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International INTERNATIONAL Journal of Civil Engineering JOURNAL and OF Technology CIVIL (IJCIET), ENGINEERING ISSN 0976 – AND 
6308 (Print), 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 79-96 © IAEME 
TECHNOLOGY (IJCIET) 
ISSN 0976 – 6308 (Print) 
ISSN 0976 – 6316(Online) 
Volume 5, Issue 11, November (2014), pp. 97-113 
© IAEME: www.iaeme.com/Ijciet.asp 
Journal Impact Factor (2014): 7.9290 (Calculated by GISI) 
www.jifactor.com 
IJCIET 
©IAEME 
ELASTO-PLASTIC BEHAVIOR OF 3-DIMENSIONAL 
REINFORCED CONCRETE ABUTMENTS CONSIDERING 
THE EFFECT OF THE WING WALL 
97 
 
Desy Setyowulan1, Tomohisa Hamamoto2, ToshitakaYamao3 
 
1Graduate School of Science and Technology, Kumamoto University, 2-39-1 Kurokami, 
Kumamoto, 860-8555, Japan 
2Departement of Civil Engineering, Gunma National College of Technology, 580, Tribamachi, 
Maebashi, Gunma 371-8530, Japan 
3Graduate School of Science and Technology, Kumamoto University, 2-39-1 Kurokami, 
Kumamoto, 860-8555, Japan 
 
ABSTRACT 
This study presents the elasto-plastic behavior of 3-dimensional reinforced concrete 
abutments with wing wall as a parametric. To analyze the structure, we used ABAQUS, the finite 
element software, with geometrical modeling of three dimensional solid elements (C3D8R) and two 
dimensional trusses (T3D2) for concrete and reinforcing bar, respectively. Four static horizontal 
loads were applied at half-height of parapet wall with the fixed boundary condition at the footing of 
abutment. Firstly, the analytical and experimental result of reinforced concrete beam was compared 
in this paper in order to check the validity of the numerical analysis. Then, numerical studies were 
carried out in four different abutment modeling approaches including the proposed model of Type 4 
in order to generate an appropriate abutment model. According to the numerical results, it was 
demonstrated that effect of the wing wall in reducing the displacement of the proposed model was 
significant in the wing wall part. Furthermore, cracking and stress distribution in the proposed model 
were also affected by the wing wall. 
Keywords: Reinforced concrete abutment, concrete damaged plasticity, elasto-plastic behavior, 
parapet wall, wing wall
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME 
98 
I. INTRODUCTION 
Reinforced concrete (RC) materials have been widely used as the main constituent material in 
the structural engineering structure, such as in the buildings, bridges, dams, etc. This material has the 
complex behavior which is mainly due to non-linear stress-strain relation of the concrete under 
multi-axial stress conditions, strain softening and anisotropic stiffness reduction, progressive 
cracking caused by tensile stresses, both between concrete and reinforcement, aggregation interlock 
and dowel action of reinforcement, time dependent behavior as creep and shrinkage [1]. 
Consequently, a proper material modelshould be capable to represent the behavior of materials, 
including elastic and elasto-plastic behavior of concrete in tension and compression, within finite 
element packages. 
Recently, many studies have investigated the behavior of concrete using finite element 
analysis. Model verifications of RC beam structures with the damage identification by Concrete 
Damaged Plasticity model in ABAQUS [2] have performed by some researchers. This code has 
shown the adequate reliability and accuracy to perform nonlinear behavior of RC structure in 
comparison with the experimental results [3-5]. 
In structural engineering, abutment refers to the end support of the bridge superstructure. It 
plays an important role on the performance of bridge, such as transferring load from superstructure 
to its foundation, resisting and/or transferring self-weight and lateral loads from earth pressure and 
wind loads, also supporting one end of an approach slab. Its behavior has been found to significantly 
influence the response of an entire bridge system under strong intensity dynamic excitation [6].On 
many bridges, abutment damage was the only damage reported indicating that it attracted a large 
portion of seismic force [7]. 
The parapets and wing walls of abutment are designed based on the Japan Specification for 
Highway Bridges, Part IV Substructures [8]. In earthquake prone area, the unseating prevention 
structures (UPS) are needed to be installed in the bridge structure in order to prevent unseating of the 
superstructure against unforeseen conditions such as unexpected seismic force, destruction of the 
surrounding ground, or unexpectedly complicated vibrations in the structural members. However, 
falling of the superstructure may lead by the breakage of the parapet when UPS are installed to the 
parapet. 
Previous study [9] has carried out an investigation on the elastic behavior of parapet 
considering to the wing wall. In comparison with the plate structure fixed three sides, it is found that 
the bending moment and shear force at the base of the parapet wall decrease and elastic deformation 
behavior is similar. In addition, an investigation on elastic and elasto-plastic behavior of the parapet-unified 
wing walls of abutment subjected to horizontal loads through unseating prevention structure 
of bridge has been conducted by another researcher [10]. From this study, it has been recognized that 
the effect of the wing walls on the behavior and bending moment at base of the parapet is very large. 
In past large earthquake, many abutments collapsed due to strong intensity of dynamic excitation. 
The collapsed mainly due to high stress as the most common problems observed during the 
inspection of the abutment failure. Therefore, it is needed to analyze the new type of abutment as the 
proposed model in order to generate an appropriate abutment model. This study is focused on 
determination of the elasto-plastic behavior of 3-D reinforced concrete abutments considering to the 
effect of the wing wall. The finite element software of ABAQUS with the Concrete Damaged 
Plasticity method was used as the finite element analysis method. In verification method, modeling 
technique of reinforced concrete beamwas verified by comparing the model prediction of RC beam 
to the experimental work in the previous research [10]. Then, numerical studies were carried out in 
four different abutment modeling approaches including a proposed model of abutment, subjected to 
horizontal loads through the unseating prevention structures. The results were used to predict the 
effect of the wing wall in the behavior of abutment.
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME 
pl 
e t e~ and ~ , respectively. 
ck 
t e~ = e −e (1) 
99 
II. NUMERICAL PROCEDURES 
 
2.1 Finite element modeling 
Numerical modeling of reinforced concrete beam and abutments were performed using 
ABAQUS [2] software. The concrete beam was idealized by homogenous material and modeled with 
eight-node solid (brick) elements, identified as C3D8R elements. Furthermore, the reinforcing bar 
was idealized by three dimensional truss elements called T3D2. 
2.2 Constitutive model of steel reinforcing bar (rebar) 
The constitutive model for steel rebar has approximately linear elastic behavior when the 
stiffness is governed by the Young’s modulus at low strain magnitudes. At higher strain magnitudes, 
it begins to behave nonlinear, inelastic behavior, which is referred to as plasticity [3]. The plastic 
behavior is described by its yield point and post-yield hardening, with the shift from elastic to plastic 
behaviors occurs at a yield point on a material stress-strain curve. Once the stress in rebarexceeds the 
yield stress, permanent (plastic) deformation begins with decreasing of the stiffness. The plastic 
deformation of this material increases its yield stress for subsequent loadings. 
2.3 Constitutive model of concrete 
In ABAQUS [2], there are three methods to simulate the damage criterion in reinforced 
concrete elements, including brittle crack concrete model, smeared crack concrete model and 
concrete damaged plasticity model (CDP). The CDP method allows in defining the complete 
inelastic behavior of concrete under tension and compression including the damage parameters. It 
provides a general capability for modeling concrete and other quasi-brittle materials in all types of 
structures (beams, trusses, shells, and solids), so it can be used with rebar to model concrete 
reinforcement.In the mechanical behavior of CDP, tensile cracking and compressive crushing are 
assumed to be the main failure mechanisms of concrete. Failure of the yield surface is controlled by 
tensile and compressive equivalent plastic strains, pl 
c 
The concrete behavior is considered independently with rebar. Effect of the bond slip and 
dowel action are modeled by introducing some “tension stiffening”, as shown in Fig. 1(a), in order to 
simulate load transfer across cracks through the rebar and to define cracking and post cracking 
properties for the concrete.The stress-strain response under uniaxial tension follows a linear elastic 
relationship up to the failure stress, t0 s , corresponds to the onset of micro-cracking in the concrete 
material. The compressive equivalent cracking strain and plastic strain values, pl 
e~ ck 
and e~ , are 
t t 
defined by (1) and (2), respectively. 
el 
t ot 
d s 
pl 
t d E 
( ) 
(2) 
1 
~ ~ 
t 
o 
t 
ck t 
t 
e e 
− 
= − 
where: t e : total tensile strain 
e el 
: The elastic tensile strain corresponding to the undamaged material, e el 
=s E 
ot ot t o 
Eo : Young’s modulus 
t s 
: tensile stress 
dt : tension damage parameter 
The compressive behavior of plain concrete under uniaxial compression outside the elastic 
range can be defined, as shown in Fig. 1(b). The stress-strain response under uniaxial compression is
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
– 6308 (Print), 
pp. 97-113 © IAEME 
 
