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15 pages, 5038 KiB  
Article
Investigation of the Automatic Monitoring System of a Solar Power Plant with Flexible PV Modules
by Žydrūnas Kavaliauskas, Igor Šajev, Giedrius Blažiūnas and Giedrius Gecevičius
Appl. Sci. 2024, 14(20), 9500; https://doi.org/10.3390/app14209500 - 17 Oct 2024
Abstract
During this research, an automatic monitoring system was developed to monitor the working parameters in a solar power plant consisting of two flexible silicon modules. The first stage of the monitoring system relies on a microcontroller, which collects data from wattmeter modules made [...] Read more.
During this research, an automatic monitoring system was developed to monitor the working parameters in a solar power plant consisting of two flexible silicon modules. The first stage of the monitoring system relies on a microcontroller, which collects data from wattmeter modules made using a microcontroller. This tier also includes DC/DC converter and RS232-TCP converter modules for data transfer. The second stage, the industrial PLC, receives data from the first stage and transmits them to the PC, where the information is stored and the processes are visualized on the HMI screen. During this study, the charging process was analyzed using PWM- and MPPT-type charging controllers, as well as the power supply of Fito LED strips for lighting plants. Using the created monitoring system, the parameters of the solar power plant with flexible PV modules were monitored. This study compared PWM and MPPT battery charging methods, finding that MPPT is more efficient, especially under unstable solar conditions. MPPT technology optimizes energy usage more efficiently, resulting in faster battery charging compared to PWM technology. Full article
(This article belongs to the Special Issue Applied Electronics and Functional Materials)
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Figure 1
<p>Conceptual diagram of the system for monitoring the working parameters of a solar power plant with flexible modules.</p>
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<p>The main block diagram of the monitoring system.</p>
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<p>Electrical diagram of power measurement.</p>
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<p>Electrical diagram of the first stage of the monitoring system.</p>
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<p>PCB of the power measurement circuit (<b>a</b>) and the circuit of the first stage of the monitoring system (<b>b</b>).</p>
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<p>An image of the main window of the PC program with settings.</p>
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<p>Control program algorithms: (<b>a</b>) power measurement module program algorithm; (<b>b</b>) algorithm of the first stage of the monitoring system and (<b>c</b>) algorithm of the second stage of the monitoring system.</p>
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<p>Dependence of PWM cycle length on battery charge level.</p>
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<p>Battery voltage dependence when PWM and MPPT systems are used for charging.</p>
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<p>Time dependence of the efficiency of PWM and MPPT charging controllers.</p>
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13 pages, 4592 KiB  
Article
Inkjet-Printed Silver Lithiophilic Sites on Copper Current Collectors: Tuning the Interfacial Electrochemistry for Anode-Free Lithium Batteries
by Seyedalireza Mirbagheri, Eugenio Gibertini and Luca Magagnin
Batteries 2024, 10(10), 369; https://doi.org/10.3390/batteries10100369 - 17 Oct 2024
Abstract
Anode-free lithium batteries (AFLBs) present an opportunity to eliminate the need for conventional graphite electrodes or excess lithium–metal anodes, thus increasing the cell energy density and streamlining the manufacturing process. However, their attributed poor coulombic efficiency leads to rapid capacity decay, underscoring the [...] Read more.
Anode-free lithium batteries (AFLBs) present an opportunity to eliminate the need for conventional graphite electrodes or excess lithium–metal anodes, thus increasing the cell energy density and streamlining the manufacturing process. However, their attributed poor coulombic efficiency leads to rapid capacity decay, underscoring the importance of achieving stable plating and stripping of Li on the negative electrode for the success of this cell configuration. A promising approach is the utilization of lithiophilic coatings such as silver to mitigate the Li nucleation overpotential on the Cu current collector, thereby improving the process of Li plating/stripping. On the other hand, inkjet printing (IJP) emerges as a promising technique for electrode modification in the manufacturing process of lithium batteries, offering a fast and scalable technology capable of depositing both thin films and patterned structures. In this work, a Fujifilm Dimatix inkjet printer was used to deposit Ag sites on a Cu current collector, aiming to modulate the interfacial electrochemistry of the system. Samples were fabricated with varying areas of coverage and the electrochemical performance of the system was systematically evaluated from bare Cu (non-lithiophilic) to a designed pattern (partially lithiophilic) and the fully coated thin film case (lithiophilic). Increasing lithiophilicity resulted in lower charge transfer resistance, higher exchange current density and reduced Li nucleation overpotential (from 55.75 mV for bare Cu to 13.5 mV for the fully coated case). Enhanced half-cell cyclability and higher coulombic efficiency were also achieved (91.22% CE over 76 cycles for bare Cu, 97.01% CE over 250 cycles for the fully coated case), alongside more uniform lithium deposition and fewer macroscopic irregularities. Moreover, our observations demonstrated that surface patterning through inkjet printing could represent an innovative, easy and scalable strategy to provide preferential Li nucleation sites to guide the subsequent Li deposition. Full article
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Figure 1
<p>(<b>a</b>) Schematic representation of interfacial litiophilicity tuning by IJP of Ag nanoparticle ink. (<b>b</b>) Optical images of the Ag40ds@Cu sample after the thermal treatment and the SEM image of a single printed dot. (<b>c</b>) XRD of the Ag10ds@Cu after thermal treatment.</p>
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<p>Cyclic voltammetry plots of half cells batteries cycled between −0.2 and 0.6 V at 0.5 mV s<sup>−1</sup> scan rate for the (<b>a</b>) 1st cycle and (<b>b</b>) 5th cycle. (<b>c</b>) Transferred charge values during the plating step in the first and fifth cycles. Tafel plots derived from CV; (<b>d</b>) 1st cycle, (<b>e</b>) 5th cycle. (<b>f</b>) Exchange current density values extrapolated from the Tafel plots.</p>
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<p>SEM images of electrode surfaces at limited Li-plated capacity (0.05 mA cm<sup>−2</sup>, 0.006 mAh cm<sup>−2</sup>); (<b>a</b>) bare Cu, (<b>b</b>) Ag40ds@Cu and (<b>c</b>) Ag10ds@Cu. SEM images of electrode surfaces for higher Li-plated capacity (0.05 mA cm<sup>−2</sup>, 0.2 mAh cm<sup>−2</sup>); (<b>d</b>) bare Cu, (<b>e</b>) Ag40ds@Cu, (<b>f</b>) Ag10ds@Cu.</p>
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<p>(<b>a</b>) Voltage profiles of plating-stripping over a maximum of 250 cycles at 0.2 mA cm<sup>−2</sup> and 0.2 mAh cm<sup>−2</sup>. The onset of irregular cycling, corresponding to a sudden drop of CE, was considered as a threshold for test stop. (<b>b</b>) Coulombic efficiency (CE %) with cycling. Voltage profiles and Li nucleation overpotentials observed from each electrode during cycling; (<b>c</b>) 10th cycle. (<b>d</b>) 30th cycle. (<b>e</b>) 50th cycle. (<b>f</b>) 70th cycle.</p>
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<p>Nyquist plots of the samples in Li-plated state (0.2 mAh cm<sup>−2</sup>, 0.1 mA cm<sup>−2</sup>); (<b>a</b>) 1st cycle, (<b>b</b>) 5th cycle and (<b>c</b>) 40th cycle; (<b>d</b>) charge transfer resistance values extracted by the fitting the plots with the equivalent circuit (inset image).</p>
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<p>SEM images at different magnitudes of electrodes in a lithiated state (0.2 mAh cm<sup>−2</sup>) after 40 cycles cycled at 0.1 mA cm<sup>−2</sup>; (<b>a</b>,<b>d</b>) bare Cu, (<b>b</b>,<b>e</b>) Ag40ds@Cu and (<b>c</b>,<b>f</b>) Ag10ds@Cu.</p>
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13 pages, 7469 KiB  
Article
An 8 × 8 CMOS Optoelectronic Readout Array of Short-Range LiDAR Sensors
by Yeojin Chon, Shinhae Choi, Jieun Joo and Sung-Min Park
Sensors 2024, 24(20), 6686; https://doi.org/10.3390/s24206686 - 17 Oct 2024
Abstract
This paper presents an 8 × 8 channel optoelectronic readout array (ORA) realized in the TSMC 180 nm 1P6M RF CMOS process for the applications of short-range light detection and ranging (LiDAR) sensors. We propose several circuit techniques in this work, including an [...] Read more.
