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Rouse theory viscoelastic spectrum

Entanglements among component-two s chains will eventually occur as W2 increases above a certain point. As they occur, the constraint effect due to entanglement will render the spectrum in the low-frequency region where the main viscoelastic response of component two occurs no longer described by the Rouse theory. Assuming that entanglements never did occur to... [Pg.228]

Chompff and Duiser (232) analyzed the viscoelastic properties of an entanglement network somewhat similar to that envisioned by Parry et al. Theirs is the only molecular theory which predicts a spectrum for the plateau as well as the transition and terminal regions. Earlier Duiser and Staverman (233) had examined a system of four identical Rouse chains, each fixed in space at one end and joined together at the other. They showed that the relaxation times of this system are the same as if two of the chains were fixed in space at both ends and the remaining two were joined to form a single chain with fixed ends of twice the original size. [Pg.89]

Thirion (239a) has suggested that the plateau and terminal regions are the result of diffuse interchain interactions in a viscoelastic medium. He obtains a modified Rouse spectrum by replacing the subchain frictional coefficient by a time dependent micro-memory function. The theory is partly phenomenological since the memory function is not specified. However, reasonable choices lead to forms for G (co) and G"(o>) which are similar to those observed experimentally. [Pg.93]


See other pages where Rouse theory viscoelastic spectrum is mentioned: [Pg.83]    [Pg.130]    [Pg.203]    [Pg.211]    [Pg.213]    [Pg.218]    [Pg.228]    [Pg.233]    [Pg.272]    [Pg.301]    [Pg.330]    [Pg.112]    [Pg.190]    [Pg.48]    [Pg.72]    [Pg.50]   


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