I. Iriepa et al. / Journal of Molecular Structure 886 (2008) 59–65
63
of 60°. This value corresponds to a non-distorted piperi-
dine ring [12].
CH3
Heq
CH3
Heq
3
Hax
Hax
4
N
From the data obtained we deduce the existence of free
rotation, in CDCl3 solution, of the amido group around
the C8–NH bond in both epimers. This conclusion is based
on the following experimental data: (a) saturation of the
proton of the N–H group showed NOE enhancements in
the signals corresponding to H8, H1 and H5; (b) the equiv-
alence of the C2 and C4, and C6 and C7 protons and also
of the C2 and C4, and C6 and C7 [13].
Hax
N
2
H
Hax
Heq
Hn
Hx
5
H
N
6
H
Hn
Hx
H
H
1
8
7
H
H
O
N
H
H
O
H
1α
1β
H
H
The NOESY spectra of epimers 1a and 1b showed a
clear correlation between N–H and H20(60) (Fig. 1) indicat-
ing a preferred trans form for the –NH–CO group. This
trans form can also be admitted for 2a–7a and 2b–7b in
agreement with IR results (see below).
Fig. 1. NOE enhancements in compounds 1a and 1b.
assigned to H6(7)n due to a clear correlation signal in the
NOESY spectrum with the signal at 2.65, which corre-
sponds to H2(4)eq. Moreover, the signal at 1.85 ppm
shows correlation in the NOESY spectrum with H8; there-
fore, it must also be assigned to H6(7)x, as said above.
For epimer 1a, saturation of the proton of the N–H group
(5.92 ppm) showed NOE enhancements in the signals at 3.98
(H8), 2.29, 1.80 and 7.75 ppm. The last three signals are
assigned to H1(5), H6(7)x and H20(60), respectively. It can
be noted, through the NOESY correlation peak with H8,
that the signal at 2.29 ppm assigned to H1(5) can also be
attributed to H2(4)ax. Finally, the signal at 2.77 ppm is
assigned to H2(4)eq due to the COSY cross peak with
H2(4)ax.
In the case of the unsaturated compounds 7a and 7b,
the 2D TOCSY spectrum confirms the assignment of
the signals corresponding to each epimer. These com-
pounds can adopt in solution two nearly planar s-cis
and s-trans conformations (Fig. 2). The detailed insight
into the conformational equilibrium generated by the
C–CO degree freedom was obtained by NOE experiments.
We may expect an observable NOE for the vinyl proton
with the N–H and CH3 in the s-cis conformation, for
both epimers. In the case of an s-trans conformation, cor-
relation between the vinyl proton and the CH3 could only
be observed (Fig. 2).
Furthermore, irradiation of the vinyl proton for 7a
(5.49 ppm) showed correlations with the signals at 5.28 and
1.77 ppm. Therefore, these signals must correspond to the
N–H and CH3 groups for the s-cis conformation of the
O@C–C@C system. In the same experiment, we indirectly
achieved saturation of the vinyl proton of the s-trans con-
former (5.78 ppm) by irradiating the vinyl proton of the
s-cis-conformer, which then undergoes saturation transfer
with the s-trans form. This result demonstrates that the equi-
librium of conformers is in the slow-exchange regime on the
NMR chemical shift time scale but in a fast exchange on the
relaxation time scale [14]. The main population of conformers
in the equilibrium corresponds to the s-cis conformer.
In the case of 7b, irradiation of the vinyl proton
(5.60 ppm) showed correlations with the signals at 5.64
and 1.80 ppm. Therefore, these signals must correspond
to the N–H and CH3 groups for the s-cis conformation
of the O@C–C@C system. Moreover, when the signal at
5.60 ppm was irradiated, the signal at 5.74 ppm was fully
saturated by transfer of saturation. The signal at 5.74 cor-
responds to the vinyl proton of the s-trans form, and the
rotation around de C–CO is in a slow-exchange regime
on the NMR chemical shift time scale but in a fast
exchange on the relaxation time scale as it occurs in the
case of 7a. The main population of conformers in the equi-
librium also corresponds to the s-cis conformer.
1
Bearing in mind the similarity of the H NMR spectra
for the amide mixture 1 and the other mixtures (2–7), the
complete assignment of the individual protons for the bicy-
clic system of the amides 2a–7a (Table 1) and the amides
2b–7b (Table 2) has been made.
The 13C NMR spectra of samples 1–7 also showed two
sets of signals for the bicyclic system and the C@O group.
The results are in agreement with the existence of both
a- and b-epimers. Once the resonances of the respective
protons were established, the analysis of the gHMQC spec-
tra allowed the distinction between the chemical shift val-
ues of the carbons of each epimer. Substituents and
electronic effects were also taken into consideration. Tables
3 and 4 show the assignment of 13C NMR chemical shifts.
3.1.2. Conformational study
From the 1H and 13C NMR data, we propose that com-
pounds 1a–7a and 1b–7b in CDCl3 solution adopt a chair-
envelope conformation with the N–CH3 in equatorial dis-
position [7].
3
In compounds 1a–7a, JH8–H1(5) was not observed;
consequently the dihedral angle H8–C–C–H1(5) is ꢁ90°
according to the Karplus relationship [12]. This fact indi-
cates that the piperidine ring is puckered at C8, probably
to relieve the interactions between the amido group and
the H6(7)x protons. On the other hand, in compounds
In conclusion, in both epimers there is equilibrium
between s-cis and s-trans conformations, being the most
populated, the s-cis form. On the other hand, s-cis/s-
trans ratio is higher for 7b. This fact can be interpreted
3
1b–7b, the values of the coupling constants JH8–H1(5)
ꢁ5 Hz are consistent with dihedral angles H8–C–C–H1(5)