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Search Results (2,635)

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15 pages, 2114 KiB  
Article
Laser-Induced Graphene Electrodes for Flexible pH Sensors
by Giulia Massaglia, Giacomo Spisni, Tommaso Serra and Marzia Quaglio
Nanomaterials 2024, 14(24), 2008; https://doi.org/10.3390/nano14242008 (registering DOI) - 14 Dec 2024
Viewed by 182
Abstract
In the growing field of personalized medicine, non-invasive wearable devices and sensors are valuable diagnostic tools for the real-time monitoring of physiological and biokinetic signals. Among all the possible multiple (bio)-entities, pH is important in defining health-related biological information, since its variations or [...] Read more.
In the growing field of personalized medicine, non-invasive wearable devices and sensors are valuable diagnostic tools for the real-time monitoring of physiological and biokinetic signals. Among all the possible multiple (bio)-entities, pH is important in defining health-related biological information, since its variations or alterations can be considered the cause or the effect of disease and disfunction within a biological system. In this work, an innovative (bio)-electrochemical flexible pH sensor was proposed by realizing three electrodes (working, reference, and counter) directly on a polyimide (Kapton) sheet through the implementation of CO2 laser writing, which locally converts the polymeric sheet into a laser-induced graphene material (LIG electrodes), preserving inherent mechanical flexibility of Kapton. A uniform distribution of nanostructured PEDOT:PSS was deposited via ultrasonic spray coating onto an LIG working electrode as the active material for pH sensing. With a pH-sensitive PEDOT coating, this flexible sensor showed good sensitivity defined through a linear Nernstian slope of (75.6 ± 9.1) mV/pH, across a pH range from 1 to 7. We demonstrated the capability to use this flexible pH sensor during dynamic experiments, and thus concluded that this device was suitable to guarantee an immediate response and good repeatability by measuring the same OCP values in correspondence with the same pH applied. Full article
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Figure 1
<p>The schematic representation of the process workflows proposed: in (<b>a</b>), the workflow referring to the realization of the LIG-PEDOT pH sensor is sketched, while in (<b>b</b>), the one followed for fabricating the commercial-PEDOT pH sensor is represented.</p>
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<p>(<b>a</b>) Morphological properties of LIG electrodes realized on Kapton sheet by implementing CO<sub>2</sub> laser writing; (<b>b</b>) morphological features of 200 μg/cm<sup>2</sup> of PEDOT onto LIG electrode.</p>
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<p>Raman spectrum of PEDOT:PSS nanostructured layer deposited onto LIG electrodes by implementing USC process. It is possible to underline the prevalence of the benzoid group (purple line) over the quinoid one (green line).</p>
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<p>(<b>a</b>) Equivalent circuit used to determine electrochemical parameters; (<b>b</b>) double-layer capacitance and charge transfer resistance variation of the electrochemical sensor with pH values.</p>
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<p>OCP measurements conducted at different pH values, defined in the range from 1 to 7, mimicking the acidic environment. Experimental data for LIG-PEDOT pH sensors (pink dot) were compared with those for commercial-PEDOT (red dot), highlighting a linear pH response (pink line for LIG-PEDOT pH sensor and red line for commercial PEDOT, respectively).</p>
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<p>OCP measurements conducted at different pH values in a dynamic way. LIG-PEDOT pH sensors were immersed in the electrolyte solution, and pH values were continuously modified by adding NaOH and HCl to move from a basic environment to a strong acidic one.</p>
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28 pages, 1492 KiB  
Article
Design and Implementation of a Decision Integration System for Monitoring and Optimizing Heating Systems: Results and Lessons Learned
by Kirill Djebko, Daniel Weidner, Marcel Waleska, Timo Krey, Bhaskar Kamble, Sven Rausch, Dietmar Seipel and Frank Puppe
Energies 2024, 17(24), 6290; https://doi.org/10.3390/en17246290 - 13 Dec 2024
Viewed by 300
Abstract
With the increasing need to tackle climate change, energy efficiency and reduced CO2 emissions are proving to be one of society’s greatest challenges. Special consideration should be given to heating systems as they are prone to inefficiency due to non-optimal controller configurations [...] Read more.
With the increasing need to tackle climate change, energy efficiency and reduced CO2 emissions are proving to be one of society’s greatest challenges. Special consideration should be given to heating systems as they are prone to inefficiency due to non-optimal controller configurations and the shortage of experts or qualified technicians to optimize the operating behavior. Especially for residential heating systems, more often than not, the target metric is the achievement of specific heating and hot water temperatures by manual adjustments with limited sensor information and with little regard to efficiency. This presents potential for computer-aided optimization based on artificial intelligence techniques. In this paper, we presented a Decision Integration System that is interfaced with a data acquisition infrastructure and allows for the analysis of measured heating system data, the generation of recommended measures for efficiency improvement, and the simulative validation of recommended controller parameter changes. We presented different parts of the Decision Integration System, the interfaced data acquisition infrastructure, as well as the non-invasive sensor appliances used. We analyzed the measured data of real heating systems and evaluated our approach by generating the recommended measures based on rules created by heating system experts, which were then partially applied to the physical heating systems and partially evaluated in simulation. Finally, we compared long-term energy consumption data against the latest monitoring period after implementing the measures. Our results showed an average reduction in energy consumption of 24.52% across all considered buildings, corresponding to an approximate reduction of 8.12 tons of CO2 emissions. Full article
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<p>Architecture of the complete system, including the time series data analysis and classification module (Daedalus), the interfaced data platform (ESS) for visualization, the Decision Support System (DSS) for generating recommendations, the Simulation System (SIM) for the qualitative verification of controller parameter recommendations, and the analytics API for the evaluation of the savings.</p>
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<p>Example display of a boiler output power time series (one hour) indicating boiler state fluctuation (SD: <math display="inline"><semantics> <mrow> <mi>b</mi> <mi>o</mi> <mi>i</mi> <mi>l</mi> <mi>e</mi> <mi>r</mi> <mi>S</mi> <mi>t</mi> <mi>a</mi> <mi>t</mi> <mi>e</mi> <mi>F</mi> <mi>l</mi> <mi>u</mi> <mi>c</mi> <mi>t</mi> <mi>u</mi> <mi>a</mi> <mi>n</mi> <mi>t</mi> </mrow> </semantics></math>). All minima and maxima are calculated and counted if they exceed the boiler’s minimum power output. More than six power cycles per hour are considered faulty behavior.</p>
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<p>Flowchart of the process of generating (verified) measures showing the interactions between the submodules during the different stages.</p>
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<p>Amount (n) and distribution of all 125 system components and subtypes. Three subtypes were defined for potable water heating: the Buffer Charging System (BCS), which is the most commonly used, the Heating Coil System (HCS), and the Fresh Water Station (FWS), also called the DHW (Domestic Hot Water) system.</p>
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<p>Monthly consumption per square meter for building “WFe21-25”. Climate correction factors were applied. Consumption data for the years 2022 and 2023 was not available.</p>
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<p>Schematic overview of the heating system of <span class="html-italic">Model 1</span> as taken from [<a href="#B25-energies-17-06290" class="html-bibr">25</a>] augmented with further details. The full black circle indicates the start, while the other black circles indicate the end of the energy flow. The blue line entering the boiler stands for the energy input in the form of natural gas and the blue line exiting the heating circuit stands for the heat generated by the heating circuit. The thick black lines represent the water flow from the heat producer to the heat consumers (flow), the thin black lines stand for the water flow from the heat consumers back to the heat producer (return), and the dotted lines stand for control signals. The colored circles illustrate the available sensors, and the colored squares indicate virtual sensors, which correspond to simulated values for which internally (sensor) values exist but are not part of the output data. The rhombus indicates values that are derived from measured values during preprocessing and are treated like external measured input during simulation (excluding the outside temperature due to readability reasons). The coloring indicates the type of sensor and is green for temperatures (°C), orange for volume flows (m³/h), blue for power (W), yellow for gas (m³), and gray for various states, e.g., on-off.</p>
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<p>Schematic overview of the heating system of <span class="html-italic">Model 2</span>. For a description of the used symbols please refer to the caption of <a href="#energies-17-06290-f006" class="html-fig">Figure 6</a>.</p>
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<p>Amount (n; percentages rounded to one decimal place) and distribution of 495 proposed measures per type.</p>
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17 pages, 4525 KiB  
Article
Highly Sensitive and Selective SnO2-Gr Sensor Photoactivated for Detection of Low NO2 Concentrations at Room Temperature
by Isabel Sayago, Carlos Sánchez-Vicente and José Pedro Santos
Nanomaterials 2024, 14(24), 1994; https://doi.org/10.3390/nano14241994 - 12 Dec 2024
Viewed by 301
Abstract
Chemical nanosensors based on nanoparticles of tin dioxide and graphene-decorated tin dioxide were developed and characterized to detect low NO2 concentrations. Sensitive layers were prepared by the drop casting method. SEM/EDX analyses have been used to investigate the surface morphology and the [...] Read more.
