Civil Engineering Reference
In-Depth Information
c
(
ρ = ρ t ), both the angle
β
and the concrete shear stress
τ
12 are equal to zero. With increasing
12 are increased. An increase of
12 reduces the compressive capacity
ρ t ratio, both
β
and
τ
τ
of the concrete struts through the reduction of f 3 (
β
) and, in turn, the softening coefficient
ζ
.
Substituting f 3 (
β
) into Equation (6.46), the softened coefficient
ζ
becomes:
5
9
1
8
f c
.
1
| β |
24
ζ =
0
.
1
(6.52)
+
400¯
ε 1
In the fixed angle theory,
β
can be calculated from the three strains
ε 1 ,
ε 2 and
γ 21 using the
compatibility equation:
2 tan 1
1
γ 12
β =
(6.53)
(
ε 1 ε 2 )
Equation (6.53) can also be derived from the Mohr strain circle, as will be shown later in
Figure 6.22(b).
6.1.8 Smeared Stress-Strain Relationship of Concrete in Tension
6.1.8.1 Smeared Stress
c
1
ε 1 of Concrete
In the measured Mohr circle for concrete stresses, as shown in Figure. 6.6, it can be seen that
the tensile stress of concrete
σ
and Smeared Strain ¯
c
1
c
σ
is small compared with the compressive stress
σ
2 , but not
c
zero. This stress
1 is an uniform tensile stress of concrete, representing the stiffening of the
steel bars by concrete in tension.
Figure 6.11 shows a typical tensile stress - strain curve of concrete. The curve consists of
two distinct branches. Before cracking the stress - strain relationship is essentially linear. After
cracking, however, a drastic drop of strength occurs and the descending branch of the curve
becomes concave. In the descending branch, the concrete is cracked and the concept of concrete
tensile stress
σ
1 and concrete tensile strain ¯
σ
ε 1 are quite different from those before cracking.
1 is defined as the smeared (or average ) concrete tensile stress and ¯
σ
ε 1 is the smeared (or
average ) concrete tensile strain. These terms will be elaborated in Section 6.1.8.2.
Based on the tests of 35 full-size panels, Belarbi and Hsu (1994) and Pang and Hsu (1995)
proposed the following analytical expressions for the
1
σ
ε 1 curve:
Ascending branch (¯
ε 1 ε cr )
1
σ
=
E c ¯
ε 1
(6.54)
where:
where
E c =
modulus of elasticity of concrete, taken as 3875 f c (MPa), where f c
and f c
are in
MPa;
ε cr =
cracking strain of concrete, taken as 0.00008 mm/mm,
Descending branch (¯
ε 1 cr )
f cr ε cr
¯
0 . 4
c
1
σ
=
(6.55)
ε 1
31 f c (MPa).
where f cr =
cracking stress of concrete, taken as 0
.
 
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