 times the input voltage gain by varying the input voltage from a 12–24 V fuel cell. The comprehensive performance of the converter, including steady-state, transient, and efficiency, was tested under D < 0.5 and D > 0.5. The experimental results show that the proposed converter possesses advantages such as high gain and low stress, a high dynamic response and low ripple, and high efficiency and high power density, which can provide a more advantageous DC-DC converter solution for airborne hybrid power supply systems. Full article
(This article belongs to the Special Issue Electric Power Systems and Components for All-Electric Aircraft)
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<p>Development planning and process of aircraft electrification technology.</p>
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<p>Schematic diagram of the structure and configuration of AEA power system based on a distributed electric propulsion architecture.</p>
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<p>The hybrid power supply system of AEA.</p>
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<p>Proposed high-gain boost converter with magnetic integrated switched coupled inductor and switched capacitor (<span class="html-italic">L</span><sub>1</sub> = <span class="html-italic">L</span><sub>2</sub> = <span class="html-italic">L</span><sub>3</sub> = <span class="html-italic">L</span><sub>4</sub> = <span class="html-italic">L</span>). (<b>a</b>) Main power topology of proposed converter. (<b>b</b>) Schematic diagram of 2-phase switched coupled inductor structure. (<b>c</b>) Equivalent circuit model of proposed 2-phase switched coupled inductor.</p>
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<p>Equivalent circuits and steady-state operating waveforms of each work modes (when 0 &lt; <span class="html-italic">D &lt;</span> 0.5). (<b>a</b>) Mode I, (<b>b</b>) Mode II and IV, (<b>c</b>) Mode III, (<b>d</b>) steady-state operating waveform of each work modes (when <span class="html-italic">D &lt;</span> 0.5).</p>
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<p>Equivalent circuits and steady-state operating waveforms of each work modes (when 0.5 &lt; <span class="html-italic">D &lt;</span> 1). (<b>a</b>) Mode I, (<b>b</b>) Mode II and IV, (<b>c</b>) Mode III, (<b>d</b>) steady-state operating waveform of each work modes (when 0.5 &lt; <span class="html-italic">D &lt;</span> 1).</p>
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<p>Comparison of gain curves between the proposed converter and other high gain converters. (<b>a</b>) 0 &lt; <span class="html-italic">D &lt;</span> 0.5, (<b>b</b>) 0.5 &lt; <span class="html-italic">D &lt;</span> 1 [<a href="#B28-aerospace-11-00965" class="html-bibr">28</a>,<a href="#B29-aerospace-11-00965" class="html-bibr">29</a>,<a href="#B31-aerospace-11-00965" class="html-bibr">31</a>,<a href="#B33-aerospace-11-00965" class="html-bibr">33</a>,<a href="#B34-aerospace-11-00965" class="html-bibr">34</a>].</p>
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<p>Under different <span class="html-italic">P</span> values, the variation of the voltage gain in pace with the duty ratio <span class="html-italic">D</span>.</p>
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<p>Contrast curve of voltage stress of output rectifier diode [<a href="#B28-aerospace-11-00965" class="html-bibr">28</a>,<a href="#B29-aerospace-11-00965" class="html-bibr">29</a>,<a href="#B31-aerospace-11-00965" class="html-bibr">31</a>,<a href="#B33-aerospace-11-00965" class="html-bibr">33</a>,<a href="#B34-aerospace-11-00965" class="html-bibr">34</a>].</p>
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<p>Equivalent inductance and steady-state current ripple with discrete inductor and coupled inductor.</p>
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<p>Ratio of current ripples under coupled and non-coupled stations.</p>
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<p>When the duty cycle increases by Δ<span class="html-italic">D</span>, the working waveforms are of transient inductor current. (<b>a</b>) Transient current of the uncoupled discrete inductor. (<b>b</b>) Transient current of the coupled inductor.</p>
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<p>Ratio of transient current increment under coupled and uncoupled stations.</p>
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<p>Normalization diagram of coupling coefficient and design criteria.</p>
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<p>The structure of the coupled inductors.</p>
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<p>Equivalent magnetic circuit.</p>
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<p>Dual transformation model.</p>
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<p>Magnetic equivalent circuit.</p>
