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Numerical Analysis of Carbon Fiber Reinforced 
Plastic (CFRP) Shear Walls and Steel Strips under 

Cyclic Loads Using Finite Element Method 
 

Nahid Askarizadeh 
Department of Civil Engineering 

Faculty of Engineering 
Bandar Abbas Branch 

Islamic Azad University 
Bandar Abbas, Iran 

Mohammad Reza Mohammadizadeh 
Department of Civil Engineering 

Faculty of Engineering 
Hormozgan University 

Bandar Abbas, Iran 

 
Abstract—Reinforced concrete shear walls are the main elements 
of resistance against lateral loads in reinforced concrete 
structures. These walls should not only provide sufficient 
resistance but also provide sufficient ductility in order to avoid 
brittle fracture, particularly under strong seismic loads. 
However, many reinforced concrete shear walls need to be 
stabilized and reinforced due to various reasons such as changes 
in requirements of seismic regulations, weaknesses in design and 
execution, passage of time, damaging environmental factors, 
patch of rebar in plastic hinges and in some cases failures and 
weaknesses caused by previous earthquakes or explosion loads. 
Recently, Fiber Reinforced Polymer (FRP) components have 
been extensively and successfully used in seismic improvement. 
This study reinforces FRP reinforced concrete shear walls and 
steel strips. CFRP and steel strips are evaluated by different yield 
and ultimate strength. Numerical and experimental studies are 
done on walls with scale 1/2. These walls are exposed to cyclic 
loading. Hysteresis curves of force, drift and strain of FRP strips 
are reviewed in order to compare results of numerical work and 
laboratory results. Both numerical and laboratory results show 
that CFRP and steel strips increase resistance, capacity and 
ductility of the structure. 

Keywords-numerical analysis; shear wall; FRP; lateral load; 
ABAQUS 

I. INTRODUCTION 
Polymer coatings used to improve concrete structures were 

first developed in 1980 in Europe and Japan. In Europe, FRP 
systems were used as an alternative to steel plates. Connection 
of steel plates to tensile part of concrete members by epoxy 
resins is a common durable method to enhance bending 
strength of these members. Steel plates are corroded and their 
corrosion leads to the collapse of steel plates with concrete. 
Moreover, they are difficult to install, because they are 
installed by heavy machinery. Thus, scientists tended to replace 
steel coatings by FRP materials. With almost 20% of the 
weight of steel coatings, FRP is approximately 8 to 10 times 
more resistant than steel. One of the problems with system 
structural calculations is the difficulty of computer modeling in 
the form of finite element. Moreover, variation in effective 
parameters on behavior of these structures challenges 

laboratory methods due to high cost and time. Numerical 
methods also require a correct understanding of non-linear 
behavior of reinforced concrete and FRP [1]. This study 
develops suitable structural models and models non-linear 
behavior of concrete, reinforcement and FRP. 

II. PROBLEM DESCRIPTION 

A. Concrete Damage Plasticity 
The most important step in numerical modeling of 

reinforced concrete structures is the determination of concrete’s 
nonlinear behavior. In the finite element software ABAQUS, 
nonlinear behavior of brittle materials can be defined through 
three models: 1) smeared cracking, 2) brittle cracking and 3) 
concrete damage plasticity [2]. Concrete damage model is the 
only model which can be used in both static and dynamic 
analysis. In this model, it is assumed that tensile cracking and 
compressive crushing are two main aspects of concrete failure 
mechanism. In modeling brittle material cracking under cyclic 
loading (alternating tension and compression), stiffness 
recovery is allowed during reciprocating loads [3]. In plastic 
damage model, elimination of elements and cracking are not 
allowed during analysis due to the lack of failure criterion, 
however, this model is able to predict location and direction of 
cracks. 

