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If we did not fix the location of the interface explicitly, the system would be unstable in the grand-canonical ensemble, i.e., the equilibrium would be a homogeneous phase
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If we did not fix the location of the interface explicitly, the system would be unstable in the grand-canonical ensemble, i.e., the equilibrium would be a homogeneous phase.
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Comparing the saturation line (Formula presented) with the complete phase diagram of the ternary system in Ref. 3, we observe that the saturation line is almost identical to the unbinding transition or the homopolymer-rich phase boundary of the three-phase region
-
Comparing the saturation line (Formula presented) with the complete phase diagram of the ternary system in Ref. 3, we observe that the saturation line is almost identical to the unbinding transition or the homopolymer-rich phase boundary of the three-phase region.
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This criterion applies only if the interaction between the lamellae is negligible, i.e., when the SCF calculations predict highly swollen lamellar phases or when a minor attractive interaction between the interfaces is overcome by repulsion due to fluctuations. Mixtures of copolymers might also prove useful in tuning the interaction between interfaces 12, which is not considered here
-
This criterion applies only if the interaction between the lamellae is negligible, i.e., when the SCF calculations predict highly swollen lamellar phases or when a minor attractive interaction between the interfaces is overcome by repulsion due to fluctuations. Mixtures of copolymers might also prove useful in tuning the interaction between interfaces 12, which is not considered here.
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C. Hiergeist, Ph.D. thesis, Universität Potsdam, 1997 (unpublished).
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The segregation of a chain to the interface is controlled by three contributions to the free energy: (i) the loss of translational entropy, (ii) the lowering of the energy by an amount (Formula presented) per chain due to extending the anchoring blocks into the A-rich phase, and (iii) the loss of conformational entropy at the interface. The latter contribution imparts a spontaneous curvature onto the interface. To a first approximation, we conceive the chain conformation of the triblock at the interface as that of individual blocks at an impenetrable surface. Each block suffers an entropy loss of the order (Formula presented) If we increase the size of the middle block (Formula presented) at fixed (Formula presented) the loss of conformational entropy will outweigh the enthalpic contribution for (Formula presented) and the triblock will be repelled from the interface
-
The segregation of a chain to the interface is controlled by three contributions to the free energy: (i) the loss of translational entropy, (ii) the lowering of the energy by an amount (Formula presented) per chain due to extending the anchoring blocks into the A-rich phase, and (iii) the loss of conformational entropy at the interface. The latter contribution imparts a spontaneous curvature onto the interface. To a first approximation, we conceive the chain conformation of the triblock at the interface as that of individual blocks at an impenetrable surface. Each block suffers an entropy loss of the order (Formula presented) If we increase the size of the middle block (Formula presented) at fixed (Formula presented) the loss of conformational entropy will outweigh the enthalpic contribution for (Formula presented) and the triblock will be repelled from the interface.
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52
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C. Frank, Diploma thesis, Universität zu Köln, 2001 (unpublished).
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