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Structural Concrete - Hassoun

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3.9 Singly Reinforced Rectangular Section in Bending 101<br />

For a balanced or an underreinforced section, T = A s f y . Then<br />

(<br />

M n = A s f y d − 1 )<br />

2 a<br />

(3.19)<br />

To get the usable design moment φ M n , the previously calculated M n must be reduced by the capacity<br />

reduction factor, φ,<br />

(<br />

φM n = φA s f y d − a ) (<br />

= φA<br />

2 s f y d −<br />

A )<br />

s f y<br />

1.7f cb<br />

′ (3.19a)<br />

Equation 3.19a can be written in terms of the steel percentage ρ:<br />

Equation 3.20 can be written as<br />

ρ = A s<br />

A<br />

bd s = ρbd<br />

(<br />

φM n = φf y ρbd d − ρbdf ) (<br />

y<br />

1.7f cb<br />

′ = φρf y bd 2 1 − ρf )<br />

y<br />

1.7f c<br />

′<br />

(3.20)<br />

φM n = R u bd 2 (3.21)<br />

where<br />

(<br />

R u = φρf y 1 − ρf )<br />

y<br />

1.7f c<br />

′ (3.22)<br />

The ratio of the equivalent compressive stress block depth, a, to the effective depth of the section,<br />

d, can be found from Eq. 3.15:<br />

0.85f ′ cab = ρbdf y<br />

a<br />

d =<br />

ρf y<br />

0.85f ′ c<br />

(3.23)<br />

3.9.2 Upper Limit of Steel Percentage<br />

The upper limit or the maximum steel percentage, ρ max , that can be used in a singly reinforced<br />

concrete section in bending is based on the net tensile strain in the tension steel, the balanced steel<br />

ratio, and the grade of steel used. The relationship between the steel percentage, ρ, in the section<br />

and the net tensile strain, ε t , is as follows:<br />

( )<br />

0.003 + fy ∕E s<br />

ε t =<br />

− 0.003 (3.24)<br />

ρ∕ρ b<br />

For f y = 60 ksi, and assuming f y /E s = 0.002,<br />

( )<br />

0.005<br />

ε t = − 0.003 (3.25)<br />

ρ∕ρ b<br />

These expressions are obtained by referring to Fig. 3.12. For a balanced section,<br />

Similarly, for any steel ratio, ρ,<br />

c b = a b<br />

β 1<br />

=<br />

c =<br />

A sb f y<br />

0.85f cbβ ′ = ρ b f y d<br />

1 0.85f cβ ′ 1<br />

ρf yd<br />

0.85f ′ cβ 1<br />

and<br />

c<br />

c b<br />

= ρ ρ b

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