Chemical nanosensors based on nanoparticles of tin dioxide and graphene-decorated tin dioxide were developed and characterized to detect low NO2 concentrations. Sensitive layers were prepared by the drop casting method. SEM/EDX analyses have been used to investigate the surface morphology and the elemental composition of the sensors. Photoactivation of the sensors allowed for detecting ultra-low NO2 concentrations (100 ppb) at room temperature. The sensors showed very good sensitivity and selectivity to NO2 with low cross-responses to the other pollutant gases tested (CO and CH4). The effect of humidity and the presence of graphene on sensor response were studied. Comparative studies revealed that graphene incorporation improved sensor performance. Detections in complex atmosphere (CO + NO2 or CH4 + NO2, in humid air) confirmed the high selectivity of the graphene sensor in near-real conditions. Thus, the responses were of 600%, 657% and 540% to NO2 (0.5 ppm), NO2 (0.5 ppm) + CO (5 ppm) and NO2 (0.5 ppm) + CH4 (10 ppm), respectively. In addition, the detection mechanisms were discussed and the possible redox equations that can change the sensor conductance were also considered. Full article
(This article belongs to the Special Issue Advanced Nanomaterials in Gas and Humidity Sensors)
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Graphical abstract

Graphical abstract
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<p>(<b>a</b>) SEM micrographs and (<b>b</b>) EDX elemental mapping images of one sensitive layer (SnO<sub>2</sub>-Gr).</p>
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<p>TEM images of (<b>a</b>) Gr-SnO<sub>2</sub> on grids (<b>b</b>) pristine SnO<sub>2</sub> nanoparticles, (<b>c</b>) Gr-SnO<sub>2</sub> and (<b>d</b>) HRTEM images of Gr-SnO<sub>2</sub>.</p>
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<p>Resistance changes in the SnO<sub>2</sub>-NPs sensor tested with and without UV-LED illumination at RT in air.</p>
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<p>SnO<sub>2</sub> sensor: (<b>a</b>) Dynamic response to NO<sub>2</sub> at RT in air atmosphere with and without UV-LED illumination and (<b>b</b>) responses to 0.5 ppm NO<sub>2</sub> under different conditions (with and without UV-LED, dry and humid air).</p>
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<p>Dynamic response curves at RT under UV-LED illumination to NO<sub>2</sub> different concentrations of the tested sensors: (<b>a</b>) SnO<sub>2</sub> and (<b>b</b>) SnO<sub>2</sub>-Gr. (<b>c</b>) Response of the SnO<sub>2</sub> and SnO<sub>2</sub>-Gr sensors to 0.1, 0.3 and 0.5 ppm NO<sub>2</sub> at RT under UV-LED illumination in dry and humid air (50% RH). (<b>d</b>) Sensor responses versus NO<sub>2</sub> gas concentration in dry and humid air (50% RH) with UV-LED illumination, where the circles denote experimental results and the dotted lines represent fitting curves.</p>
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<p>(<b>a</b>) Responses of the sensors to 0.3 ppm NO<sub>2</sub>, 5 ppm CO and 5 ppm CH<sub>4</sub> in dry and wet air. (<b>b</b>) Selectivity of the tested sensors to NO<sub>2</sub> at RT and under UV-LED illumination, in dry and humid air (50%). SnO<sub>2</sub>-Gr sensor dynamic response at RT in humid air (45% RH) and under UV-LED illumination to different gas mixtures: (<b>c</b>) mixture 1 (NO<sub>2</sub> + CO) (<b>d</b>) mixture 2 (NO<sub>2</sub> + CH<sub>4</sub>).</p>
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<p>Detection mechanism scheme.</p>
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10 pages, 2830 KiB  
Article
High-Stretchable and Transparent Ultraviolet-Curable Elastomer
by Lei Chen, Yongchang He, Lu Dai, Wang Zhang, Hao Wang and Peng Liu
Polymers 2024, 16(24), 3464; https://doi.org/10.3390/polym16243464 - 11 Dec 2024
Viewed by 292
Abstract
This work introduces an ultraviolet (UV)-curable elastomer through the co-polymerization of aliphatic polyurethane acrylate and hydroxypropyl acrylate via UV irradiation. The UV-curable elastomer presents superior mechanical properties (elongation at a break of 2992%) and high transparency (94.8% at 550 nm in the visible [...] Read more.
This work introduces an ultraviolet (UV)-curable elastomer through the co-polymerization of aliphatic polyurethane acrylate and hydroxypropyl acrylate via UV irradiation. The UV-curable elastomer presents superior mechanical properties (elongation at a break of 2992%) and high transparency (94.8% at 550 nm in the visible light region). A robust hydrogel–elastomer stretchable sensor is fabricated by coating an ionic hydrogel on the surface of an elastomer, which enables real-time monitoring of human motion. In addition, the UV-curable elastomer can be used for 3D printing, as demonstrated by complex lattice structures using a digital light processing 3D printer. Full article
(This article belongs to the Special Issue 3D Printing of Polymer Composites)
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<p>Preparation of UV-curable elastomer. (<b>a</b>) Schematic of elastomer formed by covalent cross-linking of oligomer and monomer. (<b>b</b>) The chemical structures of PUA, HPA, PEGDA, and TPO-L. HPA may have multiple isomers, one of the formulas is shown here.</p>
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<p>Transparency of UV-curable elastomer. The transmittance spectrum of the as-fabricated UVE-A3 elastomer in the visible light region.</p>
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<p>Mechanical properties of elastomer. (<b>a</b>) Snapshots of stretching a transparent elastomer specimen by about 30 times. (<b>i</b>) The original length is defined as λ. Stretching times: (<b>ii</b>) 18 times, (<b>iii</b>) 27 times, (<b>iv</b>) 30 times. (<b>b</b>) Stress–strain curves of as-fabricated elastomer with different weight ratios of PUA and HPA. (<b>c</b>) The obtained elongation at break and tensile stress from (<b>b</b>). (<b>d</b>) Stress–strain curves of as-fabricated elastomer with different PEGDA cross-linkers. (<b>e</b>) The obtained elongation at break from (<b>d</b>).</p>
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<p>Fabrication of hydrogel–elastomer stretchable sensor. (<b>a</b>) The combination of elastomer and ionic conductive hydrogel. (<b>b</b>) The sensor under large deformation (e.g., stretch) without debonding. (<b>c</b>) The LED bulb in the circuit with the sensor. (<b>i</b>–<b>iv</b>) The LED brightness decreases with increased sensor stretching.</p>
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<p>The performance of the hydrogel–elastomer stretchable sensor. (<b>a</b>) The relationship between ΔR/R<sub>0</sub> and the strain of the sensor. (<b>b</b>) The resistance response of the sensor to increasing tensile strains. (<b>c</b>) The relative resistance changes in the sensor attached to the finger upon different bending angles and (<b>d</b>) upon different bending speeds. (<b>e</b>) The response and recovery time of the sensor. (<b>f</b>–<b>i</b>) The relative resistance changes in the sensor for human body movements, such as wrist bending, knee bending, and swallowing.</p>
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<p>Application of the elastomer for DLP 3D printing. (<b>a</b>–<b>c</b>) 3D-printed structures can withstand compression and recover to the original shape.</p>
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21 pages, 12534 KiB  
Article
Sustainable Lighting Systems Implementation Methodology Aligned with SDGs and International Standards: A Case Study in a Mexican Technological Institute
by Jorge Alberto Cárdenas Magaña, Marco Antonio Celis Crisóstomo, Juan M. González López, Sergio Sandoval Pérez, Daniel A. Verde Romero, Francisco Miguel Hernández López, Efrain Villalvazo Laureano, Emmanuel Vega Negrete, Jaime Jalomo Cuevas, Ramón Chávez Bracamontes and Paulina Barragán Sánchez
Sustainability 2024, 16(24), 10831; https://doi.org/10.3390/su162410831 - 11 Dec 2024
Viewed by 461
Abstract
This paper presents a comprehensive holistic methodology implemented for sustainable lighting systems in educational institutions. The proposed methodology is aligned with the Sustainable Development Goals (SDGs), particularly with SDG 7 (Affordable and Clean Energy) and SDG 13 (Climate Action), and it follows international [...] Read more.
