Dang Thi Thanh Leab,
Vu Anh Tuanab,
Matteo Tonezzer*cd,
Chu Manh Hung
ab and
Nguyen Duc Hoa
*ab
aFaculty of Electronic Materials and Devices, School of Materials Science and Engineering (SMSE), Hanoi University of Science and Technology (HUST), No. 1, Dai Co Viet Str., Hanoi, 100000, Vietnam
bInternational Training Institute for Materials Science (ITIMS), Hanoi University of Science and Technology (HUST), No. 1, Dai Co Viet Str., Hanoi, 100000, Vietnam. E-mail: ndhoa@itims.edu.vn
cDepartment of Chemical and Geological Sciences, University of Cagliari, Campus of Monserrato (CA), Monserrato, I09042, Italy. E-mail: matteo.tonezzer@unica.it
dCenter Agriculture Food Environment, University of Trento/Fondazione Edmund Mach, Via E. Mach 1, San Michele all'Adige, 38010, Italy
First published on 9th May 2025
Cobalt oxide nanofibers (Co3O4 NFs) were synthesized using a two-step procedure involving electrospinning followed by calcination. The microstructural, morphological, and elemental properties of the nanofibers were characterized using X-ray diffraction (XRD), transmission electron microscopy (TEM), scanning electron microscopy (SEM), and energy-dispersive spectrometry (EDS). The Co3O4 NFs exhibited high structural integrity, chemical purity, and uniform diameters ranging from 20 to 50 nm. Thermal treatment at 600 °C for 3 hours transformed the electrospun fibers into elongated nanofibers composed of interconnected Co3O4 nanoparticles. The gas sensing properties of the Co3O4 NFs were evaluated for ethanol (C2H5OH) detection over a temperature range of 250 to 450 °C. The sensor demonstrated a significant response to ethanol, highlighting their potential for gas sensing applications. When employed as a thermal electronic nose, the device achieved perfect classification (100% accuracy) for six tested gases and demonstrated effective concentration estimation, with an average error of 28.6%.
Spinel cobalt oxide (Co3O4) is a mixed-valence compound comprising CoO and Co2O3 phases, exhibiting p-type semiconducting behavior with high oxygen content. It has been extensively studied for various applications, including energy storage,4 catalysis,5 sensor technology,6 and electrochemical systems.7 Co3O4 exhibits outstanding catalytic performance, characterized by high activity, durability, and stability across a range of environmentally relevant applications. Additionally, Co3O4 features diverse morphological structures, a high concentration of surface oxygen species, and excellent structural stability, rendering it a highly effective material for gas sensing applications. The gas sensing capabilities of Co3O4 are well-documented, with its sensing mechanism primarily relying on surface catalytic interactions. Recent studies reported that Co3O4-based gas sensors typically require high operational temperatures, exceeding 200 °C, to achieve optimal performance due to improved catalytic properties and high oxygen content.8–11 Thus in this study, we tested the sensors in the temperature range from 250 to 450 °C.
Ethanol, a volatile and flammable compound, has a lower and upper explosion limit of 3.3% and 19% in air, respectively, posing risks in industrial and domestic environments.12,13 Prolonged exposure to ethanol vapor can lead to intoxication, neurological damage, and other health issues. As a result, there is a growing need for advanced ethanol gas sensor for industrial safety and everyday applications.
One-dimensional (1D) nanostructures offer significant advantages for gas sensing properties due to their ability to confine charge carriers transport along a single axis, enhancing charge mobility and sensitivity. Additionally, hollow nanostructures adsorption and desorption kinetics, reducing response and recovery times. For instance, Y. Zhang et al. demonstrated that electrospun LaFeO3 nanotubes exhibited enhanced ethanol sensing performance with faster response and recovery times.14
Various methods, including thermal evaporation, self-catalytic growth, hydrothermal synthesis, and electrospinning, have been employed to produce 1D nanomaterials.15 Among these, electrospinning particularly attractive due to its simplicity and ability to grow nanomaterials with high length-to-diameter ratios, promoting efficient electron transport.16
In this study, Co3O4 nanofibers (NFs) were synthesized via electrospinning and characterized using scanning electron microscopy (SEM), X-ray diffraction (XRD), transmission electron microscopy (TEM), and energy-dispersive X-ray spectroscopy (EDS). The gas-sensing performance of the Co3O4 NFs was evaluated for ethanol detection, demonstrating a strong response, indicating their potential for gas sensing applications. The importance of this work is supported by its ability to accurately discriminate and quantify different gases using a single Co3O4 nanofiber sensor in a thermal electronic nose system. This functionality, combined with the relative simplicity of the electrospinning fabrication process, makes these Co3O4 nanofibers promising candidates for the development of high-performance ethanol sensors and compact electronic noses with reliable classification and quantification capabilities for a wide range of gases.
