M. Cepeda et al. / Chemical Physics Letters 499 (2010) 70–74
73
and [{MBSC}]_T = [{MBSC}]_w + [{MBSC - CD}] + [{MBSC}]_m are
combined with binding constants to give a third-order equation
for the concentration of uncomplexed cyclodextrin:
3
2
a
a
½CDꢂf þ b½CDꢂf þ
¼ KNKCD
c
½CDꢂf ꢁ ½CDꢂT ¼ 0
ð6Þ
ð7Þ
ð8Þ
ð9Þ
b ¼ KN þ KCD þ KNKCDð½SurfꢂT ꢁ ½CDꢂT þ ½MBSCꢂTÞ
¼ 1 þ KNð½SurfꢂT ꢁ ½CDꢂTÞ þ KCDð½MBSCꢂT ꢁ ½CDꢂTÞ
c
These equations were solved for different values of KN allowing
us to obtain the concentration of uncomplexed cyclodextrin for
each surfactant concentration. Using the [CD]f values and with
the [Dn] values, we can fit the experimental kobs values to Eq. (4).
The value of KN for which we obtain the best root-mean-square
deviation (v
2) values in fitting Eq. (4) to the experimental results
was taken as optimal. The validity of this model was tested by fit-
ting Eq. (4) to the experimental data by means of a two-tier opti-
mization process in which the optimized variable was KCD, and
the values obtained in the simple systems were taken as constants.
As can be seen in Table 1 the binding constant of MBSC to the
cyclodextrin is independent of the presence of surfactants. More-
over the binding constant of MBSC to the micelle, Km, is strongly
dependent on the hydrophobicity of the surfactant but indepen-
dent on the presence or absence of b-CD. The insensitivity of Km
to the presence of b-CD is in agreement with the absence of inter-
action between the cyclodextrins and micelles once they have been
formed.
Figure 3. Influence of the surfactant alkyl chain length on the free energy per
aggregated molecule of surfactant (
D
GM,
) and on the free energy of surfactant
complexation by b-CD ( GC, ) at 25.0 °C.
D
D
GM ¼ RT ln cmc0
ð11Þ
´
where cmc is the critical micelle concentration in mole fraction
units. Moreover, from the binding constants of the alkyl sulfonate
surfactants to the cavity of the cyclodextrins we can evaluate the
complexation free energy,
DGC. Figure 3 shows the variation of
D
GM and GC with the alkyl chain length of the surfactant. As can
D
The most important aspect of the results obtained in the pres-
ent study that should be remarked is the kobs value in the maxi-
mum of the plot kobs vs. surfactant concentration (Figure 2). This
value is lower than the value obtained in bulk water and is due
to the presence of uncomplexed cyclodextrin at the micellization
point. The difference between kobs in bulk water and in the mixed
system increases on decreasing the alkyl chain length of the surfac-
tant. In Table 1 we present the percentage of uncomplexed cyclo-
dextrin obtained from a calibration procedure. For any surfactant
concentration, it is possible to obtain the concentration of uncom-
plexed cyclodextrin from a calibration curve. The calibration curve
can be obtained by regrouping Eq. (3) and using previously ob-
tained values for KCD = (1.89 0.01) ꢀ 103 Mꢁ1; kCD = (1.43 0.03)
be observed for alkylsulfonates with very short alkyl chain length,
C4SO3Na, micellization is favored against of surfactant-CD complex-
ation. Because the percentage of uncomplexed cyclodextrin is a
consequence of the balance between micellization and CD-surfac-
tant complexation, on increasing the weight of micellization vs.
CD-surfactant complexation we expect to increase the percentage
of uncomplexed cyclodextrin. If we increase the alkyl chain length
of the surfactant, CD-surfactant complexation is energetically more
favorable than micellization and as a consequence the percentage
on uncomplexed cyclodextrin decreases on increasing the alkyl
chain length on going from C4SO3Na to C10SO3Na.
ꢀ 10ꢁ4 sꢁ1 and kw = (6.0 0.1) ꢀ 10ꢁ3 sꢁ1
.
kw ꢁ kobs
4. Conclusions
½CDꢂf ¼
ð10Þ
KCDðkobs ꢁ kCD
Þ
Mixed systems formed by surfactants and cyclodextrins are
characterized by the presence of a non-negligible amount of
uncomplexed cyclodextrin in equilibrium with the micellar system
once the micelles have been formed. In this way traditional ideas
that micelles are formed only once the complexation ability of
cyclodextrins have been saturated should be removed. The exis-
tence of an appreciable percentage of uncomplexed cyclodextrin
is a consequence of the competitive equilibria of CD-surfactant
complexation and surfactant self-assembly to form micelles. The
balance between both equilibria determines the influence of the
hydrophobic character of the surfactant on the percentage of
uncomplexed cyclodextrin. In this study we have shown that on
decreasing the alkyl chain length of the surfactant micellization
is more important than complexation by the cyclodextrin and
the precentage of uncomplexed cyclodextrin increases.
Results in Table 1 show that the percentage of uncomplexed
cyclodextrin in equilibrium with the micellar system increases
on decreasing the hydrophobic character of the surfactant. This
behaviour is contrary with that previously reported in our labora-
tory [7–9] where the percentage of uncomplexed cyclodextrin in-
creases on increasing the alkyl chain length of the surfactant for
surfactants with alkyl chain larger than ten carbon atoms. Tradi-
tional ideas on mixed CD-surfactant systems consider that the mic-
ellization process only begins once the complexation capacity of
the cyclodextrin has been saturated. Thus supposition implies
the absence of uncomplexed CD in equilibrium with the micellar
system. Our results indicate that this vision should be modified.
We should consider that the complexation equilibrium of the sur-
factant by the CD and the autoassociation of the surfactant (micel-
lization) take place simultaneously. The balance between both
processes will be the cause of the existence of uncomplexed CD
in equilibrium with the micellar system and its variation with
the nature of the surfactant.
Acknowledgments
The total free energy per aggregated molecule of surfactant [16]
in the micelles can be evaluated from the experimental cmc values,
using the following equation:
This work was supported by the Ministerio de Ciencia y Tec-
nología (Project CTQ2008-04420/BQU) and Xunta de Galicia (PGI-
DIT07-PXIB209041PR).