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Summary of branching and gelation

A wide variety of linking processes can lead to the transformation from a liquid to a solid known as gelation. This transition occurs at a particular extent of reaction, p, called the gel point. A rough estimate of the gel point for linking precursor molecules (or monomers) with functionality / is [Pg.244]

This molar mass distribution applies to all polymers below the gel point and above the gel point it applies to the sol fraction. The weight-average molar [Pg.245]

The number-average molar mass stays finite at the gel point and therefore the polydispersity index of the sol diverges at the gel point proportional to Ww. [Pg.245]

At the gel point, the distribution of molar masses is a power law, since M diverges. Above the gel point the system consists of a macroscopic gel, permeated by a polydisperse soup of microscopic molecules (the sol) described by the same self-similar distribution of molar masses. The distribution of molar masses in the sol gets progressively narrower as the reaction proceeds further beyond the gel point, since the characteristic molar mass M decreases. The fraction of the material that is a part of the gel, called the gel fraction Pgd, grows steadily above the gel point  [Pg.245]

Once the extent of reaction reaches approximately twice the gel point, nearly all monomers are attached to the gel and there is essentially no sol fraction remaining. Such well-developed networks are the subject of Chapter 7. [Pg.245]


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