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Steel Design - Compression Member - Ari Wibowo, Ph.D
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3 - Compression Member.pdf

May 02, 2017

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Page 1: 3 - Compression Member.pdf

Steel Design- Compression Member -

Ari Wibowo, Ph.D

Page 2: 3 - Compression Member.pdf

Compression Members

• Compression Members: Structural elements that are

subjected only to axial compressive forces.

• The stress can be taken as:

fa = P/A

where fa is considered to be uniform over the entire

cross section.

• This ideal state is never achieved in reality, because

some eccentricity of the load is inevitable.

Page 3: 3 - Compression Member.pdf

Columns: are the most common type of compression members occurring in buildings

and bridges.

Sometimes members are also called upon to resist bending, and in these cases the

member is a beam column.

Page 4: 3 - Compression Member.pdf

Compression Members

• Column Theory:

– Consider the long, slender compression

member.

– If the axial load P is slowly applied. it will

ultimately become large enough to cause

the member to buckle/become unstable.

– Assume the shape indicated by the dashed

line. The member is said to have buckled.

– The load at which buckling occurs is a

function of slenderness, and for very

slender members this load could be quite

small.

Page 5: 3 - Compression Member.pdf

Compression Members

Column Theory:

• The critical buckling load Pcr :

– the load that is just large enough to deflect the column

without subjected to transverse load.

– If the member is so slender, the stress just before

buckling is below the proportional limit - and the

member is still elastic - the critical buckling load is given

by:

Page 6: 3 - Compression Member.pdf

Compression Members

Page 7: 3 - Compression Member.pdf

Compression Members

• For example, case n=1,

this equation can be rewritten as :

Where:

– A is the cross-sectional area .

– r is the radius of gyration with respect to the axis of

buckling.

–The ratio L/r is the slenderness ratio .

•If the critical load is divided by the cross-sectional area,

the critical buckling stress is obtained:

Page 8: 3 - Compression Member.pdf

A WI2 x 50 is used as a column to support an axial compressive load

of 145 kips. The length is 20 feet, and the ends are pinned. Without

regard to load or resistance factors, Investigate this member for stability.

Example 1

Because the applied load of 145 kips is less than Pcr the

column remains stable and has an overall factor of safety

against buckling of 278.9/145 = 1.92

Page 9: 3 - Compression Member.pdf

Effective Length

2

2

2

2

4)2( L

EI

L

EIPcr

• Fixed and Free Ends

• Both Fixed Ends

• Fixed and Pinned Ends

• Fixed and Fixed Roller Ends

2

2

2

2 4

)5.0( L

EI

L

EIPcr

2

2

)7.0( L

EIPcr

2

2

)5.0( L

EIPcr

Page 10: 3 - Compression Member.pdf

Braced Columns

Page 11: 3 - Compression Member.pdf

Column (a)

Top : KL = 2 0.7L = 1.4 L (largest governs)

Bottom : KL = 1 0.3 = 0.3 L

Column (b)

Top : KL = 0.7 0.5 L = 0.35 L (largest governs)

Middle : KL = 1 0.3 L = 0.3 L

Bottom : KL = 0.7 0.2 L = 0.14 L

Page 12: 3 - Compression Member.pdf

Example

• Column W12 65, 12 ft, with beam constructed at x-x

axis. Determine which axis govern for compression

member calculation.

Page 13: 3 - Compression Member.pdf

in

tft

r

LK ftin

x

x

28.5

)12(24

02.3

)12(4.8

x

x

r

LK

• X axis (major/strong axis)

Kx = 2 12 = 24 ft

= 54.55

Hence, x-x axis controls since it has the biggest slenderness

ratio

• Y axis (minor/weak axis)

Ky = 0.7 12 = 8.4 ft

= 33.38

Page 14: 3 - Compression Member.pdf

Compression Members

• LRFD METHOD :

Factored load ≤ factored strength

Pu ≤ Øc Pn

Where

Slenderness parameter is used instead of Fcr as a function of

the slenderness ratio KL/r

= Sum of factored LoadsPu

= Nominal compressive strength =Ag FcrPn

C= ritical buckling stressFcr

= Resistance factor for compression member = 0.85Øc

Page 15: 3 - Compression Member.pdf

AISC REQUIRMENTS

– Critical buckling stress will be summarized as:

– Also, Graphically can be summarized as:

Page 16: 3 - Compression Member.pdf

SNI 03-1729-2002

• Nominal Load:

• Critical stress:

y

gcrgn

fAfAP ..

y

cr

ff

1

c

67.06.1

43.1

225.1 c

where:

• For c 0.25 :

(SNI 03-1729-2002 pers. 7.6-5a)

• For 0.25 < c < 1.2 :

(SNI 03-1729-2002 pers. 7.6-5b)

• For 0.25 1.2 :

Page 17: 3 - Compression Member.pdf

Compression Members

ExExample:4.2ample 4.2:

Compute the design compressive strength of a W14 x 74 with a length of 20 feet and pinned ends.

A992 steel is used.

