F. Cataldo / Tetrahedron Letters 45 (2004) 141–144
143
ene–ynes reported in literature15b and further arguments
in favor of the ene–yne nature of the products can be
inferred fromthe FT-IR spectra by the ethylenic
stretching band at 3119 cmꢀ1, by the shift of the residual
acetylenic triple bonds stretching at 2260 cmꢀ1 due to
the change in conjugation and by the development of an
5. Heath, J. R.; Zhang, Q.; OÕBrien, S. C.; Curl, R. F.;
Kroto, H. W.; Smalley, R. E. J. Am. Chem. Soc. 1987,
109, 359–363.
6. Krestinin, A. V. Combust. Flame 2000, 121, 513–524.
7. Richter, H.; Howard, J. B. Prog. Energy Combust. Sci.
2000, 26, 565–608.
8. Kroto, H. W. Angew. Chem., Int. Ed. Engl. 1992, 31, 111–
129.
allenic band at 1957 cmꢀ1
.
9. Holmes-Parker, D.; Chatterjee, K.; Wurz, P.; Lykke, K.
R.; Pellin, M. J.; Stock, L. M.; Hemminger, J. C. Carbon
1992, 30, 1167–1182.
10. Saito, R.; Dresselhaus, G.; Dresselhaus, M. S. Physical
Properties of Carbon Nanotubes; Imperial College Press:
London, 1999; pp 77–79.
The submerged electric arc technique not only permits
the one-pot and economic synthesis of long-chain
polyynes but also permits the use of these products as
cheap intermediates for the synthesis of other interesting
molecules. For instance, the simple reduction of poly-
ynes yields ene–ynes, which are another class of mole-
cule of extreme importance for their antibiotic and
antitumour activity.1
11. Cataldo, F. Carbon 2003, 41, 2671–2674.
12. (a) Cataldo, F. Fullerenes, Nanotubes and Carbon Nano-
structures. 2004, 12, issue 2, in press; (b) Cataldo, F.
Carbon, in press.
13. A 100 mL three-necked Pyrex round-bottomed flask was
filled with 70 mL of acetonitrile (HPLC grade, Fluka).
Two graphite electrodes (99.999% purity, Aldrich), having
a diameter of 3 mm and length of 15 mm, were inserted
into rubber stopcocks. The stopcocks with the electrodes
were inserted into two adjacent necks of the flask so that
the electrodes were submerged into the solvent and
arranged in a ÔVÕ geometry, in contact with each other.
The third neck of the flask was equipped with a
thermometer and used for sampling the solution. A DC
electric arc was ignited between the two electrodes at
about 15 V and a current of 10 A. For the generation of
the polyynes the electrodes were kept in contact under the
solvent and moved up and down slightly in order to
generate a very bright light. The power supply maintained
the current at 10 A while the tension was changing
15 10 V due to the movement of the electrodes. CAU-
TION: THE ELECTRODES MUST BE ELECTRI-
CALLY ISOLATED EXTERNALLY TO AVOID
ELECTRIC SHOCK. During arcing the flask was kept
suspended (but not immersed) inside a Dewar flask half
filled with a mixture of acetone and solid CO2. In this way
the temperature of acetonitrile inside the flask was
maintained at )40 ꢀC. After 1 min of arcing it was
possible to record the crude UV–vis spectrumof the
polyyne mixture formed in acetonitrile: 228, 236, 249, 259,
273, 294, 314 nm. The FT-IR of the crude mixture showed
m–CBC–H ¼ 3312 cmꢀ1 (hexane); m–CN ¼ 2247 cmꢀ1 (KBr,
sh); m–CBC– ¼ 2201 cmꢀ1 (KBr) and m–CBC– ¼ 2160 cmꢀ1
(KBr).
The easy availability of polyyne solutions has permitted
us to explore some properties of these molecules. Sur-
prisingly, diluted polyyne solutions in methanol, n-hex-
ane and decahydronaphthalene are stable for more than
a week if left in air or diffuse daylight.11;12 The polyynes
are easily photolysed by UV radiation in solution.12 We
have shown that, by using selected monochromatic
radiation, it is possible to run selective photolysis of
certain polyynes in the crude mixture whilst preserving
others.12 This may have some future practical applica-
tions.
Despite the polyyne solutions being air-stable, they are
reactive with ozone,12 as expected, and undergo easily
the addition of bromine.12
Acknowledgements
The financial support of ASI (contract I/R/070/02), the
Italian Space Agency is gratefully acknowledged.
References and Notes
14. The crude acetonitrile solution containing the polyynes
was filtered through a polyvinylidene fluoride (PVDF)
Acrodisc membrane having a pore size of 0.45 lm. From 5
to 10 lL of the filtered solution was injected into a
4.6 · 150 mm column (Zorbax Eclipse XDB-C8) con-
nected to an HPLC fromAgilent Technologies model
1100. A mobile phase of CH3CN/H2O 80/20 v/v was used
under isocratic conditions at a flow rate of 1.5 mL/min
and a pressure of 151 bar. The eluted polyynes were
detected by a diode-array detector and identified from
their characteristic UV spectra.
15. (a) Gillam, A. E.; Stern, E. S.; Jones, E. R. H. An
Introduction to Electronic Absorption Spectroscopy in
Organic Chemistry; Edward Arnold: London, 1954; pp
78–79; (b) Perkampus, H. H. UV–vis Atlas of Organic
Compounds. 2nd ed. VCH: Weinheim, 1992. Table A12T1.
16. Graphite electrodes were arced at roomtemperature and
10 A in 70 mL of n-hexane until the polyyne absorption
1. Steglich, W.; Fugmann, B.; Lang-Fugmann, S. Rompp
Encyclopedia of Natural Products; Georg Thieme: Stutt-
gart, 2000.
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Tetrahedron 1972, 28, 4601–4616; (b) Gibtner, Th.;
Hampel, F.; Gisselbrecht, J. P.; Hirsch, A. Chem. Eur.
J. 2002, 8, 408–432 (and references cited therein).
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53–63; (b) Cataldo, F. Polym. Int. 1998, 44, 191–200; (c)
Cataldo, F. Eur. J. Solid State Inorg. Chem. 1999, 35,
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15–22; (f) Cataldo, F. Carbon 1999, 37, 161–163; (g)
Cataldo, F.; Capitani, D. Mater. Chem. Phys. 1999, 59,
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153–160.
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band at 226 nmreached
a value of absorbance
A ¼ 2:5 units (about 3–4 min arcing). The crude polyyne
solution in hexane had a UV spectrumas follows: 207,