Young-Woo
Lee
,
A-Ra
Ko
,
Do-Young
Kim
,
Sang-Beom
Han
and
Kyung-Won
Park
*
Department of Chemical Engineering, Soongsil University, Seoul 156743, Republic of Korea. E-mail: kwpark@ssu.ac.kr; Fax: +82-2-812-5378; Tel: +82-2-820-0613
First published on 12th December 2011
Structure-controlled Pt-based catalysts have been known to exhibit improved electrocatalytic activities due to particularly modulated surface structures favorable for hydrogen oxidation or oxygen reduction reactions. We prepare octahedral Pt-Pd alloy nanoparticles such as Pt3Pd1, Pt1Pd1, Pt1Pd3 by reducing metal ions with glycerol as a reducing agent in an aqueous solution. The octahedral Pt-Pd nanoparticles are well-defined alloy nanostructures with dominant {111} facets. Among them, the octahedral Pt3Pd1 shows excellent electrochemical properties i.e., much enhanced electrocatalytic activity and stability for oxygen reduction reactions in comparison with conventional Pt-based catalysts.
According to the typical ORR mechanism on Pt-based electrodes in acidic medium, Pt3M1 catalysts exhibit such an improved electrocatalytic activity in comparison with Pt-M alloy catalysts with different compositions between Pt and M.13 In particular, pure Pd as a 2nd metal with similar binding energies of O and OH exhibits comparable activity to that of Pt in an ORR. It has been reported that Pt-Pd alloy catalysts have exhibited excellent electrocatalytic activity due to the modified electronic structure of the electrodes in comparison with pure Pt. The modified electronic properties of the Pt-Pd catalysts might result from Pt containing a negative charge and vacant valence d-orbital and Pd containing a positive charge and fully occupied valence d-orbital. Recently, the Pt-Pd alloy catalysts with Pt-rich composition have showed a much higher oxygen reduction activity compared to a pure Pt catalyst.14,15
In order to enhance the ORR activity of metallic nanostructure catalysts, there have been many efforts to manipulate the structure and shape of the catalysts during the synthesis process of metallic nanoparticles.16–19 The structure or shape-controlled metallic catalysts have exhibited improved electrochemical activities due to a particular surface exposure, which is favorable for electrocatalytic reactions. In general, it has been reported that the order of the ORR activity in Pt-based catalysts with low index planes is as follows: (100) < (111) < (110) in HClO4 electrolyte.20,21 Lim et al. reported a bimetallic Pt-Pd nanostructure synthesized with L−ascorbic acid in an aqueous solution that could improve oxygen reduction activity in comparison with a polycrystalline Pt catalyst.22
Herein, we synthesized octahedral Pt-Pd alloy NPs with dominant {111} facets by reducing metal ions with glycerol as a reducing agent in aqueous solution. According to the metal reduction mechanism using glycerol, metal ions are reduced to metal atoms by glyceraldehydes containing an aldehyde (–CHO) functional group, which is transformed into glyceric acid containing a carboxyl (–COOH) group.23,24 The reducing agents containing many hydroxyl functional groups may result in a much faster reduction reaction than those containing fewer hydroxyl functional groups.25,26
The morphology, crystal structure, elemental composition, and chemical states of the NPs were investigated by transmission electron microscopy (TEM), energy dispersive X-ray spectroscopy (EDX), X-ray diffraction (XRD), and X-ray photoelectron spectroscopy (XPS). The electrochemical and electrocatalytic properties of the as-prepared catalysts were obtained in a typical electrochemical cell using a potentiostat.