linear up to the initial yield, s . The response in plastic regime is characterized by stress hardening 
c0 followed by strain softening ing beyond the ultimate stress, 
s . The inelastic (or crushing) strain and 
cu plastic strain values, pl 
e~ in 
and e~ , are defined by (3) and (4), respectively. 
c c 
of the elastic modulus in compressive and tensile behavior, 
respectively. 
in 
c e~ =e −e 
el 
c oc 
d s 
pl 
c d E 
= − 
( ) c c o E = 1− d E 
(1 ) 
~ ~ 
c 
o 
c 
in c 
c 
e e 
− 
( ) t t o E = 1− d E 
where: c e : total compressive strain 
el 
oc e : The elastic tensile strain corresponding to the 
c s : Compressive stress 
dc : compression damage parameter 
(a) Tension behavior associated with 
tension stiffening 
Figure 1. 
(a) Compressive stress-strain relationship [ 
, in (5) and (6), 
Figure 2. Numerical properties of RC structure 
100 
In addition, the reduction 
Ec and Et, are given 
(3) 
(4) 
(5) 
(6) 
undamaged material, 
el 
oc e =s E 
t o 
(b) Compression behavior associated 
with compression hardening 
Concrete damaged plasticity model [2] 
11] (b) Modified tension stiffening model [ 
5]
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
In this analysis, modeling of the 
compressive stress-strain curve was d 
developed based on the 
normal strength concrete with s 
value, c s , between the yield point at 
previous research [11], which can be used for 
shown in Fig. 2(a). The compressive stress value 
0.3s cu in the descending portion is calculated by ( 
for the concreteis shown in Fig.2(b). 
through the rebar and to define cracking and post cracking prope 
– 6308 (Print), 
pp. 97-113 © IAEME 
 
cu less than 62 MPa, as 
cu 0.5s and the 
7). Furthermore, modified tension stiffening 
model 
It is introduced in order to simulate load transfer across cracks 
rties The equations, 
c cu o s ,s and E are in kip/in2 with the conversion factor of 1MPa = 0.145 kip/in 
 
( ) 
( ) cu 
b e e 
 
s b   
c o 
c s 
b e e 
c o 
 
  
 
− + 
= 
1 
[ ( )] cu o o s e E 
b 
− 
= 
1 
1 
5 3 8.9 10 2.114 10− − = x + x o cu e s 
2 3 E 1.243 x10 3.283 x10 o cu = s + 
2.4 Numerical modeling of reinforced concrete 
2. 
) 
In order to ensure the validity of the numerical analysis, a model comparison to actual 
behavior was performed. A simple model of RC beam structure shown in 
including its material properties [1 
b of 100 mm, the height h of 400 mm, 
230 mm from the beam ends.The shear span ratio ( 
respectively. Other structural properties were shown in Table 1. It was subjected to two identical 
point loads and applied symmetrically on the rigid plates. Moreover, the stress 
the concrete and rebar are shown in 
was measured by means of LVDTs. 
Figure 3. Position of the tested RC beam [1 
Fig. 3was chosen, 
with the width 
was were 0.5 and 320 mm, 
stress-strain relationship of 
mid-span 
440 
30 
100 
According to the experimental test setup data, RC beam was then simulated in X 
X-Y-Z 
coordinate system with a half-length by symmetry condition, as shown in Fig.5. X, Y, and Z axes 
were parallel to the longitudinal, depth and width of beam. The compressive strength of the 
were 27.214 MPa (taken as yielding strength 
The density, Young modulus Eo 
kg/m3, 33342.61 MPa, 3.315 MPa, and 0.167. In addition, rebar was assumed as steel material with 
the density of 7850 kg/m3, yield stress 
) fcu). 
101 
properties for the concrete. 
(7) 
(8) 
(9) 
(10) 
(RC) beam structure 
10]. As shown in this set-up, a rectangular RC beam 
900 mm long Lwas positioned horizontally and supported at 
a/d) and the depth d wer 
Fig. 4(a) and Fig. 4(b), respectively.The deflection at mid 
10] 
Table 1. Structural properties of RC 
beam 
Descriptions Dimensions (mm) 
l 
t 
r 
e concrete 
fco) and 54.427 MPa (taken as ultimate strength 
o, tensile stress t0 s , and Poisson’s ratio c u of concrete were 2400 
fyof 375.3 MPa, Young modulus Es of 205939.65 MPa, and
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
Poisson’s ratio s u of 0.3. The damaged variables, 
Fig.6(a) and Fig.6(b). 
(a) Stress-strain curve for concrete 
Figure 
4. Model input of RC beam 
(a) Applied load and boundary condition 
Figure 
(a) Tension damage 
Figure 
pp. 97-113 © IAEME 
dt and dc, are defined based on plot presented in 
(b) Stress-strain curve for steel rebar [10 
102 
(b) Solid element (c) Rebar element 
5. Model of RC beam in ABAQUS 
(b) Compression damage 
6. Damage variables of the concrete 
– 6308 (Print), 
 
10]
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
2.5 Numerical modeling of reinforced concrete abutments 
According to Japan Specifications for 
Highway Bridges, Part IV (Substructures) [ 
three different types of the wing wall shapes. The shapes and dimensions vary according to the 
installation site of the abutment, backfill height, and gradient of the slope. The numerical model of 
RC abutment Type 2 as the typical model of abutment in Japan is representative for actual model, as 
shown in Fig.7. In order to increase the strength of abutment, abutment Type 4 was analyzed as a 
proposed model to be developed from Type 1 (without wing wall 
Moreover, based on this specification, the wall of a T 
cantilever with the fixed end at the node connected to the top of the footing. Therefore, in order to 
reduce the number of nodes and elements in the modeling, it needs to simplify the model by omitting 
the footing of abutment and modeling support with fixed boundary condition. Summary of the 
comparison results in Type 1, with and without footing are described in Table 
recognized that the analytical method of RC 
behavior of abutment with footing. 
(a) Numerical model 
Figure 7. Model of abutment Type 2 as the typical model in Japan 
Table 2. Summary of the maximum result in each model 
Descriptions 
S11 
S33 
PE11 
AC Yield 
dt 
pp. 97-113 © IAEME 
103 
. wall) and Type 3 (full wing wall). 
T-shaped abutment can be designed as a 
abutment without footing is able 
(b) Real bridge 
. Type 1 
(with footing) 
Type 1 
(without footing) 
1.591 e+8 1.592 e+8 
2.493 e+6 2.507 e+6 
2.955 e-4 2.956e-4 
Similar value and position 
Similar value and position 
– 6308 (Print), 
 
