Characteristics of Carbon Nanotubes/Graphene Coatings on Stainless Steel Meshes Used as Electrodes for Air-Cathode Microbial Fuel Cells

Hsu, Wei-Hsuan; Tsai, Hung-Yin; Huang, Ying-Chen

doi:https://doi.org/10.1155/2017/9875301

Journal of Nanomaterials

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Abstract Introduction Materials and Methods Results and Discussion Conclusions Conflicts of Interest Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2017 | Article ID 9875301 | https://doi.org/10.1155/2017/9875301

Characteristics of Carbon Nanotubes/Graphene Coatings on Stainless Steel Meshes Used as Electrodes for Air-Cathode Microbial Fuel Cells

Wei-Hsuan Hsu,¹Hung-Yin Tsai,²and Ying-Chen Huang²

Academic Editor: Genggeng Qi

Received03 Oct 2016

Revised13 Feb 2017

Accepted16 Mar 2017

Published16 Apr 2017

Abstract

Microbial fuel cells (MFCs) generate low-pollution power by feeding organic matter to bacteria; MFC applications have become crucial for energy recovery and environmental protection. The electrode materials of any MFC affect its power generation capacity. In this research, nine single-chamber MFCs with various electrode configurations were investigated and compared with each other. A fabrication process for carbon-based electrode coatings was proposed, and Escherichia coli HB101 was used in the studied MFC system. The results show that applying a coat of either graphene or carbon nanotubes (CNTs) to a stainless steel mesh electrode can improve the power density and reduce the internal resistance of an MFC system. Using the proposed surface modification method, CNTs and graphene used for anodic and cathodic modification can increase power generation by approximately 3–7 and 1.5–4.5 times, respectively. Remarkably, compared to a standard MFC with an untreated anode, the internal resistances of MFCs with CNTs- and graphene-modified anodes were reduced to 18 and 30% of standard internal resistance. Measurements of the nine systems we studied clearly presented the performance levels of CNTs and graphene applied as surface modification of stainless steel mesh electrodes.

1. Introduction

As technology advances, energy consumption and shortfalls of energy supply are inevitable. Moreover, the rise of environmental awareness has motivated the development of minimally polluting renewable energy sources, such as microbial fuel cells (MFCs). Thus, MFCs have been extensively studied in the last decade. MFCs utilize microorganisms as catalysts to decompose organic or inorganic matter and harvest electrical energy [1].

The major obstacles towards commercialization of MFC are its high cost of fabrication and low power output. The cost of MFC mainly depends on the design of reactors, membrane separator, and electrode catalysts [2–4]. A typical MFC system comprises two chambers (i.e., an anode and a cathode) separated by a proton exchange membrane (PEM). Chemical energy can be converted to electric energy through anodic oxidation and cathodic reduction. Microorganisms oxidize the organic compound and produce electrons and protons in the anode chamber. Electrons are transported to the cathode by an external circuit, whereas the protons are transferred internally to the cathode chamber through the PEM. Subsequently, the electrons and protons react with oxygen to form water. According to the energy conversion process, the electric current can be generated continuously between the anode and cathode [5–7]. To allow the easy construction, a single-chamber MFC system was proposed [8], in which the cathodic and anodic electrodes were placed in a reaction chamber and a proton exchange membrane (PEM) was fused to the cathodic surface. Later, the performance of air-cathode single-chamber MFCs was further investigated to reduce the cost of MFC, and the feasibility of MFC systems without PEM materials was demonstrated [9]. Because oxygen can pass through the cathode directly in air-cathode MFC designs, these designs reduce the cost of equipment required to regulate air exposure. Thus, a single-chamber MFC has some advantages over a traditional double-chamber MFC and has potential for development.

