Solid State Ionics 145 Ž2001. 101–107 www.elsevier.comrlocaterssi Hybrid Nafion–silica membranes doped with heteropolyacids for application in direct methanol fuel cells P. Staiti, A.S. Arico, ` V. Baglio, F. Lufrano, E. Passalacqua, V. Antonucci ) Institute CNR for Transformation and Storage of Energy, Via Salita S. Lucia sopra Contesse 39 98126, St. Lucia, Messina, Italy Received 25 September 2000; received in revised form 12 January 2001; accepted 17 January 2001 Abstract Nafion–silica composite membranes doped with phosphotungstic and silicotungstic acids have been investigated for application in direct methanol fuel cells at high temperature Ž1458C.. The phosphotungstic acid-based membrane showed better electrochemical characteristics at high current densities with respect to both silicotungstic acid-modified membrane and silica–Nafion membrane. A maximum power density of 400 mW cmy2 was obtained at 1458C in the presence of oxygen feed, whereas the maximum power density in the presence of air feed was approaching 250 mW cmy2 . The results indicate that the addition of inorganic hygroscopic materials to recast Nafion extends the operating range of a direct methanol fuel cell. Operation at high temperatures significantly enhances the kinetics of methanol oxidation. q 2001 Elsevier Science B.V. All rights reserved. Keywords: Phosphotungstic acid; Silicotungstic acid; Composite Nafion membranes; Direct methanol fuel cells 1. Introduction Heteropolyacids ŽHPAs. have been largely employed as catalysts in heterogeneous reactions due to their unique structural and chemical properties. They are ionic solids based on high molecular weight anions having the general formula wX x M nO y x 3y with x F n. These materials are proton conductors with high intrinsic conductivity. In recent years, significant efforts have been addressed to evaluate such compounds as both electrolyte and surface promoters for low temperature fuel cells w1–4x. Phosphotungstic acid ŽPWA. was successfully employed as an elec- ) Corresponding author. Tel.: q39-090-624-234; fax: q39-090624-247. E-mail address: [email protected] ŽV. Antonucci.. trolyte in H 2 –O 2 fuel cells w1x, as well as a surface promoter for CO-electro-oxidation w2x, whereas, silicotungstic acid has shown interesting properties as a promoter in the electrochemical oxidation of methanol w3x. One of the main drawbacks of DMFCs relies on the slow methanol oxidation kinetics. For this reason, an increase in the operation temperature of the DMFC from 90 to about 1508C is highly desirable. In this regard, we have recently developed a composite Nafion–silica membrane capable of water retention at high temperatures. This avoids the loss of ionic conductivity up to 1458C w5,6x. In the present study, in order to further increase the level of water retention at high temperatures, two heteropolyacids ŽPWA and SiWA. were impregnated onto the silica particles, and the resulting materials were loaded in the recast Nafion. Similar materials formed by Nafion 0167-2738r01r$ - see front matter q 2001 Elsevier Science B.V. All rights reserved. PII: S 0 1 6 7 - 2 7 3 8 Ž 0 1 . 0 0 9 1 9 - 5 P. Staiti et al.r Solid State Ionics 145 (2001) 101–107 102 and silicotungstic acid with or without thiophene were recently prepared by Tazi and Savadogo w7,8x. They reported some interesting characteristics of the materials, such as conductivity, water adsorption, and performance in H 2 –O 2 fuel cells, but they do not report the behavior of their membranes at temperatures above 1008C. In the present paper, the heteropolyacid-modified membranes have been tested in a direct methanol fuel cell in a range of temperatures from 90 to 1458C, and the results have been compared with that obtained by a fuel cell using a bare silica–Nafion recast membrane. 2. Experimental 2.1. Preparation of the membranes Three different membranes were prepared having the following compositions: Ž1. Nafion–silica; Ž2. Nafion–silica–phosphotungstic acid; Ž3. Nafion– silica–silicotungstic acid, they are indicated in the text as NAS, NA30P and NA45S, respectively. The membranes were prepared by using a proprietary procedure w5x. With respect to the previous work w5x, Aerosil 200 silica from Degussa was substituted in the present work with Cabosil silica from Cabot. Both silica compounds have an average particle size of 7 nm and an amorphous structure. An appropriate amount of Nafion ionomer Ž5% wtrwt, Aldrich. was mixed with SiO 2 ŽCab–O–Sil, EH-5, Cabot. or PWArSiO2 or SiWArSiO2 powders in an ultrasonic bath for 20 min. This solution was cast in a Petri dish and heated at 808C for 20 min. The recast composite Nafion films were detached from the Petri dish by addition of distilled water and allowed to dry for 15 h at room temperature. Afterwards, they were cut to obtain a regular shape and inserted between two polytetrafluoroethylene ŽPTFE. foils and hotpressed at low pressure and increasing temperatures. The final treatment was at 1608C for 10 min. The final membranes contained 3% wtrwt of silica w5x. Heteropolyacid-modified silica powders were composed