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12 pages, 4047 KiB  
Article
Multilayer Core-Sheath Structured Nickel Wire/Copper Oxide/Cobalt Oxide Composite for Highly Sensitive Non-Enzymatic Glucose Sensor
by Yuxin Wu, Zhengwei Zhu, Xinjuan Liu and Yuhua Xue
Nanomaterials 2025, 15(6), 411; https://doi.org/10.3390/nano15060411 - 7 Mar 2025
Viewed by 68
Abstract
The development of micro glucose sensors plays a vital role in the management and monitoring of diabetes, facilitating real-time tracking of blood glucose levels. In this paper, we developed a three-layer core-sheath microwire (NW@CuO@Co3O4) with nickel wire as the [...] Read more.
The development of micro glucose sensors plays a vital role in the management and monitoring of diabetes, facilitating real-time tracking of blood glucose levels. In this paper, we developed a three-layer core-sheath microwire (NW@CuO@Co3O4) with nickel wire as the core and copper oxide and cobalt oxide nanowires as the sheath. The unique core-sheath structure of microwire enables it to have both good conductivity and excellent electrochemical catalytic activity when used as an electrode for glucose detecting. The non-enzymatic glucose sensor base on a NW@CuO@Co3O4 core-sheath wire exhibits a high sensitivity of 4053.1 μA mM−1 cm−2, a low detection limit 0.89 μM, and a short response time of less than 2 s. Full article
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Figure 1

Figure 1
<p>(<b>a</b>) XRD spectrum of the NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrode. XPS spectra of the NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrode, (<b>b</b>) full spectrum, (<b>c</b>) Cu 2p spectrum, (<b>d</b>) Ni 2p spectrum, (<b>e</b>) Co 2p spectrum, and (<b>f</b>) O 1s spectrum.</p>
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<p>(<b>a</b>) SEM image of pure nickel wire. (<b>b</b>,<b>c</b>) SEM image of nickel wire after “alloy/de-alloy” treatment. (<b>d</b>–<b>f</b>) SEM image of NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrode.</p>
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<p>(<b>a</b>) TEM image of CuO–Co<sub>3</sub>O<sub>4</sub> composite. (<b>b</b>) TEM image of Co<sub>3</sub>O<sub>4</sub> nanowires, (<b>c</b>,<b>d</b>) TEM images of CuO nanoparticles.</p>
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<p>(<b>a</b>) Cyclic voltammograms of pure nickel wire electrode and NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrode at 50 mV s<sup>−1</sup> in 0.1 M NaOH solution with and without 1mM glucose added. (<b>b</b>) Cyclic voltammograms of NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrode at 50 mV s<sup>−1</sup> in different 0.1M NaOH solutions with different concentrations of glucose added. (<b>c</b>) Cyclic voltammograms of NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrode in 0.1 M NaOH at different scan rates (25~125 mv s<sup>−1</sup>). (<b>d</b>) Linear fitting diagram of cyclic voltammograms of oxidation peak current and reduction peak current at different scan rates and the half of the scan rate.</p>
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<p>Glucose detection performance of NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrode (<b>a</b>) Current versus time curves of adding 0.5 mM glucose six times at 50 s intervals to 0.1 M NaOH solution at different voltages (0.5~0.65 V). (<b>b</b>) Selectivity curve after adding 1 mM glucose, ascorbic acid (AA), dopamine hydrochloride (UA), uric acid (DA), and glucose to 0.1 M NaOH solution in sequence. (<b>c</b>) Amperometric response curve of adding different concentrations of glucose in 0.1 M NaOH solution in sequence at 0.55 V. (<b>d</b>) Linear fitting diagram of current and glucose concentration in alkaline solution.</p>
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<p>(<b>a</b>) Stability of NW@CuO@Co<sub>3</sub>O<sub>4</sub> glucose sensors in 0.1 mM glucose solution. (<b>b</b>) EIS curves of NW and NW@CuO@Co<sub>3</sub>O<sub>4</sub>. (<b>c</b>) Current responses of five NW@CuO@Co<sub>3</sub>O<sub>4</sub> electrodes in 0.1 M NaOH with 2 mM glucose at 0.55 V.</p>
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15 pages, 8175 KiB  
Article
Aptamer Paper-Based Fluorescent Sensor for Determination of SARS-CoV-2 Spike Protein
by Jincai Yang, Zunquan Zhao, Tianyi Ma and Jialei Bai
Sensors 2025, 25(6), 1637; https://doi.org/10.3390/s25061637 - 7 Mar 2025
Viewed by 85
Abstract
Point-of-care (POC) antigen detection plays a crucial role in curbing the spread of viruses. Paper-based fluorescence aptasensors are expected to offer a low-cost tool to meet the needs of decentralized POC diagnosis. Herein, we report on a fluorescent paper-based sensing system for detecting [...] Read more.
Point-of-care (POC) antigen detection plays a crucial role in curbing the spread of viruses. Paper-based fluorescence aptasensors are expected to offer a low-cost tool to meet the needs of decentralized POC diagnosis. Herein, we report on a fluorescent paper-based sensing system for detecting the SARS-CoV-2 spike protein. The sensing system was constructed by loading multi-layer Nb2C MXene nano-quenchers and carbon-dot-labeled aptamer (G-CDs@Apt) probes onto a mixed cellulose ester (MCE) paper substrate. On the Nb2C MXene/G-CDs@Apt sensing paper, abundant G-CDs@Apt probes were attached to the multilayer MXene nano-quenchers and kept in a fluorescence-off state, while recognition of the target detached the G-CDs@Apt probes formed the nano--quenchers, resulting in fluorescence recovery of the sensing paper. The developed paper-based sensor performed well in the one-step detection of the SARS-CoV-2 S1 protein with a detection limit of 0.067 ng/mL (0.335 pg/test). The assay exhibited good selectivity and anti-interference in the detection of the SARS-CoV-2 S1 protein in artificial saliva. Moreover, the paper-based aptasensor was successfully used to detect the SARS-CoV-2 S1 protein in actual environmental samples with recoveries of 90.87–100.55% and relative standard deviations of 1.52–3.41%. The proposed technology provides a cost-effective alternative to traditional antibody test strips for a wide range of POC diagnostic applications. Full article
(This article belongs to the Special Issue Point-of-Care Biosensors: Design and Applications)
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<p>Schematic of aptamer-based fluorescence paper sensor for SARS-CoV-2 spike protein.</p>
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<p>(<b>a</b>–<b>f</b>) SEM images of Nb<sub>2</sub>C MXene nano-quenchers on MCE substrate. Scale size: (<b>a</b>) 10 μm, (<b>b</b>) 5 μm, (<b>c</b>) 2 μm, (<b>d</b>) 1 μm, (<b>e</b>) 500 nm, and (<b>f</b>) 500 nm.</p>
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<p>Fluorescence quenching of G-CDs@Apt probes by Nb<sub>2</sub>C MXene nano-quenchers. (<b>a</b>) Fluorescence spectra of G-CDs (red line) and UV-vis absorption spectra of Nb<sub>2</sub>C MXene (green line, 0.1 mg/mL). (<b>b</b>) Fluorescence spectra of G-CDs@Apt probes in absence or presence of Nb<sub>2</sub>C MXene nano-quenchers under 470 nm excitation.</p>
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<p>Determination of SARS-CoV-2 S1 protein in a liquid reaction using Nb<sub>2</sub>C MXene/G-CDs@Apt system. (<b>a</b>) Fluorescence spectra of Nb<sub>2</sub>C MXene/G-CDs@Apt system after addition of different concentrations of SARS-CoV-2 S1 protein. (<b>b</b>) Linear relationship between fluorescence signal change (F−F<sub>0</sub>) and concentration of SARS-CoV-2 S1 protein. (<b>c</b>) Fluorescence intensity of different batches of Nb<sub>2</sub>C MXene/G-CDs@Apt system in response to SARS-CoV-2 S1 protein (50 ng/mL). (<b>d</b>) Fluorescence intensity of Nb<sub>2</sub>C MXene/G-CDs@Apt system in response to SARS-CoV-2 S1 protein (50 ng/mL) with incandescent pre-exposure for 0–60 min. Excitation: at 470 nm.</p>
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<p>Feasibility of Nb<sub>2</sub>C MXene/G-CDs@Apt sensor for fluorescence paper-based detection of SARS-CoV-2 S1 protein detection. (<b>a</b>) Schematic of fabrication and utilization process of paper fluorescence sensor. (<b>b</b>) G channel values in reaction region of Nb<sub>2</sub>C MXene/G-CDs@Apt paper sensor after reaction with different concentrations of SARS-CoV-2 S1 protein were analyzed using ImageJ software. Inset: Fluorescence images of Nb<sub>2</sub>C MXene/G-CDs@Apt test paper after reaction with different concentrations of SARS-CoV-2 S1 protein for 25 min under UV light (365 nm).</p>
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<p>Optimization of experimental conditions for fluorescence paper-based assay. (<b>a</b>) Optimization of G-CDs concentration used in aptamer modification process. (<b>b</b>) Optimization of Nb<sub>2</sub>C MXene concentration loaded on paper sensor. (<b>c</b>) Optimization of pre-incubation time of Nb<sub>2</sub>C MXene/G-CDs@Apt system. (<b>d</b>) Optimization of reaction time for fluorescence recovery after addition of SARS-CoV-2 S1 protein.</p>
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<p>Detection performance of Nb<sub>2</sub>C MXene/G-CDs@Apt fluorescence paper sensor. (<b>a</b>) Determination of SARS-CoV-2 S1 protein ranging from 0 to 10 ng/mL using Nb<sub>2</sub>C MXene/G-CDs@Apt test papers. (<b>b</b>) Determination of SARS-CoV-2 S1 protein ranging from 10 to 80 ng/mL using Nb<sub>2</sub>C MXene/G-CDs@Apt test papers. (<b>c</b>) Linear relationship between ΔG value and logarithm of SARS-CoV-2 S1 protein concentration (0.1–10 ng/mL). (<b>d</b>) Linear relationship between ΔG value and SARS-CoV-2 S1 protein concentration (10–80 ng/mL).</p>
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<p>Selectivity and anti-interference of Nb<sub>2</sub>C MXene/G-CDs@Apt fluorescence paper sensor. (<b>a</b>) Selectivity of paper-based sensor for SARS-CoV-2 S1 protein towards other proteins. (<b>b</b>) Effect of dilution of artificial saliva on SARS-CoV-2 S1 protein detection by sensor. HSD: high-salt phosphate buffer solution (PBS, 100 mM, pH = 7.4) with extra NaCl (274 mM). SD: phosphate buffer solution (PBS, 100 mM, pH = 7.4). “X”: dilution of saliva with ultrapure water.</p>
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30 pages, 14392 KiB  
Article
High-Quality Perovskite Thin Films for NO2 Detection: Optimizing Pulsed Laser Deposition of Pure and Sr-Doped LaMO3 (M = Co, Fe)
by Lukasz Cieniek, Agnieszka Kopia, Kazimierz Kowalski and Tomasz Moskalewicz
Materials 2025, 18(5), 1175; https://doi.org/10.3390/ma18051175 - 6 Mar 2025
Viewed by 87
Abstract
This study investigates the structural and catalytic properties of pure and Sr-doped LaCoO3 and LaFeO3 thin films for potential use as resistive gas sensors. Thin films were deposited via pulsed laser deposition (PLD) and characterized using X-ray diffraction (XRD), X-ray photoelectron [...] Read more.