This paper presents a comprehensive holistic methodology implemented for sustainable lighting systems in educational institutions. The proposed methodology is aligned with the Sustainable Development Goals (SDGs), particularly with SDG 7 (Affordable and Clean Energy) and SDG 13 (Climate Action), and it follows international standards. The six-step process includes viability analysis, project design simulation using DIALux 4.13 software, the installation of LED lighting systems, and the redesign of some electrical circuits, followed by an analysis of return on investment and the monitorization of CO2 and energy consumption. The proposed methodology results in significant return on investment (ROI), primarily achieved through energy savings and reduced maintenance costs. The implementation of LED tubes, combined with occupancy and natural light sensors, leads to a 66% reduction in energy consumption and a reduction of 15.63 tons (metric tons) of CO2 annually, translating into a quick payback period of approximately 2.36 years. Additionally, the system includes Long-Term Monitoring, which ensures that energy consumption and lighting levels are continuously tracked. Full article
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<p>Aerial View, Building Facades, and 3D Interior Plan of Building 1 and Building 2 at the Technological Institute located in the city of Tamazula de Gordiano.</p>
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<p>Conceptual model for the implementation of sustainable lighting systems aligned with the SDGs and international standards.</p>
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<p>Holistic methodology proposal.</p>
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<p>Initial analysis of the current lighting level distribution, including measurements, and simulations using DiaLux 4.13 with T8 fluorescent tubes in Building 1.</p>
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<p>Lighting Isolux lines of a classroom in Building 1, created using DIALux 4.13 software.</p>
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<p>Lighting Isolux lines of a classroom in Building 1, created using DIALux 4.13 software.</p>
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<p>Distribution of luminaires under initial conditions and their electrical layout, created in Dialux.</p>
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<p>Proposed electrical circuit redistribution.</p>
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<p>Sensors implemented in different areas.</p>
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<p>Lighting Isolux lines in a classroom of Building 1.</p>
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<p>ROI and break-even point chart in years.</p>
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<p>Energy Measurements of Fluorescent tubes in 2023 versus two LEDs in 2024.</p>
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19 pages, 8894 KiB  
Article
The Effect of Doping rGO with Nanosized MnO2 on Its Gas Sensing Properties
by Mohamed Ayoub Alouani, Juan Casanova-Chafer, Santiago de Bernardi-Martín, Alejandra García-Gómez, Foad Salehnia, José Carlos Santos-Ceballos, Alejandro Santos-Betancourt, Xavier Vilanova and Eduard Llobet
Chemosensors 2024, 12(12), 256; https://doi.org/10.3390/chemosensors12120256 - 6 Dec 2024
Viewed by 470
Abstract
Manganese dioxide (MnO2) has drawn attention as a sensitiser to be incorporated in graphene-based chemoresistive sensors thanks to its promising properties. In this regard, a rGO@MnO2 sensing material was prepared and deposited on two different substrates (silicon and Kapton). The [...] Read more.
Manganese dioxide (MnO2) has drawn attention as a sensitiser to be incorporated in graphene-based chemoresistive sensors thanks to its promising properties. In this regard, a rGO@MnO2 sensing material was prepared and deposited on two different substrates (silicon and Kapton). The effect of the substrate nature on the morphology and sensing behaviour of the rGO@MnO2 material was thoroughly analysed and reported. These sensors were exposed to different dilutions of NO2 ranging from 200 ppb to 1000 ppb under dry and humid conditions (25% RH and 70% RH) at room temperature. rGO@MnO2 deposited on Kapton showed the highest response of 6.6% towards 1 ppm of NO2 under dry conditions at RT. Other gases or vapours such as NH3, CO, ethanol, H2 and benzene were also tested. FESEM, HRTEM, Raman, XRD and ATR-IR were used to characterise the prepared sensors. The experimental results showed that the incorporation of nanosized MnO2 in the rGO material enhanced its response towards NO2. Moreover, this material also showed very good responses toward NH3 both under dry and humid conditions, with the rGO@MnO2 sensor on silicon showing the highest response of 18.5% towards 50 ppm of NH3 under 50% RH at RT. Finally, the synthetised layers showed no cross-responsiveness towards other toxic gases. Full article
(This article belongs to the Special Issue Advanced Chemical Sensors for Gas Detection)
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<p>Pictures of the prepared sensors on the (<b>a</b>) silicon substrate and (<b>b</b>) Kapton substrate.</p>
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<p>Schematic representation of the gas detection process and used equipment.</p>
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<p>(<b>a</b>) Raman spectra of rGO and (<b>b</b>) Raman spectra of rGO@MnO<sub>2</sub>.</p>
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<p>FESEM images of (<b>a</b>) the surface of the graphene doped with MnO<sub>2</sub> deposited on the silicon substrate and (<b>b</b>) the surface of the graphene doped with MnO<sub>2</sub> deposited on the Kapton substrate.</p>
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<p>(<b>a</b>) HRTEM image of layered graphene doped with nanosized MnO<sub>2</sub>; (<b>b</b>) a zoomed HRTEM image of a scale of 50 nm of the same material; (<b>c</b>) EDS mapping showing Mn concentration on the area of analysis; (<b>d</b>) EDS map of O element in the mapped area; (<b>e</b>) EDS map of C element in the same mapped area; (<b>f</b>) overlay image of all the maps of the elements C (green), O (red) and Mn (blue); (<b>g</b>) EDS map spectrum of the studied area.</p>
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<p>(<b>a</b>) HRTEM image of layered graphene doped with nanosized MnO<sub>2</sub>; (<b>b</b>) a zoomed HRTEM image of a scale of 50 nm of the same material; (<b>c</b>) EDS mapping showing Mn concentration on the area of analysis; (<b>d</b>) EDS map of O element in the mapped area; (<b>e</b>) EDS map of C element in the same mapped area; (<b>f</b>) overlay image of all the maps of the elements C (green), O (red) and Mn (blue); (<b>g</b>) EDS map spectrum of the studied area.</p>
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<p>ATR-IR spectra of (<b>a</b>) rGO@MnO<sub>2</sub> on silicon substrate and (<b>b</b>) rGO@MnO<sub>2</sub> on Kapton substrate.</p>
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<p>(<b>a</b>) Calibration curve of the responses of the fabricated sensors towards different concentrations of NO<sub>2</sub> at room temperature and under dry conditions; (<b>b</b>) resistance changes of the rGO@MnO<sub>2</sub> on silicon substrate for 600 ppb of NO<sub>2</sub> at 25% RH; (<b>c</b>) resistance changes of the rGO@MnO<sub>2</sub> on Kapton substrate for 600 ppb of NO<sub>2</sub> at 25% RH.</p>
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<p>(<b>a</b>) calibration curves of the different sensors under 25% relative humidity at room temperature and (<b>b</b>) calibration curves under 70% relative humidity at room temperature.</p>
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<p>Comparison of the responses of the different sensors towards different gases at dry conditions to study the selectivity of the sensitive layer.</p>
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<p>(<b>a</b>) Calibration curve of the responses of the fabricated sensors towards different test conditions (Dry, 25% RH and 50% RH); (<b>b</b>) resistance changes of the sensor pristine rGO on Kapton when exposed to NH<sub>3</sub> at 25% RH; (<b>c</b>) hydrogen bonding of water and ammonia molecules.</p>
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12 pages, 4508 KiB  
Article
Fabrication of PVTF Films with High Piezoelectric Properties Through Directional Heat Treatment
by Xin Xin, Aotian Yee, Zhiyuan Zhou, Xuzhao He, Wenjian Weng, Chengwei Wu and Kui Cheng
J. Compos. Sci. 2024, 8(12), 512; https://doi.org/10.3390/jcs8120512 - 6 Dec 2024
Viewed by 383
Abstract
Piezoelectric materials can realize the mutual conversion of mechanical energy and electric energy, so they have excellent application prospects in the fields of sensors, energy collectors and biological materials. The poly(vinylidene fluoride) (PVDF)-based polymers have the best piezoelectric properties in the piezoelectric polymer, [...] Read more.
