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Structural a-Relaxation Dynamic Structure Factor

The dynamic process driving the decay of the interchain correlations in glassforming polymers is the structural a-relaxation. The direct microscopic obser- [Pg.72]

/Qj ax( ) is a generalized Debye-Waller factor giving account for the decay of the correlations at faster times. In the framework of the MCT it is also called non-ergodicity factor. The characteristic timescale r (T) is the structural relaxation time and (3 is the stretching parameter (0 jS l). [Pg.73]

The scaling the functional shape hardly depends on temperature. Curves corresponding to different temperatures superimpose in a single master curve when they are represented against a reduced time variable that includes a T-dependent shift factor. [Pg.73]

These two features are demonstrated in Fig. 4.3 for 1,4-polybutadiene (PB), in Fig. 4.4 for polyisobutylene (PIB) and atactic polypropylene (aPP), in Fig. 4.5 for polyurethane (PU) and poly(vinyl chloride) (PVC) and in Fig. 4.6 for poly(vinyl ethylene) (1,2-polybutadiene, PVE) (see Table 1.1 for microstructure). In each case 5pair(Qmax 0/Spair(Qmax 0) is Very well described by the KWW laws. [Pg.74]

At this point the question arises whether the feature usually termed as universality is also fulfilled do the timescales deduced from the investigation of different correlators in the a-relaxation regime show the same temperature [Pg.76]


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A-Relaxation

A. Dynamics

Dynamic structure factor

Dynamical structure factor

Relaxation dynamics

Relaxation factor

Structural dynamics

Structural factors

Structural relaxation

Structure dynamics

Structure factor

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