ges, 8], there are 
) 2 and Fig.8. It was 
to represent the 
Diffe-rences 
0.06% 
0.56% 
1.30%
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
pp. 97-113 © IAEME 
Figure 8. Load vs displacement 
Four different abutment modeling approach were carried out with a half 
symmetry condition, as shown in Fig.9. The dimensional configurations are depicted in Fig. 
Table 3, respectively, with parameter of 
Furthermore, the rebar arrangement is given in Fig. 11. 
(a) Type 1 (b) Type 2 
Fig 
t represents the thickness of parapet wall and wing wall. 
Figure 10. Dimensional configurations of abutments (unit: 
104 
(c) Type 3 
Figure9. Numerical models of abutments 
. – 6308 (Print), 
 
half-length model by 
10 and 
(d) Type 4 
m)
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
Table 3.Dimensional configurations of four abutments 
Descrip 
tions 
Type 1 
(m) 
Type 2 
(m) 
Type 3 
(m) 
b2 - - 
h3 - 1.0 8.0 
h4 - 3.3 0.0 
h5 5.5 5.5 5.5 
h6 - - 
t 0.5 0.5 0.5 
Figure 11. Rebar arrangement of Type 4 
pp. 97-113 © IAEME 
Figure 12. Stress-strain curve for concrete 
. Figure 13. Side view of abutment [1 
Material property of the concrete was assumed from previous research [1 
12, while for the rebar was similar with RC beam input. The compressive strengths were 13.75 MPa 
(taken as yielding strength fco) and 27.5 MPa (taken as ultimate strengt 
modulus Eo,tensile stress t0 s , and Poisson’s ratio 
MPa, and 0.2. 
2.6 Loading conditions 
There are two types of loading condition for RC beam and 
weight as a gravity load g of 9.8 
amplified under force control. Design seismic force of the unseating prevention structure 
be taken as 1.5 times dead load 
abutment with full wing wall and applied the unseating prevention structure (UPS), as shown in 
13. In this research, four static horizontal loads through UPS were applied in the half 
parapet wall, with the dead load reaction of the superstructure was 2900 kN, obtained from the deck 
weight. Therefore, each UPS will transfer the external load to the parapet wall of 543.75 kN. 
HF = 1.5 RD 
105 
ial ) strength fcu 
c u of concrete were 2400 kg/m 
RC abutments, including the self 
m/s2 and the external load. The external load in RC beam was 
reaction, RD [13]. Previous research [14] developed a model of 
. Type 4 
(m) 
- 0.5 
8.0 
0.0 
1 
- 1 
0.5 
– 6308 (Print), 
 
14] 
12], as shown in Fig. 
cu). The density, Young 
3,25000 MPa, 2.75 
self-external 
structure, HF, may 
] Fig. 
half-height of 
(11)
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
2.7 Interaction Properties 
– 6308 (Print), 
 
General contact surface algorithm was considered to determine the modeling of contact 
behavior in the interacting surfaces between concrete and steel plate in RC beam. The friction 
coefficients of contact point was 
analysis, the steel plate was used in order to transfer the external load to RC beam and to set down 
the support. The embedment was defined using an embedded constraint and was achieved by 
constraining rebar elements into solid element 
2.8 Boundary conditions 
, The RC beam and abutments were modeled as a half 
conditions in support were hinged 
RC beam was constrained with boundary condition in X 
in the mid-span of RC abutments was constrained in Z direction 
III. RESULTS AND DISCUSSIONS 
3.1 Analysis of RC beam structure 
The load-displacement curves for experime 
ntal are shown in Fig. 14. The displacement 
mid-span of RC beam structure and 
From this figure, it can be seen that the 
data up to 40 tf. Moreover, the maximum load 
48.54 tf, which is slightly larger than experimental result of 45 tf. 
pressure-over closure. In this 
, In order to visualize the cracking distribution within the FEM, the positive plastic strain can 
be mapped with color coded contours shown in 
flexural cracks initiate first in the mid 
The maximum plastic strain occurs in the “red” regions where the plastic strain equals 0.00255 
corresponds to the maximum tension damage parameter of approximately 0.9. Dark blue regions 
correspond to areas of no tension damage. According to the analysis, it could be concluded that the 
cracking distribution of RC beam is more localized within the support and mid 
Figure 14. Vertical load vs displacement curves Figure 1 
pp. 97-113 © IAEME 
106 
ral set to be 0.1 and hard contact for pressure 
element, in order to create a proper bond action. 
half-length model with the boundary 
and fixed, respectively. The surface of YZ in the middle length of 
s X-direction (U1=0), whether the surface of XY 
(U3=0). 
experimental result and numerical analysis by ABAQUS 
displacementand load shown correspond to the vertical displacement at 
the total vertical force imposed on the structure, respectively. 
, numerical resultcorrelate well with those from experimental 
aximum to be transmitted in RC beam by numerical analysis 
Fig. 15. The beam exhibit flexure 
mid-span of structure, followed by inclined flexure 
. 15. FEM magnitude of plastic strain 
is 
. flexure-shear failure where 
flexure-shear cracks. 
mid-span of the beam. 
agnitude
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
Load = 22 tf 
U2 = 0.229 mm 
(a) 
pp. 97-113 © IAEME 
Analysis (b) Experiment 
Figure 16. RC beam cracking pattern with the external load of 20 tf 
The comparison between analytical and experimental results of this behavior due to external 
load of 20 tf is shown in Fig. 16. “L 
correspond to the cracking of the concrete. Due to an automatic step increment in analysis, the result 
is figured out at load of 22 tf. It indicates that the cracking distributions in analytical 
good agreement with those from experimental results. 
3.2 Analysis of RC abutments 
3.2.1 Longitudinal displacement 
The longitudinal displacements of abutmentswere investigated in the wing wall part and half 
part of abutment, three levels in each side 
longitudinal displacement of the wing wall part 
parapet and bottom of abutment, respectively. Otherwise, in 
UB2, and U2. 
Figure 1 
(a) Middle part 
Figure 18. Longitudinal displacement of abutment (mm) 
107 
. Light blue and deep colors” regions with positive plastic strain 
butments 
isplacement 
side, as shown in Fig. 17. UT1, UB1 
in different level positions, top 
, the middle part are depi 
17. Position of the nodal displacement 
(b) Wing wall part 
. Wing wall Middle part 
part 
– 6308 (Print), 
 
ht study are in a 
half-length 
and U1 represent the 
of parapet, bottom of 
depicted as UT2,
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
Total static horizontal load which can be expected to be 
– 6308 (Print), 
pp. 97-113 © IAEME 
 
prevention structures for half-length model was 2175 kN. Applying external load affect the 
longitudinal displacement of each abutment, are depicted in Fig. 18(a) and Fig. 18(b) as 
displacement in the middle and wing wall p 
art, wall part UT1 of 10.64 mm, 3.16 mm, 0.59 mm, and 0.36 mm for abutment Type 1, Type 2, Type 4, 
and Type 3, respectively. It signifies in reducing of 59.20%, 94.33% and 92.06% for abutment Type 
2, Type 3 and Type 4, respectively. These results prove that installation of the wing wall in abutment 
have a capability in decreasing of the longitudinal displacement. 
In addition, a static pushover analysis was carried out with the external load amplification i 
order to characterize the maximum load to be transmitted in abutment. The result of load versus 
displacement curve is shown in Fig. 19. The study reported that the maximum load for abutment 
Type 1 is the smallest one of 2792.25 kN. Type 3 and Type 4 have 
which are smaller than Type 2 of 3244.43 kN. This condition is possibly due to design of the wing 
walls in Type 4 as slabs fixed on two sides to a wall and footing, which can reduce the longitudinal 
displacement and flexibility of the structure. Consequently, it leads crack at the parapet wall. 
(a) 
Figure 19. Longitudinal displacement of abutment (mm) 
3.2.2 Cracking Distribution of RC Abutments 
(a) Initial cracking 
Figure 20. Contour plot of tensile damage in RC abutment Type 
108 
transmitted through the unseating 
part, respectively. Interesting results occur in the wing 
similar value of 3009.27 kN, 
y Middle part (b) Wing wall part 
. at 1093.11 kN (b) Final cracking at 2792.25 kN 
. 1 at different external load 
in
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
(a) Initial cracking at 1093.11 kN 
pp. 97-113 © IAEME 
Figure 21. Contour plot of tensile damage in RC abutment Type 2 at different 
(a) Initial cracking at 1093.11 kN 
Figure 22. Contour plot of tensile damage in RC abutment Type 3 at different external load 
(a) Initial cracking at 1093.11 kN 
Figure 23. Contour plot of tensile damage in RC abutment Type 4 at different external load 
109 
(b) Final cracking at 3244.43 kN 
(b) Final cracking at 3009.27 kN 
(b) Final cracking at 3009.27 kN 
our – 6308 (Print), 
 
