Journal of Electroanalytical Chemistry Journal of Electroanalytical Chemistry 583 (2005) 69–76 www.elsevier.com/locate/jelechem Effect of loading level in platinum-dispersed carbon black electrocatalysts on oxygen reduction activity evaluated by rotating disk electrode Eiji Higuchi a, Hiroyuki Uchida b, Masahiro Watanabe b a,* a Clean Energy Research Center, University of Yamanashi, 4 Takeda, Kofu 400-8510, Japan Interdisciplinary Graduate School of Medicine and Engineering, University of Yamanashi, 4 Takeda, Kofu 400-8510, Japan Received 2 November 2004; received in revised form 25 December 2004; accepted 10 January 2005 Available online 6 July 2005 Abstract The dependence of oxygen reduction reaction (ORR) activity on the loading level of Pt electrocatalysts highly dispersed on carbon black (Pt/CB) has been investigated. We present a standard method for the evaluation of ORR activity at Pt/CB by a rotating disk electrode (RDE), in which Pt/CB powder was attached on a glassy carbon (GC) disk uniformly, followed by coating a thin Nafion film. We describe the optimized protocols for preparing a suspension of the Pt/CB in an ethanol aqueous solution, controlling vapor pressure during drying process, and coating very thin (0.05 lm) Nafion film. The area-specific activity for the ORR in airsaturated 0.1 M HClO4 electrolyte solution was found not to be influenced by the Pt-loading level on CB from 19.2 to 63.2 wt%, when the amount of Pt/CB on GC and the dispersion state were optimized. Ó 2005 Elsevier B.V. All rights reserved. Keywords: Rotating disk electrode; Highly dispersed platinum electrocatalyst; Oxygen reduction reaction 1. Introduction Polymer electrolyte fuel cells (PEFCs) have attracted great attention as a primary power source for electric vehicles or residences due to their high energy conversion efficiency and low emission of pollutants. Nanosized platinum particles dispersed on high surface area carbon substrates have been used as the electrocatalyst for both the anode and the cathode. When pure hydrogen is used as the fuel, the anodic hydrogen oxidation reaction (HOR) overpotential is negligibly small even at high current density of 1 A/cm2. Because a sluggish oxygen reduction reaction (ORR) causes a large overpotential at the low operating temperature, the develop- * Corresponding author. Tel.: +81 55 220 8620; fax: +81 55 254 0371. E-mail address: [email protected] (M. Watanabe). 0022-0728/$ - see front matter Ó 2005 Elsevier B.V. All rights reserved. doi:10.1016/j.jelechem.2005.01.041 ment of a high performance cathode catalyst is very important. At the first screening for the electrocatalyst, planar electrodes with well-defined characteristics (surface area, surface and bulk compositions, and crystal structure) have often been examined in aqueous acidic electrolyte solutions, for example, at platinum electrodes of polycrystalline or single crystal at around room temperature. Use of the rotating disk electrode (RDE) has a great advantage to eliminate a mass-transfer problem and evaluate precisely a kinetically controlled ORR activity [1–9]. We reported previously an effect of thickness of Nafion film covered on the Pt disk electrode on the activities for both ORR and HOR [1]. It was found that the kinetically controlled activity can be achieved as the thickness is thin enough (ca. <0.2 lm). Schmidt et al. [3,4] proposed the use of RDE to evaluate activities of Pt nanoparticles supported on carbon black (Pt/CB) in 70 E. Higuchi et al. / Journal of Electroanalytical Chemistry 583 (2005) 69–76 both ORR and HOR. Commercial Pt/CB (20 wt% Pt/ Vulcan XC72) powder was attached on a glassy carbon (GC) disk electrode by means of a thin Nafion film (ca. 0.05 lm in thickness). This method has also been applied to the activity evaluation of Pt or Pt-alloy highly dispersed on carbon substrates [10–12]. Recently, commercial Pt/CB catalysts with high Pt loading (>60 wt%) have been developed with keeping the particle