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Functional Nanomaterials in Sensing

A special issue of Sensors (ISSN 1424-8220). This special issue belongs to the section "Sensor Materials".

Deadline for manuscript submissions: 25 August 2025 | Viewed by 17630

Special Issue Editors


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Guest Editor
Department of Chemistry, National Institute of Technology Hamirpur, Hamirpur 177005, Himachal Pradesh, India
Interests: nanomaterials; nanocomposites; photocatalysts; plasmonic photocatalysts; visible light catalysts; solar cell, SERS sensing; hybrid nanomaterials; metal oxide semiconductors
Special Issues, Collections and Topics in MDPI journals

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Guest Editor
Department of Nature Sciences, Mathematics and Education, Federal University of São Carlos, Araras 13600-970, SP, Brazil
Interests: disposable sensors; 3D-printed electrodes; nanomaterials
Special Issues, Collections and Topics in MDPI journals
School of Natural Sciences, Macquarie University, Sydney, NSW 2109, Australia
Interests: electroanalytical chemistry; ultramicroelectrode voltammetry; electrochemical sensors

Special Issue Information

Dear Colleagues,

This Special Issue is devoted to forefront interdisciplinary research topics related to functional nanomaterials applied to sensing technologies. Nanomaterials of interest include, but are not limited to, metal and carbon nanomaterials developed for sensing, biosensing and other medical diagnoses. Owing to their unique physiochemical and optoelectronic properties, these functional nanomaterials often provide exceptional tunable characteristics that enhance the efficiency and stability of sensing devices. In addition, the combination of their individual unique properties can allow hybrid nanocomposites to provide a synergistic effect to their sensing performance, leading to advanced sensing technology in various fields. Accordingly, this Special Issue cordially seeks researchers willing to provide contributions demonstrating advancements in functional nanomaterial-based electrochemical sensing technology applied for the detection of relevant molecules of environmental and biological significance.

Dr. Jai Prakash
Prof. Dr. Bruno Campos Janegitz
Dr. Danny Wong
Guest Editors

Manuscript Submission Information

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Keywords

  • metal nanostructures
  • carbon-based materials
  • hybrid nanocomposites
  • sensing technologies
  • sensing devices
  • environmental sensors
  • biomedical applications

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Published Papers (10 papers)

