On the oxygen reduction reaction catalyzed by Ti
Transcription
On the oxygen reduction reaction catalyzed by Ti
On the oxygen reduction reaction catalyzed by Ti -Cu binary films in 0.5 M sulfuric acid solution Jing-Chie Lin*, Chien-Ming Lai, Hang-Chung Chu, Cheng-Lin Chuang, Yu-Sheng Chen Department of Mechanical Engineering/Institute of Materials Science and Engineering, National Central University, No.300 , Jhongda Rd, Jhongli City, Taoyuan Country 320, Taiwan. *Corresponding author:[email protected] Abstract Ti-Cu binary films co-sputtered in vacuum are catalytic active for the oxygen reduction in 0.5M H2SO4. The activity of the oxygen reduction reaction (ORR) increased with increasing the Cu-content in the Ti-Cu films and it reached to a maximum with the copper composition up to 90 at. %. Through investigation of Tafel polarization, the Ti-Cu films revealed a constant Tafel slope (i.e., 190 mV/decade) similar to that of ORR on the pure Cu film. This infers that the electrochemical reduction of oxygen is predominated on the Cu-sites in the film. In the cyclic voltammograms, the strong broad peak should be arisen from the oxidation of Cu to Cu+ and Cu2+ ions. This oxidation indicated that the Ti-Cu films are unstable and the Cu-component is susceptible to dissolution in 0.5M H2SO4. This dissolution caused a loss of catalytic activity in the films. Preparing the Ti-Cu films enriched in Ti will stabilize these films to prevent the Cu-dissolution. Keywords:Ti-Cu; binary film; oxygen reduction reaction; catalytic activity; 1 1. Introduction One of the challenging problems in the fuel cell is oxygen reduction reaction at the cathode [1]. Platinum is still considered the best electrocatalyst for the reduction of oxygen in aqueous electrolytes due to the lowest overpotentials and the best stability. The high cost and limited world’s supply of platinum are the major issues for a widespread commercialization of the fuel cell technology. These difficulties have created enormous interest in the search for less expensive, more efficient electrocatalysts as well as in lowering the catalyst loading [2-6]. With respect to identifying alternative electrocatalysts, non-platinum based metal combinations [7-13], metal oxides [14-18], metal carbides [19], and metal oxynitrides [20] have been investigated over the years for the ORR. These materials have some catalytic activity for the ORR and are stable in acid media, although it is still not sufficient when compared to platinum. Therefore, it is necessary to continuously investigate the non-platinum catalyst for the commercialization of the PEFC. Titanium and its alloys are technically superior and cost-effective construction materials for a wide variety of aerospace, industrial, marine, medical and commercial applications [21]. The kinetics of titanium metal dissolution is quite slow in the oxidant-containing aqueous media. Such a behavior is attributed to the surface of the 2 oxide film (amorphous, mainly TiO2) present in air as well as in aqueous solutions [22-25]. As a search of new ORR electrocatalysts, TiO2 catalysts were studied for their catalytic activity during the ORR and stability in acid media. It was reported that TiO2 supported the oxygen reaction in acid media [14]. The catalytic activity for the ORR of the TiO2 catalysts was low and the ORR occurred below about 0.0V (versus SHE) in a solution with pH at 1.05 [14]. However, titanium and its oxide are worth being studied as a non-platinum electrocatalyst for the PEFC cathode, because it is an abundant natural resource, and supports the electrochemical reaction such as the oxygen evolution reaction. Bard and his co-workers [11] proposed a guideline for developing the design to improve the bimetallic electrocatalysts for the ORR in acidic media. This guideline is based on the thermodynamics correlated with oxygen adsorption and its subsequent