TUHH - Prof. Rombach
• Introduction
• Beam and truss structures
• Spatial structures- shear walls- slabs- shells
• Material nonlinear analysis
• 3-d models
Design of real concrete structures with finite element software- model problems and errors –Prof. Dr.- Ing. Günter A. Rombach
Hamburg University of TechnologyE-mail: [email protected]
TUHH - Prof. Rombach
Special problems of concrete structures
• complex material behaviour (cracks, time dependant)
• detailing – arrangement of rebars significant
• construction process significant
• complex loading – exact value not known
• no mass product – fast design
• massive members (Bernoulli hypothesis not valid)
TUHH - Prof. Rombach 3
Zuse Z1 1936-38
Built the first programmable ‚computer‘ in the world
• Argyris: Civil Engineer
• Clough: Civil Engineer
• Zienkiewicz: mathematician;lecturer in faculty of civil eng.
TUHH - Prof. Rombach
The Sleipner platform
accident
Collapse: August 1991
Financial loss: 250 Mio US$
TUHH - Prof. Rombach
The Sleipner platform accident
TUHH - Prof. Rombach
The Sleipner platform accident – tricells
TUHH - Prof. Rombach
The Sleipner platform accident – tricells
7
3.453.413.252.32Tension force T1 [MN/m]
1.661.671.350.95Tension force T1-D1 [MN/m]
N4N3N2N1Elementmesh
TUHH - Prof. Rombach
The Sleipner platform accident – tricells
8
TUHH - Prof. Rombach
Sleipner platform accident
9
Consequences:
• distorted 8-noded volume elementsshould not be used
• qualified staff
• indenpendant checks
Sea Troll Plattform, Bj. 1995, h=472 m (330m)
• better hard- and software
• more elements
• substructure techniques
• adaptive mesh refinement
• nonlinear material models
• independant checksengineering knowledge required
Seite:
TUHH - Prof. Rombach
Software faults• loadcase G had not been considered since version 10.0-96
• minimum reinforcement had been estimated with fyk instead of fyd
Errors
10
Numerical errors• 245 - 0,8 - 245 = 0,8008
• 250 - 0,8 - 250 = 0,00
TUHH - Prof. Rombach
Program errors
Software faults
Model errorsmaterial model reinforced concrete behaves nonlinear
loading FE-Model considers only nodal loads
design slab, shear wall, column, tension member, shear reinforcement
modelling size of elementstype of elementsupport conditionssingularities
ErrorsReales Bauwerk
Numerisches Modell
TUHH - Prof. Rombach
Modelling
12
u2
v2
ϕ2
u1ϕ1
v1 MV
N
MBemessung
FsdFcdV
N
Spannung
Knotenlasten
reale Einwirkung Beam element
Beam element
stresses
design
loading
real structure
real loading
Numerical model
beam -, plate-, shell-,volume elements
TUHH - Prof. Rombach 13
Prof. Dr.-Ing. G. A. RombachHamburg University of Technology
E-mail: [email protected]
Design of real concrete structures with finite element software
• Introduction
• Beam and truss structures• Spatial structures- shear walls- slabs- shells
• Material nonlinear analysis
TUHH - Prof. Rombach 14
Beam or truss element
Beam element
Strains stresses
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
-190.
187.
-176.
124.
8.
-137.
138.
-178.
176.
-193.
259.
-139.
122.
-141.
142.
horizontal membrane force
System
Width of beam b = 0,22 cm
see detail
Loading q = 1 kN/m
2,5m
60 80
9,5m
Discontinuity regions
TUHH - Prof. Rombach 16
D-regions in beam or truss structures
TUHH - Prof. Rombach 17
Beam with opening
2
max
2
810 12,5 195
8
q lM
kNm
⋅= =
⋅= =
max / 195 / 0,6325
N M zkN
= ± = ± == ±
TUHH - Prof. Rombach
5,0m 5,0m
50
20
10kN/m
Opening 20/50cm 5050
Model 1 Model 2 Model 3
Beam with opening
TUHH - Prof. Rombach
50.0
-50.0
50.0
-50.0-49.8
49.7
50.4
-50.3
85.0
-15.0
29.1
-70.9
20.8
-41.7-41.7 -41.7
33.0
-76.5
20.7
-42.1-40.8
-42.8
Bending Moment
Shear Forces
5,0m 5,0m
50
20
10kN/m
Opening 20/50cm
Model 3Model 2Model 1
Beam with opening
TUHH - Prof. Rombach
Stress/Strainsection 1-1left
Stress/Strain section 1-1right
Model 1 Model 21
1
Beam with opening
Stressessection 1-1 right
Stressessection 1-1 left
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
compression forces tension forces
Beam with opening - Strut-and-Tie model
Tension tieCompression strut
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Summary 1: Beam and truss structures (D-regions)
• The Bernoulli-Hypothesis (linear strain distribution) is not valid in so-calleddiscontinuity regions. Thus beam elements, which are mostly based on a linear strain distribution, can not estimate the forces in discontinuity regions.
