Angewandte
Chemie
It is known that silica acts as an insulator and that the
conducting properties of silica can be improved through
[
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doping with electrolytes. Interestingly, with our synthetic
route to the silica microspheres, the entrapped molecules of
the ionic liquid induce their conducting properties at room
[
[
[
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temperature.
The bulk conductivity as determined by
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impedance measurements for pristine 1-butyl-3-methylimi-
+
À
dazolium hexafluorophosphate BIM PF is reported as 3.8
6
À2
2
À1 [19]
1
0
Scm mol . The conductivity of the silica spheres was
also measured by the impedance method over the frequency
range 5–50 kHz at room temperature and 608C. The con-
ductivities observed at 5 kHz at different time intervals are
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À6
À6
À6
À2
7
.87 10 , 8.50 10 (72 h), and 9.83 10 Scm (144 h) at
room temperature. The conductivity decreased after 192 h to
À6
À2
[12] B. Karmakar, G. De, D. Ganguli, J. Non-Cryst. Solids 2000, 272,
6
.77 10 Scm . Thus, the presence of entrapped ionic
119.
liquid and water were needed to improve the conductive
properties of our synthesized silica spheres. The observed
increase in the conductivity with increasing time was due to
[
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L. Shomon, H. Gottlieb, A. Gedanken, Eur. J. Inorg. Chem.
2005, 522.
[
25]
adsorption of water molecules on the silica. The conduc-
tivity was found to increase with an increase in temperature,
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À6
À6
À2
with values of 8.14 10
216 h) measured at 608C. These results are interpreted as a
result of the increased mobility of entrapped molecules of the
(194 h) and 9.76 10 Scm
[
[
[
(
[
24]
ionic liquid.
2139.
The conductivity of the silica spheres will hopefully gain
importance for their applicability in electrochemistry and
[
19] H. Tokuda, K. Hayamizu, K. Ishii, Md. A. B. H. Susan, M.
Watanabe, J. Phys. Chem. B 2004, 108, 16593.
[
26a–c]
sensors.
The conductivity is most probably due to a
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special oriented alignment of the molecules of ionic liquid
along the surface. A detailed study of the conductivity of an
individual silica sphere is in progress and will be reported
soon. The current process for the synthesis of silica spheres in
an ionic liquid has opened new directions and opportunities to
explore their application in several fields, however more
research has to be carried out to address the challenges that
remain and to explore the importance of ionic liquids in other
fields.
[
2
[
[
[
[
4583; c) R. Wang, S. Hoyano, T. Ohsaka, Chem. Lett. 2004, 33, 6.
Experimental Section
In a typical synthesis, TMOS (0.5 mL, 0.516 g, 3.38 mmol; Aldrich
+
À
Chemical Co, 99%) and BMI PF (3 g, 0.01 mol; Aldrich Chemical
6
À3
Co., 96%; density = 1.37 gcm ) were stirred in a 15-mL teflon vessel
for 1 min at room temperature to form a homogeneous transparent
solution. Then, 0.01m aq. HCl (0.25 mL) was added under stirring.
(Milli-Q water was used to prepare the acid solution and a 0.2-mm
Whatman Anotop 25 filter was used for filtration). The reaction
mixture was stirred vigorously at room temperature for 30 min and
then quenched by the addition of acetone. The white spheres were
separated by centrifuging at 9000 rpm for 10 min, and the product was
washed with acetone several times to remove excess ionic liquid, then
centrifuged at 9000 rpm for 10 min, and dried under vacuum for 24 h.
The size of the silica spheres obtained ranged from 50 to 85 mm.
Received: April 27, 2005
Published online: September 13, 2005
Keywords: conducting materials · hydrolysis · ionic liquids ·
.
silica · synthesis design
Angew. Chem. Int. Ed. 2005, 44, 6560 –6563
ꢀ 2005 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
6563