reduction on a bimetallic film. The oxygen-oxygen bond would be weakened as the molecular oxygen adsorbed on one component of film. This facilitates oxygen dissociation into atoms that could readily be reduced by the other component in the film. According to Bard’s criteria of the bimetallic catalyst, copper could be selected to improve the activity of the titanium. In this work, Ti-Cu binary films varying in Cu-composition were prepared by magnetic sputtering in vacuum. The electrochemical behavior of those Ti-Cu films for the ORR in acid solution has been 3 investigated. The electrochemical characteristics of Ti-Cu films were explored using by slow scan voltammetry (SSV), Tafel polarization and cyclic voltammetry (CV). 2. Experimental 2.1 Preparation of Ti-Cu catalysts The Ti-Cu films were sputtered on the end of a glassy carbon (GC, Alfa Aesare, USA.) rod substrate (6.15mm diameter × 10mm length) by DC magnetic sputtering system (ARC-12M, Plasma Science Inc., USA.). The Ti and Cu targets (99.9% purity, Gredmann, Well-Being Enterprise Co., Ltd, Taiwan) were fixed on a cathode. The sputtering chamber was pre-evacuated down to 8×10-6 torr, then the sputtering was performed at an argon pressure of 6×10-3 torr by supplying the power of 60 W and 20~60 W for the Ti and Cu targets, respectively. The binary films were deposited to vary their copper composition at 50, 70 and 90 at.% through controlling the sputtering power on the Cu target and the sputtering time. The thickness of the film was controlled and monitored about 200 nm by a quartz crystal microbalance (QCM) film thickness meter. The composition of the films was confirmed by energy dispersive 4 X-ray analysis (EDX, Kevex Level 3, Hitachi Co., Japan). The same sputtering procedure was employed to deposit the monotonic catalyst of pure films, such as Ti and Cu on the GC. 2.2 Electrochemical instruments and measurements The electrochemical experiments were conducted in a three electrode glass cell connected with a potentiostat (model 263, EG&G, USA.) to perform the following measurements: (i) slow scan voltammetry (SSV, in the potential ranging from 1.0 to 0.0 V with a scan rate of 5 mV s−1); (ii) Tafel polarization (Tafel, within potentials of the open circuit potential± 250 mV in a scan rate of 1 mV s−1); (iii) cyclic voltammetry (CV, in the range from 0 to 1.2 V with a scan rate at 50 mV s−1). The potential in this work was measured against a reference electrode of saturated calomel electrode (SCE) but it was reported versus the standard hydrogen electrode (SHE) for convenient comparison. Prior to the test, the electrolyte solution (0.5 M H2SO4) was saturated with oxygen or nitrogen at room temperature. The current densities were in terms of the current on the geometric surface area of the electrodes. 3. Results and discussion 5 Figure 1 show the SSV curves of (a) pure Ti and (b) Ti-Cu thin-film catalyst in 0.5 M H2SO4 saturated with N2 and O2 atmospheres. The potential at which the reduction current with Ti under O2 atmospheres slightly increased than that under N2 was about 0.1 V vs SHE, as shown as Fig. 1(a). This indicated that Ti had a very lower catalytic activity for the ORR. However, as shown in Fig 1 (b), an apparent increase of the reduction current was observed under O2 atmosphere compared to the N2 atmosphere. It indicated that the catalytic activity of the ORR was improved when Cu was added in Ti to form a binary Ti-Cu catalyst. Figure 2 displays the SSV for various thin-films in 0.5M H2SO4 saturated with O2 atmosphere. In Fig. 2, the current density increases rapidly with the potential from 0.4 to 0.0 V. This SSV diagram provides an estimation of catalytic activity for ORR on different films. A film with higher onset potential would catalyze ORR more readily; the film exhibiting higher reduction current is more active. According to Fig. 2, the onset potential