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ANALYSIS OF SECTION With Wisdom We Explore www.uthm.edu.my By: Masni A. Majid [email protected]

3. Chapter 3 - Analysis of Section

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Page 1: 3. Chapter 3 - Analysis of Section

ANALYSIS OF SECTION

With Wisdom We Explore

www.uthm.edu.my

By:Masni A. Majid

[email protected]

Page 2: 3. Chapter 3 - Analysis of Section

Consider a simply supported beam subjected to gradually increasing load. The load causes the beam to bend and exert a bending moment as shown in figure below.

With Wisdom We Explore

Behavior of Beam in Bendingwww.uthm.edu.my

The top surface of the beam is seen to shorten under compression, and the bottom surface lengthens under tension.

As the concrete cannot resist tension, steel reinforcement is introduces at the bottom surface to resist tension.

Page 3: 3. Chapter 3 - Analysis of Section

For continuous beam, the loads also cause the to bend downward between the support and upward bending over the support.

This will produce tensile zone as shown in figure below. As the concrete cannot resist flexural tension, steel reinforcement would be introduced as detail in the figure.

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Behavior of Beam in Bendingwww.uthm.edu.my

Page 4: 3. Chapter 3 - Analysis of Section

In the design of reinforced concrete beam the following assumptions are made (See EN 1991: Cl. 6.1 (2) P.) Plane section through the beam before bending remain plane

after bending. The strain in bonded reinforcement, whether in tension or

compression is the same as that in the surrounding concrete. The tensile of the concrete is ignored. The stresses in the concrete and reinforcement can be derived

from the strain by using stress-strain curve for concrete and steel.

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Basic Assumption in RC Designwww.uthm.edu.my

Page 5: 3. Chapter 3 - Analysis of Section

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Basic Assumption in RC Designwww.uthm.edu.my

Page 6: 3. Chapter 3 - Analysis of Section

Figure below shows the cross section of a RC beam subjected to bending and the resultant strain and stress distribution in the concrete.

Top surface of cross section are subjected to compressive stresses while the bottom surface subjected to tensile stresses.

The line that introduced in between the tensile and compression zones is known as the neutral axis of the member.

Due to the tensile strength of concrete is very low, all the tensile stresses at the bottom fibre are taken by reinforcement.

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Distribution of Stresses and Strainwww.uthm.edu.my

Page 7: 3. Chapter 3 - Analysis of Section

For fck < 50 N/mm2: η = 1 (defining the effective strength), εc = 0.0035,

αcc = 0.85, λ = 0.8, γc = 1.5,

fcd = 1.0 x 0.85 x fck / 1.5 = 0.567 fck

With Wisdom We Explore

Distribution of Stresses and Strainwww.uthm.edu.my

dh

b

x

εcc

εst

fcc

fst fyd

ηfcd

Fst

ηαccfck/γc

Fcc

z

s = λx

(1) (2) (3)

Page 8: 3. Chapter 3 - Analysis of Section

Stress distribution in the concreteThe triangular stress distribution applies when the stress are very nearly proportional to the strain, which generally occurs at the loading levels encountered under working load conditions and is, therefore, used at the serviceability limit state.The rectangular-parabolic stress block represents the distribution at failure when the compressive strain are within the plastic range, and it is associated with the design for ultimate limit state.The equivalent rectangular stress block is a simplified alternative to the rectangular-parabolic distribution.

With Wisdom We Explore

Distribution of Stresses and Strainwww.uthm.edu.my

Page 9: 3. Chapter 3 - Analysis of Section

The distribution of strains across the beam cross section is linear. That is, the normal strain at any points in a beam section is proportional to its distance from the neutral axis.

The steel strain in tension εst can be determined from the strain diagram as follows:

With Wisdom We Explore

Distribution of Stresses and Strainwww.uthm.edu.my

x

xd

xxd ccstccst

)(

cc

st

dx

1Therefore ;

Page 10: 3. Chapter 3 - Analysis of Section

Since, εcc = 0.0035 for class ≤ C50/60 and

For steel with fyk = 500 N/mm2 and the yield strain is εst = 0.00217.

By substituting εcc and εst ,

Hence, to ensure yielding of the tension steel at limit state the depth of neutral axis, x should be less than or equal to 0.617d.

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Introductionwww.uthm.edu.my

dx 617.0

Page 11: 3. Chapter 3 - Analysis of Section

As applied moment on the beam section increased beyond the linear elastic stage, the concrete strains and stresses enter the nonlinear stage.