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Research

19 pages, 9551 KiB  
Article
Flexible Electromagnetic Sensor with Inkjet-Printed Silver Nanoparticles on PET Substrate for Chemical and Biomedical Applications
by Muhammad Usman Ejaz, Tayyaba Irum, Muhammad Qamar and Akram Alomainy
Sensors 2024, 24(20), 6526; https://doi.org/10.3390/s24206526 - 10 Oct 2024
Cited by 1 | Viewed by 1427
Abstract
For this article, a low-cost, compact, and flexible inkjet-printed electromagnetic sensor was investigated for its chemical and biomedical applications. The investigated sensor design was used to estimate variations in the concentration of chemicals (ethanol and methanol) and biochemicals (hydrocortisone—a chemical derivative of cortisol, [...] Read more.
For this article, a low-cost, compact, and flexible inkjet-printed electromagnetic sensor was investigated for its chemical and biomedical applications. The investigated sensor design was used to estimate variations in the concentration of chemicals (ethanol and methanol) and biochemicals (hydrocortisone—a chemical derivative of cortisol, a biomarker of stress and cardiovascular effects). The proposed design’s sensitivity was further improved by carefully choosing the frequency range (0.5–4 GHz), so that the analyzed samples showed approximately linear variations in their dielectric properties. The dielectric properties were measured using a vector network analyzer (VNA) and an Agilent 85070E Dielectric Probe Kit. The sensor design had a resonant frequency at 2.2 GHz when investigated without samples, and a consistent shift in resonant frequency was observed, with variation in the concentrations of the investigated chemicals. The sensitivity of the designed sensor is decent and is comparable to its non-flexible counterparts. Furthermore, the simulation and measured results were in agreement and were comparable to similar investigated sensor prototypes based on non-flexible Rogers substrates (Rogers RO4003C) and Rogers Droid/RT 5880), demonstrating true potential for chemical, biomedical applications, and healthcare. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Role of antennas and EM sensors in biomedical applications and wireless health monitoring.</p>
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<p>Mechanism of rise in hair cortisol with the increase in chronic stress and its cardiovascular effects.</p>
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<p>Design flow chart for sensor under investigation.</p>
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<p>Proposed design: (<b>a</b>,<b>b</b>) front and back view with dimensions; (<b>c</b>,<b>d</b>) fabricated design; (<b>e</b>) measured transmission coefficient (<math display="inline"><semantics> <msub> <mi>S</mi> <mn>21</mn> </msub> </semantics></math>).</p>
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<p>Proposed design fabricated on a PET substrate: (<b>a</b>,<b>b</b>) front and back view with dimensions; (<b>c</b>,<b>d</b>) fabricated design; (<b>e</b>) measured transmission coefficient (<math display="inline"><semantics> <msub> <mi>S</mi> <mn>21</mn> </msub> </semantics></math>).</p>
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<p>PET based sensor design with equivalent circuit model.(<b>a</b>,<b>b</b>) front and back view with dimensions; (<b>c</b>) equivalent circuit model (<math display="inline"><semantics> <msub> <mi>L</mi> <mi>S</mi> </msub> </semantics></math> = inductance of SRR, <math display="inline"><semantics> <msub> <mi>C</mi> <mi>S</mi> </msub> </semantics></math> = capacitance of SRR, <math display="inline"><semantics> <msub> <mi>R</mi> <mi>S</mi> </msub> </semantics></math> = resistance of SRR, <math display="inline"><semantics> <msub> <mi>C</mi> <mi>G</mi> </msub> </semantics></math> = capacitance between ground plane and microstrip line, <math display="inline"><semantics> <msub> <mi>Z</mi> <mi>T</mi> </msub> </semantics></math> = Impedance of microstrip line, <math display="inline"><semantics> <msub> <mi>L</mi> <mi>M</mi> </msub> </semantics></math> = inductance of microstrip line).</p>
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<p>Measurement setup to compute the electrical permittivity of the prepared samples, using VNA and a dielectric probe kit.</p>
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<p>Variation in measured electrical permittivity of the prepared samples shown at 1.5 GHz.</p>
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<p>Fabricated design connected to vector network analyzer (VNA) for experimental measurements.</p>
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<p>Measured transmission coefficient (<math display="inline"><semantics> <msub> <mi>S</mi> <mn>21</mn> </msub> </semantics></math>) when ethanol and methanol samples were investigated with prototype on Rogers RO4003C.</p>
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<p>Measured transmission coefficient (<math display="inline"><semantics> <msub> <mi>S</mi> <mn>21</mn> </msub> </semantics></math>) when ethanol and methanol samples were investigated with prototype on Rogers RT/Duroid 5880.</p>
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<p>Measuredtransmission coefficient (<math display="inline"><semantics> <msub> <mi>S</mi> <mn>21</mn> </msub> </semantics></math>) when ethanol, methanol, and hydrocortisone samples were investigated with prototype on PET substrate.</p>
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<p>Graph showing variation in resonant frequency with changes in concentration of organic solvents (ethanol and methanol) and content of hydrocortisone in samples investigated with PET substrate.</p>
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<p>Variation in resonant frequency with increase in the bending radius of the cylinder on which the proposed design was bent over PET flexible substrate.</p>
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13 pages, 4894 KiB  
Article
Self-Assembled TiN-Metal Nanocomposites Integrated on Flexible Mica Substrates towards Flexible Devices
by Juncheng Liu, Yizhi Zhang, Hongyi Dou, Benson Kunhung Tsai, Abhijeet Choudhury and Haiyan Wang
Sensors 2024, 24(15), 4863; https://doi.org/10.3390/s24154863 - 26 Jul 2024
Viewed by 948
Abstract
The integration of nanocomposite thin films with combined multifunctionalities on flexible substrates is desired for flexible device design and applications. For example, combined plasmonic and magnetic properties could lead to unique optical switchable magnetic devices and sensors. In this work, a multiphase TiN-Au-Ni [...] Read more.
