46
Lecture 6 - Flexure June 13, 2003 CVEN 444

Lecture 6 - Flexure

Embed Size (px)

DESCRIPTION

Lecture 6 - Flexure. June 13, 2003 CVEN 444. Lecture Goals. Doubly Reinforced beams T Beams and L Beams. Analysis of Doubly Reinforced Sections. Effect of Compression Reinforcement on the Strength and Behavior. - PowerPoint PPT Presentation

Citation preview

Page 1: Lecture 6 - Flexure

Lecture 6 - Flexure

June 13, 2003CVEN 444

Page 2: Lecture 6 - Flexure

Lecture GoalsLecture Goals

Doubly Reinforced beamsT Beams and L Beams

Page 3: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced SectionsReinforced Sections

Effect of Compression Reinforcement on the Strength and Behavior

Less concrete is needed to resist the T and thereby moving the neutral axis (NA) up.

TC

fAT

ys

Page 4: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced SectionsReinforced Sections

Effect of Compression Reinforcement on the Strength and Behavior

12

2sc

1c

and

2; C

ReinforcedDoubly

2;

ReinforcedSingly

aa

adfAMCC

adfAMCC

ysn

ysn

Page 5: Lecture 6 - Flexure

Reasons for Providing Reasons for Providing Compression Compression ReinforcementReinforcement

Reduced sustained load deflections. Creep of concrete in compression

zone transfer load to compression steel reduced stress in concrete less creep less sustained load deflection

Page 6: Lecture 6 - Flexure

Reasons for Providing Reasons for Providing Compression ReinforcementCompression Reinforcement

Effective of compression reinforcement on sustained load deflections.

Page 7: Lecture 6 - Flexure

Reasons for Providing Reasons for Providing Compression ReinforcementCompression Reinforcement

Increased Ductility

reduced stress block depth

increase in steel strain larger curvature are obtained.

Page 8: Lecture 6 - Flexure

Reasons for Providing Reasons for Providing Compression ReinforcementCompression Reinforcement

Effect of compression reinforcement on strength and ductility of under reinforced beams.

b

Page 9: Lecture 6 - Flexure

Reasons for Providing Reasons for Providing Compression ReinforcementCompression Reinforcement

Change failure mode from compression to tension. When bal addition of As strengthens.

Effective reinforcement ratio = (’)

Compression zone

allows tension steel to yield before crushing of concrete.

Page 10: Lecture 6 - Flexure

Reasons for Providing Reasons for Providing Compression ReinforcementCompression Reinforcement

Eases in Fabrication - Use corner bars to hold & anchor

stirrups.

Page 11: Lecture 6 - Flexure

Effect of Compression Effect of Compression ReinforcementReinforcement

Compare the strain distribution in two beams with the same As

Page 12: Lecture 6 - Flexure

Effect of Compression Effect of Compression ReinforcementReinforcement

Section 1: Section 2:

Addition of A’s strengthens compression zone so that less concrete is needed to resist a given value of T. NA goes up (c2 <c1) and s increases (s2 >s1).

1c

ss1

11cc1c

ss

85.0

85.0 85.0

bf

fAc

cbfbafCT

fAT

1c

ssss2

21css

2css

1cs

ss

85.0

85.0

85.0

bf

fAfAc

cbffA

baffA

CCT

fAT

Page 13: Lecture 6 - Flexure

Doubly Reinforced Doubly Reinforced BeamsBeams

Under reinforced Failure ( Case 1 ) Compression and tension steel

yields ( Case 2 ) Only tension steel yields

Over reinforced Failure ( Case 3 ) Only compression steel yields ( Case 4 ) No yielding Concrete crushes

Four Possible Modes of Failure

Page 14: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Strain Compatibility Check Assume s’ using similar triangles

s

s

0.003

'

'*0.003

c d c

c d

c

Page 15: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Strain Compatibility

Using equilibrium and find a

s s yc s

c

s s y y

1 1 c 1 c

0.85

'

0.85 0.85

A A fT C C a

f b

A A f d fac

f b f

Page 16: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Strain Compatibility The strain in the compression steel is

s cu

1 c

y

1

0.851 0.003

'

d

c

f d

d f

Page 17: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Strain Compatibility Confirm

;E ys

s

yys

f

y y1 cs 3

y s

0.851 0.003

' E 29 x 10 ksi

f ff d

d f

Page 18: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSectionsStrain Compatibility Confirm

y1 c

y

1 c

y y

870.85

' 87

0.85 87'

87

ff d

d f

f d

d f f

Page 19: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSectionsFind c

confirm that the tension steel has yielded

s y c s y

ss s y1

c 1

0.85

0.85

A f f ba A f

A A fc a c

f b

ys cu y

sE

fd c

c

Page 20: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

If the statement is true than

else the strain in the compression steel

n s s y s y2

aM A A f d A f d d

s sf E

Page 21: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Return to the original equilibrium equation

s y s s c

s s s c 1

s s cu c 1

0.85

0.85

1 0.85

A f A f f ba

A E f b c

dA E f b c

c

Page 22: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Rearrange the equation and find a quadratic equation

Solve the quadratic and find c.

s y s s cu c 1

2c 1 s s cu s y s s cu

1 0.85

0.85 0

dA f A E f b c

c

f b c A E A f c A E d

Page 23: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Find the fs’

Check the tension steel.

s s cu1 1 87 ksid d

f Ec c

ys cu y

sE

fd c

c

Page 24: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Another option is to compute the stress in the compression steel using an iterative method.

1 c3s

y

0.8529 x 10 1 0.003

'

f df

d f

Page 25: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSectionsGo back and calculate the equilibrium with fs’

s y s s

c sc

1

s

0.85

1 87 ksi

A f A fT C C a

f b

ac

df

c

Iterate until the c value is adjusted for the fs’ until the stress converges.