The synthesized nanofibers underwent detailed morphological, structural and compositional characterizations. X-ray diffraction (XRD) analysis was performed using a Bruker D5005 diffractometer equipped with CuKα1 radiation (λ = 1.5406 Å), operating at 40 kV and 40 mA, to confirm the crystal structure. High-resolution scanning electron microscopy (SEM) and transmission electron microscopy (TEM) was respectively conducted using a Hitachi-S4800 and a JEOL 2100 microscope at voltage of 5 kV and 200 kV to analyze surface morphology, while elemental composition was determined via energy-dispersive spectroscopy (EDS) on the SEM instrument. Thermal properties were evaluated using thermogravimetric analysis (TGA) differential thermal analysis (DTA) with a Linseis TGA 1000 thermal analyzer. The measurements were conducted under ambient air conditions over a temperature range of 26–950 °C, with a heating rate of 2 °C min−1, to assess the material's thermal stability and decomposition behavior.
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Fig. 2 FESEM images of as-prepared Co(NO3)2/PVA composite nanofibers: (A) low magnification and (B) high magnification. |
The morphological changes induced by annealing were analyzed through SEM imaging, as shown in Fig. 3. After annealing at 600 °C, the Co3O4 nanofibers maintained their spiderweb arrangement, with lengths extending to several tens of microns (Fig. 3A). The average diameter, however, decreased to approximately 100–200 nm, attributed to the thermal decomposition of polyvinyl alcohol and the transformation of precursor fibers into crystalline Co3O4 nanofibers.
The calcination process was further examined using differential thermal analysis (DTA) and thermal gravimetric analysis (TGA), with results presented in Fig. 4. The TGA curve revealed distinct weight loss stages:
• Initial stage (up to 220 °C): a weight loss of ∼30%, attributed to the evaporation of low boiling points components, such as residual water.18
• Intermediate stage (220–340 °C): a slower weight loss (∼18%), associated with the decomposition of Co(NO3)2 and intermolecular cross-linking reactions.19–21 Concurrently, the degradation of PVA's side chains and the loss of –OH groups resulted in the formation of conjugated and non-conjugated polyenes.15–17
• Final stage (350–470 °C): a substantial weight loss (∼40%), with an endothermic peak at 370 °C, due to carbon oxidation and the complete decomposition of residual PVA structures.22
The elemental composition of the annealed nanofibers was examined using energy dispersive spectroscopy (EDS) and elemental mapping, as illustrated in Fig. 5. The EDS elemental spectrum confirmed the presence of cobalt (Co) and oxygen (O), with silicon (Si) originating from the Si/SiO2 substrate (Fig. 5B). Elemental mapping further demonstrated the homogeneous distribution of Co and O within the nanofibers (Fig. 5C–E).
X-ray diffraction analysis (Fig. 6) identified six distinct peaks corresponding to the cubic spinel phase of Co3O4, indexed to crystalline planes (220), (311), (400), (422), (511), and (440) (JCPDS 042-1467).23 The absence of peaks related to impurities or amorphous phases confirmed the high crystallinity of the synthesized material.
Transmission electron microscopy provided further insights into the microstructure of the Co3O4 nanofibers (Fig. 7). Low-magnification TEM images (Fig. 7A) revealed a spiderweb-like structure with fiber diameters ranging from 20 to 200 nm, while high-magnification TEM images (Fig. 7B) highlighted the presence of interconnected nanoparticles (3–10 nm), forming a porous architecture. These results demonstrate the successful formation of stable Co3O4 nanofibers with a consistent morphology.
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Fig. 7 TEM micrographs featuring the microstructure of annealed In2O3 polycrystalline nanofibers at varying levels of magnification: (A) lower magnification view and (B) higher magnification view. |
The relationship between sensor response gas and ethanol concentration at different temperatures is presented in Fig. 8B. The sensor response increased with ethanol concentration, exhibiting a rapid rise at lower concentrations (up to 125 ppm) before transitioning to a more linear trend, likely due to surface saturation effects. The optimal operating temperature was identified as 450 °C, at which the sensor achieved responses of 1.12, 1.18, 1.23, 1.25, 1.31 and 1.39 for concentrations of 25, 50, 100, 125, 250, and 500 ppm, respectively.