The power output of an MFC is affected by several factors, including the microbial inoculation, electrode materials, ionic concentration, catalyst, internal resistance, and electrode spacing [10–13]. The electrode materials play a critical role in electricity generation. An electrode with high electrical conductivity can effectively collect electrons and reduce ohmic loss. Therefore, metal electrodes are crucial for MFC systems. Conventionally, designers choose stainless steel and titanium for electrodes in MFC systems [14]. Stainless steel has the advantages of low cost and anticorrosive properties, and it has become one of the major research materials for electrodes in MFCs. However, in MFC systems, electrons are generated by metabolically and electrochemically active microorganisms at the interfaces between anodic surfaces and microbes [15, 16], and the generated electrons transfer to anode surfaces through direct contact, microbial pili, or soluble mediators [17, 18]. Thus, an electrode with a large surface area and high specific surface area can demonstrate high microbe attachment and low internal resistance [19]. To improve the attachment of bacteria on the anode, an electrode with a high specific surface area is necessary. For this purpose, numerous studies have utilized three-dimensional structures of stainless steel, such as stainless steel mesh (SSM) [20–25], stainless steel foam [26], stainless steel felt [27], and stainless steel fiber felt [28–31]. But the surface areas of this type of electrode are limited when compared with those of nanomaterial-based electrodes. Nanomaterials offer exceptionally large surface-area-to-volume ratios as well as unique electrochemical properties such as strong charge interactions with organic matter [32]. Therefore, most of the aforementioned studies have used nanomaterials for electrode modification treatment.

In recently years, carbon nanotubes (CNTs) and graphene have been intensively studied and explored in various applications for advanced technologies due to their fascinating properties, such as high electrical conductivity, surface area, and stability [33, 34]. Moreover, CNTs [21, 23, 32, 35–37] and graphene [20, 30, 37] have been used as an electrode modified material in MFC systems. Research has confirmed that SSM electrodes modified with CNTs or graphene can improve the characteristics of MFCs. For anode modification, graphene can improve electrode surface area, adhesion of bacteria, and efficiency of electron transfer [20]. Some MFCs with CNTs-SSM cathodes have achieved levels of maximum power density and Coulombic efficiency higher than those of MFCs with bare SSM cathodes [21, 23]. However, the aforementioned studies have studied diverse modification processes and coating materials with different properties. To accelerate the development of MFCs, the performance effects of SSM electrodes coated with CNTs or graphene must be comprehensively compared using the same modification process and coating materials. Thus, in this study, a set of mediatorless single-chamber MFCs was designed to examine the performance effects of different SSM electrodes coated with CNTs or graphene. The power density and internal resistance values of the MFCs with CNT- or graphene-coated electrodes were evaluated as the performance indices.

2. Materials and Methods

2.1. Electrode Modification

The process of electrode modification was described as follows. For anodic modification, carbon ink was prepared by dispersing 20 mg of multiwall CNTs (MW-CNTs; average diameter larger than 50 nm, length between 10 and 20 μm, and specific surface area approximately 60 m²/g) or multilayer graphene sheets (MG; specific surface area approximately 20 m²/g, average sheet thickness smaller than 50 nm, and lateral size approximately 20 μm) in 95% ethanol (10 mL). Ethanol with MW-CNTs or MG was ultrasonicated to obtain a homogeneous solution. A piece of SSM (average hole diameter 40 μm, thickness 100 μm, and diameter 50 μm) was then dipped into the carbon ink for 1 hour, removed, and finally baked at 150°C for 1 hour to obtain an SSM anode coated with MW-CNTs or MG.

For cathodic modification, polytetrafluoroethylene (PTFE) solution, with or without carbon-based materials, was used for waterproofing. The treated PTFE solution was prepared by dispersing 20 mg of MW-CNTs or MG in 19.98 g of PTFE solution (preparation 60 wt% dispersion in H₂O). The dispersion was performed using ultrasonic vibration to obtain a homogeneous solution. A piece of SSM was soaked in the pure or treated PTFE solution for 1 hour, removed, and then baked at 235°C for 1 hour. The soaking-baking process was repeated four times to obtain a cathode with excellent waterproofing. In some study cases, platinum (0.5 mg/cm⁻², 20 wt% Pt/C) was used to catalyze the oxygen reaction. For those case studies, the inner side of the cathode, which served as the contact surface with the reaction environment, was covered with a Pt catalyst after waterproofing and baked for 30 minutes at 350°C.