This paper presents an 8 × 8 channel optoelectronic readout array (ORA) realized in the TSMC 180 nm 1P6M RF CMOS process for the applications of short-range light detection and ranging (LiDAR) sensors. We propose several circuit techniques in this work, including an amplitude-to-voltage (A2V) converter that reduces the notorious walk errors by intensity compensation and a time-to-voltage (T2V) converter that acquires the linear slope of the output signals by exploiting a charging circuit, thus extending the input dynamic range significantly from 5 μApp to 1.1 mApp, i.e., 46.8 dB. These results correspond to the maximum detection range of 8.2 m via the action of the A2V converter and the minimum detection range of 56 cm with the aid of the proposed T2V converter. Optical measurements utilizing an 850 nm laser diode confirm that the proposed 8 × 8 ORA with 64 on-chip avalanche photodiodes (APDs) can successfully recover the narrow 5 ns light pulses even at the shortest distance of 56 cm. Hence, this work provides a potential CMOS solution for low-cost, low-power, short-range LiDAR sensors. Full article
(This article belongs to the Special Issue Recent Advances in LiDAR Sensor)
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<p>(<b>a</b>) Block diagram of a typical LiDAR sensor, (<b>b</b>) a single cell of the proposed ORA.</p>
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<p>(<b>a</b>) A cross-sectional view of a P<sup>+</sup>/N-well APD, (<b>b</b>) the layout of the on-chip APD.</p>
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<p>Schematic diagrams of (<b>a</b>) VCF-TIA with PA and (<b>b</b>) PDH.</p>
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<p>Simulated eye diagrams of the VCF-TIA at 200 Mb/s for two input currents of (<b>a</b>) 100 μA<sub>pp</sub> and (<b>b</b>) 1 mA<sub>pp</sub>, respectively.</p>
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<p>Simulated eye diagrams of the VCF-TIA at 200 Mb/s for two input currents of (<b>a</b>) 100 μA<sub>pp</sub> and (<b>b</b>) 1 mA<sub>pp</sub>, respectively.</p>
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<p>(<b>a</b>) Simulated pulse response of the A2V converter, (<b>b</b>) I–V curve and (<b>c</b>) transient response with the variations of the APD photocurrents.</p>
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<p>(<b>a</b>) Simulated pulse response of the A2V converter, (<b>b</b>) I–V curve and (<b>c</b>) transient response with the variations of the APD photocurrents.</p>
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<p>Schematic diagram of the charging circuit in the T2V converter.</p>
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<p>(<b>a</b>) Simulated pulse response and (<b>b</b>) a relationship curve of the T2V output voltage versus the time interval between the START and STOP pulses.</p>
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<p>Simulated pulse responses of the proposed 8 × 8 CMOS ORA.</p>
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<p>(<b>a</b>) Layout of a single-channel, and (<b>b</b>) test setup of the proposed 8 × 8 ORA chip.</p>
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<p>Measured A2V outputs of the 8 × 8 ORA for equivalent input currents from 5 μA<sub>pp</sub> to 500 μA<sub>pp</sub>, respectively.</p>
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<p>Measured T2V outputs of the 8 × 8 ORA for different 50 μA<sub>pp</sub>, 300 μA<sub>pp,</sub> and 1.1 mA<sub>pp</sub> input currents, respectively.</p>
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<p>(<b>a</b>) Measured 8-row outputs of the 8 × 8 ORA at the optical testing, and (<b>b</b>) measured output of a single row (magnified).</p>
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12 pages, 716 KiB  
Review
Early Diagnosis and Treatment of Kidney Injury: A Focus on Urine Protein
by Duanna Zeng, Bing Wang, Zheng Xiao, Xiongqin Wang, Xiyang Tang, Xinsheng Yao, Ping Wang, Meifang Li, Yi Dai and Xiean Yu
Int. J. Mol. Sci. 2024, 25(20), 11171; https://doi.org/10.3390/ijms252011171 - 17 Oct 2024
Abstract
The kidney, an essential excretory organ of the body, performs a series of crucial physiological functions such as waste removal, maintenance of electrolyte and acid–base balance, and endocrine regulation. Due to its rich blood flow and high metabolic activity, the kidney is susceptible [...] Read more.
