advanced topics in analysis and design of normal and high strength concrete structures volume 2...
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FACULTY OF ENGINEERING ANDINFORMATION TECHNOLOGY
The Institution of Engineers, Malaysia
Short Course on Advanced Topics in Analysis and Design of
Normal and High Strength ConcreteStructures
4 to 5 May 2006, Kuala Lumpur, Malaysia
Course MaterialsVolume 2: Lecture Notes
EIT2006
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PREFACE
The Short Course on “Advanced Topics in Analysis and Design of Normal andHigh Strength Concrete Structures” is delivered on the invitation of TheInstitution of Engineers, Malaysia. Held in Kuala Lumpur on 4 and 5 May2006, its primary objective is to acquaint the participants with the researchwork conducted in the topical areas by the researchers at Griffith Universitymainly over the last decade. The Short Course also provides the backgroundand technical details which inform the Keynote Address to be presented at the9 th International Conference on Concrete Engineering and Technology(CONCET 2006) to be held from 8 to 10 May 2006. It is hoped that thediscussion over the next two days will be helpful to the Malaysian engineeringcolleagues in their future work.
To assist the participants, the Short Course materials are given in twovolumes: “Selected Published Papers”, which is an up-to-date collection ofrelevant publications in the areas to be covered in the discussion; “LectureNotes”, which contains the hardcopy of all the PowerPoint slides to bepresented.
I wish to take this opportunity to acknowledge the contributions of all myconcrete research colleagues and students at Griffith School of Engineeringwithout which many of the advances made would not have been possible. Inparticular, I would like to thank my close collaborators
• Dr Sam Fragomeni, Associate Professor and Deputy Head of School• Dr Hong Guan, Senior Lecturer in Structural Engineering and Mechanics• Dr Sanaul Chowdhury, Lecturer in Structural Engineering, and• Dr Jeung-Hwan Doh, Associate Lecturer in Structural Engineering
for their invaluable work over the years. Special thanks are also due to DrsChowdhury and Doh for their meticulous efforts in compiling, developing andupdating these two volumes of materials.
The invitation of the Organising Committee of CONCET 2006 to present theKeynote Address and the help of its members in particular Ir. M.C. Hee, Mr.Thang Fai Li and Mr. Jamie Kheng are greatly appreciated.
Professor Yew-Chaye LooDean, Faculty of Engineering and Information TechnologyGriffith University
4 May 2006
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Section 1: Overview
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SERVICEABILITY AND STRENGTH OFNORMAL AND HIGH STRENGTHCONCRETE BEAMS, COLUMNS,
SLABS AND WALLS
Yew-Chaye LooPhD, FICE ,FIStructE, FIEAust
Professor of Civil Engineering andHead, School of Engineering
SERVICEABILITY AND STRENGTH OFNORMAL AND HIGH STRENGTH CONCRETE
STRUCTURES- OVERVIEW
Professor Yew-Chaye LooPhD, FICE ,FIStructE, FIEAust
DeanFaculty of Engineering & Information Technology
Faculty of Engineering & Information Technology
CONTENTSCONTENTSSERVICEABILITY
STRENGTH
LAYERED FINITE ELEMENTMETHOD (LFEM)
COLUMN & WALLSHORTENING
SUMMARY
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CRACK WIDTH
DAMPING CHARACTERISTICS
DEFLECTION
SERVICEABILITY
ULTIMATE STRENGTH OF WALLS
PUNCHING SHEAR STRENGTH OF FLATPLATES
STRENGTH
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CRACK WIDTHCrack width formulas for beams
Crack Width Formula*Average crack width:
wcr = (f s /E s) [0.6(c - s) + 0.1 ( Φ / ρ )] (1)
Maximum crack width:
wmax = 1.5 wcr (2)
__________________________________________________ *Chowdhury, S.H., Loo, Y.C. & Wu, T.H. 1995; Chowdhury, S.H. & Loo, Y.C. 1997, 2001, 2002, 2003,
2004a, 2004b; Chowdhury, S.H. 2001; Chowdhury, S.H. & Fragomeni, S. 2001
clear cover
spacing between bars
average bar diameter
steel ratiosteel stress
elastic modulus
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ComparisonComparison (30 test beams)(30 test beams) **
w cr, calculated in mm
0.40.30.20.1 0.0
w c r , m
e a s u r e
d i n m m
0.4
0.3
0.2
0.1
0.0
- 30% line
+ 30% linePartially prestressedconcrete beamsReinforced concretecontinuous beamsReinforced concretesolid beams
Reinforced concrete box beams
*Chowdhury, S.H. & Loo, Y.C. 1997, 2001, 2002; Chowdhury, S.H. 2001
Published data
34 PC beams Nawy (1986), Rutgers University
Fully prestressed T-beamsPPC T-beamsPPC I-beamsPost-tensioned PPC T-beams
6122
14
59 RC beams Clark (1956), ACI, USA 26
Chi & Kirstein (1958), ACI, USA 16
Hognestad (1962), PCA, USA 8
Kaar & Mattock(1963), PCA, USA 9
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Equation 1 or 2 in mm
.9.8.7.6.5.4.3.2.10.0
M e a s u r e
d c r a c
k w
i d t h s
i n m m
.9
.8
.7
.6
.5
.4
.3
.2
.1
0.0
Legend
+ 30% line
- 30% line
Kaar & Mattock's bea
Hognestad's beams
Naw y's beams
(14 post-tensioned)
Naw y's beams
(20 pre-tensioned)
Chi & Kirstein's bea
Clark's beams
93 RC & PC beams
Comparison with Code FormulasComparison with Code Formulas
CRACK WIDTH
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0 0.1 0.2 0.3 0.4
Calculated w cr in mm
M e a s u r e
d w c r
i n m m
Chowdhury & Loo's beams
Chi & Kirstein's beams
Clark's beams- 30% line
+30% line
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0 0.1 0.2 0.3 0.4
Calculated w cr in mm
M e a s u r e
d
w c r
i n m m
Chowdhury & Loo formula Eurocode formula
For average crack width
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
Calculated w max in mm
M e a s u r e
d w m a x
i n m m
Chi & Kirtstein's beamsClark's beams
- 30% lne
+ 30% line
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7Calculated w max in mm
M e a s u r e
d w m a x
i n m m
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
Calculated wmax in mm
M e a s u r e d
w m a x i n
m m
Chowdhury & Loo formula
BS formula
ACI Code formula
For maximum crack width
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DEFLECTION
Deflection
Repeated loading
Impact
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Deflection of RC beams under repeated loading
δT= δda+ δl
δda = k δdi
k = k 1 + R log 10T
number of loading cycle
1.18 + (0.029/ ρ) (M t – Md )/(M y – Mcr )(0.0015/ ρ) (M t – Md )/(M y – Mcr )
Correlation of measured and computed total deflections – proposed formulaREPEATED LOAD
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Hertz’s Contact Law and the relative approach
3/2
s K )t(F
)t,x(y)t(y)t(a ⎥⎦
⎤⎢⎣
⎡=−=
Deformation constant (materials and shapes)
ymax = y’ max [(2/m bω12) (1.25 m s v02 K 2/3)3/5]
ω1 = (π2/L2) √(EI/ ρA)
α = (m b/m s)
β = 1.47 ( ω1/π) (5m s/4Kv 01/2)2/5
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WijewardeneWijewardene ’’ss andand HussainHussain ’’ss beamsbeams
Hughes andHughes and Speir Speir ’’ss beamsbeams
DEFLECTION
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DAMPING CHARACTERISTICS
Damping of RC & PC beams
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DAMPINGDAMPING -- DEFINITIONDEFINITION