shifted slightly to higher potentials with increasing the Cu-composition in the binary films. The oxygen reduction current (µA) at 0.2V vs SHE decreases in the order of Cu (219.0) > Ti-90Cu (54.5) > Ti-70Cu (10.5) > Ti-50Cu (8.0) > Ti (1.8). Obviously, the catalytic activity for the ORR is higher on the Ti-Cu binary films than on the pure Ti film alone. The activity of the ORR increases 6 with increasing the Cu-composition from 50 to 90 at % in Ti-Cu films system. Figure 3 (a) shows the cathodic Tafel plot of different films in 0.5M H2SO4 saturated with O2 atmosphere. The Tafel slope and exchange current density could be estimated from Fig. 3 (a) and the data was collected and re-plotted in Fig. 3(b). Figure 3 (b) depicted the Tafel slope and exchange current density for the ORR on different films. The Tafel slopes on Ti-Cu films are roughly at constant (i.e., 190 mV/decade) similar to that on the pure Cu film (i.e., 198 mV/decade). Based on constant Tafel slope, we infer that the reduction of oxygen on the Cu-sites will predominate the ORR. The exchange current density of ORR (i0,ORR) was estimated by extending the Tafel slope to the current density at the potential of the oxygen reduction (i.e., 1.23 V). The magnitude of i0,ORR increases with increasing the Cu-concentration in the films. As a result, the involvement of Cu in the Ti-Cu films moves the equilibrium of ORR to higher current so that the rate of both forward and reverse reaction is accelerated. Figure 4 shows the cyclic voltammograms (CV) for the films in 0.5 M H2SO4 saturated with N2 atmosphere. In Fig.4, the enormous anodic peak in a wide range of 0.2–1.0 V may arise from the dissolution of Cu to form Cu+ or/and Cu2+ ion, especially in the films with higher Cu-composition. Evidently, the dissolution of copper results in instability of the binary films in the acid solution, especially for the films with higher Cu-composition. The intensity of the anodic peak decreases with 7 decreasing the Cu-composition in the films. The peak responsible for anodic dissolution of copper diminishes with decreasing the copper content, and it eventually disappears as the Cu-content in the Ti-Cu film is lower than 50 at.%. This implies that the dissolution of Cu will be inhibited in the Ti-Cu films enriched with Ti. The ionic concentration of copper in acid solution could be determined by ICP to confirm this inhibition. When a specimen of binary film enriched in Ti (i.e., Ti50Cu50) was immersed in 0.5M H2SO4 saturated with N2 at 0.5 V for 10 min to compare with a the pure Cu, the concentration of copper ion was measured at 0.0318 and 0.2380 ppm, respectively. This fact confirms that copper dissolution from binary films is inhibited in the presence of Ti. Therefore, Ti co-existed in the binary films stabilizes the system. 4. Conclusions The catalytic activity of the oxygen reduction reaction (ORR) on a variety of Ti-Cu films in the 0.5M H2SO4 has been investigated by using electrochemical technologies such as slow scan voltammetry (SSV), Tafel-Plot (Tafel) and cyclic voltammetry (CV). The results of SSV indicated that a combination of binary Cu-Ti films reveals higher catalytic active for ORR. The catalytic activity increases with 8 increasing the concentration of Cu (from 50 to 90 at%) in the films. Ti10Cu90 revealed higher reduction current density (i.e., 54.5 µA/cm2) than any other binary film at 0.2V. Based on the data of Tafel slope, ORR reaction on the Ti-Cu binary films is determined predominantly on the Cu-sites. In CV diagram, an enormous anodic peak in the range of 0.2–1.0 V is resulted from the oxidation of Cu to Cu+ and Cu2+ ions. An unstable film was susceptible to Cu-dissolution in 0.5M H2SO4. The anodic peak diminishes with decreasing the Cu-composition in the binary film. Enrichment of Ti in the binary film will stabilize the films. Acknowledgements The financial support of this work by the National Science Council of Republic of China under contract number NSC 95-2221-E-008-023 is gratefully acknowledged. References [1] M. Gattrell, B. MacDougall, in: W. Vielstich, H.A. Gasteiger, A. Lamm (Eds.), Handbook of Fuel Cells—Fundamentals, Technology and Applications, Electrocatalysis, vol. 2, John Wiley & Sons, 2003. 