Leiyu Fengab,
Xutao Chena,
Yue Caoa,
Yunzhi Chena,
Feng Wanga,
Yinguang Chen*a and
Yin Liuc
aState Key Laboratory of Pollution Control and Resources Reuse, School of Environmental Science and Engineering, Tongji University, Shanghai 200092, People's Republic of China. E-mail: yg2chen@yahoo.com; Fax: +86-21-65986313; Tel: +86-21-65981263
bResearch & Service Center for Environmental Industry, Yancheng 224051, Jiangsu Province, People's Republic of China
cBohai Drilling Engineering Co., Ltd., China National Petroleum Corporation, Tinajin, 300457, People's Republic of China
First published on 6th March 2017
Non-noble cathode catalysts with high performance and low cost are vital for large-scale applications of microbial fuel cell (MFC) technology. In this study, pyridinic and pyrrolic nitrogen-rich ordered mesoporous carbon (PPN-OMC) synthesized by a facile strategy were successfully applied as cathode catalysts in MFCs. In MFCs with the currently used material, the maximum power density is 1420 ± 15 mW m−2, which is comparable to a conventional platinum catalyst (Pt/C, 1425 ± 15 mW m−2), and the stability of the power output is even better. Mechanism exploration for efficient and stable power generation by electrochemical measurements revealed that the resulting PPN-OMC catalyst displayed superior electrocatalytic activity (nearly 100% of a four-electron oxygen reduction reaction (ORR) pathway) and durability (nearly no activity change after 100000 potential cycles) for ORR in a neutral phosphate buffer solution (PBS). Further characterization of PPN-OMC implied that the existence of nitrogen substitution with high pyridinic and pyrrolic ratios of 39.8% and 35.1% and a large specific surface area of 1160 m2 g−1 benefitted the electrocatalytic activity and durability. MFCs with the PPN-OMC catalyst produced power much less expensively than those with Pt/C, indicating that the present PPN-OMC material might be used as an excellent alternative to Pt/C in MFCs.
As a result, the global research efforts on MFCs have turned towards the search for a broad range of alternative cathode catalysts based on non-precious metals or their oxides,6 microorganisms,7 and metal-free doped carbons.8 Among these alternative catalysts, metal-free, heteroatom-doped carbon materials have been extensively demonstrated as having the greatest potential due to their excellent electrocatalytic activity and durability as well as the fact that non-precious metal catalysts frequently suffer from dissolution, sintering and agglomeration.
Usually, the heteroatoms used for doping carbon include nitrogen, phosphorus, boron, and sulfur. Among the heteroatom-doped carbon materials, N-doping has been the most popular choice.9 The incorporation of N can enhance the electron-donor property of the carbon matrix and introduce a certain amount of active sites, resulting in an improvement in the ORR activity. Until now, however, the ORR activities of most N-doped carbons were still on a less competitive level compared to Pt catalysts due to insufficient catalytic active sites (functional nitrogen) and a limited surface area, even when the N content was high.10–12 Usually, there are three types of N atoms in the N-doped carbons, which are pyridinic, pyrrolic, and quaternary N, whereas only the pyridinic and pyrrolic forms have planar structures and have been proven to be active in the ORR.13,14 In contrast, the quaternary N atoms, which usually possess a 3D structure and lead to the low electrical conductivity of N-doped materials due to the interruption of their p–p conjugation, are thought to be predominantly responsible for the poor catalytic activity.15–17 Therefore, the synthesis of N-doped carbon materials with more planar pyridinic and pyrrolic N atoms and fewer quaternary ones is very important for the preparation of ORR-active catalysts. Recently, nitrogen-doped ordered mesoporous carbon (N-OMC) has been reported to have a large surface area, tunable pore size and huge pore volume, which enhance its ORR activity, and it is being considered as a promising alternative to Pt/C for ORR in fuel cell systems.14 However, the documented synthesis methods for N-OMC with a relatively larger surface area are complex,18 and N-OMC materials with a high content of both pyridinic and pyrrolic N and a large surface area for more efficient oxygen reduction has seldom been reported.
