International Journal of Photoenergy

International Journal of Photoenergy / 2016 / Article

Research Article | Open Access

Volume 2016 |Article ID 2853046 | 10 pages | https://doi.org/10.1155/2016/2853046

Influence of Acid Modification Multiwall Carbon Nanotube Counter Electrodes on the Glass and Flexible Dye-Sensitized Solar Cell Performance

Academic Editor: Cláudia G. Silva
Received06 Feb 2015
Revised20 Apr 2015
Accepted29 Oct 2015
Published11 Jan 2016

Abstract

Multiwall carbon nanotubes (MWCNTs) were modified by acids (H2SO4 : HNO3) for generating active groups on the nanotube surface. Unmodified- and modified-carbon nanotubes were coated on the conductive glass and conductive plastic substrates by a slurry paste method, and they were used as the counter electrodes (CEs) of dye-sensitized solar cells (DSSCs). Scanning electron microscopy reveals that carbon nanotubes are evenly deposited on the conductive glass. The efficiency of the glass based DSSCs of unmodified- and modified-carbon nanotubes and Pt CEs is ~4.73%, ~5.66%, and ~6.08%, respectively. The efficiency of the plastic based DSSCs of the unmodified- and modified-carbon nanotubes CEs is ~0.80% and ~2.11%, respectively. The voltammogram and electrochemical impedance spectroscopy results suggest that the superior performance of the modified-carbon nanotubes DSSCs is attributable to the high electrocatalytic activity and the low charge-transfer resistance of the modified-carbon nanotubes film over the unmodified-carbon nanotubes film.

1. Introduction

Dye-sensitized solar cell (DSSC) has been intensively studied because of its simple structure, low fabrication cost, promising light harvesting efficiency, and environmental friendliness. The high energy conversion efficiency of DSSCs is accomplished through the use of a highly porous semiconductor film coated by a monolayer dye-sensitizer as the working electrode, which was developed by O’Regan and Grätzel in 1991 [1]. TiO2 nanoparticles are commonly used as a semiconductor because they deliver the highest energy conversion efficiency among semiconductors (ZnO, Nb2O5, WO3, and SnO2) [25]. TiO2 nanoparticles serve as the electron-transport medium between dye-sensitizers and the electron collector (transparent conductive substrate). Electrons from the electron collector will flow through the external load reaching the counter electrode and undergo the reduction with tri-iodide () with the help of the catalyst film. The cell efficiency is found to be strongly related to the catalyst film (counter electrode, CE).

Platinum (Pt) film is commonly used as the DSSC counter electrode because of its good catalytic activity, but Pt is an expensive material. Other cheap materials have been tested as an alternative DSSC catalyst, including carbon black, carbon nanotubes, graphene, conductive polymers, and metal sulfide [611]. Carbon nanotubes (CNTs) are applied as the DSSC counter electrode because of their unique properties such as good catalytic activity, good conductivity, high thermal stability, high aspect ratio, and comparatively lower price than Pt. Thus, by switching to a CNT counter electrode, the DSSC production cost should be minimized. However, the performance of the CNTs based DSSCs is still low compared to the Pt DSSC performances.

It is reported that the acid treatment can introduce functional groups, hydroxyl or carboxylic, on the carbon nanotube surfaces as shown in Figure 1. The presence of these functional groups is found to enhance nanotubes’ catalytic activity [1214]. This implies that by using an acid-treated CNTs film as the DSSC counter electrode, the tri-iodide reduction rate and the cell efficiency should be optimized. Various methods, chemical vapor deposition, arc discharge, electrophoretic deposition, or slurry paste [1520], were used for preparing carbon nanotube films. The slurry paste is a simple method to coat the low temperature carbon film. The low temperature process would allow the possible coating CNTs film on the plastic substrate for fabricating in the flexible DSSCs. The flexible DSSCs reduce the production cost and the cell weight. To assemble flexible DSSCs, TiO2 film was coated on the plastic by a high pressure compression as reported by Grinis et al. [21] and Fredin et al. [22]. To the best of our knowledge, there are few details on the effect of acid-treated carbon nanotubes on the dye-sensitized solar cell performance. In this work, we explored the possibility of using the carbon nanotube film as the DSSC counter electrode for both glass and plastic substrates, and the effect of the acid treatment on the solar cell performances was tested and discussed.

