Abstract

In this study, a new shear strengthening technique for reinforced self-compacting concrete (RSCC) deep beams was suggested and compared with some traditional techniques. An experimental test program consists of sixteen specimens of RSCC deep beams strengthened by different materials such as steel, glass, and carbon fiber reinforced polymers (GFRP and CFRP) was executed. Externally bonded layers (EBLs) and near-surface mounted reinforcement (NSMR) were used as two different techniques. The effects of the new technique which depends on using intertwined roving NSM GFRP rods saturated with epoxy were compared with the other models. The new technique for shear strengthening increases the load capacity from 36% to 55% depending on the anchorage length of GFRP rods. Two-dimensional nonlinear isoperimetric degenerated layered finite elements (FEs) analysis was used to represent the SCC, reinforcement, and strengthening layers of the tested models. The analytical results have been very close to the experimental results.

1. Introduction

Reinforced concrete (RC) deep beams were often used and encountered in many structural applications such as diaphragms, bridges, water tanks, precast and prestressed construction, foundations, silos, bunkers, offshore structures, and tall buildings [1, 2]. Deep beams are widely used as transfer girders in offshore structures and foundations. with the strong growth of construction work in many developing countries, deep beam design and its behaviour predication are a subject of considerable relevance.

Many experimental studies have been performed to investigate the behavioral characteristics and the cause of the shear failure of RC beams [35]. Several researchers [68] and the current codes [911] have recommended the design of deep beams using the strut-and-tie model. In these strut-and-tie models, the main function of shear reinforcement is to restrain diagonal cracks near the ends of bottle-shaped struts and to give some ductility to struts.

Thin deep girders often contain congested shear reinforcement within the web, the normal concrete often does not flow well when traveling through the web and does not completely fill the bottom bulb. This results in voids in the concrete finish, which often termed bug holes or a honeycombing effect in the finished concrete surface. In this case, many researches recommended the use of self-consolidating concrete (SCC) [1214]. Self-consolidating concrete, also known as self-compacting concrete, yields distinct advantages over typical concrete due to its liquid nature such as (a) low noise level in construction sites, (b) eliminated problems associated with vibration, (c) less labor involved, (d) faster construction, (e) improved quality and durability, and (f) higher strength. In Egypt, SCC is beginning to gain interest, especially for the precast concrete, prestressed concrete, and cast-in place construction [15]. Self-consolidating concrete was first developed in 1988 by Okamura and Ouchi [16] to achieve durable concrete structures. Since then, various investigations have been carried out and this type of concrete has been used in practical design method in different countries, mainly by large construction companies. Japan has used SCC in bridge, building, and tunnel construction since the early 1990s. A number of SCC bridges have been constructed in Europe [16, 17] and United States [18]. However, SCC is heavyly used in precast and prestressed concrete industry [19, 20].

Although SCC is a material of the future, it does not come without some disadvantages. SCC is typically made with smaller coarse aggregate sizes and a larger amount of fine materials. This may lead to a higher shrinkage values and also can negatively affect the tensile strength and shear strength of the concrete [21].

Increasing the shear strength of reinforced self-compacting concrete RSCC deep beams may be required in many cases such as change of building use, the need to perform an opening in deep beams for air conditioning, corrosion of reinforcement and finally due to construction or design errors [22]. Strengthening using advanced composite materials such as fiber-reinforced polymer (FRP) rods, strips, or woven wraps are being increasingly recognized for enhancing flexural and shear strength of concrete members instead of the traditional materials represented by steel bars or strips [22, 23]. Repair and strengthening of structural members with composite materials, such as carbon, glass, Kevlar, and aramid fiber-reinforced polymers, have recently received great attention [24, 25]. Reduced material costs, coupled with labor savings inherent with its lightweight and comparatively simple installation, its high tensile strength, low relaxation, and immunity to corrosion, have made FRP an attractive alternative to traditional retrofitting techniques. Field applications over the last years have shown excellent performance and durability of FRP-retrofitted structures [24, 25]. Nowadays, carbon and glass fiber strips, rods, and wraps woven in one or multidirections are widely used as strengthening materials.