2.2. Microorganism Culture

A single bacterium, Escherichia coli HB101, was used to convert energy; this reduced the experimental variability and facilitated precise estimation of the effects of electrode modifications on MFC performance levels. The culture process resembled the methods of a previous study [37] and is briefly described as follows: E. coli HB101 was grown anaerobically in an atmosphere of N₂ gas for 40 hours until it reached its stationary phase in lysogeny broth medium at 37°C. After culturing, the microbe was obtained by 5000 rpm centrifugation and then dissolved in M9 medium.

2.3. MFC Structure

The structure of the air-cathode MFC used in this study, which resembles previously reported MFCs [37], is shown in Figure 1. In this air-cathode MFC, the material of the cylindrical chamber was polymethylmethacrylate (PMMA) and its diameter, length, wall thickness, and reactor volume were approximately 50 mm, 60 mm, 5 mm, and 75 mL, respectively. Anodic and cathodic electrodes were placed at the ends of the cylindrical chamber; the cathodic electrode was on the side with air, and the anodic electrode was on the opposite side. The surface areas of the cathode and anode were approximately 1257 mm². Additionally, copper wires and resistors were used to connect the circuit.

2.4. Experimental Planning and Measurement

Nine types of single-chamber MFCs were constructed, as shown in Figure 2, to compare the effects of electrodes coated with MW-CNTs and MG on MFC system performance. These nine types of MFCs were named as listed in Table 1. The anodic condition was represented in the first letter, and the cathodic condition was represented in the second, third, and fourth letters. Among them, the letters “N,” “G,” and “C” represented the normal, MG-modified, and MW-CNTs-modified SSMs, respectively. Additionally, the letter “E” represented the cathode covered with pure PTFE, and “P” represented the cathode with Pt catalyst.

Stable values of power density and internal resistance were selected to compare the effects of MW-CNTs and MG on MFC system performance. The methods of measurement and calculation are described as follows. A digital electronic multimeter was employed to record the cell voltage. Before determination, a resistance of 1 kΩ was used as the external load. When the voltage output was stable, the cell voltage was recorded to evaluate the power generation. External resistance was varied from 1 to 20 kΩ to obtain the cell voltage of the MFC under testing, and then the performance of the MFCs was evaluated through the polarization and power density curves. Power density (Wm⁻²) was calculated according to the equation , in which (A), (V), and (m²) were the current, voltage, and electrode area, respectively. The slope of the polarization curve was used to determine the internal resistance of the MFC under test. The internal resistance (, Ω) was calculated from the polarization slope according to the equation , in which (mV) and (mA) were the voltage difference and current difference between two points of the polarization curve, respectively. The measurements were performed at a controlled temperature of 30°C.

3. Results and Discussion

3.1. Morphology of Electrode Surfaces

The results of the anodic modification were photographed through a scanning electron microscope (SEM) and are shown in Figures 3 and 4, which present the surface morphologies of SSM anodes coated with MW-CNTs and MG, respectively. The coating process resulted in thick coatings of MW-CNTs or MG on SSM surfaces, and the surface morphologies of the coatings were very similar at all locations. The MW-CNTs and MG were uniformly distributed over the SSM surfaces. Each MW-CNTs coating appeared to form an interconnected network, whereas each MG coating appeared to form a stacked sheet structure. According to the overall distributions of the MW-CNTs and MG on the SSMs, we can confirm that homogeneous and stable MW-CNTs- and MG-modified SSM electrodes can be fabricated by using this simple coating process.

The results of cathode modification are shown in Figure 5, in which panels (a) and (b) show the coating results when the PTFE solutions were mixed with the MG and MW-CNTs, respectively. Both types of treated PTFE (pure PTFE mixed with MG or MW-CNTs) completely coated the SSM surfaces. Moreover, the surface roughness of the PTFE mixed with the MW-CNTs was notably more pronounced than that of the PTFE mixed with the MG, as can be seen by comparing Figure 5(a) with Figure 5(b).

