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M
a
C
q
critical state
q
C
B
B
yield
ing
pre-
consolidation
c
elastic
p
0
p'
A
shea
r strain
A
p'
C
p'
A
p'
B
p'
C
p'
A
p'
B
0
<
p'
ln p'
A
v
A
v
A
A
B
B
v
B
v
B
b
C
v
C
C
v
C
swelling
swelling
isotropic compression
critical state
isotropic compression
critical state
v
v
Figure 9.2a Principle of the Modified Cam-Clay model; (a) the correspondence of the p-q
space and the v-p space for a hardening stress path A-B-C, (b) the related v-
ln
p space, (c)
hardening behaviour
M
a
B
c
q
critical state
q
B
yielding
C
C
elastic
A
p'
p
0
shea
r strain
A
p'
A
p'
C
p'
C
p'
B
p'
A
p'
B
0
<
p'
ln p'
v
C
v
C
C
C
b
A
A
v
A
v
A
v
B
v
B
B
B
swelling
swelling
isotropic compression
critical state
isotropic compression
critical state
v
v
Figure 9.2b Principle of the Modified Cam-Clay model; (a) the correspondence of the p-q
space and the v-p space for a softening stress path A-B-C, (b) the related v-
ln
p space, (c)
softening behaviour
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