# Oxygen-Containing Nanoclusters on the Surface of Pt-Electrodes and Oxygen Reduction Reaction in Alkaline Medium

Authors: Aleksey M. Trunov
Journal: International Journal of Electrochemistry
 (2018)

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## Abstract

Analysis of the role of oxygen-containing nanoclusters inoxygen reduction reaction (ORR) on Pt-electrodes in alkaline media is provided on the basis of the concept of electrochemical processes with slowed stage ofconsecutive heterogeneous chemical reaction (ConHCR). Under the ConHCR concept, the main factor determining the ORR characteristics isenergetic inhomogeneity of electrode surface (EIES) according to Temkin. A new concept, according to which EIES is determined by the Gibbs energy of formation of oxygen-containing surface structures with inclusions of surface defects of the platinum crystal structure, Pts,d, is formulated. A correlation between the level of EIES of Pt-electrodes and packing density of Pts,d atoms on the surface of Pt(hkl) monocrystals is determined. The concept, according to which the stationary potential of ORR process is considered as a “mixed potential” of two reactions (electrochemical reduction of surface atom PtIIs,d and consecutive oxidation of PtIs,d by molecular oxygen), is substantiated. It is proposed that the formation of surface nanocluster transition state [⁎(OO)PtIIs,d(OH)] defines the rate of the entire ORR process on Pt-electrodes in alkaline media.


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## Body

## 1. Introduction

Oxygen reduction reaction (ORR) is used in many electrochemical energy transformation devices (e.g., in low-temperature fuel cells). ORR process is experimentally studied in detail and, as reflected in a number of classical reviews [1–4], there is an experimental determination that platinum and platinum based alloys are characterized by the highest electrochemical activity. Nevertheless, analysis of the ORR literature data indicates that oxygen Pt-electrodes have some characteristic features which still do not have a systematic explanation. For example, one can note the following experimental facts.Fact #1. In experimental conditions, the standard value of oxygen electrode potential E=1.23 V in relation to the reversible hydrogen electrode (versus RHE) isnot reproduced in either acidic (reaction (1)) or alkaline (reaction (2)) media:(1)O2+4H++4e-⟷2H2O(2)O2+2H2O+4e-⟷4OH-As a rule, the stationary oxygen potential on polycrystalline [1–4] and monocrystalline [5–8] Pt-electrodes is reported within 0.9–1.1 V (versus RHE) range.Fact #2. There is an observation of existence on polarization curves for Pt-electrodes [9] of the current interval (10−7–10−6 А sm−2) without an appreciative change of the potential.Fact #3. According tocyclic voltammogram (CVA) data,oxygen-containing surface structures (OSS) are formed on the surface of Pt-electrodes at the range of ORR potentials [5–8, 10]. There is a report [5] that these structures influence ORR process. Thus, in a solution of HClO4 (0.1 M), ORR process on Pt(111) monocrystal proceeds in accordance with reaction (1). An addition of KBr solution (8·10-4 M) sharply changes the direction of ORR (the hydrogen peroxide H2O2 is formed instead of H2O molecule). The change of reaction direction correlates with change of state of monocrystal surface. Introduction of Br− ions leads to complete disappearance of peaks of formation of OSS on CVA (see Table 1).Table 1
Characteristics of CVA, potential of ORR start,Estart, ORR products on Pt(111) monocrystalline electrode [5].
Electrolyte Potential, V (vs RHE) ORR product Interval of anodic current Peak of anodic current Peak of cathodic current E s t a r t 0.1 M HClO4 0.55–0.85 0.75 0.75 0.90 H 2 O 0.1 M HClO4 + 10−4M KBr Absence of anodic current Absence of anodic current Absence of cathodic current 0.65 H2O2Fact #4. In 1 M H2SO4 solution, ORR process on Pt(hkl) monocrystal electrodes proceeds in accordance with reaction (1) at 0.90–0.95 V (versus RHE). Addition of 0.1 M HCl solution sharply changes the potentials of start of ORR process down to 0.720–0.620 V (the potentials of H2O2 formation) [11].Usage of concept of electrochemical process with slowed stage of consecutive heterogeneous chemical reaction (ConHCR) for systematic interpretation of characteristic parameters of ORR is substantiated in the author’s publications [12, 13]. In accordance with the concept, the ORR is described by Tafel equation with coefficient b=νRT/(pβnF), where ν is the stoichiometric number (number of repetitions of the slow stage of heterogenous chemical reaction), p is the reaction order with respect to oxygen, n is the number of electrons involved in the electrochemical actbefore the slow stage, and β is the parameter describing the energeticinhomogeneity of the electrode surface according to Temkin (0<β<1). The β=1 parameter value corresponds to energetichomogeneity of the electrode surface. An analysis of the literature data resulted in the author’s conclusion about dependence of parameter β on type of Pt(hkl) monocrystals. It indicatesenergetic heterogeneousness of surface platinum atoms. In the publications cited above, the authors also proved a concept according to which the ORR process is realized with participation ofsurface binuclear oxygen (SBNO) nanoclusters on the base of OSS formed on the surface of Pt-electrodes in molecular oxygen atmosphere.In the current work, analysis of energy characteristics of OSS (which serve as building blocks of SBNO nanoclusters) on surface of Pt-electrodes in alkaline medium is performed; these characteristics are compared with ORR process parameters. The analysis resulted in a new structure of SBNO nanoclusters and new multistage scheme of redox cycle of ORR with participation of SBNO nanoclusters.


## 2. Comparison of ORR Characteristics with Parameters of Oxygen-Containing Structures on Surface of Pt-Electrodes

### 2.1. Energy Characteristics of Electrochemical Reactions of Surface of Pt-Electrodes in Nitrogen Atmosphere (Alkaline Media)