2. Experimental

2.1. Modification of MWCNTs

The modified-multiwall carbon nanotubes (M-CNTs) were prepared by mixed multiwall carbon nanotubes (unmodified-CNTs, U-CNTs) 5 g in sulfuric acid (H2SO4, 95%) 30 mL and nitric acid (HNO3, 63%) 10 mL, then stirring for 30 min at room temperature. After that, the carbon nanotubes were rinsed with DI water several times, filtered with filter paper, and dried at 80°C for 12 h at the ambient conditions. After the modification, the carboxylic groups were generated on the CNT surface as shown in Figure 1.

2.2. Preparation of TiO2 and CNT Films
2.2.1. TiO2 Film Coated on the Conductive Glass Substrate (TiO2/FTO)

The conductive glass (fluoride doped tin oxide glass, FTO, sheet resistance of 15 Ω/sq, Solaronix) was used as a substrate for coating TiO2 films. The dense TiO2 layer was prepared by spinning the titanium diisopropoxide bis(acetylacetonate) (C16H28O6Ti) solution on the FTO substrate. The porous transparent TiO2 film was coated on the dense TiO2 film by a screen printing technique using the TiO2 paste PST-18NR (Catalysts & Chemicals Ind. Co., Ltd.). A scattered TiO2 layer was coated on the porous TiO2 film by screen printing using PST–400C (Catalysts & Chemicals Ind. Co., Ltd.). TiO2 films were annealed at 500°C for 1 h at the ambient conditions, and the postannealed TiO2 films were treated with UV light for 5 min. The UV-treated TiO2 films were immersed in the dye solution, cis-bis(isothiocyanato) bis(2,2′-bipyridyl-4,4′-dicarboxylato)-ruthenium(II)-bis-tetrabutylammonium (N719, Solaronix, 5 × 10−4 M in acetonitrile : tert-butanol at a volume ratio of 1 : 1) for 24 h at room temperature in the dark.

2.2.2. TiO2 Films Coated on the Conductive Plastic Substrate (TiO2/ITO/PEN)

The indium tin oxide coated on polyethylene naphthalate (ITO/PEN, sheet resistance of 60 Ω/sq, Peccell Technologies, Inc.) was used as the conductive flexible substrate. The TiO2 slurry, mixture of 5 g TiO2 (P25, 20 nm, Degussa, Germany) in 20 mL isopropanol, was carefully pasted on the ITO/PEN substrate and let it dry in the air. Then, TiO2 films were pressed by the hydraulic pressuring system (Model HP–10, T.M.C. Industrial Co., Ltd.) at the compression pressure of ~510 MPa, called pressed TiO2 film. The pressed TiO2 films were immersed in the N719 dye solution, 5 × 10−4 M in acetonitrile : tert-butanol at a volume ratio of 1 : 1, for 24 h at room temperature in the dark.

2.2.3. CNT Films

CNT film was deposited on the conductive glass (CNT/FTO) or conductive plastic (CNT/ITO/PEN) substrates by the slurry paste method. The carbon slurry was a mixture of 0.6 g M-CNTs (or 0.6 g U-CNTs) and 0.1 g PVDF in 3 mL N-methyl-2-pyrrolidione (NMP). The carbon slurry was stirred by the magnetic stirrer for 30 min. The slurry was pasted on the substrate by a glass rod, and then films were dried at 80°C for 6 h.

2.3. DSSC Assemble

The glass based DSSC was assembled by using dye-TiO2/FTO film as the working electrode and CNT/FTO film as the counter electrode with the cell active area of 0.7 × 0.7 cm2. These two electrodes were sandwiched together with two layers of a 60 μm thick Surlyn polymer film (Solaronix) as a plastic sealant and a cell spacer. Two Surlyn layers were applied because of the thick carbon film. A liquid electrolyte, a mixture of 0.6 M MPI (1-methyl-3-propylimidazolium iodide), 0.1 M LiI (lithium iodide anhydrous), 0.05 M (iodide), 0.5 M TBP (tert-butylpyridine), and 0.0025 M LiCO3 (lithium carbonate) in acetonitrile, was filled into the cell through the drilled hole on the counter electrode. After electrolyte filling, the hole was sealed by a Surlyn polymer film covered with a small piece of glass slide.

