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ef
c φ and
ef
c φ , accordingly) is adduced. As one can see,
a good enough conformity of the values
(15.13) and (15.14) (
2
ef
c φ , estimated by both methods, is
1
ef
c φ makes up slightly larger
than 20%). Let us note, that the effective value φ cl exceeds essentially the
nominal one, determined according to the Eq. (4.66): within the range of T
= 293÷363K by about 70% and within the range of T = 373÷413K - almost
in three times.
I n Fig. 15.13 , the comparison of experimental and calculated according
to Kerner equation (the Eq. (15.11)) with the Eqs. (15.13) and (15.14) us-
ing values of reinforcement degree by shear modulus G p / G l.m. as a function
of testing temperature T for PC is adduced. As one can see, in this case at
the usage of nanoclusters effective concentration scale (
c φ and
ef
obtained (the average discrepancy of
1
ef
c φ instead of φ cl )
the good conformity of theory and experiment is obtained (their average
discrepancy makes up 6%).
ef
c φ and
FIGURE 15.12
The comparison of nanoclusters effective concentration scale
ef
c φ , calculated according to the Eqs. (15.13) and (15.14), respectively, for PC. A straight
line shows the relation 1:1 [41].
1
2
 
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