The behavior of the beam in the nonlinear stage depends on the amount of reinforcement provided.

The reinforcing steel can sustain very high tensile strain however, the concrete can accommodate compressive strain much lower compare to it.

So, the final collapse of a normal beam at ultimate limit state is cause by the crushing of concrete in compression, regardless of whether the tension steel has yield or not.

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Type of RC Beam Failurewww.uthm.edu.my

Page 12: 3. Chapter 3 - Analysis of Section

Depending on the amount of reinforcing steel provided, flexural failure may occur in three ways: Balanced : Concrete crushed and steel yields simultaneously at the ultimate limit

state. The compressive strain of concrete reaches the ultimate strains εcu and the tensile strain of steel reaches the yield strain εy simultaneously. The depth of neutral axis, x = 0.617d.

Under-reinforced : Steel reinforcement yields before concrete crushes. The area of tension steel provided is less than balance section. The depth of neutral axis, x < 0.617d. The failure is gradual, giving ample prior warning of the impending collapse. This mode if failure is preferred in design practice.

Over-reinforced : Concrete fails in compression before steel yields. The area of steel provided is more than area provided in balance section. The depth of neutral axis, x > 0.617d. The failure is sudden (without any sign of warning) and brittle. Over-reinforced are not permitted.

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Type of RC Beam Failurewww.uthm.edu.my

Page 13: 3. Chapter 3 - Analysis of Section

For a singly reinforced beam EC2 limits the depth to the neutral axis, x to 0.45d (x ≤ 0.45d) for concrete class ≤ C50/60 to ensure that the design is for the under-reinforced case where failure is gradual, as noted above. For further understanding, see the graph shown below .

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Introductionwww.uthm.edu.my

Page 14: 3. Chapter 3 - Analysis of Section

Section 6.1 EN 1992-1-1, deal with the analysis and design of section for the ultimate limit state design consideration of structural elements subjected to bending.

The two common types of reinforced concrete beam section are: Rectangular section : Singly and doubly reinforced Flanged section : Singly and doubly reinforced

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Analysis of Sectionwww.uthm.edu.my

Page 15: 3. Chapter 3 - Analysis of Section

Beam cross section, strains and stresses distribution at ULS of singly reinforced rectangular beam

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Singly Reinforced Rectangular Beamwww.uthm.edu.my

dh

b

x

0.0035

εstFst

0.567fck

Fcc

z = d – 0.5s

s = 0.8x

Neutral axis

Notation:h = Overall depth d = Effective depthb = Width of section s = Depth of stress blockAs = Area of tension reinforcement x = Neutral axis depthfck = Characteristic strength of concrete z = Lever armfyk = Characteristic strength of reinforcement

As

Page 16: 3. Chapter 3 - Analysis of Section

Tension force of steel, Fst

Compression force of concrete, Fcc

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Singly Reinforced Rectangular Beamwww.uthm.edu.my

sky Af 87.0Fst = Stress x Area

Fcc = Stress x Area bxfxbf ckck 454.0)8.0(567.0

For equilibrium, total force in the section should be zero.

stcc FF

sykck Afbxf 87.0454.0

bf

Afx

ck

syk

454.0

87.0

Page 17: 3. Chapter 3 - Analysis of Section

Moment resistance with respect to the steel

Lets; Therefore;

Moment resistance with respect to the concrete

Area of tension reinforcement,

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Singly Reinforced Rectangular Beamwww.uthm.edu.my

zFMcc

xdbxfM ck 4.0454.0

zFMst

xdAfM sky 4.087.0

Kd

x

d

x

4.0

1454.0

2..4.0454.0

dbfd

xd

d

xck

2... dbfKM ck

)4.0.(.87.0 xdf

MA

yks

Page 18: 3. Chapter 3 - Analysis of Section

To ensure that the section designed is under-reinforced it is necessary to place a limit on the maximum depth of the neutral axis (x). EC2 suggests:

Then ultimate moment resistance of singly reinforced section or Mbal can be obtained by;

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Singly Reinforced Rectangular Beamwww.uthm.edu.my

22 [email protected] dbfKdbfM ckbalckbal

xdbxfM ckbal 4.0454.0

)]45.0(4.0)].[45.0(..454.0[ dddbfM ckbal

)82.0).(...2043.0( ddbfM ckbal

x ≤ 0.45d

Page 19: 3. Chapter 3 - Analysis of Section

Therefore;– M = K.fck.b.d2

– Mbal = Kbal.fck.b.d2

where; Kbal = 0.167

If;– M ≤ Mbal or K ≤ Kbal : Singly reinforced rectangular beam

(Tension reinforcement only)– M > Mbal or K > Kbal : Doubly reinforced rectangular beam

(Section requires compression reinforcement)

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Singly Reinforced Rectangular Beamwww.uthm.edu.my

Page 20: 3. Chapter 3 - Analysis of Section

The cross section of rectangular beam is shown in figure below. Using stress block diagram and the data given, determine the area and the number of reinforcement required.