Time t
Amplitude A
A1A n+1
n periods
Residual crack width
Lbaw= rcr,
The logarithmic decrement , δ, is obtained as:
A1),(ncycleatamplitude
Acycle1,atamplitudelog(1/n)=
1n
1e
++δ
Time t
Amplitude A
A1 A n+1
n periods
Time t
Amplitude A
A1 A n+1
n periods
Experimental Program• 14 RC beams• 12 PPC beams
Beamlength,L
l
Appliedload
Loadingbeam
100 mm 100 mm
Typcal loadingdiagram
Embedded Polystyrene
asvoid
60 180 60
2 5
1 0 0
Typical RCbox beam
2 8
300mm
3 0 0 m m
mm m m
Stages in a vibration measurement system
Test Procedure
Beam length, L
l
Applied load
Loading beam
100 mm 100 mm
Typcal loading diagram
Embedded Polystyrene
as void
60 180 60
2 5
1 0 0
Typical RC box beam
2 8
300 mm
3 0 0 m m
mm m m
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Damping prediction formulas*
– For RC beams, δ isδ = 0.048 w cr,r + 0.011 L
– For PPC beams,
δ = 0.054 w cr,r + 0.0104 L __________________________________________________________________________________________________
*Chowdhury, S.H. & Loo, Y.C 1998a, 1998b, 1999, 2001, 2003; Chowdhury,S.H. Loo, Y.C. & Fragomeni, S. 2000
W cr,r = 0.312 w cr, i
w cr, i = (f s /E s) [0.6 (c – s) + 0.1 ( φ/ ρ)]
RC beams
Predicted δ
.16.12.08.040.00
M e a s u r e
d
.16
.12
.08
.04
0.00
+ 30% limits
- 30% limits
Continuous beams
Simply-supported beams
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.16
PPC beams
Predicted δ
.16.12.08.040.00
M e a s u r e
d
.16
.12
.08
.04
0.00
- 30% limits
+ 30% limits
.16
Predicted δ
.16.12.08.040.00
M e a s u r e
d
.16
.12
.08
.04
0.00
- 30% limits
+ 30% limits
.16PPC beams
0
0.01
0.02
0.03
0.04
0.05
0.06
0.07
0.08
0.09
0 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08 0.09
Predicted δ
M e a s u r e
d
Beam HSB 1
Beam HSB 2
Beam HSB 3
Beam HSB 4
Beam HSB 5
Beam HSB 6
+ 30% Line
- 30% Line
DAMPING
6 HSC RC beams
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PUNCHING SHEAR STRENGTH OFFLAT PLATES
Typical flat plate with spandrel beams
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Punching Shear Strength
Higher punching shear due tounbalanced bending moment
Balanced bendingmoments
30 –35degrees
LOADLOAD
Bendingcracksappear atlowloading
Test setupTest setup (University of Wollongong, 1987(Univers ity of Wollongong, 1987 --90)90)
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Corner connection Edge connection
21uVVV += 21u V2VV +=
543
corner ,1342431u k k k
)V(k k k k k k V
−+−
=543
edge,1342432u k k k
)V(k k k k k k 2V
−+−
=
ely121u PnVVV −+= ely121u PnV2VV −+=Corner connection Edge connection
543
7342431u k k k
k k k k k k k V
−+−=
543
7342431u k k k
k k k k k k k 2V
−+−=
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RC Flat PlatesRC Flat Plates (19 V(19 V uu values from 9 half values from 9 half --scale models)scale models)
0
50
100
150
200
250
0 50 100 150 200 250
Predicted V u
M e a s u r e d V u
Falamaki & Loo (1992)
AS 3600-1994
45 degree line
(kN)
( k N )
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PostPost --tensioned Flat Platestensioned Flat Plates (4 half (4 half --scale models)scale models)
PUNCHING SHEAR
0
20
40
60
80
100
0 20 40 60 80 100
Predicted V u
M e a s u r e d V u
Loo & Chiang (1996)
AS 3600-1994
ACI 318-1989
BS 8110-1985
45 degree line
(kN)
( k N )
ULTIMATE STRENGTH OF WALLS
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OneOne --way and twoway and two --way actionsway actions
(a) One(a) One --way actionway action AS 3600 (2001) ACI 318 (2002)
(b) Two(b) Two --way actionway action
LimitationsLimitations AS3600-2001Hwe/tw ≤ 30f ’c ≤65 MPae ≥ tw/20one-way actiononly solid walls
ACI 318-2002Hwe/tw ≤ 25 or L/ t w ≤25f ’c ≤ 50 MPae ≤ tw/6one-way actiononly solid walls
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TestTest --rigrigset upset up
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1200x1200x401200x1200x40((f f ’’cc=35 MPa)(one=35 MPa)(one --way)way)
1200x1200x401200x1200x40((f f ’’cc= 37 MPa)(two= 37 MPa)(two --way)way)
1600x1600x401600x1600x40((f f ’’cc= 50 MPa)= 50 MPa)
(two(two --way,way,opening)opening)
Design formula*
)e2e2.1t(f 0.2 N aw7.0'
cu −−φ=φ
)/(2500t)(H w2
we=
0.6
design axial strength / unit length (N/mm)
thickness (mm)
compressive strength (MPa)
eccentricity (mm)
additional eccentricity due tosecondary effect (mm)
*Doh, J.H., Fragomeni, S. & Loo, Y.C.; Doh, H., Fragomeni, S. & Kim, J. 2001
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H/t w
N u
/ f ' c L t w
0 10 20 30 40 50 600
0.1
0.2
0.3
0.4
0.5
0.6
0.7
f' c = 30 M Paf' c = 50 M Paf' c = 80 M PaFragomeni (NSC)Fragomeni (HSC)OWNS (Stage 1)OWHS (Stage 2)Doh (HSC)Doh (NSC)
Comparison with test data –one-way action
Comparison with test data –two-way action
H/t w
N u
/ f '
c L t
w
10 20 30 40 50 60
0.3
0.4
0.5
0.6
0.7
0.8 f' c = 30 M Paf' c = 50 M Paf' c = 80 M PaSaheb & Desayi (1990)Fragomeni (NSC)(1995)Fragomeni (HSC)(1995)Doh (NSC)
Doh (HSC)
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u21uo N)k k ( N α−=Formula for wall with openings:
WALL
⎟ ⎠ ⎞
⎜⎝ ⎛ η+=α
LAA o
⎟ ⎠ ⎞
⎜⎝ ⎛ η−=η
2L
⎟⎟
⎠ ⎞
⎜⎜
⎝ ⎛
−η−=η
wow
oow2
w21
tLLt
LtLt
H
t
L/2η~
L
G3G2G1
Elevation
Lo
Ho
G3G2G1
Cross- sectional Plan
oη
η
k 1 = 1.18 (for one-way action)= 1.00 (for two-way action)
k 2 = 1.19 (for one-way action)= 0.93 (for two-way action)
WallPanels
FailureLoad (kN)
N*(kN)
N* Failure load
OW 01 253.10 250.54 0.99
OW 02 441.45 344.64 0.78
OW 11 309.02 290.30 0.94
OW 12 294.30 285.97 0.97
OW 21 185.41 184.38 0.99 O n e - w a y a c
t i o n
OW 22 195.71 200.68 1.03
TW01 735.75 707.70 0.96
TW02 1177.20 1067.90 0.91
TW11 750.47 676.21 0.90
TW12 1030.05 878.52 0.85
TW21 618.03 471.44 0.76 T w o - w a y a c
t i o n
TW22 647.46 612.48 0.95
Average 0.92
Comparison of test results and new proposed method
Degenerate shell elements composed of concreteand smeared steel layers
teSmeared-outsteel layers
12
n sn s-1
x
y
z
Mid reference plane
z c+ 1z czc- 1
z 3z2z1123
n cn c- 1
Concretelayers
Layer number
z 1z 2
z s-1z s
u
vw
θ y
xθ
5 DOFs per node- in-plane displacements,
u and v- transverse
displacement w- two independent
bending rotations aboutx and y axes, y and x
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Cracking
f c'
0.3f c'
Effect of tension stiffening
E0
f t
Effect of bulk mo
Strain-hardening model
Perfect plasticity model
loading-unloading
Crushing
σ
ε
modulus
0.8f y
0.002
Es
01
Es1f y
11
Es2
σ
ε
Smeared crack approach for cracked concrete
Material modelling
• Tri-linear σ-ε for steel
• Tension-stiffening and shear stiffnessdeterioration effects after concrete cracking
• Strain-hardening plasticity procedure forconcrete compressive behaviour
• Tension-stiffening and shear stiffnessdeterioration effects after concrete cracking
• Strain-hardening plasticity procedure forconcrete compressive behaviour
• Strain-hardening plasticity procedure forconcrete compressive behaviour
Numerical Modelling
teSmeared-outsteel layers
12
n sn s-1
x
y
z
Mid reference plane
zc+1zczc-1
z3z2z1
123
n cn c-1
Concretelayers
Layer number
z1z2
zs-1zs
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LFEM for flat plates*
Punching shear strength
Load-deflection response
Crack patterns
