Abstract:We propose a model giving the conformation of a star shaped polymer by taking into account the radial variation of the monomer concentration ϕ( r). For an isolated star when increasing r (at the centre of the star r = 0), the variation of ϕ (r) is first given by a constant value (r < f 1/2 l) then has a (r/l)-1 variation (for f1/2 / < r < f1/2 ν-1 /) and finally a (r/l)-4/3 variation (for r > f1/2 ν-1 l); wh ere f is the number of branches, N the number of monomers in a branch and ν and l are the excluded volu… Show more
“…The blob theory of branched polymers predicts a similar increase in R s with the number of arms (R s ∝ f 1/5 ). 26 Candau et al likewise suggested that R s should increase with the segmental density for branched polymers. 27 In contrast to the predictions of these theories for branched polymers, the relative independence of R s on generation number for arborescent 30K polymers is attributed to their hard spherelike behavior.…”
The radius of gyration (R g ) was determined as a function of generation number for arborescent polystyrenes with two different side chain mass average molecular mass (M w ≈ 5000, 5K, versus 30 000, 30K) by small-angle neutron scattering (SANS) measurements. The R g values obtained were analyzed in terms of the Zimm-Stockmayer model for randomly branched polymers, the scaling relation R g ∝ M w V , and the expansion factor R s ) (R g ) goodsolvent /(R g ) Θsolvent . The R g and scaling exponent V ) 0.26 ( 0.01 found for G0 through G3 polymers with 5K side chains in cyclohexane-d correspond to the values predicted by the Zimm-Stockmayer model. The R g for G0 through G3 polymers with 30K side chains deviate from the model with V ) 0.32 ( 0.02, corresponding to V ) 0.33 expected for hard spheres. Deuterated polystyrene (PS-d) side chains were grafted onto G2 and G3 polystyrene (PS) cores. These copolymers, G2PS-graft-PS-d and G3PS-graft-PS-d, were characterized as spheres with a well-defined PS core-PS-d shell structure by the SANS contrast matching method. The shape and the segment radial density profile of the core and shell for GPS-graft-PS-d were determined based on P(r) and ∆F(r) obtained by indirect Fourier transformation and deconvolution methods (P(r), pair distance distribution function and ∆F(r) ) F(r) -F(solvent), scattering length density contrast profile).
“…The blob theory of branched polymers predicts a similar increase in R s with the number of arms (R s ∝ f 1/5 ). 26 Candau et al likewise suggested that R s should increase with the segmental density for branched polymers. 27 In contrast to the predictions of these theories for branched polymers, the relative independence of R s on generation number for arborescent 30K polymers is attributed to their hard spherelike behavior.…”
The radius of gyration (R g ) was determined as a function of generation number for arborescent polystyrenes with two different side chain mass average molecular mass (M w ≈ 5000, 5K, versus 30 000, 30K) by small-angle neutron scattering (SANS) measurements. The R g values obtained were analyzed in terms of the Zimm-Stockmayer model for randomly branched polymers, the scaling relation R g ∝ M w V , and the expansion factor R s ) (R g ) goodsolvent /(R g ) Θsolvent . The R g and scaling exponent V ) 0.26 ( 0.01 found for G0 through G3 polymers with 5K side chains in cyclohexane-d correspond to the values predicted by the Zimm-Stockmayer model. The R g for G0 through G3 polymers with 30K side chains deviate from the model with V ) 0.32 ( 0.02, corresponding to V ) 0.33 expected for hard spheres. Deuterated polystyrene (PS-d) side chains were grafted onto G2 and G3 polystyrene (PS) cores. These copolymers, G2PS-graft-PS-d and G3PS-graft-PS-d, were characterized as spheres with a well-defined PS core-PS-d shell structure by the SANS contrast matching method. The shape and the segment radial density profile of the core and shell for GPS-graft-PS-d were determined based on P(r) and ∆F(r) obtained by indirect Fourier transformation and deconvolution methods (P(r), pair distance distribution function and ∆F(r) ) F(r) -F(solvent), scattering length density contrast profile).
“…For aqueous dispersions of spherical micelles, which include almost all the solutions considered in this work, different models have been applied. In the case of low pH (around 2), where the PAA is mostly neutral, the Daoud Cotton model [17] was applied to fit the data. It is based on a dense core and a corona whose radial concentration decreases with a power law.…”
We have linked the structural and dynamic properties in aqueous solution of amphiphilic charged diblock copolymers poly(butyl acrylate)-b-poly(acrylic acid), PBA-b-PAA, synthesized by controlled radical polymerization, with the physico-chemical characteristics of the samples. Despite product imperfections, the samples self-assemble in melt and aqueous solutions as predicted by monodisperse microphase separation theory. However, the PBA core are abnormally large; the swelling of PBA cores is not due to AA (the Flory parameter PBA/PAA , determined at 0.25, means strong segregation), but to h-PBA homopolymers (content determined by Liquid Chromatography at the Point of Exclusion and Adsorption Transition LC-PEAT). Beside the dominant population of micelles detected by scattering experiments, capillary electrophoresis CE analysis permitted detection of two other populations, one of h-PAA, and the other of free PBA-b-PAA chains, that have very short PBA blocks and never self-assemble. Despite the presence of these free unimers, the self-assembly in solution was found out of equilibrium: the aggregation state is history dependant and no unimer exchange between micelles occurs over months (time-evolution SANS). The high PBA/water interfacial tension, measured at 20 mN/m, prohibits unimer exchange between micelles. PBA-b-PAA solution systems are neither at thermal equilibrium nor completely frozen systems: internal fractionation of individual aggregates can occur.
“…N A and star polymers. 73,74 This analogy is particularly obvious for the extreme case N A ) 1. Bug et al 24 find that in this limit eq 2.29 again holds although n j does not increase with N but rather is a decreasing function of…”
Section: Brief Review Of the Phenomenological Theories Of The Formatimentioning
confidence: 99%
“…Finally, Halperin et al 23,25,26 again exploit the analogy with star polymers 73,74 but for the case of N A , N B at finite f. They obtain a power law Unlike in eqs 2.22, 2.25, and 2.30 n j decreases with a logarithm of N B . The cmc is…”
Section: Brief Review Of the Phenomenological Theories Of The Formatimentioning
Short block copolymers in a selective solvent (bad for A-block, good for B-block) are modeled by flexible bead-spring chains, where beads interact with short-range Morse potentials of variable strength. In particular, treating the strength E AA of attraction between monomers of the A-block as a variable, we study the mass distribution of the micelles that are formed under conditions that correspond to the vicinity of the critical micelle concentration (cmc). Choosing a composition f ) NA/N ) 1 /4 for the block copolymers, we vary their chain length N from N ) 4 to N ) 32. Only such relatively short chains can be used in thermal equilibrium, since the relaxation times of the system increase dramatically with increasing length. We show that in the regime of parameters accessible to our study, the number of chains per micelle is rather small and almost independent of chain length, implying that the core radius scales as NA 1/3 in this regime. We compare our results with existing theoretical predictions and with experiments.
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