Piezoelectric materials can realize the mutual conversion of mechanical energy and electric energy, so they have excellent application prospects in the fields of sensors, energy collectors and biological materials. The poly(vinylidene fluoride) (PVDF)-based polymers have the best piezoelectric properties in the piezoelectric polymer, but they still have a large room for improvement compared with the piezoelectric ceramics. Improving their content of the polar β phase has become a consensus to polish up the piezoelectric performance. Most available studies construct hydrogen bonds or coulomb interactions between the surface of the dopant and molecular chains by doping, which promotes the molecular chains arrangement and thus facilitates the formation of the polar β phase. Recent studies show that the ordered arrangement of molecular chains is also important for piezoelectric properties. At present, the main way to improve the piezoelectric performance of PVDF is through doping or complex heat treatment process. Here, the poly(vinylidene fluoride-co-trifluoroethylene) (P(VDF-TrFE)) film was treated by directional heat treatment which used a heating table. Compared with uniform heat treatment like muffle furnace heat treatment, this simple vertical temperature gradient has many advantages for the content of the β phase and the crystallinity of P(VDF-TrFE). The results of the experiment showed that the content of the β phase of films remained at about 88%. When the film thickness was limited to 100 μm and the heat treatment temperature was limited to 200 °C, its crystallinity could reach 75% and the highest piezoelectric coefficient could reach 33.5 ± 0.7 pC/N. P(VDF-TrFE) films based on the experimental methods described above that show great potential for future applications in electronic devices and biomedical applications. Full article
(This article belongs to the Special Issue Feature Papers in Journal of Composites Science in 2024)
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<p>(<b>a</b>) Schematic diagram of P(VDF-TrFE) obtained by the heating table heat treatment and the SEM images of P(VDF-TrFE) of different thicknesses including (<b>b</b>) 50 μm, (<b>c</b>) 100 μm and (<b>d</b>) 150 μm.</p>
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<p>Composition and crystallization analysis of films of different thicknesses. (<b>a</b>) XRD image, (<b>b</b>) FTIR image, (<b>c</b>) DSC image, (<b>d</b>) schematic diagram of crystallization of films of different thicknesses.</p>
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<p>(<b>a</b>,<b>b</b>) d<sub>33</sub> analysis of films of different thicknesses and (<b>c</b>) contact angle images.</p>
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<p>SEM images of different temperature: (<b>a</b>) 160 °C, (<b>b</b>) 180 °C.</p>
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<p>Composition and crystallization analysis of films of different temperature. (<b>a</b>) XRD image, (<b>b</b>) FTIR image, (<b>c</b>) DSC image (the sample data for the heat treatment temperature of 200 °C here is the same as above), (<b>d</b>) schematic diagram of crystallization of films of different temperature.</p>
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<p>(<b>a</b>,<b>b</b>) d<sub>33</sub> analysis of films of different annealing temperatures and (<b>c</b>) contact angle images (the sample data for the heat treatment temperature of 200 °C here are the same as above).</p>
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<p>(<b>a</b>) FTIR image and (<b>b</b>) DSC image of a 100 μm film obtained by the muffle furnace, (<b>c</b>) melting point between the upper and lower surfaces of a 100 μm film obtained by heating table treatment, KPFM images of (<b>d</b>) 100 μm film obtained by the muffle furnace, (<b>e</b>) the worst-performing sample made from a heating table and (<b>f</b>) the best-performing sample made from a heating table; (<b>g</b>) schematic diagram of crystallization of films obtained from muffle furnace and heating table.</p>
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22 pages, 11834 KiB  
Article
Open-Source Data Logger System for Real-Time Monitoring and Fault Detection in Bench Testing
by Marcio Luís Munhoz Amorim, Jorge Gomes Lima, Norah Nadia Sánchez Torres, Jose A. Afonso, Sérgio F. Lopes, João P. P. do Carmo, Lucas Vinicius Hartmann, Cicero Rocha Souto, Fabiano Salvadori and Oswaldo Hideo Ando Junior
Inventions 2024, 9(6), 120; https://doi.org/10.3390/inventions9060120 - 4 Dec 2024
Viewed by 773
Abstract
This paper presents the design and development of a proof of concept (PoC) open-source data logger system for wireless data acquisition via Wi-Fi aimed at bench testing and fault detection in combustion and electric engines. The system integrates multiple sensors, including accelerometers, microphones, [...] Read more.
This paper presents the design and development of a proof of concept (PoC) open-source data logger system for wireless data acquisition via Wi-Fi aimed at bench testing and fault detection in combustion and electric engines. The system integrates multiple sensors, including accelerometers, microphones, thermocouples, and gas sensors, to monitor critical parameters, such as vibration, sound, temperature, and CO2 levels. These measurements are crucial for detecting anomalies in engine performance, such as ignition and combustion faults. For combustion engines, temperature sensors detect operational anomalies, including diesel engines operating beyond the normal range of 80 °C to 95 °C and gasoline engines between 90 °C and 110 °C. These readings help identify failures in cooling systems, thermostat valves, or potential coolant leaks. Acoustic sensors identify abnormal noises indicative of issues such as belt misalignment, valve knocking, timing irregularities, or loose parts. Vibration sensors detect displacement issues caused by engine mount failures, cracks in the engine block, or defects in pistons and valves. These sensors can work synergistically with acoustic sensors to enhance fault detection. Additionally, CO2 and organic compound sensors monitor fuel combustion efficiency and detect failures in the exhaust system. For electric motors, temperature sensors help identify anomalies, such as overloads, bearing problems, or excessive shaft load. Acoustic sensors diagnose coil issues, phase imbalances, bearing defects, and faults in chain or belt systems. Vibration sensors detect shaft and bearing problems, inadequate motor mounting, or overload conditions. The collected data are processed and analyzed to improve engine performance, contributing to reduced greenhouse gas (GHG) emissions and enhanced energy efficiency. This PoC system leverages open-source technology to provide a cost-effective and versatile solution for both research and practical applications. Initial laboratory tests validate its feasibility for real-time data acquisition and highlight its potential for creating datasets to support advanced diagnostic algorithms. Future work will focus on enhancing telemetry capabilities, improving Wi-Fi and cloud integration, and developing machine learning-based diagnostic methodologies for combustion and electric engines. Full article
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<p>Examples of development boards and open-source hardware applications: (<b>a</b>) Open Source Hardware and Open Source Initiative logos; (<b>b</b>) Arduino Uno; (<b>c</b>) Intel Edison development board; (<b>d</b>) Texas Instruments Launchpad; (<b>e</b>) STM32 Nucleon board; (<b>f</b>) photodynamic therapy device to detect hepatitis C; (<b>g</b>) portable laboratory platform for hepatitis C detection; and (<b>h</b>) system for measuring incident light in photovoltaic applications [<a href="#B16-inventions-09-00120" class="html-bibr">16</a>,<a href="#B17-inventions-09-00120" class="html-bibr">17</a>,<a href="#B18-inventions-09-00120" class="html-bibr">18</a>,<a href="#B19-inventions-09-00120" class="html-bibr">19</a>,<a href="#B20-inventions-09-00120" class="html-bibr">20</a>,<a href="#B21-inventions-09-00120" class="html-bibr">21</a>,<a href="#B22-inventions-09-00120" class="html-bibr">22</a>,<a href="#B23-inventions-09-00120" class="html-bibr">23</a>,<a href="#B24-inventions-09-00120" class="html-bibr">24</a>].</p>
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<p>Examples of development boards and open-source hardware applications: (<b>a</b>) Open Source Hardware and Open Source Initiative logos; (<b>b</b>) Arduino Uno; (<b>c</b>) Intel Edison development board; (<b>d</b>) Texas Instruments Launchpad; (<b>e</b>) STM32 Nucleon board; (<b>f</b>) photodynamic therapy device to detect hepatitis C; (<b>g</b>) portable laboratory platform for hepatitis C detection; and (<b>h</b>) system for measuring incident light in photovoltaic applications [<a href="#B16-inventions-09-00120" class="html-bibr">16</a>,<a href="#B17-inventions-09-00120" class="html-bibr">17</a>,<a href="#B18-inventions-09-00120" class="html-bibr">18</a>,<a href="#B19-inventions-09-00120" class="html-bibr">19</a>,<a href="#B20-inventions-09-00120" class="html-bibr">20</a>,<a href="#B21-inventions-09-00120" class="html-bibr">21</a>,<a href="#B22-inventions-09-00120" class="html-bibr">22</a>,<a href="#B23-inventions-09-00120" class="html-bibr">23</a>,<a href="#B24-inventions-09-00120" class="html-bibr">24</a>].</p>
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<p>Block diagram of the electronic circuit components and connections.</p>
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<p>Perfboard with the daughter boards attached.</p>
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<p>Mainboard and peripheral boards.</p>
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<p>External and internal structures of the PoC device.</p>
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<p>Overview of the structural components and parts of the PoC.</p>
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<p>Block diagram of the code behavior.</p>
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<p>Overview of the structural test setup.</p>
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<p>Sound levels of the motor (blue), motor and load (red), and motor and generator (yellow).</p>
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<p>Overview of the vibration dispersion over time between motor, load, and generator in (<b>a</b>) x-axis and (<b>b</b>) y-axis.</p>
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<p>Overview of the temperature difference between motor, generator, and load.</p>
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<p>The FFT response from the accelerometer.</p>
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<p>The FFT response from the microphone.</p>
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17 pages, 2877 KiB  
Article
Impedimetric Sensor for SARS-CoV-2 Spike Protein Detection: Performance Assessment with an ACE2 Peptide-Mimic/Graphite Interface
by Diego Quezada, Beatriz Herrera, Rodrigo Santibáñez, Juan Luis Palma, Esteban Landaeta, Claudio A. Álvarez, Santiago Valenzuela, Kevin Cobos-Montes, David Ramírez, Paula A. Santana and Manuel Ahumada
Biosensors 2024, 14(12), 592; https://doi.org/10.3390/bios14120592 - 3 Dec 2024
Viewed by 652
Abstract
The COVID-19 pandemic has prompted the need for the development of new biosensors for SARS-CoV-2 detection. Particularly, systems with qualities such as sensitivity, fast detection, appropriate to large-scale analysis, and applicable in situ, avoiding using specific materials or personnel to undergo the test, [...] Read more.