The structure analysis of the as-synthesized Pt-Pd NPs was examined by field-emission transmission electron microscopy (FE-TEM) in Fig. 1(a–c) (Fig. S1(a, d, and g), ESI†). The average size and yield of the octahedron in the Pt3Pd1, Pt1Pd1, and Pt1Pd3 NPs are ∼11.3 nm and ∼92.4%, ∼8.3 nm and ∼97.0%, and ∼8.4 nm and ∼84.7%, respectively (Fig. 1(a–c) and Fig. S2(a–c), ESI†). In the present synthesis of the octahedral Pt-Pd NPs, the glycerol can lead to faster reduction reaction of metal ions. Also, the fast reduction reaction might tend to thermodynamically minimize crystalline surface energy thus forming crystal facets with the lower surface energy in the structure. The surface energy of {111} facets in fcc metallic structures such as Pt and Pd is lower than that of other low-index planes.27 In the case of Pt, the surface energies of {111}, {100}, and {110} facets are 1.004, 1.378, and 2.009 eV atom−1, respectively. In the case of Pd, the surface energies of {111}, {100}, and {110} facets are 0.824, 1.152, and 1.559 eV atom−1, respectively. This shows that the octahedral Pt-Pd NPs can favorably expose {111} facets caused by the rapid reduction reaction in the synthetic atmosphere. Fig. 1(d–f) show line scanning profiles using energy dispersive X-ray spectroscopy (EDX) of the octahedral Pt-Pd NPs. As confirmed by EDX profiles (Fig. S1(c, f, and i), ESI†), the elemental compositions of Pt and Pd in the octahedral NPs are 74.74 and 25.26 at% for Pt3Pd1, 47.80 and 52.20 at% for Pt1Pd1, and 25.69 and 74.31 at% for Pt1Pd3, respectively. Fig. 1(g–i) show high-resolution TEM images of the octahedral Pt-Pd NPs. The as-synthesized Pt3Pd1, Pt1Pd1, and Pt1Pd3 NPs represent a d-spacing of the {111} plane corresponding to alloy structures between Pt and Pd metallic phases. The corresponding fast Fourier transform patterns (the insets of Fig. 1(g–i)) indicate that the octahedral Pt-Pd NPs are single nanocrystals enclosed by {111} facets. Furthermore, as shown in Fig. S1(b, e, and h), ESI,† the octahedral Pt3Pd1, Pt1Pd1, and Pt1Pd3 NPs can be homogeneously deposited on carbon (Vulcan XC-72R) as carbon supported catalysts for fuel cell applications.
Fig. 1 TEM images of Pt3Pd1 (a), Pt1Pd1 (b), and Pt1Pd3 (c). The inset shows HAADF-STEM (high-angle annular dark-field scanning transmission electron microscopy) images of Pt-Pd NPs for line-scanning profiles [white scale bar is 5 nm]. Line-scanning profiles across Pt-Pd NPs: Pt3Pd1 (d), Pt1Pd1 (e), and Pt1Pd3 (f) of the inset images of Fig. 1(a–c). HR-TEM Images of Pt-Pd NPs: Pt3Pd1 (g), Pt1Pd1 (h), and Pt1Pd3 (i). The insets indicate the FFT patterns of Pt-Pd NPs. |
Fig. 2(a) shows X-ray diffraction (XRD) patterns of carbon supported octahedral Pt-Pd catalysts containing Pt3Pd1, Pt1Pd1, and Pt1Pd3 NPs. The XRD patterns of the octahedral Pt-Pd catalysts contain diffraction peaks corresponding to (111), (200) and (220) of a typical fcc crystal structure. Assuming a substitutional solid solution between metallic phases, the higher angle shift of the XRD peaks indicates alloy formation between Pt and Pd. As indicated in Fig. 2(b), the XRD peaks in the octahedral Pt-Pd NPs are shifted into higher 2θ values with an increasing amount of Pd, i.e., 67.67°, 67.75°, and 67.94° in (220) diffraction peaks corresponding to Pt3Pd1, Pt1Pd1, and Pt1Pd3 NPs, respectively. Based on the Vegard's law using the equation of dPtPd = X·dPt + (1-X)·dPd, the atomic composition of Pt and Pd in Pt3Pd1, Pt1Pd1, and Pt1Pd3 is 67.62 and 32.38 at%, 55.62 and 44.38 at%, and 27.14 and 72.86 at%, respectively. The lattice parameters of the octahedral Pt-Pd NPs reflecting the degree of alloying in the bimetallic structures are given in Fig. 2(c). Since the radius of the Pt atom (0.139 nm) is greater than the radius of a Pd atom (0.137 nm), the crystalline lattice parameters of the Pt-Pd NPs increase with increasing elemental composition of Pt. The octahedral Pt-Pd NPs appear on a straight fitted line based on the solid solution between Pt and Pd, which means a well-defined alloy formation between Pt and Pd. The surface chemical state and