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Search Results (1,708)

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29 pages, 7079 KiB  
Article
Comparison of Ferronickel Alloys Produced via Microwave and Conventional Thermal Concentration of Pyrrhotite Tailings
by Michael Jaansalu and Christopher Pickles
Minerals 2025, 15(3), 196; https://doi.org/10.3390/min15030196 (registering DOI) - 20 Feb 2025
Abstract
In modern nickel mineral processing operations, the aim is to separate pentlandite from gangue minerals. One of these gangue minerals, pyrrhotite, contains up to 1 wt% Ni but is disposed of as waste, i.e., as tailings. Declining sulfide ore grades and increasing nickel [...] Read more.
In modern nickel mineral processing operations, the aim is to separate pentlandite from gangue minerals. One of these gangue minerals, pyrrhotite, contains up to 1 wt% Ni but is disposed of as waste, i.e., as tailings. Declining sulfide ore grades and increasing nickel demand have led to renewed interest in extracting nickel from pyrrhotite tails. One proposed process is thermal concentration, which aims to recover the nickel as a ferronickel alloy via thermal treatment at temperatures greater than 900 °C. Achieving these temperatures requires substantial energy input as the reactions involved are highly endothermic. In the present research, microwave radiation was used to process a reaction mixture consisting of a concentrate of pyrrhotite tails, iron ore, and metallurgical coke. The fundamental property that determines the interaction of microwaves with a material is complex permittivity. It was found that the reaction mixture had very high real and imaginary permittivities, making it a good candidate for microwave treatment. An input power of 800 W of microwave radiation (2450 MHz) was then employed to heat various reaction mixtures for thermal treatment times of 120, 300, and 600 s. The ferroalloy grades (6–7.5 wt% Ni) were comparable to those produced by conventional heating and to those obtained by other authors using conventional heating techniques. The microwaved samples had increased metallization of nickel, which was attributed to increased melting due to the higher internal temperatures. Full article
(This article belongs to the Section Mineral Processing and Extractive Metallurgy)
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<p>Flowsheet of upgrading the pyrrhotite tails and the preparation of Reaction Mixtures A, B, and C.</p>
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<p>Schematic of microwave system.</p>
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<p>Schematic of Vycor reactor used during microwave tests.</p>
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<p>Schematic of the tube furnace used for the conventional tests.</p>
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<p>Alloy nickel grade as a function of temperature for Reaction Mixtures A, B, and C. Cover gas is 175 Nm<sup>3</sup> of N<sub>2</sub> at 1 bar.</p>
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<p>Average TGA data of Reaction Mixtures A, B, and C. Data plotted are the average of triplicate tests performed under nitrogen at a heating rate of 10 K/min.</p>
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<p>DTGA of the average TGA data from <a href="#minerals-15-00196-f006" class="html-fig">Figure 6</a> of Reaction Mixtures A, B, and C.</p>
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<p>Relative real (<b>A</b>) and imaginary (<b>B</b>) permittivities of Mixture A as a function of temperature at frequencies between 397 and 2463 MHz. The initial sample density was 2.45 ± 0.1 g/cm<sup>3</sup>.</p>
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<p>Penetration depth of Mixture A as a function of temperature at frequencies between 397 and 2463 MHz.</p>
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<p>Inferred temperature distributions of microwaved samples.</p>
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<p>Absorbed microwave energy distributions for microwaved samples.</p>
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<p>Inferred temperature as a function of microwave energy absorbed (%) for the various sample mixtures and processing times.</p>
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<p>Distribution of alloy particle Ni grades after 300 s of microwave treatment. Dots indicate outlier alloy particle compositions.</p>
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<p>Very small (&lt;5 μm) alloy particles disseminated in sulfides in Reaction Mixture A after 300 s of treatment time.</p>
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<p>Intergranular alloy particles mixed with sulfides in Reaction Mixture C after 300 s of treatment time.</p>
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<p>Alloy dendrites observed in a Reaction Mixture B briquette after 300 s of treatment time.</p>
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<p>Alloy dendrites in a Reaction Mixture C briquette after microwave treatment for 600 s.</p>
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<p>Medium-Ni (<b>A</b>) and high-Ni (<b>B</b>) alloy particles observed in a Mixture B briquette treated at 900 °C for 35 min.</p>
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<p>Elemental mapping of an oxide/sulfide/alloy bead produced from Reaction Mixture C following 10 min of thermal treatment at 1200 °C.</p>
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22 pages, 16223 KiB  
Article
Sustainable Insulating Materials for High-Voltage Equipment: Dielectric Properties of Green Synthesis-Based Nanofluids from Vegetable Oils
by Abubakar Siddique, Muhammad Usama Shahid, Waseem Aslam, Shahid Atiq, Mohammad R. Altimania, Hafiz Mudassir Munir, Ievgen Zaitsev and Vladislav Kuchanskyy
Sustainability 2025, 17(4), 1740; https://doi.org/10.3390/su17041740 (registering DOI) - 19 Feb 2025
Abstract
This study aimed to develop a cost-effective, environmentally sustainable, and technologically advanced dielectric fluid by utilizing the beneficial properties of natural ester-based vegetable oils, offering a promising alternative for transformer insulation and cooling applications. The novelty of this research lies in the formulation [...] Read more.
This study aimed to develop a cost-effective, environmentally sustainable, and technologically advanced dielectric fluid by utilizing the beneficial properties of natural ester-based vegetable oils, offering a promising alternative for transformer insulation and cooling applications. The novelty of this research lies in the formulation of a nanofluid that combines three distinct vegetable oils—castor, flaxseed, and blackseed—creating a unique base fluid. SiO2 nanoparticles were incorporated into the fluid to leverage their multiple advantageous characteristics. Extensive experiments were conducted to evaluate the superior properties of the proposed nanofluid, focusing on key dielectric properties, such as relative permittivity (εr) and the dielectric dissipation factor (tan δ). Comparative analyses with conventional mineral oil, which was used as a benchmark, demonstrated the significant advantages of the vegetable oil-based nanofluid. The novel formulation outperformed all other tested samples, highlighting its exceptional performance. Additionally, three preparation methods were examined, with the green synthesis technique producing the nanofluid with better dielectric properties. Through a detailed presentation of empirical data and compelling arguments, this study confirms the potential of natural ester-based vegetable oil nanofluids as a highly promising alternative, driven by their intrinsic properties and the environmentally friendly synthesis method employed. Full article
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<p>Preparation method of base fluid.</p>
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<p>One-step method for preparation of nanofluids.</p>
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<p>Two-step method for preparation of nanofluids.</p>
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<p>Sol-gel method for preparing nanoparticles.</p>
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<p>Green synthesis method for preparing nanoparticles.</p>
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<p>Experimental setup for evaluation of relative permittivity (<span class="html-italic">ε<sub>r</sub></span>).</p>
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<p>(<b>A</b>) BDV of GS. (<b>B</b>) BDV of MO.</p>
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<p>Measured capacitance value of all test samples.</p>
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<p><span class="html-italic">ε<sub>r</sub></span> comparison of test samples.</p>
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<p>(<b>A</b>) Experimental setup for evaluation of dissipation factor/tan <span class="html-italic">δ</span>, (<b>B</b>) control diagram for current comparison.</p>
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<p>(<b>A</b>) High-voltage laboratory overview, (<b>B</b>) measuring arrangement for dissipation factor (tan <span class="html-italic">δ</span>).</p>
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<p>Dielectric liquids under tan <span class="html-italic">δ</span> test: (<b>A</b>) proposed nanofluid, (<b>B</b>) traditional mineral oil.</p>
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<p>Measured tan <span class="html-italic">δ</span> values of all test samples.</p>
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<p>Tan <span class="html-italic">δ</span> comparison of test samples.</p>
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22 pages, 6031 KiB  
Article
Investigation of the Electrical Properties of Polycrystalline Crednerite CuMn1−xMgxO2 (x = 0–0.06)-Type Materials in a Low-Frequency Field
by Iosif Malaescu, Maria Poienar and Catalin N. Marin
Crystals 2025, 15(2), 184; https://doi.org/10.3390/cryst15020184 - 14 Feb 2025
Abstract
CuMn1−xMgxO2 (x = 0–0.06) polycrystalline samples were prepared using the hydrothermal method at T = 100 °C for 24 h in Teflon-line stainless steel autoclaves. The samples were crystallized, forming crednerite structures (C2/m space group), and the Mg [...] Read more.
