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Vogel-Fulcher-Tammann-Hesse equation temperature

A Vogel-Fulcher-Tammann-Hesse equation can be used to characterize the temperature dependence of the relaxation times for these six different degrees of cure, 0.70, 0.75, 0.80, 0.825, 0.90, and 0.95 ... [Pg.143]

Inserting Eq. (4-16) into Eq. (4-10) gives the Vogel-Fulcher-Tammann-Hesse equation, where now the Vogel temperature To = U/A.2R can be computed from the energy U between trans and gauche states. The values of U obtained indirectly in this way, using... [Pg.204]

Vogel-Fulcher-Tammann-Hesse equation or temperature vinyl alcohol... [Pg.714]

Fig. 19. Temperature dependence of the shift factors of the viscosity (T), terminal dispersion ( ), and softening dispersion (0) of app from Ref. 73. The temperature dependence of the local segmental relaxation time determined by dynamic light scattering ( ) (30) and by dynamic mechanical relaxation (o) (74). The two solid lines are separate fits to the terminal shift factor and local segmental relaxation by the Vogel-Fulcher-Tammann-Hesse equation. The uppermost dashed line is the global relaxation time tr, deduced from nmr relaxation data (75). The dashed curve in the middle is tr after a vertical shift indicated by the arrow to line up with the shift factor of viscosity (73). The lowest dashed curve is the local segmental relaxation time tgeg deduced from nmr relaxation data (75). Fig. 19. Temperature dependence of the shift factors of the viscosity (T), terminal dispersion ( ), and softening dispersion (0) of app from Ref. 73. The temperature dependence of the local segmental relaxation time determined by dynamic light scattering ( ) (30) and by dynamic mechanical relaxation (o) (74). The two solid lines are separate fits to the terminal shift factor and local segmental relaxation by the Vogel-Fulcher-Tammann-Hesse equation. The uppermost dashed line is the global relaxation time tr, deduced from nmr relaxation data (75). The dashed curve in the middle is tr after a vertical shift indicated by the arrow to line up with the shift factor of viscosity (73). The lowest dashed curve is the local segmental relaxation time tgeg deduced from nmr relaxation data (75).
Unfortunately, reliable experimental estimates of the configurational entropy are unavailable to enable explicit application of the AG model for polymer fluids. Instead, the temperature dependence of t in polymer melts is often analyzed in terms of the empirical Vogel-Fulcher-Tammann-Hesse (VFTH) equation [103],... [Pg.153]

It appears, however, that the mode-coupling theory is not able to explain some of the most significant slow-relaxation processes of these more complex glass formers. In particular, it cannot explain the success of the Vogel-Fulcher-Tammann-Hesse (VFTH) equation for the temperature-dependence of the relaxation time near the glass transition. The mode-coupling theory predicts instead a power-law dependence of the longest relaxation... [Pg.216]

In the a-process, the viscosity and consequently the relaxation time increase drastically as the temperature decreases. Thus, molecular dynamics is characterized by a wide distribution of relaxation times. A strong temperature dependence presenting departure from linearity or non-Arrhenius thermal activation is present, owing to the abrupt increase in relaxation time with the temperature decrease, thus developing a curvature near T. This dependence can be well described by the Vogel-Fulcher-Tammann-Hesse (VFTH) equation [40, 41], given by Equation 2.1 ... [Pg.17]

If the free volume shows a linear expansion with the temperature, Vf = Ef(T- T ), where Ef=dVf IdT is its specific thermal expansivity and Tq < Tg is the temperature where the (linearly extrapolated) free volume disappears, one obtains from Eq. (11.7) the well-known Vogel-Fulcher-Tammann-Hesse (VFTH) equation [Vogel, 1921 Fulcher, 1925 Tammann and Hesse, 1926] ... [Pg.447]

The average a-relaxation time of polymers exhibit a dramatic sensitivity to temperature as Tg is approached. Figure 3.1b shows the temperature dependence of the average a-relaxation time as a function of inverse temperature normalized to Tg for an amorphous polymer. The temperature dependence of the average a-relaxation (or viscosity) can be well described by the Vogel-Fulcher-Tammann-Hesse (VFTH) equation [64-66]... [Pg.51]

The temperature dependence of the ionic conductivities for the HBP-SA and the HBP-SA-co-HBP-Ac membrane in the temperature range of 60-150°C is shown in Fig. 13.1. Ionic conductivity data of the polymer and electrolyte membrane are typically interpreted using the Vogel-Tamman-Fulcher (VTF) equation (Vogel, 1921 Tammann and Hesse, 1926 Fulcher, 1925) ... [Pg.529]


See other pages where Vogel-Fulcher-Tammann-Hesse equation temperature is mentioned: [Pg.194]    [Pg.324]    [Pg.455]    [Pg.499]    [Pg.518]    [Pg.10]    [Pg.94]    [Pg.30]    [Pg.421]    [Pg.511]    [Pg.121]    [Pg.236]    [Pg.348]    [Pg.551]   
See also in sourсe #XX -- [ Pg.261 , Pg.262 , Pg.447 , Pg.448 , Pg.454 , Pg.458 , Pg.533 , Pg.539 , Pg.561 , Pg.584 ]




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Fulcher equation

Hessing

Temperature equation

Vogel

Vogel-Fulcher

Vogel-Fulcher temperature

Vogel-Fulcher-Tammann temperature

Vogel-Fulcher-Tammann-Hesse

Vogel-Fulcher-Tammann-Hesse equation

Vogel-Tammann-Fulcher equation

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