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Relaxation time melts, molar mass

Recall that Fig. 9.3 showed the linear viscoelastic response of a polybutadiene melt with MjM = 68. The squared term in brackets in Eq. (9.82) is the tube length fluctuation correction to the reptation time. With /i = 1.0 and NjN = 68, this correction is is 0.77. Hence, the Doi fluctuation model makes a very subtle correction to the terminal relaxation time of a typical linear polymer melt. However, this subtle correction imparts stronger molar mass dependences for relaxation time, diffusion coefficient, and viscosity. [Pg.385]

Consider a PDMS melt with molar mass A/ = 6 X 10 g mol . The relaxation time of a Kuhn monomer is tq — 10 s. The molar mass of a Kuhn monomer is Mo = 381g moC and the molar mass of an entanglement strand is jWg 12000g mol ... [Pg.404]

Reptation involves a one-dimensional (head-first) diffusion of the polymer in whidi lateral motion of the diain is restricted as though the chain were emfined to a tube whose effective dimensions reflect the mean entanglement spadng in the polymer melt It is widely appreciated that for reptating chains, the dqrendence of the centre-of-mass diffusion coefiBcient on molar mass (Af) is Dcm oc who eas for Rouse chains, D a oc M in addition, the melt viscosity (and terminal relaxation time) increase as for entangled chains [37]. [Pg.669]

We have already met such a molar mass dependence in Eqs. (6.119) and (6.120), when formulating the average viscoelastic relaxation time r of polymer melts. Roughly speaking, f gives the time required by a chain for a complete conformational reorganization. This also implies a full reorientation of the end-to-end distance vector of the chain. This is exactly this motion that shows up in the dielectric normal mode. [Pg.265]

Equation (8.96) provides a description of the normal mode, giving the relaxation strength as well as the relaxation time. Notice in particular that the observed molar mass dependence of Tnm for non-entangled melts as shown in Fig. 6.22,... [Pg.332]

Gpi denotes the plateau modulus and Tq, is the mean relaxation time of the Rouse mode part, agreeing with the mean relaxation time of a Rouse system of chains with Nr equal to F7r,c- Because the first term on the right-hand side of Eq. (8.117) is constant, for the molar mass dependence of the viscosity of entangled melts we obtain the expression... [Pg.338]


See other pages where Relaxation time melts, molar mass is mentioned: [Pg.573]    [Pg.45]    [Pg.387]    [Pg.704]    [Pg.258]    [Pg.65]    [Pg.252]    [Pg.180]    [Pg.365]    [Pg.37]    [Pg.206]    [Pg.77]    [Pg.80]    [Pg.105]    [Pg.211]    [Pg.381]   


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Molar mass

Molarity molar masses

Relaxation melting

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