This study investigates the structural and catalytic properties of pure and Sr-doped LaCoO3 and LaFeO3 thin films for potential use as resistive gas sensors. Thin films were deposited via pulsed laser deposition (PLD) and characterized using X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), scanning electron microscopy (SEM), atomic force microscopy (AFM), nanoindentation, and scratch tests. XRD analysis confirmed the formation of the desired perovskite phases without secondary phases. XPS revealed the presence of La3+, Co3+/Co4+, Fe3+/Fe4+, and Sr2+ oxidation states. SEM and AFM imaging showed compact, nanostructured surfaces with varying morphologies (shape and size of surface irregularities) depending on the composition. Sr doping led to surface refinement and increased nanohardness and adhesion. Transmission electron microscopy (TEM) analysis confirmed the columnar growth of nanocrystalline films. Sr-doped LaCoO3 demonstrated enhanced sensitivity and stability in the presence of NO2 gas compared to pure LaCoO3, as evidenced by electrical resistivity measurements within 230 ÷ 440 °C. At the same time, it was found that Sr doping stabilizes the catalytic activity of LaFeO3 (in the range of 300 ÷ 350 °C), although its behavior in the presence of NO2 differs from that of LaCo(Sr)O3—especially in terms of response and recovery times. These findings highlight the potential of Sr-doped LaCoO3 and LaFeO3 thin films for NO2 sensing applications. Full article
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Figure 1
<p>A representative example of the ABX<sub>3</sub> perovskite structure (<b>a</b>), along with its characteristic symmetry (<b>b</b>). The structural transformation scheme for LaMO<sub>3</sub> (M = Co, Fe) as a function of temperature is illustrated in (<b>c</b>). This transformation often leads to the formation of twin domains within the material, as depicted in (<b>d</b>).</p>
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<p>SEM images illustrating the surface topography of the targets used in the study; (<b>a</b>) LaCoO<sub>3</sub>, (<b>b</b>) La(Sr)CoO<sub>3</sub>, (<b>c</b>) LaFeO<sub>3</sub>, (<b>d</b>) La(Sr)FeO<sub>3</sub>; and (<b>e</b>) macro image of targets ready for microscopic examination and (<b>f</b>) the surface of the LaFeO<sub>3</sub> target after laser ablation.</p>
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<p>Laser ablation system (PLD) built with an Nd:YAG laser and the Neocera vacuum chamber, connected by an optical system (<b>a</b>). Schematic of the PLD process (<b>b</b>) and a view inside the process chamber (<b>c</b>).</p>
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<p>XRD phase analysis of (<b>a</b>) Sr-doped LaCoO<sub>3</sub> and (<b>b</b>) Sr-doped LaFeO<sub>3</sub> thin films, with JCPDS pattern cards and average crystallite sizes (estimated using the Williamson–Hall method).</p>
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<p>XPS detection/verification of chemical states of elements for La(Sr)CoO<sub>3</sub> thin films.</p>
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<p>XPS detection/verification of chemical states of elements for La(Sr)FeO<sub>3</sub> thin films.</p>
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<p>SEM images of the topography of perovskite thin films grown on monocrystalline Si substrates [001] with the result of EDS analysis of the chemical composition for (<b>a</b>) LaCoO<sub>3</sub> and (<b>b</b>) LaFeO<sub>3</sub>.</p>
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<p>SEM images of the topography of perovskite thin films grown on monocrystalline Si substrates [001] with the result of EDS analysis of the chemical composition for (<b>a</b>) Sr-doped LaCoO<sub>3</sub>, (<b>b</b>) Sr-doped LaFeO<sub>3</sub>.</p>
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<p>Surface topography images of perovskite thin films by atomic force microscopy (AFM) technique for (<b>a</b>) LaCoO<sub>3</sub> and (<b>b</b>) LaFeO<sub>3</sub>.</p>
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<p>Surface topography images of perovskite thin films by atomic force microscopy (AFM) technique for (<b>a</b>) Sr-doped LaCoO<sub>3</sub> and (<b>b</b>) Sr-doped LaFeO<sub>3</sub>.</p>
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<p>Examples of (<b>a</b>) indentation curve and (<b>b</b>) penetration depth and normal force plots obtained from nanohardness measurements of LaFeO<sub>3</sub> thin film on Si substrate.</p>
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<p>TEM analysis of LaCoO<sub>3</sub> thin films: (<b>a</b>) low-magnification bright-field image with selected area electron diffraction pattern, (<b>b</b>,<b>c</b>) high-resolution TEM images, and (<b>d</b>) SAED solved with TEM/EDS analysis.</p>
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<p>TEM analysis of Sr-doped LaCoO<sub>3</sub> thin films: (<b>a</b>,<b>b</b>,<b>d</b>,<b>e</b>) low-magnification bright- and (<b>c</b>,<b>f</b>) dark-field image with selected area electron diffraction patterns, and (<b>g</b>) SAED solved with TEM/EDS analysis.</p>
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<p>TEM analysis of LaFeO<sub>3</sub> thin films: (<b>a</b>,<b>b</b>) low-magnification bright- and (<b>c</b>) dark-field image with selected area electron diffraction pattern, (<b>d</b>,<b>e</b>) high-resolution TEM images, and (<b>f</b>) SAED solved with TEM/EDS analysis.</p>
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<p>TEM analysis of Sr-doped LaFeO<sub>3</sub> thin films: (<b>a</b>,<b>d</b>) low-magnification bright- and (<b>b</b>,<b>e</b>) dark-field image with selected area electron diffraction patterns, (<b>c</b>,<b>f</b>) high-resolution TEM images and (<b>g</b>) SAED pattern solved with TEM/EDS analysis.</p>
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<p>LaCoO<sub>3</sub> response at 500 °C exposed to 50 ppm of NO<sub>2</sub> using different currents: (<b>a</b>) 0.1 nA, (<b>b</b>) 1 nA, and (<b>c</b>) 10nA.</p>
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<p>Response of La(Sr)CoO<sub>3</sub> exposed to 50 ppm NO<sub>2</sub> at temperatures in the range of 230 ÷ 440 °C: (<b>a</b>) LaCoO<sub>3</sub>, (<b>b</b>) La<sub>0.9</sub>Sr<sub>0.1</sub>CoO<sub>3</sub>, and (<b>c</b>) La<sub>0</sub>.<sub>9</sub>Sr<sub>0.1</sub>CoO<sub>3</sub>.</p>
Full article ">Figure 17 Cont.
