vented by using 9-AMA as the CDA of choice and just
looking at the chemical shifts of the diastereotopic methylene
protons (Figure 1).
the 9-AMA moieties adopt two possible orientations: an sp
orientation (the carbonyl and the OMe are synperiplanar)
or an ap orientation (the carbonyl and the OMe are
antiperiplanar).
With these results in hand, the orientation of the anthryl
and carbonyl groups toward the methylene protons can be
visualized, and therefore, the anisotropic effects over those
protons are predicted for each derivative.
Thus, in the bis-(R)-9-AMA ester of a type A diol, the
carbonyl group on the primary alcohol is oriented in such a
way that induces a deshielding effect over the pro-S proton
and a shielding effect over the pro-R proton. For its part,
the anthryl groups of the two auxiliary units are not well
oriented toward the methylene group, so their anisotropic
effects do not influence significantly those two protons
(Figure 2a).
In the case of the bis-(S)-9-AMA ester of the same diol,
the situation is more complex: the carbonyl group at C(1′)
is oriented to cause shielding on pro-R H and deshielding
on pro-S H in both conformers sp and ap, but the anthryl
groups of the two 9-AMA auxiliaries are also well oriented
to act on the methylene protons producing the following
effects: in the sp conformer, pro-R H is shielded by the two
anthryl units, while the pro-S H is shielded by only the
anthryl moiety of the 9-AMA at C(1′) (Figure 2b).
In this way, the methylene protons of a 1,2-diol are
subjected in every derivative to very different shielding/
deshielding effects that should produce very different spectral
patterns for the bis-(R)-9-AMA and the bis-(S)-9-AMA
derivatives (Figure 2c). These results are summarized as
follows: in a type A 1,2-diol, the methylene protons should
resonate at closer frequencies in the bis-(R)-9-AMA than in
the bis-(S)-9-AMA derivative (Figure 2c).
Figure 1. Structures of MPA, 9-AMA, and types A and B 1,2-
diols.
Thus, conformational analysis of the bis-(R)- and bis-(S)-
9-AMA esters of (S)-propane-1,2-diol (configuration type A,
Figure 2), using a combination of theoretical and experi-
Similar analysis on the relative orientation of the aniso-
tropic groups with respect to the methylene protons in the
enantiomeric 1,2-diol (configuration type B) shows the
reverse distribution of shielding/deshielding effects (Figure
2d). This means that in a type B diol the methylene protons
should resonate at closer frequencies in the bis-(S)-9-AMA
than in the bis-(R)-9-AMA derivative (Figure 2d). Figures
2c and 2d show the actual NMR spectra of the bis-9-AMA
esters of (S)- and (R)-propane-1,2-diol (types A and B,
respectively).
Figure 2. Representative conformers of the (a) bis-(R)- and (b)
Theoretical chemical shift calculations (GIAO)7 on the sp-
II and ap-II conformers of the bis-(R)- and bis-(S)-9-AMA
esters of (S)-propane-1,2-diol showed data in very good
agreement with the experimental chemical shifts.
bis-(S)-9-AMA esters of (S)-propane-1,2-diol. Partial 1H NMR
showing the methylene protons in the bis-9-AMA esters of (c) (S)-
and (d) (R)-propane-1,2-diol, types A and B, respectively.
Experimental demonstration of the general character of
this correlation between absolute configuration of the diol
and the spectra of the methylene protons was obtained with
a series of 1,2-diols of known absolute configuration (1-9,
mental data,4 indicated that in both the bis-(R)- and the bis-
(S)-9-AMA derivatives there is a conformational equilibrium
between two main conformers: II-sp and II-ap (Figure 2).
In these conformers, the O-C(1′) bond adopts a II confor-
mation with the carbonyl of the 9-AMA at C(1′) coplanar
to the pro-S-methylene proton5 at C(1), and the C(1′)-C(2′)
bond is in a gt (gauche-trans) conformation.6 For its part,
(5) The pro-R and pro-S-methylene protons have been assigned by means
of deuteration experiments (See Figure S5 in Supporting Information). Note
that in a type A 1,2-diol, the pro-S-proton resonates at lower field and the
pro-R at higher field, while in a type B 1,2-diol, the pro-S resonates at
higher field and the pro-R at lower field.
(6) H(2)-C(2)-C(1)-H proR in gauche and C(3)-C(2)-C(1)-O in
(4) For conformational studies by CD, structure calculations, coupling
constants analysis, and selective deuteration, see Supporting Information for
details.
trans conformations.
(7) Aromatic shielding effect calculations were performed using Gaussian
98. See Supporting Information.
Org. Lett., Vol. 12, No. 2, 2010
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