Many researchers used FRP for strengthening the flexure strength of beams. Several studies investigated the use of externally bonded FRP composites [23, 24] or near-surface mounted reinforcement (NSMR) [2630] to improve the strength and stiffness of RC members.

This paper investigated a series of test specimens consisting of sixteen test specimens. This research has been conducted to assess and compare the ability and efficiency of traditional materials represented by steel bars, strips, or plates as well as advanced composite materials (ACMs) represented by GFRP and CFRP woven wraps for shear strengthening of RSCC deep beams with a central opening. The behavior and the results of the tested beams were presented, discussed, and analyzed in illustrated figures for the purpose of comparison.

A numerical analysis for modeling the method of strengthening of RSCC deep beams was developed and a computer program was prepared to model such case study. This paper explains the method of analysis using 2D nonlinear isoperimetric degenerated layered finite elements with eight nodes and five degrees of freedom at each node. The layered technique was used to represent the SCC, steel reinforcement, and the different strengthening layers of the tested deep beams. The proposed FE model results have been verified and compared by the experimental test results.

1.1. Research Objectives

The main objective of this research is to determine the improvement of the shear strength of RSCC deep beams using a new innovative technique. This technique is applied using NSM GFRP rods manufactured from intertwined GFRP roving saturated with epoxy resin in vertical and inclined directions at both sides of the beam surfaces. These rods were anchored through the thickness of the beam web in transverse direction. The new method of strengthening was compared with some other common techniques such as external bonded layers of steel and FRP wraps as well as with NSMR using steel strips and bars as well as CFRP strips and wraps in order to insure the effectiveness of the new developed method.

The goal of this research is extended to introduce a new model for the nonlinear FE method using a high performance isoparametric degenerated layered element to represent all the composite materials such as SCC, reinforcement, and strengthening layers. The FE model will be interpreted to a developed computer program to ease the analysis of many cases with other boundary conditions or material characteristics. The results of the numerical program will be verified by the experimental results.

2. Experimental Test Program

An experimental test program was carried out to investigate the behavior of RSCC deep beams strengthened using EBL and NSMR techniques. Steel, GFRP, and CFRP were used as the main strengthening materials.

The experimental program consists of sixteen test specimens that have constant cross-section with dimensions of 1200 × 500 mm and effective span (1000 mm). One specimen without opening and the other fifteen test specimens were cast with a central opening of dimension 200 × 200 mm. Each beam has a lower longitudinal reinforcement, 4Φ16 mm as a main flexural reinforcement of high tensile steel, top reinforcement 2Φ10 mm as stirrup hangers, 4Φ6 as side reinforcement and stirrups 𝜙6 mm @15 cm of mild steel. Two beams were considered as a reference control beams. One beam without opening identified BR and the other with a central opening identified BOR. Figure 1 shows the dimensions and the details of reinforcement for the reference beam BOR.

3. Materials Properties and Mix Design

SCC can be largely affected by the characteristics of materials and mix proportion. In this research, the mix design of SCC is based on a CIB method [15]. The properties of the materials used in this study were summarized as follows.

3.1. Cement

A locally produced ordinary Portland cement complied with E.S.S.373/91 requirements.

3.2. Aggregates

The fine aggregates were siliceous natural sand. The coarse aggregates were crushed dolomite with maximum nominal size 14 mm.

3.3. Silica Fume

It is a product resulting from the industry of Ferro-silicon alloys; the product is a rich silicon dioxide powder where the average size is a round 0.1 micrometers [31].

3.4. Fly Ash

One of the mineral admixtures used in this experimental is fly ash, its commercial name is Supper Pozz-5 [31].

