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International Journal of Electrochemistry
Volume 2011 (2011), Article ID 289032, 9 pages
http://dx.doi.org/10.4061/2011/289032
Research Article

The Electrochemical Development of Pt(111) Stepped Surfaces and Its Influence on Methanol Electrooxidation

1Núcleo Ingeniería Electroquímica, Facultad de Ingeniería, Instituto de Ingeniería Química-Laboratorio de Electroquímica Fundamental, Facultad de Ciencias, Instituto de Química Biológica, Rodó 1843, Udelar, Montevideo 11400, Uruguay
2Laboratorio de cristalografía, estado sólido y materiales (Cryssmat-Lab), DETEMA, Centro NanoMat, Polo Tecnológico de Pando, Facultad de Química, Gral. Flores 2224, Udelar, Montevideo 11000, Uruguay

Received 1 April 2011; Accepted 6 May 2011

Academic Editor: Maria E. Martins

Copyright © 2011 E. Teliz 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.

Abstract

The progress in the preparation of new electrode surfaces by electrochemical treatments exhibiting high faradaic efficiencies towards industrial electrocatalytic processes has gained more attention in today's scientific community. Most of the papers report new catalysts dispersed on different substrates, but some fundamental studies required for electrochemical and physical characterizations are sometimes forgotten. In this paper, we make a full staging of two electrochemical treatments that can be conducted to enhance the electrocatalytic activity of platinum surfaces, such as, electrofacetting through square wave potential programs and constant cathodic polarizations in the net hydrogen evolution region. The cathodic treatment applied at −2 V clearly develops (111) stepped planes similarly to the electrofacetting performed after applying the square wave program between 1.40 V and 0.70 V at 2.5 kHz. The X-ray diffraction patterns of both surfaces as well as on other electrofacetted platinum electrodes are obtained for comparison purposes. Moreover, the electrocatalytic activity towards methanol electrooxidation also exhibits equivalent coulombic efficiencies and 200% higher than on polycrystalline platinum as demonstrated by linear sweep voltammetry and potentiostatic current decays.

1. Introduction

A solid surface is a physical region that confines the crystal growth and the emergence of new physical properties different to those of the bulk. In the case of a solid/(liquid or gas) interface, the heterogeneous catalyst can lead to significant changes depending on the presence or the absence of an electric field. Moreover, a single-crystal (sc) solid/liquid interface is of special interest since it restricts the freedom degrees of surface mobility. Thus, surface atoms can take positions different from those expected depending on the characteristics of the applied electrode potential. This surface phenomenon is called reconstruction and is usually studied in physics with the help of ultrahigh vacuum (UHV) techniques [1]. However, this process strongly depends on the nature of the metal. Thus, platinum type metals are considered one of the most important catalysts as anodes and cathodes in polymer electrolyte fuel cells. This is mainly due to the large values of exchange current densities of the electrochemical reactions and the surface stability in the case of electrodissolution and/or electrodeposition [2, 3]. Surface reconstruction at platinum/solution interface is usually the result of an electronic redistribution occurring as a consequence of either ion adsorption or oxygen-containing species formation, finally leading to surface facets. In the case of polycrystalline (pc) surfaces, the formation of facets of a fixed crystal orientation is of particular interest for industrial applications such as electrosynthesis, fuel cell technology, and electrolysis [4, 5] due to the large stability even at potentials as high as 1.6 V.

The surface structure of a sc can be checked by a number of selected techniques such as scanning tunneling microscopy (STM) and atomic force microscopy (AFM) [6]; however, in the case of electrofaceted surfaces the atomic resolution is difficult to achieve due to the large number of defects. Moreover, other techniques are currently used to obtain the fingerprint of the electrode surface such as cyclic voltammetry (CV), which offers current versus potential data for sc and also for pc surfaces. CVs give important information about the adsorption/desorption states, phase formation of transitions, and so forth at the electrode surface as a function of potential. From the CV of platinum recorded between the potentials of solvent stability, one can distinguish the potential regions corresponding to the double-layer charging, hydroxide/oxide layer formation/reduction, and hydrogen adsorption/desorption [7].

In the case of noble metal interfaces, some CV current peaks can be assigned to defined X-ray diffraction (XRD) patterns [8, 9]. It was commonly accepted that a voltammetric peak is directly connected to a single X-ray excitation. However, it has been found that current intensities can also change between subsequent cycles because of surface restructuring induced by the electrode potential cycling [10, 11]. In the case of platinum, the effects of such cycles have been interpreted [12] as the progressive development of (110) or higher atomic stepped equivalent facets because of platinum oxide phase formation and reduction.