The integration of nanocomposite thin films with combined multifunctionalities on flexible substrates is desired for flexible device design and applications. For example, combined plasmonic and magnetic properties could lead to unique optical switchable magnetic devices and sensors. In this work, a multiphase TiN-Au-Ni nanocomposite system with core–shell-like Au-Ni nanopillars embedded in a TiN matrix has been demonstrated on flexible mica substrates. The three-phase nanocomposite film has been compared with its single metal nanocomposite counterparts, i.e., TiN-Au and TiN-Ni. Magnetic measurement results suggest that both TiN-Au-Ni/mica and TiN-Ni/mica present room-temperature ferromagnetic property. Tunable plasmonic property has been achieved by varying the metallic component of the nanocomposite films. The cyclic bending test was performed to verify the property reliability of the flexible nanocomposite thin films upon bending. This work opens a new path for integrating complex nitride-based nanocomposite designs on mica towards multifunctional flexible nanodevice applications. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Conceptual drawing of the design of the work. TiN-based nanocomposite films with plasmonic Au pillars and ferromagnetic Ni pillars as well as core–shell-like pillars demonstrated on flexible mica substrates.</p>
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<p>XRD results of the TiN-Ni/mica, TiN-Au/mica, and TiN-Au-Ni/mica films. * stands for mica (001) peaks.</p>
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<p>Schematic drawings and cross-sectional STEM image as well as the corresponding EDS mappings for (<b>a</b>) TiN-Au/mica and (<b>b</b>) TiN-Ni/mica films.</p>
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<p>(<b>a</b>) Schematic drawing of TiN-Au-Ni/mica film. (<b>b</b>) Cross-sectional STEM image with (<b>c</b>–<b>f</b>) corresponding EDS mappings. (<b>g</b>) Cross-sectional TEM image. (<b>h</b>) Plan-view TEM image. (<b>i</b>) Plan-view STEM image, with (<b>j</b>–<b>m</b>) corresponding EDS mappings.</p>
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<p>IP and OP <span class="html-italic">M-H</span> curves for the (<b>a</b>) TiN-Au-Ni/mica and (<b>b</b>) TiN-Ni/mica film. (<b>c</b>) IP and (<b>d</b>) OP <span class="html-italic">M-H</span> curves for the TiN-Au-Ni/mica film after the bending test.</p>
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<p>(<b>a</b>) IP and (<b>b</b>) OP real permittivity of the TiN-Au/mica, TiN-Ni/mica, and TiN-Au-Ni/mica films. (<b>c</b>) Transmittance of the three films. (<b>d</b>) Transmittance of the TiN-Au-Ni/mica film at different bending statuses.</p>
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<p>Proposed device on a magnetic field enhancing the Raman signal using the TiN-Au-Ni VANs on mica.</p>
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11 pages, 3136 KiB  
Article
Understanding Diffusion in a Single-Metal Organic Framework Crystal Used for Sensing Applications
by Surya Cheemalapati, Karthik Konnaiyan, Yao Chen, Shengqian Ma and Anna Pyayt
Sensors 2024, 24(12), 3842; https://doi.org/10.3390/s24123842 - 14 Jun 2024
Viewed by 1084
Abstract
Metal–organic frameworks (MOFs) stand out as remarkable materials renowned for their exceptionally high surface area and large number of pores, making them invaluable for diverse sensing applications including gas, biomedical, chemical, and optical sensing. Traditional methods of molecule infusion and release often involve [...] Read more.
Metal–organic frameworks (MOFs) stand out as remarkable materials renowned for their exceptionally high surface area and large number of pores, making them invaluable for diverse sensing applications including gas, biomedical, chemical, and optical sensing. Traditional methods of molecule infusion and release often involve a large number of crystals with varying shapes and sizes, leading to averaged outcomes across a heterogeneous crystal population. In this study, we present continuous monitoring of the infusion and release dynamics of model drug molecules, specifically vitamin B12, within individual Tb-mesoMOF crystals. Our findings underscore the critical influence of crystal size and shape on the infusion and diffusion processes and corresponding color change, underscoring the necessity to account for these factors in the design of large-scale systems. Leveraging optical microscopy, we employed a histogram-based algorithm for image processing, enabling automated tracking of diffusion phenomena. This investigation offers crucial insights into the dynamics of these processes, laying the groundwork for optimizing parameters in future sensing systems. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>First step in image processing. Image (<b>b</b>) at is subtracted from initial image (<b>a</b>) to produce the differential image (<b>c</b>).</p>
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<p>Step 2 in image processing where RGB values of subtracted images are extracted.</p>
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<p>Optical and SEM characterization images of individual crystals of Tb-mesoMOF before infusion with vitamin B<sub>12</sub>: (<b>a</b>) Optical microscope image of the MOF; (<b>b</b>) SEM image of MOF and (<b>c</b>,<b>d</b>) are higher magnification parts of the crystal shown in (<b>b</b>).</p>
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<p>Optical microscopy and SEM characterization of vitamin B<sub>12</sub> uptake in Tb-mesoMOF: (<b>a</b>) Optical microscope image of a crystal infused with vitamin B<sub>12</sub> for a short period of time; (<b>b</b>) corresponding SEM image of the same crystal in the same orientation as in the optical microscopy image.</p>
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<p>Optical microscopy monitoring of dynamics of molecular vitamin B<sub>12</sub> uptake by individual Tb-mesoMOF crystals. (<b>Ia</b>,<b>IIa</b>,<b>IIIa</b>) are schematic representations of microscopy images taken at 20 min (<b>Ib</b>), 60 min (<b>IIb</b>), and 300 min (<b>IIIb</b>), respectively, and (<b>IV</b>) is an image taken at 780 min, during the final stages of uptake.</p>
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<p>Optical microscopy monitoring of dynamics of molecular vitamin B<sub>12</sub> uptake by individual Tb-mesoMOF crystals. Image (<b>Ia</b>,<b>Ib</b>) show uncut samples of MOF infused with vitamin B<sub>12</sub> for 10 min. (<b>IIa</b>) shows uncut, and (<b>IIb</b>) shows cut MOF crystals infused with vitamin B12 for 20 min. (<b>IIIa</b>) shows uncut, and (<b>IIIb</b>) shows cut MOF crystals infused with vitamin B<sub>12</sub> for 180 min. Here, the MOF looks red from outside, but the cut sample shows there is still vacant MOF. (<b>IVa</b>) shows uncut and (<b>IVb</b>) cut MOF crystals infused with vitamin B<sub>12</sub> for 780 min. Here, the MOF is completely infused.</p>