<p>Response of La(Sr)CoO<sub>3</sub> exposed to 50 ppm NO<sub>2</sub> at temperatures in the range of 230 ÷ 440 °C: (<b>a</b>) LaCoO<sub>3</sub>, (<b>b</b>) La<sub>0.9</sub>Sr<sub>0.1</sub>CoO<sub>3</sub>, and (<b>c</b>) La<sub>0</sub>.<sub>9</sub>Sr<sub>0.1</sub>CoO<sub>3</sub>.</p>
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<p>Response of LaFeO<sub>3</sub> exposed to 50 ppm NO<sub>2</sub> for a range of temperatures: (<b>a</b>) 230 °C, (<b>b</b>) 300 °C, (<b>c</b>) 350 °C, (<b>d</b>) 400 °C, and (<b>e</b>) 440 °C.</p>
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<p>Response of La<sub>0</sub>.<sub>9</sub>Sr<sub>0</sub>.<sub>1</sub>FeO<sub>3</sub> exposed to 50 ppm NO<sub>2</sub> (summary chart) and for a range of temperatures: (<b>a</b>) 230 °C, (<b>b</b>) 300 °C, (<b>c</b>) 350 °C, and (<b>d</b>) 440 °C.</p>
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<p>Response of La<sub>0</sub>.<sub>8</sub>Sr<sub>0</sub>.<sub>2</sub>FeO<sub>3</sub> exposed to 50 ppm NO<sub>2</sub> (summary chart) and for a range of temperatures: (<b>a</b>) 230 °C, (<b>b</b>) 300 °C, (<b>c</b>) 350 °C, and (<b>d</b>) 440 °C.</p>
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24 pages, 4014 KiB  
Article
Calibration of Low-Cost LoRaWAN-Based IoT Air Quality Monitors Using the Super Learner Ensemble: A Case Study for Accurate Particulate Matter Measurement
by Gokul Balagopal, Lakitha Wijeratne, John Waczak, Prabuddha Hathurusinghe, Mazhar Iqbal, Daniel Kiv, Adam Aker, Seth Lee, Vardhan Agnihotri, Christopher Simmons and David J. Lary
Sensors 2025, 25(5), 1614; https://doi.org/10.3390/s25051614 - 6 Mar 2025
Viewed by 130
Abstract
This study calibrates an affordable, solar-powered LoRaWAN air quality monitoring prototype using the research-grade Palas Fidas Frog sensor. Motivated by the need for sustainable air quality monitoring in smart city initiatives, this work integrates low-cost, self-sustaining sensors with research-grade instruments, creating a cost-effective [...] Read more.
This study calibrates an affordable, solar-powered LoRaWAN air quality monitoring prototype using the research-grade Palas Fidas Frog sensor. Motivated by the need for sustainable air quality monitoring in smart city initiatives, this work integrates low-cost, self-sustaining sensors with research-grade instruments, creating a cost-effective hybrid network that enhances both spatial coverage and measurement accuracy. To improve calibration precision, the study leverages the Super Learner machine learning technique, which optimally combines multiple models to achieve robust PM (Particulate Matter) monitoring in low-resource settings. Data was collected by co-locating the Palas sensor and LoRaWAN devices under various climatic conditions to ensure reliability. The LoRaWAN monitor measures PM concentrations alongside meteorological parameters such as temperature, pressure, and humidity. The collected data were calibrated against precise PM concentrations and particle count densities from the Palas sensor. Various regression models were evaluated, with the stacking-based Super Learner model outperforming traditional approaches, achieving an average test R2 value of 0.96 across all target variables, including 0.99 for PM2.5 and 0.91 for PM10.0. This study presents a novel approach by integrating Super Learner-based calibration with LoRaWAN technology, offering a scalable solution for low-cost, high-accuracy air quality monitoring. The findings demonstrate the feasibility of deploying these sensors in urban areas such as the Dallas-Fort Worth metroplex, providing a valuable tool for researchers and policymakers to address air pollution challenges effectively. Full article
(This article belongs to the Section Sensor Networks)
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Figure 1
<p>Annotated figure of Palas Fidas Frog from the Palas product information page [<a href="#B18-sensors-25-01614" class="html-bibr">18</a>].</p>
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<p>Sensors used in the low-cost LoRaWAN air quality monitor. (<b>a</b>) PPD42NS—The PM sensor used in the LoRaWAN-based air quality monitor which measures particulate matter with sizes larger than 1 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m and 2.5 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m [<a href="#B20-sensors-25-01614" class="html-bibr">20</a>]. (<b>b</b>) BME280—The climate sensor used in the LoRaWAN-based air quality monitor which measures air temperature, atmospheric pressure, and relative humidity [<a href="#B21-sensors-25-01614" class="html-bibr">21</a>,<a href="#B22-sensors-25-01614" class="html-bibr">22</a>].</p>
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<p>Calibration site for LoRaWAN air quality monitor deployment (indicated by the red marker and labeled in blue).</p>
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<p>Overview of the calibration workflow using machine learning models. The process starts with LoRa prototype sensor data (features) and Palas Fidas Frog sensor data (target variables). Data preprocessing includes resampling at 30-s intervals, handling missing values, normalizing data, and selecting relevant features. Various regression models are trained separately for each target variable, along with a Stacking Regressor (SL) that combines different learner combinations. The best-performing model for each target variable is determined based on test R<sup>2</sup>, followed by hyperparameter tuning using random search. The final models undergo validation to ensure generalization to unseen data and are evaluated through scatter plots, quantile–quantile plots, permutation importance rankings, and error distributions.</p>
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<p>Scatter plots (<b>a</b>–<b>f</b>) illustrate the performance of hyperparameter-optimized stacking models for PM<sub>1.0</sub>, PM<sub>2.5</sub>, PM<sub>4.0</sub>, PM<sub>10</sub>, Total PM Concentration, and Particle Count Density, respectively. The blue and orange dots represent the training and testing datasets. Marginal distributions of the actual data (<b>top</b>) and predicted data (<b>right</b>) provide additional insights into the model’s performance. The legends include the train-test split count and R<sup>2</sup> values, quantifying the accuracy and overall effectiveness of the predictions.</p>
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<p>The plots (<b>a</b>–<b>f</b>) illustrate the Quantile–Quantile (QQ) plots for the hyperparameter-optimized stacking models for PM<sub>1.0</sub>, PM<sub>2.5</sub>, PM<sub>4.0</sub>, PM<sub>10</sub>, Total PM Concentration, and Particle Count Density, respectively. The quantiles of the actual test data are represented on the x-axis, while the quantiles of the predicted test data are shown on the y-axis. The 0th, 25th, 50th, 75th, and 100th quantiles are marked as pink, orange, green, red, and purple diamonds, respectively. These plots provide a visual comparison of the distribution alignment between the actual and predicted test data, demonstrating the performance of the stacking models.</p>
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<p>The plots (<b>a</b>–<b>f</b>) illustrate the feature importance rankings of the hyperparameter-optimized stacking models for PM<sub>1.0</sub>, PM<sub>2.5</sub>, PM<sub>4.0</sub>, PM<sub>10</sub>, Total PM Concentration, and Particle Count Density, respectively. The permutation importance rankings are displayed as horizontal bar charts, with the most important feature ranked at the top, followed by other features in descending order of importance. These rankings highlight the relative contribution of each feature to the prediction accuracy of the stacking models.</p>
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<p>The plots (<b>a</b>–<b>f</b>) illustrate the error distribution of the hyperparameter-optimized stacking models for PM<sub>1.0</sub>, PM<sub>2.5</sub>, PM<sub>4.0</sub>, PM<sub>10</sub>, Total PM Concentration, and Particle Count Density, respectively. The error distributions are displayed as histograms (in red color). The y-axis represents the frequency of errors, while the x-axis shows the prediction error for test data, calculated as the actual test data–predicted test data. The threshold for identifying significant errors is set at ±5 for each target variable.</p>
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30 pages, 4653 KiB  
Review
Nanoarchitectonics of Sustainable Food Packaging: Materials, Methods, and Environmental Factors
by Tangyu Yang and Andre G. Skirtach
Materials 2025, 18(5), 1167; https://doi.org/10.3390/ma18051167 - 6 Mar 2025
Viewed by 171
Abstract
Nanoarchitectonics influences the properties of objects at micro- and even macro-scales, aiming to develop better structures for protection of product. Although its applications were analyzed in different areas, nanoarchitectonics of food packaging—the focus of this review—has not been discussed, to the best of [...] Read more.