B. Interpretation of Moment - Curvature Curve for 
Reinforced Concrete Shear Wall Section 
Unlike the simplicity in design and construction of 

reinforced concrete shear walls, the real response of these 
elements is rather complex. Overall behavior of walls is 
influenced by bending, shear and axial responses. Wall sections 
are against compressive axial forces caused by gravity loads 
and their own weight. Axial pressure acting on the wall is 
estimated at 20% of product of concrete compressive strength, 
fc΄, in Ag (gross concrete cross section) [4]. Authors in [4] 
described the moment-curvature relationship in walls of high-
rise buildings against a unidirectional load. When bending 
moment is applied on the wall section, initial response of the 
wall is linear elastic with initial flexural stiffness. Cracking 



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occurs when moment exceeds initial elasticity and flexural 
stiffness is reduced by growth of the first crack and start of 
additional cracks. Slope of this phase results from 
approximately parallel response of flexural stiffness of the 
cracked and deformed section. Further increase in the applied 
moment leads to the weakening of steel and the section's 
capacity. It is thus considered essential to use non-linear 
analysis and theories of plasticity to simulate behavior of 
reinforced concrete shear wall.  

Uniaxial stress-strain relationship of concrete under 
pressure and tension is an important parameter in importing 
concrete damage plasticity model to the software. To do this, 
the Hognestad curve is used. Equations (1) and (2) are used to 
import compressive stress of concrete versus compressive 
strain to the software. In these equations, ε0 is the 
corresponding strain to maximum stress. For specimens of 
which ε0 is unknown, this study uses the value 0.002, which is 
a rational value for conventional concretes [5]. In (2), ''cf  is 
maximum stress in concrete element. The ks factor can be 
considered as portrayed in Table I [5] for concretes with 
cylindrical compressive strength. Descending branch of the 
modified Hognestad curve is linear which extends from ''0 c, f  
to ''cε , 0.85fu . εu  corresponds to ultimate corresponding strain 
to compressive failure of concrete, which has been reported 
from 0.003 to higher than 0.005. This study considers 0.0038. 

'' 2

0 0

2
( )c cc cf f

 
 

 
  

 
    (1) 

'' '  c s cf k f      (2) 

TABLE I.  kS VALUES IN HOGNESTAD CURVE 

'
cf (MPA)  15 20 25 30 >35 

s  k  1 0.97 0.95 0.93 0.92 
 

C. Stress-Strain Under Tension by Using ABAQUS-
Suggested Equation 
Concrete alone cannot tolerate tensile stresses and its tensile 

strength is low (7%-11% of compressive strength). Steel rebar 
is usually used to compensate these problems. Concrete tensile 
response begins with cracking and its expansion. Thus, 
concrete behavior cannot be evaluated by considering tensile 
strain. Instead, the crack should be evaluated. The concrete 
response under pressure is linear until it reaches its tensile 
strength which is associated with very fine cracks. The increase 
in loading decreases resistance and expands cracks to fracture 
under ultimate strain [6-7]. A straight line is usually used for 
softening part of tensile curve. Moreover, tensile strength and 
ultimate strain are calculated by following equations [8-10]: 

' '0.33  t cf f     (3) 

* 0.001       (4) 

In periodic loading, stiffness decreases and cracks after 
each cycle emerge. Unlike compressive cracks, these cracks are 
completely obvious and open [6]. The curves presented for the 
static scenario are in fact pushover curves of maximum stresses 
under periodic loading. 

D. Damage Parameter 
The slope of unloading curve is lower than the slope of the 

elastic curve in the softening part, which indicates damage. The 
reduced initial stiffness is shown by dt and dc (stiffness decline 
under tension, and stiffness decline under pressure 
respectively). It is assumed that these two variables are 
functions of plastic strain, temperature and other field variables 
[3]. 

 , ,        0 1plt t t i td d f d      (5) 

 , ,        0 1plc c c i cd d f d      (6) 

where, cε
pl  and plt  are corresponding plastic strains 

under pressure and tension, θ  is the temperature, and fi  is 
the field variable. In fact, concrete damage is determined by dt 
and dc in uniaxial stress-strain curves. These damage variables 
are expressed as follows: 

 , 01 t cE d E       (7) 

where E is the damaged module of elasticity, E0 is 
undamaged module of elasticity. It is important to select 
properties of damage, because excessive damage values have 
unsuitable effect on convergence rate. 