In studies [14, 15] by Appleby the “relative ΔGads(E)” parameter was used for energy characterization of adsorbed oxygen-containing –OH and/or –O particles on surface of metal electrodes. According to Appleby’s concept, this parameter is a formal thermodynamic equivalent of the electrode potential. Analysis of dependence of current characteristics of oxygen electrodes on base of Os, Ru, Rh, Pd, Pt, and Au in 85% solution of H3PO4 at 25°С was performed with utilization of “relative ΔGads(E′′)” parameter [15]. Appleby used volts as a measurement unit; the parameter was linked to the potential at which, according to anodic cyclic voltammetry, formation of oxygen-containing particles is started.Appleby’s concept about possibility of utilization of potential of formation of surface oxygen-containing particles as the energy characteristic is used in the current work for analysis of surface electrochemical processes on Pt-electrodes. The parameterΔG∗s,d is used as the energy characteristic. The parameter is formally defined as Gibbs energy of electrochemical process by the classical equation (3)ΔG∗s,d=-nFE,where n is the number of electrochemical process electrons, E is the potential, in relation to the standard hydrogen electrode (SHE), at which the electrochemical process takes place, and F is the Faraday constant. The surface Pt atoms are also defects of the platinum crystal lattice; the energy characteristics of such atoms may differ from energy characteristics of crystal body’s atoms; therefore, to highlight this, the subscripts s and d are used in the description of ΔG∗s,d parameter. The subscripts reflect terms “surface” and “defect” correspondingly.The following equation was discussed in the review [4] as a probable electrochemical reaction on Pt-electrodes in acidic media in the absence of molecular oxygen:(4)PtOH2+2H++2e-⟷Pt+2H2O.The standard potential of this reaction is equal to 0.98 V (according to data from review [4] and handbook [16]). In alkaline solutions, reaction (4) should be rewritten as (5)PtOH2+2e-⟷Pt+2OH-ΔG0298K=-29kJmol-1,with the standard reaction potential equal to 0.15 V [16]. In (5), the standard value of Gibbs energy was calculated according to (3). Taking into account value of Gibbs energy ΔG0(298K)(ОН−) = −157.3 kJ mol−1 [3], the Gibbs energy of formation of PtOH2 hydroxide was calculated on the basis of data in (5). The obtained value of Gibbs energy ΔG0(298K)Pt(OH)2 = −285 kJ mol−1 is in agreement with the reference value of −286 kJ mol−1 [17].By taking into account the fact that surface Pt atoms are defects of crystal lattice [12], (5) may be presented in different format:(6)Pts,d-2e-+2OH-⟷Pts,dOH2,where Pts,d abbreviation denotessurface platinum atom which is, at the same time, adefect of the crystal lattice. Let us note that reaction (6), contrary to reaction (5), is written in anodic format. Therefore, for this reaction, the Gibbs energy is designated with ΔGa∗s,d symbol, where subscript a indicates anodic process. Calculation of the parameter is carried out according to (3) on condition that ΔGa∗s,d=-ΔG∗s,d.Reaction (6), in principle, may occur in two stages. In first stage, oxygen-containing PtIs,d(OH) structure would be formed:(7)Pts,d-e-+OH-⟷PtIs,dOH.In the second stage, PtIIs,dOH2 structure will be formed:(8)PtIs,dOH-e-+OH-⟷PtIIs,dOH2.Symbols “I” and “II” reflect valence state of Pts,d atom as there is a difficulty in interpretation of the value of positive charge of the surface atom. In the authors’ opinion, the two-stage variant of the process finds reflection on anodic and cathodic CVA branches. The results of analysis of literature data on monocrystalline and polycrystalline Pt-electrodes are presented in Table 2.Table 2
Potentials of intervals of cyclic voltammograms and peaks potentials of anodic and cathodic currents at various temperatures on monocrystalline [7, 8] and polycrystalline [3, 10] Pt-electrodes.
Electrode materials Temperature, K Potentials∗, V (vs RHE) Interval Peak I Peak II anodic branch cathodic branch anodic branch cathodic branch Pt(111) 293 0.6–1.1 0.78 0.78 1.05 1.00∗∗ 333 0.78 0.78 0.95 0.90 Pt(110) 293 0.2–1.0 0.30∗∗ 0.45 0.75 0.65 333 0.25 0.50 0.75 0.70 Pt(100) 293 0.2–1.1 0.60∗∗ 0.60 1.00 0.95 333 0.60 0.60 0.98 0.95 Pt smooth 293 0.5–1.2 0.7 Absence of peak 1.1 0.80 T h e   ∗ values are approximate; they are results of author’s processing of graphical data from publications [3, 7, 8, 10]; Poorly∗∗ defined peak; There∗∗∗ are significant currents between peaks I and II on cyclic voltammograms’ anodic branches for Pt(110) and Pt(100) monocrystalline and polycrystalline Pt-electrodes.Table2 data indicates that two peaks of anodic current appear on anodic branches of cyclograms only for Pt(111) monocrystals and polycrystalline Pt-electrodes. Let us note that the second peak of anodic current on monocrystalline [7, 8] and polycrystalline [3, 10] Pt-electrodes takes place within the 1.0–1.1 V (versus RHE) region of stationary ORR potentials. On monocrystals Pt(110) and Pt(100), only the second anodic current peak is clearly seen. The first peak on these monocrystals is poorly defined. Reversibility of the processes for both anodic current peaks on cathodic branches of CVA is most pronounced at elevated temperatures [7, 8]. On Pt(110) and Pt(100) monocrystals, reversibility is observed at all tested temperatures [7, 8]. On cathodic branches of cyclograms for polycrystalline Pt-electrodes reversibility is absent for both peaks of anodic current [3, 10]. On the other hand, one may interpret the potential of cathodic peak at 0.8 V (versus RHE) as a summary of potentials of huge number of various monocrystals Pt (hkl) which are presented on the surface of polycrystalline platinum as a complicated mosaic. Indeed, according to Table 2 data medium sum of potentials of peaks II on cathodic branches CVA for Pt(111), Pt(110), and Pt(100) monocrystals is equal to 0.87 V (versus RHE) at 293 K temperature.During analysis of CVAs, one should take into account the character of location ofPts,d atoms on Pt(hlk) monocrystals surface; differences in CVA characters are, in author’s opinion, consequences of various locations of Pts,d atoms on surface of Pt (hkl) monocrystals. In principle, by taking into account radius of Pt atoms (139 pm) and lattice parameter (392 pm) the character of density of atoms packing may be reflected with NPts,d parameter (quantity of Pts,d atoms on 1 nm2). The most dense packing of Pts,d atoms is the characteristic of Pt(111) monocrystals. For such packing each surface atom is surrounded by 6 other atoms on interatomic distance of 278 pm (see Figure 1).Figure 1
Scheme of atoms’ locations on the surface of Pt(hkl) monocrystals.Monocrystals Pt(110) are characterized by the least dense surface atomsPts,d (NPts,d=9) packing. Two peculiarities of atoms distribution take place in this case. First, each atom has a close contact with only 2 other surface atoms (on interatomic distance of 278 pm). Second, electrolyte components obtain access to subsurface atoms of Pt crystal due to large interatomic distance (392 pm) between “remote neighbors” Pts,d atoms in the surface layer. Monocrystals Pt(100) are characterized by medium density of surface atoms Pts,d (NPts,d=13) packing. For this packing there are following peculiarities of atoms distribution. First, each surface atom has only 4 neighbor Pts,d atoms on interatomic distance of 278 pm. Second, for the medium dense packing electrolyte components also have access into subsurface platinum atoms due to large interatomic distance (392 pm) between “remote neighbors” Pts,d atoms.Due to monolithicity of surface layer of platinum atoms on Pt(111) monocrystal the proceeding of reactions (7) and (8) is expressed on CVA as two well defined anodic peaks within a fairly narrow interval of potentials (see Table 2). One may assume that peak I with anodic CVA branch maximum at 0.78 V (versus RHE) (which could be recalculated as −0.05 V (versus SHE)) corresponds to proceeding of reaction (7). Therefore, peak II with anodic CVA branch maximum at 1.05 V (versus RHE) (recalculated as 0.22 V (versus SHE)) corresponds to proceeding of reaction (8). According to (3) values of ΔGa∗s,d, parameter calculated for −0.05 and 0.22 V (versus SHE) potentials is equal to −5 and 21 kJ mol−1, correspondingly. Let us note that the subscript symbol a in description of ΔGa∗s,d parameter reflects correspondence of reactions (7) and (8) to anodic process. Following the described above method the values of ΔGa∗s,d parameter were calculated for other Pt-electrode types (see Table 3).Table 3
Potentials of CVA anodic peaks andΔGa∗s,d parameter of electrochemical reactions (7) and (8) on Pt-electrodes.
Electrode materials Potential, V (vs SHE) Δ G a ∗  s , d , kJ⋅mol−1 Peak I Peak II Reaction (7) Reaction (8) Pt(111) −0.05 0.22 −5 21 Pt(110) −0.53 −0.08 −51 −8 Pt(100) −0.23 0.17 −22 16 Pt smooth −0.13 0.27 −12 26Analysis of Table3 data leads to the following conclusions.(1) The surface oxygen-containing structurePtIs,dOH in alkaline media and absence of molecular oxygen could be considered as a stable formation on all Pt-electrode types (as for reaction (7) ΔGa∗s,d<0).(2) The surface oxygen-containing structurePtIIs,dOH2 in alkaline media is not stable formations on smooth metal, Pt (111) and Pt(100) monocrystal Pt-electrodes. These structures decompose down to PtIs,dOH as for reaction (8) ΔGa∗s,d>0.ParametersΔGa∗s,d and ΔGk∗s,d of formation of oxygen-containing structures PtIIs,dOH2 and PtIsdOH were calculated from Table 3 data. The parameters were determined for monocrystalline Pt(hkl) and polycrystalline Pt-electrodes (see Table 4). Note that the subscript symbol k in description of ΔGk∗s,d parameter reflects correspondence of reactions (7) and (8) to cathodic process. The calculations were performed for maximums of peaks on anodic and cathodic CVA branches (see Table 2). Only single wide peak is observed on cathodic CVA branch (see Table 2) for smooth platinum electrodes. Such peak could be interpreted as summing result of multiple surface Pt(hkl) monocrystals. Therefore, for smooth platinum the parameter ΔGk∗s,d is calculated as 1/3 of sum of parameter values for Pt(111), Pt(110), and Pt(100) monocrystals.Table 4
ParameterΔG∗s,d for oxygen-containing structures on the surface of Pt-electrodes in nitrogen atmosphere.
Structure Δ G ∗  s , d, kJ⋅mol−1 Pt(111)(NPts,d=17) Pt(100)(NPts,d=13) Pt(110)(NPts,d=9) Pt smooth Δ G a ∗  s , d Δ G k ∗  s , d Δ G a ∗  s , d Δ G k ∗  s , d Δ G a ∗  s , d Δ G k ∗  s , d Δ G a ∗  s , d Δ G k ∗  s , d P t I  s , d O H calculation according to reaction (7) −162 −162 −179 −179 −208 −194 −169 (−178)∗ P t I I  s , d O H 2 Calculation according to reaction (8) −298 −303 −320 −324 −373 −300 −300 (−309)∗ a v e r a g e d   ∗ value of ΔGk∗s,d parameters on Pt(hkl) monocrystals.Analysis of Table4 data leads to the following conclusions.(1) A correlation between values ofΔGa∗s,d and NPts,d parameters is detected. For all surface oxygen-containing structures decrease of density of surface atoms packing correlates with increase of parameter ΔGa∗s,d absolute value. For oxygen-containing structure PtIIs,dOH2 the decrease of parameter NPts,d values in 17, 13, 9 atoms row corresponds to increase of absolute values of parameter ΔGa∗s,d in −298, −320, and −373 kJ mol−1 row. For oxygen-containing structure PtIs,dOH the decrease of parameter NPts,d values in the same atoms row corresponds to increase of absolute values of parameter ΔGa∗s,d in −162, −179, and −208 kJ mol−1 row.(2) ParameterΔGa∗s,d values for oxygen-containing structures on smooth and Pt (111) Pt-electrodes are close to each other (300 and 298 kJ mol−1 for PtIs,dOH and 169 and 162 kJ mol−1 for PtIIs,dOH2, correspondingly). The closeness of parameter ΔGa∗s,d values means that the energy properties of polycrystalline platinum in the anodic process correspond to the most dense packing of surface atoms on Pt(111) monocrystals.(3) Nearly identical values of parametersΔGa∗s,d and ΔGk∗s,d for cases of Pt(111) and Pt(100) monocrystals reflect reversibility of reaction (7) and, correspondingly, the equality of potentials of peaks I on anodic and cathodic CVA branches (see Table 2).(4) The parametersΔGa∗s,d presented in Table 4 shall be considered as data for surface oxygen-containing structures which were obtained in specific experimental conditions. It is caused by a fact that values of ΔGa∗s,d parameters are directly connected with values of anodic peak on CVA. Note that values of ΔGa∗s,d parameter correspond to potentials of anodic peaks on smooth Pt-electrodes at 0.7 and 1.1 V (see Table 2). However, in study [18] during investigation of CVA on smooth Pt-electrodes in KOH solutions with various concentrations (from 0.1 to 6.9 M) a weak appearance of two anodic peaks on CVA was observed at different potentials. First peak the authors connected with platinum oxidation up to PtOH structure. The potential of this peak fluctuated within 0.840 to 0.820 V (versus RHE) range. The second peak the authors associated with formation of Pt(OH)2 structure. The potential of the second peak fluctuated within 0.96 to 1.00 V (versus RHE) interval.The values of parameterΔG∗s,d presented in Table 4 are directly related to potentials of anodic peaks I and II from Table 2. Let us note that the character of dependence of anodic current on potential within the range of potentials between the peaks I and II depends on type of Pt(hkl) monocrystals and surface packing density of platinum atoms (Rs,d parameter) [13]. In a case of the most dense packing of Pts,d atoms corresponding to the Pt(111) monocrystals, a sharp decrease of anodic current (between the peaks I and II) is observed up to the middle of the range of potentials between peaks I and II [7, 8]. It follows with a sharp increase of the anodic current. The observed character of dependence of anodic current on potential on Pt(111) monocrystals provessimultaneous participation of all Pts,d atoms in reaction (7), and later in reaction (8). It indicatesenergetic homogeneity of electrode surface according to Temkin on Pt(111) monocrystals. Correspondingly the parameter β in the Tafel equation is close to 1 [13].In a case of Pt(110), Pt(100) monocrystals, and polycrystalline Pt-electrodes the range of potentials between weak peaks I and II is characterized by practically the same values of the anodic current (without clearly defined minimum of the current) [7, 8, 10]. The observed character of dependence of anodic current on potential on Pt(110) and Pt(100) monocrystals indicates that the atoms with various energetic characteristics participate in reactions (7) and (8). For example, the platinum atoms from the surface and subsurface layers take part in the above reactions (see Figure 1). It indicates an existence ofenergetic inhomogeneity of electrode surface according to Temkin on such monocrystals. Correspondingly, the parameter β in the Tafel equation is significantly smaller than 1 [13].The surface of polycrystalline Pt-electrode is a complex combination of Pt(hkl) monocrystals. Therefore, the energetic properties of surface of all Pt(hkl) monocrystals shall contribute to ORR process. The analysis of literature data indicated that value of parameterβ depends on intensity of ORR process. In the range of low values of anodic current, the parameter β is equal to 1; it corresponds toenergetic homogeneity of electrode surface according to Temkin. In the range of high values of anodic current, the parameter β is sharply decreased down to 0.3–0.5 range; it corresponds toenergetic inhomogeneity of electrode surface according to Temkin. Therefore, one may assume that at low current values the ORR process is primarily realized via participation of surface atoms of Pt(111) monocrystals. Correspondingly at high current values, the surface atoms from Pt(110) and Pt(100) monocrystals get involved in the ORR process.The presented conclusions are alternative to the concepts currently used in the literature for interpretation of electrochemical processes on platinum electrodes in inert atmosphere. For example, in studies [19, 20] for analysis of “electrosorption” processes a formation of surface structures Pt3/OH and Pt3/(OH)2 is proposed on Pt(111) monocrystals and formation of Pt4/OH, Pt2/OH, Pt/OH structures is proposed on Pt(100) monocrystals. The Ptx/OH structures, in opinion of the studies’ authors, are not stoichiometric formations. The structures only reflect ratio of neutral Pt atoms and OH particulates on the surface of platinum electrode. Particles OH are formed, according to the studies’ authors, as a result of proton and electron loss by water molecule at high positive potentials (reaction Pt + H2O↔ Pt/OH + H+ + e-). But there is very low probability that hypothesis of formation of OH radical at potentials 0.9–1.0 V (versus RHE) is correct one. The fact is that the standard potential of reaction OH(г) + e-↔ OH− is equal to 2.02 V [16] (which is equivalent to 2.85 V (versus RHE)). Therefore, interpretation of electrochemical processes in absence of molecular oxygen as “electrosorption” of OH radicals on polycrystalline Pt-electrodes is seen as one which does not correspond to the real processes.In studies [2, 3] oxygen-containing particles, formed as a result of electrochemical processes on Pt-electrodes in absence of molecular oxygen, are interpreted as “chemisorbed oxygen”. Schemes which were proposed in study [2] for a case of Pt-electrodes in alkaline media have a simple format: Pt + OH−↔ PtOH + e−. Unfortunately, in the above studies attention is not accented on nature of oxygen particle “OH” and on energy state of Pt atoms. Therefore, in the above interpretation it is still unclear whether discharge of OH− happens with formation of OH radical or electrochemical oxidation of surface Pt atom takes place. In the current article a small probability of formation of OH radical was already mentioned. The author considered formation of surface oxygen-containing structure PtIs,dOH according to reaction (7) as the most probable pathway explaining electrochemical processes on Pt-electrodes in absence of molecular oxygen.


