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then
exp
i
(
q
+
p
)
r
=1
,
if
q
+
p
=0
,
(10. A.4)
exp
i
(
q
+
p
)
r
=0
,
if
q
+
p
=0
.
Substituting
δϕ
(
q
) from (10. A.2) we have
+
q
B
l
(
q
)
j
i
=
σ
ik
e
k
δσ
il
(
−
q
)
q
i
q
m
e
l
q
l
(10. A.5)
σ
im
which is the basis for calculation of the effective conductivity
σ
eff
ik
.
References
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