CuMn1−xMgxO2 (x = 0–0.06) polycrystalline samples were prepared using the hydrothermal method at T = 100 °C for 24 h in Teflon-line stainless steel autoclaves. The samples were crystallized, forming crednerite structures (C2/m space group), and the Mg2+ substitution onto the Mn3+ site induced small changes in the unit cell parameters and volume. Based on complex impedance measurements made between 20 Hz and 2 MHz, at different concentrations of Mg ions (x), the electrical conductivity (σ), the electric modulus (M), and the complex dielectric permittivity (ε) were determined. The conductivity spectrum, σ(f, x), follows the Jonscher universal law and enables the determination of the static conductivity (σDC) of the samples. The results showed that, when increasing the concentration x from 0 to 6%, σDC varied from 15.36 × 10−5 S/m to 16.42 × 10−5 S/m, with a minimum of 4.85 × 10−5 S/m found at a concentration of x = 4%. Using variable range hopping (VRH) and correlated barrier hopping (CBH) theoretical models, the electrical mechanism in the samples was explained. The band gap energy (Wm), charge carrier mobility (μ), number density (NC) of effective charge carriers, and hopping frequency (ωh) were evaluated at different concentrations (x) of substitution with Mg. In addition, using measurements of the temperature dependence of σDC(T) between 300 and 400 K, the thermal activation energy (EA) of the samples was evaluated. Additionally, the dielectric behavior of the samples was explained by the interfacial relaxation process. This knowledge of the electrical properties of the CuMn1−xMgxO2 (x = 0–0.06) polycrystalline crednerite is of interest for their use in photocatalytic, electronic, or other applications. Full article
(This article belongs to the Section Inorganic Crystalline Materials)
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<p>(<b>a</b>) Superposition of XRD patterns of CuMn1−xMg<sub>x</sub>O<sub>2</sub> (x = 0, x = 0.02, x = 0.04, and x = 0.06); experimental X-ray powder diffraction pattern (black line) and calculated pattern (red line) of CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> ((<b>b</b>) for x = 0, (<b>c</b>) for x 0.02, (<b>d</b>) for x = 0.04, and (<b>e</b>) for x = 0.06). In (<b>b</b>–<b>e</b>), the upper row of vertical marks corresponds to Bragg reflections of phase 1 (crednerite phase), and the lower row corresponds to phase 2 (CuO phase), which are indicated by the horizontal arrows.</p>
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<p>Room-temperature Raman spectra for CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> materials with x = 0, 0.02, 0.04, and 0.06.</p>
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<p>The frequency dependence of <span class="html-italic">Z′</span> (<b>a</b>) and <span class="html-italic">Z″</span> (<b>b</b>) components of the complex impedance of measurement cell, which was filled with CuMn<sub>1−x</sub> Mg<sub>x</sub>O<sub>2</sub> and measured at room temperature.</p>
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<p>The frequency dependence of the conductivity, σ, at different concentrations, x, of Mg substituted into the CuMnO<sub>2</sub> crednerite material, at room temperature.</p>
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<p>The <span class="html-italic">lnσ<sub>AC</sub>(lnω)</span> dependence at different concentrations, x, of Mg substituted into CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> samples.</p>
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<p>The concentration dependence of the ratio (<span class="html-italic">–lnA<sub>0</sub></span>/<span class="html-italic">n</span>) in CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> crednerite at room temperature.</p>
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<p>The concentration dependence of the band gap energy (<span class="html-italic">W<sub>m</sub></span>) for the CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> samples.</p>
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<p>Temperature dependence of the static conductivity, <span class="html-italic">σ<sub>DC</sub></span>(<span class="html-italic">T</span>), of crednerite CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> samples for different concentrations (x) of substituted Mg.</p>
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<p>The <span class="html-italic">ln(σ<sub>DC</sub>)(T<sup>−1</sup></span><sup>/<span class="html-italic">4</span></sup><span class="html-italic">)</span> plots of CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> crednerite samples for different concentration values (x) of substituted Mg, which agree with the VRH model.</p>
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<p>The concentration dependence of the charge carrier’s mobility (<span class="html-italic">μ</span>) from the CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> crednerite samples at room temperature.</p>
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<p>The frequency dependence of the <span class="html-italic">M′</span> and <span class="html-italic">M″</span> components of the electric modulus of the CuMn<sub>1−x</sub>Mg<sub>x</sub>O<sub>2</sub> crednerite samples at different concentration values (x) of substituted Mg.</p>
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<p>The frequency dependence of the <span class="html-italic">M″</span> component in samples at different values of x. The inset figure shows an equivalent electric circuit for the sample.</p>
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<p>The frequency dependence of the real, ε′, and imaginary, ε″, components of the complex dielectric permittivity at different values of the concentration of substituted Mg (x).</p>
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<p>Frequency dependence of the real, εʹ, and imaginary components, <math display="inline"><semantics> <mrow> <msubsup> <mi>ε</mi> <mrow> <mi>r</mi> <mi>e</mi> <mi>l</mi> </mrow> <mo>″</mo> </msubsup> </mrow> </semantics></math>, due to dielectric relaxation, for different concentration values (x) of substituted Mg.</p>
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14 pages, 3637 KiB  
Article
Conducting Rubber Anisotropy of Electrophysical and Mechanical Properties
by Stanislav Makhno, Xianpeng Wan, Oksana Lisova, Petro Gorbyk, Dongxing Wang, Hao Tang, Yuli Shi, Mykola Kartel, Kateryna Ivanenko, Sergii Hozhdzinskyi, Galyna Zaitseva, Maksym Stetsenko and Yurii Sementsov
Polymers 2025, 17(4), 492; https://doi.org/10.3390/polym17040492 - 14 Feb 2025
Abstract
The aim of this work was to determine the anisotropy of the electrophysical and mechanical properties of rubber reinforced with a hybrid filler CNTs&CB (carbon nanotubes and carbon black) as a function of CNT content and the technological parameters of the production process. [...] Read more.
The aim of this work was to determine the anisotropy of the electrophysical and mechanical properties of rubber reinforced with a hybrid filler CNTs&CB (carbon nanotubes and carbon black) as a function of CNT content and the technological parameters of the production process. A significant difference in electrical conductivity (σ) and dielectric permittivity (ε) in three perpendicular directions was found for CNT concentrations ranging from 0 to 0.007 in volume fraction. The highest values of σ and ε were observed in the calendering direction, with slightly lower values in the perpendicular direction. This effect was attributed to the orientation of polymer molecules and CNTs along the direction of movement during calendering, as well as the disruption of the cluster structure in the transverse direction. Although the calculated percolation threshold values of the investigated system differed slightly, a correlation was observed between the mechanical and electrophysical properties of CNTs&CB rubber. This correlation enables rubber products to be designed with optimal properties tailored to the desired direction. Full article
(This article belongs to the Special Issue Polymer Composites: Structure, Properties and Processing, 2nd Edition)
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<p>(<b>a</b>) TEM image of CNTs; SEM images: (<b>b</b>) agglomerations of CNTs, (<b>c</b>) carbon black, (<b>d</b>) composite CB+CNTs, and (<b>e</b>,<b>f</b>) cross-sectional view of the rubber compound.</p>
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<p>(<b>a</b>) TEM image of CNTs; SEM images: (<b>b</b>) agglomerations of CNTs, (<b>c</b>) carbon black, (<b>d</b>) composite CB+CNTs, and (<b>e</b>,<b>f</b>) cross-sectional view of the rubber compound.</p>
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<p>Scheme for measuring electrophysical and mechanical characteristics.</p>
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<p>Dependence of electrical conductivity (<b>a</b>) and dielectric permittivity (<b>b</b>) at 100 Hz on the content of CNTs in three perpendicular directions of measurement: Curve 1—in the direction of calendering; Curve 2—perpendicularly, in the same plane; Curve 3—perpendicular to the calendering plane.</p>
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<p>Dependence of electrical conductivity (<b>a</b>,<b>c</b>,<b>e</b>) and dielectric permittivity (<b>b</b>,<b>d</b>,<b>f</b>) on frequency in three perpendicular directions of measurement: (<b>a</b>,<b>b</b>) in the direction of calendering; (<b>c</b>,<b>d</b>) perpendicularly, in the same plane; (<b>e</b>,<b>f</b>) perpendicular to the calendering plane. For the content of CNT: 0 (Curve 0), 0,00035 (Curve 1), 0,00069 (Curve 2), 0,00104 (Curve 3), 0,0014 (Curve 4) v.f. to the entire composite.</p>
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<p>Dependence of electrical conductivity (<b>a</b>,<b>c</b>,<b>e</b>) and dielectric permittivity (<b>b</b>,<b>d</b>,<b>f</b>) on frequency in three perpendicular directions of measurement: (<b>a</b>,<b>b</b>) in the direction of calendering; (<b>c</b>,<b>d</b>) perpendicularly, in the same plane; (<b>e</b>,<b>f</b>) perpendicular to the calendering plane. For the content of CNT: 0 (Curve 0), 0,00035 (Curve 1), 0,00069 (Curve 2), 0,00104 (Curve 3), 0,0014 (Curve 4) v.f. to the entire composite.</p>
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<p>Dependence of the real (<b>a</b>) and imaginary (<b>b</b>) components of the complex dielectric permittivity on the content of CNTs in three perpendicular directions of measurement: Curve 1—in the direction of calendering; Curve 2—perpendicularly, in the same plane; Curve 3—perpendicular to the calendering plane.</p>
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<p>Dependence of the relative tensile strength on the content of CNTs in three perpendicular measurement directions: Curve 1—in the direction of calendering; Curve 2—perpendicularly, in the same plane; Curve 3—perpendicular to the calendering plane.</p>
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13 pages, 8457 KiB  
Article
Electromagnetic Properties of Natural Plant Leaves for Eco-Friendly and Biodegradable Substrates for Wireless IoT Devices
by Nikolay Todorov Atanasov, Blagovest Nikolaev Atanasov and Gabriela Lachezarova Atanasova
Sensors 2025, 25(4), 1118; https://doi.org/10.3390/s25041118 - 12 Feb 2025
Abstract
Today, innovative engineering solutions, including IoT devices, enable the precise monitoring of plant health and the early detection of diseases. However, the lifespan of IoT devices used for the real-time monitoring of environmental or plant parameters in precision agriculture is typically only a [...] Read more.