___________________________________________________________________________________________________
*Loo, Y.C. & Guan, H 1997; Guan, H. & Loo, Y.C. 1994, 1997a, 1997b, 2002
0
5
10
15
20
25
30
35
40
0 5 10 15 20 25 30 35 40
Deflection (mm )
L o a
d d e n s
i t y
( k N / m )
Ex per iment * ( po int 1) Pr op os ed met ho d ( poin t 1)Ex per iment * ( po int 2) Pr op os ed met ho d ( poin t 2)Ex per iment * ( po int 3) Pr op os ed met ho d ( poin t 3)
M2
12 3
Collapse load
32.7
0
5
10
15
20
25
30
35
0 5 10 15 20 25 30 35
Deflection (mm )
L o a
d d e n s
i t y
( k P a
)
Ex per iment* (point 1) Pr opos ed method ( point 1)Ex per iment* (point 2) Pr opos ed method ( point 2)
Ex per iment* (point 3) Pr opos ed method ( point 3)
W2
12 3
Collapse load
28.91
Load-Deflection
LFEM
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Comparison ofComparison of VVuu (models w ith spandrel beams)(models w ith spandrel beams)Connec- Type * Experiment LFEM AS 3600-1994
tion V u (kN) PredictedV u (kN)
PredictedExperiment
PredictedV u (kN)
PredictedExperiment
W1-A C 50.15 58.58 1.17 119.07 2.37W2-A C 48.08 52.88 1.10 120.94 2.52W3-A C 43.38 46.30 1.07 70.42 1.62W4-A C 47.07 52.14 1.11 96.12 2.04
W1-B E 117.63 116.21 0.99 146.92 1.25W2-B E 120.36 104.79 0.87 150.05 1.25W3-B E 93.57 96.47 1.03 94.99 1.02
W2-C C 45.17 46.70 1.03 113.54 2.51W3-C C 44.33 48.65 1.10 73.38 1.66W4-C C 46.32 50.79 1.10 82.93 1.79
M2-A C 53.90 56.21 1.04 82.90 1.54 M3-A C 25.70 34.10 1.33 127.31 4.95 M4-A C 58.97 65.79 1.12 114.77 1.95
M2-B E 123.22 115.43 0.94 116.24 0.94 M3-B E 76.50 68.37 0.89 214.32 2.80 M4-B E 130.24 149.69 1.15 137.82 1.06
M3-C C 24.30 29.75 1.22 131.89 5.43 M4-C C 60.09 74.50 1.24 102.75 1.71
R90-D E 36.20 † 37.73 1.04 51.71 1.43
Mean : 1.081 2.097 Note: * C - corner column; E-edge column
† This specimen did not fail in punching; the reported result is the maximum value.
Failure load (Failure load ( kPakPa ))Model Type * Experiment Predicted Predicted
Experiment W1 SB 30.63 29.50 0.96W2 SB 28.91 30.00 1.04W3 SB 24.69 23.60 0.96W4 SB 28.95 25.75 0.89
M2 SB 32.70 † 37.50 † 1.15
M3 SB 17.84 15.60 0.87 M4 SB 33.85 37.00 1.09
R90-D SB 21.70 23.00 1.06
Mean : 1.003W5 TS 19.01 18.50 0.97
M5 TS 25.18 30.50 1.21 R3-A TS 23.80 20.50 0.86 R4-A TS 22.50 19.00 0.84
R90-A TS 25.50 23.50 0.92 R90-B FE 23.80 22.50 0.95 R90-C FE 20.00 20.50 1.03
Mean : 0.969
Note: † SB - spandrel beam; ‡ TS - torsion strip; * FE - free edge† Line load in kN/m
LFEM
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Crack patternCrack pattern
ObservedObserved(bottom surface)(bottom surface)
PredictedPredicted(bottom layer)(bottom layer)
PredictedPredicted(top layer)(top layer)
ObservedObserved(top surface)(top surface)
LFEM
Features – Q1 Tower
Instrumentation; Measurements;Prediction method; Comparison
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Level 63 as of 5 October 2004
Current State of ConstructionCurrent State of Construction
Q1 TOWER
Column and WallColumn and WallLocationsLocations
14 columns and 5 walls perfloor
Number of DEMEC point 3to 9 measurements percolumn/wall
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Instrumented Levels and Concrete Compressive
Strengths for Columns at the Specific Level
Level 71, 32 MPa
Level 49, 40 MPa
Level B1 and B2,65 MPa
Level 31, 50 MPa
Dateof
Construction
25/01/200319/02/2003
10/03/2004
02/08/2004
Jan 2005
Demountable MechanicalDemountable MechanicalStrain Gauge (DEMEC)Strain Gauge (DEMEC)
Gauge Length = 200 mm
1 division = 0.002 mm or 10 microstrain
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-100
0
100
200
300
400
500
600
700
0 100 200 300 400 500 600 700 Days
S
t r a
i n
1
0 -
6
TC05TC06
StartedDate
1/2/2003 1/6/2003 31/08/2003 31/11/2003 1/02/2004 1/06/2004
LastReading
23/09/2004
No. of slabsconstructed 0 2 6 13 27 5540
AUTUMN WINTER SPRING AUTUMN WINTER SUMMER
1.35
0.68
1.13
0.90
0.45
0.23
1.56
0
S h o r t e n
i n g
( m m
)
40 days time lag
-100
0
100
200
300
400
500
600
700
0 100 200 300 400 500 600 700 Days
S
t r a
i n
1
0 -
6
TC05
TC06
StartedDate
1/2/2003 1/6/2003 31/08/2003 31/11/2003 1/02/2004 1/06/2004
LastReading
23/09/2004
No. of slabsconstructed 0 2 6 13 27 5540
AUTUMN WINTER SPRING AUTUMN WINTER SUMMER
1.35
0.68
1.13
0.90
0.45
0.23
1.56
0
S h o r t e n
i n g
( m m
)
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-100
0
100
200
300
400
500
600
700
0 100 200 300 400 500 600 700 Days
S
t r a
i n
1
0 -
6
TC10TC12
StartedDate
1/2/2003 1/6/2003 31/08/2003 31/11/2003 1/02/2004 1/06/2004
LastReading
23/09/2004
No. of slabsconstructed 0 2 6 13 27 5540
AUTUMN WINTER SPRING AUTUMN WINTER SUMMER
1.35
0.68
1.13
0.90
0.45
0.23
1.56
0
S h o r t e n
i n g
( m m
)
Differential shortening160 microstrain0.36 mm
Differential shortening estimate (80 storey)
mm22227500010160 6
=
Age Adjusted Modulus Method Age Adjusted Modulus Method((TrostTrost andand BazantBazant , 1972), 1972)
[ ] [ ]1)s,t(C).s,t()s(E)t(
)t()s,t(C1)s(E
)t( 1c
s1c
it −χ
σ∆−ε++σ=ε
Elastic + creep
Shrinkage
ReinforcementRestraint
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Age Adjusted Modulus Method Age Adjusted Modulus Method((TrostTrost andand BazantBazant , 1972), 1972)
A computer program based on this method
COLECS by Allan Beasley (1987)
[ ] [ ]1)s,t(C).s,t()s(E)t(
)t()s,t(C1)s(E
)t( 1c
s1c
it −χ
σ∆−ε++σ=ε
-0.2
0.0
0.2
0.4
0.60.8
1.0
1.2
1.4
1.6
1.8
0 100 200 300 400 500 600 700 Days
COLECS
TC06
No of slabsconstructed 0 2 6 13 27 5540
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-0.2
0.00.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
0 100 200 300 400 500 600 700 Days
COLECS
TC10
No of slabsconstructed 0 2 6 13 27 5540
-0.2
0.0
0.2
0.4
0.60.8
1.0
1.2
1.4
1.6
1.8
0 100 200 300 400 500 600 700 Days
COLECS
TC12
No of slabsconstructed 0 2 6 13 27 5540
Q1 TOWER
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SUMMARYSUMMARY
On-Going work – HSC structures – Column and wall shortening – Deep beams and walls with openings
CrackingDampingDeflection
Flat plates, walls
Serviceability
Strength
Simplified solutions: explicit formulasRigorous solution: LFEM
Complicated problems
THANK YOU THANK YOU
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Section 2: Cracking and CrackWidth Formulas
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1
CRACKING AND CRACK WIDTHFORMULAS
PROFESSOR YEW-CHAYE LOO
DeanFaculty of Engineering & Information Technology
Griffith UniversityQueensland , Australia
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OVERVIEWINTRODUCTIONCRACKING – TYPES, CAUSES & FORMULASTEST PROGRAMPROPOSED CRACK WIDTH FORMULAS FORNSC BEAMSCOMPARISON WITH TEST DATACOMPARISON WITH CODE FORMULASCOMPARISON WITH OTHER FORMULASVERIFICATION FOR HSC BEAM DATACONCLUSIONS
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2
INTRODUCTIONServiceability is one of the major considerations inthe design of structuresCracking and crack control in concrete structuresare major serviceability issuesCracking is more pronounced for high strengthconcrete (HSC) structures because of their relativebrittleness compared to normal strength concrete(NSC)
