Thi Hiep Han†
a,
Nazish Parveen†a,
Sajid Ali Ansaria,
Jun Ho Shimb,
Anh Thi Nguyet Nguyenb and
Moo Hwan Cho*a
aSchool of Chemical Engineering, Yeungnam University, Gyeongsan, Gyeongsangbuk-do 38541, Republic of Korea. E-mail: mhcho@ynu.ac.kr; Fax: +82-53-810-4631; Tel: +82-53-810-2517
bDepartment of Chemistry, Daegu University, Gyeongsan, Gyeongsangbuk-do 38453, Republic of Korea
First published on 25th October 2016
Platinum nanoparticles (PtNPs) have long been regarded as the benchmark catalyst for the oxygen reduction reaction (ORR) in the cathode of microbial fuel cells (MFCs). On the other hand, the practical applications of these catalysts are limited by the high cost and scarcity of Pt. Therefore, developing an alternative catalyst to PtNPs for efficient ORR activity is essential for meeting the future demands for practical applications in MFCs. In this study, sulfur-doped graphene (S-GN) was synthesized via the environmental friendly, economical and facile one pot electrochemical exfoliation of graphene in a unique combination of electrolytes, which both catalyzed the exfoliation reaction and acted a sulfur source. The initial activity of S-GN as an ORR active catalyst was examined by cyclic voltammetry (CV), which showed that the as-synthesized S-GN exhibited better ORR activity than the plain material. Furthermore, the application of S-GN as a cathode material was also studied in MFCs. The results showed that the MFC equipped with the S-GN cathode produced a maximum power density of 51.22 ± 6.01 mW m−2, which is 1.92 ± 0.34 times higher than that of Pt/C. The excellent performance of S-GN as a cathode catalyst in MFCs could be due to the doping of graphene with heteroatoms, which increased the surface area and improved the conductivity of graphene through a range of interactions. Based on the above MFC performance, the as-synthesized S-GN catalyst could help reduce the cost and scale up the design of MFCs for practical applications in the near future.
On the other hand, the practical applications of Pt-based ORR electrode catalysts are limited by its susceptibility and CO deactivation,5,6 as well as the high cost of Pt, sensitivity to poisoning, and the limited reserves of Pt in nature.6,7 Therefore, it is important to develop an efficient and low cost catalyst for an effective ORR using a simple and cost effective method, which will be helpful in the design of MFCs for future applications.
The innovation of graphene has opened up a new era of 2-dimensional (2D) structures in the field of science and technology. Graphene is a building block for carbon materials of all other dimensionalities, such as 1D nanotubes, and 3D graphite. This unique planar structure of graphene has attracted considerable attention worldwide for its promising applications in a range of fields, such as electrical, electrochemical, supercapacitor, photochemical, optical, etc.8 Owing to its large surface area, rich electronic states, graphitic structure, and good mechanical properties, graphene-based materials have played important roles in non-platinum-based catalysts in several fields.9–15
In recent years, single or multi-atom doped graphene has been studied widely as a good catalyst for the ORR in MFCs, which exhibited better catalytic performance than pristine graphene.6,9,16 Among them, nitrogen-doped graphene has attracted considerably more attention because of its better electrocatalytic activity, long-term stability, and comparable performance compared to the benchmark Pt catalyst. Some studies have also reported that nitrogen-doped graphene synthesized by various different methods worked well in real MFC systems. On the other hand, its catalytic performance in the ORR and stability are unsatisfactory, which limit its utilization as an effective electrode material for a range of purposes.6,16–19 These studies reported that the MFCs system catalyzed by nitrogen-doped graphene performs better than that of commercial platinum nanoparticles on a carbon black (Pt/C) catalyst.