3.5. Viscosity Enhancing Agent (VEA)

It is the superplasticizer used in this experimental and its commercial name is Sika-Viscocrete 5–400 from Sika Egypt [31].

Table 1 gives the chosen mix proportions of materials used for casting the RSCC deep beam models and Table 2 shows the properties of the used reinforcement steel.

4. Strengthening Schemes

Two reference RSCC deep beams labeled BR and BOR were loaded till failure without strengthening. The letter “R”stands for reference beam, and the letter “O” stands for beam with an opening. The other fourteen models were classified into three groups according to the strengthening materials. Three main materials were used for purpose of comparison. Steel bars 𝜙6 mm, steel plates 1 mm and 3 mm thickness were used as traditional materials, while GFRP roving and wraps as well as CFRP strips and wraps were used as advanced strengthening materials. Two main techniques for shear strengthening were executed. The first by using NSM vertical and inclined reinforcement as shown in Figure 2, and the second by EBL as shown in Figure 3. The three groups were summarized as follows.

4.1. Group (A)

Group (A) contains six models strengthened by steel; BOVSB, BOVSP=, BOVSP, BOVSP3, BOISB and BOSPL. The letter “V” stands for vertical strengthening, and “I” for inclined strengthening, while the letters “SB” stands for steel bars, and “SP” for steel plates. The symbol “=” indicates that the long side of the cross-section of the strip is parallel to the surface of the beam, while the symbol “” points to strengthening with strips in transverse direction to the surface, and “3” refers to strengthening with steel strips 3 mm thickness. “L” indicates strengthening by steel plates as external layers.

4.2. Group (B)

Group (B) consists of five models strengthened with NSM vertical and inclined GFRP intertwined rods manufactured manually from E-glass roving embedded in epoxy resin as a new technique, and also with GFRP woven wraps as EBL (Figures 2 and 3). The five models are BOIG1, BOIG2, BOVG1, BOVG2, and BOGW. The letter “G” stands for strengthening by GFRP, and (1, 2) indicate two different cases of anchored length 20 mm and 100 mm through the beam web in transverse direction, respectively. The letter “W” stands for strengthening by FRP woven wraps.

4.3. Group (C)

Group (C) comprises three models strengthened with CFRP; BOVC=, BOVC, and BOCW. The letter “C” stands for strengthening by CFRP.

Figures 2 and 3 show the different shear strengthening by NSMR and EBL techniques, respectively. In NSMR, a groove was cut in the desired direction throughout the concrete surface. The size of the groove was made to allow for clearance around the rod as shown in Figure 4. The rut was then filled halfway with epoxy paste, the strengthening reinforcement was placed in its position and lightly pressed. To force the paste to flow around the rod and fill completely any space between the rod and the sides of the groove. The groove was then filled with more paste and the surface was leveled. Steel bars and plates, GFRP intertwined rods manufactured manually from E-Glass Roving and epoxy resin [31] as showed in Figure 5 as well as CFRP strips were used as NSMR.

In the second technique, additional external bonded layers were then bonded to the concrete surfaces of the RSCC model using epoxy resin. Steel plates, GFRP woven wraps in two perpendicular directions and also CFRP woven wraps in unidirection were used. Different types of FRP used in this research are showed in Figure 6.

Table 3 shows the properties of FRP strengthening materials used in this research work.

Table 4 summarizes the experimental test program and specifies the RSCC deep beams in different groups.

5. Test Setup and Instrumentation

The reference beams were loaded up to failure without strengthening, while the other beams were loaded after strengthening up to failure. Models were tested under two concentrated loads. A steel frame of 200 ton capacity was used for testing beams in RC laboratory Collage of Engineering, Menoufiya University, Egypt. Loads were applied in increments using a hydraulic jack of 100 ton maximum capacity as shown in Figure 7. Dial gauges of 0.01 mm accuracy and a total capacity of 25 mm were fixed to measure the deflection at midspan, under the two concentrated loads and at 100 mm form the end supports. Demec points were arranged and fixed on the painted side of each tested beam near top and bottom surfaces of the beam in four rows at the center of span. Concrete strains were measured by mechanical strain gauges of 200 mm gauge length and 0.001 mm accuracy. A magnifying lens was used to observe the crack propagation clearly. Cracks were traced and marked at each load increment. Figure 7 shows the arrangement of dial gauges and Demec points.