The COVID-19 pandemic has prompted the need for the development of new biosensors for SARS-CoV-2 detection. Particularly, systems with qualities such as sensitivity, fast detection, appropriate to large-scale analysis, and applicable in situ, avoiding using specific materials or personnel to undergo the test, are highly desirable. In this regard, developing an electrochemical biosensor based on peptides derived from the angiotensin-converting enzyme receptor 2 (ACE2) is a possible answer. To this end, an impedimetric detector was developed based on a graphite electrode surface modified with an ACE2 peptide-mimic. This sensor enables accurate quantification of recombinant 2019-nCoV spike RBD protein (used as a model analyte) within a linear detection range of 0.167–0.994 ng mL−1, providing a reliable method for detecting SARS-CoV-2. The observed sensitivity was further demonstrated by molecular dynamics that established the high affinity and specificity of the peptide to the protein. Unlike other impedimetric sensors, the herein presented system can detect impedance in a single frequency, allowing a measure as fast as 3 min to complete the analysis and achieving a detection limit of 45.08 pg mL−1. Thus, the proposed peptide-based electrochemical biosensor offers fast results with adequate sensitivity, opening a path to new developments concerning other viruses of interest. Full article
(This article belongs to the Special Issue Biosensors for the Analysis and Detection of Drug, Food or Disease)
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<p>Simplified workflow of the (<b>a</b>) fabrication of the biosensor based on ACE2 peptide-mimetic and (<b>b</b>) recombinant SARS-CoV-2 spike RBD protein detection. The modification of the graphite surface is achieved by incorporating -COOH residues, which serve as anchors for the immobilization of the ACE2 peptide-mimetic (ACE2<span class="html-italic">p</span>). The recombinant SARS-CoV-2 RBD protein is detected by measuring the system’s total impedance using [Fe(CN)<sub>6</sub>]<sup>−3/−4</sup> as a redox probe.</p>
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<p>Selected conformers for the coupling simulation study.</p>
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<p>Representation of the binding site and the complexes formed between ACE2-RBD, obtained from the crystallographic structure (PDB-ID: 6CS2), and the different conformers of the ACE2 peptide-mimic complex generated through docking simulation using HADDOCK. (<b>A</b>) ACE2-RBD complex, (<b>B</b>) RBD–Conformer 1, (<b>C</b>) RBD–Conformer 2, (<b>D</b>) RBD–Conformer 3, and (<b>E</b>) RBD–Conformer 4.</p>
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<p>SEM/EDS analysis of three graphite electrodes: (<b>a</b>) blank graphite electrode (graphite), (<b>b</b>) electrografted graphite electrode (EG–graphite), and (<b>c</b>) peptide-modified graphite electrode (ACE2<span class="html-italic">p</span>–graphite). The crosses in each SEM image indicate the regions where the composition analysis was performed. The corresponding atomic concentrations of carbon, oxygen, and nitrogen are shown below each image. Scale bars represent 50 µm.</p>
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<p>Comparison of electrode surfaces via AFM. (<b>a</b>) Blank graphite electrode (graphite), (<b>b</b>) electrografted graphite electrode (EG–graphite), and (<b>c</b>) ACE2<span class="html-italic">p</span>-modified graphite electrode (ACE2<span class="html-italic">p</span>–graphite).</p>
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<p>Cyclic voltammogram of [Fe(CN)<sub>6</sub>]<sup>4−/3−</sup> 5 mM in PBS 1× pH 7.4 using graphite (black), EG-graphite (blue), and ACE2<span class="html-italic">p</span>-graphite (red) as the working electrode.</p>
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<p>(<b>a</b>) Bode graph of a series of solutions with increasing concentration of recombinant 2019-nCoV spike RBD protein. (<b>b</b>) Variation of total impedance with respect to the concentration of recombinant 2019-nCoV spike RBD protein.</p>
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17 pages, 5352 KiB  
Article
Evaluation of a Non-Enzymatic Electrochemical Sensor Based on Co(OH)2-Functionalized Carbon Nanotubes for Glucose Detection
by Diego Bolaños-Mendez, Lenys Fernández, Rafael Uribe, Alisson Cunalata-Castro, Gema González, Isamara Rojas, Andrés Chico-Proano, Alexis Debut, Luis Alberto Celi and Patricio Espinoza-Montero
Sensors 2024, 24(23), 7707; https://doi.org/10.3390/s24237707 - 2 Dec 2024
Viewed by 500
Abstract
This work reports on the assessment of a non-hydrolytic electrochemical sensor for glucose sensing that is developed using functionalized carbon nanotubes (fCNTs)/Co(OH)2. The morphology of the nanocomposite was investigated by scanning electron microscopy, which revealed that the CNTs interacted with Co(OH) [...] Read more.
This work reports on the assessment of a non-hydrolytic electrochemical sensor for glucose sensing that is developed using functionalized carbon nanotubes (fCNTs)/Co(OH)2. The morphology of the nanocomposite was investigated by scanning electron microscopy, which revealed that the CNTs interacted with Co(OH)2. This content formed a nanocomposite that improved the electrochemical characterizations of the electrode, including the electrochemical active surface area and capacitance, thus improving sensitivity to glucose. In the electrochemical characterization by cyclic voltammetry and chronoamperometry, the increase in catalytic activity by Co(OH)2 improved the stability and reproducibility of the glucose sensor without the use of enzymes, and its concentration range was between 50 and 700 μmol L−1. The sensor exhibited good linearity towards glucose with LOD value of 43.200 µmol L−1, which proved that the Co(OH)2-fCNTs composite is judicious for constructing cost effective and feasible sensor for glucose detection. Full article
(This article belongs to the Special Issue Nanomaterials for Sensor Applications)
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<p>TEM images of unfunctionalized (CNTs).</p>
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<p>TEM images of the functionalized CNTs (fCNTs).</p>
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<p>TEM images of the functionalized nanotubes modified with cobalt hydroxide (Co(OH)2-fCNTs).</p>
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<p>FTIR spectra from 4400 to 1000 cm<sup>−1</sup> of: (<b>a</b>) fCNTs and (<b>b</b>) Co(OH)<sub>2</sub>-fCNTs.</p>
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<p>Raman spectra.</p>
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<p>PXRD patterns of Co(OH)<sub>2</sub>-fCNTs and fCNT.</p>
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<p>Electrochemical characterization of glassy carbon (GC). (<b>a</b>) Cyclic voltammogram at different rates in a solution K<sub>3</sub>Fe(CN)<sub>6</sub>/K<sub>4</sub>Fe(CN)<sub>6</sub> 5.0 mM + KCl 0.1 M, (<b>b</b>) linearization of anodic and cathodic peak current versus velocity, and linearization of anodic and cathodic current versus the square root of velocity.</p>
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<p>Electrochemical characterization of the modified fCNTs/GC electrode. (<b>a</b>) Cyclic voltammogram at different rates in a solution K<sub>3</sub>Fe(CN)<sub>6</sub>/K<sub>4</sub>Fe(CN)<sub>6</sub> 5.0 mM + KCl 0.1 M, (<b>b</b>) linearization of anodic and cathodic peak current versus velocity, and linearization of anodic and cathodic current versus the square root of velocity.</p>
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<p>Electrochemical characterization of the modified Co(OH)<sub>2</sub>-fCNTs/GC. (<b>a</b>) Cyclic voltammogram at different rates in a solution K<sub>3</sub>Fe(CN)<sub>6</sub>/K<sub>4</sub>Fe(CN)<sub>6</sub> 5.0 mM + KCl 0.1 M, (<b>b</b>) linearization of anodic and cathodic peak current versus velocity, and linearization of anodic and cathodic current versus the square root of velocity.</p>
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<p>Linear regression of background current density against sweep speed (capacitance).</p>
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<p>Cyclic voltammograms of the glucose response to different concentrations in NaOH solution 0.1 mol L<sup>−1</sup> at the modified electrodes.</p>
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<p>(<b>a</b>) Cyclic voltammogram of the glucose response on the modified electrode Co(OH)<sub>2</sub>-fCNTs/GC, (<b>b</b>) chronoamperometry response of glucose to different potentials at the modified electrode Co(OH)<sub>2</sub>-fCNTs/GC.</p>
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<p>Calibration curve of glucose at modified electrode Co(OH)<sub>2</sub>-fCNTs/GC, NaOH 0.1 mol L<sup>−1</sup>. Insert: chronoamperometry detection.</p>
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<p>Possible mechanism of glucose electro-oxidation on Co(OH)<sub>2</sub>-fCNTs/GCE.</p>
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15 pages, 4618 KiB  
Article
2D Flower-like CdS@Co/Mo-MOF as Co-Reaction Accelerator of g-C3N4-Based Electrochemiluminescence Sensor for Chlorpromazine Hydrochloride
by Xiaowei Fan, Guping Zhang, Xiaodi Li, Yao Wang, Yi Wang, Shilei Hao and Defang Liu
Biosensors 2024, 14(12), 586; https://doi.org/10.3390/bios14120586 - 2 Dec 2024
Viewed by 478
Abstract
In this study, we have proposed an electrochemiluminescence (ECL) signal amplification system which is based on two-dimensional (2D) flower-like CdS@Co/Mo-MOF composites as a co-reaction accelerator of the g-C3N4/S2O82− system for ultrasensitive detection of chlorpromazine hydrochloride [...] Read more.
