M. Kathiresan et al. / Tetrahedron Letters 51 (2010) 2188–2192
2191
ꢀ
lead to the desired intermediates in good yield using simple recrys-
tallization steps without column purifications. (For detailed syn-
thetic procedures, see Supplementary data). (IV) The intermediate
2d canalso be synthesizedby brominating 5-methyldimethylisophth-
alate using NBS as shown in route IV but this reaction proceeds with
low yield because of the electron-withdrawing effects of the two ester
groups.18
delivering reasonable values. If the PF6 counter ion is omitted in
the same calculation, the lowest energy torsional angles s1–3 do
not change, indicating that the counter ion is not governing the tor-
sional angles, rather the organic structure governs the position of
PF6. The torsional energy barriers related to a 360° rotation around
s1
,s
2 and
at 10° increments without further geometry optimization (see Sup-
plementary data). For a 360° rotation around 1 (with the 2 and s3
s3 have been judged from single point energy calculations
The mono- or di-alkylation of 4,40-bipyridine is highly influ-
enced by the solubility of the products in the solvent media. Dial-
kylation can be prevented by choosing a solvent in which the
starting materials are soluble and the monoalkylated product is
insoluble. In our case, we suppress the double alkylation by adding
1 equiv of 1c slowly to 5 equiv excess of 4,40-bipyridine in CH3CN.
The precipitated product is then filtered, washed with CH3CN, dis-
solved in water and precipitated as hexafluorophosphate salt. The
pale yellow powder thus obtained is again dissolved in water,
heated to 80 °C and then cooled to yield pale yellow crystals.
(Note: the pale yellow crystals became light green upon exposure
to air). 3b is synthesized using the same procedure, that is, 1 equiv
of 1d is added slowly to 10 equiv of 4,40-bipyridine in CH3CN and
the resulting product is precipitated as hexafluorophosphate. The
detailed synthetic procedures, CV and UV–vis characterizations
are given in the Supplementary data.
s
s
values fixed at their X-ray values) a fourfold barrier with a height
below 1 kcal/mol was found, with one of the minima identical to
the X-ray value (37.9°). PM3-based Wiberg atom–atom bond order
calculations34 reveal a bond order of only 1.02 between C3 and C6
for the minimum conformation in agreement with the observed
low-energy torsional profile.
Rotation along s2 (with the s1 and s3 values fixed at their X-ray
values) shows again a low-energy barrier (2–3 kcal/mol) but two-
fold, as expected for the methylene–pyridinium interaction. Finally
for the rotation around s3 showed a low-energy barrier but twice
as that of s2 (5–6 kcal/mol) and twofold as expected for the meth-
ylene–phenyl interaction.
1H NMR spectra of the viologen dendrimers with the 3a subunit
show high symmetry indicating fast conformational changes.3 Fur-
thermore, cyclic voltammetry studies on 3a and 3b show slow fast
electron transfer rates, which is again typical for redox couples
with low activation barriers.
In summary, the conformational analysis of 3a, based on X-ray,
cyclic voltammetry and NMR data, representing a structural sub-
unit of benzylic viologen dendrimers, reveals high flexibility with
respect to the three torsional angles that play a role for the dendri-
mers shape.
3. X-ray crystallography, cyclic voltammetry and modelling
Viologen dendrimers3,4,19 and dendrons20 have been prepared
extensively from 4,40-bipyridine and 3a using sequential substitu-
tion and activation reactions discussed in the prior paragraph. The
geometry of the resulting dendritic structure has a large impact on
the pimerization of viologen subunits,20 the diffusion coefficient of
the dendrimer, which in turn depends on the hydrodynamic ra-
dius,3,19 and the size of the internal voids which is responsible
for the pickup of large counter ions.4,21
4. Conclusions
The synthesis of viologen dendrimers with 1,3,5-trimethylene-
branching units requires facile access to the CB2-type synthon,
1-[3,5-bis(hydroxymethyl)benzyl]-4-(pyridin-4-yl)pyridinium
hexafluorophosphate (Scheme 1). It is available according to
Scheme 2 from 1c and 4,40-bipyridine. So far the synthesis of 1c fol-
lowed route II (Scheme 2) involving tedious chromatographic sep-
aration. The synthetic route III given in Scheme 2, explored in this
work, allows the production of 1c without the need of chromatog-
raphy. The X-ray analysis of 1-[3,5-bis(hydroxymethyl)benzyl]-4-
(pyridin-4-yl)pyridinium hexafluorophosphate combined with
PM3-modelling studies gives a first time access to the sound esti-
mate of the viologen dendrimer conformation.
A closer look at the dendrimer structure III shown in Figure 1
reveals that the overall conformational space available for the
branches is given by only three torsional angles, that is, s1
and 3, assuming that all the bending angles do not deviate much
from their equilibrium value. The three torsional angles are located
between the two pyridine moieties ( 1), the methylene H and the
pyridine ( 2) and between the same methylene and the phenyl
group ( 3) (II in Fig. 1). Obviously, the salt 3a (I in Fig. 1) exhibits
, s2
s
s
s
s
the same set of angles. We were able to grow crystals of 3a and
to resolve its structure by X-ray analysis22 (Fig. 1 I). The X-ray
structure reveals that there are two molecules in a triclinic unit cell
and the existence of an intermolecular hydrogen bond between
O(1A)–H(1A) and N(1) (see Supplementary data). The torsional an-
gles found in 3a can be used as a reasonable starting point for the
discussion of the dendrimer conformation. The torsional angles s1
in other bipyridinium systems cover the range from 20 to 50° in
case of mono- and dialkylated viologens6,23–29 with no large influ-
ence of the counter ion. However, the oxidation state is of impor-
Acknowledgements
M.K. thanks the Graduate College 612 funded by DFG for finan-
cial support. The discussion with D. H. Taffa on the interpretation
of the electrochemical and UV–vis data is greatly appreciated.
tance, thus a diphenyl viologen shows dihedral angle (s1) of 37°
Supplementary data
and 1° for the dicationic and the radical cationic state, respectively.
The other two torsions s2 and s3 have been reported for dibenzyl
viologen by Inoue et al.30 and by Garcia et al.31 The former found
three different s3 and s2 within a single crystallographic cell, the
Supplementary data (detailed experimental procedures, 1H and
13C NMR spectra of 1c, 3a and 3b, cyclic voltammograms, UV–vis
spectra of 3a and 3b and PM3 calculations) associated with this
article can be found, in the online version, at doi:10.1016/
latter found
torsional angle preference, that is, a low torsional energy profile
for s1 s2 and s3 planes.
s3 = -88.2° and s2 = 168.8°. These findings indicate no
,
Semi-empirical PM3 calculations were performed using Argu-
slab 4.0.132 and Hyperchem 8.0.6.33 When the X-ray structure is
used as a starting point for geometry optimization, a local mini-
mum is found with only minor deviation from the solid state struc-
ture (except for a lateral shift of PF6ꢀ), indicating that PM3 is
References and notes
1. Buhleier, E.; Wehner, W.; Voegtle, F. Synthesis 1978, 155.
2. Hawker, C. J.; Frechet, J. M. J. J. Am. Chem. Soc. 1990, 112, 7638.
3. Heinen, S.; Walder, L. Angew. Chem., Int. Ed. 2000, 39, 806.