K. Srinivasan et al. / Journal of Molecular Structure 1036 (2013) 494–504
501
Table 3
where IG is the reduction peak current of guest molecule of 2,6-DNP,
and IHG is the reduction peak current of inclusion complex of 2,6-
DNP:b-CD. IHG ꢀ IG is the difference between the reduction peak
CV for 2,6-DNP:b-CD in pH ꢁ 7 and pH ꢁ 3 buffer solution, scan rate 100 mV sꢀ1, 2,6-
DNP (Conc. 2 ꢂ 10ꢀ4 M) and (a–g) 0–12 ꢂ 10ꢀ3 M b-CD concentrations.
b-CD
concentration
(M)
pH ꢁ 3
Epc (V)
pH ꢁ 7
current of inclusion complex and 2,6-DNP.
DI is the difference be-
tween the molar peak current coefficient of the inclusion complex
and 2,6-DNP. The [2,6-DNP]0 and [b-CD]0 are the initial concentra-
tion of 2,6-DNP and b-CD, respectively.
Ipc
(lA)
Epa
Ipa
Epc (V)
Ipc (lA)
(V)
(lA)
Plotting of [1/IHG ꢀ IG] verses 1/[b-CD] gives a straight line for
both pH solution as shown in Fig. 5. Good linear correlations were
obtained (r = 0.9881, 0.9841 for pH ꢁ 3 and pH ꢁ 7 respectively),
confirm that the formation of a 1:1 inclusion complex for both
pH (pH ꢁ 3 and pH ꢁ 7) solutions. From the intercept and slope
values of this plot K was evaluated, the binding constant values
for 2,6-DNP:b-CD is 16 Mꢀ1and 36 Mꢀ1 in pH ꢁ 3 and pH ꢁ 7
respectively. These values indicate that 2,6-DNP molecule is encap-
sulated in the b-CD cavity to form an inclusion complex.
Without b-CD
0.002
ꢀ0.336 ꢀ2.557
ꢀ0.534 ꢀ8.629
ꢀ0.334 ꢀ3.467
ꢀ0.531 ꢀ8.641
ꢀ0.331 ꢀ4.053
ꢀ0.529 ꢀ8.917
ꢀ0.329 ꢀ4.072
ꢀ0.529 ꢀ9.289
ꢀ0.319 ꢀ4.162
ꢀ0.519 ꢀ9.434
ꢀ0.309 ꢀ4.233
ꢀ0.512 ꢀ9.443
0.101 1.832 ꢀ0.260 ꢀ1.063
ꢀ0.705 ꢀ7.981
0.103 1.827 ꢀ0.263 ꢀ1.795
ꢀ0.700 ꢀ8.306
0.103 1.810 ꢀ0.263 ꢀ1.940
ꢀ0.697 ꢀ8.836
0.103 1.774 ꢀ0.265 ꢀ2.164
ꢀ0.692 ꢀ10.100
0.103 1.673 ꢀ0.268 ꢀ2.420
ꢀ0.688 ꢀ10.170
0.106 1.436 ꢀ0.268 ꢀ2.583
ꢀ0.688 ꢀ11.030
0.004
0.006
0.008
3.6. 1H NMR spectrum
0.010
The prepared solid inclusion complex can be analyzed by 1H
NMR spectra [16]. Fig. 6 shows the typical 1H NMR spectra of (a)
b-CD, (b) the solid inclusion complex of 2,6-DNP with b-CD (chem-
ical shift changes with b-CD), (c) 2,6-DNP and (d) the solid inclu-
sion complex (chemical shift changes with 2,6-DNP). The values
of chemical shifts, d for different protons in b-CD with solid inclu-
sion complex and 2,6-DNP with solid inclusion complex were
listed in Tables 4 and 5. The changes in chemical shift (d) of H3
and H5 protons suggested that the 2,6-DNP guest is encapsulated
into the nanohydrophobic cavity of b-CD. The phenyl ring of 2,6-
DNP shift the signals of b-CD protons (H3 and H5) upfield, due to
the anisotropic effect of the aromatic ring. On the contrary, the
chemical shifts of H1, H2, H4, which are exposed to the solvent
and H6ab, which are on the narrow opening of b-CD, as shown in
Scheme 6b, are slightly affected by the guest molecule. On the
other hand, the chemical shifts of Hb and Hc of 2,6-DNP
(Scheme 6c) which are inserted in the nanocavity of b-CD are also
shifted upfield due to the interaction between 2,6-DNP and b-CD.
