EXTENDED CHAIN CRYSTAL-GROWTH OF LOW-MOLECULAR MASS POLY(ETHYLENE OXIDE) AND ALPHA,OMEGA-METHOXY POLY(ETHYLENE OXIDE) FRACTIONS NEAR THEIR MELTING TEMPERATURES
Szd. Cheng et al., EXTENDED CHAIN CRYSTAL-GROWTH OF LOW-MOLECULAR MASS POLY(ETHYLENE OXIDE) AND ALPHA,OMEGA-METHOXY POLY(ETHYLENE OXIDE) FRACTIONS NEAR THEIR MELTING TEMPERATURES, Polymer, 33(7), 1992, pp. 1429-1436
For low molecular mass poly(ethylene oxide) (PEO) and alpha,omega-meth
oxy poly(ethylene oxide) (MPEO) fractions, extended chain crystals can
grow when isothermal crystallization temperatures are near their melt
ing temperatures (supercooling DELTA-T = T(m) - T(c) is in the range o
f a few degrees). Experimentally, observed lamellar thicknesses of the
extended chain crystals are constants in this supercooling region. Li
near relationships between crystal growth rate (G) and supercooling (D
ELTA-T) can be observed. Absolute values of the slopes of these relati
onships decrease with increasing molecular length. Additionally, MPEO
fractions generally have higher slope values when compared with their
PEO counterparts. Nevertheless, this difference between PEO and MPEO f
ractions gradually vanishes with increasing molecular length. Extended
chain single lamellar crystals are highly faceted in these temperatur
e regions, and their aspect ratios vary with supercooling as well as m
olecular length. Nucleation theory for the growth of extended chain cr
ystals is applied. The transient chain-end surface free energy, sigma'
, and the lateral surface free energy, sigma, for the PEO and MPEO fra
ctions possess entropic origins. The rough surface growth model is als
o discussed.