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Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
Effect of the Distance between Points Load on the Behavior of 
Strengthened Reinforced Concrete Beams 
Lec.AamerNajim Abbas1*Asst.Lec.NuraJasim Muhammed1**Asst.Lec.shaimaa Tariq Sakin1*** 
1. Al_Mustansiriya University ,College of Engineering ,Civil Department 
*Amir_najim@yahoo.com**nura_jacob@yahoo.com***shtsakin@yahoo.com 
6 
Abstract 
The general behavior of the reinforced concrete beams depends on many variables, including what is the 
quality of the concrete and strength and including those on reinforcement type and quantity of reinforcement in 
the beam. But there is an important variable which nature of loads application on the beam and type of load is it 
point or distributed. Sometimes the distance between points load is variable such as vehicle wheel load because 
each vehicle as different distance between wheels. 
In this research, the effect of changing the distance between the points load were studied and compared with 
model carrying a single point load at mid span, as well as studying the effect of the use of carbon fiber with a 
length equal to the distance between the points load. 
Theoretical results consists of eight models were compared in this study with the results of the previous 
experimental results. The study contains a discussion of the general behavior of the beam in addition to the study 
of the failure carrying load, cracking load, ductility and the relationship between the stages of load application 
and the deflection of concrete beams with and without carbon fiber sheets. 
Key words: Ansys, strengthening, ductility, carbon fiber. 
1. Introduction 
Concrete structural components require the understanding into the responses of these components to a variety of 
loadings application. 
A simply-supported reinforced concrete beam may fail primarily- either in flexure or in shear. Failure in flexure 
will occur if the ultimate flexural moment capacity is exceeded at any section of the beam before the conditions 
for shear failure have been satisfied at any section. Failure in shear will occur when the limiting shear-moment 
capacity is reached at some section of the beam at which inclined cracks have developed sufficiently to reduce 
the available compressive area. 
Whether a given beam will fail in flexure or in shear will depend on the relative magnitudes of the ultimate 
flexural moment (Mf), the limiting shear-moment (Ms) and the critical shear(V) at various locations along the 
span and on the actual values of moment and shear at these locations. The relationship between mode of failure 
and properties of the beam cross-section and loading arrangement is illustrated most simply by considering the 
hypothetical behavior of a simply-supported beam as illustrated in Fig.(1). 
The beam shown in Figure (l) is simply-supported at its end span is assumed to carry two concentrated loads 
arranged symmetrically about mid span. Only half of the span is shown in the Figure, The distance from the 
support to the load is called the "shear-span" and is designated by the symbol (a). For the particular type of 
loading shown, the maximum moment and the maximum shear both occur at the location of the load and their 
ratio is M/V = a.
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
Figure (1) Effect of moment-shear ratioon failure mode 
7 
2. Carbon Fiber 
Carbon fiber is defined as a fiber containing at least 92 wt % carbon, while the fiber containing at least 99 wt % 
carbon is usually called a graphite fiber. Carbon fibers generally have excellent tensile properties, low densities, 
high thermal and chemical stabilities in the absence of oxidizing agents, good thermal and electrical 
conductivities, and excellent creep resistance. They have been extensively used in composites in the form of 
woven textiles, prepregs, continuous fibers/rovings, and chopped fibers. The composite parts can be produced 
through filament winding, tape winding, pultrusion, compression molding, vacuum bagging, liquid molding, and 
injection molding. 
In terms of final mechanical properties, carbon fibers can be roughly classified into ultra-high modulus (>500 
GPa), high modulus (>300 GPa), intermediate modulus (>200 GPa), low modulus (100 GPa), and high strength 
(>4 GPa)(1). 
Ehsan Ahmed et al(2). studied the flexural behavior of reinforced concrete beams strengthened with carbon fiber 
through an experimental and theoretical study includes six models, one without carbon fiber and the others with 
different number of layers of carbon fiber. They concluded that there is an increase in member stiffness in 
addition to improvement in yield and ultimate load. Another group of researchers (tom Norris et al.)(3) used in 
their research different ways to paste carbon fiber to concrete beams to see what is the proper way to use carbon 
fiber for strengthening the concrete beams, All ways showed that there is a clear improvement in carrying 
capacity of beams in addition to the improvement in ductility and yield load. 
3. Test Program 
The experimental work program conducted by Mohammad Z.Y(4) was selected to validate the simulations 
presented in this paper. In his study, two experimental programs were carried out to investigate the behavior of 
reinforced concrete (RC) beams strengthened with CFRP fabrics between points load using a wet layup method. 