(On the other hand, as shown in Fig. 6d, when 2,6-DNP monomer
entered into the nanohydrophobic cavity of b-CD, the change of
the microenvironment of 2,6-DNP protons leads to the phenyl ring
protons was moved into upfield shift. The significant distinguish
for these 1H NMR spectra strongly confirmed that the solid com-
plex was formed in the inclusion process.
0.012
ꢀ0.287 ꢀ5.884
ꢀ0.482 ꢀ11.760
16
0.106 1.005 ꢀ0.273 ꢀ2.693
ꢀ0.683 ꢀ12.000
Binding constant
36
(Mꢀ1
)
D
G (kJ molꢀ1
)
ꢀ7
ꢀ9
Fig. 5. Benesi–Hildebrand plot of 1/IHG ꢀ IG vs.1/[b-CD] for 2,6-DNP in pH ꢁ 7 and
pH ꢁ 3 solutions.
3.7. FT-IR spectral studies
and reduction mechanism of 2,6-DNP was clearly explained in
Scheme 5.
The solid complex formation confirmed by FT-IR spectroscopy
(Fig. 7), because the bands resulting from the included part of
the guest molecule generally shifted or their intensities altered
[9]. In 2,6-DNP the two peaks are observed at 1537 cmꢀ1 and
1346 cmꢀ1 due to the characteristics stretching of aromatic nitro
group. The characteristics peak of ACAN stretching vibration ap-
peared at 855 cmꢀ1 for aromatic nitro group. The AC@CA stretch-
ing vibration appeared at 1622 cmꢀ1 and 1589 cmꢀ1 for aromatic
nuclei. The @CAO stretching vibration appears at 1154 cmꢀ1. In
the spectrum for complex the characteristics stretching peaks of
aromatic nitro group intensities are decreased and shifted to
1524 cmꢀ1 and 1337 cmꢀ1, this is due to the nitro groups were in-
cluded into the b-CD cavity. The characteristic ACAN stretching
vibration was shifted to 856 cmꢀ1 and it intensity also decreased,
this is confirmed that the nitro group was included into the b-CD
cavity. The characteristic stretching vibration of AC@CA intensities
are reduced and shifted to 1633 cmꢀ1 and 1591 cmꢀ1 this is due to
the benzene ring encapsulated into the b-CD cavity. The character-
istic @CAO stretching vibration slightly shifted to 1156 cmꢀ1 this
indicates the OH group is projected above the b-CD rim. From
The cathodic peak current (Fig. 4 and Table 3) ipc, increased with
increasing the b-CD concentration in both pH solutions (pH ꢁ 3
and pH ꢁ 7). The cathodic peak potential, Epc, shifted in positive
direction when b-CD concentration increased in both case. The re-
sult showed that the inclusion complex between 2,6-DNP and b-CD
was formed when 2,6-DNP was added into b-CD aqueous solution.
In addition, the cathodic peak current was increased with increas-
ing b-CD concentration; this is due to the nitro groups are encap-
sulated in the b-CD cavity and the catalytic behavior of b-CD to
the included guest molecule (2,6-DNP). This would lead the catho-
dic peak potential shift in positive direction and the anodic peak
potential shift in positive direction.
The binding constant (K) and stoichiometric ratios of the inclu-
sion complex of 2,6-DNP can be determined according to the Bene-
si–Hildebrand [15] relation assuming the formation of a 1:1 host–
guest complex.
1
1
1
¼
þ
ð4Þ
IHG ꢀ IG
D
I
K½2; 6-DNPꢃ0DI½b-CDꢃ0