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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
1
E 1
+ 2
E 2
+ 3
E 3
E 1 + ν 21
1 2
E 2
[8.8]
ν 32
ν 13
E 3 + ν 23
E 1 + ν 31
3 2
1 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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