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In spite of approximately equal molecular weights (i.e, 16 kg/mol, S53A39)-b-A133 and S83-b-A123 produce L phases of different characteristic sizes in the melt state, as a direct consequence of the effective Flory-Huggins interaction parameter ξeff between the two constitutive blocks: because of its statistical copolymerization with a significant amount of AA motives, S53A39) has an incompatibility with A 133 smaller than that of S83 with A123. The most remarkable repercussion of this feature is that (S53A 39)b-A133 forms a bilayer thinner and less dense in terms of surface chain density than that of S83-b-A123
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This formula is valid provided the scattering lamellar object can be considered as infinite, i.e, their thickness of the lamellae is much smaller than its lateral dimension
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This formula is valid provided the scattering lamellar object can be considered as infinite, i.e., their thickness of the lamellae is much smaller than its lateral dimension.
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The derivative ∂αB/A/∂pH vs pH, however, still clearly shows two distinct contributions to ionization, one broad in the small pH range and the other much narrower in the large pH range. These, as before, are associated with the distinct ionizations of the two constituting blocks. However, the average apparent pHplateau and 〈pK A〉 of the blocks in the diblock, 7.43 and 6.07 for (S 53A39) and Am, respectively, are slightly different from those measured when the blocks were titrated as a mixture, i.e, 7.90 and 5.75. Therefore, the topological link in diblock (S53A39)-bA133, seems to have a slight additional effect on the respective ionizations of the two blocks. As far as the purely acrylic acid block A133 is concerned, this increase in the apparent 〈pKA〉 may be attributed to a hindered polyelectrolyte structure resulting from the self-association in water, b
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A〉 may be attributed to a hindered polyelectrolyte structure resulting from the self-association in water, by analogy with what was observed with a poly(acrylic acid) covalently attached to a polyamide matrix (cf. ref 34) therefore restricted in terms of conformational entropy.
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s = 1.6 M, which may be the locus of a L ' to L transition.
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s = 1.6 M, which may be the locus of a L ' to L transition.
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The fitting procedure minimizes the reduced χ2 parameter ξ2, 1/(n- p)σ[qi2I exp(qi, qi 2Icomp(qi)]2/σ2(qi, where n is the number of experimental points, p that of adjustable parameters, I exp(qi) and Icomp(qi, the experimental and computed intensities at wave-vector qi, respectively, and qi, the experimental standard deviation at wave-vector qi
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