(a)

(b)

3.2. Performance of MFCs

To realize the diverse effects of differently coated anodic surfaces on MFC performance, three types of anodes with PTFE-coated cathodes (MFC-NE, MFC-GN, and MFC-CN) were selected for analysis. The results are shown in Figure 6, in which the solid data points represent the power densities and the hollow data points represent the cell voltages. In the case of MFC-NE, the maximum power density was 69.1 μW/m². With an anode that was coated with MG (the case of MFC-GE), the maximum power density was 231 μW/m². In the case of MFC-CE, MW-CNTs were the coating material, and the power density was 490 μW/m². The power density of MFC-GE was approximately 3.3 times that of MFC-NE, whereas the power density of MFC-CN was approximately seven times that of MFC-NE. Coating MG or MW-CNTs onto anodes can improve the efficiency of MFCs; this may be attributable to improved electron transfer routes resulting from the increased surface area of the anodes [19, 20, 32].

In the cases of MFC-NPE, MFC-GPE, and MFC-CPE, all of the cathodes were covered with pure PTFE and then coated with Pt, whereas each of the three anodes received a different treatment (MG, MW-CNTs, or nothing). The results of these three cases are shown in Figure 7. The maximum power densities of MFC-NPE, MFC-GPE, and MFC-CPE were 92.1 μW/m², 2.9 mW/m², and 2.85 mW/m², respectively. The maximum power densities of MFC-GPE and MFC-CPE were over 30 times larger than those of MFC-NPE, indicating that adding MG or MW-CNTs to an anode can substantially improve power generation. Notably, the trends in cell voltage and power density illustrated in Figure 7 are similar to those in Figure 6. Moreover, comparing Figure 5 with Figure 6, the cathode with Pt displayed a higher cell voltage and current density than did the cathodes without Pt. In other words, Pt further improved the power generation, which may be attributable to Pt catalyzing the oxygen reaction.

The effects of modified cathodes on MFC performance were evaluated, as shown in Figures 8 and 9. In Figure 8, the maximum power density of MFC-NPE is 92.95 μWm⁻² and that of MFC-NE is 69.1 μWm⁻². These two power densities differed by a factor of approximately 1.35. Thus, the cathode coated with Pt catalyzed the oxygen reaction and enhanced MFC performance. Additionally, the polarization curves of MFC-NGE and NCE can be used to understand the effects of PTFE mixed with MG and MW-CNTs, respectively, on MFC performance. The maximum power densities of MFC-NGE and NCE were 116.5 and 314 μW/m², respectively. The power densities obtained by MFC-NGE and MFC-NCE were approximately 1.7 and 4.5 times greater than those of MFC-NE. These results showed that mixing PTFE with MW-CNTs or MG to serve as a waterproof layer of the cathode can enhance the efficiency of power generation.

To compare the maximum power densities among various MFC systems as shown in Figure 8, the MG-modified cathode exhibited a similar power generation to the cathode with Pt catalyst, while the MW-CNTs-modified cathode generated more power than the MG-modified cathode (which was potentially due to the rough surface of the cathode that was observed through SEM analysis). Moreover, MG and MW-CNTs have the potential to replace Pt as a cathode catalyst in air-cathode MFC systems. Such a replacement would notably reduce the cost of materials for cathode catalysts.

Figure 8 also reveals that power generation can be improved through various means, including coating cathodes with Pt, PTFE mixed with MG, or PTFE mixed with MW-CNTs. Therefore, the power generation effects of the simultaneous application of these cathode treatments were studied, and the results are presented in Figure 9. Notably, when the cathode was coated with MG-treated PTFE and platinum (the case of MFC-NPGE), the maximum power density was 421.5 μWm⁻², which was approximately 3.6 times that of MFC-NGE. This confirms that power generation can be further increased when a platinum catalyst and treated PTFE are used simultaneously.

The objective of this study was to realize the modification effects of SSM electrodes by using carbon-based materials (MW-CNTs and MG). Therefore, experiments were conducted using a single species of microorganism. No electron transfer mediators were used because mediators might have distorted the accurate assessment of the modification effects of electrodes; this is also why the MFC power output levels in this study were lower than those reported in most related research. Besides, among all the experimental trials, the MW-CNTs-modified electrodes showed higher power generation than the MG-modified electrodes, regardless of whether the MW-CNTs were on the anode or on the cathode. A possible explanation is the differences in the surface area of MW-CNTs- and MG-coated SSMs. MW-CNTs and MG are adsorbed on SSM via carbon-metal bonding [38] or van der Waals interaction [22], and a large specific surface area can offer more adsorption sites [39]. In the studied cases, the specific surface areas of MW-CNTs and MG are approximately 60 and 20 m²/g, respectively. Thus, the adsorptive properties of MW-CNTs with SSM should be better than those of the MG. This claim can be further supported by SEM microphotographs, as shown in Figures 3 and 4. There is strong evidence that the number of MW-CNTs loading in SSM is larger than that of MG. MW-CNTs completely coated the SSM surfaces and formed a three-dimensional network structure. By contrast, part of the SSM surface was observable in the SSMs coated with MG. Therefore, the surface area of the stacked MG may be lower than that of the MW-CNTs.