### 2.2. Energy Characteristics of Electrochemical Reactions of Surface of Pt-Electrodes in Molecular Oxygen Atmosphere (Alkaline Media)

Estimations of energy parameters of reaction,(9)Pt+0.5O2+H2O⟷PtOH2,ΔG0298K=-48kJmol-1,indicate that chemical oxidation of smooth platinum is highly probable in KOH solutions in molecular oxygen atmosphere. For calculation of ΔG0(298K) parameter the values ΔG0(298K)(H2O) = −237.2 kJ mol−1 [3] and ΔG0(298K) (Pt(OH)2) = −285 kJ mol−1 were used (see (5) related calculations). Correspondingly, oxidation of surface of Pt(hkl) monocrystals and polycrystalline Pt is also a highly probable pathway. The following reactions may proceed in the presence of molecular oxygen on surface of Pt(hkl) monocrystals and smooth Pt in KON solutions:(10)Pts,d+0.25O2+0.5H2O⟷PtIs,dOH,(11)PtIs,dOH+0.25O2+0.5H2O⟷PtIIs,dOH2,(12)Pts,d+0.5O2+H2O⟷PtIIs,dOH2.To calculate values ofΔGa∗s,d parameter for reactions (10)–(12) the values of ΔGa∗s,d parameter for corresponding oxygen-containing structures from Table 4 were used. The results of such calculations are presented in Table 5.Table 5
ParameterΔGa∗s,d for chemical reactions (10)–(12) on Pt-electrodes.
Electrode material Δ G a ∗  s , d, kJ⋅mol−1 reaction (10) reaction (11) reaction (12) Pt(111) −44 −17 −61 Pt(110) −90 −46 −136 Pt(100) −60 −23 −83 Pt smooth −51 −12 −63Analysis of Table5 data leads to the following conclusions.(1) Molecular oxygen in KOH solutions is able to oxidize atoms of smooth Pt (for reaction (9) ΔG0(298K) < 0) and defects of crystal lattice Pts,d (for reactions (10), (11), and (12) ΔGa∗s,d<0).(2) ThePtIs,dOH structure may be oxidized by molecular oxygen as for reaction (11) the value of parameter ΔGa∗s,d is less than zero (ΔGa∗s,d<0) on all types of Pt-electrodes.(3) In the presence of molecular oxygenPtIIs,dOH2 structure becomes a stable formation as for reaction (12) ΔGa∗s,d<0 on all types of Pt-electrodes.(4) Energy properties of smooth Pt are the most close to those of Pt(111) monocrystals. For example, for reaction (12) values of parameter ΔGa∗s,d are equal to −63 and −61 kJ mol−1, correspondingly.(5) ParameterΔGa∗s,d for formation of surface oxygen-containing PtIIs,dOH2 structure on smooth Pt in the result of chemical reaction (12) has higher absolute value than ΔG0(298K) value of formation of hydroxide Pt(OH)2 in the result of reaction (9) (−63 and −48 kJ mol−1, correspondingly).


### 2.3. Comparison of ORR Characteristics in Alkaline Media with Parameters of Oxygen-Containing Formations on Pt-Electrodes