The aim of the research was to study the failure characteristics, deflection behavior and general performance. A 
total of six reinforced concrete beams were tested under two points bending with different distances between 
points of loading. In this test program, The variables of the beams were the distance between points load, CFRP 
bond length (equal to the distance between points load). To simulate the behavior under service, the beam named 
as (B) was selected. The geometrical properties and reinforcement details are illustrated in Table(1) and Figure 
(2). 
Table (1) Experimental Work Variables 
Beam No. Distance Between Point Load Length of Carbon Fiber 
B1 0 0 
B2 20 20 
B3 40 40 
B4 60 60
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
In this study, the main flexural and shear steel reinforcements in the finite element models were assumed to be 
an isotropic linear elastic material until the yield point. The ultimate and yield stresses are summarized in Table 
(2). The Poisson’s ratio of steel was taken as 0.3.Concrete properties are selected as (fc'=52.88, fr =4.75 and the 
Poisson’s ratio of steel was taken as 0.2). 
The dimensions of beams was selected (100x150)mm with 2ɸ4mm at the top ,2ɸ10 at the bottom and 
ɸ4@150mm shear reinforcement along the beam. 
Table (2) Steel Properties 
8 
Bar type Modulus of elasticity 
(kN/m2) 
Yield strength (fy) 
(MPa) 
Ultimate strength (fu) 
(MPa) 
Main Reinforcement 200000 484 719 
Shear Reinforcement 200000 383 620 
Figure (2) Reinforced Concrete Beam With Loading 
4. Finite Element Analysis 
ANSYS computer program has been used for the finite element modeling. Four beams that have been studied 
were of a simply supported beamslengthof1.5mand an area100X150mm and loaded with two symmetrically 
placed concentrated vertical loads with Variable distances between point load, see Figure (3) below and Table 
(3). Table (3) shows the distances between the points load and length of carbon fiber sheets for each model. 
Model includes linear relationship to the properties concrete, a linear bond-slip relation and bilinear steel 
properties. The method of load application was applied incrementally each 2 kN. See Plate below which 
represents position of load application and position of supports. In ANSYS program symmetry properties were 
applied for the purpose of representation models. 
Figure (3) FEM Discretization for a Half of the Beam 
1 
X 
Y 
Z 
APR 12 2013 
09:53:16 
ELEMENTS 
U 
F
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
Table (3) Distance Between Points Load 
Model Number Description Distance Between 
9 
Point Load (mm) 
Length of Carbon 
Fiber Sheet 
B1 Without carbon fiber 
one point load 
One point load ------- 
B2 With carbon fiber 
two point load 
200 200 
B3 With carbon fiber 
two point load 
400 400 
B4 With carbon fiber 
two point load 
600 600 
B1W Without carbon fiber 
one point load 
One point load ------- 
B2W Without carbon fiber 
two point load 
200 200 
B3W Without carbon fiber 
two point load 
400 400 
B4W Without carbon fiber 
two point load 
600 600 
5. Material Modeling 
SOLID65 isotropic element is used to represent the concrete material, since it has a capability of both cracking in 
tension and crushing in compression. SOLID65 element is defined by 8 nodes with three degrees of freedom at 
each node; translations in the nodal x, y, and z directions, see Figure below. 
LINK8 element (It is a uniaxial tension-compression member) is used to represent the reinforcing steel (main 
and stirrups steel material). LINK8 element is defined by two nodes with three degree of freedom at each node; 
translations in the nodal x, y, and z directions, see Figure below. 
SHELL41 element is used to represent the carbon fiber sheets. SHELL41 element is defined by four nodes with 
three degree of freedom at each node.it is a 3-D element having membrane (in-plane) stiffness but no bending 
(out of plane) stiffness. See Figure below. 