Data:Design moment, MED = 200 kN.m

fck = 25 N/mm2

fyk = 500 N/mm2

With Wisdom We Explore

Example 3.1www.uthm.edu.my

b = 250 mm

d = 450 mm

Page 21: 3. Chapter 3 - Analysis of Section

Calculate the ultimate moment resistance of section, Mbal

Singly reinforced sectionNeutral axis depth, x

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Solution of Example 3.1www.uthm.edu.my

2...167.0 dbfM ckbal

)450)(250)(25(167.0 2

kNmMkNm 20036.211

xdbxfM ck 4.0454.0

)4.0450)()(250)(25(454.010200 6 xx

045.17621111252 xx

Page 22: 3. Chapter 3 - Analysis of Section

x = 188 mm @ 937 mm

Use x = 188 mm

Checking;

Lever arm, z = (d – 0.4x)

= (450 – 0.4(188)) = 374.8 mm

Area of reinforcement, As

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Solution of Example 3.1www.uthm.edu.my

45.042.0450

188

d

x

zf

MA

yks 87.0 2

6

1227)8.374)(500(87.0

10200mm

)1257(204Pr 2mmAHovide sprov

Page 23: 3. Chapter 3 - Analysis of Section

Figure below shows the cross section of a singly reinforced beam. Determine the resistance moment for that cross section with the assistance of a stress block diagram. Given fck= 25 N/mm2 and fyk = 500 N/mm2.

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Example 3.2www.uthm.edu.my

450 mm

250 mm

2H25

Page 24: 3. Chapter 3 - Analysis of Section

A stress block diagram is drawn with the important values and notations.

For equilibrium;

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Solution of Example 3.2www.uthm.edu.my

d = 450

b = 250

x

Fst=0.87fykAs

0.567fck

Fcc=0.454fckbx

z = d – 0.4x

s = 0.8xNeutral axis

As = 982 mm2

stcc FF

sykck Afbxf 87.0454.0 bf

Afx

ck

syk

454.0

87.0

Page 25: 3. Chapter 3 - Analysis of Section

Checking;

Moment resistance of section;

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Solution of Example 3.2www.uthm.edu.my

mmx 151)250)(25(454.0

)982)(500(87.0

45.034.0450

151

d

x

zFMcc

xdbxfM ck 4.0454.0 ))151(4.0450)(15125025454.0( M

kNmM 167

zFMst@

Page 26: 3. Chapter 3 - Analysis of Section

When the load applied increases gradually and it will reach a state that the compressive strength of concrete is not adequate to take additional compressive stress.

Compression reinforcement is required to take the additional compressive stress.

This section is named as doubly reinforced section.

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Doubly Reinforced Rectangular Beamwww.uthm.edu.my

dh

b

d’

As

As’

Page 27: 3. Chapter 3 - Analysis of Section

Strain and stress block diagrams of doubly reinforced beam.

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Doubly Reinforced Rectangular Beamwww.uthm.edu.my

dh

b

x

0.0035

εst

Fst

0.567fck

Fcc

z = d – 0.4x

s = 0.8x

Neutral axis

d’εsc

Fsc

As

As’

z1 = d – d’

Page 28: 3. Chapter 3 - Analysis of Section

Internal force;

Lever arms;

For equilibrium of internal force;

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Doubly Reinforced Rectangular Beamwww.uthm.edu.my

bxfF ckcc 454.0

sykst AfF 87.0 '87.0 syksc AfF

xdz 4.0 '1 ddz

scccst FFF '87.0454.087.0 sykcksyk AfbxfAf

and

Page 29: 3. Chapter 3 - Analysis of Section

Taking moment about the centroid of the tension steel,

For design purpose, x = 0.45d

The area of compression reinforcement, As’