Nanoarchitectonics influences the properties of objects at micro- and even macro-scales, aiming to develop better structures for protection of product. Although its applications were analyzed in different areas, nanoarchitectonics of food packaging—the focus of this review—has not been discussed, to the best of our knowledge. The (A) structural and (B) functional hierarchy of food packaging is discussed here for the enhancement of protection, extending shelf-life, and preserving the nutritional quality of diverse products including meat, fish, dairy, fruits, vegetables, gelled items, and beverages. Interestingly, the structure and design of packaging for these diverse products often possess similar principles and methods including active packaging, gas permeation control, sensor incorporation, UV/pulsed light processing, and thermal/plasma treatment. Here, nanoarchitechtonics serves as the unifying component, enabling protection against oxidation, light, microbial contamination, temperature, and mechanical actions. Finally, materials are an essential consideration in food packaging, particularly beyond commonly used polyethylene (PE), polypropylene (PP), polyethylene terephthalate (PET), polystyrene (PS), and polyvinyl chloride (PVC) plastics, with emphasis on biodegradable (polybutylene succinate (PBS), polyvinyl alcohol (PVA), polycaprolactone (PCL), and polybutylene adipate co-terephthalate (PBAT)) as well as green even edible (bio)-materials: polysaccharides (starch, cellulose, pectin, gum, zein, alginate, agar, galactan, ulvan, galactomannan, laccase, chitin, chitosan, hyaluronic acid, etc.). Nanoarchitechnotics design of these materials eventually determines the level of food protection as well as the sustainability of the processes. Marketing, safety, sustainability, and ethics are also discussed in the context of industrial viability and consumer satisfaction. Full article
(This article belongs to the Special Issue Nanoarchitectonics in Materials Science, Second Edition)
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<p>Hierarchy of food packaging. (<b>A</b>) Structural composition of food packaging showing its constituents depending on the size and scale. Nanoarchitectonics (underlined in <span class="html-italic">italic</span> at the bottom) schematically shows the density of both molecules and package walls as it determines the properties at the micro- (investigated by digital microscopy) and macro- (photographed from food packages available in a supermarket) scales. (<b>B</b>) Functional properties nanoarchitectonics identifying protection against bacteria, oxygen, contamination, bacteria, mechanical damage (schematics at the bottom), and food packaging available in a supermarket (top).</p>
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<p>(<b>A</b>) A photograph of PAW generation. (<b>B</b>) The thermographic measurement of plasma near the water surface during PAW generation.z (<b>C</b>) PAW inactivation efficacy against <span class="html-italic">S. aureus</span> inoculated on strawberries with 4-day storage, columns with different letters indicate a significant difference (<span class="html-italic">p</span> &lt; 0.05) (adapted from [<a href="#B132-materials-18-01167" class="html-bibr">132</a>] with permission from Elsevier). (<b>D</b>) Images of colorimetric response of curcumin solution and films in buffers with different pH values: films for monitoring pork freshness (adapted from [<a href="#B119-materials-18-01167" class="html-bibr">119</a>] with permission from Elsevier). (<b>E</b>) Changes in oscillating frequency (red or blue line, left axis), from the 5th overtone from the QCM-D measurements, and energy dissipation (green line, right axis) as a function of time, recorded during the deposition of five bilayers for the PEI/EH system at pH 8 (adapted from [<a href="#B108-materials-18-01167" class="html-bibr">108</a>]). (<b>F</b>) Longitudinal tensile strength of film (adapted from [<a href="#B134-materials-18-01167" class="html-bibr">134</a>] with permission from Elsevier).</p>
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<p>Classification of plastic- and biopolymer-based materials used for packaging. (I) Polyethylene (PE), polypropylene (PP), polyethylene terephthalate (PET), polystyrene (PS), and polyvinyl chloride (PVC). (II) Polybutylene succinate (PBS), polyvinyl alcohol (PVA), polycaprolactone (PCL), and polybutylene adipate co-terephthalate (PBAT). (III) Polylactic acid (PLA), polyhydroxyalkanoates (PHA), polyhydroxybutyrate (PHB), and hyaluronic acid (HA). *—can also be synthesized in laboratory conditions.</p>
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<p>SEM cross-sectional images of glass microbeads in PLA films. (<b>A</b>) The distribution of glass microbeads in PLA; (<b>B</b>) a closer look and cone structure; (<b>C</b>) adhesion to the surface. Reproduced from [<a href="#B192-materials-18-01167" class="html-bibr">192</a>] with permission Elsevier.</p>
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<p>(<b>A</b>) Schematic diagram of the preparation process of an alginate–gellan gum–carboxymethyl cellulose (Alg-GG-CMC) hydrogel, where (<b>B</b>) molecular and ionic interaction are shown between Alg, GG, CMC, and Ca<sup>2+</sup> ions, respectively. (<b>C</b>) Cryo-SEM images of the surface (reproduced from [<a href="#B214-materials-18-01167" class="html-bibr">214</a>] with permission Elsevier).</p>
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<p>Overview of steps driving development in food packaging, shown as an iceberg (<b>left panel</b>), where consumer preferences need to be satisfied (transparently visible above the water level), while research, development, safety regulations, sustainability, and industry are shown below (often less visible/hidden under water level). Nanoarchitectonics is directly linked with the bottom blocks of the “iceberg”, but those blocks have direct relation with and influence its upper parts. Industrial production and governmental regulations accompanying development of products (<b>right panel</b>).</p>
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12 pages, 2100 KiB  
Article
Detection of IgG Antibodies Against COVID-19 N-Protein by Hybrid Graphene–Nanorod Sensor
by R. V. A. Boaventura, C. L. Pereira, C. Junqueira, K. B. Gonçalves, N. P. Rezende, I. A. Borges, R. C. Barcelos, F. B. Oréfice, F. F. Bagno, F. G. Fonseca, A. Corrêa, L. S. Gomes and R. G. Lacerda
Biosensors 2025, 15(3), 164; https://doi.org/10.3390/bios15030164 - 4 Mar 2025
Viewed by 214
Abstract
The COVID-19 pandemic highlighted the global necessity to develop fast, affordable, and user-friendly diagnostic alternatives. Alongside recognized tests such as ELISA, nanotechnologies have since been explored for direct and indirect diagnosis of SARS-CoV-2, the etiological agent of COVID-19. Accordingly, in this work, we [...] Read more.
The COVID-19 pandemic highlighted the global necessity to develop fast, affordable, and user-friendly diagnostic alternatives. Alongside recognized tests such as ELISA, nanotechnologies have since been explored for direct and indirect diagnosis of SARS-CoV-2, the etiological agent of COVID-19. Accordingly, in this work, we report a method to detect anti-SARS-CoV-2 antibodies based on graphene-based field-effect transistors (GFETs), using a nanostructured platform of graphene with added gold nanorods (GNRs) and a specific viral protein. To detect anti-N-protein IgG antibodies for COVID-19 in human sera, gold nanorods were functionalized with the nucleocapsid (N) protein of SARS-CoV-2, and subsequently deposited onto graphene devices. Our test results demonstrate that the sensor is highly sensitive and can detect antibody concentrations as low as 100 pg/mL. Using the sensor to test human sera that were previously diagnosed with ELISA showed a 90% accuracy rate compared to the ELISA results, with the test completed in under 15 min. Integrating graphene and nanorods eliminates the need for a blocker, simplifying sensor fabrication. This hybrid sensor holds robust potential to serve as a simple and efficient point-of-care platform. Full article
(This article belongs to the Special Issue Two-Dimensional Nanomaterials for (Bio)sensing Application)
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<p>(<b>a</b>) A schematic model of the process of detecting the binding between the N-protein and the IgG antibody using the graphene field-effect transistor (GFET) platform, before (I) and after (II) the addition of human serum. (<b>b</b>) The antigen/antibody binding process, wherein the IgG antibody links to the N-protein at the edges of the gold nanorod. (<b>c</b>) A model of transfer curves before (I) and after (II) the binding, showing p-type doping in graphene.</p>
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<p>The biosensor characterization was conducted using AFM and Raman spectroscopy. (<b>a</b>) An optical image depicts a graphene monolayer after the deposition of gold nanorods. (<b>b</b>) An AFM topographic image of the same graphene is presented, delineated by a dashed line, with several deposited nanorods visible as light dots in the image. (<b>c</b>) An AFM image shows three isolated nanorods, with the same topographic scale as in b and c. (<b>d</b>) A height profile of a nanorod is included, with the line indicated in c, revealing an average height of 27 nm and a length of approximately 78 nm. (<b>e</b>) Raman spectra of graphene before and after B-GNR deposition are compared. (<b>f</b>) A band shift from the 2D band in e illustrates n-type doping. (<b>g</b>) A spectral map of I<sub>2D</sub>/I<sub>G</sub> on pristine graphene is shown. (<b>h</b>) A spectral map of I<sub>2D</sub>/I<sub>G</sub> on B-GNR graphene is also provided.</p>
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<p>(<b>a</b>) The measurements of the transfer curves, with V<sub>SD</sub> = 0.1 V, for pristine graphene (black line), after B-GNR solution deposition on graphene (red line), and after antigen/antibody binding (blue line). (<b>b</b>) The variation in the normalized current at a series of concentrations (100 pg/mL~1 μg/mL) of the target monoclonal IgG antibody in pristine graphene (black line) and in B-GNR graphene, for different concentrations of target IgG monoclonal antibodies (red line). (<b>c</b>) A calibration curve for the series of target monoclonal IgG concentrations (semi-log scale). The error bars indicate standard deviation based on measurements with different devices.</p>
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<p>Transfer curves from exposure of the biosensor to human sera for 1 h. (<b>a</b>) A rightward shift in the transfer curve after exposing the biosensor to human serum that did not contain IgG antibodies (Serological Sample 1). (<b>b</b>) A rightward shift in the transfer curve after exposing the biosensor to human serum containing IgG antibodies (Serological Sample 2). (<b>c</b>) The current normalization of transfer curves A (blue) and B (red), as well as the black arrows, shows the range of results obtained from 10 different serological samples.</p>
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12 pages, 3718 KiB  
Article
Online Monitoring of Faulty Gases (O3, NO2, CO) in Substation Secondary Equipment Based on Cr-Doped BN Sensor: Insights from Density Functional Theory
by Zhiqi Guo, Peifeng Gao, Yibo Wang, Zhiqiang Wang, Jinchen Li and Hongbo Zou
Processes 2025, 13(3), 746; https://doi.org/10.3390/pr13030746 - 4 Mar 2025
Viewed by 136
Abstract
The secondary equipment of a substation is pivotal for maintaining the safe and reliable operation of the power grid. However, over time, insulation defects can inevitably arise in this equipment. Gas detection in substation secondary equipment has proven to be an effective method [...] Read more.
