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Chain Connectivity and Conformational Variability of Polymers: Clues to an Adequate Thermodynamic Description of Their Solutions, 1
Author(s) -
Bercea Maria,
Cazacu Maria,
Wolf Bernhard A.
Publication year - 2003
Publication title -
macromolecular chemistry and physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.57
H-Index - 112
eISSN - 1521-3935
pISSN - 1022-1352
DOI - 10.1002/macp.200350001
Subject(s) - flory–huggins solution theory , dilution , chemistry , virial coefficient , polymer , molar mass , chain (unit) , thermodynamics , function (biology) , generalization , molecule , chemical physics , physics , mathematics , mathematical analysis , organic chemistry , quantum mechanics , evolutionary biology , biology
This is the first of two parts investigating the Flory‐Huggins interaction parameter, χ , as a function of composition and chain length. Part 1 encompasses experimental and theoretical work. The former comprises the synthesis of poly(dimethylsiloxane)s with different molar mass and the measurements of their second osmotic virial coefficients, A 2 , in solvents of diverse quality as a function of M via light scattering and osmotic pressures. The theoretical analysis is performed by subdividing the dilution process into two clearly separable steps. It yields the following expression for χ o , the χ value in range of pair interaction: χ o  =  α  −  ζ   λ . The parameter α measures the effect of contact formation between solvent molecules and polymer segments at fixed chain conformation, whereas the parameter ζ quantifies the contributions of the conformational changes taking place in response to dilution; ζ becomes zero for theta conditions. The influences of M are exclusively contained in the parameter λ The new relation is capable of describing hitherto incomprehensible experimental findings, like a diminution of χ o with rising M . The evaluation of experimental information for different systems according to the established equation displays the existence of a linear interrelation between ζ and α . Part 2 of this investigation presents the generalization of the present approach to solutions of arbitrary composition and discusses the physical meaning of the parameters in more detail.Conformational response, ζ , as a function of α , the interaction parameter for fixed conformation.

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