I. Iriepa et al. / Journal of Molecular Structure 976 (2010) 190–195
193
For a boat disposition of one of these rings, the signal correspond-
ing to H1(5) would be an apparent doublet with a coupling con-
stant about 18 Hz [10].
compound 4 (see Table 1) can be attributed to the anisotropic ef-
fect exerted by the intramolecularly bonded pyrazine moiety over
H6(8)ax
.
In all cases, the 2J[H2(4)ax ꢁ H1(5)] value of ca. 3 Hz accountsfor a
dihedral angle of about 60° according to the Karplus relationship
[11]. In compounds 2, 3, 3J [H2(4)ax ꢁ H1(5)] ꢂ 3.3 Hz is smallerthan
3J [H6(8)ax ꢁ H1(5)] ꢂ 4.5 Hz and consequently the H2(4)ax–C–C–
H1(5) dihedral angle is greater than H6(8)ax–C–C–H1(5); this fact
is in close agreement with a flattened chair conformation for the
cyclohexane ring. Moreover, 3J [H6(8)ax ꢁ H1(5)] ꢂ 4.5 Hz is greater
than 3J [H6(8)eq ꢁ H1(5)] (<2) and 3J [H6(8)ax ꢁ H7eq] ꢂ 4.5 Hz is
greater than 3J[H6(8)eq ꢁ H7eq] (<2); therefore, the H6(8)eq–C–C–
H1(5) and H6(8)eq–C–C–H7eq dihedral angles are greater than
H6(8)ax–C–C–H1(5) and H6(8)ax–C–C–H7eq, respectively; these re-
sults confirm the distortion of the cyclohexane ring.
3.2. IR spectra
Table 3 shows the infrared frequencies (cmꢁ1) with the corre-
sponding assignments of the bands appearing in the NH and dou-
ble bond stretching regions.
Compound 2 in the solid state (KBr) showed a medium infrared
band at 3283 cmꢁ1 which is assigned to the intermolecularly
bonded NH group (see later). This band shifted to 3455 cmꢁ1 and
3462 cmꢁ1 in CDCl3 (0.06 M) and in CCl4 (0.0003 M), respectively,
due to the formation of free N–H groups. However, a small propor-
tion of bonded molecules remained even at high dilution. In the
The N–CH3 13C chemical shifts of compounds 2–5 of about
44 ppm (Table 2) agree with the values found in equatorial N–
CH3 substituted piperidines [4–9,12].
literature [16] the m (N–H) band of secondary amides in the
3340–3270 cmꢁ1 region in the solid state was assigned to a trans
bonded structure while a band in the 3220–3140 cmꢁ1 region
was attributed to the bonded band of a cis complex. Moreover,
for free N–H groups the frequency ranges given are 3470 cmꢁ1
for the trans and 3440–3420 cmꢁ1 for the cis structure. Therefore,
in accordance with 1H NMR data, IR results for compound 2 reveal
that the preferred conformation of this compound for the –NH–
CO– system is trans.
Furthermore, in the 13C NMR spectra, the twin-chair conforma-
tion is confirmed by the C2(4) (73.86–73.89 ppm) and C6(8)
(20.59–20.72 ppm) chemical shifts in agreement with previous
work [4–9]. For a boat conformation, the carbon signals would be
shifted to a higher field because of the steric compressing effect
due to the eclipsing between H2(4)ax ꢁ H1(5) and H6(8)ax ꢁ H1(5)
hydrogen atoms.
In addition, by comparing the NMR results of the a-epimers (2–
5) with those of their corresponding b-epimers [5], we can deduce
that they adopt similar preferred conformations with some slightly
In KBr two bands appeared in the carbonyl amide region at
1637 and 1622 cmꢁ1 and upon dilution in CDCl3 a strong band ap-
peared at 1652 cmꢁ1, indicating that C@O groups are implicated in
intermolecular hydrogen bonding with N–H groups (NHꢀ ꢀ ꢀO@C). In
the related b-compound the intermolecular hydrogen bond was
confirmed by the results obtained by cooling the sample at the li-
quid air temperature which showed a decrease of both N–H and
C@O stretching frequencies, as expected [5].
differences. The values
and
dC6(8)(b-epimers)-C6(8)(2–5) ꢂ 7 ppm can be attributed to
the steric syn-diaxial effect exerted by the axial amido group on
H2(4)ax for b-epimers and on H6(8)ax for -epimers (2–5). Besides,
the effect on H6(8)ax is greater for -epimers due to greater distor-
tion of the cyclohexane ring in comparison with the piperidine one.