external load
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
pp. 97-113 © IAEME 
Figs.20-23 show contour plot of output variable DAMAGET, which is a scalar degradation 
measure used to express the reduced tensile elastic modulus of concrete after it has sustaine 
cracking damage. Sequence of the concrete cracking are described as initial and final cracking, as 
shown in section (a) and (b), respectively. “Dark blue” regions correspond to areas of no tension 
damage or no cracking. The maximum tension damage occurs 
strain equals 0.00264 corresponds to the maximum tension damage parameter of approximately 0.9. 
From these figures, it can be discovered that the initial cracking of all abutments occur in two 
different positions, in peripheral of the external load and intersection between parapet wall and 
abutment wall due the external load of 1093.11 kN. In addition, cracking is also found at bottom of 
abutment wall near the footing for Type 1 and Type 2. Type 1 is found as a structur 
critical damage due to the cracking propagation in region through its width. Moreover, it propagates 
from the middle width to the edge position, lead the connection part between wing wall and parapet 
wall to crack. 
3.2.3 Load-tensile strain plot for reinforcing bar 
Fig. 24(a) shows the maximum tensile stress versus tensile strain relationship of the rebar, 
located at the reverse side of parapet wall. According to this figure, it can be seen that the tensile 
steel rebar is not yield at failure in abutment with all types of the wing wall. Otherwise, yielding 
occurs at Type 1. Furthermore, the relationship between load and maximum tensile strain in the rebar 
is depicted in Fig. 24(b). From these results, it is recognized that installation of t 
increases the stiffness of abutment, resulting on strain reduction in the rebar. 
(a) Stress- 
Figure 2 
3.2.4 Shear stress distribution of RC abutments 
Stress distribution is one of the important aspects to be evaluated in abutment. The areas 
subjected to high stress is the most common problems observed during the inspection of the failure 
of abutment in the past large earthquake. 
are studied in numerical analysis 
these figure, it can be determined that 
wallnearly the intersection with the wi 
110 
in “red” regions, where the cracking 
eripheral in ure -strain ratio (b) Load versus tensile strain 
24. Tensile strain plot for the rebar 
ribution Shear stress distributions around vertical wall of abutments 
analysis, with the results for each abutment are shown in 
maximum shear stresses occur at the region of parapet 
wing wall. 
– 6308 (Print), 
 
sustained 
structure with the most 
the wing wall 
ertical Fig. 25. From
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 
(a) Type 1 
(c) Type 3 
Figure 2 
IV. CONCLUSIONS 
The elasto-plastic behavior of 3 
– 6308 (Print), 
pp. 97-113 © IAEME 
 
effect of the wing wall were investigated in this study 
different abutment modeling approaches subjected to static 
prevention structure with consideration of the wing wall. The conclusions are summari 
following. 
1) The analytical method of Concrete Damaged Plasticity by 
the elasto-plastic behavior of RC structure. The material modeling was 
experimental results in showing the behavior of RC beam in 
cracking distribution. 
2) Installation of the wing wall in abutments ha 
summarized as 
said to be valid as 
displacement and 
displacement of 59.20%, 94.33% and 92.06% for abutment Type 2, Type 3 and Type 4 
proposed type, respectively. 
in abutment. Otherwise, there was no significant 
111 
(b) Type 2 
(d) Type 4 
25. Shear stress distribution of abutments 
3-dimensional reinforced concrete abutments considering the 
e study. Numerical studies were carried out in four 
horizontal loads through the unseating 
ABAQUS was capable to analyze 
case of 
had a capability in decreasing of the longitudinal 
9.20%, ely. This condition was affected by the increasing number of stiffness 
effect in half-length part of abutment. 
as the
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME 
3) According to the static pushover analysis, the maximum load that could be expected to be 
transmitted for the proposed type of abutment of 3009.27 kN was smaller than Type 2 of 
3244.43 kN.It was possibly due to design of the wing walls in Type 4 as slabs fixed on two 
sides to a wall and footing, which reduced the longitudinal displacement and flexibility of the 
structure. 
4) The initial cracking for all abutments occurred in two different positions, at the peripheral of 
the external load and intersection between parapet wall and abutment wall. Installation of the 
wing wall in the proposed model reduced the cracking at the bottom of wall and compressive 
strain of the concrete. 
5) The stress distribution was affected by the wing wall. From numerical analysis, it was 
depicted that the maximum shear stress occurred at the region of parapet wall nearly the 
intersection of the wing wall. Furthermore, the tensile steel of the rebar was not yielded at 
failure in abutments with the wing wall which was affected by the reduction of the axial 
strain. 
6) Although the present study found better evidence on the proposed model of abutment Type 4 
in its behavior, no earth pressure was applied. Therefore, further studies are necessary in 
order to determine the behavior of RC abutment under earth pressure and strong ground 
excitation. 
112 
ACKNOWLEDGEMENT 
The first author acknowledges DIKTI (Directorate General of Higher Education) as the 
financial supporter of the scholarship and University of Brawijaya as the home university. The 
support in completing the doctoral study in Kumamoto University is gratefully appreciated. 
REFERENCES 
[1] M. Nz M. Nazem, I. Rahimani and M. rezaee-Pajand, Nonlinear FE analysis of reinforced 
concrete structures using a tresca-type yield surface, ScienticaIranica, 16 (6), 2009, 512-519. 
[2] Dassault Systems Simulia Corp., ABAQUS/CAE User’s Manual 6.11, Providence, RI, USA, 
2011. 
[3] A. Ahmed, Modeling of a reinforced concrete beam subjected to impact vibration using 
ABAQUS, International Journal of Civil and Structural Engineering, 4 (3), 2014, 227-236. 
[4] A.R. Mohamed, M.S. Shoukryand J.M. Saeed, Prediction of the behavior of reinforced 
concrete deep beams with web openings using the finite element method, Alexandria 
Engineering Journal, 53, 2014, 329–339. 
[5] B.L. Wahalathantri,Damage assessment in reinforced concrete flexural members using modal 
strain energy based method, Doctoral diss., Queensland University of Technology, 2012. 
[6] A. Aviram, K.R. Mackie and B. Stojadinovic,Effect of abutment modeling on the seismic 
response of bridge structures, Earth EngEngVib, 7 (4), 2008, 395-402. 
[7] M.J. Karantzikis, C.C. Spyrakos, Seismic analysis of bridges including soil-abutment 
interaction, 12 World Conference on Earthquake Engineering, 2000. 
[8] Japan Road Association, Specifications for Highway Bridges Part IV: Substructures, 2002. 
[9] A. Kawachi, Investigation of the effect of wing walls on the elastic behavior of the parapet on 
the abutment, Thesis, Kumamoto University, Japan, 2007. 
[10] T. Yamao, A. Kawachiand M. Tsutsui, Static and dynamic behaviour of a parapet wall of the 
abutment, 11th International Conference on Steel, Space and Composite Structures, 2012. 
[11] L.S. Hsu and C.T.T. Hsu, Stress-strain behavior of steel-fiber high-strength concrete under 
compression, ACI structural journal, 91 (4), 1991, 448-457.
International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), 
ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME 
[12] D. Setyowulan, T. Hamamoto and T. Yamao, Eigenvalue analysis and characteristic 
behaviour of reinforced concrete abutments, 39th Conference on Our World in Concrete  
Structures, Singapore, 2014. 
[13] Japan Road Association, Specifications for Highway Bridges Part V: Seismic Design, 2002. 
[14] A. Kawachi, Proposal of the simple design method and the seismic behavior of the parapet of 
113 
abutment, Master thesis, 2009. 
[15] Yaman S.S. Al-Kamaki, Riadh Al-Mahaidi and Azad A. Mohammed, “Behavior of Concrete 
Damaged by High Temperature Exposureand Confined With CFRP Fabrics” International 
Journal of Civil Engineering  Technology (IJCIET), Volume 5, Issue 8, 2014, pp. 148 - 
162, ISSN Print: 0976 – 6308, ISSN Online: 0976 – 6316. 
[16] Prerna Nautiyal, Saurabh Singh and Geeta Batham, “A Comparative Study of The Effect of 
Infill Walls on Seismic Performance of Reinforced Concrete Buildings” International Journal 
of Civil Engineering  Technology (IJCIET), Volume 4, Issue 4, 2013, pp. 208 - 218, ISSN 
Print: 0976 – 6308, ISSN Online: 0976 – 6316.