The morphology and structure of a catalyst surface has a strong weight on its electrochemical reactivity [3]. Thermo- or potential-induced surface reconstruction has been observed on clean metal surfaces with different crystallographies depending on type of atmosphere where the process is developed. If the rearrangement of surface atoms goes much further than atomic spacing, macroscopic changes, which are called surface reshaping, could happen to the surface morphology [13]. In particular, when pc metals are treated by periodic perturbing potentials, they are susceptible to remarkable changes in surface roughness and in the distribution of crystallographic faces, which is denoted as preferred crystallographic orientations via electrochemical faceting, [6, 8]. Tian et al. [14] reported the synthesis of platinum nanocrystals using repetitive square wave routines, and the obtained nanocrystals display high-index facets with a 400% more reactive activity than existing commercial platinum catalysts. Thus, surface restructuring in electrochemistry produces changes in the kinetics or even in the mechanism of various processes because of their strong sensitivity towards the metal surface structure [12, 15]. It has to be said that pc surfaces also exhibit surface restructuring, and in the case of the application of periodic potentials, they lead to the electroformation of microfacets [12]. It is well known that the application of fast potential periodic programs on platinum, rhodium, iridium, gold, or palladium produces permanent morphological changes with defined orientations, which depend on the potential limits and frequency of the routine by a microfacetting process [1618]. The electrochemical responses of these stepped surfaces are similar to those of stepped crystalline surfaces [19, 20].

It has been shown in a previous paper [21] that besides the main forces that drive the surface restructuration and microfacetting (oxygen and hydrogen electrosorption) the frequency of the square wave potential itself leads to a single propagation mode. This is the one responsible of the crystal lattice surface rearrangement, with new equilibrium positions that can be calculated with the potential periodic perturbations as parameters.

The voltammetry for the oxidation of methanol on sc platinum shows a clear hysteresis between the positive and negative going scans due to the accumulation of the poisoning intermediate at low potentials and its oxidation above 0.7 V versus RHE [22]. Additionally, the reaction is also very sensitive to the surface structure. The Pt(111) electrode has the lowest catalytic activity and the smallest hysteresis in a single voltammetric scan whereas Pt(100) electrode displays a much higher catalytic activity and a fast poisoning reaction. On the other hand, Pt(110) electrode depends on the pretreatment of the surface [23].

Besides the studies with the three basal planes, methanol electrooxidation was also performed on stepped platinum surfaces in order to clarify how exactly the step density influences this reaction. Shin and Korzenicwski [24] suggested that an increase of the step density catalyzes methanol decomposition whereas Tripković and Popvić [25] showed that the increase in the step density leads to a decrease in the surface activity towards methanol electrooxidation, both authors using . Housmans and Koper [26] studied methanol oxidation on stepped surfaces, and reported an increase in the activity with the step density, suggesting that the presence of steps with a orientation catalyzes methanol decomposition, carbon monoxide oxidation, and also the direct methanol oxidation. These kinds of studies are relevant not only from a fundamental point of view, but also for technical purposes, that is, once the proper crystallographic orientation is found, the technical electrode can be designed. Surfaces nanoparticules should be deposited in the carbon supported with the corresponding crystallographic orientation that resulted with the best electrocatalytic performance.

2. Experimental

Electrochemical runs were performed using a three-electrode compartment cell with a pc platinum wire of 0.5 mm diameter as a working electrode (99.999% purity, from Goodfellow Cambridge). A large area smooth platinum counter electrode and a reversible hydrogen reference electrode with a Luggin-Haber capillary tip completed the electrochemical system. Potential values in the text are given on the hydrogen reference electrode (RHE) scale. We employed 1 M sulphuric acid (96–98% analytical reactive from Baker) as supporting electrolyte, which was prepared using ultrapure water from Millipore-MilliQ plus (18.2 MΩ cm of resistivity). We performed the electrochemical experiments using a PGZ 301 Voltalab potentiostat-galvanostat with the Voltamaster 4 software.

To obtain the electrofacetted platinum surfaces (PtF), the electrodes were subjected to different potential techniques. However, the most attractive of all was the repetitive square wave potential scanning (RSWPS) in the symmetric form to avoid large surface roughness. To optimize the square wave potential parameters, we changed the lower   and upper   potentials together with the applied frequency, , only in the symmetric mode during a certain time . In all cases, the process was followed by registering the CV profile of the interface between 0.05 and 1.45 V at 0.10 Vs−1, always comparing with the nonperturbed electrode. The preferential oriented surface (facetted surface) with symmetries equivalent to and are obtained by widely changing the parameters shown above. The electrochemical experiments comprised the following stages: (i) electrode pretreatment involving repetitive triangular potential cycling at 0.1 Vs−1 between 0.05 and 1.50 V until a stabilized voltammogram was attained; (ii) the pretreated electrode was subsequently subjected to an RSWPS between and at , during a certain time or a cathodic treatment at  V during 30 min; (iii) the CV of the treated electrode was recorded again under the same conditions indicated in (i); (iv) XRD of the treated electrode were then obtained systematically.