of 30% wtrwt phosphotungstic acid ŽPWA. on the silica and 45% silicotungstic acid ŽSiWA. on silica w9x. The amount of heteropolyacid loaded on silica was limited by the uptake characteristics of silica. The selected amounts correspond to uniform distribution of the heteropolyacid on the silica surface. X-ray diffraction patterns of the powders consisting of 30% PWA and 45% SiWA revealed an overlapping between the typical crystalline structure of heteropolyacid and the amorphous structures of silica ŽFig. 1.. A chemical interaction between the heteropolyacids and the silica was detected by IR analysis and reported in a previous paper w9x. The thickness of membranes was about 80 mm. The membranes were purified by using the usual procedure w5x. Fig. 1. Cu K a X-ray diffraction patterns of bare Ža. and PWA impregnated Žb. Cab–O–Sil silica powders. P. Staiti et al.r Solid State Ionics 145 (2001) 101–107 2.2. Membrane and electrodes (M & E) assembly The catalyst employed for methanol oxidation was 60% Pt–Ru Ž1:1.rC ŽE-Tek., whereas a 30% PtrC ŽE-Tek. was used for oxygen reduction. The reaction layer, for both anode and cathode, was prepared by direct mixing in an ultrasonic bath a suspension of Nafion ionomer in water with the catalyst powder, the obtained paste was spread on carbon cloth backings. The platinum loading for all the electrodes Žanodes and cathodes. used in the experiments was 2.2 " 0.2 mg cm2 . The M & E assembly was manufactured by pressing the electrodes onto the membrane at 1308C and 50 atm. 2.3. Single cell experiments Each M & E assembly was loaded into a single-cell test fixture ŽGlobe Tech. which was connected to an HP 6060B electronic load. An aqueous solution of methanol, as well as humidified oxygen were preheated at 858C and fed to the cell. Different operating temperatures for the cell were settled in the range from 90 to 1508C. The anode back-pressure was varied between 1 and 3 atm as the temperature was increased from 90 to 1508C. Whereas the cathode 103 compartment back-pressure was maintained constant at 4 atm. Methanol–water solutions of different concentrations were used in order to evaluate the appropriate concentration of fuel which allows the acquisition of the best cell performance. The inlet fluxes from anode and cathode compartments were measured on-line. 3. Results and discussion 3.1. X-ray diffraction analysis XRD patterns obtained for different membranes evidenced only slight differences in the structural characteristics ŽFig. 2.. The bare Nafion membrane shows a main peak related to the hexagonal structure of Nafion at about 2 u s 188, which overlaps with the X-ray scattering from the amorphous region of the membrane at lower Bragg angles w5x. More detailed information on these aspects are derived from a peak profile analysis carried out by using the Marquardt algorithm w5x ŽFig. 3.. The addition of silica and heteropolyacid modifies the relative ratio between the crystalline and amorphous structures of cast Nafion with respect to bare Fig. 2. Cu K a X-ray diffraction patterns of Nafion 117 Ža., silica- Žb., silica–PWA- Žc. and silica–SiWA- Žd. modified recast Nafion membranes in protonic form and dry state. 104 P. Staiti et al.r Solid State Ionics 145 (2001) 101–107 Fig. 3. X-ray diffraction profiles for Nafion 117 Ža. and silica–PWA-modified recast Nafion Žb. membranes in protonic form and dry state. The measured data are shown by dots, whereas amorphous Žlower Bragg angles. and crystalline scatterings are the deconvoluted profiles. Nafion. Yet, due to the low loading of silica and heteropolyacid in the membranes Ž3% silica, less than 1.5% heteropolyacid., it is unlikely that the inorganic materials are responsible for such a significant modification in the Nafion structure. More probably, the above changes were caused by the different thermal treatments to which the modified membrane had been subjected. 3.2. Polarization tests All the M & E assemblies equipped with the various membranes were capable of operation at 1458C. Fig. 4 shows that the cell resistances in the various systems are almost unvaried in the range between 90 and 1458C, even if a slight loss of conductivity is observed at 1458C. Yet, this does not affect signifi- Fig. 4. Variation of cell resistance with temperature during DMFC operation Žcurrent interrupter method. for the various M & E assemblies equipped with different membranes. P. Staiti et al.r Solid State Ionics 145 (2001) 101–107 105 Fig. 5. Polarization and power density curves for the various M & E assemblies equipped with different membranes. Operating conditions: 1458C, oxygen feed, methanol 2 M. cantly the cell performance due to the fact that the enhancement of methanol oxidation kinetics plays a prevailing role. The polarization curves obtained for the fuel cells equipped with the different membranes and operating under the same conditions in the presence of oxygen feed at cathode and 2 M methanol solution at anode are reported in Fig. 5. Similar electrochemical characteristics are observed up to 0.5 A cm2 . The PWA-based membrane shows lower mass-transport limitation with consequent higher cell voltages at high current densities. The best electrochemical performance is obtained with the PWA-based membrane, which gives a maximum power density of 400 mW cm2 at current density of about 1.4 A cm2 under oxygen feed operation at 1458C. Maximum power density of 340 mW cm2 is obtained from the fuel cell which uses the silica-modified membrane, whereas a lower performance was achieved with the SiWA-based membrane. It is clear that a positive Fig. 6. Comparison of the polarization and power density curves in the presence of air and oxygen feed for the M & E assembly equipped with the PWA-modified membrane at 1458C. Operating conditions: oxygen feed, 2 M methanol; air feed, 1M methanol. 