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Elasto plastic behavior of 3 dimensional reinforced concrete abutments considering the effect of the wing wall

  • 1. International INTERNATIONAL Journal of Civil Engineering JOURNAL and OF Technology CIVIL (IJCIET), ENGINEERING ISSN 0976 – AND 6308 (Print), ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 79-96 © IAEME TECHNOLOGY (IJCIET) ISSN 0976 – 6308 (Print) ISSN 0976 – 6316(Online) Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME: www.iaeme.com/Ijciet.asp Journal Impact Factor (2014): 7.9290 (Calculated by GISI) www.jifactor.com IJCIET ©IAEME ELASTO-PLASTIC BEHAVIOR OF 3-DIMENSIONAL REINFORCED CONCRETE ABUTMENTS CONSIDERING THE EFFECT OF THE WING WALL 97 Desy Setyowulan1, Tomohisa Hamamoto2, ToshitakaYamao3 1Graduate School of Science and Technology, Kumamoto University, 2-39-1 Kurokami, Kumamoto, 860-8555, Japan 2Departement of Civil Engineering, Gunma National College of Technology, 580, Tribamachi, Maebashi, Gunma 371-8530, Japan 3Graduate School of Science and Technology, Kumamoto University, 2-39-1 Kurokami, Kumamoto, 860-8555, Japan ABSTRACT This study presents the elasto-plastic behavior of 3-dimensional reinforced concrete abutments with wing wall as a parametric. To analyze the structure, we used ABAQUS, the finite element software, with geometrical modeling of three dimensional solid elements (C3D8R) and two dimensional trusses (T3D2) for concrete and reinforcing bar, respectively. Four static horizontal loads were applied at half-height of parapet wall with the fixed boundary condition at the footing of abutment. Firstly, the analytical and experimental result of reinforced concrete beam was compared in this paper in order to check the validity of the numerical analysis. Then, numerical studies were carried out in four different abutment modeling approaches including the proposed model of Type 4 in order to generate an appropriate abutment model. According to the numerical results, it was demonstrated that effect of the wing wall in reducing the displacement of the proposed model was significant in the wing wall part. Furthermore, cracking and stress distribution in the proposed model were also affected by the wing wall. Keywords: Reinforced concrete abutment, concrete damaged plasticity, elasto-plastic behavior, parapet wall, wing wall
  • 2. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME 98 I. INTRODUCTION Reinforced concrete (RC) materials have been widely used as the main constituent material in the structural engineering structure, such as in the buildings, bridges, dams, etc. This material has the complex behavior which is mainly due to non-linear stress-strain relation of the concrete under multi-axial stress conditions, strain softening and anisotropic stiffness reduction, progressive cracking caused by tensile stresses, both between concrete and reinforcement, aggregation interlock and dowel action of reinforcement, time dependent behavior as creep and shrinkage [1]. Consequently, a proper material modelshould be capable to represent the behavior of materials, including elastic and elasto-plastic behavior of concrete in tension and compression, within finite element packages. Recently, many studies have investigated the behavior of concrete using finite element analysis. Model verifications of RC beam structures with the damage identification by Concrete Damaged Plasticity model in ABAQUS [2] have performed by some researchers. This code has shown the adequate reliability and accuracy to perform nonlinear behavior of RC structure in comparison with the experimental results [3-5]. In structural engineering, abutment refers to the end support of the bridge superstructure. It plays an important role on the performance of bridge, such as transferring load from superstructure to its foundation, resisting and/or transferring self-weight and lateral loads from earth pressure and wind loads, also supporting one end of an approach slab. Its behavior has been found to significantly influence the response of an entire bridge system under strong intensity dynamic excitation [6].On many bridges, abutment damage was the only damage reported indicating that it attracted a large portion of seismic force [7]. The parapets and wing walls of abutment are designed based on the Japan Specification for Highway Bridges, Part IV Substructures [8]. In earthquake prone area, the unseating prevention structures (UPS) are needed to be installed in the bridge structure in order to prevent unseating of the superstructure against unforeseen conditions such as unexpected seismic force, destruction of the surrounding ground, or unexpectedly complicated vibrations in the structural members. However, falling of the superstructure may lead by the breakage of the parapet when UPS are installed to the parapet. Previous study [9] has carried out an investigation on the elastic behavior of parapet considering to the wing wall. In comparison with the plate structure fixed three sides, it is found that the bending moment and shear force at the base of the parapet wall decrease and elastic deformation behavior is similar. In addition, an investigation on elastic and elasto-plastic behavior of the parapet-unified wing walls of abutment subjected to horizontal loads through unseating prevention structure of bridge has been conducted by another researcher [10]. From this study, it has been recognized that the effect of the wing walls on the behavior and bending moment at base of the parapet is very large. In past large earthquake, many abutments collapsed due to strong intensity of dynamic excitation. The collapsed mainly due to high stress as the most common problems observed during the inspection of the abutment failure. Therefore, it is needed to analyze the new type of abutment as the proposed model in order to generate an appropriate abutment model. This study is focused on determination of the elasto-plastic behavior of 3-D reinforced concrete abutments considering to the effect of the wing wall. The finite element software of ABAQUS with the Concrete Damaged Plasticity method was used as the finite element analysis method. In verification method, modeling technique of reinforced concrete beamwas verified by comparing the model prediction of RC beam to the experimental work in the previous research [10]. Then, numerical studies were carried out in four different abutment modeling approaches including a proposed model of abutment, subjected to horizontal loads through the unseating prevention structures. The results were used to predict the effect of the wing wall in the behavior of abutment.
  • 3. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME pl e t e~ and ~ , respectively. ck t e~ = e −e (1) 99 II. NUMERICAL PROCEDURES 2.1 Finite element modeling Numerical modeling of reinforced concrete beam and abutments were performed using ABAQUS [2] software. The concrete beam was idealized by homogenous material and modeled with eight-node solid (brick) elements, identified as C3D8R elements. Furthermore, the reinforcing bar was idealized by three dimensional truss elements called T3D2. 2.2 Constitutive model of steel reinforcing bar (rebar) The constitutive model for steel rebar has approximately linear elastic behavior when the stiffness is governed by the Young’s modulus at low strain magnitudes. At higher strain magnitudes, it begins to behave nonlinear, inelastic behavior, which is referred to as plasticity [3]. The plastic behavior is described by its yield point and post-yield hardening, with the shift from elastic to plastic behaviors occurs at a yield point on a material stress-strain curve. Once the stress in rebarexceeds the yield stress, permanent (plastic) deformation begins with decreasing of the stiffness. The plastic deformation of this material increases its yield stress for subsequent loadings. 