We used the following criteria to estimate the development of preferred crystallographic orientation [6, 16]. The main voltammetric peak at low potentials of weakly bound hydrogen electrosorption at the platinum/acid interface ( ), originally assigned to the H-adatom-Pt(111) site interaction, corresponds to H-electrosorption on disturbed Pt(111) surfaces with a larger number of Pt(110) sites whereas the main voltammetric peak at higher potentials ( ; strongly bound H-adatoms) represents the H-adatom-Pt(100) site interaction. Accordingly, the height ratio between these two peaks, , can be taken arbitrarily to follow the degree of preferred crystallographic orientation achieved throughout the treatment described in (ii). Thus, for the untreated platinum surfaces electrode, the average ratio was ca. 0.84.

The most representative and relevant results involved a repetitive 5 KHz wave between  V and  V for faceted Pt(100) surfaces and the application of a 2.5 KHz between  V and  V for faceted Pt(111) surfaces. The current transients were recorded during the process and a potentiostatic holding at 0.05 V for 10 min was applied to eliminate dissolved molecular hydrogen under continuous nitrogen bubbling. Immediately after and under a continuous potential control, the CVs were run from 0.05 to 0.70 V at 0.10 Vs−1. All runs were achieved at 20 ± 2°C, under free oxygen conditions using nitrogen (99.998% purity) from Linde-Gas.

In order to study the electrocatalytic performance of the new surfaces produced by the electrofacetted and cathodic pretreatments two methodologies were carried out in oxygen-free 0.1 M methanol + 1 M sulphuric media, namely, linear sweep voltammetry and potentiostatic chronoamperometric curves. Linear sweep voltammetry was conducted on each surface starting from 0.10 V and scanning towards positive values at 0.010 Vs−1. Chronoamperometric curves were performed until 10 minutes at 0.60 V and 0.70 V for the nonperturbed and the treated surfaces. The charge density values under the chronoamperometric plots were calculated until that time only for comparison purposes.

X-ray powder diffraction data were collected using a Rigaku ULTIMA IV, 285 mm radius, Powder Diffractometer operating in Bragg-Brentano geometry. CuKα radiation (  Å) monochromatized with a diffracted beam bent germanium crystal was used to collect data over the 39 to 90 degree 2θ range in steps of 0.02° and 0.01° deg using a scintillation detector. Peak positions were extracted from the diffractograms using the program POWDERX [27]. Multiple datasets were collected for each sample in order to obtain representative values.

3. Results

3.1. Electrochemical Characterization

Figure 1(a) depicts the electrochemical profile of platinum after annealing. For these surfaces the current intensities ratio between and is 0.84. This is the original surface, which is taken as the blank of all the applied pretreatments. Figure 1(b) shows in this case a clear trend to develop the terraces with a ratio . The RSWPS treatment under the conditions described in Figure 1(c) produces remarkable changes in the voltammetric response of the treated surfaces as well as in the corresponding surface morphologies comparing to the blank. Likewise, the relative distribution of voltammetric peaks is modified, that is, the Pt F100 develops the ratio. On the other hand, the cyclic voltammetric profile as a result of the cathodic treatment is shown in Figure 1(d). The relative distribution of peaks is between the blank and the profile of Pt F(111), that is the ratio is 0.75. Due to the appearance of more electrochemical contributions, the voltammetric contours are slightly wider. It is likely that a stepped surface arises with global planes between that we consider the blank and the Pt F111.

fig1
Figure 1: Cyclic voltammetry in 1 M sulphuric acid between 0.05 V and 1.50 V run at 0.10 Vs−1 for (a) Pt pc annealing ; (b) Pt F(111) after a RSWPS  V,  V,  kHz, minutes, ; (c) Pt F(100) after an RSWPS  V,  V,  kHz, minutes, ; (d) CT Pt after  V, minutes. .
3.2. Structural Characterization by X-Ray Powder Diffraction (XRPD)

All the samples shown above in Figure 2 exhibit peak positions strictly corresponding to Pt0, which indicates no further oxidation at the catalyst occurring after applying the RSWPS. It is important to mention that all the samples present good stability, since they were also measured after periods of one month and presented no difference in the diffractograms.

fig2
Figure 2: Ex situ X-ray powder diffraction pattern peaks , , , , and for pc Pt (black lines), Pt F100 (light grey lines), CT Pt (grey lines), and Pt F111 (dark grey lines).

