Geoscience Reference
In-Depth Information
8.2. Study of the second-order work criterion
8.2.1.
Analytical study
Inthissectionwepresentadetailedanalysisofcondition[8.3]givenintheintroduction.
In the following we denote by
N
the matrix linking strain rate to stress rate, such as:
dε = N dσ
[8.4]
and by
M
the inverse matrix as
M = N
−1
. In principal axes and for a given tensorial
zone
1
,
N
takes the following form:
⎡
⎤
1
E
1
−
ν
21
E
2
−
ν
31
E
3
⎣
⎦
−
ν
12
E
1
1
E
2
−
ν
32
E
3
N =
[8.5]
−
ν
13
E
1
−
ν
23
E
2
1
E
3
With these notations, the shallow link between the second-order work criterion and
the condition given by:
det
N
s
=0
[8.6]
is also described.
N
s
is the symmetric part of
N
. Using the constitutive relation, we
obtain:
d
2
W =0 ⇔
t
dσ N
s
dσ =0
[8.7]
For all incrementally piece-wise linear models, equation [8.7] can be developed in
the following manner in the principal stress rate space:
ν
12
dσ
1
E
1
+
dσ
2
E
2
+
dσ
3
E
3
E
1
+
ν
21
−
dσ
1
dσ
2
E
2
[8.8]
ν
32
ν
13
E
3
+
ν
23
E
1
+
ν
31
−
dσ
3
dσ
2
−
dσ
1
dσ
3
=0
E
3
E
2
This expression describes an elliptical cone, but real solutions depend on the sign
of the eigenvalues of the quadratic form: the cone can be degenerated. After quadric
reduction, equation [8.8] takes the following form in the diagonal base:
λ
1
X
2
+ λ
2
Y
2
+ λ
3
Z
2
=0
[8.9]
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