6. Analysis of the Test Results

The different groups of RSCC deep beams were tested. The results were illustrated and compared at different stages of loadings. The load-deflection curves were plotted, the first cracking and failure loads were recorded and compared. The crack propagations were also marked after each load increment and photographed at failure.

6.1. Deflection

Figure 8 compares the load deflection curves at midspan for beams strengthened by the new technique using vertical NSM intertwined roving GFRP rods with that strengthened with NSM vertical steel bars. The results were compared also with the reference beam BOR. At the ultimate failure load of BOR, deflections of beams, BOVSB, BOVG1, and BOVG2 were decreased by about 42%, 28%, and 31% respectively. Figure 9 shows the load deflection curves at midspan for beams strengthened by the new technique using inclined NSM intertwined roving GFRP and the beams strengthened with NSM inclined steel bars. At the ultimate failure load of BOR, deflections of beams, BOISB, BOIG1, and BOIG2 were decreased by about 22%, 19%, and 36%, respectively. It is clear from Figures 8 and 9 that the new technique using GFRP improves the structural behavior and the reduction of the deflections increases with increasing the anchorage length.

Figure 10 compares the load deflection curves at midspan for beams strengthened by using vertical NSM parallel and transverse strips. At the ultimate failure load of BOR, deflections of beams, BOVSP=, and BOVC= were decreased by about 29% and 39%, respectively. Deflections of beams BOVSP, BPVSP3, and BOVC were decreased at the same level by about 22%, 42%, and 52%, respectively. The results of using vertical transverse strips showed better improvement than using the parallel strips. The maximum reduction was recorded by CFRP strips in the transverse direction.

Figure 11 shows that the use of EBL at both sides of RSCC deep beams improves the structural behavior. At the ultimate failure load of BOR, deflections of beams, BOSPL, BOGW, and BOCW were decreased by about 11%, 20, and 26%, respectively.

6.2. Cracking and Ultimate Loads

The first cracking and the ultimate failure loads were recorded for the tested beams. All the tested RSCC deep beam models failed in shear. Figure 12 compares both cracking and failure loads of the different groups of beams with the reference control beams. It is clear that the ultimate load of the control beam BR was higher than the ultimate load of control beam BOR by about 9%. As compared with the control beam BOR, the increases in the ultimate failure loads in Group (A) recorded for strengthened beams BOVSB, BOISB, and BOSPL were about 36%, 27%, and 9%, respectively. But the increase were about 13%, 31%, and 60% for beams BOVSP=, BOVSP and BOVSP3, respectively. In Group (B), the increases were about 36% and 55% for beams BOVG1 and BOVG2, while they were about 11% and 15% for beam BOIG1 and BOIG2 respectively. In Group C, the capacity of the strengthened beams BOVC=, and BOVC, were increased by about 35% and 55% of that recorded for BOR, respectively.

It was noticed form the comparison that the new technique which used intertwined roving NSM GFRP rods results in improving the overall structural behavior with respect to the traditional methods. Anchoring the rods with 100 mm drilled through the web in the transverse direction for beam BOVG2 increased the load capacity by about 13% than beam BOVG1 when the anchorage length was only 20 mm. So, it is recommended to increase the anchorage length in the transverse direction to increase the effect of the strengthening process.

The comparison also shows that shear strengthening using NSM CFRP strips in the transverse direction to the face gives the best results of both deflection and ultimate failure loads. It was noticed also that shear strengthening using NSMR increases the ultimate capacity more than the EBL technique with the corresponding material in this case study.