Figure (4) Solid 65 Figure (5) Link 8 Figure (6) Shell41
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
5.1 Real Constants 
The real constants for this model are shown in Table below 
Table (4) Real Constant 
10 
Real constant 
set 
Element type Constant 
1 
SOLID65 
concrete 
Real constant for 
Rebar 1 
Real constant for 
Rebar2 
Real constant for 
Rebar 3 
Material number 0 0 0 
Volume ratio 0 0 0 
Orientation angle 0 0 0 
2 LINK8 
Reinforce-ment 
Steel Bar Diameter (f 10 mm ) 
Cross-sectional area 
78.54 
(mm2) 
Initial strain (mm/mm) 0 
3 LINK8 
Reinforce-ment 
Steel Bar Diameter (f 4 mm ) 
Cross-sectional area 
12.566 
(mm2) 
Initial strain (mm/mm) 0 
3 SHELL41 
CFRP 
CFRP type Fabric 
Shell thickness at node I 
(mm) 
0.1 
Shell thickness at node J 
(mm) 
0.1 
Shell thickness at node 
K (mm) 
0.1 
Shell thickness at node L 
(mm) 
0.1 
Element x- axis rotation 0 
Elastic foundation 
stiffness 
0 
Added mass/unit area 0
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
5.2 Material Properties 
The material properties for this model are shown in Table below: 
Table (5) Materials Properties 
11 
Material model 
number 
Element type Material properties 
1 
SOLID65 
Linear Isotropic 
EX 34178 
PRXY 0.2 
Multilinear Isotropic 
Strain Stress 
Point 1 0.000464 15.864 
Point 2 0.001 30.94 
Point 3 0.00158 42.83 
Point 4 0.0018 45.96 
Point 5 0.00 3 52.88 
Concrete 
ShrCf-Op 0.2 
ShrCf-CI 0.3 
UnTensSt 3.64 
UnCompSt -1 
BiCompSt 0 
HydroPrs 0 
BiCompSt 0 
UnTensSt 0 
TenCrFac 0 
Material model 
number 
Element type Material properties 
2 LINK8 
Linear Isotropic 
EX 200000 
PRXY 0.3 
Bilinear Isotropic 
Yield Stress 484 
Tang Mod. 0 
3 LINK8 
Bilinear Isotropic 
Yield Stress 383 
Tang Mod. 0 
Linear Isotropic 
EX 200000 
PRXY 0.3 
4 SHELL41 
Linear Orthotropic 
Ex 234000 
Ey 1 
Ez 1 
PRXY 0.3 
PRYZ 0 
PRXZ 0 
Gxy, Gyz, Gxz 1 
6. Theoretical Results 
6.1 Failure Load 
After the data was analyzed and carefully considered, it can be said that the collected data of the failure load 
obtained from the theoretical solution for all beams is approximately equal experimental load and all the beams 
failed by flexure. The final loads for the ANSYS finite element method are the last applied load step before the 
solution diverges due to numerous cracks and large deflections. 
Through an extensive comparison between the unsupported specimens with carbon fiber and other supported 
specimens, it can be concluded that the specimens with carbon fiber have failure load more than other specimens 
without carbon fiber. This can be explained that the carbon fibers connecting both sides of the crack together and
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
delay extension more during the concrete section (increase in tensile cracking strength of concrete due to 
confinement). 
Also, the increasing Length of the carbon causes an increase in the amount of carrying capacity to bending 
stresses, because the increase in length means cover as much as possible the bending area and are controlled 
more cracks generated during download stages. 
The moment generated in the mid length of the beam is the result of multiplying the reaction by the distance 
between the reaction and applied force (couple). When the distance between the two points load increased this 
leads to decrease of the distance between the applied force and the reaction, this leads naturally to a decrease in 
couple as a result of decrease in the distance between them, for the above reasons we can say that the increasing 
in the distance between the loading points provides to some extent an increase in carrying capacity for 
specimens. 
6.2 Behavior at First Cracking 
The analysis of reinforced concrete beams in the linear region depends mainly on the appearance of cracks in 
that region where maximum bending stresses are concentrated. As was expected through a comparison between 
the different beams (different distances between the points of loading), the greater distance between points load 
delayed appearance of first cracks in the beams the reason for that is as stated previously that the increase in 
distance between point loads means decrease the applied moment on beam for same value of load if compared 
with the other models with less distance. 
A comparison of values obtained from the FE model and experimental can be seen in Table (6). The results in 
Table (6) indicate that the FE analysis of the beam prior to cracking is acceptable. 
The first cracks for the beams without carbon fiber (B1W, B2W, B3W and B4W) were observed at (27.27%, 
25%, 26.6% and 26.3%) of the ultimate load respectively where for carbon fiber reinforced beam the first crack 
load was found to be between (13.63% to 15% ) the ultimate load. There is a 11.5% to 12.8% increase in 
ultimate load for carbon fiber reinforced concrete beams when compared with beams without carbon fiber 
reinforcement. Thus the experimental results show that there is increase in the ultimate load and the first crack 
load for the fiber reinforced concrete beams. 
Table (7) Cracking and Ultimate Load Deflection 
Model Load at First Cracking (kN) Centerline Deflection 
12 
(mm) 
Ultimate load 
(kN) 
Pcr/pultimate 
% 
Exper. Theo. Exper. Theo. Exper. Theo. Exper. Theo. 
