Tsoncheva et al.
1097
spectrometer (Germany) at 298 K. The magnetic measure-
ments were performed with a Faraday-type magnetic balance
in a temperature range of 298–473 K.
Table 1. Copper content, specific surface area, and magnetic sus-
ceptibility of the initial samples obtained by different preparation
techniques.
The catalytic experiments were carried out in a flow reac-
tor with partial pressure of methanol at 1.57 kPa and WHSV
Cu content
(wt%)
BET
(m g )
χg
2
–1
6
Samples
(g ions × 10 )
–
1
at 1.5 h in a thermo-programmed regime with a heating
–
1
AC
0.0
4.0
5.0
5.0
1060
960
958
657
–0.6
19.0
7.5
rate of 1 K min . A standard catalytic test with time on
stream (about 200 min) at selected temperatures was also
performed. The on-line gas chromatographic analysis was
performed.
Cu-AC-N
Cu-AC-A1
Cu-AC-A2
18.4
Fig. 1. Total conversion vs. temperature on various copper-
loaded samples.
Re s ults a nd dis c us s ion
In Table 1 data of the copper content and specific surface
area for the initial copper-oxide-supported materials are pre-
sented. The magnetic susceptibility of the active phase, cal-
culated as CuO at 298 K, is also given. An essential
decrease in the BET surface area for all copper-loaded sam-
ples in comparison with the parent activated carbon is ob-
served. Therefore, a highly dispersed copper species, located
mainly within the pores of the support, seems to be formed.
In Fig. 1 the temperature dependencies of methanol con-
version for the copper oxide – activated carbon samples, ob-
tained by different techniques, are presented. The main
registered products are CO and H . Methyl formate (MF) is
2
also found at lower temperatures. A well-defined tendency
for increased conversion with increasing temperatures is reg-
istered for Cu-AC-A1. In this case the conversion remains
unchanged (about 100%) above 530 K. On the contrary, a
maximum in the conversion curve at 510 K for Cu-AC-N is
observed. Further increase in methanol conversion above
netic susceptibilities, per g mol Cu2+ ions in the initial sam-
ples, are rather different (Table 1). The lower magnetic sus-
ceptibility for Cu-AC-A1 could be an indication of the
presence of copper species in a lower oxidative state in this
sample, since their effective magnetic susceptibility is zero
(17). Indeed, only in the case of the initial Cu-AC-A1 does
6
00 K is also found. The catalytic activity for Cu-AC-N is
lower compared with that for Cu-AC-A1 in the whole tem-
perature interval that was investigated. The conversion curve
for Cu-AC-A2 is close to that for Cu-AC-A1, up to 600 K,
but a sharp decrease above this temperature is registered. So,
a favourable effect of active phase deposition from ammonia
solution is concluded. However, the preparation technique
that includes a four-fold spraying of the support with copper
solution facilitates the formation of more stable catalysts.
As far as the fact that the activated carbon does not ex-
hibit a catalytic activity in methanol decomposition on its
own (not shown), some significant differences in the copper
state for the initial catalysts could be assumed. Further
changes in the copper state during the catalytic process
could also be expected.
1
+
XPS analysis show the presence of Cu ions (Table 2). So,
the participation of copper species in different oxidative
2
+
2+
2+
1+
states (Cu , Cu –Cu , and Cu ) in the CAC Cu-AC-A1
2
+
2+
2+
could be assumed. On the contrary, Cu and Cu –Cu
ions are exclusively present in the CAC of the initial
Cu-AC-N. In this relation, the observed higher activity for
Cu-AC-A1 (Fig. 1) could be ascribed to the presence of
1
+
Cu ions in the initial CAC. The favourable role of the am-
monia copper precursor for these types of CAC formations
in the process of catalyst preparation is considered. This as-
sumption is also proved by the higher turnover frequencies
(TOF), calculated on the basis of the initial conversion at
different temperatures, for Cu-AC-A1 in comparison with
Cu-AC-N (Fig. 4). However, the similarities of TOF values
for both samples above 530 K could be evidence for some
essential changes in CAC for Cu-AC-N during the reaction.
This conclusion is confirmed by the XPS spectra for Cu-AC-N,
To describe the peculiarities of the active-phase state on
the investigated catalysts, a complex study by different
methods was performed. The XRD spectra for the initial
samples are identical, and CuO is the only phase observed
(
Fig. 2, curve 1). However, two ESR signals are also found
in all investigated samples (Fig. 3), in spite of the fact that
CuO does not register on ESR spectra. This is also in accor-
dance with the results in ref. 16. A sharp ESR signal, typical
0
2+
1+
where Cu , together with Cu and Cu , is found (Table 2).
2
+
2+
0
of single Cu ions, is registered. The presence of Cu ions
Intensive signals, typical of Cu , are also observed in the
2
+
2+
interacting with each other (Cu –Cu ) and characterized
with a broader ESR signal are found as well. So, despite the
nature of the used copper precursor, the CAC in the initial
sample contains predominantly Cu2 ions, differing in coor-
dination and type of interaction. This conclusion is proved
by the magnetic measurements as well. The calculated mag-
XRD spectrum for this sample (Fig. 2, curve 2). On the con-
0
trary, no Cu is found for the used Cu-AC-A1. Hence, a
more stable CAC in Cu-AC-A1 with respect to the reaction
medium influence is most probably formed.
The higher stability of CAC in the ammonia-obtained
sample compared with that in Cu-AC-N could also be
+
©
2003 NRC Canada