All major codes for design and construction withconcrete are applicable only to and based on NSC
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CRACKING – TYPES, CAUSES & FORMULASTypes of Cracks:
Cracking in reinforced concrete buildings orstructural elements is usually classified accordingto the cause of cracking
There are five major types of cracks:flexural cracks in reinforced (and prestressed)concrete beams, frames, and slabs;diagonal tension (shear cracks);splitting cracks along the reinforcement in beamsand in the anchorage zones of prestressedelements;cracking in concrete shear walls; andtemperature and shrinkage cracks
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3
There are many factors causing cracks in concreteCracks caused by load are the main ones consideredin designThe others are usually eliminated or reduced byselecting suitable material and improving the qualityof constructionFlexural crack width depends on geometrical f actorsand on loadingThe width of crack is restricted at the transverse barsin reinforced concrete members and it widens towardthe surface of the member The Concrete Cover and the Spacing of the barsare of primary importance
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Loading affects crack width several waysThe crack width is proportional to f s n ,where f s is the steel stress and n is about1.4. However, n can be taken as unitywithout significant error The distribution and width of cracks alsodepend on the variation of momentsalong the member The loading history is also important
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4
Prediction of crack widths has been studiedby many researchersMost of the available crack width formulasare based on research conducted onstructural members made of NSCThe authors also developed two NSC beamformulas
for average crack widthsfor maximum crack widths
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8 full-scale HSC beams were tested tofailure to investigate the crackingbehaviour of HSC beams
A comparison is made with the authors’proposed NSC beam formulas to verifytheir applicability to HSC beams
The NSC beam formulas are found to begenerally applicable to HSC beams
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5
TEST PROGRAMTotal 30 NSC RC & PPC beamsand 8 HSC RC beams
Beam length, L
l
Applied load
Loading beam
100 mm 100 mm
Typcal loading diagram
Embedded Polystyrene
as void
60 180 60
2 5
1 0 0
Typical RC box beam
2 8
300 mm
3 0 0 m m
mm m m
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Overall cross-section 300 mm x 300mm
180 mm x 180 mm void
3 different L – 5.5 m, 6.7 m & 8.0 m
5 different ρ values
f ′c varied from 25.4 to 37.7 MPa
11 RC simply-supported box beams
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6
12 PPC simply-supported box beams
3 different L- 5.5 m, 6.8m & 8.0 m4 different degrees of prestressingf’c varied from 25.9 to 46.4 MPa4 different ρ values
Typical PPC beam
Embedded Polystyrene
asvoid
180 60
2 5
1 0 0
300 mm
3 0 0 m m
mm
1 7 5
m m 60
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4 RC simply-supported solid beams
35 40
36 78 36
3 6 2 0
Typical RC solid beam
3540
2 1 0
4 0 2 0
Cross-section - 150 mm x 250mm All 2.5 m longf’c varied from 34.1 to 37.1 MPa3 different ρ values
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7
3 RC two-equal-span continuous beams
Embedded Polystyrene
as void
36 76 76 36
60 180 60
1 0
1 3 0
4 6
6 0
Section at mid-span
1 4 3 6
Embedded Polystyrene
as void
36 228 36
36 57 36
1 0
4 6
3 2
Section over thesupport
1 4
1 8 0
3 6
5757 57
2 8
76
12 m long - two spans 6 m eachf’c varied from 30.6 to 34.2 MPa3 different positive ρ values3 different negative ρ values
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8 HSC RC simply-supported beams
3 beams of cross-section 300 mm x 300 mm, 3 of250 mm x 250 mm and 2 of 150 mm x 200 mm6 different L – 2.4 m, 3.0 m, 4.0 m, 4.5 m, 5.0 m& 6.0 m5 different ρ valuesf ′c varied from 58.3 to 65.9 MPa
25
150
2525 100
200
300
25 250 25
25 -35
300 x 300 mm beam section 150 x 200 mm beam section
250
25 200 25
30 -35
250 x 250 mm beam section
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8
Test ProcedureBeams subjected to two-pointstatic loading
Crack widths at each load levelmeasured using a crack detectionmicroscope
Crack spacings measured at 60 to70% of ultimate load
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PROPOSED NSC BEAMCRACK WIDTH FORMULAS
Crack formation and developmentis a complex phenomenoninvolving many parameters
Crack spacing, lcr related to:(i) the Φ/ρ ratio; Φ = avg. bar dia(ii) the concrete cover, c(iii) the average spacing between
reinforcing bars, s
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9
The regression equation takes theform:
lcr = C 1 c + C 2 s + C 3 (Φ/ρ)
4 RC and 4 PPC beam data usedin the regression analysis
These are from the earlier tested30 NSC beams
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Table 1. Parameters used in development of averagecrack spacing formula
Beam
number
Average bar
diameter,
Φ (mm)
Steel ratioρ
TheratioΦ/ρ
(mm)
Averagespacing
between
bars, s(mm)
Concretecover, c
(mm)
Averagecrack
spacing, lcr
(mm)
2 20 0.01154 1733 120 12 131.66 20 0.02309 866 48 12 43.7
10 24 0.03348 717 48 12 48.711 20 0.01154 1733 120 12 120.021 6.6 0.00511 1292 40 27 126.523 10.8 0.00737 1465 62 38 126.924 8.1 0.00730 1110 38.5 27 118.230 5.6 0.00460 1217 40 40 142.0
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10
The resulting equation for averagecrack spacing:
lcr = 0.6(c - s) + 0.1 ( Φ /ρ )
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Crack Width Formulas for NSCBeams
The proposed formula for averagecrack widths, w
cr ,is developed as:
wcr = (f s /E s) [0.6(c - s) + 0.1 ( Φ /ρ)] (1)
The proposed formula for themaximum crack widths is:wmax = 1.5 (f s /E s ) [0.6(c - s) + 0.1 ( Φ /ρ)] (2)
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11
COMPARISON WITH TEST DATA Authors’ Test Beams (30 NSC)
wcr, calculated in mm
0.40.30.20.10.0
w c r ,
m e a s u r e
d i n m m
0.4
0.3
0.2
0.1
0.0
- 30% line
+ 30% linePartially prestressed concrete beamsReinforced concretecontinuous beamsReinforced concretesolid beamsReinforced concrete
box beams
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Other Beams
26 Clark’s (1956) RC beams
16 Chi & Kirstein”s (1958) RCbeams
8 Hognestad’s (1962) RC beams
9 Kaar & Mattock’s (1963) RCbeams
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12
Other Beams (Continued)
34 Nawy”s (1986) beams
• 20 pre-tensioned – 6 fully prestressed T-beams – 12 PPC T-beams – 2 PPC I-beams
• 14 post-tensioned PPC T-beams
Crack widths comparedboth at tension face and steel levelboth average and maximum
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Investigator Reinforcementstress levels,ksi
No. ofspecimens
No. of observations
Averagecrack width
Maximumcrack width
Clark (1956) 15, 20, 25,30, 35, 40, 45 26 161
Chi &Kirstein ( 1958 )
15, 20, 25,30, 35, 40
16 76
Hognestad (1962)
20, 30, 40, 50 8 32
Kaar &Mattock ( 1963 )
40 9 9
Nawy (1986) 30, 40, 60 34 102
(1 ksi = 6.895 Mpa)
Table 2. Crack width test data