When comparing the diffractograms of the treated samples, important changes can be seen in the relative intensity of the Bragg’s peaks. This fact reflects the preferential orientation obtained by the RSWPS and the stepped planes developed after the CT, see Table 1 for details.

tab1
Table 1: Integrated intensities for pc Pt, CT Pt, Pt F100, and Pt F111 electrodes. The intensities are expressed as intensity * Δ(2θ) = counts * degree.

In the first case, the starting sample corresponds to the pc platinum wire with the intensity of and reflections considerable higher than the others. Since it is difficult to establish a direct comparison between the occurrences of lattice planes with the corresponding reflection intensities, we defined a “weighted intensities” using relative currents. The weights are cleared in terms of the intensities of the bulk platinum reflections. For example, platinum bulk has and . They have equal occurrence in pc samples, so the direct ratio between unnormalized intensities leads to . If we define the weighted ratio as , the number give us a direct estimation of the proportion between lattice planes.

Table 2 presents the weighted ratio for all the studied samples. According with this data pc platinum has an important contribution from reflection in comparison with , that is, . This behavior is similar to the sample with CT, followed by the sample with faceting treatment to direction (F100). The same trend is observed for reflection in the three cases. The main difference between pc and CT platinum is in the reflection, which is considerably high for the first sample. The XRPD is not grazing incidence experiments, so the conclusions cannot be only attributed to surface phenomena, but they can be attributed to both surface and bulk material. In this sense, the pc orient planes and and can be easily interpreted in terms of and surface stepping like and . This feature is slightly modified after the CT, since the intensity of the reflection is reduced by a factor of ca. 3.8. This fact is interpreted as a reduction in the stepping, when a restitution of the reflection occurs characterized by the weighted ratio . According to this, the CT favors the and stepping as presented in Figure 2 and Table 2.

tab2
Table 2: Weighted ratio for the reflections in pc Pt, CT Pt, Pt F100, and Pt F111 electrodes.

Regarding the Pt F100 sample, the faceting process does not establish a clear change in the proportion of the lattice planes, since the weighted ratio shows the lowest value after comparing Pt F100 with pc platinum and CT platinum. Another feature is the intensity of the reflection, which shows an intermediate contribution with an intensity positioned between those of pc and CT platinum.

Finally, the Pt F111 sample is the one with greatest differences, with a nearly net contribution arises from the lattice planes referred with the lattice planes. Additionally, the contribution of and reflections is considerably lower than on the other samples. This is a confirmation that the faceting process is a process after which there is a strong decrease in the proportion of surface stepping, as observed in pc and CT platinum.

3.3. Electrocatalytic Activity Towards Methanol Oxidation
3.3.1. Linear Sweep Voltammetry in Methanol Acid Media

The first positive-going potential scan starting from 0.10 V up to 1.20 V for methanol electrooxidation on annealing Pt pc and electrofacetted platinum surfaces in 0.1 M methanol + 1 M sulfuric acid media are shown in Figure 3. A maximum current density is observed at ca. 0.85 V, above which the rate of methanol oxidation decreases due to platinum oxide formation (which also deactivates the surface). After the pretreated procedure was applied in acid solution, the peak current density for Pt F111 depicts the greatest value, very similar to CT Pt. These values were more than 200% greater than that obtained on the untreated electrode. The electrocatalytic activity of pretreated surfaces was enhanced even after several cycles; contrary to the expected results on carbon monoxide poisoning induced on platinum surfaces.

289032.fig.003
Figure 3: First positive-going potential scan for methanol oxidation run at 0.10 Vs−1 between 0.10 and 1.20 V in oxygen-free 0.1 M methanol + 1 M sulphuric media on Pt F(111) (dotted gray lines); CT Pt (gray lines); Pt F(100) (dark gray lines) and annealed Pt (black lines).
3.3.2. Chronoamperometric Plots in Methanol Acid Media

