final year project presentation (june 2015) : investigation of shear behaviour of slender beams...
TRANSCRIPT
US Air Force Warehouse, Ohio, USA(August,1955)
Kayani (2014)
Johnson M K (1989)
Taylor
Angelakos (2001)
Zararis (2003)
Kani G (1964)
AC Scordelis
Collins M P (2008)
Placas A (1971)S Mindess (2003)
Z P Bazant (1984)
Z Zheng (2000)
R Malm (2009)
C Juarez (2007)
JCM Ho FTK Au (2005)
L Vandewalle (2000)A Buuml (2010)
J Thomas (2007)
S Colombo (2005)
MZ Jumaat (2010)
L Li Y Guo (2008)
K Chansawat (2009)
KS Elliott (2002)
E Ahmad (2011)
CM Belgin (2008)
O Adwan B Bose (1999)
J Ruis J Planes (1998)
S Yuyama (1995)
P Rao SK Sekar (2011)
OVER 2000REPORTED
SHEAR TESTS IN PAST 60 YEARS
Reference: Collins et all. (2007)
INVESTIGATION OF SHEAR BEHAVIOUR OF SLENDER BEAMS
USING FINITE ELEMENT ANALYSIST H E T H I N G S W E D O F O R Y O U
PROJECT ADVISOR
DR. WASIM KHALIQ
ASSOCIATE PROFESSOR
GROUP MEMBERS
1. USMAN MAHMOOD
2. AAKIF SAEED
3. ASAD ULLAH MALIK
4. FAIZAN HAMEED
Research Scope
Why Finite Element Analysis?
Modelling procedure in ABAQUS®
Benchmark Analysis - Material Calibration
Parametric Analysis
Comparison with ACI predicted Strength
An expression for minimum shear reinforcement
OVERVIEWF I N A L Y E A R P R O J E C T
PROJECT SCOPE
Successfully modelled RC beam in shear and flexure.
Analytically studied different beams with varying
shear reinforcement and shear span ratios which
closely depicts experimental response
Validated modified equation for Ultimate Shear
Strength proposed by Kayani et al. (2014)
Proposing a modified equation for Minimum Shear
Reinforcement
F I N A L Y E A R P R O J E C T
TIME ALLOCATION
F I N A L Y E A R P R O J E C T
LEARNING PHASE
BENCHMARK ANALYSIS
PARAMETRIC ANALYSIS
5%
RESULT EXTRACTION & INTERPRETATION
15%
15%
20%
60%
Pie chart: Percentage time allocated
FINITE ELEMENT MODELLING
Can FEM serve as a replacement for experimental
testing?
Software we used?
ABAQUS 6.13 ®
F I N A L Y E A R P R O J E C T
FOUR POINT BEND TEST
WHY FOUR POINT BEND TEST?
Reference: Collins et all. (2007)
Analysed full scale – 20 beams
Benchmark Analysis - 8 beams
Parametric Analysis - 12 beams
BEAMS ANALYZED
N-SERIES BEAM
Length = 3658 mm ~ 12 ft.
Breath = 254 mm ~ 10 inches
Depth = 457 mm ~ 18 inches
N-Series – Beams without web reinforcement
A-Series- Beams with ACI minimum shear reinforcement
A-SERIES BEAM
Length = 3658 mm ~ 12 ft.
Breath = 254 mm ~ 10 inches
Depth = 457 mm ~ 18 inches
Z-Series- Beams with Zararis minimum shear reinforcement
Z-SERIES BEAM
Length = 3658 mm ~ 12 ft.
Breath = 254 mm ~ 10 inches
Depth = 457 mm ~ 18 inches
M-Series- Beams with minimum shear reinforcement
proposed by Kayani et al.
M-SERIES BEAM
Length = 3658 mm ~ 12 ft.
Breath = 254 mm ~ 10 inches
Depth = 457 mm ~ 18 inches
M’-Series- Beams with minimum shear reinforcement
proposed by Usman et al.
M’-SERIES BEAM
Length = 3658 mm ~ 12 ft.
