Civil Engineering Reference
In-Depth Information
(
)
2
1
2
bh y
yh
+
(
)
0
Nbhy
=
+
σ
=
σ
[4.13a]
c
01
3
(
)
2
0
1
6
2
σ
h
0
(
)
3
NdNb h
=
=
y
3
σ
[4.13b]
t
t
0
3
k
y
The internal moment M c caused by N c and the internal moment M t caused
by N t may be derived and expressed as follows:
(
)
2
(
)
1
6
bh y
+
h y
hy
2
(
)
(
)
0
0
Mb h
=−
+
y
2
h
y
σ
=
σ
[4.14a]
c
0
0
1
3
(
)
6
0
1
12
σ
h
0
(
)
3
(
)
MydNb h
=
=
y
42
h
+−
y
3
hy
+
σ
[4.14b]
t
t
0
0
0
3
k
y
Based on the equilibrium condition of the section, the following equa-
tions may be established:
NN
c
=
[4.15a]
t
NL
MM M
=+= 4
[4.15b]
c
t
where M is the external bending moment.
From Eqs [4.12]-[4.15], the effective stress
˜ 3 and degree of damage
D of the extreme tension fi bre at the bottom of the beam may be derived
and expressed as follows:
σ
˜ 1 ,
σ
(
)
6
hy h y
hy
+
0
0
σ 1
=
k
[4.16]
(
)
3
0
hy
hy
6
0
σ 3
=
k
[4.17]
(
)
2
0
==
σ 3
hy
hy
6
￿ ￿ ￿ ￿ ￿ ￿
0
D
[4.18]
(
)
2
k
0
As cracks form in the tensile zone of a concrete beam, failure occurs
and the load bearing capacity of the beam will depend on the effective
tensile stress
˜ 3 . When the effective tension stress of concrete
˜ 3 reaches
σ
σ
k
the critical cracking stress
σ
σσ
==
, then a beam without
cr
3
cr
2
reinforcement will fail. From Eqs [4.13] and [4.14], the displacement of
IGNA ( y 0 ) cr and N cr may also be described as follows:
y
() =− .
0 102
h
[4.19]
0
cr
0 944
.
kbh
L
2
N
=
[4.20]
cr
 
Search WWH ::




Custom Search