Consecutive realization of cathodic variant of reactions (8) and (11) is a core of the concept of ORR process with slowed stage of ConGHR with participation of SBNO nanoclusters [12, 13]. Binuclear nanoclusters model is based on a concept of proceeding of ORR process with participation of two Pt atoms (“bridge model” [21]). Let us note that binuclear model was used in theoretical study [22]. Surface binuclear oxygen structure from two neutral Pt atoms Pt--O2--Pt was a basis of that study. In the study a model based on multinuclear cluster Pt5O2(ads) was also utilized.Reaction (11) factually unites two electrochemical systems: cathodic reaction (2) and anodic reaction (8). Potential of cathodic reaction (2) in KOH solution is equal to 1.23 V (versus RHE). Anodic potential, Ea(8), of reaction (8) corresponds to potentials of anodic peaks II (see Table 2). As a result, the averaged potential, Emix, at which reaction (11)) may proceed is established. Similar methods of calculation of parameter Emix (“mixed potential”) were used in studies [23, 24] for investigation of stationary potentials on Pt-electrodes in 2 N H2SO4. The studies’ author assumed that platinum surface is not inert in relation to molecular oxygen and that reaction Pt-O + 2H+ + 2e−↔ Pt + H2O is realized in acidic solutions. The standard potential of this reaction is equal to 0.90 V [16]. Therefore, a “mixed potential” with some intermediate value in the 0.9 to 1.23 V range should be observed on Pt-electrodes. The stationary potential with values within narrow 1.17–1.16 V (versus RHE) interval was observed in experimental studies [23, 24]; it was explained by the studies’ author as manifestation of the “mixed potential”. Let us note that potential of cathodic reaction (2) remains practically unchanged value in a course of reaction (11) in the oxygen atmosphere. The potential of anodic reaction (8) which factually defines the potential of platinum electrode depends on level of oxidation of platinum electrode surface. In the ideal case when whole surface of platinum electrode is covered by the oxygen-containing PtIIs,dOH2 structures the potential of platinum electrode may reach 1.23 V value. But in real experiments, presence of various impurities in the electrolyte which have an ability to reduce the oxygen-containing PtIIs,dOH2 structures does not allow the electrode potential to reach 1.23 V value [4]. Effect of achievement of 1.23 V potential on Pt-electrode is reported in study [25]. The effect was achieved due to preliminary electrolyte purification via 60-hour anodic electrolysis. But within several hours the 1.23 V potential gradually decreased to 1.1 V value. In experiments with alkaline electrolytes without high purification the currentless potential Emix is reported in the 0.95–1.10 V range [2, 4, 25–27].Let us introduce parameter,Rs,d, to reflect a relation between surface Pt atoms with different valence PtIIs,d/PtIs,d in accordance with reaction (8). Estimation of parameter Rs,d value for platinum electrode surface may be performed with classical Nernst equation Emixs,d = E∗a(8)+0.06lg⁡(Rs,d), where E∗a(8) is the potential of surface oxygen-containing formation on Pt-electrodes at Rs,d≈1. The ratio PtIIs,d/PtIs,d is sharply increased after treatment of Pt-electrode by anodic current (preliminary anodic oxidation) or by strong oxidizer (e.g., by concentrated HNO3). Correspondingly, the parameter R(8)s,d is also increased (R(8)s,d≫1) after such treatment, and parameter Emixs,d could reach values of standard oxygen electrode of 1.23 V and even exceed this value. But with time artificially raised level of oxidation is decreased and gradually the usual value of parameter Emixs,d is set again within 0.9–1.1 V range. The described situation corresponds to experimental facts mentioned in review [4]. At the same time, the most favorable conditions for proceeding of ORR appear at potential Estart. This parameter corresponds to a minimal current on polarization curves in Tafel coordinates (as a rule, it is a value of about 10−4 A·sm−2 [2, 4]). As data on measurement of currentless potential Emixs,d are virtually absent in the literature, therefore to characterize sum of all polarization energy losses on oxygen electrode (shift of potential of oxygen electrode due to presence of impurities in the electrolyte, activation of ORR process, methods of preparation of electrode surface, and other phenomena) a concept of mixed uncontrolled polarization ηmix=1.23-Estart is introduced. Table 6 presents dependence of parameter ηmix on structure of crystal surface (parameter ηmix) and on electrolyte nature. Values of parameter Estart are presented for monocrystals in KOH solution [7, 8] and for polycrystalline (smooth) Pt-electrodes in KOH and H2SO4 solutions [2].Table 6
Potential of ORR start,Estart, and activation polarization, ηmix, for monocrystalline (in KOH solution [7, 8]) and smooth (in KOH and H2SO4 solutions [2]) Pt-electrodes.
Electrode materials PotentialEstart, V (vs RHE) Polarizationηmix, V Pt(111)(NPts,d=17) 1.05 −0.18 Pt(100)(NPts,d=13) 0.95 −0.28 Pt(110)(NPts,d=9) 0.9 −0.33 Pt smooth (KOH) 1.1 −0.13 Pt smooth (H2SO4) 1.05 −0.18Analysis of Table6 data leads to the following conclusions.(1) Correlation between parameterNPts,d and value of parameter ηmix is detected on Pt monocrystal electrodes. The smallest value of parameter ηmix corresponds to the densest packing of surface platinum atoms.(2) On smooth Pt-electrodes value of parameterηmix corresponds to similar value observed on Pt(111) monocrystals with the densest packing of surface platinum atoms.As mentioned above, the ConHCR concept assumes proceeding of ORR with participation of SBNO nanoclusters. The author assumes that in the state of limiting oxidation of oxygen electrode surface (Es,d = 1.23 V) an appearance of nanoclusters SBNO1.23 with two surface PtIIsd atoms is highly probable (see Figure 2). After transition at potential Estart into a state with an appreciable current nanoclusters SBNOstart with PtIIsd и PtIs,d atoms prevailed on surfaces of monocrystalline and smooth polycrystalline Pt-electrodes.Figure 2
Composition of SBNO nanoclusters in state of limiting oxidation of surface of oxygen electrode (Es,d = 1.23 V) and in starting state of ORR reaction ([xPt]—platinum atoms from the electrode body, H2Ox—water molecules from the coordination spheres of PtIsd and PtIIsd atoms).In author’s opinion, the appearance of SBNO1.23 nanocluster on Pt(111) electrodes in alkaline media happens during stage I of 4-electron redox cycle of ORR process (see Figure 3). Experimental confirmation of concept of ORR proceeding with participation of oxygen-containing formations on surface of Pt-electrodes is provided in studies [5, 11]. In study [5] it is determined that in pure 0.1 M HClO4 solution the ORR process on Pt(111) monocrystal electrode proceeds according to reaction (1). An addition of KBr solution (10−4M) sharply changes the direction of ORR (instead of H2O molecule a molecule of hydrogen peroxide H2O2 is formed). A change of reaction paths correlates with change of state of monocrystal surface: introduction of Br− ions result in disappearance from cyclic voltammograms of peaks corresponding to formation of oxygen-containing structures (see Table 1). As one may see, there are CVA peaks reflecting formation of surface oxygen-containing structures in pure HClO4 on surface of Pt(111)-electrode at 0.8–0.9 V interval. At the same time, this range of potentials corresponds to realization of reaction (1) with formation of water molecules. Introduction of some number of Br− ions is accompanied by disappearance of oxygen-containing structures on the Pt-electrode surface. Simultaneously potential of ORR starts to shift to 0.65 V. This value of the potential is close to the 0.695 V value of the standard potential of reduction of oxygen molecule to hydrogen peroxide [3, 16]. In publication [11] the fact that in pure 1 M H2SO4 solution at 0.90–0.95 V (RHE) potentials the ORR process proceeds in accordance with reaction (1) is established. An addition of 0.1 М HCl solution sharply changes the potential of start of ORR. This parameter has a dependence on type of Pt(hkl) monocrystal. For Pt(111), Pt(110), and Pt(100) monocrystals the potential of ORR start is equal to 0.720, 0.690, and 0.620 V, correspondingly. The change of ORR start potential is accompanied by complete disappearance of CVA peaks of formation of oxygen-containing structures in the area of potential 0.70 V (versus RHE).Figure 3
Redox cycle of ORR process in alkaline media on monocrystalline Pt(111) electrodes with participation of SBNO nanoclusters at potentialEstarts,d.Influence of I−, Br−, and Cl− ions in acidic media on state of Pt-electrode surface is described in study [19]. The effect is manifested in blocking of start of the process of formation of oxygen-containing structures. In order of blocking efficiency the ions are placed in the I− > Br− > Cl− row. For example, concentrations at which the effect demonstrates 20% blocking have an order of 10−7, 10−6, and 10−5mol l−1, correspondingly. The study [19] reports that there is no influence of any type of anion on state of Pt-electrode surface in alkaline media.


## 2.1. Energy Characteristics of Electrochemical Reactions of Surface of Pt-Electrodes in Nitrogen Atmosphere (Alkaline Media)