composition of individual components in the octahedral Pt-Pd/C catalysts were obtained by X-ray photoelectron spectroscopy (XPS) in comparison with Pt/C. For the octahedral Pt3Pd1, Pt1Pd1, and Pt1Pd3 alloy NPs, Pt 4f and Pd 3d spectra are shown in Fig. 3(a–h). The Pt 4f7/2 and 4f5/2 peaks typically appear at ∼71 and ∼74 eV, respectively, with a theoretical area ratio of 4:3. The Pd 3d5/2 and 3d3/2 peaks typically appear at ∼335 and ∼340 eV, respectively, with a theoretical area ratio of 3:2.28,29 The elemental compositions of Pt and Pd in the Pt-Pd NPs measured by XPS are as follows: 71.64 at% of Pt and 28.38 at% of Pd in the Pt3Pd1/C, 49.44 at% of Pt and 50.56 at% of Pd in the Pt1Pd1/C, and 34.07 at% of Pt and 65.93 at% of Pd in the Pt1Pd3/C. Furthermore, the Pt 4f peaks in the octahedral Pt-Pd/C and Pt/C consist of metallic and oxide states, i.e., the peaks for Pt0 and Pt2+ at 71.0 and 73.8 eV, respectively (Fig. 3(a–d)). The Pd 3d peaks in the octahedral Pt-Pd/C consist of metallic and oxide states, i.e., the peaks for Pd0, Pd2+, and Pd4+ at 335.2, 336.3 and 337.9 eV, respectively (Fig. 3(e–g)). By comparing the EDX, TEM, and XRD data of the NPs (Table 1), it can be concluded that the octahedral Pt-Pd NPs are well-defined alloy nanostructures. Furthermore, this represents that the octahedral Pt-Pd alloy NPs prepared by the present synthetic process show the homogeneous distribution of Pt and Pd atoms in surface and bulk of the alloy NPs.
Fig. 2 (a) Wide-range XRD patterns of Pt3Pd1/C, Pt1Pd1/C, and Pt1Pd3/C in comparison with XRD reference data of Pt (red) and Pd (blue). (b) The diffraction peaks of (220) planes in the catalysts are compared with XRD reference data of Pt (JCPDS No. 04-0802, red) and Pd (JCPDS No. 46-1043, blue). (c) The plot of lattice parameter versusPt atomic percentage of the Pt-Pd catalysts. |
Fig. 3 Surface and chemical analysis by XPS. Pt 4f spectra in Pt3Pd1/C (a), Pt1Pd1/C (b), Pt1Pd3/C (c), Pt/C (d). Pd 3d spectra in Pt3Pd1/C (e), Pt1Pd1/C (f), Pt1Pd3/C (g). Comparison of chemical states and ratios of Pt 4f and Pd 3d spectra of all catalysts measured and calculated from the XPS fitting data. |
Fig. 4 (a) Specific activity curves of as-prepared catalysts on oxygen reduction reaction at 0.55 V normalized to the EASAs calculated by integrating the hydrogen adsorption charge in the CVs. (b) Comparison of the ORR activities on as-prepared catalysts. Specific activity and mass activity were all measured at 0.55 V. |
The accelerated durability test of the ORR was performed by applying linear potential sweeps between 0.4 and 0.9 V in O2-saturated 0.1 M HClO4 solution at 25 °C. To confirm the effect of Pt3Pd1 alloy nanostructure on the ORR, we synthesized spherical Pt3Pd1 NPs deposited on carbon black (S–Pt3Pd1/C) by the polyol process using ethylene glycol with NaOH as additive agent (see Experimental section, ESI†). The average size of the S–Pt3Pd1 NPs is ∼3.86 nm. By EDX analysis, the elemental compositions of Pt and Pd in the as-synthesized S–Pt3Pd1 NPs are 71.64 at% and 28.36 at%, respectively (Fig. S5, ESI†). The ORR activity of the S–Pt3Pd1/C was measured using linear sweep voltammetry in O2-saturated HClO4 solution (Fig. S6, ESI†). The area-kinetic current densities (jk,Area) of Octa–Pt3Pd1/C, S–Pt3Pd1/C, and Pt/C at 0.55 V in the ORR are 1.228, 0.820, and 0.523 mA cm−2, respectively (Fig. 5(g)). Furthermore, the mass-kinetic current density (jk,Mass) of the Octa–Pt3Pd1/C (0.094 mA μg−1Pt) is 1.27 and 1.88 times higher than the S–Pt3Pd1/C (0.074 mA μg−1Pt) and Pt/C (0.050 mA μg−1Pt), respectively. Accordingly, the highly electrocatalytic activity for ORR may be due to the particular composition of the Pt3Pd1 alloy catalyst in comparison with pure Pt. Furthermore, it is confirmed that the octahedral Pt3Pd1 NPs with dominant {111} facets can provide much improved oxygen reduction reaction in comparison with spherical Pt3Pd1 NPs. Thus, we can demonstrate that the Octa–Pt3Pd1/C exhibits improved electrocatalytic properties due to octahedral shape with dominant {111} facets and particular elemental composition.
