Literature DB >> 29495469

Carbon Nitride Decorated Ball-Flower like Co₃O₄ Hybrid Composite: Hydrothermal Synthesis and Ethanol Gas Sensing Application.

Yuxiao Gong1, Yan Wang2,3, Guang Sun4, Tiekun Jia5, Lei Jia6, Fengmei Zhang7, Long Lin8, Baoqing Zhang9, Jianliang Cao10, Zhanying Zhang11.   

Abstract

Recently, semiconducting metal oxide (SMO) gas sensors have attracted the attention of researchers for high conductivity, labile features by environment, low cost, easy preparation, etc. However, traditional SMOs have some defects such as higher operating temperature and lower response value, which greatly limit their application in the field of gas sensor. In this work, the carbon nitride decorated ball-flower like Co₃O₄ composite was successfully synthesized via a facile hydrothermal method, the composition and morphology of the as-synthesized samples were studied by the techniques of X-ray powder diffraction (XRD), Field-emission scanning electron microscopy (FESEM), Transmission electron microscopy (TEM), Fourier transform infrared spectrometer (FT-IR) and N₂-sorption. As a consequence, the pure Co₃O₄ and the carbon nitride decorated Co₃O₄ both possess ball-flower like structure, and the as-synthesized carbon nitride decorated Co₃O₄ composite exhibits significant sensing properties to ethanol which is 1.6 times higher than that of pure Co₃O₄, furthermore, the composite possesses high selectivity and stability towards ethanol detection.

Entities:  

Keywords:  ball-flower like Co3O4; carbon nitride; ethanol; gas sensor; nanocomposites

Year:  2018        PMID: 29495469      PMCID: PMC5869623          DOI: 10.3390/nano8030132

Source DB:  PubMed          Journal:  Nanomaterials (Basel)        ISSN: 2079-4991            Impact factor:   5.076


1. Introduction

In the last decade, with the prosperity of the decoration market, “paint” has been widely concerning due to the harmful, volatile organic compound (VOC) that it produces. In the present study, noble metals (Au, Ag) are sensitive to gas, but they have high price, poor stability [1] (for the increasing particles affected by light, humidity, the accumulating carbonate on the surface of Au particles) and a short lifetime, making their application in gas sensors difficult to apply in industrial production and daily life. Thus, SMOs are widely researched and applied in the gas sensor to detect hazardous and toxic gases owing to their high conductivity, labile features by environment, low cost, and easy preparation, for instance, the ZnO [2,3], SnO2 [4,5], CuO [6], Co3O4 [7,8], α-Fe2O3 [9], NiO [10], In2O3 [11], and WO3 [12,13]. SMOs have defects, such as high operating temperature, low sensitivity, and poor selectivity. The key to improving the response and operating temperature of gas sensors is selecting suitable material and modifying traditional SMOs. In general, Co3O4 is an important p-type semiconductor with rich oxygen content, and is widely used in fields such as lithium-ion batteries, catalysts, and supercapacitors [14]. The researchers also apply Co3O4 in the field of gas sensors due to its good chemical stability and high specific surface area. For example, Patil et al. reported that Co3O4 nanorods had high sensitivity and fast response to CO [15]. Li et al. showed that Co3O4 nanotubes possess the property of high response to H2 and C2H5OH [7]. Hoa Nguyen et al. synthesized the porous Co3O4 nanorods, which showed good stability, fast response and recovery time when it was used as the gas sensor [8]. Researchers synthesized Co3O4 with other negative ions or metal oxides. Davide et al. improved p-type sensing materials by fluorine-doped Co3O4 nanosystems, thereby enhancing reversibility and lowering the working temperature [16]. Zhang et al. synthesized acicular nanowire of TiO2 decorated Co3O4 with high response and low operating temperature [17]. Recently, two-dimensional (2D) nanomaterials have constituted an important domain of nanostructures and were widely used in the field of gas sensors, due to their high specific surface area, unique electronic structure and excellent chemical inertness [18,19,20,21]. Wang et al. synthesized holey reduced graphene oxide nanosheets with high sensor response and reversible sensing for NH3 detection [22]. Cao et al. improved sensing properties through g-C3N4 nanosheets decorated SnO2 composites toward ethanol gas [23]. Chen et al. reported that Co3O4-rGO nanoparticles showed a good response and recovery to methanol [24]. Cao et al. synthesized the SnO2/g-C3N4 composites with high performance to ethanol via a facile calcination method [25]. Actually, reports on Co3O4 as gas sensor are limited, and there is no report on Co3O4 decorated pCNH composite for gas sensor application. The polymeric to graphitic carbon nitride (pCNH) [26,27] is one of the classes of carbon nitrides formed by themolysis and other reactions, which is a polymeric amorphous soild containing a high concentration of H component, and based on ribbon-like polyheptazine structural units like Liebig’s melon. In this paper, we report the synthesis of pCNH decorated Co3O4 composite (Co3O4/pCNH) via a simple hydrothermal method. The presence of ball-flower like Co3O4 and pCNH is characterized by the techniques of XRD, FESEM, TEM, FT-IR, and N2-sorption, and the gas sensing performance of the prepared composite is investigated by exposing to various concentration of ethanol vapor at different temperature. As a result, the Co3O4 and Co3O4/pCNH composite possesses ball-flower like structure, and the Co3O4/pCNH composite exhibits excellent performance, such as higher sensor response, excellent selectivity and stability toward ethanol vapor.

