Sensitivity Enhancement of Benzene Sensor Using Ethyl Cellulose-Coated Surface-Functionalized Carbon Nanotubes

Chobsilp, Thanattha; Muangrat, Worawut; Issro, Chaisak; Chaiwat, Weerawut; Eiad-ua, Apiluck; Suttiponparnit, Komkrit; Wongwiriyapan, Winadda; Charinpanitkul, Tawatchai

doi:https://doi.org/10.1155/2018/6956973

Journal of Sensors

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Abstract Introduction Results and Discussion Conclusion Conflicts of Interest Authors’ Contributions Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2018 | Article ID 6956973 | https://doi.org/10.1155/2018/6956973

Sensitivity Enhancement of Benzene Sensor Using Ethyl Cellulose-Coated Surface-Functionalized Carbon Nanotubes

Thanattha Chobsilp,¹Worawut Muangrat,²Chaisak Issro,¹Weerawut Chaiwat,³Apiluck Eiad-ua,^4,5Komkrit Suttiponparnit,⁶Winadda Wongwiriyapan,^4,5and Tawatchai Charinpanitkul⁷

Academic Editor: Banshi D. Gupta

Received31 Aug 2017

Revised28 Nov 2017

Accepted05 Dec 2017

Published20 May 2018

Abstract

A hybrid sensor based on the integration of functionalized multiwalled carbon nanotubes (MWCNTs) with ethyl cellulose (EC) was fabricated for sensitivity enhancement of benzene detection. To functionalize the surface of MWCNTs, MWCNTs were treated with hydrochloric acid for 60 min (A60-MWCNTs), while other MWCNTs were treated with oxygen plasma for 30, 60, 90, and 120 min (P30-MWCNTs, P60-MWCNTs, P90-MWCNTs, and P120-MWCNTs, resp.). Pristine MWCNTs, A-MWCNTs, and P-MWCNTs were dispersed in 1,2-dichloroethane, then dropped onto a printed circuit board consisting of Cu/Au electrodes used as the sensor platform. Next, EC was separately spin coated on the pristine MWCNTs, A-MWCNTs, and P-MWCNTs (EC/MWCNTs, EC/A-MWCNTs, and EC/P-MWCNTs, resp.). All sensors responded to benzene vapor at room temperature by increasing their electrical resistance which was sensitive to benzene vapor. The EC/P90-MWCNTs enabled an approximately 11-fold improvement in benzene detection compared to EC/MWCNTs. The sensitivity of all sensors would be attributed to the swelling of EC, resulting in the loosening of the MWCNT network after benzene vapor exposure. The differences of the sensing responses of the EC/MWCNTs, EC/A-MWCNTs, and EC/P-MWCNTs would be ascribed to the differences in crystallinity and functionalization of MWCNT sidewalls, suggesting that acid and oxygen plasma treatments of MWCNTs would be promising techniques for the improvement of benzene detection.

1. Introduction

Carbon nanotubes (CNTs) [1, 2] are one kind of carbon nanomaterial structure which has received widespread attention because of their exceptional properties such as high electrical [3, 4] and thermal conductivity [5], and large specific surface area [6]. Two and a half decades ago, CNTs were applied to the field of nanoelectronic technology for use in supercapacitors, field emitters, and gas sensors, especially in the application of CNTs as ultrasensitive gas sensors because of their high specific surface area as well as fast and high response at room temperature. Many studies have demonstrated ultrasensitive gas sensors based on pristine CNTs for the detection of oxidizing gases down to part-per-million levels (ppm) at room temperature [7–10]. Nevertheless, a gas sensor based on pristine CNTs is still insensitive to volatile organic compounds (VOCs) [11], especially benzene vapor. Benzene is a kind of VOC which is prevalent in outdoor air due to the emission from diesel engines. It is an abundant component in crude oil and various products derived from petrochemical processes [12]. The exposure to benzene at a level exceeding designated standards is harmful to human health and damages the environment. The National Institute for Occupational Safety and Health (NIOSH) of the U.S. limits the average concentration of benzene to lower than 0.1 ppm for an average exposure of 10 h/day [13]. However, the interaction between the pristine CNTs and benzene is very weak. To enhance the sensitivity of benzene detection, the functionalization of CNTs with metal nanoparticles and polymer has been proposed as a promising approach. For example, a gas sensor based on palladium (Pd) nanoparticles (NPs) decorated on single-walled CNTs (Pd NPs/SWCNTs) by a sputtering technique has been proposed and demonstrated for benzene detection [14]. Moreover, the Pd NP/SWCNT sensors showed weak benzene sensitivity at concentrations three orders of magnitude higher than that of the required detection threshold for ambient safety applications. In addition, multiwalled CNTs (MWCNTs) were functionalized by oxygen plasma treatment to help the adhesion and distribution of metal NPs (Rh, Pd, or Ni) on the surface of MWCNTs. Functionalized MWCNTs decorated with metal NPs could increase the sensitivity to benzene vapor. These metal NP-decorated functionalized MWCNTs can provide selective detection of benzene at trace levels with a detection limit below 50 parts per billion (ppb) [15]. Although the advantage of metal NP-decorated CNTs is the high sensitivity to benzene, the metal NP decoration technique needs a high-vacuum system which is costly. Another type of gas sensor fabricated using conductive polymer-CNT composites for benzene detection at room temperature was demonstrated. The composites of SWCNTs and ethyl cellulose (EC) enhance the ability to detect benzene vapor [16]. The polymer-CNT composites were prepared in the form of CNTs dispersing in a polymer matrix based on percolation theory by a complicated polymerization process. Recently, a simple fabrication method has been proposed by coating a thin film of EC on to the acid-functionalized MWCNT network. However, the sensitivity is limited to parts per thousand level and the chemical state of the functionalized MWCNTs has not been fully explored [17].