Chronoamperometric curves were run for methanol oxidation on all platinum surfaces under two different constant potentials 0.60 V (not shown) and 0.70 V (Figure 4). All surfaces usually illustrate a typical diffusion-controlled current decay, but at 0.70 V, pc surfaces exhibit a first current increase at very short times. This fact is the result of a competitive process between adsorbed carbon monoxide and methanol oxidations with opposite contributions in the parallel oxidation mechanism, that is, the competition between the series and direct methanol oxidations. The pc platinum surface seems to be poisoned by a greater extent of carbon monoxide adsorbates. This effect is not observed at potentials lower than 0.70 V. The charge density at a fixed potential found under the current transients evidenced the real electrocatalytic activity of the surface. Table 3 represents the integration of the charge until 10 min (as comparison) for treated and untreated electrodes as a function of the potential. At 0.60 V, methanol oxidation did show a current contribution on the cathodic treated surface as well as on the Pt F111, not distinguished on the others surfaces. However, for 0.70 V, the charge densities found on the CT and Pt F111 surfaces are always higher than those of untreated platinum and other electrofacetted surfaces.

tab3
Table 3: Integrated charge densities found under the current transients for methanol electrooxidation after 10 min. in oxygen-free 0.1 M methanol + 1 M sulphuric media on the studied platinum surfaces.
289032.fig.004
Figure 4: Chronoamperometric plots for methanol oxidation in oxygen-free 0.1 M methanol + 1 M sulphuric media at 700 mV on: pc Pt (black lines), Pt F100 (light grey lines), CT Pt (grey lines), and Pt F111 (dark grey lines).

4. Discussion

The electrode composition plays an important role in the course of an electrocatalytic reaction, especially in the poison species removal. However, the surface morphology of technical electrodes is also important since it controls other factors associated with the formation and conversion of adsorbates. The relationship between the particle shape and the surface structure is of real importance in Electrocatalysis since its optimization is one of the best ways to enhance the selectivity and efficiency in the search of an adequate surface distribution for coadsorbate reactions.

Platinum crystallizes as a face centered cubic system with a cell parameter of 3.92 Å. This system presents three base planes normal to the , , and vectors in its three-dimensional crystal lattice. In fact the plane is really , and not a true basal plane, so it is the first clue of an intrinsic atomic reconstruction. These three main vectors are the origin of the lowest Miller indices surfaces with a single type of symmetry. When the Miller indices increase, also does the complexity of the surface. For simplicity, these high Miller indices surfaces are considered as a combination of the different base planes in different proportions yielding terraces, monoatomic step and also kinks. The stepped surfaces present atomic terraces with a define orientation corresponding to a single base plane, separated by monoatomic steps of a certain symmetry. Lang et al. [28] proposed that the stepped surfaces have to be named taking the Miller indices of each terrace and step, with also the number of atomic files at the terrace. The nomenclature for a stepped surface is being the chemical symbol of the metal, the number of atomic files at the terrace, the letter between parenthesis indicates that it is a stepped surface and and ( ) the Miller indices of the base planes that define the terraces and steps, respectively.

Methanol electrooxidation on platinum stepped or disordered surfaces is driven by two important factors; the total surface charge and the presence of water adjacent molecules in the aqueous phase. At the Pt(111) single crystal surface, the methanol molecule is located at a reactive position due to the formation of hydrogen bonds with a preadsorb water molecule [29]. It has been observed that the hydrogen bond strength of the methanol-water interaction at the surfaces is larger than on , leading to a more exothermic adsorption for methanol [30]. However, the importance of the presence of preadsorbed water is demonstrated from the fact of the lower total exothermic condition for the cascade dehydrogenation (0.7 eV) at the Pt(111)/water interphase than at the Pt(111)/vacuum interphase [31, 32]. This fact is explained by the stabilization of the hydrogen bond in the complex and the weakened of the water/platinum interaction. Thus, adsorbed water molecules on platinum in acid media vibrates from 3500 to 3000–3100 cm−1, but in the presence of adsorbate neighbours changes to a new vibration range due to the asymmetric stretching of the O-H bond at 3658 cm−1 [33]. Using in situ ATR-SEIRAS techniques it is demonstrated that water coexists with adsorbed carbon monoxide derived from methanol partial oxidation. Water is consumed during oxidation according to the adsorbed water and on-top carbon monoxide intensities. This is a strong confirmation that both water and carbon monoxide molecules coexists at the surface and that each species directly react from the surface promoting the further oxidation of other methanol molecules [34].