The secondary equipment of a substation is pivotal for maintaining the safe and reliable operation of the power grid. However, over time, insulation defects can inevitably arise in this equipment. Gas detection in substation secondary equipment has proven to be an effective method for assessing its insulation status. In this paper, we employed a density functional theory (DFT) approach to simulate the adsorption process of three types of fault gases from substation secondary equipment onto Cr-modified BN nanosheets. From the doped and adsorption models, two stable structures were chosen, and by calculating their band structures, density of states, and differential charge density, we uncovered the relevant adsorption and sensing mechanisms. Our findings reveal that Cr-modified BN nanosheets possess robust gas-sensing capabilities, particularly in capturing O3, which is primarily attributable to the contribution of Cr’s 4d orbital electron layer. Specifically, the adsorption capacity of Cr-modified BN nanosheets for fault gases in substation secondary equipment follows the order: O3 > NO2 > CO. The adsorption of Cr-BN on the three target gases mainly tends to be chemisorption accompanied by chemical bond breaking. Notably, there are significant changes in the electronic properties of the adsorbent substrate before and after the adsorption of the target gas molecules, resulting in alterations in its overall conductivity. This research lays the theoretical groundwork for the experimental development of high-performance gas-sensitive sensors designed to detect fault gases in substation secondary equipment. Full article
(This article belongs to the Section Energy Systems)
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<p>The spatial configurations of fault decomposition gases emanating from secondary equipment in substations and intrinsic BN.</p>
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<p>The spatial configurations of Cr-BN resulting from various doping methods.</p>
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<p>Band structures of BN before and after doping.</p>
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<p>DOS before and after Cr doping (dashed line indicates the Fermi level).</p>
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<p>DCD after Cr doping.</p>
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<p>The most stable configurations of Cr-BN when adsorbing target fault gases.</p>
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<p>Band configurations of diverse adsorption scenarios.</p>
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<p>Charge density variation across various adsorption systems.</p>
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11 pages, 4211 KiB  
Communication
Investigation of the Influence of Adhesion Layers on the Gas Sensing Performance of CuO/Cu2O Thin Films
by Christian Maier, Larissa Egger, Anton Köck and Klaus Reichmann
Chemosensors 2025, 13(3), 80; https://doi.org/10.3390/chemosensors13030080 - 2 Mar 2025
Viewed by 284
Abstract
This parameter study examines the impact of two distinct adhesion layers, chromium (Cr) and titanium (Ti), on the performance of CuO/Cu2O-based chemoresistive gas sensors by varying the layer thickness. The sensing material utilised on a Si-SiO2 sensor chip with Pt [...] Read more.
This parameter study examines the impact of two distinct adhesion layers, chromium (Cr) and titanium (Ti), on the performance of CuO/Cu2O-based chemoresistive gas sensors by varying the layer thickness. The sensing material utilised on a Si-SiO2 sensor chip with Pt electrodes is an ultrathin CuO/Cu2O film fabricated through thermal deposition of Cu and subsequent oxidation. The sensors were evaluated by measuring the change in electrical resistance against a range of target gases, including carbon monoxide (CO), carbon dioxide (CO2) and a mixture of hydrocarbons (HCMix), in order to assess any potential cross-sensitivity issues. As the reactions occur at the surface, the surface was characterised by scanning electron microscopy (SEM) and the composition by grazing incidence X-Ray diffraction (GIXRD) measurement to gain further insight into the influence of the adhesion layer on the sensing performance. Full article
(This article belongs to the Special Issue Recent Advances in Metal Oxide-Based Gas Sensors)
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<p>Illustration of the different layers of the Si-SiO<sub>2</sub> platform chip with Ti as adhesion layer for the Pt electrodes and, on top, the adhesion layer of Cr or Ti, with the oxidised CuO/Cu<sub>2</sub>O-sensing layer.</p>
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<p>SEM pictures of the sensors with different thicknesses of adhesion layers: (<b>a</b>) 5 nm thick Cr, (<b>b</b>) 15 nm thick Cr, (<b>c</b>) 25 nm thick Cr, (<b>d</b>) 5 nm thick Ti, (<b>e</b>) 15 nm thick Ti and (<b>f</b>) 25 nm thick Ti.</p>
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<p>SEM pictures of the surfaces with different thicknesses of adhesion layers: (<b>a</b>) 5 nm thick Cr, (<b>b</b>) 15 nm thick Cr, (<b>c</b>) 25 nm thick Cr, (<b>d</b>) 5 nm thick Ti, (<b>e</b>) 15 nm thick Ti and (<b>f</b>) 25 nm thick Ti.</p>
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<p>GIXRD measurement of the samples with different thicknesses of adhesion layers: 5 nm thick Cr, 15 nm thick Cr, 25 nm thick Cr, 5 nm thick Ti, 15 nm thick Ti and 25 nm thick Ti.</p>
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<p>Resistance measurement against 5, 10 and 20 ppm exposure of CO of the samples with different thicknesses of adhesion layers: (<b>a</b>) 5, 15 and 25 nm thick Cr; (<b>b</b>) 5, 15 and 25 nm thick Ti.</p>
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<p>Calculated sensor response average values of the 16 sensors with variation in the thicknesses (5, 15 and 25 nm) of Cr (<b>a</b>–<b>c</b>) and Ti (<b>d</b>–<b>f</b>) adhesion layers for the different gases: (<b>a</b>,<b>d</b>) 1000, 2000 and 4000 ppm of CO<sub>2</sub>; (<b>b</b>,<b>e</b>) 5, 10 and 20 ppm of CO; (<b>c</b>,<b>f</b>) 5, 10 and 20 ppm of HC<sub>Mix</sub>.</p>
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<p>Calculated sensor response average values of the 16 sensors with variation in the thicknesses (5, 15 and 25 nm) of Cr (<b>a</b>–<b>c</b>) and Ti (<b>d</b>–<b>f</b>) adhesion layers plotted against the test gas concentration: (<b>a</b>,<b>d</b>) 1000, 2000 and 4000 ppm of CO<sub>2</sub>; (<b>b</b>,<b>e</b>) 5, 10 and 20 ppm of CO; (<b>c</b>,<b>f</b>) 5, 10 and 20 ppm of HC<sub>Mix</sub>.</p>
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15 pages, 662 KiB  
Review
Unravelling Shared Pathways Linking Metabolic Syndrome, Mild Cognitive Impairment, Dementia, and Sarcopenia
by Daniela Ceccarelli Ceccarelli and Sebastiano Bruno Solerte
Metabolites 2025, 15(3), 159; https://doi.org/10.3390/metabo15030159 - 27 Feb 2025
Viewed by 496
Abstract
Background: Aging is characterized by shared cellular and molecular processes, and aging-related diseases might co-exist in a cluster of comorbidities, particularly in vulnerable individuals whose phenotype meets the criteria for frailty. Whilst the multidimensional definition of frailty is still controversial, there is [...] Read more.
Background: Aging is characterized by shared cellular and molecular processes, and aging-related diseases might co-exist in a cluster of comorbidities, particularly in vulnerable individuals whose phenotype meets the criteria for frailty. Whilst the multidimensional definition of frailty is still controversial, there is an increasing understanding of the common pathways linking metabolic syndrome, cognitive decline, and sarcopenia, frequent conditions in frail elderly patients. Methods: We performed a systematic search in the electronic databases Cochrane Library and PubMed and included preclinical studies, cohort and observational studies, and trials. Discussion: Metabolic syndrome markers, such as insulin resistance and the triglyceride/HDL C ratio, correlate with early cognitive impairment. Insulin resistance is a cause of synaptic dysfunction and neurodegeneration. Conversely, fasting and fasting-mimicking agents promote neuronal resilience by enhancing mitochondrial efficiency, autophagy, and neurogenesis. Proteins acting as cellular metabolic sensors, such as SIRT1, play a pivotal role in aging, neuroprotection, and metabolic health. In AD, β-amyloid accumulation and hyperphosphorylated tau in neurofibrillary tangles can cause metabolic reprogramming in brain cells, shifting from oxidative phosphorylation to aerobic glycolysis, similar to the Warburg effect in cancer. The interrelation of metabolic syndrome, sarcopenia, and cognitive decline suggests that targeting these shared metabolic pathways could mitigate all the conditions. Pharmacological interventions, including GLP-1 receptor agonists, metformin, and SIRT 1 inducers, demonstrated neuroprotective effects in animals and some preliminary clinical models. Conclusions: These findings encourage further research on the prevention and treatment of neurodegenerative diseases as well as the drug-repurposing potential of molecules currently approved for diabetes, dyslipidemia, and metabolic syndrome. Full article
(This article belongs to the Special Issue Brain Metabolic Alterations in Neurodegenerative Diseases)
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<p>Overview of neuroprotective pathways activated by SIRT1.</p>
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14 pages, 9414 KiB  
Article
Development and Field Deployment of a Compact Dual-Range Infrared Carbon Dioxide Sensor System
by Xiaoteng Liu, Xuehua Xiao, Zhening Zhang, Fang Song, Yiding Wang and Chuantao Zheng
Sensors 2025, 25(5), 1445; https://doi.org/10.3390/s25051445 - 27 Feb 2025
Viewed by 112
Abstract
A dual-range mid-infrared carbon dioxide (CO2) sensor is developed with temperature and humidity compensation functionalities. Using the same optical path, the sensor employs dual-channel signal processing circuits to achieve measurements across two detection ranges of 200–3000 parts-per-million (ppm) (low concentration range) [...] Read more.