In this study, the ordered mesoporous metal-free carbon with a high content of both pyridinic and pyrrolic N and a large surface area (denoted as PPN-OMC for simplicity) prepared by a facile method was employed as a cathode catalyst in microbial fuel cells. The performance of the power output in MFCs with the PPN-OMC catalyst was first evaluated in terms of power density and cell voltage. For comparison, the performance of MFCs with commonly used Pt/C was also investigated. Then, a conceptual explanation of efficient and stable power generation in MFCs with the PPN-OMC catalyst was proposed based on the detailed characterization of the synthesized material and MFCs. This current novel catalyst might offer a new potential for constructing high-performance and less expensive cathodes that are crucial for the large-scale application of MFCs for energy recovery.
All MFC reactors were inoculated with suspended bacteria from an acetate-fed reactor that had been operating for more than two years and was filled with acetate-laden synthetic wastewater containing 1.0 L of neutral 50 mM phosphate buffer solution (PBS), CH3COONa, 1000 mg; NH4Cl, 310 mg; KCl 130 mg; and minerals and vitamins as described by Lovley and Phillips.22 After the voltages in the MFCs were stable, the inoculum was omitted from the solution, and the experimental data were recorded. The external resistance was fixed at 1000 Ω (except as noted), and all the reactors were operated in batch mode at 25 ± 1 °C.
The electrochemical experiments were carried out on a computer-controlled electrochemical workstation (Autolab PGSTAT 302N, Metrohm) in the neutral 50 mM PBS. The three-electrode cell consisted of an Ag/AgCl electrode (3 M KCl-filled) as the reference electrode, a platinum wire as the counter electrode, and a glassy carbon (GC) electrode/rotating ring-disk electrode (RRDE) (Pine Research Instrument Co., USA) loaded with various catalysts as the working electrode. During the preparation of the working electrode, 5.0 mg of the as-synthesized catalyst was mixed with 50 μL of Nafion solution (5.0% Nafion in ethanol) and 450 μL of deionized water. A 3.0 μL suspension of the sonicated mixture was applied onto the GC part of the RRDE, which was successively polished with 1.0 and 0.3 μm alumina powder followed by rinsing thoroughly with deionized water, and then fully dried. The catalyst loading was approximately 0.5 mg cm−2. Cyclic voltammogram (CV) measurements were carried out to characterize the electrochemical activities on the electrode surface by measuring the current response on the electrode surface to a specific range of potentials with a scan rate of 0.1 V s−1. During the RRDE tests, the potential was varied from −0.5 to 0.5 V vs. Ag/AgCl at a potential sweep rate of 0.01 V s−1. Before the electrochemical measurements, oxygen gas was saturated in the electrolyte by bubbling the gas for 30 min. All electrochemical experiments (except as noted) were carried out at 25 ± 1 °C.
The electrical conductivities of PPN-OMC and Pt/C were determined at 25 ± 1 °C according to the method of Paraknowitsch et al.23 Cathode potentials were measured in chronopotentiometry tests by applying a constant current for 60 min and recording the stable value of the response potential. The catalyst-coated side of the cathode was placed facing the solution, with the uncoated side exposed directly to air. A curve of cathode potentials against current densities was used to evaluate the performance of the cathodes. A higher potential at the same current density indicates a better performance of the cathode catalyst. The internal resistance (Rin) of the microbial fuel cells (MFCs) was determined by electrochemical impedance spectroscopy (EIS) according to the method of Bard et al.24 Impedance measurements were performed with an open circuit voltage (OCV) over a frequency range of 0.05 to 105 Hz with a sinusoidal perturbation amplitude of 10 mV. After the MFCs generated the power stably, the external resistance (Rext) was in turn shifted in the range of 10 to 104 Ω to demonstrate the electrochemical polarization and power curves. Data for each resistance were collected after the cells were operated stably for 5 h.