The
D
dC2(4)(2–5)–C2(4)(b-epimers) ꢂ 5 ppm
D
a
a
A very strong band at 1534 cmꢁ1 (1510 cmꢁ1 in CDCl3) is as-
signed to the amide II band and according to the literature the
presence of this band confirms the trans conformation of the –
NH–CO– system [17].
In the case of compound 3 the infrared spectrum in the solid
state showed a
D
d H6(8)eq(b-epimers) ꢁ H6(8)eq
(
a
-epimers) ꢂ 0.2 ppm is
attributed to the W arrangement of the equatorial protons with re-
spect to the amido group in the first case; consequently, these pro-
tons would be more sensitive to the inductive deshielding effect
[13].
m ,
(N–H) medium intensity band at 3279 cmꢁ1
which was shifted to 3449 cmꢁ1 in CDCl3 and to 3457 cmꢁ1 in
CCl4. In the carbonyl amide region two bands appeared in the spec-
trum of the solid at 1639 and 1617 cmꢁ1 and one band at
1663 cmꢁ1 in CDCl3 solution. These results agree with results for
compound 2 and are interpreted in the same way. Furthermore,
X-ray data confirm the trans NH–CO structure and the presence
of a double NHꢀ ꢀ ꢀO@C hydrogen bond amide system defining
chains along the z axis in the crystal (d Nꢀ ꢀ ꢀO = 2.930 (5) Å; d
Oꢀ ꢀ ꢀH = 2.1 (1) Å; <N–Hꢀ ꢀ ꢀO@C = 155 (5)°).
Owing to the small differences in the chemical shifts of the H7ax
and H2(4)ax among compounds 2–5 and related systems [4–8], we
can conclude that the positions adopted by the phenyl groups in
2–5 will be the same as those found in the related systems, with
near coplanarity with respect to C–H2(4)ax as it was also observed
in the crystal structure of 3.
The differences
0.2 ppm and
d [H6(8)ax(2–5) ꢁ H6(8)ax(1)(1.49 ppm)] ꢂ 0.1 ppm
can be attributed not only to the -effect exerted by the amido
D
d[H2(4)ax(2–5) ꢁ H2(4)ax(1)(3.59 ppm)] ꢂ
D
r
Contrary to the infrared results obtained for compounds 2 and
group, but also to the decreasing anisotropic effect exerted by the
lone pair of the nitrogen atom when the amino group changes into
an amido group [4].
3, in the case of 4 the m
N–H stretching frequency at 3404 cmꢁ1
in the solid did not change much upon dilution in CDCl3
(3401 cmꢁ1) or CCl4 (3411 cmꢁ1), indicating the existence of intra-
molecular bonding, in this case between the NH group and the vic-
inal heterocyclic nitrogen (NHꢀ ꢀ ꢀN), forming a five member ring as
it has also been deduced from 1H NMR results (see before). Conse-
quently, the amide I band (1681 cmꢁ1 in KBr) did not increase on
dilution in CDCl3 (1671 cmꢁ1). The intramolecular bond was also
present in the related b-epimer, this conclusion being confirmed
by cooling the solid sample at the liquid air temperature: no
change was observed in the NH and C@O stretching frequencies
[5].
The
D
d [H9(2–5) ꢁ H9(1)(3.27 ppm)] value of 1.5 ppm can be
partially attributed to the
p
deshielding effect exerted by the car-
bonyl group over H9, confirming the cis disposition between this
group and H9.
The equivalence of the C1 and C5 protons and C6 and C8 pro-
tons and also of the C1 and C5, and C6 and C8 accounts for free
rotation of the amido group around the C9-NH group [14,15].
In compound 4, the signal corresponding to the N–H amide pro-
ton appears as a doublet centered at 8.3 ppm while in compounds 2,
3 and 5 the doublet appears at 6.4–6.5 ppm. This fact indicates that
the amide proton is hydrogen bonded in CDCl3 solution (see IR re-
sults), in this case forming a five member ring through an intramo-
lecular bond with the vicinal heterocyclic nitrogen (N100, Scheme 1).
In compound 5 the spectrum of the solid showed a
m
N–H band
at about 3330 cmꢁ1 and a strong band at 1658 cmꢁ1 with a shoul-
der at about 1640 cmꢁ1. The
m
N–H band was shifted to 3437 cmꢁ1
in CDCl3 and to 3445 cmꢁ1 in CCl4. However, the amide I band
(1658 cmꢁ1) did not change much in CDCl3 (1662 cmꢁ1) and the
frequency of the amide II band was 1515 cmꢁ1 in both media. As
Moreover, the
D
d [H6(8)ax(4)-H6(8)ax(2, 3, 5)] value (ꢂ0.1 ppm)
and the fact that H6(8)ax and H6(8)eq are isochronous for