Fig. 5 Cyclic voltammograms of Octa–Pt3Pd1/C (a), S–Pt3Pd1/C (b), and Pt/C (c) before and after durability test in Ar–saturated 0.1 M HClO4 with a scan rate of 50 mV s−1 at 25 °C. The accelerated durability test was carried out by applying linear potential sweeps between 0.4 and 0.9 V for 2000 cycles with a scan rate of 50 mV s−1 in O2–saturated 0.1 M HClO4 solution at 25 °C. ORR polarization curves of Octa–Pt3Pd1/C (d), S–Pt3Pd1/C (e), and Pt/C (f) before and after the durability test in O2–saturated 0.1 M HClO4 with a scan rate of 5 mV s−1. (g) Comparison of the ORR activities on as-prepared catalysts. Specific activity and mass activity were all measured at 0.55 V before the durability test. (h) Comparison of EASAs of Octa–Pt3Pd1/C, S–Pt3Pd1/C, and Pt/C before and after durability test. (i) Comparison of ORR current density at 0.55 V of Octa–Pt3Pd1/C, S–Pt3Pd1/C, and Pt/C before and after durability test in Fig. 5(d–f). |
The EASAs of Octa–Pt3Pd1/C, S–Pt3Pd1/C, and Pt/C before and after the ORR durability test were measured by integrating the charges on the Hupd desorption region of the CVs as shown in Fig. 5(a–c). In Fig. 5(h), the Octa–Pt3Pd1/C exhibits a negligible loss of 2.0% in EASA after 2000 cycles of the durability test whereas S–Pt3Pd1/C and Pt/C exhibit losses of 57.36% and 52.77% after the durability tests, respectively. Since the change of size and morphology for catalysts before and after durability test could affect the whole activity, their size distribution and shape should be observed and compared (Fig. S7–S9, ESI†). The Octa–Pt3Pd1/C shows a slight reduction of size and nearly the same morphology after the durability test, maintaining such an improved electrocatalytic activity (Fig. S7, ESI†). The improved stability of the Octa–Pt3Pd1/C might result from shape effect due to unique morphology.33,34 In contrast, after the durability test, S–Pt3Pd1/C and Pt/C exhibit non-uniform size distribution because of instability of metal catalysts resulting in deteriorated catalytic activity (Fig. S8 and S9, ESI†). Fig. 5(d–f) show the ORR measurements before and after the durability test between 0.0 and 0.8 V with a scan rate of 5 mV s−1 in O2-saturated 0.1 M HClO4 solution at 25 °C. In the case of half-wave potentials,35 the Octa–Pt3Pd1/C exhibits a slight decrease of ∼14 mV, whereas S–Pt3Pd1/C and Pt/C exhibit a rapid decrease of ∼50 and ∼34 mV, respectively. As indicated in Fig. 5(i), based on the geometric area of the glassy carbon electrode in the Fig. 5(d–f), the current density of the Octa–Pt3Pd1/C at 0.55 V after the durability test is slightly reduced from 3.123 mA cm−2 (before the durability test) to 2.712 mA cm−2. On the other hand, the current densities of S–Pt3Pd1/C and Pt/C after the durability test are rapidly reduced from 2.456 mA cm−2 and 2.374 mA cm−2 (before the durability test) to 0.735 mA cm−2 and 1.351 mA cm−2, respectively, at 0.55 V. Accordingly, we can expect that the highly improved electrocatalytic properties of the Octa–Pt3Pd1/C may result from thermodynamically stable surface exposure of {111} facets.
Footnote |
† Electronic Supplementary Information (ESI) available: Fig. S1–S9 contains TEM, EDX, and electrochemical data. See DOI: 10.1039/c1ra00308a/ |
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