A. Burczyk et al. / Tetrahedron 61 (2005) 179–188
187
4.1.1. Procedure A. Phthalodinitrile (1) (12 mmol, 1.54 g)
and copper chloride dihydrate (2.5 mmol, 0.425 g) were
ground together and placed in a tube. The mixture was
then irradiated in the microwave reactor for time given in
Tables 1 and 2. The crude product was washed successively
with hot water, acetone, dichloromethane and then was
dried. Next the product was twice dissolved in the
concentrated H SO , precipitated from distilled water,
2
4
filtrated off and washed with water to pH neutral. After
drying under reduced pressure, the phthalocyanine–Cu was
analysed.
4.1.2. Procedure B. Phthalic anhydride (2) (10 mmol,
1.49 g), urea (20 mmol, 1.2 g), copper chloride dihydrate
(
(
2.5 mmol, 0.425 g) and ammonium molybdate as a catalyst
2.0 mmol, 0.47 g) were ground together, placed in a tube
and irradiated in the microwave reactor at high power for
time reported in Table 3. After completion of the reaction,
the product was washed hot water, acetone and dichloro-
methane. Finally, the product was twice dissolved in the
concentrated H SO , precipitated from distilled water,
2
4
filtrated off and washed with water to pH neutral. After
drying under reduced pressure, the phthalocyanine–Cu was
analysed.
Scheme 3. Mechanism for condensation of urea with phthalic anhydride.
Acknowledgements
microwave irradiation can be performed easily in a reduced
time scale applying phthalonitrile (1) or phthalic anhydride
This work was undertaken as part of the EC sponsored
programs D32 COST Program (Chemistry in High-Energy
Microenvironments) and Socrates–Erasmus student
exchange program.
(
2) as a substrate. Solvent-free conditions lead by far to the
best results and to easy-to-perform procedures with
considerable improvements over classical methods. More-
over, the application of the dedicated monomode micro-
wave reactor (Prolabo 402) with temperature monitoring
allowed directly comparing two activation modes (i.e., con-
ventional heating and microwave irradiation) and showed
that non-thermal microwave effects might be very favour-
able during microwave experiments. This can be explained
when one considers the enhancement in the polarity of the
system when the reaction is in progress thanks to a well-
fitted mechanism. Eventually, the reactions under conven-
tional conditions that were carried out in the same time scale
gave products in much lower yields of unacceptable purity.
References and notes
1
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Structure, and Function; Cambridge University Press:
Cambridge, 1998.
2
3
4
5
. Moser, F. H.; Thomas, A. L. The Phthalocyanines; CRC: Boca
Raton, 1983.
. Leznoff, C. C.; Lever, A. B. P. Phthalocyanines. Properties
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. Anthopoulos, T. D.; Shafai, T. S. Appl. Phys. Lett. 2003, 82,
4
. Experimental
1
628.
. Wrobel, D.; Boguta, A. In Molecular Low Dimensional and
Nanostructured Materials for Advanced Technology; Graja,
A., Ed.; Kluwer Academic: The Netherlands, 2002.
4
.1. Materials
,2-Dicyanobenzene, phthalic anhydride, urea, copper (II)
1
6. Pannemann, Ch.; Dyakonov, V.; Parisi, J.; Hild, O.; Wohrle,
D. Synth. Met. 2001, 121, 1585.
chloride dihydrate and cobalt (II) hexahydrate were
purchased from the Aldrich Chemical and were used
without further purification.
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Infrared spectra were recorded on the BIORAD spectro-
photometer model FTS-165 as KBr pastille. The elemental
analyses were realized in CNRS (Centre National de la
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999, 2323.
The preparation of copper phthalocyanine is representative
of the general procedures.
13. Muller, S.; Mantareva, V.; Stoichkova, N.; Kliesch, H.; Sobki,