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Open AccessJournal ArticleDOI

Conformational Entropy Contributions to the Glass Temperature of Blends of Miscible Polymers.

Hans Adam Schneider
- 01 Mar 1997 - 
- Vol. 102, Iss: 2, pp 229-248
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TLDR
Because of negligible contributions of combinatorial entropy, miscibility of polymers is attributed predominantly to favorable (exothermic) enthalpic effects of mixing, i.e., to strong interactions between the blend components, which have to overcome the cohesive forces acting within the components.
Abstract
Because of negligible contributions of combinatorial entropy, miscibility of polymers is attributed predominantly to favorable (exothermic) enthalpic effects of mixing, i.e., to strong interactions between the blend components, which have to overcome the cohesive forces acting within the components. Miscibility of amorphous polymers usually is associated with the presence of a single glass temperature of the blend. Although stronger hetero-contact interactions are thermodynamically required for polymer miscibility, the majority of miscible binary polymer blends exhibit negative deviations of the glass temperature from values predicted by the free volume or flexible bond additivity rules, suggesting a looser packing within those blends. A reasonable explanation assumes that binary hetero-contact formation within the blend may be accompanied by local interchain orientation contributing consequently to conformational entropy changes. The smaller the induced interchain orientation by hetero-contact formation, the larger the mobility in the neighborhood of the contacts and the probability of related conformational entropy changes, causing an equivalent increase of the "free volume" within the blend, i.e., a corresponding decrease of the blend Tg, which finally can be situated below the values predicted by the additivity rules. Vice versa, the corresponding argument will hold for blends with higher interchain orientation induced by intensive exothermic hetero-contact forces.

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References
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Journal ArticleDOI

Ideal copolymers and the second-order transitions of synthetic rubbers. i. non-crystalline copolymers

TL;DR: In this article, the second-order transition temperature of binary copolymers is derived from the two secondorder transition temperatures of the pure polymers and their coefficients of expansion in the glassy and rubbery states.
Journal ArticleDOI

Nature of the Glass Transition and the Glassy State

TL;DR: In this paper, a second-order transition is predicted for linear molecular chains, which occurs at a temperature which is an increasing function of both chain stiffness and chain length and a decreasing function of free volume.
Journal ArticleDOI

Studies in Newtonian Flow. II. The Dependence of the Viscosity of Liquids on Free‐Space

TL;DR: In this article, the viscosity of the liquid normal paraffins can be accurately defined as a simple function of relative free space except for values in the neighborhood of the freezing points of each compound.
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