The kidney, an essential excretory organ of the body, performs a series of crucial physiological functions such as waste removal, maintenance of electrolyte and acid–base balance, and endocrine regulation. Due to its rich blood flow and high metabolic activity, the kidney is susceptible to damage. Currently, kidney injury is classified into acute kidney injury (AKI) and chronic kidney disease (CKD), both of which are associated with high rates of morbidity and mortality on a global scale. The current clinical diagnosis of renal injury relies on the assessment of renal filtration function using creatinine and urea nitrogen as “gold-standard” markers. However, the delayed response time, limited specificity, and reduced accuracy of creatinine and urea nitrogen in evaluating kidney injury have significantly hindered advancements in diagnostic methods for kidney injury. Urinary protein is widely utilized as a biomarker for the early diagnosis of kidney injury due to the selectivity of the glomerular filtration system determining whether proteins can pass through the filtration barrier based on their size and charge. Therefore, as a complex biological sample with varying charges and particle sizes, urinary protein is considered an ideal indicator for monitoring the progression of kidney disease. Exploring the relationship between urinary protein and the advancement of kidney injury based on differences in particle size and charge offers a new perspective for assessing and treating such injuries. Hence, we conducted a comprehensive review of 74 relevant studies to gain a thorough understanding of the physiological mechanism and significance of proteinuria production. The aim was to explore the challenges and opportunities in clinical urine protein detection, as well as to discuss strategies targeting glomerular filtration barriers in order to effectively reduce urine protein levels and treat kidney injury, which could provide a new perspective for identifying the progression of kidney injury. Full article
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<p>Schematic illustration of glomerular filtration barrier composed of endothelial cells, glomerular basement membrane (GBM), and podocytes [<a href="#B28-ijms-25-11171" class="html-bibr">28</a>].</p>
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<p>(<b>a</b>) A cross-section of a normal glomerular capillary shows the foot processes with interconnecting ultrathin and uniformly wide (40 nm) slit diaphragms (arrows). Scale bar: 200 nm. (<b>b</b>) In congenital nephrotic syndrome, the foot processes are lost and the slit diaphragm between the podocytes is absent; the resultant narrow slit lacks a functional filter structure. Scale bar 200 nm. (From the American Society of Nephrology © Lahdenkari, A.T. et al. (2004) [<a href="#B29-ijms-25-11171" class="html-bibr">29</a>]. Abbreviations: FP, foot process; GBM, glomerular basement membrane.)</p>
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13 pages, 5596 KiB  
Article
The Effect of Molecular Structure on the Properties of Fluorene Derivatives for OLED Applications
by Anna Pidluzhna, Aivars Vembris, Raitis Grzibovskis, Margarita Anna Zommere, Oleksandr Bezvikonnyi, Jurate Simokaitiene, Melita Baronaite, Dmytro Volyniuk, Juozas V. Grazulevicius, Amjad Ali, Glib Baryshnikov, Khrystyna Ivaniuk, Hryhorii Starykov and Pavlo Stakhira
Molecules 2024, 29(20), 4918; https://doi.org/10.3390/molecules29204918 - 17 Oct 2024
Abstract
A new family of symmetrical fluorene derivatives with different types of substituents attached to the C-2 and C-7 positions of the fluorene core synthesized by the Sonogashira coupling reactions is reported. The electronic structures and the properties of the compounds investigated by means [...] Read more.
A new family of symmetrical fluorene derivatives with different types of substituents attached to the C-2 and C-7 positions of the fluorene core synthesized by the Sonogashira coupling reactions is reported. The electronic structures and the properties of the compounds investigated by means of photoelectron emission spectroscopy, UV–Vis absorption and photoluminescent spectroscopy as well as by DFT and TD-DFT theoretical calculations are discussed. It is shown that the nature of substituents influences the π-conjugation of the molecules. No intermolecular charge transfer within the investigated wavelength range is observed. The applicability of the synthesized compounds in organic light-emitting diodes (OLEDs) based on exciplex emission is demonstrated. The advanced co-deposition technique with the tuned OLED architecture was applied and resulted in improved OLED parameters. Full article
(This article belongs to the Special Issue Explorations in Luminescent Molecular Materials)
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Figure 1
<p>UV–Vis absorption spectra (straight lines) and photoluminescence spectra (dashed lines) with λ<sub>ex</sub> = 360 nm for THF dilute solutions (10<sup>−4</sup> M) of synthesized substances (<b>a</b>). UV–Vis absorption spectra (straight lines) and photoluminescence spectra (dashed lines) with λ<sub>ex</sub> = 360 nm for encapsulated solid films of synthesized substances (<b>b</b>).</p>
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<p>Optimized geometries of chemical structures of <b>1</b>–<b>4</b> (<b>a</b>). HOMO and LUMO orbitals of the molecules (iso value 0.02) in THF solution (<b>b</b>).</p>
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<p>Absorption (solid lines) and fluorescence (dashed lines) spectra of all dyes computed with TD-DFT-CAM-B3LYP level of theory and 6-31G(d) basis set.</p>
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<p>The structure of the OLED devices A–D (<b>a</b>) and E, F (<b>b</b>). Equilibrium energy level diagram (<b>c</b>) The EL spectra for device A and D vs. the solid film PL spectra of substances <b>1</b>, <b>2</b> and <b>4</b> (<b>d</b>).</p>
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<p>1931 CIE coordinates of OLED A (<b>a</b>) and D (<b>b</b>) at different voltages.</p>
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<p>Synthesis of fluorene-based emitters <b>1</b>–<b>4</b>.</p>
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19 pages, 4201 KiB  
Article
Novel Droop-Based Techniques for Dynamic Performance Improvement in a Linear Active Disturbance Rejection Controlled-Dual Active Bridge for Fast Battery Charging of Electric Vehicles
by Armel Asongu Nkembi, Danilo Santoro, Fawad Ahmad, Iñigo Kortabarria, Paolo Cova, Emilio Sacchi and Nicola Delmonte
Energies 2024, 17(20), 5171; https://doi.org/10.3390/en17205171 - 17 Oct 2024
Abstract
Electric vehicles (EVs) are rapidly replacing fossil-fuel-powered vehicles, creating a need for a fast-charging infrastructure that is crucial for their widespread adoption. This research addresses this challenge by improving the control of dual active bridge converters, a popular choice for high-power EV charging [...] Read more.
Electric vehicles (EVs) are rapidly replacing fossil-fuel-powered vehicles, creating a need for a fast-charging infrastructure that is crucial for their widespread adoption. This research addresses this challenge by improving the control of dual active bridge converters, a popular choice for high-power EV charging stations. A critical issue in EV battery charging is the smooth transition between charging stages (constant current and constant voltage) which can disrupt converter performance. This work proposes a novel feedforward control method using a combination of droop-based techniques combined with a sophisticated linear active disturbance rejection control system applied to a single-phase shift-modulated dual active bridge. This combination ensures a seamless transition between charging stages and enhances the robustness of the system against fluctuations in both input voltage and load. Numerical simulations using MATLAB/Simulink R2024a demonstrated that this approach not only enables smooth charging but also reduces the peak input converter current, allowing for the use of lower-rated components in the converter design. This translates to potentially lower costs for building these essential charging stations and faster adoption of EVs. Full article
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<p>Schematic of the DAB architecture.</p>
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<p>Typical theoretical waveforms of DAB converter under SPS modulation (logical PWM signals, squared voltages of the bridges, and current of the leakage inductance).</p>
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<p>Diagrammatic representation of the LADRC principle.</p>
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<p>Proposed two-loop LADR-based battery charging control system.</p>
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<p>DAB equivalent circuit model.</p>
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<p>Normalized output current curve with variation in <span class="html-italic">α</span> and <span class="html-italic">β</span> for different values of output normalized output voltage.</p>
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<p>Relationship between: (<b>a</b>) input current and output voltage; (<b>b</b>) input current and output current.</p>
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<p>Battery voltage (<b>top</b>) and average battery current (<b>bottom</b>) with (<b>left</b>) and without (<b>right</b>) feedforward.</p>
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<p>Input and inductor current transient waveforms with and without the proposed feedforward technique.</p>
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<p>Comparing the transient performance of the proposed three approaches.</p>
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<p>Comparing the conventional feedforward approach with the proposed approaches.</p>
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11 pages, 2887 KiB  
Article
Spin Current Enhancement Using Double-Ferromagnetic-Layer Structure for Magnetoelectric Spin-Orbit Logic Device
by Bayartulga Ishdorj, Shumaila Sharif and Taehui Na
Electronics 2024, 13(20), 4085; https://doi.org/10.3390/electronics13204085 - 17 Oct 2024
Abstract
The use of Moore’s law appears to be coming to an end due to technological and physical constraints, as complementary metal-oxide semiconductor (CMOS) transistors become smaller and closer to the atomic scale. Therefore, various emerging technologies are being researched as potential successors to [...] Read more.
