Mendeleev Commun., 2015, 25, 155–156
which differs from the value obtained earlier11 for the hydro-
9
6
3
0
genation of surface hydroxyl groups, 4.25×10–5 s–1 Pa–1, only
by a factor of 1.14. This reliably confirms the accuracy of the
obtained result.
In the mechanistic scheme (1)–(3), step (3) is really a macro-
scopic one, which can be presented as the sum of two elementary
steps, (4) and
Hads + OHads = H2O.
(5)
0
1000
2000
3000
Each elementary act of step (4) is immediately accompanied
by the interaction of the adsorbed hydrogen atom with the second
hydroxyl group, which results in the formation of a second water
molecule by reaction (5). Thus, step (4) is the key step of
hydrogen oxidation on silver, and the surface hydroxyl group is
a key intermediate directly involved in the formation of water.
A hydrogen molecule and a surface hydroxyl group interact with
each other to produce directly a water molecule without any
intermediate species. Thus, it has been shown for the first time
that the hydrogenation of surface hydroxyl groups during the
oxidation of hydrogen on silver follows a first-order kinetic
law with respect to hydroxyl groups. Chemical equation (4) was
earlier unknown in catalysis. Some processes resembling those
examined in this work were proposed when a model of hydrogen
interaction with oxygen adsorbed on silver was analyzed using
the density functional theory.12,13 The results obtained in this study
are novel and essential; in particular, a mechanistic similarity
between the catalytic oxidation of hydrogen on silver and the
branched chain reaction of hydrogen combustion including the
similar step:14
t/s
Figure 2 Interaction of hydrogen with the stationary adsorbed layer pro-
duced by the transformation of three successive portions of the stoichiometric
mixture (2H2 + O2). Initial hydrogen pressure, 15.7 Pa; temperature, 298 K.
The following assumptions can be made:
(1) The initial rate of the interaction of hydrogen with the
stationary adsorbed layer equals one-half of the rate of the catalytic
oxidation of hydrogen because equal amounts of hydrogen are
consumed in two steps: the formation of hydroxyl groups and
the hydrogenation of surface hydroxyl groups.
(2) The hydrogenation of surface hydroxyl groups follows
the first-order law with respect to surface hydroxyl groups, and
it can be expressed as
H2 + OHads = H2O + Hads
.
(4)
To verify these assumptions, the interaction of hydrogen with
the stationary adsorbed layer, which was produced during the
transformation of the stoichiometric mixture, was investigated
(Figure 2).
The initial rate of hydrogen interaction with the stationary
adsorbed layer is W = 6.00×10–10 mol m–2 s–1, and the steady-
state rate of hydrogen oxidation in the reaction of stoichiometric
mixture oxidation is 1.18×10–9 mol m–2 s–1. It means that the
initial rate of hydrogen interaction with the stationary adsorbed
layer is two times lower than the rate of the steady-state catalytic
oxidation of hydrogen under identical reaction conditions.
Figure 3 shows that the reaction obeys a first-order equation
with respect to surface hydroxyl groups at a constant hydrogen
pressure: ln[1/(1 – x)] = kt. Here, k is the rate constant (s–1),
and x is the conversion of surface hydroxide. These data were
acquired at relatively small changes in the hydrogen partial pres-
sure (average value of ~15.7 Pa). Nevertheless, these changes
provided the accurate determination of the conversion of the
adsorbed layer during its reaction with hydrogen.
•OH + H2 = H2O + •H,
(6)
where a hydroxyl group is the key species directly involved in
the formation of water, is of interest.
Thus, the rate-determining step of the oxidation of hydrogen
on silver is the interaction of a hydrogen molecule with a surface
hydroxyl group giving a water molecule and an adsorbed hydrogen
atom, which is described by equation (4). The adsorbed hydro-
gen atom rapidly interacts with the second surface hydroxyl group
according to equation (5).
This study was supported by the Ministry of Education and
Science of the Russian Federation (project no. 2014/139/2211).
References
1 D. L. Chapman and W. K. Hall, Royal Soc. Proc., 1929, 124, 478.
2 A. F. Benton and J. C. Elgin, J. Am. Chem. Soc., 1929, 51, 7.
3 S. Ya. Pshezhetskii and M. L. Vlodavets, Zh. Fiz. Khim., 1950, 24, 353
(in Russian).
4 A. V. Khasin and G. K. Boreskov, Kinet. Katal., 1969, 10, 613 (in Russian).
5 V. Sh. Gruver, A. V. Khasin and G. K. Boreskov, Kinet. Katal., 1971, 12,
156 (in Russian).
6 E. V. Dokuchits, A. V. Khasin and A. A. Khassin, Russ. Chem. Bull., Int.
Ed., 2012, 61, 2206 (Izv. Akad. Nauk, Ser. Khim., 2012, 2225).
7 A. Hillary and M. Stoukides, J. Catal., 1988, 113, 295.
8 R. J. Mikovsky, M. Boudart and H. S. Taylor, J. Am. Chem. Soc., 1954,
76, 3814.
The results support the hypothesis that the interaction of
hydrogen with the stationary adsorbed layer obeys a first-order
equation with respect to surface hydroxyl groups; thus, step (3)
is macroscopic and the interaction of hydrogen with the stationary
adsorbed layer is an elementary step of the catalytic reaction,
which can be expressed as reaction (4). The rate constant of this
step is k = 7.60×10–4 s–1 at a hydrogen pressure of 15.7 Pa. The
results were reproduced in the repeated series of experiments.
The apparent activation energy of the reaction at 273–473 K was
36.8 kJ mol–1. Then, the rate constant at 298 K is 4.83×10–5 s–1 Pa–1,
9 D. H. Parker, M. E. Jones and B. E. Koel, Surf. Sci., 1990, 233, 65.
10 J. Hohmeyer, E. V. Kondratenko, M. Bron, J. Kröhnert, F. C. Jentoft,
R. Schlögl and P. Claus, J. Catal., 2010, 269, 5.
0.8
0.4
0.0
11 E. V. Dokuchits, A. V. Khasin and A. A. Khassin, React. Kinet. Mech.
Catal., 2011, 103, 261.
12 A. B. Mohammad, K. H. Lim, I. V. Yudanov, K. M. Neyman and N. A.
Rösch, Phys. Chem. Chem. Phys., 2007, 9, 1247.
13 A. B. Mohammad, I. V. Yudanov, K. H. Lim, K. M. Neyman and N. A.
Rösch, J. Phys. Chem. C, 2008, 112, 1628.
0
300
600
900
1200 1500
14 V. N. Kondratiev and E. E. Nikitin, Kinetika i mekhanizm gazofaznykh
reaktsii (Kinetics and Mechanism of the Gas-phase Reactions), Nauka,
Moscow, 1974 (in Russian).
t/s
Figure 3 Experimental data on the interaction of hydrogen with the sta-
tionary adsorbed layer plotted in the coordinates of equation ln[1/(1 – x)] = kt.
Received: 29th July 2014; Com. 14/4434
– 156 –