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Doubly Reinforced Rectangular Beamwww.uthm.edu.my

1.. zFzFM sccc )').('87.0()4.0).(454.0( ddAfxdbxfM sykck

)').('87.0()]45.0(4.0).[454.0( ddAfddbxfM sykck

)').('87.0(167.0 2 ddAfbdf sykck )').('87.0( ddAfM sykbal

)'(87.0

)('

ddf

MMA

yk

bals

)'(87.0

)('

2

ddf

bdfKKA

yk

ckbals

or

Page 30: 3. Chapter 3 - Analysis of Section

The area of Tension reinforcement, As

Multiplied equilibrium internal force equation by z ,Limiting x = 0.45d and z = d – 0.4(0.45d) = 0.82d

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Doubly Reinforced Rectangular Beamwww.uthm.edu.my

zAfbxzfzAf sykcksyk '87.0454.087.0

zAfddbfzAf sykcksyk '87.0)82.0)(45.0(454.087.0 zAfbdfzAf sykcksyk '87.0167.087.0 2

'87.0

167.0 2

syk

cks A

zf

bdfA '

87.0

2

syk

ckbals A

zf

bdfKA or

Page 31: 3. Chapter 3 - Analysis of Section

Stress in compression reinforcement. The derivation of design formula for doubly reinforced section

assumed that the compression reinforcement reaches the design strength of 0.87fyk at ultimate limit state.

From the strain diagram as shown in figure below.

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Doubly Reinforced Rectangular Beamwww.uthm.edu.my

dh

b

x

0.0035

εst

d’εsc

As

As’

xdxsc 0035.0

)'(

0035.0

)'( sc

x

dx

0035.01

' sc

x

d

Page 32: 3. Chapter 3 - Analysis of Section

For the design strength 0.87fyk to be reached, εsc = 0.87fyk / Es

Therefore, if d’/x < 0.38 the compression reinforcement can be assumed reach the design strength of 0.87fyk. If d’/x > 0.38, a reduced stress should be used.

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Doubly Reinforced Rectangular Beamwww.uthm.edu.my

002175.010200

)500(87.087.03

s

yksc E

f

38.00035.0

002175.01

'

x

d

scssc Ef .

)/'1)(0035.0(10200 3 xdfsc

)/'1(700 xd

Page 33: 3. Chapter 3 - Analysis of Section

The cross section of rectangular beam is shown in figure below. Using the data given, determine the area and the number of reinforcement required.

Data:Design moment, MED = 450 kN.m

fck = 25 N/mm2

fyk = 500 N/mm2

d’ = 50 mm

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Example 3.3www.uthm.edu.my

b = 250 mm

d = 500 mm

Page 34: 3. Chapter 3 - Analysis of Section

Ultimate moment resistant of section, Mbal

Compression reinforcement is required

Area of compression reinforcement, As’

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Solution of Example 3.3www.uthm.edu.my

2...167.0 dbfM ckbal

kNmMkNm 45094.260 )10)(500)(250)(25(167.0 62

)50500)(500(87.0/10)94.260450( 6

)'(87.0/)(' ddfMMA ykbals

2966mm

Page 35: 3. Chapter 3 - Analysis of Section

Checking d’/x ratio

Compression steel achieved it design strength at 0.87fyk

Area of tension steel, As

Provide 2H25 (As’ Prov. = 982 mm2) – Compression reinforcement

5H25 (As Prov. = 2454 mm2) – Tension reinforcement

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Solution of Example 3.3www.uthm.edu.my

mmdx 225)500(45.045.0 38.022.0225/50/' xd

966)50082.0(50087.0

1094.260 6

22429mm

'87.0 s

yk

bals A

zf

MA

Page 36: 3. Chapter 3 - Analysis of Section

Calculate moment resistance of the doubly reinforced section shown in figure below. Given fck= 30 N/mm2 and fyk = 500 N/m2.