In this work, we have proposed an approach to enhance the sensitivity of a benzene sensor using EC-coated surface-functionalized MWCNTs by an oxygen plasma technique. The fabricated gas sensor could detect benzene vapor in the range of parts per thousand (ppt) down to parts per million (ppm) level at room temperature. For comparison, the sensitivity improvement of MWCNTs functionalized by different methods, that is, acid treatment and oxygen plasma treatment, was investigated.

2. Experimental Methods

2.1. Surface Functionalization of MWCNTs by Acid or Oxygen Plasma Treatments

Chemical vapor deposition-grown commercial MWCNTs (NANOCYL™ NC7000) with a purity of 90% were used in this study. The average length and diameter of the commercial MWCNTs were 1.5 μm and 9.5 nm, respectively. Functionalization of MWCNTs by acid or oxygen plasma treatment was intentionally conducted to modify their surface reactivity. For acid treatment, 30 mg of pristine MWCNTs were suspended in 15 mL of 37% hydrochloric acid (HCl) and sonicated for 60 min prior to being washed with deionized water until its pH became neutral. Finally, the HCl-treated MWCNTs (hereafter referred to as A60-MWCNTs) were gently dried at 100°C for 24 h. For oxygen plasma treatment, 60 mg of MWCNTs were treated with oxygen plasma for 30, 60, 90, and 120 min using an expanded plasma cleaner (Harrick Scientific) in order to modify their surface reactivity (hereafter referred to as P30-MWCNTs, P60-MWCNTs, P90-MWCNTs, and P120-MWCNTs, resp.).

2.2. Fabrication of Gas Sensor Device

The pristine MWCNTs, A-MWCNTs, and P-MWCNTs were separately dispersed in 1,2-dichloroethane by ultrasonication for a designated time period and subsequently dropping onto a printed circuit board consisting of interdigitated Cu/Au electrodes with a gap of 250 μm. The electrical resistance of the pristine MWCNTs, A-MWCNTs, and P-MWCNTs were adjusted to approximately 1 kΩ. EC diluted in toluene with a concentration of 1 wt% was continuously stirred for 24 h. Subsequently, the EC solution was spin coated on pristine MWCNTs, A-MWCNTs, and P-MWCNTs (hereinafter called EC/MWCNTs, EC/A-MWCNTs, and EC/P-MWCNTs, resp.) with a spinning speed of 3000 rounds per minute. Finally, all the sensors were heated at 100°C for 24 h to eliminate the residual toluene.