2. Results and Discussion

2.1. Sample Characterization

Figure 1 shows the typical patterns of pCNH, Co3O4 and Co3O4/pCNH composite. From the typical XRD patterns, the phase purity and crystallinity are clearly characterized, and Figure 1 shows two diffraction peaks at 12.9° and 27.5° of the pCNH corresponding to the (100) and (002) crystal planes. The peak at 12.9° of pCNH is the inter-layer structural packing. The highest peak at 27.5° corresponds to the characteristic inter planar staking peak of aromatic systems. The main diffraction peaks are located at 2θ of 19.0°, 31.2°, 36.8°, 38.5°, 44.8°, 55.6°, 59.3° and 65.2° corresponding to the (111), (220), (311), (222), (400), (422), (511) and (440) crystal planes, respectively [28,29,30]. All the peaks of the pure Co3O4 can be assigned to Co3O4 (JCPDS No. 42-1467). The peak intensity is strong indicting high crystalline structure of the products. No peak from other phases is detected, indicating high purity of the products. For the Co3O4/pCNH composite, it is hard to find the characteristic peak of pCNH for two reasons [31,32,33,34]. On the one hand, the quantity of pCNH in Co3O4/pCNH composite is small. Moreover, the X-ray diffraction has a limit of detection which contributes to the hard observation of the pCNH peak in XRD patterns. On the other hand, the cobalt ions can be absorbed onto the surface of the pCNH sheets through electrostatic attraction and the in situ formed Co3O4 might attach to the surfaces of pCNH nanosheets and prevent their aggregation and restacking, which can weaken the characteristic peak of pCNH [34,35,36]. One can see from the Energy Dispersive Spectrometer (EDS) element mappings of Co3O4/pCNH composite (Figure 2c) that the C, N and Co elements are simultaneously detected and these elements are highly dispersed in the composite, providing the coexistence of Co3O4 and pCNH in the as-prepared sample. Further evidence for this conjectural can be supported by TEM (Figure 2e).
Figure 1

XRD patterns of pCNH, Co3O4 and Co3O4/pCNH composite.

Figure 2

FESEM images of pure Co3O4 (a); Co3O4/pCNH composite (b); EDS element mappings of Co3O4/pCNH composite (c); and TEM images of pure Co3O4 (d) and Co3O4/pCNH composite (e).