E. Behavior of Reinforcements 
There are many stress-strain models in finite element 

software. This study uses a bilinear elastoplastic model for 
reinforcement. In ABAQUS, longitudinal and transverse 
reinforcements are modeled by two-node truss element T3D2 
which is only able to tolerate axial force and acts separately 
from concrete. 

F. Stiffness Recovery in ABAQUS 
Stiffness recovery is an important discussion in the 

mechanical response of concrete in periodic loading. In 
ABAQUS, the user can directly import the stiffness recovery 
factors, wt and wc. In the majority of quasi-brittle materials 
such as concrete reflect improvement of compressive stiffness 
resulting from closure of cracks when loading shifts from 
tension to compression. On the other hand, tensile stiffness is 
not recovered by this shift after formation of microcracks under 
concrete crushing. This behavior which is related to wt=0 and 
wc=1 is default in ABAQUS. 



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III. SPECIMENS 

A. Reinforced concrete shear walls specimens 
Group A: Five specimens of CFRP reinforced concrete 

shear walls tested by authors in [11] at scale of ½ are modeled 
in different arrangements of CFRP in ABAQUS. All specimens 
are 1000 mm in length, 100 mm in width and 1500 mm in 
height. All specimens are exposed to cyclic loading with drift 
control. Group B: Three specimens of CFRP reinforced 
concrete shear walls tested in [12] are modeled in different 
arrangements of CFRP in ABAQUS. All specimens are 1200 
mm in length, 80 mm in width and 1045 mm in height. All 
specimens are exposed to cyclic loading with drift control and 
48 kN compressive axial force and two axial forces, one 
compressive and the other tensile, in a distance which forms 
couple on top of the wall, as shown in (8) and (9). 

24 1.115A CF F      (8) 

 , 01 t cE d E      (9) 
Group C: Four specimens of steel strip reinforced concrete 

shear walls tested in [13] at scale of ½ are modeled in different 
arrangements of steel strips in ABAQUS. All specimens are 
1000 mm in length, 100 mm in width and 1500 mm in height. 
All specimens are exposed to cyclic loading with drift control 

B. Specifications of materials 
Group A: specimen 1 which is unreinforced is selected as 

reference specimen. Four other specimens are determined 
(Specimen 2, Specimen 3, Specimen 4 and Specimen 5). All 
four reinforced specimens have a layer reinforced by CFRP 
strips [11]. Group B: CW which is unreinforced is selected as 
reference specimen. Two other specimens are determined 
(RW1 and RW2). All two reinforced specimens have a layer 
reinforced by CFRP strips [2]. Group C: specimen 1 which is 
unreinforced is selected as reference. Three other specimens 
are determined (Specimen 2, Specimen 3 and Specimen 4). All 
three reinforced specimens have a layer reinforced by steel 
strips [13]. Table II shows 28-day resistance of concrete in all 
specimens. Table III shows yield and ultimate strength of rebar 
used in this experiment. Values of shear modulus (G) are given 
in Tables IV and V. 

IV. RESULTS 

A. Group A 
Figure 1 shows the force-drift hysteresis curve of numerical 

analysis for Group A specimens under cyclic load [11]. Figure 
3 shows the strain-force hysteresis curve of CFRP materials in 
numerical analysis for Group A Specimens under cyclic load. 
Table VI lists the experimental results and compares them to 
numerical results related to maximum strain. As shown, the 
numerical analysis is consistent with the experimental results.  

TABLE II.  SPECIFICATIONS OF SPECIMENS 

Group A: Five specimens of CFRP reinforced concrete shear walls 
Specimen5 Specimen4 Specimen3 Specimen2 Specimen1  

15.6 15.9 15 15.7 15.5 'cf (MPa) 
A combination of mesh and 

horizontal and parallel strips at 
the top and bottom of specimen 

A combination of X-shaped, 
horizontal and parallel strips at the 

top and bottom of specimen 

An X-shaped 
layer 

Horizontal and 
parallel strips - 

Fiber 
arrangement 

Group B: Three specimens of CFRP reinforced concrete shear walls  
RW2 RW1 CW  

37 37 45 'cf (MPa) 

