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Flory-Huggins-Staverman theory

Equation (9.9), however, only approximately describes the internal dilution of a liquid crystalline copolymer [64]. Here internal means that the diluent is part of the chain and not a second independent component. Nishi and Wang [67] have derived equation (9.10) which describes polymers diluted by polymers. Their extension of the Flory-Huggins-Staverman theory gives the melting point depression ... [Pg.278]

Definition of terms relating to individual macromolecules, their assemblies, and dilute solution.This document includes the recommended definitions for molecular weight, molecular weight averages, distribution functions, radius of gyration, end-to-end-distance vector, the Flory-Huggins-Staverman theory, solution viscosity, scattering of radiation by polymers and polymer solutions, fractionation, separation techniques, and so on. The document on dispersity is an important extension of this recommendation. [Pg.479]

Fractionation by liquid liquid phase separation relies on the molar mass dependence of the distribution coefficient which, in terms of the Flory-Huggins-Staverman theory [8 13] (FHS), reads... [Pg.380]

Parameters related to differences in size and shape and respectively change in internal energy of mixing Entropy correction terms Parameter related to average interaction energy Internal energy of the system Flory s equation of state Flory-Huggins Staverman theory... [Pg.397]

For more than two decades researchers have attempted to overcome the inadequacies of Flory s treatment in order to establish a model that will provide accurate predictions. Most of these research efforts can be grouped into two categories, i.e., attempts at corrections to the enthalpic or noncombinatorial part, and modifications to the entropic or combinatorial part of the Flory-Huggins theory. The more complex relationships derived by Huggins, Guggenheim, Stavermans, and others [53] required so many additional and poorly determined parameters that these approaches lack practical applications. A review of the more serious deficiencies... [Pg.19]

Statistical thermodynamic mean-field theory of polymer solutions, first formulated independently by Flory, Huggins, and Staverman, in which the thermodynamic quantities of the solution are derived from a simple concept of combinatorial entropy of mixing and a reduced Gibbs-energy parameter, the X interaction parameter. [Pg.55]

Besides the earliest theories by Flory (95 ), Huggins (128") and Miller (183 ), all improved theories are concerned with the effect of ring closure of chains on the mixing entropy [Staverman (237) Guggenheim and McGlashan (7) Tompa (21) MCnster (15) and Kurata, Tamura and W atari (756)]. The problem of ring closure is essentially the excluded volume problem. [Pg.286]


See other pages where Flory-Huggins-Staverman theory is mentioned: [Pg.194]    [Pg.194]    [Pg.314]    [Pg.162]    [Pg.557]    [Pg.197]    [Pg.197]    [Pg.210]    [Pg.1307]    [Pg.219]    [Pg.72]   
See also in sourсe #XX -- [ Pg.278 ]

See also in sourсe #XX -- [ Pg.289 ]




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Flory-Huggins

Flory-Huggins theory

Huggins theory

Staverman

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