Breath = 254 mm ~ 10 inches
Depth = 457 mm ~ 18 inches
ABAQUS ®F I N I T E E L E M E N T
M O D E L L I N G S T R A T E G Y
MODELLING GUIDE
MODELLING
x
y
z
XSYMM
𝑈1 = 𝑈𝑅2 = 𝑈𝑅3 = 0
ZSYMM
𝑈3 = 𝑈𝑅1 = 𝑈𝑅2 = 0
*Where 1, 2 and 3 denote the x, y and z axis respectively
USE OF SYMMETRY
MODELLING MESH DENSITY
MODELLING
0
2
4
6
8
10
12
14
16
18
0 5000 10000 15000 20000 25000 30000
Fie
ld O
utp
ut
Vari
ab
le U
2
(mm
)
Element Number
Stable Displacements
after 10,000 elements Element Number as
29,000
MESH DENSITY
Graph: Field Output Variables vs. Element Number
MODELLING SUMMARY MODULE ABAQUS/STANDARD
ANALYSIS TYPE NON-LINEAR STATIC ANALYSIS
SOLUTION TECHNIQUE NEWTON-RAPHSON METHOD
FAMILYBEAM CONTINUUM/SOLID
REINFORCEMENT WIRE/TRUSS
ELEMENT TYPE
BEAM
C3D8R WITH
HOURGLASS
CONTROL
REINFORCEMENT T3D3
LOADING DISPLACEMENT CONTROL
PLA
TE
SR
OLL
ER
SREAL TIME SNAPSHOTS
FULL ASSEMBLY
Beam tested at NICE Same beam modelled in ABAQUS®
SIMULATION
BENCHMARK ANALYSISM A T E R I A L
C A L L I B R A T I O N
ELASTIC PROPERTIES
• Young’s Modulus = 200𝑮𝑷𝒂/29000ksi
• Poisson’s Ration = 0.3
• Type = Isotropic
PLASTIC PROPERTIES
Grade 40 Steel (𝒇𝒚=276 Mpa*)
INPUT MATERIAL PROPERTIES (STEEL)
Grade 60 Steel (𝒇𝒚=414 Mpa*)
0
100
200
300
400
500
600
0 0.01 0.02 0.03 0.04 0.05 0.06
Yie
ld S
tre
ss
(M
Pa)
Plastic Strain*
ELASTIC PROPERTIES
• Young’s Modulus =200 GPa /29000 ksi
• Poisson’s Ration = 0.3
• Type = Isotropic
PLASTIC PROPERTIES
0
100
200
300
400
500
600
700
0 0.01 0.02 0.03 0.04 0.05 0.06
Yie
ld S
tre
ss
(M
Pa)
Plastic Strain*
*Courtesy: Fazal Steel Mills, Industrial Area I-9 , Islamabad
INPUT MATERIAL PROPERTIES (CONCRETE)
Normal Strength Concrete (NSC)
Compressive Strength ( ) = 4000 psi (27.6 MPa)
Density of concrete 𝑤𝑐 = 2300-2500 kg/m3 for NSC
Poisson’s ratio vc = 0.18
Klink (1985)
Young’s Modulus Ec = 26000 MPa
(ACI 8.5.2)
1.5 0.043 'c c c
E w f
5.075.17105.4 ccc fw
BASIC CONCRETE ELASTIC INPUT PROPERTIES
cf
ANALOGY
Tension
Stiffening
Bond Slip
&
Dowel ActionPost Failure Stress–
strain
Response
Vd
F
Inelastic Behavior Of Concrete In
Compression
0
5
10
15
20
25
30
0.000 0.002 0.004 0.006 0.008 0.010
Yie
ldS
tress
(M
Pa
)
Inelastic Strain
0
0.5
1
1.5
2
2.5
3
0 0.001 0.002 0.003
Yie
ld S
tress
(M
Pa)
Cracking Strain
3
( )'
'1 ( )
'
'1.55
4.7
c c
c
c
f
f
f c
Carreira and Chu (1985) Wang and Hsu (1994)
0.4( )cr
t cr
t
f
CONCRETE PLASTIC INPUT PROPERTIES
INPUT MATERIAL PROPERTIES (CONCRETE)
Inelastic Behavior Of Concrete In
Tension
55.14.32
cf
510)16871.0( xfcc
)(4 psiff ccr
el
tt
ck
tcr 0~
ν = 0.005
ν = 0.01
MATERIAL CALLIBRATION
33%24%15%40%18%43% ѱ = 2 5 ° ν = 0.01
ѱ = 31° ν = 0.01
ѱ = 35°
ѱ = 35°
ѱ = 38° ν = 0.01
ѱ = 38° ν = 0.005
PERCENTAGE ERROR
V i sc os i ty Pa r a meter
(ν )
Dilation Angle
(ѱ)
LOA
D C
AR
RYI
NG
CA
PAC
ITY
AN
D
DIS
PLA
CEM
ENT
AT
FAIL
UR
ELO
AD
CA
RR
YING
CA
PAC
ITY AN
D
DISP
LAC
EMEN
T AT FA
ILUR
E“One test on a good sample is better than 10 tests on a poor sample”
J. Michael Duncan
LOAD DEFLECTION CURVES
*Z-series represent beams designed for Zararis minimum reinforcement
Comparison of Experimental and FEM determined Mid Point Deflections for Z1* Beam
Graph: Beam Z1 - Load vs. Deflection at midpoint
0
10
20
30
40
50
60
70
80
0 4 8 12 16 20 24 28 32 36
Lo
ad
(to
n)
Deflection (mm)
Model
Experimental
Linear
Graph: Beam Z1 - Load vs. Deflection at Quarter Point midpointComparison of Experimental and FEM determined Quarter Point
Deflections for Beam Z1*
*Z-series represent beams designed
for Zararis minimum reinforcement
LOAD DEFLECTON CURVES
0
10
20
30
40
50
60
70
0 2 4 6 8 10 12 14 16 18 20 22 24 26 28 30 32 34
Lo
ad
(to
n)
Deflection (mm)
QP1
Model
MID POINT QUARTER POINT
N-Series
A-Series
Z-Series
M-Series
SIMULATION OF BEAM WITHOUT SHEAR REINFORCMENT
NO SHEAR REINFORCEMENT
ACI BEAM ZARARIS’S BEAMMODIFIED
ZARARIS BEAM a
/d=
2.5
a/d
= 3
.0a
/d=
3.5
a/d
= 4
.0
PARAMETRIC ANALYSIST H E C O M P A N Y B A C K G R O U N D SB E A M S W I T H S H E A R
R E I N F O R C E M E N T
PARAMETRIC ANALYSIS
B E A M S W I T H S H E A R R E I N F O R C E M E N T
To analyze the relation between shear span-to-depth
ratio (𝒂/𝒅) and the Ultimate Shear Strength (𝑉𝑢)
Comparison between ACI and Finite Element
Analysis predicted strengths.