Fig. 1 Comparison of cathode potentials with PPN-OMC and Pt/C at a catalyst loading of 0.5 mg cm−2. Error bars represent standard deviations of duplicate tests. |
Then, the performance of the PPN-OMC as a cathode catalyst was evaluated in the MFCs based on the output of the power energy. For comparison, the same investigation was carried out in MFCs equipped with Pt/C as the cathode catalyst. The obtained polarization curves and power densities are presented in Fig. 2. The cell voltage generated in the PPN-OMC-MFCs was 573 ± 15 mV at an external resistance of 1000 Ω, which is close to that in the Pt/C-MFCs (575 ± 18 mV). Also, as observed in Fig. 2A, the MFCs with PPN-OMC produced a maximal power density of 1420 ± 15 mW m−2, which was almost the same in the Pt/C-MFCs (1425 ± 15 mW m−2). The power output in the PPN-OMC-MFCs was comparable to that in the Pt/C-MFCs. In the previous studies, lots of alternative ORR catalysts, such as transition metals,6–8 etc., have attempted to replace or reduce Pt/C as the cathode catalyst in MFCs. As far as we know, however, the capacity of power generation in the presence of those catalysts was unsatisfying and much lower than that in the MFCs with Pt/C as the cathode catalyst.
Fig. 2 (A) Power density and cell voltage in the PPN-OMC-MFCs and Pt/C-MFCs. (B) Power density as a function of operation time at 1000 Ω. Error bars represent standard deviations of duplicate tests. |
The results of the long-time durability of the two MFCs are presented in Fig. 2B. In the PPN-OMC-MFCs, after operation for 51 days, the maximal power density decreased from 998 ± 13 to 925 ± 10 mW m−2, corresponding to about a 7.3% deterioration. Accordingly, the maximal power density in the Pt/C-MFCs declined from 1008 ± 15 to 808 ± 10 mW m−2, a deterioration of more than 19.8%, which was much higher than that in the PPN-OMC-MFCs. Typically, the decrease in the power density in the MFCs is due to the deterioration of the electrocatalytic activity of the cathode catalyst and the proton limitation caused by biofilm formation on the cathode surface. In this study, the thicknesses of the biofilms on the cathodes of the PPN-OMC-MFCs and Pt/C-MFCs were about 0.1 cm after 50 days, which might be one of the reasons for the decrease in the maximum power density. However, the drop of the power density in the MFCs without the cathode catalyst (caused by proton limitation only) was found to be about 1.8 ± 0.2%, revealing that the decrease in the power density in the PPN-OMC-MFCs and Pt/C-MFCs was mainly attributed to the deterioration of the electrocatalysts. The stability performance of the power generation in the PPN-OMC-MFCs outperformed that in the Pt/C-MFCs. Overall, the PPN-OMC-MFCs displayed a comparable performance to the Pt/C-MFCs in terms of cell voltage and power density with an even better power generation stability.
To quantify the ORR electron transfer pathway, RRDE measurements for PPN-OMC/GC were performed in the O2-saturated neutral PBS under steady-state conditions, while that for Pt/C/GC served as the contrast. As shown in Fig. 3B, one-step and four-electron pathways for ORR occurred at the Pt/C/GC. Similar to Pt/C/GC, the PPN-OMC catalyst also exhibited a one-step process for ORR at an onset potential of about 0.40 V, which was confirmed by the nearly negligible corresponding current for HO2− oxidation recorded at the Pt ring electrode (dash line). According to Bard et al., for a diffusion-controlled process, the transferred electron number (n) per oxygen molecule in the ORR process could be estimated by the Randles–Sevcik equation.24
ip = 0.4463nFAC(nFvD/RT)1/2 | (1) |
Also, continuous potential cycling was performed to investigate the electrocatalytic durability of the current PPN-OMC catalyst towards ORR. As can be seen in Fig. 3C, almost no obvious decrease in the current density occurred after 100000 continuous cycles between −0.5 V and 1.0 V in the O2-saturated PBS electrolyte. The electrocatalytic durability of the PPN-OMC catalyst for ORR was superior. When used in the bioelectrochemical systems, the metabolite tolerance ability is a crucial feature of catalysts. Thus, in the present study, the crossover behavior of the synthesized PPN-OMC was examined by adding 5 mM sodium formate, a typical metabolite in bioelectrochemical reactors, to the ORR system (Fig. S3†). It was observed that the ORR current density remained largely unchanged after the addition of sodium formate, which suggested that the PPN-OMC catalyst possessed an excellent tolerance to the metabolite crossover effect. The as-prepared PPN-OMC material might be a perfect electrocatalyst with a high metabolite tolerance ability when applied in biological systems, although the tests of the tolerance ability of PPN-OMC for other metabolites, such as sulphide and methanol, still need to be conducted.
