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mensions D cr and d f , one of possible causes of which can be the influence of
d f on local plasticity level (see chapter five) and, hence, on crack boundaries
(fracture surface) roughness degree. In Fig. 8.3, two straight lines are drawn,
giving possible theoretical relation D cr ( d f ). The straight line 1 is drawn in as-
sumption, that the brittle fracture, to which the criterion n = 0.25 (or d f = 2.5,
see the Eq. (1.9)) corresponds [11], is realized at D cr = 1, that is carried out,
and ductile fracture - at n = 0.5, that is, for true rubbers. The straight line 2
as a matter of fact is similar to straight line 1, but it is drawn in assumption
of ductile fracture achievement (sample general yielding) at n = 0.475 [11].
However as the data of Fig. 8.3 show, the value D cr = 2.0 (limiting value D cr )
is reached at d f ≈ 2.72, that is, at the transition from quasibrittle (quasiduc-
tile) fracture to ductile one [11].
FIGURE 8.3 The relation between fractal dimensions of stable crack D cr and polymer
structure d f for PASF samples. The straight lines drawing mode explanations are given in the
text [8].
In Ref. [4], it has been shown that between stress intensity factors (resis-
tance to crack propagation) for fractal crack K I ( D cr ) and smooth one-dimen-
sional cut (i.e., idealized crack with smooth boundaries) K Io the following
relationship exists with precision to a multiplicative constant of order one:
(
)
Kl -
1
D
2
K D
(
)~
cr
,
(8.1)
I
cr
I0 cr
 
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