size dPt < 3 nm. Such a highly loaded Pt/CB makes a thickness of the anode or cathode catalyst layers in PEFCs thinner than the present level at a constant Pt loading. The thin layer structure may, in principle, enhance mass-transfer rates for O2 as well as H+ when it is optimized. An evaluation of the intrinsic activity of such a catalyst before the application into practical gas-diffusion electrodes is very important for designing high performance electrodes, because one cannot eliminate effects of the utilization of catalyst particles and/or the mass-transfer rate on the performance of the practical electrodes. The intrinsic activity is considered as a clear target which one can achieve in the ideal case. For the purpose, we tried to use the evaluation technique proposed by Schmidt and co-workers [4]. However, we found the necessity of the modification of their recipe, taking into account a dispersing state of the carbon black particles and the amount of them on the GC disk electrode to ensure sufficient reactant-gas diffusion to Pt catalyst particles supported on them. In the present paper, we propose a standard method for the evaluation of ORR activity applicable to the Pt/ CB with various Pt loading amounts by using RDE method. That is the optimized protocols for preparing a suspension of the Pt/CB in an ethanol aqueous solution, controlling the atmosphere during drying the suspension on GC disk electrode, and coating a very thin (0.05 lm) Nafion film on the Pt/CB–GC. By using the optimized recipe, we, for the first time, demonstrate that the area-specific ORR activity for Pt/CB is quite constant over wide range of Pt-loading level on CB in airsaturated 0.1 M HClO4 electrolyte solution. 2. Experimental 2.1. Preparation of Pt/CB-dispersed GC disk electrodes Fig. 1 shows the preparation protocol of the working electrode, Pt/CB-dispersed GC-disk covered with thin Nafion film. GC disks (diameter = 10 mm, geometric area = 0.785 cm2) were polished with an alumina paste containing the particles in 1 lm diameter for 30 min, 0.3 lm alumina for 10 min, and finally 0.05 lm alumina for 10 min. They were washed ultrasonically in hot water, followed by degreasing with ethanol. After washing sufficiently in pure water with ultrasonic bath, we confirmed the mirror finish by an optical microscope Polishing and washing of GC electrode Pipetting catalyst suspension on GC Drying under ethanol vapor pressure Pipetting Nafion solution Drying under ethanol vapor pressure Heat treatment (120oC) Fig. 1. Preparation method of Pt/CB highly dispersed on GC disk electrode. (VH-Z250, Keyence Co. Ltd.) and a laser microscope (VK9510, Keyence Co. Ltd.). Platinum-dispersed high-surface-area carbon black catalysts (Pt/CB, Tanaka Kikinzoku Kougyo Co. Ltd.) with various Pt loading of 19.2 to 63.2 wt% were used as-received. Scanning transmission electron microscope (STEM, HD-2000, Hitachi High-Technologies Corp.) was employed to observe the catalysts with an acceleration voltage of 200 kV. Table 1 shows the physical properties of these catalysts. To make ultra-thin and uniform dispersion of Pt/CB on the GC disk, we examined various conditions for preparing Pt/CB suspension in an ethanol aqueous solution and for the drying process of the suspension on GC. Typical conditions are summarized in Table 2. A constant volume (40 lL) of the suspension was pipetted onto the GC. As the first approach, we adjusted the amount of Pt/CB in the suspension so as to keep the weight of CB support constant at wCB = 5.70 ± 0.07 lg/cm2 (Nos. 1, 4, 6, and 7 in Table 2) irrespective of Pt-wt%, i.e., the volume of CB framework is constant in the Pt/CB layer on the GC disk. In this recipe, the weight of Pt loaded on the GC (wPt) increases with Pt-wt% in the catalyst. Here, for example, we explain the procedure for the case of No. 4 in Table 2 (46.3 wt%-Pt/CB). Pt/CB powder of 8.4 mg was ultrasonically dispersed in 40 mL of 40 vol% ethanol aqueous solution for 10 