In this study, we have proposed an electrochemiluminescence (ECL) signal amplification system which is based on two-dimensional (2D) flower-like CdS@Co/Mo-MOF composites as a co-reaction accelerator of the g-C3N4/S2O82− system for ultrasensitive detection of chlorpromazine hydrochloride (CPH). Specifically, the 2D flower-like Co/Mo-MOF with mesoporous alleviated the aggregation of CdS NPs while simultaneously fostering reactant-active site contact and improving the reactant–product transport rate. This allowed the material to act as a novel co-reaction accelerator, speeding up the transformation of the S2O82− into SO4•− and enhancing the cathodic ECL emission of g-C3N4. Moreover, the signal probe which was synthesized by coupling the 2D CdS@Co/Mo-MOF and graphitic carbon nitride (g-C3N4) achieved the generation of SO4•− in situ and reduced energy loss. The results confirmed that the ECL signal was enhanced 6.2-fold and stabilized by CdS@Co/Mo-MOF. Based on the extremely strong quenching effect of chlorpromazine hydrochloride (CPH) on this system, a “signal-off” type sensor was constructed. The sensor demonstrated excellent sensitivity and linear response to CPH concentrations ranging from 1 pmol L−1 to 100 μmol L−1, with a low detection limit of 0.4 pmol L−1 (S/N = 3). Full article
(This article belongs to the Special Issue Innovative Biosensing Technologies for Sustainable Healthcare)
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<p>(<b>A</b>) Coordination process, (<b>B</b>) SEM image, and (<b>C</b>,<b>D</b>) TEM images of Co/Mo-MOF. And SEM images of (<b>E</b>) CdS NPs, (<b>F</b>) CdS@Co/Mo-MOF, and (<b>G</b>) g-C<sub>3</sub>N<sub>4</sub>.</p>
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<p>(<b>A</b>) N<sub>2</sub> adsorption/desorption isotherms and (<b>B</b>) pore size distribution plot of Co/Mo-MOF.</p>
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<p>(<b>A</b>) Survey XPS spectrum of the CdS@Co/Mo-MOF, and high-resolution XPS spectra of (<b>B</b>) Co 2p, (<b>C</b>) Cd 3d, (<b>D</b>) Mo 3d, and (<b>E</b>) C 1s. And (<b>F</b>) UV–vis spectra of different materials (Co/Mo-MOF (a), CdS (b), and CdS@Co/Mo-MOF (c)).</p>
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<p>(<b>A</b>) The ECL responses of (a) GCE/S<sub>2</sub>O<sub>8</sub><sup>2−</sup>, (b) g-C<sub>3</sub>N<sub>4</sub>, (c) g-C<sub>3</sub>N<sub>4</sub>/S<sub>2</sub>O<sub>8</sub><sup>2−</sup>, (d) g-C<sub>3</sub>N<sub>4</sub>/CdS@Co/Mo-MOF/S<sub>2</sub>O<sub>8</sub><sup>2−</sup>, (e) g-C<sub>3</sub>N<sub>4</sub>/CdS@Co/Mo-MOF, (f) CdS@Co/Mo-MOF/S<sub>2</sub>O<sub>8</sub><sup>2−</sup>, (g) g-C<sub>3</sub>N<sub>4</sub>/H-ZIF-67/S<sub>2</sub>O<sub>8</sub><sup>2−</sup>, and (h) g-C<sub>3</sub>N<sub>4</sub>/Co/Mo-MOF/S<sub>2</sub>O<sub>8</sub><sup>2−</sup>. (<b>B</b>) The CV behaviors of various modified (bare GCE (a) and CdS@Co/Mo-MOF/GCE (b)) in 7 mM K<sub>2</sub>S<sub>2</sub>O<sub>8</sub> solution. (<b>C</b>) The CV behaviors in 5 mM [Fe(CN)<sub>6</sub>]<sup>3−/4−</sup> solution containing 0.1 M KCl and (<b>D</b>) LSV behaviors in PBS buffer of various modified (GCE (a), g-C<sub>3</sub>N<sub>4</sub>/GCE (b), and g-C<sub>3</sub>N<sub>4</sub>/CdS@Co/Mo-MOF/GCE (c)). (<b>E</b>) The ECL response curves of (a) g-C<sub>3</sub>N<sub>4</sub>/S<sub>2</sub>O<sub>8</sub><sup>2−</sup> and (b) g-C<sub>3</sub>N<sub>4</sub>/CdS@Co/Mo-MOF/S<sub>2</sub>O<sub>8</sub><sup>2−</sup> systems with consecutive 10 cycles CV scans. And (<b>F</b>) the peak position of the ECL signal of (a) g-C<sub>3</sub>N<sub>4</sub> and (b) g-C<sub>3</sub>N<sub>4</sub>/CdS@Co/Mo-MOF.</p>
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<p>The CV behaviors of (<b>A</b>) ZIF-67 synthesized by the different solvent system (M-ZIF-67/GCE (a), D-ZIF-67/GCE (b), and H-ZIF-67/GCE (c)) and (<b>B</b>) various modified (H-ZIF-67/GCE (a), CdS NPs/GCE (b), Co/Mo-MOF/GCE (c), and CdS@Co/Mo-MOF/GCE (d)) in 0.1 M KCl solution containing 5 mM [Fe(CN)<sub>6</sub>]<sup>3−/4−</sup>. And (<b>C</b>) CV behaviors of different modified electrodes (H-ZIF-67/GCE (a), Co/Mo-MOF/GCE (b), and CdS@Co/Mo-MOF/GCE (c)) in 7 mM K<sub>2</sub>S<sub>2</sub>O<sub>8</sub> solution.</p>
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<p>(<b>A</b>) ECL responses and (<b>B</b>) CV behaviors of different systems (without 1.0 mM CPH (a) and containing 1.0 mM CPH (b) in the detection solution).</p>
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<p>Effect of different experimental conditions on the response signals: (<b>A</b>) pH, (<b>B</b>) the concentration of K<sub>2</sub>S<sub>2</sub>O<sub>8</sub>, (<b>C</b>) the concentration of CdS@Co/Mo-MOF, and (<b>D</b>) x%-CdS@Co/Mo-MOF. Error bars: SD, <span class="html-italic">n</span> = 3.</p>
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<p>(<b>A</b>) The ECL response curves and (<b>B</b>) the linear calibration curve of the designed ECL sensor for a series of CPH concentrations.</p>
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<p>(<b>A</b>) Selectivity, (<b>B</b>) reproducibility, and (<b>C</b>) stability of the sensor. (<b>D</b>) The stability of the luminescent signal enhancement of CdS@Co/Mo-MOF composites in aqueous solution for 15 consecutive days.</p>
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<p>The schematic for the preparation of the material.</p>
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14 pages, 2109 KiB  
Article
Monitoring Indoor Air Quality in Classrooms Using Low-Cost Sensors: Does the Perception of Teachers Match Reality?
by Nuno Canha, Carolina Correia, Sergio Mendez, Carla A. Gamelas and Miguel Felizardo
Atmosphere 2024, 15(12), 1450; https://doi.org/10.3390/atmos15121450 - 1 Dec 2024
Viewed by 511
Abstract
This study intended to understand whether teachers’ perceptions of indoor air quality (IAQ) during classes aligned with the real levels of air pollutants and comfort parameters. For this purpose, an IAQ monitoring survey based on low-cost sensors using a multi-parameter approach was carried [...] Read more.