In studies [14, 15] by Appleby the “relative ΔGads(E)” parameter was used for energy characterization of adsorbed oxygen-containing –OH and/or –O particles on surface of metal electrodes. According to Appleby’s concept, this parameter is a formal thermodynamic equivalent of the electrode potential. Analysis of dependence of current characteristics of oxygen electrodes on base of Os, Ru, Rh, Pd, Pt, and Au in 85% solution of H3PO4 at 25°С was performed with utilization of “relative ΔGads(E′′)” parameter [15]. Appleby used volts as a measurement unit; the parameter was linked to the potential at which, according to anodic cyclic voltammetry, formation of oxygen-containing particles is started.Appleby’s concept about possibility of utilization of potential of formation of surface oxygen-containing particles as the energy characteristic is used in the current work for analysis of surface electrochemical processes on Pt-electrodes. The parameterΔG∗s,d is used as the energy characteristic. The parameter is formally defined as Gibbs energy of electrochemical process by the classical equation (3)ΔG∗s,d=-nFE,where n is the number of electrochemical process electrons, E is the potential, in relation to the standard hydrogen electrode (SHE), at which the electrochemical process takes place, and F is the Faraday constant. The surface Pt atoms are also defects of the platinum crystal lattice; the energy characteristics of such atoms may differ from energy characteristics of crystal body’s atoms; therefore, to highlight this, the subscripts s and d are used in the description of ΔG∗s,d parameter. The subscripts reflect terms “surface” and “defect” correspondingly.The following equation was discussed in the review [4] as a probable electrochemical reaction on Pt-electrodes in acidic media in the absence of molecular oxygen:(4)PtOH2+2H++2e-⟷Pt+2H2O.The standard potential of this reaction is equal to 0.98 V (according to data from review [4] and handbook [16]). In alkaline solutions, reaction (4) should be rewritten as (5)PtOH2+2e-⟷Pt+2OH-ΔG0298K=-29kJmol-1,with the standard reaction potential equal to 0.15 V [16]. In (5), the standard value of Gibbs energy was calculated according to (3). Taking into account value of Gibbs energy ΔG0(298K)(ОН−) = −157.3 kJ mol−1 [3], the Gibbs energy of formation of PtOH2 hydroxide was calculated on the basis of data in (5). The obtained value of Gibbs energy ΔG0(298K)Pt(OH)2 = −285 kJ mol−1 is in agreement with the reference value of −286 kJ mol−1 [17].By taking into account the fact that surface Pt atoms are defects of crystal lattice [12], (5) may be presented in different format:(6)Pts,d-2e-+2OH-⟷Pts,dOH2,where Pts,d abbreviation denotessurface platinum atom which is, at the same time, adefect of the crystal lattice. Let us note that reaction (6), contrary to reaction (5), is written in anodic format. Therefore, for this reaction, the Gibbs energy is designated with ΔGa∗s,d symbol, where subscript a indicates anodic process. Calculation of the parameter is carried out according to (3) on condition that ΔGa∗s,d=-ΔG∗s,d.Reaction (6), in principle, may occur in two stages. In first stage, oxygen-containing PtIs,d(OH) structure would be formed:(7)Pts,d-e-+OH-⟷PtIs,dOH.In the second stage, PtIIs,dOH2 structure will be formed:(8)PtIs,dOH-e-+OH-⟷PtIIs,dOH2.Symbols “I” and “II” reflect valence state of Pts,d atom as there is a difficulty in interpretation of the value of positive charge of the surface atom. In the authors’ opinion, the two-stage variant of the process finds reflection on anodic and cathodic CVA branches. The results of analysis of literature data on monocrystalline and polycrystalline Pt-electrodes are presented in Table 2.Table 2
Potentials of intervals of cyclic voltammograms and peaks potentials of anodic and cathodic currents at various temperatures on monocrystalline [7, 8] and polycrystalline [3, 10] Pt-electrodes.
Electrode materials Temperature, K Potentials∗, V (vs RHE) Interval Peak I Peak II anodic branch cathodic branch anodic branch cathodic branch Pt(111) 293 0.6–1.1 0.78 0.78 1.05 1.00∗∗ 333 0.78 0.78 0.95 0.90 Pt(110) 293 0.2–1.0 0.30∗∗ 0.45 0.75 0.65 333 0.25 0.50 0.75 0.70 Pt(100) 293 0.2–1.1 0.60∗∗ 0.60 1.00 0.95 333 0.60 0.60 0.98 0.95 Pt smooth 293 0.5–1.2 0.7 Absence of peak 1.1 0.80 T h e   ∗ values are approximate; they are results of author’s processing of graphical data from publications [3, 7, 8, 10]; Poorly∗∗ defined peak; There∗∗∗ are significant currents between peaks I and II on cyclic voltammograms’ anodic branches for Pt(110) and Pt(100) monocrystalline and polycrystalline Pt-electrodes.Table2 data indicates that two peaks of anodic current appear on anodic branches of cyclograms only for Pt(111) monocrystals and polycrystalline Pt-electrodes. Let us note that the second peak of anodic current on monocrystalline [7, 8] and polycrystalline [3, 10] Pt-electrodes takes place within the 1.0–1.1 V (versus RHE) region of stationary ORR potentials. On monocrystals Pt(110) and Pt(100), only the second anodic current peak is clearly seen. The first peak on these monocrystals is poorly defined. Reversibility of the processes for both anodic current peaks on cathodic branches of CVA is most pronounced at elevated temperatures [7, 8]. On Pt(110) and Pt(100) monocrystals, reversibility is observed at all tested temperatures [7, 8]. On cathodic branches of cyclograms for polycrystalline Pt-electrodes reversibility is absent for both peaks of anodic current [3, 10]. On the other hand, one may interpret the potential of cathodic peak at 0.8 V (versus RHE) as a summary of potentials of huge number of various monocrystals Pt (hkl) which are presented on the surface of polycrystalline platinum as a complicated mosaic. Indeed, according to Table 2 data medium sum of potentials of peaks II on cathodic branches CVA for Pt(111), Pt(110), and Pt(100) monocrystals is equal to 0.87 V (versus RHE) at 293 K temperature.During analysis of CVAs, one should take into account the character of location ofPts,d atoms on Pt(hlk) monocrystals surface; differences in CVA characters are, in author’s opinion, consequences of various locations of Pts,d atoms on surface of Pt (hkl) monocrystals. In principle, by taking into account radius of Pt atoms (139 pm) and lattice parameter (392 pm) the character of density of atoms packing may be reflected with NPts,d parameter (quantity of Pts,d atoms on 1 nm2). The most dense packing of Pts,d atoms is the characteristic of Pt(111) monocrystals. For such packing each surface atom is surrounded by 6 other atoms on interatomic distance of 278 pm (see Figure 1).Figure 1
Scheme of atoms’ locations on the surface of Pt(hkl) monocrystals.Monocrystals Pt(110) are characterized by the least dense surface atomsPts,d (NPts,d=9) packing. Two peculiarities of atoms distribution take place in this case. First, each atom has a close contact with only 2 other surface atoms (on interatomic distance of 278 pm). Second, electrolyte components obtain access to subsurface atoms of Pt crystal due to large interatomic distance (392 pm) between “remote neighbors” Pts,d atoms in the surface layer. Monocrystals Pt(100) are characterized by medium density of surface atoms Pts,d (NPts,d=13) packing. For this packing there are following peculiarities of atoms distribution. First, each surface atom has only 4 neighbor Pts,d atoms on interatomic distance of 278 pm. Second, for the medium dense packing electrolyte components also have access into subsurface platinum atoms due to large interatomic distance (392 pm) between “remote neighbors” Pts,d atoms.Due to monolithicity of surface layer of platinum atoms on Pt(111) monocrystal the proceeding of reactions (7) and (8) is expressed on CVA as two well defined anodic peaks within a fairly narrow interval of potentials (see Table 2). One may assume that peak I with anodic CVA branch maximum at 0.78 V (versus RHE) (which could be recalculated as −0.05 V (versus SHE)) corresponds to proceeding of reaction (7). Therefore, peak II with anodic CVA branch maximum at 1.05 V (versus RHE) (recalculated as 0.22 V (versus SHE)) corresponds to proceeding of reaction (8). According to (3) values of ΔGa∗s,d, parameter calculated for −0.05 and 0.22 V (versus SHE) potentials is equal to −5 and 21 kJ mol−1, correspondingly. Let us note that the subscript symbol a in description of ΔGa∗s,d parameter reflects correspondence of reactions (7) and (8) to anodic process. Following the described above method the values of ΔGa∗s,d parameter were calculated for other Pt-electrode types (see Table 3).Table 3
Potentials of CVA anodic peaks andΔGa∗s,d parameter of electrochemical reactions (7) and (8) on Pt-electrodes.
Electrode materials Potential, V (vs SHE) Δ G a ∗  s , d , kJ⋅mol−1 Peak I Peak II Reaction (7) Reaction (8) Pt(111) −0.05 0.22 −5 21 Pt(110) −0.53 −0.08 −51 −8 Pt(100) −0.23 0.17 −22 16 Pt smooth −0.13 0.27 −12 26Analysis of Table3 data leads to the following conclusions.(1) The surface oxygen-containing structurePtIs,dOH in alkaline media and absence of molecular oxygen could be considered as a stable formation on all Pt-electrode types (as for reaction (7) ΔGa∗s,d<0).(2) The surface oxygen-containing structurePtIIs,dOH2 in alkaline media is not stable formations on smooth metal, Pt (111) and Pt(100) monocrystal Pt-electrodes. These structures decompose down to PtIs,dOH as for reaction (8) ΔGa∗s,d>0.ParametersΔGa∗s,d and ΔGk∗s,d of formation of oxygen-containing structures PtIIs,dOH2 and PtIsdOH were calculated from Table 3 data. The parameters were determined for monocrystalline Pt(hkl) and polycrystalline Pt-electrodes (see Table 4). Note that the subscript symbol k in description of ΔGk∗s,d parameter reflects correspondence of reactions (7) and (8) to cathodic process. The calculations were performed for maximums of peaks on anodic and cathodic CVA branches (see Table 2). Only single wide peak is observed on cathodic CVA branch (see Table 2) for smooth platinum electrodes. Such peak could be interpreted as summing result of multiple surface Pt(hkl) monocrystals. Therefore, for smooth platinum the parameter ΔGk∗s,d is calculated as 1/3 of sum of parameter values for Pt(111), Pt(110), and Pt(100) monocrystals.Table 4
ParameterΔG∗s,d for oxygen-containing structures on the surface of Pt-electrodes in nitrogen atmosphere.
Structure Δ G ∗  s , d, kJ⋅mol−1 Pt(111)(NPts,d=17) Pt(100)(NPts,d=13) Pt(110)(NPts,d=9) Pt smooth Δ G a ∗  s , d Δ G k ∗  s , d Δ G a ∗  s , d Δ G k ∗  s , d Δ G a ∗  s , d Δ G k ∗  s , d Δ G a ∗  s , d Δ G k ∗  s , d P t I  s , d O H calculation according to reaction (7) −162 −162 −179 −179 −208 −194 −169 (−178)∗ P t I I  s , d O H 2 Calculation according to reaction (8) −298 −303 −320 −324 −373 −300 −300 (−309)∗ a v e r a g e d   ∗ value of ΔGk∗s,d parameters on Pt(hkl) monocrystals.Analysis of Table4 data leads to the following conclusions.(1) A correlation between values ofΔGa∗s,d and NPts,d parameters is detected. For all surface oxygen-containing structures decrease of density of surface atoms packing correlates with increase of parameter ΔGa∗s,d absolute value. For oxygen-containing structure PtIIs,dOH2 the decrease of parameter NPts,d values in 17, 13, 9 atoms row corresponds to increase of absolute values of parameter ΔGa∗s,d in −298, −320, and −373 kJ mol−1 row. For oxygen-containing structure PtIs,dOH the decrease of parameter NPts,d values in the same atoms row corresponds to increase of absolute values of parameter ΔGa∗s,d in −162, −179, and −208 kJ mol−1 row.(2) ParameterΔGa∗s,d values for oxygen-containing structures on smooth and Pt (111) Pt-electrodes are close to each other (300 and 298 kJ mol−1 for PtIs,dOH and 169 and 162 kJ mol−1 for PtIIs,dOH2, correspondingly). The closeness of parameter ΔGa∗s,d values means that the energy properties of polycrystalline platinum in the anodic process correspond to the most dense packing of surface atoms on Pt(111) monocrystals.(3) Nearly identical values of parametersΔGa∗s,d and ΔGk∗s,d for cases of Pt(111) and Pt(100) monocrystals reflect reversibility of reaction (7) and, correspondingly, the equality of potentials of peaks I on anodic and cathodic CVA branches (see Table 2).(4) The parametersΔGa∗s,d presented in Table 4 shall be considered as data for surface oxygen-containing structures which were obtained in specific experimental conditions. It is caused by a fact that values of ΔGa∗s,d parameters are directly connected with values of anodic peak on CVA. Note that values of ΔGa∗s,d parameter correspond to potentials of anodic peaks on smooth Pt-electrodes at 0.7 and 1.1 V (see Table 2). However, in study [18] during investigation of CVA on smooth Pt-electrodes in KOH solutions with various concentrations (from 0.1 to 6.9 M) a weak appearance of two anodic peaks on CVA was observed at different potentials. First peak the authors connected with platinum oxidation up to PtOH structure. The potential of this peak fluctuated within 0.840 to 0.820 V (versus RHE) range. The second peak the authors associated with formation of Pt(OH)2 structure. The potential of the second peak fluctuated within 0.96 to 1.00 V (versus RHE) interval.The values of parameterΔG∗s,d presented in Table 4 are directly related to potentials of anodic peaks I and II from Table 2. Let us note that the character of dependence of anodic current on potential within the range of potentials between the peaks I and II depends on type of Pt(hkl) monocrystals and surface packing density of platinum atoms (Rs,d parameter) [13]. In a case of the most dense packing of Pts,d atoms corresponding to the Pt(111) monocrystals, a sharp decrease of anodic current (between the peaks I and II) is observed up to the middle of the range of potentials between peaks I and II [7, 8]. It follows with a sharp increase of the anodic current. The observed character of dependence of anodic current on potential on Pt(111) monocrystals provessimultaneous participation of all Pts,d atoms in reaction (7), and later in reaction (8). It indicatesenergetic homogeneity of electrode surface according to Temkin on Pt(111) monocrystals. Correspondingly the parameter β in the Tafel equation is close to 1 [13].In a case of Pt(110), Pt(100) monocrystals, and polycrystalline Pt-electrodes the range of potentials between weak peaks I and II is characterized by practically the same values of the anodic current (without clearly defined minimum of the current) [7, 8, 10]. The observed character of dependence of anodic current on potential on Pt(110) and Pt(100) monocrystals indicates that the atoms with various energetic characteristics participate in reactions (7) and (8). For example, the platinum atoms from the surface and subsurface layers take part in the above reactions (see Figure 1). It indicates an existence ofenergetic inhomogeneity of electrode surface according to Temkin on such monocrystals. Correspondingly, the parameter β in the Tafel equation is significantly smaller than 1 [13].The surface of polycrystalline Pt-electrode is a complex combination of Pt(hkl) monocrystals. Therefore, the energetic properties of surface of all Pt(hkl) monocrystals shall contribute to ORR process. The analysis of literature data indicated that value of parameterβ depends on intensity of ORR process. In the range of low values of anodic current, the parameter β is equal to 1; it corresponds toenergetic homogeneity of electrode surface according to Temkin. In the range of high values of anodic current, the parameter β is sharply decreased down to 0.3–0.5 range; it corresponds toenergetic inhomogeneity of electrode surface according to Temkin. Therefore, one may assume that at low current values the ORR process is primarily realized via participation of surface atoms of Pt(111) monocrystals. Correspondingly at high current values, the surface atoms from Pt(110) and Pt(100) monocrystals get involved in the ORR process.The presented conclusions are alternative to the concepts currently used in the literature for interpretation of electrochemical processes on platinum electrodes in inert atmosphere. For example, in studies [19, 20] for analysis of “electrosorption” processes a formation of surface structures Pt3/OH and Pt3/(OH)2 is proposed on Pt(111) monocrystals and formation of Pt4/OH, Pt2/OH, Pt/OH structures is proposed on Pt(100) monocrystals. The Ptx/OH structures, in opinion of the studies’ authors, are not stoichiometric formations. The structures only reflect ratio of neutral Pt atoms and OH particulates on the surface of platinum electrode. Particles OH are formed, according to the studies’ authors, as a result of proton and electron loss by water molecule at high positive potentials (reaction Pt + H2O↔ Pt/OH + H+ + e-). But there is very low probability that hypothesis of formation of OH radical at potentials 0.9–1.0 V (versus RHE) is correct one. The fact is that the standard potential of reaction OH(г) + e-↔ OH− is equal to 2.02 V [16] (which is equivalent to 2.85 V (versus RHE)). Therefore, interpretation of electrochemical processes in absence of molecular oxygen as “electrosorption” of OH radicals on polycrystalline Pt-electrodes is seen as one which does not correspond to the real processes.In studies [2, 3] oxygen-containing particles, formed as a result of electrochemical processes on Pt-electrodes in absence of molecular oxygen, are interpreted as “chemisorbed oxygen”. Schemes which were proposed in study [2] for a case of Pt-electrodes in alkaline media have a simple format: Pt + OH−↔ PtOH + e−. Unfortunately, in the above studies attention is not accented on nature of oxygen particle “OH” and on energy state of Pt atoms. Therefore, in the above interpretation it is still unclear whether discharge of OH− happens with formation of OH radical or electrochemical oxidation of surface Pt atom takes place. In the current article a small probability of formation of OH radical was already mentioned. The author considered formation of surface oxygen-containing structure PtIs,dOH according to reaction (7) as the most probable pathway explaining electrochemical processes on Pt-electrodes in absence of molecular oxygen.