2.3 Constitutive model of concrete In ABAQUS [2], there are three methods to simulate the damage criterion in reinforced concrete elements, including brittle crack concrete model, smeared crack concrete model and concrete damaged plasticity model (CDP). The CDP method allows in defining the complete inelastic behavior of concrete under tension and compression including the damage parameters. It provides a general capability for modeling concrete and other quasi-brittle materials in all types of structures (beams, trusses, shells, and solids), so it can be used with rebar to model concrete reinforcement.In the mechanical behavior of CDP, tensile cracking and compressive crushing are assumed to be the main failure mechanisms of concrete. Failure of the yield surface is controlled by tensile and compressive equivalent plastic strains, pl c The concrete behavior is considered independently with rebar. Effect of the bond slip and dowel action are modeled by introducing some “tension stiffening”, as shown in Fig. 1(a), in order to simulate load transfer across cracks through the rebar and to define cracking and post cracking properties for the concrete.The stress-strain response under uniaxial tension follows a linear elastic relationship up to the failure stress, t0 s , corresponds to the onset of micro-cracking in the concrete material. The compressive equivalent cracking strain and plastic strain values, pl e~ ck and e~ , are t t defined by (1) and (2), respectively. el t ot d s pl t d E ( ) (2) 1 ~ ~ t o t ck t t e e − = − where: t e : total tensile strain e el : The elastic tensile strain corresponding to the undamaged material, e el =s E ot ot t o Eo : Young’s modulus t s : tensile stress dt : tension damage parameter The compressive behavior of plain concrete under uniaxial compression outside the elastic range can be defined, as shown in Fig. 1(b). The stress-strain response under uniaxial compression is
  • 4. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), – 6308 (Print), pp. 97-113 © IAEME linear up to the initial yield, s . The response in plastic regime is characterized by stress hardening c0 followed by strain softening ing beyond the ultimate stress, s . The inelastic (or crushing) strain and cu plastic strain values, pl e~ in and e~ , are defined by (3) and (4), respectively. c c of the elastic modulus in compressive and tensile behavior, respectively. in c e~ =e −e el c oc d s pl c d E = − ( ) c c o E = 1− d E (1 ) ~ ~ c o c in c c e e − ( ) t t o E = 1− d E where: c e : total compressive strain el oc e : The elastic tensile strain corresponding to the c s : Compressive stress dc : compression damage parameter (a) Tension behavior associated with tension stiffening Figure 1. (a) Compressive stress-strain relationship [ , in (5) and (6), Figure 2. Numerical properties of RC structure 100 In addition, the reduction Ec and Et, are given (3) (4) (5) (6) undamaged material, el oc e =s E t o (b) Compression behavior associated with compression hardening Concrete damaged plasticity model [2] 11] (b) Modified tension stiffening model [ 5]
  • 5. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), In this analysis, modeling of the compressive stress-strain curve was d developed based on the normal strength concrete with s value, c s , between the yield point at previous research [11], which can be used for shown in Fig. 2(a). The compressive stress value 0.3s cu in the descending portion is calculated by ( for the concreteis shown in Fig.2(b). through the rebar and to define cracking and post cracking prope – 6308 (Print), pp. 97-113 © IAEME cu less than 62 MPa, as cu 0.5s and the 7). Furthermore, modified tension stiffening model It is introduced in order to simulate load transfer across cracks rties The equations, c cu o s ,s and E are in kip/in2 with the conversion factor of 1MPa = 0.145 kip/in ( ) ( ) cu b e e s b c o c s b e e c o − + = 1 [ ( )] cu o o s e E b − = 1 1 5 3 8.9 10 2.114 10− − = x + x o cu e s 2 3 E 1.243 x10 3.283 x10 o cu = s + 2.4 Numerical modeling of reinforced concrete 2. ) In order to ensure the validity of the numerical analysis, a model comparison to actual behavior was performed. A simple model of RC beam structure shown in including its material properties [1 b of 100 mm, the height h of 400 mm, 230 mm from the beam ends.The shear span ratio ( respectively. Other structural properties were shown in Table 1. It was subjected to two identical point loads and applied symmetrically on the rigid plates. Moreover, the stress the concrete and rebar are shown in was measured by means of LVDTs. Figure 3. Position of the tested RC beam [1 Fig. 3was chosen, with the width was were 0.5 and 320 mm, stress-strain relationship of mid-span 440 30 100 According to the experimental test setup data, RC beam was then simulated in X X-Y-Z coordinate system with a half-length by symmetry condition, as shown in Fig.5. X, Y, and Z axes were parallel to the longitudinal, depth and width of beam. The compressive strength of the were 27.214 MPa (taken as yielding strength The density, Young modulus Eo kg/m3, 33342.61 MPa, 3.315 MPa, and 0.167. In addition, rebar was assumed as steel material with the density of 7850 kg/m3, yield stress ) fcu). 101 properties for the concrete. (7) (8) (9) (10) (RC) beam structure 10]. As shown in this set-up, a rectangular RC beam 900 mm long Lwas positioned horizontally and supported at a/d) and the depth d wer Fig. 4(a) and Fig. 4(b), respectively.The deflection at mid 10] Table 1. Structural properties of RC beam Descriptions Dimensions (mm) l t r e concrete fco) and 54.427 MPa (taken as ultimate strength o, tensile stress t0 s , and Poisson’s ratio c u of concrete were 2400 fyof 375.3 MPa, Young modulus Es of 205939.65 MPa, and
  • 6. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), Poisson’s ratio s u of 0.3. The damaged variables, Fig.6(a) and Fig.6(b). (a) Stress-strain curve for concrete Figure 4. Model input of RC beam (a) Applied load and boundary condition Figure (a) Tension damage Figure pp. 97-113 © IAEME dt and dc, are defined based on plot presented in (b) Stress-strain curve for steel rebar [10 102 (b) Solid element (c) Rebar element 5. Model of RC beam in ABAQUS (b) Compression damage 6. Damage variables of the concrete – 6308 (Print), 10]
  • 7. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 2.5 Numerical modeling of reinforced concrete abutments According to Japan Specifications for Highway Bridges, Part IV (Substructures) [ three different types of the wing wall shapes. The shapes and dimensions vary according to the installation site of the abutment, backfill height, and gradient of the slope. The numerical model of RC abutment Type 2 as the typical model of abutment in Japan is representative for actual model, as shown in Fig.7. In order to increase the strength of abutment, abutment Type 4 was analyzed as a proposed model to be developed from Type 1 (without wing wall Moreover, based on this specification, the wall of a T cantilever with the fixed end at the node connected to the top of the footing. Therefore, in order to reduce the number of nodes and elements in the modeling, it needs to simplify the model by omitting the footing of abutment and modeling support with fixed boundary condition. Summary of the comparison results in Type 1, with and without footing are described in Table recognized that the analytical method of RC behavior of abutment with footing. (a) Numerical model Figure 7. Model of abutment Type 2 as the typical model in Japan Table 2. Summary of the maximum result in each model Descriptions S11 S33 PE11 AC Yield dt pp. 97-113 © IAEME 103 . wall) and Type 3 (full wing wall). T-shaped abutment can be designed as a abutment without footing is able (b) Real bridge . Type 1 (with footing) Type 1 (without footing) 1.591 e+8 1.592 e+8 2.493 e+6 2.507 e+6 2.955 e-4 2.956e-4 Similar value and position Similar value and position – 6308 (Print), ges, 8], there are ) 2 and Fig.8. It was to represent the Diffe-rences 0.06% 0.56% 1.30%
  • 8. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME Figure 8. Load vs displacement Four different abutment modeling approach were carried out with a half symmetry condition, as shown in Fig.9. The dimensional configurations are depicted in Fig. Table 3, respectively, with parameter of Furthermore, the rebar arrangement is given in Fig. 11. (a) Type 1 (b) Type 2 Fig t represents the thickness of parapet wall and wing wall. Figure 10. Dimensional configurations of abutments (unit: 104 (c) Type 3 Figure9. Numerical models of abutments . – 6308 (Print), half-length model by 10 and (d) Type 4 m)
