CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beams
Reinforced Concrete Beams
] Mathematical modeling of reinforced concrete is essential to civil engineering
] Mathematical modeling of reinforced concrete is essential to civil engineering
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Concrete as a material Concrete in a structure
Stress distribution in a reinforced concrete beam
Reinforced Concrete Beams
Reinforced Concrete Beams
] Mathematical modeling of reinforced concrete is essential to civil engineering
] Mathematical modeling of reinforced concrete is essential to civil engineering
Blast failure of a reinforced concrete wall Geometric model a reinforced concrete bridge
Reinforced Concrete Beams ] Mathematical modeling of reinforced concrete is essential to civil engineering
Blast failure of a reinforced concrete wall
Reinforced Concrete Beams ] Mathematical model for failure in an unreinforced concrete beam
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beams ] In the reinforced concrete beam project, there are three different failure mode we need to investigate
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Reinforced Concrete Beams ] First, lets consider the loading of the beam
P
P
P/2
Reinforced Concrete Beams ] The purpose of RC is the reinforcement of areas in concrete that are weak in tension
P/2
Reinforced Concrete Beams ] Let’s look at the internal forces acting on the beam and locate the tension zones
P
P
∑F
P/2
P/2
Reinforced Concrete Beams ] The shear between the applied load and the support is constant V = P/2
P/2
P/2
P/2
V
=
P 2
−V
⇒ V =
P 2
P/2
Reinforced Concrete Beams ] The shear between the applied load and the support is constant V = P/2
P/2
P/2
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beams ] The shear between the applied load and the support is constant V = P/2
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Reinforced Concrete Beams ] Let’s look at the internal moment at section between the supports and applied load
] The shear force V = P/2 is constant between the applied load and the support
P
P
∑M = 2 x
M
X max = 8 inches
P/2
P/2
P/2
Reinforced Concrete Beams ] Let’s look at the internal moment at section between the supports and applied load
x
P/2
M = P/2 4P
(in lbs )
Reinforced Concrete Beams ] The top of the beam is in compression and the bottom of the beam is in tension
] The bending g moment is the internal reaction to forces which cause a beam to bend. Compression force on the upper Bending moment distributed on part of the concrete beam
MCthe cut surface
] Bending moment can also be referred to as torque
T
P
Tension force on the lower part of the concrete beam
2
Reinforced Concrete Beams ] To model the behavior of a reinforced concrete beam we will need to understand three distinct regions in the beam. ] Two are illustrated below; the third is called shear. shear
Reinforced Concrete Beams ] We need models to help us with compression, tension, and shear failures in concrete
P
Bending moment distributed on
cut surface MCthe Compression
P 2
T
Tension
Tension
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beams ] We need models to help us with compression, tension, and shear failures in concrete
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Reinforced Concrete Beams ] We need models to help us with compression, tension, and shear failures in concrete
P
P
Compression
Shear
Reinforced Concrete Beams ] We need models to help us with compression, tension, and shear failures in concrete
Shear
Reinforced Concrete Beams ] Compression and tension failures in a reinforced concrete beam
P
Shear
Compression Tension
Shear
Reinforced Concrete Beams ] Compression and tension failures in a reinforced concrete beam
Reinforced Concrete Beams ] Shear failure in a reinforced concrete beam
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beams
Whitney Rectangular Stress Distribution
] Shear failure in a reinforced concrete beam
] In the 1930s, Whitney proposed the use of a rectangular compressive stress distribution
Whitney Rectangular Stress Distribution
Whitney Rectangular Stress Distribution
] In the 1930s, Whitney proposed the use of a rectangular compressive stress distribution k3f’c
b
0.85f’c
k2 x
C
c
] Assume that the concrete contributes nothing to the tensile strength of the beam