2.3. Characterization Techniques

The purity and crystallinity of pristine MWCNTs and functionalized MWCNTs were analyzed by Raman spectroscopy (Thermo Scientific™, DXR™ SmartRaman) with an excited laser wavelength of 532 nm (2.33 eV) in the Raman shift range of 100–3500 cm⁻¹. Pristine MWCNTs and functionalized MWCNT powder mixed with potassium bromide (KBr) were prepared in pellet form prior to being analyzed by Fourier transform-infrared (FT-IR) spectroscopy (Perkin Elmer, Spectrum One) for identifying functional groups existing on the surface of MWCNTs. Typical FT-IR spectra in transmittance mode were scanned in a range of 400–4000 cm⁻¹. Transmission electron microscopy (TEM, JEOL, JEM-2010) was used for observing the nanostructure of pristine MWCNTs and functionalized MWCNTs. The morphology of EC-coated functionalized MWCNTs was characterized by field emission scanning electron microscopy (FESEM, Hitachi S-4700). Finally, X-ray photoelectron spectroscopy (XPS, AXIS Ultra DLD, Kratos Analytical) was used to analyze the chemical composition and state of pristine MWCNT and functionalized MWCNT surfaces, with a base pressure of and a monochromatic Al Kα 1,2 radiation of 1.4 kV.

2.4. Gas Sensor Measurement

The sensor responses of EC/MWCNTs, EC/A-MWCNTs, and EC/P-MWCNTs to benzene vapor was experimentally examined by tracking temporary changes in electrical resistance with respect to elapsed time. Initially, each sensor was placed in a stainless chamber with 3.0 lpm of N₂ for 180 s. Then, benzene vapor prepared from bubbling liquid benzene with 1.5 lpm of N₂ was alternatively supplied into the chamber for 180 s. For recovery, the sensor was again purged with 3.0 lpm of N₂ until its initial electrical resistance was confirmed. The concentration of benzene vapor was varied in a range of 142–170 parts per thousand (ppt). The electrical resistance of the sensing material between the interdigitated electrodes was directly measured using a Fluke NetDAQ multimeter. The sensor response () could be determined using (1) whereas and are the resistance of a sensor exposed to benzene vapor and N₂, respectively.

To control the concentration of benzene in the range of parts per million (ppm), the benzene liquid was dropped using a micropipette into the detection chamber by controlling the volume of benzene. The sensor was placed in the stainless steel chamber under air atmosphere for 3 min, followed by the dropping of benzene liquid into the detection system and monitoring its resistance for 30 min. Finally, the sensor was recovered by air exposure. The benzene concentration was in the range of 517–51,670 ppm. is defined using (1) whereas and are the electrical resistance of the sensor under benzene vapor and air atmosphere, respectively.

3. Results and Discussion

3.1. Nanostructure, Purity, Crystallinity, Functional Group, and Elemental Composition of Pristine MWCNTs and Functionalized MWCNTs

Figure 1 shows the TEM images of (a) pristine MWCNTs, (b) A60-MWCNTs, (c) P30-MWCNTs, (d) P60-MWCNTs, (e) P90-MWCNTs, and (f) P120-MWCNTs. Pristine MWCNTs reveal partly amorphous carbon attached on their sidewalls and the metal catalytic nanoparticles (dark points in the inset of Figure 1(a)) which remain from the synthesis by the CVD method. After acid and oxygen plasma treatments, it was clearly found that the amorphous carbon and the metal catalytic nanoparticles (inset of Figures 1(b)–1(f)) were removed from their MWCNT sidewalls. The average diameters of pristine MWCNTs, A60-MWCNTs, P30-MWCNTs, P60-MWCNTs, P90-MWCNTs, and P120-MWCNTs were , , , , , and , respectively. There was a slight decrease in the diameters of treated MWCNTs compared to those of pristine MWCNTs, implying the detrimental damage by acid and oxygen plasma treatments. The Raman spectra of all samples consist of three characteristic peaks which are the D-, G-, and 2D-bands at 1340, 1580, and 2680 cm⁻¹, respectively (data not shown). The G-band indicates the presence of a signal reflecting a graphitic structure that is emitted from the stretching vibration of the sp² carbon while the D-band is attributed to a disordered carbon structure and the sp³ hybridized carbon. The 2D-band corresponds to second-order Raman scattering using a two-phonon process [18]. The intensity ratio of the G and D bands is a representation of the crystallinity of MWCNTs and treated MWCNTs. The of pristine MWCNTs, A60-MWCNTs, P30-MWCNTs, P60-MWCNTs, P90-MWCNTs, and P120-MWCNTs were , , , , , and , respectively. The higher of the A60-MWCNTs, P30-MWCNTs, and P60-MWCNTs compared with those of the pristine MWCNTs would suggest that the crystallinity of the treated MWCNTs was improved due to the removal of disordered carbon structures and impurities. However, with a longer time of oxygen plasma treatment up to 90 min, the oxygen radical generated from oxygen plasma may etch the sidewall of MWCNTs, resulting in the formation of a defect and the decrease in the ratio.