Today, innovative engineering solutions, including IoT devices, enable the precise monitoring of plant health and the early detection of diseases. However, the lifespan of IoT devices used for the real-time monitoring of environmental or plant parameters in precision agriculture is typically only a few months, from planting to harvest. This short lifespan creates challenges in managing the e-waste generated by smart agriculture. One potential solution to reduce the volume and environmental impact of e-waste is to use more environmentally friendly and biodegradable materials to replace the non-degradable components (substrates) currently used in the structure of IoT devices. In this study, we estimate the electromagnetic properties at 2565 MHz of the leaves from three widely grown crops: winter wheat, corn, and sunflower. We found that winter wheat and sunflower leaves have values of the real part of relative permittivity ranging from about 33 to 69 (wheat) and 13 to 32 (sunflower), respectively, while corn exhibits a value of about 33.5. Our research indicates that the position of a leaf on the plant stem and its distance from the soil significantly affect the relative permittivity of winter wheat and sunflower. These relationships, however, are not evident in the electromagnetic properties of corn leaves. Full article
(This article belongs to the Special Issue Electromagnetic Waves, Antennas and Sensor Technologies)
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<p>Application example of a wearable antenna on a substrate from a <span class="html-italic">ZZ plant</span> leaf: (<b>a</b>) photo of the antenna prototype; (<b>b</b>) measured reflection coefficient |S<sub>11</sub>| and 3D radiation pattern.</p>
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<p>Locations of agricultural fields and their GPS coordinates.</p>
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<p>Photos of the sample preparation procedure.</p>
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<p>Block diagram of the experimental setup.</p>
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<p>Results from measurements of winter wheat leaves during three growth stages (from Feekes 8 to Feekes 10.5) in the agriculture field near Blagoevgrad: (<b>a</b>) Real part of the relative permittivity; (<b>b</b>) Imaginary part of the relative permittivity; (<b>c</b>) Leaf length; (<b>d</b>) Plant height, soil relative humidity and temperature.</p>
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<p>Results from measurements of winter wheat leaves in the agriculture field near Stoyanovtci: (<b>a</b>) Real and imaginary parts of the relative permittivity; (<b>b</b>) Leaf length, plant height, soil relative humidity and temperature.</p>
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<p>Results from measurements of corn leaves during the R5 growth stage: (<b>a</b>) Mean value and standard deviation of real and imaginary parts of corn leaf relative permittivity measured in agricultural fields near Mezdra; (<b>b</b>) Mean value and standard deviation of real and imaginary parts of corn leaf relative permittivity measured in agricultural fields near Dabrava; (<b>c</b>) Leaf length, plant height, soil relative humidity and temperature for measurements in agricultural fields near Mezdra; (<b>d</b>) Leaf length, plant height, soil relative humidity and temperature for measurements in agricultural fields near Dabrava.</p>
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<p>Results from measurements of sunflower leaves during the seed development stage in the agriculture field near Kameno pole: (<b>a</b>) Real part of the relative permittivity; (<b>b</b>) Imaginary part of the relative permittivity; (<b>c</b>) Leaf area, plant height, soil relative humidity and temperature; (<b>d</b>) Photos.</p>
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14 pages, 4087 KiB  
Article
Design and Characteristics of Underwater Stacked Capacitive Power Transfer Coupler and Analysis of Propagation in Water Medium
by Kyeungwon Bang and Sangwook Park
Appl. Sci. 2025, 15(4), 1901; https://doi.org/10.3390/app15041901 - 12 Feb 2025
Abstract
This study provides a theoretical analysis of how the electrical characteristics of the medium affect the propagation of electric fields. Every medium has specific electrical conductivity and permittivity values and can be evaluated as a good conductor or a good dielectric depending on [...] Read more.
This study provides a theoretical analysis of how the electrical characteristics of the medium affect the propagation of electric fields. Every medium has specific electrical conductivity and permittivity values and can be evaluated as a good conductor or a good dielectric depending on the ratio of conduction current to displacement current. The strength of the electric field decreases significantly with the propagation distance due to the influence of high conductivity. In conclusion, even media with a high permittivity may be unsuitable for improving the performance of the capacitive power transfer (CPT) system depending on its conductivity. The analysis was verified for four types of water with different conductivities. In addition, we designed a stacked CPT coupler structure and analyzed its underwater transfer characteristics. In conclusion, unlike the parallel CPT coupler, the stacked CPT coupler is relatively disadvantageous for underwater use. Full article
(This article belongs to the Special Issue Electric Power Applications II)
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<p>Underwater stacked CPT system.</p>
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<p>Circuit model of capacitive coupler. (<b>a</b>) Basic representation. (<b>b</b>) Pi model.</p>
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<p>Simplified practical equivalent circuit model of underwater stacked CPT system.</p>
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<p>Underwater stacked CPT coupler design. (<b>a</b>) Single coupler quarter view. (<b>b</b>) Front view.</p>
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<p>Fabricated underwater stacked CPT system. (<b>a</b>) Stacked CPT coupler. (<b>b</b>) Experimental setup.</p>
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<p>The loss tangent values for various types of water from 0.1 to 15 MHz.</p>
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<p>The electric field attenuation of various types of water from 0 to 300 mm.</p>
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<p>Transmission coefficient of underwater stacked CPT coupler (at d = 20 mm).</p>
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<p>Coupler equivalent component variations (<math display="inline"><semantics> <mrow> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">t</mi> <mo> </mo> <mi>d</mi> <mo>=</mo> <mn>10</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">m</mi> <mo> </mo> <mi mathvariant="normal">t</mi> <mi mathvariant="normal">o</mi> <mo> </mo> <mn>200</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>).</p>
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<p>Comparison of maximum <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>S</mi> </mrow> <mrow> <mn>21</mn> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mi>m</mi> </mrow> </msub> </mrow> </semantics></math> (<math display="inline"><semantics> <mrow> <mi mathvariant="normal">a</mi> <mi mathvariant="normal">t</mi> <mo> </mo> <mi>d</mi> <mo>=</mo> <mn>10</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">m</mi> <mo> </mo> <mi mathvariant="normal">t</mi> <mi mathvariant="normal">o</mi> <mo> </mo> <mn>200</mn> <mo> </mo> <mi mathvariant="normal">m</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math>).</p>
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15 pages, 4481 KiB  
Article
A Novel Time Domain Reflectometry (TDR) System for Water Content Estimation in Soils: Development and Application
by Alessandro Comegna, Simone Di Prima, Shawcat Basel Mostafa Hassan and Antonio Coppola
Sensors 2025, 25(4), 1099; https://doi.org/10.3390/s25041099 - 12 Feb 2025
Abstract
Nowadays, there is a particular need to estimate soil water content accurately over space and time scales in various applications. For example, precision agriculture, as well as the fields of geology, ecology, and hydrology, necessitate rapid, onsite water content measurements. The time domain [...] Read more.