B1 6.5 6 0.5 0.33 36 38 18 15.8 
B1W 6 0.332 22 27.27 
B2 7 6 0.255 0.3175 44 44 15.9 13.63 
B2W 6 0.321 24 25 
B3 9 8 0.54 0.386 54 58 16.6 13.79 
B3W 8 0.392 30 26.6 
B4 10.5 10 0.52 0.414 70 68 15 14.7 
B4W 10 0.42 38 26.3
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
Figure (7)Comparison Between Theoretical Cracking, Yielding and Ultimate load. 
6.3 Load-Deflection Relationship 
The theoretical results for all specimens are displayed and compared with experimental results. Figures below 
contain a load-deflection curves predicted by ANSYS and the test results for all specimens Examined by 
Mohammad Z.Y.. The results of ANSYS converge with the non-strengthened specimens more than other 
strengthened specimens with carbon fiber because of not taking the slip between the concrete and the carbon 
fiber into account in the theoretical study. 
In general, the beams strengthened with carbon fiber were stiffer and more ductile than the control specimens 
with a higher ultimate load see Figure (7). In every stage of loading application, the deflections are reduced 
significantly thereby increasing the stiffness for the strengthened beams. 
13 
Figure (8) Experimental and Theoretical Load 
Deflection Curve for Beam (B1) 
Figure (9) Experimental and Theoretical Load 
Deflection Curve for Beam (B2)
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
14 
Figure (10) Experimental and Theoretical Load 
Deflection Curve for Beam (B3) 
Figure (11) Experimental and Theoretical Load 
Deflection Curve for Beam (B4) 
Figure (12) Theoretical Load Deflection Curve for 
Beam (B1) and (B1W) 
Figure (13) Theoretical Load Deflection Curve for Beam 
(B2) and (B2W) 
Figure (14) Theoretical Load Deflection Curve for 
Beam (B3) and (B3W) 
Figure (15) Theoretical Load Deflection Curve for Beam 
(B4) and (B4W) 
6.4 Ductility 
Ratio of curvature at crushing of concrete to that at yielding of steel gives the numerical value of ductility, 
known as ductility index. 
It can be seen that for a given dimension and strength, the load versus displacement curves for both specimens 
with carbon fiber and other specimens without carbon fiber appear similar. In addition, as can be seen in Table 
(8) the deflection at yielding and ultimate strength for beams without carbon fiber appear lower than those of 
beams with carbon fiber. It has been known that the deflection ductility, μΔ, in terms of ultimate deflection to 
yielding displacement, is highly correlated to the length of the carbon fiber sheet. As can be seen in Table (8),
Chemistry and Materials Research www.iiste.org 
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) 
Vol.6 No.8, 2014 
the ductility of both types of concrete beams exhibit a extrusive length effect, i.e., ductility increase with the 
increase of carbon fiber sheets, namely, a strengthened beam performs more ductile. 
The effect of increasing the distance between the points load seemed clear as when you increase this distance 
increases the ductility due to decrease moments that cause for ultimate deflection in the beam at failure. 
Table (8) Ductility of tested beams 
Beam No. Deflection at Yield 
(mm) 
Deflection at Failure 
(mm) 
Ductility Index 
B1 4.16 12.5045 3 
B2 4.64 13.4386 2.896 
B3 5.09 18.357 3.606 
B4 4.97 18.3 3.682 
B1W 3.1 5.22 1.683 
B2W 3.6 4.01 1.113 
B3W 4.3 15.822 3.679 
B4W 4.7 4.917 1.046 
7 .Conclusions 
Based on the results obtained from theoretical analysis and comparison with the experimental work, the 
following conclusions are drawn: 
1. At any given load level, the deflections are reduced significantly thereby increasing the stiffness for the 
15 
strengthened beams. 
2. All the beams strengthened with carbon fiber experience flexural failures. None of the beams exhibit 
brittle failure. 
3. The failure load of specimens with carbon fiber more than other specimens without carbon fiber. 
4. The bending stresses are reduced when length of the carbon was increased. 
5. The increasing in the distance between the loading points provides an increase in carrying capacity for 
specimens. 
6. In this study, the appearance of the first crack mainly depends on the distance between the points load, 
higher distance between the mount points load lead to the delay in appearance of the cracks. 
7. Through the adoption of the distance between the point load as a variable show that increasing the 
distance between the points load result a decreasing in moment in the mid span of the beam, this means 
an increase in carrying capacity for specimens. 
8. Through a comparison theoretical results with the experimental, showing that there is a convergence 
between the two results. 
9. It is very clear the development in ductility as a result of increasing the length of carbon fiber sheets and 
increase the distance between the points load. 
