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(a)
(b)
B 1
C 1
B 2
C 2
m
V
D 1
D 2
V cr
A 2
A 1
O
τ
O
θ
-V cr
( m t , θ t )
( V t , τ t )
Figure 4.15 Loading branches: (a) Bending behavior; (b) Shear behavior.
(a)
(b)
V
m
E 1
E 2
G 2
G 1
V cr
J 2
H 2
τ
O
θ
O
F 2
F 1
H 1
-V cr
( m t , θ t )
( V t , τ t )
Figure 4.16 Unloading branches: (a) Bending behavior; (b) Shear behavior.
place. While for the shear behavior, the tangent stiffness for pre-yield cracked unloading
branches E 2 F 2 can be calculated by
= k s τ τ cr
τ y τ cr
E 2 F 2
s
α
ð
k s k s 2
Þ
ð4 : 104Þ
where k s is the slope connecting origin to the crack point as shown in Figure 4.16(b); k s 2 is
the slope connecting the yield point to the crack point in the opposite side; τ is the maximum
deformation attained in the loading direction and is also where unloading takes place. However,
the tangent stiffness α s for the post-yield unloading branch G 2 H 2 should be computed accord-
ing to components above and below the cracking shear capacity V cr . Then, the tangent stiffness
α s above the cracking shear level is given by Eq. (4.105), and below the cracking shear level by
Eq. (4.106). The tangent stiffnesses α 00 f and α 00 s of the RH and SH behaviors can be calculated
according to Eq. (4.5).
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