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13
Equation 1 or 2 in mm
.9.8.7.6.5.4.3.2.10.0
M e a s u r e d c r a c
k w
i d t h s
i n m m
.9
.8
.7
.6
.5
.4
.3
.2
.1
0.0
Legend
+ 30% line
- 30% line
Kaar & Mattock's bea
Hognestad's beams
Nawy 's beams
(14 post-tensioned)
Nawy 's beams(20 pre-tensioned)
Chi & Kirstein's bea
Clark's beams
93 Other Beams (All NSC)
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COMPARISON WITH CODE FORMULASCode Formulas Compared
ACI formula (ACI, 1995)wmax at tension face for RC beams
BS formula (BS, 1985; BS, 1987)wmax at tension face for RC beams
Eurocode formula (EC2, 1991).wcr at tension face for RC beams
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14
Comparison with Eurocode formulaThe measured crack widths are divided bythe calculated widths to evaluate theaccuracy of the calculation methodsThe test data included 199 data points fromauthors’ 18 RC beams and those from Clark(1956)’s and Chi & Kirstein (1958)’s beamsThe results are presented in figure on nextslide
It can be seen that both the formulas providereasonable results, with no one methodproviding more accurate results than theother
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Eurocode versus Proposed Formula – Authors, Clark’s and Chi & Kirstein’sbeams
Measured/calculated crack width (Eurocode formula)
2.462.191.921.651.381.12.85.58.31.04
N u m
b e r o
f o b s e r v a
t i o n s
100
80
60
40
20
0
Measured/calculated crack width (Equation 1)
2.362.071.781.491.20.91.63.34.05
N u m
b e r o
f o b s e r v a
t i o n s
100
80
60
40
20
0
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15
Comparison with the ACI and the BS formulasThe measured crack widths are divided by the calculatedwidths to evaluate the accuracy of the calculationmethodsThe test data included data points from Clark (1956)’sand Chi & Kirstein (1958)’s beamsFor Chi & Kirstein’s beams the calculated crack widthswere multiplied by the strain gradient factor βThe results are presented in figure on next slide
It is found that while both the proposed and the ACI formulas reasonably deter-mine the crackwidths, the BS formula grossly underestimatesthe values
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Measured/calculated crack width (Equation 2)
5.704.904.103.302.501.70.90.10
N u m
b e r o f o b s e r v a t
i o n s
100
80
60
40
20
0
Measured/calculated crack width (ACI formula)
5.704.904.103.302.501.70.90.10
N u m
b e r o f o b s e r v a t
i o n s
100
80
60
40
20
0
Measured/calculated crack width (BS formula)
5.704.904.103.302.501.70.90.10
N u m
b e r o
f o b s e r v a
t i o n s
100
80
60
40
20
0
Comparison of formulas - Clark’s and Chi &Kirstein’s beams
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17
Calculated maximum crack w idths in mm
1.21.0.8.6.4.20.0
M e a s u r e
d m a x
i m u m c r a c
k w
i d t h s
i n m m
1.2
1.0
.8
.6
.4
.2
0.0
Legend
- 30% line
+ 30% line
Suri and Dilger
Batchelor-El Shahawi
Modified Gergely-
Lutz formula
Equation 2
Comparison of formulas – Authors’ 7 PPCbeams
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VERIFICATION FOR HSC BEAMDATA
For each beam, at different steel
stress levels both average andmaximum crack widths calculated
Measured and calculated crackwidths are compared
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18
Comparison for Average Crack Widths
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
0.5
0 0.1 0.2 0.3 0.4 0.5
Predicted average crack widths in mm
M e a s u r e d a v e r a g e c r a c
k w
i d t h s
i n m m
Beam HSB 1
Beam HSB 2
Beam HSB 3
Beam HSB 4
Beam HSB 5Beam HSB 6
Beam HSB 7
Beam HSB 8
+ 30% line
- 30% Line
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Comparison for Maximum Crack Widths
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Predicted maximum crack widths in mm
M e a s u r e
d m a x
i m u m
c r a c
k w
i d t h s
i n m m
Beam HSB 1
Beam HSB 2Beam HSB 3
Beam HSB 4
Beam HSB 5
Beam HSB 6Beam HSB 7
Beam HSB 8
+ 30% Line
- 30% Line
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19
CONCLUSIONS8 full-size HSC beams tested to investigate thecracking characteristics of HSC beams
Average and maximum crack spacings andcrack widths measured at each level of loadingfor each beam
The authors’ earlier developed NSC beamcrack width formulas verified for theirapplicability to HSC beamsThe initial findings are very encouraging asmost of the data points lay within + 30% limits
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TUTORIAL EXERCISESFor a simply supported beam of the following cross-section and aspan of 2.4 m, calculate the average crack widths (use Chowdhury& Loo formula) at 3, 5, 7, 9, 11, 13 and 15 kN loads applied at thecentre of the beam. The stirrups used are10 mm diameter plainbars. The beam cross-section is 150 mm x 250 mm.
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35 40
36 78 36
3 6 2 0
Typical beam cross-section
3540
2 1 0
4 0 2 0
2-N 12 bars3-N 20 bars
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Section 3: Damping Characteristicsand Analysis
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THE APPROACH• In total, 26 beams tested• Free-decay method was used for the
determination of damping• Damping values ( δ) predicted from the residual
crack widths and span lengths of beams• Residual crack widths are related to the
instantaneous crack widths
• 4 RC and 4 PPC beam data used forformulation
• Comparisons were made with test results fromall 26 NSC beams and 8 HSC beams
DAMPING - DEFINITION ANDMODEL
• Nature of Damping – There are mainly three ways in which energy
is dissipated:• (i) Material Damping• (ii) System Damping• (iii) Radiation Damping
– These together constitute the structuraldamping
• Damping Model – Viscous Damping
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DAMPING MODELS• Friction or Coulomb Damping due to
microcracking - Rubbing of cracked surfaces• Viscous Damping due to the moisture movement
within the pores• Solid damping due to the sliding friction within
the gel structure
• Total energy dissipation due to inelasticdeformations and energy dissipation at crackedsurfaces
DAMPING - DEFINITION ANDMODEL
• The logarithmic decrement , δ , is obtainedas:
δ = (1/n) log e
Time t
Amplitude A
A 1A n+1
n periods
1n
1
A1),(ncycleatamplitudeA1,cycleatamplitude
++
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• The damping coefficient C, or alternativelythe damping ratio ξ , where ξ = C/C c, inwhich C c is the critical damping constant,is related to δ as
δ = =
where m and ωd respectively are the massand the damped natural frequency of freevibration
ξ−
πξ21
2
ω
π
dmC
DAMPING - DEFINITION ANDMODEL
EXPERIMENTAL PROGRAM
• 11 reinforced concrete simply supported beams• Full-size box beams - overall cross-section 300
mm x 300 mm (for all beams)• 180 mm x 180 mm void in each beam -
embedded polystyrene prism• 3 different L – 5.5 m, 6.7 m and 8.0 m• 5 different ρ values – 0.01154, 0.01163,
0.02309, 0.02326 and 0.03348• f ′c varied from 25.4 to 37.7 MPa
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EXPERIMENTAL PROGRAM,CONT.