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<p>Optical microscopy characterization of vitamin B<sub>12</sub> release from an individual Tb-mesoMOF crystal. Images of the crystal infused with vitamin B<sub>12</sub> suspended in methanol, and vitamin B<sub>12</sub> diffusion out of the crystal at times (<b>a</b>) t = 15 min, (<b>b</b>) t= 30 min, (<b>c</b>) t = 60 min, (<b>d</b>) t = 100 min, (<b>e</b>) t = 200 min, (<b>f</b>) t = 300 min, (<b>g</b>) t = 500 min, (<b>h</b>) t = 1000 min, (<b>i</b>) 1600 min, (<b>j</b>) t = 2350 min, (<b>k</b>) t = 5000 min, and (<b>l</b>) t = 7000 min; (<b>m</b>) a plot demonstrating speed of release of the vitamin B<sub>12</sub> vs. time.</p>
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13 pages, 7223 KiB  
Article
Graphene Nanoplatelets/Polydimethylsiloxane Flexible Strain Sensor with Improved Sandwich Structure
by Junshu Zhang, Ke Gao, Shun Weng and Hongping Zhu
Sensors 2024, 24(9), 2856; https://doi.org/10.3390/s24092856 - 30 Apr 2024
Cited by 5 | Viewed by 1704
Abstract
In engineering measurements, metal foil strain gauges suffer from a limited range and low sensitivity, necessitating the development of flexible sensors to fill the gap. This paper presents a flexible, high-performance piezoresistive sensor using a composite consisting of graphene nanoplatelets (GNPs) and polydimethylsiloxane [...] Read more.
In engineering measurements, metal foil strain gauges suffer from a limited range and low sensitivity, necessitating the development of flexible sensors to fill the gap. This paper presents a flexible, high-performance piezoresistive sensor using a composite consisting of graphene nanoplatelets (GNPs) and polydimethylsiloxane (PDMS). The proposed sensor demonstrated a significantly wider range (97%) and higher gauge factor (GF) (6.3), effectively addressing the shortcomings of traditional strain gauges. The microstructure of the GNPs/PDMS composite was observed using a scanning electron microscope, and the distribution of the conductive network was analyzed. The mechanical behavior of the sensor encapsulation was analyzed, leading to the determination of the mechanisms influencing encapsulation. Experiments based on a standard equal-strength beam were conducted to investigate the influence of the base and coating dimensions of the sensor. The results indicated that reducing the base thickness and increasing the coating length both contributed to the enhancement of the sensor’s performance. These findings provide valuable guidance for future development and design of flexible sensors. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Fabrication process of the GNPs/PDMS nanocomposite.</p>
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<p>Photograph of the encapsulated GNPs/PDMS sensor: (<b>a</b>) front view; (<b>b</b>) cross-section.</p>
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<p>SEM image (<b>a</b>) Surface of 5 wt% GNPs (<b>b</b>) Surface of 4 wt% GNPs (<b>c</b>) Enlarged inset of the surface (<b>d</b>) Macrographic appearance of the cross-section (<b>e</b>) Cross-section of 5 wt% GNPs (<b>f</b>) Cross-section of 4 wt% GNPs (<b>g</b>) Enlarged inset of the cross-section (<b>h</b>) GNPs embedded in PDMS.</p>
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<p>Uniaxial tensile test results: (<b>a</b>) Force-displacement curve of the GNPs/PDMS sample; (<b>b</b>) Resistance-strain curve of the GNPs/PDMS sample.</p>
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<p>Dynamic stretch–release cycle response of the encapsulated GNPs/PDMS sensor for various strains from 5% to 20%: (<b>a</b>) Uniaxial cyclic tensile test of the sensor; (<b>b</b>) Resistance variation of the sensor in cyclic tensile test.</p>
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<p>Strain test system.</p>
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<p>Data from loading test: (<b>a</b>) Metal foil strain gauges; (<b>b</b>) Flexible strain sensors.</p>
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<p>Resistance variation for sensors with different base thickness.</p>
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<p>Sensors bonded with different coating length.</p>
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<p>Resistance variation for sensors with different coating length.</p>
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20 pages, 5895 KiB  
Article
Fabrications of the Flexible Non-Enzymatic Glucose Sensors Using Au-CuO-rGO and Au-CuO-rGO-MWCNTs Nanocomposites as Carriers
by Shu-Han Liao, Kai-Yi Shiau, Fang-Hsing Wang and Cheng-Fu Yang
Sensors 2023, 23(19), 8029; https://doi.org/10.3390/s23198029 - 22 Sep 2023
Cited by 6 | Viewed by 1689
Abstract
A flexible, non-enzymatic glucose sensor was developed and tested on a polyethylene terephthalate (PET) substrate. The sensor’s design involved printing Ag (silver) as the electrode and utilizing mixtures of either gold–copper oxide-modified reduced graphene oxide (Au-CuO-rGO) or gold–copper oxide-modified reduced graphene oxide-multi-walled carbon [...] Read more.
A flexible, non-enzymatic glucose sensor was developed and tested on a polyethylene terephthalate (PET) substrate. The sensor’s design involved printing Ag (silver) as the electrode and utilizing mixtures of either gold–copper oxide-modified reduced graphene oxide (Au-CuO-rGO) or gold–copper oxide-modified reduced graphene oxide-multi-walled carbon nanotubes (Au-CuO-rGO-MWCNTs) as the carrier materials. A one-pot synthesis method was employed to create a nanocomposite material, consisting of Au-CuO-rGO mixtures, which was then printed onto pre-prepared flexible electrodes. The impact of different weight ratios of MWCNTs (0~75 wt%) as a substitute for rGO was also investigated on the sensing characteristics of Au-CuO-rGO-MWCNTs glucose sensors. The fabricated electrodes underwent various material analyses, and their sensing properties for glucose in a glucose solution were measured using linear sweep voltammetry (LSV). The LSV measurement results showed that increasing the proportion of MWCNTs improved the sensor’s sensitivity for detecting low concentrations of glucose. However, it also led to a significant decrease in the upper detection limit for high-glucose concentrations. Remarkably, the research findings revealed that the electrode containing 60 wt% MWCNTs demonstrated excellent sensitivity and stability in detecting low concentrations of glucose. At the lowest concentration of 0.1 μM glucose, the nanocomposites with 75 wt% MWCNTs showed the highest oxidation peak current, approximately 5.9 μA. On the other hand, the electrode without addition of MWCNTs displayed the highest detection limit (approximately 1 mM) and an oxidation peak current of about 8.1 μA at 1 mM of glucose concentration. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Picture of the screen-printed electrodes.</p>
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<p>XRD diffraction patterns of (<b>a</b>) GO, (<b>b</b>) MWCNTs, and (<b>c</b>) Au-CuO-rGO and Au-CuO-40 wt% rGO-60 wt% MWCNTs.</p>
