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J. González-Cobos et al. / Journal of Catalysis 317 (2014) 293–302
effect also sustains the stability of the Au nanoparticles supported on
the YSZ under EPOC conditions. Hence, it is clear that the use of the
YSZ support allowed to disperse the metal nanoparticles, thus avoid-
ing the metal sintering effect, very typical in this kind of catalytic
system.
The increase in the accumulated potassium supply was found to
enhance the overall methanol conversion (not shown) and increase
the reaction rate of hydrogen (Fig. 5a), carbon dioxide, and methyl
formate (Fig. 5b). Selectivities toward H2 and HCOOCH3 were in
turn enhanced vs. those toward CO2 and H2O. At the same time,
the applied negative current caused a decrease in the catalyst
potential measured between the working and reference electrodes
(Fig. 5a), as typically observed in studies with alkali solid electro-
lytes [28,30,34]. The trend of the catalytic activity instead depends
on the NEMCA behavior of the system. According to the theory of
electrochemical promotion [16], the back-spillover of potassium
ions onto the Au–YSZ catalyst film under applied negative currents
led to the decrease in the catalyst potential and work function. It
strengthened the Au chemical bond with the electron acceptor
adsorbates (oxygen) and weakened that with the electron donors
(methanol) [20]. In fact, Broqvist et al. [35] already reported the
interest of the alkali compounds as ‘‘oxygen attractors’’ for signifi-
cantly improving the activity of CO oxidation on an Au-based cat-
alyst. It should be noted that the methanol conversion obtained in
this work did not exceed the 10% probably due to the low surface
area of the active catalyst film and reactants bypass. However, very
interestingly, the tested Au nanoparticles dispersed in a YSZ matrix
were electrochemically promoted by K+ ions leading to an
electrophilic NEMCA behavior under the explored POM reaction
conditions. Other studies have also successfully promoted metal
catalysts dispersed on YSZ both by alkali electropromotion [36]
and by alkali conventional promotion [37]. In the present work,
maximum production rates of 3.7 ꢁ 10ꢀ8 mol H2 sꢀ1, 4.3 ꢁ 10ꢀ8
mol CO2 sꢀ1, and 1.5 ꢁ 10ꢀ7 mol HCOOCH3 sꢀ1 were achieved at
the end of the negative polarization, which corresponded to
Fig. 6a and b shows the results obtained in two additional
experiments under the same POM reaction conditions, which con-
sisted of the same potentiostatic and galvanostatic transitions than
the previous one (Fig. 5), but applying higher currents during the
negative polarization: I = ꢀ10
lA (i = 3.2 l
A/cm2) in Fig. 6a-1 and
a-2, and ꢀ20 A (i = 6.4
l
l
A/cm2) in Fig. 6b-1 and b-2. The applica-
tion of a potential of +2 V at the beginning and the end of each
experiment defined again a Au–YSZ free of K-derived species
(unpromoted state). In this way, all the reaction rates remained
almost at the same values upon every positive polarization, con-
firming the complete reversibility of the promotional effect. Then,
as also observed in the first experiment during the application of a
negative current, the migration of potassium ions to the catalyst
surface at a rates, I/F = 1.04 ꢁ 10ꢀ10 mol K sꢀ1 (Fig. 6a-1 and a-2)
and 2.07 ꢁ 10ꢀ10 mol K sꢀ1 (Fig. 6b-1 and b-2) sharply enhanced
the gold catalytic activity. However, it can be found under the
polarizations at ꢀ10
l
A and, more clearly, at ꢀ20
lA that all the
production rates decreased from a certain accumulated amount
of supplied promoter, which was not achieved upon the imposition
of ꢀ5
lA. This poisoning effect could be attributed to the excessive
formation of alkali-derived surface compounds and the concomi-
tant blocking of active sites, as widely observed with both Na-
[37–39] and K-based [18,19,32] promoted systems. Moreover, the
catalyst potential measured after 65 min of negative polarization
decreased from ꢀ0.55 V (Fig. 5a) to ꢀ0.60 V (Fig. 6a-1) and
ꢀ0.74 V (Fig. 6b-1), due to an increase in the maximum potassium
coverage achieved in each experiment. A permanent EPOC was also
observed in these experiments upon the subsequent current inter-
ruption, although it was inevitably affected by the mentioned poi-
soning effect. For instance, in the case of the hydrogen production,
enhancement ratios (qi) of 8.9, 2.5 and 5.3, respectively, with
respect to the production rates obtained under unpromoted condi-
tions. Such an improvement in the catalytic activity was caused by
an accumulated promoter supply of 2.02 ꢁ 10ꢀ7 mol K+ (Eq. (7)).
