Mcm. Vandersanden et Heh. Meijer, DEFORMATION AND TOUGHNESS OF POLYMERIC SYSTEMS .3. INFLUENCE OF CROSS-LINK DENSITY, Polymer, 34(24), 1993, pp. 5063-5072
In part 1 of this series the phenomenon of a critical ligament thickne
ss (ID(c)) below which brittle polymers become ductile was investigate
d for polystyrene (PS). Using the thermoplastic polystyrene-poly(2-6-d
imethyl-1,4-phenylene ether) (PS-PPE) model system, it was demonstrate
d in part 2 of this series that the absolute value of ID(c) as well as
the maximum toughness (i.e. maximum strain to break) was dependent on
the network density of the polymer used. In this study the toughness
and ID(c) of crosslinked thermosetting polymers were investigated usin
g epoxides based on the diglycidyl ether of bisphenol A as a model sys
tem. The crosslink density (nu(c)) is varied between values comparable
with (nu(c) = 9 x 10(25) chains m-3), up to values much higher than (
nu(c) = 235 x 10(25) chains m-3), the entanglement density in the ther
moplastic PS-PPE system. The maximum macroscopic toughness proportiona
l to the strain to break (lambda(macr)) or given by the slow-speed fra
cture toughness (G(Ic)) and the notched high-speed tensile toughness (
G(h)) of core-shell rubber-modified epoxides uniquely increases with a
n increasing molecular weight between crosslinks (M(c)). Only by using
extreme testing conditions (notched high-speed impact testing), could
the ID(c) of a limited range of epoxides be determined: 0.21 mum (nu(
c) = 9 x 10(25) chains m-3) less-than-or-equal-to ID(c) less-than-or-e
qual-to 0.29 mum (nu(c) = 14 x 10(25) chains m-3). Both the experiment
ally determined values of ID(c) and the toughness of the epoxides comp
are well with the values determined for the entangled thermoplastic PS
-PPE model system in the same range of network densities, elucidating
the principal similarity of the influence of entanglements and crossli
nks on the deformation processes. Good agreement was observed between
the experimentally determined values of ID(c) of the epoxides and the
values predicted by the simple model introduced in part 2 of this seri
es.