This study intended to understand whether teachers’ perceptions of indoor air quality (IAQ) during classes aligned with the real levels of air pollutants and comfort parameters. For this purpose, an IAQ monitoring survey based on low-cost sensors using a multi-parameter approach was carried out in nine classrooms (a total of 171 monitored classes) in a Portuguese school. In each monitored class, the perception of IAQ reported by the teacher was assessed using a scale from 1 (very bad IAQ) to 10 (very good IAQ). Several exceedances regarding national legislation were found, with temperature being the parameter with a higher percentage of exceedance in all the studied classrooms (46%), followed by PM10 (32%), and then CO2 (27%). Temperature was found to be the only environmental parameter that was significantly associated with lower IAQ perception reported by the teachers, highlighting that typical pollutants such as CO2 (which can be identified as stuffy air) did not contribute to the teachers’ perceptions. Full article
(This article belongs to the Special Issue Indoor Air Quality Control)
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<p>Mean temperatures (blue bars) and their standard deviations monitored during classes in each studied classroom. The number in brackets represents the number of classes evaluated in each classroom. The triangle and square represent, respectively, the minimum and maximum mean values assessed in each classroom. The green area represents the acceptable range established by ISO 7730 [<a href="#B29-atmosphere-15-01450" class="html-bibr">29</a>], and the red dots correspond to the percentage of classes in which the mean values were outside the acceptable range.</p>
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<p>Mean RH values (blue bars) and standard deviations monitored during classes in each studied classroom. The number in brackets represents the number of classes evaluated in each classroom. The triangle and square represent, respectively, the minimum and maximum mean values assessed in each classroom. The green area represents the acceptable range established by ISO 7730 [<a href="#B29-atmosphere-15-01450" class="html-bibr">29</a>], and the red dots correspond to the percentage of classes in which the mean values were outside the acceptable range.</p>
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<p>Mean CO<sub>2</sub> levels (blue bars) and standard deviations monitored in the studied classrooms. The number in brackets represents the number of classes evaluated in each classroom. The triangle and square represent, respectively, the minimum and maximum mean values assessed in each classroom. The red line represents the limit value of 1250 ppm established by Portuguese legislation [<a href="#B31-atmosphere-15-01450" class="html-bibr">31</a>], and the red dots correspond to the percentage of classes in which the mean values were above the limit value.</p>
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<p>Mean VOC levels (blue bars) and standard deviations monitored in the studied classrooms. The number in brackets represents the number of classes evaluated in each classroom. The triangle and square represent, respectively, the minimum and maximum mean values assessed in each classroom. The red line represents the limit value of 262 ppb established by the Portuguese legislation [<a href="#B31-atmosphere-15-01450" class="html-bibr">31</a>]. Red dots correspond to the percentage of classes in which the mean values were above the limit value.</p>
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<p>Mean PM<sub>2.5</sub> levels (blue bars) and standard deviations monitored during the classes in each studied classroom. The number in brackets represents the number of classes evaluated in each classroom. The triangle and square represent, respectively, the minimum and maximum means assessed in each classroom. The red line represents the limit value of 25 μg.m<sup>−3</sup> established by Portuguese legislation [<a href="#B31-atmosphere-15-01450" class="html-bibr">31</a>], and the red dots correspond to the percentage of classes with mean values above the limit value. The green line represents the air quality guideline of 5 µg.m<sup>−3</sup> established by WHO [<a href="#B34-atmosphere-15-01450" class="html-bibr">34</a>], and the green dots correspond to the percentage of classes with mean values above this threshold.</p>
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<p>Mean PM<sub>10</sub> levels (blue bars) and standard deviations monitored during the classes in each studied classroom. The number in brackets represents the number of classes evaluated in each classroom. The triangle and square represent, respectively, the minimum and maximum means assessed in each classroom. The red line represents the limit value of 50 μg.m<sup>−3</sup> established by the Portuguese legislation [<a href="#B31-atmosphere-15-01450" class="html-bibr">31</a>] and the red dots correspond to the percentage of classes with mean values above the limit value. The green line represents the air quality guideline of 15 µg.m<sup>−3</sup> established by WHO [<a href="#B34-atmosphere-15-01450" class="html-bibr">34</a>], and the green dots correspond to the percentage of classes with mean values above this threshold.</p>
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<p>Histogram of the IAQ perception (ranging from 1, representing “very bad IAQ”, to 10, representing “very good IAQ”) of teachers during the studied 170 classes.</p>
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17 pages, 4964 KiB  
Article
Laser-Induced Graphene Decorated with MOF-Derived NiCo-LDH for Highly Sensitive Non-Enzymatic Glucose Sensor
by Longxiao Li, Yufei Han, Yuzhe Zhang, Weijia Wu, Wei Du, Guojun Wen and Siyi Cheng
Molecules 2024, 29(23), 5662; https://doi.org/10.3390/molecules29235662 - 29 Nov 2024
Viewed by 376
Abstract
Designing and fabricating a highly sensitive non-enzymatic glucose sensor is crucial for the early detection and management of diabetes. Meanwhile, the development of innovative electrode substrates has become a key focus for addressing the growing demand for constructing flexible sensors. Here, a simple [...] Read more.
Designing and fabricating a highly sensitive non-enzymatic glucose sensor is crucial for the early detection and management of diabetes. Meanwhile, the development of innovative electrode substrates has become a key focus for addressing the growing demand for constructing flexible sensors. Here, a simple one-step laser engraving method is applied for preparing laser-induced graphene (LIG) on polyimide (PI) film, which serves as the sensor substrate. NiCo-layered double hydroxides (NiCo-LDH) are synthesized on LIG as a precursor, utilizing the zeolitic imidazolate framework (ZIF-67), and then reacted with Ni(NO3)2 via solvent-thermal methods. The sensitivity of the non-enzymatic electrochemical glucose sensor is significantly improved by employing NiCo-LDH/LIG as the sensing material. The porous and interconnected structure of NiCo-LDH, derived from ZIF-67, enhances the accessibility of electrochemically active sites, while the incorporation of LIG ensures exceptional conductivity. The combination of NiCo-LDH with LIG enables efficient electron transport, leading to an increased electrochemically active surface area and enhanced catalytic efficiency. The fabricated electrode achieves a low glucose detection limit of 0.437 μM and demonstrates a high sensitivity of 1141.2 and 631.1 μA mM−2 cm−2 within the linear ranges of 0–770 μM and 770–1970 μM, respectively. Furthermore, the NiCo-LDH/LIG glucose sensor demonstrates superior reliability and little impact from other substances. A flexible integrated LIG-based non-enzymatic glucose sensor has been developed, demonstrating high sensitivity and suggesting a promising application for LIG-based chemical sensors. Full article
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<p>Three-dimensional view of the conductivity of LIG under different laser parameters.</p>
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<p>(<b>a</b>) NiCo-LDH/LIG preparation process diagram. Low- and high-resolution SEM images of the (<b>b</b>,<b>f</b>) LIG, (<b>c</b>,<b>g</b>) Co-MOF/LIG, (<b>d</b>,<b>h</b>) and NiCo-LDH/LIG. (<b>e</b>,<b>i</b>) Low- and high-resolution TEM images of the NiCo-LDH.</p>
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<p>(<b>a</b>) LIG’s adsorption/desorption isotherm and pore size distribution. (<b>b</b>) NiCo-LDH/LIG’s adsorption/desorption isotherm and pore size distribution.</p>
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<p>(<b>a</b>) XRD patterns of the LIG, Co-MOF/LIG, and NiCo-LDH/LIG. XPS spectra of the NiCo-LDH in the (<b>b</b>) survey spectrum, (<b>c</b>) Ni 2p, and (<b>d</b>) Co 2p.</p>
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<p>(<b>a</b>) CV curves for LIG and NiCo−LDH/LIG in 0.1 M NaOH, with and without 1 mM glucose, were recorded at a scan rate of 10 mV/s. (<b>b</b>) CV curves of NiCo−LDH/LIG were obtained in solutions with 0, 1, 2, and 3 mM glucose at a scan rate of 10 mV/s. (<b>c</b>) Current responses of five successive injections of 500 μM glucose at different applied voltages. (<b>d</b>) The linear fitting results with error bars.</p>
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<p>(<b>a</b>) Comparative glucose titration experiments of NiCo-LDH/LIG, NiCo-LDH/Ag, Co-MOF/LIG, and Co-MOF/Ag at 0.5 V in 0.1 M NaOH solution. (<b>b</b>) Fitting curves with error bars for the comparative experiments.</p>
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<p>(<b>a</b>) A series of amperometric I–t curves were recorded by sequentially adding different glucose concentrations (5, 10, 20, 50, 100, 200, and 400 μM, with each concentration tested twice) to a solution at an applied potential of 0.5 V using Ag/AgCl as the RE. (<b>b</b>) Linear fitting curve of the response current with glucose concentration, including error bars. (<b>c</b>) Low concentration enlargement of (<b>a</b>). (<b>d</b>) Low concentration fitting curve in (<b>b</b>). (<b>e</b>) Current responses of NiCo-LDH/LIG upon the addition of various different interferences. (<b>f</b>) Reliability test of NiCo-LDH/LIG over 7 days.</p>
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<p>(<b>a</b>) Photograph of LIG patterns on PI and the integrated three-electrode glucose sensor device. (<b>b</b>) Amperometric I–t curves of successive additions of the same concentrations of glucose (400 μM) at an applied potential of 0.5 V. (<b>c</b>) Linear fitting curve of response current with glucose concentration.</p>
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<p>(<b>a</b>) NiCo-LDH/LIG sensor was tested with synthetic blood and glucose solution in 0.1 M NaOH solution. (<b>b</b>) Comparison test of glucose with other sugars in 0.1 M NaOH solution.</p>
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17 pages, 1585 KiB  
Article
Influence of Particulate Matter and Carbon Dioxide on Students’ Emotions in a Smart Classroom
by Gabriela Fretes, Cèlia Llurba, Ramon Palau and Joan Rosell-Llompart
Appl. Sci. 2024, 14(23), 11109; https://doi.org/10.3390/app142311109 - 28 Nov 2024
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Abstract
The effects of air quality on health and cognition are well documented, but few studies have focused on its impact on emotions, leaving this area underexplored. This study investigates the influence of environmental factors—specifically particulate matter (PM1, PM2.5, and [...] Read more.