Page 18: 3 - Compression Member.pdf

Local Buckling

• If local buckling of the individual plate elements occurs, then the

column may not be able to develop its buckling strength.

• Therefore, the local buckling limit state must be prevented from

controlling the column strength.

• Two types of elements must be considered:

– unstiffened elements, which are unsupported along one edge

parallel to the direction of load, and

– stiffened elements, which are supported along both edges.

• The strength must be reduced if the shape has any slender elements.

Page 19: 3 - Compression Member.pdf

20

Local Buckling

Local buckling depends on the slenderness (width-to- thickness b/t ratio) of the plate element and the yield stress (Fy) of the material.

Each plate element must be stocky enough, i.e., have a b/t ratio that prevents local buckling from governing the column strength.

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21

Local Buckling

Page 21: 3 - Compression Member.pdf

Local Buckling

Flange Buckling

Laterally buckled beams

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23

Local Buckling

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Local Buckling- AISC

Cross-sectional shapes are classified as compact, non compact, or

slender, according to the values of the width-thickness ratios. If λ is

greater than the specified limit, denoted λr the shape is slender.

• Unstiffened Element

– For I- and H-shapes, the projecting flange is considered to be an

unstiffened element, and its width can be taken as half the full

nominal width

– where bf and tf are the width and thickness of the flange.

– The upper limit is (AISC)

Page 24: 3 - Compression Member.pdf

Local Stability - AISC

• Stiffened Elements

–The webs of I- and H-shapes are stiffened elements. and the

stiffened width is the distance between the roots of the flanges.

–The width thickness parameter is

–Where h is the distance between the roots of the flanges, and tw

is the web thickness.

–The upper limit is (AISC)

Page 25: 3 - Compression Member.pdf

AISC

Steel shape profile and value of r according to AISC

Page 26: 3 - Compression Member.pdf

Compression Members

•Local Stability:

Page 27: 3 - Compression Member.pdf

Compression Members•Local Stability:

Page 28: 3 - Compression Member.pdf

Compression Members

•Local Stability:

Page 29: 3 - Compression Member.pdf

Local Stability - SNI 03-1729-2002

This critical stress formula applies if the ratio of width to the thickness

() is smaller than r on Table 7.5-1 SNI 03-1729-2002. Ratio can

be h/tw or b/tf, depending on the element, such as : (Note: fy in Mpa)

f

ff

t

b

t

b

t

b

2

2/

yf

250

wt

h

yf

665

• Unstiffened element : without stiffener along one side parallel

to load direction.

e.g.: flange on I or H profile shape

= ; Upper limit : r =

• Stiffened Element.

e.g.: web on I or H profile shape

= ; Upper limit: r =

Page 30: 3 - Compression Member.pdf

SNI 03-1729-2002

Steel shape profile and value of r according to SNI 03-1729-2002

Page 31: 3 - Compression Member.pdf

Compression Members•Local Stability:

Example 4.3:

–Investigate the column in example 4.2 for local stability.

Page 32: 3 - Compression Member.pdf

Compression Members

•DESIGN:

–Example 4.5:

A compression member is subjected to service loads of 165 kips

dead load and 535 kips live load. The member is 26 feet long and

pinned at each end. Use A992 steel

Answer

Page 33: 3 - Compression Member.pdf

Compression Members

•DESIGN:

–Example 4.6:

Page 34: 3 - Compression Member.pdf

Compression Members

•DESIGN:

–Example 4.7:

Answer

Page 35: 3 - Compression Member.pdf

Compression Members•DESIGN:

Page 36: 3 - Compression Member.pdf

Compression Members

•DESIGN:

Page 37: 3 - Compression Member.pdf

Compression Members

Page 38: 3 - Compression Member.pdf

Slenderness Ratio

The longer the column, for the same x-section,

the greater becomes its tendency to buckle and

smaller becomes its load carrying capacity.

The tendency of column to buckle is usually

measured by its slenderness ratio

Compression Members Vs

Tension Members

Page 39: 3 - Compression Member.pdf

40

Compression Members Vs

Tension Members

Effect of material Imperfections and Flaws

Slight imperfections in tension

members are can be safely disregarded

as they are of little consequence.

On the other hand slight defects in

columns are of great significance.

A column that is slightly bent at the time

it is put in place may have significant

bending resulting from the load and

initial lateral deflection.

Page 40: 3 - Compression Member.pdf

41

Tension in members causes lengthening of members.

Compression beside compression forces causes buckling of member.

Compression Members Vs

Tension Members

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42

Presence of holes in bolted connection reduce Gross area in tension members.

Presence of bolts also contribute in taking load An = Ag

Compression Members Vs

Tension Members

Page 42: 3 - Compression Member.pdf

43

WHY column more critical

than tension member?

A column is more critical than a

beam or tension member because

minor imperfections in materials

and dimensions mean a great

deal.

Page 43: 3 - Compression Member.pdf

The bending of tension members

probably will not be serious as the

tensile loads tends to straighten

those members, but bending of

compression members is serious

because compressive loads will tend

to magnify the bending in those

members.

WHY column more critical

than tension member?