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M.E. Gurskii et al. / Journal of Organometallic Chemistry 590 (1999) 227–233
complex 6. The most dramatic change is observed for
3
the coupling J(H-6a, H-7), from approximately 12 Hz
at 246 K (Fig. 4(a)) to 5.5 Hz at room temperature
(Fig. 4(d)). The former value is characteristic for aa
couplings in cyclohexane rings [17], which means that
at 246 K the boat conformation of the carbocyclic
ring of 6 is the most stable one.
In the low-temperature 13C-NMR spectrum of 5 in
deuteropyridine, no splittings of signals similar to
those observed for solution of 5 in a neutral solvent
were observed. This is not surprising because in 6 the
p-orbital of boron is already occupied by the lone pair
of pyridine, and overlap with the lone pair on oxygen
does not occur.
Thus, it can be concluded that it is the formation of
complex 6 that leads to a change in the conforma-
tional preferences of compound 5, making the boat
conformation of the carbocyclic ring the most stable
one. This is caused by the transformation of the trigo-
nal sp2-hybridized boron atom in 5 to the tetragonal
sp3-hybridized boron atom in 6. The spatial character-
istics of an sp3-hybridized boron atom should be sub-
stantially the same as those for a carbon atom, so the
stability of the (cb) conformation found for 6 is in a
good accord with the conformational properties of
3a,7a-disubstituted bicyclo[3.3.1]nonanes.
Fig. 3. Signal of the proton H-6a, H-8a in the 1H-NMR spectrum
(C6D6, 400 MHz). (a) Of 5 at 293°K; (b) at 343°K.
Scheme 2.
The latter statement is further supported by the
conformational analysis of a stable compound with
a
tetracoordinated boron atom, viz. dibenzoyl-
pair on oxygen with the vacant p-orbital of boron.
Similar effects were earlier observed for MeOBMe2
and (Me2B)2O [16]. An account of a quantitative study
of the activation barriers for hindered rotation around
the BꢀO bond in different 3-borabicylo[3.3.1]nonanes
will be presented in a separate paper.
methanochelate 7, which we prepared from 5 (Scheme
4).
The chemical shifts and coupling constants observed
1
in the H-NMR spectrum of 7 are given in Table 1.
The coupling 3J(H-6a, H-7) is 13.4 Hz, which indi-
cates the axial location of H-7, and therefore the equa-
torial orientation of the phenyl group. Thus the
carbocyclic ring of 7 is in a boat conformation. This
conclusion is strongly supported by the results of 2D
NOESY exper-iments (see Table 4, Fig. 6), in which a
long-range (five bonds) NOE between H-7 and H-9anti
was observed. The chair conformation of the bora-
cyclic ring follows, from arguments similar to those in
2.4. The influence of complexation on the
conformational equilibrium
In Table 3 the temperature dependence of the 11B
chemical shift of a solution of 5 in deuteropyridine is
shown. The chemical shift of boron changes from 19.4
ppm at 246 K to 53.1 ppm at 348 K. The latter value
is similar to that for parent compound 5, the chemical
shift of which in CDCl3 is 53.4 ppm and is almost
independent of the temperature. The change in 11B
chemical shift with decreasing temperature reflects the
shift of the equilibrium between 5 and 6 in favor of
the latter.
4
the previous discussion, from the W-coupling J(H-4a,
H-9anti )=2.4 Hz and the NOE between H-4b and
H-9syn (see Fig. 6).
3. Conclusions
Fig. 5 displays the appearance of the signal of H-6a
The conformational analysis of 3-methoxy-7-phenyl-
1,5-dimethyl-3-borabicyclo[3.3.1]nonane 5 shows that
at room temperature the (cc) conformation is the most
stable one for this compound. An increase in tempera-
ture leads to a shift of the conformational equilibrium,
which increases the population of the (cb) conforma-
1
in the H-NMR spectrum of 5 in deuteropyridine at
different temperatures. According to the previous dis-
cussion, the changes in the spectrum taking place
when the temperature is decreased reflect the shift of
the equilibrium (Scheme 3) in favor of the pyridine