The morphology and microstructure of the obtained samples are verified by using the techniques of FESEM, EDS and TEM. As shown in Figure 2a, the pure Co3O4 possesses the hierarchical and ball-flower like structure with diameters range of 5–7 μm, and the ball-flower like structure is composed of a number of Co3O4 nanosheets. From Figure 2b, we can see that the Co3O4/pCNH composite keeps the ball-flower like structure which is similar to the pure Co3O4, and Co3O4 and pCNH is closely linked together. Figure 2c shows the EDS element mappings of Co3O4/pCNH composite, from Figure 2c one can see that the C, N and Co elements are simultaneously detected and these elements are highly dispersed in the composite, further providing the coexistence of Co3O4 and pCNH in the as-prepared sample. We can see from the TEM image of pure Co3O4 (Figure 2d) that it possesses the ball-flower like structure and the Co3O4 nanosheet is composed of a number of nanoparticles. Figure 2e displays the typical TEM image of the Co3O4/pCNH composite. The morphology and microstructure of pCNH has been verified with thin layers in our previous paper [25]. It can be seen from Figure 2e that polymeric to graphitic carbon nitride (pCNH) support the Co3O4 particles, and the Co3O4 nanoparticles are highly dispersed on the surface of pCNH nanosheet, and the high surface area of pCNH nanosheet can suppress the sintering of Co3O4 nanoparticles. Due to the high dispersion of Co3O4 nanoparticles, the target gas molecules can immigrate and the produced molecules can emigrate easily from the surface; the as-prepared ball-flower like structure composite is believed to achieve high gas sensing performance. The high-resolution transmission electron microscopy (HRTEM) of the as-prepared Co3O4/pCNH is shown in Figure 3. From this figure, the plane spacing of 0.285 nm corresponds to the lattice planes of (220) in Co3O4. This result could confirm that the nanoparicles visible are Co3O4 phase on the surface of pCNH nanosheet.
Figure 3

HRTEM image of the Co3O4/pCNH composite.

Figure 4 shows the FT-IR spectrum of pure Co3O4 and the Co3O4/pCNH composite. The FT-IR spectrum of Co3O4/pCNH composite has no new absorption peak showing that the structure of Co3O4 and pCNH in the compound has not been destroyed. The peak at 1384.90 cm−1 of Co3O4 is due to the C–H bending vibration, the sharp peak at 567.08 cm−1 and 661.59 cm−1 of pure Co3O4 are attributed to Co–O stretching vibration modes. However, the Co–O stretching vibration modes of the Co3O4/pCNH composite are at 565.15 cm−1 and 661.59 cm−1. These bands experience an offset at around 560–570 cm−1 [37]. The bands at 1637.58 cm−1 of pure Co3O4 are attributed to vibration of the C=C. Nevertheless, the vibration of the C=C of Co3O4/pCNH appears at 1627.94 cm−1. There produces a large deviation indicating an electronic transfer between the C=C and Co–O. The author thinks that there are bonding effects between the Co3O4 and pCNH for the in situ formed.
Figure 4

FT-IR spectra of Co3O4 and Co3O4/pCNH composite.

Figure 5 displays the N2 adsorption-desorption isotherms and the corresponding pore size distribution curves of the as-prepared Co3O4 and Co3O4/pCNH composite. As shown in Figure 5a, the isotherms of the Co3O4 and Co3O4/pCNH composite is categorized to type IVaccording to the IUPAC, with the hysteresis loop of H3-type [2]. This not only shows that it is categorized typical mesoporous material but it also illustrates the existence of an aggregation of the laminated structure with a narrow slit formed by the pCNH and Co3O4 composites from hysteresis loop of H3-type. Figure 5b shows the corresponding pore size distribution curves of the Co3O4 and Co3O4/pCNH composite. It can be clearly seen that the pore diameter of Co3O4 and Co3O4/pCNH composite all main distribute upon 5.44 nm. The results reveal that these two samples are categorized to typical mesoporous materials and matching well with the interlayer pores observed by SEM and TEM image. The BET surface area of Co3O4 and Co3O4/pCNH composite correspondingly turned out to be 48.6 m2·g−1 and 51.3 m2·g−1, respectively. The specific surface area of Co3O4/pCNH composite has a certain improvement over pure Co3O4. The improvement can affect the activity of materials, and in turn, enhancing the gas-sensing performance.
Figure 5

N2 adsorption-desorption isotherms (a) and the corresponding pore size distribution curves (b) of Co3O4 and Co3O4/pCNH composite.