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Example 3.4www.uthm.edu.my

d = 500 mm

b = 250 mm d’ = 50 mm

3H20

5H25

Page 37: 3. Chapter 3 - Analysis of Section

A stress block diagram is drawn with the important values and notations

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Solution of Example 3.4www.uthm.edu.my

0.8xx Fcc = 0.454fckbx

Fst = 0.87fykAs

Z

Neutral Axis

b = 250 mm

Fsc = 0.87fykAs’

Z1

d’ = 50 mm

3H20

5H25

Page 38: 3. Chapter 3 - Analysis of Section

Reinforcement used 3H20, As’ = 943 mm2 & 5H25, As = 2455 mm2

Neutral axis depth, x

Checking the stress of steel

Steel achieved it design strength 0.87fy as assumed

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Solution of Example 3.4www.uthm.edu.my

)250)(30(454.0

)9432455)(500(87.0

454.0

)'(87.0

bf

AAfx

ck

ssyk

mmx 193

38.026.0193/50/' xd

45.039.0500/193/ dx

Page 39: 3. Chapter 3 - Analysis of Section

Moment resistance of section, M

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Solution of Example 3.4www.uthm.edu.my

zFzFM ccsc .. 1

)4.0(454.0)'('87.0 xdbxfddAf cksyk

)50500)(943)(500(87.0 610))193(4.0500)(193)(250)(30(454.0

kNm462

Page 40: 3. Chapter 3 - Analysis of Section

Flanged beams occur when beams are cast integrally with and support a continuous floor slab.

Part of the slab adjacent to the beam is counted as acting in compression to form T- and L-beams as shown in figure below.

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Flange Beamwww.uthm.edu.my

Where; beff = effective flange widthbw = breadth of the web of the beam.hf = thickness of the flange.

beff beff

bw bw

hf

h

T-Beam L-Beam

Page 41: 3. Chapter 3 - Analysis of Section

The effective width of flange, beff is given in Sec. 5.3.2.1 of EC2.

beff should be based on the distance lo between points of zero moment as shown in figure below.

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Flange Beamwww.uthm.edu.my

Page 42: 3. Chapter 3 - Analysis of Section

The effective flange width, beff for T-beam or L-beam may be derived as:

Where and

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Flange Beamwww.uthm.edu.my

bbbb wieffeff ,

ooiieff llbb 2.01.02.0, iieff bb ,

Page 43: 3. Chapter 3 - Analysis of Section

Based on figure below, determine the effective flange width, beff of beam B/1-3.

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Example 3.5www.uthm.edu.my

3000 4500

2500

4000

1 2 3

A

B

C

200 x 500

200 x 500 200 x 500

200 x 500 200 x 500

200

x 50

020

0 x

500

200

x 50

020

0 x

500

FS1 (150 thk.)

FS2 (150 thk.) FS3 (150 thk.)

Page 44: 3. Chapter 3 - Analysis of Section

D

lo (distance between points of zero moment)

Effective flange width, beff

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Solution of Example 3.5www.uthm.edu.my

3000 mm 4500 mm

lo = 0.85 x 3000 = 2550 mm

lo = 0.85 x 4500 = 3825 mm

lo = 0.15 x (3000 + 4500) = 1125 mm

1 2 3

bbbb wieffeff ,

Page 45: 3. Chapter 3 - Analysis of Section

Span 1-2

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Solution of Example 3.5www.uthm.edu.my

2500 4000

b1 = 2500/2 = 1250 b2 = 4000/2 = 2000

beff,1 beff,2

bw = 200 mm

beff

b = 1250 + 2000 = 3250 mm

beff1 = 0.2(1250) + 0.1(2550) = 505 mm < 0.2lo = 510 mm < b1 = 1250 mm

beff2 = 0.2(2000) + 0.1(2550) = 655 mm > 0.2lo = 510 mm < b2 = 2000 mm

beff = (505 + 510) + 200 = 1215 mm < 3250 mm

A B C

Page 46: 3. Chapter 3 - Analysis of Section

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Solution of Example 3.5www.uthm.edu.my

Span 2-3

2500 4000

b1 = 2500/2 = 1250 b2 = 4000/2 = 2000

beff,1 beff,2

bw = 200 mm

beff

b = 1250 + 2000 = 3250 mm

beff1 = 0.2(1250) + 0.1(3825) = 632.5 mm < 0.2lo = 765 mm < b1 = 1250 mm

beff2 = 0.2(2000) + 0.1(3825) = 782.5 mm > 0.2lo = 765 mm < b2 = 2000 mm

beff = (632.5 + 765) + 200 = 1597.5 mm < 3250 mm

A B C

Page 47: 3. Chapter 3 - Analysis of Section

Span 1-2 Span 2-3

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Solution of Example 3.5www.uthm.edu.my

beff = 1215mm

bw = 200 mm

hf = 150 mm

beff = 1598 mm

bw = 200 mm

hf = 150 mm

Page 48: 3. Chapter 3 - Analysis of Section

The design procedure of flange beam depends on where the neutral axis lies. The neutral axis may lie in the flange or in the web.

