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density of up to ca. 1 A cm2 may be inferred. Hence, the
oxidation is a mass transport controlled process and not limited
by electrode kinetics. Increasing the current density beyond the
mass transport limit gives rise to additional oxygen evolution
rather than the desired Kolbe process, resulting in loss of
efficiency. Decreasing the current density below a critical value
2
We thank the Royal Society for financial support through a
University Research Fellowship (F. M.), and DeBeers Industrial
Diamond Division, UK and the EPSRC (GR/N 12051) for
supporting this work.
2
2
of ca. 0.1 A cm causes the Kolbe process to stop as the anode
potential falls below the threshold required for Kolbe elec-
trolysis.
Notes and references
The ultrasound generator employed was a VCX400 model immersion
§
horn (Sonics and Materials, USA) equipped with a 3 mm diameter stepped
titanium-alloy tip (electrically insulated) emitting 20 kHz sound with power
The Kolbe dimer is not produced exclusively: GC–MS and
NMR analysis of the electrolytic products permits the identi-
fication of the ester, amyl caproate, formed in < 5% yield. The
absence of any pentenes and pentanols is novel and surprising.
This is indicative of a trapping of the initial reaction
intermediates at the electrode surface; the pentyl carbocation is
unlikely to be formed as a free intermediate during elec-
trolysis.
22
level set to 190 W cm
(calorimetrically determined). The horn-to-
electrode distance was maintained at 7 mm. Galvanostatic electrosynthesis
3
was undertaken in the thermostatted cell (volume ca. 20 cm ) using a PAR
173 (EG&G) galvanostat fitted with a PAR 178 (EG&G) digital coulometer.
The cathode employed was a coil of platinum wire; the anode was either a
1
2 mm diameter platinum disc (Aldrich) or a 5 3 5 mm free-standing
polycrystalline boron-doped CVD diamond plate (DeBeers Industrial
Diamond Division, UK). Chemical reagents and NaOH (Aldrich) were of
the highest commercially available purity.
It is widely known that ultrasound damages the surface of
platinum electrodes. Recently, boron-doped CVD diamond
1
electrodes have been employed in the presence of ultrasound
with negligible damage to the electrode surface.16 Furthermore,
diamond surfaces are chemically inert under hostile conditions
1
For a review see F. Marken, J. C. Eklund and R. G. Compton,
Electroanalysis, 1997, 7, 509.
2 F. Marken, R. G. Compton, S. D. Bull and S. G. Davies, Chem.
Commun., 1997, 955.
3 F. Marken and R. G. Compton, Electrochim. Acta, 1998, 43, 2157.
4
5
17
and after long-term electrolysis at very positive potentials.
The level of boron doping is high, typically ca. 1020 cm ,
3
O. Behrend, K. Ax and H. Schubert, Ultrason. Sonochem., 2000, 7,
77.
H. Fees and H. Wednt, in Techniques of Electroorganic Chemistry Part
III, ed. N. L. Weinberg, Wiley, New York, 1981, p. 81.
J. F. Rusling and D. L. Zhou, J. Electroanal. Chem., 1997, 439, 89.
R. P. Akkermans, S. L. Roberts and R. G. Compton, Chem. Commun.,
corresponding to a B+C atom ratio of 1+1000, allowing a
resistivity of 0.3 mΩ m to be achieved.18
Galvanostatic electrosynthesis experiments employing a
boron-doped CVD diamond anode were conducted at different
current densities, and the products analysed as before. The
products observed in conventional Kolbe electrolyses suggest
that the electrode material exerts a strong control, with products
6
7
1
999, 1115.
8 H. Fujiwara, M. Atobe, H. Kanetsuna and T. Nonaka, J. Chin. Chem.
Soc., 1998, 45, 175.
9 M. Tashiro, H. Tsuzuki, H. Goto and S. Makata, Chem. Exp., 1991, 4,
predominantly derived from carbocation intermediates detected
at carbon anodes.14 Surprisingly, electrosynthesis at a boron-
4
1.
doped CVD diamond anode under sono-emulsion conditions
again gives rise to the detection of predominately the Kolbe
dimer (see Table 1). Current efficiencies and yields are only
slightly lower than those observed at platinum electrodes.
Interestingly, the ester, amyl caproate is again the sole by-
product, suggesting that a mechanism similar to that at platinum
electrodes is operative.
1
1
1
0 D. J. Walton, S. S. Phull, U. Geissler, A. Chyla, A. Durham, S. Ryley,
T. J. Mason and J. P. Lorimer, Electrochem. Commun., 2000, 2, 431.
1 A. Chyla, J. P. Lorimer, T. J. Mason, G. Smith and D. J. Walton,
J. Chem. Soc., Chem. Commun., 1989, 603.
2 D. J. Walton, A. Chyla, J. P. Lorimer and T. J. Mason, Synth. Commun.,
1
990, 1843.
13 A. N. Blythe, R. P. Akkermans and R. G. Compton, Electroanalysis,
2000, 12, 16.
14 C. J. Brockman, Electroorganic Chemistry, Wiley, New York, 1926.
5 C. R. Wilke and P. Chang, AIChE J., 1955, 1, 264.
6 C. H. Goeting, J. S. Foord, F. Marken and R. G. Compton, Diamond Rel.
Mater., 1999, 8, 824.
7 P. A. Michaud, E. Mahe, W. Haenni, A. Perret and C. Comninellius,
Electrochem. Solid State Lett., 2000, 3, 77.
In summary, Kolbe electrolysis has been accomplished under
the novel conditions of an emulsion generated in situ by power
ultrasound. This method of electrosynthesis renders good yields
of product and is highly charge efficient. For the first time in
1
1
1
50 years,19 the electrode material used and conditions
1
1
employed are observed to have only little effect upon the type of
products formed. Although the mechanism of the reaction is
unclear, it may involve encapsulation of intermediates within
the organic component of the emulsion. This type of electro-
synthetic methodology shows promise for wider application.
8 R. G. Compton, F. Marken, C. H. Goeting, R. A. J. McKeown, J. S.
Foord, G. Scarsbrook, R. S. Sussmann and A. J. Whitehead, Chem.
Commun., 1998, 1961.
19 H. Kolbe, Ann. Chim., 1849, 69, 257.
88
Chem. Commun., 2001, 87–88