Validation of Kayani et al. (2014) Modified
Equation for Ultimate Shear Strength (𝑉𝑢) using
Finite Element Analysis
Proposing a modified equation for Minimum Shear
Reinforcement to attain full flexure capacity
PARAMETRIC ANALYSIS
𝑉𝑢 R E L A T I O N T O 𝑎 / 𝑑
0.9
1
1.1
1.2
1.3
1.4
2 2.5 3 3.5 4 4.5 5
a/d
ACI PREDICTED STRENGTH
TREND LINE
*RSSV = Relative Shear
Strength Value
fail
predicted
V
V
B E A M S W I T H S H E A R R E I N F O R C E M E N T
𝑉𝑢 𝒂/𝒅
PARAMETRIC ANALYSISC O M P A R S I O N O F U L T I M A T E S H E A R
E Q U A T I O N S
ACI CODE
KAYANI et al. (2014)
PARAMETRIC ANALYSISC O M P A R S I O N O F U L T I M A T E S H E A R
E Q U A T I O N S
1.2 0.2 0.21 0.25 du ct v yv
la c aV d f
d d d df bd
Size effect Splitting Tensile Strength
Development Length
Reference - ACI Code 318-11-2, 11-5, 11-15
Reference – Kayani et al Modified Equation (2014)
0.9
1
1.1
1.2
1.3
1.4
2 2.5 3 3.5 4 4.5 5
RS
SV
a/d
ACI PREDICTED STRENGTH
STRENGTH PREDICTED BYMODIFIED EQUATION
PARAMETRIC ANALYSISV A L I D A T I O N O F M O D I F I E D
E Q U A T I O N
G r a p h – C o m p a r i s o n b e t w e e n A C I a n d M o d i f i e d E q u a t i o n p r e d i c t e d s t r e n g t h
PARAMETRIC ANALYSISB E A M S W I T H S H E A R
R E I N F O R C E M E N T
1
11.7
v c
c
y y
yv
f f
ff
a fd
M I N I M U M S H E A R R E I N F O R C E M E N T R A T I O T O A T T A I N F U L L F L E X U R E C A P A C I T Y
PARAMETRIC ANALYSISB E A M S W I T H S H E A R
R E I N F O R C E M E N T
1
11.7
v c
c
y y
yv
f f
ff
a fd
M I N I M U M S H E A R R E I N F O R C E M E N T R A T I O T O A T T A I N F U L L F L E X U R E C A P A C I T Y
(min)
500.75
yv y
c
v
vf f
f
Reference - ACI Code 318 - 11.4.6.3
Longitudinal reinforcement ratio
Shear span to depth ratio
PARAMETRIC ANALYSISB E A M S W I T H S H E A R
R E I N F O R C E M E N T
2.15
2.2
2.25
2.3
2.35
2.4
2.45
2.5
2 2.5 3 3.5 4 4.5
α
a/d
G r a p h – R e l a t i o n b e t w e e n α a n d a / d
𝒂/𝒅 α2.5 2.48
3.0 2.35
3.5 2.27
4.0 2.20
PARAMETRIC ANALYSISB E A M S W I T H S H E A R
R E I N F O R C E M E N T
G r a p h – R e l a t i o n o f % N o m i n a l C a p a c i t y t o T r a n s v e r s e R e i n f o r c e m e n t R a t i o .
0
20
40
60
80
100
120
140
0 0.005 0.01 0.015 0.02 0.025 0.03 0.035 0.04
% N
OM
INA
L FL
EXU
RE
CA
PAC
ITY
TRANSVERSE STEEL RATIO
No Shear Reinforcement
ACI Min Shear Reinforcement
Zararis Min Shear Reinforcement
Kayani Min Shear Reinforcement
Proposed Min Shear Reinforcement
Linear (Nominal Flexure Capacity)
CONCLUSIONSB E A M S W I T H S H E A R
R E I N F O R C E M E N T
Finite Element Modelling (FEM) is a technique
which can be used to better understand shear failure
mechanism.
FEM significantly reduces time and effort in
comparison to experimental testing
The equation devised by Kayani et al. provides a
better shear strength prediction than ACI
The proposed equation provides better prediction for
full flexure capacity of RC beams
THANK YOU!T H E T H I N G S W E D O F O R Y O U