On the other hand, the change in the structure of the interfacial water structure caused by methanol adsorption is responsible of the difference between the experimental potential of zero charge (pzc) determined for the Pt(111-) CO interaction, 1.10 V, and the pzc estimated for the Pt(111-) water, 0.23 V [35]. Using these values it is possible to calculate mean angle between the water dipolar moment and the platinum surface. At room temperature pzc, diminishes from 7.85° for Pt(111-) water to 1.46° for Pt(111)-CO [35]. Chang and Weaver [36] have found that the water coadsorption at low coverages favours on Pt(111) the formation of bridge COads. The vibration frequencies for linear and bridge geometries at high surface coverages by carbon monoxide are at least 20–30 cm−1 lower in the electrochemical environments than in UHV conditions. These environmental effects observed for the COads bond suggests that the double layer effects are much more important than expected in the early stages of the anodic electrocatalytic reactions. Besides, the same important interaction between water and COads has been also observed using in situ IRAS and STM techniques [37]. Adsorbed carbon monoxide on Pt(111) at 0.40 V shows a strong interaction with water molecules at the external layer retarding methanol oxidation to carbon dioxide, while its adsorption at 0.050 V reports lower values of oxidation onset potentials. Moreover, it has been also reported that [29] methanol oxidation starts with the formation of a strong interaction leading to a hydrogen bond between the hydroxyl group of methanol with the water molecule. The first step of the reaction is the anchorage of a carbon-hydrogen bond focused towards the platinum surface. In this sense, our results clearly shows a larger activity in the case of the cathodic treated and the (111-) faceted platinum surfaces where the presence of stepped planes are able to produce this strong interaction between partially dissociated water on steps and adsorbed carbon monoxide from methanol partial oxidation on terraces. The perfect combination of both effects of a proper crystal orientation at the steps and a distinct but adequate in the terraces are the theoretical concept in the catalysts design for the electrocatalytic oxidation reaction. The Pt F111 surface exhibit a good catalytic activity at lower potentials than CT Pt, but the latter exhibits larger charge densities at 0.70 V. This fact is the result of adsorbed hydroxyl species are produced on Pt F111 at lower potentials increasing then the catalytic activity at 0.60 V. However, since methanol posses a larger affinity towards the oriented surfaces (as a consequence of its structural spatial conformation), at 0.70 V the stepped produced from the cathodic polarization method will exhibit a higher activity towards methanol oxidation. The relation between crystallographic orientation and oxidation catalytic activities are confirmed in the case of comparing Pt F100 and pc platinum surfaces.

5. Conclusions

(a) The electrochemical perturbation of platinum surfaces through RSWPS changes the surface relative distribution of crystallographic planes. This effect reaches the bulk of the metal up to the first layers of platinum, making possible the X-ray diffraction analysis.

(b) A net and practically single plane contribution is obtained after obtaining a Pt F111 surface, however, for Pt F100, a stepped surface with a plane main contribution is developed. The latter seems to be more an intermediate surface between pc and CT platinum. Moreover, the rearrangement produced at the CT platinum surface, yields facets with stepped planes equivalent to .

(c) The electrocatalytic studies towards methanol oxidation conclude that both Pt F111 and CT Pt exhibit similar results and better than pc platinum with also a better tolerance upon surface poisoning. According to our knowledge water species are activated on terraces at lower potentials than on planes leading to adsorbed OH species with larger adsorption energies. Consequently, methanol adsorbates are not able to displace these ordered water species only enabling its surface diffusion from terraces to steps to finally adsorb there.

(d) The simple application of a constant cathodic current in the true hydrogen evolution region on pc platinum enhances the catalytic activity towards methanol electrooxidation, since the stepped are morphologically more adequate to catalyse the reaction.

Acknowledgments

The authors are greatly acknowledged to the PDT Projects of the Education Ministerial Office. V. Díaz, R. Faccio, A.W. Mombrú, and C. F. Zinola are researchers at the Chemistry Area of PEDECIBA United Nations.

