an efficient model for seismic analysis of flat slab structures with the effects of stiffness...
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An Efficient Model for Seismic Analysis ofAn Efficient Model for Seismic Analysis of
Flat Slab Structures withFlat Slab Structures with
The Effects of Stiffness DegradationThe Effects of Stiffness Degradation
Seung Jae LeeSeung Jae Lee
Sungkyunkwan UniversitySungkyunkwan University
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Introduction
• The columns directly support the flat slabs without beams.
• Providing lower story height, good lighting and ventilation
• Remarkable lateral stiffness degradation in the slab
Flat slab structure having capital and drop panel
Drop panel
Capital
Flat slab system
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Width of the equivalent frame
y
x
Equivalent frame widthin the y direction
Equ
ival
ent f
ram
e w
idth
in th
e x
dire
ctio
n
h
c1c2Floorheight
Columnabove
Columnbelow
Slab strip
Slab strip
l1
l2
• Widely used for analysis of flat slab structures in practical engineering
• Slab is modeled by equivalent frame
• Elastic analysis is performed
• Effective width proposed by Jacob S. Grossman is commonly used
Equivalent frame method
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• Investigate limitations in the Equivalent Frame Method
• Propose an efficient analysis method using FEM
Reduce modulus of elasticity
Include stiffness degradation in the slab depending on lateral drift
Use super element and fictitious beam
Reduce computational time and memory
Objectives
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: Length of span in direction parallel and transverse to lateral load
: Size of support in direction parallel and transverse to lateral load1C ,
,
FPd Kh.d//CC/llCl.Kαl )90](2)()(30[ 1212112
222 ))()(5.0())()(2.0( lKKllKK FPdFPd 2l: Equivalent width factor
dK800/sh
sh1.1 at the acceptable drift limit
1.0 at the acceptable drift limit
0.8 at the acceptable drift limit
0.5 at the acceptable drift limit
400/sh
200/sh
100/sh
2l
2C
d : Effective depth of slab h : Slab thickness
FPK 1.0 at interior supports
0.8 at exterior and edge supports
0.6 at corner supports
: Effective width of slab
: Factor considering degradation of stiffness of slabs
With limits:
: Story height
1l
Grossman method for Effective width
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Classification of Grossman method
dK )90( h.d/
Terms can be simply included in the FEM
]2)()(30[ 121211 /CC/llCl. FPK
FPd Kh.d//CC/llCl.Kαl )90](2)()(30[ 1212112
)9.0/( hdEKE dR REE : Modulus of elasticity
Terms cannot be easily considered by the FEM
)90( h.d/ Approximately 1.0
<0.9, if very thin slabd/h
: Adjusted modulus of elasticity
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Difficulty in providing stress distribution in the slab
Calculation of equivalent mass for the dynamic analysis
Troublesome calculation of effective width by the change of column size
Plans to which EFM can not be applied
Limitations of the Equivalent Frame Method
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6.4X6.4 6.4X6.4
6.4X6.4
9.6X9.6
9.6X4.8
12.8X6.4
9.6X4.8
9.6X4.8
Line of symmetry
PLAN
Na
4
3
2
b c d
1
108
72
A A
‘Pinned’ Support (typ.)
SECTION A-A(All units are in inches)
4812 32
U.C. Berkeley Test (by Prof. Jack. P. Moehle, 1990)
Test structure
LATERAL DRIFT - NS
0
20
40
60
80
100
120
LA
TE
RA
LS
TIF
FN
ES
S(k
ip/i
n.)
EFM
FEM
UCB test
1/800 1/400 1/200
LA
TE
RA
LS
TIF
FN
ES
S(k
ip/i
n.)
LATERAL DRIFT - EW
0
20
40
60
80
100
120
140
160
EFM
FEM
UCB test
1/800 1/400 1/200
Stiffness degradation in the slab
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1 1 c
I =
1 s
I =
Deformation of Entire Structure
SC
: Total lateral displacement
SC Consideration of Stiffness Degradation
S
SC RR
R
SRCR
SSR
Deformation of Columns
Deformation of Slabs
: Lateral displacement due to slab deformation
: Lateral displacement due to column deformation
: Stiffness reduction factor for structure
: Stiffness reduction factor for slab
Stiffness reduction factor for slabs
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Drift Direction Avg.
1/800NS 0.905 0.054 0.033 0.021 0.853
0.822EW 0.829 0.063 0.049 0.014 0.790
1/400NS 0.830 0.110 0.067 0.043 0.748
0.722EW 0.747 0.129 0.100 0.029 0.695
1/200NS 0.661 0.230 0.140 0.090 0.543
0.539EW 0.598 0.254 0.197 0.057 0.536
CSR SR
CR
SSR
91.099.74 LS DR
LD
LATERAL DRIFT (logarithmic)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Sla
b S
tiff
nes
s R
edu
ctio
n
1/800 1/400 1/200
: Lateral drift
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LA
TE
RA
LS
TIF
FN
ES
S(k
ip/i
n.)