It has been reported in the literature that the internal resistance plays an important role during the generation of power energy in MFCs.20 In the present investigation, therefore, the internal resistance of MFCs with different catalysts was investigated based on the EIS analysis. It was found that the Rin of MFCs with PPN-OMC and Pt/C were 89 ± 2 and 85 ± 3 Ω, respectively. Usually, the internal resistance of a MFC reactor consists of two parts: the electrolyte ohmic loss due to the movement of electrons through the electrolyte, and the electrode ohmic loss caused by the movement of electrons through the electrode and wires. In this study, due to the fact that the two MFC reactors had the same configuration, such as the anode material, electrode distance, etc., the difference in the Rin between the PPN-OMC-MFCs and Pt/C-MFCs was derived from the diversity of the electrical characteristics, especially the conductivity, between the synthesized PPN-OMC and Pt/C. The electrical conductivities of the PPN-OMC and Pt/C cathodes were measured to be about 40 ± 2 and 45 ± 2 S cm−1, respectively. The lower conductivity of the PPN-OMC cathode resulted in the slightly higher Rin of the PPN-OMC-MFCs. In this case, the power generation performance was analogous to that in the Pt/C-MFCs.
The nitrogen adsorption–desorption isotherms of the PPN-OMC material are shown in Fig. 5A. Type IV curves with a sharp capillary condensation step and a H1-type hysteresis loop were observed for the as-obtained carbon materials, which is indicative of uniform cylindrical pores. As shown in the inset of Fig. 5A, a narrow pore size distribution with a mean value of 3.8 nm was calculated from the adsorption branch using the BJH model, and a specific surface area of 1160 m2 g−1 was exhibited. In the literature, the reported specific surface area of PPN-OMC with a high content of nitrogen, especially pyridinic and pyrrolic nitrogen, was usually less than 1000 m2 g−1,23,25,26 indicating that the current strategy for PPN-OMC synthesis benefitted the improvement of the specific surface area. Usually, a PPN-OMC catalyst with a larger surface area holds more active sites to be exposed to oxygen molecules and benefits the improvement of ORR activity.
The XRD patterns were applied to characterize the structure of the mesoporous carbon, and the results are shown in Fig. 5B. The high angle region (above 2θ = 10°) of the PPN-OMC samples via the current process exhibited peaks at 2θ = 26 and 44°, which can be ascribed to (002 and 101) diffraction peaks from the graphitic pore walls, respectively. The XRD patterns indicated that the PPN-OMC sample possessed graphitic (crystalline) rather than amorphous pore walls. The small angle XRD pattern of the synthesized PPN-OMC sample is shown in the inset of Fig. 5B. A high intensity diffraction peak of (100) and two additional well-resolved diffraction peaks of (110) and (200) occurred, which can be assigned to a 2D hexagonal lattice, similar to that of the SBA-15 template, demonstrating that the mesoporous structure was retained even after the high temperature carbonization for the formation of graphitic pore walls.
To further evaluate the structure and quality of the PPN-OMC material, Raman spectroscopy measurements were taken on a Renishaw Raman spectroscope, and a typical Raman spectrum is displayed in Fig. 5C. Three main peaks were assigned, D band (∼1316 cm−1), G band (∼1594 cm−1) and 2D band (∼2653 cm−1). The G band showed a blue-shift compared to the pristine carbon black (data not shown here), which was a sign of atomic insertions. Usually, the intensity ratio of the D to G band (ID/IG) can give qualitative information on the degree of the defects, and a higher value indicates more defects present in the carbon materials. According to the Raman spectrum, the ID/IG ratio of PPN-OMC in this study was about 1.25, implying a high degree of defects in the crystalline structure of the PPN-OMC sample.