References

  1. P. V. Pávlov and A. F. Jojlov, Solid State Physics, chapter 5 and 7, Mir, Moscow, Russia, 1987.
  2. C. Sanchez and E. Leiva, “The NEMCA effect,” in Handbook of Fuel Cells, W. Vielstich, H. A. Gasteiger, and A. Lamm, Eds., vol. 2, chapter 5, John Wiley & Sons, Chichester, UK, 2003.
  3. N. M. Markoví and P. N. Ross Jr., “Surface science studies of model fuel cell electrocatalysts,” Surface Science Reports, vol. 45, no. 4-6, pp. 117–229, 2002.
  4. G. A. Somorjai, Introduction to Surface Chemistry and Catalysis, chapter 2, John Wiley & Sons, New York, NY, USA, 1994.
  5. G. A. Somorjai, Electrochemical Surface Science: Molecular Phenomena at Electrode Surfaces, American Chemical Society, Washington, DC, USA, 1988.
  6. A. J. Arvia, J. C. Canullo, E. Custidiano, C. L. Perdriel, and W. E. Triaca, “Electrochemical faceting of metal electrodes,” Electrochimica Acta, vol. 31, no. 11, pp. 1359–1368, 1986. View at Scopus
  7. S. Trasatti and O. A. Petrii, “Real surface area measurements in electrochemistry,” Journal of Electroanalytical Chemistry, vol. 327, no. 1-2, pp. 353–376, 1992. View at Scopus
  8. M. Fleischmann and B. W. Mao, “In situ X-Ray diffraction measurements of the surface structure of Pt in the presence of “weakly” adsorbed H,” Journal of Electroanalytical Chemistry, vol. 247, no. 1-2, pp. 311–313, 1988. View at Scopus
  9. H. P. Klug and L. E. Alexander, X-Ray Diffraction Procedures for Polycrystalline and Amorphous Materials, John Wiley & Sons, New York, NY, USA, 2nd edition, 1974.
  10. L. A. Kibler, A. Cuesta, M. Kleinert, and D. M. Kolb, “In-situ STM characterization of the surface morphology of platinum single crystal electrodes as a function of their preparation,” Journal of Electroanalytical Chemistry, vol. 484, no. 1, pp. 73–82, 2000. View at Publisher · View at Google Scholar · View at Scopus
  11. D. M. Kolb, “Structure studies of metal electrodes by in-situ scanning tunneling microscopy,” Electrochimica Acta, vol. 45, no. 15-16, pp. 2387–2402, 2000.
  12. W. E. Triaca and A. J. Arvia, “The electrochemical facetting of metal surfaces: preferred crystallographic orientation and roughening effects in electrocatalysis,” Journal of Applied Electrochemistry, vol. 20, no. 3, pp. 347–356, 1990. View at Publisher · View at Google Scholar · View at Scopus
  13. A. S. Dakkouri and D. M. Kolb, “Reconstruction of gold surfaces,” Interfacial Electrochemistry, chapter 10, Marcel Dekker, New York, NY, USA, 1999.
  14. N. Tian, Z. Y. Zhou, S. G. Sun, Y. Ding, and L. W. Zhong, “Synthesis of tetrahexahedral platinum nanocrystals with high-index facets and high electro-oxidation activity,” Science, vol. 316, no. 5825, pp. 732–735, 2007. View at Publisher · View at Google Scholar · View at PubMed · View at Scopus
  15. A. J. Arvia, R. C. Salvarezza, and W. E. Triaca, “The development of metal overlayers with smooth and rough topographies,” Electrochimica Acta, vol. 34, no. 8, pp. 1057–1071, 1989. View at Scopus
  16. A. Visintín, J. C. Canullo, W. E. Triaca, and A. J. Arvia, “Changes in real surface area, crystallographic orientation and morphology of platinum electrodes caused by periodic potential treatments: phenomenological approach,” Journal of Electroanalytical Chemistry, vol. 239, no. 1-2, pp. 67–89, 1988. View at Scopus
  17. W. E. Triaca, T. Kessler, J. C. Canullo, and A. J. Arvia, “Study of the optimal conditions for the development of preferred oriented platinum surfaces by means of fast square wave potential perturbations,” Journal of the Electrochemical Society, vol. 134, no. 5, pp. 1165–1172, 1987. View at Scopus
  18. A. C. Chialvo, W. E. Triaca, and A. J. Arvra, “Changes in the electrochemical response of noble metals produced by square-wave potential perturbations. A new technique for the preparation of reproducible electrode surfaces of interest in electrocatalysis,” Journal of Electroanalytical Chemistry, vol. 146, no. 1, pp. 93–108, 1983. View at Scopus
  19. J. Gómez, L. Vázquez, A. M. Baró et al., “Surface topography of (100)-type electro-faceted platinum from scanning tunnelling microscopy and electrochemistry,” Nature, vol. 323, no. 6089, pp. 612–614, 1986. View at Publisher · View at Google Scholar · View at Scopus
  20. L. Vázquez, J. Gómez, A. M. Baró et al., “Scanning tunneling microscopy of electrochemically activated platinum surfaces. A direct ex-situ determination of the electrode nanotopography,” Journal of the American Chemical Society, vol. 109, no. 6, pp. 1730–1733, 1987. View at Scopus