2.2. Gas-Sensing Performance

In order to investigate the gas sensing performance of the as-synthesized samples-based sensors to ethanol vapor, a series of tests are performed. In this study, during the gas sensing performance test, 500 ppm of ethanol is introduced into a sealed chamber (the relative humidity is 40% in the test chamber). The relative humidity can be observed on an intelligent gas sensing analysis system of CGS-4TPS (Beijing Elite Tech. Co., Ltd., Beijing, China). In order to keep humidity at around 40%, the work was continued without intermittence and completed in a day. There is a preparation of seeking optimal temperature from room temperature to high temperature before the formal work; the preparation work shows optimal temperature at around 210 °C. As a result, the formal work sets 180–250 °C as a test range and re-tests to seek optimal temperature. Gas sensing parameters are studied, such as operating temperature, gas response, response-recovery time, and stability for gas sensors. Figure 6 shows the ethanol sensing properties of Co3O4 and Co3O4/pCNH composite based sensors with an ethanol concentration of 500 ppm, and a working temperature was in the range of 180–250 °C. The optimal operating temperatures of Co3O4 and Co3O4/pCNH composite based sensors are at 220 °C and 210 °C, respectively. The response value of Co3O4/pCNH composite based sensor to ethanol vapor at 210 °C is 30.2. However, this value of pure Co3O4 based sensor is only 18.8. In the author’s view, the increased response value of Co3O4/pCNH composite based sensor toward ethanol has two causes. On the one hand, the pCNH is supporting the Co3O4 particles, and increasing the surface area of Co3O4/pCNH composite, in turn, leading to more Co3+ as the extra adsorption centers for ethanol. On the other hand, the strong coupling observed by FT-IR spectrum between the Cobalt and oxygen ions in the Co3O4/pCNH composite makes the Co–O more ionic in nature, which enhances the gas-sensing properties [34].
Figure 6

Response values of the sensors based on Co3O4 and Co3O4/pCNH composite toward 500 ppm ethanol vs. operating temperature.

Figure 7 displays the response-recovery time of Co3O4/pCNH composite at 210 °C towards 500 ppm ethanol. Response time refers to the time taken as 90% by a gas sensor upon exposure to a target gas from the first reaction to the stable end value when the signal has reached a particular percentage level. Recovery time is the time required by a sensor so as to return to 90% of the original baseline signal when the target gas is removed and the sensor is subsequently cleaned with dry air. The response time of this Co3O4/pCNH composite is 93 s and the recovery time of this Co3O4/pCNH composite is 87 s towards 500 ppm ethanol at 210 °C.
Figure 7

The response-recovery time of Co3O4/pCNH composite at 210 °C toward 500 ppm ethanol.

Figure 8 shows the repeatability (a) and stability (b) of the pure Co3O4 and Co3O4/pCNH composite based sensor towards ethanol. It can be seen from Figure 8a that through repeating the test four times, the response recovery curves of the Co3O4/pCNH composite based sensor remain the original response value at around 30, which shows that the material has good repeatability. From Figure 8b, we can see that the response values maintain more than 80% of the original values after 30 days. So, we can draw the conclusion that the Co3O4/pCNH composite based sensor possesses an unexceptionable stability for ethanol vapor detection. The good repeatability and unexceptionable stability of the material make it possible to apply in the actual application.
Figure 8

Therepeatability (a) and stability (b) of Co3O4 and Co3O4/pCNH composite based sensors toward 500 ppm at 210 °C.

Figure 9 displays the response curves to different concentrations of ethanol of Co3O4 and Co3O4/pCNH composite based sensor. From Figure 9a, we can see that the response of the Co3O4 and Co3O4/pCNH goes up trend with the increase of ethanol vapor concentration. As shown in Figure 9b, there is the linear relationship between the response values and the concentration of ethanol for the Co3O4 and Co3O4/pCNH based sensor. The enhanced response values of the Co3O4/pCNH are more obvious with the increasing of gas concentration.
Figure 9

The real time response curves (a) and the response values (b) to different concentrations of ethanol of Co3O4 and Co3O4/pCNH composite based sensor at the operation temperature of 210 °C.