The use of Moore’s law appears to be coming to an end due to technological and physical constraints, as complementary metal-oxide semiconductor (CMOS) transistors become smaller and closer to the atomic scale. Therefore, various emerging technologies are being researched as potential successors to traditional CMOS transistors, and one of the most exciting candidates is the magnetoelectric spin-orbit (MESO) device. The MESO device comprises two portions (input and output) and it cascades charge/voltage as input and output signals. In the MESO device’s output portion, ferromagnetic (FM) and high-spin-orbit-coupling layers are employed to provide spin-polarized current and charge/voltage output. In this paper, we offer a description and analysis of the operating mechanism of the MESO device’s output portion using a spin flow approach and propose a double-FM-layer structure. In the double-FM-layer structure, we implement two FM layers with antiparallel magnetization directions, instead of using a single-FM-layer structure to increase the output charge/voltage. The proposed structure is verified through the Verilog-A compact model. Full article
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<p>MESO device. (<b>a</b>) Structure of the MESO device. (<b>b</b>) Input portion of the MESO device. (<b>c</b>) Output portion of the MESO device.</p>
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<p>Schematic representation of magnetoelectricity and magnetoelectric material.</p>
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<p>Exchange bias between FM and ME layers.</p>
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<p>Illustration comparing an unpolarized current and a spin-polarized current.</p>
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<p>Processes of the output structure of the MESO device. (<b>a</b>) Output portion of the MESO. (<b>b</b>) Spin-orbit scattering. (<b>c</b>) Spin filtering. (<b>d</b>) Electric field generation.</p>
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<p>Circuit schematics of an MESO.</p>
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<p>Working principle of the readout structure of the MESO device. (<b>a</b>) Proposed double-FM-layer structure. (<b>b</b>) Spin filtering 1. (<b>c</b>) Spin-orbit scattering. (<b>d</b>) Spin filtering 2. (<b>e</b>) Electric field generation.</p>
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<p>A comparison of the output voltage difference between the previous single spin filtering structure and the proposed double spin filtering structure.</p>
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11 pages, 11784 KiB  
Article
Rational Design of High-Performance Photocontrolled Molecular Switches Based on Chiroptical Dimethylcethrene: A Theoretical Study
by Li Han, Mei Wang, Yifan Zhang, Bin Cui and Desheng Liu
Molecules 2024, 29(20), 4912; https://doi.org/10.3390/molecules29204912 - 17 Oct 2024
Abstract
The reversible photo-induced conformation transition of a single molecule with a [5]helicene backbone has garnered considerable interest in recent studies. Based on such a switching process, one can build molecular photo-driven switches for potential applications of nanoelectronics. But the achievement of high-performance reversible [...] Read more.
The reversible photo-induced conformation transition of a single molecule with a [5]helicene backbone has garnered considerable interest in recent studies. Based on such a switching process, one can build molecular photo-driven switches for potential applications of nanoelectronics. But the achievement of high-performance reversible single-molecule photoswitches is still rare. Here, we theoretically propose a 13,14-dimethylcethrene switch whose photoisomerization between the ring-closed and ring-open forms can be triggered by ultraviolet (UV) and visible light irradiation. The electronic structure transitions and charge transport characteristics, concurrent with the photo-driven electrocyclization of the molecule, are calculated by the non-equilibrium Green’s function (NEGF) in combination with density functional theory (DFT). The electrical conductivity bears great diversity between the closed and open configurations, certifying the switching behavior and leading to a maximum on–off ratio of up to 103, which is considerable in organic junctions. Further analysis confirms the evident switching behaviors affected by the molecule–electrode interfaces in molecular junctions. Our findings are helpful for the rational design of organic photoswitches at the single-molecule level based on cethrene and analogous organic molecules. Full article
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<p>A schematic diagram of (<b>a</b>) the photoisomerization process of 13,14-dimethylcethrene and (<b>b</b>) the corresponding 45° top views and (<b>c</b>) side views.</p>
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<p>A schematic diagram of (<b>a</b>) molecular junctions based on 13,14-dimethylcethrene with Au(111) electrodes. Each junction is composed of three distinct components, i.e., the left electrode, the central scattering region, and the right electrode. (<b>b</b>) Forty-five-degree top views of ring-<span class="html-italic">closed</span> and ring-<span class="html-italic">open</span> isomers with different anchor attachment sites denoted as I(II)-<span class="html-italic">closed</span> and I(II)-<span class="html-italic">open</span>, respectively.</p>
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<p>(<b>a</b>) The current–voltage (I–V) curves of the molecular junctions based on 13,14-dimethylcethrene with different molecule–electrode interfaces. The solid black and green lines represent the I–V curves of the closed and open configurations with connection I. The solid blue and red lines represent the I–V curves of the closed and open configurations with connection II. (<b>b</b>) The <span class="html-italic">on–off</span> ratio curves of the molecular junctions. The solid red and blue lines represent the <span class="html-italic">on–off</span> ratio curves of the I-configuration and II-configuration, respectively. The inset in the top right corner presents an enlarged depiction of the <span class="html-italic">on–off</span> ratio curve for the I-configuration.</p>
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<p>The bias-dependent transmission spectra of the (<b>a</b>) closed and (<b>b</b>) open configurations consist of connection I. (<b>c</b>,<b>d</b>) The same case consists of connection II. The white dotted line indicates the bias window.</p>
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<p>The bias-dependent projected density of states (PDOS) spectra of the (<b>a</b>) closed and (<b>b</b>) open configurations consists of connection I. (<b>c</b>,<b>d</b>) The same case consists of connection II. The projection subspace is segmented into three parts, i.e., the left electrode (green line), the molecule (red line), and the right electrode (blue line). The magenta line indicates the bias window.</p>
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<p>The zero-bias transmission spectra of the (<b>a</b>) I-configuration and (<b>c</b>) II-configuration based on 13,14-dimethylcethrene. The solid red and blue lines represent the transmission spectra of the closed and open configurations, respectively. The Fermi level is set to zero, and the magenta line indicates the bias window. The red and blue solid down-pointing triangles denote the MPSH eigenvalues of the <span class="html-italic">closed</span> and <span class="html-italic">open</span> molecules. H and L denote HOMO and LUMO. (<b>b</b>,<b>d</b>) The bias-dependent spatial distribution of the frontier molecular orbitals in the I-configuration and II-configuration. The isovalue is set to 0.035 for all plots.</p>
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20 pages, 24444 KiB  
Article
Preparation and Photocatalytic Performance of In2O3/Bi2WO6 Type II Heterojunction Composite Materials
by Xiuping Zhang, Fengqiu Qin, Yuanyuan Zhong, Tian Xiao, Qiang Yu, Xiaodong Zhu, Wei Feng and Zhiyong Qi
Molecules 2024, 29(20), 4911; https://doi.org/10.3390/molecules29204911 - 17 Oct 2024
Abstract
Bismuth-based photocatalytic materials have been widely used in the field of photocatalysis in recent years due to their unique layered structure. However, single bismuth-based photocatalytic materials are greatly limited in their photocatalytic performance due to their poor response to visible light and easy [...] Read more.