More recently, S-GN synthesis with high catalytic performance has attracted considerable interest in catalysts for the ORR.20–24 The high activity of the ORR of S-GN was attributed mainly to highly graphitized structures, S-related active sites, and hierarchically porous textures.23 Therefore, many studies induced catalytic behavior in graphene by the introduction of sulfur in the graphene matrix using a range of methods. Despite this, the synthetic procedure involved in the synthesis of S-GN is limited by the many steps, high running cost, and hazardous chemicals. To solve these problems, a recent study reported the one-step synthesis of S-GN using the electrochemical exfoliation technique in a unique combination of electrolytes, where the electrolyte acted as a sulfur source and also catalyzed the exfoliation reaction. The above-synthesized S-GN were characterized by X-ray diffraction (XRD), Raman spectroscopy, and X-ray photoelectron spectroscopy (XPS), which clearly revealed the presence of the S atom in the graphene sheet. Briefly, the interlayer distance obtained from the XRD pattern clearly showed a slight increase in the interlayer distance of S-GN after sulfur doping. The high-resolution XP spectra of S 2p displayed three characteristic peaks. The 2p3/2 peaks observed at a binding energy (BE) of 163.5 eV, 164.5 eV, and 168.0 eV were assigned to the different types of bonding, which are a clear indication of the presence of sulfur in S-GN. This study extended this approach further to synthesize S-GN and examine the ORR catalytic activity and real power generation in MFCs. The ORR activity of the as-synthesized S-GN electrode was examined by CV and the performance was compared with that of the commercially available Pt/C. The CV results showed that the electrode coated with S-GN exhibited much better performance than commercially available Pt/C. After the initial assessment by CV, the real assessment as an ORR catalyst was performed in a MFC equipped with the S-GN catalyst. The enhanced power generation in the MFC equipped with S-GN compared to the benchmark catalyst was attributed to the high surface area, conducting behavior, and different interactions between the sulfur and graphitic carbon. This study further highlights the potential applications of S-GN in a range of fields.
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1 ratio). The distance between the two graphite rods were kept to ∼2 cm throughout the electrochemical process. The entire process was conducted under ultra-sonication bath conditions. After 3 hours, the dissociated exfoliated graphite sheet was filtered under suction, and washed with excess water and ethanol to remove the impurities. Subsequently, the prepared S-GN was dried at 80 °C, further heated to 120 °C for 6 h, and stored in a desiccator for further experiments.
The S-GN-coated cathode electrode was prepared by mixing 90 wt% of the S-GN catalyst with 10 wt% of Nafion binder in 5 mL of ethanol and sonicated further for 60 min. The above well-dispersed suspension was coated on carbon paper, 2.5 × 4.5 cm in size, and dried at room temperature. For comparison, the carbon paper coated with commercial Pt/C was prepared using the same method with the same loading.
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100. The medium used to inoculate the bacteria and fill the anode chamber was purged with nitrogen gas for 10 min to remove any dissolved oxygen present.
The cathode chamber was filled with a 50 mM phosphate-buffered saline (PBS pH 7) solution (NH4Cl, 0.31 g L−1; KCl, 0.13 g L−1; NaH2PO4·2H2O, 3.32 g L−1; Na2HPO4·12H2O, 10.36 g L−1) and purged continuously with air at 150 cm3 air per min. The carbon paper coated with the S-GN or Pt/C catalyst was used as the cathode electrode. To avoid contamination, the MFCs were autoclaved at 121 °C for 30 min prior to set-up and all experiments were maintained under sterile conditions. The electrodes were hung on titanium wire and connected to an external resistance box with a fixed load of 1000 Ω. The experiments were duplicated to assess the reproducibility of the data. Each set of experiments consisted of three separate MFCs: one with a carbon paper cathode without a catalyst, one with the S-GN catalyst, and the other with a commercial Pt/C catalyst.
000 Hz. CV (scan rate of 10 mV s−1) was conducted in a three-electrode with platinum plate as the counter electrode, and Ag/AgCl 3 M KCl as the reference electrode. S-GN or Pt/C-coated carbon paper was used as the working electrode. The working electrodes for the electrochemical measurements were prepared in a similar manner, as mentioned above.
The linear sweep voltammetry (LSV) experiments using a rotating disk electrode (RDE) were performed using the methodology reported elsewhere.27 All electrochemical RDE experiments were carried out using a RDE-2 of BASi electrochemical analyzer (Bioanalytical Systems Inc., West Lafayette, IN). Prior to coating with the catalysts, the glassy carbon rotating disk working electrode (0.071 cm2) was wet-polished on an Alpha A polishing cloth (Mark V Lab) using 0.3 and 0.05 μm aluminum slurries, sequentially. The electrode was then rinsed with distilled water and finally sonicated in distilled water for 30 s to remove the residual aluminum slurry from the electrode surface. All RDE experiments were conducted in a 50 mM PBS solution, pH 7 saturated with either oxygen or nitrogen at a scan rate of 10 mV s−1 and a potential range from −0.6 to −0.6 V vs. a saturated calomel reference electrode (SCE) with a Pt wire counter electrode. The ORR currents were recorded at electrode rotating speeds ranging from 400 to 3600 rpm.
