C.G. Floare et al. / Journal of Molecular Structure 1044 (2013) 72–78
75
0.8
3.90
3.85
3.80
3.75
3.70
3.65
3.60
3.55
(a)
0.7
H3
H5
H6
H3
H5
H6
0.6
0.5
0.4
0.3
0.2
0.1
0.0
(a)
10
-0.1
0
2
4
6
8
0.0
0.2
0.4
0.6
0.8
1.0
[β-CD] (mM)
r1
7.9
7.8
7.7
7.6
7.5
7.4
7.3
7.2
7.1
7.0
1.0
0.8
0.6
0.4
0.2
0.0
-0.2
-0.4
(b)
H5
H4
H2
H7
R1
H5
H6
R1
H8
(b)
0
2
4
6
8
10
0.0
0.2
0.4
0.6
0.8
1.0
[FF] (mM)
r2
Fig. 5. Chemical shifts variation of some representative: (a) b-CD and (b) FF protons
as a function of their concentration, ([b-CD] + [FF] = 10 mM).
Fig. 6. Job’s plots corresponding to the induced chemical shift variation of some: (a)
b-CD and (b) TA protons for the TA: b-CD system.
methyl-phenyl or benzoic groups of the TA or trifluorophenyl and
benzoic acid moiety in the case of FF.
For the shake of concision, only several protons (the most
markedly affected) have been selected and reported in Figs. 6
and 7. In all cases, Job’s plots show a maximum at 0.5, indicating
the existence of complexes with a 1:1 stoichiometry.
The aforementioned 1H NMR observations, for the two studied
systems, could imply two main possibilities: (a) the presence of
two types of 1:1 complexes with the inclusion of both aromatic
rings inside the b-CD cavity, which corresponds to a bimodal com-
plexation or, (b) the formation of a 1:2 drug: b-CD complex, where
the inclusion phenomena are simultaneously present for the two
rings. Considering the chemical structure of TA and FF, the simul-
taneous inclusion of one guest molecule into two b-CD molecules
seems to be sterically unfavorable, which avoids the formation of
1:2 complexes. In order to elucidate which of the two above possi-
bilities is correct the continuous variation method was employed
to establish the stoichiometry of the complexes. In our case, the
continuous variation method is based on the induced chemical
Thus a binary structure formed by one b-CD molecule surround-
ing one guest molecule can be considered reliable for both systems.
To confirm the hypothesis of bimodal inclusion complexation,
ROESY spectra were acquired for TA: b-CD and FF: b-CD complexes.
Due to the rapid dynamics of the complexation process, the ROESY
effects were only quantitatively used and no conclusions on inter-
molecular distances were extracted. The ROESY spectrum of TA:
b-CD complex is reported in Fig. 8. This spectrum allows us to
establish a spatial proximity between the TA protons and the inner
protons of b-CD.
The spectrum shows several cross-peaks between H3, H5 and
H6 protons of b-CD and protons of both aromatic rings of TA (H4,
H5, H6, H7 and H8), demonstrating the inclusion of these groups
in the hydrophobic cavity.
In the case of FF: b-CD system, (Fig. 9), no cross-peaks were ob-
served between H2 on the benzoic acid ring and H3, H5 and H6
protons of b-CD. All the other protons belonging to benzoic acid
moiety and trifluorophenyl moiety give rise to medium to strong
peaks with the inner protons of b-CD, except H3 which has a
cross-peak only with the corresponding H6 proton of the b-CD. It
is worth mentioning that we found cross-peaks only with the inner
b-CD protons, which establishes intra-cavity binding without evi-
dence for outside contributions. These results confirmed the
shift variation,
of the complex.
in the absence and in the presence of the other reactant. Thus if
a physical quantity, containing d, is plotted as a function of the
D
d, which is directly related to the concentration
D
d is defined as the difference in chemical shifts
D
mol fraction of the host or guest, r, (Job’s plot), its maximum value
will occur at r1 = m/(m + n) or r2 = n/(m + n), where m and n are,
respectively, the molar ratios of b-CD and drug in the (drug)n:(b-
CD)m complex. Under fast exchange conditions, for a signal belong-
ing to b-CD, for example, the calculated quantity
D
dꢀ[b-CD] is
proportional to the complex concentration and, can be plotted
against r1, [12]. The continuous variation method was applied for
all protons of the different molecules and yielded identical results.