Transcript Slide 1

1C8 Advanced design
of steel structures
prepared by
Josef Machacek
List of lessons
1) Lateral-torsional instability of beams.
2) Buckling of plates.
3) Thin-walled steel members.
4) Torsion of members.
5) Fatigue of steel structures.
6) Composite steel and concrete structures.
7) Tall buildings.
8) Industrial halls.
9) Large-span structures.
10) Masts, towers, chimneys.
11) Tanks and pipelines.
12) Technological structures.
13) Reserve.
2
Objectives
Introduction
1. Buckling of plates
Buckling due to
direct stresses
Effective width
method
Shear buckling
Buckling under
local loading
Interaction N+M+F
Assessment
Notes
•
Introduction (plate stability and strength).
•
Buckling due to direct stresses.
•
Effective width method.
•
Shear buckling.
•
Buckling under local loading.
3
Objectives
Introduction
Introduction
Buckling due to
direct stresses
Effective width
method
Stability of an ideal (flat) plate:
Shear buckling
Buckling under
local loading
Interaction N+M+F
Assessment
Notes
various loading
various boundary
conditions
Solution is based on linearized relation
of a plate with „large deflections":
2
2
2
  4w
 4w
 4w 
*  w
*  w
*  w
  Nx
D 
2 2 2 
 2N xy
 Ny
0
4
x y
x y
y 4 
x 2
y 2
 x
+ relevant boundary conditions
Thereof infinitely many solutions:
• critical stresses * (or N*) – take the lowest
• respective shapes of deflection w (modes of buckling)
4
Objectives
Introduction
Introduction
Buckling due to
direct stresses
Effective width
method
Critical stresses are given as:
 cr  k σ   E
Shear buckling
Buckling under
local loading
critical stress factor
Interaction N+M+F
Assessment
"Euler stress"
Notes
PE
b
1
PE
or
 cr  k   E
Euler stress
E
Auxiliary value, for a compression strut of width "1":
2
PE
 2D
 2E  t 
t
E 



189800


 
1  t 1  t  b 2 12 1   2  b 
b

Critical stress factor:
k = 4
(depends on loading and
boundary conditions,
see literature)
k = 23,9
2

b
k = 5,34  4 
a
2
for
a
1
b
5
Objectives
Introduction
Introduction
Buckling due to
direct stresses
Effective width
method
Strength of an actual (imperfect) plate:
Shear buckling
Equations of a plate with „large deflections“ (Karman’s equations):
Buckling under
local loading
(1)
Interaction N+M+F
Assessment
(2)
  4w
  2  2w
 4w
 4w 
 2  2w  2  2w 



 0
D 4 2 2 2 
Et  2
2

4 
2
2
2 
x y
y 
 x
 y x 2 x y x y x y 
4
4
4
2
2
 
 
   w  w   2w 
 0
2 2 2 


x 4
 x y
y 4 x 2 y 2  xy 
Notes
Plate imperfections
stability
(buckling modes)
b
initial
deflections
residual stresses due to welding
cr,1
a
idealized
real
w0 = b/200
cr,1
w0
cr,1
w0
weld
6
Objectives
Introduction
Introduction
Buckling due to
direct stresses
Effective width
method
Example of a compression plate with initial deflections and
residual stresses:
Shear buckling
t
Buckling under
local loading
Interaction N+M+F
beff/2
b
beff/2
Assessment
initial
deflection
Notes
max = fy
Resulting strengths are used in the form of reduction (buckling)
factors  :


fy
beff

b
b
    db
0
7
Objectives
Introduction
Buckling due to direct stresses
Buckling due to
direct stresses
Effective width
method
Eurocode 1993-1-5: Plated structural elements
Shear buckling
1. Buckling due to direct stress (loading N, M):
Buckling under
local loading
Verification of class 4 cross sections:
Interaction N+M+F
Assessment
Notes
a) effective width method, in which the buckling parts of plates are
excluded,
b) reduced stress method, in which the stresses of full cross section are
determined and limited by buckling reduction factors x, z, w:
Ieff
a) aAeffA,effI,eff
b)b A,A,I I

x x
eMe
x x, zz,

w
M
Note:
b) does not include stress redistribution after buckling among
individual parts of cross section!!!
8
Objectives
Introduction
Buckling due to direct stresses
Buckling due to
direct stresses
Effective width
method
Reduction (buckling) factors:
Shear buckling
Internal elements:
Buckling under
local loading
Interaction N+M+F

 p  0,055 3   

Assessment
2
p
 1,0
p 
fy
 cr

b/t
28 ,4  k σ
 = 2/1
Notes
For outstand compression elements similarly:

 p  0,188

2
p
 1,0
For k see next tables or Eurocode.
9
Objectives
Effective width method
Introduction
Buckling due to
direct stresses
Effective width method
Effective width
method
The effectivep area of the compression zone of a plate:
Shear buckling
Interaction N+M+F
internal elements:  = 1/2
•
Buckling under
local loading
Ac,eff   Ac
1
2
Assessment
be1
1 >  ≥ 0:
beff = b
be2
bc
2
beff
5 
be2 = beff - be1
b
Notes
be1 
bt
 < 0:
be1
be2
beff =  bc = b / (1-)
be1 = 0,4 beff
be2 = 0,6 beff
b
Factors k