min (CPt/CB = 0.21 g/L) by using an ultrasonic homogenizer (US-300T, Table 1 Typical properties of commercial Pt/CB catalysts employed Catalyst No. Pt loading (wt%) dPt (estimated by XRD) (nm) TEC10E20E TEC10E30E TEC10E50E TEC10E70E 19.2 29.3 46.3 63.2 2.7 2.2 2.6 2.4 E. Higuchi et al. / Journal of Electroanalytical Chemistry 583 (2005) 69–76 Table 2 Preparation conditions of catalyst suspensions and resulting wPt and wCB by pipetting the suspension with 51 lL/cm2 on GC disk Sample No. Pt loading (wt%)a CPt/CB (g/L)b CEtOH (vol%)c wPt (lg/cm2)d wCB (lg/cm2)e 1 2 3 4 5 6 7 63.2 63.2 63.2 46.3 46.3 29.3 19.2 0.30 0.22 0.15 0.21 0.16 0.16 0.14 40 40 40 40 40 35 35 9.66 7.08 4.83 4.95 3.83 2.39 1.37 5.63 4.13 2.81 5.75 4.45 5.76 5.76 a b c d e Pt-weight percent in Pt/CB catalysts (see Table 1). Amount of Pt/CB catalyst in the suspension. Ethanol concentration in the suspension. Amount of Pt attached in the catalyst layer. Amount of CB attached in the catalyst layer. Nihon Seiki Seisakujo Co. Ltd.). A 40 lL aliquot of the suspension was pipetted onto the mirror-finished GC disk substrate (0.785 cm2), giving wPt = 4.95 lg/cm2 and wCB = 5.75 lg/cm2. This was dried at room temperature in a glass Petri dish containing ethanol. The dish was covered by a lid with a small gap to evaporate the solvent droplet slowly under the saturated vapor pressure of ethanol. An 18 lL of 0.05 wt% Nafion (diluted with ethanol) solution was put on top of the dried catalyst layer to yield the film thickness of 0.05 lm. This was dried at room temperature and under ethanol vapor pressure in the similar manner as described above. Finally, Nafion-coated catalyst layer on the GC was heat-treated at 120 °C for 1 h in air. 2.2. Electrochemical measurements The rotating disk electrode (RDE) equipment (RED-1, Nikko Keisoku Co. Ltd.) with a gas-tight Pyrex glass cell was employed to examine the ORR activity of the electrocatalyst. A platinum wire and a reversible hydrogen electrode (RHE) were used as the counter electrode and the reference electrode, respectively. All electrode potentials are reported with respect to the RHE. The electrolyte solution of 0.1 M HClO4 was prepared from reagent grade chemicals (Kanto Chemical Co., Japan) and Milli-Q water (Milli-pore Japan Co. Ltd.) and purified in advance with conventional pre-electrolysis methods [13–15]. Prior to the ORR experiments, the potential of the working disk electrode was cycled 10 times between 0.05 and 1.0 V at 0.5 V/s in 0.1 M HClO4 deaerated with N2 gas to clean the surface. The electrochemical active area of Pt, SPt, was evaluated from an electric charge for the hydrogen desorption QH in the positive-going potential scan from 0.05 to 0.40 V in cyclic voltammetry at the sweep rate of 0.1 V/s at 25 °C, supposing QH = 0.21 mC/cm2 for a smooth polycrystalline platinum [13,14]. 71 After bubbling air in 0.1 M HClO4 solution for 30 min, hydrodynamic voltammograms for the ORR at the working disk electrode were recorded by sweeping the potential from 1.0 to 0.05 V at 10 mV/s under the rotating rate of 1000–2750 rpm. All the electrochemical experiments were performed at 25 °C. 3. Results and discussion 3.1. Preparation of Pt/CB thin layer uniformly dispersed on GC disk electrode One of the important subjects in this research is to clarify the dependence of the specific ORR activity on the amount of Pt loaded on a given CB (high-surfacearea carbon black, HSA-CB) support. To avoid socalled ‘‘particle–crystallite size effect’’ [16–18], we have chosen Pt/CB catalysts with almost the same Pt particle size, irrespective of Pt-loading level. Fig. 2 shows typical STEM photographs of 19.2 wt% and 63.2 wt%-Pt/CB catalysts, which are the lowest and highest loading level among the catalysts examined, respectively. It is clearly seen that Pt particles are highly dispersed on the carbon support for both samples. The Pt particle size ranged from 2 to 3 nm. The crystallite size of Pt (dPt), estimated from X-ray