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<p>Surface SEM images of Au-CuO-rGO-MWCNTs with lower magnification for different wt% of MWCNTs (<b>a</b>) 0 wt%, (<b>b</b>) 15 wt%, (<b>c</b>) 30 wt%, and (<b>d</b>) 60 wt%. Surface SEM images of Au-CuO-rGO-MWCNTs with higher magnification are added in the inset of each image.</p>
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<p>Raman full spectrum for GO, MWCNTs, Au-CuO-rGO, and Au-CuO-40 wt% rGO-60 wt% MWCNTs.</p>
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<p>XPS analyses for (<b>a</b>) full spectrum of C1s peak spectrum, (<b>b</b>) GO, (<b>c</b>) MWCNTs, (<b>d</b>) Au-CuO-rGO, and (<b>e</b>) Au-CuO-40 wt% rGO-60 wt% MWCNTs.</p>
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<p>XPS analyses for O1s peak spectra of (<b>a</b>) GO, (<b>b</b>) MWCNTs, (<b>c</b>) Au-CuO-rGO, (<b>d</b>) Au-CuO-40 wt% rGO-60 wt% MWCNTs, and for (<b>e</b>) Cu 2p and (<b>f</b>) Au 4f.</p>
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<p>XPS analyses for O1s peak spectra of (<b>a</b>) GO, (<b>b</b>) MWCNTs, (<b>c</b>) Au-CuO-rGO, (<b>d</b>) Au-CuO-40 wt% rGO-60 wt% MWCNTs, and for (<b>e</b>) Cu 2p and (<b>f</b>) Au 4f.</p>
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<p>Glucose LSV measurements for samples with different proportions of MWCNTs, (<b>a</b>) 0 wt%, (<b>b</b>) 15 wt%, (<b>c</b>) 30 wt%, and (<b>d</b>) 60 wt%.</p>
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<p>Peak currents of the fabricated sensors measured at different glucose concentrations and with different proportions of MWCNTs. Ip: peak current.</p>
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<p>Linear characteristics of different sensors at different glucose concentrations (<b>a</b>) sample with Au-CuO-rGO as the sensor and in the range of 0.2 mM~1 mM, using Au-CuO-40 wt%rGO-60 wt% MWCNTs as the sensor and in the range of (<b>b</b>) 0.1 μM~1 μM and (<b>c</b>) 1 μM~10 μM. Ip: peak current.</p>
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<p>(<b>a</b>) Glucose selectivity of LSV measurements, (<b>b</b>) peak current comparison of different additives, and (<b>c</b>) Au-CuO-40 wt%rGO-60 wt% MWCNTs as the sensor for the measurements of NaOH (0.5 M) + glucose.</p>
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17 pages, 8837 KiB  
Article
Synthesis of ZnO Nanoflower Arrays on a Protrusion Sapphire Substrate and Application of Al-Decorated ZnO Nanoflower Matrix in Gas Sensors
by Xin Zhao, Jang-Cheng Jheng, Ni-Ni Chou, Fang-Hsing Wang and Cheng-Fu Yang
Sensors 2023, 23(12), 5629; https://doi.org/10.3390/s23125629 - 16 Jun 2023
Cited by 3 | Viewed by 1484
Abstract
In this study, we utilized a sapphire substrate with a matrix protrusion structure as a template. We employed a ZnO gel as a precursor and deposited it onto the substrate using the spin coating method. After undergoing six cycles of deposition and baking, [...] Read more.
In this study, we utilized a sapphire substrate with a matrix protrusion structure as a template. We employed a ZnO gel as a precursor and deposited it onto the substrate using the spin coating method. After undergoing six cycles of deposition and baking, a ZnO seed layer with a thickness of 170 nm was formed. Subsequently, we used a hydrothermal method to grow ZnO nanorods (NRs) on the aforementioned ZnO seed layer for different durations. ZnO NRs exhibited a uniform outward growth rate in various directions, resulting in a hexagonal and floral morphology when observed from above. This morphology was particularly evident in ZnO NRs synthesized for 30 and 45 min. Due to the protrusion structure of ZnO seed layer, the resulting ZnO nanorods (NRs) displayed a floral and matrix morphology on the protrusion ZnO seed layer. To further enhance their properties, we utilized Al nanomaterial to decorate the ZnO nanoflower matrix (NFM) using a deposition method. Subsequently, we fabricated devices using both undecorated and Al-decorated ZnO NFMs and deposited an upper electrode using an interdigital mask. We then compared the gas-sensing performance of these two types of sensors towards CO and H2 gases. The research findings indicate that sensors based on Al-decorated ZnO NFM exhibit superior gas-sensing properties compared to undecorated ZnO NFM for both CO and H2 gases. These Al-decorated sensors demonstrate faster response times and higher response rates during the sensing processes. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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Figure 1
<p>(<b>a</b>) Surface observation and (<b>b</b>) cross-sectional observation of protrusion sapphire substrate.</p>
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<p>Schematic diagram for the fabrication processes of an Al-decorated ZnO nanoroads gas sensor.</p>
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<p>(<b>a</b>) SEM images and (<b>b</b>) XRD pattern of ZnO film deposited on the protrusion sapphire substrate.</p>
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<p>SEM top view of synthesized ZnO nanoroads, (<b>a</b>) 30, (<b>b</b>) 45, and (<b>c</b>) 60 min.</p>
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<p>SEM cross-sectional of synthesized ZnO NRs, (<b>a</b>) 30, (<b>b</b>) 45, and (<b>c</b>) 60 min.</p>
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<p>XRD patterns of ZnO NRs synthesized on the sapphire protrusion substrate as the synthesis time of 30 and 60 min.</p>
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<p>TEM images taken on a single ZnO nanorod synthesized on the sapphire protrusion substrate as the synthesis time of 60 min. (<b>a</b>) high-resolution TEM micrograph and (<b>b</b>) electron diffraction pattern.</p>
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<p>PL spectrum of ZnO NFMs with (<b>a</b>) different synthesis times, (<b>b</b>) with a synthesis time of 60 min and the fitting results using the sum of four Gaussian functions, and (<b>c</b>) comparison of 60-min synthesized ZnO NFMs without and with Al decoration.</p>
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<p>The O<sub>1s</sub> peaks of ZnO NFMs using different synthesis time, (<b>a</b>) 30 min and (<b>b</b>) 60 min.</p>
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<p>Al-decorated (<b>a</b>) 30-, (<b>b</b>) 45-, and (<b>c</b>) 60-min synthesized ZnO NFMs.</p>
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<p>Dynamic analyses of 60 min-growth ZnO NFM gas sensor performed for (<b>a</b>) CO and (<b>b</b>) H<sub>2</sub> detections, including changes in resistance values and resistance responses.</p>
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<p>Dynamic analyses of Al-decorated 60 min-growth ZnO NFM gas sensors performed for (<b>a</b>) CO and (<b>b</b>) H<sub>2</sub> detections, including changes in resistance values and resistance responses.</p>
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19 pages, 5252 KiB  
Article