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<p>Magnetic simulation of an EIE-coupled induct. (<b>a</b>) Proposed EIE-type coupled inductor structure. (<b>b</b>) Two-dimensional magnetic field vector diagram of coupled inductor core. (<b>c</b>) Working flux density of proposed EIE-type coupled inductor. (<b>d</b>) Air reluctance outside the coupled inductor winding and its calculation model. (<b>e</b>) Lateral view of the magnetic field lines for one inductor winding.</p>
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<p>Improved multi-phase switched coupled inductor and switched capacitor circuit. (<b>a</b>) Three-phase circuit. (<b>b</b>) N-phase circuit.</p>
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<p>Key waveforms of CRM operation for buck/boost converter. (<b>a</b>) The key waveforms of inductor current of CRM. (<b>b</b>) Main topology of synchronous rectification boost. (<b>c</b>) Buck direction. (<b>d</b>) Boost direction. (<b>e</b>) Single-phase inductor current work waveform of the proposed multi-phase converter.</p>
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<p>Simulation and comparative analysis of inductor current. (<b>a</b>) Comparison of phase current ripple in the steady-state phase between the coupled and uncoupled inductor. (<b>b</b>) Transient current waveforms of the coupled inductor. (<b>c</b>) Transient current waveforms of the uncoupled inductor.</p>
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<p>Comparison of simulation value and theoretical value of output voltage variation with load considering the influence of parasitic parameters. (<b>a</b>) Load adjustment characteristic diagram. (<b>b</b>) Simulation value and calculated value of duty cycle when load changes.</p>
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<p>Prototype and the experimental system.</p>
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<p>Inductor prototype. (<b>a</b>) Switched coupled inductor prototype. (<b>b</b>) Uncoupled inductor prototype.</p>
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<p>Steady-state experimental waveforms of the proposed converter with a switched coupled inductor (<span class="html-italic">D &lt;</span> 0.5). (<b>a</b>) Driving signal and the steady-state current waveform (when <span class="html-italic">t</span> = 2.5 μs/div). (<b>b</b>) Driving signal of and the steady-state current waveform (when <span class="html-italic">t</span> = 1 μs/div). (<b>c</b>) Driving signal, phase current waveform, and input and output voltage waveforms. (<b>d</b>) Phase current working waveforms (when <span class="html-italic">t</span> = 2.5 μs/div). (<b>e</b>) Phase current working waveforms (when <span class="html-italic">t</span> = 1 μs/div). (<b>f</b>) Driving signal and switching tube voltage waveforms. (<b>g</b>) Switching tube voltage waveform and input and output voltage waveforms. (<b>h</b>) Output voltage, diode voltage, and switched capacitor voltage waveforms.</p>
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<p>Phase current experimental waveform of uncoupled inductors. (<b>a</b>) Driving signal and the steady-state current waveform (when <span class="html-italic">t</span> = 2.5 μs/div). (<b>b</b>) Driving signal of and the steady-state current waveform (when <span class="html-italic">t</span> = 1 μs/div).</p>
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<p>Steady-state experimental waveforms of a switched coupled inductor (<span class="html-italic">D &gt;</span> 0.5). (<b>a</b>) Driving signal and the steady-state current waveform (when <span class="html-italic">t</span> = 2.5 μs/div). (<b>b</b>) Driving signal of and the steady-state current waveform (when <span class="html-italic">t</span> = 1 μs/div). (<b>c</b>) Driving signal, phase current waveform, and input and output voltage waveforms. (<b>d</b>) Phase current working waveforms (when <span class="html-italic">t</span> = 2.5 μs/div). (<b>e</b>) Driving signal and switching tube voltage waveforms. (<b>f</b>) Output voltage, diode voltage, and switched capacitor voltage waveforms.</p>
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<p>Transient current waveforms of a converter with/without coupled inductors when Δ<span class="html-italic">D</span> = 0.05 (<span class="html-italic">D &lt;</span> 0.5). (<b>a</b>) Transient current increment of coupled inductors (<b>b</b>) Transient current increment of uncoupled inductors.</p>
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<p>Transient current waveforms of a converter with/without coupled inductors when Δ<span class="html-italic">D</span> = 0.05 (<span class="html-italic">D &gt;</span> 0.5). (<b>a</b>) Transient current increment of coupled inductors (<b>b</b>) Transient current increment of uncoupled inductors.</p>
