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(a)
0
d = fixed
-10
C -
C +
-20
N +
·
·
ε N + < ε C +
ε C - < ε N -
ε N + < ε C -
N (A ¬
·
·
-30
·
·
·
·
ε N - < ε N +
N (B α - )
ε C - < ε N +
C (B α - )
N -
·
·
·
·
ε C + < ε C -
C (A ¬ + )
+
)
-40
1.0
1.5
2.0
2.5
( T m / T )
(b)
0
-10
C -
C +
-20
N +
·
·
·
·
ε N - < ε N +
ε C + < ε C -
ε N - > ε C +
N (B α + )
ε N - < ε N +
ε C + < ε C -
ε C - > ε N -
C (A ¬ + )
·
·
·
·
-30
N -
·
·
·
·
-40
￿ ￿ ￿ ￿ ￿ ￿
1.0
1.5
2.0
2.5
( T m / T )
3.26 Transitions in creep mechanisms in ceramics for transport paths.
Suggested by (a) Gordon and (b) Chokshi.
as demonstrated by Li et al . 107 As noted in Fig. 3.27a, the stress exponent
decreases with increasing stress.
By introducing a friction stress (
0 ) the creep behavior of this alloy could
be described by the following equation:
τ
n
Q
RT
ττ
0
exp
γ
[3.62 ]
A
=
G
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