diffraction (XRD), for each catalyst is shown in Table 1. The values of dPt are 2.2–2.7 nm, in accord with that observed by STEM. Thus, these Pt/CB catalysts are suitable for our objective. Next, we present how to disperse Pt/CB catalyst uniformly on the GC disk electrode. Schmidt and co-workers [4] reported a recipe for preparing the thin-film Pt/ CB (20 wt%-Pt supported on Vulcan XC 72) catalyst layer on the GC; an aliquot of 20 lL catalyst suspension (CPt/CB = 1 g/L in pure water) was pipetted onto the GC (0.283 cm2, yielding wPt = 14.1 lg/cm2 and wCB = 56.5 lg/cm2), followed by drying in argon stream. Unfortunately, as shown in Fig. 3(a), an application of this recipe to our 19.2 wt%-Pt supported on HSA-CB resulted in aggregation (stacking) of the catalyst, especially at the circumference part of the GC disk. We have judged that the amount of the catalyst loaded on the GC in [4] is too much because the thickness of CB framework (density = 2 g/cm3) is estimated to be 0.28 lm even if the catalysts can uniformly be dispersed over the GC. Schmidt et al. [3] claimed that this thickness value is small enough compared with the hydrodynamic masstransfer boundary layer thickness (ca. 10 lm). However, we have clearly shown that the catalytic activity becomes controlled by the mass-transfer process in the Nafion film, covering Pt catalyst surface, thicker than 0.2 lm [1]. The Nafion film with the thickness of 0.1 lm in their recipe [4] may fill the space of the above CB frameworks of 0.28 lm, where the utilization of 72 E. Higuchi et al. / Journal of Electroanalytical Chemistry 583 (2005) 69–76 Fig. 2. STEM photograph of commercial Pt/CB catalysts: (a) 19.2 wt%-Pt (TEC10E20E); (b) 63.2 wt%-Pt (TEC10E70E). Fig. 3. Optical microscope photograph of Pt/CB (19.2 wt%-Pt) layer on GC disk after drying: (a) prepared by the method in [4], wPt = 14.1 lg/cm2 and wCB = 56.5 lg/cm2; (b) by our recipe No. 7 in Table 2, wPt = 1.37 lg/cm2 and wCB = 5.76 lg/cm2. the catalyst for the ORR should be different at the top and bottom of the stacked layer. To make uniform dispersion of Pt/CB particles on the GC disk, where they are separated each other ideally as a single particle, we examined various conditions regarding the solvent of the catalyst suspension, the amount of catalyst, and the evaporation rate of the solvent. For each run, we observed the catalyst layer by an optical microscope with a magnification of 250 from end to end along the diameter (typically 12 continuous pictures). Fig. 3(b) shows one of microscope photographs for 19.2 wt%-Pt/CB dispersed on the GC by our optimized recipe. Four important points to obtain such a uniformly dispersed Pt/CB layer on the GC are: (1) adjustment of amount of Pt/CB (CPt/CB) in the suspension, (2) addition of ethanol (CEtOH = 35 or 40 vol%) in water to prepare the suspension, (3) pipetting suitable volume of the suspension on the GC, and (4) evaporation of the solvent droplet on the GC slowly under saturated vapor pressure of ethanol. Regarding the amount of Pt/CB in the thin film layer on the GC, it is noted that the major framework (or volume) is constructed by the CB support, considering the density of CB (2 g/cm3) and Pt (21.4 g/cm3). The amount of CB in our catalyst layer is about 1/10 of that recommended in [4], which prevents the catalyst from the aggregation. The addition of ethanol in the suspension reduces a surface tension (or a contact angle) of the droplet on the GC, leading to uniform spreading of the suspension over whole surface and easy evaporation of the solvent. This also reduces the volume of the suspension put on the GC, i.e., 51 lL/cm2 in our recipe is about 70% of 71 lL/cm2 in [4]. Because the dispersion state of the catalysts on the GC somewhat changed depending on the E. Higuchi et al. / Journal of Electroanalytical Chemistry 583 (2005) 69–76 Pt-loading level, we tuned up the concentration of ethanol at CEtOH = 35 and 40 vol% for low Pt loading (19.2 and 29.3 wt%-Pt) and higher Pt-loading catalysts, respectively. Thus, as shown in Figs. 3(b) and 4, we succeeded to prepare thin Pt (19.2–63.2 wt%)/CB layers uniformly dispersed on the GC with a good reproducibility by the recipe shown in Table 2. 