A dual-range mid-infrared carbon dioxide (CO2) sensor is developed with temperature and humidity compensation functionalities. Using the same optical path, the sensor employs dual-channel signal processing circuits to achieve measurements across two detection ranges of 200–3000 parts-per-million (ppm) (low concentration range) and 8–25% (high concentration range), respectively. The developed sensor, with a compact size of 8.5 × 5.5 × 3.5 cm3, shows a good linear response, with fitting goodness R2 = 0.99942 for the low range and R2 = 0.9993 for the high range. Under environmental conditions of 20 °C temperature and 30% relative humidity and with an averaging time of 1 s, the limits of detection are 0.15 ppm for the low range and 32.4 ppm for the high range, respectively. A temperature and humidity compensation scheme based on multiple linear regression is proposed to mitigate the impact of environmental temperature and humidity changes. The experimental results demonstrate that the relative error after compensation is reduced from 21% to 0.87%. Indoor and outdoor CO2 measurements are performed to validate the good characteristics of the sensor system. Full article
(This article belongs to the Section Optical Sensors)
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<p>(<b>a</b>) Block diagram of the NDIR-based CO<sub>2</sub> sensor system. (<b>b</b>) Light source IR55. (<b>c</b>) Detector LIM-262-DH. (<b>d</b>) Microcontroller circuit and gas cell.</p>
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<p>The absorbance of CO<sub>2</sub>, CO, CH<sub>3</sub>OH, and CH<sub>2</sub>O was simulated under the conditions of a temperature of 300 K, a pressure of 1 atm, and an optical path length of 1 cm. Because the absorption coefficients of CO, CH<sub>3</sub>OH and CH<sub>2</sub>O are too low, close to 0, they are not obvious in the figure.</p>
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<p>Schematic diagram of signal conditioning circuit. The subscripts “<span class="html-italic">H</span>” and “<span class="html-italic">L</span>” are the parameters for the high-concentration detection channel and low-concentration detection range, respectively.</p>
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<p>(<b>a</b>) Relationship between the first harmonic amplitude and measurement time for low concentration range. (<b>b</b>) Relationship between first harmonic amplitude and concentration for low concentration range. (<b>c</b>) Relationship between first harmonic amplitude and measurement time for high concentration range. (<b>d</b>) Relationship between first harmonic amplitude and concentration for high concentration range.</p>
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<p>(<b>a</b>) Long-term measurement results of the 1000 ppm CO<sub>2</sub> sample in low concentration range. (<b>b</b>) Allan deviation curve at low concentration range. (<b>c</b>) Long-term measurement results of the 10% CO<sub>2</sub> sample in high concentration range. (<b>d</b>) Allan deviation curve at high concentration range.</p>
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<p>(<b>a</b>) A photo of the sensor temperature and humidity test. (<b>b</b>) The overall variation trend of the first harmonic amplitude under different temperatures and humidities. (<b>c</b>) The specific first harmonic amplitude data under different temperatures and humidities. (<b>d</b>) The measured gas concentration, as well as temperature and humidity, after compensation.</p>
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<p>Flowchart of temperature and humidity compensation algorithm.</p>
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<p>(<b>a</b>) Time measurement results of CO<sub>2</sub> concentration. (<b>b</b>) Spatial distribution of measured CO<sub>2</sub> concentration.</p>
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<p>(<b>a</b>) Site of an experiment for smolder detection of fire. (<b>b</b>) CO<sub>2</sub> concentration changes over time.</p>
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<p>Long-term CO<sub>2</sub> concentration detection results for three days.</p>
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<p>(<b>a</b>) Structure diagram of underwater CO<sub>2</sub> detection system. (<b>b</b>) Physical diagram of underwater CO<sub>2</sub> detection system.</p>
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<p>Underwater measurement results.</p>
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14 pages, 3567 KiB  
Article
Adsorption and Detection of Toxic Gases on CuO-Modified SnS Monolayers: A DFT Study
by Xinyue Liang, Ping Wang, Kai Zheng, Xuan Yang, Meidan Luo, Jiaying Wang, Yujuan He, Jiabing Yu and Xianping Chen
Sensors 2025, 25(5), 1439; https://doi.org/10.3390/s25051439 - 26 Feb 2025
Viewed by 320
Abstract
The emission of toxic gases such as NO2, NO, SO2, and CO from industrial activities, transportation, and energy production poses significant threats to the environment and public health. Traditional gas sensors often lack high sensitivity and selectivity. To address [...] Read more.
The emission of toxic gases such as NO2, NO, SO2, and CO from industrial activities, transportation, and energy production poses significant threats to the environment and public health. Traditional gas sensors often lack high sensitivity and selectivity. To address this, our study uses first-principles density functional theory (DFT) to investigate CuO-SnS monolayers for improved gas sensor performance. The results show that CuO modification significantly enhances the adsorption capacity and selectivity of SnS monolayers for NO2 and NO, with adsorption energies of −2.301 eV and −2.142 eV, respectively. Furthermore, CuO modification is insensitive to CO2 adsorption, demonstrating excellent selectivity. Structural and electronic analyses reveal that CuO modification reduces the band gap of SnS monolayers from 1.465 eV to 0.635 eV, improving the electrical conductivity and electron transfer, thereby enhancing the gas adsorption sensitivity. Further analyses highlight significant electronic interactions and charge transfer mechanisms between CuO-SnS monolayers and NO2 and SO2 molecules, indicating strong orbital hybridization. In conclusion, this study provides a theoretical basis for developing high-performance gas sensors, showing that CuO-SnS monolayers have great potential for detecting toxic gases. Full article
(This article belongs to the Special Issue Chemical Sensors for Toxic Chemical Detection: 2nd Edition)
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<p>Geometric structures of pure SnS and CuO-SnS: (<b>a</b>–<b>d</b>) top and side views. Geometric structures of (<b>e</b>) NO<sub>2</sub>, (<b>f</b>) NO, (<b>g</b>) CO<sub>2</sub>, (<b>h</b>) CO, and (<b>i</b>) SO<sub>2</sub> molecules.</p>
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<p>The band structures of (<b>a</b>) pure SnS and (<b>b</b>) CuO-SnS. The TDOS of (<b>c</b>) CuO-SnS and PDOS of (<b>d</b>) CuO-SnS.</p>
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<p>The most stable structure of the system after gas adsorption: (<b>a1</b>) NO<sub>2</sub>, (<b>a2</b>) NO, (<b>a3</b>) CO<sub>2</sub>, (<b>a4</b>) CO, (<b>a5</b>) SO<sub>2</sub>, and (<b>a6</b>) O<sub>2</sub> adsorbed on pure SnS; (<b>b1</b>) NO<sub>2</sub>, (<b>b2</b>) NO, (<b>b3</b>) CO<sub>2</sub>, (<b>b4</b>) CO, (<b>b5</b>) SO<sub>2</sub>, and (<b>b6</b>) O<sub>2</sub> adsorbed on CuO-SnS.</p>
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<p>Gas adsorption on pure SnS and CuO-SnS surfaces: (<b>a</b>) Adsorption energies of gases on SnS and CuO-SnS. (<b>b</b>) Electron transfer upon gas adsorption on SnS and CuO-SnS. (<b>c</b>) Adsorption energies of gases in the presence of O<sub>2</sub>. (<b>d</b>) Adsorption energies of gases on CuO-SnS in different environments.</p>
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<p>The TDOS of the system after gas adsorption by CuO-SnS: (<b>a1</b>) NO<sub>2</sub> system, (<b>a2</b>) NO system, (<b>a3</b>) CO<sub>2</sub> system, (<b>a4</b>) CO system, (<b>a5</b>) SO<sub>2</sub> system, (<b>a6</b>) O<sub>2</sub> system. The DCD of the system after gas adsorption by CuO-SnS: (<b>b1</b>) NO<sub>2</sub> system, (<b>b2</b>) NO system, (<b>b3</b>) CO<sub>2</sub> system, (<b>b4</b>) CO system, (<b>b5</b>) SO<sub>2</sub> system, (<b>b6</b>) O<sub>2</sub> system.</p>
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<p>The PTDOS of the system after gas adsorption by CuO-SnS: (<b>a</b>) NO<sub>2</sub> system, (<b>b</b>) NO system, (<b>c</b>) CO<sub>2</sub> system, (<b>d</b>) CO system, (<b>e</b>) SO<sub>2</sub> system, (<b>f</b>) O<sub>2</sub> system.</p>
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<p>The ELF of the system after gas adsorption: (<b>a1</b>) NO<sub>2</sub>, (<b>a2</b>) NO, (<b>a3</b>) CO<sub>2</sub>, (<b>a4</b>) CO, (<b>a5</b>) SO<sub>2</sub>, and (<b>a6</b>) O<sub>2</sub> adsorbed on pure SnS; (<b>b1</b>) NO<sub>2</sub>, (<b>b2</b>) NO, (<b>b3</b>) CO<sub>2</sub>, (<b>b4</b>) CO, (<b>b5</b>) SO<sub>2</sub>, and (<b>b6</b>) O<sub>2</sub> adsorbed on CuO-SnS.</p>
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<p>Band gap evolution and conductivity changes of pure SnS and CuO-SnS system before and after gas adsorption.</p>
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<p>Recovery times of various adsorption systems on the CuO-SnS substrate.</p>
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10 pages, 807 KiB  
Article
The Feasibility and Validity of Home Spirometry for People with Cystic Fibrosis: Is It Comparable to Spirometry in the Clinic?
by Athina Sopiadou, Maria Gioulvanidou, Christos Kogias, Elissavet-Anna Chrysochoou, Ioustini Kalaitzopoulou and Elpis Hatziagorou
Children 2025, 12(3), 277; https://doi.org/10.3390/children12030277 - 25 Feb 2025
Viewed by 209
Abstract
Background/Objectives: Home spirometry allows people with cystic fibrosis (CF) to monitor their lung function from home. However, there are concerns about its feasibility and validity compared to traditional clinic spirometry. The aim of this study was to evaluate the feasibility and validity [...] Read more.