(a)

(b)

(c)

(d)

(e)

(f)

The change in surface functional groups of pristine MWCNTs after acid and oxygen plasma treatments was analyzed by FT-IR (data not shown). The peak at 3780 cm⁻¹ is O-H stretching vibration [19]. All samples showed a broad transmission band at around 3430 cm⁻¹ corresponding to the O-H stretching vibration which could be due to absorbed water, O-H, or carboxylic groups on MWCNT surfaces [20]. The peaks at 2920 and 2850 cm⁻¹ could contribute to sp³ (C-H) vibration, originating from the surface or sidewalls of CNTs [21]. The small band at around 1560 and 1020 cm⁻¹ could be attributed to the presence of (C=C) and (C-O) stretching [22, 23]. Furthermore, the new peak appeared at a wave number of 1380 cm⁻¹ from A-MWCNTs and P-MWCNTs. The peak at 1380 cm⁻¹ is due to (C-O) stretching and (O-H) bending deformation in (-COOH) [24]. These results indicate that oxygen-plasma treatments are an effective method to functionalize oxygenated functional groups of (-OH) and (-COOH) on the walls of MWCNTs.

XPS was used to measure the chemical composition and chemical state of pristine MWCNTs, A-MWCNTs, and P-MWCNTs. Figure 2(a) shows the XPS survey spectrum of P90-MWCNTs. The spectrum consists of C 1s and O 1s peaks at 285 and 533 eV, respectively. For the C 1s peak, there are four different carbon groups in the XPS spectrum: sp² C=C at 285.0 eV, sp³ C-C at 285.7 eV, the carbonyl group C=O at 286.6 eV, and the carboxyl group -COOH at 287.3 eV as shown in Figure 2(b) [25]. In the case of the O 1s peak, there are two different oxygen groups in the XPS spectrum: C=O at 532.4 eV and C-O at 533.8 eV as shown in Figure 2(c) [26]. The components (%) of C 1s and O 1s of pristine MWCNTs, A-MWCNTs, and P-MWCNTs are summarized in Table 1. The relative percentages of carbon in P60-MWCNTs and P90-MWCNTs decrease from 93.57% to 92.53 and 92.30%, respectively, while the percentages of oxygen increase from 4.82% to 6.72% and 6.78%, respectively. The results showed that oxygen plasma treatment significantly generated oxygen species on MWCNTs [25, 27]. Figure 2(d) shows the top and cross-sectional (inset) views of FESEM images of EC/P90-MWCNTs. The P90-MWCNT network was shown to be buried in the EC matrix. The thickness of the EC coating on the P90-MWCNTs was 0.22 μm.

(a)

(b)

(c)

(d)

