45
Presentation on uniaxial column design Presented by Md. Saifur Rahman Sayeef Student ID: 10.01.03.160 Department of Civil Engineering AUST, Dhaka

10.01.03.160

Embed Size (px)

Citation preview

Page 1: 10.01.03.160

Presentation on

uniaxial column design

Presented by

Md. Saifur Rahman Sayeef

Student ID: 10.01.03.160

Department of Civil Engineering

AUST, Dhaka

Page 2: 10.01.03.160

UNIAXIAL COLUMN DESIGN

Page 3: 10.01.03.160

WHAT IS UNIAXIAL COLUMN?

• Uniaxial columns are those whose rotation are strictly bound about a single axis only as the load eccentricity is pure about a single axis.

Page 4: 10.01.03.160

Bending moments can occur in columns because:

• - Unbalance gravity loads

• - Lateral loads: wind, earthquake

• - In general a certain degree of eccentricity is present due to inaccuracies in construction.

Page 5: 10.01.03.160

The column types depending on applied load.

Page 6: 10.01.03.160

Column types

Page 7: 10.01.03.160

Column types based on dimensional property

SHORT – both lex/h and ley/b < 15 for braced columns

< 10 for unbraced columns

BRACED - If lateral stability to structure as a whole is

provided by walls or bracing designed to resist all lateral

forces in that plane, else unbraced.

Page 8: 10.01.03.160

UNIAXIAL SHORT COLUMN DESIGN BY INTERACTION CURCVE (USD) METHOD

Page 9: 10.01.03.160

Column subjected to eccentric compression

Page 10: 10.01.03.160
Page 11: 10.01.03.160

Balanced Failure, eb

Page 12: 10.01.03.160
Page 13: 10.01.03.160
Page 14: 10.01.03.160

Moment Strength of Column

Page 15: 10.01.03.160
Page 16: 10.01.03.160
Page 17: 10.01.03.160
Page 18: 10.01.03.160
Page 19: 10.01.03.160
Page 20: 10.01.03.160
Page 21: 10.01.03.160
Page 22: 10.01.03.160
Page 23: 10.01.03.160
Page 24: 10.01.03.160
Page 25: 10.01.03.160
Page 26: 10.01.03.160
Page 27: 10.01.03.160

UNIAXIAL SHORT COLUMN DESIGN BY (WSD) METHOD

Page 28: 10.01.03.160

1. If column controlled by compression eccentricity, e= M/P <= eb :-

• For symmetrical tied column, eb=

(0.67Pgm+0.17)d

• For spiral column, eb=

(0.43PgmDs+0.14t)

• Pg= As/Ag

• m= fy/0.85f’c

Page 29: 10.01.03.160

Selection of column is done using the relation –

(fa/Fa) + (fb/Fb) <=1, (this is also known as interaction formula.)

Where,fa= P/Ag

Fa= 0.34(1+Pgm)fc’fb= M/SS= I/c (c=0.5h)Fb= 0.45 fc’

Page 30: 10.01.03.160

2. If column controlled by tension, e>eb

Section of column shall be proportioned by using the relation-

M= Mo+ P/Pb (Mb-Mo)Pb & Mb shall be calculated by using the relation-(fa/Fa) + (fb/Fb)= 1=> (Pb/Ag)/Fa + (Pbeb/S)/Fb= 1

For symmetrical tied column, Mo= 0.4 As fy (d-d’), As is tensile steel.

For spiral column, Mo= 0.12 Ast fy Ds, Ast is total steel.

Page 31: 10.01.03.160

SLENDER COLUMN DESIGN

Page 32: 10.01.03.160

Slender columns are also becoming increasingly important and popular because of the following reasons:

(i) the development of high strength materials (concrete and steel),

(ii) improved methods of dimensioning and designing with rational and reliable design

procedures,

(iii) innovative structural concepts – specially, the architect’s expectations for creative structures.

Page 33: 10.01.03.160

HYSTERESIS?

• slender or long columns may fail at a much lower value of the load compared to short column when sudden lateral displacement of the member takes place between the ends. Thus, short columns undergo material failure, while long columns may fail by buckling (geometric failure) at a critical load or Euler’s load, which is much less in comparison to that of short columns having equal area of cross-section.

• The general expression of the critical load Pcr at which a member will fail by buckling is as follows:

• Pcr = π2EI /(kl)2 or,

• Pcr = π2EA /(kl/r)2

• Thus, Pcr of a particular column depends upon kl/r or slenderness ratio. It is worth mentioning that kl is termed as effective length le of the column.

Page 34: 10.01.03.160
Page 35: 10.01.03.160
Page 36: 10.01.03.160
Page 37: 10.01.03.160

Critical loads in terms of Pcr of hinge-hinge column and effective lengths le = klof elastic and reinforced concrete columns with different boundary conditions

and for a constant unsupported length l

Sl.

No.

Support conditions Critical load

Pcr

Effective length

le = kl

(A) Elastic single columns 1. Hinged at both ends, no

sidesway

Pcr l

2. Fixed against rotation at

both ends – no sidesway

4Pcr 0.5 l

3. Partially restrained against

rotation by top and bottom

cross-beams, no sidesway

Between Pcr and 4Pcr l > kl > l/2

4. Fixed at one end and

entirely free at other end –

sidesway not prevented

0.25 Pcr 2 l, one PI is on imaginary

extension

5. Rotationally fixed at both

ends – sidesway not

prevented

Pcr l, one PI is on imaginary

extension

6. Partially restrained against

rotation at both ends –

sidesway not prevented

Between zero and slightly

less than Pcr *

l < kl < α

(B) Reinforced concrete columns 7. Hinged portal frame – no

sidesway

> Pcr kl < l

8. Hinged portal frame –

sidesway not prevented

<< Pcr kl > 2 l

Page 38: 10.01.03.160

Additional Moment Method of analysis of short column

1.Braced columns bent symmetrically in single curvature and undergoing balanced failure

M = Mo + Py

=>Mo + P ea = Mo + Ma

• Where,

• P is the factored design load

• M are the total factored design moments

• Mo are the primary factored moments

• Ma are the additional moments

• ea are the additional eccentricities

Page 39: 10.01.03.160

DEFLECTION DIAGRAMS

Page 40: 10.01.03.160

ΦMAX= 10Δ/le2

Hence,

ea=Δ = Φ le2/10

Page 41: 10.01.03.160

Assuming the column undergoes a balanced failure when Pu= Pub, the maximum curvature at the mid-height section of the column can be expressed as given below, assuming

(i) the values of εc = 0.0035, εst = 0.002 and d’/D = 0.1, and (ii) the additional moment capacities are about eighty per cent

of the total moment. Then,

φ = eighty per cent of {(0.0035 + 0.002)/0.9D}or φ = 1/200D Substituting the value of φ , we haveea = D(le/D)2/2000

Page 42: 10.01.03.160

• Therefore, the additional moment Ma can be written as,

• Ma = Py = PΔ = Pea = (PD/2000) (le/D)2

Page 43: 10.01.03.160

2.Braced columns subjected to unequal primary moments at the two ends

• Mo max = 0.4 M1 + 0.6 M2

• Mo max ≥ 0.4 M2

Where,

• M1 is smaller end moment.

• M2 is larger end moment.

Page 44: 10.01.03.160

3. Unbraced columns

• Mo max = M2 + Ma

Page 45: 10.01.03.160