Background/Objectives: Home spirometry allows people with cystic fibrosis (CF) to monitor their lung function from home. However, there are concerns about its feasibility and validity compared to traditional clinic spirometry. The aim of this study was to evaluate the feasibility and validity of telehealth spirometry for patients with CF living in a regional setting. Methods: This retrospective study included forty-eight people with cystic fibrosis (pwCF) aged 6–33 years. Participants performed home spirometry using a portable flow sensor spirometer over a one-year period, without supervision. Spirometry readings from portable spirometers were compared with the nearest in-clinic spirometry using the intra-correlation coefficient (ICC) and Bland–Altman plots. Data were collected over a period of one year, with regular intervals of measurements. Results: In 427 of the 877 (48.6%) attempted sessions, successful spirometry at home was recorded. Although we showed good reliability between at-home and in-clinic measurements using the Bland–Altman plots and intraclass correlation co-efficient (ICC) (values ranged from 0.76 to 0.88), analysis of the 117 pairs of at-home and in-clinic spirometries showed that mean differences of forced expiratory volume in the 1st sec (FEV1) and forced vital capacity (FVC) obtained at home (both in liter and z-score) had, on average, lower values than the corresponding values at the clinic. Conclusions: Home-based telehealth spirometry is feasible among pwCF and provides advantages, especially for those from remote or secluded areas. However, lower values in FVC and FEV1 obtained through home spirometry should not be used interchangeably with clinic values. Full article
(This article belongs to the Special Issue Lung Diseases in Children: From Rarer to Commonest: 2nd Edition)
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<p>BlandAltman plot of differences in FVC (lt and z-score), FEV<sub>1</sub> (lt/s and z-score), and FEF<sub>25-75</sub> (lt/s and z-score) between at-home and in-clinic measurements (red line represents the mean difference and green lines represent the 95% limits of agreement).</p>
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32 pages, 7517 KiB  
Review
Electrochemical Performance of ZnCo2O4: Versatility in Applications
by Soyama Sitole, Mawethu Pascoe Bilibana and Natasha Ross
J. Compos. Sci. 2025, 9(3), 105; https://doi.org/10.3390/jcs9030105 - 25 Feb 2025
Viewed by 244
Abstract
Zinc cobaltite (ZnCo2O4) is a ternary metal oxide found in spinel with promising properties for various applications. Optimizing its catalytic activity requires an understanding of its electrochemical behavior. The electrochemical properties of ZnCo2O4 have significantly improved [...] Read more.
Zinc cobaltite (ZnCo2O4) is a ternary metal oxide found in spinel with promising properties for various applications. Optimizing its catalytic activity requires an understanding of its electrochemical behavior. The electrochemical properties of ZnCo2O4 have significantly improved due to recent developments in nanostructuring, doping, surface modification, hybridization, structural engineering, and electrochemical activation. These improvements have inspired and motivated researchers by presenting the latest developments in the field. The spinel structure, coupled with the redox properties of cobalt ions, semiconducting characteristics, and electrocatalytic potential, positions ZnCo2O4 as a versatile material for several electrochemical energy storage and conversion systems. This review explores these advancements; the notable properties of ZnCo2O4; and its applications in sensors, batteries, photovoltaics, and supercapacitors. Full article
(This article belongs to the Section Composites Applications)
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<p>(<b>a</b>) The cubic spinel and (<b>b</b>) tetragonal spinel structures of ZnCo<sub>2</sub>O<sub>4</sub>. Gray, blue, and red balls represent Zn, Co, and O atoms. [Reprinted with permission from Ref. [<a href="#B9-jcs-09-00105" class="html-bibr">9</a>] Copyright 2016. <span class="html-italic">Scientific Reports</span>].</p>
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<p>Applications of ZnCo<sub>2</sub>O<sub>4</sub> material.</p>
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<p>(<b>a</b>) Schematic illustration of the synthesis of ZnCo<sub>2</sub>O<sub>4</sub>. (<b>b</b>) Setup of the experiment to measure the gas sensitivity of ZnCo<sub>2</sub>O<sub>4</sub> nanoparticles. [Reproduced with permission from Ref. [<a href="#B19-jcs-09-00105" class="html-bibr">19</a>]. Copyright 2016, <span class="html-italic">Sensors</span>].</p>
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<p>The sensitivity of LaCoO<sub>3</sub> pellets versus operating temperature, CO concentration, and propane concentration. [Reproduced with permission from Ref. [<a href="#B32-jcs-09-00105" class="html-bibr">32</a>]. 2014, <span class="html-italic">Journal of Nanomaterials</span>].</p>
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<p>(<b>a</b>) Dynamic electrical resistance of the ZnCo<sub>2</sub>O<sub>4</sub> sample after exposure to 560 ppb of O<sub>3</sub> at 200 °C for different durations. (<b>b</b>) Sensor response of the ZnCo<sub>2</sub>O<sub>4</sub> sample at various operating temperatures after exposure to 560 ppb of O<sub>3</sub>. (<b>c</b>) Response of ozone concentration and recovery time ranging from 80 to 890 ppb at 200 °C. [Reproduced with permission from reference [<a href="#B37-jcs-09-00105" class="html-bibr">37</a>]. Copyright 2018, <span class="html-italic">Sensors and Actuators</span>].</p>
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<p>(<b>A</b>) Schematic representation of the ZnCo<sub>2</sub>O<sub>4</sub>/AuNPs hybrid material synthesis. (<b>B</b>) Schematic diagram of the GCE/ZCOA platform’s target-driven cascade TMSDR double-amplification ECL sensor for DNA detection. [Reproduced with permission from Ref. [<a href="#B38-jcs-09-00105" class="html-bibr">38</a>]. Copyright 2020. Elsevier].</p>
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<p>CV curves for (<b>a</b>) NZ− 0.5, (<b>b</b>) NZ−1, and (<b>c</b>) NZ−2 at various scan rates, as well as the corresponding GCD curves (<b>a′</b>–<b>c′</b>) and specific capacitance graphs (<b>a″</b>–<b>c″</b>) at different current densities. The corresponding Nyquist and Ragone plots, measured at different current densities, are displayed in the insets. [Reproduced with permission from [<a href="#B44-jcs-09-00105" class="html-bibr">44</a>]. Copyright 2022, <span class="html-italic">Nanoscale Advances</span>].</p>
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<p>(<b>a</b>) Cycling performances of the ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>, ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>−S, and ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>−B electrodes at 0.2 A·g<sup>−1</sup>. (<b>b</b>) Rate capability of the ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>, ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>−S, and ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>-B electrodes at 0.2, 0.4, 0.6, 0.8, 1, and 2 A·g<sup>−1</sup>. (<b>c</b>) Capacity retention of the ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>, ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>−S, and ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>−B electrodes at 0.2 A·g<sup>−1</sup> in different cycles (1st, 2nd, 100th, 300th, and 500th). (<b>d</b>) Charge and discharge profiles of the ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>-B electrode for the different cycles (1st, 2nd, 100th, 300th, and 500th). (<b>e</b>) Long-term cycling performance of the ZnCo<sub>2</sub>O<sub>4</sub>@C<sub>3</sub>N<sub>4</sub>−B electrode at 0.5 and 2 A·g<sup>−1</sup>. [Reproduced with permission from [<a href="#B70-jcs-09-00105" class="html-bibr">70</a>]. Copyright 2020, <span class="html-italic">RSC Advances</span>].</p>
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<p>Electrochemical performance of ZnCo<sub>2</sub>O<sub>4</sub>/C microhydrangeas: (<b>A</b>) Typical discharge–charge profiles. (<b>B</b>) The corresponding differential capacity curves from 0.01 to 3.0 V at 1 A·g<sup>−1</sup>. (<b>C</b>) Cyclic performance at 1 A·g<sup>−1</sup>. (<b>D</b>) Impedance studies. (<b>E</b>) Randles plots in the seconds and 200th cycle. [Reproduced with permission from Ref [<a href="#B74-jcs-09-00105" class="html-bibr">74</a>]. Copyright 2019, Wiley].</p>
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<p>(<b>a</b>,<b>b</b>) SEM images. (<b>c</b>,<b>d</b>) TEM images of ZnCo<sub>2</sub>O<sub>4</sub>@CNT. [Reprinted with permission from Ref [<a href="#B77-jcs-09-00105" class="html-bibr">77</a>]. Copyright 2015, American Chemical Society].</p>
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<p>(<b>a</b>) Device structure and (<b>b</b>) cross-sectional SEM image of the PSC based on the ZnCo<sub>2</sub>O<sub>4</sub> NPs layer, (<b>c</b>) energy level diagram of the whole device, (<b>d</b>) J-V characteristics, (<b>e</b>) normalized PCE evolution, and (<b>f</b>) EQE spectra and integrated current density of the PSCs based on PEDOT:PSS film or ZnCo<sub>2</sub>O<sub>4</sub> NPs. [Reprinted with permission from [<a href="#B91-jcs-09-00105" class="html-bibr">91</a>]. Copyright 2022, PMC].</p>
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<p>PCE for DSSCs equipped with Pt, ZnCo<sub>2</sub>O<sub>4</sub>/RGO, ZnCo<sub>2</sub>O<sub>4</sub>, and RGO CEs. [Reprinted with permission from Ref. [<a href="#B94-jcs-09-00105" class="html-bibr">94</a>]. Copyright 2018, Elsevier].</p>
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<p>The simulated configuration of the device. (<b>a</b>) The schematic configuration of the device. (<b>b</b>) The energy level diagram of the whole device. [Reproduced with permission from Ref. [<a href="#B100-jcs-09-00105" class="html-bibr">100</a>]. Copyright 2024, <span class="html-italic">Journal of Physics</span>].</p>
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15 pages, 2878 KiB  
Article
Preparation of Ion Composite Photosensitive Resin and Its Application in 3D-Printing Highly Sensitive Pressure Sensor
by Tong Guan, Huayang Li, Jinyun Liu, Wuxu Zhang, Siying Wang, Wentao Ye, Baoru Bian, Xiaohui Yi, Yuanzhao Wu, Yiwei Liu, Juan Du, Jie Shang and Run-Wei Li
Sensors 2025, 25(5), 1348; https://doi.org/10.3390/s25051348 - 22 Feb 2025
Viewed by 293
Abstract
Flexible pressure sensors play an extremely important role in the fields of intelligent medical treatment, humanoid robots, and so on. However, the low sensitivity and the small initial capacitance still limit its application and development. At present, the method of constructing the microstructure [...] Read more.