3.2. Sensing Characteristics of EC/MWCNT, EC/A-MWCNT, and EC/P-MWCNT Sensors

The sensor responses of EC/MWCNTs, EC/A60-MWCNTs, and EC/P60-MWCNTs under benzene vapor are shown in Figure 3(a). The inset of Figure 3(a) shows a photograph of the sensor device. All sensors exhibited an increase in the electrical resistance after exposure to benzene vapor and completely recovered to the initial values after being purged with N₂ gas. Figure 3(b) shows the normalized sensor response of the EC/MWCNT, EC/A60-MWCNT, and EC/P60-MWCNT sensors. It could be observed that the normalized sensor response of EC/A60-MWCNTs and EC/P60-MWCNTs were 3.66- and 7.47-fold higher than that of EC/MWCNTs, respectively. The preliminary sensor response results indicated that the acid- and oxygen plasma-treated MWCNTs improved the sensor response to benzene vapor. Next, the responses of the EC-coated sensors on different times of oxygen plasma treatment of MWCNTs to benzene vapor were investigated. Figure 4(a) shows the sensor response of EC/MWCNTs, EC/P30-MWCNTs, EC/P60-MWCNTs, EC/P90-MWCNTs, and EC/P120-MWCNTs exposed to benzene vapor. The electrical resistance of all sensors increased upon benzene exposure and decreased after replacing benzene with N₂ gas. Figure 4(b) shows the normalized sensor response of EC/MWCNTs, EC/P30-MWCNTs, EC/P60-MWCNTs, EC/P90-MWCNTs, and EC/P120-MWCNTs to benzene vapor. The normalized sensor response is in the following order: EC/MWCNTs < EC/P30-MWCNTs < EC/P120-MWCNTs < EC/P60-MWCNTs < EC/P90-MWCNTs. The normalized sensor response of EC/P90-MWCNTs was 10.68-fold higher than that of EC/MWCNT. The sensing mechanism of EC/MWCNTs, EC/A-MWCNTs, and EC/P-MWCNTs could be attributed to the swelling of EC [16, 28–32]. Moreover, the increase of sensor response could be explained by the oxygenated functional groups after oxygen plasma treatments. The oxygenated functional groups increased the interaction between oxygen plasma-treated MWCNTs and EC. Upon benzene exposure, EC started to swell, resulting in the loosening of the MWCNT network and followed by a large increase in the electrical resistance of MWCNTs [33, 34]. These results implied that the oxygenated functional groups forming on the surface of MWCNTs by acid and oxygen plasma treatments play an important role in benzene detection. The relative amount of oxygen in MWCNTs seemingly increased with the increase of the oxygen plasma treatment time. Nevertheless, the sensor response of EC/P120-MWCNTs is lower than that of EC/P60-MWCNTs and EC/P90-MWCNTs. These results could be explained by the increasing of oxygen plasma treatment time. The higher oxygen plasma treatment time makes the MWCNT surface to be etched and destroyed, which is consistent with TEM results (Figure 1(f)). Thus, the interaction between P120-MWCNTs and EC is lower compared to P60-MWCNTs and P90-MWCNTs, resulting in a lower sensor response.

(a)

(b)

(a)

(b)

The sensor response of the EC/P90-MWCNTs under benzene vapor in the concentration range of 517–51,670 ppm was shown in Figure 5(a). The EC/P90-MWCNTs could detect benzene vapor down to ppm level. The electrical resistance of EC/P90-MWCNTs increased under benzene exposure and recovered to their initial resistance under air exposure. The higher the benzene concentration, the higher is the sensor response. When the benzene concentration increases, a higher quantity of benzene molecules adsorb on EC/P90-MWCNTs, thus accelerating the EC swelling level, resulting in an increase in electrical resistance change and a decrease in response time. For benzene detection at 517 ppm, the gas sensor barely responded to benzene vapor. It would be the limitation of the fabricated gas sensor. For benzene detection at a 51,670 ppm concentration, the gas sensor was unable to recover to its initial resistance within 30 min. This may be due to a large swelling level at high concentration that takes a longer recovery time than that of a low swelling level at low concentration. Figure 5(b) represents the relationship between the sensor response of EC/P90-MWCNTs and benzene concentration. The results show the relation between sensor response and benzene concentrations as a curved graph. This result clearly indicates that the combination of oxygen plasma treatment and EC functionalization of CNTs is a promising approach to improve benzene sensor sensitivity down to ppm-level detection.

(a)

(b)

4. Conclusion

The gas sensors based on EC-coated surface-functionalized MWCNTs have been successfully demonstrated to detect benzene vapor from ppt down to ppm level at room temperature. Oxygen plasma and acid treatment techniques were employed for MWCNT functionalization. The fabricated sensor from EC/P90-MWCNTs exhibited a 10.68-fold improvement in the response to benzene detection compared to the EC/MWCNTs. The improvement of sensor response to benzene vapor would be ascribed to the binding interaction between functional groups on the surface of MWCNTs and coated EC on MWCNTs. The higher binding interaction improves the adhesion of EC on the functionalized MWCNT surface, resulting in the higher response of EC-coated functionalized MWCNTs compared to that of EC-coated pristine MWCNTs. These results suggest that the integration of acid- or oxygen plasma-treated MWCNTs and EC would be promising approaches for the improvement of the benzene-detecting sensor.

Conflicts of Interest

The authors declare that there is no conflict of interests regarding the publication of this paper.

Authors’ Contributions

Thanattha Chobsilp and Worawut Muangrat contributed equally to this work.

Acknowledgments

The authors acknowledge the financial and facility support from the PTT Public Company Limited via the collaborative project granted to CEPT, CU. This work is also partly supported by the National Nanotechnology Center (NANOTEC), NSTDA, Ministry of Science and Technology, Thailand, through its program of Center of Excellence Network.

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Copyright © 2018 Thanattha Chobsilp et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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