According to the measurement data, the internal resistance was evaluated using the polarization slop method; Table 2 shows the results. Regarding anodic modification, the internal resistance was reduced from 101 kΩ for both of the normal electrodes (in the case of MFC-NE) to 30 kΩ (in the case of MFC-GE) and to 19 kΩ (in the case of MFC-CE) when the anodes were modified with MG and MW-CNTs, respectively. Furthermore, the internal resistance was substantially reduced from 20 kΩ for a normal electrode with Pt catalyst (in the case of MFC-NPE) to 7 kΩ (in the case of MFC-GPE) and to 4 kΩ (in the case of MFC-CPE) when the anodes were coated with MG and MW-CNTs, respectively.

Regarding cathodic modification, the internal resistance was reduced from 101 kΩ (in the case of MFC-NE) to 83 kΩ for the case of the MG-modified cathode (in the case of MFC-NGE) and markedly decreased to 36 kΩ for the case of the MW-CNTs-modified cathode (the case of MFC-NCP). However, when the cathode was coated with pure PTFE and Pt (in the case of MFC-NPE), the internal resistance was 20 kΩ. Thus, a cathode coated with Pt has a more favorable internal resistance than does a device coated with PTFE mixed with MW-CNTs or MG. This may be explained by the amount of contact area between the materials used for modification and the reaction liquid. Additionally, internal resistance can be further improved by using Pt and treated PTFE. The internal resistance was reduced from 20 kΩ for a normal electrode with Pt catalyst (in the case of MFC-NPE) to 14 kΩ when the PTFE waterproof layer was mixed with MG (in the case of MFC-NPGE).

Comparing the performance levels of modified anodes with those of cathodes, it was noted that the anodic modification showed more obvious effects on the performance than did the cathodic modification. Moreover, the MFC systems with MW-CNTs-modified SSM electrodes showed lower internal resistance levels than those with MG-modified electrodes for the same electrode conditions. In summary, MW-CNTs- or MG-modified electrodes have lower internal resistance levels. The excellent electrical conductivity values and high surface areas of MW-CNTs and MG improve the efficiency of electron transmission.

4. Conclusions

Air-cathode MFCs were constructed using different types of composite electrodes, with or without MW-CNTs- or MG-modified SSMs. The experiments confirmed that the addition of MW-CNTs and MG enhanced the power density and reduced the internal resistance. Using MW-CNTs- or MG-modified anodes increased the maximum power density by approximately 7.1 and 3.1 times, respectively, compared with that of an untreated anode. Cathodes coated with PTFE solutions mixed with MW-CNTs and MG have maximum power densities, approximately 4.5 and 1.7 times, respectively, those of a cathode coated with pure PTFE solution. Additionally, internal resistances were substantially reduced from 101 kΩ for the normal case (MFC-NE) to 19 kΩ and 30 kΩ for the cases of anodic electrode modified by MW-CNTs (MFC-CE) and MG (MFC-GE), respectively. The electrodes modified with MW-CNTs showed superior power density and lower internal resistance than did those modified with MG. The surface area of the stacked MG may be lower than that of the MW-CNTs. The MW-CNTs coatings appeared to form interconnected networks rather than loosely overlaid MG, leading to the superior conductivity levels of MW-CNTs-coated SSMs.

Conflicts of Interest

The authors declare no conflicts of interest.

Acknowledgments

The authors are grateful to Professor Hwan-You Chang (Department of Medical Science, National Tsing Hua University) for discussion and support regarding microbes. In addition, the authors acknowledge National Nano Device Laboratories for helping SEM imaging.

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Copyright © 2017 Wei-Hsuan Hsu 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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