Page 26: Lecture 6 - Flexure

Analysis of Doubly Analysis of Doubly Reinforced Rectangular Reinforced Rectangular SectionsSections

Compute the moment capacity of the beam

n s y s s s s2

aM A f A f d A f d d

Page 27: Lecture 6 - Flexure

Limitations on Reinforcement Limitations on Reinforcement Ratio for Doubly Reinforced Ratio for Doubly Reinforced beamsbeams

Lower limit on

same as for single reinforce beams.

yy

cmin

200

3

ff

f

(ACI 10.5)

Page 28: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSection

Given:

f’c= 4000 psi fy = 60 ksi

A’s = 2 #5 As = 4 #7

d’= 2.5 in. d = 15.5 in

h=18 in. b =12 in.

Calculate Mn for the section for the given compression steel.

Page 29: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSection

Compute the reinforcement coefficients, the area of the bars #7 (0.6 in2) and #5 (0.31 in2)

2 2s

2 2s

2s

2s

4 0.6 in 2.4 in

2 0.31 in 0.62 in

2.4 in0.0129

12 in. 15.5 in.

0.62 in0.0033

12 in. 15.5 in.

A

A

A

bd

A

bd

Page 30: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSectionCompute the effective reinforcement ratio and minimum

y

c

y

min

0.0129 0.0033 0.00957

200 2000.00333

60000

3 3 4000or 0.00316

60000

0.0129 0.00333 OK!

eff

f

f

f

Page 31: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSection

Compute the effective reinforcement ratio and minimum

1 c

y y

0.85 87'

87

0.85 0.85 4 ksi 2.5 in. 870.0398

60 ksi 15.5 in. 87 60

f d

d f f

0.00957 0.0398 Compression steel has not yielded.

Page 32: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSectionInstead of iterating the equation use the quadratic method

2c 1 s s cu s y s s cu

2

2 2

2

2

2

0.85 0

0.85 4 ksi 12 in. 0.85

0.62 in 29000 ksi 0.003 2.4 in 60 ksi

0.62 in 29000 ksi 0.003 2.5 in. 0

34.68 90.06 134.85 0

2.5969 3.8884 0

f b c A E A f c A E d

c

c

c c

c c

Page 33: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSectionSolve using the quadratic formula

2

2

2.5969 3.8884 0

2.5969 2.5969 4 3.8884

23.6595 in.

c c

c

c

Page 34: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSection

Find the fs’

Check the tension steel.

s s cu

2.5 in.1 1 87 ksi

3.659 in.

27.565 ksi

df E

c

s

15.5 in. 3.659 in.0.003 0.00971 0.00207

3.659 in.

Page 35: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSection

Check to see if c works

2 2s y s s

c 1

2.4 in 60 ksi 0.62 in 27.565 ksi

0.85 0.85 4 ksi 0.85 12 in.

3.659 in.

A f A fc

f b

c

The problem worked

Page 36: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSectionCompute the moment capacity of the beam

s y s s s s

2

2

2

2

2.4 in 60 ksi 0.85 3.659 in.15.5 in.

2 0.62 in 27.565 ksi

0.62 in 27.565 ksi 15.5 in. 2.5 in.

1991.9 k - in. 166 k - ft

n

aM A f A f d A f d d

Page 37: Lecture 6 - Flexure

Example: Doubly Reinforced Example: Doubly Reinforced SectionSectionIf you want to find the Mu for the problem

u u

3.66 in.0.236

15.5 in.

0.375 0.9

0.9 166 k - ft

149.4 k - ft

c

d

c

d

M M

From ACI (figure R9.3.2)or figure (pg 100 in your text)

The resulting ultimate moment is

Page 38: Lecture 6 - Flexure

Analysis of Flanged Analysis of Flanged SectionSection

Floor systems with slabs and beams are placed in monolithic pour.Slab acts as a top flange to the beam; T-beams, and Inverted L(Spandrel) Beams.

Page 39: Lecture 6 - Flexure

Analysis of Flanged Analysis of Flanged SectionsSectionsPositive and Negative Moment Regions in a T-beam

Page 40: Lecture 6 - Flexure

Analysis of Flanged Analysis of Flanged SectionsSections

If the neutral axis falls within the slab depth analyze the beam as a rectangular beam, otherwise as a T-beam.

Page 41: Lecture 6 - Flexure

Analysis of Flanged Analysis of Flanged SectionsSectionsEffective Flange Width

Portions near the webs are more highly stressed than areas away from the web.

Page 42: Lecture 6 - Flexure

Analysis of Flanged Analysis of Flanged SectionsSections

Effective width (beff)

beff is width that is stressed uniformly to give the same compression force actually developed in compression zone of width b(actual)

Page 43: Lecture 6 - Flexure

ACI Code Provisions for ACI Code Provisions for Estimating bEstimating beffeff

From ACI 318, Section 8.10.2

T Beam Flange:

eff

f w

actual

4

16

Lb

h b

b

Page 44: Lecture 6 - Flexure

ACI Code Provisions for ACI Code Provisions for Estimating bEstimating beffeff

From ACI 318, Section 8.10.3

Inverted L Shape Flange

eff w

f w

actual w

12

6

0.5* clear distance to next web

Lb b

h b

b b

Page 45: Lecture 6 - Flexure

ACI Code Provisions for ACI Code Provisions for Estimating bEstimating beffeff

From ACI 318, Section 8.10

Isolated T-Beams

weff

wf

42bb

bh

Page 46: Lecture 6 - Flexure

Various Possible Geometries Various Possible Geometries of T-Beamsof T-Beams

Single Tee

Twin Tee

Box