Chemistry Reference
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Table 4.2  Parameters of Eq. 4.63 obtained [ 90 ] by its fitting to numerical f (α) data for equation
of random scission
Code
L
c
n
m
L2
2
1.204
1.119
0.4
L3
3
2.080
1.057
0.396
L4
4
2.929
1.039
0.394
L5
5
3.767
1.030
0.391
L6
6
4.597
1.024
0.389
L7
7
5.422
1.020
0.388
L8
8
6.242
1.017
0.386
(4.63)
m
n
f
()
ααα
=
c
(
1
) .
Table 4.2 collects the fit parameters of Eq. 4.63.
The aforementioned approach has been tested by using data on the thermal deg-
radation of poly(butylene terephthalate) (PBT), the polymer that degrades via ran-
dom scission. Figure 4.32 presents the f (  ʱ ) plots reduced to ʱ = 0.5 for experimental
data as well as some theoretical models, including the models of random scission
(L2 and L8) and some solid-state reaction models. Clearly, the random scission
models provide much better fit to the experimental data than any of the solid-state
reaction models that makes a good case for the viability of the derived f (  ʱ ) models
of random scission.
Fig. 4.32  Comparison of the f (  ʱ ) data for the thermal degradation of PBT (  points ) against theo-
retical models (  lines ). L2 and L8 represent the random scission models with L equal to 2 and 8,
respectively. (Reproduced from Sanchez-Jimenez et al. [ 90 ] with permission of Elsevier)
 
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