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)l.m.f150
f
FIGURE 12.2
The dependence of loosely packed matrix structure fractal dimension
d
on cross-linking density n c for epoxy polymers EP-2 (1) and EP-2-200 (2) [9].
It can be assumed that epoxy polymers structure loosely packed matrix
sustains the main load in indentor pressing process as the least stiff its com-
ponent. Its dimension
)l.m.f150
f
d
can be calculated according to the mixtures rule
[9]:
dd
=+- ,
cl
f
d
)l.m.f150
(1
f
)
(12.6)
f
f
cl
f
cl
where c φ is nanoclusters fractal dimension, j cl is their relative fraction.
The value
cl
f d is accepted equal to the greatest for real solids dimension
(~2.95 [14]) in virtue of their dense package [10] and the value j cl can be
calculated with the help of the Eq. (1.12).
In Fig. 12.2, the dependence of
)l.m.f150
f
d
on cross-linking density n c increase
results to )l.m.f150
f d reduction or loosely packed matrix structure loosening. This
effect should be reflected on the value H v , which is confirmed by the data of
Fig. 12.3 , on which the dependence of H v on
)l.m.f150
f d for the considered epoxy
polymers is adduced. As one can see, the linear correlation H v (
)
)l.m.f150
f
is ob-
d
)l.m.f150
tained, showing H v growth at
f d increase., that is, at loosely packed matrix
structure densification. The indicated correlation can be described analyti-
cally by the following empirical equation [9]:
( )
)l.m.f150
f
H
=
150
d
- , MPa.
1
(12.7)
v
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