3.2. Effect of Nafion film thickness on the ORR current On top of the dried Pt/CB catalyst layer prepared above, a thin Nafion layer was coated. The Nafion film thickness L (cm) was calculated by Eq. (1) L ¼ ðV d l C N Þ=ðd N A 100Þ; ð1Þ 3 where V (cm ) is the volume of Nafion solution coated on the catalyst layer, dl (0.874 g/cm3) is the density of Nafion solution, CN is weight percent of Nafion in the solution (0.05 wt% in our standard recipe), dN (2 g/cm3) 73 is the density of dried Nafion, and A (0.785 cm2) is projected surface area of the GC disk electrode. We varied the Nafion film thickness from 0.05 to 0.8 lm in order to find out the optimum condition for the RDE experiments. Fig. 5 shows hydrodynamic voltammograms recorded at 2000 rpm for the ORR at Pt/CB (wPt = 2.39 lg/cm2, wCB = 5.76 lg/cm2, No. 6 in Table 2) on GC disk electrodes coated with Nafion film of various thickness in air-saturated 0.1 M HClO4 at 25 °C. The ORR currents at the disk electrode commence at ca. 0.95 V and reach to a limiting current around 0.6 V. It is evident that the limiting current decreases with increasing L. As reported for bulk Pt disk [1] or Pt/CB dispersed on GC disk [4] electrodes, such a decrease in the ORR current with increasing L is ascribed to a mass-transport resistance in Nafion film. Then, in the same manner as in literature [1], the ORR current I is expressed by the following equation: 1 1 1 1 ¼ þ þ ; I Ik Id If ð2Þ I d ¼ 0.62nFSD2=3 Cm1=6 x1=2 ; ð3Þ where Ik, Id, and If are the kinetically controlled current, diffusion-limited current through the solution phase (socalled Levich current), and diffusion-limited current through the Nafion film, respectively. Parameters in Eq. (3) have their usual meanings in the conventional Levich equation. However, it should be careful to distinguish S from A; S is an effective projected area covered by Pt catalysts, whereas A is the (geometric) projected area of the disk electrode. Because the ORR activities of both CB itself and GC uncovered by Pt are negligibly Fig. 4. Optical microscope photograph of Pt/CB layer on GC disk after drying. (a) No. 6, (b) No. 4, and (c) No. 1. Fig. 5. Hydrodynamic voltammograms for the ORR at Pt/CB coated with Nafion of the thickness L attached on GC electrodes at 2000 rpm in air-saturated 0.1 M HClO4 at 25 °C. Scan rate, 10 mV/s; rotation rate, 2000 rpm; L, the thickness of Nafion film on GC electrodes; catalyst, 29.3 wt%-Pt/CB (2.39 lg-Pt/cm2, 5.76 lg-CB/cm2, No. 6 in Table 2). 74 E. Higuchi et al. / Journal of Electroanalytical Chemistry 583 (2005) 69–76 low at E > 0.6 V, S is smaller than A, and usually cannot be defined. Similar to the conventional Levich–Koutecky plots, I1 at a given potential was plotted against x1/2. From the slope of the plot, the number of electrons transferred n cannot be determined for the Pt/CB dispersed GC disk electrode due to a lack of S value as described above. The value of intercept (denoted as 1/2 I 1 to zero inf ) was determined by extrapolating x 1 (I d to zero). Then, the current density at the infinite rotation rate jinf was obtained by dividing the value of Iinf by the electrochemical active area of Pt (SPt). Fig. 6 shows plots of jinf as a function of L1. The value of jinf increases almost linearly in proportion to L1 for L > 0.2 lm, suggesting that a planar diffusion of the reactant oxygen may be dominant in the Nafion film [1]. With decreasing L, the value of jinf reaches a maximum constant value in the region less than 0.1 lm. By coating such a thin Nafion film on top of the Pt/CB layer, the contribution of the film diffusion resistance [the third term in Eq. (2)] to the measured current I becomes negligible. Hence, we can judge that jinf obtained at L 6 0.1 lm equals the