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Characterization of branching and gelation

Below the gel point, the system is self-similar on length scales smaller than the correlation length with a power law distribution of molar masses with Fisher exponent r = 5/2 [Eq. (6.78)]. Each branched molecule is a self-similar fractal with fractal dimension 27 = 4 for ideal branched mole-cules in the mean-field theory. The lower limit of this critical behaviour is the average distance between branch points (= ). There are very few [Pg.241]

Above the gel point there is a macroscopic molecule (the gel). The structure of the gel is also self-similar (fractal) in the same range of length scales between the average distance between crosslinks (the linear chain size) and the correlation length  [Pg.241]

The correlation length is the average distance between branch points that are connected to several branches leading to infinity (the boundary of the gel). At/ Ri 2pc (al 1) the gelation regime ends and most of the network [Pg.241]

Refractive index (line) and 15° light scattering (points) detector outputs as functions of elution volume for size exclusion chromatography on a randomly branched polyester sample dissolved in tetrahydrofiiran. Data from [Pg.242]

Knowledge of the concentration c, and weight-average molar mass of each elution volume enables calculation of the weight-average and z-average molar masses  [Pg.242]


See other pages where Characterization of branching and gelation is mentioned: [Pg.241]    [Pg.243]   


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