2
108
SHISHMAKOV et al.
3
1
drying of the sample at room temperature for 3 days.
The bands were assigned on the basis of reference data
in the C H OH group, and the band at 1035 cm , to
the stretching modes of the primary alcoholic group
in various conformations. In the spectrum of PC in
[
10]. The intensities of the spectra were processed
using the spectrometer software.
1
the range 860 400 cm , there is a broad diffuse ab-
sorption on whose background a series of ill-defined
bands characterizing various vibrations of the pyra-
nose ring and bending modes of hydroxy groups are
observed. The interaction of PC with hydrated tita-
nium dioxide in the modified samples results in vari-
The kinetic experiments were carried out in a tem-
perature-controlled reactor equipped with a reflux
condenser, with stirring of the aqueous-methanol so-
lution (volume ratio water : methanol = 1 : 1) by air
1
bubbling. The air flow rate was 3.1 l h .
ation of the intensities of the absorption bands corre-
1
TMHQ was oxidized at 50 0.2 C. The concentra-
sponding to hydroxy groups (the band
at 2900 cm
as
tion of the substrate was 66, and that of CuCl2 2H O,
was used as an internal reference). The most signif-
icant increase in the intensity (by a factor of 1.2 2) is
observed for the bands at 1159, 1054, and 1035 cm .
Variations in the spectrum of PC increase with
the fraction of the inorganic component in the sample.
Thus, variation of the spectral characteristics of PC
suggests that its hydroxy groups are involved in inter-
2
6
mM.
1
The kinetic measurements were performed by stop-
ping the reaction and determining the content of
the starting substance. The resulting functions of con-
centrations were subjected to polynomial approxima-
tion. The initial reaction rates were found by numeri-
cal differentiation and interpolation. The error in their
determination was no more than 10%. The TMHQ
content was determined by gas-liquid chromatography
on a Chrom-4 chromatograph [11].
particle interaction with TiO via hydrogen bonds.
2
Previously, [15] we have studied the model cata-
lytic liquid-phase oxidation of TMHQ with atmo-
spheric oxygen in the medium of TiO gel:
2
The resulting cellulose-inorganic materials were
studied by IR spectroscopy. The IR spectrum of ti-
tanium dioxide xerogel contains a strong absorp-
tion band peaked at 340 and 560 cm , which can
be regarded as a superposition of vibrations of
OH
O
CH3
CH3
2+
CH3
CH3
Cu , O , TiO
2
2
1
CH3
CH3
OH
O
the Ti O bonds and water librations. In the range
1
1
000 1200 cm , there are three extremely weak
It has been established by ESR spectroscopy [16]
peaks, which can be assigned to bending modes of
the Ti OH groups (1192, 1168, and 1090 cm ).
that, depending on the Cu(II)/TiO ratio, several types
2
1
of Cu(II) compounds are formed in the titanium diox-
ide phase: mono complexes, associates of mono com-
plexes, copper(II) hydroxide, and polynuclear bridged
compounds. The last kind of compounds was the most
reactive.
For modified samples of TiO , there are no changes
2
in the range of vibrations of the Ti O bonds. Weak
peaks corresponding to the Ti OH groups are not ob-
served on the background of the bands of PC. The IR
spectrum of cellulose is mainly determined by ab-
sorption of three hydroxy groups incorporated in
a glucopyranose unit. In the spectrum of PC there
Addition of powder cellulose does not affect the
course and parameters of the catalytic process. Ap-
parently, Cu(II) does not react with PC under the re-
action conditions.
1
are the following absorption bands: 3348 cm , stretch-
ing modes of hydroxy groups; in the range 3000
1
2
800 cm , stretching modes of methylene and
The dependences of the initial rate of TMHQ oxi-
dation on the Cu(II) content of the MX phase for
the samples of various compositions are shown in
Fig. 1. The dependences are nonlinear because of
the formation of various Cu(II) compounds and also
because of limitations imposed by the sorption capaci-
ty of xerogel for Cu2 ions. The maximum observed
in the dependences is caused by the formation of
the most catalytically active Cu(II) species on the sur-
face of titanium dioxide. The number of these com-
pounds increases with the fraction of PC in the sam-
1
methine groups of cellulose; 1640 cm , HOH, bend-
ing modes of water of crystallization. The band at
1
451 cm 1 corresponds to (OH); 1427, to (CH ) +
2
(
CH); 1369, to (CH); 1335, to (OH) (in-plane);
1
1
315, to (CH ) (wagging vibrations); 1281, 1248,
235, and 1203, to (OH) + (CH) [12]. According
2
+
1
to published data [13], the band at 1159 cm corre-
sponds to asymmetric stretching modes of the C O C
bridge; however, in some publications [14] this band
is assigned to the C O stretching or O H bending
modes of the C OH group. The band at 1054 cm 1
is assigned to the stretching modes of the C O bond
ple. The sample of the composition of TiO : PC =
2
0.06 : 0.94 did not affect the reaction due to the small
RUSSIAN JOURNAL OF APPLIED CHEMISTRY Vol. 80 No. 12 2007