1
6
process by in situ infrared spectroscopy. This was accomplished
employing the reaction conditions (entry 9) which provided a
nearly quantitative yield of trimethylene carbonate. Fig. 1 con-
tains the infrared traces for trimethylene carbonate formation
as a function of time, along with the reaction profile for TMC
In an attempt to gain evidence in support of the suggested
reaction pathway outlined in eqn (5), we have examined the
competitive binding ability of oxetane vs. the anion provided by
the cocatalyst n-Bu NX. In order to accomplish this we have
4
employed the anion X = azide because of its strong, isolated
band in the infrared. Upon addition of one equivalent of n-
production as monitored by the infrared absorption in the nCO
region at 1770–1750 cm . Since the nCO bands in TMC and
poly(TMC) are grossly overlapped at 1770 and 1750 cm in
toluene solution, it is important to point out here that the
infrared band monitored in Fig. 1 is exclusively that of TMC
3
-
1
Bu
4
NN
3
to VO(acac)
2
in CH
2
Cl
2
two n
N
infrared absorptions
3
3
-
1
-1
are observed at 2062 and 2005 cm , where the former is due
to VO(acac)
-
3
2
N
3
and the later to free azide ion. Subsequent
addition of 100 equivalents of oxetane resulted in an increase
in the quantity of free azide with a concomitant decrease in
the quantity of vanadium bound azide. That is, azide is a
1
as verified by H NMR spectroscopy. Fig. 2 illustrates the linear
plot obtained from the data in Fig. 1 of ln(A
•
- A
t
), where A is
the absorbance of TMC, vs. time. This provides a pseudo-first
much better ligand for VO(acac) than oxetane. It would be
anticipated that oxetane would be more competitive with the
anion bromide used in our synthetic procedure. Nevertheless as
2
-
4
-1
order rate constant of about 10
s
for a reaction involving a
◦
catalyst loading of 5 mol% VO(acac)
2
at 60 C and 3.5 MPa CO
2
pressure. Further detailed studies of this kinetically well-behaved
reaction will be forthcoming from our laboratories.
we have observed, the use of excessive quantities of n-Bu NBr
greatly inhibits the reaction’s progress. At this point in our
studies we do not have a solid state structure of the adduct
4
formed between VO(acac)
are structures in the literature between VO(acac)
base such as DMAP (4-dimethylaminopyridine) which exhibit
2
and azide or oxetane. However, there
2
and a good
17
a cis-coordination geometry. Endeavours to obtain crystals
of an oxetane derivative of VO(acac) have led to isolation of
X-ray quality crystals of VO(acac) with no oxetane bound to
vanadium or found anywhere in the crystal lattice.
2
2
18,19
Future investigations from our laboratory will be directed
at more comprehensive mechanistic studies of the selective
coupling reaction of various oxetanes and CO
2
to provide six-
membered cyclic carbonates employing a variety of vanadium
catalysts, e.g., in addition to VO(acac) , VO(salen) was found to
2
catalyze this coupling process.
We gratefully acknowledge the financial support from the
National Science Foundation (CHE 05–43133) and the Robert
A. Welch Foundation (A-0923). Professor Adolfo Horn also
gratefully acknowledges funds for a sabbatical leave from
CAPES (Brazil).
Fig. 1 (A) Three-dimensional stack plot of IR spectra collected every
3
2
min during the coupling reaction of oxetane and CO . (B) Reaction
Notes and references
profile indicating trimethylene carbonate formation with time. Reaction
carried out at 60 C in toluene in the presence of 5 mol% of VO(acac)
and 1 equiv. of n-Bu NBr at 3.5 MPa of CO pressure.
4 2
◦
2
1
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Weinheim, 2010.
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Fig. 2 Plot of ln(A
absorbances for trimethylene carbonate (1765 cm ) at time = infinitive
and time = t, respectively. Slope = 1.0 ¥ 10
•
- A
t
) vs. time, where A
•
and A
t
are the infrared
-1
-4
-1
2
s
with an R value of
0
.9985.
1
378 | Green Chem., 2010, 12, 1376–1379
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