Nowadays, there is a particular need to estimate soil water content accurately over space and time scales in various applications. For example, precision agriculture, as well as the fields of geology, ecology, and hydrology, necessitate rapid, onsite water content measurements. The time domain reflectometry (TDR) technique is a geophysical method that allows, in a time-varying electric field, the determination of dielectric permittivity and electrical conductivity for a wide class of porous materials. Measuring the volumetric water content in soils is the most frequent application of TDR in soil science and soil hydrology. TDR has grown in popularity over the last 40 years because it is a practical and non-destructive technique that provides laboratory and field-scale measurements. However, a significant limitation of this technique is the relatively high cost of TDR devices, despite the availability of a range of commercial systems with varying prices. This paper aimed to design and implement a low-cost, compact TDR device tailored for classical hydrological applications. A series of laboratory experiments were carried out on soils of different textures to calibrate and validate the proposed measuring system. The results show that the device can be used to obtain predictions for monitoring soil water status with acceptable accuracy (R2 = 0.95). Full article
(This article belongs to the Special Issue Sensors in Smart Irrigation Systems)
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<p>(<b>a</b>) Time Domain Reflectometry (TDR) hardware setup; (<b>b</b>) voltage versus travel time for an idealized TDR waveform, highlighting distinctive signal characteristics resulting from multiple reflections (adapted from [<a href="#B6-sensors-25-01099" class="html-bibr">6</a>]).</p>
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<p>Example of a TDR output waveform, showing (i) the first peak, (ii) the reflection point, and (iii) tangent lines required for the determination of these two points.</p>
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<p>(<b>a</b>) Electrical circuit diagram of the PKTDR device and (<b>b</b>) the printed circuit board (PCB) layout generated using KiCad software (version 7.0).</p>
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<p>(<b>a</b>) The printed circuit board (PCB) of the PKTDR device, (<b>b</b>) PKTDR housed within its PLA enclosure, and (<b>c</b>) the additional components needed to complete the assembly.</p>
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<p>Example of a TDR signal acquired using PKTDR with the Hantek 6254BD DSO.</p>
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<p>Laboratory apparatus for calibration and validation of the PKTDR device (adapted from [<a href="#B4-sensors-25-01099" class="html-bibr">4</a>]).</p>
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<p>Bulk dielectric permittivity (ε<sub>b</sub>) values measured using the PKTDR device plotted against the estimated θ values, calculated using Equation (2) for the four investigated soils. The red lines and red text represent θ values determined using the thermo-gravimetric method. The graphic also highlights the range of θ variability among the soils in blue text.</p>
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<p>(<b>a</b>) Comparison of θ values estimated using the PKTDR device and the commercial TDR100 device and (<b>b</b>) θ-PKTDR estimated values vs. known θ values, with reference to the four investigated soils.</p>
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<p>The PKTDR prototype.</p>
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<p>Scheme of the required components and connections for the PKTDR system.</p>
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14 pages, 3055 KiB  
Article
Ion Substitution-Induced Distorted MOF Lattice with Deviated Energy and Dielectric Properties for Quasi-Solid-State Ion Conductor
by Yike Huang, Yun Zheng, Yan Guo, Qi Zhang, Yingying Shen, Hebin Zhang, Yinan Liu, Yihao Zheng, Pingshan Jia, Rong Chen, Lifen Long, Zhiyuan Zhang, Congcong Zhang, Yuanhang Hou, Kunye Yan, Ziyu Huang, Manting Zhang, Jiangmin Jiang, Shengyang Dong, Wen Lei and Huaiyu Shaoadd Show full author list remove Hide full author list
Nanomaterials 2025, 15(4), 274; https://doi.org/10.3390/nano15040274 - 11 Feb 2025
Abstract
Solid-state electrolytes are currently receiving increasing interest due to their high mechanical strength and chemical stability for safe battery construction. However, their poor ion conduction and unclear conduction mechanism need further improvement and exploration. This study focuses on a hybrid solid-state electrolyte containing [...] Read more.
Solid-state electrolytes are currently receiving increasing interest due to their high mechanical strength and chemical stability for safe battery construction. However, their poor ion conduction and unclear conduction mechanism need further improvement and exploration. This study focuses on a hybrid solid-state electrolyte containing MOF-based scaffolds, using metal salts as the conductor. In this paper, we employ an ion substitution strategy to manipulate the scaffold structure at the lattice level by replacing hydrogen with larger alkali cations. The research systematically presents how changes in the lattice affect the physical and chemical properties of MOFs and emphasizes the role of scaffold–salt interactions in the evolution of ion conduction. The results reveal that long range-ordered structural distortion can enhance permittivity at 1 Hz, from 58 ohms to more than 10 M ohms, which can boost ion pairs dissociation and improve the transference number from 4.7% to 22.6%. Defects in the lattice can help stabilize the intermediate state in the charge transfer process and lower the corresponding impedance from 2.6 MΩ to 559 Ω. Full article
(This article belongs to the Section Inorganic Materials and Metal-Organic Frameworks)
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<p>The phase and morphology of ion-substituted MOFs for electrolyte scaffold: (<b>a</b>) the XRD pattern of ion-substituted MOFs; (<b>b</b>) the interplanar spacing <span class="html-italic">d</span> ratio calculated by the data from (<b>a</b>), the marked numbers indicate the Miller index; (<b>c</b>) the diffraction intensity ratio from (<b>a</b>), the marked numbers indicate the diffraction index; (<b>d</b>) the XRD pattern of ion-substituted MOFs after calcination; (<b>e</b>) the diffraction intensity ratio from (<b>d</b>), the marked numbers indicate the diffraction index.</p>
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<p>The morphology of MOF samples: (<b>a</b>) the SEM images of raw AlBTeC MOFs and Li and Cs-substituted ones; (<b>b</b>) the SEM images of Cs-substituted MOFs after calcination at 300 °C; (<b>c</b>) the SEM-EDS element mapping data of Cs substituted AlBTeC MOFs.</p>
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<p>The bonding structure analysis of ion-substituted MOFs for electrolyte scaffold: (<b>a</b>) the FT-IR curves of ion-substituted MOFs; (<b>b</b>) an enlarged FT-IR plot. The arrows indicated the peaks split after substitution; (<b>c</b>) the solid-state <sup>13</sup>C NMR spectrum of the raw and ion-substituted MOFs. Peaks from spectrum have been assigned carbon atoms marked in red circles.</p>
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<p>The optical picture, UV–Vis results, and permittivity properties of ion-substituted MOFs for electrolyte scaffold: (<b>a</b>) an orbital figure of ion-substituted MOFs; (<b>b</b>) the UV–Vis reflectance plot for ion-substituted MOFs; (<b>c</b>) the UV–Vis absorption plot transformed from reflectance with marked peak positions by bars; (<b>d</b>) the relative permittivity results measured by electrochemical impedance spectroscopy (EIS); (<b>e</b>) the electronic modulus results measured by EIS; (<b>f</b>) a summarization plot of the characterizations for the sole MOF scaffold without electrolyte.</p>
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<p>The impedance data and comparative trend plot: (<b>a</b>) the EIS Nyquist plot of electrolytes with different salt/MOFs ratios; (<b>b</b>) the EIS Nyquist plot of electrolytes with different ether usage; (<b>c</b>) the EIS Nyquist plot of electrolytes with different ion-substituted MOFs; (<b>d</b>) a comparative trend plot of conductance, transference number, spacing ratio, UV–Vis peak position, and permittivity.</p>
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<p>Schematic illustration of the ion substitution-induced lattice distortion of MOFs. The porous blue bricks refer to the MOF scaffold; the red balls with “H” refer to the spare hydrogen atoms from non-coordinated carboxyl groups in MOF ligands; the yellow balls with “M<sup>+</sup>” refer to the substitution alkali ions: Li<sup>+</sup>, Na<sup>+</sup>, K<sup>+</sup>, Rb<sup>+</sup>, and Cs<sup>+</sup>.</p>
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<p>Schematic illustration of the preparation (the case of Li-substitution). The structural scheme is the bonding structure of 1,2,4,5-Benzenetetracarboxylic acid, the C<sub>6</sub>H<sub>2</sub>(CO<sub>2</sub>H)<sub>4</sub>, the ligand in MIL-121. The ligand shows two spared carboxyl groups without coordination—brown balls: Carbon; red balls: Oxygen; white balls: Hydrogen.</p>
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17 pages, 4811 KiB  
Article
Non-Invasive Differential Temperature Monitoring Using Sensor Array for Microwave Hyperthermia Applications: A Subspace-Based Approach
by Ji Wu, Fan Yang, Jinchuan Zheng, Hung T. Nguyen and Rifai Chai
J. Sens. Actuator Netw. 2025, 14(1), 19; https://doi.org/10.3390/jsan14010019 - 11 Feb 2025
Abstract
Non-invasive temperature monitoring is highly valuable in applications such as microwave hyperthermia treatment, where overheating may damage healthy tissue. This paper presents a subspace-based method for real-time temperature monitoring using a sensor array configuration. The proposed method improves upon the conventional Born approximation [...] Read more.