9 [2] S. H. Joo, S. J. Choi, M. Oh, J.Kwak, Z. Liu, O. Terasaki, R. Ryoo, Nature, 412 (2001) 169. [3] V. Raghuveer, A. Manthiram, Electrochem. Solid-State Lett., 7 (2003) A336. [4] Mukerjee, S. Srinivasan, M. Soriaga, J. Electrochem. Soc., 142 (1995) 1409. [5] L. Xiong, A. Manthiram, J. Mater. Chem., 14 (2004) 1454. [6] L. Xiong, A. Manthiram, J. Electrochem. Soc., 152 (2005) A697. [7] R. Rivera-Noriega, N. Castillo-Hernandez, A. B. Soto-Guzman, O. Solorza-Feria, Int. J. Hydrogen Energy, 27 (2002) 457. [8] S. Ye, A. K. Vijh, Electrochem. Commun., 27 (2003) 272. [9] R. Pattabhiraman, Appl. Catal. A, 153 (1997) 9. [10] O. Savadago, K. Lee, K. Oishi, S. Mitsushima, N. Kamiya, K.-I. Ota, Electrochem. Commun., 105 (2004) 6. [11] J. L. Fernández, D. A. Walsh, A. J. Bard, J. Am. Chem. Soc., 127 (2005) 357. [12] H. Meng, P. K. Shen, Electrochem. Commun., 8, (2006) 588. [13] V. Raghuveer, A. Manthiram, and A. J. Bard, Journal of Physical Chemistry. B, 109 (2005) 22909. [14] V.B. Baez, E. Graves, D. Pletcher, J. Electroanal. Chem. 340 (1992) 273. [15] J.-M. Zen, R. Manoharan, J. B. Goodenough, J. Appl. Electrochem., 22 (1992) 140. 10 [16] J.-M. Zen, C.-B. Wang, J. Electrochem. Soc., 141 (1994) L51. [17] V. Raghuveer, B. Viswanathan, J. Mater. Sci. In press. [18] Y. Liu, A. Ishihara, S. Mitsushima, N. Kamiya, and K. I. Ota, Electrochem. Solid-State Lett., 8 (2005) 400. [19] R. Cote, G. Lalande, G. Faubert, D. Guay, J. P. Dodelet, G. J. Denes, New Mater. Electrochem. Syst., 1 (1998) 7. [20] A. Ishihara, K. Lee, S. Doi, S. Mitsushima, N. Kamiya, M. Hara, K. Domen, K. Fukuda, K. I. Ota, Electrochem. Solid-State Lett., 8 (2005) 201. [21] R.W. Shutz, in: B.J. Moniz, W.I. Pollock (Eds.), Process Industries Corrosion—the Theory and Practise, Houston, TX, National Association of Corrosion Engineers (NACE), 1986, p. 503. [22] R.D. Amstrong, J.A. Harrison, R. Thirsk, R. Whitfield, J. Electrochem. Soc. 117 (1970) 1007. [23] M. Pankuch, R. Bell, C.A. Melendres, Electrochim. Acta 38 (1993) 2777. [24] L.D. Arsov, C. Kormann, W. Plieth, J. Electrochem. Soc. 138 (1991) 2964. [25] M. Freelicher, A. Hugot Le Goff, V. Jovanovic, Thin Solid Films 82 (1981) 81. 11 Figure captions: Figure 1. SSV curves of (a) Ti and (b) Ti-Cu film in 0.5 M H2SO4 saturated with N2 and O2 atmospheres. Figure 2. SSV curves for different thin-film catalysts in 0.5M H2SO4 saturated with O2 atmosphere. Figure 3. (a) The potential (mV) as a function of logarithmic current density (mA cm-2), in 0.5M H2SO4 saturated with O2 atmosphere, for ORR on the pure Ti, Cu single films and Ti-xCu (x=50, 70, 90 at.%) films. (b) Tafel slope (bc) and exchange current density (i0) as a function of the Cu-composition. Figure 4. CV curves for the pure Ti, Cu film and Ti-xCu (x=50, 70, 90 at.%) films in in 0.5M H2SO4 saturated with N2 atmosphere. 12 100 (a) Ti I(µA) 50 0 N2 O2 -50 -100 0.0 0.2 0.4 0.6 0.8 1.0 0.8 1.0 E(V) vs SHE 50 (b) Ti-Cu I (µA) 0 N2 -50 O2 -100 -150 0.0 0.2 0.4 0.6 E(V) vs SHE Figure 1 13 I (µA) 0 -200 Ti Cu Ti50 Cu50 Ti30 Cu70 Ti10 Cu90 -400 -600 0.0 0.2 0.4 0.6 E (V) vs SHE Figure 2 14 0.8 1.0 0.28 E (V) vs SHE 0.26 0.24 0.22 Cu 0.20 Ti 0.18 -6.5 -6.0 Ti50 Cu50 -5.5 Ti30 Cu70 -5.0 Ti10 Cu90 -4.5 -4.0 -3.5 log I (A) 102 160 101 i0 (A/cm2) x10 -10 bc (mA/decade) 200 120 100 0 20 40 60 Cu content (at.%) Figure 3 15 80 100 1.00 Ti Ti 50 Cu50 Ti 30 Cu70 i (mΑ/cm2) 0.75 Cu70 0.50 0.25 Cu50 0.00 Ti -0.25 -0.50 0.0 0.2 0.4 0.6 0.8 1.0 1.2 E(V) v.s. SHE 200 Cu Ti10 Cu90 Cu i (mΑ/cm2) 150 100 50 Cu90 0 -50 0.0 0.2 0.4 0.6 0.8 E(V) v.s. SHE Figure 4 16 1.0 1.2