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<p>The soft switching operating waveform. (<b>a</b>) Driving signal, phase current, and switching tube voltage waveforms with s coupled inductor (when <span class="html-italic">t</span> = 1 μs/div). (<b>b</b>) Driving signal, phase current, and switching tube voltage waveforms with a coupled inductor (when <span class="html-italic">t</span> = 50 ns/div). (<b>c</b>) Driving signal, phase current, and switching tube voltage waveforms with an uncoupled inductor (when <span class="html-italic">t</span> = 1 μs/div). (<b>d</b>) Driving signal, phase current, and switching tube voltage waveforms with an uncoupled inductor (when <span class="html-italic">t</span> = 50 ns/div).</p>
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<p>Efficiency contrast curve.</p>
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8 pages, 3626 KiB  
Communication
Analysis and Design of Low-Noise Radio-Frequency Power Amplifier Supply Modulator for Frequency Division Duplex Cellular Systems
by Ji-Seon Paek
Electronics 2024, 13(23), 4635; https://doi.org/10.3390/electronics13234635 - 25 Nov 2024
Viewed by 160
Abstract
This paper describes an analysis of power supply rejection and noise improvement techniques for an envelope-tracking power amplifier. Although the envelope-tracking technique improves efficiency, its power supply rejection ratio is much lower than that of average power tracking or a fixed-supply power amplifier. [...] Read more.
This paper describes an analysis of power supply rejection and noise improvement techniques for an envelope-tracking power amplifier. Although the envelope-tracking technique improves efficiency, its power supply rejection ratio is much lower than that of average power tracking or a fixed-supply power amplifier. In FDD systems with the envelope-tracking technique, the low power supply rejection ratio generates much output noise in the RX band and degrades the receiver’s sensitivity. An SM is designed by using a 130 nm CMOS process, and the chip die area is 2 × 2 mm2 with a 25-pin wafer-level chip-scale package. The designed SM achieved peak efficiencies of 78–83% for LTE signals with a 5.8 dB PAPR and various channel bandwidths. For the low-output-noise-supply modulator, noise reduction techniques using resonant-frequency tuning and a notch filter are employed, and the measured results show maximum 1.8/5/5.3/3.8/3 dB noise reduction in LTE bands B17/B5/B2/B3/B7, respectively. Full article
(This article belongs to the Special Issue Millimeter-Wave/Terahertz Integrated Circuit Design)
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<p>RX-band noise transfer from ET PA in FDD system.</p>
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<p>PSRR of PA in linear and saturated regions near P1dB.</p>
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<p>Simulated gain and PSRRSSB curves of APT and ET.</p>
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<p>Simulated PAE, gain, and calculated PSRRSSB curves of PA at each supply voltage (1 V to 3.5 V with 0.5 V step).</p>
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<p>Average PAE, gain, output power, and PSRRSSB according to saturation level in ET operation.</p>
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<p>Block diagram of the hybrid switching supply modulator.</p>
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<p>SM output open-loop noise model and noise contribution depending on frequency offset.</p>
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<p>Proposed noise reduction techniques: (<b>a</b>) resonant-frequency tuning (RFT); (<b>b</b>) notch filter.</p>
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<p>PSRR measurement setup and chip photograph.</p>
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<p>Measured output noise of the designed supply modulator in the cases of reference sensitivity QPSK PREFSENS (Table 7.3.1-1 in [<a href="#B5-electronics-13-04635" class="html-bibr">5</a>]) for each LTE band.</p>
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21 pages, 2215 KiB  
Article
Peculiarities of Plant Mineral Composition in Semi-Desert Conditions
by Nadezhda Golubkina, Sergey Sheshnitsan, Andrew Koshevarov, Nikolay Pirogov, Ulyana Plotnikova, Alessio Vincenzo Tallarita, Otilia Cristina Murariu, Luca Merlino and Gianluca Caruso
Int. J. Plant Biol. 2024, 15(4), 1229-1249; https://doi.org/10.3390/ijpb15040085 (registering DOI) - 25 Nov 2024
Viewed by 181
Abstract
Plant–soil interactions in semi-desert conditions elicit the development of plant-specific adaptation strategies, including selective accumulation of macro- and microelements. Using an ICP-MS analysis of 12 plant species belonging to Asteraceae, Fabaceae, Poaceae, Ephedraceae, Amarantaceae, and Lamiaceae families of the Baskunchak Nature Reserve, remarkable [...] Read more.