6.3. Cracking Patterns

Figures 13 and 14 show the crack patterns at different loading stages for beams strengthened by NSM technique. The mode of failure for all illustrated beams was shear failure. It is shown from the figures that the presence of central opening has small effect in case of shear failure.

Figure 13 shows crack patterns of RSCC deep beams strengthened by inclined reinforcement. It was found that cracks started from the lower level near the center of the beam at the tension side and developed upward. For further loading, the cracks developed in the region near supports and were directed towards the loading position till the failure forming a shear failure. It is noticed from Figures 13(a) and 13(b) that strengthening bars arrest cracks form developing in the regions of strengthening. Cracks developed around the outer perimeter of the strengthening areas as shown. It is recommended to increase the length of the inclined NSM bars to get better results. Figures 13(c) and 13(d) show the crack patterns of beams, BOIG1 and BOIG2, strengthened by inclined intertwined roving NSM GFRP rods with anchorage lengths 20 mm and 100 mm, respectively. It is shown that increasing the anchorage length of the strengthening bars improves the results and increases the loading capacity.

Figure 14 shows the crack patterns of RSCC deep beams strengthened by NSM vertical reinforcement. Beam BOVSP3 had maximum load capacity as shown in Figure 14(b). Figure 4(c) indicates that using the vertical intertwined roving NSM GFRP rods improves the results. It is noticed from Figure 14(d) that shear strengthening with NSM CFRP vertical strips in the transverse direction to the surfaces gives good results.

7. Finite-Element Analysis

The reinforced concrete beams were modeled in many researches by 3D FE analysis with steel reinforcement as embedded bars [3237] SCC reinforced with FRP bars was modeled also by 3D isoparametric elements [32, 33]. In this research, RSCC deep beams were modeled using 2D plane stress isoparametric degenerated layered finite elements. The applied two-dimensional elements are degenerated from the three-dimensional elements [32, 33]. The main features of the chosen element and the nonlinear procedures will be reviewed briefly.

7.1. Geometric Definitions of the Element

Transverse shear deformations were considered by applying Reissner-Mindlin plate theory which permits the applications for both thin and thick elements. The finite element has eight nodes. Each node of the element is specified by three coordinates 𝑥, 𝑦, and 𝑧 for both the top and bottom coordinates of each node to enable the representation of the element in the space. The relation between the Cartesian coordinates of any node and the curvilinear coordinates can be written for 8-node degenerated element as follows:𝑥𝑦𝑧=8𝑖=1𝑁𝑖𝑥(𝜉,𝜂)𝑖𝑦𝑖𝑧𝑖mid+8𝑖=1𝑁𝑖𝜁(𝜉,𝜂)2𝑉3𝑖,(1) where 𝑁𝑖(𝜉,𝜂) are the shape functions and 𝜉, 𝜂, 𝜁 are the curvilinear coordinates of the point𝑉3𝑖=𝑥𝑦𝑖𝑧𝑖top𝑥𝑖𝑦𝑖𝑧𝑖bottom,(2) where 𝑉3𝑖 is a vector constructed from the nodal coordinates of the top and bottom surfaces at the node 𝑖 as shown in Figure 15(a). The shape functions for the eight boundary nodes are illustrated in Figure 15(b) which are serendipity shape functions and defined by the following equations.

