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weights and the interactions and is calculated by the model. Good agreement was
observed between the predicted micelle core radii and experimental data [ 284 ] for
PS-b-PBD within PBD, obtained using small angle neutron scattering.
Shull and Kramer [ 77 ] developed and applied the Noolandi Hong theory for the
case of polymer A/polymer B/diblock copolymer AB, but without solvent. They
found that, at a given value of the chemical potential of the copolymer in the bulk
phases m c , the ability of a copolymer to reduce g is highest for small N and small w .
However, at a given value of
f c , higher values of N result in much higher values
of
Dg due to the exponential dependence of m c on wN and because an increase in
m c results in an increase in the density of copolymer chains at the interface.
Theoretical determination of the limiting value of m c associated with the formation
of micelles was made separately [ 38 ], since the possibility of micelle formation was
not explicitly introduced in the theory. A good agreement was found with
the experimental data [ 38 ] for the total amount of copolymer segregating to a
polymer polymer interface for concentrations below CMC using only w as an
adjustable parameter. Using the best-fit value of w , they estimated
Dg for con-
centrations when micelles are not present. For concentrations higher than the
CMC, more micelles will be formed without, however, significantly increasing
the copolymer chemical potential; thus, the interfacial tension will not decrease
further. For the copolymer molecular weights used, a significant increase in the
total copolymer amount adsorbed at the interface was observed at higher copoly-
mer concentrations, which was attributed [ 38 , 102 ] to segregation of micelles to
the polymer polymer interface (as well to the polymer air surface [ 38 , 102 ,
285 ]). The location of the upturn was used to estimate the copolymer chemical
potential at the CMC, which was in good agreement with a full self-consistent-
field theoretical estimate [ 286 ].
4.3.2 Leibler Theory for Nearly Compatible Systems
Leibler [ 282 ] developed a simple mean-field formalism to study the interfacial
properties of nearly compatible mixtures of two homopolymers, A and B, and a
copolymer AB. The free energy was expressed in terms of monomer concentration
correlation functions, which were calculated in a self-consistent way within the
random phase approximation introduced by de Gennes [ 242 ]. For the very broad
interface of nearly miscible systems, a gradient expansion was carried out giving a
generalization of the Cahn Hilliard theory [ 216 ]. As mentioned by Noolandi and
Hong [ 71 ], with the gradient expansion in the theory of Leibler, the diblock
copolymer was effectively treated as a small-molecule solvent compared to the
large width of the interfacial region, and the structure of the copolymer became
irrelevant. The system, thus, behaved as a mixture of two homopolymers driven to
the consolute point by the addition of an excess of solvent. As pointed out by
Leibler, for nearly compatible species (2
4 p 2), two mechanisms of the
interfacial activity of the copolymer chains had to be distinguished: (1) the species
A and B are more closely mixed as copolymer chains and are present in both phases,
< wN
<
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