• It is important to model the stiffness in the discontinuity regions.
• D-regions can be designed by means of strut-and-tie models whereas themember forces of the truss systems at the boundaries can be used to estimate the forces in the struts.
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Modelling of support - single span girder
rigid
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Modelling of support
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Modelling of support - single span truss
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Schornbachtalbridge
Bridge column with pile foundation
11m
15m
1,8m
Ortbetonramm-pfähle d=61cm
3m
3,6m
6:1
5:1
50:1
2,6m
3,04m
1,5m
7,22m
1,6m
5,72m
1,665m
1,225m
50:1
16:1
BoredPiles
D=0.61 m
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Bending stiffness of piles is neglected
Estimation of pile forces
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Bridge column with pile foundation
Numericalmodel
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
HVM
beam
horizontalspring
Vertikal-feder
n=0
n=0,5
n=1n=2
ks
k (z)=k (d).(z/d)s sn
n= 0 bindiger Boden
n =1 nichtbindiger Boden
Elastic support of piles
Beam
Horizontal springs
Verticalsprings
Distribution of soilstiffness
n = 0 cohesive soiln = 1 non-cohesive soil
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Bending moments in the piles
H = 870 kN
Base of pile fixed vertically
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
195.
C=400MN/m
pile cap can’t move horizontally
Pile cap can move
+8
68
-22
H = 870 kN
Bending moments in the piles
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Summary 02: Beam and truss models
32
• Beam elements are based on a linear strain distributionmember forces in discontinuity region can not be calculatedbut stiffness of the D-regions has to be considered
• Nonlinear material behaviour of concrete should be considered (e.g. torsion stiffness)
• A realistic model for the support condition has a significant influence on the memberforce of the system. Restraints, which may lead to high forces, should be omitted.
• The basic parameters of an elastic support on ground should be checked. The stiffnessmodulus of the soil is estimated by an Oedometer test, where the soil is fixed by a horizontal stiff ring. Therefore the real soil stiffness can be significant smaller.
• An inclined axis of gravity (haunches) should be modelled with regard to the shear design of a beam. System und Belastung
Querkraft
-747
kN
607k
N -375kN
-375kN
Normalkraft
-90kN
-121
3kN
-125
8kN
-45kN
-1176kN
Verformung
29,3mm26,3mm
2 3 4 5 6 7 8 9 101112131415161718192021 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 414243444546474849505152535455565758596061 4,0m
12,5m12,5m 25m50m
1,0m
(g+q)=30kN/m
-824
0kN
m
-652
0kN
m
-1190kNm
1150kNm
1100kNm
Biegemoment beide Trägerenden eingespanntund unverschieblich
beide Trägerenden eingespanntein Lager horizontal verschieblich
-1240kNm.
1
TUHH - Prof. Rombach
Pin Support
Corners
Point Loads
Singularities in shear walls
TUHH - Prof. Rombach
a2
a3a4
a5
v5 v4 v3 v2 v1
a1 v =ai i.ϕF =C ai i. .ϕM =F a =C ai i i i
2. . .ϕM= M = C a =CΣ Σ ϕ ϕi i
2. . .ϕC = C aϕ .Σ i
2
ϕ
lE ,IA
c c
v ϕ
lE ,IA
c c
Deep beam supported on columns
TUHH - Prof. Rombach
h/b=24/48cm
lx=7,20m
ly=3,60m
l=2,4m
d=24cm
System and Loadingq = 20 kN/m
Finite-Elemente-Model
X
Y
0.78
Main membrane forces and beam bending moments
Deformed Structure
Deep beam supported on columns
TUHH - Prof. Rombach
Hau ptmembra nkräfte M embrank raft n (S chnitt in F eldmitte)x -50.5
54.8
Ve rschoben e Struktur
XY
membrane forces H orizontal membrane force n (section in midspan)x-50.5
54.8
Finite-Elemente-Model
Deformed Structure
X
Y
DeepBeam
supportedon
columns
TUHH - Prof. Rombach 37
Connection of different types of elements
u2
v2
u 1ϕ1
ϕ2
v1
Plane shell element (2-D) Beam element (2-D)
2 translation degrees of freedom 2 translation degrees of freedom +
1 rotation degree of freedom
TUHH - Prof. Rombach
shell element
Increase of truss length
truss element
shell element
Coupling of the mid joint
truss element
Connection of different types of elements
TUHH - Prof. Rombach
3.7
-2.5
-3.7
2.5
main membrane forces and truss bending moments
2.0
-1.6
-2.0
1.6
Deformations
Deep beam supported on columns
TUHH - Prof. Rombach
1 12 2
3
3
4
4
-80. -60.