Flexible pressure sensors play an extremely important role in the fields of intelligent medical treatment, humanoid robots, and so on. However, the low sensitivity and the small initial capacitance still limit its application and development. At present, the method of constructing the microstructure of the dielectric layer is commonly used to improve the sensitivity of the sensor, but there are some problems, such as the complex process and inaccurate control of the microstructure. In this work, an ion composite photosensitive resin based on polyurethane acrylate and ionic liquids (ILs) was prepared. The high compatibility of the photosensitive resin and ILs was achieved by adding a chitooligosaccharide (COS) chain extender. The microstructure of the dielectric layer was optimized by digital light processing (DLP) 3D-printing. Due to the introduction of ILs to construct an electric double layer (EDL), the flexible pressure sensor exhibits a high sensitivity of 32.62 kPa−1, which is 12.2 times higher than that without ILs. It also has a wide range of 100 kPa and a fast response time of 51 ms. It has a good pressure response under different pressures and can realize the demonstration application of human health. Full article
(This article belongs to the Special Issue Wearable Sensors for Continuous Health Monitoring and Analysis)
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<p>Curing principle of ion composite photosensitive resin: (<b>a</b>) chemical structure of PUA, COS, PEG(600)DMA, and [EMIM][TFSI]; and (<b>b</b>) the schematic diagram of UV curing and heat curing.</p>
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<p>(<b>a</b>) Preparation process of dielectric layer; (<b>b</b>,<b>c</b>) SEM and EDX on the surface of ion composite photosensitive resin without COS; (<b>d</b>,<b>e</b>) the cross-section SEM and EDX of ion composite photosensitive resin without COS; (<b>f</b>,<b>g</b>) SEM and EDX on the surface of ion composite photosensitive resin with COS; (<b>h</b>,<b>i</b>) the cross section SEM and EDX of ion composite photosensitive resin with COS; and (<b>j</b>) image of different structures by DLP 3D printing.</p>
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<p>Mechanical and electrical properties of ion composite photosensitive resin: (<b>a</b>–<b>c</b>) the mechanical properties changed with the content of COS, PEG(600)DMA, and ILs; (<b>d</b>) the comparison of the tensile loading–unloading curves of the ion composite photosensitive resin containing 40 wt.% ILs (PUA@ILs) and other commercial flexible photosensitive resins; and (<b>e</b>,<b>f</b>) distribution of sample conductivity before and after compression.</p>
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<p>3D printing of ion composite photosensitive resin: (<b>a</b>) relationship between viscosity of photosensitive resin and content of [EMIM][TFSI]; (<b>b</b>) the relationship between curing depth and exposure energy; (<b>c</b>) horizontal resolution of ion composite photosensitive resin; and (<b>d</b>) image of TYPE-C structure printed by ion composite photosensitive resin.</p>
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<p>Sensing performance of the 3D-printed capacitive sensor based on ion composite photosensitive resin: (<b>a</b>) sensor structure diagram; (<b>b</b>) the ΔC/C<sub>0</sub>–P relation of sensors with dielectric layers of different lattice structures; (<b>c</b>) the ΔC/C<sub>0</sub>–P relation of sensors with TYPE-C dielectric layers of different density ratios; (<b>d</b>) the ΔC/C<sub>0</sub>–P relation of TYPE-C structure with 25% density ratio; (<b>e</b>) the sensitivity of sensors with different dielectric layer materials; and (<b>f</b>) comparison of sensitivity and range (sensitivity &gt; 0.1 kPa<sup>−1</sup>) of different capacitive sensors based on photosensitive resin [<a href="#B32-sensors-25-01348" class="html-bibr">32</a>,<a href="#B37-sensors-25-01348" class="html-bibr">37</a>,<a href="#B38-sensors-25-01348" class="html-bibr">38</a>,<a href="#B39-sensors-25-01348" class="html-bibr">39</a>,<a href="#B47-sensors-25-01348" class="html-bibr">47</a>,<a href="#B48-sensors-25-01348" class="html-bibr">48</a>].</p>
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<p>Other sensing performance and application demonstrations of the 3D-printed capacitive sensor based on ion composite photosensitive resin: (<b>a</b>) response time of the sensor at approximately 3 kPa; (<b>b</b>) response of the sensor to a gradually increasing force of 20 kPa; (<b>c</b>) the cyclic response of the sensor under different pressures (1 kPa, 10 kPa, 20 kPa, 50 kPa, and 100 kPa); (<b>d</b>) response of the sensor under 1000 cycles; (<b>e</b>) real-time monitoring of human pulse; and (<b>f</b>) real-time monitoring of deep breath, swallow, and cough in the human throat.</p>
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23 pages, 929 KiB  
Article
Optimal Algorithms for Improving Pressure-Sensitive Mat Centre of Pressure Measurements
by Alexander Dawid Bincalar, Chris Freeman and m.c. schraefel
Sensors 2025, 25(5), 1283; https://doi.org/10.3390/s25051283 - 20 Feb 2025
Viewed by 260
Abstract
The accurate measurement of human balance is required in numerous analysis and training applications. Force plates are frequently used but are too costly to be suitable for home-based systems such as balance training. A growing body of research and commercial products use Pressure-Sensitive [...] Read more.
The accurate measurement of human balance is required in numerous analysis and training applications. Force plates are frequently used but are too costly to be suitable for home-based systems such as balance training. A growing body of research and commercial products use Pressure-Sensitive Mats (PSMs) for balance measurement. Low-cost PSMs are constructed with a piezoresistive material and use copper tracks as conductors. However, these lack accuracy, as they often have a low resolution and suffer from noise, non-repeatable effects, and crosstalk. This paper proposes novel algorithms that enable the Centre of Pressure (CoP) to be computed using low-cost PSM designs with significantly higher accuracy than is currently achievable. A mathematical model of a general low-cost PSM was developed and used to select the design of the PSM (track width and placement) that maximises CoP accuracy. These yield new optimal PSM geometries that decrease the mean absolute CoP error from 17.37% to 5.47% for an 8 × 8 sensor layout. Then, knowledge of the footprint was used to further optimise accuracy, showing a decrease in absolute error from 17.37% to 3.93% for an 8 × 8 sensor layout. A third algorithm was derived using models of human movement to further reduce measurement error. Full article
(This article belongs to the Special Issue Human Performance Sensing and Human-Structure Interactions)
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<p>(<b>a</b>) A pressure profile of feet with Centre of Pressure <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>x</mi> <mi>A</mi> </msub> <mo>,</mo> <msub> <mi>y</mi> <mi>A</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math>. (<b>b</b>) The pressure profile, split into segments across the x-axis. (<b>c</b>) The pressure profile, split into segments across the y-axis.</p>
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<p>A diagram of a PSM and its associated hardware. Constitutive layers are shown on the left. The circuitry is shown on the right.</p>
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<p>Pressure mat geometry with variable copper strip thickness and spacing in vertical and horizontal directions.</p>
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<p>Geometry of an individual Velostat sensor, <math display="inline"><semantics> <mrow> <mi>i</mi> <mo>,</mo> <mi>j</mi> </mrow> </semantics></math>, at position <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>x</mi> <mi>j</mi> </msub> <mo>,</mo> <msub> <mi>y</mi> <mi>i</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math>, experiencing a non-uniform pressure profile. The overall resistance is computed by dividing the area into regions and applying the parallel resistor relation.</p>
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<p>Diagram showing the movement of weight and CoP during the side weight shift scenario.</p>
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<p>Diagram showing the movement of weight and CoP during the front weight shift scenario.</p>
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<p>Diagram showing the movement of weight and CoP during the foot slide scenario.</p>
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<p>Figures showing the track geometries used in the simulations, where (<b>a</b>) is the default standard uniform track layout, while (<b>b</b>) is a track layout generated using our algorithm in <a href="#sec5dot2-sensors-25-01283" class="html-sec">Section 5.2</a>.</p>
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<p>A graphical representation of the results in <a href="#sensors-25-01283-t001" class="html-table">Table 1</a>.</p>
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