A crossed and a wrapping layer at the top 
and bottom of wall 

A vertical C-shaped layer in 
side edges and a wrapping 

layer around the wall 
- Fiber arrangement 

Group C: Four specimens of steel strip reinforced concrete shear walls  
Specimen 4 Specimen 3 Specimen 2 Specimen 1  

18.5 17.8 18.2 15.5 'cf (MPa) 
A combination of horizontal 

and vertical strips 
Horizontal and parallel 

strips A X-shaped layer - 
Arrangement of steel 

strips 

TABLE III.  SPECIFICATIONS OF REINFORCEMENTS 

Group A: CFRP reinforced concrete shear walls  
Ultimate strength (MPa) Yield strength (MPa) Reinforcement diameter (mm) 

420 325 6 
522 430 10 
515 428 12 
520 425 16 

Group B: CFRP reinforced concrete shear walls  
Ultimate strength (MPa) Yield strength (MPa) Reinforcement diameter (mm) 

550 450 10 
720 620 6 

Group C: Steel strip reinforced concrete shear walls tested  
Ultimate strength (MPa) Yield strength (MPa) Reinforcement diameter (mm) 



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420 325 6 
522 430 10 
520 425 16 

 
Fig. 1.  Force-drift hysteresis curve under cyclic load, Group A, Specimens 1-5 a) experimental b) numerical  

  
TABLE IV.  SPECIFICATIONS OF CFRP  

Group A: CFRP reinforced concrete shear walls 
Ultimate strain (%) Ultimate tensile stress (MPa) Modulus of elasticity (MPa) Thickness (mm) Fiber 

1.7 4100 231000 0.12 CFRP 
Group B: CFRP reinforced concrete shear walls  

Ultimate strain (%) Ultimate tensile stress (MPa) Modulus of elasticity (MPa) Thickness (mm) Fiber 
1.6 3790 230 0.175 CFRP 



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Group C: Steel strip reinforced concrete shear walls 
Ultimate strength (MPa) Yield strength (MPa) Thickness (mm) Steel strips 

470 340 2.5 

TABLE V.  INPUT PARAMETERS FOR MODELING FIBERS IN ABAQUS 

Group A: CFRP reinforced concrete shear walls  

2 3G   1 3G   1 2G  2 3N u  1 3N u   
 

1 2N u  3
E   2E   1E   Thickness Layer Fiber 

9625 9625 96250 0.2 0.2 0.2 23100 23100 231000 0.12 1 CFRP 
Group B: CFRP reinforced concrete shear walls 

2 3G    1 3G   1 2G  2 3N u  1 3N u  1 2N u  3E   2E   1E   Thickness Layer Fiber 
9583 9583 95833 0.2 0.2 0.2 23000 23000 230000 0.12 1 CFRP 

Group C: Steel strip reinforced concrete shear walls  
Ultimate strength (MPa) Yield strength (MPa) Thickness (mm) Steel strips 

470 340 2.5 
  

 
Fig. 2.  Push comparison of hysteresis curves of experimental results and numerical analysis (Group A)

TABLE VI.  GROUP A: COMPARISON OF MAXIMUM FORCE  

Num/ Exp Num Exp 
Specimen Pull 

(KN) 
Push 
(KN) 

Pull 
(KN) 

Push 
(KN) 

Pull 
(KN) 

Push 
(KN) 

0.99 0.97 149.55 136.072 151.33 140 Specimen1 
1.05 0.91 267.57 225.62 254.72 250 Specimen2 
1.02 0.95 234.63 204.55 230.22 215 Specimen3 

1 1.05 239 273.69 238 260 Specimen4 
1.11 0.99 272.3 248.5 245 250 Specimen5 

TABLE VII.  GROUP A: MAXIMUM CFRP STRAIN  

Num/Exp Exp Num Specimen 
- - - Specimen1 

0.97 0.0075 0.0073 Specimen2 
0.89 0.0095 0.0085 Specimen3 
0.97 0.0088 0.0085 Specimen4 
0.96 0.0083 0.008 Specimen5 

 