The selectivity of obtained materials toward different gases is displayed in Figure 10. As shown in Figure 10, the response values of Co3O4/pCNH toward acetone, methanol, ethanol, methylbenzene, and methanol are 6.97, 2.04, 30.2, 2.2, 1.22, respectively. Apparently, the Co3O4/pCNH composite possesses the highest response toward ethanol vapor. Meanwhile, it also can be seen from Figure 10 that the properties of Co3O4/pCNH composite towards several gases are higher than the pure Co3O4, indicating that the Co3O4/pCNH composite has a potential application value for ethanol detection.
Figure 10

The selectivity of Co3O4 and Co3O4/pCNH composite based sensors toward 500 ppm different gases at the operation temperature of 210 °C.

3. Materials and Methods

3.1. Sample Preparation

All chemical reagents are analytical and used without further purification. Polymeric to graphitic carbon nitride (pCNH) is synthesized by our previously reported method [38]. The synthesis of flower like pure Co3O4 follows our previous report method [39]. In a typical preparation process of carbon nitride decorated ball-flower like Co3O4 hybrid composite, 2.49 g Co(OAC)2·4H2O was first dissolved in 40 mL deionized water, 0.016 g pCNH was ultrasonic treated in 40 mL deionized water for 4 h. The two solutions were mixed, and then 6 mL of ammonia water was added slowly and stirred in the whole procedure. Then, the mixture was transferred into a 100 mL Teflon-lined stainless-steel autoclave and heated to 180 °C for 12 h under the autogenous pressure. After cooled to room temperature, the products were washed 3 times by deionized water and ethanol respectively to remove any possible impurities. Then, the obtained product was dried in a vacuum oven at 80 °C for 24 h. Finally, the powder was heated in a muffle furnace to 300 °C for 2 h at a heating rate of 2 °C·min−1. After naturally cooled to room temperature, the flower like Co3O4 and Co3O4/pCNH composite were obtained.

3.2. Characterizations

The samples were characterized by X-ray diffraction (XRD, Bruker-AXS D8, Bruker, Madison, WI, USA) with CuKα radiation at 40 kV and 25 mA. Fourier Transform Infrared Spectrometer (FT-IR) was recorded by Fourier Transform Infrared Spectrometer (TENSOR 27 Bruker plc, Madison, WI, USA). The morphology and structure of the samples were observed by the field-emission scanning electron microscopy (FESEM, Quanta™250 FEG) (FEI, Eindhoven, The Netherlands). Transmission electron microscopy (TEM) analysis was performed on a TecnaiG2 F20 microscope (FEI, Eindhoven, The Netherlands) operating at 200 kV. Nitrogen adsorption-desorption isotherms were obtained on a Quantachrome Autosorb-iQ sorption analyzer (Quantachrome, Boynton Beach, FL, USA).

3.3. Gas Sensor Fabrication and Analysis

Gas-sensing performance analysis of the as-synthesized sample was performed on an intelligent gas sensing analysis system of CGS-4TPS (Beijing Elite Tech. Co., Ltd., Beijing, China). The gas sensor fabrication method and gas sensing test produce were performed as our previously reported method [38]. Response of the gas sensor is defined as follows: Response = R/R (R and R are the resistances of the sensor measured in air and in test gas, respectively).

4. Conclusions

In summary, the ball-flower like Co3O4 and pCNH decorated ball flower-like Co3O4 composite (Co3O4/pCNH) are successfully synthesized via a facile hydrothermal route. The composition and morphology of the as-synthesized samples are studied by the techniques of XRD, FESEM, TEM, FT-IR and N2-sorption. The obtained Co3O4/pCNH composite shows good selectivity to ethanol, and the optimum temperature of Co3O4/pCNH composites is 210 °C. The response value of Co3O4/pCNH composite is 1.6 times higher than pure Co3O4 toward 500 ppm ethanol at 210 °C. The enhanced gas sensor properties are due to unique electronic structure and excellent substrate function of pCNH. The Co3O4/pCNH composite also shows a linear relationship between the response values and concentration, good repeatability and stability. The superior gas sensing properties of Co3O4/pCNH indicated that this research will be available for more applications in both laboratory and industry.
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