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Light‐scattering studies on solutions of high and low molecular weight polystyrene mixtures used as models of microgel‐containing solutions
Author(s) -
Strazielle Claude,
CzłonkowskaKohutnicka Zofia
Publication year - 1978
Publication title -
journal of applied polymer science
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.575
H-Index - 166
eISSN - 1097-4628
pISSN - 0021-8995
DOI - 10.1002/app.1978.070220422
Subject(s) - polystyrene , physics , toluene , scattering , analytical chemistry (journal) , polymer , crystallography , chemistry , chromatography , optics , nuclear magnetic resonance , organic chemistry
Abstract Diluted solutions of linear polystyrene (PS) in toluene and dioxane were studied by the light‐scattering method. The solutes were mixtures of high‐M̄ w and low M̄ w PS. The dissolved PS mixtures were regarded as polymer solutions containing microgels, the high‐M̄ w PS being looked upon as the microgel counterpart. The calculation method as proposed by Strazielle 1 and Burchard 2 was used to evaluate the microgel percentage and particle size, whereby the method could be verified against mixtures with well‐known weight composition and \documentclass{article}\pagestyle{empty}\begin{document}$ \overline {\left( {r_g ^2 } \right)} ^{{1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}} $\end{document} . The \documentclass{article}\pagestyle{empty}\begin{document}$ \overline {\left( {r_g ^2 } \right)} ^{{1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}} $\end{document} values evaluated for the mixtures from the experimental data were compared with those estimated from the molecular weights of the components, their weight concentrations, and their \documentclass{article}\pagestyle{empty}\begin{document}$ \overline {\left( {r_g ^2 } \right)} ^{{1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}} $\end{document} values. The method 1,2 was found to be useful for evaluating the microgel content in a sample, but not for \documentclass{article}\pagestyle{empty}\begin{document}$ \overline {\left( {r_g ^2 } \right)} ^{{1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}} $\end{document} values as calculated by Guinier's procedure nor those calculated by Zimm's procedure; the former were low and the latter were even incongruous. A comparative analysis of the theoretical function P −1 (θ)‐versus‐sin 2 (θ/2) and experimental ( Kc / R (θ)) c =0 ‐versus‐sin 2 (θ/2) curves allowed to discuss the effect of the course of these curves at samll angles from 0° to 30° on M̄ w and \documentclass{article}\pagestyle{empty}\begin{document}$ \overline {\left( {r_g ^2 } \right)} ^{{1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}} $\end{document} as determined for the high and low molecular weight polystyrene mixtures in toluene as solvent.

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