## 2.2. Energy Characteristics of Electrochemical Reactions of Surface of Pt-Electrodes in Molecular Oxygen Atmosphere (Alkaline Media)

Estimations of energy parameters of reaction,(9)Pt+0.5O2+H2O⟷PtOH2,ΔG0298K=-48kJmol-1,indicate that chemical oxidation of smooth platinum is highly probable in KOH solutions in molecular oxygen atmosphere. For calculation of ΔG0(298K) parameter the values ΔG0(298K)(H2O) = −237.2 kJ mol−1 [3] and ΔG0(298K) (Pt(OH)2) = −285 kJ mol−1 were used (see (5) related calculations). Correspondingly, oxidation of surface of Pt(hkl) monocrystals and polycrystalline Pt is also a highly probable pathway. The following reactions may proceed in the presence of molecular oxygen on surface of Pt(hkl) monocrystals and smooth Pt in KON solutions:(10)Pts,d+0.25O2+0.5H2O⟷PtIs,dOH,(11)PtIs,dOH+0.25O2+0.5H2O⟷PtIIs,dOH2,(12)Pts,d+0.5O2+H2O⟷PtIIs,dOH2.To calculate values ofΔGa∗s,d parameter for reactions (10)–(12) the values of ΔGa∗s,d parameter for corresponding oxygen-containing structures from Table 4 were used. The results of such calculations are presented in Table 5.Table 5
ParameterΔGa∗s,d for chemical reactions (10)–(12) on Pt-electrodes.
Electrode material Δ G a ∗  s , d, kJ⋅mol−1 reaction (10) reaction (11) reaction (12) Pt(111) −44 −17 −61 Pt(110) −90 −46 −136 Pt(100) −60 −23 −83 Pt smooth −51 −12 −63Analysis of Table5 data leads to the following conclusions.(1) Molecular oxygen in KOH solutions is able to oxidize atoms of smooth Pt (for reaction (9) ΔG0(298K) < 0) and defects of crystal lattice Pts,d (for reactions (10), (11), and (12) ΔGa∗s,d<0).(2) ThePtIs,dOH structure may be oxidized by molecular oxygen as for reaction (11) the value of parameter ΔGa∗s,d is less than zero (ΔGa∗s,d<0) on all types of Pt-electrodes.(3) In the presence of molecular oxygenPtIIs,dOH2 structure becomes a stable formation as for reaction (12) ΔGa∗s,d<0 on all types of Pt-electrodes.(4) Energy properties of smooth Pt are the most close to those of Pt(111) monocrystals. For example, for reaction (12) values of parameter ΔGa∗s,d are equal to −63 and −61 kJ mol−1, correspondingly.(5) ParameterΔGa∗s,d for formation of surface oxygen-containing PtIIs,dOH2 structure on smooth Pt in the result of chemical reaction (12) has higher absolute value than ΔG0(298K) value of formation of hydroxide Pt(OH)2 in the result of reaction (9) (−63 and −48 kJ mol−1, correspondingly).


## 2.3. Comparison of ORR Characteristics in Alkaline Media with Parameters of Oxygen-Containing Formations on Pt-Electrodes