The effects of air quality on health and cognition are well documented, but few studies have focused on its impact on emotions, leaving this area underexplored. This study investigates the influence of environmental factors—specifically particulate matter (PM1, PM2.5, and PM10) and carbon dioxide (CO2)—on students’ basic emotions in secondary school classrooms. For the collection of environmental data, we used low-cost sensors, which were carefully calibrated to ensure acceptable accuracy for monitoring air quality variables, despite inherent precision limitations compared to traditional sensors. Emotions were recorded via camera and analyzed using a custom-developed code. Based on these data, we found significant but modest correlations, such as the negative correlation between PM levels and happiness, and positive correlations of CO2 concentrations with fear and disgust. The regression models explained between 36% and 62% of the variance in emotions like neutrality, sadness, fear, and happiness, highlighting nonlinear relationships in some cases. These findings underscore the need for improved classroom environmental management, including the implementation of real-time air quality monitoring systems. Such systems would enable schools to mitigate the negative emotional effects of poor air quality, contributing to healthier and more conducive learning environments. Future research should explore the combined effects of multiple environmental factors to further understand their impact on student well-being. Full article
(This article belongs to the Section Ecology Science and Engineering)
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<p>ACTUA Kit device for environmental factors monitoring.</p>
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<p>Spearman’s correlations among environmental factors (PM and CO<sub>2</sub>) and emotions with significance levels. * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001.</p>
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<p>Explained variance (R<sup>2</sup>) and predictive accuracy (RMSE) for emotions based on environmental factors. <span class="html-italic">**</span> Statistically significant at <span class="html-italic">p</span> &lt; 0.001.</p>
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<p>Standardized regression coefficients for each emotion.</p>
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17 pages, 2885 KiB  
Article
Advanced SnO2 Thin Films: Stability and Sensitivity in CO Detection
by Nadezhda K. Maksimova, Tatiana D. Malinovskaya, Valentina V. Zhek, Nadezhda V. Sergeychenko, Evgeniy V. Chernikov, Denis V. Sokolov, Aleksandra V. Koroleva, Vitaly S. Sobolev and Petr M. Korusenko
Int. J. Mol. Sci. 2024, 25(23), 12818; https://doi.org/10.3390/ijms252312818 - 28 Nov 2024
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Abstract
This paper presents the results of a study on the characteristics of semiconductor sensors based on thin SnO2 films modified with antimony, dysprosium, and silver impurities and dispersed double Pt/Pd catalysts deposited on the surface to detect carbon monoxide (CO). An original [...] Read more.
This paper presents the results of a study on the characteristics of semiconductor sensors based on thin SnO2 films modified with antimony, dysprosium, and silver impurities and dispersed double Pt/Pd catalysts deposited on the surface to detect carbon monoxide (CO). An original technology was developed, and ceramic targets were made from powders of Sn-Sb-O, Sn–Sb-Dy–O, and Sn–Sb-Dy-Ag–O systems synthesized by the sol–gel method. Films of complex composition were obtained by RF magnetron sputtering of the corresponding targets, followed by technological annealing at various temperatures. The morphology of the films, the elemental and chemical composition, and the electrical and gas-sensitive properties were studied. Special attention was paid to the effect of the film composition on the stability of sensor parameters during long-term tests under the influence of CO. It was found that different combinations of concentrations of antimony, dysprosium, and silver had a significant effect on the size and distribution of nanocrystallites, the porosity, and the defects of films. The mechanisms of degradation under prolonged exposure to CO were examined. It was established that Pt/Pd/SnO2:0.5 at.% Sb film with optimal crystallite sizes and reduced porosity provided increased stability of carbon monoxide sensor parameters, and the response to the action of 100 ppm carbon monoxide was G1/G0 = 2–2.5. Full article
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<p>AFM images of samples: series (I)-693K (<b>a</b>), series (II)-693K (<b>b</b>), (III)-723K (<b>c</b>), series (IV)-693K (<b>d</b>), and (V)-723K (<b>e</b>).</p>
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<p>Survey PE spectra of samples: (1)—(I)-693K, (2)—(II)-693K, (3)—(III)-723K, (4)—(IV)-693K, (5)—(V)-723K, and reference SnO<sub>2</sub>.</p>
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<p>Sn 3<span class="html-italic">d</span> (<b>a</b>), O 1<span class="html-italic">s</span> with Sb 3<span class="html-italic">d</span><sub>3/2</sub> (<b>b</b>), Dy 3<span class="html-italic">d</span> (<b>c</b>), and Ag 3<span class="html-italic">d</span> (<b>d</b>) PE spectra of samples: (1)—(I)-693K, (2)—(II)-693K, (3)—(III)-723K, (4)—(IV)-693K, (5)—(V)-723K, and reference compounds (SnO<sub>2</sub>, Sb<sub>2</sub>O<sub>5</sub>, and Ag<sup>0</sup>).</p>
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<p>Raman spectra of SnO<sub>2</sub> powder as well as samples (I)-693K, (II)-693K, and (IV)-693K before and after long-term (90 days) testing under CO exposure (designated by the number 1 superscript in the sample name).</p>
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<p>Graphs of conductivity versus (<b>a</b>) CO concentration and (<b>b</b>) response of freshly prepared sensors of series: (1)—(I)-693K, (2)—(II)-693K, (4)—(IV)-693K, and (5)—(V)-723K.</p>
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<p>Concentration dependences of the response of freshly prepared sensors (curves 1) and sensors after long-term (90 days) testing (curves 2). Films from different series are presented: (<b>a</b>)—(I)-693K, (<b>b</b>)—(II)-693K, (<b>c</b>)—(IV)-693K, and (<b>d</b>)—(V)-723K.</p>
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<p>SEM images obtained in the back-scattering (BSE) mode: the sensitive element from the side of (<b>a</b>) semiconductor SnO<sub>2</sub> layer and (<b>b</b>) heater; (<b>c</b>) sensors assembled into TO-8 case: 1—sensitive element; 2—Pt electrodes; 3—sapphire substrate; 4—Pt heater.</p>
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<p>Schematic diagram of the measuring stand.</p>
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