þ
Hence, an optimum potassium coverage, hK , of 0.32 can be
permanent rate enhancement ratios (cH ) of 8.7, 6.4 and 3.2 can be
estimated in this experiment by considering the total number of
deposited Au sites, N = 6.38 ꢁ 10ꢀ7 mol Au, according to the
following equation:
2
observed at the end of the open circuit imposition in Fig. 5a,
Fig. 6a-1 and b-1, respectively. This parameter has been calculated
using the following equation:
R
t
0
jIjdt
nF
ri;per
ri;0
þ
hK
¼
ð8Þ
ci
¼
ð9Þ
N
It is also interesting to note that upon current interruption (open cir-
cuit conditions, at t = 97 min) a permanent EPOC phenomena was
observed probably due to the remaining of the promoter phases
on the catalyst surface under open circuit conditions. Thus, all the
product reaction rates were kept at their electro-promoted values.
In addition, a very slight increase in the catalyst potential close to
the open circuit potential value typically observed in this work
(V0WR ꢂ ꢀ0.4 V) was detected. This kind of irreversible promotional
effect (Permanent EPOC or Permanent NEMCA) has been reported
elsewhere for alkali-electropromoted systems [27,28,34]. It has been
mainly attributed to the high stability under reaction conditions of
certain promoter species formed on the catalyst surface, like potas-
sium oxides or superoxides [27,28]. It is very important to highlight
the practical application of the observed irreversible NEMCA behav-
where ri,per is the permanent catalytic production rate of the i com-
pound following the promoted state. Nevertheless, the optimum
amount of supplied K+ ions which maximized the catalytic activity
was found to be the same in each experiment (around 3 ꢁ 10ꢀ7
mol K+, which corresponded to a potassium coverage, hK ;opt, of
þ
about 0.5). In addition, the maximum values of the reaction rates
obtained were practically the same. Specifically, the H2, CO2 and
HCOOCH3 production rates were in all cases enhanced around 9.2,
2.6 and 5.5 times, respectively, under optimum electrochemically
promoted conditions. Then, it is interesting to note that the applied
current had no influence on the behavior and magnitude of the
electropromotional effect, but only on the speed of the promotion
process. Finally, the stability of the Au/YSZ catalyst film along the
reproducible behavior in the different experiments was also
demonstrated.
ior: not only a very low current (a few lA) is enough to enhance the
catalytic performance of the gold nanoparticles by several times, but
also a first polarization step may be already sufficient to maintain
this catalytic modification for a certain time, with the consequent
electricity saving. Finally, the imposition of a potential of +2 V again
at t = 134 min restored the initial production rates values within a
few minutes, leading to a completely reversible electropromotional
effect. It was due to the decomposition of the promoter phases and
the electrochemical pumping of the K+ ions back to the solid electro-
lyte in good agreement with the cyclic voltammetry. This reversible
The magnitude of the electrochemical promotion effect is also
typically described by the Faradaic efficiency (K) defined by:
D
r
K
¼
ð10Þ
I
nF
where
Dr is the promotion-induced change in the catalytic rate and
n is the number of electrons involved in the corresponding electro-
catalytic reaction. Under the studied POM reaction conditions at