References 
1. Xiaosong Huang, " Fabrication and Properties of Carbon Fibers ",www.mdpi.com. 
2. Ehsan, A., Habibur, R. and Norsuzailina, M. S., " Flexural performance of CFRP strengthened RC 
beams with different degrees of strengthening schemes", International Journal of the Physical Sciences, 
Malaysia, Vol. 6(9), 4 May, 2011, pp. 2229-2238. 
3. Tom, N., Hamid, S., Mohammad, R., " Shear and Flexural Strengthening of Reinforced Concrete 
Beams with Carbon Fiber Sheets", Journal of Structural Engineering, Vol.123, No.7, July, 
1997,PP.903-911. 
4. Mohammad, Z., " Reinforced Concrete Beams Strengthening by Carbon Fiber Reinforced Polymer 
Against Two Points Load Divergence", Journal of Engineering and Development" Vol.16, No.2, June, 
2012 ,PP.266-280.
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Effect ofthe distance between points load on the behavior of

  • 1. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 Effect of the Distance between Points Load on the Behavior of Strengthened Reinforced Concrete Beams Lec.AamerNajim Abbas1*Asst.Lec.NuraJasim Muhammed1**Asst.Lec.shaimaa Tariq Sakin1*** 1. Al_Mustansiriya University ,College of Engineering ,Civil Department *Amir_najim@yahoo.com**nura_jacob@yahoo.com***shtsakin@yahoo.com 6 Abstract The general behavior of the reinforced concrete beams depends on many variables, including what is the quality of the concrete and strength and including those on reinforcement type and quantity of reinforcement in the beam. But there is an important variable which nature of loads application on the beam and type of load is it point or distributed. Sometimes the distance between points load is variable such as vehicle wheel load because each vehicle as different distance between wheels. In this research, the effect of changing the distance between the points load were studied and compared with model carrying a single point load at mid span, as well as studying the effect of the use of carbon fiber with a length equal to the distance between the points load. Theoretical results consists of eight models were compared in this study with the results of the previous experimental results. The study contains a discussion of the general behavior of the beam in addition to the study of the failure carrying load, cracking load, ductility and the relationship between the stages of load application and the deflection of concrete beams with and without carbon fiber sheets. Key words: Ansys, strengthening, ductility, carbon fiber. 1. Introduction Concrete structural components require the understanding into the responses of these components to a variety of loadings application. A simply-supported reinforced concrete beam may fail primarily- either in flexure or in shear. Failure in flexure will occur if the ultimate flexural moment capacity is exceeded at any section of the beam before the conditions for shear failure have been satisfied at any section. Failure in shear will occur when the limiting shear-moment capacity is reached at some section of the beam at which inclined cracks have developed sufficiently to reduce the available compressive area. Whether a given beam will fail in flexure or in shear will depend on the relative magnitudes of the ultimate flexural moment (Mf), the limiting shear-moment (Ms) and the critical shear(V) at various locations along the span and on the actual values of moment and shear at these locations. The relationship between mode of failure and properties of the beam cross-section and loading arrangement is illustrated most simply by considering the hypothetical behavior of a simply-supported beam as illustrated in Fig.(1). The beam shown in Figure (l) is simply-supported at its end span is assumed to carry two concentrated loads arranged symmetrically about mid span. Only half of the span is shown in the Figure, The distance from the support to the load is called the "shear-span" and is designated by the symbol (a). For the particular type of loading shown, the maximum moment and the maximum shear both occur at the location of the load and their ratio is M/V = a.