Consecutive realization of cathodic variant of reactions (8) and (11) is a core of the concept of ORR process with slowed stage of ConGHR with participation of SBNO nanoclusters [12, 13]. Binuclear nanoclusters model is based on a concept of proceeding of ORR process with participation of two Pt atoms (“bridge model” [21]). Let us note that binuclear model was used in theoretical study [22]. Surface binuclear oxygen structure from two neutral Pt atoms Pt--O2--Pt was a basis of that study. In the study a model based on multinuclear cluster Pt5O2(ads) was also utilized.Reaction (11) factually unites two electrochemical systems: cathodic reaction (2) and anodic reaction (8). Potential of cathodic reaction (2) in KOH solution is equal to 1.23 V (versus RHE). Anodic potential, Ea(8), of reaction (8) corresponds to potentials of anodic peaks II (see Table 2). As a result, the averaged potential, Emix, at which reaction (11)) may proceed is established. Similar methods of calculation of parameter Emix (“mixed potential”) were used in studies [23, 24] for investigation of stationary potentials on Pt-electrodes in 2 N H2SO4. The studies’ author assumed that platinum surface is not inert in relation to molecular oxygen and that reaction Pt-O + 2H+ + 2e−↔ Pt + H2O is realized in acidic solutions. The standard potential of this reaction is equal to 0.90 V [16]. Therefore, a “mixed potential” with some intermediate value in the 0.9 to 1.23 V range should be observed on Pt-electrodes. The stationary potential with values within narrow 1.17–1.16 V (versus RHE) interval was observed in experimental studies [23, 24]; it was explained by the studies’ author as manifestation of the “mixed potential”. Let us note that potential of cathodic reaction (2) remains practically unchanged value in a course of reaction (11) in the oxygen atmosphere. The potential of anodic reaction (8) which factually defines the potential of platinum electrode depends on level of oxidation of platinum electrode surface. In the ideal case when whole surface of platinum electrode is covered by the oxygen-containing PtIIs,dOH2 structures the potential of platinum electrode may reach 1.23 V value. But in real experiments, presence of various impurities in the electrolyte which have an ability to reduce the oxygen-containing PtIIs,dOH2 structures does not allow the electrode potential to reach 1.23 V value [4]. Effect of achievement of 1.23 V potential on Pt-electrode is reported in study [25]. The effect was achieved due to preliminary electrolyte purification via 60-hour anodic electrolysis. But within several hours the 1.23 V potential gradually decreased to 1.1 V value. In experiments with alkaline electrolytes without high purification the currentless potential Emix is reported in the 0.95–1.10 V range [2, 4, 25–27].Let us introduce parameter,Rs,d, to reflect a relation between surface Pt atoms with different valence PtIIs,d/PtIs,d in accordance with reaction (8). Estimation of parameter Rs,d value for platinum electrode surface may be performed with classical Nernst equation Emixs,d = E∗a(8)+0.06lg⁡(Rs,d), where E∗a(8) is the potential of surface oxygen-containing formation on Pt-electrodes at Rs,d≈1. The ratio PtIIs,d/PtIs,d is sharply increased after treatment of Pt-electrode by anodic current (preliminary anodic oxidation) or by strong oxidizer (e.g., by concentrated HNO3). Correspondingly, the parameter R(8)s,d is also increased (R(8)s,d≫1) after such treatment, and parameter Emixs,d could reach values of standard oxygen electrode of 1.23 V and even exceed this value. But with time artificially raised level of oxidation is decreased and gradually the usual value of parameter Emixs,d is set again within 0.9–1.1 V range. The described situation corresponds to experimental facts mentioned in review [4]. At the same time, the most favorable conditions for proceeding of ORR appear at potential Estart. This parameter corresponds to a minimal current on polarization curves in Tafel coordinates (as a rule, it is a value of about 10−4 A·sm−2 [2, 4]). As data on measurement of currentless potential Emixs,d are virtually absent in the literature, therefore to characterize sum of all polarization energy losses on oxygen electrode (shift of potential of oxygen electrode due to presence of impurities in the electrolyte, activation of ORR process, methods of preparation of electrode surface, and other phenomena) a concept of mixed uncontrolled polarization ηmix=1.23-Estart is introduced. Table 6 presents dependence of parameter ηmix on structure of crystal surface (parameter ηmix) and on electrolyte nature. Values of parameter Estart are presented for monocrystals in KOH solution [7, 8] and for polycrystalline (smooth) Pt-electrodes in KOH and H2SO4 solutions [2].Table 6
Potential of ORR start,Estart, and activation polarization, ηmix, for monocrystalline (in KOH solution [7, 8]) and smooth (in KOH and H2SO4 solutions [2]) Pt-electrodes.
Electrode materials PotentialEstart, V (vs RHE) Polarizationηmix, V Pt(111)(NPts,d=17) 1.05 −0.18 Pt(100)(NPts,d=13) 0.95 −0.28 Pt(110)(NPts,d=9) 0.9 −0.33 Pt smooth (KOH) 1.1 −0.13 Pt smooth (H2SO4) 1.05 −0.18Analysis of Table6 data leads to the following conclusions.(1) Correlation between parameterNPts,d and value of parameter ηmix is detected on Pt monocrystal electrodes. The smallest value of parameter ηmix corresponds to the densest packing of surface platinum atoms.(2) On smooth Pt-electrodes value of parameterηmix corresponds to similar value observed on Pt(111) monocrystals with the densest packing of surface platinum atoms.As mentioned above, the ConHCR concept assumes proceeding of ORR with participation of SBNO nanoclusters. The author assumes that in the state of limiting oxidation of oxygen electrode surface (Es,d = 1.23 V) an appearance of nanoclusters SBNO1.23 with two surface PtIIsd atoms is highly probable (see Figure 2). After transition at potential Estart into a state with an appreciable current nanoclusters SBNOstart with PtIIsd и PtIs,d atoms prevailed on surfaces of monocrystalline and smooth polycrystalline Pt-electrodes.Figure 2
Composition of SBNO nanoclusters in state of limiting oxidation of surface of oxygen electrode (Es,d = 1.23 V) and in starting state of ORR reaction ([xPt]—platinum atoms from the electrode body, H2Ox—water molecules from the coordination spheres of PtIsd and PtIIsd atoms).In author’s opinion, the appearance of SBNO1.23 nanocluster on Pt(111) electrodes in alkaline media happens during stage I of 4-electron redox cycle of ORR process (see Figure 3). Experimental confirmation of concept of ORR proceeding with participation of oxygen-containing formations on surface of Pt-electrodes is provided in studies [5, 11]. In study [5] it is determined that in pure 0.1 M HClO4 solution the ORR process on Pt(111) monocrystal electrode proceeds according to reaction (1). An addition of KBr solution (10−4M) sharply changes the direction of ORR (instead of H2O molecule a molecule of hydrogen peroxide H2O2 is formed). A change of reaction paths correlates with change of state of monocrystal surface: introduction of Br− ions result in disappearance from cyclic voltammograms of peaks corresponding to formation of oxygen-containing structures (see Table 1). As one may see, there are CVA peaks reflecting formation of surface oxygen-containing structures in pure HClO4 on surface of Pt(111)-electrode at 0.8–0.9 V interval. At the same time, this range of potentials corresponds to realization of reaction (1) with formation of water molecules. Introduction of some number of Br− ions is accompanied by disappearance of oxygen-containing structures on the Pt-electrode surface. Simultaneously potential of ORR starts to shift to 0.65 V. This value of the potential is close to the 0.695 V value of the standard potential of reduction of oxygen molecule to hydrogen peroxide [3, 16]. In publication [11] the fact that in pure 1 M H2SO4 solution at 0.90–0.95 V (RHE) potentials the ORR process proceeds in accordance with reaction (1) is established. An addition of 0.1 М HCl solution sharply changes the potential of start of ORR. This parameter has a dependence on type of Pt(hkl) monocrystal. For Pt(111), Pt(110), and Pt(100) monocrystals the potential of ORR start is equal to 0.720, 0.690, and 0.620 V, correspondingly. The change of ORR start potential is accompanied by complete disappearance of CVA peaks of formation of oxygen-containing structures in the area of potential 0.70 V (versus RHE).Figure 3
Redox cycle of ORR process in alkaline media on monocrystalline Pt(111) electrodes with participation of SBNO nanoclusters at potentialEstarts,d.Influence of I−, Br−, and Cl− ions in acidic media on state of Pt-electrode surface is described in study [19]. The effect is manifested in blocking of start of the process of formation of oxygen-containing structures. In order of blocking efficiency the ions are placed in the I− > Br− > Cl− row. For example, concentrations at which the effect demonstrates 20% blocking have an order of 10−7, 10−6, and 10−5mol l−1, correspondingly. The study [19] reports that there is no influence of any type of anion on state of Pt-electrode surface in alkaline media.


## 3. Discussion of ORR Redox Cycle on Pt-Electrodes

The stationary potential of platinum electrodeEstationary in acidic media has a linear dependence on logarithm of partial oxygen pressure with 60 mV dec−1 slope value (see review [4, 28–31]). This experimental fact could be reflected with the following equation: (13)Estationary=Ep=1+2.3RTnF-1log⁡p,where Estationary is the oxygen electrode potential in the absence of current (stationary state), E(p=1) is the stationary (currentless) electrode potential at partial oxygen pressure p=1 atm, and n is the quantity of electrons in electrochemical reaction. Let us note that value of 2.3RTnF-1 parameter is equal to 60 mV for n=1 condition. One may conclude that the electrochemical reaction proceeds with participation of a single electron. It means that stationary (currentless) electrode potential is determined by a single-electron electrochemical reaction. As already mentioned in the author’s study [32], the formation of surface O2- structure with participation of single PtIIs,d atom in the SBNO nanocluster may be such single-electron electrochemical reaction. But probability of appearance of individual O2- radical on surface of platinum electrode during proceeding of ORR is very low. According to review [3] data the standard potential of O2 + e− = O2- reaction in water is equal to −0.284 V. The reaction O2 + e− + H+ = OOH with −0.053 (RHE) potential in acidic media has the higher probability of realization. Let us note that particle (OO)H may be formally considered as hydrogen superoxide. According to the molecular orbital theory an oxygen molecule has two unpaired electrons. After bonding of a single electron to an oxygen molecule in the formed anion radical O2- there is still one unpaired electron. Therefore, the mentioned above reaction could be formally written as two consecutive reactions: H+ + e− = H∗иO2∗∗ + H∗ = OO∗:H, where symbols “∗” and “:” indicate an unpaired electron and a covalent bond with shared pair of electrons, correspondingly.By taking into account high negative value of the standard potential one may note that for standard ORR potentials within the 0.9–1.1 V (versus RHE) range the concentration of hydrogen superoxideOO∗:H on surface of platinum electrode is a parameter with extremely small value. A higher surface content of radical structure (OO)∗ could be achieved due to a contributing factor which, as noted by the author in study [32], may be a formation of nanocluster state of hydroxide/superoxide platinum with a polar covalent bond [(OO)∗:PtIIs,d(OH)].In the ORR redox cycle in alkaline media on monocrystal Pt(111) electrodes (see Figure3) this process is presented by two stages: stage II and stage III. Both stages could be combined into single reversible nanocluster reaction(14)PtIIs,dOH2+O2∗∗+e-⟷OO∗:PtIIs,dOH+OH-.The Pt(111) electrodes were chosen as an example by taking into account the following experimental facts: first, reversibility of anodic and cathodic peaks on CVA (see Table 2.); second, absence of current on the ring electrode in the rotating ring-disk electrode (RRDE) method [7, 8].Reaction (14) corresponds to quasi-equilibrium state of oxygen electrode which, according to the experimental data, is set within 0.95–1.0 V (versus RHE) interval both in alkaline [9, 25, 26] and in acidic [33] electrolytes. By taking into account that ratio of surface states PtIIs,dOH2/OO∗:PtIIs,dOH = 1, the stationary potential of quasi-equilibrium oxygen electrode could be defined by the Nernst equation (13). Let us note that at stationary potentials within 0.90–1.0 V (versus RHE) interval reaction (14) is, practically, in equilibrium state, as the ΔG∗s,d parameter calculated according to (3) has values within −7 to −16 kJ mol−1 range.Let us note that during stage III only weakening of oxygen molecule’s bonds happens in a course ofreversible nanocluster chemical reaction(15)PtIs,dOH+O2∗∗⟷OO∗:PtIIs,dOH.Break-up of first bond in an oxygen molecule happens on stage V during formation of platinum hydroxide peroxideOHPtII:O–O:PtIIOH in the result ofirreversible nanocluster chemical reaction(16)
O
H
P
t
I
I
:
O
O
∗
----
P
t
I
O
H
⟶
O
H
P
t
I
I
:
O
–
O
:
P
t
I
I
O
H
.In principle, ORR process may stop on stage V in the result of destruction of surface structures of SBNO nanoclusters(17)OHPtIIs,d:O–O:PtIIs,dOH+H2O+OH-⟶2PtIIs,dOH2+HO2-.Formation ofHO2- ions in accordance with (16) may be detected with RRDE method. It was experimentally demonstrated (for example, [34–37]) that quantity of HO2- ions detected on the ring depends on surface conditions of polycrystalline Pt-electrode. Preliminary anodic oxidation or cathodic reduction is accompanied by a change of ring/disk current ratio. For example, investigation of ORR in 0.1 M NaOH [34] indicated that change of anodic oxidation potential within 1.0 to 1.5 V (versus RHE) is accompanied by increase of ring/disk current ratio from 10 to 70%. In study [35] it was reported that on Pt-electrodes oxidized at 1.2 V (versus RHE) potential in KOH solutions with concentrations within a range from 0.1 to 6 M the ring/disk current ratio is unchanged parameter with about 7% value. ORR process on Pt-electrode in 0.1 M KOH for cathodic polarization of 1.1 to −0.2 V (versus RHE) is accompanied by ring/disk current ratio within 20–25% interval [36]. On Pt-electrode, which was treated with preliminary cathodic reduction, the ORR process in 0.1 M KOH solution was accompanied by ring/disk current ratios within 3–5% range [37]. Let us note that in experiments with utilization of RRDE method onmonocrystalline Pt-electrodes in 0.1 M KOH solution the formation of HO2- ions on the ring electrode wasnot detected [7, 8].For explanation of appearance of current on the ring during RRDE method a hypothesis is proposed that ORR processes may proceed (for example, in alkaline media) following two parallel pathways: directly to formation of OH− ions (see equation/reaction (2)) and through formation of various intermediate particles. A large number of various variants of formation of the intermediate particles are discussed in the literature (for example, in theoretical study [38] 10 different models/variants were investigated). Nevertheless, an explanation of reasons for parallel realization of two pathways of ORR process on surface ofpolycrystalline Pt-electrode and absence of the second pathway onmonocrystalline Pt-electrodes is still missing in the literature. The author thinks that a concept of proceeding of ORR process with the very same single mechanism on all Pt-electrodes may serve as an alternative hypothesis. As experiments with utilization of RRDE method had demonstrated, on polycrystalline Pt-electrodes there are some conditions for stoppage of ORR process on stage V (see Figure 3). In this case the fraction of HO2- ions formed according to reaction (16) depends on level of perfection of structure of SBNO nanoclusters. Obviously, the perfection of structure of SBNO nanoclusters depends on the method of preparation of surface of polycrystalline Pt-electrodes for the experiment. In other words, multistage ORR process proceeds following the very same single mechanism with formation of intermediate (−O-O−) peroxide group on monocrystalline as well as on polycrystalline Pt-electrodes. The RRDE method only records an existence of stage with breakage of first bond in an oxygen molecule during some independent process. But it means that the mechanism of ORR proceeding directly following 4-electron reaction is absent. The ORR proceeds without the 4-electron reaction.Break-up of the second bond in an oxygen molecule is realized on stage VII after two electrochemical reactions on stages VI and VII. The bond breaking happens due to irreversible nanocluster chemical reaction(18)PtIs,dO–O:PtIs,d+2H2O⟶2PtIIs,dOH2.The redox cycle scheme in Figure3 reflects ORR with slowed stage of ConHCR. Heterogeneous chemical reaction of oxidation by the molecular oxygen of electrochemically reduced surface Pts,d atoms has several stages. The author believes that reaction (14) is a limiting factor for entire ConHCR. In reaction (14)nanocluster surface transitional state (NcSTS) with participation of Pts,d atoms and an oxygen molecule is formedfor the first time. Formed NcSTS creates conditions for transfer of first electron from Pts,d atoms into an oxygen molecule; it results in formation of [(OO)∗:PtIIs,d(OH)] structure. Formally this process may be considered as slowed transfer of first electron. Theoretical aspects of slowed transfer of first electron concept were multiple times discussed in the literature (e.g., [21, 38–43]). The basis of slowed transfer of first electron concept is a consideration that electron is transferred to an oxygen molecule fromneutral surface Pt atom.Quasi-equilibrium state of oxygen Pt-electrode is characterized by a fact that effect of unchanged potentials is observed in alkaline media during change of current from 10−7 to 10−6 A sm−2 [9, 25, 44]. The provided above currents may be considered as exchange current of reaction (14). An analogous experimental effect is also observed in acidic media [33, 44]. But in this case reaction (14) shall be transformed by accounting for a change of composition and structure of SBNO nanoclusters in acidic media [45]. Peculiarity of the cited above experiments is in utilization of specific methods of measurements, as described in study [9]. Each experiment was started with several alternations of anodic and cathodic polarization at potentials of 2.0 and 0.05 V (versus RHE), correspondingly. After final cathodic polarization the cycle of measurements of ORR parameters was performed (realization of “oxide-free” state [28, 29]). By accounting for thermodynamic probability of proceeding of reactions (10) and (11) the author concludes that the more correct definition of the achieved state should be “oxide fresh” state.Let us note that exchange currents on Pt-electrode, according to studies [26, 33], depend on temperature. This experimental fact and the change of activation energy of ORR at 0.8 V potential [26, 33] should become a subject of independent research efforts.Let us also note that the concept of proceeding of ORR with slowed stage of ConHCR allows us an understanding of the experimental fact of dependence of angle of polarization curves in alkaline media in Tafel coordinates (coefficientb) on type of Pt-electrode, current characteristics, and sizing of particles of disperse platinum. At low values of the current the coefficient b is equal to 60 mV per dec on all types of Pt-electrodes (smooth platinum [26, 27, 35], disperse platinum on carbon substrate [46]). At high current values the various values of coefficient b were reported: 120 mV per dec [26, 27, 46] and 200–300 mV per dec range [35]. On electrodes with platinum nanoparticles on disperse carbon [47] we detected dependence of coefficient b from size of platinum nanoparticles. An increase of platinum nanoparticles size from 3 to 24 nm resulted in corresponding decrease of the coefficient b from 80 to 65 mV per dec.Dependence of currentless (stationary) potential of oxygen electrode on oxygen pressure (see (13)) was observed in solutions of various electrolytes: KOH [31], H2SO4 [30, 31, 48], and HClO4 [28, 29]. This experimental fact indicates a single-electron character of reaction which defines the nature of currentless potential of platinum oxygen electrode. In alkaline media, it may be a reaction of formation of platinum superoxide [49]. A process of occurrence of transitional state based on platinum superoxide would be the slowed stage of reaction (14), as well as of the whole ORR on Pt-electrodes in any alkaline solution. A validity of this assumption is confirmed by identical slopes (about 60 mV/dec) of polarization curves in Tafel coordinates for various alkaline solutions (for example, KOH [31], NaOH [9], K2CO3 [18], K2B4O7 [9], and KF [9]). In terms of the concept of electrochemical reaction with slowed stage of ConHCR, it meansenergetic homogeneity of electrode surface according to Temkin at low current values.


