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where A is a constant,
the stress, f the texture parameter, d the
grain size, m (~0.4-0.7) and n (~0.8-2) are constants, and the others have
their usual meaning.
As the dislocation density in a CWSR material is high and, as glide but not
climb is the rate controlling mechanism under reactor conditions, the creep
rate of CWSR is higher than that of recrystallized material as shown in the
fi gures. The creep rate (a) increases with increase in the fl ux, (b) increases
with increase in temperature (contribution by thermal creep predominates
above 400°C), (c) is higher along the rolling direction than the transverse
direction, (d) decreases with fl uence (as radiation hardening sets in) and
(e) depends upon the type of alloy (Nb and Sn content increases creep
resistance). The irradiation creep rates of cold-worked Zr-2.5wt.%Nb alloy
are about one-third of those of cold-worked Zircaloy-2 137 at comparable
temperature, stress and fast neutron fl ux while the creep down of HANA
(High Performance Alloy for Nuclear Applications) alloy (after a dose of 12
MWd/Kg U) is half that for Zircaloy-4. 138
ϕ
the fl ux,
σ
3.9
References
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￿ ￿ ￿ ￿ ￿ ￿
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