Plant–soil interactions in semi-desert conditions elicit the development of plant-specific adaptation strategies, including selective accumulation of macro- and microelements. Using an ICP-MS analysis of 12 plant species belonging to Asteraceae, Fabaceae, Poaceae, Ephedraceae, Amarantaceae, and Lamiaceae families of the Baskunchak Nature Reserve, remarkable species differences in accumulation of 22 macro- and microelements were recorded. The most common Artemisia species and Poaceae representatives belong to two different groups of plants with high content of Na, K, Zn, Cu, V and high antioxidant status and low Si typical for the former group and the opposite characteristics for the latter one. The mentioned phenomenon indicates two diverse powerful adaptation mechanisms based on the antioxidant defense and Si protection, respectively. The high frequency of remarkable levels of Se in plants with BCF exceeding 1 (Glycyrrhiza aspera, Phlomis pungens, Tanacetum nullifolium, Helichrysum nogaicum, and Jurinea ewersmannii), Zn in all species except Poa angustifolia, and Cu in the Asteraceae plants Phlomis pungens and Krascheninnikovia ceratoides suggests the significance of these elements in plant tolerance to environmental stresses. Plant–soil positive correlations were recorded for Sr (r = 0.866; p < 0.001); plant Sr, Fe, Co, Pb levels and soil salinity (r = 0.763, p < 0.001; r = 0.606, p < 0.03; r = 0.627, p < 0.02; r = 0.548, p < 0.05, respectively); and Cr only for Asteraceae species (r = 0.986, p < 0.001). The results obtained in this research may be used in plant adaptability evaluation in conditions of environmental stress. Full article
(This article belongs to the Section Plant Physiology)
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Figure 1
<p>Sampling sites at the territory of the Bogdinsko-Baskunchak Nature Reserve. BNR: the Bogdinsko-Baskunchak Nature Reserve; Bogdo: the Big Bogdo mountain. The numbers indicate sampling places whose geographical coordinates are presented in <a href="#ijpb-15-00085-t001" class="html-table">Table 1</a> and <a href="#ijpb-15-00085-t002" class="html-table">Table 2</a>.</p>
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<p>Mean monthly temperature (<b>A</b>) and precipitation (<b>B</b>) in 2021–2022, compared to the basic long-term values.</p>
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<p>Antioxidant activity (AOA) and polyphenol content (TP) in plants of the Baskunchak Nature Reserve. For each parameter, values with the same letters do not differ statistically according to Duncan’s test at <span class="html-italic">p</span> &lt; 0.05.</p>
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<p>Correlation between soil and plant Sr levels at the BNR and the Bogdo mountain (r = 0.866, <span class="html-italic">p</span> &lt; 0.001). The linear relationship is based on data for all studied plant species (<span class="html-italic">n</span> = 12) and corresponding soil samples.</p>
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<p>Principal component analysis (PCA).</p>
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19 pages, 3994 KiB  
Article
Strengthening of Reinforced Concrete Hydraulic Structures with External Reinforcement System Made of Carbon Fiber-Based Composite Materials with Development of Calculation Recommendations
by Oleg Rubin, Dmitry Kozlov, Anton Antonov and Junhao Zhang
Buildings 2024, 14(12), 3739; https://doi.org/10.3390/buildings14123739 - 24 Nov 2024
Viewed by 313
Abstract
During the long-term operation of hydraulic structures under the action of complex loads and impacts, non-design changes occur, which lead to a decrease in the bearing capacity and safety and, accordingly, to the need for structural reinforcements. Experiments were conducted to study the [...] Read more.