Investigating the Electromechanical Sensitivity of Carbon-Nanotube-Coated Microfibers
by Elizabeth Bellott, Yushan Li, Connor Gunter, Scott Kovaleski and Matthew R. Maschmann
Sensors 2023, 23(11), 5190; https://doi.org/10.3390/s23115190 - 30 May 2023
Viewed by 1485
Abstract
The piezoresistance of carbon nanotube (CNT)-coated microfibers is examined using diametric compression. Diverse CNT forest morphologies were studied by changing the CNT length, diameter, and areal density via synthesis time and fiber surface treatment prior to CNT synthesis. Large-diameter (30–60 nm) and relatively [...] Read more.
The piezoresistance of carbon nanotube (CNT)-coated microfibers is examined using diametric compression. Diverse CNT forest morphologies were studied by changing the CNT length, diameter, and areal density via synthesis time and fiber surface treatment prior to CNT synthesis. Large-diameter (30–60 nm) and relatively low-density CNTs were synthesized on as-received glass fibers. Small-diameter (5–30 nm) and-high density CNTs were synthesized on glass fibers coated with 10 nm of alumina. The CNT length was controlled by adjusting synthesis time. Electromechanical compression was performed by measuring the electrical resistance in the axial direction during diametric compression. Gauge factors exceeding three were measured for small-diameter (<25 μm) coated fibers, corresponding to as much as 35% resistance change per micrometer of compression. The gauge factor for high-density, small-diameter CNT forests was generally greater than those for low-density, large-diameter forests. A finite element simulation shows that the piezoresistive response originates from both the contact resistance and intrinsic resistance of the forest itself. The change in contact and intrinsic resistance are balanced for relatively short CNT forests, while the response is dominated by CNT electrode contact resistance for taller CNT forests. These results are expected to guide the design of piezoresistive flow and tactile sensors. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Floating catalyst chemical vapor deposition of CNT forests. (<b>a</b>) Schematic of floating catalyst CVD setup. (<b>b</b>) CNT forest synthesis conditions.</p>
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<p>Schematic of the electromechanical test setup. The interdigitated electrode substrate resided with a nanoindenter. A 100 μm flat tip diametrically compressed a CNT-forest-coated fiber onto the patterned substrate while the electrical resistance was measured using a digital multimeter.</p>
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<p>SEM micrographs of CNT-forest-coated glass fibers. (<b>a</b>,<b>b</b>) Alumina-coated glass fibers. (<b>c</b>,<b>d</b>) As-received glass fiber substrates. Inset images in (<b>b</b>,<b>d</b>) show histograms of CNT outer diameters measured by SEM.</p>
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<p>SEM images of CNT-forest-coated microfibers. (<b>a</b>) Large-diameter CNT forests exhibit CNT banding instead of a continuous conformal coating. While most fibers exhibit two or more preferred bands, (<b>b</b>) some CNT forests collapse into a single band. The schematic in (<b>b</b>) demonstrates the position of the fiber (blue) relative to the CNT forest. (<b>c</b>) High magnification image shows catalyst nanoparticles on the glass fiber substrate and CNTs separated from the catalyst.</p>
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<p>Electromechanical indentation data from diametrically compressed CNT-forest-coated glass microfibers. (<b>a</b>) Optical image of CNT-coated fiber tested in (<b>b</b>,<b>c</b>). (<b>b</b>) Mechanical and (<b>c</b>) simultaneous electrical data from a 12 μm diameter CNT forest grown from an alumina-coated glass fiber. (<b>d</b>) Optical image of CNT-coated fiber tested in (<b>e</b>,<b>f</b>). (<b>e</b>) Mechanical and (<b>f</b>) simultaneous electrical data from a 60 μm diameter CNT forest grown from an alumina-coated glass fiber.</p>
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<p>Sensitivity of CNT-forest-coated glass fibers. (<b>a</b>) Gauge factor and (<b>b</b>) sensitivity of CNT forests grown on alumina-coated and as-received glass fibers. The gauge factor is computed with respect to diametric compression. (<b>c</b>) The initial resistance of CNT-coated fibers is inversely related to the fiber diameter.</p>
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<p>Simulated CNT morphology as a function of synthesis attributes after 600 growth time steps. The attribute combinations include (<b>a</b>) 3 × 10<sup>9</sup> CNT/cm<sup>2</sup>, 40 nm O.D., 34 nm I.D. CNT diameter, 0.1 nN force to break CNT–CNT bonds, (<b>b</b>) 3 × 10<sup>9</sup> CNT/cm<sup>2</sup>, 40 nm O.D., 20 nm I.D. CNT diameter, 1 nN force to break CNT–CNT bonds, (<b>c</b>) 3 × 10<sup>10</sup> CNT/cm<sup>2</sup>, 5 nm CNT diameter, 10 nN force to break CNT–CNT bonds. (<b>d</b>) A time evolution shows the formation of a single band using the attributes of 3 × 10<sup>10</sup> CNT/cm<sup>2</sup>, 5 nm CNT diameter, 1 nN force to break CNT–CNT bonds. Note that the formation of different band structures is stochastic in nature. One set of synthesis attributes will not ensure one specific type of band structure.</p>
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<p>Schematic of a simulated CNT forest for compression (<b>left</b>) and the electromechanical compression of the same forest (<b>right</b>). The colors within the compressed forest represent voltage.</p>
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<p>Simulated electromechanical response of compressed CNT forests as a function of compressive displacement. Panels (<b>a</b>–<b>c</b>) represent simulations with 10 nm outer diameters, and areal density 3 × 10<sup>10</sup> CNT/cm<sup>2</sup>, to simulate the CNT forests synthesized from alumina-coated fibers. Panels (<b>d</b>–<b>f</b>) represent CNT forests in which the CNT outer diameter is 40 nm and CNT areal density is 3 × 10<sup>9</sup> CNT/cm<sup>2</sup> to simulate the CNT forests synthesized from as-received glass fibers. The legend represents the height of the CNT forest before compression. Panels (<b>a</b>,<b>d</b>) display the total electrical resistance through the CNT forests between the measurement electrodes. Panels (<b>b</b>,<b>e</b>) display the electrical contact resistance established between CNTs and the electrode surfaces. Panels (<b>c</b>,<b>f</b>) display the intrinsic internal resistance within the CNT forest obtained by setting the voltage of nodes in contact with an electrode equal to the voltage of the electrode.</p>
