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Molecular Cooperativity in the Glass Transition

The fact that the relaxation times associated with the glass-rubber transition and the secondary relaxations are independent of molecular weight suggests [Pg.468]

The dynamics of polymers may be interpreted by assuming the existence of domains. At high temperature (T Tg), each domain is occupied by a single conformer and the interactions between neighboring segments or conformers are considered to be negligible. Once the potential barrier is crossed, conformers relax independently of their neighbors. Each domain [Pg.469]

Statistical mechanical principles suggest that the conformational entropy Sc of I mol of conformers occupying domains is given by [Pg.470]

This expression indicates that the size z is proportional to the reciprocal of the conformational entropy. [Pg.471]

The probability for a conformer to relax is / = exp(-Ag/i T), where Ag is the free energy barrier, while the probability that the z conformers of the same domain relax simultaneously is given by [Pg.472]


See other pages where Molecular Cooperativity in the Glass Transition is mentioned: [Pg.454]    [Pg.468]   


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