Beam length, L
l
Applied load
Loading beam
100 mm 100 mm
Typcal loading diagram
EmbeddedPolystyrene
as void
60 180 60
2 5
1 0 0
Typical RC box beam
2 8
300 mm
3 0 0 m m
mm m m
EXPERIMENTAL PROGRAM,CONT.
• 12 partially prestressed concrete simplysupported beams
• 3 different L – 5.5 m, 6.8 m and 8.0 m• f ′c varied from 25.9 to 46.4 MPa• 4 different degrees of prestressing - 0.25,
0.50, 0.75 and 1.00• 4 different ρ values – 0.00460, 0.00511,
0.00730 and 0.00737
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EXPERIMENTAL PROGRAM,CONT.
• 3 two-equal-span continuous beams• Each beam 12 m long - 2 spans 6 m each• f ′c varied from 30.6 to 34.2 MPa• 3 different positive ρ values – 0.01163,
0.02283 and 0.02361• 3 different negative ρ values – 0.01519,0.02714 and 0.02854
TEST PROCEDURE
• Beams were tested in two stages understatic loading
• Residual crack widths measured at zero
load after each load application• Free vibration with hammer excitation
used for damping measurement• Accelerometer at the center of the beam to
receive the vibration signals
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TEST PROCEDURE, CONT.
Stages in a vibration measurement system
DEVELOPMENT OF DAMPINGPREDICTION FORMULAS
• Variables influencing logarithmicdecrement , δ – beam span lengths, L – compressive strengths of concrete, f ′c – degrees of prestressing, η – steel ratios, ρ – residual crack widths, w r
• The main factors affecting the dampingvalues were found to be w r and L
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REINFORCED CONCRETEBEAMS
• Data from the following 4 beams were used in theregression analysis
• The resulting damping prediction formula isδ = 0.048 w r + 0.011 L
1 25.9 20 3 5.5
6 25.4 20 6 5.5
8 31.0 20 3 8.0
BEAMNUMBER
f c(MPa)
Bardiameter
Numberof bars
BeamLength (m)
11 27.6 20 3 6.7
PARTIALLY PRESTRESSEDCONCRETE BEAMS
• Data from the following 4 beams used in theregression analysis
• The resulting damping prediction formula is:δ = 0.054 w r + 0.0104 L
Beamnumber
f c
(MPa)Prestres-sing steel
Reinforcingsteel
Beamlength
Degree of prestressing
15 25.9 2φ5 2Y16+1Y12 5.5 0.2518 31.0 10φ5 1Y12 5.5 1.0022 31.3 7φ5 2Y12 6.8 0.7524 39.1 5φ5 4Y12 8.0 0.50
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RESIDUAL CRACK WIDTHPREDICTIONS
• Residual crack width is obtained from instantaneousaverage crack width, w i using
w r = 0.312 w i• A unified formula for the prediction of w i is given as
w i = (f s /E s ) [0.6 (c – s) + 0.1 ( ρ )]where
– f s is the average steel stress – E s is the modulus of elasticity for steel – c is the concrete cover – s is the average spacing between the reinforcing bars – Φ is the average bar diameter – ρ is the steel ratio
COMPARISON WITH TESTDATA
• For the 14 RC beams
Measured versus predicted damping values
Predicted δ - Equation 3
.16.12.08.040.00
M e a s u r e
d δ
.16
.12
.08
.04
0.00
+ 30% limits
- 30% limits
Continuous beams
Simply-supported
beams
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COMPARISON WITH TESTDATA
• A good correlation exists between the calculatedand the measured damping values
• The majority of the 191 correlation points lie wellwithin the + 30% limits
• All but one of the correlation points for the 3 two-equal-span continuous beams lie well within the+ 30% limits
• This indicates that the damping formula which isdeveloped based on simply-supported beamdata is also applicable to the individual spans ofcontinuous beams
COMPARISON WITH TESTDATA
• For the 12 PPC beams
Measured versus predicted damping values
Predicted d - Equation 4
.16.12.08.040.00
M e a s u r e
d d
.16
.12
.08
.04
0.00
- 30% limits
+ 30% limits
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COMPARISON WITH TESTDATA
• The overall correlation is acceptable as amajority of the 81 correlation points liewithin + 30% limits
• It should be pointed out that, for partiallyprestressed beams with low or no
residual crack widths, the measureddamping values varied widely for thedifferent test beams
• This may be due to the inaccuracy of thecrack measurements
COMPARISON WITH HSC BEAMS
• Eight full-size simply-supported reinforced HSC beams
• Cracking characteristics in terms of crack spacing andwidth
• Damping behaviour in terms of logarithmic decrementsin free vibration
• Beams subjected to two-point loading for crackdevelopment in a constant moment region
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DETAILS OF TEST BEMS
4.5058.34 – N20250 x 250HSB 86.0058.34 – N24300 x 300HSB 75.0065.93 – N20250 x 250HSB 64.0065.93 – N20250 x 250HSB 52.4063.43 – N16150 x 200HSB 42.4061.53 – N16150 x 200HSB 35.0062.33 – N28300 x 300HSB 23.0060.93 – N24300 x 300HSB 1
SpanL (m)
f ′ c(MPa)
A stb x D(mm x mm)
BeamDesignation
Cross Sectional Details of Test Beams
25 for HSB 130 for HSB 2
25
150
2510025
R6 stirrups @100 mm c/cfor HSB 3
250
2520025R10 stirrups@ 75 mm c/cfor HSB 4
250
300
25 250 25
R10 stirrups @110 mm c/c for HSB 1
R6 stirrups @110 mm c/cfor HSB 2
30 for HSB 535 for HSB 6
300
25 250 25
300
35
175
250
25 200 25
250
R6 stirrups @120 mm c/c
30
Beams HSB 1 and HSB 2 Beam HSB 7
Beams HSB 3 and HSB 4 Beams HSB 5 and HSB 6
Beam HSB 8
Beam length, L
l
Applied load
Loading beam
200 mm 200 mm
l = 867 mm for beam HSB 1, l = 1534 mm for beam HSB 2,l = 667 mm for beam HSB 3, l = 734 mm for beam HSB 4,
l = 1200 mm for beam HSB 5, l = 1534 mm for beam HSB 6,l = 1867 mm for beam HSB 7 and l = 1367 mm for beam HSB 8
Loading Arrangementsfor Test Beams
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COMPARISON OF DAMPINGVALUES
0
0.01
0.02
0.03
0.04
0.05
0.06
0.07
0.08
0.09
0 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08 0.09
Predicted δ
M e a s u r e
d
Beam HSB 1
Beam HSB 2
Beam HSB 5
Beam HSB 6
Beam HSB 7
Beam HSB 8
+ 30% Line
- 30% Line
CONCLUSIONS
• Two damping prediction formulasdeveloped – one for RC and one for PPCbeams
• Comparison with the test data of all the 26NSC and 8 HSC beams shows that theaccuracy of the proposed formulas is good
• The formula for RC beams is alsoapplicable to continuous beams
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Section 4: Deflection
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DEFLECTION
PROFESSOR YEW-CHAYE LOO
DeanFaculty of Engineering & Information Technology
Griffith UniversityQueensland , Australia
SHORT COURSE ON
ADVANCED TOPICS IN ANALYSIS AND DESIGN OF CONCRETE STRUCTURESSKuala Lumpur, Malaysia 5-6 September 2005
DEFLECTION
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• Deflection