-99.-213.
-182.
-131.-142.
-152.-150.
-103
.
-214
.-117
.
-133
.
Schnitt 3-3
Schnitt 1-1Schnitt 2-2
Schnitt 4-4
X
Y
Detail
Stress distribution in a corner
TUHH - Prof. Rombach
2.0
2.0
5.0
10.0 15.0
1.0
1.0
horizontal reinforcement2.07
10.42
0.41
3.49
section in midspan
3.5
4.54 .5
3.0
2.0
1.0
1.0
2.0
3.0
0.5
4.0 4.0
vertical reinforcement
7 ,20 m
3,6 m
Reinforcement
TUHH - Prof. Rombach
Reinforcement
TUHH - Prof. Rombach
Summary: Shear walls
• Singularities (e.g. pin support, single forces) should be omitted
• Modelling of the support of deep beams should be done with great care
• ‚Numerical’ restraints should be omitted (e.g. supports, coupling of nodes)
• An incompatible element mesh should be omitted (e.g. connection of beamand plain shell elements)
• An automatic design of plain shells is not possible
• Elastic finite element analysis of shear walls are useful to develop a strut-and-tie model
Scheibenelement
Stab in Scheibeverlängern
Stabelement
Scheibenelement
Gelenkige Kopplungmit Mittenknoten
Stabelement
X
Y
Z
l +a4
x l +a4
x l +a4
x l +a4
x
lxa a
ly
z
z2
z1
Zugstrebe
com
pres
sion
stru
t
Dru
ckst
rebe
Druckstrebe
horizontale Membrankraftin Feldmitte (in kN/m)
Fc=31kN
z=3,
8m0,55m
Fs=31kN
-4.80
-3.96
-8.17
36.6
+
-
TUHH - Prof. Rombach 44
Design of real concrete structures with finite element software
Prof. Dr.-Ing. G. A. RombachHamburg University of Technology
E-mail: [email protected]
• Introduction
• Beam and truss structures
• Spatial structures- shear walls- slabs- shells
• Material nonlinear analysis
• 3-d models
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Stüt zenraster 1,50mStüt zen 24/24 cm
Slabs
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
HauptmomenteLastfall g=10 kN/m2
-146.5
-125.0
-100.0
-75.0
-50.0
-25.0
0.0
25.0
50.0
75.0
100.0
Main bending moments and shear forces
Loading: g = 10 kN/m2
Stützenraster 1,50mStützen 24/24cm
2.6
25.0
50.0
75.0
100.0
125.0
150.0
175.0
200.0
225.0
250.0
728.0
Main Shear ForceLoading g=10 kN/m2
Corners
Pin support
TUHH - Prof. Rombach
Missing Support
Missing Support
Corner
Corner
Pin Support
Opening
Singularities
HauptquerkraftHauptmomente
1m
Y
Xm =0y,r
m =0x,r
10. 10.
10.
10.
90.
TUHH - Prof. Rombach
Singularities - point load
noyes
yesyes
X Y
Z
F
Fv = F U
Detail
TUHH - Prof. Rombach
Starre Scheibe
a) 2D resp. 3D Model
b) Pin support of one node
c) Pin support of all supported nodes
d) restraint of the end nodes
e) Pin support of stiff slab
f) Elastic support
Modelling of wall support
TUHH - Prof. Rombach
X
Z
Node
Coupling
Slab
Column
RestraintDeformation
One way slabLoad on left span only
Bending moments
TUHH - Prof. Rombach
Walls - partially missing support
TUHH - Prof. Rombach 52
Single-column footing
52
TUHH - Prof. Rombach 53
Single-column footing – shell analysis
Membrankraft in horizontaler Richtung in kN/m
Membrankräfte
3010.2900.
1302. 2 816.
281 7.