(i) For corner nodes (𝑖=1,3,5,7):𝑁𝑖=141+𝜉𝜉i1+𝜂𝜂𝑖𝜉𝜉𝑖+𝜂𝜂𝑖1.(3)

(ii) For midside nodes (𝑖=2,4,6,8):𝑁𝑖=𝜉2𝑖21+𝜉𝜉𝑖1𝜂2+𝜂2𝑖21+𝜂𝜂𝑖1𝜉2.(4)

7.2. Displacements

The displacement field is described by five degrees of freedom; three displacements of the midsurface node (𝑢, 𝑣, 𝑤) and two rotations (𝛼𝑖, 𝛽𝑖) as follows:𝑢𝑣𝑤=8i=1𝑁𝑖u(𝜉,𝜂)iviwimid+8i=1𝑁𝑖(𝜉,𝜂)8𝑖=1𝑁𝑖(𝜉,𝜂)𝜁𝑖2×𝑉1𝑖𝑉2𝑖𝛼𝑖𝛽𝑖,(5) where 𝑖 is the thickness of the element at the node 𝑖𝑉1𝑖=𝑖×𝑉3𝑖,𝑉2𝑖=𝑉1𝑖×𝑉3𝑖,(6) in which 𝑖 is the unit vector in the 𝑥-direction.

7.3. Layered Discretization

The FE can be divided into an optional number of concrete, steel, and any additional repair or strengthening layers as shown in Figure 16.

Each layer may have different material properties corresponding to its state of stress. The stresses are computed at the midsurface of the layer and are assumed to be constant over the thickness of each layer as shown in Figure 17. Different layer thicknesses can be taken into account as well as different numbers of layers per element.

The layer thickness was defined in terms of curvilinear coordinate 𝜁 to permit the variation of the layer thickness when the element thickness varies. The stiffness of the element 𝐾𝑒 is obtained by numerical integration through the thickness:𝑘𝑒=𝐵𝑇𝐷𝐵𝑓𝐽𝑑𝜁𝑑𝜉𝑑𝜂,𝑒=𝐵𝑇𝜎𝐽𝑑𝜁𝑑𝜉𝑑𝜂,(7) where 𝐵 is the strain matrix composed of derivatives of the shape functions and 𝐽 is the determinant of the Jacobian matrix.

8. Nonlinear Constitutive Model

The FE technique permits more realistic analysis for reinforced concrete complexities which arise from concrete cracking, tension stiffening, nonlinear multiaxial material properties, and complex interface behavior. In the present study, both the perfect and the strain-hardening plasticity approaches are considered to model the compressive behavior of the concrete. The flow theory of plasticity [34] is employed to establish the nonlinear stress-strain relations in the plastic range. The assumed yield criterion used in this analysis depends on the Kupffer’s results and can be defined as follows:𝜎𝑓(𝜎)=1.355𝑥2+𝜎𝑦2𝜎𝑥𝜎𝑦𝜏+3𝑥𝑦2+𝜏2𝑥𝑧+𝜏yz2+0.335𝜎𝑜𝜎𝑥+𝜎𝑦2=𝜎𝑜.(8)

The yielding criteria of this expression as well as Kupffer’s results and Von-Mises assumptions are compared in Figure 18.

The tension stiffening effect is considered by assuming a gradual release of the concrete stress component normal to the cracked plane [3234] as shown in Figure 19. The modulus of elasticity is decreased as the strain increases due to cracking following the next formula:𝐸𝑖=𝛼𝑓𝑡𝜀𝑖𝜀1𝑖𝜀𝑚;𝜀𝑡𝜀𝑖𝜀𝑚,(9) where 𝑓𝑡 is is the modulus of rupture of the concrete and 𝛼, 𝜀𝑚 are tension stiffening parameters.

Shear retention factors can strongly influence a nonlinear solution, especially if shear is prominent as the case of deep beams [34]. To achieve the aim of incorporating a realistic shear retention factors in order to model shear transfer across cracked concrete, a quadratic function is used [3537] based on the assumption of direct strain normal to the crack.

8.1. Reinforcement and Strengthening Layers

The properties of the strengthening materials of bars, strips, or wraps are generally well defined. Each strengthening layer has an uniaxial behavior, resisting only axial forces in the bar or fiber direction.