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<p>Simulated CNT forest conductance as a function of the quantity of (<b>a</b>,<b>b</b>) CNT–electrode contacts, and (<b>c</b>,<b>d</b>) CNT–CNT contacts. Panels (<b>a</b>,<b>c</b>) represent CNT forests in which the CNT outer diameter is 10 nm and CNT areal density is 3 × 10<sup>10</sup> CNT/cm<sup>2</sup> to simulate the CNT forests synthesized from alumina-coated fibers. Panels (<b>b</b>,<b>d</b>) represent CNT forests in which the CNT outer diameter is 40 nm and CNT areal density is 3 × 10<sup>9</sup> CNT/cm<sup>2</sup> to simulate the CNT forests synthesized from as-received glass fibers. The legend represents the height of the CNT forest before compression.</p>
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<p>The quantity of CNT–electrode and CNT–CNT contacts as a function of compressive displacement for (<b>a</b>) 40 nm O.D., 3 × 10<sup>9</sup> CNT/cm<sup>2</sup> CNT forest and (<b>b</b>) 10 nm O.D., 3 × 10<sup>10</sup> CNT/cm<sup>2</sup> CNT forest. The discretely plotted points represent CNT–electrode contacts, while the continuous lines represent CNT–CNT contacts.</p>
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13 pages, 5057 KiB  
Article
The Accumulation of Electrical Energy Due to the Quantum-Dimensional Effects and Quantum Amplification of Sensor Sensitivity in a Nanoporous SiO2 Matrix Filled with Synthetic Fulvic Acid
by Vitalii Maksymych, Dariusz Calus, Bohdan Seredyuk, Glib Baryshnikov, Rostislav Galagan, Valentina Litvin, Sławomir Bujnowski, Piotr Domanowski, Piotr Chabecki and Fedir Ivashchyshyn
Sensors 2023, 23(8), 4161; https://doi.org/10.3390/s23084161 - 21 Apr 2023
Viewed by 1689
Abstract
A heterostructured nanocomposite MCM-41<SFA> was formed using the encapsulation method, where a silicon dioxide matrix—MCM-41 was the host matrix and synthetic fulvic acid was the organic guest. Using the method of nitrogen sorption/desorption, a high degree of monoporosity in the studied matrix was [...] Read more.
A heterostructured nanocomposite MCM-41<SFA> was formed using the encapsulation method, where a silicon dioxide matrix—MCM-41 was the host matrix and synthetic fulvic acid was the organic guest. Using the method of nitrogen sorption/desorption, a high degree of monoporosity in the studied matrix was established, with a maximum for the distribution of its pores with radii of 1.42 nm. According to the results of an X-ray structural analysis, both the matrix and the encapsulate were characterized by an amorphous structure, and the absence of a manifestation of the guest component could be caused by its nanodispersity. The electrical, conductive, and polarization properties of the encapsulate were studied with impedance spectroscopy. The nature of the changes in the frequency behavior of the impedance, dielectric permittivity, and tangent of the dielectric loss angle under normal conditions, in a constant magnetic field, and under illumination, was established. The obtained results indicated the manifestation of photo- and magneto-resistive and capacitive effects. In the studied encapsulate, the combination of a high value of ε and a value of the tgδ of less than 1 in the low-frequency range was achieved, which is a prerequisite for the realization of a quantum electric energy storage device. A confirmation of the possibility of accumulating an electric charge was obtained by measuring the I-V characteristic, which took on a hysteresis behavior. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Distribution of pores in MSM-41 according to the adsorption branch of the isotherm, according to the BET method.</p>
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<p>XRD diffraction patterns of: (1) MSM-41 matrices, and (2) MSM-41&lt;SFA encapsulate.</p>
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<p>Frequency dependences of the real component of the specific impedance of the matrix MSM-41 (1) and encapsulate MSM-41&lt;SFA&gt;, measured under normal conditions (2), in a magnetic field (3), and under illumination (4).</p>
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<p>Thermally stimulated discharge currents for MSM-41&lt;SFA&gt; encapsulation.</p>
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<p>Nyquist diagrams measured for the matrix MSM-41 (1) and encapsulate MSM-41&lt;SFA&gt; under normal conditions (2), in a magnetic field (3), and under illumination (4).</p>
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<p>Frequency dependences of the dielectric constants of the matrix MSM-41 (1) and encapsulate MSM-41&lt;SFA&gt;, measured under normal conditions (2), in a magnetic field (3), and under illumination (4).</p>
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<p>Frequency dependences of the tangent angles of dielectric losses of the matrix MSM-41 (1) and encapsulate MSM-41&lt;SFA&gt;, measured under normal conditions (2), in a magnetic field (3), and under illumination (4).</p>
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<p>I-V curves of encapsulate MSM-41&lt;SFA&gt;, measured under normal conditions (1), in a magnetic field (2), and under illumination (3).</p>
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13 pages, 5394 KiB  
Article
The 0-3 Lead Zirconate-Titanate (PZT)/Polyvinyl-Butyral (PVB) Composite for Tactile Sensing
by Eun-Bee Jo, Yoon-A Lee, Yoon-A Cho, Paul A. Günther, Sylvia E. Gebhardt, Holger Neubert and Hyun-Seok Kim
Sensors 2023, 23(3), 1649; https://doi.org/10.3390/s23031649 - 2 Feb 2023
Cited by 7 | Viewed by 3253
Abstract
In this study, a 0-3 piezoelectric composite based on lead zirconate-titanate (PZT)/polyvinyl-butyral (PVB) was fabricated and characterized for its potential application in tactile sensing. The 0-3 composite was developed to incorporate the advantages of both ceramic and polymer. The paste of 0-3 PZT–PVB [...] Read more.
In this study, a 0-3 piezoelectric composite based on lead zirconate-titanate (PZT)/polyvinyl-butyral (PVB) was fabricated and characterized for its potential application in tactile sensing. The 0-3 composite was developed to incorporate the advantages of both ceramic and polymer. The paste of 0-3 PZT–PVB composite was printed using a conventional screen-printing technique on alumina and mylar substrates. The thickness of the prepared composite was approximately 80 μm. After printing the top electrode of the silver paste, 10 kV/mm of DC field was applied at 25 °C, 120 °C, and 150 °C for 10 min to align the electric dipoles in the composite. The piezoelectric charge coefficient of d33 and the piezoelectric voltage coefficient of g33 were improved by increasing the temperature of the poling process. The maximum values of d33 and g33 were 14.3 pC/N and 44.2 mV·m/N, respectively, at 150 °C. The sensor’s sensitivity to the impact force was measured by a ball drop test. The sensors showed a linear behavior in the output voltage with increasing impact force. The sensitivity of the sensor on the alumina and mylar substrates was 1.368 V/N and 0.815 V/N, respectively. The rising time of the sensor to the finger touch was 43 ms on the alumina substrate and 35 ms on the mylar substrate. Consequently, the high sensitivity and fast response time of the sensor make the 0-3 PZT–PVB composite a good candidate for tactile sensors. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Field emission scanning electron microscopy images: (<b>a</b>) PZT particles; (<b>b</b>) 0-3 PZT–PVB composite.</p>