1
1>>0
0
0 >  > -1
-1
-1 >  > -3
k
4,0
8,2/(1,05+)
7,81
7,81-6,29+9,782
23,9
5,98(1-)2
10
Objectives
Introduction
Effective width method
Buckling due to
direct stresses
Effective width
method
•
outstand elements:
beff
Shear buckling
Buckling under
local loading
1 >  ≥ 0:
1
2
 = 1/2
beff =  c
c
bt
bc
1
2
 < 0:
beff =  bc =  c /(1- )
beff
Interaction N+M+F
Assessment
Notes

1
0
-1
1 ≥  ≥ -3
k
0,43
0,57
0,85
0,57-0,21+0,0782
beff
1 >  ≥ 0:
1
2
beff =  c
beff
 < 0:
1
c
bc
bt
2
beff =  bc =  c /(1- )
Factors k

1
1>>0
0
0>>-1
-1
k
0,43
0,578/(+0,34)
1,70
1,7-5+17,12
23,8
11
Objectives
Introduction
Effective width method
Buckling due to
direct stresses
Effective width
method
Shear buckling
Effective cross sections (class 4 cross sections):
axial compression
moment
Buckling under
local loading
eM
eM
Interaction N+M+F
Assessment
eN
Notes
this eccentricity invokes additional moment from the axial
force due to shift of neutral axis in interaction of M - N
Effective parameters of class 4 cross sections (Aeff, Weff) are determined
by common way.
Verification of cross section in ULS:
1 
NEd
M  NEd eN
 Ed
 1,0
f y Aeff
f y Weff
 M0
(in stability checks:
introduce , LT)
 M0
12
Objectives
Introduction
Effective width method
Buckling due to
direct stresses
Effective width
method
Stiffened plates:
Ac,eff,loc
b1,edge,eff
b3,edge,eff
Shear buckling
Buckling under
local loading
Interaction N+M+F
Examples:
- stiffened flange of a box girder,
- web of a deep girder.
Assessment
2
b
2

2 b 3
b1
b2 2
3
2
2
2
b1
Notes
middle part

1
b2
b3
edges
Ac,eff   c Ac,eff,loc   bedge,eff t
global buckling reduction factor
(approx. given by reduction factor of the effective stiffener
- possible to calculate as a strut in compression)
[For more details see course:
Stability of plates]
13
Objectives
Introduction
Effective width method
Buckling due to
direct stresses
Effective width
method
Example of buckling of longitudinally and transversally stiffened flange
of a box girder:
Shear buckling
Buckling under
local loading
Interaction N+M+F
Assessment
Notes
14
Objectives
Introduction
Shear buckling
Buckling due to
direct stresses
Effective width
method
Shear buckling
Buckling under
local loading
Interaction N+M+F
2. Shear buckling (loading by shear force V):
Rotating stress field theory is used. Influence of stiffeners is included
proportionally to higher critical stress – after modification agrees with
tests.
Design resistance to shear (including shear buckling):
Assessment
Notes
 f y hw t
 = 1,2 up to steels S460
235
3  M1
fy
contribution from the flanges (can be ignored)
contribution from the web
Vb,Rd  Vbw,Rd  Vbf,Rd 

tf
Verification of ULS:
VEd
3 
 1,0
Vb,Rd
t
hw
tf
bf
15
Objectives
Introduction
Shear buckling
Buckling due to
direct stresses
Effective width
method
Shear buckling
Buckling under
local loading
Shear buckling may be ignored for web slenderness:
hw 72
(i.e. 60 for S235)
unstiffened webs


t

stiffened webs
(transverse, longitudinal)
hw 31

 k
t

Interaction N+M+F
Assessment
Notes
Forming of tension diagonals
in panels:
Vcr
Vt
Vf
Vcr
Phase 1
Beam behaviour
Phase 2
Vt Truss behaviour
Vf
Phase 3
frame behaviour
(influence of several %)
16
Objectives
Introduction
Shear buckling
Buckling due to
direct stresses
Effective width
method
Contribution from the web
Vbw,Rd 
 w fyw hw t
3  M1
Shear buckling
Buckling under
local loading
Factor w for the contribution of the web to the shear buckling resistance
may be (in acc. to tests) increased for rigid end post and internal panels:
Interaction N+M+F
Slenderness
Rigid end post
Non-rigid end post
 w  0,83 / 