During the long-term operation of hydraulic structures under the action of complex loads and impacts, non-design changes occur, which lead to a decrease in the bearing capacity and safety and, accordingly, to the need for structural reinforcements. Experiments were conducted to study the strengthening of reinforced concrete models of hydraulic structures with interblock construction joints (located in two directions) and with the low longitudinal reinforcement coefficients typical of hydraulic structures (μs = 0.0039 and μs = 0.0083), using the low concrete classes B15 and B25. These structures were strengthened using external reinforcement with carbon ribbons of the FibArm 530/300 type. The results revealed an increase in the bearing capacity (by 1.355- and 1.66-fold); accordingly, the high efficiency of this strengthening method for reinforced concrete hydraulic structures was proven. Using the results of these experiments, including the obtained special characteristic of the cracking of reinforced concrete structures and the results of studies by other authors, recommendations for calculations involving reinforced concrete hydraulic engineering structures strengthened with an external reinforcement system of carbon-fibre-based composite materials were developed and proposed. Carbon-fibre-based composite materials are used as elements of external reinforcement for building structures (unidirectional—tapes, bidirectional—meshes and fabrics). The calculation recommendations proposed by the authors can be taken into account for the creation of a regulatory framework for hydropower facilities, including hydroelectric power plants and pumped-storage power plants. They justify the use of an external reinforcement system made with carbon-fibre-based composite materials to strengthen hydraulic structures in operation and provide an increased level of safety for reinforced concrete structures and constructions. Full article
(This article belongs to the Section Building Materials, and Repair & Renovation)
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Figure 1

Figure 1
<p>Reinforcement schemes for RC models with vertical and horizontal interblock construction joints: (<b>a</b>) B-I15-2.1; (<b>b</b>) B-I15-2.2; (<b>c</b>) B-I25-1.1.</p>
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<p>(<b>a</b>–<b>c</b>) Schemes of beam-type model reinforcement with carbon tapes: 1—interblock construction joints; 2—150 mm wide carbon tape (2 layers); 3—150 mm wide carbon tape anchoring ties; 4—50 mm wide carbon tape ties; 5—carbon tape ties in the shear span.</p>
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<p>The view of the beam-type model reinforced with carbon composite tapes.</p>
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<p>Scheme of typical cracks in the experimental models during the first stage of tests without reinforcement: (<b>a</b>) B-15-2.1, (<b>b</b>) B-I15-2.2, and (<b>c</b>) B-I25-1.1.</p>
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<p>Fracture crack patterns of reinforced experimental beams during the second stage of the study: (<b>a</b>) B-15-2.1, (<b>b</b>) B-I15-2.2, and (<b>c</b>) B-I25-1.1.</p>
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<p>The width of the vertical normal cracks opening in the middle part of the span of the models.</p>
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<p>The opening width of the vertical interblock joint.</p>
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<p>Force diagram for the calculation regarding the vertical section of a bending reinforced concrete structure externally reinforced with composite materials.</p>
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<p>Scheme of force action when calculating a concrete structure reinforced with external reinforcement made of composite materials on an inclined section for the action of shear forces: 1—vertical joint; 2—horizontal joint; 3—inclined crack.</p>
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18 pages, 3843 KiB  
Article
EC-WAMI: Event Camera-Based Pose Optimization in Remote Sensing and Wide-Area Motion Imagery
by Isaac Nkrumah, Maryam Moshrefizadeh, Omar Tahri, Erik Blasch, Kannappan Palaniappan and Hadi AliAkbarpour
Sensors 2024, 24(23), 7493; https://doi.org/10.3390/s24237493 - 24 Nov 2024
Viewed by 274
Abstract
In this paper, we present EC-WAMI, the first successful application of neuromorphic event cameras (ECs) for Wide-Area Motion Imagery (WAMI) and Remote Sensing (RS), showcasing their potential for advancing Structure-from-Motion (SfM) and 3D reconstruction across diverse imaging scenarios. ECs, which detect asynchronous [...] Read more.