  21. C. Bello and C. F. Zinola, “Crystallographic rearrangement of platinum induced by square wave potentials,” Journal of Colloid and Interface Science, vol. 258, no. 2, pp. 259–265, 2003. View at Publisher · View at Google Scholar · View at Scopus
  22. C. Lamy, J. M. Leger, J. Clavilier, and R. Parsons, “Structural effects in electrocatalysis. A comparative study of the oxidation of CO, HCOOH and CH3OH on single crystal Pt electrodes,” Journal of Electroanalytical Chemistry, vol. 150, no. 1-2, pp. 71–77, 1983. View at Scopus
  23. M. T. M Koper, S. C. S. Lay, and E. Herrero, Fuel Cell Catalysis: A Surface Science Approach, chapter 6, John Wiley & Sons, New York, NY, USA, 2009.
  24. J. Shin and C. Korzenicwski, “Infrared spectroscopic detection of CO formed at step and terrace sites on a corrugated electrode surface plane during methanol oxidation,” Journal of Physical Chemistry, vol. 99, no. 11, pp. 3419–3422, 1995.
  25. A. V. Tripković and K. D. Popović, “Oxidation of methanol on platinum single crystal stepped electrodes from [110] zone in acid solution,” Electrochimica Acta, vol. 41, no. 15, pp. 2385–2394, 1996. View at Publisher · View at Google Scholar
  26. T. H. M. Housmans and M. T. M. Koper, “Methanol oxidation on stepped Pt[n(111) × (110)] electrodes: a chronoamperometric study,” Journal of Physical Chemistry B, vol. 107, no. 33, pp. 8557–8567, 2003. View at Scopus
  27. C. Dong, “PowderX: windows-95-based program for powder X-Ray diffraction data processing,” Journal of Applied Crystallography, vol. 32, no. 4, p. 838, 1999.
  28. B. Lang, R. W. Joyner, and G. A. Somorjai, “Low energy electron diffraction studies of high index crystal surfaces of platinum,” Surface Science, vol. 30, no. 2, pp. 440–453, 1972. View at Scopus
  29. C. Hartnig and E. Spohr, “The role of water in the initial steps of methanol oxidation on Pt(1 1 1),” Chemical Physics, vol. 319, no. 1–3, pp. 185–191, 2005. View at Publisher · View at Google Scholar · View at Scopus
  30. C. Hartnig, J. Grimminger, and E. Spohr, “The role of water in the initial steps of methanol oxidation on Pt(2 1 1),” Electrochimica Acta, vol. 52, no. 6, pp. 2236–2243, 2007. View at Publisher · View at Google Scholar · View at Scopus
  31. R. Paul and S. J. Paddison, “Variational methods for the solution of the Ornstein-Zernicke equation in inhomogeneous systems,” Physical Review E, vol. 67, no. 1, part 2, Article ID 161081, 11 pages, 2003. View at Publisher · View at Google Scholar · View at MathSciNet
  32. Y. Okamoto, O. Sugino, Y. Mochizuki, T. Ikeshoji, and Y. Morikawa, “Comparative study of dehydrogenation of methanol at Pt(1 1 1)/water and Pt(1 1 1)/vacuum interfaces,” Chemical Physics Letters, vol. 377, no. 1-2, pp. 236–242, 2003. View at Publisher · View at Google Scholar · View at Scopus
  33. H. Shiroishi, Y. Ayato, K. Kunimatsu, and T. Okada, “Study of adsorbed water on Pt during methanol oxidation by ATR-SEIRAS (surface-enhanced infrared absorption spectroscopy),” Journal of Electroanalytical Chemistry, vol. 581, no. 2, pp. 132–183, 2005. View at Publisher · View at Google Scholar
  34. A. Cuesta, H. Shiroishi, Y. Ayato, K. Kunimatsu, and T. Okada, “Comments on the paper by H. Shiroishi, Y. Ayato, K. Kunimatsu and T. Okada entitled "Study of adsorbed water on Pt during methanol oxidation by ATR-SEIRAS (surface-enhanced infrared absorption spectroscopy)" [J. Electroanal. Chem. 581 (2005) 132],” Journal of Electroanalytical Chemistry, vol. 587, no. 2, pp. 329–332, 2006. View at Publisher · View at Google Scholar · View at Scopus
  35. A. Cuesta, “Measurement of the surface charge density of CO-saturated Pt(1 1 1) electrodes as a function of potential: the potential of zero charge of Pt(1 1 1),” Surface Science, vol. 572, no. 1, pp. 11–22, 2004. View at Publisher · View at Google Scholar · View at Scopus
  36. S. C. Chang and M. J. Weaver, “Coverage- and potential-dependent binding geometries of carbon monoxide at ordered low-index platinum- and rhodium-aqueous interfaces: comparisons with adsorption in corresponding metal-vacuum environments,” Surface Science, vol. 238, no. 1–3, pp. 142–162, 1990. View at Scopus
  37. K. Yoshimi, M.-B. Song, and M. Ito, “Carbon monoxide oxidation on a Pt(111) electrode studied by in-situ IRAS and STM: coadsorption of CO with water on Pt(111),” Surface Science, vol. 368, no. 1–3, pp. 389–395, 1996. View at Publisher · View at Google Scholar