  • 2. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 Figure (1) Effect of moment-shear ratioon failure mode 7 2. Carbon Fiber Carbon fiber is defined as a fiber containing at least 92 wt % carbon, while the fiber containing at least 99 wt % carbon is usually called a graphite fiber. Carbon fibers generally have excellent tensile properties, low densities, high thermal and chemical stabilities in the absence of oxidizing agents, good thermal and electrical conductivities, and excellent creep resistance. They have been extensively used in composites in the form of woven textiles, prepregs, continuous fibers/rovings, and chopped fibers. The composite parts can be produced through filament winding, tape winding, pultrusion, compression molding, vacuum bagging, liquid molding, and injection molding. In terms of final mechanical properties, carbon fibers can be roughly classified into ultra-high modulus (>500 GPa), high modulus (>300 GPa), intermediate modulus (>200 GPa), low modulus (100 GPa), and high strength (>4 GPa)(1). Ehsan Ahmed et al(2). studied the flexural behavior of reinforced concrete beams strengthened with carbon fiber through an experimental and theoretical study includes six models, one without carbon fiber and the others with different number of layers of carbon fiber. They concluded that there is an increase in member stiffness in addition to improvement in yield and ultimate load. Another group of researchers (tom Norris et al.)(3) used in their research different ways to paste carbon fiber to concrete beams to see what is the proper way to use carbon fiber for strengthening the concrete beams, All ways showed that there is a clear improvement in carrying capacity of beams in addition to the improvement in ductility and yield load. 3. Test Program The experimental work program conducted by Mohammad Z.Y(4) was selected to validate the simulations presented in this paper. In his study, two experimental programs were carried out to investigate the behavior of reinforced concrete (RC) beams strengthened with CFRP fabrics between points load using a wet layup method. The aim of the research was to study the failure characteristics, deflection behavior and general performance. A total of six reinforced concrete beams were tested under two points bending with different distances between points of loading. In this test program, The variables of the beams were the distance between points load, CFRP bond length (equal to the distance between points load). To simulate the behavior under service, the beam named as (B) was selected. The geometrical properties and reinforcement details are illustrated in Table(1) and Figure (2). Table (1) Experimental Work Variables Beam No. Distance Between Point Load Length of Carbon Fiber B1 0 0 B2 20 20 B3 40 40 B4 60 60
  • 3. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 In this study, the main flexural and shear steel reinforcements in the finite element models were assumed to be an isotropic linear elastic material until the yield point. The ultimate and yield stresses are summarized in Table (2). The Poisson’s ratio of steel was taken as 0.3.Concrete properties are selected as (fc'=52.88, fr =4.75 and the Poisson’s ratio of steel was taken as 0.2). The dimensions of beams was selected (100x150)mm with 2ɸ4mm at the top ,2ɸ10 at the bottom and ɸ4@150mm shear reinforcement along the beam. Table (2) Steel Properties 8 Bar type Modulus of elasticity (kN/m2) Yield strength (fy) (MPa) Ultimate strength (fu) (MPa) Main Reinforcement 200000 484 719 Shear Reinforcement 200000 383 620 Figure (2) Reinforced Concrete Beam With Loading 4. Finite Element Analysis ANSYS computer program has been used for the finite element modeling. Four beams that have been studied were of a simply supported beamslengthof1.5mand an area100X150mm and loaded with two symmetrically placed concentrated vertical loads with Variable distances between point load, see Figure (3) below and Table (3). Table (3) shows the distances between the points load and length of carbon fiber sheets for each model. Model includes linear relationship to the properties concrete, a linear bond-slip relation and bilinear steel properties. The method of load application was applied incrementally each 2 kN. See Plate below which represents position of load application and position of supports. In ANSYS program symmetry properties were applied for the purpose of representation models. Figure (3) FEM Discretization for a Half of the Beam 1 X Y Z APR 12 2013 09:53:16 ELEMENTS U F
  • 4. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 Table (3) Distance Between Points Load Model Number Description Distance Between 9 Point Load (mm) Length of Carbon Fiber Sheet B1 Without carbon fiber one point load One point load ------- B2 With carbon fiber two point load 200 200 B3 With carbon fiber two point load 400 400 B4 With carbon fiber two point load 600 600 B1W Without carbon fiber one point load One point load ------- B2W Without carbon fiber two point load 200 200 B3W Without carbon fiber two point load 400 400 B4W Without carbon fiber two point load 600 600 5. Material Modeling SOLID65 isotropic element is used to represent the concrete material, since it has a capability of both cracking in tension and crushing in compression. SOLID65 element is defined by 8 nodes with three degrees of freedom at each node; translations in the nodal x, y, and z directions, see Figure below. LINK8 element (It is a uniaxial tension-compression member) is used to represent the reinforcing steel (main and stirrups steel material). LINK8 element is defined by two nodes with three degree of freedom at each node; translations in the nodal x, y, and z directions, see Figure below. SHELL41 element is used to represent the carbon fiber sheets. SHELL41 element is defined by four nodes with three degree of freedom at each node.it is a 3-D element having membrane (in-plane) stiffness but no bending (out of plane) stiffness. See Figure below. Figure (4) Solid 65 Figure (5) Link 8 Figure (6) Shell41