When ethanol is introduced, it reacts with the adsorbed oxygen species, releasing trapped electrons back into the material where they recombine with holes. This reduces holes concentration, thereby increasing resistance.
The presence of oxygen defects in Co3O4 nanofibers plays a pivotal role in enhancing their gas-sensing capabilities, particularly for ethanol detection. Oxygen defects act as active sites for gas adsorption, significantly influencing the sensor's surface chemistry. When ethanol molecules interact with the sensor's surface, oxygen defects facilitate the adsorption and subsequent catalytic oxidation of ethanol. This reaction leads to a change in surface resistance, which is the primary sensing mechanism for Co3O4-based gas sensors. Specifically, the oxygen vacancies enhance the material's ability to chemisorb oxygen molecules from the air, which are then ionized into reactive oxygen species such as O− or O2−.24,25 These species participate in the redox reactions with ethanol, releasing electrons back into the conduction band, thereby modulating the sensor's electrical resistance.
Moreover, oxygen defects also impact the electron–hole recombination process. By trapping free electrons, oxygen vacancies prolong the lifetime of photogenerated charge carriers, which is critical for maintaining a high level of sensitivity. This mechanism ensures a more pronounced and stable change in resistance upon ethanol exposure, improving the signal-to-noise ratio and the overall performance of the sensor. Furthermore, the enhanced charge carrier dynamics associated with oxygen vacancies contribute to a lower operating temperature, reducing energy consumption and making the sensor more efficient.
To benchmark the performance of the Co3O4 nanofibers sensor, a comparative analysis with recent studies was conducted (Table 1). The results indicate that the Co3O4 nanofibers synthesized via electrospinning exhibit good ethanol sensing, achieving a response of 1.39 at 500 ppm and 450 °C. This compares favorably to other Co3O4-based sensors produced using methods such as hydrothermal synthesis and wet chemical routes.23,26
Material | Method | T (°C) | C2H5OH conc. (ppm) | Response | Ref. (year) |
---|---|---|---|---|---|
Co3O4–Pt nanorods | Hydrothermal | 250 | 100 | 1.35 | 23 (2023) |
Co3O4 nanodisks | Hydrothermal | 175 | 100 | 94% | 26 (2023) |
Au@Co3O4 core–shell nanoparticles | Wet chemical | 250 | 2 | 1.7 | 27 (2022) |
Co3O4–MoTe2 nanocomposite | Wet chemical | 25 | 1 | 10% | 28 (2022) |
Co3O4nanofibers | Electrospinning | 450 | 500 | 1.39 | This work |
Fig. 9 shows a principal component analysis (PCA) plot, showing the first three principal components that together account for 99.7% of the total variance. Despite the dimensional reduction, the data points corresponding to different gases are well-separated, indicating effective discrimination. Moreover, points for each gas lie along distinct lines rather than clusters, with points at the top of the graph representing low concentrations and points further down indicating higher concentrations.
The classification of the gases was carried out using linear discriminant analysis (LDA), with the results summarized in Table 2.
Pred./True | C2H5OH | C6H15N | CH3COCH3 | H2 | H2S | NH3 |
---|---|---|---|---|---|---|
C2H5OH | 5 | |||||
C6H15N | 5 | |||||
CH3COCH3 | 5 | |||||
H2 | 5 | |||||
H2S | 5 | |||||
NH3 | 5 |
The analysis achieved perfect classification, with no misclassifications across 30 measurements, yielding an accuracy of 100.0%.
Once individual gases were identified, their concentrations were estimated using six different support vector regressors (SVRs), one for each gas. The regression results are shown in Fig. 10, which compares estimated gas concentrations against true concentrations.
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Fig. 10 Estimate of the gas concentration as a function of the true gas concentration for the tested gases. |
The data points lie close to the diagonal, indicating strong quantification performance. The error on the concentration estimate varies from gas to gas, and is reported in the boxes of Fig. 10. The electronic nose works relatively well for acetone, hydrogen sulfide and triethylamine, since it must be considered that the gas concentration spans many orders of magnitude (if the electronic nose estimates 2 ppm, there is the certainty that the true concentration is between 1 and 4 ppm, and not ppb). With hydrogen, ethanol and ammonia the electronic nose works very well, with an error ranging from 21.5 to 12.4%. The ability to accurately distinguish different gases and estimate their concentration is beyond the normal performance of a chemoresistive gas sensor, and is only possible with the thermal electronic nose approach.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ra00873e |
This journal is © The Royal Society of Chemistry 2025 |