K.H. Pannell et al. / Polyhedron 19 (2000) 291–295
295
of FcHgCl) was added dropwise to 1.0 g (3.7 mmol) of 2,5-
bis(chlorodimethylsilyl)thiophene in 30 ml of THF at
y788C. The mixture was stirred overnight and then the sol-
vent was removed in vacuo. The product was extracted with
hexane, and the solution filtered. After removal of the solvent
di-n-butylmercury was distilled to leave a gummy residue.
This was dissolved in the minimum of hexane and placed
upon a 10=2 cm silica gel column(60–200mesh)andeluted
with hexane. An orange band developed and was collected,
the solvent removed and the final residue recrystallized from
hexane to yield III, 1.2 g (2.1 mmol, 57%), m.p. 778C.
Also prepared by the same general route, in 65% yield,
was 2,5-bis(ferrocenyldiphenylsilyl)thiophene (IV) from
the reaction of ferrocenyllithium and 2,5-bis(chlorodi-
phenylsilyl)thiophene.
in Table 3 and selected bond lengths and angles are provided
in Table 2. The structures of IIa and III are illustrated in
Figs. 1 and 2, respectively.
4. Supplementary data
Crystallographic data for structures IIa and III are avail-
able from the Cambridge Crystallographic Data Centre, 12
Union Road, Cambridge CB2 1EZ, UK (fax: q44-1223-
336033; e-mail: deposit@ccdc.cam.ac.uk or www: http://
CCDC 140477 (IIa) and CCDC 140478 (III).
Acknowledgements
3.5. Structural analysis of IIa and III
This research has been supported by the R.A. Welch Foun-
dation, Houston, TX (grant no. AH-546) and the NSF.
An orange crystal of approximate dimensions
0.32=0.44=0.80 mm (IIa) and an orange–yellow crystal
approximately 0.60=0.60=0.40 mm in size (III) were
mounted on glass fibers in a random orientation. Intensity
data were collected at room temperature for IIa and y1008C
for III, which decayed under the X-ray beam at room tem-
perature, using a Siemens/Bruker four circle diffractometer
with graphite-monochromated Mo Ka radiation,ls0.71073
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˚
A. Unit cell parametersandstandarddeviationswereobtained
by least-squares fit of 25 reflections randomly distributed in
reciprocal space in the 2u range of 15–308. The v-scan tech-
nique was used for intensity measurements in both cases. A
range of 1.48 in v and variable speed of 3.00 to 20.00 8 miny1
was used for IIa and a 1.28 v-range and a 3.00 to 15.008
miny1 speed for III. Background counts were taken with
stationary crystal and total background time to scan timeratio
of 0.5. Three standard reflections were monitored in both
cases every 97 reflections and showed no significant decay
for IIa and an average intensity decay of 8.2% for III even
at y1008C. The data were corrected for Lorentz and polari-
zation effects but only IIa was corrected semi-empiricallyfor
absorption giving a min./max. transmission ratio of 0.221/
0.254.
´
´
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Both structures were solved by direct methods and refined
using the PC-version of the SHELXTL PLUS crystallo-
graphic software by Siemens. Full-matrix least-squares
refinement minimizing 8w(FoyFc)2 was carried out with
anisotropic thermal parameters for non-hydrogen atoms. The
hydrogen atoms were placed at calculated positions (C–H
˚
0.96 A; UHs0.08) during refinements. The weighing
scheme has the form wy1ss2(F)qgF2 and the final R fac-
2
tors the form Rs8NFoyFcN/8Fo and Rws[wNFoyFcN /
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2
8wFo ]1/2. Relevant crystal and refinement data areprovided
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