In case of the flexible DSSCs, the dye-pressed-TiO2/ITO/PEN films and the CNT/ITO/PEN films were used as the working electrode and the counter electrode, respectively, with the cell active area of 0.7 cm × 0.7 cm. Three layers of a 60 μm thick Surlyn film were placed between these two electrodes as a cell spacer and then tightly clipped. The liquid electrolyte was filled into these flexible cells.

2.4. Film Characterization

The film morphology and the film thickness were characterized by scanning electron microscope (SEM, LEO, SEM 1450VP, UK). The amount of adsorbed dye was estimated using a UV-visible spectrometer (UV-160A, Shimadzu) by desorbing dye molecules from TiO2 films in the 10 mL solution of a mixed 0.1 M NaOH and ethanol at a volume ratio 1 : 1. XPS measurement was carried out at Beamline 3.2a, SLRI, with maximum photon energy of 650 eV, kinetic energy step of 0.1 eV, and pass energy of 100 eV. Before XPS measurement, the Au 4f peak was used to calibrate energy shift from the instrument. The XPS was operated under the pressure of ~10−10 mbar and the temperature at 25°C. The cyclic voltammetry (CV) was measured in a three-compartment cell with Gamry Instrument Reference 3000 (Gamry, USA) at a scan rate of 20 mV/s. The Pt plate (area ~0.385 cm2) and the Ag/AgCl electrode were used as the counter electrode and the reference electrode, respectively. The Pt and carbon films were taped with an insulating tape with an open area of 0.25 cm2 prior to the CV scan. The electrochemical impedance spectroscopy (EIS) was recorded using Gamry Instrument Reference 3000 Potentiostat (Gamry, USA) under a light intensity of 100 mW·cm−2 with frequency from 0.01 Hz to 100,000 Hz and AC amplitude of 10 mV. The cell performance was measured with a super solar simulator (Wacom, Class A) system under a light intensity of 100 mW·cm−2.

3. Results and Discussion

3.1. Glass Based DSSCs

The surface morphology of TiO2 films coated on the conductive glass is characterized by SEM, and images are presented in Figure 2. The SEM results show that TiO2 films have the porous structures. The cross section image of TiO2 film (Figure 2(b)) clearly shows three different layers: a dense-TiO2 layer ~0.5 μm, a porous transparent TiO2 layer ~5.5 μm, and a scattered TiO2 layer ~3.2 μm. The amount of dye molecules adsorbed on the TiO2 films, on a TiO2 area of 0.49 cm2, was desorbed and analyzed by the UV-visible spectrometer. All three absorbance spectra in Figure 2(c) exhibit close absorbance value, implying that the TiO2 thickness of these three films is close to one another. The amount of dye loaded on the TiO2 films is calculated via the following equations:where and are the absorbance value and the specific absorbance (M−1cm−1) as a function of wavelength, respectively. is the desorbed dye concentration (), is the thickness of the standard cuvette glass (1 cm), is the volume of the dye solution (10 mL), and is the amount of dye molecules adsorbed on the TiO2 films (mol). By using the specific absorbance at = 300 nm, 5.7 × 104 M−1cm−1, the amount of dye molecules is about 10.86 × 10−8, 10.71 × 10−8, and 9.92 × 10−8 mol/cm2 (average 10.50 × 10−8 ± 0.51 × 10−8 mol/cm2).

To verify the formation of carboxylic groups on the CNTs’ surface, X-ray photoelectron spectroscopy (XPS) was scanned on the unmodified-CNTs (U-CNTs) and modified-CNTs (M-CNTs). The XPS survey spectra of U-CNTs and M-CNTs powders in Figure 3(a) mainly contain oxygen and carbon peaks. It is shown in Table 1 that the O/C area ratio increases from 0.75 to 0.89 after the acid treatment, implying formation of the oxygen functional groups on the modified nanotube surface. To see the change on M-CNTs, the C 1s peaks were deconvoluted as shown in Figure 3(b). The binding energy of each bond is listed in Table 1. It is observed that the U-CNTs consist of three bonds (C–C, C–OH, and C–O–C bonds), but M-CNTs are composed of four bonds. The extra peak at 289.3 eV was detected, which corresponds to –C=O (carboxylic groups). This clearly confirms the presence of the functional groups on the acid-treated CNTs.