  • 5. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 5.1 Real Constants The real constants for this model are shown in Table below Table (4) Real Constant 10 Real constant set Element type Constant 1 SOLID65 concrete Real constant for Rebar 1 Real constant for Rebar2 Real constant for Rebar 3 Material number 0 0 0 Volume ratio 0 0 0 Orientation angle 0 0 0 2 LINK8 Reinforce-ment Steel Bar Diameter (f 10 mm ) Cross-sectional area 78.54 (mm2) Initial strain (mm/mm) 0 3 LINK8 Reinforce-ment Steel Bar Diameter (f 4 mm ) Cross-sectional area 12.566 (mm2) Initial strain (mm/mm) 0 3 SHELL41 CFRP CFRP type Fabric Shell thickness at node I (mm) 0.1 Shell thickness at node J (mm) 0.1 Shell thickness at node K (mm) 0.1 Shell thickness at node L (mm) 0.1 Element x- axis rotation 0 Elastic foundation stiffness 0 Added mass/unit area 0
  • 6. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 5.2 Material Properties The material properties for this model are shown in Table below: Table (5) Materials Properties 11 Material model number Element type Material properties 1 SOLID65 Linear Isotropic EX 34178 PRXY 0.2 Multilinear Isotropic Strain Stress Point 1 0.000464 15.864 Point 2 0.001 30.94 Point 3 0.00158 42.83 Point 4 0.0018 45.96 Point 5 0.00 3 52.88 Concrete ShrCf-Op 0.2 ShrCf-CI 0.3 UnTensSt 3.64 UnCompSt -1 BiCompSt 0 HydroPrs 0 BiCompSt 0 UnTensSt 0 TenCrFac 0 Material model number Element type Material properties 2 LINK8 Linear Isotropic EX 200000 PRXY 0.3 Bilinear Isotropic Yield Stress 484 Tang Mod. 0 3 LINK8 Bilinear Isotropic Yield Stress 383 Tang Mod. 0 Linear Isotropic EX 200000 PRXY 0.3 4 SHELL41 Linear Orthotropic Ex 234000 Ey 1 Ez 1 PRXY 0.3 PRYZ 0 PRXZ 0 Gxy, Gyz, Gxz 1 6. Theoretical Results 6.1 Failure Load After the data was analyzed and carefully considered, it can be said that the collected data of the failure load obtained from the theoretical solution for all beams is approximately equal experimental load and all the beams failed by flexure. The final loads for the ANSYS finite element method are the last applied load step before the solution diverges due to numerous cracks and large deflections. Through an extensive comparison between the unsupported specimens with carbon fiber and other supported specimens, it can be concluded that the specimens with carbon fiber have failure load more than other specimens without carbon fiber. This can be explained that the carbon fibers connecting both sides of the crack together and
  • 7. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 delay extension more during the concrete section (increase in tensile cracking strength of concrete due to confinement). Also, the increasing Length of the carbon causes an increase in the amount of carrying capacity to bending stresses, because the increase in length means cover as much as possible the bending area and are controlled more cracks generated during download stages. The moment generated in the mid length of the beam is the result of multiplying the reaction by the distance between the reaction and applied force (couple). When the distance between the two points load increased this leads to decrease of the distance between the applied force and the reaction, this leads naturally to a decrease in couple as a result of decrease in the distance between them, for the above reasons we can say that the increasing in the distance between the loading points provides to some extent an increase in carrying capacity for specimens. 6.2 Behavior at First Cracking The analysis of reinforced concrete beams in the linear region depends mainly on the appearance of cracks in that region where maximum bending stresses are concentrated. As was expected through a comparison between the different beams (different distances between the points of loading), the greater distance between points load delayed appearance of first cracks in the beams the reason for that is as stated previously that the increase in distance between point loads means decrease the applied moment on beam for same value of load if compared with the other models with less distance. A comparison of values obtained from the FE model and experimental can be seen in Table (6). The results in Table (6) indicate that the FE analysis of the beam prior to cracking is acceptable. The first cracks for the beams without carbon fiber (B1W, B2W, B3W and B4W) were observed at (27.27%, 25%, 26.6% and 26.3%) of the ultimate load respectively where for carbon fiber reinforced beam the first crack load was found to be between (13.63% to 15% ) the ultimate load. There is a 11.5% to 12.8% increase in ultimate load for carbon fiber reinforced concrete beams when compared with beams without carbon fiber reinforcement. Thus the experimental results show that there is increase in the ultimate load and the first crack load for the fiber reinforced concrete beams. Table (7) Cracking and Ultimate Load Deflection Model Load at First Cracking (kN) Centerline Deflection 12 (mm) Ultimate load (kN) Pcr/pultimate % Exper. Theo. Exper. Theo. Exper. Theo. Exper. Theo. B1 6.5 6 0.5 0.33 36 38 18 15.8 B1W 6 0.332 22 27.27 B2 7 6 0.255 0.3175 44 44 15.9 13.63 B2W 6 0.321 24 25 B3 9 8 0.54 0.386 54 58 16.6 13.79 B3W 8 0.392 30 26.6 B4 10.5 10 0.52 0.414 70 68 15 14.7 B4W 10 0.42 38 26.3