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<p>(<b>a</b>) Schematic of the screen-printing process; (<b>b</b>) microscope image of the screen-printed sensor (left) and schematic of sensor’s structure (right).</p>
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<p>P–E hysteresis loops for 0-3 PZT–PVB composite: (<b>a</b>) 4 kV/mm, 8 kV/mm, 10 kV/mm, and 12 kV/mm for 1 cycle; (<b>b</b>) 12 kV/mm for a continuous 10 cycles.</p>
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<p>Piezoelectric charge coefficient <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mrow> <mn>33</mn> </mrow> </msub> </mrow> </semantics></math> of poled PZT–PVB composites versus poling temperature with various diameters of the electrodes: (<b>a</b>) alumina substrate; (<b>b</b>) mylar substrate.</p>
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<p>Piezoelectric voltage coefficient <math display="inline"><semantics> <mrow> <msub> <mi>g</mi> <mrow> <mn>33</mn> </mrow> </msub> </mrow> </semantics></math> of poled PZT–PVB composites versus poling temperature with various diameters of the electrodes: (<b>a</b>) alumina substrate; (<b>b</b>) mylar substrate.</p>
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<p>Distribution of the piezoelectric charge coefficient <math display="inline"><semantics> <mrow> <msub> <mi>d</mi> <mrow> <mn>33</mn> </mrow> </msub> </mrow> </semantics></math> of the PZT–PVB composites poled at 150 °C on the mylar substrate with various diameters of the electrodes.</p>
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<p>Ball drop test experimental setup for measuring the response of the PZT–PVB composite to impact force.</p>
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<p>Theoretically calculated impact force (<math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mrow> <mi>i</mi> <mi>m</mi> <mi>p</mi> <mi>a</mi> <mi>c</mi> <mi>t</mi> </mrow> </msub> </mrow> </semantics></math>), velocity of impact (<math display="inline"><semantics> <mrow> <msub> <mi>v</mi> <mrow> <mi>i</mi> <mi>m</mi> <mi>p</mi> <mi>a</mi> <mi>c</mi> <mi>t</mi> </mrow> </msub> </mrow> </semantics></math>), and potential energy: (<b>a</b>) impact force and velocity of impact as a function of drop height; (<b>b</b>) impact force and potential energy as a function of drop height.</p>
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<p>Comparison of impact force on the alumina and mylar substrates: (<b>a</b>) maximum voltage response as a function of height; (<b>b</b>) calibration curve of sensitivity of the sensor.</p>
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<p>Output voltage and response time (inset: rising time and falling time) of the 0-3 PZT–PVB composite sensor to finger touch: (<b>a</b>) alumina substrate; (<b>b</b>) mylar substrate.</p>
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10 pages, 5050 KiB  
Article
Comparison of Characteristics of a ZnO Gas Sensor Using a Low-Dimensional Carbon Allotrope
by Jihoon Lee, Jaebum Park and Jeung-Soo Huh
Sensors 2023, 23(1), 52; https://doi.org/10.3390/s23010052 - 21 Dec 2022
Cited by 1 | Viewed by 1766
Abstract
Owing to the increasing construction of new buildings, the increase in the emission of formaldehyde and volatile organic compounds, which are emitted as indoor air pollutants, is causing adverse effects on the human body, including life-threatening diseases such as cancer. A gas sensor [...] Read more.
Owing to the increasing construction of new buildings, the increase in the emission of formaldehyde and volatile organic compounds, which are emitted as indoor air pollutants, is causing adverse effects on the human body, including life-threatening diseases such as cancer. A gas sensor was fabricated and used to measure and monitor this phenomenon. An alumina substrate with Au, Pt, and Zn layers formed on the electrode was used for the gas sensor fabrication, which was then classified into two types, A and B, representing the graphene spin coating before and after the heat treatment, respectively. Ultrasonication was performed in a 0.01 M aqueous solution, and the variation in the sensing accuracy of the target gas with the operating temperature and conditions was investigated. As a result, compared to the ZnO sensor showing excellent sensing characteristics at 350 °C, it exhibited excellent sensing characteristics even at a low temperature of 150 °C, 200 °C, and 250 °C. Full article
(This article belongs to the Special Issue Functional Nanomaterials in Sensing)
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<p>Configuration diagram of the sensor substrate (<b>a</b>) front side (<b>b</b>) rear side.</p>
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<p>Manufacturing process for the type A and type B sensors.</p>
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<p>Schematic of the type A and type B sensors.</p>
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<p>Process for determining the sensing characteristics at ppb levels of the target gas.</p>
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<p>FE-SEM image of samples (<b>a</b>) type A (<b>b</b>) type B.</p>
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<p>XRD patterns for the type A and type B samples. Patterns show Al<sub>2</sub>O<sub>3</sub> (♠), Au (★), ZnO (●), C (■), and Pt (▲), and the components indicated by each peak are shown.</p>
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<p>Raman analysis results for type A samples.</p>
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<p>Raman analysis results for type B samples.</p>
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<p>Sensitivity and recovery at different operating temperatures for formaldehyde in the ppb range for the type A sensor.</p>
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<p>Sensitivity and recovery at different operating temperatures for formaldehyde in the ppb range for the type B sensor.</p>
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<p>Comparison of sensitivity and recovery to formaldehyde at 200 °C between low-dimensional allotrope modified ZnO sensor (type A and type B) and ZnO sensor.</p>
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<p>Sensitivity and recovery at different operating temperatures for toluene in the ppb range for the type A sensor.</p>
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<p>Sensitivity and recovery at different operating temperatures for toluene in the ppb range for the type B sensor.</p>
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