0.5a
d
h
As
T
k3f’c
P
d
0.85f’c
k2 x
C
c
Shear
Compression Tension T
Compression Tension
Shear T
] The height of the stress box, a, is defined as a percentage of the depth to the neural axis
C
0.85f’c
c
0.5a
C
a
Shear T
C
Whitney Rectangular Stress Distribution
0.5a
a
0.5a
a
T
] Assume that the complex distribution of compressive stress in the concrete can be approximated by a rectangle b
Shear
0.85f’c
k2 x
C
T
Whitney Rectangular Stress Distribution
As
P
c
As
h
k3f’c
b
C
a
d
h
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T
a = β1c
CIVL 1112
Introduction to Reinforced Concrete Beams
Whitney Rectangular Stress Distribution
Whitney Rectangular Stress Distribution
] The height of the stress box, a, is defined as a percentage of the depth to the neural axis
f 'c ≤ 4000 psi
⇒
] The values of the tension and compression forces are: 0.85f’c
β1 = 0.85
0.5a
C
a
f 'c ≥ 4000 psi ⎛ f 'c −4000 ⎞ ⎟ ≥ 0.65 ⎝ 1000 ⎠
T
Whitney Rectangular Stress Distribution
0.85f’c
d
a =
Asfy 0.85f 'c b
a =
Asfy 0.85f 'c b
0.5a
∑ M =T ⎛⎜⎝d
C
a
−
a⎞ ⎟ 2⎠
d
If a > d, then you have too much steel
T
=0
] The internal moment is the value of either the tension or compression force multiplied the distance between them
0.5a
C
∑F
Whitney Rectangular Stress Distribution
] If the tension force capacity of the steel is too high, than the value of a is large
a
C = 0.85f 'c ba
T = Asfy
d
β1 = 0.85 − 0.05⎜
0.85f’c
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M = Asfy ⎛⎜d − ⎝
T
a⎞ ⎟ 2⎠
Whitney Rectangular Stress Distribution
Whitney Rectangular Stress Distribution
] The internal moment is the value of either the tension or compression force multiplied the distance between them
] The internal moment is the value of either the tension or compression force multiplied the distance between them
0.85f’c
0.5a
C
a
a M = Asfy ⎛⎜d − ⎞⎟ 2⎠ ⎝
T
M = 4P
⎛
M = Asfy ⎜⎜d − 0.59 ⎝
⎝
Asfy ⎞ ⎟ f 'c b ⎟⎠
We know that the moment in our reinforced concrete beans is
M = 4P
Substitute the value for a
d
⎛
M = Asfy ⎜⎜d − 0.59
Asfy ⎞ ⎟ f 'c b ⎟⎠
Ptension =
Asfy 4
Asfy ⎞ ⎛ ⎜ d - 0.59 ⎟ f'c b ⎠ ⎝
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beams ] There is a “balanced” condition where the stress in the steel reinforcement and the stress in the concrete are both at their yield points ] The amount of steel required to reach the balanced strain condition is defined in terms of the reinforcement ratio:
A ρ= s bd
P
Compression
] The limits of the reinforcement ratio are established as: Reinforcement ratio definition
ρ =
As bd
c > 0.600 d
0.375 <
] Lets consider shear failure in reinforced concrete
P
Vs −Vcr = V =
⎛ Af v yd ⎝ s
P
Af v yd s
2
Shear
⎞ + 2 f 'c bd ⎟ ⎠
Beam failure is controlled by
compression compr ss on
c < 0.600 Transition between tension d and compression control Beam failure is controlled by
tension
Reinforced Concrete Beams ] Lets consider shear failure in unreinforced concrete
Vcr = 2 f 'c bd P V =
Reinforced Concrete Beams
Pshear = 2 ⎜
] The limits of the reinforcement ratio are established as:
ρ as function of c/d
c f 'c ρ = 0.85 β1 d fy
Shear
Reinforced Concrete Beams
c < 0.375 d
Reinforced Concrete Beams
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P
P =Shear 4 f 'c bd
Shear
2
Reinforced Concrete Beams ] Lets consider compression failure in over reinforced concrete ] First, let define an equation that given the stress in the tensile steel when concrete reaches its ultimate strain
⎛d −c ⎞ fsteel = 87, 000 psi ⎜ ⎟ ⎝ c ⎠ ] If fsteel < fy then or
c > 0.600 d
a⎞ ⎛d − c ⎞⎛ ⎟ ⎜ d − 2 ⎟ 87, 000 psi ⎠ ⎝ c ⎠⎝
Mcompression = As ⎜
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beams ] Lets consider compression failure in over reinforced concrete ] First, let define an equation that given the stress in the tensile steel when concrete reaches its ultimate strain
P
M = 4P Pcompression
Reinforced Concrete Beam Analysis ] Let’s use the failure models to predict the ultimate strength-to-weight (SWR) of one of our reinforced concrete beams from lab ] Consider a beam with the following characteristics:
only if fs < fy
Shear
A ⎛d −c = s ⎜ 4 ⎝ c
Concrete strength f’c = 5,000 psi Steel strength fy = 60,000 psi
Shear
The tension reinforcement will be 2 #4 rebars The shear reinforcement will be #3 rebars bent in a U-shape spaced at 4 inches.