Bismuth-based photocatalytic materials have been widely used in the field of photocatalysis in recent years due to their unique layered structure. However, single bismuth-based photocatalytic materials are greatly limited in their photocatalytic performance due to their poor response to visible light and easy recombination of photogenerated charges. At present, constructing semiconductor heterojunctions is an effective modification method that improves quantum efficiency by promoting the separation of photogenerated electrons and holes. In this study, the successful preparation of an In2O3/Bi2WO6 (In2O3/BWO) II-type semiconductor heterojunction composite material was achieved. XRD characterization was performed to conduct a phase analysis of the samples, SEM and TEM characterization for a morphology analysis of the samples, and DRS and XPS testing for optical property and elemental valence state analyses of the samples. In the II-type semiconductor junction system, photogenerated electrons (e) on the In2O3 conduction band (CB) migrate to the BWO CB, while holes (h+) on the BWO valence band (VB) transfer to the In2O3 VB, promoting the separation of photoinduced charges, raising the quantum efficiency. When the molar ratio of In2O3/BWO is 2:6, the photocatalytic degradation degree of rhodamine B (RhB) is 59.4% (44.0% for BWO) after 60 min illumination, showing the best photocatalytic activity. After four cycles, the degradation degree of the sample was 54.3%, which is 91.4% of that of the first photocatalytic degradation experiment, indicating that the sample has good reusability. The XRD results of 2:6 In2O3/BWO before and after the cyclic experiments show that the positions and intensities of its diffraction peaks did not change significantly, indicating excellent structural stability. The active species experiment results imply that h+ is the primary species. Additionally, this study proposes a mechanism for the separation, migration, and photocatalysis of photoinduced charges in II-type semiconductor junctions. Full article
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<p>XRD patterns of samples.</p>
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<p>SEM images of samples, with different magnifications: BWO (<b>a</b>,<b>b</b>), In<sub>2</sub>O<sub>3</sub> (<b>c</b>,<b>d</b>), 1:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>e</b>,<b>f</b>), 2:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>g</b>,<b>h</b>), 3:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>i</b>,<b>j</b>), and 4:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>k</b>,<b>l</b>).</p>
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<p>SEM images of samples, with different magnifications: BWO (<b>a</b>,<b>b</b>), In<sub>2</sub>O<sub>3</sub> (<b>c</b>,<b>d</b>), 1:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>e</b>,<b>f</b>), 2:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>g</b>,<b>h</b>), 3:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>i</b>,<b>j</b>), and 4:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>k</b>,<b>l</b>).</p>
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<p>(<b>a</b>) SEM image of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO; (<b>b</b>–<b>e</b>) element mappings of Bi, O, W, In; (<b>f</b>) EDS analysis of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO.</p>
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<p>TEM and HRTEM images of samples: BWO (<b>a</b>,<b>c</b>) and 2:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>b</b>,<b>d</b>).</p>
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<p>TEM and HRTEM images of samples: BWO (<b>a</b>,<b>c</b>) and 2:6 In<sub>2</sub>O<sub>3</sub>/BWO (<b>b</b>,<b>d</b>).</p>
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<p>XPS spectra of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO: (<b>a</b>) total spectrum; (<b>b</b>) Bi 4f; (<b>c</b>) O 1s; (<b>d</b>) W 4f; and (<b>e</b>) In 3d.</p>
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<p>XPS spectra of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO: (<b>a</b>) total spectrum; (<b>b</b>) Bi 4f; (<b>c</b>) O 1s; (<b>d</b>) W 4f; and (<b>e</b>) In 3d.</p>
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<p>N<sub>2</sub> adsorption–desorption isotherms and pore size distribution curve of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO.</p>
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<p>UV–visible diffuse reflectance spectrum (<b>a</b>) and bandgap diagram (<b>b</b>) of In<sub>2</sub>O<sub>3</sub>.</p>
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<p>PL patterns of samples.</p>
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<p>Time-resolved transient PL decay of BWO and 2:6 In<sub>2</sub>O<sub>3</sub>/BWO.</p>
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<p>Photodegradation curves (<b>a</b>) and kinetic fitting curves (<b>b</b>) of samples.</p>
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<p>The reuse experiment of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO for RhB degradation.</p>
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<p>XRD patterns of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO before and after the photocatalytic experiment.</p>
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<p>SEM images of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO at 10,000× magnification (<b>a</b>) and 100,000× magnification (<b>b</b>) after cycling experiments.</p>
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<p>XPS spectra of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO before and after the photocatalytic experiment: (<b>a</b>) Bi 4f; (<b>b</b>) W 4f; (<b>c</b>) In 3d.</p>
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<p>XPS spectra of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO before and after the photocatalytic experiment: (<b>a</b>) Bi 4f; (<b>b</b>) W 4f; (<b>c</b>) In 3d.</p>
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<p>Photocurrent response curves (<b>a</b>) and electrochemical impedance spectroscopy curves (<b>b</b>) of BWO and 2:6 In<sub>2</sub>O<sub>3</sub>/BWO.</p>
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<p>Photocurrent response curves (<b>a</b>) and electrochemical impedance spectroscopy curves (<b>b</b>) of BWO and 2:6 In<sub>2</sub>O<sub>3</sub>/BWO.</p>
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<p>The degradation degrees of 2:6 In<sub>2</sub>O<sub>3</sub>/BWO in the presence of different scavengers.</p>
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<p>Schematic diagram of photogenerated charge transfer and formation of free radicals in 2:6 In<sub>2</sub>O<sub>3</sub>/BWO.</p>
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18 pages, 8018 KiB  
Article
Photovoltaic Power Intermittency Mitigating with Battery Storage Using Improved WEEC Generic Models
by André Fernando Schiochet, Paulo Roberto Duailibe Monteiro, Thiago Trezza Borges, João Alberto Passos Filho and Janaína Gonçalves de Oliveira
Energies 2024, 17(20), 5166; https://doi.org/10.3390/en17205166 - 17 Oct 2024
Abstract
The growing integration of renewable energy sources, such as photovoltaic and wind systems, into energy grids has underscored the need for reliable control mechanisms to mitigate the inherent intermittency of these sources. According to the Brazilian grid operator (ONS), there have been cascading [...] Read more.