  • 9. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), Table 3.Dimensional configurations of four abutments Descrip tions Type 1 (m) Type 2 (m) Type 3 (m) b2 - - h3 - 1.0 8.0 h4 - 3.3 0.0 h5 5.5 5.5 5.5 h6 - - t 0.5 0.5 0.5 Figure 11. Rebar arrangement of Type 4 pp. 97-113 © IAEME Figure 12. Stress-strain curve for concrete . Figure 13. Side view of abutment [1 Material property of the concrete was assumed from previous research [1 12, while for the rebar was similar with RC beam input. The compressive strengths were 13.75 MPa (taken as yielding strength fco) and 27.5 MPa (taken as ultimate strengt modulus Eo,tensile stress t0 s , and Poisson’s ratio MPa, and 0.2. 2.6 Loading conditions There are two types of loading condition for RC beam and weight as a gravity load g of 9.8 amplified under force control. Design seismic force of the unseating prevention structure be taken as 1.5 times dead load abutment with full wing wall and applied the unseating prevention structure (UPS), as shown in 13. In this research, four static horizontal loads through UPS were applied in the half parapet wall, with the dead load reaction of the superstructure was 2900 kN, obtained from the deck weight. Therefore, each UPS will transfer the external load to the parapet wall of 543.75 kN. HF = 1.5 RD 105 ial ) strength fcu c u of concrete were 2400 kg/m RC abutments, including the self m/s2 and the external load. The external load in RC beam was reaction, RD [13]. Previous research [14] developed a model of . Type 4 (m) - 0.5 8.0 0.0 1 - 1 0.5 – 6308 (Print), 14] 12], as shown in Fig. cu). The density, Young 3,25000 MPa, 2.75 self-external structure, HF, may ] Fig. half-height of (11)
  • 10. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), 2.7 Interaction Properties – 6308 (Print), General contact surface algorithm was considered to determine the modeling of contact behavior in the interacting surfaces between concrete and steel plate in RC beam. The friction coefficients of contact point was analysis, the steel plate was used in order to transfer the external load to RC beam and to set down the support. The embedment was defined using an embedded constraint and was achieved by constraining rebar elements into solid element 2.8 Boundary conditions , The RC beam and abutments were modeled as a half conditions in support were hinged RC beam was constrained with boundary condition in X in the mid-span of RC abutments was constrained in Z direction III. RESULTS AND DISCUSSIONS 3.1 Analysis of RC beam structure The load-displacement curves for experime ntal are shown in Fig. 14. The displacement mid-span of RC beam structure and From this figure, it can be seen that the data up to 40 tf. Moreover, the maximum load 48.54 tf, which is slightly larger than experimental result of 45 tf. pressure-over closure. In this , In order to visualize the cracking distribution within the FEM, the positive plastic strain can be mapped with color coded contours shown in flexural cracks initiate first in the mid The maximum plastic strain occurs in the “red” regions where the plastic strain equals 0.00255 corresponds to the maximum tension damage parameter of approximately 0.9. Dark blue regions correspond to areas of no tension damage. According to the analysis, it could be concluded that the cracking distribution of RC beam is more localized within the support and mid Figure 14. Vertical load vs displacement curves Figure 1 pp. 97-113 © IAEME 106 ral set to be 0.1 and hard contact for pressure element, in order to create a proper bond action. half-length model with the boundary and fixed, respectively. The surface of YZ in the middle length of s X-direction (U1=0), whether the surface of XY (U3=0). experimental result and numerical analysis by ABAQUS displacementand load shown correspond to the vertical displacement at the total vertical force imposed on the structure, respectively. , numerical resultcorrelate well with those from experimental aximum to be transmitted in RC beam by numerical analysis Fig. 15. The beam exhibit flexure mid-span of structure, followed by inclined flexure . 15. FEM magnitude of plastic strain is . flexure-shear failure where flexure-shear cracks. mid-span of the beam. agnitude
  • 11. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), Load = 22 tf U2 = 0.229 mm (a) pp. 97-113 © IAEME Analysis (b) Experiment Figure 16. RC beam cracking pattern with the external load of 20 tf The comparison between analytical and experimental results of this behavior due to external load of 20 tf is shown in Fig. 16. “L correspond to the cracking of the concrete. Due to an automatic step increment in analysis, the result is figured out at load of 22 tf. It indicates that the cracking distributions in analytical good agreement with those from experimental results. 3.2 Analysis of RC abutments 3.2.1 Longitudinal displacement The longitudinal displacements of abutmentswere investigated in the wing wall part and half part of abutment, three levels in each side longitudinal displacement of the wing wall part parapet and bottom of abutment, respectively. Otherwise, in UB2, and U2. Figure 1 (a) Middle part Figure 18. Longitudinal displacement of abutment (mm) 107 . Light blue and deep colors” regions with positive plastic strain butments isplacement side, as shown in Fig. 17. UT1, UB1 in different level positions, top , the middle part are depi 17. Position of the nodal displacement (b) Wing wall part . Wing wall Middle part part – 6308 (Print), ht study are in a half-length and U1 represent the of parapet, bottom of depicted as UT2,
  • 12. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), Total static horizontal load which can be expected to be – 6308 (Print), pp. 97-113 © IAEME prevention structures for half-length model was 2175 kN. Applying external load affect the longitudinal displacement of each abutment, are depicted in Fig. 18(a) and Fig. 18(b) as displacement in the middle and wing wall p art, wall part UT1 of 10.64 mm, 3.16 mm, 0.59 mm, and 0.36 mm for abutment Type 1, Type 2, Type 4, and Type 3, respectively. It signifies in reducing of 59.20%, 94.33% and 92.06% for abutment Type 2, Type 3 and Type 4, respectively. These results prove that installation of the wing wall in abutment have a capability in decreasing of the longitudinal displacement. In addition, a static pushover analysis was carried out with the external load amplification i order to characterize the maximum load to be transmitted in abutment. The result of load versus displacement curve is shown in Fig. 19. The study reported that the maximum load for abutment Type 1 is the smallest one of 2792.25 kN. Type 3 and Type 4 have which are smaller than Type 2 of 3244.43 kN. This condition is possibly due to design of the wing walls in Type 4 as slabs fixed on two sides to a wall and footing, which can reduce the longitudinal displacement and flexibility of the structure. Consequently, it leads crack at the parapet wall. (a) Figure 19. Longitudinal displacement of abutment (mm) 3.2.2 Cracking Distribution of RC Abutments (a) Initial cracking Figure 20. Contour plot of tensile damage in RC abutment Type 108 transmitted through the unseating part, respectively. Interesting results occur in the wing similar value of 3009.27 kN, y Middle part (b) Wing wall part . at 1093.11 kN (b) Final cracking at 2792.25 kN . 1 at different external load in
  • 13. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), (a) Initial cracking at 1093.11 kN pp. 97-113 © IAEME Figure 21. Contour plot of tensile damage in RC abutment Type 2 at different (a) Initial cracking at 1093.11 kN Figure 22. Contour plot of tensile damage in RC abutment Type 3 at different external load (a) Initial cracking at 1093.11 kN Figure 23. Contour plot of tensile damage in RC abutment Type 4 at different external load 109 (b) Final cracking at 3244.43 kN (b) Final cracking at 3009.27 kN (b) Final cracking at 3009.27 kN our – 6308 (Print), external load