– static loading
– repeated loading
– impact
● A new method for incorporatingtension stiffening effects
● Curvature values at sectionsbetween adjacent cracks
● Short-term deflections for 35flexural members compared
_____________________________________________________________ *Piyasena, R., Loo, Y.C. & Fragomeni, S. 2002
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• Procedure for intensive creepdeflection of R.C. box beams*
• The intensive creep factor is
k = k 1 + R log 10 T where T is the number of loading cycles,
k1 = 1.18 + (0.029/r) {(M t – Md)/(My – Mcr )} andR = (0.0015/r) {(M t – Md)/(My – Mcr )}
____________________________________________ *Loo, Y.C. & Wong, Y.W. 1983, 1984, 1986; Wong, Y.W. & Loo, Y.C. 1985
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Deflection of RC beams under repeated loading
k versus T for M t/M v = 0.7
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k versus steel ratio for M t/M v = 0.7
• Maximum deflection of RC and PPCbeams* – deflection under repeated mid-span
impact of below yield intensity
– Deflections compared – Comparisons with other formulas – Design charts produced ___________________________________________ *Loo, Y.C. & Santos, A.P. 1985; Loo, Y.C. 1991
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Correlation of measured and computed total deflections – proposed formula
Correlation of measured and computedtotal deflections – Balaguru & Shah(1982) formula
Correlation of measured and computedtotal deflections – Lovegrove & El Din(1982) formula
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y´max = y max / [(2/m bω12) (1.25 m s v02 k 2/3)3/5]
α = (m b/m s)β = 1.47 ( ω1/π) (5m s/4kv 01/2)2/5
ω1 = (π2/L2) √(EI/ ρA)
IMPACT AND ENERGY ABSORPTION
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• Impact deflection analysis ofbeams• Precast beam-column
connections – under repeated load – under cyclic loading
• An analytical solution for instantaneousdeflection of beams under mid-spanimpact*
• An integral equation incorporatingHertz’s contact law
• Equivalent moment of inertia forrepeated loading• RC and PC beams• Comparisons with published results
___________________________________________________ *Loo, Y.C. & Santos, A.P. 1986
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Correlation of measured and computed deflections – Hussain’s (1982)and Wijewardene’s (1984) beams
Correlation of measured and computed deflections – Bate’s (1961) beams
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Correlation of measured and computed deflections – Hughesand Speir’s (1982) beams
• 18 half-scale interior connection modelstested*
• Under static and repeated loading• Two types of precast RC beam-column
connections• The precast connections were superior to
their monolithic counterparts ___________________________________________________ *Yao, B.Z. & Loo, Y.C. 1993; Loo, Y.C., Yao, B.Z. & Han, Q. 1994; Loo, Y.C. &Yao, B.Z. 1995
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Precast connection Type A Precast connection Type B
Test setup Typical load history
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Load-deflection curves under static loading
Load-deflection curves under repeated loading
• 12 half-scale interior connectionmodels tested*
• Under repeated and cyclic loading• Two types of precast RC beam-
column connections• Precast connections possessed
larger energy absorbing capacitiesthan the monolithic models ___________________________________________________ *Loo, Y.C., Yao, B.Z. & Takheklambam, S. 1996
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Load history for cyclic tests
Load-deflection curve under cyclic loading
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THANK YOU THANK YOU ALL ALL
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Section 5: Punching Shear StrengthAnalysis of Concrete FlatPlates
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1
PUNCHING SHEAR DESIGN OF REINFORCED ANDPOST-TESIONED CONCRETE FLAT PLATES: ARE THE MAJOR DESIGN CODE METHODS
ADEQUATE?
Professor Yew-Chaye Loo
Faculty of Engineering and InformationTechnology
Griffith University
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26
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Section 6: Ultimate StrengthAnalysis of Walls (Solidand with Openings)
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1
Ultimate Strength Analysis ofConcrete Walls (Solid and with
Openings)
AimAimTo investigate the failure behaviour of reinforcedTo investigate the failure behaviour of reinforcedconcrete walls with and without openingsconcrete walls with and without openings
simply supports top and bottom
onlysimply supports on all sidesSolid/ Opening panelsvarying slenderness(H/t w)
New design formula for wallwith/without openings
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3
(a) In-plane vertical load
(b) Transverse horizontal load (c) In-plane horizontal load
One and TwoOne and Two --way actionway action
Typical example of Concrete core wallsB) Two-way actionA) One-way actionAS 3600(2001)ACI 318(2005)
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4
Code MethodsCode MethodsAS3600-01 – Section 11 (Design of walls -simplified formula) – Section 10 (Design of columns for
strength and serviceability
ACI318-05
– Chapter 14
BS8110-97 – Section 3.9.4 (Identical to AS3600)
'cawu )0.6f 2e1.2e(t N −−=
AS3600AS3600--01 Wall Design Method01 Wall Design Method
⎟⎟
⎠
⎞⎜⎜
⎝
⎛ ⎥⎦
⎤⎢⎣
⎡=2
ww
'cu t32
kH-1tf 55.0 N
ACI318ACI318--02 Wall Design Method02 Wall Design Method
Ultimate strength per unit length of wall (N/mm)
Thickness of the wall
Eccentricity of load
Additional eccentricity=Hwe2/2500t w
Concrete strength
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5
LimitationsLimitations
AS3600-01Hwe/tw ≤30
f ’c ≤ 65 MPae ≥ 0.05t w(=tw/20)
Only one-way actionOnly solid walls
ACI318-05/BS8110H/t w ≤25 or L/ t w ≤25
f ’c ≤ 50 MPae ≤ tw/6Only one-way actionOnly solid walls
0
0.1
0.2
0.3
0.4
0.5
0.6
0 10 20 30 40 50
H/t
N u
/ ( f ' c A g
)
AS3600
ACI318
Pillai(1977)
Saheb/Desayi(1989)
Fragomeni(1995)(NSC)
Fragomeni(1995)(HSC)
Butler(1998)
Previous experimental results o f One-way action
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6
0
0.2
0.4
0.6
0.8
1
1.2
0 10 20 30 40 50H/t
N u
/ ( f '
c A
g )
Saheb & Dasey (1991)
Fragomeni(1995) (NSC)
Fragomeni(1995) (HSC)
Previous experimental results of Two-way action