The growing integration of renewable energy sources, such as photovoltaic and wind systems, into energy grids has underscored the need for reliable control mechanisms to mitigate the inherent intermittency of these sources. According to the Brazilian grid operator (ONS), there have been cascading disconnections in renewable energy distributed systems (REDs) in recent years, highlighting the need for robust control models. This article addresses this issue by presenting the validation of an active power ramp rate control (PRRC) function for a PV plant coupled with a Battery Energy Storage System (BESS) using WECC generic models. The proposed model underwent rigorous validation over an extended analysis period, demonstrating good accuracy using the Root Mean Squared Error (RMSE) and an R-squared (R2) metrics for the active power injected at the Point of Connection (POI), PV active power, and BESS State of Charge (SOC), providing valuable insights for medium and long-term analyses. The ramp rate control module was implemented within the plant power controller (PPC), leveraging second-generation Renewable Energy Systems (RES) models developed by the Western Electricity Coordination Council (WECC) as a foundational framework. We conducted simulations using the Anatem software, comparing the results with real-world data collected at 100 ms to 1000 ms intervals from a PV plant equipped with a BESS in Brazil. The proposed model underwent rigorous validation over an extended analysis period, with the presented results based on two days of measurements. The positive sequence model used to represent this control demonstrated good accuracy, as confirmed by metrics such as the Root Mean Squared Error (RMSE) and R-squared (R2). Furthermore, the article underscores the critical role of accurately accounting for the power sampling rate when calculating the ramp rate. Full article
(This article belongs to the Special Issue Grid Integration of Renewable Energy Conversion Systems)
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<p>Ramp rate Calculation Techniques.</p>
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<p>PV Model with network solution. Source: Author, adapted from [<a href="#B11-energies-17-05166" class="html-bibr">11</a>].</p>
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<p>BESS Model considering the new Ramp Rate Control function in the Plant Controller. Source: Author, adapted from [<a href="#B11-energies-17-05166" class="html-bibr">11</a>].</p>
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<p>Ramp rate control (RR_Control) implemented in the REPC_A controller.</p>
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<p>Ramp rate control using the Rate LM block.</p>
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<p>Block Diagram of the Charging/Discharging Mechanism of the BESS Model (REEC_C). Source: Author, adapted from [<a href="#B9-energies-17-05166" class="html-bibr">9</a>].</p>
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<p>Flowchart illustrating the Improved WECC 2nd Generation Model implementation and validation for PV and BESS [<a href="#B11-energies-17-05166" class="html-bibr">11</a>].</p>
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<p>5-bus test system with the association of Anatem codes (DMDG and DFNT) and Bus Type (<span class="html-italic">P-V</span>, <span class="html-italic">V-θ and P-Q)</span>.</p>
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<p>Active Power Measured in the POI, in the PV and BESS SOC. (<b>a</b>) Day 1—RR = 150 kW/min; (<b>b</b>) Day 2—RR = 100 kW/min.</p>
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<p>Histogram of accumulated Active Power Ramp Rate in the PV. Analysis of the sampling period ∆<span class="html-italic">t</span> and its impact on the calculation of the ramp rate control. (<b>a</b>) Day 1—RR = 150 kW/min; (<b>b</b>) Day 2—RR = 100 kW/min.</p>
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<p>Histogram of accumulated Active Power Ramp Rate in the POI. Analysis of the sampling period ∆<span class="html-italic">t</span> and its impact on the calculation of the ramp rate control. (<b>a</b>) Day 1—RR = 150 kW/min; (<b>b</b>) Day 2—RR = 100 kW/min.</p>
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<p>Represents a PV plant associated with BESS for ramp rate control.</p>
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<p>Comparison of the Anatem ramp rate control simulation results with real PV data for a 100 kW/min rate and ∆<span class="html-italic">t</span> = 60 s.</p>
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<p>Comparison of the Anatem ramp rate control simulation results with real POI data for a rate of 100 kW/min and ∆<span class="html-italic">t</span> = 60 s.</p>
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<p>Comparison of the Anatem ramp rate control simulation results with real BESS SOC data for a rate of 100 kW/min and ∆<span class="html-italic">t</span> = 60 s.</p>
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<p>Validation of Anatem ramp rate control simulation results with real data for a 100 kW/min rate.</p>
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17 pages, 4305 KiB  
Article
Asymmetric Supercapacitor Performance Enhancement Through Fe-Doped MoS₂ Nanosheets Synthesized via Hydrothermal Method
by Pritam J. Morankar, Thupakula V. M. Sreekanth, Rutuja U. Amate, Manesh A. Yewale, Aviraj M. Teli, Sonali A. Beknalkar and Chan-Wook Jeon
Coatings 2024, 14(10), 1328; https://doi.org/10.3390/coatings14101328 - 17 Oct 2024
Viewed by 94
Abstract
As modern civilization’s energy demands continue to rise, the need for efficient renewable energy solutions becomes increasingly critical. In addressing this challenge, our research explores the potential of newly developed iron (Fe)-doped molybdenum disulfide (MoS2) thin-film electrodes, synthesized through a simple [...] Read more.
As modern civilization’s energy demands continue to rise, the need for efficient renewable energy solutions becomes increasingly critical. In addressing this challenge, our research explores the potential of newly developed iron (Fe)-doped molybdenum disulfide (MoS2) thin-film electrodes, synthesized through a simple hydrothermal method, as a promising energy storage device. By systematically varying the Fe doping levels, we aim to elucidate the relationship between Fe content and the structural, morphological, and electrochemical properties of the MoS2 electrodes. The optimized FM-3 electrode exhibited a remarkable areal capacitance of 8.25 F/cm2 at a current density of 10 mA/cm2 with an energy density of 0.22 mWh/cm2 and a power density of 2.2 mW/cm2. Furthermore, the FM-3 demonstrated impressive long-term cycling stability, retaining 85.58% of its initial capacitance after 10,000 charge–discharge cycles. To further explore practical applicability, an asymmetric pouch-type supercapacitor device was assembled using an FM-3 electrode and activated carbon. The device achieved an impressive areal capacitance of 0.43 F/cm2 at a current density of 20 mA/cm2, delivering an energy density of 0.133 mWh/cm2 and a power density of 7.5 mW/cm2. The exceptional performance of the FM-3 electrode can be attributed to the enhanced diffusion rate, charge transfer efficiency, and better carrier mobility induced by Fe doping. This work not only highlights the significant electrochemical performance improvements of Fe-doped MoS2 electrodes but also demonstrates their potential for scalable energy storage solutions, making a valuable contribution to the field of next-generation energy storage technologies. Full article
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<p>Depiction of hydrothermal synthesis of Fe-doped MoS<sub>2</sub> electrodes.</p>