The onset potential, capacitance and sharpness of the oxygen reduction peak obtained from the CV are important for evaluating the ORR activity.28 The first observation is that the CVs of S-GN showed a larger background current than Pt/C, indicating that S-GN has a higher capacitance current, which is in agreement with previous work25 and the EIS data presented below. Therefore, the as-synthesized S-GN can store more electrons for the ORR. Furthermore, although the onset potential of S-GN is more negative than that of Pt/C (−0.22 vs. 0.15 V), the current peak of S-GN was much sharper with an enhanced current compared to Pt/C.
The LSV measurements on a RDE were performed to further examine the ORR activity of the as-synthesized S-GN. The current density of Pt/C and S-GN increased with increasing rotation rate from 400 to 3600 rpm (Fig. 2a and b). The LSV measurement at 1600 rpm (Fig. 2c) revealed an onset potential of S-GN of −0.15 V, which was more negative than that of Pt/C (0.22 V). This is evidently compared to the onset potential observed by CV and previous study.23
The Koutecky–Levich (K–L) plots at a potential of −0.5 V showed good linearity, indicating first-order kinetics with respect to the reactant concentration. The number of electrons transferred (n) for the ORR calculated from the slope of the K–L plots on the base of the K–L equation as following,27
According to the number of electrons transferred from the RDE measurement, the mechanism of the ORR on the surface of S-GN in the cathode of the MFC was partially revealed. Fig. 3 presents a schematic diagram of the operation principal of the MFCs with ORR mechanism of the S-GN in the cathode. The electrochemically active biofilm (EAB) on carbon paper oxidizes the carbon source to produce electrons and protons. The protons then permeate to the cathode chamber through the Nafion membrane, whereas the electrons are transferred from the anode to the cathode through an external circuit. These combined processes produced a reasonable amount of electricity, which was measured by a multi-meter. In the cathode, the general ORR can occur simultaneously through a direct four-electron transfer pathway and two-electron pathway over the equipped catalyst-coated electrode, according to the overall reaction described below.29
| Two-electron transfer pathway: O2 + 2H+ + 2e− → H2O2 |
| Four-electron transfer pathway: O2 + 4H+ + 4e− → 2H2O |
The EIS technique is the most valuable technique for examining the charge transfer resistance phenomenon occurring in the electrodes and electrolyte interface. Fig. 4 presents a Nyquist plot of S-GN-coated carbon paper, Pt/C-coated carbon paper, and plain carbon paper (no catalyst) electrodes. Charge transfer through the electrode/electrolyte interface is smaller with a smaller semicircle at the middle frequency.30 As shown in Fig. 4a, the diameter of the semicircle of the plain carbon paper electrode was quite large (165
915.9 Ω cm2), indicating the high charge transfer resistance of the plain carbon paper. With the presence of catalysts, the charge transfer resistance was reduced significantly to 4.83 Ω cm2, even though the semicircles were not observed clearly. As shown in Fig. 4c, the appropriate equivalent fitting circuit comprised three components: ohmic resistance (R1), charge transfer resistance (R2), and constant phase element (CPEdl). The ohmic resistance of S-GN was similar to Pt/C at approximately 49.09 Ω cm2. The charge transfer resistance of the electrode coated with the S-GN or Pt/C catalysts was very small compared to the plain electrode, which was attributed to the high electrical conductivity of those catalysts. A significant difference in the CPEdl value was observed among S-GN (0.082, n = 0.92), Pt/C (0.0082, n = 0.8), and without catalyst (0.000038 sn Ω−1 cm−2, n = 0.94). The higher CPEdl represented the less resistive and higher capacitive double layers of S-GN compared to Pt/C.31