Non-invasive temperature monitoring is highly valuable in applications such as microwave hyperthermia treatment, where overheating may damage healthy tissue. This paper presents a subspace-based method for real-time temperature monitoring using a sensor array configuration. The proposed method improves upon the conventional Born approximation (BA) approach by accurately estimating the total field through primary induced currents. The temperature-dependent dielectric properties of breast tissues are modeled using data from porcine tissues, and a sigmoid function is employed to create realistic temperature transition zones in the numerical breast phantom. The method is validated through extensive simulations under noise-free and noisy conditions (SNR = 30 dB and 20 dB). The results demonstrate that our method maintains consistent performance across different temperature levels (38–45 °C), achieving reconstruction accuracy within ±0.2 °C at SNR = 30 dB and ±0.5 °C at SNR = 20 dB. While the computational overhead of calculating primary induced currents slightly increases the overall processing time, it leads to a faster convergence in the cost function minimization. These findings suggest that the proposed method offers a promising solution for real-time temperature monitoring in microwave hyperthermia applications. Full article
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<p>2D configuration of the EM scattering problem. The circular sensors array is located outside the domain of interest <span class="html-italic">D</span>. Tx and Rx represent the transmitter and receiver.</p>
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<p>Temperature-dependent dielectric properties of porcine tissues at three specific frequencies: (<b>a</b>) relative permittivity of liver versus temperature, (<b>b</b>) conductivity of liver versus temperature, (<b>c</b>) relative permittivity of fat versus temperature, (<b>d</b>) conductivity of fat versus temperature, (<b>e</b>) relative permittivity of blood versus temperature, and (<b>f</b>) conductivity of blood versus temperature.</p>
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<p>Temperature-dependent dielectric properties of porcine tissues at three specific frequencies: (<b>a</b>) relative permittivity of liver versus temperature, (<b>b</b>) conductivity of liver versus temperature, (<b>c</b>) relative permittivity of fat versus temperature, (<b>d</b>) conductivity of fat versus temperature, (<b>e</b>) relative permittivity of blood versus temperature, and (<b>f</b>) conductivity of blood versus temperature.</p>
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<p>The dielectric properties of the 2D cross-section from the selected digital breast model (breast ID: 070604PA2).</p>
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<p>The relative permittivity distribution of the selected digital breast (breast ID: 070604PA2) with tumor.</p>
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<p>The sigmoid function used for modelling temperature transition, where the horizontal axis represents the distance from the heating center and the vertical axis represents the temperature.</p>
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<p>Heating effects at 40 °C: (<b>a</b>) relative permittivity distribution of the heated digital breast, (<b>b</b>) changes in relative permittivity due to heating, and (<b>c</b>) temperature distribution across the imaging domain.</p>
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<p>Comparison of temperature reconstruction results at different heating levels (38–45 °C). For each temperature level (<b>a</b>–<b>h</b>), the panels show the following: temperature distribution reconstructed by the BA method (<b>left</b>), true temperature distribution (<b>middle</b>), and temperature distribution reconstructed by the proposed method (<b>right</b>). Temperature values are indicated by the color bar in degrees Celsius.</p>
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<p>Comparison of temperature reconstruction results at different heating levels (38–45 °C) under SNR = 30 dB. For each temperature level (<b>a</b>–<b>h</b>), the panels show the following: temperature distribution reconstructed by the BA method (<b>left</b>), true temperature distribution (<b>middle</b>), and temperature distribution reconstructed by the proposed method (<b>right</b>). Temperature values are indicated by the color bar in degrees Celsius.</p>
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<p>Comparison of temperature reconstruction results at different heating levels (38–45 °C) under SNR = 30 dB. For each temperature level (<b>a</b>–<b>h</b>), the panels show the following: temperature distribution reconstructed by the BA method (<b>left</b>), true temperature distribution (<b>middle</b>), and temperature distribution reconstructed by the proposed method (<b>right</b>). Temperature values are indicated by the color bar in degrees Celsius.</p>
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<p>Comparison of temperature reconstruction results at different heating levels (38–45 °C) under SNR = 20 dB. For each temperature level (<b>a</b>–<b>h</b>), the panels show the following: temperature distribution reconstructed by the BA method (<b>left</b>), true temperature distribution (<b>middle</b>), and temperature distribution reconstructed by the proposed method (<b>right</b>). Temperature values are indicated by the color bar in degrees Celsius.</p>
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<p>Comparison of temperature reconstruction results at different heating levels (38–45 °C) under SNR = 20 dB. For each temperature level (<b>a</b>–<b>h</b>), the panels show the following: temperature distribution reconstructed by the BA method (<b>left</b>), true temperature distribution (<b>middle</b>), and temperature distribution reconstructed by the proposed method (<b>right</b>). Temperature values are indicated by the color bar in degrees Celsius.</p>
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16 pages, 3185 KiB  
Article
Microwave Sensor for Dielectric Constant of Lossy Organic Liquids Based on Negative-Resistance Oscillation
by Huan Liu and Yichao Meng
Sensors 2025, 25(3), 961; https://doi.org/10.3390/s25030961 - 5 Feb 2025
Abstract
The dielectric constant, or permittivity, is a fundamental property that characterizes a material’s electromagnetic behavior, crucial for diverse applications in agriculture, healthcare, industry, and scientific research. In microwave engineering, accurate permittivity measurement is essential for advancements in fields such as biomedicine, aerospace, and [...] Read more.
The dielectric constant, or permittivity, is a fundamental property that characterizes a material’s electromagnetic behavior, crucial for diverse applications in agriculture, healthcare, industry, and scientific research. In microwave engineering, accurate permittivity measurement is essential for advancements in fields such as biomedicine, aerospace, and microwave chemistry. However, conventional waveguide resonator methods face challenges when measuring high-loss materials, often leading to reduced accuracy and increased cost. This paper introduces a lightweight, compact system for dielectric constant measurement using a negative-resistance voltage-controlled oscillator (VCO) integrated within a frequency synthesizer. The proposed system employs phase response variations of a planar sensor embedded in the VCO’s gate network to detect changes in oscillation frequency, enabling precise measurement of high-loss materials. The experimental validation demonstrates the system’s capability to accurately measure dielectric constants of lossy organic liquids, with applications in distinguishing liquid mixtures. The contributions include the design of a resonant-network-attached oscillator, comprehensive sensor performance simulations, and successful characterization of organic liquid mixtures, showcasing the potential of this approach for practical dielectric property measurements. Full article
(This article belongs to the Section Sensors Development)
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<p>Circuit diagram of the resonant-network-attached oscillator. The framework of the oscillator is at the right bottom.</p>
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<p>Simplified schematic of the negative-resistance oscillator used for permittivity measurement.</p>
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<p>Variation in the magnitude of the reflection coefficient at the gate and drain with respect to <math display="inline"><semantics> <msub> <mi>L</mi> <mi>s</mi> </msub> </semantics></math>.</p>
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<p>Dimensions of the SRR: (<b>top</b>) front view and (<b>bottom</b>) rear view.</p>
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<p>Reflection coefficient of the simulated sensor, with and without the sample placed on top of the SRR.</p>
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<p>Electric field distribution on the bottom surface of unloaded sensor at the resonance.</p>
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<p>Gate input resistance.</p>
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<p>Circuit stability simulation.</p>
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<p>Change in output frequency (<math display="inline"><semantics> <msub> <mi>f</mi> <mn>0</mn> </msub> </semantics></math>) with varying voltage.</p>
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<p>Change in resonance output power with varying frequency.</p>
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<p>Change in VCO output power with varying frequency.</p>
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<p>VCO output spectrum simulation.</p>
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<p>Time-domain simulation plot.</p>
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<p>Fabricated VCO prototype: (<b>left</b>) front view and (<b>right</b>) back view.</p>
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<p>Chemical calibration coefficients.</p>
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<p>Permittivity of MUTs given the sample volumes between 50 and 300 μL.</p>
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<p>Frequency-shift measurements for ethanol–methanol mixtures.</p>
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19 pages, 1924 KiB  
Article
Deep Learning-Based Ground-Penetrating Radar Inversion for Tree Roots in Heterogeneous Soil
by Xibei Li, Xi Cheng, Yunjie Zhao, Binbin Xiang and Taihong Zhang
Sensors 2025, 25(3), 947; https://doi.org/10.3390/s25030947 - 5 Feb 2025
Abstract
Tree roots are vital for tree ecosystems; accurate root detection helps analyze the health of trees and supports the effective management of resources such as fertilizers, water and pesticides. In this paper, a deep learning-based ground-penetrating radar (GPR) inversion method is proposed to [...] Read more.
