Civil Engineering Reference
In-Depth Information
where:
ε cu
ultimate strain in confined concrete
ε y
ε y = f y / E s
f y yield strength of longitudinal reinforcing steel
E s modulus of elasticity of longitudinal reinforcing steel
D diameter of reinforced concrete column
D c core diameter according to Figure 4.4
ϕ w bar diameter of helical reinforcement or links
ϕ s bar diameter of longitudinal reinforcing steel.
The equations for determining the theoretically admissible axial load N u and the
associated moment M u according to Jiang [135] are as follows:
yield strain of longitudinal reinforcing steel:
sin 2 ? π ? θ
N u θ ? α 1 ? f cc ? A c ?
1
θ c θ t
? f y ? A s
(7.19)
2 ? π ? θ
!
2
? ξ 1 ? ξ 2 ? ϕ bal
l 0
π
M u N u ?
e 1
sin 3
2
3 ? α 1 ? f cc ? A c ?
D
2 ?
π ? θ
D
2 ?
sin
π ? θ c
sin
π ? θ t
f y ? A s ?
π
π
(7.20)
where:
θ
relative angle describing the position of the stress block in the cross-section:
0 θ 1
α 1
stress block geometry factor according to Equation 7.21
f cc
compressive strength of con ned concrete
A c
gross cross-sectional area of concrete in reinforced concrete column
θ c
relative angle describing the stress distribution in the distributed longitudinal
reinforcing steel subjected to compression: 0 θ c = 1.25 θ 0.125 1
θ t
relative angle describing the stress distribution in the distributed longitudinal
reinforcing steel subjected to tension: 0 θ t =
1.125
1.5
θ
1
f y yield strength of longitudinal reinforcing steel
A s cross-sectional area of longitudinal reinforcing steel
e tot eccentricity of loading according to first-order theory: e tot = e 0 + e i
e 0 intentional eccentricity of loading according to first-order theory
e i additional unintentional eccentricity of loading according to the design codes
ε ju ultimate strain in CF sheet
ε c2 longitudinal strain in concrete subjected to uniaxial compression upon reaching
compressive strength
D diameter of reinforced concrete column
ϕ bal maximum curvature
l 0
buckling length of compression member
ξ 1
factor to allow for the decrease in curvature for a rise in the compressive force N u
beyond N bal according to Equation 7.22
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