## 4. Conclusion

Four specialized parametersΔG∗s,d, NPts,d, ηmix, and Rs,d (Gibbs energy of a process with participation of surface platinum atoms, Pts,d; packing density of Pts,d atoms; uncontrolled activation polarization; level of surface oxidation as a ratio PtIIs,d/PtIs,d atoms, correspondingly) were used for characterization of surfaces of monocrystalline and polycrystalline Pt-electrodes.ParameterΔG∗s,d is the thermodynamic characteristic of proceeding of electrochemical and chemical reactions with participation of surface Pts,d atoms. Parameter ΔG∗s,d was calculated from literature experimental data on cyclic voltammograms on Pt(hkl) monocrystals and polycrystalline Pt-electrodes. The parameter was determined for surface oxygen-containing structures (which serve as building blocks for formation of SBNO nanoclusters and therefore define the structure of SBNO nanoclusters) in nitrogen atmosphere, as well as in molecular oxygen atmosphere.ParameterNPts,d (quantity of Pts,d atoms per 1 nm2 of Pt-electrode surface) characterizes packing density of Pt atoms on surface of Pt(hkl) monocrystals. The densest packing of Pts,d (NPts,d = 17) atoms is determined for Pt(111) monocrystal. Monocrystals Pt(110) and Pt(100) are characterized by less dense packing of surface platinum atoms (NPts,d = 9 and 13, correspondingly). For monocrystalline Pt-electrodes an increase of NPts,d parameter correlates with decrease of ΔG∗s,d parameter. The value of ΔG∗s,d parameter for polycrystalline Pt-electrodes is close to value of ΔG∗s,d parameter for Pt(111) monocrystals with the most dense packing of surface Pt atoms.Parameterηmix=1.23-Estart characterizes all types of polarization effects (e.g., shift of oxygen electrode potential due to presence of impurities in electrolyte, nature of electrolyte, activation of ORR process, and methods of preparation of electrode surface). The correlation between NPts,d and ηmix parameters was detected. The smallest value of parameter ηmix corresponds to the densest packing of surface platinum atoms of Pt(111) monocrystal. On smooth Pt-electrodes value of parameter ηmix corresponds to value observed on Pt monocrystals with the densest packing of surface platinum atoms.ParameterRs,d characterizes the ratio of PtIIs,d/PtIs,d atoms on surface of Pt-electrodes and as such reflects level of oxidation of platinum surface. In the stationary state PtIIs,d atoms prevail over PtIs,d atoms on surface of Pt-electrodes (Rs,d≫1). At potential of start of ORR, the quantity of PtIs,d atoms increases and value of Rs,d parameter sharply changes (Rs,d≈1). Such situation was interpreted as activation of SBNO nanoclusters and appearance of conditions for proceeding of ORR.Analysis of role of oxygen-containing nanoclusters in proceeding of ORR on Pt-electrodes was conducted on the basis of concept of electrochemical process with slowed stage ofconsecutive heterogeneous chemical reaction. Under this concept the main factor determining the ORR characteristics isenergetic inhomogeneity of electrode surface according to Temkin. New concept, according to which EIES is determined by the Gibbs energy of formation of OSS (ΔG∗s,d parameter) with participation of surface platinum atoms, Pts,d, was formulated. Analysis of determined values of ΔG∗s,d parameter resulted in the following conclusions. First, the OSS based on PtIs,d(OH) and PtIIs,dOH2 hydroxides are formed as a result of chemical reaction of oxidation by the molecular oxygen of Pts,d atoms in alkaline medium. Second, in a currentless state the OSS based on PtIIs,dOH2 hydroxide predominate on the surface of Pt-electrodes; correspondingly SBNO nanoclusters based on PtIIs,d also predominate on the surface of Pt-electrodes. Third, at ORR potentials the EIES of polycrystalline Pt-electrodes is a result of combination of characteristics of multiple different Pt(hkl) monocrystals.A correlation between EIES according to Temkin and packing density ofPts,d atoms was determined. Pt(111) monocrystals have the most dense packing of Pts,d atoms. Therefore, such crystals are characterized by the energetichomogeneity of electrode surface according to Temkin. The high level of energeticinhomogeneity of electrode surface of Pt(110) and Pt(100) monocrystals is caused by low packing density of Pts,d atoms and resulting direct influence of Pt atoms from a subsurface layer on energetic characteristics of the electrode surface. In turn, the surface of polycrystalline platinum electrodes is characterized by complex mosaic of Pt(hkl) monocrystals and corresponding complex EIES character.The redox cycle of multistage ORR in alkaline media with participation of SBNO nanoclusters and slowed stage of ConHCR was proposed. The concept according to which the stage of formation of primary nanocluster transitional state determines rate of the whole ORR process was substantiated. Formation of platinum superoxide also happens during this stage.



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*Source: 7164578-2018-06-04.xml*