B. Group B 
Figure 4 shows the force-drift hysteresis curve for Group B: 

CW, RW1 and RW2 under cyclic load [12] (Table VII). Figure 
5 compares push of force-drift hysteresis curves of specimens 
under cyclic load resulting from experimental  
numerical analysis. Table VIII lists experimental results and 
compares them to numerical analysis related to maximum 
forced obtained in reciprocating cycles. As shown, the 
numerical analysis for Group B specimens is consistent with 
the experimental results. Figure 4 shows the strain-force 
hysteresis curve of CFRP materials in numerical analysis for 
RW1 and RW2 under cyclic load. Table IX compares the 
experimental and the numerical results which are shown to be 
consistent. 

 



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Fig. 3.  Strain-force curve of CFRP in Group A, Spesimens 1-5 a) experimental b) numerical  

TABLE VIII.  GROUP B: COMPARISON OF MAXIMUM  FORCE   

Num/ Exp Num Exp Specimen Pull (KN) Push (KN) Pull (KN) Push (KN) Pull (KN) Push (KN) 
1.075 1.04 64.52 62.53 60 60 CW 
1.01 1.06 111.63 117.53 110 110 RW1 
1.11 1.14 100.33 107.82 90 94 RW2 

TABLE IX.  GROUP B: MAXIMUM CFRP STRAIN  

Num/Exp Exp Num Specimen 
1.04 5100 5300 RW1 
0.93 4300 4000 RW2 



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Fig. 4.  Force-drift hysteresis curve under cyclic load, Group B, a) experimental b) numerical  

 
Fig. 5.  Push comparison of hysteresis curves of experimental results and numerical analysis for Group B specimens. 

 

 
                                                                     (a)                                                                                               (b) 

Fig. 6.  Strain-force curve of CFRP in Group B, Specimens RW1 and RW2 a) experimental b) numerical 



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C. Group C 
Figure 7 shows force-drift hysteresis curve for Group C 

specimens under cyclic load [13]. Figure 8 compares the 
experimental and numerical push of force-drift hysteresis 
curves. Table X lists the experimental results and compares 
them to numerical analysis related to maximum forced 
obtained in reciprocating cycles. As shown numerical analysis 
results are consistent with the experimental results. 

 
TABLE X.  COMPARISON OF MAXIMUM FORCE  

Num/ Exp Num Exp 
Specimen Pull 

(KN) 
Push 
(KN) 

Pull 
(KN) 

Push 
(KN) 

Pull 
(KN) 

Push 
(KN) 

1 0.94 150 131.9 150 140 Specimen1 
1.04 1.004 254.07 239.15 245 238 Specimen2 
1.03 0.99 225.99 219.12 220 222 Specimen3 
1.09 0.96 228.65 215.73 208 225 Specimen4 

 

 
Fig. 7.  Force-drift hysteresis curve under cyclic load, Group C – Specimens 1-4 a) experimental b) numerical  



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Fig. 8.  Push comparison of hysteresis curves of experimental results and numerical analysis (Group C)

 

V. CONCLUSION 
Close results of numerical analysis and experiments on 

specimens before and after FRP reinforcement indicate that 
numerical modeling can be used as a scientific and inexpensive 
tool for analyzing the cyclic behavior of unreinforced and FRP 
reinforced concrete shear walls. Both numerical and 
experimental results showed that reinforcement of reinforced 
concrete shear walls, which have shear weakness under seismic 
loads by FRP coating, is a suitable solution for increasing their 
resistance. Adjustment of reinforced strips was effective on 
cyclic behavior of reinforced shear walls and failure mode. To 
compensate shear weakness of reinforced concrete shear walls, 
it is better to use horizontal strips along transverse 
reinforcements on both sides of the wall. To compensate 
bending weakness of reinforced concrete shear walls, FRP 
plates are installed vertically along the height of shear wall 
parallel to longitudinal reinforcements. In general, results show 
that shear positions of fibers concentrated on edges increase 
bending and shear strength of the wall. Both numerical and 
experimental results show that FRP materials increase ultimate 
strength related to reinforced walls compared to unreinforced 
ones. 

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