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<p>(<b>a</b>) XRD pattern of Fe-Mo electrodes, (<b>b</b>) high-resolution XPS survey spectra (<b>c</b>) Mo 3d before Fe doping, (<b>d</b>) Mo 3d after Fe doping, (<b>e</b>) S 2p, and (<b>f</b>) Fe 2p spectra of Fe-Mo electrodes.</p>
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<p>FE-SEM images of (<b>a<sub>1</sub></b>–<b>a<sub>3</sub></b>) FM-0, (<b>b<sub>1</sub></b>–<b>b<sub>3</sub></b>) FM-1, (<b>c<sub>1</sub></b>–<b>c<sub>3</sub></b>) FM-3, and (<b>d<sub>1</sub></b>–<b>d<sub>3</sub></b>) FM-5 samples at different magnifications.</p>
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<p>EDS analysis of (<b>a</b>) FM-0, (<b>b</b>) FM-1, (<b>c</b>) FM-3, and (<b>d</b>) FM-5 samples.</p>
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<p>Cyclic voltammetry of (<b>a</b>) Fe-Mo samples at a scan rate of 10 mV/s, in a potential window −0.2 to 0.6 V, cyclic voltammetry of (<b>b</b>) FM-0, (<b>c</b>) FM-1, (<b>d</b>) FM-3, and (<b>e</b>) FM-5 samples at different scan rates (1–100 mV/s), (<b>f</b>) plot of peak current vs. (scan rate)<sup>1/2</sup>, (<b>g</b>) plot of <span class="html-italic">log(i)</span> against the <span class="html-italic">log(ϑ)</span>.</p>
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<p>Capacitive and diffusion-controlled processes at different scan rates of (<b>a</b>) FM-0, (<b>b</b>) FM-1, (<b>c</b>) FM-3, and (<b>d</b>) FM-5 samples.</p>
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<p>CVs conducted at different scan rates within a non-faradaic region for (<b>a</b>) FM-0, (<b>b</b>) FM-1, (<b>c</b>) FM-3, and (<b>d</b>) FM-5 electrodes, (<b>e</b>) Plot of resulting current variations at different scan rates for assessments of double-layer capacitance (Cdl), and (<b>f</b>) The computed ECSA values for the Fe-MoS<sub>2</sub> electrodes.</p>
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<p>(<b>a</b>) GCD curves of FM-0, FM-1, FM-3, and FM-5 electrodes at 10 mA/cm<sup>2</sup> current density, GCD plots of (<b>b</b>) FM-0, (<b>c</b>) FM-1, (<b>d</b>) FM-3, and (<b>e</b>) FM-5 electrodes at different current densities, (<b>f</b>) EIS analysis of Fe-Mo electrodes, and (<b>g</b>) cyclic stability over 10,000 GCD cycles of FM-3 sample.</p>
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<p>(<b>a</b>) CV tests performed on the FM-3//AC device recorded at a scan rate of 100 mV/s across a potential range of 1 to 1.8 V, (<b>b</b>) CV plot of FM-3//AC device at different scan rates within the potential window of 0 to 1.8 V, (<b>c</b>) GCD measurements at different current densities for FM-3//AC device, (<b>d</b>) EIS measurement of the device, (<b>e</b>) cyclic stability of 5000 GCD cycles of FM-3//AC device.</p>
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12 pages, 2728 KiB  
Article
Assessing SOC Estimations via Reverse-Time Kalman for Small Unmanned Aircraft
by Manuel R. Arahal, Alfredo Pérez Vega-Leal, Manuel G. Satué and Sergio Esteban
Energies 2024, 17(20), 5161; https://doi.org/10.3390/en17205161 - 17 Oct 2024
Viewed by 131
Abstract
This paper presents a method to validate state of charge (SOC) estimations in batteries for their use in remotely manned aerial vehicles (UAVs). The SOC estimation must provide the mission control with a measure of the available range of the aircraft, which is [...] Read more.
This paper presents a method to validate state of charge (SOC) estimations in batteries for their use in remotely manned aerial vehicles (UAVs). The SOC estimation must provide the mission control with a measure of the available range of the aircraft, which is critical for extended missions such as search and rescue operations. However, the uncertainty about the initial state and depth of discharge during the mission makes the estimation challenging. In order to assess the estimation provided to mission control, an a posteriori re-estimation is performed. This allows for the assessment of estimation methods. A reverse-time Kalman estimator is proposed for this task. Accurate SOC estimations are crucial for optimizing the utilization of multiple UAVs in a collaborative manner, ensuring the efficient use of energy resources and maximizing mission success rates. Experimental results for LiFePO4 batteries are provided, showing the capabilities of the proposal for the assessment of online SOC estimators. Full article
(This article belongs to the Special Issue Energy-Efficient Advances in More Electric Aircraft)
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<p>Laboratory setup.</p>
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<p>Thevenin equivalent circuit model for an electric battery.</p>
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<p>Experimental values for <math display="inline"><semantics> <msup> <mi>V</mi> <mn>0</mn> </msup> </semantics></math> of a LiFePO4 battery.</p>
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<p>SOC re-estimation example.</p>
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<p>Diagram of the experimental setup for data gathering (<b>left</b>) and photograph of the rig for testing battery usage (<b>right</b>).</p>
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<p>Current (<b>top graph</b>) and terminal voltage (<b>bottom graph</b>) for trajectory T1 used in tests A, B, C and D.</p>
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<p>Current (<b>top graph</b>) and terminal voltage (<b>bottom graph</b>) for trajectory T2 used in tests E and F.</p>
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<p>SOC estimation for standard KF and for RTKF for cases (<b>A</b>–<b>D</b>).</p>
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17 pages, 1486 KiB  
Article
Comparative VUV Synchrotron Excitation Study of YAG: Eu and YAG: Cr Ceramics
by Amangeldy M. Zhunusbekov, Zhakyp T. Karipbayev, Akbota Tolegenova, Kuat K. Kumarbekov, Erik E. Nurmoldin, Muratbek M. Baizhumanov, Aleksei Kotlov and Anatoli I. Popov
Crystals 2024, 14(10), 897; https://doi.org/10.3390/cryst14100897 - 16 Oct 2024
Viewed by 257
Abstract
Using synchrotron radiation, a comparative VUV excitation study of YAG ceramics doped with Eu3+ and Cr3+ ions under VUV excitation (10.5–3.7 eV) at 9 K was conducted in this work. Both ceramics exhibit distinct excitation peaks in the VUV region, indicating [...] Read more.
Using synchrotron radiation, a comparative VUV excitation study of YAG ceramics doped with Eu3+ and Cr3+ ions under VUV excitation (10.5–3.7 eV) at 9 K was conducted in this work. Both ceramics exhibit distinct excitation peaks in the VUV region, indicating high-energy transitions related to the internal electronic levels of the dopants and interband transitions within the YAG matrix. For YAG:Eu, the main excitation peaks at 6–7 eV correspond to transitions within the 4f-shell of Eu3+ and Eu3⁺-O2− charge transfer states, showing weak dependence on the crystal field and high energy conversion efficiency. In contrast, YAG:Cr shows broad excitation bands due to transitions between levels influenced by strong crystal field interactions, resulting in lower luminescence efficiency. The study highlights the importance of crystal structure and dopant interactions in determining the spectral characteristics of YAG-based ceramics, offering potential for their application in advanced optoelectronic devices. Full article
(This article belongs to the Special Issue Structure and Properties of Ceramic Materials)
26 pages, 931 KiB  
Article
Active Battery Voltage Equalization Based on Chain-Loop Comparison Strategy
by Kuo-Ing Hwu, Yuan-Hua Lin and Jenn-Jong Shieh
Energies 2024, 17(20), 5156; https://doi.org/10.3390/en17205156 - 16 Oct 2024
Viewed by 264
Abstract
This paper describes active battery balancing based on a bidirectional buck converter, a flyback converter, and battery cells by using the proposed chain-loop comparison strategy. The role of the bidirectional buck converter is to charge/discharge the battery pack. During the charging period, the [...] Read more.