XPS measurements were performed to probe the chemical composition and nitrogen content in the PPN-OMC material. The survey scan spectrum from the XPS analysis for PPN-OMC revealed the presence of C 1s, O 1s and N 1s without any other impurities, showing that the current PPN-OMC material was completely metal-free (Fig. 6A). In the spectrum of PPN-OMC, the peaks at 285.8, 399.6, and 537.2 eV corresponded to C 1s of sp2C, N 1s, and O 1s of the absorbed oxygen, respectively, and the content of carbon, nitrogen and oxygen were measured to be about 80.0%, 16.1% and 3.9%, respectively. Generally, the reported nitrogen content in the PPN-OMC sample was less than 15.0%,27–29 suggesting that the present strategy for PPN-OMC synthesis benefited from the improvement of the nitrogen content. As PPN-OMC materials with a high nitrogen content have been demonstrated to show better physiochemical properties, such as electrocatalytic activity, electrical conductivity, etc.,14,28,29 the PPN-OMC prepared in this study might have a wide range of practical applications.
The high resolution XPS N 1s spectrum of the current PPN-OMC material is shown in Fig. 6B. It was found that the spectrum of N 1s had three components, indicating that the N atoms were in three different bonding situations. The N peaks located at around 399.3, 400.5 and 401.8 eV corresponded to the pyridinic, pyrrolic, and graphite nitrogen atoms, respectively. It is well known that the pyridinic and pyrrolic nitrogen are a kind of N that contribute one p-electron to the aromatic π-system, and they have a lone electron pair in the plane of the carbon matrix, which can increase the electron-donor property of materials. The graphite nitrogen usually represents the N atoms replacing the C atoms in the structure of the carbon material. In the N peak of the current PPN-OMC material, the content of pyridinic, pyrrolic, and graphite nitrogen was calculated to be 39.8%, 35.1% and 25.1% of the total one, which suggested that pyridinic and pyrrolic N dominated the N content of the as-prepared PPN-OMC material. In the structure of the nitrogen-doped carbon materials, the functional nitrogen responsible for ORR usually corresponds to the pyridinic and pyrrolic ones because they are obtained by doping at the edge of the carbon materials, whereas the graphite N is the result of in-plane doping.30–35 It is well known that there are three styles for O2 adsorption on the electrode surface for ORR, i.e. Griffith model, Pauling model and Yeager model.36 Meanwhile, the doping of pyridinic and pyrrolic N into graphitic sheets at the edge has been found to induce the charge delocalization of the carbon atoms, which changes the chemisorption model of O2 during the oxygen reduction.32 Thus, the following observed electrocatalytic activity and durability of the PPN-OMC catalyst was mainly due to the pyridinic and pyrrolic N-induced charge delocalization, which changed the chemisorption model of O2 from the usual end-on adsorption (Pauling model) to the side-on one (Yeager model), and it effectively weakened the O–O to facilitate the oxygen reduction on the PPN-OMC electrode.31,32
The detailed C 1s spectrum of PPN-OMC ranging from 280 to 295 eV is shown in Fig. S4.† Generally, there were three different C groups in the XPS spectrum of PPN-OMC, which were characterized by the observation of spectral peaks: C–C at 285.2 eV, C–O at 286.5 eV, and O–CO at 288.6 eV. Additionally, an obvious O 1s peak at 536.8 eV occurred for the synthesized PPN-OMC, possibly due to the adsorbed moisture, atmospheric O2, or CO2, as well as the residual oxygen-containing groups, such as carbonyl and carboxyl groups. The apparent O 1s peak was an additional advantage for the current PPN-OMC as catalysts of the ORR electrode because the nitrogen-doped carbon material with a higher O 1s content has a stronger ability for O2 adsorption, which is very important for ORR.34
Based on the above discussion, the main pathways and mechanisms of oxygen reduction in PPN-OMC-MFCs with neutral PBS as an electrolyte are proposed in Fig. 7. A four-electron pathway of the PPN-OMC catalyst for ORR in neutral PBS is favored by the side-on configuration rather than the end-on one due to the fact that doping ordered mesoporous carbon with pyridinic and pyrrolic nitrogens and a large surface area in the PPN-OMC electrode created large amounts of metal-free active sites for efficient oxygen reduction, which was one of the most important reasons for the excellent electrocatalytic activity and durability of the PPN-OMC for ORR exhibited in MFCs.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra00807d |
This journal is © The Royal Society of Chemistry 2017 |