kinetically controlled current density jk. This critical thickness is just the same as that for Pt/CB on GC [4] but is smaller than the value of 0.2 lm for a smooth Pt electrode [1]. In the case of Nafion-coated smooth Pt disk electrode, the diffusion of the reactant O2 through Nafion film to Pt surface is well expressed by planar-type diffusion, i.e., the O2 flux is perpendicular to the Nafion or Pt surface. In contrast, for Nafion-coated Pt/CB layer on the GC disk, the diffusion of O2 within the Nafion toward Pt catalyst particles cannot be regarded as a simple planar-type. Supposing that the Pt/CB is dispersed uniformly on the GC, the thickness of the catalyst layer is estimated to be about 0.03 lm at wCB = 5.76 lg/cm2. Although the planar-type O2 diffusion may be dominant toward the Pt catalysts near the top of the catalysts layer, Fig. 6. Dependence of jinf for the ORR on thickness of Nafion coating (L). O2 is supplied to the Pt particles near the GC substrate by a spherical diffusion, i.e., longer diffusion path. Therefore, for the evaluation of the catalytic activity without any effect of mass transfer, the Nafion thickness must be very thin, i.e., L 6 0.1 lm, compared with a smooth Pt electrode. Hereinafter, we performed all the experiments with L = 0.05 lm. 3.3. Effect of Pt loading on the mass or specific activities evaluated for the ORR The last important issue for the precise evaluation of the mass or specific ORR activity at Pt/CB layer by the RDE is the control of the Pt weight loaded in the layer (wPt) so as to utilize all of the Pt particles evenly. Fig. 7 shows typical examples of cyclic voltammograms (CVs) at various working disk electrodes without rotation in deaerated 0.1 M HClO4 solution. The shape of the CV is similar to that of polycrystalline bulk Pt, and considerable change in the shape is not seen among catalysts with 19.2–46.3 wt%-Pt. The value of hydrogen desorption charge QH in the positive-going potential scan at each electrode is plotted as a function of wPt in Fig. 8. Besides the regular sample with wCB = 5.70 ± 0.07 lg/cm2, we also prepared samples No. 2, 3, and 5 with less CB loading to check the effect of wPt. The value of QH increases linearly in proportion to wPt from 0 to 7.08 lg/cm2, irrespective of kind of Pt/CB catalysts. However, at sample No. 1 in Table 2 (wPt = 9.66 lg/cm2 and wCB = 5.63 lg/cm2, prepared with 63.2 wt%-Pt/ CB), the value of QH deviates from the regression line. Since any aggregation of Pt/CB was not seen by an optical microscope at the magnification of 250, the reason why the sample No. 1 with high wPt exhibited almost saturated QH value cannot be explained well. However, some fraction of Pt particles, probably inside the Fig. 7. Cyclic voltammograms for the Pt/CB–GC disk electrodes (samples No. 1, 4, 6, and 7) in deaerated 0.1 M HClO4 at 25 °C. Scan rate, 100 mV/s. Thickness of Nafion film, 0.05 lm. E. Higuchi et al. / Journal of Electroanalytical Chemistry 583 (2005) 69–76 75 a bulky smooth Pt RDE measured at 0.80 V in air-saturated 0.5 M H2SO4 at 25 °C [9]. To our knowledge, the present research is the first to demonstrate that the specific ORR activity per SPt (active Pt surface area) of Pt/CB is quite constant over wide range of Pt-loading level from 19.2 to 63.2 wt%. We can expect that the use of highly loaded Pt/CB can provide an advantage of reducing the catalyst layer thickness without losing the kinetic activity, if the catalyst layer is properly designed to achieve a good balance between the catalyst utilization and the gas diffusivity. 