In this paper, we present EC-WAMI, the first successful application of neuromorphic event cameras (ECs) for Wide-Area Motion Imagery (WAMI) and Remote Sensing (RS), showcasing their potential for advancing Structure-from-Motion (SfM) and 3D reconstruction across diverse imaging scenarios. ECs, which detect asynchronous pixel-level brightness changes, offer key advantages over traditional frame-based sensors such as high temporal resolution, low power consumption, and resilience to dynamic lighting. These capabilities allow ECs to overcome challenges such as glare, uneven lighting, and low-light conditions that are common in aerial imaging and remote sensing, while also extending UAV flight endurance. To evaluate the effectiveness of ECs in WAMI, we simulate event data from RGB WAMI imagery and integrate them into SfM pipelines for camera pose optimization and 3D point cloud generation. Using two state-of-the-art SfM methods, namely, COLMAP and Bundle Adjustment for Sequential Imagery (BA4S), we show that although ECs do not capture scene content like traditional cameras, their spike-based events, which only measure illumination changes, allow for accurate camera pose recovery in WAMI scenarios even in low-framerate(5 fps) simulations. Our results indicate that while BA4S and COLMAP provide comparable accuracy, BA4S significantly outperforms COLMAP in terms of speed. Moreover, we evaluate different feature extraction methods, showing that the deep learning-based LIGHTGLUE descriptor consistently outperforms traditional handcrafted descriptors by providing improved reliability and accuracy of event-based SfM. These results highlight the broader potential of ECs in remote sensing, aerial imaging, and 3D reconstruction beyond conventional WAMI applications. Our dataset will be made available for public use. Full article
(This article belongs to the Section Physical Sensors)
9 pages, 6197 KiB  
Article
Array of Graphene Solar Cells on 100 mm Silicon Wafers for Power Systems
by Syed M. Rahman, Md R. Kabir, Tamzeed B. Amin, James M. Mangum, Ashaduzzaman and Paul M. Thibado
Energies 2024, 17(23), 5895; https://doi.org/10.3390/en17235895 - 24 Nov 2024
Viewed by 232
Abstract
High electrical conductivity and optical transparency make graphene a suitable candidate for photovoltaic-based power systems. In this study, we present the design and fabrication of an array of graphene-based Schottky junction solar cells. Using mainstream semiconductor manufacturing methods, we produced 96 solar cells [...] Read more.
High electrical conductivity and optical transparency make graphene a suitable candidate for photovoltaic-based power systems. In this study, we present the design and fabrication of an array of graphene-based Schottky junction solar cells. Using mainstream semiconductor manufacturing methods, we produced 96 solar cells from a single 100 mm diameter silicon wafer that was precoated with an oxide layer. The fabrication process involves removing the oxide layer over a select region, depositing metal contacts on both the oxide and bare silicon regions, and transferring large-area graphene onto the exposed silicon to create the photovoltaic interface. A single solar cell can provide up to 160 μA of short-circuit current and up to 0.42 V of open-circuit voltage. A series of solar cells are wired to recharge a 3 V battery intermittently, while the battery continuously powers a device. The solar cells and rechargeable battery together form a power system for any 3-volt low-power application. Full article
(This article belongs to the Section A2: Solar Energy and Photovoltaic Systems)
27 pages, 2757 KiB  
Article
Energy, Exergy, and Economic Performance Comparison and Parametric Optimization of Organic Rankine Cycles Using Isobutane, Isopentane, and Their Mixtures for Waste Heat Recovery
by Junsheng Feng, Yaru Yan, Liang Zhao and Hui Dong
Energies 2024, 17(23), 5893; https://doi.org/10.3390/en17235893 - 24 Nov 2024
Viewed by 202
Abstract
The possibility of applying the organic Rankine cycle (ORC) to further recycle the low-grade waste heat efficiently is studied in the present work. The energy, exergy, and economic models of the ORC system are established, and the isobutane, isopentane, and their mixtures are [...] Read more.
The possibility of applying the organic Rankine cycle (ORC) to further recycle the low-grade waste heat efficiently is studied in the present work. The energy, exergy, and economic models of the ORC system are established, and the isobutane, isopentane, and their mixtures are selected as the organic working mediums (OWMs). Due to the slip characteristics of mixed OWM, four operational conditions of the ORC system are proposed, and then the contrastive analysis of energy, exergy, and economic performances under the four operational conditions are conducted. Finally, the optimal mixture mass fraction and crucial parameters of the ORC system are separately determined through the bi-objective optimization. The results show that the ORC system using the mixed OWM can achieve a larger net power output and exergy efficiency by comparing the pure OWM when the condensing temperature is set as the saturated vapor temperature during the condensation process. The electricity production cost first rises and then decreases with the rising mass fraction of isobutane in mixed OWM, and the ORC system using the isopentane can achieve the smallest electricity production cost. By taking the low-grade flue gas of 433.15 K as the ORC heat source, four operational conditions have the same optimal ORC crucial parameters, namely the evaporating temperature of 393.15 K, condensing temperature of 308.15 K, and superheat degree of 0 K. The pure OWM of isobutane can achieve better overall performance by setting the condensing temperature as the saturated liquid temperature. Full article
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