Assessment
Notes
0,83 /  w
0 ,83 /    w  1,08

1,37 / 0,7   w
 w  1,08
w
1,2
1
Rigid end post
difference 22%

0,83 /  w
0,83 /  w
Reason:
anchorage
of panels →
Non-rigid end post
1
2
w
17
Objectives
Introduction
Shear buckling
Buckling due to
direct stresses
Effective width
method
Shear buckling
Web slenderness
w
• unstiffened webs (with the exception at the beam ends):
Buckling under
local loading
w 
Interaction N+M+F
Assessment
fy / 3
 cr

hw
86,4 t 
• webs with transverse stiffeners in distance a:
Notes
hw
w 
hw
37,4 t 
na
k
Critical stress factor k:
k   5 ,34  4 ,00 hw / a 
2
k   4 ,00  5 ,34 hw / a 
2
as far as a / hw  1
as far as a / hw  1
[For webs with longitudinal stiffeners see course: Stability of plates]
18
Objectives
Introduction
Buckling under local loading
Buckling due to
direct stresses
Effective width
method
3. Buckling under local loading
3 types of loading are distinguished:
Shear buckling
a) through the flange ,
Buckling under
local loading
b) through the flange and transferred directly to the other one,
c) through the flange adjacent to an unstiffened end.
Interaction N+M+F
Type (a)
Fs
Assessment
Notes
ss
V1,s
Type (b)
Fs
V
V2,s
2,s
hw
Type (c)
Fs
ss
c
ss
Vs
a
Local design resistance:
FRd  Leff t w
fy
 M1
reduction factor due to local buckling
(governed by critical stress)
effective length of web Leff = Fℓy
effective loaded length
(governed by ss)
[In detail see Eurocode, or course: Stability of plates]
19
Objectives
Introduction
Buckling under local loading
Buckling due to
direct stresses
Effective width
method
Example of local web buckling:
Shear buckling
Buckling under
local loading
Interaction N+M+F
Assessment
Notes
20
Objectives
Introduction
Interaction N + M + F
Buckling due to
direct stresses
Effective width
method
Shear buckling
Buckling under
local loading
Verification for local buckling:
FEd
2 

FRd
FEd
Leff t w
Interaction
N+M+F
Assessment
Notes
fy
 1,0
 M1
Interaction N + M + F:
 2  0,8 1  1,4
i.e.:
FEd
Leff t w
fy
 M1




M  NEd eN 
 N
 0,8  Ed  Ed
  1,4
fy Aeff
fy Weff


 M0
  M0

21
Objectives
Introduction
Buckling due to
direct stresses
Effective width
method
Assessment
• Ideal and actual plate – differences.
Shear buckling
Buckling under
local loading
Interaction N+M+F
Assessment
Notes
• Eurocode approaches concerning
buckling effects.
• Verification of class 4 sections.
• Design resistance to shear.
• Behaviour of webs under shear.
• Types of local loading.
• Verification for local loading.
22
Objectives
Introduction
Notes to users of the lecture
Buckling due to
direct stresses
Effective width
method
•
This session requires about 90 minutes of lecturing.
Shear buckling
•
Within the lecturing, buckling of plates under direct, shear and
local loading is described. The lecture starts with linear theory
of buckling and resulting critical stress, followed with nonlinear theory of buckling of actual imperfect plate and its
resistance. The buckling resistances under direct stress,
shear and local loading in accordance with Eurocode are
commented.
•
Further readings on the relevant documents from website of
www.access-steel.com and relevant standards of national
standard institutions are strongly recommended.
•
Keywords for the lecture:
Buckling under
local loading
Interaction N+M+F
Assessment
Notes
buckling of plates, ideal plate, real plate, buckling due to direct
stresses, buckling under shear, local buckling, interaction
formulas for buckling.
Objectives
Introduction
Notes for lecturers
Buckling due to
direct stresses
Effective width
method
•
Subject: Buckling of plates.
Shear buckling
•
Lecture duration: 90 minutes.
•
Keywords: buckling of plates, ideal plate, real plate, buckling
due to direct stresses, buckling under shear, local buckling,
interaction formulas for buckling.
•
Aspects to be discussed: Ideal plate, critical stress, real plate,
reduction factor. Behaviour of plates under shear loading.
Behaviour of plates under local loading. Eurocode approach.
•
After the lecturing, determination of effective cross section
parameters (class 4 effective parameters) should be
practised.
•
Further reading: relevant documents www.access-steel.com
and relevant standards of national standard institutions are
strongly recommended.
•
Preparation for tutorial exercise: see examples prepared for
the course.
Buckling under
local loading
Interaction N+M+F
Assessment
Notes
24