  • 8. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 Figure (7)Comparison Between Theoretical Cracking, Yielding and Ultimate load. 6.3 Load-Deflection Relationship The theoretical results for all specimens are displayed and compared with experimental results. Figures below contain a load-deflection curves predicted by ANSYS and the test results for all specimens Examined by Mohammad Z.Y.. The results of ANSYS converge with the non-strengthened specimens more than other strengthened specimens with carbon fiber because of not taking the slip between the concrete and the carbon fiber into account in the theoretical study. In general, the beams strengthened with carbon fiber were stiffer and more ductile than the control specimens with a higher ultimate load see Figure (7). In every stage of loading application, the deflections are reduced significantly thereby increasing the stiffness for the strengthened beams. 13 Figure (8) Experimental and Theoretical Load Deflection Curve for Beam (B1) Figure (9) Experimental and Theoretical Load Deflection Curve for Beam (B2)
  • 9. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 14 Figure (10) Experimental and Theoretical Load Deflection Curve for Beam (B3) Figure (11) Experimental and Theoretical Load Deflection Curve for Beam (B4) Figure (12) Theoretical Load Deflection Curve for Beam (B1) and (B1W) Figure (13) Theoretical Load Deflection Curve for Beam (B2) and (B2W) Figure (14) Theoretical Load Deflection Curve for Beam (B3) and (B3W) Figure (15) Theoretical Load Deflection Curve for Beam (B4) and (B4W) 6.4 Ductility Ratio of curvature at crushing of concrete to that at yielding of steel gives the numerical value of ductility, known as ductility index. It can be seen that for a given dimension and strength, the load versus displacement curves for both specimens with carbon fiber and other specimens without carbon fiber appear similar. In addition, as can be seen in Table (8) the deflection at yielding and ultimate strength for beams without carbon fiber appear lower than those of beams with carbon fiber. It has been known that the deflection ductility, μΔ, in terms of ultimate deflection to yielding displacement, is highly correlated to the length of the carbon fiber sheet. As can be seen in Table (8),
  • 10. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol.6 No.8, 2014 the ductility of both types of concrete beams exhibit a extrusive length effect, i.e., ductility increase with the increase of carbon fiber sheets, namely, a strengthened beam performs more ductile. The effect of increasing the distance between the points load seemed clear as when you increase this distance increases the ductility due to decrease moments that cause for ultimate deflection in the beam at failure. Table (8) Ductility of tested beams Beam No. Deflection at Yield (mm) Deflection at Failure (mm) Ductility Index B1 4.16 12.5045 3 B2 4.64 13.4386 2.896 B3 5.09 18.357 3.606 B4 4.97 18.3 3.682 B1W 3.1 5.22 1.683 B2W 3.6 4.01 1.113 B3W 4.3 15.822 3.679 B4W 4.7 4.917 1.046 7 .Conclusions Based on the results obtained from theoretical analysis and comparison with the experimental work, the following conclusions are drawn: 1. At any given load level, the deflections are reduced significantly thereby increasing the stiffness for the 15 strengthened beams. 2. All the beams strengthened with carbon fiber experience flexural failures. None of the beams exhibit brittle failure. 3. The failure load of specimens with carbon fiber more than other specimens without carbon fiber. 4. The bending stresses are reduced when length of the carbon was increased. 5. The increasing in the distance between the loading points provides an increase in carrying capacity for specimens. 6. In this study, the appearance of the first crack mainly depends on the distance between the points load, higher distance between the mount points load lead to the delay in appearance of the cracks. 7. Through the adoption of the distance between the point load as a variable show that increasing the distance between the points load result a decreasing in moment in the mid span of the beam, this means an increase in carrying capacity for specimens. 8. Through a comparison theoretical results with the experimental, showing that there is a convergence between the two results. 9. It is very clear the development in ductility as a result of increasing the length of carbon fiber sheets and increase the distance between the points load. References 1. Xiaosong Huang, " Fabrication and Properties of Carbon Fibers ",www.mdpi.com. 2. Ehsan, A., Habibur, R. and Norsuzailina, M. S., " Flexural performance of CFRP strengthened RC beams with different degrees of strengthening schemes", International Journal of the Physical Sciences, Malaysia, Vol. 6(9), 4 May, 2011, pp. 2229-2238. 3. Tom, N., Hamid, S., Mohammad, R., " Shear and Flexural Strengthening of Reinforced Concrete Beams with Carbon Fiber Sheets", Journal of Structural Engineering, Vol.123, No.7, July, 1997,PP.903-911. 4. Mohammad, Z., " Reinforced Concrete Beams Strengthening by Carbon Fiber Reinforced Polymer Against Two Points Load Divergence", Journal of Engineering and Development" Vol.16, No.2, June, 2012 ,PP.266-280.
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