Fig. 5 presents the polarization tests curve and power density curve of the plain carbon paper, Pt/C-coated carbon paper, and S-GN-coated carbon paper. As expected, the MFC without the catalyst produced a very low power density of 1.96 ± 2.23 mW m−2. The MFC equipped with the S-GN catalyst and Pt/C catalyst produced a maximum power density of 51.22 ± 6.01 mW m−2 and 26.69 ± 6.52 mW m−2, respectively. Compared to the plain carbon paper and Pt/C-coated carbon paper catalyst, the power density of the S-GN-coated carbon paper was quite high. The S-GN-coated carbon paper showed double the power output of the commercially available Pt/C catalyst. Moreover, the OCV of the MFC equipped with the S-GN catalyst (0.87) was also higher than that of the Pt/C catalyst (0.65) and plain carbon paper electrode (0.55). This improved power generation in the MFC was attributed to the conducting behavior of the heteroatom-doped graphene, which is a well-established ORR catalyst in MFCs. MFCs are sustainable and prominent energy-producing devices. Therefore, the long-term durability of the prepared catalyst electrode is also an important factor. The durability of the prepared catalyst was also examined under similar conditions, i.e., the cell voltages of the cathode catalyst-equipped MFCs were examined as a function of time at a fixed external resistance. The fresh LB media was replaced whenever the cell voltage of the studied MFCs was decreased to 0.05 V. The minimal voltage generation was observed for the plain carbon paper electrode, which compelled its modification by the highly efficient ORR catalytic materials. The higher voltage generation observed on the S-GN catalyst than the Pt/C catalyst showed that S-GN has higher ORR catalytic activity than Pt/C. Fig. 6 clearly shows that the S-GN-coated carbon exhibited a stable voltage response with time compared to the other catalysts: coated and uncoated carbon paper. The S-GN-coated carbon also showed high catalytic activity for up to continuous 4 cycles (approximately 400 h of operation). A previous study also reported that the as-synthesized S-GN has excellent electrochemical stability.25
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| Fig. 6 Power density response with time of the MFCs with different catalysts. The sharp decrease in voltage indicated the complete consumption of the carbon source and new media was replaced. | ||
On the other hand, for a broader context of the work, the performance of the MFC with the S-GN was compared with that of other reported cathodic catalysts, as shown in Table 1. In addition to its own electrocatalytic property, the MFC performance depends on many other factors, such as MFC configuration, electrode material, biocatalyst, etc. Therefore, each catalyst shows a different performance in MFC. Compared to other catalysts prepared, such as Pani–MnO2 and PtOx@M-TiO2, the as-synthesized S-GN exhibited superior performance in the cathode of the same MFCs system using the same experiment set-up and under the same conditions. The as-synthesized S-GN produced a 12.3 times higher power density than PtOx@M-TiO2 (ref. 32) and was comparable to a power density of Pani–MnO2.33 The performance of the as-synthesized S-GN was also compared with that of a commercial 10 wt% Pt 0.5 mg cm−2 on carbon paper electrode purchased from Fuel Cell Earth USA, in which the catalyst synthesis and electrode preparation procedure were optimized and well controlled on a commercial scale. As a result, a maximum power density of 57.6 mW m−2 was produced by the MFC equipped with a commercial 10 wt% Pt 0.5 mg cm−2 on carbon paper electrode (data not shown), which is similar to previous reports using the same MFC design, experimental set up, and S. oneidensis as a biocatalyst.26,34 This shows that the electrocatalytic activity of as-synthesized S-GN toward the ORR is comparable to that of the commercial 10 wt% Pt 0.5 mg cm−2 on carbon paper electrode from Fuel Cell Earth. The better ORR response of commercial 10 wt% Pt 0.5 mg cm−2 on carbon paper from Fuel Cell Earth compared to that of commercial powder Pt/C-coated carbon paper might be due to the optimized preparation procedure. This means that the ORR activity of the as-synthesized S-GN can be improved by optimizing the synthesis and electrode preparation. These optimization experiments will be carried out near in the future.