Tree roots are vital for tree ecosystems; accurate root detection helps analyze the health of trees and supports the effective management of resources such as fertilizers, water and pesticides. In this paper, a deep learning-based ground-penetrating radar (GPR) inversion method is proposed to simultaneously image the spatial distribution of permittivity for subsurface tree roots and layered heterogeneous soils in real time. Additionally, a GPR simulation data set and a measured data set are built in this study, which were used to train inversion models and validate the effectiveness of GPR inversion methods.The introduced GPR inversion model is a pyramid convolutional network with vision transformer and edge inversion auxiliary task (PyViTENet), which combines pyramidal convolution and vision transformer to improve the diversity and accuracy of data feature extraction. Furthermore, by adding the task of edge inversion of the permittivity distribution of underground materials, the model focuses more on the details of heterogeneous structures. The experimental results show that, for the case of buried scatterers in layered heterogeneous soil, the PyViTENet performs better than other deep learning methods on the simulation data set. It can more accurately invert the permittivity of scatterers and the soil stratification. The most notable advantage of PyViTENet is that it can accurately capture the heterogeneous structural details of the soil within the layer since the soil around the tree roots in the real scene is layered soil and each layer of soil is also heterogeneous due to factors such as humidity, proportion of different soil particles, etc.In order to further verify the effectiveness of the proposed inversion method, this study applied the PyViTENet to GPR measured data through transfer learning for reconstructing the permittivity, shape, and position information of scatterers in the actual scene. The proposed model shows good generalization ability and accuracy, and provides a basis for non-destructive detection of underground scatterers and their surrounding medium. Full article
(This article belongs to the Section Radar Sensors)
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<p>The structure of the GPR inversion model PyViTENet.</p>
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<p>The structure of PyConvFEB.</p>
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<p>The structure of the ViTFEB module.</p>
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<p>GPR model.</p>
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<p>Soil texture classification.</p>
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<p>Inversion results. (<b>a</b>) Preprocessed B-scans. (<b>b</b>) Ground truths of the relative permittivity distribution of underground material. (<b>c</b>–<b>i</b>) Predicted relative permittivity distributions from (<b>c</b>) FWI, (<b>d</b>) U-Net, (<b>e</b>) GPRInvNet, (<b>f</b>) DMRF-UNet, (<b>g</b>) TransUNet, (<b>h</b>) EDMFEBs and (<b>i</b>) PyViTENet.</p>
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<p>An enlarged view of the inversion results on the detailed structure within the soil obtained by different inversion methods. The right side of the figure is a magnified view of the inversion results corresponding to the red area on the left side. The different colors represent the same values as in <a href="#sensors-25-00947-f006" class="html-fig">Figure 6</a>.</p>
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<p>Results of ablation experiment. (<b>a</b>) Ground truths. (<b>b</b>) The main inversion task using PyConvFEBs only. (<b>c</b>) The main inversion task using PyConvFEBs and ViTFEB. (<b>d</b>) The main inversion task using PyConvFEBs and the edge inversion auxiliary task (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>). (<b>e</b>) The main inversion task using PyConvFEBs and the edge inversion auxiliary task (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>). (<b>f</b>) PyViTENet (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>). (<b>g</b>) PyViTENet (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>β</mi> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>). The different colors represent the same values as in <a href="#sensors-25-00947-f006" class="html-fig">Figure 6</a>.</p>
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<p>The experimental site of the real dataset.</p>
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<p>Comparison of the inversion results of each method on the real dataset. (<b>a</b>) Preprocessed B-scans. (<b>b</b>) Ground truths of the relative permittivity distribution of underground material. (<b>c</b>–<b>i</b>) Predicted relative permittivity distributions from (<b>c</b>) FWI, (<b>d</b>) U-Net, (<b>e</b>) GPRInvNet, (<b>f</b>) DMRF-UNet, (<b>g</b>) TransUNet, (<b>h</b>) EDMFEBs and (<b>i</b>) PyViTENet.</p>
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17 pages, 595 KiB  
Article
A Comparative Study Between Micro and Millimeter Impedance Sensor Designs for Type-2 Diabetes Detection
by Santu Guin, Debjyoti Chowdhury and Madhurima Chattopadhyay
Micro 2025, 5(1), 7; https://doi.org/10.3390/micro5010007 - 1 Feb 2025
Abstract
In recent years, various types of sensors have been developed at both millimeter (mm) and micrometer (µm) scales for numerous biomedical applications. Each design has its own advantages and limitations. This study compares the electrical characteristics and sensitivity of millimeter- and micrometer-scale sensors, [...] Read more.
In recent years, various types of sensors have been developed at both millimeter (mm) and micrometer (µm) scales for numerous biomedical applications. Each design has its own advantages and limitations. This study compares the electrical characteristics and sensitivity of millimeter- and micrometer-scale sensors, emphasizing the superior performance of millimeter-scale designs for detecting type-2 diabetes. Elevated glucose levels in type-2 diabetes alter the complex permittivity of red blood cells (RBCs), affecting their rheological and electrical properties, such as viscosity, volume, relative permittivity, dielectric loss, and AC conductivity. These alterations may manifest as a unique bio-impedance signature, offering a diagnostic topology for diabetes. In view of this, various concentrations (ranging from 10% to 100%) of 400 µL of normal and diabetic RBCs suspended in phosphate-buffered saline (PBS) solution are examined to record the changes in bio-impedance signatures across a spectrum of frequencies, ranging from 1 MHz to 10 MHz. In this study, simulations are performed using the finite element method (FEM) with COMSOL Multiphysics® to analyze the electrical behavior of the sensors at both millimeter (mm) and micrometer (µm) scales. These simulations provide valuable insights into the performance parameters of the sensors, aiding in the selection of the most effective design by using this topology. Full article
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<p>Electrode layout with millimeter (mm) dimension with (<b>a</b>) top view; (<b>b</b>) cross-section view.</p>
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<p>Electrode layout with micrometer (µm) dimension with (<b>a</b>) top view; (<b>b</b>) cross-section view [<a href="#B53-micro-05-00007" class="html-bibr">53</a>,<a href="#B55-micro-05-00007" class="html-bibr">55</a>].</p>
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<p>Variation in the permittivity of the cell–medium with an increasing number of cells [<a href="#B53-micro-05-00007" class="html-bibr">53</a>].</p>
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<p>Surface-charge density in diabetic RBC with mm electrodes.</p>
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<p>Surface-charge density of diabetic RBC with mm electrodes (Y-Z direction).</p>
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<p>Surface-charge density of diabetic RBC with µm electrodes.</p>
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<p>Variation of the double-layer impedance of IDE within 1 MHz–10 MHz using electrodes with mm dimension and µm dimension.</p>
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<p>Variation in the average complex impedance (<math display="inline"><semantics> <msub> <mi>Z</mi> <mrow> <mi>mix</mi> </mrow> </msub> </semantics></math>) over the whole concentration range within 1–100 MHz frequency range for <span class="html-italic">N</span> = 40 (in mm dimension).</p>
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<p>Variation in the average complex impedance (<math display="inline"><semantics> <msub> <mi>Z</mi> <mrow> <mi>mix</mi> </mrow> </msub> </semantics></math>) over the whole concentration range within 1–100 MHz frequency range for <span class="html-italic">N</span> = 40 (in µm dimension).</p>
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<p>Standard deviation (SD) of <math display="inline"><semantics> <mrow> <msub> <mi>Z</mi> <mrow> <mi>mix</mi> <mspace width="4.pt"/> </mrow> </msub> <mrow> <mo>(</mo> <mi mathvariant="normal">k</mi> <mo>Ω</mo> <mo>)</mo> </mrow> </mrow> </semantics></math> for normal and diabetic RBCs over the whole range of concentration by varying the frequency range within 1–10 MHz using electrodes with mm dimension.</p>
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<p>Standard deviation (SD) of <math display="inline"><semantics> <mrow> <msub> <mi>Z</mi> <mrow> <mi>mix</mi> <mspace width="4.pt"/> </mrow> </msub> <mrow> <mo>(</mo> <mi mathvariant="normal">k</mi> <mo>Ω</mo> <mo>)</mo> </mrow> </mrow> </semantics></math> for normal and diabetic RBCs over the whole range of concentration by varying the frequency range 1–10 MHz using electrodes with µm dimension.</p>
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16 pages, 3126 KiB  
Article
A Soil Refractive Index (SRI) Model Characterizing the Functional Relationship Between Soil Moisture Content and Permittivity
by Erji Du, Lin Zhao, Guojie Hu, Zanpin Xing, Tonghua Wu, Xiaodong Wu, Ren Li, Defu Zou, Guangyue Liu, Lingxiao Wang, Zhibin Li, Yuxin Zhang, Yao Xiao and Yonghua Zhao
Water 2025, 17(3), 399; https://doi.org/10.3390/w17030399 - 31 Jan 2025
Abstract
The functional relationship between soil permittivity and soil water content serves as the theoretical foundation for electromagnetic wave-based techniques used to determine soil moisture levels. However, the response of permittivity to changes in soil water content varies significantly across different soil types. Current [...] Read more.
