Column design
R/f details
Longitudinal steel
1. Minimum of four bars for rectangular column
2. Minimum of six bars for circular column
100As
3. A ≥ 4.0
col
100π΄π
100π΄π
≤ 6.0 &
≤ 8.0πππ π£πππ‘ππππππ¦ & βππππ§πππ‘ππππ¦ πππ π‘ ππππ’πππ , πππ ππππ‘ππ£πππ¦
π΄πππ
π΄πππ
100π΄π
But at laps
≤ 10.0 πππ πππ‘β π‘π¦πππ ππ ππππ’πππ
π΄πππ
As = total area of longitudinal steel
Acol =cross sectional area of the steel
Links
1. Minimum size= ¼ x size of the largest compression bar but not less than 6 mm
2. Maximum spacing = 12 x size of the smallest compression bar
3. The links should be arranged so that every corner bar and alternate bar or
group in an outer layer of longitudinal steel is supported by a link
4. All other bars or groups not restrained by link should be within 150 mm of
restrained bar
5. In circular columns a circular link passing around a circular arrangement of
longitudinal bars is adequate
Design of short columns
Short braced axially loaded columns
Load is perfectly axial.
The ultimate axial resistance, N = 0.4 fcu.Ac + 0.8 fy. Asc
Ac = net area of the concrete
Asc = area of the longitudinal r/f
With small eccentricity, the ultimate resistance, N = 0.4 fcu.Ac + 0.75 fy. Asc
For a rectangular column & to allow for the area of concrete displaced by
the longitudinal r/f, this equation may be modified to,
N = 0.4 fcu.bh + Asc(0.75 fy - 0.4 fcu)
Short braced columns supporting an approximately symmetrical
arrangement of beams
N = 0.35 fcu.bh + Asc(0.7 fy - 0.35 fcu)
Short columns resisting moment & axial forces
The area of longitudinal steel for these columns is determined by,
1. Using design charts or constructing M-N interaction diagrams
2. A solution of the basic design equations
3. An approximate method
Whichever the method used, a column should not be designed for a moment less
than N x emin
emin = lesser value of h/20 or 20 mm
h = overall size of the column cross section in the plane of bending
Design chart & Interaction diagrams
N = Fcc + Fsc + Fs = 0.45fcubs + fscAs’ + fsAs
M = Fcc (h/2 – s/2)
π = πΉπΆπΆ
β
π
−
2
2
+ πΉπ π
β
′
−
π
2
β
− πΉπ π − 2
s = 0.9x (depth of the stress block)
use design charts - BS 8110 (Part 3)
Design equations
The symmetrical arrangement of the r/f with As’ = As is suitable for the columns of a
building where the axial loads are the dominant forces. But some members are
required to resist axial forces combined with large bending moments.
N – normal to the section
β
π
π π + − π2 = 0.45πππ’ ππ π − + ππ π π΄′π π − π ′
2
2
This equation can be solved to give a value for π΄′π .
Equilibrium of the axial forces,
π = 0.45πππ’ ππ + ππ π π΄′π + ππ π΄π
1. Select a depth of neutral axis x
2. Determine ππ π & ππ
3. Further values of x may be selected and above steps repeated until a minimum value
for π΄′π + π΄π ππ πππ‘πππππ.
Simplified design method
As an alternative to the rigorous method, approximate method may be used
with π ≥
β
− π2
2
The moment M and the axial force N are replaced by an increased moment Ma plus a
compressive force N acting through the tensile steel As.
Hence, the member is designed as a doubly r/f section
ππ = 0.156πππ’ ππ2 + 0.95ππ¦ π΄′π π − π ′
0.95ππ¦ π΄π = 0.201πππ’ ππ + 0.95ππ¦ π΄′π
The area of As calculated is reduced by amount N/0.95fy
Biaxial bending of short columns (cl. 3.8.4.5)
ο· For most of the columns, biaxial bending will not govern the design.
ο· Internal and edge columns will not usually cause large moments in both directions.
ο· Corner columns may have to resist significant bending about both axes, but axial
loads are usually small and a design similar to the adjacent edge column is
generally adequate.
Simplified method
Column subjected to an ultimate load N & moments Mx and My about the xx and yy
axes, respectively.
If Mx/h'≥ My/b'
increase single axis
design moment
Mx'= Mx+βh'b' My
If Mx/h'< My/b'
increase single axis
design moment
My'= My+βb'h' Mx
Design of slender column
•If the slenderness ratio about either axis
>15 for a braced column
Slender column
>10 for an unbraced column
•There is a general restriction on maximum slenderness, lo ≤ 60b'
•For an unbraced column, lo ≤100b’2/h'
lo = clear distance between end restraints
b'and h'-smaller and larger dimensions of the column section.
A slender column must be designed for an additional moment caused by its
curvature at ultimate condition.
Mt = Mi + Madd = Mi + N*au
Mi = initial moment in the column,
Madd = moments caused by the deflection of the column
au = deflection of the column
ππ’ = π½π πβ
1
ππ 2
π½π =
2000 π′
b’= smaller dimension
K= reduction factor to allow for the fact that the deflection must be less when there is a
large proportion of the column section is compression.
ππ’π§ − π
π=
≤ 1.0
ππ’π§ − ππππ
Nuz=ultimate axial load ππ’π§ = 0.45πππ’ π΄π + 0.95ππ¦ π΄π π
Nbal= axial load at balanced failure ππππ = 0.25πππ’ π΄π
In order to calculate k, the area Asc of the columns r/f must be known
ο· Hence, a trial and error approach is necessary
ο· Taking initial conservative value of k=1.0
ο· Value of k are also marked on the column design chart
Braced slender column
Maximum additional moment Madd occurs near the mid height of column.
At this location ππ = π. 4π1 + 0.6π2 ≥ 0.4π2
M1 = smaller initial end moment due to design ultimate load
M2 = larger initial end moment
For the usual case with double curvature of a braced column, M1 taken as negative &
M2 as positive.
ππππ
Final design moment > π2 , π1 + ππππ , π1 +
ππ
2
β
π ∗ ππππ π€ππ‘β ππππ <
ππ 20 ππ
20
Ratio of the lengths of the sides ≤ 3
Slenderness ratio
ππ
β
πππ ππππ’ππ ππππ‘ ππππ’π‘ ππ‘π πππππ ππ₯ππ ≤ 20