a⎞ ⎞⎛ ⎟ ⎜ d − 2 ⎟ 87, 000 psi ⎠ ⎠⎝
Use the minimum width to accommodate the reinforcement
Reinforced Concrete Beam Analysis ] Reinforcing bars are denoted by the bar number. The diameter and area of standard rebars are shown below. Bar #
Reinforced Concrete Beam Analysis ] Based on the choice of reinforcement we can compute an estimate of b and d #4 rebar diameter
Diameter (in) As (in 2 )
3
0.375
0.11
4
0 500 0.500
0 20 0.20
5
0.625
0.31
6
0.750
0.44
7
0.875
0.60
8
1.000
0.79
9
1.128
1.00
10
1.270
1.27
11
1.410
1.56
b
d =6− #4
4.625 in
Space between bars
Reinforced Concrete Beam Analysis ] We now have values for b, d, and As
⎛
M = Asfy ⎜⎜d − 0.59
b
0.5 0 5 −0.75 −0.375 2 #3 rebar diameter
d =
4.0 in
#4
Minimum cover
d
6”
#3 rebar diameter
b ≥ 2(0.5 in ) + 2(0.75 in ) + 2(0.375 in )
d
6”
] If we allow a minimum cover under the rebars were can estimate d
b
Minimum cover
+ 0.75 in =
Reinforced Concrete Beam Analysis Half of #4 bar diameter
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⎝
d
6” #4
Asfy ⎞ ⎟ f 'c b ⎟⎠
] The As for two #4 rebars is:
As = 2(0.20 in 2 ) = 0.40 in 2
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beam Analysis ] Compute the moment capacity
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Reinforced Concrete Beam Analysis ] Let’s check the shear model
⎛ Af v yd
Asfy ⎞ ⎛ ⎟ M = Asfy ⎜⎜d − 0.59 f 'c b ⎟⎠ ⎝
Pshear = 2 ⎜ ⎝
s
⎞ + 2 f 'c bd ⎟ ⎠
Area of two #3 rebars
⎛ 0.4in 2 (60ksi ) ⎞ = 0.4in 2 (60ksi ) ⎜ 4.625in − 0.59 ⎟ 5ksi (4in ) ⎠ ⎝
⎛ 2 ( 0.11in 2 ) ( 60, 000 psi ) 4.625 in ⎞ = 2⎜ + 2 5, 000 psi ( 4 in )( 4.625 in ) ⎟ ⎜ ⎟ 4 in ⎝ ⎠ Shear reinforcement spacing
= 94.0 k ⋅ in
⇒P =
M 4
= 23.5 kips
Reinforced Concrete Beam Analysis ] Let’s check the reinforcement ratio
ρ =
As bd
= 35,757 lbs = 35.76 kips Since Ptension < Pshear therefore Ptension controls
Reinforced Concrete Beam Analysis ] An β1 estimate is given as:
Reinforcement ratio definition
ρ = 0.85 β1
f 'c ≤ 4000 psi ρ as function of c/d
c f 'c d fy
f 'c ≥ 4000 psi ⎛ f 'c −4000 ⎞ ⎟ ≥ 0.65 ⎝ 1000 ⎠
β1 = 0.85 − 0.05⎜
⎛ 5, 000 − 4, 000 ⎞ ⎟ = 0.80 1, 000 ⎝ ⎠
β1 = 0.85 − 0.05 ⎜
To compute ρ, first we need to estimate β1
Reinforced Concrete Beam Analysis ] Check the reinforcement ratio for the maximum steel allowed for tension controlled behavior or c/d = 0.375
ρ = 0.85 β1
5 ksi c f 'c = 0.85(0.80)0.375 d fy 60 ksi
= 0.021 ρ=
0.4 in 2 As = = 0.022 bd 4in (4.625in )
] The amount of steel in this beam is just a bit over the allowable for tension controlled behavior.
β1 = 0.85
⇒
Reinforced Concrete Beam Analysis ] However, the maximum about of steel where compression is in control is c/d = 0.600
ρ = 0.85 β1
5 ksi c f 'c = 0.85(0.80)0.600 d fy 60 ksi
= 0.034 ρ=
0.4 in 2 As = = 0.022 bd 4in (4.625in )
] Therefore, the beam is in the lower part of the transition zone and for our purposes is OK.
CIVL 1112
Introduction to Reinforced Concrete Beams
Reinforced Concrete Beam Analysis ] An estimate of the weight of the beam can be made as: Size of concrete beam
W =
Unit weight of concrete
Reinforced Concrete Beam Analysis ] In summary, this reinforced concrete beam will fail in tension
(4in )(6in )(30in ) ⎛ 145lb ⎞ 1728in 3 /ft 3 ⎜⎝ ft 3 ⎟⎠
Additional weight of rebars
4”
⇒ P = 23.5 23 5 kips
Unit weight of steel
(0.4in 2 )(30in ) ⎛ 490lb − 145lb ⎞ + ⎜ ⎟ 1728in 3 /ft 3 ⎝ ft 3 ⎠
= 60.42lb + 2.39lb = 62.81lb
Reinforced Concrete Beam Analysis
Questions?
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4.625”
6”
SWR = As = 0.4 in2
23,500lb = 62.81lb
374.2