In other word, there are three cases that should be considered. Neutral axis lies in flange (M < Mf)

Neutral axis lies in web (M > Mf but < Mbal)

Neutral axis lies in web (M > Mbal)

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Flange Beamwww.uthm.edu.my

beff beff

Page 49: 3. Chapter 3 - Analysis of Section

Neutral axis lies in flange (M < Mf)

This condition occur when the depth of stress block (0.8 x) less then the thickness of flange, hf as shown in figure below.

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Flange Beamwww.uthm.edu.my

beff

bw

hf

d

0.8x Fcc

Fst

Z = d – 0.4x

x

As

0.567fck

Page 50: 3. Chapter 3 - Analysis of Section

Moment resistance of section, M

For this case, maximum depth of stress block, 0.8x are equal to hf

Where, Mf = Ultimate moment resistance of flange.

Therefore, if M ≤ Mf the neutral axis lies in flange and the design can be treated as rectangular singly reinforced beam.

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Flange Beamwww.uthm.edu.my

zFMcc

xdxbfM effcu 4.08.0567.0

2/567.0 ffckf hdbhfMM

)4.0(87.0 xdf

MA

yks

zf

MA

yks 87.0 or

Page 51: 3. Chapter 3 - Analysis of Section

The T-beam with dimension as shown in figure below is subjected to design moment, M = 250 kNm. If fck = 30 N/mm2 and fyk = 500 N/mm2 have been used, determine the area and number of reinforcement required.

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Example 3.6www.uthm.edu.my

beff = 1450 mm

bw = 250 mm

hf = 100 mm

d = 320 mm

As

Page 52: 3. Chapter 3 - Analysis of Section

Moment resistance of flange, Mf

Since M < Mf, Neutral axis lies in flange

Compression reinforcement is not required

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Solution of Example 3.6www.uthm.edu.my

2/567.0 ffeffckf hdhbfM

kNmMkNm 2509.665 6102/100320100145030567.0

mmmmx [email protected]

xdbxfM ck 4.0454.0

)4.0320)()(1450)(30(454.010250 6 xx 02.316478002 xx

Use x = 41.74mm

Page 53: 3. Chapter 3 - Analysis of Section

Checking

Lever arm,z

Area of tension reinforcement, As

Provide 4H25 (Asprov = 1964 mm2)

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Flange Beamwww.uthm.edu.my

45.013.0320

74.41

d

x

mmxdz 3.303)74.41(45.03204.0

21895mm

)3.303)(500(87.0

10250

87.0

6

zf

MA

yks

Page 54: 3. Chapter 3 - Analysis of Section

Neutral axis lies in web (Mf < M < Mbal)

If the applied moment M is greater than Mf the neutral axis lies in the web as shown in figure below.

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Flange Beamwww.uthm.edu.my

beff

bw

hf

d0.8x Fcc1

Fst

z1

x

As

0.567fck

122 Fcc2

z2

Page 55: 3. Chapter 3 - Analysis of Section

From the stress block, internal forces;

Lever arms, z

Moment resistance, M

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Flange Beamwww.uthm.edu.my

xbfxbfF wckwckcc 454.0)8.0.)(567.0(1

fweffckcc hbbfF ))(567.0(2

sykst AfF 87.0

xdz 4.01 fhdz 5.0

2

2211.. zFzFM

cccc

)5.0())(567.0(4.0454.0 ffweffckwck hdhbbfxdxbf

Page 56: 3. Chapter 3 - Analysis of Section

Ultimate moment resistance of section, Mbal (When x = 0.45d)

Divide both side by fckbeffd2, then;

Therefore;

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Flange Beamwww.uthm.edu.my

)45.0(4.045.0454.0 dddbfM wckbal

)5.0())(567.0( ffweffck hdhbbf

d

h

b

b

d

h

b

b

dbf

M f

eff

wf

eff

w

effck

bal

211567.0167.0

2

feffck

bal

dbf

M 2

2dbfM effckfbal

Page 57: 3. Chapter 3 - Analysis of Section

If applied moment M < Mbal, then compression reinforcement are not required. Area of tension reinforcement can be calculate as follows by taking moment at Fcc2.