  • 14. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME Figs.20-23 show contour plot of output variable DAMAGET, which is a scalar degradation measure used to express the reduced tensile elastic modulus of concrete after it has sustaine cracking damage. Sequence of the concrete cracking are described as initial and final cracking, as shown in section (a) and (b), respectively. “Dark blue” regions correspond to areas of no tension damage or no cracking. The maximum tension damage occurs strain equals 0.00264 corresponds to the maximum tension damage parameter of approximately 0.9. From these figures, it can be discovered that the initial cracking of all abutments occur in two different positions, in peripheral of the external load and intersection between parapet wall and abutment wall due the external load of 1093.11 kN. In addition, cracking is also found at bottom of abutment wall near the footing for Type 1 and Type 2. Type 1 is found as a structur critical damage due to the cracking propagation in region through its width. Moreover, it propagates from the middle width to the edge position, lead the connection part between wing wall and parapet wall to crack. 3.2.3 Load-tensile strain plot for reinforcing bar Fig. 24(a) shows the maximum tensile stress versus tensile strain relationship of the rebar, located at the reverse side of parapet wall. According to this figure, it can be seen that the tensile steel rebar is not yield at failure in abutment with all types of the wing wall. Otherwise, yielding occurs at Type 1. Furthermore, the relationship between load and maximum tensile strain in the rebar is depicted in Fig. 24(b). From these results, it is recognized that installation of t increases the stiffness of abutment, resulting on strain reduction in the rebar. (a) Stress- Figure 2 3.2.4 Shear stress distribution of RC abutments Stress distribution is one of the important aspects to be evaluated in abutment. The areas subjected to high stress is the most common problems observed during the inspection of the failure of abutment in the past large earthquake. are studied in numerical analysis these figure, it can be determined that wallnearly the intersection with the wi 110 in “red” regions, where the cracking eripheral in ure -strain ratio (b) Load versus tensile strain 24. Tensile strain plot for the rebar ribution Shear stress distributions around vertical wall of abutments analysis, with the results for each abutment are shown in maximum shear stresses occur at the region of parapet wing wall. – 6308 (Print), sustained structure with the most the wing wall ertical Fig. 25. From
  • 15. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), (a) Type 1 (c) Type 3 Figure 2 IV. CONCLUSIONS The elasto-plastic behavior of 3 – 6308 (Print), pp. 97-113 © IAEME effect of the wing wall were investigated in this study different abutment modeling approaches subjected to static prevention structure with consideration of the wing wall. The conclusions are summari following. 1) The analytical method of Concrete Damaged Plasticity by the elasto-plastic behavior of RC structure. The material modeling was experimental results in showing the behavior of RC beam in cracking distribution. 2) Installation of the wing wall in abutments ha summarized as said to be valid as displacement and displacement of 59.20%, 94.33% and 92.06% for abutment Type 2, Type 3 and Type 4 proposed type, respectively. in abutment. Otherwise, there was no significant 111 (b) Type 2 (d) Type 4 25. Shear stress distribution of abutments 3-dimensional reinforced concrete abutments considering the e study. Numerical studies were carried out in four horizontal loads through the unseating ABAQUS was capable to analyze case of had a capability in decreasing of the longitudinal 9.20%, ely. This condition was affected by the increasing number of stiffness effect in half-length part of abutment. as the
  • 16. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME 3) According to the static pushover analysis, the maximum load that could be expected to be transmitted for the proposed type of abutment of 3009.27 kN was smaller than Type 2 of 3244.43 kN.It was possibly due to design of the wing walls in Type 4 as slabs fixed on two sides to a wall and footing, which reduced the longitudinal displacement and flexibility of the structure. 4) The initial cracking for all abutments occurred in two different positions, at the peripheral of the external load and intersection between parapet wall and abutment wall. Installation of the wing wall in the proposed model reduced the cracking at the bottom of wall and compressive strain of the concrete. 5) The stress distribution was affected by the wing wall. From numerical analysis, it was depicted that the maximum shear stress occurred at the region of parapet wall nearly the intersection of the wing wall. Furthermore, the tensile steel of the rebar was not yielded at failure in abutments with the wing wall which was affected by the reduction of the axial strain. 6) Although the present study found better evidence on the proposed model of abutment Type 4 in its behavior, no earth pressure was applied. Therefore, further studies are necessary in order to determine the behavior of RC abutment under earth pressure and strong ground excitation. 112 ACKNOWLEDGEMENT The first author acknowledges DIKTI (Directorate General of Higher Education) as the financial supporter of the scholarship and University of Brawijaya as the home university. The support in completing the doctoral study in Kumamoto University is gratefully appreciated. REFERENCES [1] M. Nz M. Nazem, I. Rahimani and M. rezaee-Pajand, Nonlinear FE analysis of reinforced concrete structures using a tresca-type yield surface, ScienticaIranica, 16 (6), 2009, 512-519. [2] Dassault Systems Simulia Corp., ABAQUS/CAE User’s Manual 6.11, Providence, RI, USA, 2011. [3] A. Ahmed, Modeling of a reinforced concrete beam subjected to impact vibration using ABAQUS, International Journal of Civil and Structural Engineering, 4 (3), 2014, 227-236. [4] A.R. Mohamed, M.S. Shoukryand J.M. Saeed, Prediction of the behavior of reinforced concrete deep beams with web openings using the finite element method, Alexandria Engineering Journal, 53, 2014, 329–339. [5] B.L. Wahalathantri,Damage assessment in reinforced concrete flexural members using modal strain energy based method, Doctoral diss., Queensland University of Technology, 2012. [6] A. Aviram, K.R. Mackie and B. Stojadinovic,Effect of abutment modeling on the seismic response of bridge structures, Earth EngEngVib, 7 (4), 2008, 395-402. [7] M.J. Karantzikis, C.C. Spyrakos, Seismic analysis of bridges including soil-abutment interaction, 12 World Conference on Earthquake Engineering, 2000. [8] Japan Road Association, Specifications for Highway Bridges Part IV: Substructures, 2002. [9] A. Kawachi, Investigation of the effect of wing walls on the elastic behavior of the parapet on the abutment, Thesis, Kumamoto University, Japan, 2007. [10] T. Yamao, A. Kawachiand M. Tsutsui, Static and dynamic behaviour of a parapet wall of the abutment, 11th International Conference on Steel, Space and Composite Structures, 2012. [11] L.S. Hsu and C.T.T. Hsu, Stress-strain behavior of steel-fiber high-strength concrete under compression, ACI structural journal, 91 (4), 1991, 448-457.
  • 17. International Journal of Civil Engineering and Technology (IJCIET), ISSN 0976 – 6308 (Print), ISSN 0976 – 6316(Online), Volume 5, Issue 11, November (2014), pp. 97-113 © IAEME [12] D. Setyowulan, T. Hamamoto and T. Yamao, Eigenvalue analysis and characteristic behaviour of reinforced concrete abutments, 39th Conference on Our World in Concrete Structures, Singapore, 2014. [13] Japan Road Association, Specifications for Highway Bridges Part V: Seismic Design, 2002. [14] A. Kawachi, Proposal of the simple design method and the seismic behavior of the parapet of 113 abutment, Master thesis, 2009. [15] Yaman S.S. Al-Kamaki, Riadh Al-Mahaidi and Azad A. Mohammed, “Behavior of Concrete Damaged by High Temperature Exposureand Confined With CFRP Fabrics” International Journal of Civil Engineering Technology (IJCIET), Volume 5, Issue 8, 2014, pp. 148 - 162, ISSN Print: 0976 – 6308, ISSN Online: 0976 – 6316. [16] Prerna Nautiyal, Saurabh Singh and Geeta Batham, “A Comparative Study of The Effect of Infill Walls on Seismic Performance of Reinforced Concrete Buildings” International Journal of Civil Engineering Technology (IJCIET), Volume 4, Issue 4, 2013, pp. 208 - 218, ISSN Print: 0976 – 6308, ISSN Online: 0976 – 6316.