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max
min
r
-
r
,
(15.33)
D
=
max
r
where ρ max and ρ min are the greatest and the smallest density values. This
estimation gives ∆ρ ≈ 0.01. This value can be reasonable for free volume in-
crease, which is necessary for loosely matrix devitrification (accounting for
closeness of T and T ), but it is obviously small if to assume as real micro-
cracks formation. As the experiments have shown, REP extrusion at ε e > 0.52
is impossible owing to specimen cracking during extrusion process. This
allows to suppose that value ε e = 0.52 is close to the critical one. Therefore,
the critical dilatation ∆δ cr value, which is necessary for microcracks cluster
formation, can be estimated as follows [40]:
(
)(
)
21
+
n
2 3
-
n
,
(15.34)
D= -
d
cr
11
19
n
where n is Poisson's ratio.
FIGURE 15.32 The dependence of specimens density ρ on extrusion strain ε e for extruded
(1) and annealed (2) REP [62].
Accepting the average value n ≈ 0.35, we obtain ∆δ cr = 0.60, that is essen-
tially higher than the estimation ∆ρ made earlier. These calculations assume
that ρ decrease at ε e = 0.43 and 0.52 is due to instable nanoclusters decay and
to corresponding REP structure loosening.
 
 
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