| Cathodic catalyst | Anode/cathode material | MFC configuration | Power density (catalyst vs. Pt/C, mW m−2) | Biocatalyst | Reference |
|---|---|---|---|---|---|
| Co-naphthalocyanine | Carbon paper | Two-chamber | 64.7 vs. 81.3 | Anaerobic sludge | 35 |
| Pyrolyzed iron ethylenediaminetetraacetic acid | Carbon brush | Air-cathode | 1122 vs. 1166 | Mixed culture | 36 |
| Carbon nanotube supported MnO2 | Carbon cloth | Air-cathode | 97.8 vs. 152 | Mixed culture | 37 |
| MnO2–graphene nanosheet | Carbon felt/carbon paper | Air-cathode | 2083 vs. 1714 | Anaerobic sludge | 15 |
| Nanotubular MnO2/graphene oxide composites | Carbon cloth | Air-cathode | 3359 vs. 3059 | Anaerobic sludge | 11 |
| Iron- and nitrogen-functionalized graphene | Carbon felt/carbon paper | Air-cathode | 1149.8 vs. 561.1 | Anaerobic sludge | 12 |
| Cobaltosic oxide and nitrogen-doped graphene | Glass carbon | Two-chamber | 1340 vs. 1470 | S. oneidensis | 30 |
| Nitrogen-doped graphene/CoNi alloy | Carbon brush/carbon cloth | Two-chamber | 2000 vs. 2600 | Mix culture | 38 |
| Cobalt oxide/nanocarbon hybrid materials (graphene and carbon nanotube) | Carbon cloth | Air cathode | 469 vs. 603 | Anaerobic sludge | 39 |
| Nitrogen- and sulfur-co doped porous carbon nanosheets | Carbon brush/carbon cloth | Two-chamber | 1500 vs. 2300 | Mixed culture | 40 |
| Nitrogen-doped carbon | Carbon brush/carbon paper | Air cathode | 1159.3 vs. 858.59 | Anaerobic sludge | 41 |
| Nitrogen-doped carbon nanosheet on graphene | Graphite fiber brush/stainless steel mesh | Air cathode | 1041 vs. 584 | Mixed culture | 18 |
| Nitrogen-doped activated carbon | Carbon cloth | Two-chamber | 650 vs. 450 | Mix culture | 21 |
| Pani–MnO2 composite | Carbon paper | Two-chamber | 58.8 vs. — | S. oneidensis | 32 |
| PtOx@M-TiO2 nanocomposites | Carbon paper | Two-chamber | 4.34 vs. — | S. oneidensis | 33 |
| S-Doped graphene | Carbon paper | Two-chamber | 51.22 vs. 26.69 | S. oneidensis | This study |
It is well known that the rotation present in RDE measurements grants optimal conditions without the usual diffusion limitations found in MFC cathodes. Note that the experimental conditions in MFCs and LSVs measurement were completely different in this study. The MFCs were conducted at the stationary phase in PBS electrolyte with air sparging. In contrast, the LSVs by RDE were performed at high rotating speeds with oxygen sparging, in which the oxygen diffusion limitation was eliminated. In addition, the differences in catalyst layer preparation, the amount of binder, the thin layer of catalyst used in RDE measurement, compared to the large amount of catalyst used in MFC cathodes, can increase diffusion and electrical conductivity limitation.42 Therefore, it is difficult to compare RDE data with performance result from real MFC experiments.
Further information from CV in which experiment condition are more similar to MFC (same working electrode and applied air sparging under stationary conditions) may simulate the MFCs performance more precisely. In LSVs under no oxygen diffusion limitation, the current density peak of Pt/C was sharper than S-GN. When the LSVs were recorded without rotation, the LSVs were similar to the CV measurements, the current density peak of S-GN was sharper than that of Pt/C, which is well correlated with MFC result. Therefore, the ORR performance of a catalyst in a real MFC is more reliable, meaningful and practical than its performance in a three-electrode system LSV by RDE.
There are several reasons for the better performance of S-GN compared to Pt/C in MFCs. As discussed above, diffusion limitation is the key factor causing the dissimilar performances of S-GN and Pt/C in MFCs. The surface area of S-GN was 2.77 times larger than that of the commercial Pt/C (261 m2 g−1 vs. 93.67 m2 g−1). The high surface area causes the easy transfer of electrolyte ions and O2 during the ORR.41 Moreover, as presented above in the CV measurement and EIS data, S-GN has higher capacitance than Pt/C, which means that S-GN can store more electrons for the ORR. Furthermore, the formation of different types of bonds between the dopant and graphene matrix during exfoliation may also play an important role in enhancing the catalytic ORR. For example, Yang et al.20 reported that S-GN has high ORR activity due to the presence of different types of C–S interactions, which provides active sites for the catalytic ORR. They also attributed the ORR activity to the different C–S interactions, which may introduce a positive charge on the neighboring carbon atoms and create centers for the ORR. Similarly, in the present case, different interactions occur due to sulfur doping, which lead to the formation of a large number of catalytic active sites for promoting the ORR activity in the cathode chamber of the MFC. In addition, heteroatom doping in the graphitic materials also decreases the electroneutrality of graphitic materials. This leads to the development of a positive charge side for the adsorption of O2, which is also favorable for the high ORR activity.43 Overall, the presence of different interactions between similar electroneutrality atoms, i.e., carbon and sulfur, are responsible for the high ORR activity of S-GN in the cathode of MFCs. These results are also in accordance with previous studies.20,29,43 On the other hand, the precise and detail relationship between the catalytic activity and the S-GN structure is quite complicated and requires further investigation.
Footnote |
| † Thi Hiep Han and Nazish Parveen contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2016 |