The rate of crystallization of nylon 6 polymer in bulk form was measured at various temperatures with several kinds of the specimens of different molecular weight (2.6×10
3 to 19×10
4) by applying the method of determining the intensity of depolarized light, proposed by the authors in the preceding papers. The Avrami's constant
n was found to be always 4 except the initial stage of crystallization of the polymer specimen with low molecular weight at higher temperatures, where the value of
n was nearly 6 indicating homogeneous nucleation which would lead to sheaf-like crystal growth.
The crystallization rate 1/
t1/2 is expressed by the intrinsic viscosity [η], and the crystallization temperature
T by the following equation,
where,
n=4: Avrami's constant,
ED([η])=
Evis([η])/ρ([η]): activation energy for the transport of material across the liquid-crystal interface (cal/mol),
Evis ([η])=4.12×10
3 T2/{51.6+
T-
Tg([η])}
2: activation energy for viscous flow (cal/mol),
Tg([η])=581.6-1076/(1.81[η]+13.45)
0.5: glass transition point (°K), ρ([η])=20.2-8.3[η]: ratio of
Evis to
ED, C
3([η])=1/(0.309-0.206[η])-8.5 and
C4([η])=10
5/(0.82-0.52[η])+2.5×10
5: constants independent of
T,
Tm([η]): melting point (°K). 1/
Tm([η])=1/504+6.125×10
-6/[η]
1.435.
Temperature
Tmax at which the crystallization rate becomes maximum, the value of
ED, ρ. activation entropy, included in
C3 for crystallization interfacial free energy and the size of critical nuclei derived from
C4 are all dependent on the molecular weight of polymer.
View full abstract