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FIGURE 12.3 The dependence of microhardness H v on loosely packed matrix structure
fractal dimension
l.m.
f
d
for epoxy polymers EP-2 (1) and EP-2-200 (2) [9].
The Eq. (12.7) shows, that the condition H v = 0 can be realized for linear
object with dimension d f = d = 1 only (in fact for separate stretched lin-
ear macromolecule [15]), that is, for real solids, having dimension within
the range of 2.0 ÷ 2.95, zero value H v is unattainable. At minimum value
l.m.
f d = 2.0 the magnitude H v = 150 MPa, for loosely packed matrix structure
with the greatest density, that is, in the case, when nanoclusters and loosely
packed matrix structures are undistinguishable, the value H v = 293 MPa.
The loosely packed matrix microhardness
l.m.
v
H
can also be calculated
according to the mixtures rule [1, 8]:
cl
l.m.
( )
HH
=+- ,
f
H
1
f
(12.8)
v
v
cl
v
cl
cl
H is nanoclusters microhardness, by the indicated above reasons
accepted equal to 293 MPa.
In Fig. 12.4 , the dependences of H v and
where
l.m.
v H on K st are adduced. As one
can see, at K st = 0.50 and 1.50 (the least values n c = (4 ÷ 9) × 10 26 m -3 ) the
values H v and
l.m.
v H are close and at higher values in c = (10 ÷14) × 10 26 m -3 in
the case of K st = 0.75 ÷ 1.25 the distinction between H v and
l.m.
v H can reach
80 MPa, that indicates high degree of loosely packed matrix loosening.
 
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