Setzung in mm
2.83
mm
2.45
mm
5,0m
Membrane forces
Membrane forces in horizontal direction
Settlements
TUHH - Prof. Rombach
Circular Slab
TUHH - Prof. Rombach 55
Shells
25m
28m
28m
pp
SSh
2r
pppp
Fle ckenlast
Ve rtikalschnit t Horizontalschnitt
Patchload
TUHH - Prof. Rombach
Anzahl der Elemente in Umfangsrichtung bzw. über die HöheElementnetz A
16 x 11 32 x 22 64 x 44
Elementnetz B Elementnetz C
N x
200 kN/m
C B A
X
Y
Z
Mx
100 kNm/m
X
Y
Z
CB A
Shells
Inner forces in circumferentialdirection
Mesh A Mesh B Mesh C16x11 32x22 64x44
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Nonlinear analysis of concrete structures
• Introduction
• Beam and truss structures
• Spatial structures- shear walls- slabs- shells
• Material nonlinear analysis• 3-d models
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Nonlinear analysis of concrete structures
Aims• more realistic model
• correct deflections (e.g. slabs)
• more economical design due to load redistribution
• reduce restraint forces
• more realistic analysis of damages
• analysis of experiments
Problems• reinforcement must be known (e.g. linear analysis)
• load combination is not possible
• numerical model
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Nonlinear analysis of beams and columns
59
f /yk sγ
f /tk,cal sγBetonstahlσs
εsu
εs
Material modelssteel
resistance
Strains stresses andstress resultant
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Nonlinear analysis of beams and columns
60
Tension
Stiffening
Effect
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Nonlinear analysis of beams and columns
61
tension stiffening effect
modification of steel strains concrete tension
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Nonlinear analysis of beams and columns
62
Tension Stiffening Effect
fI = 25,4 mm stage I – elastic
fII,1 = 88,0 mm stage II – without TSfII,2 = 83,0 mm stage II – with TS – modification of steel strainsfII,3 = 48,0 mm stage II mit TS – concrete tension
Big differences
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Nonlinear analysis of beams and columns
63
Safety concept
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Material models
concrete: uniaxial and triaxialtensile strengthlong term behaviour (s+c)load historycracking
reinforcement: elastic - plastic
64
Nonlinear analysis of beams and columns
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
bond: with/without slip„tension stiffening“
Kornverzahnung Dübelwirkung
Numerical Modellingreinforcement bars: discret – smearedbond: fixed - softcracks: discret - smeared
65
Nonlinear analysis of concrete structures
Material models
concrete: uniaxial and triaxialtensile strengthlong term behaviour (s+c)load historycracking
reinforcement: elastic - plastic
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
66
Nonlinear analysis of concrete structures
Material parameters of concrete:• Compressive strength fck
• Tensile strength fct
• Shrinkage and creep• Elastic-Modulus• Poisson‘s ratio• ........
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
25 120
180
150
550
670cm
Draufsicht
Ansicht
67
plan view
Side-view
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
180
150
d=28/10 + s d=16/10s
d=28/10 + sd=28/10s
d=16/10s
Special ColumnSES – Bangkok
Rebar
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
The conclusion of the various analyses is that the offset colum heads, as detailed, are able to carry the design service and ultimate loads....
Nonlinear analysis of concrete structures
TUHH - Prof. Rombach
Hauptm omenteLastfall g=10 kN /m2 -146. 5-125. 0-100. 0-75 .0-50 .0-25 .00 .025 .050 .075 .0100. 0
Aims• More realistic analysis
• Fast analysis and design
• Simplifications seems not to be required
Problems• Manpower for input
• Difficult to check the results
• Important details may be overseen
• Calculation of reinforcementnot possible (e.g. shear walls) ......
• Relevant load arrangement ?
Modelling of whole structures
TUHH - Prof. Rombach
Arch bridge
Plan view
Side view
3-D (1. BA)
26,4 m
Bored piles d = 1.20m
Wing wall t = 1.0 mwall t = 0.4 m
Beam
2,2x2,0 m
TUHH - Prof. Rombach
Arch bridge
Flow of forces
detailing wrong correct
TUHH - Prof. Rombach
Arch bridge
loads
restraints
Dead load
Soil pressure
Temperature ∆ = 16 K
TUHH - Prof. Rombach
Arch bridge
Shear design
Seite:
Stirrups [cm2/m]
Bored piles d = 1.20 m
Section
A-A
TUHH - Prof. Rombach
Arch bridge
Shear design
TUHH - Prof. Rombach
Arch bridge
design
Seite:
TUHH - Prof. Rombach
Arch bridge
design
TUHH - Prof. Rombach
Arch bridge
Parametric studies on truss system
TUHH - Prof. Rombach
Arch bridge
Parametric study: soil stiffness
TUHH - Prof. Rombach
Summary: Complex 3-D-shell analysis
• Detailing and flow of forces (e.g. in frame corners oder massive members) should be considered.
• Restraint forces should be checked with regard to the cracked state.• Stiffness change of members due to cracking of concrete and variation of
possible soil stiffnesses should be considered in the design.• The numerical model should be to checked for D- and singularity regions.• Automatic design (bending, shear) of shear walls or shell structures is not
possible. Truss forces are needed for design.• Great effort is needed for checking the analysis and for the graphical and
numerical output.• Modifications of the structure requires the analysis of the whole structure.
TUHH - Prof. Rombach
Finite Element Design of Concrete Structures
Prof. Dr.-Ing. Günter A. RombachHamburg University of Technology
E-mail: [email protected]
Rombach G.: Finite elementdesign of concrete structures
Thomas TelfordISBN: 0 7277 3274 9
Published 2004
Thanks you for your attention!