4. Conclusions Fig. 8. Relation between QH and wPt for various Pt/CB–GC disk electrodes in deaerated 0.1 M HClO4 at 25 °C. Pt-loading level: 63.2 wt% (d), 46.3 wt% (h), 29.3 wt% (m), and 19.2 wt% (.). catalyst layer, might not be electrochemically utilized. In contrast, the values of QH at samples No. 2 and 3 with low wPt prepared with the same 63.2 wt%-Pt/CB are reasonably located on the regression line. Fig. 9 shows plots of the ORR activities jk [mA (Ptcm2)] at 0.76 and 0.80 V as a function of wPt for all the RDE experiments examined at 25 °C. It is striking that the area-specific ORR activity at 0.76 V or 0.80 V is constant irrespective of the Pt-loading level from 19.2 to 63.2 wt% in Pt/CB at wPt 6 7.08 lg/cm2. However, at wPt = 9.66 lg/cm2 prepared from 63.2 wt%-Pt/ CB, the value of jk at each potential is apparently low probably due to the low Pt utilization as described above. The present value of jk = ca. 0.7 mA/(Pt-cm2) for wPt 6 7.08 lg/cm2 at 0.80 V in air-saturated 0.1 M HClO4 is in good accord with jk = ca. 0.8 mA/cm2 for We have demonstrated the optimized method to prepare a Pt/CB supported RDE for the precise evaluation of ORR activity. Important points to disperse Pt/CB uniformly on the GC disk are: (1) adjustment of amount of Pt/CB so as to keep the weight of CB support constant at wCB = 5.70 ± 0.07 lg/cm2 (except 63.2 wt%-Pt) in 35 or 40 vol% ethanol aqueous suspension, (2) pipetting a suitable volume 51 lL/cm2 of the suspension on the GC, and (3) evaporation of the solvent droplet on the GC slowly under saturated vapor pressure of ethanol. Additional care must be taken for highly-loaded catalyst (63.2 wt%-Pt) so as to attach wPt 6 7 lg/cm2 on the GC for high Pt utilization. Nafion film coating on top of the catalyst layer must be very thin (<0.1 lm) in order to minimize the film diffusion resistance. We have clearly shown that the area-specific ORR activity is independent of the Pt-loading level on CB from 19.2 to 63.2 wt% in airsaturated 0.1 M HClO4 electrolyte solution when the RDE is prepared by the optimized recipe. Acknowledgements This work was supported by CREST of Japan Science and Technology (JST) Corporation, and also was supported by the fund for ‘‘Leading Project’’ of Ministry of Education, Science, Culture, Sports and Technology of Japan. References Fig. 9. Dependence of kinetically controlled current density jk (per electrochemical active Pt surface area, SPt) on wPt for various Pt/CB– GC RDE measured in air-saturated 0.1 M HClO4 at 25 °C. Thickness of Nafion film; 0.05 lm. wPt is amount of Pt per geometric surface area of GC disk. [1] M. Watanabe, H. Igarashi, K. Yoshioka, Electrochim. Acta 40 (1995) 329. [2] N.M. Markovic, T.J. Schmidt, V. Stamenkovic, P.N. Ross, Fuel Cells 1 (2001) 105. [3] T.J. Schmidt, U.A. Paulus, H.A. Gasteiger, R.J. Behm, J. Electroanal. Chem. 508 (2001) 41. [4] U.A. Paulus, T.J. Schmidt, H.A. Gasteiger, R.J. Behm, J. Electroanal. Chem. 495 (2001) 134. [5] B.N. Grgur, N.M. Markovic, P.N. Ross, Can. J. Chem. 75 (1997) 1465. 76 E. Higuchi et al. / Journal of Electroanalytical Chemistry 583 (2005) 69–76 [6] N.M. Markovic, R.R. Adzic, B.D. Cahan, E. Yeager, J. Electroanal. Chem. 377 (1994) 249. [7] E. Yeager, M. Razaq, D. Gervasio, A. Razaq, D. Tryk, in: D. Scherson et al. (Eds.), Structural Effects in Electrocatalysis and Oxygen Electrochemistry, PV 92-11, The Electrochem. Soc., Pennington, NJ, 1992, p. 440. [8] H. Inoue, S.R. Brankovic, J.X. Wang, R.R. Adzic, Electrochim. Acta 47 (2002) 3777. [9] M.T. Paffett, J.G. Beery, S. Gottesfeld, J. Electrochem. Soc. 135 (1988) 1431. [10] U.A. Paulus, A. Wokaun, G.G. Scherer, T.J. Schmidt, V. Stamenkovic, V. Radmilovic, N.M. Markovic, P.N. Ross, J. Phys. Chem. B 106 (2002) 4181. [11] V.S. Murthi, R.C. Urian, S. Mukerjee, J. Phys. Chem. B 108 (2004) 11011. [12] H. Yang, W. Vogel, C. Lamy, N. Alonso-Vante, J. Phys. Chem. B 108 (2004) 11024. [13] M. Watanabe, S. Motoo, J. Electroanal. Chem. 60 (1975) 275. [14] M. Watanabe, S. Motoo, J. Electroanal. Chem. 60 (1975) 259. [15] H. Uchida, N. Ikeda, M. Watanabe, J. Electroanal. Chem. 424 (1997) 5. [16] M.L. Sattler, P.N. Ross, Ultramicroscopy 20 (1986) 21. [17] L.J. Bregoli, Electrochim. Acta 23 (1978) 489. [18] Y. Takasu, N. Ohashi, X.G. Zhang, Y. Murakami, H. Minagawa, S. Sato, K. Yahikozawa, Electrochim. Acta 41 (1996) 2595.
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