The functional relationship between soil permittivity and soil water content serves as the theoretical foundation for electromagnetic wave-based techniques used to determine soil moisture levels. However, the response of permittivity to changes in soil water content varies significantly across different soil types. Current models that utilize soil permittivity to estimate soil water content are often based on empirical statistical relationships specific to particular soil types. Moreover, existing physical models are hindered by an excessive number of parameters, which can be difficult to measure or calculate. This study introduces a universal model, termed the Soil Refractive Index (SRI) model, to describe the relationship between soil permittivity and soil water content. The SRI model is derived from the propagation velocity of electromagnetic waves in various soil components and the functional relationship between electromagnetic wave velocity and relative permittivity. The SRI model expresses soil water content as a linear function of the square root of the relative permittivity for any soil type with the slope and intercept as the two undetermined parameters. The slope is primarily influenced by the relative permittivity of soil water, while the intercept is mainly affected by both the slope and the soil porosity. The applicability of the SRI model is validated through tested soil samples and comparison with previously published empirical statistical models. For dielectric lossless soil, the theoretical value of the slope is calculated to be 0.126. The intercept varies across different soil types and increases linearly with soil porosity. The SRI model provides a theoretical basis for calculating soil water content using permittivity across various soil types. Full article
(This article belongs to the Section Soil and Water)
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<p>Laboratory tested relative complex permittivity (ε<sub>r</sub>, ε<sub>i</sub>) and loss tangent (tanδ) under different soil water content conditions of three soils, (<b>a</b>) SS, (<b>b</b>) OS, (<b>c</b>) HS.</p>
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<p>The linear relationship fitting results between <span class="html-italic">θ</span> and <math display="inline"><semantics> <mrow> <msqrt> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </msqrt> </mrow> </semantics></math> for (<b>a</b>) SS, (<b>b</b>) OS, and (<b>c</b>) HS.</p>
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<p>The linear relationship fitting results between <span class="html-italic">θ</span> and <math display="inline"><semantics> <mrow> <msqrt> <msub> <mrow> <mi>ε</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </msqrt> </mrow> </semantics></math> for (<b>a</b>) SS, (<b>b</b>) OS, and (<b>c</b>) HS.</p>
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<p>Comparison between the measured <math display="inline"><semantics> <mrow> <mi>θ</mi> </mrow> </semantics></math> and calculated results with SRI model for (<b>a</b>) SS, (<b>b</b>) OS, and (<b>c</b>) HS.</p>
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<p>Comparison between SRI model and equations published by (<b>a</b>)Topp, (<b>b</b>) Malicki and (<b>c</b>) Roth for mineral soils.</p>
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<p>Comparison between SRI model (<math display="inline"><semantics> <mrow> <mi>A</mi> <mo>=</mo> <mn>0.126</mn> </mrow> </semantics></math> and Topp equation for (<b>a</b>) sandy loam, (<b>b</b>) clay, (<b>c</b>) SRI model (<math display="inline"><semantics> <mrow> <mi>A</mi> <mo>=</mo> <mn>0.099</mn> </mrow> </semantics></math>) and Topp equation for clay.</p>
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<p>Comparison between SRI model (<math display="inline"><semantics> <mrow> <mi>A</mi> <mo>=</mo> <mn>0.126</mn> </mrow> </semantics></math> and Topp equation for (<b>a</b>) sandy loam, (<b>b</b>) clay, (<b>c</b>) SRI model (<math display="inline"><semantics> <mrow> <mi>A</mi> <mo>=</mo> <mn>0.099</mn> </mrow> </semantics></math>) and Topp equation for clay.</p>
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<p>Comparison between SRI model and (<b>a</b>) Topp equation, (<b>b</b>) Roth equation, (<b>c</b>) Malicki equation and (<b>d</b>) Schaap equation for organic soil.</p>
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<p>Statistical relationship between soil porosity and parameter B in SRI model for different soil (red cross marks represents our tested three soils, SS, OS and HS).</p>
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17 pages, 15700 KiB  
Article
All-Organic Quantum Dots-Boosted Energy Storage Density in PVDF-Based Nanocomposites via Dielectric Enhancement and Loss Reduction
by Ru Guo, Xi Yuan, Xuefan Zhou, Haiyan Chen, Haoran Xie, Quan Hu, Hang Luo and Dou Zhang
Polymers 2025, 17(3), 390; https://doi.org/10.3390/polym17030390 - 31 Jan 2025
Abstract
Dielectric capacitors offer immense application potential in advanced electrical and electronic systems with their unique ultrahigh power density. Polymer-based dielectric composites with high energy density are urgently needed to meet the ever-growing demand for the integration and miniaturization of electronic devices. However, the [...] Read more.