SampleRelative amount of elements (%)Binding energy (eV)
OCO/CPeak 1
C–C
Peak 2
–C–OH
Peak 3
C–O–C
Peak 4
–C=O

Unmodified-CNTs
(U-CNTs)
57430.75284.1286288

Modified-CNTs
(M-CNTs)
53470.89284.2285.5287.6289.3

The optical images of U-CNTs and M-CNTs films in Figure 4 show the similar structures between these two films. However, the low magnification SEM images (Figure 4) reveal the great differences. The modified film seems to have a better nanotube spreading than the unmodified film. This may be due to the functional groups interacting to the FTO surface [23, 24]. The film thickness estimated from the cross section SEM images (Figure 4(d)) is ~33–65 μm. The CNTs films were used as the DSSC counter electrode, and the cell efficiency was analyzed by the solar simulator. The short-circuit current density (), open-circuit voltage (), fill factor (FF), and efficiency () were extracted from the curves of Figure 5(a) and listed in Table 2. M-CNTs DSSC (5.66%) produces larger efficiency than that of U-CNTs DSSC (4.73%). This could be due to the presence of carboxylic groups on CNTs’ surface strengthening the nanotube reactivity as observed by many groups [1214]. Compared to Suzuki et al. [7], Ahn et al. [8], and Sedghi and Miankushki [25] works, they obtained the efficiency of the carbon nanotube based DSSCs of 3.5%, 5.18% (prepared by aerosol deposition process), and 6.7% (prepared by spraying method), respectively. Our efficiency is between these values.


Counter electrode (Ohm) (Ohm) (Ohm) (V) (mA/cm2)FF (%)

Unmodified-CNTs 1734600.789.910.614.73
(U-CNTs/FTO/glass)

Modified-CNTs1419610.7312.700.615.66
(M-CNTs/FTO/glass)

Pt sputter163600.7610.020.806.08
(Pt/FTO/glass)

To explain the different cell behaviors, cyclic voltammetry (CV) was conducted on these three films at the scan rate of 20 mV/s in the 10 mM LiI, 1 mM , and 0.1 M LiClO4 electrolyte. The CV curve of Pt film (Figure 5(b)) exhibits two oxidation peaks at 0.34 V and 0.71 V and two reduction peaks at 0.02 V and 0.50 V. Similarly, M-CNTs film is composed of two oxidation peaks at 0.33 and 0.76 V and two reduction peaks at −0.05 and 0.49 V. In contrast, U-CNTs films do not manifest clear oxidation or reduction peaks. The CV current density of M-CNT film is higher than that of U-CNT film, implying the superior electrocatalytic activity performance of M-CNTs film above the U-CNTs. Electrochemical impedance spectroscopy (EIS) was also measured under the light intensity of 100 mW/cm2 and the EIS spectra are shown in Figure 6(b). EIS spectra consist of two semicircles similar to the literatures [26, 27]. The equivalent circuit in Figure 6(a) is used to fit the EIS curves. The equivalent circuit is comprised of an interface charge-transfer resistance (), a constant phase element (CPE), and a series resistance (). The CPE reflects the interfacial capacitance, with CPE1 and CPE2 being constant phase elements of the CE/electrolyte interface and the TiO2/dye/electrolyte interface, respectively. and are the electron-transfer resistances at the CE/electrolyte interface and at the TiO2/dye/electrolyte interface, respectively. of U-CNTs and M-CNTs DSSCs is ~34 Ω and ~19 Ω, respectively, as listed in Table 2. of M-CNTs film is smaller than that of U-CNTs film because M-CNTs film has a better spreading and stronger attaching to the glass substrate than U-CNTs film.

3.2. Plastic Based DSSCs

Figures 7(a) and 7(b) show the optical images of the unpressed and pressed TiO2 films on the conductive plastic (ITO/PEN), respectively. It observes that the pressed TiO2 film is brighter than the unpressed film, which is attributed to the densely packed TiO2 nanoparticles after compressing. The thickness of the pressed TiO2 film, estimated from the cross section SEM in Figure 7(d), is ~2.1 μm. It is worth mentioning that we had tried to prepare the thicker TiO2 film, but TiO2 film was peeled of the substrate after the film compression. The low amount of TiO2 paste on the plastic substrate was found to well attach to the substrate.