106 P. Staiti et al.r Solid State Ionics 145 (2001) 101–107 Fig. 7. Influence of operating temperature on the DMFC polarization characteristics for the M & E assembly equipped with the PWA-modified membrane in the presence of oxygen and 2 M methanol feed. effect on cell performance is given by the addition of phosphotungstic acid to the silica–Nafion membrane. Since the enhancements were observed at high current densities, one may ascribe, at a first instance, this behavior to a better ion transport through the membrane under such conditions. But such conjectures are not supported by the analysis of variations of cell resistance with temperature ŽFig. 4.. In a previous paper w10x, we have evidenced a promoting effect of phosphotungstic acid on the kinetics of electrochemical reduction of oxygen. This was mainly attributed to the high oxygen solubility in the PWA electrolyte w10x. For what concerns a possible promoting effect on methanol oxidation, it is known that CO-like products, which form at the anode during methanol oxidation reaction giving rise to a strong chemisorption on surface catalyst, are better removed in the presence of the heteropolyacid w2x. In the presence of oxygen, the best fuel cell performances were obtained, for all the membranes, with 2 M MeOH solution feed at the anode. When air is fed to the cathode compartment, the best cell performance is obtained with 1 M MeOH solution feed at the anode. This occurs because the effect of methanol crossover on cathode polarization is more significant in the presence of air as oxidant. The maximum power density obtained in air with the PWA-based membrane is 250 mW cm2 at 1458C ŽFig. 6., and 210 mW cm2 with the Nafion–SiO 2 membrane at the same temperature. The fuel cell operating with the SiWA-based membrane showed lower electrochemical performances when both air or oxygen are fed to the cathode. The effect of temperature on electrochemical polarization characteristics of a fuel cell operating with the PWA-based membrane is reported in Fig. 7. The voltage losses decrease progressively as the cell temperatures increase in the range from 90 to 1458C, in both activation and diffusion control regions. A maximum of fuel cell activity is recorded at 1458C. Experiments carried out at 1508C gave rise to an unstable electrochemical behavior. It is pointed out that the voltage gain at very low current densities Ž50 mA cm2 . passing from 90 to 1458C is about 100 mV, indicating the strong activation nature of the methanol electro-oxidation process. 4. Conclusions Heteropolyacid-modified silica–Nafion recast composite membranes showed suitable properties for operation at 1458C in a direct methanol fuel cell. Phosphotungstic acid-based membrane performed better than both bare Nafion–silica and Nafion– silica–silicotungstic acid membranes under oxygen P. Staiti et al.r Solid State Ionics 145 (2001) 101–107 and air operation. Similar cell resistance values were observed for these M & E assemblies; this evidence indicates that the enhancement effect produced by phosphotungstic acid is not related to an increase of electrolyte ionic conductivity, but more likely, it relies on its promoting behavior w9,10x. Further studies are in progress to better focus these aspects. References w1x N. Giordano, P. Staiti, S. Hocevar, A.S. Arico, ` Electrochim. Acta 41 Ž1996. 397. w2x A.S. Arico, ` E. Modica, I. Ferrara, V. Antonucci, J. Appl. Electrochem. 28 Ž1998. 881. 107 w3x A.S. Arico, ` H. Kim, A.K. Shukla, M.K. Ravikumar, V. Antonucci, N. Giordano, Electrochim. Acta 39 Ž1994. 691. w4x P. Staiti, A.S. Arico, ` S. Hocevar, V. Antonucci, J. New Mater. Electrochem. Syst. 1 Ž1998. 1. w5x A.S. Arico, ` P. Cretı, ` P.L. Antonucci, V. Antonucci, Electrochem. Solid-State Lett. 1 Ž1998. 66. w6x P.L. Antonucci, A.S. Arico, ` P. Cretı, ` E. Ramunni, V. Antonucci, Solid State Ionics 125 Ž1999. 431. w7x B. Tazi, O. Savadogo, in: O. Savadogo, P.R. Roberge ŽEds.., Proceedings of the Second International Symposium on New Materials for Fuel Cell and Modern Battery Systems, Montreal, Canada, July 6–10, 1997, p. 864. w8x B. Tazi, O. Savadogo, Electrochim. Acta 45 Ž2000. 4329. w9x P. Staiti, S. Freni, S. Hocevar, J. Power Sources 79 Ž1999. 250. w10x N. Giordano, A.S. Arico, ` S. Hocevar, P. Staiti, P.L. Antonucci, V. Antonucci, Electrochim. Acta 38 Ž1993. 1733.
© Copyright 2024 ExpyDoc