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ADVANCED MECHANICS OF
SOLIDS (CE-305)
Dr. Zafar Baig
Assistant Professor
Department of Civil Engineering
University of Management and Technology
MAXIMUM STRESS IN ECCENTRIC COLUMN
The maximum stress σmax occurs in the section
of the column where the bending moment is
maximum, i.e., in the transverse section
through the midpoint C, and can be obtained
by adding the normal stresses due to the axial
force and the bending couple exerted on that
section
2
max
max
max
max
)
(
)
31
(
Ar
c
e
y
P
A
P
I
c
M
A
P

















 1
2
sec
max
kL
e
y
)
( max e
y
P
MC 









 1
2
sec
max
cr
P
P
e
y
OR

)
32
(
2
sec
1
1
1
2
sec
1
1
2
sec
1
)
(
2
max
2
max
2
max
2
max
max


















































kL
r
ec
A
P
r
ec
kL
A
P
r
c
e
kL
e
A
P
Ar
c
e
y
P
A
P




Replacing the value of kL /2 as following
cr
P
P
L
EI
P
kL
2
2
2



)
33
(
2
sec
1
)
32
( 2
max 








cr
P
P
r
ec
A
P 

e = eccentricity of loading
c = distance from the N.A.
to extreme fibres
r = radius of gyration
A = cross-sectional area of
column
The Eqn. (33) can be used for any end condition as long as
the appropriate (K) value is used to calculate Pcr.
Since σmax does not vary linearly with load P, the principal
of superposition is not applicable to determine the stress due
to the simultaneously application of applied loads.
For the same reason any factor of safety should be used with
load not the stress.
)
34
(
2
1
sec
1
2
sec
1
2
sec
1
)
32
(
2
max
2
2
max
2
max



































r
L
EA
P
r
ec
A
P
L
EAr
P
r
ec
A
P
L
EI
P
r
ec
A
P
e
e


 2
Ar
I 

ratio
ty
Eccentrici
r
ec

2
angle
Euler
L
EAr
P e

2
2
 If the material properties, the dimensions of the column,
and the eccentricity e are known then we have two variables
in the secant formula: P and σmax. If P is also given, σmax
can be computed from the formula without difficulty.
The formula given in Eqn. (34) is referred to as the secant
formula; it defines the force per unit area (P/A), that causes a
specified maximum stress (σmax) in a column of given
effective slenderness ratio (Le /r), for a given value of the
eccentricity ratio (ec/r2).
)
34
(
2
1
sec
1 2
max


















r
L
EA
P
r
ec
A
P
e

 On the other hand, if σmax is specified, the determination
of P is considerably more complicated because Eqn. (33),
being nonlinear in P, must be solved by trial-and-error.
 The secant formula is mainly useful for intermediate
values of Le /r. However, to use it effectively, we
should know the value of the eccentricity e of the
loading


















r
L
EA
P
r
ec
A
P
e
2
1
sec
1 2
max

MPa
E
MPa
y
200
250
max


 


2
r
ec

2
r
ec

2
r
ec

2
r
ec


















r
L
EA
P
r
ec
A
P
e
2
1
sec
1 2
max

 Due to imperfections in manufacturing or specific
application of the load, a column will never suddenly
buckle; instead, it begins to bend.
 The load applied to a column is related to its deflection
in a nonlinear manner, and so the principle of
superposition does not apply.
 As the slenderness ratio increases, eccentrically loaded
columns tend to fail at or near the Euler buckling load.
Exercise: Plot the load-displacement curves of a rectangular column
for the given data with eccentricity ranging from 5-25 mm.
Data
L= 2.5 m K = 1.0, A = 30x60 mm2, e = 5 – 25 mm
Solution Imin= 60x303/12= 135,000 mm4 , rmin = 8.66 mm
P (kN) Sec(kL/2) y (mm)
0 e = 5 e =10 e =15 e =20 e =25
10
20
30
40
42.64















 1
2
sec
1
2
sec
max
cr
P
P
e
kL
e
y

kN
Pcr 64
.
42
)
2500
1
(
10
135
10
200
2
3
3
2








Problem 10.34 (Mech. of Materials, Bear & Johnston, 6th Ed)
The axial load P is applied at a point located on the x-axis at a
distance e from the geometric axis of the rolled-steel column BC.
When P = 350 kN, the horizontal deflection of the top of the
column is 5 mm. Using E =200 GPa. determine
(a) the eccentricity e of the load,
(b) the maximum stress in the column.
Data
For W250x58 Section
A= 7420 mm2 Sy = 185x103 mm3
Ix = 8700x104 mm4, rx = 108 mm
Iy = 1870x104 mm4, ry = 50.3 mm
E = 200 GPa, d = 250 mm, bf =203 mm
K = 2.0 (cantilever case), ymax = 5mm
Sample Problem 10.3:(Mech. of Materials, A Pytel, 2nd Ed)
A W14x61 section is used as a simply supported column of 25 ft
long. When the 150-kip load is applied with the 4-in. eccentricity
shown, Determine
(1) the maximum compressive stress in the column;
(2) the factor of safety against yielding; and
(3) The maximum lateral deflection.
Assume that the column does not buckle about the y-axis.
Use E = 29x106 psi and σy = 36x103 psi..
For W350x58 Section
A= 17.9 in2 Ix = 640 in4
Sx = 92.1 in3 , ey = 4 in ,
d = 14 in L = 25 ft
x
y
x
y
I
C
M
A
P 


max
max
 







cr
P
P
r
ec
A
P
2
sec
1 2
max


P
P
FOS
y

A
P
A
P
y
y
y
y .