This paper describes active battery balancing based on a bidirectional buck converter, a flyback converter, and battery cells by using the proposed chain-loop comparison strategy. The role of the bidirectional buck converter is to charge/discharge the battery pack. During the charging period, the converter is in buck mode, and its output is controlled by constant current/voltage; during the discharging period, the converter is in boost mode, and its output is controlled by constant voltage. The role of the flyback converter is voltage equalization of the battery pack, and its output is controlled by constant current. A chain-loop comparison strategy is used to control battery voltage equalization. In this work, three equalization modes, namely, charging balance, discharging balance, and static balance, were considered. The voltage difference between the maximum and minimum is 0.007 V after a balancing time of 19.75 min, 0.005 V after a balancing time of 24 min, and 0.007 V after a balancing time of 20 min for charging balance, discharging balance, and static balance, respectively. Full article
(This article belongs to the Special Issue Energy, Electrical and Power Engineering: 3rd Edition)
19 pages, 3472 KiB  
Article
Electrochemical DNA Sensor Based on Poly(proflavine) Deposited from Natural Deep Eutectic Solvents for DNA Damage Detection and Antioxidant Influence Assessment
by Anna Porfireva, Anastasia Goida, Vladimir Evtugyn, Milena Mozgovaya, Tatiana Krasnova and Gennady Evtugyn
Chemosensors 2024, 12(10), 215; https://doi.org/10.3390/chemosensors12100215 - 16 Oct 2024
Viewed by 370
Abstract
Electrochemical DNA sensors for DNA damage detection based on electroactive polymer poly(proflavine) (PPFL) that was synthesized at screen-printed carbon electrodes (SPCEs) from phosphate buffer (PB) and two natural deep eutectic solvents (NADESs) consisting of citric or malonic acids, D-glucose, and a certain amount [...] Read more.
Electrochemical DNA sensors for DNA damage detection based on electroactive polymer poly(proflavine) (PPFL) that was synthesized at screen-printed carbon electrodes (SPCEs) from phosphate buffer (PB) and two natural deep eutectic solvents (NADESs) consisting of citric or malonic acids, D-glucose, and a certain amount of water (NADES1 and NADES2) were developed. Poly(proflavine) coatings obtained from the presented media (PPFLPB, PPFLNADES1, and PPFLNADES2) were electrochemically polymerized via the multiple cycling of the potential or potentiostatic accumulation and used for the discrimination of thermal and oxidative DNA damage. The electrochemical characteristics of the poly(proflavine) coatings and their morphology were assessed using cyclic voltammetry (CV), electrochemical impedance spectroscopy (EIS), and scanning electron microscopy (SEM). The working conditions for calf thymus DNA implementation and DNA damage detection were estimated for all types of poly(proflavine) coatings. The voltammetric approach made it possible to distinguish native and chemically oxidized DNA while the impedimetric approach allowed for the successful recognition of native, thermally denatured, and chemically oxidized DNA through changes in the charge transfer resistance. The influence of different concentrations of conventional antioxidants and pharmaceutical preparations on oxidative DNA damage was characterized. Full article
(This article belongs to the Special Issue Electrochemical Biosensors: Advances and Prospects)
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<p>Chemical structure of proflavine hydrochloride.</p>
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<p>Multiple cyclic voltammograms recorded on the SPCE in (<b>a</b>) 0.025 M PB, pH 7.0, containing 0.5 mM proflavine or 0.085 M proflavine in (<b>b</b>) NADES1 and (<b>c</b>) NADES2; 0.1 V/s. Arrows indicate changes with increased number of cycles.</p>
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<p>Oxidation (black) and reduction (red) peak currents recorded in 0.025 M PB on the SPCE covered with (<b>a</b>) PPFL<sub>PB</sub>, (<b>b</b>) PPFL<sub>NADES1</sub>, and (<b>c</b>) PPFL<sub>NADES2</sub> at pH values of 2.0–9.0 (average ± S.D. for eight individual sensors).</p>
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<p>SEM images of (<b>a</b>) bare SPCE and SPCE covered with (<b>b</b>) PPFL<sub>PB</sub>, (<b>c</b>) PPFL<sub>NADES1</sub>, and (<b>d</b>) PPFL<sub>NADES2</sub>.</p>
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<p>Particle size distributions (Gaussian fitting) for (<b>a</b>) carbon ink nanoparticles of bare SPCE and microspheres of (<b>b</b>) PPFL<sub>PB</sub>, (<b>c</b>) PPFL<sub>NADES1</sub>, and (<b>d</b>) PPFL<sub>NADES2</sub> coatings.</p>
Full article ">Figure 6
<p>Relative changes in peak oxidation (black) and reduction (gray) currents after DNA immobilization on (<b>a</b>) PPFL<sub>PB</sub>, (<b>b</b>) PPFL<sub>NADES1</sub>, and (<b>c</b>) PPFL<sub>NADES2</sub>. DNA immobilization protocol: 1—drying; 2–5—incubation in DNA solution for 10, 20, 30, and 40 min, respectively. Specifications: cyclic voltammetry, 0.025 M PB; pH 7.0; from −0.6 to 0.6 V, 0.1 V/s.</p>
Full article ">Figure 7
<p>Relative changes in peak oxidation (black) and reduction (gray) currents for (<b>a</b>) PPFL<sub>PB</sub>, (<b>b</b>) PPFL<sub>NADES1</sub>, and (<b>c</b>) PPFL<sub>NADES2</sub>. Layer contents: 1—with no DNA, 2—native DNA, 3—thermally denatured DNA, and 4—chemically oxidized (Cu<sup>2+</sup>/H<sub>2</sub>O<sub>2</sub>) DNA.</p>
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<p>Equivalent circuit <span class="html-italic">Rs</span>(<span class="html-italic">R</span><sub>1</sub><span class="html-italic">C</span><sub>1</sub>)(<span class="html-italic">R</span><sub>2</sub><span class="html-italic">C</span><sub>2</sub>) for the evaluation of EIS parameters.</p>
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<p>Dependence of charge transfer resistance <span class="html-italic">R</span><sub>1</sub> on modified layer content: 1—bare SPCE, 2—SPCE/PPFL, 3—SPCE/PPFL/native DNA, 4—SPCE/PPFL/denatured DNA, 5—SPCE/PPFL/oxidized DNA, 6—SPCE/PPFL/PSS, and 7—SPCE/PPFL/H<sub>2</sub>O; (<b>a</b>) PPFL<sub>PB</sub>, (<b>b</b>) PPFL<sub>NADES1</sub>, (<b>c</b>) PPFL<sub>NADES2</sub>; 0.025 M PB, pH 7.0, in the presence of 0.01 M [Fe(CN)<sub>6</sub>]<sup>3−/4−</sup>. Average ± S.D. for ten individual sensors.</p>
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<p>Dependence of EIS parameters on antioxidant concentration. (<b>a</b>) Charge transfer resistance <span class="html-italic">R</span><sub>1</sub>, (<b>b</b>) constant phase element <span class="html-italic">C</span><sub>1</sub>; 0.025 M PB, pH 7.0, in the presence of 0.01 M [Fe(CN)<sub>6</sub>]<sup>3−/4−</sup>. Average ± S.D. values are shown for ten individual sensors.</p>
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