Test specimens and test set upTest specimens and test set up((eccecc =t/6,=t/6, ρρvv== ρρhh = 0.0031= 0.0031))
H (mm) L (mm) t w (mm) f'c(MPa) H/t w AS3600
OWNS2 1200 1200 40 35.7 30.00
OWNS3 1400 1400 40 52.0 35.00
OWNS4 1600 1600 40 51.0 40.00
OWHS2 1200 1200 40 78.2 30.00
OWHS3 1400 1400 40 63.0 35.00
OWHS4 1600 1600 40 75.9 40.00
TWNS1 1000 1000 40 45.4 25.00
TWNS2 1200 1200 40 37.0 30.00
TWNS3 1400 1400 40 51.0 35.00
TWNS4 1600 1600 40 45.8 40.00
TWHS1 1000 1000 40 68.7 25.00
TWHS2 1200 1200 40 64.8 30.00
TWHS3 1400 1400 40 60.1 35.00
TWHS4 1600 1600 40 70.2 40.00
68.544 kN68.544 kN
N/AN/AN/AN/A
N/AN/AN/AN/AN/AN/AN/AN/A
N/AN/AN/AN/AN/AN/AN/AN/A
N/AN/AN/AN/AN/AN/A
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7
H (mm) L (mm) tw (mm) f'c(MPa) H/t w H/LTAHS1 1600 1400 40 77.8 40.0 1.1TAHS2 1400 1000 40 73.8 35.0 1.4TAHS3 1600 1000 40 77.8 40.0 1.6
Test specimens and test set upTest specimens and test set up((eccecc =t/6)=t/6)
TestTest --rigrig
set upset up
(2400(2400 kNkNcapacity)capacity)
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8
Eccentricity t/6
∅23 roller
150 ×50 plate20 ×20 EA
40mm thickness test panel
Support ConditionSupport Condition(one(one --way)way)
Side Support ConditionSide Support Condition(two(two --way)way)
150 PFC
40 ×40 ×5 SHS
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9
1600x1600x40 (f 1600x1600x40 (f ’’c=50MPa)(onec=50MPa)(one --way)way)
1600x1600x40(f 1600x1600x40(f ’’c=76MPa)(onec=76MPa)(one --way)way)
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11
1600x1600x40(f 1600x1600x40(f ’’c=70MPa)(Twoc=70MPa)(Two --way)way)
1600x1000x40(f 1600x1000x40(f ’’c=78MPa)(Twoc=78MPa)(Two --way)way)
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12
Experimental results of OneOne --way actionway action
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 10 20 30 40 50
H/t
N u
/ ( f '
c A
g )
AS3600
ACI318
Pillai(1977)
Saheb/Desayi(1989)
Fragomeni(1995)(NSC)
Fragomeni(1995)(HSC)
Butler(1998)
Doh(2002)(NSC)
Doh(2002)(HSC)
Experimental results of TwoTwo --way actionway action
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 10 20 30 40 50H/t
N u
/ ( f ' c A
g )
AS3600
ACI318
Saheb/Desayi(1990)
Fragomeni(1995)(NSC)
Fragomeni(1995)(HSC)
Doh (2002)(NSC)
Doh (2002)(HSC)
Doh (2002)(HSC)
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0200400600800
10001200140016001800
0 5 10
Deflecti on (mm)
L o a
d ( k N )
TWNS4(top)TWNS4(middle)TWNS4(bottom)TWNS4(side)TWHS4(top)TWHS4(middle)TWHS4(bottom)
TWHS4(side)
LoadLoad vsvs Deflection for TWNS4 and TWHS4Deflection for TWNS4 and TWHS4
Laboratory tests (half-scale of 17 NSCand HSC wall panels)H/t w ↑ with N u/(f’cLt) ↓
Nu/(f’cLt) HSC < N u/(f’cLt) NSC
H/L ↑ with N u/(f’cLt) ↑
Summary of test resultSummary of test result
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Limitations of code methods – f’c
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for simply supported top and bottomonly
for H ≤ L when all four all sides arerestrained
for H > L when all four all sides arerestrained
2
LH
1
1
⎟ ⎠ ⎞
⎜⎝ ⎛ +
α=β
H2Lα=β
α=β
where α is eccentricity parameter and is equal to:
wte
1
1
−=α 88.0
ww t
H
18
te
1
1
⎟⎟
⎠ ⎞
⎜⎜
⎝ ⎛
×−
=α
for H/t w < 30 for H/t w ≥30
H we = H
WallPanels
Failure Load(kN)
Proposed Eq(kN)
Proposed EqFailure load
OWNS2 253.10 250.54 0.99
OWNS3 426.73 340.86 0.80OWNS4 441.45 344.69 0.78OWHS2 482.65 433.76 0.90OWHS3 441.45 389.93 0.88OWHS4 455.84 455.29 1.00
MeanStandard Deviation
0.890.09
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WallPanels
Failure load(kN)
Proposed Eq(kN)
Proposed EqFailure load
TWNS1 765.2 716.43 0.94TWNS2 735.8 707.66 0.96TWNS3 1177.2 1 1020.16 0.87TWNS4 1177.2 1 1067.91 0.91TWHS1 1147.8 957.77 0.83TWHS2 1177.2 1 1047.60 0.89TWHS3 1250.8 1144.67 0.88TWHS4 1648.1 1440.23 0.86TAHS1 1618.7 1486.51 0.92TAHS2 1118.3 1381.09 1.23TAHS3 1265.5 1137.18 0.90TAHS4 1442.1 1228.22 0.85
Mean 0.92Standard Deviation 0.11
Notes: 1 Hydraulic jacks measured 40 tonnes for these specimens (40 ×3×9.81kN).The accuracy of jack was ± 1 tonne ( = 9.81 kN).
2 Load eccentricity = tw/6
Comparison with test data –one-way action
H/t w
N u
/ f '
c L t w
0 10 20 30 40 50 600
0.1
0.2
0.3
0.4
0.5
0.6
0.7
f' c = 30 M Paf' c = 50 M Paf' c = 80 M PaFragomeni (NSC)Fragomeni (HSC)OWNS (Stage 1)OWHS (Stage 2)Doh (HSC)Doh (NSC)
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Comparison with test data – two-way action
H/t w
N u
/ f '
c L t w
10 20 30 40 50 60
0.3
0.4
0.5
0.6
0.7
0.8 f' c = 30 M Paf' c = 50 M Paf' c = 80 M PaSaheb & Desayi (1990)Fragomeni (NSC)(1995)Fragomeni (HSC)(1995)Doh (NSC)Doh (HSC)
H/L
N u
/ f ' c L t w
0.5 1 1.5 20
0.1
0.2
0.3
0.4
0.5
0.6
f' c = 30 M Paf' c = 50 M Paf' c = 80 M PaTA H S ( H /t w = 4 0)TA H S ( H /t w = 3 5)L F EM r es u lt s ( f' c = 30 M P a)L F EM r es u lt s ( f' c = 50 M P a)WASTAB resu lt s ( f' c = 30 M P a)WASTAB resu lt s ( f' c = 50 M P a)
Comparison with test data – two-way action
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Test specimensTest specimens --opening panelsopening panels
and test set upand test set up((eccecc =t/6,=t/6, ρρvv== ρρhh = 0.0031= 0.0031))WallPanel
Height(H: mm)
Length(L: mm)
Thickness(tw: mm)
Opening size(mm × mm)
Concretestrength
(f’c: MPa)H/t w
OW01 1200 1200 40 None 35.7 30
OW02 1600 1600 40 None 51.0 40
OW11 1200 1200 40 300 ×300 53.0 30OW12 1600 1600 40 400 ×400 47.0 40OW21 1200 1200 40 300 ×300 50.0 30OW22 1600 1600 40 400 ×400 51.1 40
TW01 1200 1200 40 None 37.0 30TW02 1600 1600 40 None 45.8 40
TW11 1200 1200 40 300 ×300 50.3 30TW12 1600 1600 40 400 ×400 50.3 40TW21 1200 1200 40 300 ×300 50.3 30TW22 1600 1600 40 400 ×400 50.3 40
Numberof
openings
One-wayaction
Two-wayaction
T
Typical example of concrete panel dimensions
(a) OWN11/TW11 (b)OW12/TW12
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Reinforcement layout
Shrinkagecontrol
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OW11OW11 1200x1200x401200x1200x40((f f ’’
cc= 53 MPa)= 53 MPa)
OW21OW21 1600x1600x401600x1600x40
((f f ’’cc= 50 MPa)= 50 MPa)
TW11TW11 1200x1200x401200x1200x40((f f ’’cc= 50.3MPa)= 50.3MPa)
TW12TW12 1600x1600x401600x1600x40((f f ’’cc= 50.3MPa)= 50.3MPa)
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TW21TW21 1200x1200x401200x1200x40((f f ’’
cc= 50.3MPa)= 50.3MPa)
TW22TW22 1600x1600x401600x1600x40
((f f ’’cc= 50.3MPa)= 50.3MPa)
LoadLoad vsvs Deflection for TW21Deflection for TW21
0
100
200
300
400
500
600
700
0 2 4 6 8 10
Lateral Deflection (mm)
L o a
d ( k N )
top
middle
bottom
side