Dielectric capacitors offer immense application potential in advanced electrical and electronic systems with their unique ultrahigh power density. Polymer-based dielectric composites with high energy density are urgently needed to meet the ever-growing demand for the integration and miniaturization of electronic devices. However, the universal contradictory relationship between permittivity and breakdown strength in traditional ceramic/polymer nanocomposite still poses a huge challenge for a breakthrough in energy density. In this work, all-organic carbon quantum dot CDs were synthesized and introduced into a poly(vinylidene fluoride) PVDF polymer matrix to achieve significantly boosted energy storage performance. The ultrasmall and surface functionalized CDs facilitate the polar β-phase transition and crystallinity of PVDF polymer and modulate the energy level and traps of the nanocomposite. Surprisingly, a synergistic dielectric enhancement and loss reduction were achieved in CD/PVDF nanocomposite. For one thing, the improvement in εr and high-field Dm originates from the CD-induced polar transition and interface polarization. For another thing, the suppressed dielectric loss and high-field Dr are attributed to the conductive loss depression via the introduction of deep trap levels to capture charges. More importantly, Eb was largely strengthened from 521.9 kV mm−1 to 627.2 kV mm−1 by utilizing the coulomb-blockade effect of CDs to construct energy barriers and impede carrier migration. As a result, compared to the 9.9 J cm−3 for pristine PVDF, the highest discharge energy density of 18.3 J cm−3 was obtained in a 0.5 wt% CD/PVDF nanocomposite, which is competitive with most analogous PVDF-based nanocomposites. This study demonstrates a new paradigm of organic quantum dot-enhanced ferroelectric polymer-based dielectric energy storage performance and will promote its application for electrostatic film capacitors. Full article
(This article belongs to the Special Issue Piezoelectric Polymers and Devices)
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<p>Microstructural characterization of CD powders. (<b>a</b>) High-resolution TEM image, (<b>b</b>) XRD pattern, (<b>c</b>) FTIR spectrum, (<b>d</b>) XPS full survey spectrum, (<b>e</b>) C1s, and (<b>f</b>) O1s spectra of CD powders.</p>
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<p>(<b>a</b>) Process diagram for preparing CD/PVDF nanocomposite film through the solution-casting method. Cross-sectional SEM image of nanocomposite with different CD content: (<b>b</b>) 0, (<b>c</b>) 0.05 wt%, (<b>d</b>) 0.2 wt%, (<b>e</b>) 0.5 wt%, (<b>f</b>) 1.0 wt%, and (<b>g</b>) 2.0 wt%. LSCM images of the (<b>h</b>) pristine PVDF film and (<b>i</b>) 2 wt% CD/PVDF nanocomposite.</p>
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<p>(<b>a</b>) XRD pattern, (<b>b</b>) FTIR spectra, (<b>c</b>) calculated phase content and crystallite size, (<b>d</b>) DSC thermographs, and (<b>e</b>) calculated crystallinity of the CD/PVDF nanocomposite with different CD contents. (<b>f</b>) Schematic diagram of CD-induced crystallization behavior evolution.</p>
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<p>Frequency-dependent changes in (<b>a</b>) dielectric constant and (<b>b</b>) dielectric loss of CD/PVDF nanocomposites with different CD contents. Comparison of (<b>c</b>) dielectric constant and (<b>d</b>) dielectric loss at 1 kHz.</p>
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<p>(<b>a</b>) Weibull distribution of the breakdown strength and (<b>b</b>) comparison of <span class="html-italic">E</span><sub>b</sub> of the CD/PVDF nanocomposites. (<b>c</b>) (<span class="html-italic">αhν</span>)<sup>2</sup>-h<span class="html-italic">ν</span> curves obtained from the UV−vis spectra and (<b>d</b>) the leakage current density of the CD/PVDF nanocomposites.</p>
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<p>(<b>a</b>–<b>f</b>) High-field <span class="html-italic">D-E</span> loops of CD/PVDF nanocomposites with different CD contents. (<b>g</b>) <span class="html-italic">D</span><sub>m</sub> and (<b>h</b>) <span class="html-italic">D</span><sub>r</sub> of CD/PVDF nanocomposites under varied electric fields. (<b>i</b>) Displacement difference <span class="html-italic">D</span><sub>m</sub>-<span class="html-italic">D</span><sub>r</sub> of CD/PVDF nanocomposites at maximum electric field.</p>
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<p>(<b>a</b>) Schematic <span class="html-italic">D-E</span> loop to calculate the energy storage performance. (<b>b</b>) The discharged energy density, <span class="html-italic">U</span><sub>dis</sub>, and (<b>c</b>) energy efficiency, <span class="html-italic">η</span>, of the CD/PVDF nanocomposites under different electric fields. (<b>d</b>) Comparison of <span class="html-italic">U</span><sub>dis</sub> and <span class="html-italic">η</span> at the maximum electric field. (<b>e</b>) The conduction loss and (<b>f</b>) the ferroelectric loss of the CD/PVDF nanocomposites with varied electric fields.</p>
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<p>Temperature-dependent energy storage performance: (<b>a</b>) the <span class="html-italic">D-E</span> loop and (<b>b</b>) the discharged energy density and energy efficiency at different temperatures. (<b>c</b>) The charge–discharge cycle performance of pure PVDF and composites of the 0.5 wt% CD/PVDF nanocomposite. (<b>d</b>) A comparison of the <span class="html-italic">E</span><sub>b</sub> and the corresponding <span class="html-italic">U</span><sub>dis</sub> in this work with those of other recently reported PVDF-based nanocomposites [<a href="#B12-polymers-17-00390" class="html-bibr">12</a>,<a href="#B18-polymers-17-00390" class="html-bibr">18</a>,<a href="#B29-polymers-17-00390" class="html-bibr">29</a>,<a href="#B39-polymers-17-00390" class="html-bibr">39</a>,<a href="#B40-polymers-17-00390" class="html-bibr">40</a>,<a href="#B41-polymers-17-00390" class="html-bibr">41</a>,<a href="#B42-polymers-17-00390" class="html-bibr">42</a>,<a href="#B43-polymers-17-00390" class="html-bibr">43</a>,<a href="#B44-polymers-17-00390" class="html-bibr">44</a>,<a href="#B45-polymers-17-00390" class="html-bibr">45</a>,<a href="#B46-polymers-17-00390" class="html-bibr">46</a>,<a href="#B47-polymers-17-00390" class="html-bibr">47</a>,<a href="#B48-polymers-17-00390" class="html-bibr">48</a>,<a href="#B49-polymers-17-00390" class="html-bibr">49</a>,<a href="#B50-polymers-17-00390" class="html-bibr">50</a>].</p>
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26 pages, 8318 KiB  
Article
Reflection Propagation Law of Electromagnetic Waves in U-Shaped Roadway
by Laigong Guo, Xiaolong Li, Xinkang Shi, Long Ma and Changna Guo
Appl. Sci. 2025, 15(3), 1460; https://doi.org/10.3390/app15031460 - 31 Jan 2025
Abstract
To address the complex and space-constrained characteristics of underground coal mine roadways, this study proposes an electromagnetic wave reflection model based on the mirror image method. A U-shaped roadway model was designed and a relay node was established at the center of the [...] Read more.
To address the complex and space-constrained characteristics of underground coal mine roadways, this study proposes an electromagnetic wave reflection model based on the mirror image method. A U-shaped roadway model was designed and a relay node was established at the center of the roadway to simplify calculations. The point normal vector method was used to calculate the equations and boundary ranges of eight reflection planes. The valid reflection paths were determined by calculating the mirror points, counting the number of reflection lines, and evaluating their validity. The sensitivity of the number of valid reflection lines to the positions of the transmitting and receiving points relative to the corners was determined, and the reflected field strength at the receiving point was calculated. Its sensitivity to variables such as the distance between the relay node and the receiving point, antenna transmitting frequency, relative dielectric constant of the roadway walls, and width of the U-shaped roadway was studied. The simulation results showed that the number of valid reflection lines decreased with increasing distance from the transmitting and receiving points to the corners. The horizontal position of the transmitting point has a higher effect on the number of effective reflection lines than the vertical position, while the transmitting and receiving points are favorable for electromagnetic wave propagation when they are located in the center of the roadway. As the distance between the relay node and the receiving point increases, the reflection field strength attenuation at the receiving point will decrease with a larger roadway width, a smaller relative permittivity of the roadway walls, and a lower transmitting frequency of the antenna. Full article
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<p>U-shaped roadway model diagram.</p>
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<p>Calculation of mirror points.</p>
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<p>Valid and invalid reflection lines. (<b>a</b>) Valid reflection lines; (<b>b</b>) invalid reflection lines over planes <span class="html-italic">m</span><sub>4</sub> and <span class="html-italic">m</span><sub>5</sub>; (<b>c</b>) invalid reflection lines over planes <span class="html-italic">m</span><sub>5</sub> and <span class="html-italic">m</span><sub>6</sub>; (<b>d</b>) invalid reflection lines over planes <span class="html-italic">m</span><sub>4</sub>, <span class="html-italic">m</span><sub>5</sub>, and <span class="html-italic">m</span><sub>6</sub>.</p>
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<p>Two-dimensional segmentation of the plane <span class="html-italic">m</span><sub>8</sub>.</p>
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<p>Calculation of reflection point.</p>
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<p>Two-dimensional diagram of four-time valid reflection paths.</p>
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<p>Two-dimensional diagram of five-time valid reflection paths.</p>
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<p>Two-dimensional diagram of six-time valid reflection paths.</p>
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<p>Three-dimensional primary valid reflection map.</p>
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<p>Number of valid reflection lines as a function of the distance from the launch point to the corner.</p>
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<p>Number of valid reflection lines as a function of the distance from the receiving point to the corner.</p>
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<p>Number of valid reflection lines as a function of the horizontal distance from the launch point.</p>
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<p>Number of valid reflection lines as a function of the vertical distance of the launch point.</p>
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<p>Reflected field strength at the receiving point as a function of the distance between the relay node and the receiving point for different height differences.</p>
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<p>Reflected field strength at the receiving point as a function of the distance between the relay node and the receiving point at different frequencies.</p>
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<p>Reflected field strength at the receiving point as a function of the distance between the relay node and the receiving point for different dielectric constants.</p>
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<p>Reflected field strength of the receiving point as a function of the distance between the relay node and the receiving point for different roadway widths.</p>
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<p>Modeled U-shaped roadway with antennae.</p>
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<p>Flowchart of HFSS simulation steps.</p>
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<p>Field strength at the receiving point as a function of the distance between the relay node and the receiving point for different height differences.</p>
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<p>Field strength at the receiving point as a function of the distance between the relay node and the receiving point at different frequencies.</p>
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<p>Field strength at the receiving point as a function of the distance between the relay node and the receiving point for different dielectric constants.</p>
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<p>Field strength of the receiving point as a function of the distance between the relay node and the receiving point for different roadway widths.</p>
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