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S.P. Bank et al. / Carbohydrate Polymers 111 (2014) 806–812
Table 1
-14.9
Size distribution of QAPs and QAP + QABs in aqueous ˇ-CD medium, [ˇ-CD] = 9.0 mM.
TBAP
CTAP
-14.85
-14.8
Samplesa
Mean intensity percent at various size range
0–100 nm
100–1000 nm
1000–3000 nm
-14.75
-14.7
1
2
3
4
5
6
13
52
80
07
08
09
65
60
62
35
16
11
–
–
–
-14.65
-14.6
11
05
09
-14.55
-14.5
a
Sample 1: [CTAP] = 0.5–0.9 mM, Sample 2: [TBAB] = 0.0–0.4 mM, [CTAP] = 0.5 mM
(Constant), Sample 3: [CTAB] = 0.0–0.4 mM, [CTAP] = 0.5 mM (Constant), Sample 4:
[TBAP] = 0.5–0.9 mM, Sample 5: [TBAB] = 0.0–0.4 mM, [TBAP] = 0.5 mM (Constant),
Sample 6: [CTAB] = 0.0–0.4 mM, [TBAP] = 0.5 mM (Constant).
-14.45
-14.4
0.00325
0.0033
0.00335
0.0034
1/T (k-1)
Increase in the CTAP and TBAP concentration in the aque-
ous solution with a constant ˇ-CD concentration increases the
rate constant up to a concentration of 0.8 mM of the QAPs, since
up to that concentration the inclusion complexes of ˇ-CD–QAP
exist in monomeric form. Beyond this concentration, aggregation
has been proposed resulting in a decrease in the rate constant
values. In the present case, prior to the addition of QABs, the ˇ-
CD–QAP inclusion complexes continue to remain in monomeric
form; however, addition of QABs change the rate constants of self-
oxidation/dissociation of CTAP as well as TBAP.
With CTAP as the substrate, addition of both the QABs decrease
the rate constants, which may be due to aggregation of ˇ-CD–CTAP
and ˇ-CD–QAB inclusion complexes. However, when TBAP is taken
as the substrate, which possesses a shorter hydrophobic cleft,
such an aggregation among the inclusion complexes becomes
improbable, rather both the inclusion complexes (ˇ-CD–TBAP
and ˇ-CD–QAB) may be existing in monomeric forms in the
solution, resulting in an increase in the rate constant of self-
oxidation/dissociation.
scattering experiments of the solution containing CTAP, TBAP,
CTAP + TBAB, CTAP + CTAB, TBAP + TBAB, and TBAP + CTAB in 9.0 mM
ˇ-CD solution. The mean intensity percent versus size (r) in nm
for all the samples have been analyzed within three size ranges
(Table 1).
The DLS analyses show that (i) the solutions containing CTAP
do not show any peak in the range of 1000–3000 nm, whereas
a peak in this range is definitely obtained for all the solutions
containing TBAP, (ii) solutions containing only CTAP, as well
as those with TBAB and CTAB along with CTAP show much
higher intensities at all ranges compared to the solutions with
TBAP at comparable size range, (iii) solutions containing CTAP
only, CTAP + TBAB, and CTAP + CTAB show clear enhancements of
percent intensity in the size range of 0–100 nm in the order,
CTAP < CTAP + TBAB < CTAP + CTAB; however, in the size range of
100–1000 the percent intensity remains almost a constant, and
(iv) in case of the solutions containing TBAP only, TBAP + TBAB, and
TBAP + CTAB, the intensities in each of the size range does not show
any remarkable change.
Fig. 5. Plot of ln(kobs/T) versus 1/T at a fixed ˇ-CD concentration of 9.0 mM in aque-
ous medium.
These observations fully corroborate the explanations from
kinetic data: the aggregation of CTAP molecules occurring in the
ˇ-CD solution are further enhanced by the addition of quaternary
ammonium bromide salts and this enhancement increases in order
of the addition of TBAB and CTAB. However, TBAP molecules or
any of the quaternary ammonium bromides along with TBAP in the
ˇ-CD solution do not trigger the formation of aggregated organiza-
tions (Supplementary Fig. 1 (a)–(f)).
Supplementary material related to this article can be found,
A model consistent with the above discussions with reference
to the impact of QAB concentration on the trend of rate constants
of self-oxidation/dissociation of CTAP and TBAP in ˇ-CD aqueous
phase has been presented in Scheme 2.
3.4. Temperature effect
Activation parameters for self-oxidation/dissociation of the
QAPs in ˇ-CD aqueous phase were calculated from the plots of ln
(kobs/T) versus 1/T, which are found to be linear (Fig. 5) and the data
are presented in Table 2.
The thermodynamic parameters are dependent not only on the
extent of self-oxidation/dissociation of QAPs, but also on the impact
of complexation induced by ˇ-CD. ꢄH# values are found to be sig-
nificantly higher than the TꢄS# values, indicating the complexation
process to be enthalpy driven. Besides, the higher ꢄH# value of
CTAP compared to TBAP shows a better inclusion complexation of
the former, due to its longer hydrophobic cleft. The ꢄG# values in
both the QAPs increase with temperature, which indicate better
complexation with the ˇ-CD host molecules at a lower tempera-
ture condition. The negative values of ꢄS# for both the QAPs show
lower randomness and higher stabilization of the systems in the
aqueous ˇ-CD medium.
Table 2
Thermodynamic parameters of pseudo-first order kinetics of self- oxidation/dissociation of QAPs in aqueous medium, [QAP] = 0.5 mM, [ˇ-CD] = 9.0 mM.
QAP
kobs × 105 (s−1
)
T (K)
ꢄG# (kJ/mol)
ꢄH# (kJ/mol)
−ꢄS# (J/mol/K)
57.8
65.2
83.7
295
300
305
94.6
95.8
97.0
CTAP
25.2
235.3
67.3
75.8
86.9
295
300
305
94.2
95.5
96.8
TBAP
16.6
263.0