 

















 1
2
sec
1
2
sec
max
cr
P
P
e
kL
e
y

2
2
e
x
cr
L
EI
P


(1) The maximum compressive stress in the column
(2) The factor of safety against yielding
(3) The maximum lateral deflection.

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Lec 27 - Columns 3.pdf

  • 1. 1   ADVANCED MECHANICS OF SOLIDS (CE-305) Dr. Zafar Baig Assistant Professor Department of Civil Engineering University of Management and Technology
  • 2. MAXIMUM STRESS IN ECCENTRIC COLUMN The maximum stress σmax occurs in the section of the column where the bending moment is maximum, i.e., in the transverse section through the midpoint C, and can be obtained by adding the normal stresses due to the axial force and the bending couple exerted on that section 2 max max max max ) ( ) 31 ( Ar c e y P A P I c M A P                   1 2 sec max kL e y ) ( max e y P MC            1 2 sec max cr P P e y OR 
  • 3. ) 32 ( 2 sec 1 1 1 2 sec 1 1 2 sec 1 ) ( 2 max 2 max 2 max 2 max max                                                   kL r ec A P r ec kL A P r c e kL e A P Ar c e y P A P     Replacing the value of kL /2 as following cr P P L EI P kL 2 2 2    ) 33 ( 2 sec 1 ) 32 ( 2 max          cr P P r ec A P   e = eccentricity of loading c = distance from the N.A. to extreme fibres r = radius of gyration A = cross-sectional area of column
  • 4. The Eqn. (33) can be used for any end condition as long as the appropriate (K) value is used to calculate Pcr. Since σmax does not vary linearly with load P, the principal of superposition is not applicable to determine the stress due to the simultaneously application of applied loads. For the same reason any factor of safety should be used with load not the stress. ) 34 ( 2 1 sec 1 2 sec 1 2 sec 1 ) 32 ( 2 max 2 2 max 2 max                                    r L EA P r ec A P L EAr P r ec A P L EI P r ec A P e e    2 Ar I   ratio ty Eccentrici r ec  2 angle Euler L EAr P e  2 2
  • 5.  If the material properties, the dimensions of the column, and the eccentricity e are known then we have two variables in the secant formula: P and σmax. If P is also given, σmax can be computed from the formula without difficulty. The formula given in Eqn. (34) is referred to as the secant formula; it defines the force per unit area (P/A), that causes a specified maximum stress (σmax) in a column of given effective slenderness ratio (Le /r), for a given value of the eccentricity ratio (ec/r2). ) 34 ( 2 1 sec 1 2 max                   r L EA P r ec A P e 
  • 6.  On the other hand, if σmax is specified, the determination of P is considerably more complicated because Eqn. (33), being nonlinear in P, must be solved by trial-and-error.  The secant formula is mainly useful for intermediate values of Le /r. However, to use it effectively, we should know the value of the eccentricity e of the loading
  • 9.  Due to imperfections in manufacturing or specific application of the load, a column will never suddenly buckle; instead, it begins to bend.  The load applied to a column is related to its deflection in a nonlinear manner, and so the principle of superposition does not apply.  As the slenderness ratio increases, eccentrically loaded columns tend to fail at or near the Euler buckling load.
  • 10. Exercise: Plot the load-displacement curves of a rectangular column for the given data with eccentricity ranging from 5-25 mm. Data L= 2.5 m K = 1.0, A = 30x60 mm2, e = 5 – 25 mm Solution Imin= 60x303/12= 135,000 mm4 , rmin = 8.66 mm P (kN) Sec(kL/2) y (mm) 0 e = 5 e =10 e =15 e =20 e =25 10 20 30 40 42.64                 1 2 sec 1 2 sec max cr P P e kL e y  kN Pcr 64 . 42 ) 2500 1 ( 10 135 10 200 2 3 3 2        
  • 11. Problem 10.34 (Mech. of Materials, Bear & Johnston, 6th Ed) The axial load P is applied at a point located on the x-axis at a distance e from the geometric axis of the rolled-steel column BC. When P = 350 kN, the horizontal deflection of the top of the column is 5 mm. Using E =200 GPa. determine (a) the eccentricity e of the load, (b) the maximum stress in the column. Data For W250x58 Section A= 7420 mm2 Sy = 185x103 mm3 Ix = 8700x104 mm4, rx = 108 mm Iy = 1870x104 mm4, ry = 50.3 mm E = 200 GPa, d = 250 mm, bf =203 mm K = 2.0 (cantilever case), ymax = 5mm
  • 12. Sample Problem 10.3:(Mech. of Materials, A Pytel, 2nd Ed) A W14x61 section is used as a simply supported column of 25 ft long. When the 150-kip load is applied with the 4-in. eccentricity shown, Determine (1) the maximum compressive stress in the column; (2) the factor of safety against yielding; and (3) The maximum lateral deflection. Assume that the column does not buckle about the y-axis. Use E = 29x106 psi and σy = 36x103 psi.. For W350x58 Section A= 17.9 in2 Ix = 640 in4 Sx = 92.1 in3 , ey = 4 in , d = 14 in L = 25 ft x y
  • 13. x y I C M A P    max max          cr P P r ec A P 2 sec 1 2 max   P P FOS y  A P A P y y y y .                      1 2 sec 1 2 sec max cr P P e kL e y  2 2 e x cr L EI P   (1) The maximum compressive stress in the column (2) The factor of safety against yielding (3) The maximum lateral deflection.