The amount of dye loaded on the pressed TiO2 films is analyzed by UV-visible spectrometer, and the result is presented in Figure 7(e). Three absorbance spectra show the close absorbance value, meaning that the thicknesses of the pressed TiO2 films are quite closed. By using (1) and  M−1cm−1, the average amount of dye coated on the pressed TiO2/ITO/PEN films is ~5.69 × 10−8  ± 0.41 × 10−8 mol/cm2. As expected, the amount of dye loaded on the TiO2/ITO/PEN films is much less than that of the TiO2/FTO films by ~46%. This is due to the thinner press TiO2 film (~2.1 μm) than that of the screened TiO2 film (~9.2 μm), as seen in Figures 7(d) and 2(b), respectively.

CNTs films were coated on the ITO/PEN films via the same procedure on the CNTs/FTO/glass films. The low magnification SEM images of U-CNTs and M-CNTs films, Figures 8(a) and 8(c), display the great differences. M-CNTs are found to well spread on the plastic surface, but U-CNTs form the island-like structures on the ITO/PEN surface. The well depositing of M-CNTs on the ITO/PEN surface should be attributed to the good interaction between the functional groups to the ITO surface [23, 24].

The performance of the flexible DSSCs, using dye/pressed-TiO2/ITO/PEN film as the working electrode and CNTs/ITO/PEN film as the counter electrode, is tested under the same condition with the glass based DSSCs. , , FF, and are extracted from Figure 9(a) and summarized in Table 3. The Pt flexible DSSC has the largest efficiency as observed in the glass based DSSCs. The efficiency of M-CNTs flexible DSSC (~2.31%) is higher than the U-CNTs flexible DSSC (~1.11%). CV curves in Figure 9(b) suggest that the M-CNTs/plastic film generates the better electrocatalytic activity than that of the U-CNTs film. Two possible factors limiting the U-CNTs catalytic activity are a low amount of CNTs coated on the ITO/PEN substrate and no carboxylic group presented on the nanotube surface. Comparing to the glass based DSSCs, the efficiency of the flexible solar cells is poorer than those of the glass based DSSCs. Three factors that minimize the flexible DSSC performances are the higher sheet resistance of the conductive plastic (60 Ω/sq) than that of the conductive glass (15 Ω/sq), the thinner TiO2/ITO/PEN film (~2.1 μm) than that of the TiO2/FTO film (~9.2 μm), and the less amount of dye loading on the TiO2/ITO/PEN film (~5.69 × 10−8 mol/cm2) than that of the TiO2/FTO film (~10.50 × 10−8 mol/cm2).


Counter electrode (V) (mA/cm2)FF (%)

Unmodified-CNTs0.724.930.311.11
(U-CNTs/ITO/PEN)

Modified-CNTs0.766.030.512.31
(M-CNTs/ITO/PEN)

Pt sputter0.766.370.572.67
(Pt/ITO/PEN)

4. Conclusion

The low temperature carbon nanotube film was coated on the conductive glass and conductive plastic substrates, and they exhibit the potential application as the DSSC counter electrode. The efficiency of the M-CNTs glass and plastic based DSSCs is ~5.66% and ~2.11%, respectively, which is larger than those of the U-CNTs glass and plastic based DSSCs which are ~4.73% and ~1.11%, respectively. This is because M-CNTs are surrounded by the active carboxylic groups on the surfaces and are well connected to the substrates, leading to the high film electrocatalytic activity and the low charge-transfer resistance as evidenced by CV and EIS, respectively.

Conflict of Interests

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

Acknowledgments

This work receive scholarship under the the Post-doctoral Program from Research Affairs and Graduate School, Khon Kaen University (58227). This work was supported by the Thailand Research Fund through The Royal Golden Jubilee Ph.D. Program (PHD/0080/2554), by the Thailand Research Fund and Khon Kaen University (RSA5880035), by the Nanotechnology Center (NANOTEC), NSTDA, Ministry of Science and Technology, Thailand, through its program of Center of Excellence Network, Center for Alternative Energy Research and Development, Khon Kaen University, by the Integrated Nanotechnology Research Center, Khon Kaen University, by the Higher Education Research Promotion and National Research University Project of Thailand, Office of the Higher Education Commission, through the Advanced Functional Materials Cluster of Khon Kaen University, and by the Thailand Center of Excellence in Physics, CHE, Ministry of Education, Bangkok, and Energy Policy and Planning Office, Ministry of Energy, Bangkok, Thailand.

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Copyright © 2016 Wasan Maiaugree 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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