In this research reinforcing or strengthening bars are replaced by equivalent smeared distributed lamina. The equivalent thickness of the lamina is considered as follows:𝑡𝑠=𝐴𝜙b=𝜇×𝑑,(10) where 𝐴𝜙 is the cross-sectional area of one bar, b is the spacing between bars, 𝜇 is the reinforcement ratio, and d is the effective depth of the element. The thickness of the strengthening layer and the effective depth are specified in the analyses by the curvilinear coordinate 𝜁. The orthotropic layer can be assumed to be isotropic in plane 1. If the lamina principal axes (1, 2) do not coincide with the reference axes (𝑥,𝑦) but are at some arbitrary orientation 𝜃 to them as shown in Figure 20, the constitutive relationship for each individual lamina is transformed to the reference axes. In the analysis, smeared layers are assumed to be fully bonded with concrete.

8.2. Verification of the FE Model

The previous proposed FE model is performed for the analysis of RSCC deep beams strengthened with inclined and vertical NSM reinforcement for GFRP intertwined roving rods. Figures 21 and 22 show the FE meshes for the analysis of both vertical and inclined strengthening.

Figure 23 compares the load deflection curves for the experimental and numerical results of the beam models BOR, BOVG2, and BOIG2. The FE results showed a good agreement with the experimental test results at different loading stages. At failure loads, the deflections by FE of beams BOR, BOVG2, and BOIG2 were decreased by about 11%, 12.5%, and 11.5%, respectively.

Figure 24 compares the ultimate loads of the investigated beams for both experimental and analytical results. The numerical results gave small increases than the experimental results. Specimens BOR, BOVG2, and BOIG2 showed differences of 9%, 12%, and 11%, respectively. It can be observed that the suggested FE model is quite accurate in representing the problem and can be used to study different cases of strengthened specimens that are not included in the experimental program.

9. Conclusions

The following conclusions can be drawn from this research work.(1)In this study, shear strengthening using NSM reinforcement increases the ultimate load capacity more than the EBL technique when using the same material.(2) The new technique suggested in this research work which depends on using intertwined roving NSM GFRP rods saturated with epoxy proved to be efficient for shear strengthening of RSCC deep beams with respect to the traditional methods.(3) In case of strengthening by vertical NSM intertwined roving GFRP rods, anchoring the rods through the web thickness in the transverse direction increases the ultimate load capacity by about 55%.(4) Using vertical NSM steel or CFRP strips in transverse direction to the face gives better results than using it in parallel direction.(5) In this study, it was noticed that using NSM vertical reinforcement gives higher capacity than inclined reinforcement, and this may be attributed to the increase of the strengthened area. It is recommended to the increases of the length of the inclined bars to get better results.(6) Isoparametric degenerated layered elements can represent self-consolidating concrete, steel reinforcement, different strengthening materials, and techniques such as NSM FRP rods or externally bonded FRP layers.(7)The suggested FE model for shear strengthening is quite accurate in representing the problem and the developed FE computer program can be applied to study different cases of strengthening that are not included in the experimental program.

Symbols

𝑉3𝑖:The vector constructed from the nodal coordinates of the top and bottom surfaces at the node 𝑖
𝑁𝑖 (𝜉, 𝜂):The shape functions
𝜉, 𝜂, 𝜁:The curvilinear coordinates of the point
(𝑢, 𝑣, 𝑤):The displacements of the mid-surface node
(𝛼𝑖, 𝛽𝑖):The two rotations
𝑖:The thickness of the element at the node 𝑖
𝐾𝑒:The stiffness of the element
𝐵:The strain matrix composed of derivatives of the shape functions
𝐽:The determinant of the Jacobian matrix
𝑓𝑡:The modulus of rupture of the concrete
𝛼, 𝜀𝑚:The tension stiffening parameters
𝐴𝜙:The cross-sectional area of one bar
𝜁:The curvilinear coordinate
(𝑥,𝑦):The reference axes
𝑏:The spacing between bars
𝜇:The reinforcement ratio
𝑑:The effective depth of the element.