Using; x = 0.45d

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Flange Beamwww.uthm.edu.my

)5.0(87.0

]5.04.0[454.0

fyk

fwkcs hdf

hxxbfMA

)]4.0()5.0[(454.0)5.0(87.0 xdhdxbfhdAf fwckfsyk

).(. 1212 zzFzFM ccst

)5.0(87.0

]36.0[1.0

fyk

fwkcs hdf

hddbfMA

Page 58: 3. Chapter 3 - Analysis of Section

The T-beam with dimension as shown in figure below is subjected to design moment, M = 670 kNm. If fck = 30 N/mm2 and fyk = 500 N/mm2 have been used, determine the area and number of reinforcement required.

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Example 3.7www.uthm.edu.my

beff = 1450 mm

bw = 250 mm

hf = 100 mm

d = 320 mm

Page 59: 3. Chapter 3 - Analysis of Section

Moment resistance of flange, Mf

Since M > Mf, Neutral axis lies in web

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Solution of Example 3.7www.uthm.edu.my

2/567.0 ffeffckf hdhbfM

kNmMkNm 6709.665 6102/100320100145030567.0

153.0)320(2

1001

1450

2501

320

100567.0

1450

250167.0

f

2dbfM effckfbal

kNmM bal 68210)320)(1450)(30(153.0 62

kNmMkNmM bal 670682

Page 60: 3. Chapter 3 - Analysis of Section

Compression reinforcement is not required

Area of tension reinforcement, As

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Solution of Example 3.7www.uthm.edu.my

)50320)(500(87.0

]100)320(36.0)[320)(250)(30(1.010670 6

)5.0(87.0

]36.0[1.0

fyk

fwkcs hdf

hddbfMA

25736mm

Provide 8H32 (Asprov = 6433 mm2)

Page 61: 3. Chapter 3 - Analysis of Section

Neutral axis lies in web (M > Mbal)

If the applied moment M is greater than Mbal the neutral axis lies in the web and the compression reinforcement should be provided. The stress block are shown in figure below.

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Flange Beamwww.uthm.edu.my

d

beff

bw

hf 0.8x Fcc1

Fst

z1

x

As

0.567fck

1

22 Fcc2

z2

As’ Fsc

z3

Page 62: 3. Chapter 3 - Analysis of Section

From the stress block, internal forces;

Lever arms, z

Moment resistance, M

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Flange Beamwww.uthm.edu.my

xbfxbfF wckwckcc 454.0)8.0.)(567.0(1

fweffckcc hbbfF ))(567.0(2

sykst AfF 87.0

'87.0 syksc AfF

xdz 4.01 f

hdz 5.02

'3

ddz

32211... zFzFzFM

sccccc

Page 63: 3. Chapter 3 - Analysis of Section

When x = 0.45d, then

Area of compression reinforcement, As’

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Flange Beamwww.uthm.edu.my

)5.0())(567.0(4.0454.0 ffweffcuwcu hdhbbfxdxbfM )'('87.0 ddAf syk

)'('87.0 ddAfMM sykbal

)'(87.0'

ddf

MMA

yk

bals

Page 64: 3. Chapter 3 - Analysis of Section

For equilibrium of forces

Area of tension reinforcement, As

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Flange Beamwww.uthm.edu.my

scccccstFFFF

21

'87.0)(567.0)45.0(454.087.0 sykweffckwcksyk AfbbfdbfAf

'87.0

)(567.02.0s

yk

wefffckwcks A

f

bbhfdbfA

Page 65: 3. Chapter 3 - Analysis of Section

Design Procedures for Rectangular SectionSupposed the design bending moment is M, beam section is b x d,

concrete strength is fck and steel strength is fyk, to determine the area of reinforcement, proceed as follows.

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Design Formulawww.uthm.edu.my

Page 66: 3. Chapter 3 - Analysis of Section

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Design Formulawww.uthm.edu.my

Page 67: 3. Chapter 3 - Analysis of Section

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Design Formulawww.uthm.edu.my

Page 68: 3. Chapter 3 - Analysis of Section

Design Procedures for Flange SectionSupposed the design bending moment is M, beam section is b x d,

concrete strength is fck and steel strength is fyk, to determine the area of reinforcement, proceed as follows.

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Design Formulawww.uthm.edu.my

Page 69: 3. Chapter 3 - Analysis of Section

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Design Formulawww.uthm.edu.my

Page 70: 3. Chapter 3 - Analysis of Section

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Design Formulawww.uthm.edu.my

Page 71: 3. Chapter 3 - Analysis of Section

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www.uthm.edu.my