LATERAL DRIFT - NS
0
20
40
60
80
100
120
EFM
FEM(w/o reduction)
FEM(w/ reduction)
UCB test
1/800 1/400 1/200L
AT
ER
AL
ST
IFF
NE
SS
(kip
/in
.)
LATERAL DRIFT - EW
0
20
40
60
80
100
120
140
160
EFM
FEM(w/o reduction)
FEM(w/ reduction)
UCB test
1/800 1/400 1/200
Application of stiffness reduction factor to FEM
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Modeling flat slab using super elements
Refined mesh model for floor slab
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Separate floor slab for generation of super elements
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Generation of super elements
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Assemble super elements
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Use of stiff fictitious beams
A floor slab unit between columns
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Add fictitious beams
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Added fictitious beams
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Matrix condensation
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Eliminate fictitious beams
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Super element
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Example structure 1
Floor plan
20-story example structure
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Natural periods of vibrationLateral displacements
0 2 4 6 8 10 12 14 16Displacement(cm)
0
4
8
12
16
20
Sto
ry
EFM
FEM(w/ reduction)
Proposed(w/ reduction)
1 4 7 10 13 16 19Mode
0
1
2
3
4
5
Per
iod
(sec
)
EFM
FEM(w/ reduction)
Proposed(w/ reduction)
Static & Eigenvalue analysis
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Von-Mises stress distribution
FEM
EFM
Proposed
max = 4.53E-2
max = 2.22E-2
max = 4.46E-2
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Time history analysis
Roof displacement time history (El Centro NS, 1940)
Model DOF`s
Computational time (sec)
Assemble M & K
Static analysis
Eigenvalue analysis
Time history analysis
Total
FEM 55500 230.22 394.38 17406.66 281.58 18312.84
EFM 1740 2.61 0.36 19.69 7.67 30.33
Proposed 780 13.70 0.12 5.75 3.36 22.93
0 2 4 6 8 10 12 14Time(sec)
-40
-30
-20
-10
0
10
20
30
40D
ispl
acem
ent(
cm)
12.885.4
EFM
FEM(w/ reduction)
Proposed(w/ reduction)
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Example structure 2
Floor plan
20-story example structure
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Static & Dynamic analysis
0 2 4 6 8 10 12 14 16Displacement(cm)
0
4
8
12
16
20
Sto
ry
FEM(w/ reduction)
Proposed(w/ reduction)
1 4 7 10 13 16 19Mode
0
1
2
3
4
5
Per
iod
(sec
)
FEM(w/ reduction)
Proposed(w/ reduction)
Natural periods of vibrationLateral displacements
Model DOF`s
Computational time (sec)
Assemble M & K
Static analysis
Eigenvalue analysis
Time history analysis
Total
FEM 47580 193.30 390.35 13315.33 238.41 14137.39
Proposed 780 13.48 0.09 5.86 3.33 22.76
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Example structure 3
Floor plan
3D view of example structure (20F)
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Refined mesh model for floor slab with opening
Super element for the slab with opening
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Separate floor slab for generation of super element
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Add fictitious beams
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Matrix condensation
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Eliminate fictitious beams
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Assemble the super elements
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Static & dynamic analysis
0 2 4 6 8 10 12 14 16Displacement(cm)
0
4
8
12
16
20S
tory
FEM(w/ reduction)
Proposed(w/ reduction)
1 4 7 10 13 16 19Mode
0
1
2
3
4
5
Per
iod
(sec
)
FEM(w/ reduction)
Proposed(w/ reduction)
Natural periods of vibrationLateral displacements
Model DOF`s
Computational time (sec)
Assemble M & K
Static analysis
Eigenvalue analysis
Time history analysis
Total
FEM 53580 214.13 447.98 16126.36 269.72 17058.19
Proposed 900 44.98 0.14 7.22 3.83 56.17
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Conclusions
Equivalent Frame Method
• Consider stiffness degradation in the slab
• Can be applied only to flat slab structures with a regular plan
• Cannot provide stress distribution in the slab reasonably
• Need to calculate equivalent mass for the dynamic analysis
• Troublesome calculation of effective width with the change of column size
Finite Element Method using super elements
• Consider stiffness reduction in the slab by reduced modulus of elasticity
• Can analyze flat slab structure with irregular plan and openings in the slab
• Can provide stress distribution in the slab with accuracy
• Reduced number of DOF`s Saving in computational time and memory
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