Angewandte
Chemie
hydrogen bridges.[6] The dimerization energies are difficult
to interpret in a quantitative manner because of the large
variation in hydrogen-bond lengths and orientation, but
typical energies seem to be in the range of 1.0–1.6 kcalmolꢀ1
per H···F contact. However, because of steric restrictions,[6]
the maximum dimerization energy is probably limited to
about 6–7 kcalmolꢀ1 for linear all-syn fluoroalkanes.
In summary, we have used our recently described
synthetic methodology[5] to prepare three unique diastereo-
isomeric a,b,g,d-tetrafluoroalkanes, and the conformational
preferences of each isomer in the solid and solution states has
been examined. It emerges that the avoidance of 1,3-repulsive
interactions is the dominant conformational consideration in
these multi-vicinal fluorine compounds, with the fluorine
gauche effect contributing a more subtle conformational
influence, and we have extrapolated our findings to extended
multi-vicinal fluorine systems. This workprovides the first
conformation study on this class of molecules and provides
information on the behavior and properties of future perfor-
mance molecules containing vicinal fluorine motifs.
Figure 3. Left: The simplified model system 6. Middle: Calculated
linear conformations and right: either minimum (6a, 6c) or next-
higher energyconformation ( 6b). C gray, F green, H white; red arrows
indicate g+ gꢀ-F–F interactions.[11] Relative energies are in kcalmolꢀ1
.
Inset: the model system all-syn-CH3(CHF)12CH3 with its helical mini-
mum energyconformation.
Received: May 4, 2007
Published online: September 4, 2007
Keywords: conformation analysis · fluorine · NMR spectroscopy ·
organofluorine chemistry
than the lowest-energy conformer, which corresponds to the
crystal structure of 5a (Figure 2). The lowest-energy confor-
mer calculated for isomer 6c is similar to that for the solution
structure determined by NMR spectroscopy of 5c, providing
further support that the crystal structure of 5c (Figure 2) is
dominated by packing of the tosyl groups.
The major conformational driving force for the structures
in Figure 3 appears to be avoidance of 1,3-F···F and 1,3-
F···CH3 interactions. For the “linear” conformations, 6a has
two g+ gꢀ interactions,[11] whereas 6c has only one, and 6b
none. From the sequence 6a!6c!6b it is estimated that
each g+ gꢀ-F···F interaction costs about 3.4 kcalmolꢀ1 in steric
strain.[12] For the “bent” pair 6b and 6c, the main difference is
a 1,3-F···CH3 interaction, costing 4.04 kcalmolꢀ1. In this
context, the vicinal fluorine gauche effect (ca. 0.8 kcal
molꢀ1)[7] has only a secondary influence.
.
[1] a) P. Kirsch, Modern Fluoroorganic Chemistry, Wiley-VCH,
Weinheim, 2004; b) R. D. Chambers, Fluorine in Organic
Chemistry, Blackwell, Oxford, 2004.
[3] G. G. Hougham, P. E. Cassidy, K. Johns, T. Davidson, Fluoro-
polymers: Synthesis and Properties, Kluwer Academic, New
York, 1999.
[6] See Supporting Information for further details.
[7] a) N. C. Craig, A. Chen, K. H. Suh, S. Klee, G. C. Mellau, B. P.
[8] CCDC-645778 (5b) and CCDC-645779 (5c) contain the supple-
mentary crystallographic data for this paper. These data can be
obtained free of charge from the Cambridge Crystallographic
for 5a can be found through ref. [5].
To gain insight into conformational effects in more
extended sequences, the all-syn-CH3(CHF)nCH3 series was
studied by computational analysis. For each of the homo-
logues from n = 2–12, the energies and structures of the linear
and the lowest-energy conformation were calculated at the
MP2/6-311 + G(2d,p)//B3LYP/6-31G(d) + ZPE
level
of
theory.[10] Only for n = 2 does the linear conformer represent
the energy minimum. There is a clear, first-order relationship
between relative linearization energies and the number of
g+ gꢀ-F···F contacts,[6] with each such interaction incurring an
energetic price of approximately 3.0 kcalmolꢀ1. In the lowest-
energy conformation of the extended all-syn isomers (see
Figure 3 with n = 12), a helical arrangement is adopted which
[9] Three-bond H–H and H–F coupling constants obey Karplus
ꢀ ꢀ ꢀ
ꢀ ꢀ ꢀ
relationships with the corresponding H C C H and H C C F
dihedral angles: “typical” JHH values are 1–3 Hz for gauche
3
alignments and 6–8 Hz for anti alignments (see ref. [13]), while
“typical” 3JHF values are 5–15 Hz for gauche alignments and 25–
35 Hz for anti alignments (see ref. [14]).
[10] Gaussian03 (RevisionD.01): M. J. Frisch et al., see Supporting
Information. The minimum geometries were optimized on the
B3LYP/6-31G(d) level of theory, and were verified to have only
positive eigenfrequencies. The energies of the conformers were
calculated on the MP2/6-311 + G(2d,p) level of theory, using the
B3LYP/6-31G(d) geometries and zero-point energies. The
energies of the dimers were calculated at the same level of
ꢀ
places all the C F bonds gauche with uniform handedness and
thus avoids any g+ gꢀ-F···F repulsions.
An additional stabilization of the linear-chain conforma-
tion of the shorter all-syn- and possibly also of fragments of
the longer oligofluoroalkanes (all-syn-CH3(CHF)nCH3)
might arise from the formation of intermolecular H···F
Angew. Chem. Int. Ed. 2007, 46, 7887 –7890
ꢀ 2007 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim